Stopping Powers and Ranges of

Electrons and Positrons (2nd Ed.)

U.S. DEPARTMENT OF COMMERCE

National Bureau of Standards

Washington, DC 20234

December 1982

Issued February 1 983

Prepared for: U.S. DEPARTMENT OF COMMERCE

National Bureau of Standards

Office of Standard Reference Data

Washington, DC 20234

w

-QC

100

,U56

02-2550-A

1902

Office of Health and Environmental Research

Department of Energy

Washington, DC 20545

ffice of Naval Research

rlington, Virginia 22217

NATIONAL BUREAU! OF STANDARDS

LIBRARY ^

10 1983

NBSIR 82-2550-A

STOPPING POWERS AND RANGES OF

ELECTRONS AND POSITRONS (2nd Ed.)

M. J. Berger and S. M. Seltzer

U.S. DEPARTMENT OF COMMERCE

National Bureau of Standards

Washington, DC 20234

December 1982

Issued February 1983

Prepared for: U.S. DEPARTMENT OF COMMERCE

National Bureau of Standards

Office of Standard Reference Data

Washington, DC 20234

Office of Health and Environmental Research

Department of Energy

Washington, DC 20545

Office of Naval Research

Arlington, Virginia 22217

U.S. DEPARTMENT OF COMMERCE, Malcolm Baldrige, Secretary

NATIONAL BUREAU OF STANDARDS. Ernest Ambler, Director
k
STOPPING POWERS AND RANGES OF ELECTRONS AND POSITRONS

M. J. Berger and S. M. Seltzer

Center for Radiation Research

National Bureau of Standards

Washington, D.C. 20234

ABSTRACT

Tables of stopping powers and related data are given for electrons in

25 elements and 46 mixtures and compounds, and for positrons in 14 materials.

The tables include: (1) collision stopping powers (ionization and excitation

losses); (2) radiative stopping powers (bremsstrahlung losses); (3) total

stopping powers; (4) ranges (rectified pathlengths computed in the continuousslowing-down approximation); (5) radiation yields (fraction of initial

electron energy converted to bremsstrahlung in the course of slowing down)

;

and (6) the logarithmic derivatives of all these quantities with respect to the mean excitation energy of the medium (the key parameter of the Bethe

stopping power formula) . The results are tabulated at 81 energies between

1000 MeV and 10 keV. Collision stopping powers for electrons in materials

of low atomic number are given also for energies down to 1 keV. The

principal new ingredients in the preparation of the tables are: (1) improved

values of the mean excitation energies for elements and compounds, derived

from stopping-power and range measurements and from semi-empirical oscillatorstrength distributions and dielectric- response functions; (2) density-effect

corrections evaluated according to the method of Sternheimer, using up-to-date

input parameters; and (3) use of new theoretical cross sections of Pratt and

Tseng for electron-nucleus bremsstrahlung and of Haug for electron-electron

bremsstrahlung

.

Key words: Collision stopping power; electrons; positrons; radiation yield;

radiative stopping power; range.

These tables were prepared as input for a report on stopping power to be written

by a committee sponsored by the International Commission on Radiation Units and

Measurements (ICRU). The ICRU sponsors of this committee are A. Allisy and

R. S. Caswell. The committee members are H. H. Andersen, M. J. Berger (chairman),

H. Bichsel, J. A. Dennis, M. Inokuti^D. Powers, S. M. Seltzer, and J. E. Turner.

R. M. Sternheimer is a consultant to the committee. All of the above have made

important contributions to this work. It should be emphasized that this report is

a draft submitted to the ICRU, and may be revised before being included in an ICRU

document

.

We would like to acknowledge the financial support for this work provided by the

NBS Office of Standard Reference Data, the Office of Health and Environmental

Research of the Department of Energy, and the Office of Naval Research.

Last but not least we would like to thank Mrs. Gloria Wiersma for her editorial

help in the preparation of the manuscript.

'This report is a revised edition of NBSIR 82-2550 (August 1982), and contains

updated information on positron stopping powers and ranges. The radiative stopping

power for positrons, previously assumed to be the same as that for electrons, has

been evaluated on the basis of recent theoretical results (see Section 9.4). Small errors pertaining to the density-effect correction for positrons in graphite, ASL , Cu, Ag and Pb have been corrected, and various typographical errors have been

eliminated.
\
TABLE OF CONTENTS

ABSTRACT i

1. INTRODUCTION 1 1.1. Purpose and scope

1.2. Background

1.3. New features

2. FORMULAS FOR THE COLLISION STOPPING POWER 3

2.1.

General Formulas

2.2. Stopping-power formulas for heavy charged particles

2.3. Stopping-power formulas for electrons and positrons

3. METHODS FOR ESTIMATING MEAN EXCITATION ENERGIES

3.1. Use of oscillator-strength and dielectric data

3.2. Use of stopping-power and range data

3.2.1. Bichsel's shell corrections

3.2.2. Comparisons of Bichsel's and Bonderup's shell correction

4. SELECTION OF MEAN EXCITATION ENERGIES FOR ELEMENTS 12

5. SELECTION OF MEAN EXCITATION ENERGIES FOR COMPOUNDS 13

6. DENSITY EFFECT 16

6.1. Cfinfiral Rdiiatinns

6.2. Sternheimer ' s model

6.3. Numerical evaluation

6.4. Complications for inhomogeneous media

7. RESTRICTED COLLISION STOPPING POWER 19

8. ELECTRON COLLISION STOPPING POWERS AT LOW ENERGIES 20

8.1. Calculations for gases

8.2. Calculations for solids and liquids

8.3. Comparison of stopping powers

9. RADIATIVE STOPPING POWER 23

9.1. Electron-nucleus bremsstrahlung

9.1.1. High-energy region

9.1.2. Low-energy region

9.1.3. Intermediate energy region

9.2. Electron-electron bremsstrahlung

9.2.1. High-energy region

9.2.2. Low-energy region

9.2.3. Intermediate energy region

9.3. Accuracy and comparison with experiments

9.4. Positron bremsstrahlung

10. RANGES AND RADIATION YIELDS 26

11. MISCELLANEOUS COMPARISONS 27

11.1. Positron-electron differences

11.2. Comparison of calculated and experimental stopping powers

11.3. Comparisons with previous calculations

REFERENCES 2 9 TABLES TO ACCOMPANY TEXT 41

FIGURES 66

MAIN STOPPING-POWER AND RANGE TABLES 79

li

1. INTRODUCTION

1.1. Purpose and scope . In radiation physics, chemistry, biology, and medicine,

it is often important to have accurate information about the stopping power of

various media for charged particles, that is, the average rate at which the charged

particles lose energy along their tracks. The purpose of this report is to supply

up-to-date stopping -power information, with emphasis on the requirements of biomedical

dosimetry. The contents of this report are the following: (a) In Sections 2 to 6,

topics are reviewed which are pertinent to the evaluation of stopping powers for any

charged particle within the framework of the Bethe theory. 1 These include shell

corrections, the determination of mean excitation energies from experimental data,

the use of the Bragg additivity rule for compounds, and the density-effect correction.

Recommended values of mean excitation energies are given in Table 4.3 for elemental

substances and in Table 5.5 for compounds and mixtures. (b) In Sections 7 to 11,

topics are reviewed which are pertinent mainly or entirely to electrons. These

include the radiative stopping power due to the emission of bremsstrahlung , and the

information on electron collision stopping power at energies below 10 keV where the

Bethe theory is no longer fully applicable. (c) In Section 12, electron stoppingpower tables are presented for 25 elements and 46 compounds and mixtures, covering

the energy region from 10 keV to 1000 MeV. These tables also include the range

(rectified pathlength) and the radiation yield (fraction of electron kinetic energy

converted to bremsstrahlung as the electrons slow down to rest) , both computed in

the continuous -slowing-down approximation. 2 Such data are also given for positrons

in a few materials.

1.2. Background . For electrons it is customary to separate the total stopping

power into two components: (a) the collision stopping power , which is the average

energy loss per unit pathlength due to inelastic Coulomb collisions with bound

atomic electrons of the medium resulting in ionization and excitation; (b) the

radiative stopping power , which is the average energy loss per unit pathlength due

to the emission of bremsstrahlung in the electric field of the atomic nucleus and of

the atomic electrons. 3 The separation of the electron stopping power into two

‘components is useful for two reasons. First, the methods used for the evaluation of

the two components are quite different. Second, the energy going into the ionization

and excitation of atoms is absorbed in the medium rather close to the electron

track, whereas most of the energy lost in the form of bremsstrahlung travels far

from the track before being absorbed. This distinction is important when attention

l The results obtained will be applied to the tabulation of stopping powers for

heavy charged particles in a future report.

2 In this approximation, energy-loss fluctuations are disregarded, and the rate of

energy loss at any point along the track is assumed to be equal to the stopping power.

3 The nomenclature "collision stopping power" and "radiative stopping power" is that

adopted by the International Commission on Radiation Units and Measurements (ICRU,

1980) . In the literature, the collision stopping power is often referred to as stopping

power, with the adjective "collision" omitted, especially in circumstances where

the radiative stopping power is negligible. The collision stopping power is some- times also called "ionization loss." Numerically, but not conceptually, the

collision stopping power is identical with the "linear energy transfer" (more

precisely, the unrestricted linear energy transfer LET ) often used in radiobiologv

(see, e.g. , ICRU, 1970) . The excitations contributing to the collision stopping power include not only

electronic excitations but also vibrational and rotational excitations of molecules;

however, the latter two processes are relatively unimportant above the threshold

energy for electronic excitation. Charged particles also lose some energy in

elastic collisions with atoms. The transfer of recoil energy to atoms in such

events is proportional to the ratio of the mass of the incident particle to the mass

of the atom'. This mode of energy loss is therefore unimportant for electrons except

at extremely low energies where the cross sections for electronic, vibrational, and

rotational energy losses become very small. For incident heavy particles, however,

elastic collisions with atoms constitute a significant mode of energy loss, and give

rise to a so-called "nuclear stopping power" which will be discussed in a future

report on heavy charged particles.

1
is focussed on the energy "imparted locally" to the medium along the track rather

than on the energy lost by the incident electron. Actually, even a part of the

energy lost in ionizing collisions is converted to kinetic energy of secondary

electrons, and is thus carried some distance away from the primary electron track.

In order to estimate energy imparted locally in a crude but simple manner, it is

therefore useful to introduce a restricted collision stopping power defined as the

average energy loss per unit pathlength due to excitation events and due to ionization events in which the energy transferred to secondary electrons is smaller than

some chosen limit. Some data on restricted stopping powers are also given in this

report

.

Even though electron stopping powers and ranges are widely used, they are rarely

measured and must be obtained from stopping-power theory. All previous tables as well as the tables in this report contain collision stopping powers for electrons at energies above 10 keV evaluated according to the theory of Bethe (1930, 1932, 1933).

The energy of 10 keV is a commonly accepted lower limit for the applicability of

the theory. The principal non-trivial quantity describing the properties of the

medium in Bethe ' s stopping-power formula is the mean excitation energy , which is a logarithmic average of the excitation energies of the medium weighted by the

corresponding oscillator strengths. Except for elements with very low atomic number

Z, the mean excitation energies in eV are approximately equal to 10 • Z. Accurate

ab initio calculations of mean excitation energies are possible at present only for

simple atomic gases. For most materials it is necessary to determine mean excitation

energies from experimental data. Another important quantity in the stopping-power

formula, not contained in Bethe 's original theory, is the density-effect correction,

which takes into account the reduction of the collision stopping power due to the

polarization of the medium by relativistic charged particles (Fermi, 1940). All of

the tabulations including the present one have relied on the method of Sternheimer

(1952) for the evaluation of the density-effect correction.

The first extensive electron stopping-power and range tables were calculated by

Nelms, first without and later with the density-effect correction (Nelms, 1956,

1958). The tables of Berger and Seltzer (1964, 1966) included not only the collision

stopping power but also the radiative stopping power. The latter was evaluated by a combination of bremsstrahlung cross sections given by Bethe and Heitler (1934) and

empirical corrections recommended by Koch and Motz (1959). Pages at at. (1972) in

their tables used the same mean excitation energies and bremsstrahlung cross sections

as those of Berger and Seltzer, but evaluated the density-effect correction with

somewhat different input parameters.

1.3. New features . The principal new aspects of this work are the following:

(a) A careful review has been made of the mean excitation energies derived from

the analysis of stopping-power and range measurements, and from semi-empirical dipole

oscillator-strength distributions for gases or dielectric -response functions for

liquids and solids.

(b) In the extraction of mean excitation energies from measured stopping

powers and ranges, use has been made of empirical shell corrections recently developed by Bichsel (unpublished) as an extension of his earlier work (Bichsel, 1961,

1965, 1972).

(c) For compounds for which no direct experimental information is available,

the mean excitation energies have been calculated as weighted sums of the mean excitation energies of the atomic constituents (Bragg additivity) . The required mean excitation energies of the constituents have been adjusted to take into account, at least approximately, the effects of chemical binding and the physical state of

aggregation

.

(d) The Main Tables indicate the sensitivity of the electron collision stopping

power, range, and bremsstrahlung yield to a change of the mean excitation energy.

This enables the reader to make the appropriate adjustments if he prefers values of

the mean excitation energy different from those adopted in this report.

(e) The density-e

dispersion model of Ste

results or the universa

evaluated the density e this report and values

(1975) .

ffect correction has been re-evaluated according

rnheimer (1952). Rather than using Sternheimer '

s

1 fit given by Sternheimer and Peierls (1971), we ffect using as input the mean excitation energies

of the binding energies for atomic subshells from

to the

earlier

have

adopted

Carlson

in

?
(f) The radiative stopping power for electrons has been calculated with

improved theoretical bremsstrahlung cross sections. For bremsstrahlung in the field

of the atomic nucleus, cross sections were obtained as follows: (i) At energies up

to 2 MeV, recent theoretical results were used that are based on the solution of the

Dirac equation and numerical evaluation of the pertinent matrix elements (Tseng and

Pratt, 1971; Pratt et al . , 1977). (ii) Above 50 MeV, use was made of cross sections

in the high-energy approximation (Davies, Bethe, and Maximon, 1954; Olsen, 1955),

evaluated with improved form-factor screening corrections derived from Hartree-Fock

wave functions. ( i i i ) In the energy region from 2 to 50 MeV, it has been found

possible to construct reliable cross sections by interpolating with respect to electron energy, using the accurate low- and high-energy theoretical results as anchor points. The less important process of electron bremsstrahlung in the field

of the atomic electrons was taken into account according to the theory of Haug (1975)

augmented by a screening correction. The radiative stopping power for positrons has

been evaluated on the basis of recent theoretical results of Feng et al . (1981),

extended to all cases of interest by an interpolation-extrapolation procedure.

2.1. General formulas . In this section various formulas of the Bethe theory

and its elaborations will be stated briefly without derivation. For a detailed

discussion of stopping-power theory the reader is referred to the many excellent

reviews in the literature, s.g., Bohr (1948), Bethe and Ashkin (1953), Uehling (1954),

Fano (1963), Inokuti (1971), Jackson (1975), Sigmund (1975), and Ahlen (1980).

The linear collision stopping power , with dimensions of energy/length , will be

denoted as 1 CdE/dx) or S co p. We shall find it convenient to consider also the

corresponding mass collision stopping power , S co q/p, where p is the density of

the medium. The change from linear to mass stopping power largely removes the

dependence on the density, except for a residual dependence due to the density-effect

correction. With S co j in MeV/ cm and p in g/ cm

3

, S co p/p has units of

MeV/ (g/cm 2

)

.

The collision stopping power is due to energy transfers from the incident

particle to bound atomic electrons. We denote by da/dW the cross section (per

atomic electron) for inelastic collisions resulting in an energy transfer of

magnitude W. The mass collision stopping power can then be expressed as

The leading factor, N a Z/A, represents the number of atomic electrons per gram of

the medium. N a

= 6.022045 x 10 2 3 mol 1 is Avogadro's number, and Z and A are

the atomic number and atomic weight.

Following the formulation of Uehling (1954), we now discuss the results of

Bethe' s evaluation of the stopping-powr er expression (2.1). These results are applicable to electrons and positrons, mesons, protons, alpha particles and to fullystripped heavy ions. The energy transfers W to atomic electrons in inelastic

collisions are divided into two classes, depending on whether they are smaller or larger than some value W<. which must satisfy two conditions: (a) Wc must be

large compared to the binding energies of the atomic electrons of the stopping

medium. (b) The impact parameters associated with energy losses smaller than W,~ must be large compared to atomic dimensions. The mass collision stopping power is

expressed as the sum of two components,

2. FORMULAS FOR THE COLLISION STOPPING POWER

N

( 2 . 1 )

- S . p col - S , (W < W ) + - S (W > W ) p cox c

J p col^ C

J ( 2 . 2 )

The main result of the Bethe theory, applicable to electrons and hea\ry charged

particles, is that

2mc 2

3

2 W

c

(i - mi-

- S . (W < W ) p col v c

J 3

z 8 (2.3)
where Na is Avogadro's number, r e is the classical electron radius, me 2 is the

electron rest energy, 3 is the velocity of the incident particle [projectile)

divided by the velocity of light, z is the projectile charge in units of the charge

of the electron, Z and A are the atomic number and atomic weight of the target

atoms, and I is the mean excitation energy. Note that (Particle Data Group, 1980)

2ttN a

2 ? r me"

e

c

2

tt) (6.022045 x 10

2jmol

_1

) (7.940775 x 10~ 26 cm

2

) (0.5110034 MeV)

0.153536 MeV cm

2 mol' 1

Equation (2.3) is valid when the velocity of the projectile is large compared to the

velocities of the atomic electrons. Applied to the electrons in the K shell this

implies the requirement that (Z/137B) « 1. The stopping-power component due to close collisions is evaluated as if the atomic electrons were free and at rest:

(W > w

c

) N

a

ZA

da

dw dW (2.4)

where da/dW is now the differential cross section for energy transfer W in a collision with a free electron, and where

W = 2t(t + 2)mc 2 /[l + 2 (t + 1) (m/M) + (m/M)"] (2.5)

is the largest possible energy transfer, with x- the kinetic energy of the

projectile in units of its rest mass, and m/M the ratio of the electron mass to that of the projectile.

2.2. Stopping-power formula for heavy charged particles . Formulas for heavy

charged particles are given here because they are needed for the analysis of experimental data to obtain mean excitation energies. When m « M Eq (2.5) can be

approximated by

2 2

7 2mc 3 W = 2t(t + 2) mc^ = — (2.6) m 1-3“

The differential scattering cross section is (Uehling, 1954; Fano, 1963)

2 ?

2 rr r" me" ? dW ? da = ^ z“ -yd - 3

Z W/W ) . (2.7)

3 W

Combining Eqs (2.2) to (2.7), one obtains the result

1

P col

2 2 4 tt N r me"

a e

2 2 2 me 3

"

(1 - 3

2

) I 0 ( 2 . 8 )

As expected for a consistent treatment, the quantity Wc which separates hard and

soft collisions does not appear explicitly in Eq (2.8).

The accuracy of the stopping-power formula is improved by the addition of the

following corrections:

4
(1) A shell correction

,

4 which compensates for the fact that the projectile

velocity is not necessarily large compared to the velocity of the target electrons;

(2) A density-effect correction which accounts for the reduction of the stopping power due to the polarization of the medium; and

(3) Corrections which represent departures from the first Born approximation.

Following Lindhard (1976), Andersen et al

.

(1977) and Ritchie and Brandt (1978),

the collision stopping-power formula is written as

4ir N r“ mc“

a e I

z“L(3) (2.9)

where L (3) , the stopping number per atomic electron, is expressed as the sum of

three terms,

L (3) = L

q + zL

1 + z

2 L

2

. (2.10)

The first term,

B

2 - *nl - §

- j , (2.11)

adds to Eq (2.8) a shell correction, C/Z, and a density-effect correction 6/2.

These corrections will be discussed further in Sections 3.2 and 6, respectively.

The second and third terms in Eq (2.10) extend the treatment beyond the first

Born approximation. The term zLi is often referred to as the "z 3 correction."

Because of the appearance of an odd power of z, the stopping power for particles

with positive and negative charge will differ, and this was in fact first observed by

Barkas et al. (1956). For this reason, following Lindhard (1976), we shall refer to the zLi term as the Barkas correction . It was first calculated by Ashley, Ritchie,

and Brandt (1972, 1973] in a semi-classical approximation, using a harmonicoscillator model and assuming that only distant collisions contribute to the effect.

The assumed minimum impact parameter (approximately equal to the orbital radius of

the atomic electrons) is not precisely specified by the theory, and its value must be

adjusted on the basis of experimental stopping-power data. Other derivations of the

Barkas correction have been given by Jackson and McCarthy (1972) who used a somewhat

different quantum-mechanical cut-off parameter, by Hill and Merzbacher (1974) who

carried out a quantum-mechanical perturbation calculation for distant collisions, and

by Lindhard (1976) on the basis of his free-electron-gas model. These theories lead

to results essentially equivalent to those of Ashley, Ritchie, and Brandt, especially

in view of the adjustable value of the minimum impact parameter. We shall in this

report use the theoretical results of Ashley et al., as given by them in terms of a numerical function F which is defined such that

2mc2 B

2 \

7/

zL

1 F (ba/Z/6) ( 2 . 12 )

where a = 1/137.03604 is the fine - structure constant. The multiplier b in the

argument of F is related to the choice of the minimum impact parameter, and

usually has a value between 1 and 2 (see, e.g. , Table 3.4).

'‘The name "shell correction" arose because the correction was calculated separately

for interactions with atomic electrons in different shells, starting with the

treatment of K-shell electrons by Livingston and Bethe (1937).

5
The correction term z

2 L 2 in Eq (2.10) is contained in an extension of Bethe's

stopping-power formula due to Bloch (1933), and will therefore be called the Bloch

correction . Bloch's formula is based on a quantum-mechanical impact-parameter method

that takes into account, approximately, the perturbation of the wave functions of the

atomic electrons due to the incident particle. The correction has the form

z

2 L

2 = i|;(l) - Re i|j( 1 + iy) , (2.13)

where y

= za/3 and where is the logarithmic derivative of the gamma function.

Using properties of this function (see, e.g., p. 259 in Abramowitz and Stegun, 1964) one can transform Eq (2.13) into

z 2 y

oo E

n=l

[n(n 2 + y

L

)

]

1 (2.14)

For very small y, the Bloch correction is negligible. For y » 1, the value

of z

2 L 2 can be shown to approach - 0.577 - An y. When this asymptotic value is

added to the stopping number (square brackets in Eq (2.8)), the resulting stopping

formula is the same as the classical formula of Bohr (1913)

.

2.3. Stopping-power formulas for electrons and positrons . For electrons, large

energy transfers to atomic electrons (considered as free) are governed by the Miller

(1932) cross section,

da

2 tt r

2 me

1

" dW

e

1 + (T-W) 2 (x+1) 2

(2x+l)

(x + 1)

2 W

mvj (2.15)

where x = T/mc 2 is the kinetic energy of the incident electron in units of its rest mass. The Miller cross section, valid when 137B » 1, takes into account relativity

and spin effects as well as exchange effects associated with the indistinguishability

of the incident and target electrons. By convention, the collision stopping-power

pertains to the faster of the two electrons emerging from the collision. The maximum

possible energy transfer Wm , while equal to T according to Eq (2.5), is therefore

taken to be equal to T/2. With the M011er cross section, and using Eqs (2.1),

(2.2), and (2.4), one obtains the following formulas for the electron mass collision

stopping power (Rohrlich and Carlson, 1953; Uehling, 1954):

xt 2 2

z 7T N r me _ i

S col

= l

[*n(T/I) 2 + And + x/2) + F'(x) - 6] , (2.16)

where

F'(x) = (1-g 2

) [1 + x

2 / 8 - (2x+l) A n 2] . (2.17)

One half times the quantity in square brackets in Eq (2.16) is the stopping number

per atomic electron, L(B), and is analogous to the stopping number L(3) for

protons in Eq (2. 9). 5 For positrons, energy transfers larger than Wc are treated

by the Bhabha (1936) cross section (given by Eq (10) in Uehling, 1954). There are no exchange effects, and the maximum possible energy transfer is Wra = T. The mass collision stopping-power formula for positrons is similar to that for electrons,

except that F" is replaced by

s The factor 1/2 arises because it is conventional to use 2xr for electrons and 4 tt for heavy charged particles in the leading factor of the stopping-power formula.

6
F

+ (t) = 2% 2 - (B

2 /12) [23 + 14/(x+2) + 10/(x+2) 2 + 4/(x+2) 3

] (2.18)

Some remarks are necessary regarding the absence of shell corrections from the

electron stopping-power formula, Eq (2.16). For heavy particles, such corrections

have been developed on the basis of the assumption that the projectile particle can

be considered equivalent to a perturbing potential whose center moves with constant

velocity. This assumption, while satisfied for protons down to rather low velocities,

is much less applicable to electrons, so that there is no sound theoretical basis for

extending the available shell -correction theory to electrons.

Corrections to the Bethe theory, analogous to shell corrections for stopping

power, have been discussed by Inokuti (1971) in regard to excitation cross sections.

He indicates that these corrections contain an additive term proportional to the

ratio of electron to projectile mass, m/M, such that the corrections can be

expected to be significantly larger for electrons than for protons. It seems likely

that this will also be the case for stopping-power shell corrections.

We have attempted to make a rough estimate of the possible error in the calculated electron stopping power due to the omission of a shell correction term,

assuming, arbitrarily, that the error is twice as large as the reduction of the

proton stopping power for protons with the same velocity. At an electron energy of

100 keV, the error is then estimated to be ~ 0.3% for H 2 0, ~ 0.7% for A&, ~ 1.3%

for Cu, ~ 2% for Ag, and ~ 3% for Au. At 10 keV, the corresponding error estimates

are ~ 2% for H 2 0, ~ 4% for A&, ~ 9% for Cu, ~ 12% for Ag , and ~ 21% for Au. The

use of Eq (2.16) is questionable at energies below 10 keV. However, for low-Z

materials such as water, air, or plastics, the evidence presented later in Section 8 suggests that the errors may amount to ~ 3% at 5 keV, ~ 71 at 2 keV, and 10 to 15%

at 1 keV.

3. METHODS FOR ESTIMATING MEAN EXCITATION ENERGIES

In order to obtain accurate values of the mean excitation energy I, it is

necessary to take into account the specific electronic structure of the atom, molecule,

or solid of interest. Accurate ab initio calculations of I are available for some atomic gases. For other materials one must rely on semi -empirical methods for

determining I, using data available from two sources: stopping-power and range

measurements, usually for protons and alpha particles; and dielectric-response

functions (for solids) and oscillator- strength distributions (for gases), which can often be obtained from cross sections for the interaction of photons with the medium

of interest.

Only moderate accuracy of the mean excitation energy is required for the determination of the electron collision stopping power. Let A S co j be the uncertainty of

S co l corresponding to an uncertainty AI of I. From Eq (2.16) it can be seen that

at low energies, where the density-effect correction is negligible,

A S c pl/Scol = '

( A VI)/L, where the stopping number L ranges in value from > 3 at

10 keV to ~ 15 at 1000 MeV. At high energies the I-dependence of the density-effect

correction is such as to reduce the I-dependence of the collision stopping power

further; in fact, in the limit of extremely high energies the collision stopping

power becomes independent of I (see Section 6). Figure 3.1 gives the ratio of

logarithmic derivatives - (dS CO ]_/S CO ]_)/ (dl/I) as a function of electron kinetic

energy, for a few materials. The value of this ratio decreases with increasing

electron energy. The bends in the curves for water at ~ 0.5 MeV, and for air at ~ 25 MeV, are due to the sudden onset of the density-effeet correction for non- conducting media.

3.1. Use of oscillator-strength and dielectric data . The use of such data is

growing in importance ; they are becoming more plentiful and allow the determination

of I-values as accurately as from the best stopping-power measurements. The accuracy

results in part from the fact that the oscillator-strength distributions are subject

to various sum rules which act as constraints in the evaluation of experimental data

and provide connections to other measurable physical quantities. The theory underlying the use of oscillator- strength and dielectric data has been reviewed by Fano

(1963) and Inokuti and Turner (1978).

For gases, the mean excitation energy can be obtained from the expression

7
oo An I l a£ M dE/l re

dE - (3.1)

where df/dE is the density of optical dipole oscillator strength per unit energy of

excitation above the ground state.

A variety of methods has been used to evaluate Eq (3.1). For a dilute gas of

free atoms, systematic calculations of oscillator- strength distributions and I -values,

based on the use of Hartree-Slater central potentials and a single-electron model,

have been carried out by Dehmer et al. (1975) for atomic numbers Z up to 18, and

have been continued by Inokuti et al. (1981) for Z up to 38. Critical evaluations

of experimental oscillator- strength distributions for atomic and molecular gases,

based on the use of photo-electric cross sections and inelastic electron scattering

cross sections, have been obtained by various authors, for example, Zeiss et al.

(1975; 1977a, b; 1980). Another semi -empirical method, denoted here as M(n) fit,

makes use of the moments M(n) = df/dE E ndE of the oscillator-strength distribution (Dalgarno, 1960). Noting that dE n /dn = En ^nE, one can transform Eq (3.1) into

An I (3.2)

According to the Thomas-Kuhn sum rule, M(0) = Z. The moments M(2) , M(l), and

M(-l) are calculated theoretically, and M(-2) is obtained from experimental polarizability data. By fitting these moments, an analytical function M(n) is obtained

which is then differentiated to get An I. I-values for 9 gases, obtained according to Eq (3.1) by .various theoretical and

semi-empirical methods, are given in Table 3.1, which is an adaptation and slight

extension of Table V in Dehmer et al

.

(1975). The most accurate I-values are those

derived with the use of semi-empirical oscillator-strength distributions.

The values of the ratio I/Z obtained in the systematic calculations of

Dehmer et al. (1975) and Inokuti et al

.

(1981) show a periodic variation with Z, which is interpreted as due to atomic shell structure. Quite similar variations are found when I-values are calculated on the basis of the local-plasma approximation of

Lindhard and Scharff (1953). According to this model the mean excitation energy is

obtained from the equation

OO An I = (1/Z)/ 4ir r

“ n

0

( r ) ^ n (Y f> ) dr , (3.3)

*o where

u> = (4 tt e“ n (r)/m)^

o o (3.4)

is the plasma frequency corresponding to a electron density n

Q (r) at a distance r from the nucleus, h is Planck's constant divided by 2 tt

,

ana y is a free parameter

for which the value /2 is recommended. As pointed out by Dehmer et al

.

(1975), the use of Eqs (3.3) and (3.4) is equivalent to assuming an approximate oscillatorstrength distribution

= <3 (E - y h u> 0 (r))> (3.5)

where the brackets denote the ground state expectation value and <5 is a delta

function. Expression (3.3) was evaluated by Bichsel and Laulainer (1971), by Chu and

Powers (1972), and by Ziegler (1980), with electron density distributions derived

from Hartree-Slater wave functions. Ziegler has also extended the calculations to solids, using solid-state wave functions.

8
Figure 3.2 shows the irregular Z-dependence of I/Z as calculated by Dehmer

et al . , and by Inokuti et al . , from theoretical oscillator - strength distributions,

and by Chu and Powers and by Ziegler according to the local-plasma approximation. In order to make the two types of results comparable, the local-plasma results are given

for y

= 1. As will be shown later in Section 4, the Z-dependence of the experimental I/Z ratios has similar irregularities. Moreover, the calculated and

experimental I/Z ratios can be brought into rather good agreement with y ~ 1.3.

The use of optical dipole oscillator-strength distributions is justified only

for dilute gases for which there is only a weak correlation between the positions of

the electrons in the medium. For condensed materials the mean excitation energy can

be obtained from an alternative equation, in terms of the dielectric -response

function e (ua) of the medium (Fano, 1956 , 1963):

Jin I dw uj Im[- 1/e (m) 1 &n m) (3.6)

where is

where n is

the electron.

the plasma frequency. The corresponding plasma energy 6 is

ho, = (4 tt h

2 e2 n /m)^ = 28 . 816 (pZ/A) ^ eV , (3.7)

P e

the total number of electrons per unit volume, and e is the charge of

The dielectric-response function is complex-valued; for non-magnetic materials,

its real and imaginary parts, e i (w) and e 2 (dj), can be expressed in terms of the

real and imaginary parts, n(w) and <(m), of the refractive index:

e^(o)) = n"(w) - K^(oj)

e

2 (w) = 2n (u>) k (m)

(3.8)

It is therefore possible to obtain e (oj) from optical data, and just as in the case

of oscillator-strength distributions there are sum rules which serve as consistency

checks for experimental data.

The dielectric-response function for aluminum has been evaluated by Shiles

et al. (1980) by a dispersion analysis involving the use of the reflectance, ellipsometric and transmission optical data from many experiments, and also the use of

electron energy-loss data. These authors obtained an I-value of 165.7 ± 1.0 eV for

aluminum. Mean excitation energies for various compounds, obtained in a similar manner (but usually with less abundant optical data) will be discussed in Section 5. 3.2. Use of stopping-power and range data . There is an abundant experimental

literature on stopping powers and ranges for protons and alpha particles (see, e.g.,

Andersen and Ziegler, 1977; Ziegler, 1977; .Andersen, 1977). The extraction of mean excitation energies from such data would be a routine matter if it were not for the

fact that the stopping-power theory contains correction terms which are not always

known with the accuracy desirable. From measured stopping-power data, the mean excitation energy can be determined by inverting Eq (2.9):

Jin I = (3.9)

6 The plasma energy specified in terms of Eq (3.7) is a nominal value calculated with

the electron density for all atomic electrons. It is larger than the plasma energy

used to describe collective excitations (plasmons) which is calculated with the

density of participating electrons.

9
where

z “L

2 (3.10)

is the total correction, combining the shell correction, density-effect correction,

Barkas correction, and Bloch correction.

Let AS co i denote the uncertainty of the measured value of S co q, and let Ax

denote the uncertainty of the correction term x. Assuming that the two uncertainties

can be combined quadratically , the overall uncertainty of the estimated I-value is

where LeXp is the experimental stopping number (last term in Eq (3.9)). When

range data are used to determine I-values, the error analysis is more complicated,

and must take into account the uncertainty of the experimental range value as well as the uncertainties of the correction term x at all energies up to the initial

projectile energy.

In the evaluation of the correction x we have followed a procedure suggested

by H. Bichsel, earlier versions of which have been described by Bichsel (1961, 1963,

1972). Included in the procedure are the evaluation of the Barkas correction

according to Ashley, Ritchie, and Brandt (1972,1973), the Bloch correction according

to Eq (2.14), and the shell correction by the method outlined below.

3.2.1. Bichsel's shell corrections . The total shell correction C is the sum of the contributions C^, Cp , TT7 from the different atomic shells. Theoretical

values calculated with hydrogenic wave functions are available for Ck (Walske, 1952;

Khandelwal, 1968), for Cl (Walske, 1956; Bichsel, 1967; Khandelwal, 1968), and for

Cjq (Khandelwal and Merzbacher, 1966). The error due to the use of hydrogenic wave

functions is expected to be relatively minor for the K shell, more serious for the

L shell (particularly for atomic numbers Z < 30) and probably even greater for the

M shell.

Extension of the calculations to higher shells, with use of improved wave functions, is possible but would be very laborious. Bichsel instead adopts a semiempirical scaling procedure with parameters that are determined by experimental

stopping-power data. He assumes that the dependence of on the particle velocity

is similar to that of Cp, except for scale factors, and also extends this assumption

to the higher shells. The Walske result for the L shell, Cp(0p,i?p), depends on the atomic number through the parameter 9 l and on the particle energy through the

quantity

where Z = Z - 4.15 is the effective nuclear charge for the L shell. The M-shell

correction is calculated from the scaling relation

where V„ is equal to 1/8 times the number of electrons in the M shell, and where

Hv, is an adjustable parameter. Analogous scaling relations are used for the

N

1 shell and for a combined 0-P shell.

7 For Z < 10, Eq (3.13) is also applied to the incompletely filled L shell, with

Vl as defined above and Hp = 1 . For low atomic numbers, the effective charge

for the L shell has in this work been set equal to Z - d, with values of d

taken from Clement! and Raimondi (1963).

(3.11)

t? l

= (B/aZ )

2 (3.12)

(3.13)

For Z = 3 d = 1.72

4

2 . 09

5 2.486 2.82

7 3.16

8 3.53

9 3.84

10

4.24

10
The scaling parameters Hn (for n = M, N, and 0-P), the parameter b of

the Ashley-Ritchie-Brandt theory for the Barkas correction, and the mean excitation

I were determined by Bichsel in a two-stage procedure. First he chose values of I, b, and the Hn

's by trial and error for a small number of key elements so as to obtain the best possible agreement between calculated and measured stopping powers

and ranges for protons and alpha particles, taking into account all available data.

The parameters thus chosen for C, A£, Cu, Ag, and Au are given in Table 3.2.

They are of course not unique, but provide a good fit to the data. Table 3.3 gives

illustrative values, for the same elements, of the shell corrections, Barkas

corrections, Bloch corrections, and the stopping number per electron. The relative

contributions of the various corrections to the proton stopping number for gold are indicated in Fig. 3.3 where it can be seen that at energies above 500 MeV the densityeffect correction is more important than the shell correction.

The second stage of Bichsel 's procedure consists of interpolating the parameters

Hnvs. Z, to obtain values for all elements. His interpolation scheme is given in

Table 3.4 which also lists recommended b-values for all elements. The shell

corrections thus obtained exhibit small irregularities as functions of Z, especially

at low proton energies. Before being used in the present work they were smoothed

graphically. The smoothed shell corrections of Bichsel, plotted vs. Z, are shown

in Fig. 3.4 for various proton energies from 2 MeV to 100 MeV. Bichsel ' s shell

corrections as functions of the proton energy are given in Fig. 3.5 for various

elements

.

3.2.2. Comparison of Bichsel 's and Bonderup's shell correction . Theoretical

shell corrections have been derived by Bonderup (1967) on the basis of the statistical

gas model of Lindhard and Scharff (1953) and Lindhard and Winther (1964). The

theoretical shell corrections, plotted against atomic number, are shown in Fig. 3.4

and can be seen to agree rather well with Bichsel' s empirical shell corrections for

atomic numbers Z up to ~ 50. With increasing Z the Bonderup corrections

continue to increase whereas those of Bichsel reach a peak and then decrease. 8 To investigate the influence of the adopted shell corrections we now consider

the high-energy proton range measurements of Barkas and von Friesen (1961) and the

low- and intermediate-energy stopping-power measurements of Burkig and Mackenzie

(1957), Sorensen and Andersen (1973) and Ishiwari et al

.

(1979) for the elements Cu,

Pb, and U. The proton energy in the Barkas-von Friesen experiment had the nominal value of

750 MeV but was uncertain by one or two MeV. Using the measured proton range value

of 273.29 g/cm 2 in aluminum, and using the accurate value = 166 eV from

Shiles et al. (1980), one estimates the beam energy to have been 749.0 MeV. With

this energy one obtains the I-values shown in Table 3.5, which are estimated to have

an uncertainty of ~ 10 eV. The use of Bonderup's rather then Bichsel's shell

corrections would lower the I-values for Pb and U by a few eV but leave that for

Cu unchanged. It is interesting to note that the omission of the density-effect

correction would have a much greater influence on I than the change of shell

corrections

.

Table 3.6 compares I-values deduced from medium-energy as well as high-energy

experiments. It can be seen that for copper the same I-value is obtained (within the

estimated uncertainties) regardless of the type of shell correction that is used.

For lead and uranium, however, the use of the Bonderup shell correction leads tc estimated I-values for lead and uranium that are ~ 10 percent lower for the mediumenergy experiments than for the high-energy experiment. With Bichsel's shell

corrections, approximately the same I-value is obtained regardless of energy.

Inasmuch as the mean excitation energy is a material constant independent of the

projectile energy, we have adopted Bichsel's shell corrections as providing the

better representation of the experimental situation. 9

a A similar turning over of the curve of shell correction vs. atomic number is also

characteristic of the empirical shell corrections given by Andersen and Ziegler

(1977) which lie between the Bonderup and Bichsel shell corrections.

9 It may be noted that Andersen and Nielsen (1981) also find that the Bonderup shell

correction for protons in gold at energies from 2 to 7 MeV is larger than the

empirical shell correction which they deduce from their stopping-power measurements.

These authors suggest that the discrepancy may be due to the non-relativistic

treatment of inner-shell electrons in Bonderup's theory.

11
4. SELECTION OF MEAN EXCITATION ENERGIES FOR ELEMENTS

Using Eq (3.9) with shell corrections from Bichsel, the Barkas correction

according to Ashley, Ritchie, and Brandt, and the Bloch correction, we have extracted

I-values for a large number of elements from 22 experiments. The data are mainly for

protons with energies > 5 MeV, so that the value of the correction term

x = C/Z + 6/2 - zLi - z^L 2 is in general small compared to the stopping number (see

Table 3.3). The measurements that were analyzed are listed in Table 4.1. The

deduced I-values and their uncertainties are given in Table 4.2. The overall

uncertainties have been calculated according to Eq (3.11), combining quadratically

(a) the experimental uncertainties, and (b) an assumed 10-percent uncertainty of the

correction term x. Several of the experiments listed in Table 4.1 provide stopping-power ratios

relative to a reference material. Burkig and Mackenzie (1957) and Nakano et at. (1963) measured stopping-power ratios relative to aluminum. We have interpreted

these by assuming the stopping-power for aluminum to be that calculated with an I-value of 166 eV as obtained by Shiles et at. (1980) from dielectric data. The

experiments of Bakker and Segrb (1951) and of Thompson (1952) give stopping-power

ratios with respect to copper, which we have analyzed assuming an I-value of 322 eV

for copper consistent with various other experimental results. The experiment of

Nordin and Henkelman (1979) gives stopping-power ratios relative to liquid water,

which have been analyzed assuming for water an I-value of 75 eV derived by Ritchie

et at. (1978) and Ashley (1982a) from dielectric data. The measurement uncertainties

entered into Eq (3.11) have been augmented to include the uncertainties of the

calculated stopping powers of the reference materials.

The experimental results of Thompson were also analyzed relative to water

instead of copper, and those of Nordin and Henkelman relative to aluminum instead of

water. This changed the deduced I-values by only a fraction of one percent, and an average of the values with the two reference materials was taken. The I-values from

the experiment of Bakker and Segrb , when analyzed with respect to aluminum instead of

copper, changed significantly, and both sets of I-values are given in Table 4.2.

The final choices of mean excitation for elements were made as follows. (a) For

the gases H 2 , He, N 2 , 0 2 , and Ne, the information from semi-empirical dipole

oscillator- strength distributions was judged to be more accurate than that from

stopping-power data, and I-values were selected from those given in Table 3.1.

(b) For aluminum, the value I = 166 eV was used as derived by Shiles et at. from

dielectric data; this value is also supported by the results of several stoppingpower measurements. (c) For other elements, I-values were selected by taking into

account the results from stopping-power and range experiments collected in Table 4.2.

The available information is in most cases good enough to specify I-values accurate

to a few percent.

We have also estimated I-values for elements for which no experimental information is available. Following Andersen and Ziegler (1977) we have done this by

imitating the local Z-dependence as predicted by the results of calculations done in

the local-plasma approximation (see Fig. 3.2). The following interpolation scheme was used. Denoting calculated I-values by I C (Z), experimental values by I ( Z

)

and

interpolated values by Iint(Z), we have assumed that

I- _(Z) int v 1 I(Z ) z

7

- z I(Z

2

) z - z

I (Z) i + 1

c

I (Z, ) z, - Z, I (Z„) z 7

- z. (c v l 2 1 c 2 2 1

(4.1)

where l x and Z 2 are the closest atomic numbers, with experimental I-values, that

bracket the atomic number Z of interest. Either Z, Z x , and Z 2 pertain to gases, in which case the required values of I c are taken from the results of Chu

and Powers (1972) obtained with free-atom wave functions, or Z, Zj, and Z 2 pertain to solids in which case the values of I c are taken from the results of

Ziegler (1980) obtained with solid-state wave functions (the version indicated by

Ziegler as first-order solid with continuous interstitials).

12
The value I = 700 eV listed in Table 3.1 for radon, obtained by Bell and

Dalgarno (1965) by a "M(n) fit" (see Section 3.1), is expected to be inaccurate

because of a numerical error in the moment M(- 1) and because of neglected relativistic effects. The adopted value I = 794 eV was estimated by extrapolating the

ratios I(Z)/I C(Z) for rare gases to Z = 86.

Table 4.3 gives the adopted I-values, and the corresponding ratios I/Z, for

all elements. The estimated uncertainties of the I-A^alues are given only for experimentally-based I-values. These uncertainties are intended to take into account both

the uncertainties of individual experimental results and the scatter of the results

from different experiments. 10 The interpolated I-values are enclosed in parentheses.

To indicate the irregular Z-dependence of the adopted mean excitation energies, a plot of I/Z vs. Z is shown in Fig. 4.1.

As a check on the acceptability of the adopted I-values and correction terms to the stopping-power formula, we demonstrate in Figs. (4.2) to (4.5) that close fits are obtained to a large body of experimental stopping-power data. Comparisons are made in terms of the ratio of the experimental to the calculated stopping power.

Figure 4.2, taken from 3ichsel and Porter (1982), pertains to protons and alpha

particles in N 2 and 0 2 . Figure 4.3 pertains to proton stopping poAver at energies up

to 20 MeV in Ai, Cu, Ag, Au, Pb, and U. Figures 4.4 and 4.5 pertain to the proton

stopping-power measurements of Ishiwari et at. (1979) at 6.5 MeV, and those of Burkig

and Mackenzie (1957) at 19.8 MeV, in many elements.

For a few elements, the I-values adopted in this report are compared in

Table 4.4 with I-values recommended in eleven earlier papers.

The experimental information on I-values for compounds is steadily increasing.

I-values for many gases have been determined by Zeiss et at. (1975, 1977a, b), Thomas

and Meath (1977), and Jhanwar et at. (1981) from semi-empirical dipole oscillatorstrength distributions. For liquid water and for various plastics, I-values have

been obtained by Ritchie et at. (1978), Ashley (1979) and Painter et al

.

(1980) from

dielectric data. I-values for a large nymber of condensed compounds, obtained under

uniform conditions, can be deduced from an experiment by Thompson (1952) who measured

the pathlengths traveled by protons while slowing down from 340 MeV to 200 MeV in

many organic liquids, in water, and in a few solids. Thompson showed that the ratios

of these pathlengths to the pathlength in a reference material (copper) can be

interpreted as reciprocals of the corresponding stopping-power ratios at an intermediate energy. We have re-analyzed Thompson's data, applying small multiplescattering corrections according to a procedure of Bichsel (1978) and shell

corrections for copper, to obtain stopping-power ratios relative to copper at 267.5 MeV.

There are many compounds of interest for which one needs to estimate I-values in

the absence of direct experimental information. It has been known since the early

work of Bragg and Kleeman (1905) that the collision stopping-power of a compound can

be approximated by the weighted sum of the stopping powers of the atomic constituents

of the compound. For the mass collision stopping power S co p/p, the additivity rule

takes the form

where Wj is the fraction by weight of the j ' th atomic constituent. This additivity rule is equivalent to replacing, in the stopping-power formula Eq (2.16), the

quantities Z/A, I, and 6 by

1 °The uncertainties of the I-values in Table 4.3 are figures of merit, arrived at by

subjective judgements, and with a meaning that is not easily defined. One possible

interpretation would be the following. If, in the future, the measurement accuracy

and theoretical analysis are sufficiently improved so that I-values can be determined with an accuracy an order of magnitude better than at present, Ave expect that

for at least 90 percent of the cases in Table 4.3 the future I-values will lie

within the limits of uncertainty given in this report.

5. SELECTION OF MEAN EXCITATION ENERGIES FOR COMPOUNDS

(5.1)

13
(Z/A) = E WjCZ^Aj) , (5.2)

j

£nl = E w. (Z ./A. ) £nl

.

H J J 3 J j

<1/ A>

/

<Z/A> (5.4)

where Zj , A-j , Ij , and 6j pertain to the j

' th constituent. It should be noted

that <Z/A)> is equal to the total number of electrons in the molecule divided by the

molecular weight. The use of <6> calculated from Eq (5.4) is in general not a good

approximation, and it is preferable to calculate the density-effect correction

directly for the compound of interest (see Section 6.3).

The application of this additivity rule requires the choice of appropriate

values for the mean excitation energies of the constituents. The simplest procedure,

often used in the past, is to take the same I-values for the atomic constituents of a compound as for the corresponding elemental substances. This introduces some error because of the neglect of molecular binding effects. An additional error may be

incurred when elemental I-values for gases [e.g., oxygen) are applied to the con- stituents of solid compounds.

The accuracy of the additivity rule can be improved by assigning I-values to the

constituents which are not unique but take on various values depending on the type of

compound and on the physical state of aggregation of the medium. When carried to an extreme this is equivalent to abandoning additivity and treating each compound

separately. However, it is possible to find simple rules for assigning I-values to atomic constituents with which the I-values for a large number of compounds can be

represented satisfactorily. We have adopted such an assignment scheme which is given

in Table 5.1.

A more elaborate assignment scheme was developed earlier by Thompson (1952) who

interpreted his experimental stopping powers for various compounds in terms of the

stopping powers (and I-values) of atomic constituents in various chemical environments. We have extracted I-values from Thompson's stopping powers for atomic

constituents, and have thus obtained the up-dated Thompson assignment scheme given in

Table 5.2. In this scheme, different I-values are assigned to constituents depending

on the type of chemical bond involved. Thompson's conclusions as to the influence of

bond types on the I-values of atomic constituents in organic liquids are quite

plausible. However, the available data base is not sufficient to pin these distinctions down with great precision, and there is a need for further experiments similar

to Thompson's.

Mean excitation energies for organic solids and other compounds have also been

estimated by Brandt (1956, 1958, 1960) on the basis of experimental data and

theoretical considerations. Brandt (1960) used as an initial approximation free-atom

I-values for atomic constituents according to a formula of Jensen (1937), modified

these values to take into account the valence states (aromatic, aliphatic, ...) of

atomic constituents, and then assumed Bragg additivity. Brandt also applied a "lowenergy density-effect" correction which raised the mean excitation energy for the

compound as a whole. His valence- state corrections and density-effect corrections were obtained from theoretical polarization data for atoms and experimental molarrefractivity data for molecular compounds. As will be shown later in the comparison

in Table 5.6, Brandt's theoretical I-values for low-Z compounds are not very

different from those adopted in the present work. However, his I-values for compounds

containing high-Z constituents tend to be too low, a fact already noted by Brandt

with respect to photographic emulsion.

Table 5.3 lists the presently available experimental I-values, and their origin,

for 13 gases, 27 liquids, and 14 solids. The table also gives the differences

between these I-values and corresponding Bragg - additivity I-values obtained with our adopted assignment scheme and that of Thompson. In most cases these differences are smaller than the estimated experimental uncertainties. There are large discrepancies

14
in only two cases, for liquid dichloroethane and for paraffin wax. 11 For gases our assignment scheme works particularly well. For liquids it is slightly inferior to Thompson's scheme, but for solids it is somewhat better.

Thompson's scheme includes more chemical detail than ours but on the whole works

no better and is more complicated to apply. We have therefore used our scheme

(Table 5.1) for the prediction of I-values in the absence of experimental data. For

compounds with the constituents H, C, N, and 0 (and perhaps also F and C£)

such predictions have a sound empirical basis. One would expect that the errors associated with such predictions will have the same order of magnitude as the

differences between experimental and Bragg-additivity I-values in Table 5.3. The

situation is less clear in regard to condensed materials with atomic constituents

other than those listed above. Our assignment scheme uses for these other constituents I-values that are 13 percent larger than the corresponding I-values for

condensed elemental substances as given in Table 4.3. This increase was found to be

required to obtain a good approximation to the rather accurately known experimental

I-values for A£ 2 0 3 , Si0 2 , and photographic emulsion, and is also consistent with

the less certain experimental data for LiF and CaF 2 . In the absence of other

information we have assumed that the 13-percent increase should also be applied to the constituents of other compounds such as sodium iodide and cesium iodide.

Certain composite materials, for example tissue-equivalent gases, pyrex glass,

and human tissues, have constituent molecules whose I-values are known independently

from experiments. In order to take advantage of this information, we have treated

such composite materials via a Bragg rule for the combination of atomic and molecular

constituents. For human tissues, a prominent constituent with a known I -value is

water. In Table 5.4, the water content and I-values for various types of tissue are given.

Table 5.5 lists the adopted mean excitation energies, densities and elemental

compositions for the 46 compounds and mixtures for which electron stopping-power

tables are given in this report. The symbol + indicates I-values derived directly

from experimental data or I-values for mixtures (such as air) all of whose constituents have experimentally determined I-values. The symbol ++ indicates I-values

derived by applying the additivity rule to molecular constituents one or more of

which have experimentally determined I-values. In all other cases, the I-values were obtained from the additivity rule, Eq (5.3), with constituent I-values from Table 5.1

A letter grade (A, B, or C) is given next to each I-value in Table 5.5, to indicate the relative quality of these data. The assignment of these grades was based on the information contained in Table 5.3, but also involved subjective

judgements. For the most part the following guidelines were followed. Direct

experimental I-values were given the grade A unless the experimental uncertainty

was greater than 5 percent, in which case they were given the grade B. I-values for

low-Z gas compounds were given the grade A. I-values for condensed compounds were given the grade B if the constituents consisted predominantly of the elements H,

C, N, 0, F, or C£. The grade C was given to I-values for condensed compounds

which contain mainly other constituents whose I-values were adjusted upward by the

13-percent rule. We would assign an estimated uncertainty 12 of <5 percent with

grade A, 5 to 10 percent with grade B, and 10 to 15 percent with grade C. In order to indicate how the recommended I-values for compounds have changed over the

years, a comparison with previously recommended values is given in Table 5.6.

For electrons, the dependence of the collision stopping power on the state of

aggregation can be expressed completely through the mean excitation energy, provided

the Bethe stopping-power theory (without shell corrections) is applicable. This

dependence is indicated in Table 5.7 for a few elements and compounds. It should be

noted that the values for molecular gases, liquids and solids are empirical, whereas

those for "atomic gases" are from theoretical oscillator-strength distributions.

1 'Because the experimental I-value for paraffin wax is inconsistent with those for

other straight-chain hydrocarbons (n-pentane, n-hexane, n-heptane, and polyethylene

we have adopted the I-value of 55.9 eV, using the Bragg-additivity values according

to Table 5.1. This is the only case in which the Bragg-additivity value was adopted in preference to the experimental value.

1 Concerning the meaning that might be attached to the estimated uncertainties, see footnote 10.

15
6. DENSITY EFFECT

6.1. General equations . The passage of a charged particle through a medium

results in the polarization of atoms in the medium, and this polarization in turn screens the electric field acting on the particle so as to reduce the stopping power.

This reduction is particularly strong in dense media, and is therefore called the

density effect . The greater the particle velocity, the greater is the density effect

because, by virtue of the Lorentz contraction, distant collisions become more important. In fact, at very high energies the density-effect correction to the

stopping power is significant even in dilute gases.

The density effect was first predicted by Swann (1938) and calculated by Fermi

(1940) . The results of such a calculation depend on the model used for representing

the dielectric properties of the medium. Whereas Fermi used only one dispersion

frequency, more realistic models were developed by Wick (1943) , Halpern and Hall

(1948), and Sternheimer (1952). Sternheimer introduced a procedure for making the

dielectric model consistent with the (experimentally known) mean excitation energy

for the medium, which is essential for obtaining accurate results.

As shown by Fano (1956, 1963), the density-effect correction can be expressed as follows in terms of the dielectric - response function e (to) of the medium:

CO

6 = (2/ttoj

2

) f

u du Im [ - 1/e (w) ] £n(l + £

2

/u)

2

)

- (£/w ) 2 (1 - g

2

) , (6.1)

* n ^

where ojp is the plasma frequency, proportional to the square root of the density,

given by*Eq (3.7). The quantity £ is defined, as a function of 8, as the root of

the equation

1 - 6

2

e (i£) = 0 . (6.2)

It can be shown that in the limit 8

-» 1

6 + £n[(haj

p

) 2 /(l - 6

2 )I2 ]

* 1 . (6.3)

When this result is inserted into the stopping-power Eqs (2.9) or (2.16), the mean excitation energy I disappears from the final result. Thus in the limit of very

high energies, the stopping power depends on the properties of the medium only through

the plasma energy hu and therefore only on the density and the ratio Z/A.

In the solution of Eq (6.2), a difference arises between conducting and non- conducting media. For conductors, the dielectric-response function is such that the

equation has a root for any value of 6- The density effect is then present, though

small, even at arbitrarily low energies. For insulators, however, a root exists only

above a minimum value of 8 q = e(o) _3s, which is a property of the material, and

there is no density effect for g < 8 0 . The most accurate method of evaluating the density-effect correction is to use semi-empirical dielectric-response functions in Eqs (6.1) and (6.2). This has

recently been done by Inokuti and Smith (1982) for aluminum, and by Ashley (1982b)

for water. Reliable and complete dielectric-response functions for other materials

are scarce, and in general one must rely on Sternheimer ' s method, which -- although

more approximate -- will be shown below to give results in very good agreement with

those of Inokuti and Smith and of Ashley.

6.2. Sternheimer ' s model . As discussed by Fano (1963), Sternheimer ' s model can

be related to Eqs (6.1) and (6\ 2) as follows. In Eq (6.1) one sets e = 1/ (1 - ot^) , where

a

L

(a)) (hai ) P

N£n= 1 E

"nL

- (hu) - iy T fuo nL

(6.4)

16
is the longitudinal polarizability expressed in terras of the energy levels E n p of

single atoms and the corresponding oscillator strengths fn p. In the limit in which

the damping constant y^ -* 0, the resulting expression for 6 becomes

N

= £

n=l "nL £n [1 - U/w

p

) (i - e ) (6.5)

In Eq (6.2), one sets e = 1 + ap , where ap is the transverse polarizability

and is given by an expression similar to Eq (6.4) but with different energy levels

Enp, oscillator strengths fn p, and damping term yp. In the limit yp -* 0,

Eq (6.2) is then transformed into

a,p (i£) 0%) £ -

p n= 1 t

“nT nT

(h^)'

( 6 . 6 )

The following approximations are now made:

a. The distinction between the longitudinal and transverse oscillator

strengths fnp and fn p is disregarded, and both are approximated by fn , the

fraction of electrons in the n'th atomic shell.

b. The energy levels are assumed to be

E nT

~ y St E n

E . = [pL E

2 + f (hu ) 2

] h

nL L ^St n n

l p' J ’

(6.7)

( 6 . 8 )

where the En's are atomic energy levels. The quantity pg t as the Sternheimer

factor and is given a value such that the equation

N£

n=l

fn £n[y St £n

(ha)p) J = ^1 (6.9)

is satisfied. The dielectric model is then consistent with the mean excitation

energy I (as known from experimental data) , and the density-effect correction <5 calculated according to Eq (6.5) goes into the correct asymptotic limit, Eq (6.3),

for very high particle energies. The values of pgt typically range from 1.5 to 2.5.

For conductors, the electrons in the outermost shell, n = N, are considered to be conduction electrons, and the corresponding binding energy Ejq is set equal to zero. This has the consequence that Eq (6.6) has a solution for arbitrarily small

values of 6. For insulators, on the other hand, Eq (6.6) has a solution only for

velocities greater than 8 0 given by

N£ 7 n= 1 p E^/(hm

p

) Z St

( 6 . 10 )

As a final refinement, which makes

Lorentz-Lorenz correction is applied (St

fn (h

)

2

i- n Eqs (6.8) and (6.9) by X n

A, 1/ 3 in all other cases.

little difference

ernheimer , 1952)

,

fn (hmp) 2

, where

except for liquid H 2 , a through the replacement of

Xjg = 1 for conductors, and

6.3 Numerical evaluation . The evaluation is done by first solving Eq (6.9) for

pg t , then Eq (6.6) for l as" a function of 8, and substituting the value of £ into Eq (6.5). Such calculations using I-values current at the time, were carried

17
out by Sternheimer (1952, 1956, 1966, 1967) and Sternheimer and Peierls (1971) for

many materials. The results were reported in terms of a useful approximation formula

for 6. In the present work we have systematically re-evaluated 6 using the

I-values adopted in the present report and atomic binding energies from Appendix 1 of

Carlson (1975). The number of conduction electrons for metals and semi-conductors

was taken to be equal to the lowest valence number. Compounds have been treated as insulators. For compounds, the sums with respect to n in the various equations were extended to include all atoms in the compound. Departures from simple Bragg

additivity were taken into account by using the appropriate density and mean excitation energy for the compound. We have used the direct numerical output of the

calculations rather than an analytical approximation formula when computing the

stopping-power tables. 13 These values of 6 are listed in the Main Tables.

Values of 6 for a few media, calculated by the method of Sternheimer described

above, are shown in Fig. 6.1. When expressed as functions of the particle kinetic

energy in units of the rest mass, these results are applicable to any charged

particle. Table 6.1 gives illustrative results regarding the percent reduction of

the electron collision stopping power due to the density effect.

Figure 6.2 shows the difference between the 6-value of Inokuti and Smith (1982)

and the corresponding Sternheimer value for aluminum, and Fig. 6.3 shows the

difference between the 6-value of Ashley (1982b) and the corresponding Sternheimer

value for water. In both cases the differences are positive at some energies and

negative at others. For aluminum the absolute value of the difference is always

smaller than ~ 0.04, and for water it is always smaller than ~ 0.09. Figure 6.4

shows the percent amount by which the electron collision stopping power is changed

when the more exact density-effect corrections of Inokuti and Smith or of Ashley are replaced by Sternheimer ' s corrections. It can be seen that the absolute percent

difference is smaller than 0.2 percent for aluminum and smaller than 0.5 percent for

water. The very satisfactory agreement in the cases of aluminum and water gives one confidence that Sternheimer ' s results will be accurate in general. 14

6.4. Complications for inhomogeneous media . The theory for the density effect

is designed for media that are homogeneous and isotropic. In some cases of practical

interest these conditions are not met. An important case is that of graphite, a porous material consisting of somewhat loosely packed graphite crystallites arranged

in a layered structure with a dielectric - response function that is a directiondependent tensor (Raether, 1980). The crystallite density is 2.265 g/cm 3

, whereas

the bulk density may range from 1.5 to 1.9 g/cm 3

, depending on the method by

which the graphite is manufactured. Typical densities for reactor-grade graphite are

1.7 to 1.8 g/cm 3. Th'e porosity structure is complicated (Gmelin, 1968), including

"micropores" ranging in diameter from 2 to 60 nanometers, and "macropores" ranging in

diameter up to 20 micrometers. It is not clear what density value should be used in a simple theory which neglects all these complications. In the stopping-power tables

we give results for densities of 1.7 and 2.265 g/cm 3. At energies above a few

MeV, the use of the higher density would decrease the collision stopping power by more than one percent.

Another case of interest is photographic emulsion. The standard emulsion

considered here consists of low-Z gel (17.4% by weight, average density 1.29 g/cm 3

) and silver halides (82.6% by weight, average density 6.47 g/cm 3 ). Two extreme

approaches can be considered: (a) The density effect can be calculated as if the

emulsion were homogeneous, with the bulk density 3.185 g/cm 3

; this is what was done

to produce the tabulated results. (b) The emulsion can be considered to be inhomogeneous, and the density effect can be calculated separately for the two components,

gel and silver halides, with the proper density for each. The use of method (b)

instead of (a) would lower the collision stopping power by 0.2% at 1 MeV, 0.4% at

10 MeV, 0.8% at 100 MeV and 0.7% at 1000 MeV.

Similar considerations can also be applied to A-150 tissue-equivalent plastic

which consists of an inhomogeneous mixture of polyethylene, nylon, carbon black and

calcium fluoride (Smathers et al . , 1977). In this case the use of method (b) instead

of (a) would lower the collision stopping power by no more than 0.1%.

1

3

Updated parameters for Sternheimer ’ s approximation formula will be given in a forthcoming paper (Sternheimer, Seltzer, and Berger, 1982).

14 The evidence from high-energy charged-particle penetration data also confirms the

accuracy of Sternheimer ' s method (see, e.g., Crispin and Fowler, 1970).

18
7. RESTRICTED COLLISION STOPPING POWER

In radiation dosimetry and in radiobiological modeling (track- structure theory)

one may want to know the fraction of the energy lost by an electron that is absorbed

"locally" in the medium in the vicinity of the electron track. To obtain this

fraction accurately one must carry out transport calculations that take into account

(a) the initial energy spectrum and angular distribution of the secondary electrons

set in motion in ionization events, and (b) the penetration, diffusion and slowing

down of the secondary electrons. A simple, approximate answer can be obtained in

terms of the fraction L (T , A) /Sg 0 ]_ (T) , where L(T,A) is the restricted collision

stopping power . (The symbol L(T,A) used here should not be confused with the

stopping number L discussed in Sections 2 and 3.) This quantity is defined as the mean energy loss per unit pathlength due to collisions involving energy transfers W,

from the incident electron to the medium, that are smaller than some chosen cut-off

A. The kinetic energy of the secondary electrons from ionization events is then also

smaller than A, and the range for an electron of energy A roughly specifies the

region around the track of the incident electron within which energy is absorbed

"locally". The significance of the concept of restricted stopping power, and

possible extensions and generalizations, are discussed in an ICRU report on linear

energy transfer (ICRU, 1970).

An application of restricted collision stopping powers occurs in the Bragg-Gray

theory of cavity ionization as formulated by Spencer and Attix (1955), in which the

cut-off energy A serves to specify the dimension of the cavity. Another application occurs in the Monte Carlo simulation of electron tracks. In such a calculation,

energy-loss straggling can be taken into account approximately, with reduced

computational effort, by limiting random sampling to large energy transfers, which

are rare, and by treating the numerous small energy transfers in the continuousslowing-down approximation with use of a restricted collision stopping power.

In order to obtain an expression for the restricted collision stopping power,

one must replace the maximum energy transfer Wm

in the integral in Eq (2.4) by A. The results for electrons and positrons (indicated by superscripts - and + ) are:

1 + 2u Na

r

e mc2Z 2 £

L-(T,A) = ^

| Un(T/I) Z

+ An(l + x/2) + G"(T,n) - 6]

6 (7.11

Equation (7.1) is similar to Eq (2.16), and the various symbols have the same meaning, except that the functions F^x) are replaced by G

± (T,n). For electrons,

G (x,n) = -l-B

2 + ta[4(l - n)n] + (l - n)

1

+ (1 - B

2 )[x 2 n2 /2 + (2 x + 1) ta(l - n)] (7.2)

where n = A/T is the fractional energy cut-off. For positrons

G

+

(x,r|) = ta 4n - B

2 [l + (2: - u

2

) n - (3 + u

2

) (ux/2) n°

(1 + ut)(u 2 t

2 /3) n

3

- (u

j t3 /4) n

4

] , (7.3)

where u = (x + 2)

1

. We note that G"(x,l/2) - F (t) and that G

+ (x,l) = F'(x),

so that L" (T,T/2) = S‘ ol (T) and L (T,T) = S col (T).

A condition for the validity of Eq (7.1) is that the cut-off energy A be

larger than the binding energies of the atomic electrons in the target material. For

the K- and L-shell electrons of high-Z materials this condition is difficult to satisfy for A-values of practical interest. Tables 7.1 and 7.2 give the ratios of

the restricted to the total collision stopping power for electrons and positrons in seven substances, for cut-off energies A = 100, 10 and 1 keV. The results shown are limited to cases for which A is larger than the L-shell binding energy and at least

19
comparable with the K-shell binding energy. The results for Pb for A = 100 keV,

for Ag and Cu for A = 10 keV, and for Al for A = 1 keV have been included for

completeness, but may be inaccurate.

Excluded from the definition of restricted stopping power used above is the

reduction of the collision stopping power due to the escape of Auger electrons, which

may occur subsequent to inner-shell ionization. For water, graphite, and air, the

results in Tables 7.1 and 7.2 are not affected by this possibility, because the

K-shell binding energies of these materials are ~ 1/2 keV. However, for these

materials it would not be accurate to use Eq (7.1) with a cut-off energy as low as 100 eV, as is sometimes done in radiobiological calculations.

8. ELECTRON COLLISION STOPPING POWERS AT LOW ENERGIES

There is an energy below which the concept of an electron collision stopping

power loses its usefulness. The lower the electron kinetic energy, the larger is the

fraction of the energy lost, on the average, in a single inelastic collision. For

example, it can be shown (Paretzke and Berger, 1978) that the average fractional

energy loss in a collision with a water molecule in vapor is 0.5 percent at 10 keV,

3.6 percent at 1 keV, 6.4 percent at 0.5 keV, and 22 percent at 0.1 keV. The

continuous - slowing-down approximation, i.e., the use of a stopping power to describe

the gradual energy loss along the electron track, ceases to be meaningful at energies

below several hundred eV. The evaluations of low-energy electron stopping powers

found in the literature have often extended down to lower energies (typically 20 eV)

,

but such results have significance mainly as a summary description of low-energy

energy-loss cross sections.

8.1. Calculations for gases . There have been considerable advances in recent

years in the knowledge of electron- impact ionization and excitation cross sections at energies from 10 keV down to a few eV. The need for such data has arisen in two

contexts: in the evaluation of semi -empirical oscillator-strength distributions such

as those referred to in Table 3.1, and in the calculation of electron energy degradation spectra which take into account the slowing down of electrons and the buildup

of successive generations of secondary electrons from ionization events. The often

incomplete and sparse experimental data have been supplemented by estimated cross sections obtained by theoretical modeling, the adopted cross sections have been

subjected to consistency checks in the form of sum rules, and comprehensive sets of cross sections have been assembled for a number of gases. This approach, and the

results obtained, have been described by Green and Miller (1974), Fano (1975), and

Inokuti, Douthat, and Rau (1976). For atmospheric gases, cross sections have been

given by Jackman et al

.

(1977) where references to earlier work of Green and

co-workers can also be found. From knowledge of the total cross sections for

ionization and excitation, and the ionization cross section differential in the

energy transferred to secondary electrons, one can readily construct collision

stopping powers according to Eq (2.1).

8.2. Calculations for solids and liquids . Almost all of these calculations

have been based on the approach of Lindhard (T954) , Fano (1956), and Ritchie (1959).

The stopping properties of the medium are expressed in terms of a complex-valued

dielectric- response function e (K,cu) that depends on the momentum transfer hK and

energy transfer hoi. The collision stopping power is proportional to a double

integral, with respect to K and w, over the quantity (m/K) Im[-l/e (K,w) ]

.

In the so-called statistical model, the dielectric-response function is

calculated according to the local-plasma approximation (free electron gas model) of

Lindhard (1954), which has already been mentioned in Section 3 in connection with the

evaluation of the mean excitation energy. The dielectric-response function has been

calculated by Ashley, Ritchie and collaborators using a variety of models, adapted to conductors, semi-conductors and insulators, that take into account single-electron

excitations as well as collective excitations (plasmons). Whenever possible, experimental optical data were used to obtain the dielectric-response function in the limit

of zero momentum transfer, e(o,co). 15 It was still necessary, however, to obtain

e (K

,

uj) for non-zero K through theoretical extrapolation, guided by the requirement

that very large energy transfers should be described by the Rutherford cross section,

or by the Miller cross section when exchange is taken into account. Usually the

15 e(o,w) is sufficient for the calculation of the mean excitation energy I according to Eq (3.6).

20
contribution to the stopping power from inner-shell electrons has been evaluated with

the use of theoretical atomic generalized oscillator strengths, which is justified on

the basis that the wave functions of the inner-shell electrons are insensitive to the

state of aggregation of the medium.

Tables of electron collision stopping powers have been given by Ashley et al

.

(1975) for Al and A£ 2 0 3 ; Ashley et al. (1976a) and Tung et al. (1979) for A£, Si, Ni,

Cu, Ag and Au; Ashley et al. (1976b) for Ge and GaAs ; Tung et al. (1976) for Si and

Si0 2 ; Ashley et al. (1978) for polystyrene; Ritchie et al. (1978) for water; Ashley

et al. (1979) for Al; Painter et al. (1980) for polyethylene; Ashley (1980) for

various organic solids, Ashley and Anderson (1981) for Si0 2 ; and Ashley (1982a) for

water. Other calculations based on the use of Lindhard's statistical model have been

reported by Sugiyama (1976).

8.3. Comparison of stopping powers . The case of water is especially interesting because comparisons can be made between stopping powers from different authors

for water vapor as well as liquid water. In the left-hand panel of Fig. 8.1, for

water vapor, curve 1 is from Paretzke and Berger (1978), 1 6 curve 2 is from Green, 17 and curve 3 is from the Bethe theory, Eq (2.16), with I = 71.6 eV. Curves 1 and 2 both lie below the Bethe curve 3, but the differences are smaller than 10% down to ~ 400 eV. Curves 1 and 2 agree rather closely down to ~ 150 eV, but diverge at lower energies. The main reason for this divergence lies with the total ionization

cross section which Green took from the experiment of Schutten et al. (1966) whereas

Berger relied also on those of Mark and Egger (1976) below 150 eV. In the right panel in Fig. 8.1, for liquid water, curve 4 is from Kutcher and

Green (1976), curve 5 is from Ritchie et al. (1978), curve 6 from Ashley (1982a),

and curve 7 is from the Bethe theory with I = 75 eV. The calculations leading to curves 4, 5, and 6 all take into account collective excitations (plasmons) and use

the experimental optical data of Heller et al. (1974) on uv absorption in liquid

water. Ashley constructed the dielectric function for liquid water from an insulator

model fixed by the available optical data, and treated ionization from the K shell

by theoretical generalized oscillator strengths. As explained by Ashley, the main

difference between his calculation and the earlier work of Ritchie et al

.

consists of an improved treatment of exchange effects, which results in a lowering of the peak of

the stopping-power curve at ~ 120 eV by 25 percent. The formalism for obtaining the

collision stopping power in terms of the dielectric response functions is a Bornapproximation theory. The uncertainties resulting from the use of this approximation

could easily be 10 percent at 100 eV and even greater at lower energies. The peak of

the stopping-power curve 6 of Ashley is 13 percent above the corresponding value for

water vapor (curve 1). It is not clear whether this difference is significant,

because it lies within the combined limits of uncertainties for the liquid and vapor

results

.

Figure 8.2 compares collision stopping powers in H 2 gas calculated by Green 17 and by Spencer and Pal (1978). Also shown are curves obtained with the Bethe formula

for H 2 gas (I = 19.2 eV) and for liquid hydrogen (I = 21.8 eV) . The results of

Green and of Spencer and Pal are in good agreement down to ~ 30 eV; both of these

results deviate significantly from the Bethe theory only below ~ 200 eV. Also shown

in Fig. 8.2 is a stopping-power curve for air which was constructed from the results

of Green 17 for N 2 , 0 2 , Ar, and C0 2 . Again there is good agreement with the Bethe

formula down to 200 eV. An earlier stopping -power curve for air, calculated by Green

and Peterson (1968), coincides with curve 5 in Fig. 8.2 down to 1 keV, and is

10 percent lower at 0.1 keV. Using the Green-Peterson stopping powers and taking

into account multiple elastic - scattering deflections, depth-dose curves have been

calculated for an air medium irradiated by 12-keV and 5-keV electrons (Berger et al.,

1970). These results are in good agreement with measurements in air by Grim (1957)

and in nitrogen by Cohn and Caledonia (1970).

1

5

Curve 1 is the result of a calculation by Berger given in Fig. 4 of Paretzke and

Berger (1978). That figure also shows stopping-power curves obtained independently

by Paretzke, and by Olivero, Stagat and Green (1972). These curves are all quite

similar to curves 1 and 2 in Fig. 8.2 at energies down to ~ 150 eV.

17 Green has calculated (and communicated to us in January 1978) collision stopping

powers from 15 keV down to a few eV, based on the cross sections given in Jackman

et al. (1977) and on cross sections for other gases compiled by his group. In the case of water vapor, Green's results are an updated version of stopping powers

(energy-loss functions) given earlier by Olivero, Stagat, arid Green (1972).

21
Figure 8.3 shows stopping-power results of Ashley (1982c) for polyethylene, and

results of Ashley et al

.

(1978) for polystyrene obtained from dielectric-response

functions constructed with the use of optical data for the valence electrons.

Similar results for silicon dioxide, from Ashley and Anderson (1981), are shown in

Fig. 8.4.

Figure 8.5 compares stopping-power curves for aluminum and gold from the Bethe

theory with calculations of Ashley et al. (1976a) obtained with a statistical model

of the dielectric-response function, without differentiating between inner- and

outer-shell electrons. Also shown is a stopping-power curve for aluminum calculated

by Ashley et al. (1979) with further refinements. These refinements include the

limitation of the dielectric- response function modeling to conduction electrons,

consideration of damping and core polarizability, and the use of atomic generalized

oscillator strengths from Hartree-Slater wave functions for inner-shell electrons.

It can be seen that the differences between the simple and refined calculations for

aluminum are not very great.

Other comparisons and analyses of low-energy stopping-power data can be found in

Iskef et al. (1980), and in Waibel and Grosswendt (1980).

An experimental investigation of electron stopping power in air and collodion 18 was carried out by Cole (1969). For collodion the experiment consisted of determining

the foil thicknesses for which the number transmitted was 5 percent of that in the

incident beam. For air the experiment consisted of measuring characteristic depths

such that only 1 percent of the ionization in air occurred at greater depths. Cole

considered these foil thicknesses and characteristic depths as "ranges". With this

somewhat arbitrary definition of ranges he fitted his data for collodion and air by a single polynomial curve of range vs. incident electron energy (with a stated accuracy

of 10 percent) and obtained the stopping power by differentiating this curve with

respect to energy.

Cole's results suggest that, in the case of air and collodion, gas-solid stoppingpower differences, if any, are small. This is consistent with the later findings of

Schou (1979) and Sorensen and Schou (1978), based on the analysis of their electron

penetration measurements in liquid nitrogen at 1 to 3 keV, that the stopping powers

in liquid are at most a few percent higher than the stopping powers in gas.

The results of Cole are compared in Table 8.1 with the stopping powers for

cellulose nitrate from the Bethe theory, and for air from the Bethe theory and from

the calculation of Green. 17 There is close agreement between experimental and

theoretical results down to ~ 400 eV. Below this energy the experimental values are higher, by 19 percent at 100 eV and much more at lower energies.

The significance of Cole's results is obscured by two uncertainties. First, a considerable error must have resulted from the numerical differentiation of his

range-energy curve, especially at low energies. Second, his analysis neglected the

effect of multiple-scattering angular deflections which make the pathlength traveled

by electrons greater than the depth of penetration. Thus multiple scattering would

tend to make the apparent stopping power determined by Cole larger than the true

stopping power, by an amount that is expected to increase as the electron energy

decreases

.

The comparisons in Figs. 8.1 to 8.5 indicate that the differences between the

stopping-power values from the Bethe theory and those from more elaborate low-energy

treatments are often rather small, even at energies where the conditions of applicability of the Bethe theory are no longer satisfied. We therefore give in Table 8.2

a set of stopping-power values for selected materials covering the energy region from

10 keV to 1 keV. We estimate that at 1 keV the departures of the correct stopping

powers from the tabulated results will be no greater than ~ (1/7) percent, where I is the mean excitation energy in eV.

8 Collodion is a plastic prepared as a suspension of cellulose nitrate in ether and

alcohol. The estimated mean excitation energy of cellulose nitrate is 87.0 eV, a value rather close to that for air, 85.7 eV.

22
9. RADIATIVE STOPPING POWER

The mass radiative stopping power can be expressed in terms of bremsstrahlung

cross sections as

i («L - S , (T)p rad

r r

T da

U

dk

*/o (9.1)

where dan /dk is the differential cross section for the emission of a photon of

energy k* due to the interaction of the electron with the screened Coulomb field of

the atomic nucleus, and doe /dk is the corresponding cross section due to the

Coulomb interaction with one of the atomic electrons. The upper limit of the energy

of the photons that can be emitted in electron-electron interactions is

T' = me T [T 2mc^ - 0 (T + mc“) ]

1

(9.2)

It is convenient to introduce dimensionless, scaled, radiative energy-loss cross sections

4"d * z2 > _1

/ < k/E> dk , (9.3)

and

4ld to r e>'

X f (k/E)

do

e 3ir dk , (9.4)

? where a is the fine-structure constant, and E = T + me is the total energy of

the electron. In terms of these quantities the radiative stopping power can be

written as

I

S rad< T ) * JT ° r

e E ^ 4ad m

[

E * (1 /Z) tSdl/tSu)] • C9-S)

The ratio 4a!/ ^ral has in previous work usually been assumed to be unity. As will

be shown below, this ratio is actually slightly higher than 1 at high energies, falls

to ~ 0.5 at 700 keV, and tends to vanish at low energies. 19 For compounds we assume that additivity is a good approximation, and set

— S

p rad - I w.fis

j \P ra d /

(9.6)

where w_. is the fraction by weight of the j’th constituent.

1 According to Joseph and Rohrlich (1958), the vanishing at very low energies is due

to the lack of an electric dipole moment for the electron-electron system.

23
9.1.

9.1.1. Electron-nucleus bremsstrahlung

High-energy region . For T > 50 MeV, the bremsstrahlung cross section

was evaluated from the analytical expressions of Davies, Bethe, and Maximon (1954],

and Olsen (1955). This formula corrects the Bethe (1934) Born-approximation result

through the inclusion of a Coulomb correction f(Z) derived with the use of

Sommerfeld-Maue wave functions. The formula is based on the high-energy approximation, i.e., the assumption that the energies of the electron both before and after

the bremsstrahlung event are large compared to the electron rest energy. The cross section has the form

do ^ ^ Z k rr 4 “d z ME.*) e . +

i J

l h

i (q) [l-F(q,Z)] 2 dq - f(Z) (9.7)

where q is the momentum transfer and

q Q

= me k/[2E(E - k)

]

(9.8)

the minimum momentum transfer (with both in units of me) . The Coulomb correction is

given by

f(z) = (azr £

n=l

[n(n‘ Z

2 )] (9.9)

The other quantities in Eq (9.7) are defined as follows:

g 2

g. = - 2 (E - k)/3E n = 1 + (E - k)

2 /E 2

e

l = 1

h

i = (q - q 0

) 2 /q

3

e

2 = 5/6

P - 6q

o q £n(q/qo

)

3q; q

- 4q aIP*

(9.10)

F(q,Z) is the atomic form factor, normalized such that F(0,Z) = 1. For 1 < Z < 6 the atomic form factor was taken from the non-relativistic calculations of Hubbell

et at. (1975) which include electron-correlation effects; for Z > 6 it was taken

from the work of Hubbell and 0verb0 (1979) which is relativistic but omits correlation effects.

9.1.2.

Low-energy region . For T < 2 MeV, use was made of work by Pratt et at. (1977) which constitutes a significant advance over the Born-approximation theory of

Bethe and Heitler. In this work, the bremsstrahlung process is treated as a singleelectron transition in a self-consistent screened central potential. Electron wave functions are obtained in partial wave- function expansions through the numerical

solution of the Dirac equation, and the matrix elements for the bremsstrahlung cross section are evaluated numerically from the wave functions. The required amount of

computation is very large, especially in view of the large number of partial waves which have to be included, so that results have been obtained so far only for a limited number of materials and energies. The theory underlying the computations and

initial numerical results were given by Tseng and Pratt (1971). Further numerical

results for electrons with energies from 1 to 500 keV were published by Lee et at. (1976), and 'for 1- and 2 -MeV electrons by Kissel and MacCallum (1977). An extensive

set of data for all elements 2 < Z < 92, including bremsstrahlung cross sections

differential in photon energy as well as the total energy-weighted cross section was prepared by Pratt et at. (1977) through elaborate interpolation procedures. A few

24
exploratory calculations, for 5- and 10-MeV electrons in A£ and U, have recently been

published by Tseng and Pratt (1979) which involve the calculation of selected terms

in the partial wave expansions and interpolation between them. We have used the

tables of Pratt et al. (1977) to obtain bfai and have derived values for Z = 1 and for Z = 93 to 100 by extrapolation.

9.1.3. Intermediate energy region . For T between 2 and 50 MeV, the scaled

radiative energy-loss cross section has only a mild dependence on Z and on the

electron energy T. Being anchored down firmly below 2 MeV and above 50 MeV, the curve of b^^(T) us. T in the gap region can readily be obtained by interpolation.

We have done this using a cubic-spline least - squares algorithm of Powell (1967).

Typical results of this interpolation for Z = 1, 6, 13, 29, 47 and 79 are shown in

Fig. 9.1. The results of the interpolation have been found to be quite insensitive

to the choice of the upper cut-off energy for the gap region. A shift from 50 to 100 MeV would change the integrated cross section in the gap region by less than

1 percent, and a shift down to 20 MeV would change it less than 3 percent.

In four cases (A£ and U at 5 and 10 MeV) the radiative energy-loss cross sections can also be derived directly from the differential bremsstrahlung cross sections of Tseng and Pratt (1979), and are found to agree to within 1-2 percent with

our interpolated results.

9.2. Electron- electron bremsstrahlung

9.2.1. High- energy region . For T > 50 MeV, a combination of three cross- section formulas was used. The first is the Bethe-Heitler (1934) Born-approximation

result which disregards screening and was derived in the high-energy approximation:

k

(.3Tr)

B

= 4ctr e [§1 CF. ,k) + g 2

( E , k

)J (£n(l/q

0

) - 1/2] , (9.11)

where gi, g 2 , and q 0 have the same meaning as in Eqs (9.7) to (9.10). The

second formula used is that of Wheeler and Lamb (1939) , also based on the first Born

and high-energy approximations, which treats screening with use of the incoherent

scattering function S(q,Z):

(da \

2

2 r f

1 1 WwL = 4ar“ £ g.= (E,k)

e

i = l

1 ei + I h

i (q) S (q , Z ) dq

L q 0

It can be seen that this equation can be obtained from Eq (9.7) by setting Z = 1 and replacing [1 - F(q,Z)] 2 by S(q,Z). In Eq (9.12), S(q,Z) is normalized such

that S(°°,Z) =1. We have taken the incoherent scattering function from Hubbell

et al. (1975). The third cross section used is one derived by Haug (1975) in lowest

order perturbation theory, without consideration of screening effects, but treating

recoil and exchange effects accurately. Haug also considered the Coulomb correction

(departure from Born approximation) but found it unimportant at high energies.

Haug's calculation is expressed in complicated formulas (his Eqs 2.15, Al and A2)

which are too lengthy to be reproduced here. We have used numerical values given in

Haug's paper.

Taking Haug's cross section (da e /dk) Hg as initial approximation, we have

assumed that the electron- electron differential bremsstrahlung cross section is

dc

e / do e\

ay~ ~ \mr/HG

+ [y

da

e VST” WL

(9.13)

where the first term incorporates an exchange correction and the terms in square

brackets constitute a screening correction. This treatment can be justified on the

basis that the two corrections are almost independent of each other, with exchange

affecting mainly large momentum transfers and screening mainly small momentum

transfers

.

25
assumed that

9.2.2.

Low-energy region . For T < 2 MeV, we have

rad

-rdk k

doe\

air/

HG

' idk f _ k (&)BHSR

(9.14)

where (dce /dk) H Q is again Haug ' s cross section with exchange and no screening, and

where (don /dk) g^g^ is the cross section without screening derived by Bethe and

Heitler (1934), bauter (1934), and Racah (1934) in the Born approximation but without

invoking the high-energy approximation. The so-called Elwert factor

f £

= 3(1 - exp (- 2iraZ/3)] / 3'[1 exp(- 2TrotZ/0 ’ ) ] (9.15)

which depends on the electron velocities 6 and 3' before and after the collision,

is an approximate Coulomb correction due to Elwert (1939) . For the electron-electron

bremsstrahlung cross section in the numerator of Eq (9.14) a Coulomb correction was not considered necessary. Equation (9.14) is valid to the extent that screening does

not change the ratio of radiative energy-loss cross sections significantly.

9.2.3.

Intermediate energy region . With 4>racl determined for T < 2 MeV and

for T > 50 MeV, the quantity bracl( T ) U + (1/ Z) (T) /4>ral ( T ) I was obtained in

the gap region, 2 to 50 MeV, by the same interpolation procedure^ previous ly used in

Section 9.1.3 for <I>i>5cL (T) . This completed the evaluation of b||^(T) and of the

total radiative stopping power according to Eq (9.5).

The ratio ^fcL (T) CH is shown in Fig. 9.2 for hydrogen, carbon and gold

as a function of electron energy.

9.3.

Accuracy and comparison with experiments . Pratt et al . (1977) estimate

the uncertainty of their differential bremsstrahlung cross sections to be no greater

than 10 percent. It seems plausible that the radiative stopping power, obtained as an integral over these cross sections, has a smaller uncertainty, perhaps 5 percent.

Comparisons are made in Fig. 9.3 between calculated radiative stopping powers in five

materials at energies up to 2.5 MeV, and corresponding results derived from

bremsstrahlung measurements. There is good agreement, within the limits of experimental error, with the results of Aiginger (1966), Rester and Dance 20 (1967) and

Rester and Edmonson (1972); the theoretical results are lower than those from the

earlier measurements of Motz (1955) and Motz and Placious (1958). 21 The high-energy theory of Davies, Bethe, and Maximon (1954) and Olsen (1955)

provides the cross section not only for bremsstrahlung but also for the closely

related process of pair production. Whereas there is a scarcity of experimental

bremsstrahlung measurements above 2.5 MeV, there are sufficient data to assess the

accuracy of the pair production cross section. According to Hubbell et al. (1980),

the theoretical pair production cross sections above ~ 50 MeV are confirmed by

experiments to within 1-2 percent.

In resultsthe transition region between 2 MeV and 50 MeV we

to have an accuracy of 3-5 percent.

expect our interpolated

9.4.

Positron bremsstrahlung . Whereas electrons are attracted by the nuclear

charge and repelled by the atomic orbital electrons, the opposite is the case for

positrons. This leads to differences between the bremsstrahlung cross sections for

electrons and positrons. These differences are small at high energies; in fact they

vanish in the approximation used in the theory of Davies et al

.

(1954) and Olsen (1955).

At low energies, however, the bremsstrahlung cross sections for positrons are con- siderably smaller than those for electrons of the same energy. This has been

established by Feng et al . (1981) in calculations of the bremsstrahlung emitted by

positrons in the field of the atomic nucleus, for oxygen and uranium targets at positron energies of 10, 50, and 500 keV. The calculations of Feng et al. were based

on the same detailed numerical approach used earlier for electron bremsstrahlung by

Tseng and Pratt (1977).

From the bremsstrahlung spectra (differential in photon

et al., one can obtain the scaled radiative energy-loss cross

energy)

section

by+’ Feng

for

20 A1so private communication from D. Rester (1967).

2 tester and Edmonson (1972) suggest that an incomplete background correction in the

experiment of Motz accounts for this discrepancy.

26
positrons and relate them to the corresponding quantity [dfad] for electrons. One

finds that ['t’ladl +

/ Df’raa] ~ ^ as t 'ie values 0.465, 0.708 , and 0.916 for Z = 8, and

the values 0.0944, 0.175 and 0.359 for Z = 92, at the energies 10, 50, and 500 keV,

respectively. When these six ratios are plotted as a function of the single parameter

£n(T/Z 2 ), they fall on a smooth curve, with a dependence on T/Z 2 as .indicated in

Table 9.1. We have interpolated in this table to obtain values of [f rad^ + // ^rail

" for other energies and for other atomic numbers. Admittedly the scaling law used is

strictly empirical, and the underlyihg data base is quite limited. Nevertheless, in

view of the large positron-electron differences, it seemed better to calculate these

differences with this tentative scaling law than to disregard them.

It is also necessary to estimate the contribution of positron bremsstrahlung in

the field of the atomic electrons. It is expected that at high energies there is

little differences between the scaled radiative energy-loss cross sections for

positrons and electrons, i.e., [4>j>fj] + - [^rld]"- Taking into account the formal

identity of the non- relativistic electron-proton and the positron-electron bremsstrahlung cross sections in the center-of -mass system (Joseph and Rohrlich, 1958), and the

transformation to the laboratory system, one can estimate that at very low energies

[<4aci]

+

. s ** [4a<i]'. In order to connect these two limiting cases, we have made the

assumption that [

(l

) ^ail

+ = X CT, Z) [^^adJ " »

-where > for T > 5 MeV, x(T/Z) is equal

to the ratio <{> ^ e

1 I for electrons as given in figure 9.2, and where x(T,Z)

has (for all Z)

r the values 0.539, 0.5S8, 0.587, 0.613, 0.643, 0.691, 0.732 and

0.785 for T = 0.01, 0.02, 0.05, 0.1, 0.2, 0.5, 1 and 2 MeV, respectively.

We estimate that the uncertainties of the radiative stopping-power values for

positrons, obtained as described above, are on the order of 10 to 20 percent. The

uncertainties are perhaps smaller for materials such as water, tissue or plastics

which have an average atomic number rather close to the value Z = 8 for which

Feng et al . made calculations.

10. RANGES AND RADIATION YIELDS

The ranges and radiation yields given in this report were obtained in the

continuous-slowing-down approximation (c.s.d.a.). In this approximation energy-loss

fluctuations are neglected, and electrons are assumed to lose energy continuously

along their track, with a mean energy loss per, unit pathlength given by the stopping

power. The c.s.d.a. range (in units of g cm ) is evaluated from the expression

(

T

° r

0 (T0 - Tf

) - P / [S col (T) * S rad tT}] 1

<11 , ( 10 . 1 ) X f

and represents the average pathlength 22 traveled by an electron as it slows down

from an initial energy T0 to a final energy Tf. The choice of Tf should, in

principle, be adapted to the purpose for which the range is to be used. For example,

if one wanted to know how far electrons can travel while they are capable of ionizing

atoms of the medium, it would be appropriate to set Tf equal to the lowest atomic

ionization potential.

The stopping powers needed for the evaluation of r 0 from Eq (10.1) are available from the Bethe theory only down to some intermediate energy Tf, and the part

of the integral from T = Tf to Tf must be obtained by an approximate estimate.

Fortunately this residual range is relatively small so that a simple approximation

is sufficient. We have followed Nelms (1956) in assuming that the integrand

[Scol(T) + S racj(T)] is zero at T = 0 and can be interpolated linearly to its

value at T = Tf. The range is then given by

VTo Tr) = r (T o^o Tf) ptWV + S rad (Tf)]

-1 f

1 T,

(T/Tf) dT ( 10 . 2 )

where the first term is calculated according to Eq (10.1), and the second term is

the residual range. In the range tables we give results obtained with Tf = 1 keV

and Tf = 0.

22 This is actually only an approximation, but a very close one. For example, we have determined through Monte Carlo transport calculations that in a water medium

the actual mean pathlength down to a final energy Tf = 12.6 eV is ~ 1 percent

greater ° than r (T -*• T^) for T > 10 keV.

o of' o ~

27
For some materials it is possible to avoid the crude approximation used above

for residual ranges below 1 keV, and to rely instead on estimated low-energy stopping

powers. We have made such calculations for water vapor, polystyrene, aluminum and

gold, using data from Figs. 8.1, 8.3, and 8.5. As shown in Table 10.1, the ranges

r (T0 0) from Eq (10.2), for initial energies T„ = 10 keV, actually are quite

close numerically to the more accurate ranges calculated with a final energy

T

f = 10 eV. The radiation yield (also called bremsstrahlung efficiency) is the fraction of

the initial energy T0 of an electron that is converted to bremsstrahlung energy as the electron slows down to rest. The c.s.d.a. yield is given by

Y < T

0

) - T~ /

°

[S coi m * W1 ”' 1 S rad tT) dT . (10.5)

0 o In the evaluation of this expression one is again faced with the difficulty that

neither S co p nor S racj is known accurately below an intermediate energy Tj_ = 1 keV.

We have made the assumption that S ra(^ (S co p

+ Spa^)' 1 is zero at T = 0 and

increases linearly to its value at T = Ta

.

11. MISCELLANEOUS COMPARISONS

11.1 Positron-electron differences . For the collision stopping power, differences arise because of the use of the Bhabha cross section instead of the Miller cross section for large energy transfers, and because - by definition - an electron can at most lose half its energy in a single collision, whereas a positron can lose its

entire energy. These differences are shown in Table 11.1 in terms of positron-toelectron collision stopping-power ratios for a representative set of materials.

Positron-electron differences in the radiative stopping power have been discussed in

Section 9.4 and indicated in Table 9.1. The differences in collision and radiative

stopping powers both contribute to differences in range. Positron-to-electron c.s.d.a.

range ratios are also shown in Table 11.1. 23 11.2. Comparison of calculated and experimental stopping powers . There is

available only a limited amount of experimental data pertaining to the total stopping

power (collision plus radiative). Comparisons with measurements by Paul and Reich

(1950) at 2.8 and 4.7 MeV and by Ziegler (1958) at 32 MeV are given in Table 11.3.

The experimental and calculated results agree, within the limits of experimental

uncertainty, at 2.8 and 32 MeV, but not at 4.7 MeV. Table 11.4 presents comparisons

with stopping-power ratios (relative to Be and A£) measured by Westermark (1961) and

by Hereford (1948). Experimental and theoretical values agree within the limits of

experimental uncertainty.

In Figs. 11.1 and 11.2 collision stopping powers measured by Kalil et al.

(1959) and Ishigure et al . (1978) in aluminum and by Ziemer et al. (1959) in copper

are compared with results from the Bethe theory. These figures show Fano plots,

i.e., plots of stopping power vs. energy in a scaled representation in which the

Bethe formula gives a straight line. The experimental results of Kalil et al

.

for

aluminum between 10 keV and 1 MeV, and those of Ziemer et al

.

for copper between

200 keV and 1 MeV cluster around the theoretical straight lines, but the dispersion

of the experimental points is considerable.

11.3. Comparisons with previous calculations . Differences between the stopping

powers, ranges , and radiation yields from this report and those from earlier tables

by Berger and Seltzer (1964, 1966) and Pages et al

.

(1972) are shown in Table 11.5

for a few materials. Whereas the differences in regard to the collision stopping

power amount to only a few percent, the differences in regard to the radiative

stopping power and radiation yield are much larger, especially at energies below ~ 1 MeV, due to the change from Bethe-Heitler bremsstrahlung cross sections to the more accurate results of Pratt et al

.

(1977).

23 The positron ranges used to compute the range ratios in Table 11.1 pertain to the case in which the positron slows down to rest before being annihilated. If one included the possibility of positron annihilation in flight, the positron ranges

would be slightly decreased. From results given by Heitler (1947) one can conclude

that the shortening of the positron range in lead would amount to 1.7 percent at 0.511 MeV, 4.2 percent at 5.11 MeV, 4.0 percent at 51.1 MeV, and 3.1 percent at 511 MeV.

28
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Wolke, R. L., Bishop, W. N. , Eibhler, E. , Johnson, N. R. and O'Kelley, G. D. (1963).

"Ranges and stopping cross sections of low-energy tritons," Phvs. Rev. 129,

2591 . Yates, A. C. and Langhoff, P. W. (1970). "Bounds for oscillator-strength sums from

approximate quadratures," Phys. Rev. Lett. 2_5, 1317.

Zeiss, G. D. , Meath, W. J., MacDonald, J. C. F. and Dawson, D. J. (1975). "Dipole

spectrum of water vapor and its relation to energy loss of fast charged

particles," Radiat. Res. 63^, 64.

Zeiss, G. D., Meath, W. J. , MacDonald, J. C. F. and Dawson, D. J. (1977a). "Dipole

oscillator strength distributions, sums and some related properties for Li, N,

0, H

2

, N

2

, 0

2

, NH

3

, H

2 0, NO and N2 0," Can. J. Phys. 55_, 2080.

Zeiss, G. D. , Meath, W. J. , MacDonald, J. C. F. and Dawson, D. J. (1977b). "Accurate

evaluation of stopping and straggling mean excitation energies for N, 0, Hg, 1N2 , 0£, NO, NH 3 , H

2 0, and N^O using dipole oscillator strength distributions. A

test of the validity of z Bragg's rule," Radiat. Res. 70_, 284.

Zeiss, G. D., Meath, W. J., MacDonald, J. C. F. and Dawson, D. J. (-1980). "On the

Additivity of atomic and molecular dipole properties and dispersion energies

using H, N, 0, Hg, N? , 0 7 , NO, N?0, NH 3 and HgO as models," Molec. Phys. 39 , 1055. Z

39
Ziegler, B. (1958). "Energieverlust und Energiestreuung schneller Elektronen in Be,

C und Al," Z Phys. 151 , 556.

Ziegler, J. F. (1977). Helium : Stopping Powers and Ranges in all Elemental Matter , Pergamon Press, New York.

Ziegler, J. F. (1980). "The stopping and ranges of ions in matter," Vol. 5, Handbook

of Stopping Cross Sections for Energetic Ions in all Elements , Pergamon Press,

New York.

Ziemer, P. L., Johnson, R. M. and Birkhoff, R. D. (1959). "Measurement of stopping

power of copper by calorimetric methods," Oak Ridge National Laboratory Report

ORNL-2775.

Zrelov, V. P., Kruglov, S. P., Mus , K. F., Savel'ev, V. D. and Sulek, P. (1974).

"Determination of the average excitation I„ of copper ion from the ionization

range of 660-MeV protons," Yad. Fiz. 19_, 12^6; Sov. J. Nucl . Phys. 19_, 653.

40
Table

3.1

Mean

excitation

energies

obtained

from

moments

of

dipole

oscillatorTable

3.2

Numerical

values

of

parameters

adopted

by

Bichsel

to

fit

measured

strength

distributions

(OSD).

Results

are

for

atoms

unless

indicated

stopping-power

and

range

data

for

protons

and

alpha

particles,

otherwise.

H— CNJ 4- 4-

zn s- Q O G OO L- 4- OO OO o o o o CM 4-0

I r- OO r— >»o

S- u s- u o

O -r- V i. U rj U L

•— XC u

4-> CL -M •— Q. Q. *- E E =

<+- cu <d a» ai

i e s- i i

f— 4-> 4-»

f" •*- c c

Q. CL *-> O O 4J -P f- P t- E £ *r* *r— **— •*— -r— 4-> 4-> (D CD 4- 4-> 4-» 4- 4- 4-> <D +*> <D E E GJ E E E

CD O CD O

S- C C E CD

o a r— OO OO r— flOO (B L H3 ^ •

•r- U U *r- a*r- •— CL E +-» E

CD CD CD 0)

c/> w Z > > Z Z E 4->

O O OO OO r— O O 03U

nj "3 L

O U 1-

r- *r a.

4-» 4-» E

<D CD CD

L. i- I O O -r- CD CD E

XI _C CD

<a q xj oo

s- o

L L <U U

f- •— O O CL-.- r—

S- <13 CD CD 1 t- 03

•r- UXX C -r- O

4-» CL-r- *JP O Q-'t-

•*- E -M •*- E -p» 4- CD VPPP 0) CD

I S- E C ca l U

O CD CD -r- -r- O CECDEES-E<D CD XI c O 03 OJ JC Z^p£E>i^p

oo a oo

cn T3

OHO CD <— 2 OO

TJ ON • C L Ol 'OCOr- a

i *4— “O

4- c

. O 03

o c e

4->—' i. i_ 1/10 fl ro

*• CD OO CD C7V—

i c cn .— .— <o

I -t— r— fQ 03 vO

, —' q q cn 'a o -a -o > c c c c

03 o-*>

L nj L io io n: inC 03 <D 4-

cj -*-> cn*a x: cn .

— or c c a -— <— 03 03 l- <D 03 XI XI 03 GQUUO

t-O 03 CD

i— CD a r- . •POl

r- CJ

O it/1 XI CD

<— CD 3 Ol E »— •+-» o c x:

CD

CO -r- CD C/> CD O E CO r— CD -C -f— 03 U CD CD QZQN

CD XI -r- U CD CD ZQN

co O CD O) C 4-> r—

r-T3

co c a —

Q 03 *—

03 O S- -M x ai sI— CD E 03

tn co c\j c\j cvj or co co ci or ai

co «yrNOr-^- Or-r-CO O--N01

cvi i

CO r- r—

41

360

Bell

and

Dalgarno

(1965)

M(n)

fit

320.3

Dehmer

et

al.

(1975)

theoretical

OSD
qj a> cr

co CM

in V -

r— O r—

V A

oloA

^03 VO CO CO q- O r- o I— <— r— ^

CNJ LO <T>

CT* lO r—

OVOV a

A

«— o *— o

-a •«- C QJ -M O 4-> • U

-r- rT3 r— QJ

+-> 3 U S- O <— U) i.

QJ «3 -C O

s- > o o

S_ QJ -r- O CO QJ u vn

" "4_ Qj -c cvjor

u _i •*-» O'M E n

L- 4-*

i cn-r- o 2 — i_

:_i q. *a

ca

3 E

c +-> a. o

o o E u

•«- +-» O

U II -C r—

CO T- QJ i.

+-» -r- QJ u cn jo

* qj v. £ N i- OJ O

o ti -p a •r— 4-> O CL

u c 3 qj O ro O -id

LO CO CM

CTi Ol

o o cm O LO <

CO r— O O O O O O C\J

CM CO LO O

lo cn ro m

o o o o

o co lo cn r— cm O r- r— o

o o o o o co

lo co co O ct» ui is cm ai «a- co

CM I— ^ CO I— 1

o o

o o

LO O LO o

o o* o

CM CT> LO

o% «dr**» "—* CM

O O O O O CO

CO O «3- CM <T» CO

r— O co

i— cm O O f— o

O O O O O O <3*

o o o o

CM I N N N «— CM

o o o

N N N <— \ S.. \ _J . t_J O O CM

cm co ro o O r

O O CM O O CNJ CM o o o o o

i— cn

LO o LO co O O — CM r— CM O

CO LO CM CO

CM <3- LO o o o o

CO 00 CM CO o o o o o o ^r

LO CO LO LO LO LO r— O CM LO

CO f's. lO CO LO CO o LO cm o% lo cm lo o

O O O O O LO

N N N

fs. O LO *d- LO rs. O cm o'* co cn — o cn r- LO <Tl t— O CO CO O O «— O O •— o o o O O* o’ cn

o o o o

O *3* LO CO LO CO CM O r— ^ o o ^

O r-* <— co lo cn co LOCMO>LO^-«d*«3-

CO O O ^ CO 0 0 0 0 0 0*3- O O O O O O lo

r- O rOl LO *3 LQ

CM — LO CO O O CM O O lo

N N N f— CM

42

Proton

energies

are

pertinent

to

the

analysis

of

stopping-power

measurements

i

Figs.

4.3,

4.4,

and

4.5.
Table 3.5 Analysis of range measurements of Barkas and von Friesen (1961).

I-values are evaluated assuming that 1^ = 166 eV, which implies

a proton energy of 749.0 MeV. The experimental proton ranges were

314.9 g/cm^ for Cu, 415.6 g/cm^ for Pb, and 432.5 g/cm^ for U, and have an estimated uncertainty of 0.1%. The corresponding

uncertainties of the I-values are 3 eV for Cu and 6 eV for Pb and U.

I, eV

Method of Analysis Cu Pb U

Bichsel shell correction,

with density-effect correction 314.3 821.2 889.2

Bichsel shell correction,

without density-effect correction 334.6 832.4 920.2

Bonderup shell correction,

with density-effect correction 314.6 818.3 884.8

Table 3.6. Comparison of mean excitation energies I extracted from proton stoppingpower and range measurements with the use of Bichsel's and Bonderup's shell corrections. The estimated uncertainties of the I-values are those resulting

from the uncertainties of the measurements. The measurements are from the experiments listed in Table 4.1.

I(eV), derived with use of

T Reference (MeV)

a 3 a 6 Stopping- b 6.5 power a 9 Measurements a 12 a 15 a 18 Q 19.8

Range Measurements d 749 -

a

S0rensen and Andersen (1973)

^Ishiwari et al. (1979)

Bichsel 's Shell Corrections

Cu Pb U

316±3 818± 9 91 0±1

4

31 7±3 814±12. 898±18

327±4 830± r - 319±3 810±14 886+20

319±5 806±16 881+22

31 9±5 803+17 878±24

318±6 800+17 877±25

325±5 851+20 “

31 4± 1

0

821+15 889x16

Bonderup's

Shell Corrections

Cu Pb U

310±3 745± 9 805=14

314±3 736±1

2

790±18

325±5 751+ 7 T - 318±4 738+14 789±20

31 9±5 742+16 794±22

320±6 746+17 799+24

320±6 747±18 806+25

325±6 798+20 “

31 5±10 818+15 885±16

a Burkig and Mackenzie (1957)

^Barkas and von Friesen (1961) From preliminary results of Ishiwari, Shiomi, and Sakamoto (private coimiuni cation,

January 1982).

43

.J
Table 4.1 List of stopping-power and range experiments from which mean excitation energies were deduced. S indicates stopping-power, R indicates range.

Abbrev

Bak 51 Tho 52 Bro 55 Bur 57 Bar 61 Mar 62 Nak 63

Bic 65 Tsc 68 And 67

And 68

And 69

Gar 7C

Swi 70 Han 70 S0r 73 Zre 74

And 77

Nor 79 Ish 79

Bes 79

And 81

Reference

Bakker and Segr& (1951)

Thompson (1952)

Brolley and Ribe (1955)

Burkig and Mackenzie (1957)

Barkas and von Friesen (1961)

Martin and Northcliffe (1962)

Nakano, Mackenzie, and Bichsel

(1963)

Bichsel and Tschalar (1965)

Tschalar and Bichsel (1968)

Andersen, Hanke. Sorensen, and Vajda (1967)

Andersen, Hanke, Simonsen,

Stfrensen, and Vajda (1968)

Andersen, Simonsen, SfJrenson, and Vajda (1969)

Garbincius and Hyman (1970)

Swint, Prior, and Ramirez (1970)

Hanke and Bichsel (1970) Sorensen and Andersen (1973)

Zrelov, Kruglov, Mus, Savel'ev,

and Sulek (1974)

Andersen, Bak, Knudsen, and Nielsen (1977)

Nordin and Henkelman (1979)

Ishiwari, Shiomi, and Sakamoto

(1979)

Besenbacher, Andersen, Hvelplund,

and Knudsen (1979)

Andersen and Nielsen (1981)

Type of Data

S rel. to Cu, 300-MeV protons

Partial proton range (rel. to Cu), 340-200 MeV

S, 4.45 MeV

S rel. to A£, 19.8-MeV protons

R, 750-MeV protons

S, 4 to 40-MeV alpha particles

S rel. to Aa, 28.7-MeV protons

R, 3- to 30-MeV protons

R, 3- to 30-MeV protons

S, 4.5- to 12-MeV protons

S, 5- to 12-MeV protons

S, 5- to 12-MeV protons

R, 12- to 40-MeV protons

S, 0.4- to 3.4-MeV protons

S, 1- to 9-MeV alpha particles

S, 5- to 18-MeV protons

R, 600-MeV protons

S, 0.8- to 7.2-MeV protons

S, 60-MeV pions

S, 6.5-MeV protons

S, 40-keV to 1-MeV protons,

100-keV to 1.2-MeV alpha particles

S, 0.8- to 7.2-MeV protons
73

d>

( CM , O CM <3- CM 00 CO co ,

•

1— 1— •— 1— r— CM vo LO CO

Ge +1 cn

+1 +1 +1 +1 +1 +1 3:+1 +1

I

D

+i +1 +l +1 O < co cn vo VO r— CM o CO cn rLO VO O vo vo co rv CM 'S* co VO CO P-. co LO <=3- r^v co cn oo CO CO

p**. CM r-. lo VO , VO r** *

•

CM CM 1— •

CM C +1 +1 +i +i -H +1 +1 +1 +1 +1

I'M 73 ro XT

vo o VO Q. o VO 1

.— ro o co H- VO

co CM co VO O CO CM CO CO

co CO CO «3- r^. O 03 VO cn O CM CO o co on CM co vo '

p*. r-* 6 8 4 1— CM P-* c- 1— 1— vo LO CM 1— CM 1

3 +i +1 +1 -H +i +1 +1 +1 +1 +1 +1 +1 +1 +1 +i +1 +1 +1 +1 +1 +1 O x: 73 XI vtOlO <3- cn VO cocoonon cc co CM O Cl. LO VO O O

cn CM CM co CM CM CM <— CM LO cn CM vO LO CM O co CM CO CO CO CO CO co CO CO co CO co •3- LO co r^. co 00 co co

LO o CM CO CM CM f

, co o cn o VO VO vo <

1— «o- co •

1— CM CM 1— CM r— CM

+1 +1 +1 +1 +i +1 +1 +1 +1 +1 +1 +1 +1 +1 +1 +1 Z o C 33

r>- co VO s: o cn oo o cn CM c LO CM CO *3- co

CM O co «o- o cn CO CO cn cn cm cn

co co CO co «3- LO LO «?r 1

co f'' rs co rs

, CM CO

LO VO vo OS r “ 1— CM 1—

o +1 -H +1 +1 +l +1 +1 -H o -Q c +-> LO VO cn CO VO Q_ VO cn O'! cn CO cn r>- o CM CM CM *3- r^» 00 3

vo co o o CM o '=7 CM CM vo LO 1— vo 07 r— 1— *“ CM CM

dl +1 +t +l +1 +1 +1 +1 +1 +1 +1 +1 +1 u_ t- 73 S-

•cr ivo 03 VO LO CM O vo O cn LO CM

CO vo cn CO CO CO o vo vO LO CO CM CM CM CM CM CM co «=r co

w vn in

QJ <3 rQ d> QJ a rQ QJ a -Q U CM r>. CO lo co co <o- cn cn VJ r%. co rv. cn ro cn o r>* co cn cn U CO PsCO CT»I

3 LO VO VO LO VO vo VO vo vo r-. n-s p»* 3 LO vo vcvoisfsrs c LO LO vo vo vo c lo LO LO VO VO vo f co

aj d) d) CD

i- LX -X O &. i. -X U 73 73 s_ d) •o s- X3 3 i- 73 73 I- 73 -C s- -X LX i- LX 73 x: s. LX -X S- i- LX 73 s- X 73

d) 03 03 X3 3 03 fO 3 c -a*. c o in CD 3 03 C c-ac ui d> 73 73 33 73 c in QJ 73 73 3 73 73 ca ji c

4- CQCOhCQCQZCQ<<UlN<Zi-i CQZ<<l^<*-t 4— CO CO CQ Z <C 4- CO ca co CO 2 < LO < OJ <D dl (D 03 * * cn Qi CXL

a> aj CM VO

CM VO CO i—

tl (I

33

C_3 o*

a) a> > >

CO (X3

a) ai

C£L Ctl <3 Q

id) - d> ro

• x: +-> +->

4-> X 73 </l

> O OJ E dJ

-i-> CO X3 QJ -f

d) *> 2"

O * c t- s- E

1—00 <3

- *3- cn on

+1 +1 +1 +1 +1 +1

r^- cn co i"*. r*^ vo

VO IX) LO VO VO VO

•I— -X Q. S- Q. <T3 O E aj in E d) 73

C d) 4-» •i— E u

73 dl OJ

c cu 03 E d)

4- i- -*-> d» 4-> -C O

73 a> >*+-> 3

dl O > -O I— o «o

* • dl 73 «/> -M O

•r* Ol -P C C C OO Ot- 3

0J <3- . >— +-> —« 0J c

r- u aj -Q i- CD « 73 73 -Q

4-

» OW-> u c c

4) -r- CD

;—x o

5- 73 i- O +-> d> C dJ > *• I CJVr- 03 <— -— O 4- 4JO r-O^ rd> -a s d> • C dl -r- </) XI CO 73

d» -t~» 03 OJ t/> * uo +-> 3 E

3 *r- 4- r- </l O" 3 O i— 0J 73 - LU VI

•r- L> > *— </> W C I d) O rtJ

<T> cn

-rl +i +i

VO VO

co r>» +i +i co

vo vo

+i +i vo o

CM VO

<3- CO

+i +1 r- O

ooCO

LD C Lf) +1 +1 +i +1 i— cn co co vo vo co *=r CM CM CM CM

CT» «=J- <3- «=r +1 +1 +1 -H ^ cji co vr CO CM CM CO CM CM CM CM

r- aj u ai u own

CJ E r- X3 -r- C

X OJ Q) 4-> CO *r- </> qj i- x: 73 <o 3 P (/I OU- 3 n OJCIOf—

7J 73 73«/>*r-Of—

d) <D 3 03 i/> O 0J Z E (O U 3 03 2

vo

CM CM

+1

-H CO

Cn CO

<3 rCj r-r-CMISCOlTCONOOrsaiO^ lOl^lfUOvOvOiOvOMxNrso

LXLXOS--XOU73S-.S-734-X3

0303X1 303 , «-U>C03‘€LCOVO

CQCQI— 0331031— < (J on < Z

3 03 C in

45

From

preliminary

stopping-power

data

of

Ishiwari,

Shiomi,

and

Sakamoto

(private

communication,

January

1982).
Table 4.3 Atomic number, weight, and mean excitation energies for elemental substances.

Unless noted otherwise, the I-values are for substances in the condensed

phase. The uncertainties AI attempt to take into account the uncertainties

of the underlying measurements, the errors inherent in the analysis of the measurements, and the dispersion of the I-values derived from various

sources. I-values in parentheses have been estimated by interpolation of

I/Z vs. Z, or by extrapolation for Z > 92.

z El ement Symbol A, a

q/mol I, eV AI, eV 1/1, eV

1 hydrogen H 1.0079

19.2 molecular gas

21 .8 liquid

0.4

1 .6 19.2

21 .8

2 hel ium He 4.00260 41 .8 gas 0.8 20.9

3 1 ithium Li 6.941 40.0 5 13.3

4 beryl 1 ium Be 9.01218 63.7 3 15.9

5 boron B 10.81 76.0 8 15.2

6 carbon C 12.011 78.0 graphite 7 13.0

7 nitrogen N 14.0067 82.0 molecular gas 2 11 .7

8 oxygen 0 15.9994 95.0 molecular gas 2 11.9

9 fluorine F 18.998403 (115) gas 11.5.

10 neon He 20.179 137 gas 4 13.7

11 sodium Na 22.98977 (149) 13.6

12 magnesium Mg 24.305 0 56) 13.0

13 aluminum ML 26.98154 166 2 12.8

14 silicon Si 28.0855 173 3 12.4

15 phosphorus P 30.97376 073) 11.5

16 sulfur S 32.06 (180) 11.3

17 chlorine C£ 35.453 (174) gas 10.2

18 argon Ar 39.948 188 gas 10 10.4

19 potassium K 39.0983 (190) 10.0

20 calcium Ca 40.08 191 8 9.6

21 scandium Sc 44.9559 216 8 10.3

22 titanium Ti 47.88 233 5 10.6

23 vanadium V 50.9415 245 7 10.7

24 chromium Cr 51 .996 257 10 10.7

25 manganese Mn 54.9380 272 10 10.9

26 i ron Fe 55.847 286 9 11.0

27 cobalt Co 58.9332 297 9 11.0

28 nickel Ni 58.69 311 10 11.1 29 copper Cu 63.546 322 10 11.1 30 zinc Zn 65.38 330 10 11 .0

31 gal 1 ium Ga 69.72 (334) 10.8

46
Table 4,,3 Continued

Z El ement Symbol !\, a

g/mol I, eV AI, eV I/Z, eV

32 germanium Ge 72.59 350 11 10.4

33 arsenic As 74.9216 (347) 10.5

34 selenium Se 78.96 (348) 10.2

35 bromine Br 79.904 (343) gas

(357) condensed

9.8 10.2

36 krypton Kr 83.80 352 gas 25 9.8

37 rubidium Rb 85.4678 (363) 9.8

38 strontium Sr 87.62 (366) 9.6

39 yttrium Y 88.9059 (379) 9.7 40 zirconium Zr 91.22 393 15 9.3

41 niobium Nb 92.9064 417 15 10.2 42 molybdenum Mo 95.94 424 15 10.1 43 technetium 98

Tc 97.907 (428) 10.0

44 ruthenium Ru 101.07 (441) 10.0

45 rhodium Rh 102.9055 449 20 10.0

46 palladium Pd 106.42 470 20 10.2

47 silver Ag 107.868 470 10 10.0

48 cadmium Cd 112.41 469 20 9.3 49 indium In 114.82 488 20 10.0

50 tin Sn 118.69 488 15 9.8

51 antimony Sb 121.75 (487) 9.5

52 tellurium Te 127.60 (485) 9.3

53 iodine I 126.9045 (474) gas

(491 ) condensed

8.9

9.3

54 xenon Xe 131 .29 482 gas 30 8.9

55 cesium Cs 132.9054 (488) 8.9

56 barium Ba 137.33 (491) 8.8

57 1 anthanum La 138.9055 (501) 8.8

58 cerium Ce 140.12 (523) 8.8

59 praseodymium Pr 140.9077 (535) 9.1 60 neodymium Nd 144.24 (546) 9.1

61 promethium 145Pm 144.913 (560) 9.2 62 samarium Sm 150.36 (574) 9.3

63 europium Eu 151 .96 (580) 9.2

64 gadol inium Gd 157.25 591 20 9.2 65 terbium Tb 158.9254 (614) 9.4

66 dysprosium Dy 162.50 (628) 9.5

67 hoi mi urn Ho 164.9304 (650) 9.7

47
Table 4. Z

.3 Continued

Element Symbol A,

a g/mol I, eV AI, eV I/Z, eV 68 erbium Er 167.26 (658) 9.7

69 thul ium Tm 168.9342 (674) 9.8

70 ytterbium Yb 173.04 (684) 9.8

71 1 utetium Lu 174.967 (694) 9.8

72 hafnium Hf 178.49 (705) 9.8

73 tantal urn Ta 180.9479 718 30 9.8

74 tungsten W 183.85 727 30 9.8

75 rhenium Re 186.207 (736) 9.8

76 osmium 0s 190.2 (746) 9.8

77 iridium Ir 192.22 757 30 9.8

78 platinum Pt 195.08 790 30 10.1 79 gold Au 196.9665 790 30 10.0

80 mercury Hg 200.59 (800) 10.0

81 thal 1 ium T2 204.383 (810) 10.0

82 lead Pb 207.2 823 30 10.0

83 bismuth Bi 208.9804 (823) 9.9

84 polonium 209PO 208.982 (830) 9.9

85 astatine ^At 209.987 (825) 9.7 86 radon

222

Rn 222.018 (794) gas 9.2

87 francium 223Fr 223.020 (827) 9°. 5 38 radium Ra 226.0254 (826) 9.4

89 actinium Ac 227.0278 (841) 9.4

90 thorium Th 232.0381 (847) 9.4

91 protactinium Pa 231.0359 (878) 9.6

92 uranium U 238.0289 890 30 9.7

93 neptunium Np 237.0482 (902) 9.7

94 plutonium 239Pu 239.052 (921) 9.8

95 americium 243

%, 243.061 (934) 9.8

96 curium 247

Cm 247.070 (939) 9.8

97 berkel ium ^Bk 247.070 (952) 9.8

98 californium 251 Cf 251.080 (966) 9.9

99 einsteinium 252Es 252.083 (980) 9.9 100 fermium 257

Fm 257.095 (994) 9.9

aThe atonic weights A are those recommended by the Commission on Atomic Weights of the International Union of Pure and Applied Chemistry (Holden, 1979). The values are for naturally occurring isotopic mixtures, unless a particular isotope is indicated.

48
Table

4.4

Comparison

of

mean

excitation

energies

for

elements

recommended

in

various

publications.

Values

are

given

in

units

of

eV.

-OQ_

CM O i— CM

co co

LO

cd OCM UD CO P"»

co cr>

r CD

CO

CO r—

CD CO

p-* r^.

co CO

CO CM

P*^ co

oco

*3-

COCO

*3*

cr» o cm o co p^ co

*3- «3*

CO LO o »—

co CO

CM CO CM CO O^i CM P^

r— i— CM r— .— CM <

CO CO CO CO CO CO CO O i— CM CO CM CM CO CO CO

COCOCO^j-COcOCM'd'

CO CO co CO co CO vO co

*=D COCD

S- ic*— O)C

TO S-

<L> 3

CO <—

P^. CO o o n co

cj co co - co

O'* co C*> r— C£> r—

r— r— O

cs cd

•r— l/i (U

o <3 — co —

o o> o co f— co

^ cd

0) Cl c

r- qj c: .c •»- <o

—

o

“O

c

O)a

-Q

CM CM CO CO O v-£

P3 II > ca

OJ PM > M •i- O CD

tO I

49
Table

5

1

Mean

excitation

energies

adopted

in

the

present

Table

5.2.

Mean

excitation

energies

for

atomic

constituents

of

condensed

work

for

atomic

constituents

of

compounds.

organic

compounds,

from

an

analysis

of

stopping-power

ratios

relative

to

copper

measured

by

Thompson

(1952).

The

analysis

assumes

I~

=

322

eV,

and

includes

multiple-scattering

corrections.

The

GASES

uncertainties

take

into

account

Thompson's

measurement

uncertainties

COocoo

o

or O

tQ

co

or ocr> to

o

+1

<3*

+1

c: o

o o

r- Q.S

•r- O

</> C_J o

Q- C

E Or

to o>

•r- r— QJ

O) </)

OJ TC

s_ s- a* QJ C to -C 4- c • 2 OJ ro

<u -a . IT C

« r— o

•H u u

> r— X I (U -Q MJQ ro cn +-> i

<— CD

• JZ c c

50

179.7
value

deduced

from

experiments.

B.

Liquid

Compounds

i— i— LO I cn CT> UD

CM LO CO ^ CO o o o o o o O O CM O

CMOOLOLOCMCMLOCO Oi 03 I— CM Oi CM CM CO O CO CT> CMOr— Of— OOO O .— CM O CO ro O CM

COCOCOOOCOCOCOCOOO*^'

+1 +1 +1 +1 +1 +1 +1 +1 +1 +1 <O<OCOCOCO<OCO<O<O<OCO<OCOCO<OC0

LO CO CX*

+1 +1 +1 +1 +1 +1 +1 +1 +1 O^LO^OLOCOLOr-CM+1 +1 +1 +1

^LOCOCTTLOCnLOLOLOCO.— O CM CM LOLOLOLrjLOCOLOLOOOr— LOLO!'''. LO LO LO LO LO LO lO LO LO

CT> CM CO LO

LO lO LO -C

zz nz zz o

CO LO LO U

OJ O) rLO (O I— <u r— r— O

-Q S_ r—

r— m o

QJ U r- I

i- <n r- TO r—O I— ra r— r— C

CM O CM

C r— <U " •— O T3 QJ co >» 4J r- MU C -PCM

H- -r- -r- TD QJ

- O L- O O

O

— <3- O O O O CM CM O O O CM

QJ LO r— OJ . 13 CO 3

S- C r—

I -r- 03 CO-O > ' CO CO I < -O QJ

S- JZ < CO QJ <

5 ••*“-0*0

QJ 2 C -

>> 3 CO O

JO r— -O u

fO QJ ** <J

+-> > C r— <0 C -r- • 3 .— co lo m

w e to co >

QJ X QJ L £ aaj

CM CM CM CM CM CM CM CM CM CM CM CM CM

CO CT» LO CM i— LO QjQjcocOLOLOcncn

<3 ^ O rQ rQ rCl ^ <3 rQ rQ rQ

CO O O O

QJ QJ QJ

E c\j o os- o

S- CL

OJ QJ TD O

X-M

QJ 3 —* JO

'— "O o

QJ 'tJ -*-J

</l CO

3 QJ

</) lO

+-> qj c s- o aj o

E i- *3* qj qj

J- 3 *o 3 O C

LO Q. CO ca i aj coo ECO•r- ro

L- CL

qj a c

2 O QJ

i/l i/l L.

•o 5 : CL C

I CO to — r— JC o

51

From

Thomas

and

Meath

(1977).
Footnotes

for

Table

5.3.

rQ

TD CU

CM i

CM US

• os +i

CSJ r—

O •

O 4-> O

CO C -M OS CU

•— E ~a

E c s_

IT3 3 (U V) Q- «+- E •*-

i— OS CU C

CU C CU 03 m -r-as

JC >>'— 00 Ur- •!-

•*- a. 03 CO "

I ro > s- -a <u

:ra >> r— -Q C O 03 03

• C CU a> co ai i3 sz zz r— M I 03 O C > O -rqj -a -a

oo c\j — a>

•r- • O 4-> > zr a.

ai o

i- cu *a E -cr 03 uo O +-> 03 s- at

C'sifl o •*- . I* (D tf)>

+->+->>, cu

03 O r— u c oj

•I- -*-» c • C O 03 *3- 3 O E 4- l- -H

0J 'm

in

cu <U cu —

, c E >

S- O <U 03

•r— -H 00 O

+-> S- -C

4— GJ I— 4-0 2

o o E

CU Cl O

OO I S- 5 03 cn4- o c •r- ai ^

•<- -o > o. <u 2 03 CL >

3 O VOS O0 Cl OS f— O

E r—

«— ai co lo r</> i— os < fOr03 cr > Z O 0) r S -r- 3

i- Q_ 4-J CL U 03

S- CU >

O Si— 4— S- 03

<U O

WO <u U 00 -c d a» U r— >

co > n os

f>. *-» i-

• U O OS

co c a. •

os c a> • u > O >CVJ 3

CL *r— m

<U oo i- 03 jc qj cu +-> a»

I— UT3 /o £

r- OS

o > • 0)

S T3 s

• VO

i- > CM

<u cu

3 T3

«/» C

CU 03

S- O cu cn 2

O +-> c

oo CU

OS -ro cu a

4-J -r- E cr

> 
 sz o •«— U S-r— C 4-» 4- O _ J- •au o

+1 +-> CL _

> 5» O C

* <U S- S- O

2: 4- CU -r-

> I X> 4-> lr-> U

. VO <U v/3 c

) CU O

. CU US o 4—

< r—o

co as vo os us

cm cm us i— vo vo

CO CNJ r— LO CO O O CM

1— 1— tj- U0 OO *3- 1—

oj E

£ tU

•r- S_

C3 +-> • •*>£/>

00 C 4- —' C

<u <u o as -c o

S- E o*. *-> a.

(U Ul OS o 1/1 «— S- -r- r— -d 0J

«3 3 S_

4-> WS >, '‘I C 03

<U CU E E

i-CU OsJ Cl US x as

<U r—

asc m

2 ’c o o

!— m

r— a. O E <

(T3 03 03 -r- C E CM S03 1— CO -+-> CU OS U

C jCr- OJ 03 C ^-"r—

a> a> E 31 >»-r- o cu to

i- X5 r— 4- C -C <U (O r

C 4-> > c

O E 00

o *r- E m

03 >,

: cm : _ . i_ cu H 4- 4- -a o o

> so > E . m <u

* «rt> -Q a <u

<u cO

ws c a» a -a >» o ss- a

cl o

CM 03 ra CM CU OO

03

S=

) a 2 os o.

- 00 r- E . r—• CU

us uo so

+1 -h +1 +r

,— LO co co

CO OO 00 CO C3 VO

+1 -H +1 +1 +1 +1

o r— cm

co us us co <3

- us us r*- vo co

r— C 03 JZ US >>, vo = 31 S- US CM o — CM O 03

US US VO

zz zz US US (U

CU <U

•r- -r- c

52

photographic

emulsion

h

331

polytetrafluoroethylene,

“Teflon,"

b

99.1
Table 5.4. Mean excitation energies, water content and other properties of selected human tissues. For the tissues labeled "ICRP" the compositions, densities and water content were taken from Tables 105 and

108 of ICRP (1975). For the tissues labeled "ICRU" the composition

was taken from ICRU (1964); because this reference does not give

other properties, the densities and water content were assumed to be the same as for corresponding ICRP soft or bone tissue.

Substance CeV)

Density

(g/cm3

) <Z/A) Water Content

(% by weight)

h

2 o 75.0 1.00 0.55509

ICRP adipose tissue 63.2 0.92 0.55847 15.3

ICRP skin 72.7 1.10 0.54933 61 .5 ICRP brain 73.3 1.03 0.55423 78.6

ICRP testes 75.0 1 .04 0.55108 80.0

ICRP blood 75.2 1.06 0.54995 80.0

ICRP lung 75.3 1.05 0.54965 78.0

ICRP skeletal muscle 75.3 1.04 0.54938 78.6

ICRP cortical bone 106.4 1.85 0.52130 15.0

ICRU striated muscle 74. 7 1.04 0.55005 78.6

ICRU compact bone 91.9 1.85 0.53010 15.0

53
Table 5.5. Recommended mean excitation energies I for compounds and mixtures of the indicated composition.

* -f Density 1 r

§ Composition

Material <Z/A> ( g/cn 3 ) (eV) Gr (constituent Z : fraction by ueight

A-150 TISSUE-EQUIVALENT PLASTIC 2

0.569051 1 .127E+00 65.1* 3 1 : 0.101327 6 = 0.775501 7 : 0.035057 8: 0.052316

9: 0.017622 20: 0.018373 ACETYLENE, 0.537680 1 . 0 97E-0 3 58.2 A 1 = 0.077618 6 : 0.922532 ADIPOSE TISSUE (ICRP)& 0.558663 9.200E-01 63 . 2 **B 1 : 0.1 1 9677 6: 0.637260 7 : 0.007970 8: 0.232333

11: 0.000500 12: 0.000020 15 : 0.000160 16: 0.000730

17: 0.001190

30= 0.000020

19: 0.000320 20: 0.000020 26 : 0.000020

AIP., DRY (NEAR SEA LEVEL ) a 0.699190 1 . 205E-03 85.7" A 6: 0.000126 7: 0.755267 8: 0.231781 18 = 0.012827 ALUMINUM OXIDE, 0.690332 3 . 970E+00 165.2* A 3: 0.670769 13 = 0.529251

B-100 BONE-EQUIVALENT PLASTIC ^0.527397 1 .650E+00 85 . 9

* *B 1 : 0.065671 6 = 0.536965 7 = 0.021500 8 = 0.032035

9= 0.167611 20: 0 .176589

BONE, COMPACT (ICRU) e 0.530103 1 .850E+00 91 . 9**B 1 = 0.063986 6 : 0.273000 7: 0.027000 8: 0.610C16

12: 0.002000 15: 0.070000 16: 0.002000 20: 0.167000

BONE, CORTICAL (ICRP)^ 0.521299 1 .350E+00 1 06 . 6

* *B 1: 0.067236 6 = 0.166330 7 = 0.061 990 8 = 0.666096

12= 0.002200 15: 0.106970 16 = 0.003150 20: 0.209930

30: 0.000100

C-552 AIR-EQUIVALENT PLASTIC^ 0.699637 1 .760E+00 86 . 8 + *B l: 0.026680 6: 0.501610 8: 0.006527 9 = 0.665209

16: 0.003973 CALCIUM FLUORIDE, CaF

2 0.686700 3 . 1 80E+00 166.0* B 9: 0.686659 20: 0.513361 CARBON DIOXIDE, C0o 0.699889 1 .862E-03 85.0* A 6= 0.272916 8 = 0.727086 CELLULOSE NITRATE,u C.H-, ,N_ „ 0.516237 1 . 690E+00 87.0 3 1: 0.029216 6: 0.271296 7: 0.121276 8: 0.578212 ’ 6 7.7 9.6 2.3 CERIC SULFATE DOSIMETER SOLUTION^ 0.552735 1 .030E+00 76 . 7

+ *A 1 : 0.107596 7: 0.000800 3: 0.876976 16: 0.016627

58= 0.002001 CESIUM IODIDE, Csl 0.615689 6.510E+00 553.1 C 53= 0.638651 55: 0.511569 ETHYLENE, C_H,

2 4 0.570337 1 . 175E-03 50.7 A l: 0.163711 6: 0.856289

FERROUS SULFATE DOSIMETER SOLUTION'2 0.553282 1 .026E+00 76 . 6 **A 1 : 0.108259 7: 0.000027 8: 0.378636 11 : 0.000022

16: 0.012968 17: 0.090036 26: 0.000056

GLASS. BOROSIL ICATE ("PYREX", CORNING 7760)1 0.697070 2.230E+00 1 36 . 0 **A 5: 0.060061 8: 0.539566 1 1 : 0.028191 13: 0.011666

16: 0.377220 19 = 0.003321 "KAPTON" POLYIMIDE FILM, (C,„H1 .N„O c ) ZZ iU 2 d n 0^512666 1 .620E+00 79.6 B 1: 0.026362 6: 0.691133 7: 0.073270 8: 0.209235 LITHIUM FLUORIDE, LiF 0.662617 2.635E+00 96.0* B 3= 0.267585 9 = 0.732615 LITHIUM TETRABORATE, Li„B,0-,

2 4 7 0.686869 2.660E+00 96.6 C 3: 0.082085 5 = 0.255630 8: 0.662235 METHANE, CH,

4 0.623360 6 . 672E-06 61.7* A 1 : 0.251306 6 = _ / 0.768696

MUSCLE, SKELETAL CICRP)^ 0.569373 1 . 060E+00 75 . 3 **A l: 0.100637 6 = 0.107830 7: 0.027680 8 = 0.756773

1i: 0.000750 12: 0.000190 15: 0.001800 16 = 0.002610

17: 0.000790

30: 0.000050

19: 0.003020 20: 0.000030 26: 0.000060

MUSCLE. STRIATED (ICRU)e 0.550051 1 .060E+00 76.7**A 1: 0.101997 6: 0.123000 7: 0.035000 8: 0.729003

11: 0.000800

19: 0.003000

12 = 0.000200 15: 0.002000 16: 0.005000

MUSCLE-EQUIVALENT LIQUID, WITH SUCROSE^ 0.568281 1.110E+00 76 . 3 **A 1: 0.098236 6 = 0.156216 7: 0.035651 8: 0.710100 MUSCLE-EQUIVALENT LIQUID. WITHOUT SUCROSE^ 0.550136 1 .070E+00 76. 2 **A 1 : 0.101969 6: 0.120058 7: 0.035651 8 = 0.762522

NYLON, TYPE 6 AND TYPE 6/6, (C.H^ON)

o 11 n 0.567902 1 . 16CE*00 63.9* A 1

: 0.097976 6: 0.636356 7: 0.123779 3: 0.161389 PARAFFIN WAX, C

25 H2 PHOTOGRAPHIC EMULSION*"

0.572768 9.300E-01 55.9 B 1: 0.168605 6: 0.851395 0.656532 3.815E+00 331 .0 » A l: 0.016100 6: 0.072261 7

:

0.019320 8: 0.066101

16: 0.001890 35: 0.369103 67: 0.676105 53: 0.003120 PLASTIC SCINTILLATOR < VINYLTOLUENE BASED)TM 0.561613 1 . 032E+00 66.7 B 1: 0.085000 6: 0.915000 POLYCARBONATE*^"MAKROLON" , ( Ci6

H i4°3) n 0.526968 1 .200E+00 73.1 B 1: 0.055691 6: 0.755751 8: 0.188758 POLYETHYLENE, (C,H,)

z 4 n 0.570337 9.600E-01 57.6* 8 1 * 0.16371 1 6: 0.856289 POLYETHYLENE TEREPTHALATE,°n MYLAR7

(

c10

H8°A^ n 0.520370 1 .600E+00 78.7 B 1 : 0.061959 6 : 0.625017 8: 0.333025 POLYMETHYL METHACRYLATE ,

P

(CgHgO^ 0.539369 1 .190E+00 76.0* A 1 : 0.080538 6: 0.599868 8: 0.319616 POLYPROPYLENE, (C,H c ) J j n 0.559985 9.000E-01 59.2 B 1: 0.122698 6‘- 0.377302 POLYSTYRENE, *7 (C„H0 ) o o n 0.537680 1 . 060E*00 68.7* A 1 : 0.077618 6 = 0.922582 POLYTETRAFLUOROETHYLENE/’ "TEFLON" , {C,F. ) z 4 n

0.679925 2.200E+00 99.1* A 6= 0.260183 9: 0.759817 POLYVINYL CHLORIDE, (C.H,CE)

2 3 n 0.512011 1 .300E+00 108.2 B 1 : 0.068380 6: 0.386360 17: 0.567260 PROPANE, C

3H

g 0.589620 1 .879E-03 67.1 A l: 0.182855 6: 0.817165 SILICON DIOXIDE, Si0

2 0.699298 2. 320E+00 139.2* A 8= 0.532565 16: 0.667635 SODIUM IODIDE, Nal 0.626963 3.667E+00 652.0 C 11: 0.153373 53: 0.866627 STILBENE, C

14 H 12 0.532597 9.707E-01 67.7 B 1: 0.067101 6 : 0.932899 TISSUE-EQUIVALENT GAS (METHANE BASED) 3 0.569927 1 . 066E-03 61.2* A 1: 0.101869 6: 0.656179 7: 0.035172 8 = 0.606780 TISSUE-EQUIVALENT GAS (PROPANE BASED)* 0.550263 1 .826E-03 59 • 5 **A I: 0.102672 6: 0.563960 7: 0.035022 8: 0.293366

TOLUENE, C

? Hg WATER. LIQUID, H„0

0.562651 8.669E-01 62.5* A 1 * 0.087510 6 = 0.912690 0.555087 1 . OOOE+OO 75.0* A 1 * 0.111896 8: 0.888106 WATER VAPOR, H 0 0.555087 7 . 562E-06 71.6* A 1 : 0.111896 8: 0.388106

54
CO o3 C\J o n:

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in ra

•r- OC OO O CM

O 0-5

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E o-^ . CO +j ID CO -C

i— r- cn O . -f-

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«—3 TO UO

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55
Table

5.6.

Comparison

of

mean

excitation

energies

for

compounds

reconmended

in

various

publications.

Values

are

given

in

eV.

-Q CO C LO

03 O'*

LO VO r— Or C\J LD i CO

•— *xT P^ VO

coZ vO

I O'! VO p— c£

COolO

VO

lO

VO UO rCO lO LO

VO VO VO

COVO

co

*oc

03 i-CJ CO CM

S= CZ VO O i-oi >

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COLO

LD

tn CM CO CT> on cn i— i cm

VO VO P*^ <T>

03 o

4-i CM

cr> 00 i

Q) - cn

03 a.

<3- oLD p^cop^p^oococoun

'd-CMcoLOunaovocM LDvOvovOvOvOCOi— co co

CO CMuo

56

Experimental

value

(see

Table

5.3).
Table 5.7. Dependence of the mean excitation energy on the state of

aggregation of the medium.

Substance Mean Excitation Energy I (eV)

Atomic Molecular

gasa gas0 Liquid0 Sol id^ Ratios

(a) (b) (c) (d) (b)/(a ) (c)/(b) (d)/(i

] H 15.0 19.2 21.8 1.28 1.14

6

C 62.0 78 1.26

7 n 76.9 82.0 90.5 1.07 1.10

8

0 93.5 95.0 104.3 1.02 1.10

13A£ 124 166 1.34

14

Si 132 173 1.32

22

Ti 182 233 1 .28

26

Fe 226 286 1.26

29

Cu 274 322 1.18

32Ge 292 350 1.20

h

2o 71.6 75.0 1.05

C^Hg, propane 47.1 52.0 1.10

C

r H 1? , pentane 48.2 53.6 1.11 hexane 49.1 54.0 1.10

CyH-jg, heptane 49.2 54.4 1.11

theoretical: from Brown (1950) for H; from Dehmer et al. (1975) for C, N,

0, A£, and Si; and from Inokuti et al. (1981) for Ti, Fe, Cu, and Ge. trom Tables 3.1, 5.3, and 5.5.

c From Tables 4.2 and 5.3. d

From Table 5.5.

57
Table

6.1

Percent

reduction

of

collision

stopping

power

due

to

density

effect

calculated

according

to

the

method

of

Sternheimer.

•r- LCi rO OCM

-o co

r- £

13 L

cr

•»- cr ^ O

O ~ CM li m oj

iCT> CM

ro

QJ

4-> •r- cnj CL o ro

s-Oi <—

!LI

CO O

co to O

o o

co co o O

r— CT LO CO i—

CM

cr> f—

cn

tO •— CM

CO CM f—

CO CM rCM CM CM CM

<o f— CO

CTT CM

ro «—

O O

to

CM CM CM CM

co

to co

CMCM

CO CO O O

CM

CO

CO CM CM

o o

O LO

r—- r**» to ro pLO CM rLO CM i

O O O

OJ TD

C

OJ “O

rO *p- cj o:

•r- CL

CL ro 20 V- I— o

a rC

58
Table

7.1.

Ratio

of

restricted

to

total

collision

stopping

power

for

electrons

Table

7.2.

Ratio

of

restricted

to

total

collision

stopping

power

for

positrons,

L~(T,A)/S‘

oi

(T).

Results

were

calculated

using

density-effect

corrections

L

+

(T,A)/S*

ol

(T).

Results

were

calculated

using

density-effect

corrections

obtained

from

Sternheimer

‘s

method.

obtained

from

Sternheimer’s

method.

r— t£> O Oi-Tn o n in

co x lo

co to O'*

i— co lo

cm *3- to CO Is* *o

LO CO LO oun a cun (x

to rx ,

*3" CO OM LO to f—

•

co x to

CO C' CM

cm *3- to

i— r~^ CON to

CO N O

CM «3" CO O CD CO

CTr X to

to <3- o CM CO CM

LO CO O or co n

CO to CO X LO .

cn co i - O *3* CM

SJ- CM o r— cm ocorx

CD <-r o cr. lo

or co OCON

O O X CO CM O 'O

CD N

O O LO O O CM o o cr. O O N

ooo ooo ooo ooo ooo ooo ooo ooo ooo O O r— O O r-OO r— r— O

co or lo cm o cr. io n rx

rx o lo

to to Mco cr. to

co CO Or rx to to ooo ooo

CO N to ooo

CTi or CM

to cm

co co co co n to N CO Mcm to or

to lo

co rx lo

I— O CM otr tr O CO X cn rx to

CO O LO

CO to to

LO CO O cr> co rx.

rx. lo cn CO CO IX.

rx. lo i

cr> co rx O LO r— o to rx O rx CM o co rx O r- rx O CTi rx O toCTi IX O O LO o o rx o cr. O O rx OOO OOO OOO OOO OOO OOO <— O O r— CD CD

CO «3- CO CO

CO CO rx to

CO LO o o <3- «3- rx lo

lo rx cri co CO CO

LO LO LO IX LO LO

CM CTi O LO

to LO

rx to

rx cm

CTi CTi co rx

rx to

r— CM

CTi CO

rx to

CO X r— CTi CO to

I— to

LO X CTi XXX X LO LO

CM CM

CTi LO CO rCO X

CM O •=3- CM

CO x

VO OM CM

in c rlo co

CO X LO

X CM x ^r

co x

CO CM •— o CO LO

CO x

CTi CTi

CTi CO

CO CO

CTi X

err CM CTi M" CTi CTi X

CM CM

CM LO X .

CTi CO

CTi I—

co to X CM

CD CO

O LO O LO O co O 00

O CO

LO

«3- CO

o o CD LO O toCO O toXCM

<Ti o o o o

r— O r— r—

OO co O co o cn

LO I— to

CM CO CTi CTi r— «3" CO x to X O to r— LO CM

CM CTi to

CD X to

CO 00 «3*

<=r «— x CD 00 LO

trm.

to CM to x M- CO

CD CO LO O O X OCVjLf O LO CD 00 LO O to o O co X

o co o O CO X

o o O CD

CD CD o o

O O LO O co O LO O O X

OOO OOO OOO OOO OOO OOO OOO OOO OOO r— CD CD r-OO

CO «3- LT) CO LO CM

LO LO X X LO LO

r- u-> co O *3" CO

CO CO 00 X LO LO 3XX co lo OOO COLO i— .— .— CO CO CM CO x to co X LO

CD CO r—

CD I— CM

LO LO 3T 00 X to

CO o o X CO LO

CD CO to

CO x LO

LO LO CO

to CO co

CM O 00

CD CO LO

CM O LO CM CM CD

LO CO CTi CD CO tO OOO OOO OOO ooo ooo ooo ooo ooo

CD CO x odd

OXO O LO LO X CM o co x

O tO X O O CO O O co

CD X

O CO CM

CO LO T to

CD X

ooo O O to O CD O O X

• O O r— O O

LO «3" «3" D LO CO

CO I— '=3- X X LO

00 x LO CO I— I

O CM LO

co x to

LO X O O X LO

CM CO LO

CO X LO

*3- O X

'T LO LO

CO lO

CO X LO O O CD

CM LO X LO LO LO

CO X LO

to O CO

CO LO LO

co x to 00 X LO

CD CO LO

*3- X X i— CD X CD X LO

LO CD r— O LO LO

LO CM CD

CD 00 LO O D X OOU3 O to CM CO X

O 00 CO O LO O O LO O CD XO LO CD O CO CO o <3- x

O CD X

O O X CD CO

CD CD CM O O CO OOO O O LO O O lO O O 00 OOO OOO OOO OOO OOO OOO OOO OOO r— o o •OO r— O O r— r— o r-r-O

r— O CD

CO *3- «3- t in lo X LO LO X X CO

.— LO CD

CD CD CD X tO LO OOO ooo ooo

CO x LO odd

to f— LO OtOrco CO

CO x MO

lO CD CO O CO to

CO to LO

CO x to O LO o LO X CO

/— CD X CD X LO

CM LO X r— CO CD

LO CM CD or co to O i— *3- O CM CD X CM

CO X

O LO D X «3- O O LO O CD XO LO CO OT<T

CD *3" CO O CD X

o o co O O X

O CM O co O O LO o o co O C to o o co ooo ooo ooo ooo • O O r— O O

«3- X CO o «— CM X LO

o CD O CM

CM CM X LO

LOCO X co co X to

*3- X O CD

<3- CO X to

LO CO

LO CO

LO LO X to

CM «3- CD LO

00 X X to

*3" CO *— co

CD X X to

X CM

53- CD LO i

CO X

O O

CM X CD X LO CM

CO X

CO LO CM CO r— CD co *3

- -cr X to LO

LO CM O cT CD 53- lO LO LO X to LO

CO LO LO CO co co

CO CO CO X to LO

CO LO <3- LO CM CO O O CD

co x lo

LO CO CD

CM CM CM

CO CM r— COX'O

LO CM

CO to

CD «3- C0 X

X <3- X LO D LO

CO X

O <3- LO X CO X O X <3- CD X LO

*3- CD X CD

CO X CD X

O O *3- CD

CD X

O CM

CM O CO O CO

O CM

CM o ^r

co

O CDLO O X o co

O *3- O CO o CO

O CM

CD ro O CM

CD O OO CD CD

CD CD

CD CD o o CD CD

CD CD

O CD O CO O CMCD O O o o ooo o ooo

«— o r— i— r— r—~ O O CM

to O X «3- <— LO cn co to O «3- •3- O X CO CD LO CD O CO LO O i— LO LO 3 O CD CJ O CO X

O O LO o X CO O co LO

CD X

OOO OOO OOO O O CO O O CD O co O O <3- o o co OOO OOO OOO OOO OOO OOO OOO OOO r-OO r— OO <— oo r- o r—r-o

CD CO CO

CO CO X CO LO X LO LO X LO CO D to CO

LO to X X to LO O LO r—

CM O CD r— r— O CO X vO

*3- CO I— X O «3- CO ro CM

CO X LO

CM tO CO X CM X to 3

O «3- CVJ LO CM CD

CD CO tO O LO CO O LO X CM CO X

O CO CD to CM O O LO O CD X

O CM 00 O «3- r—

«3- CO CD X

O O to O to O CM

00 O O LO O Xto ooo ooo ooo ooo ooo ooo ooo ooo •OO r— O O — OO r— r— O r— r— O

59
Table 8.1 Comparison of experimental and calculated collision stopping powers

in air and collodion. Results are given in units of MeV/(g cm'^).

T (keV)

Calculated Results

Experimental Results

of Cole (1969)

collodion & air5 cellulose

nitratea aira

air*

100 3.74 3.63

60 5.26 5.11 5.3 40 7.04 6.85 7.1 20 11.9 11.6 12.0

10 20.3 19.8 20.4 20

6 30.0 29.2 30.1 29

4 40.6 39.5 40.5 39

2 66.8 65.0 65.8 65

1 105 103 97.9 106 0.6 141 137 139 145 0.4 170 166 170 170 0.2 216 230

0.1 C\J 00 260 0.06 170 260 0.04 104 140 0.02 26.0 110

^According to Bethe theory, Eq (2.16). In the comparison, cellulose nitrate is considered equivalent to collodion (see footnote 18).

Green (see footnote 17).

c Cole‘s results are the same for collodion and air.
o Table 8.2 Collision stopping power, in MeV/(g cm }, for low-Z materials, calculated according to the Bethe

formula, Eq (2.16), at energies from 10 to 1 keV.

T H

? He Be C N2 0? Ne AS, Si Ar

(keV) graphite

10 51.3 22.7 18.6 20.1 20.0 19.4 17.7 16.5 16.9 15.0

8 61.5 27.1 22.2 23.9 23.7 23.0 20.9 19.4 19.9 17.6

6 77.8 34.0 27.7 29.8 29.5 28.6 25.9 23.9 24.5 21.6

5 90.2 39.2 31.9 34.3 33.9 32.7 29.5 27.2 27.9 24.6

4 108 46.7 37.8 40.5 40.0 38.6 34.6 31 .8 32.5 28.7

3 136 58.3 46.9 50.1 49.4 47.5 42.3 38.7 39.5 34.7

2 188 79.2 63.0 66.9 66.0 63.1 55.4 50.2 51 .1 44.7

1.5 235 98.0 77.2 81.6 80.3 76.5 66.2 59.6 60.5 52.7

1 321 131 102 106 104 98.6 83.4 73.8 74.8 64.7

T A- 1 50 acetylene adipose Air AS.,,0, B-100 bone bone C-552

(keV) plastic tissue

C. 0 plastic ( ICRU) ( ICRP) plastic

10 22.9 23.0 23.5 19.8 17.3 20.9 20.7 19.7 19.7

8 27.3 27.3 27.9 23.5 20.4 24.8 24.5 23.3 23.4

6 34.1 34.2 34.9 29.2 25.2 30.8 30.5 29.0 29.1

5 39.2 39.4 40.2 33.5 28.8 35.4 35.0 33.2 33.4

4 46.5 46.7 47.6 39.5 33.7 41 .8 41.2 39.0 39.5

3 57.6 58.0 59.1 48.8 41.1 51 .5 50.8 47.9 48.7

2 77.5 78.2 79.5 65.0 53.7 68.7 67.5 63.4 64.8

1.5 94.9 96.1 97.4 79.0 64.1 83.5 81 .9 76.5 78.8

1 125 127 128 103 80.3 108 106 98.0 102

T CaF, CO, cellulose ceric ethylene ferrous glass Kapton LiF

(keV) nitrate sulfate sulfate (Pyrex) solution solution

10 16.7 19.6 20.3 22.4 25.0 22.4 17.9 20.6 18.0

8 19.6 23.3 24.1 26.6 29.8 26.6 21 .1 24.5 21.3

6 24.2 29.0 30.0 33.1 37.3 33.2 26.1 30.5 26.5

5 27.5 33.3 34.4 38.0 43.0 38.1 29.8 35.0 30.4

4 32.2 39.3 40.6 45.0 51 .1 45.1 34.9 41 .4 35.8

3 39.1 48.4 50.1 55.6 63.7 55.8 42.7 51.2 44.1

2 50.7 64.4 66.8 74.4 86.1 74.6 55.9 68.3 58.6

1.5 60.2 78.2 81 .2 90.7 106 90.9 67.0 83.3 71 .0

1 74.6 101 105 118 141 119 84.5 108 91.6

T

(keV) methane muscle

(ICRP) muscle(ICRU) ME liquid

(with sucrose)

ME liquid

(without

sucrose)

nylon

type 6 paraffin

wax

plastic scintillatorpoly- carbonate

10 28.3 22.3 22.4 22.3 22.4 23.0 25.3 22.7 21.5

8 33.8 26.5 26.6 26.5 26.6 27.4 30.2 27.0 25.6

6 42.4 33.1 33.2 33.1 33.2 34.2 37.9 33.7 31.9

5 49.0 38.0 38.1 38.0 38.2 39.3 43.7 38.7 36.7

4 58.3 44.9 45.1 45.0 45.2 46.6 51.9 45.9 43.4

3 72.8 55.6 55.8 55.7 55.9 57.8 64.6 56.9 53.7

2 98.9 74.4 74.6 74.5 74.8 77.7 87.6 76.5 71.9

1.5 122 90.7 91.1 91.0 91.3 95.2 108 93.7 87.8

1 163 118 119 119 119 125 143 123 115

T poly- PMMA poly- poly- Teflon PVC propane

(keV) ethylene propylene styrene

10 24.4 22.0 23.8 22.2 18.4 19.3 26.2

8 29.1 26.1 28.4 26.4 21 .8 22.9 31 .2

6 36.4 32.6 35.5 33.0 27.1 28.4 39.2

5 41.9 37.4 40.9 38.0 31.1 32.4 45.2

4 49.7 44.3 48.5 44.9 36.6 38.2 53.7

3 61.8 54.8 60.2 55.7 45.1 46.9 66.9

2 83.3 73.4 81.1 74.7 59.8 62.0 90.7

1.5 102 89.6 99.5 91 .4 72.3 74.8 112

1 135 117 131 120 93.0 95.7 149

T SiO, stilbene TE gas TE gas toluene water water

(keV)

C. (methane (propane (liquid) vapor

based) based

)

10 17.8 22.1 23.2 23.3 22.9 22.6 22.8

8 21.0 26.3 27.6 27.8 27.2 26.8 27.1

6 26.0 32.8 34.5 34.7 34.0 33.4 33.8

5 29.6 37.7 39.6 40.0 39.1 38.4 38.8

4 34.7 44.7 47.0 47.4 46.4 45.4 45.9

3 42.4 55.4 58.3 58.9 57.6 56.2 56.9

2 55.5 74.3 78.5 79.3 77.4 75.2 76.2

1.5 66.3 90.9 96.2 97.2 94.9 91 .8 93.1

1 83.4 119 127 128 125 120 122

61
Table 9.1. Positron-to-electron ratios of radiative energy-loss cross sections

for bremsstrahl ung in the field of the screened nucleus. The six entries marked with an asterisk (*) were obtained from the results

of Feng et al. (1981) for Z = 8 and 92. The other entries were obtained by graphical interpolation and extrapolation, using a plot

of [

<

i) j-a(j] +

/['»> rad^" Vs ' 2n (T/Z 2

). The universal curve defined by

these entries was used to obtain the contribution of bremsstrahlung

in the field of the nucleus to the radiative stopping power for positrons.

T/Z2 (MeV)

r ,

(

n

) ]+/rA( n

) l- L+rad J /[<VadJ

T/Z 2 (MeV)

1 X 10- 7 0.014 1 X IO- 4 0.415

2 X lO* 7 0.030 1.56 X IO"4 0.465*

5 X io- 7 0.059 2 X io- 4 0.507

1 X io- 6 0.087 5 X io -4 0.640

1.18 X io- 6 0.094* 7.81 X io - 4 0.708*

2 X

>—

O

1 CT> 0.119 1 X io- 3 0.740

5 X IO -6 0.166 2 X IO* 3 0.816

5.91 X 10- 6 0.175* 5 X IO" 3 0.887

1 X 10- 5 0.206 7.81 X io - 3 0.916*

2 X 10- 5 0.253 1 X io - 2 0.928

5 X 10- 5 0.335 2 X io- 2 0.962

5.91 X 10- 5 0.359* 5 X io- 2 0.991

1 X 10* 1 1.000

61 a
Dependence

of

the

c.s.d.a.

range

on

the

assumed

residual

range

at1

keV.

The

quantity

given

is

the

ratio

r

7r

.

The

value

r

is

calculated

according

to

Eq

(10.2).

The

more

accurate

value

r*

i

o

o

o

o

obtained

by

computing

the

residual

range

using

stopping

powers

from

Figs.

8.1,

8.3,

or

8.5.

CO

d) -Q

62
Positron/electron

collision

stopping-power

and

c.s

.

d.a

.

-range

ratios.

Table

11.2

Comparison

of

positron/electron

collision

stopping-power

ratios

The

density-effect

correction

was

taken

from

Inokuti

and

Smith

(1982)

and

restricted-stopping-power

ratios

in

liquid

water.

Results

for

AH,

from

Ashley

(1982b)

for H

2

O,

and

was

calculated

according

were

calculated

using

density-effect

corrections

obtained

from

to

Sternheimer

1s

method

for

the

other

materials.

Sternheimer

's

method.

o cn cn o co r— co lo r—

On On On CT> cm on on <o o ononononooooo.— CO LO CO on o O r— 1—- r— 1—• f—

lo co on o r*. rs. rs on 01 ci 01 01

lo lo on on co o .— CM CO LO co cn 000

lOCVJr— r— OOOO

O O O

Eu O CJ)

I— I— OC'iCONkDsTLnCTtOkDClOkDtr cococorsrsrsNNrNrscir-fOkDcoo 01010101010101010101010000 ,

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co o cn (sid co 1— lo 1— lo 1— cm cm tr co co MCOCOtrDDDDM-CMODCOODCM ooooooooooocnanancoco •OOOOO

CO Lf) cn <tr I— IS Ol IS N LC r— LO 1— rs LO

1— r— ,— cm co co co co cm 1— cn d co 1— rs <cj- ooooooooooanananancoco

r-

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OOOOOOOLDCMf O O O O LD CM r— O LO CM p— OOOOOO

65
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to o o

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E co r> u

3 CD> CO CO CO CO 00 CO CO CO CO CO CO CO CO 3 CD> to *3- o —l <=£ u _

-3 3 QJ 3 3 OJ u u CD U (U Z CNJ CNI CNI CNJ CNJ CNI CNJ CNJ CNJ CNJ CNJ CNJ CNI (J aj s: CD cT^ fVl CD \ <D C ' QJ c - o ^ CD CD CD r— UJ LU LO LO

LU LU LO P^ LO LO

CD •• CO LO CO

• CO 00 CD CO

QJ CO c E to p^ o -3 E o O oo u t- \ o O 50 -C N 4) Ol o -3 a. CD -r- 03 tO CNI 4-> 4-> 53 tO o* cJ 3 ^ O CO -3 c

qj «=c C 03 • Q_ . to CO QJ CO «=c r— E O c c to 73

to o CJ =a: to o o 0J a> C

CN QJ 73 r— OJ a 73 73 QJ

ro a> 3= c w 03 =c >> >> 73 CO

+-> QJ 03 o QJ cu -3 f— -LJ 3 CO -o •3 c c c 3 -a 03 •<“ LO O qj QJ -C QJ OJ OJ QJ \ CL 03 QJ QJ QJ tO 3 tO O LO LO

+-> CO CL CO CO CO 03 QJ rQ 3 QJ -3 Nl 3 -3 3 C 4 > C a: co zn. zn

73 03 \ 03 3= CD -3 -3 3 03 cr QJ U QJ i

zn LO LO

21 03 03 cJ aj CU O s o <c o o C_J o o —1 CO z <3: LO —1 r— C E 33 3 «

CJ rQ Q) 4-,

•«“ C_> <TJ

CJ O f— X QJ »—

ra -r~

64
Table 11.5 Comparison of data given in earlier electron stopping-power and range tables with results of the present

work. The comparisons are presented in terms of the percent deviations of the results given by Berger

and Seltzer (1964) and of Pages et at. (1972) from the results calculated here, for the collision stopping

power, radiative stopping power, total stopping power, csda range and radiation yield.

Percent Deviations for Water

3

(liquid)

Stopping Power

Collision Radiative Total

T (MeV) 1

P B&S WT >

Pages

Is

p rad 3&S

(T)

Pages

- S(T)

P B&S Pages

0.01 2.8 2.8 30.0 29.1 2.8 2.7

0.1 2.0 1.9 22.6 25.6 2.0 1.9

1 1.7 1.6 34.9 38.1 1.9 1.9

10 1.2 2.7 0.8 -0.6 1.2 2.5

100 0.0 5.1 -1.3 2.3 -0.6 3.6 1000 0.0 -1.9 -1.7

csda Radiation

Range Yield

r0

( T ) Y(T)

B&S Pages B&S Pages

-3.1 -14.3 32.3 15.3

-2.2 -2.3 18.7 20.3

-1.9 -1.9 35.5 39.2

-1.7 -2.2 2.4 1.0 -0.2 -2.8 -0.8 -2.2

0.8 -0.3

z Density effect calculated according to Sternheimer in BSS, Pages; according to Ashley (1982b) in present work.

Percent Deviations for Air

0.01 -0.3 -0.3 28.6 27.6 -0.3 -0.3 0.3 -11 .9 35.2 16.7

0.1 -0.2 -0.2 21.0 24.2 -0.1 -0.2 0.2 0.0 20.0 21.6

1 -0.1 -0.2 34.3 38.3 0.1 0.1 0.0 -0.1 37.4 41.5

10 -0.1 -0.1 0.8 -0.7 0.0 -0.2 -0.1 0.0 4.1 3.4

100 0.7 -1.3 -1.3 2.2 -0.3 0.4 0.2 0.6 -0.9 1.3 1000 0.0 -1.9 -1.8 0.8 -0.4

Percent Deviations for Aluminum^

s

T (MeV)

Stopping Power csda Range

r

0

(T)

B&S Pages

Radiation

Yield

Y(T)

B&S Pages

Collision Kol (T >

B&S Pages

Radiative ?WT)

3&S Pages

Total ^S(T)

B&S Pages

$

0.01 0.5 -0.6 31.1 30.0 0.5 -0.6 -0.6 -13.8 40.8 22.0

0.1 0.4 -0.5 21.8 24.1 0.4 -0.5 -0.4 0.2 18.4 21.0 § 1 0.5 -0.6 38.4 41 .2 1.0 0.0 -0.9 0.1 39.6 44.2 1 10 -0.1 0.0 0.4 -1.2 0.0 -0.2 -0.3 -0.1 3.6 2.6 100 0.2 0.4 -0.1 2.8 0.0 2.0 0.0 -0.2 -0.2 0.2 1000 0.1 -0.3 -0.3 0.0 0.0

"Density effect calculated according to Sternheimer in B&S, Pages; according to Inokuti and Smith in present work.

Percent Deviations for Gold

0.01 -0.3 -0.4 115.3 104.7 0.0 -0.1 0.3 -27.3 176.7 108.7

0.1 0.0 -0.2 32.9 35.2 0.7 0.6 -0.4 -1.1 42.2 43.4

1 1.4 0.0 27.3 31.3 4.3 3.5 -3.0 -2.5 26.9 31.0

10 1.6 0.3 5.5 1.3 3.5 0.8 -4.3 -1 .2 6.2 2.1 100 0.6 0.5 1.3 2.3 1.2 2.2 -2.2 1.4 0.3 -0.5 1000 0.1 1.0 1.0 -1 .7 0.0

65
Fig. 3.1. Percent increase (decrease) of the collision stopping power for electrons

resulting from a 1-percent decrease (increase) of the mean excitation energy.

20r

18 - Curve A:

Curve B:

Calculated by Dehmer et at. (1975) for Z = 1 to 18 and

by Inokuti et al. (1981) for Z = 19 to 38 using the single-electron approximation and free-atom HartreeSlater wave functions.

Calculated by Chu and Powers (1972) and by Ziegler (1980), according to the local-plasma approximation with electronic

charge distributions derived from free-atom h'artree-Fock- Slater wave functions. Curve shown is for y

= 1 in Eq (3.3).

Calculated by Ziegler (1980) according to the local-plasma

approximation with solid-state electronic charge distributions designated by him as first-order solids (cont.). Curve is shown for y

= 1 in Eq (3.3).

30 40 50 60

ATOMIC NUMBER Z

Fig. 3.2. Theoretical mean excitation energies for elements.

66
0.35 8

z/o I

Fig.

3.4.

Shell

corrections

for

protons

as

functions

of

the

atomic

number.

The

solid

curves

represent

the

semi-empirical

shell

corrections

of

Bichsel,

and

the

dashed

curves

the

theoretical

shell

corrections

of

Bonderup

(1967).
Fig. 3.5. Semi-empirical shell corrections of Bichsel for selected elements,

as functions of the proton energy.

Fig. 4.1. Ratio of the mean excitation energy I to the atomic number Z for elements.

68
I$

69

Fig.

4.3.

Ratio

of

experimental

to

calculated

proton

stopping

powers.
1.01

1.00 -a zr <

CJ CO

Q.X

ID CO 0.99

A

ISHIWARI, SHIOM! AND SAKAMOTO - 6.5-MeV PROTONS

0,98 I I l I I I i I i I i I I I L_ 0 10 20 30 40 50 60 70 80

Fig. 4.4. Ratio of experimental to calculated proton stopping powers at 6 Experimental data are from Ishiwari (1979).

1.01 -i

i

1

i

1 r '"'i "I i

CJ

_l<

CJ CO

Io_XID CO

1.00 • •

• ••

0.99 BURKIG & MACKENZIE

19.8-MeV PROTONS

0.98 —I 1 1—1—i—I—

L

J i 1 i L

10 20 30 40 50 60 70 80

Fig. 4.5. Ratio of experimental to calculated proton stopping powers at 1 Experimental data are from Burkig and Mackenzie (1957).

5 MeV.

.8 MeV.

70
goo

i
PERCENT

CHANGE

INS

col

Fig. 6.3. Difference between the density-effect correction S DRp calculated by

Ashley (1982b) using a semi -empirical dielectric function for water,

and the corresponding value 6^^. obtained by Sternheimer 1 s method. The latter was calculated with I = 75.4 eV, to match the I-value

for water found by Ashley.

T, MeV

Fig. 6.4. Percent amount by which the electron collision stopping power in aluminum and water is changed, when the density-effect corrections

of Inokuti and Smith (1982) for aluminum and that of Ashley (1982b) for water are replaced by density-effect corrections calculated according to Sternheimer.
Fig. 8.1. Calculated electron collision stopping power below 10 keV in water. Curve 1 water vapor Berger (see footnote 16)

2 water vapor Green (see footnote 17)

3 water vapor Bethe formula, Eq (2.16), with I = 71.6 eV

4 liquid water Kutcher and Green (1976)

5 liquid water Ri tchie et al. (1978)

6 liquid water Ashley (1982a)

7 liquid water Bethe formula, Eq (2.16), with I = 75.0 eV

73
74
75
76

Fig.

9.1.

Radiative

energy-loss

cross

section

<ty^

for

bremsstrahlung

in

the

field

of

the

atomic

nucleus.

Points

below 2

MeV

are

from

the

calculations

of

Pratt

et

al.

(1977),

and

points

above

50

MeV

are

from

highenergy

theory

of

Davies,

Bethe,

and

Maximon

(1954)

and

Olsen

(1955).

Curves

are

from a

least-squares

fit

to

the

theoretical

points.
,

MeV/

(g

cm

Fig. 9.3. Comparison of theoretical radiative stopping power, calculated

according to Eq (9.1), with experimental results.

• Motz (1955) and Motz and Placious (1958), for Be, A2., and Au. A Aiginger (1966), for Al^O? and Au.

° Rester and Dance (1967), Rester and Edmonson (1972) and Rester (private communication) for A£, Cu, Sn, and Au.

77
T, MeV

Fig. 11.1 Comparison of theoretical and experimental values of the stopping

power in aluminum. Theoretical results: 1 Ashley et al. (1979)

2 Ashley et al. (1976a)

3 Ashley et al. (1975)

4 Bethe formula, Eq (2.16), with

Experimental results: o

I = 166 eV

Kalil et al. (1959)

a Ishigure et al. (1978)

T, MeV

Fig. 11.2 Comparison of theoretical and experimental values of the stopping

power in copper. Theoretical results: 1 Ashley et al. (1976a)

2 Bethe formula, Eq (2.16), with

I = 322 eV Experimental results: ° Ziemer et al. (1959)

78
MAIN STOPPING-POWER AND RANGE TABLES

Arrangement of Tables

A. Electrons in elemental substances . Data are given for electrons in the following

elemental substances, in order of increasing atomic number:

H

2

, He, Be, C (graphite), , Ne, AZ, Si, Ar , Ti, Fe, Cu, Ge , Kr, Mo, Ag,

Sn, Xe, Gd, W, Pt, Au, Pb, U.

B. Electrons in mixtures and compounds . Data are given for electrons in mixtures

and compounds , arranged in the same sequence in which they are listed in Table 5.5.

C. Positrons in selected materials . Data are given for positrons in graphite,

AH, Si, Cu, Ge , Ag , Pb, A-150 plastic, air, LiF, PMMA, Nal, TE gas (methane based),

TE gas (propane based), and water.

Content of Tables

The name of the material, the mean excitation energy I (in eV) and the density

p (in g/cm 3 ) are given at the head of each table. For gases, the densities are for

a pressure of 1 atmosphere (101.325 kPa) and a temperature of 20’°C.

The principal information in each table includes the mass collision stopping

power, 1/p S co l, the mass radiative stopping power, 1/p S racj, and the total mass stopping power, 1/p S C Qp + 1/p S racj, all in units of MeV/ (g cm' 2 ); the c.s.d.a.

range, r 0 , in units of g cm' 2

; and the radiation yield, Y. The auxiliary information given includes the density-effect correction 6, and

the ratio d(log )/d(log I), where the blank space stands for collision stopping

power, c.s.d.a. range or radiation yield. This ratio of logarithmic derivatives can

be interpreted as the percent change in the respective quantities that would result

from a 1 percent change of the mean excitation energy.

Stopping powers, ranges, and yields are expressed in exponential notation, with

the number that follows the letter E indicating powers of 10.

Accuracy

Above 100 keV, the uncertainty of the collision stopping power is estimated to be 1 to 2 percent; between 100 keV and 10 keV, the uncertainty is expected to be 2 to 3 percent in low-Z materials, and 5 to 10 percent in high-Z materials. The

uncertainty of the radiative stopping powers is estimated to be ~ 2 percent above

50 MeV, 2 to 5 percent between 50 and 2 MeV, and ~ 5 percent below 2 MeV.

Note on Treatment of Density Effect

The standard procedure used for all materials was to evaluate the density-effect

correction to the collision stopping power according to the method of Sternheimer.

Electron results using the density-effect correction of Inokuti and Smith (1982) for

aluminum, and the density-effect of Ashley (1982b) for water are also given; these

are indicated by an asterisk (*) at the head of the tables.

When comparisons are made, e.g., in terms of stopping-power ratios, between the

stopping power for water and that for other materials such as tissues, tissueequivalent materials, ferrous sulfate dosimeter solution or plastics, it is

recommended that water results with the Sternheimer density-effect correction be used

for the sake of consistency.

For graphite two tables are given: one for a graphite crystallite density of

2.265 g/cm 3

, and the other for a typical bulk density of 1.7 g/cm 3

. It is

recommended that these results be interpolated to the appropriate bulk density for

the graphite of interest.

79
ELECTRONS IN HYDROGEN

I = 19.2 eV DENSITY = 8.375E-05 g/ca 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV ca 2/g MeV ca 2/g MeV ca 2 /g g/cm 2 0.0100 5. 125E+01 9 . 702E-04 5.125E+01 1 . 076E-04 1 . 029E-05 0.0 -0.156 0.172 0.172

0.0125 4.271E+01 9 . 793E-04 4.271E+01 1 . 6 1 3E-04 1 . 242E-05 0.0 -0.151 0.166 0.166 0.0150 3 . 682E+0

1

9.881E-04 3 . 682E + 0

1

2.245E-04 1 . 450E-05 0.0 -0.147 0.161 0.161 0.0175 3.249E+01 9 . 964E-04 3.249E+01 2.970E-04 1 . 654E-05 0.0 -0.144 0.158 0.157

0.0200 2. 91 7E+01 1 . 004E-03 2.917E+01 3 . 783E-04 1 . 854E-05 0.0 -0.141 0.154 0.154

0.0250 2 . 439E+0

1

1 .01 9E-03 2.439E+01 5.667E-04 2.246E-05 0.0 -0.137 0.149 0.149

0.0300 2. 1 10E+01 1 . 034E-03 2. 1 10E + 01 7.878E-04 2 . 628E-05 0.0 -0.134 0.145 0.145

0.0350 1 . 870E+0

1

1 . 048E-03 1 .370E+01 1 .040E-03 3 . 003E-05 0.0 -0.131 0.142 0.142

0.0400 1 .687E+01 1 -061E-03 1 . 687E+0

1

1 -322E-03 3.371E-05 0.0 -0.129 0.140 0.139

0.0450 1 . 542E+0

1

1 .074E-03 1 . 542E+0

1

1 . 632E-03 3.733E-05 0.0 -0.127 0.138 0.137

0.0500 1 . 424E+0

1

1 . 088E-03 1 . 424E+0

1

1 . 970E-03 4.090E-05 0.0 -0.126 0.136 0.135

0.0550 1 . 327E+0

1

1 . 1 01 E-03 1 . 327E+0

1

2.334E-03 4 . 443E-05 0.0 -0.124 0.134 0.134

0.0600 1 . 245E+0

1

1 . 1 1 3E-03 1 . 245E+0

1

2.724E-03 4.791E-05 0.0 -0.123 0.133 0.132

0.0700 1 .1 14E+01 1 . 1 38E-03 1 . 1 14E+01 3.575E-03 5 . 475E-05 0.0 -0.121 0.130 0.130

0.0800 1 .015E+01 1 .164E-03 1 .015E+01 4.517E-03 6. 146E-05 0.0 -0.119 0.128 0.127

0.0900 9 . 367E+00 1 . 1 90E-03 9 . 368E+00 5.543E-03 6 .806E-05 0.0 -0.117 0.126 0.126 0.1000 8 . 737E+00 1 .216E-03 8 . 738E+00 6.650E-03 7.457E-05 0.0 -0.116 0.125 0.124

0.1250 7 . 590E+00 1 . 285E-0 3 7 . 592E+00 9.732E-03 9 . 050E-05 0.0 -0.113 0.121 0.121 0.1500 6.81 9E+00 1 . 357E-03 6 .820E+00 1 . 322E-02 1 .061E-04 0.0 -0.111 0.119 0.118

0.1750 6 . 266E+0 0 1 . 433E-0 3 6 . 267E+00 1 .705E-02 1 .215E-04 0.0 -0.109 0.117 0.116 0.2000 5.851 E+00 1 .51 IE-03 5.852E+00 2. 1 18E-02 1 . 367E-04 0.0 -0.108 0.115 0.115

0.2500 5 . 275E+00 1 . 677E-03 5 . 276E+00 3.021E-02 1 . 670E-04 0.0 -0.105 0.113 0.112

0.3000 4 . 898E+00 1 . 852E-03 4 . 8 99E+00 4.007E-02 1 .971E-04 0.0 -0.103 0.111 0.110 0.3500 4 . 635E+00 2.038E-03 4 . 637E+00 5 . 057E-02 2.273E-04 0.0 -0.102 0.109 0.108

0.4000 4 . 445E+00 2.232E-03 4 . 447E+00 6.159E-02 2.577E-04 0.0 -0.100 0.107 0.106 0.4500 4 . 302E + 00 2.436E-03 4 . 305E+00 7.303E-02 2.884E-04 0.0 -0.099 0.106 0.105

0.5000 4.1 93E+00 2.648E-03 4.1 96E+00 3 . 480E-02 3.1 94E-04 0.0 -0.098 0.105 0.103

0.5500 4.109E+00 2.869E-03 4.111 E+00 9.684E-02 3 . 508E-04 0.0 -0.097 0.104 0.102

0.6000 4 . 042E+00 3.096E-03 4 . 045E+00 1 .091E-01 3 . 825E-04 0.0 -0.096 0.103 0.101 0.7000 3. 945E+00 3 . 573E-03 3 . 949E+00 1 .341E-01 4.471E-04 0.0 -0.094 0.102 0.100 0.8000 3 . 883E+00 4.076E-03 3 . 887E+00 1 .597E-01 5.133E-04 0.0 -0.093 0.100 0.098

0.9000 3.842E+00 4 . 603E-03 3 . 847E+00 1 .856E-01 5.809E-04 0.0 -0.091 0.099 0.097

1 .0000 3.816E+00 5.152E-03 3.821 E+00 2. 117E-01 6.501E-04 0.0 -0.090 0.098 0.096

1 .2500 3 . 787E+00 5.614E-03 3 . 7 94E+00 2.774E-01 8.289E-04 0.0 -0.088 0.096 0.093

1 .5000 3 . 788E+00 8.190E-03 3 . 796E+00 3.433E-01 1 .016 E-03 0.0 -0.086 0.094 0.091

1 .7500 3 . 802E+00 9.862E-03 3.81 2E+00 4.090E-01 1 .209E-03 0.0 -0.085 0.093 0.089

2.0000 3 . 823E+00 1 . 162E-02 3 . 835E+00 4.744E-01 1 .409E-03 0.0 -0.083 0.091 0.088

2.5000 3 . 873E + 00 1 . 534E-02 3 . 888E+00 6 . 039E-0

1

1 . 324E-03 0.0 -0.081 0.089 0.086

3.0000 3 . 924E + 00 1 .931E-02 3. 943E+00 7.31 6E-01 2 . 257E-03 0.0 -0.079 0.088 0.084

3.5000 3 . 973E+00 2 . 348E-02 3. 997E+00 8.575E-01 2 . 703E-03 0.0 -0.078 0.086 0.082

4.0000 4 . 020E+00 2 . 782E-02 4 . 047E+00 9.818E-01 3. 162E-03 0.0 -0.077 0.085 0.081 4.5000 4.063E+00 3 . 230E-02 4 . 0 95E + 00 1 . 105E+00 3.631 E-03 0.0 -0.076 0.084 0 . 080 5.0000 4 . 1 03E+00 3.693E-02 4 . 1 40E+00 1 . 226E+00 4. 108E-03 0.0 -0.075 0.083 0.079

5.5000 4. 1 40E+00 4. 166E-02 4 . 1 82E+00 1 . 346E+00 4 . 593E-03 0.0 -0.074 0.082 0.078 6.0000 4. 175E+00 4.651E-02 4 . 222E+00 1 . 465E+00 5 . 084E-03 .0.0 -0.074 0.082 0.077 7.0000 4 . 239E+00 5.647E-02 4 . 295E+00 1 . 700E+00 6 .083E-03 0.0 -0.072 0.080 0.076 3.0000 4 . 295E+00 6 . 675E-02 4.361 E+00 1 . 93 1 E+00 7.101 E-03 0.0 -0.071 0.079 0.074

9.0000 4 . 345E+00 7.731E-02 4 . 422E+00 2 . 1 59E+00 8.133E-03 0.0 -0.070 0.078 0.073

10.0000 4.391 E+00 8.809E-02 4 . 479E+00 2. 383E+00 9. 177E-03 0.0 -0.070 0.077 0.072 12.5000 4 . 488E+00 1 -159E-01 4. 604E+00 2 . 934E+00 1 . 183E-02 0.0 -0.068 0.075 0 .070 15.0000 4 . 56 9E+00 1 . 448E-0

1

4.71 4E+00 3 . 470E+00 1 .451E-02 0.0 -0.067 0.074 0.069 17.5000 4 . 638E+00 1 . 744E-0

1

4.81 3E+00 3. 995E+00 1 . 722E-02 0.0 -0.066 0.073 0.068

20 .0000 4 . 6 98E+00 2.046E-01 4.903E+00 4.51 OE+OO 1 . 994E-02 0.0 -0.065 0.071 0.066 25.0000 4 . 799E+00 2.667E-01 5 . 065E + 00 5.513E+00 2.540E-02 0.0 -0.064 0.070 0.064

30.0000 4 . 88 1 E+00 3.305E-01 5.21 2E+00 6 . 485E+00 3.084E-02 0.0 -0.063 0.068 0.063

35.0000 4.951 E+00 3. 955E-01 5 . 347E+00 7 . 432E+00 3 . 625E-02 0.0 -0.062 0.067 0.061 40.0000 5.01 OE+OO 4.615E-01 5.471 E+00 8 . 357E+00 4.161E-02 1 . 250E-02 -0.052 0.065 0.060 45.0000 5 . 055E+00 5.283E-01 5 . 583E+00 9.261 E+00 4.693E-02 6 . 872E-02 -0.041 0.063 0.056 50.0000 5.091 E+00 5. 959E-01 5 . 686E+00 1 .015E+01 5.221E-02 1 .504E-01 -0.033 0.060 0.051 55.0000 5. 120E+00 6.640E-01 5 . 784E+00 1 . 1 02E+0

1

5.745E-02 2.452E-01 -0.027 0.058 0.047

60.0000 5. 144E+00 7. 326E-01 5 . 876E+00 1 . 188E+01 6.264E-02 3.459E-01 -0.023 0.055 0 .043

70 . 0000 5. 183E+00 8.71 3E-01 6 . 054E+00 1 . 355E+0

1

7 . 288E-02 5.514E-01 -0.017 0.050 0.036

80 . 0000 5.21 3E+00 1.011 E+00 6 . 225E+00 1 .518E+01 8.293E-02 7 .51 3E-01 -0.013 0.046 0.031 90.0000 5 . 238E+00 1 .153E+00 6.391 E+00 1 . 677E+0

1

9 . 277E-02 9.405E-01 -0.010 0.043 0.026 100.0000 5 . 259E+00 1 .295E+00 6 . 554E+00 1 .831E+01 1 . 024E-0

1

1 .1 18E+00 -0.008 0.040 0.023

1 25.0000 5.301 E+00 1 . 6 54E+0 0 6 . 955E+00 2 . 202E+0

1

1 . 255E-0

1

1 . 5 1 3E+00 -0.005 0.034 0.017

150.0000 5 . 333E+00 2.01 7E+00 7 . 350E+00 2.551 E+0

1

1 . 473E-0

1

1 . 84 9E+0 0 -0.004 0.030 0.013

175.0000 5 . 359E+00 2 . 383E+00 7 . 742E+00 2 . 882E+0

1

1 . 679E-01 2. 140E+00 -0.003 0.027 0.010 200.0000 5.381 E+00 2 . 752E+00 3 . 1 33E+00 3. 1 98E+01 1 .873E-01 2 . 396E+00 -0.002 0.024 0.C08 250.0000 5.41 7E+00 3 . 496E+00 8.913E+00 3 . 785E+0

1

2.231 E-01 2 . 828E+00 -0.001 0.021 0.006

300 . 0000 5. 446E+00 4 . 246E+00 9 . 692E+00 4 . 322E+0

1

2.552E-01 3 . 1 86E+00 -0.001 0.018 0.005

350.0000 5 . 470E+00 5.001 E+00 1 . 047E+0

1

4.81 9E+01 2 . 842E-0

1

3.489E+00 -0.001 0.016 0.004 400.0000 5.491 E+00 5 . 760E+00 1 . 1 25E+0

1

5 . 279E+0

1

3. 106E-01 3 . 753E+00 -0.001 0.015 0.003

450.0000 5 . 509E+00 6 . 522E+00 1 .203E+01 5.709E+01 3 . 347E-0

1

3. 987E+00 -0.000 0.014 0.002 500.0000 5 . 52SE+00 7 . 286E+00 1 .281E+01 6.1 1 1E+01 3 . 568E-01 4. 1 96E+00 -0.000 0.013 0.002 550.0000 5 . 540E+00 8 . 053E + 00 1 . 359E+01 6 . 490E+0

1

3.771E-01 4 . 386E+00 -0.000 0.012 0.002 600.0000 5 . 554E+00 8 . 821 E+00 1 . 438E+0

1

6 .848E+01 3.960E-01 4 . 559E+00 -0.000 0.012 0.002

700.0000 5 . 577E+00 1 . 036E+0

1

1 . 594E+01 7 . 508E+0

1

4 . 298E-0

1

4.866E+00 -0.000 0.011 0.001 800 . 0000 5 . 5 98E + 00 1 . 1 91E+01 1 -751E+01 3. 107E+01 4.592E-01 5. 132E+00 -0 .000 0.010 0.001 900.0000 5.61 6E+00 1 . 346E+0

1

1 . 908E+01 8 . 654E+0

1

4.853E-01 5 . 367E+00 -0.000 0.009 0.001 1000.0000 5 . 6 32E+00 1 . 502E+0

1

2 . 065E+0

1

9.157E+01 5.084E-01 5 . 577E+00 -0.000 0.009 0.001

30
ELECTRONS IN HELIUM

I = 41.8 eV DENSITY = 1.663E-04 g/cm 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log )/d( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV c» 2 /g MeV cm 2 /g MeV c» 2 /g g/cm 2 0.0100 2 . 267E+0

1

9.885E-04 2 . 267E+0

1

2.467E-04 2.412E-05 0.0 -0.178 0.200 0.200 0.0125 1 . 8 98E+0

1

9.941E-04 1 . 898E+0

1

3.678E-04 2.890E-05 0.0 -0.171 0.191 0.191 0.0150 1 . 642E+0

1

9.995E-04 1 . 642E+0

1

5 . 0 98E-0 4 3 . 352E-05 0.0 -0.166 0.185 0.185 0.0175 1 . 453E+0

1

1 . 005E-03 1 . 453E+0

1

6 . 720E-04 3.802E-05 0.0 -0.162 0.180 0.180 0.0200 1 . 307E+0

1

1 .010E-03 1 . 307E+0

1

8 . 537E-04 4.242E-05 0.0 -0.159 0.176 0.176 0.0250 1 . 0 97E+0

1

1 . 020E-03 1 . 097E+0

1

1 . 273E-03 5.096E-05 0.0 -0.154 0.169 0.169

0.0300 9.521 E+00 1 .029E-03 9 . 522E+00 1 . 764E-03 5. 923E-05 0.0 -0.150 0.164 0.164

0.0350 8 . 457E+00 1 . 0 39E-0 3 8 . 458E+00 2.322E-03 6.727E-05 0.0 -0.146 0.160 0.160 0.0400 7 . 642E+00 1 . 048E-0 3 7 . 643E+00 2 . 945E-03 7.51 0E-05 0.0 -0.144 0.157 0.157 0.0450 6 . 996E+00 1 . 057E-03 6 . 997E+00 3.630E-03 8 . 277E-0 5 0.0 -0.141 0.154 0.154

0.0500 6.471 E+00 1 . 066E-03 6 . 472E+00 4.374E-03 9 . 029E-05 0.0 -0.139 0.152 0.152

0.0550 6 . 035E+00 1 . 075E-0 3 6 . 037E+00 5 . 1 74E-03 9.766E-05 0 .

0

-0.138 0.150 0.150 0.0600 5 . 669E+00 1 . 084E-03 5 . 670E+00 6 .029E-03 1 . 049E-04 0.0 -0.136 0.148 0.148 0.0700 5 . 084E+00 1 .101E-03 5 . 085E+00 7.896E-03 1 .191E-04 0.0 -0.133 0.145 0.144

0.0800 4 . 638E+00 1.11 9E-03 4 . 639E+00 9 . 958E-0 3 1 . 328E-04 0.0 -0.131 0.142 0.142

0.0900 4 . 287E+00 1 . 1 38E-03 4 . 288E+00 1 . 220E-02 1 . 462E-04 0.0 -0.129 0.140 0.140 0.1000 4 . 003E+00 1 . 1 57E-03 4 . 004E+00 1 . 462E-02 1 . 593E-04 0.0 -0.128 0.138 0.138

0.1250 3 . 486E+00 1 . 207E-03 3 . 487E+00 2 . 1 34E-02 1 . 910E-04 0.0 -0.124 0.134 0.134 0.1500 3.1 37E+00 1 . 260E-03 3. 1 39E+00 2.891E-02 2.215E-04 0.0 -0.122 0.131 0.131 0.1750 2 . 887E+00 1 . 31 6E-03 2.889E+00 3 . 723E-02 2.51 IE-04 0.0 -0.119 0.129 0.128

0.2000 2 . 700E+00 1 . 375E-0 3 2.701 E+00 4.61 9E-02 2.800E-04 0.0 -0.118 0.127 0.126 0.2500 2 . 439E+00 1 . 499E-03 2.441 E+00 6 . 573E-02 3 . 363E-04 0.0 -0.115 0.124 0.123

0 . 3000 2.269E+00 1 . 6 32E-0 3 2 . 270 E+00 8 . 702E-02 3. 914E-04 0.0 -0.112 0.121 0.120 0.3500 2. 150E+00 1 . 774E-03 2.1 52E+00 1 .097E-01 4.457E-04 0.0 -0.110 0.119 0.118

0.4000 2 . 064E+00 1 . 924E-0 3 2 . 066E+00 1 .334E-01 4. 997E-04 0.0 -0.109 0.117 0.116 0.4500 2 . OOOE+OO 2.081E-03 2 . 002E+00 1 . 580E-0

1

5 . 536E-04 0.0 -0.107 0.116 0.114

0 . 5000 1 . 952E+00 2 . 245E-03 1 . 954E+00 1 . 833E-0

1

6 . 076E-04 0.0 -0.106 0.114 0.113

0.5500 1 . 914E+00 2.41 6E-03 1 .916E+00 2.092E-01 6.61 9E-04 0.0 -0.104 0.113 0.112

0.6000 1 . 884E+00 2.592E-03 1 . 887E+00 2.355E-01 7.165E-04 0.0 -0.103 0.112 0.110 0.7000 1 . 842E+00 2.961E-03 1 .845E+00 2.891E-01 8.269E-04 0.0 -0.101 0.110 0.108

0.8000 1 . 8 1 5E+00 3 . 350E-03 1 . 8 1 8E+00 3.437E-01 9.389E-04 0.0 -0.100 0.109 0.106

0.9000 1 .798E+00 3 . 757E-03 1 .801 E+00 3.990E-01 1 . 053E-03 0.0 -0.098 0.107 0.105

1 .0000 1 . 787E+00 4. 180E-03 1 .791 E+00 4 .547E-01 1 . 1 68E-03 0 .

0

-0.097 0.106 0.103

1 .2500 1 . 7 77E+0 0 5. 306E-03 1 . 782E+00 5. 947E-01 1 . 465E-03 0.0 -0.094 0.104 0.101

1 .5000 1 . 780E+00 6.51 5E-03 1 . 787E+00 7.349E-01 1 . 773E-03 0.0 -0.092 0.102 0.098

1 .7500 1 . 789E+00 7.793E-03 1 . 797E+00 8.744E-01 2.089E-03 0.0 -0.090 0.100 0.096

2.0000 1 .801 E+00 9. 132E-03 1 .81 0E+00 1 . 0 1 3E+00 2.414E-03 0.0 -0.089 0.098 0.095

2.5000 1 . 827E+00 1 . 1 96E-02 1 . 839E+00 1 . 287E+00 3.085E-03 0.0 -0.037 0.096 0.092

3.0000 1 . 854E+00 1 . 495E-02 1 .86 9E+0 0 1 . 557E+00 3.779E-03 0.0 -0.085 0.094 0.0 90 3.5000 1 .880E+00 1 .809E-02 1 .898E+00 1 .822E+00 4.491 E-03 0.0 -0.083 0.093 0.088 4.0000 1 . 903E+00 2. 134E-02 1 . 925E+00 2 . 084E+00 5.218E-03 0.0 -0.082 0.091 0.086 4.5000 1 . 925E+00 2.469E-02 1 . 950 E+00 2 . 342E+00 5. 957E-03 0.0 -0.081 0.090 0.085

5.0000 1 . 946 E+00 2.81 3E-02 1 . 974E+00 2 . 597E+00 6 . 706E-03 0.0 -0.080 0.089 0.084

5.5000 1 . 965E+00 3.165E-02 1 . 997E+00 2 . 848E+00 7.465E-03 0.0 -0.079 0.088 0.083

6.0000 1 . 983E+00 3 . 523E-02 2.01 8E+00 3 . 0 98E + 00 3.231 E-03 0.0 -0.078 0.087 0.082 7.0000 2.01 5E+00 4.260E-02 2 . 057E+00 3 . 588E+00 9.781 E-03 0.0 -0.077 0.086 0.080 8.0000 2 . 043E+00 5.018E-02 2 . 0 9 3E + 0 0 4 . 070E+00 1 . 1 35E-02 0.0 -0.075 0.084 0.079

9.0000 2.069E+00 5.793E-02 2. 126E+00 4 . 544E+00 1 . 293E-02 0.0 -0.074 0.083 0.077

10.0000 2 . 0 92E+0 0 6 . 584E-02 2. 157E+00 5.01 1E+00 1 . 453E-02 0.0 -0.074 0.082 0.076 12.5000 2.141 E+00 8.617E-02 2 . 227E+00 6.151 E+00 1 .855E-02 0.0 -0.072 0.080 0.074

15.0000 2. 182E+00 1 .071E-01 2 . 289E+00 7 . 258E+00 2 . 258E-02 0.0 -0.071 0.078 0.072

17.5000 2.216E+00 1 . 286E-0

1

2 . 345E+00 8 . 337E+00 2 . 662E-02 0.0 -0.069 0.077 0.071 20.0000 2 . 247E+00 1 . 505E-0

1

2 . 397E+00 9 . 39 1 E+00 3.064E-02 0.0 -0.068 0.075 0.069 25.0000 2 . 297E+00 1 . 952E-0

1

2 . 493E+00 1 . 1 44E+0

1

3.863E-02 0.0 -0.067 0.073 0.067

30.0000 2 . 339E+00 2.410E-01 2 . 580E+00 1 .341E+01 4.651 E-02 0.0 -0.066 0.071 0.065 35.0000 2 . 374E+00 2.875E-01 2 . 662E+00 1 .531E+01 5 . 426E-02 0.0 -0.065 0.070 0.063 40.0000 2 . 405E+00 3.346E-01 2.739E+00 1 .717E+01 6.187E-02 0.0 -0.064 0.068 0.062 45.0000 2 . 432E+00 3 . 822E-0

1

2.81 4E+00 1 . 897E+0

1

6.933E-02 0.0 -0.063 0.067 0.060 50.0000 2 . 456E+00 4.303E-01 2.836E+00 2 . 072E+0

1

7.665E-02 0.0 -0.063 0.066 0.059

55.0000 2 . 478E+00 4.786E-01 2 . 956E+00 2 . 243E+0

1

8 . 382E-0 2 0.0 -0.062 0.065 0.058 60.0000 2 . 498E+00 5 . 272E-0

1

3 . 025E+00 2.410 E+0

1

9 . 085E-02 0.0 -0.062 0.064 0.057 70.0000 2 . 533E+00 6.252E-01 3 . 1 58E+00 2 . 734E+0

1

1 . 045E-0

1

0.0 -0.061 0.062 0.055 80.0000 2 . 564E+00 7 . 239E-0

1

3 . 288E+00 3 . 044E+0

1

1 . 17SE-01 0.0 -0 . 060 0.061 0.054

90.0000 2 . 589E+00 8.231E-01 3.41 2E+00 3 . 343E+0

1

1 .301E-01 2. 142E-02 -0.048 0.059 0.051 100.0000 2.60 9E+0 0 9.229E-01 3 . 532E+00 3.631 E+0

1

1 . 423E-0

1

7.841 E-02 -0.039 0.057 0.048 125.0000 2 . 644E+00 1 . 1 74E+00 3.818E+00 4.31 1E+01 1 . 708E-0

1

2.879E-01 -0.024 0.051 0.039

150.0000 2 . 668E+00 1 . 427E+00 4 . 0 95E+0 0 4. 943E+01 1 .970E-01 5.234E-01 -0.017 0 . 047 0.032

175.0000 2 . 686E+00 1 .681 E+00 4 . 367E+00 5 . 534E+0

1

2.213E-01 7 . 535E-0

1

-0.012 0.043 0.027 200.0000 2 . 700E+00 1 . 937E+00 4 . 637E+00 6 . 090E+0

1

2.439E-01 9.696E-01 -0.009 0.039 0.023 250.0000 2 . 722E+00 2 . 45 1 E+00 5. 173E+00 7.110E+01 2.844E-01 1 . 356 E+0 0 -0.006 0.034 0.017 300.0000 2 . 738E+00 2 . 967E+00 5.705E+00 8 . 0 30 E+0

1

3.200E-01 1 . 688E+00 -0.004 0.031 0.013 350.0000 2 . 752E+00 3 . 486E+00 6 . 237E+00 8.868E+01 3.514E-01 1 . 976E+00 -0.003 0.028 0.011 400.0000 2 . 763E+00 4 . 006E+00 6 . 768E+00 9 . 637E+0

1

3 . 794E-0

1

2 . 230 E+0 0 -0.002 0.026 0.009 450.0000 2.773E+00 4 . 527E+00 7 . 300E+00 1 . 0 35E + 02 4.047E-01 2 . 457E+00 -0.002 0.024 0.007 500.0000 2.781 E+00 5.049E+00 7 . 83 1 E+00 1 . 1 01 E+02 4.275E-01 2.661 E+00 -0.002 0.023 0.006 550.0000 2 . 789E+00 5.573E+00 8 . 362E+00 1 . 1 63E+02 4.482E-01 2 . 847E+00 -0.001 0.022 0.006 600.0000 2.796E+00 6 . 097E+00 8.892E+00 1 . 22 1 E+02 4.672E-01 3.01 7E+00 -0.001 0.021 0.005 700.0000 2 . 808E+00 7 . 1 47E+00 9 . 955E+00 1 . 327E+02 5.008E-01 3.321 E+00 -0.001 0.019 0.004 800.0000 2.81 8E+00 8. 1 99E+00 1 . 102E+01 1 . 422E+02 5.297E-01 3 . 584E+00 -0.001 0.018 0.003 900.0000 2 . 828E+00 9 . 253E+00 1 . 208E+01 1 . 50 9E+02 5.547E-01 3.81 8E+00 -0.001 0.017 0.003

1 000.0000 2 . 836E+00 1 .031E+01 1 .314E+01 1 . 588E+02 5 . 768E-0

1

4 . 027E+00 -0.000 0.016 0.003 81
ELECTRONS IN BERYLLIUM

I = 63.7 eV DENSITY = 1 .348E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD C0P.R. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 1 . 862E+0

1

1 .815E-03 1 . 863E + 0

1

3.033E-04 5.437E-05 5 . 1 00 E-04 -0.193 0.219 0.218 0.0125 1 . 564E+0

1

1 .81 9E-03 1 . 564E+01 4.504E-04 6 . 483E-05 7 . 492E-04 -0.185 0.209 0.208

0.0150 1 . 356E+0

1

1 . 823E-03 1 . 356E+0

1

6 . 226 £-0 4 7 . 496E-05 1 .031 E-03 -0.179 0.201 0.201 0.0175 1 . 202E+0

1

1 . 827E-0 3 1 . 202E+0

1

8. 187E-04 8.472E-05 1 . 354E-03 -0.174 0.195 0.195

0.0200 1 . 083E+0

1

1 .831 E-03 1 . 084E+0

1

1 . 038E-03 9.41 9E-05 1 .718E-03 -0.170 0.190 0.190

0.0250 9.11 3E+00 1 .840E-03 9.1 15E+00 1 . 544E-03 1 . 125E-04 2 . 564E-03 -0.164 0.183 0.182

0.0300 7 . 923E+00 1 . 849E-03 7 . 925E+00 2.1 34E-03 1 . 300E-04 3 . 560E-03 -0.159 0.177 0.177

0.0350 7 . 047E+00 1 . 859E-03 7 . 049E+00 2 . 804E-03 1 .469E-04 4.701 E-03 -0.156 0.172 0.172

0.0400 6 . 375E+00 1 . 870E-0 3 6 . 376E+00 3.551 E-03 1 . 634E-04 5 . 978E-03 -0.153 0.168 0.168

0.0450 5.841 E+00 1 . 880E-0 3 5 . 843E+00 4.371E-03 1 . 794E-04 7 . 387E-03 -0.150 0.165 0.165

0.0500 5 . 407E+00 1 .891 E-03 5.409E+00 5.262E-03 1 . 951 E-04 8 . 920 E-0 3 -0.143 0.162 0.162

0.0550 5 . 0 47E+0 0 1 . 902E-03 5 . 049E+00 6.21 9E-03 2. 104E-04 1 . 057E-02 -0.146 0.160 0.160

0.0600 4 . 743E+00 1 .914E-03 4 . 745E+00 7.241E-03 2 . 253E-04 1 . 234E-0 2 -0.144 0.158 0.158

0.0700 4 . 257E+00 1 . 937E-03 4 . 259E+00 9.471 E-03 2 . 545E-04 1 .61 9E-02 -0.141 0.154 0.154

0.0800 3 . 887E+00 1 . 961 E-03 3 . 339E+00 1 . 1 93E-02 2.826E-04 2 . 043E-02 -0.139 0.151 0.151 0.0900 3 . 594E+00 1 . 987E-03 3 . 596E+00 1 .461E-02 3 . 1 00 E-04 2.504E-02 -0.137 0.149 0.148 0.1000 3 . 358E+00 2.01 4E-03 3 . 360E+00 1 . 749E-02 3 . 366E-04 2 . 997E-02 -0.135 0.147 0.146

0.1250 2 . 926 E+0 0 2.085E-03 2. 928E+00 2 . 549E-02 4.005E-04 4 . 354E-02 -0.131 0.142 0.142

0.1500 2.634E+00 2. 160E-03 2 . 636E+00 3.451 E-0 2 4.61 4E-04 5.858E-02 -0.128 0.139 0.138

0.1750 2 . 424E+00 2.241 E-03 2 . 426E+00 4 . 442E-02 5 . 200 E-04 7 . 478E-02 -0.126 0.136 0.136

0.2000 2 . 266E+00 2.326E-03 2.269E+00 5 . 508E-02 5.76 9E-04 9. 188E-02 -0.124 0.134 0.133

0.2500 2 . 046 E+00 2 . 507E-03 2 . 049E+00 7 . 836E-02 6 . 865E-04 1 . 280 E-0

1

-0.120 0.130 0.129

0.3000 1 . 90 1 E+00 2 . 704E-03 1 . 904E+00 1 . 037E-0

1

7 . 924E-04 1 . 658E-0

1

-0.118 0.127 0.127

0.3500 1 . 300E+00 2.914E-03 1 . 80 3E+00 1 . 308E-0

1

8.961 E-04 2.043E-01 -0.115 0.125 0.124

0.4000 1 .726E+00 3.1 37E-03 1 . 729E+00 1 .591 E-0

1

9 . 985E-04 2.432E-01 -0.114 0.123 0.122

0.4500 1 . 670E+00 3 . 372E-0 3 1 . 673E+00 1 . 385E-0

1

1 . 100E-03 2.81 9E-01 -0.112 0.122 0.120

0.5000 1 . 627 E+00 3.618E-03 1 .631 E+00 2. 188E-01 1 . 202E-03 3 . 204E-0

1

-0.110 0.120 0.118

0.5500 1 . 593E+00 3.875E-03 1 . 597E+00 2 . 498E-0

1

1 . 304E-03 3.583E-01 -0.109 0.119 0.117

0.6000 1 . 566E+00 4.1 39E-03 1 .571 E+00 2.814E-01 1 . 40 6 E-0 3 3 . 956 E-0

1

-0.108 0.118 0.116

0.7000 1 . 527E+00 4.693E-03 1 . 532E+00 3.459E-01 1 . 6 1 2E-03 4 . 632E-0

1

-0.105 0.115 0.113

0.8000 1 .501 E+00 5.277E-03 1 . 506E+00 4.11 8E-0

1

1 . 821 E-03 5.379E-01 -0.103 0.113 0.111 0.9000 1 . 483E+00 5.886E-03 1 . 489E+00 4 . 786 E-0

1

2.033E-03 6.047E-01 -0.101 0.112 0.109

1 .0000 1 .471 E+00 6 . 520E-03 1 . 477E+00 5 . 460E-0

1

2.248E-03 6 . 687E-0

1

-0.099 0.110 0.107

1 .2500 1 . 455E+00 8.201 E-03 1 . 463E+00 7. 162E-01 2 . 799E-03 8.178E-01 -0.095 0.107 0.103

1 .5000 1 . 450 E+0 0 1 . OOOE-02 1 . 460E+00 8 .873E-01 3 . 370E-03 9.534E-01 -0.090 0.104 0.100

1 .7500 1 . 451 E+00 1 . 1 90E-02 1 . 46 3E+0 0 1 . 058E+00 3.958E-03 1 . 078E+00 -0.086 0.101 0.096 2.0000 1 . 455E+00 1 . 388E-02 1 . 469E+00 1 . 229E+00 4 . 562E-0 3 1 . 1 94E+00 -0.082 0.099 0.093

2.5000 1 . 466E+00 1 . 80 6E-02 1 . 484E+00 1 . 568E+00 5.810E-03 1 . 405E+00 -0.074 0 .094 0.087

3.0000 1 . 477E+00 2.247E-02 1 . 500E+00 1 . 90 3E+00 7. 104E-03 1 . 596 E + 0 0 -0.066 0.090 0.081 3.5000 1 . 489E+00 2 . 707E-02 1 .51 6E+00 2 . 234E+00 8.434E-03 1 . 772E+00 -0.059 0.086 0.076

4.0000 1 . 499E+00 3. 182E-02 1 . 531 E+00 2 . 563E+00 9.795E-03 1 . 936E+00 -0.052 0.082 0.070

4.5000 1 . 508E+00 3.672E-02 1 . 545E+00 2 . 888E+00 1 . 1 18E-02 2 . 0 90 E+0 0 -0.045 0.078 0.065

5.0000 1 . 5 1 7E+00 4. 174E-02 1 . 559E+00 3.21 0E+00 1 . 259E-02 2 . 235E+00 -0.040 0.074 0.061 5.5000 1 . 525E+00 4.687E-02 1 . 572E+00 3 . 529E+00 1 . 402E-02 2 . 372E+00 -0.035 0.071 0.056

6.0000 1 . 532E+0 0 5.21 IE-02 1 . 584E+00 3 . 846E+00 1 . 546E-02 2 . 502E+00 -0.031 0.067 0.052

7.0000 1 . 544E+00 6 . 283E-02 1 . 607E+00 4 . 473E+00 1 . 840E-02 2 . 743E+0 0 -0.025 0.062 0.045

8.0000 1 . 555E+00 7.386E-02 1 . 628E+00 5.091 E+00 2.1 38E-02 2 . 962E+00 -0.020 0.057 0.039

9.0000 1 . 564E+00 8.51 4E-02 1 . 649E+00 5.701 E+00 2 . 439E-02 3. 161 E+00 -0.016 0.053 0.034

10.0000 1 . 572E+00 9 . 664E-02 1 . 6 6 9E+0 0 6 . 304E+00 2 . 743E-02 3 . 344E+00 -0.013 0.049 0.030

12.5000 1 . 589E+00 1 . 262E-0

1

1 . 7 1 5E+00 7 . 782E+00 3.509E-02 3 . 743E+00 -0.009 0.042 0.023

1 5.0000 1 . 602E+00 1 . 566E-0

1

1 . 759E+00 9.221 E+00 4.280E-02 4.07 9E+00 -0.006 0.036 0.018

17.5000 1 .61 3E+00 1 . 878E-0

1

1 .801 E+00 1 . 063E+01 5 . 050E-02 4 . 368E+00 -0.005 0 .032 0.014

20.0000 1 . 623E+00 2.1 94E-01 1 . 842E+00 1 . 200E+0

1

5.81 5E-02 4 . 622E+00 -0.004 0.029 0.012

25.0000 1 . 639E+00 2 . 840E-0

1

1 . 923E+00 1 .465E+01 7 . 323E-02 5.051 E+00 -0.002 0.024 0.008

30.0000 1 . 652E+00 3.499E-01 2 . 002E+00 1 . 720E+0

1

8.792E-02 5 . 404E+00 -0.002 0.021 0 .006 35.0000 1 . 663E+00 4.166E-01 2.07 9E+00 1 .965E+01 1 . 022E-0

1

5 . 705E+00 -0.001 0.018 0.005

40.0000 1 . 672E+00 4.841E-01 2. 156E+00 2.201E+01 1 . 160E-01 5 . 967E+00 -0.001 0.016 0.004

45.0000 1 . 680E+00 5 . 523E-0

1

2 . 232E+00 2 . 429E+0

1

1 . 293E-0

1

6 . 1 98E+00 -0.001 0.015 0.003

50.0000 1 . 687E+00 6.209E-01 2. 308E+00 2 . 650E+0

1

1 . 422E-0

1

6 . 406E+00 -0.001 0.014 0.003

55.0000 1 . 6 94E+00 6. 900E-01 2 . 384E+00 2 . 863E+0

1

1 . 547E-0

1

6 . 594E+00 -0.001 0.013 0.002

60 . 0000 1 . 700E+00 7.595E-01 2 . 460E+00 3.069E+01 1 . 667E-01 6 . 7 66E + 00 -0.001 0.012 0 .002 70.0000 1 .71 1 E+00 8 . 995E-0

1

2 . 6 1 0 E+0 0 3 . 464E+0

1

1 . 896E-01 7.071 E+00 -0.000 0.011 0.002

30.0000 1 . 720E+00 1 .041 E+00 2.761 E+00 3.836E+01 2. 1 1 0 E-0

1

7 . 336E+00 -0.000 0.010 0.001 90.0000 1 . 728E+00 1 . 183E+00 2.911 E+00 4. 189E+01 2.31 IE-01 7 . 570E+00 -0 .000 0.009 0.001 100.0000 1 . 735E+00 1 . 325E+00 3.061 E+00 4 . 524E+0

1

2 . 50 0 E-0

1

7 . 780E+00 -0.000 0.008 0.001 125.0000 1 . 75 1 E+00 1 . 685E+00 3 . 436E+00 5 . 295E+01 2. 926E-01 8 . 223E+00 -0.000 0.007 0.001

1 50.0000 1 . 7 6 3E+00 2 . 048E+00 3.811 E+00 5. 985E+01 3 . 296 E-0

1

8 . 587E+00 -0.000 0.006 0.001 175.0000 1 . 774E+00 2.41 2E+00 4 . 1 86 E + 0 0 6.61 1E+01 3 . 62 1 E-0

1

8 . 8 94E+00 -0.000 0.006 0.000 200.0000 1 . 783E+00 2.779E+00 4 . 56 1 E+00 7. 183E+01 3.91 0E-01 9. 160E+00 -0.000 0.005 0.000 250.0000 1 . 7 98E + 00 3.5I6E+00 5.31 4E+00 8.1 97E+01 4.401 E-0

1

9 . 605E+00 -0.000 0.005 0.000 300.0000 1 .81 1 E+00 4 . 256 E+0 0 6 . 067E+00 9 . 077E+0

1

4.805E-01 9. 969E+00 -0.000 0.004 0.000 350.0000 1 . 821 E+OO 5 . OOOE+OO 6.821 E+00 9 . 854E+0

1

5. 144E-01 1 . 028E+0

1

-0.000 0 . 004 0.000 400.0000 1 . 330E+00 5 . 746E+00 7 . 576E+00 1 . 0 55E+02 5 . 434E-0

1

1 . 054E+0

1

-0.000 0.004 0.000 450.0000 1 . 838E+00 6 . 494E+00 8 . 332E+00 1 . 1 1 3E+02 5.685E-01 1 . 078E+0

1

-0.000 0.003 0.000 500.0000 1 . 845E+00 7 . 242E+00 9 . 088E+00 1 . 175E+02 5 . 905E-0

1

1 . 0 99E+0

1

-0.000 0.003 0.000

550 . 0000 1 . 852E+00 7 . 993E+00 9 . 845E+00 1 . 228E + 0 2 6.099E-01 1.11 8E+01 -0.000 0.003 0.000 600.0000 1 -858E+00 3 . 744E+00 1 . 060E+01 1 . 277E+02 6 . 273E-0

1

1 . 1 35E+01 -0.000 0.003 0.000 700.0000 1 . 863E+00 1 . 025E+0

1

1 .212E+01 1 . 365E+02 6.571 E-0

1

1 , 1 66E+01 - 0.000 0.003 0.000 300.0000 1 . 878E+0 0 1 . 1 76E+01 1 . 364E+01 1 . 443E+02 6.818E-01 1 . 1 93E+01 - 0.000 0.003 0.000 900.0000 1 . 886E+00 1 . 327E+0

1

1 .515E+01 1 .513E+02 7.026E-01 1 .21 6E+01 - 0.000 0.003 0.000 1000.0000 1 . 893E+00 1 . 478E+0

1

1 . 6 67E+0

1

1 . 575E+02 7 . 204E-0

1

1 . 237E+0

1

- 0.000 0.002 0.000

82
ELECTRONS IN CARBON (GRAPHITE)

I = 78.0 eV DENSITY = 2 . 265E+00i g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log )/d( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2 /g MeV cra 2/g g/cm 2 0.0100 2.01 9E + 0 1 3. 150E-03 2.019E+01 2 . 820E-0 9 8 . 665E-05 2 . 766E-03 -0.200 0.229 0.228 0.0125 1 . 699E+0 1 3.161E-03 1 . 6 99E+0

1

9. 179E-09 1 . 0 36E-09 3.593E-03 -0.191 0.218 0.217

0.0150 1 .971E+01 3.168E-03 1 . 971 E+0

1

5 . 768E-09 1 . 1 99E-09 9 . 353E-03 -0.185 0.210 0.209 0.0175 1 . 305E+01 3.172E-03 1 . 305E+0

1

7 . 576E-09 1 . 355E-09 5.1 95E-03 -0.179 0.203 0.202

0 . 0200 1 . 177E+01 3.176E-03 1 . 1 77E+01 9.596E-09 1 . 506E-09 6 . 068E-03 -0.175 0.198 0.197 0.0250 9.91 1E+00 3 . 1 89E-0 3 9.91 5E+00 1 . 929E-03 1 . 7 96E-09 7 . 907E-03 -0.168 0.189 0.189 0.0300 8 . 629E+00 3. 1 99E-03 8 . 628E+00 1 . 967E-03 2.079E-09 9.869E-03 -0.163 0.183 0.182

0.0350 7 . 677E+00 3.209E-03 7 . 680E+00 2 . 582E-03 2.390E-09 1 . 1 99E-02 -0.159 0.177 0.177

0.0900 6 . 998E+00 3.215E-03 6.951 E+00 3 . 268E-03 2 . 597E-09 1 . 91 2E-02 -0.156 0.173 0.173

0 .0050 6 . 370E+00 3 . 228E-0 3 6 . 373E+00 9 . 020E-03 2.897E-09 1 .690E-02 -0.153 0.170 0.169

0.0500 5 . 8 99E + 00 3.291 E-03 5 . 902E+00 9 . 836E-03 3.090E-09 1 .879E-02 -0.150 0.166 0.166 0.0550 5.508E+00 3.255E-03 5.51 1E+00 5.71 3E-03 3.328E-09 2.1 27E-02 -0 . 1 98 0.169 0.163

0.0600 5.177E+00 3 . 270E-03 5.181 E+00 6 .650E-03 3.559E-09 2 . 389E-02 -0.195 0.151 0.161 0.0700 9.650E+00 3.303E-03 9 . 653E+00 8.691 E-0 3 9.009E-09 2. 926E-02 -0.192 0.157 0.157

0.0800 9 . 297E+00 3.337E-03 9 . 250E+00 1 . 0 99E-02 9 . 993E-09 3.500E-02 -0.139 0.159 0.153

0.0900 3 . 929E+00 3.375E-03 3 . 932E+00 1 . 339E-02 9.862E-09 9. 105E-02 -0.136 0.151 0.150 0.1000 3.671 E+00 3.919E-03 3 . 675E+00 1 . 603E-02 5.270E-09 9.738E-02 -0.133 0.198 0.198

0.1250 3.201 E+00 3 . 523E-03 3 . 205E+00 2 . 339E-02 6 . 296E-09 6 . 929E-02 -0.128 0.192 0.192

0.1500 2 . 883E+00 3.690E-03 2 . 887E+00 3. 158E-02 7. 173E-09 8 . 253E-02 -0.129 0.138 0 . 1 37 0.1750 2 . 659E+00 3.769E-03 2 . 658E+00 9 . 062E-02 8.061E-09 1 .01 9E-01 -0.120 0 . 1 39 0.139 0.2000 2 . 982E+00 3.896E-03 2 . 986E+00 5 . 036E-02 8.91 9E-09 1 . 221 E-0

1

-0.116 0.131 0.130 0.2500 2 . 29 1 E+0 0 9.179E-03 2 . 295E+00 7.160E-02 1 . 056E-03 1 . 699E-0

1

-0.110 0.126 0.125

0.3000 2 . 083E+00 9 . 989E-0 3 2 . 087E+00 9 . 979E-02 1 -215E-03 2.086E-01 -0.105 0.121 0.120 0.3500 1 . 972E+00 9 .820E-03 1 . 977E+00 1 . 1 99E-01 1 .369E-03 2 . 537E-0

1

-0.100 0.117 0.116 0.9000 1 .891 E+00 5.173E-03 1 .896E+00 1 .952E-01 1 . 521 E-0 3 2.992E-01 -0.096 0.119 0.112 0.9500 1 . 830E+00 5.595E-03 1 . 835E+00 1 .721 E-0

1

1 .671E-03 3.997E-01 -0.092 0.111 0.108

0.5000 1 . 782E+00 5.935E-03 1 . 788E+00 1 . 997E-0

1

1 .821 E-0 3 3.899E-01 -0.089 0.108 0.105 0.5500 1 . 795E+00 6 . 390E-03 1 . 752E+00 2.279E-01 1 .971E-03 9.397E-01 -0.086 0.105 0.102 0.6000 1 . 71 6E+00 6.759E-03 1 . 722E+00 2.567E-01 2.121 E-0 3 9 . 788E-0

1

-0.089 0.103 0.100 0.7000 1 . 672E+00 7 . 637E-03 1 . 680E+00 3.1 56E-01 2.923E-03 5.698E-01 -0.079 0.099 0.095

0.8000 1 . 693E+00 8.559E-03 1 . 651 E+00 3 . 757E-0

1

2 . 728E-03 6.976 E-01 -0.076 0.095 0.091 0.9000 1 . 623E+00 9.523E-03 1 . 632E+00 9.366E-01 3 . 037E-03 7.272E-01 -0.073 0.092 0.088

1 .0000 1 . 6 0 9E+00 1 . 053E-02 1 .61 9E+00 9.981 E-0

1

3.350E-03 8.039E-01 -0.070 0.090 0.085

1 .2500 1 . 5 90E+0 0 1 . 3 1 8E-02 1 . 603E+00 6.539E-01 9. 151E-03 9.803E-01 -0.065 0.089 0.078

1 .5000 1 . 589E+00 1 . 602E-02 1 . 600E+00 8.096E-01 9. 978E-03 1 . 1 90E+00 -0.062 0.080 0.079

1 .7500 1 . 589E+00 1 .901E-02 1 . 603E+00 9.657E-01 5.828E-03 1 . 285E+00 -0.059 0.077 0.070 2.0000 1 . 587E+00 2.21 3E-02 1 . 6 0 9E+0 0 1 .121 E+00 6 . 700E-03 1 . 9 1 7E+00 -0.057 0.079 0.067

2.5000 1 . 598E+00 2 . 870E-02 1 . 627E+00 1 . 930E+00 8.997E-03 1 .651 E+00 -0.059 0.070 0.062

3.0000 1.61 1 E+0 0 3.561E-02 1 . 696E+00 1 . 736E+00 1 . 0 35E-02 1 . 859E + 00 -0.051 0.067 0.059

3.5000 1 . 623E+00 9.281E-02 1 . 666E+00 2 . 0 38E+0 0 1 . 225E-02 2 . 0 33E+00 -0.099 0.069 0.056

<*.0000 1 . 636E+00 5 . 026E-02 1 . 686E+00 2 . 336E+00 1 .91 9E-02 2 . 1 99E+00 -0.097 0.062 0.059

<*.5000 1 . 697E+00 5.792E-02 1 . 705E+00 2.631 E+00 1 .616E-02 2 . 390E+00 -0.095 0.060 0.052

5.0000 1 . 658E+00 6 . 576E-02 1 . 723E+00 2 . 923E+00 1 .815E-02 2 . 979E+00 -0.093 0.058 0.050

5.5000 1 . 667E + 00 7 . 378E-02 1 . 79 1 E+00 3.21 1 E+00 2.016E-02 2 . 598E+00 -0.092 0.057 0.098 6.0000 1 . 676E+00 8.1 93E-02 1 . 758E+00 3 . 997E+00 2.21 9E-02 2.71 3E+00 -0.090 0.055 0.097

7.0000 1 . 6 9 3E+00 9 . 865E-02 1 .791 E+00 9.061 E+00 2 . 628E-02 2. 929E+00 -0.037 0.053 0.099

8.0000 1 . 707E+00 1 .158E-01 1 .823E+00 9.61 9E+00 3.091 E-02 3.11 9E+00 -0.033 0.050 0.091 9.0000 1 . 7 1 9E + 00 1 . 339E-0

1

1 . 853E+00 5 . 1 58E+00 3.956E-02 3 . 287E+00 -0.030 0.098 0.039

1 0 .0000 1 . 730E+0 0 1 .51 3E-01 1 .881 E+00 5 . 6 99E+0 0 3 . 872E-02 3 . 996E+00 -0.028 0.096 0.036 12.5000 1 . 753E+00 1 . 971 E-01 1 . 950 E+00 6 . 999E+00 9.91 9E-02 3 . 798E+00 -0.022 0.092 0.031 15.0000 1 . 77 0E + 00 2.999E-01 2.01 5E+00 8 . 260E+00 5.999E-02 9.101 E+00 -0.017 0.038 0.027

17.5000 1 . 785E+00 2.927E-01 2 . 077E+00 9 . 982E+00 6 . 973E-02 9 . 367E+00 -0.019 0.035 0.023 20.0000 1 . 797E+00 3.91 7E-0

1

2.1 39E+00 1 . 067E+0

1

7.981 E-02 9 . 609 E+00 -0.011 0.032 0.020 25.0000 1 .81 6E+00 9.917E-01 2 . 258E+00 1 . 299E+0

1

9. 993E-02 5.01 2E+00 -0.008 0.028 0.016 30.0000 1 . 832E+00 5.935E-01 2 . 375E+00 1 .510 E+0

1

1 . 1 83E-01 5 . 353E+00 -0.005 0.029 0.012

35.0000 1 . 895E+00 6.966E-01 2.991 E+00 1 .716E+01 1 .363E-01 5 . 696E+00 -0.009 0.022 0.010

<*0.0000 1 . 856E+00 7.508E-01 2 . 606E+00 1 . 91 2E+01 1 . 535E-0

1

5 . 902E+00 -0.003 0.020 0.008

<*5.0000 1 . 865E+00 8.559E-01 2.721 E+00 2. 100E+01 1 .699E-01 6 . 1 30E+00 -0.003 0.018 0.007 50.0000 1 .879E+00 9.617E-01 2 . 835E+00 2 . 280E+0

1

1 . 856 E-0

1

6 . 335E+00 -0.002 0.017 0 . 006 55.0000 1 .881 E+00 1 . 068E+00 2 . 999E+00 2 . 952E+0

1

2.007E-01 6.521 E+00 -0.002 0.016 0.005

60.0000 1 . 888E+00 1 . 1 75E+00 3 . 063E+00 2.61 9E+01 2. 150E-01 6 .691 E+00 -0.002 0.015 0.005 70.0000 1 . 900E+00 1 . 391 E+00 3.291 E+00 2 . 939E+0

1

2.920 E-0

1

6 . 999E+00 -0.001 0.013 0.009 80.0000 1 .91 1E+00 1 . 608E+00 3.51 9E+00 3 . 227E+0

1

2.667E-01 7 . 258E+00 -0.001 0.012 0 .003 90.0000 1 . 920E+00 1 . 826E+00 3 . 796E+00 3 . 503E+0

1

2.896E-01 7.991 E+00 -0.001 0.011 0.003 100.0000 1 . 928E+00 2 . 096 E+0 0 3. 979E+00 3 . 762E+0

1

3. 108E-01 7 . 6 99E+00 -0.001 0.011 0.002

125.0000 1 . 995E+00 2 . 598E+00 9 . 599E+00 9 . 350E+01 3.575E-01 8 . 1 92E+00 -0.000 0.009 0.002

150.0000 1 . 960E+00 3 . 1 55E+00 5.11 5E+00 9 . 868E+0

1

3.971 E-0

1

8 . 505E+00 -0.000 0.008 0.001 175.0000 1 . 972E+00 3.71 9E+00 5 . 686 E+00 5.331 E+0

1

9.312E-01 8.81 1 E+00 -0.000 0.008 0.001 200.0000 1 . 982E+00 9 . 276E+00 6 . 258E+00 5 . 750E+01 9.609E-01 9 . 077E+00 -0.000 0.007 0.001 250.0000 1 . 999E+00 5 . 905E+00 7 . 905E+00 6 . 989E+0

1

5. 1 03E-01 9 . 522E+00 -0.000 0.006 0.001 300.0000 2.01 3E+00 6 . 590E+00 8 . 553E+00 7. 1 12E+01 5.999E-01 9 . 886E+00 -0.000 0.006 0.001 350.0000 2 . 025E+00 7 . 678E+00 9.703E+00 7 . 66 0 E+0

1

5.826E-01 1.01 9E+01 -0.000 0.005 0.000 900.0000 2 . 0 35E+00 8 . 820E+00 1 . 035E+0

1

8. 197E+01 6 . 1 01 E-01 1 . 096E+01 -0.000 0.005 0.000

<*50.0000 2 . 099E+00 9. 969E+00 1 . 20 1 E+0

1

8 . 585E+0

1

6 . 335E-01 1 . 070E+01 -0.000 0.005 0.000 500.0000 2 . 052E+0 0 1.11 1 E+0

1

1 .316E+01 8 . 983E+0

1

6 .539E-01 1.091 E+0

1

-0.000 0.005 0.000 550.0000 2 . 06 0E+00 1 . 226E+0

1

1 . 9 32E+0

1

9 . 397E+0

1

6.718E-01 1 .1 10E+01 -0.000 0.009 0.000 600.0000 2 . 066E+00 1 . 390E+01 1 . 597E+0

1

9.683E+01 6.876 E-0

1

1 . 1 27E+0

1

-0.000 0.009 0.000 700.0000 2 . 078E+00 1 . 570E+0

1

1 . 778E+01 1 . 029E+02 7. 199E-01 1 . 1 58E+0

1

-0.000 0.009 0 .000 800.0000 2 . 088E+00 1 . 80 1 E+0

1

2.010E+01 1 .081 E+02 7.363E-01 1 . 185E+01 -0.000 0.009 0.000 900.0000 2 . 0 97E+00 2.031 E+0

1

2.291 E+0

1

1 . 128E+02 7.596E-01 1 . 208E+0

1

-0.000 0.009 0.000 1000.0000 2.1 06E+00 2 . 262E+0

1

2 . 973E+0

1

1 . 171E+02 7.703E-01 1 . 229E+0

1

- 0.000 0.009 0.000

83
ELECTRONS IN CARBON (GRAPHITE)

i

I = 78.0 eV DENSITY = 1 . 700E+001 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log1 )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm z/g MeV cm z/g MeV cra z/g g/cm z 0.0100 2.014E+01 3. 150E-03 2.014E+01 2 . 820E-04 8 . 665E-05 1 . 920E-03 -0.200 0.229 0.228

0.0125 1 . 6 94E+0

1

3. 161E-03 1 . 6 95E+0

1

4. 179E-04 1 . 036E-04 2.481E-03 -0.191 0.213 0.217

0.0150 1 .471E+01 3.168E-03 1 .471E+01 5 . 767E-04 1 . 1 99E-04 3.073E-03 -0.185 0.210 0.209 0.0175 1 .305E+01 3. 172E-03 1 .305E+01 7.575E-04 1 . 355E-04 3.695E-03 -0.180 0.203 0.202

0.0200 1 . 1 77E+0

1

3. 176E-03 1 . 1 77E+0

1

9 . 595E-04 1 . 506E-04 4 . 347E-03 -0.176 0.198 0.197

0.0250 9.91 3E+00 3. 184E-03 9.91 6E+00 1 . 424E-03 1 .796E-04 5.736E-03 -0.169 0.189 0.189

0.0300 8 . 626E+00 3.1 94E-03 8 . 629E+00 1 . 966E-03 2 . 073E-04 7.236E-03 -0.164 0.133 0.183

0.0350 7 . 679E+00 3 . 204E-03 7 . 682E+00 2.582E-03 2.340E-04 8.843E-03 -0.160 0.178 0.177

0 . 0400 6 . 950E+00 3.215E-03 6 . 953E+00 3.267E-03 2.597E-04 1 . 055E-02 -0.156 0.174 0.173

0 . 0450 6 . 372E+00 3 . 228E-0 3 6 . 375E+00 4.01 9E-03 2 . 847E-04 1 . 236E-02 -0.153 0.170 0.170

0.0500 5.901 E+00 3.241E-03 5. 904E+00 4.835E-03 3.090E-04 1 . 425E-02 -0.151 0.167 0.167

0.0550 5 .51 0E+00 3 . 255E-03 5.51 3E+00 5.712E-03 3 . 327E-04 1 . 624E-02 -0.149 0.164 0.164

0.0600 5. 179E+00 3 . 270E-03 5. 183E+00 6.648E-03 3 . 558E-04 1 . 832E-02 -0.147 0.162 0.162

0.0700 4 . 652E+00 3.303E-03 4 . 655E+00 8.688E-03 4 . 008E-04 2.271 E-02 -0.143 0.158 0.158

0.0800 4 . 249E+00 3 . 337E-03 4 . 253E+00 1 . 0 94E-02 4.441E-04 2 . 740E-02 -0.140 0.154 0.154

0.0900 3.931 E+00 3 . 375E-03 3 . 935E+00 1 . 339E-02 4 . 860E-04 3 . 237E-02 -0.137 0.152 0.151 0.1000 3 . 674E+00 3.414E-03 3 . 677E+00 1 . 602E-02 5.268E-04 3 . 760E-0 2 -0.135 0.149 0.149

0.1250 3 . 204E+00 3 . 523E-03 3 . 207E+00 2 . 333E-02 6 . 243E-04 5.166E-02 -0.130 0.144 0.143

0.1500 2.886E+00 3.640E-03 2 . 8 90E+0 0 3.156E-02 7 . 1 68E-04 6.694E-02 -0.126 0.140 0.139

0.1750 2 . 657E+00 3.764E-03 2.661 E+00 4 . 059E-02 8 . 055E-04 8 . 320E-02 -0.123 0.136 0.136

0.2000 2 . 485E+00 3 . 896E-0

3

2 . 489E+00 5.032E-02 8.911E-04 1 .003E-01 -0.120 0.133 0.133

0.2500 2 . 245E+00 4.179E-03 2 . 249E+00 7. 152E-02 1 . 055E-03 1 .363E-01 -0.115 0.129 0.128

0.3000 2 . 087E+00 4.489E-03 2 . 092E+00 9.462E-02 1 .21 3E-03 1 . 740E-0

1

-0.110 0.125 0.123

0.3500 1 . 977E+00 4.820E-03 1 . 981 E+00 1 .192E-01 1 .367E-03 2.129E-01 -0.106 0.121 0.120

0.4000 1 . 896E+00 5. 173E-03 1 . 90 1 E+00 1 . 450E-0

1

1 .518E-03 2 . 524E-0

1

-0.102 0.118 0.116

0 . 4500 1 . 835E+00 5.545E-03 1 . 841 E+00 1 .718E-01 1 . 668E-03 2. 922E-01 -0.099 0.115 0.113

0.5000 1 . 788E+00 5.935E-03 1 . 7 94E+00 1 . 993E-0

1

1 . 8 1 7E-03 3.321E-01 -0.095 0.113 0.110 0.5500 1 . 752E+00 6 . 340E-03 1 . 758E+00 2 . 274E-01 1 . 966E-03 3.71 9E-01 -0.092 0.110 0.108

0.6000 1 . 722E+00 6 . 759E-03 1 . 729E+00 2.561E-01 2.11 5E-03 4.114E-01 -0.090 0.108 0.105

0.7000 1 . 6 7 9E+00 7 . 637E-03 1 . 687E+00 3.147E-01 2.416E-03 4.891 E-0

1

-0.085 0.104 0.101 0.8000 1 . 650E+00 8 . 559E-03 1 . 659E+00 3.745E-01 2.71 9E-03 5 . 648E-01 -0.081 0.101 0.096

0.9000 1 .631 E+00 9 . 523E-03 1 . 640E+00 4 . 352E-0

1

3 . 026E-03 5 .382E-01 -0.077 0.098 0.093

1 .0000 1 . 6 1 7E+00 1 . 053E-02 1 . 627E+00 4.964E-01 3.337E-03 7.091 E-0

1

-0.074 0.095 0.090

1 .2500 1 . 599E+00 1 . 31 8E-02 1 . 6 1 2E+00 6.509E-01 4.1 33E-03 8 . 756 E-0

1

-0.069 0.089 0.083

1 .5000 1 . 593E+00 1 . 602E-02 1 609E+00 8.062E-01 4.954E-03 1 . 02SE+00 -0.064 0.085 0.078

1 .7500 1 .594E+00 1 .901E-02 1 .61 3E+00 9.614E-01 5.799E-03 1 . 1 67E+00 -0.061 0.081 0.073

2.0000 1 . 597E+00 2.21 3E-02 1 .61 9E+00 1 .1 1 6E+00 6 . 665E-03 1 . 295E+00 -0.059 0.078 0.070 2.5000 1 . 608E+00 2 . 870E-02 1 . 6 37E+00 1 . 423E+00 8.450E-03 1 . 522E+00 -0.055 0 .073 0.065

3.0000 1 .621 E+00 3.561E-02 1 . 6 57E+00 1 . 727E+00 1 . 029E-02 1 . 720E+00 -0.052 0.069 0.061 3.5000 1 . 634E+00 4.281E-02 1 . 677E+00 2 . 027E+00 1 -218E-02 1 .894E+00 -0.050 0.067 0.058

4.0000 1 . 647E+00 5 . 026E-02 1 . 6 97E+00 2 . 323E+00 1 .41 0E-02 2.051 E+00 -0.048 0.064 0.055

4.5000 1 . 658E+00 5.792E-02 1 . 7 1 6E+00 2.61 6E+00 1 . 606E-02 2.1 93E+00 -0.047 0.062 0.053

5.0000 1 . 66 9E+00 6 .576E-02 1 . 735E+00 2 . 906E+00 1 . 803E-02 2 . 323E+00 -0.045 0.060 0 .051 5.5000 1 . 679E+00 7 . 378E-02 1 . 753E+00 3.1 93E+00 2 . 003E-02 2 . 443E+00 -0.044 0.059 0.050 6.0000 1 . 689E+00 8. 1 93E-02 1 .771 E+00 3 . 476E+00 2 . 204E-02 2.555E+00 -0.042 0 .057 0.048

7.0000 1 . 706E+00 9.865E-02 1 . 804E+00 4 . 036E+00 2.61 0E-02 2 . 758E+00 -0.040 0.055 0.046 8.0000 1 . 720E+00 1 . 1 58E-0

1

1 . 836 E+00 4 . 585E+00 3 . 020E-02 2. 939E+00 -0.037 0.053 0.043

9.0000 1 . 733E+00 1 . 334E-0

1

1 .867E+00 5. 125E+00 3.432E-02 3 . 1 04E+00 -0.035 0.051 0.041 10.0000 1 . 745E+00 1 .513E-01 1 .396E+00 5 . 657E+00 3 . 845E-02 3 . 256E+00 -0.032 0 .049 0.039

12.5000 1 .769E+00 1 .971E-01 1 . 966E+00 6 . 952E+00 4.877E-02 3.591 E+00 -0.027 0.045 0.035

15.0000 1 . 787E+00 2.444E-01 2 . 032E+00 8 . 202E+00 5 . 903E-02 3 . 879E+00 -0.022 0.041 0.031 17.5000 1 .803E+00 2.927E-01 2 . 0 95E+0 0 9.41 4E+00 6 . 918E-02 4 . 1 33E+00 -0.018 0.038 0.027

20 . 0000 1 . 8 1 6 E + 0 0 3.417E-01 2. 157E+00 1 . 059E+0

1

7.917E-02 4.361 E+00 -0.015 0.035 0.024

25.0000 1 -836E+00 4.417E-01 2 . 278E+00 1 . 284E+0

1

9.861E-02 4 . 755E+00 -0.011 0.031 0.019

30.0000 1 . 852E+00 5.435E-01 2. 396E+00 1 . 498E+0

1

1 .173E-01 5 . 083E+00 -0.008 0 .023 0.016 35.0000 1 . 865E+00 6.466E-01 2.51 2E+00 1 . 702E+0

1

1 .351E-01 5 . 376E+00 -0.006 0.025 0.013

40.0000 1 . 877E+00 7 . 508E-0

1

2 . 627E+00 1 . 897E+0

1

1 . 522E-0

1

5 . 6 28E + 0 0 -0.005 0.023 0.011 45.0000 1 . 886E+00 8.559E-01 2 . 742E+00 2 . 083E+0

1

1 . 685E-0

1

5 . 854E+00 -0.004 0.021 0.009

50.0000 1 . 895E+00 9.617E-01 2 . 857E+00 2.262E+01 1 .841E-01 6 . 057E+00 -0.003 0.020 0.008

55.0000 1 . 90 3E + 00 1 . 068E+00 2.971 E+00 2 . 433E+0

1

1 .991E-01 6.241 E+00 -0.003 0.018 0.007

60.0000 1 . 91 OE+OO 1 . 1 75E+00 3 . 085E+00 2 . 598E+0

1

2.1 33E-0

1

6.411 E+00 -0 . 002 0.017 0.006 70.0000 1 . 922E+00 1 .391E+00 3.31 3E+00 2.91 1E+01 2.401E-01 6.71 2E+00 -0.002 0.016 0.005

80.0000 1 . 932E+00 1 . 608E+00 3.541 E+00 3.203E+01 2.648E-01 6 . 974E+00 -0.001 0.014 0.004

90.0000 1 . 942E+00 1 . 826E+00 3 . 768E+00 3 . 477E+0

1

2 . 875E-0

1

7 . 206E+00 -0.001 0.013 0.004

100.0000 1 . 950E+00 2 . 046E+00 3 . 996E+00 3 . 735E+0

1

3.087E-01 7.41 5E+00 -0.001 0.012 0.003

125.0000 1 . 967E+00 2 . 598E+00 4 . 566E+00 4.31 9E+01 3.553E-01 7 . 857E+00 -0.001 0.011 0.002

150.0000 1 . 982E+00 3.1 55E+00 5. 136E+00 4.835E+0! 3. 948E-01 8.21 9E+00 -0.000 0.010 0 .002 175.0000 1 . 993E+00 3.71 4E+00 5 . 708E+00 5 . 297E+0

1

4.283E-C1 8 . 525E+00 -0.000 0.009 0.001 200.0000 2.004E+00 4 . 276E+00 6 . 280E+00 5.714E+01 4.585E-01 8.791 E+00 -0.000 0.008 0.001 250.0000 2.021 E+00 5.405E+00 7 . 426E+00 6 . 446E+0

1

5.080E-01 9 . 236E+00 -0.000 0 .007 0.001 300.0000 2 . 035E+00 6 . 540E+00 8 . 575E+00 7 . 072E+0

1

5.476E-01 9 . 599E+00 -0.000 0.007 0.001 350.0000 2 . 047E+0 0 7 . 678E+00 9 . 725E+00 7.619E+01 5.804E-01 9 . 907E+00 - 0.000 0.006 0.001 400.0000 2 . 057E+00 8 . 820E+00 1 . 088E+0

1

8. 105E+01 6.079E-01 1 .017E+01 - 0.000 0.006 0.001 450.0000 2. 066E+00 9. 964E+00 1 .203E+01 8 . 542E+0

1

6.314E-01 1 .041E+01 - 0.000 0.005 0.000 500.0000 2.074E+00 1 . 1 1 1 E+01 1 .318E+01 8 938E+01 6 .51 9E-01 1 . 062E+0

1

-0 . 000 0.005 0.000 550.0000 2 . 082E+00 1 . 226E+0

1

1 . 434E+0

1

9.302E+01 6 .698E-01 1 .081E+01 - 0.000 0.005 0.000 600.0000 2 . 088E+00 1 . 340E+01 1 . 549E+0

1

9 . 637E+0

1

6 .856E-01 1 . 0 93E+0

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- 0.000 0.005 0.000 700.0000 2. 100E+00 1 . 570E+0

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1 . 780E+0

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1 . 024E+02 7.125E-01 1 . 1 29E+0

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- 0.000 0.005 0.000 800.0000 2. 1 1 0 E+OO 1 .801 E+01 2.012E+01 1 . 077E+02 7.346E-01 1 . 156E+01 - 0.000 0 . 004 0.000 900.0000 2 . 1 20E+00 2.031 E+01 2 . 243E+0

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1 . 1 24E+02 7 . 530E-0

1

1 . 179E+01 - 0.000 0.004 0.000 1000.0000 2. 128E+00 2 . 262E+0

1

2 . 475E+0

1

1 . 166E+02 7.687E-01 1 . 200E+0

1

- 0.000 0.004 0.000

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ELECTRONS IN OXYGEN

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ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log1 )/d( log I ) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 1 . 937E+01 4.267E-03 1 . 937E+01 2. 950E-04 1 . 207E-04 0.0 -0.209 0.241 0.239

0.0125 1 . 6 32E+0

1

4.298E-03 1 . 633E+0

1

4.362E-04 1 . 449E-04 0.0 -0.199 0.229 0.227

0.0150 1 .41 9E+01 4.316E-03 1 .41 9E+01 6 . 009E-04 1 .681 E-0 4 0.0 -0.193 0.220 0.218

0.0175 1 .260E+01 4.328E-03 1 .261 E+01 7 . 382E-04 1 . 903E-04 0.0 -0.187 0.213 0.211 0.0200 1 . 1 33E+01 4.336E-03 1 . 1 38E+0

1

9. 973E-04 2. 1 18E-04 0 .

0

-0.183 0.207 0.206

0.0250 9 . 595E+00 4.347E-03 9 . 600E+00 1 .478E-03 2 . 529E-04 0 .

0

-0.176 0.198 0.197

0.0300 8 . 359E+00 4 . 356E-03 8 . 363E+00 2 . 037E-03 2. 91 9E-04 0.0 -0.170 0.191 0.190

0.0350 7 . 447E+00 4 . 365E-03 7 . 452E+00 2 . 672E-03 3 . 293E-04 0.0 -0.166 0.185 0.185

0.0400 6 .746E+00 4 . 376E-03 6 . 750E+00 3.378E-03 3 . 653E-04 0.0 -0.163 0.181 0.130

0.0450 6. 189E+00 4.388E-03 6 . 1 93E+00 4. 153E-03 4.001 E-0 4 0.0 -0.160 0.177 0.177

0.0500 5 . 735E+00 4 . 402E-03 5 . 739E+00 4.992E-03 4.339E-04 0 .

0

-0.157 0.174 0.174

0.0550 5 . 358E+00 4.41 7E-03 5 . 362E+00 5.894E-03 4 . 668E-04 0.0 -0.155 0.171 0.171 0.0600 5.039E+00 4.434E-03 5. 044E+00 6 .856E-03 4. 988E-04 0.0 -0.153 0.169 0.169

0.0700 4 . 530E+00 4.471E-03 4 . 535E+00 8.951 E-0 3 5.608E-04 0.0 -0.150 0.165 0.164

0.0800 4.142E+00 4.51 2E-03 4. 146E+00 1 . 126E-02 6 . 204E-04 0.0 -0.147 0.161 0.161 0.0900 3 . 835E+00 4 . 558E-03 3.339E+00 1 .377E-02 6 . 779E-04 0.0 -0.145 0.158 0.158

0.1000 3 . 586E+00 4 . 607E-03 3.591 E+00 1 . 647E-02 7 . 337E-04 0.0 -0.143 0.156 0.156

0.1250 3 . 1 33E+00 4.741E-03 3. 137E+00 2 . 394E-02 3.666E-04 0.0 -0.138 0.151 0.151

0. 1500 2 . 826E+00 4.889E-03 2.831 E+00 3 . 235E-02 9. 921 E-04 0.0 -0.135 0.147 0.147

0.1750 2 . 606E+00 5 . 048E-03 2.611 E+00 4. 157E-02 1 .112E-03 0.0 -0.132 0.144 0.144

0.2000 2.441 E+00 5.215E-03 2 . 446E+00 5. 147E-02 1 . 227E-03 0.0 -0.130 0.142 0.141 0.2500 2.21 1 E+00 5 . 578E-03 2.217E+00 7 . 302E-02 1 .447E-03 0.0 -0.127 0.138 0.137

0.3000 2.061 E+00 5.975E-03 2.067E+00 9.642E-02 1 .656E-03 0.0 -0.124 0.134 0.134

0.3500 1 . 957E+00 6 . 402E-03 1 . 963E+00 1 .21 3E-01 1 .859E-03 0.0 -0.121 0.132 0.131 0.4000 1 . 882E+00 6 . 856E-03 1 -889E+00 1 .473E-01 2 . 057E-0 3 0.0 -0.119 0.130 0.128

0.4500 1 . 826 E+00 7 . 335E-03 1 .833E+00 1 . 742E-0

1

2 . 253E-03 0 .

0

-0.117 0.128 0.126

0.5000 1 . 784E+00 7.838E-03 1 .791 E+00 2.018E-01 2.446E-03 0.0 -0.116 0.126 0.125

0.5500 1 .751 E+00 8 . 362E-03 1 . 759E+00 2.299E-01 2 . 639E-03 0.0 -0.114 0.125 0.123

0.6000 1 . 725E+00 8. 904E-03 1 . 734E+00 2 . 586E-0

1

2.831 E-0 3 0.0 -0.113 0.124 0.122

0.7000 1 . 6 90E+00 1 . 004E-02 1 . 700E+00 3. 169E-01 3.215E-03 0.0 -0.111 0.121 0.119

0.8000 1 . 667E+00 1 . 122E-02 1 . 67 9E+00 3.761 E-0

1

3.600E-03 0.0 -0.109 0.119 0.117

0 . 9000 1 . 654E+00 1 . 247E-02 1 . 666E+00 4 . 359E--0 1 3.987E-03 0.0 -0.107 0.118 0.115

1 .0000 1 . 646 E+0 0 1 .376E-02 1 . 659E+00 4.961 E-0

1

4.377E-03 0.0 -0.105 0.116 0.113

1 .2500 1 .641 E+00 1 . 7 1 8E-02 1 . 658E+00 6 .469E-01 5.366E-03 0.0 -0.102 0.113 0.110

1 .5000 1 . 647E+00 2 . 084E-02 1 . 667E+00 7.973E-01 6 . 376E-03 0.0 -0.100 0.111 0.107

1 .7500 1 . 658E+00 2 . 468E-02 1 . 682E+00 9.466E-01 7.405E-03 0.0 -0.098 0.108 0.104

2.0000 1 .671 E+00 2.869E-02 1 . 6 99E + 0 0 1 . 094E+00 8.452E-03 0.0 -0.096 0.107 0.102

2.5000 1 . 6 99E+00 3.71 IE-02 1 . 736E+00 1 . 386 E+00 1 . 059E-02 0.0 -0.093 0.104 0.099

3.0000 1 . 727E+00 4.598E-02 1 . 773E+00 1 .671 E+00 1 . 276E-02 0.0 -0.091 0.101 0.096 3.5000 1 .753E+00 5.51 9E-02 1 . 808E+00 1 . 950E+00 1 . 497E-02 0.0 -0.089 0.099 0.094

4.0000 1 . 777E+00 6.471E-02 1 . 842E+00 2 . 224E+00 1 . 720E-02 0.0 -0.088 0.093 0.092

4.5000 1 . 799E+00 7 . 448E-02 1 . 874E+00 2.493E+00 1 . 945E-02 0.0 -0.086 0.096 0.090

5.0000 1 . 820E+00 8 . 449E-02 1 . 905E+00 2 . 758E + 0 0 2.171E-02 0.0 -0.085 0.095 0 . 088 5.5000 1 .839E+00 9.470E-02 1 . 934E+00 3.018E+00 2. 398E-02 0.0 -0.084 0.094 0.087

6.0000 1 . 857E+00 1 .051E-01 1 . 962E+00 3 . 275E+00 2 . 626E-02 0 .

0

-0.083 0.092 0.086

7.0000 1 .889E+00 1 . 264E-0

1

2.016 E+00 3 . 777E+00 3.081 E-0 2 0.0 -0.082 0.091 0.084

8 .0000 1 . 91 8E+00 1 . 482E-0

1

2 . 066E+00 4 . 267E+00 3.536E-02 0.0 -0.080 0.089 0.082

9.0000 1 . 944E+00 1 . 705E-0

1

2.1 14E+00 4 . 746E+00 3 . 990E-02 0.0 -0.079 0.087 0 .080 10.0000 1 . 967E+00 1 . 932E-0

1

2. 160E+00 5.21 4E+00 4.441E-02 0.0 -0.078 0.086 0.079

12.5000 2.01 6E+00 2.514E-01 2 . 268E+00 6 . 343E+00 5 . 558E-02 0.0 -0 .076 0.083 0.075

15.0000 2 . 057E+00 3. 1 12E-01 2 . 368E+00 7.421 E+00 6.652E-02 0.0 -0.075 0.081 0.073

17.5000 2 . 092E+00 3.723E-01 2.464E+00 8 . 456E+00 7 . 720E-02 0.0 -0.074 0.079 0.070 20.0000 2. 122E+00 4.343E-01 2 . 556 E+0 0 9 . 452E+00 8.762E-02 0.0 -0.073 0.077 0.068 25.0000 2. 1 73E+00 5.606E-01 2 . 733E+00 1 . 1 34E+01 1 .076E-01 0.0 -0.071 0.074 0.065

30.0000 2.21 4E+00 6.890E-01 2. 903E+00 1 .312E+01 1 . 266 E-0

1

2 . 989E-03 -0.065 0.071 0.062

35.0000 2 . 246 E + 0 0 8. 189E-01 3 . 065E+00 1 .479E+01 1 . 446E-0

1

4 . 425E-02 -0.054 0.068 0.057

40.0000 2 . 272E+00 9.502E-01 3 . 222E+00 1 . 638E+0

1

1 .617 E— 0

1

1 . 129E-01 -0.047 0.065 0.053

45.0000 2 . 292E+00 1 . 083E+00 3 . 375E+00 1 . 790E+0

1

1 .779E-01 1 . 940 E-0

1

-0.041 0.062 0.048

50.0000 2.31 OE+OO 1 . 21 6E+00 3 . 526E+00 1 . 935E+01 1 . 934E-01 2.804E-01 -0.037 0.059 0.045

55.0000 2 . 325E+00 1 . 350E+00 3 . 675E+00 2 . 074E+0

1

2.082E-01 3.682E-01 -0.034 0.057 0.041 60.0000 2. 338E+00 1 . 484E+00 3 . 823E + 0 0 2 . 207E+0

1

2 . 224E-0

1

4 . 554E-0

1

-0.031 0.055 0.038 70.0000 2.361 E+00 1 . 755E+00 4.1 1 6 E + 00 2.459E+01 2.438E-01 6 . 239E-0

1

-0 .028 0.051 0.033

80.0000 2 . 379E+00 2. 028E+00 4 . 407E+00 2.694E+01 2.732E-01 7.31 9E-01 -0 .025 0.048 0.030

90.0000 2. 395E+00 2 . 302E+00 4 . 6 97E+00 2.914E+01 2.957E-01 9.288E-01 -0.023 0.045 0.027

100.0000 2.409E+00 2 . 577E+00 4 . 986 E+00 3. 120E+01 3. 165E-01 1 . 065E+00 -0.022 0.043 0.024

125.0000 2 . 437E+00 3 . 27CE+0 0 5 . 707E+00 3.589E+01 3.624E-01 1 . 366E+00 -0.019 0.038 0 .020

1 50.0000 2 . 460E+00 3 . 967E+00 6 . 427E+00 4.001 E+0

1

4.013E-01 1 . 622E+00 -0.018 0.035 0.017 175.0000 2 . 478E+00 4 . 668E + 00 7 . 1 46E+00 4 . 370E+0

1

4.348E-01 1 . 843E+0 0 -0.017 0 .033 0.015

200 .0000 2 . 4 94E+00 5.371E+00 7 . 865E+00 4.703E+01 4.640E-01 2.038E+00 -0.016 0.031 0.013 250.0000 2 . 520 E+0 0 6 . 784E+00 9 . 304E+00 5 . 287E+0

1

5. 127E-01 2.36 9E+00 -0.015 0.028 0.011 300.0000 2.541 E+00 3 . 202E+00 1 .074E+01 5 . 787E+0

1

5.517E-01 2 . 644E+00 -0.015 0.026 0.009

350.0000 2. 558E+00 9 . 625E+00 1 .218E+01 6 . 223E+0

1

5.840E-01 2 . 879E+00 -0.014 0.024 0.008 400.0000 2 . 573E+00 1 . 105E+01 1 . 362E+0

1

6.61 1 E+0

1

6.111 E-0

1

3 . 086E+00 -0.013 0.023 0.007

450 . 0000 2 . 586E+00 1 . 248E+0

1

1 . 507E+0

1

6.960E+01 6 . 343E-0

1

3.271 E+00 -0.013 0.022 0.006 500.0000 2 . 597E+00 1 . 391 E+01 1 . 651 E+01 7 . 277E+01 6 . 544E-01 3 . 438E+00 -0.012 0.021 0 .006 550.0000 2 . 608E+00 1 . 534E+01 1 . 7 95E+0

1

7 . 568E+0

1

6 . 72 1 E-0

1

3 . 592E+00 -0.011 0.020 0.005 600.0000 2. 61 7E+00 1 . 678E+0

1

1 . 939E+01 7 . 835E+0

1

6 . 878E-01 3 . 733E+00 -0.011 0.020 0.005 700.0000 2 . 633E+00 1 . 965E+01 2 . 228E+0

1

8 . 3 1 6 E+0

1

7. 144E-01 3 . 989E+00 -0.010 0.019 0.004

800.0000 2 . 646E+0 0 2 . 252E+0

1

2.517E+01 8 . 738E+0

1

7.361 E-0

1

4.21 5E+00 -0 .008 0.018 0.004

900.0000 2 . 658E+00 2. 540E+01 2 . 805E+0

1

9.114E+01 7 . 544E-0

1

4.41 8E+00 -0.008 0.017 0.004 1000.0000 2 . 668E+00 2 . 827E+0

1

3.094E+01 9 . 454E+0

1

7.699E-01 4 . 603E+00 -0.007 0.017 0.003

86
ELECTRONS IN NEON

I = 137.0 eV DENSITY = 8.385E-04 g/cm 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. ddog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV ca 2 /g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 1 . 773E+0

1

5.273E-03 1 . 774E+0

1

3 . 265E-04 1 .622E-04 0.0 -0.226 0.266 0.262 0.0125 1 . 500E+0

1

5.340E-03 1 . 50 0 E + 0

1

4.804E-04 1 . 951 E-04 0.0 -0.215 0.251 0.248

0.0150 1 . 307E+0

1

5.384E-03 1 . 308E + 0

1

6 . 595E-04 2.266E-04 0.0 -0.207 0.240 0.237 0.0175 1 . 1 64E+01 5.416E-03 1 . 164E+01 8.625E-04 2. 569E-04 0.0 -0.201 0.232 0.229

0.0200 1 . 0 52E+0

1

5.439E-03 1 . 053E+0

1

1 . 089E-03 2 . S62E-04 0.0 -0.196 0.225 0.223

0 .0250 8 . 8 98E + 00 5.470E-03 8 . 904E+00 1 . 607E-03 3 . 422E-04 0.0 -0.188 0.214 0.212

0.0300 7 . 768E+00 5.492E-03 7 . 773E+00 2.210E-03 3.953E-04 0.0 -0.182 0.206 0.204

0.0350 6 . 932E+00 5.510E-03 6 . 938E+00 2.892E-03 4 . 46 1 E-04 0.0 -0.177 0.200 0.198

0 .0400 6 . 288E+00 5 . 526E-03 6 . 293E+00 3 . 650E-03 4 . 949E-04 0.0 -0.173 0.194 0.193

0.0450 5 . 775E + 00 5 . 543E-03 5.781 E+00 4.480E-03 5 . 420E-04 0 .

0

-0.170 0.190 0.189

0.0500 5 . 357E+00 5.559E-03 5 . 362E+00 5.379E-03 5.876 E-04 0.0 -0.167 0.186 0.186 0.0550 5.009E+00 5 . 577E-03 5.01 4E+00 6 . 344E-03 6.319E-04 0.0 -0.164 0.183 0.183

0.0600 4.715E+00 5 . 595E-03 4 . 720E+00 7.373E-03 6 . 750E-04 0.0 -0.162 0.180 0.180 0.0700 4 . 244E+00 5.634E-03 4 . 250E+00 9.61 0E-03 7 . 580E-04 0.0 -0.158 0.176 0.175

0.0800 3 . 884E+00 5.679E-03 3 . 890E+00 1 . 207E-02 8. 374E-04 0.0 -0.155 0.172 0.171 0.0900 3 . 599E+00 5.727E-03 3 . 605E+00 1 . 475E-02 9. 1 38E-04 0 .

0

-0.153 0.169 0.168

0. 1000 3.369E+00 5.781E-03 3 . 375E+00 1 . 762E-02 9 . 875E-04 0 .

0

-0.150 0.166 0.165

0.1250 2 . 948E+00 5. 934E-03 2. 954E+00 2 . 557E-02 1 . 163E-03 0.0 -0.146 0.160 0.160 0.1500 2 . 663E+00 6 . 1 06E-03 2 . 669E+00 3.449E-02 1 .327E-03 0 .

0

-0.142 0.156 0.155 0.1750 2 . 458E+00 6.296E-03 2 . 464E+00 4.426E-02 1 . 484E-0 3 0.0 -0.139 0.152 0.152 0.2000 2 . 304E+00 6 . 500E-03 2.31 OE+OO 5 . 475E-02 1 . 6 34E-0 3 0.0 -0.137 0.150 0.149

0.2500 2 . 090E+00 6 . 945E-03 2 . 0 97E+00 7.754E-02 1 . 920E-03 0.0 -0.133 0.145 0.144

0.3000 1 . 950E+00 7.432E-03 1 . 958E+00 1 . 023E-0

1

2.1 92E-03 0 .

0

-0.129 0.142 0.140

0.3500 1 . 854E+00 7 . 956E-03 1 . 86 2E+0 0 1 . 285E-0

1

2 . 456E-03 0.0 -0.127 0.139 0.137

0.4000 1 . 784E+00 3.51 IE-03 1 . 7 92E+0 0 1 . 559E-01 2.71 3E-03 0.0 -0.125 0.136 0.135

0.4500 1 . 732E+00 9.096E-03 1 .741 E+00 1 . 842E-0

1

2. 965E-03 0.0 -0.123 0.134 0.133

0.5000 1 . 693E+00 9.707E-03 1 . 703E+00 2.1 33E-01 3.215E-03 0.0 -0.121 0.132 0.131 0.5500 1 . 66 3E+00 1 . 034E-02 1 . 673E+00 2.429E-01 3.463E-03 0.0 -0.119 0.131 0.129

0.6000 1 . 6 3 9E+0 0 1 . 100E-02 1 . 650E+00 2.730E-01 3.709E-03 0.0 -0.118 0.129 0.127

0 . 7000 1 . 607E+00 1 . 236E-02 1.61 9E+00 3 . 342E-0

1

4.200E-03 0.0 -0.115 0.127 0.124

0.8000 1 . 587E+00 1 . 380E-02 1 . 60 1 E+00 3. 964E-01 4.691E-03 0.0 -0.113 0.125 0.122

0 . 9000 1 . 575E+00 1 . 530E-02 1 . 590E+00 4.591 E-0

1

5. 184E-03 0.0 -0.111 0.123 0.120

1 .0000 1 . 568E+00 1 . 686E-02 1 . 585E+00 5.221E-01 5 . 678E-03 0.0 -0.110 0.121 0.118

1 .2500 1 . 565E+00 2.100E-02 1 . 586E+00 6.799E-01 6. 929E-03 0.0 -0.106 0.118 0.114

1 .5000 1 . 572E+00 2.542E-02 1 . 5 98E+0 0 8 . 370E-0

1

8 . 202E-03 0.0 -0.104 0.115 0.111

1 .7500 1 . 584E+00 3 . 008E-02 1 . 6 1 4E+00 9. 927E-01 9.497E-03 0.0 -0.101 0.113 0.108

2.0000 1 . 598E+00 3 . 493E-02 1 . 633E+00 1 . 1 47E+00 1 .081 E-0 2 0.0 -0.099 0.111 0.106 2.5000 1 . 626E+00 4.513E-02 1 . 672E+00 1 . 44 9E + 0 0 1 . 349E-02 0.0 -0.096 0.108 0.102

3.0000 1 . 654E+00 5.586E-02 1 .710 E+00 1 . 745E+00 1 .621 E-02 0.0 -0.094 0.105 0.099

3.5000 1 .681E+00 6.701 E-02 1 . 748E+00 2 . 0 34E+00 1 . 897E-02 0.0 -0.092 0.103 0.097 4.0000 1 . 7 0 5E+0 0 7 . 852E-02 1 . 783E+00 2.31 7E+00 2. 174E-02 0.0 -0.091 0.101 0 .094 4.5000 1 . 727E+00 9 . 033E-02 1 . 8 1 7E+00 2 . 595E+00 2.454E-02 0 .

0

-0.089 0.099 0.093

5.0000 1 . 748E+00 1 . 024E-0

1

1 . 850E+00 2 . 868E+00 2 . 7 33E-02 0.0 -0.088 0.098 0.091 5.5000 1 . 767E+00 1 . 147E-01 1 . 882E+00 3.1 36E+00 3.01 4E-02 0.0 -0.087 0.097 0.089

6.0000 1 . 785E+00 1 . 273E-0

1

1 . 912E+00 3 . 399E+00 3. 294E-02 0.0 -0 . 086 0.095 0.088 7.0000 1 .81 7E+00 1 . 529E-0

1

1 . 970E+00 3.91 5E+00 3 . 853E-02 0.0 -0.084 0.093 0.086 8.0000 1 . 845E+00 1 .791E-01 2 . 024E+00 4.41 5E+00 4.41 0E-02 0.0 -0.083 0.091 0.083

9.0000 1 . 870E+00 2.058E-01 2 . 076E+00 4. 903E+00 4 . 963E-02 0.0 -0.082 0.090 0.082

10.0000 1 .893E+00 2.330E-01 2. 1 26E+00 5.379E+00 5.51 0E-02 0.0 -0.081 0.088 0.080

12.5000 1 . 942E+00 3.026E-01 2 . 245E+00 6 . 523E+0 0 6 . 854E-02 0.0 -0.079 0.085 0.076 15.0000 1 . 983E+00 3.739E-01 2 . 357E+0 0 7 . 609E+00 8. 159E-02 0.0 -0.077 0.082 0.073

17.5000 2.01 7E+00 4.466E-01 2 . 464E+00 8 . 646E+00 9. 423E-02 0.0 -0.076 0.080 0.071 20.0000 2 . 047E+00 5.204E-01 2 . 568E+00 9 . 640E+00 1 .065E-01 0.0 -0.074 0.078 0.068 25.0000 2.098E+00 6.703E-01 2 . 768E+00 1 .151 E+0

1

1 . 297E-0

1

0.0 -0.073 0.075 0.065

30.0000 2 . 1 39E+00 8.226E-01 2. 962E+00 1 . 326E+01 1 .515E-01 0.0 -0.071 0.072 0.061 35.0000 2.174E+00 9 . 766E-01 3. 1 51 E+00 1 . 490E+0

1

1 .71 9E-01 0 .

0

-0.070 0.069 0.059 40.0000 2 . 204E+00 1 . 1 32E+00 3 . 336E+00 1 . 644E+0

1

1 . 91 0E-01 0.0 -0.069 0.067 0.056 45.0000 2.231E+00 1 .289E+00 3 . 520E+00 1 . 7 90E+0

1

2.090E-01 0.0 -0.068 0.065 0.054 50.0000 2 . 255E+00 1 . 446E+00 3 . 70 1 E+00 1 . 928E+01 2.259E-01 0.0 -0.068 0.064 0.052 55.0000 2 . 277E+00 1 . 605E+00 3 . 83 1 E+00 2.060E+01 2.420E-01 0.0 -0.067 0.062 0.050 60.0000 2 . 297E+00 1 . 764E+00 4 . 060E+00 2. 186E+01 2.571 E-0

1

0.0 -0 .066 0.061 0.049 70.0000 2 . 329E+00 2 . 084E+00 4.413E+00 2.422E+01 2.852E-01 2.873E-02 -0.054 0.058 0 .045 80.0000 2 . 355E+00 2 . 406E+00 4.761 E+00 2 . 640 E+0

1

3.107E-01 9. 312E-02 -0.045 0.055 0.041 90.0000 2.376E+00 2 . 729E+00 5. 105E+00 2 . 843E+0

1

3.340E-01 1 . 74 1 E-0

1

-0.039 0.053 0.037

100.0000 2 . 393E+00 3 . 0 54E+00 5 . 447E+00 3.033E+01 3.554E-01 2.624E-01 -0.035 0.051 0.034

125.0000 2. 427E+00 3.371 E+00 6 . 293E + 0 0 3.459E+01 4 . 02 1 E-0

1

4.388E-01 -0.028 0.046 0.028 150.0000 2 . 452E+00 4 . 6 93E + 00 7 . 1 44E+00 3 . 832E+0

1

4.412E-01 7.045E-01 -0.023 0.042 0.023

175.0000 2 . 472E+00 5.51 8E + 00 7 . 990E+00 4. 162E+01 4.745E-01 9.031 E-0

1

-0.021 0.040 0.020 200.0000 2 . 488E+00 6 . 347E+00 8 . 835E+00 4 . 460E+0

1

5.033E-01 1 . 085E+00 -0.019 0.037 0.018 250.0000 2.51 5E+00 8.01 OE + OO 1 . 053E+01 4 . 978E + 0

1

5.508E-01 1 . 403E+00 -0.016 0.034 0.014 300.0000 2 . 536E+00 9 . 680E+00 1 . 222E+0

1

5.418E+01 5.886E-01 1 . 674E+00 -0.015 0.032 0.012 350.0000 2 . 554E+00 1 . 1 35E+01 1 . 39 1 E+0

1

5 . 802E+0

1

6.1 95E-01 1 . 908E+00 -0.014 0.030 0.010 400.0000 2 . 568E+00 1 .303E+01 1 . 560E+0

1

6.141 E+0

1

6 . 453E-01 2.114E+00 -0.013 0.028 0.009 450.0000 2.581E+00 1 .471E+01 1 . 729E+0

1

6 . 445E+0

1

6.673E-01 2.298E+00 -0.013 0.027 0.008 500.0000 2 . 593E+00 1 . 639E+0

1

1 . 899E+0

1

6.721 E+0

1

6.863E-01 2 . 464E+00 -0.012 0.026 0.007 550.0000 2 . 603E+00 1 . 808E+0

1

2.068E+01 6 . 973E+0

1

7.029E-01 2.616 E+00 -0.012 0.025 0.007 600.0000 2.61 2E+00 1 . 976E+01 2 . 237E+0

1

7.206E+01 7.176E-01 2 . 755E+00 -0.012 0.024 0.006 700.0000 2 . 628E+00 2.313E+01 2 . 576E+0

1

7 . 622E+0

1

7 . 423E-0

1

3 . 003E+00 -0.011 0.023 0.005 300.0000 2 . 642E+00 2.651 E+0

1

2.915E+01 7 . 987E + 0

1

7 . 625E-0

1

3 . 220E+00 -0.011 0.022 0.005

900.0000 2 . 655E+00 2. 989E+01 3.254E+01 8.311 E+0

1

7.794E-01 3.41 3E+00 -0.010 0.021 0.004 1000.0000 2 . 665E+00 3 . 327E+0

1

3 . 594E+0

1

8 . 603E+01 7.937E-01 3 . 587E+00 -0.010 0.020 0.004

87
(

ELECTRONS IN ALUMINUM

I = 166.0 eV DENSITY = 2 . 699E+00i g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS .EFF. d( loc1 )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV c» 2 /g MeV cm 2/g MeV cn 2 /g g/cm 2 0.0100 1 . 649E+0

1

6 . 559E-03 1 . 6 50E+0

1

3.539E-04 2.1 32E-04 3 . 534E-04 -0.236 0.281 0.275

0.0125 1 . 398E+0

1

6 .700E-03 1 . 398E+01 5.1 92E-04 2.583E-04 4. 937E-04 -0.224 0.265 0.260 0.0150 1 . 220E+0

1

6 .798E-03 1 .221 E+0

1

7.111E-04 3 . 01 6E-04 6 . 538E-04 -0.216 0.252 0.248 0.0175 1 . 088E + 0

1

6.871E-03 1 . 088E+0

1

9.284E-04 3.435E-04 3.332E-04 -0.209 0.243 0.239

0.0200 9 . 844E+00 6 . 926E-03 9.851 E+00 1 . 1 70E-03 3 .840E-04 1 .031 E-03 -0.203 0.235 0.232

0.0250 8 . 338E+00 7 . 004E-03 8 . 345E+00 1 .724E-03 4.S16E-04 1 . 483E-0 3 -0.195 0.224 0.221 0.0300 7 . 287E+00 7 . 059E-03 7 . 294E+00 2.367E-03 5 . 353E-04 2 . 005E-03 -0.188 0.215 0.212

0.0350 6.509E+00 7.100E-03 6.51 6E+00 3.093E-03 6 . 058E-04 2.593E-03 -0.183 0.208 0.206 0.0400 5. 909E+00 7.133E-03 5.91 6E+00 3 . 900E-03 6 . 736E-04 3 . 246E-03 -0.179 0.202 0.201 0.0450 5 . 430E+00 7. 162E-03 5 . 437E+00 4. 783E-03 7 . 390E-04 3 . 960E-03 -0.175 0.198 0.196

0.0500 5 . 039E+00 7.1 91 E-03 5 . 046E+00 5.738E-03 8.022E-04 4 . 732E-03 -0.172 0.194 0.192

0.0550 4.71 4E+00 7.217E-03 4.721 E+00 6 .763E-03 8 . 636E-04 5 . 56 0 E-0 3 -0.170 0.190 0.139

0.0600 4 . 439E+00 7.243E-03 4 . 446E+00 7 . 855E-0 3 9.232E-04 6 . 440E-0 3 -0.167 0.187 0.186

0.0700 3. 998E+00 7.295E-03 4 . 005E+00 1 . 023E-0 2 1 . 0 38E-0 3 8 . 35 1 E-0 3 -0.163 0.182 0.181 0.0800 3.661 E+00 7.350E-03 3 . 668E+0 0 1 . 284E-02 1 . 147E-03 1 . 045E-02 -0.160 0.178 0.177

0.0900 3 . 394E+00 7.41 IE-03 3.401 E+00 1 . 568E-02 1 . 252E-0 3 1 . 27 1 E-02 -0.157 0.174 0.173

0.1000 3. 177E+00 7 . 476E-03 3. 185E+00 1 .872E-02 1 . 353E-03 1 .51 3E-02 -0.155 0.171 0.170

0.1250 2.781 E+00 7 . 659E-03 2 . 789E+00 2.714E-02 1 . 593E-03 2.175E-02 -0.150 0.165 0.164

0.1500 2.51 3E+00 7.865E-03 2 .521 E+00 3 . 659E-02 1 .816E-03 2. 907E-02 -0.146 0.160 0.160 0.1750 2 . 320E+00 8.096E-03 2 . 32SE+00 4.693E-02 2.028E-03 3.694E-02 -0.143 0.157 0.156 0.2000 2 . 1 74E+00 8 . 344E-03 2. 183E+00 5.804E-02 2.231 E-03 4 . 525E-02 -0.140 0.154 0.153

0.2500 1 . 972E+00 8.888E-03 1 . 98 1 E+00 8.217E-02 2.616E-03 6 . 280 E-02 -0.136 0.149 0.148

0.3000 1 .339E+00 9.487E-03 1 . 84 9E+0 0 1 . 083E-0

1

2. 982E-03 8. 1 16E-02 -0.132 0.145 0.144

0.3500 1 . 747E+00 1 .013E-02 1 . 757E+00 1 .361E-01 3 . 335E-03 9. 997E-02 -0.129 0.142 0.141 0.4000 1 . 680E+00 1 . 082E-02 1 .691 E+00 1 .652E-01 3.678E-03 1 . 1 90E-01 -0.127 0.139 0.138

0.4500 1 . 630E+00 1 . 1 54E-02 1 . 642E+00 1 . 952E-01 4.01 6E-03 1 . 380E-0

1

-0.125 0.137 0.135

0.5000 1 . 592E+00 1 . 230E-02 1 . 604E+00 2.260E-01 4 . 349E-03 1 .569E-01 -0.123 0.135 0 . 1 33 0.5500 1 . 563E+00 1 .309E-02 1 . 576E+00 2.575E-01 4 . 680E-0 3 1 . 757E-0

1

-0.121 0.133 0.131 0.6000 1 . 540 E+00 1 . 390E-02 1 . 554E+00 2 . 894E-0

1

5.009E-03 1 . 943E-01 -0.119 0.132 0.130 0.7000 1 . 507E+00 1 . 560E-02 1 . 522E+00 3.545E-01 5.664E-03 2.307E-01 -0.116 0.129 0.126 0.8000 1 . 486E+00 1 . 7 39E-0 2 1 . 503E+00 4.206E-01 6.319E-03 2.661 E-01 -0.113 0.127 0.124

0 . 9000 1 . 473E+00 1 . 925E-02 1 . 492E+00 4.874E-01 6 . 976E-03 3.005E-01 -0.111 0.124 0.121

1 .0000 1 . 465E+00 2.11 9E-02 1 . 486E+00 5.546E-01 7 . 636E-03 3 . 339E-01 -0.108 0.122 0.119

1 .2500 1 . 457E+00 2 . 630E-02 1 . 484E+00 7.231E-01 9 . 306E-03 4.1 38E-01 -0.103 0.118 0.113

1 .5000 1 . 460E+00 3.177E-02 1 .491 E+00 8.912E-01 1 .101E-02 4.898E-01 -0.097 0.114 0 . 1 OS

1 .7500 1 . 466E+00 3.752E-02 1 . 504E+00 1 . 058E+00 1 . 274E-02 5.632E-01 -0.092 0.111 0.105

2.0000 1 . 475E+00 4 . 350E-02 1 .518E+00 1 . 224E+00 1 . 449E-02 6.349E-01 -0.087 0 . 1 08 0.101 2.5000 1 . 493E+00 5 . 605E-02 1 . 549E+00 1 . 550E+00 1 . 808E-02 7 . 757E-0

1

-0.077 0.102 0.093

3.0000 1 .51 0E+00 6 . 924E-02 1 . 580E+00 1 . 86 9E+00 2. 173E-02 9.145E-01 -0.067 0.096 0.085

3.5000 1 . 526E+00 8 , 292E-02 1 . 609E+00 2.183E+00 2 . 544E-02 1 . 0 5 1 E + 00 -0.059 0.091 0.079

4.0000 1 . 540E+00 9.702E-02 1 . 637E+00 2.491 E+00 2. 91 8E-02 1 . 1 83E+00 -0.052 0.086 0.072

4.5000 1 . 552E+00 1 .115E-01 1 . 664E+00 2 . 7 94E+00 3.296E-02 1.311 E+00 -0.047 0.082 0.067 5.0000 1 .564E+00 1 .263E-01 1 . 6 90E+0 0 3 . 092E+00 3 . 675E-02 1 . 433E+00 -0.042 0.078 0.062

5.5000 1 . 574E+00 1 .413E-01 1 . 7 1 5E+00 3 . 386E+00 4 . 055E-02 1 . 550E+00 -0.039 0.074 0.058

6.0000 1 . 583E+00 1 .567E-01 1 . 739E+00 3 . 675E+00 4 . 436E-02 1 .661 E+00 -0.036 0.071 0.054

7.0000 1 . 5 9 9E+0 0 1 . 879E-0

1

1 . 787E+00 4 . 242E+00 5.1 97E-02 1 . 868E+00 -0.032 0.066 0 .048 8.0000 1 . 6 1 3E+00 2.200E-01 1 . 833E+00 4 . 7 95E+00 5. 955E-02 2 . 055E+00 -0.029 0.061 0 .043 9.0000 1 . 625E+00 2.526E-01 1 .877E+00 5 . 334E+00 6 . 708E-02 2 . 226 E+0 0 -0.026 0.057 0.039

10.0000 1 . 6 36E+00 2.858E-01 1 . 921 E+00 5.861 E+00 7 . 454E-02 2 . 384E + 0 0 -0.025 0.054 0.035

12.5000 1 . 658E+00 3.706E-01 2 . 029E+00 7. 127E+00 9.281 E-02 2 . 727E+00 -0.022 0 .048 0.030 15.0000 1 . 676E+00 4.574E-01 2.1 34E+00 8 . 328E+00 1 .105E-01 3.01 6E+00 -0.020 0.044 0 . 026 17.5000 1 .691 E+00 5.459E-01 2 . 237E+00 9.472E+00 1 . 275E-0

1

3.265E+00 -0.018 0 .040 0.023

20.0000 1 . 704E+00 6.357E-01 2 . 340E+00 1 . 056E+0

1

1 . 438E-0

1

3 . 484E+00 -0.017 0.037 0.021 25.0000 1 . 726E+00 3. 180E-01 2 . 544E+00 1 . 26 1 E+0

1

1 . 745E-0

1

3 . 857E+00 -0.016 0 .033 0.018

30.0000 1 . 743E+00 1 . 003E+00 2 . 746 E+0 0 1 . 450E+0

1

2.027E-01 4 . 1 68E + 00 -0.014 0.030 0.015

35.0000 1 . 757E+00 1 . 1 90E+00 2 . 947E+00 1 . 626E+0

1

2 . 287E-0

1

4 . 435E+00 -0.013 0.028 0.014 40.0000 1 . 7 6 9E+00 1 . 379E+00 3. 148E+00 1 . 790E+0

1

2 . 528E-0

1

4.66 9E+00 -0.012 0.026 0.012

45.0000 1 . 780E+00 1 . 569E+00 3. 349E+00 1 . 944E+01 2.751E-01 4 . 878E+00 -0.010 0.024 0.011

50 .0000 1 . 789E+00 1 .761 E+00 3 . 550E+00 2.089E+01 2. 959E-01 5. 068E+00 -0.009 0.023 0.010 55.0000 1 . 797E+00 1 . 953E+00 3.751 E+00 2 . 226E+0

1

3.152E-01 5.241 E+00 -0.009 0 .022 0.009

60.0000 1 . 305E+00 2. 147E+00 3.951 E+00 2.356E+01 3 . 333E-0

1

5.401 E+00 -0 .008 0.021 0.009

70.0000 1 .31 8E+00 2 . 535E+00 4 . 353E+00 2.597E+01 3.662E-01 5 . 687E+00 -0.006 0.019 0 .007 80.0000 1 . 829E+00 2. 927E+00 4 . 755E+00 2.817E+01 3. 953E-01 5 . 938E+00 -0.005 0.013 0 .006 90.0000 1 .838E+00 3. 320E+00 5.1 58E+00 3.01 9E+01 4.214E-01 6.161 E+00 -0.004 0.017 0.006 100.0000 1 . 847E+00 3.71 4E+00 5 . 56 1 E+00 3 . 205E+0

1

4 . 448E-0

1

6 . 363E+00 -0.004 0.016 0.005

125.0000 1 . 864E+00 4 . 707E+00 6 . 571 E+00 3.618E+01 4.945E-01 6.794E+00 -0.003 0.014 0 .004 150.0000 1 . 87 9E + 0 0 5 . 705E+00 7 . 583E+00 3.972E+01 5.346E-01 7. 150E+00 -0.002 0.013 0.003

175.0000 1 . 8 90 E + 00 6 . 708E+00 3 . 598E+00 4 . 282E+0

1

5.678E-01 7 . 452E+00 -0.001 0.012 0.003 200.0000 1 . 900E+00 7.714E+00 9.61 4E+00 4 . 557E+0

1

5.958E-01 7.71 6E+00 -0.001 0.011 0.002

250 .0000 1 . 91 7E+00 9 . 734E+00 1 .165E+01 5 . 028E+0

1

6.406E-01 8 . 1 57E+00 -0.001 0.010 0.002

300.0000 1 . 931 E+00 1 .176E+01 1 .369E+01 5 . 424E+0

1

6.751 E-0

1

8.51 9E+00 -0.001 0.010 0.001 350.0000 1 . 943E+00 1 . 380E+0

1

1 . 574E+0

1

5 . 764E+0

1

7.027E-01 8 . 826E+00 -0 .000 0.009 0.001

400 . 0000 1 . 952E+00 1 .583E+01 1 . 778E+0

1

6 . 063E+01 7 . 253E-0

1

9.091 E+00 -0 .000 0.009 0.001 450.0000 1 . 96 1 E+00 1 . 787E+0

1

1 . 983E+01 6 . 329E+0

1

7.443E-01 9 . 326E+00 -0.000 0.008 0.001 500.0000 1 . 969E + 00 1 . 992E+01 2. 189E+01 6.56 9E+0

1

7 . 6 04E-0

1

9 . 536E+00 -0.000 0.008 0.001 550.0000 1 . 976E + 00 2.1 96E+01 2 . 394E+0

1

6 . 787E+01 7.744E-01 9 . 726 E + 0 0 -0.000 0.008 0.001 600.0000 1 . 983E+00 2.401E+01 2. 599E+01 6 . 988E+01 7.866E-01 9 . 900E+00 -0.000 0.007 0.001 700.0000 1 . 994E+00 2 .81 1 E+01 3.010E+01 7. 345E+01 8.069E-01 1 . 021 E+01 -0.000 0.007 0.001 800.0000 2. 004E+00 3.221 E+O

1

3.421E+01 7 . 656E+01 8. 233E-01 1 . 047E+01 -0.000 0.007 0.001

900 . 0000 2.01 3E+00 3.631 E+0

1

3 . 833E+0

1

7.932E+01 8 . 367E-01 1 . 0 7 1 E+0

1

- 0.000 0.007 0 .000 1000.0000 2. 021 E+00 4 . 042E+0

1

4 . 244E+0

1

8. 180E+01 8.481 E-0

1

1 . 0 92E+0

1

- 0.000 0.006 0.000

88
ELECTRONS IN ALUMINUM <*

)

I = 166.0 eV DENSITY = 2 . 699E+O0> g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD C0RR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2/g MeV cm 2 /g g/cm 2 0.0100 1 . 649E+0

1

6 . 559E-03 1 . 650E+0

1

3.539E-04 2.1 32E-04 1 . 456E-04 -0 . 236 0.281 0.275 0.0125 1 . 398E+0

1

6 . 700E-03 1 . 398E + 01 5 . 1 92E-04 2 . 583E-04 2 . 266E-04 -0.224 0.265 0.260 0.0150 1 . 220E+0

1

6.793E-03 1 . 22 1 E+0

1

7.111 E-04 3.016E-04 3.253E-04 -0.216 0.252 0.248

0.0175 1 . 08SE+01 6.871E-03 1 . 088E+0

1

9.284E-04 3.435E-04 4.41 3E-04 -0.209 0.243 0.239

0.0200 9 . 845E+00 6 . 926E-03 9 .851 E+00 1 . 1 70E-03 3 . 840E-04 5 . 747E-04 -0.203 0.235 0.232

0.0250 8. 339E+00 7 . 004E-03 8 . 346E+00 1 . 724E-03 4.615E-04 8 . 925E-04 -0.195 0.224 0.221 0.0300 7 . 288E+00 7.059E-03 7 . 295E+00 2 . 367E-0 3 5.353E-04 1 .276E-03 -0.188 0.215 0.212 0.0350 6 .51 OE+00 7 . 1 00E-03 6.51 7E+00 3.093E-03 6 .058E-04 1 -720E-03 -0.183 0.208 0.206 0.0400 5 . 909E+00 7. 133E-03 5 . 91 6E+00 3 . 900E-03 6 . 736E-04 2.21 9E-03 -0.179 0 .202 0.201 0.0450 5.431 E + 00 7.162E-03 5 . 438E+00 4.782E-03 7 . 389E-04 2 . 773E-03 -0.175 0.198 0.196 0.0500 5 . 040E+00 7 . 1 91 E-03 5 . 047E+00 5.738E-03 8.022E-04 3.391 E-03 -0.172 0.194 0.192

0.0550 4. 71 5E+00 7.217E-03 4 . 722E+00 6.763E-03 8.635E-04 4 . 080E-03 -0.170 0.190 0.139

0.0600 4 . 439E+00 7 .243E-03 4 . 447E+00 7 . 855E-03 9.231 E-04 4 .842E-03 -0.167 0.187 0.186

0 .0700 3. 999E+00 7.295E-03 4 . 006E+00 1 .023E-02 1 . 038E-03 6.497E-03 -0.163 0.182 0.181 0.0800 3.661 E+00 7.350E-03 3.669E+00 1 . 284E-0 2 1 . 147E-03 8.162E-03 -0.160 0.178 0.177 0.0900 3.394E+00 7.41 IE-03 3 . 40 2E+0 0 1 . 568E-02 1 . 252E-0 3 9.701 E-03 -0.157 0.174 0.173

0.1000 3.178E+00 7.476E-03 3. 186E+00 1 . 872E-02 1 . 353E-03 1 . 138E-02 -0 . 1 55 0.171 0.170

0 .1250 2 . 782E+00 7.659E-03 2 . 7 90E + 0 0 2.71 3E-02 1 . 592E-03 1 . 738E-02 -0.150 0.165 0.164

0.1500 2.51 4E+00 7.865E-03 2.521 E+00 3.659E-02 1 .816E-03 2.450E-02 -0.146 0.160 0.160 0.1750 2 . 320 E+0 0 8.096E-03 2. 329E+00 4.692E-02 2.028E-03 3. 142E-02 -0.143 0.157 0.156 0.2000 2. 175E+00 8 . 344E-03 2. 184E+00 5 . 802E-02 2.231 E-03 3.876E-02 -0.140 0.154 0.153

0.2500 1 . 973E+00 8.888E-03 1 . 982E+00 8.214E-02 2.615E-03 5 . 485E-02 -0.136 0.149 0.148

0 . 3000 1 . 840 E + 0 0 9.487E-03 1 . 850E+00 1 . 083E-01 2. 981 E-03 7.180E-02 -0.132 0.145 0.144

0.3500 1 . 748E+00 1 .01 3E-02 1 . 758E+00 1 . 361 E— 01 3.333E-03 8.931E-02 -0.129 0.142 0.141

0 .4000 1 . 681 E+00 1 .082E-02 1 . 692E+00 1 .651E-01 3.676E-03 1 . 072E-0

1

-0.127 0.139 0.138 0.4500 1 .631 E+00 1 . 1 54E-02 1 . 643E+00 1 . 951 E-01 4.013E-03 1 .252E-01 -0.125 0.137 0.135

0.5000 1 . 594E+00 1 . 230E-02 1 . 606E+00 2 . 259E-0

1

4 . 346E-03 1 . 433E-0

1

-0.123 0.135 0.133 0.5500 1 . 564E+00 1 . 309E-02 1 . 577E+00 2.573E-01 4 . 677E-03 1 .614E-01 -0.121 0.133 0.131 0.6000 1 . 541 E+00 1 . 390E-02 1 . 555E+00 2.893E-01 5.005E-03 1 .794E-01 -0.119 0.132 0.130 0.7000 1 . 508E+00 1 . 560E-02 1 . 524E+00 3.543E-01 5 . 660E-03 2.151 E-01 -0.116 0.129 0.126 0.8000 1 . 487E+00 1 . 739E-02 1 . 505E+00 4.203E-01 6.314E-03 2.503E-01 -0.113 0.127 0.124

0 . 9000 1 . 474E+00 1 . 925E-02 1 . 493E+00 4.871E-01 6 . 970E-03 2.848E-01 -0.111 0.124 0.121

1 .0000 1 . 466E+00 2.11 9E-02 1 . 487E+00 5.542E-01 7 . 630E-03 3. 188E-01 -0.108 0.122 0.119

1 .2500 1 . 458E+00 2 . 630E-02 1 . 485E+00 7.226E-01 9 . 299E-03 4.014E-01 -0.103 0.118 0.113

1.5000 1 . 460E+00 3. 177E-02 1 . 492E+00 8. 906E-01 1 . 100E-02 4 .81 4E-01 -0.097 0.114 0.109

1 .7500 1 . 467E+00 3 . 752E-02 1 . 504E+00 1 . 0 57E+0 0 1 . 273E-02 5.594E-01 -0.092 0.111 0.105

2.0000 1 . 475E+00 4.350E-02 1 . 5 1 8E+00 1 . 223E+00 1 . 449E-02 6 . 359E-01 -0.087 0.108 0.101 2.5000 1 . 4 92E + 0 0 5 . 605E-02 1 . 548E+00 1 . 549E+00 1 . 8 0 7E-0 2 7.845E-01 -0 . 077 0.102 0.093

3.0000 1 . 50 9E+00 6 . 924E-02 1 . 57 9E + 00 1 . 86 9E + 0 0 2. 173E-02 9.273E-01 -0.067 0.096 0 . 035 3.5000 1 . 525E+00 8.292E-02 1 . 608E+00 2. 183E+00 2.544E-02 1 . 064E+00 -0.059 0.091 0.079 4.0000 1 . 539E+00 9 . 702E-02 1 . 636E+00 2.491 E+00 2. 91 9E-02 1 . 1 94E + 00 -0.052 0 . 086 0.072

4.5000 1 . 552E+00 1 .115E-01 1 . 663E+00 2 . 794E+00 3 . 297E-02 1 . 31 8E+00 -0.047 0.082 0.067 5.0000 1 . 563E+00 1 .263E-01 1 . 690E+00 3 . 092E+00 3.676E-02 1 . 436E+00 -0 .042 0 .078 0.062 5.5000 1 . 574E+00 1 .41 3E-01 1 . 71 5E+00 3 . 386 E + 00 4.056E-02 1 . 548E + 00 -0.039 0.074 0.058

6.0000 1 . 583E+00 1 . 567E-0

1

1 . 740E+00 3 . 675E+00 4.436E-02 1 . 654E+00 -0.036 0.071 0.054

7.0000 1 . 600E+00 1 .879E-01 1 . 788E+00 4 . 242E+00 5.1 97E-02 1 . 853E+00 -0.032 0.066 0.048 8.0000 1 . 6 1 4E+00 2.200E-01 1 .834E+00 4.794E+00 5.954E-02 2 . 033E + 00 -0.029 0.061 0.043

9.0000 1 . 627E+00 2.526E-01 1 . 87 9E+00 5 . 333E+00 6 . 706E-02 2.1 99E+00 -0.026 0.057 0.039 10.0000 1 . 638E+00 2 . 858E-0

1

1 . 924E+00 5 . 859E+00 7.451E-02 2.352E+00 -0.025 0.054 0.035

12.5000 1 .661 E+00 3.706E-01 2.031 E+00 7. 123E+00 9 . 274E-02 2 . 690E+00 -0.022 0.048 0.030

15.0000 1 . 679E+00 4 . 574E-0

1

2.1 36E+00 8 . 323E + 00 1 . 104E-01 2. 977E+00 -0 .020 0.044 0.026 17.5000 1 . 694E+00 5.459E-01 2 . 240E+00 9 . 466E+00 1 .273E-01 3 . 227E+00 -0.013 0.040 0.023 20.0000 1 . 707E+00 6.357E-01 2 . 343E+00 1 . 056E+0

1

1 .436E-01 3 . 449E+00 -0.017 0.037 0.021 25.0000 1 . 728E+00 8. 180E-01 2 . 546E+00 1 . 260E+0

1

1 . 743E-0

1

3 . 829E + 00 -0.016 0.033 0.018

30.0000 1 . 744E+00 1 . 003E+00 2 . 747E + 0 0 1 . 449E+0

1

2.025E-01 4. 147E+00 -0.014 0.030 0.015

35.0000 1 . 758E+00 1 . 1 90E+00 2. 948E+00 1 . 625E+0

1

2.285E-01 4.421 E+00 -0.013 0.028 0.014 40.0000 1 . 770 E+0 0 1 .379E+00 3. 149E+00 1 .789E+01 2. 526E-01 4 . 663E+00 -0.012 0.026 0.012 45.0000 1 . 780 E+0 0 1 . 56 9E + 00 3 . 349E+00 1 . 943E+01 2.750E-01 4 . 878E+00 -0.010 0.024 0.011

50 .0000 1 . 789E+00 1 .761 E+00 3 . 550E+00 2 . 088E+0

1

2. 957E-01 5 . 073E+00 -0.009 0.023 0.010 55.0000 1 . 797E+00 1 . 953E+00 3 . 750E+00 2 . 225E+0

1

3. 1 51 E-01 5 . 250 E + 0 0 -0.009 0.022 0.009

60.0000 1 .804E+00 2. 147E+00 3 . 950E+00 2 . 355E+0

1

3.332E-01 5.41 3E+00 -0 .008 0.021 0.009 70.0000 1 .81 6E + 00 2 . 535E+00 4 . 352E+00 2 . 596E+0

1

3.661 E-01 5 . 705E+00 -0.006 0.019 0 .007 80.0000 1 . 827E+00 2. 927E+00 4 . 754E+00 2 . 81 6 E + 0

1

3.953E-01 5 . 960E+00 -0.005 0.018 0 .006 90.0000 1 . 837E+00 3 . 320 E+00 5 . 1 56E+00 3.018E+01 4.214E-01 6 . 186E+00 -0.004 0.017 0.006 100.0000 1 . 845E+00 3.71 4E+00 5 . 559E+00 3 . 204E+0

1

4.449E-01 6 . 390E+00 -0.004 0.016 0.005

125.0000 1 . 862E+00 4 . 707E+00 6 . 569E+00 3.618E+01 4. 946E-01 6 .823E+00 -0.003 0.014 0.004

150.0000 1 . 876E+00 5 . 705E+00 7 . 58 1 E+00 3 . 972E+0

1

5. 347E-01 7. 180E+00 -0.002 0.013 0 .003 175.0000 1 . 888E+00 6 . 708E+00 8 . 5 96E+00 4 . 28 1 E+0

1

5.679E-01 7 . 482E + 00 -0.001 0.012 0.003 200.0000 1 . 8 98E+0 0 7.71 4E+00 9.612E+00 4 . 556 E + 0

1

5. 959E-01 7 . 745E+00 -0.001 0.011 0.002 250.0000 1 . 91 5E+00 9 . 734E+00 1 . 165E+01 5 . 023E+0

1

6.407E-01 8.1 86E+00 -0.001 0.010 0.002 300.0000 1 . 929E+00 1 . 1 76E+0

1

1 .369E+01 5 . 423E+0

1

6 . 753E-0

1

3 . 547E+00 -0.001 0.010 0.001 350.0000 1 . 941 E+00 1 . 380E+0

1

1 . 574E+0

1

5 . 764E+0

1

7 . 028E-0

1

8 .853E+00 - 0.000 0.009 0.001 400.0000 1 . 951 E+00 1 . 583E+0

1

1 . 778E+0

1

6.063E+01 7.255E-01 9.1 18E+00 - 0.000 0.009 0.001 450.0000 1 . 959E+00 1 . 787E+0

1

1 . 983E+0

1

6.329E+01 7 . 444E-0

1

9. 352E+00 - 0.000 0.008 0.001 500.0000 1 . 967E+00 1 . 992E+0

1

2. 188E+01 6.569E+01 7.605E-01 9 . 562E+00 - 0.000 0.008 0.001 550.0000 1 . 974E+00 2.1 96E+01 2 . 394E+0

1

6 . 787E+0

1

7.745E-01 9.751 E+00 - 0.000 0.008 0.001 600.0000 1 . 981 E+00 2.401 E+0

1

2 . 599E+0

1

6 . 987E+01 7.367E-01 9. 924E+00 - 0.000 0.007 0.001 700.0000 1 . 992E+00 2.31 1E+01 3.010E+01 7 . 345E+0

1

8 . 070E-0

1

1 . 0 23E+0

1

- 0.000 0.007 0.001 800.0000 2 . 002E+00 3.221 E+0

1

3.421 E+0

1

7 . 656E+0

1

8.234E-01 1 . 050E + 0

1

- 0.000 0.007 0.001 900.0000 2.011 E+00 3.631 E+0

1

3 . 833E+0

1

7. 932E+01 8.368E-01 1 . 073E+0

1

- 0.000 0.007 0.000 1000.0000 2.01 9E+00 4 . 042E+0

1

4 . 244E+0

1

8. 180E+01 8.482E-01 1 . 0 94E+0

1

- 0.000 0.006 0.000 Evaluated with the density-effect correction of Inokuti and Smith (1982).

89
ELECTRONS IN SILICON

I = 173.0 eV DENSITY = 2 . 330E+001 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d ( log1 )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cra 2 /g MeV ci» 2 /g g/cm 2 0.0100 1 .689E + 01 7 . 255E-03 1 . 6 90E+0

1

3.461 E-04 2 . 289E-04 1 . 037E-03 -0.238 0 . 284 0.278

0.0125 1 . 432E+0

1

7.431 E-0 3 1 . 433E+01 5.074E-04 2 . 780E-04 1 . 332E-0 3 -0.226 0.268 0.262

0.0150 1 .251 E+01 7.555E-03 1 . 252E+0

1

6. 946E-04 3.252E-04 1 .641 E-03 -0.217 0.255 0.251 0.0175 1 . 1 15E+01 7.648E-03 1 . 1 16E+01 9.065E-04 3.709E-04 1 . 963E-03 -0.210 0 . 245 0.241 0.0200 1 .010E+01 7.720E-03 1 .01 1E+01 1 . 142E-03 4.151 E-04 2.293E-03 -0.205 0.238 0.234

0.0250 8 . 556E+00 7.822E-03 8 . 564E+00 1 . 682E-0 3 5 . 000E-04 3. 007E-03 -0.196 0.225 0.223

0.0300 7 . 480E+00 7 . 8 92E-0 3 7 . 487E+00 2 . 308E-03 5 . 307E-04 3 . 76 6 E-0 3 -0.189 0.216 0.214

0.0350 6 . 682E + 00 7.946E-03 6 . 6 90E+00 3.016E-03 6 . 57 9E-04 4.572E-03 -0.134 0.209 0.207

0.0400 6 . 067E+00 7.988E-03 6.075E+00 3 . 802E-03 7 . 322E-04 5.424E-03 -0.180 0.204 0.202

0.0450 5 . 57 6E+0 0 8. 026E-03 5 . 584E+00 4.661E-03 8 . 038E-04 6 . 320E-03 -0.176 0.199 0.197

0.0500 5. 175E+00 8.061 E-0 3 5. 183E+00 5.591 E-03 8.731 E-04 7.257E-03 -0.173 0.195 0.193

0.0550 4.842E+00 8.092E-03 4 . 850E+00 6.590E-03 9 . 402E-04 8.235E-03 -0.170 0.191 0.190

0.0600 4 . 559E+00 8. 123E-03 4 . 568E+00 7.653E-03 1 . 006E-03 9.251 E-03 -0.168 0.188 0.187

0.0700 4. 107E+00 8. 185E-03 4.11 6E+00 9. 964E-03 1 . 1 31 E-03 1 . 1 39E-02 -0.163 0.183 0.182

0 . 0800 3.761E+00 8.248E-03 3.769E+00 1 . 25 1 E-02 1 . 25 1 E-03 1 . 368E-02 -0.160 0.178 0.177

0.0900 3 . 487E+00 8.31 7E-03 3 . 496E+00 1 . 526E-02 1 . 366E-03 1 . 608E-02 -0.157 0.175 0.174

0.1000 3 . 265E+00 8.389E-03 3 . 274E+00 1 .822E-02 1 . 476E-03 1 . 86 1 E-02 -0.154 0.171 0.171 0.1250 2 . 859E+00 8 . 59 1 E-0 3 2 . 867E + 00 2 . 642E-02 1 . 737E-03 2 . 538E-02 -0.149 0.165 0.164

0.1500 2 . 585E+00 8.821 E-0 3 2. 592E+00 3.561 E-02 1 . 981 E-03 3.271 E-02 -0.145 0.160 0.159

0.1750 2. 385E+00 9.076E-03 2 . 394E+00 4.566E-02 2.21 2E-03 4.050E-02 -0.141 0.156 0.155

0.2000 2 . 236E+00 9 . 349E-03 2 . 245E+00 5 . 646E-02 2 . 433E-03 4 . 868E-02 -0.133 0.153 0.152

0.2500 2 . 028E+00 9.951E-03 2 . 0 38E+00 7.991 E-02 2 . 852E-03 6 .592E-02 -0.133 0.148 0.147

0 . 3000 1 . 8 92E+00 1 .062E-02 1 . 903E+00 1 . 054E-0

1

3.248E-03 8 . 402E-02 -0.129 0.143 0.142

0.3500 1 . 797E+00 1 . 133E-02 1 . 30 9E+00 1 . 323E-0

1

3.631 E-03 1 . 027E-0

1

-0.125 0.140 0.138

0.4000 1 . 729E+00 1 .209E-02 1 . 74 1 E+00 1 . 606E-0

1

4 . 003E-03 1 .216E-01 -0.122 0.137 0.135

0.4500 1 . 677E+00 1 -290E-02 1 , 6 90E+00 1 . 897E-0

1

4.368E-03 1 .407E-01 -0.119 0.134 0.132

0.5000 1 . 638E+00 1 . 374E-02 1 . 652E+00 2.1 97E-01 4.72SE-03 1 .599E-01 -0.116 0.132 0.129

0.5500 1 . 608E+Q0 1 .461 E-02 1 . 623E+00 2 . 502E-0

1

5.085E-03 1 . 7 90 E-0

1

-0.114 0.130 0.127 0.6000 1 . 585E+00 1 . 551 E-02 1 . 600E+00 2.812E-01 5.441 E-03 1 . 980E-01 -0.112 0.128 0.125

0 . 7000 1 .551E+00 1 . 740 E-02 1 . 568E+00 3 . 444E-0

1

6.148E-03 2.355E-01 -0.108 0.124 0.121 0.8000 1 . 529E+00 1 . 938E-02 1 . 549E+00 4 . 086E-01 6.855E-03 2.721E-01 -0.105 0.121 0.118

0 . 9000 1 . 5 1 6E+00 2. 145E-02 1 . 537E+00 4.734E-01 7 . 564E-03 3 . 077E-0

1

-0.102 0.119 0.115

1 .0000 1 . 507E+00 2 . 360E-02 1 . 531 E+00 5.386E-01 8 . 275E-03 3 . 424E-0

1

-0.100 0.116 0.112

1 .2500 1 . 500E+00 2 . 927E-02 1 . 529E+00 7.022E-01 1 . 007E-02 4.248E-01 -0.094 0.111 0.106

1 .5000 1 . 502E+00 3 . 533E-02 1 . 538E+00 8.652E-01 1 .1 90E-02 5 . 020 E-0

1

-0.090 0.107 0.101

1 .7500 1 . 509E+00 4.171 E-02 1 . 551 E+00 1 . 027E+00 1 . 376E-02 5.747E-01 -0 .086 0.104 0.097

2.0000 1 . 51 8E+00 4.833E-02 1 . 567E+00 1 . 1 88E+00 1 . 565E-02 6 . 439E-0

1

-0.082 0.101 0.094

2.5000 1 . 538E+00 6 . 223E-02 1 . 600E+00 1 . 503E+00 1 . 949E-02 7.743E-01 -0.075 0.096 0.087

3.0000 1 . 558E+0 0 7.682E-02 1 . 634E+00 1 .81 2E+00 2.340E-02 8.976 E-0

1

-0.069 0.091 0.082

3.5000 1 . 575E+00 9.1 97E-02 1 . 667E+00 2.11 5E+00 2.736E-02 1 . 0 1 6E+00 -0.062 0.087 0.076

4.0000 1 .591E+00 1 .076E-01 1 . 699E+00 2.41 2E+00 3.134E-02 1 .131 E+00 -0.057 0.083 0.071 4.5000 1 . 605E+00 1 . 236E-0

1

1 . 729E+00 2 . 704E+00 3 . 535E-02 1 . 243E + 00 -0.051 0.080 0 .067 5.0000 1 . 6 1 8E+00 1 . 399E-01 1 . 758E + 00 2.991 E+00 3. 937E-02 1 . 351 E+00 -0.047 0.076 0.063

5.5000 1 . 629E+00 1 .566E-01 1 . 786E+00 3 . 273E+00 4 . 340E-02 1 . 455E+00 -0.043 0.073 0.059

6.0000 1 . 639E+00 1 . 735E-0

1

1 .81 3E+00 3.551 E+00 4 . 742E-02 1 . 557E+00 -0 . 040 0.070 0.056 7.0000 1 . 657E+00 2.081 E-0

1

1 . 865E+00 4 . 0 95E+00 5 . 546 E-02 1 . 748E+00 -0.034 0.065 0.049

8.0000 1 . 672E+00 2.435E-01 1 . 91 6E+00 4 . 624E+00 6.344E-02 1 . 925E+00 -0.030 0.061 0.045

9.0000 1 . 685E+00 2.795E-01 1 . 965E+00 5 . 1 39E+00 7.136E-02 2 . 088E+00 -0.027 0.058 0.040

10.0000 1 . 697E+00 3.161 E-0

1

2.01 3E+00 5 . 642E+00 7 .91 9E-02 2 . 239E+00 -0.025 0.054 0.037

12.5000 1 .721E+00 4.098E-01 2 . 1 30E+00 6 . 84 9E+0 0 9 . 833E-02 2 . 574 E + 0 0 -0.021 0.048 0.031 15.0000 1 . 740E+00 5 . 057E-0

1

2 . 245E+0 0 7 . 992E+00 1 .168E-01 2 . 858E+00 -0.019 0.044 0.026

17.5000 1 . 756E+00 6.033E-01 2. 359E+00 9 . 078E+00 1 . 345E-0

1

3 . 1 05E+00 -0.017 0.040 0.023

20.0000 1 . 76 9E+0 0 7.023E-01 2 . 472E+00 1 .01 1 E+01 1 .514E-01 3 . 323E+00 -0.016 0.037 0.021 25.0000 1 .791E+00 9.035E-01 2 . S95E+00 1 . 205E+0

1

1 . 832E-0

1

3.694E+00 -0.015 0.033 0.017

30.0000 1 . 80 9E+00 1 . 1 08E+00 2.91 7E+00 1 . 383E+01 2. 123E-01 4 . 003E+00 -0.013 0 .030 0.015

35.0000 1 . 824E+00 1 . 31 4E+00 3 . 1 39E+00 1 . 548E+0

1

2.391 E-0

1

4 . 268E+00 -0.012 0.027 0.013

40.0000 1 . 837E+00 1 . 523E+00 3 . 360E+00 1 . 702E+0

1

2.638E-01 4.501 E+00 -0.011 0.026 0.012

45.0000 1 .848E+00 1 . 733E+00 3.581 E+00 1 . 847E+0

1

2.865E-01 4.709E+00 -0.010 0.024 0.011 50.0000 1 . 858E+00 1 . 944E+00 3 . 802E+00 1 . 982E+0

1

3.077E-01 4 . 897E+00 -0.009 0.023 0.010 55.0000 1 . 866E+00 2. 156E+00 4 . 023E+00 2. 1 10E+01 3.273E-01 5 . 068E+00 -0.009 0.022 0.009

60 . 0000 1 .874E+00 2. 369E+00 4 . 244E+00 2.231 E+0

1

3.457E-01 5 . 226E+00 -0.008 0.021 0.008 70.0000 1 888E+00 2.798E+00 4 . 686E+00 2 . 455E+0

1

3.789E-01 5 . 509E+00 -0.007 0.019 0 .007 80.0000 1 . 900E+00 3 . 230E+00 5 . 1 29E+00 2 . 659E+01 4 . 083E-0

1

5 . 757E+00 -0.006 0.018 0 .006 90.0000 1 . 91 0E+00 3 . 663E+00 5 . 573E+00 2 . 846 E+0

1

4.344E-01 5.979E+00 -0.005 0.017 0.006 100.0000 1 . 9 1 8E+00 4 . 099E+00 6.01 7E+00 3.01 9E+01 4.580E-01 6 . 179E+00 -0.004 0.016 0.005

125.0000 1 . 937E+00 5. 1 93E+00 7.1 30E+00 3 . 400E+0

1

5 . 076E-0

1

6 . 606E+00 -0.003 0.014 0.004

1 50.0000 1 . 952E+00 6 . 294E+00 8 . 246E+00 3 . 726E+0

1

5 . 474E-0

1

6 . 960E+00 -0.002 0.013 0.003

175.0000 1 . 964E+00 7.401 E+00 9 . 365E+O0 4.010E+01 5 .803E-01 7.261 E+00 -0.002 0.012 0.003 200.0000 1 . 975E+00 3.511 E+00 1 . 049E+01 4 . 262E+0

1

6.079E-01 7 . 524E+00 -0.001 0.011 0.002

250.0000 1 . 992E+00 1 . 0 74E+0

1

1 . 273E+0

1

4.694E+01 6 . 520 E-0

1

7 . 964E+00 -0.001 0.010 0.002 300.0000 2 . 006E+00 1 . 298E+0

1

1 . 498E+01 5.056E+01 6 .859E-01 8 . 325E+00 -0.001 0.010 0.001 350.0000 2.01 8E+00 1 . 522E+0

1

1 . 724E+0

1

5 . 367E+0

1

7.129E-01 8.631 E+00 -0.001 0.009 0.001

400 .0000 2 . 029E+00 1 . 747E+0

1

1 . 950E+01 5.639E+01 7 . 350 E-0

1

8 . 897E+00 -0.000 0.009 0.001

450 .0000 2 . 038E+00 1 . 972E+0

1

2. 176E+01 5.882E+01 7 . 535E-0

1

9. 1 31 E+00 -0.000 0.008 0.001 500.0000 2 . 046E+00 2.1 97E+01 2 . 402E+0

1

6.101 E+0

1

7.692E-01 9.341 E+00 -0.000 0.008 0.001 550.0000 2 . 053E+00 2 . 423E+0

1

2 . 628E+0

1

6.299E+01 7.828E-01 9.531 E+00 -0 .000 0.008 0.001 600.0000 2. 060E+00 2 . 648E+0

1

2 . 854E+0

1

6 . 482E+0

1

7. 946E-01 9 . 705E+00 -0.000 0.008 0.001

700 . 0000 2 . 072E+00 3. 100E+01 3. 308E+01 6 .807E+01 8.144E-01 1 .001 E+01 -0.000 0.007 0.001 300.0000 2 . 082E+00 3.553E+01 3.761 E+0

1

7 . 0 90 E+0

1

8 . 302E-0

1

1 . 028E+0

1

-0.000 0.007 0.001 900.0000 2.091 E+00 4 . 006E+01 4.215E+01 7.341 E+0 1 8 . 433E-0

1

1 .051 E+01 - 0.000 0.007 0.000 1000.0000 2.099E+00 4 . 459E+01 4.669E+01 7 . 567E+0

1

8.542E-01 1 . 072E+0

1

- 0.000 0 . 007 0.000

90
ELECTRONS IN ARGON

I = 188.0 eV DENSITY = 1.662E-03 g/cm 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm z/g MeV cm 2/g MeV cm 2 /g g/cm 2 0.0100 1 . 4 97E+0

1

8. 167E-03 1 . 498E+0

1

3.921E-04 2 . 846E-04 0.0 -0.243 0.292 0.284

0.0125 1 .271E+01 8.444E-03 1 .271 E+01 5 . 740E-04 3 . 487E-04 0.0 -0.231 0.274 0.268

0.0150 1 .110E+01 8 . 647E-03 1 .111E + 01 7.849E-04 4.1 08E-04 0.0 -0.222 0.261 0.255 0.0175 9 . 907E+00 8.803E-03 9.91 6E+00 1 .024E-03 4.71 2E-04 0.0 -0.215 0.251 0.246

0 .0200 8. 974E+00 8.926E-03 8 . 983E+00 1 .289E-03 5.299E-04 0 .

0

-0.209 0.243 0.238 0.0250 7 .61 0E+00 9 . 1 07E-03 7.61 9E+00 1 .895E-03 6 . 430E-04 0 .

0

-0.200 0.230 0.226 0.0300 6 . 657E+00 9.237E-03 6 . 666E+00 2.599E-03 7. SI IE-04 0.0 -0.193 0.221 0.218

0.0350 5. 950E+00 9 . 334E-03 5. 959E+00 3.394E-03 8 . 547E-04 0 . 0 -0.187 0.214 0.211 0.0400 5 . 404E+00 9.41 5E-03 5.41 4E+00 4.276 E-03 9.546E-04 0 .

0

-0.183 0.208 0.205

0 .0450 4. 969E + 00 9.482E-03 4 . 973E+00 5 . 240E-03 1 . 051 E-03 0.0 -0.179 0.203 0.200 0.0500 4.61 4E+00 9.540E-03 4 . 623E+00 6 .283E-03 1 . 144E-03 0.0 -0.176 0.199 0.196 0.0550 4.317E+00 9.593E-03 4 . 327E+00 7.402E-03 1 . 235E-03 0 .

0

-0.173 0.195 0.193

0.0500 4 . 067E + 00 9.642E-03 4 . 077E+00 8 . 593E-03 1 . 323E-03 0 .

0

-0.171 0.192 0.190 0.0700 3 . 666E + 00 9.733E-03 3 . 675E+00 1 . 1 18E-02 1 . 492E-03 0 .

0

-0.167 0.186 0.185

0.0800 3 . 358E + 00 9 .821 E-03 3 . 368E+00 1 . 40 3E-0 2 1 . 654E-03 0 .

0

-0.163 0.182 0.180 0.0900 3.1 15E+00 9. 909E-03 3. 125E+00 1 .712E-02 1 . 808E-0 3 0.0 -0.160 0.178 0.177

0.1000 2.918E+00 1 . 000E-02 2 . 928E+0 0 2 . 042E-02 1 . 957E-0 3 0.0 -0.158 0.175 0.174

0.1250 2 . 557E + 00 1 . 025E-02 2 . 567E+00 2 . 958E-02 2.307E-03 0.0 -0.153 0.169 0.168

0.1500 2. 31 2E+00 1 . 052E-02 2 . 323E+00 3 . 985E-02 2.633E-03 0.0 -0.149 0.164 0.163

0.1750 2.136E+00 1 .081E-02 2.1 47E+00 5 . 1 06E-02 2. 940E-03 0 .

0

-0.146 0.160 0.159 0.2000 2 . 004E+00 1.11 3E-02 2.01 5E+00 5.309E-02 3.233E-03 0.0 -0.143 0.157 0.156 0.2500 1 .821E+00 1 . 182E-02 1 . 832E+00 8. 920E-02 3.784E-03 0 .

0

-0.139 0.152 0.151 0.3000 1 .701 E+00 1 . 258E-02 1 . 7 1 3E+00 1 . 1 75E-0

1

4. 303E-03 0 .

0

-0.135 0.148 0.147 0.3500 1 . 6 1 8E+00 1 . 340E-02 1 .631 E+00 1 . 474E-0

1

4.799E-03 0.0 -0.132 0.145 0.143

0.4000 1 . 558E+00 1 .427E-02 1 . 572E+00 1 . 787E-0

1

5 . 280E-03 0 .

0

-0.130 0.142 0.141 0.4500 1 . 51 4E+00 1 .51 9E-02 1 . 529E+00 2.109E-01 5.749E-03 0.0 -0.128 0.140 0.138

0.5000 1 .480E+00 1 . 6 1 6E-02 1 . 497E+00 2.440E-01 6.21 IE-03 0.0 -0.126 0.138 0.136 0.5500 1 . 455E+00 1 .716E-02 1 . 472E+00 2.777E-01 6.667E-03 0.0 -0.124 0.136 0.134

0.6000 1 . 435E+00 1 .820E-02 1 . 453E+00 3.11 9E-01 7.11 9E-03 0.0 -0.122 0.135 0.132

0.7000 1 . 408E+00 2 . 036E-02 1 . 428E+00 3.814E-01 8.015E-03 0 .

0

-0.120 0.132 0.129

0.8000 1 . 391 E+00 2.264E-02 1 .414E+00 4.518E-01 8.905E-03 0.0 -0.117 0.129 0.127

0.9000 1 . 381 E+00 2 . 502E-02 1 . 406E+00 5.227E-01 9.794E-03 0.0 -0.115 0.127 0.124

1 .0000 1 . 376E+00 2.748E-02 1 . 404E + 0 0 5.939E-01 1 . 068E-02 0.0 -0.114 0.126 0.122

1 .2500 1 . 375E+00 3.399E-02 1 . 409E+00 7.718E-01 1 . 291 E-02 0.0 -0.110 0.122 0.118

1 .5000 1 . 383E+0 0 4.094E-02 1 . 424E+00 9.483E-01 1 .517E-02 0 . 0 -0.107 0.119 0.114

1.7500 1 . 394E+00 4.822E-02 1 . 442E+00 1 . 123E+00 1 . 744E-02 0 .

0

-0.105 0.116 0.111 2.0000 1 . 407E+00 5.581E-02 1 . 463E+00 1 . 295E+00 1 . 973E-02 0.0 -0.103 0.114 0.109

2.5000 1 . 434E+00 7. 168E-02 1 .505E+00 1 . 6 32E + 00 2 . 436E-02 0 .

0

-0.099 0.111 0.104

3.0000 1 .460E+00 8.831 E-02 1 . 548E+00 1 . 959E+00 2. 903E-02 0 .

0

-0.097 0.108 0.101 3.5000 1 . 484E+00 1 . 056E-0

1

1 . 589E+00 2 . 278E+00 3 . 370E-02 0.0 -0.095 0.105 0.098

4.0000 1 . 506E+00 1 . 233E-0

1

1 . 629E+00 2 . 589E+00 3 . 837E-02 0 .

0

-0.093 0.103 0.096 4.5000 1 . 526E+00 1 .415E-01 1 . 668E+00 2 . 892E+00 4.303E-02 0.0 -0.092 0.101 0.093

5.0000 1 . 545E+00 1 .600E-01 1 . 705E+00 3. 189E+00 4.766 E-02 0.0 -0.090 0.099 0.091 5.5000 1 . 562E+00 1 .789E-01 1 .741 E+00 3.47 9E+00 5.227E-02 0.0 -0.089 0.098 0.090 6.0000 1 .579E+00 1 . 981 E-01 1 . 777E+00 3 . 763E+00 5.634E-02 0.0 -0.088 0.096 0.088

7.0000 1 . 608E+00 2.373E-01 1 . 845E+00 4.31 5E+00 6 . 588E-02 0.0 -0.087 0.094 0.085 8.0000 1 . 634E+00 2.773E-01 1.911 E+00 4 . 848E+00 7.476 E-02 0.0 -0.085 0.092 0 . 083 9.0000 1 . 657E+00 3.181 E-01 1 . 975E+00 5 . 363E+00 8 . 347E-02 0.0 -0.084 0.090 0.080 10.0000 1 . 678E+00 3.595E-01 2 . 0 37E+00 5.861 E+00 9 . 200E-02 0.0 -0.083 0.088 0.078 12.5000 1 . 722E+00 4.651 E-01 2. 187E+00 7 . 045E+00 1 .126E-01 0.0 -0.081 0.084 0.074

15.0000 1 . 759E+00 5.733E-01 2 . 332E+00 8. 1 51 E+00 1 . 320E-0

1

0.0 -0.079 0.081 0.070

17.5000 1 . 790E+00 6 . 833E-0

1

2 . 474E+00 9.1 92E+00 1 . 505E-0

1

0.0 -0.077 0.079 0.067 20.0000 1 .81 8E+00 7.949E-01 2.61 3E+00 1 .018E+01 1 . 680E-0

1

0.0 -0.076 0.076 0.064 25.0000 1 . 864E+00 1 .021 E+00 2 . 885E+00 1 . 200E+01 2.004E-01 0.0 -0.074 0.072 0.060 30.0000 1 . 90 1 E+00 1 . 251 E+00 3.152E+00 1 .365E+01 2.296E-01 6 . 376E-04 -0.071 0.069 0.056 35.0000 1 . 931 E+00 1 . 484E+00 3.41 5E+00 1 .518E+01 2.563E-01 2.31 IE-02 -0.063 0.066 0.052

40.0000 1 . 956E+00 1 . 7 1 8E+00 3 . 674E+00 1 . 659E+01 2 . 807E-0

1

6 . 443E-02 -0.057 0.063 0.048 45.0000 1 . 977E+00 1 . 954E+00 3.931 E+00 1 . 790E+01 3.031 E-0

1

1 . 1 44E-01 -0.053 0.061 0.045 50.0000 1 . 995E+00 2 . 1 92E+00 4 . 1 87E+00 1 .913E+01 3.238E-01 1 . 680E-0

1

-0 .050 0.059 0.042

55.0000 2.01 1 E+00 2 . 430E+00 4.441 E+00 2 . 029E+0

1

3.431 E-0

1

2 . 226 E-0

1

-0.048 0.056 0.039

60.0000 2 . 025E+00 2 . 6 70E+0 0 4 . 695E+00 2. 1 39E+01 3.610E-01 2.769E-01 -0.046 0.055 0.037 70.0000 2 . 050E+00 3 . 1 52E+00 5 . 202E+00 2.341 E+0

1

3. 934E-01 3 . 820 E-0

1

-0 .043 0.052 0.033 80.0000 2.071 E+00 3 . 6 37E+00 5 . 708E+00 2 . 525E+0

1

4 . 220E-0

1

4.807E-01 -0.041 0.049 0.030 90.0000 2.089E+00 4 . 1 25E+00 6 .21 4E+00 2.692E+01 4.474E-01 5 . 729E-01 -0.040 0.047 0.027 100.0000 2. 105E+00 4.61 4E+00 6.71 9E+00 2 . 847E+0

1

4.702E-01 6 . 588E-0

1

-0.038 0.045 0.025

125.0000 2.1 38E+00 5.845E+00 7 . 982E+00 3. 188E+01 5. 183E-01 8.51 OE-OI -0.036 0.041 0.021

1 50.0000 2.164E+00 7 . 083E+00 9 . 247E+00 3.479E+01 5.569E-01 1 . 0 1 8E+00 -0.034 0.039 0.018 175.0000 2. 185E+00 8 . 326E+00 1 .051 E+01 3 . 732E+0

1

5 . 887E-0

1

1 . 1 66E+00 -0.032 0.036 0.016 200.0000 2 . 204E+00 9 . 573E+00 1 . 178E+01 3 . 957E+0

1

6.155E-01 1 . 301 E+00 -0.030 0.035 0.015 250.0000 2 . 234E+00 1 . 208E+0

1

1 .431 E+01 4.341 E+0

1

6 . 583E-01 1 . 54 1 E+00 -0.027 0.032 0.012 300.0000 2 . 257E+00 1 .459E+01 1 . 685E+0

1

4.663E+01 6.911 E-0

1

1 . 754E+00 -0.024 0.030 0.010 350.0000 2 . 275E+00 1 .71 1E+01 1 . 933E+0

1

4. 940E+01 7.174E-01 1 . 947E+00 -0.021 0 .029 0.009 400.0000 2.291 E+00 1 . 963E+0

1

2.1 92E+01 5.182E+01 7.389E-01 2 . 1 25E+00 -0.019 0.027 0.008

450 .0000 2 . 304E+00 2.216E+01 2 . 446E+0

1

5 . 398E+0

1

7.569E-01 2 . 290E+00 -0.017 0 .026 0.007 500.0000 2.31 5E+00 2.469E+01 2 . 700E+01 5.592E+01 7.722E-01 2 . 444E+00 -0.016 0 .026 0.007 550.0000 2 . 325E+00 2.722E+01 2 . 954E+0

1

5.769E+01 7.854E-01 2 . 587E+00 -0.014 0.025 0.006 600.0000 2 . 334E+00 2.975E+01 3.209E+01 5. 932E+01 7.970 E-0

1

2.721 E+00 -0.013 0.024 0.006 700.0000 2.349E+00 3 . 483E+0

1

3.718E+01 6 . 22 1 E+0

1

8.163E-01 2 . 966E+00 -0.011 0.023 0.005 800.0000 2.361 E+00 3.990E+01 4 . 227E+0

1

6 -473E+01 8.31 9E-01 3. 184E+00 -0.010 0.022 0.004

900.0000 2 . 372E+00 4 . 499E+0

1

4 . 736E+0

1

6.696E+01 8.447E-01 3 . 380 E+00 -0.009 0.021 0.004

1 000.0000 2 . 382E+00 5.007E+01 5.245E+01 6 . 897E+0

1

8 . 554E-0

1

3 . 558E+00 -0.009 0.021 0.003

91
ELECTRONS IN TITANIUM

I = 233.0 eV DENSITY = 9 . 590E+0 0> g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log1 )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2/g MeV cm 2/g g/cm 2 0.0100 1 . 997E+01 9.835E-03 1 . 997E + 0

1

9.109E-09 3.509E-09 2 . 037E-03 -0.256 0.313 0.303

0.0125 1 .231E+01 1 . 025E-02 1 . 232E+0

1

5. 983E-09 9.31 9E-09 2.585E-03 -0.292 0.293 0.289

0.0150 1 . 0 78E+0

1

1 . 056E-02 1 . 079E+01 8.157E-09 5. 109E-09 3.198E-03 -0.232 0.278 0 . 270 0.0175 9 . 639E+00 1 .080E-02 9 . 699E+00 1 .061 E-0 3 5 . 878E-09 3.727E-03 -0.229 0.266 0.259

0.0200 8 . 737E + 00 1 -099E-02 8 . 798E+00 1 . 339E-03 6 .629E-09 9.320E-03 -0.218 0 .257 0.250 0.0250 7 . 929E+00 1 . 1 29E-02 7 . 935E+00 1 . 956E-03 8.081E-09 5 . 55 1 E-0 3 -0.208 0.293 0.237

0.0300 6 . 503E + 00 1 . 1 50E-02 6.519E+00 2 . 677E-03 9 . 972E-09 6 . 833E-0 3 -0.200 0.232 0.227

0.0350 5.81 9E+00 1 . 167E-02 5 .831 E+00 3 . 990E-03 1 .081 E-03 8. 181 E-03 -0.199 0.229 0.220

0.0900 5 . 290E+00 1 . 180E-02 5 . 30 1 E+00 9 . 390E-03 1 .210 E-03 9.578E-03 -0.189 0.217 0.219

0 .0450 9.867E+00 1 . 1 92E-02 9.87 9E+00 5 . 375E-03 1 . 335E-03 1 . 1 03E-02 -0.185 0.212 0.203

0.0500 9 . 522E+00 1 . 202E-02 9 . 539E+00 6 . 939E-0 3 1 . 9 56 E-0 3 1 . 253E-02 -0.181 0.207 0 . 209 0.0550 9 . 239E+00 1 .210E-02 9 . 296E+00 7 .579E-03 1 .579E-03 1 .907E-02 -0.178 0.203 0.200 0.0600 3. 990E+00 1 .218E-02 9 . 002E+00 8.793E-03 1 .689E-03 1 . 567E-02 -0.175 0.199 0.196 0.0700 3 . 598E + 00 1 . 233E-02 3.611 E+00 1 . 193E-02 1 . 909E-03 1 .899E-02 -0.170 0.193 0.191 0.0800 3 . 298E + 0 0 1 .296E-02 3.31 1E+00 1 . 933E-02 2.11 9E-03 2 . 297E-02 -0.166 0.188 0.186

0.0900 3.060E+00 1 . 259E-02 3 . 073E+00 1 . 796E-02 2.321 E-03 2.611 E-02 -0.163 0.183 0.182

0.1000 2 . 867E+00 1 . 272E-02 2 . 880E+00 2.083E-02 2.519E-03 2 . 987E-02 -0.160 0.180 0.178

0.1250 2.519E+00 1 .306E-02 2 . 527E+00 3.013E-02 2.971 E-03 3 . 978E-02 -0.153 0.172 0.171 0.1500 2 . 279E+00 1 .391E-02 2 . 287E+00 9 . 056E-02 3 . 396 E-0 3 5 . 023E-02 -0.198 0.166 0.165

0.1750 2. 101E+00 1 . 379E-02 2.1 15E+00 5.1 95E-02 3 . 796E-03 6 . 1 05E-02 -0.199 0.162 0.160

0.2000 1 .971E+00 1 .91 9E-02 1 . 985E+00 6 . 9 1 6 E-02 9.176 E-03 7.212E-02 -0.190 0.158 0.156

0.2500 1 . 78 9E+0 0 1 . 506E-02 1 . 809E+00 9 . 067E-02 9 . 892E-03 9.967E-02 -0.139 0.151 0.150

0.3000 1 . 670E + 00 1 .600E-02 1 . 686E+00 1 . 1 99E-01 5.563E-03 1 . 1 79E-01 -0.129 0.196 0.195

0.3500 1 . 588E+00 1 . 702E-02 1 . 605E+00 1 .998E-01 6.209E-03 1 . 902E-01 -0.125 0.192 0.190 0.9000 1 . 528E+00 1 .81 IE-02 1 . 596E+00 1 .81 6E-01 6 . 829E-03 1 .629E-01 -0.121 0.138 0.136

0.9500 1 . 983E+00 1 . 925E-02 1 . 502E+00 2.1 99E-01 7.928E-03 1 . 855E-0

1

-0.118 0.135 0.133

0.5000 1 . 999E+00 2 . 099E-02 1 . 970E+00 2.981 E-01 8 . 021 E-03 2 . 080 E-0

1

-0.115 0.133 0.130 0.5500 1 . 923E+00 2. 1 69E-02 1 . 995E+00 2.829E-01 8.607E-03 2 . 309E-0

1

-0.112 0.130 0.127

0.6000 1 . 902E+00 2 . 297E-02 1 . 925E+00 3.173E-01 9. 186E-03 2.526E-01 -0.109 0.128 0.129

0.7000 1 -373E+00 2. 566E-02 1 . 399E+00 3.881 E-01 1 . 039E-02 2.969E-01 -0.109 0 . 1 23 0.120

0.8000 1 . 355E+0 0 2 . 898E-02 1 . 383E+00 9.601 E-0

1

1 .198E-02 3.907E-01 -0.100 0.120 0.116

0 . 9000 1 . 393E+00 3. 1 91 E-02 1 . 379E+00 5.326E-01 1 . 26 1 E-02 3.891 E-01 -0.096 0.116 0.112

1 .0000 1 . 335E+0 0 3 . 996E-02 1 . 370E+00 6 . 055E-01 1 . 375E-02 9 . 270E-01 -0.092 0.113 0.108

1 .2500 1 . 328E+00 9 . 250E-02 1 . 371 E+00 7.881 E-01 1 . 662E-02 5.317E-01 -0.089 0.107 0.100

1 .5000 1 . 330E+00 5. 107E-02 1 .381 E+00 9.699E-01 1 . 951 E-02 6.321 E-01 -0.078 0.102 0.099

1 .7500 1 . 336E+00 6 .006E-02 1 . 396E+00 1 . 1 50E+00 2.299E-02 7.277E-01 -0.073 0.097 0.089

2.0000 1 . 393E+00 6 . 990E-02 1 . 9 1 2E+00 1 . 328E+00 2 . 539E-02 8. 183E-01 -0.070 0.093 0.089

2.5000 1 .359E+00 8.899E-02 1 . 998E+00 1 . 678E+00 3.137E-02 9 . 855E-0

1

-0.069 0 .087 0.076

3.0000 1 . 376E+00 1 . 0 99E-0

1

1 . 985E+00 2.01 9E+00 3.790E-02 1 . 1 36E+00 -0.060 0.082 0.071 3.5000 1 .391 E+00 1 .306E-01 1 . 521 E+00 2 . 35 1 E+00 9.395E-02 1 . 271 E+00 -0.057 0.078 0.066

9.0000 1 . 905E+00 1 . 523E-0

1

1 . 557E+00 2 . 676E+00 9 . 999E-02 1 . 395E+00 -0.059 0.075 0 .063 9.5000 1 . 91 8E+00 1 .796E-01 1 . 593E+00 2. 993E+00 5 . 552E-02 1 . 509E+00 -0.052 0.072 0 .059 5.0000 1 . 930E+00 1 . 979E-0

1

1 . 627E+00 3 . 309E+00 6 . 1 52E-02 1 . 6 1 5E+00 -0.050 0.069 0.057

5.5000 1 . 99 1 E+00 2.205E-01 1 .661 E+00 3 . 608E+00 6.797 E-02 1 .71 3E+00 -0.098 0.067 0 .059 6.0000 1 .951 E+00 2.990E-01 1 . 6 95E+00 3 . 906E+00 7. 337E-02 1 . 806E+00 -0.097 0.065 0.052

7.0000 1 . 96 9E + 00 2.919E-01 1.761 E+00 9 . 985E+00 8 . 502E-02 1 . 975E+00 -0.099 0.062 0.099 8.0000 1 . 985E+00 3.908E-01 1 .825E+00 5 . 092E+00 9 . 693E-02 2. 129E+00 -0.091 0.059 0.095

9.0000 1 . 998E+00 3.906E-01 1 . 889E+00 5.581 E+00 1 .076E-01 2.271 E+00 -0.038 0.056 0.093

10.0000 1 .51 0E+00 9.91 IE-01 1 . 952E+00 6. 102E+00 1 . 185E-01 2.902E+00 -0.036 0.059 0 . 090 12.5000 1 .535E+00 5.701E-01 2 . 1 05E+00 7 . 335E+00 1 . 995E-0

1

2 . 6 96E + 00 -0.030 0.099 0.035

15.0000 1 . 555E + 00 7.01 9E-01 2 . 257E+00 8.981 E+00 1 . 690E-0

1

2. 953E+00 -0.026 0.095 0.031 17.5000 1 . 57 1 E+00 8.361E-01 2 . 907E+00 9 . 559E+00 1 . 91 9E-01 3. 182E+00 -0.023 0.092 0.027 20.0000 1 . 589E+00 9.721 E-0

1

2 . 556 E+00 1 . 056E+0

1

2.1 39E-01 3 . 388E+0 0 -0.020 0.039 0 . 029 25.0000 1 . 606E+00 1 . 298E+00 2 . 859E+00 1 .291 E+0

1

2.527E-01 3 . 796 E+0 0 -0.016 0.035 0.020

30.0000 1 . 622E+00 1 . 528E+0 0 3. 150E+00 1 . 908E+0

1

2.875E-01 9 . 050E+00 -0.019 0.032 0.017

35.0000 1 . 636E+00 1 .81 1E+00 3 . 997E+00 1 . 560E+0

1

3. 187E-01 9.31 3E+00 -0.013 0.029 0.019 90.0000 1 . 698E+00 2.096E+00 3 . 799E+00 1 . 6 9 9E + 0

1

3.967E-01 9 . 595E+00 -0.011 0.027 0.013

95.0000 1 . 658E+00 2. 389E+00 9 . 0 92E+00 1 . 827E+0

1

3.721 E-0

1

9 . 752E+00 -0.010 0.026 0.011 50.0000 1 . 667E+00 2 . 673E+00 9 . 390E+00 1 . 996E+01 3. 952E-01 9. 939E+00 -0.010 0.029 0.010 55.0000 1 . 675E+00 2. 963E+00 9 . 639E+00 2.058E+01 9. 1 63E-01 5. 1 I 0 E+00 -0.009 0.023 0.009

60.0000 1 . 683E+00 3 . 255E+00 9. 938E+00 2 . 1 62E+01 9.357E-01 5 . 266E+00 -0.009 0.022 0.009

70.0000 1 . 6 96 E+0 0 3.893E+00 5 . 538E+00 2 . 353E+0

1

9.702E-01 5 . 597E+00 -0.008 0.021 0.007 80.0000 1 . 707E+00 9 . 933E+00 6 . 190E+00 2 . 525E+0

1

5 .OOOE-OI 5 . 792E+0 0 -0.007 0.019 0 .006 90.0000 1 .71 6E+00 5 . 027E+00 6 . 793E+00 2 . 680E+0

1

5.260E-01 6.01 OE+OO -0.006 0.018 0.006 100.0000 1 . 729E+00 5 . 623E+00 7 . 398E+00 2.822E+01 5.990E-01 6 . 206E+00 -0.006 0.018 0.005

125.0000 1 . 792E + 0 0 7 . 1 22E+00 8 . 869E+00 3.1 32E+01 5. 963E-01 6 . 626E+00 -0.005 0.016 0.009

1 50.0000 1 . 756E+00 8.629E+00 1 . 0 39E+0

1

3.392E+01 6.332E-01 6 . 979E+00 -0.009 0.015 0.003

175.0000 1 . 763E+00 1 .019E+01 1 . 1 9 1 E+0

1

3.617E+01 6 . 6 30 E-0

1

7 . 270E+00 -0.003 0.019 0.003

200 .0000 1 . 778E+00 1 . 166E+01 1 . 399E+0

1

3.819E+01 6.87 6 E-0

1

7 . 529EJ-00 -0 .002 0.013 0.003 250.0000 1 . 7 99E + 0 0 1 .971E+01 1 . 6 5 1 E+0

1

9.199E+01 7.262E-01 7. 965E+00 -0.002 0.012 0 .002 300.0000 1 . 308E+00 1 . 777E+0

1

1 . 958E+01 9.927E+01 7.551 E-0

1

8 . 323E+00 -0.001 0.011 0 .002 350.0000 1 .81 9E+00 2 . 089E+0

1

2 . 266E+0

1

9 . 669E+0

1

7 . 778E-0

1

8 . 627E+00 -0.001 0.011 0.001 900.0000 1 . 328E+00 2.391 E+0

1

2.579E+01 9.871 E+0

1

7. 962E-01 8.891 E+00 -0.001 0.010 0.001 950.0000 1 . 837E+00 2.698E+01 2 . 882E+0

1

5.055E+01 8.11 3E-01 9.125E+00 -0.001 0.010 0.001 500.0000 1 .899E+00 3 . 006E+0

1

3 . 1 9 1 E+0

1

5.21 9E+01 8.291 E-0

1

9 . 339E+00 -0.001 0.010 0.001 550.0000 1 .851 E+00 3.315E+01 3 . 500E+0

1

5.369E+01 8.351 E-01 9 . 529E+00 -0.000 0.009 0 .001 600 .0000 1 . 857E+00 3 . 623E+0

1

3.809E+01 5 . 50 6 E + 0

1

8.996E-01 9 . 697E+00 -0.000 0.009 0.001 700.0000 1 .868E+00 9.291 E+0

1

9 , 928E+0 5 5.799E+01 8.603E-01 1 .00 0 E+0

1

-0.000 0.009 0.001

800 . 0000 1 .878E+00 9 . 859E+0

1

5 . 097E+0

1

5. 960E+01 8 . 728E-0

1

1 . 027E+0

1

-0 .000 0.009 0.001 900.0000 1 . 886E+00 5 . 978E+0

1

5 . 666 E+0

1

6.197E+01 3.831 E-0

1

1 . 051 E+0

1

-0 .000 0.008 0.001 1000.0000 1 . 893E+00 6 . 097E+0

1

6 . 286E+0

1

6.315E+01 8. 916E-01 1 . 072E+01 -0.000 0.008 0.001

92
ELECTRONS IN IRON

I = 286.0 eV DENSITY = 7 . 874E+001 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log1 )/d( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cra 2 /g MeV cm 2 /g g/cra 2 0.0100 1 . 388E+0

1

1 . 138E-02 1 . 390E+01 4 . 329E-04 4.203E-04 2 . 474E-0 3 -0.270 0 . 338 0.324 0.0125 1 . 185E+01 1 . 1 93E-02 1 . 186E+01 6 . 284E-04 5. 138E-04 3 . 1 57E-03 -0.255 0.314 0 . 302 0.0150 1 . 040 E + 0

1

1 . 235E-0 2 1 .041 E+01 8 . 539E-04 6.151 E-04 3 .866E-03 -0.244 0.297 0.286 0.0175 9.31 OE+OO 1 .269E-02 9 . 323E + 0 0 1 . 108E-03 7.092E-04 4.602E-03 -0.235 0.234 0.274 0.0200 8 . 456E+00 1 .296E-02 8.469E+00 1 . 390E-03 8.01 3E-04 5.365E-03 -0.228 0.273 0.264

0.0250 7.1 99E+00 1 . 338E-02 7.21 3E+00 2 . 032E-03 9 . 800 E-04 6 . 975E-03 -0.217 0.257 0.249 0.0300 6 . 31 6E+00 1 .369E-02 6 . 330E+00 2 . 774E-03 1 . 1 52E-03 8 . 6 96 E-0 3 -0.209 0.245 0.239

0.0350 5 . 658E+00 1 .394E-02 5 . 672E+00 3.610 E-0 3 1 .317E-03 1 . 053E-02 -0.202 0.235 0.230 0.0400 5. 149E+00 1 .414E-02 5 . 1 63E+00 4.536E-03 1 . 478E-03 1 . 248E-02 -0.196 0.228 0.223

0.0450 4.741 E+00 1 .431 E-02 4 . 756E + 00 5. 546E-03 1 . S33E-03 1 .455E-02 -0.192 0.222 0.217 0.0500 4 . 408E+00 1 . 446E-02 4 . 422E + 00 6.637E-03 1 . 784E-0 3 1 .673E-02 -0.188 0.216 0.212

0.0550 4. 129E+00 1 .459E-02 4. 144E+00 7 . 80 6 E-0 3 1 . 930E-03 1 . 902E-02 -0.184 0.212 0.208

0.0600 3.893E+00 1 .471 E-02 3 . 908E+00 9.050E-03 2 . 073E-03 2.1 43E-02 -0.181 0.207 0.204

0 .0700 3.51 4E+00 1 .493E-02 3 . 529E+00 1 . 1 75E-02 2.348E-03 2.657E-02 -0.175 0.200 0.198

0.0800 3 . 223E+00 1 .512E-02 3 . 238E+0 0 1 . 471 E-02 2.61 1 E-0 3 3.21 IE-02 -0.170 0.195 0.192 0.0900 2. 992E+00 1 . 531 E-02 3 . 007E+00 1 .792E-02 2.863E-03 3.801 E-02 -0.166 0.190 0.187

0.1000 2 . 804E+00 1 . 548E-02 2 . 820E+00 2 . 1 36E-02 3.106E-03 4.422E-02 -0.162 0.185 0.183

0.1250 2.460E+00 1 . 593E-02 2 . 476E+00 3 . 085E-02 3.679E-03 6 .070E-02 -0.154 0.177 0.175

0.1500 2 . 226E+00 1 .639E-02 2 . 242E+00 4. 149E-02 4.212E-03 7 . 794E-02 -0.148 0.170 0.168

0.1750 2 . 057E+00 1 .687E-02 2 . 074E+00 5.31 0E-02 4.714E-03 9.53SE-02 -0.143 0.164 0.162

0.2000 1 . 930E+00 1 . 736E-02 1 . 947E+00 6 . 556E-02 5.1 90E-03 1 . 127E-01 -0.139 0.160 0.158

0.2500 1 . 7 53E + 0 0 1 . 842E-02 1 . 77 1 E+00 9 . 257E-02 6 . 085E-03 1 . 467E-0

1

-0.133 0.152 0.151 0.3000 1 . 636E+00 1 . 956E-02 1 . 656E+00 1 . 2 1 8 E-0

1

6 . 923E-03 1 .797E-01 -0.128 0.147 0.145

0 . 3500 1 . 556 E + 00 2 . 079E-02 1 . 576E+00 1 . 528E-0

1

7 . 720E-03 2.1 1 6E-01 -0.124 0.142 0.140 0.4000 1 . 497E+00 2 . 209E-02 1 .51 9E+00 1 .851 E-0

1

8.489E-03 2.427E-01 -0.120 0.138 0.136

0 . 4500 1 . 453E + 0 0 2.346E-02 1 . 477E+00 2. 186E-01 9 . 236E-03 2.731 E-0

1

-0.117 0 . 1 35 0.133 0.5000 1 . 420E+00 2.489E-02 1 . 445E+00 2.528E-01 9. 968E-03 3.027E-01 -0.114 0.132 0.129

0.5500 1 . 394E+00 2 . 638E-02 1 . 421 E+00 2.877E-01 1 . 06 9E-02 3.317 E-0

1

-0.112 0.130 0.127 0.6000 1 . 374E+00 2 . 7 9 1 E-02 1 . 402E+00 3.231 E-0

1

1 . 1 40E-02 3.601 E-0

1

-0.109 0.127 0.124

0.7000 1 . 345E+00 3.11 2E-02 1 . 376E+00 3. 952E-01 1 . 281 E-02 4.1 52E-01 -0.105 0.123 0.120

0.8000 1 . 327E+00 3 . 448E-02 1 . 362E+00 4.683E-01 1 . 420 E-02 4.682E-01 -0.101 0.120 0.116

0 . 9000 1 . 3 1 6E+00 3 . 797E-02 1 . 354E+00 5.420E-01 1 . 559E-02 5. 1 95E-01 -0.098 0.117 0.112

1 .0000 1 . 308E+00 4 . 1 60E-02 1 . 350E+00 6.159E-01 1 . 6 97E-02 5 . 6 90 E-0

1

-0.095 0.114 0.109

1 .2500 1 . 302E+00 5.117E-02 1 . 353E+00 8.01 IE-01 2 . 044E-02 6 . 865E-0

1

-0.088 0.108 0.102

1 .5000 1 . 304E+00 6.137E-02 1 . 365E+00 9 . 85 1 E-0

1

2.393E-02 7.. 962E-01 -0.082 0.103 0.096

1 .7500 1 . 31 OE+OO 7 . 206E-02 1 . 382E+00 1 . 167E+00 2 . 745E-02 8 . 990E-01 -0.077 0.099 0.091 2.0000 1 . 3 1 7E+00 8.31 5E-02 1 . 400E+00 1 . 347E+00 3.099E-02 9. 959E-01 -0.073 0.095 0.086 2.5000 1 . 333E+00 1 .063E-01 1 . 440E+00 1 . 6 99E + 00 3.81 2E-02 1 . 1 74E+00 -0.067 0.089 0.079

3.0000 1 . 349E+00 1 . 306E-01 1 . 480 E+00 2. 042E+00 4.527E-02 1 . 333E+00 -0.062 0 . 084 0.073

3.5000 1 . 365E+00 1 .557E-01 1 . 520 E+0 0 2 . 375E+00 5 . 243E-02 1 . 478E+00 -0.059 0.080 0.068

4.0000 1 . 378E+00 1 .814E-01 1 . 560E+00 2 . 700E+00 5 . 954E-02 1 . 6 1 OE+OO -0.056 0.076 0.064

4.5000 1 . 391 E+00 2.077E-01 1 . 599E+00 3 . 0 1 6 E + 0 0 6.661 E-02 1 . 730E+00 -0.054 0.073 0.061 5.0000 1 . 40 3E + 00 2.346E-01 1 . 638E+00 3 . 325E+00 7.361 E-02 1 . S42E+00 -0.052 0.071 0.058

5.5000 1 . 4 1 4E+00 2.61 9E-01 1 . 676E+00 3 . 627E+0 0 8.053E-02 1 . 946E+00 -0.050 0.069 0.056 6.0000 1 . 424E+00 2.896E-01 1 .71 3E+00 3 . 922E+00 8 . 738E-02 2 . 043E+00 -0.049 0.066 0.053 7.0000 1 . 442E+00 3.460E-01 1 . 738E+00 4 . 493E+00 1 . 008E-0

1

2.21 9E+00 -0.046 0.063 0.050 8.0000 1 . 457E+00 4.036E-01 1 .861 E+00 5 . 042E+00 1 . 1 39E-01 2 . 377E+00 -0.044 0.060 0.047

9.0000 1 .471E+00 4.622E-01 1 . 933E+00 5.569E+00 1 . 266E-0

1

2.521 E+00 -0.042 0.057 0.044

10.0000 1 . 483E+00 5.216E-01 2 . 005E+00 6 . 077E+00 1 .389E-01 2 . 652E+00 -0.040 0.055 0.041 12.5000 1 .5C9E+00 6.731 E-0

1

2. 182E+00 7 . 272E+00 1 . 63 1 E-0

1

2 . 942E+0 0 -0.036 0.051 0.037

15.0000 1 . 529E+00 3.279E-01 2 . 357E+00 8 . 374E+00 1 .951 E-0

1

3. 1 92E+00 -0.032 0.047 0.033

1 7 . 5000 1 . 546E+00 9.852E-01 2.531 E+00 9 . 397E+00 2.202E-01 3.41 2E+00 -0.029 0 .044 0.029

20.0000 1 . 560E+00 1 . 145E+00 2 . 704E+00 1 . 0 35E+0

1

2.435E-01 3 . 6 1 0 E + 0 0 -0.026 0.041 0.027 25.0000 1 . 583E+00 1 . 468E+00 3 . 0 50 E + 0 0 1 .209E+01 2.854E-01 3. 956E+00 -0 .021 0.037 0.022 30.0000 1 . 600E+00 1 . 795E+00 3 . 396E+00 1 . 365E+0

1

3.221 E-0

1

4.251 E+00 -0.018 0.034 0.019

35.0000 1 . 6 1 5E+00 2. 126E+00 3.741 E+00 1 .505E+01 3.546E-01 4 . 508E+00 -0.016 0.032 0.016 40.0000 1 . 627E+00 2 . 460E+00 4 . 087E+00 1 . 6 33E+0

1

3.834E-01 4 . 736E+00 -0.014 0.030 0.014 45.0000 1 . 6 38E+0 0 2 . 7 97E+00 4 . 434E+00 1 . 750E+0

1

4.094E-01 4.941 E+00 -0.013 0.028 0.013

50.0000 1 . 647E+00 3.1 35E+00 4 . 782E + 0 0 1 . 859E+0

1

4 . 328E-01 5 . 1 26E+00 -0.012 0.027 0.012

55.0000 1 . 655E+00 3 . 475E+00 5. 130E+00 1 . 959E+01 4 . 54 0 E-0

1

5 . 295E+00 -0.011 0.025 0.011 60.0000 1 . 663E+00 3 . 8 1 6 E+0 0 5.479E+00 2 . 054E+0

1

4.735E-01 5 . 45 1 E + 0 0 -0.010 0.024 0.010 70.0000 1 . 676E+00 4.503E+00 6 . 1 78E+00 2 . 226E+0

1

5 . 077 E-0

1

5.729E+00 -0.009 0 .023 0 .008 80.0000 1 . 687E+00 5. 1 93E+00 6 . 880E+00 2.379E+01 5 . 37 0 E-0

1

5. 973E+00 -0.008 0.021 0.007

90.0000 1 . 6 97E+00 5 . 887E+00 7 . 584E+00 2.517E+01 5.625E-01 6 . 189E+00 -0.008 0.020 0.006 100.0000 1 . 705E+00 6 . 584E+00 3 . 289E+00 2 . 643E+01 5.848E-01 6 . 384E+00 -0.007 0.019 0 .006 125.0000 1 . 723E+00 8 . 336E+00 1 . 006E+0

1

2.917E+01 6 . 303E-0

1

6 .801 E+00 -0.006 0.018 0.005

150.0000 1 . 7 33E+0 0 1 .010E+01 1 . 184E+01 3. 146E+01 6 .655E-01 7 . 1 46 E + 00 -0 .005 0.017 0.004 175.0000 1 . 750E+00 1 . 187E+01 1 . 362E+0

1

3 . 342E+0

1

6.937E-01 7 . 440E+00 -0.004 0.016 0.003 200.0000 1 . 76 0 E+0 0 1 . 364E+0

1

1 . 540E+0

1

3.515E+01 7. 1 69E-01 7 . 6 96 E + 0 0 -0.004 0.015 0.003 250.0000 1 . 777E+00 1 .720E+01 1 . 8 98E + 0

1

3 . 807E+0

1

7.528E-01 8. 128E+00 -0.003 0.014 0.002 300.0000 1 . 79 1 E+00 2.077E+01 2.256E+01 4 . 048E+0

1

7.797E-01 8 . 484E+00 -0.002 0.013 0.002 350.0000 1 . 802E+00 2.435E+0

1

2.615E+01 4 . 254E+0

1

8.006E-01 8 . 787E+00 -0.002 0.012 0.002 400.0000 1 .81 2E+00 2 . 793E+0

1

2. 974E+01 4.433E+01 8 . 1 74E-01 9 . 050E+00 -0.001 0.012 0.001 450.0000 1 . 820 E+0 0 3. 152E+01 3 . 334E+0

1

4.592E+01 8.313E-01 9 . 283E+00 -0.001 0.011 0.001 500.0000 1 . 828E+00 3.512E+01 3.694E+01 4 . 734E+01 8 . 430 E-0

1

9.491 E+00 -0.001 0.011 0.001 550.0000 1 .835E+00 3.871E+01 4.055E+01 4.863E+01 8 . 530 E-0

1

9 . 680E+00 -0.001 0.011 0.001 600.0000 1 .841 E+00 4 .231 E+01 4.415E+01 4 . 98 1 E+0

1

8.616E-01 9 . 853E+00 -0.001 0.011 0.001 700.0000 1 . 852E + 0 0 4.951E+01 5.1 37E+01 5. 1 91 E+01 8.758E-01 1 .01 6E+01 -0.001 0.010 0.001 800.0000 1 .862E+00 5 . 673E+0

1

5.859E+01 5 . 373E+0

1

8.871 E-0

1

1 . 043E+01 - 0.000 0.010 0.001 900.0000 1 .87 1 E+00 6 . 394E+0

1

6.581 E+0

1

5 . 534E+0

1

S.963E-01 1 . 066E+01 - 0.000 0.010 0.001 1000.0000 1 .878E+00 7.116E+01 7 . 304E+0

1

5 . 678E+0

1

9.040E-01 1 . 087E+0

1

- 0.000 0.009 0.001

93
ELECTRONS IN COPPER

I = 322.0 eV DENSITY = 8 . 960E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS . EFF. d ( log[ )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2/g MeV cm 2 /g g/cra 2 0.0100 1 .318E+01 1 .213E-02 1 .319E+01 4.601E-04 4.701E-04 1 . 244E-03 -0.280 0 . 354 0.337

0.0125 1 .127E + 01 1 . 277E-02 1 . 1 28E+01 6.658E-04 5.814E-04 1 . 585E-03 -0.263 0.328 0.314

0.0150 9. 904E+00 1 . 327E-02 9.91 7E+00 9 . 028E-04 6 . 904E-04 1 . 938E-03 -0.251 0.310 0.297 0.0175 8 . 874E + 0 0 1 . 366E-02 8 . 837E + 00 1 . 170E-03 7. 972E-04 2. 304E-03 -0.242 0.295 0.284

0.0200 8 . 066E + 00 1 . 399E-02 8 . 080E+00 1 . 46 5E-0 3 9.01 9E-04 2 . 683E-03 -0.235 0.284 0.273

0.0250 6 . 877E+00 1 . 449E-02 6 . 892E+00 2.138E-03 1 . 1 05E-03 3.481E-03 -0.223 0.266 0.257

0.0300 6 . 040E+00 1 . 488E-02 6 . 055E+00 2.914E-03 1 .301E-03 4.334E-03 -0.214 0.253 0.246

0.0350 5.41 6E+00 1 .518E-02 5.431 E+00 3.788E-03 1 .491E-03 5.247E-03 -0.208 0.243 0.237

0.0400 4.931 E+00 1 . 543E-02 4. 947E+00 4.754E-03 1 . 674E-03 6 . 220E-03 -0.202 0.235 0.230

0.0450 4 . 544E+00 1 . 564E-02 4 . 560E+00 5.808E-03 1 . 852E-0 3 7.259E-03 -0.197 0.229 0.224 0.0500 4 . 226 E+00 1 . 583E-02 4 . 242E+00 6 . 946E-03 2 . 025E-03 8.365E-03 -0.193 0.223 0.218

0.0550 3.961 E+00 1 . 600E-02 3 . 977E+00 8.164E-03 2.1 94E-03 9.542E-03 -0.189 0.218 0.214

0.0600 3 . 736E+00 1 .615E-02 3 . 753E+00 9.459E-03 2.358E-03 1 . 080E-02 -0.186 0.214 0.210 0.0700 3 . 375E+00 1 .641E-02 3 . 392E+00 1 . 227E-02 2.674E-03 1 .354E-02 -0.180 0.207 0.203

0.0800 3 . 0 98E+00 1 . 665E-02 3.1 14E+00 1 . 535E-02 2 . 977E-03 1 . 664E-02 -0.175 0.201 0.198

0.0900 2.877E+00 1 . 688E-02 2 . 8 94E+0 0 1 . 368E-02 3.267E-03 2.0! 3E-02 -0.171 0.196 0.193

0.1000 2 . 6 98E+0 0 1 .710E-02 2.71 5E+00 2.225E-02 3.547E-03 2.404E-02 -0.167 0.191 0.189

0.1250 2 . 370E+00 1 . 763E-02 2 . 387E+0 0 3.21 IE-02 4.208E-03 3.583E-02 -0.157 0.182 0.180

0.1500 2. 146E+00 1 .816E-02 2. 164E+00 4.31 4E-02 4.822E-03 5 . 053E-02 -0.149 0.174 0.172

0.1750 1 . 984E+00 1 . 870E-02 2 . 002E+00 5.517E-02 5.401E-03 6 . 758E-02 -0.141 0.168 0.165

0.2000 1 .861 E+00 1 . 926E-02 1 . 88 1 E+00 6 .807E-02 5. 950E-03 8.595E-02 -0.135 0.162 0.159

0.2500 1 .691 E+00 2.045E-02 1 .711 E+00 9.603E-02 6.981E-03 1 .236E-01 -0.127 0.152 0.150 0.3000 1 . 579E+00 2. 172E-02 1 . 6 0 1 E+00 1 .263E-01 7.945E-03 1 . 603E-0

1

-0.121 0.145 0.143

0.3500 1 . 50 1 E+00 2.307E-02 1 . 524E+00 1 . 584E-0

1

8.860E-03 1 . 958E-01 -0.116 0.139 0.137

0.4000 1 . 444E+00 2 . 450E-02 1 .469E+00 1 .918E-01 9.741E-03 2.302E-01 -0.112 0.135 0.132

0.4500 1 . 402E+00 2.600E-02 1 . 428E+00 2.263E-01 1 . 060E-02 2.635E-01 -0.109 0.131 0.127

0.5000 1 . 370 E + 00 2.757E-02 1 . 398E+00 2.61 7E-01 1 .143E-02 2. 958E-01 -0.106 0.127 0.124

0.5500 1 . 345E+00 2.91 9E-02 1 . 375E+00 2. 978E-01 1 .226E-02 3.273E-01 -0.104 0.124 0.121 0.6000 1 . 326E+00 3 . 087E-02 1 . 357E+00 3.345E-01 1 . 307E-02 3.581E-01 -0.101 0.122 0.118

0.7000 1 . 298E+00 3.437E-02 1 . 333E+00 4 . 089E-01 1 . 467E-02 4. I73E-01 -0.097 0.117 0.113

0.8000 1 . 281 E+00 3 . 803E-02 1 .31 9E+00 4.843E-01 1 . 625E-02 4.739E-01 -0.094 0.113 0.109

0 . 9000 1 . 270E+00 4. 185E-02 1 . 31 2E+00 5.604E-01 1 .782E-02 5.280E-01 -0.091 0.110 0.105

1 .0000 1 . 26 3E+0 0 4.580E-02 1 . 309E+00 6.367E-01 1 . 938E-02 5.799E-01 -0.088 0.107 0.102

1 .2500 1 . 257E+00 5.623E-02 1 .31 3E+00 8.276E-01 2 . 328E-02 7.01 IE-01 -0.083 0.101 0.095

1 .5000 1 . 259E+00 6 . 733E-02 1 . 327E+00 1 .017E+00 2.720E-02 3. 121 E-01 -0.078 0.097 0.090

1 .7500 1 .265E+00 7 . 8 96E-02 1 . 344E+00 1 . 204E+00 3.11 3E-02 9.149E-01 -0.074 0.093 0.085

2.0000 1 . 273E+00 9.103E-02 1 . 364E+00 1 .389E+00 3 . 509E-02 1.011 E+00 -0.071 0.090 0.081 2.5000 1 . 289E+00 1 .162E-01 1 . 405E+00 1 . 7 50 E+0 0 4.302E-02 1 . 186E+00 -0.065 0.084 0.075

3.0000 1 . 305E + 00 1 . 425E-0

1

1 . 448E+00 2.101 E+00 5.095E-02 1 .343E+00 -0.060 0.079 0.069

3.5000 1 . 320E+00 1 .697E-01 1 . 490 E+00 2.441 E+00 5.885E-02 1 . 486E+00 -0.056 0.076 0.065

4.0000 1 . 334E+00 1 . 976E-01 1 . 531 E+00 2 . 772E+00 6 . 668E-02 1 . 6 1 7E+00 -0.053 0.072 0.061 4.5000 1 . 346E+00 2.261E-01 1 . 573E+00 3 . 094E+00 7.443E-02 1 . 738E+00 -0.051 0.069 0.058

5.0000 1 . 358E+00 2.552E-01 1 .61 3E+00 3 . 408E+00 8.209E-02 1 . 8 50E+0 0 -0 .049 0.067 0.055

5.5000 1 . 368E+00 2.847E-01 1 . 653E+00 3.71 5E+00 8. 965E-02 1 . 954E+00 -0.047 0.065 0.052

6.0000 1 . 378E + 00 3. 146E-01 1 . 6 93E+00 4.01 3E+00 9.710E-02 2 . 052E+0 0 -0.046 0 .063 0 .050

7 . 0000 1 . 396E+00 3.756E-01 1 . 77 1 E+00 4.591 E+00 1.11 7E-01 2 . 229E+00 -0.043 0.059 0 .046 8.0000 1 .41 1 E+00 4.378E-01 1 . 849E+00 5. 143E+00 1 -258E-01 2. 388E+00 -0.041 0.056 0.043

9.0000 1 . 424E+00 5.009E-01 1 . 925E+00 5 . 673E+00 1 .394E-01 2 . 532E+00 -0.040 0.054 0.041 10.0000 1 . 436E+00 5 . 650E-0

1

2.001 E+00 6 . 1 83E+00 1 . 526E-0

1

2 . 664E+00 -0.038 0.052 0.039

12.5000 1 . 462E+00 7.282E-01 2 . 1 90 E+00 7 . 376E+00 1 .837E-01 2 . 95 1 E + 0 0 -0.035 0.048 0.034

15.0000 1 . 482E+00 8. 949E-01 2 . 377E+00 8 . 472E+00 2.122E-01 3.1 94E+00 -0.033 0.044 0.031 17.5000 1 . 499E+00 1 . 064E+00 2 . 563E+00 9 . 484E+00 2.385E-01 3 . 407E+00 -0 .030 0 .042 0.028 20.0000 1 . 5 1 3E+00 1 . 236E+00 2 . 749E+00 1 . 043E+01 2.623E-01 3 . 597E+00 -0.028 0.039 0.026 25.0000 1 . 537E+00 1 . 583E+00 3. 120E+00 1 .213E+01 3.061 E-01 3 . 927E+0 0 -0.024 0.036 0.022

30.0000 1 . 555E+00 1 . 936E+00 3.491 E+00 1 . 365E+0

1

3.437E-01 4.209E+00 -0.021 0.033 0.019

35.0000 1 . 570E+00 2 . 29 1 E+00 3.861 E+00 1 .501 E+01 3.767E-01 4 . 456E+00 -0.018 0.031 0.017

40.0000 1 . 582E+00 2 . 650E+00 4 . 233E+00 1 . 624E+0

1

4.059E-01 4 . 676E+00 -0.016 0.029 0.015 45.0000 1 . 593E+00 3.01 2E+00 4 . 605E+00 1 . 738E+01 4 . 320E-0

1

4 .874E+00 -0.015 0.027 0.013

50 .0000 1 . 60 3E+00 3 . 375E+00 4 . 978E+00 1 . 842E+0

1

4.554E-01 5 . 054E+00 -0.013 0.026 0.012

55.0000 1 .611 E+00 3 . 740E+00 5.351 E+00 1 . 939E+01 4.766E-01 5.21 9E+00 -0.012 0.025 0.011 60.0000 1 .61 9E+00 4. 107E+00 5 . 725E+00 2 . 029E+0

1

4.959E-01 5 . 372E+00 -0.011 0.024 0.010 70.0000 1 . 632E+00 4 . 844E+00 6 . 476E+00 2.1 93E+01 5.298E-01 5 . 646E+00 -0.010 0.022 0.009 80.0000 1 . 643E+00 5 . 586E+00 7 . 229E+00 2.339E+01 5.587E-01 5 . 886E+0 0 -0.009 0.021 0.008

90.0000 1 . 653E+00 6 . 330E+00 7 . 983E+00 2.471 E+0

1

5.836E-01 6 . 1 OOE+OO -0.008 0 .020 0.007

100.0000 1 .661 E+00 7.079E+00 8 . 740E+00 2.591 E+0

1

6 . 0 54E-0

1

6 . 292E+00 -0 . 008 0.019 0.006 125.0000 1 . 679E+00 8. 953E+00 1 . 064E+0

1

2.850E+01 6.498E-01 6 . 705E+00 -0.006 0.018 0.005

150.0000 1 . 6 94E+00 1 . 085E+0

1

1 . 254E+01 3.066E+01 6 .838E-01 7 . 046E+00 -0.006 0.016 0.004 175.0000 1 . 706E+00 1 . 275E+0

1

1 . 445E+0

1

3 . 25 1 E+0

1

7.110E-01 7 . 336E+00 -0.005 0.016 0.003 200.0000 1 . 7 1 6E+00 1 . 465E+0

1

1 . 637E+0

1

3.414E+01 7.332E-01 7 . 590E + 00 -0.004 0.015 0.003 250.0000 1 . 7 33E+00 1 . 847E+0

1

2.020E+01 3 . 688E+0

1

7 . 676E-01 8.01 7E+00 -0.003 0.014 0.002

300.0000 1 . 747E+00 2.230E+01 2 . 404E+0

1

3. 91 5E+0

1

7. 932E-01 8 . 37 0 E+00 -0.003 0.013 0 .002 350.0000 1 . 758E+00 2.61 3E+01 2 . 789E+0

1

4.108E+01 8.131E-01 8 . 670E+00 -0.002 0.012 0.002 400.0000 1 . 768E+00 2 . 998E+01 3.174E+01 4 . 276E+0

1

8.291E-01 3.931 E+00 -0.002 0.012 0.002 450.0000 1 . 776E+00 3 . 382E+0

1

3 . 560E+0

1

4.424E+01 8.422E-01 9. 1 62E+00 -0.002 0.012 0.001 500.0000 1 . 784 E+0 0 3 . 767E+0

1

3 . 946E+0

1

4 . 558E+0

1

8 . 532E-0

1

9.369E+00 -0.001 0.011 0.001 550.0000 1 . 7 9 1 E+0 0 4.153E+01 4 . 332E+0

1

4.679E+01 8 . 626E-01 9 . 558 E+0 0 -0.001 0.011 0.001 600.0000 1 . 797E+00 4 . 539E+0

1

4.713E+01 4 . 789E+0

1

8.703E-01 9 . 730E+00 -0.001 0.011 0.001 700.0000 1 .803E+00 5.31 1E+01 5.491 E+0

1

4. 985E+01 8.842E-01 1 . 004E+0

1

-0.001 0.010 0.001 300.0000 1 . 81 8E+00 6 . 083E+01 6.265E+01 5 . 1 56 E+0

1

8.948E-01 1 . 030E+01 -0.001 0.010 0.001 900.0000 1 . 326E+00 6 . 856E+0

1

7 . 039E+0

1

5.306E+01 9.034E-01 1 . 053E+0

1

-0.001 0.010 0.001 1000.0000 1 . 833E+00 7 . 629E+0

1

7.81 3E+01 5. 441 E+01 9.106E-01 1 . 074E+0

1

-0.000 0.009 0.001

f

’

94
ELECTRONS IN GERMANIUM

I = 350.0 eV DENSITY = 5 . 323E+0 0 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS. EFT. d ( loo1 )/d ( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2/g MeV cm 2 /g g/cm 2 0.0100 1 . 243E+0

1

1 . 267E-02 1 . 244E+0

1

4 . 908E-04 5 . 1 71 E-04 5. 175E-04 -0.286 0.367 0.347

0.0125 1 . 065E+0

1

1 . 339E-02 1 .066E+01 7 . 087E-04 6.413E-04 6 -632E-04 -0.269 0.540 0.322

0.0150 9 . 367E+00 1 . 395E-02 9.381 E+00 9.593E-04 7 . 631 E-04 8 . 1 52E-04 -0.257 0.319 0 . 304 0.0175 8 . 400E+00 1 . 439E-02 8.41 4E+00 1 .241 E-0 3 8 . 825E-04 9.734E-04 -0.247 0.304 0.291

0 .0200 7 . 641 E+00 1 . 475E-02 7 . 655E+00 1 .553E-03 9 . 996 E-0 4 1 . 1 3SE-03 -0.240 0.292 0.280 0.0250 6.521 E+OQ 1 . 532E-02 6 . 536E+00 2.263E-03 1 .227E-03 1 . 484E-0 3 -0 . 223 0.273 0.263 0.0300 5.731 E+00 1 . 575E-02 5 . 747E+00 3.081 E-0 3 1 . 447 E-0 3 1 . 853E-05 -0.219 0.260 0.251 0.0350 5 . 1 42E+00 1 . 609E-02 5. 158E+00 4.001 E-03 1 . 659E-03 2.244E-03 -0.212 0.249 0.242

0 . 0400 4 . 685E+00 1 . 633E-02 4.701 E+00 5.018E-03 1 .364E-03 2.656E-03 -0.206 0.241 0.235

0 .0450 4.31 8E + 00 1 .663E-02 4 . 335E+00 6. 127E-03 2 . 064E-03 3.089E-03 -0.201 0.234 0.228

0.0500 4.01 8E+00 1 .684E-02 4 . 035E+00 7 . 323E-0 3 2.258E-03 3.541E-03 -0.197 0.228 0.223

0.0550 3 . 768E + 0 0 1 .704E-02 3 . 785E+00 3 . 60 4 E-0 3 2 . 44 7 E-0 3 4.01 3E-03 -0.194 0.223 0.218

0.0500 3 . 555E+0 0 1 . 722E-02 3 . 572E+00 9.964E-03 2 . 6 32E-0 3 4.502E-03 -0.191 0.219 0.214

0.0700 3.21 3E+00 1 . 755E-02 3.231 E+00 1 . 291 E-02 2. 989E-03 5 . 535E-03 -0.185 0.212 0.208

0.0800 2 . 950E+00 1 .784E-02 2. 968E+00 1 .615E-02 3 . 330 E-0 3 6 . 634E-03 -0.181 0.206 0.202

0.0900 2. 742E+00 1.811 E-02 2 . 760E+00 1 . 965E-02 3 . 659E-03 7.795E-03 -0.177 0.201 0.198 0.1000 2 . 572E+00 1 . 837E-02 2.591 E+00 2.339E-02 3. 976E-03 9.014E-03 -0.174 0.197 0.194

0.1250 2 . 262E+00 1 . 900E-02 2.281 E+00 3.371 E-02 4.725E-03 1 . 230E-02 -0.168 0.188 0.186 0.1500 2 . 050E+00 1 . 960E-02 2. 070E+00 4.525E-02 5.422E-03 1 . 588E-02 -0.163 0.182 0.180 0.1750 1 . 898E+00 2 . 020E-02 1 . 918E+00 5 . 782E-02 6 . 077E-03 1 . 973E-02 -0.158 0.177 0.175 0.2000 1 . 783E+00 2.081 E-02 1 . 804E+00 7.127E-02 6 . 6 97E-03 2.381 E-02 -0.155 0.173 0.171 0.2500 1 . 624E+00 2.208E-02 1 . 646E+00 1 . 004E-0

1

7 . 854E-03 3 . 258E-02 -0.149 0.166 0.164

0.3000 1 . 520E+00 2 . 344E-02 1 . 543E+00 1 .318E-01 8. 930E-03 4 . 209E-02 -0.144 0.161 0.159

0 . 3500 1 . 447E+00 2.488E-02 1 . 472E+0 0 1 . 650E-0

1

9. 947E-03 5 . 225E-02 -0.139 0.156 0.154

0.4000 1 . 395E+00 2.641 E-02 1 . 422E+00 1 . 996E-0

1

1 . 092E-02 6 . 300E-02 -0.135 0.153 0.150 0.4500 1 . 357E+00 2 . 802E-02 1 . 385E+00 2.353E-01 1 . 186E-02 7 . 432E-02 -0.132 0.149 0.147

0.5000 1 . 328E+00 2.971 E-02 1 . 357E+00 2.718E-01 1 . 278E-02 8.61 9E-02 -0.128 0.146 0.144

0.5500 1 . 305E+00 3. 146E-02 1 . 337E+00 3.089E-01 1 .369E-02 9 .857E-02 -0.125 0.144 0.141 0.6000 1 . 288E+00 3 . 326E-02 1 . 321 E+00 3.465E-01 1 . 458E-02 1 . 1 14E-01 -0.122 0.141 0.138

0.7000 1 . 263E+00 3 . 702E-02 1 . 300E+00 4.229E-01 1 . 633E-02 1 . 386E-0

1

-0.116 0.137 0.133

0.8000 1 . 248E+00 4.095E-02 1 . 289E+00 5.001 E-0

1

1 .805E-02 1 .673E-01 -0.111 0.133 0.128

0 . 9000 1 . 239E+00 4.504E-02 1 . 284E+00 5 . 779E-0

1

1 . 976E-02 1 . 973E-01 -0.106 0.129 0.124

1 .0000 1 . 234E+00 4.926E-02 1 . 283E+00 6 . 558E-0

1

2.145E-02 2.282E-01 -0.102 0.125 0.120

1 .2500 1 .231 E+00 6.036E-02 1 .291 E+00 8.501 E-0

1

2 . 567E-02 3.083E-01 -0.092 0.118 0.111

1 .5000 1 . 235E+00 7 .21 3E-02 1 . 307E+00 1 . 043E+00 2. 989E-02 3.894E-01 -0.085 0.112 0.103

1 .7500 1 . 242E+00 8 . 442E-02 1 . 326E+00 1 . 233E+00 3.41 IE-02 4.695E-01 -0.080 0.106 0.097 2.0000 1 . 250 E + 0 0 9.714E-02 1 . 347E+00 1 . 420E+00 3.833E-02 5 . 47 4 E-0

1

-0.075 0.102 0.091 2.5000 1 . 268E+00 1 . 236E-0

1

1 .391E+00 1 . 785E+00 4 . 676E-02 6 . 953E-0I -0.068 0.094 0.082

3.0000 1 . 284E+00 1 .512E-01 1 . 436E+00 2.1 39E+00 5.516E-02 8 . 323E-0

1

-0.063 0.089 0.075

3.5000 1 . 300E+00 1 .797E-01 1 . 480E+00 2 . 482E+00 6 . 348E-02 9.593E-01 -0.058 0.084 0.070 4.0000 1 . 31 4E+00 2.089E-01 1 . 523E+00 2.81 5E+00 7.171 E-02 1 . 077E+00 -0.055 0.080 0.065

4.5000 1 . 327E+00 2.387E-01 1 . 566E+00 3. 1 38E+00 7 . 984E-02 1 . 188E+00 -0.052 0.076 0.061 5.0000 1 . 338E+00 2.691 E-0

1

1 . 608E+00 3 . 454E+00 8 . 736E-02 1 . 292E + 00 -0.049 0.073 0.058

5.5000 1 . 349E+00 2. 999E-01 1 . 649E+00 3.761 E+00 9.575E-02 1 . 389E+00 -0 .047 0.070 0.055

6.0000 1 . 359E+00 3.312E-01 1 .690E+00 4 . 060E+00 1 . 0 35E-0

1

1 .481 E+00 -0.045 0.068 0.052

7.0000 1 . 376E+00 3. 949E-01 1 . 77 1 E+00 4 . 638E+00 1 . 187E-01 1 .651 E+00 -0.042 0.064 0.048 8.0000 1 .391 E+00 4.598E-01 1 . 85 1 E+00 5.1 90E+00 1 . 333E-0

1

1 . 80 5E + 00 -0.040 0.060 0.044

9.0000 1 . 404E+00 5.257E-01 1 . 930E+00 5.71 9E+00 1 .474E-01 1 . 945E+00 -0.038 0.057 0.041 10.0000 1 . 4 1 6 E + 00 5. 926E-01 2 . 009E+00 6 . 227E+00 1 . 6 1 1 E-0

1

2 . 074E+00 -0.036 0.055 0.039

12.5000 1 . 44 1 E+00 7.631 E-0

1

2 . 204E+00 7.41 5E+00 1 . 931 E-0

1

2 . 357E+00 -0.033 0.050 0.034

15.0000 1 .461 E+00 9.373E-01 2 . 393E+00 8 . 502E+0 0 2.224E-01 2 . 597E+00 -0.031 0.046 0.030

17.5000 1 . 477E+00 1 . 1 14E+00 2 . 592E+00 9 . 504E+00 2 . 493E-01 2.806E+00 -0.029 0.043 0.027 20.0000 1 . 492E+00 1 . 294E+00 2 . 786E+00 1 . 043E+0

1

2 . 74 1 E-0

1

2 . 991 E+00 -0.028 0.041 0.025 25.0000 1 .51 5E+00 1 . 659E+00 3 . 1 73E+00 1 .212E+01 3.182E-01 3.31 1 E+00 -0.025 0.037 0.021 30.0000 1 . 533E+00 2 . 029E+00 3 . 562E+00 1 . 360E+0

1

3.564E-01 3.583E+00 -0 .022 0.034 0.018

35.0000 1 . 548E+00 2.403E+00 3. 952E+00 1 . 4 93E+0

1

3.897E-01 3 . 820 E+0 0 -0.020 0.032 0.016 40.0000 1 . 561 E+00 2.781 E+00 4 . 342E+00 1 .614E+01 4.191 E-0

1

4.031 E+00 -0.018 0.030 0.015

45.0000 1 . 572E+00 3. 1 62E+00 4 . 734E+00 1 . 724E+0

1

4 . 452E-0

1

4 . 222E+00 -0.016 0.028 0.013

50.0000 1 . 58 1 E+00 3 . 545E+00 5 . 1 27E+00 1 . 826E+0

1

4.687E-01 4 . 396E + 00 -0.015 0.027 0.012 55.0000 1 . 590E+00 3 . 930E+00 5 . 520 E+00 1 . 920E+0

1

4.899E-01 4 . 556E + 00 -0.014 0.026 0.011 60.0000 1 . 598E+00 4.31 6E+00 5 . 91 4E+00 2.007E+01 5.092E-01 4 . 704E + 00 -0.013 0.025 0.010 70.0000 1.611 E+00 5.093E+00 6 . 704E + 0 0 2. 166E+01 5.429E-01 4.971 E+00 -0.011 0.023 0.009 80.0000 1 . 6 22E + 00 5.874E+00 7 . 495E+00 2 . 307E+0

1

5.716 E-0

1

5 . 206E+00 -0.010 0.022 0.008

90.0000 1 .631 E+00 6 . 658E+00 8 . 289E+00 2 . 434E+0

1

5. 963E-01 5.41 7E+00 -0.009 0.021 0.007 100.0000 1 . 640E+00 7 . 445E+00 9 . 085E+00 2 . 549E+0

1

6. 178E-01 5 . 607E + 00 -0.008 0.020 0.006 125.0000 1 . 658E+00 9 . 420E+00 1 . 1 08E+0

1

2.798E+01 6.614E-01 6 . 01 5E+00 -0.007 0.019 0.005

150.0000 1 . 672E+00 1 . 141E+01 1 . 308E+0

1

3 . 005E+0

1

6.948E-01 6 . 352E+00 -0.006 0.017 0.004

175.0000 1 . 684E+0 0 1 . 340E+01 1 . 508E+0

1

3.183E+01 7.214E-01 6 . 640E+00 -0.005 0.016 0.004 200.0000 1 . 6 94E+00 1 .540E+01 1 .709E+01 3 . 339E+0

1

7.430E-01 6 .891 E+00 -0.005 0.016 0.003 250.0000 1 .710E+00 1 . 940E+01 2. 1 1 1 E+01 3.601 E + 0

1

7.765E-01 7 . 31 5E+00 -0.004 0.015 0.002 300.0000 1 . 724E+00 2 . 342E+0

1

2.514E+01 3.818E+01 8.014E-01 7 . 664E+00 -0.003 0.014 0.002 350.0000 1 . 735E+00 2 . 744E+0

1

2.918E+01 4.003E+01 8.206E-01 7 . 96 1 E+00 -0.003 0.013 0.002 400.0000 1 . 744E+00 3.148E+01 3 . 322E+0

1

4.163E+01 8 . 36 1 E-0

1

8 . 220E+00 -0.002 0.013 0.002 450.0000 1 . 753E+00 3 . 552E+0

1

3 . 727E+0

1

4.305E+01 8.488E-01 8 . 449E+00 -0.002 0.012 0.001 500.0000 1 . 760E+00 3. 956E+01 4. 132E+01 4 . 433E+0

1

8.594E-01 8 . 655E+00 -0 .002 0.012 0.001 550.0000 1 .767E+00 4 . 360E+0

1

4 . 537E+0

1

4 . 548E+0

1

8 . 685E-0

1

8.842E+00 -0.001 0.012 0.001 600.0000 1 . 77 3E+00 4 . 765E+0

1

4. 943E+01 4.654E+01 8 . 763E-01 9.01 4E+00 -0.001 0.011 0.001 700.0000 1 . 784E+00 5.576E+01 5 . 754E+C

1

4.841 E+0

1

8.893E-01 9.31 8E+00 -0.001 0.011 0.001 800.0000 1 . 793E+00 6 . 387E+01 6.566E+01 5 . 003E+0

1

8.995E-01 9 . 582E+00 -0.001 0.011 0.001 900.0000 1 .801 E+00 7. 1 99E+01 7.379E+01 5.147E+01 9.078E-01 9.81 5E+00 -0.001 0.010 0.001 1000.0000 1 .808E+00 8.01 1E+01 8.1 92E+01 5 . 276E+0

1

9.147E-01 1 . 002E+0

1

-0.001 0.010 0.001

95
ELECTRONS IN KRYPTON

I = 352.0 eV DENSITY = 3.478E-03 g/cm 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d ( log[ )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD C0RR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cra 2/g MeV ca 2/g g/cm 2 0.0100 1 .210E+01 1 . 344E-02 1 .21 1E+01 5.046E-04 5 . 575E-04 0.0 -0.287 0.368 0.347

0.0125 1 . 0 36E+0

1

1 . 427E-02 1 . 038E+0

1

7 . 235E-04 6 . 946E-04 0.0 -0.270 0 . 340 0.322

0.0150 9.11 6E + 00 1 .491E-02 9.131 E+00 9 . 860E-04 8.296E-04 0.0 -0.257 0.320 0.304

0.0175 8. 175E+00 1 . 543E-02 8 . 1 9 1 E+00 1 . 276E-03 9.624E-04 0.0 -0.248 0.305 0.291 0.0200 7 . 437E+00 1 . 586E-02 7 . 452E + 00 1 .596E-03 1 . 0 93E-0 3 0.0 -0.240 0.292 0 . 280 0.0250 6 . 347E+00 1 .654E-02 6 . 364E+00 2.325E-03 1 . 348E-0 3 0.0 -0.228 0.274 0.263

0.0300 5 . 579E+00 1 . 707E-02 5 . 5 96 E+0 0 3. 165E-03 1 . 594E-03 0.0 -0.219 0.260 0.251 0.0350 5 . 006E+00 1 . 750E-02 5 . 024E+00 4.1 10E-03 1 .833E-03 0.0 -0.212 0.250 0.242

0.0400 4.561 E+00 1 . 785E-02 4.579E+00 5.154E-03 2 . 065E-03 0.0 -0.207 0.242 0.235

0.0450 4 . 205E+00 1 .816E-02 4 . 223E+00 6 . 292E-03 2.292E-03 0.0 -0.202 0.235 0.223

0.0500 3. 91 3E+00 1 .844E-02 3.931 E+00 7.521E-03 2.512E-03 0.0 -0.198 0.229 0.223

0.0550 3.669E+00 1 -869E-02 3 . 688E+00 8.835E-03 2 . 727E-03 0.0 -0.195 0.224 0.219

0.0600 3.462E+00 1 .891E-02 3.481 E+00 1 . 023E-02 2. 933E-03 0.0 -0.191 0.219 0.215

0.0700 3. 129E+00 1 . 932E-02 3 . 1 49E+00 1 . 326E-02 3.345E-03 0.0 -0.186 0.212 0.208

0.0800 2 . 874 E + 00 1 . 969E-02 2 . 893E+00 1 . 658E-02 3.736E-03 0.0 -0.182 0.206 0.203

0.0900 2.671 E+00 2.003E-02 2.691 E+00 2.016E-02 4.113E-03 0.0 -0.178 0.201 0.198

0.1000 2 . 506E+00 2.035E-02 2 . 527E+00 2 . 400 E-02 4.476E-03 0.0 -0.175 0.197 0.194

0.1250 2 . 204E+00 2.111 E-02 2 . 225E+00 3 . 459E-02 5 . 337E-03 0.0 -0.169 0.189 0.186

0.1500 1 . 999E+00 2. 182E-02 2.021 E+00 4 . 640E-02 6 . 1 39E-03 0.0 -0.164 0.183 0.180

0.1750 1 . 85 1 E+00 2.252E-02 1 . 873E+00 5 . 923E-02 6 .893E-03 0.0 -0.160 0.178 0.176

0.2000 1 . 740E+00 2.322E-02 1 . 763E+00 7.305E-02 7 . 606E-03 0.0 -0.157 0.174 0.172

0.2500 1 . 585E+00 2.465E-02 1 . 6 1 OE+00 1 . 028E-0

1

8. 936E-03 0.0 -0.152 0.168 0.165

0.3000 1 . 484E+00 2.617E-02 1 .51 0E+00 1 . 350E-0

1

1 . 0 1 7E-02 0.0 -0.147 0.163 0.160 0.3500 1 . 41 5E+00 2 . 777E-02 1 . 442E+0 0 1 . 689E-0

1

1 . 133E-02 0.0 -0.144 0.159 0.156 0.4000 1 . 365E+00 2.947E-02 1 . 394E+00 2.042E-01 1 . 244E-02 0.0 -0.141 0.155 0.153

0.4500 1 . 328E+00 3. 125E-02 1 . 359E+00 2.405E-01 1 . 351 E-02 0.0 -0.139 0.153 0.150 0.5000 1 . 300E+00 3.31 IE-02 1 . 333E+00 2.777E-01 1 . 455E-02 0.0 -0.136 0.150 0.147

0.5500 1 .279E+00 3 . 504E-02 1 . 31 4E+00 3.154E-01 1 . 557E-02 0.0 -0.134 0.148 0.145

0.6000 1 . 26 3E+00 3 . 703E-02 1 . 300E+00 3.537E-01 1 . 657E-02 0.0 -0.133 0.146 0.143

0.7000 1 .241 E+00 4.116E-02 1 . 283E+00 4.312E-01 1 . 853E-02 0.0 -0.129 0.143 0.139

0.8000 1 . 229E+00 4 . 547E-02 1 . 274E+00 5.094E-01 2 . 045E-02 0.0 -0.127 0.140 0.136

0 . 9000 1 . 222E+00 4 . 996E-02 1 . 272E+00 5.880E-01 2.234E-02 0.0 -0.124 0.137 0.133

1 .0000 1 .21 9E+00 5 . 459E-02 1 . 273E+00 6.666E-01 2.421 E-02 0 .

0

-0.122 0.135 0.131

1 .2500 1 . 221 E+00 6 .673E-02 1 . 288E+00 8.620E-01 2.834E-02 0.0 -0.118 0.130 0.125

1 .5000 1 . 230E+00 7.957E-02 1 . 31 0E+00 1 . 055E+00 3.342E-02 0.0 -0.115 0.127 0.121

1 .7500 1 . 242E+00 9 . 297E-02 1 . 335E+00 1 . 244E+00 3 . 796E-02 0.0 -0.112 0.123 0.117

2.0000 1 . 255E+00 1 . 068E-0

1

1 . 362E+00 1 . 429E+00 4.247E-02 0.0 -0.110 0.121 0.114

2.5000 1 . 282E+00 1 .356E-01 1 . 41 7E+00 1 . 789E+00 5.139E-02 0.0 -0.106 0.116 0.109

3.0000 1 . 307E+00 1 . 656E-0

1

1 . 473E+00 2. 135E+00 6.018E-02 0.0 -0.103 0.113 0.104

3.5000 1 . 330E+00 1 . 965E-0

1

1 . 527E+00 2 . 468E+00 6.882E-02 0.0 -0.101 0.110 0.101 4.0000 1 . 352E+00 2.282E-01 1 . 580E+00 2 . 790E+00 7.729E-02 0 .

0

-0 .099 0.107 0.098 4.5000 1 . 371 E+00 2.605E-01 1 . 632E+00 3 . 1 02E+00 8 . 560E-02 0.0 -0.097 0.104 0.095

5.0000 1 . 389E+00 2. 933E-01 1 . 683E+00 3.403E+00 9 . 374E-02 0.0 -0.096 0.102 0.092

5.5000 1 . 406E+00 3.267E-01 1 . 733E+00 3 . 696E+00 1 .017E-01 0.0 -0.095 0.100 0.090

5.0000 1 . 422E+00 3.605E-01 1 . 782E+00 3.981 E+00 1 . 0 95E-0

1

0.0 -0.093 0.099 0.083 7.0000 1 . 450E+00 4.293E-01 1 . 879E+00 4 . 527E+00 1 . 247E-0

1

0.0 -0.092 0.095 0.084

8.0000 1 . 474E+00 4.995E-01 1 . 974E+00 5 . 046E+00 1 .392E-01 0.0 -0.090 0.093 0.081 9.0000 1 . 497E+00 5.708E-01 2 . 067E+00 5.541 E+00 1 .531E-01 0.0 -0.089 0.090 0.078

10.0000 1 . 51 6E+00 6.430E-01 2 . 1 59E+00 6.01 4E+00 1 .665E-01 0.0 -0.087 0.088 0.075

12.5000 1 . 559E+00 8.269E-01 2 . 386E+00 7.11 5E+00 1 . 978E-01 0.0 -0.085 0 . 084 0.070

15.0000 1 . 594E+00 1 . 0 1 5E+00 2.609E+00 8 . 1 1 6 E+00 2 . 262E-0

1

0.0 -0.083 0.080 0.065

17.5000 1 . 624E+00 1 . 206E+00 2 . 830E+00 9 . 036E+00 2.521E-01 0.0 -0.081 0.077 0.061 20.0000 1 . 650E+00 1 . 399E+00 3 . 050E+00 9 . 887E+00 2 . 760E-0

1

0.0 -0.080 0.074 0.058

25.0000 1 . 6 94E + 00 1 . 7 92E+00 3 . 486E+00 1 . 142E+01 3. 183E-01 0.0 -0.078 0.069 0.053

30.0000 1 . 729E+00 2. 1 91 E+00 3.921 E+00 1 . 277E+0

1

3.548E-01 7.431E-03 -0.072 0.066 0.048

35.0000 1 . 758E+00 2 . 5 95E+0 0 4 . 353E+00 1 . 3 98E+0

1

3.867E-01 3.031 E-02 -0.068 0.063 0.044

40.0000 1 . 782E+00 3 . 002E+00 4 . 785E+00 1 . 508E+0

1

4. 149E-01 6 . 047E-02 -0.064 0.060 0.041 45.0000 1 . 803E+00 3.41 3E+00 5.21 6E+00 1 . 608E+0

1

4.400E-01 9.396E-02 -0.062 0.058 0.038

50 .0000 1 . 322E+00 3 . 825E+00 5 . 647E+00 1 . 7 00 E+0

1

4.626E-01 1 .2S9E-01 -0.060 0.056 0.035 55.0000 1 . 838E+00 4 . 240E+00 6 . 078E+00 1 .785E+01 4 .831 E-01 1 . 643E-01 -0.058 0.054 0.033

50.0000 1 . 853E+00 4 . 656E+00 6 . 509E+00 1 . 865E+0

1

5.017E-01 1 . 998E-01 -0.056 0.052 0.031 70.0000 1 . 879E+00 5 . 493E+00 7 . 372E+00 2.009E+01 5. 344E-01 2.700E-01 -0.053 0.050 0.028

80.0000 1 . 901 E+00 6 . 334E+00 3 . 235E+00 2.137E+01 5.623E-01 3.388E-01 -0.050 0.047 0.025

90.0000 1 . 920 E+00 7. 179E+00 9.098E+00 2.253E+01 5.864E-01 4.061E-01 -0.048 0.046 0.023

100.0000 1 . 936E+00 8 . 027E+00 9 . 963E+00 2 . 358E+0

1

S.076E-01 4.721 E-01 -0.046 0.044 0.021 125.0000 1 . 970E+00 1 .015E+01 1 .212E+01 2 . 585E+0

1

6.506E-01 6 . 31 6E-01 -0 .041 0 .041 0.018

150.0000 1 . 996E+00 1 . 229E+0

1

1 . 429E+0

1

2 . 774E+0

1

6 . 837E-0

1

7.830E-01 -0.037 0.033 0.016 175.0000 2.017E+00 1 . 444E+0

1

1 . 646E+C

1

2 . 937E+0

1

7.102E-01 9 . 258E-0

1

-0.034 0.036 0.014

200.0000 2 . 034E+00 1 . 6 59E + 0

1

1 . 363E+0

1

3 . 080E+0

1

7.320E-01 1 . 060E+00 -0.031 0.035 0.012

250.0000 2 . 062E+00 2.091 E+0

1

2 . 297E+0

1

3 . 32 1 E+0

1

7.653E-01 1 . 304E+00 -0.027 0.033 0.010 300.0000 2 . 084E+00 2 . 524E+0

1

2 . 732E+0

1

3 . 52 1 E+0

1

7.911 E-01 1 .521 E + 00 -0.025 0.031 0 .008 350.0000 2. 102E+00 2. 958E+01 3. 168E+01 3.690E+01 8.108E-01 1 .714E+00 -0.023 0.030 0.007 400.0000 2.1 17E+00 3 . 392E+0

1

3.604E+01 3 . 838E+0

1

8.266E-01 1 . 887E + 00 -0.021 0.029 0.007 450.0000 2. 130E+00 3 . 827E+0

1

4 . 040E+0

1

3. 969E+01 8 . 397E-0

1

2 . 045E+00 -0.020 0 .028 0.006 500.0000 2.141 E+00 4.262E+01 4 . 476E+0

1

4 . 037E+0

1

8.507E-01 2. 189E+00 -0.019 0.027 0.005

550.0000 2.151 E+00 4.698E+01 4.913E+01 4 . 1 93E+0

1

8.601E-01 2 . 322E + 00 -0.013 0.026 0.005

600.0000 2 . 1 60E+00 5.1 34E+01 5 . 350E+01 4.291 E+0

1

8.683E-01 2 . 445E+00 -0.018 0.026 0.005

700.0000 2. 176E+00 6 . 007E+0

1

6 . 225E+0

1

4 . 464E+0

1

8.81 7E-01 2 . 667E+00 -0.016 0.025 0.004

800 .0000 2. 1 90E+00 6.381 E+0

1

7. 100E+01 4.614E+01 8. 924E-01 2.864E+00 -0.015 0.024 0.003

900.0000 2.201 E+00 7 . 755E+0

1

7 . 975E+0

1

4 . 747E+0

1

9.01 IE-01 3 . 042E+00 -0.015 0.023 0.003

1000.0000 2.21 1E+00 8 . 630E+01 8.851 E+0

1

4.866E+01 9.084E-01 3 . 203E+00 -0.014 0.023 0.003

96
ELECTRONS IN MOLYBDENUM

I = 424.0 eV DENSITY = 1 . 022E+0

1

g/cn 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d ( loo1 )/d(loorI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MsV MeV cm 2 /g MeV cm 2 /g MeV cra 2 /g g/cm 2

0.0100- 1 . 1 67E+01 1 . 524E-02 1 . 1 68E+0

1

5.31 9E-04 6 . 528E-04 7 . 953E-04 -0.303 0.402 0 . 373 0.0125 1 . 003E+0

1

1 . 627E-02 1 . 004E+0

1

7.636E-04 3.148E-04 1 . 029E-03 -0.284 0.359 0 . 344 0.0150 8 . 343E+00 1 .709E-02 8.860E+00 1 . 029E-03 9 . 749E-04 1 -275E-03 -0.270 0.345 0 . 323 0.0175 7. 945E+00 1 .776E-02 7 . 963E+00 1 . 327E-03 1 . 1 33E-03 1 . 535E-0 3 -0.260 0.327 0.308

0.0200 7 . 238E+00 1 . 832E-0 2 7 . 256E+00 1 . 657E-03 1 . 288E-03 1 .807E-03 -0.251 0.312 0.295

0.0250 6 . 1 92E+00 1 . 922E-02 6 .21 1 E+00 2.404E-03 1 .593E-03 2 . 389E-03 -0.238 0.291 0.277

0.0300 5 . 452E+0 0 1 . 9 92E-02 5 . 47 2E+0 0 3.264E-03 1 . 889E-03 3.01 7E-03 -0.223 0.275 0.264

0.0350 4 . 3 98E + 00 2.050E-02 4. 918E+00 4 . 230E-03 2. 177E-03 3.692E-03 -0.221 0.263 0.253

0 .0*100 4 . 467E+00 2.099E-02 4 . 488E+00 5.296E-03 2. 458E-03 4.410 E-03 -0.214 0.254 0.245

0 . 0<t50 4. 122E+00 2.142E-02 4.1 43E+00 6 . 457E-03 2 . 732E-03 5. 1 69E-03 -0.209 0.245 0.238

0.0500 3.838E+00 2. 181 E-02 3.860E+00 7.703E-03 3.000E-03 5. 969E-03 -0.205 0.240 0.232

0.0550 3.601 E+00 2.21 6E-02 3 . 6 23E+00 9 . 046E-03 3 . 262E-03 6 . 307E-03 -0.201 0.234 0.227 0.0600 3 . 400E+00 2.247E-02 3 . 422E+00 1 . 047E-02 3.51 9E-03 7.681 E-03 -0.198 0.229 0 . 223 0.0700 3 . 076E+00 2.305E-02 3 . 0 99E+00 1 . 354E-02 4.017E-03 9.535E-03 -0.192 0.221 0.216 0.0800 2 . 826 E+00 2 . 357E-02 2 . 850E+00 1 .691 E-02 4.497E-03 1 . 1 52E-02 -0.187 0.214 0.210 0.0900 2. 628E+00 2 . 404E-02 2 . 652E+00 2 . 055E-02 4.961 E-03 1 . 362E-02 -0.183 0.209 0.204 0.1000 2 . 467E+00 2.449E-02 2 . 492E+00 2 . 445E-02 5.409E-03 1 .5S4E-02 -0.180 0.204 0.200 0.1250 2. 1 7 1 E+00 2.551 E-02 2.1 97E+00 3.51 7E-02 6.474E-03 2. 180E-02 -0.173 0.195 0.192

0.1500 1 . 970E+00 2 . 646 E-02 1 . 996E+00 4.71 4E-02 7 . 469E-03 2 . 830E-02 -0.167 0.188 0.185

0.1750 1 . 825E+00 2.737E-02 1 . 852E+00 6 . 01 6E-02 8 . 406E-03 3 . 523E-02 -0.163 0.133 0.180 0.2000 1 . 7 1 5E+00 2.826E-02 1 . 743E+00 7.409E-02 9.292E-03 4 . 252E-0 2 -0.159 0.178 0.175

0.2500 1 . 563E+00 3 . 005E-02 1 . 593E+00 1 . 042E-01 1 . 0 95E-0 2 5.795E-02 -0.153 0.171 0.168

0.3000 1 . 463E+00 3.1 92E-02 1 . 4 95E+0 0 1 . 367E-0

1

1 . 248E-02 7 . 422E-02 -0.147 0.165 0.162

0.3500 1 . 394E+00 3 . 388E-02 1 . 427E+00 1 .709E-01 1 . 391 E-02 9. 1 09E-02 -0.143 0.160 0.157 0.4000 1 . 344E+00 3.593E-02 1 . 380E+00 2.066E-01 1 .529E-02 1 . 084E-0

1

-0.139 0.156 0.153

0.4500 1 . 307E+00 3 . 808E-02 1 . 345E+00 2.433E-01 1 .661 E-02 1 .259E-01 -0.135 0.153 0.150 0.5000 1 .279E+00 4.032E-02 1 .31 9E+00 2.809E-01 1 .789E-02 1 . 437E-0

1

-0.132 0.150 0.146 0.5500 1 . 257E+00 4.264E-02 1 . 300E+00 3. 1 9 1 E-0

1

1 . 91 5E-02 1 . 615E-01 -0.129 0.147 0.143

0.6000 1 . 240E+0 0 4 . 502E-02 1 . 285E+00 3.578E-01 2 . 038E-02 1 . 7 94E-0

1

-0.126 0.144 0.141 0.7000 1 .21 7E+00 4. 996E-02 1 . 267E+00 4 . 362E-0

1

2.279E-02 2.151 E-0

1

-0.122 0.140 0.136 0.8000 1 . 203E+00 5.51 0E-02 1 . 258E+00 5.155E-01 2.51 4E-02 2.505E-01 -0.117 0.136 0.131 0.9000 1 . 1 94E+00 6 . 043E-02 1 . 255E+00 5.951 E-0

1

2 . 746E-02 2.854E-01 -0.113 0.133 0.127

1.0000 1 . 1 90E+00 6.592E-02 1 . 255E+00 6 . 748E-0

1

2. 974E-02 3.1 98E-01 -0.110 0.129 0.124

1 .2500 1 . 187E+00 8 . 032E-02 1 . 268E+00 8.731 E-0

1

3 . 538E-02 4.028E-01 -0.103 0.123 0.116

1 .5000 1 . 1 92E+00 9 . 550E-02 1 . 288E+00 1 . 0 6 9E+0 0 4.095E-02 4.81 6E-01 -0.097 0.117 0.110

1 .7500 1 .200E+00 1.11 3E-01 1 .31 1 E+00 1 . 26 1 E+00 4 . 646E-02 5.563E-01 -0.093 0.113 0.104

2.0000 1 . 20 9E+00 1 . 276E-0

1

1 . 337E+00 1 .450E+00 5.1 93E-02 6 . 275E-0

1

-0.088 0.109 0.099

2.5000 1 . 228E+00 1 .615E-01 1 . 389E+00 1 . 8 1 7E+00 6 . 272E-02 7 . 60 6 E-0

1

-0.081 0.102 0.091 3.0000 1 . 246E+00 1 . 967E-0

1

1 . 442E+C 0 2. 170E+00 7 . 333E-02 8 . 838E-0

1

-0.075 0.097 0.085 3.5000 1 . 262E+00 2.329E-01 1 . 495E+00 2.51 1E+00 8.373E-02 9.994E-01 -0.070 0.092 0.079 4.0000 1 . 277E+0 0 2.699E-01 1 . 547E+00 2 . 840E+0 0 9. 392E-02 1 . 1 09E+00 -0.065 0.088 0.074

4.5000 1 . 290E+00 3.077E-01 1 . 598E+00 3. 158E+00 1 .039E-01 1 . 21 2E+00 -0.061 0.084 0.070 5.0000 1 . 302E+00 3.461 E-0

1

1 . 648E+00 3 . 466E+00 1 . 1 36E-01 1 .31 1E+00 -0.057 0.081 0.066 5.5000 1 .313E+00 3.851E-01 1 . 6 98E+00 3 . 765E+00 1 . 232E-0

1

1 . 406E+00 -0.054 0.073 0.062

6.0000 1 . 322E+00 4.246E-01 1 . 747E+00 4 . 055E+00 1 . 325E-0

1

1 . 496E+00 -0.051 0.075 0.059 7.0000 1 . 340E+00 5.049E-01 1 . 845E+0 0 4.51 2E+00 1 . 505E-0

1

1 . 6 6 6 E+0 0 -0.046 0.070 0.053 8.0000 1 . 355E+00 5.867E-01 1 . 941 E+00 5 . 1 40E+00 1 .677E-01 1 . 822E+00 -0.042 0.066 0.049

9.0000 1 . 367E+00 6.697E-01 2 . 037E+0 0 5 . 643E+00 1 .841 E-0

1

1 . 966E+00 -0.039 0.063 0.045 10.0000 1 . 379E+00 7.538E-01 2.133E+00 6 . 1 23E+00 1 . 999E-01 2. 1 00E+00 -0.037 0.060 0.041 12.5000 1 . 402E+00 9.680E-01 2 . 370E+00 7 . 234E+00 2.362E-01 2 . 398E+00 -0.032 0.054 0.035

15.0000 1 . 421 E+00 1 . 1 87E+00 2 . 608E+00 8.239E+00 2.689E-01 2 . 653E+00 -0.029 0.050 0.030 17.5000 1 . 437E+00 1 . 40 9E+00 2 . 845E+00 9. 157E+00 2. 984E-01 2 . 877E+0 0 -0.027 0.046 0.027 20.0000 1 . 450E+0 0 1 . 6 34E+0 0 3 . 084E+0 0 1 . 00 0 E+0

1

3 . 252E-0

1

3 . 075E+00 -0.025 0.043 0.024 25.0000 1 . 47 1 E+00 2.091 E+00 3 . 562E+00 1 . 1 5 1 E+0

1

3.721 E-0

1

3.418E+00 -0.022 0.039 0.020

30 .0000 1 . 48SE+00 2 . 555E+00 4 . 043E+00 1 . 282E+0

1

4.118E-01 3 . 707E+00 -0.019 0.035 0.017 35.0000 1 .502E+00 3 . 024E+00 4 . 526E+00 1 .399E+01 4 . 459E-0

1

3. 959E+00 -0.017 0.033 0.015 40.0000 1 . 5 1 4E+00 3 . 4 97E+00 5.011 E+00 1 .504E+01 4.756E-01 4. 182E+00 -0.015 0.031 0.013

45.0000 1 .524E+00 3. 974E+00 5 . 49SE+00 1 . 5 99E + 0

1

5.017E-01 4 . 382E+0 0 -0.014 0.030 0.012

50.0000 1 . 533E+00 4 . 453E+0 0 5 . 987E+00 1 . 687E+0

1

5.249E-01 4 . 564E+00 -0.013 0 .023 0.011 55.0000 1 .541 E+00 4. 935E+00 6 . 477E+00 1 . 767E+0

1

5.457E-01 4 . 730E + 00 -0.012 0.027 0.010 60.0000 1 . 549E+00 5.41 9E+00 6 . 968E+00 1 . 84 1 E+0

1

5.644E-01 4 . 884E + 00 -0.011 0.026 0.009 70.0000 1 .561 E+00 6 . 392E+0 0 7. 953E+00 1 . 976E+0

1

5. 968E-01 5. 160E + 00 -0.009 0 .025 0.008 80.0000 1 . 572E+00 7 . 370E+00 8 . 942E+00 2.094E+01 5.240E-01 5 . 403E+00 -0.008 0.023 0.007

90.0000 1 . 581 E+00 8 . 352E+00 9 . 933E+00 2.200E+01 6 . 472E-0

1

5.61 9E+00 -0.007 0.022 0.006 100.0000 1 .539E+00 9 . 339E+00 1 . 0 93E+0

1

2 . 296E+0

1

6 . 673E-01 5.81 4E+00 -0.007 0.021 0.005 125.0000 1 . 606E+00 1 . 181E+01 1 . 342E+0

1

2 . 502E+0

1

7.075E-01 6.231 E+00 -0.006 0.020 0.004

150.0000 1 .619E+00 1 .430E+01 1 . 592E+0

1

2 . 673E+0

1

7.379E-01 6 . 575E+00 -0.005 0.019 0 .003 175.0000 1 . 631 E+00 1 . 680E+0

1

1 . 843E+0

1

2.81 9E+01 7.618E-01 6 . 868E+00 -0.004 0.018 0.003 200.0000 1 . 641 E+00 1 .931E+01 2.095E+01 2 . 946 E+0

1

7.81 IE-01 7 . 1 24E+00 -0.004 0.017 0.003

250 .0000 1 . 657E+00 2 . 433E+0

1

2.598E+01 3 . 1 6 0 E + 0

1

8.108E-01 7.553E+00 -0.003 0.016 0.002 300.0000 1 . 670E+00 2.936E+01 3 . 1 03E+01 3 . 336E+01 8.326E-01 7. 907E+00 -0 .002 0.015 0.002 350.0000 1 . 680 E+00 3.441E+01 3.609E+01 3 . 485E+0

1

8.494E-01 8 . 208E+0 0 -0.002 0.014 0.001 400.0000 1 .690E+00 3. 946E+01 4.11 5E+01 3.615E+01 8 . 627E-0

1

8.469E+00 -0.002 0.014 0.001 450.0000 1 . 6 98E+00 4 . 452E+0

1

4 . 622E+0

1

3 . 729E+0

1

3 . 737E-0

1

8.701 E+00 -0.001 0.013 0.001 500.0000 1 . 705E+00 4. 959E+01 5. 129E+01 3 . 832E+0

1

8 . 828E-0

1

8 . 909E+00 -0.001 0.013 0.001 550.0000 1 .712E+00 5.466E+01 5.637E+01 3. 925E+01 8.906 E-0

1

9 . 0 97E+00 -0.001 0.013 0.001 600.0000 1 .718E+00 5. 973E+01 6.145E+01 4.010E+01 8. 973E-01 9.269E+00 -0.001 0.012 0.001 700.0000 1 . 728E+00 6 . 988E+01 7.161E+01 4 . 1 60E+01 9.082E-01 9 . 575E+00 -0.001 0.012 0.001 800.0000 1 . 737E+00 8 . 004E+0

1

8.178E+01 4.291 E+0

1

9. 1 69E-01 9.340E+00 -0.001 0.012 0.001 900.0000 1 . 745E+00 9 . 022E+0

1

9.1 96E+01 4 . 406E+0

1

9.239E-01 1 . 007E+0

1

-0.001 0.011 0.001 1000.0000 1 . 753E+00 1 . 004E+02 1 .021E+02 4.509E+01 9 . 297E-01 1 . 028E+0

1

- 0.000 0.011 0.001

97
ELECTRONS IN SILVER

I = 470.0 eV DENSITY = 1 . 0 50 E+0

1

g/c,n 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log[ )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2/g MaV c» 2 /g g/cm 2 O.OIOO 1 . 1 25E+0

1

1 . 634E-02 1 . 127E+01 5.577E-04 7.226E-04 1 . 1 26 E-0 3 -0.313 0.424 0.389

0.0125 9 . 687E+00 1 . 754E-02 9 . 704E+00 7 . 976E-04 9.040E-04 1 . 445E-03 -0.292 0 . 387 0.357

0.0150 8.556E+00 1 . 849E-02 8 . 574E+00 1 . 072E-03 1 . 084E-03 1 .731 E-03 -0.278 0.361 0.335

0.0175 7.696E+00 1 . 927E-02 7.71 5E+00 1 . 380E-03 1 .261E-03 2. 1 35E-03 -0.267 0.341 0.318

0.0200 7.017E+00 1 . 992E-02 7 . 037E+00 1 .720E-03 1 .437E-03 2.508E-03 -0.258 0.325 0 . 305 0.0250 6.01 1E+00 2.C99E-02 6 . 032E+00 2 . 490E-03 1 .781 E-0 3 3.312E-03 -0.244 0.302 0.285

0.0300 5 . 297E+00 2. 184E-02 5.31 9E+00 3 . 375E-03 2.1 17E-03 4.203E-03 -0.233 0.285 0.271 0.0350 4.763E+00 2 . 254E-02 4 . 786E+00 4.368E-03 2.444E-03 5. 1 90E-03 -0.225 0.272 0.260

0.0400 4 . 347E+00 2.314E-02 4 . 370 E + 0 0 5 . 463E-03 2.764E-03 6 . 284E-03 -0.219 0.262 0.251 0.0450 4.01 2E+00 2.367E-02 4 . 036E+00 6 . 655E-03 3 . 077E-03 7.495E-03 -0.213 0.253 0.244

0.0500 3 . 738E+00 2.414E-02 3 . 762E+00 7.939E-03 3.383E-03 8.836E-03 -0.203 0.246 0.237

0.0550 3 . 508E+00 2 . 458E-02 3 . 533E+00 9.312E-03 3.684E-03 1 .032E-02 -0.204 0.240 0.232

0.0600 3.31 3E+00 2 . 497E-02 3 . 338E+00 1 . 077E-02 3. 979E-03 1 . 1 96E-02 -0.200 0.235 0.227

0.0700 2 . 999E+00 2.569E-02 3 . 024E+00 1 .392E-02 4.552E-03 1 . 573E-02 -0.193 0.225 0.219

0.0800 2 . 756E+00 2 . 634E-02 2 . 782E+00 1 . 737E-02 5 . 1 06 E-0 3 2.022E-02 -0.186 0.218 0.212

0.0900 2 . 563E+00 2.693E-02 2 . 5 90 E+00 2.11 0E-02 5 . 643E-03 2.543E-02 -0.181 0.211 0.206

0.1000 2 . 406E+00 2.748E-02 2 . 434E+00 2.509E-02 6.163E-03 3. 125E-02 -0.176 0.206 0.201 0.1250 2.11 7E+00 2 . 875E-02 2.146E+00 3.607E-02 7.402E-03 4.754E-02 -0.166 0.194 0.190

0.1500 1 . 920E + 00 2. 990E-02 1 . 950E+00 4 . 832E-02 8 . 564E-03 6 . 453E-02 -0.159 0.186 0.181 0.1750 1 . 778E+00 3.098E-02 1 . 80 9E+0 0 6 . 1 65E-02 9.661E-03 8.111 E-02 -0.154 0.179 0.175

0.2000 1 .671E+00 3.203E-02 1 . 703E+00 7.591E-02 1 . 070E-02 9 . 702E-02 -0.149 0.173 0.169

0.2500 1 . 522E+00 3.41 3E-02 1 . 556E+00 1 .067E-01 1 . 264E-02 1 . 270E-0

1

-0.143 0.164 0.161 0.3000 1 . 424E+00 3 . 628E-02 1 . 460E+00 1 . 400E-01 1 . 443E-02 1 . 550E-0

1

-0.138 0.158 0.154

0.3500 1 . 356E+00 3 . 852E-02 1 . 395E+00 1 . 750E-0

1

1 .612E-02 1 .81 6E-01 -0.133 0.153 0.149

0.4000 1 . 308E+00 4 . 085E-02 1 . 348E+00 2.115E-01 1 . 772E-02 2 . 070 E-0

1

-0.130 0.148 0.145

0.4500 1 .271E+00 4 . 328E-02 1 . 3 1 5E+00 2.491E-01 1 . 927E-02 2.315E-01 -0.126 0.145 0.141 0.5000 1 . 244E+00 4 . 580E-02 1 . 290E+00 2.875E-01 2 . 076E-02 2.552E-01 -0.123 0.141 0.137

0.5500 1 . 223E+00 4 . 840E-02 1 . 27 1 E+00 3.266E-01 2 . 222E-02 2.783E-01 -0.121 0.139 0.135

0.6000 1 . 20 7E+00 5.107E-02 1 . 258E+00 3.661 E-01 2 . 365E-02 3 . 0 07E-0

1

-0.119 0.136 0.132

0.7000 1 . 184E+00 5.659E-02 1 . 241 E+00 4.462E-01 2.643E-02 3.438E-01 -0.114 0.132 0.127

0.8000 1 . 1 70E+00 6.233E-02 1 . 233E+00 5.271E-01 2.914E-02 3.851 E-0

1

-0.111 0.128 0.123

0.9000 1 . 1 62E+00 6 . 827E-02 1 . 230E+00 6.084E-01 3. 179E-02 4.246E-01 -0.103 0.125 0.119

1 .0000 1 . 1 58E+00 7 . 439E-02 1 .232E+00 6 . 896E-0

1

3.441E-02 4.626E-01 -0.105 0.122 0.116

1 .2500 1 . 1 56E+00 9.038E-02 1 . 246E+00 8. 915E-01 4 . 082E-02 5.520E-01 -0.099 0.116 0.109

1 .5000 1 .161E+00 1 . 072E-0

1

1 . 268E+00 1 . 0 90E+00 4.711 E-02 6 . 346 E-0

1

-0.094 0.111 0.103

1 .7500 1 . 1 6 9E+00 1 . 247E-0

1

1 . 294E+00 1 . 286E+00 5 . 330 E-0 2 7. 1 16E-01 -0.090 0.107 0.099

2.0000 1 . 178E + 00 1 .428E-01 1 . 321 E+00 1 . 47 7E+00 5. 942E-02 7.836E-01 -0.086 0.103 0.094

2.5000 1 . 1 97E+00 1 . 802E-0

1

1 . 377E+00 1 . 848E+00 7. 144E-02 9.157E-01 -0.081 0.097 0 .087 3.0000 1 . 21 5E+00 2.1 90E-01 1 . 434E+00 2 . 203E+00 8.31 7E-02 1 . 0 35E+00 -0.076 0.092 0.082

3.5000 1 . 232E+00 2.589E-01 1 . 491 E+00 2 . 545E+00 9.461 E-02 1 . 1 43E+00 -0.072 0.088 0.077

4.0000 1 . 248E+00 2. 997E-01 1 . 547E+00 2 . 874E+00 1 .057E-01 1 . 243E+00 -0.069 0.085 0.073

4.5000 1 . 261 E+00 3.412E-01 1 . 60 3E+00 3.1 92E+00 1 . 166E-01 1 . 337E+00 -0.066 0.082 0.069

5.0000 1 . 274E+00 3.834E-01 1 . 658E+00 3 . 499E+00 1 . 27 1 E-0

1

1 . 425E+00 -0.063 0.079 0.066 5.5000 1 . 286E+00 4.263E-01 1 . 71 2E+00 3 . 7 95E+0 0 1 . 374E-01 1 . 508E+00 -0.060 0.076 0.063

6.0000 1 . 296E+00 4.696E-01 1 . 766E+00 4 . 083E+00 1 . 474E-0

1

1 . 587E+00 -0.058 0.074 0.060 7.0000 1 . 31 5E+00 5 . 577E-0

1

1 . 873E+00 4 . 633E+00 1 . 667E-0

1

1 . 735E+00 -0.054 0 .070 0.055

8.0000 1 . 331 E+00 6.474E-01 1 . 978E+00 5. 152E+00 1 .849E-01 1 . 873E+00 -0.050 0.067 0.051 9.0000 1 . 345E+00 7. 384E-01 2. 083E+00 5 . 645E+00 2.023E-01 2.001 E+00 -0.046 0.063 0.047

1 0.0000 1 . 357E+00 8.305E-01 2. 188E+00 6.11 3E+00 2. 188E-01 2. 1 21 E+00 -0.043 0.061 0.044

12.5000 1 . 382E+00 1 . 065E+00 2 . 447E+00 7.1 93E+00 2.567E-01 2 . 392E+00 -0.037 0.055 0.038

15.0000 1 . 402E+00 1 . 304E+00 2 . 707E+00 8. 1 64E+00 2.904E-01 2 . 630E+00 -0.033 0.051 0.033

17.5000 1 -418E+00 1 . 547E+00 2. 966E+00 9 . 046E+00 3.207E-01 2.841 E+00 -0.030 0.047 0 .029 20.0000 1 . 432E+00 1 . 7 94E+00 3 . 226E+00 9 . 854E+00 3.480E-01 3 . 030E+00 -0.028 0.045 0.026 25.0000 1 . 455E+00 2 . 293E+00 3 . 748E+00 1 . 129E+01 3 . 954E-0

1

3.359E+00 -0.024 0.040 0.021 30.0000 1 . 472E+00 2 . 800E+00 4 . 272E+00 1 . 254E+0

1

4.353E-01 3 . 638E+00 -0.022 0.037 0.018

35.0000 1 . 487E+00 3.31 3E+00 4 .800E+00 1 . 364E+01 4.693E-01 3 . 330 E+0 0 -0.020 0.035 0.016 40.0000 1 . 4 99E+0 0 3.831 E+00 5 . 330E+00 1 . 463E+0

1

4. 988E-01 4 . 0 94E+0 0 -0.018 0.033 0.014

45.0000 1 . 5 1 0 E + 00 4 . 352E+00 5 .862E+00 1 . 553E+0

1

5 . 246 E-0

1

4 . 287E+00 -0.017 0.031 0.013

50.0000 1 .51 9E+00 4 . 876E+00 6 . 395E+00 1 . 634E+0

1

5.474E-01 4 . 462E+00 -0.015 0.030 0.011 55.0000 1 . 528E+00 5.403E+00 6 . 930E+00 1 . 709E+01 5.677E-01 4 . 622E+00 -0.014 0.029 0.010 60.0000 1 . 535E+00 5 . 932E+00 7 . 467E+00 1 .779E+01 5.860E-01 4.771 E+00 -0.013 0.028 0.010 70.0000 1 . 548E+00 6 . 995E+00 8.543E+00 1 . 904E+01 6 . 1 76 E-0

1

5 . 038E+00 -0.012 0.026 0.008 80.0000 1 . 559E+00 8 . 065E+00 9 . 624E+00 2.014E+01 6 . 440E-0

1

5 . 274E+00 -0.010 0.025 0.007

90.0000 1 . 56 9E+00 9. 139E+00 1 .071 E+0

1

2.11 3E+01 6.664E-01 5 . 484E+00 -0.009 0.024 0.006

100.0000 1 . 577E+00 1 . 022E+0

1

1 . 179E+01 2 . 202E+0

1

6 .858E-01 5 . 675E+00 -0.008 0.023 0 .006 125.0000 1 . 594E+00 1 . 293E+0

1

1 . 452E+0

1

2.392E+01 7.245E-01 6 . 084E+00 -0.007 0.021 0.005

150.0000 1 . 608E+00 1 .565E+01 1 . 725E+0

1

2 . 550E+0

1

7.535E-01 6 . 424E+00 -0.006 0.020 0.004

175.0000 1 . 620E+00 1 . 338E+0

1

2 . 000 E+0

1

2 . 684E+0

1

7.763E-01 6 .71 3E+00 -0.005 0.019 0.003

200.0000 1 . 630E+00 2.1 12E+01 2 . 275E+0

1

2 . 802E+0

1

7. 948E-01 6 . 966E+00 -0.005 0.018 0.003 250.0000 1 . 6 46 E + 00 2.661 E+0

1

2 . 825E+0

1

2 . 998E+0

1

8.229E-01 7. 392E+00 -0.004 0.017 0.002 300.0000 1 . 65 9E+00 3.21 1E+01 3 . 377E+0

1

3. 160E+01 8.435E-01 7 . 742E+00 -0.003 0.016 0.002

350.0000 1 . 670E+00 3 . 763E+0

1

3. 930E+01 3.297E+01 8.594E-01 8 . 040E+00 -0.003 0.015 0.002

400 . 0000 1 . 679E+00 4.316E+01 4 . 483E+0

1

3.41 6E+01 8 . 720 E-0

1

8 . 299E+00 -0.002 0.015 0.001

450 .0000 1 . 638E+00 4.869E+01 5.037E+01 3.521 E+0

1

8 . 823E-0

1

8 . 529E+00 -0 .002 0.014 0.001 500.0000 1 . 695E+00 5 . 422E+0

1

5.592E+01 3. 61 6E+01 8. 908E-01 8 . 735E+00 -0.002 0.014 0.001

550 .0000 1 . 7 0 2E+00 5 . 976E+0

1

6. 147E+01 3.701 E+0

1

8 . 981 E-01 8 . 922E+00 -0.002 0.014 0.001 600.0000 1 . 708E+00 6.531 E+O

1

6 . 702E+0

1

3 . 779E+0

1

9.044E-01 9 . 0 93E+00 -0.001 0.013 0.001 700.0000 1 . 71 8E+00 7.641 E+0

1

7.813E+01 3.917E+01 9. 147E-01 9 . 397E+00 -0.001 0.013 0.001 800.0000 1 . 727E+00 8.751 E+0

1

3. 924E+01 4.036E+01 9.228E-01 9.661 E+00 -0.001 0.013 0.001 900.0000 1 . 735E+00 9.863E+01 1 . 004E+02 4. 142E+01 9.293E-01 9 . 894E+00 -0.001 0.012 0.001 1000.0000 1 . 743E+00 1 . 0 98E+02 1 . 1 1 5E+02 4.237E+01 9.347E-01 1 .010E+01 -0.001 0.012 0.001

98
ELECTRONS IN TIN

I = 488.0 eV DENSITY = 7.31 OE+OOi g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cra 2/g MeV cra 2 /g MeV cm 2 /g g/cm 2 0.0100 1 . 075E+0

1

1 . 645E-02 1 . 077E + 0

1

5.861 E-04 7 . 576E-04 6 . 966E-04 -0.316 0.434 0.395 0.0125 9 . 263E + 00 1 . 76 9E-02 9.281 E+00 8 . 371 E-04 9 . 496E-04 8.851 E-04 -0.296 0.395 0.362

0.0150 8 . 1 86E+00 1 . 86 9E-0 2 8 . 205E+00 1 . 124E-03 1 . 140E-03 1 .079E-03 -0.281 0 . 367 0.339 0.0175 7 . 366E+00 1 . 951 E-02 7 . 386E+00 1 . 446E-03 1 . 329E-03 1 .279E-03 -0.269 0.347 0.322

0.0200 6.719E+00 2.021E-02 6 . 740E+00 1 .801E-03 1 .515E-03 1 . 484E-03 -0.260 0 . 330 0.308 0.0250 5 . 759E+00 2.1 34E-02 5.781 E+00 2 . 6 0 5E-0 3 1 . 882E-0 3 1 . 91 0E-03 -0.246 0.306 0.288

0.0300 5 . 078E+00 2 . 224E-02 5 . 1 OOE+OO 3 . 528E-03 2 . 239E-03 2. 358E-03 -0 .236 0.289 0.274 0.0350 4 . 567E+00 2 . 299E-02 4 . 590E+00 4.564E-03 2.589E-03 2 . 827E-03 -0.228 0.276 0.263 0.0400 4. 1 69E+00 2 . 364E-02 4 . 1 93E+00 5 . 705E-0 3 2. 931 E-03 3.316E-03 -0.221 0.265 0.254 0.0450 3 . 850E+00 2.422E-02 3 . 874E+00 6.947E-03 3 . 266E-03 3.326E-03 -0.216 0.256 0.246 0.0500 3 . 587E+00 2.473E-02 3.61 2E+00 8 . 285E-03 3.595E-03 4.355E-03 -0.211 0.249 0.240 0.0550 3 . 367E+00 2 . 520E-0 2 3 . 393E+00 9.714E-03 3. 91 7E-03 4 . 904E-03 -0.207 0.243 0.235

0.0600 3. 181E+00 2.564E-02 3 . 206E+00 1 . 1 23E-02 4 . 233E-03 5.473E-03 -0.203 0.238 0.230

0.0700 2.880E+00 2 . 642E-02 2. 907E+00 1 .451 E-02 4.349E-03 6.667E-03 -0.197 0.229 0.222

0.0800 2 . 649E+00 2.713E-02 2. 676E+00 1 . 8 1 0E-02 5 . 445E-0 3 7 . 935E-03 -0 . 1 92 0.222 0.215

0.0900 2 . 465E+00 2 . 778E-02 2 . 492E+00 2.1 98E-02 6 . 023E-03 9.276 E-03 -0.188 0.216 0.210 0.1000 2.31 5E + 00 2 . 838E-02 2.343E+00 2.61 2E-02 6 . 584E-0 3 1 . 069E-02 -0.184 0.211 0.205

0.1250 2.039E+00 2.975E-02 2.069E+00 3 . 752E-02 7.920E-03 1 . 451 E-02 -0.177 0.201 0.196 0.1500 1 . 852E+00 3. 100E-02 1 . 883E+00 5 . 021 E-02 9.1 72E-03 1 .875E-02 -0.171 0.193 0.189

0.1750 1 .71 7E+00 3.21 6 E-02 1 . 749E + 00 6.401 E-02 1 . 035E-02 2 . 338E-02 -0.166 0.187 0.183

0.2000 1 . 6 1 5E+00 3.328E-02 1 . 648E+00 7.876E-02 1 .147E-02 2 . 838E-02 -0.161 0.182 0.178

0.2500 1 . 473E+00 3.550E-02 1 . 508E+00 1 . 106E-01 1 . 356E-02 3 . 942E-02 -0.154 0.174 0.171 0.3000 1 . 380E+00 3.776E-02 1 . 4 1 8E+00 1 . 448E-01 1 . 548E-0 2 5 . 1 66E-02 -0.148 0.168 0.164

0.3500 1 .316E+00 4.01 0E-02 1 . 356E+00 1 .809E-01 1 . 729E-02 6 . 492E-02 -0.142 0.162 0.159

0.4000 1 . 26 9E + 00 4.252E-02 1 . 31 2E+00 2.185E-01 1 . 900E-02 7 . 898E-02 -0.137 0.158 0.154

0.4500 1 . 235E+00 4 . 505E-02 1 . 280 E+0 0 2.571E-01 2.065E-02 9 . 366E-02 -0.133 0.154 0.150 0.5000 1 . 20 9E+00 4.766E-02 1 . 257E+00 2. 965E-01 2 . 224E-02 1 . 088E-0

1

-0.129 0.150 0.146 0.5500 1 . 189E+00 5.035E-02 1 .239E+00 3.366E-01 2 . 379E-02 1 . 243E-0

1

-0.126 0.147 0.142

0.6000 1 . 1 74E+00 5.31 IE-02 1 . 227E+00 3.772E-01 2 . 530E-02 1 . 399E-0

1

-0.122 0.144 0.139

0.7000 1 . 152E+00 5.881 E-02 1 .21 1 E+00 4.593E-01 2 . 825E-02 1 .717 E— 0

1

-0.117 0.138 0.133

0.8000 1 . 140E+00 6 . 472E-02 1 . 204E + 00 5.421E-01 3.111 E-02 2.036E-01 -0.112 0.134 0.128

0 . 9000 1 . 1 32E+00 7 . 083E-02 1 . 20 3E+0 0 6.252E-01 3.391 E-02 2 . 354E-0

1

-0.108 0.130 0.124

1.0000 1 . 12SE+00 7.71 2E-02 1 . 205E+00 7 . 083E-0

1

3 . 666E-02 2.669E-01 -0.105 0.126 0.120

1 .2500 1 . 1 27E+00 9.354E-02 1 . 220E+00 9.146E-01 4 . 340E-02 3.436E-01 -0.098 0.119 0.111

1 .5000 1 . 1 32E + 0 0 1 . 108E-01 1 . 243E+00 1 . 1 18E+00 4. 998E-02 4.1 68E-01 -0.092 0.113 0.105

1 .7500 1 . 1 40E+0 0 1 . 287E-01 1 . 26 9E + 00 1 . 31 7E+00 5 . 646E-02 4.863E-01 -0.088 0.108 0.099 2.0000 1 . 149E+00 1 . 472E-0

1

1 . 297E+00 1 .51 2E+00 6.284E-02 5 . 525E-0

1

-0.084 0.104 0.094 2.5000 1 . 1 68E+00 1 . 855E-0

1

1 . 354E+0 0 1 .889E+00 7 . 534E-0 2 6.753E-01 -0.078 0.098 0.087

3.0000 1 . 186E+00 2.251 E-01 1 . 4 1 2E+00 2.251 E+00 8.750E-02 7.874E-01 -0.074 0.092 0.080 3.5000 1 .203E+00 2.659E-01 1 .469E+00 2.598E+00 9. 933E-02 8. 904E-01 -0.070 0.088 0.075

4.0000 1 . 21 8E+00 3 . 075E-0

1

1 . 526E+00 2. 932E+00 1 . 108E-01 9.857E-01 -0.067 0.084 0.071 4.5000 1 . 232E+00 3.499E-01 1 . 582E+00 3 . 254E+00 1 . 220E-0

1

1 . 075E+00 -0.064 0.081 0 .067 5.0000 1 . 244E+00 3.930E-01 1 . 6 37E + 00 3.564E+00 1 . 329E-0

1

1 . 1 58E+00 -0.062 0.078 0.064

5.5000 1 . 256E+00 4.366E-01 1 . 6 92E+00 3 . 865E+0 0 1 . 434E-0

1

1 . 236E + 00 -0.060 0.076 0.061

6 .0000 1 . 266E+00 4 . 808E-0

1

1 . 747E+00 4 . 1 55E+00 1 . 537E-0

1

1.311 E+00 -0 .058 0.073 0.059

7.0000 1 . 285E+00 5.706E-0T 1 . 856 E+00 4.71 1 E+00 1 . 734E-0

1

1 . 449E + 00 -0.054 0.069 0.054 8.0000 1 .301E+00 6 . 620E-01 1 . 963E+00 5 . 234E+00 1 . 920E-01 1 . 57 6E + 00 -0.051 0.066 0.050

9.0000 1 . 31 5E+00 7.547E-01 2 . 070E+00 5 . 730E+00 2.097E-01 1 . 6 95E+00 -0.048 0.063 0.047

10.0000 1 . 328E+00 8.486E-01 2.176E+00 6 . 202E+00 2.265E-01 1 . 80 5E+00 -0.045 0.061 0.044

12.5000 1 . 353E+00 1 . 087E+0 0 2. 441 E+00 7 . 286 E+0 0 2.649E-01 2 . 057E+00 -0.040 0.055 0.038

15.0000 1 . 374E+00 1 . 331 E+00 2 . 705E+00 8 . 258E+00 2. 990E-01 2.279E+00 -0.035 0.051 0.033

17.5000 1 . 390E+00 1 . 578E+00 2. 969E+00 9. 1 40 E + 0 0 3 . 295E-0

1

2 . 478E+00 -0.032 0.048 0.029

20.0000 1 . 404E+00 1 . 82 9E + 0 0 3 . 233E+00 9 . 947E+0 0 3.570E-01 2 . 658E+00 -0.029 0.045 0.026 25.0000 1 . 426E+00 2 . 338E+00 3.764E+00 1 . 138E+01 4.045E-01 2 . 974E+00 -0.025 0.041 0.022

30.0000 1 . 444E+00 2 . 854E+00 4 . 298E+00 1 . 262E+0

1

4.443E-01 3 . 244E+00 -0.022 0.038 0.019

35.0000 1 . 459E+00 3 . 376E+0 0 4 . 834E+00 1 . 372E+0

1

4 . 782E-0

1

3 . 480E+00 -0.020 0.035 0.016 40.0000 1 .471E+00 3. 902E+00 5. 373E+00 1 .470 E+0

1

5.075E-01 3 . 689E+00 -0.019 0.033 0.014

45.0000 1 .481 E+00 4 . 433E+00 5.91 4E+00 1 . 559E+0

1

5.332E-01 3 . 878E+00 -0.017 0.031 0.013 50.0000 1 .491 E+00 4. 966E+00 6 . 457E+00 1 . 6 39E + 0

1

5 . 558E-0

1

4 . 049E+00 -0.016 0.030 0.012 55.0000 1 . 499E+00 5 . 503E+00 7 . 002E+00 1 .714E+01 5.760E-01 4. 206E+00 -0.015 0.029 0.011 60.0000 1 . 506E+00 6.041 E+00 7 . 547E+00 1 . 783E+0

1

5.941E-01 4.351 E+00 -0.014 0.028 0.010 70.0000 1 .51 9E+00 7 . 1 24E+00 8 . 643E+00 1 . 906E+0

1

6 . 253E-0

1

4.61 2E+00 -0.013 0.026 0.008 80.0000 1 . 530 E+0 0 8.21 3E+00 9 . 743E+00 2.015E+01 6.514E-01 4.843E+00 -0.011 0.025 0.007 90.0000 1 . 540E+00 9 . 307E+00 1 . 085E+0

1

2.1 12E+01 6 .736E-01 5 . 050E + 00 -0.010 0.024 0.007 100.0000 1 . 548E+00 1 . 040E+01 1 . 1 95E+0

1

2.200E+01 6 . 927E-01 5 . 237E+00 -0.009 0.023 0.006 125.0000 1 . 565E+00 1 .316E+01 1 . 473E+0

1

2. 388E+01 7 . 307E-0

1

5 . 640E+00 -0.007 0.021 0.005

1 50.0000 1 .579E+00 1 . 593E+0

1

1 .751 E+0

1

2 . 544E+0

1

7.593E-01 5. 976E+00 -0.006 0.020 0.004 175.0000 1 . 590 E + 0 0 1 . 872E+0

1

2.031 E+0

1

2 . 676E+0

1

7.817E-01 6 . 263E+00 -0.005 0.019 0.003 200.0000 1 . 600E+00 2.150E+01 2.310E+01 2 . 792E+0

1

7.998E-01 6.51 3E+00 -0.005 0.018 0.003 250.0000 1 . 6 1 6E+00 2.710E+01 2 . 87 1 E+0

1

2. 985E+01 8 . 274E-0

1

6 . 936E+00 -0.004 0.017 0.002

300 .0000 1 . 6 29E + 0 0 3 . 270E+0

1

3 . 433E+0

1

3.144E+01 8.475E-01 7 . 284E+00 -0.003 0.016 0.002 350.0000 1 . 639E+00 3 . 832E+0

1

3. 996E+01 3.279E+01 8.630E-01 7 . 53 1 E+00 -0.003 0.016 0.002 400.0000 1 . 649E+00 4.395E+01 4 . 560E+0

1

3.396E+01 8.753E-01 7 . 839E+00 -0.003 0.015 0.002 450.0000 1 . 657E+00 4 . 958E+01 5.124E+01 3 . 500E+0

1

8 . 854E-0

1

8 . 067E+00 -0.002 0.015 0.001 500.0000 1 . 664E+00 5 . 522E+0

1

5 . 688E+0

1

3.592E+01 8 . 938E-01 8 . 272E+00 -0.002 0.014 0.001 550.0000 1 . 670E+00 6 .086E+01 6 . 253E+0

1

3 . 676E+0

1

9.009E-01 8 . 458E+00 -0.002 0.014 0.001 600.0000 1 . 67 6 E+OO 6.651 E+0

1

6.81 9E+01 3 . 753E+0

1

9.070E-01 8 . 629E+00 -0.002 0.014 0.001 700.0000 1 . 687E+00 7.781E+01 7 . 950 E+0

1

3.88SE+01 9. 170E-01 8.931 E+00 -0.001 0.013 0.001 800.0000 1 . 6 95E+00 8.913E+01 9 . 082E+0

1

4.006E+01 9.249E-01 9 . 1 94E+00 -0.001 0.013 0.001 900.0000 1 . 70 3E+0 0 1 . 004E+02 1 .021E+02 4.1 1 0 E+0

1

9.31 3E-01 9 . 427E+00 -0.001 0.013 0.001

1 000.0000 1 .710E+00 1 .1 18E+02 1 . 1 35E+02 4 . 202E+0

1

9.366E-01 9 . 635E + 00 -0.001 0.012 0.001

99
ELECTRONS IN XENON

I = 482.0 eV DENSITY = 5.485E-03 g/cra 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV ca 2 /g MeV ca 2/g MeV cn 2 /g g/cra 2 0.0100 1 . 054E+0

1

1 . 686E-02 1 . 055E+0

1

5.971 E-04 7 . 837E-04 0 .

0

-0.315 0.431 0.391 0.0125 9 . 078E+00 1 .820E-02 9 . 0 97E+00 8.531E-04 9.869E-04 0.0 -0.295 0.393 0.359

0.0150 8 . 022E + 00 1 . 927E-02 8.041 E+00 1 . 1 46E-03 1 . 189E-03 0 .

0

-0.280 0.365 0.337 0.0175 7.218E+00 2.016E-02 7 . 238E+00 1 . 47 4E-0 3 1 .389E-03 0 .

0

-0.269 0.345 0.320

0 .0200 6 . 583E + 00 2 . 092E-02 6 . 604E+00 1 .836E-03 1 .583E-03 0.0 -0.260 0.329 0.307

0.0250 5.641 E+00 2.216E-02 5 . 664E+00 2 . 657E-03 1 . 979E-03 0.0 -0.246 0 . 305 0.287

0.0300 4. 974E+00 2.315E-02 4. 997E+00 3 . 600E-03 2.361E-03 0.0 -0.236 0.288 0.272

0.0350 4 . 473E+00 2.399E-02 4 . 497E+00 4.656E-03 2.736E-03 0.0 -0.228 0.275 0.261 0.0400 4 . 083E+00 2.471 E-02 4. 108E+00 5.821E-03 3.104E-03 0.0 -0.221 0.264 0.253

0.0450 3.77CE+00 2.535E-02 3 . 796E+00 7 . 089E-03 3.464E-03 0.0 -0.216 0.256 0.245

0.0500 3.513E+00 2 . 5 93E-0 2 3 . 539E+00 8.454E-03 3.818E-03 0.0 -0.211 0.249 0.239

0.0550 3 . 298E+00 2 . 646E-02 3 . 324E+00 9. 91 3E-03 4. 166E-03 0.0 -0.207 0.243 0.234

0.0600 3.1 15E+00 2.695E-02 3. 142E+00 1 . 146E-02 4 . 508E-03 0.0 -0.204 0.237 0.229

0.0700 2.821 E+00 2 . 784E-02 2.849E+00 1 .481 E-02 5. 175E-03 0.0 -0.198 0.229 0.222

0.0800 2 . 594E+00 2.864E-02 2 . 623E+00 1 . 847E-02 5.822E-03 0.0 -0.193 0.222 0.215

0.0900 2.41 4E+00 2. 938E-02 2 . 443E+00 2.243E-02 6 . 450E-03 0.0 -0.189 0.216 0.210

0.1000 2 . 267E+00 3 . 006E-02 2 . 298E+00 2 . 665E-02 7.060E-03 0.0 -0.185 0.211 0.206 0.1250 1 . 998E+00 3.161 E-02 2.030E+00 3.327E-02 8.517E-03 0.0 -0.178 0.201 0.197

0.1500 1 .81 5E+00 3 . 300E-02 1 . 848E+00 5.121 E-02 9 . 886E-03 0.0 -0.173 0.194 0.190

0.1750 1 . 683E+00 3.429E-02 1 . 71 7E+00 6 . 527E-02 1 . 1 18E-02 0.0 -0.169 0.188 0.184

0.2000 1 . 584E+00 3.554E-02 1 . 6 1 9E+00 8 . 028E-02 1 . 240E-02 0.0 -0.165 0.184 0.180 0.2500 1 . 445E+00 3.797E-02 1 . 483E+00 1 . 126E-01 1 . 468E-0 2 0.0 -0.159 0.176 0.173

0.3000 1 . 355E+00 4 . 042E-02 1 . 396E+00 1 . 475E-0

1

1 . 678E-02 0.0 -0.155 0.171 0.167

0.3500 1 . 293E+00 4.295E-02 1 . 336E+00 1 .841E-01 1 . 875E-02 0.0 -0.151 0.166 0.163

0.4000 1 . 249E+00 4 . 555E-02 1 . 294E+00 2 . 222E-0

1

2.062E-02 0.0 -0.148 0.162 0.159

0.4500 1 .21 6E+00 4.824E-02 1 . 264E+00 2.613E-01 2 . 240E-02 0.0 -0.145 0.159 0.156

0.5000 1 . 1 92E+00 5. 103E-02 1 . 243E+00 3.012E-01 2.41 2E-02 0.0 -0.142 0 . 1 56 0.153

0.5500 1 . 1 73E+00 5 . 389E-02 1 . 227E+00 3.417E-01 2.579E-02 0.0 -0.140 0.154 0.150

0.6000 1 . 1 59E+00 5.681E-02 1 . 21 6E+00 3 . 826E-0

1

2 . 742E-0 2 '0.0 -0.138 0.152 0.148

0.7000 1 . 1 40E+00 6 . 285E-02 1 . 203E+00 4.654E-01 3 . 057E-02 0.0 -0.135 0.148 0.144

0.8000 1 . 1 30E + 00 6.91 0E-02 1 . 1 99E+00 5.487E-01 3 . 362E-02 0.0 -0.132 0.144 0.140 0.9000 1 . 124E+00 7.555E-02 1 . 200 E+00 6.321E-01 3 . 659E-02 0.0 -0.129 0.142 0.137

1 .0000 1 . 122E+00 8.217E-02 1 . 204E+00 7.153E-01 3 . 949E-02 0.0 -0.127 0.139 0.134

1 .2500 1 . 126E+00 9. 943E-02 1 . 225E+00 9.21 3E-01 4 . 654E-02 0.0 -0.123 0.134 0.128

1 .5000 1 . 1 35E+00 1 . 176E-01 1 . 253E+00 1 . 1 23E+00 5 . 337E-02 0.0 -0.119 0.130 0.123

1 .7500 1 . 147E+00 1 . 364E-0

1

1 . 284E+00 1 . 320E+00 6 . 004E-02 0.0 -0.116 0 . 1 26 0.119

2.0000 1 . 160E+00 1 . 557E-0

1

1 . 31 6E+00 1 .51 3E+00 6 . 657E-02 0.0 -0.114 0.123 0.115

2.5000 1 . 186E+00 1 . 958E-0

1

1 . 382E+00 1 . 883E+00 7 . 927E-02 0.0 -0.110 0.118 0.1C9

3.0000 1.211 E+00 2.373E-01 1 . 448E+00 2 . 237E+00 9.153E-02 0.0 -0.107 0.114 0.104

3.5000 1 . 233E+00 2.798E-01 1 .51 3E+00 2 . 574E+00 1 .034E-01 0.0 -0.104 0.110 0.100 4.0000 1 . 254E+00 3.233E-01 1 . 577E+00 2.898E+00 1 . 1 48E-0

1

0.0 -0.102 0.107 0.097 4.5000 1 . 273E+00 3.675E-01 1 . 640E+00 3 . 209E+00 1 .259E-01 0.0 -0.100 0.105 0.093

5.0000 1 . 290E+00 4.124E-01 1 . 703E+00 3 . 508E+0 0 1 . 366E-01 0.0 -0.099 0.102 0.090

5.5000 1 . 306E+00 4.580E-01 1 . 764E+00 3 . 796E+00 1 . 470E-0

1

0.0 -0.097 0.100 0 . 088 6.0000 1 . 321 E+00 5.040E-01 1 . 825E+00 4 . 075E+00 1 .571E-01 0.0 -0.096 0.098 0.085

7.0000 1 . 348E+00 5.976E-01 1 . 946E+00 4 . 606E+00 1 . 764E-0

1

0.0 -0.094 0.094 0.081

8 .0000 1 . 372E+00 6 . 927E-01 2 . 065E+00 5. 104E+00 1 . 945E-0

1

0.0 -0.092 0.091 0.077

9.0000 1 . 393E+00 7.893E-01 2. 182E+00 5 . 575E+00 2.11 7E-01 0.0 -0.091 0.089 0.074

10.0000 1 . 41 2E+00 8.870E-01 2 . 299E+00 6 . 022E+00 2.279E-01 0.0 -0.090 0.086 0.071 12.5000 1 . 453E+00 1 . 1 36E+00 2 . 58 9E+0 0 7 . 046E+00 2 . 649E-0

1

0.0 -0.087 0.081 0.065

15.0000 1 . 487E+00 1 . 389E+00 2 . 876E+00 7 . 962E+00 2.977E-01 0.0 -0 .085 0.077 0.060

17.5000 1 . 5 1 5E+00 1 . 647E+00 3. 162E+00 8 . 790E+00 3.269E-01 0.0 -0.084 0.074 0.056

20 .0000 1 . 540E+00 1 . 907E+00 3 . 447E+00 9 . 547E+00 3 . 532E-0

1

2.396E-03 -0.080 0.071 0.053

25.0000 1 . 58 1 E+00 2 . 436E+00 4 .01 7E+00 1 . 089E+0

1

3. 988E-01 2 . 422E-02 -0.074 0.066 0.047

30.0000 1 . 6 1 3E+00 2 . 973E+00 4 . 586E+00 1 . 205E+0

1

4.370E-01 5.61 4E-02 -0.070 0.063 0.042

35.0000 1 . 640E+00 3.51 7E+00 5. 156E+00 1 . 308E+0

1

4.697E-01 9. 173E-02 -0.067 0.059 0.038

40.0000 1 . 662E+00 4 . 064E+00 5 . 727E+00 1 . 400E+0

1

4.980E-01 1 . 286E-0

1

-0.065 0.057 0.035

45.0000 1 . 682E+00 4.61 6E+00 6 . 299E+00 1 . 483E+0

1

5.229E-01 1 . 660E-01 -0.062 0.055 0.032

50.0000 1 . 700E+00 5.171 E+00 6 .871 E+00 1 .559E+01 5.449E-01 2.033E-01 -0.060 0.053 0.030 55.0000 1 . 71 6E+00 5 . 730E+00 7 . 445E+00 1 . 629E+0

1

5 . 646E-0

1

2.405E-01 -0.059 0.051 0.028 60.0000 1 . 730E+00 6 . 290E+00 8 . 020E+00 1 -694E+01 5.823E-01 2 . 775E-0

1

-0.057 0.050 0.026 70.0000 1 . 754E+00 7.41 7E+00 9. 172E+00 1 . 8 1 0 E + 0

1

6 . 1 30E-01 3.504E-01 -0.054 0.047 0 .024 30.0000 1 .775E+00 8.551 E+00 1 . 033E+0

1

1 . 91 3E+01 6.387E-01 4.215E-01 -0.051 0.045 0.021 90.0000 1 . 793E+00 9 . 689E+00 1 . 1 48E+0

1

2 . 005E+0

1

6.606E-01 4 . 905E-01 -0 .049 0.044 0.020 100.0000 1 .809E+00 1 . 083E+0

1

1 .264E+01 2.088E+01 6 . 7 96E-0

1

5.571E-01 -0.047 0.042 0.018

125.0000 1 .841 E+00 1 . 370E+01 1 . 554E+0

1

2 . 266E+0

1

7.177E-01 7.131E-01 -0.043 0.039 0.015

150.0000 1 . 867E+00 1 . 6 59E+0

1

1 . 846E+01 2.41 3E+01 7.465E-01 8.546E-01 -0.040 0.037 0.013

175.0000 1 .888E+00 1 . 949E+01 2.1 37E+01 2 . 539E+0

1

7.693E-01 9.836E-01 -0.038 0.035 0.011 200.0000 1 . 905E+00 2 . 239E+0

1

2 . 430E+0

1

2 . 649E+0

1

7.877E-01 1 . 102E+00 -0.036 0.034 0.010 250.0000 1 . 934E+00 2.821 E+01 3.015E+01 2 . 833E+0

1

8. 160E-01 1 .313E+00 -0.033 0.032 0.009

300.0000 1 . 957E+00 3 . 405E+0

1

3.601 E+0

1

2 . 935E+0

1

8 . 368E-0

1

1 . 499E+00 -0.031 0.031 0.007

350.0000 1 . 976E+00 3 . 990E+0

1

4. 188E+01 3. 1 13E+01 8.529E-01 1 . 665E+00 -0.029 0.029 0.006 400.0000 1 . 992E+00 4 . 576E+0

1

4 . 775E+0

1

3 . 225E+0

1

8.658E-01 1 .81 6E+00 -0.027 0.028 0.006 450.0000 2.005E+00 5. 163E+01 5.363E+01 3 . 324E+0

1

8.763E-01 1 . 956E+00 -0.025 0.028 0.005 500.0000 2.01 7E+00 5 . 750E+0

1

5. 952E+01 3.412E+01 8.851E-01 2 . 086E+00 -0.023 0 .027 0 .005 550.0000 2 . 027E+00 6 . 337E+0

1

6 . 540E+0

1

3.492E+01 8 . 926E-0

1

2 . 208E + 00 -0.022 0.026 0.004

600.0000 2 . 0 36E+00 6 . 926E+0

1

7. 129E+01 3 . 56 6 E+0

1

8.991E-01 2 . 322E+00 -0.021 0.026 0.004 700.0000 2 . 052E+00 8. 102E+01 8 . 308E+0

1

3.695E+01 9.097E-01 2 . 532E+00 -0.019 0.025 0.003 800.0000 2 . 066E+00 9 . 280E+0

1

9 . 487E+0

1

3 . 808E+0

1

9. 131 E-01 2 . 722E+00 -0.017 0 .024 0.003

900.0000 2 . 077E+00 1 . 046E+02 1 . 067E+02 3. 907E+01 9.249E-01 2 . 894E+00 -0.016 0.024 0.003

1000.0000 2 . 087E+00 1 . 1 64E+02 1 . 185E+02 3 . 996E+01 9 . 306E-01 3.052E+00 -0.015 0.023 0.003

100
ELECTRONS IN GADOLINIUM

I = 591 .0 eV DENSITY = 7 . 900E+00i g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(loqI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

Me V MeV cm 2 /g MeV cn 2 /g MeV cm 2 /g g/cm 2 0.0100 9 . 753E+00 1 . 847E-02 9.771 E+00 6.627E-04 9.223E-04 2.078E-03 -0.337 0.491 0.430 0.0125 8 . 440E + 00 2.008E-02 8 . 460 E + 00 9 . 385E-04 1 . 1 64E-03 2.671 E-03 -0.313 0.442 0.391 0.0150 7.481 E+00 2. 140E-02 7 . 502E+00 1 . 253E-03 1 . 406E-03 3 . 295E-03 -0.297 0.407 0 . 364 0.0175 6 . 747E+00 2 . 250E-02 6.769E+00 1 .604E-03 1 . 646E-03 3. 950E-03 -0.284 0.381 0 .344

0 . 0200 6 . 1 65E+00 2 . 345E-02 6. 189E+00 1 . 991 E-03 1 . 885E-03 4. 637E-03 -0.273 0.361 0.328

0.0250 5 . 299E+00 2.501 E-02 5 . 324E+00 2.866E-03 2. 357E-03 6 . 1 06E-03 -0.258 0 . 331 0 . 305 0.0300 4 . 681 E+00 2. 628E-02 4 . 707E+00 3 . 867E-0 3 2.821 E-03 7.705E-03 -0.246 0.310 0.288

0.0350 4.21 6E+00 2 . 736E-02 4 . 244E+00 4. 983E-03 3.278E-03 9 . 430E-03 -0.237 0.295 0 .276 0.0000 3 . 853E+00 2.831 E-02 3 . 88 2E+0 0 6.221 E-03 3.727E-03 1 . 1 28E-02 -0.230 0.282 0.266 0.0050 3.561 E+00 2.91 6E-02 3 .590E+00 7 . 562E-03 4 . 1 70E-03 1 . 324E-02 -0.223 0.272 0.257 0.0500 3.321 E+00 2 . 993E-02 3.351 E+00 9 . 005E-03 4 . 605E-03 1 . 530E-02 -0.218 0.263 0.250 0.0550 3 . 1 20E+00 3 . 064E-02 3.1 50E+00 1 . 054E-02 5 . 035E-03 1 . 746E-02 -0.213 0.256 0.244 0.0600 2. 948E+00 3.1 30 E-02 2. 980E+00 1 . 21 8E-02 5 . 458E-03 1 . 970E-02 -0.209 0.250 0.239

0 .0700 2 . 6 72E+00 3 . 25 1 E-02 2 . 705E+00 1 .571 E-02 6 . 288E-03 2.439E-02 -0.202 0.239 0.230 0.0800 2. 459E+00 3 . 360E-02 2 . 492E+00 1 . 956E-02 7 . 097E-03 2 . 926E-02 -0.197 0.231 0.222

0.0900 2 . 289E+00 3.461 E-02 2 . 324E+00 2 . 372E-02 7 . 885E-0 3 3.424E-02 -0.192 0.224 0.216 0.1000 2 . 1 5 1 E+00 3 . 554E-02 2. 186E+00 2.81 6E-02 8 . 655E-03 3.927E-02 -0.187 0.218 0.211 0.1250 1 . 896E+00 3 . 765E-02 1 . 934E+00 4 . 037E-02 1 . 050E-02 5 . 1 87 E-0 2 -0.179 0.207 0.200 0.1500 1 . 723E+00 3. 952E-02 1 . 762E+00 5. 394E-02 1 . 224E-02 6 .425E-02 -0.173 0.198 0.192 0.1750 1 . 597E+00 4 . 1 24E-02 1 . 539E+00 6 .868E-02 1 . 390E-02 7 . 632E-02 -0.168 0.191 0.186 0.2000 1 . 503E+00 4 . 287E-02 1 . 546E+00 8 . 440E-02 1 . 547E-02 8 . 808E-02 -0.163 0.185 0.180 0.2500 1 .371 E+00 4.601 E-02 1 . 41 7E+00 1 . 183E-01 1 .840E-02 1 . 108E-01 -0.156 0.177 0.172

0.3000 1 . 285E+00 4.91 2E-02 1 . 334E+00 1 . 547E-0

1

2.111 E-02 1 . 327E-0

1

-0.151 0.170 0.165

0 . 3500 1 . 225E+00 5.225E-02 1 . 278E+00 1 .931E-01 2 . 365E-02 1 . 538E-0

1

-0.146 0.164 0.160 0.4000 1 . 183E+00 5 . 547E-02 1 . 238E+00 2 . 329E-0

1

2 . 605E-02 1 . 743E-01 -0.142 0.160 0.155

0.4500 1 .151 E+00 5.875E-02 1 .21 0E+00 2.737E-01 2.835E-02 1 . 943E-01 -0.138 0.156 0.151 0.5000 1 . 1 27E+00 6.21 IE-02 1 . 189E+00 3.1 54E-01 3 . 055E-02 2.138E-01 -0.135 0.152 0.148

0.5500 1 . 1 09E+00 6 . 553E-02 1 . 1 74E+00 3.578E-01 3.269E-02 2 . 328E-0

1

-0.132 0.149 0.145 0.6000 1 . 095E+00 6 . 903E-02 1 . 1 64E+0C 4.006E-01 3 . 476E-02 2.514E-01 -0 . 1 30 0.147 0.142

0.7000 1 . 075E+00 7.61 9E-02 1 . 1 52E+00 4.870E-01 3.876 E-0 2 2 . 876E-0

1

-0.125 0.142 0.137

0.8000 1 . 064E+00 8.356E-02 1 . 1 48E+00 5.740E-01 4 . 26 0 E-0 2 3 . 223E-0

1

-0.121 0.138 0.132

0 . 9000 1 . 057E+00 9.11 2E-02 1 . 149E+00 6.61 IE-01 4.632E-02 3.556E-01 -0.118 0.134 0.128

1 .0000 1 . 054E+00 9.888E-02 1 . 1 53E+00 7.481E-01 4. 994E-02 3.878E-01 -0.115 0.131 0.125

1 .2500 1 . 054E+00 1 . 1 90E-01 1 . 1 7 3 E+00 9.631E-01 5 . 868E-02 4 . 637E-01 -0.109 0.124 0.117

1 .5000 1 . 060E+00 1 .399E-01 1 . 20 0 E + 0 0 1 . 1 74E+00 6 . 707E-02 5 . 337 E-0

1

-0.104 0.119 0.111

1 .7500 1 . 06 9E+00 1 .616E-01 1 . 231 E+00 1 . 380E+00 7 . 520E-02 5 . 989E-01 -0.100 0.114 0.106 2.0000 1 .079E+00 1 .839E-01 1 . 262E+00 1 . 580E+00 8.312E-02 6 . 60 0 E-0

1

-0.096 0.111 0.101 2.5000 1 . 098E+00 2.299E-01 1 . 328E+00 1 . 966E+00 9 . 840 E-0 2 7 . 725E-01 -0.090 0.104 0.094

3.0000 1 . 1 16E+00 2 . 773E-0

1

1 . 394E+00 2 . 334E+0 0 1 .130E-01 8.746E-01 -0.085 0.099 0.087

3.5000 1 . 1 33E+00 3 . 259E-0

1

1 . 459E+00 2 . 684E+00 1 .271E-01 9.689E-01 -0.081 0.095 0.082

4.0000 1 . 1 48E+00 3 . 754E-01 1 . 524E+00 3 . 020E+00 1 . 406E-0

1

1 . 057E+00 -0.077 0.091 0.078 4.5000 1 . 1 62E+00 4.258E-01 1 . 588E+0 0 3.341 E+00 1 .535E-01 1 . 1 39E+00 -0.074 0.087 0.074 5.0000 1 . 1 74E+00 4.770E-01 1 .651 E+00 3 . 650E+00 1 .661E-01 1 .217E+00 -0.071 0 . 084 0 .070 5.5000 1 . 186E+00 5.288E-01 1 . 71 5E+00 3. 947E+00 1 .781E-01 1 . 291 E+00 -0.068 0.082 0.067

6.0000 1 . 1 96E+00 5.31 IE-01 1 . 777E+00 4 . 234E+00 1 . 89SE-0

1

1 . 36 1 E + 0 0 -0 .066 0.079 0.064

7.0000 1 .21 5E+00 6 . 874E-0

1

1 . 902E+00 4 . 777E+00 2.11 9E-01 1 . 492E+00 -0.062 0.075 0.059

8 .0000 1 .231 E+00 7. 954E-01 2 . 026E+00 5 . 287E+00 2.325E-01 1 .612E+00 -0.059 0.072 0.054

9.0000 1 . 245E+00 9.049E-01 2 . 1 50 E+OO 5 . 766E+00 2.51 9E-01 1 . 723E+00 -0.056 0.068 0.051 10.0000 1 . 257E+00 1 .016 E+00 2 . 273E+00 6.21 8E+00 2.701 E-01 1 . 82 6 E+0 0 -0.054 0.066 0 .048 12.5000 1 . 284E+00 1 . 298E+00 2. 581 E+00 7 .249E+00 3.1 12E-01 2 . 056E+00 -0.049 0.060 0.041 15.0000 1 . 304E+00 1 . 585E+00 2.889E+00 8 . 1 64E+00 3.471 E-01 2 . 255E+00 -0.046 0.056 0.037

17.5000 1 . 322E+00 1 . 877E+00 3. 1 98E+00 8. 986E+00 3.787E-01 2 . 433E+00 -0.042 0.053 0.033

20 .0000 1 . 337E+00 2.172E+00 3 . 508E+00 9 . 732E+00 4.068E-01 2. 593E+00 -0.040 0.050 0.030 25.0000 1 . 360E+00 2.771 E+00 4.131 E+00 1 . 1 04E+0

1

4.546E-01 2 . 875E+00 -0.035 0.045 0 .025 30.0000 1 . 379E+00 3 . 379E+00 4 . 758E+00 1 .21 7E+01 4 . 941 E-01 3.11 9E+00 -0.031 0.042 0 .022 35.0000 1 . 394E+00 3. 994E+00 5 . 388E+00 1 .316E+01 5 . 272E-0

1

3. 334E+00 -0.028 0.040 0.019 40.0000 1 . 407E+00 4.61 5E+00 6 . 022E+00 1 . 404E+0

1

5.556E-01 3 . 528E+00 -0.026 0.038 0.017 45.0000 1 . 4 1 8E+00 5 . 240 E+0 0 6 . 6 58E+00 1 . 482E+0

1

5.802E-01 3 . 704E+00 -0.024 0.036 0.015 50.0000 1 . 428E+00 5.869E+00 7 . 297E+00 1 . 554E+0

1

6.018E-01 3 . 865E+00 -0.022 0.034 0.014 55.0000 1 . 436E+00 6 . 502E+00 7 . 938E+00 1 .620E+01 6 .209E-01 4.01 4E+00 -0.020 0.033 0.013 60.0000 1 . 444E+00 7 . 1 36 E+00 8 . 580E+00 1 . 680E+01 6 .379E-01 4 . 1 52E+00 -0.019 0.032 0.012 70.0000 1 . 457E+00 8.41 4E+00 9 . 87 1 E+00 1 . 789E+0

1

6 . 672E-0

1

4 . 40 0 E+0 0 -0.017 0.030 0.010 80.0000 1 . 468E+00 9 . 6 98E+00 1 . 1 17E+01 1 . 884E+0

1

6 . 91 4E-01 4.621 E+00 -0.016 0.029 0.009

90.0000 1 . 478E+00 1 . 0 9 9E+0

1

1 . 247E+0

1

1 . 969E+01 7 . 1 18E-01 4.818 E+00 -0.015 0.028 0.008

100.0000 1 . 487E+00 1 . 229E+01 1 . 377E+01 2.045E+01 7.293E-01 4 . 997E+00 -0.013 0 .027 0 .007 125.0000 1 . 504E+00 1 . 554E+0

1

1 . 704E+0

1

2 . 208E+0

1

7.640E-01 5 . 334E+00 -0.011 0.025 0.006

150.0000 1 . 51 8E+00 1 .881 E+01 2.033E+01 2 . 342E+0

1

7 . 898E-0

1

5.707E+00 -0.010 0.024 0.005

175.0000 1 . 530E+00 2.210E+01 2.363E+01 2 . 456E+0

1

8 . 0 99E-0

1

5 . 984E+00 -0.008 0.023 0.004 200.0000 1 . 540E+00 2 . 539E+0

1

2.693E+01 2 . 555E+0

1

8.260E-01 6 . 228E+00 -0.007 0.022 0.004 250.0000 1 . 556E+00 3.199E+01 3 . 355E+0

1

2.721 E+01 8.506 E-0

1

6.641 E+00 -0 .006 0.020 0.003 300.0000 1 . 568E+00 3.861E+01 4.018E+01 2.857E+01 8 . 684E-0

1

6 . 983E+00 -0.005 0.019 0.002 350.0000 1 . 57 9E+0 0 4 . 524E+0

1

4 . 682E+0

1

2 . 972E+0

1

8 . 820 E-0

1

7 . 27 5E + 0 0 -0.004 0.019 0 .002 400.0000 1 . 588E+00 5 . 188E+01 5.346E+01 3 . 072E+0

1

8 . 928E-01 7 . 530E + 00 -0.004 0.018 0.002 450.0000 1 . 596E+00 5.853E+01 6.012E+01 3. 160E+01 9 . 0 1 6 E-0

1

7 . 756E+00 -0.004 0.018 0.002 500.0000 1 . 6 0 3E+00 6.518E+01 6 . 678E+0

1

3 . 239E+0

1

9.089E-01 7 . 958E+00 -0.003 0.017 0.002 550.0000 1 . 6 1 0E+00 7.184E+01 7 . 345E+0

1

3.31 1E+01 9. 151 E-01 8 . 1 42E + 00 -0.003 0.017 0.001 600.0000 1 . 6 1 5E+00 7.850E+01 8.01 1 E+01 3 . 376E+0

1

9.204E-01 8.31 1 E+00 -0.003 0.016 0.001 700.0000 1 . 626E+00 9.185E+01 9 . 346E+0

1

3.491E+01 9.291 E-0

1

8.61 0E+00 -0.002 0.016 0.001 800.0000 1 . 634E+00 1 . 052E+02 1 . 068E+02 3.591 E+0

1

9 . 359E-0

1

8 . 87 1 E + 0 0 -0.002 0.015 0.001 900.0000 1 . 642E+00 1 . 185E+02 1 . 202E+02 3 . 680E+0

1

9.41 5E-01 9. 1 01 E+00 -0 .002 0.015 0.001 1000.0000 1 . 649E+00 1 .31 9E+02 1 . 335E+02 3 . 758E+0

1

9. 460E-01 9 . 308E+00 -0.002 0.015 0.001

101
ELECTRONS IN TUNGSTEN

I = 727.0 eV DENSITY = 1 . 930E+01 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2/g MeV cm 2/g g/cm 2 0.0100 8. 974E+00 1 . 977E-02 8. 993E+00 7.489E-04 1 . 076E-03 9.91 IE-04 -0 . 362 0.595 0.487

0.0125 7.806E+00 2. 165E-02 7 . 828E+00 1 . 048E-03 1 . 357E-0

3

1 .263E-03 -0 . 335 0.524 0 . 435 0.0150 6 . 945E+00 2 . 320E-02 6 . 968E+00 1 . 387E-0

3

1 .639E-03 1 . 544E-03 -0.316 0.475 0.401 0.0175 6.281E+00 2 . 450E-02 6 . 306E+00 1 . 765E-03 1 . 920E-03 1 . 8 34E-0 3 -0 . 302 0.439 0 . 376 0.0200 5 . 753E+00 2.563E-02 5.779E+00 2.179E-03 2.200E-03 2.133E-03 -0.290 0.412 0.357

0.0250 4.961 E+00 2 . 752E-02 4.989E+00 3.11 4E-03 2.756E-03 2.758E-03 -0.273 0.372 0.329

0.0300 4. 394E+00 2. 908E-02 4 . 423E+00 4. 181E-03 3 . 304E-03 3.417E-03 -0.260 0 . 345 0.309

0.0350 3. 966E+00 3 . 042E-02 3 . 996 E + 00 5. 372E-03 3.846E-03 4.109E-03 -0.250 0.324 0.294

0.0400 3.631 E+00 3.160E-02 3 . 662E+00 6.681E-03 4.381E-03 4.834E-03 -0.242 0.309 0.283

0.0450 3 . 360E+00 3 . 267E-02 3 . 393E+00 8.101E-03 4.908E-03 5.591 E-0 3 -0.236 0.296 0.273

0.0500 3.1 37E+00 3 . 364E-02 3.171 E+00 9 . 627E-03 5.430E-03 6 . 378E-0 3 -0.230 0.286 0.265

0.0550 2 . 950 E+00 3.454E-02 2 . 985E+00 1 . 125E-02 5 . 944E-03 7 . 1 95E-03 -0.225 0.277 0.258

0.0600 2.791 E+00 3 . 539E-02 2 . 826 E+0 0 1 . 298E-02 6.453E-03 8.041E-03 -0.221 0.269 0.252

0.0700 2 . 533E + 00 3.694E-02 2 . 570E+00 1 .669E-02 7.453E-03 9.817E-03 -0.214 0.257 0.243

0.0300 2. 335E + 00 3 . 834E-02 2 . 373E+00 2.075E-02 8.430E-03 1 . 170E-02 -0.208 0.247 0.235

0.0900 2. 176E + 00 3.964E-02 2.21 6E+00 2.51 IE-02 9.385E-03 1 . 369E-02 -0.203 0.239 0.228

0.1000 2 . 047E + 00 4.084E-02 2 . 088E+00 2 . 977E-02 1 . 032E-02 1 . 577E-02 -0.198 0.233 0.222

0.1250 1 .808E+00 4 . 355E-02 1 . 85ZE+00 4 . 253E-02 1 . 257E-02 2.1 39E-02 -0.190 0.220 0.211 0.1500 1 . 646E+00 4 . 595E-02 1 . 6 92E+00 5 . 668E-02 1 . 470E-02 2 . 755E-02 -0.183 0.210 0.202

0.1750 1 . 528E+00 4.81 4E-02 1 . 576E+00 7 . 202E-02 1 .673E-02 3 . 420E-02 -0.177 0.203 0.196 0.2000 1 . 439E+00 5.021E-02 1 . 490E+00 8 . 835E-02 1 .865E-02 4.131E-02 -0.172 0.196 0.190

0.2500 1 . 31 5E+00 5.41 4E-02 1 . 370E+00 1 . 235E-0

1

2 . 226E-02 5.677E-02 -0.163 0.186 0.180

0.3000 1 . 234E+00 5 . 797E-02 1 . 292E+00 1 .61 IE-01 2.558E-02 7. 370E-02 -0.156 0.178 0.173

0.3500 1 . 178E+00 6.179E-02 1 . 240E+00 2.007E-01 2 . 870E-02 9. 188E-02 -0.149 0.172 0.166

0.4000 1 . 1 38E+00 6 . 565E-02 1 . 203E+00 2.416E-01 3. 164E-02 1 .111 E-0

1

-0.143 0.166 0.160

0.4500 1 . 108E+00 6.956E-02 1 . 177E+00 2.836E-01 3 . 443E-02 1 .310 E-0

1

-0.138 0.161 0.155

0.5000 1 . 085E+00 7 . 353E-02 1 . 159E+00 3.265E-01 3.712E-02 1 .515E-01 -0.134 0.157 0.151 0.5500 1 . 068E+00 7.755E-02 1 . 1 46E+00 3.699E-01 3. 971E-02 1 . 723E-0

1

-0.130 0.153 0.147

0 . 6000 1 . 055E+00 8 . 1 62E-02 1 . 1 36E+00 4.137E-01 4.221E-02 1 . 932E-01 -0.126 0.149 0.143

0.7000 1 . 036E+0 0 8 . 993E-02 1 . 126E+00 5.022E-01 4.702E-02 2.352E-01 -0.120 0.143 0.136

0.8000 1 . 025E+00 9.841E-02 1 . 124E+00 5.911 E— 0

1

5.161E-02 2.768E-01 -0.114 0.138 0.130

0 . 9000 1 .01 9E+00 1 .071E-01 1 . 1 26E+00 6.800E-01 5 . 602E-02 3.176E-01 -0.110 0.133 0.125

1 .0000 1 . 0 1 6E+0 0 1 .159E-01 1 . 1 32E+00 7.686E-01 6 . 030E-02 3.575E-01 -0.106 0.129 0.121

1 .2500 1 .01 6E+00 1 . 387E-0

1

1 . 154E+00 9.875E-01 7.051E-02 4.528E-01 -0.099 0.120 0.111

1 .5000 1 .021 E+00 1 .624E-01 1 . 183E+00 1 . 20 1 E+00 8.022E-02 5.416E-01 -0.094 0.114 0.104

1 .7500 1 . 029E+00 1 .368E-01 1 .21 5E+00 1 . 41 0E+00 8 . 955E-02 6 . 242E-01 -0.089 0.109 0.098

2.0000 1 . 037E+00 2.1 17E-01 1 . 249E+00 1 .61 3E+00 9.856E-02 7 .01 5E-01 -0.086 0.104 0.093

2.5000 1 . 055E+00 2.630E-01 1 .318E+00 2 . 003E+00 1 . 1 58E-0

1

8 . 423E-01 -0.080 0.097 0.085

3.0000 1 . 072E+00 3. 158E-01 1 . 388E+00 2 . 372E+00 1 .321E-01 9 . 684E-0

1

-0.075 0.092 0 .078 3.5000 1 . 087E+00 3.698E-01 1 . 457E+00 2. 724E+00 1 . 476E-0

1

1 . 083E+00 -0.072 0.087 0.073

4.0000 1 . 101E+00 4.248E-01 1 . 526E+00 3 . 059E+00 1 . 625E-0

1

1 . 188E+00 -0.068 0.083 0.069

4.5000 1 . 1 14E+00 4.806E-01 1 . 595E+00 3 . 380E+00 1 .766E-01 1 . 286 E + 0 0 -0.065 0.080 0.065

5.0000 1 . 1 26E+00 5.372E-01 1 . 663E+00 3 . 687E+00 1 . 902E-01 1 . 378E+00 -0.063 0.077 0.061 5.5000 1 . 1 36E+00 5.945E-01 1 . 731 E+00 3.981 E+00 2 . 032E-0

1

1 .463E+00 -0.061 0 .074 0.058

6.0000 1 . 1 46E+00 6 .523E-01 1 . 7 93E+00 4 . 265E+00 2.157E-01 1 . 544E+00 -0.059 0.072 0.056 7.0000 1 . 163E+00 7.697E-01 1 . 933E+00 4.801 E+00 2. 393E-01 1 . 694E+00 -0.055 0.068 0.051 3.0000 1 . 1 78E+00 8.890E-01 2 . 067E+00 5.301 E+00 2.612E-01 1 . 830E+00 -0.052 0.064 0.047

9.0000 1 . 1 91 E+00 1 .01 0E+00 2.201 E+00 5 . 770E+00 2.816E-01 1 . 955E+00 -0.050 0.061 0.044

10.0000 1 . 203E+00 1 . 1 32E+00 2 . 335E+00 6.211 E+00 3 . 006E-0

1

2 . 070E+00 -0.048 0.059 0.041 12.5000 1 . 227E+00 1 . 443E+00 2 . 670E+00 7.21 2E+00 3.432E-01 2 . 324E+00 -0 .043 0.054 0.035

15.0000 1 . 247E+00 1 . 759E+00 3 . 006E+00 3 . 0 94E+00 3.800E-01 2 . 544E + 0 0 -0.040 0.050 0.031 17.5000 1 . 263E+00 2.081 E+00 3 . 343E+00 8 . 882E+00 4.120E-01 2 . 737E+00 -0.037 0.047 0.028

20.0000 1 . 277E+00 2 . 406E+00 3 . 682E+00 9 . 594E+00 4.403E-01 2 . 91 0E+00 -0.035 0.044 0.025

25.0000 1 . 299E+00 3 . 065E+00 4.364E+00 1 . 034E+0

1

4.881E-01 3.21 2E+00 -0.031 0.040 0.021 30.0000 1 . 31 6E+00 3 . 7 35E+00 5.051 E+00 1 . 1 90E+01 5.270E-01 3.471 E+00 -0.027 0.038 0.018

35.0000 1 .331 E+00 4.41 2E+00 5 . 743E+00 1 . 283E+0

1

5 . 595E-0

1

3 . 698E+00 -0.025 0.035 0.016 40.0000 1 . 343E+00 5 . 0 96 E+0 0 6 . 439E+00 1 .365E+01 5.871E-01 3 . 90 1 E+00 -0.023 0.034 0.014

45.0000 1 . 353E+00 5 . 784E+00 7 . 1 38E+00 1 . 439E+0

1

6.109E-01 4 . 084E+00 -0.021 0.032 0.013

50 . 0000 1 . 362E+00 6 . 477E+00 7 . 840E+00 1 .506E+01 6.316E-01 4 . 252E+00 -0.019 0.031 0.012

55.0000 1 .371 E+00 7. 174E+00 8 . 544E+00 1 . 567E+0

1

6.500E-01 4 . 405E+00 -0.018 0.030 0.011 60.0000 1 . 378E+00 7 . 873E+00 9.251 E+00 1 . 623E+0

1

6 .662E-01 4 . 548E+00 -0.017 0.029 0.010 70.0000 1 . 391 E+00 9 . 280E+00 1 . 067E+0

1

1 . 724E+01 6 . 940E-0

1

4 . 804E+00 -0.015 0.027 0 .008 80.0000 1 . 401 E+00 1 . 070E+0

1

1 . 21 0E+0

1

1 .812E+01 7.169E-01 5 . 031 E+00 -0.014 0.026 0.007

90.0000 1 .411 E+00 1 .212E+01 1 . 353E+0

1

1 . 890E+0

1

7.362E-01 5 . 233E+00 -0.013 0.025 0.007

100.0000 1 .41 9E+00 1 . 355E+0

1

1 .496E+01 1 . 960E+0

1

7.526E-01 5.417E+00 -0.012 0 .024 0.006 125.0000 1 . 436E+00 1 .71 3E+01 1 . 857E+0

1

2.1 10E+01 7 .850E-01 5.812E+00 -0.010 0.022 0.005

150.0000 1 . 449E+00 2 . 074E+0

1

2.21 9E+01 2 . 233E+0

1

8.090E-01 S. 1 4 1 E + 0 0 -0.008 0.021 0 .004 175.0000 1 . 460E+00 2.436E+01 2 . 582E+0

1

2. 337E+01 3.276E-01 6 . 423E+00 -0.007 0.020 0.003 200.0000 1 . 470 E+00 2.798E+01 2 . 945E+0

1

2 . 428E+0

1

8 . 425E-0

1

6 . 670E+00 -0.006 0.020 0.003 250.0000 1 . 485E+00 3 . 525E+0

1

3.674E+01 2.579E+01 8.651E-01 7 . 088E+00 -0.005 0.018 0.002

300.0000 1 . 498E+00 4 . 254E+0

1

4.404E+01 2 . 704E+0

1

8.814E-01 7 . 433E+00 -0.004 0.018 0.002

350.0000 1 . 508E+00 4. 984E+01 5.1 35E+01 2.809E+01 8. 938E-01 7 . 728E+00 -0.004 0.017 0.002

400.0000 1 . 51 7E+00 5.715E+01 5.866E+01 2. 900E+01 9.036E-01 7 . 984E+00 -0 . 003 0.016 0.002

450 .0000 1 . 525E+00 6 . 446E+0

1

6 . 599E+0

1

2 . 980E+0

1

9.1 16E-01 8.21 2E+00 -0.003 0.016 0.001 500.0000 1 . 532E+00 7.178E+01 7.331E+01 3.052E+01 9. 183E-01 8.416 E+00 -0.003 0.016 0.001 550.0000 1 . 538E+00 7.91 1E+01 8 . 065E+0

1

3. 1 17E+01 9.239E-01 8 . 601 E+00 -0.003 0.015 0.001 600.0000 1 . 544E+00 8 . 645E+0

1

8.799E+01 3. 176E+01 9.287E-01 8 . 770E+00 -0.002 0.015 0.001 700.0000 1 . 554E-*-00 1 .01 1E+02 1 . 027E+02 3.281 E+0

1

9.366E-01 9.071 E+00 -0.002 0.015 0.001 800.0000 1 . 562E+00 1 . 1 58E+02 1 . 1 74E+02 3 . 372E+0

1

9. 427E-01 9 . 333E+00 -0.002 0.014 0.001 900.0000 1 . 570E+00 1 . 305E+02 1 .321E+02 3 . 453E+0

1

9 . 477E-0

1

9 . 564E+00 -0.002 0.014 0.001 1000.0000 1 . 576E+00 1 . 452E+02 1 . 468E+02 3.524E+01 9.518E-01 9 .771 E+00 -0.001 0.014 0.001

102
ELECTRONS IN PLATINUM

I = 790.0 eV DENSITY = 2.145E+01 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DEHS.EFF. d( loc1 ) /d ( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2 /g MeV cm 2/g g/cra 2 0.0100 8 . 646E + 00 2.01 7E-02 8 . 666E+00 7 . 943E-04 1 . 1 44E-03 1 . 0S4E-03 -0 . 373 0.665 0.520 0.0125 7 . 533E+00 2.215E-02 7 . 560E + 00 1 . 1 04E-03 1 . 441 E-03 1 . 393E-03 -0.345 0.579 0.460 0.0150 5 . 71 7E+00 2.377E-02 6 .741 E+00 1 .455E-03 1 . 739E-03 1 .717E-03 -0 . 325 0.520 0.421 0.0175 6 . 083E+00 2.515E-02 6 . 1 08E+00 1 . 845E-03 2.037E-03 2 . 059E-03 -0.310 0.476 0.393

0.0200 5 . 577E+00 2.635E-02 5 . 603E+00 2 . 273E-03 2 . 334E-03 2.413E-03 -0.297 0.444 0.371 0.0250 4.81 6E+00 2 . 833E-02 4 . 845E + 00 3.236E-03 2. 923E-03 3 . 1 90 E-0 3 -0.279 0.397 0 .340 0.0300 4.270E+00 3.005E-02 4 . 30 0E+0 0 4.334E-03 3.507E-03 4 . 039E-03 -0.266 0.365 0.319 0.0350 3 . 857E+00 3. 149E-02 3 . 889E+00 5.559E-03 4.084E-03 4. 967E-03 -0.256 0.341 0.303

0 . 0400 3 . 533E+00 3 . 277E-02 3 . 566E+00 6 . 904E-03 4 . 654E-03 5 . 979E-03 -0 . 247 0.323 0.290 0.0450 3 . 272E+00 3.392E-02 3 . 306E+00 8. 361 E-03 5.218E-03 7 . 076E-03 -0 .240 0.309 0.230 0.0500 3 . 056E+00 3 . 497E-02 3 . 091 E+00 9 . 927E-03 5.775E-03 8.259E-03 -0.234 0.297 0.272

0.0550 2 . 875E+00 3.595E-02 2.911 E+00 1 . 160E-02 6 . 326E-03 9 . 528 E-0 3 -0.229 0.287 0.264

0.0600 2 . 720E+00 3.687E-02 2 . 757E+00 1 . 336E-02 6 .870E-03 1 . 088E-02 -0.224 0.279 0.258

0.0700 2.471E+00 3.856E-02 2.509E+00 1 . 7 1 7E-02 7.943E-03 1 . 382E-02 -0.216 0 . 265 0.247

0.0800 2 . 277E+00 4.008E-02 2.31 7E+00 2.132E-02 8 . 992E-03 1 . 702E-02 -0.210 0.254 0.239

0.0900 2. 123E+00 4. 149E-02 2 . 1 65E+00 2. 579E-02 1 . 002E-02 2.043E-02 -0.204 0.246 0.232

0.1000 1 . 998E+00 4 . 279E-02 2.040E+00 3.055E-02 1 . 1 02E-02 2.399E-02 -0.200 0.238 0.225

0.1250 1 . 766E+00 4.575E-02 1.811 E+00 4 . 360E-02 1 . 345E-02 3 . 320E-02 -0.190 0 . 224 0.213 0.1500 1 . 607E+00 4.836E-02 1 . 656E+00 5 . 807E-02 1 . 575E-02 4 . 250 E-0 2 -0.183 0.213 0.204

0.1750 1 . 493E + 00 5.075E-02 1 . 543E+00 7.374E-02 1 . 7 94E-02 5. 1 7 0 E-0 2 -0.177 0.205 0.197 0.2000 1 . 406E+00 5. 300E-02 1 . 459E+00 9 . 042E-02 2 . 002E-02 6 . 076E-02 -0.173 0.193 0.191

0 . 2500 1 . 286E+00 5.727E-02 1 . 343E+00 1 .262E-01 2.393E-02 7.850E-02 -0.165 0.188 0.181

0 .3000 1 . 207E+00 6 . 1 41 E-02 1 . 268E+00 1 . 646E-01 2 . 753E-02 9.536E-02 -0.159 0.130 0.174

0.3500 1 . 1 53E+00 6 . 552E-02 1 . 21 8E+00 2.049E-01 3 . 0 90E-02 1 . 1 30E-01 -0.153 0.174 0.168 0.4000 1.11 4E+00 6 . 965E-02 1 . 183E+00 2.466E-01 3 . 408E-0 2 1 . 30 0 E-0

1

-0.149 0.169 0.162

0.4500 1 . 085E+00 7 . 381 E-02 1 . 1 59E+00 2.893E-01 3.71 IE-02 1 . 468E-0

1

-0.145 0.164 0.158

0.5000 1 . 063E+00 7 . 803E-02 1 . 1 42E+00 3. 328E-01 4 . 000E-O2 1 . 6 36 E-0 1 -0.141 0.160 0.154 0.5500 1 . 047E+00 8.230E-02 1 . 129E+00 3.768E-01 4.278E-02 1 .803E-01 -0.137 0.156 0.150 0.6000 1 . 035E+00 8 . 662E-02 1.121 E+00 4.21 3E-01 4.547E-02 1 . 971 E-01 -0.134 0.153 0.147

0.7000 1 .017E+00 9 . 538E-02 1.11 3E+00 5. 109E-01 5.062E-02 2. 304E-01 -0.128 0.147 0.141 0.8000 1 . 008E+00 1 .C43E-01 1 . 1 12E+00 6 . 008E-0

1

5 . 552E-02 2.637E-01 -0.123 0.142 0.135

0 . 9000 1 . 002E+00 1 . 1 34E-01 1 . 1 15E+00 6 . 9O6E-01 6.021 E-02 2. 970E-01 -0.118 0.138 0.131

1 .0000 9. 995E-01 1 . 226E-0

1

1 . 1 22E+00 7.800E-01 6 . 474E-02 3.300E-01 -0.114 0.134 0.126

1 .2500 1 . OOOE+OO 1 . 465E-0

1

J . 147E+00 1 .001 E+00 7.551E-02 4.11 6E-01 -0.105 0.126 0.117

1 .5000 1 . 007E+00 1.71 IE-01 1 . 1 78E+00 1 . 2 1 6 E+0 0 8.568E-02 4. 907E-01 -0.093 0.119 0.109

1 .7500 1 . 0 1 5E+00 1 . 964E-01 1 .21 1 E+00 1 . 425E + 00 9.541 E-02 5.668E-01 -0.093 0.113 0.103

2.0000 1 . 024E+00 2 . 223E-0

1

1 . 246E+00 1 . 629E+00 1 . 048E-0

1

6 . 395E-0

1

-0.088 0.109 0.097 2.5000 1 . 042E+00 2.754E-01 1 .317E+00 2.01 9E+00 1 .226E-01 7 . 75 1 E-0

1

-0.081 0.101 0.083

3.0000 1 . 059E+00 3.299E-01 1 . 389E+00 2 . 389E+00 1 . 394E-01 8. 987E-01 -0 .076 0.095 0.081 3.5000 1 . 074E+00 3.857E-01 1 . 460E+00 2 . 740E+00 1 . 554E-0

1

1 .01 2E+00 -0.072 0.090 0.075

4.0000 1 . 088E+00 4 . 425E-0

1

1 .531 E+00 3.074E+00 1 . 705E-0

1

1 . 1 1 7E+00 -0.068 0.085 0.070 4.5000 1 . 101E+00 5.001 E-01 1 .601 E+00 3 . 393E+00 1 .850E-01 1 . 21 4E+00 -0.065 0 . 082 0.066 5.0000 1.11 2E+00 5.586E-01 1 .671E+00 3. 699E+00 1 . 989E-01 1 . 305E+00 -0.063 0.079 0.062 5.5000 1 . 123E+00 6. 177E-01 1 . 7 40E+00 3. 992E+00 2.121 E-0

1

1 . 391 E+00 -0.060 0.076 0.059

6 .0000 1 . 1 32E+00 6.774E-01 1 .81 0E+00 4 . 274E+00 2.248E-01 1 . 472E+00 -0.053 0.073 0.056 7.0000 1 . 1 50E+00 7.985E-01 1 . 948E+00 4 . 806E+00 2 . 488E-0

1

1 . 622E + 00 -0.055 0.069 0.051 8.0000 1 . 1 64E+00 9.215E-01 2 . 086 E+00 5 . 302E+00 2.710E-01 1 . 7 5 9E + 00 -0 .052 0.065 0.047

9.0000 1 . 177E+00 1 . 046E+00 2 . 224E+00 5 . 767E+00 2.916 E-0

1

1 . 884E+00 -0.049 0.062 0.044

1 0 .0000 1 . 189E+00 1 . 172E+00 2.361E+00 6 . 203E+00 3. 108E-01 2. OOOE+OO -0.047 0.060 0.041 12.5000 1 .21 3E+00 1 . 493E+00 2 . 706E+00 7.1 9 1 E+00 3.536E-01 2 . 256E+00 -0.043 0.054 0.035

15.0000 1 . 232E+00 1.81 9E+00 3.051 E+00 8.061 E+00 3. 905E-01 2 . 477E+0 0 -0 .040 0.051 0.031 17.5000 1 . 248E+00 2. 1 51 E+00 3 . 399E+00 8.837E+00 4.226E-01 2.671 E+00 -0.037 0 .047 0.027

20 .0000 1 . 262E+00 2 . 486E+00 3 . 748E+00 9 . 537E+00 4 . 508E-0

1

2 . 845E+00 -0.034 0.045 0.025 25.0000 1 . 284E+00 3 . 1 67E+00 4.451E+00 1 .0 76 E+0

1

4.984E-01 3. 148E+00 -0.031 0.041 0.021 30.0000 1 .301E+00 3 . 358E+00 5 . 1 60E+00 1 . 1 80 E+0

1

5.371 E-0

1

3 . 407E+00 -0.027 0.038 0.018

35.0000 1 . 31 6E+00 4 . 557E+00 5 . 873E+00 1 . 27 1 E+0

1

5.692E-01 3 . 634E+00 -0.025 0.036 0.016 40.0000 1 . 328E+00 5 . 263E+00 6 . 590E+00 1 . 351 E+0

1

5. 965E-01 3 . 837E + 00 -0.023 0.034 0.014 45.0000 1 . 338E+00 5. 973E+00 7.31 2E+00 1 . 423E+0

1

6.200 E-0

1

4 . 020E+00 -0.021 0.032 0.012 50.0000 1 . 347E+00 6 . 689E+00 8 . 036E+00 1 . 489E+0

1

6 .405E-01 4. 187E+00 -0.019 0.031 0.011 55.0000 1 . 355E+00 7 . 408E+00 8 . 763E+00 1 . 548E+0

1

6 . 586E-01 4.341 E+00 -0.013 0.030 0.010 60.0000 1 . 363E+00 8. 1 30E+00 9 . 493E+00 1 . 603E+0

1

6.746E-01 4 . 483E+00 -0.017 0.029 0.010 70.0000 1 . 375E+00 9. 583E+00 1 . 0 96E + 0

1

1 .701 E+01 7.01 9E-01 4 . 740 E+00 -0.015 0.023 0.008

80 .0000 1 . 386E+00 1 . 1 04E+01 1 . 243E+01 1 . 787E+0

1

7 . 244E-0

1

4 . 966E+00 -0.014 0.026 0.007

90.0000 1 . 395E+00 1 .251E+01 1 .391E+01 1 .863E+01 7.433E-01 5.16 9E+00 -0.013 0.025 0.007

100.0000 1 . 403E+00 1 . 399E+01 1 .539E+01 1 .931 E+0

1

7 . 594 E-0

1

5. 352E+00 -0.012 0.024 0.006 125.0000 1 . 420E+00 1 .769E+01 1.911 E+0

1

2 . 076E+0

1

7.91 IE-01 5 . 747E+00 -0.010 0.023 0.005

150.0000 1 . 433E+00 2. 141E+01 2 . 285E+0

1

2.1 96 E+0

1

8. 145E-01 6.076 E+0 0 -0.008 0.022 0.004

175.0000 1 . 444E+0 0 2.515E+01 2.659E+01 2 . 297 E + 0

1

3.327E-01 6 . 357E+00 -0.007 0.021 0.003 200.0000 1 . 454E+00 2.889E+01 3.035E+01 2 . 385E+0

I

8.472E-01 6 . 604E+00 -0.006 0.020 0.003 250.0000 1 . 46 9E+00 3 . 640E+0

1

3 . 787E+0

1

2 . 532E+0

1

8.692E-01 7 . 022E+00 -0.005 0.019 0.002 300.0000 1 . 482E + 0 0 4.393E+01 4 . 54 1 E+0

1

2 . 653E+0

1

8.851 E-0

1

7 . 367E+00 -0 .004 0.018 0 .002 350.0000 1 . 4 92E+00 5. 146E+01 5.295E+01 2.755E+01 S.972E-01 7 . 662E+00 -0.004 0.017 0.002 400.0000 1 .501E+00 5.901E+01 6 .051 E+01 2 . 843E+0

1

9 . 067E-01 7.918E+00 -0.003 0.017 0.002 450.0000 1 . 50 9E+00 6 . 656E+01 6 . 807E+0

1

2 . 92 1 E+0

1

9. 145E-01 8. 1 45E+00 -0.003 0.016 0.001 500.0000 1 . 51 5E+00 7 . 41 2E+01 7 . 563E+01 2 . 990E+0

1

9.209E-01 8.349E+00 -0.003 0.016 0.001 550.0000 1 . 522E+00 3. 168E+01 8 . 320E+0

1

3.053E+01 9.264E-01 8 . 534E + 00 -0.003 0.016 0.001 600.0000 1 . 527E+00 3. 925E+01 9.078E+01 3. 1 1 1 E+01 9 . 3 1 0 E-0

1

8 . 704E+00 -0.002 0.015 0.001

700 . 0000 1 . 5 37E + 0 0 1 . 044E+02 1 . 059E+02 3.21 3E+01 9.387E-01 9 . 005E+00 -0.002 0.015 0.001 800.0000 1 . 546E+00 1 . 1 96E+02 1.211 E+02 3.301 E+0

1

9 . 446 E-0

1

9.266 E+00 -0.002 0.014 0.001 900.0000 1 . 553E+00 1 . 347E+02 1 . 363E+02 3.379E+01 9.494E-01 9 . 4 97E + 00 -0.002 0.014 0.001 1000.0000 1 . 560E+00 1 . 499E+02 1 .51 5E+02 3 . 448E+0

1

9.534E-01 9 . 705E+00 -0.001 0.014 0.001

103
ELECTRONS IN GOLD

I = 790.0 eV DENSITY = 1 . 932E+01 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d ( log1 )/d( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2/g MeV cm 2 /g g/cn 2 0.0100 8.673E+00 2 . 036E-02 8 . 6 94E+00 7.917E-04 1 . 150E-03 6 . 025E-04 -0.373 0.665 0.519

0.0125 7.562E+00 2.237E-02 7 . 585E+00 1 .101E-03 1 . 449E-03 7 .709E-04 -0.345 0.579 0.460 0.0150 6 . 739E+00 2.402E-02 6 . 763E+00 1 . 450E-03 1 .749E-03 9 . 470E-04 -0 . 325 0.520 0.421 0.0175 6 . 1 03E+00 2.543E-02 6 . 1 28E+00 1 .839E-03 2 . 050E-03 1 . 1 31 E — 03 -0.310 0.476 0.392

0.0200 5 . 595E+00 2 . 666E-02 5 . 622E+00 2.266E-03 2.349E-03 1 . 323E-03 -0.298 0.444 0.371 0.0250 4 . 832E+00 2.872E-02 4.361 E+00 3.226E-03 2.945E-03 1 . 735E-0 3 -0.279 0.397 0 . 340 0.0300 4 . 284E+00 3 . 043E-02 4 . 31 5E+00 4 . 320E-03 3.534E-03 2. 183E-03 -0.266 0.365 0.319

0.0350 3 . 870E+00 3.1 90E-02 3 . 902E+00 5.541E-03 4 . 1 1 7E-03 2.673E-03 -0.256 0.341 0.303

0 .0400 3.545E+00 3.321E-02 3.579E+00 6 . 880E-03 4.694E-03 3.208E-03 -0.243 0.324 0.291 0.0450 3 . 283E+00 3.439E-02 3. 318E+00 8.333E-03 5.264E-03 3.791E-03 -0.241 0.309 0.280

0.0500 3.067E+00 3.547E-02 3.102E+00 9.393E-03 5.828E-03 4 . 427E-0 3 -0.235 0.298 0 . 272 0.0550 2 . 885E+00 3.647E-02 2. 922E+00 1 . 155E-02 6 . 385E-03 5.121E-03 -0.230 0.288 0.265

0.0600 2 . 730E+00 3.741E-02 2 . 768E+00 1 . 331 E-02 6 . 936E-03 5 . 877E-03 -0.225 0.279 0.258

0.0700 2 . 480E+00 3.914E-02 2.51 9E+00 1 .71 IE-02 8.022E-03 7.597E-03 -0.217 0.266 0.248

0.0800 2 . 286E+00 4.070E-0

2

2 . 327E+00 2. 124E-02 9 . 084E-03 9 . 624E-03 -0.211 0.255 0.239

0.0900 2. 132E+00 4.214E-02 2. 1 74E+00 2.569E-02 1 .012E-02 1 . 1 99E-02 -0.205 0.246 0.232

0.1000 2 . 006E + 00 4.348E-02 2 . 049E+00 3 . 044E-02 1 .114E-02 1 . 471 E-02 -0.200 0.239 0.226

0. 1250 1 . 773E+00 4.651 E-02 1 .81 9E+00 4.343E-02 1 . 360E-02 2.28SE-02 -0.189 0.224 0.213

0.1500 1 . 6 1 4E+00 4.920E-02 1 . 6 6 3E+0 0 5 . 784E-02 1 . 593E-02 3 . 23 1 E-02 -0.181 0.213 0.203

0.1750 1 . 499E+00 5. 164E-02 1 . 550E+00 7 . 343E-02 1 .815E-02 4.212E-02 -0.174 0.204 0.196

0.2000 1 . 41 2E+00 5 . 395E-02 1 . 466E+00 9.004E-02 2 . 027E-02 5.187E-02 -0.169 0.197 0.189

0.2500 1 .291E+00 5.833E-02 1 . 349E+00 1 . 257E-0

1

2 . 423E-0 2 7 . 074E-02 -0.161 0.186 0.179

0.3000 1 .212E+00 6 . 256E-02 1 . 274E+00 1 .639E-01 2 . 7S9E-0 2 8 . 883E-02 -0.155 0.178 0.171 0.3500 1 . 1 57E+00 6 . 677E-02 1 . 224E+00 2.040E-01 3.1 32E-02 1 .063E-01 -0.150 0.171 0.165

0.4000 1 . 1 18E+00 7 . 099E-02 1 . 1 89E+00 2 . 455E-0

1

3.455E-02 1 .234E-01 -0.145 0.166 0.160

0.4500 1 . 089E+00 7.524E-02 1 . 164E+00 2.880E-01 3 . 762E-02 1 .401E-01 -0.142 0.161 0.155

0.5000 1 . 067E+00 7 . 954E-02 1 . 1 47E+00 3.313E-01 4 . 056E-02 1 . 566E-0

1

-0.138 0.157 0.151 0.5500 1 .051E+00 8.389E-02 1 . 1 35E+00 3.751E-01 4.338E-02 1 . 729E-0

1

-0.135 0.154 0.147

0.6000 1 . 038E+00 8.828E-02 1 . 1 27E+00 4.1 94E-01 4.612E-02 1 .891 E-01 -0.132 0.150 0.144

0.7000 1 .021 E+00 9.720E-02 1.11 9E+00 5.085E-01 5. 134E-02 2.209E-01 -0.126 0.145 0.138

0.8000 1 .011 E+00 1 . 063E-0

1

1 . 1 18E+00 5. 980E-01 5.630E-02 2.524E-01 -0.122 0.140 0.133

0 . 9000 1 . 006E+00 1 . 1 55E-0

1

1 . 122E+00 6 . 873E-0

1

6.105E-02 2 . 335E-0

1

-0.117 0.136 0.128

1 .0000 1 . 004E+00 1 . 249E-0

1

1 . 1 29E+00 7 . 762E-0

1

6 . 563E-02 3.143E-01 -0.113 0.132 0.124

1 .2500 1 . 0 05E + 00 1 .491E-01 1 . 1 54E+00 9 . 954E-0

1

7.651 E-02 3. 903E-01 -0.105 0.124 0.115

1 .5000 1 .01 1 E+00 1 .741E-01 1 . 186E+00 1 . 20 9E+00 8.673E-02 4 .643E-01 -0.098 0.118 9.108

1 .7500 1 . 020E+00 1 . 998E-01 1 . 220E+00 1 . 41 7E+00 9 . 658E-02 5.361 E-0

1

-0.092 0.112 0.101 2.0000 1 . 029E+00 2.260E-01 1 . 255E+00 1 .61 9E+00 1 .060E-01 6.052E-01 -0.088 0.107 0.096

2.5000 1 . 048E+00 2.799E-01 1 . 327E+00 2 . 006E+00 1 . 239E-0

1

7.354E-01 -0.081 0.100 0.087

3.0000 1 . 065E+00 3.352E-01 1 . 400E+00 2 . 373E+00 1 . 408E-0

1

8 . 55 1 E-0

1

-0.075 0.094 0.080 3.5000 1 . 080E+00 3. 917E-01 1 . 472E+00 2.721 E+00 1 . 568E-0

1

9.655E-01 -0.071 0.089 0.074

4.0000 1 . 095E+00 4.492E-01 1 . 544E+00 3 . 053E+00 1 .721E-01 1 . 068E+00 -0.067 0 .084 0.069

4.5000 1 . 107E+00 5.077E-01 1 . 6 1 5E+00 3.370 E+00 1 .866E-01 1 . 1 63E+00 -0.064 0.081 0.065

5.0000 1.11 9E+00 5.668E-01 1 . 686E+00 3 . 673E+00 2.005E-01 1 . 253E+00 -0.062 0.078 0.061 5.5000 1 . 1 30E+00 6 .267E-01 1 . 756E+00 3. 963E+00 2.1 38E-01 1 . 337E+00 -0.059 0.075 0 . 058 6.0000 1 . 1 39E+00 6.872E-01 1 . 827E+00 4 . 242E+00 2.265E-01 1 .417E+00 -0.057 0.072 0.055

7.0000 1 . 1 57E+00 8.098E-01 1 . 967E+00 4 . 770E+00 2.505E-01 1 . 565E+00 -0.054 0.068 0.050 3.0000 1 . 1 72E+00 9. 343E-01 2. 106E+00 5.261 E+00 2.727E-01 1 . 699E+00 -0.051 0.065 0.046

9.0000 1 . 185E+00 1 .061 E+00 2 . 245E+00 5.721 E+00 2.933E-01 1 . 823E+00 -0.048 0.062 0.043

10.0000 1 . 1 96E+00 1 . 188E+00 2. 385E+00 6 . 1 53E+00 3.125E-01 1 . 937E+00 -0.046 0.059 0.040

12.5000 1 .221 E+00 1 .51 3E+00 2 . 733E+00 7 . 1 32E+00 3 . 554E-0

1

2.1 91 E+00 -0.042 0.054 0.034

15.0000 1 . 240 E+0 0 1 .843E+00 3 . 083E+00 7 . 992E+00 3. 922E-01 2 . 409E+00 -0.039 0.050 0.030

17.5000 1 . 256E+00 2. 179E+00 3 . 435E+00 8 . 760E+00 4.243E-01 2 . 602E+00 -0.036 0.047 0.027

20.0000 1 . 270E+00 2.51 8E+00 3 . 788E+00 9 . 453E+00 4 . 525E-0

1

2 . 775E+00 -0 .034 0.044 0 .024 25.0000 1 . 292E+00 3 . 207E+00 4 . 500E+00 1 . 066E+0

1

5.000E-01 3 . 075E+00 -0.030 0.040 0.020

30.0000 1 .31 0E+00 3. 907E+00 5.217E+00 1 . 169E+01 5.386E-01 3.331 E+00 -0.027 0.037 0.018 35.0000 1 . 325E+00 4.61 5E+00 5 . 939E+00 1 . 259E+0

1

5.707E-01 3 . 556E+00 -0.025 0.035 0.015

40.0000 1 . 337E+00 5 . 329E+00 6 . 666E+00 1 .339E+01 5. 979E-01 3 . 757E+00 -0.022 0.033 0.014

45.0000 1 . 347E+00 6 . 049E+00 7 . 396E+00 1 .410E+01 6 . 21 4E-01 3. 939E+00 -0.021 0.032 0.012

50.0000 1 . 356E+00 6 . 772E+00 8. 129E+00 1 . 474E+0

1

6.418E-01 4 . 1 05E+00 -0.019 0.031 0.011 55.0000 1 . 365E+00 7 . 500E+00 8.865E+00 1 . 533E+0

1

6.598E-01 4 . 257 E+0 0 -0.018 0.030 0.010 60.0000 1 . 372E+00 8 . 232E+00 9 . 604E+00 1 . 587E+0

1

6 . 758E-0

1

4 . 399E+00 -0.017 0.029 0.009

70.0000 1 . 385E+00 9. 702E+00 1 . 109E+01 1 . 684E+01 7.031E-01 4 . 653E+00 -0.015 0.027 0.008

80 . 0000 1 . 395E+00 1 . 1 13E+01 1 . 258E+0

1

1 .769E+01 7.255E-01 4 . 878E+00 -0.014 0.026 0.007

90.0000 1 . 405E+00 1 . 267E+0

1

1 . 407E+0

1

1 . 844E+0

1

7.443E-01 5 . 080E+00 -0.013 0.025 0.006 100.0000 1 . 4 1 3E+00 1 .416E+01 1 . 557E+0

1

1 . 91 1E+01 7.603E-01 5 . 262E+00 -0.012 0.024 0 .006 125.0000 1 . 430E+C0 1 .791 E+01 1 . 934E+01 2 . 055E+0

1

7 . 91 9E-01 5 . 656E+00 -0.010 0.023 0.005

150.0000 1 . 443E+00 2.168E+01 2.312E+01 2. 173E+01 8. 153E-01 5 . 983E+00 -0.008 0.021 0 . 004 175.0000 1 . 455E+00 2.546E+01 2.692E+01 2 . 273E+0

1

8 . 334E-0

1

6 . 264E+00 -0.007 0.020 0 . 003 200.0000 1 . 464E+00 2. 925E+01 3 . 072E+0

1

2 . 360 E + 0

1

8.479E-01 6.51 OE+OO -0.007 0.020 0.003

250.0000 1 . 480E+00 3 . 685E+0

1

3.833E+01 2 . 506 E + 0

1

8.697E-01 6 . 926E+00 -0.005 0.019 0.002

300.0000 1 . 492E+00 4 . 447E+0

1

4.596E+01 2. 625E+01 8 . 856E-0

1

7.271 E+00 -0.004 0.018 0.002

350.0000 1 . 503E+00 5.21 0E+0

1

5 . 360E+0

1

2 . 725E+0

1

8. 976E-01 7 . 564E+0 0 -0.004 0.017 0.002 400.0000 1 .51 1E+00 5. 974E+01 6. 125E+01 2.812E+01 9.071E-01 7 . 820E+00 -0.003 0.017 0.002 450.0000 1 .51 9E+00 6 . 739E+0

1

6.891 E+0

1

2.889E+01 9.148E-01 8 . 047E+00 -0.003 0.016 0.001 500.0000 1 . 526E+00 7 . 504E+0

1

7.656E+01 2 . 958E+0

1

9.213E-01 8.251 E+00 -0.003 0.016 0.001 550.0000 1 . 532E+00 8 . 270E+0

1

8 . 423E+0

1

3 . 020E+0

1

9.267E-01 8 . 436E+00 -0.003 0.015 0.001 600.0000 1 . 538E+00 9 . 036E+0

1

9 . 1 90E+01 3 . 077E+0

1

9. 31 3E-01 8 . 605E+00 -0 .002 0.015 0.001 700.0000 1 . 548E+00 1 . 057E+02 1 . 072E+02 3. 178E+01 9. 389E-01 8 . 905E+00 -0 .002 0.015 0.001 800.0000 1 . 557E+00 1 . 21 0E+02 1 . 226E+02 3 . 265E+0

1

9.449E-01 9 . 1 67E+00 -0.002 0.014 0.001 900.0000 1 . 564E+00 1 . 364E+02 1 . 380E+02 3.342E+01 9.497E-01 9 . 393E+00 -0 . 002 0.014 0.001

1000 ,0000 1 .571 E+00 1 . 51 8E+02 1 . 533E+02 3.410E+01 9.536E-01 9 . 605E+00 -0.001 0.014 0.001

104
ELECTRONS IN LEAD

I = 323.0 eV DENSITY =1.1 35E+01 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS . EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD COP.R

.

COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cra 2 /g MeV cra 2 /g MeV cm 2 /g g/cm 2 0.0100 8 . 428E+00 2 . 045E-02 8 . 448E+00 8 . 253E-04 1 . 1 91 E-03 4 .841 E-04 -0.379 0.713 0.539 0.0125 7 . 357E+00 2.251E-02 7.379E+00 1 . 1 43E-03 1 .500E-03 6 . 1 47E-04 -0.350 0.615 0.475

0.0150 6.561E+00 2.421E-02 6 . 585E+00 1 . 502E-03 1 .81 0E-03 7 . 491 E-04 -0.329 0.549 0.432 0.0175 5 . 946E+00 2.566E-02 5. 971 E+00 1 .901E-03 2.121 E— 0 3 8.872E-04 -0.314 0.501 0.402 0.0200 5 . 453E+00 2.693E-02 5 . 480E+00 2.339E-03 2 . 432E-03 1 . 029E-03 -0.301 0.464 0.379

0.0250 4.71 4E+00 2. 908E-02 4 . 7 43E+00 3 . 323E-03 3.051E-03 1 . 324E-03 -0 . 283 0.413 0 . 347 0.0300 4 . 1 82E+00 3.086E-02 4.213E+00 4.444E-03 3.664E-03 1 .633E-03 -0.269 0 . 378 0 . 324 0.0350 3.779E+00 3.240E-02 3.81 2E+00 5.694E-03 4.271 E-03 1 . 956E-03 -0.259 0 . 352 0 .308 0.0400 3.463E+00 3 . 376E-02 3 . 497E+00 7.066E-03 4.872E-03 2.294E-03 -0.250 0.333 0.295

0.0450 3 . 208E+00 3 . 500E-02 3 . 243E+00 8.552E-03 5.467E-03 2.646E-03 -0.243 0.317 0 . 284 0.0500 2. 997E+00 3.613E-02 3.034E+00 1 .01 5E-02 6 . 055E-03 3.011 E-03 -0.238 0.305 0.276 0.0550 2.821 E+00 3.718E-02 2 . 858E+00 1 . 1 85E-02 6 .638E-03 3.390E-03 -0.232 0.294 0.268

0.0600 2 . 670E+00 3 .31 7E-02 2 . 7 03E+00 1 . 365E-02 7.214E-03 3 . 783E-03 -0.228 0.285 0.262

0.0700 2.426E+00 3. 998E-02 2 . 46 6 E + 00 1 . 752E-02 8.349E-03 4.608E-03 -0.220 0.271 0.251 0.0800 2 . 237 E+00 4.1 62E-02 2 . 279E+00 2. 175E-02 9.461 E-03 5 . 485E-03 -0.214 0.260 0.242

0.0900 2 . 087E+00 4.313E-02 2.1 30E+00 2.629E-02 1 . 055E-02 6.413E-03 -0.209 0.251 0.235

0.1000 1 . 964E+00 4.454E-02 2 . 008E+00 3.11 3E-02 1 . 1 62E-02 7.392E-03 -0.205 0 . 243 0.229

0.1250 1 . 738E+00 4.772E-02 1 . 785E+00 4.438E-02 1 .41 9E-02 1 . 005E-02 -0.196 0.229 0.217

0.1500 1 . 583E+00 5 . 054E-02 1 . 6 33E+0 0 5. 905E-02 1 . 664E-02 1 . 300E-02 -0.189 0.218 0.208

0.1750 1 . 47 1 E+00 5. 312E-02 1 . 524E+00 7.492E-02 1 . 896E-02 1 . 623E-02 -0.183 0.210 0.201 0.2000 1 . 387E+00 5 . 555E-02 1 . 442E+00 9.180E-02 2. 1 18E-02 1 . 971 E-02 -0.173 0.203 0.195

0.2500 1 .269E+00 6.015E-02 1 . 329E+00 1 . 280E-0

1

2 . 533E-02 2 . 736E-02 -0.170 0.193 0.186 0.3000 1 . 1 93E+00 6.460E-02 1 . 257E+00 1 -668E-01 2.917E-02 3.579E-02 -0.163 0.185 0.178

0.3500 1 . 1 40E+00 6 . 900E-02 1 .209E+00 2.074E-01 3.276E-02 4 . 484E-02 -0.157 0.178 0.172

0.4000 1 . 102E+00 7.340E-02 1 . 175E+00 2.494E-01 3.614E-02 5.437E-02 -0.153 0.173 0.166 0.4500 1 . 074E+00 7.781 E-02 1 . 1 52E+00 2. 924E-01 3 . 935E-02 6.426E-02 -0.148 0.168 0.162

0.5000 1 . 053E+00 8.228E-02 1 . 1 35E+00 3.361 E- 0

1

4.241 E-02 7.442E-02 -0.144 0.164 0.157

0.5500 1 . 037E+00 8.677E-02 1 . 1 24E+00 3.804E-01 4 . 536E-02 8.479E-02 -0.141 0.160 0.154

0.6000 1 . 026E+00 9.1 32E-02 1.11 7E+00 4.250E-01 4.820E-02 9.529E-02 -0.138 0.157 0.150 0.7000 1 . 00 9E + 00 1 . 005E-0

1

1 . 1 10E+00 5.149E-01 5.363E-02 1 . 1 66E-01 -0.132 0.151 0.144

0.8000 1 . 000E+00 1 .098E-01 1 . 1 1 0E+00 6.050E-01 5.877E-02 1 .380E-01 -0.128 0.146 0.139

0.9000 9.957E-01 1 . 1 93E-01 1 . 1 15E+00 6 . 949E-01 6.369E-02 1 . 5 95E-0

1

-0.124 0.142 0.134

1 .0000 9. 939E-01 1 . 290E-0

1

1 . 1 23E+00 7.843E-01 6 . 842E-02 1 .809E-01 -0.120 0.138 0.130

1 .2500 9.966E-01 1 . 537E-0

1

1 . 1 50E+00 1 . 004E+00 7 . 960E-02 2.337E-01 -0.113 0.130 0.121

1 .5000 1 . 004E+00 1 .792E-01 1 . 183E+00 1 .21 9E+00 9.009E-02 2.854E-01 -0.107 0 . 1 24 • 0.114

1 .7500 1 .01 4E+00 2.053E-01 1 .21 9E+00 1 . 427E + 0 0 1 .001E-01 3 . 360E-01 -0.102 0.118 0.108

2.0000 1 . 024E+00 2.319E-01 1 . 256E+00 1 . 629E+00 1 .096E-01 3 . 855E-01 -0.097 0.114 0.103 2.5000 1 . 044E+00 2.866E-01 1 . 331 E+00 2.01 6E+00 1 . 277E-0

1

4.817E-01 -0.089 0.106 0.094

3.0000 1 . 063E+00 3.427E-01 1 . 406E+00 2. 381 E+00 1 . 447E-0

1

5 . 743E-01 -0.083 0.100 0.086

3.5000 1 . 080E+00 3. 999E-01 1 . 480E+00 2 . 728E+00 1 .608E-01 6 .631 E-01 -0.078 0.095 0.080 4.0000 1 . 095E+00 4.582E-01 1 . 553E+00 3 . 057E+00 1 .761E-01 7 . 479E-01 -0 .073 0.091 0.075

4.5000 1 . 1 08E+00 5. 174E-01 1 . 626E+00 3 . 372E+0 0 1 . 906E-01 3.239E-01 -0.070 0.087 0.070 5.0000 1 . 120E+00 5.773E-01 1 . 6 98E+00 3 . 673E+00 2.045E-01 9.061 E— 0

1

-0.067 0.083 0.066 5.5000 1 . 1 32E+00 6.379E-01 1 . 76 9E+00 3. 962E+00 2. 177E-01 9.793E-01 -0.064 0.080 0.063 6.0000 1 . 142E+00 6.991E-01 1 .841 E+00 4 . 239E+00 2 . 304E-0

1

1 . 050E+00 -0.061 0 .078 0.060 7.0000 1 . 1 60E+00 8.233E-01 1 . 983E+00 4 . 7 62E + 00 2.543E-01 1 . 182E+00 -0 .057 0 .073 0.054

8.0000 1 . 175E+00 9.495E-01 2. 125E+00 5 . 249E+00 2 . 765E-0

1

1 . 304E+00 -0.054 0.069 0 .050 9.0000 1 . 189E+00 1 . 077E+00 2 . 266E+00 5 . 705E+00 2. 970E-01 1 .417E+00 -0.051 0 .066 0.046

10.0000 1 . 20 1 E+00 1 . 206E+00 2 . 407E+00 6.133E+00 3. 162E-01 1 . 523E+00 -0.049 0.063 0.043

12.5000 1 . 226E+00 1 . 535E+00 2.761 E+00 7 . 1 02E+00 3.589E-01 1 . 759E+00 -0 .044 0.058 0.037

15.0000 1 . 246E+00 1 . 870 E+0 0 3. 1 1 6E+00 7. 954E+00 3. 955E-01 1 . 964E+00 -0.041 0.053 0.032

17.5000 1 . 262E+00 2 . 2 1 0 E + 0 0 3 . 472E+00 8.71 3E+00 4.274E-01 2 . 1 47E+00 -0.038 0 .050 0.029

20.0000 1 . 277E+00 2 . 554E+00 3 . 830 E+00 9 . 399E+00 4.555E-01 2.31 OE+OO -0.036 0.047 0.026 25.0000 1 . 299E+00 3 . 252E + 0 0 4.551 E+00 1 .059E+01 5.028E-01 2 . 596E+00 -0.032 0 .043 0.022

30.0000 1 . 31 8E+00 3.961 E+00 5 . 278E+00 1 .161E+01 5.412E-01 2.841E+00 -0.029 0.040 0.019 35.0000 1 . 332E+00 4 . 678E+00 6.01 1 E+00 1 . 250E+0

1

5.731E-01 3 . 055E+00 -0.027 0.038 0.016 40.0000 1 . 345E+00 5 . 402E+00 6 . 747E+00 1 . 329E+0

1

6 .002E-01 3 . 247E+00 -0.025 0.036 0.015 45.0000 1 . 356E+00 6 . 1 32E+00 7 . 488E+00 1 . 399E+0

1

6 . 235E-01 3 . 420E + 00 -0.023 0.034 0.013 50.0000 1 . 365E+00 6 . 865E+00 8 . 23 1 E+00 1 . 463E+0

1

6 .439E-01 3 . 579E + 00 -0.021 0.033 0.012 55.0000 1 . 374E+00 7.603E+00 8 . 977E+00 1 .521E+01 6.618E-01 3 . 725E + 00 -0.020 0.032 0.011

60 .0000 1 . 381 E+00 8 . 345E + 0 0 9 . 726E+00 1 . 574E+01 6.777E-01 3 . 36 1 E+00 -0.019 0.031 0.010

70 .0000 1 . 395E+00 9 . 8 36E+0 0 1 . 123E+01 1 . 670E+0

1

7 . 048E-01 4. 107E+00 -0.017 0 .029 0.009 80.0000 1 . 406E+00 1 . 134E+01 1 .274E+01 1 . 753E+0

1

7 . 270E-0

1

4.326E+00 -0.015 0 .028 0 .008 90.0000 1 . 41 5E+00 1 . 284E+0

1

1 . 426E+0

1

1 . 828E+0

1

7.457E-01 4 . 52 1 E+00 -0.014 0.027 0.007 100.0000 1 . 423E+00 1 . 436E+0

1

1 . 578E+0

1

1 . 8 94E+0

1

7.617E-01 4.699E+00 -0.013 0.026 0.006 125.0000 1 .441 E+00 1 .816E+01 1 . 960E+01 2. 036E+01 7.931E-01 5 . 083E+00 -0.011 0.024 0 .005 150.0000 1 . 455E+00 2. 1 98E+01 2. 344E+01 2.1 53E+01 8 . 1 64E-01 5 . 404E+00 -0.010 0.023 0 .004 175.0000 1 . 466E+00 2. 582E+01 2 . 729E+0

1

2.251E+01 8.343E-01 5.67 9E+00 -0.009 0.022 0.004 200.0000 1 .476E+00 2. 966E+01 3. 114E+01 2 . 337E+0

1

8.488E-01 5. 921 E+00 -0.008 0.021 0.003 250.0000 1 .491 E+00 3 . 737E+0

1

3.886E+01 2.480E+01 8.705E-01 6 . 330 E+00 -0.006 0.020 0.003 300.0000 1 . 504E+00 4.509E+01 4.660E+01 2 . 598E+0

1

8.862E-01 6.670E+00 -0.005 0.019 0.002

350 . 0000 1 . 51 4E+00 5 . 283E+0

1

5.435E+01 2. 697E+01 8 . 982E-01 6 . 960E+00 -0.005 0.018 0.002 400.0000 1 . 523E+00 6 . 058E+01 6.210E+01 2 . 783E+0

1

9.077E-01 7.21 3E+00 -0 .004 0.018 0.002 450.0000 1 .531 E+00 6.833E+01 6 . 986E+01 2.859E+01 9.153E-01 7 . 438E+00 -0 .004 0.017 0.001 500.0000 1 . 538E+00 7 . 609E+0

1

7.763E+01 2. 927E+01 9.217E-01 7 . 640E+00 -0.003 0.017 0.001 550.0000 1 . 544E+00 8 . 386E+01 8 . 540E+01 2. 988E+01 9.271E-01 7.824E+00 -0.003 0.017 0.001 600.0000 1 . 550E+00 9. 163E+01 9.318E+01 3.044E+01 9.317E-01 7 . 992E+00 -0.003 0.016 0.001 700.0000 1 . 560E+00 1 . 072E+02 1 . 087E + 0 2 3. 143E+01 9.393E-01 8 . 290E+00 -0.002 0.016 0.001 800.0000 1 . 568E+00 1 . 227E+02 1 . 243E+02 3.229E+01 9.452E-01 8 . 550E+00 -0.002 0.015 0.001 900.0000 1 . 576E+00 1 . 383E+02 1 . 399E+02 3.305E+01 9.500E-01 8 . 780E+00 -0.002 0.015 0.001 1000.0000 1 . 583E+00 1 . 539E+02 1 . 555E+02 3 . 373E+0

1

9.539E-01 8 . 98SE + 00 -0.002 0.015 0.001

105
ELECTRONS IN URANIUM

I = 890.0 eV DENSITY = 1 . 895E+0

1

g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( logI )/d( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 7 . 989E+00 2.101E-02 8 . 005E + 00 8. 979E-09 1 . 292E-0 3 1 .81 0E-03 -0.391 0.898 0.589

0.0125 6 . 986E+00 2 . 327E-02 7.00 9E+00 1 . 233E-03 1 . 628E-03 2.329E-03 -0.360 0.719 0.510 0.0150 6.291 E+00 2.51 6E-02 6 . 266E+00 1.61 IE-03 1 . 968E-03 2.863E-03 -0 .338 0.631 0.959

0.0175 5 . 662E+00 2 . 679E-02 5 . 688E+00 2.030E-03 2.31 0E-03 3.923E-03 -0.321 0.569 0 .929 0.0200 5.1 98E+00 2 . 822E-02 5 . 226E+00 2 . 989E-03 2.653E-03 9.006E-03 -0.308 0.521 0 .397 0.0250 9 . 999E+00 3.0S7E-02 9 . 530E+00 3 . 520E-03 3 . 390E-03 5.231 E-0 3 -0.289 0.955 0.360

0.0300 3. 995E+00 3 . 273E-02 9 . 028E+00 9.699E-03 9.025E-03 6 . 526E-03 -0 . 279 0.911 0 . 335 0.0350 3.61 3E+00 3 . 952E-02 3 . 698E+00 6 . OOOE-03 9.707E-03 7 . 832E-0 3 -0.263 0 . 380 0.317

0.0900 3.31 3E+00 3.612E-02 3 . 399E+00 7 . 933E-03 5.389E-03 9.289E-03 -0 . 259 0 . 356 0.302

0 . 0450 3 . 070E+00 3.756E-02 3. 108E+00 8. 989E-03 6 .056E-03 1 .079E-02 -0.297 0.337 0.291 0.0500 2 . 87 0 E + 0 0 3 . 888E-02 2.909E+00 1 . 065E-02 6 .729E-03 1 . 222E-02 -0.291 0.322 0.281 0.0550 2.701 E+00 9.01 IE-02 2.791E+00 1 .292E-02 7.385E-03 1 . 372E-02 -0.235 0.310 0.273

0.0600 2 . 557E+00 9.127E-02 2.598E+00 1 .929E-02 8.091E-03 1 . 525E-02 -0.231 0.299 0.266

0.0700 2 . 325E+00 9.339E-02 2 . 368E + 0 0 1 . 833E-02 9 . 337E-03 1 . 839E-02 -0.223 0.282 0.255

0.0800 2.1 99E+00 9.531E-02 2.1 90E+00 2 . 273E-02 1 .061E-02 2.1 97E-02 -0.216 0.269 0.296

0.0900 2.001 E+00 9 . 709E-02 2 . 093E+00 2.796E-02 1 . 186E-02 2 . 962E-02 -0.211 0.259 0 . 238 0.1000 1 . 833E+00 9.875E-02 1 . 932E + 0 0 3 . 299E-02 1 . 308E-02 2 . 776E-02 -0.206 0.250 0.232

0.1250 1 . 666E+00 5.299E-02 1 .71 9E+00 9.626E-02 1 . 605E-02 3.560 E-02 -0.196 0.239 0.219

0.1500 1 . 5 1 8E+00 5 . 585E-02 1 . 579E+00 6.199E-02 1 . 888E-02 9 . 336E-02 -0.189 0.222 0.209

0.1750 1 .91 1E+00 5.899E-02 1 . 970E+00 7 . 795E-02 2. 159E-02 5. 103E-02 -0.183 0.213 0.202

0.2000 1 . 330E+00 6 . 189E-02 1 . 3 92E + 00 9 . 599E-02 2.91 7E-02 5 . 860E-02 -0.178 0.206 0.195

0.2500 1 . 21 8E+00 6 .735E-02 1 . 285E+00 1 . 329E-0

1

2. 903E-02 7 . 399E-02 -0.170 0.199 0.185

0.3000 1 . 199E+00 7 . 263E-02 1 .21 7E+00 1 . 730E-0

1

3 . 355E-02 8.799E-02 -0.169 0.186 0.178

0.3500 1 . 0 93E+0 0 7.781E-02 1 . 171E+00 2. 199E-01 3.777E-02 1 . 021 E-0

1

-0.158 0.179 0.171

0 .9000 1 . 057E+00 8.299E-02 1 . 1 90E+00 2.582E-01 9. 175E-02 1 . 1 60E-01 -0.159 0.173 0.165

0.9500 1 .031 E+00 8 . 805E-02 1.11 9E+00 3.025E-01 9 . 553E-02 1 . 296E-0

1

-0.150 0.168 0.161 0.5000 1 .01 1E+00 9.316E-02 1 . 1 09E+00 3.975E-01 9.91 3E-02 1 . 930E-0

1

-0.196 0.169 0.157

0.5500 9. 956E-01 9 . 828E-02 1 . 0 99E+0 0 3.931E-01 5.259E-02 1 . 56 1 E-0

1

-0.193 0.160 0.153

0.6000 9.892E-01 1 .039E-01 1 . 088E+00 9.389E-01 5.591E-02 1 .6 91 E-0

1

-0.190 0.157 0.150

0.7000 9.690E-01 1 .137E-01 1 . 083E+00 5.311 E-01 6 . 223E-02 1 .995E-01 -0.135 0.151 0.199

0.8000 9.609E-01 1 .291E-01 1 . 089E+00 6 . 239E-0

1

6 .817E-02 2.1 92E-01 -0.130 0.196 0.138

0.9000 9.560E-01 1 . 396E-01 1 .091 E+00 7. 159E-01 7 . 382E-02 2 . 939E-0

1

-0.127 0.192 0.139

1 .0000 9.599E-01 1 . 952E-0

1

1 . 1 00E+00 8 . 068E-01 7.921 E-02 2.672E-01 -0.123 0.138 0.130

1 .2500 9.572E-01 1 .721E-01 1 . 129E+00 1 . 031 E+00 9. 189E-02 3.296E-01 -0.116 0.130 0.121

1 .5000 9.699E-01 1 . 995E-0

1

1 . 1 69E+00 1 . 299E+00 1 . 035E-01 3.799E-01 -0.110 0.129 0.119

1 .7500 9.799E-01 2.275E-01 1 . 202E+00 1 .961 E+00 1 .195E-01 9.332E-01 -0.109 0.119 0.108

2.0000 9.899E-01 2.559E-01 1 . 290E+00 1 . 665E+00 1 .299E-01 9.897E-01 -0.100 0.119 0.103

2.5000 1 . 009E+00 3.139E-01 1 . 31 8E+00 2 . 056E+00 1 . 999E-0

1

5.832E-01 -0.092 0.107 0.099

3.0000 1 . 022E+00 3.732E-01 1 . 396E+00 2 . 925E+00 1 . 625E-0

1

6.762E-01 -0.086 0.101 0.087

3.5000 1 . 039E+00 9.338E-01 1 . 973E+00 2 . 779E+00 1 . 795E-0

1

7.695E-01 -0.081 0.096 0.081 9.0000 1 . 059E+00 9. 955E-01 1 .599E+00 3 . 1 05E+00 1 . 955E-01 8.988E-01 -0.076 0.091 0.076 9.5000 1 . 067E+00 5.580E-01 1 . 625E+00 3 . 920E+00 2. 106E-01 9.299E-01 -0.073 0 .087 0.071 5.0000 1 . 079E+00 6 .21 9E-01 1 . 700E+00 3 . 72 1 E+00 2.250E-01 1 . 007E+00 -0.069 0 . 089 0.067

5.5000 1 . 0 90 E+0 0 6.856E-01 1 . 775E+00 9 . 008E+00 2.387E-01 1 . 081 E+00 -0.066 0.081 0.069

6.0000 1 . 1 OOE+OO 7 .509E-01 1 .850E+00 9 . 2S9E+00 2.518E-01 1 . 1 52E+00 -0.063 0.078 0 .060 7.0000 1 . 1 1 7E+00 3.818E-01 1 . 999E+00 9 . 80 9E + 0 0 2 . 769E-01 1 . 287E+00 -0.058 0 . 079 0.055 8.0000 1 . 1 32E+00 1 . 0 1 5E+00 2 . 1 97E+00 5 . 287E+00 2. 990E-01 1 .912E+00 -0.059 0.070 0.050

9.0000 1 . 1 95E+00 1 .151 E+00 2 . 296E+00 5 . 737E+00 3.1 99E-01 1 . 529E+00 -0.051 0.066 0.096

10.0000 1 . 1 57E+00 1 . 288E+00 2 . 999E+00 6 . 1 59E+00 3.399E-01 1 . 639E+00 -0.098 0.063 0.093

12.5000 1 . 1 80E+00 1 . 636E+00 2.81 6E+00 7.111 E+00 3.825E-01 1 . 886E+00 -0.093 0.058 0.036

15.0000 1 . 1 99E+00 1 . 991 E+00 3.191 E+00 7 . 995E+00 9.193E-01 2. 102E + 00 -0.039 0.053 0 .032 17.5000 1 . 21 5E+00 2 . 352E+00 3 . 567E+00 8 . 685E+00 9.51 IE-01 2 . 299E+00 -0.036 0.050 0.028 20.0000 1 . 228E+00 2.71 7E+00 3 . 995E + C 0 9 . 352E + 0 0 9.790E-01 2 . 967E+00 -0 .039 0.097 0.025

25.0000 1 .250E+00 3 . 957E+00 9 . 706E+00 1 .051E+01 5.258E-01 2 . 768E+00 -0.030 0.093 0.021 30.0000 1 . 26 6 E + 00 9 . 208E+00 5 . 979E+00 1 . 1 99E+0

1

5.636E-01 3 . 026E + 00 -0.027 0.090 0.013

35.0000 1 . 280 E + 0 0 9 . 967E+00 6 . 298E+00 1 . 235E+0

1

5.998E-01 3 . 252E+00 -0.029 0.038 0.015

90.0000 1 . 2.92E+00 5 . 733E+00 7 . 025E+00 1 .310E+01 6.212E-01 3 . 953E+00 -0.022 0.036 0.019 95.0000 1 . 302E+00 6 . 505E+00 7 . 807E+00 1 . 378E+01 6.938E-01 3 . 635E+00 -0.021 0 .039 0.012

50.0000 1 .31 1E+00 7 . 282E+00 8 . 593E+00 1 . 939E+0

1

6.635E-01 3 . 802E+00 -0.019 0.033 0.011 55.0000 1 . 31 9E+00 8 . 063E+00 9. 382E+00 1 . 995E+0

1

6 .808E-01 3. 959E+00 -0.018 0.032 0.010 60.0000 1 . 326E+00 8 . 397E+00 1 .017E+01 1 . 596E+0

1

6.961 E-0

1

9 . 0 96 E + 0 0 -0.017 0.031 0.009

70.0000 1 . 33SE+00 1 . 093E+0

1

1 . 176E+01 1 . 6 37E+0

1

7.221E-01 9.351 E+00 -0.015 0.029 0 .008 80.0000 1 . 399E+00 1 .201E+01 1 . 336E+0

1

1 .717E+01 7.935E-01 9 . 577E+00 -0.013 0.028 0.907

90.0000 1 . 357E+00 1 .361E+01 1 . 997E+0

1

1 . 787E+0

1

7.619E-01 9 . 779E+00 -0.012 0.027 0 .006 100.0000 1 . 365E+00 1 .521E+01 1 . 6 58E+0

1

1 .851E+01 7 . 766E-0

1

9 . 962E+00 -0.011 0.026 0.006

1 25.0000 1 . 382E+00 1 . 929E+01 2 . 062E+0

1

1 . 986E+01 8.069E-01 5 . 357E+00 -0.010 0.029 0.905

150.0000 1 . 395E+00 2 . 329E+0

1

2.969E+01 2.096E+01 8.285E-01 5 . 635E X 00 -0.008 0.023 0.009

175.0000 1 . 905E+00 2 . 736E+0

1

2.877E+01 2. 1 90E+01 3.955E-01 5 . 96 6 E+0 0 -0 .007 0.022 0.003 200.0000 1 . 91 9E+00 3. 199E+01 3.286E+01 2.271 E+0

1

8.591 E-0

1

6 .21 3E+00 -0.006 0.021 0.003 250.0000 1 . 929E + 00 3 . 962E+0

1

9.105E+01 2 . 907E+0

1

8.795E-01 6 . 630E+00 -0.005 0 .020 0.092

300.0000 1 . 99 1 E+00 9 . 782E+0

1

9.926E+01 2.513E+01 3. 993E-01 6 . 975E+00 -0.009 0.019 0.002

350.0000 1 . 95 1 E+00 5 . 609E+0

1

5.799E+01 2.612E+01 9.055E-01 7 . 268E+00 -0.009 0.019 0.002 900.0000 1 . 960E+00 6 . 926E+01 6 . 572E+0

1

2.693E+01 9. 199E-01 7 . 525E+00 -0.003 0.018 0.001 950.0000 1 . 967E + 00 7.250E+01 7.397E+01 2.765E+01 9.215E-01 7 . 752E+00 -0.003 0.017 0.001 500.0000 1 . 979E + 00 8 . 079E+0

1

8.221 E+O

1

2.S29E+01 9 . 275E-0

1

7. 956E+00 -0.003 0.017 0.001 550.0000 1 .980E+C0 3.899E+01 9 . 097E+0

1

2 . 887E+0

1

9 . 325E-0

1

8.191 E+00 -0.002 0.017 0.001 600.0000 1 . 986E+00 9 . 729E+0

1

9 . 872E+0

1

2. 990 E + 0

1

9.369E-01 8.31 OE+OO -0.002 0.016 0.001

700 .0000 1 . 995E+00 1 . 1 37E + 02 1 . 1 52E+02 3 . 039E+01 9.939E-01 8.61 1 E+00 -0.002 0.916 0.001 800.0000 1 . 50 3E+00 1 . 30 3E+02 1 . 31 8E+02 3. 1 15E+01 9.999E-01 8 . 87 2E + 0 0 -0.002 0.016 9.001 900.0000 1 .51 1 E+00 1 . 968E+02 1 . 983E+02 3. 186E+01 9.533E-01 9. 103E+00 -0 . 002 0.015 0.001 1000.0000 1 . 51 7E+00 1 . 633E+02 1 . 698E+02 3 . 250E+0

1

9.575E-01 9.31 OE+OO -0.001 0.015 0.001

106
ELECTRONS IN A-150 TISSUE-EQUIVALENT PLASTIC

T = 65.1 eV DENSITY =1.1 27E+0Ci g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD COP.R

.

COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MsV cm 2 /g g/cm 2 0.0100 2 . 294E+01 3 . 1 56E-03 2 . 295E+0

1

2.463E-04 7 . 529E-05 0.0 -0.193 0.220 0.219 0.0125 1 . 927E+01 3.174E-03 1 . 927E+01 3.657E-04 9.048E-05 0.0 -0.186 0.210 0.209

0.0150 1 .671E + 01 3. 188E-03 1 .671E+01 5.054E-04 1 . 050E-04 0 . 0 -0.180 0.202 0.201 0.0175 1 . 482E+0

1

3.1 97E-03 1 . 482E+0

1

6 . 646E-04 1 . 1 91 E-04 0 . 0 -0.175 0.196 0.195

0 .0200 1 . 335E+0

1

3.205E-03 1 . 336E + 01 8.426E-04 1 .327E-04 0 .

0

-0.171 0.191 0.190 0.0250 1 . 124E+01 3.21 9E-03 1 . 124E + 01 1 . 253E-03 1 . 583E-04 0.0 -0.165 0.183 0.183

0.0300 9 . 769E+00 3.232E-03 9 . 772E+00 1 .731E-03 1 .83SE-04 0.0 -0.160 0.178 0.177 0.0350 3.691E+00 3 . 245E-03 8.694E+00 2 . 275E-03 2.079E-04 0.0 -0.156 0.173 0.173

0 .0400 7 .363E+00 3 . 253E-03 7 .866E+00 2 . 880E-03 2.31 IE-04 0.0 -0.153 0.169 0.169

0.0450 7 . 206E+00 3.273E-03 7 .209E+00 3.545E-03 2 . 537 E-04 0 .

0

-0.151 0.166 0.166

0.0500 6.671E+00 3.287E-03 6 . 675E+00 4 . 267E-05 2 . 756 E-04 0 . 0 -0.143 0.163 0.163

0 .0550 6 . 228E+00 3.302E-03 6 . 231 E+00 5.043E-03 2.971 E-04 0 . 0 -0.147 0.161 0.160 0.0600 5 . 853E+00 3.31 9E-03 5 . 857E + 0 0 5.871E-03 3. 180E-04 0 . 0 -0.145 0.159 0.158 0.0700 5 . 256E+00 3.352E-03 5 . 259E+00 7.677E-03 3.586E-04 0.0 -0.142 0.155 0.155

0.0800 4.800E+00 3.388E-03 4.303E+00 9.669E-03 3.977E-04 0 . 0 -0.139 0.152 0.152

0 .0900 4.441E+00 3.427E-03 4 . 444E+00 1 . 184E-02 4 . 356E-04 0.0 -0.137 0.149 0.149

0 . 1000 4.1 50E+00 3.467E-03 4 . 1 53E+00 1 . 41 7E-02 4.723E-04 0.0 -0.135 0.147 0.147

0.1250 3 . 620E+00 3.578E-03 3 . 623E+00 2 . 064E-02 5 . 602E-04 0.0 -0.132 0.143 0.142

0.1500 3 . 262E+00 3.697E-03 3 . 265E+00 2.792E-02 6.436E-04 0 . 0 -0.129 0.139 0.139

0.1750 3 . 005E+00 3.824E-03 3.009E+00 3 . 592E-02 7.234E-04 0.0 -0.126 0.137 0.136 0.2000 2.312E+00 3. 959E-03 2.81 6E+00 4.452E-02 8 . 003E-04 0.0 -0.124 0.134 0.134

0 . 2500 2 . 544E+00 4.247E-03 2 . 548E+00 6.325E-02 9. 476E-04 0.0 -0.121 0.131 0.130 0.3000 2.369E+00 4.563E-03 2 . 373E+00 8 . 362E-02 1 . 089E-03 0.0 -0.118 0.128 0.127 0.3500 2 . 247E+00 4.901E-03 2 . 252E+00 1 . 053E-0

1

1 .226E-03 0.0 -0.106 0.125 0.124

0.4000 2 . 1 56E+00 5.260E-03 2.161 E+00 1 . 280E-0

1

1 .361E-03 2. 969E-02 -0 . 088 0.120 0.118

0.4500 2 . 086E+00 5.639E-03 2.092E+00 1 .51 5E-01 1 . 4 95E-0 3 6 .264E-02 -0.082 0.114 0.111 0.5000 2.033E+00 6.036E-03 2.039E+00 1 .757E-01 1 . 628E-03 9.751 E-02 -0.077 0.109 0.106 0.5500 1 . 991 E+00 6 . 448E-0 3 1 . 997E+00 2.005E-01 1 .761 E-03 1 . 337E-01 -0 .072 0.105 0.101 0.6000 1 . 957E+00 6 .875E-03 1 . 964E+00 2 . 258E-0

1

1 .895E-03 1 . 708E-0

1

-0 .068 0.101 0 .096 0.7000 1 . 908E+00 7 . 768E-0 3 1 . 91 5E+00 2.774E-01 2. 164E-03 2 . 464E-0

1

-0.061 0.094 0 .088 0.8000 1 . 874E+00 8 . 706E-03 1 . 883E+00 3.300E-01 2.436E-03 3 . 223E-0

1

-0.056 0 . 089 0.082

0 . 9000 1 .851 E+00 9 . 687E-03 1 . 860E+00 3 . 835E-0

1

2.71 IE-03 3. 975E-01 -0.052 0 . 084 0.076

1 .0000 1 . 834E+00 1 .071E-02 1 . 845E+00 4.375E-01 2. 990E-03 4.712E-01 -0.049 0.080 0.071

1 .2500 1 . 8 1 2E+00 1 .341E-02 1 . 825E + 0 0 5.739E-01 3 . 706E-03 6.472E-01 -0.043 0.072 0.062

1 .5000 1 . 80 3E+0 0 1 . 630E-0 2 1.81 9E+00 7. 1 1 IE-01 4 . 447E-03 3.100 E-0

1

-0.039 0.066 0 .056

1 .7500 1 . 802E+00 1 .934E-02 1 . 821 E+00 8.485E-01 5.209E-03 9 . 601 E-01 -0.036 0.061 0.051 2.0000 1 . 804E+00 2 . 252E-02 1 . 827 E+0 0 9 . 856E-0

1

5. 992E-03 1 . 099E + 00 -0.034 0 .057 0 .047 2.5000 1 .814E+00 2.920E-02 1 . 843E+00 1 . 258E+00 7.609E-03 1 . 346E+00 -0.031 0.052 0.041 3.0000 1 . 827E + 0 0 3.625E-02 1 . 86 3E + 00 1 . 528E+0 0 9.281 E-03 1 . 56 1 E+00 -0.029 0.048 0.038

3.5000 1 .839E+00 4.358E-02 1 . 883E+00 1 . 7 95E+0 0 1 . 1 00E-02 1 .751 E+00 -0.023 0 .045 0.035

4.0000 1 . 852E+00 5 . 1 1 6E-02 1 . 903E+00 2. 059E+00 1 . 275E-02 1 . 922E+00 -0 .026 0.043 0.033

4.5000 1 . 863E+00 5.896E-02 1 . 922E+00 2 . 320E+00 1 .453E-02 2 . 077E+00 -0.025 0.041 0.031 5.0000 1 . 874E+00 6 .695E-02 1 . 941 E+00 2.579E+00 1 . 633E-02 2.21 8E+00 -0.024 0.039 0.030 5.5000 1 . 884E+00 7.51 IE-02 1 . 959E+00 2 . 836E+0 0 1 .81 6E-02 2. 349E+00 -0.024 0.038 0.029

6.0000 1 . 894E+00 8.341E-02 1 . 977E+00 3 . 0 90 E+0 0 2 . 000E-02 2.47 OE + OO -0.023 0.036 0 .027 7.0000 1.911 E+00 1 . 004E-0

1

2.01 1 E+00 3.591 E+00 2 . 372E-0 2 2 . 6 9 1 E + 0 0 -0.021 0.034 0.026 8.0000 1 . 926E+00 1 . 179E-01 2 . 044E+00 4 . 084E+00 2.748E-02 2.S87E+00 -0.020 0.032 0.024

9.0000 1 . 939E+00 1 . 358E-0

1

2 . 075E+00 4 . 57 0 E+0 0 3. 127E-02 3 . 064E+00 -0.018 0.031 0.023

10.0000 1 . 951 E+00 1 . 540E-0

1

2. 105E+00 5 . 048E+00 3 . 508E-02 3 . 227E+00 -0.017 0.029 0.021 12.5000 1 . 975E+00 2.007E-01 2 . 1 76 E+00 6.21 6E+00 4.461E-02 3 . 582E+00 -0.014 0.027 0.019

1

5

. 0000 1 . 995E+00 2.488E-01 2 . 243E+00 7 . 348E+00 5.411 E-02 3 . 885E+00 -0.011 0 .024 0.016

17.5000 2.01 OE+OO 2.979E-01 2 . 308E+00 8 . 446E+00 6 . 352E-02 4 . 1 50 E+00 -0.010 0.022 0.014 20.0000 2 . 024E+00 3.478E-01 2 . 372E+00 9.51 5E+00 7.282E-02 4. 385E+00 -0.008 0.021 0.013 25.0000 2 . 046E+00 4.496E-01 2 . 495E+00 1 . 1 57E+0

1

9 . 097E-02 4 . 788E+00 -0.006 0.018 0.010 30.0000 2 . 063E+00 5 . 532E-0

1

2.61 6E+00 1 . 353E+0

1

1 . 085E-0

1

5 . 1 26E+00 -0.004 0.016 0.008 35.0000 2 . 077E+00 6.582E-01 2 . 735E+00 1 .540E+01 1 . 253E-0

1

5.41 7E+00 -0.003 0.014 0 .007 40.0000 2 . 08 9E + 0 0 7.643E-01 2 . 854E+00 1 .718E+01 1 .414E-01 5 . 671 E+00 -0.003 0.013 0.006 45.0000 2 . 1 OOE+OO 8.714E-01 2.971E+00 1 .890E+01 1 .569E-01 5 . 897E+00 -0.002 0.012 0.005

50.0000 2. 1 09E+00 9.792E-01 3 . 089E+00 2.055E+01 1 .717E-01 6 . 1 01 E+00 -0.002 0.011 0.004 55.0000 2.11 8E+00 1 . 088E+00 3 . 205E+00 2.214E+01 1 .860E-01 6 . 286E+00 -0.002 0.011 0.004 60.0000 2. 125E+00 1 . 1 97E+00 3 . 322E+00 2 . 367E+0

1

1 . 996E-01 6 . 456E+00 -0.001 0.010 0.003 70.0000 2.1 39E+00 1 . 41 6E+00 3 . 555E+00 2 . 658E+0

1

2.254E-01 6 . 758E+00 -0.001 0.009 0.003 80.0000 2. 1 51 E+00 1 . 638E+00 3 . 788E+00 2.931 E+0

1

2.491E-01 7 . 020E+00 -0.001 0 .008 0 .002 90.0000 2. 1 61 E+00 1 . 86 OE+OO 4.021 E+00 3. 187E+01 2.712E-01 7 . 253E+00 -0.001 0 .008 0.002 100.0000 2. 170E+00 2 . 084E+00 4 . 254E+0 0 3 . 429E+0

1

2. 917E-01 7 . 461 E+00 -0.001 0.007 0.002

125.0000 2. 139E+00 2 . 647E+00 4 . 8 36E+0 0 3. 979E+01 3.373E-01 7. 903E+00 -0.000 0.006 0.001 150.0000 2 . 204E+00 3.21 4E+00 5.41 8E+00 4 . 468E+0

1

3.763E-01 8 . 265E+00 -0.000 0.005 0.001 175.0000 2.218E+00 3 . 784E+00 6 . 002E+00 4 . 906E+0

1

4. 100E-01 8 . 571 E+00 -0 .000 0 .005 0.001 200.0000 2 . 229E+00 4 . 357E+00 6 . 586E+00 5.303E+01 4.396E-01 8 . 837E+00 -0.000 0.005 0.001 250.0000 2 . 248E+00 5 . 508E+00 7 . 756E+00 6 . 002E+0

1

4.891 E-0

1

9 . 28 1 E + 0 0 -0 .000 0 .004 0.001 300.0000 2 . 26 3E+0 0 6 . 665E+00 8 . 928E+00 6 . 603E+0

1

5.291 E-01 9 . 645E+00 -0 .000 0.004 0.000 350.0000 2 . 276E+00 7 .826E+00 1 .010E+01 7. 129E+01 5.623E-01 9. 952E+00 -0.000 0.003 0.000 400.0000 2 . 288E+00 8. 990E+00 1 . 1 28E+0

1

7.597E+01 5. 903E-01 1 . 022E+01 -0.000 0.003 0 .000 450.0000 2 . 298E+0 0 1 .016E+01 1 . 245E+0

1

8.01 9E+01 6 . 143E-01 1 . 045E+0

1

-0.000 0.003 0.000 500.0000 2 . 307E+00 1 -132E+01 1 . 363E+0

1

8 . 402E+0

1

6.352E-01 1 . 066E+01 -0.000 0.003 0.000 550.0000 2.31 5E+00 1 . 249E+0

1

1 .481E+01 8 . 754E+0

1

6 . 536 E-0

1

1 . 085E+0

1

-0.000 0.003 0.000 600.0000 2 . 322E+00 1 . 367E+0

1

1 .599E+01 9 . 079E+01 6.699E-01 1 . 1 03E+01 -0.000 0.003 0 .000 700.0000 2. 335E+00 1 .601 E+01 1 . 8 35E+0

1

9.662E+01 6 . 977 E-0

1

1 . 1 34E+01 -0.000 0.003 0.000 800.0000 2 . 346 E+0 0 1 .836E+0

1

2.071E+01 1 . 0 1 8E+02 7 . 204E-0

1

1 . 1 60E+01 -0.000 0.002 0.000 900.0000 2. 356E+00 2.072E+01 2 . 307E+0

1

1 . 063E+02 7.396E-01 1 . 184E+01 -0.000 0.002 0.000 1000.0000 2 . 365E+00 2 . 307E+0

1

2 . 544E+0

1

1 . 1 04E+02 7.559E-01 1 . 205E+0

1

-0.000 0.002 0 .000

107
ELECTRONS IN ACETYLENE

I = 58.2 eV DENSITY = 1.097E-03 g/cm 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d ( logl )/d( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cra 2 /g MeV cm 2 /g MeV cm 2 /g g/cn 2 0.0100 2 . 296E+0

1

2 . 982E-03 2 . 296E+0

1

2 . 455E-04 7 . 1 43E-05 0.0 -0.189 0.214 0.213

0.0125 1 . 927E+01 2. 992E-03 1 . 927E+0

1

3.649E-04 8 . 568E-05 0.0 -0.182 0.205 0 . 204 0.0150 1 .670E+01 2. 999E-03 1 . 670E + 0

1

5.047E-04 9.932E-05 0.0 -0.176 0.198 0.197

0.0175 1 . 480E+0

1

3 . 004E-03 1 . 480E+0

1

6.641E-04 1 .125E-04 0.0 -0.171 0.192 0.191 0.0200 1 . 333E+0

1

3 . 008E-03 1 . 333E+0

1

8.423E-04 1 . 252E-0 4 0.0 -0.168 0.187 0.187

0.0250 1 . 121E+01 3.017E-03 1 . 1 21 E+01 1 . 253E-0 3 1 . 497E-04 0.0 -0.162 0.180 0.179

0.0300 9.739E+00 3.027E-03 9 . 742E+00 1 . 733E-03 1 .731E-04 0.0 -0.157 0.174 0.174

0.0350 8.661E+00 3.037E-03 8 . 664E+00 2.279E-03 1 . 956E-04 0 .

0

-0.154 0.170 0.169

0.0400 7 . 833E+00 3.043E-03 7 . 836E+00 2.886E-03 2. 174E-04 0.0 -0.151 0.166 0.166

0.0450 7 . 1 76E+00 3.061E-03 7.179E+00 3.554E-03 2. 385E-04 0.0 -0.143 0.163 0.163

0.0500 6 . 642E+00 3 . 074E-03 6 . 645E+00 4.279E-03 2.591E-04 0.0 -0.146 0.160 0.160

0.0550 6 . 1 99E+00 3 . 088E-03 6 . 202E+00 5.058E-03 2 . 792E-04 0.0 -0.144 0.153 0.158

0.0600 5.825E+00 3.103E-03 5 . 829E+0 0 5.890E-03 2. 989E-04 0.0 -0.142 0.156 0.155

0.0700 5 . 229E+00 3. 135E-03 5 . 232E+00 7 . 705E-03 3.371E-04 0.0 -0.140 0.152 0.152

0.0800 4 . 774E+00 3.169E-03 4 . 777E+00 9.708E-03 3.739E-04 0.0 -0.137 0.149 0.149

0.0900 4.41 6E+00 3.206E-03 4.41 9E+00 1 . 1 89E-02 4 . 095E-04 0.0 -0.135 0.147 0.147

0.1000 4 . 1 26E+00 3 . 244E-03 4 . 1 29E+00 1 . 423E-02 4.441E-04 0.0 -0.133 0.145 0.144

0.1250 3.597E+00 3 . 350E-03 3 . 600E+00 2.074E-02 5 . 270E-04 0.0 -0.130 0.141 0.140

0.1500 3.240E+00 3.463E-03 3 . 244E+00 2 . 808E-02 6 . 058E-04 0.0 -0.127 0.137 0.137

0.1750 2. 984E+00 3.584E-03 2 . 988E+0 0 3.612E-02 6.812E-04 0.0 -0.124 0.135 0.134 0.2000 2 . 792E+00 3.71 IE-03 2 . 796E+00 4 . 478E-02 7 . 540E-04 0.0 -0.122 0.132 0.132

0.2500 2 . 525E+00 3.985E-03 2 . 529E+00 6.365E-02 8. 937E-04 0.0 -0.119 0.129 0.128

0.3000 2.351E+00 4 . 284E-03 2 . 355E+00 8.418E-02 1 . 0 28E-0 3 0 .

0

-0.117 0.126 0.125

0.3500 2 . 229E+00 4 . 604E-03 2 . 234E+00 1 . 060E-0

1

1 . 1 58E-03 0.0 -0.114 0.124 0.123

0.4000 2. 142E+00 4.945E-03 2 . 1 47E+00 1 . 289E-01 1 . 286E-0 3 0.0 -0.113 0.122 0.121 0.4500 2 . 076E+00 5.304E-03 2 . 082E+00 1 . 525E-0

1

1 .413E-03 0.0 -0.111 0.120 0.119

0.5000 2 . 027E+00 5.680E-03 2 . 032E+00 1 .769E-01 1 . 539E-0 3 0.0 -0.110 0.119 0.117 0.5500 1 . 988E+00 6.071E-03 1 . 994E+00 2.017E-01 1 . 664E-03 0.0 -0.108 0.118 0.116 0.6000 1 . 958E+00 6.475E-03 1 . 965E+00 2.270E-01 1 . 7 90E-03 0.0 -0.107 0.116 0.115

0.7000 1 . 91 5E+00 7.322E-03 1 . 923E+00 2.785E-01 2.041 E-03 0.0 -0.105 0.114 0.112

0.8000 1 .888E+00 8.212E-03 1 . 897E+0 0 3.309E-01 2 . 295E-03 0.0 -0.103 0.113 0.110 0.9000 1 .871E+00 9. 142E-03 1 . 881 E+00 3.838E-01 2 . 550E-03 0.0 -0.102 0.111 0.109

1 .0000 1 .861E+00 1 .011E-02 1 .871 E+00 4.372E-01 2.808E-03 0.0 -0.100 0.110 0.107

1 .2500 1 . 853E+00 1 . 267E-02 1 .865E+00 5.71 IE-01 3 . 466E-03 0.0 -0.097 0.107 0.104

1 .5000 1 . 857E+00 1 .541E-02 1 . 873E+00 7.049E-01 4. 1 39E-03 0.0 -0.095 0.105 0.101

1 .7500 1 .863E+00 1 . 830E-02 1 .886E+00 8.380E-01 4 . 829E-03 0.0 -0.093 0.103 0.099

2.0000 1 .881E+00 2.1 32E-02 1 . 902E+00 9.699E-01 5 . 532E-03 0.0 -0.092 0.102 0.097

2.5000 1 . 91 OE+OO 2.766E-02 1 . 938E+00 1 . 230 E + 00 6 . 973E-03 0.0 -0.089 0.099 0.094

3.0000 1 . 939E+00 3 . 435E-02 1 . 974E+00 1 . 486E+00 8.450E-03 0.0 -0 . 087 0.097 0.092

3.5000 1 . 967E+00 4.1 32E-02 2 . 008E+00 1 . 737E+00 9. 955E-03 0.0 -0.085 0.095 0.090 4.0000 1 . 993E+00 4 . 852E-02 2.041 E+00 1 . 984E+00 1 . T48E-02 0.0 -0.084 0.094 0.088

4.5000 2.01 7E+00 5 . 593E-02 2 . 073E+00 2 . 227E+00 1 . 303E-02 0.0 -0.083 0.092 0.087

5.0000 2 . 039E+00 6 . 353E-02 2. 102E+00 2 . 467E+00 1 . 458E-0 2 0.0 -0.082 0.091 0.085

5.5000 2.059E+00 7.1 29E-02 2 . 1 3 1 E+00 2 . 703E+00 1 .615E-02 0.0 -0.081 0.090 0.084

6.0000 2 . 078E+00 7.91 9E-02 2.1 58E+00 2 . 9 36 E + 0 0 1 . 773E-02 0.0 -0.080 0 .089 0.083

7.0000 2.11 3E+00 9.539E-02 2 . 208E+00 3 . 394E+00 2.090E-02 0.0 -0.079 0.087 0.081 8.0000 2 . 1 44E+00 1 . 1 20E-01 2 . 256E+00 3 . 842E+0 0 2.409E-02 0.0 -0.077 0.086 0.080

9.0000 2.171 E+00 1 . 290E-0

1

2 . 300E+00 4.281 E+00 2 . 729E-02 0.0 -0.076 0.084 0.078

1 0.0000 2.1 96E+00 1 . 464E-0

1

2 . 342E+00 4.71 2E+00 3 . 049E-02 0.0 -0.075 0.083 0.077

12.5000 2.249E+00 1 . 909E-01 2 . 440E+00 5 . 757E+00 3.847E-02 0.0 -0 .074 0.081 0.074

1 5.0000 2 . 293E+00 2. 367E-01 2 . 530E+00 6 . 763E+00 4.638E-02 0.0 -0 .072 0.079 0.072

17.5000 2 . 330 E+0 0 2.835E-01 2.61 4E+00 7 . 735E+00 5.419E-02 0.0 -0.071 0.077 0.070 20.0000 2 . 363E+00 3.31 IE-01 2.694E+00 8 . 677E+00 6. 188E-02 2 . 424E-0 5 -0.069 0.075 0.068

25.0000 2.41 3E+00 4.282E-01 2.841 E+00 1 . 048E+0

1

7 . 689E-02 5 . 648E-02 -0.052 0 . 071 0.062

30.0000 2 . 448E+00 5 . 270E-0

1

2 . 975E+00 1 . 220E+0

1

9 . 1 42E-02 1 .676E-01 -0.042 0.067 0.055

35.0000 2 . 476E+00 6.271E-01 3 . 1 03E+00 1 . 385E+0

1

1 . 055E-0

1

2.951E-01 -0.036 0.063 0.049

40.0000 2 . 4 98E+00 7.284E-01 3 . 226E+00 1 .543E+01 1 .190E-01 4.244E-01 -0.032 0.059 0.044

45.0000 2.517E+00 8.306E-01 3 . 347E+00 1 . 6 95E+0

1

1 . 321 E— 01 5.501 E-0

1

-0.029 0 .056 0.040 50.0000 2.533E+00 9.334E-01 3 . 466E+00 1 . 842E+0

1

1 . 448E-0

1

6 . 699E-01 -0.027 0.053 0.036 55.0000 2 . 547E+00 1 . 037E+00 3 . 584E+00 1 . 984E+01 1 .570E-01 7 . 833E-0

1

-0.025 0.050 0.034

60 . 0000 2 . 560E+00 1 .141 E+00 3.701 E+00 2.121 E+OI 1 . 689E-0

1

8.903E-01 -0.024 0.048 0.031 70.0000 2.581 E+00 1 .351 E+0 0 3 . 932E+00 2.383E+01 1 .914E-01 1 . 087E+00 -0.022 0.045 0.027

80.0000 2 . 600E+00 1 . 562E+00 4 . 1 62E+00 2.630E+01 2. 124E-01 1 . 263E+00 -0.021 0.042 0.025

90.0000 2.616E+00 1 . 77 4E + 00 4 . 390E+00 2 . 864E+0

1

2.321E-01 1 . 422E+00 -0.020 0.039 0.022

1 00.0000 2 . 6 30E + 0 0 1 . 988E+00 4 .613E+00 3 . 086E+0

1

2 . 507E-0

1

1 . 567E+00 -0.019 0.037 0.020

125.0000 2 . 659E+00 2 . 525E+00 5. 185E+00 3.597E+01 2.925E-01 1 . 880E+00 -0.018 0.034 0.017

150.0000 2 . 683E+00 3 . 067E+00 5 . 750E+00 4.054E+01 3 . 289E-0

1

2. 1 42E+00 -0.017 0.031 0.015

175.0000 2 . 702E+00 3.611 E+00 6.31 4E+00 4.469E+01 3.609E-01 2 . 36 9E+00 -0.016 0.029 0.013

200.0000 2.71 9E+00 4. 158E+00 6 .877E+00 4 . 848E+0

1

3.894E-01 2.569E+00 -0.015 0.027 0.012 250.0000 2 . 746E+00 5 . 258E+00 8 . 003E+00 5 . 522E+0

1

4.379E-01 2.912E+00 -0.013 0.024 0.010 300.0000 2 . 767E+00 6 . 362E+00 9. 1 29E+00 6.106E+01 4.779E-01 3.201E+00 -0.012 0 .022 0.009

350.0000 2 . 784E+00 7.471 E+00 1 . 026E+0

1

6 . 623E+0

1

5. 1 15E-01 3 . 454E+00 -0.010 0.021 0.008 400.0000 2 . 7 9 9E+0 0 8 . 583E+00 1 . 1 38E+01 7 . 085E+0

1

5 . 403E-0

1

3 . 679E+00 -0.009 0.020 0.007 450.0000 2.811 E+00 9 . 697E+00 1 . 251 E+01 7 . 504E+0

1

5.653E-01 3 . 882E+00 -0.008 0.019 0.006 500.0000 2 . 822E + 00 1 .081E+01 1 . 364E+0

1

7 . 887E+0

1

5.872E-01 4 . 067E+00 -0.007 0.018 0.005 550.0000 2 . 832E+0 0 1 . 1 93E+01 1 . 47 6E+0

1

8 . 239E+0

1

6 .066E-01 4 . 237E+00 -0.006 0.017 0.005 600.0000 2 . 840 E+0 0 1 . 305E+0

1

1 .589E + 01 3.566E+01 6 . 240E-0

1

4 . 395E+00 -0.005 0.016 0.004

700.0000 2 . 855E+00 1 . 529E+0

1

1 .81 5E + 01 9.154E+01 6 . 537E-01 4 . 680E+00 -0 .004 0.015 0.004 800.0000 2 . 867E+00 1 . 754E+0

1

2 . 040E+0

1

9 . 674E+0

1

6 .785E-01 4. 930E+00 -0.003 0.015 0.003

900.0000 2 . 878E+00 1 . 978E+01 2 . 266E+0

1

1 .01 4E+02 6.993E-01 5 . 1 54E+00 -0.003 0.014 0.003

1000.0000 2 . 887E+00 2 . 203E+0

1

2.492E+01 1 . 056E+02 7.173E-01 5.356E+00 -0.002 0.013 0.003

108
ELECTRONS IN ADIPOSE TISSUE (ICRP)

I = 63.2 eV DENSITY = 9.200E-01 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. ddog )/d(loqI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

MeV cm 2 /g

(DELTA) LOSS RANGE YIELD

Me V MeV cm 2/g MeV cm 2/g g/cm 2 0.0100 2 . 347E+0

1

3. 168E-03 2 . 347E+0

1

2 . 406E-04 7 . 396E-05 0.0 -0.192 0.218 0.217 0.0125 1 . 971 E+01 3. 184E-03 1 . 971 E + 01 3.574E-04 8.884E-05 0.0 -0.184 0.209 0.207 0.0150 1 . 709E + 01 3.1 94E-03 1 .709E + 01 4 . 940E-04 1 . 031 E-04 0 .

0

-0.179 0.201 0.200 0.0175 1 .515E+01 3.201E-03 1 . 51 5E+01 6 . 497E-04 1 . 1 68E-04 0.0 -0.174 0 . 1 95 0.194

0.0200 1 . 565E+01 3 . 207E-03 1 . 365E+0

1

8 . 237E-0 4 1 . 30 1 E-04 0 .

0

-0.170 0.190 0.189

0.0250 1 . 148E+01 3.217E-03 1 .149E+01 1 . 225E-0 3 1 . 556E-04 0.0 -0.164 0.182 0.182

0.0300 9 . 984E+0 0 3.227E-03 9 . 987E+00 1 . 6 93E-03 1 . 800E-04 0.0 -0.159 0.177 0.176 0.0350 8.8S1E+00 3.238E-03 8 . 884E+00 2 . 225E-03 2 . 034E-04 0.0 -0.156 0.172 0.172

0.0400 8 . 034E+00 3 . 249E-03 3 . 0 37E+0 0 2.818E-03 2 . 260E-04 0.0 -0.153 0.163 0.168

0 . 0450 7 . 362E+00 3.262E-03 7 . 365E+00 3 . 463E-03 2.480E-04 0.0 -0.150 0.165 0.165

0.0500 6 .81 6E+00 3.275E-03 6.81 9E+00 4. 175E-03 2 . 6 93E-04 0.0 -0 . 1 48 0.162 0.162

0.0550 6 . 362E+00 3.290E-03 6 . 365E+00 4. 934E-03 2. 902E-04 0.0 -0.146 0.160 0.160 0.0600 5 . 979E+00 3 . 305E-03 5. 983E+00 5.745E-03 3. 106E-04 0.0 -0.144 0.158 0.158

0.0700 5 . 369E+00 3 . 333E-03 5 . 372E+00 7.513E-03 3.501 E-04 0 .

0

-0.141 0.154 0.154

0.0800 4 . 903E+00 3.373E-03 4. 906E+00 9.464E-03 3.881 E-04 0.0 -0.139 0.151 0.151 0.0900 4 . 535E+00 3.411E-03 4 . 539E+00 1 . 159E-02 4 . 250E-04 0.0 -0.137 0.149 0.148

0.1000 4 . 238E+00 3.452E-03 4.241 E+00 1 . 387E-02 4.608E-04 0.0 -0.135 0.147 0.146

0.1250 3.696E+00 3.562E-03 3 . 700 E+00 2 . 020E-02 5.464E-04 0.0 -0.131 0.142 0.142 0.1500 3.330E+00 3.681 E-03 3 . 334E+00 2 . 734E-02 6 . 277E-04 0.0 -0.128 0.139 0.138 0.1750 3 . 0 68E + 00 3 . 808E-0 3 3.071 E+00 3.51 7E-02 7 . 055E-04 0.0 -0.126 0 . 1 36 0.136 0.2000 2.871 E+00 3. 943E-03 2 . 875E+00 4.359E-02 7 . 806 E-04 0.0 -0.124 0.134 0.133

0.2500 2 . 597E+00 4.232E-03 2.601 E+00 6.1 94E-02 9.244E-04 0.0 -0.120 0.130 0.130 0.3000 2.418E+00 4 . 547E-03 2 . 422E+00 8.1 90E-02 1 . 062E-03 0 . 0 -0.118 0.127 0.127

0 . 3500 2 . 294E+00 4.885E-03 2 . 299E+00 1 .031 E-0

1

1 . 1 96E-03 0.0 -0.116 0.125 0.124

0.4000 2 . 204E+00 5.244E-03 2.209E+00 1 . 253E-0

1

1 . 328E-03 0.0 -0.115 0.123 0.122

0.4500 2.1 35E+00 5.623E-03 2. 1 41 E+00 1 . 483E-0

1

1 . 458E-03 1 .471 E-02 -0.090 0.120 0.118

0.5000 2.081 E+00 6 . 020E-03 2 . 087E+00 1 . 720E-0

1

1 . 588E-0 3 4. 184E-02 -0.084 0.115 0.113 0.5500 2.039E+00 6 . 433E-0 3 2 . 045E+00 1 . 962E-01 1 . 7 1 8E-03 7 . 1 41 E-02 -0.078 0.111 0.107

0.6000 2 . 005E+00 6 . 86 0 E-03 2.01 1 E+00 2.209E-01 1 . 848E-03 1 . 028E-0

1

-0.074 0.107 0.103

0.7000 1 . 954E+00 7 . 753E-03 1 . 962E+00 2.712E-01 2 . 1 09E-03 1 . 6 9 1 E-0

1

-0.066 0.100 0.094

0.8000 1 . 921 E+00 8.692E-03 1 . 929E+00 3.227E-01 2 . 374E-03 2.381 E-0

1

-0.060 0.094 0.087

0 . 9000 1 . 897E+00 9.674E-03 1 . 907E+00 3.748E-01 2.642E-03 3.080E-01 -0.055 0.089 0.081

1 .0000 1 . 880E+00 1 . 070E-02 1 .891 E+00 4.275E-01 2.915E-03 3.776E-01 -0.051 0.034 0.076

1 .2500 1 . 858E+00 1 . 340E-02 1 .871E+00 5.605E-01 3.612E-03 5.471 E-0

1

-0.044 0.075 0.066

1 .5000 1 . 849E+00 1 .629E-02 1 .865E+00 6 . 944E-01 4.334E-03 7.067E-01 -0.039 0.069 0.058

1 .7500 1 . 848E+00 1 . 934E-02 1 . 867E+00 8.284E-01 5.078E-03 8.554E-01 -0.036 0.064 0.052

2.0000 1 . 850 E + 0 0 2 . 252E-02 1 . 873E+00 9 . 62 1 E-0

1

5 . 842E-03 9. 936E-01 -0.033 0.060 C.048

2.5000 1 . 860E+00 2.921E-02 1 .889E+00 1 . 228E+00 7 .421 E-03 1 . 242E+00 -0.030 0.053 0.042 3.0000 1 . 872E+00 3 . 626E-02 1 . 908E+00 1 .491 E+00 9 . 055E-0 3 1 . 459E+00 -0.028 0.049 0.037

3.5000 1 . 883E+00 4 . 360E-02 1 . 928E+00 1 . 752E+00 1 . 0 7 3E-02 1 . 652E+00 -0.026 0.046 0.034

4.0000 1 .897E+00 5. 120E-02 1 . 948E+00 2.01 0E+00 1 .245E-02 1 . 825E+0 0 -0.025 0.043 0.032

4.5000 1 . 909E + 00 5. 901E-02 1 . 968E+00 2 . 265E+00 1.41 9E-02 1 . 981 E+00 -0.024 0.041 0.030 5.0000 1 . 920E+00 6.701E-02 1 . 987E+00 2.51 8E+00 1 . 596E-02 2. 125E+00 -0.023 0.039 0.029 5.5000 1 . 930E+00 7.518E-02 2.005E+00 2.769E+00 1 .774E-02 2 . 257E+00 -0.022 0.037 0.027

6.0000 1 . 939E+00 8 . 350E-02 2 . 023E+00 3.01 7E+00 1 . 955E-02 2.379E+00 -0.022 0.036 0.026 7.0000 1 . 956E+00 1 .005E-01 2 . 057E+00 3 . 507E+00 2.31 9E-02 2.601 E+00 -0.020 0.034 0 .025 8.0000 1 . 972E+00 1 . 181E-01 2 . 0 90E+00 3 . 990E+00 2. 688E-02 2 . 7 98E+00 -0.019 0.032 0.023

9.0000 1 . 985E+00 1 .360E-01 2.121 E+00 4 . 465E+00 3.059E-02 2. 976E+00 -0.018 0.030 0.022

10.0000 1 . 997E+00 1 . 542E-0

1

2.151 E+00 4 . 933E+0 0 3.432E-02 3 . 1 37E+00 -0.017 0.029 0 .021 12.5000 2 . 022E+00 2.010E-01 2 . 223E+00 6 . 076E+00 4 . 368E-02 3.491 E+00 -0.014 0.026 0.013

15.0000 2 . 042E+00 2.492E-01 2.291E+00 7. 183E+00 5 . 300E-02 3 . 7 90E+00 -0.012 0.024 0.016

17.5000 2. 059E+00 2.984E-01 2 . 357E+00 8.259E+00 6.225E-02 4 . 050E+00 -0.010 0.022 0.015 20.0000 2 . 073E+00 3.485E-01 2.421 E+00 9 . 305E+00 7.138E-02 4 . 282E+00 -0.009 0.021 0.013 25.0000 2.095E+00 4.505E-01 2.546E+00 1 . 1 32E+01 8 . 923E-02 4 . 679E+00 -0.007 0.018 0.011 30.0000 2.11 3E+00 5.544E-01 2 . 668E+00 1 . 324E+0

1

1 . 065E-0

1

5.01 2E+00 -0.005 0.016 0.009

35.0000 2. 128E+00 6 . 597E-0

1

2 . 788E+00 1 . 507E+0

1

1 . 230 E-0

1

5.299E+00 -0.004 0.015 0.008 40.0000 2. 1 41 E+00 7.661 E-0

1

2. 907E+00 1 . 683E+0

1

1 . 389E-0

1

5.551 E+00 -0.003 0.013 0.007 45.0000 2. 152E+00 8.734E-01 3 . 025E+00 1 .851 E+01 1 . 542E-0

1

5 . 776E+00 -0.003 0.012 0 .006 50.0000 2.161 E+00 9.815E-01 3. 143E+00 2.013E+01 1 . 688E-01 5. 979E+00 -0.002 0.012 0.005 55.0000 2 . 1 70 E+0 0 1 . 090E+00 3 . 260E+00 2. 170E+01 1 . 829E-0

1

6. 163E+00 -0.002 0.011 0.004 60.0000 2. 178E+00 1 . 200E+00 3 . 377E+00 2 . 320E+0

1

1 . 964E-01 6 . 332E+00 -0.002 0.010 0.004 70.0000 2. 1 92E+00 1 . 420E+00 3.61 1E+00 2 . 607E+0

1

2.218E-01 6 . 632E + 00 -0.001 0.009 0.003 80.0000 2.203E+00 1 . 6 42E+0 0 3 . 845E+00 2 . 875E+0

1

2.454E-01 6 . 894E+00 -0.001 0.003 0.003

90.0000 2.214E+00 1 .865E+00 4.07 9E+00 3. 127E+01 2 . 673E-01 7 . 1 26E+00 -0.001 0.008 0.002

100.0000 2 . 223E+00 2 . 089E+00 4.31 2E+00 3.366E+01 2.877E-01 7 . 334E+00 -0.001 0 .007 0.002

125.0000 2.242E+00 2 . 653E+00 4.896E+00 3.910E+01 3.330E-01 7 . 775E+00 -0.000 0.006 0.001 150.0000 2. 258E+00 3 . 222E+00 5 . 480E+0 0 4.392E+01 3.718E-01 8.1 37E+00 -0.000 0.006 0.001 175.0000 2 . 272E+00 3 . 794E+00 6 . 065E+00 4 . 825E+0

1

4 . 054E-0

1

8 . 444E+00 -0.000 0.005 0.001 200.0000 2 . 283E+00 4 . 368E + 00 6.651 E+00 5.21 9E+01 4.350E-01 8.709E+00 -0.000 0.005 0.001 250.0000 2.302E+00 5 . 522E+00 7 . 824E+00 5. 91 1 E+01 4 . 345E-0

1

9. 154E+00 -0.000 0.004 0.001 300.0000 2.318E+00 6 . 632E+00 9 . OOOE+OO 6 . 507E+0

1

5.245E-01 9.51 8E+00 -0.000 0.004 0.001 350.0000 2. 331 E+00 7.845E+00 1 .018E+01 7 . 029E+0

1

5 . 578E-0

1

9.825E+00 -0.000 0.004 0.000 400.0000 2 . 343E+00 9.01 2E+00 1 . 1 36E+01 7.494E+01 5.859E-01 1 . 009E+01 -0 .000 0.003 0 .000 450.0000 2 . 353E+00 1 .018E+01 1 . 253E+0

1

7. 91 3E+01 6 . 100E-01 1 . 033E+0

1

-0.000 0.003 0.000 500.0000 2 . 362E+0 0 1 . 1 35E+0

1

1 .371E+01 8 . 294E+0

1

6.31 IE-01 1 . 0 54E+0

1

-0 .000 0.003 0.000 550.0000 2 . 370E+0 0 1 . 253E+0

1

1 . 490E+0

1

8 . 643E+0

1

6.496E-01 1 . 073E+0

1

-0 .000 0.003 0.000 600.0000 2 . 378E+00 1 . 370E+01 1 . 608E+0

1

8. 966E+01 6 . 660E-0

1

1 .090E+01 -0.000 0.003 0 .000 700.0000 2.391E+00 1 . 605E+0

1

1 . 844E+0

1

9 . 547E+0

1

6 . 939E-01 1 .121E+01 -0.000 0.003 0.000 800.0000 2 . 402E+00 1 .841 E+01 2.081E+01 1 . 006E+02 7. 169E-01 1 . 1 48E+01 -0.000 0.003 0.000 900.0000 2.41 3E+00 2 . 077E+0

1

2.318E+01 1 . 051 E+02 7.362E-01 1 .171E+01 -0.000 0.002 0.000 1000.0000 2 . 422E+00 2.31 3E+01 2 . 555E+0

1

1 . 092E+02 7.526E-01 1 . 1 92E+01 -0.000 0.002 0.000

109
ELECTRONS IN AIR, DRY (NEAR SEA LEVEL)

I = 85.7 eV DENSITY = 1.205E-03 g/cra 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log[ )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2/g MeV ca 2 /g g/cm 2 0.0100 1 . 975E+01 3 . 897E-03 1 . 976E+01 2 . 883E-0

A

1 . 082E-0

A

0.0 -0.20A 0.235 0.233 0.0125 1 . 663E+0

1

3.921E-03 1 .663E+01 A.269E-0A 1 . 299E-0

A

0.0 -0.195 0.223 0.222

0.0150 1 . AA5E+01 3. 937E-03 1 . AA5E+01 5.886E-0A 1 . 506E-0A 0.0 -0.189 0.215 0.213 0.0175 1 . 283E+0

1

3.9A6E-03 1 . 283E+0

1

7.726E-0A 1 . 706E-0

A

0.0 -0. 18A 0.208 0.207

0.0200 1 . 1 57E+01 3.95AE-03 1 . 158E+01 9.781 E-0

A

1 . 898E-0

A

0.0 -0.179 0.202 0.201 0.0250 9 . 753E+00 3. 966E-03 9 . 757E+00 1 . A51 E-03 2 . 267E-0

A

0.0 -0.173 0 . 1 9A 0.193

0.0300 8 . A92E+00 3.976E-03 8. A96E+00 2.001 E-0 3 2.618E-0A 0.0 -0.167 0.187 0.186 0.0350 7.563E+00 3.986E-03 7 . 567E+00 2 . 626E-03 2. 955E-0A 0.0 -0.163 0.182 0.181

0 .OAOO 6 . 8A8E+00 3.998E-03 6 . 852E+00 3 . 322E-03 3 . 280E-0

A

0.0 -0.160 0.178 0.177

0 .0450 6.281 E+0 0 A. 01 IE-03 6 . 285E+00 A . 035E-03 3 . 59AE-0

A

0.0 -0.157 0 . 1 7 A 0 . 1 7 A 0.0500 5.81 9E+00 A . 025E-03 5 . 823E + 00 A.912E-03 3 . 900E-0

A

0.0 -0.155 0.171 0.171 0.0550 5. A35E+00 A . 0A0E-03 5 . A39E+00 5 . 80 1 E-0 3 A . 1 97E-0

A

0.0 -0.153 0.168 0.168

0.0600 5.111E+00 A . 057E-03 5.11 5E+00 6.750E-03 A. A88E-0A 0 .0 -0.151 0.166 0.166 0.0700 A . 593E+00 A . 0 93E-03 A. 597E+00 8.817E-03 5 . 0A9E-0A 0.0 -0.1A7 0.162 0.162

0.0800 A. 1 98E+00 A. 1 33E-03 A . 202E+00 1 .1 10E-02 5 . 590 E-0

A

0.0 -0.1A5 0.159 0.158

0.0900 3 . 886E+0 0 A.175E-03 3 . 890E+00 1 . 357E-02 6.112E-0A 0.0 -0.1A2 0.156 0.156

0.1000 3 . 633E+00 A . 222E-03 3 . 637E+00 1 . 623E-02 6.618E-0A 0.0 -0.1 AO 0.153 0.153

0.1250 3. 172E+00 A . 3A8E-03 3 . 1 77E+00 2.362E-02 7.826E-0A 0.0 -0.136 0 . 1 A9 0 . 1 A8 0.1500 2.861E+00 A. A85E-03 2 . 865E+00 3.193E-02 8 . 968E-OA 0.0 -0.133 0.1 A5 0.1A5

0.1750 2 . 637E+00 A . 633E-03 2 . 6 A2E+00 A.103E-02 1 . 006E-03 0.0 -0.131 0.1 A2 0 . 1 A2 0.2000 2. A70E+00 A . 789E-03 2. A7AE+00 5 . 082E-02 1 .111 E-03 0.0 -0.128 0.1 AO 0.139

0.2500 2 . 236E+0 0 5.126E-03 2 . 2A2E+00 7.212E-02 1 .31 IE-03 0.0 -0.125 0.136 0.135

0.3000 2 . 08AE+00 5.A95E-03 2 . 089E+00 9 . 527E-02 1 . 50 2E-0 3 0.0 -0.122 0.133 0.132

0.3500 1 . 978E+00 5 . 890E-03 1 . 98AE+00 1 . 1 99E-0

1

1 .688E-03 0.0 -0.120 0.130 0.129

0 . A000 1 . 902E+00 6.311E-03 1 . 908E+00 1 . A56E-0

1

1 . 86 9E-0 3 0.0 -0.118 0.128 0.127

0 . A500 1 . 8A5E+00 6 . 757E-0 3 1 . 852E+00 1 . 722E-0

1

2.0A8E-03 0.0 -0.116 0.126 0.125

0.5000 1 . 302E+00 7 . 223E-0 3 1 . 80 9E+00 1 . 995E-0

1

2 . 225E-03 0.0 -0.1 1 A 0.125 0.123

0.5500 1 . 76 9E+00 7 . 708E-03 1 . 776E+00 2.27AE-01 2. A01 E-03 0.0 -0.113 0.123 0.122

0.6000 1 . 7A3E+00 8.21 0E-O3 1 -751E+00 2.558E-01 2.577E-03 0.0 -0.112 0.122 0.120

0.7000 1 . 706E+00 9 . 258E-03 1 . 71 5E+00 3.135E-01 2. 929E-03 0.0 -0.109 0.120 0.118

0.8000 1 . 683E+00 1 . 036E-02 1 . 6 9AE+00 3 . 722E-0

1

3 . 2S3E-03 0.0 -0.107 0.118 0.115

0.9000 1 . 66 9E+00 1 .151E-02 1 .681E+00 A.315E-01 3 . 638E-03 0.0 -0.106 0.116 0 . 1 1 A

1 .0000 1 .661E+00 1 .271 E-02 1 . 67AE+00 A.912E-01 3.997E-03 0.0 -0.10A 0.115 0.112

1 .2500 1 . 655E+00 1 . 588E-02 1 .671E+00 6. A08E-01 A . 906E-03 0.0 -0.101 0.112 0.108

1 .5000 1 .661E+00 1 . 927E-02 1 . 680E+00 7 . 900 E-0

1

5 . 836E-03 0.0 -0.099 0.109 0.106

1 .7500 1 . 672E+00 2 . 28AE-02 1 . 6 9AE+00 9 . 382E-0

1

6.78AE-03 0.0 -0.097 0.107 0.103

2.0000 1 . 68AE+00 2 . 656E-02 1 .71 1E+00 1 . 085E+00 7 . 7A8E-0 3 0.0 -0.095 0.106 0.101 2.5000 1 -712E+00 3.A37E-02 1 . 7A7E+00 1 . 37AE+00 9.71 6E-03 0.0 -0.092 0.103 0.098

3.0000 1 . 7A0E+00 A.260E-02 1 . 783E+0 0 1 . 658E+00 1 . 1 73E-02 0.0 -0.090 0.100 0.095

3.5000 1 . 766E+00 5.1 15E-02 1 .81 7E+00 1 . 935E+00 1 . 377E-02 0.0 -0.088 0.098 0.093

A. 0000 1 . 790E+00 5. 999E-02 1 .850E+00 2 . 208E+00 1 . 583E-02 0.0 -0.087 0.097 0.091

A .5000 1 .812E+00 6 . 908E-02 1 . 882E+00 2 . A76E+00 1 . 792E-02 0.0 -0.086 0.095 0.089

5.0000 1 . 833E+00 7 . 838E-02 1.911 E+0 0 2 . 7A0E+00 2.001 E-02 0.0 -0 .08A 0 .09A 0.088

5.5000 1 .852E + 00 8.787E-02 1 . 9A0E+O0 2. 999E+00 2.21 IE-02 0.0 -0.083 0.093 0.086 6.0000 1 . 870E + 0 0 9.75AE-02 1 . 968E+00 3 . 255E+00 2 . A22E-02 0.0 -0.083 0.092 0.085

7.0000 1 . 902E+00 1 .173E-01 2 . 020E+00 3 . 757E+00 2 . 8A5E-02 0.0 -0.081 0.090 0.083 8.0000 1 .931E+00 1 .376E-01 2 . 068E+00 A . 2A6E+00 3.269E-02 0.0 -0.080 0.088 0.081 9.0000 1 . 956E+00 1 . 58AE-0

1

2.11 5E+00 A . 72AE+00 3.692E-02 0.0 -0.079 0.087 0.080

10.0000 1 . 97 9E+00 1 . 795E-0

1

2 . 1 59E+00 5.1 92E+00 A.113E-02 0.0 -0.078 0.085 0.078

12.5000 2 . 029E+00 2.337E-01 2 . 262E+00 6 . 323E+00 5. 156E-02 0.0 -0.076 0.083 0.075

15.0000 2.06 9E+00 2.895E-01 2 . 359E+00 7. A05E+00 6.181 E-02 0.0 -0.07A 0.080 0.072

17.5000 2. 10AE+00 3. A6AE-01 2. A51 E+00 8 . AAAE+00 7. 185E-02 0.0 -0.073 0.073 0.070 20.0000 2.1 3AE+00 A.0A2E-01 2.539E+00 9. AA6E+00 3.167E-02 0.0 -0.072 0.076 0.068

25.0000 2. 185E+00 5.219E-01 2. 707E+00 1 . 1 35E+01 1 . 006E-0

1

0.0 -0.070 0.073 0.065

30.0000 2 . 226E+00 6.A17E-01 2 . 868E+0 0 1 . 31 5E+01 1 . 1 8 6 E-0

1

7 . 636E-03 -0.062 0.071 0.062

35.0000 2. 257E+00 7.630E-01 3 . 020E+00 1 . A85E+01 1 . 357E-0

1

5.98AE-02 -0.052 0.068 0.057

AO .0000 2 . 282E+00 8.855E-01 3 . 1 67E+00 1 . 6 A6E+0

1

1 .520E-01 1 . 378E-01 -0 . 0 A

A

0 . 06 A 0.052

A5.0000 2 . 302E+00 1 . 00 9E+00 3.31 1 E+00 1 .801 E+0

1

1 . 676E-01 2.266E-01 -0.039 0.061 0.0A8

50.0000 2.31 9E+00 1 . 1 33E+00 3 . A52E+00 1 . 9A8E+01 1 .825E-01 3.1 92E-01 -0.035 0.059 O.OAA

55.0000 2 . 33AE+00 1 . 258E+00 3 . 592E+00 2.090E+01 1 . 968E-0

1

A. 120E-01 -0.032 0.056 0.0A0 60.0000 2, 3A7E+00 1 . 38AE+00 3.731 E+00 2 . 227E+0

1

2. 10AE-01 5.029E-01 -0.030 0 .05A 0.037

70.0000 2.369E+00 1 . 637E+00 A . 006E+00 2. A86E+01 2.361 E-0

1

6 .762E-01 -0.027 0.050 0.033 80.0000 2 . 387E+00 1 . 892E+00 A . 279E+00 2 . 727E+0

1

2.598E-01 8.365E-01 -0.025 0 .0A7 0.029

90.0000 2. A03E+00 2. 1 A8E+00 A . 551 E+00 2. 95AE+01 2.818E-01 9.8A2E-01 -0.023 O.OAA 0.026 100.0000 2.A17E+00 2 . A05E+00 A.822E+00 3.167E+01 3 . 022E-01 1 . 1 20E+00 -0.022 0.0A2 0.02A

125.0000 2. AA5E+00 3 . 053E+00 5 . A98E+00 3 . 652E+0

1

3. A7AE-01 1 . A 1 9E+00 -0.020 0.038 0.020

150.0000 2. A68E+00 3 . 705E+00 6 . 1 73E+00 A . 08 1 E+0

1

3.859E-01 1 . 670E+00 -0.019 0.035 0.017

175.0000 2. A86E+00 A . 360E+00 6 .8A7E+00 A. A65E+01 A. 1 92E-01 1 . 887E+00 -0.018 0.032 0.015 200.0000 2 . 502E+00 5.01 8E+00 7 . 520E+00 A. 81 AE+01 A . A8AE-0

1

2 . 078E+00 -0.017 0.030 0.013 250.0000 2 . 529E+00 6 . 3A0E+0O 3 . 868E+00 5. A25E+01 A . 972E-01 2. A03E+00 -0.016 0.028 0.011 300.0000 2 . 550E+00 7 . 667E+00 1 . 022E+0

1

5 . 950E+0

1

5.365E-01 2 . 675E+00 -0.015 0.026 0.009 350.0000 2 . 567E+00 8. 998E+00 1 . 157E+01 6.A10E+01 5.691 E-0

1

2. 909E+00 -0.01 A 0.02A 0.008 A00.0000 2 . 582E+00 1 . 033E+01 1 . 292E+0

1

6.819E+01 5. 967E-01 3.1 16E+00 -0.013 0.023 0.007 A50.0000 2 . 595E+00 1 . 1 67E+0

1

1 .A27E+01 7. 187E+01 6 .203E-01 3 . 302E + 00 -0.012 0.022 0.007

500.0000 2. 606E+00 1 .301 E+0

1

1 . 562E+0

1

7 . 522E+0

1

6 . A09E-01 3. A72E+00 -0.011 0.021 0.006 550.0000 2.61 6E + 00 1 . A35E+01 1 . 6 97E+0

1

7 . 829E+0

1

6 . 589E-0

1

3 . 628E+00 -0.010 0.020 0.006 600.0000 2 . 625E+00 1 .569E+01 1 . 832E+0

1

8.1 12E+01 6 . 7 50 E-0

1

3 . 772E+00 -0.010 0.019 0.005 700.0000 2.6A1E+00 1 . 838E+0

1

2. 102E+01 8 . 622E+0

1

7 . 022E-0

1

A . 0 3 AE+0 0 -0.008 0.018 0 .00A 800.0000 2 . 653E+00 2. 107E+01 2 . 372E+0

1

9.069E+01 7.2A7E-01 A . 267E+00 -0.007 0.017 0 . 00 A 900.0000 2.66AE+00 2 . 376E+0

1

2 . 6A3E+01 9 . A68E+0

1

7.A35E-01 A . A77E+00 -0.006 0.017 0 .OOA 1000.0000 2 . 67AE+00 2.6A6E+01 2.913E+01 9 . 829E+0

1

7 . 595E-0

1

A . 668E+00 -0.005 0.016 0.003

110
ELECTRONS IN ALUMINUM OXIDE

I = 145.2 eV DENSITY = 3 . 970E+0Ci g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS .EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2/g g/cm 2 0.0100 1 .731 E+01 5.480E-03 1 . 732E+0

1

3.351E-04 1 . 7 1 4E-04 0.0 -0.229 0.270 0.266 0.0125 1 . 465E+0

1

5.569E-03 1 . 466E+0

1

4. 927E-04 2.068E-04 0.0 -0.218 0.255 0.251 0.0150 1 . 278E+0

1

5.629E-03 1 . 278E + 0

1

6 . 758E-04 2 . 407E-04 0.0 -0.210 0.244 0.241 0.0175 1 . 1 38E+01 5.674E-03 1 . 1 38E+0

1

8.835E-04 2.734E-04 0.0 -0.203 0.235 0.232

0.0200 1 . 029E+0

1

5.707E-03 1 . 030E + 0

1

1.11 5E-03 3.050E-04 0 .

0

-0.198 0.228 0.225

0.0250 8.709E+00 5 . 753E-03 8.71 5E+00 1 .645E-03 3.656E-04 0.0 -0.190 0.217 0.215

0.0300 7 . 605E+00 5.786E-03 7.611 E+00 2.261E-03 4.231E-04 0.0 -0.184 0.208 0.207 0.0350 6 . 789E+00 5.812E-03 6 . 795E + 00 2. 957E-03 4.781 E-04 0.0 -0.179 0.202 0.201 0.0000 6 . 1 60E+00 5.835E-03 6 . 1 65E+00 3.731 E-03 5.31 OE-04 0 .

0

-0.175 0.197 0.195 0.0050 5 . 658E+00 5.856E-03 5 . 664E+00 4.578E-03 5 . 820 E-04 0 .

0

-0.171 0.192 0.191 0.0500 5.249E+00 5.878E-03 5 . 255E+0 0 5.495E-03 6 . 31 5E-04 0.0 -0.169 0.189 0.188 0.0550 4 . 909E+00 5.399E-03 4.915E+00 6 .480E-03 6.795E-04 0.0 -0.166 0.185 0.184 0.0600 4 .621 E+00 5. 921 E-03 4 . 627E+00 7.529E-03 7.262E-04 0.0 -0.164 0.132 0.182

0.0700 4. 161E+00 5. 965E-03 4.167E+00 9.81 IE-03 8 . 1 62E-04 0.0 -0.160 0.178 0.177 0.0800 3.809E+00 6.014E-03 3.81 5E+00 1 . 232E-0 2 9.023E-04 0.0 -0.157 0.174 0.173

0.0900 3 . 530E+00 6 . 068E-03 3 . 536E+00 1 . 50 5E-02 9 . 850E-04 0.0 -0.154 0.170 0.170 0.1000 3 . 305E+00 6 . 126E-03 3.31 1 E+00 1 .797E-02 1 . 065E-03 0 .

0

-0.152 0.167 0.167 0.1250 2 . 8 92E+0 0 6.285E-03 2 . 8 98E+0 0 2 . 608E-02 1 . 254E-03 0.0 -0.147 0.162 0.161 0.1500 2.613E+00 6 . 464E-03 2.61 9E+00 3.517E-02 1 . 432E-03 0.0 -0.143 0.157 0.157 0.1750 2.412E+00 6.661 E-03 2.41 9E+00 4.51 2E-02 1 . 600E-03 0.0 -0.140 0.154 0.153 0.2000 2 . 262E+00 6 .871E-03 2.269E+00 5.581E-02 1 . 762E-03 0.0 -0.138 0.151 0.150 0.2500 2 . 0 52E+0 0 7.330E-03 2 . 059E+00 7.902E-02 2 . 068E-03 1 . 0 94E-0 3 -0.125 0.146 0.145

0 . 3000 1 . 91 2E+00 7 .834E-03 1 . 920E+00 1 .042E-01 2 . 360 E-03 2.440E-02 -0.113 0.139 0.137

0.3500 1 .81 5E+00 8 . 376E-03 1 . 823E+00 1 .310E-01 2.643E-03 4.961 E-02 -0.107 0.133 0.131 0.4000 1 . 744E+00 8. 954E-03 1 . 753E+00 1 . 590E-0

1

2.91 9E-03 7 . 609E-02 -0.102 0.128 0.125

0.4500 1 .691 E+00 9.563E-03 1 . 700E+00 1 .879E-01 3.1 91 E-03 1 .034E-01 -0.097 0.123 0.120 0.5000 1 . 650E+00 1 . 020E-02 1 . 660E+00 2. 177E-01 3 . 460E-03 1 . 3 1 4E-0

1

-0.094 0.119 0.116 0.5500 1 . 6 1 8E+00 1 . 086E-02 1 . 629E+00 2.481E-01 3.728E-03 1 .597E-01 -0.090 0.116 0.112

0 .6000 1 . 593E+00 1 .155E-02 1 . 605E+00 2.791E-01 3 . 995E-03 1 . 883E-0

1

-0.087 0.113 0.109

0.7000 1 . 557E+00 1 . 298E-02 1 . 570E+00 3.421E-01 4.529E-03 2.455E-01 -0.082 0.108 0.103

0.8000 1 . 533E+00 1 . 449E-02 1 . 547E+00 4.063E-01 5 . 064E-03 3.026E-01 -0.078 0.103 0.097

0 . 9000 1 .517E+00 1 . 606E-02 1 . 533E+0O 4.712E-01 5 . 603E-03 3.589E-01 -0.074 0.099 0.093

1 .0000 1 . 507E+0 0 1 . 7 6 9E-0 2 1 . 524E+0 0 5.367E-01 6.147E-03 4.143E-01 -0.071 0.096 0.089

1 .2500 1 . 4 94E+0 0 2.201E-02 1 . 51 6E+00 7.013E-01 7.528E-03 5.479E-01 -0.064 0 . 089 0.081 1.5000 1 . 492E+00 2.662E-02 1.51 9E+00 8 . 661 E-01 8 . 942E-03 6 .744E-01 -0.059 0.083 0.075

1 .7500 1 . 495E+00 3. 148E-02 1 . 527E+00 1 . 030E+00 1 .039E-02 7 . 938E-01 -0.054 0.079 0.070 2.0000 1 .501 E+00 3 . 6 53E-02 1 . 537E+0 0 1 . 1 93E+00 1 . 136E-02 9.069E-01 -0.050 0.075 0 . 065

2 . 5000 1 . 51 4E+00 4.714E-02 1 .561 E+00 1 .51 6E+00 1 . 488E-02 1 . 1 1 6E+00 -0.044 0.069 0.058

3.0000 1 . 523E+00 5 . 829E-02 1 . 586E+00 1 .834E+00 1 .798E-02 1 . 306E+00 -0.040 0.064 0.053 3.5000 1 . 541 E+00 6.987E-02 1 .61 1E+00 2. 147E+00 2.11 3E-02 1 . 47 9E+00 -0.036 0.060 0.048

4 .0000 1 . 553E+0 0 8.181E-02 1 . 635E+00 2 . 455E+0 0 2.433E-02 1 . 638E+00 -0.033 0.057 0.045 4.5000 1 . 564E+00 9 . 407E-02 1 . 658E+00 2 . 759E+00 2.756 E-02 1 . 785E + 00 -0.031 0.054 0.041 5.0000 1 . 575E+00 1 .066E-01 1 .681 E+00 3 . 058E+00 3.081E-02 1 . 921 E+00 -0.029 0.051 0.039

5.5000 1 . 584E+00 1 . 1 94E-01 1 . 704E+00 3 . 353E+00 3.408E-02 2 . 048E+00 -0.027 0.049 0.037 6.0000 1 . 593E+00 1 . 324E-0

1

1 . 725E+00 3 . 645E+00 3.735E-02 2 . 1 67E+00 -0.026 0.047 0.035 7.0000 1 . 60 9E+00 1 .590E-01 1 . 767E+00 4.21 8E+00 4.392E-02 2 . 384E+00 -0.024 0.044 0.031 8.0000 1 . 6 22E + 0 0 1 .862E-01 1 . 808E+00 4 . 777E+00 5 . 049E-02 2 . 578E+00 -0.022 0.041 0.029

9.0000 1 . 6 34E + 0 0 2. 140E-01 1 . 848E+00 5 . 324E+00 5.704E-02 2 . 754E+00 -0.020 0.039 0.027

10.0000 1 . 645E+00 2.422E-01 1 .887E+00 5 . 859E+00 6 . 354E-02 2. 91 4E+00 -0.019 0.037 0.025

12.5000 1 . 667E+00 3.145E-01 1 . 982E+00 7 . 1 52E+00 7 . 956E-02 3 . 263E + 00 -0.017 0.033 0.021 15.0000 1 . 685E+00 3.886E-01 2 . 074E+00 8 . 385E+00 9 . 51 6E-02 3 . 557E + 00 -0.015 0.030 0.019

17.5000 1 . 700E+00 4.642E-01 2. 164E+00 9 . 565E+00 1 . 1 03E-01 3.81 2E+00 -0.013 0.028 0.017 20.0000 1 . 7 1 3E+00 5.409E-01 2 . 254E+00 1 . 070E+0

1

1 .249E-01 4 . 038E+00 -0.012 0.026 0.015 25.0000 1 . 734E+00 6.968E-01 2.431 E+00 1 . 283E+0

1

1 . 527E-0

1

4 . 424E+00 -0.010 0.023 0.013 30.0000 1 . 750E+00 8.552E-01 2 . 606E+00 1 . 482E+0

1

1 . 786E-0

1

4 . 747E+00 -0.008 0.021 0.011 35.0000 1 . 764E+00 1 .01 5E+00 2 . 780E+00 1 . 668E+0

1

2.026E-01 5 . 025E+00 -0.007 0.019 0.010 40.0000 1 . 776 E + 0 0 1 . 177E+00 2 . 953E+00 1 . 842E+0

1

2.251E-01 5 . 26 9E+00 -0.006 0.018 0.008 45.0000 1 .786E+00 1 . 340E+00 3 . 1 26E+00 2 . 007E+0

1

2.461E-01 5 . 487E+00 -0.005 0.016 0.008

50.0000 1 . 7 95E+0 0 1 . 504E + 00 3 . 299E+00 2. 162E+01 2. 657E-01 5 . 684E+00 -0.005 0.015 0.007 55.0000 1 .803E+00 1 . 669E+00 3 . 472E+00 2.310E+01 2.842E-01 5 . 364E+00 -0.004 0.015 0.006 60.0000 1 . 81 0E+00 1 . 835E+00 3 . 645E+00 2.451 E+01 3.015E-01 6 . 029E+00 -0.004 0.014 0.006 70.0000 1 . 822E+00 2.1 68E+00 3. 990E+00 2.71 3E+01 3.333E-01 6 . 323E+00 -0.003 0.013 0 .005 80.0000 1 .833E+00 2.503E+00 4 . 337E+00 2. 953E+01 3.617E-01 6.581 E+00 -0.002 0.012 0 .004 90.0000 1 .842E+00 2.841 E+00 4 . 683E+00 3.1 75E+01 3.873E-01 6 . 80 9E + 00 -0.002 0.011 0.003

100.0000 1 .851 E+00 3.17 9E+00 5.030E+00 3.381E+01 4.106E-01 7.015E+00 -0.002 0.010 0.003

125.0000 1 . 868E+00 4 .030E+00 5 . 898E+00 3.839E+01 4 . 602E-01 7 . 452E+00 -0.001 0.009 0.002

150.0000 1 . 882E+00 4 . 887E + 00 6 . 76 9E+00 4 . 235E+0

1

5.008E-01 7.812E+00 -0.001 0.008 0 .002 175.0000 1 . 894E+00 5 . 747E+00 7.641 E+00 4.582E+01 5.346E-01 8. 117E+00 -0.001 0.008 0 .002 200.0000 1 . 904E+00 6.611 E+00 8.51 5E+00 4.892E+01 5.634E-01 8 . 382E+00 -0.001 0 .007 0.001 250.0000 1 . 921 E+00 8 . 345E + 00 1 . 027E+0

1

5.426E+01 6 . 098E-01 8.825E+00 -0 .000 0.007 0.001 300.0000 1 . 935E+00 1 .009E+01 1 . 202E+0

1

5.876E+01 6 . 460E-0

1

9 . 1 38 E+0 0 -0.000 0.006 0.001 350.0000 1 . 947E+00 1 . 183E+01 1 . 378E+0

1

6.264E+01 6 . 750E-01 9 . 495E+00 -0.000 0 .006 0.001 400.0000 1 . 957E+00 1 . 358E+0

1

1 . 554E+0

1

6.605E+01 6.990E-01 9.761 E+00 -0.000 0.005 0.001 450.0000 1 . 966E+00 1 .533E+01 1 . 730E+0

1

6.910E+01 7.1 91E-01 9 . 996E+00 -0.000 0.005 0.001 500.0000 1 . 974E+00 1 .709E+01 1 . 906E+01 7. 185E+01 7.364E-01 1 .02! E+01 -0.000 0.005 0.001 550.0000 1 . 981 E+00 1 . 885E+0

1

2 . 083E+0

1

7 . 436E+0

1

7.513E-01 1 . 040E+0

1

-0.000 0.005 0.000 600.0000 1 . 988E+00 2 . 060E+0

1

2.259E+01 7 . 667E+0

1

7.644E-01 1 . 057E+0

1

-0.000 0.005 0.000 700.0000 1 . 999E+00 2.412E+01 2.612E+01 8 . 078E+0

1

7 . 864E-01 1 . 088E+0

1

-0.000 0.004 0.000 800.0000 2.009E+00 2 . 765E+0

1

2.966E+01 8.437E+01 8.041E-01 1 . 1 15E+01 -0.000 0.004 0.000 900.0000 2.01 8E+00 3. 1 17E+01 3.319E+01 8 . 756E+0

1

8. 187E-01 1 . 138E+01 -0.000 0.004 0 .000 1000.0000 2 . 026E+00 3 , 470E+0

1

3 . 673E+0

1

9 . 042E+0

1

8.311 E-01 1 .159E+01 - 0.000 0.004 0.000

111
ELECTRONS IN B-IOO BONE-EQUIVALENT PLASTIC

I = 85.9 eV DENSITY = 1 . 950E+00i g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log1 )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2/g g/cm 2 0.0100 2 . 086E+0

1

9.977E-03 2.086E+01 2.731E-09 1 . 1 93E-09 0.0 -0.209 0.235 0.232 0.0125 1 .756E+01 9.559E-03 1 . 756E+0

1

9 . 093E-09 1 . 389E-09 0.0 -0.196 0.223 0.221 0.0150 1 . 525E+0

1

9.618E-03 1 .526E+01 5.579E-09 1 . 626E-09 0.0 -0.189 0.215 0.213

0.0175 1 . 359E+0

1

9.669E-03 1 . 355E+0

1

7.317E-09 1 .856E-09 0.0 -0.189 0.208 0 . 206 0.0200 1 . 222E+0

1

9.700E-03 1 . 222E+0

1

9.263E-09 2.080E-09 0.0 -0.179 0.202 0.201 0.0250 1 . 030E+01 9.759E-03 1 . 0 30E + 0

1

1 . 379E-0

3

2.511 E-09 0.0 -0.173 0 . 1 99 0.192

0.0300 8. 967E+00 9 . 796E-03 8. 972E+00 1 .895E-03 2. 923E-09 0.0 -0.168 0.187 0.186 0.0350 7 . 986E+00 9.830E-03 7 . 991 E+00 2.937E-03 3.31 9E-09 0.0 -0.169 0.182 0.181

0 .0400 7 . 232E+00 9.860E-03 7 . 237E+0 0 3. 196E-03 3.702E-09 0.0 -0.160 0.173 0.177 0.0950 6.633E+00 9.888E-03 6 . 637E + 0 0 3.868E-03 9.073E-09 0.0 -0.157 0.179 0.173

0.0500 6. 195E+00 9.919E-03 6 . 150E+00 9.651E-03 9.939E-09 0 .

0

-0.155 0.171 0.170

0.0550 5 . 739E+00 9. 939E-03 5 . 799E+00 5 . 993E-03 9 . 785E-09 0.0 -0.153 0.168 0.168

0.0600 5 . 397E+00 9 . 963E-03 5 . 902E+00 6 . 392E-03 5.127E-09 0.0 -0.151 0.166 0.165

0.0700 9 . 850E+0 0 5.01 3E-03 9.855E+00 8.398E-03 5.789E-09 0.0 -0.198 0.162 0.161 0.0800 9 . 933E+00 5.063E-03 9 . 938E+00 1 .051E-02 6 . 929E-09 0.0 -0.195 0.159 0.158

0.0900 9. 103E+00 5. 1 16E-03 9 . 1 09E+00 1 . 285E-02 7.036E-09 0.0 -0.193 0.156 0.155

0.1000 3 . 837E+00 5. 170E-03 3 . 892E+00 1 . 537E-02 7 . 628E-09 0.0 -0.191 0.159 0.153

0.1250 3 . 350E+00 5.318E-03 3 . 355E+00 2 . 236E-02 9.036E-09 0.0 -0.136 0.199 0.198

0.1500 3.021E+00 5.979E-03 3 . 027E+00 3.023E-02 1 . 036E-03 0.0 -0.133 0.195 0.199

0.1750 2 . 785E+00 5.651E-03 2.791 E+00 3.889E-02 1 . 162E-03 0.0 -0.131 0.192 0.191 0.2000 2 . 608E+00 5 . 835E-03 2.61 9E+00 9.81 IE-02 1 . 283E-0 3 0.0 -0.129 0.190 0.139

0.2500 2 . 362E+00 6.231E-03 2 . 368E+00 6 . 827E-02 1 .51 3E-03 0.0 -0.125 0.136 0.135

0.3000 2.201 E+00 6 . 665E-03 2 . 208E+00 9.01 9E-02 1 . 732E-03 0.0 -0.122 0.133 0 . 1 32 0.3500 2 . 089E+00 7.131E-03 2 . 0 96E+0 0 1 . 1 35E-0

1

1 .993E-03 9 . 066E-03 -0.105 0.130 0.128

0.9000 2 . 005E+00 7 . 626E-03 2.01 3E+00 1 . 378E-01 2.150E-03 2 . 983E-02 -0.095 0.129 0.122

0.9500 1 . 992E+00 8. 199E-03 1 . 950E+00 1 .631E-01 2.353E-03 5.881 E-02 -0.089 0.119 0.116

0.5000 1 .893E+00 8.695E-03 1 . 902E+00 1 .891E-01 2.555E-03 8. 971 E-02 -0.083 0.119 0.111 0.5500 1 . 855E+00 9.253E-03 1 . 869E+00 2.156E-01 2 . 757E-03 1 .21 9E-01 -0.079 0.110 0.106 0.6000 1 . 825E+00 9.852E-03 1 . 835E+00 2.927E-01 2. 958E-03 1 . 598E-0

1

-0.075 0.107 0.102

0.7000 1 . 780E+00 1 . 108E-02 1 . 7 91 E + 00 2. 979E-01 3.360E-03 2.222E-01 -0.069 0.100 0.099

0.8000 1 . 750E+00 1 . 237E-02 1 . 762E+00 3.592E-01 3 . 766E-03 2.901 E-0

1

-0.063 0.099 0.088

0 . 9000 1 . 730E+00 1 . 372E-02 1 . 793E+00 9.11 3E-01 9.179E-03 3.577E-01 -0.059 0.090 0.083

1 .0000 1 .71 5E+00 1 .512E-02 1 .731 E+00 9 . 688E-0

1

9 . 587E-03 9.292E-01 -0.056 0.086 0.078

1 .2500 1 . 6 97E+00 1 . 882E-02 1 .715E+00 6. 191E-01 5.639E-03 5.890E-01 -0.099 0.078 0.069

1 .5000 1 .691 E+00 2 . 279E-02 1 . 71 9E+00 7.599E-01 6.721 E-0 3 7 . 33 1 E-0

1

-0.095 0.072 0 .062

1 .7500 1 . 691 E+00 2.695E-02 1 . 7 1 8E+00 9.057E-01 7.830E-03 3.71 9E-01 -0.092 0.067 0.057 2.0000 1 . 695E+00 3.129E-02 1 .726E+00 1 . 051 E+00 8.969E-03 9. 997E-01 -0.039 0.063 0.053

2.5000 1 .706E+00 9.091E-02 1 . 797E+00 1 .339E+00 1 . 1 30E-02 1 . 230E+00 -0.036 0.058 0.097

3.0000 1 .71 9E+00 9. 999E-02 1 . 76 9E + 00 1 . 623E+00 1 . 36 9E-02 1 . 932E+00 -0.033 0.053 0.093

3.5000 1 . 733E+00 5 . 995E-02 1 . 793E+00 1 . 909E+00 1 .619E-02 1 .61 2E+00 -0.032 0.050 0.090 9.0000 1 . 795E+00 7 . 022E-02 1 .81 6E+00 2.181 E+00 1 . 86 3E-02 1 .773E+00 -0.030 0.098 0.037

9.5000 1 . 757E+00 8 . 077E-02 1 . 838E+00 2 . 955E+00 2.11 5E-02 1 . 920E + 00 -0.029 0.095 0.035 5.0000 1 . 768E+00 9. 156E-02 1 . 860E+00 2 . 725E+00 2.370 E-0 2 2 . 0 59E + 0 0 -0.028 0.099 0.039

5.5000 1 . 77 9E+00 1 .026E-01 1.881 E+00 2. 993E+00 2 . 626E-02 2 . 1 79E+00 -0.027 0.092 0.032

6.0000 1 . 788E+00 1 . 1 38E-01 1 . 902E+00 3 . 257E+00 2 . 883E-02 2.299E+00 -0.026 0.091 0.031 7.0000 1 . 806E+00 1 . 367E-0

1

1 . 992E+0 0 3 . 777E+00 3 . 90 1 E-0 2 2 . 509E+00 -0 .029 0.038 0.029

8.0000 1 .821 E+00 1 .601 E-01 1 . 981 E+00 9 . 287E+00 3.921 E-02 2.692E+00 -0.023 0.036 0.027

9.0000 1 .839E+00 1 .891E-01 2.01 8E+00 9 . 787E+00 9.992E-02 2 . 862E + 0 0 -0.021 0.035 0.026

10.0000 1 .896E+00 2.089E-01 2 . 059E+00 5 . 278E+00 9. 961 E-02 3.01 7E+00 -0 .020 0.033 0.029

12.5000 1 . 870 E+00 2.708E-01 2.191 E+00 6 . 970E+00 6 . 250E-02 3 . 359E+00 -0.017 0.030 0.021 15.0000 1 . 890E+00 3.398E-01 2 . 225E+00 7 .61 5E+00 7.51 8E-02 3 . 650E+00 -0.019 0 .028 0.019

17.5000 1 . 906E+00 9.002E-01 2 . 306E+00 8.71 9E+00 8 .759E-02 3. 905E+00 -0.012 0.025 0.017 20.0000 1 . 920 E+OO 9.665E-01 2 . 386E+00 9 . 789E+00 9 . 972E-02 9. 1 31 E+00 -0.011 0.029 0.015

25.0000 1 . 992E+00 6.019E-01 2 . 593E+00 1 . 181E+01 1 . 230 E-0

1

9 . 522E+0 0 -0.003 0.021 0.012

30.0000 1 . 959E+00 7 . 385E-0

1

2 . 6 98E+00 1 . 372E+0

1

1 . 95 1 E-0

1

9.850E+00 -0.007 0.019 0.010 35.0000 1 . 973E+00 3.779E-01 2.851 E+00 1 . 552E+0

1

1 . 659E-0

1

5 . 1 33E+00 -0.005 0.017 0.009

90.0000 1 . 986E+00 1 . 0 1 8E+00 3 . 003E+00 1 . 723E+0

1

1 . 856 E-0

1

5 . 381 E+00 -0.005 0.016 0.008

95.0000 1 . 996E+00 1 . 1 59E+00 3 . 1 55E+00 1 . 886E+0

1

2 . 093E-0

1

5 . 602E+00 -0 .009 0.015 0 .007

50 .0000 2 . 006E+00 1 . 30 1 E+OO 3 . 307E+00 2.090E+01 2.21 9E-01 5.802E+00 -0.009 0.019 0 .006 55.0000 2.01 9E+00 1 . 999E+00 3 . 958E+00 2. 188E+01 2.386E-01 5 . 983E+00 -0.003 0.013 0 .005 60.0000 2 . 022E+00 1 . 588E+00 3.61 0E+00 2.330E+01 2. 595E-01 6 . 1 50E+00 -0.003 0.012 0.005

70.0000 2 . 035E+00 1 . 878E+00 3. 91 3E+00 2.596E+01 2.839E-01 6 . 997E+00 -0.002 0.011 0.009

80.0000 2 . 096E+00 2.169E+00 9.21 6E+00 2 . 892E+0

1

3. 1 06E-01 6 . 705E+00 -0.002 0.010 0.003

90.0000 2 . 056E+00 2.962E+00 9 .51 9E+00 3.071 E+0

1

3.350E-01 6 . 939E+00 -0.002 0.010 0.003

1 00.0000 2 . 065E+00 2 . 757E+00 9 . 822E+00 3 . 285E+0

1

3.579E-01 7. 1 39E+00 -0.002 0.009 0.003

1 25.0000 2 . 089E+00 3 . 997E+00 5 . 582E+00 3 . 767E+0

1

9.060E-01 7 . 576E+00 -0.001 0 .008 0.002

1 50.0000 2.099E+00 9 . 293E+00 6 . 393E+00 9. 187E+01 9.969E-01 7. 939E+00 -0.001 0.007 0.002

175.0000 2.11 2E+00 9 . 993E+00 7.105E+00 9 . 559E+0

1

9 . 807E-0

1

8 . 233E+00 -0.001 0.007 0.001 200.0000 2. 123E+00 5 . 795E+00 7 .868E+00 9.893E+01 5. 102E-01 8 . 502E+0 0 -0.001 0.006 0.001 250.0000 2.192E+00 7 . 256E+00 9 . 398E+00 5 . 979E+0

1

5.586E-01 8. 999E+00 -0.001 0.006 0.001 300.0000 2 . 1 57E+00 8 . 779E+00 1 . 0 93E+0

1

5 . 967E+0

1

5.969E-01 9 . 306E+00 -0 .000 0.005 0.001 350.0000 2.16 9E+00 1 . 030E+0

1

1 . 297E+0

1

6 . 395E+0

1

6 . 280 E-0

1

9 . 61 2E+00 -0.000 0.005 3.001 900.0000 2.180E+00 1 . 182E+01 1 .900E+01 6 . 773E+0

1

6.590E-01 9 . 878E+00 -0.000 0 .005 0.001 950.0000 2.1 90E+00 1 . 335E+0

1

1 . 559E+0

1

7. 112E+Q1 6 . 76 0 E-0

1

1 .01 1E+01 -0.000 0.009 0.001 500.0000 2. 1 98E+00 1 . 988E+0

1

1 . 708E+01 7.918E+01 6 . 999E-01 1 . 0 32E + 0

1

-0.000 0.009 0.000 550.0000 2 . 206 E + 00 1 . 692E+0

1

1 -862E+01 7.699E+01 7.11 9E-01 1 .051 E+0

1

-0.000 0.009 0.000 600.0000 2.21 3E+00 1 . 7 95E + 0

1

2.016E+01 7 . 957E+01 7.260E-01 1 . 069E+01 -0.000 0 .009 0 .000 700.0000 2 . 226E+00 2. 102E+01 2 . 325E+0

1

8.918E+01 7.505E-01 1 . 0 99E + 0

1

-0.000 0 .009 0 .000 800.0000 2 . 237E+00 2.910E+01 2. 639E+01 8 . 822E+0

1

7.709E-01 1 . 1 26 E+0

1

-0.000 0.003 0.000 900.0000 2 . 296E+00 2.71SE+01 2.993E+01 9.181 E+0

1

7.870E-01 1 . 1 50 E+0

1

-0.000 0.003 0.000 1000.0000 2 . 255E+00 3 . 026E+0

1

3 . 252E+0

1

9 . 509E+0

1

8.010E-01 1 . 171E+01 -0.000 0.003 0.000

11
ELECTRONS IN BONE, COMPACT (ICRU)

I = 91.9 eV DENSITY = 1 . 850 E+0 0i g/cm 3

ENERGY STOPPING POWER C5DA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV csn 2 /g MeV cm 2 /g g/cm 2 0.0100 2 . 068E+O1 9.793E-03 2 . 068E+0

1

2.761E-09 1 .236E-09 0 .

0

-0.207 0.239 0.236 0.0125 1 . 792E+0

1

9.880E-03 1 . 792E+0

1

9. 039E-09 1 .501E-09 0.0 -0.198 0.227 0.229

0.0150 1 .519E+01 9. 992E-03 1 .519E+01 5.623E-09 1 . 756E-09 0.0 -0.191 0.218 0.216 0.0175 1 . 399E+0

1

9. 989E-03 1 . 395E+0

1

7 . 383E-09 2.009E-09 0.0 -0.186 0.211 0.209

0.0200 1 .21 3E+01 5.026E-03 1 .21 9E+01 9 . 393E-09 2.299E-09 0 . 0 -0.182 0 . 205 0.203

0.0250 1 . 023E+01 5 . 0S0E-03 1 . 029E+0

1

1 . 38 5E-0 3 2 . 706E-09 0.0 -0.175 0.196 0.195

0.0300 8 . 91 2E+00 5 . 1 21 E-03 3.91 7E+00 1 . 91 0E-03 3.198E-09 0.0 -0.169 0.190 0.188

0.0350 7 . 939E+00 5.1 55E-03 7 . 999E+00 2.505E-03 3 . 572E-09 0.0 -0.165 0.139 0.183

0 .0400 7. 1 90E+00 5 . 1 89E-03 7 . 1 96E+00 3.163E-03 3. 982E-09 0.0 -0.162 0.180 0.179

0 .0450 6 .596E+00 5.21 IE-03 6 .601 E+00 3.899E-03 9. 379E-09 0.0 -0.159 0.176 0.175

0.0500 6.11 2E+00 5 . 237E-03 6.11 7E+00 9.682E-03 9.769E-09 0.0 -0.156 0.173 0.172

0.0550 5 . 70 9E+00 5.263E-03 5.71 5E+00 5.528E-03 5 . 1 39E-09 0.0 -0.159 0.170 0.170 0.0600 5 . 370E+00 5.288E-03 5 . 375E+00 6 . 931 E-03 5.509E-09 0.0 -0.152 0.168 0.167

0.0700 9 . 827E+00 5.338E-03 9 . 832E+00 3.397E-03 6.210E-09 0.0 -0.199 0.169 0.163

0.0800 9.91 2E + 0 0 5 . 390E-03 9.91 7E+00 1 . 056E-02 6 .887E-09 0.0 -0.196 0.160 0.160 0.0900 9 . 085E + 00 5 . 995E-0 3 9 . 090E+00 1 . 292E-02 7 . 590E-09 0.0 -0.199 0.158 0.157 0.1000 3 . 820E+00 5.502E-03 3 . 825E+00 1 . 595E-02 8.171E-09 0.0 -0.192 0.155 0.155

0.1250 3 . 336E+00 5 . 657E-03 3 . 392E+00 2.297E-02 9.670E-09 0.0 -0.138 0.150 0.150 0.1500 3.01 0E+00 5.826E-03 3.01 5E+00 3.037E-02 1 . 108E-03 0 .

0

-0.135 0.197 0.196 0.1750 2 . 775E+00 6 . 007E-03 2.781 E+00 3.901E-02 1 . 292E-03 0.0 -0.132 0.193 0.193

0.2000 2.599E+00 6 . 200E-03 2 . 605E+00 9.832E-02 1 .371E-03 0.0 -0.130 0.191 0.190 0.2500 2.359E+00 6.618E-03 2.361 E+00 6 . 855E-02 1 .61 5E-03 0 .

0

-0.126 0 . 1 37 0.136 0.3000 2.1 99E+00 7.075E-03 2.201 E+00 9.053E-02 1 . 898E-0 3 0.0 -0.118 0.139 0.133

0.3500 2.079E+00 7 . 567E-03 2 . 087E+00 1 . 1 39E-01 2.072E-03 2.893E-02 -0.096 0.127 0.126

0 .9000 1 . 996E+00 8.090E-03 2.009E+00 1 .389E-01 2 . 292E-03 6 . 250 E-0 2 -0.089 0.121 0.119

0 . 9500 1 . 932E+00 8.693E-03 1 . 991 E+00 1 . 6 37E-0

1

2.509E-03 9.798E-02 -0.089 0.116 0.112

0.5000 1 . 88 3E+0 0 9.221 E-03 1 . 8 9 3E+0 0 1 .898E-01 2.729E-03 1 . 392E-0

1

-0.079 0.111 0.107 0.5500 1 . 895E+00 9.823E-03 1 . 855E+00 2. 165E-01 2. 939E-03 1 .710 E-0

1

-0.075 0.107 0.102

0.6000 1 .81 5E+00 1 . 095E-02 1 . 825E+00 2.937E-01 3. 153E-03 2.079E-01 -0.071 0.103 0.098

0.7000 1 . 770E+00 1 . 1 75E-02 1 . 782E+00 2. 992E-01 3 . 582E-03 2.817E-01 -0.066 0.096 0.091 0.8000 1 .790E+00 1 .31 IE-02 1 . 753E+00 3 . 558E-0

1

9.019E-03 3.598E-01 -0.061 0.091 0.089

0 . 9000 1 . 7 1 9E+00 1 . 959E-02 1 . 739E+00 9.1 32E-01 9.999E-03 9.265E-01 -0.057 0.086 0.079

1 . 0000 1 . 705E+00 1 . 602E-02 1 .721 E+00 9.71 IE-01 9.839E-03 9. 969E-01 -0.059 0.083 0.075

1 .2500 1 . 686E+00 1 . 995E-02 1 . 70 6 E+0 0 6. 171E-01 6 . 009E-03 6 . 6 26 E-0

1

-0.098 0.075 0.066

1 .5000 1 . 630E+00 2.919E-02 1 . 70 5E+00 7.638E-01 7.161 E-03 8.160E-01 -0.099 0.069 0.060

1 .7500 1 .681E+00 2.859E-02 1 . 709E+00 9 . 1 03E-01 8.391 E-03 9.575E-01 -0.091 0.065 0.055 2.0000 1 . 639E+00 3.31 3E-02 1 . 7 1 8E+00 1 . 056E+00 9 . 597E-03 1 . 088E+00 -0.039 0.061 0.051 2.5000 1 .696E+00 9 . 277E-02 1 . 739E+00 1 . 396 E+00 1 . 202E-02 1 . 323E+00 -0.035 0.056 0.096 3.0000 1 .709E+00 5.289E-02 1 . 762E+00 1 .631 E+00 1 . 957E-02 1 . 527E+00 -0.033 0.052 0.092

3.5000 1 . 722E+00 6.391E-02 1 . 786E+00 1 . 91 3E+00 1 .717E-02 1 .709E+00 -0.031 0.099 0.039 9.0000 1 . 735E+00 7.927E-02 1 . 80 9E+00 2 . 1 9 1 E+00 1 . 981 E-02 1 . 872E+0 0 -0.030 0.096 0.037 9.5000 1 . 797E+00 8.591E-02 1 . 832E+00 2 . 966 E + 00 2.298E-02 2.020E+00 -0 . 029 0.099 0.035

5.0000 1 . 758E+00 9 . 630E-02 1 . 855E+00 2 . 7 37E+0 0 2.51 7E-02 2 . 1 56 E+00 -0.027 0.093 0.033

5.5000 1 . 768E+00 1 . 089E-0

1

1 .877E+00 3.005E+00 2.788E-02 2 . 282E+00 -0.026 0.091 0.032

6.0000 1 . 778E+00 1 . 202E-0

1

1 . 898E+00 3 . 270E+00 3 . 060E-02 2. 399E+00 -0.025 0.090 0.031 7.0000 1 . 7 95E + 00 1 .999E-01 1 . 939E+00 3 . 7 9 1 E + 00 3.607E-02 2.61 1 E + 0 0 -0.029 0.037 0.028 8.0000 1 .81 OE+OO 1 .692E-01 1 . 979E+00 9.301 E+00 9.156E-02 2.801 E+00 -0.022 0.035 0.027

9.0000 1 .823E+00 1 . 995E-0

1

2.018E+00 9 . 802E+0 0 9.705E-02 2. 972E+00 -0.021 0.039 0.025

1 0.0000 1 . 835E+00 2 . 202E-0

1

2 . 055E+00 5.293E+00 5 . 252E-02 3. 1 29E+00 -0.019 0.032 0.029

12.5000 1 . 36 OE+OO 2.860E-01 2. 196E+00 6 . 983E+00 6 . 608E-02 3 . 973E+00 -0.017 0.029 0.021 15.0000 1 . 879E+00 3.537E-01 2 . 233E+00 7 . 625E+00 7. 939E-02 3 . 765E+00 -0.019 0.027 0.019

17.5000 1 .896E+00 9.226E-01 2.318E+00 8 . 729E+00 9 . 290E-02 9.021 E+00 -0.012 0.025 0.017 20.0000 1 . 909E+00 9.926E-01 2 . 902E+00 9 . 783E+00 1 .051 E-01 9 . 297E+00 -0.011 0.023 0.015 25.0000 1 . 931 E+00 6.351E-01 2 . 56 6 E+0 0 1 . 180E+0! 1 .299E-01 9 . 637E+00 -0.008 0.021 0.012 30.0000 1 . 999E+00 7.799E-01 2 . 729E+00 1 .369E+01 1 . 523E-0

1

9. 965E+00 -0.007 0.018 0.010 35.0000 1 . 963E+00 9.269E-01 2 . 8 90E + 0 0 1 . 597E+0

1

1 .739E-01 5 . 297E+00 -0.006 0.017 0.009 90.0000 1 . 976E+00 1 . 079E+00 3 . 050E+00 1 .715E+01 1 . 993E-01 5 . 995E+00 -0.005 0.016 0.008 95.0000 1 . 986E+00 1 . 229E+00 3.21 OE+OO 1 . 875E+0

1

2.1 39E-01 5 . 7 1 6 E+00 -0.009 0.019 0.007

50 .0000 1 . 996E+00 1 . 379E+00 3.369E+00 2 . 027E+0

1

2.316E-01 5. 915E+00 -0 .009 0.019 0.006 55.0000 2 . 009E+00 1 . 525E+00 3.529E+00 2. 172E+01 2.987E-01 6 . 097E+00 -0.003 0.013 0.005 60.0000 2.01 2E+00 1 . 676E+00 3 . 688E+00 2.31 0E+01 2.699E-01 6 . 2S3E+00 -0.003 0.012 0.005 70.0000 2 . 025E+00 1 . 982E+00 9 . 007E+00 2.570E+01 2.999E-01 6 . 559E+00 -0 .003 0.011 0.009 80.0000 2.037E+00 2.289E+00 9 . 326E+00 2.811 E+0

1

3.221E-01 6 .81 7E+O0 -0.002 0.010 0.009 90.0000 2 . 097E+00 2 . 598E+00 9 . 695E+00 3 . 039E+0

1

3.968E-01 7 . 096E+00 -0 .002 0.010 0.003

100.0000 2 . 056E+00 2. 909E+00 9. 965E+00 3 . 292E+0

1

3.699E-01 7.251 E+00 -0.002 0.009 0.003 125.0000 2 . 075E+00 3 . 6 90E+00 5 . 765E + 0 0 3.709E+01 9. 189E-01 7 . 688E+00 -0.001 0 .008 0.002

150.0000 2 . 0 90 E+OO 9 . 976E+00 6 . 566E+00 9.11 5E+01 9.590E-01 8 . 096E+00 -0.001 0.007 0 .002 175.0000 2. 103E+00 5 . 266E+00 7 . 369E+00 9 . 979E+0

1

9 . 932E-01 8 . 350E+00 -0.001 0.007 0.001 200.0000 2.11 9E+00 6 . 059E+00 8 . 1 73E+00 9.796E+01 5.226E-01 8.61 9E+00 -0.001 0.006 0.001 250.0000 2.1 33E+00 7 . 652E+00 9 . 789E+00 5 . 359E+0

1

5.707E-01 9 . 057E+00 -0.001 0.006 0.001 300.0000 2 . 1 98E+00 9.251 E+00 1 . 1 90E+01 5 . 827E+0

1

6.085E-01 9.91 9E+00 -0.000 0.005 0.001 350.0000 2.1 60E+00 1 . 036E+0

1

1 . 302E+0

1

6 . 238E+0

1

6 . 392E-0

1

9 . 726E+00 -0.000 0.005 0.001 900.0000 2 . 1 7 1 E+00 1 . 296E+0

1

1 . 969E+01 6 . 600 E + 0

1

6 . 697E-01 9.991 E+00 -0.000 0.005 0.001 950.0000 2.181 E+00 1 . 907E+0

1

1 . 626E+0

1

6.929E+01 6 .853E-01 1 . 023E+01 -0.000 0.009 0.001 500.0000 2. 189E+00 1 .569E+01 1 . 788E+0

1

7.217E+01 7.098E-01 1 . 099E+0

1

-0.000 0.009 0.000 550.0000 2.1 97E+00 1 . 730E+0

1

1 . 950E+01 7 . 985E+0

1

7.210E-01 1 . 063E+0

1

-0.000 0.009 0.000 600.0000 2 . 209E+00 1 . 892E+0

1

2. 1 12E+01 7 .731 E+01 7.352E-01 1 . 080E+0

1

-0.000 0.009 0.000 700.0000 2.21 7E+00 2.21 6 E+O 1 2 . 937E+0

1

8 . 1 7 1 E+0

1

7.591 E-0

1

1 . 1 1 1 E+0

1

-0.000 0.009 0.000 800.0000 2 . 228E+00 2.590E+01 2.763E+01 8 . 556E+0

1

7.785E-01 1 .137E+01 -0.000 0.009 0.000 900.0000 2 . 237E+00 2 . 869E+0

1

3 . 038E+01 8 . 898E+0

1

7. 997E-01 1 . 1 6 1 E+0

1

-0.000 0.003 0.000 1000.0000 2 . 296 E+0 0 3. 189E+01 3.91 9E+01 9 . 206E+0

1

8 . 083E-0

1

1 . 182E+01 -0.000 0.003 0.000

113
ELECTRONS IN BONE, CORTICAL (ICRP)

I = 106. A eV DENSITY = 1 . 850E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DEHS.EFF. d( log1 )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD COP.R. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 1 .971E+01 5. A61E-03 1 . 972E+01 2. 909E-0A 1 . A68E-0A 0.0 -0.21A 0.2A8 0.2AA 0.0125 1 . 663E+0

1

5.579E-03 1 . 66AE+0

1

A.295E-0A 1 .787E-0A 0.0 -0.20A 0.235 0 . 232 0.0150 1 . AA7E+0

1

5.66AE-03 1 . AA7E+01 5.911E-0A 2.095E-0A 0.0 -0.197 0 . 226 0 . 223 0.0175 1 . 286E+0

1

5.728E-03 1 . 287E + 0

1

7.7A7E-0A 2.393E-0A 0.0 -0.191 0.213 0.216

0.0200 1 .161E+01 5 . 778E-03 1 . 162E+01 9.795E-0A 2 . 683E-0

A

0.0 -0.187 0.212 0.210

0.0250 9.80AE+00 5.853E-03 9.81 OE+OO 1 . A50E-03 3.2A2E-0A 0.0 -0.179 0.202 0.200 0.0300 8 . 5A6E+00 5. 907E-03 3 . 552E+00 1 . 997E-03 3.775E-0A 0.0 -0 . 1 7A 0.195 0 . 1 9A 0.0350 7.618E+00 5.951E-03 7 . 62AE+00 2.618E-03 A . 287E-0

A

0 .

0

-0.169 0.190 0.188

0.0A00 6 . 903E+00 5. 989E-03 6 . 909E+00 3.308E-03 A.781E-0A 0.0 -0.166 0.185 0. ISA O.OA50 6 . 335E+00 6 . 022E-03 6 . 3A1 E+00 A.06AE-03 5.259E-0A 0.0 -0.163 0.181 0.180

0.0500 5 . 872E+00 6.05AE-03 5 .87 9E+00 A.38AE-03 5.723E-0A 0.0 -0.160 0.173 0.177

0.0550 5 . A88E+00 6.08AE-03 5. A9AE+00 5.76AE-03 6. 175E-0A 0.0 -0.158 0.175 0 . 1 7A 0.0600 5. 163E+00 6 . 1 13E-03 5. 169E+00 6.703E-03 6.61AE-0A 0.0 -0.156 0.172 0.171 0.0700 A . 6A3E+00 6.171E-03 A . 6 A 9E + 0 0 8.7A8E-03 7.A63E-0A 0.0 -0.152 0.168 0.167

0.0800 A.2A6E+00 6 . 230E-03 A . 252E+00 1 . 1 00E-02 8.276E-0A 0.0 -0.1A9 0 . 1 6A 0 . 1 6 A 0.0900 3 . 932E+00 6 . 292E-0 3 3 . 939E+00 1 . 3A5E-02 9 . 059E-0A 0.0 -0. 1 A7 0.161 0.161 0.1000 3 . 678E+00 6.356E-03 3 . 635E+00 1 . 607E-02 9.81 AE-OA 0.0 -0.1A5 0.159 0.158

0.1250 3.21 5E+00 6 .530E-03 3.221 E+00 2.336E-02 1 .161 E— 0 3 0.0 -0.1A1 0 . 1 5A 0.153

0.1500 2.901 E+00 6 .71 9E-03 2. 908E+00 3. 155E-02 1 . 329E-03 0.0 -0.137 0.150 0 . 1 A9 0.1750 2 . 676E+00 6 . 923E-03 2 . 633E+00 A .051 E-02 1 . A39E-03 0.0 -0.1 3A 0.1A7 0.1A6 0.2000 2 . 507E+00 7 . 1 A0E-03 2.51 AE+OO 5.01 5E-02 1 .SA1E-03 0.0 -0.132 0.1 AA 0.1A3

0.2500 2 . 272E+00 7.612E-03 2 . 280E+00 7.11 IE-02 1 . 931 E-03 0.0 -0.128 0.1 AO 0.139

0 . 3000 2.11 9E+00 8. 129E-03 2. 127E+00 9 . 386E-02 2.206E-03 0.0 -0.125 0.137 0.136 0.3500 2.01 1E+00 8 . 685E-03 2 . 020E+00 1 . 180E-01 2.A71E-03 8. 920E-03 -0.105 0.133 0.131 0.A000 1 . 931 E+OO 9.276E-03 1 . 9A1 E+00 1 .A33E-01 2.730E-03 3 . A 1 IE-02 -0.098 0.127 0.125

0 . 4500 1 .871 E+00 9.901E-03 1 . 88 1 E+00 1 .695E-01 2. 93AE-03 6 . 200E-02 -0.092 0.122 0.119

0.5000 1 . 825E+00 1 . 055E-02 1 . 836E+00 1 . 96AE-01 3 . 236E-03 9.1A6E-02 -0.087 0.118 0. 1 1 A 0.5500 1 . 789E+00 1 . 12AE-02 1 . 800E+00 2.239E-01 3.A87E-03 1 .21 9E-01 -0.083 0.113 0.109

0.6000 1 . 760E+00 1 . 1 9AE-02 1 . 772E+00 2.51 9E-01 3.737E-03 1 . 531 E-0

1

-0.079 0.110 0.105

0.7000 1 . 7 1 8E+00 1 .3A1E-02 1 . 732E+00 3.090E-01 A . 237E-0 3 2.166 E-0

1

-0.073 0.103 0.093

0.8000 1 . 6 90E + 00 1 .A95E-02 1 . 705E+00 3.673E-01 A.7A0E-03 2 . 80 6 E-0

1

-0.068 0.098 0.092

0.9000 1 .671 E+00 1 . 657E-02 1 . 688E+00 A.262E-01 5 . 2A5E-03 3. AA2E-01 -0.063 0.093 0.086

1 .0000 1 . 658E+00 1 . 82AE-02 1 . 677E+00 A . 857E-0

1

5.755E-03 A.069E-01 -0.060 0.089 0.082

1 .2500 1 . 6 A2E+00 2.267E-02 1 . 665E+00 6 . 35AE-0

1

7 . 052E-03 5 . 580 E-0

1

-0.053 0.082 0.073

1 .5000 1 . 637E+00 2.7A0E-02 1 . 665E+00 7.857E-01 8.382E-03 6.99AE-01 -0 .0A9 0.076 0.066

1 .7500 1 . 6 3 9E+00 3.237E-02 1 .671 E+00 9 . 356E-0

1

9.7A3E-03 3.310 E-0

1

-0 .0A5 0.071 0.061 2.0000 1 . 6A3E+00 3 . 755E-02 1 .681 E+00 1 . 085E+00 1.11 3E-02 9.53AE-01 -0 . 0A3 0.067 0.057 2.5000 1 . 656E+00 A.8A0E-02 1 . 70AE+00 1 . 380E+00 1 . 398E-02 1 . 1 7AE+00 -0.039 0.061 0.051 3.0000 1 . 670E+00 5.981E-02 1 . 7 30 E + 0 0 1 .671 E+00 1 . 689E-02 1 . 368E+00 -0 .036 0 . 057 0.0A6 3.5000 1 . 68 AE+OO 7.165E-02 1 . 755E+00 1 . 958E+00 1 .987E-02 1 . 5A1 E+00 -0.03A 0 .05A 0 .0A3

A. 0000 1 . 697E+00 8.386E-02 1 .781 E+OO 2.2A1E+00 2 . 288E-02 1 . 6 97E+00 -0.033 0.051 O.OAO

A. 5000 1 . 709E+00 9 . 638E-02 1 . 80 5E+0 0 2 . 520E+00 2 . 592E-02 1 . 839E+00 -0.031 0 . 0A9 0.038

5.0000 1 . 720E+00 1 .092E-01 1 . 829E+00 2 . 7 95E + 0 0 2 . 398E-02 1 . 97 OE + OO -0.030 0.0A7 0.036 5.5000 1 .731 E+00 1 . 222E-0

1

1 . 853E+00 3 . 067E+00 3 . 206E-02 2.091 E+00 -0.029 0 .0A5 0.035

6.0000 1 . 7A0E+00 1 . 355E-01 1 . 87 6 E+0 0 3 . 335E+00 3.51 AE-02 2.203E+00 -0.028 0 . 0 A A 0 .033 7.0000 1 . 758E+00 1 . 626E-01 1 . 921 E+00 3.862E+00 A. 133E-02 2 . A08E+00 -0.026 0 . 0 A

1

0.031 8.0000 1 . 773E+00 1 . 90AE-01 1 . 96 AE+OO A . 377E+00 A . 752E-02 2.591 E+00 -0.025 0.039 0.029

9.0000 1 . 787E+00 2. 188E-01 2 . 006E+00 A . 880 E + 00 5.369E-02 2 . 757E+00 -0.023 0.037 0.028

10.0000 1 . 799E+00 2.A76E-01 2 . 0 A6E + 00 5 . 37AE+00 5. 983E-02 2 . 908E+00 -0.022 0.036 0.026 12.5000 1 . 82AE+00 3.21AE-01 2.1 A5E+00 6 . 567E+00 7.A97E-02 3 . 2 A 1 E+0 0 -0.019 0.032 0.023

15.0000 1 . 8AAE+00 3.971E-01 2.2A1E+00 7 . 707E+00 8.97AE-02 3 . 525E+00 -0.016 0.030 0.020

17.5000 1 . 860E+00 A . 7A2E-0

1

2. 335E+00 8 . 80 0 E+0 0 1 .0A1E-01 3 . 773E+00 -0 .01 A 0.028 0.018

20.0000 1 . 87 AE+OO 5 . 525E-01 2. A27E+00 9 . 850E+00 1 . 180E-01 3 . 99AE+00 -0.013 0.026 0.017 25.0000 1 . 8 97E+0 0 7.1 17E-01 2 . 609E+00 1 . 18AE+0! 1 . AA6E-01 A . 375E+00 -0.010 0.023 0 . 0 1 A 30.0000 1 . 91 5E + 00 8.735E-01 2 . 788E+0 0 1 . 369E+0

1

1 .69AE-01 A . 6 96 E+0 0 -0.003 0.021 0.012

35.0000 1 . 929E + 00 1 . 0 37E+00 2. 966E+00 1 . 5 A3E+0

1

1 . 926E-0

1

A. 973E+00 -0.007 0.019 0.010

AO. 0000 1 . 9A2E+00 1 .202E+00 3. 1 AAE+OO 1 . 707E+0

1

2.1A3E-01 5.217E+00 -0.006 0.017 0.009

A5.0000 1 . 952E + 00 1 . 36 9E+00 3 . 32 1 E+00 1 .861 E+0

1

2.3A7E-01 5. A3AE+00 -0.005 0.016 0.008 50.0000 1 . 962E+00 1 . 537E+00 3. A98E+00 2 . 008E+0

1

2.538E-01 5.631 E+00 -0.005 0.015 0.007

55.0000 1 . 970E + 00 1 . 705E+00 3 . 676E+00 2.1A7E+01 2.718E-01 5.81 OE+OO -0.00A 0 . 0 1 A 0 .006 60.0000 1 . 978E+00 1 . 875E+00 3 . 353E+00 2 . 280E+0

1

2.888E-01 5 . 97AE+00 -0 . 00 A 0 . 01 A 0.006 70.0000 1 . 992E+00 2.21 5E+00 A . 207E+00 2.529E+01 3.1 99E-01 6 . 267E + 00 -0.003 0.013 0.005 80.0000 2.003E+00 2 . 558E+00 A . 56 1 E+00 2 . 757E+0

1

3. A80E-01 6 . 523E + 00 -0.003 0.012 0 .OOA 90.0000 2.01 3E+00 2 . 903E+00 A.916E+00 2. 968E+01 3.733E-01 6.7A9E+00 -0.003 0.011 0 . 00 A 100.0000 2 . 022E+00 3 . 2A9E+00 5 . 272E+00 3.16AE+01 3.96AE-01 6 . 953E+00 -0.002 0.010 0.003

125.0000 2 . 0 A 1 E + 00 A . 1 20E+00 6 . 1 61 E+00 3 . 602E+C

1

A. A59E-01 7 . 387E + 00 -0.002 0.009 0.003

150.0000 2 . 056 E + 00 A. 997E+00 7 . 053E+00 3 . 98 1 E+0

1

A.865E-01 7 . 7A3E+00 -0.001 0.008 0.002

175.0000 2.069E+00 5 . 878E+00 7 . 9A7E+00 A.315E+01 5.205E-01 8.0A6E+00 -0.001 0.008 0.002 200.0000 2 . 080E + 00 6 . 762E+00 8 . 8A2E + 00 A. 61 3E+01 5. A95E-01 8 . 309E+00 -0.001 0.007 0.002 250.0000 2.093E+00 3 . 537E+00 1 . 06AE+0

1

5. 128E+01 5.966E-01 8 . 7 50E+0 0 -0.001 0.007 0.001 300.0000 2.11 3E+00 1 . 0 32E+0

1

1 . 2A3E+0

1

5 . 563E+0

1

6.333E-01 9.11 1 E+00 -0.001 0.006 0.001 350.0000 2 . 1 26E+00 1 .21 1 E+01 1 . A23E+01 5. 938E+01 6.630E-01 9.A17E+00 -0.000 0.006 0.001 A00.0000 2.136E+00 1 . 390E+0

1

1 .60AE+01 6.269E+01 6 . 875E-0

1

9 . 683E+00 -0.000 0.005 0.001

A50 .0000 2.1 A6E+00 1 .569E+01 1 . 78AE+0

1

6 .56AE+01 7.081 E-0

1

9.917 E+00 -0.000 0.005 0.001 500.0000 2 . 1 5AE + 00 1 .7A9E+01 1 .96AE+01 6.831 E+0

1

7.258E-01 1 .01 3E+01 -0 .000 0.005 0.001 550.0000 2.162E+00 1 . 929E+01 2.1A5E+01 7 . 075E+0

1

7.A12E-01 1 . 0 32E + 0

1

-0.000 0.005 0.001 600.0000 2.169E+00 2. 109E+01 2 . 326E+0

1

7 . 299E+0

1

7.5A7E-01 1 .0A9E+O1 -0.000 0.005 0.000

700 .0000 2. 131 E+00 2. A70E+01 2 . 688E+0

1

7 . 6 98E+0

1

7.773E-01 1 . 080 E+0

1

-0.000 0 . OOA 0 .000 800.0000 2.1 92E+00 2.831 E+0

1

3 . 050E+0

1

8 . OA7E+0

1

7 . 956E-01 1 . 1 07E+01 -o.ooo 0 .OOA 0.000

900 .0000 2 . 202E + 00 3.192E+01 3.A12E+01 8 . 357E+0

1

8. 108E-01 1 . 1 30 E + 0

1

- 0.000 0 .OOA 0.000 1000.0000 2.21 OE+OO 3 . 553E+0

1

3 . 77AE+0

1

8.636E+01 8.235E-01 1 .151 E+01 -0 .000 0 .OOA 0.000

114
ELECTRONS IN C-552 AIR-EQUIVALENT PLASTIC

I = 86.8 eV DENSITY = 1 . 760E+00 g/cra 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. cKlog )/d(loqI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2 /g g/cm 2 O.OIOO 1 . 972E+01 3 . 767E-03 1 . 972E+01 2.890E-04 1 . 046E-04 0.0 -0.205 0 . 235 0.233 0.0125 1 .660E+01 3.794E-03 1 .661E + 01 4 . 277E-04 1 . 257E-04 0.0 -0.196 0.224 0.222

0.0150 1 . 442E+0

1

3.812E-03 1 . 443E+0

1

5 .397E-04 1 . 458E-04 0.0 -0.189 0.215 0.214 0.0175 1 .281E+01 3.824E-03 1 .281E+01 7 . 739E-04 1 .652E-04 0.0 -0.184 0.203 0.207

0.0200 1 . 156E+01 3.834E-03 1 . 1 56E+01 9.797E-04 1 .339E-04 0.0 -0.180 0.203 0.202

0.0250 9.741E+00 3 . 34SE-03 9 . 745E+00 1 . 453E-0 3 2. 1 99E-04 0.0 -0.173 0.194 0.193 0.0300 8 . 482E+00 3 . 860E-03 8 . 486 E+00 2.004E-03 2.541 E-04 0 .

0

-0.168 0.188 0.187 0.0350 7 . 554E+0 0 3.871E-03 7 . 55SE+0 0 2 . 630E-03 2.369E-04 0.0 -0.164 0.182 0.182

0.0400 6 .341 E+00 3.883E-03 6 . 845E+0 0 3 . 326 E-0 3 3 . 185E-04 0.0 -0.160 0.178 0.178

0 . 0450 6 . 274E+0 0 3 . 8 96E-0 3 6 . 278E+00 4.090E-03 3.491E-04 0.0 -0.158 0.174 0.174 0.0500 5.81 3E+00 3. 909E-03 5.816E+00 4.918E-03 3.789E-04 0.0 -0.155 0.171 0.171

0 .0550 5 . 429E+00 3. 924E-03 5 . 433E+00 5 . SO 9E-03 4.078E-04 0.0 -0.153 0.169 0.163 0.0600 5. 1 06E+00 3. 939E-03 5.110 E+00 6 . 758E-03 4 . 360E-04 0.0 -0.151 0.166 0.166 0.0700 4 . 589E+00 3 . 973E-03 4 . 593E+00 8 . 827E-0 3 4. 907E-04 0.0 -0.148 0.162 0.162

0.0800 4 . 1 94E+00 4.010E-03 4.1 98E+00 1.111 E-02 5.431 E-04 0 .

0

-0.145 0.159 0.159

0.0900 3 . 882E+00 4.050E-03 3 . 88 6 E+0 0 1 . 359E-02 5. 938E-04 0.0 -0.143 0.156 0.156 0.1000 3 . 630E+00 4.093E-03 3 . 634E+00 1 . 625E-02 6 . 429E-04 0 .

0

-0.141 0.154 0.153

0.1250 3.1 70E+00 4.214E-03 3. 174E+00 2 . 364E-02 7.599E-04 0.0 -0.137 0.149 0.149

0.1500 2.859E+00 4 . 347E-03 2 . 863E+00 3. 1 96E-02 8.705E-04 0.0 -0.133 0.145 0.145

0.1750 2 . 635E+00 4 . 490E-03 2 . 640E+00 4.107E-02 9 . 76 2E-0 4 0.0 -0.131 0.142 0.142

0.2000 2 . 468E + 0 0 4 . 643E-03 2 . 473E+00 5 . 086E-02 1 . 078E-03 0.0 -0.129 0.140 0.139

0.2500 2 . 235E+00 4.974E-03 2 . 240E+00 7.218E-02 1 . 272E-03 0.0 -0.125 0.136 0.135

0.3000 2 . 083E+00 5 . 336E-03 2 . 088E+00 9 . 535E-02 1 . 458E-0 3 0.0 -0.122 0.133 0.132

0.3500 1 . 977E+00 5 . 723E-03 1 . 983E+00 1 . 200E-0

1

1 . 639E-03 0.0 -0.121 0.130 0.129

0.4000 1 .899E+00 6.134E-03 1 . 906E+00 1 . 457E-0

1

1 .815E-03 1 . 229E-02 -0.097 0.127 0.125

0 . 4500 1 . 840E+00 6 . 567E-0 3 1 . 847E+00 1 . 724E-0

1

1 . 990E-03 3 . 896E-02 -0.091 0.122 0.119

0.5000 1 . 794E+00 7 . 020E-03 1 .80 1 E+00 1 . 998E-0

1

2. 164E-03 6.802E-02 -0.085 0.117 0.114

0.5500 1 . 758E+00 7 . 491 E-03 1 .765E+00 2.279E-01 2.337E-03 9.881 E-02 -0.080 0.113 0.109

0.6000 1 . 729E+00 7 . 977E-03 1 . 737E+00 2.564E-01 2.510E-03 1 . 308E-0

1

-0.076 0.109 0.104

0.7000 1 . 687E+00 8 . 995E-03 1 . 6 96E+00 3.147E-01 2.853E-03 1 . 972E-01 -0.069 0.102 0.096

0.8000 1 . 659E+00 1 . 006E-02 1 .669E+00 3.742E-01 3.209E-03 2.651 E-0

1

-0.063 0.096 0 .089

0 . 9000 1 . 639E+00 1 .1 18E-02 1 . 650E+00 4 . 345E-0

1

3 . 564E-03 3 . 33 1 E-0

1

-0.059 0.091 0.084

1 .0000 1 . 626E+00 1 . 234E-02 1 . 638E+00 4 . 953E-0

1

3. 923E-03 4 . 005E-0

1

-0.055 0.087 0.079

1 .2500 1 . 608E+00 1 . 542E-02 1 . 623E+00 6.488E-01 4 . 840 E-03 5 . 636E-0

1

-0.048 0.078 0.069

1 .5000 1 . 602E+00 1 .871E-02 1 . 620E+00 8 . 0 30 E-0

1

5 . 787E-03 7.163E-01 -0.043 0 .072 0.062

1 .7500 1 . 602E+00 2.218E-02 1 . 624E+0 0 9.572E-01 6 . 760E-03 8 . 594E-01 -0.040 0.067 0.056 2.0000 1 . 605E+00 2.531 E-02 1 . 630E+00 1.111 E+00 7 . 758E-0 3 9 . 920E-01 -0 .037 0.063 0.052

2.5000 1 .61 5E+00 3. 342E-02 1 . 648E+00 1 .41 6E+00 9.814E-03 1 .231 E+00 -0.034 0.057 0 .045 3.0000 1 . 627E+00 4.144E-02 1 . 668E+00 1 . 71 7E+00 1 . 1 94E-02 1 .441 E+00 -0.031 0.052 0.041 3.5000 1 . 639E+00 4.973E-02 1 . 689E+00 2.015E+00 1.411 E-02 1 . 627E+00 -0.029 0.049 0.038 4.0000 1 . 650E+00 5 . 840 E-02 1 .709E+00 2.31 0E+00 1 . 632E-02 1 . 794E+00 -0.028 0 .046 0 .035 4.5000 1 .661 E+00 6 . 726E-02 1 . 729E+00 2 . 6 0 1 E+0 0 1 . 857E-02 1 . 947E+00 -0.027 0.044 0.033

5.0000 1 .671 E+00 7.633E-02 1 . 748E+00 2.888E+00 2 . 084E-02 2 . 0S6E+00 -0.026 0.042 0 .032 5.5000 1 . 631 E+00 8 . 559E-02 1 .766E+00 3 . 1 73E+00 2.31 4E-02 2.21 5E+00 -0.025 0.041 0.030 6.0000 1 . 690E+00 9.501 E-02 1 . 785E+00 3 . 454E+00 2 . 544E-02 2. 335E+00 -0 .024 0.039 0.029

7.0000 1 . 705E+00 1 . 1 43E-0

1

1 . 820E+00 4 . 009E+00 3 . 01 OE-02 2 . 552E+00 -0.022 0.037 0.027 8.0000 1 .71 9E+00 1.341 E-0

1

1 . 853E+00 4 . 554E+00 3 . 478E-02 2 . 745E+00 -0.021 0 .035 0.025

9.0000 1 .731 E+00 1 . 543E-0

1

1 . 886 E + 00 5 . 089E+00 3. 948E-02 2. 920E+00 -0.020 0.033 0.024

1 0 . 0000 1 . 742E+00 1 . 748E-0

1

1 . 917E+00 5.61 4E+00 4.41 9E-02 3.0S0E+00 -0.018 0.032 0.023

12.5000 1 . 765E+00 2.275E-01 1 . 993E+00 6 .893E+00 5 . 5 90 E-0 2 3 . 428E+00 -0.016 0.029 0.020 15.0000 1 . 783E+00 2.817E-01 2 . 065E+00 8. 125E+00 6 . 748E-02 3 . 724E+00 -0.014 0.026 0.018 17.5000 1 . 7 9 9E+0 0 3.370 E-0

1

2 . 1 35E+00 9.31 6E+00 7.886E-02 3. 981 E+00 -0.012 0.024 0.016 20.0000 1.811 E+00 3.931 E-0

1

2 . 204E+00 1 . 047E+0

1

9.002E-02 4.21 0E+00 -0.010 0.023 0.014 25.0000 1 .832E+00 5.073E-01 2 . 339E+00 1 . 267E+0

1

1.11 6E-01 4 . 602E+00 -0.008 0.020 0.012 30.0000 1 . 848E+00 6 . 235E-0

1

2 . 472E+00 1 . 475E+0

1

1 . 32 1 E-0

1

4 . 932E+00 -0.006 0.018 0.010 35.0000 1 . 862E+00 7.412E-01 2 . 503E+00 1 . 672E+0

1

1 .516E-01 5.216E+00 -0.005 0.016 0.008 40.0000 1 . 373E+00 8.601 E-0

1

2 . 733E+00 1 . 359E+0

1

1 . 702E-0

1

5 . 466E+00 -0.004 0.015 0.007 45.0000 1 . 883E+00 9.799E-01 2.863E+00 2 . 038E+0

1

1 . 878E-0

1

5 . 689E+00 -0.003 0.014 0 .006 50.0000 1 .892E+00 1 .101 E+00 2. 992E+00 2.209E+01 2.045E-01 5 . 8 90 E + 0 0 -0.003 0.013 0.006 55.0000 1 . 900E+00 1 . 222E+00 3.1 22E+00 2 . 372E+0

1

2 . 204E-0

1

6.073E+00 -0.002 0.012 0 .005 60.0000 1 . 907E+00 1 . 344E+00 3.251 E+00 2 . 529E+0

1

2 . 356 E-0

1

6.241 E+00 -0.002 0.011 0.005 70.0000 1 .91 9E+00 1 . 589E+00 3.509E+00 2 . 825E+0

1

2.639E-01 6 . 540E+00 -0.002 0.010 0.004 80.0000 1 . 930E+00 1 . 8 36 E+0 0 3 . 766E+00 3. 1 OOE+OI 2 . 8 98 E-0

1

6.801E+00 -0.001 0.010 0.003

90.0000 1 . 939E+00 2 . 085E+00 4 . 024E+00 3 . 357E+0

1

3.1 35E-01 7 . 032E+00 -0.001 0.009 0.003

1 00.0000 1 . 948E+00 2 . 335E+00 4 . 282E+00 3 . 598E+0

1

3.353E-01 7 . 239E+00 -0.001 0.008 0.002

125.0000 1 . 965E+00 2.962E+00 4 . 928E+00 4.142E+01 3 . 8 3 1 E-0

1

7 . 680E+00 -0.001 0.007 0.002

150.0000 1 . 97 9E + 00 3 . 595E+00 5 . 574E+00 4.61 9E+01 4.233E-01 8 . 042E+00 -0.000 0.007 0.001 175.0000 1 . 991 E+00 4 . 230E+00 6 . 222E+00 5 . 043E+01 4 . 575E-0

1

8 . 343E+00 -0.000 0.006 0.001 200.0000 2 . 002E+00 4.86 9E + 00 6 . 870E+00 5 . 425E+0

1

4.872E-01 8.61 3E+00 -0.000 0 .006 0.001 250.0000 2.01 9E+00 6 . 1 51 E+00 8. 169E+00 6.092E+01 5.361 E-0

1

9 . 058E + 00 -0.000 0.005 0.001

300 . 0000 2 . 033E+00 7 . 438E+00 9.471 E+00 6 . 660E+0

1

5.751 E-0

1

9.421 E+00 -0.000 0 .005 0.001 350.0000 2 . 045E+00 8 . 730E+00 1 . 077E+0

1

7. 154E+01 6 . 070E-0

1

9 . 729E+00 -0.000 0.004 0.001 400.0000 2 . 055E+00 1 . 002E+01 1 . 208E+0

1

7 . 592E+0

1

6 . 337E-0

1

9 . 995E + 00 -0.000 0.004 0.000 450.0000 2 . 064E+00 1 . 132E+01 1 .339E+01 7.985E+01 6.564E-01 1 . 023E+0

1

-0.000 0.004 0 .000 500.0000 2 . 072E+00 1 . 262E+0

1

1 .469E+01 8 . 342E+0

1

6.760E-01 1 . 044E+01 -0.000 0.004 0.000 550.0000 2 . 080E+00 1 . 3 92E + 0

1

1 .600E+01 8.668E+01 6.931 E-0

1

1 .063E+01 -0.000 0.004 0.000 600.0000 2 . 08 6 E+OO 1 . 522E+0

1

1 .731 E+01 8. 968E+01 7 . 083E-0

1

1 . 030E+0

1

-0.000 0.003 0.000 700.0000 2 . 0 98E + 00 1 . 783E+0

1

1 . 993E+01 9 . 506E+0

1

7.339E-01 1.11 1E+01 -0.000 0.003 0.000 800.0000 2.1 08E+00 2 . 044E+0

1

2 . 255E+0

1

9. 978E+01 7.548E-01 1 . 1 38E+01 -0.000 0.003 0.000 900.0000 2.11 7E+00 2 . 305E+01 2.517E+01 1 . 040E+02 7 . 722E-0

1

1 . 1 61 E+01 - 0.000 0.003 0.000 1000.0000 2. 1 26E+00 2.567E+01 2 . 779E+0

1

1 . 078E+02 7.869E-01 1 . 183E+01 - 0.000 0.003 0.000

115
ELECTRONS IN CALCIUM FLUORIDE

I = 166.0 eV DENSITY = 3 . 1 80E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DEHS.EFF. d ( log[ )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD COP.R. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2/g MeV cm 2 /g g/cm 2

O.OIOO 1 . 666E+0

1

7.284E-03 1 . 667E+0

1

3.503E-04 2.300E-04 0.0 -0.236 0.281 0.275

0.0125 1 .412E + 01 7 .499E-03 1 .41 3E+01 5. 1 39E-04 2.809E-04 0.0 -0.224 0.265 0.259

0.0150 1 . 233E+0

1

7.657E-03 1 . 233E+0

I

7.039E-04 3.301E-04 0.0 -0 .216 0.253 0.248 0.0175 1 . 0 99E+0

1

7.773E-03 1 . 0 99E+0

1

9.1 90E-04 3 . 778E-04 0.0 -0.209 0.243 0.239

0.0200 9 . 945E+00 7.874E-03 9 . 953E+00 1 .158E-03 4.243E-04 0.0 -0.203 0.235 0.231 0.0250 8 . 424E+00 3.016E-03 8 . 432E+00 1 . 706E-03 5. 1 38E-04 0.0 -0.195 0.224 0.220 0.0300 7 . 363E+00 8. 1 18E-03 7.371 E+00 2 . 343E-03 5. 993E-04 0.0 -0.188 0.215 0.212

0.0350 6 . 577E+00 8.1 97E-03 6 . 585E+00 3 . 062E-0 3 6.813E-04 0 .

0

-0.183 0.203 0.205

0.0400 5 . 970E+00 8.263E-03 5. 979E+00 3.860E-03 7 . 604E-04 0.0 -0.179 0.202 0.200

0 .0450 5 . 487E+00 8.31 9E-03 5 . 495E+00 4.733E-03 8.368E-04 0.0 -0.175 0.198 0.196 0.0500 5.093E+00 8 . 370E-03 5.101 E+00 5.678E-03 9. 1 09E-04 0.0 -0.172 0.194 0.192

0.0550 4 . 764E + 00 8.416E-03 4 . 773E+00 6 .693E-03 9 . 829E-04 0.0 -0.170 0.190 0.189

0.0600 4 . 486E + 00 8.458E-03 4 . 495E+00 7.773E-03 1 . 053E-03 0.0 -0.167 0.137 0.186 0.0700 4.041 E + 00 8.541 E-03 4 . 050E+00 1 .012E-02 1 . 188E-03 0.0 -0.163 0.182 0.181 0.0800 3.701 E+00 8.621 E-0 3 3 . 709E+00 1 .271E-02 1 . 3 1 6 E-0 3 0.0 -0.160 0.178 0.177

0.0900 3 . 432E+00 8.704E-03 3 . 440E+00 1 .551E-02 1 . 440E-03 0.0 -0.157 0.174 0.173

0.1000 3.213E+00 8.788E-03 3 . 222E+00 1 .851 E-02 1 . 559E-0 3 0.0 -0.155 0.171 0.170 0.1250 2.81 4E+00 9.016E-03 2 . 823E+00 2 . 684E-02 1 . 840E-0 3 0.0 -0.150 0.165 0.164

0.1500 2 . 544E+00 9.265E-03 2 . 553E+00 3.617E-02 2. 102E-03 0.0 -0.146 0.161 0.160 0.1750 2 . 349E+00 9 . 534E-03 2 . 359E+00 4 . 638E-02 2 . 350E-03 0.0 -0.143 0.157 0.156 0.2000 2 . 203E+00 9.821 E-03 2.21 3E+00 5.733E-02 2.586E-03 0.0 -0.140 0.154 0.153

0.2500 2 . 000E+00 1 . 045E-02 2.01 1 E+00 8.111 E-02 3.033E-03 0.0 -0.136 0.149 0.148

0.3000 1 . 867E+00 1 .113E-02 1 . 878E+0 0 1 .069E-01 3.455E-03 5 . 037E-03 -0.125 0.145 0.143

0.3500 1 . 774E+00 1 . 187E-02 1 . 786E+00 1 . 342E-0

1

3 . 859E-0 3 1 . 737E-02 -0.119 0.140 0.138

0.4000 1 . 706E+00 1 . 266E-02 1 .71 9E+00 1 -628E-01 4.252E-03 3 . 256E-02 -0.113 0.135 0.133

0.4500 1 . 656E+00 1 . 348E-02 1 . 669E+00 1 . 923E-01 4 . 638E-03 5 . 026E-02 -0.107 0.131 0.129

0.5000 1 . 6 1 7E+00 1 . 435E-02 1 .631 E+00 2.226E-01 5.017E-03 7 . 003E-02 -0.103 0.128 0.125

0.5500 1 . 587E+00 1 . 525E-02 1 . 602E+00 2 . 536E-01 5 . 394E-03 9.144E-02 -0.098 0.124 0.121 0.6000 1 . 563E+00 1 .618E-02 1 . 579E+00 2.850E-01 5.768E-03 1 . 1 4 1 E-0

1

-0.094 0.121 0.117

0.7000 1 . 528E+00 1 . 8 1 2E-02 1 . 547E+00 3.491 E-0

1

6.512E-03 1 . 623E-0

1

-0.037 0.115 0.110

0.8000 1 . 506 E+00 2.016E-02 1 . 526E+00 4. 142E-01 7 . 256E-03 2.128E-01 -0.081 0.110 0.104

0.9000 1 .491 E+00 2.229E-02 1 . 5 1 3E+00 4.800E-01 8 . 002E-03 2.645E-01 -0.076 0.106 0.099

1 .0000 1 .481E+00 2.450E-02 1 . 505E+00 5.463E-01 8 . 752E-03 3.167E-01 -0.072 0.102 0.095

1 .2500 1 . 470E+00 3.034E-02 1 . 500 E + 0 0 7. 128E-01 1 . 065E-02 4.459E-01 -0.064 0.093 0.085

1 .5000 1 . 468E+00 3.658E-02 1 . 505E+00 8.793E-01 1 . 258E-0 2 5.70 0 E-0

1

-0.059 0 . 087 0.078

1 .7500 1 .471 E+00 4.31 3E-02 1 .51 5E+00 1 . 045E+00 1 . 456E-02 6 . 875E-0

1

-0.054 0.082 0.072

2.0000 1 . 477E+00 4.995E-02 1 . 527E+00 1 .209E+00 1 . 656E-02 7 . 980 E-0

1

-0.051 0.078 0.067

2.5000 1 .491 E+00 6 . 423E-02 1 . 555E+00 1 . 534E+00 2.065E-02 9. 994E-01 -0.047 0.071 0.060 3.0000 1 . 506E+00 7 . 922E-02 1 . 585E+00 1 . 852E+00 2 . 48 1 E-02 1 . 1 78E+00 -0.044 0.066 0.055

3.5000 1 . 520E+00 9 . 476E-02 1 . 6 1 5E+00 2.165E+00 2. 903E-02 1 . 338E+00 -0.041 0 .063 0.051 4.0000 1 . 533E+00 1 . 108E-01 1 . 644E+00 2 . 472E+00 3 . 328E-02 1 . 482E+00 -0.039 0.060 0.048

4.5000 1 . 545E+00 1 . 272E-0

1

1 . 673E+00 2 . 77 3E + 0 0 3 . 755E-02 1 . 6 1 4E+00 -0.038 0.057 0.045

5.0000 1 . 557E+00 1 . 439E-0

1

1 . 70 1 E+00 3 . 070E+00 4. 183E-02 1 . 735E+00 -0.037 0.055 0.043

5.5000 1 . 567E+00 1 .610E-01 1 . 728E+00 3.361 E+00 4.61 1 E-02 1 . 848 E+00 -0.035 0.053 0.041 6.0000 1 . 577E+00 1 .783E-01 1 . 755E+00 3.649E+00 5 . 038E-02 1 . 953E+00 -0 .034 0.051 0 .040 7.0000 1 . 5 94E + 0 0 2.1 37E-01 1 . 808E+00 4.21 0E+00 5 . 889E-02 2 . 1 44E+00 -0.032 0.048 0.037 8.0000 1 . 6 1 0E+00 2.499E-01 1 . 85 9E+0 0 4 . 755E+00 6 . 732E-02 2.31 6E+00 -0.030 0.046 0.035

9.0000 1 . 623E+00 2.868E-01 1 . 91 0E+00 5 . 286E+00 7 . 566E-02 2 . 472E+00 -0.028 0.044 0.033

10.0000 1 . 635E+00 3.243E-01 1 . 959E+00 5 . 803E+00 8.388E-02 2.615E+00 -0.027 0.042 0.031 12.5000 1 . 660E+00 4.1 99E-01 2.079E+00 7 . 04 1 E+00 1 .039E-01 2 . 931 E+00 -0.023 0.033 0.027

15.0000 1 . 679E+00 5. 180E-01 2.1 97E+00 8.21 OE+OO 1 . 231 E-0

1

3.203E+00 -0 . 020 0.035 0.024

1 7.5000 1 . 6 95E + 00 6 . 177E-01 2.31 3E+00 9.31 9E+00 1 .415E-01 3 . 442E+00 -0.018 0.033 0.022

20.0000 1 . 709E+00 7.189E-01 2 . 428E+00 1 . 0 37E+0

1

1 . 590E-0

1

3 . 656E+00 -0.016 0.031 0.019

25.0000 1 .731 E+00 9.243E-01 2 . 655E+00 1 . 234E+0

1

1 .917E-01 4 . 026E+00 -0.013 0.027 0.016 30.0000 1 . 748E + 0 0 1 . 133E+00 2 . 88 1 E+00 1 .415E+01 2.217E-01 4 . 338E+00 -0.011 0.025 0.014

35.0000 1 . 762E+00 1 . 344E+00 3. 106E+00 1 . 582E+0

1

2 . 4 9 1 E-0

1

4.609E+00 -0.009 0.023 0.012

40 . 0000 1 . 774E+00 1 . 557E+00 3.331 E+00 1 . 738E+0

1

2.742E-01 4 . 848E+00 -0 . 008 0.021 0.010 45.0000 1 . 784E+00 1 . 771 E+00 3 . 555E+00 1 . 883E+0

1

2.974E-01 5.061 E+00 -0.007 0.020 0.009

50.0000 1 . 793E+00 1 . 987E+00 3 . 780E+00 2.01 9E+01 3. 189E-01 5 . 253E+00 -0.007 0.019 0.008

55.0000 1 . 802E+00 2 . 204E+00 4 .005E+00 2. 148E+01 3. 388E-01 5 . 429E+00 -0.006 0.018 0.007 60.0000 1 . 30 9E+00 2 . 422E+00 4 . 23 1 E+00 2.269E+01 3.574E-01 5 . 5 90 E+0 0 -0 . 006 0.017 0.007

70.0000 1 .822E+00 2 . 860E+00 4 . 682E+00 2 . 494E+0

1

3. 909E-01 5 . 878E+00 -0.005 0.016 0.006 80.0000 1 .833E+00 3.301 E+00 5.1 34E+00 2.698E+01 4.205E-01 6 . 1 30 E + 00 -0.004 0.015 0.005

90.0000 1 .843E+00 3 . 744E+00 5 . 587E+00 2 . 884E+0

1

4.463E-01 6 . 353E+00 -0.004 0.014 0 .004 100.0000 1 . 351 E+00 4. 189E+00 6 . 040E+00 3 . 056E+0

1

4.703E-01 6 . 554E+00 -0 .003 0.013 0 .004 125.0000 1 . 86 9E+0 0 5 . 308E+00 7 . 1 77E+00 3 . 436E+0

1

5.1 98E-01 6 . 983E+00 -0.003 0.012 0.003

150.0000 1 . 884E+00 6 . 434E+00 8.31 7E+00 3 . 759E+0

1

5.594E-01 7 . 336E+00 -0.002 0.011 0.003

175.0000 1 . 8 96 E + 0 0 7 . 565E+00 9 . 460E+00 4 . 04 1 E+0

1

5.91 9E-01 7 . 636E+00 -0.002 0.010 0.002

200.0000 1 . 906E+00 8 . 699E+00 1 .061E+01 4 . 290E+0

1

6 . 1 92E-01 7 . 898E+0 0 -0.001 0.009 0.002 250.0000 1 . 923E+00 1 . 0 98E + 0

1

1 . 290E+0

1

4.717E+01 6.627E-01 3 . 337E+00 -0.001 0.009 0.001 300.0000 1 . 937E+00 1 -326E+01 1 . 520E+01 5 . 074E+0

1

6 . 959E-0

1

8.697E+00 -0.001 0.008 0.001 350.0000 1 . 949E+00 1 . 556E+0

1

1 . 750E+0

1

5.380E+01 7 . 224E-0

1

9 . 003E+00 -0.001 0.008 0.001 400.0000 1 . 959E+00 1 . 735E+0

1

1 . 981 E + 01 5 . 648E+0

1

7.440E-01 9 . 268E+00 -0.001 0.007 0.001 450.0000 1 . 968E+00 2.015E+01 2.212E+01 5 . 837E+0

1

7 . 620 E-0

1

9 . 502E+00 -0.000 0.007 0.001 500.0000 1 . 976E+00 2 . 246E+0

1

2.443E+01 6. 102E+01 7.773E-01 9.71 2E+00 -0.000 0.007 0.001 550.0000 1 . 983E+00 2 . 476E+0

1

2 . 675E+0

1

6 . 297E+0

1

7. 905E-01 9. 902E+00 -0 .000 0.006 0.001 600.0000 1 . 990E+00 2 . 707E+0

1

2 . 906E+0

1

6 . 477E+0

1

8.021 E-0

1

1 . 008E+0

1

-0.000 0.005 0.001

700 .OOOC 2 .001 E+00 3. 1 69E+01 3.369E+01 6 . 7 96E+0

1

8.212E-01 1 . 038E+01 -0.000 0.006 0.001 300.0000 2.01 1 E+00 3.631 E+O

1

3 . 832E+0

1

7 . 074E+0

1

8.366E-01 1 . 065E+0

1

-0.000 0.006 0.000

900.0000 2 . 020E+00 4.094E+01 4 . 296 E+0

1

7 . 320E+0

1

8.492E-01 1 . 088E+0

1

- 0.000 0.006 0.000 1000.0000 2 . 028E+00 4 . 557E+0

1

4 . 760E+0

1

7 . 542E+0

1

8 . 5 98E-0

1

1 . 109E+01 - 0.000 0.005 0.000

116
ELECTRONS IN CARBON DIOXIDE

I = 85.0 eV DENSITY = 1.842E-03 g/ca 3 (20® C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV ca 2 /g MeV cm 2 /g g/cra 2 0.0100 1 . 931 E+01 3. 962E-03 1 . 982E+01 2.874E-04 1 . 096E-04 0.0 -0.204 0.234 0.232

0.0125 1 . 6 68E+0

1

3. 988E-03 1 . 668E+0

1

4.255E-04 1 . 31 6E-04 0.0 -0.195 0.223 0.221 0.0150 1 . 449E+0

1

4.003E-03 1 .449E+01 5.868E-04 1 . 526E-04 0.0 -0.189 0.214 0.213 0.0175 1 .286E+01 4.012E-03 1 . 287E+01 7.703E-04 1 .728E-04 0.0 -0.183 0.207 0.206 0.0200 1 . 1 60E+01 4.01 9E-03 1 .161E+01 9.752E-04 1 . 924E-04 0.0 -0.179 0.202 0.201 0.0250 9 . 780E+00 4 . 029E-03 9 . 784E+00 1 . 446E-03 2.298E-04 0.0 -0.172 0.193 0 . 1 92 0.0300 8.51 5E+00 4.039E-03 8.51 9E+00 1 . 996E-03 2.654E-04 0.0 -0.167 0.187 0.186 0.0350 7 . 533E+00 4 . 048E-03 7 . 587E+00 2.61 9E-03 2. 994E-04 0.0 -0.163 0.132 0.181 0.0400 6 . 866E+00 4.059E-03 6 .370E+00 3.31 3E-03 3 . 323E-04 0.0 -0.160 0.177 0.177 0.0450 6 . 297E+00 4.072E-03 6.301 E+00 4 . 074E-03 3.641E-04 0.0 -0.157 0.174 0.173

0.0500 5 . 834E+00 4.085E-03 5 . 838E+00 4 . 899E-03 3.950E-04 0.0 -0 . 1 55 0.171 0.170 0.0550 5.449E+00 4.100E-03 5 . 453E+00 5.786E-03 4.251E-04 0.0 -0.152 0.163 0.168

0.0600 5 . 1 24E+00 4. 1 16E-03 5 . 1 28E+00 6.732E-03 4.545E-04 0.0 -0.151 0.166 0.165 0.0700 4 . 605E+00 4. 152E-03 4 . 609E+00 8.793E-03 5.11 3E-04 0 . 0 -0.147 0.162 0.161 0.0800 4 . 208E+00 4. 1 92E-03 4.21 2E+00 1 . 107E-02 5 . 659E-04 0.0 -0.145 0.158 0.158

0.0900 3 .895E+00 4.235E-03 3 . 900E+00 1 .354E-02 6 . 187E-04 0.0 -0.142 0.156 0.155 0.1000 3 . 642E+00 4 . 282E-03 3 . 646 E+00 1 .61 9E-02 6.698E-04 0.0 -0.140 0.153 0.153 0.1250 3. 180E+00 4.409E-03 3 . 1 84E+00 2 . 356E-02 7. 920E-04 0.0 -0.136 0.149 0.148 0.1500 2 . 863E+00 4.548E-03 2 . 873E+00 3. 184E-02 9.074E-04 0.0 -0.133 0.145 0.144

0.1750 2 . 644E+00 4.697E-03 2 . 648E + 00 4.092E-02 1 .018E-03 0.0 -0.131 0.142 0.141 0.2000 2 . 476E+00 4.855E-03 2 . 480 E + 0 0 5.069E-02 1 . 124E-03 0.0 -0.128 0.139 0.139

0.2500 2 . 242E+00 5.1 96E-03 2 . 247E+00 7.194E-02 1 . 326E-0 3 0.0 -0.125 0.136 0.135

0.3000 2 . 089E+00 5.570E-03 2 . 0 94E+00 9 . 504E-02 1 . 520E-03 0 .

0

-0.122 0.132 0.132

0.3500 1 . 983E+00 5.970E-03 1 . 989E+00 1 . 1 96E-01 1 . 707E-03 0.0 -0.120 0.130 0.129

0.4000 1 . 906E+00 6.397E-03 1 . 91 3E+00 1 . 452E-0

1

1 . 890E-03 0.0 -0.118 0.128 0.127

0.4500 1 . 84 9E+0 0 6 .847E-03 1 . 856E+00 1 .718E-01 2.071E-03 0.0 -0.116 0.126 0.125

0.5000 1 .806E+00 7.319E-03 1 .81 3E+00 1 .991E-01 2.250E-03 0.0 -0.114 0.125 0.123 0.5500 1 . 773E+0 0 7.810E-03 1 .781 E+00 2.269E-01 2 . 428E-0 3 0.0 -0.113 0.123 0.121 0.6000 1 . 747E+00 8.318E-03 1 . 755E+00 2.552E-01 2.606E-03 0.0 -0.112 0.122 0.120 0.7000 1 .71 0E+00 9.381E-03 1 .71 9E+00 3.128E-01 2.962E-03 0.0 -0.109 0.120 0.117

0.8000 1 . 687E+00 1 .050E-02 1 . 6 98E+00 3.714E-01 3.31 9E-03 0.0 -0.107 0.118 0.115

0 . 9000 1 . 673E+00 1 . 1 67E-02 1 . 685E+00 4 . 305E-0

1

3 . 678E-03 0.0 -0.106 0.116 0.113

1 .0000 1 . 665E+00 1 . 288E-02 1 . 677E+00 4. 900E-01 4.041E-03 0.0 -0.104 0.115 0.112

1 .2500 1 . 65 9E + 00 1 .609E-02 1 . 675E+Q0 6.393E-01 4. 960E-03 0.0 -0.101 0.112 0.108

1 .5000 1 . 664E+00 1 . 952E-02 1 . 684E+0 0 7.882E-01 5.899E-03 0.0 -0.099 0.109 0.105

1 .7500 1 . 6 75E + 00 2.31 4E-02 1 . 6 98E + 00 9.361 E-01 6 .857E-03 0.0 -0.097 0.107 0.103 2.0000 1 . 688E+00 2 . 6 90E-02 1 .71 5E+00 1 . 083E+00 7 .831 E-03 0.0 -0.095 0.105 0.101 2.5000 1 . 7 1 5E+00 3 . 482E-02 1 .751 E+00 1 . 37 1 E+00 9.821E-03 0.0 -0.092 0.103 0.098

3.0000 1 . 744E+00 4. 31 5E-02 1 . 787E+00 1 . 654E+00 1 . 185E-02 0.0 -0.090 0.100 0.095

3.5000 1 . 770E+00 5. 181E-02 1 . 822E+00 1 . 931 E+00 1 . 392E-02 0.0 -0.088 0.098 0.093

4.0000 1 . 7 94E+00 6.077E-02 1 . 855E+00 2.203E+00 1 . 600E-02 0.0 -0 . 087 0.097 0.091 4.5000 1 .31 6E+00 6 . 996E-02 1 .886E+00 2 . 470E+00 1 .810E-02 0.0 -0.086 0.095 0.089

5.0000 1 . 837E+00 7. 938E-02 1 . 91 6E+00 2 . 733E+00 2. 022E-02 0.0 -0.084 0.094 0.088 5.5000 1 . 856E+00 8.899E-02 1 . 945E+00 2. 992E+00 2 . 234E-02 0.0 -0.083 0.093 0.086 6.0000 1 . 874E+00 9.877E-02 1 . 973E+00 3 . 247E+00 2.448E-02 0.0 -0.083 0.092 0.085 7.0000 1 . 906E+00 1 . 188E-01 2 . 025E+00 3 . 748E+00 2 . 875E-02 0.0 -0.081 0.090 0.083 8.0000 1 . 935E+00 1 . 394E-01 2 . 0 74E+00 4 . 236E+00 3 . 302E-02 0.0 -0.080 0.088 0.081 9.0000 1 . 960E+00 1 .604E-01 2.121 E+00 4.712E+00 3 . 729E-02 0.0 -0.079 0.087 0.080 10.0000 1 . 983E+00 1 .817E-01 2 . 1 65E+00 5 . 1 79E+00 4.1 54E-02 0.0 -0.078 0.085 0.078

12.5000 2 . 0 33E + 0 0 2.366E-01 2.269E+00 6 . 306E+00 5 . 206E-02 0.0 -0.076 0.082 0.075

15.0000 2.07 4E+00 2.930E-01 2 . 367E+00 7 . 385E+00 6 . 240E-02 0.0 -0.074 0.080 0.072

17.5000 2 . 1 08E+00 3.506E-01 2.459E+00 3.421 E+00 7 . 252E-02 0.0 -0.073 0 .078 0.070 20.0000 2. 1 39E+00 4.091E-01 2 . 548E+00 9 . 420E+00 8.241E-02 0.0 -0.072 0.076 0.068 25.0000 2 . 1 87E+00 5.281E-01 2.71 5E+00 1 .132E+01 1 .015E-01 2 . 736E-02 -0.059 0.073 0.063 30.0000 2. 222E+00 6 . 493E-01 2 . 872E+00 1 .31 1E+01 1 . 1 96E-01 1 . 1 33E-0

1

-0.048 0.068 0.057 35.0000 2 . 249E+00 7.71 9E-01 3.021 E+00 1 .481E+01 1 . 370E-0

1

2.215E-01 -0.041 0.065 0.051 40.0000 2.271 E+00 8. 958E-01 3 . 1 67E+00 1 . 642E+0

1

1 . 535E-0

1

3.361E-01 -0.036 0.061 0.046 45.0000 2.289E+00 1 .021 E+00 3 . 3 1 0 E+0 0 1 . 797E+0

1

1 .693E-01 4.504E-01 -0.033 0.058 0.042 50.0000 2 . 305E+00 1 . 1 46E+00 3.451 E+00 1 . 945E+01 1 .844E-01 5.614E-01 -0.030 0.055 0.033 55.0000 2.31 9E+00 1 . 273E+00 3.591 E+00 2. 087E+01 1 . 989E-01 6.680E-01 -0.028 0.053 0.035 60.0000 2.331 E+00 1 . 400E+00 3.731 E+00 2 . 223E+0

1

2.127E-01 7 .697E-01 -0.026 0.050 0.033

70 .0000 2 . 352E+00 1 . 656E+00 4 . 007E+00 2.482E+01 2 . 387E-0

1

9.585E-01 -0.024 0.047 0.029

80.0000 2.369E+00 1 . 91 3E+00 4 . 282E+00 2 . 723E+0

1

2.627E-01 1 . 1 30E+00 -0.022 0.044 0.025

90.0000 2 . 384E+00 2 . 1 72E+00 4 . 557E+00 2.949E+01 2.848E-01 1 . 285E+00 -0.021 0.041 0.023

100.0000 2 . 398E+00 2 . 432E+00 4 . 830E+00 3. 1 63E+01 3.054E-01 1 . 427E+00 -0.020 0.039 0.021 125.0000 2 . 425E+00 3. 087E+00 5.51 2E+00 3. 647E+01 3.509E-01 1 . 737E+00 -0.019 0.035 0.017 150.0000 2 . 447E+00 3 . 745E+00 6 . 1 93E+00 4 . 074E+0

1

3.896E-01 1 . 996E+00 -0.018 0.032 0.015

175.0000 2 . 466E+00 4 . 408E+00 6 . 873E+00 4 . 457E+0

1

4 . 230E-0

1

2 . 220 E+0 0 -0.017 0.030 0.013 200.0000 2.481 E+00 5 . 072E+00 7 . 554E+00 4.804E+01 4.523E-01 2.41 7E+00 -0.016 0.028 0.012 250.0000 2 . 507E+00 6 . 408E+00 8.91 4E+00 5.41 3E+01 5.01 IE-01 2 . 752E+00 -0.015 0.026 0.010 300.0000 2 . 527E+00 7.749E+00 1 . 028E+0

1

5 . 935E+0

1

5.404E-01 3.032E+00 -0.014 0.024 0.008 350.0000 2 . 544E+00 9 . 0 94E+0 0 1 . 1 64E+01 6 . 392E+0

1

5.730E-01 3 . 274E+00 -0.012 0.022 0.007 400.0000 2 . 559E+00 1 . 044E+0

1

1 . 300E+0

1

6.798E+01 6 . 004E-01 3 . 489E+00 -0.011 0.021 0.007 450.0000 2.571 E+00 1 . 179E+01 1 .436E+01 7.164E+01 6.240E-01 3.681 E+00 -0.010 0.020 0.006 500.0000 2 . 582E+00 1 .31 5E+01 1 .573E+01 7.496E+01 6.445E-01 3 . 857E+00 -0.010 0.019 0.005 550.0000 2 . 59 1 E+00 1 . 450E+01 1 .709E+01 7.801 E+01 6.624E-01 4.01 8E+00 -0.009 0.019 0.005 600.0000 2.600E+00 1 . 586E+0

1

1 . 846E+0

1

8 . 083E+01 6.784E-01 4.168E+00 -0.008 0.018 0 .005 700.0000 2.61 5E+00 1 . 857E+0

1

2. 1 18E+01 8 . 588E+0

1

7 . 055E-01 4 . 438E + 0 0 -0.007 0.017 0.004 800.0000 2 . 627E+00 2. 129E+01 2.392E+01 9.032E+01 7.278E-01 4 . 677E+00 -0 .006 0.016 0.003

900.0000 2 . 638E+00 2.401 E+01 2 . 665E+0

1

9 . 428E+0

1

7 . 465E-01 4.891 E+00 -0.005 0.016 0.003 1000.0000 2 . 647E+00 2 . 673E+01 2.938E+01 9 . 785E+0

1

7.624E-01 5 . 086E+00 -0.004 0.015 0.003

117
ELECTRONS IN CELLULOSE NITRATE

I = 87.0 eV DENSITY = 1 . 490E+00i g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. dCloc1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD C0RR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV ci» 2 /g MeV cra 2/g g/cm 2 0.0100 2 . 028E+0

1

3.800E-03 2 . 029E+0

1

2.809E-04 1 . 029E-04 0.0 -0.205 0.236 0.234

0.0125 1 . 708E+0

1

3 . 824E-03 1 . 7 08E+0

1

4. 158E-04 1 . 234E-04 0 .

0

-0.196 0.224 0.222

0.0150 1 . 484E+0

1

3.837E-03 1 . 484E + 0

1

5 . 733E-04 1 .431 E-04 0.0 -0.189 0.215 0.214

0.0175 1 .317E+01 3.847E-03 1 .318E+01 7.524E-04 1 . 620E-04 0.0 -0.184 0.209 0 . 207 0.0200 1 . 189E+01 3 . 853E-03 1 . 189E + 01 9.524E-04 1 .802E-04 0.0 -0.180 0.203 0.202

0.0250 1 . 002E+0

1

3.863E-03 1 . 002E+0

1

1 .412E-03 2. 152E-04 0.0 -0.173 0.194 0.193

0.0300 3 . 725E+00 3.872E-03 8 . 729E+00 1 . 949E-03 2.485E-04 0.0 -0.163 0.133 0.137

0.0350 7.771E+00 3.832E-03 7 . 775E+00 2.557E-03 2.803E-04 0.0 -0.164 0.182 0.182

0 .0400 7 . 037E+00 3 . 893E-03 7 . 04 1 E+00 3.234E-03 3.111 E-04 0 .

0

-0.160 0.178 0.178

0 . 0450 6 . 454E+00 3. 906E-03 6 . 453E+00 3.976E-03 3.409E-04 0.0 -0.158 0.175 0.174

0.0500 5. 980E+00 3.91 9E-03 5 . 984E+00 4.781 E-03 3.698E-04 0.0 -0.155 0.171 0.171 0.0550 5 . 585E+00 3. 934E-03 5 . 589E+00 5.647E-03 3. 979E-04 0 .

0

-0.153 0.169 0.168

0.0600 5 . 252E+00 3. 950E-03 5 . 256E+00 6 . 570E-03 4 . 254E-04 0.0 -0.151 0.166 0.166 0.0700 4.721 E+00 3. 985E-03 4 . 725E+00 8 . 580E-03 4.786E-04 0.0 -0.143 0.162 0.162

0.0800 4.31 4E+00 4 . 024E-03 4.318E+00 1 .080E-02 5 . 298E-04 0.0 -0.145 0.159 0.159

0.0900 3 . 994E+00 4.066E-03 3. 998E+00 1 .321E-02 5.792E-04 0.0 -0.143 0.156 0.156

0.1000 3 . 734E+00 4.111E-03 3 . 739E+00 1 . 580E-02 6.271 E-04 0.0 -0.141 0.154 0.154

0.1250 3.261 E+00 4 . 235E-03 3 . 265E+00 2 . 298E-02 7.416E-04 0.0 -0.137 0.149 0.149

0 . 1 500 2. 941 E+00 4 . 370E-03 2. 945E+0O 3. 106E-02 8.499E-04 0.0 -0.134 0.145 0.145

0.1750 2.711 E+00 4.515E-03 2.71 6E+00 3 . 992E-02 9.533E-04 0.0 -0.131 0.142 0.142

0.2000 2 . 539E+00 4.669E-03 2 . 544E+00 4. 944E-02 1 . 053E-03 0.0 -0.129 0.140 0.139

0.2500 2 . 299E+00 4. 999E-03 2 . 304E+00 7.016E-02 1 . 243E-03 0.0 -0.125 0.136 0.135

0.3000 2.143E+00 5.361 E-03 2. 148E+00 9.268E-02 1 . 425E-03 0.0 -0.122 0.133 0.132

0.3500 2.034E+00 5 . 749E-03 2 . 040E+00 1 .166E-01 1 . 60 1 E-03 0.0 -0.120 0.130 0.129

0.4000 1 . 956E+00 6.162E-03 1 . 962E+00 1 .416E-01 1 . 773E-03 0.0 -0.118 0.128 0.127

0.4500 1 . 896E+00 6.597E-03 1 . 903E+00 1 . 675E-0

1

1 . 943E-03 8 . 343E-03 -0.096 0.125 0.124

0.5000 1 . 350E+00 7.054E-03 1 . 857E+00 1 .941E-01 2. 1 12E-03 3.1 98E-02 -0.091 0.121 0.118

0.5500 1 .81 3E+00 7 . 530E-03 1 . 820E+0 0 2.21 3E-01 2.281 E-03 5.810E-02 -0 . 085 0.117 0.114

0.6000 1 . 783E+00 8 . 022E-03 1 . 7 92E+00 2.490E-01 2 . 449E-03 8.61 IE-02 -0.080 0.113 0.109

0.7000 1 .741 E+00 9.050E-03 1 . 750E+00 3.056E-01 2 . 789E-03 1 . 460E-0

1

-0.072 0.106 0.101 0.8000 1 .71 2E+00 1 . 0 1 3E-02 1 . 722E+00 3 . 632E-0

1

3.131 E-03 2 . 0 90 E-0 1 -0.066 0.100 0.093

0.9000 1 . 6 92E+00 1 . 126E-02 1 . 703E+00 4.216E-01 3.477E-03 2.734E-01 -0.061 0.095 0.087

1 . 0000 1 . 678E+00 1 . 244E-02 1 .6 91 E+0 0 4.806E-01 3 . 828E-0 3 3 . 380 E-0

1

-0.056 0 .090 0 . 082

1 .2500 1 . 660 E+00 1 . 554E-02 1 . 675E+00 6.293E-01 4 . 724E-03 4.966E-01 -0.049 0.081 0.071

1 .5000 1 . 654E+00 1 .387E-02 1 . 673E+00 7.787E-01 5.649E-03 6.473E-01 -0.044 0.074 0.064

1 .7500 1 . 654E+00 2 . 237E-02 1 . 676E+00 9 . 280E-0

1

6 . 600E-03 7 . 886E-0

1

-0.040 0.069 0.058

2.0000 1 . 657E+00 2 . 602E-02 1 . 683E+00 1 . 077E+00 7.575E-03 9 . 206E-0

1

-0.037 0.065 0.053

2.5000 1 . 667E+00 3.368E-02 1 .701 E+00 1 . 372E+00 9.534E-03 1 . 159E+00 -0.033 0.058 0.046

3.0000 1 . 680E+00 4. 176E-02 1 .721 E+00 1 . 665E+00 1 . 166E-02 1 . 368E+00 -0.031 0.054 0.041 3.5000 1 . 6 92E+0 0 5.016E-02 1 . 742E+00 1 . 953E+00 1 . 378E-02 1 . 554E+00 -0.029 0.050 0.038

4 .0000 1 . 704E+00 5 . 383E-02 1 . 763E+00 2 . 239E+00 1 . 5 94E-02 1 .721 E+00 -0 .028 0.047 0.035

4.5000 1 -715E+00 6 . 775E-02 1 . 783E+00 2.521 E+00 1 .81 4E-02 1 . 873E+00 -0.027 0.045 0.033

5.0000 1 . 726E+00 7.688E-02 1 . 8 0 3E+0 0 2 . 800 E+0 0 2 . 035E-02 2.01 2E+00 -0.026 0.043 0.032 5.5000 1 . 735E+00 8 . 620E-02 1 .822E+00 3 . 076E+00 2.259E-02 2. 140E+00 -0.025 0.041 0.030 6.0000 1 . 745E+00 9.569E-02 1 .840E+00 3.349E+00 2 . 485E-02 2 . 258E+00 -0 .024 0.040 0 .029 7.0000 1 .761 E+00 1 .151E-01 1 . 876E+00 3 . 887E+0 0 2.940E-02 2 . 473E+00 -0.023 0.037 0.027

8.0000 1 . 775E+00 1 .351E-01 1 . 91 OE+00 4.41 5E+00 3 . 398E-02 2 . 663E+00 -0.022 0.035 0 .026 9.0000 1 . 788E+00 1 . 554E-0

1

1 . 944E+00 4. 934E+00 3 . 857E-02 2 . 835E+00 -0.021 0.034 0.024

10.0000 1 . 800E+00 1 . 762E-0

1

1 . 976E+00 5 . 444E+00 4.317E-02 2.991 E+00 -0.020 0.032 0.023

12.5000 1 . 824E+00 2.294E-01 2 . 053E+00 6 . 635E+00 5 . 464E-02 3.331 E+00 -0.017 0.029 0.021 15.0000 1 -343E+00 2.842E-01 2. 127E+00 7 .881 E+00 6.599E-02 3.61 9E+00 -0.015 0.027 0.019

17.5000 1 . 85 9E+0 0 3.401E-01 2.1 99E+00 9 . 036E+00 7.71 6E-02 3 . 870E+00 -0.013 0.025 0.017

20.0000 1 . 873E+00 3. 969E-01 2 . 270E+00 1 .016E+01 8.81 2E-02 4 . 0 93E+00 -0.012 0.024 0.016 25.0000 1 .895E+00 5. 126E-01 2 . 407E+00 1 . 229E+0

1

1 .093E-01 4 . 478E+00 -0.009 0.021 0.013

30.0000 1 . 91 2E+00 6.303E-01 2 . 542E+00 1 .431E+01 1 . 295E-0

1

4 . 302E+00 -0.007 0.019 0.01 1 35.0000 1 . 926E+00 7.495E-01 2 . 676E+00 1 . 623E+0

1

1 . 488E-0

1

5 . 083E+00 -0.006 0.017 0.009

40.0000 1 . 938E+00 3.699E-01 2 . 808E+00 1 . 805E+0

1

1 .671E-01 5 . 330E+00 -0.005 0.016 0.008

45.0000 1 . 948E+00 9.91 3E-01 2 . 940E+00 1 . 980E+01 1 . 845E-0

1

5 . 552E+00 -0.004 0.015 0.007 50.0000 1 . 958E+00 1.11 3E+00 3.071 E+00 2.146E+01 2.010E-01 5.751 E+00 -0.003 0.014 0.006 55.0000 1 . 966E+00 1 . 236 E+00 3 . 202E+00 2 . 305E+0

1

2. 168E-01 5. 934E+00 -0.003 0.013 0.006

60 . 0000 1 . 973E+00 1 . 360E+00 3 . 333E+00 2 . 458E+0

1

2.318E-01 6 . 1 01 E+00 -0.002 0.012 0.005

70 .0000 1 . 986E+00 1 . 60 9E + 00 3 . 595E+00 2 . 747E+0

1

2.599E-01 6 . 399E+00 -0.002 0.011 0 .004 80.0000 1 . 997E+00 1 . 859E+00 3 . 856E+00 3.016E+01 2.856E-01 6 . 660E+00 -0.001 0.010 0.004

90.0000 2 . 007E+00 2.11 1 E+00 4.1 18E+00 3 . 267E+0

1

3.091E-01 6 .891 E+00 -0.001 0.009 0.003

100.0000 2.01 5E+00 2 . 364E+00 4 . 379E+00 3 . 502E+0

1

3.309E-01 7 . 098E+00 -0.001 0.009 0.003

125.0000 2 . 033E+00 3 . 000E+00 5 . 034E+00 4.034E+01 3.785E-01 7 . 538E+00 -0.001 0.008 0.002

150.0000 2 . 048E+00 3.641 E+00 5 . 689E+00 4.501 E+0

1

4. 186E-01 7 . 899E+00 -0.000 0.007 0 .002 175.0000 2 . 06 0 E + 00 4 . 285E+00 6.346E+00 4.917E+01 4.528E-01 8 . 205E+00 -0.000 0.006 0.001

200 . 0000 2. 071 E+00 4 . 932E+00 7 . 003E+00 5 . 292E+0

1

4.825E-01 8 . 471 E+00 -0 .000 0.006 0.001 250.0000 2 . 089E+00 6 . 232E+00 8 . 320E+00 5 . 946 E+0

1

5.316 E-0

1

8.91 5E+00 -0.000 0.005 0.001 300.0000 2. 103E+00 7.537E+00 9 . 640E+00 6 . 504E+0

1

5.707E-01 9 . 279E+00 -0 .000 0.005 0.001 350.0000 2.11 5E+00 8 . 84 6 E+0 0 1 . 096E+O1 6 . 990E+01 6 . 027E-0

1

9 . 586E+0 0 -0 .000 0.005 0.001 400.0000 2. 126E+00 1 .016E+01 1 . 223E+0

1

7.421 E+0

1

6 .296E-01 9 . 853E+00 - 0.000 0.004 0.000 450.0000 2. 135E+00 1 . 147E+01 1 .361E+01 7 . 807E+0

1

6 . 524E-01 1 . 009E+0

1

-0.000 0.004 0.000 500.0000 2. 1 43E+00 1 .279E+01 1 . 4 93E+0

1

8. 158E+01 6.722E-01 1 . 030E+0

1

- 0.000 0.004 0.000 550.0000 2.151 E+00 1 .41 1E+01 1 . 626E+0

1

8.479E+01 6.895E-01 1 .049E+01 -0.000 0.004 0.000

600 . 0000 2 . 1 58E+00 1 . 543E+0

1

1 . 759E+0

1

8 . 774E+0

1

7 . 047E-01 1 . 066E+0

1

-0 .000 0.004 0.000 700.0000 2 . 1 70E+00 1 . 307E+0

1

2 . 024E+0

1

9 . 304E+01 7.305E-01 1 . 0 97E+0

1

- 0.000 0.003 0.000 300.0000 2. 1 8 1 E+00 2.072E+01 2.290E+01 9.768E+01 7.516 E-0

1

1 . 124E+01 - 0.000 0.003 0 .000 900.0000 2. 1 90E+00 2 . 337E+0

1

2.556E+01 1 .01 8E+02 7.692E-01 1 . 147E+01 -0.000 0.003 0 . 000 1000.0000 2.1 98E+00 2 . 602E+0

1

2.822E+01 1 . 055E+02 7.841 E-01 1 . 1 68E+01 -0.000 0.003 0.000

118

d
ELECTRONS IN CERIC SULFATE DOSIMETER SOLUTION

I = 76.7 eV DENSITY = 1 . 030E+0Ci g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS . EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cra 2 /g MeV cm 2 /g g/cm 2 0.0100 2.237E+01 3.996E-03 2 . 237E+0

1

2 . 538E-04 9.70 3E-0 5 0.0 -0.200 0.229 0.226 0.0125 1 .881 E + 01 4.031E-03 1 . 832E+0

1

3.762E-04 1 . 169E-04 0.0 -0.191 0.218 0.216 0.0150 1 . 6 33E + 0

1

4.052E-03 1 . 633E+0

1

5 . 1 93E-04 1 . 360E-04 0.0 -0.185 0.209 0.208 0.0175 1 . 449E + 0 1 4.067E-03 1 . 449E+01 6.S21E-04 1 . 543E-04 0.0 -0.180 0.203 0.202

0.0200 1 . 307E+01 4.078E-03 1 . 307E+0

1

8 . 640E-04 1 .721 E-04 0.0 -0.176 0 . 1 98 0.197 0.0250 1 . 1 01 E + 01 4.094E-03 1 . 1 01 E+01 1 .233E-03 2 . 061 E-04 0 .

0

-0.169 0.189 0.139

0 .0300 9 . 577E+00 4. 108E-03 9. 581 E+00 1.771 E-03 2 . 38 5 E-04 0.0 -0.164 0.183 0.182

0.0350 8 . 525E+00 4.120E-03 8 . 529E + 0 0 2.325E-03 2 . 6 96E-04 0.0 -0.161 0.178 0.173

0 . 0400 7.71 7E+00 4.134E-03 7.721 E+00 2 . 942E-0 3 2 . 996E-04 0 .

0

-0.157 0.174 0.174

0.0450 7 . 075E+00 4. 148E-03 7.07 9E + 00 3.620E-03 3.236E-04 0.0 -0.155 0.171 0.170 0.0500 6 . 553E+00 4. 164E-03 6 . 557E+00 4.354E-03 3 . 568E-04 0.0 -0.152 0.168 0.167 0.0550 6.11 9E+00 4 . 180E-03 6. 123E+00 5 . 1 44E-03 3 . 843E-04 0.0 -0.150 0.165 0.165 0.0600 5 . 753E+00 4.1 98E-03 5 . 757E+00 5 . 987E-03 4.111 E-04 0.0 -0.148 0.163 0.163

0.0700 5. 169E+00 4.236E-03 5. 173E+00 7.823E-03 4.630E-04 0.0 -0.145 0.159 0.159

0.0800 4 . 722E+00 4 . 278E-03 4 . 727E+00 9 .848E-03 5. 129E-04 0.0 -0.143 0.156 0.156 0.0900 4 . 370E+00 4.324E-03 4 . 374E+00 1 . 205E-02 5.611 E-04 0.0 -0.140 0.153 0.153

0 .1000 4 . 085E+00 4.373E-03 4 . 090E+00 1 . 442E-02 6 . 079E-04 0.0 -0 . 1 38 0.151 0.151 0.1250 3 . 566E+00 4.505E-03 3 . 570E+00 2.099E-02 7.1 96E-04 0.0 -0.134 0.146 0.146 0.1500 3.215E+00 4.649E-03 3.21 9E+00 2 . 838E-02 8 . 253E-04 0.0 -0.131 0.143 0.142

0.1750 2. 963E+00 4.803E-03 2. 967E+00 3 . 64SE-02 9 . 263E-04 0.0 -0.129 0.140 0.139

0.2000 2 . 773E + 00 4 . 966E-03 2 . 778E+00 4.520E-02 1 . 023E-03 0.0 -0.127 0.137 0.137

0.2500 2.51 1E+00 5.31 6E-03 2. 51 6E+00 6.41 8E-02 1 .209E-03 0.0 -0.123 0.134 0.133

0.3000 2.339E+00 5.700E-03 2 . 344E+00 8.481 E-02 1 . 386E-03 0.0 -0.120 0.131 0.130 0.3500 2.21 9E+00 6.11 IE-03 2 . 226E+00 1 . 067E-0

1

1 . 558E-03 0.0 -0.118 0.128 0.127

0.4000 2 . 1 33E+00 6 . 548E-03 2. 140E+00 1 . 297E-0

1

1 . 726E-03 0.0 -0.116 0.126 0.125

0.4500 2.06 9E+00 7.009E-03 2 . 076E+00 1 . 534E-0

1

1 . 892E-03 0.0 -0.114 0.125 0.123

0.5000 2.021E+00 7.492E-03 2 . 028E+00 1 .778E-01 2 . 056E-03 0.0 -0.109 0.123 0.121 0.5500 1 . 981 E+OO 7 . 995E-03 1 . 989E+00 2.027E-01 2.220E-03 1 . 324E-0 2 -0.094 0.120 0.118

0.6000 1 . 950E+00 8.515E-03 1 . 959E+00 2 . 280E-0

1

2.383E-03 3.21 4E-02 -0 . 088 0.117 0.114

0.7000 1 . 904E+00 9 . 602E-03 1 . 91 4E+00 2.797E-01 2.712E-03 7.786E-02 -0.078 0.110 0.106 0.8000 1 . 873E+00 1 . 074E-02 1 . 884E+00 3.324E-01 3 . 043E-03 1 .307E-01 -0 .070 0.105 0.099

0 . 9000 1 . 352E+00 1 . 1 94E-02 1 . 86 3E+00 3.858E-01 3 . 377E-03 1 . 876E-0

1

-0.064 0.099 0.093

1 .0000 1 .837E+00 1 . 3 1 8E-02 1 .850E+00 4.397E-01 3.716 E-03 2 . 470E-0

1

-0.059 0.095 0.087

1 .2500 1 .81 6E+00 1 .646E-02 1 . 833E+00 5.756E-01 4 . 582E-03 3.983E-01 -0.050 0.085 0.075

1 .5000 1 .81 0E+00 1 . 997E-02 1 .830E+00 7. 121E-01 5.476E-03 5 . 470 E-0

1

-0.043 0.077 0.066

1 .7500 1 .809E+00 2 . 367E-02 1 .833E+00 8.487E-01 6.395E-03 6.891E-01 -0 .039 0.071 0.059 2.0000 1 . 81 2E+00 2 . 752E-02 1 . 839E+00 9.849E-01 7 . 337E-03 8.234E-01 -0.035 0.067 0.054 2.5000 1 . 822E+00 3.561E-02 1 . 858E+00 1 . 255E+00 9.281 E-03 1 . 06 9E + 00 -0.031 0.059 0.046

3.0000 1 .834E+00 4 .41 3E-02 1 . 87 9E + 00 1 . 523E+00 1 . 1 29E-02 1 . 287E+00 -0 .028 0.054 0.040

3.5000 1 .847E+00 5.299E-02 1 . 900E+00 1 . 788E+00 1 . 334E-02 1 .481 E+00 -0.026 0.050 0.036 4.0000 1 .859E+00 6.21 4E-02 1 . 921 E+00 2.049E+00 1 . 544E-02 1 . 656E+00 -0.024 0 .046 0.034 4.5000 1 . 870E+00 7. 154E-02 1 . 942E+00 2 . 308E+00 1 . 757E-02 1 . 81 5E+00 -0 .023 0 .044 0.031 5.0000 1 .881 E+OO 8. 1 17E-02 1 . 962E+00 2 . 564E+00 1 . 972E-02 1 . 961 E+00 -0.022 0.042 0.029

5 . 5000 1 .891E+00 9.099E-02 1 . 982E+00 2.81 8E+00 2.1 90E-02 2 . 095E+00 -0 . 022 0.040 0.028 6.0000 1 . 900E+00 1 .010E-01 2.001 E+00 3.069E+00 2.409E-02 2.21 9E+00 -0.021 0.038 0.027 7.0000 1 . 91 7E+00 1 .215E-01 2 . 0 38E+00 3 . 564E+00 2.851 E-02 2 . 444E+00 -0.020 0.036 0.025 8.0000 1 . 932E+00 1 . 425E-0

1

2.074E+00 4 . 050E+00 3 . 296E-02 2 . 642E+00 -0.019 0.034 0.023

9.0000 1 . 945E+00 1 .639E-01 2. 109E+00 4 . 529E+00 3 . 743E-02 2.81 9E+00 -0.019 0.032 0.022

10.0000 1 . 957E+00 1 . 858E-0

1

2. 1 43E+00 4. 999E+00 4. 1 9 1 E-02 2. 980E+00 -0.018 0.030 0.021 12.5000 1 . 982E+00 2.418E-01 2 . 224E+00 6 . 144E+00 5 . 308E-02 3 . 328E+00 -0.016 0.028 0.019

15.0000 2 . 003E+00 2. 994E-01 2 . 302E+00 7.249E+00 6.41 5E-02 3.61 9E+00 -0.015 0.026 0.017

17.5000 2 . 020E+00 3.583E-01 2 . 378E+00 8.317E+00 7 . 504E-02 3 . 870 E + 0 0 -0.014 0.024 0.016 20.0000 2 . 035E+00 4. 180E-01 2 . 453E+00 9 . 352E+00 8 . 573E-02 4 . 0 92E + 00 -0.013 0.022 0.015

25.0000 2 . 059E+00 5.397E-01 2 . 598E+00 1 . 1 33E+01 1 . 065E-0

1

4.471 E+00 -0.011 0.020 0.013

30.0000 2 . 078E+00 6 .635E-01 2.741 E+00 1 .320E+01 1 . 262E-0

1

4 . 7 90 E + 0 0 -0.009 0.018 0.011 35.0000 2 . 0 93E+00 7.889E-01 2 . 882E+00 1 . 4 98E + 0

1

1 .451E-01 5 . 066E+00 -0.007 0.017 0.010 40.0000 2 . 1 0 6 E+OO 9.155E-01 3 . 022E+00 1 . 668E+0

1

1 .630E-01 5.309E+00 -0.006 0.016 0.009 45.0000 2.11 8E+00 1 . 043E+00 3.161 E+00 1 .330E+01 1.801 E-01 5 . 527E+00 -0.005 0.015 0.008 50.0000 2. 128E+00 1 . 1 72E + 00 3 . 300E+00 1 . 9S4E+0

1

1 . 963E-01 5 . 724E+00 -0.004 0.014 0.007 55.0000 2 . 1 37E+00 1 .301 E+OO 3 . 438E+00 2.1 33E+01 2. 1 18E-01 5 . 904E+00 -0.004 0.013 0.006

60 .0000 2. 145E+00 1 . 431 E+00 3.576 E + 00 2.275E+01 2 . 266E-01 6 . 070E+00 -0.003 0.012 0.006 70.0000 2. 1 59E+00 1 . 693E+00 3 . 852E+00 2 . 545E+0

1

2.543E-01 6 . 365E+00 -0.003 0.011 0.005

80.0000 2. 1 7 1 E+OO 1 . 956E + 00 4 . 1 27E+00 2.796E+01 2.796E-01 6 . 623E+00 -0.002 0.010 0.004

90 . 0000 2. 181 E+OO 2 . 22 1 E+0 0 4 . 402E+00 3 . 030E+0

1

3.030E-01 6 . 853E+00 -0.002 0.010 0.004

100.0000 2.191 E+OO 2 . 487E+00 4 . 678E+00 3 . 250E+0

1

3 . 245E-0

1

7 . 059E+00 -0.001 0.009 0.003

125.0000 2. 21 0E+00 3.1 56E+00 5 . 367E+00 3 . 749E+0

1

3.718E-01 7 . 497E+00 -0.001 0.008 0.002

150.0000 2 . 226E+00 3 .830E+00 6 . 056E+00 4. 187E+01 4. 1 17E-01 7 . 857E+00 -0.001 0.007 0.002

175.0000 2 . 240E+00 4.507E+00 6 . 747E+00 4 . 578E+0

1

4 . 459E-0

1

8.162E+00 -0.001 0.006 0.002 200.0000 2.251 E+00 5. 187E + 00 7 . 438E+00 4.931E+01 4 . 755E-0

1

8 . 427E+00 -0 .000 0.006 0.001 250.0000 2 . 270E+00 6 . 553E+0 0 8.824E+00 5 . 547E+0

1

5.247E-01 3.871 E+00 -0 .000 0.005 0.001 300.0000 2.286E+00 7. 926E+00 1 .021E+01 6 . 074E+01 5.639E-01 9 . 234E+00 -0.000 0.005 0.001 350.0000 2 . 299E+00 9 . 302E+00 1 . 160E+01 6 . 533E+0

1

5. 962E-01 9 . 54 1 E+00 -0.000 0.005 0.001 400.0000 2.31 OE+OO 1 . 068E+0

1

1 . 299E+01 6 . 940E+01 6 . 232E-0

1

9 . 807E+00 -0 .000 0.004 0.001 450.0000 2. 320E+00 1 . 206E+0

1

1 . 438E+0

1

7.305E+01 6.462E-01 1 . 0 04E + 0

1

-0 .000 0.004 0.001 500.0000 2.329E+00 1 . 345E+0

1

1 . 578E+0

1

7 . 637E+0

1

6.662E-01 1 . 025E + 0

1

-0.000 0 . 004 0.000 550.0000 2 . 337E+00 1 . 484E+0

1

1 .717E+01 7. 941E+01 6 .837E-01 1 . 044E+0

1

-0.000 0.004 0.000 600.0000 2 . 345E+00 1 . 622E+0

1

1 . 857E+0

1

8.221 E+0

1

6.991 E-0

1

1 . 062E+0

1

-0.000 0 .004 0.000 700.0000 2 . 358E+00 1 . 900E+0

1

2.136E+01 8 . 723E+0

1

7 . 252E-0

1

1 .092E+01 -0.000 0.003 0.000 800.0000 2 . 369E+00 2. 178E+01 2.415E+01 9.162E+01 7 . 466E-0

1

1.11 9E+01 -0.000 0.003 0.000 900.0000 2.379E+00 2 . 457E+0

1

2.695E+01 9 . 554E+0

1

7.644E-01 1 . 143E+01 -0 .000 0.003 0.000 1000.0000 2 . 388E+00 2 . 736E+0

1

2.975E+01 9. 907E+01 7.795E-01 1 . 164E+01 -0.000 0.003 0 .000

119
ELECTRONS IN CESIUM IODIDE

I = 553.1 eV DENSITY = 4.51 OE+OO' g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. dC log1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2 /g MeV cm 2/g g/cm 2 0.0100 1 .01 9E+01 1 . 704E-02 1 . 020E+01 6.284E-04 8 . 286E-04 0.0 -0 .330 0.469 0.419 0.0125 8.803E+00 1 .839E-02 8.821 E+00 8 . 928E-04 1 . 0 39E-0 3 0.0 -0 . 307 0.424 0.382

0.0150 7 . 7 95E+00 1 . 948E-02 7.814E+00 1 . 1 95E-03 1 .247E-03 0.0 -0.291 0.392 0.356 0.0175 7 . 025E+00 2 . 038E-02 7 . 045E+00 1 . 532E-0 3 1 . 454E-0 3 0.0 -0.279 0 . 368 0.337

0 .0200 6.41 5E+00 2. 1 14E-02 6 . 437E+00 1 . 904E-03 1 . 658E-03 0.0 -0.269 0.350 0.322

0.0250 5.509E+00 2.240E-02 5.531 E+00 2.745E-03 2 . 060E-03 0.0 -0.254 0 . 322 0.300 0.0300 4 . 864E+00 2.340E-02 4 . 887E+00 3.709E-03 2 . 454E-03 0.0 -0 . 243 0.303 0.284

0.0350 4 . 379E+00 2 . 425E-02 4 . 404E+00 4 . 789E-03 2 . 839E-03 0.0 -0.235 0.288 0.272

0.0400 4.001 E+00 2.498E-02 4 . 026E+00 5.978E-03 3.216 E-0 3 0.0 -0.228 0.277 0.263

0.0450 3 . 697E+00 2.563E-02 3 . 723E+0 0 7.271 E-03 3.586E-03 0.0 -0.222 0.267 0.255

0.0500 3 . 447E+00 2.621 E-02 3 . 474E+00 8 . 662E-03 3. 949E-03 0.0 -0.218 0.259 0.248

0.0550 3 . 238E+00 2.675E-02 3 . 265E+00 1 .01 5E-02 4.306 E-0 3 0.0 -0.213 0.253 0.242

0.0600 3 . 060E+00 2 . 724E-02 3 . 087E+00 1 . 1 72E-02 4.656E-03 0.0 -0.210 0.247 0.237

0.0700 2 . 773E+00 2.81 4E-02 2 . 802E+00 1 .513E-02 5 . 339E-03 0.0 -0.203 0.237 0.229

0.0800 2 . 552E+00 2 . 896E-02 2.581 E+00 1 . 885E-02 6.001 E-0 3 0.0 -0.198 0.230 0.222

0.0900 2. 376E+00 2. 970E-02 2 . 406E+00 2.287E-02 6 . 644E-03 0.0 -0.194 0.223 0.217

0.1000 2.233E+00 3 . 039E-02 2 . 264E+00 2.716E-02 7.268E-03 0.0 -0.190 0.218 0.212

0.1250 1 . 970E+00 3.1 96E-02 2 . 002E+00 3.895E-02 8.757E-03 0.0 -0.183 0.208 0.202

0.1500 1 .791 E+00 3.337E-02 1 . 824E+00 5 . 206E-02 1 .01 5E-02 0.0 -0.177 0.200 0.195

0.1750 1 .661 E+00 3 . 467E-02 1 . 6 96 E+0 0 6 . 630E-02 1 . 147E-02 0.0 -0.173 0.194 0.189

0.2000 1 . 564E+00 3 . 593E-02 1 . 600E+00 8.149E-02 1 . 272E-02 0.0 -0.169 0.189 0.185

0.2500 1 . 429E+00 3 . 839E-02 1 . 467E+00 1 . 1 42E-0

1

1 . 505E-02 2. 448E-04 -0.161 0.181 0.177

0.3000 1 . 340E+00 4.087E-02 1 . 381 E+00 1 . 494E-0

1

1 .71 9E-02 4 . 939E-03 -0.154 0.174 0.170

0.3500 1 . 279E+00 4 . 342E-02 1 . 322E+00 1 . 865E-0

1

1 . 91 9E-02 1 . 113E-02 -0.148 0.169 0.165

0.4000 1 . 235E+00 4 . 606E-02 1 . 281 E+00 2.249E-01 2.1 10E-02 1 . 844E-02 -0.143 0.164 0.160

0.4500 1 . 202E+00 4.879E-02 1 . 251 E+00 2.645E-01 2 . 292E-02 2 . 646E-02 -0.139 0.160 0.155

0.5000 1 . 178E+00 5.161 E-02 1 . 229E+00 3.048E-01 2 . 468E-02 3 . 493E-02 -0.135 0.156 0.151 0.5500 1 . 159E+00 5.449E-02 1 .214E+00 3.457E-01 2 . 638E-02 4.373E-02 -0.132 0.152 0.148

0.6000 1 . 1 45E+00 5 . 745E-02 1 . 202E+00 3.871E-01 2.804E-02 5 . 275E-02 -0.129 0.149 0.145

0.7000 1 . 126E+00 6 . 355E-02 1 . 189E+00 4 . 708E-0

1

3.127E-02 7. 128E-02 -0.124 0.144 0.139

0.8000 1 . 1 1 4E+00 6 . 987E-02 1 . 1 84E+00 5.551E-01 3 . 439E-02 9.021 E-02 -0.120 0.140 0 . 1 34 0.9000 1 . 108E + 00 7 . 639E-02 1 . 184E+00 6.396E-01 3 . 743E-02 1 . 094E-0

1

-0.116 0.136 0.130

1 .0000 1 . 105E+00 8 . 308E-02 1 . 188E+00 7.239E-01 4.041 E-02 1 . 286E-0

1

-0.113 0.133 0.126

1 .2500 1 . 1 06E + 00 1 .005E-01 1 . 207E+00 9.329E-01 4.766E-02 1 . 767E-0

1

-0.106 0.126 0.118

1 .5000 1 . 1 13E+00 1 . 139E-01 1 . 232E+00 1 . 1 33E+00 5 . 470E-02 2.245E-01 -0.101 0.120 0.111

1 .7500 1 . 1 23E+00 1 -379E-01 1 .261 E+00 1 . 339E+00 6 . 1 59E-02 2.717E-01 -0.096 0.115 0.106

2.0000 1 . 1 33E+00 1 . 574E-0

1

1 . 291 E+00 1 . 535E+00 6 . 835E-02 3. 183E-01 -0.091 0.111 0.101 2.5000 1 . 1 54E+00 1 . 979E-01 1 . 352E+00 1 . 91 3E+00 8.1 54E-02 4.090E-01 -0.084 0.104 0.093

3.0000 1 . 173E+00 2.399E-01 1 . 4 1 3E+00 2 . 275E+00 9.431 E-02 4.962E-01 -0.079 0.098 0 .086 3.5000 1 .191 E+00 2.829E-01 1 . 474E+00 2.621 E+00 1 . 0 67E-0

1

5 . 797E-0

1

-0.074 0.094 0.080

4.0000 1 . 207E+00 3.268E-01 1 . 534E+00 2. 954E+00 1 . 187E-01 6 . 592E-0

1

-0.071 0.090 0.076

4.5000 1 . 22 1 E+00 3.715E-01 1 . 593E+00 3 . 274E+00 1 .303E-01 7.349E-01 -0.067 0.086 0.071 5.0000 1 . 234E+00 4. 169E-01 1 . 651 E+00 3 . 582E+0 0 1 . 4 1 6 E-0

1

8 . 070 E-0

1

-0.065 0.083 0 .068 5.5000 1 . 246E+00 4.630E-01 1 . 7 0 9E+00 3.879E+00 1 . 525E-0

1

8 . 758E-0

1

-0.062 0.080 0.064

6.0000 1 . 257E+00 5.095E-01 1 . 767E+00 4. 167E+00 1 .631 E-0

1

9.414E-01 -0.060 0.078 0.062

7.0000 1 . 277E+00 6.041E-01 1 . 88 1 E+00 4.71 6E+00 1 . 834E-0

1

1 . 064E+00 -0 .057 0 .073 0.057 8.0000 1 . 293E+00 7.003E-01 1 . 994E+00 5 . 232E+00 2.025E-01 1 . 178E+00 -0.054 0.070 0.052

9.0000 1 . 308E+00 7.979E-01 2 . 1 06E+00 5 . 720E+00 2.206E-01 1 . 283E+00 -0.051 0.067 0.049

10.0000 1 . 321 E+00 8.967E-01 2.21 8E+00 6 . 182E+00 2.377E-01 1 . 381 E+00 -0.049 0.064 0.046

12.5000 1 . 348E+00 1 . 148E+00 2 . 497E+00 7 . 244E+00 2 . 768E-0

1

1 . 602E+00 -0.044 0.059 0.040

15.0000 1 . 370E+00 1 . 404E+00 2 . 774E+00 8.1 94E+00 3. 1 12E-01 1 . 7 98E+0 0 -0.040 0.054 0.035

17.5000 1 . 388E+00 1 . 665E+00 3 . 053E+00 9 . 052E+00 3 . 420E-0

1

1 . 973E+00 -0.037 0.051 0.032

20.0000 1 . 403E+00 1 . 928E+00 3.331 E+00 9 . 836 E+00 3.695E-01 2.1 34E+00 -0.034 0.048 0.028

25.0000 1 . 427E+00 2 . 463E+00 3 . 890 E+00 1 . 122E+01 4.171 E-0

1

2 . 420E+00 -0.029 0.044 0.024

30 .0000 1 . 446E+00 3 . 006E+00 4.451 E+00 1 . 242E+0

1

4.567E-01 2 . 668E+00 -0.026 0.040 0.020 35.0000 1 .461 E+00 3 . 555E+00 5 . 0 1 6 E+0 0 1 . 348E+0

1

4. 904E-01 2 . 888E+00 -0.023 0.033 0.018

40.0000 1 . 474E+00 4. 109E+00 5 . 583E+00 1 . 443E+0

1

5.1 95E-01 3 . 085E+00 -0.021 0.036 0.016 45.0000 1 . 485E+00 4 . 667 E+00 6. 152E+00 1 .528E+01 5.448E-01 3 . 264E+00 -0.020 0.034 0.014

50.0000 1 . 495E+00 5 . 228E + 0 0 6 . 723E+00 1 . 606E+0

1

5 . 672E-0

1

3 . 427E+00 -0.018 0.033 0.013

55.0000 1 . 503E+00 5 . 7 92E+00 7 . 296E+00 1 . 677E+0

1

5.871 E-0

1

3 . 577E+00 -0.017 0.031 0.012

60.0000 1.511 E+00 6 . 359E+00 7.870 E+00 1 . 743E+0

1

6 . 049E-0

1

3 . 7 1 6 E+0 0 -0.016 0 .030 0.011 70.0000 1 . 524E+00 7 . 498E+00 9 . 0 23E+00 1 . 862E+0

1

6 . 356 E-0

1

3 . 967E+00 -0.015 0 .029 0.009

80.0000 1 . 536E+00 8 . 644E+00 1 .018E+01 1 . 966E+01 6.612E-01 4. 188E+00 -0.013 0.027 0.008

90.0000 1 . 546E+00 9 . 7 95E+00 1 . 134E+01 2 . 059E+0

1

6 . 830E-0

1

4. 387E+00 -0.012 0.026 0.007

100.0000 1 . 554E+00 1 . 0 95E+0

1

1 .251E+01 2.143E+01 7.016E-01 4 . 567E+00 -0.011 0.025 0.007

125.0000 1 . 572E+00 1 . 385E+01 1 . 543E+0

1

2 . 323E+0

1

7 . 388E-0

1

4 . 957E+00 -0.009 0.023 0.005

150.0000 1 . 586E+00 1 . 677E+0

1

1 . 836E+0

1

2.471 E+0

1

7.668E-01 5 . 283E+00 -0.008 0.022 0.004

175.0000 1 . 5 93E+0 0 1 . 970E+01 2.1 30E+01 2 . 597E+0

1

7 . 886E-0

1

5 . 562E+00 -0.007 0.021 0 .004 200.0000 1 . 608E+00 2 .264E+01 2 . 424E+0

1

2.707E+01 8.062E-01 5 . 808E+00 -0.006 0.020 0.003 250.0000 1 . 624E+00 2 . 852E+01 3.015E+01 2.892E+01 8 . 330E-0

1

6 . 223E+00 -0.005 0.019 0.003

300 . 0000 1 . 637E+00 3 . 443E+0

1

3 . 607E+0

1

3 . 043E+0

1

8 . 526 E-0

1

6 . 567E+00 -0 .004 0.018 0.002

350.0000 1 . 643E+00 4 . 034E+0

1

4.1 99E+01 3.172E+01 8 . 677E-0

1

6 .860E+00 -0.004 0.017 0.002

400.0000 1 . 657E+00 4 . 627E+01 4 . 792E+0

1

3 . 283E+0

1

8.796E-01 7.1 15E+00 -0.003 0.017 0.002

450.0000 1 . 66 5E + 00 5 . 220E+0

1

5 . 386E+0

1

3.381 E+0

1

8.893E-01 7 . 342E+00 -0.003 0.016 0.002

500.0000 1 . 672E+00 5.81 3E+01 5. 981 E+01 3.469E+01 8. 975E-01 7 . 545E+00 -0.003 0.016 0.001 550.0000 1 . 679E + 00 6 . 407E+0

1

6 . 575E+0

1

3.549E+01 9 . 044E-01 7 . 729E+00 -0.002 0.015 0.001 600.0000 1 . 685E + 00 7 . 002E+0

1

7. 171E+01 3 . 622E+0

1

9. 1 03E-01 7 . 898E+00 -0.002 0.015 0.001 700.0000 1 . 6 95E + 00 8. 192E+01 8.361E+01 3.751 E+0

1

9 . 20 0 E-0

1

8 . 1 98E+00 -0.002 0.015 0.001 800.0000 1 . 704E + 00 9.383E+01 9 . 553E+0

1

3.863E+01 9 . 276E-0

1

8 . 459E+00 -0.002 0.014 0.001 900.0000 1 . 7 1 2E+0 0 1 . 057E+02 1 . 075E+02 3.961 E+0

1

9 . 338E-0

1

8 . 6 90 E+00 -0.001 0.014 0.001 1000.0000 1 .71 9E+00 1 . 177E+02 1 . 1 94E+02 4 . 050E+0

1

9.389E-01 8 . 897E+00 -0.001 0.013 0.001

120

J
ELECTRONS IN ETHYLENE

I = 50.7 eV DENSITY = 1.175E-03 g/cm 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV ci» :/g MeV cm 2/g MeV cm 2/g g/cm 2 0.0100 2.499E+01 2.837E-03 2 . 499E+01 2 . 248E-04 6 . 226E-05 0.0 -0.184 0.208 0 . 207 0.0125 2. 095E+01 2.847E-03 2.095E+01 3 . 345E-04 7.476E-05 0.0 -0.177 0.199 0.198

0.0150 1 .814E+01 2 . 854E-03 1 .814E+01 4.631E-04 8.675E-05 0.0 -0.172 0.192 0.191 0.0175 1 .607E+01 2.360E-03 1 . 607E+01 6 . 098E-04 9.831E-05 0.0 -0.167 0.187 0.186 0.0200 1 . 447E+0

1

2.364E-03 1 . 447E+0

1

7.741E-04 1 .095E-04 0.0 -0.164 0.132 0.182

0.0250 1 .215E+01 2.873E-03 1 .216E+01 1 . 153E-03 1 .31 IE-04 0.0 -0.158 0.175 0.175

0.0300 1 . 056E+0

1

2 . 383E-0 3 1 . 056E+0

1

1 . 596E-03 1 . 5 1 7E-04 0 .

0

-0.154 0.170 0.170 0.0350 9 . 382E+00 2.894E-03 9 . 335E+00 2.099E-03 1 .716E-04 0 .

0

-0.151 0.166 0.165

0 .0400 3 . 482E+0 0 2. 905E-03 8 . 485E+00 2.660E-03 1 . 908E-04 0.0 -0.148 0.162 0.162

0.0450 7 . 768E+00 2.918E-03 7.771 E+00 3.277E-03 2 . 0 95E-04 0.0 -0.145 0.159 0.159

0 .0500 7. 133E+00 2 . 931 E-03 7 . 1 91 E+00 3. 946E-03 2.277E-04 0 .

0

-0.143 0.157 0.156 0.0550 6 . 707E+00 2.945E-03 6.710E+00 4.667E-03 2. 455E-04 0 .

0

-0.141 0.154 0.154

0.0600 6 . 301 E+00 2. 960E-03 6 . 304E+00 5.436E-03 2.629E-04 0.0 -0.140 0.152 0.152

0.0700 5 . 654E+00 2 . 992E-03 5 . 657E+00 7.1 14E-03 2. 967E-04 0.0 -0.137 0.149 0.149

0.0800 5. 160E+00 3.025E-03 5. 163E+00 8. 967E-03 3 . 293E-04 0.0 -0.135 0 . 1 46 0.146 0.0900 4.771 E+00 3.061 E-03 4 . 774E+00 1 . 0 98E-02 3.609E-04 0.0 -0.133 0.144 0.144

0.1000 4 . 457E+00 3.099E-03 4 . 460E+00 1 .315E-02 3. 91 6E-04 0.0 -0.131 0.142 0.142

0.1250 3 . 884E+00 3.201 E-03 3 . 887E+00 1 .918E-02 4 . 652E-04 0.0 -0 . 1 27 0.138 0.137

0.1500 3 . 497E+00 3.312E-03 3.501 E+00 2 . 593E-02 5. 352E-04 0.0 -0.125 0.135 0.134

0.1750 3 . 220E+00 3.429E-03 3 . 223E+00 3.343E-02 6 . 024E-04 0.0 -0.122 0.132 0.132

0.2000 3.01 2E + 00 3 . 553E-03 3.01 5E+00 4.146E-02 6 . 672E-04 0.0 -0.120 0.130 0.129

0.2500 2.723E+00 3 . 820E-03 2 . 727E+00 5 . 896E-02 7.91 8E-04 0 .

0

-0.117 0.127 0.126 0.3000 2 . 534E+00 4.11 OE-03 2 . 538E+00 7.801E-02 9. 1 16E-04 0.0 -0.115 0.124 0.123

0.3500 2 . 402E+00 4.420E-03 2 . 407E+00 9.827E-02 1 . 028E-03 0.0 -0.113 0.122 0.121 0.4000 2 . 307E+00 4.750E-03 2.31 2E+00 1 . 1 95E-01 1 .143E-03 0.0 -0.111 0.120 0.119

0.4500 2 . 236 E+00 5.098E-03 2.241 E+00 1 .415E-01 1 .256E-03 0.0 -0.109 0.118 0.117

0.5000 2. 182E+00 5.462E-03 2. 188E+00 1 .641 E-01 1 . 369E-03 0.0 -0.108 0.117 0.116 0.5500 2.141 E+00 5.841 E-03 2. 146E+00 1 .871 E-01 1 . 482E-0 3 0.0 -0.107 0.116 0.114

0.6000 2. 108E+00 6 . 233E-03 2.11 4E+00 2. 106E-01 1 . 595E-03 0.0 -0.105 0.115 0.113

0.7000 2.061 E+00 7.053E-03 2 . 068E+00 2 . 585E-0

1

1 .821 E-03 0 .

0

-0.103 0.113 0.111 0.8000 2 . 032E+00 7.915E-03 2 . 040E+00 3 . 072E-0

1

2 . 049E-03 0.0 -0.102 0.111 0.109

0 . 9000 2.01 3E+00 8.816E-03 2. 022E+00 3.565E-01 2.279E-03 0.0 -0.100 0.110 0.107

1 .0000 2 . 002E+00 9 . 754E-03 2.01 1E+00 4.061E-01 2.51 IE-03 0.0 -0.099 0.108 0.106

1 .2500 1 . 992E+00 1 . 224E-02 2 . 004E+00 5.307E-01 3.104E-03 0.0 -0.096 0.106 0.103

1 .5000 1 . 996E+00 1 . 490E-02 2.01 1 E+00 6.553E-01 3.712E-03 0 .

0

-0.094 0.103 0.100

1.7500 2 . 007E+00 1 . 770E-02 2 . 024E+00 7.792E-01 4 . 335E-03 0.0 -0.092 0.102 0.098

2.0000 2.021 E+00 2 . 062E-02 2 .041 E+00 9.022E-01 4.971E-03 0.0 -0.091 0.100 0.096 2.5000 2.051 E+00 2 . 678E-02 2 . 078E+00 1 . 1 45E+00 6 . 275E-03 0.0 -0 .088 0.098 0.093

3.0000 2 . 082E+00 3 . 327E-02 2.11 5E+00 1 . 383E+00 7.613E-03 0 .

0

-0.086 0.096 0.091 3.5000 2.1 1 1E+00 4.004E-02 2.151 E+00 1 . 6 1 8E+00 8 . 977E-03 0.0 -0.084 0.094 0.089 4.0000 2. 139E+00 4 . 704E-02 2 . 1 86E+00 1 . 848E+00 1 . 036E-02 0.0 -0.083 0.092 0.087 4.5000 2. 164E+00 5 . 424E-02 2.21 8E+00 2 . 075E+00 1 . 1 77E-02 0.0 -0 . 082 0.091 0.086 5.0000 2 . 1 87E+00 6.162E-02 2 . 249E+00 2 . 299E+00 1 .318E-02 0.0 -0.081 0.090 0.085

5.5000 2 . 209E+00 6.91 6E-02 2 . 278E+00 2 . 520 E + 00 1 .461 E-02 0.0 -0 .080 0.089 0.083

6.0000 2.229E+00 7 . 684E-02 2.306E+00 2 . 738E+0 0 1 . 604E-02 0.0 -0.079 0.088 0.082 7.0000 2 . 266E+00 9.259E-02 2 . 358E+0 0 3. 167E+00 1 .894E-02 0.0 -0.078 0.086 0.080 8.0000 2 . 298E+00 1 .088E-01 2 . 407E+00 3 . 587E+00 2. 135E-02 0.0 -0.077 0.085 0.079

9.0000 2 . 327E+00 1 . 253E-0

1

2 . 453E+00 3. 998E+00 2.477E-02 0.0 -0.076 0.034 0.077 10.0000 2 . 354E+00 1 . 422E-0

1

2 . 496 E+00 4 . 402E+00 2.770E-02 0.0 -0.075 0.082 0.076 12.5000 2.41 0E+0O 1 . 855E-0

1

2.595E+00 5 . 384E+00 3.500E-02 0.0 -0.073 0.080 0.074

15.0000 2 . 456E + 0 0 2.301E-01 2 . 687E+00 6.331 E+00 4 . 227E-0 2 0.0 -0.071 0.078 0.071 17.5000 2 . 4 96E+0 0 2.757E-01 2 . 772E+00 7 . 247E+00 4.945E-02 0.0 -0.070 0.076 0.069

20.0000 2 . 529E+00 3.220E-01 2.851 E+00 8.1 36E+00 5.655E-02 1 . 778E-02 -0.059 0 .074 0.067

25.0000 2 . 577E+0 0 4.166E-01 2 . 994E+00 9 . 846E+00 7 . 047E-02 1 . 288E-0

1

-0.044 0.069 0.059 30.0000 2.612E+00 5.129E-01 3 . 1 25E+00 1 . 1 48E+01 8.401 E-02 2.760E-01 -0.036 0.064 0.051 35.0000 2 . 639E+00 6. 105E-01 3 . 249E+00 1 . 305E+0

1

9.717 E-02 4.292E-01 -0.031 0.060 0.045 40.0000 2 . 660E+00 7.092E-01 3 . 370E+00 1 . 456E+01 1 .099E-01 5.780E-01 -0.027 0.056 0.040 45.0000 2.679E+00 8 . 088E-0

1

3. 438E+00 1 .602E+01 1 . 223E-0

1

7 . 1 91 E-01 -0.025 0.053 0.036 50.0000 2 . 6 95E + 00 9.092E-01 3 . 604E+00 1 . 743E+0

1

1 . 343E-0

1

8 . 51 6E-01 -0.023 0.050 0.033

55.0000 2.70 9E + 00 1 . 0 1 0E+00 3.71 9E+00 1 .879E+01 1 .459E-01 9 . 757E-01 -0.022 0.047 0.030 60.0000 2 . 722E+00 1 . 1 12E+00 3 . 833E+00 2.012E+01 1 . 572E-0

1

1 . 0 92E + 00 -0.021 0.045 0.028

70 .0000 2 . 743E+00 1 . 31 6 E+00 4 . 060E+00 2.265E+01 1 .786E-01 1 . 304E+00 -0.019 0.042 0.024 80.0000 2.762E+00 1 . 522E+00 4 . 284E+00 2 . 505E+0

1

1 . 988E-01 1 . 492E+00 -0.018 0.039 0.022

90.0000 2 . 778E+00 1 . 730E+00 4 . 508E+0 0 2 . 733E+0

1

2.1 78E-01 1 . 662E+00 -0.017 0.037 0.020 100.0000 2 . 7 92E + 00 1 . 938E+00 4 . 730E+00 2.949E+01 2.357E-01 1 .81 6E+00 -0.017 0.035 0.018

125.0000 2 . 822E+00 2.463E+00 5 . 234E+00 3.449E+01 2.763E-01 2. 148E+00 -0.015 0.031 0.015

150.0000 2 . 845E + 0 0 2. 991 E+00 5.837E+00 3.899E+01 3.11 9E-01 2 . 425E+00 -0.014 0.028 0.013

175.0000 2 . 865E+00 3 . 523E+00 6 . 388E+00 4 . 308E+0

1

3 . 434E-0

1

2 . 664E+00 -0.013 0.026 0.012 200.0000 2.881 E+00 4 . 057E+00 6 . 939E+00 4 . 684E+0

1

3.716 E-01 2 . 87 5E + 0 0 -0.012 0.025 0.011 250.0000 2. 908E+00 5.131 E+00 8 . 040E+00 5 . 352E+0

1

4.1 98E-01 3 . 235E+00 -0.011 0.022 0.009 300.0000 2 . 930 E+00 6.210E+00 9. 140E+00 5 . 935E+0

1

4.598E-01 3 . 539E+00 -0.009 0.020 0.008 350.0000 2. 947E+00 7 . 294E+00 1 . 024E+0

1

6 . 452E+0

1

4. 936E-01 3.802E+00 -0.008 0.019 0.007 400.0000 2. 962E+00 8. 380E+00 1 . 1 34E+0

1

6.915E+01 5.226E-01 4 . 0 36E+00 -0.007 0.018 0.006

450 .0000 2 . 974E+00 9.469E+00 1 .244E+01 7.336E+01 5.479E-01 4 . 246E+00 -0.006 0.017 0.005 500.0000 2. 985E+00 1 . 056E+0

1

1 . 354E+0

1

7.721 E+0

1

5 . 702E-0

1

4 . 43SE+00 -0.005 0.016 0.005 550.0000 2 . 995E+00 1 .165E+01 1 .465E+01 8.076E+01 5.900E-01 4.61 3E+00 -0.004 0.015 0.004 600.0000 3 . 004E+00 1 . 275E+01 1 . 575E+0

1

8.405E+01 6 . 077E-01 4 . 775E + 0 0 -0.004 0.015 0.004 700.0000 3.01 9E+00 1 . 494E+0

1

1 . 7 96E+0

1

9 . 000 E+0

1

6.382E-01 5 . 065E+00 -0.003 0.014 0.003 800.0000 3.031 E+00 1 .71 3E+01 2.01 6E+01 9.525E+01 6.635E-01 5 . 320E+00 -0.002 0.013 0.003

900.0000 3 . 042E+00 1 . 933E+01 2 . 237E+0

1

9.995E+01 6 . 850E-0

1

5 . 547E+00 -0.002 0.013 0.002 1000.0000 3 . 052E+00 2. 153E+01 2 . 458E+0

1

1 . 042E+02 7.035E-01 5.751 E+00 -0.002 0.012 0.002

121
ELECTRONS IN FERROUS SULFATE DOSIMETER SOLUTION

l

I = 76.4 eV DENSITY = 1 . 024E+00' g/cn 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV c» 2 /g MeV cm 2/g MeV cra 2/g g/cn 2 0.0100 2.241 E+0

1

3. 961 E-03 2.241 E+01 2 . 533E-04 9 . 61 5E-05 0 .

0

-0.200 0.228 0.226 0.0125 1 . 885E+0

1

3. 993E-03 1 . 835E+0

1

3 . 755E-04 1 .155E-04 0.0 -0.191 0.217 0.216 0.0150 1 . 636E+0

1

4.012E-03 1 . 636E+0

1

5. 183E-04 1 . 346E-04 0 .

0

-0.185 0.209 0 . 208 0.0175 1 . 452E+0

1

4.025E-03 1 . 452E+0

1

6.808E-04 1 . 527E-04 0.0 -0.180 0.203 0 .202 0.0200 1 .309E+01 4.034E-03 1 .309E+01 8.624E-04 1 . 702E-04 0.0 -0.176 0.197 0.196 0.0250 1 . 102E+01 4 . 047E-03 1 . 1 03E+01 1 . 280E-03 2.037E-04 0.0 -0.169 0.189 0.188

0.0300 9 . 594E+00 4.058E-03 9 . 598E+00 1 . 7 68E-0 3 2 . 356E-04 0.0 -0.164 0.183 0.182

0.0350 8 . 540E+00 4.069E-03 8 . 544E+00 2.321 E-03 2.662E-04 0 . 0 -0.160 0.178 0.177

0 .0400 7 . 730E+00 4.031 E-03 7 . 734E+00 2 . 937E-0 3 2. 957E-04 0.0 -0.157 0.174 0.173

0.0450 7 . 087E+00 4.094E-03 7.091 E+00 3.613E-03 3 . 242E-04 0 .

0

-0.154 0.171 0.170

0.0500 6 . 564E+00 4. 108E-03 6 . 568E+00 4.347E-03 3.520E-04 0 .

0

-0.152 0.168 0.167

0.0550 6.129E+00 4 . 1 23E-03 6 . 1 34E+00 5.1 35E-03 3.790E-04 0 .

0

-0.150 0.165 0.165

0.0600 5 . 763E+00 4. 140E-03 5 . 767E+00 5.976E-03 4.053E-04 0 .

0

-0.148 0.163 0.162

0.0700 5. 177E+00 4.176E-03 5.181 E+00 7 .810E-03 4.563E-04 0.0 -0.145 0.159 0.159

0.0800 4 . 730E+00 4.216E-03 4 . 734E+00 9.832E-03 5 . 053E-04 0.0 -0.142 0.156 0.155

0.0900 4 . 377E+00 4.260E-03 4.381 E+00 1 . 20 3E-02 5 . 527E-04 0.0 -0.140 0.153 0.153

0.1000 4 . 092E+00 4 . 307E-03 4 . 0 96 E+0 0 1 . 439E-02 5 . 986E-04 0.0 -0.138 0.151 0.150

0.1250 3.571 E+00 4.436E-03 3.576E+00 2.095E-02 7.083E-04 0.0 -0.134 0.146 0.146 0.1500 3 . 220E+00 4.577E-03 3 . 224E+00 2.333E-02 8. 120E-04 0.0 -0.131 0.143 0.142

0.1750 2 . 967E+00 4.728E-03 2. 972E+00 3 . 643E-02 9.111E-04 0.0 -0.129 0.140 0.139

0.2000 2 . 778E+00 4.888E-03 2 . 783E+00 4.513E-02 1 . 007E-03 0.0 -0.127 0.137 0.137

0.2500 2.51 4E+00 5.233E-03 2 . 520E+00 6 . 408E-02 1 .189E-03 0.0 -0.123 0.134 0.133

0 . 3000 2 . 342E+00 5.61 IE-03 2 . 348E+00 8.468E-02 1 .363E-03 0 .

0

-0.120 0.131 0.130 0.3500 2 . 223E+00 6 .017E-03 2 . 229E+00 1 . 066E-0

1

1 . 532E-03 0.0 -0.118 0.128 0.127

0.4000 2 . 1 37E+00 6 . 448E-03 2 . 1 43E+00 1 . 295E-0

1

1 . 6 97E-0 3 0 .

0

-0.116 0.126 0.125

0 . 4500 2 . 072E+00 6 . 904E-03 2 . 079E+00 1 . 532E-0

1

1 .860E-03 0.0 -0.114 0.124 0.123

0.5000 2 . 023E+00 7.381 E-03 2.031 E+00 1 .775E-01 2.022E-03 0.0 -0.110 0.123 0.121 0.5500 1 . 984E+00 7 . 878E-03 1 . 992E+00 2.024E-01 2. 183E-03 1 . 262E-02 -0.094 0.120 0.118

0.6000 1 . 953E+00 8.392E-03 1 . 961 E+00 2.277E-01 2 . 344 E-03 3.1 36E-02 -0.088 0.117 0.114

0.7000 1 . 907E+00 9 . 466E-03 1 . 91 6E+00 2.793E-01 2 . 667E-03 7.687E-02 -0.078 0.110 0.106 0.8000 1 . 876E+00 1 . 060E-02 1 . 386E+00 3.31 9E-01 2.994E-03 1 . 295E-0

1

-0.070 0.105 0.099

0.9000 1 . 854E+00 1 . 178E-02 1 . 866E+00 3.852E-01 3.324E-03 1 . 864E-01 -0.064 0.099 0.093

1 .0000 1 . 839E+00 1 . 300E-02 1 .852E+00 4.390E-01 3.658E-03 2.457E-01 -0.059 0.095 0.087

1 .2500 1.81 9E+00 1 . 6 25E-0 2 1 . 835E+00 5.747E-01 4.512E-03 3. 970E-01 -0.050 0.085 0.075

1 .5000 1 . 81 2E+00 1 . 972E-02 1 . 832E+00 7.111 E— 0

1

5.394E-03 5.458E-01 -0.043 0 .077 0.066

1 .7500 1 . 8 1 2E+00 2 . 338E-02 1 .835E+00 8.475E-01 6 . 302E-03 6 . 880E-0

1

-0.039 0.071 0.059

2.0000 1 . 8 1 5E+00 2.71 9E-02 1 . 842E+00 9.835E-01 7.233E-03 8 . 225E-0

1

-0.035 0.067 0.054

2.5000 1 . 825E+00 3 . 520E-02 1 . 86 0 E + 0 0 1 . 254E+00 9. 1 53E-03 1 . 068E+00 -0.031 0.059 0.046 3.0000 1 . 837E+00 4.363E-02 1 . 88 1 E+00 1 .521 E+00 1 .114E-02 1 . 286 E+0 0 -0.028 0.054 0 .040 3.5000 1 . 84 9E+00 5 . 240E-02 1 . 902E+00 1 . 785E+00 1 .317E-02 1 . 481 E+00 -0.026 0.050 0.036 4.0000 1 . 86 1 E+00 6. 147E-02 1 . 923E+00 2 . 047E+00 1 . 524E-02 1 . 6 57E+00 -0.024 0.046 0.033

4.5000 1 . 87 3E+00 7 . 078E-02 1 . 944E+00 2. 306E+00 1 . 7 35E-0 2 1 .81 6E+00 -0.023 0.044 0.031 5.0000 1 . 383E+00 8.032E-02 1 . 964E+00 2.561 E+00 1 . 948E-02 1 . 962E+00 -0.022 0.042 0.029

5.5000 1 .893E+00 9.004E-02 1 . 983E+00 2.81 5E+00 2.163E-02 2 . 0 96 E+0 0 -0 . 022 0.040 0.028

6.0000 1 . 903E+00 9 . 995E-02 2 . 002E+00 3 . 066E+00 2.380E-02 2 . 220 E+00 -0.021 0.038 0.026 7.0000 1 . 91 9E+00 1 . 202E-0

1

2 . 040E+00 3.561 E+00 2.818E-02 2 . 445E+00 -0.020 0.036 0.025 3.0000 1 . 934E+00 1 .410E-01 2 . 075E+00 4 . 047E+00 3.259E-02 2 . 643E+00 -0.019 0.033 0 . 023 9.0000 1 . 947E+00 1 . 6 23E-0

1

2.11 0E+00 4 . 524E+00 3 . 702E-02 2.821 E+00 -0.018 0.032 0.022

10.0000 1 . 959E+00 1 . 840E-0

1

2 . 1 43E+00 4 . 995E+00 4. 145E-02 2 . 982E+00 -0.018 0.030 0.021 12.5000 1 . 985E+00 2.395E-01 2 . 224E+00 6.1 39E+00 5 . 252E-02 3 . 330E+00 -0.016 0.028 0.019

15.0000 2 . 005E+00 2. 966E-01 2 . 302E+00 7 . 244E+00 6 . 349E-02 3.621 E+00 -0.015 0.025 0.017

17.5000 2 . 022E+00 3.549E-01 2. 377E+00 8.313E+00 7.430E-02 3 . 873E+00 -0.014 0.024 0.016 20.0000 2 . 037E+00 4. 142E-01 2 . 451 E+00 9 . 348E+00 8.491E-02 4 . 0 95E + 00 -0.013 0.022 0.015

25.0000 2.061 E+00 5.348E-01 2 . 596E+00 1 . 133E+01 1 . 055E-0

1

4 . 474E+00 -0.010 0.020 0.013

30.0000 2 . 080E+00 6.575E-01 2 . 733E+00 1 . 320E+0

1

1 .251E-01 4 . 7 93E+00 -0.009 0.018 0.011 35.0000 2 . 0 96E+0 0 7.818E-01 2.878E+00 1 . 499E+0

1

1 .43SE-01 5 . 070E+00 -0.007 0.017 0.010 40.0000 2. 109E+00 9 . 073E-0

1

3.01 6E+00 1 . 668E+0

1

1 .617E-01 5.31 3E+00 -0.006 0.016 0.009 45.0000 2. 120E+00 1 . 0 34E+00 3. 154E+00 1 . 830E+0

1

1 .786E-01 5.531 E+00 -0.005 0.015 0.008 50.0000 2 . 1 30E+00 1.161 E+00 3 . 292E+00 1 . 986E+0

1

1 . 948E-01 5 . 728E+00 -0.004 0.014 0.007 55.0000 2. 1 39E+00 1 . 290E+00 3 . 429E+00 2.1 34E+01 2. 103E-01 5 . 908E+00 -0.004 0.013 0.006 60.0000 2. 147E+00 1 . 4 1 8E+00 3 . 566E+00 2 . 277E+01 2.250E-01 6 . 073E+00 -0.003 0.012 0.006 70.0000 2. 1 6 1 E+00 1 . 678E+00 3 . 839E+00 2 . 548E+0

1

2 . 525E-0

1

6 . 369E+00 -0.003 0.011 0.005 30.0000 2. 173E+00 1 . 939E+00 4.1 12E+00 2.799E+01 2.778E-01 6 . 627E+00 -0.002 0.010 0 . 004 90.0000 2. 184E+00 2.201 E+00 4 . 385E+00 3 . 035E+0

1

3.010E-01 6 . 857E+00 -0.002 0.010 0.004

100.0000 2.1 93E+00 2 . 465E+00 4 . 658E+00 3 . 256E+0

1

3.225E-01 7 . 063E+00 -0.001 0.009 0.003 125.0000 2.21 3E+00 3. 129E+00 5 . 342E+00 3 . 757E+0

1

3.698E-01 7.501 E+00 -0.001 0 .008 0.002

150.0000 2 . 229E+00 3 . 7 97E + 00 6 . 026E+00 4. 1 97E+01 4.096E-01 7.861 E+00 -0.001 0.007 0 . 002 175.0000 2 . 242E+00 4 . 468E+00 6 . 7 1 0E+00 4 . 5 90 E+0

1

4.437E-01 8 . 1 67E+00 -0.001 0.006 0 .002 200.0000 2 . 253E+00 5 . 1 43E+00 7 . 396E+00 4. 945E+01 4.734E-01 8 . 432E+00 -0.000 0.006 0.001 250.0000 2 . 273E+00 6 . 497E+00 8 . 770E+00 5 . 565E+0

1

5 . 226E-0

1

8 . 876 E+0 0 -0.000 0.005 0.001 300.0000 2. 288E+00 7 . 858E+00 1 .015E+01 6 . 0 94E+0

1

5.619E-01 9.239E+00 -0.000 0.005 0.001 350.0000 2.301 E+00 9 . 222E+00 1 . 152E+01 6 . 557E+0

1

5.942E-01 9 . 546E+00 -0.000 0.005 0.001 400.0000 2.31 3E+00 1 . 059E+0

1

1 . 290E+01 6 . 966E+0

1

6.213E-01 9.812E+00 -0.000 0.004 0.001 450.0000 2 . 323E+00 1 . 1 96E+01 1 . 428E+0

1

7 . 334E+0

1

6.444E-01 1 . 005E+0

1

-0.000 0.004 0.001 500.0000 2. 332E+00 1 . 333E+01 1 . 567E+0

1

7 . 669E+0

1

6 . 644E-01 1 . 026E+0

1

-0.000 0.004 0.000 550.0000 2 . 34 0 E+00 1 . 47 1 E+0

1

1 . 705E+0

1

7 . 974E+0

1

6.81 9E-01 1 . 045E+0

1

-0.000 0.004 0.000 600.0000 2 . 347E+00 1 . 6 08E+0

1

1 . 843E+0

1

8 . 256E+0

1

6 . 974E-01 1 . 062E+0

1

-0 .000 0.004 0.000

700 .0000 2.361 E+00 1 . 884E+0

1

2. 120E+01 8.762E+01 7.236E-01 1 .093E+01 -0.000 0.003 0.000 800.0000 2 . 372E+00 2. 1 60E+01 2.397E+01 9 . 205E+0

1

7 . 451 E-01 1 . 1 20E+01 -0.000 0.003 0.000

900.0000 2 . 382E+00 2 . 436E+0

1

2.674E+01 9 . 600E+0

1

7.630E-01 1 . 143E+01 -0.000 0.003 0.000

1 000.0000 2.391 E+00 2.71 3E+01 2 . 952E+0

1

9. 956E+01 7 . 78ZE-0

1

1 . 1 64E+01 - 0.000 0.003 0.000

122

d
ELECTRONS IN GLASS, BOROSILICATE ("PYREX", CORNING 77A0)

I = 1 3 A . 0 eV DENSITY = 2.230E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log )/d(

:

logl) COLLISION RADIATIVE TOTAL RANGE YIELD COP.R. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2/g PleV cm 2 /g g/cm 2 0.0100 1 . 787E+0

1

5. A00E-03 1 . 788E+01 3.237E-0A 1 . 632E-0A 0 . 0 -0 . 225 0 .26A 0.260 0.0125 1 . 51 1 E + 01 5. A88E-03 1 .512E+01 A.76AE-0A 1 .971E-0A 0.0 -0.21A 0.250 0.2A6 0.0150 1 .317E + 01 5.5A8E-03 1 .317E+01 6 . 5A0E-0A 2.296E-0A 0.0 -0 . 206 0.239 0.236 0.0175 1 . 172E + 01 5 . 593E-03 1 . 173E + 01 8.556E-0A 2.610E-0A 0 .

0

-0.200 0.230 0.228

0.0200 1 .060E+01 5.626E-03 1 . 060E + 0

1

1 .080E-03 2.91AE-0A 0.0 -0.195 0.223 0.221 0.0250 8 . 962E+00 5.67AE-03 8. 968E + 00 1 .595E-03 3. A95E-0A 0.0 -0.187 0.213 0.211

0 .0300 7 . 822E+00 5.707E-03 7 . 828E+00 2. 1 9AE-03 A.0A8E-0A 0 .

0

-0.181 0.205 0.203

0.0350 6 . 980E+00 5 . 735E-03 6 . 986E+00 2.871E-03 A.578E-0A 0 .

0

-0.176 0.199 0.1 97 O.OAOO 6.331E+00 5.759E-03 6 . 336E + 00 3.62AE-03 5.087E-0A 0.0 -0.172 0 . 1 9A 0.192

0 . OA50 5.81 AE+00 5.781E-03 5 . 820E+00 A . AA3E-03 5 . 579E-0A 0.0 -0.169 0.189 0.188

0.0500 5 . 393E+00 5.803E-03 5. 398E+00 5.3A1E-03 6 . 055E-0A 0 . 0 -0.166 0.186 0.185

0 .0550 5 . 0A2E+00 5.82AE-03 5 . 0A3E+00 6 . 300E-03 6.518E-0A 0 . 0 -0 . 1 6A 0.182 0.182

0.0600 A.7A6E+00 5 . 8 A7E-0 3 A . 7 52E + 0 0 7 . 321 E-03 6.968E-0A 0.0 -0.162 0.180 0.179

0.0700 A . 272E+00 5.893E-03 A . 278E + 00 9.5AAE-03 7.837E-0A 0 .

0

-0.158 0 . 1 75 0.1 7A 0.0800 3. 909E+00 5.9A3E-03 3.91 5E+00 1 . 1 99E-02 8.668E-0A 0.0 -0.155 0.171 0.170 0.0900 3 . 622E+00 5. 997E-03 3 . 628E+00 1 . A65E-02 9.A67E-0A 0.0 -0.152 0.168 0.167

0.1000 3 . 390E+00 6.055E-03 3 . 396E+00 1 . 750E-02 1 . 02AE-03 0.0 -0.150 0.165 0 . 1 6 A 0.1250 2. 966E+00 6.215E-03 2 . 972E+00 2 . 5 A0E-02 1 . 207E-03 0.0 -0 . 1 A5 0.159 0.159

0.1500 2. 679E+00 6 . 393E-03 2 . 685E+00 3. A27E-02 1 .379E-03 0.0 -0.1A2 0.155 0.155

0.1750 2 . A73E+00 6 . 588E-03 2. A79E+00 A.398E-02 1 . 5 A2E-0 3 0.0 -0.139 0.152 0.151

0 . 2000 2.318E+00 6 .796E-03 2. 325E+00 5. AA0E-02 1 .698E-03 0.0 -0.136 0 . 1 A9 0. 1 A8 0.2500 2.1 02E+00 7.250E-03 2.11 OE+OO 7.706E-02 1 . 995E-03 0 .

0

-0.132 0. 1 A5 0 . 1 AA

0 . 3000 1 . 962E+00 7.7A9E-03 1 . 970E+00 1 .016E-01 2.277E-03 0.0 -0.129 0 . 1 A

1

0 . 1 AO 0.3500 1 . 86 AE+OO 8 . 286E-03 1 . 873E+00 1 . 277E-0

1

2.5A9E-03 0.0 -0.127 0.138 0.137

O.AOOO 1 . 793E+00 8 .857E-03 1 .802E+00 1 . 5A9E-0

1

2.81 AE-03 8. 985E-03 -0.110 0.135 0.133

0 .A500 1 . 739E+00 9. A61 E-03 1 . 7A9E+00 1 .331 E-01 3.075E-03 2 . 665E-02 -0.105 0.130 0.128

0.5000 1 . 6 98E + 00 1 . 009E-02 1 . 708E+00 2.121E-01 3 . 333E-03 A.637E-02 -0.100 0.126 0.12A

0.5500 1 . 665E+00 1 . 075E-02 1 . 67 6E+00 2.A16E-01 3.590E-03 6 . 760E-02 -0.095 0.123 0.119 0.6000 1 . 6A0E+00 1 . 1 A3E-02 1 . 65 1 E+00 2.717E-01 3.8A6E-03 8. 997E-02 -0.091 0.119 0.115

0.7000 1 . 60 3E+00 1 . 285E-02 1 .616E+00 3.330E-01 A.359E-03 1 .371E-01 -0.085 0 . 1 1 A 0.109

0.8000 1 . 57 9E+00 1 . A3AE-02 1 . 593E+00 3.953E-01 A . 873E-03 1 .860E-01 -0.080 0.108 0.103

0 . 9000 1 . 563E+00 1 .590E-02 1 . 57 9E+00 A.58AE-01 5.391 E-03 2.359E-01 -0.075 0.10A 0.098

1 .0000 1 . 552E+00 1 .751E-02 1 . 570E+00 5.220E-01 5.913E-03 2.859E-01 -0.072 0.100 0.093

1 .2500 1 . 5A0E+00 2. 179E-02 1 . 56 1 E+00 6.818E-01 7 . 2A0E-03 A.090E-01 -0.06A 0.092 0 . 08 A

1 .5000 1 . 538E+00 2 . 6 36E-02 1 . 56 AE+00 8 . A13E-01 8.599E-03 5.271 E-01 -0.059 0.086 0.077

1 .7500 1 .5A1E+00 3.11 7E-02 1 . 572E+00 1 .001 E+00 9. 990E-03 6 . 390E-01 -0.055 0.082 0.072

2.0000 1 .5A7E+00 3.61 7E-02 1 . 583E+0 0 1 . 1 60E+00 1 .1A1E-02 7.AA8E-01 -0.052 0.078 0 .067 2.5000 1 .561E+00 A . 668E-02 1 . 608E+00 1 . A73E+00 1 .A31E-02 9 . 392E-01 -0 .0A7 0.071 0.060 3.0000 1 . 576E+00 5.771E-02 1 . 63AE+00 1 . 782E+0 0 1 . 729E-02 1.11 AE+00 -0 . 0A3 0 .066 0.055

3.5000 1 . 590E + 0 0 6.918E-02 1 . 660E+00 2 . 085E+00 2.032E-02 1 . 273E+00 -0.0A0 0.063 0.051

A. 0000 1 . 60AE+00 8. 102E-02 1 . 685E+00 2. 38AE+00 2. 339E-02 1 . A1 9E+00 -0.037 0.059 0.0A7

A. 5000 1 . 61 6E+00 9.315E-02 1 .709E+00 2.679E+00 2.6A9E-02 1 . 55AE+00 -0.035 0.057 0 . 0A5 5.0000 1 . 627E+00 1 . 056E-0

1

1 . 733E+00 2. 970E+00 2.961E-02 1 . 679E+00 -0.033 0 . 05A 0.0A2

5.5000 1 . 637E+00 1 . 182E-01 1 . 756E+00 3 . 256E+00 3.275E-02 1 . 7 97E + 0 0 -0.031 0.052 0 .OAO 6.0000 1 . 6 A7E+00 1 .31 1 E-01 1 . 778E+00 3 . 539E+00 3.590E-02 1 . 907E+00 -0.030 0.050 0.038 7.0000 1 . 66AE+00 1 . 57AE-0

1

1 .821 E+00 A . 0 95E+00 A.222E-02 2.1 1 OE+OO -0.027 0 .0A7 0.035 8.0000 1 . 678E+00 1 .8AAE-01 1 . 863E+00 A . 638E+00 A.853E-02 2 . 292E+00 -0.025 0 . 0 AA 0.032

9.0000 1 .691E+00 2.11 9E-01 1 . 903E+00 5.16 9E+00 5. A83E-02 2 . A58E+00 -0.023 0.0A2 0.030 10.0000 1 . 703E+00 2.399E-01 1 . 9A3E+00 5 . 689E+00 6. 109E-02 2.611 E+00 -0.022 0 .0A0 0.028

12.5000 1 . 726E+00 3.115E-01 2 . 038E+00 6.9A5E+00 7.653E-02 2 . 9A5E+00 -0.019 0.036 0 .02A 15.0000 1 . 7A6E+00 3.850E-01 2.131 E+00 8. 1 A5E+00 9. 159E-02 3 . 229E+00 -0.017 0.033 0.021 17.5000 1 .761E+00 A.599E-01 2.221 E+00 9.29AE+00 1 .062E-01 3 . A76E+00 -0.015 0.030 0.019 20.0000 1 . 775E+00 5.360E-01 2.311 E+00 1 . 0 AOE+O

1

1 .20AE-01 3 . 6 95E+00 -0.01A 0.028 0.017 25.0000 1 . 7 97E+00 6 . 906E-01 2 . A87E+00 1 . 2A8E+0

1

1 . A7AE-01 A . 07 1 E+00 -0.011 0.025 0 . 0 1 A 30.0000 1 .81 AE+00 8.A77E-01 2.S62E+00 1 . A A2E+0

1

1 .725E-01 A . 388E+00 -0.010 0.023 0.012

35.0000 1 .828E+00 1 . 00 7E + 00 2 . 835E+00 1 . 62AE+0

1

1 . 961 E— 01 A . 66 1 E+00 -0.008 0.021 0.011

AO. 0000 1 . 8AOE+00 1 . 167E+00 3 . 007E+00 1 . 7 96E+0

1

2. 180E-01 A. 901 E+00 -0.007 0.019 0.010 A5.0000 1 .851 E+00 1 . 329E+00 3. 179E+00 1 . 957E+01 2.386E-01 5.11 5E+00 -0.006 0.018 0.009

50.0000 1 . 860E+00 1 . A91 E+00 3.351 E+00 2.1 1 1E+01 2.579E-01 5.309E+00 -0 .006 0.017 0 .008 55.0000 1 . 868E+00 1 . 6 55E + 0 0 3 . 523E+00 2 . 256E+0

1

2.761 E-01 5. A86E+00 -0.005 0.016 0.007 60.0000 1 . 376E+00 1 .81 9E+00 3 . 6 95E + 00 2 . 395E+0

1

2. 932E-01 5 . 6A9E+00 -0 .005 0.015 0.006 70.0000 1 . S89E+00 2. 1 50E+00 A . 039E+00 2 . 653E+0

1

3 . 2A6E-0

1

5 . 9A0E+0O -0 . 00

A

0 . 01 A 0.005 80.0000 1 . 900E+00 2 . A83E+00 A . 383E+00 2.891 E+0

1

3.527E-01 6. 1 9AE+00 -0.003 0.013 0.005

90.0000 1 . 909E+00 2.817 E+00 A . 727E+00 3.111 E+0

1

3.782E-01 6 . A20E+00 -0.003 0.012 0 .00A 100.0000 1 . 918E+00 3. 153E+00 5.071 E+00 3.315E+01 A. 01 3E-01 6 . 62AE+00 -0.002 0.011 0 .OOA 125.0000 1 . 936 E + 00 3. 998E+00 5. 93AE+00 3 . 770E+0

1

A.508E-01 7 . 058E+00 -0 .002 0.010 0.003

1 50.0000 1 . 950E+00 A . 8A8E+00 6.798E+00 A. 1 63E+01 A.91AE-01 7.A15E+00 -0.001 0.009 0.002

175.0000 1 . 963E + 00 5 . 702E+00 7 . 665E+00 A.510E+01 5 . 25AE-0

1

7.71 8E+00 -0.001 0.009 0 . 002 200.0000 1 . 973E+00 6 . 559E+00 8 . 532E+0 0 A. 81 9E+01 5.5A3E-01 7 . 982E+00 -0.001 0.008 0.002 250.0000 1 . 990E+00 3.280E+00 1 . 027E+0

1

5.352E+01 6.01 IE-01 8 . A2AE + 00 -0.001 0.007 0.001 300.0000 2 . 00 AE+00 1 .001E+01 1 .201E+01 5 . 802E+0

1

6.377E-01 8 . 786E+00 -0.000 0.007 0.001 350.0000 2 . 0 1 6 E+0 0 1 . 17AE+01 1 . 376E+0

1

6 . 1 90 E+0

1

6.671E-01 9 . 0 93E+00 -0.000 0.006 0.001

AOO .0000 2 . 027E+00 1 . 3A8E+0

1

1 . 550E+0

1

6 . 532E+0

1

6 . 91 AE-01 9 . 359E+00 -0.000 0.006 0.001 A50.0000 2.036E+00 1 . 522E+0

1

1 . 725E+0

1

6 . 838E+0

1

7.11 9E-01 9 . 5 9AE+00 -0.000 0.006 0.001 500.0000 2 . 0AAE+00 1 .696E+01 1 . 900E+01 7.1 1 AE+01 7.295E-01 9.80AE+00 -0 .000 0.006 0.001 550.0000 2 . 05 1 E+00 1 . 870E+0

1

2 . 075E+0

1

7.366E+01 7. AA7E-01 9. 99AE + 00 -0.000 0.005 0.001 600.0000 2 . 058E+00 2.0A5E+01 2.251E+01 7.597E+01 7.581E-01 1 .017E + 01 -0.000 0.005 0.001 700.0000 2.06 9E+00 2 . 39AE+0

1

2. 601 E+01 8 . 0 1 0 E+0

1

7.80AE-01 1 . 0 A 8 E+0

1

-0.000 0.005 0 . 000 800.0000 2 . 080E+00 2.7AAE+01 2. 952E+01 8 . 37 1 E+0

1

7. 985E-01 1 .07AE+01 -0.000 0.005 0.000 900.0000 2 . 089E+00 3.09AE+01 3 . 303E+0

1

8.691 E+0

1

8.1 35E-01 1 . 0 98E+0

1

- 0.000 0.005 0.000 1000.0000 2 . 097E+00 3. AA5E+01 3.65AE+01 8. 978E+01 8.261E-01 1.11 9E+01 - 0.000 0 .00A 0.000

123
ELECTRONS IN "KAPTON" POLYIMIDE FILM

I = 79.6 eV DENSITY = 1 . 420E+001 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log[ )/d( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD (DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2/g g/cm 2

0.0100 2 . 059E+0

1

3 . 368E-03 2 . 059E+0

1

2.760E-04 9 . 020E-05 0.0 -0.201 0.231 0.229

0.0125 1 . 732E+0

1

3 . 383E-03 1 . 733E + 0

1

4.089E-04 1 .081E-04 0.0 -0.193 0.219 0.218

0.0150 1 . 504E+0

1

3.392E-03 1 . 504E+0

1

5 . 642E-04 1 .251E-04 0.0 -0.186 0.211 0.210 0.0175 1 . 335E+0

1

3.399E-03 1 . 335E+01 7.41 0E-04 1 .41 6E-04 0.0 -0.181 0.205 0.204

0.0200 1 .204E + 01 3 . 404E-03 1 .204E+01 9.385E-04 1 .574E-04 0.0 -0.177 0.199 0.198

0.0250 1 .014E+01 3.413E-03 1 .015E+01 1 . 393E-03 1 .879E-04 0 . 0 -0.170 0.191 0.190

0.0300 8 . 823E + 0 0 3 . 422E-03 8 . 832E+00 1 . 923E-03 2. 169E-04 0.0 -0.165 0.184 0. 184 0.0350 7 . 860E+00 3 . 432E-03 7 . 864E+00 2 . 524E-03 2 . 448E-04 0.0 -0.161 0.179 0.179

0.0400 7.11 6E+00 3.443E-03 7.11 9E+00 3.1 93E-03 2.717E-04 0.0 -0 . 1 58 0.175 0.175

0.0450 6 . 525E+00 3.456E-03 6 . 528E+00 3 . 923E-03 2. 978E-04 0.0 -0.155 0.172 0.171 0.0500 6 . 044E+00 3.469E-03 6 . 047E+00 4.724E-03 3.232E-04 0.0 -0.153 0.169 0.168

0.0550 5 . 644E+00 3.484E-03 5 . 647E+00 5.580E-03 3.480E-04 0.0 -0.151 0.166 0.166 0.0600 5 . 307E+00 3 . 499E-03 5.31 OE+OO 6 .494E-03 3.721E-04 0.0 -0.149 0.164 0.164

0.0700 4 . 768E+00 3.532E-03 4 . 772E+00 8.485E-03 4.1 90E-04 0.0 -0.146 0.160 0.160 0.0800 4 . 357E+00 3.569E-03 4 . 360E+00 1 . 068E-02 4 . 640E-04 0.0 -0.143 0.157 0.157

0.09C0 4 . 032E+00 3.608E-03 4 . 036E+00 1 . 307E-02 5.076E-04 0.0 -0.141 0.154 0.154

0.1000 3.770E+00 3 . 649E-03 3 . 773E+00 1 .563E-02 5 . 499E-04 0.0 -0.139 0.152 0.151 0.1250 3.290E+00 3 . 763E-03 3 . 294E+00 2 . 275E-02 6.511E-04 0.0 -0.135 0.147 0.147

0.1500 2. 967E+00 3.886E-03 2.971 E+00 3 . 076E-02 7 .469E-04 0.0 -0.132 0.143 0.143

0.1750 2 . 735E+00 4.013E-03 2 . 739E+00 3.955E-02 8 . 385E-04 0.0 -0.129 0.141 0.140

0.2000 2 . 560E+00 4.157E-03 2.564E+00 4.899E-02 9 . 267E-04 0.0 -0.127 0.138 0.138

0.2500 2.31 8E+00 4.457E-03 2 . 322E+00 6.955E-02 1 .096E-03 0.0 -0.124 0.134 0.134

0.3000 2.159E+00 4 . 784E-03 2. 164E+00 9.1 90E-02 1 . 257E-03 0.0 -0.121 0.131 0.130

0.3500 2 . 049E+00 5. 135E-03 2 . 055E+00 1 .156E-01 1 .414E-03 0 .

0

-0.119 0.129 0.128

0.4000 1 . 969E+00 5.509E-03 1 . 974E+00 1 . 405E-0

1

1 . 568E-03 1 . 309E-02 -0.095 0.125 0.123

0.4500 1 . 906E+00 5.903E-03 1 . 91 2E+00 1 . 662E-0

1

1 .720E-03 4. 101E-02 -0.089 0.120 0.117

0.5000 1 . 85 9E+00 6.316E-03 1 . 865E+00 1 . 927E-01 1 .872E-03 7.122E-02 -0.083 0.115 0.112

0.5500 1 .821E+00 6 . 745E-03 1 . 828E+00 2.1 98E-01 2.023E-03 1 .031E-01 -0.078 0.111 0.107

0.6000 1 .791E+00 7.189E-03 1 . 798E+00 2.474E-01 2. 175E-03 1 .361 E-01 -0.074 0.107 0.102

0.7000 1 . 747E+00 8.11 9E-03 1 .755E+00 3.038E-01 2.480E-03 2.042E-01 -0.067 0.100 0.094

0.8000 1 . 71 7E+00 9.096E-03 1 . 726E+00 3.61 3E-01 2 . 789E-03 2.735E-01 -0.062 0.094 0.088

0 . 9000 1 . 6 96E+00 1 .012E-02 1 . 707E+00 4.1 95E-01 3. 101E-03 3.426E-01 -0.057 0.090 0.082

1 .0000 1 . 682E+00 1 . 1 18E-02 1 . 693E+00 4.784E-01 3.417E-03 4.109E-01 -0.054 0.085 0.077

1 .2500 1 . 663E+00 1 . 399E-02 1 . 677E+00 6 .269E-01 4.227E-03 5.751 E— 0

1

-0.048 0.077 0.067

1 .5000 1 . 657E+00 1 . 700E-02 1 . 674E+00 7.761E-01 5 . 063E-03 7.282E-01 -0.043 0.071 0.061

1 .7500 1 . 657E+00 2.017E-02 1 . 677E+00 9.254E-01 5. 923E-03 8.700E-01 -0.040 0 .066 0.055

2.0000 1 . 660E+00 2 . 347E-02 1 . 683E+00 1 . 074E+00 6 . 806E-03 1 . 00 1 E+00 -0.038 0.062 0.051 2.5000 1 . 670E+00 3.041E-02 1 .701 E+00 1 . 370E+00 8 . 625E-03 1 . 237E+00 -0.035 0.056 0.046

3.0000 1 . 683E+00 3 . 773E-02 1 .721 E+00 1 . 662E+00 1 . 050E-02 1 . 442E+00 -0.032 0.052 0.041 3.5000 1 . 696E+00 4 . 535E-02 1 .741 E+00 1 . 951 E+00 1 . 243E-02 1 . 624E+00 -0.031 0.049 0.039

4.0000 1 . 708E+00 5 . 322E-02 1 .761 E+00 2 . 237E+00 1 . 439E-02 1 . 788E+00 -0.029 0.047 0.036 4.5000 1 .71 9E+00 6.132E-02 1 . 780E+00 2.51 9E+00 1 . 639E-02 1 . 936E+00 -0.028 0.045 0.034

5.0000 1 . 730E+00 6.961E-02 1 . 7 99E+00 2 . 798E+00 1 . 840E-02 2 . 072E+00 -0.027 0.043 0.033

5.5000 1 .740E+00 7 . 807E-02 1 . 8 1 8E+00 3 . 075E+00 2 . 044E-02 2.1 97E+00 -0.026 0.041 0.032

6.0000 1 . 749E+00 8.669E-02 1 . 836E+00 3 . 348E+00 2.249E-02 2.31 4E+00 -0.025 0 .040 0.030 7.0000 1 . 765E+00 1 . 044E-0

1

1 . 870E+00 3 . 888E+00 2.664E-02 2 . 526E+00 -0.024 0.038 0.029

8.0000 1 . 780E+00 1 . 225E-0

1

1 . 902E+00 4.418E+00 3 . 082E-02 2.71 5E+00 -0.022 0.036 0.027

9.0000 1 . 793E+00 1 .410E-01 1 . 934E+00 4 . 940E+00 3.503E-02 2.886E+00 -0.021 0.034 0.025

10.0000 1 .804E+00 1 . 599E-0

1

1 . 964E+00 5 . 453E+00 3.924E-02 3 . 043E+00 -0.019 0.033 0.024

12.5000 1 .828E+00 2.084E-01 2 . 036 E+00 6 . 703E+00 4.978E-02 3 . 387E+00 -0.016 0.030 0.021 15.0000 1 . 847E+00 2.582E-01 2 . 1 05E+00 7.91 OE+OO 6 . 024E-02 3 . 68 1 E+00 -0.014 0.027 0.019

17.5000 1 . 862E+00 3.091 E-01 2.171 E+00 9 . 079E+00 7.057E-02 3 . 939E+00 -0.011 0.025 0.017

20.0000 1 . 875E+00 3.609E-01 2 . 236E+00 1 .021E+01 8 . 074E-02 4. 168E+00 -0.010 0.023 0.015

25.0000 1 .896E+00 4.664E-01 2 . 363E+00 1 .239E+01 1 . 005E-0

1

4.564E+00 -0.007 0.020 0.012

30.0000 1 . 91 3E+00 5.737E-01 2 . 486 E+00 1 . 445E+0

1

1 . 1 95E-01 4 . 8 97E+0 0 -0.005 0.018 0.010 35.0000 1 . 926E+00 6.824E-01 2.609E+00 1 .641E+01 1 . 376E-0

1

5. 184E+00 -0.004 0.016 0.008

40.0000 1 . 938E+00 7.923E-01 2 . 730E+00 1 . 829E+0

1

1 -549E-01 5 . 437E+0 0 -0.003 0.015 0.007

45.0000 1 . 948E+00 9.031E-01 2.851 E+00 2 . 008E+0

1

1 .714E-01 5 . 662E+00 -0.003 0.014 0.006 50.0000 1 . 957E+00 1 . 0 1 5E+00 2.971 E+00 2. 180E+01 1 . 872E-0

1

5 . 864E+00 -0.002 0.013 0.005

55.0000 1 . 965E+00 1 . 1 27E+00 3 . 0 9 1 E + 0 0 2.345E+01 2 . 023E-0

1

6 . 049E+00 -0.002 0.012 0.005

60.0000 1 . 972E+00 1 . 240E+00 3.212E+00 2.503E+01 2. 167E-01 6.21 8E+00 -0.002 0.011 0.004

70.0000 1 . 984E+00 1 . 467E+00 3.451 E+00 2.804E+01 2.438E-01 6.51 9E+00 -0.001 0.010 0.003 80.0000 1 . 995E+00 1 . 6 96E+00 3.691 E+00 3 . 084E+0

1

2.686E-01 6.781 E+00 -0.001 0.009 0.003

90.0000 2 . 005E+00 1 . 926E+00 3.931 E+00 3.346E+01 2.915E-01 7.01 3E+00 -0.001 0.009 0.002

100.0000 2.01 3E+00 2. 157E+00 4 . 1 70 E+00 3 . 593E+0

1

3. 128E-01 7.221 E+00 -0.001 0.008 0.002

125.0000 2.031E+00 2 . 739E+00 4 . 770E+00 4. 153E+01 3.596E-01 7 . 663E+00 -0.000 0.007 0.002

1 50.0000 2 . 046E+00 3 . 325E+00 5.371 E+00 4 . 647E+0

1

3.993E-01 8 . 025E+00 -0.000 0.006 0.001 175.0000 2.058E+00 3.914E+00 5 . 972E+00 5.088E+01 4.333E-01 8.331 E+00 -0.000 0.006 0.001 200.0000 2.068E+00 4 . 506E+00 6 . 574E+00 5 . 487E+0

1

4 . S30E-01 8 . 597E+00 -0.000 0.005 0.001 250.0000 2 . 086E+00 5 . 6 95E+00 7.781 E+00 6 . 185E+01 5. 124E-01 9 . 042E+00 -0.000 0.005 0.001 300.0000 2.101E+00 6 . 88 9E+0 0 8 . 990E+00 6 . 783E+0

1

5.520E-01 9 . 405E+00 -0.000 0.004 0.001 350.0000 2.1 13E+00 8 . 088E+00 1 . 020E+0

1

7 . 304E+0

1

5.846E-01 9.71 3E+00 -0.000 0.004 0.000 400.0000 2. 123E+00 9.289E+00 1 .141E+01 7 . 768E+0

1

6.120E-01 9. 979E+00 -0.000 0 .004 0 .000 450.0000 2. 133E+00 1 .049E+01 1 .263E+01 8. 184E+01 6 . 354E-0

1

1 . 0 2 1 E+0

1

-0.000 0.004 0.000 500.0000 2. 141E+00 1 . 170E+01 1 . 334E+01 8 . 562E+0

1

6.557E-01 1 . 0 43E+0

1

-0.000 0.003 0.000 550.0000 2 . 1 48E+00 1 .291E+01 1 . 505E+0

1

8. 908E+01 6 . 735E-0

1

1 . 062E+0

1

-0.000 0.003 0.000 600.0000 2. 155E+00 1 .41 1 E+01 1 . 627E+0

1

9 . 228E+0

1

6 . 893E-0

1

1 .079E+01 -0.000 0.003 0.000 700.0000 2. 167E+00 1 . 654E+0

1

1 . 870E+0

1

9.801 E+0

1

7 . 1 60E-01 1 . 1 1 0 E+0

1

-0.000 0.003 0.000 300.0000 2 . 1 78E+00 1 .896E+01 2. 1 14E+01 1 . 030E+02 7.378E-01 1 . 1 36E+01 -0.000 0.003 0.000 900.0000 2. 187E+00 2.139E+01 2 . 357E+0

1

1 . 075E+02 7.561 E-01 1 . 1 60 E+0

1

-0.000 0.003 0.000 1000.0000 2.1 96E+00 2 . 382E+0

1

2.601 E+01 1 .1 15E+02 7.716E-01 1 . 181 E+01 -0.000 0.003 0.000

124
ELECTRONS IN LITHIUM FLUORIDE

I =

STOPPING POWER COLLISION RADIATIVE

ENERGY

MeV

0.0100 0.0125

0.0150 0.0175

0.0200

0 .0250 0.0300

0.0350

0 .0000 0.0A50

0.0500

0.0550

0.0600

0.0700

0 .0800 0.0900 0.1000

0.1250

0.1500 0.1750

0.2000

0.2500

0.3000 0.3500

0 .A000

0 . 0500 0.5000

0.5500 0.6000

0.7000

0 .8000

0 . 9000

1 .0000

1 .2500

1 .5000

1 .7500 2.0000 2.5000

3.0000

3.5000

A. 0000

A. 5000 5.0000 5.5000

6.0000

7.0000 5.0000

9.0000 10.0000

12.5000

15.0000 17.5000

20 .0000 25.0000

30.0000

35.0000

AO. 0000 A5.0000

50.0000

55.0000

50 .0000 70.0000 80.0000

90 .0000 100.0000

125.0000

150.0000 175.0000 200.0000

250 .0000 300.0000 350.0000

A00 .0000 A50.0000

500.0000

550.0000

600.0000 700.0000 800.0000

900.0000 1000.0000

MeV cm 2 /g

1 . 7 96E + 0

1

1 .513E+01

1 .315E+01

1 . 168E+01

1 . 055E+01

8 . 89AE+00

7 . 7 A3E + 00

6 . 902E+00

6 . 252E+00

5 . 736E+00

5 . 31 5E+00

A. 965E+00

A . 670E+00

A. 1 98E+00

3 . 833E+00

3.553E+00

3 . 323E+00

2. 903E+00

2.61 9E+00 2.A15E+00

2.261 E+00 2.0A8E+00

1 . 907E+00

1 . 80 9E+00

1 . 737E+00

1 . 683E+00

1 . 6A2E+00

1 . 6 0 9E+00

1 . 583E+00

1 . 5A6E+00

1 .521E+00

1 . 50 3E + 00

1 .A91E+00

1 .A76E+00

1 . A71 E+00

1 . A71 E + 00

1 . A7AE+00

1 . A83E+00

1 . A93E + 00

1 . 503E+00

1 . 5 1 3E+00

1 . 523E+00

1 .531 E+00

1 . 53 9E + 00

1 . 5A7E+00

1 . 560E+00

1 . 572E+00

1 . 583E+00

1 . 592E+00

1 .612E+00

1 . 629E+00

1 . 6A2E+00

1 . 65AE+00

1 . 673E+00

1 . 688E+00

1 . 700E+00

1 .711 E+00

1 . 720E+00

1 . 728E+00

1 . 736E+00

1 . 7 A2E+00

1 . 75AE+00

1 . 76 AE+00

1 . 772E+00

1 .780E+00

1 . 796 E+00

I . 30 9E + 00

1 .820E+00

1 . 830E+00

1 .8A6E+00

1 .359E+00

1 .870E+00

1 . 879E+00

1 .888E+00

1 . 895E+00

1 . 902E+00

1 . 908E+00

1 .91 9E+00

1 . 929E+00

1 . 937E+00

1 . 9A5E+00

MeV cra z /g

3.678E-03

3.712E-03

3.735E-03

3 . 750E-03

3 . 762E-03

3.779E-03

3.792E-03

3.30AE-03

3.815E-03

3 . 827E-03

3 .8A0E-03 3.853E-03

3.867E-03

3 . 898E-03

3 . 932E-03

3.970E-03

A. 01 IE-03 A.125E-03

A.253E-03

A.392E-03

A.5A0E-03

A.863E-03

5.215E-03

5.592E-03

5.992E-03

6

.

A 1 2E-0 3 6.852E-03

7.308E-03

7.779E-03

8.765E-03

9.800E-03

1 .088E-02

1 . 200E-02

1 . A99E-02

1 . 8 1 8E-02

2.1 5AE-02

2 . 505E-02

3 . 2AAE-02

A.021E-02

A.830E-02

5 . 666E-02

6.52AE-02

7.

A02E-02

8 . 298E-02

9.21 IE-02

1 . 108E-01

1 .299E-0)

1 . A9AE-01

1 .693E-01 2.201E-01 2.723E-01

3.256E-01

3.797E-01

A.896E-01

6.01AE-01

7.1 A6E-01 8.289E-01

9 . A A 1 E-0 1

1 . 060E + 00

1 . 177E+00

1 . 29AE + 00

1 . 530E+00

1 . 767E+00

2 . 006E+00

2 . 2A5E + 00

2 . 3A8E + 0 0 3. A55E+00

A . 065E+00

A . 677E+00

5 . 907E+00

7. 1 A2E+00

8 . 38 1 E+00

9 . 622E+00

1 . 087E+0

1

1 .21 1E+01

1 . 336E+0

1

1

.

A61E+01

1 .71 1E+01

1 .961E+01

2.21 1E+01

2.

A62E+01

9A.0 eV

TOTAL MeV cm 2 /g

1 .796E + 01

1 .51 AE+01

1 .316E+01

1 . 169E+01

1 . 055E+01

8 . 898E+00

7.751 E+00

6 . 906E+00

6 . 256E+00

5 . 739E+00

5.31 9E+00

A . 969E+00

A . 67AE+00

A . 202E+00

3 . 8A2E+00

3 . 557E+00

3 . 327E+00

2 . 907E+00

2 . 623E+00

2 . A 1 9E + 00 2.266E+00

2.053E+00

1 . 91 2E+00

1 .81 AE+00

1 .7A3E+00

1 . 6 90E + 00

1 . 6A9E+00

1 . 6 1 7E+00

1 . 591 E+00

1 . 555E+00

1 . 530E+00

1 .51 AE + 00

1 . 50 AE+00

1 . A91 E+00

1 . A89E+00

1 . A93E+00

1

.

A99E+00

1 . 51 5E+00

1 . 533E+00

1 . 552E+00

1 . 570E+00

1 . 588E + 0 0

1 . 605E+00

1 . 622E+00

1 . 639E+00

1 . 671 E+00

1 . 702E+00

1 . 732E+0 0

1 .761 E+00

1 . 832E+0 0

1 . 901 E+00

1 . 968E + 00

2 . 03AE+00 2.163E+00

2 . 289E+00

2.

A15E+00

2.5A0E+O0

2 . 66 AE + 00

2 . 788E+00

2. 91 2E+00

3.036 E+00

3 . 283E+00

3.531 E+00

3 . 778E+00

A . 025E+0 0 A . 6AAE+00

5 . 26 AE+00 5.885E+00

6 . 507E+00

7 . 753E+00

9.001 E+00

1 . 025E+0

1

1 . 1 50E+01

1 . 275E+0

1

1

.

A01E+01

1 . 526E+0

1

1 .651E+01

1 .902E+01

2. 15AE+01

2.

A05E+01

2 . 656E+0

1

DENSITY = 2 . 635E+001 g/cm 3

CSDA RADIATION DEMS.EFF. d( log )/d( loa I

)

RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

g/cra 2

3.181 E-OA 1 . 1 1 7E-0A 0.0 -0.208 0 .2A0 0.238 A.70AE-0A 1 . 3AAE-0

A

0.0 -0.199 0.228 0.226

5 . A89E-0

A

1 . 561 E-OA 0.0 -0.192 0.219 0.217

8 . 50 1 E-0

A

1 . 770E-0

A

0.0 -0.187 0.212 0.211

1 . 076E-03 1 . 973E-0A 0.0 -0.182 0.206 0.205

1 .59AE-03 2.360E-0A 0.0 -0.175 0.197 0.196

2. 1 93E-03 2.729E-0A 0 . 0 -0.170 0.190 0.190

2 . 883E-03 3.032E-0A 0.0 -0.166 0.185 0.13A

3 . 6A5E-03 3. A23E-0A 0.0 -0.162 0.181 0.130

A. A80E-03 3.752E-0A 0 .

0

-0.160 0.177 0.176

5 . 386E-03 A. 071 E-OA 0.0 -0.157 0. 17A 0.173 6.359E-03 A.382E-0A 0.0 -0.155 0.171 0.171 7.397E-03 A.68AE-0A 0.0 -0.153 0.169 0.168

9 . 659E-03 5.269E-0A 0.0 -0.150 0 . 1 6 A 0. 16A

1 .215E-02 5.831 E-OA 0.0 -0 . 1 A7 0.161 0.161

1 . A86E-02 6 . 372E-0

A

0.0 -0 . 1 AA 0.158 0.158

1 . 777E-02 6.896E-0A 0.0 -0.1A2 0.156 0.155

2 . 58AE-02 8. 1 A3E-0A 0.0 -0.138 0.151 0.150

3. A92E-02 9.321 E-OA 0.0 -0.135 0.1 A7 0.1A7

A . A86E-02 1 . 0A5E-03 0.0 -0.132 0 . 1 AA 0 . 1 A3

5 . 555E-02 1 . 1 53E-03 0.0 -0.130 0 . 1 A 1 0. 1A1

7 .881 E-02 1 . 360E-03 6 . 058E-03 -0.118 0.136 0.135

1 . 0 A 1 E-0

1

1 . 558E-03 2.1 36E-02 -0.112 0.131 0.130

1 . 3 1 0 E-0

1

1 . 750 E-0 3 3 . 978E-02 -0.106 0.126 0.125

1 .591 E-0

1

1 .939E-03 6.095E-02 -0.100 0.122 0.120

1 . 883E-0

1

2. 125E-03 8.AA5E-02 -0.095 0.118 0.116

2. 183E-01 2.310E-03 1 . 0 98E-0

1

-0.090 0.115 0.112

2 . A89E-0

1

2. A95E-03 1 . 367E-0

1

-0.086 0.112 0.108

2.801 E-0

1

2.679E-03 1 .6A8E-01 -0.082 0.108 0 . 1 OA 3.A37E-01 3.0A8E-03 2.236E-01 -0.075 0.103 0.098

A . 086E-0

1

3.A19E-03 2.8A6E-01 -0.070 0.098 0.092 A.7A3E-01 3 . 79AE-03 3. A67E-01 -0.065 0 .09A 0.087

5. A06E-01 A. 173E-03 A.093E-01 -0.060 0.090 0.083 7.077E-01 5 . 1 A 1 E-0 3 5.6AAE-01 -0.052 0.082 0.073

8 . 756 E-0

1

6 . 1 38E-03 7. 1A2E-01 -0.0A6 0 . 075 0 .066

1 . 0 A3E+00 7. 163E-03 3.568E-01 -0 . 0 A 1 0.070 0.059

1 . 2 1 0 E+0 0 8.21AE-03 9.917E-01 -0.037 0.066 0.05A

1 . 5A2E+00 1 . 038E-02 1 . 2A0E+00 -0.032 0.059 0.0A7

1 . 87 0 E+0 0 1 . 262E-02 1 . A6 1 E+00 -0 .028 0 .05A 0.0A1

2.1 9AE+00 1 .A91E-02 1 . 660E+00 -0.026 0 . 0A9 0.037

2.51 5E+00 1 . 725E-02 1 .839E+00 -0 .02A 0.0A6 0.03A

2 . 832E+00 1 . 962E-02 2 . 003E+00 -0.022 O.OAA 0.031

3.1 A5E+00 2 . 202E-02 2. 15AE + 00 -0.021 0 . 0A1 0.029

3. A55E+00 2 . AAAE-02 2 . 293E+00 -0 .020 0.039 0.027

3.761 E+00 2 . 687 E-0 2 2 . A22E+00 -0.019 0.038 0 .026

A . 365E+00 3. 178E-02 2 . 655E+0 0 -0.018 0.035 0 . 02A

A. 958E+00 3 . 672E-02 2.861 E+00 -0.017 0.033 0.022

5.5A1 E+00 A . 1 68E-02 3 . 0A6E+00 -0.016 0.031 0.020

6.11 3E+00 A . 663E-02 3.21 AE+00 -0.016 0.029 0.019

7 . 50AE+00 5.89AE-02 3 . 577E+00 -0.01 A 0.026 0.017 8.8AAE+00 7 . 1 08E-02 3 .881 E+00 -0.013 0.02A 0.015

1 .01AE+01 8.299E-02 A . 1 A3E+00 -0.011 0.022 0.01 A

1 . 1 39E+01 9.A63E-02 A. 37AE+00 -0.010 0.021 0.013

1 . 377E+01 1.171 E-0

1

A.769E+00 -0.008 0.018 0.011

1 .602E+01 1 .38AE-01 5 . 099E+00 -0.007 0.017 0.009

1 .81 AE+01 1 .585E-01 5 . 383E+00 -0.005 0.015 0.008 2.016E+01 1 . 776 E-0

1

5 . 633E+00 -0.00A 0 . 0 1 A 0.007

2 . 208E+0

1

1 . 957 E-0

1

5 . 856 E+0 0 -0 .00A 0.013 0.006

2 . 392E+0

1

2.129E-01 6 . 057E + 00 -0.003 0.012 0.005

2 . 567E+0

1

2.292E-01 6 . 2AOE+00 -0.003 0.011 0.005 2.735E+01 2.AA7E-01 6 . A08E + 00 -0.002 0.011 0 . 00 A 3.052E+01 2.735E-01 5 . 707E+00 -0.002 0.010 0 .00A

3 . 3A6E+0

1

2.998E-01 6 . 968E+00 -0.001 0.009 0.003

3.61 9E+01 3.238E-01 7.1 99E+00 -0.001 0.008 0.003

3.876E+01 3.A59E-01 7 . A06E+00 -0.001 0.008 0.002

A . A53E+0

1

3.9A1E-01 7 . 8A7E + 00 -0.001 0.007 0.002 A.959E+01 A.3A3E-01 8.209E+00 -0.000 0.006 0.001

5. A08E+01 A . 686 E-0

1

8.51 5E+00 -0 .000 0.006 0.001

5.81 1E+01 A.982E-01 8 . 780E + 00 -0.000 0.005 0.001 6.51AE+01 5. A68E-01 9 . 225E + 00 -0.000 0.005 0.001 7.112E+01 5.85AE-01 9 . 538E + 00 -0.000 0 .00A 0.001

7 . 633E+0

1

6.170E-01 9 . 896E+00 -0.000 0 .00A 0.001

8 . 093E+0

1

6.A33E-01 1 .016E+01 -0.000 0 . 00 A 0.000

8 . 505E+0

1

6.656E-01 1 .0A0E+01 -0.000 0 . 00 A 0.000

8 . 879E+0

1

6 .8A9E-01 1.061 E+0

1

-0.000 0 . 00 A 0 .000 9.221 E+01 7.018E-01 1 . 080E+0

1

-0.000 0.003 0.000 9.536E+01 7.166E-01 1 . 0 97E+0

1

-0.000 0.003 0.000

1 .01 0E+02 7.A17E-01 1 . 1 28E+01 -0.000 0.003 0.000

1 . 059E+02 7.621E-01 1 . 1 55E+0

1

-0.000 0.003 0.000

1 . 1 03E+02 7 .791 E-01 1 . 178E+01 -0 .000 0.003 0.000

1 . 1 A3E+02 7. 935E-01 1 . 1 99E+01 -0.000 0.003 0.000

125
ELECTRONS IN LITHIUM TETRABORATE

I = 9A.6 eV DENSITY = 2 . AAOE+OO g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log: ) /d ( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV c» 2/g MeV cm 2/g g/cm 2 0.0100 1 .880E+01 3.5A7E-03 1 . 830E+0

1

3.OAOE-0A 1 . 039E-0A 0.0 -0 . 208 0.2A1 0.239

0.0125 1 . 58AE+0

1

3.569E-03 1 . 58AE + 0

1

A. A9AE-0A 1 . 2A5E-0

A

0.0 -0.199 0.229 0.227

0.0150 1 . 377E+0

1

3.582E-03 1 . 377E+0

1

6 . 1 92E-0A 1 . A42E-0

A

0 .

0

-0.192 0.220 0.213

0.0175 1 .223E+01 3.591 E-03 1 . 223E+0

1

8.122E-0A 1 .632E-0A 0.0 -0.187 0.212 0.211 0.0200 1 . 1 OAE + O

1

3.598E-03 1 . 1 OAE+O

1

1 . 028E-03 1 .315E-0A 0.0 -0.133 0.207 0.205

0.0250 9.31 1E+00 3.603E-03 9.315E+00 1 . 523E-03 2.165E-0A 0.0 -0.176 0.193 0.197

0.0300 8.111 E+00 3.617E-03 8.11 5E+00 2. 100E-03 2 . A99E-0A 0.0 -0.170 0.191 0.190

0.0350 7 . 227E+00 3 . 627E-03 7 . 230E+00 2.75AE-03 2.81 9E-0A 0.0 -0.156 0.135 0.185

0.0A00 6 . 5 A6E+0 0 3.638E-03 6 . 550E+00 3. A82E-03 3. 1 28E-0A 0.0 -0.163 0.181 0.180

0.0A50 6 . 005E+00 3.6A9E-03 6 . 00 9E + 00 A . 280E-03 3. A26E-0A 0.0 -0.160 0.177 0.177

0.0500 5 . 565E+00 3 . 662E-03 5.569E+00 5.1A5E-03 3.716E-0A 0.0 -0.157 0 . 1 7A 0 . 17A 0.0550 5.1 99E+00 3.676E-03 5.203E+00 6 . 07AE-03 3. 999E-0A 0.0 -0.155 0.171 0.171 0.0600 A.890E+00 3.692E-03 A . 893E+00 7.066 E-03 A.27AE-0A 0.0 -0.153 0.169 0.168

0.0700 A . 3 96 E+00 3.725E-03 A . A00E+00 9 . 226E-03 A.808E-0A 0.0 -0.150 0.165 0 . 1 6 A 0.0800 A. 01 9E+00 3.761 E-03 A . 022E+00 1 .161E-02 5.321 E-OA 0.0 -0.1 A7 0.161 0.161 0.0900 3.721 E+00 3.801 E-03 3 . 725E+00 1 . A1 9E-02 5.816E-0A 0.0 -0. 1 A5 0.158 0.158

0.1000 3. A80E+00 3 . 8A3E-0 3 3. A8AE+00 1 .697E-02 6 .297E-0A 0.0 -0.1A2 0.156 0.156 0.1250 3 . 0 AO E + 00 3. 959E-03 3 . 0A3E + 00 2 . A68E-02 7 . AAAE-OA 0.0 -0.138 0.151 0.151 0.1500 2 . 7A2E+00 A.086E-03 2 . 7 A6E+0 0 3 . 335E-02 8 . 528E-Q

A

0.0 -0.135 0.1A7 0.1A7

0.1750 2 . 528E+00 A.222E-03 2 . 533E+00 A . 285E-02 9 . 56AE-0

A

0.0 -0.132 0 . 1 A A 0 . 1 AA 0.2000 2 . 368E+00 A . 365E-03 2 . 373E+00 5.306E-02 1 .056E-03 0.0 -0.130 0.1A2 0. 1A1 0.2500 2.1 A5E+00 A . 675E-03 2.150E+00 7 . 527E-02 1 .2A6E-03 0.0 -0.126 0.138 0.137

0.3000 1 . 999E+00 5 . 01 3E-03 2 . 00 AE+OO 9.9A1E-02 1 . A28E-03 8 . 258E-03 -0.107 0.133 0.132

0.3500 1 . 895E+0 0 5 . 376E-03 1 . 900E+00 1 .251E-01 1 . 605E-03 3 . A57E-02 -0.099 0.127 0.125

0.A000 1 .81 9E+00 5 . 763E-03 1 . 825E+00 1 .51 9E-01 1 . 779E-03 6.AA2E-02 -0.092 0.121 0.119

0.A500 1 . 762E+00 6.171 E-03 1 . 768E+00 1 .798E-01 1 .951E-03 9.625E-02 -0.087 0.116 0.113

0.5000 1 . 7 1 7E+00 6.598E-03 1 . 72AE+00 2.085E-01 2.121E-03 1 .29AE-01 -0.082 0.112 0.108

0.5500 1 . 683E+00 7 . OAAE-03 1 . 6 90E+00 2.378E-01 2 . 292E-03 1 .633E-01 -0.078 0.108 0. 10A 0.6000 1 . 655E+00 7.50AE-03 1 . 663E+00 2.676E-01 2. A63E-03 1 . 979E-01 -0.075 0 . 1 OA 0.100 0.7000 1 . 6 1 5E+00 8 . A67E-03 1 . 623E+00 3.285E-01 2 . 806E-03 2.679E-01 -0.069 0.098 0.092

0.8000 1 . 588E+00 9.A79E-03 1 . 597E+00 3.907E-01 3. 152E-03 3.381E-01 -0.06A 0.093 0.087

0.9000 1 . 569E+00 1 . 05AE-02 1 .580E+00 A.536E-01 3.501 E-03 A . 076E-0

1

-0.060 0.089 0.081

1 .0000 1 . 557E+00 1 .16AE-02 1 . 568E+00 5. 172E-01 3.856E-03 A.759E-01 -0.056 0.085 0.077

1 .2500 1 . 5A0E+00 1 . A55E-02 1 . 55 AE+OO 6 .775E-01 A . 76 1 E-03 6 . 398E-01 -0.050 0.077 0.068

1 .5000 1 . 53AE+00 1 . 766E-02 1 . 552E+0 0 8.385E-01 5 . 695E-03 7.928E-01 -O.OA5 0.071 0.062

1 .7500 1 . 535E+00 2.09AE-02 1 . 556E + 00 9.99AE-01 6 .655E-03 9.3A9E-01 -0 .0A2 0.067 0.057

2.0000 1 . 538E+00 2. A35E-02 1 . 56 2E+0 0 1 . 160E+00 7 . 638E-03 1 . 067E+00 -0.039 0.063 0.053

2.5000 1 . 5A8E+00 3. 153E-02 1 . 580 E + 00 1 . A78E+00 9.663E-03 1 . 305E+00 -0.035 0.057 0.0A7

3.0000 1 . 560E+00 3. 909E-02 1 . 599E+00 1 . 7 93E+0 0 1 . 175E-02 1 . 5 1 AE+OO -0.033 0.053 0.0A2

3.5000 1 . 572E+00 A.695E-02 1 .61 9E+00 2 . 1 0 AE+OO 1 .389E-02 1 .701 E+00 -0.030 0.050 0.039

A. 0000 1 . 583E+00 5 . 508E-02 1 . 6 38E+00 2 . A 1 1 E+00 1 . 607E-02 1 . 869E+00 -0.029 0.0A7 0.037

A. 5000 1 . 593E+00 6 . 3A2E-02 1 . 6 57E+00 2.71 AE+OO 1 . 828E-02 2 . 023E+00 -0.027 0 .0A5 0.035

5.0000 1 . 6 0 3E+0 0 7 . 1 97E-02 1 . 675E+00 3.01 AE+OO 2.051E-02 2. 1 63E+00 -0.026 0.0A3 0.033

5.5000 1 .61 2E+00 8.069E-02 1 . 6 93E + 00 3.31 1E+00 2.277E-02 2 . 293E+00 -0.025 O.OA1 0.031 6.0000 1 . 621 E+00 8.958E-02 1 .710 E+00 3 . 605E+00 2.50AE-02 2.A15E+00 -0.02A 0 . 0A0 0.030 7.0000 1 . 636E+00 1 . 078E-0

1

1 . 7AAE+00 A. 18AE+00 2. 962E-02 2 . 635E+00 -0.022 0.037 0 . 028 8.0000 1 . 6 A 9E+00 1 . 26AE-0

1

1 . 775E+00 A . 752E+00 3 . A23E-02 2.831 E+00 -0.021 0.035 0.026

9.0000 1 . 66 1 E+00 1 . A55E-01 1 .806E+00 5.31 1 E+00 3 . 886E-02 3 . 008E+00 -0.019 0.033 0.02A

10.0000 1 .671 E+00 1 .6A9E-01 1 . 836E+00 5 . 860E+00 A . 3A9E-02 3 . 1 70E+00 -0.018 0.032 0.023

12.5000 1 . 6 93E + 00 2.1A8E-01 1 . 908E+00 7. 195E+00 5.505E-02 3 . 52AE+00 -0.015 0.029 0.020 15.0000 1 . 71 0E+00 2.660E-01 1 . 976E+00 8 . A83E+00 6.6A8E-02 3 . 823E+00 -0.013 0.026 0.018

17.5000 1 . 725E+00 3. 18AE-01 2 . 0A3E+00 9 . 727E+00 7 . 77AE-02 A . 083E+00 -0.011 0 .02A 0.016 20.0000 1 . 737E + 00 3.716E-01 2.109E+00 1 . 0 93E+0

1

8 . 878E-02 A . 31 AE+OO -0.010 0.023 0.01 A 25.0000 1 . 757E+00 A.798E-01 2 . 237E+00 1 . 323E+0

1

1 .102E-01 A . 7 1 0E+00 -0.008 0.020 0.012

30.0000 1 . 772E+00 5.900E-01 2 . 362E+00 1 . 5 A 1 E+0

1

1 . 305E-0

1

5.0A2E+00 -0.006 0.018 0.010 35.0000 1 . 785E+00 7.015E-01 2. A87E+00 1 .7A7E+01 1 . A99E-01 5 . 329E+00 -0.005 0.016 0.008

AO. 0000 1 . 796E+00 8.1A2E-01 2.61 1E+00 1 . 9A3E+0

1

1 . 683E-0

1

5 . 580E+00 -0 . 00

A

0.015 0.007

A5.0000 1 . 806E+00 9.278E-01 2 . 73AE+00 2.130E+01 1 .858E-01 5.805E+00 -0.003 0.01 A 0.006 50.0000 1 . 8 1 AE + OO 1 . 0A2E+00 2 . 856E+00 2.309E+01 2.025E-01 6 . 00 7E+00 -0.003 0.013 0.005

55.0000 1 . 822E+0 0 1 . 1 57E+00 2. 979E+00 2.A81E+01 2. 183E-01 6.191 E+00 -0.002 0.012 0.005

60.0000 1 -829E+00 1 . 273E+00 3. 102E+00 2.6A5E+01 2.33AE-01 6 . 360E+00 -0 .002 0.011 0 . OOA 70.0000 1 .3A1E+00 1 . 506E+00 3 . 3A6E+00 2 . 955E+0

1

2.616E-01 6 . 660E+00 -0.001 0.010 0.003

80 .0000 1 .851 E+00 1 . 7A0E+00 3.591 E+00 3 . 2AAE+0

1

2.873E-01 6 . 922E+00 -0.001 0.009 0.003

90.0000 1 . 860E+00 1 . 976E+00 3 . 836E+00 3.513E+01 3. 1 1 0E-01 7. 15AE+00 -0.001 0.009 0 .002 100.0000 1 . 868E+00 2.21 2E+00 A . 080E+00 3 . 766E+0

1

3.328E-01 7.361 E+00 -0.001 0.008 0.002

125.0000 1 . 885E+00 2 . 808E+00 A . 693E+00 A . 337E+0

1

3.805E-01 7.303E+00 -0.001 0 . 007 0 .002 150.0000 1 . 89 9E+00 3 . A08E+00 5 . 30 6 E + 00 A.838E+01 A.206E-01 8. 165E+00 -0 .000 0.006 0.001 175.0000 1 . 91 0E+00 A. 01 1 E+00 5.921E+00 5 . 283E+0

1

A.5A9E-01 8.A71E+00 -0.000 0.005 0.001 200.0000 1 . 920E+00 A. 61 6E+00 6 . 536E+00 5 . 685E+0

1

A.8A6E-01 8 . 737E+00 -0.000 0.005 0.001 250.0000 1 . 937E+00 5 . 832E+00 7 . 769E+00 6 . 336 E + 0

1

5.336E-01 9. 181 E+00 -0.000 0.005 0.001

300 0000 1 . 95 1 E+00 7 . 053E+00 9.00AE+00 6 . 983E+0

1

5 . 726E-0

1

9 . 5A5E+00 -0.000 0.005 0.001 350.0000 1 . 962E+00 8 . 279E+00 1 . 02AE+0

1

7.503E+01 6 .0A6E-01 9 . 853E+00 -0 . 000 0 . 00 A 0.000 AOO.OOOO 1 . 972E+00 9 . 507E+00 1 . 1 A8E+0

1

7. 96AE+01 6.313E-01 1 .012E+01 -0 .000 0 . OOA 0.000

A50 .0000 1 . 93 1 E+00 1 .07AE+01 1 . 272E+0

1

8 . 378E+0

1

6.5A1E-01 1 . 0 35E + 0

1

-0.000 0 . 00 A 0.000 500.0000 1 . 989E+00 1 . 1 97E+01 1 . 396E+01 8 . 753E+0

1

6 . 738E-01 1 . 056E+0

1

-0 .000 0 . 00 A 0 .000 550.0000 1 . 996E+00 1 . 320E+0

1

1 . 520E+0

1

9.096E+01 5.91 IE-01 1 . 076E+0

1

-0.000 0.003 0.000 600.0000 2 . 002E+00 1 . AAAE+01 1 . 6 A AE+0

1

9.A13E+01 7.063E-01 1 . 093E+01 -0 .000 0.003 0.000

700 .0000 2 . 0 1 A E+00 1 .691E+01 1 . 893E+0

1

9.979E+01 7.320E-01 1 . 1 2AE+01 -0 .000 0.003 0.000 800.0000 2 . 02AE+00 1 . 939E+0

1

2. 1 A1E+01 1 . 0 A8E+02 7.530E-01 1 . 150E+01 -0 .000 0.003 0.000 900.0000 2 . 033E+00 2. 187E+01 2. 390E+01 1 . 0 92E+02 7.70AE-01 1 . 17AE+01 - 0.000 0.003 0 .000 1000.0000 2 . 0A0E+00 2 . A35E+0

1

2.639E+01 1 . 1 32E+02 7.853E-01 1 . 1 95E+01 - 0.000 0.003 0.000

126
ELECTRONS IN METHANE

I = A 1 . 7 eV DENSITY = 6 . 672E-0 A g/cm 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(loqI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cra 2 /g g/cm 2 O.OIOO 2 . 829E+01 2 . 603E-03 2.829E+01 1 . 977E-0A 5.026E-05 0 .

0

-0.178 0.200 0.199 0.0125 2.369E+01 2.612E-03 2 . 369E+01 2. 9A7E-0A 6 . 0A5E-05 0 .

0

-0.171 0.191 0.191 0.0150 2.0ASE+01 2 . 620E-03 2.0A9E+01 A.085E-0A 7 . 022E-05 0.0 -0.166 0.185 0 . 1 8 A 0.0175 1 .813E+01 2.625E-03 1 .81 3E+01 5 . 385E-0

A

7 . 967E-05 0 . 0 -0.162 0.180 0.179

0 .0200 1 . 631 E+01 2.630E-03 1 . 632E+01 6 . 8A0E-0

A

8 . 88AE-05 0.0 -0.159 0.176 0.175

0.0250 1 . 369E+01 2 . 6A0E-03 1 .369E+01 1 . 020E-03 1 . 065E-0A 0 . 0 -0 . 1 5A 0.169 0.169

0 .0300 1 . 188E+01 2.651E-03 1 . 188E+01 1 . A1 3E-03 1 . 23AE-0

A

0.0 -0. 1A9 0 . 1 6 A 0 . 1 6 A 0.0350 1 . 055E+0

1

2.662E-03 1 . 056E+0

1

1 .861 E-0 3 1 . 397E-0A 0.0 -0.1A6 0.160 0.160 0.0000 9.536E+00 2.67AE-03 9 . 539E+00 2.360E-03 1 . 556E-0A 0.0 -0 . 1 AA 0.157 0.157

0.0050 8 . 730E+00 2.637E-03 8 . 733E+00 2. 90SE-03 1 .710E-0A 0.0 -0 . 1 A 1 0. 15A 0 . 1 5 A 0.0500 8 . 075E+00 2.700E-03 8 . 078E+00 3 . 50AE-03 1 . 86 0 E-0

A

0.0 -0.139 0.152 0.152

0 . 0550 7 . 532E+00 2.71 AE-03 7 . 53AE+00 A. 1A6E-03 2.006E-0A 0.0 -0.138 0.150 0.150 0.0600 7 . 07AE+00 2.728E-03 7 . 077E+00 A . 83 1 E-0 3 2.1 50E-0A 0.0 -0.136 0.1A8 0. 1 A8

0 .0700 6 . 3AAE+00 2.759E-03 6 . 3A7E+00 6 . 326E-03 2. A29E-0A 0.0 -0.133 0 . 1 A5 0. 1 A5 0.0800 5 . 788E+00 2.791 E-03 5 . 7 90E + 00 7. 978E-03 2.698E-0A 0.0 -0.131 0 . 1 A2 0.1A2

0.0900 5 . 3A9E+00 2 . 826E-03 5 . 352E+00 9 . 777E-03 2. 960E-0A 0.0 -0.129 0. 1A0 0.1 AO 0.1000 A. 995E+00 2.862E-03 A . 998E+00 1 .171 E-02 3.21 AE-0

A

0 .

0

-0.123 0.138 0.138

0.1250 A.350E+00 2.960 E-0 3 A . 353E+00 1 . 70 9E-02 3 . 825E-0

A

0.0 -0 . 1 2A 0.13A 0.1 3A 0.1500 3.915E+00 3 . 066E-03 3.918E+00 2.31 6E-02 A.A07E-0A 0.0 -0.122 0.131 0.131 0.1750 3 . 603E+00 3.178E-03 3 . 606E+00 2. 983E-02 A . 966E-0A 0.0 -0.119 0.129 0.128

0.2000 3.369E+00 3.297E-03 3 . 372E+00 3 . 70 1 E-0 2 5 . 508E-0

A

0.0 -0.118 0.127 0.126 0.2500 3 . 0 AAE+OO 3 . 550 E-0 3 3 . 0 A7E+00 5.266E-02 6 . 550E-0A 0.0 -0.115 0. 12A 0.123

0 . 3000 2.831E+00 3.826E-03 2 . 835E+00 6 . 971 E-02 7.55AE-0A 0.0 -0.112 0.121 0.120

0.3500 2 . 683E+00 A . 1 2 1 E-0 3 2 . 687E+00 8 . 785E-02 8 . 53AE-0

A

0.0 -0.110 0.119 0.118 0.0000 2.576E+00 A. A3AE-03 2 . 580E+00 1 .069E-01 9 . 500E-0

A

0.0 -0.109 0.117 0.116

0.0500 2 . A 96E+0 0 A . 76AE-03 2.501E+00 1 . 266E-0

1

1 . 0A6E-03 0.0 -0.107 0.116 0 . 1 1 A 0.5000 2 . A35E+00 5. 109E-03 2. AA0E+00 1 . A68E-01 1 . 1 A1E-03 0.0 -0.106 0 . 1 1 A 0.113

0.5500 2 . 388E+00 5.A67E-03 2 . 3 93E+0 0 1 .675E-01 1 . 236E-03 0.0 -0 . 1 OA 0.113 0.112

0.6000 2. 351 E+00 5.839E-03 2 . 357E+00 1 .886E-01 1 . 332E-0 3 0.0 -0.103 0.112 0.110

0.7000 2 . 298E+00 6.616E-03 2. 305E+00 2.315E-01 1 . 523E-0 3 0.0 -0.101 0.110 0.108

0.8000 2 . 26AE+00 7 . A32E-03 2 . 272E + 0 0 2.752E-01 1 .717E-03 0.0 -0.100 0.109 0.107 0.9000 2 . 2A3E+00 8.287E-03 2.251 E+00 3.1 95E-01 1 .912E-03 0.0 -0.098 0.107 0.105

1.0000 2 . 230E+00 9.176 E-0 3 2 . 239E+00 3.6A0E-01 2.11 0E-03 0.0 -0.097 0.106 0.10A

1 .2500 2.21 7E+00 1 . 1 53E-02 2 . 229E+00 A.760E-01 2.61 AE-03 0 .

0

-0 .09A 0 . 1 OA 0.101

1 .5000 2.221 E+00 1 . A05E-02 2 . 235E+0 0 5.881 E-0

1

3.133E-03 0.0 -0.092 0.101 0.0 98

1 .7500 2 . 232E+00 1 . 67 1 E-0 2 2 . 2A9E+00 6 . 996E-0

1

3 . 665E-03 0.0 -0.090 0.100 0.096 2.0000 2 . 2A7E+00 1 . 9A9E-02 2 . 26 7E+0 0 8. 103E-01 A . 208E-03 0.0 -0.089 0.0 98 0.09A 2.5000 2 . 280E+00 2 . 53AE-02 2 . 306E+00 1 . 02 9E+00 5.325E-03 0.0 -0.087 0.096 0.092

3.0000 2. 31 AE+00 3.1 52E-02 2.3A5E+00 1 . 2AAE+00 6.A73E-03 0.0 -0.085 0 .09A 0.089

3.5000 2 . 3A5E+00 3 . 7 95E-02 2 . 383E + 0 0 1 . A56E+00 7.6A5E-03 0.0 -0.083 0.092 0.088

A. 0000 2 . 375E+00 A . A62E-02 2. A20E+00 1 . 66 AE+00 8 . 837E-03 0.0 -0.082 0.091 0 . 086

A . 5000 2 . A03E+00 5 . 1 A8E-02 2. A5AE+00 1 .869E+00 1 . OOAE-02 0.0 -0.081 0.090 0.085

5 .0000 2 . A28E+00 5 . 852E-02 2. A87E+00 2.071 E+00 1 . 127E-02 0 .

0

-0.080 0.088 0.083

5.5000 2. A52E+00 6.571 E-02 2.51 7E+00 2.271 E+00 1 . 250 E-02 0.0 -0.079 0.087 0.082

6.0000 2 . A7AE+00 7 . 303E-02 2 . 5A7E+00 2. A69E+00 1 .37AE-02 0.0 -0.078 0 .087 0.081 7.0000 2.51 AE+00 8 . 805E-02 2 . 602E+00 2 . 857E+00 1 . 62AE-02 0.0 -0.077 0.085 0.079

8 . 0000 2 . 5A9E+00 1 . 035E-0

1

2 . 653E+00 3 . 238E+00 1 . 376E-02 0.0 -0.075 0 . 08

A

0.078

9.0000 2.581 E+00 1 . 1 93E-01 2 . 70 0 E+0 0 3.61 1 E+00 2.1 30E-02 0.0 -0 .07A 0.082 0.077 10.0000 2.61 0E+00 1 . 35AE-0

1

2 . 7A5E+00 3. 978E+00 2. 385E-02 0.0 -0 . 07A 0.081 0.075

12.5000 2.671 E+00 1 . 767E-0

1

2 . 8A8E+00 A . 872E+00 3 . 022E-02 0.0 -0 .072 0.079 0.073

15.0000 2 . 722E+00 2.1 9AE-01 2. 9A1 E+00 5.736E+00 3 . 657E-02 0.0 -0.070 0.077 0.071 17.5000 2 . 765E+00 2 . 629E-0

1

3 . 028E+00 6 . 57 3E + 00 A.288E-02 0.0 -0.069 0.075 0.069 20.0000 2 . 803E+00 3 . 073E-0

1

3.110 E + 00 7 . 388E+00 A . 91 2E-02 0.0 -0.063 0 . 07 A 0 .068 25.0000 2 . 863E+00 3. 977E-01 3 . 26 1 E+00 8. 957E+00 6.139E-02 3 . 726E-02 -0.053 0.071 0.063

30 .0000 2. 90AE+00 A . 899E-0

1

3 . 39AE+00 1 .0A6E+01 7 . 336E-02 1 .A61E-01 -0 .0A1 0.066 0.056 35.0000 2 . 935E+00 5 . 835E-0

1

3.51 9E+00 1 . 1 91E+01 8 . 505E-02 2.797E-01 -0.033 0.062 0.0A9

AO .0000 2.960E+00 6.781 E-0

1

3 . 6 38E+00 1 . 330E+0

1

9 . 6 AAE-02 A. 187E-01 -0.028 0.058 O.OAA A5.0000 2.981 E+00 7 . 736E-0

1

3 . 75 AE+00 1 . A66E+01 1 . 075E-0

1

5 . 553E-0

1

-0.025 0.055 0.039 50.0000 2. 998E+00 8.698E-01 3 . 868E+00 1 . 597E+0

1

1 . 183E-01 6.S65E-01 -0.023 0.052 0.036 55.0000 3.01 AE+00 9.667E-01 3. 980E+00 1 . 72AE+0

1

1 . 288E-0

1

8. 1 12E-01 -0.021 0.0A9 0.032

60.0000 3 . 027E+00 1 . 06AE+00 A. 091 E+00 1 . 8 A8E+0

1

1 .391 E-0

1

9.293E-01 -0.019 0 .0A7 0.030 70.0000 3.051 E+OO 1 . 260E+00 A. 31 1 E+00 2 . 086E+0

1

1 . 587E-01 1 . 1 A6E+00 -0.017 0 . 0A3 0.026 80.0000 3 . 070E+00 1 . A58E+00 A . 528E+00 2.312E+01 1 . 773E-0

1

1 .3A1E+00 -0.016 O.OAO 0.023 90.0000 3 . 087E+00 1 . 657E+00 A . 7AAE+00 2.523E+01 1 . 9A9E-0

1

1 . 5 1 7E+00 -0.015 0.037 0.020 100.0000 3. 102E+00 1 . 857E+00 A . 959E+00 2 . 73AE+0

1

2.11 6 E-0

1

1 . 677E+00 -0.01 A 0.035 0.018 125.0000 3. 133E+00 2 . 36 1 E+00 5. A9AE+00 3.21 3E+01 2. A99E-01 2 . 023E + 00 -0.013 0.031 0.015

150.0000 3. 158E+00 2.869E+00 6 . 027E+00 3.6A7E+01 2 . 838E-0

1

2.31 2E+00 -0.012 0.028 0.013

175.0000 3. 178E+00 3 . 380 E + 0 0 6 . 558E+00 A.0A5E+01 3. 1A2E-01 2 . 560E+00 -0.011 0.026 0.011

200 . 0000 3.1 96E+00 3 . 893E+00 7 . 089E+00 A . A 1 1 E + 01 3. A15E-01 2 . 778E+0 0 -0.011 0.02A 0.010 250.0000 3 . 22AE+00 A. 926E+00 8. 150E+00 5.069E+01 3 . 388E-0

1

3. 1 A8E+00 -0.010 0.022 0 .008 300.0000 3 . 2A7E+00 5 . 96 AE+00 9.21 1E+00 5.6A5E+01 A .28AE-01 3 . A57E+00 -0.008 0.020 0.007 350.0000 3 . 26 6 E+0 0 7 . 005E+00 1 . 027E+0

1

6.159E+01 A.623E-01 3 . 72AE+00 -0.008 0.019 0.006

A00 .0000 3 . 282E+0 0 8.051 E+00 1 . 1 33E+01 6 . 622E+0

1

A . 91 6 E-0

1

3. 959E+00 -0.007 0.017 0.006 A50.0000 3 . 295E+00 9 . 099E+00 1 . 239E+0

1

7.0AAE+01 5. 173E-01 A. 169E+00 -0.006 0.016 0.005 500.0000 3 . 307E+00 1 .015E+01 1 . 3A6E+0

1

7.A31E+01 5 . AOOE-O

1

A . 360E+00 -0.005 0.016 0.005 550.0000 3.31 8E+00 1 . 120E+01 1 . A52E+0

1

7.789E+01 5.603E-01 A . 535E+00 -0.005 0.015 O.OOA 600.0000 3 . 328E+00 1 . 225E+0

1

1 . 553E+0

1

8.121E+01 5 . 785E-0

1

A . 6 96E+00 -0 . 00A 0 .01 A 0 . 00 A 700.0000 3 . 3 AAE+OO 1 . A36E+0

1

1 .771 E+01 8 . 723E+0

1

6.100E-01 A. 985E+00 -0.003 0 . 0 1 A 0.003 800.0000 3 . 358E+00 1 . 6 A8E+0

1

1 . 983E+01 9 . 256E+0

1

6.36AE-01 5 . 238E+00 -0.003 0.013 0.003 900.0000 3. 370E+00 1 . 859E+0

1

2.1 96E+01 9 . 735E+0

1

6 . 589E-01 5. A6AE+00 -0.002 0.012 0.002 1000.0000 3.381 E+OO 2.071E+01 2.A09E+01 1 . 01 7E+02 6 .78AE-01 5 . 668E+00 -0.002 0.012 0.002

127
ELECTRONS IN MUSCLE, SKELETAL (ICRP)

I = 75.3 eV DENSITY = 1 . 0 40E+0 0 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS. EPF. d( log1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2/g MeV cm 2 /g g/cm 2 0.0100 2.231E+01 3 .835E-03 2.231E+01 2 . 543E-04 9.366E-05 0.0 -0.199 0.228 0.226 0.0125 1 . 876E+0

1

3.863E-03 1 . 877E + 0

1

3.771 E-04 1 . 1 27E-04 0.0 -0.191 0.217 0.215

0.0150 1 . 628E+0

1

3.880E-03 1 . 629E + 0

1

5 . 205E-04 1 . 3 1 0 E-0 4 0.0 -0.184 0.209 0.207 0.0175 1 . 445E+0

1

3.892E-03 1 . 445E+0

1

6 .338E-04 1 . 485E-04 0.0 -0.179 0.202 0.201 0.0200 1 .303E+01 3. 901 E-03 1 . 303E+0

1

8 .662E-04 1 . 655E-04 0.0 -0.175 0.197 0.196

0.0250 1 . 0 97E + 0

1

3.913E-03 1 . 098E+0

1

1 . 286E-03 1 . 980E-04 0.0 -0.169 0.189 0.138

0.0300 9 . 547E+00 3. 924E-03 9.551 E+00 1 .776E-03 2 . 2 90 E-04 0.0 -0.164 0.183 0.182

0.0350 8 . 493E+00 3.934E-03 8.502E+00 2.332E-03 2 . 587E-04 0.0 -0.160 0.178 0.177

0.0400 7 . 6 92E+00 3 . 946E-03 7 .696E+00 2.951E-03 2.874E-04 0.0 -0.157 0.174 0.173

0.0450 7 . 052E+00 3. 959E-03 7 . 056E+00 3.631 E-03 3.151 E-04 0.0 -0.154 0.170 0.170

0.0500 6 .531 E+00 3. 973E-03 6 . 535E+00 4.368E-03 3.421 E-04 0 .0 -0.152 0.167 0.167

0.0550 6 . 0 99E + 00 3.988E-03 6 . 1 02E+00 5. 160E-03 3 . 683E-04 0.0 -0.150 0.165 0.164

0 .0600 5 . 733E+00 4.004E-03 5 . 737E+00 6.006E-03 3. 939E-04 0 .

0

-0.143 0.162 0.162

0.0700 5. 1 5 1 E+00 4 . 040E-03 5 . 1 55E+00 7.848E-03 4 . 435E-04 0.0 -0.145 0.159 0.158

0.0800 4 . 706E + 00 4.079E-03 4.710 E+00 9.881E-03 4. 912E-04 0.0 -0.142 0.155 0.155

0.0900 4 . 355E+00 4. 122E-03 4 . 359E+00 1 . 20 9E-02 5 . 373E-04 0.0 -0.140 0.153 0.152

0.1000 4.071 E+00 4.168E-03 4 . 075E+00 1 . 447E-02 5.821 E-04 0.0 -0.138 0.150 0.150 0.1250 3 . 552E+00 4.294E-03 3 . 557E+00 2. 106E-02 6 . 389E-04 0.0 -0.134 0.146 0.145

0.1500 3.203E+00 4.431 E-03 3 . 207E+00 2.848E-02 7 . 899E-04 0.0 -0.131 0.142 0.142

0.1750 2.951 E+00 4.579E-03 2 . 956E+00 3 . 662E-02 8.865E-04 0.0 -0.129 0.139 0.139

0.2000 2.763E+00 4 . 734E-03 2 . 768E+00 4.537E-02 9 . 7 95E-0 4 0.0 -0.126 0.137 0.137

0.2500 2.501 E+00 5 . 070E-03 2 . 506E+00 6 . 442E-02 1 . 1 57E-03 0.0 -0.123 0.133 0.133

0 . 3000 2 . 329E+00 5.438E-03 2 . 335E+00 8.51 3E-02 1 . 327E-03 0.0 -0.120 0.130 0.129

0.3500 2.21 1E+00 5 . 8 32E-0 3 2.21 6E+00 1 .071E-01 1 . 4 92E-0 3 0.0 -0.118 0.128 0.127

0.4000 2. 125E+00 6.252E-03 2.131 E+00 1 . 302E-0

1

1 . 653E-03 0.0 -0.116 0.126 0.125

0.4500 2.061 E+00 6 . 694E-03 2 . 068E+00 1 . 540E-0

1

1 .812E-03 0.0 -0.114 0.124 0.123

0.5000 2.01 2E+00 7.158E-03 2.01 9E+00 1 . 785E-0

1

1 . 970E-03 2.181 E-03 -0.102 0.122 0.121 0.5500 1 . 972E+00 7.642E-03 1 . 980E+00 2 . 035E-0

1

2. 128E-03 2. 071 E-02 -0.091 0.119 0.117

0.6000 1 . 941 E+00 8.141 E-03 1 . 949E+00 2.290E-01 2 . 285E-03 4.241 E-02 -0.085 0.115 0.112

0.7000 1 . 895E+00 9 . 1 86 E-03 1 . 904E+00 2.809E-01 2 . 602E-03 9 . 262E-02 -0.076 0.109 0.104

0.8000 1 . 863E+0 0 1 . 028E-02 1 . 874E+00 3.339E-01 2.921 E-03 1 . 488E-0

1

-0.068 0.103 0.097

0 . 9000 1 . 842E+00 1 . 1 43E-02 1 . 853E+00 3.876E-01 3 . 244E-03 2 . 084E-0

1

-0.062 0.098 0.091

1 .0000 1 . 827E+00 1 . 262E-02 1 . 839E+00 4.418E-01 3.571 E-03 2.697E-01 -0.057 0.093 0.085

1 .2500 1 . 806 E+00 1 . 578E-02 1 . 822E+00 5.734E-01 4 . 408E-03 4 . 245E-01 -0.043 0.083 0.073

1 .5000 1 . 799E+00 1 . 91 6E-02 1 . 8 1 8E+0 0 7.158E-01 5 . 272E-03 5.750E-01 -0.042 0.076 0.065

1 .7500 1 . 7 99E+00 2.271 E-02 1 .821 E+00 8.532E-01 6.162E-03 7.181E-01 -0.038 0.070 0.058

2.0000 1 .801 E+00 2.642E-02 1 . 828E+00 9.903E-01 7.074E-03 3 . 529E-01 -0.035 0.065 0.053

2.5000 1 . 8 1 2E+00 3.421 E-02 1 . 846E+00 1 . 263E+00 8. 956E-03 1 . 098E+00 -0.031 0.058 0.045

3.0000 1 . 824E+00 4.241 E-02 1 . 866E+00 1 . 532E+00 1 .090E-02 1 . 31 6E + 00 -0.028 0.053 0.040

3.5000 1 .836E+00 5.095E-02 1 . 887E+00 1 . 798E+00 1 . 289E-02 1 . 50 9E+0 0 -0.026 0.049 0.036

4.0000 1 . 848E+00 5 . 977E-02 1 . 908E+00 2 . 062E+00 1 . 493E-02 1 . 683E+00 -0.025 0.046 0.033

4.5000 1 . 860E+00 6 . 883E-02 1 . 928E+00 2 . 323E+00 1 . 699E-02 1 . 842E+00 -0.023 0.043 0.031 5.0000 1 .870E+00 7.81 IE-02 1 . 948E+00 2 . 580E+00 1 . 908E-02 1 . 986E + 00 -0.023 0.041 0.029

5.5000 1 .880E+00 8.758E-02 1 . 968E + 00 2 . 836E+00 2.11 9E-02 2 . 1 20E+00 -0.022 0.039 0 . 028

6 .0000 1 .889E+00 9.722E-02 1 . 987E+00 3 . 089E+00 2 . 332E-02 2 . 243E+00 -0.021 0.038 0.027 7.0000 1 . 906E+00 1 . 1 70E-0

1

2 . 023E+00 3 . 587E+00 2.761 E-02 2 . 466E+00 -0.020 0.035 0.025

8.0000 1 . 921 E+00 1 .372E-01 2 . 058E+00 4 . 077E+00 3.1 94E-02 2 . 664E+00 -0.019 0.033 0.023

9.0000 1 . 934E+00 1 .579E-01 2 . 092E+00 4 . 559E+00 3.629E-02 2 . 840E+00 -0.019 0.032 0.022

1 0.0000 1 . 946E+00 1 . 7 90E-0

1

2. 125E+00 5 . 033E+00 4.065E-02 3.001 E+00 -0.018 0.030 0.021 12.5000 1 . 971 E+00 2.331E-01 2.205E+00 6. 188E+00 5 . 1 52E-02 3 . 348E+00 -0.016 0.027 0.019

15.0000 1 . 992E+00 2.887E-01 2.281 E+00 7 . 303E+00 6.231 E-02 3 . 640E+00 -0.015 0 .025 0.017

17.5000 2 . 009E+00 3 . 455E-0

1

2 . 354E + 00 8 . 332E+00 7 . 294E-02 3.892E+00 -0.013 0.024 0.016 20.0000 2 . 023E+00 4 . 032E-0

1

2 . 427E + 00 9 . 428E+00 8. 339E-02 4.11 5E+00 -0.012 0.022 0.015 25.0000 2 . 047E+00 5 . 208E-0

1

2 . 568E + 00 1 . 143E+01 1 .037E-01 4 . 497E+00 -0.010 0.020 0.013

30.0000 2 . 066E+00 6.403E-01 2 . 706E+00 1 . 333E+0

1

1 .230E-01 4.818E+00 -0 .008 0.018 0.011 35.0000 2.081 E+00 7.615E-01 2 . 842E+00 1 .51 3E+01 1 .41 5E-01 5 . 096E+00 -0.007 0.017 C.010 40.0000 2 . 0 94E+0 0 8 . 838E-0

1

2. 978E+00 1 . 685E+0

1

1 . 592E-0

1

5 . 341 E+00 -0.006 0.015 0.008

45.0000 2 . 1 05E+00 1 . 007E + 00 3.11 2E+00 1 .849E+01 1 . 760E-0

1

5 . 560E+00 -0.005 0.014 0.007 50.0000 2.1 15E+00 1 .131 E+00 3 . 247E+00 2.006E+01 1 . 920E-01 5 . 758E+00 -0.004 0.013 0.007 55.0000 2. 124E+00 1 . 256E+00 3. 380E+00 2. 157E+01 2.073E-01 5 . 938E+00 -0.003 0.013 0.006 60.0000 2 . 1 32E+00 1 . 382E+00 3.51 4E+00 2 . 302E+0

1

2.21 9E-01 6 . 1 05E+00 -0.003 0.012 0.005

70.0000 2. 146E+00 1 . 635E+00 3 . 780E+00 2 . 577E+0

1

2 . 492E-0

1

6.401 E+00 -0.002 0.011 0.004 80.0000 2 . 1 58E+00 1 . 88 9E+0 0 4 . 0 47E+0 0 2 . 832E+0

1

2.743E-01 6 . 660E+00 -0.002 0.010 0.004

90.0000 2 . 1 68E+00 2. 145E+00 4.31 3E+00 3.071 E+0

1

2. 974E-01 6 . 890E+00 -0.001 0.009 0.003

100.0000 2 . i 77E+00 2 . 402E+00 4 . 580E+00 3 . 296E+0

1

3. 188E-01 7 . 096E+00 -0.001 0.009 0.003

125.0000 2.1 97E+00 3.049E+00 5 . 246E+00 3 . 806E+0

1

3 . 659E-01 7 . 536E+00 -0.001 0.008 0 . 002 150.0000 2.21 2E+00 3 . 70 1 E+00 5. 91 3E+00 4 . 255E+0

1

4.056E-01 7 . 8 96 E + 0 0 -0.001 0 . 007 0.002

175.0000 2 . 226 E+0 0 4 . 356E+00 6.581 E+00 4 . 655E+0

1

4 . 398E-0

1

8 . 202E+00 -0 .000 0.006 0.001 200.0000 2 . 237E+00 5.01 3E+00 7 . 250 E+0 0 5.017E+01 4.694E-01 8 . 4S7E+00 -0.000 0 .006 0.001

250 .0000 2 . 256E+00 6 . 334E+00 8 . 590E+00 5 . 650E+0

1

5. 187E-01 8.911 E+00 -0.000 0.005 0.001 300.0000 2. 271 E+00 7.661 E+00 9 . 932E+00 6.191 E+0

1

5.581E-01 9 . 274E+00 -0.000 0.005 0.001 350.0000 2 . 284E + 0 0 3. 992E+00 1 . 128E+01 6 . 663E+0

1

5. 905E-01 9.581 E+00 -0.000 0.004 0.001 400.0000 2 . 296E+00 1 . 0 33E+0

1

1 . 262E+0

1

7 . 082E+0

1

6 . 177E-01 9 . 848E+00 -0.000 0.004 0.001

450 .0000 2 . 306E+00 1 . 1 66E + 01 1 . 397E+0

1

7 . 458E+0

1

6.409E-01 1 . 008E+0

1

-0.000 0.004 0.000 500.0000 2. 31 5E+00 1 . 300E+0

1

1 . 53ZE+0

1

7 . 800E+0

1

6.610E-01 1 . 029E+01 -0.000 0.004 0 .000 550.0000 2.323E+00 1 . 434E+0

1

1 . 667E+0

1

8.11 3E+01 6 . 787E-0

1

1 . 048E+0

1

-0.000 0.004 0 .000 600.0000 2. 330E+00 1 . 568E + 01 1 .301E+01 8.401 E+01 6 . 943E-01 1 . 066 E + 0

1

-0 . 000 0.004 0.000 700.0000 2 . 343E+00 1 . 837E+0

1

2 . 072E+01 8.918E+01 7.207E-01 1 . 0 97E + 0

1

-0.000 0.003 0.000 800.0000 2 . 354E+00 2. 1 06E+01 2.342E+01 9 . 372E+0

1

7.423E-01 1 . 1 23E+0

1

-0.000 0.003 0 .000 900.0000 2. 364E+00 2.376E+01 2.612E+01 9 . 776 E+0

1

7.603E-01 1 . 1 47E+01 -0.000 0.003 0.000 1000.0000 2. 373E+00 2 . 64 5E+0

1

2.883E+01 1 . 0 1 4E+02 7.756E-01 1 . 1 68E+01 - 0.000 0.003 0.000

128
ELECTRONS IN MUSCLE, STRIATED (ICRU)

I = 7 A . 7 eV

ENERGY STOPPING POWER COLLISION RADIATIVE TOTAL MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2/g 0.0100 2 . 237E+0

1

3.816E-03 2 . 238E+0

1

0.0125 1 .881E+01 3.8AAE-03 1 . 882E+0

1

0.0150 1 . 6 33E+0

1

3.862E-03 1 . 633E+0

1

0.0175 1 . AA9E+01 3.873E-03 1 . AA9E+01 0.0200 1 . 306E+01 3.882E-03 1 . 307E+0

1

0.0250 1 . 100E+01 3.89AE-03 1 . 1 00E+01 0.0300 9.571 E+00 3. 905E-03 9 . 575E+00 0.0350 8.51 9E+00 3.916E-03 8 . 523E+00

0 .OAOO 7.71 1E+00 3. 928E-03 7.71 5E+00 0.0A50 7.069E+00 3.9A1E-03 7.073E+00

0.0500 6 . 5A7E+00 3 . 955E-03 6 .551 E+00 0.0550 6.1 13E+00 3 . 970E-03 6 . 1 1 7E+00 0.0600 5 . 7A7E+00 3. 986E-03 5.751 E+00 0.0700 5.163E+00 A . 0 22E-03 5. 167E+00

0.0800 A.717E+00 A.061E-03 A . 72 1 E+00 0.0900 A . 365E+00 A. 10AE-03 A . 369E+00

0.1000 A . 080 E+00 A . 1 50E-03 A . 08AE+00

0.1250 3.561 E+00 A . 275E-03 3.565E+00

0.1500 3 . 2 1 0 E + 00 A.A12E-03 3.21 AE+00

0.1750 2 . 958E+00 A . 558E-03 2. 962E+00

0.2000 2.769E+00 A. 71 AE-03 2.77 AE+0 0

0 . 2500 2 . 506E+00 5.0A8E-03 2.51 1E+00 0.3000 2 . 335E+00 5.A15E-03 2 . 3A0E+00

0 . 3500 2.21 5E+00 5.808E-03 2.221 E+00

0 . AOOO 2. 129E+00 6 . 226E-03 2.1 36E+00

0 . A500 2 . 065E+00 6 . 666E-03 2 . 072E+00

0.5000 2.01 6E+00 7.1 29E-03 2 . 023E+00

0.5500 1 . 97 6 E+00 7.610E-03 1 . 98AE+00

0 .6000 1 . 9A5E+00 8.108E-03 1 . 953E+00

0.7000 1 . 398E+00 9. 1 A8E-03 1 . 907E+00

0.8000 1 . 86 6 E + 0 0 1 . 02AE-02 1 .877E+00

0 . 9000 1 . 8A5E+00 1 . 1 39E-02 1 .856E+00

1.0000 1 .830E+00 1 . 257E-02 1 . 8A2E+0 0

1 .2500 1 . 80 9E + 0 0 1 . 572E-02 1 . 825E+00

1 .5000 1 . 80 2E+0 0 1 . 908E-02 1 .821 E+00

1 .7500 1 .801 E+00 2.263E-02 1 . 82AE+00

2.0000 1 .80AE+00 2 . 632E-02 1 .830E+00

2.5000 1 .81 AE+00 3. A08E-02 1 . 8A8E+0 0 3.0000 1 . 826 E+OO A . 225E-02 1 . 86 9E+00 3.5000 1 . 83 9E+00 5 . 076E-02 1 . 890E+00

A. 0000 1 .851 E+00 5. 95AE-02 1 . 91 OE+OO

A. 5000 1 .862E+00 6 . 857E-02 1 . 931 E+00 5.0000 1 . 87 3E + 00 7.782E-02 1 . 951 E+00 5.5000 1 . 883E+00 8 . 725E-02 1 . 970E+00

6 .0000 1 . 892E+00 9.686E-02 1 . 989E+00 7.0000 1 . 909E+00 1 .165E-01 2 . 026E+00 8.0000 1 . 92AE+00 1 .367E-01 2.061 E+00 9.0000 1 . 937E+00 1 .57AE-01 2 . 09AE+00

10.0000 1 . 9A9E+00 1 . 78AE-0

1

2 . 1 27E+00

12.5000 1 . 97AE+00 2.323E-01 2 . 206E+00

15.0000 1 . 995E+00 2 . 877E-0

1

2 . 282E+00

17.5000 2.01 2E+00 3. AA3E-01 2 . 356E+00

20.0000 2 . 026E+00 A.018E-01 2 . A28E+00

25.0000 2 . 050E+00 5. 189E-01 2.569E+00

30.0000 2 . 068E+00 6.381E-01 2 . 706E+00

35.0000 2 . 08 AE+OO 7.588E-01 2 . 8A2E+00

AO. 0000 2 . 0 97E+00 8.807E-01 2. 977E+00 A5.0000 2 . 1 08E+00 1 . 00 AE+00 3.11 1 E+00 50.0000 2.11 8E+00 1 . 1 27E+00 3 . 2A5E+00

55.0000 2. 1 26E+00 1 . 252E+00 3 . 378E+00

60 .0000 2. 13AE+00 1 . 377E+00 3.51 2E+00 70.0000 2.1 A8E+00 1 . 629E+00 3 . 777E+00

80.0000 2. 160E+00 1 . 883E+00 A . 0 A3E+00

90.0000 2.171 E+00 2.1 38E+00 A . 308E+00

100.0000 2 . 1 80E+00 2 . 39AE+00 A . 57 AE+00 125.0000 2.1 99E+00 3 . 039E+00 5 . 238E+00

1 50.0000 2.21 5E+00 3. 688E+00 5 . 903E+00

175.0000 2 . 228E+00 A. 3A1E+00 6.569E+00

200.0000 2 . 2A0E+00 A . 996E+00 7 . 236E+00

250.0000 2 . 259E+00 6.31 3E+00 8.571 E+00 300.0000 2 . 27AE+00 7 . 6 35E+0 0 9. 90 9E + 00 350.0000 2 . 287E + 00 8. 962E+00 1 . 1 25E+0

1

AOO.OOOO 2 . 299E+00 1 . 029E+0

1

1 . 259E+0

1

A50 .0000 2. 309E+00 1 . 162E+01 1 . 393E+0

1

500.0000 2.31 7E+00 1 .296E+01 1 . 528E+0

1

550 .0000 2 . 325E+00 1 . A30E+01 1 . 662E+0

1

500.0000 2 . 333E+00 1 .563E+01 1 . 7 97E+0

1

700.0000 2 . 3A6E+00 1 .831 E+01 2.066E+01 800.0000 2 . 357E+00 2.099E+01 2 . 335E+0

1

900.0000 2 . 367E+00 2. 368E+01 2. 605E+01 1000.0000 2 . 376E+00 2 . 637E+0

1

2.87AE+01

r

DENSITY = 1 . OAOE+OOi g/cm 3

CSDA RADIATION DENS.EFF. d( log )/d( logl

)

RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

g/cm 2 536E-0A 9 . 293E-05 0.0 -0.199 0.227 0.225 759E-0A 1.11 9E-0A 0 .

0

-0.190 0.216 0.215

1 90E-0A 1 . 300E-OA 0.0 -0 . 18A 0 . 208 0.207 818E-0A 1 . A7AE-0A 0.0 -0.179 0.202 0.201 638E-0A 1 . 6 A2E-0

A

0.0 -0.175 0.197 0.196 2S3E-03 1 . 965E-0A 0.0 -0.169 0.188 0.188

771 E-03 2 . 273E-0A 0.0 -0 . 1 6A 0.182 0.182 326E-03 2.568E-0A 0.0 -0.160 0.177 0.177

9AAE-03 2.853E-0A 0.0 -0.157 0.173 0.173

621 E-03 3.128E-0A 0 .

0

-0 . 1 5A 0.170 0.169 356E-03 3 . 396E-0

A

0 .0 -0.152 0.167 0.167

1 A7E-03 3.657E-0A 0 . 0 -0.150 0 . 1 6 A 0 . 1 6A

991 E-03 3.911 E-OA 0 .0 -0 . 1 A8 0.162 0.162 829E-03 A. AOAE-OA 0.0 -0 . 1 A5 0.158 0.158 857E-03 A.878E-0A 0.0 -0.1A2 0.155 0 . 1 55 206E-02 5.336E-0A 0.0 -0 . 1 AO 0.153 0.152 AA3E-02 5 . 780 E-OA 0.0 -0.138 0.150 0.150 101E-02 6 .8A1 E-OA 0.0 -0.1 3A 0 . 1 A6 0.1 A5 8A1E-02 7.8A5E-0A 0.0 -0.131 0 . 1 A2 0.1A2 653E-02 8 .805E-0A 0.0 -0 . 1 28 0.139 0.139 526E-02 9.728E-0A 0.0 -0.126 0.137 0.136 A27E-02 1 .1A9E-03 0 . 0 -0.123 0.133 0.132 A9AE-02 1 .318E-03 0.0 -0 . 1 20 0.130 0.129

069E-01 1 . A82E-03 0 .

0

-0.118 0.128 0.127

299E-01 1 . 6A2E-03 0.0 -0.116 0.126 0.125

537E-01 1 .801E-03 0.0 -0 . 1 1 A 0 . 1 2 A 0.123

781 E-01 1 . 957E-03 A.2A0E-03 -0.098 0.122 0.120

031E-01 2.1 1 AE-03 2 . 378E-02 -0.090 0.118 0.116

285E-01 2.271 E-03 A . 63AE-02 -0 .08A 0.115 0.112

803E-01 2 . 585E-0 3 9 . 793E-02 -0.075 0.108 0 . 1 0 A 332E-01 2.903E-03 1 .553E-01 -0.068 0.102 0.096 868E-01 3 . 22AE-03 2. 158E-01 -0.062 0.097 0.090

A09E-01 3.550E-03 2.778E-01 -0.057 0.092 0 . 08 A 77AE-01 A . 382E-03- A.339E-01 -0.0A8 0.083 0.073

1A6E-01 5 . 2A2E-03 5.852E-01 -O.OA2 0.0 75 0 .06A 513E-01 6. 127E-03 7 .289E-01 -0.038 0.070 0.057

886E-01 7.035E-03 8.6A1E-01 -0.035 0.065 0.052

26 1 E+00 8.907E-03 1 . 1 1 OE + OO -0.031 0 .058 0 .0A5 530E+00 1 . 08AE-0 2 1 . 327E+00 -0.028 0.053 0.0A0 796E+00 1 . 283E-02 1 .521 E+00 -0.026 0 .0A9 0.036 059E+00 1 . A85E-02 1 . 695E+00 -0 .02A 0 .0A6 0.033

31 9E+00 1 . 690E-02 1 . 853E+00 -0.023 0 .0A3 0.031 577E+00 1 .898E-02 1 . 998E+00 -0.023 0 .0A1 0.029 832E+00 2. 108E-02 2 . 1 31 E + 00 -0.022 0.039 0.023 08AE+00 2.320E-02 2 . 255E+00 -0.021 0.038 0.027 583E+00 2 . 7A7E-02 2 . A78E+00 -0.020 0.035 0.025 072E+00 3. 178E-02 2.675E+00 -0.019 0.033 0.023 553E+00 3.61 IE-02 2 . 852E+0 0 -0.018 0.032 0.022 027E+00 A . 0 A5E-02 3.01 3E+00 -0.018 0.030 0.021

181 E+00 5. 128E-02 3.361 E+00 -0.016 0.027 0.019 295E+00 6 . 202E-02 3 . 6 52E+0 0 -0.015 0.025 0.017 373E+00 7.261E-02 3. 905E+00 -0.013 0.02A 0.016 A18E+00 8 . 302E-02 A.128E+00 -0.012 0.022 0.015

1 A2E+01 1 .032E-01 A. 51 1 E+00 -0.010 0.020 0.012

332E+01 1 .225E-01 A . 333E+00 -0 .008 0.018 0.011 512E+01 1 . A1 0E-01 5.11 1 E+00 -0.007 0.016 0.009

68AE+01 1 . 585E-0

1

5 . 356 E+00 -0.005 0.015 0.008

8A8E+01 1 . 753E-0

1

5 . 576E+00 -0.005 0.01 A 0.007

005E+01 1 . 91 3E-01 5 . 77 AE+00 -0 .00A 0.013 0.007

156E+01 2.065E-01 5 . 955E+00 -0.003 0.013 0.006 301E+01 2.21 1 E-01 6.121 E+00 -0.003 0.012 0.005

576E+01 2.A8AE-01 6.A18E+00 -0 .002 0.011 0 . 00A 832E+01 2.735E-01 6 . 677E+00 -0.002 0.010 0 . OOA

071 E+01 2 . 965E-0

1

6 . 907E+00 -0.001 0.009 0.003

297E+01 3. 179E-01 7.11 3E+00 -0.001 0.009 0.003

807E+01 3 .6A9E-01 7 . 553E+00 -0.001 0.008 0 .002 256E+01 A.0A6E-01 7.91 3E+00 -0.001 0.007 0.002

658E+01 A . 388E-0

1

8.21 9E+00 -0.000 0.006 0.001 020E+01 A.68AE-01 • 8 . A8AE+00 -0.000 0.006 0.001 65AE+01 5. 1 77E-01 8 . 923E+00 -0.000 0.005 0.001

1 96E+01 5.571E-01 9. 291 E+00 -0.000 0.005 0.001 670E+01 5 . 8 95E-0

1

9 . 593E+00 -0.000 0 .00A 0.001 089E+01 6 . 1 68E-01 9 . 865E+00 -0.000 0 .00A 0.001 A67E+01 6.A00E-O1 1 .010E + 01 -0 .000 O.OOA 0 . 000 809E+01 6 .602E-01 1 .031 E+01 -0 .000 0 .00A 0.000

123E+01 6 .778E-01 1 . 050E+01 -0.000 O.OOA 0.000

A12E+01 6 . 935E-01 1 . 067E+01 -0.000 0.003 0.000

931E+01 7 . 1 99E-01 1 . 098E+0

1

-0.000 0.003 0.000

386E+01 7.A16E-01 1 . 125E+01 -0.000 0.003 0 .000 791E+01 7 . 596E-0

1

1 . 1 A8E+01 -0.000 0.003 0.000

01 6E+02 7.750E-01 1 . 170E+01 -0.000 0.003 0.000

129

2

35

6S

1

12

2

3A

55

7

9

1

12

2

3

A

68

1

1

1

12

2

2

33

A

5

78

9

1

1

1

2

2

22

3

3A

A

5

678

9

1

1

1

1

12

2

2

2

2

3

3

3A

A

55

66

7

7

7

88

8

9

9

1
ELECTRONS IN MUSCLE-EQUIVALENT LIQUID, WITH SUCROSE

I = 74.3 eV DENSITY =1.1 1 OE+OO1 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS . EFF. d ( log1 )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV c» 2/g MeV cm 2 /g MeV cm 2/g g/cm 2 0.0100 2.233E+01 3.749E-03 2 . 233E + 0

1

2.541E-04 9.1 64E-05 0 .

0

-0.198 0.227 0.225

0.0125 1 . 877E+0

1

3.774E-03 1 . 878E+0

1

3 . 767E-04 1 . 102E-04 0.0 -0.190 0.216 0.215

0.0150 1 . 629E+0

1

3. 789E-03 1 .630E+01 5.201E-04 1 . 280E-04 0.0 -0.184 0.208 0.207 0.0175 1 . 445E+0

1

3.799E-03 1 . 446E+01 6 . 833E-04 1 .451 E-04 0.0 -0.179 0.202 0.201 0.0200 1 .303E+01 3.807E-03 1 . 304E+0

1

8 . 657E-04 1 .617E-04 0.0 -0.175 0.196 0.195

0.0250 1 . 0 98E+0

1

3.818E-03 1 . 0 98E + 0

1

1 . 285E-0 3 1 . 934E-04 0.0 -0.163 0.188 0.187

0.0300 9 . 549E+00 3.827E-03 9 . 553E+00 1 .775E-03 2 . 235E-04 0 . 0 -0.164 0.182 0.181 0.0350 8 . 499E+00 3 . 837E-03 8 . 503E+00 2.331E-03 2 . 525E-04 0.0 -0.160 0.177 0.177

0 .0400 7 . 6 93E+00 3.848E-03 7 . 6 96E+00 2 . 950E-03 2.804E-04 0 .

0

-0.157 0.173 0.173

0.0450 7 . 052E+00 3.861E-03 7 . 056E+00 3.630E-03 3 . 074E-04 0.0 -0.154 0.170 0.169

0.0500 6.531 E+00 3.874E-03 6 . 535E+00 4 . 367E-03 3 . 337E-04 0.0 -0.151 0.167 0.166 0.0550 6.099E+00 3.889E-03 6 . 1 02E+00 5.159E-03 3 . 593E-04 0.0 -0.149 0.164 0.164

0.0600 5 . 733E+00 3. 905E-03 5 . 737E+00 6 . 005E-03 3.843E-04 0.0 -0.148 0.162 0.162

0.0700 5. 150E+00 3 . 940E-03 5 . 1 54E+00 7 . 847E-03 4 . 326 E-04 0.0 -0.144 0.158 0.158

0.0800 4 . 705E+00 3. 979E-03 4.709E+00 9.880E-03 4.792E-04 0.0 -0 . 1 42 0.155 0.155

0.0900 4 . 354E+00 4.021E-03 4 . 358E+00 1 . 20 9E-02 5.241 E-04 0.0 -0.140 0.152 0.152

0.1000 4 . 070E+00 4 . 066E-03 4 . 074E+00 1 . 447E-02 5.678E-04 0.0 -0.138 0.150 0.150

0.1250 3 . 552E+00 4 . 1 90E-03 3 . 556E+00 2.106E-02 6.720E-04 0.0 -0.134 0.146 0.145

0.1500 3 . 202E+00 4.325E-03 3 . 206E+00 2.848E-02 7 . 707E-04 0.0 -0.131 0.142 0.142

0.1750 2 . 950E+00 4.469E-03 2 . 955E+00 3 . 662E-02 8.651 E-04 0.0 -0.128 0.139 0.139

0.2000 2 . 762E+00 4.622E-03 2 . 767E+00 4 . 538E-02 9 . 559E-04 0.0 -0.126 0.137 0.136

0.2500 2. 500E+00 4.951E-03 2 . 505E+00 6 . 444E-02 1 . 1 30E-03 0.0 -0.123 0.133 0.132

0.3000 2 . 329E+00 5.31 IE-03 2 . 334E+00 8.51 6E-02 1 . 296E-03 0.0 -0.120 0.130 0.129

0 . 3500 2.21 0E+00 5.698E-03 2.21 5E+00 1 . 072E-0

1

1 . 457E-03 0.0 -0.118 0.128 0.127

0.4000 2. 124E+00 6 . 109E-03 2 . 1 30E+00 1 . 302E-0

1

1 .615E-03 0.0 -0.116 0.126 0.125

0.4500 2 . 060E+00 6.543E-03 2 . 066E+00 1 .541 E-01 1 .771 E-03 0.0 -0.113 0.124 0.123

0.5000 2. 01 OE+OO 6.997E-03 2.01 7E+00 1 . 786E-0

1

1 . 925E-03 1 .51 9E-02 -0.092 0.121 0.119

0.5500 1 . 970E+00 7.470E-03 1 . 977E+00 2.036E-01 2.080E-03 3 . 828E-02 -0.086 0.117 0.114 0.6000 1 . 938E+00 7 . 960E-03 1 . 946E+00 2.291E-01 2 . 234E-03 6 . 393E-02 -0.081 0.113 0.109

0.7000 1 .891 E+00 8. 983E-03 1 . 900E+00 2.812E-01 2 . 545E-03 1 .207E-01 -0.072 0.106 0.101 0.8000 1 . 85 9E+00 1 . 006E-02 1 . 86 9E+00 3.343E-01 2.859E-03 1 .821 E-01 -0.065 0.100 0.094

0 . 9000 1 .837E+00 1 .1 18E-02 1 .848E+00 3.881E-01 3. 176E-03 2.460E-01 -0.060 0.095 0.087

1 .0000 1 . 822E+00 1 . 235E-02 1 . 834E+00 4.424E-01 3.498E-03 3.108E-01 -0.055 0.090 0.082

1 .2500 1 .80 1 E+00 1 . 545E-02 1 .81 6E+00 5.795E-01 4.321 E-03 4.720E-01 -0.047 0.081 0.071

1 .5000 1 . 793E+00 1 .876E-02 1 . 8 1 2E+00 7. 174E-01 5.171 E-03 6 .269E-01 -0.041 0.073 0.062

1 .7500 1 . 7 93E+00 2 . 224E-02 1 .81 5E+00 8 . 553E-0

1

6.046E-03 7 . 7 30 E-0

1

-0.037 0.068 0.056 2.0000 1 . 795E+00 2.587E-02 1 .821 E+00 9.928E-01 6 . 944E-03 9.100E-01 -0.034 0.063 0.051 2.5000 1 . 805E+00 3.351E-02 1 . 839E+00 1 . 266 E+00 8.797E-03 1 . 1 58E+00 -0.030 0.056 0.044

3.0000 1 .81 7E+00 4.155E-02 1 . 85 9E+00 1 . 537E+00 1 .071E-02 1 . 377E+00 -0.027 0.051 0.039

3.5000 1 .830E+00 4. 992E-02 1 . 880 E+00 1 .804E+00 1 . 267E-02 1 . 572E+00 -0.026 0.048 0.035

4.0000 1 . 842E+00 5.857E-02 1 . 900E+00 2.069E+00 1 . 468E-02 1 . 747E+00 -0.024 0.045 0.033

4.5000 1 . 853E + 0 0 6 . 746E-02 1 . 920E+00 2 . 330E+00 1 .671E-02 1 . 905E+00 -0.023 0.042 0.030 5.0000 1 . 86 3E+0 0 7 . 656E-02 1 . 940E+00 2.589E+00 1 . 877E-02 2 . 050E+00 -0.022 0.040 0.029 5.5000 1 . 873E+00 8.585E-02 1 . 959E+00 2 . 846 E + 0 0 2 . 085E-02 2. 184E+00 -0.022 0.038 0.027 6.0000 1 . 883E+00 9.531E-02 1 . 978E+00 3. 100E+00 2.294E-02 2 . 308E+00 -0.021 0.037 0.026

7.0000 1 . 899E+00 1 . 147E-01 2.01 4E+00 3.601 E+00 2.71 8E-02 2.531 E+00 -0.020 0.035 0.024

8.0000 1 . 9 1 4E+00 1 .346E-01 2 . 049E+00 4 . 0 93E+00 3. 144E-02 2 . 729E+00 -0.019 0.033 0.023

9.0000 1 . 927E+00 1 . 549E-0

1

2 . 082E+00 4 . 577E+00 3 . 573E-02 2 . 906E+00 -0.018 0.031 0.022

10.0000 1 . 939E+00 1 . 756E-0

1

2.11 5E+00 5 . 054E+00 4.003E-02 3 . 067E+00 -0.018 0.030 0.021 12.5000 1 . 964E+00 2.287E-01 2.1 93E+00 6.21 5E+00 5 . 076E-02 3.41 6E+00 -0.016 0.027 0.019

15.0000 1 . 984E+00 2 . 832E-0

1

2 . 268E+00 7 . 336E+00 6.141 E-02 3.709E+00 -0.014 0.025 0.017

17.5000 2.001 E+00 3.390E-01 2.340E+00 8.421 E+00 7 . 1 92E-02 3. 963E+00 -0.013 0.023 0.016 20.0000 2.01 6E+00 3.957E-01 2.41 1E+00 9 . 473E+00 8 . 224E-02 4 . 187E+00 -0.012 0.022 0.014

25.0000 2 . 039E + 00 5.11 IE-01 2 . 550E+00 1 . 1 49E+01 1 . 023E-0

1

4 . 57 2E+00 -0.009 0.019 0.012

30.0000 2 . 057E+00 6.285E-01 2 . 686E+00 1 . 340E+0

1

1 .215E-01 4 . 8 95E+0 0 -0.008 0.018 0.011 35.0000 2. 072E+00 7 . 474E-0

1

2 . 820E+00 1 . 522E+0

1

1 . 398E-0

1

5. 175E+00 -0.006 0.016 0.009

40.0000 2 . 085E+00 8 . 676E-0

1

2 . 953E+00 1 . 6 95E+0

1

1 . 573E-0

1

5 . 422E+00 -0.005 0.015 0.008

45.0000 2 . 0 96E+00 9 . 887E-0

1

3 . 085E+00 1 . 860E+0

1

1 . 740E-0

1

5 . 642E+00 -0 .004 0.014 0.007

50.0000 2. 106E+00 1 . 1 1 1E+00 3.217E+00 2.01 9E+01 1 .899E-01 5.841 E+00 -0.004 0.013 0.006 55.0000 2.11 5E+00 1 . 233E+00 3 . 348E+00 2. 172E+01 2.050E-01 6 . 023E+00 -0.003 0.012 0.006 60.0000 2. 123E+00 1 . 357E+00 3 . 479E+00 2.318E+01 2.1 96E-01 6 . 1 89E+00 -0.003 0.012 0.005

70.0000 2.1 37E+00 1 . 6 0 5E+0 0 3 . 742E+00 2 . 595E+0

1

2.468E-01 6 . 487E+00 -0.002 0.010 0.004

80.0000 2 . 1 48E+00 1 . 855E+0 0 4.003E+00 2 . 853E+0

1

2.717E-01 6 . 747E+00 -0.002 0.010 0.004

90.0000 2. 159E+00 2. 107E+00 4 . 265E+00 3.095E+01 2. 948E-01 6 . 97 7 E+00 -0.001 0.009 0.003

100.0000 2 . 1 68E+00 2 . 359E+00 4 . 527E+00 3 . 323E+0

1

3.161 E— 0

1

7 . 1 84E+00 -0.001 0.008 0.003

125.0000 2. 187E+00 2 . 995E+00 5 . 1 82E+00 3.839E+01 3.630E-01 7 . 624E+00 -0.001 0.007 0.002

1 50 . 0000 2.203E+00 3 . 6 35E+00 5 . 337E+00 4 . 293E+0

1

4.027E-01 7 . 985E+00 -0.001 0 .007 0 . 002 175.0000 2.21 6E+00 4 . 278E+00 6 . 494E+00 4.699E+01 4.368E-01 8 . 2 91 E+0 0 -0.000 0.006 0.001 200.0000 2 . 227E+00 4. 924E+00 7.151 E+00 5 . 066E+01 4.664E-01 8 . 556E + 00 -0.000 0.006 0.001 250.0000 2 . 246E + 00 6 .221 E+00 8 . 468E+00 5 . 707E+0

1

5.1 57E-01 9 . OOOE + OO -0.000 0.005 0.001 300.0000 2 . 262E + 00 7 . 525E+00 9 . 787E+00 6 . 256 E + 0

1

5.552E-01 9 . 364E+00 -0.000 0.005 0.001 350.0000 2 . 275E+00 8 . 833E+00 1 . 1 1 1E+01 6 . 736E+0

1

5.877E-01 9.671 E+00 -0 .000 0.004 0.001 400.0000 2 . 286E+00 1 .014E+01 1 . 243E+0

1

7.161 E+01 6.150E-01 9. 938E+00 -o.coo 0.004 0.000 450.0000 2 . 296E+00 1 . 146E+01 1 . 375E+01 7 . 543E+0

1

6.383E-01 1 . 0 1 7E + 01 -0 .000 0.004 0.000 500.0000 2. 305E+00 1 . 277E+0

1

1 . 508E+0

1

7 . 890E+0

1

6.585E-01 1 . 038E + 01 -0.000 0 .004 0.000 550.0000 2.31 3E+00 1 .409E+01 1 . 640E+0

1

8 . 208E+0

1

6 . 762E-0

1

1 . 057E+0

1

-0.000 0.003 0.000 600.0000 2 . 320E+00 1 .541 E+01 1 . 773E+0

1

8.501 E+0

1

6 .91 9E-01 1 . 075E+0

1

-0.000 0.003 0.000 700.0000 2 . 333E+00 1 . 805E+0

1

2 . 038E+0

1

9 . 027E+0

1

7. 184E-01 1 . 106E + 01 -0.000 0.003 0.000 300.0000 2 . 344E+00 2 . 069E+0

1

2 . 304E+01 9 . 483E+0

1

7.401 E-0

1

1 . 1 32E+01 -0.000 0.003 0.000 900.0000 2. 354E+00 2. 334E+01 2.570 E+0

1

9 . 899E+0

1

7 . 583E-0

1

1 . 1 56 E+0

1

-0.000 0.003 0.000 1000.0000 2 . 363E+00 2 . 599E+0

1

2 . 835E+0

1

1 . 027E+02 7.737E-01 1 . 1 77E+01 -0.000 0.003 0.000

130
ELECTRONS IN MUSCLE-EQUIVALENT LIQUID, WITHOUT SUCROSE

I = 74.2 eV DENSITY = 1 . 070E+0Ci g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. cKlog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cra 2/g MeV cm 2/g g/cm 2 0.0100 2.241E+01 3.777E-03 2.241E+01 2.531 E-04 9.1 94E-05 0.0 -0.198 0.227 0.225

0.0125 1 . 884E+0

1

3.803E-03 1 . 885E + 0

1

3 . 753E-04 1 . 1 06E-04 0 .0 -0.190 0.216 0.214 0.0150 1 . 6 35E + 0

1

3.818E-03 1 .636E+01 5. 181 E-04 1 . 285E-04 0.0 -0.184 0 . 208 0.207 0.0175 1 .451E+01 3.829E-03 1 .451 E+01 6 .807E-04 1 . 456E-04 0 .0 -0.179 0.202 0.200 0.0200 1 . 308E+0

1

3.836E-03 1 .309E+01 3 . 625E-04 1 . 623E-04 0.0 -0.175 0.196 0.195 0.0250 1 . 102E+01 3 . 847E-03 1 . 1 02E+01 1 -281E-03 1 . 941 E-04 0.0 -0.168 0.188 0.187 0.0300 9 . 584E+00 3.857E-03 9 . 5S8E+00 1 . 769E-03 2 . 244E-04 0.0 -0.164 0.182 0.181 0.0350 8 . 530E+00 3.867E-03 3 . 534E+00 2.323E-03 2 . 535E-04 0.0 -0.160 0.177 0.177

0 .0400 7.721 E+00 3.878E-03 7 . 725E+00 2. 939E-03 2.81 5E-04 0.0 -0.156 0.173 0.173

0 .0450 7 . 078E+00 3.890E-03 7 . 082E+00 3.61 6E-03 3.086E-04 0.0 -0.154 0.170 0.169

0.0500 6 . 555E+00 3 . 904E-03 6 . 559E+00 4.351E-03 3.350E-04 0 . 0 -0.151 0.167 0.166

0.0550 6. 1 21 E+00 3.91 9E-03 6 . 125E+00 5.1 40E-03 3.607E-04 0 . 0 -0.149 0.164 0.164

0.0600 5 . 754E+00 3 . 935E-03 5.758E+00 5. 983E-03 3.853E-04 0.0 -0.148 0.162 0.162

0.0700 5.16 9E+00 3. 970E-03 5. 173E+00 7.81 9E-03 4 . 343E-04 0.0 -0.144 0.158 0.158 0.0300 4 . 722E+00 4.009E-03 4 . 726E+00 9.844E-03 4.811 E-04 0.0 -0.142 0.155 0.155

0.0900 4 . 370E+00 4.051E-03 4 . 374E+00 1 . 205E-02 5 . 262E-04 0 . 0 -0.140 0.152 0.152

0 . 1000 4 . 085E+00 4.097E-03 4 . 039E+00 1 .441E-02 5.700E-04 0.0 -0.138 0.150 0.150 0.1250 3 . 565E + 00 4.221E-03 3.569E+00 2 . 0 98E-02 6 . 747E-04 0.0 -0.134 0.146 0.145

0.1500 3.213E+00 4.357E-03 3.218E+00 2 . 838E-02 7 . 7 37E-04 0.0 -0.131 0.142 0.142

0 .1750 2.961 E+00 4.502E-03 2. 966E+00 3 . 649E-02 8.684E-04 0.0 -0.128 0.139 0.139 0.2000 2 . 772E + 00 4 . 656E-03 2 . 777E+00 4.521E-02 9.596E-04 0.0 -0.126 0.137 0.136

0.2500 2 . 509E+00 4 . 987E-03 2.514E+00 6 . 420E-02 1 . 1 34E-03 0.0 -0.123 0.133 0.132

0.3000 2 . 337E+00 5.350E-03 2 . 342E+00 8 . 485E-02 1 .301E-03 0.0 -0 . 1 20 0.130 0.129 0.3500 2.21 8E+00 5 . 739E-03 2 . 223E+00 1 . 068E-01 1 . 462E-0 3 0.0 -0.118 0.128 0.127

0.4000 2.131 E+00 S.152E-03 2.1 38E+00 1 . 297E-0

1

1 .621E-03 0.0 -0.116 0.126 0.124

0.4500 2 . 067E+00 6.589E-03 2 . 074E+00 1 . 535E-0

1

1 . 777E-0 3 0.0 -0.115 0.124 0.123

0.5000 2.01 8E+00 7 . 047E-03 2 . 025E+00 1 .779E-01 1 . 932E-03 8 . 567E-03 -0.094 0.121 0.120 0.5500 1 . 978E+00 7 . 523E-0 3 1 . 985E+00 2.029E-01 2.087E-03 2 . 960E-02 -0.088 0.118 0.115

0.6000 1 . 946E+00 8.016E-03 1 . 954E+00 2 . 283E-0

1

2 . 242E-03 5 . 348E-02 -0.083 0.114 0.111 0.7000 1 . 899E+00 9.046E-03 1 . 908E+00 2.801E-01 2 . 553E-03 1 .074E-01 -0.074 0.107 0.102

0.8000 1 . 867E + 0 0 1 .01 3E-02 1 . 877E+00 3.330E-01 2.867E-03 1 . 666E-0

1

-0 .066 0.101 0.095

0 . 9000 1 . 845E+00 1 . 126E-02 1 . 857E+00 3.866E-01 3. 185E-03 2.287E-01 -0.061 0.096 0.089

1 .0000 1 .830E+00 1 . 244E-02 1 . 842E+00 4 . 406E-0

1

3 . 508E-0 3 2. 922E-01 -0.056 0.091 0.083

1 .2500 1 .809E+00 1 . 555E-02 1 . 825E+00 5.771E-01 4. 332E-03 4 . 51 0E-01 -0.047 0.082 0.072

1 .5000 1 . 80 2E+0 0 1 . 88SE-02 1 .821 E+00 7. 143E-01 5. 184E-03 6.045E-01 -0.041 0.074 0.063

1 .7500 1 .801 E + 00 2.239E-02 1 .823E+00 8.516E-01 6.061E-03 7 . 4 98E-0

1

-0.037 0.059 V . 057 2.0000 1 . 80 4E+0 0 2 . 605E-02 1 .830E+00 9 . 885E-0

1

6 . 960E-03 8.863E-01 -0.034 0.064 0.052

2.5000 1 .814E+00 3 . 373E-02 1 . 847E+00 1 . 260E+00 8.81 5E-03 1 . 1 34E+00 -0.030 0.057 0.044

3.0000 1 . 826E+00 4. 133E-02 1 .868E+00 1 . 530E+00 1 . 073E-02 1 . 353E+00 -0.027 0.052 0.039

3.5000 1 . 838E+00 5 . 025E-02 1 . 888E+00 1 . 796E+00 1 .270E-02 1 . 548E+00 -0.026 0.048 0.035 4.0000 1 . 850E+00 5.896E-02 1 . 909E+00 2 . 059E+00 1 .471E-02 1 . 723E+0 0 -0.024 0.045 0.033 4.5000 1 .861 E + 00 6 .790E-02 1 . 929E+00 2 . 320E+00 1 . 674E-02 1 . 882E+0 0 -0.023 0.042 0.030

5.0000 1 . 872E+00 7 . 706E-02 1 . 949E+00 2 . 578E+00 1 .880E-02 2 . 028E+0 0 -0.022 0.040 0.029

5.5000 1 . 882E+00 8.641E-02 1 . 968E+00 2.833E+00 2 . 089E-02 2.1 62E+00 -0.022 0.039 0 .027 6.0000 1 .891 E + 00 9.593E-02 1 . 987E+00 3.086E+00 2 . 299E-02 2 . 286 E+00 -0.021 0.037 0.026 7.0000 1 . 908E+00 1 . 1 54E-0

1

2 . 023E+00 3 . 584E+00 2.723E-02 2 . 51 OE+OO -0.020 0.035 0.024 3.0000 1 . 923E+00 1 .354E-01 2. 058E+00 4 . 074E+00 3. 150E-02 2 . 708E+00 -0.019 0.033 0.023

9.0000 1 . 936E+00 1 .559E-01 2 . 0 92E+00 4 . 556E+00 3 . 580E-02 2 . 835E+00 -0.018 0.031 0.022

10.0000 1 . 948E + 00 1 .767E-01 2. 124E+00 5.031 E+00 4.01 0E-02 3 . 046E + 00 -0.018 0.030 0.021 12.5000 1 . 973E+00 2.301E-01 2.203E+00 6 . 186E+00 5.085E-02 3 . 395E+00 -0.016 0 .027 0.019

15.0000 1 . 993E+00 2.850E-01 2 . 278E+00 7 . 302E+00 6 . 152E-02 3 . 687E+00 -0.014 0 .025 0.017 17.5000 2 . 0 1 0 E + 0 0 3.41 IE-01 2.351 E+00 8 . 382E+00 7 . 204E-02 3 . 940E+00 -0.013 0.023 0.0)6 20.0000 2 . 025E+00 3.982E-01 2 . 423E+00 9 . 429E+00 8 . 238E-02 4. 1 64E+00 -0.012 0 .022 0.014 25.0000 2 . 048E + 00 5.143E-01 2 . 562E+00 1 . 144E+01 1 . 025E-01 4 . 548E+00 -0.010 0 . 020 0.012

30.0000 2 . 067E + 00 6 .324E-01 2.699E+00 1 . 334E+0

1

1 .217E-01 4 .871 E+00 -0.008 0.018 0.011 35.0000 2 . 082E+00 7 . 520E-0

1

2 . 834E+00 1 .514E+01 1 .400E-01 5 . 1 49E+00 -0.006 0.016 0.009 40.0000 2 . 0 95E+0 0 8.729E-01 2. 968E+00 1 . 687E+0

1

1 . 575E-0

1

5 . 395E+00 -0.005 0.015 0.003 45.0000 2 . 1 06E+00 9. 949E-01 3.101E+00 1 . 852E+0

1

1 .742E-01 5.615E+00 -0 .004 0.014 0.007 50.0000 2.11 6E+00 1 . 1 18E+00 3 . 233E+00 2.01 0E+01 1 . 901 E-01 5.81 4E+00 -0.004 0.013 0.006 55.0000 2 . 1 25E+00 1 .241 E+00 3 . 366E+00 2.161 E+01 2.053E-01 5. 995E+00 -0.003 0.012 0.006 60.0000 2. 1 33E+00 1 . 365E+00 3 . 498E+00 2 . 307E+0

1

2.1 98E-01 6 . 1 61 E+00 -0.003 0.012 0.005 70.0000 2. 146E+00 1 . 6 1 5E+00 3.761 E+00 2 . 582E+0

1

2.470E-01 6 . 459E+00 -0.002 0.011 0 .004 80.0000 2.1 58E+00 1 . 86 6E+0 0 4 . 025E+00 2 . 839E+0

1

2.720E-01 6 . 7 1 8 E + 0 0 -0.002 0.010 0.004

90.0000 2. 169E+00 2.11 9E+00 4 . 288E+00 3.080E+01 2.950E-01 6 . 948E+00 -0.001 0.009 0.003

100.0000 2. 178E+00 2 . 373E+00 4.551 E+00 3. 306E+01 3.164E-01 7.155E+00 -0.001 0.008 0.003

1 25.0000 2.1 97E+00 3.01 3E+00 5.21 0E+00 3.81 9E+01 3.633E-01 7 . 595E+00 -0.001 0.007 0.002

150.0000 2.21 3E+00 3 . 657E+00 5 . 870 E+00 4. 271 E+01 4.030E-01 7. 955E + 00 -0.001 0.007 0.002

175.0000 2 . 226 E+0 0 4 . 304E+00 6 . 530E+00 4 . 675E+0

1

4.371E-01 8.261 E+00 -0.000 0.006 0.001 200.0000 2 . 238E+00 4 . 954E + 0 0 7. 1 91 E+00 5.040E+01 4.668E-01 8 . 526E + 00 -0.000 0.006 0.001 250.0000 2 . 257E+00 6 . 259E+00 8.51 5E+00 5 . 678E+0

1

5.160E-01 8.971 E+00 -0 .000 0.005 0.001 300.0000 2 . 272E+0 0 7 . 570E+00 9 . 842E+00 6 . 223E+0

1

5.555E-01 9 . 334E + 00 -0.000 0.005 0.001 350.0000 2 . 285E+00 8.886E+00 1 .117E+01 6.700E+01 5.880E-01 9.641 E+00 -0.000 0.004 0.001 400.0000 2 . 296E+00 1 . 020E+0

1

1 .250E+01 7. 123E+01 6 . 1 53E-01 9 . 908E+00 -0.000 0.004 0.001 450.0000 2 . 306E+00 1 . 1 53E+01 1 . 383E+0

1

7.503E+01 6 . 386E-01 1 .014E+01 -0.000 0.004 0.000 500.0000 2.31 5E+00 1 . 285E+0

1

1 .516E+01 7 . 848E+0

1

6.588E-01 1 . 0 35E+0

1

-0.000 0.004 0 .000 550.0000 2 . 323E+00 1 .417E+01 1 . 650E+0

1

8.164E+01 6 . 765E-0

1

1 . 054E+0

1

-0.000 0.004 0.000 600.0000 2. 331 E+00 1 . 550E+0

1

1 . 783E+0

1

8 . 455E+0

1

6 . 921 E-01 1 . 072E+0

1

-0.000 0.003 0.000 700.0000 2 . 344E+00 1 .816E+01 2.050E+01 8 . 978E+01 7. 187E-01 1 . 103E+01 -0.000 0.003 0 .000 800.0000 2 . 355E+00 2 . 082E+0

1

2.317E+01 9 . 437E+0

1

7.404E-01 1 . 1 29E+01 -0.000 0.003 0 .000 900.0000 2 . 365E+00 2 . 348E+0

1

2 . 585E+0

1

9 . S45E+0

1

7 . 585E-01 1 . 1 53E+01 - 0.000 0.003 0.000 1000.0000 2 . 374E+00 2.615E+01 2 . 852E+0

1

1 .021 E+02 7 . 739E-0

1

1 . 1 74E+01 - 0.000 0.003 0.000

131
ELECTRONS IN NYLON, TYPE 6 AND TYPE 6/6

I = 63.9 eV DENSITY =1.1 40E+0Ci g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log )/d(logI

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cra 2/g MeV cm 2/g MeV cra 2 /g g/cm 2 0.0100 2 . 298E+01 3. 164E-03 2 . 298E+0

1

2.458E-04 7.558E-05 0.0 -0.193 0.219 0.218

0.0125 1 . 930E+01 3. 178E-03 1 . 930E+01 3.651E-04 9 . 072E-05 0.0 -0.185 0.209 0.208

0.0150 1 . 673E+0

1

3. 187E-03 1 . 674E+0

1

5.046E-04 1 . 052E-04 0 .

0

-0.179 0.201 0.201 0.0175 1 . 483E+0

1

3.1 94E-03 1 . 484E+0

1

6 .636E-04 1 . 1 92E-04 0.0 -0.174 0.195 0.195

0.0200 1 . 337E+0

1

3.1 99E-03 1 . 337E+0

1

8.414E-04 1 .327E-04 0.0 -0.170 0.191 0.190

0.0250 1 . 125E+01 3.208E-03 1 . 1 25E+01 1 .251 E-03 1 .586E-04 0.0 -0.164 0.183 0.182

0.0300 9 . 778E+00 3.218E-03 9.781 E+00 1 . 729E-03 1 .834E-04 0.0 -0.160 0.177 0.177

0.0350 8 . 6 98E+00 3.228E-03 8.701 E+00 2 . 272E-03 2.072E-04 0.0 -0.156 0.172 0.172

0.0400 7.869E+00 3 . 239E-03 7 . 872E+00 2.877E-03 2 . 302E-04 0.0 -0.153 0.169 0.168

0 .0450 7.21 1E+00 3.252E-03 7.21 4E+00 3.542E-03 2.526E-04 0.0 -0.150 0.165 0.165

0.0500 6 . 676E+00 3.265E-03 6 . 679E+00 4.263E-03 2.743E-04 0 .

0

-0.148 0.163 0.162

0.0550 6 . 232E+00 3.279E-03 6 . 235E+00 5.038E-03 2. 955E-04 0.0 -0.146 0.160 0.160

0.0600 5 . 857E+0 0 3 . 295E-03 5 . 86 0 E+0 0 5.866E-03 3.162E-04 0.0 -0.144 0.158 0.158

0.0700 5.259E+00 3.327E-03 5 . 262E+00 7.670E-03 3.564E-04 0.0 -0.141 0.154 0.154

0.0800 4 .803E+00 3.363E-03 4 . 806E+00 9 . 662E-03 3.951 E-04 0.0 -0.139 0.151 0.151 0.0900 4 . 443E+00 3.401 E-03 4 . 446E+00 1 . 183E-02 4.326E-04 0.0 -0.137 0.149 0.149

0.1000 4 . 1 52E+00 3.441 E-03 4.155E+00 1 . 41 6E-02 4 . 690E-04 0.0 -0.135 0.147 0.146

0.1250 3.621E+00 3.551E-03 3 . 625E+00 2 . 063E-02 5.561 E-04 0.0 -0.131 0.142 0.142

0.1500 3.263E+00 3.669E-03 3 . 266E+00 2.791 E-02 6 . 388E-04 0 .

0

-0.128 0.139 0.139

0.1750 3 . 006E+00 3.796E-03 3 . 009E+00 3.590E-02 7.179E-04 0.0 -0.126 0.136 0.136 0.2000 2.81 3E+00 3. 930E-03 2.81 7E+00 4 . 450 E-0 2 7.943E-04 0.0 -0.124 0.134 0.133

0.2500 2 . 544E + 0 0 4.213E-03 2.549E+00 6 . 322E-02 9 . 406E-04 0.0 -0.121 0.130 0.130 0.3000 2.369E+00 4.532E-03 2. 374E+00 8 . 359E-02 1 .081E-03 0.0 -0.118 0.128 0.127

0.3500 2 . 247E + 00 4.868E-03 2 . 252E+00 1 . 052E-0

1

1 .217E-03 0.0 -0.106 0.125 0.124

0.4000 2 . 1 56E+00 5 . 226E-03 2.161 E+00 1 . 279E-0

1

1 .351 E-03 3. 157E-02 -0.087 0.119 0.117

0.4500 2 . 086E+00 5.604E-03 2 . 0 92E+00 1 .515E-01 1 . 484E-03 6 . 655E-02 -0.080 0.114 0.111 0.5000 2.032E+00 5. 999E-03 2 . 0 38E+00 1 . 757E-01 1 .617E-03 1 . 0 32E-0

1

-0.075 0.109 0.105

0.5500 1 . 990E+00 6.41 0E-03 1 . 996E+00 2.005E-01 1 . 750E-03 1 .409E-01 -0.070 0.104 0.100 0.6000 1 . 956E+00 6 . 8 36E-0 3 1 . 963E+00 2.258E-01 1 . 883E-0 3 1 . 793E-0

1

-0.066 0.100 0.095

0.7000 1 . 906E+00 7 . 726E-03 1 . 91 4E+00 2.774E-01 2.151 E-03 2.572E-01 -0.060 0.093 0.037

0.8000 1 . 872E+00 8.661 E-03 1 .881 E+00 3.301E-01 2.422E-03 3.350E-01 -0.055 0 . 087 0.080

0 . 9000 1 . 849E+00 9.639E-03 1 . 859E+00 3.836E-01 2.696E-03 4.119E-01 -0.051 0.083 0.075

1 .0000 1 . 832E+00 1 .066E-02 1 . 843E+00 4.377E-01 2.975E-03 4 . 872E-01 -0.048 0.078 0.070

1 .2500 1 .809E+00 1 . 335E-02 1 . 823E+00 5 . 742E-0

1

3 . 689E-03 6 .664E-01 -0.042 0.070 0.061

1 .5000 1 .801 E+00 1 . 623E-02 1 .81 7E+00 7. 1 1 6E-01 4 . 428E-03 8 . 31 9E-01 -0.038 0 .064 0.054

1 .7500 1 . 799E+00 1 . 927E-02 1 .81 9E+00 8 . 492E-0

1

5.190E-03 9.843E-01 -0.035 0.060 0.049

2.0000 1 -802E+00 2 . 244E-02 1 . 824E+00 9.865E-01 5 . 972E-03 1 . 1 25E+00 -0.033 0.056 0.046

2.5000 1 .81 1 E+00 2.910E-02 1 . 840E+00 1 . 259E+00 7.587E-03 1 . 375E+00 -0.030 0.051 0.040

3.0000 1 . 823E+0 0 3.612E-02 1 . 85 9E+00 1 . 530E+00 9.258E-03 1 . 5 94E+00 -0.028 0.047 0.036 3.5000 1 .836E+00 4.343E-02 1 . 87 9E+00 1 . 797E+00 1 .097E-02 1 . 786E+00 -0.027 0.044 0.034

4.0000 1 . 848E+00 5. 100E-02 1 .899E+00 2 . 062E+00 1 . 272E-02 1 . 959E+00 -0.025 0.041 0.032

4.5000 1 . 859E+00 5 . 873E-02 1 . 91 8E+00 2 . 324E+00 1 . 450E-02 2.11 5E+00 -0.024 0.039 0.030 5.0000 1 -870E+00 6 .674E-02 1 . 937E+00 2 . 583E+00 1 .631 E-02 2 . 258E+00 -0.023 0.038 0.029

5.5000 1 . 880E+00 7 . 488E-02 1 . 955E+00 2 . 840E+00 1 .81 3E-02 2 . 390E+00 -0.023 0.036 0.027 6.0000 1 .889E + 00 8.317E-02 1 . 973E+00 3 . 0 95E + 00 1 . 997E-02 2.51 3E+00 -0.022 0.035 0.026

7 . 0000 1 . 906E+00 1 . 002E-0

1

2 . 006E+00 3 . 597E+00 2. 370E-02 2 . 735E+00 -0 .020 0.033 0.025

3 .0000 1 .921 E+00 1 . 176E-01 2 . 0 39E+00 4.092E+00 2.746E-02 2. 932E+00 -0.019 0.031 0.023

9.0000 1 . 934E+00 1 . 354E-0

1

2 . 070E+00 4.579E+00 3. 125E-02 3.11 0E+00 -0.018 0.030 0.022

10.0000 1 . 946E+00 1 . 536E-01 2 . 0 9 9E+0 0 5 . 058E+00 3.505E-02 3 . 273E+00 -0.016 0.028 0.021

1 2 . 5000 1 . 970E+00 2.002E-01 2. 170E+00 6 . 229E+00 4.459E-02 3 . 630E+00 -0.014 0.026 0.018

15.0000 1 . 990E+00 2.482E-01 2 . 238E+00 7 . 363E+00 5.41 0E-02 3 . 933E + 00 -0.011 0.023 0.016 17.5000 2 . 0 06E+00 2.973E-01 2 . 303E+00 8 . 465E+00 6 . 352E-02 4 . 1 97E+00 -0.010 0.022 0.014 20.0000 2.01 9E+00 3.472E-01 2.366E+00 9 . 536E+00 7.283E-02 4.431 E+00 -0.008 0.020 0.013

25 . 0000 2.041 E+00 4 . 488E-01 2. 490E+00 1 . 1 60E+0

1

9 . 1 00E-02 4 . 834E+00 -0.006 0.018 0.010 30.0000 2 . 058E+00 5 . 523E-0

1

2.61 0E+00 1 .356E+01 1 . 085E-0

1

5.171 E+00 -0 .004 0.016 0.008 35.0000 2 . 072E+00 6.571E-01 2 . 729E+00 1 . 543E+0

1

1 .253E-01 5.461 E+00 -0.003 0.014 0.007

40.0000 2 . 085E+00 7.631E-01 2 . 848E+0 0 1 . 722E+0

1

1 . 4 1 5E-0

1

5.71 5E+00 -0 .003 0.013 0 .005 45.0000 2 . 095E+00 8.700E-01 2. 965E+00 1 . 894E+0

1

1 .570E-01 5. 942E+00 -0.002 0.012 0.005 50.0000 2. 1 04E+00 9.777E-01 3 . 082E+00 2.060E+01 1 .718E-01 6. 145E+00 -0.002 0.011 0.004 55.0000 2.11 3E+00 1 . 086E+00 3 . 1 99E+00 2.21 9E+01 1 .861 E-01 6 . 331 E+00 -0.002 0.010 0.004

60 . 0000 2 . 1 2 1 E+00 1 . 1 95E+00 3.316 E+00 2.372E+01 1 . 997E-01 6 . 500E+00 -0.001 0.010 0 .003 70.0000 2 . 1 34E+00 1 . 41 4E+00 3 . 548E+00 2.664E+01 2.255E-01 6 .802E+00 -0.001 0.009 0.003

30 .0000 2 . 1 45E+00 1 . 635E+00 3.781 E+00 2. 937E+01 2.493E-01 7 . 065E+00 -0.001 0 .008 0 .002

90 .0000 2 . 1 56 E+00 1 . 858E+00 4.01 3E+00 3.1 94E+01 2.713E-01 7 . 297E+00 -0.001 0.007 0.002

100.0000 2. 165E+00 2. 081 E+00 4 . 245E+00 3 . 436E+0

1

2.919E-01 7 . 506E+00 -0.001 0.007 0.002 125.0000 2. 134E+00 2 . 643E+00 4 . 827E+00 3. 988E+01 3.375E-01 7 . 948E+00 -0.000 0.006 0.001

1 50 .0000 2. 1 99E+00 3.209E+00 5 . 409E+00 4 . 477E+0

1

3.765E-01 8.31 0E+00 -0.000 0.005 0.001 175.0000 2.21 2E+00 3 . 779E+00 5.991 E+00 4.916E+01 4.102E-01 8.61 7E+00 -0.000 0.005 0.001

200 .0000 2 . 224E+00 4.351 E+00 6 . 57 4E+00 5.314E+01 4 . 398E-01 8 . 883E+00 -0 .000 0.005 0.001 250.0000 2 . 243E+00 5 . 500E+00 7 . 7 42E + 00 6.014E+01 4.893E-01 9 . 327E+00 -0 . 000 0 .004 0.001 300.0000 2 . 258E+00 6 . 655E+00 8 . 91 3E+00 6.615E+01 5.293E-01 9.691 E+00 -0 .000 0.004 0.000

350 .0000 2.271 E+00 7.814E+00 1 . 008E+0

1

7. 143E+01 5.624E-01 9 . 999E+00 -0.000 0.003 0.000

400 . 0000 2 . 282E+00 8. 976E+00 1 . 1 26E+0

1

7.612E+01 5.904E-01 1 . 027E+0

1

-0.000 0.003 0.000

450 .0000 2 . 292E+00 1 .014E+01 1 . 243E+0

1

8 . 034E+0

1

6.145E-01 1 . 050E+0

1

-0.000 0.003 0.000 500.0000 2 . 30 1 E+00 1 . 1 31E+01 1 .361 E+01 8.418E+01 6.354E-01 1 .071E+01 -0.000 0.003 0 .000 550.0000 2 . 309E+00 1 . 248E+0

1

1 . 478E+0

1

8.771E+01 6 . 538E-0

1

1 .090E+01 -0.000 0.003 0.000

600 .0000 2.31 6E+00 1 . 364E+01 1 . 596E+01 9.096E+01 6.701E-01 1 . 1 08E+0

1

-0.000 0.003 0.000 700.0000 2. 329E+00 1 . 599E+0

1

1 . 832E+0

1

9 . 680E+0

1

6 . 978E-01 1 . 1 38E+01 -0.000 0.003 0.000 300.0000 2 . 341 E+00 1 . 833E+0

1

2 . 067E+0

1

1 . 0 1 9E+02 7.206E-01 1 . 1 65E+0

1

-0.000 0.002 0 .000 900.0000 2 . 35 1 E+00 2 . 063E+0

1

2.303E+01 1 . 0 6 5E+0 2 7.397E-01 1 . 189E+01 -0.000 0.002 0.000 1000.0000 2 . 359E+00 2.303E+01 2 . 539E+0

1

1 . 1 07E+02 7.560E-01 1 .210E+01 -0.000 0.002 0.000

132
ELECTRONS IN PARAFFIN WAX

I = 55.9 eV DENSITY = 9 . 300E-0

1

g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. dClog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD COP.R

.

COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV c» z /g MeV cn 2 /g g/ca 2 0.0100 2.A6AE+01 2.826E-03 2. A6AE+01 2 . 285E-0

A

6 . 305E-05 0 .

0

-0.188 0.213 0.212

0.0125 2.067E+01 2.837E-03 2 . 067E+0

1

3 . 3 98 E-0 A 7.565E-05 0 .

0

-0.180 0.203 0.202

0.0150 1 .791 E+01 2.8AAE-03 1 . 7 9 1 E + 0

1

A. 701 E-OA 8 . 772E-05 0.0 -0.175 0.196 0.195 0.0175 1 .587E+01 2.8A9E-03 1 . 587E + 0

1

6 . 137E-0A 9 . 936E-05 0.0 -0.170 0.190 0.190 0.0200 1 . 429E+0

1

2.85AE-03 1 . A30E+01 7.8A9E-0A 1 . 106E-0A 0.0 -0.167 0.186 0.185

0.0250 1 .201E+01 2.863E-03 1 . 202E + 0

1

1 . 1 68E-03 1 . 323E-0

A

0.0 -0.161 0.178 0.178

0.0300 1 . OAAE+O

1

2.873E-03 1 . 0AAE + 01 1 . 6 1 6 E-0 3 1 . 531 E-OA 0 .

0

-0.156 0.173 0.172

0.0350 9 . 282E+00 2.88AE-03 9 . 285E+00 2. 125E-03 1 . 73 1 E-0

A

0.0 -0.153 0.168 0.168 0.0400 3 . 394E+00 2.895E-03 8 . 396E + 00 2.692E-03 1 . 92AE-0A 0 .

0

-0.150 0.165 0.165

0 .0450 7.689E+00 2. 908E-03 7 . 6 92E + 00 3.31 5E-03 2.1 12E-0A 0.0 -0 . 1 A7 0.162 0.161 0.0500 7.117E+00 2.921E-03 7.11 9E+00 3 . 991 E-03 2.295E-0A 0 .

0

-0. 1A5 0.159 0.159

0.0550 6.6A1E+00 2. 935E-03 6 . 64AE+00 A. 71 9E-03 2 . A73E-0A 0.0 -0 . 1 A3 0.157 0.157 0.0600 6 . 2A 1 E+00 2 . 950E-03 6.2A3E+00 5 . A 96 E-0 3 2.6A8E-0A 0.0 -0 . 1 A2 0.155 0.155

0.0700 5.601 E+00 2.981E-03 5 . 60AE+00 7.1 90 E-0 3 2 . 988E-0A 0.0 -0.139 0.151 0.151

0 .0800 5.11 3E+00 3.01 AE-03 5 . 1 1 6E+00 9 . 060E-03 3.31 5E-0A 0.0 -0.136 0.1 AS 0 . 1 A8 0.0900 A.729E+00 3.050E-03 A.732E+00 1 . 1 1 0E-02 3 . 632E-0A 0.0 -0.13A 0.1A6 0 . 1 46 0.1000 A . A 1 8 E+0 0 3.088E-03 A.A21E+00 1 . 328E-02 3 . 9A1 E-OA 0.0 -0.133 0 . 1 AA 0 . 1 AA 0.1250 3 . 85 1 E+00 3. 1 90E-03 3 . 8 55E + 0 0 1 . 936E-02 A . 680E-0A 0.0 -0.129 0 . 1 AO 0.139

0.1500 3.A69E+00 3.300E-03 3 . A72E+00 2 . 622E-02 5 . 382E-0A 0 .

0

-0.126 0.136 0.136 0.1750 3.1 95E+00 3.A18E-03 3 . 1 98E+00 3 . 373E-02 6 . 056E-0A 0 .0 -0 . 12A 0 . 1 3 A 0.133

0.2000 2. 989E+00 3.5A2E-03 2. 992E+00 A . 182E-02 6 . 707E-0A 0 .

0

-0.122 0.132 0.131

0 . 2500 2 . 703E+00 3.807E-03 2 . 7 06E + 00 5. 9A5E-02 7. 957E-0A 0 .

0

-0.119 0.128 0.127

0 .3000 2.51 5E+00 A.097E-03 2 . 520 E+0 0 7 .86AE-02 9 . 1 59E-0A 0.0 -0.116 0.126 0.125

0.3500 2.385E+00 A . A06E-03 2 . 390E+00 9 . 905E-02 1 . 033E-03 2.AA9E-03 -0.100 0.123 0.122

0.4000 2 . 287E+00 A . 736E-03 2 . 292E+00 1 . 20AE-0

1

1 . 1 A8E-0 3 3.A26E-02 -0.085 0.117 0.115

0 . A 50 0 2.21 3E+00 5.083E-03 2.21 8E+00 1 .426E-01 1 .263E-03 6 .'887E-02 -0.079 0.111 0.108

0.5000 2 . 1 56 E+00 5. AA6E-03 2.161 E+00 1 . 6 55E-0

1

1 . 377E-0 3 1 . 055E-0

1

-0.073 0.106 0.103

0.5500 2.111 E+00 5.82AE-03 2.1 1 6E+00 1 .889E-01 1 . A9 1 E-0 3 1 . A 3 A E-0

1

-0.069 0.102 0.098

0.6000 2 . 07AE+00 6.21 5E-03 2 . 08 1 E+0 0 2. 127E-01 1 . 6 06 E-0 3 1 . 823E-0

1

-0.065 0.098 0.093

0.7000 2.021 E+00 7.033E-03 2.028E+00 2.61 AE-01 1 . 8 38E-0 3 2 . 6 1 A E-0

1

-0 . 058 0.091 0.085

0.8000 1 . 98AE+00 7.893E-03 1 . 992E+00 3 . 11 2E-0

1

2.072E-03 3.A08E-01 -0.053 0 . 086 0.078

0.9000 1 . 959E+00 8.792E-03 1 . 968E+00 3.617E-01 2 . 3 1 0 E-0 3 A. 1 93E-01 -0 .0A9 0.081 0.073

1.0000 1 . 9 A 1 E + 00 9.728E-03 1 . 951 E+00 A . 1 28E-0

1

2 . 552E-0 3 A.962E-01 -0 .0A6 0.077 0.068

1 .2500 1 . 91 6E+00 1 .221E-02 1 . 928E+00 5.A18E-01 3. 172E-03 6 .79AE-01 -0.0A0 0.069 0.059

1 .5000 1 . 90 6 E+0 0 1 . A86E-02 1 . 921 E+00 6.71 8E-0

1

3.81 5E-03 8.A85E-01 -0.037 0.063 0.053

1.7500 1 . 90AE+00 1 .765E-02 1 . 922E+00 8.01 9E-01 A . A78E-03 1 . 004E+00 -0.03A 0.058 0 .048 2.0000 1 . 906E+00 2.057E-02 1 . 926E+00 9.31 9E-01 5. 159E-03 1 . 1 A7E+00 -0.032 0.055 O.OAA

2.5000 1 .91 5E+00 2.671 E-0 2 1 . 9A2E+00 1 . 1 90E+00 6 .569E-03 1 . A03E+00 -0.029 0 . 0A9 0.039

3.0000 1 . 927E+00 3.31 9E-02 1 . 960E+00 1 . AA7E+00 8 . 0 3 1 E-0 3 1 . 625E+00 -0.027 0 . 0A5 0.035

3.5000 1 . 9A0E+00 3.99AE-02 1 . 980E+00 1 .701 E+00 9.533E-03 1 .821 E+00 -0.026 0 .042 0.033

A. 0000 1 . 952E+00 A . 6 93E-02 1 . 999E+00 1 . 952E+00 1 . 1 07E-02 1 . 997E+00 -0.02A 0.0A0 0.031

A .5000 1 . 96 AE+00 5. A1 IE-02 2.01 8E+00 2.201 E+00 1 . 263E-02 2 . 1 56 E+00 -0.023 0.038 0 .029 5.0000 1 . 975E+00 6 . 1 A8E-02 2 . 036E+00 2.AA8E+00 1 . A22E-02 2 . 302E+00 -0.023 0.037 0.028

5.5000 1 . 985E+00 6 . 900E-02 2 . 0 5AE + 0 0 2 . 6 92E + 00 1 . 583E-02 2.A36E+00 -0.022 0 .035 0.027

6.0000 1 . 995E+00 7 . 667E-02 2.071 E+00 2. 93AE+00 1 . 7A5E-02 2.561 E+00 -0.021 0.03A 0.026

7.0000 2.01 2E+00 9.238E-02 2.1 0AE+00 3 . A 1 3E + 00 2 . 07AE-02 2 . 787E+00 -0.019 0.032 0 . 0 2 A 8.0000 2 . 027 E + 00 1 .085E-01 2.1 35E+00 3 . 885E + 00 2.A06E-02 2 . 988E+00 -0.018 0.030 0 .022 9.0000 2 . 0 AO E + 00 1 . 250 E-0

1

2 . 1 65E+00 A . 350E+00 2 . 7A2E-02 3.16 9E+00 -0.017 0.029 0.021 10.0000 2.052E+00 1 .41 9E-01 2.1 9AE+00 A.809E+00 3 . 080E-02 3 . 3 36 E + 0 0 -0.015 0.027 0.020

12.5000 2.077E+00 1 .851 E-0

1

2 . 262E+00 5 . 931 E+00 3 . 929E-02 3 . 6 99E+00 -0.012 0.025 0.017

15.0000 2 . 0 97 E + 00 2.296E-01 2 . 326 E + 0 0 7.021 E+00 A.779E-02 A . 008E+00 -0.010 0.022 0.015

17.5000 2.11 3E + 00 2.751 E-0

1

2 . 388E + 0 0 8 . 08 1 E+00 5 . 625E-02 A . 277E+00 -0.008 0.021 0.013

20 .0000 2 . 1 27E + 00 3.21 AE-01 2. AA8E+00 9.115E+00 6 . A62E-02 A. 51 5E+00 -0.007 0.019 0.012 25.0000 2. 1A9E+00 A. 157E-01 2.565E+00 1.111 E+01 8. 107E-02 A . 92AE+00 -0.005 0.016 0.009

30 .0000 2 . 1 67E + 00 5. 118E-01 2 . 678E+00 1 . 302E+0

1

9.701 E-02 5.265E+00 -0 .00A 0.015 0.007

35.0000 2. 181 E+00 6 .093E-01 2.791 E+00 1 . A85E+0

1

1 .12AE-01 5 . 558E+00 -0.003 0.013 0.006

AO . 0000 2.1 9AE + 00 7 . 078E-0

1

2. 902E+00 1 .660E+01 1 . 273E-0

1

5.815E+00 -0.002 0.012 0.005

A 5 . 0000 2.205 E+00 8 . 072E-0

1

3.01 2E+00 1 . 829E+0

1

1 . A 1 6 E-0

1

6 . 0 A2E+00 -0.002 0.011 0 . 00 A 50.0000 2.21 AE+00 9.07AE-01 3. 122E+00 1 . 992E+01 1 . 55AE-0

1

6 . 2A7E+00 -0.001 0.010 0 .004 55.0000 2 . 223 E + 0 0 1 . 008E+00 3.231 E+00 2 . 1 50 E + 0

1

1 . 686 E-0 1 6 . A33E+00 -0.001 0.009 0.003 60.0000 2.231 E+00 1 . 1 1 0E+00 3.3A1E+00 2 . 302E+0

1

1 .81 AE-01 6 . 60AE+00 -0.001 0.009 0.003

70.0000 2.2A5E+00 1 . 3 1 A E + 0 0 3 . 559E+00 2.592E+01 2 . 057 E-0

1

6 . 907E+00 -0.001 0 . 008 0.002 80.0000 2 . 257E+00 1.51 9E+00 3 . 776 E+0 0 2.865E+01 2.282E-01 7 . 170E+00 -0.001 0 .007 0.002

90.0000 2 . 268E+00 1 . 726E+00 3. 99AE+00 3.122E+01 2.A92E-01 7 . A03E+00 -0.001 0.007 0.002

1 00 .0000 2 . 277E+00 1 . 93AE+00 A. 21 1 E+00 3 . 36 6 E+0

1

2.689E-01 7.61 2E+00 -0.000 0 .006 0.001 125.0000 2.297E+00 2 . A58E + 0 0 A . 755E+00 3. 92AE + 01 3. 130E-01 8 . 0 5 AE + 00 -0.000 0.005 0.001

1 50 .0000 2 . 3 1 3E+00 2. 986E+00 5 . 299E+00 A . A22E + 0

1

3 . 5 1 0 E-0

1

8 . A 1 7 E + 0 0 -0.000 0.005 0.001 175.0000 2 . 327E+00 3.517E+00 5 . 8A3E+00 A .871 E+01 3 . 8A2E-0

1

8 . 72AE+00 -0.000 0.004 0.001 200.0000 2.339E+00 A . 050E+00 6 . 388E+00 5 . 280E+0

1

A.13AE-01 8 . 990E + 00 -0.000 0 .004 0.001 250.0000 2 . 358E+00 5 . 1 22E+00 7 . A80E+00 6 . 003E+0

1

A.629E-01 9 . A35E+00 -0.000 0 . 004 0.000

300 . 0000 2 . 37AE+00 6.1 99E+00 8 . 573E+0 0 6 . 627E+0

1

5.032E-01 9 . 7 98 E+0 0 -0.000 0.003 0.000

350 .0000 2 . 388 E + 0 0 7 . 280E+00 9 . 668E+00 7 . 1 76 E+0

1

5.368E-01 1 .01 1 E+01 -0.000 0.003 0.000

A00 .0000 2.AOCE+00 8 . 365E+00 1 . 07 6 E + 0

1

7 . 666E+0

1

5.65AE-01 1 . 0 37E+0

1

-0.000 0.003 0.000

A50 . 0000 2 . A 1 0 E + 0 0 9 . A52E+00 1 . 186E+01 8.108E+01 5. 900E-01 1 . 0 6 1 E + 0

1

-0.000 0.003 0.000 500.0000 2 . A 1 SE + 00 1 . 05AE+0

1

1 . 296 E + 0

1

8.51 1 E+0

1

6.116 E-0

1

1 . 082E+0

1

-0.000 0.003 0.000

550 .0000 2 . A28E+00 1 . 163E+01 1 . A06E+01 8 . 88 1 E+0

1

6 . 30 6 E-0

1

1 . 101 E+01 -0.000 0.002 0.000 600.0000 2 . A35E+00 1 . 272E+0

1

1 .51 6E+01 9.22AE+01 6 . A75E-01 1 . 1 1 8 E + 0

1

-0.000 0.002 0.000 700.0000 2.AASE+00 1 . A91 E+01 1 . 7 36 E + 0 1 9 . 8 AO E + 0

1

6.763E-01 1 . 1 A 9 E + 0

1

-0.000 0.002 0.000 800.0000 2 . A 6 1 E+00 1 .71 0E+01 1 . 956E + 01 1 . 038E+02 7.002E-01 1 . 1 76 E+0

1

-0.000 0.002 0.000 900.0000 2. A71 E+00 1 . 930E+01 2. 177E+01 1 . C87E + 0 2 7.202E-01 1 . 1 99E+01 -0.000 0.002 0 .000

1 000 .0000 2.A8CE+00 2. 1 A9E+01 2 . 397E+0

1

1 . 1 30E+02 7.37AE-01 1 . 22CE+0

1

-0.000 0.002 0.000
ELECTRONS IN PHOTOGRAPHIC EMULSION

I = 331 .0 eV DENSITY = 3.81 5E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS .EFF. d( logi )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 1 . 302E + 0

1

1 .310E-02 1 . 304E+0

1

4 . 664E-04 4. 991 E-04 0 .

0

-0 . 282 0 . 359 0 .338 0.0125 1 .1 14E+01 1 . 396E-02 1 .116E+01 6.745E-04 6 .250E-04 0 .

0

-0.266 0.332 0.315

0.0150 9 . 798E + 00 1 .463E-02 9.81 3E+00 9.140E-04 7.494E-04 0.0 -0.253 0.313 0.298

0.0175 8 . 782E+00 1 .51SE-02 8 . 797E+00 1 . 184E-03 8.722E-04 0.0 -0.244 0.298 0.285

0.0200 7. 984E+00 1 .565E-02 8 . 000E+00 1 . 482E-03 9. 934E-04 0 .

0

-0.237 0 . 236 0.274

0.0250 6 .81 0E+00 1 . 639E-02 6 . 827E+00 2. 1 61 E-03 1 . 231 E-03 0.0 -0.225 0.269 0.258

0.0300 5. 983E+00 1 .697E-02 6 . OOOE+OO 2. 945E-03 1 . 462E-0 3 0.0 -0.216 0.256 0.247

0.0350 5 . 366E + 00 1 .745E-02 5 . 383E+00 3.826E-03 1 . 687E-03 0.0 -0.210 0.246 0.238

0 .0400 4 . 887E+00 1 . 786E-02 4. 905E+00 4.801 E-03 1 . 906E-03 0.0 -0.204 0.238 0.231

0 .0450 4 . 504E+00 1 . 822E-02 4 . 522E+00 5.863E-03 2 . 1 21 E-03 0.0 -0.200 0.231 0.225

0.0500 4.1 90E+00 1 .354E-02 4 . 209E+00 7.01 IE-03 2.330E-03 0.0 -0.196 0.225 0 . 220 0.0550 3. 92SE+00 1 .384E-02 3 . 947E+00 8.238E-03 2 . 536E-0 3 0.0 -0.192 0.221 0.215

0.0600 3.706E+00 1 . 91 0E-02 3.725E+00 9.543E-03 2.737E-03 0 . 0 -0.189 0.216 0.211 0.0700 3.349E+00 1 . 959E-02 3.369E+00 1 . 237E-02 3 . 1 28E-03 0.0 -0 . 134 0.209 0.205

0.0800 3.075E+00 2.003E-02 3.095E+00 1 . 547E-02 3.506E-03 0.0 -0.180 0.204 0.200 0.0900 2 . 857E+00 2 . 044E-02 2 . 878E+00 1 . 883E-02 3.870 E-0 3 0.0 -0.176 0.199 0.195

0.1000 2 . 680E+00 2.081E-02 2.701 E+00 2 . 242E-02 4.224E-03 0.0 -0.173 0.195 0.191 0.1250 2 . 356E+00 2.16 9E-02 2 . 378E+00 3.232E-02 5.064E-03 0.0 -0.167 0.187 0.184

0.1500 2.1 36E+00 2.251 E-02 2. 159E+00 4.338E-02 5.350E-03 0.0 -0.162 0.181 0.173

0.1750 1 . 978E+00 2 . 329E-02 2.001 E+00 5.543E-02 6 . 592E-0 3 0 . 0 -0.159 0.176 0.173

0.2000 1 . 858E+00 2.405E-02 1 .383E+00 6 . 833E-02 7.294E-03 0 .

0

-0.155 0.172 0.170

0.2500 1 . 6 93E+00 2.560E-02 1 . 71 8E+00 9 . 622E-02 8 . 606E-03 0.0 -0.150 0.166 0.163

0.3000 1 . 585E+00 2.721 E-02 1 .612E+00 1 .263E-01 9.822E-03 0.0 -0.147 0.161 0.159

0.3500 1 . 50 9E+00 2 . 890E-02 1 . 537E+00 1 .581E-01 1 . 0 97E-02 1 . 408E-02 -0.127 0.155 0.152

0. 4000 1 . 453E+0 0 3.066E-02 1 . 484E+00 1 . 91 3E-01 1 . 206E-02 3 . 297E-02 -0.121 0.149 0.146 0.4500 1 . 4 1 2E+00 3.251 E-02 1 . 444E+00 2.254E-01 1 . 31 2E-02 5 . 225E-02 -0.117 0.144 0.141 0.5000 1 .381E+00 3.443E-02 1 .41 5E + 00 2.604E-01 1 .415E-02 7.178E-02 -0.113 0.140 0.136

0.5500 1 . 356E+00 3.642E-02 1 . 3 93E+00 2.960E-01 1 .516E-02 9. 146E-02 -0.109 0.136 0.132

0.6000 1 . 338E+00 3 . 846 E-0 2 1 . 37 6E+0 0 3.322E-01 1 .61 5E-02 1 . 1 12E-01 -0.106 0.133 0.128

0.7000 1 .31 1E+00 4.269E-02 1 . 354E+00 4.055E-01 1 .809E-02 1 .505E-01 -0.101 0.127 0.122

0.8000 1 . 295E+00 4.711 E-02 1 . 342E+00 4.797E-01 2 . OOOE-02 1 .895E-01 -0.097 0.122 0.116

0 . 9000 1 . 284E+00 5 . 1 68E-02 1 . 336E+00 5.544E-01 2. I87E-02 2.273E-01 -0.094 0.118 0.112

1 .0000 1 . 273E+00 5 . 640E-02 1 . 335E+00 6.293E-01 2.373E-02 2.652E-01 -0.090 0.114 0.108

1 .2500 1 . 274E+00 6 .874E-02 1 . 343E+00 3. 162E-01 2 . 833E-02 3.551E-01 -0.084 0.107 0.100

1 .5000 1 . 278E+00 8. 177E-02 1 . 360E+00 1 .001 E+00 3.289E-02 4.394E-01 -0.080 0.102 0.093

1 .7500 1 . 285E+00 9 . 534E-02 1 . 380E+00 1 . 1 84E+00 3.742E-02 5.186E-01 -0.076 0.097 0.088

2.0000 1 . 294E+00 1 .094E-01 1 . 403E+00 1 . 363E+00 4 . 1 93E-02 5.933E-01 -0.073 0.094 0 .084 2.5000 1 . 3 1 2E+00 1 .385E-01 1 . 45 1 E+00 I . 7 1 4E+00 5 . 089E-02 7.310E-01 -0.067 0.087 0.077

3.0000 1 .331E+00 1 .687E-01 1 . 4 99E + 00 2 . 053E+00 5.974E-02 8.560E-01 -0.063 0.083 0.072

3.5000 1 .347E+00 1 .999E-01 1 . 547E+00 2.381 E+00 6 .848E-02 9.707E-01 -0.060 0.079 0.067

A. 0000 1 . 363E+00 2.317E-01 1 . 595E+00 2 . 6 99E+00 7.708E-02 1 . 077E+00 -0.057 0.075 0.063

4 . 5000 1 . 377E+00 2.642E-01 1 .641 E+00 3 . 008E+00 8. 554E-02 1 . 175E + 00 -0.054 0.072 0.060 5.0000 1 . 390E+00 2. 973E-01 1 . 687E+00 3 .309E+00 9.3S5E-02 1 . 268E + 00 -0.052 0.070 0 .057 5.5000 1 .401E+00 3.309E-01 1 . 732E+00 3.601 E+00 1 . 020E-0

1

1 . 355E + 00 -0.050 0 .068 0.055

6.0000 1 . 4 1 2E+00 3.649E-01 1 . 777E+00 3 . 886 E+0 0 1 .100E-01 1 . 437E+00 -0.048 0.066 0.052

7.0000 1 .431E+00 4.340E-01 1 . 865E+00 4 . 436E+00 1 .256E-01 1 . 590E + 00 -0 .045 0.062 0.049 8.0000 1 . 448E+00 5.045E-01 1 . 952E+00 4 . 960E+00 1 .406E-01 1 . 729E+00 -0.043 0.059 0.045

9.0000 1 . 462E+00 5.760E-01 2.038E+00 5.461 E+00 1 .551E-01 1 . 8 56E + 0 0 -0.040 0.056 0.042

10.0000 1 . 475E+00 6 . 485E-0

1

2.1 23E+00 5. 942E+00 1 . 6 90E-0

1

1 . 975E+00 -0.038 0.054 0.040

12.5000 1 . 502E+00 3.331E-01 2 . 335E+00 7 . 064E+00 2.015E-01 2 . 240E + 0 0 -0.034 0.049 0.035

15.0000 1 . 523E+00 1 . 0 22E+00 2 . 545E+00 8 . 089E+00 2.31 2E-0

1

2 . 47 1 E + 0 0 -0.031 0.046 0.031 17.5000 1 . 540E+00 1 .21 3E+00 2 . 754E+00 9 . 033E+00 2.584E-01 2 . 675E+00 -0.028 0 .043 0.027

20.0000 1 . 555E+00 1 . 407E+00 2 . 963E+00 9. 909E+00 2.334E-01 2 . 853E+00 -0.026 0.040 0.025 25.0000 1 .579E+00 1 . 802E+00 3.381 E+00 1 .149E+01 3.277E-01 3. 178E+00 -0.023 0.036 0.021

30 .0000 1 . 598E+00 2 . 202E+00 3 . 800E+00 1 .2S8E+01 3 . 659E-0

1

3.451 E+00 -0.020 0.033 0.018 35.0000 1 . 6 1 3E+00 2. 606E+00 4 . 220E+00 1 .413E+01 3 . 993E-0

1

3. 589E+00 -0.013 0.031 0.016 40.0000 1 . 626E+00 3.01 5E+00 4.641 E+00 1 . 526E+0

1

4.286E-01 3 . 8 9 9E + 0 0 -0.017 0.029 0.014

45.0000 1 . 6 38E + 00 3 . 426E+00 5 . 064E+00 1 . 629E+0

1

4.547E-01 4 . 039E+00 -0.016 0.023 0.013

50.0000 1 . 648E+00 3.840E+00 5 . 488E+00 1 . 724E+0

1

4.781E-01 4.261 E+00 -0.015 0.027 0.012

55.0000 1 . 657E+00 4.256E+00 5.91 3E+00 1 .81 2E+01 4 . 992E-01 4.41 9E+00 -0.014 0.025 0.011 60.0000 1 . 665E+00 4 . 674E+00 6 . 338E+00 1 . 8 93E+0

1

5 . 133E-01 4 . 565E+00 -0.013 0.025 0.010 70.0000 1 . 678E+00 5.51 3E+00 7 . 1 92E+00 2.041 E+C

1

5.518E-01 4 . 828E+00 -0.011 0 .023 0.008 30.0000 1 . 6 90E+00 6 . 358E+00 8 . 048E+00 2. 173E+01 5.801E-01 5 . 059E+00 -0.010 0.022 0 .007 90.0000 1 . 700E+00 7 . 206E+00 8 . 906E+00 2.291 E+0

1

6 . 045E-0

1

5 . 266E+00 -0.009 0.021 0.007

100.0000 1 . 7 0 9E+0 0 3 . 056E+00 9.766E+00 2 . 398E+0

1

6 . 258E-0

1

5 . 453E+00 -0 .009 0.020 0.006 125.0000 1 . 728E+00 1 .01 9E+01 1 . 1 92E+01 2. 629E+0

1

6 . 633E-01 5 . 855E+00 -0 .007 0.018 0.005

150.0000 1 . 743E+00 1 . 234E+0

1

1 .409E+01 2.322E+01 7 .017E-01 6 . 1 90E+00 -0.006 0.017 0.004

175.0000 1 .755E+00 1 . 450E+0

1

1 . S25E+0

1

2. 987E+01 7.279E-01 6.47 6 E + 0 0 -0.005 0.016 0.003 200.0000 1 . 766E+00 1 .666E+01 1 . 843E+0

1

3.131 E+0

1

7.492E-C1 6 . 726E+00 -0.005 0.015 0.003

250 . 0000 1 . 783E+00 2. 1 00E+01 2 . 278E+0

1

3 . 375E+0

1

7 .820E-01 7 . 1 47E+00 -0.004 0.014 0.002

300.0900 1 . 797E+00 2 . 535E+0

1

2.714E+01 3 . 57 6 E+0

1

8.064E-01 7 . 495E+00 -0.003 0.014 0.002 350.0000 1 -308E+00 2. 970E+0I 3. 151E+01 3 . 747E+0

1

8 . 252E-0

1

7.791 E+00 -0.003 0.013 0.002

400.0000 1 . 8 1 8E+00 3.407E+01 3.589E+01 3 . 395E+0

1

3.404E-01 8 . 048E+00 -0.003 0.012 0.002

450.0000 1 . 827E+00 3 . 844E+0

1

4 . 027E+0

1

4 . 027E+0

1

8.528E-01 3 . 276E+00 -0.002 0.012 0.001 500.0000 1 .835E+00 4.281 E+O

1

4.465E+01 4 . 1 45E+01 S . 632E-01 8 . 48 1 E+00 -0.002 0.012 0.001 550.0000 1 . 842E + 0 0 4.719E+01 4.903E+01 4 . 25 1 E+0

1

8.720E-01 8.666 E+00 -0.002 0.011 0.001

6CO .0000 1 . 848E+00 5. 157E+01 5 . 342E+0

1

4. 349E+01 8.797E-01 8 . 836E+00 -0 .002 0.011 0.001 700.0000 1 . 85 9E+0 0 6.034E+01 6 . 220E+0

1

4.522E+01 3. 923E-01 9 . 1 38E + 0 0 -0.001 0.011 0.001 300.0000 1 . 36 9E+00 6.912E+01 7 .099E+01 4.673E+01 9 . 023E-01 9.401 E+00 -0.001 0.010 0.001 900.0000 1 . 878E+00 7.790E+01 7 . 978E+0

1

4.306E+01 5.104E-01 9 . 633E+00 -0.001 0.010 0.001 1000.0000 1 . 885E+00 8.669E+01 8 . 358E+0

1

4. 924E+01 9.171E-01 9.341 E+00 -0.001 0.010 0.001

134
ELECTRONS IN PLASTIC SCINTILLATOR ( VINYLTOLUENE BASED)

I = 6 A . 7 eV DENSITY = 1.032E+00 g/ci 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. dClog )/d( loq I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

NeV NeV c« 2/g NeV cn 2/g NeV ca 2 /g g/cm 2 0.0100 2.265E+01 2.965E-03 2 . 265E+0

1

2. A95E-0A 7.21 9E-05 0.0 -0.193 0.220 0.218 0.0125 1 . 902E+0

1

2. 975E-03 1 . 903E+01 3.70AE-0A 8 . 650E-05 0 .

0

-0.185 0.210 0.209 0.0150 1 -650E+01 2.982E-03 1 .650E+01 5. 120E-0A 1 . 002E-0

A

0.0 -0.179 0.202 0.201 0.0175 1 .A63E+01 2. 987E-03 1 . A63E+01 6.732E-0A 1 . 1 3AE-0A 0.0 -0.175 0.196 0.195 0.0200 1 .318E+01 2.992E-03 1 .318E+01 8.535E-0A 1 .262E-0A 0.0 -0.171 0.191 0.190

0 .0250 1 . 1 09E+01 3 . 000E-03 1 . 109E+01 1 .269E-03 1 . 507E-0

A

0.0 -0.165 0.183 0.183

0.0300 9.6A2E+00 3.01 0E-03 9 . 6A5E+00 1 .75AE-03 1 . 7A2E-0A 0 .

0

-0.160 0.177 0.177 0.0350 8 . 578E+00 3.021E-03 8.581 E+00 2.305E-03 1 . 967E-0A 0.0 -0.156 0.173 0.172

0 . 0A00 7.760E+00 3 . 032E-03 7.763E+00 2.918E-03 2. 186E-0A 0.0 -0.153 0 . 1 fc 9 0.169

0 . 0 A50 7.1 12E+00 3.0A5E-03 7.11 5E+00 3 . 592E-03 2.398E-0A 0.0 -0.151 0.166 0.165 0.0500 6 .58AE+00 3 . 058E-03 6 . 587E+00 A . 323E-03 2.60AE-0A 0.0 -0. 1A8 0.163 0.163

0 .0550 6 . 1 A6E+00 3 . 072E-03 6 . 1 50E+00 5. 109E-03 2.805E-0A 0 . 0 -0 . 1 A6 0.161 0.160 0.0600 5.777E+00 3.087E-03 5 . 780E + 0 0 5. 9A8E-03 3 . 002E-0A 0.0 -0 . 1 A5 0.158 0.158 0.0700 5.187E+00 3.11 9E-03 5. 1 90E+00 7.778E-03 3 . 38AE-0A 0.0 -0 . 1 A2 0.155 0.155 0.0800 A . 7 37E + 0 0 3. 153E-03 A .7AOE+00 9.797E-03 3.753E-0A 0.0 -0.139 0.152 0.152 0.0900 A . 382E+00 3. 189E-03 A . 38 6 E + 00 1 . 1 99E-02 A . 1 09E-OA 0.0 -0.137 0 . 1 A9 0.1A9 0.1000 A .095E + 00 3.228E-03 A . 099E+00 1 .A35E-02 A . A56E-0A 0.0 -0.135 0.1A7 0.1A7 0.1250 3.572E+00 3.333E-03 3 . 575E+00 2.091 E-02 5.286E-0A 0.0 -0.131 0 . 1 A3 0 . 1 A2 0.1500 3.21 9E + 00 3. AA6E-03 3 . 222E+00 2.830E-02 6 . 07AE-0A 0.0 -0.128 0.139 0.139 0.1750 2. 965E+00 3.566E-03 2.969E+00 3.639E-02 6 . 828E-0

A

0.0 -0.126 0.137 0.136 0.2000 2.775E+00 3.693E-03 2.779E+00 A. 51 1 E-02 7.557E-0A 0 . 0 -0 . 12A 0.1 3A 0. 13A

0 .2500 2.51 OE+OO 3. 966E-03 2.51 AE+00 6 -A09E-02 8. 953E-0A 0.0 -0.121 0.131 0.130 0.3000 2.337E+00 A.26AE-03 2 . 3A2E+00 8.A7AE-02 1 . 029E-03 0.0 -0.118 0.128 0.127

0 . 3500 2.21 7E+00 A.583E-03 2 . 222E + 0 0 1 . 067E-0

1

1 .160E-03 0.0 -0.117 0.126 0.125

0 . A000 2.129E+00 A . 923E-03 2 . 1 3 AE+00 1 . 297E-0

1

1 . 288E-0 3 1 . 600E-02 -0.092 0.121 0.120

0 . 4500 2.061 E+00 5.281 E-03 2 . 066E+00 1 . 535E-0

1

1 .A15E-03 A . AA7E-02 -0.086 0.116 0 . 1 1 A

0 .5000 2.009E+00 5 . 655E-03 2.01 AE+00 1 .780E-01 1 .5A1E-03 7.551 E-02 -0.080 0.112 0.108

0 . 5500 1 . 967E+00 6 . 0A5E-03 1 . 973E+00 2.031E-01 1 . 668E-03 1 .08AE-01 -0.075 0.107 0.103 0.6000 1 . 93AE+00 6 . AA8E-03 1 . 9A1E+00 2.287E-01 1 . 7 95E-0 3 1 . A26E-01 -0.071 0 . 1 OA 0.099

0.7000 1 . 886 E + 00 7.291E-03 1 . 893E+00 2.809E-01 2 . 0 5 1 E-0 3 2.1 3AE-01 -0 . 06 A 0.097 0.091 0.8000 1 .853E+00 8.178E-03 1 .861 E+00 3.3A2E-01 2.31 0E-03 2.85AE-01 -0.059 0.091 0.08A

0 . 9000 1 .830E + 00 9. 105E-03 1 . 83 9E+00 3.883E-01 2.572E-03 3.57AE-01 -0.055 0.086 0.079

1 .0000 1 .81 AE+00 1 . 007E-02 1 .82AE+00 A.A29E-01 2 . 839E-0 3 A . 28AE-01 -0 . 051 0.082 0 . 07 A

1 .2500 1 .792E+00 1 .262E-02 1 . 80 A E+OO 5 . 808E-0

1

3.521 E-03 5. 989E-01 -0 . 0A5 0.07A 0 . 06 A

1 .5000 1 . 78 A E+00 1 . 535E-02 1 . 7 9 9E+0 0 7.1 96E-01 A . 228E-03 7.575E-01 -0 .0A1 0.068 0.058

1 .7500 1 . 783E+00 1 . 823E-02 1 .801 E+00 8.586E-01 A. 956E-03 9.0A1E-01 -0.038 0.063 0.053 2.0000 1 .785E+00 2 . 1 2AE-02 1 . 807E+00 9. 972E-01 5 . 70AE-03 1 . 0A0E+00 -0.036 0.059 0.0A9 2.5000 1 .7 96E + 00 2 . 756E-02 1 . 823E+00 1 . 273E + 0 0 7.2A9E-03 1 . 28 2 E+0 0 -0.033 0.05A 0.0A3

3.0000 1 .808E+00 3. A23E-02 1 .8A2E+00 1 . 5A6E + 0 0 8.8A8E-03 1 . A93E+00 -0.031 0.050 0.039

3.5000 1 .821 E+00 A.117E-02 1 . 8 6 2E+0 0 1 .81 6E+00 1 .0A9E-02 1 . 680 E+00 -0.029 0.0A7 0.037

A . 0000 1 . 833E+00 A . 835E-02 1 . 8S2E+00 2 . 083E+00 1 . 2 1 7E-02 1 . 8 A8E+00 -0.028 O.OAA 0.03A

A .5000 1 . 8A5E+00 5.57AE-02 1 . 90 1 E+00 2 . 3A7E+00 1 . 387E-02 2 . 0 0 0 E+0 0 -0.027 0.0A2 0.033

5 .0000 1 . 856 E + 00 6.331E-02 1.91 9E+00 2.609E+00 1 .56 0 E-0 2 2 . 1 39E+00 -0.026 0 .0A1 0.031

5 . 5000 1 .866E+00 7 . 1 05E-02 1 . 937E+00 2 . 868E+00 1 . 735E-02 2 . 268E+00 -0.025 0.039 0.030 6.0000 1 . 875E + 00 7.892E-02 1 . 95AE+00 3.125E+00 1 .911 E-02 2 . 387E+00 -0 . 02A 0.038 0.029 7.0000 1 . 8 92E + 0 0 9 . 507E-02 1 . 988E+00 3 . 632E+00 2 . 268E-02 2.60AE+00 -0.022 0.036 0.027

8 . OOOO 1 . 907E+00 i . 1 16E-01 2.01 9E+00 A . 1 32E+00 2 . 6 2 9E-0 2 2 . 798E+00 -0.021 0 .03A 0.025

9.0000 1 . 921 E+00 1 .286E-01 2.0A9E+00 A . 623E+00 2. 993E-02 2 . 973E+00 -0.019 0.032 0.02A

10 .0000 1 . 932E+00 1 . A59E-01 2. 078E+00 5 . 1 08E+00 3.359E-02 3 . 1 3AE+O0 -0.018 0.031 0.023

12.5000 1 . 957E+00 1 . 902E-01 2 . 1 A7E+00 6 .291 E+00 A . 275E-02 3 . A87E+00 -0.015 0.028 0.020

15.0000 1 . 97 6 E+00 2.359E-01 2.21 2E+00 7 . A38E+00 5.1 91 E-02 3 . 788E+00 -0.012 0.025 0.017 17.5000 1 . 992E+00 2.826E-01 2 . 27AE+00 8 . 553E+00 6.099E-02 A . 05 1 E+00 -0.010 0.023 0.015 20.0000 2 . 005E + 0 0 3.301 E-Q

1

2 . 335E+00 9 . 637E+00 6 . 998E-02 A . 286E+00 -0.008 0.022 0.013 25.0000 2 . 027E+00 A.268E-01 2. A53E+00 1 . 173E+01 8 . 755E-02 A.689E+00 -0.006 0.019 0.011 30.0000 2.0A3E+00 S.25AE-01 2.569E+00 1 -372E+01 1 . OA5E-0

1

5 . 028E+00 -0 . OOA 0.017 0.009

35.0000 2 . 0 58E+00 6 . 252E-0

1

2 .683E+00 1 .562E+01 1 .209E-01 5.31 9E+00 -0.003 0.015 0 .007

AO .0000 2.069E+00 7.262E-01 2 . 7 96 E + 00 1 . 7 A5E + 0

1

1 .366E-01 5 . 57 A E+0 0 -0.003 0 .01 A 0.006

A5 . 0000 2.080 E + 00 8.281E-01 2. 908E+00 1 . 920 E + 0

1

1 . 5 1 7E-0

1

5.801 E+00 -0.002 0.012 0.005

50.0000 2 . 08 9 E+0 0 9.306E-01 3 . 020E+00 2.089E+01 1 .662E-01 6 . 005E+00 -0.002 0.012 0 .OOA 55.0000 2.097E+00 1 . 0 3AE + 0 0 3. 1 3 1 E + 00 2 . 25 1 E+0

1

1 .801E-01 6 . 1 91 E+00 -0.001 0.011 0 . 00 A 60.0000 2.10 5 E+00 1 . 1 38E+00 3 . 2A3E+00 2. A08E+01 1 . 935E-01 6 . 36 1 E+00 -0.001 0.010 0.003 70.0000 2.11 8E+00 1 . 3A7E+00 3 . A65E+00 2. 707E+01 2. 187E-01 6 .663E+00 -0.001 0.009 0.003 80.0000 2. 1 29E+00 1 . 557E+00 3 . 687E+00 2.986 E + 0

1

2.A21E-01 6 . 926E+00 -0.001 0.008 0.002

90.0000 2 . 1 39E+00 1 . 7 6 9E+00 3 . 909E+00 3 . 250E+0

1

2.638E-01 7. 159E+00 -0.001 0 .008 0.002 100.0000 2 . 1 A8E+00 1 . 982E+00 A . 1 30E+00 3. A99E+01 2.8A1E-01 7 . 367E+00 -0.001 0.007 0 .002 125.0000 2 . 1 67 E + 00 2.51 8E+00 A . 685E+00 A . 06 6 E + 0

1

3.292E-01 7.81 OE+OO -0.000 0.006 0.001 150.0000 2 . 1 82E+00 3 . 058E+00 5.2A1E+00 A . 57 1 E + 0 1 3.679E-01 8. 172E+00 -0.000 0.006 0.001 175.0000 2. 1 95E+00 3.601 E+00 5 . 7 97E + 0 0 5 . 02AE+01 A.015E-01 8.A79E+00 -0.000 0.005 0.001 200.0000 2.207E+00 A . 1 A7E + 00 6 . 353E+00 5 . A 36 E + 0 1 A.310E-01 8 . 7A5E+00 -0.000 0.005 0.001

250 .0000 2 . 225E+00 5.2A3E+00 7 . A68E+00 6 . 1 6 1 E+0

1

A.805E-01 9. 1 90 E + 0 0 -0.000 0 . OOA 0.001 300.0000 2 . 2A0 E+0 0 6 . 3A5E+00 8 . 58 5 E + 00 6 . 785E+0

1

5.207E-01 9 . 55AE+00 -0.000 0 . 0 0 A 0.000 350.0000 2 . 253E+00 7.A51E+00 9 . 70AE+00 7 . 332E+0

1

5.5A0E-01 9.861 E+00 -0.000 0 .OOA 0.000

A00 .0000 2 . 26 A E+00 8 . 560E+00 1 . 082E + 0

1

7 .820E+01 5.822E-01 1 .013E+01 -0.000 0 . CO 3 0.000

A50 .0000 2 . 27 AE + 0 0 9 . 67 1 E+00 1 . 1 95E+01 8 . 26 0 E + 0

1

6.065E-01 1 . 0 36 E + 0

1

-0 .000 0.003 0.000 500.0000 2.283E+00 1 . 073E+0

1

1 . 30 7 E + 0

1

8 . 6 6 0 E+0

1

6 .276E-01 1 . 0 57 E+0

1

-0.000 0.003 0.000 550.0000 2.291 E+00 1 . 1 90E+01 1 . A1 9E + 01 9 . 027E+0

1

6 . A62E-01 1 . 076E X 01 -0.000 0.003 0.000

600 .0000 2.298E+00 1 . 302E+01 1 . 531 E + O

1

9 . 366E + 0 1 6.627E-01 1 . 09AE+01 -0.000 0.003 0.000

700 .0000 2.311 E+00 1 .52SE+01 1 . 7 56 E + 0

1

9. 975E+C1 6 . 908E-01 1 . 125E+01 -0.000 0.003 0.000

800 .0000 2.322E+00 1 • 7 A 9E + 0

1

1 . 98 1 E + 0 1 1 . 051 E+02 7.1A0E-01 1 . 1 5 1 E+0

1

-0.000 0.002 0 .000 900.0000 2 . 332E+00 1 . 973E+01 2.206 E+0

1

1 . 0 9 9 E+0 2 7.33AE-01 1 . 175E+01 -0.000 0.002 0 .000

1 000 .0000 2-3A1 E+00 2.1 98E+01 2. A32E+01 1 . 1 A2E+02 7.500E-01 1 . 1 96E+01 -0.000 0.002 0 . 000

155
ELECTRONS IN POLYCARBONATE, "MAKROLON" , "LEXAN"

I = 73.1 eV DENSITY = 1 . 200E+00i g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d ( loc1 ; /d ( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(delta; LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2/g MeV cm 2/g g/cm 2 0.0100 2. 153E+01 3.240E-03 2. 153E+01 2 . 634E-04 8 . 29 1 E-0 5 0 .

0

-0.198 0.226 0.225 0.0125 1 .81 OE+OI 3.254E-03 1 .810E + 01 3.906E-04 9. 938E-05 0.0 -0.190 0.215 0.214

0.0150 1 .571E+01 3.263E-03 1 .571E+01 5.393E-04 1 . 151 E-04 0.0 -0.183 0.207 0.206 0.0175 1 . 393E+0

1

3.270E-03 1 . 394E+0

1

7.086E-04 1 . 303E-04 0.0 -0.178 0.201 0.200 0.0200 1 .256E+01 3 . 275E-03 1 . 257E+0

1

8. 973E-04 1 . 450E-04 0.0 -0.174 0.196 0.195

0.0250 1 . 058E+0

1

3.284E-03 1 . 058E+0

1

1 . 333E-03 1 . 731 E-04 0.0 -0.168 0.188 0.187

0.0300 9 . 202E+00 3.293E-03 9 . 205E+00 1 . 842E-0 3 2 . OOOE-04 0.0 -0.163 0.181 0.181 0.0350 8.1 90E+00 3. 304E-03 8.1 93E+00 2.41 9E-03 2 . 258E-04 0.0 -0.159 0.177 0.176

0.0400 7.41 2E+00 3.315E-03 7.41 6E+00 3.061E-03 2 . 507E-04 0.0 -0 . 1 56 0.173 0.172

0.0450 6 . 795E+00 3.327E-03 6 . 7 98E+00 3.766E-03 2 . 749E-04 0.0 -0.153 0.169 0.169

0.0500 6 . 293E+00 3.340E-03 6 . 296E+00 4.531E-03 2. 984E-04 0 . 0 -0.151 0.166 0.166 0.0550 5.876E+00 3.355E-03 5 . 87 9E+00 5.354E-03 3.213E-04 0.0 -0.149 0.164 0.164

0.0600 5 . 524E+00 3.370E-03 5 . 527E+00 6.231E-03 3 . 437E-04 0.0 -0.147 0.162 0.161 0.0700 4 . 962E+00 3 . 403E-03 4. 965E+00 8.1 44E-03 3.872E-04 0.0 -0.144 0.158 0.158

0.0800 4 . 533E+00 3 . 439E-03 4 . 536E+00 1 . 025E-02 4 . 290E-04 0.0 -0.142 0.155 0.154

0.0900 4.1 94E+00 3.477E-03 4.1 98E+00 1 . 255E-02 4.695E-04 0.0 -0.139 0.152 0.152

0.1000 3 . 920E+00 3.518E-03 3 . 924E + 00 1 . 502E-02 5 . 088E-04 0.0 -0.137 0.150 0.149

0.1250 3.421 E+00 3 . 629E-03 3 . 425E+00 2. 186E-02 6 . 028E-04 0.0 -0.134 0.145 0 .. 1 45 0.1500 3 . 084E+00 3 . 749E-03 3 . 088E + 00 2. 957E-02 6 . 91 9E-04 0.0 -0.131 0.142 0.141

0 .1750 2 . 842E + 00 3.877E-03 2 . 846 E+0 0 3.302E-02 7 . 772E-04 0.0 -0.128 0.139 0.133 0.2000 2 . 66 0 E + 0 0 4.01 3E-03 2 . 664E+00 4.71 IE-02 8.594E-04 0.0 -0.126 0.137 0.136 0.2500 2.407E+00 4 . 304E-03 2.412E+00 6.691E-02 1 .017E-03 0.0 -0.123 0.133 0.132

0 . 3000 2 . 242E+00 4.623E-03 2 . 247E+00 8 . 843E-02 1 . 168E-03 0.0 -0.120 0.130 0.129

0.3500 2. 128E+00 4 . 964E-03 2. 133E+00 1.11 3E-01 1 . 31 4E-03 0.0 -0.118 0.128 0.126 0.4000 2 . 044E+00 5.327E-03 2 . 050E+00 1 . 352E-0

1

1 . 458E-0 3 5 . 680E-03 -0.098 0.125 0.123

0.4500 1 . 980E+00 5.71 0E-03 1 . 986E+00 1 . 600E-0

1

1 . 600E-03 3.1 96E-02 -0 . 089 0.120 0.117

0.5000 1 . 930E+00 6.11 2E-03 1 . 936E+00 1 . 855E-0

1

1 . 74 1 E-0 3 6.091E-02 -0.083 0.115 0.112

0.5500 1 .391 E+00 6 . 529E-03 1 . 8 97E+0 0 2.116 E-0

1

1 . 883E-0 3 9. 181 E-02 -0.078 0.111 0.107

0 .6000 1 . 859E+00 6.961E-03 1 . 866 E+00 2 . 582E-0

1

2 . 025E-03 1 . 241 E-0

1

-0.074 0.107 0.102

0.7000 1 .81 3E+00 7 . 864E-03 1 .321 E+00 2. 925E-01 2.31 0E-03 1.91 3E-01 -0.067 0.100 0.094

0.8000 1 . 782E+00 8.313E-03 1 .791 E+00 3.479E-01 2 . 599E-03 2.602E-01 -0.061 0.094 0.087

0 . 9000 1 .761 E+00 9.806E-03 1 .771 E+00 4.041 E-0

I

2.891E-03 3 . 293E-0

1

-0.057 0.089 0.082

1 .0000 1 . 746E+00 1 .084E-02 1 . 757E+00 4.608E-01 3. 187E-03 3. 978E-01 -0.053 0.035 0.077

1 .2500 1 . 726E+00 1 . 357E-02 1 . 739E+00 6 . 039E-0

1

3. 946E-03 5.631E-01 -0.047 0.077 0.067

1 .5000 1 .71 9E+00 1 . 650E-02 1 . 735E+00 7.479E-01 4 . 730E-03 7. 177E-01 -0.042 0.070 0 .060

1 .7500 1 . 71 8E + 00 1 . 953E-02 1 .738E+00 8.919E-01 5.537E-03 8.61 IE-01 -0.039 0.065 0.055

2.0000 1 . 721 E+00 2 . 279E-02 1 . 744E+00 1 . 036E+00 6 . 365E-03 9.941 E-0

1

-0.037 0.062 0.050 2.5000 1 .731 E+00 2.955E-02 1 . 76 1 E+00 1 .321E+00 8.075E-03 1 . 233E+00 -0.033 0.056 0.045

3.0000 1 . 744E+00 3 . 667E-02 1 .781 E+00 1 . 603E+00 9 . 842E-03 1 . 441 E+00 -0.031 0.051 0.040

3.5000 1 . 757E+00 4 . 408E-02 1 . 80 1 E+00 1 . 883E+00 1 . 1 65E-02 1 . 626E+00 -0 .030 0.043 0.038

4.0000 1 . 7 6 9E+00 5.174E-02 1 .821 E+00 2.159E+00 1 . 350E-02 1 . 792E+00 -0.028 0.046 0.035

4.5000 1 . 780 E + 0 0 5. 962E-02 1 . 840E+00 2 . 432E+00 1 . 538E-02 1 . 942E+00 -0.027 0.044 0.033

5.0000 1 . 79 1 E+00 6.770E-02 1 . 859E+00 2 . 702E+00 1 . 728E-02 2 . 080E+00 -0.026 0.042 0.032

5.5000 1 .801 E+00 7.594E-02 1 . 377E+00 2. 970E+00 1 .92IE-02 2 . 207E+00 -0.025 0.040 0.031 6.0000 1 .81 1 E+00 3.434E-02 1 . 8 95E+00 3 . 235E+00 2. 1 15E-02 2 . 325E + 00 -0.024 0.039 0.029 7.0000 1 . 327E+00 1 .015E-01 1 . 929E+00 3 . 758E+00 2 . 506E-02 2 . 539E+00 -0.023 0.037 0.023 8.0000 1 . 842E+00 1 . 1 92E-01 1 . 96 1 E+00 4 . 272E+00 2 . 902E-02 2 . 730E+00 -0 . 021 0.035 0.026

9.0000 1 . 855E+00 1 . 373E-01 1 . 992E+00 4 . 778E+00 3 . 300E-02 2. 903E+00 -0.020 0.033 0.024 10.0000 1 . 367E+00 1 . 557E-01 2 . 022E+00 5 . 276E+00 3 . 6 99E-02 3.061 E+00 -0.019 0.032 0.023

12.5000 1 .891 E+00 2.029E-01 2.094E+00 6.491 E+00 4.699E-02 3 . 408E+0 0 -0.016 0.029 0.020

15.0000 1 . 91 0E+00 2.5' 5E-0

1

2. 162E+00 7 . 665E+00 5 . 6 93E-02 3 . 704E+00 -0.013 0.026 0.013

17.5000 1 . 926 E + 00 3.01 IE-01 2.227E+00 8 . 805E+00 6 . 677E-02 3. 963E+00 -0.011 0.024 0.016 20.0000 1 . 939E+00 3.516E-01 2.291 E+00 9.911 E+00 7 . 648E-02 4.1 93E+00 -0.009 0.023 0.014

25.0000 1 . 96 1 E + 00 4.544E-01 2.41 5E+00 1 . 204E+0

1

9.539E-02 4.590E+00 -0 .007 0.020 0.012

30.0000 1 . 978E+00 5.591 E— 01 2 . 537E+00 1 .406E+01 1 . 1 36E-0

1

4 . 924E+00 -0.005 0.018 0.009

35.0000 1 . 992E+00 6 . 652E-01 2 . 657E+00 1 . 5 98E + 0

1

1 .310E-01 5.21 2E+00 -0 .004 0.016 0.008 40.0000 2 . 003E+00 7.724E-01 2.776E+00 1 . 782E+0

1

1 . 477E-0

1

5 . 464E+00 -0.003 0.015 0.007 45.0000 2.01 4E+00 8 . 805E-0

1

2. S94E+00 1 .959E+01 1 . 637E-0

1

5 . 689E+00 -0.003 0.013 0 . 006 50.0000 2 . 023E+00 9.894E-01 3.01 2E+00 2.1 28E+01 1 . 789E-0

1

5 . 8 92E + 00 -0 .002 0.012 0 .005 55.0000 2 . 0 3 1 E + 0 0 1 . 0 99E+00 3 . 1 30E+00 2.291 E+O

1

1 . 936 E-0

1

6 . 077E+00 -0.002 0.012 0.005 60.0000 2 . 0 38 E+00 1 . 20 9E+0 0 3 . 247E+00 2 . 448E+0

1

2.076E-01 6 . 246 E + 00 -0.002 0.011 0.004 70.0000 2.051 E+00 1 .431 E+00 3 . 482E+00 2.745E+01 2.339E-01 6 . 547E+00 -0.001 0.010 0.003 80.0000 2 . 062E+00 1 . 654E+00 3.71 7E+00 3 . 023E+0

1

2.582E-01 6.80 9E+00 -0.001 0.009 0.003

90.0000 2 . 072E+00 1 . S79E+00 3.951 E+00 3 . 284E+0

1

2 . 807E-0

1

7.041 E+00 -0.001 0.008 0.002

100.0000 2.081 E+00 2. 105E+00 4 . 1 35E+00 3 . 530E+0

1

3.016 E-0

1

7 .249E+00 -0.001 0.008 0.002

1 25.0000 2.099E+00 2 . 673E+00 4 . 772E+00 4 . 089E+0

1

3.473E-01 7.691 E+00 -0.000 0.007 0.001

1 50 .0000 2.1 14E+00 3 . 245E+00 5.359E+00 4 . 583E+0

1

3.871E-01 8 . 053E+00 -0.000 0.006 0.001 175.0000 2. 127E+00 3 . 3 20 E+0 0 5 . 947E+00 5 . 025E+0

1

4.210 E-0

1

8 . 360E+00 -0.000 0.006 0.001 200.0000 2 . 1 38E+00 4 . 398E+00 6 . 536 E+0 0 5 . 426E+0

1

4.507E-01 8 . 625E+00 -0.000 0.005 0.001 250.0000 2 . 1 56 E+0 0 5 . 560E+00 7.71 5E+00 6 . 1 30E+01 5.001 E-0

1

9 . 070E+00 -0.000 0.005 0.001 300.0000 2. 171 E+00 6 . 726E+00 8 . 897E+00 6 . 733E+01 5 . 400E-01 9 . 434E+00 -0.000 0.004 0.001 350.0000 2. 183E+00 7 . 897E+00 1 . 008E+0

1

7 . 260E+0

1

5 . 729E-0

1

9.741 E+00 -0.000 0.004 0.000 400.0000 2 . 1 94E+00 9.071 E+00 1 . 127E+01 7 . 729E+0

1

6 . 006 E-0

1

1 .001E+01 -0.000 0.004 0.000 450.0000 2 . 204E+00 1 . 025E+0

1

1 . 24SE+0

1

8. 151E+01 6.244E-01 1 . 0 24E+0

1

-0 .000 0.003 0 . 000 500.0000 2.21 2E+00 1 .143E+01 1 . 364E+0

1

8 . 535E+01 6 . 450E-01 1 . 045E+0

1

-0.000 0.003 0 .000 550.0000 2 . 220 E+0 0 1 .261E+01 1 .483E+01 3.886E+01 6.631 E-0

1

1 . 064E+0

1

-0.000 0.003 0 .000 600.0000 2 . 227E+00 1 . 379E+01 1 .601E+01 9.21 1 E+01 6 . 7 9 1 E-0

1

1 . 082E+0

1

-0 .000 0.003 0 . 000 700.0000 2 . 239E + 00 1 .615E+01 1 .339E+01 9 . 793E+0

1

7.064 E-0

1

1.11 3E+01 -0.000 0 .003 0.000 800.0000 2 . 250E+00 1 . 352E+0

1

2 . 077E+0

1

1 .030E+02 7 . 288E-0

1

1 .139E+01 -0.000 0.003 0 . 000 900.0000 2 . 260E+00 2. 089E+01 2.315E+01 1 . 076E+02 7.475E-01 1 .163E+01 -0.000 0.003 0.000 1000.0000 2 . 263E+00 2.327E+01 2 . 554E+0

1

1 . 1 17E+02 7.634E-01 1 . 1 S4E+0

1

-0 .000 0.003 0.000
ELECTRONS IN POLYETHYLENE

I = 57.4 eV DENSITY = 9.400E-01 g/cs 3

ENERGY STOPPING POWER C3DA RADIATION DENS . EFF

.

dClog )/d(loqI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2 /g g/cra 2 0.0100 2.441 E+O

1

2. 837E-03 2 . 442E+0

1

2 . 308E-04 6 . 391 E-05 0.0 -0.189 0.214 0.213 0.0125 2.049E+01 2.847E-03 2.049E+01 3 . 430E-04 7.666E-05 0.0 -0.181 0.204 0.203

0.0150 1 . 775E+01 2.854E-03 1 . 776E+0

1

4 . 745E-04 8 .337E-05 0.0 -0.176 0.197 0.196 0.0175 1 . 573E+0

1

2.360E-03 1 . 573E+0

1

6 . 244E-04 1 . 007E-04 0.0 -0.171 0.191 0.191 0.0200 1 . 4 1 7 E + O

1

2 . 864E-03 1 . 41 7E+01 7.921E-04 1 .121E-04 0 . 0 -0.167 0.187 0.186 0.0250 1 . 191 E+O

1

2.873E-03 1 . 1 92E+01 1 .179E-03 1 . 340E-04 0.0 -0.161 0.179 0.179

0.0300 1 . 035E+0

1

2.383E-03 1 . 0 36E+0

1

1 . 630E-03 1 . 550E-04 0 .

0

-0 . 1 57 0.174 0.173

0.0350 9 . 206E+00 2 . 894E-03 9.209E+00 2.1 43E-03 1 . 752E-04 0 .0 -0.153 0.169 0.169 0.0400 8 . 325E+00 2. 905E-03 8 . 328E+00 2.715E-03 1 . 948E-04 0 .

0

-0.150 0.166 0.165

0.0450 7 . 627E+00 2. 918E-03 7 . 630E+00 3.343E-03 2. 138E-04 0 . 0 -0.148 0.162 0.162

0.0500 7 . 060E+00 2.931 E-03 7.063E+00 4.025E-03 2 . 323E-0

4

0.0 -0.146 0.160 0.160 0.0550 6 . 589E+00 2. 945E-03 6 . 592E+00 4.758E-03 2.503E-04 0.0 -0.144 0.157 0 . 1 57 O.OSOO 6.191 E+00 2 . 960 E-0 3 6 . 1 94E+00 5.541 E-03 2 . 680E-04 0.0 -0.142 0.155 0.155

0.0700 5 . 557E+00 2. 992E-03 5 . 560E+00 7.249E-03 3.023E-04 0.0 -0.139 0.152 0.152

0.0800 5 . 074E+00 3.025E-03 5 . 077E+00 9.1 34E-03 3.354E-04 0 .

0

-0.137 0.149 0.149

0.0900 4. 692E+00 3.061 E-03 4 . 696E+00 1 . 1 18E-02 3 . 675E-04 0 .

0

-0.135 0.147 0.146

0. 1000 4 . 384E+00 3.099E-03 4 . 387E+00 1 . 339E-02 3 . 987E-04 0.0 -0.133 0.144 0.144 0.1250 3.822E+00 3.201 E-03 3 . 825E+00 1 . 952E-02 4 . 733E-04 0 .

0

-0.129 0.140 0.140 0.1500 3 . 443E+00 3.312E-03 3 . 446 E + 0 0 2.642E-02 5.443E-04 0.0 -0.127 0.137 0.137

0.1750 3 . 1 7 1 E + O 0 3 . 429E-03 3. 174E+00 3 . 399E-02 6.124E-04 0 .

0

-0.124 0.134 0.134

0.2000 2. 967E+00 3.553E-03 2. 970E+00 4.21 5E-02 6 . 782E-04 0 .

0

-0.122 0.132 0.132

0.2500 2 . 683E+00 3 . 320E-0 3 2 . 687E+00 5. 991 E-02 8 . 045E-04 0.0 -0.119 0.129 0 . 1 23 0.3000 2 . 4 97E + 0 0 4.110 E-03 2.501 E+00 7 . 923E-02 9 . 258E-04 0.0 -0.116 0.126 0.125

0.3500 2 . 368E+00 4 . 420E-03 2 . 373E+00 9.979E-02 1 .044E-03 0.0 -0.109 0.124 0.123

0.4000 2 . 272E+00 4.750E-03 2 . 277E+00 1 .213E-01 1 . 1 60E-03 2 . 6 26 E-0 2 -0.087 0.118 0.116

0 . 4500 2.1 99E+00 5.098E-03 2 . 204E+00 1 .437E-01 1 . 276E-03 5 . 906E-02 -0.081 0.113 0.110 0.5000 2. 142E+00 5.462E-03 2. 147E+00 1 . 667E-0

1

1 . 391 E-03 9.409E-02 -0.075 0.108 0.104

0.5500 2 . 0 97E+0 0 5.841 E-03 2. 103E+00 1 . 902E-0

1

1 . 506 E-0 3 1 . 307E-0

1

-0.070 0.104 0.099

0.6000 2.061 E+00 6 . 233E-03 2.063E+00 2. 142E-01 1 . 622E-03 1 . 683E-0

1

-0.066 0.100 0.095

0.7000 2 . 008E+00 7 . 053E-03 2.01 6E+00 2.632E-01 1 . 356E-0 3 2.453E-01 -0.060 0.093 0.087

0.3000 1 . 972E+00 7. 91 5E-03 1 . 980E+00 3.133E-01 2.092E-03 3.231 E-01 -0.054 0.087 0.080

0 . 9000 1 . 947E+00 8.816E-03 1 . 956E+00 3.641E-01 2.332E-03 4.002E-01 -0.050 0.082 0.074

1.0000 1 . 930E+00 9.754E-03 1 . 940E+00 4. 155E-01 2.575E-03 4.759E-01 -0.047 0.078 0.069

1 .2500 1 . 905E+00 1 . 224E-02 1 . 91 7E+00 5 . 452E-0

1

3 . 200E-03 6 . 568E-0

1

-0.041 0.070 0.060

1.5000 1 .895E+00 1 . 490E-02 1 . 91 OE+OO 6 . 759E-0

1

3 . 848E-03 3.243E-01 -0.037 0.064 0.054

1 .7500 1 .393E+00 1 . 770E-02 1 .911 E+00 8.068E-01 4.516E-03 9.785E-01 -0.034 0.059 0.049

2.0000 1 . 3 95E+0 0 2 . 062E-02 1 . 91 6E+00 9 . 375E-0

1

5.203E-03 1 . 1 21 E+00 -0.032 0.055 0.045

2.5000 1 . 905E+00 2 . 673E-02 1 . 932E+00 1 . 1 97E+00 6 . 623E-03 1 . 375E+00 -0.029 0.050 0.039

3.0000 1 . 91 7E+00 3 . 327E-02 1 . 950E+00 1 . 455E+00 8.095E-03 1 . 596E+00 -0 .027 0.046 0.036 3.5000 1 . 930E+00 4 . 004E-02 1 . 970E+00 1 . 71 OE+OO 9 . 608E-03 1 .791 E+00 -0.026 0.043 0.033

4.0000 1 . 942E+00 4 . 704E-02 1 . 989E+00 1 . 963E+00 1.11 6E-02 1 . 966E+00 -0 .025 0.041 0.031 4.5000 1 . 954E+00 5.424E-02 2 . 008E+00 2.21 3E+00 1 . 273E-02 2. 1 24E+00 -0 . 024 0.039 0.029

5.0000 1 . 96 5E+00 6 . 1 62E-02 2 . 026 E+O 0 2.461 E+00 1 . 433E-02 2.269E+00 -0.023 0.037 0.023 5.5000 1 . 975E+00 6.916E-02 2 . 044E+00 2 . 706E+00 1 . 594E-02 2 . 402E+00 -0.022 0.036 0.027 6.0000 1 . 984E+00 7 . 684E-02 2.061 E+00 2. 950E+00 1 . 753E-02 2 . 527E+00 -0.021 0.035 0.026 7.0000 2 . 0 02E+0 0 9 . 259E-02 2.094E+00 3. 431 E+00 2. 089E-02 2.751 E+00 -0.020 0.032 0 .024 8.0000 2.017E+00 1 . 088E-0

1

2. 126E+00 3. 905E+00 2.424E-02 2 . 952E+00 -0.018 0.031 0.023

9.0000 2.030E+00 1 . 253E-01 2. 1 56E+00 4 . 372E+00 2 . 762E-02 3.1 32E+00 -0.017 0.029 0.021 10.0000 2 . 042E+00 1 . 422E-0

1

2. 184E+00 4 . 833E+00 3 . 1 02E-02 3 . 293E+00 -0.016 0.028 0 . 020 12.5000 2 . 067E+00 1 . 855E-0

1

2 . 253E+00 5. 960E+00 3. 956E-02 3 . 660E+00 -0.013 0.025 0.017

15.0000 2 . 087E+00 2.301E-01 2.31 7E+00 7 . 054E+00 4.811 E-02 3. 967E + 00 -0.010 0.023 0.015

17.5000 2 . 1 03E+00 2.757E-01 2 . 379E+00 8.11 9E+00 5.661 E-02 4 . 235E+0 0 -0.009 0.021 0.013

20 .0000 2.1 17E+00 3 . 220E-0

1

2.439E+00 9 . 1 57E+00 6 . 503E-02 4 . 473E+00 -0.007 0.019 0.012

25.0000 2.1 39E+00 4.166E-01 2 . 556E+00 1 . 1 1 6 E + O

1

8. 1 56 E-02 4 . 880E + 00 -0.005 0.017 0.009 30.0000 2.157E+00 5. 129E-01 2 . 6 70E+0 0 1 . 307E+0

1

9.759E-02 5 . 22 1 E+0 0 -0.004 0.015 0.008 35.0000 2. 1 71 E+00 6.105E-01 2 . 782E+00 1 .491 E+01 1 . 1 31 E-01 5.514E+00 -0.003 0.013 0.006 40.0000 2. 184E+00 7.092E-01 2 . 893E+00 1 . 667E+0

1

1 . 280E-01 5 . 770E + 00 -0.002 0.012 0.005 45.0000 2.1 95E+00 8 . 08SE-0

1

3 . 004E+00 1 . 837E+0

1

1 . 424E-0

1

5. 997E+00 -0.002 0.011 0.005 50.0000 2 . 204E+00 9. 092E-01 3.11 4E+00 2 . 00 0 E+O

1

1 . 562E-0

1

6 . 202E+00 -0.001 0.010 0.004 55.0000 2.21 3E+00 1 .01 OE+OO 3 . 223E+00 2.1 58E+01 1 .695E-01 6 . 338E+00 -0.001 0.010 0.003 60.0000 2.221 E+00 1.11 2E+00 3 . 333E + 0 0 2.310E+01 1 .824E-01 6 . 558E+00 -0.001 0.009 0.003 70.0000 2 . 235E+00 1 . 31 SE+OO 3.551 E+00 2. 601 E+01 2.067E-01 6.361 E+00 -0.001 0.008 0.002

80 .0000 2 . 247E+00 1 . 522E+00 3.769E+00 2.874E+01 2.293E-01 7. 125E+00 -0.001 0.007 0 .002 90.0000 2 . 257E+00 1 . 730E+00 3 . 987E+00 3.132E+01 2 . 504E-0

1

7 . 357E+00 -0.001 0 .007 0 .002 100.0000 2 . 267E+00 1 . 938E+00 4 . 205E+00 3 . 376E+0

1

2.701E-01 7 . 566E+00 -0.000 0.006 0.002 125.0000 2 . 287E+00 2.463E+00 4 . 749E+00 3 . 936E+0

1

3.142E-01 3.009E+00 -0.000 0.005 0.001 150.0000 2 . 303E+00 2. 991 E+00 5 . 294E+00 4 . 434E+0

1

3 . 523E-0

1

8.371 E+00 -0.000 0.005 0.001 175.0000 2 . 31 6E+00 3 . 523E + 00 5 .339E+00 4 . 883E+0

1

3.855E-01 8 . 678E+00 -0.000 0.004 0.001 200.0000 2. 328E+00 4 . 057E+00 6 . 3S5E+00 5 . 293E+0

1

4.148E-01 8. 944E+00 -0 . 000 0.004 0.001 250.0000 2 . 348E+00 5.131 E+00 7 . 479E+00 6 . 01 5E+01 4 . 642E-0

1

9 . 339E+00 -0.000 0.004 0.000 300.0000 2.364E+00 6.21 OE+OO 8 . 574E+00 6 . 639E+0

1

5.045E-01 9 . 753E+00 -0.000 0.003 0.000 350.0000 2 . 377E+00 7 . 294E+00 9.671 E+00 7.138E+01 5.381E-01 1 . 006E+0

1

-0.000 0.003 0.000 400.0000 2.339E+00 8 . 380E+00 1 . 077E+0

1

7 . 678E+0

1

5.667E-01 1 . 0 33E+0

1

-0.000 0.003 0.000 450.0000 2 . 3 9 9E+00 9.469E+00 1 . 187E+01 3. 120E+01 5.913E-01 1 . 056E+01 -0 .000 0.003 0.000 500.0000 2.409E+00 1 . C56E+0

1

1 . 297E+0

1

3 . 523E+0

1

6 . 1 28E-01 1 . 077E+0

1

-0.000 0.003 0.000 550.0000 2.417E+00 1 .165E+05 1 . 407E+0

1

S.893E+01 6.313E-01 1 . 0 96 E + O

1

-0 .000 0.002 0.000 600.0000 2 . 425E+00 1 . 275E+0

1

1 .517E+01 9. 235E+01 6 . 487E-0

1

1 .1 14E+01 -0.000 0.002 0.000 700.0000 2 . 438E+00 1 . 4 94E+0

1

1 . 738E+0

1

9.351 E+O

1

6.775E-01 1 . 1 44E+01 -0.000 0.002 0 .000 800.0000 2 . 450E+00 1 .713E+01 1 . 953E+01 1 .039E+02 7.012E-01 1 .171 E+O

1

-0 .000 0.002 0 . 000 900.0000 2 . 460E+00 1 . 933E+01 2. 179E+01 1 . 088E+02 7.212E-01 1 . 1 95E+01 - 0.000 0.002 0.000 1000.0000 2.469E+00 2. 1 53E+01 2 . 400E+0

1

1 . 1 31 E+02 7. 383E-01 1 .21 6E+01 -0 .000 0.002 0.000

137
ELECTRONS IN POLYETHYLENE TEREPTHALATE, "MYLAR

I = 78.7 eV DENSITY = 1 . 400E+001 g/cra 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log1 )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV ci» 2 /g MeV cm 2/g MeV cisVg g/cm 2

0.0100 2.095E+01 3.431E-03 2.095E+01 2.712E-04 9.01 3E-05 0.0 -0.201 0.230 0.228

0.0125 1 .762E+01 3.448E-03 1 .763E + 01 4.01 9E-04 1 .081 E-0 4 0.0 -0.192 0.219 0.213

0.0150 1 . 530E+0

1

3 . 459E-03 1 . 530E + 0

1

5.545E-04 1 . 252E-04 0.0 -0.136 0.211 0.210 0.0175 1 .353E+01 3 . 466E-03 1 . 358E + 0

1

7.283E-04 1 . 41 7E-04 0.0 -0.181 0.204 0.203

0.0200 1 . 225E+0

1

3.471E-03 1 . 225E+0

1

9.224E-04 1 . 577E-04 0.0 -0.177 0.199 0.198

0.0250 1 . 032E+0

1

3.481E-03 1 . 0 32E + 0

1

1 . 369E-03 1 . 882E-04 0.0 -0.170 0.190 0.190

0.0300 8. 978E+00 3. 490E-03 8. 982E+00 1 . 890E-03 2.174E-04 0.0 -0.165 0.184 0.183

0.0350 7 . 993E+00 3 . 500E-03 7. 997E+00 2.481 E-03 2 . 454E-04 0.0 -0.161 0.179 0.179

0.0400 7 . 236E+0 0 3.51 IE-03 7 . 239E+00 3.1 39E-03 2.724E-04 0.0 -0.158 0.175 0.174

0.0450 6 . 635E+00 3.524E-03 6 . 638E+00 3.862E-03 2. 986E-04 0.0 -0.155 0.171 0.171 0.0500 6 . 1 45E+00 3 . 537E-03 6 . 1 49E+00 4.645E-03 3 . 240E-04 0.0 -0.153 0.168 0.168

0.0550 5 . 739E+00 3.552E-03 5 . 742E+00 5.487E-03 3 . 48SE-04 0.0 -0.151 0.166 0.166

0 . 0600 5 . 396E+00 3.567E-03 5 . 399E+00 6 . 386 E-0 3 3.731 E-04 0.0 -0.149 0.164 0.163

0.0700 4.843E+00 3.601E-03 4.852E+00 3.344E-03 4 . 200E-04 0.0 -0.146 0.160 0.159

0.0800 4 . 430E+00 3.637E-03 4 . 433E+00 1 . Q50E-02 4 . 652E-04 0.0 -0.143 0.157 0.156 0.0900 4. 100E+00 3.677E-03 4. 103E+00 1 . 285E-02 5.039E-04 0.0 -0.141 0.154 0.153

0.1000 3 . 832E+00 3.71 9E-03 3.836E+00 1 . 537E-02 5.51 3E-04 0.0 -0.139 0.151 0.151 0.1250 3 . 345E+00 3 . 835E-03 3 . 349E+00 2 . 238E-02 6 . 527E-04 0.0 -0.135 0.147 0.146

0.1500 3.01 6E+00 3 . 960E-03 3 . 020E+00 3 . 026E-02 7 . 487E-04 0.0 -0.132 0.143 0.143

0.1750 2 . 780E+00 4.094E-03 2 . 784E+00 3 . 8 90 E-0 2 8 . 405E-04 0.0 -0.129 0.140 0.140

0.2000 2 . 60 3E + 0 0 4 . 235E-03 2. 607E+00 4.81 9E-02 9 . 290E-04 0.0 -0.127 0.138 0.137

0.2500 2.356E+00 4.540E-03 2.361 E+00 6 .841 E-02 1 . 0 98E-03 0.0 -0.124 0.134 0.133

0.3000 2.1 95E+00 4.873E-03 2 . 200E+00 9 . 040E-02 1 . 260E-03 0.0 -0.121 0.131 0.130

0.3500 2 . 083E+0 0 5.230E-03 2 . 088E+00 1 . 1 38E-0

1

1 .417E-03 0.0 -0.119 0.129 0.128

0 . 4000 2.001 E+00 5.61 0E-03 2 . 007E+00 1 . 382E-0

1

1 . 57 1 E-03 9 . 379E-03 -0.094 0.125 0.124

0.4500 1 . 938E+00 6.01 IE-03 1 . 944E+00 1 .635E-01 1 . 724E-03 3 . 706E-02 -0.089 0.120 0.118

0.5000 1 . 889E+00 6.431 E-03 1 . 896E+00 1 . 8 96 E-0

1

1 . 875E-03 6 . 70 9E-02 -0.083 0.116 0.112

0.5500 1 .851 E+00 6.868E-03 1 . 858E+00 2. 162E-01 2 . 027E-03 9 . 382E-02 -0.078 0.111 0.107

0.6000 1 .821 E+00 7.320E-03 1 . 828E+00 2. 434E-01 2. 179E-03 1 .318E-01 -0.074 0.107 0.103

0.7000 1 . 776E+00 8.265E-03 1 . 784E+ 00 2. 988E-01 2.484E-03 1 . 999E-01 -0.067 0.100 0.094

0.8000 1 . 745E+00 9.259E-03 1 . 755E+00 3 . 554E-0

1

2.793E-03 2.694E-01 -0.061 0.094 0.088

0 . 9000 1 . 724E+00 1 . 030E-02 1 . 735E+00 4.1 27E-01 3. 106E-03 3.390E-01 -0.057 0.090 0.082

1 . 0000 1 . 7 1 OE+OO 1 . 138E-02 1 . 721 E+00 4.706E-01 3.422E-03 4.077E-01 -0.053 0.085 0.077

1 .2500 1 . 6 90E+00 1 . 424E-02 1 . 705E+00 6.167E-01 4 . 233E-0 3 5.734E-01 -0.047 0.077 0.067

1 .5000 1 . 684E+00 1 . 730 E-02 1 .701 E+00 7.635E-01 5 . 070E-03 7.283E-01 -0.042 0.070 0.060

1 .7500 1 . 683E+00 2 . 0 52E-0 2 1 . 704E+00 9. 104E-01 5.931 E-03 8.719E-01 -0.039 0.066 0.055 2.0000 1 . 686E+00 2 . 388E-02 1 . 7 1 OE+OO 1 . 057E+00 6 .31 5E-03 1 . 005E+00 -0.037 0.062 0.051 2.5000 1 . 6 97E+00 3 . 0 94E-02 1 . 728E+00 1 . 348E+00 8.637E-03 1 . 244E+00 -0.033 0.056 0.045

3.0000 1 . 709E+00 3 . 833E-02 1 . 748E+00 1 . 636E+00 1 . 052E-02 1 . 453E+00 -0.031 0.052 0.041 3.5000 1 . 722E+00 4.61 2E-02 1 . 763E+00 1 . 920E+00 1 . 245E-02 1 . 638E+00 -0.030 0.048 0.038

4.0000 1 . 734E+00 5.41 3E-02 1 . 788E+00 2.201 E+00 1 . 44 1 E-02 1 . 80 4E+0 0 -0.028 0.046 0.035

4.5000 1 . 745E+00 6 . 236E-0

2

1 . 808E+00 2 . 479E+00 1 . 641 E-02 1 . 955E+00 -0.027 0.044 0.033

5.0000 1 . 756E+00 7 . 079E-02 1 . 827E+00 2 . 755E+00 1 .S43E-02 2.093E+00 -0.026 0.042 0.032

5.5000 1 . 766 E + 0 0 7 . 940E-02 1 .845E+00 3 . 027E+00 2 . 047 E-0 2 2 . 220E+00 -0.025 0.040 0.031 6.0000 1 . 775E+00 8.81 6E-02 1 .863E+00 3 . 2 96 E + 0 0 2.253E-02 2 . 339E+00 -0.024 0 .039 0.029

7.0000 1 . 792E+00 1 .061E-01 1 . 898E+00 3 . 828 E+0 0 2.66 9E-02 2 . 553E+00 -0.023 0.037 0.027

8.0000 1 . 806E+00 1 . 245E-0

1

1 . 931 E+00 4.351 E+00 3.0S8E-02 2.744E+00 -0.022 0.035 0.026

9.0000 1 .81 9E+00 1 .434E-01 1 . 963E+00 4 . 364E+00 3.509E-02 2.91 7E+00 -0.020 0.033 0.024

10.0000 1 .831 E+00 1 . 626E-0

1

1 . 993E+00 5 . 370E+00 3.931 E-02 3 . 075E+00 -0.019 0.032 0.023

12.5000 1 . 355E+00 2.1 18E-01 2 . 066E+00 6.601 E+00 4 . 986E-02 3 . 420E+00 -0.016 0.029 0.020

15.0000 1 . 37 4E + 00 2 . 625E-0

1

2.1 36E+00 7 . 79 1 E+00 6 . 034E-02 3.71 5E+00 -0.014 0.026 0.018

17.5000 1 . 889E+00 3.142E-01 2 . 204E+00 8 . 943E+00 7 . 069E-02 3 . 972E+00 -0.012 0.024 0.016 20.0000 1 . 903E+00 3 . 668E-01 2 . 270E+00 1 . 006E+0

1

8. 087E-02 4 . 201 E+00 -0.010 0.023 0.015

25.0000 1 . 924E+00 4.740E-01 2 . 398E+00 1 . 220E+0

1

1 . 007E-01 4 . 595E+00 -0.007 0.020 0.012

30.0000 1 . 941 E+00 5 . 330E-0

1

2 . 524E+00 1 . 424E+0

1

1 . 1 96 E-0

1

4 . 927E+00 -0.006 0.018 0.010 35.0000 1 . 955E+00 6 . 934E-01 2 . 648E+00 1 .S17E+01 1 . 378E-0

1

5.21 3E+00 -0.004 0.016 0.008

40.0000 1 . 967E+00 8.051 E-0

1

2 . 772E+00 1 .801 E+0

1

1.551 E-0

1

5 . 464E+00 -0.004 0.015 0.007 45.0000 1 . 977E+00 9.177E-01 2.894E+00 1 . 978E+01 1 .716E-01 5 . 689E+00 -0.003 0.014 0.006 50.0000 1 . 986E+00 1 . 031 E+00 3.01 7E+00 2. 147E+01 1 . 874E-0

1

5.891 E+00 -0.002 0.013 0.005 55.0000 1 . 994E+00 1 . 145E + 00 3 . 1 39E+00 2.310E+01 2 . 025E-0

1

6 . 075E+00 -0.002 0.012 0.005 60.0000 2.001 E+00 1 . 260E + 00 3.261 E+00 2.466E+01 2.169E-01 6 . 244E+0 0 -0.002 0.011 0.004

70.0000 2.01 4E+00 1 . 4 90E+0 0 3 . 504E+00 2 . 762E+0

1

2 . 4 40 E-0

1

6 . 544E+00 -0.001 0.010 0.003

80.0000 2. 025E+00 1 . 723E+00 3 . 748 E+0 0 3.038E+01 2.688E-01 6 . 806E+00 -0.001 0.009 0.003

90.0000 2 . 035E+00 1 . 957E+00 3.991 E+00 3 . 296 E+0

1

2. 918E-01 7 . 033E+00 -0.001 0.009 0.002

100.0000 2 . 043E+00 2 . 1 9 1 E+00 4 . 235E+00 3 . 539E+0

1

3.1 30E-01 7 . 245E+00 -0.001 0.008 0.002

125.0000 2 . 062E+00 2 . 782E+00 4 . 844E+00 4 . 0 9 1 E + 0

1

3.598E-01 7 . 687E+00 -0.001 0.007 0.002

150.0000 2 . 07 6 E + 0 0 3 . 378E+00 5 . 454E+00 4.577E+01 3. 995E-01 3 . 049E+00 -0 .000 0.006 0.001 175.0000 2 . 089E+00 3. 976E+00 6 . 065E+00 5.01 1E+01 4 . 336E-01 3.355E+00 -0.000 0.006 0.001 200.0000 2.1 00E+00 4 . 577E+00 6 . 676E+00 5 . 404E+0

1

4.632E-01 8 . 6 2 1 E + 0 0 -0.000 0.005 0.001 250.0000 2.11 8E+00 5 . 784E+00 7 . 902E+00 6 . 0 92E + 0

1

5 . 1 26E-01 9 . 065E+00 -0.000 0.005 0.001 300.0000 2.1 32E+00 6 . 997E+00 9. 129E+00 6 . 680 E+0

1

5.522E-01 9. 429E+00 -0.000 0.004 0.001 350.0000 2. 145E+00 8.21 4E+00 1 . 036E+01 7.194E+01 5.848E-01 9.737E+00 -0.000 0.004 0.000 400.0000 2. 155E+00 9 . 434E+00 1 . 159E+01 7 . 650E+01 6 . 1 21 E-0

1

1 . OOOE+O

1

-0.000 0.004 0.000

450 .0000 2 . 1 65E+00 1 . 066E+01 1 . 282E+0

1

8 . 060 E+0

1

6.356 E-0 1 1 . 024E+01 -0.000 0.004 0.000 500.0000 2 . 1 73E+00 1 . I88E+01 1

. A05E+0

1

8.432E+01 6 . 559E-0

1

1 . 045E+0

1

-0.000 0.003 0.000

550 . 0000 2. 1 8 1 E+0 0 1 .31 1 E+0

1

1 . 529E+0

1

8 . 773E+0

1

6 . 73SE-01 1 . 064E+0

1

-0.000 0.C03 0 .000 600 .0000 2. 188E+00 1 . 433E+0

1

1 . S52E+0

1

9 . 088E+0

1

6 . 8 94E-0

1

1 .031 E+0

1

-0.000 0.003 0.000 700.0000 2 . 20 0 E+0 0 1 . 679E+01 1 . 899E+0

1

9 . 652E+0

1

7.161 E-0

1

1.11 2E+01 -0.000 0.003 0.000 800.0000 2.21 1 E+00 1 . 926E+01 2. 1 47E+0

1

1 .01 5E+02 7.379E-01 1 . 1 39E+01 - 0.000 0.003 0.000 900.0000 2 . 220E+00 2. 172E+01 2 . 394E+0

1

1 . 059E+02 7.562E-01 1 . 1 62E+0

1

- 0.000 0.003 0.000 1000.0000 2 . 229E+00 2.419E+01 2.641 E+C

1

1 . 0 99E+02 7.717E-01 1 . 133E+01 - 0.000 0.003 0.000

138

r
ELECTRONS IN POLYMETHYL METHACRYLATE, "LUCITE", "PERSPEX” , "PLEXIGLAS"

I = 74.0 eV DENSITY =1.1 90E+00i g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(loqI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR

.

COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 2.1 98E+01 3 . 332E-03 2.1 98E+01 2.580E-04 8 . 329E-05 0.0 -0.193 0.227 0.225

0.0125 1 . 848E+0

1

3.349E-03 1 -849E+01 3.826E-04 9 . 993E-05 0.0 -0.190 0.216 0.215

0.0150 1 .604E+01 3 . 35 9E-0 3 1 . 604E+0

1

5 . 282E-04 1 . 1 58E-04 0.0 -0.184 0.208 0.207 0.0175 1 . 423E+0

1

3.366E-03 1 . 423E+0

1

6.940E-04 1.311 E-04 0.0 -0.179 0.201 0.201 0.0200 1 .283E+01 3 . 372E-03 1 . 284E+0

1

8.792E-04 1 . 460E-04 0.0 -0.175 0.196 0.195

0 .0250 1 . 030E+0

1

3. 382E-03 1 . 081 E+0

1

1 . 306E-03 1 .744E-04 0.0 -0.168 0.188 0.187 0.0300 9 . 400E+00 3.391 E-03 9 . 404E+00 1 .803E-03 2.015E-04 0.0 -0.163 0.182 0.181 0.0350 8 . 367E+00 3.401E-03 8 . 370E+00 2 . 363E-03 2.275E-04 0.0 -0.160 0.177 0.177

0 .0400 7 . 573E+00 3.41 3E-03 7 . 576E+00 2. 997E-03 2 . 526 E-04 0.0 -0.156 0.173 0.173

0 .0450 6 . 942E+00 3 . 425E-03 6 . 946E+00 3.687E-03 2.770E-04 0.0 -0.154 0.170 0.169

0 .0500 6 . 429E+00 3.438E-03 6 . 433E+00 4 . 436E-03 3.007E-04 0.0 -0.151 0.167 0.166

0 .0550 6 . 003E+00 3 . 453E-03 6 . 007E+00 5.241 E-03 3 . 238E-04 0 . 0 -0.149 0.164 0.164

0.0600 5 . 644E+00 3 . 463E-03 5 . 647E+00 6.100 E-03 3.464E-04 0.0 -0.147 0.162 0.162

0.0700 5 . 070E+00 3.502E-03 5 . 073E+00 7. 972E-03 3. 901 E-04 0.0 -0 . 1 44 0.158 0.153

0 .OSOO 4.631E+00 3.538E-03 4 . 635E+00 1 . 004E-02 4 . 322E-04 0.0 -0.142 0.155 0.155

0.0900 4 . 286E+00 3.577E-03 4 . 289E+00 1 . 228E-0 2 4.729E-04 0.0 -0.140 0.152 0.152

0 . 1 000 4 . 006E+00 3.619E-03 4.010E+00 1 . 470E-02 5.125E-04 0.0 -0.138 0.150 0.150

0.1250 3 . 496E+00 3.732E-03 3 . 500E+00 2.1 40E-02 6.070 E-04 0.0 -0.134 0.145 0.145

0.1500 3.152E+00 3.855E-03 3. 155E+00 2.894E-02 6 . 966E-04 0.0 -0.131 0.142 0.142

0 . 1 750 2 . 904E+00 3. 987E-03 2 . 908E+00 3.721 E-02 7.824E-04 0.0 -0.128 0.139 0.139

0.2000 2.71 9E+00 4. 126E-03 2 . 723E+00 4.510 E-02 8 . 650E-04 0.0 -0.126 0.137 0.136

0 . 2500 2.461 E+00 4.425E-03 2 . 465E+00 6 .547E-02 1 . 023E-0 3 0.0 -0.123 0.133 0.132

0.3000 2.292E+00 4.751 E-03 2 . 297 E + 0 0 3 . 653E-02 1 . 1 75E-03 0.0 -0.120 0.130 0.129

0.3500 2. 175E+00 5.101 E-03 2. 180E+00 1 . 089E-0

1

1 . 322E-0 3 0.0 -0.118 0.128 0.127

0.4000 2 . 0 90E+0 0 5 . 474E-03 2 . 096E+00 1 . 323E-0

1

1 .466E-03 0.0 -0.117 0.126 0.125

0.4500 2. 026E+00 5.867E-03 2.032E+00 1 .566E-01 1 . 609E-03 1 . 466E-02 -0.092 0.122 0.120 0.5000 1 . 975E+00 6 .278E-03 1 . 981 E+00 1 .81 5E-01 1 . 751 E-03 4.112E-02 -0.086 0.118 0.115

0.5500 1 . 935E+00 6 . 707E-03 1 . 942E+00 2.070E-01 1 . 8 92E-0 3 6 . 992E-02 -0.081 0.113 0.110 0.6000 1 . 903E+00 7. 149E-03 1 . 91 0E+00 2.330E-01 2.035E-03 1 . 005E-0

1

-0.076 0.109 0.105

0.7000 1 .356E+00 8 . 076E-03 1 . 864E+00 2.860E-01 2. 320E-03 1 .650E-01 -0.063 0.102 0.097

0.8000 1 . 825E+00 9.050E-03 1 . 834E+00 3.401E-01 2.609E-03 2.321E-01 -0.062 0.096 0.090 0.9000 1 . 80 3E+0 0 1 . 007E-02 1 .81 3E+00 3.950E-01 2.902E-03 3.001 E-01 -0.057 0.091 0.083

1 . 0000 1 . 788E+00 1 .113E-02 1 . 7 99E+0 0 4 .504E-01 3.1 99E-03 3.679E-01 -0.053 0.087 0.078

1 .2500 1 . 767E+00 1 . 393E-02 1 . 78 1 E+00 5. 902E-01 3. 959E-03 5.330E-01 -0.046 0.078 0.068

1.5000 1 . 760E+00 1 . 6 93E-02 1 . 776E+00 7 . 308E-01 4.744E-03 6 .S87E-01 -0.041 0.071 0.060

1 .7500 1 . 759E+00 2.009E-02 1 . 779E+00 3.715E-01 5 . 553E-03 8.339E-01 -0.033 0.066 0.055

2.0000 1 .762E+00 2.333E-02 1 . 735E+00 1 . 0 1 2E+00 6.383E-03 9. 689E-01 -0.035 0.062 0.050 2.5000 1 . 772E+00 3.031 E-02 1 . 80 2E+0 0 1 .291 E+00 8 . 096E-03 1 . 21 2E+00 -0.032 0.056 0.044

3.0000 1 . 734E+00 3 . 761 E-02 1 . 322E+00 1 . 567E+00 9 . 868E-03 1 . 425E+00 -0.029 0.051 0.039

3.5000 1 . 7 97E+00 4 . 521 E-02 1 . 842E+00 1 .839E+00 1 . 163E-02 1 .61 3E+00 -0.028 0.048 0.036 4.0000 1 . 30 9E+0 0 5 . 307E-02 1 . 862E+00 2. 1 09E+00 1 . 354E-02 1 . 783E+00 -0.027 0.045 0.034

4.5000 1 .821 E+00 6.11 5E-02 1 . 832E+00 2 . 376 E+0 0 1 . 542E-02 1 . 936E+00 -0.025 0 .043 0 .032

5 .0000 1 -832E+00 6 . 943E-02 1 . 90 1 E + 00 2.641 E+00 1 . 7 33E-02 2 . 077E+00 -0.025 0.041 0 .030 5.5000 1 . 842E + 0 0 7 .783E-C2 1 . 920E+00 2. 903E + 00 1 . 925E-02 2 . 207E+00 -0.024 0.039 0.029

6.0000 1 .851 E+00 8.648E-02 1 . 938E+00 3 . 1 62E+00 2. 120E-02 2 . 327E+00 -0.023 0.038 0 .028 7.0000 1 . 868E+00 1 .041E-01 1 . 972E+00 3 . 673E + 00 2.51 3E-02 2 . 545E + 0 0 -0 .022 0 .036 0.026 8.0000 1 . 333E+00 1 .222E-01 2 . 005E+00 4. 176E+00 2.91 OE-02 2 . 739E+00 -0 .020 0.034 0.025

9.0000 1 . 896E+00 1 .407E-01 2 . 0 37E + 0 0 4.671 E+00 3.309E-02 2 . 91 4E+00 -0.019 0.032 0.023

10.0000 1 . 908E+00 1 .596E-01 2 . 06 7E+0 0 5 . 1 58E+00 3.71 0E-02 3 . 073E+00 -0.018 0.031 0.022

12.5000 1 . 932E+00 2.079E-01 2. 140E+00 6 . 346E+00 4.712E-02 3.421 E+00 -0.015 0 .023 0.020

1 5 .0000 1 . 952E+00 2.577E-01 2.21 0E+00 7 . 496E+00 5.709E-02 3.71 6E+00 -0.013 0 . 025 0.017

17.5000 1 . 963E+00 3. 086E-01 2 . 277E+00 8 . 6 1 0 E + 0 0 6 . 695E-02 3. 974E+00 -0.011 0.024 0.016 20.0000 1 . 982E+00 3.603E-01 2 . 342E+00 9.693E+00 7.667E-02 4 . 202E+00 -0.010 0.022 0.014 25.0000 2 . 004E+00 4.656E-01 2 . 4 70E+0 0 1 . 177E+01 9.561 E-02 4 . 596E+00 -0.007 0.019 0.012

30.0000 2. 022E+00 5.728E-01 2 . 5 95E+0 0 1 . 375E+0

1

1 . 1 38E-0

1

4. 927E+00 -0.006 0.017 0.010 35.0000 2 . 036E+0 0 6.815E-01 2.718E+00 1 .563E+01 1 . 31 3E-01 5.21 2E+00 -0.005 0.016 0.008 40.0000 2 . 049E+00 7.912E-01 2.340E+00 1 . 743E+0

1

1 . 480E-0

1

5.463E+00 -0.004 0.014 0.007 45.0000 2.059E+00 9.020E-01 2.961 E+00 1 . 91 5E+01 1 . 639E-01 5 . 687E+00 -0.003 0.013 0.006 50.0000 2 . 06 9E+00 1 .013E+00 3 . 082E+00 2 . 08 1 E+0

1

1 . 7 92E-0

1

5.389E+00 -0.003 0.012 0 .005 55.0000 2 . 077E+00 1 . 1 26E+00 3.203E+00 2 . 240E+0

1

1 . 939E-01 6 . 072E+00 -0.002 0.012 0.005 60.0000 2 . 085E+00 1 . 233E+00 3. 323E+00 2 . 393E+0

1

2.079E-01 6.241 E+00 -0.002 0.011 0.004 70.0000 2 . 0 98E+00 1 . 465E+00 3 . 563E+00 2 . 684E+0

1

2 . 342E-0

1

6 . 541 E+00 -0.001 0.010 0.004

80 .0000 2. 1 09E+00 1 . 6 94E + 00 3 . 804E + 0 0 2 . 955E+0

1

2.585E-01 6.80 3E + 00 -0.001 0.009 0 .003 90.0000 2. 120E+00 1 . 924E+00 4 . 044E+00 3.210E+01 2.81 OE-OI 7 . 034E+00 -0.001 0.008 0.003 100.0000 2 . 1 28E+00 2. 1 55E+00 4 . 284E+00 3 . 450E+0

1

3.01 9E-01 7 . 242E+00 -0.001 0.003 0.002 125.0000 2 . 1 47E+00 2 . 7 37E+0 0 4 . 884E+00 3 . 996 E+0

1

3.481E-01 7 .683E+00 -0.001 0.007 0.002 150.0000 2.16 3E+00 3 . 323E+00 5 . 436E+00 4.479E+01 3 . 874E-0

1

8 . 045E+00 -0.000 0.006 0.001 175.0000 2. 176E+00 3 . 91 2E+00 6 . 037E+00 4.912E+01 4.213E-01 8.351 E+00 - o.ooo 0 .006 0.001 200.0000 2. 187E+00 4.503E+00 6 . 6 90 E+0 0 5 . 303E+0

1

4.509E-01 8.61 7E+00 -0.000 0.005 0.001 250.0000 2 . 205E+00 5.692E+00 7 . 897E+00 5 . 9 90 E+0

1

5.004E-01 9 . 0 6 1 E + 0 0 -0.000 0.005 0.001 300.0000 2. 220E+00 6 . 387E+00 9. 107E+00 6.579E+01 5.402E-01 9 . 425E+00 -0.000 0 .004 0.001 350.0000 2 . 233E+00 8 . 085E+00 1 . 032E+0

1

7.095E+01 5.731E-01 9 . 733E+00 - 0.000 0.004 0.000 400.0000 2 . 244E+00 9 . 286E+00 1 . 1 53E+0

1

7.553E+01 S.008E-01 9. 999E+00 - 0 .000 0 .004 0.000 450.0000 2 . 254E+00 1 . 0* 9E + 0

1

1 . 274E+0

1

7. 965E+01 6 .246E-01 1 .023E+01 -0 .000 0.003 0.000 500.0000 2 . 263E+00 1 . 170E+01 1 . 3 96 E+0

1

3 . 340E+0

1

6.452E-01 1 . 044E+0

1

- 0.000 0.003 0.000 550.0000 2.271 E+00 1 .290E+01 1 .51 8E+01 8 . 634E+0

1

6 . 633E-01 1 . 0 64E+0 1 - 0.000 0.003 0.000 600.0000 2 . 278E+00 1.411 E+0

1

1 . 639E+01 9 . 000E+01 6 . 793E-01 1 . 08

1

E +0

1

- 0 .000 0 . 003 a .ooo 700.0000 2.291 E+00 1 . 653E+0

1

1 . 3S2E+0

1

9.569E+01 7.066E-01 1 . 1 12E+01 - 0.000 0.003 0.000 800.0000 2 . 302E+00 1 . 3 96 E+O

1

2. 126E+0! 1 . 007E+02 7.289E-01 1 . 1 38E+0

1

- 0.000 0.003 0.000 900.0000 2.31 2E+00 2. 1 39E+01 2. 370E+01 1 .051 E+02 7.476E-01 1 . 1 62E+01 - 0.000 0 .003 0.000

1 000.0000 2 . 320E+00 2.382E+01 2.614E+01 1 . 092E+02 7 . 636E-01 1 . 183E + 01 - 0.000 0.003 0.000

159
ELECTRONS IN POLYPROPYLENE

I = 59.2 eV DENSITY = 9.000E-01 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DEMS.EFF. d( log1 )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2 /g MeV cm 2/g g/cm 2 0.0100 2 . 383E+01 2.883E-03 2 . 383E+0

1

2 . 366E-04 6 . 658E-05 0.0 -0.190 0.215 0.214 0.0125 2.000 E+0

1

2.893E-03 2 . 000 E+0

1

3.51 6E-04 7 . 985E-05 0.0 -0.182 0.206 0.205

0.0150 1 . 733E+0

1

2. 900E-03 1 . 734E+0

1

4.863E-04 9.254E-05 0.0 -0.177 0.193 0.193

0.0175 1 . 536 E + 0

1

2.905E-03 1 . 536E+0

1

6.398E-04 1 . 048E-04 0 .

0

-0.172 0.193 0.192

0.0200 1 . 384E+01 2. 91 0E-03 1 . 384E+0

1

8. 1 15E-04 1 . 1 67E-04 0.0 -0.168 0.188 0.187

0.0250 1 . 1 64E+0

1

2.91 9E-03 1 . 1 64E+01 1 .207E-03 1 . 394E-04 0.0 -0.162 0.180 0.180

0.0300 1.01 1 E+0

1

2.929E-03 1 .012E+01 1 .669E-03 1 .612E-04 0.0 -0 . 1 58 0.175 0.174

0.0350 8. 995E+00 2. 939E-03 8 . 998E+00 2.1 95E-03 1 . 822E-04 0.0 -0.154 0.170 0.170 0.0400 8.136E+00 2.951E-03 8.1 39E+00 2 . 780E-03 2.025E-04 0.0 -0.151 0.166 0.166

0.0450 7 . 454E+00 2.963E-03 7 . 457E+00 3.422E-03 2.223E-04 0.0 -0.149 0.163 0.163

0.0500 6 . 900E+00 2. 976E-03 6 . 903E+00 4. 1 20E-03 2.41 5E-04 0 . 0 -0.146 0.161 0.160

0.0550 6 . 440E+00 2.991E-03 6 . 443E+00 4 .870E-03 2 . 602E-04 0 . 0 -0.145 0.153 0.158

0.0600 6 . 052E + 00 3 . 006E-03 6 . 055E+00 5.671E-03 2.786E-04 0.0 -0.143 0.156 0.156 0.0700 5 . 433E+00 3 . 037E-03 5 . 436 E + 0 0 7.418E-03 3. 142E-04 0.0 -0.140 0.153 0.152

0.0800 4 . 960E+00 3.071E-03 4.963E+00 9.347E-03 3 . 435E-04 0.0 -0.137 0.150 0.149

0.0900 4 . 588E+00 3. 107E-03 4 . 59 1 E+00 1 . 144E-02 3.813E-04 0.0 -0 . 1 35 0.147 0.147 0.1000 4 . 287E+00 3. 145E-03 4 . 290E+00 1 . 370E-02 4. 1 41 E-04 0.0 -0.134 0.145 0.145

0.1250 3 . 738E + 00 3.243E-03 3.741 E+00 1 . 997E-02 4.91 5E-04 0.0 -0.130 0.141 0.140

0.1500 3 . 367E + 00 3.360E-03 3 . 370 E + 0 0 2.703E-02 5.651 E-04 0.0 -0.127 0.133 0.137

0.1750 3. 101E+00 3 . 478E-03 3. 105E+00 3 . 477E-02 6 . 357E-04 0 .

0

-0.125 0.135 0.134 0.2000 2. 902E + 00 3 . 603E-03 2 . 905E+00 4.31 0E-02 7.038E-04 0.0 -0.123 0.133 0.132

0 .2500 2 . 624E+00 3.872E-03 2 . 628E+00 6 . 126E-02 3 . 345E-04 0.0 -0.119 0.129 0.128

0.3000 2 . 443E+00 4.165E-03 2. 447E+00 8. 102E-02 9.601 E-04 0.0 -0.117 0.126 0.126 0.3500 2.31 7E+00 4 . 478E-03 2 . 322E+00 1 . 020E-0

1

1 . 082E-03 0.0 -0.115 0.124 0.123

0.4000 2 . 225E+00 4.812E-03 2 . 229E+00 1 .240E-01 1 . 202E-0 3 1 . 122E-02 -0.091 0.121 0.119

0.4500 2 . 1 53E + 00 5. 163E-03 2. 159E+00 1 . 468E-0

1

1 . 322E-0 3 3. 973E-02 -0.085 0.116 0.113

0.5000 2 . 0 98E+0 0 5.531E-03 2.104E+00 1 . 70 3E-0

1

1 . 440E-03 7.098E-02 -0.079 0.111 0.108

0.5500 2 . 055E + 00 5.914E-03 2.061 E+00 1 . 943E-01 1 .559E-03 1 . 042E-0

1

-0.074 0.107 0.103

0.6000 2 . 020E+00 6.310E-03 2 . 027E+00 2. 188E-01 1 . 679E-03 1 . 388E-0

1

-0.070 0.103 0.098

0.7000 1 . 969E + 00 7.138E-03 1 . 976E+00 2.688E-01 1 .91 9E-03 2. 107E-01 -0.063 0.096 0.090

0.8000 1 . 934E + 00 8.009E-03 1 . 942E+00 3. 1 99E-01 2. 163E-03 2.841E-01 -0.057 0.090 0.083

0 . 9000 1 . 91 0E+00 8.919E-03 1 . 91 9E+00 3.717E-01 2.409E-03 3.575E-01 -0.053 0.085 0.077

1 .0000 1 . 893E+00 9.867E-03 1 . 903E+00 4.240E-01 2.660E-03 4.300E-01 -0.049 0.081 0.072

1 .2500 1 . 86 9E + 00 1 . 238E-02 1 . 882E+00 5.563E-01 3.303E-03 6 .045E-01 -0.043 0.072 0.063

1 .5000 1 . 860E+00 1 -506E-02 1 .376E+00 6 .894E-01 3. 969E-03 7.670E-01 -0.039 0.065 0.056

1 .7500 1 . 859E+00 1 . 78 9E-0 2 1 . 877E+00 8.227E-01 4.656E-03 9.173E-01 -0.036 0.062 0.051 2.0000 1 .861 E + 00 2.084E-02 1 . 882E+00 9.557E-01 5.361E-03 1 . 056E+00 -0.034 0.058 0.047

2.5000 1 . 87 1 E+0 0 2 . 706E-02 1 . 898E+00 1 . 220E+00 6.821E-03 1 .305E+00 -0.031 0.052 0.041 3.0000 1 . 883E + 00 3.361E-02 1 . 91 7E+00 1 . 483E+00 3.332E-03 1 . 52 1 E+00 -0.029 0.043 0.037

3.5000 1 -896E + 00 4.044E-02 1 . 936E+00 1 .742E+00 9.886E-03 1 .71 3E+00 -0.027 0.045 0.035

4 .0000 1 . 903E+00 4.751E-02 1 . 956E+00 1 . 999E+00 1 . 147E-02 1 .885E + 00 -0.026 0.042 0.032

4.5000 1 . 920 E+0 0 5 . 477E-02 1 . 97 5E + 0 0 2 . 253E+00 1 . 309E-02 2 . 040E+00 -0.025 0.040 0.031 5.0000 1 . 931 E+00 6 . 222E-02 1 . 993E+00 2.505E+00 1 . 473E-02 2. 183E+00 -0.024 0.039 0.029

5.5000 1 . 941 E+00 6 . 984E-02 2.01 1 E+00 2 . 7 55E+0 0 1 . 639E-02 2.314E+00 -0.023 0.037 0 .028

6 .0000 1 . 951 E+00 7.759E-02 2 . 028E+00 3 . 003E+00 1 . S06E-02 2 . 436E+00 -0.022 0.036 0 . 027 7.0000 1 . 968E+00 9.343E-02 2 . 062E+00 3. 492E+00 2.1 45E-02 2 . 658E+00 -0 .021 0.034 0.025 8.0000 1 . 983E + 00 1 .098E-01 2 . 093E+00 3 . 973E+00 2. 488E-02 2 . 35 5 E+00 -0.019 0.032 0 . 024 9.0000 1 . 997E+00 1 .265E-01 2 . 1 23E+00 4 . 447E+00 2.334E-02 3 . 0 33E+00 -0.018 0.031 0.022

10.0000 2 . 008E+00 1 .435E-01 2.1 52E+00 4.915E+00 3. 182E-02 3.1 96E+00 -0.017 0.029 0.021 12.5000 2 . 033E+00 1 . 872E-0

1

2.221 E+00 6 . 059E+00 4 . 056E-02 3 . 553E+00 -0.014 0.026 0.013

15.0000 2 . 053E+00 2.322E-01 2 . 285E+00 7.168E+00 4 . 930E-02 3 . 856 E+0 0 -0.011 0.024 0.016

17.5000 2 . 069E+00 2.782E-01 2.347E+00 8 . 248E+00 5.798E-02 4. 1 22E+00 -0.009 0.022 0.014

20.0000 2 . 083E+00 3.249E-01 2 . 408E+00 9.299E+00 6.658E-02 4 . 357E+00 -0.008 0.020 0.013

25.0000 2. 105E+00 4.202E-01 2 . 525E+00 1 . 1 33E+01 3 . 343E-02 4 . 762E+00 -0.005 0.018 0.010

30.0000 2. 123E+00 5. 173E-01 2 . 640E+00 1 . 326E+0

1

9.975E-02 5.101 E+00 -0.004 0.016 0.003

35.0000 2. 137E+00 6.153E-01 2. 753E+00 1 .512E+01 1 . 155E-01 5 . 392E+00 -0.003 0.014 0.007 40.0000 2 . 1 49E+00 7.153E-01 2 . 365E+00 1 . 6 90E+0

1

1 . 307E-0

1

5 . 648E+00 -0.002 0.013 0.006 45.0000 2. 160E+00 8.157E-01 2. 976E+00 1 . 86 1 E+0

1

1 .453E-01 5 . S75E+00 -0.002 0.012 0.005

50.0000 2. 170E+00 9. 1S9E-01 3 . 086E+00 2 . 026 E+0

1

1 . 593E-0

1

6 . 079E+00 -0.002 0.011 0.004

55.0000 2. 178E+00 1 .01 9E+00 3.1 97E+00 2. 185E+01 1 . 728E-0

1

6 . 265E+00 -0.001 0.010 0.004

60.0000 2. 186E+00 1 .121 E+00 3. 307E+00 2 . 339E+0

1

1 . 858E-0

1

6 . 435E+00 -0.001 0.010 0.003

70 .0000 2 . 200 E+0 0 1 . 327E+00 3 . 527E+00 2 . 632E+0

1

2. 104E-01 6 . 738E+00 -0.001 0.009 0.003

80 . 0000 2.211 E+00 1 . 5 35E + 0 0 3 . 746 E + 00 2. 907E+01 2.333E-01 7.001 E+00 -0.001 0.008 0.002

90.0000 2 . 222E+00 1 . 744E+00 3. 966E+00 3. 166E+01 2.546E-01 7 . 233E+00 -0.001 0.007 0.002

100.0000 2 . 23 1 E+00 1 . 954E+00 4. 185E+00 3.412E+01 2.745E-01 7 . 442E+00 -0.000 0.007 0.002

1 25.0000 2. 250E+00 2 . 483E+00 4 . 733E+00 3. 973E+01 3. 189E-01 7 .834E+00 -0 .000 0.006 0.001 150.0000 2 . 26 6 E+0 0 3.01 5E+00 5 . 282E+00 4.473E+01 3.572E-01 8 . 247E+00 -0.000 0.005 0.001 175.0000 2. 230E+00 3 . 55 1 E+00 5.331 E+00 4 . 923E+0

1

3.905E-01 8 . 553E+00 -0.000 0.005 0.001

200 .0000 2.291 E+00 4 . 089E+00 6 . 380E+00 5 . 333E+0

1

4. ! 99E-01 8.81 9E+00 -0.000 0.004 0.001 250.0000 2 . 3 1 0 E+00 5. 1 71 E+00 7 . 482E+00 6 . 056 E + 0

1

4.694E-01 9 . 254E+00 -0.000 0.004 0.001 300.0000 2 . 326E+00 6 . 259E+00 8 . 585E+00 6.679E+01 5 . 0 96E-0 1 9 . 6 28 E + 00 -0.000 0.004 0.000

350 .0000 2 . 339E+00 7 . 350E+00 9 . 689E+00 7.227E+01 5.432E-01 9 . 936E+00 -0.000 0.003 o.oco 400.0000 2.351 E+00 3.444E+00 1 . 080E+0

1

7.716E+01 5.716E-01 1 . 020E+0

1

-0.000 0.003 0.000

450 . 0000 2.361 E+00 9.541 E+00 1 . 1 90 E+0 1 3 . 1 57 E+0 1 5.961E-01 1 . 044E+0

1

-0 .000 0.003 0.000 500.0000 2 . 370 E+0 0 1 . 064E+0

1

1 . 30 1 E+0

1

8 . 558E+0

1

6 . 1 75E-01 1 . 065E+01 -0 . 000 0.003 o.ooo 550.0000 2. 373E + 00 1 . 1 74E+0

1

1 .412E+01 8 . 927E + 0

1

5 . 364E-0

1

1 . 034E+0

1

-0.000 0.003 0.000 600.0000 2 . 386 E+0 0 1 . 284E+01 1 . 523E+0

1

9.268E+01 6 .531E-01 1.101 E+0

1

-0.000 0.003 0.000

700 .0000 2. 399E+00 1 . 505E+0

1

1 . 745E+01 9 . 88 1 E+0

1

6.817E-01 1 . 1 32E+01 -0 .000 0 .002 0 .000 800 .0000 2.411 E+00 1 . 726 E + 0 1 1 . 967E + 0

1

1 . 042E+02 7.053E-01 1 . 1 59E+01 -0.000 0.002 0.000

900 .0000 2.421 E+00 1 . 947E+01 2. 189E+01 1 . 090E+02 7.251E-01 1 . 182E+01 -0.000 0.002 0.000 1000.0000 2 . 430E+00 2. 1 69E+01 2.412E+01 1 .134E+02 7.421E-01 1 . 203E+01 - 0.000 0.002 0.000

140 r
ELECTRONS IN POLYSTYRENE

iL.

I = 63.7 eV

ENERGY STOPPING POWER COLLISION RADIATIVE TOTAL MeV MeV c» 2/g MeV cm 2 /g MeV cm 2 /g 0.0100 2 . 223E+0

1

2.982E-03 2.224E+01

0.0125 1 . 868E+01 2. 992E-03 1 .869E + 01 0.0150 1 .621E+01 2. 999E-03 1 .621 E+0

1

0.0175 1 . 437E+0

1

3.004E-03 1 . 438E+0

1

0.0200 1 .296E+01 3.008E-03 1 . 296E+0

1

0.0250 1 . 091 E+01 3.017E-03 1 . 091 E+01 0.0300 9 . 485E+00 3 . 027E-03 9 . 488E + 00 0.0350 8 . 440E+00 3.037E-03 3 . 443E+0 0

0 .0400 7 . 6 37E+0 0 3 . 048E-03 7 . 640 E+0 0 0.0450 7 . 000E+00 3.061E-03 7 . 003E+00

0.0500 6.481 E+00 3.074E-03 6 . 484E+0 0 0.0550 6.051 E+00 3.083E-03 6 . 054E+00

0.0600 5.688E+00 3.103E-03 5.691 E+00 0.0700 5. 103E+00 3. 135E-03 5.11 1 E+00 0.0800 4 . 566E+00 3.169E-03 4.66 9E + 00

0 .0900 4.317E+00 3.206E-03 4 . 320E+00

0.1000 4 . 034E+00 3.244E-03 4 . 038E+00

0.1250 3 . 520E+00 3.350E-03 3 . 523E+00

0.1500 3. 172E+00 3.463E-03 3 . 1 76E+00

0.1750 2. 923E+00 3.584E-03 2 . 926E+00

0.2000 2 . 735E+0 0 3.711 E-03 2 . 739E+00

0.2500 2 . 475E+00 3. 935E-03 2 . 479E+00

0.3000 2 . 305E+00 4.284E-03 2. 309E+00

0.3500 2. 187E+00 4.604E-03 2.1 92E+00

0.4000 2.101 E+00 4 . 945E-03 2 . 1 06 E+00 0.4500 2 . 035E+00 5.304E-03 2 . 040E + 00 0.5000 1 . 984E+00 5.680E-03 1 . 990E+00

0.5500 1 . 943E+00 6.071 E-03 1 . 950E + 00 0.6000 1 .911 E+00 6.475E-03 1 . 918E+00

0.7000 1 . 864E+00 7.322E-03 1 .871 E+00 0.8000 1 . 832E+00 8.212E-03 1 .840E+00

0 . 9000 1 .81 OE+OO 9. 142E-03 1 .81 9E+00

1 .0000 1 . 794E+00 1 .01 IE-02 1 . 804E+00

1 .2500 1 . 773E+00 1 . 267E-02 1 . 7S6E + 00

1 .5000 1 .766E+00 1 .541E-02 1 .781 E+00

1 .7500 1 .765E+00 1 .830E-02 1 . 783E+00

2.0000 1 . 768E+00 2.1 32E-02 1 . 789E+00

2.5000 1 . 778E+00 2 . 766E-02 1 . 80 6E + 0 0 3.0000 1 . 791 E+00 3 . 435E-02 1 . 825E+00

3.5000 1 . 804E+00 4.132E-02 1 . 845E+00

4.0000 1 .S16E+00 4.852E-02 1 . 86 5E+0 0 4.5000 1 . 828E+00 5 . 593E-02 1 . 884E+00

5.0000 1 .339E+00 6 . 353E-02 1 . 902E+00

5.5000 1 . 849E+00 7.129E-02 1 . 920E+00

6.0000 1 .S59E+00 7.91 9E-02 1 . 933E+00

7.0000 1 . 876 E + 0 0 9.539E-02 1 . 971 E+00 8.0000 1 .891 E+00 1 . 120E-01 2. 003E+00

9.0000 1 . 904E+00 1 . 290E-0

1

2 . 0 33E+00

10.0000 1 . 916E+00 1 .464E-01 2 . 062E+00

12.5000 1 . 940E+00 1 .909E-01 2. 1 31 E+00 15.0000 1 . 960E+00 2.367E-01 2 . 1 96E+00

17.5000 1 . 975E+00 2.835E-01 2 . 259E+00

20.0000 1 . 989E+00 3.31 IE-01 2 . 320E+00

25.0000 2.01 OE+OO 4.2S2E-01 2 . 439E+00

30.0000 2 . 027E+00 5 . 270E-0

1

2 . 554E+00

35.0000 2.041 E+00 6.271E-01 2 . 669E+00

40.0000 2 . 053E+00 7.284E-01 2 . 782E+00

45.0000 2 . 064E+00 8.306E-01 2 . 894E+00

50.0000 2 . 073E+00 9 . 334E-01 3 . 006E+00

55.0000 2.081 E+00 1 . 0 37E+00 3.1 18E+00 60.0000 2 . 089E+00 1 .141 E+00 3 . 230E+00

70.0000 2. 102E+00 1 . 35 1 E+00 3 . 452E+00

80.0000 2.11 3E+00 1 . 56 2E+0 0 3 . 675E+00

90.0000 2. 1 23E+00 1 . 774E+00 3 . 897E+00

100.0000 2 . 1 32E+00 1 . 988E+00 4. 120E+00

1 25.0000 2.151E+00 2 . 525E+00 4 . 67 6E+0 0 150.0000 2. 166E+00 3 . 067E+00 5 . 233E+00

175.0000 2. 179E+00 3.611 E+00 5 . 790E+00

200.0000 2. 1 90E+00 4.158E+00 6 . 348E+00 250.0000 2 . 208E+00 5 . 258E + 00 7 . 466 E+0 0 300.0000 2.223E+00 6 . 362E+00 8 . 58 6E+0 0 350.0000 2 . 236E+00 7.471 E+00 9 . 707E+00

400.0000 2 . 247E+00 8 . 583E+00 1 . 083E+0

1

450.0000 2 . 257E+00 9 . 697E+00 1 . 1 95E+01 500.0000 2 .2S6E+00 1 .081E+01 1 . 308E+0

1

550.0000 2 . 274E+00 1 . 1 93E+01 1 . 4 20E + 0

1

600.0000 2.281 E+00 1 . 305E + 0

1

1 . 533E+0

1

700.0000 2 . 293E+00 1 . 529E+0

1

1 . 758E+0

1

300.0000 2. 304E+00 1 . 754E+01 1 . 984E+01 900.0000 2.31 4E+00 1 . 978E+01 2.210E+01 1000.0000 2 . 323E+00 2 . 203E+01 2 . 436E+0

1

DENSITY = 1 . 060E+00i g/cm 3

CSDA RADIATION DENS.EFF. d(log )/d(logI) RANGE YIELD CORR

.

COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

g/cm 2 546E-04 7 . 406E-05 0.0 -0.195 0.223 0.221 777E-04 8 .869E-05 0.0 -0.187 0.212 0.211 218E-04 1 .C27E-04 0.0 -0.131 0.205 0.204 859E-04 1 . 1 6 2E-04 0.0 -0.176 0 . 1 98 0.198 694E-04 1 .292E-04 0.0 -0.172 0.193 0.193 292E-03 1 . 543E-04 0.0 -0.166 0.135 0.185 785E-03 1 .782E-04 0.0 -0.162 0.179 0.179 345E-03 2.013E-04 0.0 -0.158 0.175 0.174 968E-03 2 . 235E-04 0 .

0

-0.155 0.171 0.170 653E-03 2.452E-04 0.0 -0.152 0.167 0.167 395E-03 2.662E-04 0.0 -0.150 0.165 0.164

1 94E-03 2.S67E-04 0 .

0

-0.148 0.162 0.162 047E-03 3 . 068E-04 0.0 -0.146 0.160 0.160 905E-03 3 . 458E-04 0.0 -0.143 0.156 0.156 955E-03 3.334E-04 0.0 -0.140 0.153 0.153 213E-02 4. 1 97E-04 0.0 -0.138 0.151 0.150 458E-02 4 . 550E-04 0.0 -0.136 0.148 0.148 124E-02 5.396E-04 0.0 -0.132 0.144 0.144 873E-02 6 . 1 99E-04 0.0 -0.129 0.140 0.140 695E-02 5 . 967E-04 0.0 -0.127 0.138 0 . 1 37 579E-02 7.709E-04 0.0 -0.125 0 . 1 35 0.135 504E-02 9. 1 31E-04 0.0 -0.122 0.132 0.131 598E-02 1 . 050E-03 0.0 -0.119 0.129 0.128

082E-01 1 . 182E-03 0.0 -0.117 0.127 0.125

31 5E-01 1 . 31 2E-03 2 . 729E-0 3 -0.102 0.124 0 . 123 557E-01 1 .441E-03 2.688E-02 -0.090 0.119 0.117 805E-01 1 . 570E-03 5 . 420E-02 -0.084 0.115 0.112

059E-01 1 .699E-03 8 . 383E-02 -0.079 0.111 0.107

318E-01 1 . 327E-0 3 1 . 1 52E-0

1

-0.074 0.107 0.102

846E-01 2.087E-03 1 .81 0 E-0

1

-0.067 0.100 0.094

385E-01 2 . 349E-03 2.492E-01 -0.061 0.094 0 . 088 932E-01 2.615E-03 3.179E-01 -0.057 0.089 0.082

484E-01 2.885E-03 3.862E-01 -0.053 0 . 085 0.077

878E-01 3 . 577E-03 5.515E-01 -0.046 0.077 0 .067

281 E-01 4 . 293E-03 7 . 064E-01 -0.042 0.070 0.060

684E-01 5.030E-03 8.501 E-0

1

-0.039 0.065 0.055 008E+00 5.783E-03 9.834E-01 -0.037 0.062 0.050

. 287E+00 7.352E-03 1 . 222E+00 -0.034 0.055 0.045 562E+00 8. 970E-03 1 . 431 E+00 -0.031 0.051 0.041

. 335E+00 1 . 063E-02 1 .61 6E+00 -0.030 0.048 0.038

104E+00 1 . 233E-02 1 . 782E+00 -0.029 0.046 0.035

371 E+00 1 . 405E-02 1 . 932E+00 -0.027 0.044 0.034 635E+00 1 .580E-02 2 . 070E+00 -0.026 0.042 0.032 897E+00 1 . 757E-02 2.1 97E+00 -0.025 0.040 0.031

1 56 E+00 1 . 936E-02 2. 31 6E+00 -0.025 0.039 0.030 667E+00 2.297E-02 2.531 E+00 -0.023 0.037 0.028

1 71 E+00 2 . 662E-02 2 . 722E+00 -0.021 0.035 0 .026 666E+00 3.029E-02 2 . 8 96E+0 0 -0.020 0.033 0.025

155E+00 3 . 399E-02 3 . 054E+00 -0.019 0.032 0.023 347E+00 4 . 325E-02 3 . 40 3E+0 0 -0.015 0.029 0.020 502E+00 5.249E-02 3 . 702E+00 -0.013 0.026 0.018 625E+00 6 . 1 66E-02 3 . 963E+00 -0.010 0.024 0.016

71 7E+00 7 . 072E-02 4. 1 96 E+00 -0.009 0.022 0.014

182E+01 8.844E-02 4 . 596E+00 -0.005 0.019 0.011 332E+01 1 .056E-01 4. 933E+00 -0.005 0.017 0.009

574E+01 1 .220E-01 5 . 223E+00 -0.003 0.016 0 .008 757E+01 1 . 378E-0

1

5 . 478E+00 -0.003 0.014 0.006

933E+01 1 .530E-01 5 . 704E+00 -0.002 0.013 0.005

1 03E+01 1 .676E-01 5 . 908E+00 -0 .002 0.012 0.005

26 6 E+0

1

1 .816E-01 6 . 093E+00 -0.002 0.011 0.004

424E+01 1 . 951 E-0

1

6 . 26 3E + 00 -0.001 o . on 0.004

723E+01 2.204E-01 6 . 565E+00 -0.001 0.010 0.003

004E+01 2 . 439E-0

1

6 . 828E + 0 0 -0.001 0.009 0.002

268E+01 2.658E-01 7 . 060E+00 -0.001 0.008 0.002

518E+01 2.861 E-0

1

7.269E+00 -0.001 0.008 0.002

087E+01 3.31 4E-01 7.711 E+00 -0.000 0.006 0.001 592E+01 3.701 E-0

1

8 . 073E+00 -0 .000 0.006 0.001

0 46 E + 0

1

4 . 037E-0

1

8 . 380E+00 -0.000 0.005 0.001 458E+01 4.333E-01 8 . 646E+00 -0.000 0.005 0.001 184E+01 4.S28E-01 9.091 E+00 -0.000 0.004 0.001 808E+01 5 . 229E-0

1

9 . 454E+0 0 -0 .000 0.004 0.000

355E+01 5.562E-01 9. 762E+00 -0.000 0 .004 0.000 342E+01 5.843E-01 1 .003E+01 -0.000 0.003 0.000

282E+01 6 . 085E-0

1

1 . 026E+0

1

-0.000 0.003 0.000

681 E+01 6 . 296E-0

1

1 . 047E+O

1

-0.000 0.003 0.000 043E+01 6.482E-01 1 . 066E+01 -0 .000 0.003 0.000

337E+01 6 . 646E-0

1

1 . 084E+0

1

-0.000 0.003 0.000

9 96 E+0

1

6.926E-01 1 . 1 1 5E+01 -0 .000 0.003 0.000 053E+02 7.157E-01 1 . 141 E+01 -0.000 0.003 0 .000 101E+02 7.350E-01 1 . 1 65E+01 -0.000 0.002 0.000 144E+02 7.515E-01 1 . 186E+01 -0.000 0 . 002 0.000

2

35

68

1

12

2

3

4

5

67

9

1

12

2

3

9

68

1

1

1

122

2

33

4

578

1

1

1

1

2

2

22

3

394

5

678

9

1

1

1

1

122

2

2

33

34

4

55

6

67

7

88

99

9

I

1

1

141
ELECTRONS IN POLYPROPYLENE

I = 59.2 eV DENSITY = 9.000E-01 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log1 )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD COP.R. COLL CSDA RAD (DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2/g MeV cra 2 /g g/cra 2

0.0100 2 . 383E+0

1

2.883E-03 2 . 383E+0

1

2.366E-04 6 . 658E-05 0 . 0 -0.190 0.215 0.214

0.0125 2.000E+01 2.893E-03 2 . OOOE+O

1

3.516E-04 7.985E-05 0.0 -0.182 0.206 0.205

0.0150 1 . 733E+0

1

2. 900E-03 1 . 734E + 01 4.863E-04 9.254E-05 0 .

0

-0.177 0.198 0.198 0.0175 1 .536E+01 2.905E-03 1 . 536E+0

1

6 . 398E-04 1 .048E-04 0 . 0 -0.172 0.193 0.192

0.0200 1 . 384E+01 2.910E-03 1 . 384E+01 8.1 15E-04 1 . 1 67E-04 0 .

0

-0.168 0.188 0.187

0.0250 1 . 164E+01 2.919E-03 1 . 1 64E+01 1 . 207E-0 3 1 . 394E-04 0 . 0 -0.162 0.180 0.180 0.0300 1 .011E+01 2 . 929E-03 1 .012E+01 1 .669E-03 1 .61 2E-04 0.0 -0.158 0.175 0.174

0.0350 8. 995E+00 2.939E-03 8 . 998E+00 2.1 95E-03 1 . 822E-04 0 .0 -0.154 0.170 0.170

0.0400 8 . 1 36E+00 2.951E-03 8. 1 39E+00 2 . 780E-03 2 . 025E-04 0.0 -0.151 0.166 0.166

0.0450 7 . 454E+00 2. 963E-03 7 . 457E+00 3.422E-03 2 . 223E-04 0.0 -0.149 0.163 0.163

0.0500 6 . 900E+00 2. 976E-03 6 . 903E+00 4. 120E-03 2.415E-04 0.0 -0.146 0.161 0.160

0.0550 6 . 440E+00 2. 991 E-03 6 . 443E+00 4.870E-03 2.602E-04 0 . 0 -0.145 0.158 0.158

0.0600 6 . 052E+00 3 . 006E-03 6 . 055E+00 5.671 E-03 2.786E-04 0.0 -0.143 0.156 0.156 0.0700 5.433E+00 3.037E-03 5 . 436E+00 7.418E-03 3. 1 42E-04 0.0 -0.140 0.153 0.152

0.0800 4 . 960E+00 3.071 E-03 4 . 963E+00 9 . 347E-03 3.485E-04 0.0 -0 . 1 37 0.150 0.149

0.0900 4 . 588E+00 3.107E-03 4.591 E+00 1 . 144E-02 3.818E-04 0.0 -0.135 0.147 0.147

0.1000 4 . 287E+00 3. 145E-03 4 . 290E+00 1 . 370E-02 4.141E-04 0.0 -0.134 0.145 0.145

0.1250 3 . 7 38E+00 3.248E-03 3 . 74 1 E+00 1 . 997E-02 4.91 5E-04 0 . 0 -0.130 0.141 0.140

0.1500 3 . 367E+00 3.360 E-03 3 . 370E+00 2 . 703E-02 5.651 E-04 0.0 -0.127 0.138 0.137

0 . 1750 3.101E+00 3.478E-03 3. 105E+00 3.477E-02 6 . 357E-04 0.0 -0.125 0.135 0.134

0.2000 2. 902E+00 3.603E-03 2. 905E+00 4.310E-02 7 . 038E-04 0.0 -0.123 0.133 0.132

0.2500 2 . 624E+00 3 .872E-03 2 . 628E+00 6.126E-02 8. 345E-04 0.0 -0.119 0.129 0.128

0.3000 2 . 443E+00 4. 165E-03 2 . 447E+00 8.102E-02 9.601 E-04 0.0 -0.117 0.126 0.126 0.3500 2.31 7E+00 4.478E-03 2 . 322E+00 1 .020E-01 1 . 082E-03 0.0 -0.115 0.124 0.123

0.4000 2 . 225E+00 4.812E-03 2 . 229E+00 1 . 240E-0

1

1 . 202E-03 1 .122E-02 -0.091 0.121 0.119

0.4500 2 . 1 53E+00 5.163E-03 2.1 59E+00 1 . 468E-0

1

1 .322E-03 3. 973E-02 -0.085 0.116 0.113

0.5000 2.098E+00 5.531 E-03 2.1 04E+00 1 . 703E-0

1

1 . 440E-03 7.098E-02 -0.079 0.111 0.108

0.5500 2 . 055E+00 5.914E-03 2.061 E+00 1 .943E-01 1 . 559E-03 1 . 042E-01 -0 .074 0.107 0.103

0.6000 2 . 020E+00 6.310E-03 2 . 027E+00 2. 188E-01 1 . 679E-03 1 . 388E-01 -0.070 0.103 0.098

0.7000 1 . 969E+00 7.138E-03 1 . 976E+00 2.688E-01 1 .91 9E-03 2. 107E-01 -0.063 0.096 0.090

0.8000 1 . 934E+00 8 . 009E-03 1 . 942E+00 3.1 99E-01 2. 163E-03 2.841E-01 -0.057 0.090 0.083

0 . 9000 1 . 91 0E+00 8.91 9E-03 1 .91 9E+00 3.717E-01 2.409E-03 3 . 575E-01 -0.053 0.085 0.077

1 .0000 1 . 893E+00 9 . 867E-03 1 . 90 3E+00 4.240E-01 2.660 E-03 4.300E-01 -0.049 0.081 0.072

1 .2500 1 . 86 9E+00 1 . 233E-02 1 . 882E+00 5.563E-01 3.303E-03 6.045E-01 -0.043 0.072 0.063

1 .5000 1 .860E + 00 1 . 506E-02 1 . 876E+00 6.894E-01 3. 969E-03 7.670E-01 -0.039 0.066 0 .056

1 .7500 1 . 859E+00 1 .789E-02 1 . 877E+00 8.227E-01 4.656E-03 9.173E-01 -0.036 0.062 0.051 2.0000 1 .861E+00 2 . 084E-02 1 . 882E+00 9.557E-01 5.361 E-03 1 . 056E + 00 -0.034 0.058 0 .047 2.5000 1 .371 E + 00 2.706E-02 1 . 898E+00 1 . 220E+00 6 . 821 E-03 1 . 305E+00 -0.031 0.052 0.041 3.0000 1 .883E+00 3.361 E-02 1 . 917E+00 1 . 483E+00 8 . 332E-03 1 . 521 E+00 -0.029 0.048 0.037

3.5000 1 .396E+00 4 . 044E-02 1 . 936E+00 1 . 742E+00 9.886E-03 1 . 7 1 3E+00 -0.027 0.045 0 .035 4.0000 1 . 908E + 00 4.751 E-02 1 . 956E+00 1 . 999E+00 1 . 1 47E-02 1 . 885E + 00 -0.026 0.042 0.032

4.5000 1 . 920E+00 5.477E-02 1 . 975E+00 2 . 253E+00 1 .309E-02 2 . 040E+00 -0.025 0.040 0.031 5.0000 1 . 931 E+00 6 .222E-02 1 . 993E+00 2 . 505E+00 1 . 473E-02 2 . 1 83E+00 -0.024 0.039 0.029 5.5000 1 . 941 E+00 6 . 984E-02 2.01 1 E+00 2 . 755E+00 1 .639E-02 2.31 4E+00 -0.023 0.037 0.028

6.0000 1 . 951 E+00 7.759E-02 2 . 028E+00 3.003E+00 1 .806E-02 2 . 436E+00 -0.022 0.036 0 .027

7 .0000 1 . 968E+00 9. 348E-02 2 . 062E+00 3 . 492E+00 2. 145E-02 2 . 658E+00 -0.021 0 . 034 0.025

8.0000 1 . 983E+00 1 .098E-01 2 . 0 93E+00 3. 973E+00 2.488E-02 2 . 355E+0 0 -0.019 0.032 0 .024 9.0000 1 . 997E+00 1 .265E-01 2. 123E+00 4 . 447E+00 2.834E-02 3 . 033E + 00 -0.013 0.031 0.022

1 0 .0000 2 . 008E+00 1 . 435E-0

1

2.152E+00 4. 91 5E+00 3. 182E-02 3.1 96E+00 -0.017 0.029 0.021 12.5000 2 . 033E+00 1 .872E-01 2.221 E+00 5 . 059E+00 4.056E-02 3 . 553E+00 -0.014 0.026 0.018

15.0000 2 . 053E+00 2.322E-01 2 . 285E+00 7.168E+00 4.930E-02 3 . 856 E+0 0 -0.011 0.024 0.016

17.5000 2.06 9E + 00 2.782E-01 2 . 347E+00 8 . 248E+00 5 . 798E-02 4.122E+00 -0.009 0.022 0.014 20.0000 2 . 033E+00 3.249E-01 2. 408E+00 9 . 299E+00 6 . 65SE-02 4 . 357E+00 -0 .008 0.020 0.013

25.0000 2. 105E+00 4.202E-01 2 . 525E+00 1 . 1 33E+01 8.343E-02 4 . 762E+00 -0.005 0.018 0.010

30 .0000 2.1 23E+00 5.173E-01 2 . 640E+00 1 .326E+01 9.975E-02 5.101 E+00 -0.004 0.016 0.008

35.0000 2.1 37E+00 5.158E-01 2 . 753E+00 1 .512E+01 1 . 155E-01 5 . 392E+00 -0.003 0.014 0.007

40.0000 2.149E+00 7.1 53E-01 2.865E+00 1 . 6 90E+0

1

1 .307E-01 5 . 648E+00 -0.002 0.013 0 .006 45.0000 2 . 1 60 E+00 8.157E-01 2. 976E+00 1 .861E+01 1 .453E-01 5.875E+00 -0.002 0.012 0.005 50.0000 2. 170E+00 9. 169E-01 3 . 086E+00 2.026E+01 1 . 593E-0

1

6 . 079E+00 -0.002 0.011 0.004

55.0000 2. 178E+00 1 .01 9E + 00 3. 1 97E+00 2. 135E+01 1 .728E-01 6 . 265E+00 -0.001 0.010 0.004 60.0000 2. 186E+00 1 . 1 21 E+00 3 . 307E+00 2 . 339E+0

1

1 . 858E-0

1

6 . 435E+00 -0.001 0.010 0 .003 70.0000 2.200E+00 1 . 327E+00 3 . 527E+00 2.632E+01 2.1 04E-01 6 . 738E+00 -0.001 0.009 0 .003

80 .0000 2.211 E+00 1 . 535E+00 3 . 746E+00 2. 907E+01 2.333E-01 7.00! E+00 -0.001 0 . 005 0 .002 90.0000 2 . 222E+00 1 . 744E+00 3. 966E+00 3. 166E+01 2.546E-01 7 . 233E+00 -0.001 0.007 0 .002 100.0000 2.231 E+00 1 . 954E+00 4. 185E+00 3.412E+01 2.745E-01 7 . 442E+00 -0 .000 0.007 0.002

1 25 .0000 2 . 250E+00 2 . 483E+00 4 . 7 33E+0 0 3. 973E+01 3. 189E-01 7 . 884E+00 -0 .000 0.006 0.001 150.0000 2.266E+00 3.01 5E+00 5 . 282E+00 4.473E+01 3.572E-01 8 . 247E+00 -0.000 0.005 0.001 175.0000 2 . 280E+00 3.551 E+00 5.831 E+00 4 . 923E+01 3 . 905E-01 S.553E+00 -0.000 0.005 0.001 200.0000 2.291 E+00 4 . 089E+00 6 . 380E+00 5.333E+01 4 . 1 99E-01 8.81 9E+00 -0 .000 0.004 0.001 250.0000 2 . 31 0E+00 5. 171E+00 7 . 482E+00 6 . 056E+0

1

4.694E-01 9 . 264E+00 -0.000 0.004 0.001 300.0000 2. 326E+00 6 .259E+00 8 . 585E+00 6 . 679E+01 5.096E-01 9 . 628E + 0 0 -0.000 0.004 0.000

350.0000 2 . 33 9E+0 0 7 . 350E+00 9 . 689E+00 7.227E+01 5.432E-01 9. 936E+00 -0.000 0.003 0.000

400 .0000 2.351 E+00 3 . 444E+00 1 . 080E+0

1

7.716E+0I 5.716E-01 1 . 0 20E+0

1

-0.000 0.003 0.000 450.0000 2.361 E+00 9.541 E+00 1 . 1 90E+01 8 . 1 57E+01 5. 961E-01 1 . 044E+0

1

-0 .000 0.003 0 . 000 500.0000 2 . 370E+00 1 .064E+01 1 .301E+01 8 . 558E+0

1

6 . 175E-01 1 .065E+01 -0.000 0.003 0.000 550.0000 2 . 373E+00 1 . 174E+01 1 .412E+01 8 . 927E+01 6 . 364E-01 1 . 084E+0

1

-0.000 0.003 0.000 600.0000 2 . 386E+00 1 . 284E+01 1 . 523E+01 9 . 268E+0

1

6.531E-01 1 .101E+01 -0 .000 0.003 0 .000 700 .0000 2.399E+00 1 . 505E+0

1

1 .745E+01 9.881 E+01 6.817E-01 1 . 1 32E+01 -0.000 0.002 0.000 800.0000 2.411 E+00 1 . 726E+0

1

1 . 967E+01 1 . 042E+02 7.053E-01 1 .159E+01 -0.000 0.002 0.000 900.0000 2.421 E+00 1 . 947E+0

1

2. 189E+01 1 . 090E+02 7.251E-01 1 .182E+01 -0.000 0.002 0.000 1000.0000 2 . 430E+00 2. 1 69E+01 2.412E+01 1 . 1 34E+02 7.421E-01 1 . 203E+0

1

- 0.000 0.002 0.000

140
ELECTRONS IN POLYVINYL CHLORIDE

I = 108.2 eV DENSITY = 1 . 300E+OCl g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2/g g/cm 2 0.0100 1 . 930E+01 5. 953E-03 1 . 930E+01 2 . 974E-04 1 . 61 7E-04 0 .

0

-0.214 0.249 0.245 0.0125 1 .628E+01 6 . 1 06E-03 1 . 629E+0

1

4.390E-04 1 . 977E-04 0.0 -0.205 0.236 0.232

0.0150 1 .416E+01 6.218E-03 1 .417E+01 6.041E-04 2 . 326E-04 0 . 0 -0.198 0.227 0.223

0.0175 1 .259E+01 6 .302E-03 1 . 260E+0

1

7.916E-04 2 . 665E-04 0 .0 -0.192 0.219 0.216 0.0200 1 . 1 37E+01 6.369E-03 1 . 1 38E + 01 1 . 00 1 E-03 2. 995E-04 0.0 -0.187 0.213 0.210 0.0250 9.601 E+00 6 . 468E-0 3 9 . 608E+00 1 .481 E-03 3 . 630E-04 0 .

0

-0.180 0.203 0.201 0.0300 8 . 370E+00 6 .539E-03 8 . 377E+0 0 2.040E-03 4.237E-04 0 .

0

-0.174 0.196 0 . 1 94 0.0350 7 . 462E+00 6 . 595E-03 7 . 468E+00 2.673E-03 4.821 E-04 0.0 -0.170 0.190 0.189

0.0400 6 . 762E+00 6 . 641 E-03 6 -769E+00 3.378E-03 5 . 384E-04 0.0 -0.166 0.186 0.184

0.0450 6 . 20SE+00 6.631 E-03 6.213E+00 4 . 1 50E-03 5. 92SE-04 0 .

0

-0.163 0.182 0.180 0.0500 5 . 753E+00 6.717E-03 5 . 759E+00 4. 987E-03 6 . 457E-04 0.0 -0.161 0.178 0.177

0.0550 5 . 37 6 E + 0 0 6.751 E-03 5 . 383E + 00 5.885E-03 6 . 970E-04 0.0 -0.158 0.175 0.174

0.0600 5 . 058E+00 6.783E-03 5 . 065E+00 6.844E-03 7.470E-04 0.0 -0.156 0.173 0.172

0.0700 4 . 549E+00 6 .846E-03 4 . 556E+00 8 . 930E-03 8.434E-04 0 .

0

-0.153 0.168 0.168

0.0300 4. 160E+00 5 . 908E-03 4 . 1 67E+00 1 . 1 23E-02 9 . 356E-04 0.0 -0.150 0.165 0.164

0.0900 3 . 853E+00 6 .972E-03 3.860E+00 1 . 372E-02 1 . 024E-0 3 0.0 -0.147 0.162 0.161 0.1000 3 . 604E+00 7.040E-03 3.61 1 E+00 1 . 641 E-02 1 . 1 1 0E-03 0.0 -0.145 0.159 0.159 0.1250 3.150E+00 7.222E-03 3. 1 57E+00 2 . 384E-02 1 .31 2E-03 0.0 -0.141 0.154 0.153

0 . 1 500 2.843E+00 7.424E-03 2.851 E+00 3.21 9E-02 1 .501 E-03 0.0 -0.138 0.150 0.149

0.1750 2 . 623E+00 7.642E-03 2. 630E+00 4. 134E-02 1 . 680E-03 0.0 -0.135 0.147 0.146

0.2000 2 . 457E+00 7 . 877E-03 2.465E+00 5.11 7E-02 1 . 852E-03 0.0 -0.132 0.144 0.144

0.2500 2 . 227E+00 8. 337E-03 2 . 235E+00 7 . 254E-02 2.17 6 E-0 3 0.0 -0.129 0.140 0.139

0.3000 2 . 077E+00 8 . 949E-03 2 . 086 E+00 9 . 575E-02 2 . 484E-03 0.0 -0.126 0.137 0.136 0.3500 1 . 972E+00 9 . 554E-03 1 . 982E+00 1 . 204E-0

1

2.780E-03 0.0 -0.123 0.134 0.133

0.4000 1 . 896 E + 0 0 1 . 020E-02 1 .907E+00 1 .461 E-0

1

3 . 063E-03 7 . 976E-03 -0.102 0.131 0.129

0.4500 1 . 838E+00 1 . 088E-02 1 . 84 9E+00 1 . 728E-0

1

3.351 E-0 3 3 . 082E-02 -0.097 0.126 0.124

0.5000 1 . 7 93E+0 0 1 .159E-02 1 . 805E+00 2. 001 E-01 3.631 E-03 5 . 539E-02 -0.092 0.122 0.119

0.5500 1 . 7 58E + 0 0 1 . 233E-02 1 . 770E+00 2.281 E-01 3.9! 0E-03 8.121 E-02 -0.088 0.118 0.114

0 .6000 1 . 730E+00 1 . 31 0E-02 1 . 743E+00 2 . 566 E-0

1

4. 187E-03 1 .079E-01 -0.084 0.114 0.110

0.7000 1 . 690E+00 1 .469E-02 1 . 704E+00 3.147E-01 4.741 E-0 3 1 . 629E-0

1

-0.078 0.108 0.103

0.8000 1 . 663E+00 1 . 637E-02 1 . 679E+00 3 . 738E-0

1

5 . 296E-03 2. 189E-01 -0 .073 0.103 0.097

0 . 9000 1 . 645E+00 1 .81 3E-02 1 . 663E+00 4 . 337E--0 1 5.855E-03 2 . 747E-0

1

-0.069 0.098 0.092

1 .0000 1 . 633E+00 1 . 995E-02 1 . 653E+00 4. 940E-01 6.418E-03 3.299E-01 -0.066 0.094 0.087

1 .2500 1 . 6 1 8E+00 2 . 476E-02 1 . 643E+00 6 . 458E-0

1

7 . 846 E-0 3 4 . 627E-0

1

-0.060 0.087 0.078

1 .5000 1 .615E+00 2. 990E-02 1 . 645E+00 7 . 980E-01 9 . 308E-03 5.867E-01 -0.056 0.081 0.072

1 .7500 1 . 6 1 8E+00 3 . 530E-02 1 . 653E+00 9 . 496E-0

1

1 . 080E-02 7.018E-01 -0.053 0.077 0.067

2.0000 1 . 623E+00 4.092E-02 1 . 664E+00 1 . 1 00E + 00 1 . 23 2 E-0

2

S.087E-01 -0.051 0.073 0.063

2.5000 1 . 638E+00 5 . 270E-02 1 . 690E+00 1 . 399E + 00 1 . 543E-0 2 1 .001 E+00 -0.047 0.068 0.057 3.0000 1 . 653E+00 S.507E-02 1 .718E+00 1 . 6 92E+0 0 1 .861 E-02 1 . 170E+00 -0.044 0.064 0.053 3.5000 1 . 66 9E+00 7.791 E-02 1 . 747E+00 1 . 981 E+00 2. 184E-02 1 . 32 1 E+00 -0.042 0.060 0.050 4.0000 1 . 683E+00 9.11 4E-02 1 . 774E+00 2 . 265E+00 2.511 E-02 1 . 458E+00 -0.040 0 .058 0.048 4.5000 1 . 6 96 E+0 0 1 .047E-01 1 .301 E+00 2 . 544E+00 2.841 E-02 1 . 583E+00 -0.039 0.055 0 .045 5.0000 1 . 708E+00 1 . 186E-01 1 . 327E+00 2 . 820E+00 3. 172E-02 1 . 6 99E+00 -0.037 0.054 0 .044 5.5000 1 . 720E+00 1 . 327E-0

1

1 . 853E+00 3 . 0 92E+00 3.504E-02 1 . 807E+00 -0.036 0.052 0 .042 6.0000 1 . 730E+00 1 .471E-01 1 . 377E+00 3 . 360E+00 3 . 837E-02 1 . 903E+00 -0.034 0.050 0 .040 7.0000 1 .749E+00 1 . 764E-0

1

1 . 925E+00 3 . 836E+00 4.503E-02 2 . 0 95E+00 -0.031 0.048 0.037 3.0000 1 .765E+00 2.065E-01 1 . 971 E+00 4 . 399E+00 5 . 1 68E-02 2 . 264E + 00 -0.029 0.045 0.035

9.0000 1 . 779E+00 2. 371 E-0

1

2.01 6E+00 4.901 E+00 5 . 830 E-0 2 2 . 420E+00 -0.027 0.043 0.033

10.0000 1 .791 E+00 2 . 683E-0

1

2 . 060 E+00 5.391 E+00 6 . 486E-02 2 . 564E+00 -0.024 0.041 0.031 12.5000 1 .81 7E+00 3.479E-01 2 . 1 65E+00 6 . 575E+00 8.101 E-02 2 . 888E+00 -0.020 0.037 0.026

15.0000 1 . 837E+00 4.295E-01 2.266E+00 7 . 704E+00 9 . 672E-02 3. 168E + 00 -0.017 0.034 0.023

17.5000 1 . 353E+00 5. 127E-01 2 . 366E+00 8 . 783E+00 1.11 9E-01 3.41 5E+00 -0.014 0.031 0.020

20 .0000 1 . S66E+00 5.971 E-0

1

2 . 464E+00 9.81 9E+00 1 . 267E-0

1

3 . 6 36 E+0 0 -0.012 0.029 0.018 25.0000 1 . 889E+00 7.686E-01 2 . 657E+00 1 . 177E+01 1 . 546 E-0

1

4.01 7E+00 -0.010 0 .026 0.015

30.0000 1 . 906E+00 9.428E-01 2 . 84 9E + 0 0 1 . 359E+0

1

1 . 806 E-0

1

4 . 337E+00 -0.009 0.023 0.012

35.0000 1 . 921 E+00 1.11 9E+00 3 . 040E+00 1 .529E+01 2.048E-01 4.61 3E+00 -0.007 0.021 0.011 40.0000 1 . 933E+00 1 . 297E+00 3 . 230E+00 1 . 688E+0

1

2 . 273E-0

1

4 . 854E+00 -0.007 0.019 0.009 45.0000 1 .94&E+00 1 . 476 E + 0 0 3 . 420 E+00 1 . 839E+0

1

2.484E-01 5.069E+00 -0.006 0.018 0.008 50.0000 1 . 953E+00 1 . 657E+00 3.61 0E+00 1 . 981 E+01 2.631 E-0

1

5 . 263E+00 -0.006 0.017 0.007 55.0000 1 . 962E+00 1 . 8 38E + 0 0 3.800E+00 2.11 6E+01 2.866 E-0

1

5 . 440E+00 -0.005 0.016 0.007 60.0000 1 . 969E+00 2 . 020E+00 3 . 990E+00 2.244E+01 3.040E-01 5 . 602E+00 -0.005 0.015 0 . 006 70.0000 1 . 983E+00 2 . 387E+00 4.370 E+00 2 . 484E+0

1

3 . 358 E-0

1

5 . 890E+00 -0.005 0.014 0.005 80.0000 1 . 995E+00 2 . 756E+00 4.750E+00 2.703E+01 3 . 643E-01 6 . 1 42E+00 -0 .004 0.013 0.005

90.0000 2 . 005E+00 3. 127E+00 5.1 32E+00 2. 906E+01 3.899E-01 6 . 365E+00 -0.004 0.012 0.004 100.0000 2.014E+00 3 . 4 99E + 0 0 5.51 3E+00 3.094E+01 4 . 1 32E-01 6 . 56 6 E+0 0 -0.003 0.012 0.004

125.0000 2 . 033E+00 4 . 436E+00 6.469E+00 3.512E+01 4.628E-01 6 . 995E+00 -0.003 0.010 0.003 150.0000 2 . 048E+00 5.379E+00 7 . 427E+00 3 . 872E+0

1

5.033E-01 7 . 348E+00 -0.002 0.010 0.002

175.0000 2.061 E+00 6 . 326E+00 8 . 386E+00 4. 189E+01 5.371 E-0

1

7 . 649E+00 -0.002 0.009 0.002 200.0000 2 . 072E+00 7 . 27 6 E+0 0 9. 347E+00 4.471E+01 5.658E-01 7 . 9 1 0 E+0 0 -0.001 0 .008 0.002 250.0000 2 . 0 90E+00 3. 185E+00 1 . 127E+01 4 . 958E+0

1

6. 122E-01 3.349E+00 -0.001 0 . 008 0.001 300.0000 2.1 04E+00 1 . 1 10E+01 1 .321E+01 5 . 367E+0

1

6 .482E-01 8.71 0E+00 -0.001 0 .007 0.001 350.0000 2.117 E+00 1 . 302E+01 1 .514E+01 5.720E+01 6 .771 E-01 9 . 01 5E+00 -0.001 0.007 0.001 400.0000 2.127E+00 1 . 495E+01 1 . 708E+0

1

6.031 E+0

1

7.010 E-01 9.281 E+00 -0.000 0.006 0.001 450.0000 2.1 37E+00 1 . 638E+01 1 .901E+01 6 . 308E+0

1

7.21 IE-01 9.51 5E+00 -0.000 0.006 0.001 500.0000 2. 145E+00 1 .881E+01 2. 095E+01 6 . 559E+0

1

7 . 383E-0

1

9 . 725E+00 -0 .000 0.006 0.001 550.0000 2. 153E+00 2.074E+01 2.289E+01 6 . 787E+0

1

7.53! E-01 9.91 5E+00 -0.000 0 .006 0.001 600.0000 2. 159E+00 2 . 263E+0

1

2 . 484E+0

1

6.397E+01 7.662E-01 1 .009E+01 -0.000 0.005 0.001 700.0000 2. 172E+00 2 . 655E+0

1

2 . 872E+0

1

7.371 E+01 7 . 380 E-0

1

1 . 0 40 E+0

1

-0.000 0.005 0 . 000 300.0000 2. 182E+00 3 . 043E+0

1

3.261 E+01 7.697E+01 8 . 056 E-0

1

1 . 066E+01 -0 .000 0.005 0 .000 900.0000 2.1 91 E+00 3.431E+01 3 . 650E+01 7.937E+01 8.202E-01 1 . 0 90 E+0

1

-0 .000 0.005 0.000 1000.0000 2 . 200E+00 3 . 820E+0

1

4 . 040E+0

1

8 . 247E+0

1

3.324E-01 1 . 1 1 1 E+01 -0.000 0.005 0.000

143
ELECTRONS IN PROPANE

I = 47.1 eV DENSITY = 1.879E-03 g/cm 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( logi )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD COP.R

.

COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 2.618E+01 2 . 752E-03 2.618E+01 2.142E-04 5.755E-05 0.0 -0.182 0.205 0.204

0.0125 2.1 94E+01 2.762E-03 2.1 94E+01 3. 189E-04 6.916E-05 0.0 -0.175 0.196 0.195

0.0150 1 . 899E+0

1

2.769E-03 1 .899E+01 4.418E-04 8.028E-05 0.0 -0.170 0.189 0.189

0.0175 1 .681E+01 2 . 774E-0 3 1 . 681 E+01 5 . 820E-04 9.102E-05 0.0 -0.165 0.184 0.184

0.0200 1 .513E+01 2.779E-03 1 .514E+01 7 . 390E-04 1 . 0 1 4E-04 0.0 -0.162 0.180 0.179

0.0250 1 .271 E+01 2.789E-03 1 .271E+01 1 . 101E-03 1 .215E-04 0.0 -0.156 0.173 0.173

0.0300 1 . 103E+01 2.799E-03 1 . 104E+01 1 . 525E-0 3 1 . 407E-04 0.0 -0.152 0.168 0.167

0.0350 9.806E+00 2.310E-03 9 . 808E+00 2.006E-03 1 . 592E-04 0.0 -0.149 0.164 0.163

0.0400 8.86IE+00 2.821E-03 8 . 865E+00 2. 543E-03 1 .771 E-04 0 .

0

-0.146 0.160 0.160 0.0450 8. 1 16E+00 2.334E-03 8.11 9E+00 3.133E-03 1 . 945E-04 0.0 -0.144 0.157 0.157

0.0500 7.509E+00 2.847E-03 7.51 1 E+00 3.774E-03 2.114E-04 0.0 -0.142 0.155 0.155

0.0550 7 . 005E+00 2.861E-03 7.008E+00 4.464E-03 2.280E-04 0 .

0

-0.140 0.153 0.152

0.0600 6 . 580E+00 2 . 876E-03 6 . 583E+00 5.201E-03 2.442E-04 0.0 -0.138 0.151 0.150

0.0700 5. 903E+00 2.907E-03 5 . 906E+00 6 . 808E-0 3 2. 757E-04 0 .

0

-0.136 0.1^7 0.147

0.0800 5 . 387E+00 2. 940E-03 5. 390E+00 3.583E-03 3.061 E-04 0.0 -0.133 0.145 0.144

0.0900 4. 980E+00 2. 975E-03 4. 983E+00 1 .051E-02 3 . 356E-04 0.0 -0.131 0.142 0.142

0.1000 4 . 652E+00 3.013E-03 4 . 655E+00 1 . 259E-02 3 . 643E-04 0.0 -0.130 0.140 0.140

0.1250 4 . 052E+00 3.114E-03 4 . 056E+00 1 . 837E-02 4 . 330 E-04 0.0 -0.126 0.136 0.136

0.1500 3 . 648E+00 3 . 222E-03 3 . 652E+00 2.438E-02 4. 984E-04 0.0 -0.123 0.133 0.133

0.1750 3 . 358E+0 0 3.338E-03 3 . 362E+00 3 . 203E-02 5.61 2E-04 0.0 -0.121 0.131 0.130 0.2000 3.141 E+00 3.460E-03 3. 144E+00 3. 973E-02 6.21 9E-04 0.0 -0.119 0.129 0.128

0.2500 2 . 839E + 00 3.722E-03 2 . 842E+00 5.651E-02 7.386E-04 0 .

0

-0.116 0.125 0.125

0.3000 2 . 64 1 E+00 4.007E-03 2 . 645E+00 7 . 479E-02 8.509E-04 0.0 -0.114 0.123 0.122

0.3500 2 . 504E+00 4.31 IE-03 2 . 508E + 0 0 9 . 423E-02 9 . 603E-04 0.0 -0.112 0.121 0.120 0.4000 2 . 404E+00 4 . 635E-03 2.409E+00 1 . 1 46E-0

1

1 . 068E-03 0.0 -0.110 0.119 0.118

0.4500 2 . 330E+00 4. 976E-03 2 . 335E+00 1 . 357E-0

1

1 . 174E-03 0.0 -0.108 0.117 0.116

0.5000 2 . 274E+00 5.334E-03 2 . 279E+00 1 .574E-01 1 .281E-03 0.0 -0.107 0.116 0.115

0.5500 2 . 230E+00 5 . 705E-03 2 . 236E+00 1 . 795E-0

1

1 . 386E-03 0.0 -0.106 0.115 0.113

0.6000 2.1 96E+00 6 .089E-03 2 . 202E+00 2.021E-01 1 . 492E-03 0.0 -0.105 0.114 0.112

0.7000 2. 147E+00 6.894E-03 2. 154E+00 2.480E-01 1 . 705E-03 0.0 -0.103 0.112 0.110

0.8000 2. 116E+00 7 . 739E-03 2. 124E+00 2. 948E-01 1 . 920E-03 0 .0 -0.101 0.110 0.108

0 . 9000 2 . 0 96E+0 0 8.623E-03 2.105E+00 3.421E-01 2.1 37E-03 0.0 -0.100 0.109 0 . 1 06

1 .0000 2 . 084E+00 9.544E-03 2 . 0 94E+00 3.898E-01 2 . 356E-03 0.0 -0.098 0.107 0.105

1 .2500 2 . 073E+0 0 1 . 1 98E-02 2 . 085E+00 5.095E-01 2. 91 4E-03 0.0 -0.095 0.105 0.102

1 .5000 2 . 078E+00 1 .459E-02 2 . 0 92E+00 6 . 293E-01 3.488E-03 0.0 -0.093 0.103 0.099

1 .7500 2 . 088E+00 1 . 7 34E-0 2 2 . 1 06E+00 7 . 484E-0

1

4 . 075E-03 0.0 -0.091 0.101 0.0 97 2.0000 2. 1 03E+00 2.021E-02 2 . 1 23E+00 8.666E-01 4 . 675E-03 0.0 -0.090 0.099 0.096

2.5000 2 . 1 34E+00 2.626E-02 2 . 1 60E+00 1 . 1 00E+00 5. 907E-03 0.0 -0.087 0.097 0.093

3.0000 2. 166E+0C 3.263E-02 2.1 99E+00 1 . 330E+00 7.171 E— 0 3 0.0 -0.086 0.095 0.090

3.5000 2.1 96E+00 3 . 928E-02 2 . 235E+00 1 . 555E+00 8 . 462E-03 0.0 -0.084 0.093 0.088

4.0000 2 . 224E+00 4.616E-02 2 . 270E+00 1 . 777E+00 9.772E-03 0.0 -0 . 083 0.092 0 . 087 4.5000 2 . 250E+00 5 . 323E-02 2 . 304E+00 1 . 996E+00 1 . 1 1 0E-02 0.0 -0.081 0.091 0.085

5.0000 2 . 274E+00 6 . 049E-02 2 . 335E+00 2.21 1 E+00 1 .244E-02 0.0 -0.080 0.089 0.084

5.5000 2 . 297E+00 6.790E-02 2 . 365E+00 2 . 424E+00 1 . 379E-02 0 .

0

-0.080 0.088 0.083

6.0000 2.31 8E+00 7 . 546E-02 2 . 393E+00 2 . 634E+00 1 .51 5E-02 0.0 -0.079 0.087 0.C82

7.0000 2 . 356E+00 9.094E-02 2 . 447E+00 3 . 047E+00 1 . 790E-02 0.0 -0.077 0.086 0 .080 8.0000 2. 389E+00 1 . 063E-01 2 . 496E+00 3 . 452E+0 0 2.066E-02 0.0 -0.076 0.084 0.079

9.0000 2.41 9E+00 1 -231E-01 2 . 542E+00 3.S49E+00 2 . 343E-02 0.0 -0.075 0.083 0 . 077

1 0.0000 2 . 446E+00 1 . 397E-0

1

2 . 536 E+00 4 . 239E+00 2.621E-02 0.0 -0 .074 0.082 0.076 12.5000 2.505E+00 1 . 323E-0

1

2 . 637E+00 5 . 1 87E+00 3.31 6E-02 0.0 -0.073 0.080 0.073

15.0000 2.551 E+00 2.262E-01 2 . 777E+00 6 . 102E+00 4.007E-02 1 . 733E-02 -0.061 0.077 0.070

17.5000 2 . 586E+00 2.710E-01 2 . 857E+00 6 . 989E+00 4 . 695E-02 8.510E-02 -0.049 0.074 0.065

20 .0000 2.61 3E+00 3.1 67E-01 2. 930E+00 7.853E+00 5.376E-02 1 .770E-01 -0.041 0.070 0.059 25.0000 2 . 655E+00 4.097E-01 3 . 064E+00 9.521 E+00 6.721E-02 3.825E-01 -0.032 0.063 0.049

30.0000 2 . 685E+00 5 . 045E-0

1

3.1 90E+00 1 . 1 12E+01 8.035E-02 5.859E-01 -0.027 0 .058 0.042

35 .0000 2.71 OE+OO 6 . 007E-01 3.31 OE+OO 1 . 266E+0

1

9.31 4E-02 7.756E-01 -0.024 0.053 0.036 40.0000 2 . 730 E+00 6.979E-01 3 . 428E+00 1 .414E+01 1 . 056E-0

1

9.500E-01 -0.022 0.050 0.032

45.0000 2 . 747E+00 7 . 960E-01 3 . 543E + 00 1 . 558E+0

1

1 . 176E-01 1 .1 1 OE+OO -0 .020 0.047 0.029

50.0000 2 . 763E+00 3. 948E-01 3 . 657E+00 1 . 6 97E+0

1

1 . 294E-0

1

1 . 257E+00 -0.019 0.044 0.026 55.0000 2 . 776E + 00 9.944E-01 3 . 770E + 00 1 .831E+01 1 . 407E-0

1

1 . 393E+00 -0.018 0.042 0.024

60.0000 2 . 788E+00 1 . 094E+00 3 . 88 3E+0 0 1 . 962E+0

1

1 .517E-01 1 .51 9E+00 -0.017 0.040 0 . 023 70.0000 2.309E+00 1 . 296E+00 4. 105E+00 2.212E+01 1 . 728E-0

1

1 . 746E+00 -0.016 0.037 0.020 80.0000 2 . 828E + 00 1 . 499E+00 4 . 326E+00 2 . 450E+01 1 . 926E-01 1 . 946E+00 -0.015 0.034 0.018 90.0000 2 . 843E + 00 1 . 70 3E + 00 4 . 546E+00 2 . 675E+0

1

2.113E-01 2 . 1 25E+00 -0.015 0.032 0.016 100.0000 2.857E+00 1 . 909E+00 4 . 766E+00 2 . 890E+0

1

2.289E-01 2 . 287E+00 -0.014 0.030 0.015

125.0000 2 . 386E + 00 2 . 426E+00 5.31 2E+00 3. 336E+01 2.690E-01 2 . 637E+00 -0.013 0.027 0.013

150.0000 2. 909E+00 2 . 947E+00 5 . 856E + 00 3 . 835E+0

1

3 . 043E-0

1

2. S28E+00 -0.012 0.025 0.011 175.0000 2. 928E + 00 3.471 E+00 5 . 399E+00 4.243E+01 3 . 356E-01 3 . 1 80 E+00 -0.011 0.023 0.010 200.0000 2. 944E+00 3. 998E+00 6 . 942E + 00 4.618E+01 3.636E-01 3 . 402E+00 -0.010 0.021 0.009

250 . 0000 2. 970E+00 5 . 056E+00 8 . 027E+00 5 . 287E+0

1

4 . 1 17E-01 3 . 733E + 00 -0.008 0.019 0.007

300.0000 2. 991 E+00 6 . 1 21 E+00 9.111 E+00 5 .871 E+01 4.517E-01 4 . 1 03E+00 -0.007 0.017 0.006

350.0000 3 . 008E+00 7. 189E+00 1 . 020E+0

1

6 . 390E+01 4.856E-01 4 . 381 E+00 -0.005 0.016 0.005 400.0000 3 . 022E+00 8 . 260E+00 1 . 128E+01 6 . 856E+0

1

5.148E-01 4 . 626E+00 -0.005 0.015 0.005 450.0000 3.034E+00 9.334E+00 1 . 237E+0

1

7.279E+01 5.402E-01 4 . 845E+00 -0.004 0.014 0.004 500.0000 3 . 044E+00 1 .041E+01 1 . 345E+0

1

7 . 666E+01 5 . 626E-0

1

5 . 044E+00 -0.003 0.014 0.004 550.0000 3 . 0 54E + 00 1 . 149E+01 1 . 454E+0

1

3.024E+01 5.826E-01 5 . 225E+00 -0.003 0.013 0.003 600.0000 3 . 062E+00 1 . 257E+0

1

1 , 563E+9

1

3. 355E+0

1

6 . 005E-0

1

5. 392E+00 -0.902 0.013 0.003 700.0000 3 . 077E+00 1 . 473E+0

1

1 .781E+01 8. 954E+01 6 . 31 3E-01 5 . 689E+00 -0.002 0.012 0.003 800.0000 3 . 0 90 E+0 0 1 . S3 9E+0

1

1 . 998E+01 9 . 434E+0

1

6 .569E-01 5 . 949E+00 -0.001 0.011 0.002 900.0000 3.101 E+00 1 . 906E+01 2.216 E+01 9. 959E+01 6 . 787E-0

1

6 . 1 SOE+OO -0.001 0.011 0 .002 1000.0000 3.111 E+00 2.1 23E+01 2.434E+01 1 . 039E+02 6.975E-01 6 . 387E+00 -0.001 0.010 0.002

144
ELECTRONS IN SILICON DIOXIDE

I = 139.2 eV DENSITY = 2 . 320E+00' g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DEHS.EFF. cK log )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORK. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2 /g MeV cm 2/g g/cm 2 0.0100 1 . 780E+0

1

5.669E-03 1 .781 E+01 3.255E-09 1 .71 6E-09 0.0 -0.227 0.267 0.263 0.0125 1 . 506E+0

1

5.762E-03 1 . 506E+0

1

9.78SE-09 2 . 079E-09 0.0 -0.216 0.252 0.298

0.0150 1 -313E+0! 5 . 830E-0 3 1 . 31 3E+01 6 . 570E-09 2.91 7E-09 0 .

0

-0.208 0.291 0.238 0.0175 1 . 169E+01 5.380E-03 1 . 1 69E+01 8.592E-09 2.799E-09 0 .

0

-0 . 202 0.232 0.230 0.0200 1 . 0 57E + 0

1

5.913E-03 1 . 057E+0

1

1 . 089E-03 3.06 9E-09 0.0 -0.196 0.225 0.223

0.0250 3. 939E+00 5 . 971 E-03 8 . 995E+00 1 .601 E-03 3.689E-09 0 . 0 -0.188 0.215 0.213

0.0300 7 . 809E+00 6 . 009E-03 7.31 0E+00 2.201 E-03 9.268E-09 0.0 -0.182 0.207 0.205

0.0350 6 . S65E+00 6 .039E-03 6 . 371 E+00 2.880E-03 9.327E-09 0.0 -0.177 0.200 0.199

0 .0400 6.31 8E+00 6 . 065E-03 5 . 329E+00 3.639E-03 5 . 365E-09 0 . 0 -0.179 0.195 0.199

0 .04 50 5 . 803E+00 5 .089E-03 5 . 809E+00 9.960E-03 5 . 889E-09 0 .0 -0.170 0.191 0.190 0.0500 5 . 383E+00 6.112E-03 5 . 389E+00 5.355E-03 6 . 387E-09 0 .0 -0.167 0.187 0.186

0.0550 5 . 033E+00 6 . 1 35E-03 5 . 090E+00 6.315E-03 6 .876E-09 0.0 -0.165 0.189 0.183

0 .0600 9 . 738E+00 6 . 1 59E-03 9 . 799E+00 7.338E-03 7 .351 E-09 0.0 -0.163 0.181 0.180

0.0700 9.265E+00 6.207E-03 9.271 E+00 9.569E-03 3.267E-09 0.0 -0.159 0.176 0.175

0.0800 3. 909E+00 6 . 25 9E-0 3 3.91 0E+00 1 .201 E-02 9 . 1 93E-09 0.0 -0.156 0.172 0.172

0.0900 3.61 8E+00 6.315E-03 3 . 629E+00 1 . 967E-02 9.985E-09 0.0 -0.153 0.169 0.168

0.1000 3 . 386E+00 6.375E-03 3 . 393E+00 1 . 753E-02 1 .080E-03 0.0 -0.151 0.166 0.165

0.1250 2. 963E+00 6.591E-03 2.969E+00 2. 599E-02 1 . 272E-03 0.0 -0.196 0.160 0.160

0 . 1 500 2 . 677E+00 6.727E-03 2 . 683E+00 3 . 932E-02 1 . 953E-03 0.0 -0.192 0.156 0.156

0.1750 2.971E+00 6 . 930E-03 2 . 978E+00 9 . 903E-02 1 . 6 29E-03 0.0 -0.190 0.153 0.152

0.2000 2.31 6E+00 7 . 1 98E-03 2.323E+00 5.996E-02 1 . 7 8 9E-0 3 0.0 -0.137 0.150 0.199

0.2500 2. 1 01 E+00 7.622E-03 2. 1 09E+00 7.713E-02 2. 100E-03 0.0 -0.133 0.195 0.199

0 .3000 1 . 961 E+00 3 . 1 99E-03 1 . 969E+00 1 .017E-01 2.396E-03 0.0 -0.130 0.192 0.191 0.3500 1 . 36 9E + 00 8.706E-03 1 . 872E+0 0 1 . 278E-0

1

2.682E-03 0.0 -0.125 0.139 0.138

0.9000 1 . 792E+00 9 . 309E-03 1 .801 E+00 1 . 550E-0

1

2.960E-03 1 . 399E-02 -0.110 0.135 0.133

0.9500 1 . 73SE+00 9. 935E-03 1 . 7 98E + 00 1 .832E-01 3 . 233E-03 3 . 1 75E-02 -0.109 0.130 0.128

0.5000 1 . 6 97E+00 1 . 060E-02 1 . 708E+00 2. 122E-01 3 . 509E-03 5.190E-02 -0.100 0.126 0.123

0.5500 1 . 665E+00 1 . 1 28E-02 1 . 676E+00 2.917E-01 3.779E-03 7.393E-02 -0.096 0.123 0.119

0.6000 1 . 639E+00 1 . 1 99E-02 1 . 651 E+00 2.718E-01 9.092E-03 9 . 597E-02 -0.092 0.119 0.116 0.7000 1 . 603E+00 1 . 398E-02 1 .61 6E+00 3.331E-01 9.579E-03 1 .931E-01 -0.086 0.119 0.109

0.8000 1 . 579E+00 1 .509E-02 1 . 599E+00 3.959E-01 5.1 18E-03 1 . 91 9E-01 -0.081 0.109 0.103

0 . 9000 1 . 56 3E + 00 1 . 667E-02 1 . 57 9E+00 9.585E-01 5.659E-03 2.913E-01 -0.076 0.109 0.098

1 . 0000 1 . 552E+00 1 . 836E-02 1 . 570E+00 5.220E-01 6 . 20 6 E-03 2. 907E-01 -0.073 0.101 0.099

1 .2500 1 . 590 E+0 0 2 . 283E-02 1 . 563E+00 6.81 7E-0

1

7.593E-03 9.1 18E-01 -0.066 0.093 0.085

1 .5000 1 . 538E+0 0 2.761E-02 1 . 566E+00 8.916E-01 9.013E-03 5.276E-01 -0.061 0 . 087 0.078

1 .7500 1 . 592E + 0 0 3.269E-02 1 . 575E+00 1 1 0 0 1 E + 00 1 . 096E-02 6 . 371 E-01 -0.057 0.083 0 .073 2.0000 1 . 598E+00 3 . 787E-02 1 . 586E+00 1 . 159E+00 1 . 1 99E-02 7.905E-01 -0.059 0.079 0.068

2.5000 1 . 563E+00 9.886E-02 1 . 6 1 2E+00 1 . 972E+00 1 . 997E-02 9.306E-01 -0.099 0.072 0.061 3.0000 1 . 573E+00 6 . 039E-02 1 . 639E+00 1 . 7S0E+00 1 .807E-02 1 . 102E+00 -0.095 0.068 0.056

3.5000 1 . 593E+00 7.238E-02 1 . 665E+00 2 . 082E+00 2. 123E-02 1 . 253E+00 -0.091 0.069 0.052 9.0000 1 . 606E+00 8 . 975E-02 1 . 6 9 1 E+00 2. 380E+00 2.992E-02 1 . 902E+00 -0.038 0.061 0.099

9.5000 1.61 9E+00 9.793E-02 1 . 7 1 6E+00 2 . 6 79E+0 0 2.76 5E-0 2 1 . 535E+00 -0.036 0.058 0.096 5.0000 1 . 630E+00 1 . 1 09E-01 1 .791 E+00 2 . 963E+00 3 . 0S9E-02 1 . 659E+00 -0.039 0.055 0.093

5.5000 1 . 691 E+00 1 .236E-01 1 . 7 6 9E+0 0 3 . 298E+00 3.915E-02 1 . 77 6 E + 00 -0.032 0.053 0.091 6.0000 1 . 650E+00 1 .371E-01 1 . 787E+00 3 . 530E+00 3.792E-02 1 . 885E+00 -0.030 0.051 0.039

7.0000 1 . 667E+00 1 .696E-01 1 . 832E+00 9 . 082E+00 9.397E-02 2 . 087E+00 -0.028 0.098 0.036 8.0000 1 . 632E+00 1 . 927E-0

1

1 .875E+00 9 . 622E+00 5 . 052E-02 2.269E+00 -0.025 0.095 0.033

9.0000 1 . 695E+00 2.219E-01 1 . 91 6E+00 5. 150E+00 5.709E-02 2 . 935E+00 -0.029 0.093 0.030

10.0000 1 . 706E+00 2.507E-01 1 . 957E+00 5 . 666E+00 6 . 352E-02 2 . 587E+00 -0.022 0.091 0.028 12.5000 1 . 730E+00 3.259E-01 2 . 0 56E+0 0 6 . 91 2E+00 7 . 998E-02 2. 921 E+00 -0.019 0.036 0 .025 15.0000 1 . 79 9E+0 0 9.021 E-01 2.1 52E+00 8. 1 0 1 E+00 9.502E-02 3 . 205E+00 -0.017 0.033 0.022

17.5000 1 . 765E+00 9 .803E-01 2 . 296 E+0 0 9 . 238E+00 1 . 1 01 E-01 3 . 952E+00 -0.015 0.031 0.019 20.0000 1 . 77 9E + 00 5.596E-01 2 . 338E+00 1 . 0 33E+0

1

1 . 297E-0

1

3.671 E+00 -0.019 0.029 0.017 25.0000 1 . 80 1 E+00 7.209E-01 2 . 522E+00 1 .239E+01 1 . 523E-0

1

9 . 097E+00 -0.012 0.025 0.015

30 . 0000 1 . 8 1 8E+00 8.897E-01 2 . 703E+00 1 . 930E+0

1

1 . 781 E-01 9 . 362E+00 -0.010 0.023 0.013 35.0000 1 .833E+00 1 . 050E+00 2 . 833E+00 1 .609E+01 2.021E-01 9 . 635E+00 -0.009 0.021 0.011 90.0000 1 . 895E+00 1 . 21 8E+00 3 . 063E+00 1 . 778E+0

1

2.295E-01 9 . 87 i E+0 0 -0.008 0.020 0.010 95.0000 1 . 355E+00 1 . 386E+00 3 . 292E+00 1 .936E+01 2 . 955E-0

1

5.08 9E + 00 -0.007 0.018 0.009

50.0000 1 . 865E+00 1 . 556E+00 3.921 E+00 2.086E+01 2.651 E-01 5 . 282E+00 -0.006 0.017 0.008 55.0000 1 . 873E+00 1 . 727E+00 3 . 600E+00 2 . 229E+0

1

2.835E-01 5. 959E+00 -0.005 0.016 0.007 60.0000 1 . 880 E+0 0 1 .898E+00 3 . 778E+00 2 . 369E+0

1

3.008E-01 5 . 621 E+00 -0.005 0.016 0.007

70.0000 1 . 899E+00 2. 293E+00 9. 1 36E+00 2.617E+01 3. 325E-01 5.911 E+00 -0.009 0.019 0.006 80.0000 1 . 905E+00 2 . 5 90E+0 0 9 . 999E+00 2.899E+01 3.609E-01 6 . 1 65E+00 -0.003 0.013 0 .005 90.0000 1 . 915E+00 2. 938E+00 9 . 353E+00 3.063E+01 3.365E-01 6 . 3 9 1 E + 0 0 -0.003 0.012 0.009 100.0000 1 . 923E+00 3 . 288E+00 5.21 2E+00 3.262E+01 9.097E-01 6 . 599E+00 -0.003 0.012 0.009

125.0000 1 . 991 E+00 9. 169E+00 6.11 0E+00 3 . 705E+0

1

9.593E-01 7 . 027E+00 -0.002 0.010 0.003

150.0000 1 . 956E+00 5 . 055E+00 7.011 E+00 9.086E+01 9 . 999E-01 7 . 3S9E+00 -0.001 0.010 0.002

175.0000 1 . 968E+00 5. 995E+00 7 . 91 3E+00 9 . 922E+0

1

5.337E-01 7 . 687E+00 -0.001 0.009 0.002 200.0000 1 . 978E+00 6 . 839E+00 8.317E+00 9.721E+01 5 . 625E-0

1

7.951 E+00 -0.001 0.008 0.002 250.0000 1 . 996E+00 8 . 633E+00 1 .063E+01 5.237E+01 6 .090E-01 3. 393E+00 -0.001 0.008 0.001 300.0000 2.01 0E+00 1 . 093E+0

1

1 . 299E+0

1

5.671 E+0

1

6 . 952E-0

1

8 . 755E+00 -0.000 0 .007 0.001 350.0000 2 . 022E+00 1 . 229E+0

1

1 . 926E+0

1

6 . 096E+0

1

6.792E-01 9 . 062E+00 -0.000 0.007 0.001 900.0000 2 . 032E+00 1 . 905E+0

1

1 . 608E+01 6 . 376E+01 6 . 982E-01 9.328E+00 -0.000 0.006 0.001 950.0000 2.091 E+00 1 .586E+01 1 . 7 90E+0

1

6 . 670E+01 7.189E-01 9 . 563E+00 -0.000 0 .006 0.001 500.0000 2. 099E+00 1 . 768E+0

1

1 . 973E+01 6 . 936E+0

1

7.357E-01 9 . 773E + 00 -0 . 000 0.006 0.001 550.0000 2 . 057E+00 1 . 950E+01 2.1 55E+01 7. 179E+01 7.507E-01 9 . 963E+00 -o.ooo 0.006 0.001 500.0000 2.063E+00 2. 1 31 E+01 2 . 333E+0

1

7.901 E+0

1

7.633E-01 1 . 01 9E+01 -0.000 0.005 0.001 700.0000 2 . 075E+00 2 . 996E+01 2.703E+01 7.799E+01 7 . 858E-0

1

1 . 099E+0

1

-0.000 0.005 0.000 300.0000 2 . 086E+00 2.360E+01 3.069E+01 8 . 1 96E+01 8.036E-01 1 .071 E+01 -0 .000 0.005 o.ooo 900.0000 2 . 0 95E+00 3 . 225E+0

1

3 . 939E+0

1

3 . 959E+0

1

8. 132E-01 1 . 0 95E+0

1

-0 . 000 0.005 0.000 1000.0000 2 . 1 03E+00 3 . 590E+0

1

3 . 800E+0

1

8 . 730E+0

1

8. 306E-01 1 . 1 1 6E+01 -0.000 0.005 0.000

145
ELECTRONS IN SODIUM IODIDE

I = 452.0 eV DENSITY = 3 . 667E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DEHS.EFF. d( log[ )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD COP.R. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MaV ca 2/g MeV cm 2 /g MeV cn 2 /g g/cji 2 0.0100 1 . 1 1 6E+01 1 . 5 1 8E-02 1 . 1 17E+01 5.598E-04 6.717E-04 0 .

0

-0.309 0.416 0.382

0.0125 9 . 603E+00 1 . 6 32E-02 9.61 9E+00 8.018E-04 8.429E-04 0.0 -0.289 0 . 380 0.351 0.0150 8 . 477E+00 1 . 723E-02 8 . 494E+00 1 .079E-03 1 .013E-03 0.0 -0.275 0 . 355 0.330 0.0175 7 . 622E+00 1 . 798E-0 2 7 . 640E+00 1 . 390E-03 1 . 131 E-03 0 .

0

-0.264 0.336 0.314

0.0200 6 . 948E+00 1 . 862E-02 6 . 966E+00 1 . 733E-03 1 . 348E-03 0.0 -0.255 0.320 0.301 0.0250 5. 949E+00 1 . 967E-02 5. 968E+00 2.51 IE-03 1 .675E-03 0.0 -0.242 0.298 0.282

0.0300 5.241E+00 2 . 050E-02 5 . 262E+00 3 . 406E-03 1 . 996E-03 0.0 -0.232 0.281 0.268

0.0350 4.711 E+00 2. 120E-02 4 . 733E+00 4.410E-03 2.309E-03 0.0 -0.224 0.269 0.257

0.0400 4 . 299E+00 2. 180E-02 4 . 32 1 E+00 5.517E-03 2.616E-03 0.0 -0.218 0.259 0.249

0.0450 3. 968E+00 2.234E-02 3. 990E+00 6 . 723E-03 2.917E-03 0 .

0

-0.213 0.251 0.242

0.0500 3 . 6 96 E+00 2.282E-02 3.71 9E+00 8 . 022E-03 3.212E-03 0.0 -0.208 0.244 0.236

0.0550 3.469E+00 2 . 326E-02 3 . 492E+00 9.410 E-03 3 . 502E-03 0.0 -0.204 0.239 0.231 0.0600 3 . 276E+00 2.367E-02 3 . 300E+00 1 . 088E-02 3 . 786E-03 0.0 -0.201 0.234 0.226 0.0700 2. 965E+00 2.442E-02 2. 990E+00 1 . 407E-02 4 . 342E-03 0.0 -0.195 0.225 0.219

0.0800 2 . 726E+00 2.509E-02 2.751 E+00 1 . 757E-02 4 . 380 E-0 3 0.0 -0.191 0.218 0.213

0.0900 2 . 536E+00 2.571E-02 2 . 562E+00 2.134E-02 5 . 402E-03 0.0 -0.187 0.213 0.208

0.1000 2.382E+00 2 . 628E-02 2 . 408E+00 2.536E-02 5.91 0E-03 0.0 -0.183 0.208 0.203

0.1250 2 . 0 98E+00 2 . 7 6 0E-02 2 . 1 26E+00 3 . 646E-02 7. 120E-03 0.0 -0.176 0.199 0.195

0.1500 1 . 905E+00 2.878E-02 1 . 934E+00 4.882E-02 8 . 258E-03 0.0 -0.171 0.192 0.188

0.1750 1 . 766E+00 2.989E-02 1 . 7 96E + 00 6 . 225E-02 9. 332E-03 0.0 -0.167 0.186 0.183

0.2000 1 .661 E+00 3.096E-02 1 . 6 92E + 00 7.661E-02 1 . 035E-02 0.0 -0.163 0.182 0.178

0.2500 1 . 51 6E+00 3.306E-02 1 . 54 9E + 00 1 . 076E-0

1

1 . 225E-02 0.0 -0.158 0.175 0.171

0 . 3000 1 . 421 E+00 3.519E-02 1 . 456E+00 1 .410E-01 1 . 40 QE-02 0.0 -0.153 0.169 0.166 0.3500 1 . 355E+00 3 . 739E-02 1 . 393E+00 1 .761 E-0

1

1 . 565E-02 1 . 1 29E-03 -0.146 0.165 0.162

0.4000 1 . 308E+00 3. 967E-02 1 . 348E+00 2 . 1 26 E-0

1

1 .721E-02 5 . 582E-03 -0.141 0.160 0.157

0.4500 1 . 273E+00 4 . 204E-02 1 . 3 1 5E+00 2 . 502E-0

1

1 .871 E-02 1 . 097E-02 -0.137 0.157 0.153

0.5000 1 . 247E+00 4 . 448E-02 1 .291 E+00 2 . 886 E-0

1

2.01 6E-02 1 .71 IE-02 -0.134 0.153 0.149

0.5500 1 . 227E+00 4.698E-02 1 . 274E+00 3 . 276E-0

1

2. 157E-02 2. 388E-02 -0.131 0.150 0.146

0.6000 1 .21 1 E+00 4 . 956E-02 1 . 26 1 E+00 3.671 E-0

1

2 . 295E-02 3.11 9E-02 -0.128 0.147 0.143

0.7000 1 . 1 90E+00 5 . 486E-02 1 . 245E+00 4.469E-01 2 . 562E-02 4.71 IE-02 -0.122 0.142 0.133

0.8000 1 . 178E+00 6 . 037E-02 1 . 23SE+00 5.275E-01 2 . 822E-02 6 . 443E-02 -0.113 0.138 0.133

0.9000 1 . 1 70E+00 6 . 605E-02 1 . 236E+00 6.084E-01 3 . 076E-02 3.284E-02 -0.113 0.134 0.129

1 .0000 1 . 167E+00 7.189E-02 1 . 239E+00 6.892E-01 3 . 326E-02 1 .021E-01 -0.110 0.131 0.125

1 .2500 1 . 167E+00 8.71 4E-02 1 . 254E+00 8.899E-01 3. 936E-02 1 . 530 E-0

1

-0.102 0.124 0.116

1 .5000 1 . 173E+00 1 .031E-01 1 . 276E+00 1 . 088E+00 4 . 533E-02 2.065E-01 -0.095 0.118 0.109

1 .7500 1 . 182E+00 1 .198E-01 1 . 302E+00 1 . 282E+00 5. 120E-02 2.610 E-0

1

-0.089 0.113 0.103 2.0000 1 . 1 92E+00 1 .369E-01 1 . 329E+00 1 . 472E+00 5 . 700E-02 3. 159E-01 -0.035 0.108 0.093

2.5000 1 . 21 2E+00 1 . 725E-0

1

1 . 384E+00 1 .840E+00 6 . 833E-0 2 4.239E-01 -0.077 0.1C1 0.089

3.0000 1 . 230E+00 2.093E-01 1 . 439E+00 2.1 95E+00 7 . 949E-02 5 . 275E-0

1

-0.071 0.095 0.082

3.5000 1 . 247E+00 2.471 E-0

i

1 . 494E+00 2 . 536E+00 9.034E-02 6 .258E-01 -0.067 0.090 0.076 4.0000 1 . 263E+00 2.857E-01 1 . 548E+00 2 . 864E+00 1 .009E-01 7. 184E-01 -0.064 0.086 0.071 4.5000 1 . 277E+00 3 . 250E-0

1

1 .601 E+00 3. 182E+00 1 .1 12E-01 3.057E-01 -0.061 0.082 0.067

5.0000 1 . 289E+00 3.649E-01 1 . 654E+00 3 . 489E+00 1 .21 3E-01 8.831 E-0

1

-0.058 0.079 0.064

5.5000 1 . 301 E+00 4.055E-01 1 . 706E+00 3 . 787E+00 1 .31 IE-01 9.660E-01 -0.056 0.076 0.061 6.0000 1.311 E+00 4.464E-01 1 . 758E+00 4 . 075E+00 1 . 407 E-0

1

1 . 040E+00 -0.054 0.074 0 . 058 7.0000 1 . 330E+00 5.297E-01 1 . 860 E + 00 4 . 628E+00 1 .591 E-0

1

1 . 177E+00 -0.051 0.070 0.053

8.0000 1 . 347E+00 6 . 1 45E-01 1 . 96 1 E+00 5 . 1 52E+00 1 . 766E-0

1

1 . 30 1 E+00 -0 . 049 0.066 0.049

9.0000 1 .36 1 E+00 7.005E-01 2 . 062E+00 5 . 649E+00 1 . 933E-01 1 . 4 1 6E+00 -0.047 0.063 0.046

10.0000 1 . 374E+00 7.876E-01 2.162E+00 6.122E+00 2.092E-01 1 . 522E+00 -0.045 0.061 0.043

12.5000 1 .401 E+00 1 . 009E+00 2.41 0E+00 7.21 7E+00 2.458E-01 1 . 759E+00 -0.041 0.055 0.038

15.0000 1 . 423E+00 1 . 235E+00 2 . 658E+00 8 . 204E+00 2.785E-01 1 . 964E+00 -0.038 0.051 0.034

17.5000 1 .441E+00 1 . 465E+00 2 . 906E+00 9 . 1 03E+00 3 . 080E-0

1

2. 147E+00 -0.035 0 .048 0.030 20.0000 1 . 456E+00 1 . 6 97E+00 3. 153E+00 9. 929E+00 3.347E-01 2.31 2E+00 -0.032 0.046 0.023

25.0000 1 . 480E+00 2. 169E+00 3.649E+00 1 . 140E+01 3.81 3E-01 2 . 605E+00 -0.028 0.041 0.023

30.0000 1 . 49 9E + 0 0 2 . 648E+00 4. 147E+00 1 .269E+01 4 . 206 E-0

1

2 . 853E+00 -0.025 0.038 0.020

35.0000 1 . 5 1 4E+00 3.133E+00 4. 647E+00 1 . 382E+0

1

4 . 544E-0

1

3.081 E+00 -0.022 0.036 0.018

40.0000 1 . 527E+00 3 . 622E+00 5. 149E+00 1 . 485E+0

1

4.837E-01 3.281 E+00 -0.020 0.034 0.016 45.0000 1 . 53 9E+00 4.11 4E+00 5 . 652E+00 1 . 577E+0

1

5.095E-01 3 . 463E+00 -0.019 0 .032 0.014

50.0000 1 . 543E+00 4 . 609E+00 6 . 1 58E+00 1 . 662E+0

1

5.324E-01 3 . 628E + 00 -0.017 0.031 0.013

55.0000 1 . 557E+00 5 . 1 07E+00 6 . 664E+00 1 . 740E+0

1

5 . 529E-0

1

3.780 E+00 -0.016 0.029 0.012 60.0000 1 . 56 5E + 00 5 . 607E+00 7. 172E+00 1 .312E+01 5.71 3E-01 3.921 E+00 -0.015 0.028 0.011 70.0000 1 . 57 9E + 00 6.61 2E+00 3.1 91 E+00 1 . 943E+01 6.033E-01 4 . 1 75E+00 -0.014 0.027 0.009 80.0000 1 . 590E+00 7 . 623E+00 9.21 3E+00 2 . 058E+0

1

6 . 30 1 E-0

1

4 . 399E+00 -0.013 0.025 0.008

90.0000 1 . 600E+00 8 . 639E+00 1 . 024E+0

1

2. 161E+01 6 . 530 E-0

1

4 . 600E+00 -0.012 0.024 0.007 100.0000 1 . 609E+00 9 . 659E+00 1 .127E+01 2 . 254E+0

1

6.727E-01 4 . 782E+00 -0.011 0.023 0.007

1 25.0000 1 . 627E+00 1 . 222E+0

1

1 . 385E+0

1

2.454E+01 7.123E-01 5 . 1 74E+00 -0.009 0.022 0 .005 150.0000 1 . 641 E+00 1 . 4 7 9E+0

1

1 . 644E+0

1

2.61 9E+01 7.422E-01 5 . 502E+00 -0.008 0.020 0.004

175.0000 1 . 653E+00 1 . 738E+0

1

1 . 903E+01 2.760E+01 7 . 658E-01 5.783E+00 -0.007 0.019 0.004

200.0000 1 . 663E+00 1 . 997E + 0

1

2. 163E+01 2 . 883E+0

1

7.848E-01 6 . 029E+00 -0 .006 0.018 0.003 250.0000 1 . 630E+00 2.516E+01 2 . 684E+0

1

3.091 E+0

1

8 . 1 40 E-0

1

6 . 445E+00 -0.005 0.017 0 .003 300.0000 1 . 6 93E+00 3. 037E+01 3 . 207E+0

1

3.261E+01 8 . 354E-0

1

6 . 7 90E+0 0 -0.004 0.016 0.002

350.0000 1 . 704E+00 3 . 560E + 0

1

3.730E+01 3 . 405E+0

1

8.519E-01 7 . 0S3E+00 -0.003 0.016 0.002 400.0000 1 .714E+00 4 . 082E+0

1

4 . 254E+0

1

3 . 531 E+0

1

8.651 E-0

1

7 . 339E+00 -0.003 0.015 0.002

450.0000 1 . 722E+00 4 . 606E+0

1

4 . 778E+01 3.641 E+0

1

8.759E-01 7 . 566E+00 -0.003 0.015 0.002

500.0000 1 . 729E+00 5. 1 30E+0

1

5. 303E+01 3.741 E+0

1

8 . 848E-0

1

7.76 9E + 00 -0.003 0.014 0.001 550.0000 1 . 735E+00 5.654E+01 5 . 827E+0

1

3.831 E+0

1

3 . 925E-0

1

7 . 954E+00 -0.002 0.014 0.001

600 .0000 1 . 742E+00 6. 178E+01 6 . 353E+0

1

3.913E+01 3 . 99 1 E-0

1

8. 123E+00 -0.002 0 . 0 1 4 0.001 700.0000 1 . 753E+00 7 . 229E+0

1

7 . 404E+0

1

4 . 058E+0

1

9.098E-01 8 . 423E+00 -0.002 0.013 0.001 800.0000 1 . 762E+00 8 . 280E+0

1

8.456E i oi 4. 185E+01 9.183E-01 8 . 684E+00 -0.002 0.013 0.001 900.0000 1 . 770 E+00 9 . 332E+0

1

9.509E+01 4 . 296 E+0

1

9 . 252E-0

1

3. 915E+00 -0.001 0.012 0.001 1000.0000 1 . 777E+00 1 . 038E+02 1 . 056E-L 02 4 . 396E+0

1

9.309E-01 9 . I 22E+00 -0.001 0.012 0.001

146
ELECTRONS IN STILBENE

i

I = 67.7 eV

ENERGY STOPPING POWER

COLLISION RADIATIVE TOTAL

MeV MeV cm 2/g MeV cm 2/g MeV cm 2/g O.OIOO 2.209E+01 3 . 004E-03 2.209E+01

0.0125 1 . 856E+0

1

3.014E-03 1 . 356E+0

1

0.0150 1 .610E+01 3.021E-03 1 .610E + 01 0.0175 1 . 428E+0

1

3.026E-03 1 . 428E + 0

1

0.0200 1 . 287E+0

1

3.031E-03 1 . 287E + 0

1

0 . 0250 1 . 083E+01 3.039E-03 1 . 083E+0

1

0.0300 9.41 8E+00 3.049E-03 9.421 E+00 0.0350 8 . 380E+00 3 . 059E-03 8 . 383E+00

0.0400 7 . 582E+C0 3 . 070E-03 7 . 585E+00

0.0450 6 . 949E+00 3.083E-03 6 . 953E+00

0.0500 6 . 435E+00 3.096E-03 6 . 438E+00

0.0550 6 . 007E+00 3.1 10E-03 6.010 E+00 0.0600 5 . 646E+00 3. 126E-03 5 . 650E+00

0.0700 5.071 E + 0 0 3. 157E-03 5 . 074E+00

0.0800 4.631E+00 3.1 91E-03 4 . 635E+00

0.0900 4 . 285E+00 3.228E-03 4 . 288E+00

0.1000 4 . 005E+00 3 . 267E-03 4 . 008E+00

0.1250 3 . 493E+00 3.373E-03 3 . 497E+00

0.1500 3.148E+00 3.487E-03 3. 152E+00 0.1750 2. 901E+00 3.608E-03 2. 904E+00

0.2000 2.71 5E+00 3.736E-03 2.71 8E+00

0.2500 2 . 456 E+0 0 4.01 IE-03 2 . 46 0 E + 0 0 0.3000 2. 287E+00 4.312E-03 2 . 292E+00

0 . 3500 2.1 70E+00 4.633E-03 2. 175E+00 0.4000 2 . 085E+00 4 . 975E-03 2 . 0 90E+00

0.4500 2 . 020 £+00 5.336E-03 2 . 026E+00

0.5000 1 . 969E+00 5.714E-03 1 . 975E+00

0.5500 1 . 930E+00 6 . 107E-03 1 . 936E+00

0.6000 1 . 898E+00 6.51 3E-03 1 . 904E+00

0.7000 1 .851 E+00 7 . 364E-03 1 . 858E+00

0.8000 1 .81 9E+00 8.258E-03 1 . 8 27E+0 0

0 . 9000 1 . 7 97E+00 9.1 93E-03 1 . 807E+00

1 .0000 1 . 782E+00 1 . 0 1 7E-02 1 . 792E+00

1 .2500 1 .761 E+00 1 . 274E-02 1 . 774E+00

1 .5000 1 . 754E+00 1 .550E-02 1 .770E + 00

1 .7500 1 . 753E+00 1 .340E-02 1 . 77 2E + 0 0 2.0000 1 . 756E+00 2. 1 43E-02 1 . 778 E + 00 2.5000 1 . 7 6 7E+0 0 2.780E-02 1 . 795E+00

3.0000 1 . 780E+00 3.452E-02 1 .31 4E+00

3.5000 1 . 7 93E+00 4. 152E-02 1 . 834E+00

4.0000 1 .805E+00 4 . 875E-02 1 .854E+00 4.5000 1 .81 7E+00 5 . 620E-02 1 . 8 73E+00

5.0000 1 .828E+00 6.333E-02 1 .891 E+00 5.5000 1 .838E+00 7.162E-02 1 . 909E+00

6.0000 1 . 847E+00 7. 956E-02 1 . 927E+00

7.0000 1 . 36 4E+0 0 9 . 582E-0 2 1 . 960E+00 3.0000 1 . 87 9E + 0 0 1 . 1 25E-0

1

1 . 992E+00

9.0000 1 . 8 93E+0 0 1 . 296E-0

1

2 . 022E+00

10.0000 1 . 904E+00 1 .470E-01 2.051 E+00

12.5000 1 . 929E+00 1 .917E-01 2 . 1 2 1 E+0 0 15.0000 1 . 948E+00 2.377E-01 2 . 1 86 E+00 17.5000 1 . 964E+00 2.847E-01 2.249E+00

20.0000 1 . 97SE+00 3.325E-01 2. 31 0E+00 25.0000 1 . 999E+00 4.300E-01 2 . 429E+00

30.0000 2.01 6E+00 5.292E-01 2 . 545E+0 0 35.0000 2 . 0 30E+00 6 .297E-01 2 . 660E+00

40.0000 2 . 042E+00 7.314E-01 2 . 773E+00

45.0000 2.052E+00 8.339E-01 2 . 886 E+0 0 50.0000 2.061 E+00 9.372E-01 2. 998E+00 55.0000 2.06 9E+00 1 .041 E+00 3 . 1 1 OE+OO 60.0000 2 . 077E+00 1 . 146E+00 3 . 222E+00

70.0000 2 . 0 SOE+OO 1 . 356E+00 3 . 446E+00

30.0000 2. 1 01 E+00 1 . 568E+00 3.669E+00

90.0000 2.111 E+00 1 .781 E+00 3 . 3 92E+0 0 100.0000 2.120E+00 1 . 996E+00 4. 1 15E+00 125.0000 2.1 38E+00 2 . 5 35 E+0 0 4. 673E+00

1 50.0000 2. 153E+00 3 . 079E+00 5 . 232E+00

175.0000 2 . 1 66E+00 3. 625E+00 5.791 E+00 200.0000 2.177E+00 4. 174E+00 6.351 E+00

250 .0000 2.1 95E+00 5 . 277E+00 7 . 473E+00

300.0000 2.210E+00 6 . 386E+00 S . 5 96 E+00 350.0000 2 . 223E+00 7 . 499E+00 9 . 722E+00

400.0000 2 . 234E+00 8.61 4E+00 1 . 085E+0

1

450.0000 2 . 244E+00 9 . 733E+00 1 . 1 93E+0

1

500.0000 2 . 252E+0 0 1 . 085E+0

1

1 . 3! OE+OI

550 . 0000 2 . 26 0E J-0 0 1 . 1 97E+01 1 . 423E+0

1

600.0000 2 . 267E + 00 1 .310E+01 1 . 5 36 E+0

1

700.0000 2 . 280E+00 1 . 535E+0

1

1 .763E+01 800.0000 2.291 E+00 1 . 76 0 E+0

1

1 . 989E+01 900.0000 2 . 300E+00 1 . 985E+0

1

2.216 E+0

1

1000.0000 2.309E+00 2.211 E+0

1

2 . 442E+0

1

DENSITY = 9.707E-01 g/cm 3

CSDA RADIATION DENS.EFF. d< loc1 )/d(logI) RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

g/cm 2 561E-04 7 . 507E-05 0.0 -0 . 1 95 0.222 0.221 801E-04 8.992E-05 0.0 -O . 187 0.212 0.211 251E-04 1 .041 E-04 0.0 -0.181 0.204 0.203 904E-04 1 . 1 73E-04 0 .

0

-0.176 0.198 0 . 1 97 751 E-04 1 . 31 0E-04 0.0 -0.172 0.193 0.192 300E-03 1 . 565E-04 0 .

0

-0.166 0.185 0.184 797E-03 1 . 808E-04 0 .

0

-0.161 0.179 0.178

361 E-03 2.041 E-04 0.0 -0.157 0.174 0.174 989E-03 2.267E-04 0.0 -0.154 0.170 0.170 678E-03 2 . 437E-0 4 0.0 -0.152 0.167 0.167 426E-03 2.700E-04 0.0 -0.149 0.164 0.164

231 E-03 2. 909E-04 0.0 -0.147 0.162 0.161 089E-03 3.11 3E-04 0.0 -0.146 0.160 0.159

961 E-03 3 . 508E-04 0 .0 -0.143 0.156 0.156 003E-02 3 . 889E-04 0.0 -0.140 0.153 0.153 227E-02 4 . 258E-04 0.0 -0.138 0.150 0.150 469E-02 4.616E-04 0.0 -0.136 0.148 0.148

1 39E-02 5 . 474E-0 4 0.0 -0.132 0.144 0.143 894E-02 6 . 288E-04 0.0 -0.129 0.140 0.140 722E-02 7.068E-04 0.0 -0.127 0 . 1 37 0.137

61 3E-02 7 . 820E-04 0.0 -0.125 0.135 0.135 553E-02 9 .262E-04 0.0 -0.121 0.131 0.131 663E-02 1 .065E-03 0.0 -0.119 0.129 0.128

091E-01 1 .1 99E-03 0.0 -0.116 0.126 0.125

325E-01 1 .331 E-03 0.0 -0.110 0.124 0.123

56SE-01 1 . 462E-0 3 1 . 936E-02 -0.092 0.120 0.118

31 9E-01 1 . 592E-03 4 . 453E-02 -0.086 0.116 0.113

074E-01 1 . 722E-0 3 7 . 225E-02 -0.031 0.112 0.108

335E-01 1 . 852E-0 3 1.01 9E-01 -0.076 0.108 0.104 867E-01 2. 1 15E-03 1 -648E-01 -0.068 0.101 0.096

410E-01 2.381 E-03 2.305E-01 -0 .063 0.096 0.089

960E-01 2 . 6 50E-03 2.971 E-0

1

-0.058 0.091 0.083

516E-01 2. 923E-03 3 . 636E-01 -0.054 0.086 0.078

920E-01 3 . 622E-03 5 . 253E-0

1

-0.047 0.078 0 .068

331 E-01 4 . 346E-03 6 . 774E-0

1

-0.043 0.071 0.061 743E-01 5.092E-03 8. 1 90 E-0

1

-0.040 0.066 0.056

01 5E+00 5.857E-03 9.504E-01 -0.037 0.063 0.051 295E+00 7 . 438E-03 1 . 186E+00 -0.034 0.057 0 .045 572E+00 9.074E-03 1 . 393E+00 -0.032 0.052 0.041 846E+00 1 . 075E-02 1 . 576E+00 -0.030 0.049 0.033 118E+00 1 . 247E-02 1 . 740E+00 -0.029 0.047 0.036 386E+00 1 .421E-02 1 . 83 9E+0 0 -0.028 0.044 0.034 652E+00 1 . 5 98E-02 2 . 025E+00 -0.027 0.043 0.033

91 5E+00 1 . 776E-02 2. 1 51 E+00 -0.026 0.041 0.031 175E+00 1 . 957E-02 2.269E+00 -0.025 0.040 0.030

6 90 E+00 2.321E-02 2.481 E+00 -0.024 0.037 0.028

1 96 E+00 2.639E-02 2.571 E+00 -0.022 0.036 0.027 694E+00 3.061 E-02 2.343E+00 -0.020 0.034 0.025

185E+00 3 . 433E-02 3.001 E+00 -0.019 0.032 0.024 383E+00 4 . 368E-02 3 . 347E+00 -0.016 0.029 0.021 544E+00 5.300E-02 3 . 643E+00 -0.013 0.027 0.013 672E+00 6 . 224E-02 3 . 90 3 E+0 0 -0.011 0.025 0.016 768E+00 7. 133E-02 4.134E+00 -0.009 0.023 0.014

188E+01 3. 924E-02 4 . 533E+00 -0.006 0.020 0.012

339E+01 1 . 065E-0

1

4.86 9E+00 -0.005 0.018 0.009

58 1 E+0

1

1 . 230E-01 5 . 1 58E+00 -0.004 0.016 0.008

765E+01 1 . 390E-01 5 . 41 2E+00 -0.003 0.015 0 .007 942E+01 1 . 542E-0

1

5 . 638E+00 -0.002 0.013 0.006

1 12E+01 1 .689E-01 5 . S^2E+00 -0 .002 0.012 0.005

27 6 E + 0

1

1 . 830E-0

1

6 . 027E+00 -0.002 0.012 0.004

434E+01 1 . 965E-01 6 . 1 97E + 00 -0.001 0.011 0.004

734E+01 2.220E-01 6 . 499E + 00 -0.001 0.010 0.003

015E+01 2 . 456E-01 6 .761 E+00 -0.001 0.009 0.003

279E+01 2.675E-01 6 . 994E+00 -0.001 0.008 0.002

529E+01 2.879E-01 7 . 202E+00 -0.001 0.008 0 .002 099E+01 3 . 333E-0

1

7 . 644E+00 -0 .000 0.007 0.001 604E+01 3.721 E-0

1

8. 006E+00 -0.000 0.006 0.001 058E+01 4.058E-01 8. 31 3E+00 -0 .000 0.005 0.001

47 0 E + 0

1

4.353E-01 8.579E+00 -0 .000 0.005 0.001

1 95E+0

1

4.849E-01 9 . 024E+00 -0.000 0.004 0.001

81 9E+01 5.249E-01 9 . 387E+0 0 -0.000 0.004 0.000

365E+01 5.532E-01 9 . 6 95E+00 -0 . 000 0.004 0 .000 352E+01 5.863E-01 9 . 962E+00 -0.000 0.004 0.000

290 E + 0

1

6.105E-01 1 . 020E+01 -0.000 0.003 0 .000 639E+0

1

6 .315E-01 1 .041 E+0

1

-0.000 0.003 0.000

055E+01 6 . 500 E-0

1

1 . 060E+01 -0.000 0.003 0.000

393E+01 6 .664E-01 1 . 0 77E+0

1

-0.000 0.003 0.000 000E+02 6.943E-01 ! . 1 08E+01 -0.000 0.003 0.000 053E+02 7. 173E-01 1 . 1 35E+01 -0.000 0.003 0.000 101E+02 7 . 365E-0

1

1 . 1 58E+01 -0 .000 0.003 0 .000 144E+02 7 . 530E-01 1 . 179E+01 -0.000 0.002 0.000

2

3

5

68

1

12

2

34

5

67

1

1

12

2

34

6S

1

1

1

122

2

3

3

4

5

73

1

1

1

1

2

2

2

2

3

344

5

678

9

1

1

1

1122

22

3

3

3

44

55

6

67

7

3

3

99

1

1

1

1

147
ELECTRONS IN TISSUE-EQUIVALENT GAS (METHANE BASED)

I = 61.2 eV DENSITY = 1.06AE-03 g/cm 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV ca 2 /g MeV ca 2 /g MeV cm 2 /g g/cm 2 0.0100 2 . 325E+0

1

3. A02E-03 2 . 326E+0

1

2. A26E-0A 7. 986E-05 0.0 -0.191 0.217 0.215

0.0125 1 . 952E+0

1

3.A21E-03 1 . 953E+01 3.605E-0A 9.606E-05 0.0 -0.183 0.207 0.206 0.0150 1 . 6 92E+0

1

3. A33E-03 1 . 6 93E+0

1

A . 98AE-0

A

1 . 1 16E-0A 0.0 -0.178 0.200 0.199

0.0175 1 . 500E+0

1

3.AA1E-03 1 .500E+01 6 . 556E-0

A

1 . 265E-0

A

0.0 -0.173 0. 1 9A 0.193

0.0200 1 . 352E+0

1

3. AA7E-03 1 . 352E+0

1

8.31 AE-OA 1 . A 1 0 E-0

A

0 .

0

-0.169 0.189 0.188

0.0250 1 . 1 37E+0

1

3.A57E-03 1 . 1 37E+0

1

1 . 237E-03 1 . 687E-0

A

0.0 -0.163 0.181 0.181 0.0300 9 . 882E+00 3.A67E-03 9 . 885E+0 0 1 . 71 0E-03 1 . 952E-0A 0.0 -0.159 0.176 0.175

0.0350 8 . 789E+00 3. A77E-03 8 . 792E+00 2.2A7E-03 2 . 206E-0

A

0.0 -0.155 0.171 0.171

0 .OAOO 7.950E+00 3. A88E-03 7 . 953E+00 2 . 8A6E-03 2. A52E-0A 0.0 -0.152 0.167 0.167

0.0A50 7 . 285E+00 3.501E-03 7 . 288E+00 3 . 50 AE-03 2.690E-0A 0 .

0

-0.1A9 0 . 1 6 A 0 . 1 6A 0.0500 6 . 7 A3E+00 3.51 AE-03 6 . 7A7E + 00 A.217E-03 2.922E-0A 0.0 -0 . 1 A7 0.161 0.161 0.0550 6 . 29AE+00 3.529E-03 6 . 298E+00 A. 985E-03 3. 1 A8E-0A 0.0 -0 . 1 A5 0.159 0.159

0.0600 5.91 5E+00 3.5AAE-03 5.91 SE+00 5 . 805E-03 3 . 368E-0

A

0.0 -0.1A3 0.157 0.157

0.0700 5.31 OE+OO 3.578E-03 5.31 AE+00 7.591E-03 3 . 796E-0

A

0.0 -0. 1A1 0.153 0.153

0.0800 A .8A9E+00 3.61 AE-03 A . 853E+00 9.56AE-03 A.208E-0A 0.0 -0.138 0.150 0.150

0.0900 A . A85E+00 3.65AE-03 A . A89E+00 1 . 171E-02 A . 607E-0A 0.0 -0.136 0. 1 A8 0. 1A8 0.1000 A. 1 91 E+00 3.696E-03 A . 1 95E+00 1 . A02E-02 A. 99AE-0A 0 .

0

-0.13A 0.1A6 0.1A6

0.1250 3 . 655E+00 3.812E-03 3.659E+00 2 . 0 A2E-02 5. 920E-OA 0.0 -0.130 0.1A2 0 . 1 A

1

0.1500 3 . 293E+00 3. 937E-03 3 . 297E+00 2.76AE-02 6 . 797E-0

A

0.0 -0.128 0.138 0.133

0.1750 3 . 033E+00 A.071E-03 3 . 037E+00 3.556E-02 7 . 638E-0A 0.0 -0.125 0.136 0.135

0.2000 2 . 838E+00 A.213E-03 2 . 8A2E+00 A . A08E-02 8 . AA7E-0

A

0.0 -0.123 0.133 0.133

0.2500 2 . 567E+00 A.518E-03 2 . 572E+00 6 . 263E-02 9. 998E-0A 0.0 -0.120 0.130 0.129

0.3000 2.390E+00 A.851E-03 2 . 395E+00 3 . 282E-02 1 . 1 A8E-03 0.0 -0.117 0.127 0.126

0.3500 2 . 267E+00 5 . 208E-03 2 . 272E+00 1 .0A3E-01 1 . 293E-0 3 0.0 -0.115 0.125 0. 12A 0.A000 2. 178E+00 5 . 587E-03 2. 18AE+00 1 . 268E-0

1

1 . A3AE-03 0.0 -0.113 0.123 0.122

0. 9500 2.1 12E+00 5.988E-03 2.11 8E+00 1 . 500E-0

1

1 .57AE-03 0.0 -0.112 0.121 0.120

0.5000 2.061 E+00 6. A07E-03 2 . 068E+00 1 . 739E-0

1

1 .71 3E-03 0.0 -0.110 0.120 0.118

0.5500 2 . 022E+00 6.8AAE-03 2 . 029E+00 1 . 983E-01 1 .851E-03 0.0 -0.109 0.118 0.117

0.6000 1 . 992E+00 7.296E-03 1 . 999E+00 2 . 232E-0

1

1 . 990E-03 0.0 -0.108 0.117 0.115

0.7000 1 . 9A9E+00 8.2A1E-03 1 . 957E+00 2.738E-01 2.267E-03 0.0 -0.106 0.115 0.113

0.8000 1 . 921 E+00 9.233E-03 1 . 931 E+00 3 . 253E-0

1

2.5A6E-03 0.0 -0. 10A 0.113 0.111 0.9000 1 . 90AE+00 1 . 027E-02 1 . 91 AE+00 3 . 773E-0

1

2.826E-03 0.0 -0.102 0.112 0.109

1 .0000 1 .89AE+00 1 . 135E-02 1 . 905E+00 A.297E-01 3.11 0E-03 0.0 -0.101 0.111 0.108

1 .2500 1 . 886E+00 1 .A21E-02 1 . 900E+00 5.612E-01 3.831 E-0 3 0.0 -0.098 0.108 0.105

1 .5000 1 .890E+00 1 . 727E-02 1 . 908E+00 6 . 926E-0

1

A.569E-03 0.0 -0.096 0.105 0.102

1 .7500 1 . 90 1 E+00 2.0A9E-02 1 . 922E+00 8.232E-01 5.32AE-03 0.0 -0.09A 0 . 1 0 A 0.100

2.0000 1 . 91 5E+00 2 . 385E-02 1 . 939E+00 9.527E-01 6 . 093E-03 0.0 -0.092 0.102 0.098

2.5000 1 . 9A5E+00 3.091E-02 1 . 976E+00 1 . 208E+00 7 . 668E-03 0.0 -0.089 0.099 0.095

3.0000 1 . 975E+00 3.835E-02 2.01 3E+00 1 . A59E+00 9 . 280E-0 3 0.0 -0.087 0.097 0.092

3.5000 2 . 003E+00 A.610E-02 2 . 0A9E+00 1 . 705E+00 1 . 0 92E-02 0.0 -0 . 086 0.095 0.090

A. 0000 2 . 030E+00 5.A11E-02 2 . 08AE+00 1 . 9A7E+00 1 . 258E-02 0.0 -0 .08A 0 .09A 0.089

A. 5000 2 . 05AE+00 6 .23AE-02 2.116 E+00 2. 185E+00 1 . A26E-02 0.0 -0.083 0.093 0.087

5.0000 2. 077E+00 7.077E-02 2.1A7E+00 2. A20E+00 1 . 596E-92 0.0 -0.082 0.091 0.086

5.5000 2. 098E+00 7 . 938E-02 2. 177E+00 2.651 E+00 1 . 766E-02 0 .

0

-0.081 0.090 0 . 08 A 6.0000 2.11 7E+00 8.81 5E-02 2 . 205E+00 2 . 879E+00 1 . 938E-02 0.0 -0.080 0.089 0.083

7.0000 2. 153E+00 1 .061E-01 2 . 259E+00 3 . 327E+00 2.282E-02 0.0 -0.079 0.087 0.081 8.0000 2. 18AE+00 1 . 2A6E-0

1

2 . 308E+00 3 . 765E+00 2 . 628E-02 0.0 -0.078 0.086 0.080

9.0000 2.21 2E+00 1 . A3AE-01 2 . 355E+00 A. 1 9AE+00 2. 97AE-02 0.0 -0.077 0.C85 0 . 078

1 0 .0000 2 . 237E+00 1 . 626E-0

1

2. A00E+00 A. 61 AE+00 3 . 320E-02 0.0 -0.076 0.083 0.077

12.5000 2 . 292E+00 2.119E-01 2 . 50 AE+00 5 . 63AE+00 A. 180E-02 0.0 -0 .07A 0.081 0 . 07 A 15.0000 2 . 337E+00 2.626E-01 2 . 599E+00 6.61 3E+00 5 . 032E-02 0.0 -0.072 0.079 0.072

17.5000 2 . 375E+00 3. 1 AAE-01 2.689E+00 7 . 559E+00 5.870E-02 0.0 -0.071 0 . 077 0.070 20.0000 2. A08E+00 3.671 E-0

1

2 . 775E+00 8 . A7AE+00 6.69AE-02 0.0 -0.070 0.075 0.068

25.0000 2. A62E+00 A.7A3E-01 2 . 937E+00 1 . 022E+0

1

8 . 296E-02 1 . 908E-02 -0.059 0.072 0 . 06 A 30.0000 2.501 E+00 5.835E-01 3 . 085E+00 1 . 188E+01 9.838E-02 1 . 033E-0

1

-0 . 0 A 6 0.068 0.058

35.0000 2 . 530E+0 0 6. 9A2E-01 3 . 225E+0 0 1 . 3A7E+0

1

1 . 132E-01 2.153E-01 -0.039 0.06A 0.051

AO. 0000 2 . 55AE+00 8 . 060E-0

1

3 . 360E+00 1 . A99E+01 1 . 275E-0

1

3.356E-01 -0.03A 0.060 0 .0A6 A5.0000 2 . 573E+00 9. 188E-01 3 . A92E+00 1 . 6 A5E+0

1

1 . A13E-01 A . 562E-0

1

-0.030 0.057 O.OA2

50.0000 2 . 5 90E+0 0 1 . 032E+00 3 . 622E+00 1 . 785E+0

1

1 . 5A6E-0

1

5 . 735E-0

1

-0.027 0.05A 0.038

55.0000 2 . 605E+00 1 . 1 A7E+00 3.751 E+00 1 . 921 E+0

1

1 . 67AE-01 6.861 E-0

1

-0.025 0.052 0.035

60.0000 2.613E+00 1 . 26 1 E+00 3 . 879E+00 2.052E+01 1 .798E-01 7 . 93AE-01 -0 .02A 0 . 0A9 0.032

70.0000 2 . 6A0E+00 1 . A 9 3E+00 A.132E+00 2 . 302E+0

1

2.032E-01 9 . 92AE-01 -0.021 0 .0A6 0.028 80.0000 2 . 658E+00 1 . 725E+00 A . 38AE+00 2 . 537E+0

1

2.250E-01 1 . 172E+00 -0.020 0 .0A3 0.025

90 .0000 2.67AE+00 1 . 960E+00 A . 63AE+00 2 . 759E+0

1

2 . A5AE-0

1

1 . 336E+00 -0.01

9

O.OAO 0.022

100.0000 2 . 688E+00 2.1 95E+00 A . 833E+00 2. 969E+01 2.6A5E-01 1 . A85E+00 -0.018 0.038 0 .020 125.0000 2.71 7E+00 2 . 787E+00 5. 505E+00 3.A51E+01 3.07AE-01 1 .809E+00 -0.016 0.03A 0.017

150.0000 2.7A1E+00 3.38AE+00 6 . 1 2AE+00 3.881 E+O

1

3. AA5E-01 2.081 E+00 -0.015 0.031 0.01 A 175.0000 2 . 760E+00 3 . 98AE+00 6 . 7 A3E+0 0 A . 270E+0

1

3 . 770 E-0

1

2.31 5E+00 -0.01A 0.029 0.013 200.0000 2 . 776E+00 A . 586E+00 7 . 362E+00 A . 625E+0

1

A.058E-01 2 . 520E+00 -0 . 0 1 A 0.027 0.011 250.0000 2.303E+00 5 . 796E+00 8 . 599E+00 5.252E+01 A.5A6E-01 2 . 370E+00 -0.012 0.02A 0.009

300.0000 2 . 825E + 0 0 7.01 2E+00 9 . 837E+00 5 . 796E+0

1

A. 9A5E-01 3. 1 62E+00 -0.011 0.022 0.008

350.0000 2 . 3 A3E+00 8 . 232E+00 1 . 1 07E+0

1

6 .27AE+01 5 . 280 E-0

1

3. A1 AE+00 -0.010 0.021 0.007 A00.0000 2 . 858E+00 9. A56E+00 1 . 231 E+01 6 . 702E+0

1

5.565E-01 3 . 636E+00 -0.009 0.020 0.006 A50.000C 2.871 E+00 1 . 068E+0

1

1 . 355E+0

1

7.089E+01 5.81 IE-01 3 . 836 E + 0 0 -0.009 0.019 0.006 500.0000 2 . 832E+00 1 . 1 91 E+01 1 . A79E+0

1

7. AA2E+01 6 . 027E-01 A.017E+00 -0.008 0.018 0.005

550.0000 2 . 8 92E + 00 1 .31 AE+01 1 . 603E+0

1

7 . 767E+0

1

6.21 8E-0

1

A . 1 8AE+00 -0.007 0.017 0.005 600.0000 2.901 E+00 1 . A37E+01 1 . 727E+0

1

8 . 067E+0

1

6 . 388E-0

1

A . 338E+00 -0.007 0.017 0.00A

700 . 0000 2.91 7 E + 00 1 . 633E+0

1

1 . 975E+01 8 . 608E+0

1

6.679E-01 A. 61 AE+00 -0.005 0.016 0 . 00 A 800.0000 2 . 930 E + 0 0 1 . 930E+01 2.223E+01 9 . 085E+0

1

6.920E-01 A . 859E+00 -0 .005 0.015 0.003

900.0000 2.9A1E+00 2. 177E+01 2. A72E+01 9.512E+01 7 . 123E-01 5 . 077E+00 -0.00A 0.01 A 0.003 1000.0000 2 . 951 E+00 2 . A25E+0

1

2.720E+01 9.897E+01 7 . 297E-0

1

5 . 275E+00 -0.003 0 . 0 1 A 0.003

148
I.

ELECTRONS IN TISSUE-EQUIVALENT GAS (PROPANE BASED)

I = 59.5 eV DENSITY = 1.826E-03 g/cra 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS . EFF. d( log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2/g MeV cm 2/g g/cm 2 0.0100 2 . 340E+0

1

3.274E-03 2 . 340E+0

1

2.41 0E-04 7 . 648E-05 0 .

0

-0.190 0.215 0.214

0.0125 1 . 964E+01 3.290E-03 1 . 964E+01 3 . 581 E-04 9. 1 95E-05 0 .

0

-0.182 0.206 0.205

0.0150 1 . 702E+0

1

3.301E-03 1 .703E+01 4. 952E-04 1 .068E-04 0.0 -0.177 0.198 0.198 0.0175 1 .509E+01 3.308E-03 1 .509E+01 6.516E-04 1 .21 0E-04 0.0 -0.172 0.193 0.192

0 . 0200 1 . 359E+01 3.314E-03 1 . 359E+0

1

8.264E-04 1 . 348E-04 0.0 -0.168 0.188 0.187

0.0250 1 . 1 43E+0

1

3 . 323E-03 1 . 143E+01 1 . 229E-03 1 .614E-04 0.0 -0.162 0.180 0.180 0.0300 9 . 933E+00 3 . 333E-03 9 . 937E+00 1 .700E-03 1 . 867E-04 0.0 -0.158 0.175 0.174

0.0350 8 . 834E+00 3.343E-03 8 . 837E+00 2.235E-03 2.1 10E-04 0.0 -0.154 0.170 0.170

0 . 0400 7 . 990E+00 3.355E-03 7 . 993E+00 2.830E-03 2 . 345E-04 0.0 -0.151 0.167 0.166 0.0450 7.321 E+00 3. 367E-03 7 . 324E+00 3.485E-03 2.573E-04 0 .

0

-0.149 0.163 0.163

0.0500 6 . 776E+00 3.381E-03 6 . 780E+00 4 . 1 95E-03 2. 795E-04 0.0 -0.147 0.161 0.160 0.0550 6 . 325E+00 3.395E-03 6 . 328E + 00 4.959E-03 3.01 2E-04 0.0 -0.145 0.158 0.158

0 .0600 5. 944E+00 3.410E-03 5 . 947E + 00 5.775E-03 3 . 223E-04 0.0 -0.143 0.156 0.156

0 .0700 5 . 335E+00 3.443E-03 5 . 339E+00 7 . 553E-03 3 . 633E-04 0.0 -0.140 0.153 0.152

0.0800 4 . 872E+00 3.479E-03 4.875E+00 9.516E-03 4.029E-04 0.0 -0.138 0.150 0.150 0.0900 4 . 506E+00 3.518E-03 4.509E+00 1 .165E-02 4.41 IE-04 0.0 -0.135 0.147 0.147 0.1000 4.210E+00 3 . 559E-03 4.214E+00 1 . 395E-02 4 . 783E-04 0.0 -0.134 0.145 0.145

0 .1250 3.671 E+00 3 . 672E-03 3 . 675E+00 2.033E-02 5.672E-04 0.0 -0.130 0.141 0.141

0 . 1 500 3 . 307E+00 3.794E-03 3.311 E+00 2.751 E-02 6.51 5E-04 0.0 -0.127 0.138 0.137 0.1750 3 . 046E+00 3. 924E-03 3 . 050E+00 3.540E-02 7 . 322E-04 0.0 -0.125 0.135 0.134

0.2000 2.850E+00 4.061E-03 2 . 854E+00 4.388E-02 8. 100E-04 0 .

0

-0.123 0.133 0.132

0.2500 2 . 578E+00 4.357E-03 2 . 532E+00 6 . 236E-02 9.592E-04 0.0 -0.119 0.129 0.128

0 . 3000 2 . 40 0 E+0 0 4.630E-03 2 . 404E+00 8 . 247E-02 1 . 1 02E-03 0.0 -0.117 0.126 0.126 0.3500 2 . 276E+00 5.026E-03 2.281 E+00 1 .039E-01 1 .241E-03 0.0 -0.115 0.124 0.123

0.4000 2. 187E+00 5.394E-03 2.1 92E+00 1 . 262E-0

1

1 . 378E-03 0.0 -0.113 0.122 0.121 0.4500 2. 120E+00 5 . 732E-03 2. 126E+00 1 . 494E-0

1

1 .512E-03 0.0 -0.111 0.121 0.119

0.5000 2.069E+00 6. 189E-03 2 . 075E+00 1 .732E-01 1 .646E-03 0.0 -0.110 0.119 0.118

0.5500 2 . 0 30E+00 6.612E-03 2 . 037E+00 1 .976E-01 1 . 780E-03 0.0 -0.108 0.118 0.115

0.6000 1 . 999E+00 7 . 050E-03 2 . 006E+00 2.223E-01 1 . 91 3E-03 0.0 -0.107 0.117 0.115

0.7000 1 . 956E+00 7. 965E-03 1 . 964E+00 2.727E-01 2. 180E-03 0.0 -0.105 0.115 0.113

0.8000 1 . 928E+00 8. 927E-03 1 . 937E+00 3.240E-01 2.449E-03 0.0 -0.103 0.113 0.111

0 . 9000 1 . 91 1 E+00 9. 934E-03 1 . 921 E+00 3.759E-01 2.720E-03 0.0 -0.102 0.112 0.109

1 .0000 1 . 901 E+00 1 .098E-02 1 . 9 1 2E+00 4. 28 IE-01 2 . 994E-0 3 0.0 -0.100 0.110 0.107

1 .2500 1 . 8 92E + 0 0 1 . 375E-02 1 . 906E+00 5.592E-01 3 . 690E-03 0.0 -0.098 0.107 0.104

1 .5000 1 . 897E+00 1 .671 E-02 1 . 91 4E+00 6 . 901 E-01 4.404E-03 0.0 -0.095 0.105 0.102

1 .7500 1 . 908E+00 1 . 984E-02 1 . 927E+00 3.203E-01 5. 133E-03 0.0 -0.093 0.103 0.099

2.0000 1 . 921 E+00 2.309E-02 1 . 944E+00 9.495E-01 5 . 877E-03 0.0 -0.092 0.102 0.098

2.5000 1 . 95 1 E+00 2. 994E-02 1 . 981 E+00 1 . 204E+00 7 . 399E-03 0.0 -0.089 0.099 0.095

3.0000 1 . 981 E+00 3.716 E-02 2.01 8E+00 1 . 454E+00 8 . 959E-03 0.0 -0.087 0.097 0.092

3.5000 2.010E+00 4 . 468E-02 2 . 054E+00 1 . 700E+00 1 . 055E-02 0.0 -0.086 0.095 0.090 4.0000 2 . 036E+00 5 . 245E-02 2 . 088E+00 1 . 941 E+00 1 .21 6 E-0 2 0.0 -0.084 0.094 0.088

4.5000 2 . 060E+00 6 . 044E-02 2. 121 E+00 2. 179E+00 1 .379E-02 0.0 -0.083 0.092 0.087

5.0000 2 . 083E+00 6 . 862E-02 2 . 1 52E+00 2.41 3E+00 1 . 543E-02 0.0 -0.082 0.091 0.085

5.5000 2 . 1 04E+00 7.698E-02 2. 181 E+00 2 . 644E+00 1 . 708E-02 0.0 -0.081 0.090 0.084

6.0000 2.123E+00 3.550E-02 2.209E+00 2.871 E+00 1 . 874E-02 0.0 -0 . 080 0.089 0.083 7.0000 2 . 1 59E+00 1 .029E-01 2 . 262E+00 3.31 9E+00 2.208E-02 0.0 -0 .079 0.087 0.081 8.0000 2. 1 90E+00 1 . 203E-0

1

2.31 1 E+00 3 . 756E+00 2 . 543E-02 0.0 -0.078 0.086 0.080

9.0000 2.213E+00 1 .392E-01 2 . 357E+00 4. 184E+00 2 . 379E-02 0.0 -0.076 0.084 0.078

10.0000 2 . 244E+00 1 . 578E-0

1

2.401 E+00 4 . 605E+00 3.21 5E-02 0.0 -0.076 0.083 0.077

12.5000 2 . 298E+00 2 . 057E-0

1

2 . 504E+00 5 . 624E+00 4.051 E-02 0.0 -0 . 074 0.081 0.074

15.0000 2 . 343E+00 2.549E-01 2 . 5 98E+0 0 6 . 604E+00 4.879E-02 0.0 -0.072 0.079 0.072

17.5000 2. 381 E+00 3.053E-01 2 . 686 E+00 7 . 550E+00 5.695E-02 7 . 537E-03 -0.064 0.077 0.069

20 .0000 2.41 OE+OO 3 . 565E-0

1

2 . 767E+00 8 . 467E+00 6 . 499E-02 5 . 064E-02 -0.054 0.074 0.065 25.0000 2. 454E+00 4.607E-01 2. 91 5E+00 1 . 023E+0

1

8.071 E-02 1 . 907E-01 -0.041 0.068 0.056 30.0000 2 . 486E+00 5 . 669E-01 3 . 053E+00 1 . 1 90E+01 9 . 592E-02 3.525E-01 -0.034 0.063 0.049

35.0000 2.512E+00 6.744E-01 3. 186E+00 1 . 350E+0

1

1 .106E-01 5. 1 39E-01 -0.030 0.058 0.043 40.0000 2 . 532E+0 0 7.831E-01 3.31 5E+00 1 . 504E+0

1

1 .248E-01 6 . 676E-0

1

-0.027 0.055 0.038 45.0000 2 . 550 E+00 8. 923E-01 3 . 443E+00 1 . 552E+0

1

1 . 335E-0

1

8. 1 13E-01 -0.024 0.052 0.034 50.0000 2 . 56 5E+0 0 1 . 003E+00 3 . 568E+00 1 . 7 95E+0

1

1 .517E-01 9.464E-01 -0.023 0.049 0.031 55.0000 2 . 578E+00 1 . 1 14E+00 3 . 6 93E+00 1 . 933E+01 1 . 6 44E-0

1

1 . 072E+00 -0.021 0.046 0.029

60 .0000 2.591 E+00 1 . 226 E+0 0 3.81 7E+00 2 . 066E+0

1

1 .766E-01 1 . 1 89E+00 -0.020 0.044 0.027 70.0000 2.61 2E+00 1 .451 E+00 4 . 062E+00 2 . 320E+0

1

1 . 999E-01 1 . 403E+00 -0.019 0.041 0.023

80.0000 2 . 629E+00 1 . 677E+00 4 . 307E+00 2.559E+01 2.216E-01 1 . 593E+00 -0.018 0.038 0.021 90.0000 2 . 645E+00 1 . 905E+00 4 . 550E+00 2.785E+01 2.41 9E-01 1 . 7 6 3E+00 -0.017 0.036 0.019

1 00.0000 2 . 658E+00 2 . 1 34E+00 4 . 7 92E+0 0 2 . 999E+0

1

2.610E-01 1 . 91 7E+00 -0.017 0.034 0.017 125.0000 2 . 687E+00 2.71 OE+OO 5 . 397E+00 3 . 490E+0

1

3.037E-01 2 . 25 1 E+00 -0.015 0.030 0.015

150.0000 2.70 9E+0 0 3.291 E+00 6 . OOOE+OO 3 . 929E+0

1

3.40SE-01 2 . 529E+00 -0.014 0.028 0.013 175.0000 2 . 728E+0 0 3.874E+00 6 . 602E+00 4 . 326E+0

1

3.733E-01 2.76 9E+00 -0.013 0.026 0.011 200.0000 2 . 744E+00 4 . 460E+00 7 . 205E+00 4 . 639E+0

1

4.020E-01 2. 980E+00 -0.012 0.024 0.010 250.0000 2 . 770E+0 0 5.638E+00 8 . 408E+00 5. 330E+01 4.508E-01 3 . 34 1 E+00 -0.011 0.022 0 . 008 300.0000 2 . 7 9 1 E+0 0 6 . 822E+00 9.61 2E+00 5 . 886 E+0

1

4. 909E-01 3 . 644E+00 -0.010 0.020 0.007 350.0000 2 . 808E+00 8.009E+00 1 . 082E+0

1

6 . 376 E+0 1 5 . 244E-0

1

3. 907E+00 -0.008 0.019 0.006 400.0000 2 . 822E+00 9 . 200E+00 1 . 202E+0

1

6.314E+01 5.530E-01 4. 140E+00 -0.007 0.018 0 .006 450.0000 2 . 834E+00 1 . 039E+01 1 . 323E+0

1

7.21 1E+01 5.778E-01 4 . 349E+00 -0.006 0.017 0 .005 500.0000 2 . 845E+00 1 . 1 59E+01 1 . 443E+0

1

7 . 573E+0

1

5.994E-01 4 . 5 39E+00 -0.006 0.016 0 .004 550.0000 2 . 854E+00 1 .279E+01 1 . 564E+0

1

7. 905E+0

1

6.186E-01 4 .71 3E+00 -0.005 0.015 0.004 600.0000 2.863E+00 1 . 3 98E+0

1

1 . 685E+0

1

8.213E+01 6 . 357E-0

1

4.873E+00 -0.004 0.015 0.004 700.0000 2 . 877E+00 1 . 638E+0

1

1 . 926E+01 3.768E+01 6 . 650E-01 5 . 1 61 E+00 -0.003 0.014 0.003 300.0000 2 . 890E+00 1 .879E+01 2.1 68E+01 9 . 257E+0

1

6 .893E-01 5 . 4 1 4 E+0 0 -0.003 0.013 0.003

900.0000 2.901 E+00 2.11 9E+01 2.409E+01 9.695E+01 7. 097E-01 5 . 640 E+0 0 -0.002 0.013 0.002 1000.0000 2.91 OE+OO 2 . 360E+0

1

2.651 E+0

1

1 . 009E+02 7 . 273E-0

1

5 . 843E+00 -0.002 9.012 0.002

149
ELECTRONS IN TOLUENE

I = 62.5 eV DENSITY = 3.669E-01 g/cn 3

ENERGY STOPPING POWER CSDA RADIATION DENS .EFF. d( log[ )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR

.

COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cn 2/g MeV cm 2 /g g/cm 2

0.0100 2.285E+01 2. 960E-03 2 . 286E+0

1

2.470E-04 7.135E-05 0.0 -0.192 0.218 0.217

0.0125 1 .919E+01 2. 970E-03 1 .91 9E+01 3.669E-04 3 . 552E-05 0.0 -0.184 0 . 208 0.207

0.0150 1 .664E+01 2 . 977E-03 1 . 664E+0

1

5 . 072E-04 9. 908E-05 0.0 -0.173 0.201 0.200 0.0175 1 . 475E+0

1

2.982E-03 1 . 475E+0

1

6.671E-04 1 . 1 22E-04 0.0 -0.174 0.195 0.194

0.0200 1 .329E+01 2. 986E-03 1 . 329E+0

1

8 . 459E-04 1 .248E-04 0 . 0 -0.170 0.190 0.189

0.0250 1 . 1 1SE+01 2. 995E-03 1 . 1 18E+01 1 . 258E-03 1 . 491 E-04 0.0 -0.164 0.182 0.182

0.0300 9.71 9E+00 3.005E-03 9 . 722E+00 1 . 739E-03 1 . 724E-04 0 . 0 -0.159 0.176 0.176

0.0350 8 . 645E+00 3.01 5E-03 8 . 648E+00 2 . 285E-0

3

1 . 948E-04 0.0 -0.155 0.172 0.171 0.0400 7.820E+00 3 . 026E-03 7 . 823E+00 2.894E-03 2.164E-04 0.0 -0.152 0.168 0.168

0.0450 7. 166E+00 3 . 039E-03 7 . 1 69E+00 3.563E-03 2.374E-04 0.0 -0.150 0.165 0.164

0.0500 6 . 6 34E+00 3.052E-03 6 . 637E+00 4.233E-03 2.579E-04 0.0 -0.143 0.162 0.162

0.0550 6.1 92E+00 3.067E-03 6 . 1 95E+00 5.069E-03 2 . 778E-04 0.0 -0.146 0.160 0.159

0.0600 5.81 9E+00 3.082E-03 5 . 823E+00 5 . 902E-03 2.974E-04 0.0 -0.144 0.153 0.157

0.0700 5 . 225E+00 3. 1 13E-03 5 . 228E+00 7.713E-03 3.353E-04 0.0 -0.141 0.154 0.154

0.0800 4.771 E+00 3.147E-03 4.774E+00 9.723E-03 3.71 SE-04 0.0 -0.138 0.151 0.151 0.0900 4.41 3E+00 3. 184E-03 4.41 7E+00 1 . 1 90E-02 4.072E-04 0.0 -0.136 0.143 0.148

0.1000 4 . 1 24E+00 3.222E-03 4. 127E+00 1 . 425E-02 4.415E-04 0.0 -0.135 0.146 0.146

0.1250 3.597E+00 3.327E-03 3 . 600E+00 2.076E-02 5.238E-04 0.0 -0.131 0.142 0.142

0 .1500 3.241 E+00 3.440E-03 3 . 244E+00 2.309E-02 6 . 020E-04 0.0 -0.128 0.139 0.138

0.1750 2. 985E+00 3 . 560E-03 2.939E+00 3.614E-02 6.769E-04 0.0 -0.126 0.136 0.135

0.2000 2.793E+00 3.687E-03 2 . 797E+00 4.480E-02 7.492E-04 0.0 -0.123 0.134 0.133

0.2500 2 . 527E+00 3.960E-03 2.531 E+00 6 . 365E-0 2 3.378E-04 0 .

0

-0.120 0.130 0.129

0.3000 2 . 353E+00 4.258E-03 2 . 357E+00 3.417E-02 1 .021E-03 0 .

0

-0.118 0.127 0.126 0.3500 2 . 232E+00 4 . 576E-03 2 . 236E+00 1 .060E-01 1 . 1 50E-03 0.0 -0.115 0.125 0.124

0.4000 2 . 1 44E+00 4.915E-03 2 . 1 49E+00 1 . 288E--0

1

1 . 277E-03 0.0 -0.108 0.123 0.122

0.4500 2 . 077E+00 5.273E-03 2 . 082E+0 0 1 . 525E-0

1

1 .403E-03 2.097E-02 -0.090 0.119 0.117

0.5000 2 . 024E+00 5 . 647E-03 2 . 030E+00 1 . 763E-0

1

1 . 528E-03 4 . 725E-02 -0.084 0.114 0.112

0.5500 1 . 983E+00 6 .036E-03 1 . 989E+00 2.01 7E-01 1 . 654E-0 3 7 . 602E-02 -0.079 0.110 0.107

0 .6000 1 . 950E+00 6.438E-03 1 . 956E+00 2.271E-01 1 . 780E-03 1 .066E-01 -0.074 0.106 0.102

0.7000 1 . 90 1 E+00 7.281E-03 1 . 903E+00 2.788E-01 2.033E-03 1 .71 5E-01 -0.067 0.100 0.094

0.8000 1 . 868E+00 8. 167E-03 1 . 876E+00 3.317E-01 2.2S9E-03 2.389E-01 -0.061 0.094 0.087

0.9000 1 . 845E+00 9.092E-03 1 . 855E+00 3.853E-01 2.549E-03 3.071E-01 -0.056 0.089 0.081

1 .0000 1 . 830E+00 1 . 006E-02 1 . 840E+00 4.395E-01 2.812E-03 3.751 E- 0

1

-0.053 0.085 0.076

1 .2500 1 . 808E+00 1 .261E-02 1 . 820 E+00 5.762E-01 3 . 488E-03 5 . 402E-0

1

-0.046 0.076 0.067

1 .5000 1 .300E+00 1 . 534E-02 1 .315E+00 7.138E-01 4. 187E-03 6 . 953E-01 -0.041 0 . 070 0.059

1 .7500 1 . 799E+00 1 .821E-02 1 . 8 1 7E+00 8.515E-01 4 . 908E-03 8 . 395E-0

1

-0.038 0.065 0.054

2.0000 1 .801 E+00 2. 121E-02 1 . 823E+00 9.889E-01 5.648E-03 9.733E-01 -0.036 0.061 0 . 050 2.5000 1 . 8 1 2E+00 2 . 753E-02 1 . 839E+0 0 1 . 262E+00 7. 177E-03 1.21 3E+00 -0 .033 0.055 0.044

3.0000 1 . 824E+00 3.41 9E-02 1 . 858E+00 1 . 533E+00 8 . 760E-03 1 . 423E+00 -0.031 0.051 0.040

3.5000 1 . 837E+0 0 4. 1 12E-02 1 .878E+00 1 .300E+00 1 . 039E-02 1 . 60 9E + 00 -0.029 0.048 0.037

4.0000 1 . 349E+00 4 . 830E-02 1 . 898E+00 2 . 065E+00 1 . 205E-02 1 . 776E+00 -0.028 0.045 0.035

4.5000 1 .86 1 E+00 5.563E-02 1 . 91 7E+00 2 . 327E+0 0 1 . 374E-02 1 . 927E+00 -0.027 0 .043 0.033

5.0000 1 . 872E+00 6 . 324E-02 1 . 935E+00 2 . 587E + 00 1 .545E-02 2 . 066E+00 -0.026 0.041 0.031 5.5000 1 . 882E+00 7 .097E-02 1 . 953E+00 2 . 844E+00 1 -718E-02 2.1 93E+00 -0.025 0.040 0.030 6.0000 1 .392E+00 7 . 8S3E-02 1 . 971 E+00 3 . 0 99E + 00 1 .893E-02 2. 312E+00 -0.024 0.033 0.029

7.0000 1 . 909E+00 9.496E-02 2 . 004E+00 3 . 602E+00 2 . 247E-02 2 . 528E+00 -0.022 0.036 0.027 3.0000 1 . 924E+00 1.11 5E-01 2 . 036E+00 4 . 0 97 E + 00 2 . 604E-02 2.720E+00 -0.021 0.034 0.025

9.0000 1 . 937E+00 1 . 235E-0

1

2 . 066E+00 4 . 585E+00 2. 965E-02 2 . 8 94E+00 -0.020 0.033 0.024

10.0000 1 . 949E+00 1 . 457E-0

1

2 . 095E+00 5 . 065E+00 3 . 327E-02 3 . 0 53E+00 -0.018 0.031 0.023

12.5000 1 . 974E+00 1 . 900E-01 2 . 1 64E+00 6 . 239E+00 4.236E-02 3 . 403E+00 -0.015 0.028 0.020

15.0000 1 . 994E+00 2.357E-01 2 . 229E+00 7 . 377E+00 5. 143E-02 3.701 E+00 -0.012 0.026 0.018

17.5000 2.010E+00 2.823E-01 2 . 292E+00 8 . 483E+00 6.044E-02 3. 962E+00 -0.010 0.024 0.016 20.0000 2 . 023E+00 3.297E-01 2. 353E+00 9 . 560E+00 6 . 935E-02 4 . 1 95E+00 -0.009 0.022 0.014

25.0000 2 . 045E+00 4.264E-01 2 . 47 1 E+00 1 . 163E+01 8 . 678E-02 4 . 595E+00 -0.006 0.019 0.011 30.0000 2 . 062E+00 5.248E-01 2 . 587E+00 1 .361E+01 1 .036E-01 4. 932E+00 -0.005 0.017 0.009

35.0000 2.076 E+0 0 6.246E-01 2.701 E+00 1 . 550E+0

1

1 . 1 99E-01 5.221 E+00 -0.003 0.015 0.007

40.0000 2 . 088E+0 0 7.254E-01 2.81 4E+00 1 . 732E i 0

1

1 .355E-01 5 . 476E+00 -0.003 0.014 0.006 45.0000 2 . 0 99E+00 S.273E-01 2. 926E+00 1 . 906E+01 1 .505E-01 5 . 702E+00 -0.002 0.013 0.005

50.0000 2. 108E+00 9.297E-01 3 . 038E+00 2 . 073E+0

1

1 . 649E-0

1

5. 906E+00 -0.002 0.012 0 .005 55.0000 2.1 16E+00 1 . 033E + 00 3. 149E+00 2 . 235E+0

1

1 . 787E-01 6 . 091 E+00 -0.002 0.01! 0.004

60.0000 2. 124E+00 1 . 1 37E+00 3 . 260E+00 2.391E+01 1 . 920E-01 6.261 E+00 -0.001 0.010 0.004 70.0000 2.1 37E+00 1 . 345E+00 3 . 433E+00 2 . 688E+0

1

2.171E-01 6 . 56 3E+00 -0.001 0.009 0.003

80.0000 2. 149E+00 1 . 556 E+OO 3 . 704E+00 2. 966E+01 2.404E-01 6 . 825E+00 -0.001 0.009 0.002

90.0000 2 . 1 59E+00 1 . 763E+00 3 . 926E+0 0 3.228E+01 2.621E-01 7 . 058E+00 -0.001 0.008 0.002

100.0000 2. i 68E+00 1 . 980E+00 4. 148E+00 3 . 476E+0

1

2.823E-01 7 . 266E+00 -0.001 0.007 0.002

125.0000 2. 186E+00 2.51 6E+00 4 . 702E+00 4 . 042E+0

1

3.273E-01 7 . 708E+00 -0.000 0.006 0.001

1 50.0000 2 . 202E+00 3 . 055E+00 5 . 257E+00 4.544E+01 3.659E-01 8.071 E+00 -0.000 0.006 0.001 175.0000 2.21 5E+00 3 . 593E+00 5.31 3E+00 4.996E+01 3. 994E-01 3 . 377 E+0 0 -0.000 0.005 0.001

200 . 0000 2 . 226E+00 4. 143E+00 6.369E+00 5 . 407E+0

1

4.289E-01 8 . 643E+00 -0.000 0.005 0.001 250.0000 2 . 245E+00 5 . 238E+00 7 . 483E+0 0 6.131E+01 4.784E-01 9 . 088E+00 -0.000 0.004 0.001 300.0000 2 . 260E+00 6 . 339E+00 8. 599E+00 6 . 754E+0

1

5. 186E-01 9 . 452E+00 -0.000 0.004 0.000 350.0000 2 . 273E+00 7 . 444E+00 9.71 7E+00 7 . 300E+01 5.520E-01 9.759E+00 -0.000 0.004 0.000 400.0000 2 . 284E+00 &.55ZZ-00 1 . 084E+0

1

7 . 787E+0

1

5.802E-01 1 . 003E+0

1

-0.000 0.003 0.000 450.0000 2 . 294E+00 9 . 662E+00 1 . 1 96E+01 8 . 226E+0

1

6 . 045E-01 1 . 02SE+0

1

-0.000 0.003 0.000 500.0000 2 . 303E+00 1 . 077E+0

1

1 . 308E+0

1

3 . 626E+0

1

6 . 257E-01 1 . 047E+01 -0.000 0.003 0 . 000 550.0000 2.31 1E+00 1 . 139E+01 1 .420E+01 8 . 993E+01 6.444E-01 1 . 066E+01 -0.000 0.003 0.000 600.0000 2.31 8E+00 1 . 300E+0

1

1 . 532E+0

1

9 . 332E+01 6.609E-01 1 . 084 E+0

1

-0.000 0.003 0.000 700.0000 2.33IE+00 1 . 524E+ 0

1

1 . 7 57E+0

1

9.941 E+0

1

6.891E-01 1 . 114E+01 -0.000 0.003 0.000 800.0000 2. 342E+00 1 . 747E+01 1 . 982E+0

1

1 . 048E+02 7. 124E-01 1 .141 E+0

1

-0.000 0.003 0.000

900.0000 2 . 352E+00 1 . 972E+01 2 . 207E+0

1

1 . 095E+02 7.319E-01 1 . 1 65E+01 -0.000 0.002 0.000 1000.0000 2 . 360E+00 2.1 96E+01 2 . 432E+01 1 . 1 3 9E+02 7.485E-01 1 . 186E+01 -0 . 000 0.002 0.000

150
ELECTRONS IN WATER, LIQUID

I = 75.0 eV DENSITY = 1 . 000E + 0Ci g/cm 2

ENERGY STOPPING POWER CSDA RADIATION DENS. EPF. d ( log )/d( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 2.256E+01 3.398E-03 2 . 257E+0

1

2.515E-04 9 . 408E-0 5 0.0 -0.199 0.227 0.225 0.0125 1 . 8 97E + 0

1

3 . 927E-03 1 . 8 98E+0

1

3.728E-04 1 . 1 33E-04 0.0 -0.190 0.217 0.215

0.0150 1 .647E+01 3. 944E-03 1 . 647E+0

1

5. 147E-04 1 .316E-04 0 .

0

-0.184 0.208 0.207 0.0175 1 .461E+01 3. 955E-03 1 .461 E+0

1

6.761E-04 1 . 4 92E-04 0 .

0

-0.179 0.202 0.201

0 .0200 1 .317E+01 3. 963E-03 1 .318E + 01 8.566E-04 1 . 663E-04 0 .

0

-0.175 0.197 0.196 0.0250 1 .109E+01 3 . 974E-03 1 . 1 10E + 01 1 . 272E-03 1 . 990E-04 0.0 -0.169 0.189 0.188

0.0300 9 . 653E+00 3. 984E-03 9 . 657E+00 1 .756E-03 2.301 E-04 0.0 -0.164 0.182 0.182

0.0350 8 . 592E+00 3. 994E-03 8 . 596E+00 2.306E-03 2.599E-04 0.0 -0.160 0.177 0.177 0.0400 7 . 777E+00 4. 005E-03 7.781 E+00 2.91 9E-03 2 . 886 E-04 0.0 -0.157 0.173 0.173

0.0450 7.130E+00 4.018E-03 7 . 1 34E+00 3.591E-03 3. 165E-04 0.0 -0.154 0.170 0.170

0 . 0500 S .S03E+00 4.031E-03 6 . 607E+00 4.320E-03 3.435E-04 0 .

0

-0.152 0.167 0.167

0.0550 6 . 166E+00 4.046E-03 6 . 1 70E+00 5. 1 03E-03 3.698E-04 0 .

0

-0.150 0.165 0.164

0.0600 5 . 7 97E+00 4 . 062E-03 5.801 E+00 5 . 940E-03 3.955E-04 0.0 -0.148 0.162 0.162

0.0700 5 . 207E+00 4.098E-03 5.21 1 E+00 7.762E-03 4 . 452E-04 0.0 -0.145 0.158 0.158 0.0800 4 . 757E + 00 4.138E-03 4 . 762E+00 9 . 773E-03 4 . 931 E-04 0.0 -0.142 0.155 0.155

0.0900 4 . 402E+00 4.181E-03 4 . 407E+00 1 . 1 96E-02 5.393E-04 0 .0 -0.140 0.153 0.152

0.1000 4. 1 15E+00 4.228E-03 4. 120E+00 1 -431E-02 5.841 E-04 0.0 -0.138 0.150 0.150

0 .1250 3.591 E+00 4.355E-03 3 . 596E+00 2 . 083E-02 6 . 91 2E-04 0 . 0 -0.134 0.146 0.145

0.1500 3 . 238E+00 4.494E-03 3 . 242E+00 2.317E-02 7.926E-04 0.0 -0.131 0.142 0.142

0.1750 2. 984E+00 4 . 643E-03 2. 988E+00 3.622E-02 8 . 8 94E-0 4 0.0 -0.128 0.139 0.139

0.2000 2 . 793E+00 4.801E-03 2 . 798E+00 4.437E-02 9 . 326E-04 0.0 -0.126 0.137 0.136 0.2500 2 . 528E+00 5. 141E-03 2 . 533E+00 6.372E-02 1 .161E-03 0 .

0

-0.123 0.133 0.132

0.3000 2 . 355E+00 5.514E-03 2. 360E+00 8.421E-02 1 .331E-03 0.0 -0.120 0.130 0.129

0 . 3500 2 . 235E+00 5. 91 3E-03 2 . 24 1 E+00 1 .060E-01 1 . 496E-0 3 0 .

0

-0.118 0.123 0.127 0.4000 2.148E+00 6.339E-03 2 . 1 54E+00 1 . 238E-0

1

1 . 6 58E-0 3 0.0 -0.116 0.126 0.125 0.4500 2. 083E+00 6 . 737E-03 2 . 090E+00 1 . 523E-0

1

1 .818E-03 0.0 -0.114 0.124 0.123

0.5000 2. 034E+00 7.257E-03 2.041 E+00 1 .766E-01 1 . 976E-03 0 .

0

-0.111 0.123 0.121

0 .5500 1 . 995E+00 7.747E-03 2 . 003E+00 2. 01 3E-01 2. 134E-03 1 . 103E-02 -0.094 0.120 0.118

0 .6000 1 . 963E+00 8 . 254E-03 1 . 972E+00 2.265E-01 2 . 292E-03 2. 938E-02 -0.088 0.117 0.114

0 . 7000 1 . 91 7E+00 9.312E-03 1 . 926E+00 2.778E-01 2. 608E-03 7.435E-02 -0.078 0.110 0.106 0.8000 1 . 88 6E + 0 0 1 . 043E-02 1 . 896E+00 3 . 302E-01 2. 928E-03 1 . 267E-0

1

-0.070 0.105 0.099

0.9000 1 . 864E+00 1 . 1 59E-02 1 . 876E+00 3.832E-01 3.251E-03 1 . 335E-0

1

-0.064 0.099 0.093

1 .0000 1 . 849E+00 1 . 2S0E-02 1 . 862E+00 4.367E-01 3. 579E-03 2 . 428E-0

1

-0.059 0.095 0 . 087

1 .2500 1 . 829E+00 1 . 600E-02 1 . 845E+00 5.717E-01 4.416E-03 3.944E-01 -0.049 0.085 0.075

1 .5000 1 . S22E+0 0 1 . 942E-02 1 .841 E+00 7 .075E-01 5.281E-03 5 . 437E-01 -0.043 0.077 0.066

1 .7500 1 .821 E+00 2.303E-02 1 . 844E+00 8.432E-01 6.171 E— 0 3 6 .866E-01 -0.033 0.071 0.059

2.0000 1 . 824E+00 2 . 678E-02 1 . 8 50 E+0 0 9.785E-01 7 . 085E-03 8.218E-01 -0.035 0.066 0.053 2.5000 1 . 834E+0 0 3.463E-02 1 . 868E+00 1 . 247E+0Q 8 . 969E-03 1 . 069E+00 -0.030 0.059 0.045

3.0000 1 .846E+00 4 . 299E-02 1 .889E+00 1 . 51 4E+00 1 . 0 92E-02 1 . 288E+00 -0 .027 0.054 0.040

3.5000 1 .858E+00 5.1 64E-02 1 . 91 0E+00 1 . 777E+00 1 .291E-02 1 . 484E+00 -0.025 0.049 0.036

4 .0000 1 . 870E+00 6 . 058E-02 1 . 931 E+00 2 . 037E+00 1 . 495E-02 1 . 660E+00 -0.024 0.046 0.033 4.5000 1 . 882E+00 6 . 976E-02 1 . 951 E+00 2 . 295E+00 1 . 702E-02 1 .821 E+00 -0.023 0.043 0.031 5.0000 1 . 892E+00 7.91 7E-02 1 . 971 E+00 2 . 550E+00 1.911 E-02 1 . 9S7E+00 -0.022 0.041 0.029

5 . 5000 1 . 902E+00 8.876E-02 1 . 991 E+00 2 . 802E+00 2.123E-02 2. 102E+00 -0.021 0.039 0.027

6 .0000 1.91! E+00 9 . 854E-02 2.01 0E+00 3 . 052E+00 2 . 336 E-02 2 . 227E+00 -0.021 0.038 0.026 7.0000 1 . 928E+00 1 . 185E-01 2 . 047E+00 3 . 545E+00 2 . 76 6 E-0 2 2 . 453E+00 -0.020 0.035 0.024 8.0000 1 . 943E+00 1 .391E-01 2 . 082E+00 4 . 0 30 E + 0 0 3.200E-02 2 . 652E+00 -0.019 0.033 0.023

9.0000 1 . 956E+00 1 .601E-01 2. 1 1 6E+00 4 . 506E+00 3 . 636E-02 2.331 E+00 -0.018 0.031 0.021 10.0000 1 . 968E+00 1 -814E-01 2. 149E+00 4. 975E+00 4.072E-02 2. 992E+00 -0.018 0.030 0.020 12.5000 1 . 993E+00 2.362E-01 2 . 230E+00 6 . 1 1 7E+00 5. 163E-02 3.341 E+00 -0.016 0.027 0.019

15.0000 2. 01 4E+00 2. 926E-01 2 . 306E+00 7.21 9E+00 6 . 243E-02 3 . 633E+00 -0.015 0.025 0.017 17.5000 2.031E+00 3.501E-01 2.381 E+00 8 . 286E+00 7 . 309E-02 3 . 885E+00 -0.014 0.024 0.016

20 .0000 2 . 046E+00 4.086E-01 2 . 454E+00 9 . 320E+00 8 . 355E-02 4. 107E+00 -0.013 0.022 0.015

25.0000 2 . 070 E+00 5.277E-01 2 . 598E+00 1 . 1 30 E+0 1 1 . 0 3 9E-0

1

4 . 487E + 00 -0.010 0.020 0.013

30 .0000 2.089E+00 6 . 489E-0

1

2 . 738E+00 1 .317E + 01 1 . 233E-0

1

4 . 306E+00 -0.009 0.018 0.011 35.0000 2 . 1 05E+00 7.716E-01 2.876 E+00 1 . 496E+0

1

1 .418E-01 5 . 032E+00 -0.007 0.017 0.010 40.0000 2.1 18E+00 8. 955E-01 3 . 01 3E+00 1 . 665E+01 1 . 5 94E-0

1

5 . 326E+00 -0 .006 0.015 0.009

45 .0000 2. 129E+00 1 .021 E+00 3. 150E+00 1 . 828E+0

1

1 . 762E-0

1

5 . 544E+0 0 -0.005 0.014 0 .008 50.0000 2.1 39E+00 1 . 1 46E+00 3 . 286E+00 1 . 983E+01 1 . 923E-01 5.741 E+00 -0.004 0.014 0.007 55.0000 2. 148E+00 1 . 273E+00 3.421 E+00 2.132E+01 2 . 076E-0

1

5 . 921 E+00 -0.004 0.013 0.006 60.0000 2.1 56E+00 1 . 400E+00 3 . 556 E+00 2 . 276E+0

1

2.222E-01 6 . 087E+00 -0.003 0.012 0.006 70.0000 2. 170E+00 1 . 656E+00 3.327E+00 2 . 547E+0

1

2.496E-01 6 . 383E+00 -0.002 0.011 0.005 80.0000 2. 182E+00 1 . 91 4E+00 4 . 0 96 E+00 2 . 799E+01 2 . 747E-0

1

5.641 E+00 -0 .002 0.010 0.004 90.0000 2.1 93E+00 2 . 1 73E+00 4 . 366E+00 3.035E+01 2.978E-01 6 .871 E+00 -0.002 0.009 0.003 100.0000 2 . 202E+0 0 2 . 434E+00 4 . 636E+00 3 . 258E+0

1

3.192E-01 7 . 077E+00 -0.001 0.009 0.003 125.0000 2 . 222E+00 3 . 089E+00 5.311 E+00 3.761 E+0

1

3.662E-01 7 . 51 6E+00 -0.001 0.008 0.002

1 50 .0000 2 . 238E+00 3 . 749E+00 5. 987E+00 4 . 204E+0

1

4 . 060E-0

1

7 . 876E+00 -0.001 0.007 0.002

175.0000 2.251 E+00 4.41 2E+00 6 . 663E+00 4.600E+01 4.401 E-01 3 . 1 32E + 00 -0.001 0 .006 0.001 200.0000 2 . 263E+00 5 . 078E+00 7.341 E+00 4. 957E+01 4.698E-01 8 . 447E+00 -0.000 0 . 006 0.001 250.0000 2.282E+00 6 . 41 6E+00 8 . 6 98E+00 5 . 532E+0

1

5.1 90 E-01 8.891 E+00 -0.000 0.005 0.001 300.0000 2.297E+00 7 . 760 E+0 0 1 . 0 06E + O

1

6 . 1 1 6E+01 5 . 584E-0

1

9 . 254E+00 -0.000 0.005 0.001 350.0000 2.311 E+00 9 . 1 07E+00 1 . 1 42E+01 6 . 583E+0

1

5. 908E-01 9.561 E+00 -0.000 0.005 0.001 400.0000 2 . 322E+00 1 . 046E+01 1 . 278E+0

1

6 . 996E+01 6 . 180E-01 9 . 827E+00 -0.000 0.004 0.001 450.0000 2. 332E+00 1.181 E+0

1

1 . 4I4E+01 7 . 363E+0

1

6 .412E-01 1 . 006E+0

1

-0 .000 0 .004 0 .000 500.0000 2.341E+00 1 .317E+C1 1 . 551 E+0

1

7 . 705E+0

1

6.613E-01 1 . 027E+0

1

-0 .000 0.004 0 .000 550.0000 2. 349E+00 1 . 453E+0

1

1 . 688E+0

1

8.014E+01 6 . 789E-01 1 . 0 46 E + 0

1

-0.000 0 .004 0 .000 600.0000 2 . 357E+00 1 . 589E+01 1 . 824E+0

1

3 . 299E+01 5 . 945E-01 1 . 064E+01 -0.000 0.004 0 . 000 700.0000 2 . 370E+00 1-861 E+0

1

2.093E+01 3.810E+01 7 .209E-01 1 . 0 94E+0

1

-0.000 0.003 0.000 800.0000 2.381E+00 2.133E+01 2 . 37 1 E+0

1

9 . 258E+0

1

7 . 425E-0

1

1 . 1 2 1 E+0

1

-0.000 0.003 0.000 900.0000 2.391 E+00 2 . 406E+0

1

2 . 645E+0

1

9 . 657E+01 7 . 605E-0

1

1 . 145E+01 - 0.000 0.003 0.000 1000.0000 2 . 400E+00 2 . S79E+0

1

2.91 9E+01 1 . 0 0 2 E + 0 2 7 . 759E-0

1

1 . 1 66E+01 - 0.000 0.003 0.000

151
ELECTRONS IN WATER * LIQUID (#)

I = 75.0 eV DENSITY = 1 . 000E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d ( logI )/d ( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV c» 2 /g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 2.256E+01 3 . 898E-03 2 . 257E+0

1

2.515E-04 9.408E-05 0.0 -0.199 0.227 0.225 0.0125 1 . 397E+0

1

3. 927E-03 1 . 398E + 0

1

3.728E-04 1 . 1 33E-04 0.0 -0.190 0.217 0.215

0.0150 1 . 6 47E+0

1

3. 944E-03 1 . 647E+0

1

5. 147E-04 1 . 31 6E-04 0.0 -0.184 0 . 203 0.207 0.0175 1 .461E+01 3 . 955E-03 1 .461 E+01 6.761E-04 1 . 492E-04 0.0 -0.179 0.202 0.201 0.0200 1 . 31 7E+01 3. 963E-03 1 .318E+01 8 . 566E-04 1 . 663E-04 0 .0 -0.175 0.197 0.196 0.0250 1 . 1 09E+01 3. 974E-03 1 . 1 10E+01 1 . 272E-03 1 . 990E-04 0.0 -0.169 0.189 0.138

0.0300 9 . 653E+00 3.984E-03 9 . 657E+00 1 .756E-03 2.301 E-04 0.0 -0.164 0.182 0.182 0.0350 3 . 592E+00 3. 994E-03 8 . 596E+00 2 . 306E-03 2 . 599E-04 0.0 -0.160 0.177 0.177

0.0400 7 . 777E+00 4 . 005E-03 7.781 E+00 2.91 9E-03 2.336E-04 0.0 -0.157 0.173 0.173

0.0450 7.1 30E+00 4.018E-03 7.134E+00 3.591E-03 3 . 1 65E-04 0.0 -0.154 0 . 170 0.170 0.0500 6 . 603E+00 4.031E-03 6 . 607E+00 4 . 320E-03 3.435E-04 0 .0 -0.152 0.167 0.167

0.0550 6. 166E+00 4 . 046E-03 6 . 1 70E+00 5.1 03E-03 3.698E-04 0 .

0

-0.150 0.165 0.164

0.0600 5 . 7 97E+00 4.062E-03 5.801 E+00 5. 940E-03 3. 955E-04 0 . 0 -0.148 0.162 0.162

0.0700 5 . 207E+00 4.098E-03 5.21 1 E+00 7.762E-03 4.452E-04 0 . 0 -0.145 0.158 0.153

0.0800 4 . 757E+0 0 4.1 38E-03 4 . 762E+00 9.773E-03 4 . 931 E-04 0.0 -0.142 0.155 0.155

0.0900 4 . 402E+00 4. 131E-03 4.407E+00 1 . 1 96E-02 5 . 393E-04 0 .

0

-0.140 0.153 0.152

0.1000 4.11 5E+00 4.228E-03 4 . 1 20E+00 1 .431E-02 5.841 E-04 0.0 -0.138 0.150 0.150

0.1250 3.591 E+00 4.355E-03 3 . 596E+00 2.083E-02 6 . 91 2E-04 0.0 -0.134 0.146 0.145

0.1500 3 . 238E+00 4.494E-03 3 . 242E+00 2.817E-02 7.926E-04 0.0 -0.131 0.142 0.142

0.1750 2 . 984E+00 4 . 643E-03 2. 938E+00 3 . 622E-02 8.894E-04 0.0 -0.128 0.139 0.139

0 . 2000 2 . 7 9 3E+0 0 4.801E-03 2 . 798E+0 0 4.487E-02 9 . 826E-04 0.0 -0.126 0.137 0.136

0.2500 2 . 528E+0 0 5.141E-03 2. 533E+00 6 . 372E-02 1 .161E-03 0.0 -0.123 0.133 0.132

0 . 3000 2 . 355E+0 0 5.514E-03 2 . 360E+00 8.421E-02 1 .331 E-03 2. 187E-03 -0.120 0.130 0.129

0.3500 2 . 233E+00 5.913E-03 2 . 239E+00 1 . 060E-0

1

1 .497E-03 1 .051 E-02 -0.118 0.128 0.127

0.4000 2. 145E+00 6 . 339E-03 2 . 1 52E+00 1 . 288E-0

1

1 .659E-03 2. 188E-02 -0.116 0.126 0.125

0.4500 2.079E+00 6 . 787E-03 2 . 086E+00 1 . 524E-0

1

1 .81 9E-03 3.663E-02 -0.114 0.124 0.123

0.5000 2 . 028E+00 7.257E-03 2 . 0 35E+0 0 1 .767E-01 1 . 978E-03 5.424E-02 -0.111 0.123 0.121 0.5500 1 . 988E+00 7 . 747E-0 3 1 . 996E+00 2.015E-01 2.137E-03 7 . 393E-02 -0.094 0.120 0.118

0.6000 1 . 956E+00 8.254E-03 1 . 965E+00 2.268E-01 2 . 2 95E-0 3 9.533E-02 -0.088 0.117 0.114

0.7000 1 . 91 0E+00 9. 31 2E-03 1 .91 9E+00 2.733E-01 2.614E-03 1 . 422E-0

1

-0.078 0.110 0.106 0.8000 1 .879E+00 1 .043E-02 1 . 890E+00 3 . 308E-01 2. 935E-03 1 . 925E-0

1

-0.070 0.105 0.099

0 . 9000 1 . 858E+00 1 . 159E-02 1 . 870E + 0 0 3.841E-01 3.260E-03 2.448E-01 -0.064 0.099 0.093

1 .0000 1 . 844E+00 1 . 280E-02 1 . 857E+00 4.378E-01 3.588E-03 2. 983E-01 -0.059 0.095 0.087

1 .2500 1 .825E+00 1 . 600E-02 1 .841 E+00 5.731E-01 4.428E-03 4.331 E-0

1

-0.049 0 .085 0.075

1 .5000 1 . 820E+00 1 . 942E-02 1 .839E+00 7.090E-01 5 . 293E-03 5.648E-01 -0.043 0.077 0.066

1 .7500 1 .821 E+00 2.303E-02 1 . 844E+00 8.448E-01 6 . 1S3E-03 5.91 IE-01 -0.038 0.071 0.059

2.0000 1 .825E+00 2.678E-02 1 .851 E+00 9.801E-01 7 . 094E-03 8.11 9E-01 -0.035 0.066 0.053

2.5000 1 . 837E+00 3.468E-02 1 .871 E+00 1 . 249E+00 8.973E-03 1 . 0 36E + 00 -0.030 0.059 0.045

3.0000 1 . 850E+00 4.299E-02 1 . 8 93E+00 1 . 51 4E+00 1 .091E-02 1 . 238E+00 -0.027 0.054 0 . 040 3.5000 1 .864E+00 5.164E-02 1 . 91 6E+00 1 . 777E+00 1 .290E-02 1 .41 9E+00 -0.025 0.049 0.036 4.0000 1 -877E+00 6.058E-02 1 . 937E+00 2 . 037E+00 1 . 493E-02 1 . 585E+00 -0.024 0.046 0.033

4.5000 1 . 889E+00 6 . 976E-02 1 . 958E+00 2 . 2 93E+0 0 1 . 698E-02 1 . 738E+C0 -0.023 0.043 0.031 5.0000 1 . 900E+00 7 . 91 7E-02 1 . 979E+00 2 . 547E+00 1 . 907E-02 1 . 880E+00 -0 .022 0.041 0.029

5.5000 1 . 91 0E+00 8 . 876E-02 1 . 999E+00 2 . 7 99E+00 2.1 17E-02 2.011 E+00 -0.021 0.039 0.027

6 .0000 1 .91 9E+00 9.854E-02 2.01 SE+00 3 . 048E+00 2.329E-02 2.1 33E+00 -0.021 0.038 0.026 7.0000 1 . 936E+00 1 . 185E-01 2 . 055E+00 3.539E+00 2. 757E-02 2. 359E+00 -0.020 0.035 0.024

8.0000 1 . 95 1 E+00 1 .391E-01 2 . 0 90 E + 0 0 4.021 E+00 3. 189E-02 2 . 555E+00 -0.019 0.033 0.023

9.0000 1 . 964E+00 1 .601E-01 2.124E+00 4 . 496E+00 3 . 623E-02 2 . 7 36 E+00 -0.018 0.031 0.021 10.0000 1 . 976E+00 1 .814E-01 2. 157E+00 4 . 963E+00 4 . 058E-Q2 2. 900E+00 -0.018 0.030 0 . 020 12.5000 2 . 000E+00 2.362E-01 2 . 237E+00 6.101 E+00 5. 145E-02 3 . 257E+00 -0.016 0.027 0.019

15.0000 2 . 020E+00 2. 926E-01 2.31 3E+00 7 . 200E+00 6 . 222E-0 2 3 . 558E+00 -0.015 0.025 0.017

17.5000 2 . 037E+00 3.501E-01 2. 387E+00 8 . 264E+00 7.286E-02 3.81 9E+00 -0.014 0.024 0.016 20.0000 2.051 E+00 4.086E-01 2.459E+00 9 . 295E+00 8.331E-02 4 . 050E+00 -0.013 0.022 0.015

25.0000 2. 074E+00 5.277E-01 2.601 E+00 1 . 1 27E+0

1

1 .036E-01 4 . 444E+00 -0.010 0.020 0.013

30 . 0000 2. 092E+00 6 . 489E-0

1

2.741 E+00 1 .314E+01 1 . 233E-0

1

4 . 773E+00 -0.009 0.018 0.011 35.0000 2. 107E+00 7.716E-01 2 . 878E+0 0 1 . 4 92E+0

1

1 .415E-01 5 . 056E+00 -0.007 0.017 0.010

40 . 0000 2 . 1 20E + 00 8. 955E-01 3.015E+00 1 . 6 62E+0

1

1 . 592E-0

1

5 . 305E+00 -0 .006 0.015 0.009

45.0000 2.131 E+00 1 .021 E+00 3. 1 51 E+00 1 . 824E+0

1

1 .760E-01 5 . 527E+00 -0.005 0.014 0 . 008

50 .0000 2. 1 41 E+00 1 . 1 46E+00 3 . 287E+00 1 . 980E+01 1 .920E-01 5 . 726E+00 -0.004 0.014 0.007

55.0000 2. 149E+00 1 . 273E+00 3 . 422E+00 2.129E+01 2.074E-01 5. 908E+00 -0.004 0.013 0.006 60.0000 2. 157E+00 1 . 400E+00 3 . 558E+00 2 . 272E+0

1

2 . 220E-01 6 . 074E+00 -0.003 0.012 0.006 70.0000 2.171 E+00 1 . 656E+00 3.823E+00 2 . 543E+0

1

2.494E-01 6 . 372E + 00 -0.002 0.011 0.005 80.0000 2. 183E+00 1 . 91 4E+00 4 . 0 97E+00 2 . 795E+0

1

2. 745E-01 6 .631 E+00 -0.002 0.010 0.004

90.0000 2.1 94E+00 2 . 1 73E+00 4 . 367E+00 3.032E+01 2. 976E-01 6.861 E+00 -0.002 0.009 0 .003

1 00 .0000 2 . 203E+00 2 . 434E+00 4 . 637E+00 3.254E+01 3. 1 90E-01 7 . 067E+00 -0.001 0.009 0.003

125.0000 2 . 223E+0 0 3 . 089E+00 5.31 2E+00 3 . 757E+0

1

3.661 E-0

1

7 . 505E+00 -0.001 0.008 0 .002 150.0000 2 . 239E+0 0 3 . 749E+00 5 . 988E+00 4 . 200E+0

1

4.058E-01 7.364E+00 -0.001 0.007 0.002

175.0000 2 . 252E+00 4.41 2E+00 6 . 664E+00 4 . 596 E+0

1

4.400E-01 3.17 0 E + 0 0 -0.001 0.006 0.001 200.0000 2 . 264E+00 5. 078E+00 7 . 342E+00 4. 953E+01 4 . 6 96 E-0

1

8 . 434E+00 -0.000 0.006 0.001 250.0000 2 . 283E+00 6 . 41 6E+00 8 . 6 99E+00 5.578E+01 5. 189E-01 8 . 878E+00 -0.000 0.005 0.001 300.0000 2 . 298E+00 7 . 760E+00 1 . 006E+0

1

6 . 1 12E+01 5.583E-01 9 . 243E+00 -0.000 0.005 0.001 350.0000 2.31 2E+00 9. 107E+00 1 .142E+01 6 . 578E+0

1

5.907E-01 9.551 E+0 0 -0.000 0.005 0.001 400.0000 2. 323E+00 1 . 046E+0

1

1 . 278E+0

1

6 . 992E+01 6.179E-01 9.81 8E+00 -0.000 0.004 0.001 450.0000 2 . 333E+00 1 . 181 E+01 1 .415E+01 7.364E+01 6.41 IE-01 1 . 005E+0

1

-0.000 0.004 0.000 500.0000 2.342E+00 1 .317E+01 1 .551 E+01 7.701 E+01 6.612E-01 1 . 0 27 E + 0 1 -0.000 0.004 0.000

550 .0000 2 . 350E+00 1 . 453E+0

1

1 . 633E+0

1

8 .01 0E+01 6.783E-01 1 . 046 E+0

1

-0.000 0.004 0.000

600 . 0000 2 . 357E + 0 0 1 . 589E+01 1 . 824E+0

1

8 . 295E+0

1

6 . 944 E-0

1

1 . 063E+01 -0.000 0.004 0.000 700.0000 2 . 370E+00 1 .861E+01 2.098E+01 8 . 80 6 E+0

1

7 . 208E-0

1

1 . 094E+01 -0.000 0.003 0.000

800 . 0000 2 . 332E+00 2.1 33E+01 2.371 E+0

1

9 . 254E+0

1

7.424E-01 1 . 121E+01 -0 .000 0.003 0 .000

900 . 0000 2 . 392E+0 0 2.406E+01 2. 645E+01 9 . 653E+0

1

7 . 605E-01 1 . 1 45E+01 -0.000 0 .003 o.ooo 1000.0000 2 . 400E+00 2 . 679E+0

1

2.91 9E+01 1 .001E+02 7.758E-01 1 . 1 66E+01 -0.000 0.003 0.000

k Evaluated with the density-effect correction of Ashley (1982b).

IS
i

& .

ELECTRONS IN WATER VAPOR

I = 71.6 eV DENSITY = 7.562E-04 g/cm 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS .EFF. d( log )/d( log I

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 2 . 277E+0

1

3.398E-03 2 . 277E+0

1

2 . 489E-04 9.31 IE-05 0 .

0

-0.197 0.225 0 . 223 0.0125 1 . 91 4E+01 3 . 927E-03 1 . 91 4E+01 3.691E-04 1 . 121E-04 0.0 -0.189 0.214 0.213

0.0150 1 .661E+01 3. 944E-03 1 .661E+01 5.097E-04 1 . 303E-04 0.0 -0.183 0.206 0.205 0.0175 1 .473E+01 3.955E-03 1 .474E+01 6.699E-04 1 . 479E-04 0.0 -0.178 0.200 0.199

0.0200 1 . 328E + 0 1 3.963E-03 1 . 329E+01 8 . 488E-04 1 . 648E-04 0.0 -0.174 0.195 0.194

0.0250 1 . 1 13E+01 3.974E-03 1.11 9E+01 1 .261 E-03 1 . 973E-04 0.0 -0.167 0.187 0.186 0.0300 9 . 726E+00 3 . 984E-03 9 . 730E+00 1 . 742E-0 3 2 . 282E-04 0.0 -0.163 0.181 0.180 0.0350 3 . 656E+00 3.994E-03 3 . 66 0 E + 0 0 2.287E-03 2.578E-04 0.0 -0.159 0.176 0.175

0.0400 7 . 834E+00 4.005E-03 7 . 838E+00 2.895E-03 2.863E-04 0 .

0

-0.156 0.172 0.172

0.0450 7. 181E+00 4.018E-03 7 . 1 85E+00 3.563E-03 3.1 40E-04 0 .

0

-0.153 0.169 0.168 0.0500 6 . 650E+00 4.031E-03 6 . 654E+00 4.286E-03 3.409E-04 0.0 -0.151 0.166 0.165

0.0550 6 . 209E+00 4.046E-03 6 .21 3E+00 5.065E-03 3.670E-04 0.0 -0.149 0.163 0.163

0.0600 5 . 836E+00 4.062E-03 5.341 E+00 5.895E-03 3.926E-04 0.0 -0.147 0.161 0.161 0.0700 5 . 242E+00 4 .093E-03 5 . 246E+00 7.706E-03 4 . 420E-04 0.0 -0.144 0.157 0.157

0.0300 4 . 789E+00 4. 1 38E-03 4 . 793E+00 9.703E-03 4.896E-04 0 . 0 -0.141 0.154 0.154

0.0900 4.431 E+00 4. 181E-03 4 . 435E+0 0 1 . 187E-02 5.355E-04 0.0 -0.139 0.152 0.151 0.1000 4 . 1 42E+00 4.228E-03 4. 146E+00 1 .421E-02 5.801 E-04 0.0 -0.137 0.149 0.149

0.1250 3.61 4E+00 4.355E-03 3.61 3E+00 2.069E-02 6 . 866E-04 0.0 -0.133 0.145 0.144

0.1500 3 . 257E+00 4.494E-03 3 . 262E+00 2.799E-02 7 . 874E-04 0.0 -0.130 0.141 0.141 0.1750 3.001 E+00 4.643E-03 3 . 006E+00 3.598E-02 3 .837E-04 0.0 -0.128 0.138 0.138

0.2000 2.809E+00 4.801 E-03 2.81 4E+00 4.459E-02 9 . 765E-04 0 .0 -0.126 0.136 0.136

0.2500 2. 542E+00 5.141E-03 2 . 543E+00 6 . 333E-02 1 . 1 54E-03 0.0 -0.122 0.132 0.132

0 . 3000 2 . 368E+00 5.51 4E-03 2 . 374E + 0 0 8.370E-02 1 . 323E-03 0.0 -0.119 0.130 0.129

0.3500 2 . 247E+00 5. 91 3E-03 2 . 253E+00 1 .054E-01 1 .488E-03 0.0 -0.117 0.127 0.126

0 . 4000 2. 159E+00 6 . 339E-03 2 . 1 66E+00 1 . 280E-0

1

1 . 649E-03 0.0 -0.115 0.125 0.124

0.4500 2 . 094E+00 6.787E-03 2 . 1 0 1 E+00 1 . 5 1 5E-0

1

1 . 808E-0 3 0 .

0

-0.114 0.123 0.122

0.5000 2 . 045E+00 7.257E-03 2 . 052E+00 1 .756E-01 1 . 965E-03 0.0 -0.112 0.122 0.120

0 .5500 2.007E+00 7.747E-03 2.01 4E+00 2.002E-01 2.122E-03 0.0 -0.111 0.121 0.119

0 .6000 1 . 977E+00 8.254E-03 1 . 985E+00 2.252E-01 2 . 27 9E-0 3 0.0 -0.109 0.119 0.118

0 . 7000 1 . 934E+00 9.312E-03 1 . 944E+00 2.761E-01 2 . 592E-03 0.0 -0.107 0.117 0.115 0.8000 1 . 908E+00 1 . 043E-02 1 . 91 8E+00 3.279E-01 2. 907E-03 0.0 -0.105 0.115 0.113

0 . 9000 1 .891 E+00 1 . 1 59E-02 1 . 903E+00 3.803E-01 3 . 224E-03 0.0 -0.104 0.114 0.111

1 .0000 1 . 88 1 E+00 1 . 280E-02 1 . 8 94E+0 0 4.330E-01 3.544E-03 0.0 -0.102 0.112 0.110

1 .2500 1 . 87 4E + 0 0 1 . 600E-02 1 . 8 90 E + 0 0 5.652E-01 4.356E-03 0.0 -0.099 0.110 0.106

1 . 5000 1 .880E+00 1 . 942E-02 1 .899E+00 6.972E-01 5. 187E-03 0.0 -0.097 0.107 0.104

1 .7500 1 .891 E+00 2.303E-02 1 . 914E+00 8.284E-01 6 . 036E-03 0.0 -0.095 0.105 0.101 2.0000 1 . 905E+00 2 . 673E-02 1 . 932E+00 9.584E-01 6 .899E-03 0 .

0

-0.093 0.104 0.099

2.5000 1 . 936E+00 3 . 468E-02 1 . 970E+00 1 .21 5E+00 8.665E-03 0.0 -0.091 0.101 0.096 3.0000 1 . 966E+00 4.299E-02 2 . 009E+00 1 . 466E+00 1 .047E-02 0 .

0

-0 . 089 0.099 0.094

3.5000 1 . 995E+00 5. 164E-02 2 . 047E+00 1 . 7 1 3E+00 1 . 230E-02 0.0 -0.087 0.097 0.091 4.0000 2 . 022E+00 6 . 053E-02 2 . 082E+00 1 . 955E+00 1 .41 6E-02 0.0 -0.086 0.095 0.090 4.5000 2 . 046E+00 6 . 976E-02 2.1 1 6E+00 2.1 93E+00 1 . 604E-02 0.0 -0.084 0.094 0.038

5.0000 2.06 9E+00 7 . 91 7E-02 2 . 1 48E+00 2 . 427E+00 1 . 7 92E-02 0 . 0 -0.083 0.093 0.087

5.5000 2.090E+00 8.876E-02 2. 179E+00 2.658E+00 1 . 982E-02 0.0 -0.082 0.091 0.085

6.0000 2. 1 10E+00 9 . 854E-02 2.209E+00 2 . 886 E+0 0 2.172E-02 0.0 -0.081 0.090 0.084

7.0000 2. 146E+00 1 . 185E-01 2 . 265E+00 3 . 333E+00 2.555E-02 0.0 -0.080 0.089 0.082 3.0000 2. 178E+00 1 .391 E-01 2 . 3 1 7 E+0 0 3 . 770E+00 2. 938E-02 0 .

0

-0.079 0.087 0 . 080 9.0000 2 . 206E+00 1 .601E-01 2 . 366E+00 4.1 97E+00 3.321 E-02 0.0 -0 .078 0.086 0.079

10.0000 2 . 232E+00 1 .814E-01 2.41 3E+00 4.61 6E+00 3 . 703E-02 0.0 -0.077 0.084 0.077

12.5000 2 . 286E+00 2.362E-01 2 . 523E+00 5 . 628E+00 4.652E-02 0 .

0

-0 .075 0.082 0.074

1 5.0000 2. 332E+00 2. 926E-01 2 . 624E+00 6 . 600E+00 5.587E-02 0.0 -0.073 0.079 0.072

17.5000 2 . 37 0 E + 00 3.501E-01 2.721 E+00 7 . 535E+00 6 . 505E-02 0.0 -0.072 0.077 0.070 20.0000 2 . 404E+00 4.086E-01 2.81 3E+00 8.439E+00 7 . 405E-02 0.0 -0.071 0.076 0.068 25.0000 2 . 460E+00 5.277E-01 2. 988E+00 1 .016E+01 9. 147E-02 0 .

0

-0.069 0.073 0.065 30.0000 2 . 507E+00 6 . 489E-01 3 . 1 55E+00 1 . 179E+01 1 . 081 E-01 0 .

0

-0.068 0.071 0.062 35.0000 2 . 544E+00 7.716E-01 3.31 6E+00 1 . 334E+0

1

1 . 240E-0

1

1 . 43 1 E-02 -0.058 0.063 0.059 40.0000 2 . 574E+00 8. 955E-01 3.469E+00 1 . 48 1 E+0

1

1 .392E-01 6.811 E-02 -0.049 0 .065 0.055 45.0000 2 . 598E+00 1 .021 E+00 3.61 8E+00 1 . 622E+0

1

1 . 537E-01 1 .414E-01 -0 .042 0.063 0.051 50.0000 2.61 7E+00 1 . 1 46E+00 3 . 764E+00 1 . 758E+0

1

1 .677E-01 2 . 242E-0

1

-0.037 0.060 0.047 55.0000 2 . 634E+00 1 . 27 3E+00 3 . 907E+00 1 . 888E+0

1

1 .81 IE-01 3. 103E-01 -0.033 0 .057 0.043 60.0000 2 . 649E+00 1 .400E+00 4.049E+00 2.014E+01 1 . 940E-01 3 . 984E-01 -0.030 0 .055 0.040 70.0000 2 . 674E+00 1 . 656 E+0 0 4 . 330E+00 2 . 252E+0

1

2. 184E-01 5.703E-01 -0 . 026 0.051 0.035

80 .0000 2 . 6 94E+00 1 . 91 4E+00 4 . 608E+00 2.476E+C1 2. 41 0E-01 7 . 335E-01 -0.023 0.048 0.031 90.0000 2.711 E+00 2 . 1 73E+00 4 . 384E+00 2 . 687E+0

1

2.620E-01 8.863E-01 -0.021 0 . 045 0.027 100.0000 2 . 726E+00 2. 434E+00 5 . 1 59E+00 2.S86E+01 2.817E-01 1 . 029E+00 -0.019 0.043 0.025

125.0000 2 . 756E+00 3 . 089E+00 5 . 845E+00 3.341 E+0

1

3 . 256E-0

1

1 . 345E+00 -0.017 0.038 0.020 150.0000 2.779E+00 3 . 749E+00 6 . 528E+00 3 . 746E+0

1

3.634E-01 1 . 6 1 4E+00 -0.015 0.035 0.017

1 75.0000 2 . 799E+00 4.41 2E+00 7.211 E+00 4.1 1 0E+01 3. 963E-01 1 . 848E+00 -0.014 0.032 0.014 200.0000 2.815E+00 5 . 078E+00 7.894E+00 4.441 E+0

1

4.252E-01 2 . 053E+00 -0.014 0.030 0.013 250.0000 2 . 843E + 0 0 6.41 6E+00 9 . 258E+00 5 . 025E+0

1

4.741 E-01 2 . 402E+00 -0.013 0.027 0.010 300.0000 2.865E+00 7 . 7 6 0 E + 0 0 1 . 062E+0

1

5 . 529E+0

1

5.1 38E-01 2 . 692E+00 -0.012 0.025 0.009 350.0000 2 . 883E+0 0 9. 107E+00 1 . 1 99E+01 5. 972E+01 5.469E-01 2. 939E+00 -0.011 0.023 0.008 400.0000 2 . 8 99E + 0 0 1 . 046E+01 1 . 336E+0

1

6 . 367E+0

1

5 . 750E-0

1

3 . 1 56E+00 -0.011 0.022 0.007 450.0000 2. 91 2E+00 1 .131E+01 1 . 473E+0

1

6 . 723E+0

1

5. 992E-01 3 . 348E+00 -0.011 0.021 0 .006 500.0000 2. 924E+00 1 .317E+01 1 . 609E+01 7 . 048E+0

1

6 . 203E-01 3 . 522E+00 -0.010 0.020 0.006 550.0000 2 . 935E+00 1 . 453E+0

1

1 .746E+01 7 . 346E+01 6 . 390E-0

1

3.681 E+00 -0.010 0.020 0.005 600.0000 2. 945E+00 1 .589E+01 1 . 883E+0

1

7.S22E+01 6 . 555E-0

1

3 . 827E + 00 -0.009 0.019 0.005 700.0000 2 . 962E+00 1 .361 E+01 2.157E+01 8.11 7E+01 6 . 838E-0

1

4 . 088E+00 -0.008 0.018 0.004 300.0000 2. 977E+00 2.133E+01 2.431 E+0

1

8.554E+0! 7 . 072E-01 4.318E+00 -0 .003 0.017 0.004

900.0000 2. 989E+00 2 . 406E+0

1

2 . 705E+0

1

8. 944E+01 7.268E-01 4 . 524E+00 -0 .007 0.016 0.003 1000.0000 3 . OOOE+OO 2.679E+01 2. 979E+01 9 . 296E+0

1

7 . 435E-0

1

4.71 1E+00 -0.005 0.016 0.003

r

153
POSITRONS IN CARBON (GRAPHITE)

I = 78.0 eV DENSITY = 2.265E+00 g/cn 3

ENERGY STOPPING POWER CSDA RADIATION DENS . EFF. d ( log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2/g MeV cm 2 /g g/cn 2 0.0100 2.21SE+01 2 . 02AE-03 2.21 9E+01 2.521E-0A A . A 1 IE-05 2.766E-03 -0.181 0 . 20 A 0.200 0.0125 1 .356E+01 2.135E-03 1 . 856 E+0

1

3.753E-0A 5.591E-05 3.5A3E-03 -0.17A 0.195 0.192

0.0150 1 . 60AE+0

1

2 . 225E-03 1 .605E+01 5.21 1E-0A 6.773E-05 A.353E-03 -0.169 0.139 0.1S5

0.0175 1 . A1 SE+01 2.301E-03 1 . A1 SE+01 6 .372E-0A 7 . 955E-05 5 . 1 95E-03 -0.165 0.133 0.130

0.0200 1 . 276E + 0

1

2.369E-03 1 . 276 E+0

1

8 . 733E-0

A

9.1 35E-05 6 . 063E-03 -0.162 0.179 0.176 0.0250 1 .069E+01 2. A35E-03 1 .06SE+01 1 .303E-03 1 . 1A9E-0A 7. S07E-03 -0.156 0.172 0.170 0.0300 9.25SE+00 2 . 575E-03 9.261 E+00 1 .30SE-03 1 . 3S3E-0

A

9.86AE-03 -0.152 0.167 0.165

0.0350 8 . 21 0E + 00 2.6A7E-03 3.21 3E+00 2.332E-03 1 .615E-0A 1 . 1 9AE-02 -0 . 1 A9 0.163 0.161

0 .0A00 7. A06E+00 2 . 707E-03 7. A09E+00 3 . 02AE-03 1 .8A3E-0A 1 .A12E-02 -0.1 A6 0.160 0.153

O.0A5O 6 . 7 6 9E+00 2.761E-03 6 . 772E + 00 3.731 E-03 2 . 068E-OA 1 . 6 A0E-02 -0 . 1 AA 0.157 0.155

0.0500 6 . 252E+00 2.809E-03 6 . 25AE+00 A.500E-03 2.2S9E-0A 1 . 87 9E-0 2 -0 . 1 A

1

0 . 1 5A 0.153

0.0550 5 . 822E+00 2.85AE-03 5 . 825E+0 0 5.329E-03 2 . 503E-0

A

2.127E-02 -0 . 1 AO 0.152 0.151 0.0600 5 . ASOE+OO 2.896E-03 5 . A63E + 00 6 . 21 6E-03 2.72AE-0A 2. 33AE-02 -0.138 0.150 0 . 1 A9 0.0700 A . 883E+00 2.971E-03 A .886E+00 8. 156E-03 3. 1 A8E-0A 2 . 926E-02 -0.135 0 . 1 A7 0 . 1 A 6 0.0800 A . A A2E + 0 0 3.039E-03 A. AA5E+00 1 .031 E-02 3.562E-0A 3 . 500E-02 -0.132 0 . 1 AA 0 . 1 A3 0.0900 A . 0 95E+00 3. 102E-03 A . 0 93E+00 1 . 265E-02 3. 967E-0A A . 1 05E-02 -0.130 0 . 1 A2 0 . 1 AO 0.1000 3.S15E+00 3.163E-03 3.81 8E+00 1 .518E-02 A . 363E-0A A . 738E-02 -0.128 0 . 1 AO 0.138

0.1250 3 . 303E+00 3.31 3E-03 3 . 306E+00 2.225E-02 5 . 322E-0

A

6 . A29E-02 -0.12A 0.135 0 . 1 3A 0.1500 2 . 957E+00 3.A60E-03 2.961 E+00 3.026E-02 6 . 2A5E-0A 8 . 253E-02 -0.120 0.132 0.131 0.1750 2.70 9E+00 3.60AE-03 2.712E+00 3. 910E-02 7.137E-0A 1.01 9E-01 -0.117 0.129 0.128

0.2000 2 . 522E+00 3.7A8E-03 2 . 526 E + 00 A.867E-02 8.00AE-0A 1 .221E-01 -0 . 1 1 A 0.126 0.125

0.2500 2.261 E+00 A.053E-03 2 . 265E+00 6 . 96AE-02 9.677E-OA 1 .6AAE-01 -0.109 0.122 0.120

0 . 3000 2 . 090E+00 A.378E-03 2 . 09AE+00 9.265E-02 1 . 1 30E-03 2 . 086E-01 -0.10A 0.118 0.116 0.3500 1 . 970E+00 A.718E-03 1 . 97AE+00 1 . 173E-01 1 . 288E-03 2.537E-01 -0.100 0.115 0.113

0 .0000 1 . 882E+00 5 . 079E-03 1 . S37E+00 1 -A32E-01 1 . AA5E-03 2. 992E-01 -0.096 0.112 0.110

0-A500 1 .81 6E+00 5.A59E-03 1 .821 E+00 1 .702E-01 1 . 600E-03 3.AA7E-01 -0.093 0.109 0.107

0.5000 1 . 76 AE + 00 5.856E-03 1 . 770E+00 1 . 981 E-01 1 . 756 E-03 3.399E-01 -0.090 0.106 0 . 1 OA 0.5500 1 . 724E+00 6 .265E-03 1 . 730E+00 2.266E-01 1 . 91 1 E-03 A.3A7E-01 -0.037 0 . 1 0 A 0.101 0.6000 1 . 6 92E + 00 6 . 6 86E-0 3 1 . 6 93E+00 2.553E-01 2.067E-03 A.788E-01 -0 . 035 0.102 0.099

0.7000 1 . 6 AAE+00 7.565E-03 1 . 652E+00 3. 156E-01 2.379E-03 5.6A8E-01 -0.031 0.098 0.095

0.8000 1 . 6 1 2E+00 3 . A88E-03 1 . 620E+00 3.767E-01 2.695E-03 6 . A76E-01 -0.077 0.095 0.091

0 . 9000 1 . 590E+00 9. A5AE-03 1 . 599E+00 A.389E-01 3.01 5E-03 7.272E-01 -0.07A 0.092 0.038

1 .0000 1 . 57AE+00 1 .0A6E-02 1 . 58AE + 00 5.017E-01 3.339E-03 8.03AE-01 -0.072 0.090 0.085

1 .2500 1 . 552E + 00 1 .31 IE-02 1 . 565E + 00 6.607E-01 A. 1 68E-03 9.803E-01 -0.067 0.085 0.079

1.5000 1 . 5AAE+00 1 .596E-02 1 . 560E+00 8 .207E-01 5 . 02AE-03 1 . 1 AOE+OO -0 .063 0.081 0.075

1 .7500 1 . 5A3E + 00 1 .897E-02 1.561 E+00 9.810E-01 5.90AE-03 1 . 285E+00 -0.061 0.073 0.071 2.0000 1 . 5A5E + 00 2.210E-02 1 . 567E+00 1 . 1 A1 E+00 6 .806E-03 1 . A1 7E+00 -0.059 0.075 0.063

2.5000 1 . 55AE+00 2 . 867E-02 1 . 533E+00 1 . A53E+00 8.66AE-03 1 . 651 E+00 -0.055 0.071 0.063

3.0000 1 . 56 6E + 0 0 3.561 E-02 1 .601 E+00 1 . 773E+00 1 . 058E-02 1 . 35AE + 00 -0.053 0.068 0 .060 3.5000 1 . 578E+00 A . 283E-02 1 .621 E+00 2 . 083E+00 1 . 255E-02 2 . 0 33E+0 0 -0.050 0.065 0.057

A. 0000 1 . 589E + 00 5 . 027E-02 1 . 6 AOE+OO 2 . 3 90E+0 0 1 . A55E-02 2. 1 9AE+00 -0 . OAS 0.063 0.055

A. 5000 1 . 600E+00 5.792E-02 1 . 658E+00 2 . 6 93E + 00 1 . 657E-02 2 . 3A0E+00 -0 . 0A6 0.061 0.053

5.0000 1.61 1 E+00 6.57SE-02 1 . 676E + 00 2. 993E+00 1 . 862E-02 2. A7AE + 00 -0 . 0A5 0.059 0.051 5.5000 1 . 620E+00 7.377E-02 1 . 69AE+00 3.2S9E+00 2.069E-02 2 . 5 93E+0 0 -0.0A3 0.053 0.0A9

6.0000 1 . 629E + 00 8.1 93E-02 1.711 E+00 3 . 583E+00 2.278E-02 2.713E+00 -0.0A1 0.056 0.0A3

7.0000 1 . 6 A5E + 00 9.865E-02 1 .7AAE+00 A. 1 S2E+00 2.699E-02 2. 92AE+00 -0.033 0 .05A 0 . OAS 8.0000 1 . 6 5 9E+00 1 . 1 58E-0

1

1 . 775E+00 A . 731 E+00 3 . 1 23E-02 3.11 AE+00 -0 .03A 0.051 0 .0A2 9.0000 1 . 67 1 E+00 1 .33AE-01 1 .SOAE+OO 5 . 239E+00 3.5A9E-02 3 . 287E+00 -0.031 0.0A9 0.0A0

10.0000 1 . 682E+00 1 -513E-01 1 . 833E+00 5 . 839E+00 3 . 977E-02 3. AA6E+00 -0.028 0.0A7 0.037

12.5000 1 . 70 AE+0 0 1 .971E-01 1 . 901 E+00 7 . 1 73E+00 5.0AAE-02 3 . 798E+00 -0 .022 0 .0A2 0.032

15.0000 1 .721 E+00 2.AAAE-01 1 . 966E+00 8. A71E+00 6 . 105E-02 A. 1 0 1 E+00 -0.013 0.039 0 .027 17.5000 1 . 7 36 E + 00 2. 927E-01 2 . 028E+00 9 . 723E+00 7. 152E-02 A.367E+00 -0 . 01 A 0.035 0 . 0 2 A 20.0000 1 . 7A8E+00 3.A17E-01 2 . 089E+00 1 .09AE+01 8.183E-02 A . 60 AE+00 -0.011 0.033 0.021 25.0000 1 . 767E+00 A.A17E-01 2 . 209E+00 1 . 326 E+0

1

1.01 9E-01 5.01 2E+00 -0 .003 0 .028 0.016 30.0000 1 . 782E + 00 5 . A35E-0

1

2 . 326E+00 1 . 5A7E+0

1

1 .21 IE-01 5 . 353E+00 -0.006 0 .025 0.013

35.0000 1 . 7 95E+00 6.A66E-01 2. AA2E+00 1 . 757E+0

1

1 . 3 9AE-0

1

5 . 6 A6E+00 -0 .00A 0.022 0.010

AO .0000 1 . 806E+00 7.508E-01 2 . 557E+00 1 . 957E+01 1 -569E-01 5. 902E+00 -0.003 0.020 0.009

A5.0000 1 .81 5E+00 8.559E-01 2.671 E+00 2. 1 ASE+01 1 .736E-01 6 . 1 30E+00 -0.003 0.019 0.007 50.0000 1 . 32AE+00 9.617E-01 2 . 785E+00 2 . 332E+0

1

1 .895E-01 6 . 335E+00 -0 . 002 0.017 0.006

55.0000 1 .331 E+00 1 . 063E+00 2. 900E+00 2 . 507E+01 2.0A8E-01 6.521 E+00 -0 .002 0.016 0.006 60.0000 1 .838E+00 1 . 1 75E+00 3.01 AE+00 2 . 677E+0

1

2. 1 93E-01 6.691E+00 -0 .002 0.015 0 . 005

70 . 0000 1 . 350E+00 1 .391 E+00 3.2A1E+00 2.997E+01 2 . A66E-0

1

6 . 99AE+00 -0.001 0 . 0 1 A O.OOA

30.0000 1 .361 E+00 1 . 608E+00 3. A69E+00 3 . 295E+0

1

2.716E-01 7 . 25SE+00 -0.001 0.013 0.003

90 . 0000 1 .870E+00 1 .826E+00 3 . 6 96E + 00 3.57AE+01 2.9A6E-01 7.A91E+00 -0.001 0.012 0.003

100.0000 1 . 878E+00 2 . 0A6E+00 3 . 92AE+00 3 . 836 E+0

1

3.160E-01 7.S99E+00 -0.001 0.011 0.002

1 25.0000 1 .S95E+00 2 . 598E+00 A. A9AE+00 A . A3 1 E+0

1

3.630E-01 8 . 1 A2E+00 -0.000 0.009 0.002

150.0000 1 . 909E+00 3. 1 55E+00 5 . 06AE+00 A . 955E+0

1

A . 027E-0

1

3 . 505E+00 -0.000 0.003 0.001 175.0000 1 . 921 E+00 3.71 AE+00 5 . 6 36E+00 5 . A23E+0

1

A.369E-01 3.31 1 E+00 -0.000 0.003 0.001 200.0000 1 . 932E+00 A.276E+00 6 . 208E+00 5 . 3A5E+0

1

A . 666E-0

1

9 . 077E+00 -0.000 0.007 0.001

250 .0000 1 . 9A9E+00 5. A05E+00 7 . 35AE+00 6 . 53AE+0

1

5.159E-01 9 . 522E+00 -o.oco 0.006 0.001 300.0000 1 . 963E+00 5 . 5A0E+OO 8.503E+00 7.216E+01 5.55AE-01 S . 886E+00 -0 . 000 0 .006 0.001 350.0000 1 . 975E+00 7 . 673E+00 9 . 653E+00 7 . 768 E+0

1

5 . 879E-0

1

1 .01 9E+01 -0.000 0.005 0.000 AOO.OOOO 1 . 985E + 00 3 . 820E+00 1 . 080E+0

1

8 . 257E+01 6.152E-01 1 . 0 A6E+0

1

-0 . 000 0.005 o.ooo

A50 .0000 1 . 99AE+00 9. 96AE+00 1 . 1 96E+01 8 . 697E+01 6 . 385E-0

1

1 . 070E+0

1

-0.000 0.005 o.oco 500.0000 2 . 002E+00 1.111 E+O

1

1 .31 1E+01 9.096E+01 6 . 5S7E-01 1 .091E+01 -0.000 0.005 0.000 550.0000 2 . 009E+00 1 . 226E+0

1

1 . A27E+0

1

9.A61E+01 6. 76AE-01 1 . 1 1 0 E+0

1

-0.000 0.005 0.000

600 . 0000 2 . 0 1 6 E + 00 1 . 3A0E+0

1

1 . 5A2E+0

1

9.793E+01 6 . 920E-01 1 . 1 27E+01 -0.000 0 .00A 0.000 700.0000 2 . 028E+00 1 . 570E+0

1

1 .773E + 01 1 . 0 A0E+02 7.136E-01 1 .15SE+01 -0.000 0 . 00 A 0.000 800.0000 2 . 033 E+00 1 .301E+01 2 . 005E+01 1 . 0 93E+02 7.A03E-01 1 . 185E+01 - 0.000 0 . 00 A 0.000 900.0000 2.0A7E+00 2.031 E+0

1

2 . 236 E+0

1

1 . 1 A0E+02 7 . 53AE-0

1

1 . 208E+0

1

- 0.000 0 . 00 A 0.000 1000.0000 2 . 055E+00 2 . 262E+0

1

2 . A68E+0

1

1 . 183E+02 7 . 739E-0

1

1 . 229E+0

1

- 0.000 O.OOA 0.000

154
POSITRONS IN CARBON (GRAPHITE)

I = 73.0 eV DENSITY - 1.700E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

Me V MeV cm 2 /g MeV cm 2 /g MeV cm 2/g g/cm 2 0.0100 2.21 9E+01 2 . 024E-03 2.21 9E+01 2.521E-04 4.411 E-05 1 . 920E-03 -0.182 0.204 0.200 0.0125 1 .3562+0

1

2.135E-03 1 . S57E+0

1

3 . 753E-04 5.591E-05 2.431 E-03 -0.175 0 . 1 95 0.192

0.0150 1 . 605E+0

1

2 . 225E-03 1 . 605E+0

1

5.21 IE-04 6 . 773E-05 3 . Q73E-03 -0.170 0.139 0.186 0.0175 1 .41 9E+01 2.301 E-03 1 .41 9E+01 6.871E-04 7 . 954E-05 3. 695E-03 -0.165 0.134 0.131 0.0200 1 . 276E+0

1

2. 369E-03 1 . 276E+0

1

8.732E-04 9. 1 342-05 4 . 347E-0 3 -0.162 0.179 0.177

0.0250 1 .069E+01 2.4S5E-03 1 .069E+01 1 . 303E-03 1 . 149E-04 5 . 736E-03 -0.157 0.173 0.170 0.0500 9 . 260E+00 2 . 575E-03 9 . 26 3E+0 0 1 . 8Q7E-03 1 . gS o E— 0 4 7 . 236 E-0 3 -0.153 0.163 0.165

0.0350 8.21 2E+00 2.647E-03 8 .21 5E+00 2. 332E-03 1 .614E-04 8.343E-03 -0.149 0.164 0.161 0.0400 7 . 408E+00 2 . 707E-03 7.41 1 E+00 3 . 024E-03 1 . 842E-04 1 . 055E-02 -0.147 0.160 0.158

0.0450 6.771 E+00 2.761 E-03 6 . 774E+00 3 . 730E-03 2.067E-04 1 .2362-02 -0.144 0.157 0.156 0.0500 6 . 254E+0 0 2. 809E-C3 6 . 256E+00 4 .499E-03 2.2S9S-04 1 . 425E-92 -0.142 0.155 0.153

0.0550 5 . 324E+00 2.S54E-03 5.S27E+00 5 . 323E-03 2.507E-04 1 . 624E-02 -0.141 0.153 0.151 O.OSOO 5 . 462E+00 2.396E-03 5 . 465E+00 6.215E-03 2 . 723E-04 1 .332E-02 -0.139 0.151 0.149 0.0700 4 . 385E+0 0 2.971 E-0 3 4 . 83SE+00 8.154E-03 3.147E-04 2.271 E-0 2 -0.136 0.148 0.146 O.OSOO 4 . 445E+00 3.039E-03 4 . 448E+00 1 . 030E-02 3.561E-04 2 . 740E-02 -0.134 0.145 0.144 0.0900 4. 098E+00 3. 102E-03 4.101E+00 1 . 2S5E-C2 3. 965E-04 3 . 237E-02 -0.132 0.143 0.142

0.1000 3.817E+00 3. 163E-03 3 . 820 E+0 0 1 .51SE-02 4.361E-04 3.760E-02 -0.130 0.141 0.140

0.1250 3 . 306E+00 3.313E-03 3.309E+00 2 . 224E-02 5.31 9E-04 5.1 66E-02 -0.126 0.137 0.136

0 .1500 2 . 960E+00 3.460E-03 2 . 964E+00 3 . 024E-02 6 .241 E-04 6 . 6 94E-02 -0.123 0.134 0.132

0.1750 2.712E+00 3 . 604E-03 2.71 5E+00 3. 907E-02 7. 132E-04 3 . 320E-02 -0.121 0.131 0.130 0.2000 2 . 525E+0 0 3 . 743E-03 2 . 529E+00 4 .862E-02 7.997E-04 1 .003E-01 -0.118 0.129 0.127

0.2500 2 . 26 5E+0 0 4 . 053E-03 2.269E+00 6 . 957E-02 9 . 666 E-04 1 .363E-01 -0.114 0.125 0.123

0.3000 2.094E+00 4.378E-03 2 . 0 99E + 00 9 . 253E-02 1 . 128E-03 1 . 740E-0

1

-0.110 0.121 0.120 0.3500 1 . 975E+00 4.718E-03 1 . 979E+00 1 . 1 7 1 E-0

1

1 . 286E-03 2. 129E-01 -0.106 0.118 0.117

0.4000 1 . 887E+00 5.079E-03 1 . 892E+00 1 . 430E-0

1

1 . 442E-03 2.524E-01 -0.102 0.116 0.114

0.4500 1 .821 E+00 5 . 459E-03 1 .327E+00 1 . 6 99E-0

1

1 .597E-03 2.922E-01 -0.099 0.113 0.111 0.5000 1 . 77 0 E+0 0 5.S56E-03 1 . 776E+0 0 1 . 977E-01 1 . 752E-03 3.321 E-0

1

-0.096 0.111 0.109

0.5500 1 . 730E+00 6 . 265E-03 1 . 737E+00 2.261 E-0

1

1 . 906E-03 3.71 9E-01 -0.094 0.109 0.106 0.6000 1 . 6 98E + 0 0 6 . 636E-03 1 . 7 0 5E+0 0 2 . 552E-0

1

2.061 E-03 4.1 14E-01 -0.091 0.107 0.104

0.7000 1 .651 E+OO 7.565E-05 1 . 65 9E + 00 3 . 1 47E-01 2.372E-03 4 . 8 9 1 E-0

1

-0.036 0.104 0.100

0 .8000 1.61 9E+00 8 . 483E-03 1 . 628E+0 0 3 . 75 6 E-0

1

2 . 6 87E-0 3 5.648E-01 -0.082 0.100 0.095

0 . 9000 1 . 597E+00 9.454E-03 1 . 607E+00 4.375E-01 3.004E-03 6.382E-01 -0.079 0.098 0.093

1 .0000 1 . 582E+00 1 . 046E-02 1 . 5 92E + 0 0 5 . 000 E-0

1

3 . 326 E-0 3 7. 091 E-01 -0.076 0.095 0.090

1 .2500 1 .561 E+00 1 .31 IE-02 1 . 574E+0 0 6.58! E-0 1 4.150E-03 3 . 756 E-0

1

-0.070 0.090 0 . 034

1 .5000 1 . 553E+0 0 1 .596E-02 1 . 56 9E+00 8. 172E-01 4 . 999E-03 1 . 028E+00 -0.066 0.085 0.079

1 .7500 1 . 552E+00 1 . 397E-02 1 . 571 E+00 9.765E-01 5.374E-03 1 . 1 67E+00 -0 . 063 0.082 0.075

2.0000 1 . 555E+00 2.21 0E-02 1 . 377E+0 0 1 . 1 35E+00 6 . 770E-03 1 . 295E+00 -0.060 0.079 0.071 2.5000 1 . 564E+00 2 . S67E-02 1 . 593E+00 1 . 451 E+00 8.615E-03 1 . 522E+00 -0.056 0.074 0.066

3.0000 1 .57 6 E+0 0 3.561E-02 1 . 6 1 2E+00 1 . 763E+00 1 . 052E-02 1 . 720 E+0 0 -0.054 0.070 0.062

3.5000 1 . 589E+00 4 . 283E-02 1 .631 E+00 2.071 E+00 1 . 247E-02 1 . 3 94E+00 -0.051 0 .063 0.059

4.0000 1 . 600F+00 5.027E-02 1 . 651 E+00 2 . 376E+00 1 . 445E-02 2.051 E+00 -0.050 0.065 0 .057 4.5000 1 . 6 1 2E+00 5.792E-02 1 . 670E+00 2. 677E+00 1 . 647E-02 2 . 1 93E+00 -0.043 0.063 0.055

5.0000 1 . 622E+00 6 . 57SE-02 1 . 638E+00 2 . 975E+00 1 . 850E-02 2 . 323E+0 0 -0.046 0.061 0 . 053 5.5000 1 . 632E+00 7.377E-02 1.706 1.+0 0 3 . 270E+00 2.056E-02 2 . 443E+00 -0.045 0.060 0.051 6.0000 1 . 641 E+00 8.1 93E-02 1 . 723E+00 3.561 E+00 2 . 263E-02 2.555E+00 -0.044 0 .058 0.050

7.0000 1 . 658E+00 9 . 865E-02 1 . 756E+00 4 . 1 36E+00 2.680E-02 2. 758E+00 -0.041 0.056 0.047 8.0000 1 . 672E+00 1 . 1 53E-01 1 . 738E+00 4 . 70 0 E + 0 0 3 . 1 0 1 E-0 2 2. 939E+00 -0.038 0.054 0.045

9.0000 1 . 685E+00 1 . 3 34 E-0

1

1 . 8 1 8E+00 5 . 255E+00 3.524E-02 3. 104E+00 -0.036 0.052 0.042 10.0000 1 . 6 96E+00 1 .51 3E-01 1 .347E+00 5 , 800 E+00 3. 948E-02 3 . 256E+00 -0.033 0.050 0.040 12.5000 1 . 720 E+0 0 1 . 97 1 E-0

1

1 . 91 7E+00 7 . 1 29E+00 5.006E-02 3.591 E+00 -0.028 0.046 0.036 15.0000 1 . 733E+00 2 . 444E-0

1

1 . 983E+00 8.41 1 E+00 6 . 057E-02 3 . 879E+00 -0.023 0 . 042 0.031 17.5000 1 . 754E+00 2 . 927E-0

1

2 . 046E + 00 9 . 552E+00 7.095E-02 4.1 33E+00 -0.019 0.039 0.028 20.0000 1 .7S6E+00 3.417E-01 2.1 08E+00 1 . 086E+01 8 . 1 1 6E-02 4.361 E+00 -0.016 0 .036 0.025 25.0000 1 . 787E+00 4.417E-01 2 . 228E+0 0 1 .31 6E+01 1 . 0 1 0 E-0

1

4 . 755E+00 -0.011 0.032 0.020 30.0000 1 .803E+00 5 . 435E-0

1

2 . 346 E+00 1 . 535E+0

1

1 . 200 E-0

1

5 . 038E+00 -0.008 0.028 0.016 35.0000 1 .81 6E+00 6.466 E-0

1

2 . 462E+00 1 . 743E+0

1

1 . 382E-0

1

5 . 376E + 00 -0.006 0.026 0.013 40.0000 1 .827E+00 7.508E-01 2 . 578E+00 1 . 941 E+01 1 . 556E-0

1

5 . 628E+00 -0.005 0.023 0.011 45.0000 1 . 837E+00 8.559E-01 2 . 6 92E+0 0 2. 1 31 E+01 1 . 7 22E-0

1

5 .354E+00 -0.004 0.022 0.010 50.0000 1 -845E+00 9.617E-01 2 . 807E+00 2 . 31 3E+0

1

1 . 830 E-0

1

6 . 057E+00 -0.003 0.020 0.008

55.0000 1 .353E+00 1 . 068E+00 2. 921 E+00 2 . 483E+0

1

2.031 E-0

1

6.241 E+00 -0.003 0.019 0.007 60.0000 1 .860E+00 1 . 1 75E+00 3 . 0 35E+00 2 . 655E+0

1

2 . 1 76 E-0

1

6.411 E+00 -0.002 0.018 0.006 70.0000 1 . 872E+0 0 1 .391 E+00 3 . 263E+00 2. 973E+01 2.447E-01 6 .71 2E+00 -0.002 0.016 0.005 80.0000 1 .882E+00 1 . 608E+00 3 . 490E+00 3.269E+01 2.696E-01 6 . 974E+00 -0.001 0.015 0 .004 90.0000 1 . 8 92E+0 0 1 . 326E+00 3.71 SE+00 3 . 547E+0

1

2.925E-01 7 . 206E+00 -0.001 0.013 0.004 100.0000 1 . 900E+00 2 . 046E+00 3 . 946E+00 3 . 808E+0

1

3.138E-01 7.41 5E+00 -0.001 0.013 0.003 125.0000 1 .S17E+00 2.598E+00 4.516E+00 4.400E+01 3.S07E-01 7.857E+00 -0.001 0.011 0.002 150.0000 1 . 931 E+00 3. 155E+00 5 . 086E+00 4.921 E+0

1

4 . 003E-0

1

3.21 9E+00 -0.000 0.010 0.002

175.0000 1 . 943E+00 3.71 4E+00 5 . 653E+00 5 . 337E+0

1

4 . 344E-01 3 . 525S+00 -0.000 0.009 0.001 200.0000 1 . 954E+00 4 . 27 6 E+0 0 6 . 230E+00 5 . S08E+0

1

4.641 E-0

1

8 . 7 9 1 E+0 0 -o.ooo 0 .003 0.00! 250.0000 1 . 971 E+00 5 . 40 5E+0 0 7 . 37SE+00 6 . 545E+0

1

5 . 1 35E-01 9 . 236E+00 -0.000 0.007 0.001 300.0000 1 . 935E+00 6 . 540 E + 00 8 . 525E+00 7 . 1 75E+0

1

5 .530E-01 9 . 599E+00 -0 .000 0 . 007 0.001 350.0000 1 . 997E+00 7 . 678E+00 9 . 6 75E+0 0 7 . 725E+0

1

5.356E-01 9. 907E+00 -0.000 0.006 0.001 400.0000 2 . 007E+00 3.S20E+00 1 . 083E+0

1

8.213E+01 6.129E-01 1 .017E+01 -0.000 0.006 0.001 450.0000 2.016E+00 9 . 964E+00 1 . 1 9SE+C1 3 . 652E+0

1

6 . 363E-C

1

1 . 04 1 E+0

1

-0.000 0 . 006 0 . COO 500.0000 2 . 024E+00 1 . 1 T1E+01 1 .31 3E + 01 9 . 050E+01 6 . 566E-01 1 . 062E+01 -0.000 0.005 0.000 550.0000 2.031 E+OO 1 .226E+01 1 . 429E+0

1

9.41 5E+01 6.744E-01 1 .031 E+01 -0.000 0.005 0.000 600.0000 2 . 038E+00 1 . 340E+01 1 . 544E+0

1

9 . 752E+0

1

6 . 901 E-01 1 .09SE+01 -0.000 0.005 0.000 700.0000 2 . 050E+00 1 . 570E+0

1

1 .775E+01 1 . 0 36E+02 7.167E-01 1 . 129E+01 -0 . 000 0.005 0 .000 800.0000 2 . 060E+00 1 .801 E+01 2 . 007E+0

1

1 . 038E+02 7.385E-01 1 . 1 56E+01 - 0.000 0.005 0.000 900.0000 2.069E+00 2.031E+01 2.238E+01 1 . 1 36E+02 7 . 568E-0

1

1 . 179E+01 - 0.000 0.004 0.000 1000.0000 2 . 077E+00 2 . 262E+0

1

2 . 470E+0

1

1 . 178E+02 7.723E-01 1 .200E+01 - 0.000 0.004 0.000

155
POSITRONS IN ALUMINUM

I = 166.0 eV DENSITY = 2 . 6 99E+00 g/cn 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(IogI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR

.

COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2 /g MeV cm 2 /g g/cn 2 0.0100 1 . 846E+0

1

2.5S8E-03 1 . 846 E+0

1

3.091E-04 6 . 444E-0 5 3 . 534E-04 -0.211 0.243 0.235

0.0125 1 . 554E+0

1

2.316E-03 1 . 554E+0

1

4.573E-04 8 . 368E-05 4. 937E-04 -0.202 0.231 0.224

0.0150 1 .349E+01 3.005E-03 1 . 350E+0

1

6.304E-04 1 .034E-04 6 . 538E-04 -0.195 0.222 0.216 0.0175 1 . 1 97E+01 3.170E-03 1 . 1 93E+01 8 . 275E-04 1 . 234E-04 8 . 332E-04 -0.190 0.215 0.209

0 .0200 1 .030E+01 3.315E-03 1 . 080E+0

1

1 . 048E-03 1 . 437E-04 1 . 031 E-03 -0.185 0.209 0.204

0.0250 9 . 086E+00 3.561E-03 9.08 9E + 00 1 . 555E-0 3 1 .849E-04 1 . 483E-03 -0.179 0 . 200 0.195

0.0300 7 .S99E+00 3.763E-03 7 . 903E+00 2 . 1 46 E-0 3 2.264E-04 2.005E-03 -0.174 0.194 0.189

0.0550 7 . 024E+00 3. 936E-03 7 . 028E+00 2.81 9E-03 2 . 6S0E-04 2 . 593E-03 -0.170 0.183 0.184

0.0400 6.351 E+00 4 . 039E-03 6 . 355E+00 3 . 5SSE-03 3.09SE-04 3 . 246E-03 -0.166 0.134 0.180 0.0450 5.816E+00 4.226E-03 5 . 820E+0

0

4 . 3 9 1 E-0 3 3.5! 4E-04 3 . 960E-03 -0.164 0.180 0.177

0.0500 5 . 330E+00 4.353E-03 5 . 334E+00 5 . 285E-03 3. 930E-04 4 . 732E-03 -0.161 0.177 0.174

0.0550 5.01 8 E+00 4 . 468E-03 5 . 022E+00 6 . 248E-03 4 . 345E-04 5.560E-03 -0.159 0.175 0.172

0.0600 4.71 2E+00 4.575E-03 4.71 6E+00 7 . 276E-03 4.758E-04 6 . 440E-03 -0.153 0.172 0.169

0.0700 4 . 223E+00 4.771 E-0 3 4 . 227E+00 9 . 520 E-0 3 5 . 578E-04 8.351 E-03 -0.155 0.168 0.166

0 .0800 3.349E+00 4 . 949E-03 3 . 854E+00 1 . 200E-02 6.389E-04 1 . 045E-02 -0.152 0.165 0.163

0.0900 3.554E+00 5.11 9E-03 3.559E+00 1 . 470E-02 7.1 91E-04 1 . 27 1 E-02 -0.150 0.163 0.160 0.1000 3.31 5E + 00 5.2S2E-03 3.321 E+00 1 . 762E-0 2 7 . 987E-04 1 .51 3E-02 -0.148 0.160 0.158

0.1250 2.879E+00 5.661E-03 2 . 885E+00 2.573E-02 9. 945E-04 2.1 75E-02 -0.145 0.156 0.154

0.1500 2 . 534E+00 6 . 002E-03 2 . 590E+00 3 . 490E-02 1 . 186E-03 2. 907E-02 -0.142 0.152 0.150 0.1750 2 . 372E+00 6 . 323E-03 2.379E+00 4.499E-02 1 . 372E-03 3.694E-02 -0.140 0.150 0.148

0.2000 2.21 3E+00 6 .639E-03 2 . 220E+00 5 . 588E-02 1 . 553E-03 4 . 525E-02 -0.133 0.147 0.146

0.2500 1 . 991 E+00 7 . 273E-03 1 . 999E+00 7.971 E-02 1 . 906E-03 6 .280E-02 -0.134 0.144 0.142

0.3000 1 .346E+00 7 . 922E-03 1 . 854E+00 1 . 057E-0

1

2.248E-03 8.1 16E-02 -0.132 0.141 0.139

0.3500 1 . 745E+00 8.589E-03 1 . 753E+00 1 . 335E-0

1

2 . 582E-03 9. 997E-02 -0.129 0.139 0.137

0.4000 1 . 672E+00 9.279E-03 1 .681 E+00 1 .627E-01 2.91 OE-03 1 . 1 90E-01 -0.127 0.137 0.135

0.4500 1 . 6 1 7E + 00 9. 991 E-03 1 . 627E+00 1 . 929E-0

1

3 . 235E-03 1 . 380E-01 -0.126 0.135 0.133

0.5000 1 . 575E + 00 1 . 073E-02 1 . 536E+00 2.241 E-0

1

3 . 557E-03 1 .569E-01 -0.124 0.134 0.131 0.5500 1 . 542E+00 1 . 150E-02 1 . 554E+00 2.559E-01 3.377E-03 1 . 757E-0

1

-0.122 0.132 0.130

0.6000 1 .51 7E+00 1 . 229E-02 1 . 529E+00 2.884E-01 4.1 97E-03 1 . 943E-01 -0.121 0.131 0.123

0.7000 1 . 430E+00 1 . 393E-02 1 . 494E+00 3 . 546 E-0

1

4.837E-03 2.307E-01 -0.118 0.129 0.126 0.3000 1 . 456 E + 0 0 1 . 56 5E-0 2 1 . 472E+00 4.221 E-0 1 5 . 480E-03 2.661 E-0

1

-0.116 0.126 0.124

0 . 9000 1 .441 E+00 1 . 743E-02 1 . 458E+00 4. 904E-01 6. 125E-03 3.005E-01 -0.113 0.125 0.121

1 .0000 1 .431 E+00 1 . 929E-02 1 . 450E+00 5 . 592E-01 6 . 775E-03 3.339E-01 -0.111 0.123 0.119

1 .2500 1 .421 E+00 2 . 425E-02 1 . 445E+00 7 . 320 E-0

1

8.427E-03 4. 138E-01 -0.105 0.119 0.115

1 .5000 1 . 421 E+00 2 . 956E-02 1 . 451 E+00 9.048E-01 1 . 0 1 2E-02 4 .898E-01 -0.100 0.115 0.110

1 .7500 1 . 426E+00 3.516E-02 1 .461 E+00 1 . 077E+00 1 . 184E-02 5.632E-01 -0.095 0.112 0.106

2.0000 1 . 434E+00 4. 104E-02 1 . 475E+00 1 . 247E+00 1 . 361 E-02 6.349E-01 -0.089 0.109 0.102

2.5000 1 .451 E+00 5.346E-02 1 . 504E+00 1 . 583E+00 1 . 722E-02 7 . 757E-01 -0.079 0.103 0.094

3.0000 1 . 467E+00 6.651E-02 1 . 534E+00 1 . 91 2E+00 2.092E-02 9.145E-01 -0.069 0.093 0.087

3.5000 1 . 482E+00 8.010E-02 1 . 562E+00 2 . 235E+00 2.469E-02 1 . 051 E+00 -0.061 0.092 0 . 080 4.0000 1 . 495E+00 9.418E-02 1 . 590E+00 2 . 552E+00 2.851 E-02 1 . 183E+00 -0.054 0.083 0.074 4.5000 1 . 508E+00 1 .087E-01 1 .616 E+OO 2 . 864E+00 3 . 237E-02 1 .31 1E+00 -0.048 0.033 0.068

5.0000 1 . 5 1 3E+00 1 . 235E-0

1

1 . 642E+00 3. 1 7 1 E+00 3 . 626E-02 1 . 433E+00 -0.044 0.079 0.063

5.5000 1 . 523E+00 1 . 386E-01 1 . 667E+00 3 . 473E+00 4 . 0 1 6 E-0 2 1 . 550E+00 -0 .040 0.076 0.059

6.0000 1 . 537E+00 1 . 540E-0

1

1 . 6 91 E+0 0 3.771 E+00 4.406E-02 1 . 66 1 E+00 -0 .037 0.073 0 .055 7.0000 1 . 553E+00 1 . 855E-0

1

1 . 738E+00 4 . 554E+0 0 5. 1 91 E-02 1 . S68E+00 -0.033 0.067 0.048

8.0000 1 . 566E+00 2.179E-01 1 . 734E+00 4.922E+00 5 . 973E-02 2 . 055E+00 -0.029 0.063 0.043

9.0000 1 .578E+00 2 . 503E-0

1

1 . 329E+00 5 . 476E+00 6 . 750 E-02 2 . 226 E+0 0 -0.027 0.059 0.039

1 0.0000 1 . 53 9E + 00 2.841 E-0

1

1 - 873E+00 6.01 6E+00 7.51 9E-02 2 . 384E+0 0 -0.025 0.055 0.036

12.5000 1.61 1 E+00 3.695E-01 1 . 930E+00 7.314E+00 9.402E-02 2 . 727E+00 -0.022 0.049 0.030 15.0000 1 . 6 29E+0 0 4 . 57 1 E-0

1

2 . 086E+00 8 . 544E+00 1 .122E-0! 3.016E+00 -0.020 0.044 0.026

17.5000 1 . 644E+00 5.459E-01 2.1 90E+00 9.71 3E+00 1 . 297E-0

1

3 . 265E+00 -0.019 0.041 0.023 20.0000 I . 657E+00 6.357E-01 2 . 292E+00 1 . 083E+0

1

1 .464E-01 3 . 484E+00 -0.018 0 .03S 0.021 25.0000 1 . 678E+00 3.130E-01 2 . 496E+00 1 . 292E+0

1

1 . 777E-0

1

3 . 857E+00 -0.016 0.034 0.013

30.0000 1 . 6 95E+00 1 . 00 3E+00 2 . 698E+00 1 . 434 E+0

1

2 . 065E-01 4. 168E+00 -0.014 0.031 0.016 35.0000 1 . 70 9E + 00 i . 1 90E+00 2 . 399E+00 1 . 663E+0

1

2.329E-01 4 . 435E+00 -0.013 0.028 0.014

40.0000 1 .721 E+00 1 . 379E+00 3 . 1 OOE+OO 1 .830E+01 2.573E-01 4. 669E+00 -0.012 0.026 0.013

45.0000 1 . 732E+00 1 .56 9E+0 0 3.301 E+00 1 . 986E+01 2.799E-01 4 . 878E+00 -0.011 0.025 0.011 50.0000 1 . 741 E+OO 1 .761 E+00 3 . 502E+00 2. 1 33E+01 3.008E-01 5 . 068E+C0 -0.010 0.023 0.010 55.0000 1 . 749E+00 1 . 953E+00 3.703E+00 2 . 272E+0

1

3.203E-01 5.241 E+00 -0.009 0.022 0.010 60.0000 1 . 757E+00 2 . 1 47E+00 3. 903E+00 2 . 404E+0

1

3. 335E-01 5.401 E+00 -0 .008 0.021 0.009

70.0000 1 . 770E+00 2 . 535E+00 4 . 305E+00 2 . 647E+0

1

3.71 6E-01 5 . 687E+00 -0.007 0.020 0.008 80.0000 1 .781 E+00 2. 927E+00 4 . 707E+00 2 . 870 E+0

1

4.009E-01 5. 938E+00 -0.005 0.018 0.007

90.0000 1 . 7 90 E + 00 3 . 320E+00 5.1 10E+00 3 . 073E+0

1

4 . 270 E-0

1

6 . 1 6 1 E+0 0 -0.005 0.017 0.006 100.0000 1 . 799E+00 3.714E+00 5.51 3E+00 3 . 262E+0

1

4 . 505E-0

1

6.363E+00 -0.004 0.016 0.005

125.0000 1 .31 6E+00 4 . 707E+00 6 . 523E+00 3 . 678E+0

1

5.002E-01 6 . 7 94E+00 -0.003 0.015 0.004

150.0000 1 .330E+00 5 . 705E+00 7 . 535E+00 4.035E+01 5.402E-01 7 . 1 50E+00 -0.002 0.013 0.003

175.0000 1 . 342E+00 6 . 7 08E+00 8.549E+00 4 . 346 E + 0

1

5.732E-01 7 . 452E+00 -0.001 0.012 0.003 200.0000 1 .352E+00 7.71 4E+00 9 . 566E+00 4.622E+01 6.010E-01 7 . 7 1 6 E+0 0 -0.001 0.012 0.002 250.0000 1 . 36 9E + 00 9 . 734E+00 1 . 1 60E+01 5.096E+01 6 . 456 E-0

1

8. 157E+00 -0.001 0.011 0.002 300.0000 1 . 333E+00 1 . 1 76E+01 1 . 364E+01 5 . 493E+0

1

6 . 7 93 E-0

1

8.51 9E+00 -0.001 0.010 0.001 350.0000 1 . 394E+00 1 . 380E+01 1 .569E+01 5 . 834E+0

1

7.071 E-0

1

8 . 826E+0 0 -0.000 0.009 0.001 400.0000 1 . 904E+00 1 . 533E+0

1

1 . 774E+0

1

S.134E+01 7.295E-01 9.091 E+00 -0.000 0.009 0.001 450.0000 1.91 3E+00 1 . 787E+0

1

1 . 979E+01 6.401 E+0

1

7.483E-01 9 . 326E+00 -0.000 0.009 0.001 500.0000 1 . 921 E+00 1 . 992E+0

1

2. 184E+01 6.641 E+0

1

7.642E-01 9 . 53SE+00 -0.000 0.003 0.001 550.0000 1 . 928E+00 2. 1 96E+01 2.339E+01 6 . 360E+01 7 . 780 E-0

1

9 . 726E + 0 0 -0.000 O.COS 0.001 600.0000 1 . 934E+00 2.401 E+0

1

2 . 594E+0

1

7. 061 E+01 7 . 900E-0

1

9 . 900E+00 -0.000 0.008 0.001 700.0000 1 . 946E+00 2.81 1 E+01 3.005E+01 7.41 9E+01 3.101 E-0

1

1 . 021 E+0

1

-0.000 0.007 0.0C1 800.0000 1 . 956E+00 3 . 22 1 E+0

1

3.416 E+0

1

7 . 731 E+01 3.262E-01 1 . 047E+0

1

-0.000 0.007 0.001 900.0000 1 . 954E+00 3.631 E+0 1 3 . 828E+0

1

8 . 007E+0

1

8.395E-01 1 .071 E+0

1

-0.000 0.007 0.000 1000.0000 1 . 972E+00 4 . 042E+0

1

4.239E+01 8 . 255E+0

1

8.507E-01 1 . 0 92E+0

1

-0.000 0.007 0 .000 156
POSITRONS IN SILICON

T = 173.0 eV DENSITY = 2.330E+00 g/cm 3

ENERGY STOPPING PGLiER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) L05S RANGE YIELD

MeV MeV cm 2 /g MeV cm 2/g MeV cn 2 /g g/cn 2 0.0100 1 .893E+01 2.723E-03 1 . 894E+0

1

3.018E-04 6 . 5S5E-05 1 . 0 37E-0 3 -0.213 0.246 0.237 0.0125 1 . 5 94E + 0

1

2.975E-03 1 . 5 94E + 0

1

4 . 463E-04 S.570E-05 1 . 332E-0 3 -0.203 0.233 0.226

0.0150 1 . 385E+0

1

3. 185E-03 1 . 385E+0

1

6. 150E-04 1 .061 E-04 1 . 641 E-03 -0.196 0.224 0.217 0.0175 1 . 229E+0

1

3 . 366S-03 1 .229E+01 8.070E-04 1 . 27 0 E-0 4 1 . 963E-03 -0.191 0.217 0.211 0.0200 1 . 108E+01 3.525E-03 1 . 1 09E+01 1 .022E-03 1 .431 E-04 2.29SE-03 -0.187 0.211 0.205

0.0250 9 . 330E+00 3.799E-03 9 . 333E+00 1 .515E-03 1 . 909E-04 3 . 007E-03 -0. ISO 0.202 0.197 0.0300 3.11 2E+00 4 . 026E-03 3 . 1 1 6E+00 2.092E-03 2.344E-04 3 . 766 E

_ 0 3 -0.175 0.195 0.190 0.0350 7.215E+00 4.21 9E-03 7.21 9E+00 2.746E-03 2.731 E-04 4 . 572E-0 3 -0.170 0.139 0.185 0.0400 6 . 524E+00 4.338E-03 6 . 528E+0 0 3.476E-03 3.21 9E-04 5.424E-03 -0.167 0.185 0.181 0.0450 5 . 975E+00 4 . 542E-03 5. 979E+00 4.277E-03 3.657E-04 6 . 320 E-0 3 -0.164 0.181 0.178

0.0500 5 . 52SE+00 4.633E-03 5 . 532E+00 5. 147E-03 4.094E-04 7.257E-03 -0.162 0.178 0.175

0.0550 5. 156E+00 4.812E-03 5. 1 61 E+00 S . 034E-03 4.530E-04 3 . 23 5E-0 3 -0.160 0.176 0.172

0.0600 4 . 342E+00 4.933E-03 4.847E+00 7 . 084E-03 4. 966E-04 9.251 E-03 -0.158 0.173 0.170 0.0700 4.340E+00 5.152E-03 4 . 345E+00 9.263E-03 5.831 E-04 1 . 139E-02 -0.155 0.169 0.166 0.0800 3 . 956E+00 5.351E-03 3 . 962E+00 1 . 168E-02 6 . 687E-04 1 . 368E-02 -0.152 0.166 0.163 0.0900 3 . 653E+00 5.536E-03 3 . 659E+00 1 .431 E-02 7 . 536E-04 1 . 603E-02 -0.150 0.163 0.160 0.1000 3 . 408E+00 5.713E-03 3.41 4E+00 1 .71 4E-02 8.375E-04 1 .861 E-02 -0.148 0.161 0.158 0.1250 2. 960E+00 6 . 1 37E-05 2. 966E+00 2 . 503E-02 1 . 044E-03 2 . 53SE-02 -0.144 0.156 0.154

0.1500 2 . 657E+00 6 . 532E-03 2 . 664E+00 3.395E-02 1 . 247E-0 3 3.271 E-02 -0.141 0.152 0 . 1 5C

0 . 1750 2.440E+00 6 . 900E-03 2.446E+00 4.376E-02 1 . 446E-03 4 . 050E-02 -0.138 0.149 0.147 0.2000 2 . 276E + 0 0 7.253E-03 2 . 283E+00 5 . 435E-02 1 . 640E-03 4.868E-02 -0.136 0.147 0.145

0.2500 2.048E+00 7 . 960E-03 2 . 05 6 E+00 7.751 E-02 2.017E-03 6 . 592E-02 -0.131 0.143 0.141 0.3000 1 . 899E+00 3.634E-03 1 . 903E+00 1 .02SE-01 2 . 383E-Q 5 3 . 402E-02 -0. 123 0.139 0.137

0 . 3500 1 . 7 95E+00 9 . 423E-03 1 . 805E+00 1 . 298E-0

1

2.741E-03 1 . 027E-0

1

-0.125 0.136 0.134

0.4000 1 . 720E+00 1 .01 9E-02 1 . 730E+00 1 .5S1E-01 3.093E-03 1 . 21 6E-01 -0.122 0.134 0.132

0.4500 1 . 664E+00 1 .099E-02 1 . 675E+00 1 . 875E-0

1

3.441E-03 1 .407E-01 -0.120 0.132 0.129 0.5000 1 .621 E+00 1 . 180E-02 1 . 632E+00 2. 17SE-01 3 . 787E-03 1 . 599E-0

1

-0.113 0.130 0.127 0.5500 1 . 587E+Q0 1 . 265E-02 1 . 600E+00 2.437E-01 4.131 E-03 1 . 790E-01 -0.115 0.128 0.125

0.6000 1 .561 E+00 1 . 352E-02 1 . 574E+00 2.803E-01 4 . 473E-03 1 . 980E-01 -0.114 0.127 0.124

0.7000 1 . 523E+00 1 . 533E-02 1 . 538E+00 3.446E-01 5.159E-03 2.355E-01 -0.110 0.124 0.120 0.8000 1 .499E+00 1 . 723E-02 1 . 51 6E+00 4.101E-01 5 .848E-03 2.721 E-01 -0.107 0.121 0.117 0.9000 1 . 483E+00 1 . 921 E-02 1 . 502E+00 4.764E-01 6.540E-03 3.C77E-01 -0.104 0.119 0.115

1 .0000 1 . 473E+00 2. 1 26E-02 1 . 494E+00 5 . 432E-0

1

7 . 237E-0 3 3.424E-01 -0.102 0.117 0.112

1 .2500 1 . 462E+00 2.670 E-0 2 1 . 489E+00 7.1 10E-01 9.004E-03 4 . 24SE-0

1

-0.097 0.112 0.107

1 .5000 1 . 462E+00 3 . 257E-02 1 . 495E+00 3.736E-01 1 .031 E-02 5 . 020E-01 -0.092 0.103 0.103

1 .7500 1 . 46SE+00 3 . 875E-02 1 . 507E+00 1 . 045E+00 1 .26 6 E-0 2 5 . 747E-0

1

-0.038 0.105 0.099 2.0000 1 . 476E+00 4 . 520 E-0 2 1 . 52 1 E+00 1 . 21 OE+OO 1 . 454E-02 6 . 439E-0

1

-0.084 0.102 0.095 2.5000 1 . 494E+00 5.8S8E-02 1 . 553E+00 1 . 536E+00 1 .339E-02 7 . 743 E-0

1

-0.077 0.097 0 .0S9 3.0000 1 . 5 1 3E+00 7.332E-02 1 .586E+00 1 . 354E+00 2.234E-02 3. 976E-01 -0.071 0.093 0 . 083 3.5000 1 .530E+00 8.832E-02 1 . 6 1 8E+00 2.1 66E+00 2 . 635E-02 1 . 0 1 6E+00 -0.064 0.033 0.078 4.0000 1 . 545E+0 0 1 .038E-01 1 . 649E+00 2.472E+00 3 . 040E-02 1 .131 E+00 -0.058 0.085 0.073 4.5000 1 . 55 9E+00 1 . 1 98E-01 1 . 678E+00 2 . 773E+00 3.449E-02 1 . 243E+00 -0.053 0.031 0.063 5.0000 1 .571 E+00 1 . 362E-01 1 . 707E+00 3 . 06 8E+00 3.360E-02 1 . 351 E+00 -0.048 0.073 0.064 5.5000 1 . 532E+00 1 . 529E-0

1

1 . 735E+00 3.359E+00 4 . 272E-02 1 . 456E+00 -0.044 0.075 0.060

6.0000 1 .592E+00 1 .699E-01 1 . 762E+00 3 . 645E+00 4.685E-02 1 . 557 E+0 0 -0.041 0.072 0.057

7.0000 1 . 60 9E+00 2 . 045E-0

1

1 .81 4E+00 4 . 204E+00 5.510E-02 1 . 743E+0 0 -0.035 0.067 0.050 8.0000 1 . S24E+00 2.402E-01 1 . S64E+00 4 . 74SE+00 6.332E-02 1 . 925E+00 -0.031 0.063 0.045

9.0000 1 . 637E+00 2. 766E-01 1 . 91 4E+00 5 . 277E+00 7.147E-02 2. 088E+00 -0.028 0.059 0.041 10.0000 1 . 648E+00 3 . 1 36E-01 1 . 962E+00 5 . 794E+00 7. 955E-02 2.239E+00 -0.026 0.056 0 .038 12.5000 1 . 672E+00 4.078E-01 2. 080E+00 7.031 E+00 9.927E-02 2 . 574E+00 -0 .022 0.049 0.031 15.0000 1 .691 E+00 5 . 0 4 4E-0

1

2. 1 95E+00 8.201 E+00 1 . 183E-01 2.358E+00 -0.020 0.045 0 .027 17.5000 1 . 706E+00 6 . 029E-01 2.309E+00 9.311 E+00 1 . 364E-0

1

3. 1C5E+00 -0.013 0.041 0.023 20.0000 1 . 72CE+00 7.023E-01 2 . 422E+00 1 . 037E+0

1

1 .539E-01 3 . 323E+00 -0.017 0.033 0.021 25.0000 1 .742E+00 9.035E-01 2 . 646E+00 1 . 234E+0

1

1 .864E-01 3 . 6 94E+0 0 -0.015 0.034 0.013 30.0000 1 .760E+00 1 . 1 08E+00 2.863E+00 1 .416E+01 2 . 1 60E-01 4.00 3E+00 -0.014 0.031 0.015 35.0000 1 . 775E+00 1 . 31 4E+00 3.039E+00 1 . 584E+0

1

2.432E-01 4 . 268E+00 -0.012 0.028 0.013 40.0000 1 . 787E+00 1 . 523E+00 3.310E+00 1 .740E+01 2.682E-01 4.501 E+00 -0.011 0.026 0.012 45.0000 1 . 7 98E + 00 1 . 7 33E+0 0 3.531 E+00 1 . 886E+0

1

2.913E-01 4.70 9E+00 -0.011 0.025 0.011 50.0000 1 .308E+00 1 . 944E+00 3 . 752E+00 2 . 024E+0

1

3. 1 26E-01 4.397E+00 -0.010 0.023 0.010 55.0000 1 .81 7E+00 2. 156E+00 3 . 973E+00 2.1 53E+01 3.324E-01 5 . 063E+00 -0.009 0.022 0.009 60.0000 1 . 824E+00 2.369E+00 4.1 94E+00 2.27SE+01 3.509E-01 5 . 226E+00 -0.003 0.021 0.008 70.0000 1 .838E+00 2 . 793E+00 4 . 635E+00 2 . 502E+0

1

3.843E-01 5.509E+00 -0.007 0 .020 0 .007 30.0000 1 . 850 E+0 0 3 . 230E+00 5.079E+00 2 . 708E+0

1

4. 13SE-01 5 . 757E+00 -0.006 0.013 0.006 90.0000 1 .860E+00 3 . 663E+00 5 . 523E+00 2.897E+01 4.400E-01 5 . 979E+00 -0.005 0.017 0.006 100.0000 1 .S69E+00 4 . 0 99E + 00 5 . 967E+00 3.071 E+01 4.636E-01 6 . 1 79E+00 -0.004 0.016 0 .005 125.0000 1 . 837E + 0 0 5.1 93E+00 7 . 030E+00 3 . 455E+0

1

5. 1 31 E-01 6 . 606E+00 -0.003 0.015 0.004

150.0000 1 . 932E+00 6 . 294E+00 3. 1 9SE+00 3. 783E+0

1

5.529E-01 6 . 960E+00 -0.002 0.013 0.003 175.0000 1 . 91 4E+00 7.401 E+00 9.315E+00 4.069E+01 5 .356E-01 7.261 E+00 -0.002 0.013 0.003

200 . 0000 1 . 925E+O0 3.51 1 E+00 1 . 044E+0

1

4 . 323E+0

1

6 . 1 31 E-01 7.524E+00 -0.001 0.012 0.002 250.0000 1 . 942E+00 1 . 074E+0

1

1 . 268E+0

1

4 . 757E+0

1

6.569E-01 7 . 964E+00 -0.001 0.011 0.002 300.0000 1 . 956E+00 1 . 298E+0

1

1 . 493E+01 5.11 9E+0

1

6 . 905E-01 3. 325E+00 -0.001 0.010 0.001 350.0000 1 . 968E+00 1 . 522E+0

1

1 .71 9E+01 5.431 E+0

1

7.172E-01 8.631 E+00 -0.001 0.009 0.001 400.0000 1 . 978E+00 1 . 747E+01 1 . 944E+01 5.705E+01 7.391E-01 8 . 397E+00 -0.000 0.009 0.001 450.0000 1 . 9S3E+00 1 . 972E+01 2. 171E+01 5.943E+01 7.574E-01 9.131 E+00 -0.000 0.009 0.001

500 .0000 1 . 996E+00 2. 1 97E+01 2 . 397E+0

1

6.167E+01 7.729E-01 9.341 E+00 -0.000 0.008 0.001 550.0000 2 . 003E+00 2.423E+01 2 . 623E+0

1

6 . 366E+0

1

7.363E-01 9.531 E+00 -0.000 0.008 0.001 600.0000 2.01 0E+00 2 . 643E+0

1

2 . 849E+01 6 .54SE+01 7.980E-01 9 . 705E+00 -0.000 0.003 0 .001 700.0000 2 . 022E+00 3. 100E+01 3.303S+01 6 . 575E+0

1

8. 175E-01 1 . 001 E+01 -0.000 0.007 0.001 800.0000 2 . 0 32E+00 3 . 553E+0

1

3 . 756E+01 7. 159E+01 3.331E-01 1 . 028E+0

1

-0.000 0.007 0.001 900.0000 2.041 E+00 4 . 006E+0

1

4 .21 0E+01 7.410E+01 8.460E-01 1 .051 E+01 -0.000 0.007 0.000

1 000.0000 2 . 049E+00 4.459E+01 4 . 664E+01 7 . 636E+0

1

3 . 567E-0

1

1 . 072E+0

1

-0.000 0.007 0.000

157
POSITRONS IN COPPER

I = 322.0 eV DENSITY = 8.960E+00 g/cm 3

ENERGY STOPPING POUER CSDA RADIATION DENS.EFF. dClog )/<J(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cm 2 /g MeV cn 2 /g g/ci 2 0.0100 1 . 504E+0

1

2.358E-03 1 . 505E + 0

1

3.893E-04 3.275E-05 1 . 244E-0 3 -0.245 0.293 0.277 0.0125 1 . 275E+0

1

3.206E-03 1 . 275E + 0

1

5.706E-04 1 . 103E-04 1 . 535E-0 3 -0.233 0.276 0.262

0.0150 1 . 1 13E+01 3.49SE-03 1.11 3E+01 7 .31 0E-04 1 . 390E-04 1 . 933E-03 -0.224 0.263 0.250 0.0175 9.913E+00 3.755E-03 9 . 91 7E+00 1 .019E-03 1 .6S7E-04 2.304E-03 -0.217 0.253 0.241 0.0200 8 . 967E+00 3.991E-03 8.971 E+00 1 . 285E-0 3 1 . 990E-04 2.633E-03 -0.211 0.245 0.234

0.0250 7 . 585E+00 4.411 E-03 7 . 590E+00 1 .393E-03 2.617E-04 3.431 E-03 -0.202 0.232 0.223

0.0500 6.61 9E+00 4.730 E-0

3

6 . 624E+00 2.601 E-03 3.267E-04 4.334E-03 -0.196 0.223 0.215

0.0350 5.903E+00 5. 103E-03 5 . 90SE + 00 3.402E-03 3. 932E-04 5.247E-03 -0.190 0.216 0.209

0.0400 5 . 350E+00 5 . 390E-03 5 . 356E+00 4.292E-03 4.609E-04 6 . 220 E-0 3 -0.186 0.210 0.203

0.0450 4.909E+00 5.659E-03 4.91 5E+00 5 . 268E-03 5.296E-04 7.259E-03 -0.132 0.205 0.199

0.0500 4 . 549E + 00 5. 91 2E-03 4 .555E+00 6.325E-03 5 . 991 E-04 8.365E-03 -0.179 0.201 0.195

0.0550 4 . 249E+00 S.143E-03 4 . 255E + 00 7.462E-03 6 .693E-04 9 . 542E-03 -0.177 0.193 0.192

0.0600 3. 995E + 00 6.366 E-C 3 4.001 E+00 3.675E-03 7 . 400E-04 1 . 080E-02 -0.174 0.194 0.139

0.0700 3 . 5SSE + 00 6 . 767E-03 3.595E+00 1 . 1 32E-02 8 . 824E-04 1 . 354E-02 -0.170 0.189 0.134

0.0300 3.276 E + 00 7.134E-03 3 . 283E+00 1 . 423E-02 1 . 026 E~0 3 1 .664E-02 -0.166 0.135 0.130

0.0900 3 . 029E+00 7.479E-03 3 . 037E+00 1 . 740E-02 1 .169E-03 2.01 3E-02 -0.162 0.181 0.176 0.1000 2 . 829E + 00 7 . 807E-0 3 2 . 837E+00 2.081E-02 1 .313E-03 2 . 404E-0 2 -0.159 0.178 0.173

0.1250 2 . 462E + 00 8 . 567E-03 2.471 E+00 3 . 029E-02 1 . 673E-03 3.533E-02 -0.152 0.170 0.166

0.1500 2.21 3E+00 9.266E-03 2 . 223E+00 4.099E-02 2 . 030E-03 5 . 053E-02 -0.144 0.164 0.160

0.1750 2.034E+00 9. 932E-03 2.044E+00 5 . 274E-02 2 . 385E-0 3 6 . 75SE-02 -0.138 0.159 0.155

0.2000 1 . 8 93E+0 0 1 . 053E-02 1 . 909E+00 6 . S42E-02 2 . 738E-03 8.595E-02 -0.133 0.154 0.150

0.2500 1 .709E + 00 1 . 1S3E-02 1 .721 E+00 9.310E-02 3 . 435E-03 1 . 236 E-0

1

-0.126 0.147 0.142

0 .3000 1 . 585E+00 1 .31SE-02 1 . 599E+00 1 . 233E-0

1

4. 125E-03 1 . 603E-0

1

-0.121 0.141 0.136

0.3500 1 . 499E+00 1 .450E-02 1 .51 4E+00 1 . 555E-0

1

4.809E-03 1 . 958E-0

1

-0.117 0.136 0.131 0.4000 1 . 436E+00 1 . 536E-02 1 . 452E+00 1 . 8.9 3E-0

1

5.489E-03 2.302E-01 -0.113 0.132 0.127

0 . 4500 1 . 390E + 00 1 . 72SE-02 1 . 407 E+0 0 2 . 243E-0

1

6 . 1 68E-03 2.635E-01 -0.110 0.123 0.123

0.5000 1 . 354E + 00 1 .375E-02 1 . 373E+00 2.603E-01 6.349E-03 2. 958E-01 -0.107 0.126 0.120 0.5500 1 . 326 E+ 0 0 2.027E-02 1 . 346E+00 2 . 971 E-0

1

7.531 E-03 3.273E-0 1 -0.105 0.123 0 . 1 1S 0.6000 1 . 304E+00 2. 183E-02 1 . 326E+00 3.345E-01 8.217E-03 3.531 E-0

1

-0.103 0.121 0.115

0.7000 1 . 273E + 00 2.502E-02 1 . 293E+00 4. 108E-01 9 . 596E-03 4. 173E-01 -0.099 0.117 0.111 0.8000 1 . 253E+00 2.331E-02 1 .281 E+00 4 . S84E-0

1

1 .098E-02 4 . 739E-0

1

-0.096 0.113 0.107

0.9000 1 . 23 9E + 00 3. 173E-02 1 . 27 1 E+00 5.668E-01 1 . 238E-02 5 . 230E-0

1

-0.093 0.110 0.104

1 .0000 1 .231 E+00 3 . 527E-02 1 . 266E+00 6 . 456E-01 1 . 373E-02 5.799E-01 -0.090 0.108 0.101

1 .2500 1 . 222E+00 4 . 464E-02 1 . 267E+00 8.432E-01 1 . 7 3 3E-0 2 7.01 IE-01 -0.085 0.102 0.095

1 .5000 1 . 223E+00 5 . 467E-02 1 . 277E+00 1 . 040E+00 2.094E-02 8 . 1 2 1 E-0

1

-0.080 0.093 0.090

1 .7500 1 . 227E+00 6.521E-02 1 . 292E+00 1 . 234E+00 2.461E-02 9.149E-01 -0 . 076 0.094 0.086 2.0000 1 . 234E+00 7.618E-02 1 .31 0E+00 1 . 427E+00 2 . 832E-02 1.011 E+00 -0.073 0.091 0.082

2.5000 1 . 249E+00 9. 928E-02 1 . 348 E+00 1 . 803E+00 3 . 5S4E-02 1 . 186E+00 -0.067 0.036 0.076

3.0000 1 . 264E+00 1 . 237E-0

1

1 . 388E+00 2. 1 69E+00 4 . 343E-02 1 . 343E+00 -0.062 0.081 0.071 3.5000 1 . 278E+00 1 .491 E-0

1

1 . 427E+00 2 . 524E+00 5. 106E-02 1 . 486E+00 -0.058 0.077 0.066 4.0000 1 . 292E+00 1 . 753E-0

1

1 . 467E+00 2.869E+00 5 . 868E-02 1 . 6 1 7E+00 -0.055 0.074 0.062

4.5000 1 . 304E+00 2.022E-01 1 . 506E+00 3 . 20 6 E + 0 0 6 . 62SE-02 1 . 738E+00 -0.053 0.071 0.059

5.0000 1 . 315E+00 2.293E-01 1 . 545E+00 3 . 533E+00 7.379E-02 1 . 850E+00 -0.050 0.069 0.056 5.5000 1 . 325E+00 2.580E-01 1 . 583E+00 3 . 353E+00 8. 125E-02 1 . 954E+00 -0.049 0.067 0.054

6.0000 1 . 335E+00 2.868E-01 1 . 6 22E+0 0 4. 165E+00 8.864E-02 2.052E+00 -0.047 0.065 0.051 7.0000 1 . 352E+00 3.453E-01 1 . 6 93E+00 4 . 763E+0 0 1 .052E-01 2 . 229E+00 -0.045 0.061 9.048

3.0000 1 . 367E+00 4.061 E-0

1

1 . 773E+00 5 . 344E + 00 1 . 173E-01 2 . 388E+00 -0.043 0 .058 0.045

9.0000 1 .380E+00 4.678E-01 1 . 848E+00 5 . 896E+00 1 .31 IE-01 2 . 532E+00 -0.041 0.056 0.042

1 0.0000 1 . 392E+00 5.309E-01 1 . 923E+00 6 . 427E+00 1 . 445E-0

1

2.664E+00 -0.039 0.054 0.040

12.5000 1 . 41 7E+00 6.927E-01 2.1 10E+00 7 . 66SE+00 1 . 76 1 E-0

1

2. 951 E+00 -0 .036 0.049 0.035

15.0000 1 . 437E+00 3.581 E-0

1

2 . 295E+00 8 . 80 3E+0 0 2.054E-01 3. 1 94E+00 -0.034 0.046 0.032

17.5000 1 . 454E+00 1 . 027E+00 2.431 E+00 9.851E+0C 2.324E-01 3 . 407E+00 -0.031 0.043 0.029

20.0000 1 . 468E+00 1 . 1 93E+00 2 . 667E+00 1 . 082E+0

1

2.573E-01 3 . 597E+00 -0.029 0.041 0.026 25.0000 1 . 491 E+00 1 . 54SE+00 3 . 039E+00 1 . 253E+0

1

3.019E-01 3 . 927E+00 -0.025 0.037 0.022

30.0000 1 . 5 ! 0E+00 1 . 902E+00 3.41 1E+00 1 .41 3E+01 3.406E-01 4.209E+00 -0.021 0.034 0.019

35.0000 1 . 524E+00 2.251 E+00 3 . 735E+0 0 1 . 552E+0

1

3.745E-01 4 . 4 56E + 0 0 -0.019 0.032 0.017

40.0000 1 . 537E+00 2 . 624E+00 4.161 E+00 1 . 678E+0

1

4 . 045E-0

1

4 . 676E+00 -0.017 0.030 0.015 45.0000 1 . 548E+00 2. 989E+00 4 . 537E+0 0 1 . 7 93E + 0

1

4. 31 3E-01 4 . 874E+00 -0.015 0.028 0.013

50 .0000 1 . 557E+00 3 . 355E+00 4.91 2E+00 1 . 8 9 9E+0

1

4 . 553E-0

1

5 . 054E+00 -0.014 0.027 0.012

55.0000 1 . 565E+00 3 . 723E + 00 5 . 288E+00 1 . 997E+0

1

4.769E-01 5.21 9E+00 -0.012 0.026 0.011 60.0000 1 . 573E+00 4. 093E+00 5 . 666E+00 2 . 038E+0

1

4.966 E-0

1

5. 372E+00 -0.012 0.025 0.010 70.0000 1 . 536 E+00 4.337E+00 6 . 423E+00 2 . 254E+0

1

5.312E-01 5 . 646E+00 -0.010 0.023 0.009

30.0000 1 . 5 97E+0 0 5 . 534E+00 7.131 E+00 2 . 40 1 E+0

1

5.605E-01 5 . 386 E+0 0 -0.009 0.022 0.008

90.0000 1 . 607E+00 6 . 330E+00 7 . 937E+00 2 . 534E+0

1

5 . 35SE-0

1

6 . 1 OOE+OO -0.008 0.021 0.007

100.0000 1 . 6 1 6E+00 7.079E+00 S.694E+00 2.654E+01 6 .073E-01 6 . 292E+00 -0.008 0.020 0.006 125.0000 1 . 634E+00 3. 953E+00 1 .059E+91 2.914E+01 6 . 524E-0

1

6 . 705E+00 -0.007 0.018 0.005

150.0000 1 . 648E+00 1 . 035E+0

1

1 .250E+01 3 . 1 3 1 E+0

1

6 .866E-01 7 . 046E+00 -0.006 0.017 0.004

175.0000 1 . 660E+00 1 . 275E+0

1

1 .441 E+01 3.317E+01 7.1 33E-01 7 . 336E+00 -0.005 0.016 0.003

200 . 0000 1 . 670E+00 1 . 465E+0

1

1 . 632E+01 3 . 430E+01 7 . 360E-01 7 . 590E+00 -0.004 0.016 0.003 250.0000 1 . 687E+00 1 . 847E+0

1

2.015E+01 3 . 755E+0

1

7.703E-01 8.01 7E+00 -0.004 0.014 0.002

300.0000 1 .701 E+00 2.230E+01 2.400E+01 3. 982E+01 7. 953E-01 8 . 370E+00 -0.003 0.014 0.002 350.0000 1 . 7 1 2E+00 2.61 3E+01 2 . 734E+0

1

4. 176E+01 8. 155E-01 8 . 670E+00 -0.002 0.013 0 .002

400 .0000 1 . 722E+00 2. 998E+01 3. 170E+01 4 . 344E+0

1

8.314E-01 8. 931 E+00 -0.002 0.013 0.002 450.0000 1 . 7 30 E + 0 0 3 . 332E+0

1

3.555E+01 4.493E+01 8 . 444E-0

1

9 . 1 62E+00 -0.002 0.012 0.001 500.0000 1 . 738E+00 3.767E+01 3.941 E+0

1

4.626E+01 8.553E-01 9. 369E+00 -0.001 0.012 0.001 550.0000 1 . 745E+00 4. 1 53E+01 4 . 327E+0

1

4 . 747E+0

1

8.646E-01 9 . 55SE+00 -0.C01 0.011 0.001 600.0000 1 .751 E+00 4 . 539E+01 4.714E+01 4.358E+01 8.727E-01 9 . 7 30E+0 0 -0.001 0.011 0.901 700.0000 1 . 762E+00 5.31 1E+01 5 . 487E+0

1

5 . 054E+0

1

8 . S60E-0

1

1 . 004E+0

1

-0.001 0.011 0.001 800.0000 1 . 772Ei OO 6.083E+01 6 . 260E + 0 1 5 . 225E+0

1

8.964E-01 1 . 0 30 E+0

1

-0.001 0.010 0.001 900.0000 1 . 730 E+0 0 6 . 856E+0

1

7.034E+01 5. 376E+01 9.050E-01 1 . 053E+0

1

-0.001 0.010 0.001 1000.0000 1 . 737E+00 7 . 629E+0

1

7 . 8C8E+01 5.510E+01 9.121E-01 1 . 074E+0

1

- 0.000 0.010 0.001

158
POSITRONS IN GERMANIUM

I = 350.0 eV DENSITY = 5 . 323E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. dClog )/d( loql

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. CDLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cra 2/g MeV cm 2/g MeV cm 2 /g g/cra 2 0.0100 1 . 424E+0

1

2.805E-03 1 . 424E+0

1

4.131E-04 S.503E-05 5.175E-04 -0.250 0.301 0.283 0.0125 1 . 208E+0

1

3. 153E-03 1 . 203E+0

1

6 . 045E-04 1 . 1 3SE-04 6 . 6 32E-04 -0.237 0.233 0.267

0.0150 1 . 055E+0

1

3 . 465E-03 1 . 055E+01 8.256E-04 1 . 440E-04 3.152E-04 -0.228 0.269 0.255 0.0175 9.403E+00 3 . 728E-03 9 . 407E+00 1 . 07SE-03 1 . 752E-04 9 . 734E-04 -0.221 0.259 0.246 0.0200 8.51 1E+00 3. 962E-03 3.515E+00 1 . 353E-0 3 2.071E-04 1 . 1 3SE-03 -0.215 0.250 0.239

0.0250 7 . 205E+00 4.373E-03 7.209E+00 1 . 999E-03 2 . 728E-04 1 . 484E-03 -0.206 0.237 0.227

0.0300 6.291 E+00 4.747E-05 6 . 2 96E+0 0 2.743E-03 3.407E-04 1 . 353E-03 -0.199 0.223 0.219 0.0350 5.6I3E+00 5.079E-03 5.61 8E+00 3 . 535E-03 4 . 1 05E-04 2.244E-03 -0.194 0.221 0.213 0.0400 5 . 089E+00 5.380E-03 5.094E+00 4 . 521 E-03 4.S17E-04 2 . 656E-03 -0.190 0.215 0.207 0.0450 4.671 E+00 5 . 649E-03 4 . 677E+00 5.547E-03 5.539E-04 3.089E-03 -0.186 0.210 0.203

0.0500 4 . 330E+00 5. 900E-03 4 . 336E+00 6 . 6 58E-0 3 6 .269E-04 3.541 E-03 -0.133 0.205 0.199

0.0550 4 . 045E+00 6 . 1 43E-03 4.051 E+00 7.852E-03 7 . 007E-04 4.013E-03 -0.131 0.202 0.196 0.0500 3 . 304E+00 6.374E-03 3.311 E+00 9.126E-03 7.752E-04 4.502E-03 -0.173 0.199 0.193

0.0700 3.41 8E + 00 6.801E-03 3 . 425E+00 1 . 1 90E-02 9.257E-04 5 . 535E-03 -0.174 0.193 0.188

0.0800 3. 123E+00 7.188E-03 3 . 1 30E+00 1 . 496E-02 1 . 073E-0 3 6 . 634E-03 -0.171 0.189 0.184

0.0900 2.839E+00 7.551 E-03 2.896E+00 1 . S28E-02 1 . 230E-03 7.7S5E-03 -0.168 0.135 0.131 0.1000 2.699E+00 7 . 894E-03 2 . 70 7E + 0 0 2. 1 86E-02 1 . 384E-03 9.014E-03 -0.166 0.132 0.178

0.1250 2 . 35 1 E+00 3.703E-03 2 . 360E+00 3. 179E-02 1 . 767E-03 1 . 230E-02 -0.161 0.176 0.172

0.1500 2.1 16E+00 9 . 449E-03 2 . 1 25E+00 4.293E-02 2.151 E-03 1 . 583E-02 -0.157 0.172 0.16S 0.1750 1 . 946E+00 1 .015E-02 1 . 956E+00 5.527E-02 2.532E-03 1 . 973E-02 -0.154 0.168 0.165 0.2000 1 .81 9E+00 1 . 083E-02 1 . 830E+0 0 6.850E-02 2.910E-03 2.381 E-02 -0.152 0.165 0.162

0.2500 1 . 642E+00 1 .217E-02 1 . 654E+00 9.734E-02 3.656E-03 3 . 258E-02 -0.147 0.160 0.157

0.3000 1 . 526 E+0 0 1 . 352E-02 1 . 539E+00 1 . 237E-0

1

4.392E-03 4.209E-02 -0.143 0.156 0.153

0 . 3500 1 .446E+00 1 .490E-02 1 . 460E+00 1 .621E-01 5. 120E-03 5 . 225E-02 -0.140 0.153 0.149

0.4000 1 . 388E+00 1 .631E-02 1 . 404E+00 1 . 971 E-01 5.844E-03 6 . 300E-02 -0.136 0.150 0.146 0.4500 1 . 344E+00 1 . 778E-02 1 . 362E+00 2.333E-01 6 . 565E-03 7 . 432E-02 -0.133 0.147 0.144

0.5000 1 . 31 2E+00 1 . 929E-02 1 . 331 E+00 2.704E-01 7 . 286E-03 8.61 9E-02 -0.130 0.145 0.141 0.5500 1 . 286E+00 2.037E-02 1 . 307E+00 3.083E-01 8 . 007E-03 9 . 857E-0 2 -0.127 0.143 0.138

0 .6000 1 . 267E+00 2 . 250E-02 1 .289E+00 3.469E-01 8.732E-03 1 .1 14E-01 -0.124 0.140 0.136 0.7000 1 . 23 9E+00 2 . 588E-02 1 . 265E+00 4.252E-01 1 .01 9E-02 1 . 386E-0

1

-0.119 0.136 0.131 0.8000 1 .221 E+OO 2 . 940E-02 1 . 25 1 E+00 5.048E-01 1 . 1 67E-02 1 . 673E-0

1

-0.113 0.133 0.127

0 . 9000 1 . 21 0E+00 3.302E-02 1 . 243E+0 0 5.850E-01 1 . 31 5E-02 1 . 973E-01 -0.109 0.129 0.123

1 .0000 1 . 203E+00 3 . 675E-02 1 . 240E+00 6.656E-01 1 . 465E-02 2.282E-01 -0.104 0.126 0.119

1 .2500 1 . 1 97E+00 4.658E-02 1 . 244E+00 3.671 E-01 1 . 342E-02 3 . 083E-01 -0.095 0.119 0.111

1 .5000 1 . 1 99E+00 5.707E-02 1 . 257E+00 1 . 067E+00 2 . 225E-02 3.894E-01 -0.088 0.113 0.104

1 .7500 1 . 20 5E+0 0 6.811 E-02 1 . 273E+00 1 . 265E+00 2.614E-02 4.695E-01 -0.082 0.108 0.097

2.0000 1 .21 3E+00 7.959E-02 1 . 292E+00 1 . 460E+0 0 3.007E-02 5.474E-01 -0.077 0.104 0.092

2.5000 1 . 22 9E+00 1 . 036E-0

1

1 . 332E+00 1 .841 E+00 3.799E-02 6 . 953E-01 -0 . 070 0.095 0 . 033 3.0000 1 . 245E+00 1 .239E-01 1 . 37 4E+00 2.21 OE+OO 4 . 596E-02 8.323E-01 -0.065 0.091 0.076

3.5000 1 . 260 E+OO 1 . 553E-0

1

1 .41 5E+00 2.56 9E+00 5 . 394E-02 9.593E-01 -0.060 0.086 0.071 4.0000 1 . 273E+0 0 1 . 825E-0

1

1 . 456E+00 2.917E+00 6.1 90 E-02 1 . 077E+00 -0.057 0.082 0.066 4.5000 1 . 286E+00 2.105E-01 1 . 496E+00 3 . 256E+00 6 . 931 E-02 1 . 188E+00 -0.053 0.078 0.062

5.0000 1 . 297E+0 0 2.391E-01 1 . 53SE+00 3 . 586E+00 7.765E-02 1 . 292E + 0 0 -0.051 0.075 0.059

5.5000 1 . 307E+00 2.632E-01 1 . 576E+00 3. 907E+00 8 . 540 E-02 1 . 3S9E + 00 -0.049 0.072 0.056 6.0000 1 . 31 7E+00 2.979E-01 1 .615E+00 4.221 E+00 9 . 307E-02 1 .481 E+00 -0.047 0.070 0.053

7.0000 1 . 334E+00 3.539E-01 1 . 6 93E+00 4.325E+00 1 .081 E-01 1 .651 E+00 -0.044 0.066 0.049

8.0000 1 . 349E+00 4.216E-01 1 . 770E+0 0 5 . 403E+00 1 . 227E-0

1

1 . 805E+00 -0.041 0.062 0.045

9.0000 1 . 362E+00 4.355E-01 1 . 847E+00 5. 956E+00 1 .369E-01 1 . 945E+00 -0.039 0.059 0.042

10.0000 1 . 373E+00 5.505E-01 1 . 924E+00 6 . 486E+00 1 . 507E-0

1

2 . 074E+00 -0.037 0.057 0.039

12.5000 1 . 393E+00 7. 180E-01 2.1 16E+00 7 . 725E+00 1 .332E-01 2 . 357E+00 -0.034 0.051 0.034

15.0000 1 . 41 7E+00 8.908E-01 2 . 303E+00 8 . 856E+00 2.1 32E-01 2.597E+00 -0.032 0.048 0.031 17.5000 1 . 434E+00 1 . 067E+00 2.501 E+00 9 . 396E+00 2.409E-01 2.806E+00 -0.030 0.045 0.028

20 .0000 1 . 448E+00 1 . 245E+00 2 . 6 93E+00 1 .036E+01 2.663E-01 2. 991 E+00 -0 . 028 0.042 0.025 25.0000 1 .471 E+00 1 . 6 1 0E+00 3.031 E+00 1 .259E+01 3 . 1 18E-01 3.31 1E+00 -0.025 0.038 0.022 30.0000 1 . 48 9E+0 0 1 . 982E+00 3 . 472E+00 1 .412E+01 3.51 IE-01 3 . 583E+00 -0 .023 0.035 0.019 35.0000 1 . 504E+00 2.359E+0O 3 . 863E+00 1 . 549E+0

1

3.854E-01 3.820E+00 -0.020 0.033 0.017 40.0000 1 .51 7E+00 2 . 739E+00 4 . 256E+00 1 . 572E+01 4.157E-01 4.031 E+00 -0.013 0.031 0.015 45.0000 1 . 528E+00 3. 125E+00 4 . 652E+00 1 . 784E+0

1

4.426E-01 4 . 222E+00 -0.017 0.029 0.013 30.0000 1 . 537E+00 3 .51 3E+00 5 . 050E+00 1 . 887E+0

1

4.667E-01 4 . 396E+00 -0.015 0 .028 0.012 55.0000 1 . 546E+00 3.901 E+00 5 . 447E+00 1 . S33E+01 4.885E-01 4.556E+00 -0.014 0.027 0.011 60.0000 1 . 553E+00 4 . 290E+00 5 . 343E+00 2.071 E+01 5 . 032E-0

1

4 . 704E+0 0 -0.013 0.026 0.010 70.0000 1 .567E+00 5 . 073E+00 6.63 9E+00 2 . 232E+0

1

5 . 427E-0

1

4. 971 E+0 0 -0.011 0 .024 0.009 80.0000 1 . 573E+00 5 . 86 1 E+00 7 . 43SE+00 2 . 374E+0

1

5.71 9E-01 5 . 206E+00 -0.010 0.023 0.003

90.0000 1 . 537E+00 6. 651 E+00 8 . 239E+00 2.502E+01 5.971 E-01 5.417E+00 -0.009 0.022 0.007 100.0000 1 . 596E+00 7 . 444E+00 9.039E+00 2.61SE+01 6.189E-01 5 . 607E+00 -0.008 0.021 0.006 125.0000 1 .613E+00 9 . 420 E+OO 1 . 103E+01 2 . S67E+0

1

6.630E-01 6.015E+00 -0.007 0.019 0 .005

1 50.0000 1 . 628E+00 1 . 1 41 E+01 1 .303E+01 3.076E+01 6 . 967E-0

1

6 . 352E + 00 -0 .006 0.013 0.004 175.0000 1 . 63SE+00 1 .340E+01 1 . 504E+01 3 . 254E+0

1

7.234E-01 6 . 640E+00 -0.005 0.017 0.004 200.0000 1 . 649E+00 1 .539E+01 1 . 704E+01 3.410E+01 7.451E-01 6.891 E+00 -0.005 0.016 0.003 250.0000 1 . 666E+00 1 . 940E+01 2.107E+01 3.674E+01 7.786E-01 7.315E+00 -0.004 0.015 0 .002 300.0000 1 . 6 7 9E+00 2 . 342E+0

1

2.51 0E+01 3.891 E+01 8 . 034E-01 7 . 664E+00 -0.003 0.014 0.002 350.0000 1 .691 E+00 2 . 744E+0

1

2.914E+01 4 . 075E+0

1

8.226E-01 7.961 E+00 -0.003 0.014 0.002 400.0000 1 .700E+00 3.148E+01 3.318E+01 4 . 236E+0

1

8.380E-01 8 . 220 E+00 -0.002 0.013 0.002 450.0000 1 . 703E+00 3 . 552E+0

1

3 . 722E+01 4 . 378E+0

1

S.506E-01 3-449E+00 -0.002 0.013 0.001 500.0000 1 .71 6E+00 3 . 956E+0

1

4 . 1 27E+01 4 . 506E+0

1

3.612E-01 8 . 555E+00 -0.002 0.012 0.001 550.0000 1 . 723E+00 4.360E+01 4 . 533E+0

1

4.621 E+0

1

3 . 702E-01 8 . 842E+00 -0.002 0.012 0.001 600.0000 1 . 725E+00 4 . 755E+0

1

4. 93SE+01 4 . 727E+0

1

8.780E-01 9.01 4E+00 -0.001 0.012 0.001 700.0000 1 . 739E+00 5.576E+01 5 . 750E+0

1

4. 915E+01 8. 907E-01 9. 318E+00 -0.001 0.011 0.001 800 .0000 1 . 749E+00 6 . 387E+0

1

6 . 562E+01 5 . 077E+0

1

9.009E-01 9 . 5S2E+00 -0.001 0.011 0.001

S00 .0000 1 . 757E+00 7.1 >9E+01 7.374E+01 5.221 E+0

1

9.091 E-01 9.81 5E+00 -0.001 0.011 0.001 1000.0000 1 . 764E+00 8. Oil E+01 3 . 133E+01 5 . 350E+0

1

9.159E-01 1 .002E+01 -0.001 0.011 0.001

159
POSITRONS IN SILVER

I = 470.0 eV DENSITY = 1 .050E+0:1 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CCRR

.

COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cra

2 /g g/cu 2 0.0100 1 . 303E+0

1

2.312E-03 1 . 303E+0

1

4 . 590E-04 8.91 6E-05 1 . 126E-03 -0.270 0.334 0 . 308 0.0125 1 . 1 1 0E+01 3.231E-03 1 .110E+01 6.676 E-04 1 .21 9E-04 1 . 445E-03 -0.255 0.312 0.239

0.0150 9.724E+00 3 . 602E-03 9 . 727E+00 9 . 038E-04 1 . 567E-04 1 .781 E-03 -0.244 0.295 0.275

0.0175 8 . 63SE+00 3.933E-03 8 . 6 92E+00 1 .181 E-03 1 . 930E-04 2.1 35E-03 -0.236 0.233 0.264

0.0200 7.877E+00 4.222E-03 7 . 882E+00 1 .434E-03 2. 307E-04 2 . 508E-03 -0.229 0.272 0.256

0.0250 6 . 637E+00 4.733E-03 6 . 6 92E+00 2. 175E-03 3.038E-04 3.312E-03 -0.219 0.257 0.243

0.0300 5.851E+00 5 . 200E-03 5 . 856E+00 2.976 E-0 3 3. 902E-04 4.203E-03 -0.211 0.246 0.233

0.0350 5 . 229E+00 5 . 606E-03 5 . 234E + 00 3 .881 E-03 4.744E-04 5. 1 90E-03 -0.205 0.237 0.226 0.0400 4 . 746E+00 5 . 970E-03 4 . 752E+00 4.385E-03 5 . 605E-04 6 . 284E-03 -0.200 0.230 0.220 0.0450 4.361E+00 6 . 308E-03 4 . 367E+00 5. 934E-03 6.433E-04 7 . 495E-03 -0.196 0.224 0.215

0.0500 4 . 046E + 00 6 . 62SE-03 4 . 0 52E+00 7.173E-03 7.374E-04 8 . 8 36 E-0 3 -0.192 0.219 0.210

0.0550 3 . 783E+00 6 . 935E-03 3 . 7 90E + 00 3.450E-03 8 . 278E-04 1 . 032E-02 -0.189 0.214 0.206 0.0600 3 . 560E+00 7.230E-03 3 . 567E+00 9.81 IE-03 9.1 95E-04 1 . 1 96E-02 -0.136 0.211 0.203

0.0700 3 . 202E+00 7.791 E-03 3 . 209E + 00 1 . 277E-0 2 1 . 106E-03 1 . 573E-02 -0.130 0.204 0.197

0.0800 2 . 927E+00 3.318E-03 2. 935E+00 1 . 604E-02 1 . 297E-03 2 . 022E-02 -0.175 0.199 0.192

0.0900 2 . 708E+00 3.308E-03 2.71 7E+00 1 . 958E-02 1 . 490E-03 2 . 543E-02 -0.171 0.194 0.138

0.1000 2.531 E+00 9.26SE-03 2 . 540E+00 2.339E-02 1 . 686 E-0 3 3. 125E-02 -0.167 0.190 0.184

0.1250 2.206E+00 1 . 037E-02 2.21 6E+00 3 . 3 97E-02 2.181 E-03 4 . 754E-02 -0.159 0.131 0.175

0.1500 1 . 985E+00 1 . 140E-02 1 . 996E+00 4 . 533E-02 2.633E-03 6 . 453E-02 -0.154 0.174 0.169

0.1750 1 .826E+00 1 . 236E-02 1 . 838E+00 5.396E-02 3. 188E-03 8.11 IE-02 -0.150 0.169 0.164

0.2000 1 . 706E+00 1 . 328E-02 1 .71 9E+00 7 . 304E-02 3.692E-03 9 . 702E-02 -0.146 0.165 0.160 0.2500 1 . 539E+00 1 .509E-02 1 . 555E+00 1 . 037E-0

1

4.698E-03 1 . 270 E-0

1

-0.141 0.158 0.153

0.3000 1 . 430E+00 1 . 690E-02 1 . 447E+00 1.371 E-0

1

5.697E-03 1 . 550E-0

1

-0.137 0.153 0.148

0.3500 1 . 355E+00 1 .873E-02 1 . 373E+00 1 . 727E-0

1

6.692E-03 1 .81 6E-01 -0 . 1 33 0.149 0.144

0.4000 1 . 300E+00 2 . 059E-02 1 . 320E+00 2.098E-01 7.632E-03 2 . 070E-0

1

-0.130 0.146 0.141 0.4500 1 . 25 9E + 00 2 . 250E-02 1 .282E+00 2.483E-01 8.670E-03 2.315E-01 -0.128 0.143 0.138

0.5000 1 .223E+00 2 . 447E-02 1 . 253E+00 2.873E-01 9.657E-03 2.552E-01 -0.125 0.140 0.135

0.5500 1 . 205E + 00 2.651 E-0 2 1 . 231 E+00 3 . 280E-0

1

1 . 065E-02 2.733E-01 -0.123 0.138 0.133

0.6000 1 . 136E+00 2.859E-02 1 . 21 5E + 00 3.689E-01 1 . 164E-02 3.007E-01 -0.121 0.136 0.130

0.7000 1 . 1 60E+00 3.293E-02 1 . 1 93E+00 4.521 E-0

1

1 .363E-02 3.433E-01 -0.117 0.132 0.126

0.8000 1 . 1 43E+00 3 . 745E-02 1.181 E+00 5.364E-01 1 . 563E-02 3.851 E-0

1

-0.113 0.129 0.123

0.9000 1 . 1 33E+00 4.217E-02 1 . 175E + 00 6.213E-01 1 . 765E-02 4 . 246E-0

1

-0.110 0.125 0.120

1 .0000 1 . 1 27E+00 4 . 707E-02 1 . 174E + 00 7.065E-01 1 . 968E-02 4 . 626E-0

1

-0.108 0.123 0.117

1 .2500 1 . 1 23E+00 6.017E-02 1 . 183E+00 9. 188E-01 2.484E-02 5.520E-01 -0.102 0.118 0.111

1 .5000 1 . 1 26E+00 7.432E-02 1 . 200 E + 0 0 1 . 1 29E+00 3.01 0E-02 6 . 346E-0

1

-0.097 0.113 0.105

1 .7500 1 . 1 33E+00 8.920E-02 1 . 222E+0 0 1 . 335E+00 3.543E-02 7. 1 1 6 E-0

1

-0.093 0.110 0.101 2.0000 1 .141 E+00 1 .046E-01 1 . 246 E + 0 0 1 . 538E+00 4.0S2E-02 7 . 836 E-0

1

-0.089 0.106 0.096

2.5000 1 . 1 59E+00 1 . 369E-01 1 . 296E+00 1 . 932E+00 5. 162E-02 9. 157E-01 -0.083 0.100 0.090

3.0000 1 . 1 76E+00 1 .709E-01 1 . 347E+00 2.31 OE+OO 6 . 240E-02 1 . 0 35E+00 -0.079 0.096 0.084

3.5000 1 . 1 92E+00 2.062E-01 1 . 399E+00 2 . 674E+00 7.309E-02 1 . 1 43E+00 -0.075 0.092 0.079

4.0000 1 . 207E+00 2.427E-01 1 . 450E+00 3 . 025E+00 3 . 364E-02 1 . 243E+00 -0.071 0.08S 0.075

4.5000 1 .221 E+00 2.801 E-0

1

1 .501 E+00 3 . 364E+00 9.402E-02 1 . 337E+00 -0 .068 0.085 0.071 5.0000 1 . 233E + 0 0 3.183E-01 1 . 55 1 E+00 3 . 6 92E + 00 1 . 042E-0

1

1 . 425E+00 -0.065 0.082 0 . 068 5.5000 1 . 244E+00 3.572E-01 1 . 602E+00 4.009E+00 1 . 142E-01 1 . 503E + 00 -0.062 0.080 0.065

6.0000 1 . 255E+00 3.968E-01 1 . 652E+00 4.31 6E+00 1 . 240 E-0

1

1 . 587E+00 -0.060 0.077 0.062

7.0000 1 .273E+00 4 . 78 0 E-0

1

1 . 751 E+00 4 . 904E+00 1 .430E-01 1 . 735E + 00 -0 .055 0.073 0.057

8.0000 1 . 28 9 £ + 00 5.614E-01 1 . 850E+00 5 . 460E+00 1 .61 IE-01 1 . 873E+00 -0.051 0.070 0.053

9.0000 1 . 303E+00 6.466E-01 1 . 949E+00 5 . 986E+00 1 . 735E-0

1

2. 001 E+00 -0.043 0.066 0.049

1 0.0000 1 . 31 5E+00 7.333E-01 2 . 048E+00 6 . 437E+00 1 . 952E-0

1

2 . 1 21 E+00 -0.045 0.064 0.046

12.5000 1 . 340E+00 9.549E-01 2 . 295E+00 7 . 639E+00 2.337E-01 2 . 392E+00 -0.038 0.058 0.039

15.0000 1 . 359E+00 1 . 134E+00 2 . 543E+00 3 . 674E+00 2.684E-01 2 . 630 E+00 -0.034 0.053 0.034

17.5000 1 . 376E+00 1 .41 9E+00 2 . 795E+00 9.611 E+00 2 . 996E-01 2.841 E+00 -0.031 0.050 0.030 20.0000 1 . 389E+00 1 . 653E+00 3 . 047E+00 1 . 047E+0

1

3.280E-01 3 . 030E+00 -0.028 0.047 0.027

25.0000 1 .41 1 E+00 2. 147E+00 3 . 553E+00 1 . 1 93E+0

1

3.774E-01 3 . 359E+00 -0.025 0.042 0.022

30.0000 1 . 429E+00 2 . 6 49E+0 0 4 . 073E+00 1 . 330E+01 4.191 E-0

1

3 . 638E+00 -0.022 0.039 0.019

35.0000 1 . 443E+00 3. 159E+00 4 . 603E+0Q 1 . 445E+0

1

4.547E-01 3 . 830 E+00 -0.020 0.037 0.016 40.0000 1 . 456E+00 3 . 674E+00 5. 129E+00 1 . 548E+0

1

4 . 856 E-0

1

4 . 0 94E+00 -0.019 0.035 0.014 45.0000 1 . 466E + 00 4 . 1 93E+00 5 . 659E+00 1 . 64 1 E+0

1

5 . 1 26 E-0

1

4 . 287E+00 -0.017 0.033 0.013

50.0000 1 . 476E+00 4.718E+00 6 . 1 94E+00 1 . 725E+0

1

5.365E-01 4 . 462E+00 -0.016 0.031 0.012

55.0000 1 . 484E+00 5 . 247E+00 6.731 E+00 1 . 802E+0

1

5.573E-01 4 . 622E+00 -0.015 0.030 0.011 60.0000 1 .491 E+00 5 . 779E+00 7.271 E+00 1 .874E+01 5 . 770 E-0

1

4 . 771 E+00 -0.014 0.029 0.010 70.0000 1 . 504E+00 6 . 849E+00 8 . 354E+00 2.002E+01 6.100E-01 5 . 033E+00 -0.012 0 .027 0.003

30 .0000 1 .515E+00 7 . 925E+0 0 9. 440E+00 2. 1 15E+01 6.375E-01 5 . 274E+00 -0.011 0.026 0.007

90.0000 1 . 525E+00 9.01 0E+00 1 . 053E+01 2.215E+01 6.603E-01 5 . 484E+00 -0.009 0.025 0.007

100.0000 1 . 533E+00 1 .010E+01 1 . 1 64E+01 2 . 305E+0

1

6 .809E-01 5 . 675E+00 -0.009 0 .024 0.006 125.0000 1 .551 E+00 1 . 234E+0

1

1 . 439E+01 2.498E+01 7.21 0E-01 6 . 084E+00 -0.007 0.022 0.005

150.0000 1 . 564E+00 1 . 553E+0

1

1 .715E+01 2 . 657E+0

1

7.510E-01 6 . 424E + 0 0 -0 .006 0.021 0.004

175.0000 1 . 576E+00 1 . S34E+01 1 . 9 92E + 0

1

2.792E+01 7.744E-01 6.71 3E+00 -0.005 0.020 0.003 200.0000 1 .586E+00 2. 1 10E+01 2.269E+01 2.910E+01 7. 933E-01 6 . 966E+00 -0.005 0.019 0 .003 250.0000 1 . 602E+00 2.661 E+O

1

2.821 E+01 3 . 1 07E+01 3.221 E-01 7 . 392E+00 -0.004 0.013 0.0C2

300 .0000 1 . 6 1 5E+00 3.21 1E+01 3.373E+01 3.269E+01 8.451 E-0

1

7.742E+00 -0.003 0.017 0.002

350.0000 1 . 626E+00 3 . 763E+0

1

3. 925E+01 3.406E+01 8.591 E-01 8 . 040E+00 -0.003 0.016 0.002 400.0000 1 . 6 36E+0 0 4.315E+01 4 . 479E+0

1

3 . 525E+0

1

8.71 9E-01 8 . 299E+O0 -0.002 0.016 0.001 450.0000 1 . 644E+00 4.869E+01 5 . 033E+01 3.631 E+0

1

3.823E-01 8 . 529E+00 -0.002 0.015 0.001 500.0000 1 .651 E+00 5 . 422E+0

1

5 . 583E+0

1

3 . 725E+01 8.909E-01 3 . 735E+00 -0.002 0.015 0.001 550.0000 1 . 653E+00 5 . 976E+0

1

6 . 1 42E+01 3.81 OE+O

1

3. 983E-01 8 . 922E+00 -0.002 0.015 0.001 600.0000 1 . 664E+00 5 .531 E+01 6.697E+01 3 . 883E+0

1

9.046E-01 9 . 0 93E + 00 -0.001 0.014 0.001 700.0000 1 . 674E+00 7.641 E+0

1

7 . 308E+0

1

4 . 026 E+0

1

9. 149E-01 9 . 3 97E+0 0 -0.001 0.014 0.001 300.0000 1 . 684E+00 8.751 E+01 8. 920E+01 4. 1 46 E + 0

1

9 .231 E-01 9.661 E+00 -0.001 0.014 0.001 900.0000 1 . 692E+00 9.363E+01 1 -003E+02 4 . 252E+0

1

9.296E-01 9 . S94E+00 -0.001 0.013 0.001 1000.0000 1 . 6 99E+0 0 1 . 0 98E+02 1.11 4E+02 4 . 346E+0

1

9.351 E-01 1 . 0 1 OE+O

I

-0.001 0.013 0.001

160
POSITRONS IN LEAD

I — 823.0 eV DENSITY - 1.1 35E+0 1 g/c7i 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. dClog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2/g MeV cn 2 /g MeV cn 2/g g/cm 2 0.0100 1 . 005E+0

1

2 . 273E-03 1 . 005E+01 6 . 245E-04 3.656E-05 4 .841 E-04 -0.318 0.432 0.368 0.0125 S . 640E + 00 2.747E-03 3 . 643E+00 3.937E-04 1 . 235E-04 6 . 1 47E-04 -0.298 0.395 0.341 0.0150 7 . 622E+00 3.172E-03 7 . 6 25E+00 1 . 202E-0 3 1 . 640E-04 7.491 E-04 -0.284 0 .36S 0.322 0.0175 6 . S47E+00 3.55SE-03 6.S50E+00 1 . 549E-03 2.073E-04 8.372E-04 -0.272 0.348 0.308 0.0200 6 . 235E+00 3.914E-03 6 . 239E+00 1 . 932E-03 2 . 530E-04 1 . 029E-03 -0.264 0.332 0.2S6 0.0250 5 . 323E + 0 0 4 . 564E-03 5 . 332E+00 2.302E-03 3.505E-04 1 . 324E-03 -0.250 0 . 3CS 0.279

0.0300 4 . 634E+00 5.146E-03 4 . 639E + 00 3 .S05E-03 4 . 547E-04 1 . 6 33E-0 3 -0.240 0.292 0.267 0.0350 4.202E+00 5.674E-03 4 . 20SE+00 4. 933E-03 5 . 643E-04 1 . 956E-03 -0.233 0.279 0.257

0 .0400 3 . S26E+00 S.161E-03 3 . 832E+0 0 6. 179E-03 5 . 785E-04 2.294E-03 -0.227 0.269 0.250 0.0450 3 . 525E+00 6 . 623E-03 3.531E+00 7.540E-03 7 . 966E-04 2.646E-03 -0.222 0.261 0.243 0.0500 3 . 277E + 0 0 7.071E-03 3 . 284E+00 9.010E-03 9. 184E-04 3.01 IE-03 -0.217 0.254 0.238

0.0550 3 . 070E+00 7.487E-03 3. 077E+00 1 . 05SE-02 1 . 043E-03 3 . 390E-03 -0.214 0.243 0.233

0 .0600 2 . 394E+00 7.877E-03 2. 902E+00 1 . 226E-02 1 . 1 71 E-03 3.783E-03 -0.210 0.243 0.229 0.0700 2.61 0E+00 8.620E-03 2.61 9E+00 1 .589E-02 1 .432E-03 4 . 6 08E-0 3 -0.205 0.235 0.223

0 .0300 2. 392E+00 9 . 335E-03 2.401 E+0 0 1 . 939E-02 1 . 702E-0 3 5.435E-03 -0.200 0.223 0.217

0.0900 2.213E+00 1 .002E-02 2 . 229E+00 2.421E-02 1 . 978E-03 6 . 41 3E-03 -0.197 0.223 0.212

0.1000 2 . 077E+00 1 . 067E-02 2 . 088E+00 2.385E-02 2.261 E-03 7 . 392E-03 -0.193 0.213 0.209

0. 1250 1 .81 SE+00 1 .217E-02 1 . 830E+00 4.169E-02 2. 9S4E-03 1 .005E-02 -0.187 0.209 0.201 0.1500 1 . 642E+00 1 . 357E-02 1 . 655E+00 5.609E-02 3 . 724E-03 1 .300E-02 -0.132 0.202 0.195

0.1750 1 . 51 4E+00 1 . 4 92E-0 2 1 . 529E+00 7.1S3E-02 4.474E-03 1 . 623E-02 -0.173 0.197 0.190

0.2000 1 .41 9E+00 1 . 624E-02 1 . 435E+00 3.873E-02 5.232E-03 1 .971E-02 -0.174 0.193 0.186 0.2500 1 . 2S5E+00 1 .833E-02 1 . 304E+00 1 . 254E-0

1

6 .762E-03 2 . 736E-02 -0.168 0.186 0.179

0.3000 1 . 1 98E+00 2.135E-02 1 . 220E+00 1 .651 E-01 8.297E-03 3.579E-02 -0.162 0.130 0.174

0.3500 1 . 1 3SE+00 2.388E-02 1 . 1 62E+00 2.072E-01 9.830E-03 4.484E-02 -0.158 0.175 0.169 0.4000 1 . 0 95E + 0 0 2 . 648E-02 1 . 1 21 E+OO 2.510E-01 1 .136E-02 5 . 437E-02 -0.154 0.171 0.165 0.4500 1 . 06 3E + 00 2. 910E-02 1 . 0 92E+00 2. 963E-01 1 . 289E-02 6 . 426E-02 -0.150 0.163 0.161

0 . 5000 1 . 039E+00 3.176E-02 1 .071E+00 3.425E-01 1 . 442E-02 7.442E-02 -0.146 0.164 0.158 0.5500 1 .021 E+OO 3 . 445E-02 1 . 055E+00 3.396E-01 1 . 594E-02 8 . 479E-02 -0.143 0.162 0.155

O.SOOO 1 . 007E+00 3.71 9E-02 1 . 044E+00 4.372E-01 1 . 7 46E-02 9 . 529E-0 2 -0.140 0.159 0.152

0.7000 9.S73E-01 4 . 283E-02 1 . 030E+00 5.337E-01 2 . 048E-02 1 .166E-01 -0.135 0.154 0.147 O.SOOO 9.759E-01 4 . 868E-02 1 . 025E+00 6.31 IE-01 2 . 349E-02 1 . 380E-0

1

-0.131 0.150 0.142

0.9000 9.694E-01 5 . 472E-02 1 . 024E+00 7 . 233E-0

1

2 . 643E-02 1 . 5 95E-0

1

-0.127 0.146 0.138

1 . 0000 9.662E-01 6 . 093E-02 1 . 027E+00 8 . 263E-0

1

2.947E-02 1 .309E-01 -0.124 0.143 0.134

1 .2500 9.664E-01 7.717E-02 1 . 044E+00 1 . 068E+00 3.691E-02 2 . 337E-0

1

-0.116 0.136 0.126

1 .5000 9.725E-01 9 . 447E-02 1 . 067E+00 1 . 305E+00 4 . 430E-02 2.854E-01 -0.110 0.130 0.119

1 .7500 9.810E-01 1 .127E-01 1 . 0 94E+00 1 .536E+00 5.166E-02 3 . 360E-0

1

-0.105 0.125 0.113 2.0000 9 . 905E-01 1 .31 8E-01 1 . 1 22E+00 1 . 7 6 2E+0 0 5 . 8 98E-02 3 . 855E-01 -0.100 0.121 0.103

2.5000 1 .010E+00 1 .7. IE-01 1 . 182E+00 2. 1 96E+00 7.351E-02 4.817E-01 -0.092 0.113 0.099

3.0000 1 . 027E+00 2.1 48E-01 1 . 242E+00 2.60 9E+00 3.782E-02 5.743E-01 -0.086 0.107 0.092

3.5000 1 . 044E+00 2.599E-01 1 . 303E+0 0 3 . 002E+00 1.01 9E-01 6.631 E-01 -0.080 0.102 0.085

4.0000 1 . 058E+00 3.071E-01 1 . 365E+00 3 . 377E+00 1 . 157E-01 7.479E-01 -0.076 0.098 0 . 080 4.5000 1 .071E+00 3.560E-01 1 . 427E+00 3 . 735E+00 1 . 292E-01 3.289E-01 -0.072 0.094 0.075

5.0000 1 . 083E+00 4.063E-01 1 . 489E+00 4. 07SE+00 1 .424E-01 9.061 E-0

1

-0.069 0.090 0.071 5.5000 1 . 0 94E + 00 4.575E-01 1 . 552E+00 4 . 407E+00 1 . 553E-0

1

9.798E-01 -0 .066 0.087 0.067 6.0000 1 . 1 04E+00 5.094E-01 1 . 6 1 3E+00 4 . 723E+00 1 . 678E-0

1

! . 050E+00 -0.064 0 . 084 0.064

7.0000 1 . 122E+00 6 . 157E-01 1 . 737E+0 0 5 . 320E+00 1 .917E-01 1 . 132E+00 -0.059 0.079 0.058 S.OOOO 1 . 1 37E+00 7.251 E-Q

1

1 . 86 2E+00 5 . 876E+0 0 2. 143E-01 1 . 304E+00 -0.056 0.075 0.053

9.0000 1 . 150E+00 8.371E-01 1 . 938E+00 6 . 395E+00 2.355E-01 1 . 41 7E+00 -0.053 0.072 0.049

1 0.0000 1 . 1 S2E+00 9.514E-01 2.11 4E+00 6 . 883E+00 2 . 556E-01 1 . 523E+00 -0.051 0.069 0.046 12.5000 1 . 137E+00 1 . 245E+00 2 . 433E+00 7 . 985E+00 3.009E-01 1 . 7 5 9E+0 0 -0.046 0.063 0.039 15.0000 1 . 207E+00 1 . 548E+00 2 . 755E+00 8 . 950E+00 3 . 404E-0

1

1 . 964E+00 -0.042 0.058 0.034

17.5000 1 . 223E+00 1 .858E+00 3.031 E+00 9.803E+00 3.750E-01 2 . 1 47E + 00 -0.039 0.055 0.030 20.0000 1 . 237E+00 2. 174E+00 3.41 1 E+0 0 1 . 053E+0

1

4.057E-01 2.31 OE+OO -0.037 0.052 0.027 25.0000 1 .260E+00 2 . 824E+00 4 . 084E+00 1 .1 92E+01 4 . 577E-0

1

2 . 5 96E+00 -0.033 0.047 0.023 30.0000 1 . 278E+00 3 . 490E+00 4.76 9E+0 0 1 . 305E+01 5.002E-01 2.341 E+00 -0.030 0.044 0.020 35.0000 1 . 293E+00 4 . 1 68E+00 5.461 E+00 1 . 403E+01 5 . 356 E-01 3 . 055E + 00 -0.028 0.041 0.C17 40.0000 1 . 306E+00 4 . S55E+00 6.161 E+00 1 -489E+01 5.657E-01 3 . 247E+00 -0.026 0.039 0.015

45.0000 1 .316E+00 5 . 55SE+00 6 . 87 3E+00 1 . 566 E+0

1

5.916E-01 3 . 420 E+0 0 -0.024 0.038 0.014 50.0000 1 . 326E+00 6 . 267E+00 7 . 5 92E+00 1 . 6 35E + 0

1

6. 141E-01 3 . 579E+00 -0.022 0.036 0.012 55.0000 1 . 334E+00 6 . 983E+00 8.31 7E+00 1 . 6 93E + 0

1

6 . 340E-0

1

3 . 725E+00 -0.021 0.035 0.011 60.0000 1 . 342E+00 7 . 702E+00 9. 044E+00 1 . 756E+01 6 .51 6E-01 3. 861 E+00 -0.019 0.034 0.011 70.0000 1 . 355E+00 9. 159E+00 1 . 0 5 1 E^O 1 1 . 853E+0

1

6.317E-01 4. 107E+00 -0.017 0 .032 0.009

80 .0000 1 . 366E+00 1 .064E+01 1 . 20 1 E+0

1

1 . 947E+01 7.063E-01 4 . 326E+00 -0.016 0.031 0.008 90.0000 1 . 375E+00 1 .214E+01 1 .351 E+0

1

2 . 025E+0

1

7.270E-01 4.521 E+00 -0.015 0.030 0.007 100.0000 1 . 3S4E+00 1 . 364E+0

1

1 .503E+01 2.096E+01 7.446E-01 4 . 699E+00 -0.013 0.029 0.006 125.0000 1.401 E+OO 1 . 743E+0

1

1 .383E+01 2 . 244E+0

1

7.792E-01 5 . 083E+00 -0.011 0.027 0.005

150.0000 1 . 41 5E+00 2.125E+01 2 . 267E+0

1

2 .-365E + 0

1

8.046E-01 5 . 404E+00 -0.010 0.026 0.004 175.0000 1 . 426E+00 2.51 1E+01 2 . 654E+0

1

2 . 467E+0

1

8 . 243E-0

1

5. 679E+00 -0.009 0.025 0.004 200.0000 1 . 436E+0Q 2.898E+01 5 . 042E+0

1

2 . 555E+0

1

8 . 400E-01 5.921 E+00 -0.003 0.024 0.003 250.0000 1 . 452E+00 3 . 674E+01 3 . 820 E+0

1

2.701 E+0

1

8.635E-0! 6 . 330E+00 -0.006 0.022 0.003 300.0000 1 . 4S4E+00 4 . 457E+01 4 . 6 0 3E+0

1

2 . 820 E+0

1

8.S05E-01 6 . 670E+00 -0.005 0.022 0.002 350.0000 1 . 475E+00 5 . 240E+0

1

5 . 338E+0

1

2 . 920 E+0

1

3.933E-01 6 . 960E+00 -0.005 0.021 0.002 400.0000 1 . 484E+00 5.021E+01 6.169E+01 3 . 007E+0

1

9.035E-01 7.21 3E+00 -0.004 0 .020 0.002 450.0000 1 .491 E+OO 6 . 803E+0

1

6 . 952E+01 3 . 083E+01 9.1 17E-01 7 . 438E+00 -0 .004 0.020 0.002 500.0000 1 . 4 98E+0 0 7 . 587E+0

1

7 . 737E+0

1

3.151E+01 9.1S5E-01 7 . 640E+00 -0.003 0.019 0.001 550.0000 1 . 504E+00 8.371 E+O

1

8 . 522E+0

1

3.21 3E+01 9.242E-01 7 . 824E+00 -0.003 0.019 0.001 600.0000 1 .51 0E+00 9. 155E+01 9. 306E+01 3.269E+01 9 .291 E-01 7 . 992E+00 -0.003 0.019 0.001 700.0000 1 .SEOE-'-OO 1 . 072S+02 1 . 087E+02 3 . 368E+0

1

9 . 371 E-01 3 . 2 90 E + 0 0 -0.002 0.013 0.001 800.0000 1 . 529E+00 1 . 227E+02 1 . 243E+02 3 . 454E+0

1

9 . 433E-0

1

8 . 550E+00 -0.002 0.018 0.001 900.0000 1 .536E+00 1 . 383E+02 1 . 398E+02 3 . 530E+0

1

9.433E-01 8 . 780E+00 -0.002 0.017 0.001 1000.0000 1 .543E+00 1 . 539E+02 1 . 554E+02 3 . 598E+01 9 . 524E-0

1

8 . 986E+00 -0.002 0.017 0.001

161
POSITRONS IN A-150 TISSUE-EQUIVALENT PLASTIC

I = 65.1 eV DENSITY =1.1 27E+0Ci g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(log )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV ReV cin 2 /g MeV cin 2 /g ReV cra 2 /g g/ct> 2 O.OIOO 2.51 SE+01 2.002E-03 2.51 9E+01 2.212E-04 3.S41E-05 0.0 -0.176 0.197 0.193

0.0125 2. 105E+01 2. 1 12E-03 2. 106E+01 3 . 302E-04 4.871E-05 0.0 -0.170 0.189 0.136 0.0150 1 .81SE+01 2.201E-03 1 .31 9E+01 4 . 584E-04 5. 904E-05 0.0 -0.165 0.183 0.130

0.0175 1 . 607E+0

1

2 . 277E-03 1 . 607E+0

1

6 . 050E-04 6 . 937E-05 0.0 -0.161 0.173 0.175

0.0200 1 . 444E+0

1

2.344E-03 1 . 444E+0

1

7.693E-04 7 . 970E-05 0.0 -0.153 0.174 0.172

0.0250 1 .209E+01 2 . 459E-03 1 .209E+01 1 . 150E-C3 1 . 00 3E-04 0.0 -0.153 0.163 0.166 0.0300 1 . 0 47E + 0

1

2.5’ 9E-0 3 1 . 0 47E + 0

1

1 .595E-03 1 . 20 9E-04 0.0 -0.149 0.163 0.161 0.0350 9 . 277E+00 2.623E-03 9. 280E+00 2. 1 04E-03 1 .412E-04 0.0 -0.147 0.160 0.158

0.0400 3 . 366E+00 2. 6S6E-03 S . 369E+00 2.672E-03 1 .613E-04 0.0 -0.144 0.156 0.155

0.0450 7 . 645E + 00 2 . 742E-03 7 . 648E+00 3.293E-03 1 .SI 1 E-04 0.0 -0.142 0.154 0.152

0.0500 7 . 059E+00 2.792E-03 7 . 062E+00 3.979E-03 2 . 007E-04 0.0 -0.140 0.152 0.150 0.0550 6 . 574E+00 2.S38E-03 6 . 576 E+00 4.713E-03 2 . 200E-04 0 . 0 -0.139 0.150 0.148

0.0500 6 . 1 64E+00 2 .331 E-03 6. 167E+00 5 . 499E-03 2 . 392E-04 0.0 -0.137 0.148 0.147

0.0700 5.51 2E+00 2. 959E-03 5.515E+00 7.21 7E-03 2 . 767E-04 0.0 -0.135 0.145 0.144

0.0300 5.01 5E+00 3 . 030E-03 5.018E+00 9. 122E-03 3.134E-04 0.0 -0.133 0.143 0.142

0.0900 4 . 623E+00 3.095E-03 4 . 626E+00 1 . 120E-02 3.493E-04 0.0 -0.132 0.141 0.140

0.1000 4 . 307E+00 3.1 58E-03 4.31 OE+OO 1 . 344E-02 3 . 345E-04 0.0 -0.130 0.139 0.133

0.1250 3.731E+00 3.313E-03 3 . 735E+00 1 . 970E-02 4.697E-04 0.0 -0.128 0.136 0.135 0.1500 3 . 343E+00 3.463E-03 3 . 347E+00 2.679E-02 5.51 7E-04 0.0 -0.125 0.133 0.132

0.1750 3 . 065E+00 3.61 IE-03 3 . 068E+00 3.461E-02 6.309E-04 0.0 -0.124 0.131 0.130

0.2000 2 . 856E+00 3.760E-03 2 . S60E + 0 0 4 . 306E-02 7.078E-04 0.0 -0.122 0.130 0.129

0.2500 2.566E+00 4.071 E-03 2 . 570E+00 6.157E-02 8 . 562E-04 0.0 -0.120 0.127 0.126

0.3000 2.377E+00 4.402E-03 2.381 E+00 8. 182E-02 9. 996E-04 0.0 -0.113 0.125 0.124

0.3500 2 . 245E+00 4.747E-03 2 . 250E+00 1 . 035E-0

1

1 . 140E-03 0.0 -0.107 0.123 0.122

0.4000 2.146E+00 5.1 12E-03 2.151 E+00 1 . 2S2E-0

1

1 . 278E-0 3 2. 969E-02 -0.089 0.118 0.116 0.4500 2.071E+00 5 . 497E-03 2 . 077E+00 1 . 499E-0

1

1 . 41 5E-03 6 .264E-02 -0.083 0.113 0.110

0.5000 2.01 3E+00 5.897E-03 2.01 9E+00 1 . 743E-0

1

1 . 552E-03 9.751 E-02 -0.077 0.108 0.104

0.5500 1 . 968E+00 6.311 E-03 1 . 974E+00 1 . 994E-0

1

1 .689E-03 1 . 337E-0

1

-0.073 0.104 0.099

0.6000 1 .931E+00 6 . 737E-03 1 . 938E+00 2.249E-01 1 . 826E-0 3 1 . 708E-0

1

-0.069 0.100 0.095

0.7000 1 . 377E+00 7 . 626E-03 1 . 884E+00 2.773E-01 2. 102E-03 2.464E-01 -0.062 0.093 0.037

0.8000 1 . 340E+00 8.559E-03 1 .843E+00 3.309E-01 2 . 382E-03 3.223E-01 -0.057 0.088 0.081 0.9000 1 .31 4E+00 9.536E-05 1 . 824E+0O 3.854E-01 2 . S65E-03 3. 975E-01 -0.053 0.083 0.076

1 .0000 1 . 796E+00 1 . 055E-02 1 .306E+00 4.405E-01 2. 952E-03 4.712E-01 -0.050 0.079 0.071

1 .2500 1 .770E+00 1 . 324E-02 1 . 783E+00 5.300E-01 3 . 687E-03 6 . 472E-01 -0.044 0.071 0 . 062

1 .5000 1 . 75 9E + 0 0 1 . 6 1 2E-02 1 . 775E+00 7.206E-01 4 . 447E-0 3 8. 100E-01 -0 . 040 0.066 0.056

1 .7500 1 . 756E+00 1 . 916E-02 1 . 775E+00 8.614E-01 5 . 230E-03 9.601 E-01 -0.037 0.061 0.051 2.0000 1 . 75SE+00 2 . 233E-02 1 . 780E+00 1 . 002E+00 6 .035E-03 1 . 0 39E + 00 -0.035 0.053 0.047

2.5000 1 . 766E+00 2.900E-02 1 . 7 95E+00 1 . 282E+0 0 7.696E-03 1 . 346E+00 -0.032 0.052 0.042

3.0000 1 .777E+00 3.605E-02 1 .31 3E+00 1 . 559E+00 9.415E-03 1 .551E+00 -0.030 0.043 0.038

3.5000 1 . 789E+00 4 . 339E-02 1 . 333E+00 1 . 333E+00 1 . 1 1SE-02 1 .751 E+00 -0.029 0.045 0.036

4.0000 1 .301 E+00 5.095E-02 1 . 852E+00 2. 105E+00 1 . 293E-02 1 . 922E+00 -0.027 0.043 0.034

4.5000 1 .312E+00 5 . 874E-02 1 .371 E+00 2 . 373E+00 1 .431 E-02 2 . 077E+00 -0.026 0.041 0.032

5.0000 1 . 323E+00 6 . 672E-02 1 . 88 9E + 00 2 . 639E+00 1 . 667E-02 2.218E+00 -0.025 0.039 0 .030 5.5000 1 . 832E+00 7.483E-02 1 . 907E+00 2. 903E+00 1 . 854E-02 2. 349E+00 -0.024 0.038 0.029

6.0000 1 .S42E+00 3.31 9E-02 1 . 925E+00 3 . 1 64E+00 2. 043E-02 2 . 47 0 E + 0 0 -0.023 0.037 0.023 7.0000 1 . 353E+00 1 .002E-01 1 . 953E+00 3 . 679E+00 2 . 425E-02 2.691E+C0 -0.022 0.035 0.026 8.0000 1 . 873E+00 1 . 1 77E-0

1

1 . 990E+00 4. 185E+00 2.81 2E-02 2.8S7E+00 -0.020 0.033 0.025

9.0000 1 .336E+00 1 . 355E-0

1

2.021 E+00 4 . 684E+00 3 . 200E-02 3 . 064E+00 -0.019 0.031 0.023

10.0000 1 . S97E+00 1 . 533E-01 2.051 E+00 5. 175E+00 3 . 590E-02 3 . 227E+00 -0.017 0.030 0.022

12.5000 1 . 921 E+00 2.005E-01 2.1 22E+00 6 . 373E+00 4.567E-02 3 . 532E+00 -0.014 0.027 0.019

15.0000 1 . 941 E+00 2.486E-01 2. 189E+00 7 . 533E+00 5.540E-02 3 . 885E+00 -0.012 0.025 0.017

17.5000 1 . 956E+00 2. 977E-01 2 . 254E+00 8 . 658E+00 6 . 504E-02 4.150E+00 -0.010 0.023 0.015

20.0000 1 . 970E+00 3.477E-01 2.31 7E+00 9 . 752E+00 7 . 455E-02 4 . 335E+00 -0 .008 0.021 0.013 25.0000 1 . 991 E+00 4.495E-01 2.441 E+00 1 . 185E+01 9.310 E-02 4 . 78SE+00 -0.006 0.013 0.010 30.0000 2 . 003E+00 5.531E-01 2 . 562E+Q0 1 . 335E+01 1 . 1 1 0E-01 5.1 26E+00 -0.004 0.016 0.009

35.0000 2 . 023E+00 6.581E-01 2.631 E+00 1 . 576E+0

1

1 .281 E-01 5.417E+00 -0.003 0.015 0.007 40.0000 2 . 0 35E+00 7.643E-01 2 . 799E+00 1 .759E+01 1 . 445E-0

1

5.671 E+OO -0.003 0.013 0.006 45.0000 2 . 045E+00 8.71 4E-01 2.91 7E+00 1 . 934E+01 1 . 602E-01 5.897E+00 -0.002 0.012 0 . 005 50.0000 2 . 055E+00 9.792E-01 3 . 0 34E+00 2.1 02E+0

1

1 . 753E-0

1

6.101 E+00 -0.002 0.011 0.005 55.0000 2. 063E+00 1 . 088E+00 3 . 1 5 1 E+00 2.263E+01 1 . 897E-0

1

6 . 236E+00 -0.002 0.011 0.004 60.0000 2.071 E+00 1 . 1 97E+00 3 . 26 7E+0 0 2.419E+01 2.036E-01 6 . 456 E + 00 -0.001 0.010 0.004 70.0000 2 . 034E+00 1 . 41 6E+00 3 . 500E+00 2.715E+01 2 . 296E-0

1

6 . 753E+00 -0.001 0.009 0.003

30 .0000 2 . 096E+00 1 . 638E+00 3 . 7 33E + 00 2.991E+01 2 . 537E-0

1

7 . 020E+00 -0.001 0.008 0.002

90.0000 2. 106E+00 1 .360E+00 3 . 966E+00 3.251E+01 2.759E-01 7 . 253E+00 -0.001 0.008 0.002

100.0000 2.11 5E+00 2 . 034E+00 4.1 99E+00 3.496E+01 2.966E-01 7.461 E+00 -0.001 0.007 0.002

125.0000 2 . 1 34E+00 2 . 647E+00 4.731 E+00 4 . 054E+0

1

3.425E-01 7. 903E+00 -0.000 0.005 0.001

1 50.0000 2 . 1 49E+00 3.214E+00 5 . 3S3E+00 4.547E+01 3.817E-01 8 . 265E+00 -0 .000 0.006 0.001 175.0000 2 . 1 6 2E+00 3 . 734E+00 5 . 947E+00 4. 990E+01 4. 155E-01 8.571 E+00 -0.000 0.005 0.001 200.0000 2 . 1 74E+00 4 . 357E+00 6 . 531 E+00 5.391E+01 4.451 E-0

1

8 . 837E+00 -0.000 0.005 0.001 250.0000 2.1 93E+00 5 . 508E+00 7.701 E+00 6.095E+01 4.946E-01 9.231 E+00 -0.000 0 .004 0.001 300.0000 2 . 203E+00 6 . 665E+00 8 . 873E+00 6.700E+01 5.345E-01 9 . 6 45E + 00 -0.000 0.004 0.000 350.0000 2.221 E+00 7 . 826E+0 0 1 . 005E+0

1

7 . 229E+0

1

5.675E-01 9 . 952E+00 -0.000 0.004 0.000 400.0000 2 . 232E+00 8. 990E+00 1 . 1 22E+0

1

7.699E+01 5 . 953E-0

1

1 . 022E+01 -0.000 0.003 0.000 450.0000 2 . 242E+00 1 .016E+01 1 .240E+01 3 . 1 23E+01 6.192E-01 1 . 045E+0

1

-0.000 0 .003 0.000 500.0000 2.251 E+00 1 . 1 32E+0

1

1 . 358E+0

1

S.508E+01 6 .400E-01 1 .066E+01 -0.000 0.003 0.000 550.0000 2 . 259E+00 1 .2' 9E+01 1 . 475E+0

1

3 . 862E+0

1

6 . 5S2E-01 1 . 085E+0

1

-0.000 0.003 0 . 000 600.0000 2 . 267E+00 1 . 367E+01 1 . 5 9 3E + 0

1

9. 183E+C1 6.744E-01 1 . 103E+0! -0.000 0.003 0.000 700.0000 2 . 280E+00 1 .601E+01 1 . 829E+0

1

9 . 773E+0

1

7.01 9E-01 I . 134E+01 -0.000 0.003 0.000 800.0000 2.291 E+00 1 .336E+01 2.065E+01 1 . 029E+02 7.245E-01 1 . 1 60E+0

1

-0.000 0.003 0.000 900.0000 2.301 E+00 2 . 072E+0

1

2 . 302E+0

1

1 . 075E+02 7 . 434E-0

1

1 . 1S4E+01 -0.000 0.002 0.000 1000.0000 2.31 OE+OO 2 . 307E+0

1

2.535E+01 1.11 6E+02 7.595E-01 1 . 205E+01 -0.000 0.002 0 .000

162
POSITRONS IN AIR, DRY (NEAR SEA LEVEL)

I = 35.7 eV DENSITY = 1.205E-03 g/cra 3 (20° C)

ENERGY STOPPING POUER CSDA RADIATION DENS.EFF. d ( log )/d ( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2 /g MeV cm 2/g g/cm 2 0.0100 2. 180E+01 2.210E-03 2. 180E+01 2.571 E-04 4.831E-05 0.0 -0.135 0.203 0.204 0.0125 1 . 825E+0

1

2.346E-03 1 . 325E + 0

1

3 . 830E-04 6.164E-05 0.0 -0.173 0.199 0.196 0.0150 1 . 578E+0

1

2.459E-03 1 .579E + 01 5.308E-04 7 . 506E-05 0.0 -0.173 0.193 0.189 0.0175 1 .396E+01 2.553E-03 1 . 396E+0

1

6.995E-04 8 . 852E-05 0.0 -0.169 0.137 0.184

0.0200 1 .256E+01 2.635E-03 1 .256E+01 8.836E-04 1 . 020E-04 0.0 -0.165 0.183 0.130 0.0250 1 . 0 53E+0

1

2.772E-03 1 . 053E+01 1 . 325E-03 1 . 289E-04 0.0 -0.160 0.176 0.173 0.0300 9 . 1 26E+00 2 . 888E-03 9. 129E+00 1 . 837E-03 1 . 557E-04 0.0 -0.156 0.171 0.169 0.0350 8 . 096E+00 2 . 988E-03 8 . 0 99E+00 2.420E-03 1 . 824E-04 0.0 -0.153 0.167 0.165

0.0400 7 . 306E+00 3 . 074E-03 7.309E+00 3.071 E-03 2 . 0 90E-04 0.0 -0.150 0.164 0.162

0.0450 6 . 680E+00 3. 147E-03 6 . 683E+00 3 . 7S7E-03 2 . 353E-04 0.0 -0.148 0.161 0.159 0.0500 6.171E+00 3 .21 2E-03 6 . 1 75E+00 4.566E-03 2.61 3E-04 0.0 -0.146 0.158 0.157 0.0550 5 . 749E+00 3.271 E-03 5 . 752E+00 5 . 406E-03 2.871 E-04 0.0 -0.144 0.155 0.155

0.0600 5 . 393E+00 3 . 326E-03 5 . 397E+00 6 . 304E-03 3.125E-04 0.0 -0.143 0.155 0.153

0.0700 4.S26E+00 3.425E-03 4.829E+00 8.267E-03 3 . 626E-04 0.0 -0.140 0.151 0.150 0.0800 4 . 393E+0 0 3.51 6E-03 4 . 396E+00 1 . 044E-02 4 . 1 1 6E-04 0.0 -0.133 0.149 0.147 0.0900 4 . 052E+00 3.600E-03 4 . 055E+00 1 . 281 E-02 4.597E-04 0 .

0

-0.137 0.147 0.145

0.1000 3 . 776E+00 3 . 630E-03 3 . 780E+00 1 . 537E-02 5 . 068E-04 0.0 -0.135 0.145 0.144

0.1250 3 . 274E+00 3.368E-03 3 . 278E+00 2 . 250E-02 6.21 0E-04 0.0 -0.132 0.141 0.140 0.1500 2 . 935E+00 4 . 047E-03 2.939E+00 3 . 058E-02 7 . 307E-04 0.0 -0.130 0.139 0.137

0.1750 2 . 6 92E+00 4 . 225E-03 2.696 E+00 3. 948E-02 8 . 366E-04 0.0 -0.128 0.136 0.135

0.2000 2.51 0E+00 4 . 405E-03 2.51 4E+00 4. 909E-02 9 . 396E-04 0.0 -0.126 0.134 0.133

0.2500 2 . 257L+00 4.772E-03 2.261 E+00 7.01 4E-02 1 .138E-03 0.0 -0.124 0.132 0.130

0.3000 2.091 E + 00 5.156E-03 2 . 096E+00 9.31 5E-02 1 . 329E-03 0.0 -0.122 0.129 0.123

0.3500 1 . 976E+00 5.5S4E-03 1 . 932E+00 1 . 177E-01 1 .51 6E-03 0.0 -0.120 0.127 0.126

0 . 4000 1 . 8 93E+00 5.993E-03 1 . 899E+00 1 . 435E-0

1

1 .699E-03 0.0 -0.113 0.126 0.125 0.4500 1 .331 E+00 6 . 4 42E-0 3 1 . 838E+00 1 -703E-01 1 .830E-03 0.0 -0.117 0.124 0.123

0.5000 1 . 784E+00 6 . 908E-03 1 .791 E+00 1 . 979E-01 2. 060E-03 0.0 -0.116 0.123 0.122

0.5500 1 . 748E+00 7.395E-03 1 . 755E+00 2.261E-01 2 . 240E-03 0.0 -0.114 0.122 0.121 0.6000 1 .71 9E+00 7.397E-03 1 . 727E+00 2.548E-01 2.41 9E-03 0.0 -0.113 0.121 0.119 0.7000 1 . 673E+00 8 . 947E-03 1 . 637E+00 3.1 35E-01 2.779E-03 0.0 -0.111 0.119 0.117

0.8000 1 . 652E+00 1 . 005E-02 1 . 662E+00 3.732E-01 3 . 1 41 E-03 0.0 -0.109 0.113 0.116 0.9000 1 . 636E+00 1.11 9E-02 1 . 647E+00 4.337E-01 3 . 505E-03 0.0 -0.108 0.116 0.114

1 .0000 1 . 626E+00 1 . 239E-02 1 . 638E+00 4.946E-01 3 . 872E-03 0.0 -0.107 0.115 0.113

1.2500 1 . 6 1 7E+00 1 . 5

!'5E-0 2 1 . 633E+00 6 . 475E-0

1

4.805E-03 0.0 -0.104 0.113 0.110

1 .5000 1 .621 E+00 1 . 393E-02 1 . 640E+00 8 . 0 0 4 E - 0

1

5 . 758E-0 3 0.0 -0.101 0.110 0.107

1 .7500 1 . 530E+00 2.249E-02 1 . 653E+00 9.523E-01 5 . 732E-03 0.0 -0.099 0.109 0.105

2.0000 1 . 642E+00 2.621 E-02 1 . 663E+00 1 . 1 03E+00 7.723E-03 0.0 -0.097 0.107 0.103

2.5000 1 . 5 63E + 00 3 . 405E-02 1 .703E+00 1 . 400E + 00 9.748E-03 0 .

0

-0.095 0.104 0.100 3.0000 1 . 6 95E+00 4 . 230E-02 1 . 737E+00 1 . 6 90E+00 1 . 132E-02 0.0 -0.092 0.102 0.097

3.5000 1 . 720E+00 5.0S9E-02 1 . 771 E+00 1 . 975E+00 1 . 392E-02 0.0 -0.091 0.100 0.095

4.0000 1 . 744E+00 5 . 977E-02 1 . 804E+00 2 . 255E+00 1 . 605E-02 0.0 -0.089 0.099 0.093

4.5000 1 . 766E+00 6 .391 E-02 1 . 835E+00 2 . 530E + 00 1 .81 9E-02 0.0 -0 . 083 0.097 0.091 5.0000 1 .736E+00 7 . 825E-02 1 . 36 4E + 00 2 . 800E+00 2.035E-02 0.0 -0.087 0.096 0.090 5.5000 1 . 305E+0 0 8 . 775E-02 1 . 3 93E+00 3 . 066E+00 2.251 E-02 0.0 -0.086 0.095 0.089

6.0000 1 .323E+00 9.743E-02 1 . 920E+00 3 . 329E+00 2 . 463E-02 0.0 -0.085 0.094 0.037

7.0000 1 . S54E+00 1 . 172E-01 1 . 972E+00 3 . S42E+00 2. 903E-02 0.0 -0.083 0.092 0.085 8.0000 1 . 333E+00 1 . 375E-0

1

2 . 020E+00 4 .343E+00 3.337E-02 0.0 -0.082 0.090 0.033

9.0000 1 . 903E+00 1 . 583E-0

1

2 . 066E+00 4 . 833E+00 3.770E-02 0.0 -0.081 0.089 0.082

10.0000 1 . 931 E+00 1 . 794E-0

1

2.11 0E+00 5.31 2E+00 4 . 202E-02 0.0 -0.080 0.037 0.080

12.5000 1 . 980E+00 2 . 336E-01 2.21 3E+00 6 . 468E+00 5.268E-02 0.0 -0.078 0.034 0.077

15.0000 2 . 020E+00 2.894E-01 2. 31 0E+00 7 . 573E+00 6.315E-02 0.0 -0.076 0.082 0.074

17.5000 2 . 055E+00 3.463E-01 2.401 E+00 3 . 635E+00 7 . 339E-02 0.0 -0.075 0.080 0.072 20.0000 2 . 085E+00 4 . 042E-01 2.489E+00 9 . 657E+00 8.339E-02 0.0 -0.074 0.073 0.070 25.0000 2 . 1 36 E + 0 0 5.21 9E-01 2 . 657E+00 1 . 1 60E+0

1

1 .025E-01 0.0 -0.072 0.075 0.066 30.0000 2.17 6E+00 6.41 7E-0

1

2.31 SE+00 1 . 343E+0

1

1 .209E-01 7 . 636E-03 -0.064 0.072 0.063 35.0000 2 . 208E+00 7.630E-01 2.971 E+00 1 .515E+01 1 . 3S3E-0

1

5 . 984E-02 -0.053 0.069 0.053 40.0000 2 . 232E+00 8.855E-01 3.1 13E+00 1 . 630E+01 1 . 543E-0

1

1 . 373E-0

1

-0.045 0.066 0.053 45.0000 2 . 252E+00 1 . 00 9E + 00 3.261 E+00 1 . 336E+0

1

1 . 706E-0

1

2.266E-01 -0.040 0.063 0 .049 50.0000 2.26 9E + 00 1 . 1 33E+00 3 . 403E+00 1 . 987E+01 1 . S57E-0

1

3.1 92E-01 -0.036 0.060 0.045 55.0000 2 . 2S4E+00 1 . 253E+00 3 . 542E+00 2.131 E+01 2.001 E-0

1

4. 120E-01 -0 .033 0.057 0.041 60.0000 2 . 297E+00 1 . 334E+00 3.681 E+00 2.259E+01 2. 1 39E-01 5.029E-01 -0.051 0.055 0.038 70.0000 2.31 9E+00 1 . 6 37E+00 3. 956E+00 2.531 E+01 2.398E-01 6 . 762E-01 -0.027 0.051 0.033 80.0000 2 . 337E+00 1 .392E+00 4 . 229E+00 2.775E+01 2.637E-01 8.365E-01 -0.025 0.043 0.030

90.0000 2 . 353E+00 2.1 48E+00 4.501 E+00 3 . 005E+0

1

2.353E-01 9 . 842E-0

1

-0.023 0.045 0.027 100.0000 2 . 367E+00 2 . 405E+00 4 . 772E+00 3 . 220E+0

1

3 . 063E-0

1

1 . 1 20E+00 -0.022 0.043 0.024

125.0000 2 . 3 95E+00 3 . 053E+00 5 . 448E+00 3.71 0E+01 3.517E-01 1 .41 9E+00 -0.020 0.039 0.020 150.0000 2.41 3E+00 3.705E+00 6 . 1 22E+00 4.143E+01 3. 904E-01 1 . 670E+00 -0.019 0.036 0.017 175.0000 2 . 436E+00 4 . 360E+00 6 . 7 96 E+0 0 4.530E+01 4.237E-01 1 . 887E+00 -0.013 0.033 0.015 200.0000 2 . 452E+00 5.01 8E+00 7 . 47 0 E+00 4.331 E+9

1

4 . 529E-0

1

2 . 073E+0 0 -0.017 0.031 0.013 250.0000 2.479E+00 6 . 340E+00 8.81 3E+00 5 . 49SE+0

1

5.016 E-0

1

2 . 403E+00 -0.016 0.028 0.011 300.0000 2 . 500E+00 7 . 667E+00 1 .017E+01 6 . 024E+0

1

5.409E-01 2 . 675E+00 -0.015 0.026 0.009 350.0000 2.517E+00 S. 998E+00 1 . 1 52E+0

1

6 . 486E+01 5.734E-01 2. 909E+00 -0.014 0.025 0.003 400.0000 2 . 532E+00 1 . 033E+01 1 . 286E+0

1

6 . 8 96E+0

1

6 . 008E-0

1

3.1 1 6E+00 -0.013 0.023 0 .007 450.0000 2 . 545E+00 1 . 1 67E+01 1 . 422E+0

1

7.266E+01 6 . 24 3 E-0

1

3 . 302E+00 -0.012 0.022 0 . 007 500.0000 2 . 556E+00 1 .301 E+01 1 . 557E+0

1

7.602E+01 6 .447E-01 3 . 472E+00 -0.011 0.021 0.006 550.0000 2 .566E+00 1 . 435E+01 1 . 692E+01 7.910 E+0

1

6 . 627E-0

1

3 . 623E+00 -0.011 0.021 0.006 500.0000 2 . 575E+00 1 .569E+01 1 . 827E+0

1

3.1 94E+01 5 .78 6 E-0

1

3 . 772E+00 -0.010 0.020 0.005 700.0000 2. 590E+00 1 . 338E+0

1

2.097E+01 8.705E+01 7.057E-01 4 . 0 34E+0 0 -0.003 0.019 0.005 300.0000 2 . 603E+00 2. 107E+01 2.367E+01 9. 153E+01 7.279E-01 4 . 267E+00 -0.007 0.018 0.004 900.0000 2.61 4E+00 2 . 376E+0

1

2 . 638E+0

1

9 . 553E+0

1

7.466E-01 4 . 477E+00 -0.006 0.017 0.004 1000.0000 2 . 624E+0 0 2 . 646E+0

1

2 . 908E+0

1

9. 91 4E+01 7.624E-01 4 . 668E+00 -0.005 0.017 0.003

163
POSITRONS IN LITHIUM FLUORIDE

I = 94.0 eV DENSITY = 2.635E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d ( log )/d( logl ) COLLISION RADIATIVE TOTAL RANGE YIELD COP.R

.

COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

KeV MeV cm 2 /g MeV cn 2 /g MeV cji 2 /g g/cm 2

0.0100 1 . 985E+01 1 . 993E-03 1 . 985E+0

1

2 . 829E-04 4.775E-05 0.0 -0.188 0.212 0.208

0.0125 1 . 563E+01 2.121E-03 1 .664E+01 4.21 IE-04 S.099E-05 0.0 -0.181 0.203 0.199

0.0150 1 . 439E+0

1

2.225E-03 1 . 439E+01 5.832E-04 7.433E-05 0.0 -0.176 0.196 0.193 0.0175 1 . 27 4E+0

1

2.313E-03 1 . 274E+0

1

7 . 682E-04 3 . 773E-05 0.0 -0.171 0.191 0.137

0.0200 1 . 1 46E+01 2 . 390E-03 1 . 1 46E+01 9.754E-04 1.01 IE-04 0.0 -0.168 0.186 0.133

0.0250 9.61 2E+00 2.51 9E-03 9.61 4E+00 1 . 454E-0 3 1 . 230E-04 0 .

0

-0.162 0.179 0.176 0.0300 S.335E+00 2.624E-03 8 . 33SE+00 2.014E-03 1 . 547E-04 0.0 -0.153 0.174 0.171 0.0350 7.397E+00 2.715E-03 7 . 399E+00 2.652E-03 1 .81 3E-04 0.0 -0.155 0.170 0.167

0.0400 6 . S77E + 00 2.794E-03 6 . 679E+00 3 . 365E-03 2 . 077E-04 0.0 -0.152 0.166 0.164

0.0450 6 . 1 06E + 00 2 . 867E-0 3 6 . 1 09E+00 4 . 1 43E-03 2.340E-04 0.0 -0 .150 0.163 0.161 0.0500 5 . 642E+00 2 . 935E-03 5 . 645E+00 5.001E-03 2.600E-04 0.0 -0 . 1 48 0.161 0.159

0.0550 5 . 257E+00 2 . 997E-0 3 5 . 250E+00 5.919E-03 2 . S59E-04 0.0 -0.146 0.159 0.157

0.0600 4 . 932E+00 3 . 055E-03 4 . 935E+00 6 . 901 E-03 3.117E-04 0.0 -0.145 0.157 0.155

0.0700 4.41 4E+00 3.1 5SE-03 4 . 4 1 7 E+0 0 9.048E-03 3.624E-04 0.0 -0.142 0.154 0.152

0.0300 4.019E+00 3.244E-03 4 . 022E+00 1 . 142E-02 4. 122E-04 0.0 -0.140 0.151 0.149

0.0900 3 . 707E+00 3.325E-03 3.711 E+00 1 .402E-02 4.61 0E-04 0.0 -0.138 0.149 0.147 0.1000 3.456E+00 3.402E-03 3 . 459E+00 1 .631E-02 5 . 089E-04 0.0 -0.137 0.147 0.145

0.1250 2. 997E+00 3 . 537E-03 3 . OOOE+OO 2.460E-02 6 . 252E-04 0.0 -0.134 0.143 0.142

0.1500 2 . 687E+00 3.763E-03 2.691 E+00 3.343E-02 7.373E-04 0 .

0

-0.131 0.140 0.139

0.1750 2 . 465E+00 3 . 934E-03 2 . 469E+00 4.314E-02 8.457E-04 0.0 -0.130 0.133 0.137

0.2000 2.299E+00 4.104E-03 2 . 303E+00 5 . 364E-02 9.510E-04 0.0 -0.123 0.136 0.135

0.2500 2 . 0 66E + 90 4 . 455E-03 2. 071 E+00 7.662E-02 1 . 1 54E-03 6 .058E-03 -0.117 0.132 0.131 0.3000 1 . 91 3E+00 4.326E-03 1 . 91 8E+00 1 .018E-01 1 . 351 E-03 2 . 1 36E-02 -0.111 0.128 0.126

0.3500 1 .807E+00 5.212E-03 1 .31 2E+00 1 .286E-01 1 . 543E-0 3 3.978E-02 -0.106 0.124 0.122

0.4000 1 . 729E+00 5.61 6E-03 1 . 734E+00 1 . 5S8E-0

1

1 . 732E-0 3 6.095E-02 -0.101 0.120 0.117

0.4500 1 . 670E+00 6 . 033E-03 1 . 676 E+00 1 .862E-01 1 . 920E-03 8.445E-02 -0.096 0.116 0.114

0.5000 1 . 625E+00 6 .469E-03 1 . 632E+00 2.164E-01 2. 106E-03 1 . 0 98E-0

1

-0.091 0.113 0.110

0.5500 1 . 590E+00 6 . 922E-03 1 . 597 E+00 2.474E-01 2.292E-03 1 . 367E-01 -0.087 0.110 0.106 0.6000 1 .561E+00 7.391E-03 1 .56 9E+00 2.790E-01 2 . 473E-03 1 .648E-01 -0.083 0.107 0.103

0.7000 1 . 520E+00 8.365E-03 1 . 528E+00 3.437E-01 2.851E-03 2 . 236E-0

1

-0.077 0.102 0.097

0.8000 1 . 492E+00 9.385E-03 1 . 501 E+00 4.097E-01 3 . 227E-03 2.846E-01 -0.071 0.097 0.092

0.9000 1 . 473E+00 1 . 045E-02 1 . 433E+00 4.763E-01 3.607E-03 3.467E-01 -0 .066 0.093 0.037

1 .0000 1 . 459E+00 1 . 1 57E-02 1 . 47 1 E+00 5.445E-01 3. 992E-03 4.093E-01 -0 . 062 0.090 0.032

1 .2500 1 .441E + 00 1 . 453E-02 1 . 455E+00 7. 156E-01 4. 973E-03 5.644E-01 -0.053 0.082 0.073

1 .5000 1 . 434E+00 1 .770E-02 1 .451 E+00 8.877E-01 5 . 995E-03 7.142E-01 -0.047 0.075 0.066

1 .7500 1 . 433E+00 2. 104E-02 1 . 454E+00 1 . 060E+00 7 . 043E-03 8 . 568E-0

1

-0.042 0.070 0.060

2.0000 1 . 434E + 00 2.454E-02 1 . 459E+00 1 . 232E+00 8.113E-03 9.917E-01 -0.038 0.066 0.055

2.5000 1 . 442E+00 3.1 92E-02 1 . 474E+00 1 . 573E+00 1 . 0 34E-02 1 . 240 E + 0 0 -0.033 0.059 0.047

3.0000 1 .451E+00 3. 970E-02 1 . 491 E+00 1 . 91 0E+00 1 . 264E-02 1 . 46 1 E+00 -0.029 0.054 0.042

3.5000 1 .461 E+00 4 . 783E-02 1 .509E+00 2 . 243E+00 1 . 500E-02 1 . 660E+00 -0.026 0.050 0.038

4.0000 1 .471E+00 5 . 624E-02 1 . 527E+00 2 . 573E+00 1 . 740E-02 1 . 839E+00 -0.024 0 . 047 0.034

4.5000 1 . 479E+00 6 . 487E-02 1 . 544E+00 2.398E+00 1 . 985E-02 2 . 003E+00 -0.023 0.044 0.032

5.0000 1 . 483E+00 7.369E-02 1 .561 E+00 3 . 220E+00 2 . 233E-02 2 . 1 54E+00 -0.022 0.042 0.030

5.5000 1 . 495E+00 8 . 270E-02 1 . 573E+00 3.539E+00 2 . 482E-02 2 . 293E+00 -0.021 0.040 0.023

6.0000 1 . 50 3E + 00 9. 188E-02 1 . 595E+00 3 . 354E+00 2.734E-02 2 . 422E+00 -0.020 0.038 0.026

7.0000 1 .51 6E+00 1 .107E-01 1 . 627E+00 4 . 475E+00 3.241E-02 2 . 6 55E+0 0 -0.019 0.035 0.024

3.0000 1 . 523E+00 1 .299E-01 1 . 657E+00 5 . 084E+00 3.751 E-02 2.861 E+00 -0.013 0.033 0 .022 9.0000 1 . 538E+00 1 -494E-01 1 . 687E+00 5 . 632E+00 4.262E-02 3 . 046E+00 -0.017 0.031 0.021 10.0000 1 . 547E+00 1 .693E-01 1 .71 7E+00 6 . 26 9E+00 4.771 E-02 3 .21 4E+00 -0.016 0.030 0.020 12.5000 1 . 567E+00 2.201E-01 1 . 787E+00 7 . 6 96 E + 00 6 . 036E-02 3 . 577E+00 -0.014 0.027 0.017

15.0000 1 . 583E+00 2 . 723E-01 1 .356E+00 9.069E+00 7.281 E-02 3.881 E+00 -0.013 0.024 0.016

17.5000 1 . 597E+00 3 . 256E-01 1 . 922E+00 1 .039E+01 8 . 500E-02 4. 143E+00 -0.012 0.023 0.014 20.0000 1 . 603E+00 3.797E-01 1 . 938E+00 1 . 1 67E+01 9.691 E-02 4 . 374E+00 -0.010 0.021 0.013

25.0000 1 . 627E+00 4.896E-01 2.11 7E+00 1 .41 1E+01 1 . 1 93E-01 4.769E+00 -0 .003 0.019 0.011 30.0000 1 . 642E+00 6.014E-01 2 . 243E+00 1 . 640E+0

1

1 .415E-01 5.099E+00 -0.007 0.017 0.009

35.0000 1 . 654E+00 7. 146E-01 2.369E+00 1 . 357E+0

1

1 .620E-01 5 . 383E+00 -0.005 0.015 0.C08 40.0000 1 . 665E+00 3 . 289E-0

1

2 . 4 94E+00 2.063E+01 1 .814E-01 5 . 633E+00 -0.005 0.014 0.007

45.0000 1 . 674E+00 9.441E-01 2.61 8E+00 2 . 253E+0

1

1 . 993E-01 5 . 856E+00 -0 . 004 0.013 0.006 50.0000 1 . 682E+00 1 . 060E+00 2 . 742E+00 2 . 445E+0

1

2.172E-01 6 . 057E+00 -0.003 0.012 0.006

55 .0000 1 . 639E+00 1 . 1 77E+00 2 . 866 E+00 2 . 623E+0

1

2.337E-01 6 . 240E+00 -0.003 0.012 0.005

60.0000 1 . S 96E + 00 1 . 294E+00 2. 990E+00 2.794E+01 2.494E-01 6 . 408E+00 -0.002 0.011 0 .005 70.0000 1 . 707E+00 1 . 530E+0 0 3 . 237E+00 3.1 15E+01 2 . 785E-01 6 . 707E+00 -0.002 0.010 0 .004 30.0000 1 .717E+00 1 . 767E+00 3 . 484E+00 3.41 3E+01 3.049E-01 6 . 968E+00 -0.001 0.009 0.003

90.0000 1 .726E+00 2 . 006E+00 3.731 E+00 3.690E+01 3.291E-01 7 . 1 99E+00 -0.001 0.009 0.003

100.0000 1 . 734E+00 2 . 245E+00 3.979E+00 3. 950E+01 3.513E-01 7 . 406E+00 -0.001 0.008 0.002

125.0000 1 .750E+00 2 . 843E+00 4 . 598E+00 4 . 534E+0

1

3.997E-01 7 . S47E+00 -0.001 0.007 0.002

1 50 .0000 1 . 763E+00 3 . 455E+00 5.21 SE+00 5 . 044E+0

1

4.400E-01 3.209E+00 -0.000 0.006 0.001 175.0000 1 . 77 4E+00 4. 065E+00 5 . S3 9E+00 5.497E+01 4.743E-01 8.51 5E+00 -0.000 0.006 0.001 200.0000 1 . 733E+00 4 . 677E+00 6.461E+00 5 . 904E+0

1

5.03SE-01 8.7SOE+00 -0.000 0.006 0.001 250.0000 1 . 799E+00 5. 907E+00 7 . 707E+00 6. 6 11 E+01 5.523E-01 9 . 225E+0 0 -0.000 0.005 0.001

300 .0000 1 . 31 2E+00 7 . 1 42E+00 8. 955E+00 7.21 3E+01 5 . 907E-01 9 . 588E+00 -0.000 0.005 0.001 350.0000 1 . 323E+00 8.331 E+00 1 . 0 20E+0

1

7 . 735E+0

1

6.221E-01 9 . 896E+00 -0.000 0.004 0.001 400.0000 1 .333E+00 9 . 622E+00 1 . 146E+01 3.1 97E+01 6 . 482E-01 1 .016E+01 -0.000 0.004 0.000 450.0000 1 .341 E+00 1 . 037E+01 1 -271E+01 3.512E+01 6 . 7 0 4E-0

1

1 . 040E+0

1

-0.000 0.004 0.000 500.0000 1 .349E+00 1 .21 1 E + 01 1 . 396E+01 8. 937E+01 6 .895E-01 1 . 06 1 E + 01 -0 .000 0.004 0.000 550.0000 1 .356E+00 1 . 336E+0

1

1 .521 E+01 9 . 330E+0

1

7.062E-01 1 . 080E+01 -0.000 0.004 0.000 600.0000 1 . 862E+00 1 . 46 1 E+01 1 . 647E+0

1

9.646E+01 7.209E-01 1 .097E+01 -O . 000 0.003 0.000 700.0000 1 . 87 3E+0 0 1.711 E+01 1 . 8 98E + 0

1

1 .021E+02 7 . 457E-0

1

1 . 1 2SE+01 -0.000 0.003 0.000 300.0000 1 .3821+00 1 .9S1E+01 2. 1 49E+01 1 .071 E+02 7.653E-01 1 . 155E+01 -0.000 0.003 0.000 900.0000 1 .391 E+00 2.21 1E+01 2 . 400E+0

1

1 . 1 15E+02 7.82SE-01 1 . 1 78E+0

1

-0.000 0.003 0.000 1000.0000 1 . 3 98E + 0 0 2 . 462E+0

1

2 . 652E+0

1

1 . 154E+02 7.969E-01 1 . 1 99E+01 -0.000 0.003 0.000

164
POSITRONS IN POLYMETHYL METHACRYLATE, "LUCITE", "PERSPEX" , "PLEXIGLAS"

I = 7 A . 0 eV DENSITY =1.1 90E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log )/d(logI

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cra 2 /g MeV cm 2 /g MeV cm 2 /g g/cm 2 0.0100 2 . A 1 9E + 01 2.06AE-03 2.A1 9E+01 2.309E-0A A. 1 1 1 E-05 0 .

0

-0.130 0.202 0.198 0.0125 2 . 023E+0

1

2. 1 80E-03 2 . 023E+0

1

3. AA5E-0A 5.21 9E-05 0.0 -0. 1 7A 0 . 1 9A 0.190 0.0150 1 .7A9E+01 2 . 275E-03 1 . 7A9E+01 A.773E-0A 6 . 331 E-05 0.0 -0.169 0.187 0 . 18A 0.0175 1 . 5A6E+0

1

2.355E-03 1 . 5A6E+0

1

6 . 302E-0A 7. AAAE-05 0.0 -0.165 0.182 0.179 0.0200 1 . 390E+0

1

2. A26E-03 1 . 390E+01 3.010E-OA 8 . 5 57 E-0 5 0.0 -0.161 0.178 0.175

0.0250 1 . 16AE+01 2.5A5E-03 1 . 16AE+01 1 . 1 96E-03 1 .073E-0A 0.0 -0.156 0.172 0.169

0.0300 1 . 009E+01 2.6A0E-03 1 .009E+01 1 . 559E-03 1 .293E-0A 0.0 -0.152 0.167 0.165

0.0350 8 . 9A3E+00 2.720E-03 8. 9A6E+00 2. 186E-03 1 .517E-0A 0.0 -0 . 1 A9 0.163 0.161

0 .0400 8 . 068E+00 2 . 7S8E-03 8 . 070E+00 2.776E-03 1 .73AE-0A 0.0 -0 . 1 A7 0.160 0.158

0 .0A50 7 . 37AE+00 2.850E-03 7 . 377E+00 3. A2AE-03 1 . 9A3E-0A 0.0 -0 . 1 A5 0.157 0.155

0 .0500 6 .81 0E+00 2. 90AE-03 6 .81 3E+00 A.130E-03 2.15SE-0A 0.0 -0.1A3 0.155 0.153 0.0550 6 . 3A3E+00 2.95AE-03 6 . 3A6E+00 A . 8 92E-0 3 2.368E-0A 0.0 -0.1A1 0.153 0.151 0.0600 5. 9A9E+00 3.000E-03 5. 952E+00 5.706E-03 2.575E-0A 0.0 -0 . 1 AO 0.151 0.150 0.0700 5.321 E+00 3.083E-03 5.32AE+00 7 . A86E-03 2. 981 E-OA 0.0 -0 . 1 38 0.1 A8 0.1 A7 0.0300 A.3A2E+00 3. 157E-03 A . SA6E+00 9. A53E-03 3.378E-0A 0.0 -0.136 0.1 A6 0 . 1 AA 0.0900 A . A65E+00 3.22SE-03 A.A69E+00 1 .161E-02 3 . 766E-0A 0.0 -0.13A 0.1 AA 0.1A2 0.1000 A . 1 6 1 E+00 3 . 29AE-03 A . 1 6 AE+00 1 . 393E-02 A.1A6E-0A 0.0 -0.133 0.1A2 0 . 1 A1 0.1250 3 . 6 06E + 00 3. A57E-03 3.609E+00 2.0A1 E-02 5 . 067E-0A 0.0 -0.130 0.138 0.137

0.1500 3 . 232E+00 3.61 3E-03 3 . 235E+00 2 . 77AE-02 5 . 952E-0

A

0.0 -0.127 0.136 0.135

0.1750 2 . 963E+00 3 . 766E-03 2 . 967E+00 3 . 583E-02 6 . 807E-0

A

0.0 -0.126 0 . 1 3 A 0.133

0.2000 2.762E+00 3.920E-03 2 . 766E+00 A. A57E-02 7.636E-0A 0.0 -0.12A 0.132 0.131 0.2500 2. A82E+00 A.2A3E-03 2.A87E+00 6 . 370E-02 9.233E-0A 0.0 -0.122 0.129 0.128 0.3000 2 . 300E+00 A . 58AE-03 2 . 30 AE+00 8.A6AE-02 1 . 077E-03 0.0 -0.120 0.127 0.126 0.3500 2.173E+00 A . 9A1 E-03 2. 178E+00 1 . 070E-0

1

1 . 22SE-0 3 0.0 -0.118 0.125 0.12A

0.A000 2.081 E+00 5.31 9E-03 2 . 086E+00 1 . 305E-0

1

1 . 375E-03 0.0 -0.118 0 . 1 2 A 0.122

0 . 6500 2.01 1 E+00 5.718E-03 2.016 E+00 1 .5A9E-01 1 . 522E-0 3 1 . A66E-02 -0.093 0.120 0.119

0.5000 1 . 956E+00 6.133E-03 1 . 962E+00 1 . 80 0E-0

1

1 . 663E-03 A. 1 12E-02 -0.087 0.116 0.113 0.5500 1 . 91 2E+00 6 .563E-03 1.91 9E+00 2.058E-01 1 .81 AE-03 6 . 992E-02 -0.082 0.112 0.109

0.6000 1 . 877E+0 0 7.005E-03 1 . 88AE+00 2.321E-01 1 . 960E-03 1 . 005E-0

1

-0.077 0.108 0 . 10A 0.7000 1 .826E+00 7. 923E-03 1 . S3 AE+00 2.359E-01 2 . 25AE-03 1 . 650E-0

1

-0.069 0.102 0.096 0.8000 1 .791 E+00 8.901 E-03 1 . 800E+00 3.A10E-01 2.551 E-03 2.321E-01 -0.063 0.096 0.089

0 . 9000 1 . 767E+00 9.91 9E-03 1 . 777E+00 3.969E-01 2.852E-03 3.001E-01 -0.053 0.091 0.033

1 .0000 1 . 750E+00 1 . 0 98E-02 1 .761 E+00 A.535E-01 3. 15SE-03 3.679E-01 -0.05A 0.086 0.073

1 .2500 1 . 726E+00 1 . 377E-02 1 . 739E+00 5 . 965E-01 3 . 9A0E-03 5 . 330E-01 -0.0A7 0.078 0.068

1 .5000 1 . 71 6E+00 1 . 677E-02 1 . 7 33E+0 0 7.A05E-01 A.7A8E-03 6 -887E-01 -0.0A2 0.071 0.061

1 .7500 1 .71 AE+00 1 . 993E-02 1 . 73AE+00 8.8A8E-01 5.531 E-03 3 . 339E-0

1

-0.039 0.066 0.055

2.0000 1 . 7 1 6E+00 2.323E-02 1 . 739E+00 1 . 029E+00 6 . A36E-03 9.639E-01 -0.036 0.062 0.051 2.5000 1 . 72AE+00 3.01 6E-02 1 . 755E+00 1 . 31 5E+00 8 . 201 E-03 1 . 21 2E+00 -0.033 0.056 O.OAA

3.0000 1 . 736 E+0 0 3.7A9E-02 1 . 773E+00 1 . 599E + 00 1 . 003E-02 1 . A25E+00 -0.030 0.051 O.OAO

3.5000 1 . 7A8E+00 A.512E-02 1 . 793E+00 1 . 87 9E+00 1 . 1 90E-02 1 .61 3E+00 -0.029 0.0A8 0.037

A. 0000 1 .759E+00 5 . 298E-02 1 .81 2E+00 2. 156E + 00 1 .381 E-02 1 . 733E+00 -0.027 0.0A5 0.03A

A. 5000 1 . 770E+00 6 . 1 07E-02 1 .832E+00 2 . A3 1 E+0 0 1 . 576E-02 1 . 936E+00 -0.026 0 .0A3 0.033

5.0000 1 .781 E+00 6 . 937E-02 1 . 850E+00 2 . 702E+00 1 . 772E-02 2 . 077E+00 -0.025 0 .0A1 0.031 5.5000 1 -791E+00 7 . 78AE-02 1 . 868E+00 2.971 E+00 1 . 971 E-02 2 . 207E+00 -0 .02A O.OAO 0.030 6.0000 1 . 800E+00 8.6A7E-02 1 -S86E+00 3 . 238E+00 2.171 E-02 2. 327E+00 -0.02A 0.033 0.029

7.0000 1 .81 6E+00 1 . 0 A 1 E-Ol 1 . 920E+00 3 . 763E+00 2 . 57 6 E-0 2 2 . 5A5E+00 -0.022 0.036 0.027 8.0000 1 .831 E+00 1 . 222E-0

1

1 . 953E+00 A . 279E+00 2. 98AE-02 2.73SE+00 -0.021 0.03A 0.025

9.0000 1 . 8AAE+00 1 .A07E-01 1 . 9S5E+00 A . 737E+00 3 . 39AE-02 2.91 AE+00 -0.020 0 .033 0.02A

10.0000 1 . 855E+0 0 1 . 596E-0

1

2.01 5E+00 5 . 287E+00 3 . 805E-02 3 . 073E+00 -0.019 0.031 0.023

12.5000 1 .330E+00 2.079E-01 2 . 088E+0 0 6 . 506E+00 A . 833E-02 3.A21E+00 -0.016 0.028 0.020

15.0000 1 .399E+00 2.577E-01 2 . 1 57E+00 7 . 68AE+00 5 . 85AE-02 3.71 6E+00 -0 .01 A 0.026 0.018

17.5000 1 . 91 5E+00 3.086E-01 2 . 22AE+0 0 8 . 825E+00 6 . 863E-02 3. 97AE+00 -0.012 0.02A 0.016 20.0000 1 . 929E+00 3.S03E-01 2.289E+00 9 . 933E+00 7 . 857E-02 A . 202E+00 -0.010 0.022 0 . 0 1 A 25.0000 1 . 951 E+00 A . 656E-0

1

2.A17E+00 1 .206E+01 9 . 7 9CE-02 A . 596E+00 -0 .008 0.020 0.012 30.0000 1 . 968E+00 5.728E-01 2.5A1E+00 1 . A08E+0

1

1 . 165E-01 A . 927 E + 0 0 -0.006 0.018 0.010 35.0000 1 . 983E+00 6 .81 5E-01 2 . 66AE+00 1 . 600E+0

1

1 .3A2E-01 5.21 2E+00 -0.005 0.016 0.008

AO . 0000 1 . 995E+00 7. 91 2E-01 2 . 786E+00 1 . 783E+0

1

1 .512E-01 5. A63E+00 -0.00A 0.015 0.007 A5.0000 2 . 005E+00 9.020E-01 2. 907E+OO 1 . 959E+01 1 . 67AE-0

1

5 . 687E+00 -0.003 0.01 A 0.006 50.0000 2.01 5E+00 1.01 3E+00 3 . 028E+00 2. 127E+01 1 . 329E-0

1

5.839E+00 -0.003 0.013 0.006 55.0000 2 . 023E+00 1 . 126E+00 3. 1 A9E+00 2 . 239E+0

1

1 . 978E-01 6 . 072E+00 -0.002 0.012 0.005

60 .0000 2.031 E+00 1 . 238E+00 3.269E+00 2. AA5E+01 2. 1 20E-01 6 . 2A1 E+00 -0.002 0.011 0 . 00 A 70.0000 2.0AAE+00 1 . A65E+00 3.509E+00 2.7AOE+01 2 . 337E-01 6 . 5 A 1 E+00 -0.001 0.010 0 . 0 0 A 80.0000 2 . 055E+00 1 . 6 9AE+00 3 . 750E+00 3.016 E+0

1

2 . 632E-0

1

6 . 80 3E+0 0 -0.001 0.009 0.003

90 .0000 2 . 065E+00 1 . 92AE+00 3 . 990E+00 3 . 27AE+0

1

2.859E-01 7 . 0 3AE+00 -0.001 0.009 0.003 100.0000 2 . 07 AE+00 2.1 55E+00 A . 230E+00 3.518E+01 3.069E-01 7 . 2A2E+00 -0.001 0.003 0.002

125.0000 2 . 0 93E+00 2 . 7 37E+0 0 A . 830E+00 A . 07 1 E+0

1

3 . 53AE-0

1

7.683E+00 -0.001 0.007 0.002 150.0000 2. 108E+00 3 . 323E+00 5 . A31 E+00 A . 553E+0

1

3. 923E-01 8 . 0A5E+00 -0.000 0.006 0.001 175.0000 2. 1 2 1 E+00 3.91 2E+00 6 . 033E+00 A . 995E+01 A.268E-01 8.351 E+00 -0.000 0.006 0.001 200.0000 2.1 33E+00 A.503E+00 6 . 636E+00 5 . 3 90 E+0

1

A.565E-01 8.61 7E+00 -0.000 0.005 0.001 250.0000 2.151 E+00 5 . 6 92E+00 7 .8A3E+00 6 . 082E+0

1

5.059E-01 9.061 E+00 -0.000 0.005 0.001 300.0000 2. 166E+00 6 . 837E+00 9 . 053E+00 6 . 675E+0

1

5 . A56E-0

1

9. A25E+00 -0.000 0 . 00A 0.001 350.0000 2 . 1 79E+00 8 . 085E+00 1 .026E+01 7 . 1 93E+01 5 . 733E-0

1

9 . 735E+00 -0.000 0 .00A 0.000

A00 .0000 2.1 90E+00 9 . 286E+00 1 . 1 A8E+0

1

7 . 65AE+0

1

6 . 059E-O1 9. 999E+00 -0.000 0 .00A 0.000

A50 .0000 2 . 20 0 E+0 0 1 . 0A9E+01 1 .269E+01 3 . 063E+0

1

6 . 295E-0

1

1 . 023E+0

1

-0 .000 0.00A 0.000 500.0000 2.209E+00 1 . 1 70E+01 1 . 391 E+01 8.AAAE+01 6.A99E-01 1 .0AAE+01 -0.000 0.003 0.000 550.0000 2.21 7E+00 1 . 290E+0

1

1 .51 2E+01 8 . 789E+0

1

6 . 679E-01 1 .06AE+01 -0.000 0.003 0.000 600.0000 2 . 22AE+00 1 . All E+01 1 .63AE+01 9 . 1 07E+01 6 . 338E-0

1

1 . 081 E+01 -0.000 0.003 0 .000 700.0000 2 . 237E+00 1 . 653E + 0

1

1 . 877E+0

1

9. 678E+01 7.103E-01 1.11 2E+01 -0.000 0.003 0.000 800.0000 2 . 2A8E+00 1 . 8 96E+0

1

2.121E+01 1 . 0 1 8E+02 7 . 329E-0

1

1 . 1 38E+01 -0.000 0.003 0.000 900.0000 2.257E+00 2.1 39E+01 2 . 36AE+01 1 . 062E+02 7.51 AE-01 1 . 1 62E+01 -0.000 0.003 0.000 1000.0000 2 . 266E+00 2 . 382E+0

1

2 . 608E+0

1

1 . 103E+02 7.672E-01 1 . 183E+01 - 0.000 0.003 0.000

165
POSITRONS IN SODIUM IODIDE

I = 452.0 eV DENSITY = 3.667E+00 g/ca 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm 2 /g MeV cm 2/g MeV cm 2 /g g/csi 2 0.0100 1 .291 E+01 2.640E-03 1 .291 E+01 4 . 623E-04 8 . 502E-05 0.0 -0.267 0.330 0.305

0.0125 1 . 099E+0

1

3 . 032E-03 1 . 0 99E+0

1

6 . 730E-04 1 .160E-04 0.0 -0.253 0 . 303 0 . 286 0.0150 9.621 E+00 3 . 372E-03 9.625E+00 9.1 67E-04 1 . 488E-04 0.0 -0.242 0.292 0.272

0.0175 8 . 594E+00 3 . 677E-03 8 . 598E+00 1 . 1 92E-03 1 .831 E-04 0.0 -0.234 0.279 0.262

0.0200 7.791 E+00 3 . 957E-03 7 . 795E+0 0 1 .498E-03 2. 186E-04 0.0 -0.228 0.269 0.254

0.0250 6 . 61 1 E+00 4.439E-03 6 .61 6E+00 2.1 97E-03 2. 927E-04 0.0 -0.213 0.254 0.241 0.0300 5 . 783E+00 4.854E-03 5 . 788E+00 3 . 007E-03 3.696E-04 0.0 -0.210 0.243 C .232 0.0350 5 . 1 6SE+00 5 . 239E-03 5. 1 73E+00 3 . 923E-03 4.490E-04 0 .

0

-0.205 0.235 0.224

0 . 0400 4.691 E+00 5.539E-03 4 . 6 96E+00 4 . 939E-03 5 . 306E-04 0.0 -0.200 0.223 0.219

0.0450 4 .31 0E+00 5.903E-03 4.31 6E+00 6.051 E-0 3 6 . 1 38E-04 0.0 -0.196 0.223 0.214

0.0500 3. 99SE+0Q 6 .203E-03 4 . 004E+00 7.255E-03 6 . 933E-04 0.0 -0.193 0.218 0.210 0.0550 3 . 738E+00 5.481E-03 3 . 745E+00 8.547E-03 7.839E-04 0.0 -0.190 0.214 0.206

0.0600 3.51 SE+OO 6 .743E-03 3 . 525E+00 9. 924E-03 8.704E-04 0.0 -0.187 0.210 0.203

0.0700 3.164E+00 7.260E-03 3 . 1 72E+00 1 . 292E-0 2 1 . 046E-03 0.0 -0.183 0.204 0.193

0.0800 2 . 8 93E+00 7.745E-03 2. 901 E+00 1 . 622E-02 1 . 225E-03 0.0 -0.180 0.199 0.193

0.0900 2.679E+00 8 . 207E-03 2 . 687E+00 1 . 981 E-02 1 . 407E-03 0.0 -0.177 0.196 0.190 0.1000 2 . 504E+00 8 . 649E-03 2.51 3E+00 2.366E-02 1 .591E-03 0.0 -0.174 0.192 0.187

0.1250 2. 135E+00 9.665E-03 2.1 95E+00 3.435E-02 2 . 058E-03 0.0 -0.169 0.136 0.181 0.1500 1 . 963E+00 1 . 06 1 E-02 1 . 979E+00 4 . 638E-02 2 . 529E-03 0.0 -0.166 0.181 0.176

0.1750 1 .81 3E+00 1 . 153E-02 1 . 824E+00 5. 956E-02 3.002E-03 0.0 -0.163 0.177 0.173

0.2000 1 . 696E+00 1 . 240E-02 1 . 708E+00 7.374E-02 3 . 47 6 E-0 3 0.0 -0.160 0.174 0.170 0.2500 1 . 533E+0 0 1 .409E-02 1 . 547E+00 1 . 0 46 E-0

1

4.418E-03 0.0 -0.156 0.169 0.165

0.3000 1 . 427E+00 1 . 578E-02 1 . 443E+00 1 . 33 1 E-0

1

5.353E-03 0.0 -0.152 0.165 0.161 0.3500 1 . 354E+00 1 . 750E-02 1 . 371 E+00 1 . 737E-Q

1

6.281 E-0 3 1 . 129E-03 -0.146 0.161 0.157

0.4000 1 . 301 E+00 1 . 925E-02 1 . 320E+00 2.110E-01 7 . 206 E-0 3 5.532E-03 -0.142 0.153 0.154

0.4500 1 .261 E+OO 2.104E-02 1 . 282E+00 2.494E-01 3. 127E-03 1 . 0 97E-02 -0.139 0.155 0.151 0.5000 1 . 232E+00 2.233E-02 1 . 254E+00 2.339E-01 9 . 047E-0 3 1 .71 IE-02 -0.135 0.152 0.147

0.5500 1 . 20 9E+00 2.476E-02 1 . 233E+00 3.291 E-0

1

9 . 966E-03 2 . 388E-02 -0.132 0.150 0.145

0.6000 1 .191 E+00 2.670E-02 1 .218E+00 3.699E-01 1 . 089E-02 3.11 9E-02 -0.130 0.147 0.142

0.7000 1 . 166E+00 3 . 072E-02 1 . 1 97E+00 4.528E-01 1 . 273E-02 4.71 IE-02 -0.125 0.143 0.137

0.8000 1 .151E+00 3.4"3E-02 1 . 186E+00 5.367E-01 1 . 453E-02 6 . 443E-02 -0.120 0.139 0.133

0 . 9000 1 . 1 42E+00 3.930E-02 1 . 181E+00 6.212E-01 1 . 6 44E-02 8 . 284E-02 -0.116 0.136 0.129

1 .0000 1 . 137E+00 4. 384E-02 1 . 181E+00 7.059E-01 1 . 832E-02 1 .021 E-0

1

-0.113 0.133 0.125

1 .2500 1 . 134E+00 5.588E-02 1 . 1 90E+00 9.1 70E-01 2 . 30 6 E-0 2 1 . 530 E-0

1

-0.105 0.126 0.118

1 .5000 1 . 1 39E+00 6 .337E-02 1 . 208E+00 1 . 126E+00 2 . 788E-02 2.0S5E-01 -0.098 0.121 0.111

1 .7500 1 . 1 46E+00 8 . 273E-02 1 . 229E+00 1 . 331 E+00 3 . 273E-02 2.610 E-0

1

-0.092 0.116 0.105

2.0000 1 . 155E+00 9.724E-02 1 . 253E+00 1 . 532E+00 3.774E-02 3. 1 59E-01 -0.087 0.111 0.100

2.5000 1 . 174E+00 1 .276E-01 1 . 302E+00 1 . 924E+00 4.776E-02 4.239E-01 -0.080 0.104 0.091 3.0000 1 . 1 92E+00 1 .594E-01 1 . 35 1 E+00 2.301 E+00 5.781 E-02 5.275E-01 -0.074 0.098 0.034

3.5000 1 . 208E+00 1 . 925E-01 1 . 401 E+00 2 . 6 64E+00 6 . 730E-02 6.25SE-01 -0.069 0.093 0.078

4.0000 1 . 223E + 00 2.267E-01 1 . 450E+00 3.01 5E+00 7.770E-02 7. 184E-01 -0.066 0.089 0.073

4.5000 1 . 237E + 00 2.618E-01 1 . 499E+00 3 . 354E+00 8 . 746E-02 8.057E-01 -0.063 0 . 086 0.069

5.0000 1 . 24 9E+00 2. 978E-01 1 . 547E+00 3 . 683E+00 9.70SE-02 3.381 E-0

1

-0.060 0.082 0.065

5.5000 1 . 250E+00 3.345E-01 1 . 595E + 0 0 4.001 E+00 1 . 065E-0

1

9.660E-01 -0.053 0.080 0.062

6.0000 1 .271 E+00 3.717E-01 1 . 643E+00 4.31 OE+OO 1 . 1 53 E-0 1 1 . 040E+00 -0.056 0.077 0.060

7.0000 1 . 290E+00 4.477E-01 1 . 737E + 00 4. 902E+00 1 . 339E-0

1

1 . 1 77E+00 -0.053 0.073 0.055

8.0000 1 . 306E+00 5.257E-01 1 .831 E+00 5 . 462E+00 1 .512E-01 1 . 30 1 E+00 -0.051 0.069 0.051 9.0000 1 . 320E+00 6 . 055E-0

1

1 . 926E+00 5 . 995E+00 1 . 673E-0

1

1 .416 E+00 -0.043 0.066 0 . 048 10.0000 1 . 333E+00 6 . 368E-0

1

2 . 020E+00 6 . 502E+00 1 . 833E-0

1

1 . 522E+00 -0.046 0.063 0.045

12.5000 1 .359E+00 8.955E-01 2 . 255E+00 7 . 673E+00 2.209E-01 1 . 759E+00 -0.042 0.058 0.039

15.0000 1 .381 E+00 1 . 1 1 OE+OO 2 . 490E+00 8 . 727E+00 2.544E-01 1 . 964E+00 -0.039 0.054 0.035

17.5000 1 . 399E+00 1 . 329E+00 2 . 727E+00 9 . 686E+00 2.848E-01 2. 147E+00 -0.036 0.051 0.031 20.0000 1 . 41 3E+00 1 . 553E+00 2. 967E+00 1 . 057E+0

1

3.124E-01 2.31 2E+00 -0.033 0.048 0.023 25.0000 1 . 433E+00 2.01 1E+00 3 . 449E+00 1 .21 3E+01 3.608E-01 2 . 605E+00 -0.029 0.043 0.024

30.0000 1 . 457E+00 2 . 479E+00 3 . 936E+00 1 . 348E+0

1

4.01 9E-01 2 . 858E+0 0 -0.025 0.040 0.021 35.0000 1 . 472E+00 2 . 958E+00 4 . 430E+00 1 . 468E+0

1

4.373E-01 3.081 E+00 -0.023 0.038 0.018

40.0000 1 . 485EJ-00 3 . 444E+00 4 . 929E+0 0 1 . 575E+01 4.681 E-0

1

3.281 E+00 -0.021 0.035 0.016 45.0000 1 . 496E+00 3 . 934E+00 5 . 430E+00 1 .672E+01 4.952E-01 3 . 463E+00 -0.019 0.034 0.014

50.0000 1 . 506 E + 0 0 4 . 426E+00 5 . 932E+00 1 .760E+01 5.1 93E-01 3 . 628E+00 -0.018 0.032 0.013 55.0000 1 . 5 1 5E+00 4 . 922E+00 6 . 437E+00 1 .841E+01 5 . 407 E-0

1

3 . 780E+00 -0.017 0.031 0.012

60.0000 1 . 522E+00 5 . 422E+00 6 . 945E+00 1 .915E+01 5 . 60 1 E-0

1

3. 921 E+00 -0.016 0.030 0.011 70.0000 1 . 536E+00 6 . 431 E+00 7.967E+00 2 . 050E+0

1

5.936E-01 4 . 1 75E+00 -0.014 0.028 0.009

80 .0000 1 . 547E + 0 0 7 . 448E+00 8 . 995E+00 2. 168E+01 6 . 21 6E-01 4.399E+00 -0.013 0.027 0.008

90 .0000 1 . 557E+00 3 . 470E+00 1 . 003E+0

1

2 . 273E+0

1

6.455E-01 4 . 600 E+OO -0.012 0.026 0.007

100.0000 1 . 566E+00 9 . 496 E+OO 1 . 1 06E+01 2 . 368E+0

1

6.662E-01 4 . 782E+00 -0.011 0.025 0.007

125.0000 1 . 584E+00 1 . 208E+0

1

1 . 3S7E+0

1

2.571 E+0

1

7 . 073E-0

1

5. 174E+00 -0.009 0.023 0.005

1 50.0000 1 . 599E+00 1 .469E+01 1 .629E+01 2 . 738E+0

1

7.384E-01 5 . 502E+00 -0.008 0.022 0.005

175.0000 1 . 6 1 OE+OO 1 . 729E+0

1

1 . 8 90E + 0

1

2.881 E+0

1

7 . 6 27 E-0 1 5 . 783E+00 -0.007 0.021 0.004 200.0000 1 .621 E+00 1 .990E+01 2.152E+01 3.004E+01 7.823E-01 6 . 029E+00 -0.006 0.020 0.003

250.0000 1 . 637E+00 2.51 4E+01 2 . 673E+0

1

3.212E+01 8.123E-01 6 . 445E+00 -0.005 0.018 0.003 300.0000 1 . 650E+00 3.037E+01 3 . 202E + 0

1

3 . 383E+0

1

8 . 343E-0

1

6 . 7 90E+00 -0.004 0.018 0.002 350.0000 1 .661 E+00 3.560E+01 3.726E+01 3 . 527E+0

1

8.51 IE-01 7 . 083E+00 -0.004 0.017 0.002

400 .0000 1 .671 E+00 4 . 082E+0

1

4.249E+01 3.653E+01 8.645E-01 7 . 339E+00 -0.003 0.016 0.002 450.0000 1 . 6 7 9E + 0 0 4 . 605E+0

1

4 . 773E+0

1

3 . 764E+0

1

8 . 754E-0

1

7 . 566 E+00 -0.003 0.016 0.002 500.0000 1 . 637E+00 5.129E+01 5 . 298E+0

1

3 . 863E+0

1

8.345E-01 7.769E+00 -0.003 0.015 0.001 550.0000 1 . 693E+00 5 . 654E+0

1

5 . 823E+0 5 3. 953E+01 8. 923E-01 7 . 954E+00 -0.002 0.015 0.001 600.0000 1 . 6 99E + 00 6.178E+01 6 . 348E+0

1

4.035E+01 8.989E-01 8. 1 23E+00 -0.002 0.015 0.001 700.0000 1 . 71 OE+OO 7 . 229E+0

1

7 .400E + 01 4. 131 E+01 9.093E-01 8 . 423E+00 -0 .002 0.014 0.001 300.0000 1 .719E+00 8.230E+01 8 . 452E+0

1

4 . 308E+0

1

9. 184E-01 8 . 684E+00 -0.002 0.014 0.001 900.0000 1 . 727E+00 9 . 332E+0

1

9 . 504E+0

1

4.41 9E+01 9.253E-01 8.91 5E+00 -0.001 0.013 0.001 1000.0000 1 . 734E+00 1 . 038E+02 1 . 056E+02 4.51 9E+01 9.31 IE-01 9. 122E+00 -0.001 0.013 0.001

166
POSITRONS IN TISSUE-EQUIVALENT GAS (METHANE BASED)

I = 61.2 eV DENSITY = 1.06AE-03 g/cra 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS . EFF. d(i,oq )/d(loqI) COLLISION RADIATIVE TOTAL RANGE YIELD CORK

.

COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

Me V MeV cn 2 /g MeV cn 2 /g MeV cm 2 /g g/cm 2 0.0100 2 . 550E+0

1

2.080E-03 2.551 E+O

1

2. 182E-0A 3.912E-05 0 .

0

-0.17A 0.1 9A 0.191 0.0125 2 . 1 31 E+01 2. 1 98E-03 2.131E+01 3.259E-0A A . 977E-05 0.0 -0.168 0.187 0.183

0.0150 1 .SA0E+01 2.295E-03 1 .8A0E+01 A . 525E-0

A

6 . 0A7E-0 5 0.0 -0.163 0.181 0.178 0.0175 1 -625E+01 2.378E-03 1 . 626E+0

1

5 . 97AE-0A 7.11 9E-05 0.0 -0.160 0.176 0.173 0.0200 1 . A60E+0

1

2 . AA9E-03 1 . A60E+0

1

7 . 599E-0A 8. 191E-05 0.0 -0.157 0.172 0.170

0 .0250 1 . 222E+0

1

2 . 570E-03 1 . 222E+0

1

1 . 1 36 E-0 3 1 . 033E-0A 0.0 -0.152 0.166 0 . 1 6A 0.0300 1 . 058E + 0 1 2.66SE-03 1 . 0 58E + 0

1

1 . 577 E-0 3 1 . 2A7E-0

A

0.0 -0 . 1 A8 0.162 0.160 0.0350 9.376E+00 2.750E-03 9. 379E+00 2 . 080E-03 1 . A58E-0A 0 .

0

-0 . 1 A5 0.158 0.156 0.0A00 8 . A55E+00 2.821 E-03 8 . A57E+00 2 . 6A2E-03 1 . 66SE-0A 0.0 -0 . 1 A3 0.155 0.153

0 . 0A50 7.725E+00 2.S85E-03 7 . 728E+00 3.262E-03 1 . S7SE-0A 0 .

0

-0 . 1A1 0.152 0.151

0 .0500 7.132E+00 2. 9A2E-03 7 . 1 35E+00 3 . 9 36 E-0

3

2 . 080E-OA 0 .

0

-0.139 0.150 0 . 1 A9 0.0550 6.6A1E+00 2 . 9SAE-03 6 . 6AAE+00 A.663E-03 2.2SAE-0A 0.0 -0.138 0.1A8 0.1 A7 0.0600 6 .227E+00 3 . 0A1 E-03 6 . 230E+00 5 . AA 0 E-0 3 2. A85E-0A 0.0 -0.136 0.1A7 0.1A5

0 . 0700 5 . 567E+00 3. 126E-03 5 . 570E+00 7 . 1 A2E-03 2.3SOE-OA 0.0 -0 . 1 3A 0 . 1 A A 0 . 1 A 3 0.0800 5 . 06AE+00 3.20AE-03 5. 067E+00 9 . 027E-03 3.266E-OA 0 .

0

-0.132 0.1A2 0 . 1 AO

0 .0500 A . 66SE+00 3.276E-03 A . 672E+0O 1 . 108E-02 3.6AAE-OA 0.0 -0.131 0 . 1 AO 0.139

0 . 1000 A . 3A9E+00 3 . 3A5E-0 3 A . 352E+00 1 . 330E-02 A.015E-0A 0.0 -0.129 0.138 0.137

0.1250 3 . 767E+00 3.51 2E-03 3.770E+00 1 . 950E-02 A . 91 3E-0A 0.0 -0.127 0.135 0 . 1 3A 0.1500 3 . 37AE+00 3.671E-03 3 . 378E+00 2.653E-02 5.777E-0A 0.0 -0 . 12A 0.132 0.131 0.1750 3.093E+00 3 . S2SE-03 3 . 0 S7E + 00 3. A27E-02 6 . 612E-0A 0 . 0 -0.123 0.130 0.129

0.2000 2 . 882E + 0 0 3. 986E-03 2 . 88 6 E+0 0 A . 26AE-02 7 . A21 E-OA 0 .

0

-0.121 0.129 0.128

0 . 2500 2. 589E+00 A.315E-03 2.59AE+00 6 .099E-02 8 . 983E-OA 0 . 0 -0.119 0.126 0.125 0.3000 2.398E+00 A . 662E-03 2.A02E+00 8 . 1 06E-02 1 .0A9E-03 0 .

0

-0.117 0 . 12A 0.123

0 .3500 2.265E+00 5 . 026E-03 2 . 27 0 E+0 0 1 .025E-01 1 . 1 96E-03 0 .

0

-0.115 0.122 0.121

0 . A000 2.168E+00 5. A10E-03 2.1 7AE+00 1 . 250E-0

1

1 . 3AOE-03 0 .

0

-0 . 1 1 A 0.121 0.120

0 .A500 2.096E+00 5.816E-03 2 . 1 02E+00 1 . ASAE-0

1

1 . A83E-03 0 . 0 -0.112 0.120 0.118 0.5000 2 . 0A2E+0O 6 .239E-03 2 . 0ASE+00 1 . 726E-0

1

1 . 6 26 E-0 3 0 .

0

-0.111 0.118 0.117

0 .5500 1 . 999E+00 6.676E-03 2 . 006E+00 1 . 972E-01 1 . 768E-03 0 .0 -0.110 0.117 0.116

0 .6000 1 . 966E+00 7 . 126E-03 1 . 973E+00 2 . 22AE-0

1

1 . 909E-03 0 .

0

-0.109 0.116 0.115

0.7000 1 . 918E+00 8 . 066E-03 1 . 926E+00 2.737E-01 2. 1 9AE-03 0.0 -0.107 0.115 0.113

0.8000 1 .887E+00 9.057E-03 1 . 8 96E + 00 3.261 E-0

1

2. A80E-03 0.0 -0.106 0.113 0.111 0.9000 1 . 868E + 0 0 1 . 009E-02 1 . 878E + 0 0 3 . 7 9 1 E-0

1

2 . 768E-0

3

0.0 -0 . 1 OA 0.112 0.110

1 .0000 1 . 855E+00 1.11 7E-02 1 . 866E+00 A.325E-01 3 . 059E-03 0.0 -0.103 0.111 0.109

1.2500 1 . 8AAE+00 1 . A02E-02 1 . 858E+00 5.669E-01 3. 799E-03 0.0 -0.100 0.109 0.106

1.5000 1 .8A6E+00 1 . 707E-02 1 . 86 3E + 00 7.01AE-01 A.558E-03 0.0 -0.098 0.107 0.103

1.7500 1 .856E+00 2 . 029E-02 1 . 87 6E + 00 8.351 E-0

1

5 . 333E-0 3 0.0 -0.096 0.105 0.101 2.0000 1 -868E+00 2.365E-02 1 . 8 92E + 0 0 9.678E-01 6 . 12AE-03 0.0 -0 . 09A 0.103 0.100 2.5000 1 .897E+00 3.072E-02 1 . 927E+00 1 . 230E+00 7 . 7 A 1 E-0 3 0.0 -0.092 0.101 0.097

3.0000 1 . 925E+0 0 3.81 9E-02 1 . 96AE+00 1 . A87E+00 9 . 399E-03 0.0 -0.090 0.099 0 .09A 3.5000 1 . S53E+00 A . 597E-02 1 . 999E+00 1 . 739E+00 1 . 1 09E-02 0.0 -0.088 0.097 0.092

A . 0000 1 . 979E+00 5.399E-02 2 . 0 33E+00 1 . 987E+00 1 . 280E-02 0.0 -0.087 0.096 0.091

A .5000 2.003E+00 6 . 22AE-02 2 . 065E+00 2.231 E+00 1 . A53E-02 0.0 -0.085 0 .09A 0.089

5.0000 2 . 025E+00 7.070E-02 2 . 0 96E+00 2.A71 E+00 1 . 627E-02 0.0 -0 .08A 0.093 0.088

5.5000 2 . 0A6E+OO 7 . 93AE-02 2. 125E+00 2 . 708E+00 1 .802E-02 0.0 -0.083 0.092 0.086 6.0000 2 . 065E+00 8.81 3E-02 2. 1 53E+00 2. 9A2E+00 1 . 978E-02 0.0 -0.082 0.091 0.085 7.0000 2 . 1 00E+00 1 .061E-01 2.206E+00 3 . AO 1 E+00 2. 331E-02 0.0 -0.081 0.089 0.083

8.0000 2.131F+00 1 .2A6E-01 2 . 256E+00 3.8A9E+00 2 . 686E-02 0 .0 -0.080 0.088 0.082

9.0000 2. 159E+00 1 . A3AE-0

1

2 . 302E+00 A . 288E+00 3 . 0A0E-02 0.0 -0.079 0.086 0.080

1 0.0000 2.18AE+00 1 .626E-01 2. 3A7E+00 A . 71 8E+00 3.39AE-02 0 .

0

-0.078 0.085 0.079

12.5000 2 . 23EE+00 2.11 9E-01 2 . A 50 E+00 5 . 760E+00 A . 27AE-02 0.0 -0 .076 0.083 0.076 15.0000 2.283E+00 2.626E-01 2 . 5 A5E+00 6.761 E+00 5. 1 A3E-02 0 .0 -0 . 07 A 0.080 0.073

1 7.5000 2.321E+00 3 . 1 AAE-01 2 . 6 35E + 00 7 . 727E+00 5 . 998E-02 0.0 -0.073 0.078 0.071

20 .0000 2 . 35AE+00 3.671 E-0

1

2.721E+00 8 . 660E+00 6 . 838E-02 0.0 -0.072 0.077 0.069 25.0000 2 . A08E+00 A.7A3E-01 2.882E+00 1 .OAAE+Ol 8. A68E-02 1 . 908E-02 -0.060 0 . 07 A 0.065

30.0000 2 . AA6E+00 5.835E-01 3 . 0 30 E + 00 1 .21 AE+01 1 . OOAE-O

1

1 . 033E-0

1

-0 .0A7 0.069 0.059

35.0000 2.A76E+00 6 .9A2E-01 3 . 1 70E+00 1 . 375E+0

1

1 . 1 5AE-0

1

2.153E-01 -O.OAO 0.065 0.052

AO .0000 2 . A99E+00 8.06 0 E-0

1

3. 305E+00 1 . 529E+01 1 . 300E-01 3 . 356E-0

1

-0 -03A 0.062 0 . 0A7

A5 .0000 2.518E+00 9. 188E-01 3. A37E+00 1 . 678E+0

1

1 . A35E-01 A . 562E-0

1

-0.031 0.058 0 .0A3

50 .0000 2 . 535E+00 1 . 032E+00 3 . 567E+00 1 . 820 E + O

1

1 .57AE-01 5.735E-01 -0.028 0.055 0.039 55.0000 2.550E+00 1 .

1

' 7E+00 3.6 96 E + 00 1 . 953E+01 1 .703E-01 6 . 86 1 E-0

1

-0.026 0.053 0.036 60.0000 2.563E+00 1.261 E + 00 3 . 82 A E + 00 2 . 0 9 1 E + O

1

1 . 82SE-0

1

7 . 93AE-01 -0 .02A 0.051 0.033

70 .0000 2.585E+00 1 . A93E+00 A . 077E+00 2 . 3AAE+01 2.065E-01 9 . 92AE-0

1

-0.022 0.0A7 0 .029 80.0000 2 . 603E+00 1 . 725E+0 0 A . 329E+00 2 . 582E+01 2.285E-01 1 . 172E+00 -0 .020 0 . 0 A A 0.025

90 .0000 2.61 9E+00 1 . 960E+00 A.579E+00 2 . 807E+0

1

2 . A 90 E-0 1 1 . 336E+00 -0.019 0 .OA1 0.023 100.0000 2.633E+00 2. 1 95E+00 A . 828E+00 3 . 020 E+0

1

2.683E-01 1 . A85E+00 -0.018 0.039 0.021 125.0000 2 . 662E+00 2 . 7S7E+00 5 . A50E+00 3 . 507E+0

1

3.11 5E-01 1 . 80 9E + 00 -0.017 0.035 0.017 150.0000 2 . 685E+00 3 . 38AE+00 6 . 06 5E+00 3. 9A1 E+01 3 . AS8E-0

1

2.081 E+00 -0.016 0.032 0.015 175.0000 2.705E+00 3 . 98AE+00 6 . 688E+00 A . 333E+0

1

3.81AE-01 2.315E+00 -0.015 0.029 0.013 200.0000 2.721E+00 A .586E+00 7 . 307E+00 A . 6 9 1 E + O

1

A. 1 02E-01 2 . 520E+00 -0.01 A 0.028 0.012 250.0000 2 . 7A8E+00 5 . 7 9 6 E + 0 0 8 . 5AAE+00 5 . 323E+0

1

A . 590E-0

1

2 . 870E+00 -0.013 0.025 0.010 300.0000 2.770E+00 7.01 2E+00 9 . 782E+00 5.869E+01 A . 98SE-01 3. 162E + 00 -0.012 0.023 0.008 350.0000 2.787E+00 8.232E+00 1 . 1 02E+01 6.351 E+O

1

5.323E-01 3.A1AE+00 -0.011 0.021 0.007

A00 . 0000 2 . 802E+00 9 . A56E+00 1 .226E+01 6 . 78 1 E+O

1

5.607E-01 3 . 636E + 00 -0.010 0.020 0 . 006 A50 . 0000 2.615E+00 1 .068E+01 1 .350E+01 7.169E+01 5 .853E-01 3.836E+00 -0.009 0.019 0.006 500.0000 2.827E+00 1 . 1 91 E+01 1 .A7AE+01 7 . S2AE+0

1

6 . 06SE-0

1

A.017E+00 -0.008 0.018 0 .005 550.0000 2 . 8 37E + 00 1 .31AE+01 1 . 598E+0

1

7 . S50E+0

1

6 . 257E-0 1 A . 18AE+00 -0.007 0.018 0 .005 600.0000 2.8A6E+00 1 . A37E+0

1

1 .721E+01 8 . 1 51 E+01 6 .A26E-01 A . 338E + 00 -0.007 0.017 0 .OOA 700.0000 2.S61E+00 1 .63 3E + 0

1

1 . 97CE+01 8 . 69AE+01 6 . 7 1 6 E-0

1

A . 6 1 AE + 00 -0 . 006 0.016 0 .OOA 800.0000 2 . 875E+00 1 . 930E+01 2.21SE+01 9. 172E+01 6 . 955E-01 A.859E+00 -0.005 0.015 0.003 900.0000 2.886E J-00 2. 177E+01 2. A66E+01 9 . 599E+0

1

7 . 1 56 E-0

1

5 . 077E + 00 -0 .OOA 0.015 0.003

1000 .0000 2.896E+00 2 . A25E+0

1

2.71AE+01 9 . 986 E + O

1

7.325E-01 5 . 27 5E + 0 0 -0.003 0 .01 A 0.003

16 7
POSITRONS IN TISSUE-EQUIVALENT GAS (PROPANE BASED)

I = 59.5 eV DENSITY = 1.826E-03 g/cn 3 <20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS . EFF. d( log )/d( logl

)

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cra 2 /g MeV cm 2 /g MeV cra 2 /g g/cm 2 0.0100 2 . 565E+0

1

2 . 048E-03 2.565E+01 2.163E-04 3 . 840E-05 0.0 -0.173 0.193 0.190 0.0125 2.1 43E+01 2.162E-03 2. 143E + 01 3 . 239E-04 4.S79E-05 0.0 -0.167 0.185 0.183

0.0150 1 .850E+01 2 . 255E-03 1 . S50E + 0

1

4.499E-04 5.922E-05 0.0 -0.163 0.180 0.177 0.0175 1 . 634E+0

1

2.334E-03 1 . 634E+0

1

5.940E-04 6 . 967E-05 0.0 -0.159 0.175 0.173

0.0200 1 . 468E+0

1

2 . 40 3E-0 3 1 . 468E+0

1

7 . 557E-04 3.012E-05 0.0 -0.156 0.171 0.169

0 .0250 1 . 223E+0

1

2.520E-03 1 . 229E+0

1

1 . 1 30E-03 1 . 01 0E-04 0.0 -0.151 0.165 0.163

0 . 0300 1 .0S3E+01 2.614E-03 1 . 063E+01 1 .569E-03 1 . 2 1 7E-04 0.0 -0.147 0.161 0.159

0.0350 9 . 422E+00 2.692E-03 9 . 425E+00 2.069E-03 1 . 423E-04 0.0 -0.145 0.157 0.155

0 . 0400 3 . 495E+00 2.759E-03 8 . 498E+00 2.629E-03 1 . 627E-04 0.0 -0.142 0.154 0.153

0.0450 7.761 E+00 2.81 9E-03 7 . 764E+00 3.245E-03 1 . 823E-04 0.0 -0.140 0.152 0.150

0.0500 7. 1 65E+00 2 .873E-03 7. 163E+00 3. 91 6E-03 2 . 027E-04 0 .

0

-0.139 0.150 0.148

0.0550 6.671 E + 00 2. 922E-03 6 . 674E+00 4.640E-03 2 . 224E-04 0.0 -0.137 0.148 0.146

0.0600 6 . 255E + 0 0 2 . 9S7E-03 6 . 253E+00 5.41 4E-03 2.41 9E-04 0.0 -0.136 0.146 0.145

0.0700 5.592E+00 3 . 048E-03 5 . 595E+00 7.103E-03 2.801E-04 0 .

0

-0.134 0.143 0.142

0.0300 5 . 087E+00 3.122E-03 5 . 0 90E + 0 0 8.985E-03 3. 175E-04 0.0 -0.132 0.141 0.140

0.0900 4 . 689E+00 3.1 90E-03 4 . 692E+00 1 . 103E-02 3.541 E-04 0.0 -0.130 0.139 0 . 1 38 0.1000 4 . 363E+00 3.256E-03 4.371 E+00 1 . 324E-02 3.399E-04 0.0 -0.129 0.138 0.136

0.1250 3 . 7S3E+00 3.416E-03 3 . 736 E+0 0 1 . 942E-02 4 . 768E-0 4 0.0 -0.126 0.134 0.133

0.1500 3 . 339E+00 3.570 E-0 3 3 . 392E+00 2.641E-02 5. 603E-04 0.0 -0.124 0.132 0.131 0.1750 3 . 1 06E+00 3.721E-03 3.1 1 0E+00 3.412E-02 6.40 9E-04 0.0 -0.122 0.130 0.129

0.2000 2 . 8 94E+0 0 3.373E-03 2 . 893E+0 0 4.246E-02 7.1 92E-04 0.0 -0.121 0 . 1 23 0.127

0.2500 2 . 600E+00 4 . 1 91 E-03 2. 604E+00 6 . 073E-02 8 . 700E-04 0.0 -0.118 0.125 0.125

0.3000 2 . 407E+00 4 . 528E-03 2.41 2E+00 3 . 072E-02 1 . 0 1 6 E-0 3 0.0 -0.117 0.123 0.122

0.3500 2 . 274E+00 4.881 E-03 2.279E+00 1.021 E-0 1 1 . 153E-03 0 .0 -0.115 0.122 0.121 0.4000 2. 177E+00 5.254E-03 2. 182E+00 1 . 245E-0

1

1 . 297E-03 0.0 -0.113 0.120 0.119

0.4500 2. 1 05E+00 5 . 648E-03 2.1 1 0E+00 1 . 478E-0

1

1 . 436E-03 0.0 -0.112 0.119 0.118

0.5000 2.049E+00 6.058E-03 2. 056E+00 1 .71 9E-01 1 .573E-03 0.0 -0.111 0.118 0.117

0.5500 2.007E+00 6 . 482E-03 2.01 3E+00 1 . 965E-0

1

1 .710E-03 0.0 -0.110 0.117 0.116

0.6000 1 . 973E+00 6 . 91 9E-03 1 . 930 E+00 2.215E-01 1 .843E-03 0.0 -0.109 0.116 0.115

0.7000 1 . 925E+00 7.831 E-03 1 . 933E+00 2.727E-01 2. 123E-03 0.0 -0.107 0.114 0.113

0.8000 1 . 3 94E+00 8 . 7 92E-0 3 1 . 903E+00 3.248E-01 2 . 399E-03 0.0 -0.105 0.113 0.111 0.9000 1 . 374E+00 9.797E-03 1 . 884E + 0 0 3.777E-01 2 . 673E-03 0.0 -0.104 0.112 0.110

1 .0000 1 . 862E+00 1 . 084E-02 1 . 873E+00 4.309E-01 2 . 960E-03 0.0 -0.103 0.111 0.103

1 .2500 1 . 850E+00 1 . 360E-02 1 . 86 4E + 00 5.649E-01 3.675E-03 0.0 -0.100 0.103 0.106

1 .5000 1 .853E+00 1 . 656E-02 1 . 86 9E+00 6 . 939E-01 4.409E-03 0.0 -0.098 0.106 0.103

1 .7500 1 . 36 2E+0 0 1 . 969E-02 1 . 882E+00 8 . 322E-0

1

5. 159E-03 0.0 -0.096 0.105 0.101 2.0000 1 . 374E+0 0 2.295E-02 1 .897E+00 9.645E-01 5 . 923E-03 0.0 -0.094 0.103 0.099

2.5000 1 . 903E+00 2 . 980E-02 1 . 933E+00 1 . 226E+00 7 .489E-03 0 .

0

-0.092 0.101 0.097

3.0000 1 . 932E+00 3 . 705E-02 1 . 969E+00 1 . 482E+00 9.093E-03 0.0 -0 . 089 0.099 0.094

3.5000 1 . 959E+00 4 . 459E-02 2 . 004E+00 1 . 734E+00 1 . 073E-02 0.0 -0.033 0.097 0.092

4.0000 1 . 985E+00 5 . 237E-02 2 . 037E+00 1 . 981 E+00 1 . 238E-02 0.0 -0.086 0.095 0.090

4.5000 2.009E+00 6 . 037E-02 2.06 9E+00 2 . 225E+0 0 1 . 406E-02 0.0 -0.085 0.094 0.089

5.0000 2.031 E+00 6 . 357E-02 2 . 1 00E+00 2 . 465E+00 1 . 574E-02 0 . 0 -0.084 0.093 0 . 037 5.5000 2 . 052E+00 7.695E-02 2. 129E+00 2 . 70 1 E+00 1 . 744E-02 0.0 -0.083 0.092 0.086

6.0000 2.071 E+00 3 . 548E-02 2.1 57E+00 2. 934E+00 1 . 91 4E-02 0.0 -0.082 0.091 0 .085 7.0000 2 . 1 06E+00 1 .029E-C1 2.209E+00 3.392E+00 2 . 257E-02 0.0 -0.031 0.089 0.033 8.0000 2.137E+00 1 . 208E-0

1

2 . 258E+00 3 . 840E+00 2 . 600E-02 0.0 -0.079 0.088 0 . 0S1 9.0000 2.1 65E+00 1 . 392E-01 2 . 304E+00 4 . 278E+00 2. 944E-02 0 .

0

-0.073 0.086 0.030

10.0000 2.190E+00 1 . 573E-0

1

2 . 348E+00 4 . 708E+00 3 . 288E-02 0.0 -0.077 0.085 0.079

12.5000 2 . 244E+00 2.057E-01 2 . 450E+00 5 . 750E+00 4. 143E-02 0.0 -0 .076 0.082 0.076 15.0000 2 . 289E+00 2.549E-01 2 . 544E+00 6.751 E+00 4. 988E-02 0.0 -0.074 0 . 030 0.073

17.5000 2 . 326E+00 3.053E-01 2 . 632E+00 7.717E+00 5.820E-02 7 . 537E-0 3 -0.066 0.073 C .071 20.0000 2 . 356 E+0 0 3 . 565E-0

1

2.71 2E+00 8 . 653E+00 6 . 639E-02 5 . 064E-02 -0.055 0.075 0.067 25.0000 2 . 400E+00 4.607E-01 2 . 85 0 E + 0 0 1 . 045E+0

1

8 . 239E-02 1 . 907E-0

1

-0.042 0.070 0.057

30.0000 2 . 432E+00 5.669E-01 2. 999E+00 1 .21 5E+01 9 . 736E-02 3.525E-01 -0.035 0 .064 0.050 35.0000 2 . 457E+00 6 . 744E-0

1

3. 1 31 E+00 1 . 379E+0

1

1 . 128E-01 5. 139E-01 -0.030 0.060 0.044

40.0000 2 . 477E+00 7.831 E-0

1

3 . 260E+00 1 . 535E+0

1

1 . 272E-0

1

6 . 676E-0

1

-0.027 0.056 0.039

45.0000 2 . 495E+00 8. 928E-01 3 . 388E+00 1 . 685E+0

1

1 .410 E-0

1

S.113E-01 -0.025 0.053 0.035

50.0000 2.51 0E+00 1 . 003E+00 3.513E+00 1 .830E+01 1 . 544E-0

1

9 . 464E-0

1

-0.023 0 . 050 0.032

55.0000 2 . 524E+00 1.11 4E+00 3 . 638E+00 1 . 970E+01 1 . 673E-0

1

1 . 072E+00 -0.022 0 .047 0.029

60.0000 2 . 536E+00 1 . 226 E+00 3 . 762E+00 2.1 05E+01 1 . 797E-0

1

1 . 189E+00 -0.021 0.045 0.027 70.0000 2. 556E+00 1 . 451 E+00 4 . 007E+00 2 . 363E+0

1

2.032E-01 1 . 403E+00 -0.019 0.042 0.024

80.0000 2.574E+00 1 . 677E+00 4.252E+00 2 . 605E+0

1

2.251 E-0

1

1 . 593E+00 -0.013 0.039 0.021

90 .0000 2 . 590E+00 1 . 905E+00 4 . 495E+00 2 . 834E+0

1

2 . 456 E-0

1

1 . 763E+00 -0.018 0.037 0.019

100.0000 2 . 603E+00 2. 1 34E+00 4.737E+00 3.051E+01 2.648E-01 1 . 91 7E+00 -0.017 0.035 0.018

125.0000 2.631 E+00 2.71 0E+00 5 . 342E+00 3 . 547E+0

1

3.073E-01 2.251 E+00 -0.016 0.031 0.015

150.0000 2 . 654E+00 3.291 E+00 5 . 945E+00 3.991 E+0

1

3 . 45 1 E-0

1

2 . 529E+00 -0.015 0.028 0.013

175.0000 2 . 673E+0 0 3 . 874E+00 6 . 547E+00 4.391E+01 3.777E-01 2.76 9E+0 0 -0.014 0.026 0.011 200.0000 2.689E+00 4 . 460E+00 7 . 1 49E+00 4 . 756E+0

1

4.065E-01 2. 980E+00 -0.013 0.025 0.010 250.0000 2.71 5E+00 •5 . 638E+00 8 . 353E+00 5.403E+01 4 . 553E-0

1

3.341 E+00 -0.011 0.022 0.009 300.0000 2 . 735E+0 0 6 . 822E+00 9 . 557E+00 5. 962E+01 4.953E-01 3 . 644E+00 -0.010 0.021 0.007 350.0000 2 . 752E+00 3.00 9E+00 1 .076E+01 6 . 455E+0

1

5 . 283E-0

1

3. 907E+00 -0.003 0.019 0.006 400.0000 2.766E+00 9 . 200E+00 1 . 1 97E+01 6.895E+01 5 . 573E-0

1

4 . 1 40E+00 -0 .007 0.018 0.006 450.0000 2 . 779E+00 1 . 039E+01 1 .317E+01 7 . 293E+0

1

5.820E-01 4 . 349E+00 -0.006 0.017 0.005 500.0000 2 . 739E+00 1 . 1 59E+01 1 . 4 38E+0

1

7.656E+01 5.035E-01 4.539E+00 -0.006 0.016 0.005 550.0000 2 . 7 99E + 00 1 .279E+01 1 . 558E+0

1

7 . 990 E + 0

1

6 . 226 E-0

1

4.71 3E+00 -0.005 0.016 0.004

600.0000 2 . 307E+00 1 . 393E+0

1

1 . 67 9E + 01 8 . 299E+01 6 . 396E-0

1

4 . 873E+00 -0.004 0.015 0.004 700.0000 2 . 322E+00 1 . 6 38E+0

1

1 . 920E+01 8 . 856 E+0

1

6.637E-01 5.161 E+00 -0.004 0.014 0.003 300.0000 2 . 8 34E + 00 1 .879E+01 2.162E+01 9 . 346 E+0

1

6 . 923 E-0

1

5 .41 4E+00 -0.003 0.014 0 .003 900.0000 2 . 345E+00 2.11 9E+01 2.404E+01 9 . 735E+01 7 . 1 31 E-01 5 . 640E+00 -0.002 0.013 0 .002 1000.0000 2 . 355E+00 2.360E+01 2 . 646E+0

1

1 .013E+02 7.305E-01 5.843E+00 -0.002 0.013 0.002

168
POSITRONS IN WATER, LIQUID

I = 75.0 eV DENSITY = 1.000E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d(loq )/d(loqI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cn 2/g MeV cra 2/g MeV cm 2/g g/cra 2 0.0100 2 . 483E+0

1

2 . 204E-0 3 2 . 483E+0

1

2 . 250E-04 4 . 226E-05 0 .

0

-0.131 0.202 0.199 0.0125 2 . 077E+0

1

2.339E-03 2 . 0 78E+0 1 3.356E-04 5 . 394E-05 0.0 -0.174 0.194 0.191 0.0150 1 . 7 95E+0

1

2 . 450E-03 1 . 7 95E + 0

1

4 . 654E-04 6 . 570E-05 0.0 -0.169 0.183 0.184

0.0175 1 . 587E+0

1

2 . 544E-03 1 . 588E+0

1

6.138E-04 7 . 750E-05 0.0 -0.165 0.133 0.180 0.0200 1 . 427E+0

1

2.62SE-03 1 . 427E+0

1

7.802E-04 8.933E-05 0.0 -0.162 0.179 0 . 1 75 0.0250 1 . 1 96E+01 2.761E-03 1 . 1 96E+01 1 . 1 65E-03 1 . 1 30E-04 0.0 -0.157 0.172 0.170

0.0300 1 -036E+01 2.873E-03 1 .036E+01 1 .61 5E-03 1 . 365E-04 0.0 -0.153 0.167 0.165

0.0350 9. 185E+00 2. 971 E-03 9.1SSE+00 2. 129E-03 1 . 599E-04 0.0 -0.150 0.163 0.161

0 .0400 8 . 236E+00 3 . 060E-03 8 . 239E+00 2.703E-03 1 . 832E-04 0.0 -0.147 0.160 0.15S

0 .0450 7 . 574E+00 3.139E-03 7 . 577E+00 3 . 334E-03 2 . 064E-04 0.0 -0.145 0.157 0.156 0.0500 6 . 995E+00 3.209E-03 6 . 999E+00 4.022E-03 2 . 294E-04 0.0 -0.143 0.155 0 . 1 u3 0.0550 6 .51 6E+00 3.270E-03 6 . 5 i 9E+0 0 4 . 763E-03 2 . 522E-04 0.0 -0.142 0.155 0.151 0.0600 6.111 E+00 3.327E-03 6.11 4E+00 5.555E-03 2 . 747E-04 0.0 -0.140 0.151 0.150 0.0700 5.466E+00 3 . 428E-03 5.469E+00 7.288E-03 3. 1 92E-04 0.0 -0.138 0.148 0.147

0.0800 4 . 974E+00 3.521 E-03 4 . 978E+00 9 . 208E-0 3 3.627E-04 0.0 -0.136 0.146 0.145

0.0900 4 . 587E+00 3.607E-03 4.591 E+00 1 .130E-02 4 . 053E-04 0.0 -0.134 0.144 0.143

0.1000 4 . 274E+00 3.690E-03 4 . 278E+00 1 .356E-02 4 . 472E-04 0.0 -0.133 0.142 0.141 0.1250 3.704E+00 3 . 873E-0 3 3 . 708E+00 1 . 986E-02 5.489E-04 0.0 -0.130 0.139 0.137 0.1500 3 . 320E+00 4 . 065E-03 3 . 324E+00 2.700E-02 6 . 467E-04 0.0 -0.128 0.136 0.135 0.1750 3 . 044E+00 4.243E-03 3 . 049E+00 3 . 487E-02 7.412E-04 0 .

0

-0.126 0.134 0.133 0.2000 2 . 338E+00 4.423E-03 2 . 842E+00 4 . 33SE-02 8.323E-04 0.0 -0.124 0.132 0.131 0.2500 2.551 E+00 4.794E-03 2 . 555E+00 6 . 200E-02 1 . 01 OE-03 0.0 -0.122 0.129 0.128 0.3000 2 . 363E+00 5. 183E-03 2 . 368E+00 8.237E-02 1 . 180E-03 0.0 -0.120 0.127 0.126 0.3500 2 . 233E+00 5.588E-03 2 . 238E+00 1 .041E-01 1 -346E-03 0.0 -0.118 0.125 0.124

0.4000 2 . 1 38E+00 6.01 6E-03 2. 144E+00 1 . 270E-01 1 . 50 9E-03 0.0 -0.116 0.124 0.123

0.4500 2.068E+00 6 .468E-03 2. 074E+00 1 . 507E-01 1 . 671 E-03 0.0 -0.115 0.122 0.121 0.5000 2.01 4E+00 6 . 939E-03 2.021 E+00 1 .751E-01 1 .831 E-03 0.0 -0.113 0.121 0 . 1 20 0.5500 1 . 971 E+00 7.426E-03 1 . 979E+00 2.001E-01 1 . 991 E-03 1 . 1 03E-02 -0.095 0.119 0.117

0.6000 1 . 937E+00 7. 92SE-03 1 . 945E+00 2.256E-01 2. 1 52E-03 2 . 933E-02 -0.090 0.116 0.113 0.7000 1 . 886E+00 8. 979E-03 1 . 8 95E+0 0 2.778E-01 2.474E-03 7.435E-02 -0.080 0.110 0.106 0.3000 1 .851 E+00 1 . 0 0 9E-0 2 1 .861 E+00 3.31 0E-01 2 . 799E-03 1 .267E-01 -0.072 0.104 0.099

0 . 9000 1 . 827E+00 1 . 1 25E-02 1 . 839E+00 3.851E-01 3. 129E-03 1 . 835E-0

1

-0.065 0 .099 0.092

1 .0000 1 .81 OE+OO 1 . 245E-02 1 . 823E+00 4.398E-01 3.463E-03 2 . 428E-0

1

-0.060 0.095 0.087

1 .2500 1 . 786E+00 1 . 563E-02 1 .802E+00 5.778E-01 4.31 9E-03 3. 944E-01 -0.050 0.085 0.075

1 .5000 1 . 777E+00 1 . 904E-02 1 . 796E+00 7.169 ET— 0

1

5 . 204E-03 5.437E-01 -0.044 0.078 0.066

1 . 7500 1 . 775E+00 2 . 264E-02 1 . 7 97E+00 3.560E-01 6 . 1 1 7E-03 6 . 866E-0

1

-0.039 0.072 0.059

2.0000 1 . 776E+00 2 . 639E-02 1 . 803E+0 0 9. 949E-01 7 . 054E-03 8.218E-01 -0.036 0.067 0.054

2.5000 1 . 785E+00 3 . 429E-02 1 .81 9E+00 1 . 27 1 E+00 8 . 989E-03 1 .069E+00 -0.031 0.059 0.046

3.0000 1 . 796E+00 4.265E-02 1 .839E+00 1 . 545E+00 1 . 0 99E-0 2 1 . 238E+00 -0.028 0.054 0.040 3.5000 1 .308E+00 5.1 35E-02 1 .859E+00 1 . 8 1 5E+00 1 . 305E-02 1 . 484E+00 -0.026 0.050 0.037

4.0000 1 .81 9E+00 6 . 032E-02 1 . 879E+00 2 . 082E+00 1 .51 5E-02 1 . 660E+00 -0.024 0.047 0.034

4.5000 1 .830E+00 6 . 955E-02 1 . 399E+00 2 . 347E+00 1 . 729E-02 1 .821 E+00 -0.023 0.044 0.031 5.0000 1 . 340 E + 00 7.901E-02 1.91 9E+00 2.60 9E+00 1 . 945E-02 1 . 967E+00 -0.022 0.042 0.029

5.5000 1 . 849E+00 8.867E-02 1 . 938E + 00 2 . 868E+00 2. 163E-02 2. 1 02E+00 -0.022 0 .040 0.023

6.0000 1 .853E+00 9.350E-02 1 . 957E+00 3. 125E+00 2 . 383E-02 2 . 227E+00 -0.021 0.038 0.027

7.0000 1 .875E+00 1 . 135E-01 1 . 993E + 00 3.631 E+00 2 . 827E-02 2 . 453E+00 -0.020 0.036 0.025

8.0000 1 .889E+00 1 .391 E— 0

1

2 . 028E+00 4. 129E+00 3 . 274E-02 2 . 652E+00 -0.019 0.034 0.023

9.0000 1 . 902E+00 1 .601E-01 2 . 062E+00 4.61 7E+00 3 . 722E-02 2 .831 E+00 -0.019 0.032 0.022

10.0000 1 . 91 4E+00 1 .814E-01 2 . 0 95E+00 5 . 0 98E + 00 4.171E-02 2 . 992E+00 -0.018 0.030 0.021 12.5000 1 . 939E+00 2.362E-01 2. 175E+00 6.269E+00 5 . 290E-02 3.341 E+00 -0.017 0.028 0.019

15.0000 1 . 959E+00 2. 926E-01 2 . 252E+00 7 . 399E+00 6 . 397E-02 3 . 633E+00 -0.015 0 .026 0.017

17.5000 1 . 976E+00 3.501 E-01 2 . 327E+00 8.491 E+00 7 . 487E-02 3 . 3S5E+0 0 -0.014 0.024 0.016 20.0000 1 . 991 E+00 4 . 03SE-0

1

2 . 400E+00 9 . 549E+00 3 . 557E-02 4 . 1 07E+00 -0.013 0.023 0.015 25.0000 2.01 5E+00 5.277E-01 2 . 542E+00 1 . 157E+0

1

1 .063E-01 4 . 487E+00 -0.011 0.020 0.013 30.0000 2 . 0 34E+0 0 6 .489E-01 2 . 683E+00 1 . 349E+0

1

1.261 E-0

1

4 . 80 6 E+0 0 -0.009 0.018 0.011 35.0000 2 . 049E+00 7.716E-01 2 .821 E+00 1 . 530E+0

1

1 . 449E-01 5 . 082E+00 -0.007 0.017 0.010 40.0000 2 . 062E+00 8. 955E-01 2. 958E+00 1 . 703E+0

1

1 . 628E-01 5 . 326 E+00 -0 .006 0.016 0.009

45.0000 2 . 074E+00 1 .021 E+00 3 . 094E+00 1 .869E+01 1 . 7 9 9 E - 0

1

5 . 544E+00 -0.005 0.015 0.008 50.0000 2 . 084E+00 1 . 1 46E + 00 3.230E+00 2. 027E+01 1 . 962E-01 5 . 74 1 E+00 -0.004 0.014 0.007

55 .0000 2.093E+00 1 . 273E+00 3 . 366E+00 2.179E+01 2.11 7E-01 5 . 921 E+00 -0.004 0.013 0.006 60.0000 2. 1 01 E+00 1 . 400E+00 3 . 50 1 E+00 2 . 324E+0

1

2 . 265E-0

1

6 . 087E+00 -0.003 0.012 0.006 70.0000 2.11 5E+00 1 . 656E+00 3.771 E+00 2.599E+01 2.541 E-01 6 . 333E+00 -0.003 0.011 0 .005 80.0000 2 . 1 27E+00 1 . 91 4E + 00 4.041 E+00 2 . 855E+0

1

2.794E-01 6 .641 E+00 -0.002 0.010 0.004

90.0000 2. 1 37E+00 2. 1 73E+00 4.31 1E+00 3.095E+01 3.028E-01 6.371 E+00 -0.002 0.010 0.004

100.0000 2. 147E+00 2 . 434E+00 4 . 530E+00 3 . 320E+0

1

3 . 243E-0

1

7 . 077E+00 -0.001 0.009 0.003 125.0000 2. 1 66E+00 3 . 089E+00 5 . 255E+00 3.329E+01 3.716E-01 7.51 6E+00 -0.001 0.003 0.002 150.0000 2. 182E+00 3 . 749E+00 5 . 931 E+00 4 . 277E+0

1

4.11 5E-01 7 . 876 E + 00 -0.001 0.007 0.002

175.0000 2.1 95E+00 4.41 2E+00 6 . 608E+00 4.676E+01 4.456E-01 3 . 182E+00 -0.001 0.007 0.002 200.0000 2 . 207E+00 5 . 073E+00 7 . 285E+00 5.036E+01 4.753E-01 8 . 447E+00 -0 .000 0.006 0.001

250 .0000 2 . 226E+00 6.416E+00 8 . 642E+00 5 . 6S5E+0

1

5.244E-01 8 .891 E+00 -0.000 0.005 0.00! 300.0000 2 . 242E+00 7 . 7 6 0 E + 00 1 . OOOE+O

1

6 . 20 3E+0

1

5.S37E-01 9 . 254E+00 -0.000 0.005 0.001 350.0000 2 . 255E+00 9. 107E+00 1 . 1 36E+01 6 . 672E+01 5.959E-01 9.551 E+00 -0.000 0.005 0.001 400.0000 2 . 266E+00 1 . 046E+01 1 . 273E+0

1

7 . 037E+01 6 . 229E-0

1

9 . 327E+00 -0.000 0.004 0.001 450.0000 2 . 276E+00 1 .181E+01 1 .409E+01 7 . 460E+0

1

6 . 460E-01 1 . 006E+0

1

-0.000 0.004 0.001 500.0000 2 . 2S5E+00 1 .317E+01 1 . 545E+0

1

7 . 799E+01 6.S59E-01 1 . 027E+0

1

-0.000 0 . 0C4 0.000 550.0000 2 . 294E+00 1 . 453E+01 1 . 632E+01 8.109E+01 6 . 834E-0

1

1 . 046E+01 -0.000 0.004 0.000 600.0000 2.301 E+00 1 . 5S9E+0

1

1 .81 9E+01 8 . 3S5E+01 6 . 933E-01 1 . 064E+0

1

-0.000 0.004 0.000 700.0000 2.31 4E+00 1 .861E+01 2.092E+01 3 . 907E+0

1

7 . 250E-0

1

1 . 0 94E+0

1

-0.000 0.003 0.000 800.0000 2 . 326 E+0 0 2.1 33E+01 2 . 366E+0

1

9 . 356E+0

1

7 . 463E-0

1

1.121 E+0

1

-0.000 0.003 0.000 900.0000 2 . 336E+00 2 . 406E+0

1

2 . 640E+0

1

9 . 756E+0

1

7.641 E-0

1

1 . 1 45E+01 -0.000 0.003 0.000 1000.0000 2 . 345E+00 2 . 679E+0

1

2.914E+01 1 .012E+02 7.793E-01 1 . 1 66E+0

1

-0.000 0.003 0.000

169
U.S. DEPT. OF COMM.

BIBLIOGRAPHIC DATA

SHEET (See instructions)

1. PUBLICATION OR

REPORT NO.

NBSIR 82-2550-A

2. Performing Organ. Report No.l 3. Publi

4. TITLE AND SUBTITLE

cation Date

December 1982

STOPPING POWERS AND RANGES OF ELECTRONS AND POSITRONS (2nd Ed.)

5. AUTHOR(S)

Martin J. Berger and Stephen M. Seltzer

6. PERFORMING ORGANIZATION (If joint or other than NBS. see in struction s) 7. Contract/Grant No. NATIONAL BUREAU OF STANDARDS

DEPARTMENT OF COMMERCE 8. Type of Report & Period Covered

WASHINGTON, D.C. 20234

9. SPONSORING ORGANI ZATION _NAME AND COMPLETE ADDRESS (Street. City. State. ZIP)

U.S. Dept, of Energy Office of Naval Research

Washington, D.C. Arlington, VA 22217

10. SUPPLEMENTARY NOTES ~

[ | Document describes a computer program; SF-185, FIPS Software Summary, is attached.

11. ABSTRACT (A 200-word or less factual summary of most significant information. If document includes a significant

bibliography or literature survey, mention it here)

Tables of stopping powers and related data are given for electrons in 25 elements

and 46 mixtures and compounds, and for positrons in 14 materials. The tables include:

(1) collision stopping powers (ionization and excitation losses); (2) radiative

stopping powers (bremsstrahl ung losses); (3) total stopping powers; (4) ranges

(rectified pathlengths computed in the continuous-slowing-down approximation);

(5)' radiation yields (fraction of initial electron energy converted to bremsstrahl ung

in the course of slowing down); and (6) the logarithmic derivatives of all these

quantities with respect to the mean excitation energy of the medium (the key parameter

of the Bethe stopping power formula). The results are tabulated at 81 energies

between 1000 MeV and 10 keV. Collision stopping powers for electrons in materials of

low atomic number are given also for energies down to 1 keV. The principal new ingredients in the preparation of the tables are: (1) improved values of the mean excitation energies for elements and compounds, derived from stopping-power and range

measurements and from semi-empirical oscillator-strength distributions and dielectricresponse functions; (2) density-effect corrections evaluated according to the method

of Sternheimer, using up-to-date input parameters; and (3) use of new theoretical

cross sections of Pratt and Tseng for electron-nucleus bremsstrahl ung and of Haug for

el ectron-el ectron bremsstrahl ung

.

12.

K.EY. WORDS (Six to twelve entries; alphabetical order; capitalize only proper names; and separate key words by semicolons)

collision stopping power; electrons; positrons; radiation yield; radiative stopping

power; range.

13.

AVAILABILITY

|X. [ Uni imited

14. NO. OF

PRINTED PAGES

j I For Official Distribution. Do Not Release to NTIS 173

| | Order From Superintendent of Documents, U.S. Government Printing Office, Washington, D.C.

20402. 15. Price

Order From National Technical Information Service (NTIS), Springfield, VA. 22161 $ 15 .00

USCOMM-OC 6043-P80
a