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NBSIR 82-2550

Stopping Powers and Ranges of

Electrons and Positrons

U.S. DEPARTMENT OF COMMERCE

National Bureau of Standards

Washington, DC 20234

August 1 982

Prepared for: Office of Standard Reference Data

National Bureau of Standards

Washington, DC 20234

Office of Health and Environmental Research

Department of Energy

Washington, DC 20545

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NBSIR 82-2550

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Stopping Powers and Ranges of

Electrons and Positrons

U.S. DEPARTMENT OF COMMERCE

National Bureau of Standards

Washington, DC 20234

August 1982

Prepared for: Office of Standard Reference Data

National Bureau of Standards

Washington, DC 20234

Office of Health and Environmental Research

Department of Energy

Washington, DC 20545

Office of Naval Research

Arlington, Virginia 22217

NBSIR 82-2550

Stopping Powers and Ranges of

Electrons and Positrons

M. J. Berger and S. M. Seltzer

U.S. DEPARTMENT OF COMMERCE

National Bureau of Standards

Washington, DC 20234

August 1 982

Prepared for: Office of Standard Reference Data

National Bureau of Standards

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
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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 8 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) densityeffect 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, and J. E. Turner. Consultants to

the committee are S. M. Seltzer and R. M. Sternheimer. 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.

TABLE OF CONTENTS

ABSTRACT

1.

INTRODUCTION

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 7 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. General equations

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

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 29

TABLES TO ACCOMPANY TEXT 41

FIGURES 66

MAIN STOPPING-POWER AND RANGE TABLES 79

11

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. ^ 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.^ 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.^ 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

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

heavy charged particles in a future report.

^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.

^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 radiobiology

(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

ah 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-effeet 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 et al

(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,

1963, 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-effect correction has been re-evaluated according to the

dispersion model of Sternheimer (1952). Rather than using Sternheimer ' s earlier

results or the universal fit given by Sternheimer and Peierls (1971), we have

evaluated the density effect using as input the mean excitation energies adopted in

this report and values of the binding energies for atomic subshells from Carlson

(1975) .

2
(£) The radiative stopping power 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. (iii) 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 bremsstrahlung in the field of the atomic electrons was taken into account according to the theory of Haug (1975) augmented by a screening

correction.

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, e.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"^^ ^ ("dE/dx) or S^qI- We shall find it convenient to consider also the

corresponding mass collision stopping power, Spnl/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 Sf-Qi in MeV/cm and p in g/cm^, Sroi/p has units of

MeV/ (g/cm^ )

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

particle to bound atomic electrons. We denote by do/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^Z/A, represents the number of atomic electrons per gram of

the medium. = 6.022045 x 10^^ mol ^ 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-power 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) W,- 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

- S T p col

N Z a

( 2 . 1 ) A

- S T p col ( 2 . 2 )

The main result of the Bethe theory, applicable to electrons and heavy charged

particles, is that

- S , (W < W ) p col'' C-’

2mc^ 3^ W^

(1 - 3 ^) 1 ^

2 (2.3)

3

1
where is Avogadro's number, Vq is the classical electron radius, mc^ is the

electron rest energy, 3 is the velocity o£ 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)

ZTTN^r^mc^ = (2^) (6.022045 x lO^^mol"^) (7.940775 x 10‘^^cm^) (0.5110034 MeV)

3 0

= 0.153536 MeV cm^ mol"^

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/1376) « 1. The stopping-power component due to

close collisions is evaluated as if the atomic electrons were free and at rest:

- S (W > W ) p col ^ c^= N

a A

-W

Iw

w

da

aw

dW (2.4)

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

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

is the largest possible energy transfer, with t 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

. 2mc^ 3^

W = 2t(t + 2) mc^ =

y

. (2.6) 1-3

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

27Tr^mc^ «dW ^ da = (I - 3

^ w/W ) 3 ^

(2.7)

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

« 2 2

, 47TNrmc„-, 1 c _ a e Z 2 p col q2 a2 me

2 .2

^n

(1 - 3^)1

- 3‘

( 2 . 8 )

As expected for a consistent treatment, the quantity W(~ 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,** 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

a A z\(B) (2.9)

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

three terms.

L(3) L + zL, + o 1

( 2 . 10 )

The first term.

( 2 . 11 )

adds to Eq (2.8) a shell correction, C/Z, and a dens ity- 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^ 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 at. (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, 1973j 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 at., as given by them in terms of a numerical function F which is defined such that

zL

1

7 3

z Za —^ F(ba/Z/3)

3

( 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^Lz in Eq (2.10) is contained in an extension o£ 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

= ijj(l) - Re ip(l + 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

00 E

n=l

r . 2 ^ 2. -1

[n(n + y )] (2.14)

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

of z^La can be shown to approach - 0.577 - <in 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.

do

2tt dW

1 + W

(T-W)

2 T

(t+1)^

(2t^) ^

(x.l)2 (T-W) (2.15)

where t = T/mc^ is the kinetic energy of the incident electron in units of its rest

mass. The Miller cross section, valid when 1373 » 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 W^, while equal to T according to Eq (2.5), is therefore

taken to be equal to T/2. With the Miller 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):

, 271 N r me „ ^ i ^col

" A

[^^(T/I) + ^n(l + t/2) + F'(t) - 6] , (2.16)

3 where

F'(t) = (1-3^) [1 + t^/8 - (2t+ 1) ^n 2] . (2.17)

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

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

protons in Eq (2.9).^ For positrons, energy transfers larger than W^. 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 Wj„ = T. The mass collision stopping-power formula for positrons is similar to that for electrons,

except that F" is replaced by

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

6
F""(t) = 2% 2 - (3^/12) [23 + 14/(t + 2) + 10/(t + 2)^ + 4/(t + 2)^] (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 ~ 0.31 for H 2 O, ~ 0.7% for , ~ 1.3%

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

are ~ 2% for H 2 O, ~ 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, ~ 7% 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 ^S^qI be the uncertainty of

Scol corresponding to an uncertainty Al of I. From Eq (2.16) it can be seen that

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

^Scpl/Scol (^I/I)/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^-Q^/Sj-Ql)/ (dl/I) 3.5 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-effect 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
00 00

Jin I I (3.1)

d£

JE £nE dEI

d£

3e dE 9

where d£/dE is the density o£ optical dipole oscillator strength per unit energy o£

excitation above the ground state.

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

£ree atoms, systematic calculations o£ oscillator- strength distributions and I-values,

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

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

have been continued by Inokuti et al

(1981) £or Z up to 38. Critical evaluations

o£ experimental oscillator- strength distributions £or atomic and molecular gases,

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

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

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

makes use o£ the moments M(n) = / d£/dE E^dE o£ the oscillator- strength distribution (Dalgarno, 1960). Noting that dE^/dn = E^^nE, one can trans£orm Eq (3.1) into

Jin I 1 fdM(n)l

MX^ L dn J (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 £rom experimental polarizability data. By £itting these moments, an analytical £unction M(n) is obtained

which is then di££erentiated to get £nl.

I-values £or 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 o£ Table V in Dehmer et al

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

derived with the use o£ semi-empirical oscillator- strength distributions.

The values o£ the ratio I/Z obtained in the systematic calculations o£

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 £ound when I-values are calculated on the basis o£ the local-plasma approximation o£

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

obtained £rom the equation

00

Jlnl = (1/Z) J 4it r^ ^ri(Y ^ (^q) di" > (3.3)

*0

where

0)^ = (4tt e^ n^(r)/m)"^ (3.4)

is the plasma £requency corresponding to a electron density ng(r) at a distance r £rom the nucleus, h is Planck's constant divided by 2-n

and y is a £ree parameter

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

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

= <6(E - Y w^(r))> , (3.5)

where the brackets denote the ground state expectation value and 6 is a delta

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

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

£rom Hartree-Slater wave £unctions. Ziegler has also extended the calculations to

solids, using solid-state wave £unctions.

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

et al .

and by Inokuti et al . y 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

“ 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 (w) of the medium (Fano, 1956, 1963):

ilnl do) 03 Im[- 1/e (o3) ] £n (ho3 ) (3.6)

where oa P is the plasma frequency. The corresponding plasma energy® is

ho) = ( 47t n /m)'^ = 28 . 816 (pZ/A)^ eV , P ®

(3.7)

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

the electron.

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

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

real and imaginary parts, n(o)) and k(o3), of the refractive index:

e (o)) = n^ (oj) - (o))

I (3.8)

62 (

03 ) = 2 n(o)) k(o))

j

It is therefore possible to obtain e (03) 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):

ilnl > (3.9)

®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

X =

62 zL, (3.10)

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

Barkas correction, and Bloch correction.

Let ASqoI denote the uncertainty of the measured value of SqqIj 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

AI = I • [(AS ,/S ,)^ + (Ax)^]^ (3.11)

where Lgxp 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 Cj(, Cp , from the different atomic shells. Theoretical

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

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

Cj^j (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 Cjq 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, Cl(9l,t?l), depends on

the atomic number through the parameter 9 l and on the particle energy through the

quantity

= (B/aZ )^ (3.12)

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

correction is calculated from the scaling relation

(3.13)

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

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

N shell and for a combined 0-P shell.'

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

V£ as defined above and Hp = 1 . For low atomic numbers, the effective charge Z for the L shell has in this work been set equal to Z - d, with values of d

taken from Clement! and Raimondi (1963)

For Z=3 ,4 ,5 ,6 ,7 ,8 ,9. ,10

d = 1.72 , 2.09 , 2.48 , 2.82 , 3.16 , 3.53 , 3.84 , 4.24 .

10
The scaling parameters (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 Hj^'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

vs. 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.®

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 at. (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^ 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 1-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 to

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.®

®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.

®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 Segrfe (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 Segrfe, 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 , O 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 1^(2), experimental values by I(Z) and

interpolated values by Iint(^)» have assumed that

I. ^(Z) = I (Z) int^ ^ ' I(Z^) Z

2

- Z KZ 2

) Z

I (Z.) Z^ - Z-, I (Z-,) z, - z. c^l-^ 2 1 2

-' 2 1

(4.1)

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

bracket the atomic number Z of interest. Either Z, Zi, and Z 2 pertain to

gases, in which case the required values of I(^ are taken from the results of Chu

and Powers (1972) obtained with free-atom wave functions, or Z, Zi, and I 2 pertain to solids in which case the values of I(- 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(-(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-values 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.^” 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 Bichsel and Porter (1982), pertains to protons and alpha

particles in Na and O 2 . Figure 4.3 pertains to proton stopping power at energies up

to 20 MeV in A£, Cu, kg, 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.

5. SELECTION OF MEAN EXCITATION ENERGIES FOR COMPOUNDS

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

I-values for many gases have been determined by Zeiss et al. (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 al. (1978), Ashley (1979) and Painter et al

(1980) from

dielectric data. I-values for a large number 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 (1954) 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

takes the form

- S n = L w- - S T p col ^ J p col

J

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

Scol/P> the additivity rule

, (5.1)

^ “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, we 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.

13
Z/A = E w. (Z./A.) , (5.2)

£nl = E w.(Z./A.)£nlj|/,

L 3 <Z/A> (5.3)

6 = E w.(Z./A-)<5-

L j

j J r 3 <Z/A> (5.4)

where Zj , Aj , I j , and 6j pertain to the j ' th constituent. It should be noted

that <Z/A> IS equal to the total number o£ 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.^^ 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 AJI 2 O 3 , SiOa , and photographic emulsion, and is also consistent with

the less certain experimental data for LiF and CaFa. 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^^ 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.

^ ^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.

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

15
6. DENSITY EFFECT

6.1. General equations . The passage o£ 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 (w) of the medium:

oo

6 = (2/uw ^) /

CO do) Im[- 1/e (cj) ] iln(l + £^/(o^) - (£/(o )^ (1 - 6^) , (6.1)

P *n P

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

given by^Eq (3.7). The quantity I is defined, as a function of 6, as the root of

the equation

1 - e (is,) = 0 . (6.2)

It can be shown that in the limit B 1

6 -V £n[(htOp)^/(l - B^)I^] - 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 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 B- 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 Bo ~ ^(o)'^> which is a property of the material, and

there is no density effect for B < Bq

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 [F.2) as follows. In Eq (6.1) one sets e =1/(1 - a^)

where

a. (o)) = (hm )^ I: (6.4)

^ n=l Ej^p - (km) - iy^

16
is the longitudinal polarizability expressed in terms o£ the energy levels of

single atoms and the corresponding oscillator strengths fnL* limit in which

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

6 N

n=l

(hio'/E^L] (£/o)p)2 (1 - (6.5)

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

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

EnT, oscillator strengths fnT> damping term yy. In the limit yy ^ 0,

Eq (6.2) is then transformed into

Urp (i£) (ho)p)

N

E

n=l E

nT

nT

(hil)

( 6 . 6 )

The following approximations are now made:

a. The distinction between the longitudinal and transverse oscillator

strengths f^y and f^y is disregarded, and both are approximated by fj^, the

fraction of electrons in the n'th atomic shell.

b. The energy levels are assumed to be

^nT ^St ^n

"nL = t^St e; ^ 1

(6.7)

( 6 . 8 )

where the Ej^ ' s are atomic energy levels. The quantity y 5 -t is the Sternheimer

factor and is given a value such that the equation

n=l ^ (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 6 calculated according to Eq (6.5) goes into the correct asymptotic limit, Eq (6.3),

for very high particle energies. The values of ygy 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 Ejyj is set equal to zero. This has the consequence that Eq (6.6) has a solution for arbitrarily small

values of 3. For insulators, on the other hand, Eq (6.6) has a solution only for

velocities greater than Bq given by

1 N f^

^ ^ ^

7^ ^ ^St

( 6 . 10 )

As a final refinement, which makes little difference except for liquid H 2 , a Lorentz-Lorenz correction is applied (Sternheimer, 1952), through the replacement of

fn(^‘‘^p)^ in Eqs (6.8) and (6.9) by fn(f>Wp)^, where Aj^j = 1 for conductors, and

Aj^ = 2/3 in all other cases.

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

y 5 t, then Eq (6.6) for £ as" a function of B, 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. 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.^**

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^, whereas

the bulk density may range from 1.5 to 1.9 g/cm^, depending on the method by

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

1.7 to 1.8 g/cm^. 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^,- 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^)

and silver halides (82.6% by weight, average density 6.47 g/cm^) . 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^; 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%.

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

^“*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)/S(^oi (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 Wj,^ in the integral in Eq (2.4) by A. The results for electrons and positrons (indicated by superscripts - and + ) are:

1P L-(T,A)

9 M 2 2

2tt N„ r me

a e ZJ

[£n(T/I)" + £n(l + x/2) + G"(T,n) <5] (7.1)

Equation (7.1) is similar to Eq (2.16), and the various symbols have the same meaning, except that the functions F±(t) are replaced by G-(T,n). For electrons,

G‘(T,n) = -1-3^ + £n[4(l - n)n] + (1 - n)'^

+ (1 - 3^)[T^n^/2 + (2t + 1) £n(l - n)] (7.2)

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

c (T,n) = Jin 4n - 3^[1 (2 - u^) n (3 + u^)(ux/2)

+ (1 + ux) (u^x^/3) - (u^x^/4) n^] , (7.3)

where u = (x + 2) ^

. We note that G (x,l/2) = F (x) and that G^(x,l) = F'*^(x), so that L'(T,T/2) = (T) and L (T,T) = S^^^(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 A£ 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, A.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,co) that depends on the momentum transfer hK and

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

integral, with respect to K and to, over the quantity (m/K) Im [ - 1/e (K, to) ]

. 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,m).^^ It was still necessary, however, to obtain

e(K,co) 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

^^e(o,m) 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 at.

(1975) for kl and A£ 203 ; Ashley et al. (1976a) and Tung et al. (1979) for kl

Si, Ni,

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

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

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

various organic solids, Ashley and Anderson (1981) for SiOa; 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),^® curve 2 is from Green,

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 101 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^^

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^^ for N 2 , O 2 , Ar, and CO 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 Griin (1957)

and in nitrogen by Cohn and Caledonia (1970).

^ ^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.

* ’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 o£ 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^®

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 x>s. 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. 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.

^®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

1

P (T) =

f

da^

dk dk + Z

•'/-V

da^

3F dk (9.1)

where da^/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 dog/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' = mc^ T[T + 2mc^ - 6(T + mc^)]'^ . (9.2)

It is convenient to introduce dimensionless, scaled, radiative energy-loss cross sections

o and

a/E)^dk , (9.4J

2 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

-a 2 „ o E [l (1/Z) (9.5)

The ratio 411/4 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.^®

For compounds we assume that additivity is a good approximation, and set

- S ^ (T) = X) w. — S . • (T)

p rad^ j p- rad,j ^ ^ (9.6)

where w^ is the fraction by weight of the j ' th constituent.

^ ^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. Electron-nucleus bremsstrahlung

9.1.1. High-energy region . For T > 50 MeV, the bremsstrahlung cross section

was evaluated from the analytical expressions o£ 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

k

^ = 4arJ g.(E,10

“i ^ h. (q) [l-F(q,Z)]^ dq - f(Z) (9.7)

where q is the momentum transfer and

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) = (aZ)^ E [n(n^ + Z^)]'^

n=l

(9.9)

The other quantities in Eq (9.7) are defined as follows;

g^ = 1 + (E - k)VE^ g2

= - 2(E - k)/3E

ei = 1

= (q - q^)^/q^

02 = 5/6 (9.10)

^2

3 2 q

- 6q^ q £n(q/q^)

+ 3q^ q

- 4q^ /q^

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 al

(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 al.

(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 al

(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 al. (1977) through elaborate interpolation procedures. A few

24
exploratory calculations, for 5- and 10-MeV electrons in Ail 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 and have derived values for 1 = 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 '^>rad^^^ ^ S^P ^^gion 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:

4ar^ [g^(E,k) + g 2 (E,k)] [£n(l/q^) - 1/2] (9.11)

where gi, gz, and qQ 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):

7 2 r 1

WwL 4ar^ g.(E,k) fif + / h.(q) S(q,Z) dq

L ^0 J

It can be seen that this equation can be obtained from Eq (9.7) by setting Z = 1 and replacing [1 - F(q,Z)]^ 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 as initial approximation, we have assumed that the

electron-electron differential bremsstrahlung cross section is

(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
9.2.2. Low-energy region . For T < 2 MeV, we have assumed that

dk k dk £„ k

E

do

( dk BHSR

(9.14)

where (dOg/dk)pjg is again Haug ' s cross section with exchange and no screening, and

where (dog/dk) is the cross section without screening derived by Bethe and

Heitler (1934), Sauter (1934), and Racah (1934) in the Born approximation but without

invoking the high-energy approximation. The so-called Elwert factor

£g = 3[1 - exp(- 2TTaZ/B)] / B'[l - exp(- 2TraZ/3')] (9.15)

which depends on the electron velocities 3 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 . (n) for T > 50 MeV, the quantity rad (T)

With (j)

1 + (1/Z)

(®1 determined for

^Jad

T < 2 MeV and was obtained in

the gap region, 2 to 50 MeV, by the same interpolation procedure previously used in

Section 9.1.3 for 'f’rad^^^* This completed the evaluation of (T) and of the rad ^ total radiative stopping power according to Eq (9.5).

The ratio 4>ra^ ^T) (T) 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 at. (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^° (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).^^

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 the transition region between 2 MeV and 50 MeV we expect our interpolated

results to have an accuracy of 3-5 percent.

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

^°Also private communication from D. Rester (1967).

^ ^Rester and Edmonson (1972) suggest that an incomplete background correction in the

experiment of Motz accounts for this discrepancy.

26
r (T ^ T.)

o ' o

£' X ( 10 . 1 )

I ° (S„i(T) . S^^,(T)]-l dT .

and represents the average pathlength^^ traveled by an electron as it slows down

from an initial energy Tq to a final energy Tp. The choice of Tp 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 Tp equal to the lowest atomic

ionization potential.

The stopping powers needed for the evaluation of Vq from Eq (10.1) are available from the Bethe theory only down to some intermediate energy Tp, and the part

of the integral from T = Tp to Tp 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;pg^j(T)]"^ is zero at T = 0 and can be interpolated linearly to its

value at T = Tp. The range is then given by

Tf) ’i) P[Scol(Tp) + S rad (T.)]

-1 /' (T/T.) 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 Tp = 1 keV

and Tp = 0.

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

^^ 0(^0 0) from Eq (10.2), for initial energies Tq = 10 keV, actually are quite

close numerically to the more accurate ranges calculated with a final energy

T^ s 10 eV.

The radiation yield (also called bremsstrahlung efficiency) is the fraction of

the initial energy Tq 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 ) (10.3)

In the evaluation of this expression one is again faced with the difficulty that

neither S^op nor S;ra.d is known accurately below an intermediate energy Tp = 1 keV.

We have made the assumption that (SqqI + Sj.a,d)

' ^ is zero at T = 0 and

increases linearly to its value at T = Tp.

11. MISCELLANEOUS COMPARISONS

11.1 Positron-electron differences . For the collision stopping power and

range, differences arise because of the use of the Bhabha cross section instead of

the Miller cross sections for large energy transfers. Table 11.1 shows ratios of

positron stopping powers to electron stopping powers, and ratios of positron ranges

^^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 T£ = 12.6 eV is ~ 1 percent

greater than r^(T^ T^) for T^ > 10 keV.

27
to electron ranges, for a representative set of materials. Table 11.2 gives the

ratio of the restricted collision stopping power for positrons to that for electrons

in water.

In our tabulations, the radiative stopping power for positrons has been assumed

to be the same as that for electrons, which is a good approximation at energies

above, say, 10 MeV. However, it should be mentioned that exploratory calculations by

Feng et at. (1981), employing the same method as that previously used by them for

electrons, indicate significant differences between positrons and electrons in regard

to the differential bremsstrahlung cross sections in oxygen and uranium at 500, 50,

and 10 keV.

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 kl) 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 at.

(1959) and Ishigure et al

(1978) in aluminum and by Ziemer et at. (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).

^^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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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.

O

O)

• CVJ «4- «4- ^ S.

I O O O » S- 4- (/) 00

» O O O O00 I— f—

i >>o ta tc

> U U <J

• Or-«i-*i-

. 0) fO U V.

• ^ U

L-t-> ‘f- CL Q.

4-> E E

> -M Oj OJ 01 C L. I I

: E <U E E

» o ^ a; (u

» E CO t/>

O O fd OO 00 .13 ^ O O S- i- 3 3

r- I— +-) 4->

•I- T- C C

Q. Q.4>» O O

E E -r- -r- . 01 0) 4-» •!-> < II fO fO E E C C C

O) rd <d

t/> i/1 :e > >

1/1 OO >oO >»o

L. L. o »— o •—

0) <d (U /d x: u jc o

4. 4^ OJ 4-> OJ c s. c u —^ Q> o o> o

C E O) E 0^ x: o ^ 4-> E

o o o a I— OO OO r—

<d O o <d

(d id

•#“ o U -I- Q.*r- •!- Q. E -M E

01 OJ Oi 0^

I fc. u I •r- O O

E 0» O) E

O) ^ ^ 0>

00o o o OO OO r— O O id U U T-

•f- »f- Q.

4^ 4-> E

OJ 01 0)

I- &. I 0 0 *

1“

0> o» £ ^ ^ <u

-*-> 4-> U)

OO

id O XI OO o &. o O 3

I— CO rid O >>>>&. id 0 &. 0) U

I— O O Qu*fL. id 0) O • &. U £ C »r-

> Q.<r- 4-> 4-> O O.

' E E

. 0> 0) 4-> 4-> <4-> 01

1 u c c id I *r* O 0/ 0J»^*»-

: E 01 E E s. E

Q> ^ Q O id 01

: </) E E > </i

t/i O o00 r— >>o id u u

O ^ *f- 0> id w ^ o •*-

4-» 4-> •*- Q.

-- 4-» E i«. 4^ 01 0) ^ C W I Oi O *«- C E o; £

Q f 0>

0> id <u ^r- >- C'

id 5 c iO O 03 o I VO ez u i 01 *0 id OQ ( #— c —" id C4- T3C

id I- o id

•r- o -c O •*-» 01T5 . i-UCiid Id O O ^ U- (

id jO un LT> to VO oi Ol

o c c

4->^ 0- 0.

(/) O id id o>vo oi C Ol r- #—

id id Q

VO

VO OI 0> r-

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CO 4-> I—

S- ^ id ' id ov-^ >- o» c »— • VO r— id r>* "O VO id _j oi c a

Oi O id •o^ 44 c

L. id s. id id id idc Id a> c»“

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O) id xr x:

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01 *r- . u •— a> 3

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id <L) id o O CD >- 2: .

LT) iO OI

oi

r*N. r«4 • 44 0> a

0) r- CJ 44 O 0) 44 C <U

S. U

id <U i/> C7> 3 E 1/1 CO x: -f- id U 0/ o Q S Q r>i

in VO

VO VO oi cn

tr> itj oi ns. I— oi

fss. ts4 • OI a

r- <3

0) u ^

•I- <D t/» 3 E 1/1 0 ^*1- U <D 0) 2: Q r>si

OI o>»—

»— r— r>. id id OI

Q Q r—

0 CM

rss rs.—

01 oi cn r— r— rs. s-^^Ol

<+- cil s—

H. 0/ O 4-> • X= id ts4 Oi>- o

•— f— o (U 0/ u

CD CD s

""O id i C 'I- u

» id 3' O E • OI ^ id

0) 0> E 4-> C

Id id x: >- -J OO

O E X x:

id a> OO a

LT> pss. VO oi

OI I—

OI r*s. O 0) Ol C 44 •—

u. id

r— "o OI

Id c o •— O id +i •0 4-^ 1- C 0>

id O I- 44 .C 0/ u

r— C7> E id I— C -C o>

o) id a> OI

CO ^ O LU

uo

VOOI

OI • r“ ts4 id Cj

VO

COo

vn VO r>. CM CM CM

CD! CO CO CTi Ol OI O r— I— CO I— C71 CO O 00

VO CM

cn CO

41
Table

3.3

Shell

correction

C/Z,

Barkas

correction

z

L^,

Bloch

correction

Table

3.4

Bichsel's

formulas

for

evaluating

the

parameters

and

in

Eq

(3.13

z2l

2>

and

total

correction

x

-

(C/Z)tot

-z

L]

-

z2l

2,

evaluated

Also

given

isa

list

of

values

of

the

parameter

b

in

the

Ashley-Ritchieat

various

proton

energies

with

the

computer

program

of

Bichsel.

L

is

the

stopping

number

per

electron

computed

with

these

corrections.

Brandt

theory

of

the

Barkas

correction

(see

Eq

(2.12)).

o'd’ V

rsj

o

V'Vo

tno

o

A

i.O

okO

tvi

okOA

r*«4

COA

rsi

CM

roA

IM

O

rsi

o

II

M

CO CM

rM ^

V • O fNl

CMCOVM

CM

kO

CM

I

rsi \CM

ir>

ro X

D

O

Q.

kO 00 O r—

k£> O m CO ^ ro ro

O r>. m o CM »— I— CM u) at

I— r— ^ r*N. LD oo

Lf) O O O CM o o o I I

ot at ^ •d’ CM "d" m CO

CM f— at o I— O O kO o o o f—

I

o in ^ r*N. 'd' kO

«d- r— CO kO "d- kO at

fo f— VO iT) o r— m O O CM O O CM VO O O O O O O CM

I I

r— o «d- VO

CM lO CM

CM ^ CO ro O O CM o

o o o o

VO -d- CM

CM rs. ro o o rs. O CM CM O O ro

I

r««* o m 'd’ CM ot 00 at

r— ir> Ot o o •— o

o o o o

VOo

o

r«. o00doOt

CO

ro

ot

<c O «d- O O ^ ^ m I

kO O 00 l— 0 O CM f— o o o o

ot ^ «d- CO «d- r— r>. ro O *— O

O O CM

I

ro CM 00 ^ ^ r>» ot ^ CM at ko ^ O O CM o o o o o*— CM

«d- o in o ro kO O CM r—

Cp O ro

f— at ^ 00

in o in ro O O •— CM O I— CM O

d d d d

kOCMoo

d

CM

atd o

r-VOd

at

roo

o

VOo

d

m

d

VOro

ro

ro

o VO at ro m m o *d- ot CM

VO O r— CM

CM r— o ^

O O O O CM

r** 00 o ^ ^ 00 ^ o CM at ro o VO o O O O O O O CO

ot

CMo

o

VO ro

CM ro O ro

»— d d I

O ^ VO

in r** CM

ro ro —

0 O »— d d d

ro VO ro CM O r— r>. ro

»— O •— VO O •— O o O ^

Ct O CO kO «d- ot

CO Ot ro «d* «d-CMr>.r^f— O •— f— o o

o o o o o

r— CM

•— ro

CM «d* O ro

kO ro ^ ro

.— O ro r— «d- vO

«d“ r- CM O in O O r— O O

o o o o o o

in

ot

ro

ro

kO ro

CM I—

in CM O O

o o

m

r**- o

o

VO

CMO

O

kO

VO

VOOor**. at okOroO

d

f-W. CMO

o

CO

inoo

d

VOoo

d

ato

o

o

in

in

CMO

ro CO o C3t r*N. r** CM cjt «d- CO r— ^ ro •— f— o *— O o •— O O O O O

Oto

ot

ro

ro

ato

o

at r— o «d- oo r— O d- O O

o o o in

inat

CMO

d

ro

inood

vO 00

CM VO O CM o o

d d I

oat

VO

in

o ot

VO ^ CM *— o »— o o O o o o o o o

VOo

d

VOoo

rM M CM r— CM

^ -J _l O O O CM M M fN| r— CM rM rvj rM •— cm a

42

Proton

energies

are

pertinent

to

the

analysis

of

stopping-power

measurements

in

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 = 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

Bichsel 's Shell Corrections

Bonderup '

Shell Corrections

Reference (MeV) Cu Pb U Cu Pb U

a 3 316±3 818+ 9 910±14 31013 7451 9 805114 a 6 317±3 814+12. 89811

31413 736112 790H8

Stopping- b 6.5 327±4 830± V - 32515 7511 7

- power a 9 319±3 810+14 886120 31814 738114 789120 Measurements a 12 319±5 806±16 881 ±22 31915 74211

794122

a 15 319±5 803±17 878124 32016 746117 799124 a 18 318±6 800±17 877125 32016 747118 806125

o 19.8 325±5 851 ±20 “ 32516 798120 •

Range Measurements d 749 0 314±10 821110 889110 315H0 818110 885110

^S^rensen and Andersen (1973)

^Ishiwari et al. (1979)

“^Burkig and Mackenzie (1957)

“^Barkas and von Friesen (1961)

^From preliminary results of Ishiwari, Shiomi, and Sakamoto (private communication,

January 1982).

43
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. Reference

Bak 51 Bakker and Segrfe (1951)

Tho 52 Thompson (1952)

Bro 55 Brolley and Ribe (1955)

Bur 57 Burkig and Mackenzie (1957)

Bar 61 Barkas and von Friesen (1961)

Mar 62 Martin and Northcliffe (1962)

Nak 63 Nakano, Mackenzie, and Bichsel

(1963)

Bic 65 Bichsel and Tschalar (1967)

Tsc 68 Tschalar and Bichsel (1968)

And 67 Andersen, Hanke, Sorensen, and

Vajda (1967)

And 68 Andersen, Hanke, Simonsen,

Sorensen, and Vajda (1968)

And 69 Andersen, Simonsen, Sjirenson,

and Vajda (1969)

Gar 70 Garbincius and Hyman (1970)

Swi 70 Swint, Prior, and Ramirez (1970)

Han 70 Hanke and Bichsel (1970)

S0r 73 S?5rensen and Andersen (1973)

Zre 74 Zrelov, kruglov, Mus, Savel'ev,

and Sulek (1974)

And 77 Andersen, Bak, knudsen, and

Nielsen (1977)

Nor 79 Nordin and Henkelman (1979)

Ish 79 Ishiwari, Shiomi, and Sakamoto

(1979)

Bes 79 Besenbacher, Andersen, Hvelplund,

and knudsen (1979)

And 81 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 Ail, 19.8-MeV protons

R, 750-MeV protons

S, 4 to 40-MeV alpha particles

S rel. to Ail, 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

44
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0)3C

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pr- r- ^ ^ ^ CM CO CO

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CO

CO SVO VO Op f>. ^ ^

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fx- 00

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to

+1 +1 +1 +1 £

41 CO o vr> CL o CO ro O CO H- VO

ro CM CO r%. CO O 00 CM ro 00

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< 4-> +1 41 41 41 in in

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45
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 Element Symbol k,^ q/mol I, eV AI, eV I/Z, eV

1 hydrogen H 1.0079

19.2 molecular gas

21 .8 liquid

0.4

1.6

19.2

21.8

2 hel i urn He 4.00260 41 .8 gas 0.8 20.9

3 lithium Li 6.941 40.0 5 13.3

4 beryl 1 i urn 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 Ne 20.179 137 gas 4 13.7

11 sodium Na 22.98977 (149) 13.6

12 magnesium Mg 24.305 (156) 13.0

13 al uminum kl 26.98154 166 2 12.8

14 silicon Si 28.0855 173 3 12.4

15 phosphorus P 30.97376 (173) 11.5

16 sulfur S 32.06 (180) 11.3

17 chlorine Zl 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 iron 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 gallium Ga 69.72 (334) 10.8

46
Table 4.3 Continued

z El ement Symbol 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 9.8

41 niobium Nb 92.9064 417 15 10.2

42 molybdenum Mo 95.94 424 15 10.1

43 technetium 98tc 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 9.8

49 i nd i urn 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 lanthanum 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 144.913 (560) 9.2

62 samarium Sm 150.36 (574) 9.3

63 europium Eu 151.96 (580) 9.2

64 gadolinium 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

Z

4.3 Continued

Element Symbol A,° q/mol I. eV AI, eV I/Z, eV 68 erbium Er 167.26 (658) 9.7

69 thulium Tm 168.9342 (674) 9.8

70 ytterbium Yb 173.04 (684) 9.8

71 lutetium 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 Os 190.2 (746) 9.8

77 i ridium 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 u 204.383 (810) 10.0

82 lead Pb 207.2 823 30 10.0

83 bismuth Bi 208.9804 (823) 9.9

84 polonium 208.982 (830) 9.9

85 astatine ^At 209.987 (825) 9.7

86 radon 222.018 (794) gas 9.2

87 francium 223p, 223.020 (827) 9.5

88 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 “9pu 239.052 (921) 9.8

95 americium 2«An, 243.061 (934) 9.8

96 curium 247.070 (939) 9.8

97 berkelium ^Bk 247.070 (952) 9.8

98 cal ifornium ^Cf 251.080 (966) 9.9

99 einsteinium 252.083 (980) 9.9

100 fermium ^Fm 257.095 (994) 9.9

'^The atomic 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.

CVJ o IT) Oi o CO ov CO 00 CO

o. CVJ o> Cv CVJ VO pw lO as VO 00 CM 00 00 r*. fk 00 00 c*. 00

CVI 00

O ov IT) VO vn VO as o CVJ o <£ C.O 00 lf> VO Ck VO VO Cs. VO r>* 3 VO m CSJ 00 CVJ VO tr> CM o CM O o r— CVJ CM fmm CO CVI CM m CO m CO CO CO CO CO CO CO CO CO

cai CO CO CO CO VO CM CM o VO < VO VO VO VO VO VO VO VO VO VO VO VO

r*

ov fk un

O (/) . . • • C\J 1 1 ov § o r** CO CO o> VO VO o 00 o o OV OV o% OV

(/)

m VO fk. 00 o CVJ fO 1 1 • • . • . z a> vn 00 a> CO VO CVJ VO CM

00 00 00 CO 00 00 00

(U

•r- «:! CO CVJ CO o 00 o • • • . • • . o o. 00 r* 00 CO 00 1

as OV CO 00

to 00 rk 00 t>v f>^ r>.

CO CO rk CO CVJ CM 00 LO CM

CVJ ro 1 • . • • . . • • • a: o) 00 00 00 00 00 ov 00 00 ov o o>

r— r— r— r— r— CVI f" co

01

L.

(U .C VO

4-> CT> E ^ O

tk

u- a;c

•o

k

o; 3 c »-

to T3C

.O (O O o c c

Q) <0 u.

<U

O > k

<0 Vf- sz c

v/> 01

0) ^ 3 <0 I— 4-> <0>

I—I II 00. • M

T5 kJ O •£-

P».

>0>II ca

a;

M > o o 0) o> u

as OJ 01 i/> 1 OJ

k_<i> o> o •r OJ •o - c T

00 • CVJ o c 0) OJn

a VO VO

M 00 4->

k •-H

cr» VO as

a as o cr» o O. 0) CO VO r* oO 00 00 O «4- c

VO VO Ch cy> C7V o 0) o? as ov r— 0) c p— r— <Q k

p“

O 01

u II OJ s- 0) to 0) to (L) z LO 0) (/) &. c r* o; «/> HH

O. o 1 C c a> 0) o> c 3 0) c U1 c o s. o -o r—

QJ c p— c o ro < TO 3 c lO h— z Li. z O CD 1— 00 <c ct 1^ > o

49
•*-> <0

CO

O O) CO CD • o •r- E C (J CO CO CO CO CO CO o CM C7^ <D +J 3 O C ‘r- X> (O CO T- 3 CO O O CM CM ro O cn •O' C ^ CO >> > o ro U 4-> t— CD +1 +1 +1 +1 +1 +1 +1 +1 +1 u s- o> C ro

CD CO S. CD

CO o r-» CO o VO •O’

<4- 5 S- E (O 1—

o O CO O CD a\ CO <y\ CO •O' •0* Q. U 4- ro r— f— CO CO o CO o crt CO 1 r— 3 4-» r-“ LJ 3> <0 CO ro c C C C ro "O

CD -I- ro •»“ CD 3 CL S. E <D

4-> O. (D OJ

X

O

X -L> CO •*->

M +-> h- 4-> -

CO CO ro c c C U o •*- o 4- • CO CO • u O 1 CL 4-> O

CM 0) E c X3 •M

u CO ir> f—O CD (D <D

•r“ •f- CLX L. X3 F CO •— •»- H- CD C XJ X3 to

p o +J X C 3 X3 <D T3 <D c CO

+-» 4->

CO Oj CD 4-> CD •p- OJ C7J (O m c c o

i- fO O CL C E

to o

CO s:

<U E I ••- O

O) S- >>

S- M- -Q

0>C '• X)

(1) CO <D XJ i- C C 3 O 3 CO E 3O iA

COU 0>

<DU *rO «t> 4-> 3 C — O T- U +J ro C C +J

»- •<- t-0) -o OJ u o

CO

Oo

CL

C

rO E E

4->

OU S- (j O)Q.

CL

C

O

C

fO CT» <U SO 2 O +J

QJ TCVJ

C rO

CVJ -r- ro ro r—

4-» I—

II s. 0> D 2

3U OC CO

O

O c

(UCO

0)

S- • CL CO "O

o> c ^ 3

+->

O

CL c E

•rOU

XJ

<u

+-> o

Q-o CO XJ 4-> ro C

<V

CO 3

O) -»->

CVJ

CT»O Osj f— CO

C7> +-> S- CO

0) e c o

<L)u

CO

O -r-

•r- E

-t-J

O

fO -*-> -L> «T3

LO

UJ

(-0 <o cI 0)3

4->

U

U -M

X

O CO

CD 4-

CO

C -X C_) n3 s-

(D

O

s: s

c^ ^ O

0> r— CSJ CO

QZ

<c

4-> 01 c > 0) •»- E a^

CO o>

•»- I— <u

a; (o

<o

•-H o> x:

JO CL

4>> <U X5

S. L. (D O) O CO J= C • 5 0> OO

O) *o • 3 C

«i—

O

«--i CO

U OJ > rX I (U ^ •-H JC CO ro 4-) Hr— 0> • X c c

oio

cOooo

CO

s.<D JZMO

in

CD

50

179.7
value

deduced

from

experiments.

B.

Liquid

Compounds

r-V£>»—-OLDOCsJUnCO^rOr— »— o iO OOOr— OOOOvOOOOOO OO I— <vj I— r-

<MOOir>mc\jcsj^cooo>«^-oOr— csja> rsjcvjr>.<^oroa^o^r**. COO^i— I— r— CNJOi— o OOOOOr- CMOO<^COOCM»— OCVJ

CO CO CO CO CO CO CO CO CO

+l +1 +1 +1 cococococorococococococo+1 +J +1 +1 +1 +1 +1 +1

CO CO

+1 -H m CO o% o o> ^ OtOOOVOf~CVlOCSiUO

L£) CO r—• <U

LD OO LD ^ 3= Z X O

CO to to o U O O I—

0) O 0) »—

VO C I—

* o

o> t. c o

to r—

o 0> O c* L. f X O o +> o

r» 0> U

JZ f— f—

X- O I— O "O ^

VO VO CSJ I—

f— ^ X O f— o I X r- o X JZ

tN. X CO *• mo > o VO X a» o u O O C f—

m ^ (O

o> * « N a> C O I— c c ^ 40 c o <o >>

4->“ lO C ^ 4^ O.

' o c o

r— o CNJ >> O 0> O) X a. Q.

>» 01 JZ 00 00 >) o X 0) X X f—

CO o r>. 4J X

CJ &. CO 0> O 00 O P CM (O

• f— * C X « X o» o * C U C I— • <L» <U 40 01 X u c

S. 3 u 01 0> >>•<-> f— •*- -4J f—

•M 0> O ^ 40 >>

«A 4-> 4>> 4-» 2 X

T- 0)

S- T? 3

0> C 4->

CM 3 m

*0 0) M <U »—

i/) C X » c •*- <o •— O 40 hj ' L)

> CO- X E * o o

O)!2.

CO

</> 4— 0) 3 0> 3

1. C I—

I ‘f- 40 o>*o >

CT 40 i 40 a; »~4 X CO o>

0) X X X 4-> U hC3

CO o 2*^

CO o>

o ^

f— ^ ^ CO o o

CM VO ^ CM O

CM CM O O O CM

CMCMCMCMCMCMCMCMCMCMCMCMCM

+1 +1 +1 +l +J +1 +J +1 +1 +1 +1 +1 +1

•f- 0> T-

<o E 4/* •M 0) >>

i- u ^

2 • -r- 0) 3 X I— T?

40 Q> X > c • C *r- 3 r- 40 O lO 4J E 4-> X 40 C O 4— •

*0 T3 c s. 40 O m tA

Q>

<D 3

4—4 >— m

o

m00 ^ CM f— m <y» r—

CO

Cn. 00

o> m CM I— VO

r**. I—

c a; 40 QJ X -O o +-» c •!>- X • EO <L> S. X

t_ CL t/> 0> X OJ X 0) L. a rQ a rQ .Ci rQ

0> r—

I— ^ VO X r- O) X X X *0 CM O VO O *f“ CO O C_> O

L. X Of 0^ *o o

«> (1) (LI

Ol Q> <U •«- «r51

From

alpha-particle

stopping-power

measurements

of

Bichsel

and

Hilko

(1980).

Note

that

an

analysis

of

the

stopping-power

results

of

Bader

et

al.

(1956)

for

protons

with

energies

between

300

and

400

keV

leads

toa

value

of

88.7

±

7.1

eV.
Experimental

I-value

was

obtained

in

our

analysis

of

Thompson's

(1952)

measurement

of

partial

proton

ranges.

oo

oj s. :>

lO 0) <u c 5 0

CL Q. •

I Qj cnm

i- c

1 •!- <U U Q. 3

•I- CLr~ U O fO

o • •

<4- <U

CSJ LO

OJ--' . CSJ I—

CNJ LT>

• a^ +1

CSJ I—

KO - "LO

csj at csj

i E

cn 3

C t/1

fo E a; O 3

d) sz > h- <T3

ta

at •

*o 0) • c -M at o o>

) C rQ

ro I— o> o> c

at c o) tD

t/t x: >»'^ vn U I— -I-

•I- Q. <0

fiO

I It) s- *o at

IfO >» ^ c o ft) ID • ^ > E ^ 0 at I—

(/) at t— lt> ^ ^

• c at

at CO at 3

-c X »—

•M I fO O C >

•o -r- 01 *0-0

tA csj s. at

•1“ . o +J > ^ Z CL

at f"** o

s- at -o EX'" i/> o +->

It) at

i/» O o

CO c +-> o> at r- E -O

at

i- at

• 3 r— .

i/t at O 'tJ 00

O) 4-> It)

X «4- <4- X

O I— C oo o . •I- at u) > •M 4^ >> at

fO o f— u c fo r>* *»- 4-» C . c O It) ^ 3 O §

0- U +1 3 o at o u at

(/)

at at E >

at IQ

at •

t- D_ ^ O. U It) ' 1- at >

o u

+J 4-t 3 c C U i/> It) •r- C It) <0 3 at i/t Cu M- E ‘r-

-«-> at u at E

at at i/> I— c\j u -

at 3 c

•r- +1 tA O *0 It) (A r— at Q.

at cn. g £ X o

-t-> &. X 0- at I— <-0 5 o o E

at o. o

^ at I i- £ 03 a>o- o i. c

T; at -I- *d

ti > CL at 2 « Q. >

3 o •»“ f— at -M i- I? X u) at "o

at c

E r- o

U +1

E O > o i/> • at

S- -r- tvL -O S <- X « C

t— 03 Lf> oO -4^ • •r- at r***. > C U > CM

at o at at

•r- 4-» Z 4->

r>. 4-> u IQ

• o O <7t CO c a. • (A

13 c at • u

> O > CM 3

^•1— «/) at CO u It) X at at -M at I— t- -o lO E

k. s.

•I- oiO O3

•— 00 *

3 *0

iO C

at IQ

&. ou

at CO 50 c

Q. at

1 at at 5

C 4<t •r- at Q.X

CLO <A 4^ at

lA •»-at E sco13 C ^ O

U 4-> 13 O

OO k.CL

o-O 4->

3

atat (A

o> a

lA X O -r- 3 U .1- r-

_) C 4J 4- O -I- l- O •- CC "O o

032 4-> 09

»— 00 at VO

D- CM CM LH

r>. CO in

r— VD U9

> at k. k- o . s 4- at -rI "O 4-> s

CO CM I— m 00 O O CM ^ ^ p- ^ m CO ^ I—

CO l- at LO m m VO oo^^vococooocovo

at CM

a. in X crt at r—

o o» -c o 4J CL

to at o CO

•f— r— X at CO k. >> I r— C U

fO <0 1^ c E CM k. 3 r— CO 4J

at OV U

c I— at 3 C '^1—

at at E X ^ o at -o k--Or—

) 4- c X at 3 CO X : c 4J

) > c

> at • 4- L -O "9 O

: r-. S-

> • o E CO

: CM z o rs- at

+1 14-. i*- -o o o

> VO >• E

• CO at

) 4J -O

• r*^ c ^ Qt

at 3

(A C

•f- 3

E

o s_

k- 3

Q. O

< 4- a

at 3 -o >>

cO C l—

CM 3 3 •—

CM at 3

CO E •*' o

II s. CO s- at r>^ •!- 3 3 0» CL 00 r- £

41 41 41 41 41 41 41 41 41

3“ O 0% CO

f— m CO 00

a OtQrCj o'xa

»n >» X X $-

Uf) CM L) CM O 3

CO Lt. U- O 3 *1“ CM O —I

at at T- »r-

•r- ‘I- C 4- C C o 3

at 3 1— 1-

o I— »—

CO O T52

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 (eV)

Densil^

(g/cm^ <Z/A>

Water Content

(% by weight)

H2O 75.0 1.00 0.55509

ICRP adipose tissue 63.2 0.92 0.55847 15.3

ICRP skin 72.6 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 75.1 1.06 0.54995 80.0

ICRP lung 75.2 1.05 0.54965 78.0

ICRP skeletal muscle 75.3 1.04 0.54938 78.6

ICRP cortical bone 106.7 1.85 0.52130 15.0

ICRU striated muscle 74.6 1.04 0.55005 78.6

ICRU compact bone 92.1 1.85 0.53010 15.0

53
Table 5.5. Recommended mean excitation energies I for

Material <Z/A>

k Density

( g/cm ^)

A-150 TISSUE-EQUIVALENT PLASTIC‘S 0.569031 1 .127E+00

ACETYLENE, 0.537680 1 .097E-03 ADIPOSE TISSUE (ICRPlfc 0.558668 9.200E-01

AIR, DRY (NEAR SEA LEVEL) 0.699190 1 .205E-03 ALUMINUM OXIDE. AS, 0 0.690382 3.970E+00

* 2 3 B-lOO BONE-EQUIVALENT PLASTIC^ 0.527397 1 .650E+00

BONE, COMPACT (ICRU)® 0.530103 1 .850E+00

BONE, CORTICAL (ICRP)^ 0.521299 1 .850E+00

C-552 AIR-EQUIVALENT PLASTIC^ 0.699687 1 .760E+00

CALCIUM FLUORIDE, CaF^ 0.686700 3.180E+00

CARBON DIOXIDE, CO^ 0.699889 1 .862E-03 CELLULOSE NITRATE

0.516237 1 .690E+00 CERIC SULFATE DOSIMETER SOLUTION^ 0.552785 1 .030E+00

CESIUM IODIDE, Csl 0.615689 6.510E+00

ETHYLENE, C.H,

2 4 0.570337 1 .175E-03 FERROUS SULFATE DOSIMETER SOLUTION^ 0.553282 1 .026E+00

GLASS, BOROSILICATE ("PYREX", CORNING 77A0)’' 0.697070 2.230E+00

"KAPTON" POLYIMIDE FILM, (C22Hj^gN20^)^ o!512666 1 .620E+00 LITHIUM FLUORIDE, LlF 0.662617 2.635E+00 LITHIUM TETRABORATE, Li,B,0,

2 4 7 0.686869 2.660E+00 METHANE, CH,

4 0.623360 6.672E-06

MUSCLE, SKELETAL (ICRP)^ 0.569378 1 .060E+00

MUSCLE, STRIATED (ICRU)® 0.550051 1 .060Et00

MUSCLE-EQUIVALENT LIQUID, WITH SUCROSE^ 0.568281 1 .110E+00 MUSCLE-EQUIVALENT LIQUID, WITHOUT SUCROSE^ 0.550136 1 .070E+00 NYLON, TYPE 6 AND TYPE 6/6, (C,H, ,0N)

0 11 n 0.567902 1 .160E+00 PARAFFIN WAX, C2^H^2 PHOTOGRAPHIC EMULSION^

0.572768 9.300E-01 0.656532 3.815E+60

PLASTIC SCINTILLATOR ( VINYLTOLUENE BASED)”* 0.561615 1 .032E+00 POLYCARBONATE,'*"MAKROLON", 0.526968 1 .200E+00 POLYETHYLENE, (C,H,

2 H n 0.570337 9.600E-01 POLYETHYLENE TEREPTHALATE,‘’"MYLARV 0.520370 1 .600E+00 POLYMETHYL METHACRYLATE,P (C,HqO.)

^ o 2 n 0.539369 1 .190E+00 POLYPROPYLENE, (C-H.)

J 3 n 0.559985 9.000E-01 POLYSTYRENE,^ (CoH^)

o o n 0.537680 1 .060E+00 POLYTETRAFLUOROETHYLENE,^ "TEFLON", (C.F, ) 2 4 n 0.679925 2.200E+00 POLYVINYL CHLORIDE, {C,H,Cil)

X J n 0.512011 1 .300E+00 PROPANE, CjHg 0.589620 1 .879E-03 SILICON DIOXIDE, S102 0.699298 2.320E+00 SODIUM IODIDE, Nal 0.626968 3.667E+00

STILBENE, C^^Hj^2 0.532597 9.707E-01 TISSUE-EQUIVALENT GAS (METHANE BASED)® 0.569927 1 .066E-03 TISSUE-EQUIVALENT GAS (PROPANE BASED)* 0.550268 1 .826E-03 TOLUENE, CjHg 0.562651 8.669E-01

WATER, LIQUID, H

2 O 0.555087 1 .OOOE+00 WATER VAPOR, H 0

2 0.555087 7.562E-06

compounds and mixtures of the indicated composition.

I 6 Composition

(eV) Gr (constituent Z = fraction by ueight)

65.1* B 1

! 0.101327 6: 0.775501 7! 0.035057 8! 0.052316

9 : 0.017622 20 : 0.018378

58.2 A 1

! 0.077618 6: 0.922582

63.2**B 1

: 0.119677 6: 0.637260 7! 0.007970 8! 0.232333

1 1 : 0.000500 12 : 0.000020 15! 0.000160 16: 0.000730

17: 0.001190 19: 0.000320 20! 0.000020 26: 0.000020

30: 0.000020 85.7* A 6: 0.000126 7 : 0.755267 8! 0.231781 18: 0.012827

165.2* A 8! 0.670769 13 : 0.529251 85.9**B 1

: 0.065671 6: 0.536965 7: 0.021500 8: 0.032035

9 : 0.1676120 : 0.176589

91 .9**B 1

: 0.063986 6: 0.278000 7! 0.027000 8: 0.610016

12 : 0.002000 15 : 0.070000 16: 0.002000 20! 0.167000 106.6**B 1

: 0.067236 6: 0.166330 7! 0.061990 8s 0.666096

12 : 0.002200 15: 0.106970 16! 0.003150 20 : 0.209930

30 = 0.000100 86.8**B 1

: 16: 0.026680 0.003973

6: 0.501610 8: 0.006527 9! 0.665209

166.0* B 9 : 0.686659 20: 0.513361 85.0* A 6: 0.272916 8: 0.727086

87.0 B 1

: 0.029216 6: 0.271296 7! 0.121276 8: 0.578212 76.7**A 1

: 58: 0.107596

0.002001

7 : 0.000800 8: 0.876976 16: 0.016627

553.1 C 53 : 0.688651 55 : 0.511569

50.7 A 1

: 0.163711 6: 0.856289

76.6**A 1

: 0.108259 7 : 0.000027 8: 0.878636 11 ! 0.000022

16: 0.012968 17 : 0.000036 26: 0.000056

136.0**A 5 : 0.060061 8: 0.539566 11 ! 0.028191 13! 0.011666

16: 0.377220 19: 0.003321

79.6 B 1

: 0.026362 6: 0.691133 7: 0.073270 8: 0.209235

96.0* B 3 : 0.267585 9 : 0.732615

96.6 C 31 0.082085 5 : 0.255680 8: 0.662235

61 .7* A 1

: 0.251306 6: 0.768696

75.3**A 1

: 0.100637 6: 0.107830 7! 0.027680 8: 0.756773

11 ! 0.000750 12! 0.000190 15! 0.001800 16! 0.002610

17 : 0.000790 19! 0.003020 20 > 0.000030 26: 0.000060

30: 0.000050 76.7**A 1

: 0.101997 6< 0.123000 7! 0.035000 8: 0.729003

11 : 0.000800 12! 0.000200 15! 0.002000 16: 0.005000

19 : 0.003000 76.3**A 1

> 0.098236 6< 0.156216 7! 0.035651 8: 0.710100 76.2**A l! 0.101969 6: 0.120058 71 0.035651 8: 0.762522

63.9* A 1 : 0.097976 6) 0.636856 71 0.123779 8: 0.161389

55.9 B 1

I 0.168605 6: 0.851395

331.0* A 1 : 0.016100 6: 0.072261 7 : 0.019320 8: 0.066101

16> 0.001890 35! 0.369103 67! 0.676105 53! 0.003120

66.7 B 1

s 0.085000 6: 0.915000

73.1 B 1

: 0.055691 6! 0.755751 S: 0.188758

57.6* B 1

> 0.163711 6: 0.856289

78.7 B 1

: 0.061959 6< 0.625017 S: 0.333025

76.0* A 10.080538 6> 0.599868 8i 0.319616

59.2 B 1

: 0.122698 6: 0.877302

68.7* A 10.077618 6: 0.922582

99.1 * A 6> 0.260183 9! 0.759817

108.2 B 1

: 0.068380 6: 0.386360 17! 0.567260

67.1 * A 1

: 0.182855 6! 0.817165

139.2* A 8: 0.532565 16! 0.667635

652.0 C in 0.153373 53 : 0.866627

67.7 B 1

: 0.067101 6: 0.932899

61.2* A 1

: 0.101869 6: 0.656179 7! 0.035172 8: 0.606780 59.5**A 1

: 0.102672 6: 0.568960 7! 0.035022 8: 0.293366 62.5* A 1

: 0.087510 6: 0.912690 75.0* A 1

: 0.111896 8: 0.888106 71.6* A 1

: 0.111896 8: 0.888106

54
</> (U

4<> Oc

4-> oo 3

*o ^103 CM

<0 ^o "O 00

CM

<0 ^ u z

*U CM 3

<4- • f— CM 3 ^CO O Z 00 CO'-' • 0> o oc ^ •I- POoQ) a\

I— "O 3 C

lO ro 3

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fO ^ O

•r- 0^ 4-» CO 3 O

CO

lO ^ 3 OO 00

0) CM 3 Zcr

rtj ^o^

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ro *> OO CM Z£.3 S'? 4- O • ^3 CO ^ CO CT O CO >, C C7>

0) o 4-> 2 <0

fO ro Z —i »— ^ 3 “O CO

CO

C

Oro O I .d

•I- S- c o *o o c E ro ro *‘0

CO <U CM 3 C Z O O) CO W <U .

s- s- • O

CD

•o

00CO

CO oCM

IOro CM

ID 00 . O

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C CM E ^•D «0* I— s- z O o z O O'—

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uo

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00 I—

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Qi

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iA U. U 4-> 0> O

U 4-> f- 10

(J •»- 0)

(O Q. f— US U

ro 3 “ 2^ CO ^ •I- 4-> o *o >»|- 0) +J •»- U

•1-0-3

CO S "O C O

Q>s

U

*o •a O r- CO C r- U

ro

O

CO 0) cn COo

CO ^

•M •• roQ.

r— rm

0\ r—

-o ••>- 0)0 0. • CO I— = U

ro r—C

-Q -O '—Ul C Z ro ••

CO

O

O

O o: —

I C O)

ro *r- E <D -a s o

<S ^ a;

•»- CM

U

to

O 4-> Q.

O »—O

U

CL ^ (D

X

O)

to

roC3oco

CO 5O

4-> COX

0)CL

COu

a; o. ou

00

O'u

ro

*oc

ro Zos

•* ^ o

CM cn^ Z 0 3 « 2:: ^ Z 0) • CO u

cr> o ' *oc

ro

U CO c *p- r-H O -M

•f- to r-

(Oo u

Q.«^

O sou O fCO ro 0) *f- 0) 4-> 4^ Z g

•r- ro

C

X Q. ro O 0) u u u 0. 0. 0) CL lO ro 0) •»-

r— tn r— C r—

C •!- 5 •»- 0)u

#.-0 4-> 01 d) (/•) CO (O 0 3 4-O

I— .^CO

to r— O O>

CO

>oo

roX 3 O) O’-M

ro 0) CO 4->

r— “D

ro 0) > CO I CO ^ O Z 3

CMr— O 4-

<U UO >>00

HH 3 ^ C U ^ ro

O) CO •— ^ • • 4-> "O C C CO

ro I— E

Tr-- E

I— > 4-» 1— JC • LU O)

TAa 4-> 0) C 2

+i o

O- >, 3 X)

CO TD •

01 ^ o

f— • ^

Qu r—uo cn CL*—

D) QC

CCO

O •-*

r— q; -o I— .c c E O O U

to 4- 0) • C

Q) x: “O cn

r- 0)

'o'-'

O. CM o ^ •!- ^ C/0 CO‘ o

r-. •!— "o

4-> CO uo ^Q.U^ 0) CO

QC • O zQ£ *D

55
Table

5.6.

Comparison

of

mean

excitation

energies

for

compounds

recommended

in

various

publications.

Values

are

•o CO LO LD o r— O LO LO LO LO f— C LT> • • • • ns r— <T» CM lO o^ CM LO 1 CM LD CO

S- f— LO LO LO VO LO VO

CQ ^ r— r— r— CM

Z LO CO LD VO LO CO

• cn • • • • • • OO r- o 1 CO LO LO VO 1 1 ^ o CO

LO LO LO VO LO CO o CM CO CM CO

"Oc

(0 SQJ CO CM CO iO CM CO <Tt c C LO • • • • * • o r— LO I LO cr» 1 CM 1 1 1 1 1— Q

O 1—

h- —" LO LO LO LO

CM

o\

CO CO CO CO LO

l/> f— o CM CO LO LO a^ LO CM 1 1 1 CO CO

cu —

cr> ns

LO LO LO VO VO VO VO CO CO CM

LO

Q.

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 Enerqy I (eV)

AtomiMolecular

gas^ gas^ Liquid‘s Solid“ Ratios

(a) (b) (c) (d) (b)/(a) (c)/(b) (d)/(a)

'h 15.0 19.2 21.8 1.28 1.14

62.0 78 1.26

76.9 82.0 90.5 1.07 1.10

93.5 95.0 104.3 1.02 1.10

124 166 1.34

^^Si 132 173 1.32

182 233 1.28

26Fe 226 286 1.26

29cu 274 322 1.18

292 350 1.20

H2O 71.6 75.0 1.05

C^Hg, propane 47.1 52.0 1.10

CcjH-ip, pentane 48.2 53.6 1.11

CgH^^, hexane 49.1 54.0 1.10

C^H^g, heptane 49.2 54.4 1.11

‘^Theoretical: from Brown (1950) for H; from Dehmer et al. (1975) for C, N,

0, At, and Si; and from Inokuti et al. (1981) for Ti, Fe, Cu, and Ge.

^From Tables 3.1, 5.3, and 5.5.

‘^From Tables 4.2 and 5.3.

“^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.

Q) X

CO

I X

LD

COm

IId

u

CO

Io

X

LOoCSJ

zs

3

O’

•r- CT O r-

<NI II n: Qj

CO

3 E o u

•M

•f^ O)

“S- o

s-0> f—

ila

CO o

CO ^ ^ CO

CO I— O

o c5

00 CO O O

r— tr> 00 P-

^ O to 0^p-L0t0p— CSJIOCSJ

r^io^ooioi— o^tooocsif- o o csj Osj cvj I— p- pCO CM r— LO VO VO LO CM o> CM

a\ r— 00 00 CO p— 0) CM CM CM CM r— P^ •4->

0>

4->

E

u

cn

<T> o o LO VO <3- CO On. f— CM

sz LO

Cl LO O VO CO o VO 00 o VO ^ CM

ra

S-Oi

CM

CM

IIO.

CO CM CM CM CM P“ o o

CM CM CM VO VO LO

• o CO LO CM o^ LO CM

oo CM CM CM f—

p-» f*>* to 00

VO

• • I— o

COo

o o o o o O O O O LO O LO CVi ^

o o CM r—

LO CM I—

LO CM f— o o o

Q.

to

0) *o

o>

s-o

u

fO

Q)

L/> c

a;

3

Q.

<3

58

Graphite

crystallite

density
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'p

1

(T).

Results

were

calculated

using

density-effect

corrections

L^(T,A)/S^^

1

(T)

.

Results

were

calculated

using

density-effect

corrections

obtained

from

Sternheimer's

method.

obtained

from

Sternheimer's

method.

f— VO O ro VO to CNJ to VO f— 00 CNJ 00 p^ o to cn f— to o ^ r— ^ o CNJ o ^ ^ o O ps O O to

VO 1— r- ro to Oi to o ro CNJ CNJ ^ to CNJ ^ ro 00 ro CNJ CNI ro CNJ CO VO ro O CNJ o at to o CO CNJ O O CNJ u O ro LO ro to to VO P^ p*«. p^ p>. O 0> 00 CNJ »— cn to ro o Ps to ^ O ps CNJ o cn ro o ^ VO o o at

00 VO 00 VO CO to 00 VO 00 VO VO at 00 VO cn CO ps at CO ps O 00 O 00 ps. o at ps. O O Ps o o o o o O o o o o o o o o o o o o o o o o o o d d o P- o o P- o o *— o o *— r- d

ro <Ti LO VO VO r- CT> ro cn CTl CNJ 00 ^ r— O CNJ to ^ to ro o to ps to cn O VO p- §123 O ^ Ps O O IT)

CNJ O 00 CTl to ro ^ VO VO ^ CNi CNJ VO cn o ^ 00 ^ CNJ ro to VO CO 00 ps O VO ps o cn ps o o ps o VO CO CO CTi ro ro ro VO to ^ o 00 CNJ 1— cn to ro o ps to 1— O ps CNJ o o ^ o VO o o at

CNJ 3 r*«. VO Lo rv VO to 00 r^ VO 00 VO 00 VO cn pN. to cn CO VO cn CO ps at 00 ps O CO ps o cn ps o at Ps o o ps o o o o o o o o o o o o o o o o o o o o o d o o o o o P- o o P- o o r- o o r— 1— o

VO VO to 00 ro p^ to ps o o o o

r>. to 00 ro CNJ to cn o o o o CO to 00 o ro PN. o ro VO o o o o

Q_ r>s. 00 00 00 cn at cn o o o o

o o CD o d d d o d •“ rCO ^ CNJ CTV CNJ VO r- CNJ CNJ cn O VD cn o> CNJ CNJ o to o o o VO o o

00 CO O to o> cr» ro r«-. o to P^ CNJ o to cn CO CNJ to O VO O VO O ps. o o m ro ro VO to CO f— ro r— p^ f— VO ro 00 ps 1— O ro O VO O CNJ o o

<C VO VO p>» VO 00 VO 00 CO P^ cn ps. cn ps 0> 00 O CO O CO o at o o

o o O CD CD o <=> d o d d d d o d o o d 1— o 1— o »— o 1— •—

ro VO o> to 1— VO ro f— CNJ CO CNJ ps. CNJ cn ^ cn •— O CO O CNJ o ^ o o O o 1— CO 1— CNJ to O CNJ O r- O ro to CNJ cn ro to O VO o to o ro o o 3 VO to cn 00 f— o CNJ CO to 1— p^ ^ cn ps CNJ o S

O ps o ro o o O VO VO r*N. vD 00 rv 00 CO P^ cn p^ o ps cn CO O 00 o cn o o

o o o o o c> CD CD d d d d d d d d d d 1— o r- d »— o r- •—

LT> Oi f— ^ VO ro O ro P^ CNJ O VO CNJ CNJ VD r— VO P>. O VO CNJ i— to VO f— O O ps O VO o O VO to o O VO

fo CO ro to cr> to ro o cn ro VD to ^ r— CNJ ro cn r— VO CNJ CO 00 ^ VO CNJ to O CNJ «C3- O CO ps* o 1— ro O O oo

iO LT) VO rs. r>. o o O CNJ CNJ »— to ^ ro P^ ^ CNJ cn to •— ps. ps. ^ CO o VO at O GO O O ^ ro O O VO < VO to r%. VO to CO p^ VO 00 VO CO p^ VO 00 P^ VO cn ps. VO cn 00 to cn CO VO O CO VC O CO Ps o cn Ps O O ps O O O O O C) o o o O CD CD o o o o o o d o d o d o o o o r— O O r- O O 1—0 0 O

ro ro ^ to 1— to 00 ^ 00 to cn 00 r— ro o o to to ro CNJ O to to cn ps O ps. o O VO ps O 00 CNI O O o U 00 Vf> CNJ O ^ 00 o o o ^ O VO cn 1— CNJ p^ ro to VO CO ro CNJ CNJ cn CO VO ^ o to to O O CO O CO VO o O VO \ to to Cn. CO CO 00 ro ro CNJ to to cn CO to CNJ O CO to ro cn ps to r— O ps CNJ o o ro O ^ VO o o at O o> VO to PN. VO to 00 P^ VO CO f*^ VO CO p^ VO 00 P^ VO cn CO VO cn 00 VO cn CO ps o 00 ps o at ps o cn Ps O O ps

PN* d o o o o o o o o o o o o o o o d o o o o o o o o d o r- d O 1—0 0 f— d o 1— 1— O

> O O r— o o •— O O 1— O O 1— O O r— O O f— O O 1— O O 1— O O 1— O O 1— O O 1— O O r- O O r—

<3 0) o O f— o •— O r- o •— O I— O 1— O r- O f— o •— O r- O I— O 1—

•“ r— r- *“ f—

to CNJ to CNJ o o o

> o o o o to CNJ o d o o d o 1— <D o to CNJ — r—

to 00 ps VO to Ps o ^ O ps o o cn VD O CO ON ro to to ON r— O ON ps o 00 ro O to ON O O ps o o o cn VO ro ro ps 1— O Ps to ^ to to CNJ to ps ro to to ^ ps ps o to to O ON ^ o to o o ro CO O O ro O O to CO I— ^ O CNJ to CNJ ro to ro ^ to to to to CO ps to r— ON Ps to CNJ cn O to CNJ o o ir> O ^ ps O O CM O O VD 5

ps Ps VO 00 ps VO 00 PS VO CO ps VO CO ps to CO ps VO ON ps to ON CO to O CO ps O ON ps O ON ps O O 00 O O 00 o o o o o o o o o o o o d o d o o o o o o o o o •— o o 1—0 0 .— O O f— r— O 1— f— o

1— o cn to Ps o ps ps CO 00 cn ON VD 1— to to ON co O to o CNJ to ps O 1— ^ o VO cn o VD rn O O 00 O O VD -o ro ^ ro t— o I— to cn ^ ^ ^ O VO 1— O 00 VO to ps 00 1— 00 ON o CNJ cn o ps ^ O ro O O ps O O 00 o ^ to VO VO ps CO cn ON at ^ ro ro CO VO to 1— ON ps to CNJ ON O ps CNJ o o to O ^ 00 O O CM O O VD

CNJ 3 Ps VO to ps to to ps to to CO ps VO CO ps to CO ps to cn ps to cn CO to O CO ps O ON Ps O ON Ps O O GO O O 00

DC O- 5

o o o o o o o o o o o o o d o o o o o o o o o o .— do r— O O r- O O r- 1— O o

ps 00 o VO ro ro ON o o o o o VO to CNJ ro CO CO ps CNJ o o o o o Xi ro VO 00 o s

00 ro o o o o o Cu ps ps ps ps CO 00 ON o o o o o

o d d d d d d O •- — •— ^ ps to r— to CO CNJ ^ CNJ ^ ps CNJ ir> CNJ ON O CM O ON o CM o o o o 00 o CO ps VO 00 cn to ^ CNJ ^ ON ro to PS ON O CM o tr> O ro o o o o cn 1— CNJ ro ro VO to CO Ps 1— cn to r— ON ^ ro ps O ro O PS O CNJ o o o o <c ps to ps VO ps to ps to CO VO C0 PS 00 PS ON ps O 00 O 00 o a> o o o o

d d d d d d CDO o o d o d d d d r-^ d r-^ d 1— d — — - —

o cn ps to CO «:J- CO ^ ps CNJ ps PS to ps O CM O 1— O ON o o o o O CNI o cn CO 1— 1— 00 ps ps ON ps ps to o o O CM o S

O 00 o o o o 3 CNJ CNJ ro to VO cn ps r— ON to CNJ ON to ^ ON O O CM o o o o o ps VO ps VO ps to ps to 00 VD CO ps CO PS ON ps O 00 O CO o a» o o o o d d o d o d o o d d d d d o d d O d r— O .— r- -

CO to CNJ to CNJ O CO to VO 00 to to 00 ON ps o VO O CJ- to O O CNJ O ^ «;J- O 1— tf> O O VD o o o O O ON

ro 1— cn ^ at ro ro ro to CNJ CO CNJ CNJ CNJ 1— CNJ 1— Ps 00 ps to o rs O ps CO o VO «a* O ps ro o o o O O CO

ro ^ ^ to to VO CO 00 00 O O ON ro CNJ i— ps to ro O PS ^ 1— to o to cn O ON CM O ro to o o o G CD ^ <c ps VO to ps to to ps to to CO PS to CO Ps to CO ps to cn Ps to ON 00 VO O 00 VO O 00 p^ O ON ps O O 00 O O 00 o o o odd o o o o o o o o o o o o odd o o o »— o o .— do o o r— r- O r— r- O

roE cn ro CO ps to ro 00 to •— o to f— ^ 00 f— CNJ to ro to Ps to ^ VO o VO ro o 00 ON O CM 00 O O VD o o in u CO CO Ps at VO ro CO <— -d- CNJ o cn ps o Ps CNJ ps CNJ CO O «:J- CNI O O VO O VD CM o ^ O O VD O O ps

ro ^ to to to Ps CO cn cn r— o ro ro CNJ ps to <3* f— cn to to CNJ cn O ps CM O o UD o CO O O CM O O to

cn ps to to ps to to ps to to CO Ps to 00 Ps VD 00 ps to cn ps to ON GO VD O 00 rs O ON ps o cn rs O O CO O O 00

Ps o o o o o o o o o o o o o o o o o o o o o d o o r- O O .— o o .— o o o r— t— O

> O O r— O O r— o o *— o o •— O O 1— O O 1— O O 1— o o »— o o O O f— O O f— O O 1— O O r- < OJ O r— O I— O 1— O I— O 1— O I— o •— O r- o o .— o »— O 1— O r—

' ' *“ r— r—

to CM

to CM o o o

> o o o o to CNJ d d o o o o cu o to CNJ

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)

cellulose collodion & air^

ni trate^

air^ ai/

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

0.1 218 260

0.06 170 260

0.04 104 140

0.02 26.0 no

^According to Bethe theory, Eq (2.16). In the comparison, cellulose nitrate is

considered equivalent to collodion {see footnote 18).

-L. Green (see footnote 17).

“^Cole's results are the same for collodion and air.

60
o Table 8.2 Collision stopping power, in MeV/(g cm ), for low-Z materials, calculated according to the Bethe

formula. Eg (2.16), at energies from 10 to 1 keV.

T Hp He Be C N- 0. Ne A«. 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 (keV) A- 150 plastic

acetylene adipose

tissue

Air At.,0,

L 3 B-lOO plastic

bone

(ICRU) bone

(ICRP) C-552

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

(keV)

Cap2 CO

2 cellulose

nitrate

ceric sulfate solution

ethylene ferrous sulfate solutionglass

(Pyrex)

Kapton LiF

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 paraffinwax plastic

scintillator

poly- 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, stil bene TE gas TE gas toluene water water

(keV) (methane (propane (liquid) vapor

basedbased

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

10.1.

Dependence

of

the

c.s.d.a.

range

on

the

assumed

residual

range

at1

keV.

The

quantity

given

is

the

ratio r

/r.

The

value r

is

calculated

according

to

Eq

(10.2).

The

more

accurate

value ri

in00

CO

00

00

tocn

scu5o

CL

CL

CLoc

d)CD

(O3

“O

•r"in

:> (Us.

O) XI

-l-> CDc3

Q.EO

-o

(Uco

62
Table

11.1

Positron/electron

collision

stopping

power

and

range

ratios.

The

Table

11.2

Comparison

of

positron/electron

collision

stopping-power

ratios

density-effect

correction

was

taken

from

Inokuti

and

Smith

(1982)

and

restricted-stopping-power

ratios

in

liquid

water.

Results

for

At,

from

Ashley

(1982b)

for H

2

O,

and

was

calculated

according

were

calculated

using

density-effect

corrections

obtained

from

to

Sternheimer

for

the

other

materials.

Sternheimer'

s

method.

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r— OOOOr-i— r-f— rm CO o o VO u>

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1—

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1 0 0 r^r^r^r^r^rv-tOLOLDr^cocMLOCOCMun W O) to <c 0 0 0 0 0 0 0 0 0 0 0 0 0 0 r— r— OOOOOOOOOOOr— 1— 1— r-rH- + 0 r—0

+ U

c/> LO^cofOcMf— »“ 0 *— r^«— oo»— r>-cMCM 3 r^r^r^r^r^r^r^r^r^r^ocMLor^i— 3 0 OOOOOOOOOOOOOOf— r— 0 OOOOOOOOOOOi— 1— »— r— f—

vovOLf>«;:3-rocM »—

— cMr^CDCoror^r».a> r^r^r^r^r^r^r^r^r^r^cOr— «^ocT)r— 0? <c 0 CD CT) (T» CTi CT) O) 0> CD O (J) O O O O r— c OOOOOOOOodcDi— r-r- C— f—

CO CO E E u VDVDL0 «=l-^CMCMCM'NrC0 OL0 CJ>O«Cl-CM u

covoooo \ 0 0 o^O) 0)cyio^o^o^o^c^»o^CT^oooor— 0 C3)

r>. OOOodoOoddcDi— r-r-i— •—

r— , m CM 1—

vn CM 1— 0 0 0

> > OOOOOOOlDCMi— 000000 h- <D h- <U 0 0 0 0 Lf) CM 1— 2: s: 0 Lf) CM I—

'

»“

o»— ^r^OCMC0CMrs.r^r— vor>.ococM Or-f— I— CMCMCMCMi—OOlO^COOO 00000000000000000

•— I— I— r-p-r-r-r-r-i— 000000

OCMVOOCMLf>inCOr^r^CMrN.OOr— r-lf> I— I— f— r-CMCMCMCMf— OOvD«;fCOr-0 00000000000000000

f-f— I— •— »— r-i— f— r— r-OOOOOO

r>.ooocM^r«*Or— voir)ir)oor^CM^vo 000 «— •— I— CMCNJf— OOO'tTr— COCMUT) ooooooooooooooooor^

r-«— I— r-r-i— r-OOOOOO

cooi— covoococMr-Hvor^oovoocMCM 00 «— •— •— CMCMCMi— OCOCOCMOVDCM OOOOOOOOOOOOOOCOCO

^^^r-r-r-OOOOOO

coocM^tJ-r^f— comr^Lnr««.LncMOvDMD 00 »— »— r-CMCMCMf— OCOtf)COOr^«a- OOOOOOOOOOOOOOCOCO

I— I— f— I— r— r— f— I— 000000

O'— — c\iOi— loco Or-'«— I— CMCMCMCMf— OOvD^CMOr^ OOOOOOOOOOOOOOCOCO

r-i— I— I— •— I— I— »— 000000

ocovoocoLOLn^a-r^r^r-^or^i—o^^-

•— 1— r— CMCMCSJCMCMi— OOVD«tTCO<— O oooooooooooooooco

I— r-i— I— I— r-i— 000000

Lf) CM I—

LD CM 1— 000

OOOOOOOuftCMi— 000000 O O O O Lf> CM ^ O Lf) CM ^

63
</> "O E <0 to O c O r—

•I- ro i- fO

4-> 4- O -I- C OJ U w o c :c cu ^ IT3 <TJ O E

>«-> ^-

QJ •!- 5 r- o •— CL o

O.T- Q.-0 O 3

I/) - ‘ <u

<T3 ^ -C 5 c\j +J CO o

c cr» o I— <u

Q. 0) X *-> UJ (/>

»— CVJCVJtOVOtOOOO

CVJCNJCSJr— oooooooo ^^CVJr—

+1 +l +l +1 +1 +l +l +1 ^orocvjOCT>vor^ OOOOOOOrCO <y» 00 CO o o o o o+1 +1 +1 +1 +l ^cotococ>>

<\J to r- r«» CO

CM ctj CsJ I— I—

00

<0 ^ CM CM CM CM o o o o

o o o o

to to

Oi 0) m

to CM

i.0 </) U <C 1-

I cu

: E E

I U O TL <U L. <u ^ t|- x:c

: CD 1.

1 «=>? CD

L >>< 4->

CT»*>l-COCOOUOCT»tO CMOtOOOmOOC>*C*«‘ Or-OOOOO*— o r*«. CM to CO

CM CM CM f— r~

IT) CO CO ^ ^ CO 00 O CO

*o Jl

CO to CO CM

lO to CO

^ «t < M

OOCOCOCOOOOOCOCO

CMCMCMCMCMCMCMCM

00 GO CO CO CO

CM CM CM CM CM ^ to ^ O

r- f— rs. o>

-I <t ^ M

o Q. C ^ O

to <3

- m to

CT> •• CO r— to CO CO CO 0% CO •

O QJ fO C «T3

z> ^ < <c

CM 0> 'tJ ^ X C I— 0) V,

4-> 0>

0>

i/i CM

r>. o CO

• cx. • E Oo

u

>» >*

o

>>

<D X (D 0> (U (D \ CO Q.CQCOOOOO OirQ

•r- U fO CTl <X ^ C7>z 2lcC(/):>^^

4-> C

I u <D

I <C O rQ

f— o to to X CO X X

r**> X to to 0 0 0,0 O Q) ^

Q. JO o "a

<o to o>

a o «—

to "O r—

a a rCi a « rQ o a <j a a o

E

o

<D

t/>

o

E

0>Q.X

LlI

*o

a>fO

<0 o

too I— r— CM OCM O O O o o o o o o o o o

+1 +1 +1 +1 +1 +1 +l +1 +l +l +1 +1 to CO ^ o

CO o>

LD CO «d' CO ^ o

CO CO

CO «:t CM CM r— CM

<Ttir)co ir)CM«a- to cm co to ^ Lf> O to I— ^ ^ to CO to

r- I— CM

(U CQ o.

to

o%

00

CM ^

oCM X

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 al. (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‘d (liquid)

Stopping Power

Collision Radiative Total

T

(MeV)

1

P B&S Pages

i

p B&S Pages

ls(T)

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 Range

BSS Pages

Radiation

Yield

Y(T)

B&S Pages

-3.1

-2.2 -1.9

-1.7

-0.2

0.8

-14.3 -2.3

-1.9

-2.2

- 2.8

32.3

18.7

35.5

2.4

-0.8

-0.3

15.3 20.3

39.2 1.0

-2.2

^Density effect calculated according to Sternheimer in B&S, 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^

Stopping Power csda Range

Radiation

VIolH

Collision Radiative Total

T (MeV)

i

P i

P 1S(T) ^o(T) Y(T)

B&S Pages B&S Pages B&S Pages B&S Pages 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

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 5.6 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
0.01 0.1 1 10 100 1000

T, MeV

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

IBIS

>0) N

14

12 —

10

Curve A:

Curve B:

Curve

Calculated by Dehmer et al. (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 Hartree- Slater 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 Hartree-FockSlater 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).

3(3 40 50^

ATOMIC NUMBER Z

Fig. 3.2. Theoretical mean excitation energies for elements.

66
0.35

67
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
DTVDs/ -l^«5

r— —

»— »—

(O >> >» ^ 0> 0> c ^ I— a; O) r— ot^

t/> O C r—

P- 01

•*- >»

O) U ITS O -C“ o

CO CD -J 3 O

• < O X -f 0

ro o%

LO I—

4-> E •—

<U ^ r««i 4-» Q 3^ CO <3

ITS C to •XO

f— O) +i-J ‘t^O^+S 3 0> OS Q »— <i) U >» TS Q

r— X t/> C +i *0

Its O T3 fO +i 0) *P- C

0) "O to

; u c o u

: u •»“ 3

I 0) 2 O O

: ^ CO oc CO

o f—

69

Fig.

4.3.

Ratio

of

experimental

to

calculated

proton

stopping

powers.
1.01 -1—^—

—I—^—

—I—I—I—^—

1.00 o_i<

a

ifi

CLXHi CO 0.99

A

ISHIWARI, SHIOMI AND SAKAMOTO - 6.5-MeV PROTONS

0.98 I I I I I I I ^ L_1 J 1 L 0 10 20 30 40 50 60 70 80

Fig. 4.4, Ratio of experimental to calculated proton stopping powers at 6.5 MeV. Experimental data are from Ishiwari (1979).

1.01 T 1 T T—T—T-7—^T~'i—j—n-j

o-J<

o

(O

1.00

• ••

Q.XLU CO

0.99 -

0.98 —

BURKIG & MACKENZIE

19.8-MeV PROTONS

I 1 I I L_j L_j I I I I I I 10 20 30 40 50 60 70 80

Fig. 4.5. Ratio of experimental to calculated proton stopping powers at 19.8 MeV. Experimental data are from Burkig and Mackenzie (1957).

70
900

71
PERCENT

CHANGE

IN

8^0!

Fig. 6.3. Difference between the density-effect correction calculated by

Ashley (1982b) using a semi -empirical dielectric function for water,

and the corresponding value 6^^ obtained by Sternheimer 's method.

The latter was calculated with I = 75.4 eV, to match the I-value

for water found by Ashley.

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.

72
Fig. 8.1. Calculated electron collision stopping power below 10 keV in water. Curve 12

34

56

7

water vapor water vapor water vapor

liquid water

liquid water

liquid water

liquid water

Berger (see footnote 16)

Green (see footnote 17)

Bethe fonmila, Eq (2.16), with I = 71.6 eV Kutcher and Green (1976)

Ritchie et al. (1978)

Ashley (1982a)

Bethe formula, Eq (2.16), with I = 75.0 eV.

73
u

O)2

o

a.

ro

CO

u.

CD ' CO '

S=o

w

>»

•M

O

Q.

~o

fl5

<u

s:

OJ

4-^ o;o

o.

a.

Q.o

o

L, 4-> (JV

0>

cO P5 csj o" O) cr 0) <y»

• yj UJ ^ •* ^ cvj W-

^ • « • • (j <o ro cs: • CnJ 14- I— lO f— «^0 CO O 3 3 a 0> S tl £ tl ^

r- di i. i. +i 3 O O • 0) I— ^ »4- >> f >C >>

0) > 0) 4^ OJ -M 0> ^ I ^ -p- JZ -f- I— ^>—14^ 2 4-J 2 ^ OJ <U

0) c

a;

4-> <U>>o

a.

o»>

3O

CQ

01c

o;

jC

4-» 0> o

CL

CM

CD

0) c

(U

0? >>o

Q.

CM

«3 00 — VO 3

£ II L.O l-H 4-

o; -C T-

•*-> 3

OJ CO

0) 0) c c

0) q;

&- &- >> >»

+-> 4->

(/) l/» o "o a. Q.

74
75
cnc —^-D »r- C ro -M

-e- ^3

^ (/) -O l/> cu <o o

-e- ^

>»

in s.

c: (U o c

•f- <u U 0) 0> >

t/> •»-

cn cn *rQ) £1

4-)

£

d)

s.

OJ «/>•*-

o;

s.Q.

<U

4->^-0

ro 0) ro

•I S- TD -efKS M &.

•M C (t) O'*-' s. •M -©-

>> -- I— fO

(1> c

> o

u s- 0) o

Q. Q.

in o

0) &.

&. o.

M (/)

jr2

7b
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, A£, and Au. ^ Aiginger (1966), for AJI2O 0 and Au.

o Rester and Dance (1967), Res ter and Edmonson (1972) and

Rester (private communication) for AA, Cu, Sn, and Au.

77
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)

Ishigure et al. (1978)

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:

II 2

, He, Be, C (grapliite) , N

2

, O

2

, Ne, A£, Si, Ar , Ti, Fe, Gu , 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,

aluminum , copper , silver , lead , air , polymethylmethacrylate, and water.

Gontent 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 Scol > Lhe mass radiative stopping power, 1/p and the total mass stopping power, 1/p ^/P Sj-aj, all in units of MeV/(g cm"^); the c.s.d.a.

range, rQ, in units of g cm' ^ ; 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

tlie 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, tissueecjuivalent 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^, and the other for a typical bulk density of 1.7 g/cm^. It is

recommended that tliese 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/cm3 (200 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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 5. 125E+01 9.702E-09 5.125E+01 1 .076E-09 1 . 029E-05 0.0 -0.156 0.172 0.172

0.0125 9.271E+01 9.793E-09 9.271E+01 1 .61 3E-09 1 .292E-05 0.0 -0.151 0.166 0.166 0.0150 3.682E+01 9.881E-09 3.682E+01 2.295E-09 1 .950E-05 0.0 -0.197 0.161 0.161 0.0175 3.299E+01 9 . 969E-09 3.299E+01 2.970E-09 1 .659E-05 0.0 -0.199 0.158 0.157

0 . 0200 2.917E+01 1 .009E-03 2. 917E + 01 3.783E-09 1 .859E-05 0.0 -0.191 0.159 0.159

0.0250 2.939E+01 1 .01 9E-03 2.939E+01 5.667E-09 2.296E-05 0.0 -0.137 0.199 0.199

0.0300 2. 1 10E+01 1 .039E-03 2.1 10E+01 7.878E-09 2.628E-05 0.0 -0.139 0.195 0.195

0.0350 1 .870E+01 1 .098E-03 1 .870E+01 1 .090E-03 3.003E-05 0.0 -0.131 0.192 0.192

0 .O'iOO 1 .687E+01 1 .061E-03 1 .687E+01 1 .322E-03 3.371E-05 0.0 -0.129 0.190 0.139

0 . 0«(50 1 .592E+01 1 .079E-03 1 .592E+01 1 .632E-03 3.733E-05 0.0 -0.127 0.138 0.137

0.0500 1 .929E+01 1 .088E-03 1 .929E+01 1 . 970E-03 9.090E-05 0.0 -0.126 0.136 0.135

0 .0550 1 .327E+01 1 .101E-03 1 . 327E+01 2.339E-03 9.993E-05 0.0 -0.129 0.139 0.139

0.0600 1 .295E+01 1.11 3E-03 1 .295E + 01 2.729E-03 9.791E-05 0.0 -0.123 0.133 0.132

0 .0700 1 . 1 19E+01 1 . 1 38E-03 1 . 1 19E + 01 3.575E-03 5.975E-05 0.0 -0.121 0.130 0.130

0 . 0800 1 .015E+01 1 . 1 69E-03 1 .015E+01 9.517E-03 6.196E-05 0.0 -0.119 0.128 0.127

0.0900 9 . 367E+00 1 . 1 90E-03 9.368E+00 5.593E-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 7.957E-05 0.0 -0.116 0.125 0.129

0.1250 7.590E+00 1 .285E-03 7.592E+00 9.732E-03 9.050E-05 0.0 -0.113 0.121 0.121

0 . 1 500 6.81 9E+00 1 .357E-03 6.820E+00 1 .322E-02 1 .061E-09 0.0 -0.111 0.119 0.118

0.1750 6.266E+00 1 .933E-03 6 .267E + 00 1 .705E-02 1 .215E-09 0.0 -0.109 0.117 0.116

0.2000 5.851E+00 1 .51 IE-03 5.852E+00 2. 1 18E-02 1 .367E-09 0.0 -0.108 0.115 0.115

0.2500 5.275E+00 1 .677E-03 5.276E+00 3.021E-02 1 .670E-09 0.0 -0.105 0.113 0.112

0 . 3000 9.898E+00 1 .852E-03 9.899E+00 9.007E-02 1 .971E-09 0.0 -0.103 0.111 0.110

0 . 3500 9.635E+00 2.038E-03 9.637E+00 5.057E-02 2.273E-09 0.0 -0.102 0.109 0.108

0.9000 9.995E+00 2.232E-03 9.997E+00 6.159E-02 2.577E-09 0.0 -0.100 0.107 0.106

0.9500 9.302E+00 2.936E-03 9.305E+00 7.303E-02 2.889E-09 0.0 -0.099 0.106 0.105

0 . 5000 9. 1 93E+00 2.698E-03 9.196E+00 8.980E-02 3.199E-09 0.0 -0.098 0.105 0.103

0.5500 9.109E+00 2.869E-03 9.111E+00 9.689E-02 3.508E-09 0.0 -0.097 0.109 0.102

0.6000 9.092E+00 3.096E-03 9.095E+00 1 .091E-01 3.825E-09 0.0 -0.096 0.103 0.101

0 .7000 3. 995E+00 3.573E-03 3.999E+00 1 .391E-01 9.971E-09 0.0 -0.099 0.102 0.100

0.8000 3.883E+00 9.076E-03 3.887E+00 1 .597E-01 5.133E-09 0.0 -0.093 0.100 0.098

0 . 9000 3.892E+00 9.603E-03 3.897E+00 1 .856E-01 5.809E-09 0.0 -0.091 0.099 0.097

1 .0000 3.816E+00 5.152E-03 3.821E+00 2.117E-01 6.501E-09 0.0 -0.090 0.098 0.096

1 .2500 3.787E+00 6.619E-03 3.799E+00 2.779E-01 8.289E-09 0.0 -0.088 0.096 0.093

1 .5000 3.788E+00 8. 1 90E-03 3.796E+00 3.933E-01 1 .016E-03 0.0 -0.086 0.099 0.091

1 . 7500 3.802E+00 9.862E-03 3.812E+00 9.090E-01 1 .209E-03 0.0 -0.085 0.093 0.089

2.0000 3.823E+00 1 . 162E-02 3.835E+00 9.799E-01 1 .909E-03 0.0 -0.083 0.091 0.088

2.5000 3.873E+00 1 .539E-02 3.888E+00 6 .039E-01 1 .829E-03 0.0 -0.081 0.089 0.086

3.0000 3. 929E+00 1 .931E-02 3.993E+00 7.316E-01 2.257E-03 0.0 -0.079 0.088 0.089

3.5000 3.973E+00 2.398E-02 3.997E+00 8.575E-01 2.703E-03 0.0 -0.078 0.086 0.082

9 .0000 9 . 020E+00 2.782E-02 9.097E+00 9.818E-01 3.162E-03 0.0 -0.077 0.085 0.081 9.5000 9.063E+00 3.230E-02 9.095E+00 1 .105E+00 3.631E-03 0.0 -0.076 0.089 0.080

5.0000 9.103E+00 3.693E-02 9.190E+00 1 .226E+00 9.108E-03 0.0 -0.075 0.083 0.079

5 . 5000 9. 190E+00 9.166E-02 9. 182E+00 1 .396E+00 9.593E-03 0.0 -0.079 0.082 0.078

6 .0000 9. 175E+00 9.651E-02 9.222E+00 1 .965E+00 5.089E-03 ,0.0 -0.079 0.082 0.077

7.0000 9.239E+00 5.697E-02 9.295E+00 1 .700E+00 6.083E-03 0.0 -0.072 0.080 0.076

8.0000 9.295E+00 6.675E-02 9.361E+00 1 .931E+00 7.101E-03 0.0 -0.071 0.079 0.079

9.0000 9.395E+00 7.731E-02 9.922E+00 2. 159E+00 8.133E-03 0.0 -0.070 0.078 0.073

10.0000 9.391E+00 8.809E-02 9.979E+00 2.383E+00 9.177E-03 0.0 -0.070 0.077 0.072

12.5000 9.988E+00 1 . 159E-01 9.609E+00 2.939E+00 1 . 183E-02 0.0 -0.068 0.075 0.070

15.0000 9.569E+00 1 .998E-01 9.719E+00 3.970E+00 1 .951E-02 0.0 -0.067 0.079 0.069

17.5000 9 .638E+00 1 .799E-01 9.81 3E+00 3.995E+00 1 .722E-02 0.0 -0.066 0.073 0.068

20.0000 9.698E+00 2.096E-01 9.903E+00 9.510E+00 1 . 999E-02 0.0 -0.065 0.071 0.066

25.0000 9.799E+00 2.667E-01 5.065E+00 5.513E+00 2.590E-02 0.0 -0.069 0.070 0.069

30 .0000 9 .881 E+00 3.305E-01 5.212E+00 6 .985E+00 3.089E-02 0.0 -0.063 0.068 0.063

35.0000 9.951E+00 3.955E-01 5.397E+00 7.932E+00 3.625E-02 0.0 -0.062 0.067 0.061 90.0000 5.010E+00 9.615E-01 5.971 E+00 8.357E+00 9. 161E-02 1 .250E-02 -0.052 0.065 0.060

95.0000 5.055E+00 5.283E-01 5.583E+00 9.261 E+00 9.693E-02 6 .872E-02 -0.091 0.063 0.056

50.0000 5.091E+00 5. 959E-01 5.686E+00 1 .015E+01 5.221E-02 1 .509E-01 -0.033 0.060 0.051 55.0000 5. 120E+00 6.690E-01 5.789E+00 1 .102E+01 5.795E-02 2.952E-01 -0.027 0.058 0.097

60.0000 5. 199E+00 7.326E-01 5.876E+00 1 . 188E+01 6.269E-02 3.959E-01 -0.023 0.055 0.093

70.0000 5. 183E+00 8.713E-01 6 .059E+00 1 .355E+01 7.288E-02 5.519E-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 7.513E-01 -0.013 0.096 0.031 90.0000 5.238E+00 1 . 153E+00 6.391E+00 1 .677E+01 9.277E-02 9.905E-01 -0.010 0.093 0.026

100 .0000 5.259E+00 1 .295E+00 6 .559E+00 1 .831E+01 1 .029E-01 1 . 1 18E+00 -0.008 0.090 0.023

1 25 .0000 5.301 E+00 1 . 659E+00 6.955E+00 2.202E+01 1 .255E-01 1 .513E+00 -0.005 0.039 0.017

150.0000 5 . 333E+00 2.017E+00 7.350E+00 2.551E+01 1 .973E-01 1 .899E+00 -0.009 0.030 0.013

175.0000 5.359E+00 2.383E+00 7.792E+00 2.882E+01 1 .679E-01 2. 190E+00 -0.003 0.027 0.010

200.0000 5.381E+00 2.752E+00 8.1 33E+00 3.1 98E+01 1 .873E-01 2. 396E+00 -0.002 0.029 0.008

250.0000 5.917E+00 3 . 996E+00 8.913E+00 3.785E+01 2.231E-01 2.828E+00 -0.001 0.021 0.006

300.0000 5.996E+00 9 .296E+00 9.692E+00 9.322E+01 2.552E-01 3. 186E+00 -0.001 0.018 0.005

350.0000 5.970E+00 5.001E+00 1 .097E+01 9.81 9E+01 2.892E-01 3.989E+00 -0.001 0.016 0.009

900 .0000 5.991E+00 5.760E+00 1 . 125E+01 5.279E+01 3. 106E-01 3.753E+00 -0.001 0.015 0.003

950.0000 5. 509E+00 6 . 522E+00 1 .203E+01 5.709E+01 3.397E-01 3. 987E+00 -0.000 0.019 0.002

500 .0000 5 . 526E+00 7.286E+00 1 .281E+01 6.111E+01 3.568E-01 9.1 96E+00 -0.000 0.013 0.002

550.0000 5.590E+00 8.053E+00 1 .359E+01 6 .990E+01 3.771E-01 9.386E+00 -0.000 0.012 0.002

600 .0000 5.559E+00 8.821E+00 1 .938E+01 6 .898E+01 3.960E-01 9.559E+00 -0.000 0.012 0.002

700.0000 5.577E+00 1 .036E+01 1 .599E+01 7.508E+01 9.298E-01 9.866E+00 -0.000 0.011 0.001 800.0000 5.598E+00 1 . 1 91E + 01 1 .751E+01 8. 107E+01 9.592E-01 5. 1 32E+00 -0.000 0.010 0.001 900.0000 5.616E+00 1 . 396E+01 1 .908E+01 8.659E+01 9.853E-01 5.367E+00 -0.000 0.009 0.001

1000 .0000 5.632E+00 1 .502E+01 2.065E+01 9. 157E+01 5.089E-01 5.577E+00 -0.000 0.009 0.001
ELECTRONS IN HELIUM

I = 61 . 8 eV DENSITY = 1 .663E-06 g/cn>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 cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.267E+01 9.885E-06 2.267E+01 2.667E-06 2.612E-05 0.0 -0.178 0.200 0.200

0.0125 1 .898E+01 9. 961 E-06 1 .898E+01 3.678E-06 2.890E-05 0.0 -0.171 0.191 0.191 0.0150 1 .662E+01 9.995E-06 1 .662E+01 5.098E-06 3.352E-05 0.0 -0.166 0.185 0.185

0.0175 1 .653E+01 1 .005E-03 1 .653E+01 6.720E-06 3.802E-05 0.0 -0.162 0.180 0.180

0.0200 1 .307E + 01 1 .01 OE-03 1 .307E+01 8.537E-06 6.262E-05 0.0 -0.159 0.176 0.176

0.0250 1 .097E+01 1 .020E-03 1 .097E+01 1 .273E-03 5.096E-05 0.0 -0.156 0.169 0.169

0.0300 9.521E+00 1 .029E-03 9.522E+00 1 .766E-03 5 . 923E-05 0.0 -0.150 0.166 0.166

0.0350 8.657E+00 1 .039E-03 8.658E+00 2.322E-03 6 .727E-05 0.0 -0.166 0.160 0.160

O.O'^tOO 7.662E+00 1 .068E-03 7.663E+00 2. 965E-03 7.510E-05 0.0 -0.166 0.157 0.157

0 . 0'»50 6 . 996E+00 1 .057E-03 6 . 997E+00 3.630E-03 8.277E-05 0.0 -0.161 0.156 0.156

0.0500 6.671E+00 1 . 066E-03 6.672E+00 6.376E-03 9.029E-05 0.0 -0.139 0.152 0.152

0 .0550 6 .035E+00 1 .075E-03 6.037E+00 5. 176E-03 9.766E-05 0.0 -0.138 0.150 0.150

0.0600 5.669E+00 1 .086E-03 5.670E+00 6 .029E-03 1 .069E-06 0.0 -0.136 0.168 0.168

0.0700 5 . 086E+00 1 .101E-03 5.085E+00 7.896E-03 1 .191E-06 0.0 -0.133 0.165 0.166

0.0800 6.638E+00 1.11 9E-03 6.639E+00 9.958E-03 1 .328E-06 0.0 -0.131 0.162 0.162

0.0900 6.287E+00 1 . 1 38E-03 6.288E+00 1 .220E-02 1 .662E-06 0.0 -0.129 0.160 0.160

0.1000 6.003E+00 1 . 157E-03 6.006E+00 1 .662E-02 1 .593E-06 0.0 -0.128 0.138 0.138

0 . 1 250 3.686E+00 1 .207E-03 3.687E+00 2.136E-02 1 . 91 OE-06 0.0 -0.126 0.136 0.136

0.1500 3.1 37E+00 1 .260E-03 3.1 39E+00 2.891E-02 2.215E-06 0.0 -0.122 0.131 0.131 0.1750 2.887E+00 1 .316E-03 2.889E+00 3.723E-02 2.51 IE-06 0.0 -0.119 0.129 0.128

0 .2000 2.700E+00 1 .375E-03 2.701E+00 6.61 9E-02 2.800E-06 0.0 -0.118 0.127 0.126

0.2500 2.639E+00 1 .699E-03 2.661E+00 6.573E-02 3.363E-06 0.0 -0.115 0.126 0.123

0.3000 2.269E+00 1 .632E-03 2.270E+00 8.702E-02 3.916E-06 0.0 -0.112 0.121 0.120

0 . 3500 2. 150E+00 1 .776E-03 2.152E+00 1 .097E-01 6.657E-06 0.0 -0.110 0.119 0.118

0.6000 2.066E+00 1 . 926E-03 2.066E+00 1 .336E-01 6.997E-06 0.0 -0.109 0.117 0.116

0.6500 2.000E+00 2.081E-03 2.002E+00 1 .580E-01 5.536E-06 0.0 -0.107 0.116 0.116

0 . 5000 1 . 952E + 00 2.265E-03 1 .956E+00 1 .833E-01 6.076E-06 0.0 -0.106 0.116 0.113

0.5500 1 . 916E + 00 2.616E-03 1 .916E+00 2.092E-01 6.619E-06 0.0 -0.106 0.113 0.112

0.6000 1 .886E+00 2.592E-03 1 .887E+00 2.355E-01 7. 165E-06 0.0 -0.103 0.112 0.110

0 .7000 1 .862E + 00 2.961E-03 1 .865E+00 2.891E-01 8.269E-06 0.0 -0.101 0.110 0.108

0.8000 1 .81 5E+00 3.350E-03 1 .818E+00 3.637E-01 9.389E-06 0.0 -0.100 0.109 0.106

0.9000 1 .798E+00 3.757E-03 1 .801E+00 3.990E-01 1 .053E-03 0.0 -0.098 0.107 0.105

1.0000 1 .787E+00 6. 180E-03 1 .791E+00 6.567E-01 1 . 168E-03 0.0 -0.097 0.106 0.103

1 .2500 1 .777E+00 5. 306E-03 1 .782E+00 5.967E-01 1 .665E-03 0.0 -0.096 0.106 0.101 1.5000 1 .780E+00 6.515E-03 1 .787E+00 7.369E-01 1 .773E-03 0.0 -0.092 0.102 0.098

1 .7500 1 .789E+00 7.793E-03 1 .797E+00 8.766E-01 2.089E-03 0.0 -0.090 0.100 0.096

2.0000 1 .801 E+00 9.1 32E-03 1 .810E+00 1 .013E+00 2.616E-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 -0.087 0.096 0.092

3.0000 1 .856E + 00 1 .695E-02 1 .869E+00 1 .557E+00 3.779E-03 0.0 -0.085 0.096 0.090

3.5000 1 .880E+00 1 .809E-02 1 .898E+00 1 .822E+00 6.691E-03 0.0 -0.083 0.093 0.088

6 .0000 1 . 903E+00 2. 136E-02 1 .925E+00 2.086E+00 5.218E-03 0.0 -0.082 0.091 0.086

6.5000 1 . 925E + 00 2.669E-02 1 .950E+00 2.362E+00 5.957E-03 0.0 -0.081 0.090 0.085

5.0000 1 . 966E+00 2.81 3E-02 1 .976E+00 2.597E+00 6.706E-03 0.0 -0.080 0.089 0.086

5.5000 1 . 965E+00 3. 165E-02 1 .997E+00 2.868E+00 7.665E-03 0.0 -0.079 0.088 0.083

6.0000 1 . 983E + 00 3.523E-02 2.018E+00 3.098E+00 8.231E-03 0.0 -0.078 0.087 0.082

7.0000 2.01 5E+00 6.260E-02 2.057E+00 3.588E+00 9.781E-03 0.0 -0.077 0.086 0.080

8.0000 2.063E+00 5.018E-02 2.093E+00 6.070E+00 1 .135E-02 0.0 -0.075 0.086 0.079

9.0000 2.069E+00 5.793E-02 2.126E+00 6.566E+00 1 .293E-02 0.0 -0.076 0.083 0.077

10.0000 2.092E+00 6.586E-02 2.157E+00 5.01 lE+00 1 .653E-02 0.0 -0.076 0.082 0.076

12.5000 2.161E+00 8.617E-02 2.227E+00 6.151E+00 1 .855E-02 0.0 -0.072 0.080 0.076

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-01 2.365E+00 8.337E+00 2.662E-02 0.0 -0.069 0.077 0.071 20.0000 2.267E+00 1 .505E-01 2.397E+00 9.391E+00 3.066E-02 0.0 -0.068 0.075 0.069

25.0000 2.297E+00 1 .952E-01 2.693E+00 1 . 166E+01 3.863E-02 0.0 -0.067 0.073 0.067

30.0000 2. 339E+00 2.610E-01 2.580E+00 1 .361E+01 6.651E-02 0.0 -0.066 0.071 0.065

35.0000 2.376E+00 2.875E-01 2.662E+00 1 .531E+01 5.626E-02 0.0 -0.065 0.070 0.063

60.0000 2.605E+00 3.366E-01 2.739E+00 1 .717E+01 6.187E-02 0.0 -0.066 0.068 0.062

65.0000 2.632E+00 3.822E-01 2.816E+00 1 .897E+01 6. 933E-02 0.0 -0.063 0.067 0.060

50.0000 2.656E+00 6.303E-01 2.886E+00 2.072E+01 7.665E-02 0.0 -0.063 0.066 0.059

55.0000 2.678E+00 6.786E-01 2.956E+00 2.263E+01 8.382E-02 0.0 -0.062 0.065 0.058

60.0000 2.698E+00 5.272E-01 3.025E+00 2.610E+01 9.085E-02 0.0 -0.062 0.066 0.057

70.0000 2.533E+00 6.252E-01 3. 158E+00 2.736E+01 1 .065E-01 0.0 -0.061 0.062 0.055

80.0000 2.566E+00 7.239E-01 3.288E+00 3.066E+01 1 .176E-01 0.0 -0.060 0.061 0.056

90.0000 2.589E+00 8.231E-01 3.612E+00 3.363E+01 1 .301E-01 2. 162E-02 -0.068 0.059 0.051 100.0000 2.609E+00 9.229E-01 3.532E+00 3.631E+0I 1 .623E-01 7.861E-02 -0.039 0.057 0.068

125.0000 2.666E+00 1 . 1 76E+00 3.818E+00 6.31 1E+01 1 .708E-01 2.879E-01 -0.026 0.051 0.039

150.0000 2.668E+00 1 .627E+00 6.095E+00 6.963E+01 1 .970E-01 5.236E-01 -0.017 0.067 0.032

175.0000 2.686E+00 1 .681E+00 6.367E+00 5.536E+01 2.21 3E-01 7.535E-01 -0.012 0.063 0.027

200 .0000 2.700E+00 1 . 937E+00 6.637E+00 6.090E+01 2.639E-01 9.696E-01 -0.009 0.039 0.023

250.0000 2.722E+00 2.651E+00 5. 173E+00 7.110E+01 2.866E-01 1 .356E+00 -0.006 0.036 0.017

300.0000 2.738E+00 2 . 967E+00 5.705E+00 8.030E+01 3.200E-01 1 .688E+00 -0.006 0.031 0.013

350.0000 2.752E+00 3.686E+00 6.237E+00 8.868E+01 3.516E-01 1 . 976E+00 -0.003 0.028 0.01 1 600.0000 2.763E+00 6 .006E+00 6.768E+00 9.637E+01 3.796E-01 2.230E+00 -0.002 0.026 0.009

650 .0000 2.773E+00 6.527E+00 7 . 300E + 00 1 .035E+02 6.067E-01 2.657E+00 -0.002 0.026 0.007

500.0000 2.781 E+00 5.069E+00 7.831E+00 1 .101E+02 6.275E-01 2.661 E+00 -0.002 0.023 0.006

550.0000 2.789E+00 5.573E+00 8.362E+00 1 .163E+02 6.682E-01 2.867E+00 -0.001 0.022 0.006

600.0000 2.796E+00 6 .097E+00 8.892E+00 1 .221 E+02 6.672E-01 3.017E+00 -0.001 0.021 0.005

700.0000 2.808E+00 7. 167E+00 9.955E+00 1 .327E+02 5.008E-01 3.321E+00 -0.001 0.019 0.006

800.0000 2.818E+00 8. 1 99E+00 1 . 102E+01 1 .622E+02 5.297E-01 3.586E+00 -0.001 0.018 0.003

900.0000 2.828E+00 9.253E+00 1 .208E+01 1 .509E+02 5.567E-01 3.818E+00 -0.001 0.017 0.003

1000.0000 2.836E+00 1 .031 E+01 1 .316E+01 1 .588E+02 5.768E-01 6.027E+00 -0.000 0.016 0.003

81
ELECTRONS IN BERYLLIUM

I = 63.7 eV DENSITY = 1 .898E+00 g/cm ^

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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .862E+01 1 .81 5E-03 1 .863E + 01 3.033E-09 5.937E-05 5.100E-09 -0.193 0.219 0.218

0.0125 1 .569E + 01 1 .81 9E-03 1 .569E+01 9.509E-09 6 .988E-05 7.992E-09 -0.185 0.209 0.208

0.0150 1 . 356E+01 1 .823E-03 1 .356E+01 6 .226E-09 7 .996E-05 1 .031 E-03 -0.179 0.201 0.201 0.0175 1 .202E+01 1 .827E-03 1 .202E+01 8. 187E-09 8.972E-05 1 .359E-03 -0.179 0.195 0.195

0.0200 1 .083E+01 1 .831 E-03 1 .089E+01 1 .038E-03 9.91 9E-05 1 .718E-03 -0.170 0.190 0.190

0.0250 9.11 3E+00 1 .890E-03 9.11 5E+00 1 .599E-03 1 . 1 25E-09 2.569E-03 -0.169 0.183 0.182

0.0300 7 . 923E+00 1 .899E-03 7.925E+00 2.1 39E-03 1 . 300E-09 3.560E-03 -0.159 0.177 0.177

0.0350 7 . 097E+00 1 .859E-03 7.099E+00 2.809E-03 1 .969E-09 9.701 E-03 -0.156 0.172 0.172

0 . 0«i00 6 . 375E+00 1 .870E-03 6.376E+00 3.551E-03 1 .639E-09 5. 978E-03 -0.153 0.168 0.168

0 .0't50 5.891E+00 1 .880E-03 5.893E+00 9.371E-03 1 .799E-09 7.387E-03 -0.150 0.165 0.165

0 . 0500 5.907E+00 1 .891 E-03 5.909E+00 5.262E-03 1 .951E-09 8.920E-03 -0.198 0.162 0.162

0.0550 5 . 097E+00 1 . 902E-03 5.099E+00 6.21 9E-03 2.109E-09 1 .057E-02 -0.196 0.160 0.160

0.0600 9.793E+00 1 . 91 9E-03 9.795E+00 7.291E-03 2.253E-09 1 .239E-02 -0.199 0.158 0.158

0 .0700 9.257E+00 1 . 937E-03 9.259E+00 9.971E-03 2.595E-09 1 .61 9E-02 -0.191 0.159 0.159

0 .0800 3.887E+00 1 .961E-03 3.889E+00 1 . 1 93E-02 2.826E-09 2.093E-02 -0.139 0.151 0.151 0.0900 3.599E+00 1 . 987E-03 3.596E+00 1 .961E-02 3. lOOE-09 2.509E-02 -0.137 0.199 0.198

0.1000 3.358E+00 2.019E-03 3.360E+00 1 .799E-02 3.366E-09 2.997E-02 -0.135 0.197 0.196

0.1250 2.926E+00 2.085E-03 2.928E+00 2.599E-02 9.005E-09 9.359E-02 -0.131 0.192 0.192

0 . 1 500 2.639E+00 2. 160E-03 2.636E+00 3.951E-02 9.619E-09 5.858E-02 -0.128 0.139 0.138

0.1750 2 . 929E+00 2.291 E-03 2.926E+00 9.992E-02 5.200E-09 7.978E-02 -0.126 0.136 0.136

0 . 2000 2.266E+00 2.326E-03 2.269E+00 5.508E-02 5.769E-09 9. 188E-02 -0.129 0.139 0.133

0 . 2500 2.096E+00 2.507E-03 2.099E+00 7.836E-02 6 .865E-09 1 .280E-01 -0.120 0.130 0.129

0 . 3000 1 . 901 E+00 2.709E-03 1 .909E+00 1 .037E-01 7.929E-09 1 .658E-01 -0.118 0.127 0.127

0 . 3500 1 .800E+00 2.919E-03 1 .803E+00 1 .308E-01 8.961E-09 2.093E-01 -0.115 0.125 0.129

0.9000 1 .726E+00 3.1 37E-03 1 .729E+00 1 .591E-01 9.985E-09 2.932E-01 -0.119 0.123 0.122

0 .9500 1 .670E+00 3.372E-03 1 .673E+00 1 .885E-01 1 . lOOE-03 2.81 9E-01 -0.112 0.122 0.120

0 . 5000 1 .627E+00 3.618E-03 1 .631E+00 2. 188E-01 1 .202E-03 3.209E-01 -0.110 0.120 0.118

0 .5500 1 .593E+00 3.875E-03 1 .597E+00 2.998E-01 1 .309E-03 3.583E-01 -0.109 0.119 0.117

0.6000 1 .566E+00 9.139E-03 1 .571E+00 2.819E-01 1 .906E-03 3.956E-01 -0.108 0.118 0.116

0.7000 1 .527E+00 9.693E-03 1 .532E+00 3.959E-01 1 .612E-03 9.682E-01 -0.105 0.115 0.113

0.8000 1 .501E+00 5.277E-03 1 .506E+00 9. 1 18E-01 1 .821E-03 5.379E-01 -0.103 0.113 0.111

0 . 9000 1 .983E+00 5.886E-03 1 .989E+00 9.786E-01 2.033E-03 6.097E-01 -0.101 0.112 0.109

1 .0000 1 .971E+00 6.520E-03 1 .977E+00 5.960E-01 2.298E-03 6.687E-01 -0.099 0.110 0.107

1 .2500 1 .955E+00 8.201E-03 1 .963E+00 7. 162E-01 2.799E-03 8.178E-01 -0.095 0.107 0.103

1 .5000 1 .950E+00 1 .OOOE-02 1 .960E+00 8.873E-01 3.370E-03 9.539E-01 -0.090 0.109 0.100

1 .7500 1 .951 E+00 1 . 1 90E-02 1 .963E+00 1 .058E+00 3.958E-03 1 .078E+00 -0.086 0.101 0.096

2.0000 1 .955E+00 1 .388E-02 1 .969E+00 1 .229E+00 9.562E-03 1 .199E+00 -0.082 0.099 0.093

2 . 5000 1 .966E+00 1 .806E-02 1 .989E+00 1 .568E+00 5.810E-03 1 .905E+00 -0.079 0.099 0.087

3.0000 1 .977E+00 2.297E-02 1 .500E+00 1 .903E+00 7.109E-03 1 .596E+00 -0.066 0.090 0.081

3 . 5000 1 .989E+00 2.707E-02 1 .516E+00 2.239E+00 8.939E-03 1 .772E+00 -0.059 0.086 0.076

9.0000 1 .999E+00 3. 182E-02 1 .531E+00 2.563E+00 9.795E-03 1 .936E+00 -0.052 0.082 0.070

9.5000 1 .508E+00 3.672E-02 1 .595E+00 2.888E+00 1 . 1 18E-02 2.090E+00 -0.095 0.078 0.065

5 .0000 1 .517E+00 9. 179E-02 1 .559E+00 3.210E+00 1 .259E-02 2.235E+00 -0.090 0.079 0.061 5.5000 1 .525E+00 9.687E-02 1 .572E+00 3.529E+00 1 .902E-02 2.372E+00 -0.035 0.071 0.056

6.0000 1 .532E+00 5.21 IE-02 1 .589E+00 3.896E+00 1 .596E-02 2.502E+00 -0.031 0.067 0.052

7.0000 1 .599E+00 6.283E-02 1 .607E+00 9.973E+00 1 .890E-02 2.793E+00 -0.025 0.062 0.095

8 .0000 1 .555E+00 7.386E-02 1 .628E+00 5.091E+00 2.1 38E-02 2.962E+00 -0.020 0.057 0.039

9.0000 1 .569E+00 8.519E-02 1 .699E+00 5.701E+00 2.939E-02 3.161E+00 -0.016 0.053 0.039

10.0000 1 .572E+00 9.669E-02 1 .669E+00 6.309E+00 2.793E-02 3.399E+00 -0.013 0.099 0.030

12.5000 1 .589E+00 1 .262E-01 1 .715E+00 7.782E+00 3.509E-02 3.793E+00 -0.009 0.092 0.023

15.0000 1 .602E+00 1 .566E-01 1 .759E+00 9.221E+00 9.280E-02 9.079E+00 -0.006 0.036 0.018

17.5000 1 .61 3E+00 1 .878E-01 1 .801E+00 1 .063E+01 5.050E-02 9.368E+00 -0.005 0.032 0.019

20.0000 1 .623E+00 2.1 99E-01 1 .892E+00 1 .200E+01 5.815E-02 9.622E+00 -0.009 0.029 0.012

25 .0000 1 .639E+00 2.890E-01 1 .923E+00 1 .965E+01 7.323E-02 5.051 E+00 -0.002 0.029 0.008

30.0000 1 . 652E+00 3.999E-01 2.002E+00 1 .720E+01 8.792E-02 5.909E+00 -0.002 0.021 0.006

35.0000 1 .663E+00 9. 166E-01 2.079E+00 1 . 965E+01 1 .022E-01 5.705E+00 -0.001 0.018 0.005

90.0000 1 .672E+00 9.891E-01 2. 156E+00 2.201E+01 1 .160E-01 5.967E+00 -0.001 0.016 0.009

95.0000 1 .680E+00 5.523E-01 2.232E+00 2.929E+01 1 .293E-01 6.198E+00 -0.001 0.015 0.003

50.0000 1 .687E+00 6.209E-01 2.308E+00 2.650E+01 1 .922E-01 6.906E+00 -0.001 0.019 0.003

55.0000 1 .699E+00 6.900E-01 2.389E+00 2.863E+01 1 .597E-01 6.599E+00 -0.001 0.013 0.002

60.0000 1 . 700E+00 7.595E-01 2.960E+00 3.069E+01 1 .667E-01 6.766E+00 -0.001 0.012 0.002

70.0000 1 .71 1E+00 8.995E-01 2.610E+00 3.969E+01 1 .896E-01 7.071E+00 -0.000 0.011 0.002

80.0000 1 .720E+00 1 .091E+00 2.761E+00 3.836E+01 2.110E-01 7.336E+00 -0.000 0.010 0.001 90.0000 1 .728E+00 1 . 183E + 00 2.911E+00 9. 189E+01 2.311E-01 7.570E+00 -0.000 0.009 0.001 100.0000 1 .735E+00 1 . 325E+00 3.061E+00 9.529E+01 2.500E-01 7.780E+00 -0.000 0.008 0.001

1 25 . 0000 1 .751 E+00 1 .685E+00 3.936E+00 5.295E+01 2. 926E-01 8.223E+00 -0.000 0.007 0.001

1 50 .0000 1 .763E+00 2.098E+00 3.81 1E+00 5. 985E+01 3.296E-01 8.587E+00 -0.000 0.006 0.001 175.0000 1 .779E+00 2.912E+00 9. 186E+00 6 .61 lE+01 3.621E-01 8.899E+00 -0.000 0.006 0.000

200 .0000 1 .783E+00 2.779E+00 9.561 E+00 7. 183E+01 3.910E-01 9. 160E+00 -0.000 0.005 0.000

250.0000 1 .798E+00 3.516E+00 5.319E+00 8.1 97E+01 9.901E-01 9.605E+00 -0.000 0.005 0.000

300.0000 1.811 E+00 9.256E+00 6 .067E+00 9.077E+01 9.805E-01 9.969E+00 -0.000 0.009 0.000

350 .0000 1 .821 E+00 5.000E+00 6 .821 E+00 9.859E+01 5. 199E-01 1 .028E+01 -0.000 0.009 0.000

900 .0000 1 .830E+00 5.796E+00 7.576E+00 1 .055E+02 5.939E-01 1 .059E+01 -0.000 0.009 0.000

950 .0000 1 .838E+00 6 .999E+00 8.332E+00 1 . 1 18E+02 5.685E-01 1 .078E+01 -0.000 0.003 0.000

500 .0000 1 .895E+00 7 . 292E+00 9.088E+00 1 . 1 75E+02 5. 905E-01 1 .099E+01 -0.000 0.003 0.000

550.0000 1 .852E+00 7 . 993E+00 9.895E+00 1 .228E+02 6.099E-01 1 . 1 18E+01 -0.000 0.003 0.000

600.0000 1 .858E+00 8.799E+00 1 .060E+01 1 .277E+02 6.273E-01 1 . 135E+01 -0.000 0.003 0.000

700.0000 1 .868E+00 1 .025E + 01 1 .212E+01 1 . 365E+02 6 .571 E-01 1 . 166E+01 -0.000 0.003 0.000

800.0000 1 .878E+00 1 . 1 76E+01 1 . 369E+01 1 .993E+02 6 .818E-01 1 . 1 93E+01 -0.000 0.003 0.000

900.0000 1 .886E+00 1 . 327E+01 1 .51 5E+01 1 .51 3E+02 7.026E-01 1 .21 6E+01 -0.000 0.003 0.000

1000.0000 1 .893E+00 1 .978E+01 1 .667E+01 1 .575E+02 7.209E-01 1 .237E+01 -0.000 0.002 0.000

82
ELECTRONS IN CARBON (GRAPHITE)

I = 78.0 eV DENSITY = 2.265E+00i g/cm^

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. ddoo1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.01AE+01 3.150E-03 2.01 AE+01 2.820E-0A 8.665E-05 2.766E-03 -0.200 0.229 0.228

0.0125 1 .69AE + 01 3. 161E-03 1 .69AE+01 A. 1 79E-0A 1 .036E-0A 3.5A3E-03 -0.191 0.218 0.217

0.0150 1 .A71E+01 3. 168E-03 1 .A71E+01 5.768E-0A 1 . 1 99E-0A A.353E-03 -0.185 0.210 0.209

0.0175 1 . 305E + 01 3. 172E-03 1 .305E+01 7.576E-0A 1 . 355E-0A 5.1 95E-03 -0.179 0.203 0.202

0.0200 1 . 177E + 01 3. 176E-03 1 . 177E+01 9.596E-0A 1 .506E-0A 6 .068E-03 -0.175 0.198 0 . 1 97 0.0250 9.91 1E+00 3. 18AE-03 9.915E+00 1 . A2AE-03 1 .796E-0A 7 . 907E-03 -0.168 0.189 0.189

0.0300 8.62AE+00 3.19AE-03 8.628E+00 1 . 967E-03 2.07AE-0A 9.86AE-03 -0.163 0.183 0.182

0.0350 7.677E+00 3.20AE-03 7.680E+00 2.582E-03 2.3A0E-0A 1 . 1 9AE-02 -0.159 0.177 0.177

0 .OAOO 6.9A8E+00 3.215E-03 6.951E+00 3.268E-03 2.597E-0A 1 .A12E-02 -0.156 0.173 0.173

0 . 0A50 6 . 370E+00 3.228E-03 6.373E+00 A.020E-03 2.8A7E-0A 1 .6A0E-02 -0.153 0.170 0.169

0 .0500 5.899E+00 3.2A1E-03 5.902E+00 A.836E-03 3.090E-0A 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-0A 2.127E-02 -0.1 A8 0.16A 0.163

0.0600 5. 177E+00 3.270E-03 5.181E+00 6.650E-03 3.559E-0A 2.38AE-02 -0.1A5 0.161 0.161

0 . 0700 A . 650E+00 3.303E-03 A.653E+00 8.691E-03 A.009E-0A 2. 926E-02 -0. 1 A2 0.157 0.157

0 .0800 A.2A7E+00 3. 337E-03 A.250E+00 1 .09AE-02 A.AA3E-0A 3.500E-02 -0.139 0.1 5A 0.153

0.0900 3. 929E+00 3. 375E-03 3. 932E+00 1 .339E-02 A.862E-0A A.105E-02 -0.136 0.151 0.150

0 . 1 000 3.671 E+00 3. A1 AE-03 3.675E+00 1 .603E-02 5.270E-0A A.738E-02 -0 . 1 33 0.1 A8 0.1 A8 0.1250 3.201E+00 3.523E-03 3.205E+00 2.33AE-02 6.2A6E-0A 6.A29E-02 -0.128 0.1 A2 0.1 A2

0 . 1 500 2.883E+00 3.6A0E-03 2.887E+00 3. 158E-02 7.173E-0A 8.253E-02 -0. 12A 0.138 0.137

0.1750 2.65AE+00 3.76AE-03 2.658E+00 A.062E-02 8.061E-0A 1 .01 9E-01 -0.120 0.1 3A 0.1 3A 0.2000 2.A82E+00 3.896E-03 2. A86E+00 5.036E-02 8.919E-0A 1 .221E-01 -0.116 0.131 0.130

0 . 2500 2.2A1E+00 A. 179E-03 2.2A5E+00 7.160E-02 1 .056E-03 1 .6AAE-01 -0.110 0.126 0.125

0 . 3000 2.083E+00 A.A89E-03 2.087E+00 9. A7AE-02 1 .215E-03 2.086E-01 -0.105 0.121 0.120

0.3500 1 . 972E+00 A.820E-03 1 .977E+00 1 . 1 9AE-01 1 .369E-03 2.537E-01 -0.100 0.117 0.116

O.AOOO 1 .891 E + 00 5.173E-03 1 .896E+00 1 . A52E-01 1 .521E-03 2. 992E-01 -0.096 0.11A 0.112

0 .<*500 1 .830E + 00 5.5A5E-03 1 .835E+00 1 .721E-01 1 .671E-03 3. AA7E-01 -0.092 0.111 0.108

0 . 5000 1 .782E+00 5. 935E-03 1 .788E+00 1 .997E-01 1 .821E-03 3.899E-01 -0.089 0.108 0.105

0 . 5500 1 . 7A5E+00 6.3A0E-03 1 .752E+00 2.279E-01 1 .971E-03 A.3A7E-01 -0.086 0.105 0.102

0.6000 1 .716E + 00 6 .759E-03 1 .722E+00 2.567E-01 2.121E-03 A.788E-01 -0 .08A 0.103 0.100

0.7000 1 .672E + 00 7.637E-03 1 .680E+00 3.156E-01 2.A23E-03 5.6A8E-01 -0.079 0.099 0.095

0.8000 1 . 6A3E + 00 8.559E-03 1 .651E+00 3.757E-01 2.728E-03 6 .A76E-01 -0.076 0.095 0.091 0.9000 1 .623E+00 9.523E-03 1 .632E+00 A.366E-01 3.037E-03 7.272E-01 -0.073 0.092 0.088

1 .0000 1 .609E+00 1 .053E-02 1 .61 9E+00 A.981E-01 3.350E-03 8.03AE-01 -0.070 0.090 0.085

1 .2500 1 .590E+00 1 .318E-02 1 .603E+00 6 .53AE-01 A. 151E-03 9.303E-01 -0.065 0.08A 0.078

1 . 5000 1 . 58AE+00 1 .602E-02 1 .600E+00 8.096E-01 A. 978E-03 1 . 1 AOE+00 -0.062 0.080 0.07A

1 .7500 1 . 58AE+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 2.213E-02 1 .609E+00 1 .121E+00 6.700E-03 1 .A17E+00 -0.057 0 .07A 0.067

2 . 5000 1 .598E+00 2.870E-02 1 .627E+00 1 . A30E+00 8.A97E-03 1 .651E+00 -0.05A 0.070 0.062

3.0000 1.611 E+00 3.561E-02 1 .6A6E+00 1 .736E+00 1 .035E-02 1 .85AE+00 -0.051 0.067 0.059

3 . 5000 1 .623E+00 A.281E-02 1 .666E+00 2.038E+00 1 .225E-02 2.033E+00 -0.0A9 0.06A 0.056

A .0000 1 .636E+00 5.026E-02 1 .686E+00 2.336E+00 1 .A1 9E-02 2.1 9AE+00 -0.0A7 0.062 0.05A

A .5000 1 .6A7E+00 5.792E-02 1 .705E+00 2.631E+00 1 .616E-02 2.3A0E+00 -0 .0A5 0.060 0.052

5.0000 1 .658E+00 6 .576E-02 1 .723E+00 2.923E+00 1 .815E-02 2.A7AE+00 -0 .0A3 0.058 0.050

5.5000 1 .667E+00 7.378E-02 1 .7A1E+00 3.211E+00 2.016E-02 2.598E+00 -0.0A2 0.057 0.0A8

6 .0000 1 .676E+00 8.1 93E-02 1 .758E+00 3.A97E+00 2.21 9E-02 2.713E+00 -O.OAO 0.055 0.0A7

7.0000 1 .693E+00 9.865E-02 1 .791E+00 A.061E+00 2.628E-02 2. 92AE+00 -0.037 0.053 O.OAA

8.0000 1 .707E+00 1 .158E-01 1 .823E+00 A.61 AE+00 3.0A1E-02 3.11AE+00 -0.033 0.050 0.0A1 9.0000 1.71 9E+00 1 .33AE-01 1 .853E+00 5.158E+00 3.A56E-02 3.287E+00 -0.030 0 .0A8 0.039

1 0.0000 1 .730E+00 1 .51 3E-01 1 .881E+00 5.69AE+00 3.872E-02 3.AA6E+00 -0.028 0.0A6 0.036

12.5000 1 .753E+00 1 .971E-01 1 .950E+00 6.999E+00 A.91 AE-02 3.798E+00 -0.022 0.0A2 0.031 15.0000 1 .770E+00 2. AAAE-01 2.015E+00 8.260E+00 5.9A9E-02 A.101E+00 -0.017 0.038 0.027

17.5000 1 .785E+00 2.927E-01 2.077E+00 9.A82E+00 6.973E-02 A.367E+00 -O.OIA 0.035 0.023

20.0000 1 .797E+00 3.A17E-01 2.139E+00 1 .067E+01 7.981E-02 A.60AE+00 -0.011 0.032 0.020

25.0000 1 .81 6E+00 A.A17E-01 2.258E+00 1 .29AE+01 9.9A3E-02 5.012E+00 -0.008 0.028 0.016

30.0000 1 .832E+00 5.A35E-01 2.375E+00 1 .510E+01 1 . 183E-01 5.353E+00 -0.005 0 .02A 0.012

35.0000 1 .8A5E+00 6.A66E-01 2.A91E+00 1 .716E+01 1 .363E-01 5.6A6E+00 -O.OOA 0.022 0.010

AO. 0000 1 .856E+00 7.508E-01 2.606E+00 1 .912E+01 1 .535E-01 5.902E+00 -0.003 0.020 0.008

A5.0000 1 .865E+00 8.559E-01 2.721E+00 2.100E+01 1 .699E-01 6.130E+00 -0.003 0.018 0.007

50.0000 1 .87AE+00 9.617E-01 2.835E+00 2.280E+01 1 .856E-01 6.335E+00 -0.002 0.017 0.006

55.0000 1 .881E+00 1 .068E+00 2.9A9E+00 2. A52E+01 2.007E-01 6.521E+00 -0.002 0.016 0.005

60.0000 1 .888E+00 1 .175E+00 3.063E+00 2.61 9E+01 2.150E-01 6.691E+00 -0.002 0.015 0.005

70.0000 1 .900E+00 1 .391E+00 3.291E+00 2. 93AE+01 2.A20E-01 6.99AE+00 -0.001 0.013 O.OOA 80.0000 1 .91 1E+00 1 .608E+00 3.51 9E+00 3.227E+01 2.667E-01 7.258E+00 -0.001 0.012 0.003

90.0000 1 . 920E+00 1 .826E+00 3.7A6E+00 3.503E+01 2.896E-01 7.A91E+00 -0.001 0.011 0.003

100.0000 1 .928E+00 2.0A6E+00 3.97AE+00 3.762E+01 3.108E-01 7.699E+00 -0.001 0.011 0.002

125.0000 1 . 9A5E+00 2.598E+00 A.5AAE+00 A.350E+01 3.575E-01 8.1A2E+00 -0.000 0.009 0.002

1 50 .0000 1 . 960E+00 3 . 1 55E+00 5. 1 15E+00 A.868E+01 3.971E-01 8.505E+00 -0.000 0.008 0.001 175.0000 1 . 972E+00 3.71AE+00 5.686E+00 5.331E+01 A.312E-01 8.81 lE+00 -0.000 0.008 0.001 200.0000 1 . 982E + 00 A.276E+00 6.258E+00 5.750E+01 A.609E-01 9.077E+00 -0.000 0.007 0.001

250 .0000 1 . 999E+00 5. A05E+00 7.A05E+00 6 . A8AE+01 5. 103E-01 9.522E+00 -0.000 0.006 0.001

300 .0000 2.01 3E+00 6 . 5A0E+00 8.553E+00 7.112E+01 5. A99E-01 9.886E+00 -0.000 0.006 0.001 350.0000 2.025E+00 7 .678E+00 9.703E+00 7.660E+01 5.826E-01 1 .01 9E+01 -0.000 0.005 0.000

AOO . 0000 2 . 035E+00 8 .820E+00 1 .085E+01 8 . 1 A7E+01 6 . 1 01 E-01 1 . 0A6E+01 -0.000 0.005 0.000

A50.0000 2 . OAAE+00 9. 96AE+00 1 .201E+01 8.585E+01 6.335E-01 1 . 070E+01 -0.000 0.005 0.000

500.0000 2 . 052E+00 1.111 E+01 1 . 31 6E+01 8. 983E+01 6.539E-01 1 .091E+01 -0.000 0.005 0.000

550.0000 2 . 060E+00 1 .226E+01 1 . A32E+01 9. 3A7E+01 6.718E-01 1 .110E+01 -0.000 O.OOA 0.000

600 . 0000 2.066E+00 1 . 3A0E+01 1 .5A7E+01 9.683E+01 6 .876E-01 1 .127E+01 -0.000 O.OOA 0.000

700.0000 2.078E+00 1 .570E+01 1 .778E+01 1 .029E+02 7. 1 AAE-01 1 .158E+01 -0.000 O.OOA 0.000

800.0000 2 . 088E+00 1 .801E+01 2.010E+01 1 . 081 E+02 7.363E-01 1 . 185E+01 -0.000 O.OOA 0.000

900 . 0000 2.097E+00 2.031E+01 2.2A1 E+01 1 . 128E+02 7.5A6E-01 1 .208E+01 -0.000 O.OOA 0.000

1000.0000 2.106E+00 2.262E+01 2. A73E+01 1 . 171E+02 7.703E-01 1 .229E+01 -0.000 O.OOA 0.000

83
ELECTRONS IN CARBON (GRAPHITE)

I = 78.0 eV DENSITY = 1 .700E+00 g/cm ^

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^/g MeV cm^/g MeV cm^/g g/cm 2 0.0100 2.019E+01 3. 150E-03 2.019E+01 2.820E-09 8.665E-05 1 . 920E-03 -0.200 0.229 0.228

0.0125 1 .699E+01 3. 161E-03 1 .695E+01 9. 179E-09 1 .036E-09 2.981E-03 -0.191 0.218 0.217

0.0150 1 .971E+01 3 . 1 68E-03 1 .971 E+01 5.767E-09 1 . 1 99E-09 3.073E-03 -0.185 0.210 0.209

0.0175 1 .305E+01 3.172E-03 1 .305E+01 7.575E-09 1 .355E-09 3.695E-03 -0.180 0.203 0.202

0 .0200 1 . 1 77E+0

3. 176E-03 1 . 177E+01 9.595E-09 1 .506E-09 9.397E-03 -0.176 0.198 0.197

0.0250 9.913E+00 3. 189E-03 9.916E+00 1 .929E-03 1 .796E-09 5.736E-03 -0.169 0.189 0.189

0 .0300 8.626E+00 3. 1 99E-03 8.629E+00 1 .966E-03 2.073E-09 7.236E-03 -0.169 0.183 0.183

0.0350 7 .679E+00 3.209E-03 7.682E+00 2.582E-03 2.390E-09 8.893E-03 -0.160 0.178 0.177

0 . OAOO 6 . 950E+00 3.215E-03 6 . 953E+00 3.267E-03 2.597E-09 1 .055E-02 -0.156 0.179 0.173

0 . 0A50 6 . 372E+00 3.228E-03 6.375E+00 9.01 9E-03 2.897E-09 1 .236E-02 -0.153 0.170 0.170

0 .0500 5.901 E+00 3.291E-03 5. 909E+00 9.835E-03 3.090E-09 1 .925E-02 -0.151 0.167 0.167

0 .0550 5.510E+00 3 . 255E-03 5.51 3E+00 5.71 2E-03 3.327E-09 1 .629E-02 -0.199 0.169 0.169

0 . 0600 5. 179E+00 3.270E-03 5. 183E+00 6.698E-03 3.558E-09 1 .832E-02 -0.197 0.162 0.162

0 .0700 9.652E+00 3.303E-03 9.655E+00 8.688E-03 9.008E-09 2.271E-02 -0.193 0.158 0.158

0 .0800 9 . 299E+00 3 . 337E-03 9.253E+00 1 .099E-02 9.991E-09 2.790E-02 -0.190 0.159 0.159

0.0900 3.931 E+00 3.375E-03 3. 935E+00 1 .339E-02 9.860E-09 3.237E-02 -0.137 0.152 0.151 0.1000 3 . 679E+00 3.91 9E-03 3.677E+00 1 .602E-02 5.268E-09 3.760E-02 -0.135 0.199 0.199

0 . 1 250 3.209E+00 3.523E-03 3.207E+00 2.333E-02 6.293E-09 5.166E-02 -0.130 0.199 0.193

0 . 1 500 2 .886E+00 3.690E-03 2.890E+00 3. 156E-02 7. 168E-09 6.699E-02 -0.126 0.190 0.139

0 . 1 750 2 .657E+00 3.769E-03 2.661E+00 9.059E-02 8.055E-09 8.320E-02 -0.123 0.136 0.136 0.2000 2.985E+00 3.896E-03 2.989E+00 5.032E-02 8.911E-09 1 .003E-01 -0.120 0.133 0.133

0 . 2500 2.295E+00 9. 179E-03 2.299E+00 7.152E-02 1 .055E-03 1 .363E-01 -0.115 0.129 0.128

0 . 3000 2.087E+00 9.989E-03 2.092E+00 9.962E-02 1 .21 3E-03 1 .790E-01 -0.110 0.125 0.123

0 . 3500 1 . 977E+00 9.820E-03 1 .981E+00 1 . 1 92E-01 1 .367E-03 2.129E-01 -0.106 0.121 0.120

0.9000 1 .896E+00 5. 173E-03 1 .901E+00 1 .950E-01 1 .518E-03 2.529E-01 -0.102 0.118 0.116

0.9500 1 .835E+00 5.595E-03 1 .891E+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 .799E+00 1 .993E-01 1 .817E-03 3.321E-01 -0.095 0.113 0.110

0.5500 1 .752E+00 6 . 390E-03 1 .758E+00 2.279E-01 1 . 966E-03 3.719E-01 -0.092 0.110 0.108

0.6000 1 .722E+00 6 .759E-03 1 .729E+00 2.561E-01 2. 1 15E-03 9.119E-01 -0.090 0.108 0.105

0 .7000 1 . 679E+00 7 .637E-03 1 .687E+00 3. 197E-01 2.916E-03 9.891E-01 -0.085 0.109 0.101 0.8000 1 .650E+00 8.559E-03 1 .659E+00 3.795E-01 2.71 9E-03 5.698E-01 -0.081 0.101 0.096

0 . 9000 1 . 631 E+00 9.523E-03 1 .690E+00 9.352E-01 3.026E-03 6.382E-01 -0.077 0.0 98 0.093

1 .0000 1 .617E+00 1 .053E-02 1 .627E+00 9.969E-01 3.337E-03 7.091E-01 -0.079 0.095 0.090

1 . 2500 1 . 599E+00 1 . 318E-02 1 .612E+00 6 .509E-01 9.133E-03 8.756E-01 -0.069 0.089 0.083

1 . 5000 1 . 593E+00 1 .602E-02 1 .609E+00 8.062E-01 9.959E-03 1 .028E+00 -0.069 0.085 0.078

1 .7500 1 .599E+00 1 . 901 E-02 1 .61 3E+00 9.619E-01 5.799E-03 1 .167E+00 -0.061 0.081 0.073

2 .0000 1 . 597E+00 2.21 3E-02 1 .61 9E+00 1.11 6E+00 6 .665E-03 1 .295E+00 -0.059 0.078 0.070

2.5000 1 . 608E+00 2.870E-02 1 .637E+00 1 .923E+00 8.950E-03 1 .522E+00 -0.055 0.073 0.065

3.0000 1 .621 E+00 3.561E-02 1 .657E+00 1 .727E+00 1 .029E-02 1 .720E+00 -0.052 0.069 0.061

3 . 5000 1 .639E+00 9.281E-02 1 .677E+00 2.027E+00 1 .218E-02 1 .899E+00 -0.050 0.067 0.058

9 . 0000 1 .697E+00 5.026E-02 1 .697E+00 2.323E+00 1 .910E-02 2.051E+00 -0.098 0.069 0.055

9.5000 1 .658E+00 5.792E-02 1 .716E+00 2.616E+00 1 .606E-02 2.1 93E+00 -0.097 0.062 0.053

5.0000 1 .669E+00 6 .576E-02 1 .735E+00 2.906E+00 1 .803E-02 2.323E+00 -0.095 0.060 0.051 5.5000 1 .679E+00 7.378E-02 1 .753E+00 3.193E+00 2.003E-02 2.993E+00 -0.099 0.059 0.050

6 .0000 1 .689E+00 8.1 93E-02 1 .771E+00 3.976E+00 2.209E-02 2.555E+00 -0.092 0.057 0.098

7.0000 1 .706E+00 9.865E-02 1 .809E+00 9.036E+00 2.610E-02 2.758E+00 -0.090 0.055 0.096

8.0000 1 . 720E+00 1 . 158E-01 1 .836E+00 9.585E+00 3.020E-02 2. 939E+00 -0.037 0.053 0.093

9.0000 1 .733E+00 1 .339E-01 1 .867E+00 5.125E+00 3.932E-02 3. 109E+00 -0.035 0.051 0.091 10.0000 1 .795E+00 1 .513E-01 1 .896E+00 5.657E+00 3.895E-02 3.256E+00 -0.032 0.099 0.039

12.5000 1 .769E+00 1 .971E-01 1 .966E+00 6.952E+00 9.877E-02 3.591E+00 -0.027 0.095 0.035

15.0000 1 .787E+00 2.999E-01 2.032E+00 8.202E+00 5.903E-02 3.879E+00 -0.022 0.091 0.031 17.5000 1 .803E+00 2.927E-01 2.095E+00 9.919E+00 6 . 918E-02 9.133E+00 -0.018 0.038 0.027

20.0000 1 .81 6E+00 3.917E-01 2.157E+00 1 .059E+01 7.917E-02 9.361E+00 -0.015 0.035 0.029

25 .0000 1 .836E+00 9.917E-01 2.278E+00 1 .289E+01 9.861E-02 9.755E+00 -0.011 0.031 0.019

30.0000 1 .852E+00 5.935E-01 2.396E+00 1 .998E+01 1 .173E-01 5.088E+00 -0.008 0.028 0.016

35.0000 1 .865E+00 6 .966E-01 2.512E+00 1 .702E+01 1 .351E-01 5.376E+00 -0.006 0.025 0.013

90 .0000 1 .877E+00 7.508E-01 2.627E+00 1 .897E+01 1 .522E-01 5.628E+00 -0.005 0.023 0.011 95.0000 1 .886E+00 8.559E-01 2.792E+00 2.083E+01 1 .685E-01 5.859E+00 -0.009 0.021 0.009

50.0000 1 .895E+00 9.617E-01 2.857E+00 2.262E+01 1 .891E-01 6 .057E+00 -0.003 0.020 0.008

55.0000 1 . 903E+00 1 .068E+00 2.971E+00 2.933E+01 1 .991E-01 6 .291E+00 -0.003 0.018 0.007

60.0000 1 . 91 OE+00 1 . 1 75E+00 3.085E+00 2.598E+01 2. 133E-01 6.91 lE+00 -0.002 0.017 0.006

70.0000 1 . 922E+00 1 . 391 E+00 3.313E+00 2. 911E+01 2.901E-01 6.712E+00 -0.002 0.016 0.005

80.0000 1 . 932E+00 1 .608E + 00 3.591 E+00 3.203E+01 2.698E-01 6.979E+00 -0.001 0.019 0.009

90 .0000 1 . 992E+00 1 .826E+00 3.768E+00 3.977E+01 2.875E-01 7.206E+00 -0.001 0.013 0.009

1 00 .0000 1 . 950E+00 2.096E+00 3.996E+00 3.735E+01 3.087E-01 7.915E+00 -0.001 0.012 0.003

1 25 .0000 1 . 967E+00 2.598E+00 9.566E+00 9.31 9E+01 3.553E-01 7.857E+00 -0.001 0.011 0.002

1 50.0000 1 . 982E+00 3 . 1 55E+00 5. 136E+00 9.835E+01 3. 998E-01 8.21 9E+00 -0.000 0.010 0.002

175.0000 1 . 993E+00 3.719E+00 5.708E+00 5.297E+01 9.288E-01 8.525E+00 -0.000 0.009 0.001

200 . 0000 2.009E+00 9 . 276E+00 6 .280E+00 5.719E+01 9.585E-01 8.791E+00 -0.000 0.008 0.001

250 .0000 2.021E+00 5.905E+00 7.926E+00 6 .996E+01 5.080E-01 9.236E+00 -0.000 0.007 0.001

300 .0000 2.035E+00 6.590E+00 8. 575E+00 7.072E+01 5.976E-01 9.599E+00 -0.000 0.007 0.001

350 .0000 2.097E+00 7 .678E+00 9.725E+00 7.619E+01 5.809E-01 9. 907E+00 -0.000 0.006 0.001

900 .0000 2.057E+00 8.820E+00 1 .088E+01 8. 105E+01 6 .079E-01 1 .017E+01 -0.000 0.006 0.001

950 .0000 2 . 066E+00 9 . 969E+00 1 .203E+01 8.592E+01 6.319E-01 1 .091E+01 -0.000 0.005 0.000

500 .0000 2.079E+00 1.111 E+01 1 . 318E+01 8. 938E+01 6.51 9E-01 1 .062E+01 -0.000 0.005 0.000

550.0000 2.082E+00 1 .226E + 01 1 .939E+01 9.302E+01 6 .698E-01 1 .081E+01 -0.000 0.005 0.000

600.0000 2.088E+00 1 . 390E+01 1 .599E+01 9.637E+01 6.856E-01 1 .098E+01 -0.000 0.005 0.000

700 .0000 2 . 1 OOE+00 1 .570E+01 1 .780E+01 1 .029E+02 7. 125E-01 1 . 129E+01 -0.000 0.005 0.000

800 .0000 2 . 1 1 OE+00 1 .801E+01 2.012E+01 1 .077E+02 7.396E-01 1 . 156E+01 -0.000 0.009 0.000

900 .0000 2. 120E+00 2.031E+01 2.293E+01 1 . 129E+02 7.530E-01 1 . 179E+01 -0.000 0.009 0.000

1000.0000 2. 128E+00 2.262E+01 2.975E+01 1 . 1 66E+02 7 .687E-0I 1 .200E+01 -0.000 0.009 0.000

84
ELECTRONS IN NITROGEN

I = 82.0 eV DENSITY = 1.165E-03 g/cm 3 (20° C)

ENERGY STOPPING POWER CSDA RADIATION DEN5.EFF. d( log1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm 2 0.0100 1 . 995E+01 3.711E-03 1 .996E+01 2.851E-09 1 .023E-09 0.0 -0.202 0.232 0.230

0.0125 1 .679E+01 3.729E-03 1 .680E + 01 9.223E-09 1 .227E-09 0.0 -0.199 0.221 0.220

0.0150 1 .958E+01 3.790E-03 1 .959E+01 5.825E-09 1 .921E-09 0.0 -0.187 0.213 0.211 0.0175 1 .299E+01 3.797E-03 1 .295E+01 7.698E-09 1 .608E-09 0.0 -0.182 0.206 0.205

0 .0200 1 .168E+01 3.753E-03 1 . 168E + 01 9.689E-09 1 .789E-09 0.0 -0.178 0.200 0.200

0.0250 9.838E+00 3.762E-03 9.892E+00 1 .937E-03 2.1 35E-09 0.0 -0.171 0.192 0.191 0.0300 8.569E+00 3 . 770E-03 8.568E+00 1 . 983E-03 2.965E-09 0.0 -0.166 0.185 0.185

0 .0350 7.626E+00 3.779E-03 7 .629E+00 2.603E-03 2.781E-09 0.0 -0.162 0.180 0.180

0 . 0<i00 6 . 909E+00 3.790E-03 6.908E+00 3.293E-03 3.086E-09 0.0 -0.159 0.176 0.176

0. 0^(50 6 . 331 E+00 3.803E-03 6.335E+00 9.099E-03 3.382E-09 0.0 -0.156 0.173 0.172

0 .0500 5.865E+00 3.816E-03 5.868E+00 9.870E-03 3.669E-09 0.0 -0.159 0.170 0.169

0.0550 5.977E+00 3.831E-03 5.981E+00 5.753E-03 3.999E-09 0.0 -0.152 0.167 0.167

0 .0600 5. 150E+00 3.896E-03 5.159E+00 6 .699E-03 9.222E-09 0.0 -0.150 0.165 0.169

0.0700 9 .628E+00 3.881E-03 9.632E+00 8.795E-03 9.751E-09 0.0 -0.197 0.161 0.160

0 .0800 9.229E+00 3. 920E-03 9.233E+00 1 .lOlE-02 5.260E-09 0.0 -0.199 0.158 0.157

0.0900 3.919E+00 3.961E-03 3.918E+00 1 .397E-02 5.752E-09 0.0 -0.192 0.155 0.155

0 . 1000 3.660E+00 9 .005E-03 3.669E+00 1 .61 lE-02 6.229E-09 0.0 -0.190 0.152 0.152

0.1250 3. 1 95E+00 9. 127E-03 3.1 99E+00 2.399E-02 7.368E-09 0.0 -0.136 0.198 0.197

0 . 1 500 2 .881 E+00 9.259E-03 2.885E+00 3. 169E-02 8.997E-09 0.0 -0.132 0.199 0.199

0.1750 2.655E+00 9.900E-03 2.660E+00 9.073E-02 9.977E-09 0.0 -0.130 0.191 0.191 0.2000 2.986E+00 9.550E-03 2.991E+00 5.096E-02 1 .097E-03 0.0 -0.128 0.139 0.138

0.2500 2.251E+00 9.879E-03 2.256E+00 7. 162E-02 1 .236E-03 0.0 -0.129 0.135 0.139

0 . 3000 2.097E+00 5.227E-03 2. 103E+00 9.962E-02 1 .918E-03 0.0 -0.121 0.132 0.131

0 . 3500 1 . 991 E+00 5.606E-03 1 . 996E+00 1 .191E-01 1 .593E-03 0.0 -0.119 0.129 0.128

0 .9000 1 .919E+00 6 .009E-03 1 .920E+00 1 .996E-01 1 .765E-03 0.0 -0.117 0.127 0.126

0 . 9500 1 .857E+00 6.936E-03 1 .863E+00 1 .71 lE-01 1 .935E-03 0.0 -0.115 0.126 0.129

0 . 5000 1 .81 3E+00 6 .882E-03 1 .820E+00 1 .982E-01 2.103E-03 0.0 -0.119 0.129 0.122

0.5500 1 .779E+00 7.397E-03 1 .787E+00 2.260E-01 2.271E-03 0.0 -0.112 0.123 0.121 0.6000 1 .753E+00 7.827E-03 1 .761E+00 2.592E-01 2.938E-03 0.0 -0.111 0.121 0.119

0 . 7000 1 .716E+00 8.831E-03 1 .725E+00 3. 1 16E-01 2.773E-03 0.0 -0.109 0.119 0.117

0 .8000 1 .693E+00 9.889E-03 1 .703E+00 3.700E-01 3. 109E-03 0.0 -0.107 0.117 0.115

0.9000 1 .679E+00 1 .099E-02 1 .690E+00 9.289E-01 3.997E-03 0.0 -0.105 0.116 0.113

1.0000 1 .670E+00 1 .219E-02 1 .683E+00 9.883E-01 3.788E-03 0.0 -0.109 0.119 0.111

1 .2500 1 .665E+00 1 .518E-02 1 .680E+00 6.371E-01 9.655E-03 0.0 -0.101 0.111 0.108

1 . 5000 1 .670E+00 1 .892E-02 1 .688E+00 7.856E-01 5.591 E-03 0.0 -0.098 0.109 0.105

1 .7500 1 .681E+00 2. 189E-02 1 .702E+00 9.331E-01 6.999E-03 0.0 -0.096 0.107 0.103

2.0000 1 .693E+00 2.590E-02 1 .71 9E+00 1 .079E+00 7.369E-03 0.0 -0.095 0.105 0.101 2.5000 1 .721 E+00 3.290E-02 1 .759E+00 1 .367E+00 9.293E-03 0.0 -0.092 0.102 0.097

3.0000 1 .799E+00 9.078E-02 1 .790E+00 1 .699E+00 1 . 1 16E-02 0.0 -0.090 0.100 0.095

3.5000 1 -775E+00 9.899E-02 1 .829E+00 1 . 926E+00 1 .31 lE-02 0.0 -0.088 0.0 98 0.093

9 .0000 1 .799E+00 5.797E-02 1 .857E+00 2.1 98E+00 1 .509E-02 0.0 -0.087 0.096 0.091 9.5000 1 .821E+00 6 .620E-02 1 .888E+00 2.965E+00 1 .708E-02 0.0 -0.085 0.095 0.089

5.0000 1 .892E+00 7.512E-02 1 .917E+00 2.728E+00 1 .909E-02 0.0 -0.089 0.099 0.088

5.5000 1 .861 E+00 8.923E-02 1 .995E+00 2.987E+00 2. 1 10E-02 0.0 -0.083 0.093 0.086

6.0000 1 .879E+00 9.352E-02 1 .972E+00 3.292E+00 2.312E-02 0.0 -0.082 0.091 0.085

7.0000 1 .91 lE+00 1 .125E-01 2.029E+00 3.792E+00 2.718E-02 0.0 -0.081 0.090 0.083

8.0000 1 .990E+00 1 .320E-01 2.072E+00 9.231E+00 3. 129E-02 0.0 -0.080 0.088 0.081 9.0000 1 . 965E+00 1 .520E-01 2. 1 17E+00 9.708E+00 3.530E-02 0.0 -0.078 0.086 0.080

10.0000 1 . 988E+00 1 .723E-01 2. 161E+00 5. 176E+00 3.939E-02 0.0 -0.077 0.085 0.078

12.5000 2.038E+00 2.299E-01 2.262E+00 6.306E+00 9.938E-02 0.0 -0.076 0.082 0.075

15.0000 2.079E+00 2.780E-01 2.356E+00 7.388E+00 5. 926E-02 0.0 -0.079 0.080 0.072

17.5000 2.1 13E+00 3.327E-01 2.996E+00 8.930E+00 6 .899E-02 0.0 -0.073 0.078 0.070

20.0000 2.199E+00 3.889E-01 2.532E+00 9.939E+00 7.892E-02 0.0 -0.072 0.076 0.068

25.0000 2.1 99E+00 5.016E-01 2.696E+00 1 . 1 35E+01 9.672E-02 0.0 -0.070 0.073 0.065

30.0000 2.235E+00 6.169E-01 2.852E+00 1 .315E+01 1 . 192E-01 9.661E-03 -0.061 0.071 0.062

35.0000 2.266E+00 7.336E-01 3.000E+00 1 .986E+01 1 .308E-01 6.591E-02 -0.050 0.068 0.057

90 .0000 2.290E+00 8.515E-01 3.192E+00 1 .699E+01 1 .967E-01 1 .979E-01 -0.093 0.069 0.052

95.0000 2.310E+00 9.709E-01 3.281E+00 1 .809E+01 1 .61 9E-01 2.393E-01 -0.038 0.061 0.097

50.0000 2.327E+00 1 .090E + 00 3.917E+00 1 . 959E+01 1 .765E-01 3.399E-01 -0.039 0.058 0.099

55.0000 2.392E+00 1 .21 lE+00 3.552E+00 2.097E+01 1 .909E-01 9.291E-01 -0.032 0.056 0.090

60.0000 2. 355E+00 1 .332E + 00 3.686E+00 2.235E+01 2.038E-01 5.217E-01 -0.029 0.059 0.037

70.0000 2. 377E+00 1 .575E+00 3. 952E+00 2.997E+01 2.290E-01 6.973E-01 -0.026 0.050 0.032

80.0000 2. 395E+00 1 .821E+00 9.216E+00 2.792E+01 2.523E-01 8.590E-01 -0.029 0.097 0.029

90 .0000 2.91 lE+00 2.067E+00 9.978E+00 2. 972E+01 2.790E-01 1 .008E+00 -0.023 0.099 0.026

1 00 .0000 2.929E+00 2. 31 5E+00 9.790E+00 3. 189E+01 2.991E-01 1 .199E+00 -0.022 0.092 0.029

125.0000 2.953E+00 2. 939E+00 5.392E+00 3.689E+01 3.389E-01 1 .993E+00 -0.020 0.038 0.019

150.0000 2.975E+00 3.567E+00 6 .092E+00 9.121E+01 3.771E-01 1 .695E+00 -0.019 0.035 0.017

175.0000 2.999E+00 9 . 1 98E+00 6.693E+00 9.519E+01 9. 103E-01 1.911 E+00 -0.018 0.032 0.015

200.0000 2.51 OE+00 9.832E+00 7.393E+00 9.871E+01 9.399E-01 2. 102E+00 -0.017 0.030 0.013

250.0000 2 . 537E+00 6 . 1 06E+00 8.693E+00 5.998E+01 9.883E-01 2.927E+00 -0.016 0.027 0.01 1 300.0000 2.558E+00 7.385E+00 9. 993E+00 6.037E+01 5.278E-01 2.699E+00 -0.015 0.025 0.009

350.0000 2.575E+00 8 . 668E+00 1 . 129E+01 6.509E+01 5.606E-01 2.939E+00 -0.019 0.029 0.008

900.0000 2.590E+00 9. 955E+00 1 .259E+01 6.930E+01 5.883E-01 3. 192E+00 -0.013 0.023 0.007

950.0000 2.603E+00 1 . 129E+01 1 . 385E+01 7 . 309E+01 6.122E-01 3.329E+00 -0.012 0.021 0.007

500 .0000 2.619E+00 1 .253E+01 1 .515E+01 7.659E+01 6.330E-01 3.999E+00 -0.011 0.021 0.006

550.0000 2.629E+00 1 .383E+01 1 .695E+01 7.971E+01 6.513E-01 3.657E+00 -0.010 0.020 0.006

600 .0000 2 . 633E+00 1 .512E+01 1 .775E+01 8.269E+01 6.675E-01 3.803E+00 -0.009 0.019 0.005

700 .0000 2.698E+00 1 .771E+01 2.036E+01 8.789E+01 6.952E-01 9.067E+00 -0.008 0.018 0.009

800.0000 2.660E+00 2.031E+01 2.297E+01 9.251E+01 7. 180E-01 9.303E+00 -0.006 0.017 0.009

900.0000 2.671E+00 2.290E+01 2.558E+01 9.669E+01 7.371E-01 9.515E+00 -0.005 0.017 0.003

1000.0000 2.681E+00 2.550E+01 2.818E+01 1 .009E+02 7.539E-01 9.707E+00 -0.005 0.016 0.003
ELECTRONS IN OXYGEN

I = 95.0 eV DENSITY = 1.332E-03 g/citi 3 (20<> C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. dClog1 )/d(loqI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm 2 0.0100 1 . 937E+01 9 .267E-03 1 . 937E+01 2. 950E-09 1 .207E-09 0.0 -0.209 0.291 0.239

0.0125 1 .632E+01 9 . 298E-03 1 .633E + 01 9.362E-09 1 .999E-09 0.0 -0.199 0.229 0.227

0.0150 1 .91 9E+01 9.316E-03 1 .91 9E+01 6 .009E-09 1 .681E-09 0.0 -0.193 0.220 0.218

0.0175 1 .260E+01 9.328E-03 1 .261E+01 7 .882E-09 1 . 903E-09 0.0 -0.187 0.213 0.211

0 .0200 1 . 1 38E+01 9 . 336E-03 1 . 1 38E+01 9 . 973E-09 2.1 18E-09 0.0 -0.183 0.207 0.206

0.0250 9.595E+00 9 . 397E-03 9.600E+00 1 .978E-03 2 . 529E-09 0.0 -0.176 0.198 0.197

0 .0300 8 . 359E+00 9 . 356E-03 8.363E+00 2.037E-03 2. 91 9E-09 0.0 -0.170 0.191 0.190

0.0350 7.997E+00 9.365E-03 7.952E+00 2.672E-03 3.293E-09 0.0 -0.166 0.185 0.185

0.0900 6 .796E+00 9.376E-03 6.750E+00 3.378E-03 3.653E-09 0.0 -0.163 0.181 0.180

0 .0950 6 . 189E+00 9 . 388E-03 6 . 1 93E+00 9.153E-03 9.001E-09 0.0 -0.160 0.177 0.177

0 .0500 5.735E+00 9.902E-03 5.739E+00 9. 992E-03 9. 339E-09 0.0 -0.157 0.179 0.179

0 .0550 5 . 358E+00 9.917E-03 5.362E+00 5.899E-03 9.668E-09 0.0 -0.155 0.171 0.171 0.0600 5 . 039E+00 9.939E-03 5.099E+00 6 .856E-03 9.988E-09 0.0 -0.153 0.169 0.169

0 .0700 9.530E+00 9.971E-03 9.535E+00 8.951E-03 5.608E-09 0.0 -0.150 0.165 0.169

0 . 0800 9 . 1 92E + 00 9.512E-03 9. 196E+00 1 . 126E-02 6.209E-09 0.0 -0.197 0.161 0.161 0.0900 3 .835E+00 9 . 558E-03 3.839E+00 1 .377E-02 6.779E-09 0.0 -0.195 0.158 0.158

0.1000 3 . 586E+00 9.607E-03 3.591E+00 1 .697E-02 7.337E-09 0.0 -0.193 0.156 0.156

0 . 1 250 3.1 33E+00 9.791E-03 3.1 37E+00 2.399E-02 8.666E-09 0.0 -0.138 0.151 0.151 0.1500 2.826E+00 9 .889E-03 2.831E+00 3.235E-02 9. 921E-09 0.0 -0.135 0.197 0.197

0 . 1750 2.606E+00 5.098E-03 2.611 E+00 9.157E-02 1 .1 12E-03 0.0 -0.132 0.199 0.199

0.2000 2. 991 E+00 5.215E-03 2.996E+00 5.197E-02 1 .227E-03 0.0 -0.130 0.192 0.191

0 . 2500 2.211 E+00 5.578E-03 2.217E+00 7. 302E-02 1 .997E-03 0.0 -0.127 0.138 0.137

0 . 3000 2.061 E+00 5 . 975E-03 2.067E+00 9.692E-02 1 .656E-03 0.0 -0.129 0.139 0.139

0 . 3500 1 . 957E+00 6.902E-03 1 . 963E+00 1 .21 3E-01 1 .859E-03 0.0 -0.121 0.132 0.131 0.9000 1 .882E+00 5 .856E-03 1 .889E+00 1 .973E-01 2.057E-03 0.0 -0.119 0.130 0.128

0.9500 1 .826E + 00 7.335E-03 1 .833E+00 1 .792E-01 2.253E-03 0.0 -0.117 0.128 0.126

0 . 5000 1 .789E+00 7 .838E-03 1 .791E+00 2.018E-01 2.996E-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 -0.119 0.125 0.123

0.6000 1 .725E+00 8. 909E-03 1 .739E+00 2.586E-01 2.831E-03 0.0 -0.113 0.129 0.122

0.7000 1 .690E + 00 1 .009E-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 .679E+00 3.761E-01 3.600E-03 0.0 -0.109 0.119 0.117

0 . 9000 1 .659E + 00 1 .297E-02 1 .666E+00 9.359E-01 3. 987E-03 0.0 -0.107 0.118 0.115

1 .0000 1 .696E+00 1 .376E-02 1 .659E+00 9.961E-01 9.377E-03 0.0 -0.105 0.116 0.113

1 .2500 1 .691E+00 1 .718E-02 1 .658E+00 6.969E-01 5.366E-03 0.0 -0.102 0.113 0.110

1 . 5000 1 .697E + 00 2.089E-02 1 .667E+00 7.973E-01 6.376E-03 0.0 -0.100 0.111 0.107

1 .7500 1 . 658E + 00 2.968E-02 1 .682E+00 9.966E-01 7.905E-03 0.0 -0.098 0.108 0.109

2 .0000 1 .671 E+00 2.869E-02 1 .699E+00 1 .099E+00 8.952E-03 0.0 -0.096 0.107 0.102

2.5000 1 .699E+00 3.71 IE-02 1 .736E+00 1 .386E+00 1 .059E-02 0.0 -0.093 0.109 0.099

3 .0000 1 .727E+00 9.598E-02 1 .773E+00 1 .671E+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 .997E-02 0.0 -0.089 0.099 0.099

9.0000 1 .777E+00 6.971E-02 1 .892E+00 2.229E+00 1 .720E-02 0.0 -0.088 0.098 0.092

9.5000 1 .799E + 00 7.998E-02 1 .879E+00 2.993E+00 1 .995E-02 0.0 -0.086 0.096 0.090

5 .0000 1 .820E + 00 8.999E-02 1 . 905E+00 2.758E+00 2.171E-02 0.0 -0.085 0.095 0.088

5.5000 1 .839E+00 9.970E-02 1 .939E+00 3.018E+00 2.398E-02 0.0 -0.089 0.099 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 .269E-01 2.016E+00 3.777E+00 3.081E-02 0.0 -0.082 0.091 0.089

8.0000 1 .918E+00 1 .982E-01 2.066E+00 9.267E+00 3.536E-02 0.0 -0.080 0.089 0.082

9.0000 1 . 999E+00 1 .705E-01 2.119E+00 9.796E+00 3.990E-02 0.0 -0.079 0.087 0.080

10.0000 1 . 967E+00 1 .932E-01 2. 160E+00 5.219E+00 9.991E-02 0.0 -0.078 0.086 0.079

12.5000 2.016E+00 2.519E-01 2.268E+00 6.393E+00 5.558E-02 0.0 -0.076 0.083 0.075

15.0000 2.057E+00 3. 1 12E-01 2.368E+00 7.921E+00 6.652E-02 0.0 -0.075 0.081 0.073

17.5000 2.092E+00 3.723E-01 2.969E+00 8.956E+00 7.720E-02 0.0 -0.079 0.079 0.070

20.0000 2. 122E+00 9.393E-01 2.556E+00 9.952E+00 8.762E-02 0.0 -0.073 0.077 0.068

25.0000 2.173E+00 5.606E-01 2.733E+00 1 .139E+01 1 .076E-01 0.0 -0.071 0.079 0.065

30 .0000 2.219E+00 6.890E-01 2.903E+00 1 .312E+01 1 -266E-01 2.989E-03 -0.065 0.071 0.062

35.0000 2.296E+00 8. 189E-01 3.065E+00 1 .979E+01 1 .996E-01 9.925E-02 -0.059 0.068 0.057

90.0000 2.272E+00 9.502E-01 3.222E+00 1 -638E+01 1 .617E-01 1 .129E-01 -0.097 0.065 0.053

95.0000 2.292E+00 1 .083E+00 3.375E+00 1 .790E+01 1 .779E-01 1 . 990E-01 -0.091 0.062 0.098

50.0000 2.310E+00 1 .216E+00 3.526E+00 1 .935E+01 1 .939E-01 2.809E-01 -0.037 0.059 0.095

55.0000 2. 325E+00 1 .350E+00 3.675E+00 2.079E+01 2.082E-01 3.682E-01 -0.039 0.057 0.091 60.0000 2.338E+00 1 .989E+00 3.823E+00 2.207E+01 2.229E-01 9.559E-01 -0.031 0.055 0.038

70.0000 2 . 361 E+00 1 .755E+00 9.116E+00 2.959E+01 2.988E-01 6.239E-01 -0.028 0.051 0.033

80 .0000 2. 379E+00 2.028E+00 9.907E+00 2.699E+01 2.732E-01 7.819E-01 -0.025 0.098 0.030

90 .0000 2 . 395E+00 2.302E+00 9.697E+00 2.919E+01 2. 957E-01 9.288E-01 -0.023 0.095 0.027

1 00 .0000 2.909E+00 2 . 577E+00 9 . 986E+00 3.1 20E+01 3. 165E-01 1 .065E+00 -0.022 0.093 0.029

125.0000 2.937E+00 3 . 270E+00 5.707E+00 3.589E+01 3.629E-01 1 .366E+00 -0.019 0.0 38 0.020

150.0000 2 . 960E+00 3.967E+00 6 .927E+00 9.001E+01 9.013E-01 1 .622E+00 -0.018 0.035 0.017

175.0000 2.978E+00 9 . 668E+00 7 . 1 96E+00 9 . 370E+01 9.398E-01 1 .893E+00 -0.017 0.033 0.015

200.0000 2.999E+00 5.371E+00 7.865E+00 9.703E+01 9.690E-01 2.038E+00 -0.016 0.031 0.013

250 .0000 2. 520E+00 6 . 789E+00 9. 309E+00 5.287E+01 5. 127E-01 2.369E+00 -0.015 0.028 0.011

300 .0000 2.591E+00 8 . 202E+00 1 . 079E+01 5.787E+01 5.517E-01 2.699E+00 -0.015 0.026 0.009

350.0000 2.558E+00 9 . 625E+00 1 .218E+01 6 .223E+01 5.890E-01 2.879E+00 -0.019 0.029 0.008

900.0000 2.573E+00 1 . 1 05E+01 1 . 362E+01 6.61 1E+01 6.111 E-01 3.086E+00 -0.013 0.023 0.007

950 .0000 2.586E+00 1 .298E+01 1 .507E+01 6 . 960E+01 6 . 393E-01 3.271E+00 -0.013 0.022 0.006

500.0000 2.597E+00 1 . 391 E+01 1 . 651 E+01 7.277E+01 6 .599E-01 3.938E+00 -0.012 0.021 0.006

550.0000 2.608E+00 1 . 539E+01 1 .795E + 01 7.568E+01 6 .721 E-01 3.592E+00 -0.011 0.020 0.005

500.0000 2.617E+00 1 .678E+01 1 . 939E + 01 7 .835E+01 6 .878E-01 3.733E+00 -0.011 0.020 0.005

700.0000 2 . 633E+00 1 . 965E+01 2.228E+01 8.316E+01 7.199E-01 3.989E+00 -0.010 0.019 0.009

800.0000 2.696E+00 2.252E+01 2.517E+01 8.738E+01 7.361E-01 9 . 21 5E+00 -0.008 0.018 0.009

900 .0000 2.658E+00 2 . 590E+01 2.805E+01 9. 1 19E+01 7.599E-01 9.918E+00 -0.008 0.017 0.009

1000 .0000 2. 668E+00 2.827E+01 3.099E+01 9. 959E+01 7.699E-01 9.603E+00 -0.007 0.017 0.003

80
ELECTRONS IN NEON

I = 137.0 oV DENSITY = 8.385E-0<* g/cm^ (20<> C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. cUlog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .773E+01 5.273E-03 1 .77<(E+01 3.265E-0<» 1 .622E-0<( 0.0 -0.226 0.266 0.262

0.0125 1 .500E+01 5.3A0E-03 1 .500E+01 <(.80<(E-0<( 1 .951E-0<( 0.0 -0.215 0.251 0.248

0.0150 1 .307E+01 5.38<(E-03 1 .308E+01 6 .595E-0A 2.266E-0<( 0.0 -0.207 0.240 0.237

0.0175 1 . 16<(E+01 5.<(16E-03 1 .16<(E + 01 8.625E-0<( 2.569E-0<( 0.0 -0.201 0.232 0.229

0.0200 1 .052E+01 5.<(39E-03 1 .053E+01 1 .089E-03 2.862E-0A 0.0 -0.196 0.225 0.223

0 .0250 8 .898E + 00 5.<(70E-03 8.90<(E+00 1 .607E-03 3. A22E-0<( 0.0 -0.188 0.214 0.212

0.0300 7 . 768E + 00 5.A92E-03 7.773E+00 2.210E-03 3. 953E-0<( 0.0 -0.182 0.206 0.204

0.0350 6 . 932E+00 5.510E-03 6.938E+00 2.892E-03 A.<461E-0<( 0.0 -0.177 0.200 0.198

0 .0^00 6.288E+00 5.526E-03 6.293E+00 3.650E-03 <( . 9<(9E-0<( 0.0 -0.173 0.194 0.193

0 . 0'(50 5.775E+00 5.5<(3E-03 5.781E+00 <(.<(80E-03 5.<(20E-0<( 0.0 -0.170 0.190 0.189

0 .0500 5.357E+00 5.559E-03 5.362E+00 5.379E-03 5.876E-0<( 0.0 -0.167 0.186 0.186

0.0550 5.009E+00 5.577E-03 5.01<(E + 00 6.3<(<(E-03 6.319E-0<( 0.0 -0.164 0.183 0.183

0.0600 <( .71 5E + 00 5.595E-03 <(.720E+00 7.373E-03 6.750E-0<( 0.0 -0.162 0.180 0.180

0.0700 <( . 2<(<(E + 00 5.63<(E-03 <(.250E+00 9.610E-03 7.580E-0<( 0.0 -0.158 0.176 0.175

0 .0800 3.88<(E + 00 5.679E-03 3.890E+00 1 .207E-02 8.37<(E-0<1 0.0 -0.155 0.172 0.171 0.0900 3.599E+00 5.727E-03 3.605E+00 1 .<(75E-02 9.138E-0A 0.0 -0.153 0.169 0.168

0.1000 3 . 369E+00 5.781E-03 3. 375E+00 1 .762E-02 9.875E-0<( 0.0 -0.150 0.166 0.165

0 . 1 250 2. 9<(8E+00 5.93<(E-03 2. 95<(E+00 2.557E-02 1 . 163E-03 0.0 -0.146 0.160 0.160

0.1500 2.663E+00 6. 106E-03 2.669E+00 3.<(<(9E-02 1 .327E-03 0.0 -0.142 0.156 0.155

0 . 1750 2.<(58E+00 6 .296E-03 2.<(6<(E + 00 <(.<(26E-02 1 .<(8<(E-03 0.0 -0.139 0.152 0.152

0.2000 2. 30<(E+00 6 .500E-03 2.310E+00 5.<(75E-02 1 .63<(E-03 0.0 -0.137 0.150 0.149

0 .2500 2.090E+00 6 . 9<(5E-03 2.097E+00 7.75<(E-02 1 .920E-03 0.0 -0.133 0.145 0.144

0.3000 1 . 950E+00 7 .<(32E-03 1 .958E+00 1 .023E-01 2.1 92E-03 0.0 -0.129 0.142 0.140

0.3500 1 .85<(E+00 7.956E-03 1 .862E+00 1 .285E-01 2.<156E-03 0.0 -0.127 0.139 0.137

0 . <(000 1 .78<(E + 00 8.51 lE-03 1 .792E+00 1 .559E-01 2.713E-03 0.0 -0.125 0.136 0.135

0.<(500 1 .732E+00 9.096E-03 1 .7<(lE+00 1 .8A2E-01 2. 965E-03 0.0 -0.123 0.134 0.133

0.5000 1 .693E + 00 9.707E-03 1 .703E+00 2.133E-01 3.215E-03 0.0 -0.121 0.132 0.131 0.5500 1 .663E+00 1 .03<(E-02 1 .673E+00 2.A29E-01 3.<(63E-03 0.0 -0.119 0.131 0.129

0.6000 1 .639E + 00 1 .lOOE-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 3.3<(2E-01 <(.200E-03 0.0 -0.115 0.127 0.124

0 .8000 1 .587E+00 1 .380E-02 1 .601E+00 3.96<(E-01 <(.691E-03 0.0 -0.113 0.125 0.122

0 . 9000 1 .575E+00 1 .530E-02 1 .590E+00 <(.591E-01 5. 18<(E-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 2.5<(2E-02 1 .598E+00 8.370E-01 8.202E-03 0.0 -0.104 0.115 0.111

1 .7500 1 .58<(E+00 3.008E-02 1 .61<(E+00 9.927E-01 9.497E-03 0.0 -0.101 0.113 0.108

2.0000 1 .598E+00 3.<(93E-02 1 .633E+00 1 . 1<(7E+00 1 .081E-02 0.0 -0.099 0.111 0.106

2.5000 1 .626E+00 <(.513E-02 1 .672E+00 1 .<(<i9E+00 1 .3<(9E-02 0.0 -0.096 0.108 0.102

3.0000 1 .65<(E+00 5.586E-02 1 .710E+00 1 .745E+00 1 .621E-02 0.0 -0.094 0.105 0.099

3.5000 1 .681E+00 6.701E-02 1 .7<(8E+00 2.03<(E+00 1 .897E-02 0.0 -0.092 0.103 0.097

<( .0000 1 .705E+00 7.852E-02 1 .783E+00 2.317E+00 2.17<(E-02 0.0 -0.091 0.101 0.094

<( . 5000 1 .727E+00 9.033E-02 1 .817E+00 2.595E+00 2.45AE-02 0.0 -0.089 0.099 0.093

5.0000 1 .7<(8E + 00 1 .02<*E-01 1 .850E+00 2.868E+00 2.733E-02 0.0 -0.088 0.098 0 .091 5.5000 1 .767E+00 1 .1<(7E-01 1 .882E+00 3.1 36E+00 3.01<(E-02 0.0 -0.087 0.097 0.089

6.0000 1 .785E+00 1 .273E-01 1 .912E+00 3.399E+00 3.29<(E-02 0.0 -0.086 0.095 0.088

7.0000 1 .817E+00 1 .529E-01 1 . 970E + 00 3.915E+00 3.853E-02 0.0 -0.084 0.093 0.086

8.0000 1 .8<(5E+00 1 .791E-01 2.02<(E+00 <(.<(15E+00 <(.<(10E-02 0.0 -0.083 0.091 0.083

9 .0000 1 .870E+00 2.058E-01 2.076E+00 <1.903E+00 <(.963E-02 0.0 -0.082 0.090 0.082

10.0000 1 .893E+00 2. 330E-01 2. 126E+00 5.379E+00 5.510E-02 0.0 -0.081 0.088 0.080

12.5000 1 . 9<(2E+00 3.026E-01 2.2<(5E+00 6.523E+00 6.85<(E-02 0.0 -0.079 0.085 0.076

15.0000 1 . 983E+00 3.739E-01 2.357E+00 7.609E+00 8. 159E-02 0.0 -0.077 0.082 0.073

17.5000 2.017E+00 <(.<(66E-01 2.<(6<(E+00 8.6<(6E+00 9.<i23E-02 0.0 -0.076 0.080 0.071 20.0000 2.017E+00 5.20<(E-01 2.568E+00 9.6<(0E+00 1 .065E-01 0.0 -0.074 0.078 0.068

25.0000 2.098E+00 6 .703E-01 2.768E+00 1 . 151E+01 1 .297E-01 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. 17<(E+00 9.766E-01 3.151E+00 1 .<(90E+01 1 .71 9E-01 0.0 -0.070 0.069 0.059

<(0.0000 2.20<(E+00 1 . 1 32E+00 3.336E+00 1 .6<(<(E+01 1 .910E-01 0.0 -0.069 0.067 0.056

<15.0000 2.231E+00 1 .289E+00 3.520E+00 1 .790E+01 2.090E-01 0.0 -0.068 0.065 0.054

50.0000 2.255E+00 1 .<(<(6E+00 3.701 E+00 1 .928E+01 2.259E-01 0.0 -0.068 0.064 0.052

55.0000 2.277E+00 1 .605E400 3.881E+00 2.060E+01 2.420E-01 0.0 -0.067 0.062 0.050

60.0000 2.297E+00 1 .76<1E+00 <(.060E + 00 2. 186E+01 2.571E-01 0.0 -0.066 0.061 0.049

70.0000 2.329E+00 2.08<(E+00 <(.<(1 3E+00 2.<(22E+01 2.852E-01 2.873E-02 -0.054 0.058 0.045

80.0000 2.355E+00 2.<(06E + 00 <(.761E+00 2.6<(0E+01 3. 107E-01 9.312E-02 -0.045 0.055 0.041 90.0000 2.376E+00 2.729E+00 5. 105E+00 2.8<(3E+01 3.3<t0E-01 1 .7<i1E-01 -0.039 0.053 0.037

100.0000 2. 393E+00 3.05AE+00 5.<(<(7E+00 3.033E+01 3.55<(E-01 2.62<(E-01 -0.035 0.051 0.034

1 25 .0000 2.<(27E + 00 3.871E+00 6 .298E+00 3.<(59E+01 <(.021E-01 <(.888E-01 -0.028 0.046 0.028

1 50.0000 2.<(52E+00 <(.693E + 00 7.1A<(E+00 3.832E+01 <(.<(12E-01 7 .0<(5E-01 -0.023 0.042 0.023

175.0000 2.<(72E + 00 5.518E+00 7.990E+00 <(.162E+01 <(.7<(5E-01 9.031E-01 -0.021 0.040 0.020

200.0000 2.<(88E + 00 6 . 3<(7E + 00 8.835E+00 <(.<160E+01 5.033E-01 1 .085E+00 -0.019 0.037 0.018

250.0000 2.515E+00 8.010E+00 1 .053E + 01 <t.978E + 01 5.508E-01 1 .<(03E+00 -0.016 0.034 0.014

300.0000 2.536E+00 9 . 680E+00 1 .222E+01 5.<(18E+01 5.886E-01 1 .67<(E+00 -0.015 0.032 0.012

350 .0000 2.55<(E+00 1 . 1 35E+01 1 .391E+01 5.802E+01 6.195E-01 1 .908E+00 -0.014 0.030 0.010

<(00.0000 2. 568E+00 1 . 303E+01 1 .560E+01 6. 1<(1E+01 6.453E-01 2. 1 1<(E+00 -0.013 0.028 0.009

<(50 .0000 2. 581 E+00 1 .<(71 E+01 1 .729E + 01 6 .A<(5E+01 6 .673E-01 2.298E+00 -0.013 0.027 0.008

500.0000 2 . 593E400 1 .639E+01 1 .899E+01 6 . 721 E+01 6 .863E-01 2.<(6<(E+00 -0.012 0.026 0.007

550.0000 2.603E+00 1 .808E+01 2.068E+01 6.973E+01 7.029E-01 2.616E+00 -0.012 0.025 0.007

600 .0000 2.612E+00 1 . 976E+01 2.237E+01 7 .206E+01 7.176E-01 2.755E+00 -0.012 0.024 0.006

700 .0000 2 . 628E+00 2.31 3E+01 2.576E+01 7.622E+01 7.<(23E-01 3.003E+00 -0.011 0.023 0.005

800.0000 2 . 6<(2E+00 2.651E+01 2.915E+01 7.987E+01 7.625E-01 3.220E+00 -0.011 0.022 0.005

900.0000 2.655E+00 2 . 989E+01 3.25<(E + 01 8.311E+01 7.794E-01 3.<(13E+00 -0.010 0.021 0.004

1000.0000 2.665E+00 3.327E+01 3.59<(E+01 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+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log l/dClogl) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cra^/g g/cm ^ 0.0100 1 .699E+01 6 . 559E-03 1 .650E + 01 3.539E-09 2.1 32E-09 3.539E-09 -0.236 0.281 0.275

0.0125 1 . 398E+01 6 .700E-03 1 .398E + 01 5. 1 92E-09 2.583E-09 9 . 937E-09 -0.229 0.265 0.260 0.0150 1 . 220E+0

6 .798E-03 1 .221E+01 7.111 E-09 3.016E-09 6.538E-09 -0.216 0 .252 0.298

0.0175 1 .088E+01 6 . 871 E-03 1 .088E+01 9.289E-09 3.935E-09 8.332E-09 -0.209 0.293 0.239

0 .0200 9.899E+00 6 . 926E-03 9.851E+00 1 . 170E-03 3.890E-09 1 .031 E-03 -0.203 0.235 0.232

0.0250 8 . 338E+00 7.009E-03 8. 395E + 00 1 .729E-03 9.616E-09 1 .983E-03 -0.195 0.229 0.221 0.0300 7 . 287E+00 7 . 059E-03 7.299E+00 2.367E-03 5.353E-09 2.005E-03 -0.188 0.215 0.212

0 .0350 6 . 509E+00 7 . 1 OOE-03 6.516E+00 3.093E-03 6.058E-09 2.593E-03 -0.183 0.208 0.206

0 . OAOO 5 . 909E+00 7.133E-03 5.916E+00 3. 900E-03 6 . 736E-09 3.296E-03 -0.179 0.202 0.201

0 .0A50 5 . 930E+00 7 . 1 62E-03 5.937E+00 9.783E-03 7.390E-09 3.960E-03 -0.175 0.198 0.196

0.0500 5.039E+00 7 . 1 91 E-03 5.096E+00 5.738E-03 8.022E-09 9.732E-03 -0.172 0.199 0.192

0.0550 9.719E+00 7 . 21 7E-03 9.721E+00 6.763E-03 8.636E-09 5.560E-03 -0.170 0.190 0.189

0.0600 9 . 939E+00 7 . 293E-03 9.996E+00 7.855E-03 9.232E-09 6 .990E-03 -0.167 0.187 0.186

0.0700 3. 998E+00 7 .295E-03 9.005E+00 1 .023E-02 1 .038E-03 8.351E-03 -0.163 0.182 0.181

0 .0800 3 .661 E+00 7 . 350E-03 3.668E+00 1 .289E-02 1 .197E-03 1 .095E-02 -0.160 0.178 0.177

0 .0900 3. 399E+00 7.91 lE-03 3.901 E+00 1 .568E-02 1 .252E-03 1 .271E-02 -0.157 0.179 0.173

0.1000 3. 177E+00 7 . 976E-03 3. 185E+00 1 .872E-02 1 .353E-03 1 .51 3E-02 -0.155 0.171 0.170

0 . 1250 2.781E+00 7 . 659E-03 2.789E+00 2.719E-02 1 .593E-03 2. 175E-02 -0.150 0.165 0.169

0 . 1 500 2.51 3E+00 7 .865E-03 2.521 E+00 3.659E-02 1 .81 6E-03 2. 907E-02 -0.196 0.160 0.160 0.1750 2 . 320E+00 8.096E-03 2.328E+00 9.693E-02 2.028E-03 3.699E-02 -0.193 0.157 0.156

0.2000 2. 179E+00 8.399E-03 2. 183E+00 5.809E-02 2.231E-03 9.525E-02 -0.190 0.159 0.153

0.2500 1 . 972E+00 8.888E-03 1 .981E + 00 8.21 7E-02 2.616E-03 6.280E-02 -0.136 0.199 0.198

0.3000 1 .839E+00 9.987E-03 1 .899E+00 1 .083E-01 2.982E-03 8.116E-02 -0.132 0.195 0.199

0.3500 1 . 797E+00 1 .013E-02 1 .757E+00 1 .361E-01 3.335E-03 9. 997E-02 -0.129 0.192 0.191

0 .9000 1 .680E+00 1 .082E-02 1 .691E+00 1 .652E-01 3.678E-03 1 . 1 90E-01 -0.127 0.139 0.138

0.9500 1 . 630E+00 1 . 1 59E-02 1 .692E+00 1 . 952E-01 9.016E-03 1 . 380E-01 -0.125 0.137 0.135

0 . 5000 1 . 592E+00 1 .230E-02 1 .609E+00 2.260E-01 9.399E-03 1 .569E-01 -0.123 0.135 0.133

0 . 5500 1 . 563E+00 1 .309E-02 1 .576E+00 2.575E-01 9.680E-03 1 .757E-01 -0.121 0.133 0.131 0.6000 1 . 590E+00 1 . 390E-02 1 .559E+00 2.899E-01 5.009E-03 1 .993E-01 -0.119 0.132 0.130

0.7000 1 . 507E+00 1 .560E-02 1 .522E+00 3.595E-01 5.669E-03 2.307E-01 -0.116 0.129 0.126

0.8000 1 . 986E+00 1 .739E-02 1 .503E+00 9.206E-01 6.31 9E-03 2.661E-01 -0.113 0.127 0.129

0.9000 1 . 973E+00 1 . 925E-02 1 .992E+00 9.879E-01 6.976E-03 3.005E-01 -0.111 0.129 0.121

1 .0000 1 .965E+00 2.11 9E-02 1 .986E+00 5.596E-01 7.636E-03 3.339E-01 -0.108 0.122 0.119

1 .2500 1 .957E+00 2.630E-02 1 .989E+00 7.231E-01 9.306E-03 9.1 38E-01 -0.103 0.118 0.113

1.5000 1 . 960E+00 3. 177E-02 1 .991E+00 8.912E-01 1 . 101E-02 9.898E-01 -0.097 0.119 0.109

1 .7500 1 .966E+00 3.752E-02 1 .509E+00 1 .058E+00 1 .279E-02 5.632E-01 -0.092 0.111 0.105

2.0000 1 . 975E + 00 9.350E-02 1 .518E+00 1 .229E+00 1 .999E-02 6.399E-01 -0.087 0.108 0.101

2 . 5000 1 .993E+00 5.605E-02 1 .599E+00 1 .550E+00 1 .808E-02 7.757E-01 -0.077 0.102 0.093

3.0000 1 .510E+00 6.929E-02 1 .580E+00 1 .869E+00 2. 173E-02 9.195E-01 -0.067 0.096 0.085

3.5000 1 . 526E + 00 8.292E-02 1 -609E+00 2. 183E+00 2.599E-02 1 .051E+00 -0.059 0.091 0.079

9.0000 1 . 590E+00 9.702E-02 1 .637E+00 2.991E+00 2. 918E-02 1 . 183E+00 -0.052 0.086 0.072

9.5000 1 . 552E+00 1 .115E-01 1 .669E+00 2.799E+00 3.296E-02 1 .31 lE+00 -0.097 0.082 0.067

5.0000 1 . 569E+00 1 .263E-01 1 .690E+00 3.092E+00 3.675E-02 1 .933E+00 -0 .092 0.078 0.062

5.5000 1 . 579E+00 1 .913E-01 1 .715E+00 3.386E+00 9.055E-02 1 .550E+00 -0.039 0.079 0.058

6.0000 1 . 583E+00 1 .567E-01 1 .739E+00 3.675E+00 9.936E-02 1 .661E+00 -0.036 0.071 0.059

7 .0000 1 . 599E + 00 1 .879E-01 1 .787E+00 9.292E+00 5.1 97E-02 1 .868E+00 -0.032 0.066 0.098

8.0000 1 .61 3E+00 2.200E-01 1 .833E+00 9.795E+00 5.955E-02 2.055E+00 -0.029 0.061 0.093

9.0000 1 .625E+00 2.526E-01 1 .877E+00 5.339E+00 6.708E-02 2.226E+00 -0.026 0.057 0.039

10.0000 1 .636E+00 2.858E-01 1 .921E+00 5.861E+00 7.959E-02 2.389E+00 -0.025 0.059 0.035

12.5000 1 .658E+00 3.706E-01 2.029E+00 7.127E+00 9.281E-02 2.727E+00 -0.022 0.098 0.030

15.0000 1 .676E+00 9.579E-01 2.1 39E+00 8.328E+00 1 .105E-01 3.016E+00 -0.020 0.099 0.026

1 7 . 5000 1 .691E+00 5.959E-01 2.237E+00 9.972E+00 1 .275E-01 3.265E+00 -0.018 0.090 0.023

20 .0000 1 . 709E+00 6 . 357E-01 2.390E+00 1 .056E+01 1 .938E-01 3.989E+00 -0.017 0.037 0.021 25.0000 1 .726E+00 8. 180E-01 2.599E+00 1 .261E+01 1 .795E-01 3.857E+00 -0.016 0.033 0.018

30 .0000 1 .793E+00 1 .003E+00 2.796E+00 1 .950E+01 2.027E-01 9. 168E+00 -0.019 0.030 0.015

35.0000 1 .757E+00 1 . 1 90E+00 2.997E+00 1 .626E+01 2.287E-01 9.935E+00 -0.013 0.028 0.019

90.0000 1 .769E+00 1 .379E+00 3.198E+00 1 .790E+01 2.528E-01 9.669E+00 -0.012 0.026 0.012

95.0000 1 .780E+00 1 .569E+00 3.399E+00 1 .999E+01 2.751E-01 9.878E+00 -0.010 0.029 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 3.751E+00 2.226E+01 3. 152E-01 5.291E+00 -0.009 0.022 0.009

60.0000 1 .805E+00 2. 197E+00 3.951E+00 2.356E+01 3.333E-01 5.901E+00 -0.008 0.021 0.009

70.0000 1 .818E+00 2.535E+00 9. 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 9.755E+00 2.817E+01 3. 953E-01 5. 938E+00 -0.005 0.018 0.006

90.0000 1 .838E+00 3. 320E+00 5. 158E+00 3.01 9E+01 9.219E-01 6.161E+00 -0.009 0.017 0.006

100.0000 1 .897E+00 3.719E+00 5.561E+00 3.205E+01 9.998E-01 6.363E+00 -0.009 0.016 0.005

125.0000 1 .869E+00 9.707E+00 6.571E+00 3.618E+01 9.995E-01 6 .799E+00 -0.003 0.019 0.009

150.0000 1 .879E+00 5.705E+00 7.583E+00 3.972E+01 5. 396E-01 7. 150E+00 -0.002 0.013 0.003

175.0000 1 .890E+00 6 .708E+00 8.598E+00 9.282E+01 5.678E-01 7 .952E+00 -0.001 0.012 0.003

200.0000 1 . 900E+00 7.719E+00 9.619E+00 9.557E+01 5. 958E-01 7.716E+00 -0.001 0.011 0.002

250.0000 1 . 91 7E+00 9.739E+00 1 . 165E+01 5.028E+01 6.906E-01 8.157E+00 -0.001 0.010 0.002

300.0000 1 . 931 E+00 1 . 176E+01 1 .369E+01 5.929E+01 6.751E-01 8.51 9E+00 -0.001 0.010 0.001

350 .0000 1 . 993E+00 1 . 380E+01 1 .579E+01 5.769E+01 7.027E-01 8.826E+00 -0.000 0.009 0.001

900 .0000 1 . 952E+00 1 .583E+01 1 .778E+01 6 . 063E+01 7.253E-01 9.091E+00 -0.000 0.009 0.001 950.0000 1 . 961 E+00 1 .787E+01 1 . 983E+01 6 . 329E+01 7.993E-01 9.326E+00 -0.000 0.008 0.001 500.0000 1 . 969E+00 1 . 992E+01 2. 189E+01 6.569E+01 7.609E-01 9.536E+00 -0 .000 0.008 0.001

550 .0000 1 . 976E+00 2. 1 96E+01 2.399E+01 6 .787E+01 7.799E-01 9.726E+00 -0.000 0.008 0.001 600.0000 1 . 983E+00 2.901 E+01 2.599E+01 6 . 988E+01 7 .866E-01 9. 900E+00 -0.000 0.007 0.001 700.0000 1 . 999E+00 2.81 1E+01 3.010E+01 7.395E+01 8.069E-01 1 .021E+01 -0.000 0 .007 0.001 800.0000 2 . 009E+00 3.221E+01 3.921E+01 7.656E+01 8.233E-01 1 .097E+01 -0 .000 0 .007 0.001 900.0000 2.01 3E+00 3 . 631 E+01 3.833E+01 7 . 932E+01 8.367E-01 1 .071E+01 -0.000 0.007 0.000 1000.0000 2.021E+00 9.092E+01 9.299E+01 8. 180E+01 8.981E-01 1 .092E+01 -0.000 0.006 0.000

88
ELECTRONS IN ALUMINUM OO

I = 166.0 eV DENSITY = 2.699E+00 g/cm^

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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .699E+01 6 . 559E-03 1 .650E+01 3.539E-09 2. 132E-09 1 .956E-09 -0.236 0.281 0.275

0.0125 1 . 398E+01 6 .700E-03 1 . 398E+01 5.192E-09 2.583E-09 2.266E-09 -0.229 0.265 0.260

0.0150 1 .220E+01 6 .798E-03 1 .221 E+01 7.111E-09 3.016E-09 3.253E-09 -0.216 0.252 0.298

0.0175 1 .088E+01 6.871E-03 1 .088E+01 9.289E-09 3.935E-09 9.913E-09 -0.209 0.293 0.239

0.0200 9.895E+00 6 . 926E-03 9.851E+00 1 . 170E-03 3.890E-09 5.797E-09 -0.203 0.235 0.232

0 .0250 8.339E+00 7.009E-03 8.396E+00 1 .729E-03 9.615E-09 8. 925E-09 -0.195 0.229 0.221 0.0300 7.288E+00 7.059E-03 7.295E+00 2. 367E-03 5.353E-09 1 .276E-03 -0.188 0.215 0.212

0.0350 6 . 51 OE+00 7.100E-03 6.517E+00 3.093E-03 6 .058E-09 1 .720E-03 -0.183 0.208 0.206

0 . OAOO 5 . 909E+00 7. 1 33E-03 5.916E+00 3. 900E-03 6.736E-09 2.21 9E-03 -0.179 0.202 0.201

0 . 0A5O 5.931E+00 7. 162E-03 5.938E+00 9.782E-03 7.389E-09 2.773E-03 -0.175 0.198 0.196

0.0500 5 . 090E+00 7 . 1 91 E-03 5.097E+00 5.738E-03 8.022E-09 3.391E-03 -0.172 0.199 0.192

0 .0550 9.715E+00 7.217E-03 9.722E+00 6 .763E-03 8.635E-09 9.080E-03 -0.170 0.190 0.189

0 .0600 9 .939E + 00 7 . 293E-03 9.997E+00 7.855E-03 9.231E-09 9.892E-03 -0.167 0.187 0.186

0.0700 3 . 999E+00 7 .295E-03 9.006E+00 1 .023E-02 1 .038E-03 6 .997E-03 -0.163 0.182 0.181

0 . 0800 3.661E+00 7.350E-03 3.669E+00 1 .289E-02 1 . 197E-03 8.162E-03 -0.160 0.178 0.177

0.0900 3. 399E+00 7.91 IE-03 3.902E+00 1 .568E-02 1 .252E-03 9.701E-03 -0.157 0.179 0.173

0.1000 3. 178E+00 7.976E-03 3.186E+00 1 .872E-02 1 .353E-03 1 .138E-02 -0.155 0.171 0.170

0 . 1250 2.782E+00 7.659E-03 2.790E+00 2.71 3E-02 1 .592E-03 1 .738E-02 -0.150 0.165 0.169

0.1500 2.519E+00 7.865E-03 2.521 E+00 3.659E-02 1 .816E-03 2.950E-02 -0.196 0.160 0.160

0.1750 2 . 320E+00 8.096E-03 2.329E+00 9.692E-02 2.028E-03 3. 192E-02 -0.193 0.157 0.156

0 . 2000 2 . 1 75E + 00 8. 399E-03 2. 189E+00 5.802E-02 2.231E-03 3.876E-02 -0.190 0.159 0.153

0 . 2500 1 . 973E+00 8.888E-03 1 . 982E+00 8.219E-02 2.615E-03 5.985E-02 -0.136 0.199 0.198

0 . 3000 1 .890E+00 9.987E-03 1 .850E+00 1 .083E-01 2.981E-03 7. 180E-02 -0.132 0.195 0.199

0 . 3500 1 .798E+00 1 .01 3E-02 1 .758E+00 1 .361E-01 3.333E-03 8.931E-02 -0.129 0.192 0.191

0 .9000 1 .681E+00 1 .082E-02 1 .692E+00 1 .651E-01 3.676E-03 1 .072E-01 -0.127 0.139 0.138

0 .9500 1 . 631 E+00 1 . 1 59E-02 1 .693E+00 1 .951E-01 9.01 3E-03 1 .252E-01 -0.125 0.137 0.135

0 . 5000 1 . 599E+00 1 .230E-02 1 .606E+00 2.259E-01 9.396E-03 1 .933E-01 -0.123 0.135 0.133

0 . 5500 1 .569E + 00 1 .309E-02 1 .577E+00 2.573E-01 9.677E-03 1 .619E-01 -0.121 0.133 0.131 0.6000 1 .591E+00 1 .390E-02 1 .555E+00 2.893E-01 5.005E-03 1 .799E-01 -0.119 0.132 0.130

0 .7000 1 . 508E+00 1 .560E-02 1 .529E+00 3.593E-01 5.660E-03 2.151E-01 -0.116 0.129 0.126

0.8000 1 .987E + 00 1 .739E-02 1 .505E+00 9.203E-01 6.319E-03 2.503E-01 -0.113 0.127 0.129

0 . 9000 1 .979E+00 1 . 925E-02 1 .993E+00 9.871E-01 6.970E-03 2.898E-01 -0.111 0.129 0.121

1 .0000 1 .966E+00 2.11 9E-02 1 .987E+00 5.592E-01 7.630E-03 3. 188E-01 -0.108 0.122 0.119

1 .2500 1 .958E+00 2.630E-02 1 .985E+00 7.226E-01 9.299E-03 9.019E-01 -0.103 0.118 0.113

1 . 5000 1 .960E + 00 3. 177E-02 1 .992E+00 8.906E-01 1 . 100E-02 9.819E-01 -0.097 0.119 0.109

1 .7500 1 .967E+00 3.752E-02 1 .509E+00 1 .057E+00 1 .273E-02 5.599E-01 -0.092 0.111 0.105

2.0000 1 .975E+00 9. 350E-02 1 .518E+00 1 .223E+00 1 .999E-02 6.359E-01 -0.087 0.108 0.101 2.5000 1 .992E+00 5.605E-02 1 .598E+00 1 .599E+00 1 .807E-02 7.895E-01 -0.077 0.102 0.093

3.0000 1 .509E+00 6.929E-02 1 .579E+00 1 .869E+00 2. 173E-02 9.273E-01 -0.067 0.096 0.085

3.5000 1 -525E+00 8.292E-02 1 .608E+00 2. 183E+00 2.599E-02 1 .069E+00 -0.059 0.091 0.079

9 .0000 1 .539E+00 9.702E-02 1 .636E+00 2.991E+00 2.919E-02 1 .199E+00 -0.052 0.086 0.072

9.5000 1 -552E+00 1.11 5E-01 1 .663E+00 2.799E+00 3.297E-02 1 .318E+00 -0.097 0.082 0.067

5.0000 1 .563E+00 1 .263E-01 1 .690E+00 3.092E+00 3.676E-02 1 .936E+00 -0.092 0.078 0.062

5.5000 1 .579E + 00 1 .91 3E-01 1 .715E+00 3.386E+00 9.056E-02 1 .598E+00 -0.039 0.079 0.058

6 .0000 1 .583E+00 1 .567E-01 1 .790E+00 3.675E+00 9.936E-02 1 .659E+00 -0.036 0.071 0.059

7.0000 1 .600E+00 1 .879E-01 1 .788E+00 9.292E+00 5.197E-02 1 .853E+00 -0.032 0.066 0.098

8.0000 1 .619E+00 2.200E-01 1 .839E+00 9.799E+00 5.959E-02 2.033E+00 -0.029 0.061 0.093

9.0000 1 .627E+00 2.526E-01 1 .879E+00 5.333E+00 6.706E-02 2.1 99E+00 -0.026 0.057 0.039

10.0000 1 .638E+00 2.858E-01 1 .929E+00 5.859E+00 7.951E-02 2.352E+00 -0.025 0.059 0.035

12.5000 1 .661E+00 3.706E-01 2.031E+00 7. 123E+00 9.279E-02 2.690E+00 -0.022 0.098 0.030

15.0000 1 .679E+00 9.579E-01 2.136E+00 8.323E+00 1 . 109E-01 2.977E+00 -0.020 0.099 0.026

17.5000 1 .699E + 00 5.959E-01 2.290E+00 9.966E+00 1 .273E-01 3.227E+00 -0.018 0.090 0.023

20.0000 1 .707E+00 6.357E-01 2.393E+00 1 .056E+01 1 .936E-01 3.999E+00 -0.017 0.037 0.021 25.0000 1 .728E+00 8.180E-01 2.596E+00 1 .260E+01 1 .793E-01 3.829E+00 -0.016 0.033 0.018

30.0000 1 .799E+00 1 .003E+00 2.797E+00 1 .999E+01 2.025E-01 9. 197E+00 -0.019 0.030 0.015

35.0000 1 .758E+00 1 . 1 90E+00 2.998E+00 1 .625E+01 2.285E-01 9.921E+00 -0.013 0.028 0.019

90.0000 1 .770E+00 1 .379E+00 3. 199E+00 1 .789E+01 2.526E-01 9.663E+00 -0.012 0.026 0.012

95.0000 1 -780E+00 1 .569E+00 3.399E+00 1 . 993E+01 2.750E-01 9.878E+00 -0.010 0.029 0.011 50.0000 1 . 789E + 00 1 .761E+00 3.550E+00 2.088E+01 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+01 3. 151E-01 5.250E+00 -0.009 0.022 0.009

60.0000 1 .809E+00 2. 197E+00 3.950E+00 2.355E+01 3.332E-01 5.913E+00 -0.008 0.021 0.009

70.0000 1 .81 6E+00 2.535E+00 9.352E+00 2.596E+01 3.661E-01 5.705E+00 -0.006 0.019 0.007

80.0000 1 .827E+00 2 . 927E+00 9.759E+00 2.816E+01 3.953E-01 5.960E+00 -0.005 0.018 0.006

90.0000 1 .837E+00 3.320E+00 5. 156E+00 3.018E+01 9.219E-01 6.186E+00 -0.009 0.017 0.006

100 .0000 1 .895E+00 3.719E+00 5.559E+00 3.209E+01 9.999E-01 6.390E+00 -0.009 0.016 0.005

1 25 .0000 1 .862E+00 9 . 707E+00 6.569E+00 3.618E+01 9. 996E-01 6 .823E+00 -0.003 0.019 0.009

150.0000 1 .876E+00 5.705E+00 7.581E+00 3.972E+01 5. 397E-01 7. 180E+00 -0.002 0.013 0.003

175.0000 1 .888E+00 6 .708E+00 8.596E+00 9.281E+01 5.679E-01 7 .982E+00 -0.001 0.012 0.003

200.0000 1 .898E + 00 7 .719E+00 9.612E+00 9.556E+01 5. 959E-01 7.795E+00 -0.001 0.011 0.002

250 .0000 1 . 91 5E+00 9.739E+00 1 . 165E+01 5.028E+01 6 .907E-01 8. 186E+00 -0.001 0.010 0.002

300 .0000 1 . 929E+00 1 . 176E + 01 1 .369E+01 5.923E+01 6 .753E-01 8.597E+00 -0.001 0.010 0.001

350 .0000 1 . 991 E+00 1 . 380E+01 1 .579E+01 5.769E+01 7.028E-01 8.853E+00 -0.000 0.009 0.001

900 .0000 1 . 951 E+00 1 .583E + 01 1 .778E+01 6.063E+01 7.255E-01 9.1 18E+00 -0.000 0.009 0.001

950 .0000 1 . 959E+00 1 .787E+01 1 .983E+01 6.329E+01 7.999E-01 9.352E+00 -0.000 0.008 0.001

500 .0000 1 . 967E+00 1 . 992E+0

2. 188E+01 6 . 569E+01 7.605E-01 9.562E+00 -0.000 0.008 0.001 550.0000 1 . 979E+00 2. 1 96E+01 2. 399E+01 6 .787E+01 7 .795E-01 9.751E+00 -0.000 0.008 0.001 600.0000 1 . 981 E+00 2.901E+01 2.599E+01 6.987E+01 7.867E-01 9. 929E+00 -0.000 0.007 0.001 700.0000 1 . 992E+00 2.81 1E+01 3.010E+01 7.395E+01 8.070E-01 1 .023E+01 -0.000 0.007 0.001 800.0000 2.002E+00 3.221E+01 3.921 E+01 7.656E+01 8.239E-01 1 .050E+01 -0.000 0.007 0.001

900 . 0000 2.01 1E+00 3.631E+01 3.833E+01 7.932E+01 8.368E-01 1 .073E+01 -0.000 0.007 0.000

1000.0000 2.01 9E+00 9 .092E + 01 9.299E+01 8.180E+01 8.982E-01 1 .099E+01 -0.000 0.006 0.000

k Ev.iluaLod wit.li the densily-eifect correction of inokuti and Smith (1982).

89
ELECTRONS IN SILICON

I = 173.0 eV DENSITY = 2.330E+00 g/cm ^

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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 . 689E+0

7.255E-03 1 .690E+01 3.961E-09 2.289E-09 1 .037E-03 -0.238 0.289 0.278

0.0125 1 .932E+01 7.931 E-03 1 .933E+01 5.079E-09 2.780E-09 1 .332E-03 -0.226 0.268 0.262

0.0150 1 .251 E+01 7.555E-03 1 .252E + 01 6 . 996E-09 3.252E-09 1 .691E-03 -0.217 0.255 0.251 0.0175 1 . 1 15E+01 7.698E-03 1.11 6E+01 9.065E-09 3.709E-09 1 . 963E-03 -0.210 0.295 0.291

0 .0200 1 .010E+01 7 .720E-03 1 . 01 1 E+01 1 . 192E-03 9 . 1 51 E-09 2.298E-03 -0.205 0.238 0.239

0.0250 8 . 556E+00 7 .822E-03 8.569E+00 1 .682E-03 5.000E-09 3.007E-03 -0.196 0.225 0.223

0 .0300 7 .980E+00 7 .892E-03 7.987E+00 2 . 308E-03 5.807E-09 3.766E-03 -0.189 0.216 0.219

0.0350 6 .682E+00 7 . 996E-03 6 .690E+00 3.016E-03 6 .579E-09 9.572E-03 -0.189 0.209 0.207

0 . 0<<00 6 . 067E+00 7 . 988E-03 6 .075E+00 3.802E-03 7.322E-09 5.929E-03 -0.180 0.209 0.202

0 .0^150 5 . 576E+00 8 . 026E-03 5.589E+00 9.661E-03 8.038E-09 6.320E-03 -0.176 0.199 0.197

0.0500 5. 175E+00 8.061 E-03 5. 183E+00 5.591E-03 8.731E-09 7.257E-03 -0.173 0.195 0.193

0 .0550 9.892E+00 8.092E-03 9.850E+00 6.590E-03 9.902E-09 8.235E-03 -0.170 0.191 0.190

0.0600 9.559E+00 8 . 1 23E-03 9.568E+00 7.653E-03 1 .006E-03 9.251E-03 -0.168 0.188 0.187

0.0700 9.107E+00 8 . 185E-03 9. 1 16E+00 9.969E-03 1 .131E-03 1 . 1 39E-02 -0.163 0.183 0.182

0 .0800 3.761E+00 8.298E-03 3.769E+00 1 .251 E-02 1 .251E-03 1 .368E-02 -0.160 0.178 0.177

0 .0900 3 . 987E+00 8.317E-03 3.996E+00 1 .526E-02 1 . 366E-03 1 .608E-02 -0.157 0.175 0.179

0.1000 3.265E+00 8.389E-03 3.279E+00 1 .822E-02 1 .976E-03 1 .861E-02 -0.159 0.171 0.171 0.1250 2.859E+00 8.591E-03 2.867E+00 2.692E-02 1 .737E-03 2.538E-02 -0.199 0.165 0.169

0 . 1 500 2.583E+00 8.821E-03 2.592E+00 3.561E-02 1 .981E-03 3.271E-02 -0.195 0.160 0.159

0.1750 2.385E+00 9.076E-03 2.399E+00 9.566E-02 2.212E-03 9.050E-02 -0.191 0.156 0.155

0 .2000 2 . 236E+00 9.399E-03 2.295E+00 5.696E-02 2.933E-03 9.868E-02 -0.138 0.153 0.152

0 . 2500 2.028E+00 9. 951 E-03 2.038E+00 7.991E-02 2.852E-03 6.592E-02 -0.133 0.198 0.197

0.3000 1 .892E+00 1 .062E-02 1 .903E+00 1 .059E-01 3.298E-03 8.902E-02 -0.129 0.193 0.192

0 . 3500 1 .797E+00 1 . 1 33E-02 1 .809E+00 1 . 323E-01 3.631E-03 1 .027E-01 -0.125 0.190 0.138

0.9000 1 .729E+00 1 .209E-02 1 .791E+00 1 .606E-01 9.003E-03 1 .216E-01 -0.122 0.137 0.135

0.9500 1 .677E+00 1 .290E-02 1 .690E+00 1 .897E-01 9.368E-03 1 .907E-01 -0.119 0.139 0.132

0 . 5000 1 . 638E+00 1 .379E-02 1 .652E+00 2.1 97E-01 9.728E-03 1 .599E-01 -0.116 0.132 0.129

0 .5500 1 .608E+00 1 .961 E-02 1 .623E+00 2.502E-01 5.085E-03 1 .790E-01 -0.119 0.130 0.127

0.6000 1 .585E+00 1 .551E-02 1 .600E+00 2.812E-01 5.991E-03 1 .980E-01 -0.112 0.128 0.125

0 .7000 1 . 551 E+00 1 .790E-02 1 .568E+00 3.999E-01 6 . 198E-03 2.355E-01 -0.108 0.129 0.121 0.8000 1 .529E+00 1 . 938E-02 1 .599E+00 9.086E-01 6 .855E-03 2.721E-01 -0.105 0.121 0.118

0 . 9000 1 .51 6E+00 2. 195E-02 1 .537E+00 9.739E-01 7.569E-03 3.077E-01 -0.102 0.119 0.115

1.0000 1 .507E+00 2. 360E-02 1 .531E+00 5.386E-01 8.275E-03 3.929E-01 -0.100 0.116 0.112

1 .2500 1 . 500E+00 2. 927E-02 1 .529E+00 7.022E-01 1 .007E-02 9.298E-01 -0.099 0.111 0.106

1 .5000 1 .502E+00 3.533E-02 1 .538E+00 8.652E-01 1 . 1 90E-02 5.020E-01 -0.090 0.107 0.101

1 .7500 1 .509E+00 9.171E-02 1 .551E+00 1 .027E+00 1 .376E-02 5.797E-01 -0.086 0.109 0.097

2.0000 1 .518E+00 9 .833E-02 1 .567E+00 1 . 188E+00 1 .565E-02 6 .939E-01 -0.082 0.101 0.099

2.5000 1 .538E+00 6 .223E-02 1 .600E+00 1 .503E+00 1 . 999E-02 7.793E-01 -0.075 0.096 0.087

3.0000 1 . 558E+00 7.682E-02 1 .639E+00 1 .812E+00 2.390E-02 8.976E-01 -0.069 0.091 0.082

3.5000 1 .575E+00 9.1 97E-02 1 .667E+00 2. 1 15E+00 2.736E-02 1 .016E+00 -0.062 0.087 0.076

9.0000 1 .591E+00 1 .076E-01 1 .699E+00 2.912E+00 3.139E-02 1 .131E+00 -0.057 0.083 0.071 9.5000 1 .605E+00 1 .236E-0I 1 .729E+00 2.709E+00 3.535E-02 1 .293E+00 -0.051 0.080 0.067

5 .0000 1 .618E+00 1 .399E-01 1 .758E+00 2.991E+00 3. 937E-02 1 .351E+00 -0.097 0.076 0.063

5.5000 1 .629E+00 1 .566E-01 1 .786E+00 3.273E+00 9.390E-02 1 .956E+00 -0.093 0.073 0.059

6.0000 1 . 639E+00 1 .735E-01 1 .81 3E+00 3.551 E+00 9.792E-02 1 .557E+00 -0.090 0.070 0.056

7.0000 1 .657E+00 2.081 E-01 1 .865E+00 9.095E+00 5.596E-02 1 .798E+00 -0.039 0.065 0.099

8.0000 1 . 672E+00 2.935E-01 1 . 91 6E+00 9.629E+00 6 .399E-02 1 .925E+00 -0.030 0.061 0.095

9.0000 1 .685E+00 2.795E-01 1 .965E+00 5.139E+00 7.136E-02 2.088E+00 -0.027 0.058 0.090

10.0000 1 .697E+00 3. 161E-01 2.01 3E+00 5.692E+00 7.91 9E-02 2.239E+00 -0.025 0.059 0.037

12.5000 1 .721E+00 9.098E-01 2.1 30E+00 6 .899E+00 9.833E-02 2.579E+00 -0.021 0.098 0.031 15.0000 1 .790E+00 5.057E-01 2.295E+00 7. 992E+00 1 .168E-01 2.858E+00 -0.019 0.099 0.026

17.5000 1 .756E+00 6.033E-01 2.359E+00 9.078E+00 1 .395E-01 3.105E+00 -0.017 0.090 0.023

20 .0000 1 .769E+00 7.023E-01 2.972E+00 1 .01 1E+01 1 .51 9E-01 3.323E+00 -0.016 0.037 0.021 25.0000 1 .791E+00 9.035E-01 2.695E+00 1 .205E+01 1 .832E-01 3.699E+00 -0.015 0.033 0.017

30 .0000 1 .809E+00 1 .108E+00 2.917E+00 1 .383E+01 2. 123E-01 9.003E+00 -0.013 0.030 0.015

35.0000 1 .829E+00 1 .319E+00 3.1 39E+00 1 .598E+01 2.391E-01 9.268E+00 -0.012 0.027 0.013

90 .0000 1 .837E+00 1 .523E+00 3.360E+00 1 .702E+01 2.638E-01 9.501E+00 -0.011 0.026 0.012

95.0000 1 .898E+00 1 .733E+00 3.581 E+00 1 .897E+01 2.865E-01 9.709E+00 -0.010 0.029 0.011 50.0000 1 .858E+00 1 . 999E+00 3.802E+00 1 . 982E+01 3.077E-01 9.897E+00 -0.009 0.023 0.010

55.0000 1 .866E+00 2. 156E+00 9.023E+00 2. 1 lOE+01 3.273E-01 5.068E+00 -0.009 0.022 0.009

60.0000 1 .879E+00 2.369E+00 9.299E+00 2.231E+01 3.957E-01 5.226E+00 -0.008 0.021 0.008

70 .0000 1 .888E+00 2.798E+00 9.686E+00 2.955E+01 3.789E-01 5.509E+00 -0.007 0.019 0.007

80.0000 1 . 900E+00 3.230E+00 5.129E+00 2.659E+01 9.083E-01 5.757E+00 -0.006 0.018 0.006

90.0000 1 . 91 OE+00 3.663E+00 5.573E+00 2.896E+01 9.399E-01 5.979E+00 -0.005 0.017 0.006

100.0000 1 . 918E+00 9.099E+00 6.017E+00 3.01 9E+01 9.580E-01 6. 179E+00 -0.009 0.016 0.005

125.0000 1 . 937E+00 5. 1 93E+00 7.1 30E+00 3.900E+01 5.076E-01 6 .606E+00 -0.003 0.019 0.009

1 50.0000 1 . 952E+00 6 . 299E+00 8.296E+00 3.726E+01 5.979E-01 6.960E+00 -0.002 0.013 0.003

175.0000 1 . 969E+00 7.901 E+00 9.365E+00 9.010E+01 5.803E-01 7.261E+00 -0.002 0.012 0.003

200.0000 1 . 975E+00 8.51 1E+00 1 .099E+01 9.262E+01 6.079E-01 7.529E+00 -0.001 0.011 0.002

250.0000 1 . 992E+00 1 .079E+01 1 .273E+01 9.699E+01 6.520E-01 7.969E+00 -0.001 0.010 0.002

300.0000 2.006E+00 1 .298E+01 1 .998E+01 5.056E+01 6 .859E-01 8.325E+00 -0.001 0.010 0.001 350.0000 2.018E+00 1 .522E+01 1 .729E+01 5.367E+01 7.129E-01 8.631E+00 -0.001 0.009 0.001 900.0000 2.029E+00 1 .797E+01 1 . 950E+01 5.639E+01 7.350E-01 8.897E+00 -0.000 0.009 0.001 950.0000 2.038E+00 1 .972E+01 2. 176E+01 5.882E+0i 7.535E-01 9. 131E+00 -0.000 0.008 0.001

500 . 0000 2.096E+00 2. 1 97E+01 2.902E+01 6. 101E+01 7.692E-01 9.391E+00 -0 .000 0.008 0.001 550.0000 2.053E+00 2.923E+01 2.628E+01 6 .299E+01 7.828E-01 9.531E+00 -0.000 0.008 0.001 600.0000 2 . 060E+00 2.698E+01 2.859E+01 6 .982E+01 7.996E-01 9.705E+00 -0.000 0.008 0.001

700 .0000 2.072E+00 3 . 1 OOE+01 3.308E+01 6 .807E+01 8. 199E-01 1 .001E+01 -0.000 0.007 0.001 800.0000 2.082E+00 3.553E+01 3.761E+01 7.090E+01 8. 302E-01 1 .028E+01 -0.000 0.007 0.001 900.0000 2 . 091 E+00 9 . 006E+01 9.215E+01 7.391E+01 8.933E-01 1 .051E+01 -0.000 0 . 007 0.000

1000.0000 2 . 099E+00 9 . 959E+01 9.669E+01 7.567E+01 8 . 592E-01 1 .072E+01 -0.000 0.007 0.000

90
ELECTRONS IN ARGON

I = 188.0 oV DENSITY = 1.662E-03 g/cm^ (20° C)

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 citi^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .997E+01 8. 167E-03 1 .998E+01 3 . 921 E-09 2.896E-09 0.0 -0.293 0.292 0.289

0.0125 1 .271E+01 8.999E-03 1 .271E+01 5.790E-09 3.987E-09 0.0 -0.231 0.279 0.268

0.0150 1 . 1 1 OE+0

8.697E-03 1 .111E+01 7.899E-09 9. 108E-09 0.0 -0.222 0.261 0.255

0.0175 9 . 907E+00 8 .803E-03 9.916E+00 1 .029E-03 9.712E-09 0.0 -0.215 0.251 0.296

0.0200 8.979E+00 8. 926E-03 8.983E+00 1 .289E-03 5.299E-09 0.0 -0.209 0.293 0.238

0 .0250 7 .61 OE+00 9 . 1 07E-03 7.61 9E+00 1 .896E-03 6 .930E-09 0.0 -0.200 0.230 0.226

0.0300 6.657E+00 9.237E-03 6.666E+00 2.599E-03 7.51 lE-09 0.0 -0.193 0.221 0.218

0.0350 5. 950E+00 9.339E-03 5. 959E+00 3. 399E-03 8.597E-09 0.0 -0.187 0.219 0.211

0 . OAOO 5.909E+00 9.915E-03 5.919E+00 9 .276E-03 9.596E-09 0.0 -0.183 0.208 0.205

0 . 0A50 9 . 969E+00 9.982E-03 9.978E+00 5.290E-03 1 .051E-03 0.0 -0.179 0.203 0.200

0 .0500 9.619E+00 9.590E-03 9.623E+00 6.283E-03 1 .199E-03 0.0 -0.176 0.199 0.196

0 .0550 9 . 31 7E+00 9 . 593E-03 9.327E+00 7 .902E-03 1 .235E-03 0.0 -0.173 0.195 0.193

0 .0600 9.067E+00 9.692E-03 9.077E+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 .992E-03 0.0 -0.167 0.186 0.185

0 . 0800 3 . 358E+00 9.821 E-03 3. 368E+00 1 .903E-02 1 .659E-03 0.0 -0.163 0.182 0.180

0.0900 3.11 5E+00 9 . 909E-03 3. 125E+00 1 .712E-02 1 .808E-03 0.0 -0.160 0.178 0.177

0 . 1000 2. 918E+00 1 .OOOE-02 2.928E+00 2.092E-02 1 . 957E-03 0.0 -0.158 0.175 0.179

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 . 1 500 2.312E+00 1 .052E-02 2.323E+00 3.985E-02 2.633E-03 0.0 -0.199 0.169 0.163

0 . 1750 2 . 1 36E+00 1 .081E-02 2. 197E+00 5. 106E-02 2. 990E-03 0.0 -0.196 0.160 0.159

0.2000 2 . 009E+00 1.11 3E-02 2.015E+00 6.309E-02 3.233E-03 0.0 -0.193 0.157 0.156

0 .2500 1 .821 E+00 1 . 182E-02 1 .832E+00 8.920E-02 3.789E-03 0.0 -0.139 0.152 0.151

0 . 3000 1.701 E+00 1 .258E-02 1 .713E+00 1 . 175E-01 9.303E-03 0.0 -0.135 0.198 0.197

0 . 3500 1 .618E+00 1 .390E-02 1 .631E+00 1 .979E-01 9.799E-03 0.0 -0.132 0.195 0.193

0 .9000 1 . 558E+00 1 .927E-02 1 .572E+00 1 .787E-01 5.280E-03 0.0 -0.130 0.192 0.191 0.9500 1 .519E+00 1 .51 9E-02 1 .529E+00 2.109E-01 5.799E-03 0.0 -0.128 0.190 0.138

0.5000 1 .980E+00 1 -616E-02 1 .997E+00 2.990E-01 6.21 lE-03 0.0 -0.126 0.138 0.136

0 . 5500 1 .955E+00 1 .716E-02 1 .972E+00 2.777E-01 6.667E-03 0.0 -0.129 0.136 0.139

0 .6000 1 .935E+00 1 .820E-02 1 .953E+00 3.11 9E-01 7.11 9E-03 0.0 -0.122 0.135 0.132

0 .7000 1 .908E+00 2.036E-02 1 .928E+00 3.819E-01 8.015E-03 0.0 -0.120 0.132 0.129

0.8000 1 . 391 E+00 2.269E-02 1 .919E+00 9.518E-01 8.905E-03 0.0 -0.117 0.129 0.127

0.9000 1 .381E+00 2.502E-02 1 .906E+00 5.227E-01 9.799E-03 0.0 -0.115 0.127 0.129

1 .0000 1 . 376E+00 2.798E-02 1 .909E+00 5.939E-01 1 .068E-02 0.0 -0.119 0.126 0.122

1 .2500 1 . 375E+00 3.399E-02 1 .909E+00 7.718E-01 1 .291E-02 0.0 -0.110 0.122 0.118

1 .5000 1 . 383E+00 9.099E-02 1 .929E+00 9.983E-01 1 .517E-02 0.0 -0.107 0.119 0.119

1 .7500 1 . 399E+00 9.822E-02 1 .992E+00 1 .123E+00 1 .799E-02 0.0 -0.105 0.116 0.111 2.0000 1 . 907E+00 5.581E-02 1 .963E+00 1 -295E+00 1 .973E-02 0.0 -0.103 0.119 0.109

2 . 5000 1 .939E+00 7. 168E-02 1 .505E+00 1 .632E+00 2.936E-02 0.0 -0.099 0.111 0.109

3.0000 1 . 960E+00 8.831E-02 1 .598E+00 1 .959E+00 2.903E-02 0.0 -0.097 0.108 0.101

3 . 5000 1 .989E+00 1 .056E-01 1 .589E+00 2.278E+00 3.370E-02 0.0 -0.095 0.105 0.098

9.0000 1 . 506E+00 1 .233E-01 1 .629E+00 2.589E+00 3.837E-02 0.0 -0.093 0.103 0.096

9.5000 1 .526E+00 1 .915E-01 1 .568E+00 2.892E+00 9.303E-02 0.0 -0.092 0.101 0.093

5 .0000 1 .595E+00 1 .600E-01 1 .705E+00 3. 189E+00 9.766E-02 0.0 -0.090 0.099 0.091 5.5000 1 .562E+00 1 .789E-01 1 .791E+00 3.979E+00 5.227E-02 0.0 -0.089 0.0 98 0.090

6 . 0000 1 .579E+00 1 . 981 E-01 1 .777E+00 3.763E+00 5.689E-02 0.0 -0.088 0.0 96 0.088

7.0000 1 .608E+00 2.373E-01 1 .895E+00 9.315E+00 6.588E-02 0.0 -0.087 0.099 0.085

8.0000 1 .639E+00 2.773E-01 1 .91 lE+00 9.898E+00 7.976E-02 0.0 -0.085 0.0 92 0.083

9.0000 1 .657E+00 3.181E-01 1 .975E+00 5.363E+00 8.397E-02 0.0 -0.089 0.090 0.080

1 0 .0000 1 . 678E+00 3.595E-01 2.037E+00 5.861E+00 9.200E-02 0.0 -0.083 0.088 0.078

12.5000 1 .722E+00 9.651E-01 2. 187E+00 7.095E+00 1 .126E-01 0.0 -0.081 0.089 0.079

15.0000 1 .759E+00 5.733E-01 2.332E+00 8. 151E+00 1 .320E-01 0.0 -0.079 0.081 0.070

17.5000 1 .790E+00 6.833E-01 2.979E+00 9.1 92E+00 1 .505E-01 0.0 -0.077 0.079 0.067

20.0000 1 .818E+00 7.999E-01 2.613E+00 1 .018E+01 1 .680E-01 0.0 -0.076 0.076 0.069

25.0000 1 .869E+00 1 .021E+00 2.885E+00 1 .200E+01 2.009E-01 0.0 -0.079 0.072 0.060

30 .0000 1 . 901 E+00 1 .251E+00 3.152E+00 1 .365E+01 2.296E-01 6.376E-09 -0.071 0.069 0.056

35.0000 1 . 931 E+00 1 .989E+00 3.915E+00 1 .518E+01 2.563E-01 2.311E-02 -0.063 0.066 0.052

90 .0000 1 . 956E+00 1 .718E+00 3.679E+00 1 .659E+01 2.807E-01 6.993E-02 -0.057 0.063 0.098

95.0000 1 . 977E+00 1 . 959E+00 3.931E+00 1 .790E+01 3.031E-01 1 .199E-01 -0.053 0.061 0.095

50 .0000 1 .995E+00 2.1 92E+00 9.187E+00 1 .913E+01 3.238E-01 1 .680E-01 -0.050 0.059 0.092

55.0000 2.01 1E+00 2.930E+00 9.991E+00 2.029E+01 3.931E-01 2.226E-01 -0.098 0.056 0.039

60.0000 2.025E+00 2.670E+00 9.695E+00 2.1 39E+01 3.610E-O1 2.769E-01 -0.096 0.055 0.037

70 .0000 2.050E+00 3.1 52E+00 5.202E+00 2.391E+01 3.939E-01 3.820E-01 -0.093 0.052 0.033

80.0000 2 .071 E+00 3.637E+00 5.708E+00 2.525E+01 9.220E-01 9.807E-01 -0.091 0.099 0.030

90 .0000 2.089E+00 9 . 1 25E+00 6.219E+00 2.692E+01 9.979E-01 5.729E-01 -0.090 0.097 0.027

100.0000 2. 105E+00 9.619E+00 6 .71 9E+00 2.897E+01 9.702E-01 6 .588E-01 -0.038 0.095 0.025

125.0000 2 . 1 38E+00 5.895E+00 7 . 982E+00 3. 188E+01 5. 183E-01 8.510E-01 -0.036 0.091 0.021

1 50 .0000 2 . 1 69E+00 7 .083E+00 9.297E+00 3.979E+01 5.569E-01 1 .018E+00 -0.039 0.039 0.018

175.0000 2 . 1 85E+00 8. 326E+00 1 .051E+01 3.732E+01 5.887E-01 1 .166E+00 -0.032 0.036 0.016

200 .0000 2 . 209E+00 9.573E+00 1 .178E+01 3.957E+01 6.155E-01 1 .301E+00 -0.030 0.035 0.015

250 .0000 2. 239E+00 1 .208E+01 1 .931E+01 9.391E+01 6.583E-01 1 .591E+00 -0.027 0.032 0.012

300.0000 2.257E+00 1 .959E+01 1 .685E+01 9.663E+01 6.91 1 E-01 1 .759E+00 -0.029 0.030 0.010

350.0000 2.275E+00 1 .71 1E+01 1 .938E+01 9 . 990E+01 7. 179E-01 1 .997E+00 -0.021 0.029 0.009

900.0000 2 . 291 E+00 1 . 963E+01 2. 1 92E+01 5. 182E+01 7.389E-01 2.125E+00 -0.019 0.027 0 .008

950 .0000 2 . 309E+00 2.216E+01 2.996E+01 5. 398E+01 7.569E-01 2.290E+00 -0.017 0.026 0.007

500 .0000 2.315E+00 2.969E+01 2.700E+01 5.592E+01 7.722E-01 2.999E+00 -0.016 0.026 0.007

550.0000 2 . 325E+00 2.722E+01 2. 959E+01 5.769E+01 7.859E-01 2.587E+00 -0.019 0.025 0.006

600 . 0000 2. 339E+00 2. 975E+01 3.209E+01 5 . 932E+01 7.970E-01 2.721E+00 -0.013 0.029 0.006

700 .0000 2. 399E+00 3.983E+01 3.718E+01 6 .221 E+01 8. 163E-01 2. 966E+00 -0.011 0.023 0.005

800.0000 2. 361E+00 3.990E+01 9.227E+01 6 .973E+01 8.319E-01 3. 189E+00 -0.010 0.022 0.009

900.0000 2. 372E+00 9 .999E+01 9.736E+01 6.696E+01 8.997E-01 3.380E+00 -0.009 0.021 0.009

1000.0000 2. 382E+00 5 . 007E+01 5.295E+01 6 .897E+01 8.559E-01 3.558E+00 -0.009 0.021 0.003
ELECTRONS IN TITANIUM

I = 233.0 eV DENSITY = A.5A0E+00 g/cm^

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d ( looI )/dCloqI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

CDELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .667E+01 9 .835E-03 1 .667E+01 6 . 1 06E-06 3.509E-06 2.037E-03 -0.256 0.313 0.303

0.0125 1 .231E + 01 1 .025E-02 1 .232E+01 5.983E-06 6.31 9E-06 2.585E-03 -0.262 0.293 0.286

0.0150 1 .078E + 01 1 .056E-02 1 .079E+01 8. 157E-06 5. 109E-06 3. 168E-03 -0.232 0.278 0.270 0.0175 9.636E+00 1 .080E-02 9.666E+00 1 .061 E-03 5.878E-06 3.727E-03 -0.226 0.266 0.259

0 .0200 8 . 737E+00 1 . 099E-02 8 . 768E+00 1 . 336E-03 6 .629E-06 6.320E-03 -0.218 0.257 0.250

0.0250 7 . 626E+00 1 . 1 29E-02 7 .635E+00 1 . 956E-03 8 . 081 E-06 5.551E-03 -0.208 0 . 263 0.237

0.0300 6 . 503E + 00 1 . 1 50E-02 6 . 51 6E+00 2.677E-03 9.672E-06 6 .838E-03 -0 . 200 0.232 0.227

0 .0350 5.81 9E+00 1 . 167E-02 5.831E+00 3.690E-03 1 .081 E-03 8.181E-03 -0.196 0.226 0.220

0 . OAOO 5 . 290E + 00 1 . 180E-02 5 . 301 E+00 6 . 390E-03 1 .210E-03 9.578E-03 -0.189 0.217 0.216

0 . 0A50 6 .867E + 00 1 . 1 92E-02 6.879E+00 5. 375E-03 1 .335E-03 1 . 103E-02 -0.185 0.212 0.208

0.0500 6 . 522E+00 1 .202E-02 6 . 536E+00 6.639E-03 1 .656E-03 1 .253E-02 -0.181 0.207 0.206

0 .0550 6 . 236E+00 1 . 21 OE-02 6.266E+00 7 .579E-03 1 .576E-03 1 .607E-02 -0.178 0.203 0.200 0.0600 3 . 990E+00 1 .218E-02 6.002E+00 8.793E-03 1 .689E-03 1 .567E-02 -0.175 0.199 0.196 0.0700 3 . 598E + 00 1 .233E-02 3.61 1E+00 1 .163E-02 1 . 909E-03 1 .899E-02 -0.170 0.193 0.191

0 . 0800 3.298E+00 1 .266E-02 3.31 1E+00 1 .633E-02 2.11 9E-03 2.267E-02 -0.166 0.188 0.186

0.0900 3 . 060E+00 1 .259E-02 3.073E+00 1 .766E-02 2.321E-03 2.61 IE-02 -0.163 0.183 0.182

0.1000 2 . 867E+00 1 .272E-02 2.880E+00 2.083E-02 2.51 6E-03 2.987E-02 -0.160 0.180 0.178

0 . 1 250 2 . 51 6E+00 1 .306E-02 2.527E+00 3.013E-02 2. 971E-03 3.978E-02 -0.153 0.172 0.171

0 . 1 500 2 . 276E+00 1 . 361 E-02 2.287E+00 6.056E-02 3.396E-03 5.023E-02 -0.168 0.166 0.165

0 . 1 750 2 . 1 01 E+00 1 . 379E-02 2.115E+00 5.1 95E-02 3.796E-03 6 . 1 05E-02 -0.166 0.162 0.160

0 . 2000 1 . 971 E + 00 1.61 9E-02 1 . 985E+00 6.616E-02 6.176E-03 7.212E-02 -0.160 0.158 0.156

0 .2500 1 . 789E + 00 1 .506E-02 1 .806E+00 9.067E-02 6.892E-03 9.667E-02 -0.136 0.151 0.150

0 . 3000 1 . 670E + 00 1 . 600E-02 1 .686E+00 1 .196E-01 5.563E-03 1 .176E-01 -0.129 0.166 0.165

0.3500 1 .588E + 00 1 .702E-02 1 .605E+00 1 .698E-01 6.206E-03 1 .602E-01 -0.125 0.162 0.160

0 .6000 1 . 528E + 00 1 .81 IE-02 1 .566E+00 1 .816E-01 6 .826E-03 1 .629E-01 -0.121 0.138 0.136

0.6500 1 . 683E + 00 1 . 925E-02 1 .502E+00 2.166E-01 7.628E-03 1 .855E-01 -0.118 0.135 0.133

0.5000 1 . 669E + 00 2.066E-02 1 .670E+00 2.681E-01 8 . 021 E-03 2.080E-01 -0.115 0.133 0.130

0.5500 1 .623E+00 2.169E-02 1 .665E+00 2.826E-01 8.607E-03 2.306E-01 -0.112 0.130 0.127

0.6000 1 .602E+00 2.297E-02 1 .625E+00 3. 173E-01 9. 186E-03 2.526E-01 -0.109 0.128 0.126

0.7000 1 . 373E+00 2.566E-02 1 . 399E+00 3.881E-01 1 .036E-02 2. 969E-01 -0.106 0.123 0.120

0.8000 1 . 355E+00 2.868E-02 1 .383E+00 6.601E-01 1 .168E-02 3.607E-01 -0.100 0.120 0.116

0 . 9000 1 . 363E + 00 3.161E-02 1 .376E+00 5.326E-01 1 .261E-02 3.861E-01 -0.096 0.116 0.112

1 .0000 1 . 335E+00 3.666E-02 1 .370E+00 6.055E-01 1 .375E-02 6.270E-01 -0.092 0.113 0.108

1 .2500 1 . 328E + 00 6.250E-02 1 .371E+00 7.881E-01 1 .662E-02 5.317E-01 -0.086 0.107 0.100

1 . 5000 1 . 330E + 00 5 . 1 07E-02 1 .381E+00 9.699E-01 1 .951E-02 6.321E-01 -0.078 0.102 0.096

1 .7500 1 .336E + 00 6.006E-02 1 .396E+00 1 . 150E+00 2.266E-02 7.277E-01 -0.073 0.097 0.089

2 .0000 1 . 363E + 00 6 . 960E-02 1 .612E+00 1 .328E+00 2.539E-02 8. 183E-01 -0.070 0.093 0.086

2.5000 1 . 359E + 00 8.896E-02 1 .668E+00 1 .678E+00 3.1 37E-02 9.855E-01 -0.066 0.087 0.076

3.0000 1 . 376E+00 1 .096E-01 1 .685E+00 2.01 9E+00 3.760E-02 1 .136E+00 -0.060 0.082 0.071 3.5000 1 .391E+00 1 .306E-01 1 .521E+00 2.351E+00 6.365E-02 1 .271E+00 -0.057 0.078 0.066

6.0000 1 .605E+00 1 .523E-01 1 .557E+00 2.676E+00 6.969E-02 1 .395E+00 -0.056 0.075 0.063

6.5000 1 .618E+00 1 .766E-01 1 .593E+00 2. 993E+00 5.552E-02 1 -509E+00 -0.052 0.072 0.059

5.0000 1 .630E+00 1 . 976E-01 1 .627E+00 3.306E+00 6.152E-02 1 .615E+00 -0.050 0.069 0.057

5.5000 1 .661E+00 2.205E-01 1 .661E+00 3.608E+00 6.767E-02 1 .71 3E+00 -0.068 0.067 0.056

6.0000 1 .651E+00 2.660E-01 1 .695E+00 3.906E+00 7.337E-02 1 .806E+00 -0.067 0.065 0.052

7.0000 1 .669E+00 2. 91 9E-01 1 .761E+00 6.685E+00 8.502E-02 1 .975E+00 -0.066 0.062 0.069

8.0000 1 .685E + 00 3.608E-01 1 .825E+00 5.062E+00 9.663E-02 2. 129E+00 -0.061 0.059 0.065

9 .0000 1 .698E+00 3.906E-01 1 .889E+00 5.581E+00 1 .076E-01 2.271E+00 -0.038 0.056 0.063

10.0000 1 .510E + 00 6.61 lE-01 1 .952E+00 6 . 1 02E+00 1 . 185E-01 2.602E+00 -0.036 0.056 0.060

12.5000 1 .535E+00 5.701E-01 2.105E+00 7.335E+00 1 .665E-01 2.696E+00 -0.030 0.069 0.035

15.0000 1 .555E + 00 7.01 9E-01 2.257E+00 8.681E+00 1 .690E-01 2. 953E+00 -0.026 0.065 0.031

1 7 . 5000 1 . 571 E+00 8.361E-01 2.607E+00 9.556E+00 1 .919E-01 3.182E+00 -0.023 0.062 0.027

20 .0000 1 .586E+00 9.721E-01 2.556E+00 1 .056E+01 2.136E-01 3.388E+00 -0.020 0.039 0.026

25.0000 1 .606E+00 1 .268E+00 2.856E+00 1 .261E+01 2.527E-01 3.766E+00 -0.016 0.035 0.020

30.0000 1 .622E+00 1 .528E+00 3. 150E+00 1 .608E+01 2.875E-01 6.050E+00 -0.016 0.032 0.017

35.0000 1 .636E+00 1 .81 1E+00 3.667E+00 1 .560E+01 3.187E-01 6.313E+00 -0.013 0.029 0.016

60.0000 1 .668E+00 2.096E+00 3.766E+00 1 .699E+01 3.667E-01 6.565E+00 -0.011 0.027 0.013

65.0000 1 . 658E+00 2.386E+00 6.062E+00 1 .827E+01 3.721 E-01 6.752E+00 -0.010 0.026 0.011 50.0000 1 . 667E+00 2.673E+00 6.360E+00 1 . 966E+01 3. 952E-01 6.939E+00 -0.010 0.026 0.010

55 .0000 1 .675E+00 2 . 963E+00 6.639E+00 2.058E+01 6. 163E-01 5.110E+00 -0.009 0.023 0.009

60.0000 1 .683E+00 3 . 255E+00 6. 938E+00 2.162E+01 6.357E-01 5.266E+00 -0.009 0.022 0.009

70.0000 1 .696E+00 3.863E+00 5.538E+00 2.353E+01 6.702E-01 5.567E+00 -0.008 0.021 0.007

80 .0000 1 .707E+00 6.633E+00 6.160E+00 2.525E+01 5.000E-01 5.792E+00 -0.007 0.019 0.006 90.0000 1 .716E+00 5 . 027E+00 6.763E+00 2.680E+01 5.260E-01 6.010E+00 -0.006 0.018 0.006

100 .0000 1 .726E+00 5.623E+00 7 . 368E+00 2.822E+01 5.690E-01 6.206E+00 -0.006 0.018 0.005

125.0000 1 .762E+00 7. 122E+00 8.866E+00 3.1 32E+01 5. 963E-01 6.626E+00 -0.005 0.016 0.006

150.0000 1 .756E+00 8. 629E+00 1 .039E+01 3.392E+01 6.332E-01 6.976E+00 -0.006 0.015 0.003

175.0000 1 .768E+00 1 . 01 6E+01 1 .191E+01 3.617E+01 6 .630E-01 7.270E+00 -0.003 0.016 0.003

200 .0000 1 .778E+00 1 . 166E+01 1 .366E+01 3.816E+01 6 .876E-01 7.529E+00 -0.002 0.013 0.003

250.0000 1 . 796E+00 1 .671E+01 1 . 651 E+01 6. 169E+01 7.262E-01 7.965E+00 -0.002 0.012 0.002

300 .0000 1 .808E+00 1 . 777E+01 1 . 958E+01 6.627E+01 7.551E-01 8.323E+00 -0.001 0.011 0.002

350 .0000 1.81 9E+00 2 . 086E+01 2 . 266E+01 6.666E+01 7.778E-01 8.627E+00 -0.001 0.011 0.001

600 .0000 1 .828E+00 2.391E+01 2.576E+01 6.871E+01 7.962E-01 8.891E+00 -0.001 0.010 0.001

650 .0000 1 .837E+00 2.698E+01 2.882E+01 5.055E+01 8.11 3E-01 9. 125E+00 -0.001 0.010 0.001 500.0000 1 .866E+00 3. 006E+01 3 . 1 91 E+01 5.21 9E+01 8.261E-01 9.336E+00 -0.001 0.010 0.001 550.0000 1 .851 E+00 3.315E+01 3.500E+01 5. 369E+01 8.351E-01 9.526E+00 -0.000 0.009 0.001 600.0000 1 .857E+00 3 . 623E+01 3.809E+01 5.506E+01 8.666E-01 9.697E+00 -0.000 0.009 0.001 700.0000 1 .868E+00 6.261E+01 6.628E+01 5.769E+01 8.603E-01 1 .OOOE+01 -0.000 0.009 0.001 800.0000 1 .878E+00 6 .859E+01 5.067E+01 5. 960E+01 8.728E-01 1 .027E + 01 -0.000 0.009 0.001

900 .0000 1 .886E+00 5.678E+01 5.656E+01 6.167E+01 8.831E-01 1 .051E+01 -0.000 0.008 0.001

1 000 .0000 1 .893E+00 6 .097E+01 6.286E+01 6 . 31 5E+01 8.916E-01 1 .072E+01 -0.000 0.008 0.001

92
ELECTRONS IN IRON

I = 286.0 eV DENSITY = 7.879E+00 g/cm ^

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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 . 388E+01 1 . 1 38E-02 1 .390E+01 9.329E-09 9.203E-09 2.979E-03 -0.270 0.338 0.329

0.0125 1 . 185E+01 1 . 1 93E-02 1 . 186E+01 6.289E-09 5. 188E-09 3. 157E-03 -0.255 0.319 0.302

0.0150 1 .090E<-01 1 .235E-02 1 .091 E+01 8.539E-09 6 . 1 51 E-09 3.866E-03 -0.299 0.297 0.286

0.0175 9. 31 OE + 00 1 .269E-02 9. 323E+00 1 . 108E-03 7.092E-09 9.602E-03 -0.235 0.289 0.279

0 .0200 8 . 956E+00 1 .296E-02 8.969E+00 1 . 390E-03 8.013E-09 5.365E-03 -0.228 0.273 0.269

0.0250 7 . 1 99E + 00 1 . 338E-02 7.213E+00 2.032E-03 9 .800E-09 6 . 975E-03 -0.217 0.257 0.299

0.0300 6 . 31 6E+00 1 . 369E-02 6.330E+00 2.779E-03 1 . 152E-03 8.696E-03 -0.209 0.295 0.239

0.0350 5.658E+00 1 . 399E-02 5.672E+00 3.610E-03 1 . 31 7E-03 1 .053E-02 -0.202 0.235 0.230

0 . 0<i00 5 . 1 99E+00 1 .919E-02 5.163E+00 9.536E-03 1 .978E-03 1 .298E-02 -0.196 0.228 0.223

0.0050 9.791 E+00 1 .931 E-02 9.756E+00 5.596E-03 1 .633E-03 1 .955E-02 -0.192 0.222 0.217

0.0500 9 . 908E + 00 1 .996E-02 9.922E+00 6.637E-03 1 .789E-03 1 .673E-02 -0.188 0.216 0.212

0.0550 9 . 1 29E + 00 1 .959E-02 9. 199E+00 7.806E-03 1 . 930E-03 1 . 902E-02 -0.189 0.212 0.208

0.0600 3.893E+00 1 .971 E-02 3.908E+00 9.050E-03 2.073E-03 2. 193E-02 -0.181 0.207 0.209

0.0700 3 . 51 9E + 00 1 .993E-02 3.529E+00 1 . 175E-02 2.398E-03 2.657E-02 -0.175 0.200 0.198

0 .0800 3.223E+00 1 .512E-02 3.238E+00 1 .971 E-02 2.61 lE-03 3.211E-02 -0.170 0.195 0.192

0.0900 2. 992E+00 1 .531E-02 3.007E+00 1 .792E-02 2.863E-03 3.801E-02 -0.166 0.190 0.187

0.1000 2.809E+00 1 .598E-02 2.820E+00 2.1 36E-02 3. 106E-03 9.922E-02 -0.162 0.185 0.183

0 . 1 250 2 . 960E + 00 1 .593E-02 2.976E+00 3.085E-02 3.679E-03 6 .070E-02 -0.159 0.177 0.175

0.1500 2.226E+00 1 .639E-02 2.292E+00 9. 199E-02 9.212E-03 7.799E-02 -0.198 0.170 0.168

0.1750 2.057E+00 1 .687E-02 2.079E+00 5.310E-02 9.719E-03 9.538E-02 -0.193 0.169 0.162

0.2000 1 . 930E+00 1 .736E-02 1 . 997E+00 6 .556E-02 5.1 90E-03 1 .127E-01 -0.139 0.160 0.158

0.2500 1 .753E+00 1 .892E-02 1 .771E+00 9.257E-02 6.085E-03 1 .967E-01 -0.133 0.152 0.151 0.3000 1 .636E+00 1 .956E-02 1 .656E+00 1 .218E-01 6.923E-03 1 .797E-01 -0.128 0.197 0.195

0 . 3500 1 . 556E + 00 2.079E-02 1 .576E+00 1 .528E-01 7.720E-03 2. 1 16E-01 -0.129 0.192 0.190

0 .9000 1 .997E+00 2.209E-02 1 .51 9E+00 1 .851E-01 8.989E-03 2.927E-01 -0.120 0.138 0.136

0 .9500 1 .953E+00 2.396E-02 1 .977E+00 2. 186E-01 9.236E-03 2.731E-01 -0.117 0.135 0.133

0 . 5000 1 .920E+00 2.989E-02 1 .995E+00 2.528E-01 9.968E-03 3.027E-01 -0.119 0.132 0.129

0.5500 1 . 399E+00 2.638E-02 1 .921E+00 2.877E-01 1 .069E-02 3.317E-01 -0.112 0.130 0.127

0 .6000 1 . 379E+00 2.791E-02 1 .902E+00 3.231E-01 1 . 190E-02 3.601E-01 -0.109 0.127 0.129

0.7000 1 . 395E+00 3. 1 12E-02 1 .376E+00 3. 952E-01 1 .281E-02 9.152E-01 -0.105 0.123 0.120

0.8000 1 . 327E+00 3.998E-02 1 .362E+00 9.683E-01 1 .920E-02 9.682E-01 -0.101 0.120 0.116

0 . 9000 1 . 31 6E+00 3.797E-02 1 .359E+00 5.920E-01 1 .559E-02 5.1 95E-01 -0.098 0.117 0.112

1 .0000 1 . 308E+00 9. 160E-02 1 .350E+00 6.159E-01 1 .697E-02 5.690E-01 -0.095 0.119 0.109

1 . 2500 1 .302E+00 5. 117E-02 1 .353E+00 8.01 IE-01 2.099E-02 6 .865E-01 -0.088 0.108 0.102

1 .5000 1 . 309E+00 6 . 1 37E-02 1 .365E+00 9.851E-01 2.393E-02 7. 962E-01 -0.082 0.103 0.096

1 .7500 1 .310E+00 7.206E-02 1 .382E+00 1 . 167E+00 2.795E-02 8.990E-01 -0.077 0.099 0.091

2 .0000 1 .317E+00 8.315E-02 1 .900E+00 1 .397E+00 3.099E-02 9. 959E-01 -0.073 0.095 0.086

2.5000 1 . 333E+00 1 .063E-01 1 .990E+00 1 .699E+00 3.812E-02 1 . 179E+00 -0.067 0.089 0.079

3.0000 1 . 399E+00 1 .306E-01 1 .980E+00 2.092E+00 9.527E-02 1 .333E+00 -0.062 0.089 0.073

3.5000 1 .365E+00 1 .557E-01 1 .520E+00 2.375E+00 5.293E-02 1 .978E+00 -0.059 0.080 0.068

9 .0000 1 .378E+00 1 .819E-01 1 .560E+00 2.700E+00 5. 959E-02 1 .610E+00 -0.056 0.076 0.069

9 . 5000 I . 391 E + 00 2.077E-01 1 .599E+00 3.016E+00 6.661E-02 1 .730E+00 -0.059 0.073 0.061 5.0000 1 .903E+00 2. 396E-01 1 .638E+00 3.325E+00 7.361E-02 1 .892E+00 -0.052 0.071 0.058

5.5000 1 .91 9E+00 2.61 9E-01 1 .676E+00 3.627E+00 8.053E-02 1 .996E+00 -0.050 0.069 0.056

6 .0000 1 .929E+00 2.896E-01 1 .713E+00 3.922E+00 8.738E-02 2.093E+00 -0.099 0.066 0.053

7.0000 1 .992E+00 3.960E-01 1 .788E+00 9.993E+00 1 .008E-01 2.21 9E+00 -0.096 0.063 0.050

8.0000 1 .957E+00 9 .036E-01 1 .861E+00 5.092E+00 1 .139E-01 2.377E+00 -0.099 0.060 0.097

9 .0000 1 .971 E+00 9.622E-01 1 .933E+00 5.569E+00 1 .266E-01 2.521E+00 -0.092 0.057 0.099

10.0000 1 .983E+00 5.216E-01 2.005E+00 6.077E+00 1 .389E-01 2.652E+00 -0.090 0.055 0.091 12.5000 1 .509E+00 6 .731E-01 2. 182E+00 7.272E+00 1 .681E-01 2.992E+00 -0.036 0.051 0.037

15.0000 1 .529E+00 8.279E-01 2.357E+00 8.379E+00 1 .951E-01 3.1 92E+00 -0.032 0.097 0.033

17.5000 1 .596E+00 9.852E-01 2.531E+00 9.397E+00 2.202E-01 3.912E+00 -0.029 0.099 0.029

20.0000 1 .560E+00 1 . 195E+00 2.709E+00 1 .035E+01 2.935E-01 3.610E+00 -0.026 0.091 0.027

25.0000 1 .583E+00 1 .968E+00 3.050E+00 1 .209E+01 2.859E-01 3.956E+00 -0.021 0.037 0.022

30.0000 1 .600E+00 1 .795E+00 3.396E+00 1 .365E+01 3.221E-01 9.251E+00 -0.018 0.039 0.019

35.0000 1 .615E+00 2. 126E+00 3.791E+00 1 .505E+01 3.596E-01 9.508E+00 -0.016 0.032 0.016

90.0000 1 .627E+00 2.960E+00 9.087E+00 1 .633E+01 3.839E-01 9.736E+00 -0.019 0.030 0.019

95.0000 1 .638E+00 2.797E+00 9.939E+00 1 .750E+01 9.099E-01 9.991E+00 -0.013 0.028 0.013

50.0000 1 .697E+00 3.135E+00 9.782E+00 1 .859E+01 9.328E-01 5. 126E+00 -0.012 0.027 0.012

55.0000 1 .655E+00 3.975E+00 5. 130E+00 1 . 959E+01 9.590E-01 5.295E+00 -0.011 0.025 0.011 60.0000 1 .663E+00 3.816E+00 5.979E+00 2.059E+01 9.735E-01 5.951E+00 -0.010 0.029 0.010

70.0000 1 .676E+00 9.503E+00 6.178E+00 2.226E+01 5.077E-01 5.729E+00 -0.009 0.023 0.003

80.0000 1 .687E+00 5.1 93E+00 6 .880E+00 2.379E+01 5.370E-01 5. 973E+00 -0.008 0.021 0.007

90.0000 1 .697E+00 5.887E+00 7.589E+00 2.517E+01 5.625E-01 6.189E+00 -0.008 0.020 0.006

100.0000 1 .705E+00 6 . 589E+00 8.289E+00 2.693E+01 5.898E-01 6.389E+00 -0.007 0.019 0.006

1 25 .0000 1 .723E+00 8 . 336E+00 1 .006E+01 2.917E+01 6.303E-01 6.801E+00 -0.006 0.018 0.005

1 50.0000 1 .738E+00 1 . 0 1 OE+0

1 . 189E+01 3. 196E+01 6 .655E-01 7. 196E+00 -0.005 0.017 0.009

175.0000 1 .750E+00 1 . 187E+01 1 .362E+01 3. 392E+01 6 . 937E-01 7.990E+00 -0.009 0.016 0.003

200 .0000 1 .760E+00 1 .369E+01 1 .590E+01 3.515E+01 7. 169E-01 7 .696E+00 -0.009 0.015 0.003

250 . 0000 1 . 777E + 00 1 .720E+01 1 .898E+01 3.807E+01 7 .528E-01 8 . 1 28E+00 -0.003 0.019 0.002

300 .0000 1 .791E+00 2.077E+01 2.256E+01 9.098E+01 7 .797E-01 8.989E+00 -0.002 0.013 0.002

350.0000 1 .802E+00 2.935E+01 2.615E+01 9.259E+01 8.006E-01 8.787E+00 -0.002 0.012 0.002

900 . 0000 1 .8I2E+00 2.793E+01 2.979E+01 9.933E+01 8. 179E-01 9.050E+00 -0.001 0.012 0.001

950 .0000 1 .820E+00 3. 1 52E+01 3.339E+01 9.592E+01 8.31 3E-01 9.283E+00 -0.001 0.011 0.001

500 .0000 1 .828E+00 3.512E+01 3.699E+01 9.739E+01 8.930E-01 9.991E+00 -0.001 0.011 0.001

550 .0000 1 .835E+00 3.871E+01 9.055E+01 9.863E+01 8.530E-01 9.680E+00 -0.001 0.011 0.001

600 .0000 1 .891E + 00 9.231E+01 9 .91 5E+01 9.981E+01 8.616E-01 9.853E+00 -0.001 0.011 0.001 700.0000 1 .852E+00 9 . 951 E+01 5.1 37E+01 5. 1 91E+01 8.758E-01 1 .016E+01 -0.001 0.010 0.001 800.0000 1 .862E+00 5.673E+01 5.859E+01 5.373E+01 8.871E-01 1 .093E+01 -0.000 0.010 0.001

900 .0000 1 .871E+00 6 . 399E+01 6.581E+01 5.539E+01 8. 963E-01 1 .066E+01 -0.000 0.010 0.001 1000.0000 1 .878E+00 7.1 16E+01 7.309E+01 5.678E+01 9.090E-01 1 .087E+01 -0.000 0.009 0.001
ELECTRONS IN COPPER

I = 322.0 eV DENSITY = 8.960E+00 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( logI )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .318E+01 1 .21 3E-02 1 .319E+01 4.601E-04 4.701E-04 1 .244E-03 -0.280 0.354 0.337

0.0125 1 . 1 27E+0

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 9.917E+00 9.028E-04 6 . 904E-04 1 . 938E-03 -0.251 0.310 0.297

0.0175 8.874E+00 1 . 366E-02 8.887E+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 .465E-03 9.01 9E-04 2.683E-03 -0.235 0.284 0.273

0 .0250 6 .877E+00 1 .449E-02 6 .892E + 00 2.1 38E-03 1 . 105E-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 5.416E+00 1 .518E-02 5.431E+00 3.788E-03 1 .491 E-03 5.247E-03 -0.208 0.243 0.237

0.0400 4.931E+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-03 7.259E-03 -0.197 0.229 0.224

0.0500 4 . 226E+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. 961E+00 1 .600E-02 3. 977E+00 8. 164E-03 2.194E-03 9.542E-03 -0.189 0.218 0.214

0.0600 3 . 736E^00 1.61 5E-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 3.098E+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 2.894E+00 1 .868E-02 3.267E-03 2.013E-02 -0.171 0.196 0.193

0.1000 2.698E+00 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+00 3.211E-02 4.208E-03 3.583E-02 -0.157 0.182 0.180

0.1500 2 . 1 46E+00 1 .816E-02 2. 164E+00 4.314E-02 4.822E-03 5.053E-02 -0.149 0.174 0.172

0 . 1 750 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 .881E+00 6 .807E-02 5. 950E-03 8.595E-02 -0.135 0.162 0.159

0 . 2500 1 .691E+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 .601E+00 1 .263E-01 7.945E-03 1 .603E-01 -0.121 0.145 0.143

0.3500 1 .501E+00 2.307E-02 1 .524E+00 1 .584E-01 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 .370E+00 2.757E-02 1 .398E+00 2.617E-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 4.173E-01 -0.097 0.117 0.113

0 .8000 1 .281 E+00 3.803E-02 1 .319E+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 .312E+00 5.604E-01 1 .782E-02 5.280E-01 -0.091 0.110 0.105

1 .0000 1 .263E+00 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 .313E+00 8.276E-01 2.328E-02 7.01 1 E-01 -0.083 0.101 0.095

1 .5000 1 .259E+00 6 .733E-02 1 .327E+00 1 .017E+00 2.720E-02 8. 121E-01 -0.078 0.097 0.090

1 .7500 1 .265E+00 7 .896E-02 1 .344E+00 1 .204E+00 3.113E-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 .01 lE+00 -0.071 0.090 0.081 2.5000 1 .289E+00 1 . 162E-01 1 .405E+00 1 .750E+00 4.302E-02 1 . 186E+00 -0.065 0.084 0.075

3.0000 1 .305E+00 1 .425E-01 1 .448E+00 2.101E+00 5.095E-02 1 .343E+00 -0.060 0.079 0.069

3.5000 1 . 320E+00 1 .697E-01 1 .490E+00 2.441E+00 5.885E-02 1 .486E+00 -0.056 0.076 0.065

4.0000 1 . 334E+00 1 . 976E-01 1 .531E+00 2.772E+00 6.668E-02 1 .617E+00 -0.053 0.072 0.061 4.5000 1 . 346E+00 2.261 E-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 .850E+00 -0.049 0.067 0.055

5.5000 1 . 368E+00 2.847E-01 1 .653E+00 3.715E+00 8.965E-02 1 .954E+00 -0.047 0.065 0.052

6.0000 1 . 378E+00 3. 146E-01 1 .693E+00 4.013E+00 9.710E-02 2.052E+00 -0.046 0.063 0.050

7 .0000 1 . 396E+00 3.756E-01 1 .771E+00 4.591E+00 1 .117E-01 2.229E+00 -0.043 0.059 0.046 8.0000 1.41 lE+00 4.378E-0I 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-01 2.001E+00 6.183E+00 1 .526E-01 2.664E+00 -0.038 0.052 0.039

12.5000 1 .462E+00 7.282E-01 2.1 90E+00 7.376E+00 1 .837E-01 2. 951E+00 -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 .513E+00 1 .236E+00 2.749E+00 1 .043E+01 2.628E-01 3.597E+00 -0.028 0.039 0.026

25.0000 1 .537E+00 1 .583E+00 3. 120E+00 1 .21 3E+01 3.061E-01 3.927E+00 -0.024 0.036 0.022

30.0000 1 .555E+00 1 . 936E+00 3.491E+00 1 . 365E+01 3.437E-01 4.209E+00 -0.021 0.033 0.019

35.0000 1 .570E+00 2.291E+00 3.861E+00 1 .501E+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+01 4.059E-01 4.676E+00 -0.016 0.029 0.015

45.0000 1 .593E+00 3.012E+00 4.605E+00 1 .738E+01 4.320E-01 4.874E+00 -0.015 0.027 0.013

50.0000 1 .603E+00 3.375E+00 4.978E+00 1 .842E+01 4.554E-01 5.054E+00 -0.013 0.026 0.012

55.0000 1 .61 1E+00 3.740E+00 5.351E+00 1 .939E+01 4.766E-01 5.21 9E+00 -0.012 0.025 0.01 1 60.0000 1 .61 9E+00 4.107E+00 5.725E+00 2.029E+01 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+00 -0.009 0.021 0.008

90.0000 1 .653E+00 6 . 330E+00 7.983E+00 2.471E+01 5.836E-01 6.100E+00 -0.008 0.020 0.007

1 00 .0000 1.661 E+00 7.079E+00 8.740E+00 2.591E+01 6.054E-01 6 .292E+00 -0.008 0.019 0.006 125.0000 1 . 679E+00 8 . 958E+00 1 .064E+01 2.850E+01 6 .498E-01 6 .705E+00 -0.006 0.018 0.005

1 50 .0000 1 . 694E+00 1 . 085E+01 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+01 1 .445E+01 3.251 E+01 7.11 OE-01 7.336E+00 -0.005 0.016 0.003

200 .0000 1 .71 6E+00 1 .465E+01 1 .637E+01 3.414E+01 7.332E-01 7.590E+00 -0.004 0.015 0 .003

250 .0000 1 . 733E+00 1 .847E+01 2.020E+01 3.688E+01 7.676E-01 8.017E+00 -0.003 0.014 0.002

300.0000 1 . 747E+00 2.230E+01 2.404E+01 3.915E+01 7.932E-01 8.370E+00 -0.003 0.013 0.002

350.0000 1 .758E+00 2.61 3E+01 2.789E+01 4. 108E+01 8. 1 31 E-01 8.670E+00 -0.002 0.012 0.002

400.0000 1 . 768E+00 2. 998E+01 3. 174E+01 4.276E+01 8.291E-01 8 . 931 E+00 -0.002 0.012 0.002

450 .0000 1 .776E+00 3 . 382E+01 3.560E+01 4.424E+01 8.422E-01 9.162E+00 -0.002 0.012 0.001

500 .0000 1 . 784E+00 3 . 767E+01 3.946E+01 4 . 558E+01 8.532E-01 9 . 369E+00 -0.001 0.011 0.001 550.0000 1 .791E+00 4. 153E+01 4.332E+01 4.679E+01 8.626E-01 9.558E+00 -0.001 0.011 0.001 600.0000 1 .797E+00 4.539E+01 4.718E+01 4.789E+01 8.708E-01 9.730E+00 -0.001 0.011 0.001 700.0000 1 .808E+00 5.31 1E+01 5.491E+01 4.985E+01 8.842E-01 1 .004E+01 -0.001 0.010 0.001 800.0000 1 .818E+00 6 . 083E+01 6 .265E + 01 5. 156E+01 8.948E-01 1 .030E+01 -0.001 0.010 0.001 900.0000 1 .826E+00 6 .856E+01 7.039E+01 5.306E+01 9.034E-01 1 .053E+01 -0.001 0.010 0.001 1000.0000 1 .833E+00 7 .629E+01 7.81 3E+01 5.441E+01 9. 106E-01 1 .074E+01 -0.000 0.009 0.001

94
ELECTROMS IN GERMANIUM

I = 350.0 eV DENSITY = 5.323E+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^/g MeV cm^/g MeV cm^/g g/cm 2 0.0100 1 .293E+01 1 .267E-02 1 .299E+01 9.908E-09 5.171E-09 5. 175E-09 -0.286 0.367 0.397

0.0125 1 .065E+01 1 . 339E-02 1 .066E+01 7 .087E-09 6 .91 3E-09 6 .632E-09 -0.269 0.390 0.322

0.0150 9.367E+00 1 . 395E-02 9.381E+00 9.593E-09 7.631E-09 8. 152E-09 -0.257 0.319 0.309

0.0175 8.900E+00 1 .939E-02 8.91 9E+00 1 .291E-03 8.825E-09 9.739E-09 -0.297 0.309 0.291

0 .0200 7 .691 E+00 1 .975E-02 7.655E+00 1 .553E-03 9. 996E-09 1 . 1 38E-03 -0.290 0.292 0.280

0.0250 6.521E+00 1 .532E-02 6 .536E+00 2.263E-03 1 .227E-03 1 .989E-03 -0.228 0.273 0.263

0.0300 5.731 E+00 1 . 575E-02 5.797E+00 3.081E-03 1 .997E-03 1 .853E-03 -0.219 0.260 0.251 0.0350 5. 192E+00 1 .609E-02 5. 158E+00 9.001E-03 1 .659E-03 2.299E-03 -0.212 0.299 0.292

0 .OAOO 9 . 685E+00 1 .638E-02 9.701 E+00 5.018E-03 1 .869E-03 2.656E-03 -0.206 0.291 0.235

0 . 0A50 9.318E+00 1 . 663E-02 9.335E+00 6.127E-03 2.069E-03 3.089E-03 -0.201 0.239 0.228

0 . 0500 9.018E+00 1 .689E-02 9.035E+00 7.323E-03 2.258E-03 3.591E-03 -0.197 0.228 0.223

0.0550 3.768E+00 1 .709E-02 3.785E+00 8.609E-03 2.997E-03 9.013E-03 -0.199 0.223 0.218

0.0600 3.555E+00 1 .722E-02 3.572E+00 9. 969E-03 2.632E-03 9.502E-03 -0.191 0.219 0.219

0.0700 3.21 3E+00 1 .755E-02 3.231E+00 1 .291E-02 2. 989E-03 5.535E-03 -0.185 0.212 0.208

0 .0800 2.950E+00 1 .789E-02 2.968E+00 1 .615E-02 3.330E-03 6.639E-03 -0.181 0.206 0.202

0.0900 2.792E+00 1 .81 IE-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 2.591E+00 2.339E-02 3.976E-03 9.019E-03 -0.179 0.197 0.199

0.1250 2.262E+00 1 . 900E-02 2.281E+00 3.371E-02 9.725E-03 1 .230E-02 -0.168 0.188 0.186

0 . 1 500 2.050E+00 1 . 960E-02 2.070E+00 9.525E-02 5.922E-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 2.081E-02 1 .809E+00 7.127E-02 6.697E-03 2.381E-02 -0.155 0.173 0.171 0.2500 1 .629E+00 2.208E-02 1 .696E+00 1 .009E-01 7.859E-03 3.258E-02 -0.199 0.166 0.169

0 . 3000 1 .520E+00 2. 399E-02 1 .593E+00 1 .318E-01 8. 930E-03 9.209E-02 -0.199 0.161 0.159

0 . 3500 1 .997E+00 2.988E-02 1 .972E+00 1 .650E-01 9.997E-03 5.225E-02 -0.139 0.156 0.159

0 .9000 1 . 395E+00 2.691E-02 1 .922E+00 1 .996E-01 1 .092E-02 6.300E-02 -0.135 0.153 0.150

0 . 9500 1 . 357E+00 2.802E-02 1 .385E+00 2.353E-01 1 . 186E-02 7.932E-02 -0.132 0.199 0.197

0.5000 1 . 328E+00 2.971E-02 1 .357E+00 2.718E-01 1 .278E-02 8.619E-02 -0.128 0.196 0.199

0 . 5500 1 .305E+00 3. 196E-02 1 .337E+00 3.089E-01 1 .369E-02 9.857E-02 -0.125 0.199 0.191 0.6000 1 .288E+00 3.326E-02 1 .321E+00 3.965E-01 1 .958E-02 1 . 1 19E-01 -0.122 0.191 0.138

0.7000 1 .263E+00 3.702E-02 1 .300E+00 9.229E-01 1 .633E-02 1 .386E-01 -0.116 0.137 0.133

0.8000 1 .298E+00 9.095E-02 1 .289E+00 5.001E-01 1 .805E-02 1 .673E-01 -0.111 0.133 0.128

0 . 9000 1 .239E+00 9.509E-02 1 .289E+00 5.779E-01 1 .976E-02 1 .973E-01 -0.106 0.129 0.129

1 .0000 1 .239E+00 9.926E-02 1 .283E+00 6 .558E-01 2. 195E-02 2.282E-01 -0.102 0.125 0.120

1 . 2500 1 .231E+00 6 .036E-02 1 .291E+00 8.501E-01 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 .093E+00 2.989E-02 3.899E-01 -0.085 0.112 0.103

1 .7500 1 .292E+00 8.992E-02 1 .326E+00 1 .233E+00 3.91 IE-02 9.695E-01 -0.080 0.106 0.097

2.0000 1 .250E+00 9.719E-02 1 .397E+00 1 .920E+00 3.833E-02 5.979E-01 -0.075 0.102 0.091 2.5000 1 .268E+00 1 .236E-01 1 .391E+00 1 .785E+00 9.676E-02 6.953E-01 -0.068 0.099 0.082

3.0000 1 .289E+00 1 .512E-01 1 .936E+00 2.139E+00 5.516E-02 8.323E-01 -0.063 0.089 0.075

3.5000 1 . 300E+00 1 .797E-01 1 .980E+00 2.982E+00 6.398E-02 9.593E-01 -0.058 0.089 0.070

9.0000 1 . 319E+00 2.089E-01 1 .523E+00 2.815E+00 7.171E-02 1 .077E+00 -0.055 0.080 0.065

9 . 5000 1 . 327E+00 2. 387E-01 1 .566E+00 3.138E+00 7.989E-02 1 .188E+00 -0.052 0.076 0.061 5.0000 1 . 338E+00 2.691E-01 1 -608E+00 3.959E+00 8.786E-02 1 .292E+00 -0.099 0.073 0.058

5.5000 1 . 399E+00 2. 999E-01 1 .699E+00 3.761E+00 9.575E-02 1 .389E+00 -0.097 0.070 0.055

6.0000 1 . 359E+00 3.312E-01 1 .690E+00 9.060E+00 1 .035E-01 1 .981E+00 -0.095 0.068 0.052

7.0000 1 .376E+00 3. 999E-01 1 .771E+00 9.638E+00 1 . 187E-01 1 .651E+00 -0.092 0.069 0.098

8 .0000 1 . 391 E+00 9.598E-01 1 .851E+00 5.1 90E+00 1 .333E-01 1 .805E+00 -0.090 O.OSO 0.099

9.0000 1 .909E+00 5.257E-01 1 .930E+00 5.71 9E+00 1 .979E-01 1 .995E+00 -0.038 0.057 0.091 10.0000 1 .916E+00 5. 926E-01 2.009E+00 6.227E+00 1 .611E-01 2.079E+00 -0.036 0.055 0.039

12.5000 1 .991E+00 7.631 E-01 2.209E+00 7.915E+00 1 .931E-01 2.357E+00 -0.033 0.050 0.039

15.0000 1 .961E+00 9.373E-01 2.398E+00 8.502E+00 2.229E-01 2.597E+00 -0.031 0.096 0.030

17.5000 1 .977E+00 1 . 1 19E+00 2.592E+00 9.509E+00 2.993E-01 2.806E+00 -0.029 0.093 0.027

20.0000 1 .992E+00 1 .299E+00 2.786E+00 1 .093E+01 2.791E-01 2.991E+00 -0.028 0.091 0.025

25.0000 1 .515E+00 1 .659E+00 3.173E+00 1 .212E+01 3. 182E-01 3.311E+00 -0.025 0.037 0.021 30.0000 1 .533E+00 2.029E+00 3.562E+00 1 .360E+01 3.569E-01 3.583E+00 -0.022 0.039 0.018

35.0000 1 .598E+00 2.903E+00 3.952E+00 1 .993E+01 3.897E-01 3.820E+00 -0.020 0.032 0.016

90.0000 1 .561E+00 2.781E+00 9.392E+00 1 .619E+01 9.191E-01 9.031E+00 -0.018 0.030 0.015

95.0000 1 .572E+00 3. 162E+00 9.739E+00 1 .729E+01 9.952E-01 9.222E+00 -0.016 0.028 0.013

50.0000 1 .581E+00 3.595E+00 5.127E+00 1 .826E+01 9.687E-01 9.396E+00 -0.015 0.027 0.012

55.0000 1 .590E+00 3.930E+00 5.520E+00 1 .920E+01 9.899E-01 9.556E+00 -0.019 0.026 0.011 60.0000 1 .598E+00 9.316E+00 5.919E+00 2.007E+01 5.092E-01 9.709E+00 -0.013 0.025 0.010

70.0000 1.61 1E+00 5.093E+00 6.709E+00 2. 166E+01 5.929E-01 9.971E+00 -0.011 0.023 0.009

80.0000 1 .622E+00 5.879E+00 7.995E+00 2.307E+01 5.716E-01 5.206E+00 -0.010 0,022 0.008

90.0000 1 .631E+00 6.658E+00 8.289E+00 2.939E+01 5.963E-01 5.917E+00 -0.009 0.021 0.007

100.0000 1 .690E+00 7 . 995E+00 9.085E+00 2.599E+01 6.178E-01 5.607E+00 -0.008 0.020 0.006

125.0000 1 .658E+00 9.920E+00 1 .108E+01 2.798E+01 6.619E-01 6 .01 5E+00 -0.007 0.019 0.005

1 50 .0000 1 .672E+00 1 . 191E+01 1 .308E+01 3.005E+01 6 . 998E-01 6 .352E+00 -0.006 0.017 0.009

175.0000 1 .689E+00 1 .390E+01 1 .508E+01 3. 183E+01 7.219E-01 6.690E+00 -0.005 0.016 0.009

200 .0000 1 .699E+00 1 .590E+01 1 .709E+01 3.339E+01 7.930E-01 6.891E+00 -0.005 0.016 0.003

250 .0000 1 .710E+00 1 . 990E+01 2.111 E+0

3.601E+01 7.765E-01 7.315E+00 -0.009 0.015 0.002

300.0000 1 . 729E+00 2.392E+01 2.519E+01 3.818E+01 8.019E-01 7.669E+00 -0.003 0.019 0.002

350.0000 1 .735E+00 2.799E+01 2. 918E+01 9.003E+01 8.206E-01 7.961E+00 -0.003 0.013 0.002

900 .0000 1 .799E+00 3. 198E+01 3.322E+01 9. 163E+01 8.361E-01 8.220E+00 -0.002 0.013 0.002

950.0000 1 .753E+00 3.552E+01 3.727E+01 9.305E+01 8.988E-01 8.999E+00 -0.002 0.012 0.001

500 .0000 1 .760E+00 3. 956E+01 9.132E+01 9.933E+01 8.599E-01 8.655E+00 -0.002 0.012 0.001 550.0000 1 . 767E+00 9 . 360E+01 9.537E+01 9.598E+01 8.685E-01 8.892E+00 -0.001 0.012 0.001

600 .0000 1 . 773E+00 9.765E+01 9.993E+01 9.659E+01 8.763E-01 9.019E+00 -0.001 0.011 0.001 700.0000 1 . 789E+00 5.576E+01 5.759E+01 9.891E+01 8.893E-01 9.318E+00 -0.001 0.011 0.001

800 .0000 1 . 793E+00 6 . 387E+01 6.566E+01 5.003E+01 8. 995E-01 9.582E+00 -0.001 0.011 0.001 900.0000 1 .801E+00 7. 1 99E+01 7.379E+01 5.197E+01 9.078E-01 9.815E+00 -0.001 0.010 0.001 1000.0000 1 .808E+00 8.01 1E+01 8.1 92E+01 5.276E+01 9. 197E-01 1 .002E+01 -0.001 0.010 0.001

‘J5
ELECTRONS IN KRYPTON

I = 352.0 eV DENSITY = 3.^i78E-03 g/cm^ (20° C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( logI )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .210E+01 1 . 399E-02 1 .21 1 E+01 5.096E-09 5.575E-09 0.0 -0.287 0.368 0.397

0.0125 1 .036E+01 1 .927E-02 1 .038E + 01 7.285E-09 6.996E-09 0.0 -0.270 0.390 0.322

0.0150 9.1 1 6E+00 1 .991E-02 9. 1 31 E+00 9.860E-09 8.296E-09 0.0 -0.257 0.320 0.309

0.0175 8. 175E+00 1 .593E-02 8.1 91E+00 1 .276E-03 9.629E-09 0.0 -0.298 0.305 0.291 0.0200 7.937E+00 1 .586E-02 7.952E+00 1 .596E-03 1 .093E-03 0.0 -0.290 0.292 0.280

0.0250 6 . 397E+00 1 .659E-02 6.369E+00 2.325E-03 1 . 398E-03 0.0 -0.228 0.279 0.263

0.0300 5.579E+00 1 .707E-02 5.596E+00 3. 165E-03 1 .599E-03 0.0 -0.219 0.260 0.251 0.0350 5.006E+00 1 .750E-02 5.029E+00 9. 1 10E-03 1 .833E-03 0.0 -0.212 0.250 0.292

0 ,0‘tOO 9.561E+00 1 .785E-02 9.579E+00 5. 159E-03 2.065E-03 0.0 -0.207 0.292 0.235

0 . 0<150 9.205E+00 1 .81 6E-02 9.223E+00 6.292E-03 2.292E-03 0.0 -0.202 0.235 0.228

0.0500 3.913E+00 1 .899E-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 . 1 95 0.229 0.219

0.0600 3 . 962E+00 1 .891 E-02 3.981E+00 1 .023E-02 2. 938E-03 0.0 -0.191 0.219 0.215

0.0700 3 . 1 29E + 00 1 . 932E-02 3.199E+00 1 .326E-02 3. 395E-03 0.0 -0.186 0.212 0.208

0 .0800 2.879E+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 9.113E-03 0.0 -0.178 0.201 0.198

0.1000 2.506E+00 2 . 035E-02 2.527E+00 2.900E-02 9.976E-03 0.0 -0.175 0.197 0.199

0.1250 2 . 209E+00 2.111 E-02 2.225E+00 3.959E-02 5.337E-03 0.0 -0.169 0.189 0.186

0.1500 1 . 999E1-00 2. 182E-02 2.021E+00 9 . 690E-02 6 . 1 39E-03 0.0 -0.169 0.183 0.180 0.1750 1 .851E + 00 2.252E-02 1 .873E+00 5.928E-02 6 .893E-03 0.0 -0.160 0.178 0.176

0.2000 1 . 790E + 00 2 . 322E-02 1 .763E+00 7 . 305E-02 7.606E-03 0.0 -0.157 0.179 0.172

0 .2500 1 . 585E + 00 2.965E-02 1 .610E+00 1 .028E-01 8.936E-03 0.0 -0.152 0.168 0.165

0.3000 1 . 989E+00 2 . 6 1 7E-02 1 .510E+00 1 .350E-01 1 .017E-02 0.0 -0.197 0.163 0.160

0 . 3500 1.91 5E+00 2.777E-02 1 .992E+00 1 .689E-01 1 . 133E-02 0.0 -0.199 0.159 0.156

0 . ^tOOO 1 . 365E+00 2.997E-02 1 .399E+00 2.092E-01 1 .299E-02 0.0 -0.191 0.155 0.153

0 . ^>500 1 . 328E+00 3. 125E-02 1 .359E+00 2.905E-01 1 .351E-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 .955E-02 0.0 -0.136 0.150 0.197

0.5500 1 .279E+00 3.509E-02 1 .319E+00 3.159E-01 1 .557E-02 0.0 -0.139 0.198 0.195

0.6000 1 . 263E + 00 3.703E-02 1 .300E+00 3.537E-01 1 .657E-02 0.0 -0.133 0.196 0.193

0.7000 1 .291E+00 9 . 1 1 6E-02 1 .283E+00 9.312E-01 1 .853E-02 0.0 -0.129 0.193 0.139

0 .8000 1 .229E + 00 9.597E-02 1 .279E+00 5.099E-01 2.095E-02 0.0 -0.127 0.190 0.136

0 . 9000 1 . 222E+00 9 . 996E-02 1 .272E+00 5.880E-01 2.239E-02 0.0 -0.129 0.137 0.133

1 . 0000 1.21 9E+00 5.959E-02 1 .273E+00 6 .666E-01 2.921E-02 0.0 -0.122 0.135 0.131

1 .2500 1 .221E+00 6 .673E-02 1 .288E+00 8.620E-01 2.889E-02 0.0 -0.118 0.130 0.125

1 . 5000 1 . 230E + 00 7 . 957E-02 1 .310E+00 1 .055E+00 3.392E-02 0.0 -0.115 0.127 0.121

1 .7500 1 .292E + 00 9.297E-02 1 .335E+00 1 .299E+00 3.796E-02 0.0 -0.112 0.123 0.117

2.0000 1 .255E + 00 1 .068E-01 1 .362E+00 1 .929E+00 9.297E-02 0.0 -0.110 0.121 0.119

2.5000 1 .282E + 00 1 .356E-01 1 .917E+00 1 .789E+00 5.1 39E-02 0.0 -0.106 0.116 0.109

3 .0000 1 . 307E + 00 1 .656E-01 1 .973E+00 2.135E+00 6.018E-02 0.0 -0.103 0.113 0.109

3.5000 1 . 330E+00 1 .965E-01 1 .527E+00 2.968E+00 6.882E-02 0.0 -0.101 0.110 0.101

^t.OOOO 1 .352E+00 2.282E-01 1 .580E+00 2.790E+00 7.729E-02 0.0 -0.099 0.107 0.0 98 9.5000 1 .371E + 00 2.605E-01 1 .632E+00 3. 102E+00 8.560E-02 0.0 -0.097 0.109 0.095

5.0000 1 . 389E + 00 2.933E-01 1 .683E+00 3.903E+00 9.379E-02 0.0 -0.096 0.102 0.092

5.5000 1 .906E + 00 3.267E-01 1 .733E+00 3.696E+00 1 .017E-01 0.0 -0.095 0.100 0.090

6.0000 1 .922E+00 3.605E-01 1 .782E+00 3. 981E+00 1 .095E-01 0.0 -0.093 0.099 0.088

7.0000 1 .950E + 00 9.293E-01 1 .879E+00 9.527E+00 1 .297E-01 0.0 -0.092 0.095 0.089

8.0000 1 .979E+00 9 . 995E-01 1 . 979E+00 5.096E+00 1 .392E-01 0.0 -0.090 0.093 0.081 9.0000 1 .997E+00 5.708E-01 2.067E+00 5.591E+00 1 .531E-01 0.0 -0.089 0.090 0.078

10.0000 1 .516E + 00 6.930E-01 2.159E+00 6.019E+00 1 .665E-01 0.0 -0.087 0.088 0.075

12.5000 1 .559E + 00 8.269E-01 2.386E+00 7.115E+00 1 .978E-01 0.0 -0.085 0.089 0.070

15.0000 1 .599E + 00 1 .015E + 00 2.609E+00 8. 1 16E+00 2.262E-01 0.0 -0.083 0.080 0.065

17.5000 1 . 629E + 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-01 0.0 -0.080 0.079 0.058

25.0000 1 .699E + 00 1 .792E+00 3.986E+00 1 . 192E+01 3. 183E-01 0.0 -0.078 0.069 0.053

30.0000 1 . 729E+00 2. 1 91E+00 3. 921 E+00 1 .277E+01 3.598E-01 7.931E-03 -0.072 0.066 0.098

35.0000 1 .758E + 00 2.595E+00 9.353E+00 1 .398E+01 3.867E-01 3.031E-02 -0.068 0.063 0.099

90 .0000 1 .782E + 00 3.002E+00 9.785E+00 1 .508E+01 9. 199E-01 6.097E-02 -0.069 0.060 0.091 95.0000 1 .803E + 00 3.91 3E+00 5.216E+00 1 .608E+01 9.900E-01 9.396E-02 -0.062 0.058 0.038

50 .0000 1 .822E + 00 3.825E+00 5.697E+00 1 .700E+01 9.626E-01 1 .289E-01 -0.060 0.056 0.035

55.0000 1 .838E+00 9.290E+00 6.078E+00 1 .785E+01 9.831E-01 1 .693E-01 -0.058 0.059 0.033

60.0000 1 .853E + 00 9.656E+00 6.509E+00 1 .865E+01 5.017E-01 1 .998E-01 -0.056 0.052 0.031 70.0000 1 .879E + 00 5 . 993E+00 7.372E+00 2.009E+01 5. 399E-01 2.700E-01 -0.053 0.050 0.028

80.0000 1 .901E + 00 6 . 339E+00 8.235E+00 2.1 37E+01 5.623E-01 3.388E-01 -0.050 0.097 0.025

90.0000 1 . 920E+00 7 . 1 79E+00 9.098E+00 2.253E+01 5.869E-01 9.061E-01 -0.098 0.096 0.023

1 00 .0000 1 . 936E+00 8 . 027E+00 9. 963E+00 2.358E+01 6.076E-01 9.721E-01 -0.096 0.099 0.021 125.0000 1 . 970E+00 1 .015E+01 1 .212E+01 2.585E+01 6.506E-01 6.316E-01 -0.091 0.091 0.018

1 50 .0000 1 . 996E+00 1 .229E+01 1 .929E+01 2.779E+01 6 .837E-01 7.830E-01 -0.037 0.038 0.016

175.0000 2.017E+00 1 .999E+01 1 .696E+01 2. 937E+01 7.102E-01 9.258E-01 -0.039 0.036 0.019

200.0000 2 . 039E+00 1 .659E+01 1 .863E+01 3.080E+01 7.320E-01 1 .060E+00 -0.031 0.035 0.012

250 .0000 2.062E+00 2.091E+01 2.297E+01 3.321E+01 7.658E-01 1 .309E+00 -0.027 0.033 0.010

300.0000 2.089E+00 2.529E+01 2.732E+01 3.521E+01 7.911E-01 1 .521E+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 .719E+00 -0.023 0.030 0.007

900.0000 2. 1 17E+00 3. 392E+01 3.609E+01 3.838E+01 8.266E-01 1 .887E+00 -0.021 0.029 0.007

950 .0000 2. 1 30E+00 3.827E+01 9.090E+01 3. 969E+01 8.397E-01 2.095E+00 -0.020 0.028 0.006

500.0000 2.191E+00 9.262E+01 9.976E+01 9 . 087E+01 8.507E-01 2. 189E+00 -0.019 0 . 027 0.005

550.0000 2.151E+00 9.698E+01 9.913E+01 9 . 1 93E+01 8.601E-01 2.322E+00 -0.018 0.026 0.005

600.0000 2. 160E+00 5. 1 39E+01 5.350E+01 9.291E+01 8.683E-01 2. 995E+00 -0.018 0.026 0.005

700.0000 2. 1 76E+00 6.007E+01 6 .225E+01 9.969E+01 8.817E-01 2.667E+00 -0.016 0.025 0.009

800.0000 2. 1 90E-t00 6 .881 E+01 7.1 OOE+01 9.619E+01 8. 929E-01 2.869E+00 -0.015 0.029 0.003

900.0000 2.201E+00 7.755E+01 7 . 975E+01 9.797E+01 9.01 IE-01 3.092E+00 -0.015 0.023 0.003

1000.0000 2.21 lE+00 8.630E+01 8 .851 E+01 9.866E+01 9.089E-01 3.203E+00 -0.019 0.023 0.003

90
ELECTRONS IN MOLYBDENUM

I = 929.0 eV DENSITY = 1 .022E+01 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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 . 1 67E+0

1 .529E-02 1 .168E + 01 5.319E-09 6 .528E-09 7 . 953E-09 -0.303 0.902 0.373

0.0125 1 .003E+01 1 .627E-02 1 .009E+01 7.636E-09 8. 198E-09 1 .029E-03 -0.289 0.369 0.399

0.0150 8.893E+00 1 .709E-02 8.860E+00 1 .029E-03 9.799E-09 1 .275E-03 -0.270 0.395 0.323

0.0175 7 . 995E+00 1 .776E-02 7 . 963E+00 1 . 327E-03 1 . 1 33E-03 1 .535E-03 -0.260 0 . 327 0.308

0 .0200 7.238E+00 1 .832E-02 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 6.211 E+00 2.909E-03 1 .593E-03 2.389E-03 -0.238 0.291 0.277

0.0300 5.952E+00 1 . 992E-02 5.972E+00 3.269E-03 1 .889E-03 3.017E-03 -0.228 0.275 0.269

0 .0350 9.898E+00 2.050E-02 9.918E+00 9.230E-03 2.177E-03 3.692E-03 -0.221 0.263 0.253

0 . O^iOO 9 . 967E+00 2.099E-02 9.988E+00 5.296E-03 2.958E-03 9.910E-03 -0.219 0.259 0.295

0 .0<*50 9 . 1 22E+00 2. 192E-02 9. 193E+00 6 .957E-03 2.732E-03 5. 169E-03 -0.209 0.296 0.238

0.0500 3.838E+00 2. 181E-02 3.860E+00 7.708E-03 3.000E-03 5.969E-03 -0.205 0.290 0.232

0 .0550 3.601E+00 2.216E-02 3.623E+00 9.096E-03 3.262E-03 6 .807E-03 -0.201 0.239 0.227

0.0600 3.900E+00 2.297E-02 3.922E+00 1 .097E-02 3.519E-03 7.681E-03 -0.198 0.229 0.223

0 . 0700 3. 076E+00 2.305E-02 3.099E+00 1 . 359E-02 9.017E-03 9.535E-03 -0.192 0.221 0.216

0 .0800 2.826E+00 2.357E-02 2.850E+00 1 .691E-02 9.997E-03 1 .152E-02 -0.187 0.219 0.210

0.0900 2.628E+00 2.909E-02 2.652E+00 2.055E-02 9.961E-03 1 .362E-02 -0.183 0.209 0.209

0.1000 2.967E+00 2.999E-02 2.992E+00 2.995E-02 5.909E-03 1 .589E-02 -0.180 0.209 0.200

0 . 1 250 2.171 E+00 2.551E-02 2.1 97E+00 3.517E-02 6 .979E-03 2. 180E-02 -0.173 0.195 0.192

0.1500 1 . 970E+00 2.696E-02 1 .996E+00 9.719E-02 7.969E-03 2.830E-02 -0.167 0.188 0.185

0 . 1750 1 .825E+00 2.737E-02 1 .852E+00 6.016E-02 8.906E-03 3.523E-02 -0.163 0.183 0.180

0 . 2000 1 .715E+00 2.826E-02 1 .793E+00 7.909E-02 9.292E-03 9.252E-02 -0.159 0.178 0.175

0.2500 1 . 563E+00 3.005E-02 1 .593E+00 1 .092E-01 1 .095E-02 5.795E-02 -0.153 0.171 0.168

0.3000 1 .963E+00 3. 1 92E-02 1 .995E+00 1 .367E-01 1 .298E-02 7.922E-02 -0.197 0.165 0.162

0 . 3500 1 . 399E+00 3. 388E-02 1 .927E+00 1 .709E-01 1 .391E-02 9.109E-02 -0.193 0.160 0.157

0.9000 1 . 399E+00 3.593E-02 1 .380E+00 2.066E-01 1 .529E-02 1 .089E-01 -0.139 0.156 0.153

0.9500 1 . 307E+00 3.808E-02 1 .395E+00 2.933E-01 1 .661E-02 1 .259E-01 -0.135 0.153 0.150

0 . 5000 1 .279E+00 9.032E-02 1 .31 9E+00 2.809E-01 1 .789E-02 1 .937E-01 -0.132 0.150 0.196

0 .5500 1 .257E+00 9 .269E-02 1 .300E+00 3.191E-01 1 .915E-02 1 .615E-01 -0.129 0.197 0.193

0.6000 1 .290E+00 9.502E-02 1 .285E+00 3.578E-01 2.038E-02 1 .799E-01 -0.126 0.199 0.191 0.7000 1 .21 7E+00 9.996E-02 1 .267E+00 9.362E-01 2.279E-02 2.151E-01 -0.122 0.190 0.136

0.8000 1 .203E+00 5.510E-02 1 .258E+00 5.155E-01 2.519E-02 2.505E-01 -0.117 0.136 0.131

0 . 9000 1 . 1 99E+00 6.093E-02 1 .255E+00 5.951E-01 2.796E-02 2.859E-01 -0.113 0.133 0.127

1 .0000 1 . 1 90E+00 6 .592E-02 1 .255E+00 6.798E-01 2.979E-02 3.198E-01 -0.110 0.129 0.129

1 .2500 1 . 187E+00 8.032E-02 1 .268E+00 8.731E-01 3.538E-02 9.028E-01 -0.103 0.123 0.116

1 .5000 1 . 1 92E+00 9.550E-02 1 .288E+00 1 .069E+00 9.095E-02 9.816E-01 -0.097 0.117 0.110

1 .7500 1 .200E+00 1.11 3E-01 1 .31 1E+00 1 .261E+00 9.696E-02 5.563E-01 -0.093 0.113 0.109

2.0000 1 .209E+00 1 .276E-01 1 .337E+00 1 .950E+00 5.193E-02 6.275E-01 -0.088 0.109 0.099

2.5000 1 .228E+00 1 .615E-01 1 .389E+00 1 .817E+00 6.272E-02 7.606E-01 -0.081 0.102 0.091 3.0000 1 .296E + 00 1 .967E-01 1 .992E+00 2.170E+00 7.333E-02 8.838E-01 -0.075 0.097 0.085

3.5000 1 .262E+00 2.329E-01 1 .995E+00 2.51 lE+00 8.373E-02 9. 999E-01 -0.070 0.092 0.079

9 .0000 1 .277E+00 2.699E-01 1 .597E+00 2.890E+00 9.392E-02 1 .109E+00 -0.065 0.088 0.079

9 . 5000 1 . 290E+00 3.077E-01 1 .598E+00 3. 158E+00 1 .039E-01 1 .212E+00 -0.061 0.089 0.070

5.0000 1 . 302E+00 3.961 E-01 1 .698E+00 3.966E+00 1 .136E-01 1 .311E+00 -0.057 0.081 0.066

5.5000 1 . 31 3E+00 3.851E-01 1 .698E+00 3.765E+00 1 .232E-01 1 .906E+00 -0.059 0.078 0.062

6.0000 1 . 322E+00 9.296E-01 1 .797E+00 9.055E+00 1 .325E-01 1 .996E+00 -0.051 0.075 0.059

7 .0000 1 . 390E+00 5.099E-01 1 .895E+00 9.612E+00 1 .505E-01 1 .666E+00 -0.096 0.070 0.053

8.0000 1 . 355E+00 5.867E-01 1 .991E+00 5. 190E+00 1 .677E-01 1 .822E+00 -0.092 0.066 0.099

9.0000 1 . 367E+00 6.697E-01 2.037E+00 5.693E+00 1 -891E-01 1 .966E+00 -0.039 0.063 0.095

1 0 .0000 1 .379E+00 7.538E-01 2.1 33E+00 6.123E+00 1 .999E-01 2.100E+00 -0.037 0.060 0.091 12.5000 1 .902E+00 9.680E-01 2.370E+00 7.239E+00 2.362E-01 2.398E+00 -0.032 0.059 0.035

15.0000 1 .921E+00 1 . 187E+00 2.608E+00 8.239E+00 2.689E-01 2.653E+00 -0.029 0.050 0.030

17.5000 1 .937E+00 1 .909E+00 2.895E+00 9. 157E+00 2.989E-01 2.877E+00 -0.027 0.096 0.027

20.0000 1 .950E+00 1 .639E+00 3.089E+00 1 .OOOE+01 3.252E-01 3.075E+00 -0.025 0.093 0.029

25.0000 1 .971E+00 2.091E+00 3.562E+00 1 .151E+01 3.721E-01 3.918E+00 -0.022 0.039 0.020

30.0000 1 .988E+00 2.555E+00 9.093E+00 1 .282E+01 9. 1 18E-01 3.707E+00 -0.019 0.036 0.017

35.0000 1 .502E+00 3.029E+00 9.526E+00 1 .399E+01 9.959E-01 3. 959E+00 -0.017 0.033 0.015

90.0000 1 .519E + 00 3.997E+00 5.01 lE+00 1 .509E+01 9.756E-0I 9. 182E+00 -0.015 0.031 0.013

95.0000 1 .529E+00 3. 979E+00 5.998E+00 1 .599E+01 5.017E-01 9.382E+00 -0.019 0.030 0.012

50.0000 1 .533E+00 9.953E+00 5.987E+00 1 .687E+01 5.299E-01 9.569E+00 -0.013 0.028 0.011 55.0000 1 .591E+00 9. 935E+00 6.977E+00 1 .767E+01 5.957E-01 9.730E+00 -0.012 0.027 0.010

60.0000 1 .599E+00 5.91 9E+00 6.968E+00 1 .891E+01 5.699E-01 9.889E+00 -0.011 0.026 0.009

70.0000 1 .561E+00 6.392E+00 7.953E+00 1 . 976E+01 5.968E-01 5. 160E+00 -0.009 0.025 0.008

80.0000 1 .572E+00 7 . 370E+00 8. 992E+00 2.099E+01 6.290E-01 5.903E+00 -0.008 0.023 0.007

90.0000 1 .581E+00 8.352E+00 9.933E+00 2.200E+01 6.972E-01 5.61 9E+00 -0.007 0.022 0.006

100.0000 1 . 589E+00 9.339E+00 1 .093E+01 2.296E+01 6.673E-01 5.819E+00 -0.007 0.021 0.005

1 25.0000 1 . 606E+00 1 . 181 E+01 1 .392E+01 2.502E+01 7.075E-01 6.231E+00 -0.006 0.020 0.009

1 50 .0000 1 .61 9E+00 1 .930E+01 1 .592E+01 2.673E+01 7.379E-01 6.575E+00 -0.005 0.019 0.003

175.0000 1 .631E+00 1 .680E+01 1 .893E+01 2.81 9E+01 7.618E-01 6 .868E+00 -0.009 0.018 0.003

200.0000 1 .691E+00 1 .931E+01 2.095E+01 2. 996E+01 7.811E-01 7. 129E+00 -0.009 0.017 0.003

250.0000 1 .657E+00 2.933E+01 2.598E+01 3.160E+01 8.108E-01 7.553E+00 -0.003 0.016 0.002

300 .0000 1 .670E+00 2.936E+01 3.103E+01 3. 336E+01 8.326E-01 7.907E+00 -0.002 0.015 0.002

350.0000 1 .680E+00 3.991E+01 3.609E+01 3.985E+01 8.999E-01 8.208E+00 -0.002 0.019 0.001

900 .0000 1 .690E+00 3. 996E+01 9.11 5E+01 3.615E+01 8.627E-01 8.969E+00 -0.002 0.019 0.001

950 .0000 1 .698E+00 9.952E+01 9.622E+01 3.729E+01 8.737E-01 8.701E+00 -0.001 0.013 0.001

500 .0000 1 .705E+00 9 . 959E+01 5. 129E+01 3.832E+01 8.828E-01 8. 909E+00 -0.001 0.013 0.001 550.0000 1 .712E+00 5.966E+01 5.637E+01 3. 925E+01 8.906E-01 9.097E+00 -0.001 0.013 0.001 600.0000 1 .718E+00 5 . 973E+01 6. 195E+01 9.010E+01 8. 973E-01 9.269E+00 -0.001 0.012 0.001

700 .0000 1 .728E+00 6 . 988E+01 7.161E+01 9. 160E+01 9.082E-01 9.575E+00 -0.001 0.012 0.001 800.0000 1 . 737E + 00 8.009E+01 8. 178E+01 9.291E+01 9. 169E-01 9.890E+00 -0.001 0.012 0.001 900.0000 1 .795E + 00 9.022E+01 9.1 96E+01 9.906E+01 9.239E-01 1 .007E+01 -0.001 0.011 0.001 1000.0000 1 .753E+00 1 .009E+02 1 .021E+02 9.509E+01 9.297E-01 1 .028E+01 -0.000 0.011 0.001
ELECTRONS IN SILVER

I = 970.0 eV DENSITY = 1 .050E+01 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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 . 1 25E+0

1 . 639E-02 1 . 127E + 01 5 . 577E-09 7.226E-09 1 . 1 26E-03 -0.313 0.929 0.389

0.0125 9.687E+00 1 .759E-02 9.709E+00 7 . 976E-09 9.090E-09 1 .995E-03 -0.292 0.387 0.357

0.0150 8.556E+00 1 .899E-02 8.579E+00 1 .072E-03 1 .089E-03 1 .781 E-03 -0.278 0.361 0.335

0.0175 7.696E+00 1 . 927E-02 7.715E+00 1 . 380E-03 1 .261 E-03 2.1 35E-03 -0.267 0.391 0.318

0.0200 7.017E+00 1 . 992E-02 7.037E+00 1 .720E-03 1 .937E-03 2.508E-03 -0.258 0.325 0.305

0.0250 6 . 0 1 1 E+00 2.099E-02 6 .032E + 00 2.990E-03 1 .781 E-03 3. 31 2E-03 -0.299 0.302 0.285

0.0300 5.297E+00 2. 189E-02 5.31 9E+00 3.375E-03 2.11 7E-03 9.203E-03 -0.233 0.285 0.271 0.0350 9.763E+00 2 . 259E-02 9.786E+00 9.368E-03 2.999E-03 5.1 90E-03 -0.225 0.272 0.260

0 .0^(00 9.397E+00 2.319E-02 9.370E+00 5.963E-03 2.769E-03 6.289E-03 -0.219 0.262 0.251

0 .0<t50 9.01 2E+00 2 . 367E-02 9.036E+00 6.655E-03 3.077E-03 7.995E-03 -0.213 0.253 0.299

0.0500 3.738E+00 2.919E-02 3.762E+00 7.939E-03 3.383E-03 8.836E-03 -0.208 0.296 0.237

0 .0550 3 . 508E+00 2 . 958E-02 3.533E+00 9.312E-03 3.689E-03 1 .032E-02 -0.209 0.290 0.232

0.0600 3 . 31 3E+00 2.997E-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 3.029E+00 1 . 392E-02 9.552E-03 1 .573E-02 -0.193 0.225 0.219

0 . 0800 2.756E+00 2.639E-02 2.782E+00 1 .737E-02 5. 106E-03 2.022E-02 -0.186 0.218 0.212

0.0900 2.563E+00 2 . 693E-02 2.590E+00 2.1 10E-02 5.693E-03 2.593E-02 -0.181 0.211 0.206

0.1000 2.906E+00 2.798E-02 2.939E+00 2.509E-02 6.163E-03 3.125E-02 -0.176 0.206 0.201 0.1250 2. 1 17E+00 2.875E-02 2. 196E+00 3.607E-02 7.902E-03 9.759E-02 -0.166 0.199 0.190

0.1500 1 . 920E+00 2 . 990E-02 1 .950E+00 9.832E-02 8.569E-03 6 .953E-02 -0.159 0.186 0.181 0.1750 1 .778E+00 3.098E-02 1 .809E+00 6.165E-02 9.661 E-03 8.111E-02 -0.159 0.179 0.175

0.2000 1 .671E+00 3.203E-02 1 .703E+00 7.591E-02 1 .070E-02 9.702E-02 -0.199 0.173 0.169

0 . 2500 1 .522E+00 3.91 3E-02 1 .556E+00 1 .067E-01 1 .269E-02 1 .270E-01 -0.193 0.169 0.161 0.3000 1 . 929E+00 3.628E-02 1 .960E+00 1 .900E-01 1 .993E-02 1 .550E-01 -0.138 0.158 0.159

0 . 3500 1 . 356E+00 3.852E-02 1 .395E+00 1 .750E-01 1 .612E-02 1 .816E-01 -0.133 0.153 0.199

0 . 9000 1 . 308E+00 9 .085E-02 1 .398E+00 2.115E-01 1 .772E-02 2.070E-01 -0.130 0.198 0.195

0.9500 1 .271E+00 9.328E-02 1 .315E+00 2.991E-01 1 .927E-02 2.315E-01 -0.126 0.195 0.191 0.5000 1 .299E+00 9 . 580E-02 1 .290E+00 2.875E-01 2.076E-02 2.552E-01 -0.123 0.191 0.137

0 . 5500 1 .223E+00 9 .890E-02 1 .271 E+00 3.266E-01 2.222E-02 2.783E-01 -0.121 0.139 0.135

0 .6000 1 .207E+00 5. 107E-02 1 .258E + 00 3.661E-01 2.365E-02 3.007E-01 -0.119 0.136 0.132

0 .7000 1 . 189E+00 5.659E-02 1 .291E+00 9.962E-01 2.693E-02 3.938E-01 -0.119 0.132 0.127

0 .8000 1 . 170E+00 6 .233E-02 1 .233E+00 5.271E-01 2.919E-02 3.851E-01 -0.111 0.128 0.123

0.9000 1 . 162E+00 6 .827E-02 1 .230E+00 6 .089E-01 3.179E-02 9.296E-01 -0.108 0.125 0.119

1 .0000 1 . 1 58E+00 7 . 939E-02 1 .232E+00 6 .896E-01 3.991E-02 9.626E-01 -0.105 0.122 0.116

1 .2500 1 . 156E+00 9.038E-02 1 .296E+00 8.915E-01 9.082E-02 5.520E-01 -0.099 0.116 0.109

1 . 5000 1 . 161E+00 1 .072E-01 1 .268E+00 1 .090E+00 9.71 IE-02 6.396E-01 -0.099 0.111 0.103

1 .7500 1 . 169E+00 1 .297E-01 1 .299E+00 1 .286E+00 5.330E-02 7.116E-01 -0.090 0.107 0.099

2 .0000 1 . 178E+00 1 .928E-01 1 .321E+00 1 .977E+00 5.992E-02 7.836E-01 -0.086 0.103 0.099

2.5000 1 . 1 97E+00 1 -802E-01 1 .377E+00 1 .898E+00 7.199E-02 9. 157E-01 -0.081 0.097 0.087

3.0000 1 .21 5E+00 2.1 90E-01 1 .939E + 00 2.203E+00 8.317E-02 1 .035E+00 -0.076 0.092 0.082

3.5000 1 .232E+00 2.589E-01 1 .991E+00 2.595E+00 9.961E-02 1 . 193E+00 -0.072 0.088 0.077

9 .0000 1 .298E+00 2.997E-01 1 .597E+00 2.879E+00 1 .057E-01 1 .293E+00 -0.069 0.085 0.073

9 . 5000 1 .261E+00 3.912E-01 1 .603E + 00 3.1 92E+00 1 . 166E-01 1 .337E+00 -0.066 0.082 0.069

5.0000 1 .279E+00 3.839E-01 1 .658E + 00 3.999E+00 1 .271E-01 1 .925E+00 -0.063 0.079 0.066

5.5000 1 .286E+00 9.263E-01 1 .712E+00 3.795E+00 1 .379E-01 1 .508E+00 -0.060 0.076 0.063

6.0000 1 .296E+00 9.696E-01 1 .766E+00 9.083E+00 1 .979E-01 1 .587E+00 -0.058 0.079 0.060

7.0000 1 .315E+00 5.577E-01 1 .873E+00 9.633E+00 1 .667E-01 1 .735E + 00 -0.059 0.070 0.055

8.0000 1 . 331 E+00 6 .979E-01 1 .978E+00 5.152E+00 1 .899E-01 1 .873E+00 -0.050 0.067 0.051 9.0000 1 . 395E+00 7.389E-01 2.083E+00 5.695E+00 2.023E-01 2.001E+00 -0.096 0.063 0.097

1 0 .0000 1 . 357E+00 8. 305E-01 2. 188E + 00 6.11 3E+00 2. 188E-01 2. 121E+00 -0.093 0.061 0.099

1 2 . 5000 1 . 382E+00 1 .065E+00 2.997E+00 7.193E+00 2.567E-01 2.392E+00 -0.037 0.055 0.038

15.0000 1 . 902E+00 1 . 309E+00 2.707E+00 8. 169E+00 2. 909E-01 2.630E+00 -0.033 0.051 0.033

1 7 . 5000 1 .918E+00 1 .597E+00 2. 966E+00 9.096E+00 3.207E-01 2.891E+00 -0.030 0.097 0.029

20.0000 1 .932E+00 1 .799E+00 3.226E+00 9.859E+00 3.980E-01 3.030E+00 -0.028 0.095 0.026

25.0000 1 . 955E+00 2.293E+00 3.798E+00 1 .129E+01 3.959E-01 3.359E+00 -0.029 0.090 0.021 30.0000 1 .972E+00 2.800E+00 9.272E+00 1 .259E+01 9.353E-01 3.638E+00 -0.022 0.037 0.018

35.0000 1 .987E+00 3. 31 3E+00 9.800E+00 1 .369E+01 9.693E-01 3.880E+00 -0.020 0.035 0.016

90.0000 1 . 999E+00 3 .831 E+00 5.330E+00 1 .963E+01 9.988E-01 9.099E+00 -0.018 0.033 0.019

95.0000 1 .510E+00 9 . 352E+00 5.862E+00 1 .553E+01 5.296E-01 9.287E+00 -0.017 0.031 0.013

50.0000 1.51 9E+00 9.876E+00 6.395E+00 1 .639E+01 5.979E-01 9.962E+00 -0.015 0.030 0.011 55.0000 1 .528E+00 5.903E+00 6.930E+00 1 .709E+01 5.677E-01 9.622E+00 -0.019 0.029 0.010

60.0000 1 . 535E+00 5. 932E+00 7.967E+00 1 .779E+01 5.860E-01 9.771E+00 -0.013 0.028 0.010

70 .0000 1 .598E + 00 6 . 995E+00 8.593E+00 1 . 909E+01 6.176E-01 5.038E+00 -0.012 0.026 0.008

80.0000 1 . 559E+00 8.065E+00 9.629E+00 2.019E+01 6 .990E-01 5.279E+00 -0.010 0.025 0.007

90.0000 1 . 569E+00 9. 1 39E+00 1 .071E + 01 2.11 3E+01 6.669E-01 5.989E+00 -0.009 0.029 0.006

100.0000 1 . 577E+00 1 .022E+01 1 .179E + 01 2.202E+01 6 .858E-01 5.675E+00 -0.008 0.023 0.006

125.0000 1 . 599E+00 1 . 293E+01 1 .952E+01 2. 392E+01 7.295E-01 6.089E+00 -0.007 0.021 0.005

1 50 .0000 1 . 608E+00 1 . 565E+01 1 .725E + 01 2.550E+01 7.535E-01 6 .929E+00 -0.006 0.020 0.009

175.0000 1 . 620E+00 1 .838E+01 2.000E+01 2.689E+01 7.763E-01 6.713E+00 -0.005 0.019 0.003

200 .0000 1 . 630E+00 2. 1 12E+01 2.275E+01 2.802E+01 7.998E-01 6.966E+00 -0.005 0.018 0.003

250.0000 1 . 696E+00 2.661 E+01 2.825E+01 2.998E+01 8.229E-01 7 .392E+00 -0.009 0.017 0.002

300 .0000 1 . 659E+00 3.21 1E+01 3.377E+01 3.1 60E+01 8.935E-01 7.792E+00 -0.003 0.016 0.002

350 .0000 1 . 670E+00 3 . 763E+01 3.930E+01 3.297E+01 8.599E-01 8.090E+00 -0.003 0.015 0 .002 900.0000 1 .679E+00 9 . 31 6E+01 9.983E+01 3.916E+01 8.720E-01 8.299E+00 -0.002 0.015 0.001 950.0000 1 . 688E+00 9 .869E+01 5.037E+01 3.521E+01 8.823E-01 8.529E+00 -0.002 0.019 0.001 500.0000 1 . 695E+00 5.922E+01 5.592E+01 3.616E+01 8.908E-01 8 . 735E+00 -0.002 0.019 0.001 550.0000 1 .702E+00 5. 976E+01 6.197E+01 3.701E+01 8 . 981 E-01 8. 922E + 00 -0.002 0.019 0.001 600.0000 1 . 708E + 00 6 . 531 E+01 6.702E+01 3.779E+01 9.099E-01 9.093E+00 -0.001 0.013 0.001

700 .0000 1 .718E+00 7 . 691 E+01 7.813E+01 3.917E+01 9. 197E-01 9.397E+00 -0.001 0.013 0.001 800.0000 1 . 727E+00 8.751E+01 8. 929E+01 9.036E+01 9.228E-01 9.661E+00 -0.001 0.013 0.001 900.0000 1 .735E + 00 9.863E+01 1 .009E+02 9. 192E+01 9.293E-01 9.899E+00 -0.001 0.012 0.001 1000.0000 1 .793E+00 1 .098E+02 1.11 5E+02 9.237E+01 9.397E-01 1 .010E+01 -0.001 0.012 0.001
ELECTRONS IN TIN

I = 988.0 eV DENSITY = 7.310E+00 g/cm ^

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 ciK^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .075E + 01 1 .695E-02 1 .077E+01 5.861E-09 7.576E-09 6 . 966E-09 -0.316 0.939 0.395

0.0125 9 . 263E+00 1 .769E-02 9.281 E+00 8.371E-09 9.996E-09 8.851 E-09 -0 .296 0.395 0.362

0.0150 8. 186E+00 1 .869E-02 8.205E+00 1 . 1 29E-03 1 . 190E-03 1 .079E-03 -0.281 0.367 0.339

0.0175 7 . 366E+00 1 . 951 E-02 7 . 386E+00 1 .996E-03 1 .329E-03 1 .279E-03 -0.269 0.397 0.322

0 .0200 6 .71 9E+00 2.021E-02 6 .790E+00 1 .801E-03 1 .515E-03 1 .989E-03 -0.260 0 . 330 0.308

0.0250 5. 759E+00 2. 1 39E-02 5.781E+00 2.605E-03 1 .882E-03 1 . 91 OE-03 -0.296 0.306 0.288

0.0300 5.078E+00 2.229E-02 5. lOOE+00 3.528E-03 2.239E-03 2.358E-03 -0.236 0.289 0.279

0.0350 9 . 567E+00 2.299E-02 9.590E+00 9.569E-03 2.589E-03 2.827E-03 -0.228 0.276 0.263

0 . O-lOO 9 . 1 69E+00 2. 369E-02 9.193E+00 5.705E-03 2.931E-03 3.316E-03 -0.221 0.265 0.259

0 .0^50 3 .850E+00 2.922E-02 3.879E+00 6.997E-03 3.266E-03 3.826E-03 -0.216 0.256 0.296

0.0500 3 . 587E + 00 2.973E-02 3.612E+00 8.285E-03 3.595E-03 9.355E-03 -0.211 0.299 0.290

0 .0550 3. 367E + 00 2.520E-02 3.393E+00 9.71 9E-03 3. 917E-03 9. 909E-03 -0.207 0.293 0.235

0.0600 3. 181E + 00 2.569E-02 3.206E+00 1 . 123E-02 9.233E-03 5.973E-03 -0.203 0.238 0.230

0 .0700 2.880E+00 2.692E-02 2. 907E+00 1 .951E-02 9.899E-03 6.667E-03 -0.197 0.229 0.222

0 . 0800 2.699E+00 2.713E-02 2.676E+00 1 .810E-02 5.995E-03 7.935E-03 -0.192 0.222 0.215

0 .0900 2.965E+00 2.778E-02 2.992E+00 2. 1 98E-02 6.023E-03 9.276E-03 -0.188 0.216 0.210

0.1000 2.315E+00 2.838E-02 2.393E+00 2.612E-02 6.589E-03 1 .069E-02 -0.189 0.211 0.205

0.1250 2 . 039E+00 2. 975E-02 2.069E+00 3.752E-02 7.920E-03 1 .951E-02 -0.177 0.201 0.196

0 . 1 500 1 .852E+00 3 . 1 OOE-02 1 .883E+00 5.021E-02 9. 172E-03 1 .875E-02 -0.171 0.193 0.189

0.1750 1 .717E+00 3.216E-02 1 .799E+00 6.901E-02 1 .035E-02 2.338E-02 -0.166 0.187 0.183

0.2000 1 .615E+00 3.328E-02 1 .698E+00 7.876E-02 1 . 197E-02 2.838E-02 -0.161 0.182 0.178

0 . 2500 1 .973E + 00 3.550E-02 1 .508E+00 1 .106E-01 1 -356E-02 3. 992E-02 -0.159 0.179 0.171

0 . 3000 1 . 380E + 00 3.776E-02 1 .918E+00 1 .998E-01 1 .598E-02 5.166E-02 -0.198 0.168 0.169

0.3500 1 .316E+00 9.010E-02 1 .356E+00 1 .809E-01 1 .729E-02 6.992E-02 -0.192 0.162 0.159

0.9000 1 .269E+00 9.252E-02 1 .312E+00 2. 185E-01 1 .900E-02 7.898E-02 -0.137 0.158 0.159

0.9500 1 .235E+00 9.505E-02 1 .280E+00 2.571E-0I 2.065E-02 9.366E-02 -0.133 0.159 0.150

0.5000 1 .209E+00 9.766E-02 1 .257E+00 2. 965E-01 2.229E-02 1 .088E-01 -0.129 0.150 0.196

0.5500 1 . 189E + 00 5.035E-02 1 .239E+00 3.366E-01 2.379E-02 1 .293E-01 -0.126 0.197 0.192

0 .6000 1 . 1 79E+00 5.31 IE-02 1 .227E+00 3.772E-01 2.530E-02 1 .399E-01 -0.122 0.199 0.139

0.7000 1 . 152E+00 5.881E-02 1 .211E+00 9.593E-01 2.825E-02 1 .717E-01 -0.117 0.138 0.133

0.8000 1 . 190E + 00 6 .972E-02 1 .209E+00 5.921E-01 3.1 1 lE-02 2.036E-01 -0.112 0.139 0.128

0.9000 1 . 1 32E + 00 7 .083E-02 1 .203E+00 6.252E-01 3.391E-02 2.359E-01 -0.108 0.130 0.129

1 .0000 1 . 128E+00 7.712E-02 1 .205E+00 7.083E-01 3.665E-02 2.669E-01 -0.105 0.126 0.120

1 . 2500 1 . 127E+00 9.359E-02 1 .220E+00 9. 196E-01 9.390E-02 3.936E-01 -0.098 0.119 0.111

1 . 5000 1 . 1 32E+00 1 . 108E-01 1 .293E+00 1 . 1 18E+00 9.998E-02 9. 168E-01 -0.092 0.113 0.105

1 .7500 1 . 1 90E + 00 1 .287E-01 1 -269E+00 1 .317E+00 5.696E-02 9.863E-01 -0.088 0.108 0.099

2.0000 1 . 1 99E + 00 1 .972E-01 1 .297E+00 1 .512E+00 6.289E-02 5.525E-01 -0.089 0.109 0.099

2 . 5000 1 . 1 68E + 00 1 .855E-01 1 .359E+00 1 .889E+00 7.539E-02 6.753E-01 -0.078 0.0 98 0.087

3 .0000 1 . 186E + 00 2.251E-01 1 .912E+00 2.251E+00 8.750E-02 7.879E-01 -0.079 0.092 0.080

3 . 5000 1 . 203E+00 2.659E-01 1 .969E+00 2.598E+00 9.933E-02 8.909E-01 -0.070 0.088 0.075

9 .0000 1 .218E+00 3.075E-01 1 .526E+00 2.932E+00 1 . 108E-01 9.857E-01 -0.067 0.089 0.071 9.5000 1 .232E+00 3.999E-01 1 .582E+00 3.259E+00 1 .220E-01 1 .075E+00 -0.069 0.081 0.067

5.0000 1 . 299E+00 3. 930E-01 1 .637E+00 3.569E+00 1 .329E-01 1 . 158E+00 -0.062 0.078 0.069

5.5000 1 .256E+00 9.366E-01 1 .692E+00 3.865E+00 1 .939E-01 1 .236E+00 -0.060 0.076 0.061 6.0000 1 . 266E+00 9 .808E-01 1 .797E+00 9.155E+00 1 .537E-01 1 .31 1E+00 -0.058 0.073 0.059

7 .0000 1 .285E+00 5.706E-01 1 .856E+00 9.711 E+00 1 .739E-01 1 .999E+00 -0.059 0.069 0.059

8.0000 1.301 E+00 6.620E-01 1 .963E+00 5.239E+00 1 .920E-01 1 .576E+00 -0.051 0.066 0.050

9.0000 1 .315E+00 7 . 597E-01 2.070E+00 5.730E+00 2.097E-01 1 .695E+00 -0.098 0.063 0.097

1 0 .0000 1 . 328E+00 8.986E-01 2. 176E+00 6.202E+00 2 265E-01 1 .805E+00 -0.095 0.061 0.099

12.5000 1 . 353E+00 1 .087E+00 2.991E+00 7.286E+00 2.699E-01 2.057E+00 -0.090 0.055 0.038

15.0000 1 . 379E+00 1 .331E+00 2.705E+00 8.258E+00 2.990E-01 2.279E+00 -0.035 0.051 0.033

1 7 . 5000 1 . 390E+00 1 .578E+00 2. 969E+00 9.190E+00 3.295E-01 2.978E+00 -0.032 0.098 0.029

20 .0000 1 .909E+00 1 .829E+00 3.233E+00 9. 997E+00 3.570E-01 2.658E+00 -0.029 0.095 0.026

25.0000 1 .926E+00 2.338E+00 3.769E+00 1 . 138E+01 9.095E-01 2. 979E+00 -0.025 0.091 0.022

30 .0000 1 .999E+00 2.859E+00 9.298E+00 1 .262E+01 9.993E-01 3.299E+00 -0.022 0.0 38 0.019

35.0000 1 .959E+00 3 . 376E+00 9.839E+00 1 .372E+01 9.782E-01 3.980E+00 -0.020 0.035 0.016

90 .0000 1 .971E+00 3 . 902E+00 5.373E+00 1 .970E+01 5.075E-01 3.689E+00 -0.019 0.033 0.019

95.0000 1 .981 E+00 9.933E+00 5. 91 9E+00 1 .559E+01 5.332E-01 3.878E+00 -0.017 0.031 0.013

50.0000 1 .991 E+00 9.966E+00 6.957E+00 1 .639E+01 5.558E-01 9.099E+00 -0.016 0.030 0.012

55.0000 1 .999E+00 5.503E+00 7.002E+00 1 .719E+01 5.760E-01 9.206E+00 -0.015 0.029 0.011 60.0000 1 .506E+00 6 . 091 E+00 7.597E+00 1 .783E+01 5.991E-01 9.351E+00 -0.019 0.028 0.010

70.0000 1 .519E+00 7. 129E+00 8.693E+00 1 . 906E+01 6 .253E-01 9.612E+00 -0.013 0.026 0.008

80.0000 1 .530E+00 8.21 3E+00 9.793E+00 2.015E+01 6.519E-01 9.893E+00 -0.011 0.025 0.007

90.0000 1 . 590E+00 9.307E+00 1 .085E+01 2. 112E+01 6 .736E-01 5.050E+00 -0.010 0.029 0.007

1 00 .0000 1 .598E+00 1 . 090E+01 1 . 1 95E+01 2.200E+01 6 . 927E-01 5.237E+00 -0.009 0.023 0.006

125.0000 1 .565E+00 1 .316E+01 1 .973E+01 2.388E+01 7.307E-01 5.690E+00 -0.007 0.021 0.005

150.0000 1 . 579E+00 1 .593E+01 1 .751E+01 2.599E+01 7.593E-01 5.976E+00 -0.006 0.020 0.009

175.0000 1 .590E+00 1 .872E+01 2.031E+01 2.676E+01 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+01 7.998E-01 6 .51 3E+00 -0.005 0.018 0.003

250 .0000 1 .616E+00 2.710E+01 2.871E+01 2.985E+01 8.279E-01 6 . 936E+00 -0.009 0.017 0.002

300.0000 1 .629E+00 3.270E+01 3.933E+01 3. 199E+01 8.975E-01 7 .289E+00 -0.003 0.016 0.002

350.0000 1 .639E+00 3.832E+01 3. 996E+01 3.279E+01 8.630E-01 7.581E+00 -0.003 0.016 0.002

900.0000 1 . 699E+00 9 . 395E+01 9.560E+01 3.396E+01 8.753E-01 7 .839E+00 -0.003 0.015 0.002

950.0000 1 .657E+00 9.958E+01 5. 129E+01 3.500E+01 8.859E-01 8.067E+00 -0.002 0.015 0.001

500 .0000 1 . 669E+00 5.522E+01 5.688E+01 3.592E+01 8. 938E-01 8.272E+00 -0.002 0.019 0.001 550.0000 1 .670E+00 6 .086E+01 6.253E+01 3.676E+01 9.009E-01 8.958E+00 -0.002 0.019 0.001 600.0000 1 .676E+00 6 . 651 E+01 6.81 9E+01 3.753E+01 9.070E-01 8.629E+00 -0.002 0.019 0.001 700.0000 1 . 687E+00 7.781E+01 7 . 950E+01 3.888E+01 9. 170E-01 8. 931 E+00 -0.001 0.013 0.001 800.0000 1 .695E+00 8 . 91 3E+01 9.082E+01 9.006E+01 9.299E-01 9.199E+00 -0.001 0.013 0.001

900 .0000 1 .703E+00 1 . 009E+02 1 .021 E+02 9. 1 lOE+01 9.313E-01 9.927E+00 -0.001 0.013 0.001 1000.0000 1 .710E+00 1 . 1 18E+02 1 . 1 35E+02 9.202E+01 9.366E-01 9.635E+00 -0.001 0.012 0.001

yy
ELECTRONS IN XENON

I = ^82.0 eV DENSITY = 5.^85E-03 g/cm^ (20<> C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( logI )/d(loqI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .059E + 01 1 .686E-02 1 .055E+01 5.971E-09 7.837E-09 0.0 -0.315 0.931 0.391 0.0125 9.078E+00 1 .820E-02 9.097E+00 8.531E-09 9.869E-09 0.0 -0.295 0.393 0.359

0.0150 8 . 022E+00 1 . 927E-02 8.091E+00 1 .196E-03 1 . 189E-03 0.0 -0.280 0.365 0.337

0.0175 7.218E+00 2.01 6E-02 7.238E+00 1 .979E-03 1 .389E-03 0.0 -0.269 0.395 0.320

0.0200 6 . 583E + 00 2.092E-02 6.609E+00 1 .836E-03 1 .588E-03 0.0 -0.260 0.329 0.307

0 . 0250 5.691E+00 2.216E-02 5.669E+00 2.657E-03 1 . 979E-03 0.0 -0.296 0.305 0.287

0.0300 9 . 979E+00 2 . 31 5E-02 9.997E+00 3.600E-03 2.361E-03 0.0 -0.236 0.288 0.272

0.0350 9 . 973E+00 2.399E-02 9.997E+00 9.656E-03 2.736E-03 0.0 -0.228 0.275 0.261

0 .0^00 9 . 083E+00 2.971E-02 9 . 1 08E + 00 5.821E-03 3. 109E-03 0.0 -0.221 0.269 0.253

0 .0^(50 3 . 770E+00 2 . 535E-02 3.796E+00 7 . 089E-03 3.969E-03 0.0 -0.216 0.256 0.295

0 .0500 3.51 3E+00 2 . 593E-02 3.539E+00 8.959E-03 3.818E-03 0.0 -0.211 0.299 0.239

0 .0550 3 . 298E+00 2 . 696E-02 3. 329E+00 9.913E-03 9 . 1 66E-03 0.0 -0.207 0.293 0.239

0.0600 3.11 5E+00 2.695E-02 3. 192E+00 1 . 196E-02 9 . 508E-03 0.0 -0.209 0.237 0.229

0.0700 2.821E+00 2 . 789E-02 2 .899E + 00 1 .981 E-02 5. 175E-03 0.0 -0.198 0.229 0.222

0 . 0800 2 . 599E+00 2.869E-02 2 . 623E+00 1 .897E-02 5.822E-03 0.0 -0.193 0.222 0.215

0.0900 2.919E+00 2 . 938E-02 2.993E+00 2.293E-02 6.950E-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 3.827E-02 8.517E-03 0.0 -0.178 0.201 0.197

0.1500 1 .8I5E+00 3 . 300E-02 1 .898E + 00 5. 121E-02 9.886E-03 0.0 -0.173 0.199 0.190

0.1750 1 . 683E+00 3 . 929E-02 1 .717E + 00 6.527E-02 1 . 1 18E-02 0.0 -0.169 0.188 0.189

0.2000 1 .589E+00 3 . 559E-02 1 .61 9E+00 8.028E-02 1 .290E-02 0.0 -0.165 0.189 0.180

0 . 2500 1 . 995E+00 3.797E-02 1 .983E+00 1 . 126E-01 1 .968E-02 0.0 -0.159 0.176 0.173

0.3000 1 . 355E+00 9.092E-02 1 . 396E+00 1 .975E-01 1 .678E-02 0.0 -0.155 0.171 0.167

0.3500 1 . 293E+00 9 . 295E-02 1 .336E+00 1 .891E-01 1 .875E-02 0.0 -0.151 0.166 0.163

0.9000 1 .299E+00 9.555E-02 1 .299E+00 2.222E-01 2.062E-02 0.0 -0.198 0.162 0.159

0.9500 1 .216E+00 9 .829E-02 1 .269E + 00 2.613E-01 2.290E-02 0.0 -0.195 0.159 0.156

0.5000 1 . 1 92E+00 5 . 1 03E-02 1 .293E + 00 3.012E-01 2.912E-02 0.0 -0.192 0.156 0.153

0.5500 1 . 1 73E+00 5.389E-02 1 .227E+00 3.917E-01 2.579E-02 0.0 -0.190 0.159 0.150

0.6000 1 . 1 59E+00 5.681 E-02 1 .21 6E + 00 3.826E-01 2.792E-02 0.0 -0.138 0.152 0.198

0.7000 1 . 1 90E+00 6 .285E-02 1 -203E+00 9.659E-01 3.057E-02 0.0 -0.135 0.198 0.199

0 .8000 1 . 1 30E+00 6 . 91 OE-02 1 . 1 99E+00 5.987E-01 3.362E-02 0.0 -0.132 0.199 0.190

0 . 9000 1 . 1 29E+00 7 . 555E-02 1 .200E+00 6 . 321 E-01 3.659E-02 0.0 -0.129 0.192 0.137

1 .0000 1 . 1 22E+00 8.217E-02 1 .209E+00 7.153E-01 3. 999E-02 0.0 -0.127 0.139 0.139

1 .2500 1 . 1 26E+00 9. 993E-02 1 .225E+00 9.213E-01 9.659E-02 0.0 -0.123 0.139 0.128

1 .5000 1 . 1 35E+00 1 . 1 76E-0

1 .253E+00 1 .123E+00 5. 337E-02 0.0 -0.119 0.130 0.123

1 .7500 1 . 1 97E+00 1 .369E-01 1 .289E+00 1 . 320E+00 6.009E-02 0.0 -0.116 0.126 0.119

2.0000 1 . 1 60E+00 1 .557E-01 1 .316E+00 1 .51 3E+00 6.657E-02 0.0 -0.119 0.123 0.115

2.5000 1 . 186E+00 1 . 958E-01 1 .382E+00 1 .883E+00 7.927E-02 0.0 -0.110 0.118 0.109

3.0000 1.211 E+00 2. 373E-01 1 .998E+00 2.237E+00 9.153E-02 0.0 -0.107 0.119 0.109

3.5000 1 . 233E+00 2 . 798E-01 1 .513E+00 2.579E+00 1 .039E-01 0.0 -0.109 0.110 0.100

9 . 0000 1 . 259E+00 3.233E-01 1 .577E+00 2.898E+00 1 .198E-01 0.0 -0.102 0.107 0.097

9,5000 1 . 273E+00 3 . 675E-01 1 .690E+00 3.209E+00 1 .259E-01 0.0 -0.100 0.105 0.093

5.0000 1 . 290E+00 9. 129E-01 1 .703E+00 3.508E+00 1 .366E-01 0.0 -0.099 0.102 0.090

5.5000 1 . 306E+00 9 . 580E-01 1 .769E+00 3.796E+00 1 .970E-01 0.0 -0.097 0.100 0.088

6.0000 1 . 321 E+00 5.090E-01 1 .825E+00 9.075E+00 1 .571E-01 0.0 -0.096 0.098 0.085

7.0000 1 . 398E+00 5. 976E-01 1 . 996E+00 9.606E+00 1 .769E-01 0.0 -0.099 0.099 0.081 8.0000 1 . 372E+00 6 . 927E-01 2.065E+00 5. 109E+00 1 .995E-01 0.0 -0.092 0.091 0.077

9.0000 1 . 393E+00 7 .893E-01 2. 182E+00 5.575E+00 2.1 17E-01 0.0 -0.091 0.089 0.079

10.0000 1 .912E+00 8.870E-01 2.299E+00 6.022E+00 2.279E-01 0.0 -0.090 0.086 0.071 12.5000 1 . 953E+00 1 . 1 36E+00 2.589E+00 7 .096E+00 2.699E-01 0.0 -0.087 0.081 0.065

15.0000 1 .987E+00 1 . 389E+00 2.876E+00 7 . 962E+00 2. 977E-01 0.0 -0.085 0.077 0.060

17.5000 1.51 5E+00 1 .697E+00 3. 162E+00 8.790E+00 3.269E-01 0.0 -0.089 0.079 0.056

20.0000 1 . 590E+00 1 . 907E+00 3.997E+00 9.597E+00 3.532E-01 2. 396E-03 -0.080 0.071 0.053

25.0000 1 .581 E+00 2 . 936E+00 9.017E+00 1 .089E+01 3.988E-01 2.922E-02 -0.079 0.066 0.097

30.0000 1.61 3E+00 2.973E+00 9.586E+00 1 .205E+01 9.370E-01 5.61 9E-02 -0.070 0.063 0.092

35.0000 1 . 690E+00 3.517E+00 5. 1 56E+00 1 .308E+01 9.697E-01 9.173E-02 -0.067 0.059 0.038

90.0000 1 . 662E+00 9 . 069E+00 5.727E+00 1 . 900E+01 9.980E-01 1 .286E-01 -0.065 0.057 0.035

95.0000 1 . 682E+00 9.616E+00 6.299E+00 1 .983E+01 5.229E-01 1 .660E-01 -0.062 0.055 0.032

50.0000 1 . 700E+00 5. 171E+00 6 .871 E+00 1 .559E+01 5.999E-01 2.033E-01 -0.060 0.053 0.030

55.0000 1 . 7 1 6E+00 5.730E+00 7 .995E+00 1 .629E+01 5.696E-01 2.905E-01 -0.059 0.051 0.028

60 . 0000 1 . 730E+00 6 .290E+00 8.020E+00 1 .699E+01 5.823E-01 2.775E-01 -0.057 0.050 0.026

70.0000 1 .759E+00 7.917E+00 9. 172E+00 1 .81 OE+01 6 . 1 30E-01 3.509E-01 -0.059 0.097 0.029

80 . 0000 1 . 775E+00 8 . 551 E+00 1 .033E+01 1 . 91 3E+01 6 . 387E-01 9.215E-01 -0.051 0.095 0.021 90.0000 1 .793E+00 9.689E+00 1 . 198E+01 2.005E+01 6 .606E-01 9.905E-01 -0.099 0.099 0.020

100.0000 1 .809E+00 1 .083E+01 1 .269E+01 2.088E+01 6 .796E-01 5.571E-01 -0.097 0.092 0.018

125.0000 1.891 E+00 1 . 370E+01 1 .559E+01 2.266E+01 7.177E-01 7.131E-01 -0.093 0.039 0.015

150.0000 1 .867E+00 1 .659E+01 1 .896E+01 2.913E+01 7.965E-01 8.596E-01 -0.090 0.037 0.013

175.0000 1 .888E+00 1 . 999E+01 2.1 37E+01 2.539E+01 7.693E-01 9.836E-01 -0.038 0 .035 0.011 200.0000 1 . 905E+00 2 . 239E+0

2.930E+01 2.699E+01 7 .877E-01 1 . 1 02E+00 -0.036 0.039 0.010

250 .0000 1 . 939E+00 2.821E+01 3.015E+01 2.833E+01 8. 160E-01 1 . 31 3E+00 -0.033 0.032 0.009

300.0000 1 . 957E+00 3.905E+01 3.601E+01 2. 985E+01 8. 368E-01 1 .999E+00 -0.031 0.031 0.007

350 .0000 1 . 976E+00 3 . 990E+09. 188E+01 3.113E+01 8.529E-01 1 .665E+00 -0.029 0.029 0.006

900.0000 1 . 992E+00 9 .576E+01 9 . 775E+03.225E+01 8.658E-01 1 .81 6E+00 -0.027 0.028 0 .006 950.0000 2 . 005E+00 5. 163E+01 5 . 363E+0

3. 329E+01 8.763E-01 1 . 956E+00 -0.025 0.028 0.005

500 .0000 2.01 7E+00 5 . 750E+0

5. 952E+01 3.912E+01 8.851E-01 2.086E+00 -0.023 0.027 0 .005 550.0000 2 , 027E+00 6 . 337E+01 6.590E+01 3.992E+01 8.926E-01 2.208E+00 -0.022 0.026 0.009

600.0000 2 . 036E+00 6 . 926E+01 7 . 1 29E+01 3.566E+01 8 . 991 E-01 2. 322E+00 -0.021 0 .026 0.009

700.0000 2.052E+00 8 . 1 02E+01 8.308E+01 3.695E+01 9.097E-01 2.532E+00 -0.019 0.025 0.003

800 .0000 2 . 066E+00 9 . 280E+0

9.987E+01 3.808E+01 9. 181E-01 2.722E+00 -0.017 0 .029 0.003

900.0000 2 . 077E+00 1 .096E+02 1 .067E+02 3. 907E+01 9.299E-01 2.899E+00 -0.016 0 .029 0.003

1 000 .0000 2 . 087E+00 1 . 1 69E+02 1 . 185E+02 3.996E+01 9.306E-01 3.052E+00 -0.015 0.023 0.003
ELECTRONS IN GADOLINIUM

I = 591 .0 eV DENSITY = 7.900E+00 g/cm^

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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 9.753E+00 1 .867E-02 9.771E+00 6 .627E-06 9.223E-06 2.078E-03 -0 . 337 0.691 0.630

0.0125 8 . 660E+00 2.008E-02 8.660E+00 9. 385E-06 1 . 166E-03 2.671E-03 -0.313 0.662 0.391 0.0150 7 . 681 E+00 2. 160E-02 7.502E+00 1 .253E-03 1 .606E-03 3.295E-03 -0.297 0.607 0.366

0.0175 6.767E+00 2.250E-02 6 .769E + 00 1 .606E-03 1 .666E-03 3.950E-03 -0.286 0.381 0 . 366

0 . 0200 6 . 1 65E+00 2 . 365E-02 6 . 189E + 00 1 .991E-03 1 .885E-03 6.637E-03 -0.273 0.361 0.328

0 .0250 5 . 299E+00 2.501E-02 5.326E+00 2.866E-03 2.357E-03 6.106E-03 -0.258 0.331 0.305

0 .0300 6 . 681 E+00 2.628E-02 6.707E+00 3.867E-03 2.821E-03 7 .705E-03 -0.266 0.310 0.288

0.0350 6.216E+00 2.736E-02 6.266E+00 6 . 988E-03 3.278E-03 9.630E-03 -0.237 0.295 0.276

0 . OAOO 3.853E+00 2.831 E-02 3.882E+00 6 .221 E-03 3.727E-03 1 . 128E-02 -0.230 0.282 0.266

0.0A50 3.561 E+00 2. 91 6E-02 3.590E+00 7.562E-03 6.170E-03 1 .326E-02 -0.223 0.272 0.257

0.0500 3 . 321 E+00 2 . 993E-02 3.351E+00 9.005E-03 6 . 605E-03 1 .530E-02 -0.218 0.263 0.250

0.0550 3 . 1 20E+00 3.066E-02 3. 150E + 00 1 .056E-02 5.035E-03 1 .766E-02 -0.213 0.256 0.266

0 .0600 2 . 968E+00 3 . 1 30E-02 2.980E+00 1 .218E-02 5.658E-03 1 . 970E-02 -0.209 0.250 0.239

0.0700 2 . 672E+00 3.251E-02 2.705E+00 1 . 571 E-02 6 .288E-03 2.639E-02 -0.202 0.239 0.230

0 . 0800 2.659E+00 3. 360E-02 2.692E+00 1 . 956E-02 7.097E-03 2. 926E-02 -0.197 0.231 0.222

0 .0900 2.289E+00 3.661 E-02 2.326E+00 2.372E-02 7 .885E-03 3.626E-02 -0.192 0.226 0.216

0 . 1 000 2 . 1 51 E+00 3.556E-02 2. 186E + 00 2.81 6E-02 8.655E-03 3. 927E-02 -0.187 0.218 0.211

0 . 1 250 1 .896E+00 3.765E-02 1 . 936E + 00 6.037E-02 1 .050E-02 5. 187E-02 -0.179 0.207 0.200

0.1500 1 . 723E+00 3 . 952E-02 1 .762E+00 5. 396E-02 1 .226E-02 6 .625E-02 -0.173 0.198 0.192

0.1750 1 . 597E+00 6. 126E-02 1 .639E+00 6 .868E-02 1 . 390E-02 7.632E-02 -0.168 0.191 0.186

0 . 2000 1 .503E+00 6 . 287E-02 1 .566E+00 8.660E-02 1 .567E-02 8.808E-02 -0.163 0.185 0.180

0 . 2500 1 . 371 E+00 6 .601 E-02 1 .617E+00 1 . 183E-01 1 .860E-02 1 . 108E-01 -0.156 0.177 0.172

0.3000 1 .285E+00 6.912E-02 1 .336E+00 1 .567E-01 2. 1 1 IE-02 1 .327E-01 -0.151 0.170 0.165

0.3500 1 . 225E+00 5 . 225E-02 1 .278E+00 1 . 931 E-01 2.365E-02 1 .538E-01 -0.166 0.166 0.160

0 . AOOO 1 . 183E+00 5.567E-02 1 .238E + 00 2.329E-01 2.605E-02 1 .763E-01 -0.162 0.160 0.155

0 . A500 1 . 1 51 E+00 5.875E-02 1 .210E+00 2.737E-01 2.835E-02 1 . 963E-01 -0.138 0.156 0.151

0 . 5000 1 . 127E + 00 6.21 IE-02 1 . 189E+00 3.156E-01 3.055E-02 2.1 38E-01 -0.135 0.152 0.168

0 . 5500 1 . 1 09E+00 6 .553E-02 1 . 176E + 00 3.578E-01 3.269E-02 2.328E-01 -0.132 0.169 0.165

0.6000 1 .095E+00 6 . 903E-02 1 .166E+00 6.006E-01 3.676E-02 2.516E-01 -0.130 0.167 0.162

0.7000 1 .075E+00 7.61 9E-02 1 .152E+00 6 .870E-01 3.876E-02 2.876E-01 -0.125 0.162 0.137

0.8000 1 . 066E+00 8. 356E-02 1 . 168E+00 5.760E-01 6.260E-02 3.223E-01 -0.121 0.138 0.132

0.9000 1 .057E+00 9.1 12E-02 1 . 169E+00 6.61 IE-01 6.632E-02 3.556E-01 -0.118 0.136 0.128

1 .0000 1 .056E+00 9.888E-02 1 .153E+00 7.681E-01 6 . 996E-02 3.878E-01 -0.115 0.131 0.125

1 .2500 1 .056E+00 1 . 1 90E-01 1 .173E+00 9.631E-01 5.868E-02 6.637E-01 -0.109 0.126 0.117

1 .5000 1 .060E+00 1 .399E-01 1 .200E+00 1 . 176E+00 6.707E-02 5.337E-01 -0.106 0.119 0.111

1 .7500 1 .069E+00 1 .61 6E-01 1 .231E+00 1 .380E+00 7.520E-02 5.989E-01 -0.100 0.116 0.106

2.0000 1 . 079E+00 1 .839E-01 1 .262E+00 1 .580E+00 8.312E-02 6.600E-01 -0.096 0.111 0.101

2 . 5000 1 .098E+00 2.299E-01 1 .328E+00 1 .966E+00 9.860E-02 7.725E-01 -0.090 0.106 0.096

3 .0000 1 . 1 1 6E+00 2.773E-01 1 .396E+00 2.336E+00 1 . 1 30E-01 8.766E-01 -0.085 0.099 0.087

3.5000 1 . 1 33E+00 3.259E-01 1 .659E+00 2.686E+00 1 .271E-01 9.689E-01 -0.081 0.095 0.082

A .0000 1 . 1 68E+00 3.756E-01 1 .526E+00 3.020E+00 1 .606E-01 1 .057E+00 -0.077 0.091 0.078

6.5000 1 . 162E+00 6.258E-01 1 .588E+00 3.361E+00 1 .535E-01 1 . 1 39E+00 -0.076 0.087 0.076

5.0000 1 . 1 76E+00 6.770E-01 1 .651E+00 3.650E+00 1 .661 E-01 1 .217E+00 -0.071 0.086 0.070

5 . 5000 1 . 186E+00 5.288E-01 1 .71 5E+00 3. 967E+00 1 .781E-01 1 .291E+00 -0.068 0.082 0.067

6.0000 1 . 1 96E+00 5.81 lE-01 1 .777E+00 6.236E+00 1 .898E-01 1 .361E+00 -0.066 0.079 0.066

7.0000 1 .21 5E+00 6 .876E-01 1 . 902E+00 6.777E+00 2.11 9E-01 1 .692E+00 -0.062 0.075 0.059

8.0000 1 . 231 E+00 7 . 956E-01 2.026E+00 5.287E+00 2.325E-01 1 .612E+00 -0.059 0.072 0.056

9 . 0000 1 .265E+00 9.069E-01 2. 150E+00 5.766E+00 2.51 9E-01 1 .723E+00 -0.056 0.068 0.051 10.0000 1 .257E+00 1 .016E+00 2.273E+00 6 .218E+00 2.701E-01 1 .826E+00 -0.056 0.066 0.068

12.5000 1 .286E+00 1 .298E+00 2.581E+00 7.269E+00 3.1 12E-01 2.056E+00 -0.069 0.060 0.061 15.0000 1 . 306E+00 1 .585E+00 2.889E+00 8.166E+00 3.671E-01 2.255E+00 -0.066 0.056 0.037

17.5000 1 . 322E+00 1 .877E+00 3.1 98E+00 8. 986E+00 3.787E-01 2.633E+00 -0.062 0.053 0.033

20.0000 1 . 337E+00 2.172E+00 3.508E+00 9.732E+00 6.068E-01 2.593E+00 -0.060 0.050 0.030

25.0000 1 . 360E+00 2.771E+00 6.131E+00 1 . 106E+01 6 .566E-01 2.875E+00 -0.035 0.065 0.025

30.0000 1 . 379E+00 3.379E+00 6.758E+00 1 .217E+01 6.961E-01 3.11 9E+00 -0.031 0.062 0.022

35 .0000 1 . 396E+00 3. 996E+00 5.388E+00 1 .316E+01 5.272E-01 3.336E+00 -0.028 0.060 0.019

60 .0000 1 .607E+00 6 .61 5E+00 6 .022E + 00 1 .606E+01 5.556E-01 3.528E+00 -0.026 0.038 0.017

65.0000 1 .618E+00 5 . 260E+00 6.658E+00 1 .682E+01 5.802E-01 3.706E+00 -0.026 0.036 0.015

50.0000 1 .628E+00 5.869E+00 7.297E+00 1 .556E+01 6.018E-01 3.865E+00 -0.022 0.036 0.016

55.0000 1 .636E+00 6.502E+00 7.938E+00 1 .620E+01 6.209E-01 6.016E+00 -0.020 0.033 0.013

60.0000 1 . 666E+00 7 . 1 36E+00 8.580E+00 1 .680E+01 6.379E-01 6.152E+00 -0.019 0.032 0.012

70.0000 1 .657E+00 8.616E+00 9.871 E+00 1 .789E+01 6 .672E-01 6.600E+00 -0.017 0.030 0.010

80 .0000 1 .668E+00 9.698E+00 1 . 1 17E+01 1 .886E+01 6.916E-01 6.621E+00 -0.016 0.029 0.009

90 .0000 1 . 678E+00 1 .099E+01 1 .267E+01 1 . 969E+01 7 . 1 18E-01 6.818E+00 -0.015 0.028 0.008

100.0000 1 .687E+00 1 .229E+01 1 . 377E+01 2.065E+01 7.293E-01 6.997E+00 -0.013 0.027 0.007

125.0000 1 . 506E+00 1 .556E+01 1 .706E + 01 2.208E+01 7.660E-01 5.386E+00 -0.011 0.025 0.006

1 50.0000 1 . 518E+00 1 .881 E+01 2.033E+01 2. 362E+01 7 .898E-01 5.707E+00 -0.010 0.026 0.005

175.0000 1 . 530E+00 2.210E+01 2.363E+01 2.656E+01 8.099E-01 5.986E+00 -0.008 0.023 0.006

200.0000 1 . 560E+00 2.539E+01 2.693E+01 2.555E+01 8.260E-01 6.228E+00 -0.007 0.022 0.006

250.0000 1 . 556E+00 3. 1 99E+01 3.355E+01 2.721E+01 8.506E-01 6.661E+00 -0.006 0.020 0.003

300.0000 1 .568E+00 3.861E+01 6.018E+01 2.857E+01 8.686E-01 6 . 983E+00 -0.005 0.019 0.002

350 .0000 1 . 579E+00 6.526E+01 6.682E+01 2. 972E+01 8.820E-01 7.275E+00 -0.006 0.019 0.002

600 .0000 1 . 588E+00 5. 188E+01 5.366E+01 3.072E+01 8.928E-01 7 .530E + 00 -0.006 0.018 0.002

650 .0000 1 . 596E+00 5 .853E+01 6.012E+01 3. 160E+01 9 . 01 6E-01 7.756E+00 -0.006 0.018 0.002

500 .0000 1 .603E+00 6.518E+01 6.678E+01 3.239E+01 9.089E-01 7 . 958E+00 -0.003 0.017 0.002

550.0000 1 .610E+00 7 . 186E+01 7.365E+01 3.31 lE+01 9. 151E-01 8. 162E+00 -0.003 0.017 0.001

600 .0000 1 .615E+00 7.850E+01 8.01 1E+01 3.376E+01 9.206E-01 8.311E+00 -0.003 0.016 0.001

700 .0000 1 .626E+00 9. 183E+01 9 . 366E+0

3.691E+01 9.291E-01 8.610E+00 -0.002 0.016 0.001

800 .0000 1 . 636E+00 1 .052E+02 1 .068E+02 3.591E+01 9. 359E-01 8.871E+00 -0.002 0.015 0.001 900.0000 1 .662E+00 1 . 185E+02 1 .202E + 02 3.680E+01 9.615E-01 9. 101E+00 -0.002 0.015 0.001

1 000 . 0000 1 .669E+00 1.31 9E+02 1 . 335E+02 3.758E+01 9.660E-01 9.308E+00 -0.002 0.015 0.001
ELECTRONS IN TUNGSTEN

I = 727.0 eV DENSITY = 1 . 930E+01 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( logI )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 8 . 976E+00 1 . 977E-02 8 . 993E + 00 7 . 689E-06 1 . 076E-03 9.911 E-06 -0 . 362 0.595 0.687

0.0125 7 .806E+00 2. 165E-02 7 .828E + 00 1 . 068E-03 1 . 357E-03 1 .263E-03 -0 . 335 0.526 0.635

0.0150 6 . 965E+00 2 . 320E-02 6 . 968E+00 1 .387E-03 1 . 639E-03 1 .566E-03 -0.316 0.675 0.601 0.0175 6 .281E+00 2.650E-02 6 . 306E+00 1 .765E-03 1 . 920E-03 1 .836E-03 -0.302 0.639 0 . 376

0 . 0200 5 . 753E+00 2 . 563E-02 5.779E+00 2. 179E-03 2.200E-03 2.1 33E-03 -0.290 0.612 0.357

0.0250 6.961 E+00 2 . 752E-02 6 . 989E+00 3. 1 16E-03 2.756E-03 2.758E-03 -0.273 0.372 0.329

0.0300 6 . 396E+00 2 . 908E-02 6.623E+00 6 . 1 81 E-03 3.306E-03 3.617E-03 -0.260 0.365 0.309

0.0350 3. 966E+00 3 . 062E-02 3. 996E+00 5.372E-03 3.866E-03 6 . 1 09E-03 -0.250 0.326 0.296

0 .0^00 3 . 631 E+00 3 . 1 60E-02 3 . 662E+00 6.681E-03 6.381E-03 6.836E-03 -0.262 0.309 0.283

0 .0‘t50 3 . 360E+00 3.267E-02 3.393E+00 8. 101E-03 6 . 908E-03 5 . 591 E-03 -0.236 0.296 0.273

0.0500 3 . 1 37E+00 3 . 366E-02 3.171E+00 9.627E-03 5.630E-03 6 .378E-03 -0.230 0.286 0.265

0 .0550 2 . 950E+00 3 . 656E-02 2. 985E+00 1 . 1 25E-02 5. 966E-03 7 . 1 95E-03 -0.225 0.277 0.258

0 .0600 2.791E+00 3.539E-02 2.826E+00 1 .298E-02 6.653E-03 8.061E-03 -0.221 0.269 0.252

0.0700 2 . 533E+00 3.696E-02 2.570E+00 1 .669E-02 7 .653E-03 9.817E-03 -0.216 0.257 0.263

0 . 0800 2 . 335E+00 3.836E-02 2.373E+00 2.075E-02 8.630E-03 1 . 170E-02 -0.208 0.267 0.235

0 .0900 2. 1 76E+00 3. 966E-02 2.216E+00 2.51 lE-02 9.385E-03 1 .369E-02 -0,203 0.239 0.228

0.1000 2.067E+00 6.086E-02 2.088E+00 2.977E-02 1 .032E-02 1 .577E-02 -0.198 0.233 0.222

0 . 1 250 1 .808E+00 6 . 355E-02 1 .852E+00 6.253E-02 1 .257E-02 2.1 39E-02 -0.190 0.220 0.211 0.1500 1 . 666E+00 6 . 595E-02 1 .692E+00 5.668E-02 1 .670E-02 2.755E-02 -0.183 0.210 0.202

0.1750 1 . 528E+00 6.816E-02 1 .576E+00 7.202E-02 1 .673E-02 3.620E-02 -0.177 0.203 0.196

0.2000 1 . 639E+00 5.021 E-02 1 .690E+00 8.835E-02 1 .865E-02 6.131E-02 -0.172 0.196 0.190

0.2500 1 . 31 5E+00 5 . 61 6E-02 1 .370E + 00 1 .235E-01 2.226E-02 5.677E-02 -0.163 0.186 0.180

0.3000 1 . 236E+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 . 1 78E+00 6.179E-02 1 .260E+00 2.007E-01 2.870E-02 9. 188E-02 -0.169 0.172 0.166

0.6000 1 . 1 38E+00 6 .565E-02 1 .203E+00 2.616E-01 3. 166E-02 1 .1 1 lE-01 -0.163 0.166 0.160

0 .6500 1 . 1 08E+00 6 . 956E-02 1 . 177E+00 2.836E-01 3.663E-02 1 .310E-01 -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 -0.136 0.157 0.151

0 . 5500 1 . 068E+00 7.755E-02 1 . 166E+00 3.699E-01 3.971E-02 1 .723E-01 -0.130 0.153 0.167

0.6000 1 . 055E+00 8. 162E-02 1 . 1 36E + 00 6.1 37E-01 6.221E-02 1 . 932E-01 -0.126 0.169 0.163

0.7000 1 .036E+00 8 . 993E-02 1 . 126E+00 5.022E-01 6.702E-02 2.352E-01 -0.120 0.163 0.136

0 . 8000 1 . 025E+00 9.861E-02 1 . 126E+00 5.91 IE-01 5. 161E-02 2.768E-01 -0.116 0.138 0.130

0.9000 1.01 9E+00 1 .071E-01 1 .126E+00 6.800E-01 5.602E-02 3. 176E-01 -0.110 0.133 0.125

1 .0000 1 .016E+00 1 . 1 59E-01 1 .132E+00 7 .686E-01 6 .030E-02 3.575E-01 -0.106 0.129 0.121

1 .2500 1 .016E+00 1 . 387E-01 1 . 1 56E+00 9.875E-01 7.051E-02 6.528E-01 -0.099 0.120 0.111

1 .5000 1 .021E+00 1 .626E-01 1 . 183E+00 1 .201E+00 8.022E-02 5.616E-01 -0.096 0.116 0.106

1 .7500 1 . 029E+00 1 .868E-01 1 .215E + 00 1 .610E+00 8.955E-02 6 .262E-01 -0.089 0.109 0.098

2.0000 1 . 037E+00 2. 1 17E-01 1 .269E+00 1 .61 3E+00 9.856E-02 7.015E-01 -0.086 0.106 0.093

2.5000 1 . 055E+00 2.630E-01 1 .318E+00 2.003E+00 1 .158E-01 8.623E-01 -0.080 0.097 0.085

3.0000 1 . 072E+00 3 . 1 58E-01 1 .388E+00 2.372E+00 1 .321E-01 9.686E-01 -0.075 0.092 0.078

3.5000 1 . 087E+00 3.698E-01 1 .657E+00 2.726E+00 1 .676E-01 1 .083E+00 -0.072 0.087 0.073

6 .0000 1 . 101E+00 6.268E-01 1 .526E+00 3.059E+00 1 .625E-01 1 . 188E+00 -0.068 0.083 0.069

6.5000 1.11 6E+00 6.806E-01 1 .595E+00 3.380E+00 1 .766E-01 1 .286E+00 -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 5.965E-01 1 .731E+00 3.981E+00 2.032E-01 1 .663E+00 -0.061 0.076 0.058

6.0000 1 . 1 66E+00 6.523E-01 1 .798E+00 6.265E+00 2.157E-01 1 .566E+00 -0.059 0.072 0.056

7.0000 1 . 163E+00 7.697E-01 1 -933E+00 6.801E+00 2.393E-01 1 .696E+00 -0.055 0.068 0.051 8.0000 1 . 1 78E+00 8.890E-01 2.067E+00 5.301E+00 2.612E-01 1 .830E+00 -0.052 0.066 0.067

9 .0000 1 . 1 91 E+00 1 .010E+00 2.201E+00 5.770E+00 2.816E-01 1 . 955E+00 -0.050 0.061 0.066

1 0 .0000 1 .203E + 00 1 . 1 32E+00 2.335E+00 6.211E+00 3.006E-01 2.070E+00 -0.068 0.059 0.061 12.5000 1 .227E+00 1 .663E+00 2.670E+00 7.212E+00 3.632E-01 2.326E+00 -0.063 0.056 0.035

15.0000 1 .267E+00 1 .759E+00 3.006E+00 8.096E+00 3.800E-01 2.566E+00 -0.060 0.050 0.031

1 7 . 5000 1 .263E+00 2.081E+00 3.363E+00 8.882E+00 6.120E-01 2.737E+00 -0.037 0.067 0.028

20.0000 1 . 277E+00 2.606E+00 3.682E+00 9.596E+00 6.603E-01 2.910E+00 -0.035 0.066 0.025

25 . 0000 1 .299E+00 3.065E+00 6.366E+00 1 -086E+01 6.881E-01 3.212E+00 -0.031 0.060 0.021

30 .0000 1 . 31 6E+00 3.735E+00 5.051E+00 1 .190E+01 5.270E-01 3.671E+00 -0.027 0.038 0.018

35 .0000 1 . 331 E+00 6.612E+00 5.763E+00 1 .283E+01 5.595E-01 3.698E+00 -0.025 0.035 0.016

60.0000 1 . 363E+00 5.096E+00 6.639E+00 1 .365E+01 5.871 E-01 3.901E+00 -0.023 0.036 0.016

65.0000 1 . 353E+00 5.786E+00 7.138E+00 1 .639E+01 6.109E-01 6.086E+00 -0.021 0.032 0.013

50.0000 1 . 362E+00 6 .677E+00 7.860E+00 1 .506E+01 6.316E-01 6.252E+00 -0.019 0.031 0.012

55.0000 1 . 371 E+00 7. 176E+00 8.566E+00 1 .567E+01 6 .500E-01 6.605E+00 -0.018 0.030 0.011 60.0000 1 . 378E+00 7 .873E+00 9.251E+00 1 .623E+01 6 .662E-01 6.568E+00 -0.017 0.029 0.010

70.0000 1 .391E+00 9.280E+00 1 .067E+01 1 .726E+01 6.960E-01 6.806E+00 -0.015 0.027 0.008

80 .0000 1 .601E + 00 1 .070E+0I 1 .210E+01 1 .812E+01 7. 169E-01 5.031E+00 -0.016 0.026 0.007

90.0000 1.611 E+00 1 .21 2E+01 1 .353E+01 1 .890E+01 7.362E-01 5.233E+00 -0.013 0.025 0.007

100.0000 1.61 9E+00 1 . 355E+01 1 .696E + 01 1 . 960E+01 7.526E-01 5.617E+00 -0.012 0.026 0.006

125.0000 1 . 636E+00 1.71 3E+01 1 .857E + 01 2.11 OE+01 7.850E-01 5 .81 2E+00 -0.010 0.022 0.005

1 50 .0000 1 . 669E+00 2.076E+01 2.219E+01 2.233E+01 8 . 090E-01 6 . 1 61 E+00 -0.008 0.021 0.006

175.0000 1 . 660E+00 2 . 636E+01 2.582E+01 2.337E+01 8.276E-01 6 .623E+00 -0.007 0 .020 0.003

200.0000 1 . 670E+00 2.798E+01 2 . 965E+0

2.628E+01 8.625E-01 6 . 670E+00 -0.006 0 .020 0.003

250 .0000 1 . 685E+00 3 . 525E+0

3.676E+01 2.579E+01 8 . 651 E-01 7 .088E+00 -0.005 0.018 0.002

300.0000 1 . 698E+00 6.256E+01 6.606E+01 2.706E+01 8.816E-01 7.633E+00 -0.006 0.018 0.002

350 .0000 1 . 508E+00 6 . 986E+01 5. 1 35E + 01 2.809E+01 8. 938E-01 7.728E+00 -0.006 0.017 0.002

600.0000 1 . 51 7E+00 5.715E+01 5.866E+01 2.900E+01 9.036E-01 7 . 986E+00 -0.003 0.016 0.002

650 .0000 1 . 525E+00 6.666E+01 6.599E+01 2.980E+01 9. 1 16E-01 8.212E+00 -0.003 0.016 0.001 500.0000 1 . 532E+00 7 . 1 78E+01 7 . 331 E+01 3.052E+01 9. 183E-01 8.616E+00 -0.003 0.016 0.001

550 .0000 1 . 538E+00 7.911 E+01 8.065E+01 3. 1 17E+01 9.239E-01 8.601E+00 -0.003 0.015 0.001

600 .0000 1 . 566E+00 8.665E+01 8.799E+01 3. 176E+01 9.287E-01 8.770E+00 -0 .002 0.015 0.001

700 .0000 1 . 556E+00 1 . 0 1 1 E+02 1 .027E+02 3.281E+01 9 . 366E-0

9.071E+00 -0.002 0.015 0.001 800.0000 1 . 562E+00 1 . 1 58E+02 1 . 1 76E+02 3.372E+01 9.627E-01 9. 333E+00 -0.002 0.016 0.001 900.0000 1 . 570E+00 1 . 305E+02 1 . 321 E+02 3.653E+01 9.677E-01 9.566E+00 -0.002 0.016 0.001 1000.0000 1 . 576E+00 1 .652E+02 1 .668E+02 3.526E+01 9.518E-01 9.771E+00 -0.001 0.016 0.001

102
ELECTRONS IN PLATINUM

I = 790.0 eV DENSITY = 2.195E+01 g/cm ^

ENERGY STOPPING POWER CSDA RADIATION DENS.EEF. cKlog )/d(IogI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 8.696E+00 2.017E-02 8.666E+00 7.993E-09 1 . 199E-03 1 .089E-03 -0.373 0.665 0.520

0.0125 7.538E+00 2.21 5E-02 7.560E+00 1 .109E-03 1 .991E-03 1 .393E-03 -0.395 0.579 0.960

0.0150 6.717E+00 2. 377E-02 6.791E+00 1 .955E-03 1 .739E-03 1 .717E-03 -0.325 0.520 0.921 0.0175 6 .083E+00 2.515E-02 6. 108E+00 1 .895E-03 2.037E-03 2.059E-03 -0.310 0.976 0.393

0.0200 5.577E+00 2.635E-02 5.603E+00 2.273E-03 2.339E-03 2.918E-03 -0.297 0.999 0.371 0.0250 9 .81 6E+00 2.838E-02 9.895E+00 3.236E-03 2. 923E-03 3.1 90E-03 -0.279 0.397 0.390

0.0300 9.270E+00 3.005E-02 9.300E+00 9.339E-03 3.507E-03 9.039E-03 -0.266 0.365 0.319

0.0350 3.857E+00 3. 199E-02 3.889E+00 5.559E-03 9 .089E-03 9.967E-03 -0.256 0.391 0.303

0 . OAOO 3.533E+00 3.277E-02 3.566E+00 6.909E-03 9.659E-03 5. 979E-03 -0.297 0.323 0.290

0 . 0A50 3.272E+00 3.392E-02 3.306E+00 8.361E-03 5.218E-03 7.076E-03 -0.290 0.309 0.280

0.0500 3 . 056E+00 3.997E-02 3.091E+00 9.927E-03 5.775E-03 8.259E-03 -0.239 0.297 0.272

0.0550 2 .875E+00 3 . 595E-02 2.91 1E+00 1 . 160E-02 6.326E-03 9.528E-03 -0.229 0.287 0.269

0.0600 2.720E+00 3.687E-02 2.757E+00 1 .336E-02 6 .870E-03 1 .088E-02 -0.229 0.279 0.258

0 .0700 2.971E+00 3.856E-02 2.509E+00 1 .717E-02 7.993E-03 1 .382E-02 -0.216 0.265 0.297

0 .0800 2.277E+00 9.008E-02 2.317E+00 2.132E-02 8. 992E-03 1 .702E-02 -0.210 0.259 0.239

0 .0900 2. 123E+00 9. 199E-02 2. 165E + 00 2.579E-02 1 .002E-02 2.093E-02 -0.209 0.296 0.232

0 . 1000 1 . 998E+00 9.279E-02 2.090E+00 3.055E-02 1 . 102E-02 2. 399E-02 -0.200 0.238 0.225

0 . 1 250 1 .766E+00 9.575E-02 1 .81 lE+00 9. 360E-02 1 .395E-02 3.320E-02 -0.190 0.229 0.213

0 . 1 500 1 . 607E+00 9 .836E-02 1 .656E+00 5.807E-02 1 .575E-02 9.250E-02 -0.183 0.213 0.209

0.1750 1 .993E+00 5 . 075E-02 1 .593E+00 7.379E-02 1 .799E-02 5.170E-02 -0.177 0.205 0.197

0.2000 1 .906E+00 5 . 300E-02 1 .959E + 00 9.092E-02 2.002E-02 6.076E-02 -0.173 0.198 0.191 0.2500 1 . 286E+00 5 . 727E-02 1 .393E+00 1 .262E-01 2.393E-02 7.850E-02 -0.165 0.188 0.181 0.3000 1 . 207E+00 6 . 1 91 E-02 1 . 268E+00 1 .696E-01 2.753E-02 9.586E-02 -0.159 0.180 0.179

0.3500 1 . 1 53E+00 6 . 552E-02 1 .218E+00 2.099E-01 3.090E-02 1 . 1 30E-01 -0.153 0.179 0.168

0.0000 1 . 1 1 9E+00 6 . 965E-02 1 . 183E + 00 2.966E-01 3.908E-02 1 .300E-01 -0.199 0.169 0.162

0.0500 1 . 085E+00 7 . 381 E-02 1 . 159E+00 2.893E-01 3.71 IE-02 1 .968E-01 -0.195 0.169 0.158

0 . 5''00 1 .063E+00 7 . 803E-02 1 . 1 92E+00 3.328E-01 9 . OOOE-02 1 . 636E-01 -0.191 0.160 0.159

0.5500 1 . 097E+00 8 .230E-02 1 . 1 29E + 00 3.768E-01 9.278E-02 1 .803E-01 -0.137 0.156 0.150

0.6000 1 . 035E+00 8.662E-02 1 . 1 21 E+00 9.213E-01 9.597E-02 1 . 971 E-01 -0.139 0.153 0.197

0.7000 1 .017E+00 9 . 538E-02 1.11 3E+00 5. 109E-01 5.062E-02 2.309E-01 -0.128 0.197 0.191 0.8000 1 . 008E+00 1 .093E-01 1.11 2E+00 6 .008E-01 5.552E-02 2.637E-01 -0.123 0.192 0.135

0.9000 1 . 002E+00 1 . 1 39E-01 1 . 1 15E+00 6.906E-01 6.021E-02 2.970E-01 -0.118 0.138 0.131

1 .0000 9 . 995E-0 1 1 .226E-01 1 . 122E+00 7.800E-01 6.979E-02 3. 300E-01 -0.119 0.139 0.126

1 .2500 1 . OOOE+00 1 .965E-01 1 . 1 97E+00 1 .001 E+00 7.551E-02 9.116E-01 -0.105 0.126 0.117

1 .5000 1 . 007E+00 1.71 IE-01 1 . 178E+00 1 .216E+00 8.568E-02 9.907E-01 -0.098 0.119 0.109

1 .7500 1.01 5E+00 1 . 969E-01 1 .21 1E+00 1 .925E+00 9.591E-02 5.668E-01 -0.093 0.113 0.103

2.0000 1 . 029E+00 2.223E-01 1 .296E+00 1 .629E+00 1 .098E-01 6 .395E-01 -0.088 0.109 0.097

2 . 5000 1 . 092E+00 2 . 759E-0

1 .317E+00 2.01 9E+00 1 .226E-01 7.751E-01 -0.081 0.101 0.088

3.0000 1 . 059E+00 3.299E-01 1 .389E+00 2.389E+00 1 . 399E-01 8.987E-01 -0.076 0.095 0.081 3.5000 1 .079E+00 3.857E-01 1 .960E+00 2.790E+00 1 .559E-01 1 .012E+00 -0.072 0.090 0.075

9.0000 1 .088E+00 9.925E-01 1 .531E+00 3.079E+00 1 .705E-01 1 . 1 17E+00 -0.068 0.085 0.070

9 . 5000 1 . 1 0 1 E+00 5.001 E-01 1 .601E+00 3.393E+00 1 .850E-01 1 .219E+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 .790E+00 3.992E+00 2.121E-01 1 .391E+00 -0.060 0.076 0.059

6.0000 1 . 1 32E+00 6.779E-01 1 .81 OE+00 9.279E+00 2.298E-01 1 .972E+00 -0.058 0.073 0.056

7.0000 1 . 150E+00 7.985E-01 1 .998E+00 9.806E+00 2.988E-01 1 .622E+00 -0.055 0.069 0.051 8.0000 1 . 1 69E+00 9.215E-01 2.086E+00 5.302E+00 2.710E-01 1 .759E+00 -0.052 0.065 0.097

9.0000 1 . 1 77E+00 1 .096E+00 2.229E+00 5.767E+00 2.916E-01 1 .889E+00 -0.099 0.062 0.099

1 0 .0000 1 . 189E+00 1 . 172E+00 2.361E+00 6 .203E+00 3. 108E-01 2.000E+00 -0.097 0.060 0.091

1 2 . 5000 1.21 3E+00 1 .993E+00 2.706E+00 7. 1 91E+00 3.536E-01 2.256E+00 -0.093 0.059 0.035

15.0000 1 .232E+00 1 .81 9E+00 3.051 E+00 8.0S1E+00 3. 905E-01 2.977E+00 -0.090 0.051 0.031

1 7 .5000 1 .298E+00 2. 151E+00 3.399E+00 8.837E+00 9.226E-01 2.671E+00 -0.037 0.097 0.027

20.0000 1 .262E+00 2.986E+00 3.798E+00 9.537E+00 9.508E-01 2.895E+00 -0.039 0.095 0.025

25.0000 1 . 289E+00 3 . 1 67E+00 9.951E+00 1 .076E+01 9.989E-01 3. 198E+00 -0.031 0.091 0.021

30 .0000 1 . 301E+00 3.858E+00 5. 160E+00 1 . 180E+01 5.371E-01 3.907E+00 -0.027 0.038 0.018

35 .0000 1 . 31 6E+00 9 . 557E+00 5.873E+00 1 .271E+01 5.692E-01 3.639E+00 -0.025 0.036 0.016

90 .0000 1 . 328E+00 5.263E+00 6.590E+00 1 .351E+01 5.965E-01 3.837E+00 -0.023 0.039 0.019

95.0000 1 . 338E+00 5.973E+00 7 . 31 2E+00 1 .923E+01 6.200E-01 9.020E+00 -0.021 0.032 0.012

50.0000 1 . 397E+00 6 . 689E+00 8.036E+00 1 .989E+01 6.905E-01 9. 187E+00 -0.019 0.031 0.011

55 .0000 1 . 355E+00 7 .908E+00 8.763E+00 1 .598E+01 6 .586E-01 9.391E+00 -0.018 0.030 0.010

60 .0000 1 . 363E+00 8 . 1 30E+00 9.993E+00 1 .603E+01 6.796E-01 9.983E+00 -0.017 0.029 0.010

70.0000 1 .375E+00 9.583E+00 1 .096E+01 1 .701E+01 7.019E-01 9.790E+00 -0.015 0.028 0.008

80 .0000 1 . 386E+00 1 . 109E+01 1 .293E+01 1 .787E+01 7.299E-01 9.966E+00 -0.019 0.026 0.007

90 .0000 1 . 395E+00 1 . 251 E+01 1 .391E+01 1 .863E+01 7.933E-01 5.169E+00 -0.013 0.025 0.007

100.0000 1 . 903E+00 1 . 399E+01 1 .539E+01 1 .931E+01 7.599E-01 5.352E+00 -0.012 0.029 0.006

125.0000 1 .920E+00 1 . 769E+01 1 .91 1E+01 2.076E+01 7.911E-01 5.797E+00 -0.010 0.023 0.005

150.0000 1 .933E4-00 2. 191E+01 2.285E+01 2 . 1 96E+01 8. 195E-01 6 .076E+00 -0.008 0.022 0.009

175.0000 1 . 999E + 00 2.515E+01 2.659E+01 2.297E+01 8.327E-01 6.357E+00 -0.007 0.021 0.003

200 .0000 1 . 959E+00 2.889E+01 3.035E+01 2.385E+01 8.972E-01 6 .609E+00 -0.006 0.020 0.003

250 .0000 1 . 969E+00 3 . 690E+01 3.787E+01 2.532E+01 8.692E-01 7.022E+00 -0.005 0.019 0.002

300 .0000 1 .982E+00 9 . 393E+01 9.591E+01 2.653E+01 8.851 E-01 7.367E+00 -0.009 0.018 0.002

350.0000 1 . 992E+00 5. 196E+01 5.295E+01 2.755E+01 8. 972E-01 7.662E+00 -0.009 0.017 0.002

900 .0000 1 .501E+00 5.901E+01 6 .051 E+01 2.893E+01 9.067E-01 7.918E+00 -0.003 0.017 0.002

950 .0000 1 . 509E+00 6 . 656E+01 6 .807E+01 2 . 921 E+01 9. 195E-01 8. 195E+00 -0.003 0.016 0.001 500.0000 1 . 51 5E+00 7.912E+01 7.563E+01 2. 990E+01 9.209E-01 8 . 399E+00 -0.003 0.016 0.001 550.0000 1 . 522E+00 8 . 1 68E+01 8. 320E+01 3.053E+01 9.269E-01 8.539E+00 -0.003 0.016 0.001

600 . 0000 1 . 527E+00 8 . 925E+01 9 . 078E+0

3.111 E+01 9 . 31 OE-01 8.709E+00 -0.002 0.015 0.001

700 .0000 1 . 537E+00 1 . 099E+02 1 . 059E^02 3.21 3E+01 9.387E-01 9.005E+00 -0.002 0.015 0.001 800.0000 1 . 596E+00 1 . 1 96E+02 1.211 E+02 3.301E+01 9.996E-01 9 . 266E+00 -0.002 0.019 0.001

900 . 0000 1 . 553E+00 1 . 397E+02 1 . 363E+02 3. 379E+01 9.999E-01 9 . 997E+00 -0.002 0.019 0.001

1 000 .0000 1 .560E + 00 1 . 999E+02 1 .515E+02 3.998E+01 9.539E-01 9.705E+00 -0.001 0.019 0.001
ELECTRONS IN GOLD

I = 790.0 eV DENSITY = 1 .932E+01 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( logI )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 8 . 673E+00 2 . 036E-02 8 . 699E+00 7.917E-09 1 . 150E-03 6 .025E-09 -0 . 373 0.665 0.519

0.0125 7 . 562E+00 2 .237E-02 7.585E+00 1 . lOlE-03 1 .999E-03 7 .709E-09 -0.395 0.579 0.960

0.0150 6 . 739E+00 2 . 902E-02 6 .763E + 00 1 .950E-03 1 .799E-03 9.970E-09 -0.325 0.520 0.921 0.0175 6 . 1 03E+00 2.593E-02 6 . 1 28E + 00 1 .839E-03 2.050E-03 1 . 1 31 E-03 -0.310 0.976 0.392

0.0200 5 . 595E+00 2 . 666E-02 5 . 622E+00 2.266E-03 2. 399E-03 1 .323E-03 -0.298 0 .999 0.371

0 .0250 9 .832E+00 2 .872E-02 9 .861 E+00 3.226E-03 2.995E-03 1 .735E-03 -0.279 0.397 0.390

0.0300 9 . 289E+00 3 . 093E-02 9.315E+00 9.320E-03 3.539E-03 2. 183E-03 -0.266 0.365 0.319

0.0350 3 .870E+00 3 . 1 90E-02 3.902E+00 5.591E-03 9 . 1 1 7E-03 2.673E-03 -0.256 0.391 0.303

0 . O'tOO 3 . 595E+00 3.321E-02 3.579E+00 6 .880E-03 9.699E-03 3.208E-03 -0.298 0.329 0.291

0 . 0^50 3 . 283E+00 3 . 939E-02 3.318E+00 8.333E-03 5.269E-03 3.791E-03 -0.291 0.309 0.280 0.0500 3 . 067E+00 3 . 597E-02 3. 102E+00 9.893E-03 5.828E-03 9.927E-03 -0.235 0.298 0.272

0 .0550 2 .885E+00 3 . 697E-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 . 791 E-02 2.768E+00 1 .331E-02 6 . 936E-03 5.877E-03 -0.225 0.279 0.258

0.0700 2 . 980E+00 3 . 91 9E-02 2.51 9E+00 1 .71 lE-02 8.022E-03 7.597E-03 -0.217 0.266 0.298

0 . 0800 2 . 286E+00 9 . 070E-02 2.327E+00 2.129E-02 9.089E-03 9.629E-03 -0.211 0.255 0.239

0.0900 2 . 1 32E+00 9.219E-02 2 . 1 79E+00 2.569E-02 1 .012E-02 1 . 1 99E-02 -0.205 0.296 0.232

0.1000 2 . 006E+00 9 . 398E-02 2.099E+00 3.099E-02 1 . 1 19E-02 1 .971E-02 -0.200 0.239 0.226

0 . 1 250 1 . 773E+00 9 . 651 E-02 1.81 9E+00 9.393E-02 1 . 360E-02 2.288E-02 -0.189 0.229 0.213

0.1500 1 . 6 1 9E+00 9 . 920E-02 1 .663E+00 5.789E-02 1 .593E-02 3.231 E-02 -0.181 0.213 0.203

0.1750 1 . 999E+00 5 . 1 69E-02 1 . 550E+00 7 . 393E-02 1 .815E-02 9.212E-02 -0.179 0.209 0.196

0 . 2000 1 . 91 2E+00 5. 395E-02 1 .966E+00 9.009E-02 2. 027E-02 5. 187E-02 -0.169 0.197 0.189

0 .2500 1.291 E+00 5.833E-02 1 . 399E+00 1 .257E-01 2.923E-02 7.079E-02 -0.161 0.186 0.179

0.3000 1 . 21 2E+00 6.256E-02 1 .279E+00 1 .639E-01 2.789E-02 8.883E-02 -0.155 0.178 0.171

0 . 3500 1 . 1 57E+00 6 . 677E-02 1 .229E+00 2.090E-01 3.1 32E-02 1 .063E-01 -0.150 0.171 0.165

0.9000 1 . 1 1 8E+00 7 . 099E-02 1 . 189E+00 2.955E-01 3.955E-02 1 .239E-01 -0.195 0.166 0.160

0.9500 1 . 089E+00 7 . 529E-02 1 . 169E+00 2.880E-01 3.762E-02 1 .901E-01 -0.192 0.161 0.155

0.5000 1 . 067E+00 7 . 959E-02 1 .197E+00 3.313E-01 9.056E-02 1 .566E-01 -0.138 0.157 0.151 0.5500 1 . 051 E+00 8 . 389E-02 1 . 1 35E+00 3.751E-01 9.338E-02 1 .729E-01 -0.135 0.159 0.197

0.6000 1 .038E+00 8.828E-02 1 . 1 27E+00 9.199E-01 9.612E-02 1 .891 E-01 -0.132 0.150 0.199

0.7000 1 .021E+00 9.720E-02 1.11 9E+00 5.085E-01 5 . 1 39E-02 2.209E-01 -0.126 0.195 0.138

0 .8000 1.01 lE+00 1 .063E-01 1 . 1 18E+00 5. 980E-01 5.630E-02 2.529E-01 -0.122 0.190 0.133

0.9000 1 . 006E+00 1 . 1 55E-01 1 .122E+00 6.873E-01 6.105E-02 2.835E-01 -0.117 0.136 0.128

1 .0000 1 . 009E+00 1 .299E-01 1 . 1 29E+00 7.762E-01 6 .563E-02 3.193E-01 -0.113 0.132 0.129

1 .2500 1 . 005E+00 1 .991E-01 1 . 1 59E+00 9.959E-01 7.651E-02 3.903E-01 -0.105 0.129 0.115

1 . 5000 1.011 E+00 1 .791E-01 1 . 186E+00 1 .209E+00 8.678E-02 9.693E-01 -0.098 0.118 0.108

1 . 7500 1 . 020E+00 1 . 998E-01 1 .220E+00 1 .917E+00 9.658E-02 5.361E-01 -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 . 098E+00 2.799E-01 1 .327E+00 2.006E+00 1 .239E-01 7.359E-01 -0.081 0.100 0.087

3.0000 1 . 065E+00 3. 352E-01 1 .900E+00 2. 373E+00 1 .908E-01 8.551E-01 -0.075 0.099 0.080

3 . 5000 1 .080E+00 3.917E-01 1 .972E+00 2.721E+00 1 .568E-01 9.655E-01 -0.071 0.089 0.079

9.0000 1 . 095E+00 9.992E-01 1 .599E+00 3.053E+00 1 .721E-01 1 .068E+00 -0.067 0.089 0.069

9.5000 1 . 1 07E + 00 5.077E-01 1 .615E+00 3.370E+00 1 .866E-01 1 .163E+00 -0.069 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 9.292E+00 2.265E-01 1 .917E+00 -0.057 0.072 0.055

7.0000 1 . 1 57E+00 8.098E-01 1 . 967E+00 9.770E+00 2.505E-01 1 .565E+00 -0.059 0.068 0.050

8.0000 1 . 1 72E+00 9.393E-01 2.106E+00 5.261E+00 2.727E-01 1 .699E+00 -0.051 0.065 0.096

9 .0000 1 . 185E + 00 1 .061 E + 00 2.295E+00 5.721E+00 2.933E-01 1 .823E+00 -0.098 0.062 0.093

1 0 .0000 1 . 1 96E+00 1 . 188E+00 2.385E+00 6.153E+00 3.125E-01 1 .937E+00 -0.096 0.059 0.090

12.5000 1 . 221 E+00 1 .513E+00 2.733E+00 7.132E+00 3.559E-01 2.1 91E+00 -0.092 0.059 0.039

15.0000 1 .290E+00 1 .893E+00 3.083E+00 7.992E+00 3. 922E-01 2.909E+00 -0.039 0.050 0.030

17.5000 1 .256E+00 2.179E+00 3.935E+00 8.760E+00 9.293E-01 2.602E+00 -0.036 0.097 0.027

20 .0000 1 .270E+00 2.518E+00 3.788E+00 9.953E+00 9.525E-01 2.775E+00 -0.039 0.099 0.029

25.0000 1 .292E+00 3.207E+00 9.500E+00 1 .066E+01 5.000E-01 3.075E+00 -0.030 0.090 0.020

30.0000 1 .310E+00 3.907E+00 5.217E+00 1 . 169E+01 5.386E-01 3.331E+00 -0.027 0.037 0.018

35.0000 1 . 325E+00 9 .61 5E+00 5.939E+00 1 .259E+01 5.707E-01 3.556E+00 -0.025 0.035 0.015

90 .0000 1 . 337E+00 5 . 329E+00 6 .666E+00 1 . 339E+01 5.979E-01 3.757E+00 -0.022 0.033 0.019

95.0000 1 . 397E+00 6 . 099E+00 7.396E+00 1 .91 OE+01 6.219E-01 3. 939E+00 -0.021 0.032 0.012

50.0000 1 . 356E+00 6 . 772E+00 8 . 1 29E+00 1 .979E+01 6.918E-01 9.105E+00 -0.019 0.031 0.011

55 .0000 1 . 365E+00 7 . 500E+00 8.865E+00 1 .533E+01 6 .598E-01 9.257E+00 -0.018 0.030 0.010

60 .0000 1 . 372E+00 8 . 232E+00 9.609E+00 1 .587E+01 6 .758E-01 9.399E+00 -0.017 0.029 0.009

70.0000 1 . 385E+00 9 . 702E+00 1 . 1 09E+01 1 .689E+01 7.031E-01 9.653E+00 -0.015 0.027 0.008

80.0000 1 . 395E+00 1 . 1 18E+01 1 .258E+01 1 .769E+01 7 .255E-01 9.878E+00 -0.019 0.026 0.007

90 .0000 1 . 905E+00 1 .267E+01 1 .907E+01 1 .899E+01 7 .993E-01 5.080E+00 -0.013 0.025 0.006

100.0000 1.91 3E+00 1 .916E+01 1 . 557E+01 1.911 E+01 7.603E-01 5.262E+00 -0.012 0.029 0 .006 125.0000 1 . 930E+00 1.791 E+01 1 . 939E+01 2.055E+01 7.91 9E-01 5.656E+00 -0.010 0.023 0.005

150.0000 1 . 993E+00 2. 168E+01 2.312E+01 2. 173E+01 8 . 1 53E-01 5.983E+00 -0.008 0.021 0.009

175.0000 1 . 955E+00 2.596E+01 2.692E+01 2.273E+01 8.339E-01 6.269E+00 -0.007 0 .020 0.003

200 .0000 1 .969E+00 2 . 925E+01 3.072E+01 2.360E+01 8 . 979E-01 6 . 51 OE+00 -0.007 0.020 0.003

250 .0000 1 . 980E+00 3.685E+01 3.833E+01 2 . 506E+01 8 . 697E-01 6 . 926E+00 -0.005 0.019 0.002

300 . 0000 1 . 992E+00 9 . 997E + 01 9. 596E+01 2.625E+01 8.856E-01 7.271E+00 -0.009 0.018 0.002

350 .0000 1 . 503E+00 5.210E+01 5.360E+01 2.725E+01 8.976E-01 7 .569E+00 -0.009 0.017 0.002

900 .0000 1.511 E+00 5 . 979E+0

6 . I 25E+01 2.812E+01 9.071E-01 7 .820E + 00 -0.003 0.017 0.002

950.0000 1.51 9E+00 6 . 739E+01 6 .891 E+01 2 .889E+01 9. 198E-01 8.097E+00 -0.003 0.016 0.001

500 .0000 1 . 526E+00 7.509E+01 7.656E+01 2. 958E+01 9.21 3E-01 8.251E+00 -0.003 0.016 0.001 550.0000 1 . 532E+00 8.270E+01 8.923E+01 3 . 020E+01 9 . 267E-01 8.936E+00 -0.003 0.015 0.001 600.0000 1 . 538E+00 9.036E+01 9.190E+01 3.077E+01 9. 31 3E-01 8.605E+00 -0.002 0.015 0.001

700 .0000 1 . 598E+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 .210E+02 1 .226E+02 3 . 265E+01 9.999E-01 9. 167E+00 -0.002 0.019 0.001

900 .0000 1 . 569E+00 1 . 369E+02 1 . 380E+02 3 . 392E+01 9.997E-01 9.398E+00 -0.002 0.019 0.001 1000.0000 1 .571E+00 1 .518E+02 1 .533E+02 3.910E+01 9 . 536E-01 9.605E+00 -0.001 0.019 0.001

104
ELECTRONS IN LEAD

I = 823.0 eV DENSITY = 1 .135E+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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 8.928E+00 2.095E-02 8.998E+00 8.253E-09 1 .191E-03 9.891E-09 -0.379 0.713 0.539

0.0125 7.357E+00 2.251E-02 7.379E+00 1 . 193E-03 1 .500E-03 6. 197E-09 -0.350 0.615 0.975

0.0150 6.561E+00 2.921E-02 6.585E+00 1 .502E-03 1 .810E-03 7.991E-09 -0.329 0.599 0.932

0.0175 5.996E+00 2.566E-02 5.971E+00 1 .901E-03 2. 121E-03 8.872E-09 -0.319 0.501 0.902

0 .0200 5.953E+00 2.693E-02 5.980E+00 2.339E-03 2.932E-03 1 .029E-03 -0.301 0.969 0.379

0 .0250 9.719E+00 2 . 908E-02 9.793E+00 3.323E-03 3.051E-03 1 .329E-03 -0.283 0.913 0.397

0.0300 9. 182E+00 3 . 086E-02 9.21 3E+00 9.999E-03 3.669E-03 1 .633E-03 -0.269 0 . 378 0.329

0.0350 3.779E+00 3.290E-02 3.812E+00 5.699E-03 9.271E-03 1 .956E-03 -0.259 0.352 0.308

0 . 0<i00 3.963E+00 3.376E-02 3.997E+00 7.066E-03 9.872E-03 2.299E-03 -0.250 0.333 0.295

0 . 0'150 3 . 208E+00 3 . 500E-02 3.293E+00 8.552E-03 5.967E-03 2.696E-03 -0.293 0.317 0.289

0.0500 2 . 997E+00 3 .61 3E-02 3.039E+00 1 .015E-02 6.055E-03 3.01 lE-03 -0.238 0.305 0.276

0 .0550 2.821E+00 3.718E-02 2.858E+00 1 . 185E-02 6 .638E-03 3.390E-03 -0.232 0.299 0.268

0 .0600 2.670E+00 3.817E-02 2.708E+00 1 .365E-02 7.219E-03 3.783E-03 -0.228 0.285 0.262

0 .0700 2.926E+00 3 . 998E-02 2.966E+00 1 .752E-02 8.399E-03 9.608E-03 -0.220 0.271 0.251

0 .0800 2.237E+00 9.162E-02 2.279E+00 2. 175E-02 9.961E-03 5.985E-03 -0.219 0.260 0.292

0 .0900 2.087E+00 9.31 3E-02 2.130E+00 2.629E-02 1 .055E-02 6.913E-03 -0.209 0.251 0.235

0 . 1000 1 . 969E + 00 9.959E-02 2.008E+00 3.11 3E-02 1 . 162E-02 7.392E-03 -0.205 0.293 0.229

0 . 1250 1 .73BE+00 9.772E-02 1 .785E+00 9.938E-02 1 .91 9E-02 1 .005E-02 -0.196 0.229 0.217

0 . 1 500 1 . 583E + 00 5 . 059E-02 1 .633E+00 5.905E-02 1 .669E-02 1 .300E-02 -0.189 0.218 0.208

0.1750 1 .971 E + 00 5.312E-02 1 .529E+00 7.992E-02 1 .896E-02 1 .623E-02 -0.183 0.210 0.201

0 . 2000 1 . 387E+00 5.555E-02 1 .992E+00 9.180E-02 2. 1 18E-02 1 .971E-02 -0.178 0.203 0.195

0 . 2500 1 .269E+00 6.015E-02 1 .329E+00 1 .280E-01 2.533E-02 2.736E-02 -0.170 0.193 0.186

0 . 3000 1 . 1 93E+00 6 .960E-02 1 .257E+00 1 .668E-01 2.917E-02 3.579E-02 -0.163 0.185 0.178

0.3500 1 . 1 90E+00 6 . 900E-02 1 .209E+00 2.079E-01 3.276E-02 9.989E-02 -0.157 0.178 0.172

0.9000 1 . 1 02E+00 7 . 390E-02 1 . 175E+00 2.999E-01 3.619E-02 5.937E-02 -0.153 0.173 0.166

0.9500 1 .079E+00 7.781E-02 1 .152E+00 2.929E-01 3.935E-02 6.926E-02 -0.198 0.168 0.162

0 . 5000 1 .053E+00 8.228E-02 1 .135E+00 3.361E-01 9.291E-02 7.992E-02 -0.199 0.169 0.157

0 .5500 1 .037E+00 8.677E-02 1 . 129E+00 3.809E-01 9.536E-02 8.979E-02 -0.191 0.160 0.159

0.6000 1 .026E+00 9.132E-02 1 .117E+00 9.250E-01 9.820E-02 9.529E-02 -0.138 0.157 0.150

0.7000 1 .009E+00 1 .005E-01 1 . 1 lOE+00 5. 199E-01 5.363E-02 1 . 166E-01 -0.132 0.151 0.199

0 .8000 1 .OOOE+00 1 .098E-01 1 .1 lOE+00 6.050E-01 5.877E-02 1 .380E-01 -0.128 0.196 0.139

0 . 9000 9. 957E-01 1 . 1 93E-01 1 .115E+00 6.999E-01 6.369E-02 1 .595E-01 -0.129 0.192 0.139

1 .0000 9.939E-01 1 .290E-01 1 . 123E+00 7.893E-01 6.892E-02 1 .809E-01 -0.120 0.138 0.130

1 .2500 9.966E-01 1 .537E-01 1 . 150E+00 1 .009E+00 7.960E-02 2.337E-01 -0.113 0.130 0.121

1 . 5000 1 . 009E+00 1 .792E-01 1 . 183E+00 1 .21 9E+00 9.009E-02 2.859E-01 -0.107 0.129 0.119

1 .7500 1 .019E+00 2.053E-01 1 .21 9E+00 1 .927E+00 1 .OOlE-01 3.360E-01 -0.102 0.118 0.108

2.0000 1 .029E+00 2.31 9E-01 1 .256E+00 1 .629E+00 1 .096E-01 3.855E-01 -0.097 0.119 0.103

2.5000 1 . 099E+00 2.866E-01 1 .331E+00 2.016E+00 1 .277E-01 9.817E-01 -0.089 0.106 0.099

3.0000 1 .063E+00 3.927E-01 1 -906E+00 2.381E+00 1 .997E-01 5.793E-01 -0.083 0.100 0.086

3 . 5000 1 .080E+00 3.999E-01 1 .980E+00 2.728E+00 1 .608E-01 6.631E-01 -0.078 0.095 0.080

9 .0000 1 .095E+00 9.582E-01 1 .553E+00 3.057E+00 1 .761E-01 7.979E-01 -0.073 0.091 0.075

9.5000 1 . 1 08E+00 5.179E-01 1 .626E+00 3.372E+00 1 .906E-01 8.289E-01 -0.070 0.087 0.070

5 .0000 1 . 1 20E+00 5.773E-01 1 .698E+00 3.673E+00 2.095E-01 9.061E-OI -0.067 0.083 0.066

5 . 5000 1 . 1 32E+00 6 . 379E-01 1 .769E+00 3.962E+00 2. 177E-01 9.798E-01 -0.069 0.080 0.063

6.0000 1 . 1 92E+00 6 . 991 E-01 1 .891 E+00 9.239E+00 2.309E-01 1 .050E+00 -0.061 0.078 0.060

7.0000 1 . 1 60E+00 8.233E-01 1 . 983E+00 9.762E+00 2.593E-01 1 . 182E+00 -0.057 0.073 0.059

8.0000 1 . 1 75E+00 9.995E-01 2. 125E+00 5.299E+00 2.765E-01 1 .309E+00 -0.059 0.069 0.050

9.0000 1 . 189E+00 1 .077E+00 2.266E+00 5.705E+00 2.970E-01 1 .917E+00 -0.051 0.066 0.096

1 0 .0000 1 .201E+00 1 .206E+00 2.907E+00 6.133E+00 3. 162E-01 1 .523E+00 -0.099 0.063 0.093

1 2 . 5000 1 .225E+00 1 .535E+00 2.761E+00 7.102E+00 3.589E-01 1 .759E+00 -0.099 0.058 0.037

15.0000 1 . 296E+00 1 .870E+00 3. 1 16E+00 7.959E+00 3.955E-01 1 .969E+00 -0.091 0.053 0.032

1 7 . 5000 1 .262E+00 2.210E+00 3.972E+00 8.71 3E+00 9.279E-01 2. 197E+00 -0.038 0.050 0.029

20 .0000 1 .277E+00 2.559E+00 3.830E+00 9.399E+00 9.555E-01 2.310E+00 -0.036 0.097 0.026

25.0000 1 . 299E+00 3.252E+00 9.551E+00 1 .059E+01 5.028E-01 2.596E+00 -0.032 0.093 0.022

30.0000 1 . 318E+00 3.961E+00 5.278E+00 1 . 161E+01 5.912E-01 2.891E+00 -0.029 0.090 0.019

35.0000 1 . 332E+00 9.678E+00 6.01 1E+00 1 .250E+01 5.731E-01 3.055E+00 -0.027 0.038 0.016

90.0000 1 . 395E+00 5.902E+00 6.797E+00 1 .329E+01 6.002E-01 3.297E+00 -0.025 0.036 0.015

95.0000 1 . 356E+00 6.132E+00 7.988E+00 1 .399E+01 6.235E-01 3.920E+00 -0.023 0.039 0.013

50 .0000 1 . 365E+00 6 .865E+00 8.231E+00 1 .963E+01 6.939E-01 3.579E+00 -0.021 0.033 0.012

55.0000 1 . 379E+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 .381E+00 8.395E+00 9.726E+00 1 .579E+01 6.777E-01 3.861E+00 -0.019 0.031 0.010

70.0000 1 .395E+00 9.836E+00 1 .123E+01 1 .670E+01 7.098E-01 9. 107E+00 -0.017 0.029 0.009

80.0000 1 .906E+00 1 . 1 39E+01 1 .279E+01 1 .753E+01 7.270E-01 9.326E+00 -0.015 0.028 0.008

90 .0000 1 .915E+00 1 .289E+01 1 .926E+01 1 .828E+01 7.957E-01 9.521E+00 -0.019 0.027 0.007

100.0000 1 .923E+00 1 .936E+01 1 .578E+01 1 .899E+01 7.617E-01 9.699E+00 -0.013 0.026 0.006

125.0000 1 .991E+00 1 .816E+01 1 . 960E+01 2.036E+01 7.931E-01 5.083E+00 -0.011 0.029 0.005

1 50.0000 1 .955E+00 2. 1 98E+01 2.399E+01 2. 153E+01 8.169E-01 5.909E+00 -0.010 0.023 0.009

175.0000 1 . 966E+00 2.582E+01 2.729E+01 2.251E+01 8.393E-01 5.679E+00 -0.009 0.022 0.009

200.0000 1 .976E*00 2. 966E+01 3. 1 19E+01 2.337E+01 8.988E-01 5.921E+00 -0.008 0.021 0.003

250 .0000 1 . 991 E+00 3.737E+01 3.886E+01 2.980E+01 8.705E-01 6.330E+00 -0.006 0.020 0.003

300.0000 1 . 509E+00 9 . 509E+01 9.660E+01 2.598E+01 8.862E-01 6.670E+00 -0.005 0.019 0.002

350 .0000 1 . 51 9E+00 5.283E+01 5.935E+01 2.697E+01 8.982E-01 6.960E+00 -0.005 0.018 0.002

900 .0000 1 . 523E+00 6 . 058E+01 6.210E+01 2.783E+01 9.077E-01 7.213E+00 -0.009 0.018 0.002

950 .0000 1 . 531 E+00 6 .833E+01 6.986E+01 2.859E+01 9. 153E-01 7.938E+00 -0.009 0.017 0.001

500 .0000 1 . 538E+00 7.609E+01 7.763E+01 2. 927E+01 9.217E-01 7.690E+00 -0.003 0.017 0.001

550 .0000 1 .599E+00 8.386E+01 8.590E+01 2. 988E+01 9.271E-01 7.829E+00 -0.003 0.017 0.001 600.0000 1 . 550E+00 9. 163E+01 9.318E+01 3.099E+01 9. 317E-01 7.992E+00 -0.003 0.016 0.001

700 .0000 1 . 560E+00 1 .072E+02 1 .087E+02 3. 193E+01 9.393E-01 8.290E+00 -0.002 0.016 0.001

800 .0000 1 . 568E+00 1 .227E+02 1 .293E+02 3.229E+01 9.952E-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

1 000.0000 1 .583E+00 1 .539E+02 1 . 555E+02 3. 373E+01 9.539E-01 8. 986E+00 -0.002 0.015 0.001
ERGY

eV0)00 0125

0150

0 175 0200

0250

0300

0350

0<100 0^50

0500

0550

0600

0700 0800

0 900 1000

1 250

1 500 1750 2000

2500

3000

3500 9000 9500

5000

5500 6000

7000 8000

9000

0000 2500

5000 7500

0000

5000

0000 5000

0000

5000 0000

5000 0000

0000

0000

0000

0000

5000

0000

5000 0000

0000

0000

0000 0000

.0000

.0000

.0000

.0000

.0000

.0000

.0000 .0000

,0000

.0000

.0000

.0000

.0000

.0000

.0000

.0000

.0000 .0000

.0000

.0000

.0000

.0000 .0000

. 0000

ELECTRONS IN URANIUM

I = 890.0 eV DENSITY

STOPPING POWER CSDA COLLISION RADIATIVE TOTAL RANGE

MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^

7 . 9S9E+00 2 . 1 01 E-02 8.005E+00 8. 979E-09

6 . 986E + 00 2 . 327E-02 7 . 009E+00 1 .233E-03

6 .291 E+00 2.516E-02 6.266E+00 1.611 E-03

5 . 662E+00 2.679E-02 5.688E+00 2 . 030E-03

5 . 1 98E+00 2.822E-02 5.226E+00 2.989E-03

9 . 999E + 00 3 . 067E-02 9.530E+00 3.520E-03

3 . 995E+00 3.273E-02 9.028E+00 9.699E-03

3.61 3E+00 3.952E-02 3.698E+00 6 .OOOE-03

3.31 3E+00 3.612E-02 3.399E+00 7.933E-03

3 . 070E + 00 3 . 756E-02 3. 108E+00 8. 989E-03

2 .870E + 00 3.888E-02 2. 909E+00 1 .065E-02

2.701 E+00 9.011 E-02 2.791E+00 1 .292E-02

2 . 557E + 00 9 . 1 27E-02 2.598E+00 1 .929E-02

2.325E+00 9 . 339E-02 2.368E+00 1 .833E-02

2 . 1 99E + 00 9.531E-02 2.190E+00 2.273E-02

2.001E+00 9.709E-02 2.098E+00 2.796E-02

1 . 833E+00 9.875E-02 1 .932E+00 3.299E-02

1 . 666E + 00 5.299E-02 1 .71 9E+00 9.626E-02

1 .518E+00 5.585E-02 1 .579E+00 6. 199E-02

1 .9) lE+00 5.899E-02 1 .970E+00 7.795E-02

1 . 33CC + C0 6. 189E-02 1 . 392E+00 9.599E-02

1 . 218E + 00 6.735E-02 1 .285E+00 1 .329E-01

1 . 1 99E + 00 7.263E-02 1 .217E+00 1 .730E-01

1 .093E+00 7.781E-02 1 .171E+00 2.199E-01

1 .057E + 00 8.299E-02 1 . 190E+00 2.582E-01

1 . 031 E + 00 8.805E-02 1.11 9E+00 3.025E-01

1.011 E+00 9.316E-02 1 .109E+00 3.975E-01

9. 956E-01 9.828E-02 1 .099E+00 3.931E-01

9 .892E-01 1 .039E-01 1 .088E+00 9.389E-01

9.690E-01 1 . 1 37E-01 1 .083E+00 5.31 IE-01 9.609E-01 1 .291E-01 1 .089E+00 6 .239E-01 9.560E-01 1 .396E-01 1 .091E+00 7.159E-01

9.599E-01 1 .952E-01 1 .100E+00 8.068E-01

9.572E-01 1 .721E-01 1 .129E+00 1 .031E+00

9 . 699E-01 1 . 995E-01 1 .169E+00 1 .299E+00

9.799E-01 2.275E-01 1 .202E+00 1 .961E+00

9.899E-01 2.559E-01 1 .290E+00 1 .665E+00

1 . 009E+00 3.1 39E-01 1 .318E + 00 2.056E+00

1 .022E+00 3.732E-01 1 .396E+00 2.925E+00

1 .039E+00 9 . 338E-01 1 .973E+00 2.779E+00

1 . 059E+00 9. 955E-01 1 .599E+00 3. 105E+00

1 . 067E+00 5.580E-01 1 .625E+00 3.920E+00

1 . 079E+00 6 .21 9E-01 1 .700E+00 3.721E+00

1 . 090E+00 6 .856E-01 1 .775E+00 9.008E+00

1 . 1 OOE+00 7.509E-01 1 .850E+00 9.289E+00

1 . 1 1 7E+00 8.818E-01 1 .999E+00 9.809E+00

1 . 1 32E+00 1 .01 5E+00 2. 197E+00 5.287E+00

1 . 195E+00 1 . 151E+00 2.296E+00 5.737E+00

1 . 1 57E+00 1 .288E+00 2.999E+00 6.159E+00

1 . 180E+00 1 .636E+00 2.816E+00 7.111E+00

1 . 1 99E+00 1 .991E+00 3.1 91E+00 7.995E+00

1 .21 5E+00 2.352E+00 3.567E+00 8.685E+00

1 . 228E+00 2.717E+00 3.995E+00 9.352E+00

1 .250E+00 3.957E+00 9.706E+00 1 .051E+01

1 -266E+00 9.208E+00 5.979E+00 1 .199E+01

1 .280E+00 9.967E+00 6.298E+00 1 .235E+01

1 .292E+00 5.733E+00 7.025E+00 1 .310E+01

1 . 302E+00 6.505E+00 7.807E+00 1 . 378E+01

1.311 E+00 7.282E+00 8.593E+00 1 .939E+01

1.31 9E+00 8.063E+00 9.382E+00 1 .995E+01

1 . 326E+00 8.897E+00 1 .017E+01 1 .596E+01

1 . 338E+00 1 . 093E+01 1 . 176E+01 1 .637E+01

1 . 399E+00 1 .201E+01 1 .336E+01 1 .71 7E+01

1 . 357E+00 1 . 361 E + 01 1 .997E + 01 1 .787E+01

1 . 365E+00 1 .521E + 01 1 .658E + 01 1 .851 E+01

1 . 382E+00 1 . 929E + 01 2.062E+01 1 . 986E+01

1 . 395E+00 2.329E+01 2.969E+01 2.096E+01

1 . 905E+00 2.736E+01 2.877E+01 2. 1 90E+01

1 .919E+00 3. 199E + 01 3.286E+01 2.271E+01

1 . 929E+00 3 . 962E+0 1 9.105E+01 2.907E+01

1 . 99 1 E+00 9.782E+01 9. 926E+01 2.518E+01

1 . 951 E+00 5 . 609E + 01 5.799E+01 2.612E+01

1 . 960E+00 6 . 926E + 0 1 6.572E+01 2.693E+01

1 . 967E+00 7 . 250E + 01 7.397E+01 2.765E+01

1 . 979E+00 8.079E+01 8.221E+01 2.829E+01

1 . 980E+00 8 .899E+01 9.097E+01 2.887E+01

1 .986E+00 9 . 729E+01 9.872E+01 2. 990E+01

1 . 995E+00 1 . 1 37E+02 1 . 1 52E+02 3.039E+01

1 . 503E+00 1 . 303E+02 1 .318E+02 3. 1 15E+01

1 .51 1E+00 1 . 968E+02 1 .983E+02 3. 186E+01

1 . 51 7E+00 1 .633E+02 1 .698E+02 3.250E+01

.10 6

= 1 .895E+01 g/cm3

RADIATION DENS.EFF. dClog )/d(logI) YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

1 .292E-03 1 .810E-03 -0 . 391 0.898 0.589

1 .628E-03 2.329E-03 -0.360 0.719 0.510

1 . 968E-03 2.863E-03 -0.338 0.631 0.959

2.310E-03 3.923E-03 -0.321 0.569 0.929

2.653E-03 9.006E-03 -0.308 0.521 0.397

3.390E-03 5.231 E-03 -0.289 0.955 0.360

9.025E-03 6.526E-03 -0.279 0.911 0.335

9.707E-03 7 .882E-03 -0.263 0.380 0.317

5.389E-03 9.289E-03 -0.259 0.356 0.302

6 .056E-03 1 .079E-02 -0.297 0.337 0.291

6 .729E-03 1 .222E-02 -0.291 0.322 0.281 7.385E-03 1 .372E-02 -0.235 0.310 0.273

8.091E-03 1 .525E-02 -0.231 0.299 0.266

9.337E-03 1 .839E-02 -0.223 0.282 0.255

1 .061E-02 2. 197E-02 -0.216 0.269 0.296

1 . 186E-02 2.962E-02 -0.211 0.259 0.238

1 .308E-02 2.776E-02 -0.206 0.250 0.232

1 .605E-02 3.560E-02 -0.196 0.239 0.219

1 .888E-02 9.336E-02 -0.189 0.222 0.209

2.159E-02 5. 103E-02 -0.183 0.213 0.202

2.917E-02 5.860E-02 -0.178 0.206 0.195

2. 903E-02 7.399E-02 -0.170 0.199 0.185

3. 355E-02 8.799E-02 -0.169 0.186 0.178

3.777E-02 1 .021E-01 -0.158 0.179 0.171

9. 175E-02 1 .160E-01 -0.159 0.173 0.166

9.553E-02 1 .296E-01 -0.150 0.168 0.161 9.913E-02 1 .930E-01 -0.196 0.169 0.157

5.259E-02 1 .561E-01 -0.193 0.160 0.153

5.591E-02 1 .691E-01 -0.190 0.157 0.150

6.223E-02 1 .995E-01 -0.135 0.151 0.199

6.817E-02 2.1 92E-01 -0.130 0.196 0.138

7.382E-02 2.939E-01 -0.127 0.192 0.139

7.921E-02 2.672E-01 -0.123 0.138 0.130

9.189E-02 3.296E-01 -0.116 0.130 0.121

1 .035E-01 3.799E-01 -0.110 0.129 0.119

1 . 195E-01 9.332E-01 -0.109 0.119 0.108

1 .299E-01 9.897E-01 -0.100 0.119 0.103

1 .999E-01 5.832E-01 -0.092 0.107 0.099

1 .625E-01 6 .762E-01 -0.086 0.101 0.087

1 .795E-01 7.695E-01 -0.081 0.096 0.081

1 . 955E-01 8.988E-01 -0.076 0.091 0.076

2. 106E-01 9.299E-01 -0.073 0.087 0.071 2.250E-01 1 .007E+00 -0.069 0.089 0.067

2.387E-01 1 .081E+00 -0.066 0.081 0.069

2.518E-01 1 .152E+00 -0.063 0.078 0.060

2.769E-01 1 .287E+00 -0.058 0.079 0.055

2.990E-01 1 .912E+00 -0.059 0.070 0.050

3.199E-01 1 .529E+00 -0.051 0.066 0.096

3.399E-01 1 .639E+00 -0.098 0.063 0.093

3.825E-01 1 .886E+00 -0.093 0.058 0.036

9.1 93E-01 2.102E+00 -0.039 0.053 0.032

9.51 IE-01 2.299E+00 -0.036 0.050 0.028

9.790E-01 2.967E+00 -0.039 0.097 0.025

5.258E-01 2.768E+00 -0.030 0.093 0.021 5.636E-01 3.026E+00 -0.027 0.090 0.018

5.998E-01 3.252E+00 -0.029 0.038 0.015

6.212E-01 3.953E+00 -0.022 0.036 0.019

6.938E-01 3.635E+00 -0.021 0.039 0.012

6 .635E-01 3.802E+00 -0.019 0.033 0.011 6.808E-01 3.959E+00 -0.018 0.032 0.010

6.961E-01 9.096E+00 -0.017 0.031 0.009

7.221E-01 9.351E+00 -0.015 0.029 0.008

7.935E-01 9.577E+00 -0.013 0.028 0.007

7 .61 9E-01 9.779E+0O -0.012 0.027 0.006

7 . 766E-01 9.962E+00 -0.011 0 .026 0 .006 8.069E-01 5.357E+00 -0.010 0.029 0.005

8 .285E-01 5.685E+00 -0.008 0.023 0.009

8.955E-01 5. 966E+00 -0.007 0.022 0.003

8.591E-01 6 . 21 3E+00 -0.006 0.021 0.003

8.795E-01 6 . 630E+00 -0.005 0.020 0.002

8. 993E-01 6 . 975E+00 -0.009 0.019 0.002

9.055E-01 7.268E+00 -0.009 0.019 0.002

9.1 99E-01 7.525E+00 -0.003 0.018 0.001 9.215E-01 7 .752E+00 -0.003 0.017 0.001 9.275E-01 7. 956E+00 -0.003 0.017 0.001 9.325E-01 8.191E+00 -0.002 0.017 0.001 9.369E-01 8.310E+00 -0.002 0.016 0.001 9.939E-01 8.61 lE+00 -0.002 0.016 0.001 9.999E-01 8.872E+00 -0.002 0.016 0.001 9.538E-01 9. 103E+00 -0.002 0.015 0.001 9.575E-01 9.310E+00 -0.001 0.015 0.001
ELECTRONS IN A-150 TISSUE-EQUIVALENT PLASTIC

I = 65.1 eV DENSITY = 1 .127E+00 g/cm^

ENERGY STOPPING POWER CSDA RADIATION DEMS.EFF. d( log1 }/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MoV cm^/g MeV cm^/g g/cm^

0.0100 2.299E+01 3. 156E-03 2.295E+01 2.963E-09 7.529E-05 0.0 -0.193 0.220 0.219

0.0125 1 . 927E+01 3. 179E-03 1 .927E + 01 3.657E-09 9.098E-05 0.0 -0.186 0.210 0.209

0.0150 1 .671E+01 3. 188E-03 1 .671E+01 5.059E-09 1 .050E-09 0.0 -0.180 0.202 0.201 0.0175 1 .982E+01 3.197E-03 1 .982E+01 6.696E-09 1 .191E-09 0.0 -0.175 0.196 0.195

0.0200 1 . 335E+01 3.205E-03 1 .336E+01 8.926E-09 1 .327E-09 0.0 -0.171 0.191 0.190

0.0250 1 .129E+01 3.21 9E-03 1 . 129E+01 1 .253E-03 1 .588E-09 0.0 -0.165 0.183 0.183

0.0300 9.769E+00 3.232E-03 9.772E+00 1 .731E-03 1 .838E-09 0.0 -0.160 0.178 0.177

0.0350 8.691E+00 3.295E-03 8.699E+00 2.275E-03 2.079E-09 0.0 -0.156 0.173 0.173

0 .OAOO 7 .863E+00 3.258E-03 7.866E+00 2.880E-03 2.31 IE-09 0.0 -0.153 0.169 0.169

0 .0'(50 7.205E+00 3 .273E-03 7.209E+00 3.595E-03 2.537E-09 0.0 -0.151 0.166 0.166

0.0500 6.671E+00 3.287E-03 6.675E+00 9.267E-03 2.756E-09 0.0 -0.198 0.163 0.163

0.0550 6 .228E+00 3.302E-03 6.231E+00 5.093E-03 2.971E-09 0.0 -0.197 0.161 0.160

0.0600 5.853E+00 3.319E-03 5.857E+00 5.871E-03 3. 180E-09 0.0 -0.195 0.159 0.158

0 .0700 5.256E+00 3.352E-03 5.259E+00 7.677E-03 3.586E-09 0.0 -0.192 0.155 0.155

0 .0800 9 .800E+00 3.388E-03 9.803E+00 9.669E-03 3.977E-09 0.0 -0.139 0.152 0.152

0.0900 9.991E+00 3.927E-03 9.999E+00 1 . 189E-02 9.356E-09 0.0 -0.137 0.199 0.199

0 . 1 000 9 . 1 50E+00 3.967E-03 9.153E+00 1 .917E-02 9.723E-09 0.0 -0.135 0.197 0.197

0.1250 3 . 620E+00 3.578E-03 3.623E+00 2.069E-02 5.602E-09 0.0 -0.132 0.193 0.192

0.1500 3.262E+00 3 . 697E-03 3.265E+00 2.792E-02 6 .936E-09 0.0 -0.129 0.139 0.139

0.1750 3 . 005E+00 3.829E-03 3.009E+00 3.592E-02 7.239E-09 0.0 -0.126 0.137 0.136

0.2000 2.812E+00 3 . 959E-03 2.816E+00 9.952E-02 8.003E-09 0.0 -0.129 0.139 0.139

0 .2500 2 . 599E+00 9 . 297E-03 2.598E+00 6.325E-02 9.976E-09 0.0 -0.121 0.131 0.130

0.3000 2 . 369Et00 9 . 563E-03 2.373E+00 8.362E-02 1 .089E-03 0.0 -0.118 0.128 0.127

0.3500 2 . 297E-* 00 9 . 901 E-03 2.252E+00 1 .053E-01 1 .226E-03 0.0 -0.106 0.125 0.129

0.0000 2 . 1 56E+00 5 . 260E-03 2.161E+00 1 .280E-01 1 .361E-03 2. 969E-02 -0.088 0.120 0.118

0.0500 2 . 056E+00 5.639E-03 2.092E+00 1 .515E-01 1 .995E-03 6 .269E-02 -0.082 0.119 0.111 0.5000 2.033E+00 6 .036E-03 2.039E+00 1 .757E-01 1 .628E-03 9.751E-02 -0.077 0.109 0.106

0 .5500 1 . 991 E+00 6 . 998E-03 1 . 997E + 00 2.005E-01 1 .761E-03 1 .337E-01 -0.072 0.105 0.101 0.6000 1 . 957E+00 6 .875E-03 1 .969E + 00 2.258E-01 1 .895E-03 1 .708E-01 -0.068 0.101 0.096

0.7000 1 . 908E+00 7 .768E-03 1 . 91 5E+00 2.779E-01 2. 169E-03 2.969E-01 -0.061 0.099 0.088

0 .8000 1 . 879E+00 8.706E-03 1 .883E+00 3.300E-01 2.936E-03 3.223E-01 -0.056 0.089 0.082

0 . 9000 1 .851 E+00 9.687E-03 1 .860E+00 3.835E-01 2.71 IE-03 3.975E-01 -0.052 0.089 0.076

1 .0000 1 .839E+00 1 .071E-02 1 .895E+00 9.375E-01 2. 990E-03 9.712E-01 -0.099 0.080 0.071

1 .2500 1 .81 2E+00 1 .391E-02 1 .825E+00 5.739E-01 3.706E-03 6.972E-01 -0.093 0.072 0.062

1 . 5000 1 .803E+00 1 .630E-02 1 .81 9E+00 7.11 IE-01 9.997E-03 8. 100E-01 -0.039 0.066 0.056

1 .7500 1 .802E+00 1 .939E-02 1 .821E+00 8.985E-01 5.209E-03 9.601E-01 -0.036 0.061 0.051 2.0000 1 .809E+00 2.252E-02 1 .827E+00 9.856E-01 5. 992E-03 1 .099E+00 -0.039 0.057 0.097

2 . 5000 1 .81 9E + 00 2. 920E-02 1 .893E+00 1 .258E+00 7.609E-03 1 .396E+00 -0.031 0.052 0.091 3.0000 1 .827E+00 3 .625E-02 1 .863E+00 1 .528E+00 9.281E-03 1 .561E+00 -0.029 0.098 0.038

3.5000 1 .839E + 00 9.358E-02 1 .883E+00 1 .795E+00 1 .100E-02 1 .751E+00 -0.028 0.095 0.035

9 .0000 1 .852E+00 5.116E-02 1 . 903E+00 2.059E+00 1 .275E-02 1 .922E+00 -0.026 0.093 0.033

9.5000 1 .863E+00 5.896E-02 1 .922E+00 2.320E+00 1 .953E-02 2.077E+00 -0.025 0.091 0.031 5.0000 1 .879E+00 6 .695E-02 1 .991E+00 2.579E+00 1 .633E-02 2.218E+00 -0.029 0.039 0.030

5.5000 1 .889E+00 7.51 IE-02 1 . 959E+00 2.836E+00 1 .816E-02 2.399E+00 -0.029 0.038 0.029

6.0000 1 .899E+00 8.391E-02 1 .977E+00 3.090E+00 2.000E-02 2.970E+00 -0.023 0.036 0.027

7 .0000 1.911 E+00 1 .009E-01 2.01 1E+00 3.591E+00 2.372E-02 2.691E+00 -0.021 0.039 0.026

8 .0000 1 . 926E+00 1 . 179E-01 2.099E+00 9.089E+00 2.798E-02 2.887E+00 -0.020 0.032 0.029

9.0000 1 . 939E+00 1 .358E-01 2.075E+00 9.570E+00 3. 127E-02 3.069E+00 -0.018 0.031 0.023

1 0 .0000 1 -951E+00 1 .590E-01 2. 105E+00 5.098E+00 3.508E-02 3.227E+00 -0.017 0.029 0.021 12.5000 1 . 975E + 00 2.007E-01 2. 176E+00 6.216E+00 9.961 E-02 3.582E+00 -0.019 0.027 0.019

15.0000 1 . 995E + 00 2.988E-01 2.293E+00 7.398E+00 5.91 IE-02 3.885E+00 -0.011 0.029 0.016

1 7 . 5000 2.010E+00 2. 979E-01 2.308E+00 8.996E+00 6.352E-02 9.150E+00 -0.010 0.022 0.019

20.0000 2.029E+00 3.978E-01 2.372E+00 9.515E+00 7.282E-02 9.385E+00 -0.008 0.021 0.013

25.0000 2 . 096E+00 9.996E-01 2.995E+00 1 . 157E+01 9.097E-02 9.788E+00 -0.006 0.018 0.010

30 .0000 2.063E+00 5.532E-01 2.616E+00 1 .353E+01 1 .085E-01 5.126E+00 -0.009 0.016 0.008

35.0000 2.077E+00 6.582E-01 2.735E+00 1 .590E+01 1 .253E-01 5.917E+00 -0.003 0.019 0.007

90 .0000 2 . 089E+00 7.693E-01 2.859E+00 1 .718E+01 1 .919E-01 5.671E+00 -0.003 0.013 0.006

95.0000 2 . 1 OOE+00 8.719E-01 2.971E+00 1 .890E+01 1 .569E-01 5.897E+00 -0.002 0.012 0.005

50 .0000 2. 109E+00 9.792E-01 3.089E+00 2.055E+01 1 .717E-01 6.101E+00 -0.002 0.011 0.009

55.0000 2. 1 18E+00 1 .088E+00 3.205E+00 2.219E+01 1 .860E-01 6.286E+00 -0.002 0.011 0.009

60.0000 2. 125E+00 1 . 1 97E+00 3.322E+00 2.367E+01 1 .996E-01 6.956E+00 -0.001 0.010 0.003

70.0000 2. 1 39E+00 1 .916E+00 3.555E+00 2.658E+01 2.259E-01 6 .758E+00 -0.001 0.009 0.003

80 .0000 2. 151E+00 1 .638E+00 3.788E+00 2.931E+01 2.991E-01 7.020E+00 -0.001 0.008 0.002

90.0000 2. 161E+00 1 .860E+00 9.021 E+00 3. 187E+01 2.712E-01 7.253E+00 -0.001 0.008 0.002

100.0000 2. 170E+00 2.089E+00 9.259E+00 3.929E+01 2.917E-01 7 .961E+00 -0.001 0.007 0.002

125.0000 2. 189E+00 2 . 697E+00 9 .836E+00 3.979E+01 3.373E-01 7.903E+00 -0.000 0.006 0.001

1 50 .0000 2.209E+00 3.219E+00 5.918E+00 9.968E+01 3.763E-01 8.265E+00 -0.000 0.005 0.001 175.0000 2.218E+00 3.789E+00 6.002E+00 9.906E+01 9.100E-01 8.571E+00 -0.000 0.005 0.001 200.0000 2 . 229E+00 9 . 357E+00 6 .586E+00 5. 303E+01 9.396E-01 8.837E+00 -0.000 0.005 0.001 250.0000 2 . 298E+00 5.508E+00 7.756E+00 6.002E+01 9.891E-01 9.281E+00 -0.000 0.009 0.001

300 .0000 2.263E+00 6 . 665E+00 8.928E+00 6 .603E+01 5.291E-01 9.695E+00 -0.000 0.009 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

900 .0000 2.288E+00 8 . 990E+00 1 . 128E+01 7.597E+01 5.903E-01 1 .022E+01 -0.000 0.003 0.000

950 .0000 2.298E+00 1 .016E+01 1 .295E+01 8.01 9E+01 6.193E-01 1 .095E+01 -0.000 0.003 0.000

500.0000 2 . 307E + 00 1 . 1 32E+01 1 . 363E+01 8.902E+01 6.352E-01 1 .066E+01 -0.000 0.003 0.000

550.0000 2.315E+00 1 .299E+01 1 .981 E+01 8.759E+01 6.536E-01 1 .085E+01 -0.000 0.003 0.000

600 .0000 2 . 322E+00 1 . 367E+01 1 .599E+01 9.079E+01 6.699E-01 1 . 103E+01 -0.000 0.003 0.000

700.0000 2 . 335E+00 1 .601E+01 1 .835E+01 9.662E+01 6 . 977E-01 1 . 1 39E+01 -0.000 0.003 0.000

800 .0000 2.396E+00 1 .836E+01 2.071E+01 1 .018E+02 7.209E-01 1 . 160E+01 -0.000 0.002 0.000

900.0000 2 . 356E+00 2.072E+01 2. 307E+01 1 .063E+02 7.396E-01 1 . 189E+01 -0.000 0.002 0.000

1000.0000 2. 365E+00 2. 307E+01 2.599E+01 1 . 109E+02 7.559E-01 1 .205E+01 -0.000 0.002 0.000
ELECTRONS IN ACETYLENE

I = 58.2 oV DENSITY = 1.097E-03 g/cm3 (20® C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. dClog1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2 . 296E+0

2. 982E-03 2.296E+01 2.955E-09 7. 193E-05 0.0 -0.189 0.219 0.213

0.0125 1 . 927E+01 2 . 992E-03 1 . 927E + 01 3.699E-09 8.568E-05 0.0 -0.182 0.205 0.209

0.0150 1 . 670E+02 . 999E-03 1 .670E + 01 5.097E-09 9. 932E-05 0.0 -0.176 0.198 0.197

0.0175 1 .980E+01 3.009E-03 1 .980E + 01 6 .691 E-09 1 . 125E-09 0.0 -0.171 0.192 0.191

0 .0200 1 .333E+01 3 .008E-03 1 .333E+01 8.923E-09 1 .252E-09 0.0 -0.168 0.187 0.187

0.0250 1 . 121E+01 3.01 7E-03 1 .121E+01 1 .253E-03 1 .997E-09 0.0 -0.162 0.180 0.179

0.0300 9 . 739E+00 3.027E-03 9.792E+00 1 .733E-03 1 .731E-09 0.0 -0.157 0.179 0.179

0.0350 8.661 E+00 3.037E-03 8.669E+00 2.279E-03 1 . 956E-09 0.0 -0.159 0.170 0.169

0.0900 7 .833E+00 3.098E-03 7.836E+00 2.886E-03 2.179E-09 0.0 -0.151 0.166 0.166

0.0950 7 . 1 76E+00 3.061E-03 7.179E+00 3.559E-03 2.385E-09 0.0 -0.198 0.163 0.163

0.0500 6 . 692E+00 3.079E-03 6 .695E + 00 9.279E-03 2.591E-09 0.0 -0.196 0.160 0.160

0.0550 6 . 1 99E+00 3.088E-03 6 .202E+00 5.058E-03 2.792E-09 0.0 -0.199 0.158 0.158

0.0600 5 .825E + 00 3. 103E-03 5.829E+00 5.890E-03 2.989E-09 0.0 -0.192 0.156 0.155

0.0700 5.229E+00 3. 1 35E-03 5.232E+00 7.705E-03 3.371E-09 0.0 -0.190 0.152 0.152

0 . 0800 9 .779E+00 3. 169E-03 9.777E+00 9.708E-03 3.739E-09 0.0 -0.137 0.199 0.199

0.0900 9.91 6E+00 3.206E-03 9.91 9E+00 1 . 189E-02 9.095E-09 0.0 -0.135 0.197 0.197

0.1000 9 . 1 26E+00 3.299E-03 9.129E+00 1 .923E-02 9.991E-09 0.0 -0.133 0.195 0.199

0.1250 3.597E+00 3. 350E-03 3.600E+00 2.079E-02 5.270E-09 0.0 -0.130 0.191 0.190

0.1500 3 . 290E+00 3.963E-03 3.299E+00 2.808E-02 6 .058E-09 0.0 -0.127 0.137 0.137

0.1750 2 . 989E+00 3.589E-03 2. 988E+00 3.612E-02 6.812E-09 0.0 -0.129 0.135 0.139

0.2000 2.792E+00 3.71 IE-03 2.796E+00 9.978E-02 7.590E-09 0.0 -0.122 0.132 0.132

0.2500 2.525E+00 3.985E-03 2.529E+00 6.365E-02 8.937E-09 0.0 -0.119 0.129 0.128

0.3000 2 . 351 E + 00 9 . 289E-03 2.355E+00 8.918E-02 1 .028E-03 0.0 -0.117 0.126 0.125

0.3500 2 . 229E+00 9.609E-03 2.239E+00 1 .060E-01 1 .158E-03 0.0 -0.119 0.129 0.123

0 .9000 2. 192E + 00 9 . 995E-03 2. 197E+00 1 .289E-01 1 .286E-03 0.0 -0.113 0.122 0.121 0.9500 2.076E+00 5.309E-03 2.082E+00 1 .525E-01 1 .91 3E-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-03 0.0 -0.110 0.119 0.117

0.5500 1 . 988E + 00 6.071E-03 1 .999E+00 2.017E-01 1 .669E-03 0.0 -0.108 0.118 0.116

0.6000 1 . 958E+00 6 .975E-03 1 .965E+00 2.270E-01 1 .790E-03 0.0 -0.107 0.116 0.115

0.7000 1.91 5E+00 7.322E-03 1 . 923E+00 2.785E-01 2.091E-03 0.0 -0.105 0.119 0.112

0 .8000 1 .888E + 00 8.212E-03 1 .897E+00 3.309E-01 2.295E-03 0.0 -0.103 0.113 0.110

0.9000 1 .871 E+00 9. 192E-03 1 .881E+00 3.838E-01 2.550E-03 0.0 -0.102 0.111 0.109

1 .0000 1 .861 E+00 1.01 lE-02 1 .871E+00 9.372E-01 2.808E-03 0.0 -0.100 0.110 0.107

1 . 2500 1 .853E+00 1 .267E-02 1 .865E+00 5.711E-01 3.966E-03 0.0 -0.097 0.107 0.109

1 .5000 1 .857E+00 1 .591E-02 1 .873E+00 7.099E-01 9.139E-03 0.0 -0.095 0.105 0.101

1 .7500 1 .868E+00 1 .830E-02 1 -886E + 00 8.380E-01 9.829E-03 0.0 -0.093 0.103 0.099

2.0000 1 .881 E+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+00 2.766E-02 1 .938E+00 1 .230E+00 6.973E-03 0.0 -0.089 0.099 0.099

3.0000 1 . 939E+00 3.935E-02 1 .979E+00 1 .986E+00 8.950E-03 0.0 -0.087 0.0 97 0.092

3.5000 1 . 967E+00 9 . 1 32E-02 2.008E+00 1 .737E+00 9. 955E-03 0.0 -0.085 0.095 0.090

9.0000 1 . 993E+00 9 .852E-02 2.091E+00 1 .989E+00 1 . 198E-02 0.0 -0.089 0.099 0.088

9.5000 2.017E+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 2.967E+00 1 .958E-02 0.0 -0.082 0.091 0.085

5.5000 2 . 059E+00 7 . 1 29E-02 2. 1 31 E+00 2.703E+00 1 .615E-02 0.0 -0.081 0.090 0.089

6.0000 2.078E+00 7.919E-02 2.158E+00 2. 936E+00 1 .773E-02 0.0 -0.080 0.089 0.083

7.0000 2.11 3E+00 9.539E-02 2.208E+00 3.399E+00 2.090E-02 0.0 -0.079 0.087 0.081 8.0000 2.199E+00 1 .120E-01 2.256E+00 3.892E+00 2.909E-02 0.0 -0.077 0.086 0.080

9.0000 2. 171E+00 1 .290E-01 2.300E+00 9.281E+00 2.729E-02 0.0 -0.076 0.089 0.078

1 0.0000 2 . 1 96E+00 1 .969E-01 2.392E+00 9.712E+00 3.099E-02 0.0 -0.075 0.083 0.077

12.5000 2.299E+00 1 . 909E-01 2.990E+00 5.757E+00 3.897E-02 0.0 -0.079 0.081 0.079

15.0000 2.293E+00 2. 367E-01 2.530E+00 6.763E+00 9.638E-02 0.0 -0.072 0.079 0.072

1 7 . 5000 2.330E+00 2.835E-01 2.619E+00 7.735E+00 5.91 9E-02 0.0 -0.071 0.077 0.070

20.0000 2.363E+00 3.31 lE-01 2.699E+00 8.677E+00 6.188E-02 2.929E-05 -0.069 0.075 0.068

25.0000 2.91 3E+00 9.282E-01 2.891E+00 1 .098E+01 7.689E-02 5.698E-02 -0.052 0.071 0.062

30.0000 2.998E+00 5.270E-01 2.975E+00 1 .220E+01 9. 192E-02 1 .676E-01 -0.092 0.067 0.055

35.0000 2.976E+00 6.271E-01 3.103E+00 1 .385E+01 1 .055E-01 2.951E-01 -0.036 0.063 0.099

90.0000 2 . 998E+00 7.289E-01 3.226E+00 1 .593E+01 1 .190E-01 9.299E-01 -0.032 0.059 0.099

95.0000 2.517E+00 8. 306E-01 3. 397E+00 1 .695E + 01 1 .321E-01 5.501E-01 -0.029 0.056 0.090

50.0000 2 . 533E+00 9.339E-01 3.966E+00 1 .892E+01 1 .998E-01 6 .699E-01 -0.027 0.053 0.036

55.0000 2 . 597E+00 1 .037E+00 3.589E+00 1 . 989E+01 1 .570E-01 7.833E-01 -0.025 0.050 0.039

60.0000 2 . 560E+00 1 . 191E+00 3.701E+00 2. 121E+01 1 .689E-01 8. 903E-01 -0.029 0.098 0.031

70 .0000 2.581E+00 1 . 351 E+00 3. 932E+00 2. 383E+01 1 .919E-01 1 .087E+00 -0.022 0.095 0.027

80.0000 2.600E+00 1 .562E+00 9. 162E+00 2.630E+01 2. 129E-01 1 .263E+00 -0.021 0.092 0.025

90.0000 2.616E+00 1 .779E+00 9.390E+00 2.869E+01 2.321E-01 1 .922E+00 -0.020 0.039 0.022

100.0000 2.630E+00 1 . 988E+00 9.618E+00 3.086E+01 2.507E-01 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 0.039 0.017

150.0000 2 . 683E+00 3 . 067E+00 5.750E+00 9.059E+01 3.289E-01 2. 192E+00 -0.017 0.031 0.015

175.0000 2 . 702E+00 3.61 1E+00 6.319E+00 9.969E+01 3.609E-01 2.369E+00 -0.016 0.029 0.013

200 .0000 2.71 9E+00 9 . 1 58E+00 6 .877E+00 9.898E+01 3.899E-01 2.569E+00 -0.015 0.027 0.012

250 .0000 2.796E+00 5.258E+00 8.003E+00 5.522E+01 9.379E-01 2.912E+00 -0.013 0.029 0.010

300 . 0000 2 . 767E+00 6 . 362E+00 9. 129E+00 6. 106E+01 9.779E-01 3.201E+00 -0.012 0.022 0.009

350 .0000 2 . 789E+00 7.971E+00 1 .026E+01 6.623E+01 5. 1 15E-01 3.959E+00 -0.010 0.021 0.008

900 .0000 2.799E+00 8 . 583E+00 1 .138E+01 7.085E+01 5.903E-01 3.679E+00 -0.009 0.020 0.007

950.0000 2.81 1E+00 9.697E+00 1 .251 E + 01 7.509E+01 5.653E-01 3.882E+00 -0.008 0.019 0.006

500.0000 2.822E+00 1 .081E+01 1 .369E+01 7.887E+01 5 .872E-01 9.067E+00 -0.007 0.018 0.005

550.0000 2.832E+00 1 . 1 93E+01 1 .976E + 01 8.239E+01 6 .066E-01 9.237E+00 -0.006 0.017 0.005

600.0000 2.890E+00 1 . 305E+01 1 .589E+01 8.566E+01 6.290E-01 9.395E+00 -0.005 0.016 0.009

700 .0000 2.855E+00 1 .529E+01 1 .815E+01 9.159E+01 6.537E-01 9.580E+00 -0.009 0.015 0.009

800.0000 2.867E+00 1 . 759E+0

2.090E+01 9.679E+01 6.785E-01 9.930E+00 -0.003 0.015 0.003

900 .0000 2.878E+00 1 . 978E+01 2.266E+01 1 .019E+02 6 . 993E-01 5. 159E+00 -0.003 0.019 0.003

1 000 .0000 2.887E+00 2.203E+01 2.992E+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. d( log1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2. 397E+01 3. 168E-03 2.397E+01 2.906E-09 7.396E-05 0.0 -0.192 0.218 0.217

0.0125 1 .971E+01 3. 189E-03 1 .971E + 01 3.579E-09 8.889E-05 0.0 -0.189 0.209 0.207

0.0150 1 .709E+01 3. 199E-03 1 .709E+01 9. 990E-09 1 .031 E-09 0.0 -0.179 0.201 0.200

0.0175 1 .515E+01 3.201 E-03 1 .51 5E+01 6 .997E-09 1 . 168E-09 0.0 -0.179 0.195 0.199

0 .0200 1 . 365E+01 3 . 207E-03 1 .365E+01 8.237E-09 1 .301E-09 0.0 -0.170 0.190 0.189

0.0250 1 . 198E+01 3.217E-03 1 . 199E+01 1 .225E-03 1 .556E-09 0.0 -0.169 0.182 0.182

0.0300 9 . 989E+00 3.227E-03 9.987E+00 1 .693E-03 1 .800E-09 0.0 -0.159 0.177 0.176

0.0350 8.881E+00 3.238E-03 8.889E+00 2.225E-03 2.039E-09 0.0 -0.156 0.172 0.172

0,0000 8 . 039E+00 3.299E-03 8.037E+00 2.818E-03 2.260E-09 0.0 -0.153 0.168 0.168

0.0050 7 . 362E+00 3.262E-03 7.365E+00 3.968E-03 2.980E-09 0.0 -0.150 0.165 0.165

0.0500 6 . 81 6E+00 3.275E-03 6 .81 9E+00 9.175E-03 2.693E-09 0.0 -0.198 0.162 0.162

0.0550 6 . 362EJ-00 3.290E-03 6.365E+00 9.939E-03 2.902E-09 0.0 -0.196 0.160 0.160

0.0600 5 . 979E+00 3. 305E-03 5.983E+00 5.795E-03 3. 106E-09 0.0 -0.199 0.158 0.158

0,0700 5 . 369E+00 3 . 338E-03 5.372E+00 7.513E-03 3.501E-09 0.0 -0.191 0.159 0.159

0 . 0800 9 . 903E+00 3.373E-03 9.906E+00 9.969E-03 3.881 E-09 0.0 -0.139 0.151 0.151

0 .0 900 9 . 535E + 00 3.91 IE-03 9.539E+00 1 . 159E-02 9.250E-09 0.0 -0.137 0.199 0.198

0.1000 9 . 238E+00 3.952E-03 9.291E+00 1 .387E-02 9.608E-09 0.0 -0.135 0.197 0.196

0 . 1250 3.696E+00 3.562E-03 3.700E+00 2.020E-02 5.969E-09 0.0 -0.131 0.192 0.192

0.1500 3 . 330E+00 3 . 681 E-03 3.339E+00 2.739E-02 6.277E-09 0.0 -0.128 0.139 0.138

0.1750 3 . 068E + 00 3 .808E-03 3.071E+00 3.517E-02 7.055E-09 0.0 -0.126 0.136 0.136

0.2000 2.871E+00 3. 993E-03 2.875E+00 9.359E-02 7.806E-09 0.0 -0.129 0.139 0.133

0.2500 2.597E+00 9.232E-03 2.601E+00 6.199E-02 9.299E-09 0.0 -0.120 0.130 0.130

0 . 3000 2.918E+00 9 . 597E-03 2.922E+00 8.1 90E-02 1 .062E-03 0.0 -0.118 0.127 0.127

0.3500 2.299E+00 9.885E-03 2.299E+00 1 .031E-01 1 . 1 96E-03 0.0 -0.116 0.125 0.129

0.9000 2.209E+00 5.299E-03 2.209E+00 1 .253E-01 1 .328E-03 0.0 -0.115 0.123 0.122

0.9500 2 . 1 35E + 00 5.623E-03 2.191E+00 1 .983E-01 1 .958E-03 1 .971E-02 -0.090 0.120 0.118

0 , 5000 2.081E+00 6 .020E-03 2.087E+00 1 .720E-01 1 .588E-03 9. 189E-02 -0.089 0.115 0.113

0.5500 2 . 039E + 00 6 .933E-03 2.095E+00 1 . 962E-01 1 .718E-03 7.191E-02 -0.078 0.111 0.107

0.6000 2.005E+00 6 .860E-03 2.011 E+00 2.209E-01 1 .898E-03 1 .028E-01 -0.079 0.107 0.103

0.7000 1 . 959E+00 7 .753E-03 1 . 962E+00 2.712E-01 2.109E-03 1 .691E-01 -0.066 0.100 0.099

0 .8000 1 . 921E+00 8.692E-03 1 . 929E+00 3.227E-01 2.379E-03 2.381E-01 -0.060 0.099 0.087

0 . 9000 1 .897E+00 9.679E-03 1 .907E+00 3.798E-01 2.692E-03 3.080E-01 -0.055 0.089 0.081 1.0000 1 .880E+00 1 .070E-02 1 .891E+00 9.275E-01 2.915E-03 3.776E-01 -0.051 0.089 0.076

1 .2500 1 .858E+00 1 .390E-02 1 .871E+00 5.605E-01 3.612E-03 5.971E-01 -0.099 0.075 0.066

1 .5000 1 .899E+00 1 .629E-02 1 .865E+00 6.999E-01 9.339E-03 7.067E-01 -0.039 0.069 0.058

1 ,7500 1 .898E + 00 1 . 939E-02 1 .867E+00 8.289E-01 5.078E-03 8.559E-01 -0.036 0.069 0.052

2.0000 1 .850E+00 2.252E-02 1 .873E+00 9.621E-01 5.892E-03 9.936E-01 -0.033 0.060 0.098

2 . 5000 1 .860E+00 2.921E-02 1 .889E+00 1 .228E+00 7.921E-03 1 .292E+00 -0.030 0.053 0.092

3.0000 1 .872E+00 3.626E-02 1 .908E+00 1 .991E+00 9.055E-03 1 .959E+00 -0.028 0.099 0.037

3.5000 1 .885E+00 9. 360E-02 1 .928E+00 1 .752E+00 1 .073E-02 1 .652E+00 -0.026 0.096 0.039

9.0000 1 .897E+00 5. 120E-02 1 .998E+00 2.010E+00 1 .295E-02 1 .825E+00 -0.025 0.093 0.032

9.5000 1 . 909E + 00 5. 901E-02 1 -968E+00 2.265E+00 1 .91 9E-02 1 . 981E+00 -0.029 0.091 0.030

5.0000 1 . 920E + 00 6 .701 E-02 1 . 987E+00 2.518E+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 .779E-02 2.257E+00 -0.022 0.037 0.027

6.0000 1 . 939E+00 8.350E-02 2.023E+00 3.017E+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 2.601E+00 -0.020 0.039 0.025

8 .0000 1 . 972E + 00 1 . 181E-01 2.090E+00 3. 990E+00 2.688E-02 2.798E+00 -0.019 0.032 0.023

9.0000 1 . 985E+00 1 .360E-01 2.I21E+00 9.965E+00 3.059E-02 2.976E+00 -0.018 0.030 0.022

1 0 .0000 1 . 997E+00 1 .592E-01 2. 151E+00 9.933E+00 3.932E-02 3. 137E+00 -0.017 0.029 0.021

1 2 . 5000 2.022E+00 2.010E-01 2.223E+00 6.076E+00 9.368E-02 3.991E+00 -0.019 0.026 0.018

15.0000 2.092E+00 2.992E-01 2.291E+00 7.183E+00 5.300E-02 3.790E+00 -0.012 0.029 0.016

17.5000 2.059E+00 2.989E-01 2.357E+00 8.259E+00 6.225E-02 9.050E+00 -0.010 0.022 0.015

20.0000 2.073E+00 3.985E-01 2.921E+00 9.305E+00 7.138E-02 9.282E+00 -0.009 0.021 0.013

25.0000 2.095E+00 9.505E-01 2.596E+00 1 .132E+01 8.923E-02 9.679E+00 -0.007 0.018 0.011 30.0000 2.11 3E+00 5.599E-01 2.668E+00 1 .329E+01 1 .065E-01 5.012E+00 -0.005 0.016 0.009

35.0000 2. 128E+00 6 .597E-01 2.788E+00 1 .507E+01 1 .230E-01 5.299E+00 -0.009 0.015 0.008

90.0000 2. 191E+00 7.661E-01 2.907E+00 1 .683E+01 1 .389E-01 5.551E+00 -0.003 0.013 0.007

95.0000 2. 152E+00 8.739E-01 3.025E+00 1 .851E+01 1 .592E-01 5.776E+00 -0.003 0.012 0.006

50.0000 2. 161E+00 9.81 5E-01 3. 193E+00 2.013E+01 1 .688E-01 5. 979E+00 -0.002 0.012 0.005

55.0000 2. 170E+00 1 -090E+00 3.260E+00 2. 170E+01 1 .829E-01 6.163E+00 -0.002 0.011 0.009

60.0000 2. 178E+00 1 .200E+00 3.377E+00 2.320E+01 1 . 969E-01 6.332E+00 -0.002 0.010 0.009

70.0000 2.1 92E+00 1 .920E+00 3.61 lE+00 2.607E+01 2.218E-01 6.632E+00 -0.001 0.009 0.003

80 .0000 2.203E+00 1 .692E+00 3.895E+00 2.875E+01 2.959E-01 6 .899E+00 -0.001 0.008 0.003

90 .0000 2.219E+00 1 .865E+00 9.079E+00 3. 127E+01 2.673E-01 7. 126E+00 -0.001 0.008 0.002

1 00 .0000 2.223E+00 2.089E+00 9.312E+00 3. 366E+01 2.877E-01 7.339E+00 -0.001 0.007 0.002

125.0000 2.292E+00 2.653E+00 9.896E+00 3. 910E+01 3.330E-01 7.775E+00 -0.000 0.006 0.001

1 50 .0000 2.258E+00 3 . 222E+00 5.980E+00 9 . 392E+01 3.718E-01 8. 137E+00 -0.000 0.006 0.001 175.0000 2.272E+00 3 . 799E+00 6 .065E+00 9 .825E+01 9.059E-01 8.999E+00 -0.000 0.005 0.001 200.0000 2.283E+00 9 . 368E+00 6 .651 E+00 5.219E+01 9.350E-01 8.709E+00 -0.000 0.005 0.001

250 .0000 2 . 302E+00 5 . 522E+00 7 .829E+00 5.911 E+01 9.895E-01 9. 159E+00 -0.000 0.009 0.001 300.0000 2. 318E100 6 . 682E+00 9.000E+00 6.507E+01 5.295E-01 9.518E+00 -0.000 0.009 0.001

350 .0000 2 331 E+00 7 .895E+00 1 .018E+01 7.029E+01 5.578E-01 9.825E+00 -0.000 0.009 0 .000 900.0000 2 . 393E^00 9 . 0 1 2E+00 1 . 1 36E+0

7.999E+01 5.859E-01 1 .009E+01 -0.000 0.003 0.000

950.0000 2 . 353E+00 1 .018E+01 1 .253E+0

7.91 3E+01 6 . 100E-01 1 .033E+01 -0.000 0.003 0.000

500 .0000 2 . 362E+00 1 . 1 35E^0

1 .371E+01 8 . 299E+06.31 IE-01 1 .059E+01 -0.000 0.003 0.000

550.0000 2 . 370E+00 1 .253E+01 1 .990E+0

8.693E+01 6 .996E-01 1 .073E+01 -0.000 0.003 0.000

600.0000 2. 378E+00 1 . 370E+01 1 .608E+01 8. 966E+01 6 .660E-01 1 .090E+01 -0.000 0.003 0.000

700.0000 2.391E+00 1 .605E+01 1 .899E+01 9. 597E+01 6 . 939E-01 1 .121E+01 -0.000 0.003 0.000

800 .0000 2.902E+00 1 .891 E+01 2.081E+01 1 .006E+02 7. 169E-01 1 .198E+01 -0.000 0.003 0.000

900.0000 2.913E+00 2.077E+01 2.318E+01 1 .051E+02 7.362E-01 1 . 171E+01 -0.000 0.002 0.000

1000.0000 2.922E+00 2.31 3E+01 2.555E+01 1 . 092E+02 7.526E-01 1 . 1 92E+01 -0.000 0.002 0.000
ELECTRONS IN AIR, DRY (NEAR SEA LEVEL)

I = 85.7 oV DENSITY = 1.205E-03 g/cm^ (20® C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. ddogi )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MoV cm^/g g/cm ^ 0.0100 1 . 975E+01 3.897E-03 1 . 976E + 01 2.883E-09 1 .082E-09 0.0 -0.209 0.235 0.233

0.0125 1 .663E + 01 3.921E-03 1 .663E + 01 9.269E-09 1 .299E-09 0.0 -0.195 0.223 0.222

0.0150 1 .995E+01 3 . 937E-03 1 .995E+01 5 .886E-09 1 .506E-09 0.0 -0.189 0.215 0.213

0.0175 1 .283E+01 3 . 996E-03 1 .283E+01 7 .726E-09 1 .706E-09 0.0 -0.189 0.208 0.207

0.0200 1 . 1 57E+01 3. 959E-03 1 .158E+01 9.781E-09 1 .898E-09 0.0 -0.179 0.202 0.201 0.0250 9.753E+00 3 . 966E-03 9.757E+00 1 .951E-03 2.267E-09 0.0 -0.173 0.199 0.193

0.0300 8.992E+00 3 . 976E-03 8.996E+00 2.001E-03 2.618E-09 0.0 -0.167 0.187 0.186

0.0350 7 .563E+00 3. 986E-03 7.567E+00 2.626E-03 2. 955E-09 0.0 -0.163 0.182 0.181 0.0^00 6 .898E+00 3. 998E-03 6 .852E+00 3. 322E-03 3.280E-09 0.0 -0.160 0.178 0.177

0 . 0^(50 6 . 281 E+00 9 .01 1 E-03 6.285E+00 9.085E-03 3.599E-09 0.0 -0.157 0.179 0.179

0.0500 5.81 9E+00 9.025E-03 5.823E+00 9.912E-03 3.900E-09 0.0 -0.155 0.171 0.171

0 .0550 5.935E+00 9.090E-03 5.939E+00 5.801E-03 9.1 97E-09 0.0 -0.153 0.168 0.168

0.0600 5.111E+00 9 .057E-03 5.115E+00 6 .750E-03 9.988E-09 0.0 -0.151 0.166 0.166

0.0700 9 .593E+00 9.093E-03 9.597E+00 8.817E-03 5.099E-09 0.0 -0.197 0.162 0.162

0 . 0800 9 . 1 98E+00 9 . 1 33E-03 9.202E+00 1.11 OE-02 5.590E-09 0.0 -0.195 0.159 0.158

0 .0900 3.886E+00 9. 175E-03 3.890E+00 1 .357E-02 6.112E-09 0.0 -0.192 0.156 0.156

0.1000 3 . 633E+00 9.222E-03 3.637E+00 1 .623E-02 6.618E-09 0.0 -0.190 0.153 0.153

0 . 1 250 3 . 1 72E+00 9.398E-03 3. 177E+00 2.362E-02 7.826E-09 0.0 -0.136 0.199 0.198

0.1500 2.861E+00 9.985E-03 2.865E+00 3.193E-02 8.968E-09 0.0 -0.133 0.195 0.195

0.1750 2.637E+00 9.633E-03 2.692E+00 9.103E-02 1 .006E-03 0.0 -0.131 0.192 0.192

0.2000 2 . 970E+00 9.789E-03 2.979E+00 5.082E-02 1 .11 IE-03 0.0 -0.128 0.190 0.139

0 .2500 2.236E+00 5. 126E-03 2.292E+00 7.212E-02 1 .31 lE-03 0.0 -0.125 0.136 0.135

0.3000 2 . 089E+00 5.995E-03 2.089E+00 9.527E-02 1 .502E-03 0.0 -0.122 0.133 0.132

0 .3500 1 . 978E+00 5 .890E-03 1 .989E+00 1 . 1 99E-01 1 .688E-03 0.0 -0.120 0.130 0.129

0 .9000 1 . 902E+00 6.311E-03 1 . 908E+00 1 .956E-01 1 .869E-03 0.0 -0.118 0.128 0.127

0.9500 1 .895E+00 6.757E-03 1 .852E+00 1 .722E-01 2.098E-03 0.0 -0.116 0.126 0.125

0.5000 1 .802E+00 7.223E-03 1 .809E+00 1 .995E-01 2.225E-03 0.0 -0.119 0.125 0.123

0.5500 1 .769E+00 7.708E-03 1 .776E+00 2.279E-01 2.901E-03 0.0 -0.113 0.123 0.122

0.6000 1 .793E+00 8.210E-03 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 .699E+00 3.722E-01 3.283E-03 0.0 -0.107 0.118 0.115

0.9000 1 . 669E+00 1 . 151E-02 1 .681E+00 9.315E-01 3.638E-03 0.0 -0.106 0.116 0.119

1 .0000 1 .661E+00 1 .271E-02 1 .679E+00 9.912E-01 3. 997E-03 0.0 -0.109 0.115 0.112

1 .2500 1 . 655E+00 1 .588E-02 1 .671 E+00 6.908E-01 9.906E-03 0.0 -0.101 0.112 0.108

1 .5000 1 .661 E+00 1 . 927E-02 1 .680E+00 7.900E-01 5.836E-03 0.0 -0.099 0.109 0.106

1 .7500 1 .672E+00 2.289E-02 1 .699E+00 9.382E-01 6.789E-03 0.0 -0.097 0.107 0.103

2.0000 1 .689E+00 2.656E-02 1 .71 lE+00 1 .085E+00 7.798E-03 0.0 -0.095 0.106 0.101 2.5000 1 .712E+00 3.937E-02 1 .797E+00 1 .379E+00 9.716E-03 0.0 -0.092 0.103 0.0 98 3.0000 1 . 790E+00 9.260E-02 1 .783E+00 1 .658E+00 1 . 173E-02 0.0 -0.090 0.100 0.095

3.5000 1 .766E+00 5.11 5E-02 1 .817E+00 1 .935E+00 1 .377E-02 0.0 -0.088 0.098 0.093

9.0000 1 . 790E+00 5. 999E-02 1 .850E+00 2.208E+00 1 .583E-02 0.0 -0.087 0.097 0.091 9.5000 1 .81 2E+00 6 . 908E-02 1 .882E+00 2.976E+00 1 .792E-02 0.0 -0.086 0.095 0.089

5.0000 1 .833E+00 7 .838E-02 1.911 E+00 2.790E+00 2.001E-02 0.0 -0.089 0.099 0.088

5.5000 1 .852E+00 8.787E-02 1 . 990E+00 2.999E+00 2.21 lE-02 0.0 -0.083 0.093 0.086

6 .0000 1 .870E+00 9.759E-02 1 .968E+00 3.255E+00 2.922E-02 0.0 -0.083 0.092 0.085

7.0000 1 . 902E+00 1 . 173E-01 2.020E+00 3.757E+00 2.895E-02 0.0 -0.081 0.090 0.083

8.0000 1 . 931 E+00 1 .376E-01 2.068E+00 9.296E+00 3.269E-02 0.0 -0.080 0.088 0.081 9.0000 1 . 956E+00 1 .589E-01 2. 1 15E+00 9.729E+00 3.692E-02 0.0 -0.079 0.087 0.080

1 0 .0000 1 . 979E+00 1 .795E-01 2.159E+00 5.1 92E+00 9.11 3E-02 0.0 -0.078 0.085 0.078

1 2 .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 2.069E+00 2.895E-01 2.359E+00 7.905E+00 6.181E-02 0.0 -0.079 0.080 0.072

17.5000 2. 109E+00 3.969E-01 2.951E+00 8.999E+00 7. 185E-02 0.0 -0.073 0.078 0.070

20.0000 2 . 1 39E+00 9.092E-01 2.539E+00 9.996E+00 8.167E-02 0.0 -0.072 0.076 0.068

25.0000 2. 185E+00 5.21 9E-01 2.707E+00 1 . 1 35E+01 1 .006E-01 0.0 -0.070 0.073 0.065

30.0000 2 . 226E+00 6 . 91 7E-01 2.868E+00 1 .315E+01 1 . 186E-01 7.636E-03 -0.062 0.071 0.062

35.0000 2 . 257E+00 7.630E-01 3.020E+00 1 .985E+01 1 .357E-01 5.989E-02 -0.052 0.068 0.057

90.0000 2.282E+00 8.855E-01 3.167E+00 1 .696E+01 1 .520E-01 1 .378E-01 -0.099 0.069 0.052

95.0000 2.302E+00 1 .009E+00 3.31 lE+00 1 .801E+01 1 .676E-01 2.266E-01 -0.039 0.061 0.098

50 .0000 2. 31 9E+00 1 . 1 33E+00 3.952E+00 1 . 998E+01 1 .825E-01 3.1 92E-01 -0.035 0.059 0.099

55.0000 2 . 339E+00 1 .258E+00 3.592E+00 2.090E+01 1 . 968E-01 9.120E-01 -0.032 0.056 0.090

60.0000 2.397E+00 1 .389E+00 3.731E+00 2.227E+01 2. 109E-01 5.029E-01 -0.030 0.059 0.037

70.0000 2. 369E+00 1 .637E + 00 9 . 006E+00 2.986E+01 2.361E-01 6.762E-01 -0.027 0.050 0.033

80.0000 2 . 387E+00 1 .892E+00 9.279E+00 2.727E+01 2.598E-01 8.365E-01 -0.025 0.097 0.029

90.0000 2.903E+00 2. 198E+00 9 .551 E+00 2.959E+01 2.818E-01 9.892E-01 -0.023 0.099 0.026

1 00 .0000 2 . 91 7E+00 2.905E+00 9.822E+00 3 . 1 67E+01 3.022E-01 1 . 120E+00 -0.022 0.092 0.029

125.0000 2.995E+00 3.053E+00 5.998E+00 3.652E+01 3.979E-01 1 .91 9E+00 -0.020 0.038 0.020

150.0000 2.968E+00 3.705E+00 6 . 173E+00 9.081E+01 3.859E-01 1 .670E+00 -0.019 0.035 0.017

175.0000 2.986E+00 9. 360E+00 6 .897E+00 9.965E+01 9. 1 92E-01 1 .887E+00 -0.018 0.032 0.015

200.0000 2 . 502E + 00 5.018E+00 7 . 520E+00 9.819E+01 9.989E-01 2.078E+00 -0.017 0.030 0.013

250 .0000 2 . 529E+00 6 . 390E+00 8 .868E+00 5.925E+01 9. 972E-01 2.903E+00 -0.016 0.028 0.011 300.0000 2 . 550E+00 7 . 667E+00 1 .022E+01 5 . 950E+01 5. 365E-01 2.675E+00 -0.015 0.026 0.009

350 .0000 2 . 567E+00 8 . 998E+00 1 . 1 57E+01 6.910E+01 5.691E-01 2.909E+00 -0.019 0.029 0.008

900.0000 2. 582E+00 1 . 033E+01 1 .292E+01 6.81 9E+01 5. 967E-01 3. 1 16E+00 -0.013 0.023 0.007

950.0000 2 . 595E+00 1 . 1 67E+01 1 .927E+01 7 . 187E+01 6.203E-01 3.302E+00 -0.012 0.022 0.007

500.0000 2 . 606E+00 1 . 301 E+01 1 .562E+01 7.522E+01 6 . 909E-01 3.972E+00 -0.011 0.021 0.006

550.0000 2.616E+00 1 .935E+01 1 .697E+01 7.829E+01 6 .589E-01 3.628E+00 -0.010 0.020 0.006

600 .0000 2 . 625E+00 1 . 569E + 01 1 .832E+01 8.1 12E+01 6.750E-01 3.772E+00 -0.010 0.019 0.005

700.0000 2. 691 E+00 1 .838E+01 2.1 02E+01 8.622E+01 7.022E-01 9.039E+00 -0.008 0.018 0.009

800.0000 2.653E+00 2. 107E+01 2. 372E+01 9.069E+01 7.297E-01 9.267E+00 -0.007 0.017 0.009

900.0000 2.669E+00 2. 376E+01 2.693E+01 9.968E+01 7.935E-01 9.977E+00 -0.006 0.017 0.009

1 000 .0000 2 . 679E+00 2 . 696E+01 2.91 3E+01 9.829E+01 7.595E-01 9.668E+00 -0.005 0.016 0.003
ELECTRONS IN ALUMINUM OXIDE

I = 165.2 eV DENSITY = 3.970E+00i g/cm^

ENERGY STOPPING POWER CSDA RADIATION DEHS.EFF. d( log[ )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^

0.0100 1 .731 E+01 5.680E-03 1 .732E+01 3.351E-06 1 .716E-06 0 .

-0.229 0.270 0.266 0.0125 1 .665E+01 5.569E-03 1 .666E + 01 6 . 927E-06 2 . 068E-06 0.0 -0.218 0 .255 0.251 0.0150 1 .278E+01 5.629E-03 1 .278E+01 6.758E-06 2 . 607E-06 0.0 -0.210 0.266 0.261 0.0175 1 . 138E+01 5.676E-03 1 . 138E+01 8.835E-06 2.736E-06 0.0 -0.203 0.235 0.232

0.0200 1 .029E+01 5.707E-03 1 .030E+01 1.11 5E-03 3.050E-06 0.0 -0.198 0.228 0.225

0.0250 8.709E+00 5.753E-03 8.71 5E+00 1 .665E-03 3.656E-06 0.0 -0.190 0.217 0.215

0.0300 7.605E+00 5.786E-03 7.61 lE+00 2.261E-03 6.231E-06 0.0 -0.186 0.208 0.207

0.0350 6.789E+00 5.81 2E-03 6.795E+00 2. 957E-03 6.781E-06 0.0 -0.179 0.202 0.201

0 .OAOO 6 . 1 60E+00 5.835E-03 6 . 165E+00 3.731E-03 5.310E-06 0.0 -0.175 0.197 0.195

0 .0A50 5.658E+00 5.856E-03 5.666E+00 6.578E-03 5.820E-06 0.0 -0.171 0.192 0.191 0.0500 5.269E+00 5.878E-03 5.255E+00 5.695E-03 6.315E-06 0.0 -0.169 0.189 0.188

0.0550 6.909E+00 5.899E-03 6.915E+00 6 .680E-03 6 . 795E-06 0.0 -0.166 0.185 0.186

0.0600 6.621E+00 5.921E-03 6.627E+00 7.529E-03 7.262E-06 0.0 -0.166 0.182 0.182

0.0700 6. 161E+00 5. 965E-03 6.167E+00 9.81 lE-03 8.162E-06 0.0 -0.160 0.178 0.177

0.0800 3.809E+00 6.016E-03 3.815E+00 1 .232E-02 9.023E-06 0.0 -0.157 0.176 0.173

0.0900 3.530E+00 6 .068E-03 3.536E+00 1 .505E-02 9.850E-06 0.0 -0.156 0.170 0.170

0.1000 3.305E+00 6 . 126E-03 3.31 1E+00 1 .797E-02 1 .065E-03 0.0 -0.152 0.167 0.167

0.1250 2.892E+00 6 .285E-03 2.898E+00 2.608E-02 1 .256E-03 0.0 -0.167 0.162 0.161 0.1500 2.61 3E+00 6.666E-03 2.61 9E+00 3.517E-02 1 .632E-03 0.0 -0.163 0.157 0.157

0 . 1750 2.612E+00 6.661E-03 2.61 9E+00 6.512E-02 1 .600E-03 0.0 -0.160 0.156 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 2.052E+00 7.330E-03 2.059E+00 7.902E-02 2.068E-03 1 .096E-03 -0.125 0.166 0.165

0 . 3000 1 . 91 2E+00 7.836E-03 1 .920E+00 1 .062E-01 2.360E-03 2.660E-02 -0.113 0.139 0.137

0.3500 1 .815E+00 8.376E-03 1 .823E+00 1 .310E-01 2.663E-03 6.961E-02 -0.107 0.133 0.131

0 .<*000 1 .766E+00 8.956E-03 1 .753E+00 1 .590E-01 2.91 9E-03 7.609E-02 -0.102 0.128 0.125

0 . A500 1 .691E+00 9.563E-03 1 .700E+00 1 .879E-01 3.191E-03 1 .036E-01 -0.097 0.123 0.120

0.5000 1 .650E+00 1 .020E-02 1 .660E+00 2.177E-01 3.660E-03 1 .316E-01 -0.096 0.119 0.116

0.5500 1 .618E+00 1 .086E-02 1 .629E+00 2.681E-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-01 -0.087 0.113 0.109

0.7000 1 .557E+00 1 .298E-02 1 .570E+00 3.621E-01 6.529E-03 2.655E-01 -0.082 0.108 0.103

0.8000 1 .533E+00 1 .669E-02 1 .567E+00 6.063E-01 5.066E-03 3.026E-01 -0.078 0.103 0.097

0.9000 1 .517E+00 1 .606E-02 1 .533E+00 6.712E-01 5.603E-03 3.589E-01 -0.076 0.099 0.093

1 .0000 1 .507E+00 1 .769E-02 1 .526E+00 5.367E-01 6.167E-03 6. 163E-01 -0.071 0.096 0.089

1 .2500 1 .696E+00 2.201E-02 1 .516E+00 7.01 3E-01 7.528E-03 5.679E-01 -0.066 0.089 0.081

1 .5000 1 .692E+00 2.662E-02 1 .51 9E+00 8.661E-01 8. 962E-03 6 .766E-01 -0.059 0.083 0.075

1 .7500 1 .695E+00 3.168E-02 1 .527E+00 1 .030E+00 1 .039E-02 7.938E-01 -0.056 0.079 0.070

2.0000 1 .501E+00 3.653E-02 1 .537E+00 1 .193E+00 1 . 186E-02 9.069E-01 -0.050 0.075 0.065

2.5000 1 .516E+00 6.716E-02 1 .561E+00 1 .516E+00 1 .688E-02 1 . 1 16E+00 -0.066 0.069 0.058

3.0000 1 .528E+00 5.829E-02 1 .586E+00 1 .836E+00 1 .798E-02 1 .306E+00 -0.060 0.066 0.053

3.5000 1 .561E+00 5.987E-02 1 .611E+00 2. 167E+00 2.113E-02 1 .679E+00 -0.036 0.060 0.068

<*.0000 1 .553E+00 8. 181E-02 1 .635E+00 2.655E+00 2.633E-02 1 .638E+00 -0.033 0.057 0.065

A.5000 1 .566E+00 9.607E-02 1 .658E+00 2.759E+00 2.756E-02 1 .785E + 00 -0.031 0.056 0.061 5.0000 1 .575E+00 1 .066E-01 1 .681E+00 3.058E+00 3.081E-02 1 .921E+00 -0.029 0.051 0.039

5.5000 1 .586E+00 1 . 1 96E-01 1 .706E+00 3.353E+00 3.608E-02 2.068E+00 -0.027 0.069 0.037

6.0000 1 .593E+00 1 .326E-01 1 .725E+00 3.665E+00 3.735E-02 2. 167E+00 -0.026 0.067 0.035

7.0000 1 .609E+00 1 .590E-01 1 .767E+00 6.218E+00 6.392E-02 2.386E+00 -0.026 0.066 0.031 8.0000 1 .622E+00 1 .862E-01 1 .808E+00 6.777E+00 5.069E-02 2.578E+00 -0.022 0.061 0.029

9.0000 1 .636E+00 2.160E-01 1 .868E+00 5.326E+00 5.706E-02 2.756E+00 -0.020 0.039 0.027

1 0 .0000 1 .665E+00 2.622E-01 1 .887E+00 5.859E+00 6.356E-02 2. 916E+00 -0.019 0.037 0.025

12.5000 1 .667E+00 3. 165E-01 1 .982E+00 7.152E+00 7.956E-02 3.263E+00 -0.017 0.033 0.021 15.0000 1 .685E+00 3.886E-01 2.076E+00 8.385E+00 9.516E-02 3.557E+00 -0.015 0.030 0.019

17.5000 1 .700E+00 6.662E-01 2.166E+00 9.565E+00 1 .103E-01 3.812E+00 -0.013 0.028 0.017

20.0000 1 .713E+00 5.609E-01 2.256E+00 1 .070E+01 1 .269E-01 6.038E+00 -0.012 0.026 0.015

25.0000 1 .736E+00 6.968E-01 2.631E+00 1 .283E+01 1 .527E-01 6.626E+00 -0.010 0.023 0.013

30.0000 1 .750E+00 8.552E-01 2.606E+00 1 .682E+01 1 .786E-01 6.767E+00 -0.008 0.021 0.011 35.0000 1 .766E+00 1 .015E+00 2.780E+00 1 .668E+01 2.026E-01 5.025E+00 -0.007 0.019 0.010

60.0000 1 .776E+00 1 .177E+00 2.953E+00 1 .862E+01 2.251E-01 5.269E+00 -0.006 0.018 0.008

65.0000 1 .786E+00 1 . 360E+00 3.126E+00 2.007E+01 2.661 E-01 5.687E+00 -0.005 0.016 0.008

50.0000 1 .795E+00 1 .506E+00 3.299E+00 2. 162E+01 2.657E-01 5.686E+00 -0.005 0.015 0.007

55.0000 1 .803E+00 1 .669E+00 3.672E+00 2.31 OE+01 2.862E-01 5.866E+00 -0.006 0.015 0.006

60.0000 1 .810E+00 1 .835E+00 3.665E+00 2.651E+01 3.01 5E-01 6 .029E+00 -0.006 0.016 0.006

70.0000 1 .822E+00 2. 168E + 00 3.990E+00 2.713E+01 3.333E-01 6.323E+00 -0.003 0.013 0.005

80.0000 1 .833E+00 2.503E+00 6.337E+00 2.953E+01 3.617E-01 6.581E+00 -0.002 0.012 0.006

90.0000 1 .862E+00 2.861E+00 6.683E+00 3. 175E+01 3.873E-01 6.809E+00 -0.002 0.011 0.003

100.0000 1 .851E+00 3. 179E+00 5.030E+00 3.381E+01 6. 106E-01 7.015E+00 -0.002 0.010 0.003

1 25 .0000 1 .868E+00 6.030E+00 5.898E+00 3.839E+01 6 .602E-01 7 .652E+00 -0.001 0.009 0.002

150.0000 1 .882E+00 6 .887E + 00 6.769E+00 6.235E+01 5.008E-01 7.812E+00 -0.001 0.008 0.002

175.0000 1 .896E+00 5.767E+00 7.661E+00 6.582E+01 5.366E-01 8. 1 17E+00 -0.001 0.008 0.002

200.0000 1 . 906E+00 6.61 1E+00 8.515E+00 6.892E+01 5.636E-01 8. 382E+00 -0.001 0.007 0.001

250 .0000 1 . 921 E+00 8. 365E+00 1 .027E+01 5.626E+01 6.098E-01 8.825E+00 -0.000 0 .007 0.001

300 .0000 1 . 935E+00 1 .009E+01 1 .202E+01 5.876E+01 6 .660E-01 9. 188E+00 -0.000 0.006 0.001

350 .0000 1 . 967E+00 1 . 183E+01 1 .378E+01 6 .266E+01 6.750E-01 9.695E+00 -0.000 0.006 0.001

600 .0000 1 . 957E+00 1 . 358E+01 1 .556E+01 6 .605E+01 6.990E-01 9.761 E+00 -0.000 0.005 0.001

650 .0000 1 . 966E+00 1 .533E+01 1 .730E+01 6.910E+01 7.191E-01 9. 996E+00 -0.000 0.005 0.001 500.0000 1 . 976E+00 1 .709E+01 1 . 906E+01 7.185E+01 7.366E-01 1 .021E+01 -0.000 0.005 0.001 550.0000 1 . 981 E+00 1 .885E + 01 2.083E+01 7.636E+01 7.513E-01 1 .060E+01 -0.000 0.005 0.000

600.0000 1 . 988E+00 2.060E+01 2.259E+01 7 . 667E+01 7 .666E-01 1 .057E+01 -0.000 0.005 0.000

700.0000 1 . 999E+00 2.612E+01 2.612E+01 8.078E+01 7 .866E-01 1 . 088E+01 -0.000 0.006 0.000

800.0000 2.009E+00 2.765E+01 2. 966E+01 8.637E+01 8.061E-01 1 . 1 15E+01 -0.000 0.006 0.000

900.0000 2.018E+00 3. 1 17E+01 3.319E+01 8.756E+01 8. 187E-01 1 . 138E+01 -0.000 0.006 0.000

1000.0000 2.026E+00 3.670E+01 3.673E+01 9.062E+01 8.311E-01 1 .159E+01 -0 .000 0.006 0.000

111
ELECTRONS IN B-100 BONE-EQUIVALENT PLASTIC

I = 85.9 eV DENSITY = 1 .950E+0C1 g/cm-l

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^/g MeV cm^/g MeV cm^/g g/cm 2 0.0100 2.086E+01 9.977E-03 2.086E+01 2.731E-09 1 .193E-09 0.0 -0.209 0.235 0.232

0.0125 1 .756E+01 9 . 559E-03 1 .756E+01 9.093E-09 1 .389E-09 0.0 -0.196 0.223 0.221 0.0150 1 .525E+01 9.618E-03 1 .526E+01 5.579E-09 1 .626E-09 0.0 -0.189 0.215 0.213

0.0175 1 .359E+01 9.669E-03 1 .355E+01 7.317E-09 1 .856E-09 0.0 -0.189 0.208 0.206 0.0200 1 .222E+01 9.700E-03 1 .222E+01 9.263E-09 2.080E-09 0.0 -0.179 0.202 0.201 0.0250 1 .030E+01 9.759E-03 1 .030E+01 1 .379E-03 2.51 IE-09 0.0 -0.173 0.199 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 7.991E+00 2.987E-03 3.319E-09 0.0 -0.169 0.182 0.181

0 .OAOO 7 .232E+00 9.860E-03 7.237E+00 3.196E-03 3.702E-09 0.0 -0.160 0.178 0.177

0 .OA50 6 .633E+00 9.888E-03 6 .637E+00 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+00 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 .051 E-02 6 .929E-09 0.0 -0.195 0.159 0.158

0.0900 9 . 103E+00 5. 1 16E-03 9. 109E+00 1 .285E-02 7.036E-09 0.0 -0.193 0.156 0.155

0 . I 000 3 . 837E+00 5 . 1 70E-03 3.892E+00 1 . 537E-02 7 . 628E-09 0.0 -0.191 0.159 0.153

0.1250 3 . 350E+00 5 . 31 8E-0 3 3.355E+00 2.236E-02 9.036E-09 0.0 -0.136 0.199 0.198

0.1500 3.021 E+00 5 . 979E-03 3.027E+00 3.023E-02 1 . 036E-03 0 .

-0.133 0.195 0.199

0.1750 2 . 785E+00 5 . 651 E-03 2 . 791 E + 00 3.889E-02 1 . 1 62E-03 0 .

-0.131 0.192 0.191

0 . 2000 2 . 60GE+00 5.835E-03 2.619E+00 9.81 IE-02 1 .283E-03 0.0 -0.129 0.190 0.139

0 . 2 5 0 0 2 . 362E+00 6.231 E-03 2.368E+00 6 .827E-02 1 .513E-03 0.0 -0.125 0.136 0.135

0 . 5 0 0 0 2.201 C+00 6 . 665E-03 2 . 208E+00 9.01 9E-02 1 .732E-03 0.0 -0.122 0.133 0.132

0 . 5 0 0 2 . 089C+00 7 . 1 31 E-03 2 . 096E+00 1 . 1 35E-01 1 . 993E-03 9.066E-03 -0.105 0.130 0.128

0 . 9 000 2 . 005E + 00 7 .626E-03 2.013E+00 1 .378E-01 2.150E-03 2.983E-02 -0.095 0.129 0.122

0 . 9500 1 . 99.2E + 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 .891 E-01 2.555E-03 8. 971 E-02 -0.083 0.119 0.111

0 .5500 1 .855E+00 9 . 263E-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-01 -0.075 0.107 0.102

0.7000 1 . 7S0E+00 1 . 1 08E-02 1 .791E + 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 2.901E-01 -0.063 0.099 0.088

0 . 9000 1 . 730E+00 1 . 372E-02 1 .793E + 00 9.113E-01 9.179E-03 3.577E-01 -0.059 0.090 0.083

1 .0000 1 .715E+00 1 . 51 2E-02 1 .731E+00 9.688E-01 9.587E-03 9.292E-01 -0.056 0.086 0.078

1 . 2500 1 .697E+00 1 .882E-02 1 .71 5E + 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 .719E + 00 7.599E-01 6.721E-03 7.331E-01 -0.095 0.072 0.062

1 .7500 1.691 E+00 2.695E-02 1 .718E + 00 9.057E-01 7.830E-03 8.719E-01 -0.092 0.067 0.057

2.0000 1 . 695E+00 3 . 1 29E-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 . 091 E-02 1 .797E+00 1 .339E+00 1 .130E-02 1 .230E+00 -0.036 0.058 0.097

3 .0000 1.71 9E+00 9 . 999E-02 1 .769E+00 1 .623E+00 1 .369E-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 .612E+00 -0.032 0.050 0.090 9.0000 1 .7950+00 7 . 022E-02 1 .816E+00 2.181E+00 1 .863E-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. 1 15E-02 1 .920E + 00 -0.029 0.095 0.035

5.0000 1 .7680+00 9. 156E-02 1 .860E+00 2.725E+00 2.370E-02 2.059E+00 -0.028 0.099 0.039

5.5000 1 . 779E+00 1 . 026E-01 1 .881 E+00 2. 993E+00 2.626E-02 2. 179E+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-01 1 . 992E+00 3.777E+00 3 . 901 E-02 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. 921E-02 2.692E+00 -0.023 0.036 0.027

9 .0000 1 .839E+00 1 . 891 E-01 2.018E+00 9. 787E+00 9.992E-02 2.862E+00 -0.021 0.035 0.026

1 0 .0000 1 .896E+00 2.089E-01 2.059E+00 5.278E+00 9 . 961 E-02 3.017E+00 -0.020 0.033 0.029

12.5000 1 .870E+00 2.708E-01 2.191E+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 7.615E+00 7.518E-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 . 920E+00 9.665E-01 2.386E+00 9.789E+00 9.972E-02 9.131E+00 -0.011 0.029 0.015

25.0000 1 . 992E+00 6.019E-01 2.593E+00 1 . 181E+01 1 .230E-01 9.522E+00 -0.008 0.021 0.012

30.0000 1 . 959E+00 7 . 385E-01 2.698E+00 1 .372E+01 1 . 951 E-01 9.850E+00 -0.007 0.019 0.010

35.0000 1 . 973E+00 8.779E-01 2.851E+00 1 .552E+01 1 . 659E-01 5.133E+00 -0.005 0.017 0.009

90 .0000 1 . 986E+00 1 . 0 1 8E+00 3.003E+00 1 .723E+01 1 .856E-01 5.381E+00 -0.005 0.016 0.008

95.0000 1 . 996E+00 1 . 1 59E+ 00 3.1 55E+00 1 .886E+01 2.093E-01 5.602E+00 -0 .009 0.015 0.007

50 .0000 2 . 006E+00 1.301 E+00 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 . 9S3E+00 -0.003 0.013 0.005

60.0000 2.022E+00 1 . 588E+00 3.610E+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 9.216E+00 2.892E+01 3. 106E-01 6 .705E+00 -0.002 0.010 0.003

90.0000 2 . 056E+00 2.962E+00 9.519E+00 3.071E+01 3.350E-01 6.939E+00 -0.002 0.010 0.003

100.0000 2.065E+00 2 . 757E+00 9.822E+00 3.285E+01 3.579E-01 7 . 1 39E + 00 -0.002 0.009 0.003

125.0000 2 . 089E+00 3.997E+00 5.582E+00 3.767E+01 9.060E-01 7 .576E + 00 -0.001 0.008 0.002

150.0000 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 . 1 1 '>£ + 00 9 . 993E+00 7. 105E+00 9.559E+01 9.807E-01 8.238E+00 -0.001 0.007 0.001 2000000 2 . 1 ^ 1E + 00 5 . 795E+00 7.868E+00 9 .893E+01 5. 102E-01 8.502E+00 -0.001 0 .006 0.001

250 .0000 2 . 1 97E+00 7 .256E+00 9 . 398E+00 5.979E+01 5.586E-01 8. 999E + 00 -0.001 0.006 0.001 300.0000 2 . 1

.^- /E + OO 8 . 779E+00 1 .093E+01 5. 967E+01 5.969E-01 9. 306E + 00 -0.000 0.005 0.001

350 . 0000 2 . 1 6 9E + 00 1 .030E+01 1 .297E+01 6 . 395E+01 6.280E-01 9.612E+00 -0.000 0.005 0.001

900 .0000 2 . 1 8 '.E + OO 1 . 1 C2E+0

1 . 900E+06 .773E+01 6 . 590E-0

9 .878E + 00 -0.000 0.005 0.001

950 .0000 2.r E + 00 1 . 3 3 5 E 1 0 1 1 .559E+01 7. 1 12E+01 6 .760E-01 1.011 E+01 -0.000 0.009 0.001

500 . 0000 2 . 1 98E+00 1 . 9 8 8 E < 0 1 1 .708E+01 7.918E+01 6 . 999E-01 .032E+01 -0 .000 0.009 0.000

550 .0000 2 . 206E+00 1 . 692E^ 0

1 .862E+01 7.699E+01 7.11 9E-01 1 .051 E+01 -0.000 0.009 0.000

600 .0000 2.21 3E+00 1 . 7 95E + 01 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+01 8.918E+01 7.505E-01 1 .099E+01 -0.000 0 .009 0.000 800.0000 2 . 237E+00 2.910E+01 2.639E+01 8.822E+01 7.709E-01 1 . 1 26E+01 -0.000 0.003 0.000

900 . 0000 2 . 296E+00 2.718E+01 2. 993E+01 9. 181E+01 7.870E-01 1 . 1 50E+01 -0.000 0.003 0.000

1 000 .0000 2.255E+00 3.026E+01 3.252E+01 9.509E+01 8.010E-01 1 . 1 71 E+01 -0.000 0.003 0.000
ELECTRONS IN BONE, COMPACT (ICRU)

I = 91.9 eV DENSITY = 1 .850E+0C1 g/cm^

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^/g MeV cm^/g MeV cm^/g g/cm 2 0.0100 2.068E+01 A . 793E-03 2.068E+01 2.761E-0A 1 .236E-0A 0.0 -0.207 0.239 0.236 0.0125 1 .7A2E+01 A .880E-03 1 .7A2E + 01 A.08AE-0A 1 .501 E-OA 0.0 -0.198 0 . 227 0 .22A 0.0150 1 . 51 AE + 01 A.9A2E-03 1 .51 AE+01 5.628E-0A 1 .756E-0A 0 .

-0.191 0.218 0.216 0.0175 1 .3AAE+01 A. 989E-03 1 .3A5E+01 7.383E-0A 2.00AE-0A 0.0 -0.186 0.211 0.209

0.0200 1 .21 3E+01 5.026E-03 1 .21 AE+01 9.3A3E-0A 2.2AAE-0A 0.0 -0 . 182 0 . 205 0.203

0.0250 1 .023E+01 5.080E-03 1 .02AE+01 1 .385E-03 2.706E-0A 0.0 -0.175 0.196 0.195

0.0300 8.912E+00 5. 121E-03 8.917E+00 1 .910E-03 3. 1 A8E-0A 0.0 -0.169 0.190 0.188

0.0350 7.939E+00 5. 155E-03 7.9AAE+00 2.505E-03 3.572E-0A 0.0 -0.165 0 . 18A 0.183

0 . OAOO 7 . 1 90E+00 5. 18AE-03 7 . 1 96E+00 3 . 1 68E-03 3. 982E-0A 0.0 -0.162 0.180 0.179

0.0A5O 6 . 596E+00 5.21 lE-03 6 .601E+00 3.89AE-03 A . 379E-0A 0.0 -0.159 0.176 0.175

0 .0500 6 . 1 1 2E+00 5 .237E-03 6 . 117E+00 A.682E-03 A.76AE-0A 0.0 -0.156 0.173 0.172

0 .0550 5 . 709E+00 5.263E-03 5.715E+00 5.528E-03 5.139E-0A 0.0 -0 . 1 5A 0.170 0.170

0.0600 5. 370E+00 5 . 288E-03 5.375E+00 6 . A31 E-03 5 . 50AE-0A 0.0 -0.152 0.168 0.167

0.0700 A .827E+00 5 . 338E-03 A .832E+00 8 . 397E-03 6.210E-0A 0.0 -0 . 1 A9 0 . 1 6A 0.163

0 . 0800 A . A 1 2E + 00 5.390E-03 A.A17E+00 1 .056E-02 6 .887E-0A 0.0 -0.1A6 0.160 0.160

0.0900 A . 035E+00 5 . AA5E-03 A.090E+00 1 . 292E-02 7.5A0E-0A 0 . 0 -0 . 1 AA 0.158 0.157

0 . 1 000 3 .822E+00 5.502E-03 3.825E+00 1 .5A5E-02 8. 171E-0A 0.0 -0.1A2 0.155 0.155

0.1250 3 . 336E+00 5.657E-03 3.3A2E+00 2.2A7E-02 9.670E-0A 0.0 -0.138 0.150 0.150

0 . 1500 3 . 0 1 9E+00 5 . S26E-03 3.015E+00 3 . 037E-02 1 . 1 08E-03 0 . 0 -0.135 0.1A7 0 . 1A6 0.1750 2 . 7 7',)E+00 6 . 007E-03 2.781E+00 3. 901E-02 1 .2A2E-03 0.0 -0.132 0 . 1 A3 0 . 1 A3

0 . 2000 2 . 59 7E+00 6 . 200E-03 2 . 605E+00 A .832E-02 1 .371E-03 0.0 -0.130 0.1A1 O.IAO 0.2500 2 . 3 ; .E+00 6 . 6 1 8E-03 2.361E+00 6 .855E-02 1 .615E-03 0.0 -0.126 0.137 0.136

0.3000 2 . 1 E+00 7.075E-03 2.201E+00 9.053E-02 1 .8ASE-03 0.0 -0.118 0 . 1 3A 0.133

0 . 3500 2.0,' E + 00 7 . 567E-03 2.087E+00 1 . 1 39E-01 2.072E-03 2.8A3E-02 -0.096 0.127 0.126

0.0000 1 . 9 >6 E+0 0 8.090E-03 2.00AE+00 1 . 38AE-01 2.292E-03 6.250E-02 -0.089 0.121 0.119

0 . 0500 1 . 932E + 00 8 . 6A3E-03 1 . 9A1 E+00 1 .637E-01 2.509E-03 9.798E-02 -0 .08A 0.116 0.112

0.5000 1 .833E + 00 9.221E-03 1 .893E+00 1 .898E-01 2.72AE-03 1 .3A2E-01 -0.079 0.111 0.107

0.5500 1 .8A5E + 00 9.823E-03 1 .855E+00 2.165E-01 2.939E-03 1 .710E-01 -0.075 0.107 0.102

0 .6000 1.81 5E+00 1 .0A5E-02 1 .825E+00 2. A37E-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 0.3000 1 . 7A0E+00 1.311 E-02 1 .753E+00 3.558E-01 A.Ol AE-03 3.5A8E-01 -0.061 0.091 0.08A

0.9000 1.71 9E+00 1 . A5AE-02 1 .73AE+00 A.132E-01 A. AA9E-03 A.265E-01 -0.057 0.086 0.079

1 .0000 1 .705E+00 1 . 602E-02 1 .721 E+00 A. 71 IE-01 A.889E-03 A. 96AE-01 -0 .05A 0.083 0.075

1 .2500 1 .6S6E+00 1 . 995E-02 1 .706E+00 6. 17IE-01 6.009E-03 6.626E-01 -0 .OAS 0.075 0.066

1 .5000 1 . 680E+00 2.A1AE-02 1 .705E+00 7.638E-01 7. 161E-03 8.160E-01 -O.OAA 0.069 0.060

1 .7500 1 .6S1E+00 2 .85AE-02 1 .709E+00 9.103E-01 8.3A1E-03 9.575E-01 -0 .0A1 0.065 0.055

2.0000 1 .62AE+00 3.31 3E-02 1 .718E+00 1 . 056E+00 9.5A7E-03 1 .088E+00 -0.039 0.061 0.051 2.5000 1 .696E+00 A.277E-02 1 .739E+00 1 .3A6E+00 1 .202E-02 1 .323E+00 -0.035 0 .056 0.0A6

3.0000 1 .709E+00 5 . 289E-02 1 .762E+00 1 .631E+00 1 . A57E-02 1 .527E+00 -0.033 0.052 0 .0A2 3.5000 1 . 722E+00 6.3A1E-02 1 .786E+00 1 . 91 3E+00 1 .717E-02 1 .709E+00 -0.031 0 .0A9 0.039

A .0000 1 .735E+00 7.A27E-02 1 .809E+00 2.191E+00 1 .981E-02 1 .872E+00 -0.030 0.0A6 0.037

A . 5000 1 .7A7E+00 8.5A1E-02 1 .832E+00 2. A66E+00 2.2A8E-02 2.020E+00 -0.029 O.OAA 0.035

5 .0000 1 .75CE+00 9.680E-02 1 .855E+00 2.737E+00 2.517E-02 2.156E+00 -0.027 0 .0A3 0.033

5.5000 1 .768E+00 1 . 08AE-01 1 .877E+00 3.005E+00 2.788E-02 2.282E+00 -0.026 0 .0A1 0.032

6.0000 1 . 775E+00 1 .202E-01 1 .898E+00 3.270E+00 3.060E-02 2.399E+00 -0.025 0 .OAO 0.031

7 .0000 1 .795E+00 1 .AAAE-01 1 .939E+00 3.791E+00 3.607E-02 2.61 1E+00 -0 .02A 0.037 0.028

8 .0000 1 .81 OE+00 1 .692E-01 1 . 979E+00 A.301E+00 A.156E-02 2.801E+00 -0.022 0.035 0.027

9 .0000 1 .823E+00 1 . 9A5E-01 2.018E+00 A.802E+00 A.705E-02 2.972E+00 -0.021 0 .03A 0.025

10.0000 1 .835E+00 2.202E-01 2.055E+00 5.293E+00 5.252E-02 3. 129E+00 -0.019 0.032 0.02A

12.5000 1 .860E+00 2.860E-01 2. 1 A6E+00 6.A83E+00 6.608E-02 3. A73E+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 -O.OIA 0.027 0.019

17.5000 1 .896E+00 A.226E-01 2.318E+00 8.72AE+00 9.2A0E-02 A.021E+00 -0.012 0.025 0.017

20.0000 1 . 909E+00 A.926E-01 2. A02E+00 9.783E+00 1 .051E-01 A.2A7E+00 -0.011 0.023 0.015

25.0000 1 . 931 E+00 6.351E-01 2.566E+00 1 . 180E+01 1 .29AE-01 A.637E+00 -0.008 0.021 0.012

30.0000 1 . 9A9E+00 7 . 799E-01 2.729E+00 1 .369E+01 1 .523E-01 A.965E+00 -0.007 0.018 0.010

35.0000 1 . 963E+00 9.26AE-01 2.890E+00 1 .5A7E+01 1 .739E-01 5.2A7E+00 -0.006 0.017 0.009

AO .0000 1 . 976E+00 1 . 07AE+00 3.050E+00 1 .715E+01 1 . 9A3E-01 5. A95E+00 -0.005 0.016 0.008

A5.0000 1 . 986E+00 1 .22AE + 00 3.210E+00 1 .875E+01 2.13AE-01 5.716E+00 -O.OOA O.OIA 0.007

50.0000 1 . 996E+00 1 .37AE+00 3.369E+00 2.027E+01 2.316E-01 5.915E+00 -O.OOA O.OIA 0.006

55.0000 2.00AE+00 1 .525E+00 3.529E+00 2. 172E+01 2. A87E-01 6 .097E+00 -0.003 0.013 0.005

60.0000 2.012E+00 1 .676E+00 3.688E+00 2.310E+01 2.6A9E-01 6.263E+00 -0.003 0.012 0.005

70.0000 2.025E+00 1 . 982E+00 A.007E+00 2.570E+01 2.9A9E-01 6.559E+00 -0.003 0.011 O.OOA

80.0000 2.037E+00 2.289E+00 A.326E+00 2.81 lE+01 3.221E-01 6.817E+00 -0.002 0.010 O.OOA

90 .0000 2.0A7E+00 2.598E+00 A.6A5E+00 3.03AE+01 3.A68E-01 7.0A6E+00 -0.002 0.010 0.003

1 00 .0000 2.056E+00 2. 909E+00 A. 965E+00 3.2A2E+01 3.69AE-01 7.251E+00 -0.002 0.009 0.003

1 25 .0000 2.075E+00 3.690E+00 5.765E+00 3.709E+01 A.18AE-01 7 . 688E+00 -0.001 0.008 0.002

150.0000 2.090E+00 A . A76E+00 6.566E+00 A. 1 15E+01 A.590E-01 8.0A6E+00 -0.001 0.007 0.002

175.0000 2. 103E+00 5.266E+00 7.369E+00 A.A7AE+01 A.932E-01 8.350E+00 -0.001 0.007 0.001 200.0000 2. 1 lAE+00 6 .059E+00 8. 173E+00 A.796E+01 5.226E-01 8.61 AE+00 -0.001 0.006 0.001 250.0000 2. 1 33E+00 7.652E+00 9.78AE+00 5.35AE+01 5.707E-01 9 . 057E+00 -0.001 0.006 0.001

300 .0000 2. 1 A8E+00 9 . 251 E+00 1 . 1 AOE+01 5.827E+01 6 .085E-01 9.A19E+00 -0.000 0.005 0.001 350.0000 2. 1 60E+00 1 .086E+01 1 .302E+01 6.238E+01 6 . 392E-01 9.726E+00 -0.000 0.005 0.001 AOO.OOOO 2 . 1 71 E+00 1 .2A6E+01 1 . A6AE+01 6.600E+01 6.6A7E-01 9 . 991 E+00 -0.000 0 .005 0.001

A50 .0000 2. 181 E+00 1 . A07E+01 1 .626E+01 6 . 92AE+01 6 .863E-01 1 .023E+01 -0.000 0 . OOA 0.001 500.0000 2. 189E+00 1 .569E+01 1 .788E+01 7.217E+01 7.0A8E-01 1 .OAAE+01 -0.000 0 .OOA 0.000

550.0000 2. 1 97E+00 1 .730E+01 1 . 950E+01 7. A85E+01 7.210E-01 1 .063E+01 -0.000 O.OOA 0.000

600.0000 2.20AE+00 1 .892E+01 2. 1 12E+01 7.731E+01 7. 352E-01 1 .080E+01 -0.000 O.OOA 0.000

700.0000 2.217E+00 2.21 6E+01 2.A37E+01 8. 171E+01 7.591E-01 1 . 1 1 1 E+01 -0.000 O.OOA 0.000

800.0000 2.228E+00 2.5A0E+01 2.763E+01 8.556E+01 7.785E-01 1 . 1 37E+01 -0.000 O.OOA 0.000

900.0000 2.237E+00 2.86AE+01 3.088E+01 8.898E+01 7.9A7E-01 1 .161E+01 -0.000 0.003 0.000

1000.0000 2.2A6E+00 3. 189E+01 3. A1 AE+01 9.206E+01 8.083E-01 1 . 182E+01 -0.000 0.003 0.000

113
ELECTRONS IN BONE, CORTICAL (ICRP)

I = 106.9 eV DENSITY = 1 .850E+001 g/cm^

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( loo1 ) /d ( log I

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 . 971 E+01 5.961E-03 1 . 972E+01 2. 909E-09 1 .968E-09 0.0 -0.219 0.298 0.299

0.0125 1 .663E+01 5.579E-03 1 .669E+01 9.295E-09 1 .787E-09 0.0 -0.209 0.235 0.232

0.0150 1 .997E + 01 5.669E-03 1 .997E+01 5.911 E-09 2.095E-09 0.0 -0.197 0.226 0.223

0.0175 1 .286E + 01 5.728E-03 1 .287E+01 7.797E-09 2.393E-09 0.0 -0.191 0.218 0.216

0.0200 1 . 161E+01 5.778E-03 1 . 162E+01 9.795E-09 2.683E-09 0.0 -0.187 0.212 0.210

0.0250 9.809E+00 5.853E-03 9.810E+00 1 .950E-03 3.292E-09 0.0 -0.179 0.202 0.200

0.0300 8.596E+00 5. 907E-03 8.552E+00 1 . 997E-03 3.775E-09 0.0 -0.179 0.195 0.199

0.0350 7.618E+00 5. 951 E-03 7 .629E+00 2.618E-03 9.287E-09 0.0 -0.169 0.190 0.188

O.OAOO 6 . 903E+00 5. 989E-03 6 . 909E+00 3.308E-03 9.781E-09 0.0 -0.166 0.185 0.189

0 .0A50 6 . 335E+00 6 .022E-03 6 . 391 E+00 9.069E-03 5.259E-09 0.0 -0.163 0.181 0.180

0 .0500 5.872E+00 6 .059E-03 5.879E+00 9.889E-03 5.723E-09 0.0 -0.160 0.178 0.177

0.0550 5.988E+00 6 . 089E-03 5.999E+00 5.769E-03 6 . 1 75E-09 0.0 -0.158 0.175 0.179

0.0600 5 . 1 63E+00 6.11 3E-03 5. 169E+00 6.703E-03 6.619E-09 0.0 -0.156 0.172 0.171 0.0700 9.693E+00 6 . 1 71 E-03 9.699E+00 8.798E-03 7 .963E-09 0.0 -0.152 0.168 0.167

0.0800 9 . 296E+00 6 .230E-03 9.252E+00 1 .100E-02 8.276E-09 0.0 -0.199 0.169 0.169

0.0900 3. 932E+00 6 .292E-03 3. 939E+00 1 .395E-02 9.059E-09 0.0 -0.197 0.161 0.161 0.1000 3.678E+00 6 . 356E-03 3.685E+00 1 .607E-02 9.819E-09 0.0 -0.195 0.159 0.158

0.1250 3.21 5E+00 6.530E-03 3.221E+00 2. 336E-02 1 . 161E-03 0.0 -0.191 0.159 0.153

0 . 1 500 2.901 E+00 6.71 9E-03 2. 908E+00 3. 155E-02 1 . 329E-03 0.0 -0.137 0.150 0.199

0.1750 2.676E+00 6 . 923E-03 2.683E+00 9.051E-02 1 . 989E-03 0.0 -0.139 0.197 0.196

0.2000 2.507E+00 7. 190E-03 2.519E+00 5.015E-02 1 .691E-03 0.0 -0.132 0.199 0.193

0.2500 2.272E+00 7.612E-03 2.280E+00 7.11 lE-02 1 . 931E-03 0.0 -0.128 0.190 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 lE+00 8 . 685E-03 2.020E+00 1 . 180E-01 2.971E-03 8. 920E-03 -0.105 0.133 0.131 O.AOOO 1 . 931 E+00 9.276E-03 1 .991E+00 1 .933E-01 2.730E-03 3.91 lE-02 -0.098 0.127 0.125

0 . 9500 1 .871E+00 9. 901E-03 1 .881 E+00 1 .695E-01 2. 989E-03 6 .200E-02 -0.092 0.122 0.119

0.5000 1 .825E+00 1 .055E-02 1 .836E+00 1 . 969E-01 3.236E-03 9.1 96E-02 -0.087 0.118 0.119

0 . 5500 1 .789E+00 1 . 1 29E-02 1 .800E+00 2.239E-01 3.987E-03 1 .21 9E-01 -0.083 0.113 0.109

0.6000 1 .760E+00 1 . 1 99E-02 1 .772E+00 2.51 9E-01 3.737E-03 1 .531E-01 -0.079 0.110 0.105

0.7000 1 .718E+00 1 .391E-02 1 .732E+00 3.090E-01 9.237E-03 2. 166E-01 -0.073 0.103 0.098

0.8000 1 .690E+00 1 .995E-02 1 .705E+00 3.673E-01 9.790E-03 2.806E-01 -0.068 0.098 0.092

0.9000 1 .671 E+00 1 .657E-02 1 .688E+00 9.262E-01 5.295E-03 3.992E-01 -0.063 0.093 0.086

1 .0000 1 .658E+00 1 .829E-02 1 .677E+00 9.857E-01 5.755E-03 9.069E-01 -0.060 0.089 0.082

1 .2500 1 . 692E+00 2.267E-02 1 .665E+00 6.359E-01 7.052E-03 5.580E-01 -0.053 0.082 0.073

1 .5000 1 .637E+00 2 . 790E-02 1 . 665E+00 7.857E-01 8.382E-03 6 . 999E-01 -0.099 0.076 0.066

1 .7500 1 .639E+00 3.237E-02 1 .671E+00 9.356E-01 9.793E-03 8.310E-01 -0.095 0.071 0.061

2 . 0000 1 . 693E+00 3 . 755E-02 1 .681E+00 1 .085E+00 1.11 3E-02 9.539E-01 -0.093 0.067 0.057

2 . 5000 1 .656E+00 9.890E-02 1 .709E+00 1 .380E+00 1 .398E-02 1 . 179E+00 -0.039 0.061 0.051 3.0000 1 . 670E+00 5.981E-02 1 .730E+00 1 .671E+00 1 .689E-02 1 .368E+00 -0.036 0.057 0.096

3 . 5000 1 .689E+00 7 . 1 65E-02 1 .755E+00 1 . 958E+00 1 .987E-02 1 .591E+00 -0.039 0.059 0.093

9 .0000 1 .697E+00 8.386E-02 1 .781E+00 2.291E+00 2.288E-02 1 .697E+00 -0.033 0.051 0.090

9.5000 1 . 709E+00 9.638E-02 1 .805E+00 2.520E+00 2.592E-02 1 .839E+00 -0.031 0.099 0.038

5.0000 1 . 720E+00 1 .092E-01 1 .829E+00 2.795E+00 2.898E-02 1 . 970E+00 -0.030 0.097 0.036

5.5000 1 .731E+00 1 .222E-01 1 .853E+00 3.067E+00 3.206E-02 2.091E+00 -0.029 0.095 0.035

6.0000 1 .790E+00 1 . 355E-01 1 .876E+00 3.335E+00 3.519E-02 2.203E+00 -0.028 0.099 0.033

7.0000 1 .758E+00 1 .626E-01 1 .921E+00 3.862E+00 9.1 33E-02 2.908E+00 -0.026 0.091 0.031 8.0000 1 .773E+00 1 . 909E-01 1 . 969E+00 9.377E+00 9.752E-02 2.591E+00 -0.025 0.039 0.029

9.0000 1 . 787E+00 2. 188E-01 2.006E+00 9.880E+00 5.369E-02 2.757E+00 -0.023 0.037 0.028

1 0 .0000 1 .799E+00 2.976E-01 2.096E+00 5.379E+00 5.983E-02 2.908E+00 -0.022 0.036 0.026

12.5000 1 .829E+00 3.219E-01 2.195E+00 6.567E+00 7.997E-02 3.291E+00 -0.019 0.032 0.023

15.0000 1 .899E+00 3. 971 E-01 2.291E+00 7.707E+00 8. 979E-02 3.525E+00 -0.016 0.030 0.020

17.5000 1 .860E+00 9.792E-01 2.335E+00 8.800E+00 1 .091E-01 3.773E+00 -0.019 0.028 0.018

20.0000 1 .879E+00 5.525E-01 2.927E+00 9.850E+00 1 . 180E-01 3. 999E+00 -0.013 0.026 0.017

25.0000 1 .897E+00 7.1 17E-01 2.609E+00 1 . 189E+01 1 .996E-01 9.375E+00 -0.010 0.023 0.019

30.0000 1 . 91 5E+00 8.735E-01 2.788E+00 1 .369E+01 1 .699E-01 9.696E+00 -0.008 0.021 0.012

35 .0000 1 . 929E+00 1 .037E+00 2.966E+00 1 .593E+01 1 . 926E-01 9. 973E+00 -0.007 0.019 0.010

90 .0000 1 .992E+00 1 .202E+00 3.199E+00 1 .707E+01 2. 193E-01 5.217E+00 -0.006 0.017 0.009

95.0000 1 . 952E+00 1 . 369E+00 3 . 321 E+00 1 .861 E+01 2.397E-01 5.939E+00 -0.005 0.016 0.008

50.0000 1 . 962E+00 1 . 537E+00 3.998E+00 2.008E+01 2.538E-01 5.631E+00 -0.005 0.015 0.007

55.0000 1 . 970E+00 1 .705E+00 3.676E+00 2.197E+01 2.718E-01 5.81 OE+00 -0.009 0.019 0.006

60.0000 1 . 978E+00 1 .875E+00 3.853E+00 2.280E+01 2.888E-01 5.979E+00 -0.009 0.019 0.006

70.0000 1 . 992E+00 2.215E+00 9.207E+00 2.529E+01 3.199E-01 6 .267E+00 -0.003 0.013 0.005

80.0000 2.003E+00 2. 558E + 00 9.561 E+00 2.757E+01 3.980E-01 6 .523E+00 -0.003 0.012 0.009

90.0000 2.013E+00 2. 903E + 00 9.916E+00 2. 968E+01 3.733E-01 6 .799E+00 -0.003 0.011 0.009

1 00 .0000 2.022E+00 3.299E+00 5.272E+00 3. 169E+01 3.969E-01 6.953E+00 -0.002 0.010 0.003

125.0000 2.091E+00 9.120E+00 6.161E+00 3.602E+01 9.959E-01 7.387E+00 -0.002 0.009 0.003

150.0000 2 . 056E+00 9 . 997E+00 7.053E+00 3. 981 E+01 9.865E-01 7.793E+00 -0.001 0.008 0.002

175.0000 2 . 069E+00 5.878E+00 7 . 997E+00 9.315E+01 5.205E-01 8.096E+00 -0.001 0.008 0.002

200 .0000 2 . 080E+00 6 .762E + 00 8.892E+00 9.61 3E+01 5.995E-01 8.309E+00 -0.001 0.007 0.002

250.0000 2.098E+00 8.537E+00 1 .069E+01 5. 128E+01 5. 966E-01 8.750E+00 -0.001 0.007 0.001 300.0000 2.11 3E+00 1 .032E + 01 1 . 293E+01 5.563E+01 6 . 333E-01 9.1 1 1E+00 -0.001 0.006 0.001 350.0000 2. 126E+00 1 .21 1E + 01 1 .923E+01 5.938E+01 6.630E-01 9.917E+00 -0.000 0.006 0.001

900 .0000 2.136E+00 1 .390E + 01 1 .609E+01 6 .269E+01 6 .875E-01 9.683E+00 -0.000 0.005 0.001

950 .0000 2. 1 96E+00 1 .569E + 01 1 .789E+01 6.569E+01 7.081E-01 9. 91 7E+00 -0.000 0.005 0.001

500 .0000 2. 1 59E+00 1 .799E+01 1 .969E+01 6 .831 E+01 7.258E-01 1 .01 3E + 01 -0.000 0.005 0.001 550.0000 2. 162E+00 1 . 929E + 01 2. 195E+01 7.075E+01 7.912E-01 1 .032E+01 -0.000 0.005 0.001 600.0000 2. 1 69E+00 2. 109E + 01 2.326E+01 7.299E+01 7.597E-01 1 .099E+01 -0.000 0.005 0.000 700.0000 2 . 1 81 E+00 2.970E+01 2.688E+01 7.698E+01 7.773E-01 1 .080E+01 -0.000 0.009 0.000 800.0000 2. 1 92E+00 2.831E+01 3.050E+01 8.097E+01 7 . 956E-01 1 . 1 07E+01 -0.000 0.009 0.000 900.0000 2.202E+00 3.192E+01 3.912E+01 8.357E+01 8. 108E-01 1 .130E + 01 -0.000 0.009 0.000 1000.0000 2.210E+00 3.553E+01 3.779E+01 8.636E+01 8.235E-01 1 . 151E+01 -0.000 0 .009 0.000

114
ELECTRONS IN C-552 AIR-EQUIVALENT PLASTIC

I = 86.8 eV DENSITY = 1 .760E+00 g/cm 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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 . 972E+01 3 . 767E-03 1 . 972E + 01 2.890E-09 1 . 096E-09 0.0 -0.205 0.235 0.233

0.0125 1 . 660E+01 3 . 799E-03 1 .661E + 01 9.277E-09 1 .257E-09 0.0 -0.196 0.229 0.222

0.0150 1 . 992E+0

3.812E-03 1 .993E + 01 5 .897E-09 1 .958E-09 0.0 -0.189 0.215 0.219

0.0175 1 .281 E+01 3.829E-03 1 .281 E+01 7.739E-09 1 .652E-09 0.0 -0.189 0.208 0.207

0 .0200 1 . 1 56E+01 3 . 839E-03 1 . 156E+01 9 . 797E-09 1 .839E-09 0.0 -0.180 0.203 0.202

0.0250 9.791E+00 3.898E-03 9.795E+00 1 . 953E-03 2. 1 99E-09 0.0 -0.173 0.199 0.193

0.0300 8. 982E+00 3.860E-03 8.986E+00 2.009E-03 2.591E-09 0.0 -0.168 0.188 0.187

0 .0350 7.559E+00 3.871E-03 7.558E+00 2.630E-03 2.869E-09 0.0 -0.169 0.182 0.182

0 . OAOO 6.891E+00 3.883E-03 6 .895E+00 3. 326E-03 3. 185E-09 0.0 -0.160 0.178 0.178

0 .0A50 6 .279E+00 3 .896E-03 6 .278E+00 9 .090E-03 3.991E-09 0.0 -0.158 0.179 0.179

0 .0500 5.813E+00 3. 909E-03 5 .81 6E+00 9.918E-03 3.789E-09 0.0 -0.155 0.171 0.171

0 .0550 5 . 929E+00 3.929E-03 5.933E+00 5.809E-03 9.078E-09 0.0 -0.153 0.169 0.168

0 .0600 5. 1 06E+00 3.939E-03 5.1 1 OE+00 6.758E-03 9 . 360E-09 0.0 -0.151 0.166 0.166

0 .0700 9.539E+00 3.973E-03 9.593E+00 8.827E-03 9 . 907E-09 0.0 -0.198 0.162 0.162

0.0800 9 . 1 99E+00 9.010E-03 9.1 98E+00 1.11 lE-02 5.931E-09 0.0 -0.195 0.159 0.159

0.0900 3 .882E+00 9.050E-03 3.886E+00 1 .359E-02 5.938E-09 0.0 -0.193 0.156 0.156

0.1000 3.630E+00 9 . 093E-03 3.639E+00 1 .625E-02 6.929E-09 0.0 -0.191 0.159 0.153

0.1250 3 . 1 70E+00 9.219E-03 3.179E+00 2.369E-02 7.599E-09 0.0 -0.137 0.199 0.199

0.1500 2 .859E+00 9.397E-03 2.863E+00 3.1 96E-02 8.705E-09 0.0 -0.133 0.195 0.195

0.1750 2.635E+00 9.990E-03 2.690E+00 9. 107E-02 9.762E-09 0.0 -0.131 0.192 0.192

0 . 2000 2.968E+00 9.693E-03 2.973E+00 5.086E-02 1 .078E-03 0.0 -0.129 0.190 0.139

0 . 2500 2.235E+00 9 . 979E-03 2.290E+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 .958E-03 0.0 -0.122 0.133 0.132

0 . 3500 1 . 977E+00 5.723E-03 1 .983E+00 1 .200E-01 1 .639E-03 0.0 -0.121 0.130 0.129

0 .9000 1 .899E+00 6 . 1 39E-03 1 .906E+00 1 .957E-01 1 .815E-03 1 .229E-02 -0.097 0.127 0.125

0.9500 1 .890E+00 6 .567E-03 1 .897E+00 1 .729E-01 1 . 990E-03 3.896E-02 -0.091 0.122 0.119

0.5000 1 . 799E+00 7.020E-03 1 .801 E+00 1 . 998E-01 2. 169E-03 6 .802E-02 -0.085 0.117 0.119

0.5500 1 .758E+00 7.991E-03 1 .765E+00 2.279E-01 2.337E-03 9.881E-02 -0.080 0.113 0.109

0.6000 1 .729E+00 7.977E-03 1 .737E+00 2.569E-01 2.510E-03 1 .303E-01 -0.076 0.109 0.109

0 .7000 1 . 687E+00 8.995E-03 1 .696E+00 3. 197E-01 2.858E-03 1 .972E-01 -0.069 0.102 0.096

0.8000 1 .659E+00 1 .006E-02 1 .669E+00 3.792E-01 3.209E-03 2.651E-01 -0.063 0.096 0.089

0 . 9000 1 .639E+00 1 . 1 18E-02 1 .650E+00 9.395E-01 3.569E-03 3.331E-01 -0.059 0.091 0.089

1 .0000 1 . 626E+00 1 .239E-02 1 .638E+00 9.953E-01 3. 923E-03 9.005E-01 -0.055 0.087 0.079

1 .2500 1 .608E+00 1 .592E-02 1 .623E+00 6.988E-01 9.890E-03 5.636E-01 -0.098 0.078 0.069

1 .5000 1 . 602E+00 1 .871E-02 1 .620E+00 8.030E-01 5.787E-03 7.168E-01 -0.093 0.072 0.062

1 .7500 1 .602E+00 2.218E-02 1 .629E+00 9.572E-01 6 .760E-03 8.599E-01 -0.090 0.067 0.056

2.0000 1 .605E+00 2.581E-02 1 .630E+00 1 .lllE+00 7.758E-03 9. 920E-01 -0.037 0.063 0.052

2.5000 1 .615E+00 3.392E-02 1 .698E+00 1 .916E+00 9.819E-03 1 .231E+00 -0.039 0.057 0.095

3.0000 1 .627E+00 9. 199E-02 1 .668E+00 1 .717E+00 1 . 1 99E-02 1 .991E+00 -0.031 0.052 0.091 3.5000 1 .639E+00 9.978E-02 1 .689E+00 2.015E+00 1 .91 lE-02 1 .627E+00 -0.029 0.099 0.038

9 .0000 1 .650E+00 5.890E-02 1 .709E+00 2.310E+00 1 .632E-02 1 .799E+00 -0.028 0.096 0.035

9.5000 1 .661 E+00 6.726E-02 1 .729E+00 2.601 E+00 1 .857E-02 1 . 997E+00 -0.027 0.099 0.033

5.0000 1 .671E+00 7.633E-02 1 .798E+00 2.888E+00 2.089E-02 2.086E+00 -0.025 0.092 0.032

5.5000 1 .681E+00 8.559E-02 1 .766E+00 3. 173E+00 2.319E-02 2.215E+00 -0.025 0.091 0.030

6 .0000 1 .690E+00 9.501E-02 1 .785E+00 3.959E+00 2.599E-02 2.335E+00 -0.029 0.039 0.029

7.0000 1 .705E+00 1 . 193E-01 1 .320E+00 9.009E+00 3.010E-02 2.552E+00 -0.022 0.037 0.027

8.0000 1 .719E+00 1 . 391 E-01 1 .853E+00 9.559E+00 3.978E-02 2.795E+00 -0.021 0.035 0.025

9.0000 1 .731 E+00 1 .593E-01 1 .886E+00 5.089E+00 3.998E-02 2. 920E+00 -0.020 0.033 0.029

10.0000 1 .792E+00 1 .798E-01 1 .917E+00 5.619E+00 9.919E-02 3.080E+00 -0.018 0.032 0.023

12.5000 1 .765E+00 2.275E-01 1 . 993E+00 6 .893E+00 5.590E-02 3.928E+00 -0.016 0.029 0.020

15.0000 1 .783E+00 2.817E-01 2.065E+00 8.125E+00 6.798E-02 3.729E+00 -0.019 0.026 0.018

17.5000 1 .799E+00 3.370E-01 2.135E+00 9.316E+00 7.886E-02 3. 981E+00 -0.012 0.029 0.016

20.0000 1 .811E+00 3.931E-01 2.209E+00 1 .097E+01 9.002E-02 9.210E+00 -0.010 0.023 0.019

25.0000 1 .832E+00 5.073E-01 2.339E+00 1 .267E+01 1 .116E-01 9.602E+00 -0.008 0.020 0.012

30.0000 1 .898E+00 6 .235E-01 2.972E+00 1 .975E+01 1 .321E-01 9. 932E+00 -0.006 0.018 0.010

35.0000 1 .862E+00 7.912E-01 2.603E+00 1 .672E+01 1 .516E-01 5.216E+00 -0.005 0.016 0.008

90.0000 1 .873E+00 8.601E-01 2.733E+00 1 .859E+01 1 .702E-01 5.966E+00 -0.009 0.015 0.007

95.0000 1 .883E+00 9.799E-01 2.863E+00 2.038E+01 1 .878E-01 5.689E+00 -0.003 0.019 0.006

50.0000 1 .892E+00 1 . 101 E+00 2. 992E+00 2.209E+01 2.095E-01 5.890E+00 -0.003 0.013 0.006

55.0000 1 . 900E+00 1 .222E+00 3. 122E+00 2.372E+01 2.209E-01 6.073E+00 -0.002 0.012 0.005

60.0000 1 . 907E+00 1 .399E+00 3.251E+00 2.529E+01 2. 356E-01 6.291E+00 -0.002 0.011 0.005

70.0000 1 . 91 9E+00 1 . 589E+00 3.509E+00 2.825E+01 2.639E-01 6 .590E+00 -0.002 0.010 0.009

80.0000 1 . 930E+00 1 .836E+00 3.766E+00 3. lOOE+01 2.898E-01 6.801E+00 -0.001 0.010 0.003

90.0000 1 . 939E+00 2.085E+00 9.029E+00 3.357E+01 3.135E-01 7.032E+00 -0.001 0.009 0.003

100.0000 1 . 998E+00 2.335E+00 9.282E+00 3.598E+01 3.353E-01 7.239E+00 -0.001 0.008 0.002

125.0000 1 . 965E+00 2. 962E+00 9.928E+00 9.192E+01 3.831E-01 7 .680E+00 -0.001 0.007 0.002

1 50.0000 1 . 979E+00 3.595E+00 5.579E+00 9.619E+01 9 .233E-01 8.092E+00 -0.000 0.007 0.001 175.0000 1 . 991 E+00 9.230E+00 6 .222E+00 5.093E+01 9.575E-01 8.398E+00 -0.000 0.006 0.001 200.0000 2.002E+00 9.869E+00 6 .870E+00 5.925E+01 9.872E-01 8.613E+00 -0.000 0.006 0.001 250.0000 2.01 9E+00 6.151E+00 8. 169E+00 6 .092E+01 5.361E-01 9.058E+00 -0.000 0.005 0.001 300.0000 2.033E+00 7.938E+00 9.971E+00 6 .660E+01 5.751E-01 9.921E+00 -0.000 0.005 0.001 350.0000 2.095E+00 8.730E+00 1 .077E+01 7. 159E+01 6 .070E-01 9.729E+00 -0.000 0.009 0.001 900.0000 2.055E+00 1 .002E+01 1 .208E+01 7.592E+01 6 . 337E-01 9. 995E+00 -0.000 0.009 0.000

950.0000 2.069E+00 1 . 132E+01 1 .339E+01 7.985E+01 6 .569E-01 1 .023E+01 -0.000 0 . 009 0.000

500 .0000 2.072E+00 1 .262E+01 1 .969E+01 8.392E+01 6 .760E-01 1 .099E+01 -0.000 0.009 0.000

550 .0000 2.080E+00 1 . 392E+01 1 .600E+01 8.668E+01 6 . 931 E-01 1 .063E+01 -0.000 0 .009 0.000

600.0000 2.086E+00 1 .522E+01 1 .731E+01 8. 968E+01 7 .083E-01 1 .080E+01 -0.000 0.003 0.000

700.0000 2.098E+00 1 .783E+01 1 . 993E+01 9.506E+01 7.339E-01 1 . 1 1 lE+01 -0.000 0.003 0.000

800.0000 2. 1 08E+00 2.099E+01 2.255E+01 9. 978E+01 7 . 598E-01 1 . 1 38E+01 -0.000 0.003 0.000 900.0000 2. 1 17E+00 2.305E+01 2.517E+01 1 .090E+02 7.722E-01 1 .161E+01 -0.000 0.003 0.000

000 .0000 2. 126E+00 2.567E+01 2.779E+01 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 = 3.180E+0C1 g/cm

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 cra^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .666E+01 7 . 28AE-03 1 .667E+01 3.503E-0A 2.300E-0A 0.0 -0.236 0.281 0.275

0.0125 1 .A12E+01 7. A99E-03 1 .A13E+01 5.1 39E-0A 2.809E-0A 0.0 -0 .22A 0.265 0.259

0.0150 1 .233E+01 7.657E-03 1 .233E+01 7.039E-0A 3.301E-0A 0.0 -0.216 0.253 0 .2A8 0.0175 1 .099E+01 7.778E-03 1 .099E+01 9.1 90E-0A 3.778E-0A 0.0 -0.209 0 .2A3 0.239

0.0200 9.9A5E+00 7 .87AE-03 9. 953E+00 1 . 1 58E-03 A.2A3E-0A 0.0 -0.203 0.235 0.231 0.0250 8.A2AE+00 8.016E-03 8. A32E+00 1 .706E-03 5.1 3SE-0A 0.0 -0.195 0.22A 0.220 0.0300 7 . 363E+00 8. 1 18E-03 7 . 371 E+00 2.3A3E-03 5.993E-0A 0.0 -0.188 0.215 0.212

0.0350 6.577E+00 8.197E-03 6 .585E+00 3.062E-03 6.813E-0A 0.0 -0.183 0.208 0.205

0 . OAOO 5 . 970E+00 8 . 263E-03 5. 979E+00 3.860E-03 7.60AE-0A 0.0 -0.179 0.202 0.200

0 . OA50 5 . A87E+00 8.31 9E-03 5.A95E+00 A . 733E-03 8.368E-0A 0.0 -0.175 0.198 0.196

0 .0500 5.093E+00 8 . 370E-03 5.101E+00 5.678E-03 9. 1 09E-0A 0 .0 -0.172 0 . 1 9A 0.192

0.0550 A . 76AE+00 8.A16E-03 A.773E+00 6.693E-03 9.829E-0A 0.0 -0.170 0.190 0.189

0 . C f) 0 0 A . A86E+00 8 . A53E-03 A. A95E+00 7.773E-03 1 .053E-03 0.0 -0.167 0.187 0.186 0.0700 A.OAlE+00 8.5A1 E-03 A.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-03 3.709E+00 1 .271E-02 1 . 31 6E-03 0.0 -0.160 0.178 0.177

0.0900 3 . A32E+00 8.70AE-03 3.AA0E+00 1 .551E-02 1 . AAOE-03 0.0 -0.157 0.17A 0.173

0.1000 3.21 3E+00 8.788E-03 3.222E+00 1 .851E-02 1 .559E-03 0.0 -0.155 0.171 0.170

0,1250 2 .81 AE+00 9 . 0 1 6E-03 2 .823E+00 2.68AE-02 1 .8A0E-03 0.0 -0.150 0.165 0.16A

0.1500 2.5AAE+00 9 . 265E-03 2.553E+00 3.617E-02 2. 102E-03 0.0 -0.1A6 0.161 0.160 0.1750 2 . 3A9E+00 9 . 53AE-03 2.359E+00 A.638E-02 2. 350E-03 0.0 -0.1A3 0.157 0.156 0.2000 2 . 203E+00 9.821E-03 2.21 3E+00 5.733E-02 2 . 586E-03 0.0 -O.IAO 0.15A 0.153

0 . 2500 2 . OOOE+00 1 .0A5E-02 2.011 E+00 8.111E-02 3.033E-03 0.0 -0.136 0.1A9 0.1 A8 0.3000 1 .867E+00 1.11 3E-02 1 .878E+00 1 .069E-01 3. A55E-03 5.037E-03 -0.125 0.1A5 0.1A3

0.3500 1 .77AE+00 1 . 187E-02 1 .786E+00 1 .3A2E-01 3.859E-03 1 .737E-02 -0.119 O.IAO 0.138

0.0000 1 .706E+00 1 .266E-02 1 .71 9E+00 1 .628E-01 A.252E-03 3.256E-02 -0.113 0.135 0.133

0 .0500 1 .656E+00 1 .3A8E-02 1 .669E+00 1 . 923E-01 A.638E-03 5.026E-02 -0.107 0.131 0.129

0 . 5000 1 .617E+00 1 . A35E-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 5.39AE-03 9.1AAE-02 -0.098 0.1 2A 0.121 0.6000 1 .563E+00 1 .618E-02 1 .579E+00 2.850E-01 5.768E-03 1 .1A1E-01 -0 .09A 0.121 0.117

0.7000 1 .528E+00 1 .812E-02 1 .5A7E+00 3.A91E-01 6 .512E-03 1 .623E-01 -0.087 0.115 0.110

0.8000 1 . 506E+00 2.016E-02 1 .526E+00 A. 1A2E-01 7.256E-03 2. 128E-01 -0.081 0.110 0.10A

0 . 9000 1 .A91E+00 2.229E-02 1 .51 3E+00 A.800E-01 8.002E-03 2.6A5E-01 -0.076 0.106 0.099

1 .0000 1 . A81 E+00 2. A50E-02 1 .505E+00 5. A63E-01 8.752E-03 3.167E-01 -0.072 0.102 0.095

1 .2500 1 . A70E+00 3.03AE-02 1 .500E+00 7.128E-01 1 .065E-02 A. A59E-01 -0 .06A 0.093 0.085

1 .5000 1 . A68E+00 3.658E-02 1 .505E+00 8.793E-01 1 .258E-02 5.700E-01 -0.059 0.087 0.078

1 .7500 1 .A71E+00 A. 31 3E-02 1 .515E+00 1 .0A5E+00 1 . A56E-02 6 .875E-01 -0 .05A 0.082 0.072

2.0000 1 . A77E+00 A.995E-02 1 .527E+00 1 .209E+00 1 .656E-02 7.980E-01 -0.051 0.078 0.067

2 . 5000 1 . A91 E+00 6. A23E-02 1 .555E+00 1 .53AE+00 2.065E-02 9. 99AE-01 -0.0A7 0.071 0.060

3.0000 1 .506E+00 7 . 922E-02 1 .585E+00 1 .852E+00 2. A81E-02 1 . 178E+00 -0 .OAA 0.066 0.055

3.5000 1 .520E+00 9. A76E-02 1 .615E+00 2.165E+00 2.903E-02 1 .338E+00 -0 .OAl 0.063 0.051

A .0000 1 . 533E+00 1 . 108E-01 1 .6AAE+00 2.A72E+00 3.328E-02 1 . A82E+00 -0.039 0.060 0 .0A8 0.5000 1 . 5A5E+00 1 .272E-01 1 .673E+00 2.773E+00 3.755E-02 1 .61 AE+00 -0.038 0.057 O.OA5

5.0000 1 . 557E+00 1 . A39E-01 1 .701E+00 3.070E+00 A. 183E-02 1 .735E+00 -0.037 0.055 0 .0A3 5.5000 1 .567E+00 1 .610E-01 1 .728E+00 3.361E+00 A. 61 lE-02 1 .8A8E+00 -0.035 0.053 O.OA1 6.0000 1 .577E+00 1 .783E-01 1 .755E+00 3.6A9E+00 5.038E-02 1 . 953E+00 -0 .03A 0.051 O.OAO 7.0000 1 .59AE+00 2.1 37E-01 1 .808E+00 A.210E+00 5.889E-02 2. 1 AAE+00 -0.032 0 .0A8 0.037

8.0000 1 . 61 OE+00 2.A99E-01 1 .859E+00 A.755E+00 6.732E-02 2.316E+00 -0.030 0 .0A6 0.035

9.0000 1 .623E+00 2.868E-01 1 .910E+00 5.286E+00 7.566E-02 2.A72E+00 -0.028 O.OAA 0.033

1 0 .0000 1 .635E+00 3.2A3E-01 1 . 959E+00 5.803E+00 8.388E-02 2.615E+00 -0.027 0.0A2 0.031 12.5000 1 . 660E+00 A. 1 99E-01 2.079E+00 7.0A1E+00 1 .039E-01 2.931E+00 -0.023 0.038 0.027

15.0000 1 . 679E+00 5.180E-01 2.1 97E+00 8.210E+00 1 .231 E-01 3.203E+00 -0.020 0.035 0.02A

17.5000 1 .695E+00 6 . 1 77E-01 2.313E+00 9.319E+00 1 .A15E-01 3. AA2E+00 -0.018 0.033 0.022

20.0000 1 .709E+00 7.189E-01 2. A28E+00 1 .037E+01 1 .590E-01 3.656E+00 -0.016 0.031 0.019

25.0000 1 .731E+00 9.2A3E-01 2.655E+00 1 .23AE+01 1 .917E-01 A.026E+00 -0.013 0.027 0.016 30.0000 1 .7A8E+00 1 . 1 33E+00 2.881E+00 1 .A15E+01 2.217E-01 A.338E+00 -0.011 0.025 0.01 A 35.0000 1 .762E+00 1 .3AAE+00 3. 106E+00 1 .582E+01 2.A91E-01 A.609E+00 -0.009 0.023 0.012

AO .0000 1 .77AE+00 1 .557E+00 3.331E+00 1 .738E+01 2.7A2E-01 A.8A8E+00 -0.008 0.021 0.010 A5.0000 1 .78AE+00 1 .771 E + 00 3.555E+00 1 .883E+01 2. 97AE-01 5.061E+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 2.20AE+00 A.005E+00 2.1A8E+01 3. 388E-01 5. A29E+00 -0.006 0.018 0.007

60.0000 1 .809E+00 2.A22E+00 A.231E+00 2.269E+01 3.57AE-01 5.590E+00 -0.006 0.017 0.007

70.0000 1 .822E+00 2.860E+00 A.682E+00 2. A9AE+01 3. 909E-01 5.878E+00 -0.005 0.016 0.006

80 .0000 1 .833E+00 3.301E+00 5.1 3AE+00 2.698E+01 A.205E-01 6.130E+00 -O.OOA 0.015 0.005

90.0000 1 .8A3E+00 3.7AAE+00 5.587E+00 2.88AE+01 A.A68E-01 6.353E+00 -O.OOA 0.01 A O.OOA

100.0000 1 .851 E+00 A. 189E+00 6.0A0E+00 3.056E+01 A.703E-01 6.55AE+00 -0.003 0.013 O.OOA 125.0000 1 .869E+00 5 . 308E+00 7. 177E+00 3.A36E+01 5.1 98E-01 6 . 983E+00 -0.003 0.012 0.003

1 50 . 0000 1 .88AE+00 6 . A3AE+00 8.317E+00 3.759E+01 5.59AE-01 7.336E+00 -0.002 0.011 0.003

1 75 .0000 1 .896E+00 7 . 565E+00 9. A60E+00 A.0A1E+01 5.91 9E-01 7.636E+00 -0.002 0.010 0.002

200.0000 1 . 906E+00 8.699E+00 1 .061E+01 A.290E+01 6 . 1 92E-01 7 .898E+00 -0.001 0.009 0.002

250 .0000 1 . 923E+00 1 .098E+01 1 .290E+01 A.717E+01 6.627E-01 8.337E+00 -0.001 0.009 0.001

300 .0000 1 . 937E+00 1 . 326E+01 1 .520E+01 5.07AE+01 6 . 959E-01 8.697E+00 -0.001 0 .008 0.001

350 .0000 1 . 9A9E+00 1 . 556E+01 1 .750E+01 5.380E+01 7.22AE-01 9.003E+00 -0.001 0.008 0.001

AOO . 0000 1 . 959E+00 1 .785E+01 1 .981E+01 5.6A8E+01 7 . AAOE-01 9.268E+00 -0.001 0.007 0.001 A50.0000 1 . 968E+00 2.015E+01 2.212E+01 5.887E+01 7.620E-01 9.502E+00 -0.000 0.007 0.001 500.0000 1 . 976E+00 2.2A6E+01 2. AA3E+01 6 . 1 02E+01 7.773E-01 9.712E+00 -0.000 0.007 0.001 550.0000 1 .983E+00 2. A76E+01 2.675E+01 6.297E+01 7 . 905E-01 9.902E+00 -0.000 0.006 0.001 600.0000 1 . 990E+00 2.707E+01 2.906E+01 6 . A77E+01 8 . 021 E-01 1 .008E+01 -0.000 0.006 0.001 700.0000 2.001E+00 3. 1 69E+01 3.369E+01 6.796E+01 8.212E-01 1 .038E+01 -0.000 0.006 0.001 800.0000 2.011 E+00 3.631E+01 3.832E+01 7.07AE+01 8.366E-01 1 .065E+01 -0.000 0.006 0.000 900.0000 2.020E+00 A.09AE+01 A.296E+01 7.320E+01 8. A92E-01 1 . 088E+01 -0.000 0.006 0.000

1000.0000 2.028E+00 A.557E+01 A.760E+01 7.5A2E+01 8 . 598E-01 1 .109E+01 -0.000 0.005 0.000

116
ELECTRONS IN CARBON DIOXIDE

I = 85.0 eV DENSITY = 1 .8A2E-03 g/cm^ (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^/g MeV cm^/g MeV cm^/g g/cm 2 0.0100 1 . 981 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 .668E+01 3 . 988E-03 1 .668E+01 4.255E-04 1 .316E-04 0.0 -0.195 0.223 0.221 0.0150 1 .<1<19E+01 <1.003E-03 1 .449E+01 5.868E-04 1 .526E-04 0.0 -0.189 0.214 0.213

0.0175 1 .286E+01 <1.012E-03 1 .287E+01 7.703E-04 1 .728E-04 0.0 -0.183 0.207 0.206

0.0200 1 . 160E+01 <1.019E-03 1 . 161E+01 9.752E-04 1 . 924E-04 0.0 -0.179 0.202 0.201 0.0250 9.780E+00 <1.029E-03 9.784E+00 1 .446E-03 2.298E-04 0.0 -0.172 0.193 0.192

0.0300 8.515E+00 <1.039E-03 8.51 9E+00 1 . 996E-03 2.654E-04 0.0 -0.167 0.187 0.186

0.0350 7.533E+00 <1.048E-03 7.587E+00 2.61 9E-03 2.994E-04 0.0 -0.163 0.182 0.181

0 .OAOO 6 .866E+00 4.059E-03 6.870E+00 3.313E-03 3.323E-04 0.0 -0.160 0.177 0.177

0 . 0A50 6.297E+00 <^.072E-03 6 .301 E+00 4.074E-03 3.641E-04 0.0 -0.157 0.174 0.173

0.0500 5 .83AE + 00 4.085E-03 5.838E+00 4.899E-03 3. 950E-04 0.0 -0.155 0.171 0.170

0.0550 5.<i99E+00 <1.100E-03 5.453E+00 5.786E-03 4.251E-04 0.0 -0.152 0.168 0.168

0.0600 5. 1 2<lE+00 <.1 16E-03 5.128E+00 6.732E-03 4.545E-04 0.0 -0.151 0.166 0.165

0.0700 < . 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 4.192E-03 4.212E+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 3.646E+00 1 .61 9E-02 6.698E-04 0.0 -0.140 0.153 0.153

0.1250 3. 180E+00 4.409E-03 3.184E+00 2.356E-02 7.920E-04 0.0 -0.136 0.149 0.148

0 . 1 500 2.868E+00 4.548E-03 2.873E+00 3. 184E-02 9.074E-04 0.0 -0.133 0.145 0.144

0 .1750 2.6<i<lE + 00 4.697E-03 2.648E+00 4.092E-02 1 .018E-03 0.0 -0.131 0.142 0.141

0 . 2000 2.<176E+00 4.855E-03 2.480E+00 5.069E-02 1 . 124E-03 0.0 -0.128 0.139 0.139

0.2500 2.242E+00 5.196E-03 2.247E+00 7. 194E-02 1 .326E-03 0.0 -0.125 0.136 0.135

0.3000 2.089E+00 5.570E-03 2.094E+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.<»000 1 .906E+C0 6.397E-03 1 .913E+00 1 .452E-01 1 .890E-03 0.0 -0.118 0.128 0.127

O.A500 1 .849E+00 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 .813E+00 1 .991E-01 2.250E-03 0.0 -0.114 0.125 0.123

0 .5500 1 .773E+00 7 .81 OE-03 1 .781E+00 2.269E-01 2.428E-03 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 .710E+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 .698E+00 3.714E-01 3.319E-03 0.0 -0.107 0.118 0.115

0.9000 1 .673E+00 1 .167E-02 1 .685E+00 4.305E-01 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 .659E+00 1 .609E-02 1 .675E+00 6 .393E-01 4.960E-03 0.0 -0.101 0.112 0.108

1 .5000 1 . 664E+00 1 . 952E-02 1 .684E+00 7.882E-01 5.899E-03 0.0 -0.099 0.109 0.105

1 .7500 1 .675E+00 2.314E-02 1 .698E+00 9.361E-01 6 .857E-03 0.0 -0.097 0.107 0.103

2.0000 1 .688E+00 2.690E-02 1 .715E+00 1 .083E+00 7.831E-03 0.0 -0.095 0.105 0.101 2.5000 1 .716E+00 3.482E-02 1 .751E+00 1 .371E+00 9.821E-03 0.0 -0.092 0.103 0.0 98 3.0000 1 .7<l<iE+00 4.315E-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 .931E+00 1 .392E-02 0.0 -0.088 0.098 0.093

A. 0000 1 .79<iE+00 6.077E-02 1 .855E+00 2.203E+00 1 .600E-02 0.0 -0.087 0.097 0.091

A. 5000 1 .81 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 .916E+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 2.074E+00 4.236E+00 3.302E-02 0.0 -0.080 0.088 0.081 9.0000 1 . 960E+00 1 .604E-01 2.121E+00 4.712E+00 3.729E-02 0.0 -0.079 0.087 0.080

10.0000 1 . 983E+00 1 .817E-01 2.165E+00 5.179E+00 4.154E-02 0.0 -0.078 0.085 0.078

12.5000 2.033E+00 2.366E-01 2.269E+00 6.306E+00 5.206E-02 0.0 -0.076 0.082 0.075

15.0000 2.07<iE+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 8.421E+00 7.252E-02 0.0 -0.073 0.078 0.070

20.0000 2.139E+00 4.091E-01 2.548E+00 9.420E+00 8.241E-02 0.0 -0.072 0.076 0.068

25.0000 2. 187E+00 5.281E-01 2.715E+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 lE+01 1 . 1 96E-01 1 .133E-01 -0.048 0.068 0.057

35.0000 2.249E+00 7.71 9E-01 3.021E+00 1 .481E+01 1 .370E-01 2.215E-01 -0.041 0.065 0.051 <0.0000 2.271E+00 8 . 958E-01 3. 167E+00 1 .642E+01 1 .535E-01 3.361E-01 -0.036 0.061 0.046

<5.0000 2.289E+00 1 .021E+00 3.310E+00 1 .797E+01 1 .693E-01 4.504E-01 -0.033 0.058 0.042

50.0000 2.305E+00 1 . 146E+00 3.451E+00 1 . 945E+01 1 .844E-01 5.614E-01 -0.030 0.055 0.038

55.0000 2.319E+00 1 .273E+00 3.591E+00 2.087E+01 1 .989E-01 6.680E-01 -0.028 0.053 0.035

60.0000 2.331E+00 1 .400E+00 3.731E+00 2.223E+01 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-01 9.585E-01 -0.024 0.047 0.029

80 .0000 2.369E+00 1 . 91 3E+00 4.282E+00 2.723E+01 2.627E-01 1 . 130E+00 -0.022 0.044 0.025

90.0000 2.38<lE+00 2. 172E+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 3.163E+01 3.054E-01 1 .427E+00 -0.020 0.039 0.021 125.0000 2.<125E+00 3.087E+00 5.512E+00 3.647E+01 3.509E-01 1 .737E+00 -0.019 0.035 0.017

150.0000 2.<l<17E+00 3.745E+00 6.193E+00 4.074E+01 3.896E-01 1 . 996E+00 -0.018 0.032 0.015

175.0000 2.<i66E+00 4.408E+00 6 .873E+00 4.457E+01 4.230E-01 2.220E+00 -0.017 0.030 0.013

200.0000 2.<181E+00 5.072E+00 7.554E+00 4.804E+01 4.523E-01 2.417E+00 -0.016 0.028 0.012

250.0000 2.507E+00 6 .408E+00 8.914E+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+01 5. 935E+01 5.404E-01 3.032E+00 -0.014 0.024 0.008

350.0000 2. 5<l<lE+00 9.094E+00 1 . 164E+01 6.392E+01 5.730E-01 3.274E+00 -0.012 0.022 0.007

<00.0000 2.559E+00 1 . 044E+01 1 .300E+01 6.798E+01 6.004E-01 3.489E+00 -0.011 0.021 0.007

<150.0000 2.571E+00 1 . 1 79E+01 1 .436E+01 7.164E+01 6 .240E-01 3.681E+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 2.591E+00 1 . 450E+01 1 .709E+01 7.801 E+01 6 .624E-01 4.018E+00 -0.009 0.019 0.005

600.0000 2.600E+00 1 .586E+01 1 .846E+01 8.083E+01 6.784E-01 4.168E+00 -0.008 0.018 0.005

700.0000 2.615E+00 1 .857E+01 2. 1 18E+01 8.588E+01 7.055E-01 4.438E+00 -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 2.401E+01 2.665E+01 9.428E+01 7.465E-01 4.891E+00 -0.005 0.016 0.003

1000.0000 2.6<i7E+00 2.673E+01 2. 938E+01 9.785E+01 7.624E-01 5.086E+00 -0.004 0.015 0.003

117
ELECTRONS IN CELLULOSE NITRATE

I = 87.0 eV DENSITY = 1 .990E+00 g/cm^

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( loo1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^

0.0100 2.028E+01 3.800E-03 2.029E+01 2 .809E-09 1 .029E-09 0.0 -0.205 0.236 0.239

0.0125 1 .708E+03 . 829E-03 1 .708E+01 9.1 58E-09 1 .239E-09 0.0 -0.196 0.229 0.222

0.0150 1 .939E+01 3 .837E-03 1 .989E+01 5.733E-09 1 .931E-09 0.0 -0.189 0.215 0.219

0.0175 1 .317E+01 3 .897E-03 1 .318E + 01 7.529E-09 1 .620E-09 0.0 -0.189 0.209 0.207

0 .0200 1 . 189E+01 3 .853E-03 1 . 189E+01 9.529E-09 1 .802E-09 0.0 -0.180 0.203 0.202

0 .0250 1 .002E+01 3.863E-03 1 .002E+01 1 .912E-03 2. 152E-09 0.0 -0.173 0.199 0.193

0.0300 8.725E+00 3.872E-03 8.729E+00 1 .999E-03 2.985E-09 0.0 -0.168 0.188 0.187

0.0350 7.771E+00 3 .882E-03 7.775E+00 2.557E-03 2.803E-09 0.0 -0.169 0.182 0.182

0 .OAOO 7 . 037E+00 3 .893E-03 7.091E+00 3.239E-03 3.11 lE-09 0.0 -0.160 0.178 0.178

0.0A50 6 . 959E+00 3. 906E-03 6.958E+00 3 . 976E-03 3 . 909E-09 0.0 -0.158 0.175 0.179

0 .0500 5 . 930E+00 3 . 91 9E-03 5.989E+00 9.781E-03 3.698E-09 0.0 -0.155 0.171 0.171 0.0550 5.585E+00 3.939E-03 5.589E+00 5.697E-03 3. 979E-09 0.0 -0.153 0.169 0.168

0.0600 5.252E+00 3 . 950E-03 5.256E+00 6.570E-03 9.259E-09 0.0 -0.151 0.166 0.166

0.0700 9.721E+00 3.985E-03 9.725E+00 8.580E-03 9.786E-09 0.0 -0.198 0.162 0.162

0.0800 9 . 31 9E+00 9.029E-03 9.318E+00 1 .080E-02 5.298E-09 0.0 -0.195 0.159 0.159

0.0900 3. 999E+00 9.066E-03 3.998E+00 1 .321E-02 5.792E-09 0.0 -0.193 0.156 0.156

0. 1000 3 . 739E+00 9.111 E-03 3.739E+00 1 .580E-02 6 .271 E-09 0.0 -0.191 0.159 0.159

0.1250 3.261E+00 9.235E-03 3.265E+00 2.298E-02 7.916E-09 0.0 -0.137 0.199 0.199

0 . 1 500 2.991E+00 9 . 370E-03 2.995E+00 3.106E-02 8.999E-09 0.0 -0.139 0.195 0.195

0 . 1750 2.71 1E+00 9 . 51 5E-03 2.71 6E+00 3.992E-02 9.533E-09 0.0 -0.131 0.192 0.192

0 . 2000 2.539E+00 9.669E-03 2.599E+00 9. 999E-02 1 .053E-03 0.0 -0.129 0.190 0.139

0.2500 2.299E+00 9. 999E-03 2.309E+00 7.016E-02 1 .293E-03 0.0 -0.125 0.136 0.135

0.3000 2. 193E+00 5.361E-03 2. 198E+00 9.268E-02 1 . 925E-03 0.0 -0.122 0.133 0.132

0.3500 2.039E+00 5.799E-03 2.090E+00 1 . 166E-01 1 .601E-03 0.0 -0.120 0.130 0.129

0 . 9000 1 . 956E + 00 6.162E-03 1 . 962E+00 1 .916E-01 1 .773E-03 0.0 -0.118 0.128 0.127

0.9500 1 .896E + 00 6 . 597E-03 1 . 903E+00 1 .675E-01 1 .993E-03 8.393E-03 -0.096 0.125 0.129

0.5000 1 .850E+00 7 .059E-03 1 .857E+00 1 .991E-01 2.112E-03 3.198E-02 -0.091 0.121 0.118

0.5500 1 .81 3E+00 7.530E-03 1 .820E+00 2.21 3E-01 2.281E-03 5.810E-02 -0.085 0.117 0.119

0 .6000 1 .783E+00 8.022E-03 1 .792E+00 2.990E-01 2.999E-03 3.61 lE-02 -0.080 0.113 0.109

0 .7000 1 . 791 E+00 9.050E-03 1 .750E+00 3.056E-01 2.789E-03 1 .960E-01 -0.072 0.106 0.101 0.8000 1 .71 2E+00 1 .013E-02 1 .722E+00 3.632E-01 3. 131 E-03 2.090E-01 -0.066 0.100 0.093

0 . 9000 1 .692E+00 1 . 126E-02 1 .703E+00 9.216E-01 3.977E-03 2.739E-01 -0.061 0.095 0.087

1 .0000 1 .678E+00 1 .299E-02 1 .691E+00 9.806E-01 3.828E-03 3.380E-01 -0.056 0.090 0.082

1 .2500 1 .660E+00 1 .559E-02 1 .675E+00 6.293E-01 9.729E-03 9.966E-01 -0.099 0.081 0.071

1 .5000 1 .659E+00 1 .887E-02 1 .673E+00 7.787E-01 5.699E-03 6.973E-01 -0.099 0.079 0.069

1 .7500 1 .659E+00 2.237E-02 1 .676E+00 9.280E-01 6.600E-03 7.886E-01 -0.090 0.069 0.058

2.0000 1 .657E+00 2.602E-02 1 .683E+00 1 .077E+00 7.575E-03 9.206E-01 -0.037 0.065 0.053

2.5000 1 .667E+00 3.368E-02 1 .701E+00 1 .372E+00 9.589E-03 1 . 159E+00 -0.033 0.058 0.096

3.0000 1 .680E+00 9.176E-02 1 .721 E+00 1 .665E+00 1 . 166E-02 1 .368E+00 -0.031 0.059 0.091 3.5000 1 .692E+00 5.016E-02 1 .792E+00 1 .953E+00 1 .378E-02 1 -559E+00 -0.029 0.050 0.038

9.0000 1 .709E+00 5.883E-02 1 .763E+00 2.239E+00 1 .599E-02 1 .721E+00 -0.028 0.097 0.035

9.5000 1 .715E+00 6 .775E-02 1 .783E+00 2.521E+00 1 .81 9E-02 1 .873E+00 -0.027 0.095 0.033

5.0000 1 .726E+00 7 . 688E-02 1 .803E+00 2.800E+00 2.035E-02 2.012E+00 -0.026 0.093 0.032

5.5000 1 .735E+00 8.620E-02 1 .822E+00 3.076E+00 2.259E-02 2. 190E+00 -0.025 0.091 0.030

6.0000 1 .795E+00 9 . 569E-02 1 .890E+00 3.399E+00 2.985E-02 2.258E+00 -0.029 0.090 0.029

7.0000 1 .761E+00 1 . 1 51 E-01 1 .876E+00 3.887E+00 2.990E-02 2.973E+00 -0.023 0.037 0.027

8.0000 1 .775E+00 1 . 351 E-01 1 . 91 OE+00 9.915E+00 3.398E-02 2.663E+00 -0.022 0.035 0.026 9.0000 1 .788E+00 1 .559E-01 1 . 999E+00 9. 939E+00 3.857E-02 2.835E+00 -0.021 0.039 0.029

10.0000 1 .800E+00 1 .762E-01 1 .976E+00 5.999E+00 9.317E-02 2.991E+00 -0.020 0.032 0.023

12.5000 1 .829E+00 2.299E-01 2.053E+00 6 .685E+00 5.969E-02 3.331E+00 -0.017 0.029 0.021 15.0000 1 .893E+00 2.892E-01 2. 127E+00 7.881E+00 6 .599E-02 3.61 9E+00 -0.015 0.027 0.019

17.5000 1 .859E+00 3.901E-01 2.1 99E+00 9.036E+00 7.716E-02 3.870E+00 -0.013 0.025 0.017

20.0000 1 .873E+00 3. 969E-01 2.270E+00 1 .016E+01 8.812E-02 9.093E+00 -0.012 0.029 0.016

25.0000 1 .895E+00 5. 126E-01 2.907E+00 1 .229E+01 1 .093E-01 9.978E+00 -0.009 0.021 0.013

30.0000 1 . 91 2E+00 6 . 303E-01 2.592E+00 1 .931E+01 1 .295E-01 9.802E+00 -0.007 0.019 0.011 35.0000 1 . 926E+00 7.995E-01 2.676E+00 1 .623E+01 1 .988E-01 5.083E+00 -0.006 0.017 0.009

90.0000 1 . 938E+00 8.699E-01 2.808E+00 1 .805E+01 1 .671E-01 5.330E+00 -0.005 0.016 0.008

95.0000 1 .998E+00 9. 91 3E-01 2.990E+00 1 . 980E+01 1 .895E-01 5.552E+00 -0.009 0.015 0.007

50.0000 1 . 958E+00 1.11 3E+00 3.071E+00 2.196E+01 2.010E-01 5.751E+00 -0.003 0.019 0.006 55.0000 1 . 966E+00 1 .236E+00 3.202E+00 2.305E+01 2.168E-01 5. 939E+00 -0.003 0.013 0.006

60.0000 1 . 973E+00 1 . 360E+00 3.333E+00 2.958E+01 2.318E-01 6 . 1 01 E+00 -0.002 0.012 0.005

70.0000 1 . 986E+00 1 .609E+00 3.595E+00 2.797E+01 2.599E-01 6.399E+00 -0 .002 0.011 0.009

80.0000 1 . 997E+00 1 .859E+00 3 .856E+00 3.016E+01 2.856E-01 6.660E+00 -0.001 0.010 0.009

90.0000 2.007E+00 2.11 1E+00 9.1 18E+00 3.267E+01 3.091E-01 6.891E+00 -0.001 0.009 0.003

100.0000 2.015E+00 2.369E+00 9.379E+00 3.502E+01 3.309E-01 7.098E+00 -0.001 0.009 0.003

125.0000 2.033E+00 3 . OOOE+00 5.039E+00 9.039E+01 3.785E-01 7.538E+00 -0.001 0.008 0.002

150.0000 2 . 098E+00 3.691 E+00 5.689E+00 9.501E+01 9 . 186E-01 7.899E+00 -0.000 0.007 0.002

175.0000 2.060E+00 9 . 285E+00 6 . 396E+00 9.917E+01 9.528E-01 8.205E+00 -0.000 0.006 0.001

200 .0000 2.071E+00 9 . 932E+00 7.003E+00 5.292E+01 9.825E-01 8.971E+00 -0.000 0.006 0.001 250.0000 2.089E+00 6 . 232E+00 8.320E+00 5. 996E+01 5.316E-01 8. 91 5E+00 -0.000 0.005 0.001 300.0000 2 . 1 03E+00 7 .537E+00 9.690E+00 6.509E+01 5.707E-01 9.279E+00 -0.000 0 .005 0.001 350.0000 2 . 1 1 5E+00 8.896E+00 1 .096E+01 6 . 990E+01 6 .027E-01 9.586E+00 -0.000 0 .005 0.001 900.0000 2. 126E+00 1 .016E+01 1 .228E + 01 7.921E+01 6.296E-01 9.853E+00 -0 .000 0.009 0 .000 950 .0000 2 . 1 35E+00 1 . 197E+01 1 . 36 1 E + 0

7.807E+01 6.529E-01 1 .009E+01 -0.000 0.009 0 .000 500.0000 2. 1 93E+00 1 .279E+01 1 .993E + 01 8.158E+01 6.722E-01 1 .030E + 01 -0 .000 0.009 0 .000 550 .0000 2. 1 51 E+00 1.911 E+01 1 .626E + 01 8.979E+01 6 .895E-01 1 .099E+01 -0.000 0.009 0.000 600.0000 2.1 58E+00 1 .593E + 01 1 .759E + 01 8.779E+01 7.097E-01 1 .066E+01 -0.000 0 .009 0.000

700.0000 2. 170E+00 1 .807E+01 2.029E+01 9.309E+01 7.305E-01 1 .097E+01 -0.000 0.003 0.000

800 .0000 2. 181E+00 2.072E+01 2.290E+01 9.768E+01 7.516E-01 1 . 1 29E+01 -0.000 0.003 0.000

900.0000 2.1 90E+00 2.337E+01 2.556E+01 1 .018E+02 7.692E-01 1 . 1 97E+01 -0.000 0.003 0.000

1000.0000 2.1 98E+00 2.602E+01 2.822E+01 1 .055E+02 7.891E-01 1 .168E+01 -0.000 0.003 0.000

118
ELECTRONS IN CERIC SULFATE DOSIMETER SOLUTION

I = 76.7 eV DENSITY = 1 .030E+0C1 g/cm^

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. dClog )/d(] og I

COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.237E+01 3 . 996E-03 2.237E+01 2.538E-06 9.703E-05 0.0 -0.200 0.229 0.226

0.0125 1 .881E+01 6.031E-03 1 .882E+01 3.762E-06 1 . 169E-06 0.0 -0.191 0.218 0.216

0.0150 1 .633E+01 6.052E-03 1 .633E+01 5.1 93E-06 1 .360E-06 0.0 -0.185 0.209 0.208

0.0175 1 .669E+01 6.067E-03 1 .669E+01 6.821E-06 1 .563E-06 0.0 -0.180 0.203 0.202

0.0200 1 . 307E+01 6 .078E-03 1 .307E+01 8.660E-06 1 . 721 E-06 0.0 -0.176 0.198 0.197

0.0250 1 .101E+01 6.096E-03 1 . 101E+01 1 .283E-03 2.061E-06 0.0 -0.169 0.189 0.189

0.0300 9.577E+00 6. 108E-03 9.581E+00 1 .771E-03 2.385E-06 0.0 -0.166 0.183 0.182

0.0350 8.525E+00 6 . 1 20E-03 8.529E+00 2.325E-03 2.696E-06 0.0 -0.161 0.178 0.178

0 . OAOO 7.717E+00 6.136E-03 7.721E+00 2.962E-03 2. 996E-06 0.0 -0.157 0.176 0.176

0 .0050 7.075E+00 6 . 1 68E-03 7.079E+00 3.620E-03 3.286E-06 0.0 -0.155 0.171 0.170

0.0500 6 . 553E + 00 6. 166E-03 6.557E+00 6.356E-03 3.568E-06 0.0 -0.152 0.168 0.167

0 .0550 6.11 9E+00 6. 180E-03 6.123E+00 5. 166E-03 3.863E-06 0.0 -0.150 0.165 0.165

0.0600 5.753E+00 6.1 98E-03 5.757E+00 5.987E-03 6.111E-06 0.0 -0.168 0.163 0.163

0.0700 5. 169E+00 6.236E-03 5. 173E+00 7.823E-03 6.630E-06 0.0 -0.165 0.159 0.159

0.0800 6.722E+00 6.278E-03 6.727E+00 9.868E-03 5.129E-06 0.0 -0.163 0.156 0.156

0.0900 6 . 370E+00 6.326E-03 6.376E+00 1 .205E-02 5.61 lE-06 0.0 -0.160 0.153 0.153

0.1000 6.085E+00 6. 373E-03 6.090E+00 1 .662E-02 6 .079E-06 0.0 -0.138 0.151 0.151 0.1250 3.566E+00 6.505E-03 3.570E+00 2.099E-02 7.196E-06 0.0 -0.136 0.166 0.166

0 . 1 500 3.21 5E+00 6.669E-03 3.21 9E+00 2.838E-02 8.253E-06 0.0 -0.131 0.163 0.162

0.1750 2.963E+00 6.803E-03 2.967E+00 3.668E-02 9.263E-06 0.0 -0.129 0.160 0.139

0.2000 2.773E+00 6. 966E-03 2.778E+00 6.520E-02 1 .023E-03 0.0 -0.127 0.137 0.137

0.2500 2.51 1E+00 5.316E-03 2.51 6E+00 6 .618E-02 1 .209E-03 0.0 -0.123 0.136 0.133

0.3000 2.339E+00 5.700E-03 2.366E+00 8.681E-02 1 . 386E-03 0.0 -0.120 0.131 0.130

0.3500 2.21 9E+00 6.111E-03 2.226E+00 1 .067E-01 1 .558E-03 0.0 -0.118 0.128 0.127

O.AOOO 2. 1 33E+00 6 .568E-03 2. 160E+00 1 .297E-01 1 .726E-03 0.0 -0.116 0.126 0.125

0.6500 2.069E+00 7 .009E-03 2.076E+00 1 .536E-01 1 .892E-03 0.0 -0.116 0.125 0.123

0.5000 2.021E+00 7.692E-03 2.028E+00 1 .778E-01 2.056E-03 0.0 -0.109 0.123 0.121 0.5500 1 . 981 E+00 7.995E-03 1 . 989E+00 2.027E-01 2.220E-03 1 .326E-02 -0.096 0.120 0.118

0.6000 1 . 950E+00 8.515E-03 1 . 959E+00 2.280E-01 2.383E-03 3.216E-02 -0.088 0.117 0.116

0.7000 1 . 906E+00 9.602E-03 1 .916E+00 2.797E-01 2.712E-03 7.786E-02 -0.078 0.110 0.106

0.8000 1 .873E+00 1 .076E-02 1 .886E+00 3.326E-01 3.063E-03 1 .307E-01 -0.070 0.105 0.099

0 . 9000 1 .852E+00 1 . 1 96E-02 1 .863E+00 3.858E-01 3.377E-03 1 .876E-01 -0.066 0.099 0.093

1 .0000 1 .837E+00 1 .318E-02 1 .850E+00 6.397E-01 3.716E-03 2.670E-01 -0.059 0.095 0.087

1 .2500 1 .81 6E+00 1 .666E-02 1 .833E+00 5.756E-01 6.582E-03 3. 983E-01 -0.050 0.085 0.075

1 .5000 1 .81 OE+00 1 . 997E-02 1 .830E+00 7.121E-01 5.676E-03 5.670E-01 -0.063 0.077 0.066

1 .7500 1 .809E+00 2.367E-02 1 .833E+00 8.687E-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 9.869E-01 7.337E-03 8.236E-01 -0.035 0.067 0.056

2.5000 1 .822E+00 3.561E-02 1 .858E+00 1 .255E+00 9.281E-03 1 .069E+00 -0.031 0.059 0.066

3.0000 1 .836E+00 6.613E-02 1 .879E+00 1 .523E+00 1 . 129E-02 1 .287E+00 -0.028 0.056 0.060

3.5000 1 .867E+00 5.299E-02 1 .900E+00 1 .788E+00 1 .336E-02 1 .681E+00 -0.026 0.050 0.036

6.0000 1 .859E+00 6 .216E-02 1 .921E+00 2.069E+00 1 .566E-02 1 .656E+00 -0.026 0.066 0.036

6.5000 1 .870E+00 7. 156E-02 1 .962E+00 2.308E+00 1 .757E-02 1 .815E+00 -0.023 0 .066 0.031 5.0000 1 .881E+00 8.117E-02 1 .962E+00 2.566E+00 1 . 972E-02 1 .961E+00 -0.022 0.062 0.029

5.5000 1 .891E+00 9.099E-02 1 .982E+00 2.818E+00 2.190E-02 2.095E+00 -0.022 0.060 0.028

6.0000 1 . 900E+00 1 .010E-01 2.001E+00 3.069E+00 2.609E-02 2.21 9E+00 -0.021 0.038 0.027

7.0000 1 .917E+00 1 .215E-01 2.038E+00 3.566E+00 2.851E-02 2.666E+00 -0.020 0.036 0.025

8.0000 1 . 932E+00 1 .625E-01 2.076E+00 6.050E+00 3.296E-02 2.662E+00 -0.019 0.036 0.023

9.0000 1 . 965E+00 1 .639E-01 2.109E+00 6.529E+00 3.763E-02 2.81 9E+00 -0.019 0.032 0.022

10.0000 1 .957E+00 1 .858E-01 2.163E+00 6.999E+00 6.191E-02 2. 980E+00 -0.018 0.030 0.021 12.5000 1 .982E+00 2.618E-01 2.226E+00 6.166E+00 5.308E-02 3.328E+00 -0.016 0.028 0.019

15.0000 2.003E+00 2.996E-01 2.302E+00 7.269E+00 6.615E-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 7.506E-02 3.870E+00 -0.016 0.026 0.016

20.0000 2.035E+00 6.180E-01 2.653E+00 9.352E+00 8.573E-02 6.092E+00 -0.013 0.022 0.015

25.0000 2.059E+00 5.397E-01 2.598E+00 1 .133E+01 1 .065E-01 6.671E+00 -0.011 0.020 0.013

30.0000 2.078E+00 6 .635E-01 2.761E+00 1 .320E+01 1 .262E-01 6.790E+00 -0.009 0.018 0.011 35.0000 2.093E+00 7.889E-01 2.882E+00 1 .698E+01 1 .651E-01 5.066E+00 -0.007 0.017 0.010

60.0000 2. 106E+00 9. 155E-01 3.022E+00 1 .668E+01 1 .630E-01 5.309E+00 -0.006 0.016 0.009

65.0000 2.1 18E+00 1 .063E + 00 3. 161E+00 1 .830E+01 1 .801E-01 5.527E+00 -0.005 0.015 0.008

50.0000 2. 128E+00 1 .172E + 00 3.300E+00 1 . 986E+01 1 .963E-01 5.726E+00 -0.006 0.016 0.007

55.0000 2.137E+00 1 .301E+00 3.638E+00 2. 133E+01 2. 118E-01 5.906E+00 -0.006 0.013 0.006

60.0000 2.165E+00 1 .631E+00 3.576E+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 2.565E+01 2.563E-01 6.365E+00 -0.003 0.01 1 0.005

80.0000 2.171E+00 1 . 956E+00 6.127E+00 2.796E+01 2.796E-01 6.623E+00 -0.002 0.010 0.006

90.0000 2. 181E+00 2.221E+00 6.602E+00 3.030E+01 3.030E-01 6.853E+00 -0.002 0.010 0.006

100.0000 2.1 91E+00 2.687E+00 6.678E+00 3.250E+01 3.265E-01 7.059E+00 -0.001 0.009 0.003

125.0000 2.210E+00 3. 156E+00 5.367E+00 3.769E+01 3.718E-01 7.697E+00 -0.001 0.008 0.002

150.0000 2.226E+00 3.830E+00 6.056E+00 6.187E+01 6.117E-01 7.857E+00 -0.001 0.007 0.002

175.0000 2.260E+00 6.507E+00 6.767E+00 6.578E+01 6.659E-01 8. 162E+00 -0.001 0.006 0.002

200 .0000 2.251 E+00 5. 187E+00 7.638E+00 6.931E+01 6.755E-01 8.627E+00 -0.000 0.006 0.001 250.0000 2.270E+00 6 . 553E+00 8.826E+00 5.567E+01 5.267E-01 8.871E+00 -0.000 0.005 0.001 300.0000 2.286E+00 7 . 926E+00 1 .021E+01 6.076E+01 5.639E-01 9.236E+00 -0.000 0.005 0.001 350.0000 2.299E+00 9 . 302E+00 1 . 160E+01 6.533E+01 5. 962E-01 9.561E+00 -0.000 0.005 0.001

600 .0000 2.310E+00 1 .068E+01 1 .299E + 01 6 . 960E+01 6 .232E-01 9.807E+00 -0.000 0.006 0.001 650.0000 2.320E+00 1 .206E+01 1 .638E+01 7.305E+01 6 .662E-01 1 .006E+01 -0.000 0.006 0.001 500.0000 2.329E+00 1 . 365E+01 1 .578E + 01 7.637E+01 6 . 662E-01 1 . 025E + 01 -0.000 0 .006 0.000

550.0000 2.337E+00 1 .686E+01 1 .71 7E+01 7. 961 E+01 6 .837E-01 1 .066E+01 -0.000 0.006 0.000 600.0000 2.365E+00 1 .622E+01 1 .857E+01 8.221E+01 6.991E-01 1 .062E+01 -0.000 0.006 0.000

700.0000 2.358E+00 1 . 900E+01 2.1 36E+01 8.723E+0I 7.252E-01 1 .092E+01 -0.000 0.003 0.000

800.0000 2.369E+00 2. 178E + 01 2.615E+01 9. 162E+01 7.666E-01 1.11 9E+01 -0.000 0.003 0.000

900.0000 2.379E+00 2.657E+01 2.695E+01 9.556E+01 7.666E-01 1 . 163E+01 -0.000 0.003 0.000

1000.0000 2.388E+00 2.736E+01 2.975E+01 9.907E+01 7.795E-01 1 .166E+01 -0.000 0.003 0.000
ELECTRONS IN CESIUM IODIDE

I = 553.1 eV DENSITY = 9.510E+0Ct g/cm^

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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .01 9E+01 1 .709E-02 1 .020E + 01 6.289E-09 8.286E-09 0.0 -0.330 0.969 0.919

0.0125 8.803E+00 1 .839E-02 8.821 E+00 8 . 928E-09 1 . 039E-03 0 .

-0.307 0.929 0.382

0.0150 7.795E+00 1 . 998E-02 7.819E+00 1 . 1 95E-03 1 .297E-03 0.0 -0.291 0 .392 0.356

0.0175 7.025E+00 2.038E-02 7.095E+00 1 .532E-03 1 .959E-03 0.0 -0.279 0 . 368 0.337

0.0200 6.915E+00 2.11 9E-02 6.937E+00 1 . 909E-03 1 .658E-03 0.0 -0.269 0.350 0.322

0.0250 5.509E+00 2 . 290E-02 5.531E+00 2.795E-03 2.060E-03 0.0 -0.259 0 . 322 0.300 0.0300 9 .869E+00 2.390E-02 9.887E+00 3.709E-03 2.959E-03 0.0 -0.293 0.303 0.289

0.0350 9. 379E+00 2.925E-02 9.909E+00 9.789E-03 2.839E-03 0.0 -0.235 0.288 0.272

0 . 0<100 9.001E+00 2.998E-02 9 . 026E+00 5. 978E-03 3.216E-03 0 .

-0.228 0.277 0.263

0.0^50 3 . 697E+00 2.563E-02 3.723E+00 7.271E-03 3.586E-03 0.0 -0.222 0.267 0.255

0.0500 3.997E+00 2.621 E-02 3.979E+00 8.662E-03 3. 999E-03 0.0 -0.218 0.259 0.298

0.0550 3 . 238E+00 2 . 675E-02 3.265E+00 1 . 01 5E-02 9.306E-03 0.0 -0.213 0.253 0.292

0 .0600 3 . 060E+00 2.729E-02 3.087E+00 1 . 1 72E-02 9.656E-03 0.0 -0.210 0.297 0.237 0.0700 2.773E+00 2.819E-02 2.802E+00 1 .51 3E-02 5.339E-03 0.0 -0.203 0.237 0.229

0 . 0800 2.552E+00 2.896E-02 2.581E+00 1 .885E-02 6.001E-03 0.0 -0.198 0.230 0.222

0.0900 2. 376E+00 2 . 970E-02 2.906E+00 2.287E-02 6 .699E-03 0.0 -0.199 0.223 0.217

0 . 1000 2 . 233E+00 3.039E-02 2.269E+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 . 1 500 1 .791E+00 3 . 337E-02 1 .829E+00 5.206E-02 1 .015E-02 0.0 -0.177 0.200 0.195

0 . 1750 1 .661E+00 3.967E-02 1 .696E+00 6.630E-02 1 . 197E-02 0.0 -0.173 0.199 0.189

0 . 2000 1 . 569E+00 3.593E-02 1 .600E+00 8. 199E-02 1 .272E-02 0.0 -0.169 0.189 0.185

0 . 2500 1 .929E+00 3.839E-02 1 .967E+00 1 .192E-01 1 .505E-02 2.998E-09 -0.161 0.181 0.177

0 . 3000 1 . 390E+00 9.087E-02 1 .381E+00 1 .999E-01 1 .71 9E-02 9.939E-03 -0.159 0.179 0.170

0 . 3500 1 . 279E+00 9 . 392E-02 1 .322E+00 1 .865E-01 1 .91 9E-02 1 .113E-02 -0.198 0.169 0.165

0.9000 1 . 235E+00 9.606E-02 1 .281E+00 2.299E-01 2.110E-02 1 .899E-02 -0.193 0.169 0.160

0 .9500 1 .202E+00 9 .879E-02 1 .251 E+00 2.695E-01 2.292E-02 2.696E-02 -0.139 0.160 0.155

0.5000 1 . 1 78E+00 5.161E-02 1 .229E+00 3.098E-01 2.968E-02 3.993E-02 -0.135 0.156 0.151 0.5500 1 . 1 59E+00 5.999E-02 1 .21 9E+00 3.957E-01 2.638E-02 9.373E-02 -0.132 0.152 0.198

0 .6000 1 . 1 95E+00 5.795E-02 1 .202E+00 3.871E-01 2.809E-02 5.275E-02 -0.129 0.199 0.195

0.7000 1 . 1 26E+00 6.355E-02 1 . 189E+00 9.708E-01 3.127E-02 7.128E-02 -0.129 0.199 0.139

0.8000 1 . 1 1 9E+00 6.987E-02 1 . 189E+00 5.551E-01 3.939E-02 9.021E-02 -0.120 0.190 0.139

0.9000 1 . 1 08E+00 7.639E-02 1 . 189E+00 6 .396E-01 3.793E-02 1 .099E-01 -0.116 0.136 0.130

1 .0000 1 .105E+00 8.308E-02 1 . 188E+00 7 .239E-01 9.091E-02 1 . 286E-01 -0.113 0.133 0.126

1 .2500 1 . 1 06E+00 1 .005E-01 1 .207E+00 9.329E-01 9.766E-02 1 .767E-01 -0.106 0.126 0.118

1 .5000 1.11 3E+00 1 . 189E-01 1 .232E+00 1 . 1 38E+00 5.970E-02 2.295E-01 -0.101 0.120 0.111

1 .7500 1 . 123E+00 1 .379E-01 1 .261E+00 1 .339E+00 6.159E-02 2.717E-01 -0.096 0.115 0.106

2 .0000 1 . 1 33E+00 1 -579E-01 1 .291E+00 1 .535E+00 6.835E-02 3. 183E-01 -0.091 0.111 0.101 2.5000 1 . 1 59E+00 1 . 979E-01 1 .352E+00 1 .913E+00 8.159E-02 9.090E-01 -0.089 0.109 0.093

3.0000 1 . 1 73E+00 2.399E-01 1 .91 3E+00 2.275E+00 9.931E-02 9.962E-01 -0.079 0.098 0.086

3.5000 1 . 1 91E+00 2.829E-01 1 .979E+00 2.621E+00 1 .067E-01 5.797E-01 -0.079 0.099 0.080

9.0000 1 . 207E+00 3.268E-01 1 .539E+00 2.959E+00 1 .187E-01 6.592E-01 -0.071 0.090 0.076

9.5000 1 .221E+00 3.71 5E-01 1 .593E+00 3.279E+00 1 .303E-01 7.399E-01 -0.067 0.086 0.071

5 .0000 1 .239E+00 9.169E-01 1 .651 E+00 3.582E+00 1 .916E-01 8.070E-01 -0.065 0.083 0.068

5.5000 1 . 296E+00 9 .630E-01 1 .709E+00 3.879E+00 1 .525E-01 8.758E-01 -0.062 0.080 0.069

6 .0000 1 .257E+00 5.095E-01 1 .767E+00 9.167E+00 1 .631 E-01 9.919E-01 -0.060 0.078 0.062

7.0000 1 .277E+00 6.091E-01 1 .881 E+00 9.716E+00 1 .839E-01 1 .069E+00 -0.057 0.073 0.057

8.0000 1 .293E+00 7.003E-01 1 .999E+00 5.232E+00 2.025E-01 1 . 178E+00 -0.059 0.070 0.052

9.0000 1 . 308E+00 7.979E-01 2.106E+00 5.720E+00 2.206E-01 1 .283E+00 -0.051 0.067 0.099

1 0 .0000 1 .321E+00 8. 967E-01 2.218E+00 6.182E+00 2.377E-01 1 .381E+00 -0.099 0.069 0.096

12.5000 1 .398E+00 1 .198E+00 2.997E+00 7.299E+00 2.768E-01 1 .602E+00 -0.099 0.059 0.090

15.0000 1 .370E+00 1 .909E+00 2.779E+00 8.199E+00 3.112E-01 1 .798E+00 -0.090 0.059 0.035

17.5000 1 . 388E+00 1 .665E+00 3.053E+00 9.052E+00 3.920E-01 1 .973E+00 -0.037 0.051 0.032

20.0000 1 .903E+00 1 . 928E+00 3.331E+00 9.836E+00 3.695E-01 2.139E+00 -0.039 0.098 0.028

25.0000 1 .927E+00 2.963E+00 3.890E+00 1 . 122E+01 9.171E-01 2.920E+00 -0.029 0.099 0.029

30 .0000 1 . 996E+00 3.006E+00 9.951 E+00 1 .292E+01 9.567E-01 2.668E+00 -0.026 0.090 0.020

35.0000 1 . 961 E+00 3.555E+00 5.016E+00 1 .398E+01 9.909E-01 2.888E+00 -0.023 0.038 0.018

90 .0000 1 .979E+00 9 . 1 09E+00 5.583E+00 1 .993E+01 5.195E-01 3.085E+00 -0.021 0.036 0.016

95.0000 1 .985E+00 9 . 667E+00 6.152E+00 1 .528E+01 5.998E-01 3.269E+00 -0.020 0.039 0.019

50.0000 1 .995E+00 5 . 228E+00 6.723E+00 1 .606E+01 5.672E-01 3.927E+00 -0.018 0.033 0.013

55.0000 1 .503E+00 5.792E+00 7.296E+00 1 .677E+01 5.871E-01 3.577E+00 -0.017 0.031 0.012

60.0000 1.511 E+00 6.359E+00 7.870E+00 1 .793E+01 6 .099E-01 3.716E+00 -0.016 0.030 0.011 70.0000 1 .529E+00 7 .998E+00 9.023E+00 1 .862E+01 6.356E-01 3.967E+00 -0.015 0.029 0.009

80.0000 1 .536E+00 8.699E+00 1 .018E+01 1 . 966E+01 6.612E-01 9.188E+00 -0.013 0.027 0.008

90.0000 1 .596E+00 9.795E+00 1 .139E+01 2.059E+01 6 .830E-01 9.387E+00 -0.012 0.026 0.007

100.0000 1 .559E+00 1 .095E+01 1 .251E+01 2.193E+01 7.016E-01 9.567E+00 -0.011 0.025 0.007

1 25 .0000 1 .572E+00 1 . 385E+01 1 .593E+01 2. 323E+01 7.388E-01 9.957E+00 -0.009 0.023 0.005

150.0000 1 . 586E+00 1 .677E+01 1 .836E+01 2.971 E+01 7.668E-01 5.283E+00 -0.008 0.022 0.009

175.0000 1 . 598E+00 1 . 970E + 01 2. 130E+01 2.597E+01 7 .886E-01 5.562E+00 -0.007 0.021 0.009

200.0000 1 .608E+00 2.269E+01 2.929E+01 2.707E+01 8.062E-01 5.808E+00 -0.006 0 .020 0.003

250 .0000 1 . 629E+00 2.852E+01 3.01 5E+01 2.892E+01 8.330E-01 6 .223E+00 -0.005 0.019 0.003

300 .0000 1 . 637E+00 3.993E+01 3.607E+01 3.093E+01 8.526E-01 6.567E+00 -0.009 0.018 0.002

350.0000 1 . 698E+00 9.039E+01 9.1 99E+01 3.172E+01 8.677E-01 6 .860E+00 -0.009 0.017 0.002

900 .0000 1 .657E+00 9 . 627E+01 9.792E+01 3.283E+01 8.796E-01 7.11 5E+00 -0.003 0.017 0.002

950.0000 1 . 665E+00 5.220E+01 5.386E+01 3.381E+01 8.893E-01 7 . 392E+00 -0.003 0.016 0.002

500 .0000 1 .672E+00 5.813E+01 5.981E+01 3.969E+01 8 . 975E-01 7.595E+00 -0.003 0.016 0.001

550 .0000 1 .679E+00 6 .907E + 01 6 .575E+01 3.599E+01 9.099E-01 7 .729E+00 -0.002 0.015 0.001 600.0000 1 . 685E+00 7.002E+01 7.171E+01 3.622E+01 9.103E-01 7.898E+00 -0.002 0.015 0.001 700.0000 1 .695E+00 8. 1 92E + 01 8.361E+01 3.751E+01 9.200E-01 8 . 1 98E+00 -0.002 0.015 0.001 800.0000 1 .709E+00 9 . 383E+01 9.553E+01 3.863E+01 9.276E-01 8.959E+00 -0.002 0.019 0.001 900.0000 1 .712E+00 1 .057E+02 1 .075E+02 3.961E+01 9.338E-01 8.690E+00 -0.001 0.019 0.001 1000.0000 1 .71 9E+00 1 . 1 77E+02 1 . 1 99E+02 9.050E+01 9. 389E-01 8 .897E+00 -0.001 0.013 0.001

120
ELECTRONS IN ETHYLENE

I = 50,.7 eV DENSITY = 1 .175E-03 g/cn>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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.699E+01 2.837E-03 2.699E+01 2.268E-06 6 .226E-05 0.0 -0.186 0.208 0.207

0.0125 2.095E+01 2.867E-03 2.095E+01 3.365E-06 7.676E-05 0.0 -0.177 0.199 0.198

0.0150 1 .816E+01 2.856E-03 1 .816E + 01 6.631E-06 8.675E-05 0.0 -0.172 0.192 0.191 0.0175 1 .607E+01 2.860E-03 1 .607E+01 6 .098E-06 9.831E-05 0.0 -0.167 0.187 0.186

0.0200 1 .667E+01 2.866E-03 1 .667E + 01 7.761E-06 1 .095E-06 0.0 -0.166 0.182 0.182

0.0250 1 .215E+01 2.873E-03 1 .216E + 01 1 . 153E-03 1 .31 lE-06 0.0 -0.158 0.175 0.175

0.0300 1 .056E+01 2.883E-03 1 .056E+01 1 .596E-03 1 .517E-06 0.0 -0.156 0.170 0.170

0.0350 9.382E+00 2.896E-03 9.385E+00 2.099E-03 1 .716E-06 0.0 -0.151 0.166 0.165

0 . 0<i00 8.682E+00 2.905E-03 8.685E+00 2.660E-03 1 . 908E-06 0.0 -0.168 0.162 0.162

0 . 0<i50 7.768E+00 2.918E-03 7.771E+00 3.277E-03 2.095E-06 0.0 -0.165 0.159 0.159

0.0500 7 . 1 88E+00 2.931E-03 7.191E+00 3.966E-03 2.277E-06 0.0 -0.163 0.157 0.156

0.0550 6.707E+00 2. 965E-03 6.710E+00 6.667E-03 2.655E-06 0.0 -0.161 0.156 0.156

0.0600 6.301E+00 2.960E-03 6.306E+00 5.636E-03 2.629E-06 0.0 -0.160 0.152 0.152

0.0700 5.656E+00 2. 992E-03 5.657E+00 7. 1 16E-03 2.967E-06 0.0 -0.137 0.169 0.169

0.0800 5. 160E+00 3.025E-03 5. 163E+00 8. 967E-03 3.293E-06 0.0 -0.135 0.166 0.166

0.0900 6.771E+00 3.061E-03 6.776E+00 1 .098E-02 3.609E-06 0.0 -0.133 0.166 0.166

0.1000 6.657E+00 3.099E-03 6.660E+00 1 .315E-02 3. 916E-06 0.0 -0.131 0.162 0.162

0.1250 3 .886E+00 3.201 E-03 3.887E+00 1 .918E-02 6.652E-06 0.0 -0.127 0.138 0.137

0.1500 3.697E+00 3.312E-03 3.501 E+00 2.598E-02 5.352E-06 0.0 -0.125 0.135 0.136

0.1750 3.220E+00 3.629E-03 3.223E+00 3.363E-02 6 .026E-06 0.0 -0.122 0.132 0.132

0 . 2000 3.012E+00 3.553E-03 3.015E+00 6.166E-02 6.672E-06 0.0 -0.120 0.130 0.129

0.2500 2.723E+00 3.820E-03 2.727E+00 5.896E-02 7.918E-06 0.0 -0.117 0.127 0.126

0.3000 2.536E+00 6. 1 lOE-03 2.538E+00 7.801E-02 9. 1 16E-06 0.0 -0.115 0.126 0.123

0.3500 2.602E+00 6.620E-03 2.607E+00 9.827E-02 1 .028E-03 0.0 -0.113 0.122 0.121

0 .'iOOO 2.307E+00 6.750E-03 2.312E+00 1 . 1 95E-01 1 . 163E-03 0.0 -0.111 0.120 0.119

0.6500 2.236E+00 5.098E-03 2.261E+00 1 .615E-01 1 .256E-03 0.0 -0.109 0.118 0.117

0 . 5000 2. 182E+00 5.662E-03 2. 188E+00 1 .661E-01 1 .369E-03 0.0 -0.108 0.117 0.116

0.5500 2.161E+00 5.861E-03 2. 166E+00 1 .871E-01 1 .682E-03 0.0 -0.107 0.116 0.116

0.6000 2. 108E+00 6.233E-03 2.116E+00 2. 106E-01 1 .595E-03 0.0 -0.105 0.115 0.113

0.7000 2.061E+00 7.053E-03 2.068E+00 2.585E-01 1 .821E-03 0.0 -0.103 0.113 0.111 0.8000 2.032E+00 7.915E-03 2.060E+00 3.072E-01 2.069E-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 9.756E-03 2.01 lE+00 6.061E-01 2.51 lE-03 0.0 -0.099 0.108 0.106

1 .2500 1 .992E+00 1 .226E-02 2.006E+00 5.307E-01 3.106E-03 0.0 -0.096 0.106 0.103

1 .5000 1 . 996E+00 1 .690E-02 2.01 lE+00 6.553E-01 3.712E-03 0.0 -0.096 0.103 0.100

1 .7500 2.007E+00 1 .770E-02 2.026E+00 7.792E-01 6.335E-03 0.0 -0.092 0.102 0.098

2.0000 2.021E+00 2.062E-02 2.061E+00 9.022E-01 6.971E-03 0.0 -0.091 0.100 0.096

2.5000 2.051E+00 2.678E-02 2.078E+00 1 . 165E+00 6.275E-03 0.0 -0.088 0.098 0.093

3.0000 2.082E+00 3.327E-02 2. 1 15E+00 1 .383E+00 7.613E-03 0.0 -0.036 0.096 0.091 3.5000 2.1 1 lE+00 6.006E-02 2.151E+00 1 .618E+00 8.977E-03 0.0 -0.086 0.096 0.089

6.0000 2.1 39E+00 6.706E-02 2. 186E+00 1 .868E+00 1 .036E-02 0.0 -0.083 0.092 0.087

6.5000 2. 166E+00 5.626E-02 2.218E+00 2.075E+00 1 .177E-02 0.0 -0.082 0.091 0.086

5.0000 2. 187E+00 6 . 162E-02 2.269E+00 2.299E+00 1 .318E-02 0.0 -0.081 0.090 0.085

5.5000 2.209E+00 6.916E-02 2.278E+00 2.520E+00 1 .661E-02 0.0 -0.080 0.089 0.083

6.0000 2.229E+00 7.686E-02 2.306E+00 2.738E+00 1 .606E-02 0.0 -0.079 0.088 0.082

7.0000 2.266E+00 9.259E-02 2.358E+00 3. 167E+00 1 .896E-02 0.0 -0.078 0.086 0.080

8.0000 2.298E+00 1 .088E-01 2.607E+00 3.587E+00 2. 185E-02 0.0 -0.077 0.085 0.079

9.0000 2. 327E+00 1 .253E-01 2.653E+00 3. 998E+00 2.677E-02 0.0 -0.076 0.086 0.077

10.0000 2.356E+00 1 .622E-01 2.696E+00 6.602E+00 2.770E-02 0.0 -0.075 0.082 0.076

12.5000 2.610E+00 1 .855E-01 2.595E+00 5.386E+00 3.500E-02 0.0 -0.073 0.080 0.076

15.0000 2.656E+00 2.301E-01 2.687E+00 6.331E+00 6.227E-02 0.0 -0.071 0.078 0.071 17.5000 2.696E+00 2.757E-01 2.772E+00 7.267E+00 6.965E-02 0.0 -0.070 0.076 0.069

20.0000 2.529E+00 3.220E-01 2.851E+00 8.136E+00 5.655E-02 1 .778E-02 -0.059 0.076 0.067

25.0000 2.577E+00 6. 166E-01 2.996E+00 9.866E+00 7.067E-02 1 .288E-01 -0.066 0.069 0.059

30.0000 2.612E+00 5. 129E-01 3. 125E+00 1 . 168E+01 8.601E-02 2.760E-01 -0.036 0.066 0.051 35.0000 2.639E+00 6.105E-01 3.269E+00 1 .305E+01 9.717E-02 6.292E-01 -0.031 0.060 0.065

60.0000 2.660E+00 7.092E-01 3.370E+00 1 .656E+01 1 .099E-01 5.780E-01 -0.027 0.056 0.060

65.0000 2.679E+00 8.088E-01 3.688E+00 1 .602E+01 1 .223E-01 7. 1 91 E-01 -0.025 0.053 0.036

50.0000 2.695E+00 9.092E-01 3.606E+00 1 .763E+01 1 .363E-01 8.516E-01 -0.023 0.050 0.033

55.0000 2.709E+00 1 .OlOE+00 3.71 9E+00 1 .879E+01 1 .659E-01 9.757E-01 -0.022 0.067 0.030

60.0000 2.722E+00 1 .112E+00 3.833E+00 2.012E+01 1 .572E-01 1 .092E+00 -0.021 0.065 0.028

70.0000 2.763E+00 1 .316E+00 6.060E+00 2.265E+01 1 .786E-01 1 .306E+00 -0.019 0.062 0.026

80.0000 2.762E+00 1 .522E+00 6.286E+00 2.505E+01 1 . 988E-01 1 .692E+00 -0.018 0.039 0.022

90.0000 2.778E+00 1 .730E+00 6.508E+00 2.733E+01 2. 178E-01 1 .662E+00 -0.017 0.037 0.020

100.0000 2.792E+00 1 . 938E+00 6.730E+00 2. 969E+01 2.357E-01 1 .816E+00 -0.017 0.035 0.018

125.0000 2 .822E+00 2.663E+00 5.286E+00 3.669E+01 2.763E-01 2. 168E + 00 -0.015 0.031 0.015

150.0000 2.865E+00 2. 991E+00 5.837E+00 3.899E+01 3.11 9E-01 2.625E+00 -0.016 0.028 0.013

175.0000 2.865E+00 3.523E+00 6.388E+00 6.308E+01 3.636E-01 2.666E+00 -0.013 0.026 0.012

200 .0000 2.881E+00 6.057E+00 6 . 939E+00 6.686E+01 3.716E-01 2.875E+00 -0.012 0.025 0.011 250.0000 2. 908E+00 5. I31E+00 8.060E+00 5.352E+01 6.1 98E-01 3.235E+00 -0.011 0.022 0.009

300.0000 2. 930E+00 6.210E+00 9.160E+00 5. 935E+01 6.598E-01 3.539E+00 -0.009 0.020 0.008

350.0000 2. 967E+00 7.296E+00 1 .026E+01 6.652E+01 6.936E-01 3.802E+00 -0.008 0.019 0.007

600.0000 2. 962E+00 8 . 380E+00 1 . 1 36E+01 6.915E+01 5.226E-01 6.036E+00 -0.007 0.018 0.006

650 .0000 2. 976E+00 9.669E+00 1 .266E+01 7.336E+01 5.679E-01 6.266E+00 -0.006 0.017 0.005

500 .0000 2. 985E+00 1 .056E+01 1 .356E+01 7.721E+01 5.702E-01 6 .633E+00 -0.005 0.016 0.005

550.0000 2. 995E+00 1 . 165E+01 1 .665E+01 8.076E+01 5. 900E-01 6.61 3E+00 -0.006 0.015 0.006

600.0000 3.006E+00 1 .275E+01 1 .575E+01 8.605E+01 6 . 077E-01 6.775E+00 -0.006 0.015 0.006

700.0000 3.019E+00 1 .696E+01 1 .796E+01 9.000E+01 6 . 382E-01 5.065E+00 -0.003 0.016 0.003

800.0000 3.031 E+00 1 .713E+01 2.016E+01 9.525E+01 6.635E-01 5.320E+00 -0.002 0.013 0.003

900.0000 3.062E+00 1 . 933E+01 2.237E+01 9. 995E+01 6 .850E-01 5.567E+00 -0.002 0.013 0.002

1000.0000 3.052E+00 2. 153E+01 2.658E+01 1 .062E+02 7.035E-01 5.751E+00 -0.002 0.012 0.002

121
ELECTRONS IN FERROUS SULFATE DOSIMETER SOLUTION

I = 76. A eV

ENERGY STOPPING POWER COLLISION RADIATIVE TOTAL MeV MeV cm^/g MeV cm^/g MeV cm^/g

0.0100 2.291E+01 3.961E-03 2.291E+01 2 0.0125 1 .885E+01 3 . 993E-03 1 .885E + 01 3 0.0150 1 .636E+01 9.012E-03 1 .636E+01 5 0.0175 1 .952E+01 9.025E-03 1 .952E+01 6 0 .0200 1 .309E+01 9 . 039E-03 1 .309E+01 8 0.0250 1 . 102E+01 9.097E-03 1 .103E+01 1 0.0300 9 . 599E+00 9.058E-03 9.598E+00 1 0.0350 8.590E+00 9 . 069E-03 8.599E+00 2

0 .0900 7 .730E+00 9 . 081 E-03 7 .739E+00 2 0.0950 7 . 087E+00 9 . 099E-03 7.091E+00 3 0.0500 6 . 569E+00 9 . 1 08E-03 6 . 568E+00 9

0 .0550 6 . 1 29E+00 9.123E-03 6.139E+00 5

0 .0600 5.763E+00 9 . 1 90E-03 5.767E+00 5 0.0700 5 . 1 77E+00 9 . 1 76E-03 5, 181 E+00 7

0 . 0800 9.730E+00 9 . 21 6E-03 9.739E+00 9 0.0900 9 . 377E+00 9 . 260E-03 9 . 381 E+00 1

0 . 1000 9.092E+00 9 . 307E-03 9.096E+00 1 0.1250 3.571 E+00 9.936E-03 3.576E+00 2 0.1500 3.220E+00 9 . 577E-03 3.229E+00 2 0.1750 2 . 967E+00 9.728E-03 2. 972E+00 3 0.2000 2.778E+00 9 .888E-03 2.783E+00 9 0.2500 2.519E+00 5.233E-03 2.520E+00 6 0.3000 2.392E+00 5.611 E-03 2.398E+00 8

0 . 3500 2.223E+00 6.017E-03 2.229E+00 1 0.9000 2.1 37E+00 6 . 998E-03 2.193E+00 1 0.9500 2.072E+00 6 . 909E-03 2.079E+00 1 0.5000 2.023E+00 7.381E-03 2.031E+00 1 0 . 5500 1 . 989E+00 7 .878E-03 1 .992E+00 2 0.6000 1 . 953E+00 8.392E-03 1 .961E+00 2

0 .7000 1 . 907E+00 9.966E-03 1 .916E+00 2 0.8000 1 .876E+00 1 .060E-02 1 .886E+00 3

0 . 9000 1 .859E+00 1 . 178E-02 1 .866E+00 3

1 .0000 1 .839E+00 1 .300E-02 1 .852E+00 9

1 .2500 1 .81 9E+00 1 .625E-02 1 .835E+00 5

1 .5000 1 .81 2E+00 1 . 972E-02 1 .832E+00 7

1 .7500 1 .81 2E+00 2.338E-02 1 .835E+00 8 2.0000 1 .815E+00 2.71 9E-02 1 .892E+00 9 2.5000 1 .825E+00 3.520E-02 1 .860E+00 1 3.0000 1 .837E+00 9.363E-02 1 .881E+00 1 3.5000 1 .899E+00 5.290E-02 1 . 902E+00 1 9.0000 1 .861 E+00 6. 197E-02 1 . 923E+00 2 9.5000 1 .873E+00 7.078E-02 1 .999E+00 2 5.0000 1 .883E+00 8.032E-02 1 . 969E+00 2 5.5000 1 .893E+00 9.009E-02 1 . 983E+00 2 6.0000 1 . 903E+00 9 . 995E-02 2.002E+00 3 7.0000 1 . 91 9E+00 1 .202E-01 2.090E+00 3 8.0000 1 . 939E+00 1 . 91 OE-01 2.075E+00 9

9 .0000 1 .997E+00 1 .623E-01 2.110E+00 9 10.0000 1 . 959E+00 1 .890E-01 2. 193E+00 9 12.5000 1 .985E+00 2.395E-01 2.229E+00 6 15.0000 2.005E+00 2. 966E-01 2.302E+00 7 17.5000 2.022E+00 3.599E-01 2.377E+00 8 20.0000 2.037E+00 9. 192E-01 2.951E+00 9 25.0000 2.061E+00 5.398E-01 2.596E+00 1 30.0000 2.080E+00 6 .575E-01 2.738E+00 1 35.0000 2.096E+00 7 .818E-01 2.878E+00 1 90.0000 2. 1 09E+00 9.073E-01 3.016E+00 1 95.0000 2.120E+00 1 .039E+00 3. 159E+00 1 50.0000 2. 1 30E+00 1 .161E+00 3.292E+00 1 55.0000 2. 1 39E+00 1 .290E+00 3.929E+00 2 60.0000 2.197E+00 1 .918E+00 3.566E+00 2 70.0000 2. 1 61 E+00 1 . 678E+00 3.839E+00 2 80.0000 2. 1 73E+00 1 . 939E+00 9.112E+00 2 90.0000 2. 189E+00 2.201E+00 9.385E+00 3 100.0000 2. 1 93E+00 2.965E+00 9.658E+00 3 125.0000 2.213E+00 3. 129E+00 5.392E+00 3 150.0000 2.229E+00 3.797E+00 6 .026E+00 9 175.0000 2 . 292E+00 9 . 968E+00 6 .71 OE+00 9 200.0000 2.253E+00 5.193E+00 7.396E+00 9 250.0000 2.273E+00 6 .997E+00 8.770E+00 5 300.0000 2.288E+00 7 .858E+00 1 .01 5E+01 6 350 .0000 2.301E+00 9.222E+00 1 .152E+01 6 900.0000 2.313E+00 1 .059E+01 1 .290E+01 6 950.0000 2.323E+00 1 . 1 96E+01 1 .928E+01 7 500.0000 2. 332E+00 1 . 333E+01 1 . 567E+01 7 550.0000 2.390E+00 1 .971 E+01 1 .705E+01 7 600.0000 2.397E+00 1 .608E+01 1 .893E+01 8 700.0000 2.361E+00 1 .889E+01 2. 120E+01 8 800.0000 2.372E+00 2. 160E+01 2.397E+01 9 900.0000 2.382E+00 2.936E+01 2.679E+01 9 1000.0000 2.391E+00 2.71 3E+01 2.952E+01 9

= 1 .024E+00 g/cm3

RADIATION DENS . EFF. dClog )/d(logI) YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

9.615E-05 0.0 -0.200 0.228 0.226

1 . 158E-09 0.0 -0.191 0.217 0.216

1 .396E-09 0.0 -0.185 0.209 0.208

1 . 527E-09 0.0 -0.180 0.203 0.202

1 .702E-09 0.0 -0.176 0.197 0.196

2.037E-09 0.0 -0.169 0.189 0.188

2.356E-09 0 .

-0.169 0.183 0.182

2.662E-09 0.0 -0.160 0.178 0.177

2. 957E-09 0.0 -0.157 0.179 0.173

3.292E-09 0.0 -0.159 0.171 0.170

3.520E-09 0.0 -0.152 0.168 0.167

3.790E-09 0.0 -0.150 0.165 0.165

9.053E-09 0.0 -0.198 0.163 0.162

9.563E-09 0.0 -0.195 0.159 0.159

5.053E-09 0.0 -0.192 0.156 0.155

5.527E-09 0.0 -0.190 0.153 0.153

5. 986E-09 0.0 -0.138 0.151 0.150

7.083E-09 0.0 -0.139 0.196 0.196

8.120E-09 0.0 -0.131 0.193 0.192

9.111E-09 0.0 -0.129 0.190 0.139

1 .007E-03 0.0 -0.127 0.137 0.137

1 . 189E-03 0.0 -0.123 0.139 0.133

1 .363E-03 0.0 -0.120 0.131 0.130

1 .532E-03 0.0 -0.118 0.128 0.127

1 .697E-03 0.0 -0.116 0.126 0.125

1 .860E-03 0.0 -0.119 0.129 0.123

2.022E-03 0.0 -0.110 0.123 0.121

2. 183E-03 1 .262E-02 -0.099 0.120 0.118

2. 399E-03 3.1 36E-02 -0.088 0.117 0.119

2.667E-03 7.687E-02 -0.078 0.110 0.106

2. 999E-03 1 .295E-01 -0.070 0.105 0.099

3.329E-03 1 .869E-01 -0.069 0.099 0.093

3.658E-03 2.957E-01 -0.059 0.095 0.087

9.512E-03 3. 970E-01 -0.050 0.085 0.075

5.399E-03 5.958E-01 -0.093 0.077 0.066

6.302E-03 6.880E-01 -0.039 0.071 0.059

7.233E-03 8.225E-01 -0.035 0.067 0.059

9.1 53E-03 1 .068E+00 -0.031 0.059 0.096

1 . 1 19E-02 1 .286E+00 -0.028 0.059 0.090

1 .317E-02 1 .981E+00 -0.026 0.050 0.036

1 .529E-02 1 .657E+00 -0.029 0.096 0.033

1 .735E-02 1 .816E+00 -0.023 0.099 0.031

1 . 998E-02 1 . 962E+00 -0.022 0.092 0.029

2.163E-02 2.096E+00 -0.022 0.090 0.028

2.380E-02 2.220E+00 -0.021 0.038 0.026

2.818E-02 2.995E+00 -0.020 0.036 0.025

3.259E-02 2.693E+00 -0.019 0.033 0.023

3.702E-02 2.821E+00 -0.018 0.032 0.022

9. 195E-02 2.982E+00 -0.018 0.030 0.021 5.252E-02 3.330E+00 -0.016 0.028 0.019

6.399E-02 3.621E+00 -0.015 0.025 0.017

7.930E-02 3.873E+00 -0.019 0.029 0.016

8.991E-02 9.095E+00 -0.013 0.022 0.015

1 .055E-01 9.979E+00 -0.010 0.020 0.013

1 .251E-01 9.793E+00 -0.009 0.018 0.011

1 .938E-01 5.070E+00 -0.007 0.017 0.010

1 .617E-01 5.313E+00 -0.006 0.016 0.009

1 . 786E-01 5.531E+00 -0.005 0.015 0.008

1 . 993E-01 5.728E+00 -0.009 0.019 0.007

2. 103E-01 5. 908E+00 -0.009 0.013 0.006 2.250E-01 6 . 073E+00 -0.003 0.012 0.006 2.525E-01 6 . 369E+00 -0.003 0.011 0.005

2.778E-01 6 .627E+00 -0.002 0.010 0.009

3.010E-01 6 .857E+00 -0.002 0.010 0.009

3.225E-01 7 .063E+00 -0.001 0.009 0.003

3.698E-01 7.501E+00 -0.001 0.008 0.002

9.096E-01 7.861E+00 -0.001 0.007 0.002

9.937E-01 8. 167E+00 -0.001 0.006 0.002

9.739E-01 8 . 932E+00 -0.000 0.006 0.001 5.226E-01 8 .876E+00 -0.000 0.005 0.001

5.61 9E-01 9.239E+00 -0.000 0.005 0.001

5. 992E-01 9.596E+00 -0.000 0.005 0.001

6 .21 3E-01 9.812E+00 -0 .000 0.009 0.001

6 .999E-01 1 .005E+01 -0.000 0.009 0.001

6 .699E-01 1 . 026E+01 -0.000 0.009 0.000

6.81 9E-01 1 .095E+01 -0.000 0.009 0.000

6.979E-01 1 .062E+01 -0.000 0.009 0.000

7 . 236E-01 .093E+01 -0.000 0.003 0.000

7.951 E-01 1 . 1 20E+01 -0.000 0.003 0.000

7.630E-01 1 . 1 93E+01 -0 .000 0.003 0.000

7.782E-01 1 .169E+01 -0.000 0.003 0.000

DENSITY

CSDA RANGE

g/cm 2

. 533E-0A

.TSSE-O't

. 183E-0A

.808E-0A

.ezi^E-o^ •280E-03

.768E-03

.321E-03

. 937E-03

.61 3E-03

.3A7E-03

. 135E-03

.976E-03

.81 OE-03

.832E-03

.203E-02

. A39E-02

.095E-02

.833E-02

.6<13E-02

.51 3E-02

.908E-02

. A68E-02

.066E-01

.295E-01

.532E-01

.775E-01

.02AE-01

.277E-01

.793E-01

.31 9E-01 .852E-01

.390E-01

.7A7E-01

. 1 1 lE-01

. A75E-01

.835E-01 .259E+00

.521E+00

.785E+00

:.0<17E+00 ;.306E+00

:.561E + 00 ;.815E+00

I.066E+00

i.561E+00

.097E+00

.52AE+00

.995E+00

. 1 39E+00

.29'IE+OO .313E+00

.398E+00

. 133E+01

. 320E+01

. A99E+01

.668E+01

.830E+01 .986E+01

. 1 3AE+01 277E+01

.548E+01

.799E+01

.035E+01

.256E+01

.757E+01

. 1 97E+01 .590E+01

. 9A5E+01

.565E+01

.09AE+01 .557E+01

. 966E+01

. 33AE+01

.669E+01

. 97AE+01

.256E+01

. 762E+01

.205E+01

.600E+01

. 956E+01

122
ELECTRONS IN GLASS, BOROSILICATE ("PYREX". CORNING 77A0)

I = 139.0 eV DENSITY = 2.230E+0C1 g/cm^

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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .787E+01 5.900E-03 1 .788E+01 3.237E-09 1 .632E-09 0.0 -0.225 0.269 0.260

0.0125 1 .51 1E+01 5 .988E-03 1 .51 2E+01 9.769E-09 1 . 971 E-09 0.0 -0.219 0.250 0.296

0.0150 1 .317E+01 5.598E-03 1 .317E+01 6.590E-09 2.296E-09 0.0 -0.206 0.239 0.236

0.0175 1 . 172E+01 5.593E-03 1 . 173E+01 8.556E-09 2.610E-09 0.0 -0.200 0.230 0.228

0.0200 1 .060E+01 5.626E-03 1 .060E+01 1 .080E-03 2.919E-09 0.0 -0.195 0.223 0.221 0.0250 8. 962E+00 5.679E-03 8. 968E+00 1 .595E-03 3.995E-09 0.0 -0.187 0.213 0.211 0.0300 7 .822E + 00 5.707E-03 7 .828E+00 2.1 99E-03 9.098E-09 0.0 -0.181 0.205 0.203

0.0350 6 . 980E+00 5.735E-03 6 . 986E+00 2.871E-03 9.578E-09 0.0 -0.176 0.199 0.197

0 .O'iOO 6.331E+00 5.759E-03 6.336E+00 3.629E-03 5.087E-09 0.0 -0.172 0.199 0.192

0 . OA50 5.819E+00 5.781E-03 5.820E+00 9.998E-03 5.579E-09 0.0 -0.169 0.189 0.188

0.0500 5 . 393E+00 5.803E-03 5.398E+00 5.391E-03 6 .055E-09 0.0 -0.166 0.186 0.185

0 .0550 5 . 092E+00 5.829E-03 5.098E+00 6.300E-03 6 .518E-09 0.0 -0.169 0.182 0.182

0 .0600 9.796E+00 5.897E-03 9.752E+00 7.321E-03 6 . 968E-09 0.0 -0.162 0.180 0.179

0.0700 9.272E+00 5.893E-03 9.278E+00 9.599E-03 7.837E-09 0.0 -0.158 0.175 0.179

0.0800 3.909E+00 5 . 993E-03 3.915E+00 1 . 1 99E-02 8.668E-09 0.0 -0.155 0.171 0.170

0.0900 3 . 622E+00 5. 997E-03 3.628E+00 1 .965E-02 9.967E-09 0.0 -0.152 0.168 0.167

0 . 1 000 3.390E+00 6.055E-03 3.396E+00 1 .750E-02 1 .029E-03 0.0 -0.150 0.165 0.169

0.1250 2.966E+00 6.215E-03 2. 972E+00 2.590E-02 1 .207E-03 0.0 -0.195 0.159 0.159

0 . 1 500 2.679E+00 6 . 393E-03 2.685E+00 3.927E-02 1 .379E-03 0.0 -0.192 0.155 0.155

0 . 1750 2.973E+00 6 .588E-03 2.979E+00 9.398E-02 1 .592E-03 0.0 -0.139 0.152 0.151 0.2000 2.318E+00 6 .796E-03 2.325E+00 5.990E-02 1 .698E-03 0.0 -0.136 0.199 0.198

0.2500 2. 102E+00 7.250E-03 2. 1 10E+00 7.706E-02 1 . 995E-03 0.0 -0.132 0.195 0.199

0 . 3000 1 . 962E+00 7.799E-03 1 . 970E+00 1 .016E-01 2.277E-03 0.0 -0.129 0.191 0.190

0 . 3500 1 .869E+00 8.286E-03 1 .873E+00 1 .277E-01 2.599E-03 0.0 -0.127 0.138 0.137

0 . AOOO 1 .793E+00 8.857E-03 1 .802E+00 1 .599E-01 2.819E-03 8. 985E-03 -0.110 0.135 0.133

0.9500 1 .739E+00 9.961 E-03 1 .799E+00 1 .831E-01 3.075E-03 2.665E-02 -0.105 0.130 0.128

0.5000 1 .698E+00 1 .009E-02 1 .708E+00 2. 121E-01 3.333E-03 9.637E-02 -0.100 0.126 0.129

0.5500 1 .665E+00 1 .075E-02 1 .676E+00 2.916E-01 3.590E-03 6.760E-02 -0.095 0.123 0.119

0 .6000 1 .690E+00 1 .193E-02 1 .651E+00 2.717E-01 3.896E-03 8.997E-02 -0.091 0.119 0.115

0.7000 1 .603E+00 1 .285E-02 1 .616E+00 3.330E-01 9.359E-03 1 .371E-01 -0.085 0.119 0.109

0.8000 1 .579E+00 1 .939E-02 1 .593E+00 3.953E-01 9.873E-03 1 .860E-01 -0.080 0.108 0.103

0 . 9000 1 .563E+00 1 .590E-02 1 .579E+00 9.589E-01 5.391E-03 2.359E-01 -0.075 0.109 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 .590E+00 2.179E-02 1 .561 E+00 6.818E-01 7.290E-03 9.090E-0) -0.069 0.092 0.089

1 .5000 1 .538E+00 2.636E-02 1 .569E+00 8.918E-01 8.599E-03 5. 271 E-01 -0.059 0.086 0.077

1 .7500 1 .591E+00 3. 1 17E-02 1 .572E+00 1 .OOlE+00 9.990E-03 6.390E-01 -0.055 0.082 0.072

2.0000 1 .597E+00 3.617E-02 1 .583E+00 1 . 160E+00 1 .191E-02 7.998E-01 -0.052 0.078 0.067

2.5000 1 .561E+00 9.668E-02 1 .608E+00 1 .973E+00 1 .931E-02 9.392E-01 -0.097 0.071 0.060

3.0000 1 .576E+00 5.771E-02 1 .639E+00 1 .782E+00 1 .729E-02 1 . 1 19E+00 -0.093 0.066 0.055

3.5000 1 .590E+00 6.918E-02 1 .660E+00 2.085E+00 2.032E-02 1 .273E+00 -0.090 0.063 0.051 9.0000 1 .609E+00 8. 102E-02 1 .685E+00 2.389E+00 2.339E-02 1 .91 9E+00 -0.037 0.059 0.097

9.5000 1 .616E+00 9.315E-02 1 .709E+00 2.679E+00 2.699E-02 1 .559E+00 -0.035 0.057 0.095

5.0000 1 . 627E+00 1 .056E-01 1 .733E+00 2.970E+00 2.961E-02 1 .679E+00 -0.033 0.059 0.092

5.5000 1 .637E+00 1 . 182E-01 1 .756E+00 3.256E+00 3.275E-02 1 .797E+00 -0.031 0.052 0.090

6.0000 1 .697E+00 1.311 E-01 1 .778E+00 3.539E+00 3.590E-02 1 .907E+00 -0.030 0.050 0.038

7.0000 1 .669E+00 1 .579E-01 1 .821E+00 9.095E+00 9.222E-02 2.110E+00 -0.027 0.097 0.035

8.0000 1 .678E+00 1 .899E-01 1 .863E+00 9.638E+00 9.853E-02 2.292E+00 -0.025 0.099 0.032

9.0000 1 .691 E+00 2.119E-01 1 .903E+00 5.169E+00 5.983E-02 2.958E+00 -0.023 0.092 0.030

10.0000 1 .703E+00 2.399E-01 1 .993E+00 5.689E+00 6. 109E-02 2.61 lE+00 -0.022 0.090 0.028

12.5000 1 .726E+00 3.11 5E-01 2.038E+00 6.995E+00 7.653E-02 2.995E+00 -0.019 0.036 0.029

15.0000 1 .796E+00 3.850E-01 2.131E+00 8. 195E+00 9.159E-02 3.229E+00 -0.017 0.033 0.021 17.5000 1 .761E+00 9.599E-01 2.221E+00 9.299E+00 1 .062E-01 3.976E+00 -0.015 0.030 0.019

20.0000 1 .775E+00 5 . 360E-01 2.31 1E+00 1 .090E+01 1 .209E-01 3.695E+00 -0.019 0.028 0.017

25.0000 1 .797E+00 6.906E-01 2.987E+00 1 .298E+01 1 .979E-01 9.071E+00 -0.011 0.025 0.019

30.0000 1 .81 9E+00 8.977E-01 2.662E+00 1 .992E+01 1 .725E-01 9.388E+00 -0.010 0.023 0.012

35.0000 1 .828E+00 1 .007E+00 2.835E+00 1 .629E+01 1 .961E-01 9.661E+00 -0.008 0.021 0.011 90.0000 1 .890E+00 1 . 167E + 00 3.007E+00 1 .796E+01 2. 180E-01 9.901E+00 -0.007 0.019 0.010

95.0000 1 .851E+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 .991E+00 3.351E+00 2.1 1 1E+01 2.579E-01 5.309E+00 -0.006 0.017 0.008

55.0000 1 .868E+00 1 .655E+00 3.523E+00 2.256E+01 2.761E-01 5.986E+00 -0.005 0.016 0.007

60.0000 1 .876E+00 1 .81 9E+00 3.695E+00 2.395E+01 2. 932E-01 5.699E+00 -0.005 0.015 0.006

70.0000 1 .889E+00 2. 150E+00 9.039E+00 2.653E+01 3.296E-01 5.990E+00 -0.009 0.019 0.005

80.0000 1 .900E+00 2.983E+00 9.383E+00 2.891 E+01 3.527E-01 6 . 1 99E+00 -0.003 0.013 0.005

90.0000 1 . 909E+00 2.817E+00 9.727E+00 3.1 1 1E+01 3.782E-01 6 .920E+00 -0.003 0.012 0.009

100.0000 1 .918E+00 3. 1 53E+00 5.071E+00 3.315E+01 9.013E-01 6 .629E+00 -0.002 0.011 0.009

125.0000 1 . 936E+00 3 . 998E+00 5.939E+00 3.770E+01 9.508E-01 7.058E+00 -0.002 0.010 0.003

150.0000 1 . 950E+00 9 .898E+00 6 .798E+00 9.163E+01 9.919E-01 7.915E+00 -0.001 0.009 0.002

175.0000 1 . 963E+00 5.702E+00 7.665E+00 9.510E+01 5.259E-01 7.718E+00 -0.001 0.009 0.002

200.0000 1 . 973E+00 6 .559E+00 8.532E+00 9.819E+01 5.593E-01 7.982E+00 -0.001 0.008 0.002

250.0000 1 . 990E+00 8 . 280E+00 1 .027E+01 5.352E+01 6.01 IE-01 8.929E+00 -0.001 0.007 0.001

300 .0000 2.009E+00 1 .001E+01 1 .201E+01 5.802E+01 6 .377E-01 8.786E+00 -0.000 0.007 0.001 350.0000 2.016E+00 1 . 1 79E+01 1 .376E+01 6.190E+01 6.671E-01 9.093E+00 -0.000 0.006 0.001 900.0000 2.027E+00 1 . 398E+01 1 .550E+01 6 . 532E+01 6 . 91 9E-01 9.359E+00 -0.000 0.006 0.001 950.0000 2.036E+00 1 .522E+01 1 .725E+01 6.838E+01 7.119E-01 9.599E+00 -0.000 0.006 0.001 500.0000 2.099E+00 1 .696E+01 1 . 900E+01 7.11 9E+01 7.295E-01 9.809E+00 -0.000 0.006 0.001 550.0000 2.051E+00 1 .870E+01 2.075E+01 7.366E+01 7.997E-01 9. 999E+00 -0.000 0.005 0.001 600.0000 2.058E+00 2.095E+01 2.251E+01 7.597E+01 7.581E-01 1 .017E+01 -0.000 0.005 0.001 700.0000 2.069E+00 2.399E+01 2.601E+01 8.010E+01 7.809E-01 1 .098E+01 -0.000 0.005 0.000

800.0000 2. 080E+00 2.799E+01 2. 952E+01 8.371E+01 7.985E-01 1 .079E+01 -0.000 0.005 0.000

900.0000 2.089E+00 3.099E+01 3.303E+01 8.691E+01 8.135E-01 1 .098E+01 -0.000 0.005 0.000

1000.0000 2.097E+00 3.995E+01 3.659E+01 8. 978E+01 8.261E-01 1.11 9E+01 -0.000 0.009 0.000

123
ELECTRONS IN "KAPTON" POLYIMIDE FILM

I = 79.6 eV DENSITY = 1 .420E+00 g/cm^

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^/g MeV cm^/g MeV cm^/'g g/cm ^ 0.0100 2.059E+01 3 . 368E-03 2.059E+01 2.760E-04 9.020E-05 0.0 -0.201 0.231 0.229

0.0125 1 .732E+01 3.383E-03 1 .733E+01 4.089E-04 1 .081E-04 0.0 -0.193 0.219 0.218

0.0150 1 .504E+01 3.392E-03 1 .504E+01 5.642E-04 1 .251E-04 0.0 -0.186 0.211 0.210 0.0175 1 . 335E+01 3.399E-03 1 .335E+01 7.410E-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 .01 5E+01 1 .393E-03 1 .879E-04 0.0 -0.170 0.191 0.190

0 .0300 8.828E+00 3.422E-03 8.832E+00 1 . 923E-03 2. 1 69E-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

O.OAOO 7. 1 16E+00 3 . 443E-03 7.11 9E+00 3.1 93E-03 2.717E-04 0.0 -0.158 0.175 0.175

0.0450 6.525E+00 3.456E-03 6.528E+00 3. 928E-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 5.310E+00 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

0.0900 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 . 1 500 2 . 967E+00 3.886E-03 2.971E+00 3.076E-02 7.469E-04 0.0 -0.132 0.143 0.143

0.1750 2.735E+00 4.018E-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 2.318E+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-01 1 .568E-03 1 .309E-02 -0.095 0.125 0.123

0.4500 1 . 906E+00 5.903E-03 1 .912E+00 1 .662E-01 1 .720E-03 4. 101E-02 -0.089 0.120 0.117

0.5000 1 .859E+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 .361E-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 .717E+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 .696E+00 1 .012E-02 1 .707E+00 4.195E-01 3. 101E-03 3.426E-01 -0.057 0.090 0.082

1 .0000 1 .682E+00 1 . 118E-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 5.751E-01 -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 .001E+00 -0.038 0.062 0.051 2.5000 1 .670E+00 3.041E-02 1 .701E+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 .721E+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 .741E+00 1 .951E+00 1 .243E-02 1 .624E+00 -0.031 0.049 0.039

4.0000 1 .708E+00 5.322E-02 1 .761E+00 2.237E+00 1 .439E-02 1 .788E+00 -0.029 0.047 0.036

4.5000 1 .71 9E+00 6 . 1 32E-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 .799E+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 .818E + 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 2.314E+00 -0.025 0.040 0.030

7.0000 1 .765E+00 1 .044E-01 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-01 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-01 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 2.036E+00 6.703E+00 4.978E-02 3.387E+00 -0.016 0.030 0.021 15.0000 1 .847E+00 2.582E-01 2.105E+00 7.910E+00 6.024E-02 3.681E+00 -0.014 0.027 0.019

17.5000 1 .862E+00 3.091E-01 2.171E+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-01 4.564E+00 -0.007 0.020 0.012

30.0000 1 .913E+00 5.737E-01 2.486E+00 1 .445E+01 1 . 1 95E-01 4.897E+00 -0.005 0.018 0.010 35.0000 1 .926E+00 6.824E-01 2.609E+00 1 .641E+01 1 .376E-01 5.184E+00 -0.004 0.016 0.008

40.0000 1 . 938E + 00 7.923E-01 2.730E+00 1 .829E+01 1 .549E-01 5.437E+00 -0.003 0.015 0.007

45.0000 1 . 948E + 00 9.031E-01 2.851E+00 2.008E+01 1 .714E-01 5.662E+00 -0.003 0.014 0.006

50.0000 1 . 957E + 00 1 .015E+00 2.971E+00 2. 180E+01 1 .872E-01 5.864E+00 -0.002 0.013 0.005

55.0000 1 . 965E + 00 1 . 127E+00 3.091 E+00 2.345E+01 2.023E-01 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 .218E+00 -0.002 0.011 0.004

70.0000 1 .984E + 00 1 .467E+00 3.451E+00 2.804E+01 2.438E-01 6 .51 9E+00 -0.001 0.010 0.003

80.0000 1 . 995E+00 1 .696E+00 3.691 E+00 3.084E+01 2.686E-01 6.781E+00 -0.001 0.009 0.003

90.0000 2. 005E+00 1 . 926E+00 3.931E+00 3.346E+01 2.915E-01 7.013E+00 -0.001 0.009 0.002

100.0000 2.013E+00 2.1 57E+00 4.170E+00 3.593E+01 3. 128E-01 7 .221E+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

150.0000 2.046E+00 3 . 325E+00 5. 371 E+00 4.647E+01 3. 993E-01 8.025E+00 -0.000 0.006 0.001 175.0000 2.058E+00 3. 91 4E+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 4.506Et-00 6.574E+00 5.487E+01 4.630E-01 8.597E+00 -0.000 0.005 0.001 250.0000 2.086E+00 5.695E+00 7.781E+00 6. 185E+01 5.124E-01 9.042E+00 -0.000 0.005 0.001 300.0000 2.101E+00 6 .889E+00 8. 990E+00 6 .783E + 01 5.520E-01 9.405E+00 -0.000 0.004 0.001 350.0000 2.11 3E+00 8.088E+00 1 .020E+01 7.304E+01 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+01 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-01 1 .021E+01 -0.000 0.004 0.000 500.0000 2. 141E+00 1 . 1 70E+01 1 .384E+01 8.562E+01 6.557E-01 1 .043E+01 -0.000 0.003 0.000

550.0000 2.148E+00 1 .291E + 01 1 .505E+01 8.908E+01 6.735E-01 1 .062E+01 -0.000 0.003 0.000 600.0000 2. 155E+00 1 .41 1E + 01 1 .627E+01 9.228E+01 6 .893E-01 1 .079E+01 -0.000 0.003 0.000

700.0000 2. 167E+00 1 .654E+01 1 .870E+01 9.801E+01 7. 160E-01 1 . 1 1 OE+01 -0.000 0.003 0.000

800.0000 2.178E+00 1 .896E + 01 2.1 14E+01 1 .030E+02 7.378E-01 1 .136E+01 -0.000 0.003 0.000 900.0000 2. 187E+00 2.1 39E+01 2. 357E+01 1 .075E+02 7.561E-01 1 . 1 60E+01 -0.000 0.003 0.000

1000.0000 2.1 96E+00 2.382E+01 2.601E+01 1 . 1 15E+02 7.716E-01 1 . 181E+01 -0.000 0.003 0.000

124
ELECTRONS IN LITHIUM FLUORIDE

I = 99.0 eV DENSITY = 2.635E+0C• g/cm ^

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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .796E+01 3.678E-03 1 .796E + 01 3.181E-09 1.11 7E-09 0.0 -0.203 0.290 0.238

0.0125 1 .513E+01 3.712E-03 1 .519E+01 9.709E-09 1 .399E-09 0.0 -0.199 0.228 0.226

0.0150 1 .315E+01 3.735E-03 1 .316E1-01 6 .980E-09 1 .561E-09 0.0 -0.192 0.219 0.217

0.0175 1 . 168E+01 3.750E-03 1 . 169E+01 8.501E-09 1 .770E-09 0.0 -0.187 0.212 0.211

0 .0200 1 .055E+01 3.762E-03 1 .055E+01 1 .076E-03 1 . 973E-09 0.0 -0.182 0.206 0.205

0.0250 8.899E+00 3.779E-03 8.898E+00 1 .599E-03 2.360E-09 0.0 -0.175 0.197 0.196

0.0300 7 .798E+00 3.792E-03 7 .751 E+00 2.1 9SE-03 2.729E-09 0.0 -0.170 0.190 0.190

0.0350 6 . 902E+00 3.809E-03 6.906E+00 2.883E-03 3.0S2E-09 0.0 -0.166 0.185 0.189

0 . 0«t00 6 .252E+00 3.815E-03 6.256E+00 3.695E-03 3.923E-09 0.0 -0.162 0.181 0.180

0 . 0<i50 5.736E+00 3.827E-03 5.739E+00 9.980E-03 3.752E-09 0.0 -0.160 0.177 0.176

0.0500 5.315E+00 3.890E-03 5.31 9E+00 5.386E-03 9.071E-09 0.0 -0.157 0.179 0.173

0 .0550 9. 965E+00 3.853E-03 9. 969E+00 6.359E-03 9. 382E-09 0.0 -0.155 0.171 0.171 0.0600 9.670E+00 3.867E-03 9.679E+00 7.397E-03 9.689E-09 0.0 -0.153 0.169 0.168

0 .0700 9.1 98E+00 3.898E-03 9.202E+00 9.659E-03 5.269E-09 0.0 -0.150 0.169 0.169

0.0800 3.838E+00 3. 932E-03 3.892E+00 1 .215E-02 5.831E-09 0.0 -0.197 0.161 0.161 0.0900 3.553E+00 3. 970E-03 3.557E+00 1 .986E-02 6.372E-09 0.0 -0.199 0.158 0.158

0 . 1000 3.323E+00 9.011 E-03 3.327E+00 1 .777E-02 6.896E-09 0.0 -0.192 0.156 0.155

0 . 1250 2. 903E+00 9. 125E-03 2. 907E+00 2.589E-02 8. 193E-09 0.0 -0.138 0.151 0.150

0.1500 2.61 9E+00 9.253E-03 2.623E+00 3.992E-02 9.321E-09 0.0 -0.135 0.197 0.197

0.1750 2.91 5E+00 9.392E-03 2.91 9E+00 9.986E-02 1 .095E-03 0.0 -0.132 0.199 0.193

0.2000 2.261E+00 9.590E-03 2.266E+00 5.555E-02 1 . 153E-03 0.0 -0.130 0.191 0.191 0.2500 2.098E+00 9.863E-03 2.053E+00 7.881E-02 1 .360E-03 6.058E-03 -0.113 0.136 0.135

0 . 3000 1 . 907E+00 5.215E-03 1 .912E+00 1 .091 E-01 1 .558E-03 2.136E-02 -0.112 0.131 0.130

0.3500 1 .809E+00 5.592E-03 1 .819E+00 1 .310E-01 1 .750E-03 3.978E-02 -0.106 0.126 0.125

0.^000 1 .737E+00 5.992E-03 1 .793E+00 1 .591E-01 1 . 939E-03 6.095E-02 -0.100 0.122 0.120

0.9500 1 .683E+00 6.912E-03 1 .690E+00 1 .883E-01 2.125E-03 8.995E-02 -0.095 0.118 0.116

0.5000 1 .692E+00 6 .852E-03 1 .699E+00 2. 183E-01 2.310E-03 1 .098E-01 -0.090 0.115 0.112

0.5500 1 .609E+00 7.308E-03 1 .617E+00 2.989E-01 2.995E-03 1 .367E-01 -0.086 0.112 0.108

0.6000 1 .583E+00 7.779E-03 1 .591E+00 2.801E-0I 2.679E-03 1 .698E-01 -0.082 0.108 0.109

0.7000 1 .596E+00 8.765E-03 1 .555E+00 3.937E-01 3.098E-03 2.236E-01 -0.075 0.103 0.098

0.8000 1 .521E+00 9.800E-03 1 .530E+00 9.086E-01 3.91 9E-03 2.896E-01 -0.070 0.0 98 0.092

0.9000 1 .503E+00 1 .088E-02 1 .519E+00 9.793E-01 3.799E-03 3.967E-01 -0.065 0.099 0.087

1 .0000 1 .991E+00 1 .200E-02 1 .509E+00 5.906E-01 9.173E-03 9.093E-01 -0.060 0.090 0.083

1 .2500 1 .976E+00 1 .999E-02 1 .991E+00 7.077E-01 5.191E-03 5.699E-01 -0.052 0.082 0.073

1 .5000 1 .971E+00 1 .818E-02 1 .989E+00 8.756E-01 6.138E-03 7. 192E-01 -0.096 0.075 0.066

1 .7500 1 .971E+00 2.1 59E-02 1 .993E+00 1 .093E+00 7.163E-03 8.568E-01 -0.091 0.070 0.059

2.0000 1 .979E+00 2.505E-02 1 .999E+00 1 .210E+00 8.219E-03 9.917E-01 -0.037 0 .066 0.059

2.5000 1 .983E+00 3.299E-02 1 .515E+00 1 .592E+00 1 .038E-02 1 .290E+00 -0.032 0.059 0.097

3.0000 1 .993E+00 9.021E-02 1 .533E+00 1 .870E+00 1 .262E-02 1 .961E+00 -0.023 0.059 0.091 3.5000 1 .503E+00 9.830E-02 1 .552E+00 2.199E+00 1 .991E-02 1 .660E+00 -0.026 0.099 0.037

9.0000 1 .513E+00 5.666E-02 1 .570E+00 2.515E+00 1 .725E-02 1 .839E+00 -0.029 0.096 0.039

9.5000 1 .523E+00 6.529E-02 1 .588E+00 2.832E+00 1 . 962E-02 2.003E+00 -0.022 0.099 0.031 5.0000 1 .531 E+00 7.902E-02 1 .605E+00 3. 195E+00 2.202E-02 2.159E+00 -0.021 0.091 0.029

5.5000 1 .539E+00 8.298E-02 1 .622E+00 3.955E+00 2.999E-02 2.293E+00 -0.020 0.039 0.027

6.0000 1 .597E+00 9.21 lE-02 1 .639E+00 3.761E+00 2.687E-02 2.922E+00 -0.019 0.038 0.026

7.0000 1 .560E+00 1 .108E-01 1 .671E+00 9.365E+00 3. 178E-02 2.655E+00 -0.018 0.035 0.029

8.0000 1 .572E+00 1 .299E-01 1 .702E+00 9.958E+00 3.672E-02 2.861E+00 -0.017 0.033 0.022

9.0000 1 .583E+00 1 .999E-01 1 .732E+00 5.591E+00 9.168E-02 3.096E+00 -0.016 0.031 0.020

10.0000 1 .592E+00 1 .693E-01 1 .761E+00 6.113E+00 9.663E-02 3.219E+00 -0.016 0.029 0.019

12.5000 1 .612E+00 2.201E-01 1 .832E+00 7.509E+00 5.899E-02 3.577E+00 -0.019 0.026 0.017

15.0000 1 .629E+00 2.723E-01 1 .901E+00 8.899E+00 7. 108E-02 3.881E+00 -0.013 0.029 0.015

17.5000 1 .692E+00 3.256E-01 1 .968E+00 1 .019E+01 8.299E-02 9. 193E+00 -0.011 0.022 0.019

20.0000 1 .659E+00 3.797E-01 2.039E+00 1 .139E+01 9.963E-02 9.379E+00 -0.010 0.021 0.013

25.0000 1 .673E+00 9.896E-01 2.163E+00 1 .377E+01 1 .171E-01 9.769E+00 -0.008 0.018 0.011 30.0000 1 .688E+00 6.019E-01 2.289E+00 1 .602E+01 1 .389E-01 5.099E+00 -0.007 0.017 0.009

35.0000 1 .700E+00 7. 196E-01 2.915E+00 1 .819E+01 1 .585E-01 5.383E+00 -0.005 0.015 0.008

90.0000 1 .71 lE+00 8.289E-01 2.590E+00 2.016E+01 1 .776E-01 5.633E+00 -0.009 0.019 0.007

95.0000 1 .720E+00 9.991 E-01 2.669E+00 2.208E+01 1 . 957E-01 5.856E+00 -0.009 0.013 0.006

50.0000 1 .728E+00 1 .060E+00 2.788E+00 2.392E+01 2.129E-01 6.057E+00 -0.003 0.012 0.005

55.0000 1 .736E+00 1 . 177E+00 2. 912E+00 2.567E+01 2.292E-01 6.290E+00 -0.003 0.011 0.005

60.0000 1 .792E+00 1 .299E+00 3.036E+00 2.735E+01 2.997E-01 6.908E+00 -0.002 0.011 0.009

70.0000 1 .759E+00 1 .530E+00 3.283E+00 3.052E+01 2.735E-01 6 .707E+00 -0.002 0.010 0.009

80.0000 1 .769E+00 1 .767E+00 3.531E+00 3.396E+01 2. 998E-01 6 . 968E + 00 -0.001 0.009 0.003

90.0000 1 .772E+00 2.006E+00 3.778E+00 3.61 9E+01 3.238E-01 7.1 99E+00 -0.001 0.008 0.003

100.0000 1 .780E+00 2.295E+00 9.025E+00 3.876E+01 3.959E-01 7.906E+00 -0.001 0.008 0.002

125.0000 1 .796E+00 2.898E+00 9.699E+00 9.953E+01 3.991E-01 7.897E+00 -0.001 0.007 0.002

150.0000 1 .809E+00 3.955E+00 5.269E+00 9. 959E+01 9.393E-01 8.209E+00 -0.000 0.006 0.001 175.0000 1 .820E+00 9.065E+00 5 .885E+00 5.908E+01 9.686E-01 8.515E+00 -0.000 0.006 0.001 200.0000 1 .830E+00 9.677E+00 6 .507E+00 5.81 1E+01 9.982E-01 8.780E+00 -0.000 0.005 0.001

250 .0000 1 .896E+00 5 . 907E+00 7.753E+00 6.519E+01 5.968E-01 9.225E+00 -0.000 0.005 0.001

300 . 0000 1 .859E+00 7.192E+00 9.001E+00 7.112E+01 5.859E-01 9.588E+00 -0.000 0.009 0.001 350.0000 1 .870E+00 8.381E+00 1 .025E+01 7.633E+01 6.170E-01 9.896E+00 -0.000 0.009 0.001 900.0000 1 .879E+00 9 . 622E+00 1 . 1 50E+01 8.093E+01 6.933E-01 1 .016E+01 -0.000 0.009 0.000

950.0000 1 .888E+00 1 .087E+01 1 .275E+01 8.505E+01 6 .656E-01 1 .090E+01 -0.000 0.009 0.000

500.0000 1 .895E+00 1 .21 1E+01 1 .901E+01 8.879E+01 6.899E-01 1 .061E + 01 -0.000 0.009 0.000

550.0000 1 . 902E+00 1 . 336E+01 1 .526E+01 9.221E+01 7.018E-01 1 .080E+01 -0.000 0.003 0.000

600.0000 1 . 908E+00 1 .961E+01 1 .651E+01 9.536E+01 7.166E-01 1 .097E+01 -0.000 0.003 0.000

700.0000 1 .919E+00 1 .71 1E+01 1 . 902E+01 1 .01 OE+02 7.917E-01 1 .128E+01 -0.000 0.003 0.000

800.0000 1 . 929E+00 1 .961E+01 2. 159E+01 1 .059E+02 7.621E-01 1 . 155E+01 -0.000 0.003 0.000

900.0000 1 . 937E+00 2.21 lE+01 2.905E+01 1 . 103E+02 7.791 E-01 1 .178E+01 -0.000 0.003 0.000

1000.0000 1 .995E+00 2.962E+01 2.656E+01 1 . 193E+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.AA0E+0C• g/cm^

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^/g MeV cm^/g MeV cm^/g g/cm 2 0.0100 1 .880E+01 3.5A7E-03 1 .880E+01 3.0A0E-0A 1 .039E-0A 0.0 -0.208 0 .2A1 0.239

0.0125 1 .58AE+01 3.569E-03 1 .58AE+01 A. A9AE-0A 1 .2A5E-0A 0.0 -0.199 0.229 0.227

0.0150 1 . 377E + 01 3.582E-03 1 .377E+0I 6.192E-0A 1 . AA2E-0A 0.0 -0.192 0.220 0.218

0.0175 1 .223E+01 3.591E-03 1 .223E+01 8. 122E-0A 1 .632E-0A 0.0 -0.187 0.212 0.211

0 .0200 1 . 1 OAE + 01 3.598E-03 1 .lOAE+01 1 .028E-03 1 .81 5E-0A 0.0 -0.183 0 . 207 0.206 0.0250 9.31 1E+00 3.608E-03 9.315E+00 1 .523E-03 2. 166E-0A 0.0 -0.176 0.198 0.197

0.0300 8.111 E+00 3.617E-03 8.1 15E+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 -0.166 0.185 0.185

0 .OAOO 6 . 5A6E+00 3.638E-03 6 .550E+00 3. A82E-03 3.128E-0A 0.0 -0.163 0.181 0.180

0 . 0A50 6 .005E+00 3.6A9E-03 6 .009E+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. 1 A5E-03 3.716E-0A 0.0 -0.157 0.17A 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 7.066E-03 A.27AE-0A 0.0 -0.153 0.169 0.168

0.0700 A.396E+00 3.725E-03 A. AOOE+00 9.226E-03 A.808E-0A 0.0 -0.150 0.165 0.16A

0 . 0800 A. 01 9E+00 3.761E-03 A.022E+00 1 . 161E-02 5.321E-0A 0.0 -0 . 1 A7 0.161 0.161 0.0900 3.721E+00 3.801E-03 3.725E+00 1 . A1 9E-02 5.816E-0A 0.0 -0.1A5 0.158 0.158

0 . 1 000 3. A80E+00 3.8A3E-03 3. A8AE+00 1 .697E-02 6 .297E-0A 0.0 -0.1A2 0.156 0.156

0 . 1250 3.0AOE+00 3. 959E-03 3.0A3E+00 2. A68E-02 7.AAAE-0A 0.0 -0.138 0.151 0.151 0.1500 2.7A2E+00 A.086E-03 2.7A6E+00 3.335E-02 8.528E-0A 0.0 -0.135 0 . 1 A7 0.1 A7 0.1750 2.528E+00 A.222E-03 2.533E+00 A.285E-02 9.56AE-0A 0.0 -0.132 0. 1 AA O.IAA

0 . 2000 2. 368E+00 A.365E-03 2.373E+00 5.306E-02 1 .056E-03 0.0 -0.130 0. 1A2 O.lAl 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 5.013E-03 2.00AE+00 9.9A1E-02 1 . A28E-03 8.258E-03 -0.107 0.133 0.132

0 . 3500 1 .895E+00 5. 376E-03 1 .900E+00 1 .251E-01 1 .605E-03 3.A57E-02 -0.099 0.127 0.125

0 .AOOO 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 6.171E-03 1 .768E+00 1 .798E-01 1 .951E-03 9.625E-02 -0.087 0.116 0.113

0.5000 1 .717E+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 7.0AAE-03 1 .690E+00 2.378E-01 2.292E-03 1 .633E-01 -0.078 0.108 O.lOA

0.6000 1 .655E+00 7.50AE-03 1 .663E+00 2.676E-01 2. A63E-03 1 .979E-01 -0.075 0. 10A 0.100

0.7000 1 .615E+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 3.501E-03 A.076E-01 -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+0O 1 . A55E-02 1 .55AE+00 6.775E-01 A.761E-03 6.398E-01 -0.050 0.077 0.068

1 .5000 1 .53AE+00 1 .766E-02 1 .552E+00 8.385E-01 5.695E-03 7.928E-01 -0.0A5 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 .562E+00 1 .160E+00 7.638E-03 1 .067E+00 -0.039 0.063 0.053

2.5000 1 .5A8E+00 3. 153E-02 1 .580E+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 .793E+00 1 .175E-02 1 .51 AE+00 -0.033 0.053 0.0A2

3.5000 1 .572E+00 A.695E-02 1 .61 9E+00 2.10AE+00 1 .389E-02 1 .701E+00 -0.030 0.050 0.039

A. 0000 1 .583E+00 5.508E-02 1 .638E+00 2.A11E+00 1 .607E-02 1 .869E+00 -0.029 0.0A7 0.037

A. 5000 1 .593E+00 6.3A2E-02 1 .657E+00 2.71 AE+00 1 .828E-02 2.023E+00 -0.027 0.0A5 0.035

5.0000 1 .603E+00 7.1 97E-02 1 .675E+00 3.01 AE+00 2.051E-02 2.163E+00 -0.026 0.0A3 0.033

5.5000 1 .612E+00 8.069E-02 1 .693E+00 3.31 lE+00 2.277E-02 2.293E+00 -0.025 0.0A1 0.031 6.0000 1 .621E+00 8. 958E-02 1 .710E+00 3.605E+00 2.50AE-02 2. A15E+00 -0.02A O.OAO 0.030

7.0000 1 .636E+00 1 .078E-01 1 .7AAE+00 A. 18AE+00 2.962E-02 2.635E+00 -0.022 0.037 0.028

8.0000 1 . 6A9E+00 1 .26AE-01 1 .775E+00 A.752E+00 3. A23E-02 2.831E+00 -0.021 0.035 0.026

9.0000 1 .661E+00 1 .A55E-01 1 .806E+00 5.31 1E+00 3.886E-02 3.008E+00 -0.019 0.033 0.02A

10.0000 1 .671E+00 1 .6A9E-01 1 .836E+00 5.860E+00 A.3A9E-02 3. 170E+00 -0.018 0.032 0.023

12.5000 1 .693E+00 2. 1 A8E-01 1 .908E+00 7.1 95E+00 5.505E-02 3.52AE+00 -0.015 0.029 0.020

15.0000 1 .710E+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 .093E+01 8.878E-02 A. 31 AE+00 -0.010 0.023 0.01 A 25.0000 1 .757E+00 A.798E-01 2.237E+00 1 .323E+01 1 . 102E-01 A.710E+00 -0.008 0.020 0.012

30.0000 1 .772E+00 5. 900E-01 2.362E+00 1 .5A1E+01 1 .305E-01 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 . 1 A2E-01 2.61 1E+00 1 . 9A3E+01 1 .683E-01 5.580E+00 -0 .OOA 0.015 0.007

A5.0000 1 .806E+00 9.278E-01 2.73AE+00 2.1 30E+01 1 .858E-01 5.805E+00 -0.003 0.01A 0.006 50.0000 1 .81 AE+00 1 .OA2E+00 2.856E+00 2.309E+01 2.025E-01 6.007E+00 -0.003 0.013 0.005

55.0000 1 .822E+00 1 .157E+00 2.979E+00 2.A81E+01 2. 183E-01 6.1 91E+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 O.OOA

70.0000 1 .8A1E+00 1 .506E+00 3.3A6E+00 2. 955E+01 2.616E-01 6.660E+00 -0.001 0.010 0.003

80.0000 1 .851E+00 1 .7A0E+00 3.591E+00 3.2AAE+01 2.873E-01 6.922E+00 -0.001 0.009 0.003

90.0000 1 .860E+00 1 . 976E+00 3.836E+00 3.51 3E+01 3.11 OE-01 7. 15AE+00 -0.001 0.009 0.002

100.0000 1 .863E+00 2.212E+00 A.080E+00 3.766E+01 3.328E-01 7.361E+00 -0.001 0 .008 0.002

125.0000 1 .885E+00 2.808E+00 A.693E+00 A.337E+01 3.805E-01 7.803E+00 -0.001 0.007 0.002

1 50.0000 1 .899E+00 3.A08E+00 5.306E+00 A.838E+01 A.206E-01 8.165E+00 -0.000 0.006 0.001 175.0000 1 . 91 OE+00 A. 01 1E+00 5. 921E+00 5.283E+01 A.5A9E-01 8.A71E+00 -0.000 0.006 0.001 200.0000 1 . 920E+00 A.616E+00 6.536E+00 5.685E+01 A.8A6E-01 8.737E+00 -0.000 0.005 0.001 250.0000 1 . 937E+00 5 .832E+00 7.769E+00 6.386E+01 5.336E-01 9. 181E+00 -0.000 0.005 0.001 300.0000 1 .951E+00 7.053E+00 9.00AE+00 6.983E+01 5.726E-01 9.5A5E+00 -0.000 0.005 0.001 350.0000 1 .962E+00 8.279E+00 1 .02AE+01 7.503E+01 6.0A6E-01 9.853E+00 -0.000 0 .OOA 0.000 AOO.OOOO 1 .972E+00 9.507E+00 1 . 1 A8E+01 7.96AE+01 6.313E-01 1 .012E+01 -0.000 0 . OOA 0.000 A50.0000 1 .981E+00 1 .07AE+01 1 .272E+01 8 . 378E+01 6.5A1E-01 1 .035E+01 -0.000 O.OOA 0.000 500.0000 1 . 989E+00 1 . 1 97E+01 1 . 395E+01 8.753E+01 6 . 738E-01 1 .056E+01 -0.000 O.OOA 0.000

550.0000 1 . 996E+00 1 .320E+01 1 .520E+01 9.096E+01 6.91 IE-01 1 .076E + 01 -0.000 0.003 0.000 600.0000 2.002E+00 1 . AAAE+01 1 .6AAE+01 9. A1 3E+01 7.063E-01 1 .093E + 01 -0.000 0.003 0.000 700.0000 2.01 AE+00 1 .691E+01 1 .893E+01 9.979E+01 7.320E-01 1 . 12AE+01 -0.000 0.003 0.000

800.0000 2.02AE+00 1 . 939E+01 2.1A1E+01 1 .0A8E+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 .092E+02 7.70AE-01 1 . 17AE+01 -0.000 0.003 0.000 1000.0000 2.0AOE+00 2. A35E+01 2.639E+01 1 . 132E+02 7.853E-01 1 . 1 95E+01 -0.000 0.003 0.000

126
ELECTRONS IN METHANE

I = AI.7 eV DENSITY = 6.672E-0<i g/cm^ (20® C)

ENERGY STOPPING POWER CSDA RADIATION DEHS.EFF. ddog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.829E+01 2 . 603E-03 2.829E+01 1 . 977E-04 5.026E-05 0 .

-0.178 0.200 0.199

0.0125 2. 369E+01 2.612E-03 2.369E+01 2. 947E-04 6.045E-05 0.0 -0.171 0.191 0.191 0.0150 2.049E+01 2 . 620E-03 2.049E+01 4.085E-04 7 . 022E-05 0.0 -0.166 0.185 0.184

0.0175 1 .81 3E+01 2.625E-03 1 .813E+01 5.385E-04 7. 967E-05 0.0 -0.162 0.180 0.179

0.0200 1 .631E+01 2.630E-03 1 .632E+01 6 .840E-04 8.884E-05 0 .

-0.159 0.176 0.175

0.0250 1 .369E+01 2 . 640E-03 1 .369E+01 1 .020E-03 1 .065E-04 0.0 -0.154 0.169 0.169

0.0300 1 . 188E+01 2.651E-03 1 . 188E+01 1 .41 3E-03 1 .234E-04 0.0 -0.149 0.164 0.164

0.0350 1 .055E+01 2.662E-03 1 .056E+01 1 .861E-03 1 .397E-04 0.0 -0.146 0.160 0.160

0 .0000 9.536E+00 2.674E-03 9.539E+00 2.360E-03 1 .556E-04 0.0 -0.144 0.157 0.157

0 .0050 8.730E+00 2.687E-03 8.733E+00 2. 908E-03 1 .710E-04 0.0 -0.141 0.154 0.154

0 .0500 8.075E+00 2.700E-03 8.078E+00 3.504E-03 1 .860E-04 0.0 -0.139 0.152 0.152

0.0550 7.532E+00 2.714E-03 7.534E+00 4. 146E-03 2.006E-04 0.0 -0.138 0.150 0.150

0.0600 7.074E+00 2.728E-03 7.077E+00 4.831E-03 2. 150E-04 0.0 -0.136 0.148 0.148

0 .0700 6 . 344E+00 2.759E-03 6.347E+00 6.326E-03 2.429E-04 0.0 -0.133 0.145 0.145

0.0800 5.788E+00 2.791E-03 5.790E+00 7.978E-03 2.698E-04 0.0 -0.131 0.142 0.142

0.0900 5 . 349E+00 2.826E-03 5.352E+00 9.777E-03 2. 960E-04 0.0 -0.129 0.140 0.140

0.1000 4.995E+00 2.862E-03 4.998E+00 1 .171E-02 3.21 4E-04 0.0 -0.128 0.138 0.138

0.1250 4 . 350E+00 2. 960E-03 4.353E+00 1 .709E-02 3.825E-04 0.0 -0.124 0.134 0.134

0.1500 3.915E+00 3.066E-03 3. 918E+00 2.316E-02 4.407E-04 0.0 -0.122 0.131 0.131 0.1750 3.603E+00 3. 178E-03 3.606E+00 2. 983E-02 4.966E-04 0.0 -0.119 0.129 0.128

0.2000 3.369E+00 3.297E-03 3.372E+00 3.701E-02 5.508E-04 0.0 -0.118 0.127 0.126

0.2500 3.044E+00 3.550E-03 3.047E+00 5.266E-02 6.550E-04 0.0 -0.115 0.124 0.123

0.3000 2.831E+00 3.826E-03 2.835E+00 6.971E-02 7.554E-04 0.0 -0.112 0.121 0.120

0.3500 2.683E+00 4. 121E-03 2.687E+00 8.785E-02 8.534E-04 0.0 -0.110 0.119 0.118

O.AOOO 2.576E+00 4.434E-03 2.580E+00 1 .069E-01 9.500E-04 0.0 -0.109 0.117 0.116

0.4500 2.496E+00 4.764E-03 2.501E+00 1 .266E-01 1 .046E-03 0.0 -0.107 0.116 0.114

0.5000 2.435E+00 5.109E-03 2.440E+00 1 .468E-01 1 .141E-03 0.0 -0.106 0.114 0.113

0.5500 2.388E+00 5.467E-03 2.393E+00 1 .675E-01 1 .236E-03 0.0 -0.104 0.113 0.112

0.6000 2.351E+00 5.839E-03 2.357E+00 1 .886E-01 1 .332E-03 0.0 -0.103 0.112 0.110

0.7000 2.298E+00 6.616E-03 2.305E+00 2.315E-01 1 .523E-03 0.0 -0.101 0.110 0.108

0.8000 2.264E+00 7.432E-03 2.272E+00 2.752E-01 1 .717E-03 0.0 -0.100 0.109 0.107

0 . 9000 2.243E+00 8.287E-03 2.251E+00 3.1 95E-01 1 .912E-03 0.0 -0.098 0.107 0.105

1 .0000 2.230E+00 9.176E-03 2.239E+00 3.640E-01 2. 1 lOE-03 0.0 -0.097 0.106 0.104

1 .2500 2.217E+00 1 .153E-02 2.229E+00 4.760E-01 2.614E-03 0.0 -0.094 0.104 0.101

1 .5000 2.221E+00 1 .405E-02 2.235E+00 5.881E-01 3.133E-03 0.0 -0.092 0.101 0.098

1 .7500 2.232E+00 1 .671E-02 2.249E+00 6.996E-01 3.665E-03 0.0 -0.090 0.100 0.096

2.0000 2.247E+00 1 .949E-02 2.267E+00 8. 103E-01 4.208E-03 0.0 -0.089 0.098 0.094

2.5000 2.280E+00 2.534E-02 2.306E+00 1 .029E+00 5.325E-03 0.0 -0.087 0.096 0.092

3.0000 2.314E+00 3.152E-02 2.345E+00 1 .244E+00 6.473E-03 0.0 -0.085 0.094 0.089

3.5000 2.345E+00 3.795E-02 2.383E+00 1 .456E+00 7.645E-03 0.0 -0.083 0.092 0.088

4.0000 2.375E+00 4.462E-02 2.420E+00 1 .664E+00 8.837E-03 0.0 -0.082 0.091 0.086

4.5000 2.403E+00 5. 148E-02 2.454E+00 1 .869E+00 1 .004E-02 0.0 -0.081 0.090 0.085

5.0000 2.428E+00 5.852E-02 2.487E+00 2.071E+00 1 . 127E-02 0.0 -0.080 0.088 0.083

5.5000 2.452E+00 6.571E-02 2.517E+00 2.271E+00 1 .250E-02 0.0 -0.079 0.087 0.082

6.0000 2.474E+00 7.303E-02 2.547E+00 2.469E+00 1 .374E-02 0.0 -0.078 0.087 0.081 7.0000 2.51 4E+00 8.805E-02 2.602E+00 2.857E+00 1 .624E-02 0.0 -0.077 0.085 0.079

8.0000 2.549E+00 1 .035E-01 2.653E+00 3.238E+00 1 .876E-02 0.0 -0.075 0.084 0.078

9.0000 2.581E+00 1 . 1 93E-01 2.700E+00 3.61 lE+00 2.130E-02 0.0 -0.074 0.082 0.077

10.0000 2.610E+00 1 .354E-01 2.745E+00 3. 978E+00 2.385E-02 0.0 -0.074 0.081 0.075

12.5000 2.671E+00 1 .767E-01 2.848E+00 4.872E+00 3.022E-02 0.0 -0.072 0.079 0.073

15.0000 2.722E+00 2.1 94E-01 2.941E+00 5.736E+00 3.657E-02 0.0 -0.070 0.077 0.071 17.5000 2.765E+00 2.629E-01 3.028E+00 6.573E+00 4.288E-02 0.0 -0.069 0.075 0.069

20.0000 2.803E+00 3.073E-01 3. 1 10E+00 7.388E+00 4.912E-02 0.0 -0.068 0.074 0.068

25.0000 2.863E+00 3.977E-01 3.261 E+00 8.957E+00 6.139E-02 3.726E-02 -0.053 0.071 0.063

30.0000 2. 904E+00 4.899E-01 3.394E+00 1 .046E+01 7.336E-02 1 .461E-01 -0.041 0.066 0.056

35.0000 2. 935E+00 5.835E-01 3.51 9E+00 1 .191E+01 8.505E-02 2.797E-01 -0.033 0.062 0.049

40.0000 2. 960E+00 6.781E-01 3.638E+00 1 .330E+01 9.644E-02 4. 187E-01 -0.028 0.058 0.044

45.0000 2.981E+00 7.736E-01 3.754E+00 1 .466E+01 1 .075E-01 5.553E-01 -0.025 0.055 0.039

50.0000 2. 998E+00 8.698E-01 3.868E+00 1 .597E+01 1 . 183E-01 6 .865E-01 -0.023 0.052 0.036

55.0000 3.014E+00 9.667E-01 3.980E+00 1 .724E+01 1 .288E-01 8.112E-01 -0.021 0.049 0.032

60.0000 3.027E+00 1 .064E+00 4.091E+00 1 .848E+01 1 .391E-01 9.293E-01 -0.019 0.047 0.030

70.0000 3.051E+00 1 .260E+00 4.31 lE+00 2.086E+01 1 .587E-01 1 . 146E+00 -0.017 0.043 0.026

80.0000 3.070E+00 1 .458E+00 4.528E+00 2.312E+01 1 .773E-01 1 .341E+00 -0.016 0.040 0.023

90.0000 3.087E+00 1 .657E+00 4.744E+00 2.528E+01 1 .949E-01 1 .517E+00 -0.015 0.037 0.020

100.0000 3. 102E+00 1 .857E+00 4.959E+00 2.734E+01 2.116E-01 1 .677E+00 -0.014 0.035 0.018

125.0000 3.1 33E+00 2.361E+00 5.494E+00 3.21 3E+01 2.499E-01 2.023E+00 -0.013 0.031 0.015

150.0000 3.158E+00 2.869E+00 6.027E+00 3.647E+01 2.838E-01 2.312E+00 -0.012 0.028 0.013

175.0000 3.178E+00 3.380E+00 6.558E+00 4.045E+01 3. 142E-01 2.560E+00 -0.011 0.026 0.011 200.0000 3.1 96E+00 3.893E+00 7 .089E+00 4.41 1 E+01 3.415E-01 2.778E+00 -0.011 0.024 0.010

250.0000 3.224E+00 4. 926E+00 8 . 1 50E+00 5.069E+01 3.888E-01 3. 148E+00 -0.010 0.022 0.008

300.0000 3.247E+00 5. 964E+00 9.21 lE+00 5.645E+01 4.284E-01 3.457E+00 -0.008 0.020 0.007

350.0000 3.266E+00 7.005E+00 1 .027E+01 6. 159E+01 4.623E-01 3.724E+00 -0.008 0.019 0.006

400.0000 3.282E+00 8.051E+00 1 . 133E+01 6.622E+01 4.916E-01 3. 959E+00 -0.007 0.017 0.006

450.0000 3.295E+00 9.099E+00 1 .239E+01 7.044E+01 5. 173E-01 4. 169E+00 -0.006 0.016 0.005

500 .0000 3.307E+00 1 .015E+01 1 . 346E+01 7.431E+01 5.400E-01 4 . 360E+00 -0.005 0.016 0.005

550.0000 3.318E+00 1 . 120E+01 1 .452E+01 7.789E+01 5.603E-01 4.535E+00 -0.005 0.015 0.004

600 .0000 3 . 328E+00 1 .225E+01 1 .558E+01 8. 121E+01 5.785E-01 4.696E+00 -0.004 0.014 0.004

700 .0000 3.344E+00 1 .436E + 01 1 .771 E+01 8.723E+01 6.100E-01 4. 985E+00 -0.003 0.014 0.003

800.0000 3.358E+00 1 . 648E+01 1 .983E+01 9.256E+01 6.364E-01 5.238E+00 -0.003 0.013 0.003

900.0000 3. 370E+00 1 .859E+01 2.1 96E+01 9.735E+01 6.589E-01 5.464E+00 -0.002 0.012 0.002

1000.0000 3.381E+00 2.071E+01 2.409E+01 1 .017E+02 6.784E-01 5.668E+00 -0.002 0.012 0.002

127
ELECTRONS IN MUSCLE, SKELETAL (ICRP)

I = 75.3 eV DENSITY = 1 .090E+00i g/cm

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d ( loc[ )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm7/g MeV cm7/g MeV cm^/g g/cm ^ 0.0100 2.231 E+01 3.835E-03 2.231E+01 2 . 593E-09 9.366E-05 0 .

-0.199 0.228 0.226

0.0125 1 .876E+01 3.863E-03 1 .877E+01 3.771E-09 1 . 1 27E-09 0 .

-0.191 0.217 0.215

0.0150 1 .628E+01 3.880E-03 1 .629E+01 5.205E-09 1 . 31 OE-09 0.0 -0.189 0.209 0.207

0.0175 1 .995E+01 3.892E-03 1 .995E+01 6 .838E-09 1 .985E-09 0.0 -0.179 0 . 202 0.201

0 .0200 1 . 303E+01 3.901E-03 1 .303E+01 8.662E-09 1 .655E-09 0.0 -0.175 0.197 0.196

0.0250 1 .097E+01 3. 91 3E-03 1 .098E+01 1 .286E-03 1 . 980E-09 0.0 -0.169 0.189 0.188

0.0300 9.597E+00 3 . 929E-03 9.551E+00 1 .776E-03 2. 290E-09 0.0 -0.169 0.183 0.182

0.0350 8.998E+00 3.939E-03 8.502E+00 2.332E-03 2.587E-09 0.0 -0.160 0.178 0.177

0 . OAOO 7 . 692E+00 3. 996E-03 7.696E+00 2.951E-03 2.879E-09 0.0 -0.157 0.179 0.173

0 . 0<*50 7 . 052E+00 3. 959E-03 7.056E+00 3.631E-03 3. 151E-09 0.0 -0.159 0.170 0.170

0.0500 6.531E+00 3 . 973E-03 6.535E+00 9.368E-03 3.921E-09 0.0 -0.152 0.167 0.167

0 .0550 6.099E+00 3.988E-03 6 . 102E+00 5. 160E-03 3.683E-09 0.0 -0.150 0.165 0.169

0.0600 5.733E+00 9 . 009E-03 5.737E+00 6 .006E-03 3.939E-09 0.0 -0.198 0.162 0.162

0.0700 5. 151E + 00 9.090E-03 5. 155E+00 7.898E-03 9.935E-09 0.0 -0.195 0.159 0.158

0 .0800 9 .706E+00 9.079E-03 9.710E+00 9.881E-03 9.912E-09 0.0 -0.192 0.155 0.155

0.0900 9. 355E+00 9. 122E-03 9.359E+00 1 .209E-02 5.373E-09 0.0 -0.190 0.153 0.152

0.1000 9.071E+00 9. 168E-03 9.075E+00 1 .997E-02 5.821E-09 0.0 -0.138 0.150 0.150

0 . 1250 3.552E+00 9 .299E-03 3.557E+00 2.106E-02 6 .889E-09 0.0 -0.139 0.196 0.195

0.1500 3.203E+00 9.931E-03 3.207E+00 2.898E-02 7.899E-09 0.0 -0.131 0.192 0.192

0.1750 2. 951E+00 9.579E-03 2.956E+00 3.662E-02 8.865E-09 0.0 -0.129 0.139 0.139

0 .2000 2.763E+00 9.739E-03 2.768E+00 9.537E-02 9.795E-09 0.0 -0.126 0.137 0.137

0 .2500 2.501E+00 5.070E-03 2.506E+00 6 .992E-02 1 . 157E-03 0.0 -0.123 0.133 0.133

0 . 3000 2 . 329E+00 5.938E-03 2.335E+00 8.513E-02 1 . 327E-03 0.0 -0.120 0.130 0.129

0 . 3500 2.21 1E+00 5.832E-03 2.216E+00 1 .071E-01 1 .992E-03 0.0 -0.118 0.128 0.127

0 .9000 2. 125E+00 6.252E-03 2.131E+00 1 .302E-01 1 .653E-03 0.0 -0.116 0.126 0.125

0.9500 2.061 E+00 6.699E-03 2.068E+00 1 .590E-01 1 .812E-03 0.0 -0.119 0.129 0.123

0.5000 2.012E+00 7 . 1 58E-03 2.01 9E+00 1 .785E-01 1 . 970E-03 2. 181E-03 -0.102 0.122 0.121 0.5500 1 . 972E+00 7 .692E-03 1 . 980E+00 2.035E-01 2. 128E-03 2.071E-02 -0.091 0.119 0.117

0.6000 1 .991E + 00 8.191E-03 1 . 999E+00 2.290E-01 2.285E-03 9.291E-02 -0.085 0.115 0.112

0.7000 1 .895E+00 9.186E-03 1 .909E+00 2.809E-01 2.602E-03 9.262E-02 -0.076 0.109 0.109

0.8000 1 .863E+00 1 .028E-02 1 .879E+00 3.339E-01 2.921E-03 1 .988E-01 -0.068 0.103 0.097

0 . 9000 1 .892E+00 1 . 193E-02 1 .853E+00 3.876E-01 3.299E-03 2.089E-01 -0.062 0.098 0.091

1 .0000 1 .827E+00 1 .262E-02 1 .839E+00 9.918E-01 3.571E-03 2.697E-01 -0.057 0.093 0.085

1 .2500 1 .806E+00 1 .578E-02 1 .822E+00 5.789E-01 9.908E-03 9.295E-01 -0.098 0.083 0.073

1 .5000 1 .799E+00 1 . 916E-02 1 .818E+00 7. 158E-01 5.272E-03 5.750E-01 -0.092 0.076 0.065

1 .7500 1 .799E+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 .801E+00 2.692E-02 1 .828E+00 9.903E-01 7.079E-03 8.529E-01 -0.035 0.065 0.053

2.5000 1 .81 2E+00 3.921 E-02 1 .896E+00 1 .263E+00 8.956E-03 1 .098E+00 -0.031 0.058 0.095

3.0000 1 .829E+00 9.291E-02 1 .866E+00 1 .532E+00 1 .090E-02 1 .316E+00 -0.028 0.053 0.090

3.5000 1 .836E + 00 5.095E-02 1 .887E+00 1 .798E+00 1 .289E-02 1 .509E+00 -0.026 0.099 0.036

9 .0000 1 .898E+00 5.977E-02 1 .908E+00 2.062E+00 1 .993E-02 1 .683E+00 -0.025 0.096 0.033

9.5000 1 .860E+00 6 .883E-02 1 . 928E+00 2.323E+00 1 .699E-02 1 .892E+00 -0.023 0.093 0.031 5.0000 1 .870E+00 7.81 IE-02 1 .998E+00 2.580E+00 1 .908E-02 1 .986E+00 -0.023 0.091 0.029

5.5000 1 .880E+00 8.758E-02 1 . 968E+00 2.836E+00 2.11 9E-02 2.120E+00 -0.022 0.039 0.028

6 .0000 1 .889E+00 9.722E-02 1 .987E+00 3.089E+00 2.332E-02 2.293E+00 -0.021 0.038 0.027

7.0000 1 . 906E + 00 1 . 1 70E-01 2.023E+00 3.587E+00 2.761E-02 2.966E+00 -0.020 0.035 0.025

8 .0000 1 .921E + 00 1 . 372E-01 2.058E+00 9.077E+00 3.1 99E-02 2.669E+00 -0.019 0.033 0.023

9.0000 1 . 939E+00 1 .579E-01 2.092E+00 9.559E+00 3.629E-02 2.890E+00 -0.019 0.032 0.022

10.0000 1 .996E+00 1 .790E-01 2.125E+00 5.033E+00 9.065E-02 3.001E+00 -0.018 0.030 0.021 12.5000 1 .971E+00 2.331E-01 2.205E+00 6. 188E+00 5.152E-02 3.398E+00 -0.016 0.027 0.019

15.0000 1 . 992E+00 2.887E-01 2.281E+00 7.303E+00 6.231E-02 3.690E+00 -0.015 0.025 0.017

17.5000 2.009E+00 3.955E-01 2.359E+00 8.382E+00 7.299E-02 3.892E+00 -0.013 0.029 0.016

20.0000 2.023E+00 9.032E-01 2.927E+00 9.928E+00 8.339E-02 9.115E+00 -0.012 0.022 0.015

25.0000 2.097E+00 5.208E-01 2.568E+00 1 . 193E+01 1 .037E-01 9.997E+00 -0.010 0.020 0.013

30.0000 2.066E+00 6.903E-01 2.706E+00 1 .333E+01 1 .230E-01 9.818E+00 -0.008 0.018 0.011 35.0000 2.081E+00 7.615E-01 2.892E+00 1 .513E+01 1 .915E-01 5.096E+00 -0.007 0.017 0.010

90.0000 2.099E+00 8.838E-01 2.978E+00 1 .685E+01 1 .592E-01 5.391E+00 -0.006 0.015 0.008

95.0000 2. 1 05E+00 1 .007E+00 3.112E+00 1 .899E+01 1 .760E-01 5.560E+00 -0.005 0.019 0.007

50.0000 2.1 15E+00 1 . 1 31 E+00 3.297E+00 2.006E+01 1 . 920E-01 5.758E+00 -0.009 0.013 0.007

55.0000 2.1 29E+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 3.519E+00 2.302E+01 2.21 9E-01 6 . 1 05E+00 -0.003 0.012 0.005

70.0000 2.196E+00 1 .635E+00 3.780E+00 2.577E+01 2.992E-01 6.901E+00 -0.002 0.011 0.009

80.0000 2 . 1 58E+00 1 .889E+00 9.097E+00 2.832E+01 2.793E-01 6 .660E+00 -0.002 0.010 0.009

90.0000 2. 168E+00 2. 195E+00 9.313E+00 3.071E+01 2.979E-01 6.890E+00 -0.001 0.009 0.003

100.0000 2. 177E+00 2.902E+00 9.580E+00 3.296E+01 3. 188E-01 7.096E+00 -0.001 0.009 0.003

125.0000 2. 1 97E+00 3.099E+00 5.296E+00 3.806E+01 3.659E-01 7.536E+00 -0.001 0.008 0.002

150.0000 2.212E+00 3.701E+00 5.91 3E+00 9.255E+01 9.056E-01 7 .896E+00 -0.001 0.007 0.002

175.0000 2.226E+00 9 . 356E+00 6.581E+00 9.655E+01 9 . 398E-01 8.202E+00 -0.000 0.006 0.001 200.0000 2.237E+00 5.01 3E+00 7.250E+00 5.017E+01 9.699E-01 8.967E+00 -0.000 0.006 0.001

250 .0000 2.256E+00 6 . 339E+00 8.590E+00 5.650E+01 5. 187E-01 8.911 E+00 -0.000 0.005 0.001

300 .0000 2.271E+00 7.661E+00 9. 932E+00 6 . 1 91 E+01 5.581E-01 9.279E+00 -0.000 0.005 0.001

350 .0000 2.289E+00 8. 992E+00 1 . 128E+01 6.663E+01 5.905E-01 9.581E+00 -0.000 0.009 0.001 900.0000 2.296E+00 1 .033E+01 1 . 262E+01 7.082E+01 6 . 1 77E-01 9.898E+00 -0.000 0.009 0.001 950.0000 2.306E+00 1 . 1 66E+01 1 .397E + 01 7 .958E + 01 6 .909E-01 1 .008E + 01 -0.000 0.009 0.000

500 .0000 2.315E+00 1 . 300E+01 1 .532E+01 7 .800E+01 6.610E-01 1 .029E+01 -0.000 0 .009 0.000

550.0000 2. 323E+00 1 .939E+01 1 .667E+01 8.11 3E+01 6 .787E-01 1 .098E+01 -0.000 0.009 0.000

600.0000 2. 330E+00 1 .568E+01 1 .801 E+01 8.901 E+01 6 . 993E-01 1 .066E+01 -0.000 0.009 0.000

700 .0000 2 . 393E+00 1 .837E+01 2.072E+01 8.918E+01 7.207E-01 1 .097E + 01 -0.000 0.003 0.000

800.0000 2.359E+00 2. 106E+01 2.392E+01 9.372E+01 7.923E-01 1 . 123E+01 -0 .000 0.003 0.000 900.0000 2.369E+00 2.376E+01 2.612E+01 9.776E+01 7.603E-01 1 . 1 97E+01 -0.000 0.003 0.000 1000.0000 2.373E+00 2.695E+01 2.883E+01 1 .019E+02 7.756E-01 1 .168E+01 -0.000 0.003 0.000

128
ELECTRONS IN MUSCLE, STRIATED (ICRU)

I = 79.7 eV DENSITY = 1 . 090E+001 g/cm

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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.237E+01 3.816E-03 2.238E+01 2.536E-09 9.293E-05 0.0 -0.199 0.227 0.225

0.0125 1 .881E + 01 3.899E-03 1 .882E+01 3.759E-09 1.11 9E-09 0.0 -0.190 0.216 0.215

0.0150 1 .633E+01 3.862E-03 1 .633E+01 5.1 90E-09 1 .300E-09 0.0 -0.189 0.208 0.207

0.0175 1 .999E+01 3.873E-03 1 .999E+01 6.818E-09 1 .979E-09 0.0 -0.179 0.202 0.201 0.0200 1 . 306E+01 3.882E-03 1 .307E+01 8.638E-09 1 .692E-09 0.0 -0.175 0.197 0.196

0.0250 1 . 100E+01 3.899E-03 1 . 100E+01 1 .283E-03 1 . 965E-09 0.0 -0.169 0.188 0.188

0.0300 9.571E+00 3.905E-03 9.575E+00 1 .771E-03 2.273E-09 0.0 -0.169 0.182 0.182

0 .0350 8.51 9E+00 3.916E-03 8.523E+00 2.326E-03 2.568E-09 0.0 -0.160 0.177 0.177

0 .OAOO 7.71 1E+00 3.928E-03 7.715E+00 2. 999E-03 2.853E-09 0.0 -0.157 0.173 0.173

0 .OA50 7.069E+00 3 . 991 E-03 7 .073E + 00 3.621E-03 3.128E-09 0.0 -0.159 0.170 0.169

0 .0500 6 .597E+00 3.955E-03 6 .551 E+00 9.356E-03 3.396E-09 0.0 -0.152 0.167 0.167

0.0550 6.11 3E+00 3. 970E-03 6.117E+00 5. 197E-03 3.657E-09 0.0 -0.150 0.169 0.169

0.0600 5.797E+00 3. 986E-03 5.751E+00 5.991E-03 3.911E-09 0.0 -0.198 0.162 0.162

0.0700 5. 163E+00 9.022E-03 5.167E+00 7.829E-03 9.909E-09 0.0 -0.195 0.158 0.158

0.0800 9.717E+00 9.061E-03 9.721E+00 9.857E-03 9.878E-09 0.0 -0.192 0.155 0.155

0.0900 9.365E+00 9.109E-03 9.369E+00 1 .206E-02 5.336E-09 0.0 -0.190 0.153 0.152

0.1000 9.080E+00 9.1 50E-03 9.089E+00 1 .993E-02 5.780E-09 0.0 -0.138 0.150 0.150

0.1250 3.561E+00 9.275E-03 3.565E+00 2.101E-02 6 .891E-09 0.0 -0.139 0.196 0.195

0 . 1 500 3 . 21 OE+00 9.912E-03 3.219E+00 2.891E-02 7.895E-09 0.0 -0.131 0.192 0.192

0 . 1 750 2. 95SE+00 9.558E-03 2. 962E+00 3.653E-02 8.805E-09 0.0 -0.128 0.139 0.139

0.2000 2 . 769E+00 9.719E-03 2.779E+00 9.526E-02 9.728E-09 0.0 -0.126 0.137 0.136

0 . 2500 2.506E+00 5.098E-03 2.511 E+00 6.927E-02 1 . 199E-03 0.0 -0.123 0.133 0.132

0 . 3000 2.335E+00 5.91 5E-03 2.390E+00 8.999E-02 1 .318E-03 0.0 -0.120 0.130 0.129

0.3500 2.215E+00 5 .808E-03 2.221E+00 1 .069E-01 1 .982E-03 0.0 -0.118 0.128 0.127

0 .9000 2 . 1 29E+00 6 .226E-03 2.1 36E+00 1 .299E-01 1 .692E-03 0.0 -0.116 0.126 0.125

0.9500 2.065E+00 6 .666E-03 2.072E+00 1 .537E-01 1 .801E-03 0.0 -0.119 0.129 0.123

0.5000 2.01 6E+00 7. 129E-03 2.023E+00 1 .781E-01 1 .957E-03 9.290E-03 -0.098 0.122 0.120

0.5500 1 . 976E+00 7.610E-03 1 .989E+00 2.031E-01 2.119E-03 2.378E-02 -0.090 0.118 0.116

0.6000 1 . 995E+00 8. 108E-03 1 .953E+00 2.285E-01 2.271E-03 9.639E-02 -0.089 0.115 0.112

0.7000 1 .898E+00 9. 198E-03 1 . 907E+00 2.803E-01 2.585E-03 9.798E-02 -0.075 0.108 0.109

0.8000 1 .866E+00 1 .029E-02 1 .877E+00 3.332E-01 2.903E-03 1 .553E-01 -0.068 0.102 0.096

0 . 9000 1 .895E+00 1 . 1 39E-02 1 .856E+00 3.868E-01 3.229E-03 2. 158E-01 -0.062 0.097 0.090

1 .0000 1 .830E+00 1 .257E-02 1 .892E+00 9.909E-01 3.550E-03 2.778E-01 -0.057 0.092 0.089

1 .2500 1 .809E+00 1 .572E-02 1 .825E+00 5.779E-01 9.382E-03 9.339E-01 -0.098 0.083 0.073

1 .5000 1 .802E+00 1 .908E-02 1 .821E+00 7. 196E-01 5.292E-03 5.852E-01 -0.092 0.075 0.069

1 .7500 1 .801E+00 2.263E-02 1 .829E+00 8.518E-01 6.127E-03 7.289E-01 -0.038 0.070 0.057

2.0000 1 .809E+00 2.632E-02 1 .830E+00 9.886E-01 7.035E-03 8.691E-01 -0.035 0.065 0.052

2.5000 1 .819E+00 3.908E-02 1 .898E+00 1 .261E+00 8.907E-03 1 . 1 lOE+00 -0.031 0.058 0.095

3.0000 1 .826E+00 9.225E-02 1 .869E+00 1 .530E+00 1 .089E-02 1 .327E+00 -0.028 0.053 0.090

3.5000 1 .839E+00 5.076E-02 1 .890E+00 1 .796E+00 1 .283E-02 1 .521E+00 -0.026 0.099 0.036

9.0000 1 .851E+00 5. 959E-02 1 .910E+00 2.059E+00 1 .985E-02 1 .695E+00 -0.029 0.096 0.033

9.5000 1 .862E+00 6.857E-02 1 .931E+00 2.31 9E+00 1 .690E-02 1 .853E+00 -0.023 0.093 0.031

5 .0000 1 .873E+00 7.782E-02 1 .951E+00 2.577E+00 1 .898E-02 1 .998E+00 -0.023 0.091 0.029

5.5000 1 .883E+00 8.725E-02 1 .970E+00 2.832E+00 2.108E-02 2.131E+00 -0.022 0.039 0.028

6.0000 1 .892E+00 9.686E-02 1 .989E+00 3.089E+00 2.320E-02 2.255E+00 -0.021 0.038 0.027

7.0000 1 . 909E+00 1 . 165E-01 2.026E+00 3.583E+00 2.797E-02 2.978E+00 -0.020 0.035 0.025

8.0000 1 . 929E+00 1 .367E-01 2.061E+00 9.072E+00 3. 178E-02 2.675E+00 -0.019 0.033 0.023

9.0000 1 .937E+00 1 .579E-01 2.099E+00 9.553E+00 3.61 IE-02 2.852E+00 -0.018 0.032 0.022

10.0000 1 . 999E+00 1 .789E-01 2.127E+00 5.027E+00 9.095E-02 3.013E+00 -0.018 0.030 0.021 12.5000 1 .979E+00 2.323E-01 2.206E+00 6.181E+00 5. 128E-02 3.361E+00 -0.016 0.027 0.019

15.0000 1 . 995E+00 2.877E-01 2.282E+00 7.295E+00 6.202E-02 3.652E+00 -0.015 0.025 0.017

17.5000 2.012E+00 3.993E-01 2.356E+00 8.373E+00 7.261E-02 3. 905E+00 -0.013 0.029 0.016

20.0000 2.026E+00 9.018E-01 2.928E+00 9.918E+00 8.302E-02 9.128E+00 -0.012 0.022 0.015

25.0000 2.050E+00 5. 189E-01 2.569E+00 1 . 192E+01 1 .032E-01 9.51 lE+00 -0.010 0.020 0.012

30.0000 2.068E+00 6.381E-01 2.706E+00 1 .332E+01 1 .225E-01 9.833E+00 -0.008 0.018 0.011 35.0000 2.089E+00 7 .588E-01 2.892E+00 1 .512E+01 1 .910E-01 5.111E+00 -0.007 0.016 0.009

90.0000 2.097E+00 8.807E-01 2.977E+00 1 .689E+01 1 .585E-01 5.356E+00 -0.005 0.015 0.008

95.0000 2. 108E+00 1 .009E+00 3.111 E+00 1 .898E+01 1 .753E-01 5.576E+00 -0.005 0.019 0.007

50.0000 2.1 18E+00 1 . 127E+00 3.295E+00 2.005E+01 1 . 91 3E-01 5.779E+00 -0.009 0.013 0.007

55.0000 2. 126E+00 1 .252E+00 3.378E+00 2. 156E+01 2.065E-01 5. 955E+00 -0.003 0.013 0.006

60.0000 2.139E+00 1 . 377E+00 3.512E+00 2.301E+01 2.211E-01 6.121E+00 -0.003 0.012 0.005

70.0000 2. 198E+00 1 .629E+00 3.777E+00 2.576E+01 2.989E-01 6 .918E+00 -0.002 0.011 0.009

80.0000 2. 160E+00 1 .883E+00 9.093E+00 2.832E+01 2.735E-01 6 .677E+00 -0.002 0.010 0.009

90.0000 2. 171E+00 2. 1 38E+00 9.308E+00 3.071E+01 2. 965E-01 6.907E+00 -0.001 0.009 0.003

100.0000 2. 180E+00 2 . 399E+00 9.579E+00 3.297E+01 3. 179E-01 7.113E+00 -0.001 0.009 0.003

125.0000 2. 1 99E+00 3.039E+00 5.238E+00 3.807E+01 3.699E-01 7.553E+00 -0.001 0.008 0.002

150.0000 2. 21 5E+00 3.688E+00 5. 903E+00 9.256E+01 9.096E-01 7.91 3E+00 -0.001 0.007 0.002

175.0000 2 . 228E+00 9.391E+00 6.569E+00 9.658E+01 9.388E-01 8.21 9E+00 -0.000 0.006 0.001 200.0000 2.290E+00 9. 996E+00 7.236E+00 5.020E+01 9.689E-01 8.9S9E+00 -0.000 0.006 0.001 250.0000 2.259E+00 6 . 31 3E+00 8.571E+00 5.659E+01 5. 177E-01 8. 928E+00 -0.000 0.005 0.001 300.0000 2.279E+00 7 .635E+00 9.909E+00 6.1 96E+01 5.571E-01 9.291E+00 -0.000 0.005 0.001 350.0000 2.287E+00 8 . 962E+00 1 .125E+01 6.670E+01 5.895E-01 9.598E+00 -0.000 0.009 0.001 900.0000 2.299E+00 1 . 029E+01 1 .259E+01 7.089E+01 6 . 1 68E-01 9.865E+00 -0.000 0.009 0.001 950.0000 2. 309E+00 1 . 162E+01 1 .393E+01 7.967E+01 6 .900E-01 1 .OlOE+01 -0 .000 0.009 0.000

500.0000 2.317E+00 1 .296E+01 1 .528E+01 7 .809E+01 6.602E-01 1 .031E+01 -0 .000 0.009 0.000

550.0000 2. 325E+00 1 .930E+01 1 .662E+01 8.123E+01 6 .778E-01 1 .050E+01 -0.000 0.009 0.000

600.0000 2. 333E+00 1 . 563E+01 1 .797E+01 8.912E+01 6 . 935E-01 1 .067E+01 -0.000 0.003 0.000

700.0000 2.396E+00 1 .831 E+01 2.066E+01 8.931E+01 7.199E-01 1 .098E+01 -0.000 0.003 0.000

800.0000 2.357E+00 2.099E+01 2.335E+01 9.386E+01 7.916E-01 1 . 125E+01 -0.000 0.003 0.000

900.0000 2.367E+00 2. 368E+01 2.605E+01 9.791 E+01 7.596E-01 1 . 198E+01 -0.000 0.003 0.000

1000.0000 2. 376E+00 2.637E+01 2.879E+01 1 .016E+02 7 .750E-01 1 .170E+01 -0.000 0.003 0.000

129
ELECTRONS IN MUSCLE-EQUIVALENT LIQUID. WITH SUCROSE

I = 7A.3 eV DENSITY = 1 . 1 10E+0C1 g/cm^

ENERGY STOPPING POWER CSDA RADIATION DENS. EPF. dClog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.233E+01 3.7A9E-03 2.233E+01 2.5A1E-0A 9.16AE-05 0.0 -0.198 0.227 0.225

0.0125 1 .877E + 01 3.77AE-03 1 .878E+01 3.767E-0A 1 . 1 02E-0A 0.0 -0.190 0.216 0.215

0.0150 1 .629E+01 3.789E-03 1 .630E+01 5.201 E-OA 1 .280E-0A 0.0 -0 . 18A 0.208 0.207

0.0175 1 . AA5E+01 3.799E-03 1 . AA6E+01 6.833E-0A 1 . A51 E-OA 0.0 -0.179 0 . 202 0.201 0.0200 1 . 303E+01 3.807E-03 1 .30AE+01 8.657E-0A 1 .617E-0A 0.0 -0.175 0.196 0.195

0.0250 1 .098E+01 3.818E-03 1 .098E+01 1 .285E-03 1 . 93AE-0A 0.0 -0.168 0.188 0.187

0.0300 9.5A9E+00 3.827E-03 9.553E+00 1 .775E-03 2.235E-0A 0.0 -0.16A 0.182 0.181

0 .0350 8. A99E+00 3.837E-03 8.503E+00 2.331E-03 2.525E-0A 0.0 -0.160 0.177 0.177

0 . OAOO 7 . 693E+00 3.8A8E-03 7.696E+00 2. 950E-03 2.80AE-0A 0.0 -0.157 0.173 0.173

0 . 0A50 7 .052E+00 3.861E-03 7.056E+00 3.630E-03 3.07AE-0A 0.0 -0 . 1 5A 0.170 0.169

0.0500 6 .531E+00 3.87AE-03 6 . 535E+00 A. 367E-03 3.337E-0A 0.0 -0.151 0.167 0.166

0 . 0550 6 . 099E+00 3.889E-03 6. 102E+00 5. 159E-03 3.593E-0A 0.0 -0. 1A9 0. 16A 0.16A

0 .0600 5.733E+00 3 . 905E-03 5.737E+00 6.005E-03 3.8A3E-0A 0.0 -0 . 1 A8 0.162 0.162

0 .0700 5. 150E+00 3.9A0E-03 5. 15AE+00 7.8A7E-03 A.326E-0A 0.0 -0 . 1 AA 0.158 0.158

0 . 0800 A . 705E+00 3. 979E-03 A.709E+00 9.880E-03 A.792E-0A 0.0 -0 . 1 A2 0.155 0.155

0.0900 A. 35AE+00 A.021E-03 A.358E+00 1 .209E-02 5.2A1E-0A 0.0 -O.IAO 0.152 0.152

0 . 1 000 A . 070E+00 A.066E-03 A.07AE+00 1 .AA7E-02 5.678E-0A 0.0 -0.138 0.150 0.150

0.1250 3.552E+00 A . 1 90E-03 3.556E+00 2. 106E-02 6 .720E-0A 0.0 -0.1 3A 0.1A6 0.1 A5 0.1500 3.202E+00 A. 325E-03 3.206E+00 2.8A8E-02 7 .707E-0A 0.0 -0.131 0 . 1 A2 0.1 A2

0 . 1750 2. 950E+00 A.A69E-03 2.955E+00 3.662E-02 8.651E-0A 0.0 -0.128 0.139 0.139

0 . 2000 2.762E+00 A.622E-03 2.767E+00 A .538E-02 9.559E-0A 0.0 -0.126 0.137 0.136

0.2500 2.500E+00 A.951E-03 2.505E+00 6 . AAAE-02 1 . 1 30E-03 0.0 -0.123 0.133 0.132

0 . 3000 2 . 329E+00 5.31 IE-03 2.33AE+00 8.516E-02 1 .296E-03 0.0 -0.120 0.130 0.129

0.3500 2.210E+00 5.698E-03 2.215E+00 1 . 072E-01 1 . A57E-03 0.0 -0.118 0.128 0.127

0 . AOOO 2. 12AE+00 6.109E-03 2.1 30E+00 1 .302E-01 1 .615E-03 0.0 -0.116 0.126 0.125

0 . A500 2.060E+00 6.5A3E-03 2.066E+00 1 .5A1E-01 1 .771E-03 0.0 -0.113 0. 12A 0.123

0 . 5000 2.010E+00 6.997E-03 2.017E+00 1 .786E-01 1 . 925E-03 1 .51 9E-02 -0.092 0.121 0.119

0.5500 1 . 970E+00 7.A70E-03 1 . 977E+00 2.036E-01 2.080E-03 3.828E-02 -0.086 0.117 0.1 lA 0.6000 1 . 938E+00 7.960E-03 1 . 9A6E+00 2.291E-01 2.23AE-03 6.393E-02 -0.081 0.113 0.109

0 .7000 1 .891E+00 8. 983E-03 1 .900E+00 2.812E-01 2.5A5E-03 1 .207E-01 -0.072 0.106 0.101 0.8000 1 .859E+00 1 .006E-02 1 .869E+00 3. 3A3E-01 2.859E-03 1 .821E-01 -0.065 0.100 0.09A

0 . 9000 1 .837E+00 1 . 1 18E-02 1 .8A8E+00 3.881E-01 3. 176E-03 2. A60E-01 -0.060 0.095 0.087

1 .0000 1 .822E+00 1 .235E-02 1 .83AE+00 A. A2AE-01 3. A98E-03 3. 108E-01 -0.055 0.090 0.082

1 .2500 1 .801E+00 1 .5A5E-02 1 .816E+00 5.795E-01 A.321E-03 A.720E-01 -0 .0A7 0.081 0.071

1 .5000 1 .793E+00 1 .876E-02 1 .812E+00 7.17AE-01 5.171E-03 6 .269E-01 -0 .0A1 0.073 0.062

1 .7500 1 .793E+00 2.22AE-02 1 .81 5E+00 8.553E-01 6 .0A6E-03 7.730E-01 -0.037 0.068 0.056

2.0000 1 . 795E+00 2.587E-02 1 .821E+00 9. 928E-01 6 . 9AAE-03 9. lOOE-01 -0.03A 0.063 0.051

2 . 5000 1 .805E+00 3.351E-02 1 .839E+00 1 .266E+00 8.797E-03 1 .158E+00 -0.030 0.056 O.OAA

3 .0000 1 .81 7E+00 A. 1 55E-02 1 .859E+00 1 .537E+00 1 .071 E-02 1 .377E+00 -0.027 0.051 0.039

3.5000 1 .830E+00 A.992E-02 1 .880E+00 1 .80AE+00 1 .267E-02 1 .572E+00 -0.026 0.0A8 0.035

A. 0000 1 .8A2E+00 5.857E-02 1 .900E+00 2.069E+00 1 . A68E-02 1 .7A7E+00 -0.02A 0.0A5 0.033

A. 5000 1 .853E+00 6 .7A6E-02 1 . 920E+00 2.330E+00 1 .671E-02 1 . 905E+00 -0.023 0 .0A2 0.030

5.0000 1 .863E+00 7.656E-02 1 .9A0E+00 2.589E+00 1 .877E-02 2.050E+00 -0.022 0 .OAO 0.029

5.5000 1 .873E+00 8.585E-02 1 .959E+00 2.8A6E+00 2.085E-02 2. 18AE+00 -0.022 0.038 0.027

6 .0000 1 .883E+00 9.531E-02 1 . S78E+00 3. 100E+00 2.29AE-02 2. 308E+00 -0.021 0.037 0.026

7.0000 1 .899E+00 1 . 1 A7E-01 2.01 AE+00 3.601E+00 2.718E-02 2.531E+00 -0.020 0.035 0.02A

8.0000 1 . 91 AE+00 1 .3A6E-01 2.0A9E+00 A.093E+00 3. 1 AAE-02 2.729E+00 -0.019 0.033 0.023

9.0000 1 . 927E+00 1 .5A9E-01 2.082E+00 A.577E+00 3.573E-02 2.906E+00 -0.018 0.031 0.022

10.0000 1 . 939E+00 1 .756E-01 2. 1 15E+00 5.05AE+00 A.003E-02 3.067E+00 -0.018 0.030 0.021 12.5000 1 . 96AE+00 2.287E-01 2.193E+00 6.215E+00 5.076E-02 3.A16E+00 -0.016 0.027 0.019

15.0000 1 . 98AE+00 2.832E-01 2.268E+00 7.336E+00 6. lAlE-02 3.709E+00 -0.01 A 0.025 0.017

17.5000 2. 001 E+00 3.390E-01 2.3A0E+00 8.A21E+00 7.1 92E-02 3.963E+00 -0.013 0.023 0.016

20 .0000 2.016E+00 3. 957E-01 2.A1 1E+00 9.A73E+00 8.22AE-02 A. 187E+00 -0.012 0.022 O.OIA

25.0000 2.039E+00 5.11 IE-01 2.550E+00 1 .1 A9E+01 1 .023E-01 A.572E+00 -0.009 0.019 0.012

30 .0000 2.057E+00 6 .285E-01 2.686E+00 1 .3A0E+01 1 .215E-01 A.895E+00 -0.008 0.018 0.011 35.0000 2.072E+00 7.A7AE-01 2.820E+00 1 .522E+01 1 .398E-01 5. 175E+00 -0.006 0.016 0.009

AO. 0000 2.085E+00 8.676E-01 2.953E+00 1 .695E+01 1 .573E-01 5. A22E+00 -0.005 0.015 0.008

A5.0000 2.096E+00 9.887E-01 3.085E+00 1 .860E+01 1 .7A0E-01 5.6A2E+00 -0 .OOA O.OIA 0.007

50.0000 2. 106E+00 1.111 E+00 3.217E+00 2.01 9E+01 1 .899E-01 5.8A1E+00 -0 .OOA 0.013 0.006

55.0000 2.11 5E+00 1 .233E + 00 3.3A8E+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. A79E+00 2.318E+01 2.1 96E-01 6.189E+00 -0.003 0.012 0.005

70.0000 2.1 37E+00 1 .605E+00 3.7A2E+00 2.595E+01 2. A68E-01 6 . A87E+00 -0.002 0.010 O.OOA

80.0000 2. 1A8E+00 1 .855E+00 A.003E+00 2.853E+01 2.717E-01 6 .7A7E+00 -0.002 0.010 O.OOA

90.0000 2 . 1 59E+00 2. 107E+00 A.265E+00 3.095E+01 2. 9A8E-01 5.977E+00 -0.001 0.009 0.003

100.0000 2. 168E+00 2.359E+00 A.527E+00 3.323E+01 3. 161E-01 7 . 18AE + 00 -0.001 0.008 0.003

125.0000 2. 187E+00 2. 995E+00 5. 182E+00 3.839E+01 3.630E-01 7.62AE+00 -0.001 0.007 0.002

150.0000 2.203E+00 3 . 635E+00 5.837E+00 A.293E+01 A.027E-01 7 . 985E+00 -0.001 0.007 0.002

175.0000 2.216E+00 A . 278E+00 6.A9AE+00 A.699E+01 A.368E-01 8.291E+00 -0.000 0.006 0.001 200.0000 2.227E+00 A . 92AE+00 7 . 1 51 E+00 5.066E+01 A.66AE-01 8.556E+00 -0.000 0.006 0.001 250.0000 2.2A6E+00 6 .221 E+00 8. A68E+00 5.707E+01 5. 157E-01 9.000E+00 -0.000 0.005 0.001 300.0000 2.262E+00 7 . 525E+00 9.787E+00 6.256E+01 5.552E-01 9. 36AE+00 -0.000 0.005 0.001 350.0000 2.275E+00 8 .833E+00 1.11 1E+01 6.736E+01 5.877E-01 9.671E+00 -0.000 0 .OOA 0.001 AOO.OOOO 2.286E+00 1 .01 AE+01 1 .2A3E+01 7.161E+01 6.150E-01 9. 938E+00 -0.000 O.OOA 0.000

A50.0000 2.296E+00 1 . 1 A6E+01 1 .375E+01 7.5A3E+01 6 . 383E-01 1 .017E+01 -0.000 O.OOA 0.000

500.0000 2. 305E+00 1 .277E+01 1 .508E+01 7 .890E+01 6.585E-01 1 . 038E+01 -0 .000 O.OOA 0.000

550.0000 2.313E+00 1 . A09E+01 1 .6A0E+01 8.208E+01 6 .762E-01 1 .057E+01 -0.000 0.003 0.000 600.0000 2.320E+00 1 .5A1E+01 1 .773E+01 8.501E+01 6 . 91 9E-01 1 .075E+01 -0.000 0.003 0.000

700.0000 2. 333E+00 1 .805E+01 2.038E+01 9.027E+01 7 . 18AE-01 1 .106E+01 -0.000 0.003 0.000

800 .0000 2. 3AAE+00 2 . 069E+01 2.30AE+01 9. A88E+01 7.A01E-01 1 . 1 32E+01 -0.000 0.003 0.000

900.0000 2. 35AE+00 2. 33AE+01 2.570E+01 9.899E+01 7.583E-01 1 . 1 56E+01 -0.000 0.003 0.000

1000.0000 2. 363E+00 2. 599E+01 2.835E+01 1 .027E+02 7.737E-01 1 .177E+01 -0.000 0.003 0.000

130
ELECTRONS IN MUSCLE-EQUIVALENT LIQUID, WITHOUT SUCROSE

I = 74.2 eV DENSITY = 1 .070E+0C1 g/cm^

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^/g MeV cm^/g MeV cm^/g g/cm ^

0.0100 2.241E+01 3.777E-03 2.241E+01 2.531E-04 9.1 94E-05 0.0 -0.198 0.227 0.225

0.0125 1 .884E+01 3.803E-03 1 .885E+01 3.753E-04 1 .106E-04 0.0 -0.190 0.216 0.214

0.0150 1 .635E+01 3.818E-03 1 .636E+01 5.181E-04 1 .285E-04 0.0 -0.184 0.208 0.207

0.0175 1 .451 E+01 3.829E-03 1 .451E+01 6.807E-04 1 .456E-04 0.0 -0.179 0.202 0.200

0.0200 1 . 308E+01 3.836E-03 1 .309E+01 8.625E-04 1 .623E-04 0 .

-0.175 0.196 0.195

0.0250 1 . 102E+01 3.847E-03 1 . 102E+01 1 .281 E-03 1 .941E-04 0.0 -0.168 0.188 0.187

0.0300 9.584E+00 3.857E-03 9.588E+00 1 .769E-03 2.244E-04 0.0 -0.164 0.182 0.181 0.0350 8.530E+00 3.867E-03 8.534E+00 2. 323E-03 2.535E-04 0.0 -0.160 0.177 0.177

0 .OAOO 7.721E+00 3.878E-03 7.725E+00 2. 939E-03 2.81 5E-04 0.0 -0.156 0.173 0.173

O.OA50 7 . 078E+00 3.890E-03 7.082E+00 3.616E-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. 121E+00 3. 91 9E-03 6.125E+00 5. 140E-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 3.858E-04 0.0 -0.148 0.162 0.162

0.0700 5. 169E+00 3. 970E-03 5. 173E+00 7.81 9E-03 4.343E-04 0.0 -0.144 0.158 0.158

0.0800 4.722E+00 4.009E-03 4.726E+00 9.844E-03 4.81 IE-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 4.089E+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 2.098E-02 6.747E-04 0.0 -0.134 0.146 0.145

0 . 1 500 3.213E+00 4.357E-03 3.218E+00 2.838E-02 7.737E-04 0.0 -0.131 0.142 0.142

0.1750 2.961E+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 -0.120 0.130 0.129

0.3500 2.218E+00 5.739E-03 2.223E+00 1 .068E-01 1 .462E-03 0.0 -0.118 0.128 0.127

0.4000 2.131E+00 6.152E-03 2.1 38E+00 1 .297E-01 1 .621E-03 0.0 -0.116 0.126 0.124

0.4500 2.067E+00 6.589E-03 2.074E+00 1 .535E-01 1 .777E-03 0.0 -0.115 0.124 0.123

0.5000 2.018E+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-03 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-01 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+00 1 .01 3E-02 1 .877E+00 3.330E-01 2.867E-03 1 .666E-01 -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-01 3.508E-03 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 4.510E-01 -0.047 0.082 0.072

1 . 5000 1 .802E+00 1 .888E-02 1 .821E+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 7.498E-01 -0.037 0.069 0.057

2.0000 1 .804E+00 2.605E-02 1 .830E+00 9.885E-01 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 8.815E-03 1 .134E+00 -0.030 0.057 0.044

3.0000 1 .826E+00 4. 183E-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+00 -0.024 0.045 0.033

4.5000 1 .861E+00 6 .790E-02 1 .929E+00 2.320E+00 1 .674E-02 1 .882E+00 -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+00 -0.022 0.040 0.029

5.5000 1 .882E+00 8.641E-02 1 .968E+00 2.833E+00 2.089E-02 2. 162E+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 2.286E+00 -0.021 0.037 0.026

7.0000 1 . 908E+00 1 .154E-01 2.023E+00 3.584E+00 2.723E-02 2.510E+00 -0.020 0.035 0.024

8.0000 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 2.092E+00 4.556E+00 3.580E-02 2.885E+00 -0.018 0.031 0.022

1 0.0000 1 . 948E+00 1 .767E-01 2.124E+00 5.031E+00 4.010E-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 2.010E+00 3.41 IE-01 2.351E+00 8.382E+00 7.204E-02 3.940E+00 -0.013 0.023 0.016

20.0000 2.025E+00 3.982E-01 2.423E+00 9.429E+00 8.238E-02 4.164E+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+01 1 .217E-01 4.871E+00 -0.008 0.018 0.011

35 .0000 2.082E+00 7 . 520E-01 2.834E+00 1 .514E+01 1 .400E-01 5.149E+00 -0.006 0.016 0.009

40.0000 2 . 095E+00 8.729E-01 2.968E+00 1 .687E+01 1 .575E-01 5.395E+00 -0.005 0.015 0.008

45.0000 2.106E+00 9.949E-01 3.101E+00 1 .852E+01 1 .742E-01 5.615E+00 -0.004 0.014 0.007

50.0000 2.1 16E+00 1 . 1 18E+00 3.233E+00 2.010E+01 1 .901E-01 5.814E+00 -0.004 0.013 0.006

55.0000 2. 125E+00 1 .241E+00 3.366E+00 2.161E+01 2.053E-01 5.995E+00 -0.003 0.012 0.006

60.0000 2. 133E+00 1 .365E+00 3.498E+00 2.307E+01 2.1 98E-01 6.161E+00 -0.003 0.012 0.005

70.0000 2.146E+00 1 .615E+00 3.761 E+00 2.582E+01 2.470E-01 6 .459E+00 -0.002 0.011 0.004

80.0000 2. 158E+00 1 .866E+00 4.025E+00 2.839E+01 2.720E-01 6.718E+00 -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 4.551E+00 3.306E+01 3.164E-01 7.155E+00 -0.001 0.008 0.003

125.0000 2.1 97E+00 3.01 3E+00 5.210E+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 .870E+00 4.271E+01 4.030E-01 7.955E+00 -0.001 0.007 0.002

175.0000 2.226E+00 4 . 304E+00 6.530E+00 4.675E+01 4.371E-01 8.261E+00 -0.000 0.006 0.001 200.0000 2.238E+00 4.954E+00 7.191E+00 5.040E+01 4.668E-01 8.526E+00 -0.000 0.006 0.001 250.0000 2.257E+00 6.259E+00 8.515E+00 5.678E+01 5. 160E-01 8. 971E+00 -0.000 0.005 0.001 300.0000 2.272E+00 7.570E+00 9.842E+00 6.223E+01 5.555E-01 9.334E+00 -0.000 0 .005 0.001 350.0000 2.285E+00 8.886E+00 1 . 1 17E+01 6.700E+01 5.880E-01 9.641E+00 -0.000 0.004 0.001 400.0000 2.296E+00 1 .020E+01 1 .250E+01 7. 123E+01 6. 153E-01 9. 908E+00 -0.000 0.004 0.001 450.0000 2.306E+00 1 . 153E+01 1 .383E+01 7.503E+01 6.386E-01 1 .014E+01 -0.000 0.004 0.000

500.0000 2.315E+00 1 .285E+01 1 .516E+01 7.848E+01 6 .588E-01 1 .035E+01 -0 .000 0.004 0.000

550.0000 2. 323E+00 1 .417E+01 1 .650E+01 8. 164E+01 6 .765E-01 1 .054E+01 -0.000 0.004 0.000

600.0000 2.331E+00 1 .550E+01 1 .783E+01 8.455E+01 6.921E-01 1 .072E+01 -0.000 0.003 0.000

700.0000 2.344E+00 1 .81 6E+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+01 2.317E+01 9.437E+01 7.404E-01 1 .129E+01 -0.000 0.003 0.000

900.0000 2.365E+00 2.348E+01 2.585E+01 9.845E+01 7.585E-01 1 .153E+01 -0.000 0.003 0.000

1000.0000 2.374E+00 2.615E+01 2.852E+01 1 .021E+02 7.739E-01 1 .174E+01 -0.000 0.003 0.000

131
ELECTRONS IN NYLON, TYPE 6 AND TYPE 6/6

I = 63.9 eV

ENERGY STOPPING POWER

COLLISION RADIATIVE TOTAL

MeV MeV cm^/g MeV cm^/g MeV cm^/g

0.0100 2.298E+01 3.16AE-03 2.298E+01 2 0.0125 1 . 930E+01 3 . 1 78E-03 1 . 930E+01 3 0.0150 1 .673E+01 3 . 1 87E-03 1 .67AE+01 5 0.0175 1 . A83E+01 3.1 9AE-03 1 . A8AE+01 6 0.0200 1 .337E+01 3. 1 99E-03 1 .337E+01 8

0 .0250 1 .125E+01 3.208E-03 1 .125E+01 1 0.0300 9.778E+00 3.218E-03 9.781 E+00 1 0.0350 8.698E+00 3.228E-03 8.701 E+00 2

0 . OAOO 7 .869E+00 3 . 239E-03 7.872E+00 2

0 . 0A50 7.211 E+00 3.252E-03 7.21AE+00 3 0.0500 6 .676E+00 3.265E-03 6 .679E+00 A

0 .0550 6 . 232E+00 3.279E-03 6 .235E+00 5 0.0600 5.857E+00 3.295E-03 5.860E+00 5 0.0700 5.259E+00 3. 327E-03 5.262E+00 7

0 . 0800 A .803E+00 3.363E-03 A.806E+00 9

0 .0900 A.AA3E+00 3.A01E-03 A.AA6E+00 1

0 . 1000 A.152E+00 3.AA1E-03 A.155E+00 1 0.1250 3.621E+00 3.551E-03 3.625E+00 2 0.1500 3.263E+00 3 . 669E-03 3.266E+00 2 0.1750 3.006E+00 3.796E-03 3.009E+00 3

0 . 2000 2.81 3E+00 3.930E-03 2.817E+00 A 0.2500 2.5AAE+00 A.218E-03 2.5A9E+00 6

0 . 3000 2.369E+00 A.532E-03 2 . 37AE+00 8

0 . 3500 2.2A7E+00 A.868E-03 2.252E+00 1

0 . AOOO 2. 156E+00 5.226E-03 2.161E+00 1 0 . A500 2.086E+00 5 . 60AE-03 2.092E+00 1 0.5000 2 . 032E+00 5. 999E-03 2.038E+00 1 0.5500 1 .990E+00 6.A10E-03 1 . 996E+00 2 0.6000 1 . 956E+00 6 .836E-03 1 .963E+00 2 0.7000 1 . 906E+00 7.726E-03 1 .91AE+00 2 0.8000 1 .872E+00 8.661E-03 1 .881 E+00 3

0 . 9000 1 .8A9E+00 9.639E-03 1 .859E+00 3

1 .0000 1 .832E+00 1 .066E-02 1 .8A3E+00 A

1 .2500 1 .809E+00 1 .335E-02 1 .823E+00 5

1 . 5000 1 .801 E+00 1 .623E-02 1 .8I7E+00 7

1 .7500 1 .799E+00 1 . 927E-02 1 .81 9E+00 8 2.0000 1 .802E+00 2.2AAE-02 1 .82AE+00 9 2.5000 1 .81 lE+00 2. 91 OE-02 1 .8A0E+00 1 3.0000 1 .823E+00 3.612E-02 1 .859E+00 1 3.5000 1 .836E+00 A.3A3E-02 1 .879E+00 1

A. 0000 1 .8A8E+00 5. 100E-02 1 .899E+00 2 A. 5000 1 .859E+00 5.878E-02 1 . 918E+00 2 5.0000 1 .870E+00 6 .67AE-02 1 .937E+00 2 5.5000 1 .880E+00 7.A88E-02 1 . 955E+00 2 6.0000 1 .889E+00 8.317E-02 1 . 973E+00 3 7.0000 1 . 906E+00 1 .002E-01 2.006E+00 3 8.0000 1 . 921 E+00 1 .176E-01 2.039E+00 A 9.0000 1 .93AE+00 1 .35AE-01 2.070E+00 A 10.0000 1 . 9A6E+00 1 .536E-01 2.099E+00 5 12.5000 1 . 970E+00 2.002E-01 2. 170E+00 6 15.0000 1 . 990E+00 2.A82E-01 2.238E+00 7 17.5000 2.006E+00 2.973E-01 2.303E+00 8 20.0000 2. 01 9E+00 3.A72E-01 2.366E+00 9 25.0000 2.0A1E+00 A. A88E-01 2.A90E+00 1 30.0000 2.058E+00 5.523E-01 2.610E+00 1 35.0000 2.072E+00 6.571E-01 2.729E+00 1 AO . 0000 2.085E+00 7.631E-01 2.8A8E+00 1 A5.0000 2.095E+00 8.700E-01 2.965E+00 1 50.0000 2. lOAE+00 9.777E-01 3.082E+00 2 55.0000 2.11 3E+00 1 .086E+00 3.1 99E+00 2 60.0000 2.121E+00 1 . 1 95E+00 3.316E+00 2 70.0000 2.1 3AE+00 1 . A1 AE+00 3.5A8E+00 2 80.0000 2.1 A5E+00 1 .635E+00 3.781E+00 2 90.0000 2.1 56E+00 1 .853E+00 A.013E+00 3 100.0000 2. 165E+00 2.081 E+00 A.2A5E+00 3

1 25 .0000 2. 18AE+00 2.6A3E+00 A .827E+00 3

1 50 .0000 2. 1 99E+00 3.209E+00 5. A09E+00 A

1 75 .0000 2 .21 2E+00 3.779E+00 5.991E+00 A 200.0000 2.22AE+00 A . 351 E+00 6.57AE+00 5 250.0000 2.2A3E+00 5 . 500E+00 7 . 7A2E+00 6 300.0000 2.258E+00 6 .655E+00 8.913E+00 6 350.0000 2.271E+00 7 .81 AE+00 1 .008E+01 7 AOO . 0000 2.282E+00 8. 976E+00 1 . 1 26E+01 7 A50 .0000 2.292E+00 1 .01AE+01 1 .2A3E+01 8 500.0000 2.301E+00 1 . 1 31 E+01 1 .361E+01 8 550.0000 2.309E+00 1 . 2A8E+01 1 . A78E+01 8 600.0000 2.316E+00 1 . 36AE+01 1 .596E+01 9 700.0000 2.329E+00 1 .599E+01 1 .832E+01 9 800.0000 2. 3A1 E+00 1 .833E+01 2.067E+01 1 900.0000 2.351E+00 2.068E+01 2. 303E+01 1 1000.0000 2. 359E+00 2.303E+01 2.539E+01 1

- 1.1A0E+00 g/cm^

RADIATION DENS.EFF. dClog )/d(logI) YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

7.558E-05 0 .

-0.193 0.219 0.218

9.072E-05 0.0 -0.185 0.209 0.208

1 .052E-0A 0.0 -0.179 0.201 0.201

1 . 1 92E-0A 0.0 -0 . 1 7A 0.195 0.195

1 .327E-0A 0.0 -0.170 0.191 0.190

1 .586E-0A 0.0 -0 . 1 6A 0.183 0.182

1 .83AE-0A 0.0 -0.160 0.177 0.177

2.072E-0A 0.0 -0.156 0.172 0.172

2.302E-0A 0.0 -0.153 0.169 0.168

2.526E-0A 0.0 -0.150 0.165 0.165

2.7A3E-0A 0.0 -0.1A8 0.163 0.162

2.955E-0A 0.0 -0. 1 A6 0.160 0.160

3.162E-0A 0.0 -0 . 1 AA 0.158 0.158

3.56AE-0A 0.0 -0.1A1 0.15A 0 . 15A 3.951E-0A 0.0 -0.139 0.151 0.151 A.326E-0A 0.0 -0.137 0.1A9 0.1A9

A.690E-0A 0.0 -0.135 0 . 1 A7 0.1 A6 5.561E-0A 0.0 -0.131 0 . 1 A2 0.1 A2

6 . 3S8E-0A 0.0 -0.128 0.139 0.139

7. 179E-0A 0.0 -0.126 0.136 0.136

7.9A3E-0A 0.0 -0.12A 0 . 1 3A 0.133

9.A06E-0A 0.0 -0.121 0.130 0.130

1 .081E-03 0.0 -0.118 0.128 0.127

1 .217E-03 0.0 -0.106 0.125 0.1 2A

1 .351E-03 3. 157E-02 -0.087 0.119 0.117

1 . A8AE-03 6.655E-02 -0.080 O.llA 0.111

1 .617E-03 1 .032E-01 -0.075 0.109 0.105

1 .750E-03 1 . A09E-01 -0.070 0.10A 0.100

1 .883E-03 1 .793E-01 -0.066 0.100 0.095

2.151E-03 2.572E-01 -0.060 0.093 0.087

2.A22E-03 3.350E-01 -0.055 0.087 0.080

2.696E-03 A. 1 1 9E-01 -0.051 0.083 0.075

2.975E-03 A.872E-01 -0.0A8 0.078 0.070

3.689E-03 6.66AE-01 -0.0A2 0.070 0.061

A. A28E-03 8.319E-01 -0.038 0.06A 0.05A

5.1 90E-03 9.8A3E-01 -0.035 0.060 0.0A9

5.972E-03 1 . 125E+00 -0.033 0.056 0.0A6

7.587E-03 1 .375E+00 -0.030 0.051 O.OAO 9.258E-03 1 .59AE+00 -0.028 0.0A7 0.036

1 .097E-02 1 .786E+00 -0.027 O.OAA 0.03A

1 .272E-02 1 .959E+00 -0.025 0 .OAl 0.032

1 . A50E-02 2. 1 15E+00 -0.02A 0.039 0.030

1 .631E-02 2.258E+00 -0.023 0.038 0.029

1 .813E-02 2.390E+00 -0.023 0.036 0.027

1 .997E-02 2.513E+00 -0.022 0.035 0.026

2.370E-02 2.735E+00 -0.020 0.033 0.025

2.7A6E-02 2.932E+00 -0.019 0.031 0.023

3. 125E-02 3. 1 lOE+00 -0.018 0.030 0.022

3.505E-02 3.273E+00 -0.016 0.028 0.021

A. A59E-02 3.630E+00 -O.OIA 0.026 0.018

5. AlOE-02 3.933E+00 -0.011 0.023 0.016

6.352E-02 A.197E+00 -0.010 0.022 O.OIA 7.283E-02 A. A31E+00 -0.008 0.020 0.013

9.100E-02 A.83AE+00 -0.006 0.018 0.010

1 .085E-01 5. 171E+00 -O.OOA 0.016 0.008

1 .253E-01 5.A61E+00 -0.003 O.OIA 0.007

1 .A15E-01 5.715E+00 -0.003 0.013 0.006

1 .570E-01 5.9A2E+00 -0.002 0.012 0.005

1 .718E-01 6.1A5E+00 -0.002 0.011 O.OOA

1 .861E-01 6.331E+00 -0.002 0.010 O.OOA

1 . 997E-01 6.500E+00 -0.001 0.010 0.003

2.255E-01 6.802E+00 -0.001 0.009 0.003

2. A93E-01 7.065E+00 -0.001 0.008 0.002

2.71 3E-01 7.297E+00 -0.001 0.007 0.002

2.919E-01 7.506E+00 -0.001 0.007 0.002

3.375E-01 7. 9A8E+00 -0.000 0.006 0.001 3.765E-01 8.310E+00 -0.000 0.005 0.001

A. 102E-01 8.617E+00 -0.000 0.005 0.001 A.398E-01 8.883E+00 -0.000 0.005 0.001 A.893E-01 9. 327E+00 -0.000 O.OOA 0.001 5.293E-01 9.691E+00 -0.000 O.OOA 0.000

5.62AE-01 9. 999E+00 -0.000 0.003 0.000

5 . 90AE-01 1 .027E+01 -0.000 0.003 0.000

6 . 1 A5E-01 1 .050E+01 -0.000 0.003 0.000 6.35AE-01 1 .071E+01 -0.000 0.003 0.000

6.538E-01 1 .090E+01 -0.000 0.003 0.000

6.701E-01 1 . 1 08E+01 -0.000 0.003 0.000

6 . 978E-01 1 . 138E+01 -0.000 0.003 0.000

7.206E-01 1 . 165E+01 -0.000 0.002 0.000 7.397E-01 1 . 189E+01 -0 . 000 0.002 0.000 7.560E-01 1 .210E+01 -0.000 0.002 0.000

DENSITY

CSDA RANGE

g/cm ^ 458E-0A

651E-0‘t

0<i6E-0A 636E-0A

A1 AE-OA 251E-03

729E-03

272E-03

877E-03

5A2E-03

263E-03

038E-03

866E-03

670E-03

662E-03

183E-02

A16E-02

063E-02

791E-02

590E-02

A50E-02

322E-02

359E-02

052E-01 279E-01

515E-01 757E-01

C05E-01

258E-01

77AE-01

301E-01 836E-01

377E-01 7A2E-01

116E-01 A92E-01

865E-01

259E+00

530E+00

797E+00

062E+00

32AE+00

583E+00

8AOE+00

095E+00

597E+00

092E+00

579E+00

058E+00

229E+00

363E+00

A65E+00

536E+00

160E+01 356E+01 5A3E+01 722E+01

89AE+01

060E+01

21 9E+01 372E+01 66AE+01

937E+0I

1 9AE+01 A36E+01

988E+01 A77E+01

916E+01

31 AE+01

01 AE+01 615E+01

1 A3E+01 612E+01

03AE+01 A18E+01

771E+01

096E+01

680E+01

01 9E+02

065E+02

107E+02

132
ENERGY

MeV

0.0100

0.0125

0.0150

0.0175

0.0200

0.0250

0.0300

0.0350

0 . 0

<

t 00

0 . 0^50 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 . <*000 0.9500

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

9.0000

9.5000

5.0000

5.5000

6.0000

7 .0000 8.0000

9.0000

10.0000

12.5000

15.0000 17.5000

20.0000

25.0000

30.0000

35.0000

90.0000

95.0000

50.0000

55.0000

60.0000

70.0000

80.0000

90.0000

100.0000

125.0000

150.0000

175.0000

200.0000

250 .0000 300.0000

350.0000

900.0000

950.0000

500.0000

550.0000

600.0000

700.0000

800.0000

900.0000

1000.0000

ELECTRONS IN PARAFFIN WAX

55.9 eV DENSITY = 9.300E-01 g/cm

I =

STOPPING POWER

COLLISION RADIATIVE

dClog )/d(logI)

COLL CSDA RAD

LOSS RANGE YIELD

MeV cm^/g

2.969E+01

2.067E+01

1 .791E+01

1 .587E+01

1 .929E+01

1 .201 E+01

1 .099E+01 9.282E+00

8.399E+00

7.689E+00

7.1 17E+00

6 . 691 E+00

6 .291 E+00 5.601E+00

5.11 3E+00

9 .729E+00 9.918E+00

3.851E+00

3.969E+00

3.1 95E+00

2. 989E+00

2.703E+00

2.51 5E+00 2.385E+00

MeV cm^/g

2.826E-03

2.837E-03

2.899E-03

2.899E-03

2.859E-03

2.863E-03

2.873E-03

2.889E-03

2.895E-03

2. 908E-03

2. 921 E-03

2. 935E-03

2. 950E-03

2.981E-03

3.019E-03

3.050E-03

3.088E-03

3.1 90E-03

3. 300E-03

3.918E-03

3.592E-03

3.807E-03

9.097E-03

9.906E-03

TOTAL MeV cm^/g

2.969E+01

2.067E+01

1 .791E+01

1 .587E + 01

1 .930E + 01

1 .202E+01

1 .099E+01 9.285E+00

8.396E+00

7.692E+00

7.11 9E+00 6.699E+00

6.293E+00

5.609E+00

5.116E+00

9.732E+00

9.921E+00

3.855E+00

3.972E+00

3.1 98E+00

2.992E+00

2.706E+00

2.520E+00

2.390E+00

CSDA RANGE

g/cm ^ 2.285E-09

3. 398E-09

9.701E-09

6 . 187E-09

7.899E-09

1 . 168E-03

1 .616E-03

2.125E-03

2.692E-03

3 . 31 5E-03

3.991E-03

9.71 9E-03

5.996E-03

7.190E-03

9.060E-03

1 . 1 10E-02

1 .328E-02

1 . 936E-02

2.622E-02

3.373E-02

9. 182E-02

5.995E-02

7.869E-02

9.905E-02

RADIATION

YIELD

6 . 305E-05

7.565E-05

8.772E-05

9.936E-05

1 . 106E-09

1 . 323E-09

1 .531E-09

1 .731E-09

1 . 929E-09

2. 1 12E-09

2.295E-09

2.973E-09

2.698E-09

2. 988E-09

3.315E-09

3.632E-09

3.991E-09

9.680E-09

5.382E-09

6 .056E-09

6.707E-09

7.957E-09

9. 159E-09

1 .033E-03

DENS.EFF.

COP.R. (DELTA)

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0

0.0 0.0

0.0

0.0

0.0

0.0 0.0

0.0 0.0

0.0 0.0

0.0 2.999E-03

-0.188 0. -0.180 0. -0.175 0. -0.170 0. -0.167 0. -0.161 0. -0.156 0. -0.153 0. -0.150 0. -0.197 0. -0.195 0. -0.193 0. -0.192 0. -0.139 0. -0.136 0. -0.139 0. -0.133 0. -0.129 0. -0.126 0. -0.129 0.

- 0.122 0 . -0.119 0. -0.116 0.

- 0.100 0 .

213 0.212

203 0.202

196 0.195

190 0.190

186 0.185

178 0.178

173 0.172

168 0.168

165 0.165

162 0.161

159 0.159

157 0.157

155 0.155

151 0.151

198 0.198

196 0.196

199 0.199

190 0.139

136 0.136

139 0.133

132 0.131

128 0.127

126 0.125

123 0.122

2.287E+00

2.21 3E+00

2.1 56E+00

2.1 1 1E+00 2.079E+00

2.021E+00

1 . 989E+00

1 . 959E+00

9.736E-03

5.083E-03

5.996E-03

5.829E-03

6.215E-03

7.033E-03

7.893E-03

8.792E-03

2.292E+00

2.218E+00

2.161E+00

2.116E+00

2.081E+00

2.028E+00

1 .992E+00

1 .968E+00

1 .209E-01

1 .926E-01

1 .655E-01

1 .889E-01

2. 127E-01 2.619E-01

3. 1 12E-01 3.617E-01

1 . 198E-03 3.926E-02 -0.085 0.117 0.115

1 .263E-03 6.887E-02 -0.079 0.111 0.108

1 .377E-03 1 .055E-01 -0.073 0.106 0.103

1 .991E-03 1 .939E-01 -0.069 0.102 0.098

1 .606E-03 1 .823E-01 -0.065 0.098 0.093

1 .838E-03 2.619E-01 -0.058 0.091 0.085

2.072E-03 3.908E-01 -0.053 0.086 0.078

2.310E-03 9.1 93E-01 -0.099 0.081 0.073

1 . 991 E+00

1 .916E+00

1 . 906E+00

1 . 909E+00

1 .906E+00

1 .915E+00

1 .927E+00

1 . 990E+00

9.728E-03

1 .221E-02

1 .986E-02

1 .765E-02

2.057E-02

2.671 E-02

3.319E-02

3.999E-02

1 .951E+00

1 .928E+00

1 .921E+00

1 .922E+00

1 .926E+00

1 .992E+00

1 .960E+00

1 . 980E+00

9. 128E-01 5.918E-01

6.718E-01

8.01 9E-01

9.31 9E-01

1 .190E+00

1 .997E+00

1 .701E+00

2.552E-03

3. 172E-03

3.815E-03

9.978E-03

5. 159E-03

6.569E-03

8.031E-03

9.533E-03

9.962E-01

6.799E-01

8.985E-01

1 .009E+00

1 .197E+00

1 .903E+00

1 .625E+00

1 .821E+00

0.096

0.090

0.037

0.039

0.032

0.029

0.027

0.026

0.077

0.069

0.063

0.058

0.055

0.099

0.095

0.092

0.068

0.059

0.053

0.098

0.099

0.039

0.035

0.033

1 . 952E+00

1 . 969E+00

1 .975E + 00

1 . 985E+00

1 .995E+00 2.012E+00

2.027E+00

2. 090E+00

9.693E-02

5.91 IE-02 6.198E-02

6.900E-02

7.667E-02

9.238E-02

1 .085E-01

1 .250E-01

1 .999E+00

2.018E+00

2.036E+00

2.059E+00

2.071E+00

2. 109E+00

2.135E+00

2. 165E+00

1 .952E+00

2.201E+00

2.998E+00

2.692E+00

2.939E+00

3.913E+00

3.885E+00

9.350E+00

1 . 107E-02

1 .263E-02

1 .922E-02

1 .583E-02

1 .795E-02

2.079E-02

2.906E-02

2.792E-02

1 .997E+00

2.156E+00

2.302E+00

2.936E+00

2.561E+00

2.787E+00

2. 988E+00

3. 169E+00

0.029

0.023

0.023

0.022

0.021 0.019

0.018

0.017

0.090

0.038

0.037

0.035

0.039

0.032

0.030

0.029

0.031 0.029

0.028

0.027

0.026

0.029

0.022

0.021 2.052E+00

2.077E+00

2.097E+00

2.113E+00

2. 127E+00

2. 199E+00

2.167E+00

2. 181E+00

1 .91 9E-01

1 .851E-01 2.296E-01

2.751E-01

3.219E-01

9. 157E-01

5. 1 18E-01 6.093E-01

2.199E+00

2.262E+00

2.326E+00

2.388E+00

2.998E+00

2.565E+00

2.678E+00

2.791E+00

9.809E+00

5.931E+00

7.021E+00

8.081E+00

9.115E+00

1 .111E+01

1 .302E+01

1 .985E+01

3.080E-02

3.929E-02

9.779E-02

5.625E-02

6.962E-02

8.107E-02

9.701E-02

1 .129E-01

3.336E+00

3.699E+00

9.008E+00

9.277E+00

9.515E+00

9. 929E+00

5.265E+00

5.558E+00

0.015

0.012

0.010

0.008

0.007

0.005

0.009

0.003

0.027

0.025

0.022

0.021 0.019

0.016

0.015

0.013

0.020

0.017

0.015

0.013

0.012

0.009

0.007

0.006

2.1 99E+00

2.205E+00

2.219E+00

2.223E+00

2.231 E+00 2.295E+00

2.257E+00

2.268E+00

7.078E-01

8.072E-01

9.079E-01

1 . 008E+00

1 .1 10E+00

1 . 31 9E+00

1 .51 9E+00

1 .726E+00

2.902E+00

3.012E+00

3. 122E+00

3.231E+00

3.391E+00

3.559E+00

3.776E+00

3.999E+00

1 .660E+01

1 .829E+01

1 .992E+01 2.150E+01

2.302E+01

2.592E+01

2.865E+01

3.122E+01

1.273E-01 5.815E+00

1.916E-01 6.092E+00

1.559E-01 6.297E+00

1.686E-01 6.933E+00

1.819E-01 6.609E+00

2.057E-01 6.907E+00

2.282E-01 7.170E+00

2.992E-01 7.903E+00

-0.002 0.012 0.005

-0.002 0.011 0.009

-0.001 0.010 0.009

-0.001 0.009 0.003

-0.001 0.009 0.003

-0.001 0.008 0.002

-0.001 0.007 0.002

-0.001 0.007 0.002

2.277E+00

2.297E+00

2. 31 3E+00

2 . 327E+00

2 . 339E+00

2 . 358E+00

2.379E+00

2. 388E+00

1 . 939E+00

2.958E+00

2. 986E+00

3 . 51 7E+00 9.050E+00

5. 1 22E+00

6 . 1 99E+00

7.280E+00

9.21 1E+00 9.755E+00

5.299E+00

5.893E+00

6 . 388E+00

7.980E+00

8.573E+00

9.668E+00

3.366E+01

3.929E+01

9.922E+01

9.871E+01

5.280E+01

6 . 003E+01

6 . 627E+01

7. 176E+01

2.689E-01

3.1 30E-01 3.510E-01

3.892E-01

9.139E-01

9.629E-01

5.032E-01

5.368E-01

7.612E+00

8.059E+00

8.917E+00

8.729E+00

8.990E+00

9.935E+00

9.798E+00

1 .01 1E+01

- 0.000 0 - 0.000 0 - 0.000 0 - 0.000 0 - 0.000 0 - 0.000 0 - 0.000 0 - 0.000 0

.006 0.001

.005 0.001

.005 0.001

.009 0.001

.009 0.001

.009 0.000

.003 0.000

.003 0.000

2.900E+00

2.910E+00

2.91 9E+00 2.928E+00

2.935E+00

2.999E+00

2.961E+00

2.971E+00

8 . 365E+00

9.952E+00

1 .059E+01

1 . 1 63E+01

1 .272E + 01

1 .991 E+01

1 .710E+01

1 . 930E+01

1 .076E+01

1 . 186E+01

1 .296E+01

1 .906E+01

1 .516E+01

1 .736E+01

1 . 956E+01

2. 177E+01

7.666E+01

8. 108E+01

8.51 1E+01 8.881E+01

9.229E+01

9.890E+01

1 .038E+02

1 .087E+02

5.659E-01

5. 900E-01

6 . 1 1 6E-01

6 . 306E-01 6.975E-01

6.763E-01

7.002E-01

7.202E-01

1 .037E+01

1 .061E+01

1 .082E+01

1 . 101E+01

1 . 1 18E+01

1 . 199E+01

1 . 176E+01

1 . 1 99E+01

- 0.000 0 . - 0.000 0 . - 0.000 0 . - 0.000 0 . - 0.000 0 . - 0.000 0 . - 0.000 0 . - 0.000 0 .

003 0.000

003 0.000

003 0.000

002

0.000

002 0.000

002 0.000

002 0.000

002 0.000

2.980E+00 2.199E+01 2.397E+01 1 .130E+02 7.379E-01 1 .220E+01 - 0.000 0.002 0.000

133
ELECTRONS IN PHOTOGRAPHIC EMULSION

I = 331 .0 eV DENSITY = 3.815E+00 g/cm^

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^/g MeV cra^/g MeV cra^/g g/cm ^

0.0100 1 .302E+01 1 .310E-02 1 .304E + 01 4.664E-04 4.991E-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 .518E-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 0.286 0.274

0.0250 6.810E+00 1 .639E-02 6 .827E+00 2.161E-03 1 .231E-03 0.0 -0.225 0.269 0.258

0 .0300 5.983E+00 1 . 697E-02 6.000E+00 2. 945E-03 1 .462E-03 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 . OAOO 4.887E+00 1 .786E-02 4.905E+00 4.801E-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 2.121E-03 0.0 -0.200 0.231 0.225

0.0500 4.1 90E+00 1 .854E-02 4.209E+00 7.01 IE-03 2 . 330E-03 0.0 -0.196 0.225 0.220

0.0550 3 . 928E+00 1 .884E-02 3.947E+00 8.238E-03 2.536E-03 0.0 -0.192 0.221 0.215

0.0600 3.706E+00 1 . 91 OE-02 3.725E+00 9.543E-03 2.737E-03 0.0 -0.189 0.216 0.21 1 0.0700 3.349E+00 1 . 959E-02 3.369E+00 1 .237E-02 3.128E-03 0.0 -0.184 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 .870E-03 0.0 -0.176 0.199 0.195

0.1000 2.680E+00 2.081E-02 2.701E+00 2.242E-02 4.224E-03 0.0 -0.173 0.195 0.191 0.1250 2.356E+00 2.169E-02 2.378E+00 3.232E-02 5.064E-03 0.0 -0.167 0.187 0.184

0.1500 2. 1 36E+00 2.251E-02 2.159E+00 4.338E-02 5.850E-03 0.0 -0.162 0.181 0.178

0.1750 1 . 978E+00 2.329E-02 2.001 E+00 5.543E-02 6 .592E-03 0.0 -0.159 0.176 0.173

0 . 2000 1 .858E+00 2.405E-02 1 .883E+00 6 .833E-02 7.294E-03 0.0 -0.155 0.172 0.170

0 . 2500 1 .693E+00 2.560E-02 1 .718E+00 9.622E-02 8.606E-03 0.0 -0.150 0.166 0.163

0 . 3000 1 .585E+00 2.721E-02 1 .612E+00 1 .263E-01 9.822E-03 0.0 -0.147 0.161 0.159

0.3500 1 .509E+00 2.890E-02 1 .537E+00 1 .581E-01 1 .097E-02 1 .408E-02 -0.127 0.155 0.152

0 . 4000 1 .453E+00 3.066E-02 1 .484E+00 1 .913E-01 1 .206E-02 3.297E-02 -0.121 0.149 0.146

0.4500 1 .412E+00 3.251E-02 1 .444E+00 2.254E-01 1 .312E-02 5.225E-02 -0.117 0.144 0.141 0.5000 1 .381E+00 3.443E-02 1 .415E+00 2.604E-01 1 .41 5E-02 7.178E-02 -0.113 0.140 0.136 0.5500 1 . 356E+00 3.642E-02 1 .393E+00 2.960E-01 1 .516E-02 9. 146E-02 -0.109 0.136 0.132

0 .6000 1 . 338E+00 3 .846E-02 1 .376E+00 3.322E-01 1 .615E-02 1 .112E-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 4.71 lE-02 1 .342E+00 4.797E-01 2.000E-02 1 .895E-01 -0.097 0.122 0.116

0.9000 1 .284E+00 5.168E-02 1 .336E+00 5.544E-01 2. 187E-02 2.278E-01 -0.094 0.118 0.112

1 .0000 1 .278E+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 8. 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 .001E+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 .184E+00 3.742E-02 5. 186E-0

-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 .312E+00 1 .385E-01 1 .451E+00 1 .714E+00 5.089E-02 7.310E-01 -0.067 0.087 0.077

3.0000 1 . 331 E+00 1 .687E-01 1 .499E+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 2.381E+00 6.848E-02 9.707E-01 -0.060 0.079 0.067

4.0000 1 . 363E+00 2.317E-01 1 .595E+00 2.699E+00 7.708E-02 1 .077E+00 -0.057 0.075 0.063

4.5000 1 .377E+00 2.642E-01 1 .641E+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 9.385E-02 1 .268E+00 -0.052 0.070 0.057

5.5000 1 .401E+00 3.309E-01 1 .732E+00 3.601E+00 1 .020E-01 1 .355E+00 -0.050 0.068 0.055

6.0000 1 .412E+00 3.649E-01 1 .777E+00 3.886E+00 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 5.461E+00 1 .551E-01 1 .856E+00 -0.040 0.056 0.042

10.0000 1 .475E+00 6 .485E-01 2.123E+00 5. 942E+00 1 .690E-01 1 .975E+00 -0.038 0.054 0.040

12.5000 1 .502E+00 8.331E-01 2.335E+00 7.064E+00 2.015E-01 2.240E+00 -0.034 0.049 0.035

15.0000 1 .523E+00 1 .022E+00 2.545E+00 8.089E+00 2.312E-01 2.471E+00 -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 2.834E-01 2.858E+00 -0.026 0.040 0.025

25.0000 1 .579E+00 1 .802E+00 3.381E+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 .288E+01 3.659E-01 3.451E+00 -0.020 0.033 0.018

35.0000 1 .613E+00 2.606E+00 4.220E+00 1 .41 3E+01 3. 993E-01 3.689E+00 -0.018 0.031 0.016

40.0000 1 . 626E+00 3.015E+00 4.641E+00 1 .526E+01 4.286E-01 3.899E+00 -0.017 0.029 0.014

45.0000 1 .638E+00 3.426E+00 5.064E+00 1 .629E+01 4.547E-01 4.089E+00 -0.016 0.028 0.013

50.0000 1 . 648E+00 3.840E+00 5.488E+00 1 .724E+01 4.781E-01 4.261E+00 -0.015 0.027 0.012

55.0000 1 .657E+00 4.256E+00 5.913E+00 1 .812E+01 4. 992E-01 4.419E+00 -0.014 0.025 0.011 60.0000 1 .665E+00 4.674E+00 6.338E+00 1 .893E+01 5. 183E-01 4.565E+00 -0.013 0.025 0.010

70.0000 1 .678E+00 5.51 3E+00 7.192E+00 2.041E+01 5.518E-01 4.828E+00 -0.011 0.023 0.008

80.0000 1 .690E+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 2.291E+01 6.045E-01 5.266E+00 -0.009 0.021 0.007

100.0000 1 .709E+00 8.056E+00 9.766E+00 2.398E+01 6.258E-01 5.453E+00 -0.009 0.020 0.006 125.0000 1 .728E+00 1 .01 9E+01 1 . 1 92E+01 2.629E+01 6.688E-01 5.855E+00 -0.007 0.018 0.005

150.0000 1 .743E+00 1 .234E+01 1 .409E+01 2.822E+01 7.017E-01 6.190E+00 -0.006 0.017 0.004

175.0000 1 .755E+00 1 .450E+01 1 .625E+01 2.987E+01 7.279E-01 6 .476E+00 -0.005 0.016 0.003

200.0000 1 .766E+00 1 .666E+01 1 .843E+01 3.131E+01 7.492E-01 6.726E+00 -0.005 0.015 0.003

250.0000 1 .783E+00 2. 1 OOE+01 2.278E+01 3.375E+01 7.820E-01 7.147E+00 -0.004 0.014 0.002

300.0000 1 .797E+00 2.535E+01 2.714E+01 3.576E+01 8.064E-01 7.495E+00 -0.003 0.014 0.002

350.0000 1 .808E+00 2. 970E+01 3.151E+01 3.747E+01 8.252E-01 7.791E+00 -0.003 0.013 0.002

400.0000 1 .81 8E+00 3.407E+01 3.589E+01 3.895E+01 8.404E-01 8 . 048E+00 -0.003 0.012 0.002

450.0000 1 .827E+00 3.844E+01 4.027E+01 4.027E+01 8.528E-01 8.276E+00 -0.002 0.012 0.001 500.0000 1 .835E+00 4 . 281 E+01 4.465E+01 4. 145E+01 8 .632E-01 8.481E+00 -0.002 0.012 0.001 550.0000 1 .842E+00 4.71 9E+01 4. 903E+01 4.251E+01 8.720E-01 8.666E+00 -0 .002 0.011 0.001 600.0000 1 .848E+00 5. 157E+01 5.342E+01 4 . 349E+01 8.797E-01 8 .836E+00 -0.002 0.011 0.001

700 .0000 1 .859E+00 6 .034E+01 6.220E+01 4.522E+01 8.923E-01 9.1 38E+00 -0.001 0.011 0.001 800.0000 1 .869E+00 6 . 91 2E+01 7.099E+01 4.673E+01 9.023E-01 9.401E+00 -0.001 0.010 0.001 900.0000 1 .878E+00 7.790E+01 7.978E+01 4.806E+01 9.104E-01 9.633E+00 -0.001 0.010 0.001 1000.0000 1 .885E+00 8.669E+01 8.858E+01 4. 924E+01 9. 1 71 E-01 9.841E+00 -0.001 0.010 0.001

134
ELECTRONS IN PLASTIC SCINTILLATOR ( VINYLTOLUENE BASED)

I = 69.7 eV DENSITY = 1 .032E+0C• g/cm^

ENERGY STOPPING POWER CSDA RADIATION DENS. EPF. dClog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.265E+01 2. 965E-03 2.265E+01 2.995E-09 7.219E-05 0.0 -0 . 1 93 0.220 0.218

0.0125 1 .902E+01 2. 975E-03 1 .903E+01 3.709E-09 8.650E-05 0.0 -0.185 0.210 0.209

0.0150 1 .650E+01 2. 982E-03 1 .650E+01 5. 120E-09 1 .002E-09 0.0 -0.179 0 . 202 0.201 0.0175 1 .963E+01 2.987E-03 1 .963E+01 6 .732E-09 1 . 1 39E-09 0.0 -0.175 0.196 0.195

0.0200 1 . 318E+01 2.992E-03 1 .318E+01 8.535E-09 1 .262E-09 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-09 0.0 -0.165 0.183 0.183

0.0300 9.692E+00 3.010E-03 9.695E+00 1 .759E-03 1 .792E-09 0 .

-0.160 0.177 0.177

0.0350 8.578E+00 3.021E-03 8.581E+00 2.305E-03 1 .967E-09 0.0 -0.156 0.173 0.172

0 .OAOO 7.760E+00 3.032E-03 7.763E+00 2. 918E-03 2. 186E-09 0.0 -0.153 0.169 0.169

0.0A50 7.112E+00 3.095E-03 7.11 5E+00 3.592E-03 2.398E-09 0.0 -0.151 0.166 0.165

0 .0500 6.589E+00 3.058E-03 6.587E+00 9.323E-03 2.609E-09 0.0 -0.198 0.163 0.163

0.0550 6 . 1 96E+00 3.072E-03 6 . 1 50E+00 5. 109E-03 2.805E-09 0.0 -0.196 0.161 0.160

0.0600 5 .777E+00 3.087E-03 5.780E+00 5.998E-03 3.002E-09 0.0 -0.195 0.158 0.158

0.0700 5. 187E+00 3.11 9E-03 5.1 90E+00 7.778E-03 3. 389E-09 0.0 -0.192 0.155 0.155

0 .0300 9.737E+00 3. 153E-03 9.790E+00 9.797E-03 3.753E-09 0.0 -0.139 0.152 0.152

0.0900 9 . 382E+00 3. 189E-03 9.386E+00 1 . 1 99E-02 9.109E-09 0.0 -0.137 0.199 0.199

0.1000 9.095E+00 3.228E-03 9.099E+00 1 .935E-02 9.956E-09 0.0 -0.135 0.197 0.197

0.1250 3 . 572E+00 3.333E-03 3.575E+00 2.091E-02 5.286E-09 0.0 -0.131 0.193 0.192

0.1500 3.21 SE+00 3 . 996E-03 3.222E+00 2.830E-02 6 . 079E-09 0.0 -0.128 0.139 0.139

0.1750 2 . 965E+00 3 . 566E-03 2.969E+00 3.639E-02 6.823E-09 0.0 -0.126 0.137 0.136

0 .2000 2.775E+00 3.693E-03 2.779E+00 9.51 IE-02 7.557E-09 0.0 -0.129 0.139 0.139

0 . 2500 2.510E+00 3. 966E-03 2.519E+00 6.909E-02 8.953E-09 0.0 -0.121 0.131 0.130

0 . 3000 2 . 337E+00 9.269E-03 2.392E+00 8.979E-02 1 .029E-03 0.0 -0.118 0.128 0.127

0 . 3500 2.217E+00 9.583E-03 2.222E+00 1 .067E-01 1 . 160E-03 0.0 -0.117 0.126 0.125

0.9000 2 . 1 29E+00 9.923E-03 2.139E+00 1 .297E-01 1 .288E-03 1 .600E-02 -0.092 0.121 0.120

0.9500 2.061E+00 5.281E-03 2.066E+00 1 .535E-01 1 .915E-03 9.997E-02 -0.086 0.116 0.119

0.5000 2.009E+00 5.655E-03 2.019E+00 1 .780E-01 1 .591E-03 7.551E-02 -0.080 0.112 0.108

0.5500 1 . 967E+00 6 .095E-03 1 . 973E+00 2.031E-01 1 .668E-03 1 .089E-01 -0.075 0.107 0.103

0.6000 1 . 939E+00 6.998E-03 1 .991E+00 2.287E-01 1 .795E-03 1 .926E-01 -0.071 0.109 0.099

0 .7000 1 .886E+00 7.291E-03 1 .893E+00 2.809E-01 2.051E-03 2.1 39E-01 -0.069 0.097 0.091 0.8000 1 .853E+00 8. 178E-03 1 .861E+00 3.392E-01 2.310E-03 2.859E-01 -0.059 0.091 0.089

0 . 9000 1 .830E+00 9. 105E-03 1 .839E+00 3.883E-01 2.572E-03 3.579E-01 -0.055 0.086 0.079

1 .0000 1 .819E+00 1 .007E-02 1 .829E+00 9.929E-01 2.839E-03 9.289E-01 -0.051 0.082 0.079

1 .2500 1 .792E+00 1 .252E-02 1 .809E+00 5.808E-01 3.521E-03 5. 989E-01 -0.095 0 .079 0.06A

1.5000 1 .789E+00 1 .535E-02 1 .799E+00 7.1 96E-01 9.228E-03 7.575E-01 -0.091 0.068 0.053

1 .7500 1 .783E+00 1 .823E--02 1 .801E+00 8.586E-C1 9. 956E-03 9.091E-01 -0.038 0.063 0.053

2.0000 1 .785E + 00 2. 129E-02 1 .807E+00 9.972E-01 5.709E-03 1 .090E+00 -0.036 0.059 0.099

2.5000 1 .796E+00 2.756E-02 1 .823E+00 1 .273E+00 7.299E-03 1 .282E+00 -0.033 0.059 0.093

3.0000 1 .808E+00 3.923E-02 1 .892E+00 1 .596E+00 8.898E-03 1 .993E+00 -0.031 0.050 0.039

3.5000 1 .821 E+00 9.11 7E-02 1 .862E+C0 1 .816E+00 1 .099E-02 1 .680E+00 -0.029 0.097 0.037

9.0000 1 .833E+00 9.835E-02 1 .882E+00 2.083E+00 1 .217E-02 1 .898E+00 -0.028 0.099 0.039

9.5000 1 .895E+00 5.579E-02 1 .901E+00 2.397E+00 1 .387E-02 2.000E+00 -0.027 0.092 0.033

5.0000 1 .856E+00 6.331E-02 1 .919E+00 2.609E+00 1 .560E-02 2.139E+00 -0.026 0.091 0.031 5.5000 1 .866E+00 7. 105E-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 .959E+00 3.125E+00 1 .91 IE-02 2.387E+00 -0.029 0.038 0.029

7.0000 1 .892E+00 9.507E-02 1 -988E+00 3.632E+00 2.268E-02 2.609E+00 -0.022 0.036 0.027

8.0000 1 . 907E+00 1 . 1 16E-01 2.01 9E+00 9.132E+00 2.629E-02 2.798E+00 -0.021 0.039 0.025

9.0000 1 .921E+00 1 .286E-01 2.099E+00 9.623E+00 2.993E-02 2.973E+00 -0.019 0.032 0.029

10.0000 1 . 932E+00 1 .959E-01 2.078E+00 5. 108E+00 3.359E-02 3.139E+00 -0.018 0.031 0.023

12.5000 1 .957E+00 1 . 902E-01 2.197E+00 6.291E+00 9.275E-02 3.987E+00 -0.015 0.028 0.020

15.0000 1 . 976E+00 2.359E-01 2.212E+00 7.938E+00 5.191E-02 3.788E+00 -0.012 0.025 0.017

17.5000 1 .992E+00 2.826E-01 2.279E+00 8.553E+00 6.099E-02 9.051E+00 -0.010 0.023 0.015

20.0000 2.005E+00 3.301E-01 2.335E+00 9.637E+00 6.998E-02 9.286E+00 -0.008 0.022 0.013

25.0000 2.027E+00 9.268E-01 2.953E+00 1 . 173E+01 8.755E-02 9.689E+00 -0.006 0.019 0.011 30.0000 2.093E+00 5.259E-01 2.569E+00 1 .372E+01 1 .095E-01 5.028E+00 -0.009 0.017 0.009

35.0000 2.058E+00 6.252E-01 2.683E+00 1 .562E+01 1 .209E-01 5.319E+00 -0.003 0.015 0.007

90 .0000 2.069E+00 7.262E-01 2.796E+00 1 .795E+01 1 .366E-01 5.579E+00 -0.003 0.019 0.006

95.0000 2.080E+00 8.281E-01 2. 908E+00 1 .920E+01 1 .517E-01 5.801E+00 -0.002 0.012 0.005

50.0000 2.089E+00 9.306E-01 3.020E+00 2.089E+01 1 .662E-01 6 .005E+00 -0.002 0.012 0.009

55.0000 2.097E+00 1 .039E+00 3. 131E+00 2.251E+01 1 .801E-01 6.191E+00 -0.001 0.011 0.009

60.0000 2. 105E+00 1 . 1 38E+00 3.293E+00 2.908E+01 1 . 935E-01 6.361E+00 -0.001 0.010 0.003

70.0000 2. 1 18E+00 1 .397E+00 3.965E+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 2.986E+01 2.921E-01 6 . 926E+00 -0.001 0.008 0.002

90.0000 2. 1 39E+00 1 .769E+00 3. 909E+00 3.250E+01 2.638E-01 7.159E+00 -0.001 0.008 0.002

100.0000 2.198E+00 1 . 982E+00 9.130E+00 3.999E+01 2.891E-01 7.367E+00 -0.001 0.007 0.002

125.0000 2. 167E+00 2.518E+00 9.685E+00 9.066E+01 3.292E-01 7.810E+00 -0 . 000 0 .006 0.001 150.0000 2. 182E+00 3.058E+00 5.291E+00 9.571E+01 3.679E-01 8. 172E+00 -0.000 0.006 0.001 175.0000 2. 1 95E+00 3.601E+00 5.797E+00 5.029E+01 9.015E-01 8.979E+00 -0.000 0.005 0.001 200.0000 2.207E+00 9 . 1 97E+00 6.353E+00 5.936E+01 9.310E-01 8.795E+00 -0.000 0.005 0.001 250.0000 2.225E+00 5.293E+00 7 . 968E+00 6.161E+01 9.805E-01 9.1 90E+00 -0.000 0 .009 0.001 300.0000 2.290E+00 6 . 395E+00 8.585E+00 6.785E+01 5.207E-01 9.559E+00 -0.000 0.009 0.000

350.0000 2.253E+00 7.951E+00 9.709E+00 7.332E+01 5.590E-01 9 .861 E+00 -0.000 0 .009 0.000

900 .0000 2.269E+00 8 . 560E+00 1 .082E+01 7.820E+01 5.822E-01 1 .013E+01 -0.000 0 .003 0.000

950.0000 2.279E+00 9.671E+00 1 . 1 95E+01 8.260E+01 6 .065E-01 1 .036E+01 -0.000 0.003 0.000

500 .0000 2.283E+00 1 .078E+01 1 .307E+01 8.660E+01 6 .276E-01 1 .057E+01 -0 .000 0.003 0.000

550.0000 2.291E+00 1 . 1 90E+01 1 .91 9E+01 9.027E+01 6 .962E-01 1 .076E+01 -0.000 0.003 0.000

600.0000 2.298E+00 1 . 302E+01 1 .531E+01 9.366E+01 6.627E-01 1 .099E+01 -0.000 0.003 0.000

700.0000 2.31 1E+00 1 .525E+01 1 .756E+01 9. 975E+01 6 . 908E-01 1 . 125E+01 -0.000 0.003 0.000

800.0000 2.322E+00 1 .799E401 1 . 981 E+01 1 .051 E+02 7. 190E-01 1 .151E+01 -0 .000 0.002 0.000

900.0000 2.332E+00 1 . 973E+01 2.206E+01 1 .099E+02 7.339E-01 1 . 175E+01 -0.000 0.002 0.000

1000.0000 2.391E+00 2.1 98E+01 2.932E+01 1 .192E+02 7.500E-01 1 . 1 96E+01 -0.000 0.002 0.000

135
ELECTRONS IN POLYCARBONATE, "MAKROLON "LEXAN

I = 73.1 eV DENSITY = 1.200E+00 g/cm^

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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.1 53E+01 3.290E-03 2.153E+01 2.639E-09 8.291E-05 0.0 -0.198 0.226 0.225

0.0125 1 .810E+01 3.259E-03 1 .81 OE + 01 3 . 906E-09 9.938E-05 0.0 -0.190 0.215 0.219

0.0150 1 .571E+0I 3.263E-03 1 .571E + 01 5.393E-09 1 . 151E-09 0.0 -0.183 0.207 0.206

0.0175 1 .393E+01 3.270E-03 1 . 399E + 01 7 .086E-09 1 .303E-09 0.0 -0.178 0.201 0.200 0.0200 1 .256E+01 3.275E-03 1 .257E+01 8. 978E-09 1 .950E-09 0.0 -0.179 0.196 0.195

0.0250 1 .058E+01 3.289E-03 1 .058E+01 1 . 333E-03 1 .731E-09 0.0 -0.168 0.188 0.187

0.0300 9.202E+00 3.293E-03 9.205E+00 1 .892E-03 2.000E-09 0.0 -0.163 0.181 0.181 0.0350 8 . 1 90E+00 3. 309E-03 8.1 93E+00 2.91 9E-03 2.258E-09 0.0 -0.159 0.177 0.176

0 .OAOO 7.912E+00 3.315E-03 7.916E+00 3.061E-03 2.507E-09 0.0 -0.156 0.173 0.172

0 .0A50 6 .795E+00 3 . 327E-03 6.798E+00 3.766E-03 2.799E-09 0.0 -0.153 0.169 0.169

0.0500 6 .293E+00 3.390E-03 6 .296E+00 9.531E-03 2. 989E-09 0.0 -0.151 0.166 0.166

0.0550 5.876E+00 3.355E-03 5.879E+00 5.359E-03 3.213E-09 0.0 -0.199 0.169 0.169

0.0500 5.529E+00 3.370E-03 5.527E+00 6.231E-03 3.937E-09 0.0 -0.197 0.162 0.161

0 .0700 9. 962E+00 3.903E-03 9. 965E+00 8.199E-03 3.872E-09 0.0 -0.199 0.158 0.158

0.0800 9.533E+00 3.939E-03 9.536E+00 1 .025E-02 9.290E-09 0.0 -0.192 0.155 0.159

0.0900 9.199E+00 3.977E-03 9.1 98E+00 1 .255E-02 9.695E-09 0.0 -0.139 0.152 0.152

0.1000 3.920E+00 3.518E-03 3. 929E+00 1 .502E-02 5.088E-09 0.0 -0.137 0.150 0.199

0.1250 3.921E+00 3.629E-03 3.925E+00 2. 186E-02 6 .028E-09 0.0 -0.139 0.195 0.195

0.1500 3.089E+00 3.799E-03 3.088E+00 2.957E-02 6 . 91 9E-09 0.0 -0.131 0.192 0.191 0.1750 2.892E+00 3.877E-03 2.896E+00 3.802E-02 7.772E-09 0.0 -0.128 0.139 0.138

0.2000 2.660E+00 9.013E-03 2.669E+00 9.71 lE-02 8.599E-09 0.0 -0.126 0.137 0.136

0.2500 2.907E+00 9.309E-03 2.912E+00 6.691E-02 1 .017E-03 0.0 -0.123 0.133 0.132

0 . 3000 2.292E+00 9.623E-03 2.297E+00 8.893E-02 1 . 168E-03 0.0 -0.120 0.130 0.129

0.3500 2. 128E+00 9.969E-03 2.133E+00 1 . 1 13E-01 1 .319E-03 0.0 -0.118 0.128 0.126

0 . AOOO 2.099E+00 5.327E-03 2.050E+00 1 .352E-01 1 .958E-03 5.680E-03 -0.098 0.125 0.123

0 .9500 1 . 980E+00 5.710E-03 1 . 986E+00 1 .600E-01 1 .600E-03 3.1 96E-02 -0.089 0.120 0.117

0.5000 1 . 930E+00 6 . 1 12E-03 1 .936E+00 1 .855E-01 1 .791E-03 6.091E-02 -0.083 0.115 0.112

0.5500 1 .891E+00 6.529E-03 1 .897E+00 2. 1 16E-01 1 .883E-03 9.181 E-02 -0.078 0.111 0.107

0.6000 1 .859E+00 6.961E-03 1 .866E+00 2.382E-01 2.025E-03 1 .291E-01 -0.079 0.107 0.102

0.7000 1 .81 3E+00 7 .869E-03 1 .821 E+00 2. 925E-01 2.31 OE-03 1 . 91 3E-01 -0.067 0.100 0.099

0.8000 1 .782E+00 8.813E-03 1 .791E+00 3.979E-01 2.599E-03 2.602E-01 -0.061 0.099 0.087

0.9000 1 .761 E+00 9.806E-03 1 .771E+00 9.091 E-01 2.891E-03 3.293E-01 -0.057 0.089 0.082

1 . 0000 1 .796E+00 1 .089E-02 1 .757E+00 9.608E-01 3. 187E-03 3. 978E-01 -0.053 0.085 0.077

1 .2500 1 .726E+00 1 .357E-02 1 .739E+00 6 .039E-01 3.996E-03 5.631E-01 -0.097 0.077 0.067

1 .5000 1 .71 9E+00 1 .650E-02 1 .735E+00 7.979E-01 9.730E-03 7. 177E-01 -0.092 0.070 0.060

1 .7500 1 .718E+00 1 . 958E-02 1 .738E+00 8.91 9E-01 5.537E-03 8.61 lE-01 -0.039 0.065 0.055

2.0000 1 .721E+00 2.279E-02 1 .799E+00 1 .036E+00 6.365E-03 9.991E-01 -0.037 0.062 0.050

2.5000 1 .731E+00 2.955E-02 1 .761E+00 1 .321E+00 8.075E-03 1 .233E+00 -0.033 0.056 0.095

3.0000 1 .799E+00 3.667E-02 1 .781E+00 1 .603E+00 9.892E-03 1 .991E+00 -0.031 0.051 0.090

3.5000 1 .757E+00 9.908E-02 1 .801E+00 1 .883E+00 1 . 165E-02 1 .626E+00 -0.030 0.098 0.038

9.0000 1 .769E+00 5. 179E-02 1 .821E+00 2.159E+00 1 .350E-02 1 .792E+00 -0.028 0.096 0.035

9.5000 1 .780E+00 5. 962E-02 1 .890E+00 2.932E+00 1 .538E-02 1 .992E+00 -0.027 0.099 0.033

5.0000 1 .791E+00 6.770E-02 1 .859E+00 2.702E+00 1 .728E-02 2.080E+00 -0.026 0.092 0.032

5.5000 1 .801E+00 7.599E-02 1 .877E+00 2.970E+00 1 .921E-02 2.207E+00 -0.025 0.090 0.031 6.0000 1 .81 lE+00 8.939E-02 1 .895E+00 3.235E+00 2.1 15E-02 2.325E+00 -0.029 0.039 0.029

7.0000 1 .827E+00 1 .015E-01 1 .929E+00 3.758E+00 2.506E-02 2.539E+00 -0.023 0.037 0.028

8.0000 1 .892E+00 1 . 1 92E-01 1 .961E+00 9.272E+00 2.902E-02 2.730E+00 -0.021 0.035 0.026

9.0000 1 .855E+00 1 .373E-01 1 .992E+00 9.778E+00 3.300E-02 2. 903E+00 -0.020 0.033 0.029

10.0000 1 .867E+00 1 .557E-01 2.022E+00 5.276E+00 3.699E-02 3.061E+00 -0.019 0.032 0.023

12.5000 1 .891E+00 2.029E-01 2.099E+00 6.991E+00 9.699E-02 3.908E+00 -0.016 0.029 0.020

15.0000 1 . 910E+00 2.515E-01 2. 162E+00 7.665E+00 5.693E-02 3.709E+00 -0.013 0.026 0.018

17.5000 1 . 926E+00 3.01 IE-01 2.227E+00 8.805E+00 6 .677E-02 3.963E+00 -0.011 0.029 0.016

20.0000 1 . 939E+00 3.516E-01 2.291E+00 9.911E+00 7.698E-02 9.1 93E+00 -0.009 0.023 0.019

25.0000 1 .961E+00 9.599E-01 2.915E+00 1 .209E+01 9.539E-02 9.590E+00 -0.007 0.020 0.012

30.0000 1 . 978E+00 5.591E-01 2.537E+00 1 .906E+01 1 . 1 36E-01 9. 929E+00 -0.005 0.018 0.009

35.0000 1 . 992E+00 6 .652E-01 2.657E+00 1 .598E+01 1 .310E-01 5.212E+00 -0.009 0.016 0.008

90.0000 2.003E+00 7.729E-01 2.776E+00 1 .782E+01 1 .977E-01 5.969E+00 -0.003 0.015 0.007

95.0000 2.019E+00 8.805E-01 2.899E+00 1 .959E+01 1 .637E-01 5.689E+00 -0.003 0.013 0.006

50.0000 2.023E+00 9.899E-01 3.012E+00 2.128E+01 1 .789E-01 5.892E+00 -0.002 0.012 0.005

55.0000 2.031E+00 1 .099E+00 3.130E+00 2.291E+01 1 .936E-01 6.077E+00 -0.002 0.012 0.005

60.0000 2.038E+00 1 .209E+00 3.297E+00 2.998E+01 2.076E-01 6.296E+00 -0.002 0.011 0.009

70.0000 2.051E+00 1 .931E+00 3.982E+00 2.795E+01 2.339E-01 6.597E+00 -0.001 0.010 0.003

80.0000 2.062E+00 t .659E+00 3.717E+00 3.023E+01 2.582E-01 6.809E+00 -0.001 0.009 0.003

90.0000 2.072E+00 1 -879E+00 3.951E+00 3.289E+01 2.807E-01 7.091E+00 -0.001 0.008 0.002

100.0000 2.081E+00 2.105E+00 9. 185E+00 3.530E+01 3.016E-01 7.299E+00 -0.001 0.008 0.002

125.0000 2.099E+00 2.673E+00 9.772E+00 9.089E+01 3.978E-01 7.691E+00 -0.000 0.007 0.001 150.0000 2.1 19E+00 3.295E+00 5.359E+00 9.583E+01 3.871E-01 8.053E+00 -0.000 0.006 0.001 175.0000 2. 127E+00 3.820E+00 5.997E+00 5.025E+01 9.210E-01 8. 360E+00 -0.000 0.006 0.001 200.0000 2. 138E+00 9.398E+00 6 .536E+00 5.926E+01 9.507E-01 8.625E+00 -0.000 0.005 0.001 250.0000 2. 156E+00 5 . 560E+00 7.715E+00 6.130E+01 5.001E-01 9.070E+00 -0.000 0.005 0.001 300.0000 2. 171E+00 6 .726E + 00 8.897E+00 6 .733E+01 5.900E-01 9.939E+00 -0.000 0.009 0.001 350.0000 2. 183E+00 7.897E+00 1 .008E+01 7.260E+01 5.729E-01 9.791E+00 -0.000 0.009 0.000

900,0000 2. 1 99E+00 9.071E+00 1 . 127E+01 7.729E+01 6 .006E-01 1 .001 E+01 -0.000 0.009 0 .000 950.0000 2.209E+00 1 .025E+01 1 .295E+01 8 . 1 51 E+01 6 . 299E-01 1 .029E+01 -0.000 0.003 0.000

500.0000 2.212E+00 1 . 193E+01 1 .369E+01 8.535E+0I 6 .950E-01 1 .095E+01 -0.000 0.003 0.000

550.0000 2.220E+00 1 .261 E+01 1 .983E+01 8 .886E+01 6 .631 E-01 1 .069E+01 -0.000 0.003 0.000

600.0000 2.227E+00 1 .379E+01 1 .601 E+01 9.21 1E+01 6 . 791 E-01 1 .082E+01 -0.000 0.003 0.000 700.0000 2.239E+00 1 .61 5E+01 1 .839E+01 9.793E+01 7.069E-01 1 .113E+01 -0.000 0.003 0.000 800.0000 2.250E+00 1 .852E+01 2.077E+01 1 .030E+02 7.288E-01 1 . 139E+01 -0.000 0.003 0.000

900.0000 2.260E+00 2.089E+01 2.315E+01 1 .076E+02 7.975E-01 1 . 163E+01 -0.000 0.003 0.000

1000.0000 2.268E+00 2.327E+01 2.559E+01 1 . 1 17E+02 7.639E-01 1 . 189E+01 -0.000 0.003 0.000

136
ELECTRONS IN POLYETHYLENE

I = 57.4 eV DENSITY = 9.400E-01 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. d( log1 )/cKlogI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^

0.0100 2.441E+01 2.837E-03 2.442E+01 2.308E-04 6.391E-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+01 4.745E-04 8.887E-05 0.0 -0.176 0.197 0.196

0.0175 1 .573E+01 2.860E-03 1 .573E+01 6.244E-04 1 . 007E-04 0.0 -0.171 0.191 0.191 0.0200 1 .417E+01 2.864E-03 1 .417E+01 7.921E-04 1 . 121E-04 0.0 -0.167 0.187 0.186

0.0250 1 .191E+01 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+01 2.883E-03 1 .036E+01 1 .630E-03 1 .550E-04 0.0 -0.157 0.174 0.173

0.0350 9.206E+00 2.894E-03 9.209E+00 2. 143E-03 1 .752E-04 0.0 -0.153 0.169 0.169

0.0^00 8.325E+00 2. 905E-03 8.328E+00 2.71 5E-03 1 . 948E-04 0.0 -0.150 0.166 0.165

0. 0^(50 7.627E+00 2. 918E-03 7.630E+00 3.343E-03 2.1 38E-04 0.0 -0.148 0.162 0.162

0.0500 7.060E+00 2.931E-03 7.063E+00 4.025E-03 2.323E-04 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 0.157

0.0600 6.191E+00 2. 960E-03 6.194E+00 5.541E-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 3.061E-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 3.201E-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 3.446E+00 2.642E-02 5.443E-04 0.0 -0.127 0.137 0.137

0.1750 3. 171E+00 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 4.215E-02 6.782E-04 0.0 -0.122 0.132 0.132

0.2500 2.683E+00 3.820E-03 2.687E+00 5.991E-02 8.045E-04 0.0 -0.119 0.129 0.128

0 . 3000 2.497E+00 4.110E-03 2.501E+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.^000 2.272E+00 4.750E-03 2.277E+00 1 .213E-01 1 . 160E-03 2.626E-02 -0.087 0.118 0.116

0.4500 2.199E+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-01 1 .391E-03 9.409E-02 -0.075 0.108 0.104

0.5500 2.097E+00 5.841E-03 2. 103E+00 1 .902E-01 1 .506E-03 1 .307E-01 -0.070 0.104 0.099

0.6000 2.061E+00 6.233E-03 2.068E+00 2. 142E-01 1 .622E-03 1 .683E-01 -0.066 0.100 0.095

0.7000 2.008E+00 7.053E-03 2.016E+00 2.632E-01 1 .856E-03 2.453E-01 -0.060 0.093 0.087

0.8000 1 . 972E+00 7.915E-03 1 .980E+00 3.133E-01 2.092E-03 3.231E-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 .917E+00 5.452E-01 3.200E-03 6.568E-01 -0.041 0.070 0.060

1 .5000 1 .895E+00 1 .490E-02 1 .910E+00 6.759E-01 3.848E-03 8.243E-01 -0.037 0.064 0.054

1 .7500 1 .893E+00 1 .770E-02 1 .911E+00 8.068E-01 4.516E-03 9.785E-01 -0.034 0.059 0.049

2.0000 1 .895E+00 2.062E-02 1 .916E+00 9.375E-01 5.203E-03 1 .121E+00 -0.032 0.055 0.045

2.5000 1 .905E+00 2.678E-02 1 .932E+00 1 .197E+00 6 .623E-03 1 .375E+00 -0.029 0.050 0.039

3.0000 1 .917E+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 .710E+00 9.608E-03 1 .791E+00 -0.026 0.043 0.033

4.0000 1 -942E+00 4.704E-02 1 .989E+00 1 .963E+00 1 . 1 16E-02 1 .966E+00 -0.025 0.041 0.031 4.5000 1 . 954E+00 5.424E-02 2.008E+00 2.213E+00 1 .273E-02 2. 124E+00 -0.024 0.039 0.029

5.0000 1 . 965E+00 6.162E-02 2.026E+00 2.461E+00 1 .433E-02 2.269E+00 -0.023 0.037 0.028

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 2.061E+00 2.950E+00 1 .758E-02 2.527E+00 -0.021 0.035 0.026

7.0000 2.002E+00 9.259E-02 2.094E+00 3.431E+00 2.089E-02 2.751E+00 -0.020 0.032 0.024

8.0000 2.017E+00 1 .088E-01 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 2.156E+00 4.372E+00 2.762E-02 3.132E+00 -0.017 0.029 0.021 10.0000 2.042E+00 1 .422E-01 2. 184E+00 4.833E+00 3.102E-02 3.298E+00 -0.016 0.028 0.020

12.5000 2.067E+00 1 .855E-01 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 2.317E+00 7.054E+00 4.81 IE-02 3.967E+00 -0.010 0.023 0.015

17.5000 2. 103E+00 2.757E-01 2.379E+00 8.119E+00 5.661E-02 4.235E+00 -0.009 0.021 0.013

20.0000 2. 1 17E+00 3.220E-01 2.439E+00 9.157E+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 16E+01 8.156E-02 4.880E+00 -0.005 0.017 0.009

30.0000 2.157E+00 5. 129E-01 2.670E+00 1 .307E+01 9.759E-02 5.221E+00 -0.004 0.015 0.008

35.0000 2. 171E+00 6. 105E-01 2.782E+00 1 .491E+01 1 .131E-01 5.514E+00 -0.003 0.013 0.006

40.0000 2. 184E+00 7.092E-01 2.893E+00 1 .667E+01 1 .280E-01 5.770E+00 -0.002 0.012 0.005

45.0000 2.1 95E+00 8.088E-01 3.004E+00 1 .837E+01 1 .424E-01 5.997E+00 -0.002 0.011 0.005

50.0000 2.204E+00 9.092E-01 3.114E+00 2.000E+01 1 .562E-01 6.202E+00 -0.001 0.010 0.004

55.0000 2.21 3E+00 1 .OlOE+00 3.223E+00 2. 158E+01 1 .695E-01 6.388E+00 -0.001 0.010 0.003

60.0000 2.221E+00 1 . 1 12E+00 3.333E+00 2.310E+01 1 .824E-01 6 .558E+00 -0.001 0.009 0.003

70.0000 2.235E+00 1 .316E+00 3.551E+00 2.601E+01 2.067E-01 6.861E+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 3.1 32E+01 2.504E-01 7.357E+00 -0.001 0.007 0.002

100.0000 2.267E+00 1 .938E+00 4.205E+00 3.376E+01 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+01 3. 142E-01 8.009E+00 -0.000 0.005 0.001 150.0000 2.303E+00 2.991E+00 5.294E+00 4.434E+01 3.523E-01 8.371E+00 -0.000 0.005 0.001 175.0000 2.316E+00 3.523E+00 5 .839E + 00 4.883E+01 3.855E-01 8.678E+00 -0.000 0.004 0.001 200.0000 2.328E+00 4.057E+00 6.385E+00 5.293E+01 4. 148E-01 8.944E+00 -0.000 0.004 0.001 250.0000 2. 348E+00 5.1 31E+00 7.479E+00 6.015E+01 4.642E-01 9.389E+00 -0.000 0.004 0.000

300.0000 2.364E+00 6.210E+00 8.574E+00 6.639E+01 5.045E-01 9.753E+00 -0.000 0.003 0.000

350.0000 2.377E+00 7.294E+00 9.671E+00 7. 188E+01 5.381E-01 1 .006E+01 -0.000 0.003 0.000

400.0000 2.389E+00 8 . 380E+00 1 .077E+01 7.678E+01 5.667E-01 1 .033E+01 -0.000 0.003 0.000

450.0000 2.399E+00 9.469E+00 1 . 187E + 01 8. 120E+01 5. 91 3E-01 1 .056E+01 -0.000 0.003 0.000

500.0000 2.409E+00 1 .056E+01 1 .297E+01 8.523E+01 6. 128E-01 1 .077E+01 -0.000 0.003 0.000

550.0000 2.417E+00 1 . 165E+01 1 .407E + 01 8.893E+01 6.318E-01 1 .096E+01 -0.000 0.002 0.000

600.0000 2.425E+00 1 .275E+01 1 .517E+01 9.235E+01 6.487E-01 1 . 1 14E+01 -0.000 0.002 0.000

700.0000 2.438E+00 1 .494E+01 1 .738E+01 9.851E+01 6 .775E-01 1 . 144E+01 -0.000 0.002 0.000

800.0000 2.450E+00 1.71 3E+01 1 . 958E+01 1 .039E+02 7.012E-01 1 . 171E+01 -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+01 1 . 1 31E+02 7 . 383E-01 1 .216E+01 -0.000 0.002 0.000
ELECTRONS IN POLYETHYLENE TEREPTHALATE. "MYLAR

I = 78.7 eV DENSITY = 1 .AOOE+00' g/cm

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 cm^/g MeV cm^/g MeV cra^/g g/cm ^

0.0100 2.095E+01 3.A31E-03 2.095E+01 2.712E-0A 9.01 3E-05 0.0 -0.201 0.230 0.228

0.0125 1 .762E+01 3. AA8E-03 1 .763E+01 A.019E-0A 1 .081E-0A 0.0 -0.192 0.219 0.218

0.0150 1 .530E+01 3. A59E-03 1 -530E+01 5.5A5E-0A 1 .252E-0A 0.0 -0.186 0.211 0.210

0.0175 1 .358E+01 3.A66E-03 1 .358E+01 7.283E-0A 1 .A17E-0A 0.0 -0.181 0 .20A 0.203

0.0200 1 .225E+01 3. A71E-03 1 .225E+01 9.22AE-0A 1 .577E-0A 0.0 -0.177 0.199 0.198

0.0250 1 .032E+01 3.A81E-03 1 .032E+01 1 .369E-03 1 .882E-0A 0.0 -0.170 0.190 0.190

0.0300 8. 978E+00 3. A90E-03 8.982E+00 1 .890E-03 2.17AE-0A 0.0 -0.165 0.18A 0.183

0.0350 7.993E+00 3.500E-03 7. 997E+00 2. A81E-03 2. A5AE-0A 0.0 -0.161 0.179 0.179

O.OAOO 7.236E+00 3.51 lE-03 7.239E+00 3.1 39E-03 2.72AE-0A 0.0 -0.158 0.175 0.1 7A

0 . 0A50 6.635E+00 3.52AE-03 6 .638E+00 3.862E-03 2. 986E-0A 0.0 -0.155 0.171 0.171 0.0500 6. 1A5E + 00 3.537E-03 6.1A9E+00 A.6A5E-03 3.2A0E-0A 0.0 -0.153 0.168 0.168

0.0550 5.739E+00 3.552E-03 5.7A2E+00 5. A87E-03 3. A8SE-0A 0.0 -0.151 0.166 0.166

0 .0600 5.396E+00 3.567E-03 5.399E+00 6.386E-03 3.731E-0A 0.0 -0.1A9 0.16A 0.163

0.0700 A .8A8E+00 3.601E-03 A.852E+00 8.3AAE-03 A.200E-0A 0.0 -0.1 A6 0.160 0.159

0 .0800 A. A30E+00 3.637E-03 A. A33E+00 1 .050E-02 A.652E-0A 0.0 -0.1A3 0.157 0.156

0.0900 A . 1 OOE+00 3.677E-03 A. 103E+00 1 .285E-02 5.089E-0A 0.0 -O.lAl 0.1 5A 0.153

0.1000 3.832E+00 3.71 9E-03 3.836E+00 1 .537E-02 5.51 3E-0A 0.0 -0.139 0.151 0.151

0 . 1 250 3. 3A5E+00 3.835E-03 3.3A9E+00 2.238E-02 6 .527E-0A 0.0 -0.135 0.1A7 0 . 1 A6 0.1500 3.016E+00 3.960E-03 3.020E+00 3.026E-02 7.A87E-0A 0.0 -0.132 0.1A3 0. 1A3 0.1750 2.780E+00 A.09AE-03 2.78AE+00 3.890E-02 8. A05E-OA 0.0 -0.129 0. 1 AO O.IAO 0.2000 2.603E+00 A.235E-03 2.607E+00 A.81 9E-02 9.290E-OA 0.0 -0.127 0.138 0.137

0.2500 2.356E+00 A.5A0E-03 2.361E+00 6.8A1E-02 1 .098E-03 0.0 -0.1 2A 0.1 3A 0.133

0.3000 2.195E+00 A.873E-03 2.200E+00 9.0A0E-02 1 .260E-03 0.0 -0.121 0.131 0.130

0.3500 2.083E+00 5.230E-03 2.088E+00 1 .138E-01 1 .A17E-03 0.0 -0.119 0.129 0.128

0 .0000 2.001E+00 5.610E-03 2.007E+00 1 .382E-01 1 .571E-03 9.379E-03 -0.09A 0.125 0.12A

0.0500 1 . 938E+00 6.011E-03 1 .9AAE+00 1 .635E-01 1 .72AE-03 3.706E-02 -0.089 0.120 0.118

0.5000 1 .889E+00 6.A31E-03 1 .896E+00 1 .896E-01 1 .875E-03 6.709E-02 -0.083 0.116 0.112

0.5500 1 .851E+00 6 .868E-03 1 .858E+00 2.162E-01 2.027E-03 9.882E-02 -0.078 0.111 0.107

0.6000 1 .821E+00 7.320E-03 1 .828E+00 2. A3AE-01 2.179E-03 1 .318E-01 -0.07A 0.107 0.103

0 .7000 1 .776E+00 8.265E-03 1 .78AE+00 2.988E-01 2.A8AE-03 1 .999E-01 -0.067 0.100 0.09A

0.8000 1 .7A5E+00 9.259E-03 1 .755E+00 3.55AE-01 2.793E-03 2.69AE-01 -0.061 0.09A 0.088

0 . 9000 1 .72AE+00 1 .030E-02 1 .735E+00 A.127E-01 3.106E-03 3.390E-01 -0.057 0.090 0.082

1 . 0000 1 .710E+00 1 . 1 38E-02 1 .721E+00 A.706E-01 3.A22E-03 A.077E-01 -0.053 0.085 0.077

1 .2500 1 .690E+00 1 . A2AE-02 1 .705E+00 6.167E-01 A.233E-03 5.73AE-01 -0.0A7 0.077 0.067

1.5000 1 .68AE+00 1 .730E-02 1 .701 E+00 7.635E-01 5.070E-03 7.283E-01 -0.0A2 0.070 0.060

1 .7500 1 .683E+00 2.052E-02 1 .70AE+00 9.10AE-01 5. 931E-03 8.71 9E-01 -0.039 0.066 0.055

2.0000 1 .686E+00 2.388E-02 1 .710E+00 1 .057E+00 6.815E-03 1 .005E+00 -0.037 0.062 0.051 2.5000 1 .697E+00 3.09AE-02 1 .728E+00 1 .3A8E+00 8.637E-03 1 .2AAE+00 -0.033 0.056 0.0A5

3 .0000 1 .709E+00 3.838E-02 1 .7A8E+00 1 .636E+00 1 .052E-02 1 . A53E+00 -0.031 0.052 0.0A1 3.5000 1 .722E+00 A.612E-02 1 .768E+00 1 . 920E+00 1 .2A5E-02 1 .638E+00 -0.030 0.0A8 0.038

A. 0000 1 .73AE+00 5. A1 3E-02 1 .788E+00 2.201E+00 1 .AAlE-02 1 .80AE+00 -0.028 0.0A6 0.035

A .5000 1 .7A5E+00 6.236E-02 1 .808E+00 2. A79E+00 1 .6A1E-02 1 .955E+00 -0.027 O.OAA 0.033

5.0000 1 .756E+00 7.079E-02 1 .827E+00 2.755E+00 1 .8A3E-02 2.093E+00 -0.026 0.0A2 0.032

5.5000 1 .766E+00 7.9A0E-02 1 .8A5E+00 3.027E+00 2.0A7E-02 2.220E+00 -0.025 O.OAO 0.031 6.0000 1 .775E+00 8.816E-02 1 .863E+00 3.296E+00 2.253E-02 2.339E+00 -0.02A 0.039 0.029

7.0000 1 .792E+00 1 .061E-01 1 .898E+00 3.828E+00 2.669E-02 2.553E+00 -0.023 0.037 0.027

8.0000 1 .806E+00 1 .2A5E-01 1 .931E+00 A.351E+00 3.088E-02 2.7AAE+00 -0.022 0.035 0.026

9.0000 1 .81 9E+00 1 . A3AE-01 1 .963E+00 A.86AE+00 3.509E-02 2.917E+00 -0.020 0.033 0.02A

10.0000 1 .831E+00 1 .626E-01 1 .993E+00 5.370E+00 3.931E-02 3.075E+00 -0.019 0.032 0.023

12.5000 1 .855E+00 2.1 18E-01 2.066E+00 6.601E+00 A.986E-02 3. A20E+00 -0.016 0.029 0.020 15.0000 1 .87AE-^00 2.625E-01 2.136E+00 7.791E+00 6 .03AE-02 3.715E+00 -0.01 A 0.026 0.018

17.5000 1 .889E+00 3. 1 A2E-01 2.20AE+00 8.9A3E+00 7.069E-02 3.972E+00 -0.012 0.02A 0.016

20 .0000 1 .903E+00 3.668E-01 2.270E+00 1 .006E+01 8.087E-02 A.201E+00 -0.010 0.023 0.015

25.0000 1 . 92AE+00 A.7A0E-01 2.398E+00 1 .220E+01 1 .007E-01 A.595E+00 -0.007 0.020 0.012

30.0000 1 . 9A1 E+00 5.830E-01 2.52AE+00 1 .A2AE+01 1 . 1 96E-01 A.927E+00 -0.006 0.018 0.010

35.0000 1 . 955E+00 6.93AE-01 2.6A8E+00 1 .617E+01 1 .378E-01 5.213E+00 -O.OOA 0.016 0.008

AO .0000 1 .967E+00 8.051E-01 2.772E+00 1 .801E+01 1 .551E-01 5. A6AE+00 -0 .OOA 0.015 0.007

A5.0000 1 .977E+00 9. 177E-01 2.89AE+00 1 . 978E+01 1 .716E-01 5.689E+00 -0.003 0.01 A 0.006

50.0000 1 . 986E+00 1 .031E+00 3.017E+00 2.1A7E+01 1 .87AE-01 5.891E+00 -0.002 0.013 0.005

55.0000 1 .99AE+00 1 . 1 A5E+00 3.139E+00 2.310E+01 2.025E-01 6 .075E+00 -0.002 0.012 0.005

60.0000 2.001E+00 1 .260E+00 3.261 E+00 2. A66E+01 2.169E-01 6 .2AAE+00 -0.002 0.011 O.OOA

70.0000 2.01 AE+00 1 . A90E+00 3.50AE+00 2.762E+01 2. AAOE-01 6.5AAE+00 -0.001 0.010 0.003

80.0000 2.025E+00 1 . 723E+00 3.7A8E+00 3.038E+01 2.688E-01 6 .806E+00 -0.001 0.009 0.003

90.0000 2.035E+00 1 .957E+00 3.991E+00 3.296E+01 2.918E-01 7.038E+00 -0.001 0.009 0.002

100.0000 2.0A3E+00 2.191E+00 A.235E+00 3.539E+01 3.130E-01 7.2A5E+00 -0.001 0.008 0.002

125.0000 2.062E+00 2.782E+00 A.8AAE+00 A.091E+01 3.598E-01 7 .687E+00 -0.001 0.007 0.002

150.0000 2.076E+00 3.378E+00 5. A5AE+00 A.577E+01 3. 995E-01 8.0A9E+00 -0 .000 0.006 0.001 175.0000 2.089E+00 3 . 976E+00 6.065E+00 5.011E+01 A.336E-01 8.355E+00 -0.000 0.006 0.001 200.0000 2. 100E+00 A.577E+00 6.676E+00 5. AOAE+01 A.632E-01 8.621E+00 -0.000 0.005 0.001 250.0000 2. 1 18E+00 5.78AE+00 7 . 902E+00 6.092E+01 5.126E-01 9.065E+00 -0.000 0.005 0.001 300.0000 2.132E+00 6 . 997E+00 9.129E+00 6 .680E+01 5.522E-01 9.A29E+00 -0.000 O.OOA 0.001 350.0000 2.1A5E^^00 8.21 AE+00 1 .036E+01 7.1 9AE+01 5.8A8E-01 9.737E+00 -0.000 O.OOA 0.000

AOO . 0000 2.155E+00 9 . A3AE+00 1 . 159E+01 7.650E+01 6.121E-01 1 .OOOE+01 -0.000 O.OOA 0.000

A50 .0000 2. 165E+00 1 .066E+01 1 .282E+01 8.060E+01 6.356E-01 1 .02AE+01 -0.000 O.OOA 0.000

500.0000 2 . 1 73E + 00 1 . 188E+01 1 . A05E+01 8. A32E+01 6 .559E-01 1 .0A5E+01 -0.000 0.003 0.000 550.0000 2. 181E + 00 1 .31 lE+01 1 .529E+01 8.773E+01 6 .736E-01 1 .06AE+01 -0.000 0.003 0.000 600.0000 2. 188E+00 1 . A33E+01 1 .652E+01 9.088E+01 6.89AE-01 1 .081E+01 -0 .000 0.003 0.000 700.0000 2.200E+00 1 .679E+01 1 .899E+01 9.652E+01 7.161E-01 1 .112E+01 -0.000 0.003 0.000 800.0000 2.21 lE+00 1 . 926E+01 2.1A7E+01 1 .015E+02 7.379E-01 1 .139E+01 -0.000 0.003 0.000

900.0000 2.220E+00 2.172E+01 2.39AE+01 1 .059E+02 7.562E-01 1 .162E+01 -0.000 0.003 0.000 1000.0000 2.229E+00 2.A1 9E+01 2.6A1E+01 1 .099E+02 7.717E-01 1 . 183E+01 -0.000 0.003 0.000

138
ELECTRONS IN POLYMETHYL METHACRYLATE, "LUCITE". "PERSPEX". "PLEXIGLAS"

I = 76.0 eV DENSITY = 1 .190E+00 g/cm3

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. ddog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MoV cm^/g MeV cm^/g MeV cm^/g g/cm ^

0.0100 2.1 98E+01 3.332E-03 2.1 98E+01 2.580E-06 8. 329E-05 0.0 -0.198 0.227 0.225

0.0125 1 .868E+01 3.369E-03 1 .869E+01 3.826E-06 9.993E-05 0.0 -0.190 0.216 0.215

0.0150 1 .606E+01 3.359E-03 1 .606E+01 5.282E-06 1 .158E-06 0.0 -0.186 0.208 0.207

0.0175 1 .623E+01 3.366E-03 1 .623E + 01 6.960E-06 1 .31 lE-06 0.0 -0.179 0.201 0.201 0.0200 1 .283E+01 3.372E-03 1 .286E + 01 8.792E-06 1 .660E-06 0.0 -0.175 0.196 0.195

0.0250 1 .080E+01 3.382E-03 1 .081E + 01 1 .306E-03 1 .766E-06 0.0 -0.168 0.188 0.187

0.0300 9.600E+00 3.391E-03 9.606E+00 1 .803E-03 2.015E-06 0.0 -0.163 0.182 0.181 0.0350 8 . 367E+00 3.601 E-03 8.370E+00 2.368E-03 2.275E-06 0.0 -0.160 0.177 0.177

0 .OAOO 7.573E+00 3.61 3E-03 7.576E+00 2.997E-03 2.526E-06 0.0 -0.156 0.173 0.173

0 .0A50 6.962E+00 3.625E-03 6.966E+00 3.687E-03 2.770E-06 0.0 -0.156 0.170 0.169

0 .0500 6 .629E+00 3.638E-03 6.633E+00 6.636E-03 3.007E-06 0.0 -0.151 0.167 0.166

0.0550 6 .003E+00 3.653E-03 6.007E+00 5.261E-03 3.238E-06 0.0 -0.169 0.166 0.166

0.0600 5.666E+00 3.668E-03 5.667E+00 6.100E-03 3.666E-06 0.0 -0.167 0.162 0.162

0 .0700 5.070E+00 3.502E-03 5.073E+00 7.972E-03 3.901E-06 0.0 -0.166 0.158 0.158

0.0800 6.631E+00 3.538E-03 6.635E+00 1 .006E-02 6.322E-06 0.0 -0.162 0.155 0.155

0.0900 6.286E+00 3.577E-03 6.289E+00 1 .228E-02 6.729E-06 0.0 -0.160 0.152 0.152

0.1000 6.006E+00 3.61 9E-03 6.010E+00 1 .670E-02 5.125E-06 0.0 -0.138 0.150 0.150

0.1250 3.696E+00 3.732E-03 3.500E+00 2.160E-02 6.070E-06 0.0 -0.136 0.165 0.165

0.1500 3. 1 52E+00 3.855E-03 3. 155E+00 2.896E-02 6.966E-06 0.0 -0.131 0.162 0.162

0.1750 2.906E+00 3. 987E-03 2. 908E+00 3.721E-02 7.826E-06 0.0 -0.128 0.139 0.139

0.2000 2.719E+00 6. 126E-03 2.723E+00 6.610E-02 8.650E-06 0.0 -0.126 0.137 0.136

0.2500 2.661E+00 6.625E-03 2.665E+00 6.567E-02 1 .023E-03 0.0 -0.123 0.133 0.132

0.3000 2.292E+00 6.751E-03 2.297E+00 8.653E-02 1 .175E-03 0.0 -0.120 0.130 0.129

0.3500 2. 175E+00 5.101E-03 2. 180E+00 1 .089E-01 1 .322E-03 0.0 -0.118 0.128 0.127

0 . AOOO 2.090E+00 5.676E-03 2.096E+00 1 .323E-01 1 .666E-03 0.0 -0.117 0.126 0.125

0.6500 2.026E+00 5.867E-03 2.032E+00 1 .566E-01 1 .609E-03 1 .666E-02 -0.092 0.122 0.120

0 . 5000 1 . 975E+00 6 .278E-03 1 .981E+00 1 .815E-01 1 .751E-03 6.112E-02 -0.086 0.118 0.115

0.5500 1 .935E+00 6 .707E-03 1 .962E+00 2.070E-01 1 .892E-03 6.992E-02 -0.081 0.113 0.110

0.6000 1 .903E+00 7. 169E-03 1 .910E + 00 2.330E-01 2.035E-03 1 .005E-01 -0.076 0.109 0.105

0.7000 1 .856E+00 8.076E-03 1 .866E+00 2.860E-01 2.320E-03 1 .650E-01 -0.068 0.102 0.097

0.8000 1 .825E+00 9.050E-03 1 .836E+00 3.601E-01 2.609E-03 2.321E-01 -0.062 0.096 0.090

0.9000 1 .803E+00 1 .007E-02 1 .813E+00 3.950E-01 2.902E-03 3.001E-01 -0.057 0.091 0.083

1 .0000 1 .788E+00 1 .113E-02 1 .799E+00 6.506E-01 3.199E-03 3.679E-01 -0.053 0.087 0.078

1 .2500 1 .767E+00 1 .393E-02 1 .781E+00 5.902E-01 3.959E-03 5.330E-01 -0.066 0.078 0.068

1 .5000 1 .760E+00 1 .693E-02 1 .776E+00 7.308E-01 6.766E-03 6.887E-01 -0.061 0.071 0.060

1 .7500 1 .759E+00 2.009E-02 1 .779E+00 8.715E-01 5.553E-03 8.339E-01 -0.038 0.066 0.055

2.0000 1 .762E+00 2.338E-02 1 .785E+00 1 .012E+00 6.383E-03 9.689E-01 -0.035 0.062 0.050

2.5000 1 .772E+00 3.031E-02 1 .802E+00 1 .291E+00 8.096E-03 1 .212E+00 -0.032 0.056 0.066

3.0000 1 .786E+00 3.761E-02 1 .822E+00 1 .567E+00 9.868E-03 1 .625E+00 -0.029 0.051 0.039

3.5000 1 .797E+00 6.521E-02 1 .862E+00 1 .839E+00 1 .168E-02 1 .613E+00 -0.028 0.068 0.036

6.0000 1 .809E+00 5.307E-02 1 .862E+00 2.109E+00 1 .356E-02 1 .783E+00 -0.027 0.065 0.036

6.5000 1 .821E+00 6.115E-02 1 .882E+00 2.376E+00 1 .562E-02 1 .936E+00 -0.025 0.063 0.032

5.0000 1 .832E+00 6.963E-02 1 .901E+00 2.661E+00 1 .733E-02 2.077E+00 -0.025 0.061 0.030

5.5000 1 .862E+00 7.788E-02 1 .920E+00 2.903E+00 1 .926E-02 2.207E+00 -0.026 0.039 0.029

6.0000 1 .851E+00 8.668E-02 1 .938E+00 3. 162E+00 2. 120E-02 2.327E+00 -0.023 0.038 0.028

7.0000 1 .868E+00 1 .061E-01 1 .972E+00 3.673E+00 2.513E-02 2.565E+00 -0.022 0.036 0.026

8.0000 1 .883E+00 1 .222E-01 2.005E+00 6. 176E+00 2.910E-02 2.739E+00 -0.020 0.036 0.025

9.0000 1 .896E+00 1 .607E-01 2.037E+00 6.671E+00 3.309E-02 2.916E+00 -0.019 0.032 0.023

10.0000 1 .908E+00 1 .596E-01 2.067E+00 5.158E+00 3.710E-02 3.073E+00 -0.018 0.031 0.022

12.5000 1 .932E+00 2.079E-01 2.160E+00 6.366E+00 6.712E-02 3.621E+00 -0.015 0.028 0.020

15.0000 1 .952E+00 2.577E-01 2.210E+00 7.696E+00 5.709E-02 3.716E+00 -0.013 0.025 0.017

17.5000 1 . 968E+00 3.086E-01 2.277E+00 8.610E+00 6.695E-02 3.976E+00 -0.011 0.026 0.016

20.0000 1 .982E+00 3.603E-01 2.362E+00 9.693E+00 7.667E-02 6.202E+00 -0.010 0.022 0.016

25.0000 2.006E+00 6.656E-01 2.670E+00 1 . 177E+01 9.561E-02 6.596E+00 -0.007 0.019 0.012

30.0000 2.022E+00 5.728E-01 2.595E+00 1 .375E+01 1 .138E-01 6.927E+00 -0.006 0.017 0.010

35.0000 2.036E+00 6.815E-01 2.718E+00 1 .563E+01 1 .31 3E-01 5.212E+00 -0.005 0.016 0.008

60.0000 2.069E+00 7.912E-01 2.860E+00 1 .763E+01 1 .680E-01 5.663E+00 -0.006 0.016 0.007

65.0000 2.059E+00 9.020E-01 2.961E+00 1 .915E+01 1 .639E-01 5.687E+00 -0.003 0.013 0.006

50.0000 2.069E+00 1 .01 3E+00 3.082E+00 2.081E+01 1 .792E-01 5.889E+00 -0.003 0.012 0.005

55.0000 2.077E+00 1 .126E+00 3.203E+00 2.260E+01 1 .939E-01 6.072E+00 -0.002 0.012 0.005

60.0000 2.085E+00 1 .238E+00 3.323E+00 2.393E+01 2.079E-01 6.261E+00 -0.002 0.011 0.006

70.0000 2.098E+00 1 .665E+00 3.563E+00 2.686E+01 2.362E-01 6.561E+00 -0.001 0.010 0.006

80.0000 2. 109E+00 1 .696E+00 3.806E+00 2. 955E+01 2.585E-01 6.803E+00 -0.001 0.009 0.003

90.0000 2. 120E+00 1 . 926E+00 6.066E+00 3.210E+01 2.810E-01 7.036E+00 -0.001 0.008 0.003

100.0000 2.128E+00 2.155E+00 6.286E+00 3.650E+01 3.01 9E-01 7.262E+00 -0.001 0.008 0.002

125.0000 2. 167E+00 2.737E+00 6.886E+00 3.996E+01 3.681E-01 7.683E+00 -0.001 0.007 0.002

150.0000 2. 163E+00 3.323E+00 5.686E+00 6.679E+01 3.876E-01 8.065E+00 -0.000 0.006 0.001 175.0000 2.176E+00 3.912E+00 6.087E+00 6.912E+01 6.213E-01 8.351E+00 -0.000 0.006 0.001 200.0000 2. 187E+00 6 .503E+00 6.690E+00 5.303E+01 6.509E-01 8.617E+00 -0.000 0.005 0.001 250.0000 2.205E+00 5.692E+00 7.897E+00 5.990E+01 5.006E-01 9.061E+00 -0.000 0.005 0.001 300.0000 2.220E+00 6 .887E+00 9.107E+00 6 .579E+01 5.602E-01 9.625E+00 -0.000 0.006 0.001 350.0000 2.233E+00 8 . 085E+00 1 .032E+01 7.095E+01 5.731E-01 9.733E+00 -0.000 0.006 0.000

600.0000 2.266E+00 9.286E+00 1 . 153E+01 7.553E+01 6 .008E-01 9. 999E+00 -0.000 0.006 0.000

650.0000 2.256E+00 1 .069E+01 1 .276E+01 7. 965E+01 6.266E-01 1 .023E+01 -0.000 0.003 0.000

500.0000 2.263E+00 1 . 1 70E+01 1 . 396E+01 8.360E+01 6.652E-01 1 .066E+01 -0.000 0.003 0.000

550.0000 2.271E+00 1 .290E+01 1 .518E+01 8.686E+01 6.633E-01 1 .066E+01 -0.000 0.003 0.000

600.0000 2.278E+00 1 .61 1E+01 1 .639E+01 9.000E+01 6.793E-01 1 .081E+01 -0.000 0.003 0.000

700.0000 2.291E+00 1 .653E+01 1 .882E+01 9.569E+01 7.066E-01 1 . 1 12E+01 -0.000 0.003 0.000

800.0000 2.302E+00 1 .896E+01 2. 126E+01 1 .007E+02 7.289E-01 1 .138E+01 -0.000 0.003 0.000

900.0000 2.312E+00 2. 1 39E+01 2.370E+01 1 .051E+02 7.676E-01 1 .162E+01 -0.000 0.003 0.000

1000.0000 2. 320E+00 2.382E+01 2.616E+01 1 .092E+02 7.636E-01 1 . 183E+01 -0.000 0.003 0.000

139
ELECTRONS IN POLYPROPYLENE

I = 59.2 eV DENSITY = 9.000E-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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.383E+01 2.883E-03 2.383E+01 2.366E-09 6.658E-05 0.0 -0.190 0.215 0.219

0.0125 2.000E+01 2.893E-03 2.000E+01 3.516E-09 7.985E-05 0.0 -0.182 0.206 0.205

0.0150 1 .733E+01 2. 900E-03 1 .739E + 01 9.863E-09 9.259E-05 0.0 -0.177 0.198 0.198

0.0175 1 .536E + 01 2. 905E-03 1 .536E+01 6.398E-09 1 .098E-09 0.0 -0.172 0.193 0.192

0.0200 1 .389E+01 2.910E-03 1 .389E+01 8.115E-09 1 . 167E-09 0.0 -0.168 0.188 0.187

0.0250 1 . 169E+01 2.919E-03 1 . 169E+01 1 .207E-03 1 .399E-09 0.0 -0.162 0.180 0.180

0.0300 1 .011E+01 2.929E-03 1 .012E+01 1 .669E-03 1 .612E-09 0.0 -0.158 0.175 0.179

0.0350 8. 995E+00 2. 939E-03 8.998E+00 2.195E-03 1 .822E-09 0.0 -0.159 0.170 0.170

0 . 0<i00 8.136E+00 2.951E-03 8.139E+00 2.780E-03 2.025E-09 0.0 -0.151 0.166 0.166

0 .0‘150 7.959E+00 2. 963E-03 7.957E+00 3.922E-03 2.223E-09 0.0 -0.199 0.163 0.163

0.0500 6 . 900E+00 2. 976E-03 6.903E+00 9. 120E-03 2.915E-09 0.0 -0.196 0.161 0.160

0.0550 6 .990E+00 2. 991 E-03 6.993E+00 9.870E-03 2.602E-09 0.0 -0.195 0.158 0.158

0 .0600 6 .052E + 00 3.006E-03 6 .055E+00 5.671 E-03 2.786E-09 0.0 -0.193 0.156 0.156

0.0700 5.933E+00 3.037E-03 5.936E+00 7.918E-03 3.192E-09 0.0 -0.190 0.153 0.152

0.0800 9 . 960E+00 3.071E-03 9.963E+00 9.397E-03 3.985E-09 0.0 -0.137 0.150 0.199

0.0900 9.588E+00 3. 107E-03 9.591E+00 1 . 199E-02 3.818E-09 0.0 -0.135 0.197 0.197

0.1000 9.287E+00 3. 195E-03 9.290E+00 1 .370E-02 9. 191E-09 0.0 -0.139 0.195 0.195

0.1250 3.738E+00 3 . 298E-03 3.791E+00 1 . 997E-02 9.915E-09 0.0 -0.130 0.191 0.190

0.1500 3 . 367E+00 3 . 360E-03 3.370E+00 2.703E-02 5.651E-09 0.0 -0.127 0.138 0.137

0.1750 3. lOlE+00 3.978E-03 3.105E+00 3.977E-02 6 . 357E-09 0.0 -0.125 0.135 0.139

0.2000 2 . 902E+00 3 . 603E-03 2. 905E+00 9.310E-02 7.038E-09 0.0 -0.123 0.133 0.132

0 .2500 2 . 62'(E + 00 3.872E-03 2.628E+00 6. 126E-02 8.395E-09 0.0 -0.119 0.129 0.128

0.3000 2 . 993E+00 9 . 1 65E-03 2.997E+00 8. 102E-02 9.601E-09 0.0 -0.117 0.126 0.126

0 . 3500 2.317E+00 9.978E-03 2.322E+00 1 .020E-01 1 .082E-03 0.0 -0.115 0.129 0.123

O.'tOOO 2.225E+00 9.812E-03 2.229E+00 1 .290E-01 1 .202E-03 1 .122E-02 -0.091 0.121 0.119

0.9500 2. 1 53E+00 5. 163E-03 2.159E+00 1 .968E-01 1 .322E-03 3. 973E-02 -0.085 0.116 0.113

0.5000 2.098E+00 5.531 E-03 2. 109E+00 1 .703E-01 1 .990E-03 7.098E-02 -0.079 0.111 0.108

0.5500 2.055E+00 5.919E-03 2.061E+00 1 .993E-01 1 .559E-03 1 .092E-01 -0.079 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 0.0 98 0.7000 1 . 969E + 00 7. 138E-03 1 .976E+00 2.688E-01 1 .919E-03 2.107E-01 -0.063 0.096 0.090

0.8000 1 . 939E + 00 8.009E-03 1 .992E+00 3.1 99E-01 2. 163E-03 2.891E-01 -0.057 0.090 0.083

0 . 9000 1 . 91 OE+00 8.91 9E-03 1 .919E+00 3.717E-01 2.909E-03 3.575E-01 -0.053 0.085 0.077

1 .0000 1 .893E+00 9.867E-03 1 .903E+00 9.290E-01 2.660E-03 9.300E-01 -0.099 0.081 0.072

1 .2500 1 .869E+00 1 .238E-02 1 .882E+00 5.563E-01 3.303E-03 6.095E-01 -0.093 0.072 0.063

1 .5000 1 .860E + 00 1 .506E-02 1 .876E+00 6.899E-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 9.656E-03 9.173E-01 -0.036 0.062 0.051 2.0000 1 .861 E+00 2.089E-02 1 .882E+00 9.557E-01 5.361E-03 1 .056E+00 -0.039 0.058 0.097

2.5000 1 .871E+00 2.706E-02 1 .898E+00 1 .220E+00 6.821E-03 1 .305E+00 -0.031 0.052 0.091

3 .0000 1 .883E+00 3.361E-02 1 .917E+00 1 .983E+00 8.332E-03 1 .521E+00 -0.029 0.098 0.037

3.5000 1 .896E+00 9.099E-02 1 .936E+00 1 .792E+00 9.886E-03 1 .71 3E+00 -0.027 0.095 0.035

9 .0000 1 . 908E+00 9.751E-02 1 .956E+00 1 .999E+00 1 . 197E-02 1 .885E+00 -0.026 0.092 0.032

9 . 5000 1 . 920E+00 5.977E-02 1 .975E+00 2.253E+00 1 .309E-02 2.090E+00 -0.025 0.090 0.031 5.0000 1 . 931 E+00 6 .222E-02 1 .993E+00 2.505E+00 1 .973E-02 2. 183E+00 -0.029 0.039 0.029

5.5000 1 .991E+00 6.989E-02 2.01 lE+00 2.755E+00 1 .639E-02 2.319E+00 -0.023 0.037 0.028

6 .0000 1 .951E+00 7.759E-02 2.028E+00 3.003E+00 1 .806E-02 2.936E+00 -0.022 0.036 0.027

7 .0000 1 . 968E+00 9.398E-02 2.062E+00 3.992E+00 2.195E-02 2.658E+00 -0.021 0.039 0.025

8.0000 1 . 983E+00 1 .098E-01 2.093E+00 3.973E+00 2.988E-02 2.855E+00 -0.019 0.032 0.029

9.0000 1 .997E+00 1 .265E-01 2. 123E+00 9.997E+00 2.839E-02 3.033E+00 -0.018 0.031 0.022

10.0000 2.008E+00 1 .935E-01 2.152E+00 9.915E+00 3.182E-02 3.1 96E+00 -0.017 0.029 0.021 12.5000 2.033E+00 1 .872E-01 2.221E+00 6.059E+00 9.056E-02 3.553E+00 -0.019 0.026 0.018

15.0000 2.053E+00 2.322E-01 2.285E+00 7.168E+00 9.930E-02 3.856E+00 -0.011 0.029 0.016

17.5000 2.069E+00 2.782E-01 2.397E+00 8.298E+00 5.798E-02 9.122E+00 -0.009 0.022 0.019

20.0000 2.083E+00 3.299E-01 2.908E+00 9.299E+00 6.658E-02 9.357E+00 -0.008 0.020 0.013

25.0000 2.105E+00 9.202E-01 2.525E+00 1 .133E+01 8.393E-02 9.762E+00 -0.005 0.018 0.010

30 . 0000 2. 1 23E+00 5. 173E-01 2.690E+00 1 .326E+01 9.975E-02 5. lOlE+00 -0.009 0.016 0.008

35.0000 2.1 37E+00 6.158E-01 2.753E+00 1 .512E+01 1 .155E-01 5.392E+00 -0.003 0.019 0.007

90.0000 2.199E+00 7.1 53E-01 2.865E+00 1 .690E+01 1 .307E-01 5.698E+00 -0.002 0.013 0.006

95.0000 2.160E+00 8. 157E-01 2.976E+00 1 .861E+01 1 .953E-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-01 6.079E+00 -0.002 0.011 0.009

55.0000 2. 178E+00 1 .01 9E+00 3.1 97E+00 2. 185E+01 1 .728E-01 6.265E+00 -0.001 0.010 0.009

60.0000 2. 186E+00 1 . 121E+00 3.307E+00 2.339E+01 1 .858E-01 6.935E+00 -0.001 0.010 0.003

70.0000 2.200E+00 1 .327E+00 3.527E+00 2.632E+01 2.109E-01 6.738E+00 -0.001 0.009 0.003

80.0000 2.21 1E+00 1 .535E+00 3.796E+00 2.907E+01 2.333E-01 7.001E+00 -0.001 0.008 0.002

90.0000 2.222E+00 1 .799E+00 3. 966E+00 3. 166E+01 2.596E-01 7.233E+00 -0.001 0.007 0.002

100.0000 2.231 E+00 1 . 959E+00 9.185E+00 3.912E+01 2.795E-01 7.992E+00 -0.000 0.007 0.002

125.0000 2. 250E+00 2.983E+00 9.733E+00 3.973E+01 3. 189E-01 7.889E+00 -0.000 0.006 0.001 150.0000 2.266E+00 3.01 5E+00 5.282E+00 9.973E+01 3.572E-01 8.297E+00 -0.000 0.005 0.001 175.0000 2.280E+00 3.551E+00 5.831E+00 9.923E+01 3.905E-01 8.553E+00 -0.000 0.005 0.001

200 .0000 2.291 E+00 9.089E+00 6.380E+00 5.333E+01 9.1 99E-01 8.819E+00 -0.000 0.009 0.001 250.0000 2.310E+00 5. 171E+00 7 .982E+00 6 .056E+01 9.699E-01 9.269E+00 -0.000 0.009 0.001 300.0000 2.326E+00 6 . 259E+00 8.585E+00 6 .679E+01 5.096E-01 9.628E+00 -0.000 0.009 0.000

350.0000 2.339E+00 7.350E+00 9.689E+00 7.227E+01 5.932E-01 9. 936E+00 -0.000 0.003 0.000

900.0000 2.351E+00 8.999E+00 1 .080E+01 7.716E+01 5.716E-01 1 .020E+01 -0.000 0.003 0.000

950 .0000 2.361E+00 9.591E+00 1 . 1 90E+01 8.1 57E+01 5.961E-01 1 .099E+01 -0.000 0.003 0.000

500.0000 2.370E+00 1 .069E+01 1 .301E+01 8.558E+01 6.175E-01 1 .065E+01 -0.000 0.003 0.000

550.0000 2.378E+00 1 .179E+01 1 .912E+01 8. 927E+01 6.369E-01 1 .089E+01 -0.000 0.003 0.000

600.0000 2.386E+00 1 .289E+01 1 .523E+01 9.268E+01 6.531E-01 1 .101E+01 -0.000 0.003 0.000

700.0000 2.399E+00 1 .505E+01 1 .795E+01 9.881E+01 6.817E-01 1 .132E+01 -0.000 0.002 0.000

800.0000 2.91 1E+00 1 .726E+01 1 .967E+01 1 .092E+02 7.053E-01 1 .159E+01 -0.000 0.002 0.000

900.0000 2.921E+00 1 . 997E+01 2. 189E+01 1 .090E+02 7.251E-01 1 . 182E+01 -0.000 0.002 0.000

1000.0000 2.930E+00 2.169E+01 2.912E+01 1 .139E+02 7.921E-01 1 .203E+01 -0.000 0.002 0.000

140
ELECTRONS IN POLYSTYRENE

I = 68.7 eV DENSITY = 1 . 060E+00 g/cra

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 cm*/g MeV cm^/g MeV cm^/g g/cm ^

0.0100 2.223E+01 2.982E-03 2.22<*E+01 2.5<16E-0<1 7.<106E-05 0.0 -0.195 0.223 0.221 0.0125 1 .868E+01 2.992E-03 1 .869E+01 3.777E-0<* 8.869E-05 0.0 -0.187 0.212 0.211 0.0150 1 .621E+01 2.999E-03 1 .621 E+01 5.218E-0<1 1 .027E-0<1 0.0 -0.181 0.205 0.204

0.0175 1 .<*37E+01 3.00<tE-03 1 .<138E + 01 6.859E-0<1 1 .162E-0<1 0.0 -0.176 0.198 0.198

0.0200 1 .296E+01 3.008E-03 1 .296E+01 8.69<1E-0<* 1 .292E-0<1 0.0 -0.172 0.193 0.193

0.0250 1 .091E+01 3.017E-03 1 .091 E+01 1 .292E-03 1 .5<13E-0<i 0.0 -0.166 0.185 0.185

0.0300 9.<i85E+00 3.027E-03 9.<*88E + 00 1 .785E-03 1 .782E-04 0.0 -0.162 0.179 0.179

0.0350 8.<*<*0E+00 3.037E-03 8.<1<*3E+00 2.3<*5E-03 2.013E-0<* 0.0 -0.158 0.175 0.174

0 .0«(00 7.637E+00 3.0<*8E-03 7.6<*0E+00 2.968E-03 2.235E-0<1 0.0 -0.155 0.171 0.170

0.0<*50 7.000E+00 3.061E-03 7.003E+00 3.653E-03 2.<*52E-0<* 0.0 -0.152 0.167 0.167

0.0500 6.<*81E+00 3.07<*E-03 6.<18<tE + 00 <1.395E-03 2.662E-0<i 0.0 -0.150 0.165 0.164

0.0550 6.051E+00 3.088E-03 6.05<1E+00 5.1 9<1E-03 2.867E-0<1 0.0 -0.148 0.162 0.162

0.0600 5.688E+00 3.103E-03 5.691E+00 6.0<*7E-03 3.068E-0<* 0.0 -0.146 0.160 0.160

0.0700 5. 108E+00 3. 135E-03 5.111 E+00 7.905E-03 3.<*58E-0<1 0.0 -0.143 0.156 0.156

0.0800 <* .666E+00 3. 169E-03 <*.669E + 00 9.955E-03 3.83<*E-0<* 0.0 -0.140 0.153 0.153

0.0900 <*.317E+00 3.206E-03 <1.320E+00 1 .218E-02 <1.1 97E-0<* 0.0 -0.138 0.151 0.150

0.1000 <*.03^E+00 3.2<*<*E-03 <*.038E+00 1 .<*58E-02 <1.550E-0<* 0.0 -0.136 0.148 0.148

0.1250 3.520E+00 3.350E-03 3.523E+00 2. 12<*E-02 5.396E-0<i 0.0 -0.132 0.144 0.144

0.1500 3. 172E+00 3.<*63E-03 3. 176E+00 2.873E-02 6.199E-0<* 0.0 -0.129 0.140 0.140

0.1750 2.923E+00 3.58<*E-03 2.926E+00 3.695E-02 6.967E-0<1 0.0 -0.127 0.138 0.137

0.2000 2.735E+00 3.71 IE-03 2.739E+00 <*.579E-02 7.709E-0<1 0.0 -0.125 0.135 0.135

0.2500 2.<*75E+00 3.985E-03 2.<179E+00 6.50<1E-02 9.131E-0<* 0.0 -0.122 0.132 0.131 0.3000 2.305E+00 <*.28<tE-03 2.309E+00 8.598E-02 1 .050E-03 0.0 -0.119 0.129 0.128

0.3500 2. 187E+00 <*.60<*E-03 2.192E+00 1 .082E-01 1 . 182E-03 0.0 -0.117 0.127 0.125

O.'iOOO 2.101E+00 <*.9<*5E-03 2.106E+00 1 .315E-01 1 .312E-03 2.729E-03 -0.102 0.124 0.123

0 .<*500 2.035E+00 5.30<*E-03 2.0<*0E+00 1 .557E-01 1 .<1<11E-03 2.688E-02 -0.090 0.119 0.117

0.5000 1 .98<tE+00 5.680E-03 1 .990E + 00 1 .805E-01 1 .570E-03 5.<120E-02 -0.084 0.115 0.112

0.5500 1 .9<i3E+00 6.071E-03 1 .950E+00 2.059E-01 1 .699E-03 8.383E-02 -0.079 0.111 0.107

0.6000 1 .911E+00 6.<*75E-03 1 .918E+00 2.318E-01 1 .827E-03 1 .152E-01 -0.074 0.107 0.102

0.7000 1 .86<*E+00 7.322E-03 1 .871E+00 2.8<16E-01 2.087E-03 1 .810E-01 -0.067 0.100 0.094

0.8000 1 .832E+00 8.212E-03 1 .8<10E+00 3.385E-01 2.3<19E-03 2.<*92E-01 -0.061 0.094 0.088

0.9000 1 .810E+00 9. 1<i2E-03 1 .81 9E+00 3.932E-01 2.615E-03 3.179E-01 -0.057 0.089 0.082

1 .0000 1 .79<*E+00 1 .01 IE-02 1 .80<1E+00 <*.<18<*E-01 2.885E-03 3.862E-01 -0.053 0.085 0.077

1 .2500 1 .773E+00 1 .267E-02 1 .786E+00 5.878E-01 3.577E-03 5.515E-01 -0.046 0.077 0.067

1 .5000 1 .766E+00 1 .5<*1E-02 1 .781E+00 7.281E-01 <1.293E-03 7.06<1E-01 -0.042 0.070 0.060

1 .7500 1 .765E+00 1 .830E-02 1 .783E+00 8.68<*E-01 5.030E-03 8.501E-01 -0.039 0.065 0.055

2.0000 1 .768E+00 2.132E-02 1 .789E+00 1 .008E+00 5.788E-03 9.834E-01 -0.037 0.062 0.050

2.5000 1 .778E+00 2.766E-02 1 .806E+00 1 .287E+00 7.352E-03 1 .222E+00 -0.034 0.056 0.045

3.0000 1 .791E + 00 3.<*35E-02 1 .825E+00 1 .562E+00 8.970E-03 1 .431E+00 -0.031 0.051 0.041 3.5000 1 .80<*E+00 <1.1 32E-02 1 .8<15E+00 1 .835E+00 1 .063E-02 1 .616E+00 -0.030 0.048 0.038

•i.OOOO 1 .816E+00 <1.852E-02 1 .865E+00 2.10<*E+00 1 .233E-02 1 .782E+00 -0.029 0.046 0.035

<*.5000 1 .828E+00 5.593E-02 1 .88<iE+00 2.371E+00 1 .<*05E-02 1 .932E+00 -0.027 0.044 0.034

5.0000 1 .839E+00 6.353E-02 1 .902E+00 2.635E+00 1 .580E-02 2.070E+00 -0.026 0.042 0.032

5.5000 1 .SIOE+OO 7. 129E-02 1 . 920E+00 2.897E+00 1 .757E-02 2.197E+00 -0.025 0.040 0.031 6.0000 1 .859E+00 7.919E-02 1 .938E+00 3. 156E+00 1 .936E-02 2.316E+00 -0.025 0.039 0.030

7.0000 1 .876E+00 9.539E-02 1 .971E+00 3.667E+00 2.297E-02 2.531E+00 -0.023 0.037 0.028

8.0000 1 .891E+00 1 . 120E-01 2.003E+00 <*. 171E+00 2.662E-02 2.722E+00 -0.021 0.035 0.026

9.0000 1 . 90<1E+00 1 .290E-01 2.033E+00 <1.666E+00 3.029E-02 2.896E+00 -0.020 0.033 0.025

10.0000 1 .916E+00 1 .<16<*E-01 2.062E+00 5. 155E+00 3.399E-02 3.05<*E+00 -0.019 0.032 0.023

12.5000 1 . 9<*0E+O0 1 . 909E-01 2.131E+00 6.3<17E+00 <1.325E-02 3.<103E+00 -0.015 0.029 0.020

15.0000 1 .960E+00 2.367E-01 2.196E+00 7.502E+00 5.2<*9E-02 3.702E+00 -0.013 0.026 0.018

17.5000 1 .975E+00 2.835E-01 2.259E+00 8.625E+00 6.166E-02 3.963E+00 -0.010 0.024 0.016

20.0000 1 .989E+00 3.31 lE-01 2.320E+00 9.717E+00 7.072E-02 4.1 96E+00 -0.009 0.022 0.014

25.0000 2.01 OE+00 <1.282E-01 2.<139E+00 1 . 182E+01 8.8<1<1E-02 4.596E+00 -0.006 0.019 0.011 30.0000 2.027E+00 5.270E-01 2.55<*E+00 1 .382E+01 1 .056E-01 4.933E+00 -0.005 0.017 0.009

35.0000 2.0<*1E+00 6.271E-01 2.669E+00 1 .57<1E+01 1 .220E-01 5.223E+00 -0.003 0.016 0.008

<i0.0000 2.053E+00 7.28<1E-01 2.782E+00 1 .757E+01 1 .378E-01 5.478E+00 -0.003 0.014 0.006

<*5.0000 2.06<1E+00 8.306E-01 2.89AE+00 1 .933E+01 1 .530E-01 5.704E+00 -0.002 0.013 0.005

50.0000 2.073E+00 9.33<*E-01 3.006E+00 2.103E+01 1 .676E-01 5.908E+00 -0.002 0.012 0.005

55.0000 2.081E+00 1 .037E+00 3. 1 18E+00 2.266E+01 1 .816E-01 6.093E+00 -0.002 0.011 0.004

60.0000 2.089E+00 1 .l<tlE+00 3.230E+00 2.<12<*E+01 1 .951E-01 6.263E+00 -0.001 0.01 1 0.004

70.0000 2. 1 02E+00 1 .351E+00 3.<*52E+00 2.723E+01 2.20<*E-01 6.565E+00 -0.001 0.010 0.003

80.0000 2.113E+00 1 .562E + 00 3.675E+00 3.00<*E+01 2.<139E-01 6.828E+00 -0.001 0.009 0.002

90.0000 2. 123E+00 1 .77<1E+00 3.897E+00 3.268E+01 2.658E-01 7.060E+00 -0.001 0.008 0.002

100.0000 2.132E+00 1 . 988E+00 <1. 120E+00 3.518E+01 2.861E-01 7.269E+00 -0.001 0.008 0.002

125.0000 2. 151E+00 2.525E+00 <i.676E+00 <*.087E+01 3.31<1E-01 7.71 lE+00 -0.000 0.006 0.001 150.0000 2. 166E+00 3.067E+00 5.233E+00 <*.592E+01 3.701E-01 8.073E+00 -0.000 0.006 0.001 175.0000 2.179E+00 3.61 lE+00 5.790E+00 5.0<*6E+01 <1.037E-01 8.380E+00 -0.000 0.005 0.001 200.0000 2. 1 90E + 00 <1. 158E+00 6.3<18E+00 5.<158E+01 <1.333E-01 8.646E+00 -0.000 0.005 0.001 250.0000 2.208E+00 5.258E+00 7 .<166E+00 6.18<1E+01 <1.828E-01 9.091E+00 -0.000 0.004 0.001 300.0000 2.223E+00 6 . 362E+00 8.586E+00 6.808E+01 5.229E-01 9.454E+00 -0.000 0.004 0.000

350.0000 2.236E+00 7.<171E+00 9.707E+00 7.355E+01 5.562E-01 9.762E+00 -0.000 0.004 0.000

<100 .0000 2.2<*7E+00 8.583E+00 1 .083E+01 7 .8<*2E+01 5.8<*3E-01 1 .003E+01 -0.000 0.003 0.000

<*50.0000 2.257E+00 9.697E+00 1 . 1 95E+01 8.282E+01 6.085E-01 1 .026E+01 -0.000 0.003 0.000

500.0000 2.256E+00 1 .081 E+01 1 . 308E+01 8. 681 E+01 6 .296E-01 1 .047E+01 -0.000 0.003 0.000

550.0000 2.27<*E+00 1 . 1 93E + 01 1 .<120E+01 9.0<18E+01 6.<182E-01 1 .066E+01 -0.000 0.003 0.000 600.0000 2.281 E+00 1 . 305E+01 1 .533E+01 9.387E+01 6.646E-01 1 .084E+01 -0.000 0.003 0.000

700.0000 2.293E+00 1 .529E+01 1 .758E+01 9.996E+01 6. 926E-01 1 . 1 15E+01 -0.000 0.003 0.000

800.0000 2. 30<*E+00 1 .75<1E+01 1 .98<1E+01 1 .053E+02 7.157E-01 1 . 141E+01 -0.000 0.003 0.000

900.0000 2.31<*E+00 1 .978E+01 2.210E+01 1 .101E+02 7.350E-01 1 . 165E+01 -0.000 0.002 0.000

1000.0000 2.323E+00 2.203E+01 2.<*36E+01 1 .l<1<*E+02 7.515E-01 1 .186E+01 -0.000 0.002 0.000

141
ELECTRONS IN POLYTETRAFLUOROETHYLENE. "TEFLON

I = 99.1 eV DENSITY = 2.200E+001 g/cm

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. ddog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV KeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .8A3E+01 A.21 lE-03 1 .8A3E+01 3.105E-0A 1 .2A9E-0A 0.0 -0.210 0 .2A3 0 .2A1 0.0125 1 .553E+01 A.2A7E-03 1 .55AE+01 A.589E-0A 1 .502E-OA 0.0 -0.201 0.231 0.229

0.0150 1 .351E+01 A.271E-03 1 .351 E+01 6.320E-0A 1 .7A3E-0A 0.0 -0.19A 0.222 0.220

0.0175 1 .200E+01 A.287E-03 1 .201 E + 01 8.287E-0A 1 .975E-0A 0.0 -0.189 0.215 0.213

0.0200 1 . 08AE+01 A . 300E-03 1 .08AE+01 1 .0A8E-03 2.1 99E-0A 0.0 -0 . 18A 0.209 0.207

0.0250 9.1A1E+00 A.316E-03 9.1A6E+00 1 .553E-03 2.629E-0A 0.0 -0.177 0.199 0.198

0.0300 7.965E+00 A.329E-03 7.970E+00 2.1A0E-03 3.037E-0A 0.0 -0.172 0.192 0.192

0.0350 7.098E+00 A.3A1E-03 7. 102E+00 2.806E-03 3. A28E-0A 0.0 -0.167 0.187 0.186

0.0^00 6 . A30E+00 A.353E-03 6 . A35E+00 3.5A7E-03 3.805E-0A 0.0 -0 . 16A 0.182 0.182

0 . 0^50 5 . 900E+00 A . 366E-03 5. 90AE+00 A.359E-03 A.169E-0A 0.0 -0.161 0.179 0.178

0.0500 5 .A68E+00 A.380E-03 5. A72E+00 5.239E-03 A.522E-0A 0.0 -0.158 0.175 0.175

0.0550 5. 109E+00 A.395E-03 5.11 3E+00 6.185E-03 A.865E-0A 0.0 -0.156 0.173 0.172

0.0600 A.806E+00 A.AlOE-03 A.810E+00 7.19AE-03 5.200E-OA 0.0 -0.1 5A 0.170 0.170

0 .0700 A . 321 E+00 A.AAAE-03 A.325E+00 9.391E-03 5.8A7E-0A 0.0 -0.151 0.166 0.166

0 .0800 3 . 951 E+00 A . A83E-03 3. 955E+00 1 .181E-02 6 .A67E-0A 0.0 -0.1 A8 0.163 0.162

0.0900 3.658E+00 A.525E-03 3.663E+00 1 . AAAE-02 7.065E-0A 0.0 -0 . 1 A5 0.160 0.159

0.1000 3.A21E+00 A.571E-03 3.A26E+00 1 .727E-02 7.6A3E-0A 0.0 -0.1A3 0.157 0.157

0.1250 2 . 989E+00 A.700E-03 2.99AE+00 2.51 lE-02 9.021E-0A 0.0 -0.139 0.152 0.152

0 . 1 500 2.697E+00 A.8AAE-03 2.702E+00 3.392E-02 1 .032E-03 0.0 -0.136 0.1 A8 0.1 A8 0.1750 2. A87E+00 5.000E-03 2.A92E+00 A.357E-02 1 . 156E-03 0.0 -0.133 0.1A5 0.1A5

0.2000 2.330E+00 5. 167E-03 2.335E+00 5.395E-02 1 .275E-03 0.0 -0.131 0.1A3 0. 1 A2 0.2500 2.11 1E+00 5.530E-03 2. 1 17E+00 7.651E-02 1 .503E-03 0.0 -0.127 0.138 0.138

0.3000 1 . 968E+00 5. 928E-03 1 .97AE+00 1 .OlOE-01 1 .721E-03 0.0 -0.12A 0.135 0.13A

0.3500 1 .869E+00 6 .353E-03 1 .875E+00 1 .271E-01 1 .931E-03 0.0 -0.122 0.133 0.132

0 . AOOO 1 .797E+00 6 .805E-03 1 .80AE+00 1 .5A5E-01 2.1 37E-03 2.29AE-03 -0.108 0.130 0.129

0. A500 1 .7A2E+00 7.279E-03 1 .7A9E+00 1 .82AE-01 2.3A1E-03 2.338E-02 -0.097 0.126 0.123

0.5000 1 .699E+00 7.775E-03 1 .707E+00 2.1 lAE-01 2.5A3E-03 A.753E-02 -0.091 0.121 0.118

0.5500 1 .665E+00 8.291 E-03 1 .67AE+00 2.A10E-01 2.7AAE-03 7.398E-02 -0.085 0.117 0.113

0.6000 1 .639E+00 8.823E-03 1 .6A7E+00 2.71 lE-01 2.9A5E-03 1 .022E-01 -0.081 0.113 0.109

0.7000 1 .600E+00 9.937E-03 1 .610E+00 3.326E-01 3.3A7E-03 1 .623E-01 -0.073 0.106 0.101 0.8000 1 .573E+00 1 .lllE-02 1 .585E+00 3.952E-01 3.753E-03 2.253E-01 -0.067 0.101 0.09A

0.9000 1 .555E+00 1 .233E-02 1 .568E+00 A.587E-01 A.162E-03 2.896E-01 -0.062 0.095 0.088

1 .0000 1 .5A3E+00 1 .360E-02 1 .557E+00 5.227E-01 A.575E-03 3.5A1E-01 -0.058 0.091 0.083

1 .2500 1 .527E+00 1 .697E-02 1 .5AAE+00 6.8A1E-01 5.631E-03 5. 127E-01 -0.050 0.082 0.072

1 . 5000 1 .522E+00 2.057E-02 1 .5A2E+00 8. A62E-01 6.719E-03 6 .637E-01 -0.0A5 0.075 0.065

1 .7500 1 -522E+00 2. A37E-02 1 .5A6E+00 1 .008E+00 7.837E-03 8.056E-01 -0.0A1 0.070 0.059

2.0000 1 .525E+00 2.83AE-02 1 .553E+00 1 . 169E+00 8. 983E-03 9.382E-01 -0.038 0.066 0.05A

2.5000 1 .535E+00 3.667E-02 1 .572E+00 1 .A90E+00 1 .13AE-02 1 . 178E+00 -0.03A 0.059 0.0A7

3.0000 1 .5A6E+00 A.5AAE-02 1 .592E+00 1 .806E+00 1 .377E-02 1 .390E+00 -0.031 0.05A 0.0A2

3.5000 1 .558E+00 5. A56E-02 1 .612E+00 2. 1 18E+00 1 .626E-02 1 .578E+00 -0.029 0.051 0.039

A .0000 1 .569E+00 6.399E-02 1 .633E+00 2. A26E+00 1 .879E-02 1 .7A8E+00 -0.028 0.0A8 0.036

^.5000 1 .579E+00 7.367E-02 1 .653E+00 2.730E+00 2.1 36E-02 1 .902E+00 -0.027 0.0A5 0.03A

5.0000 1 .589E+00 8.357E-02 1 .672E+00 3.031E+00 2.395E-02 2.0A3E+00 -0.026 0.0A3 0.032

5.5000 1 .598E+00 9.367E-02 1 .692E+00 3.328E+00 2.656E-02 2.173E+00 -0.025 0.0A2 0.031

6 .0000 1 .606E+00 1 .OAOE-01 1 .710E+00 3.622E+00 2.919E-02 2.29AE+00 -0.02A O.OAO 0.029

7.0000 1 .621E+00 1 .250E-01 1 .7A6E+00 A.201E+00 3. AA7E-02 2.512E+00 -0.023 0.038 0.027

8.0000 1 .635E+00 1 -A66E-01 1 .781E+00 A.768E+00 3. 978E-02 2.706E+00 -0.021 0.036 0.026

9 .0000 1 .6A6E+00 1 .686E-01 1 .815E+00 5.32AE+00 A.509E-02 2.880E+00 -0.020 0.03A 0.02A

10.0000 1 .657E+00 1 .910E-01 1 .8A8E+00 5.870E+00 5.0A0E-02 3.039E+00 -0.019 0.032 0.023

12.5000 1 .679E+00 2. A83E-01 1 .927E+00 7.19AE+00 6.355E-02 3.385E+00 -0.017 0.029 0.020

15.0000 1 .697E+00 3.071E-01 2.00AE+00 8.A66E+00 7.6A8E-02 3.677E+00 -0.015 0.027 0.018

17.5000 1 .712E+00 3.672E-01 2.079E+00 9.691E+00 8.913E-02 3.930E+00 -0.013 0.025 0.017

20.0000 1 .72AE+00 A.281E-01 2.152E+00 1 .087E+01 1 .015E-01 A.155E+00 -0.012 0.023 0.015

25.0000 1 .7A5E+00 5.521E-01 2.297E+00 1 .312E+01 1 .252E-01 A.5A1E+00 -0.009 0.021 0.013

30.0000 1 .761E+00 6.781E-01 2. A39E+00 1 .523E+01 1 .A76E-01 A.866E+00 -0.008 0.019 0.011 35.0000 1 .77AE+00 8.056E-01 2.579E+00 1 .723E+01 1 .687E-01 5. 1 A6E+00 -0.006 0.017 0.009

AO. 0000 1 .785E+00 9.3AAE-01 2.71 9E+00 1 .911E+01 1 .886E-01 5.39AE+00 -0.005 0.016 0.008

A5.0000 1 .795E+00 1 .06AE+00 2.859E+00 2.091E+01 2.075E-01 5.61 AE+00 -O.OOA 0.015 0.007

50.0000 1 .803E+00 1 . 1 95E+00 2.998E+00 2.262E+01 2.253E-01 5.81 AE+00 -O.OOA O.OIA 0.006

55.0000 1 .81 1E+00 1 .326E+00 3.137E+00 2.A25E+01 2.A21E-01 5.996E+00 -0.003 0.013 0.006

60.0000 1 .818E+00 1 . A58E+00 3.276E+00 2.580E+01 2.581E-01 6.163E+00 -0.003 0.012 0.005

70.0000 1 .830E+00 1 .72AE+00 3.55AE+00 2.87AE+01 2.878E-01 6.A61E+00 -0.002 0.011 O.OOA

80.0000 1 .8AOE+00 1 .991E+00 3.831E+00 3.1AAE+01 3.1A7E-01 5.721E+00 -0.002 0.010 O.OOA

90.0000 1 .8A9E+00 2.260E+00 A.109E+00 3.396E+01 3.392E-01 6.952E+00 -0.001 0.010 0.003

100.0000 1 .857E+00 2.530E+00 A.387E+00 3.632E+01 3.616E-01 7. 159E+00 -0.001 0.009 0.003

125.0000 1 .87AE+00 3.209E+00 5.083E+00 A. 161E+01 A. lOAE-01 7.599E+00 -0.001 0.008 0.002

150.0000 1 .887E+00 3.893E+00 5.780E+00 A.622E+01 A.508E-01 7.960E+00 -0.001 0.007 0.002

175.0000 1 .899E+00 A.580E+00 6.A79E+00 5.030E+01 A.851E-01 8.266E+00 -0.000 0.007 0.001 200.0000 1 .909E+00 5.269E+00 7.178E+00 5.396E+01 5. 1 A6E-01 8.531E+00 -0.000 0.006 0.001 250.0000 1 .926E+00 6.655E+00 8.580E+00 6.033E+01 5.629E-01 8. 976E+00 -0.000 0.006 0.001 300.0000 1 .939E+00 8.0A5E+00 9.98AE+00 6 .572E+01 6.010E-01 9.339E+00 -0.000 0.005 0.001 350.0000 1 -950E+00 9.AAOE+00 1 . 139E+01 7.0A1E+01 6.319E-01 9.6A6E+00 -0.000 0.005 0.001 AOO.OOOO 1 .960E+00 1 .08AE+01 1 .280E+01 7.A55E+01 6.577E-01 9.913E+00 -0.000 0.005 0.001

A50 .0000 1 .969E+00 1 .22AE+01 1 .A21E+01 7.825E+01 6.796E-01 1 .015E+01 -0.000 O.OOA 0.000

500.0000 1 . 977E+00 1 .36AE+01 1 .562E+01 8.161E+01 6 . 98AE-01 1 .036E+01 -0.000 O.OOA 0.000

550.0000 1 .98AE+00 1 .50AE+01 1 .703E+01 8. A68E+01 7.1A8E-01 1 .055E+01 -0.000 O.OOA 0.000

600.0000 1 . 990E+00 1 .6A5E+01 1 .8AAE+01 8.750E+01 7.292E-01 1 .072E+01 -0.000 O.OOA 0.000

700.0000 2.002E+00 1 .926E+01 2. 126E+01 9.25AE+01 7.535E-01 1 . 103E+01 -0.000 O.OOA 0.000

800.0000 2.012E+00 2.208E+01 2.A09E+01 9.696E+01 7.732E-01 1 . 1 30E+01 -0.000 0.003 0.000

900.0000 2.020E+00 2. A90E+01 2.692E+01 1 .009E+02 7.896E-01 1 .153E+01 -0.000 0.003 0.000

1000.0000 2.028E+00 2.772E+01 2.975E+01 1 .OAAE+02 8.035E-01 1 . 17AE+01 -0.000 0.003 0.000

142
ELECTRONS IN POLYVINYL CHLORIDE

I = 108.2 eV DENSITY = 1 .300E+001 g/cm®

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 cm*/g MeV cm^/g MeV cm*/g g/cm * 0.0100 1 .930E+01 5. 953E-03 1 .930E+01 2.97<1E-0<i 1 .617E-0<1 0.0 -0.21<1 0.2<19 0.245

0.0125 1 .628E+01 6.106E-03 1 .629E+01 <1.390E-0<1 1 .977E-0<i 0.0 -0.205 0.236 0.232

0.0150 1 .<il6E+01 6.218E-03 1 .<117E+01 6.0HE-0<1 2.326E-0<1 0.0 -0.198 0.227 0.223

0.0175 1 .259E+01 6.302E-03 1 .260E+01 7.916E-0<1 2.665E-0<1 0.0 -0.192 0.219 0.216

0.0200 1 . 1 37E+01 6.369E-03 1 . 1 38E+01 1 .001E-03 2.995E-0<i 0.0 -0.187 0.213 0.210

0.0250 9.601E+00 6.<168E-03 9.608E+00 1 .<181E-03 3.630E-0A 0.0 -0.180 0.203 0.201 0.0300 8.370E+00 6.539E-03 8.377E+00 2.0<10E-03 <1.237E-0<1 0.0 -0.17<1 0.196 0.194

0.0350 7.<162E+00 6.595E-03 7. A68E+00 2.673E-03 <1.821E-0<1 0.0 -0.170 0.190 0.189

0.0<*00 6.762E+00 6.6<11E-03 6.769E+00 3.378E-03 5.38<1E-0<1 0.0 -0.166 0.186 0.184

0 .O'iSO 6.206E+00 6.681E-03 6.213E+00 <1. 150E-03 5.928E-0<1 0.0 -0.163 0.182 0.180

0.0500 5.753E+00 6.717E-03 5.759E+00 <1.987E-03 6.<157E-0<1 0.0 -0.161 0.178 0.177

0.0550 5.376E+00 6.751E-03 5.383E+00 5.885E-03 6.970E-0<1 0.0 -0.158 0.175 0.174

0.0600 5.05SE+00 6.783E-03 5.065E+00 6.8<1<1E-03 7.<170E-0<i 0.0 -0.156 0.173 0.172

0.0700 9.599E+00 6 .8A6E-03 <1.556E+00 8. 930E-03 8.<13<1E-0<1 0.0 -0.153 0.168 0.168

0.0800 <1.160E+00 6 . 908E-03 <1. 167E+00 1 .123E-02 9.356E-0<1 0.0 -0.150 0.165 0.164

0.0900 3.853E+00 6.972E-03 3.860E+00 1 .372E-02 1 .02<1E-03 0.0 -0.1<17 0.162 0.161 0.1000 3.601E+00 7.0A0E-03 3.611 E+00 1 .6<11E-02 1 .1 10E-03 0.0 -0.1 <15 0.159 0.159

0.1250 3.150E+00 7 .222E-03 3.157E+00 2.38<1E-02 1 .312E-03 0.0 -0.1<11 0.1 5<* 0.153

0.1500 2.8<13E+00 7.<12<1E-03 2.851E+00 3.21 9E-02 1 .501E-03 0.0 -0.138 0.150 0.149

0 . 1750 2.623E+00 7 .6<12E-03 2.630E+00 <1.13<1E-02 1 .680E-03 0.0 -0.135 0.1<17 0.146

0.2000 2.<157E+00 7 .877E-03 2.<165E + 00 5.117E-02 1 .852E-03 0.0 -0.132 0.1<i<* 0.144

0.2500 2.227E+00 8.387E-03 2.235E+00 7.25<1E-02 2.176E-03 0.0 -0.129 0.1<t0 0.139

0 . 3000 2.077E+00 8.9<19E-03 2.086E+00 9.575E-02 2.A8<1E-03 0.0 -0.126 0.137 0.136

0.3500 1 . 972E+00 9.55<1E-03 1 .982E+00 1 .20<1E-01 2.780E-03 0.0 -0.123 0.13<» 0.133

0.^000 1 .896E+00 1 .020E-02 1 .907E+00 1 .<161E-01 3.068E-03 7.976E-03 -0.102 0.131 0.129

0.^500 1 .838E+00 1 .088E-02 1 .8<19E+00 1 .728E-01 3.351E-03 3.082E-02 -0.097 0.126 0.124

0.5000 1 .793E+00 1 .159E-02 1 .805E+00 2.001E-01 3.631E-03 5.539E-02 -0.092 0.122 0.119

0 .5500 1 .758E+00 1 .233E-02 1 .770E+00 2.281E-01 3.910E-03 8. 121E-02 -0.088 0.118 0.114

0.6000 1 .730E+00 1 -310E-02 1 .7<13E+00 2.566E-01 <1. 187E-03 1 .079E-01 -0.08<1 0.11<1 0.110

0.7000 1 .690E+00 1 .<169E-02 1 .70AE+00 3. 1<17E-01 <1.741E-03 1 .629E-01 -0.078 0.108 0.103

0.8000 1 .663E+00 1 .637E-02 1 .679E+00 3.738E-01 5.296E-03 2. 189E-01 -0.073 0.103 0.097

0 . 9000 1 .6<»5E+00 1 .81 3E-02 1 .663E+00 <1.337E-01 5.855E-03 2.7<17E-01 -0.069 0.098 0.092

1 .0000 1 .633E+00 1 . 995E-02 1 .653E+00 <1. 9<10E-01 6.<118E-03 3.299E-01 -0.066 0.094 0.087

1 .2500 1 .618E+00 2.<176E-02 1 .6<13E+00 6.<158E-01 7.8<16E-03 <1.627E-01 -0.060 0.087 0.078

1 .5000 1 .615E+00 2. 990E-02 1 .6<15E+00 7.980E-01 9.308E-03 5.867E-01 -0.056 0.081 0.072

1 .7500 1 .618E+00 3.530E-02 1 .653E+00 9.<196E-01 1 .080E-02 7.018E-01 -0.053 0.077 0.067

2.0000 1 .623E+00 <1.092E-02 1 .66<1E+00 1 .100E+00 1 .232E-02 8.087E-01 -0.051 0.073 0.063

2.5000 1 .638E+00 5.270E-02 1 .690E+00 1 .399E+00 1 .5<13E-02 1 .001E+00 -0.0<17 0.068 0.057

3.0000 1 .653E+00 6.507E-02 1 .718E+00 1 .692E+00 1 .861E-02 1 .170E+00 -0.0<1<1 0.064 0.053

3.5000 1 .669E+00 7.791E-02 1 .7<17E+00 1 .981 E+00 2.18<1E-02 1 .321E+00 -0.0<12 0.060 0.050

<1.0000 1 .683E+00 9.11<1E-02 1 .77<1E+00 2.265E+00 2.51 IE-02 1 .<158E+00 -0.0<10 0.058 0.048

<1.5000 1 .696E+00 1 .0<17E-01 1 .801E+00 2.5<1<1E+00 2.8<11E-02 1 .583E+00 -0.039 0.055 0.045

5.0000 1 .708E+00 1 . 186E-01 1 .827E+00 2.820E+00 3.172E-02 1 .699E+00 -0.037 0.054 0.044

5.5000 1 .720E+00 1 -327E-01 1 .853E+00 3.092E+00 3.50<1E-02 1 .807E+00 -0.036 0.052 0.042

6.0000 1 .730E+00 1 .<171E-01 1 .877E+00 3.360E+00 3.837E-02 1 .908E+00 -0.03<1 0.050 0.040

7.0000 1 .7<19E+00 1 .76<1E-01 1 .925E+00 3.886E+00 <1.503E-02 2.095E+00 -0.031 0.048 0.037

8.0000 1 .765E+00 2.065E-01 1 .971E+00 <1.399E+00 5. 168E-02 2.26<1E+00 -0.029 0.045 0.035

9.0000 1 .779E+00 2.371E-01 2.016E+00 <1.901E+00 5.830E-02 2.<120E+00 -0.027 0.043 0.033

10.0000 1 .791E + 00 2.683E-01 2.060E+00 5.391E+00 6.<186E-02 2.56<1E+00 -0.02<1 0.041 0.031 12.5000 1 .81 7E+00 3.<179E-01 2. 165E+00 6 .575E+00 8.101E-02 2.888E+00 -0.020 0.037 0.026

15.0000 1 .837E+00 <1.295E-01 2.266E+00 7.70<1E+00 9.672E-02 3.168E+00 -0.017 0.034 0.023

17.5000 1 .853E+00 5.127E-01 2.366E+00 8.783E+00 1 .119E-01 3.415E+00 -0.01<1 0.031 0.020

20.0000 1 .866E+00 5.971E-01 2. A6<1E+00 9.819E+00 1 .267E-01 3.636E+00 -0.012 0.029 0.018

25.0000 1 .889E+00 7.686E-01 2.657E+00 1 . 177E+01 1 .5<16E-01 <i.017E+00 -0.010 0.026 0.015

30.0000 1 . 906E+00 9.A28E-01 2.8<19E+00 1 .359E+01 1 .806E-01 <1.337E+00 -0.009 0.023 0.012

35.0000 1 .921E+00 1.11 9E+00 3.0<10E+00 1 .529E+01 2.0<18E-01 <1.613E+00 -0.007 0.021 0.011

<10.0000 1 . 933E+00 1 .297E + 00 3.230E+00 1 .688E+01 2.273E-01 <1.85<1E+00 -0.007 0.019 0.009

<15.0000 1 . 9<1<1E+00 1 .<176E+00 3.<120E+00 1 .839E+01 2.<18<1E-01 5.069E+00 -0.006 0.018 0.008

50.0000 1 .953E+00 1 .657E + 00 3.610E+00 1 .981E+01 2.681E-01 5.263E+00 -0.006 0.017 0.007

55.0000 1 .962E+00 1 .838E+00 3.800E+00 2.116E+01 2.866E-01 5.<1<10E+00 -0.005 0.016 0.007

60.0000 1 . 969E+00 2.020E+00 3.990E+00 2.2<1<1E+01 3.0<10E-01 5.602E+00 -0.005 0.015 0.006

70.0000 1 .983E+00 2.387E+00 <1.370E+00 2.<18<1E+01 3.358E-01 5.890E+00 -0.005 0.014 0.005

80.0000 1 .995E+00 2.756E+00 <1.750E+00 2.703E+01 3.6<13E-01 6.1<12E+00 -0.00<1 0.013 0.005

90.0000 2.005E+00 3. 127E+00 5.132E+00 2.906E+01 3.899E-01 6.365E+00 -0.00<1 0.012 0.004

100.0000 2.01<1E+00 3.<199E+00 5.51 3E+00 3.09AE+01 <1.1 32E-01 6 .566E+00 -0.003 0.012 0.004

125.0000 2.033E+00 <i.<136E + 00 6.<169E+00 3.512E+01 <1.628E-01 6.995E+00 -0.003 0.010 0.003

150.0000 2.0<18E+00 5.379E+00 7.<127E+00 3.872E+01 5.033E-01 7.3<18E+00 -0.002 0.010 0.002

175.0000 2.061E+00 6 . 326E+00 8.386E+00 <1. 189E+01 5.371E-01 7.6<19E+00 -0.002 0.009 0.002

200.0000 2.072E+00 7 .276E + 00 9.3<17E+00 <1.<171E+01 5.658E-01 7.910E+00 -0.001 0.008 0.002

250 .0000 2.090E+00 9. 185E+00 1 . 127E+01 <1. 958E+01 6 . 122E-01 8.3A9E+00 -0.001 0.008 0.001 300.0000 2. 10<1E+00 1 . 1 lOE+01 1 .321E+01 5.367E+01 6.<182E-01 8.710E+00 -0.001 0.007 0.001 350.0000 2. 1 17E+00 1 .302E+01 1 .51<1E+01 5.720E+01 6.771E-01 9.015E+00 -0.001 0.007 0.001

<100.0000 2. 127E+00 1 . A95E+01 1 .708E+01 6.031E+01 7.010E-01 9.281E+00 -0.000 0.006 0.001

<150.0000 2.137E+00 1 .688E+01 1 .901E+01 6.308E+01 7.21 IE-01 9.515E+00 -0.000 0.006 0.001 500.0000 2. 1 <15E + 00 1 .881 E + 01 2.095E+01 6.559E+01 7.383E-01 9.725E+00 -0.000 0.006 0.001

550 .0000 2. 153E+00 2.07<1E+01 2.289E+01 6.787E+01 7.531E-01 9.915E+00 -0.000 0.006 0.001 600.0000 2.1 59E+00 2.268E+01 2.<18<1E+01 6 . 997E+01 7.662E-01 1 .009E+01 -0.000 0.005 0.001 700.0000 2. 172E+00 2.655E+01 2.872E+01 7.371E+01 7.880E-01 1 .0<10E+01 -0.000 0.005 0.000

800.0000 2. 182E+00 3. 0<13E+01 3.261 E+01 7.697E+01 8.056E-01 1 .066E+01 -0.000 0.005 0.000

900.0000 2.191E+00 3.<131E+01 3.650E+01 7.987E+01 8.202E-01 1 .090E+01 -0.000 0.005 0.000

1000.0000 2.200E+00 3.820E+01 <1.0<10E+01 8.2<17E+01 8.32<1E-01 1 .111E+01 -0.000 0.005 0.000

143
ELECTRONS IN PROPANE

I = A7.1 eV DENSITY = 1 .879E-03 g/cm^ (20<> C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFP. d( log1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.618E+01 2.752E-03 2.618E+01 2.1 A2E-0A 5.755E-05 0.0 -0.182 0.205 0.20A

0.0125 2.1 9AE+01 2.762E-03 2.1 9AE+01 3. 189E-0A 6.916E-05 0.0 -0.175 0.196 0.195

0.0150 1 .899E+01 2.769E-03 1 .899E+01 A. A18E-0A 8.028E-05 0.0 -0.170 0.189 0.189

0.0175 1 .681E+01 2.77AE-03 1 .681E+01 5.820E-0A 9. 102E-05 0.0 -0.165 0.18A 0.18A

0.0200 1 .513E+01 2.779E-03 1 .51 AE+01 7.390E-0A 1 .01 AE-OA 0.0 -0.162 0.180 0.179

0.0250 1 .271E+01 2.789E-03 1 .271E+01 1 .101E-03 1 .215E-0A 0.0 -0.156 0.173 0.173

0.0300 1 .103E+01 2.799E-03 1 .lOAE+01 1 .525E-03 1 . A07E-0A 0.0 -0.152 0.168 0.167

0.0350 9.806E+00 2.810E-03 9.808E+00 2.006E-03 1 .592E-0A 0.0 -0.1A9 0. 16A 0.163

0 .OAOO 8.863E+00 2.821E-03 8.866E+00 2.5A3E-03 1 .771E-0A 0.0 -0 . 1 A6 0.160 0.160

0.0A50 8.1 16E+00 2.83AE-03 8.11 9E+00 3.1 33E-03 1 . 9A5E-0A 0.0 -0 . 1 AA 0.157 0.157

0.0500 7.509E+00 2.8A7E-03 7.511E+00 3.77AE-03 2. 1 1 AE-OA 0.0 -0.1A2 0.155 0.155

0.0550 7.005E+00 2.861E-03 7.008E+00 A.A6AE-03 2.280E-0A 0.0 -0.1A0 0.153 0.152

0.0600 6 .580E+00 2.876E-03 6.583E+00 5.201E-03 2. AA2E-0A 0.0 -0.138 0.151 0.150

0 .0700 5.903E+00 2.907E-03 5. 906E+00 6 .808E-03 2.757E-0A 0.0 -0.136 0.1A7 0.1A7

0.0800 5. 387E+00 2.9A0E-03 5.390E+00 8.583E-03 3.061E-0A 0.0 -0.133 0.1A5 O.IAA

0.0900 A. 980E+00 2.975E-03 A. 983E+00 1 .051E-02 3.356E-0A 0.0 -0.131 0.1A2 0.1 A2 0.1000 A.652E+00 3.01 3E-03 A.655E+00 1 .259E-02 3.6A3E-0A 0.0 -0.130 0.1A0 0.1 AO 0.1250 A.052E+00 3. 1 1 AE-03 A.056E+00 1 .837E-02 A.330E-0A 0.0 -0.126 0.136 0.136

0.1500 3.6A8E+00 3.222E-03 3.652E+00 2.A88E-02 A.98AE-0A 0.0 -0.123 0.133 0.133

0.1750 3.358E+00 3.338E-03 3.362E+00 3.203E-02 5.612E-0A 0.0 -0.121 0.131 0.130 0.2000 3.1A1E+00 3. A60E-03 3. 1 AAE+00 3.973E-02 6.21 9E-0A 0.0 -0.119 0.129 0.128

0.2500 2.839E+00 3.722E-03 2.8A2E+00 5.651E-02 7.386E-0A 0.0 -0.116 0.125 0.125

0.3000 2.6A1 E+00 A.007E-03 2.6A5E+00 7. A79E-02 8.509E-0A 0.0 -0.11 A 0.123 0.122

0.3500 2.50AE+00 A.31 lE-03 2.508E+00 9. A23E-02 9.603E-0A 0.0 -0.112 0.121 0.120

0 . AOOO 2. AOAE+00 A.635E-03 2.A09E+00 1 . 1 A6E-01 1 .068E-03 0.0 -0.110 0.119 0.118

0.A500 2.330E+00 A. 976E-03 2.335E+00 1 .357E-01 1 . 17AE-03 0.0 -0.108 0.117 0.116

0.5000 2.27AE+00 5.33AE-03 2.279E+00 1 .57AE-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-01 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 . A92E-03 0.0 -0.105 0.1 1A 0.112

0.7000 2. 1 A7E+00 6.89AE-03 2. 15AE+00 2. A80E-01 1 .705E-03 0.0 -0.103 0.112 0.110

0.8000 2. 1 16E+00 7.739E-03 2.12AE+00 2.9A8E-01 1 . 920E-03 0.0 -0.101 0.110 0.108

0.9000 2.096E+00 8.623E-03 2.105E+00 3.A21E-01 2. 137E-03 0.0 -0.100 0.109 0.106

1.0000 2.08AE+00 9.5AAE-03 2.09AE+00 3.898E-01 2.356E-03 0.0 -0.098 0.107 0.105

1 .2500 2.073E+00 1 . 1 98E-02 2.085E+00 5.095E-01 2. 91 AE-03 0.0 -0.095 0.105 0.102

1 .5000 2.078E+00 1 .A59E-02 2.092E+00 6.293E-01 3. A88E-03 0.0 -0.093 0.103 0.099

1 .7500 2.088E+00 1 .73AE-02 2.106E+00 7.A8AE-01 A.075E-03 0.0 -0.091 0.101 0.097

2.0000 2.103E+00 2.021E-02 2.123E+00 8.666E-01 A.675E-03 0.0 -0.090 0.099 0.096

2.5000 2.1 3AE+00 2.626E-02 2.160E+00 1 .100E+00 5. 907E-03 0.0 -0.087 0.097 0.093

3.0000 2.166E+00 3.263E-02 2.199E+00 1 .330E+00 7.171E-03 0.0 -0.086 0.095 0.090

3.5000 2.1 96E+00 3. 928E-02 2.235E+00 1 .555E+00 8.A62E-03 0.0 -0.08A 0.093 0.088

A .0000 2.22AE+00 A.616E-02 2.270E+00 1 .777E+00 9.772E-03 0.0 -0.083 0.092 0.087

A .5000 2.250E+00 5.323E-02 2.30AE+00 1 .996E+00 1 . 1 10E-02 0.0 -0.081 0.091 0.085

5.0000 2.27AE+00 6 .0A9E-02 2.335E+00 2.21 1E+00 1 .2AAE-02 0.0 -0.080 0.089 0.08A

5.5000 2.297E+00 6 .790E-02 2.365E+00 2. A2AE+00 1 .379E-02 0.0 -0.080 0.088 0.083

6.0000 2 . 318E+00 7.5A6E-02 2.393E+00 2.63AE+00 1 .515E-02 0.0 -0.079 0.087 0.082

7.0000 2.356E+00 9.09AE-02 2. AA7E+00 3.0A7E+00 1 .790E-02 0.0 -0.077 0.086 0.080 8.0000 2.389E+00 1 .068E-01 2.A96E+00 3. A52E+00 2.066E-02 0.0 -0.076 0.08A 0.079

9.0000 2.A1 9E+00 1 .231E-01 2.5A2E+00 3.8A9E+00 2.3A3E-02 0.0 -0.075 0.083 0.077

10.0000 2 . AA6E+00 1 .397E-01 2.586E+00 A.239E+00 2.621E-02 0.0 -0 .07A 0.082 0.076 12.5000 2.505E+00 1 .823E-01 2.687E+00 5. 187E+00 3.316E-02 0.0 -0.073 0.080 0.073

15.0000 2.551E+00 2.262E-01 2.777E+00 6 . 1 02E+00 A.007E-02 1 .733E-02 -0.061 0.077 0.070

17.5000 2.586E+00 2.710E-01 2.857E+00 6.9S9E+00 A.695E-02 8.510E-02 -0.0A9 0.07A 0.065

20.0000 2.61 3E+00 3.167E-01 2.930E+00 7.853E+00 5.376E-02 1 .770E-01 -O.OAl 0.070 0.059

25.0000 2.655E+00 A.097E-01 3.06AE+00 9.521E+00 6.721E-02 3.825E-01 -0.032 0.063 0.0A9

30.0000 2.685E+00 5.0A5E-01 3.1 90E+00 1 . 1 12E+01 8.035E-02 5.859E-01 -0.027 0.058 O.OA2

35.0000 2.710E+00 6.007E-01 3.310E+00 1 .266E+01 9.31 AE-02 7.756E-01 -0.02A 0.053 0.036

AO .0000 2.730E+00 6 . 979E-01 3.A28E+00 1 .A1 AE+01 1 .056E-01 9.500E-01 -0.022 0.050 0.032

A5.0000 2.7A7E+00 7.960E-01 3.5A3E+00 1 .558E+01 1 . 176E-01 1 .1 10E+00 -0.020 0.0A7 0.029

50.0000 2.763E+00 8.9A8E-01 3.657E+00 1 .697E+01 1 .29AE-01 1 .257E+00 -0.019 O.OAA 0.026 55.0000 2.776E+00 9.9AAE-01 3.770E+00 1 .831E+01 1 . A07E-01 1 .393E+00 -0.018 0.0A2 0.02A

60.0000 2.788E+00 1 .09AE+00 3.883E+00 1 . 962E+01 1 .517E-01 1 .51 9E+00 -0.017 O.OAO 0.023

70.0000 2.809E+00 1 .296E+00 A.105E+00 2.212E+01 1 .728E-01 1 .7A6E+00 -0.016 0.037 0.020

80.0000 2.828E+00 1 . A99E+00 A.326E+00 2. A50E+01 1 . 926E-01 1 .9A6E+00 -0.015 0.03A 0.018

90.0000 2.8A3E+00 1 .703E+00 A.5A6E+00 2.675E+01 2.11 3E-01 2.125E+00 -0.015 0.032 0.016

100.0000 2.857E+00 1 .909E+00 A.766E+00 2.890E+01 2.289E-01 2.287E+00 -0.01 A 0.030 0.015

125.0000 2 .886E+00 2. A26E+00 5.312E+00 3.386E+01 2.690E-01 2.637E+00 -0.013 0.027 0.013

150.0000 2 . 909E+00 2. 9A7E+00 5.856E+00 3.835E+01 3.0A3E-01 2.928E+00 -0.012 0.025 0.011 175.0000 2.928E+00 3.A71E+00 6.399E+00 A.2A3E+01 3.356E-01 3.180E+00 -0.011 0.023 0.010

200.0000 2.9AAE+00 3.998E+00 6.9A2E+00 A.618E+01 3.636E-01 3. A02E+00 -0.010 0.021 0.009

250.0000 2. 970E+00 5.056E+00 8.027E+00 5.287E+01 A.117E-01 3.783E+00 -0.008 0.019 0.007

300.0000 2.991E+00 6.121E+00 9.1 1 lE+00 5.871E+01 A.517E-01 A.103E+00 -0.007 0.017 0.006

350.0000 3.008E+00 7 . 189E+00 1 .020E+01 6.390E+01 A.856E-01 A.381E+00 -0.005 0.016 0.005 AOO.OOOO 3.022E+00 8.260E+00 1 .128E+01 6.856E+01 5. 1 A8E-01 A.626E+00 -0.005 0.015 0.005

A50 .0000 3.03AE+00 9.33AE+00 1 .237E+01 7.279E+01 5. A02E-01 A.8A5E+00 -0 .OOA 0.01A O.OOA 500.0000 3.0AAE+00 1 .OAlE+01 1 .3A5E+01 7.666E+01 5.626E-01 5.0AAE+00 -0.003 0.01 A O.OOA 550.0000 3.05AE+00 1 .1 A9E+01 1 . A5AE+01 8.02AE+01 5.826E-01 5.225E+00 -0.003 0.013 0.003

600.0000 3.062E+00 1 .257E+01 1 .563E+01 8.355E+01 6 .005E-01 5.392E+00 -0.002 0.013 0.003

700.0000 3.077E+00 1 .A73E+01 1 .781E+01 8.95AE+01 6.313E-01 5.689E+00 -0.002 0.012 0.003

800.0000 3.090E+00 1 .689E+01 1 .998E+01 9. A8AE+01 6.569E-01 5.9A9E+00 -0.001 0.011 0.002

900.0000 3. 101E+00 1 . 906E+01 2.216E+01 9.959E+01 6.787E-01 6.180E+00 -0.001 0.011 0.002

1000.0000 3.111E+00 2.123E+01 2. A3AE+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 o/cm^

ENERGY STOPPING COLLISION RADIATIVE

MeV MeV cm*/g MeV cm^/g

0.0100 1 .780E+01 5.66AE-03

0.0125 1 .506E+01 5.762E-03

0.0150 1 .313E+01 5.830E-03

0.0175 1 . 169E+01 5.880E-03

0.0200 1 .057E+01 5. 918E-03

0.0250 8.939E+00 5.971E-03

0.0300 7.80AE+00 6.009E-03

0.0350 6.965E+00 6.039E-03

O.OAOO 6.318E+00 6.065E-03

0 .0A50 5.803E+00 6 .089E-03

0.0500 5.383E+00 6. 1 12E-03

0.0550 5.033E+00 6.135E-03

0.0600 A.738E+00 6.159E-03

0.0700 A.265E+00 6.207E-03

0.0800 3. 90AE+00 6.259E-03

0.0900 3.618E+00 6.315E-03

0.1000 3.386E+00 6.375E-03

0.1250 2. 963E+00 6.5A1E-03

0.1500 2.677E+00 6.727E-03

0.1750 2.A71E+00 6.930E-03

0.2000 2.316E+00 7. 1A8E-03

0.2500 2.101E+00 7.622E-03

0.3000 1 .961E+00 8. 1 AAE-03

0.3500 1 .86AE+00 8.706E-03

0. AOOO 1 .792E+00 9.30AE-03

0.A500 1 .738E+00 9.935E-03

0.5000 1 .697E+00 1 -060E-02

0.5500 1 .665E+00 1 .128E-02

0.6000 1 .639E+00 1 . 1 99E-02

0.7000 1 .603E+00 1 .3A8E-02

0.8000 1 .579E+00 1 .50AE-02

0.9000 1 .563E+00 1 .667E-02

1 .0000 1 .552E+00 1 .836E-02

1 .2500 1 .5A0E+00 2.283E-02

1 .5000 1 .538E+00 2.761E-02

1 .7500 1 .5A2E+00 3.26AE-02

2.0000 1 .5A8E+00 3.787E-02

2.5000 1 .563E+00 A.886E-02

3.0000 1 .578E+00 6.039E-02

3.5000 1 .593E+00 7.238E-02

A. 0000 1 .606E+00 8.A75E-02

A. 5000 1 .61 9E+00 9.7A3E-02

5.0000 1 .630E+00 1 . 10AE-01 5.5000 1 .6A1E+00 1 .236E-01 6.0000 1 .650E+00 1 .371E-01 7.0000 1 .667E+00 1 .6A6E-01 8.0000 1 .682E+00 1 .927E-01 9.0000 1 .695E+00 2.21 AE-01 10.0000 1 .706E+00 2.507E-01

12.5000 1 .730E+00 3.25AE-01

15.0000 1 .7A9E+00 A.021E-01

17.5000 1 .765E+00 A.803E-01

20.0000 1 .779E+00 5.596E-01

25.0000 1 .801E+00 7.209E-01

30.0000 1 .818E+00 8.8A7E-01

35.0000 1 .833E+00 1 .050E+00

AO. 0000 1 .8A5E+00 1 .218E+00

A5.0000 1 .855E+00 1 .386E+00

50.0000 1 .865E+00 1 .556E+00

55.0000 1 .873E+00 1 .727E+00

60.0000 1 .880E+00 1 .898E+00 70.0000 1 .89AE+00 2.2A3E+00

80.0000 1 .905E+00 2.590E+00

90.0000 1 .915E+00 2.938E+00

100.0000 1 .923E+00 3.288E+00

125.0000 1 .9A1E+00 A. 169E+00

150.0000 1 .956E+00 5.055E+00

175.0000 1 .968E+00 5. 9A5E+00

200.0000 1 .978E+00 6.839E+00

250.0000 1 . 996E+00 8.633E+00

300.0000 2.010E+00 1 .OA3E+01 350.0000 2.022E+00 1 .22AE+01 AOO.OOOO 2.032E+00 1 . A05E+01

A50 .0000 2.0A1E+00 1 .586E+01 500.0000 2.0A9E+00 1 .768E+01 550.0000 2.057E+00 1 . 950E + 01 600.0000 2.063E+00 2.131E+01

700.0000 2.075E+00 2. A96E + 01 800.0000 2.086E+00 2.860E+01

900.0000 2.095E+00 3.225E+01

1000.0000 2. 103E+00 3.590E+01

CSDA RADIATION

TOTAL RANGE YIELD

MeV cm^/g g/cm^

1.781E+01 3.255E-0A 1.716E-0A

1.506E+01 A.788E-0A 2.07AE-0A

1.313E+01 6.570E-0A 2.A17E-0A

1.169E+01 8.592E-0A 2.7A9E-0A

1.057E+01 1.08AE-03 3.069E-0A

8.9A5E+00 1.60IE-03 3.68AE-0A

7.810E+00 2.201E-03 A.268E-0A

6.971E+00 2.880E-03 A.827E-0A

6.32AE+00 3.63AE-03 5.365E-0A

5.809E+00 A.A60E-03 5.88AE-0A

5.389E+00 5.355E-03 6.387E-0A

5.0A0E+00 6.315E-03 6.876E-0A

A.7AAE+00 7.338E-03 7.351E-0A

A.271E+00 9.56AE-03 8.267E-04

3.910E+00 1.201E-02 9.1A3E-04

3.62AE+00 1.A67E-02 9.985E-0A

3.393E+00 1.753E-02 1.080E-03

2.969E+00 2.5AAE-02 1.272E-03

2.683E+00 3.A32E-02 1.A53E-03

2.

A78E+00 A.A03E-02 1.62AE-03

2.323E+00 5.AA6E-02 1.789E-03

2.109E+00 7.713E-02 2.100E-03

1.969E+00 1.017E-01 2.396E-03

1.872E+00 1.278E-01 2.682E-03

1.801E+00 1.550E-01 2.960E-03

1.7A8E+00 1.832E-01 3.233E-03

1.708E+00 2.122E-01 3.504E-03

1.676E+00 2.A17E-01 3.77AE-03

1.651E+00 2.718E-01 A.042E-03

1.616E+00 3.331E-01 A.579E-03

1.59AE+00 3.95AE-01 5.118E-03

1.579E+00 A.585E-01 5.659E-03

1.570E+00 5.220E-01 6.206E-03

1.563E+00 6.817E-01 7.593E-03

1.566E+00 8.A16E-01 9.013E-03

1.575E+00 l.OOlE+00 1.0A6E-02

1.586E+00 1.159E+00 1.19AE-02

1.612E+00 1.A72E+00 1.A97E-02

1.639E+00 1.780E+00 1.807E-02

1.665E+00 2.082E+00 2.123E-02

1.691E+00 2.380E+00 2.AA2E-02

1.716E+00 2.67AE+00 2.765E-02

1.7A1E+00 2.963E+00 3.089E-02

1.76AE+00 3.2A8E+00 3.A15E-02

1.787E+00 3.530E+00 3.7A2E-02

1.832E+00 A.082E+00 4.397E-02

1.875E+00 A.622E+00 5.052E-02

1.916E+00 5.150E+00 5.70AE-02

1.957E+00 5.666E+00 6.352E-02

2.056E+00 6.912E+00 7.9A8E-02

2.152E+00 8.101E+00 9.502E-02

2.2A6E+00 9.238E+00 1.101E-01

2.338E+00 1.033E+01 1.2A7E-01

2.522E+00 1.239E+01 1.523E-01

2.703E+00 1.A30E+01 1.781E-01

2.883E+00 1.609E+01 2.021E-01

3.063E+00 1.778E+01 2.2A5E-01

3.2A2E+00 1.936E+01 2.A55E-01

3.

A21E+00 2.086E+01 2.651E-01

3.600E+00 2.229E+01 2.835E-01

3.778E+00 2.36AE+01 3.008E-01

A.136E+00 2.617E+01 3.325E-01

A.A9AE+00 2.8A9E+01 3.609E-01

A.853E+00 3.063E+01 3.865E-01

5.212E+00 3.262E+01 A.097E-01

6.110E+00 3.705E+01 4.593E-01

7.011E+00 A.086E+01 A.999E-01

7.9I3E+00 A.A22E+01 5.337E-01

8.817E+00 A.721E+01 5.625E-01

1.063E+01 5.237E+01 6.090E-01

1.2AAE+01 5.671E+01 6.A52E-01

1.A26E+01 6.0A6E+01 6.7A2E-01

1.608E+01 6.376E+01 6.982E-01

1.790E+01 6.670E+01 7.18AE-01

1.973E+01 6.936E+01 7.357E-01

2.155E+01 7.179E+01 7.507E-01

2.338E+01 7.A01E+01 7.638E-01

2.703E+01 7.799E+01 7.858E-01

3.069E+01 8.1A6E+01 8.036E-01

3.A3AE+01 8.A5AE+01 8.182E-01

3.800E+01 8.730E+01 8.306E-01

DEMS.EFF. dUog )/d(logI)

CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

0.0 -0.227 0.267 0.263

0.0 -0.216 0.252 0.2A8

0.0 -0.208 0.2A1 0.238

0.0 -0.202 0.232 0.230

0.0 -0.196 0.225 0.223

0.0 -0.188 0.215 0.213

0.0 -0.182 0.207 0.205

0.0 -0.177 0.200 0.199

0.0 -0.17A 0.195 0.1 9A 0.0 -0.170 0.191 0.190

0.0 -0.167 0.187 0.186

0.0 -0.165 0.18A 0.183

0.0 -0.163 0.181 0.180

0.0 -0.159 0.176 0.175

0.0 -0.156 0.172 0.172

0.0 -0.153 0.169 0.168

0.0 -0.151 0.166 0.165

0.0 -0.1 A6 0.160 0.160

0.0 -0.1A2 0.156 0.156

0.0 -0.1A0 0.153 0.152

0.0 -0.137 0.150 0.1A9

0.0 -0.133 0.1A5 0.1AA

0.0 -0.130 0.1A2 0.1A1

0.0 -0.125 0.139 0.138

1 .3AAE-02 -0.110 0.135 0.133

3. 175E-02 -0.10A 0.130 0.128

5.190E-02 -0.100 0.126 0.123

7.3A3E-02 -0.096 0.123 0.119

9.597E-02 -0.092 0.119 0.116

1 .A31E-01 -0.086 0.11A 0.109

1.91 9E-01 -0.081 0.109 0.103

2.A13E-01 -0.076 0.10A 0.0 98 2.907E-01 -0.073 0.101 0.09A

A. 1 18E-01 -0.066 0.093 0.085

5.276E-01 -0.061 0.087 0.078

6.371E-01 -0.057 0.083 0.073

7.A05E-01 -0.05A 0.079 0.068

9.306E-01 -0.0A9 0.072 0.061

1 .102E+00 -0 .0A5 0.068 0.056

1 .258E+00 -0.0A1 0.06A 0.052

1 .A02E+00 -0.038 0.061 0.0A9

1 .535E+00 -0.036 0.058 0.0A6

1 .659E+00 -0.03A 0.055 0.0A3

1 .776E+00 -0.032 0.053 0.0A1

1 .885E+00 -0.030 0.051 0.039

2.087E+00 -0.028 0.0A8 0.036

2.269E+00 -0.025 0.0A5 0.033

2.A35E+00 -0.02A 0.0A3 0.030

2.587E+00 -0.022 0.0A1 0.028

2.921E+00 -0.019 0.036 0.025

3.205E+00 -0.017 0.033 0.022

3.A52E+00 -0.015 0.031 0.019

3.671E+00 -0.01 A 0.029 0.017

A.0A7E+00 -0.012 0.025 0.015

A.362E+00 -0.010 0.023 0.013

A.635E+00 -0.009 0.021 0.011 A.87AE+00 -0.008 0.020 0.010

5.089E+00 -0.007 0.018 0.009

5.282E+00 -0.006 0.017 0.008

5. A59E+00 -0.005 0.016 0.007

5.621E+00 -0.005 0.016 0.007

5.91 1E+00 -O.OOA 0.01 A 0.006

6.165E+00 -0.003 0.013 0.005

6.391E+00 -0.003 0.012 O.OOA 6.59AE+00 -0.003 0.012 O.OOA 7.027E+00 -0.002 0.010 0.003

7.38AE+00 -0.001 0.010 0.002

7.687E+00 -0.001 0.009 0.002

7.951E+00 -0.001 0.008 0.002

8.393E+00 -0.001 0.008 0.001 8.755E+00 -0.000 0.007 0.001 9.062E+00 -0.000 0.007 0.001 9.328E+00 -0.000 0.006 0.001 9.563E+00 -0.000 0.006 0.001 9.773E+00 -0.000 0.006 0.001 9.963E+00 -0.000 0.006 0.001

1 .01 AE+01 -0.000 0.005 0.001

1 .OAAE+01 -0.000 0.005 0.000

1 .071E+01 -0.000 0.005 0.000

1 .095E+01 -0.000 0.005 0.000

1 . 1 16E+01 -0.000 0.005 0.000

145
ELECTRONS IN SODIUM IODIDE

I = 452.0 eV DENSITY = 3.667E+001 g/cm^

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. cUlog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

CDELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^

0.0100 1 . 1 16E+01 1 .518E-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 .632E-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 .01 3E-03 0.0 -0.275 0.355 0.330

0.0175 7.622E+00 1 .798E-02 7.640E+00 1 .390E-03 1 .181E-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 lE-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 4.71 1E+00 2. 120E-02 4.733E+00 4.410E-03 2.309E-03 0.0 -0.224 0.269 0.257

0 .0^00 4.299E+00 2. 180E-02 4.321E+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 3.696E+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 9.410E-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 0.21 9

0 . 0800 2.726E+00 2.509E-02 2.751E+00 1 .757E-02 4.880E-03 0.0 -0.191 0.218 0.213

0.0900 2.536E+00 2.571 E-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 5.910E-03 0.0 -0.183 0.208 0.203

0.1250 2.098E+00 2.760E-02 2.126E+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 .796E+00 6 .225E-02 9.332E-03 0.0 -0.167 0.186 0.183

0.2000 1 .661E+00 3.096E-02 1 .692E+00 7.661E-02 1 .035E-02 0.0 -0.163 0.182 0.178

0.2500 1 .516E+00 3.306E-02 1 .549E+00 1 .076E-01 1 .225E-02 0.0 -0.158 0.175 0.171 0.3000 1 .421E + 00 3.51 9E-02 1 .456E+00 1 .410E-01 1 .400E-02 0.0 -0.153 0.169 0.166 0.3500 1 .355E+00 3.739E-02 1 .393E+00 1 .761E-01 1 .565E-02 1 . 129E-03 -0.146 0.165 0.162

0.4000 1 .308E+00 3.967E-02 1 .348E+00 2.126E-01 1 .721E-02 5.582E-03 -0.141 0.160 0.157

0.4500 1 .273E+00 4.204E-02 1 .315E+00 2.502E-01 1 .871E-02 1 .097E-02 -0.137 0.157 0.153

0.5000 1 .247E+00 4.448E-02 1 .291E+00 2.886E-01 2.016E-02 1 .71 IE-02 -0.134 0.153 0.149

0.5500 1 .227E+00 4.698E-02 1 .274E+00 3.276E-01 2.157E-02 2.388E-02 -0.131 0.150 0.146 0.6000 1 .21 1E+00 4. 956E-02 1 .261E+00 3.671E-01 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 0.138

0.8000 1 .178E+00 6.037E-02 1 .238E+00 5.275E-01 2.822E-02 6.443E-02 -0.118 0.138 0.133

0.9000 1 . 1 70E+00 6.605E-02 1 .236E+00 6.084E-01 3.076E-02 8.284E-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 . 1 67E+00 8.714E-02 1 .254E+00 8.899E-01 3.936E-02 1 .530E-01 -0.102 0.124 0.116

1 .5000 1 .173E+00 1 .031 E-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 . 1 98E-01 1 .302E+00 1 .282E+00 5.120E-02 2.610E-01 -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 -0.085 0.108 0.098

2.5000 1 .212E+00 1 .725E-01 1 .384E+00 1 .840E+00 6 .838E-02 4.239E-01 -0.077 0.101 0.089

3.0000 1 .230E+00 2.093E-01 1 .439E+00 2.1 95E+00 7. 949E-02 5.275E-01 -0.071 0.0 95 0.082

3.5000 1 .247E+00 2.471E-01 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-01 1 .601E+00 3. 182E+00 1 . 1 12E-01 8.057E-01 -0.061 0.082 0.067

5.0000 1 .289E + 00 3.649E-01 1 .654E+00 3.489E+00 1 .213E-01 8.881E-01 -0.058 0.079 0.064

5.5000 1 . 301 E+00 4.055E-01 1 .706E+00 3.787E+00 1 .311E-01 9.660E-01 -0.056 0.076 0.061 6.0000 1 .31 1E+00 4.464E-01 1 .758E+00 4.075E+00 1 .407E-01 1 .040E+00 -0.054 0.074 0.058

7.0000 1 .330E+00 5.297E-01 1 .860E+00 4.628E+00 1 .591E-01 1 .177E+00 -0.051 0.070 0.053

8.0000 1 .347E+00 6. 145E-01 1 .961E+00 5.152E+00 1 .766E-01 1 .301E+00 -0.049 0.066 0.049

9.0000 1 .361E+00 7.005E-01 2.062E+00 5.649E+00 1 .933E-01 1 .416E+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 .401E+00 1 .009E+00 2.410E+00 7.217E+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 9.103E+00 3.080E-01 2.147E+00 -0.035 0.048 0.030

20.0000 1 .456E+00 1 .697E+00 3.153E+00 9.929E+00 3.347E-01 2.312E+00 -0.032 0.046 0.028

25.0000 1 .480E+00 2. 1 69E+00 3.649E+00 1 .140E+01 3.813E-01 2.605E+00 -0.028 0.041 0.023

30.0000 1 .499E+00 2.648E+00 4. 147E+00 1 .269E+01 4.206E-01 2.858E+00 -0.025 0.038 0.020

35.0000 1 .514E+00 3.1 33E+00 4.647E+00 1 .382E+01 4.544E-01 3.081E+00 -0.022 0.036 0.018

40.0000 1 .527E+00 3.622E+00 5.149E+00 1 .485E+01 4.837E-01 3.281E+00 -0.020 0.034 0.016

45.0000 1 .539E+00 4.114E+00 5.652E+00 1 .577E+01 5.095E-01 3.463E+00 -0.019 0.032 0.014

50.0000 1 .548E+00 4.609E+00 6.158E+00 1 .662E+01 5.324E-01 3.628E+00 -0.017 0.031 0.013

55.0000 1 .557E+00 5.107E+00 6 .664E+00 1 .740E+01 5.529E-01 3.780E+00 -0.016 0.029 0.012

60.0000 1 .555E+00 5.607E+00 7.172E+00 1 .812E+01 5.71 3E-01 3.921E+00 -0.015 0.028 0.011 70.0000 1 .579E+00 6 .612E+00 8.1 91 E+00 1 . 943E+01 6 .033E-01 4.175E+00 -0.014 0.027 0.009

80.0000 1 .590E+00 7.623E+00 9.213E+00 2.058E+01 6.301E-01 4.399E+00 -0.013 0.025 0.008

90.0000 1 .600E+00 8.639E+00 1 .024E+01 2.161E+01 6.530E-01 4.600E+00 -0.012 0.024 0.007

100.0000 1 . 609E+00 9.659E+00 1 .127E+01 2.254E+01 6.727E-01 4.782E+00 -0.011 0.023 0.007

125.0000 1 .627E+00 1 .222E+01 1 .385E+01 2.454E+01 7.123E-01 5. 174E+00 -0.009 0.022 0.005

150.0000 1 .641E+00 1 .479E+01 1 .644E+01 2.61 9E+01 7.422E-01 5.502E+00 -0.008 0.020 0.004

175.0000 1 . 653E+00 1 .738E+01 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+01 2.163E+01 2.883E+01 7.848E-01 6 .029E+00 -0.006 0.018 0.003

250.0000 1 .680E+00 2.516E+01 2.684E+01 3.091E+01 8.140E-01 6 .445E+00 -0.005 0.017 0.003

300.0000 1 .693E+00 3.037E+01 3.207E+01 3.261E+01 8.354E-01 6.790E+00 -0.004 0.016 0.002

350.0000 1 .704E+00 3.560E+01 3.730E+01 3.405E+01 8.51 9E-01 7.083E+00 -0.003 0.016 0.002

400.0000 1 .714E+00 4.082E+01 4.254E+01 3.531E+01 8.651E-01 7.339E+00 -0.003 0.015 0.002

450.0000 1 .722E+00 4.606E+01 4.778E+01 3.641E+01 8.759E-01 7.566E+00 -0.003 0.015 0.002

500.0000 1 .729E+00 5.1 30E+01 5.303E+01 3.741E+01 8.848E-01 7.769E+00 -0.003 0.014 0.001 550.0000 1 .736E+00 5.654E+01 5.827E+01 3.831E+01 8.925E-01 7.954E+00 -0.002 0.014 0.001 600.0000 1 .742E+00 6.178E+01 6.353E+01 3.913E+01 8.991E-01 8. 123E+00 -0.002 0.014 0.001 700.0000 1 .753E+00 7.229E+01 7.404E+01 4.058E+01 9.098E-01 8.423E+00 -0.002 0.013 0.001 800.0000 1 .762E + 00 8.280E+01 8.456E+01 4. 185E+01 9.183E-01 8.684E+00 -0.002 0.013 0.001 900.0000 1 .770E+00 9.332E+01 9.509E+01 4.296E+01 9.252E-01 8.915E+00 -0.001 0.012 0.001 1000.0000 1 .777E+00 1 .038E+02 1 .056E+02 4.396E+01 9.309E-01 9.122E+00 -0.001 0.012 0.001

146
ELECTRONS IN STILBENE

I = 67.7 *V DENSITY = 9.707E-01 g/'cm 7

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. ddog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

NeV MeV cm^/g MeV cm^/g MoV cmVg g/cn * 0.0100 2.209E+01 3.009E-03 2.209E+01 2.561E-09 7.507E-05 0.0 -0.195 0.222 0.221 0.0125 1 .856E+01 3.019E-03 1 .856E+01 3.801E-09 8.992E-05 0.0 -0.187 0.212 0.211 0.0150 1 .610E+01 3.021E-03 1 .610E+01 5.251E-09 1 .091 E-09 0.0 -0.181 0.209 0.203

0.0175 1 .928E+01 3.026E-03 1 .928E+01 6.909E-09 1 . 178E-09 0.0 -0.176 0.198 0.197

0.0200 1 .287E+01 3.031E-03 1 .287E+01 8.751E-09 1 .310E-09 0.0 -0.172 0.193 0.192

0.0250 1 .083E+01 3.039E-03 1 .083E+01 1 .300E-03 1 .565E-09 0.0 -0.166 0.185 0.189

0.0300 9.918E+00 3.099E-03 9.921E+00 1 .797E-03 1 .808E-09 0.0 -0.161 0.179 0.178

0.0350 8.380E+00 3.059E-03 8.383E+00 2.361E-03 2.091E-09 0.0 -0.157 0.179 0.179

O.O^iOO 7.582E+00 3.070E-03 7.585E+00 2. 989E-03 2.267E-09 0.0 -0.159 0.170 0.170

0.0<f50 6 . 999E+00 3.083E-03 6.953E+00 3.678E-03 2.987E-09 0.0 -0.152 0.167 0.167

0.0500 6.935E+00 3.096E-03 6 .938E+00 9.926E-03 2.700E-09 0.0 -0.199 0.169 0.169

0.0550 6 .007E+00 3. 1 10E-03 6.010E+00 5.231E-03 2.909E-09 0.0 -0.197 0.162 0.161 0.0600 5.696E+00 3. 126E-03 5.650E+00 6 .089E-03 3.113E-09 0.0 -0.196 0.160 0.159

0.0700 5.071E+00 3.157E-03 5.079E+00 7.961E-03 3.508E-09 0.0 -0.193 0.156 0.156

0.0800 9.631E+00 3.191E-03 9.635E+00 1 .003E-02 3.889E-09 0.0 -0.190 0.153 0.153

0.0900 9.285E+00 3.228E-03 9.288E+00 1 .227E-02 9.258E-09 0.0 -0.138 0.150 0.150

0.1000 9.005E+00 3.267E-03 9.008E+00 1 .969E-02 9.616E-09 0.0 -0.136 0.198 0.198

0.1250 3.993E+00 3.373E-03 3.997E+00 2.1 39E-02 5.979E-09 0.0 -0.132 0.199 0.193

0.1500 3. 198E+00 3.987E-03 3. 152E+00 2.899E-02 6.288E-09 0.0 -0.129 0.190 0.190

0.1750 2. 901E+00 3.608E-03 2.909E+00 3.722E-02 7.068E-09 0.0 -0.127 0.137 0.137

0.2000 2.715E+00 3.736E-03 2.718E+00 9.61 3E-02 7.820E-09 0.0 -0.125 0.135 0.135

0.2500 2.956E+00 9.01 IE-0 3 2.960E+00 6 .553E-02 9.262E-09 0.0 -0.121 0.131 0.131

0 . 3000 2.287E+00 9.312E-03 2.292E+00 8.663E-02 1 .065E-03 0.0 -0.119 0.129 0.128

0.3500 2.170E+00 9.633E-03 2.175E+00 1 .091E-01 1 . 1 99E-03 0.0 -0.116 0.126 0.125

O.'iOOO 2.085E+00 9.975E-03 2.090E+00 1 .325E-01 1 .331E-03 0.0 -0.110 0.129 0.123

0 . 9500 2.020E+00 5.336E-03 2.026E+00 1 .568E-01 1 .962E-03 1 . 936E-02 -0.092 0.120 0.118

0.5000 1 .969E+00 5.719E-03 1 .975E+00 1 .81 9E-01 1 .592E-03 9.953E-02 -0.086 0.116 0.113

0.5500 1 .930E+00 6.107E-03 1 .936E+00 2.079E-01 1 .722E-03 7.225E-02 -0.081 0.112 0.108

0.6000 1 .898E+00 6.513E-03 1 .909E+00 2.335E-01 1 .852E-03 1 .01 9E-01 -0.076 0.108 0.109

0.7000 1 .851E+00 7.369E-03 1 .858E+00 2.867E-01 2. 115E-03 1 .698E-01 -0.068 0.101 0.096

0.8000 1 .819E+00 8.258E-03 1 .827E+00 3.910E-01 2.381E-03 2.305E-01 -0.063 0.096 0.089

0.9000 1 .797E+00 9.1 93E-03 1 .807E+00 3.960E-01 2.650E-03 2.971E-01 -0.058 0.091 0.083

1 .0000 1 .782E+00 1 .017E-02 1 .792E+00 9.516E-01 2. 923E-03 3.636E-01 -0.059 0.086 0.078

1 .2500 1 .761E+00 1 .279E-02 1 .779E+00 5. 920E-01 3.622E-03 5.253E-01 -0.097 0.078 0.068

1 .5000 1 .759E+00 1 .550E-02 1 .770E+00 7.331E-01 9.396E-03 6.779E-01 -0.093 0.071 0.061

1 .7500 1 .753E+00 1 .890E-02 1 .772E+00 8.793E-01 5.092E-03 8.190E-01 -0.090 0.066 0.056

2.0000 1 .756E+00 2.193E-02 1 .778E+00 1 .015E+00 5.857E-03 9.509E-01 -0.037 0.063 0.051 2.5000 1 .767E+00 2.780E-02 1 .795E+00 1 .295E+00 7.938E-03 1 .186E+00 -0.039 0.057 0.095

3.0000 1 .780E+00 3.952E-02 1 .819E+00 1 .572E+00 9.079E-03 1 .393E+00 -0.032 0.052 0.091 3.5000 1 .793E+00 9.152E-02 1 .839E+00 1 .896E+00 1 .075E-02 1 .576E+00 -0.030 0.099 0.038

9.0000 1 .805E+00 9.875E-02 1 .859E+00 2. 1 18E+00 1 .297E-02 1 .790E+00 -0.029 0.097 0.036

9.5000 1 .817E+00 5.620E-02 1 .873E+00 2.386E+00 1 .921E-02 1 .889E+00 -0.028 0.099 0.039

5.0000 1 .828E+00 6 .383E-02 1 .891E+00 2.652E+00 1 .598E-02 2.025E+00 -0.027 0.093 0.033

5.5000 1 .838E+00 7.162E-02 1 .909E+00 2.915E+00 1 .776E-02 2. 151E+00 -0.026 0.091 0.031 6.0000 1 .897E+00 7.956E-02 1 .927E+00 3. 175E+00 1 .957E-02 2.269E+00 -0.025 0.090 0.030

7.0000 1 .869E+00 9.582E-02 1 .960E+00 3.690E+00 2.321E-02 2.981E+00 -0.029 0.037 0.028

8.0000 1 .879E+00 1 .125E-01 1 .992E+00 9.196E+00 2.689E-02 2.671E+00 -0.022 0.036 0.027

9.0000 1 .893E+00 1 .296E-01 2.022E+00 9.699E+00 3.061E-02 2.893E+00 -0.020 0.039 0.025

10.0000 1 .909E+00 1 .970E-01 2.051E+00 5.185E+00 3.933E-02 3.001E+00 -0.019 0.032 0.029

12.5000 1 .929E+00 1 . 917E-01 2.121E+00 6.383E+00 9.368E-02 3.397E+00 -0.016 0.029 0.021 15.0000 1 .998E+00 2.377E-01 2.186E+00 7.599E+00 5.300E-02 3.693E+00 -0.013 0.027 0.018

17.5000 1 .969E+00 2.897E-01 2.299E+00 8.672E+00 6.229E-02 3.903E+00 -0.011 0.025 0.016

20.0000 1 .978E+00 3.325E-01 2.310E+00 9.768E+00 7. 138E-02 9.139E+00 -0.009 0.023 0.019

25.0000 1 . 999E+00 9.300E-01 2.929E+00 1 . 188E+01 8.929E-02 9.533E+00 -0.006 0.020 0.012

30.0000 2.016E+00 5.292E-01 2.595E+00 1 .389E+01 1 .065E-01 9.869E+00 -0.005 0.018 0.009

35.0000 2.030E+00 6.297E-01 2.660E+00 1 .581E+01 1 .230E-01 5.158E+00 -0.009 0.016 0.008

90.0000 2.092E+00 7.319E-01 2.773E+00 1 .765E+01 1 .390E-01 5.912E+00 -0.003 0.015 0.007

95.0000 2.052E+00 8.339E-01 2.886E+00 1 . 992E+01 1 .592E-01 5.638E+00 -0.002 0.013 0.006

50.0000 2.061E+00 9.372E-01 2.998E+00 2. 1 12E+01 1 .689E-01 5.892E+00 -0.002 0.012 0.005

55.0000 2.069E+00 1 .091E+00 3. 1 10E+00 2.276E+01 1 .830E-01 6.027E+00 -0.002 0.012 0.009

60.0000 2.077E+00 1 .196E+00 3.222E+00 2.939E+01 1 .965E-01 6 . 1 97E+00 -0.001 0.011 0.009

70.0000 2.090E+00 1 .356E+00 3.996E+00 2.739E+01 2.220E-01 6.999E+00 -0.001 0.010 0.003

80.0000 2. 101E+00 1 .568E+00 3.669E+00 3.015E+01 2.956E-01 6.761E+00 -0.001 0.009 0.003

90.0000 2.111E+00 1 .781E+00 3.892E+00 3.279E+01 2.675E-01 6.999E+00 -0.001 0.008 0.002

100.0000 2. 120E+00 1 . 996E+00 9. 1 15E+00 3.529E+01 2.879E-01 7.202E+00 -0.001 0.008 0.002

125.0000 2. 1 38E+00 2.535E+00 9.673E+00 9.099E+01 3.333E-01 7.699E+00 -0.000 0.007 0.001 150.0000 2. 1 53E+00 3.079E+00 5.232E+00 9.609E+01 3.721E-01 8.006E+00 -0.000 0.006 0.001 175.0000 2.166E+00 3.625E+00 5.791E+00 5.058E+01 9.058E-01 8.31 3E+00 -0.000 0.005 0.001 200.0000 2. 177E+00 9 . 1 79E+00 6.351E+00 5.970E+01 9.353E-01 8.579E+00 -0.000 0.005 0.001 250.0000 2.1 95E+00 5.277E+00 7.973E+00 6 . 1 95E+01 9.899E-01 9.029E+00 -0.000 0.009 0.001 300.0000 2.210E+00 6.386E+00 8.596E+00 6.81 9E+01 5.299E-01 9.387E+00 -0.000 0.009 0.000

350.0000 2.223E+00 7.999E+00 9.722E+00 7.365E+01 5.582E-01 9.695E+00 -0.000 0.009 0.000

900.0000 2.239E+00 8.619E+00 1 .085E+01 7.852E+01 5.863E-01 9. 962E+00 -0.000 0.009 0.000

950.0000 2.299E+00 9.733E+00 1 . 1 98E+01 8.290E+01 6.105E-01 1 .020E+01 -0.000 0.003 0.000

500.0000 2.252E+00 1 .085E+01 1 .310E+01 8.689E+01 6.315E-01 1 .091E+01 -0.000 0.003 0.000

550.0000 2.260E+00 1 . 1 97E1-01 1 .923E+01 9.055E+01 6 .500E-01 1 .060E+01 -0.000 0.003 0.000

600.0000 2.267E+00 1 . 31 OE+01 1 .536E+01 9.393E+01 6 . 669E-01 1 .077E+01 -0.000 0.003 0.000

700.0000 2.280E+00 1 .535E+01 1 .763E+01 1 .OOOE+02 6.993E-01 1 . 108E+01 -0.000 0.003 0.000

800.0000 2.291E+00 1 .760E+01 1 . 989E+01 1 .053E+02 7. 173E-01 1 . 1 35E+01 -0.000 0.003 0.000

900.0000 2.300E+00 1 .985E+01 2.216E+01 1 .101E+02 7.365E-01 1 . 158E+01 -0.000 0.003 0.000

1000.0000 2.309E+00 2.21 1 E+01 2.992E+01 1 .199E+02 7.530E-01 1 .179E+01 -0.000 0.002 0.000

147
ELECTRONS IN TISSUE-EQUIVALENT GAS (METHANE BASED)

I = 61.2 eV DENSITY = 1.06AE-03 g/ci»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 cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2.325E+01 3.402E-03 2.326E+01 2.426E-04 7.986E-05 0.0 -0.191 0.217 0.215

0.0125 1 .952E+01 3.421E-03 1 .953E+01 3.605E-04 9.606E-05 0.0 -0.183 0.207 0.206

0.0150 1 .692E+01 3.433E-03 1 .693E+01 4. 984E-04 1 .116E-04 0.0 -0.178 0.200 0.199

0.0175 1 .500E+01 3.441E-03 1 .500E+01 6 .556E-04 1 .265E-04 0.0 -0.173 0.194 0.193

0.0200 1 .352E+01 3.447E-03 1 .352E+01 8.314E-04 1 .410E-04 0.0 -0.169 0.189 0.188

0.0250 1 .137E + 01 3.457E-03 1 . 1 37E+01 1 .237E-03 1 .687E-04 0.0 -0.163 0.181 0.181 0.0300 9.882E+00 3.467E-03 9.885E+00 1 .710E-03 1 . 952E-04 0.0 -0.159 0.176 0.175

0.0350 8.789E+00 3.477E-03 8.792E+00 2.247E-03 2.206E-04 0.0 -0.155 0.171 0.171 0.0400 7.950E+00 3.488E-03 7.953E+00 2.846E-03 2.452E-04 0.0 -0.152 0.167 0.167

0 .0450 7.285E+00 3.501 E-03 7.288E+00 3.504E-03 2.690E-04 0.0 -0.149 0.164 0.164

0.0500 6 .743E + 00 3.514E-03 6.747E+00 4.217E-03 2.922E-04 0.0 -0.147 0.161 0.161

0 .0550 6 .294E+00 3.529E-03 6.298E+00 4.985E-03 3. 148E-04 0.0 -0.145 0.159 0.159

0 .0600 5 . 91 5E+00 3 .544E-03 5.91 9E+00 5.805E-03 3.368E-04 0.0 -0.143 0.157 0.157

0 .0700 5.310E+00 3.578E-03 5.314E+00 7.591E-03 3.796E-04 0.0 -0.141 0.153 0.153

0 . 0800 4 .849E+00 3.61 4E-03 4.853E+00 9.564E-03 4.208E-04 0.0 -0.138 0.150 0.150

0.0900 4.485E+00 3.654E-03 4.489E+00 1 .171E-02 4.607E-04 0.0 -0.136 0.148 0.148

0 . 1000 4.191E+00 3.696E-03 4.195E+00 1 .402E-02 4. 994E-04 0.0 -0.134 0.146 0.146

0.1250 3.655E+00 3.812E-03 3.659E+00 2.042E-02 5.920E-04 0.0 -0.130 0.142 0.141 0.1500 3.293E+00 3. 937E-03 3.297E+00 2.764E-02 6.797E-04 0.0 -0.128 0.138 0.138

0.1750 3.033E+00 4.071 E-03 3.037E+00 3.556E-02 7.638E-04 0.0 -0.125 0.136 0.135

0.2000 2.838E+00 4.213E-03 2.842E+00 4.408E-02 8.447E-04 0.0 -0.123 0.133 0.133

0 . 2500 2.567E+00 4.518E-03 2.572E+00 6.263E-02 9.998E-04 0.0 -0.120 0.130 0.129

0 . 3000 2.390E+00 4.851E-03 2.395E+00 8.282E-02 1 . 148E-03 0.0 -0.117 0.127 0.126

0 . 3500 2.267E+00 5.208E-03 2.272E+00 1 .043E-01 1 .293E-03 0.0 -0.115 0.125 0.124

0.4000 2. 178E+00 5.587E-03 2.184E+00 1 .268E-01 1 .434E-03 0.0 -0.113 0.123 0.122

0 . 4500 2.1 12E+00 5.988E-03 2.1 18E+00 1 .500E-01 1 .574E-03 0.0 -0.112 0.121 0.120

0 . 5000 2.061E+00 6 .407E-03 2.068E+00 1 .739E-01 1 .713E-03 0.0 -0.110 0.120 0.118

0.5500 2.022E+00 6.844E-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-01 1 .990E-03 0.0 -0.108 0.117 0.115

0.7000 1 . 949E+00 8.241 E-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 .931E+00 3.253E-01 2.546E-03 0.0 -0.104 0.113 0.111

0 . 9000 1 .904E+00 1 .027E-02 1 .914E+00 3.773E-01 2.826E-03 0.0 -0.102 0.112 0.109

1 .0000 1 .894E+00 1 . 1 35E-02 1 .905E+00 4.297E-01 3.110E-03 0.0 -0.101 0.111 0.108

1 .2500 1 .886E+00 1 .421 E-02 1 .900E+00 5.612E-01 3.831E-03 0.0 -0.098 0.108 0.105

1 .5000 1 .890E+00 1 .727E-02 1 .908E+00 6.926E-01 4.569E-03 0.0 -0.096 0.105 0.102

1 .7500 1 .901E+00 2.049E-02 1 .922E+00 8.232E-01 5.324E-03 0.0 -0.094 0.104 0.100

2.0000 1 .915E+00 2.385E-02 1 .939E+00 9.527E-01 6.093E-03 0.0 -0.092 0.102 0.0 98 2.5000 1 .945E+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 2.013E+00 1 .459E+00 9.280E-03 0.0 -0.087 0.097 0.092

3.5000 2.003E+00 4.610E-02 2.049E+00 1 .705E+00 1 .092E-02 0.0 -0.086 0.095 0.090

4.0000 2.030E+00 5.41 lE-02 2.084E+00 1 .947E+00 1 .258E-02 0.0 -0.084 0.094 0.089

4.5000 2.054E+00 6 .234E-02 2.116E+00 2.185E+00 1 .426E-02 0.0 -0.083 0.093 0.087

5.0000 2.077E+00 7.077E-02 2.147E+00 2.420E+00 1 .596E-02 0.0 -0.082 0.091 0.086

5.5000 2.098E+00 7.938E-02 2. 177E+00 2.651E+00 1 .766E-02 0.0 -0.081 0.090 0.084

6.0000 2.1 17E+00 8.815E-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. 184E+00 1 .246E-01 2.308E+00 3.765E+00 2.628E-02 0.0 -0.078 0.086 0.080

9.0000 2.212E+00 1 .434E-01 2.355E+00 4.1 94E+00 2.974E-02 0.0 -0.077 0.085 0.078

10.0000 2.237E+00 1 .626E-01 2.400E+00 4.614E+00 3.320E-02 0.0 -0.076 0.083 0.077

12.5000 2.292E+00 2.119E-01 2.504E+00 5.634E+00 4. 180E-02 0.0 -0.074 0.081 0.074

15.0000 2.337E+00 2.626E-01 2.599E+00 6.613E+00 5.032E-02 0.0 -0.072 0.079 0.072

17.5000 2.375E+00 3. 144E-01 2.689E+00 7.559E+00 5.870E-02 0.0 -0.071 0.077 0.070

20.0000 2.408E+00 3.671E-01 2.775E+00 8.474E+00 6.694E-02 0.0 -0.070 0.075 0.068

25.0000 2.462E+00 4.743E-01 2.937E+00 1 .022E+01 8.296E-02 1 .908E-02 -0.059 0.072 0.064

30.0000 2.501E+00 5.835E-01 3.085E+00 1 .188E+01 9.838E-02 1 .033E-01 -0.046 0.068 0.058

35.0000 2.530E+00 6.942E-01 3.225E+00 1 .347E+01 1 .132E-01 2. 153E-01 -0.039 0.064 0.051 40.0000 2.554E+00 8.060E-01 3.360E+00 1 .499E+01 1 .275E-01 3.356E-01 -0.034 0.060 0.046

45.0000 2.573E+00 9.188E-01 3.492E+00 1 .645E+01 1 .413E-01 4.562E-01 -0.030 0.057 0.042

50.0000 2.590E+00 1 .032E+00 3.622E+00 1 .785E+01 1 .546E-01 5.735E-01 -0.027 0.054 0.038

55.0000 2.605E+00 1 . 147E+00 3.751E+00 1 .921E+01 1 .674E-01 6.861E-01 -0.025 0.052 0.035

60.0000 2.618E+00 1 .261E+00 3.879E+00 2.052E+01 1 .798E-01 7.934E-01 -0.024 0.049 0.032

70.0000 2.640E+00 1 .493E+00 4.132E+00 2.302E+01 2.032E-01 9.924E-01 -0.021 0.046 0.028

80.0000 2.658E+00 1 .725E+00 4.384E+00 2.537E+01 2.250E-01 1 .172E+00 -0.020 0.043 0.025

90.0000 2.674E+00 1 . 960E+00 4.634E+00 2.759E+01 2.454E-01 1 .336E+00 -0.019 0.040 0.022

1 00.0000 2.688E+00 2.1 95E+00 4.883E+00 2.969E+01 2.645E-01 1 .485E+00 -0.018 0.038 0.020

125.0000 2.717E+00 2.787E+00 5.505E+00 3.451E+01 3.074E-01 1 .809E+00 -0.016 0.034 0.017

150.0000 2.741E+00 3.384E+00 6.124E+00 3.881E+01 3.445E-01 2.081E+00 -0.015 0.031 0.014

175.0000 2.760E+00 3. 984E+00 6.743E+00 4.270E+01 3.770E-01 2.315E+00 -0.014 0.029 0.013

200.0000 2.776E+00 4.586E+00 7.362E+00 4.625E+01 4.058E-01 2.520E+00 -0.014 0.027 0.011 250.0000 2.803E+00 5.796E+00 8.599E+00 5.252E+01 4.546E-01 2.870E+00 -0.012 0.024 0.009

300.0000 2.825E+00 7.012E+00 9.837E+00 5.796E+01 4. 945E-01 3. 162E+00 -0.011 0.022 0.008

350.0000 2.843E+00 8.232E+00 1 .107E+01 6.274E+01 5.280E-01 3.414E+00 -0.010 0.021 0.007

400.0000 2 .858E+00 9.456E+00 1 .231 E+01 6.702E+01 5.565E-01 3.636E+00 -0.009 0.020 0.006

450.0000 2.871E+00 1 .068E+01 1 .355E+01 7.089E+01 5.811 E-01 3.836E+00 -0.009 0.019 0.006 500.0000 2.882E+00 1 . 1 91 E+01 1 .479E+01 7.442E+01 6.027E-01 4.017E+00 -0.008 0.018 0.005

550.0000 2.892E+00 1 .314E+01 1 .603E+01 7.767E+01 6.218E-01 4.184E+00 -0.007 0.017 0.005

600.0000 2. 901 E+00 1 .437E+01 1 .727E+01 8.067E+01 6.388E-01 4.338E+00 -0.007 0.017 0.004

700.0000 2.917E+00 1 .683E+01 1 .975E+01 8.608E+01 6.679E-01 4.614E+00 -0.005 0.016 0.004

800.0000 2. 930E+00 1 .930E+01 2.223E+01 9.085E+01 6.920E-01 4.859E+00 -0.005 0.015 0.003

900.0000 2.941E+00 2.177E+01 2.472E+01 9.512E+01 7.123E-01 5.077E+00 -0.004 0.014 0.003

1000.0000 2.951E+00 2.425E+01 2.720E+01 9.897E+01 7.297E-01 5.275E+00 -0.003 0.014 0.003

148
ELECTRONS IN TISSUE-EQUIVALENT GAS (PROPANE BASED)

I = 59.5 eV DENSITY = 1 .826E-03 b/c»’ (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 MoV cm*/g MeV cm^/g MeV cmVg g/cm^

0.0100 2.390E+01 3.279E-03 2.390E+01 2.910E-09 7.698E-05 0.0 -0.190 0.215 0.219

0.0125 1 .969E+01 3.290E-03 1 .969E+01 3.581E-09 9.1 95E-05 0.0 -0.182 0.206 0.205

0.0150 1 .702E+01 3.301E-03 1 .703E+01 9.952E-09 1 .068E-09 0.0 -0.177 0.198 0.198

0.0175 1 .509E+01 3.308E-03 1 .509E+01 6.516E-09 1 .210E-09 0.0 -0.172 0.193 0.192

0.0200 1 .359E+01 3.319E-03 1 .359E+01 8.269E-09 1 .398E-09 0.0 -0.168 0.188 0.187

0.0250 1 .193E+01 3.323E-03 1 .193E+01 1 .229E-03 1 .619E-09 0.0 -0.162 0.180 0.180

0.0300 9.933E+00 3.333E-03 9. 937E+00 1 .700E-03 1 .867E-09 0.0 -0.158 0.175 0.179

0.0350 8.839E+00 3.393E-03 8.837E+00 2.235E-03 2.1 lOE-09 0.0 -0.159 0.170 0.170

O.OAOO 7.990E+00 3.355E-03 7.993E+00 2.830E-03 2.395E-09 0.0 -0.151 0.167 0.166

0.0A50 7.321E+00 3.367E-03 7.329E+00 3.985E-03 2.573E-09 0.0 -0.199 0.163 0.163

0.0500 6 .776E+00 3.381E-03 6.780E+00 9.195E-03 2.795E-09 0.0 -0.197 0.161 0.160

0.0550 6.325E+00 3.395E-03 6.328E+00 9.959E-03 3.012E-09 0.0 -0.195 0.158 0.158

0.0600 5.999E+00 3.910E-03 5.997E+00 5.775E-03 3.223E-09 0.0 -0.193 0.156 0.156

0.0700 5.335E+00 3.993E-03 5.339E+00 7.553E-03 3.633E-09 0.0 -0.190 0.153 0.152

0.0800 9.872E+00 3.979E-03 9.875E+00 9.516E-03 9.029E-09 0.0 -0.138 0.150 0.150

0.0900 9.506E+00 3.518E-03 9.509E+00 1 .165E-02 9.91 lE-09 0.0 -0.135 0.197 0.197

0.1000 9.210E+00 3.559E-03 9.219E+00 1 .395E-02 9.783E-09 0.0 -0.139 0.195 0.195

0.1250 3.671E+00 3.672E-03 3.675E+00 2.033E-02 5.672E-09 0.0 -0.130 0.191 0.191 0.1500 3.307E+00 3.799E-03 3.31 1E+00 2.751E-02 6.515E-09 0.0 -0.127 0.138 0.137

0.1750 3.096E+00 3.929E-03 3.050E+00 3.590E-02 7.322E-09 0.0 -0.125 0.135 0.139

0.2000 2.850E+00 9.061E-03 2.859E+00 9.388E-02 8. lOOE-09 0.0 -0.123 0.133 0.132

0.2500 2.578E+00 9.357E-03 2.582E+00 6.236E-02 9.592E-09 0.0 -0.119 0.129 0.128

0.3000 2.900E+00 9.680E-03 2.909E+00 8.297E-02 1 .102E-03 0.0 -0.117 0.126 0.126

0.3500 2.276E+00 5.026E-03 2.281E+00 1 .039E-01 1 .291E-03 0.0 -0.115 0.129 0.123

0.9000 2.187E+00 5.399E-03 2.192E+00 1 .262E-01 1 .378E-03 0.0 -0.113 0.122 0.121 0.9500 2. 120E+00 5.782E-03 2. 126E+00 1 .999E-01 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 .696E-03 0.0 -0.110 0.119 0.118

0.5500 2.030E+00 6.612E-03 2.037E+00 1 .976E-01 1 .780E-03 0.0 -0.108 0.118 0.116

0.6000 1 .999E+00 7.050E-03 2.006E+00 2.223E-01 1 .913E-03 0.0 -0.107 0.117 0.115

0.7000 1 .956E+00 7.965E-03 1 . 969E+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 3.290E-01 2.999E-03 0.0 -0.103 0.113 0.111 0.9000 1 .91 1E+00 9.939E-03 1 .921E+00 3.759E-01 2.720E-03 0.0 -0.102 0.112 0.109

1 .0000 1 .901E+00 1 .098E-02 1 .912E+00 9.281E-01 2.999E-03 0.0 -0.100 0.110 0.107

1 .2500 1 .892E+00 1 .375E-02 1 .906E+00 5.592E-01 3.690E-03 0.0 -0.098 0.107 0.109

1 .5000 1 .897E+00 1 .671E-02 1 .919E+00 6.901E-01 9.909E-03 0.0 -0.095 0.105 0.102

1 .7500 1 .908E+00 1 .989E-02 1 .927E+00 8.203E-01 5. 133E-03 0.0 -0.093 0.103 0.099

2.0000 1 .921E+00 2.309E-02 1 .999E+00 9.995E-01 5.877E-03 0.0 -0.092 0.102 0.0 98 2.5000 1 .951E+00 2.999E-02 1 .981E+00 1 .209E+00 7.399E-03 0.0 -0.089 0.099 0.095

3.0000 1 .981E+00 3.716E-02 2.018E+00 1 .959E+00 8.959E-03 0.0 -0.087 0.097 0.092

3.5000 2.010E+00 9.968E-02 2.059E+00 1 .700E+00 1 .055E-02 0.0 -0.086 0.095 0.090

9.0000 2.036E+00 5.295E-02 2.088E+00 1 .991E+00 1 .216E-02 0.0 -0.089 0.099 0.088

9.5000 2.060E+00 6.099E-02 2.121E+00 2. 179E+00 1 .379E-02 0.0 -0.083 0.092 0.087

5.0000 2.083E+00 6.862E-02 2.152E+00 2.913E+00 1 .593E-02 0.0 -0.082 0.091 0.085

5.5000 2.109E+00 7.698E-02 2.181E+00 2.699E+00 1 .708E-02 0.0 -0.081 0.090 0.089

6.0000 2. 123E+00 8.550E-02 2.209E+00 2.871E+00 1 .879E-02 0.0 -0.080 0.089 0.083

7.0000 2. 159E+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 .208E-0

2.31 1E+00 3.756E+00 2.593E-02 0.0 -0.078 0.086 0.080

9.0000 2.218E+00 1 .392E-01 2.357E+00 9.189E+00 2.879E-02 0.0 -0.076 0.089 0.078

10.0000 2.299E+00 1 .578E-01 2.901E+00 9.605E+00 3.215E-02 0.0 -0.076 0.083 0.077

12.5000 2.298E+00 2.057E-01 2.509E+00 5.629E+00 9.051E-02 0.0 -0.079 0.081 0.079

15.0000 2.393E+00 2.599E-01 2.598E+00 6.609E+00 9.879E-02 0.0 -0.072 0.079 0.072

17.5000 2.381E+00 3.053E-01 2.686E+00 7.550E+00 5.695E-02 7.537E-03 -0.069 0.077 0.069

20.0000 2.910E+00 3.565E-01 2.767E+00 8.967E+00 6.999E-02 5.069E-02 -0.059 0.079 0.065

25.0000 2.959E+00 9.607E-01 2.915E+00 1 .023E+01 8.071E-02 1 .907E-01 -0.091 0.068 0.056

30.0000 2.986E+00 5.669E-01 3.053E+00 1 .190E+01 9.592E-02 3.525E-01 -0.039 0.063 0.099

35.0000 2.512E+00 6.799E-01 3.186E+00 1 .350E+01 1 .106E-01 5.139E-01 -0.030 0.058 0.093

90.0000 2.532E+00 7.831E-01 3.315E+00 1 .509E+01 1 .298E-01 6.676E-01 -0.027 0.055 0.038

95.0000 2.550E+00 8.928E-01 3.993E+00 1 .652E+01 1 .385E-01 8.1 18E-01 -0.029 0.052 0.039

50.0000 2.565E+00 1 .003E+00 3.568E+00 1 .795E+01 1 .517E-01 9.969E-01 -0.023 0.099 0.031 55.0000 2.578E+00 1 . 1 19E+00 3.693E+00 1 .933E+01 1 .699E-01 1 .072E+00 -0.021 0.096 0.029

60.0000 2.591E+00 1 .226E+00 3.817E+00 2.066E+01 1 .766E-01 1 .189E+00 -0.020 0.099 0.027

70.0000 2.612E+00 1 .951E+00 9.062E+00 2.320E+01 1 .999E-01 1 .903E+00 -0.019 0.091 0.023

80.0000 2.629E+00 1 .677E+00 9.307E+00 2.559E+01 2.216E-01 1 .593E+00 -0.018 0.038 0.021 90.0000 2.695E+00 1 .905E+00 9.550E+00 2.785E+01 2.919E-01 1 .763E+00 -0.017 0.036 0.019

100.0000 2.658E+00 2.139E+00 9.792E+00 2.999E+01 2.610E-01 1 .917E+00 -0.017 0.039 0.017

125.0000 2.687E+00 2.710E+00 5.397E+00 3.990E+01 3.037E-01 2.251E+00 -0.015 0.030 0.015

150.0000 2.709E+00 3.291E+00 6 .OOOE+00 3.929E+01 3.908E-01 2.529E+00 -0.019 0.028 0.013

175.0000 2.728E+00 3.879E+00 6.602E+00 9.326E+01 3.733E-01 2.769E+00 -0.013 0.026 0.011 200.0000 2.799E+00 9.960E+00 7.205E+00 9.689E+01 9.020E-01 2.980E+00 -0.012 0.029 0.010

250.0000 2.770E+00 5.638E+00 8.908E+00 5.330E+01 9.508E-01 3.391E+00 -0.011 0.022 0.008

300.0000 2.791E+00 6 .822E + 00 9.612E+00 5.886E+01 9.909E-01 3.699E+00 -0.010 0.020 0.007

350.0000 2.808E+00 8.009E+00 1 .082E+01 6.376E+01 5.299E-01 3.907E+00 -0.008 0.019 0.006

900.0000 2.822E+00 9.200E+00 1 .202E+01 6.819E+01 5.530E-01 9.190E+00 -0.007 0.018 0.006

950.0000 2.839E+00 1 .039E+01 1 .323E+01 7.21 1E+01 5.778E-01 9.399E+00 -0.006 0.017 0.005

500.0000 2.895E+00 1 . 1 59E+01 1 .993E+01 7.573E+01 5.999E-01 9.539E+00 -0.006 0.016 0.009

550.0000 2.859E+00 1 .279E+01 1 .569E+01 7.905E+01 6. 186E-01 9.713E+00 -0.005 0.015 0.009

600.0000 2.863E+00 1 . 398E+01 1 .685E+01 8.21 3E+01 6.357E-01 9.873E+00 -0.009 0.015 0.009

700.0000 2.877E+00 1 .638E+01 1 .926E+01 8.768E+01 6.650E-01 5. 161E+00 -0.003 0.019 0.003

800.0000 2.890E+00 1 .879E+01 2. 168E+01 9.257E+01 6.893E-01 5.919E+00 -0.003 0.013 0.003

900.0000 2.901E+00 2.119E+01 2.909E+01 9.695E+01 7.097E-01 5.690E+00 -0.002 0.013 0.002

1000.0000 2.910E+00 2.360E+01 2.651E+01 1 .009E+02 7.273E-01 5.893E+00 -0.002 0.012 0.002

149
ELECTRONS IN TOLUENE

I = 62.5 eV DENSITY = 8.669E-01 g/cm ^

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^/g MeV cm^/g MeV cm^/g g/cm ^

0.0100 2.285E+01 2.960E-03 2.286E+01 2.470E-04 7.135E-05 0.0 -0.192 0.218 0.217

0.0125 1 . 91 9E+01 2.970E-03 1.91 9E+01 3.669E-04 8.552E-05 0.0 -0.184 0.208 0.207

0.0150 1 .664E+01 2. 977E-03 1 .664E+01 5.072E-04 9. 908E-05 0.0 -0.178 0.201 0.200

0.0175 1 .475E+01 2. 982E-03 1 .475E+01 6.671E-04 1 . 122E-04 0.0 -0.174 0.195 0.194

0.0200 1 .329E+01 2. 986E-03 1 .329E+01 8.459E-04 1 .24SE-04 0.0 -0.170 0.190 0.189

0.0250 1 . 1 18E+01 2.995E-03 1 .1 lSE+01 1 .258E-03 1 .491E-04 0.0 -0.164 0.182 0.182

0 .0300 9.719E+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 3.015E-03 8.648E+00 2.285E-03 1 . 948E-04 0.0 -0.155 0.172 0.171

O.O'iOO 7.820E+00 3.026E-03 7 .823E+00 2.894E-03 2.164E-04 0.0 -0.152 0.168 0.168

0 .0^50 7 . 1 66E+00 3.039E-03 7.169E+00 3.563E-03 2.374E-04 0.0 -0.150 0.165 0.164

0 .0500 6.634E+00 3.052E-03 6.637E+00 4.28SE-03 2.579E-04 0.0 -0.148 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 5.819E+00 3.082E-03 5.823E+00 5. 902E-03 2. 974E-04 0.0 -0.144 0.158 0.157

0.0700 5.225E+00 3. 1 13E-03 5.228E+00 7.718E-03 3.353E-04 0.0 -0.141 0.154 0.154

0.0800 4.771E+00 3. 147E-03 4.774E+00 9.723E-03 3.718E-04 0.0 -0.138 0.151 0.151 0.0900 4 . 41 3E+00 3. 184E-03 4.417E+00 1 . 1 90E-02 4.072E-04 0.0 -0.136 0.148 0.148

0.1000 4. 124E+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 3.241E+00 3.440E-03 3.244E+00 2.809E-02 6 .020E-04 0.0 -0.128 0.139 0.138

0.1750 2. 985E+00 3.560E-03 2.989E+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 2.531E+00 6.365E-02 8.878E-04 0.0 -0.120 0.130 0.129

0.3000 2.353E+00 4.258E-03 2. 357E+00 8.417E-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 . 150E-03 0.0 -0.115 0.125 0.124

0.^000 2. 144E+00 4.915E-03 2.1 49E+00 1 .288E-01 1 .277E-03 0.0 -0.108 0.123 0.122

0 .'1500 2.077E+00 5.273E-03 2.082E+00 1 .525E-01 1 .403E-03 2.097E-02 -0.090 0.119 0.117

0.5000 2.024E+00 5.647E-03 2.030E+00 1 .768E-01 1 .528E-03 4.725E-02 -0.084 0.114 0.112

0.5500 1 .983E+00 6 .036E-03 1 . 989E+00 2.017E-01 1 .654E-03 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 . 901E+00 7.281E-03 1 .908E + 00 2.788E-01 2.033E-03 1 .715E-01 -0.067 0.100 0.094

0.8000 1 .868E+00 8. 167E-03 1 .876E+00 3.317E-01 2.289E-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 3.751E-01 -0.053 0.085 0.076

1 .2500 1 .808E+00 1 .261 E-02 1 .820E+00 5.762E-01 3.488E-03 5.402E-01 -0.046 0.076 0.067

1 .5000 1 .800E+00 1 .534E-02 1 .815E+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 .817E+00 8.515E-01 4.908E-03 8.395E-01 -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 .812E+00 2.753E-02 1 .839E+00 1 .262E+00 7.177E-03 1 .213E+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 + 00 4. 1 12E-02 1 .878E+00 1 .800E+00 1 .039E-02 1 .609E+00 -0.029 0.048 0.037

4.0000 1 .849E+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 .861 E+00 5.568E-02 1 .917E+00 2.327E+00 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 .892E+00 7 .883E-02 1 .971E+00 3.099E+00 1 .893E-02 2.312E+00 -0.024 0.038 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

8.0000 1 . 924E+00 1 . 1 15E-01 2.036E+00 4.097E+00 2.604E-02 2.720E+00 -0.021 0.034 0.025

9.0000 1 . 937E+00 1 .285E-01 2.066E+00 4.585E+00 2.965E-02 2.894E+00 -0.020 0.033 0.024

10.0000 1 . 949E+00 1 .457E-01 2.095E+00 5.065E+00 3.327E-02 3.053E+00 -0.018 0.031 0.023

12.5000 1 . 974E+00 1 .900E-01 2.164E+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 3.701E+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 2.471E+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 2.076E+00 6.246E-01 2.701E+00 1 .550E+01 1 .199E-01 5.221E+00 -0.003 0.015 0.007

40.0000 2.088E+00 7.254E-01 2.814E+00 1 .732E+01 1 .355E-01 5.476E+00 -0.003 0.014 0.006

45.0000 2.099E+00 8.273E-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+01 1 .649E-01 5.906E+00 -0.002 0.012 0.005

55.0000 2.116E+00 1 .033E+00 3. 149E+00 2.235E+01 1 .787E-01 6.091E+00 -0.002 0.011 0.004

60.0000 2.124E+00 1 . 1 37E+00 3.260E+00 2.391E+01 1 . 920E-01 6.261E+00 -0.001 0.010 0.004

70.0000 2.1 37E+00 1 .345E+00 3.483E+00 2.688E+01 2.171E-01 6 .563E+00 -0.001 0.009 0.003

80.0000 2. 149E+00 1 .556E+00 3.704E+00 2. 966E+01 2.404E-01 6.825E+00 -0.001 0.009 0.002

90.0000 2.159E+00 1 .768E+00 3.926E+00 3.228E+01 2.621E-01 7.058E+00 -0.001 0.008 0.002

1 00.0000 2.168E+00 1 . 980E+00 4.148E+00 3.476E+01 2.823E-01 7.266E+00 -0.001 0.007 0.002

125.0000 2. 186E+00 2.516E+00 4.702E+00 4.042E+01 3.273E-01 7.708E+00 -0.000 0 .006 0.001 150.0000 2.202E+00 3.055E+00 5.257E+00 4.544E+01 3.659E-01 8.071E+00 -0.000 0.006 0.001 175.0000 2.215E+00 3.598E+00 5.81 3E+00 4.996E+01 3.994E-01 8. 377E+00 -0.000 0.005 0.001 200.0000 2.226E+00 4. 143E+00 6 . 369E+00 5.407E+01 4.289E-01 8.643E+00 -0.000 0.005 0.001 250.0000 2.245E+00 5.238E+00 7.483E+00 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+01 5. 186E-01 9.452E+00 -0.000 0.004 0.000

350.0000 2.273E+00 7.444E+00 9.717E+00 7.300E+01 5.520E-01 9.759E+00 -0.000 0.004 0.000

400.0000 2 . 284E+00 8.552E+00 1 .084E+01 7.787E+01 5.802E-01 1 .003E+01 -0.000 0.003 0.000

450.0000 2.294E+00 9.662E+00 1 . 1 96E+01 8.226E+01 6 .045E-01 1 .026E+01 -0.000 0.003 0.000

500.0000 2. 303E+00 1 . 077E+01 1 . 308E+01 8.626E+01 6.257E-01 1 .047E+01 -0.000 0.003 0.000

550.0000 2.31 lE+00 1 . 189E+01 1 .420E+01 8.993E+01 6 .444E-01 1 .066E+01 -0.000 0.003 0.000

600.0000 2.318E+00 1 .300E+01 1 .532E+01 9.332E+01 6.609E-01 1 .084E + 01 -0.000 0.003 0.000

700.0000 2.331E+00 1 .524E+01 1 .757E+01 9.941E+01 6.891E-01 1 . 1 14E + 01 -0.000 0.003 0.000

800.0000 2.342E+00 1 .747E+01 1 . 982E+01 1 .048E+02 7.124E-01 1 .141E+01 -0.000 0.003 0.000

900.0000 2.352E+00 1 .972E+01 2.207E+01 1 .095E+02 7.319E-01 1 . 165E+01 -0.000 0.002 0.000

1000.0000 2.360E+00 2.1 96E+01 2.432E+01 1 .139E+02 7.485E-01 1 . 186E+01 -0.000 0.002 0.000

150
ELECTRONS IN WATER, LIQUID

I = 75.0 eV DENSITY = 1 .OOOE+OO1 g/cm^

ENERGY STOPPING POWER CSDA RADIATION DEHS.EFF. dClog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm*/g MeV cm^/g MeV cm^/g g/cm ^

0.0100 2.256E+01 3.898E-03 2.257E+01 2.515E-0A 9. A08E-05 0.0 -0.199 0.227 0.225

0.0125 1 .897E+01 3.927E-03 1 .898E+01 3.728E-0A 1 . 133E-0A 0.0 -0.190 0.217 0.215

0.0150 1 .6A7E+01 3. 9AAE-03 1 .6A7E+01 5. 1 A7E-0A 1 .316E-0A 0.0 -0 . 18A 0.208 0.207

0.0175 1 .A61E+01 3. 955E-03 1 .A61E+01 6.761E-0A 1 . A92E-0A 0.0 -0.179 0.202 0.201 0.0200 1 .317E+01 3. 963E-03 1 .318E+01 8.566E-0A 1 .663E-0A 0.0 -0.175 0.197 0.196

0.0250 1 . 109E+01 3.97AE-03 1 . 1 10E+01 1 .272E-03 1 . 990E-0A 0.0 -0.169 0.189 0.188

0.0300 9.653E+00 3.98AE-03 9.657E+00 1 .756E-03 2.301E-0A 0.0 -0. 16A 0.182 0.182

0.0350 8.592E+00 3. 99AE-03 8.596E+00 2.306E-03 2.599E-0A 0.0 -0.160 0.177 0.177

O.OAOO 7.777E+00 A.005E-03 7.781E+00 2.919E-03 2.886E-0A 0.0 -0.157 0.173 0.173

0 . 0A50 7.130E+00 A.018E-03 7.13AE+00 3.591E-03 3. 165E-0A 0.0 -0.1 5A 0.170 0.170

0.0500 6 .603E+00 A.031E-03 6 .607E+00 A.320E-03 3. A35E-0A 0.0 -0.152 0.167 0.167

0.0550 6.166E+00 A.0A6E-03 6. 170E+00 5.103E-03 3.698E-0A 0.0 -0.150 0.165 0.16A

0.0600 5.797E+00 A.062E-03 5.801 E+00 5. 9A0E-03 3.955E-0A 0.0 -0.1 A8 0.162 0.162

0.0700 5.207E+00 A.098E-03 5.211 E+00 7.762E-03 A.A52E-0A 0.0 -0.1A5 0.158 0.158

0.0800 A.757E+00 A.138E-03 A.762E+00 9.773E-03 A.931E-0A 0.0 -0.1A2 0.155 0.155

0.0900 A.A02E+00 A.181E-03 A.A07E+00 1 . 1 96E-02 5.393E-0A 0.0 -O.IAO 0.153 0.152

0.1000 A. 1 15E+00 A.228E-03 A. 120E+00 1 . A31E-02 5.8A1E-0A 0.0 -0.138 0.150 0.150

0.1250 3.591E+00 A.355E-03 3.596E+00 2.083E-02 6.912E-0A 0.0 -0.1 3A 0.1 A6 0. 1 A5 0.1500 3.238E+00 A.A9AE-03 3.2A2E+00 2.817E-02 7.926E-0A 0.0 -0.131 0.1A2 0.1A2

0.1750 2. 98AE+00 A.6A3E-03 2.988E+00 3.622E-02 8.89AE-0A 0.0 -0.128 0.139 0.139

0.2000 2.793E+00 A.801E-03 2.798E+00 A.A87E-02 9.826E-0A 0.0 -0.126 0.137 0.136

0.2500 2.528E+00 5. 1 A1E-03 2.533E+00 6.372E-02 1 .161E-03 0.0 -0.123 0.133 0.132

0 . 3000 2.355E+00 5.51 AE-03 2.360E+00 8.A21E-02 1 .331E-03 0.0 -0.120 0.130 0.129

0.3500 2.235E+00 5.913E-03 2.2A1E+00 1 .060E-01 1 .A96E-03 0.0 -0.118 0.128 0.127

O.AOOO 2. 1A8E+00 6.339E-03 2.15AE+00 1 .288E-01 1 .658E-03 0.0 -0.116 0.126 0.125

0.A500 2.083E+00 6.787E-03 2.090E+00 1 .523E-01 1 .818E-03 0.0 -0.11A 0.12A 0.123

0.5000 2.03AE+00 7.257E-03 2.0A1E+00 1 .766E-01 1 .976E-03 0.0 -0.111 0.123 0.121 0.5500 1 . 995E+00 7.7A7E-03 2.003E+00 2.013E-01 2.13AE-03 1 . 103E-02 -0.09A 0.120 0.118

0.6000 1 . 963E+00 8.25AE-03 1 .972E+00 2.265E-01 2.292E-03 2.938E-02 -0.088 0.117 0.1 1A 0.7000 1 .917E+00 9.312E-03 1 .926E+00 2.778E-01 2.608E-03 7.A35E-02 -0.078 0.110 0.106

0.8000 1 .886E+00 1 .0A3E-02 1 .896E+00 3.302E-01 2.928E-03 1 .267E-01 -0.070 0.105 0.099

0.9000 1 .86AE+00 1 . 159E-02 1 .876E+00 3.832E-01 3.251E-03 1 .835E-01 -0.06A 0.099 0.093

1 .0000 1 .8A9E+00 1 .280E-02 1 .862E+00 A.367E-01 3.579E-03 2.A28E-01 -0.059 0.095 0.087

1 .2500 1 .829E+00 1 .600E-02 1 .8A5E+00 5.717E-01 A. A16E-03 3.9AAE-01 -0.0A9 0.085 0.075

1 .5000 1 .822E+00 1 .9A2E-02 1 .8A1E+00 7.075E-01 5.281E-03 5.A37E-01 -O.OA3 0.077 0.066

1 .7500 1 .821E+00 2.303E-02 1 .8AAE+00 8.A32E-01 6. 171E-03 6.866E-01 -0.038 0.071 0.059

2.0000 1 .82AE+00 2.678E-02 1 .850E+00 9.785E-01 7.085E-03 8.218E-01 -0.035 0.066 0.053

2.5000 1 .83AE+00 3. A68E-02 1 .868E+00 1 .2A7E+00 8.969E-03 1 .069E+00 -0.030 0.059 O.OA5

3.0000 1 .8A6E+00 A.299E-02 1 .889E+00 1 .51 AE+00 1 .092E-02 1 .288E+00 -0.027 0.05A O.OAO

3.5000 1 .858E+00 5.16AE-02 1 .910E+00 1 .777E+00 1 .291E-02 1 .A8AE+00 -0.025 0.0A9 0.036

A.OOOO 1 .870E+00 6 .058E-02 1 .931E+00 2.037E+00 1 .A95E-02 1 .660E+00 -0.02A 0.0A6 0.033

A. 5000 1 .882E+00 6.976E-02 1 .951E+00 2.295E+00 1 .702E-02 1 .821E+00 -0.023 0.0A3 0.031 5.0000 1 .892E+00 7.917E-02 1 .971E+00 2.550E+00 1 .91 IE-02 1 .967E+00 -0.022 0.0A1 0.029

5.5000 1 .902E+00 8.876E-02 1 .991E+00 2.802E+00 2.123E-02 2.102E+00 -0.021 0.039 0.027

6.0000 1 .91 lE+00 9.85AE-02 2.010E+00 3.052E+00 2.336E-02 2.227E+00 -0.021 0.038 0.026

7.0000 1 .928E+00 1 .185E-01 2.0A7E+00 3.5A5E+00 2.766E-02 2.A53E+00 -0.020 0.035 0.02A

8.0000 1 .9A3E+00 1 .391E-01 2.082E+00 A.030E+00 3.200E-02 2.652E+00 -0.019 0.033 0.023

9.0000 1 .956E+00 1 .601E-01 2.116E+00 A.506E+00 3.636E-02 2.831E+00 -0.018 0.031 0.021 10.0000 1 .968E+00 1 .81 AE-01 2. 1 A9E+00 A.975E+00 A.072E-02 2.992E+00 -0.018 0.030 0.020

12.5000 1 .993E+00 2.362E-01 2.230E+00 6.117E+00 5. 163E-02 3.3A1E+00 -0.016 0.027 0.019

15.0000 2.01 AE+00 2.926E-01 2.306E+00 7.21 9E+00 6.2A3E-02 3.633E+00 -0.015 0.025 0.017

17.5000 2.031E+00 3.501E-01 2.381E+00 8.286E+00 7.309E-02 3.885E+00 -0.01 A 0.02A 0.016

20.0000 2.0A6E+00 A.086E-01 2. A5AE+00 9.320E+00 8.355E-02 A. 107E+00 -0.013 0.022 0.015

25.0000 2.070E+00 5.277E-01 2.598E+00 1 .130E+01 1 .039E-01 A.A87E+00 -0.010 0.020 0.013

30.0000 2.089E+00 6.A89E-01 2.738E+00 1 .317E+01 1 .233E-01 A.806E+00 -0.009 0.018 0.011 35.0000 2. 1 05E+00 7.716E-01 2.876E+00 1 .A96E+01 1 .A18E-01 5.082E+00 -0.007 0.017 0.010

AO. 0000 2. 1 18E+00 8.955E-01 3.01 3E+00 1 .665E+01 1 .59AE-01 5.326E+00 -0.006 0.015 0.009

A5.0000 2. 129E+00 1 .021E+00 3.150E+00 1 .828E+01 1 .762E-01 5.5AAE+00 -0.005 0.01A 0.008

50.0000 2.139E+00 1 . 1 A6E+00 3.286E+00 1 .983E+01 1 .923E-01 5.7A1E+00 -O.OOA 0.01A 0.007

55.0000 2.1 A8E+00 1 .273E+00 3.A21E+00 2.1 32E+01 2.076E-01 5.921E+00 -O.OOA 0.013 0.006

60.0000 2.156E+00 1 . AOOE+00 3.556E+00 2.276E+01 2.222E-01 6.087E+00 -0.003 0.012 0.006

70.0000 2.170E+00 1 .656E+00 3.827E+00 2.5A7E+01 2.A96E-01 6.383E+00 -0.002 0.011 0.005

80.0000 2.182E+00 1 . 91 AE+00 A.096E+00 2.799E+01 2.7A7E-01 6.6A1E+00 -0.002 0.010 O.OOA

90.0000 2.1 93E+00 2.173E+00 A.366E+00 3.035E+01 2.978E-01 6 .871E+00 -0.002 0.009 0.003

100.0000 2.202E+00 2. A3AE+00 A.636E+00 3.258E+01 3.192E-01 7.077E+00 -0.001 0.009 0.003

125.0000 2.222E+00 3.089E+00 5.31 1E+00 3.761E+01 3.662E-01 7.516E+00 -0.001 0.008 0.002

1 50.0000 2.238E+00 3.7A9E+00 5.987E+00 A.20AE+01 A.060E-01 7.876E+00 -0.001 0.007 0.002

175.0000 2.251E+00 A.A12E+00 6.663E+00 A.600E+01 A.AOlE-01 8. 182E+00 -0.001 0.006 0.001 200.0000 2.263E+00 5.078E+00 7.3A1E+00 A.957E+01 A.698E-01 8. AA7E+00 -0.000 0.006 0.001 250.0000 2.282E+00 6 . A16E+00 8.698E+00 5.582E+01 5.190E-01 8.891E+00 -0.000 0.005 0.001 300.0000 2.297E+00 7.760E+00 1 .006E+01 6. 1 16E+01 5.58AE-01 9.25AE+00 -0.000 0.005 0.001 350.0000 2.311 E+00 9. 107E+00 1 .1A2E+01 6.583E+01 5.908E-01 9.561E+00 -0.000 0.005 0.001

AOO .0000 2.322E+00 1 . 0A6E+01 1 .278E+01 6 . 996E+01 6.180E-01 9.827E+00 -0.000 O.OOA 0.001 A50.0000 2.332E+00 1 . 181E+01 1 .A1 AE+01 7 . 368E+01 6.A12E-01 1 .006E+01 -0.000 O.OOA 0.000

500.0000 2.3A1E+00 1 .317E+01 1 . 551 E+01 7.705E+01 6.613E-01 1 .027E+01 -0.000 O.OOA 0.000

550.0000 2.3A9E+00 1 . A53E+01 1 .688E+01 8.01 AE+01 6 .789E-01 1 .0A6E+01 -0.000 O.OOA 0.000

600.0000 2.357E+00 1 .589E+01 1 .82AE+01 8.299E+01 6.9A5E-01 1 .06AE+01 -0.000 O.OOA 0.000

700.0000 2.370E+00 1 .861 E+01 2.098E+01 8.810E+01 7.209E-01 1 .09AE+01 -0.000 0.003 0.000

800.0000 2.381E+00 2.133E+01 2.371E+01 9.258E+01 7. A25E-01 1 . 121E+01 -0.000 0.003 0.000

900.0000 2.391E+00 2. A06E+01 2.6A5E+01 9.657E+01 7.605E-01 1 .1A5E+01 -0.000 0.003 0.000

1000.0000 2. AOOE+00 2.679E+01 2.91 9E+01 1 .002E+02 7.759E-01 1 . 166E+01 -0.000 0.003 0.000

151
ELECTRONS IN WATER, LIQUID OO

I = 75.0 eV DENSITY = 1 .OOOE+00 g/cm^

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^/g MeV cm^/g MeV cm^/g g/cm ^

0.0100 2.256E+01 3 .898E-03 2.257E+01 2.515E-0A 9.A08E-05 0.0 -0.199 0.227 0.225

0.0125 1 .897E+01 3.927E-03 1 .898E+01 3.728E-0A 1 .133E-0A 0.0 -0.190 0.217 0.215

0.0150 1 .6A7E+01 3. 9AAE-03 1 .6A7E+01 5.1A7E-0A 1 .316E-0A 0.0 -0.18A 0.208 0.207

0.0175 1 .A61E+01 3.955E-03 1 .A61E+01 6.761E-0A 1 . A92E-0A 0.0 -0.179 0.202 0.201 0.0200 1 .317E+01 3.963E-03 1 .318E+01 8.566E-0A 1 .663E-0A 0.0 -0.175 0.197 0.196 0.0250 1 . 109E+01 3.97AE-03 1 . 1 10E+01 1 .272E-03 1 . 990E-0A 0.0 -0.169 0.189 0.188

0.0300 9.653E+00 3. 98AE-03 9.657E+00 1 .756E-03 2.301E-0A 0.0 -0.16A 0.182 0.182

0 .0350 8.592E+00 3. 99AE-03 8.596E+00 2.306E-03 2.599E-0A 0.0 -0.160 0.177 0.177

0.0^00 7.777E+00 A.005E-03 7.781E+00 2.919E-03 2.886E-0A 0.0 -0.157 0.173 0.173

0 . 0<t50 7.130E+00 A.018E-03 7. 13AE+00 3.591 E-03 3.165E-0A 0.0 -0.1 5A 0.170 0.170

0.0500 6 .603E+00 A.031E-03 6 .607E+00 A.320E-03 3.A35E-0A 0.0 -0.152 0.167 0.167

0 .0550 6 . 1 66E+00 A.0A6E-O3 6 . 170E+00 5.103E-03 3.698E-0A 0.0 -0.150 0.165 0.16A

0.0600 5.797E+00 A.062E-03 5.801E+00 5.9A0E-03 3.955E-0A 0.0 -0.1 A8 0.162 0.162

0 . 0700 5.207E+00 A.098E-03 5.21 1E+00 7.762E-03 A. A52E-0A 0.0 -0.1 A5 0.158 0.158

0 .0800 A.757E+00 A. 1 38E-03 A.762E+00 9.773E-03 A.931E-0A 0.0 -0.1A2 0.155 0.155

0 .0900 A. A02E+00 A. 181E-03 A.A07E+00 1 . 1 96E-02 5.393E-0A 0.0 -0.1A0 0.153 0.152

0.1000 A.115E+00 A.228E-03 A.120E+00 1 .A31E-02 5.8A1E-0A 0.0 -0.138 0.150 0.150

0.1250 3.591 E+00 A.355E-03 3.596E+00 2.083E-02 6.912E-0A 0.0 -0.13A 0.1 A6 0.1A5

0 . 1 500 3.238E+00 A. A9AE-03 3.2A2E+00 2.817E-02 7.926E-0A 0.0 -0.131 0.1A2 0.1A2

0 . 1 750 2.98AE+00 A.6A3E-03 2.988E+00 3.622E-02 8.89AE-0A 0.0 -0.128 0.139 0.139

0.2000 2.793E+00 A.801E-03 2 .798E+00 A. A87E-02 9.826E-0A 0.0 -0.126 0.137 0.136

0.2500 2.528E+00 5.1A1E-03 2.533E+00 6.372E-02 1 .161E-03 0.0 -0.123 0.133 0.132

0 . 3000 2.355E+00 5.51 AE-03 2.360E+00 8.A21E-02 1 .331E-03 2.187E-03 -0.120 0.130 0.129

0.3500 2.233E+00 5.913E-03 2.239E+00 1 .060E-01 1 .A97E-03 1 .051E-02 -0.118 0.128 0.127

0 . AOOO 2.1A5E+00 6.339E-03 2.152E+00 1 .288E-01 1 .659E-03 2. 188E-02 -0.116 0.126 0.125

0 . A500 2.079E+00 6 .787E-03 2.086E+00 1 .52AE-01 1 .81 9E-03 3.663E-02 -0.11 A 0.12A 0.123

0.5000 2.028E+00 7.257E-03 2.035E+00 1 .767E-01 1 .978E-03 5. A2AE-02 -0.111 0.123 0.121 0.5500 1 . 988E+00 7.7A7E-03 1 .996E+00 2.015E-01 2.137E-03 7.393E-02 -0.09A 0.120 0.118

0.6000 1 .956E+00 8.25AE-03 1 .965E+00 2.268E-01 2.295E-03 9.538E-02 -0.088 0.117 0.11A

0 .7000 1 . 91 OE+00 9.312E-03 1 .919E+00 2.783E-01 2.61 AE-03 1 . A22E-01 -0.078 0.110 0.106 0.8000 1 .879E+00 1 .0A3E-02 1 .890E+00 3.308E-01 2. 935E-03 1 . 925E-01 -0.070 0.105 0.099

0.9000 1 .858E+00 1 .159E-02 1 .870E+00 3.8A1E-01 3.260E-03 2.AA8E-01 -0.06A 0.099 0.093

1 .0000 1 .8AAE+00 1 .280E-02 1 .857E+00 A.378E-01 3.588E-03 2. 983E-01 -0.059 0.095 0.087

1 .2500 1 .825E+00 1 .600E-02 1 .8A1E+00 5.731E-01 A.A28E-03 A.331E-01 -0 .0A9 0.085 0.075

1 .5000 1 .820E+00 1 . 9A2E-02 1 .839E+00 7.090E-01 5.293E-03 5.6A8E-01 -0.0A3 0.077 0.066

1 .7500 1 .821 E+00 2.303E-02 1 .8AAE+00 8.AA8E-01 6.183E-03 6.911E-01 -0.038 0.071 0.059

2.0000 1 .825E+00 2.678E-02 1 .851E+00 9.801E-01 7.09AE-03 8.119E-01 -0.035 0.066 0.053

2 . 5000 1 .837E+00 3. A68E-02 1 .871E+00 1 .2A9E+00 8.973E-03 1 .036E+00 -0.030 0.059 0.0A5

3.0000 1 .850E+00 A.299E-02 1 .893E+00 1 .51 AE+00 1 .091E-02 1 .238E+00 -0.027 0.05A O.OAO

3.5000 1 .86AE+00 5. 16AE-02 1 .916E+00 1 .777E+00 1 .290E-02 1 .A19E+00 -0.025 0.0A9 0.036

A. 0000 1 .877E+00 6.058E-02 1 .937E+00 2.037E+00 1 . A93E-02 1 .585E+00 -0.02A 0.0A6 0.033

A .5000 1 .889E+00 6 . 976E-02 1 .958E+00 2.293E+00 1 .698E-02 1 .738E+00 -0.023 0.0A3 0.031 5.0000 1 . 900E+00 7.917E-02 1 .979E+00 2.5A7E+00 1 .907E-02 1 .880E+00 -0.022 O.OAl 0.029

5.5000 1 .910E+00 8.876E-02 1 .999E+00 2.799E+00 2. 1 17E-02 2.01 lE+00 -0.021 0.039 0.027

6.0000 1.91 9E+00 9.85AE-02 2.018E+00 3.0A8E+00 2.329E-02 2.133E+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 0.02A

8.0000 1 . 951 E+00 1 .391E-01 2.090E+00 A.021E+00 3. 189E-02 2.555E+00 -0.019 0.033 0.023

9.0000 1 . 96AE+00 1 .601 E-01 2.12AE+00 A. A96E+00 3.623E-02 2.736E+00 -0.018 0.031 0.021 10.0000 1 . 976E+00 1 .81 AE-01 2.157E+00 A.963E+00 A.058E-02 2.900E+00 -0.018 0.030 0.020

12.5000 2.000E+00 2.362E-01 2.237E+00 6.101E+00 5. 1 A5E-02 3.257E+00 -0.016 0.027 0.019

15.0000 2.020E+00 2. 926E-01 2.313E+00 7.200E+00 6.222E-02 3.558E+00 -0.015 0.025 0.017

17.5000 2.037E+00 3.501E-01 2.387E+00 8.26AE+00 7.286E-02 3.81 9E+00 -0.01 A 0.02A 0.016

20.0000 2.051E+00 A.086E-01 2.A59E+00 9.295E+00 8.331E-02 A.050E+00 -0.013 0.022 0.015

25.0000 2.07AE+00 5.277E-01 2.601E+00 1 . 127E+01 1 .036E-01 A.AAAE+00 -0.010 0.020 0.013

30.0000 2.092E+00 6 . A89E-01 2.7A1 E+00 1 .31 AE+01 1 .230E-01 A.773E+00 -0.009 0.018 0.011 35.0000 2. 1 07E+00 7 .71 6E-01 2.878E+00 1 . A92E+01 1 .A15E-01 5.056E+00 -0.007 0.017 0.010

AO .0000 2.1 20E+00 8.955E-01 3.015E+00 1 .662E+01 1 .592E-01 5.305E+00 -0.006 0.015 0.009

A5.0000 2. 1 31 E+00 1 .021E+00 3. 151 E+00 1 .82AE+01 1 .760E-01 5.527E+00 -0.005 0.01A 0.008

50.0000 2.1A1E+00 1 . 1 A6E+00 3.287E+00 1 . 980E+01 1 . 920E-01 5.726E+00 -0 .OOA 0.01 A 0.007

55.0000 2. 1 A9E+00 1 .273E+00 3.A22E+00 2.129E+01 2.07AE-01 5.908E+00 -0 .OOA 0.013 0.006 60.0000 2.157E+00 1 . AOOE + 00 3.558E+00 2.272E+01 2.220E-01 6.07AE+00 -0.003 0.012 0.006

70.0000 2.171E+00 1 .656E+00 3.828E+00 2.5A3E+01 2. A9AE-01 6.372E+00 -0.002 0.011 0.005

80.0000 2. 183E+00 1 . 91 AE+00 A.097E+00 2.795E+01 2.7A5E-01 6.631E+00 -0.002 0.010 O.OOA

90.0000 2.1 9AE+00 2. 1 73E+00 A.367E+00 3.032E+01 2.976E-01 6.861E+00 -0.002 0.009 0.003

100.0000 2.203E+00 2.A3AE+00 A.637E+00 3.25AE+01 3.1 90E-01 7.067E+00 -0.001 0.009 0.003

125.0000 2.223E+00 3.089E+00 5.312E+00 3.757E+01 3.661E-01 7.505E+00 -0.001 0.008 0.002

1 50.0000 2.239E+00 3.7A9E+00 5.988E+00 A.200E+01 A.058E-01 7.86AE+00 -0.001 0.007 0.002

175.0000 2.252E+00 A.A12E+00 6.66AE+00 A.596E+01 A. AOOE-01 8.170E+00 -0.001 0.006 0.001 200.0000 2.26AE+00 5.078E+00 7.3A2E+00 A. 953E+01 A.696E-01 8.A3AE+00 -0.000 0.006 0.001 250.0000 2.283E+00 6.A16E+00 8.699E+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+01 6.1 12E+01 5.583E-01 9.2A3E+00 -0.000 0.005 0.001 350.0000 2.312E+00 9.107E+00 1 .1A2E + 01 6.578E+01 5. 907E-01 9.551E+00 -0.000 0.005 0.001

AOO .0000 2.323E+00 1 .0A6E+01 1 .278E+01 6 . 992E+01 6.179E-01 9.818E+00 -0.000 O.OOA 0.001

A50 .0000 2.333E+00 1 .181E+01 1 .A15E+01 7.36AE+01 6.A1 lE-01 1 .005E+01 -0.000 0 .OOA 0.000 500.0000 2. 3A2E+00 1 .317E+01 1 .551E+01 7.701E+01 6.612E-01 1 .027E+01 -0.000 O.OOA 0.000 550.0000 2.350E+00 1 . A53E+01 1 .688E+01 8.010E+01 6.788E-01 1 .0A6E+01 -0.000 O.OOA 0.000 600.0000 2.357E+00 1 .589E+01 1 .82AE+01 8.295E+01 6.9AAE-01 1 .063E+01 -0.000 O.OOA 0.000 700.0000 2.370E+00 1 .861 E+01 2.098E+01 8.806E+01 7.208E-01 1 .09AE+01 -0.000 0.003 0.000 800.0000 2. 382E+00 2.1 33E+01 2.371E+01 9.25AE+01 7. A2AE-01 1 . 121E+01 -0.000 0.003 0.000 900.0000 2.392E+00 2. A06E+01 2.6A5E+01 9.653E+01 7.605E-01 1 . 1 A5E+01 -0.000 0.003 0.000 1000.0000 2. AOOE+00 2.679E+01 2.91 9E+01 1 .001E+02 7.758E-01 1 .166E+01 -0.000 0.003 0.000

* Evaluated with the density-effect correction of Ashley (1982b).

152
ELECTRONS IN WATER VAPOR

I = 71.6 eV DENSITY = 7.562E-0A g/cm® (20® C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. dClog1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MoV MeV cm®/g MoV cm^/g MoV cm^/g g/cm®

0.0100 2.277E+01 3.898E-03 2.277E+01 2.189E-01 9.31 IE-05 0.0 -0.197 0.225 0.223

0.0125 1 .911E+01 3.927E-03 1 .911E + 01 3.691E-01 1 .121E-01 0.0 -0.189 0.211 0.213

0.0150 1 .661E+01 3. 911E-03 1 .661E+01 5.097E-01 1 .303E-01 0.0 -0.183 0.206 0.205

0.0175 1 .173E+01 3.955E-03 1 .171E+01 6.699E-01 1 .179E-01 0.0 -0.178 0.200 0.199

0.0200 1 .328E+01 3. 963E-03 1 .329E+01 8.188E-01 1 .618E-01 0.0 -0.171 0.195 0.191

0.0250 1 . 1 18E+01 3.971E-03 1.11 9E+01 1 .261E-03 1 .973E-01 0.0 -0.167 0.187 0.186

0.0300 9.726E+00 3. 981E-03 9.730E+00 1 .712E-03 2.282E-01 0.0 -0.163 0.181 0.180

0.0350 8.656E+00 3.991E-03 8.660E+00 2.287E-03 2.578E-01 0.0 -0.159 0.176 0.175

O.OAOO 7.831E+00 1.005E-03 7.838E+00 2.895E-03 2.863E-01 0.0 -0.156 0.172 0.172

0.0A50 7. 181E+00 1.018E-03 7.185E+00 3.563E-03 3. 110E-01 0.0 -0.153 0.169 0.168

0.0500 6.650E+00 1.031E-03 6.651E+00 1.286E-03 3.109E-01 0.0 -0.151 0.166 0.165

0.0550 6.209E+00 1.016E-03 6.213E+00 5.065E-03 3.670E-01 0.0 -0.119 0.163 0.163

0.0600 5.836E+00 1.062E-03 5.811E+00 5.895E-03 3.926E-01 0.0 -0.117 0.161 0.161 0.0700 5.212E+00 1.098E-03 5.216E+00 7.706E-03 1.120E-01 0.0 -0.111 0.157 0.157

0.0800 1.789E+00 1.138E-03 1.793E+00 9.703E-03 1.896E-01 0.0 -0.111 0.151 0.151

0.0900 1.131E+00 1. 181E-03 1.135E+00 1 .187E-02 5.355E-01 0.0 -0.139 0.152 0.151 0.1000 1. 112E+00 1.228E-03 1.116E+00 1 .121E-02 5.801E-01 0.0 -0.137 0.119 0.119

0.1250 3.611E+00 1.355E-03 3.618E+00 2.069E-02 6.866E-01 0.0 -0.133 0.115 0.111

0.1500 3.257E+00 1.191E-03 3.262E+00 2.799E-02 7.871E-01 0.0 -0.130 0.111 0.111 0.1750 3.001E+00 1.613E-03 3.006E+00 3.598E-02 8.837E-01 0.0 -0.128 0.138 0.138

0.2000 2.809E+00 1.801E-03 2.811E+00 1.159E-02 9.765E-01 0.0 -0.126 0.136 0.136

0.2500 2.512E+00 5.111E-03 2.518E+00 6.333E-02 1 .151E-03 0.0 -0.122 0.132 0.132

0.3000 2.368E+00 5.511E-03 2.371E+00 8.370E-02 1 .323E-03 0.0 -0.119 0.130 0.129

0.3500 2.217E+00 5.913E-03 2.253E+00 1 .051E-01 1 .188E-03 0.0 -0.117 0.127 0.126

O.AOOO 2. 159E+00 6.339E-03 2.166E+00 1 .280E-01 1 .619E-03 0.0 -0.115 0.125 0.121

0.1500 2.091E+00 6 .787E-03 2.101E+00 1 .515E-01 1 .808E-03 0.0 -0.111 0.123 0.122

0.5000 2.015E+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 .717E-03 2.011E+00 2.002E-01 2.122E-03 0.0 -0.111 0.121 0.119

0.6000 1 .977E+00 8.251E-03 1 .985E+00 2.252E-01 2.279E-03 0.0 -0.109 0.119 0.118

0.7000 1 .931E+00 9.312E-03 1 .911E+00 2.761E-01 2.592E-03 0.0 -0.107 0.117 0.115

0.8000 1 .908E+00 1 .013E-02 1 .918E+00 3.279E-01 2.907E-03 0.0 -0.105 0.115 0.113

0.9000 1 .891E+00 1 .159E-02 1 .903E+00 3.803E-01 3.221E-03 0.0 -0.101 0.111 0.111

1 .0000 1 .881E+00 1 .280E-02 1 .891E+00 1.330E-01 3.511E-03 0.0 -0.102 0.112 0.110

1 .2500 1 .871E+00 1 .600E-02 1 .890E+00 5.652E-01 1.356E-03 0.0 -0.099 0.110 0.106

1 .5000 1 .880E+00 1 .912E-02 1 .899E+00 6.972E-01 5.187E-03 0.0 -0.097 0.107 0.101

1 .7500 1 .891E+00 2.303E-02 1 .911E+00 8.281E-01 6.036E-03 0.0 -0.095 0.105 0.101 2.0000 1 . 905E+00 2.678E-02 1 .932E+00 9.581E-01 6.899E-03 0.0 -0.093 0.101 0.099

2.5000 1 .936E+00 3.168E-02 1 .970E+00 1 .215E+00 8.665E-03 0.0 -0.091 0.101 0.096

3.0000 1 .966E+00 1.299E-02 2.009E+00 1 .166E+00 1 .017E-02 0.0 -0.089 0.099 0.091

3.5000 1 .995E+00 5.161E-02 2.017E+00 1 .713E+00 1 .230E-02 0.0 -0.087 0.097 0.091 1.0000 2.022E+00 6.058E-02 2.082E+00 1 .955E+00 1 .116E-02 0.0 -0.086 0.095 0.090

1.5000 2.016E+00 6.976E-02 2.1 16E+00 2.1 93E+00 1 .601E-02 0.0 -0.081 0.091 0.088

5.0000 2.069E+00 7.917E-02 2.118E+00 2.127E+00 1 .792E-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 2.110E+00 9.851E-02 2.209E+00 2.886E+00 2. 172E-02 0.0 -0.081 0.090 0.081

7.0000 2. 116E+00 1 . 185E-01 2.265E+00 3.333E+00 2.555E-02 0.0 -0.080 0.089 0.082

8.0000 2. 178E+00 1 .391E-01 2.317E+00 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 1.197E+00 3.321E-02 0.0 -0.078 0.086 0.079

10.0000 2.232E+00 1 .811E-01 2.11 3E+00 1.616E+00 3.703E-02 0.0 -0.077 0.081 0.077

12.5000 2.286E+00 2.362E-01 2.523E+00 5.628E+00 1.652E-02 0.0 -0.075 0.082 0.071

15.0000 2.332E+00 2.926E-01 2.621E+00 6.600E+00 5.587E-02 0.0 -0.073 0.079 0.072

17.5000 2.370E+00 3.501E-01 2.721E+00 7.535E+00 6.505E-02 0.0 -0.072 0.077 0.070

20.0000 2.101E+00 1.086E-01 2.813E+00 8.139E+00 7.105E-02 0.0 -0.071 0.076 0.068

25.0000 2.160E+00 5.277E-01 2.988E+00 1 .016E+01 9.117E-02 0.0 -0.069 0.073 0.065

30.0000 2.507E+00 6 .189E-01 3.155E+00 1 .179E+01 1 .081E-01 0.0 -0.068 0.071 0.062

35.0000 2.511E+00 7.716E-01 3.316E+00 1 .331E+01 1 .210E-01 1 .181E-02 -0.058 0.068 0.059

10.0000 2.571E+00 8. 955E-01 3.169E+00 1 .181E+01 1 .392E-01 6.811E-02 -0.019 0.065 0.055

15.0000 2.598E+00 1 .021E+00 3.618E+00 1 .622E+01 1 .537E-01 1 .111E-01 -0.012 0.063 0.051 50.0000 2.617E+00 1 . 116E+00 3.761E+00 1 .758E+01 1 .677E-01 2.212E-01 -0.037 0.060 0.017

55.0000 2.631E+00 1 .273E+00 3. 907E+00 1 .888E+01 1 .81 IE-01 3.108E-01 -0.033 0.057 0.013

60.0000 2.619E+00 1 .100E+00 1.019E+00 2.011E+01 1 .910E-01 3.981E-01 -0.030 0.055 0.010

70.0000 2.671E+00 1 .656E+00 1.330E+00 2.252E+01 2. 181E-01 5.703E-01 -0.026 0.051 0.035

80.0000 2.691E+00 1 .911E + 00 1.608E+00 2.176E+01 2.110E-01 7.335E-01 -0.023 0.018 0.031 90.0000 2.71 1E+00 2.173E+00 1.881E+00 2.687E+01 2.620E-01 8.863E-01 -0.021 0.015 0.027

100.0000 2.726E+00 2.131E+00 5.159E+00 2.886E+01 2.817E-01 1 .029E+00 -0.019 0.013 0.025

125.0000 2.756E+00 3.089E+00 5.815E+00 3.311E+01 3.256E-01 1 .315E+00 -0.017 0.038 0.020

1 50.0000 2.779E+00 3.719E+00 6.528E+00 3.716E+01 3.631E-01 1 .611E+00 -0.015 0.035 0.017

175.0000 2.799E+00 1.112E+00 7.21 1E+00 1. 1 10E+01 3.963E-01 1 .818E+00 -0.011 0.032 0.011

200.0000 2.815E+00 5.078E+00 7.891E+00 1.111E+01 1.252E-01 2.053E+00 -0.011 0.030 0.013

250.0000 2.813E+00 6.116E+00 9.258E+00 5.025E+01 1.711E-01 2.102E+00 -0.013 0.027 0.010

300.0000 2.865E+00 7 .760E+00 1 .062E+01 5.529E+01 5.138E-01 2.692E+00 -0.012 0.025 0.009

350.0000 2.883E+00 9. 107E+00 1 . 1 99E+01 5.972E+01 5.169E-01 2.939E+00 -0.011 0.023 0.008

100.0000 2.899E+00 1 .016E+01 1 . 336E+01 6.367E+01 5.750E-01 3.156E+00 -0.011 0.022 0.007

150.0000 2. 912E+00 1 . 181 E+01 1 .173E+01 6.723E+01 5.992E-01 3.318E+00 -0.011 0.021 0.006

500.0000 2. 921E+00 1 .317E+01 1 .609E+01 7.018E+01 6 .203E-01 3.522E+00 -0.010 0.020 0.006

550.0000 2.935E+00 1 .153E+01 1 .716E+01 7.316E+01 6.390E-01 3.681E+00 -0.010 0.020 0.005

600.0000 2.915E+00 1 .589E+01 1 .883E+01 7.622E+01 6.555E-01 3.827E+00 -0.009 0.019 0.005

700.0000 2.962E+00 1 .861 E+01 2. 157E+01 8.1 17E+01 6.838E-01 1.088E+00 -0.008 0.018 0.001

800.0000 2. 977E+00 2.1 33E+01 2.131E+01 8.551E+01 7.072E-01 1.318E+00 -0.008 0.017 0.001

900.0000 2. 989E+00 2.106E+01 2.705E+01 8.911E+01 7.268E-01 1.521E+00 -0.007 0.016 0.003

1000.0000 3.000E+00 2.679E+01 2.979E+01 9.296E+01 7.135E-01 1.71 1E+00 -0.006 0.016 0.003

153
POSITRONS IN CARBON (GRAPHITE)

I = 78.0 eV DENSITY = 2.265E+00 g/cm^

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^/g MeV cm^/g MeV cm^/g g/cm 2 0.0100 2.21 9E+01 3.150E-03 2.21 9E+01 2.520E-09 7.799E-05 0.0 -0.182 0.209 0.203

0.0125 1 .857E+01 3.161E-03 1 .857E+01 3.757E-09 9. 323E-05 0.0 -0.175 0.196 0.195

0.0150 1 .605E+01 3.1 68E-03 1 .605E+01 5.210E-09 1 .083E-09 0.0 -0.170 0.189 0.188

0.0175 1 .91 9E+01 3. 172E-03 1 .920E+01 6 .869E-09 1 .229E-09 0.0 -0.166 0.189 0.183

0.0200 1 .276E+01 3. 176E-03 1 .276E+01 8.730E-09 1 .371E-09 0.0 -0.163 0.180 0.179

0.0250 1 .069E+01 3. 189E-03 1 .070E+01 1 .303E-03 1 .699E-09 0.0 -0.158 0.173 0.173

0.0300 9.266E+00 3.1 99E-03 9.269E+00 1 .807E-03 1 . 905E-09 0.0 -0.159 0.168 0.168

0.0350 8.218E+00 3.209E-03 8.221 E+00 2.381E-03 2. 158E-09 0.0 -0.151 0.169 0.169

0 .OAOO 7.919E+00 3.215E-03 7.917E+00 3.022E-03 2.903E-09 0.0 -0.198 0.161 0.161 0.0A50 6 .777E+00 3.228E-03 6.781E+00 3.728E-03 2.691E-09 0.0 -0.196 0.158 0.158

0.0500 6 .260E+00 3.291E-03 6.263E+00 9.996E-03 2.879E-09 0.0 -0.199 0.156 0.156

0.0550 5.831E+00 3.255E-03 5.839E+00 5.329E-03 3. 101E-09 0.0 -0.192 0.159 0.159

0.0600 5.969E+00 3.270E-03 5.973E+00 6.209E-03 3.329E-09 0.0 -0.191 0.152 0.152

0 .0700 9 .893E+00 3. 303E-03 9.896E+00 8.196E-03 3.758E-09 0.0 -0.139 0.199 0.199

0.0800 9 .953E+00 3.337E-03 9.956E+00 1 .029E-02 9. 179E-09 0.0 -0.137 0.197 0.197

0.0900 9. 107E+00 3.375E-03 9.1 lOE+00 1 .263E-02 9.587E-09 0.0 -0.135 0.195 0.199

0 . 1000 3.827E+00 3.919E-03 3.830E+00 1 .515E-02 9.985E-09 0.0 -0.133 0.193 0.193

0.1250 3. 31 7E+00 3.523E-03 3.320E+00 2.21 9E-02 5. 992E-09 0.0 -0.131 0.139 0.139

0 . 1 500 2 . 973E+00 3.690E-03 2. 977E+00 3.017E-02 6 .855E-09 0.0 -0.128 0.137 0.136

0.1750 2.725E+00 3.769E-03 2.730E+00 3.895E-02 7.735E-09 0.0 -0.127 0.135 0.139

0.2000 2.591E+00 3.896E-03 2.595E+00 9.895E-02 8.587E-09 0.0 -0.123 0.133 0.132

0.2500 2.280E+00 9.179E-03 2.289E+00 6.926E-02 1 .023E-03 3.996E-02 -0.097 0.129 0.123

0 . 3000 2. 107E+00 9.989E-03 2.111E+00 9.209E-02 1 . 182E-03 7.681E-02 -0.089 0.116 0.119

0.3500 1 . 986E+00 9.820E-03 1 . 990E+00 1 .165E-01 1 .338E-03 1 .205E-01 -0.089 0.110 0.108

0 .9000 1 .897E+00 5. 173E-03 1 . 902E+00 1 .922E-01 1 .992E-03 1 .650E-01 -0.079 0.105 0.102

0.9500 1 .830E+00 5.595E-03 1 .836E+00 1 .690E-01 1 .695E-03 2.097E-01 -0.075 0.100 0.097

0.5000 1 .778E+00 5.935E-03 1 .789E+00 1 .967E-01 1 .798E-03 2.593E-01 -0.072 0.096 0.093

0.5500 1 .738E+00 6.390E-03 1 .799E+00 2.250E-01 1 . 951E-03 2.986E-01 -0.069 0.093 0.089

0.6000 1 .705E+00 6 .759E-03 1 .712E+00 2.590E-01 2.109E-03 3.929E-01 -0.066 0.090 0.086

0 .7000 1 .657E+00 7.637E-03 1 .665E+00 3.133E-01 2.91 3E-03 9.282E-01 -0.062 0.085 0.080

0.8000 1 .629E+00 8.559E-03 1 .633E+00 3.790E-01 2.726E-03 5.1 1 IE-01 -0.059 0.081 0.076

0 . 9000 1 .602E+00 9.523E-03 1 .61 lE+00 9.356E-01 3.092E-03 5.909E-01 -0.056 0.078 0.072

1 .0000 1 .586E+00 1 .053E-02 1 .596E+00 9.980E-01 3.363E-03 6.675E-01 -0.059 0.075 0.069

1 .2500 1 .563E+00 1 .318E-02 1 .576E+00 6.558E-01 9. 185E-03 8.958E-01 -0.050 0.069 0.063

1 .5000 1 .555E+00 1 .602E-02 1 .571E+00 8. 197E-01 5.033E-03 1 .007E+00 -0.097 0.065 0.058

1 .7500 1 .553E+00 1 .901E-02 1 .572E+00 9.739E-01 5.906E-03 1 .153E+00 -0.095 0.062 0.055

2.0000 1 .555E+00 2.21 3E-02 1 .577E+00 1 .133E+00 6.800E-03 1 .287E+00 -0.093 0.059 0.052

2.5000 1 .569E+00 2.870E-02 1 .593E+00 1 .998E+00 8.693E-03 1 .529E+00 -0.090 0.055 0.098

3.0000 1 .575E+00 3.561E-02 1 .61 lE+00 1 .760E+00 1 .055E-02 1 .730E+00 -0.038 0.052 0.095

3.5000 1 .587E+00 9.281 E-02 1 .630E+00 2.069E+00 1 .299E-02 1 .913E+00 -0.036 0.050 0.092

9.0000 1 . 598E+00 5.026E-02 1 .699E+00 2.379E+00 1 .998E-02 2.077E+00 -0.039 0.098 0.090

9.5000 1 .609E+00 5.792E-02 1 .667E+00 2.675E+00 1 .699E-02 2.226E+00 -0.032 0.096 0.038

5.0000 1 .61 9E+00 6 .576E-02 1 .685E+00 2.979E+00 1 .853E-02 2.369E+00 -0.031 0.099 0.037

5.5000 1 .628E+00 7.378E-02 1 .702E+00 3.269E+00 2.059E-02 2.992E+00 -0.029 0.093 0.035

6.0000 1 .637E+00 8.1 93E-02 1 .71 9E+00 3.561E+00 2.267E-02 2.612E+00 -0.028 0.092 0.039

7.0000 1 .652E+00 9.865E-02 1 .751E+00 9.138E+00 2.686E-02 2.831E+00 -0.025 0.039 0.031 8.0000 1 .665E+00 1 .158E-01 1 .781E+00 9.709E+00 3. 109E-02 3.029E+00 -0.022 0.037 0.029

9.0000 1 .677E+00 1 .339E-01 1 .810E+00 5.261E+00 3.539E-02 3.210E+00 -0.019 0.035 0.027

1 0 .0000 1 .687E+00 1 .513E-01 1 .838E+00 5.809E+00 3.960E-02 3.377E+00 -0.017 0.039 0.025

12.5000 1 .708E+00 1 .971E-01 1 .905E+00 7.195E+00 5.027E-02 3.795E+00 -0.013 0.030 0.021 15.0000 1 .725E+00 2.999E-01 1 .969E+00 8.935E+00 6.087E-02 9.059E+00 -0.010 0.027 0.017

17.5000 1 .738E+00 2.927E-01 2.031E+00 9.686E+00 7.139E-02 9.339E+00 -0.008 0.029 0.015

20.0000 1 .750E+00 3.917E-01 2.091E+00 1 .090E+01 8. 165E-02 9.577E+00 -0.006 0.022 0.013

25.0000 1 .768E+00 9.917E-01 2.210E+00 1 .322E+01 1 .017E-01 9.993E+00 -0.009 0.019 0.010

30 .0000 1 .783E+00 5.935E-01 2.327E+00 1 .593E+01 1 .209E-01 5.339E+00 -0.003 0.017 0.008

35.0000 1 .796E+00 6.966E-01 2.992E+00 1 .753E+01 1 .393E-01 5.636E+00 -0.002 0.015 0.006

90.0000 1 .806E+00 7.508E-01 2.557E+00 1 .953E+01 1 .568E-01 5.899E+00 -0.002 0.019 0.005

95.0000 1 .816E+00 8.559E-01 2.672E+00 2. 199E+01 1 .735E-01 6 . 129E+00 -0.001 0.012 0.009

50.0000 1 .829E+00 9.617E-01 2.786E+00 2.327E+01 1 .899E-01 6.330E+00 -0.001 0.012 0.009

55.0000 1 .832E+00 1 .068E+00 2. 900E+00 2.503E+01 2.096E-01 6.517E+00 -0.001 0.011 0.003

60.0000 1 .838E+00 1 . 1 75E+00 3.019E+00 2.672E+01 2.1 92E-01 6.688E+00 -0.001 0.010 0.003

70.0000 1 .850E+00 1 .391E+00 3.291E+00 2.992E+01 2.965E-01 6 .992E+00 -0.001 0.009 0.002

80.0000 1 .861E+00 1 .608E+00 3.969E+00 3.290E+01 2.715E-01 7.256E+00 -0.001 0.008 0.002

90.0000 1 .870E+00 1 .826E + 00 3.696E+00 3.569E+01 2.996E-01 7.989E+00 -0.000 0.008 0.002

100.0000 1 .878E+00 2.096E+00 3. 929E+00 3.832E+01 3. 159E-01 7.698E+00 -0.000 0.007 0.001 125.0000 1 .895E+00 2.598E+00 9.999E+00 9.927E+01 3.629E-01 8.191E+00 -0.000 0.006 0.001 150.0000 1 . 91 OE+00 3 . 1 55E+00 5.069E+00 9.951E+01 9.027E-01 8.509E+00 -0.000 0.006 0.001 175.0000 1 . 921 E+00 3.719E+00 5.636E+00 5.918E+01 9.368E-01 8.81 1E+00 -0.000 0 .005 0.001 200.0000 1 .932E+00 9.276E+00 6.208E+00 5.891E+01 9.665E-01 9.077E+00 -0.000 0.005 0.001 250.0000 1 . 999E+00 5.905E+00 7.359E+00 6.580E+01 5.158E-01 9.522E+00 -0.000 0.009 0.000

300.0000 1 .963E+00 6.590E+00 8.503E+00 7.212E+01 5.553E-01 9.886E+00 -0.000 0.009 0.000

350.0000 1 -975E+00 7.678E+00 9.653E+00 7.763E+01 5.878E-01 1 .01 9E+01 -0.000 0.009 0.000

900.0000 1 . 985E+00 8.820E+00 1 .080E+01 8.253E+01 6.151E-01 1 .096E+01 -0.000 0.003 0.000

950.0000 1 . 999E+00 9. 969E + 00 1 . 1 96E+01 8.692E+01 6.385E-01 1 .070E+01 -0.000 0.003 0.000

500.0000 2.002E+00 1.111 E+01 1 .31 lE+01 9.091E+01 6 .587E-01 1 .091E+01 -0.000 0.003 0.000

550.0000 2.009E+00 1 .226E+01 1 .927E+01 9.957E+01 6 .769E-01 1 . 1 10E+01 -0.000 0.003 0.000

600.0000 2.016E+00 1 . 390E+01 1 .592E+01 9.799E+01 6.920E-01 1 .127E+01 -0.000 0.003 0.000

700.0000 2.028E+00 1 .570E+01 1 .773E+01 1 .090E+02 7. 186E-01 1 . 1 58E+01 -0.000 0.003 0.000

800.0000 2.038E+00 1 .801 E+01 2.005E+01 1 .093E+02 7.903E-01 1 .185E+01 -0.000 0.003 0.000

900.0000 2.097E+00 2.031E+01 2.236E+01 1 . 190E+02 7.589E-01 1 .208E+01 -0.000 0.002 0.000 1000.0000 2.055E+00 2.262E+01 2.968E+01 1 . 183E+02 7.739E-01 1 .229E+01 -0.000 0.002 0.000

154
POSITRONS IN CARBON (GRAPHITE)

I = 78.0 eV DENSITY = 1 .700E+001 g/cm

ENERGY STOPPING POWER CSDA RADIATION DEMS.EFF. ddog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MoV cmVg MeV cm^/g MeV cm^/g g/cm ^

0.0100 2.21 9E+01 3.150E-03 2.21 9E+01 2.520E-0A 7.750E-05 1 .920E-03 -0.182 0.20A 0.203

0.0125 1 .856E+01 3.161E-03 1 .857E+01 3.758E-0A 9.32AE-05 2.A81E-03 -0.175 0.195 0 . 1 9A 0.0150 1 .605E+01 3.168E-03 1 .605E+01 5.21 lE-OA 1 .083E-0A 3.073E-03 -0.170 0.189 0.188

0.0175 1 .A1 9E+01 3. 172E-03 1 .A19E+01 6.871E-0A 1 .229E-0A 3.695E-03 -0.165 0.18A 0.183

0.0200 1 .276E+01 3.176E-03 1 .276E+01 8.732E-0A 1 .371E-0A A.3A7E-03 -0.162 0.179 0.179

0.0250 1 .069E+01 3. 18AE-03 1 .069E+01 1 .303E-03 1 .6AAE-0A 5.736E-03 -0.157 0.173 0.172

0.0300 9.260E+00 3.1 9AE-03 9.26AE+00 1 .807E-03 1 . 906E-0A 7.236E-03 -0.153 0.168 0.167

0.0350 8.212E+00 3.20AE-03 8.215E+00 2.382E-03 2. 159E-0A 8.8A3E-03 -0.1A9 0.16A 0.163

O.OAOO 7. A08E+00 3.215E-03 7.A12E+00 3.02AE-03 2. AOAE-OA 1 .055E-02 -0.1 A7 0.160 0.160

0.0‘*50 6.771E+00 3.228E-03 6.775E+00 3.730E-03 2.6A2E-0A 1 .236E-02 -0.1 AA 0.157 0.157

0.0500 6.25AE+00 3.2A1 E-03 6.257E+00 A. A99E-03 2.875E-0A 1 . A25E-02 -0.1A2 0.155 0.155

0.0550 5.82AE+00 3.255E-03 5.828E+00 5.328E-03 3. 103E-0A 1 .62AE-02 -0.1A1 0.153 0.153

0.0600 5.A62E+00 3.270E-03 5.A65E+00 6.21 AE-03 3.327E-0A 1 .832E-02 -0.139 0.151 0.151 0.0700 A.885E+00 3.303E-03 A.888E+00 8. 153E-03 3.762E-0A 2.271E-02 -0.136 0. 1 A8 0.1 A8 0.0300 A.AA5E+00 3.337E-03 A. AA8E+00 1 .030E-02 A. 183E-0A 2.7A0E-02 -0.1 3A 0.1A5 0.1A5

0.0900 A.098E+00 3.375E-03 A.lOlE+00 1 .265E-02 A.593E-0A 3.237E-02 -0.132 0 . 1 A3 0.1A3

0.1000 3.817E+00 3.A1 AE-03 3.820E+00 1 .517E-02 A.992E-0A 3.760E-02 -0.130 0.1A1 0.1 A1 0.1250 3.306E+00 3.523E-03 3.309E+00 2.22AE-02 5.953E-0A 5. 166E-02 -0.126 0.137 0.136

0.1500 2.960E+00 3.6A0E-03 2.96AE+00 3.02AE-02 6.872E-0A 6.69AE-02 -0.123 0. 13A 0.133

0.1750 2.712E+00 3.76AE-03 2.716E+00 3.907E-02 7.758E-0A 8.320E-02 -0.121 0.131 0.130

0.2000 2.525E+00 3.896E-03 2.529E+00 A.862E-02 8.618E-0A 1 .003E-01 -0.118 0.129 0.128

0.2500 2.265E+00 A.179E-03 2.270E+00 6.957E-02 1 .028E-03 1 .363E-01 -0.11 A 0.125 0.12A

0.3000 2.09AE+00 A. A89E-03 2.099E+00 9.253E-02 1 . 188E-03 1 .7A0E-01 -0.110 0.121 0.120

0.3500 1 .975E+00 A.820E-03 1 .979E+00 1 . 171E-01 1 .3A5E-03 2. 129E-01 -0.106 0.118 0.117

O.AOOO 1 .887E+00 5. 173E-03 1 .892E+00 1 . A30E-01 1 .500E-03 2.52AE-01 -0.102 0.116 0.11A

0.A500 1 .821 E+00 5.5A5E-03 1 .827E+00 1 .699E-01 1 .65AE-03 2.922E-01 -0.099 0.113 0.112

0.5000 1 .770E+00 5. 935E-03 1 .776E+00 1 . 976E-01 1 .807E-03 3.321E-01 -0.096 0.111 0.109

0.5500 1 .730E+00 6.3A0E-03 1 .737E+00 2.261E-01 1 .961E-03 3.71 9E-01 -0.09A 0.109 0.107

0.6000 1 .698E+00 6.759E-03 1 .705E+00 2.552E-01 2.11AE-03 A.11AE-01 -0.091 0.107 0.105

0.7000 1 .651E+00 7.637E-03 1 .659E+00 3.1A7E-01 2. A2AE-03 A.891E-01 -0.086 0.10A 0.100

0.8000 1 .619E+00 8.559E-03 1 .628E+00 3.756E-01 2.737E-03 5.6A8E-01 -0.082 0.100 0.097

0.9000 1 .597E+00 9.523E-03 1 .607E+00 A.37AE-01 3.05AE-03 6.382E-01 -0.079 0.0 98 0.093

1 .0000 1 .582E+00 1 .053E-02 1 .592E+00 5.000E-01 3.376E-03 7.091E-01 -0.076 0.095 0.090

1 .2500 1 .561E+00 1 -318E-02 1 .57AE+00 6.580E-01 A.198E-03 8.756E-01 -0.070 0.090 0.08A

1 . 5000 1 .553E+00 1 .602E-02 1 .569E+00 8. 172E-01 5.0A6E-03 1 .028E+00 -0.066 0.085 0.079

1 .7500 1 .552E+00 1 .901E-02 1 .571E+00 9.765E-01 5.918E-03 1 .167E+00 -0.063 0.082 0.075

2.0000 1 .555E+00 2.213E-02 1 .577E+00 1 .135E+00 6.812E-03 1 .295E+00 -0.060 0.079 0.071 2.5000 1 .56AE+00 2.870E-02 1 .593E+00 1 .A51E+00 8.653E-03 1 .522E+00 -0.056 0.07A 0.066

3.0000 1 .576E+00 3.561E-02 1 .612E+00 1 .763E+00 1 .055E-02 1 .720E+00 -0.05A 0.070 0.062

3.5000 1 .589E+00 A.281E-02 1 .631E+00 2.071E+00 1 .250E-02 1 .89AE+00 -0.051 0.068 0.059

A. 0000 1 .600E+00 5.026E-02 1 .651E+00 2.376E+00 1 .AA8E-02 2.051E+00 -0.050 0.065 0.057

A. 5000 1 .612E+00 5.792E-02 1 .670E+00 2.677E+00 1 .6A9E-02 2.1 93E+00 -O.OA8 0.063 0.055

5.0000 1 .622E+00 6.576E-02 1 .688E+00 2.975E+00 1 .852E-02 2.323E+00 -0.0A6 0.061 0.053

5.5000 1 .632E+00 7.378E-02 1 .706E+00 3.270E+00 2.057E-02 2.AA3E+00 -O.OA5 0.060 0.051 6.0000 1 .6A1E+00 8.1 93E-02 1 .723E+00 3.561E+00 2.26AE-02 2.555E+00 -O.OAA 0.058 0.050

7.0000 1 .658E+00 9.865E-02 1 .756E+00 A.136E+00 2.682E-02 2.758E+00 -0.0A1 0.056 0.0A7

8.0000 1 .672E+00 1 . 158E-01 1 .788E+00 A.700E+00 3. 102E-02 2.939E+00 -0.038 0.05A 0.0A5

9.0000 1 .685E+00 1 .33AE-01 1 .818E+00 5.255E+00 3.525E-02 3.10AE+00 -0.036 0.052 0.0A2

10.0000 1 .696E+00 1 .513E-01 1 .8A7E+00 5.800E+00 3.9A9E-02 3.256E+00 -0.033 0.050 O.OAO

12.5000 1 .720E+00 1 .971E-01 1 .917E+00 7.129E+00 5.007E-02 3.591E+00 -0.028 0.0A6 0.036

15.0000 1 .738E+00 2.AAAE-01 1 .983E+00 8.A1 lE+00 6.058E-02 3.879E+00 -0.023 0.0A2 0.031 17.5000 1 .75AE+00 2.927E-01 2.0A6E+00 9.652E+00 7.095E-02 A.133E+00 -0.019 0.039 0.028

20.0000 1 .766E+00 3.A17E-01 2.108E+00 1 .086E+01 8.116E-02 A.361E+00 -0.016 0.036 0.025

25.0000 1 .787E+00 A. A17E-01 2.228E+00 1 .316E+01 1 .OlOE-01 A.755E+00 -0.011 0.032 0.020

30.0000 1 .803E+00 5. A35E-01 2.3A6E+00 1 .535E+01 1 .200E-01 5.088E+00 -0.008 0.028 0.016

35.0000 1 .81 6E+00 6.A66E-01 2.A62E+00 1 .7A3E+01 1 .382E-01 5.376E+00 -0.006 0.026 0.013

AO .0000 1 .827E+00 7.508E-01 2.578E+00 1 . 9A1E+01 1 .556E-01 5.628E+00 -0.005 0.023 0.011 A5.0000 1 .837E+00 8.559E-01 2.692E+00 2.131E+01 1 .722E-01 5.85AE+00 -O.OOA 0.022 0.010

50.0000 1 .8A5E+00 9.617E-01 2.807E+00 2.313E+01 1 .880E-01 6.057E+00 -0.003 0.020 0.008

55.0000 1 .853E+00 1 .068E+00 2.921E+00 2. A88E+01 2.031E-01 6.2A1E+00 -0.003 0.019 0.007

60.0000 1 .860E+00 1 .175E+00 3.035E+00 2.655E+01 2. 176E-01 6.A11E+00 -0.002 0.018 0.006

70.0000 1 .872E+00 1 . 391 E+00 3.263E+00 2.973E+01 2.AA7E-01 6.712E+00 -0.002 0.016 0.005

80.0000 1 .882E+00 1 .608E+00 3.A90E+00 3.269E+01 2.696E-01 6.97AE+00 -0.001 0.015 O.OOA

90.0000 1 .892E+00 1 .826E+00 3.718E+00 3.5A7E+01 2.925E-01 7.206E+00 -0.001 0.013 O.OOA

100.0000 1 .900E+00 2.0A6E+00 3.9A6E+00 3.808E+01 3. 138E-01 7.A15E+00 -0.001 0.013 0.003

125.0000 1 . 91 7E+00 2.598E+00 A.516E+00 A. AOOE+01 3.607E-01 7.857E+00 -0.001 0.011 0.002

150.0000 1 .931E+00 3.155E+00 5.086E+00 A.921E+01 A.003E-01 8.21 9E+00 -0.000 0.010 0.002

175.0000 1 . 9A3E+00 3.71AE+00 5.658E+00 5.387E+01 A.3AAE-01 8.525E+00 -0.000 0.009 0.001 200.0000 1 .95AE+00 A.276E+00 6.230E+00 5.808E+01 A.6A1E-01 8.791E+00 -0.000 0.008 0.001 250.0000 1 .971 E+00 5. A05E+00 7.376E+00 6.5A5E+01 5.1 35E-01 9.236E+00 -0.000 0.007 0.001 300.0000 1 . 985E+00 6.5A0E+00 8.525E+00 7.175E+01 5.530E-01 9.599E+00 -0.000 0.007 0.001 350.0000 1 .997E+00 7.678E+00 9.675E+00 7.725E+01 5.856E-01 9.907E+00 -0.000 0.006 0.001 AOO.OOOO 2.007E+00 8.820E+00 1 .083E + 01 8.21 3E+01 6.129E-01 1 .017E+01 -0.000 0.006 0.001

A50 .0000 2.016E+00 9. 96AE+00 1 . 1 98E+01 8.652E+01 6.363E-01 1 .0A1E+01 -0.000 0.006 0.000

500 .0000 2.02AE+00 1.111 E+01 1 . 31 3E+01 9.050E+01 6.566E-01 1 .062E+01 -0 . 000 0.005 0.000

550.0000 2.031E+00 1 .226E+01 1 , A29E+01 9.A1 5E+01 6.7AAE-01 1 -081E+01 -0.000 0.005 0.000

600.0000 2.038E+00 1 . 3A0E+01 1 .5AAE+01 9.752E+01 6 . 901 E-01 1 .098E+01 -0.000 0.005 0.000

700.0000 2.050E+00 1 .570E+01 1 .775E+01 1 .036E+02 7. 167E-01 1 .129E+01 -0.000 0.005 0.000

800.0000 2.060E+00 1 .801 E+01 2.007E+01 1 .088E+02 7.385E-01 1 . 156E+01 -0.000 0.005 0.000

900.0000 2.069E+00 2.031E+01 2.238E+01 1 .136E+02 7.568E-01 1 .179E+01 -0.000 O.OOA 0.000

1000.0000 2.077E+00 2.262E+01 2.A70E+01 1 . 178E+02 7.723E-01 1 .200E+01 -0.000 O.OOA 0.000

155
POSITRONS IN ALUMINUM

I = 166.0 eV DENSITY = 2.699E+00 g/cra^

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^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .866E+01 6 .559E-03 1 .867E+01 3.090E-06 1 .867E-06 0.0 -0.211 0.263 0.239

0.0125 1 .556E+01 6 .700E-03 1 .555E+01 6.572E-06 2.280E-06 0.0 -0.202 0.231 0.228

0.0150 1 .369E+01 6 .798E-03 1 .350E+01 6 .303E-06 2.679E-06 0.0 -0.195 0.222 0.219

0.0175 1 . 1 97E+01 6 .871 E-03 1 . 1 98E+01 8.273E-06 3.066E-06 0.0 -0.190 0.215 0.212

0.0200 1 .080E+01 6 . 926E-03 1 .080E+01 1 .067E-03 3.662E-06 0.0 -0.186 0.209 0.207

0 .0250 9.087E+00 7.006E-03 9.096E+00 1 .556E-03 6. 166E-06 0.0 -0.179 0.200 0.198

0.0300 7.900E+00 7.059E-03 7.907E+00 2.165E-03 6.853E-06 0.0 -0.176 0.196 0.192

0.0350 7.026E+00 7.100E-03 7.033E+00 2.817E-03 5.526E-06 0.0 -0.170 0.188 0.187

0.0000 6.352E+00 7.133E-03 6.359E+00 3.566E-03 6.166E-06 0.0 -0.167 0.186 0.183

0.0050 5.817E+00 7.162E-03 5.825E+00 6.389E-03 6.787E-06 0.0 -0.166 0.180 0.179

0.0500 5.382E+00 7.191E-03 5.389E+00 5.282E-03 7.391E-06 0.0 -0.162 0.177 0.176

0 .0550 5.020E+00 7.217E-03 5.027E+00 6.266E-03 7.978E-06 0.0 -0.160 0.175 0.176

0 .0600 6.716E+00 7.263E-03 6.721E+00 7.271E-03 8.551E-06 0.0 -0.158 0.172 0.172

0.0700 6.225E+00 7.295E-03 6.233E+00 9.512E-03 9.657E-06 0.0 -0.155 0.169 0.168

0.0800 3.852E+00 7.350E-03 3.859E+00 1 .199E-02 1 .072E-03 0.0 -0.152 0.165 0.165

0.0900 3.557E+00 7.61 lE-03 3.565E+00 1 .669E-02 1 . 176E-03 0.0 -0.150 0.163 0.162

0.1000 3.31 9E+00 7 .676E-03 3.326E+00 1 .760E-02 1 .273E-03 0.0 -0.168 0.160 0.160

0.1250 2 .886E+00 7.659E-03 2.891E+00 2.569E-02 1 .509E-03 0.0 -0.165 0.156 0.155

0.1500 2 . 590E+00 7.865E-03 2.598E+00 3.686E-02 1 .730E-03 0.0 -0.162 0.153 0.152

0.1750 2 . 378E+00 8.096E-03 2.387E+00 6.690E-02 1 .962E-03 0.0 -0.160 0.150 0.169

0.2000 2.220E+00 8 . 366E-03 2.228E+00 5.575E-02 2.165E-03 0.0 -0.138 0.168 0.167

0.2500 2.000E+00 8.888E-03 2.009E+00 7.967E-02 2.536E-03 0.0 -0.136 0.166 0.163

0 . 3000 1 .855E+00 9.687E-03 1 .865E+00 1 .056E-01 2.906E-03 7.102E-03 -0.126 0.160 0.139

0.3500 1 .756E + 00 1 .01 3E-02 1 .765E+00 1 .330E-01 3.263E-03 1 .706E-02 -0.122 0.137 0.135

0.0000 1 .681E+00 1 .082E-02 1 .692E+00 1 .61 9E-01 3.616E-03 2.867E-02 -0.118 0.136 0.132

0.0500 1 .627E+00 1 . 1 56E-02 1 .638E+00 1 .920E-01 3. 959E-03 6.168E-02 -0.115 0.131 0.129

0.5000 1 .585E+00 1 .230E-02 1 .597E+00 2.229E-01 6.300E-03 5.517E-02 -0.112 0.128 0.126

0.5500 1 .553E+00 1 .309E-02 1 .566E+00 2.565E-01 6.639E-03 6.950E-02 -0.110 0.126 0.126

0 .6000 1 .527E+00 1 .390E-02 1 .561E+00 2.867E-01 6.977E-03 8.629E-02 -0.108 0.126 0.121 0.7000 1 .690E + 00 1 .560E-02 1 .506E+00 3.526E-01 5.650E-03 1 . 167E-01 -0.106 0.120 0.117

0.8000 1 .667E+00 1 .739E-02 1 .686E+00 6.1 96E-01 6.323E-03 1 .658E-01 -0.100 0.117 0.116

0.9000 1 .651E+00 1 .925E-02 1 .671E+00 6.871E-01 6.999E-03 1 .771E-01 -0.097 0.115 0.111

1 .0000 1 .661E+00 2.11 9E-02 1 .663E+00 5.553E-01 7.678E-03 2.086E-01 -0.095 0.112 0.108

1 .2500 1 .631E+00 2.630E-02 1 .657E+00 7.267E-01 9.396E-03 2.862E-01 -0.088 0.107 0.101

1 .5000 1 .631 E+00 3.177E-02 1 .663E+00 8.980E-01 1 .116E-02 3.630E-01 -0.082 0.102 0.096

1 .7500 1 .636E+00 3.752E-02 1 .673E+00 1 .068E+00 1 .292E-02 6.393E-01 -0.077 0.098 0.091 2.0000 1 -663E+00 6.350E-02 1 .686E+00 1 .237E+00 1 .672E-02 5.153E-01 -0.072 0.095 0.087

2.5000 1 .659E+00 5.605E-02 1 .515E+00 1 .570E+00 1 .860E-02 6.671E-01 -0.062 0.088 0.079

3.0000 1 .676E+00 6.926E-02 1 .566E+00 1 .897E+00 2.216E-02 8.175E-01 -0.053 0.083 0.071 3.5000 1 .689E+00 8.292E-02 1 .571E+00 2.218E+00 2.596E-02 9.663E-01 -0.066 0.077 0.065

0.0000 1 .501E+00 9.702E-02 1 .598E+00 2.536E+00 2. 981E-02 1 .106E+00 -0.061 0.073 0.059

0.5000 1 .51 3E+00 1.11 5E-01 1 .626E+00 2.866E+00 3.368E-02 1 .260E+00 -0.037 0.069 0.056

5.0000 1 .523E+00 1 .263E-01 1 .669E+00 3.150E+00 3.758E-02 1 .368E+00 -0.033 0.065 0.050

5.5000 1 .533E+00 1 .613E-01 1 .676E+00 3.651E+00 6.168E-02 1 .690E+00 -0.031 0.062 0.066

6.0000 1 .561E+00 1 .567E-01 1 .698E+00 3.767E+00 6.538E-02 1 .605E+00 -0.029 0.059 0.063

7.0000 1 .556E+00 1 .879E-01 1 .766E+00 6.328E+00 5.319E-02 1 .817E+00 -0.025 0.055 0.038

8.0000 1 .570E+00 2.200E-01 1 .790E+00 6.896E+00 6.096E-02 2.009E+00 -0.023 0.051 0.036

9.0000 1 .581E+00 2.526E-01 1 .836E+00 5.666E+00 6.867E-02 2. 186E+00 -0.021 0.068 0.031

1 0.0000 1 .592E+00 2.858E-01 1 .877E+00 5.985E+00 7.631E-02 2.363E+00 -0.020 0.065 0.028

12.5000 1 .616E+00 3.706E-01 1 .986E+00 7.280E+00 9.698E-02 2.690E+00 -0.018 0.060 0.026

15.0000 1 .631E+00 6.576E-01 2.089E+00 8.508E+00 1 .130E-01 2.982E+00 -0.016 0.036 0.021 17.5000 1 .666E+00 5.659E-01 2.1 92E+00 9.676E+00 1 .303E-01 3.233E+00 -0.015 0.033 0.019

20.0000 1 .659E+00 6.357E-01 2.295E+00 1 .079E+01 1 .669E-01 3.656E+00 -0.016 0.031 0.017

25.0000 1 .680E+00 8. 180E-01 2.698E+00 1 .288E+01 1 .781E-01 3.830E+00 -0.013 0.027 0.016

30 .0000 1 .697E+00 1 .003E+00 2.700E+00 1 .680E+01 2.068E-01 6.163E+00 -0.011 0.025 0.012

35.0000 1.71 lE+00 1 . 1 90E+00 2.901E+00 1 .659E+01 2.331E-01 6.612E+00 -0.010 0.023 0.011 60.0000 1 .723E+00 1 .379E+00 3. 102E+00 1 .826E+01 2.575E-01 6.669E+00 -0.009 0.021 0.010

65.0000 1 .733E+00 1 .569E+00 3.303E+00 1 .982E+01 2.800E-01 6.860E+00 -0.008 0.020 0.009

50.0000 1 .762E+00 1 .761E+00 3.503E+00 2.129E+01 3.009E-01 5.051E+00 -0.007 0.019 0.008

55.0000 1 .750E+00 1 .953E+00 3.706E+00 2.268E+01 3.206E-01 5.226E+00 -0.007 0.018 0.007

60.0000 1 .758E+00 2. 167E+00 3. 906E+00 2.399E+01 3.386E-01 5.387E+00 -0.006 0.017 0.007

70.0000 1 .770E+00 2.535E+00 6.306E+00 2.663E+01 3.716E-01 5.676E+00 -0.005 0.016 0.006

80.0000 1 .781E+00 2.927E+00 6.708E+00 2.865E+01 6.009E-01 5. 928E+00 -0.006 0.015 0.005

90.0000 1 .791E+00 3.320E+00 5. 1 lOE+00 3.069E+01 6.270E-01 6.153E+00 -0.003 0.016 0.006

100.0000 1 .799E+00 3.716E+00 5.51 3E+00 3.257E+01 6.505E-01 6.356E+00 -0.003 0.013 0.006

125.0000 1 .816E+00 6.707E+00 6 .523E+00 3.673E+01 5.002E-01 6.790E+00 -0.002 0.012 0.003

150.0000 1 .830E+00 5.705E+00 7.535E+00 6.030E+01 5.602E-01 7.167E+00 -0.001 0.011 0.002

175.0000 1 .862E+00 6.708E+00 8.550E+00 6.361E+01 5.732E-01 7.650E+00 -0.001 0.010 0.002

200.0000 1 .852E+00 7.716E+00 9.566E+00 6.617E+01 6.010E-01 7.716E+00 -0.001 0.009 0.002

250.0000 1 .869E+00 9.736E+00 1 .160E+01 5.091E+01 6.656E-01 8.156E+00 -0.001 0.008 0.001 300.0000 1 .883E+00 1 .176E+01 1 .366E+01 5.688E+01 6.798E-01 8.518E+00 -0.000 0.008 0.001 350.0000 1 .896E+00 1 .380E+01 1 .569E+01 5.830E+01 7.071E-01 8.825E+00 -0.000 0.007 0.001 600.0000 1 . 906E+00 1 .583E+01 1 .776E+01 6.129E+01 7.295E-01 9.091E+00 -0.000 0.007 0.001 650.0000 1 . 91 3E+00 1 .787E+01 1 . 979E+01 6.396E+01 7.683E-01 9.326E+00 -0.000 0.007 0.001 500.0000 1 . 921 E+00 1 . 992E+01 2. 186E + 01 6.636E+01 7.662E-01 9.536E+00 -0.000 0.007 0.001 550.0000 1 . 928E+00 2.1 96E+01 2.389E+01 6.855E+01 7.780E-01 9.726E+00 -0.000 0.006 0.001 600.0000 1 . 936E+00 2.601E+01 2.596E+01 7.056E+01 7.900E-01 9.900E+00 -0.000 0.006 0.001 700.0000 1 .966E+00 2.81 lE+01 3.005E+01 7.616E+01 8. 101E-01 1 .021E+01 -0.000 0.006 0.000

800.0000 1 .956E+00 3.221E+01 3.616E+01 7.726E+01 8.262E-01 1 .067E+01 -0.000 0.006 0.000 900.0000 1 .966E+00 3.631E+01 3.828E+01 8.002E+01 8.395E-01 1 .071E+01 -0.000 0.005 0.000

1000.0000 1 .972E+00 6.062E+01 6.239E+01 8.250E+01 8.507E-01 1 .092E+01 -0.000 0.005 0.000

156
POSITRONS IN COPPER

ENERGY

MoV

0.0100

0.0125

0.0150

0.0175

0.0200

0.0250

0.0300

0.0350

0.0<t00

0.0<150 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

0.6000

0.6500

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

6.0000

6.5000

5.0000

5.5000

6.0000

7.0000

8.0000

9.0000 10.0000 12.5000

15.0000 17.5000

20.0000

25.0000

30.0000

35.0000

60.0000

65.0000

50.0000

55.0000

60.0000

70.0000

80.0000

90.0000

100 .0000 125.0000

150.0000 175.0000 200.0000

250.0000

300.0000

350.0000

600.0000

650.0000

500 .0000 550.0000

600 .0000 700.0000

800.0000

900.0000

1000.0000

I = 322.0 oV DENSITY

STOPPING POWER CSDA COLLISION RADIATIVE TOTAL RANGE

MoV cm^/g MeV cm^/g MeV cm^/g g/cm^

1 .505E+01 1 .21 3E-02 1 .506E*-01 3.891E-06

1 .275E + 01 1 .277E-02 1 .276E + 01 5.702E-06

1 . 1 13E+01 1 .327E-02 1 . 1 16E + 01 7.806E-06

9.915E+00 1 .366E-02 9.929E+00 1 .01 9E-03

8.970E+00 1 .399E-02 8.986E+00 1 .286E-03

7.588E+00 1 .669E-02 7.603E+00 1 .891E-03

6.622E+00 1 .688E-02 6.637E+00 2.597E-03

5.906E+00 1 .518E-02 5.921E+00 3.396E-03

5.353E+00 1 .563E-02 5.369E+00 6.285E-03

6.912E+00 1 .566E-02 6.928E+00 5.258E-03

6.552E+00 1 .583E-02 6.568E+00 6.313E-03

6.252E+00 1 .600E-02 6.268E+00 7.666E-03

3.999E+00 1 .615E-02 6.015E+00 8.655E-03

3.592E+00 1 .661E-02 3.609E+00 1 . 129E-02

3.281E+00 1 .665E-02 3.297E+00 1 .61 9E-02

3.036E+00 1 .688E-02 3.051E+00 1 .735E-02

2.835E+00 1 .710E-02 2.852E+00 2.076E-02

2.669E+00 1 .763E-02 2.687E+00 3.017E-02

2.222E+00 1 .816E-02 2.260E+00 6.078E-02

2.060E+00 1 .870E-02 2.059E+00 5.265E-02

1 .906E+00 1 . 926E-02 1 .923E+00 6.503E-02

1 .716E+00 2.065E-02 1 .735E+00 9.250E-02

1 .590E+00 2. 172E-02 1 .612E+00 1 .225E-01

1 .503E+00 2.307E-02 1 .526E+00 1 .566E-01

1 .660E+00 2.650E-02 1 .665E+00 1 .879E-01

1 .393E+00 2.600E-02 1 .61 9E+00 2.226E-01

1 .358E+00 2.757E-02 1 .385E+00 2.582E-01

1 .330E+00 2. 91 9E-02 1 .359E+00 2.967E-01

1 .308E+00 3.087E-02 1 .339E+00 3.318E-01

1 .276E+00 3.637E-02 1 .310E+00 6.076E-01

1 .256E+00 3.803E-02 1 .296E+00 6.862E-01

1 .263E+00 6. 185E-02 1 .286E+00 5.618E-01

1 .236E+00 6.580E-02 1 .280E+00 6.398E-01

1 .225E+00 5.623E-02 1 .281E+00 8.352E-01

1 .225E+00 6.733E-02 1 .293E+00 1 .030E+00

1 .230E+00 7.896E-02 1 .309E+00 1 .222E+00

1 .236E+00 9.103E-02 1 .327E+00 1 .612E+00

1 .251E+00 1 .162E-01 1 .367E+00 1 .783E+00

1 .266E+00 1 .625E-01 1 .609E+00 2. 163E+00

1 .280E+00 1 .697E-01 1 .650E+00 2.693E+00

1 .296E+00 1 .976E-01 1 -691E+00 2.833E+00

1 .306E+00 2.261E-01 1 .532E+00 3.166E+00

1 .317E+00 2.552E-01 1 .572E+00 3.686E+00

1 .327E+00 2.867E-01 1 .612E+00 3.800E+00

1 .337E+00 3.166E-01 1 .651E+00 6.107E+00

1 . 356E+00 3.756E-01 1 .729E+00 6.698E+00

1 .369E+00 6.378E-01 1 .806E+00 5.266E+00

1 .382E+00 5.009E-01 1 .883E+00 5.806E+00

1 .396E+00 5.650E-01 1 .959E+00 6.327E+00

1 .618E+00 7.282E-01 2.167E+00 7.566E+00

1 .639E+00 8. 969E-01 2.333E+00 8.662E+00

1 .655E+00 1 .066E+00 2.51 9E+00 9.693E+00

1 .669E+00 1 .236E+00 2.705E+00 1 .065E+01

1 .692E+00 1 .583E+00 3.076E+00 1 .238E+01

1 .510E+00 1 .936E+00 3.666E+00 1 .392E+01

1 .525E+00 2.291E+00 3.817E+00 1 .530E+01

1 .538E+00 2.650E+00 6. 188E+00 1 .655E+01

1 .568E+00 3.012E+00 6.560E+00 1 .769E+01

1 .558E+00 3.375E+00 6.933E+00 1 .876E+01

1 .566E+00 3.760E+00 5.306E+00 1 . 972E+01

1 .573E+00 6. 107E+00 5.680E+00 2.063E+01

1 .587E+00 6.866E+00 6.630E+00 2.229E+01

1 .598E+00 5.586E+00 7. 183E+00 2.376E+01

1 .607E+00 6 . 330E+00 7 . 938E+00 2.508E+01

1 .616E+00 7 . 079E+00 8.695E+00 2.628E+01

1 .636E+00 8. 958E+00 1 .059E+01 2.888E+01

1 . 668E+00 1 .085E+01 1 .250E+01 3. 105E+01

1 .660E+00 1 .275E+01 1 .661E+01 3.292E+01

1 .670E + 00 1 .665E+01 1 .632E+01 3.655E+01

1 .687E+00 1 .867E+01 2.015E+01 3.730E+01

1 .701E+00 2.230E+01 2.600E+01 3.957E+01

1 .712E+00 2.61 3E+01 2.786E+01 6. 150E+01

1 .722E+00 2. 998E+01 3. 170E+01 6 . 318E+01

1 .731E+00 3.382E+01 3.555E+01 6.667E+01

1 . 738E+00 3 . 767E+01 3.961E+01 6.601E+01

1 .765E+00 6. 153E+01 6.327E+01 6.722E+01

1 .751E+00 6.539E+01 6.716E+01 6.832E+01

1 .762E+00 5.31 1E+01 5.687E+01 5.029E+01

1 .772E + 00 6 .083E+01 6 .260E+01 5.1 99E+01

1 .780E+00 6.856E+01 7.036E+01 5.350E+01

1 .787E+00 7.629E+01 7.808E+01 5.685E+01

= 8.960E+00 g/cm3

RADIATION DENS. EPF. dClog )/d(logI) YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

6.006E-06 0.0 -0.265 0.293 0.283

5.01 IE-06 0.0 -0.233 0.276 0.267

6.003E-06 0.0 -0.226 0.263 0.255

6.979E-06 0.0 -0.217 0.253 0.266

7.960E-06 0.0 -0.211 0.265 0.239

9.81 9E-06 0.0 -0.203 0.233 0.227

1 .166E-03 0.0 -0.196 0.223 0.219

1 .361E-03 0.0 -0.191 0.216 0.212

1 .513E-03 0.0 -0.187 0.211 0.207

1 .681E-03 0.0 -0.186 0.206 0.203

1 .865E-03 0.0 -0.181 0.202 0.199

2.005E-03 0.0 -0.178 0.198 0.196

2. 162E-03 0.0 -0.176 0.195 0.193

2.666E-03 0.0 -0.172 0.190 0.188

2.758E-03 0.0 -0.169 0.185 0.186

3.039E-03 0.0 -0.167 0.183 0.181 3.312E-03 0.0 -0.165 0.180 0.178

3.960E-03 0.0 -0.160 0.176 0.172

6.567E-03 2.607E-03 -0.161 0.169 0.167

5. 163E-03 2.660E-02 -0.131 0.161 0.159

5.696E-03 6.565E-02 -0.128 0.156 0.153

6.737E-03 8.670E-02 -0.122 0.165 0.163

7.721E-03 1 .217E-01 -0.117 0.138 0.136

8.660E-03 1 .572E-01 -0.113 0.133 0.131 9.567E-03 1 .916E-01 -0.110 0.129 0.126

1 .065E-02 2.269E-01 -0.107 0.125 0.123

1 .132E-02 2.573E-01 -0.106 0.122 0.119

1 .217E-02 2.889E-01 -0.102 0.120 0.116

1 .301E-02 3.1 98E-01 -0.100 0.117 0.116

1 .667E-02 3.796E-01 -0.096 0.113 0.109

1 .631E-02 6.363E-01 -0.093 0.110 0.106

1 .795E-02 6.907E-01 -0.090 0.107 0.102

1 .957E-02 5.630E-01 -0.087 0.106 0.099

2.362E-02 6.652E-01 -0.082 0.099 0.093

2.768E-02 7.772E-01 -0.077 0.096 0.088

3. 176E-02 8.810E-01 -0.073 0.091 0.086

3.585E-02 9.779E-01 -0.070 0.088 0.080

6.606E-02 1 .155E+00 -0.066 0.082 0.076

5.222E-02 1 .316E+00 -0.060 0.078 0.068

6.035E-02 1 .658E+00 -0.056 0.076 0.066

6.861E-02 1 .590E+00 -0.053 0.071 0.060

7.638E-02 1 .712E+00 -0.050 0.068 0.057

8.626E-02 1 .825E+00 -0.068 0.066 0.056

9.1 99E-02 1 . 929E+00 -0.067 0.066 0.052

9.962E-02 2.027E+00 -0.065 0.062 0.050

1 . 165E-01 2.206E+00 -0.063 0.058 0.066

1 .290E-01 2.366E+00 -0.061 0.055 0.063

1 .629E-01 2.510E+00 -0.039 0.053 0.060

1 .563E-01 2.662E+00 -0.038 0.051 0.038

1 .880E-01 2.931E+00 -0.035 0.067 0.036

2. 169E-01 3. 176E+00 -0.032 0.066 0.030

2.636E-01 3.390E+00 -0.030 0.061 0.028

2.681E-01 3.581E+00 -0.027 0.039 0.025

3.11 9E-01 3.913E+00 -0.026 0.035 0.021 3.697E-01 6.1 97E+00 -0.020 0.032 0.018

3.829E-01 6.665E+00 -0.018 0.030 0.016

6. 121E-01 6.666E+00 -0.016 0.028 0.016

6.382E-01 6.865E+00 -0.016 0.027 0.013

6.617E-01 5.066E+00 -0.013 0.026 0.012

6.829E-01 5.212E+00 -0.012 0.025 0.011 5.021E-01 5.365E+00 -0.011 0.026 0.010

5.359E-01 5.639E+00 -0.010 0.022 0.008

5.667E-01 5.880E+00 -0.009 0.021 0.007

5.895E-01 6.096E+00 -0.008 0.020 0.007

6.11 IE-01 6 .288E+00 -0.007 0.019 0.006

6.551E-01 6.701E+00 -0.006 0.017 0.005

6 .888E-01 7.062E+00 -0.005 0.016 0.006

7.157E-01 7.333E+00 -0.005 0.015 0.003

7. 377E-01 7.5C7E+00 -0.006 0.015 0.003

7.716E-01 8.015E+00 -0.003 0.016 0.002

7.969E-01 8.368E+00 -0.003 0.013 0.002

8.165E-01 8.668E+00 -0.002 0.012 0.002

8.322E-01 8. 930E+00 -0.002 0.012 0.001 8.651E-01 9. 161E+00 -0.001 0.011 0.001 8.560E-01 9.369E+00 -0.001 0.011 0.001 8.652E-01 9.557E+00 -0.001 0.011 0.001 8.733E-01 9.729E+00 -0.001 0.011 0.001 8.866E-01 1 .003E+01 -0.001 0.010 0.001

8 . 969E-01 1 .030E+01 -0.001 0.010 0.001 9.053E-01 1 .053E+01 -0.000 0.010 0.001 9.126E-01 1 .076E+01 -0.000 0.009 0.001

157
POSITRONS IN SILVER

I = 470.0 eV DENSITY = 1 .050E+01 g/cm 3

ENERGY STOPPING POWER CSDA RADIATION DENS. EPF. dClog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 1 .303E+01 1 .634E-02 1 .305E+01 4.587E-04 6 .026E-04 0.0 -0.270 0.334 0.317

0.0125 1 .1 lOE+01 1 .754E-02 1 . 1 12E+01 6.670E-04 7.651E-04 0.0 -0.255 0.312 0.296 0.0150 9.726E+00 1 .849E-02 9.744E+00 9.078E-04 9.272E-04 0.0 -0.245 0.295 0.282

0.0175 8.690E+00 1 .927E-02 8.709E+00 1 . 180E-03 1 .088E-03 0.0 -0.237 0.282 0.270

0.0200 7 .880E+00 1 . 992E-02 7.900E+00 1 .482E-03 1 .248E-03 0.0 -0.230 0.272 0.261 0.0250 6 .689E+00 2.099E-02 6 .710E+00 2. 171E-03 1 .564E-03 0.0 -0.220 0.257 0.248

0.0300 5.853E+00 2. 184E-02 5.875E+00 2. 970E-03 1 .874E-03 0.0 -0.212 0.246 0.238

0.0350 5.231E+00 2.254E-02 5.254E+00 3.871E-03 2. 178E-03 0.0 -0.206 0.237 0.230

0.0^00 4.749E+00 2.314E-02 4.773E+00 4.872E-03 2.477E-03 0.0 -0.201 0.230 0.224

0 .0‘+50 4. 364E+00 2.367E-02 4.388E+00 5.965E-03 2.771E-03 0.0 -0.197 0.224 0.218

0.0500 4.049E+00 2.414E-02 4.073E+00 7.149E-03 3.060E-03 0.0 -0.194 0.21 9 0.214

0.0550 3.786E+00 2.458E-02 3.811 E+00 8.41 9E-03 3.345E-03 0.0 -0.191 0.215 0.210

0.0600 3.564E+00 2.497E-02 3.589E+00 9.772E-03 3.625E-03 0.0 -0.189 0.211 0.207

0.0700 3.206E+00 2.569E-02 3.232E+00 1 .271E-02 4. 172E-03 0.0 -0.184 0.205 0.201 0.0800 2. 932E+00 2.634E-02 2.958E+00 1 .595E-02 4.704E-03 0.0 -0.181 0.200 0.197

0.0900 2.715E+00 2.693E-02 2.742E+00 1 .947E-02 5.222E-03 0.0 -0.178 0.196 0.193

0.1000 2.537E+00 2.748E-02 2.564E+00 2.324E-02 5.727E-03 5.406E-03 -0.159 0.191 0.188

0.1250 2.210E+00 2.875E-02 2.239E+00 3.372E-02 6.940E-03 2.558E-02 -0.155 0.180 0.177

0.1500 1 . 989E+00 2. 990E-02 2.018E+00 4.551E-02 8.090E-03 4.392E-02 -0.151 0.172 0.169

0.1750 1 .829E+00 3.098E-02 1 .860E+00 5.844E-02 9. 183E-03 6.093E-02 -0.147 0.167 0.164

0.2000 1 .709E+00 3.203E-02 1 .741E+00 7.235E-02 1 .023E-02 7.694E-02 -0.144 0.162 0.159

0.2500 1 .542E+00 3.413E-02 1 .576E+00 1 .026E-01 1 .21 9E-02 1 .068E-01 -0.139 0.155 0.152

0 . 3000 1 .433E+00 3.628E-02 1 .469E+00 1 .356E-01 1 .403E-02 1 .348E-01 -0.135 0.150 0.147

0.3500 1 .357E+00 3.852E-02 1 .395E+00 1 .705E-01 1 .576E-02 1 .613E-01 -0.131 0.146 0.143

0.^000 1 .302E+00 4.085E-02 1 .343E+00 2.071E-01 1 .742E-02 1 .867E-01 -0.128 0.142 0.139

0.0500 1 .261E+00 4.328E-02 1 .304E+00 2.449E-01 1 .902E-02 2.112E-01 -0.125 0.139 0.136

0.5000 1 .230E+00 4.580E-02 1 .276E+00 2.837E-01 2.057E-02 2.349E-01 -0.123 0.136 0.133

0.5500 1 .206E+00 4.840E-02 1 .255E+00 3.232E-01 2.208E-02 2.580E-01 -0.120 0.134 0.131 0.6000 1 . 188E+00 5. 107E-02 1 .239E+00 3.633E-01 2.357E-02 2.804E-01 -0.118 0.132 0.129

0.7000 1 .161E+00 5.659E-02 1 .218E+00 4.448E-01 2.647E-02 3.237E-01 -0.115 0.128 0.125

0.8000 1 . 1 45E+00 6 .233E-02 1 .207E+00 5.273E-01 2.929E-02 3.651E-01 -0.111 0.125 0.121

0 . 9000 1 . 1 35E+00 6 .827E-02 1 .203E+00 6.104E-01 3.206E-02 4.048E-01 -0.108 0.122 0.118

1 .0000 1 . 129E+00 7.439E-02 1 .203E+00 6.935E-01 3.478E-02 4.429E-01 -0.105 0.119 0.115

1 .2500 1 .124E+00 9.038E-02 1 .214E+00 9.005E-01 4. 145E-02 5.328E-01 -0.100 0.114 0.108

1 .5000 1 .127E+00 1 .072E-01 1 .234E+00 1 .105E+00 4.799E-02 6. 158E-01 -0.095 0.109 0.103

1 .7500 1 . 1 34E+00 1 .247E-01 1 .259E+00 1 .305E+00 5.442E-02 6.931E-01 -0.091 0.105 0.098

2.0000 1 . 142E+00 1 .428E-01 1 .285E+00 1 .502E+00 6.075E-02 7.656E-01 -0.087 0.102 0.094

2.5000 1 . 1 60E+00 1 .802E-01 1 .340E+00 1 .883E+00 7.317E-02 8.983E-01 -0.081 0.096 0.087

3.0000 1 . 177E+00 2.1 90E-01 1 .396E+00 2.249E+00 8.526E-02 1 .018E+00 -0.077 0.092 0.082

3.5000 1 . 1 94E+00 2.589E-01 1 .452E+00 2.600E+00 9.703E-02 1 . 127E+00 -0.073 0.088 0.077

4.0000 1 .208E+00 2.997E-01 1 .508E+00 2.937E+00 1 .085E-01 1 .228E+00 -0.070 0.084 0.073

4.5000 1 .222E+00 3.412E-01 1 .563E+00 3.263E+00 1 . 1 96E-01 1 .322E+00 -0.066 0.081 0.069

5.0000 1 .234E+00 3.834E-01 1 .618E+00 3.577E+00 1 .304E-01 1 .410E+00 -0.064 0.079 0.066

5.5000 1 .245E+00 4.263E-01 1 .672E+00 3.882E+00 1 .409E-01 1 .494E+00 -0.061 0.076 0.063

6.0000 1 .256E+00 4.696E-01 1 .725E+00 4.176E+00 1 .51 lE-01 1 .573E+00 -0.058 0.074 0.060

7.0000 1 .274E+00 5.577E-01 1 .832E+00 4.738E+00 1 .708E-01 1 .722E+00 -0.054 0.070 0.055

8.0000 1 .290E+00 6.474E-01 1 .937E+00 5.269E+00 1 .894E-01 1 .860E+00 -0.050 0.066 0.051 9.0000 1 . 303E+00 7.384E-01 2.042E+00 5.772E+00 2.070E-01 1 .989E+00 -0.046 0.063 0.047

10.0000 1 .315E+00 8.305E-01 2.146E+00 6 .250E+00 2.237E-01 2.110E+00 -0.043 0.061 0.044

12.5000 1 .340E+00 1 .065E+00 2.405E+00 7.349E+00 2.621E-01 2.383E+00 -0.037 0.055 0.038

15.0000 1 .360E+00 1 .304E+00 2.664E+00 8.336E+00 2.963E-01 2.621E+00 -0.033 0.051 0.033

17.5000 1 .376E+00 1 .547E+00 2.923E+00 9.232E+00 3.268E-01 2.833E+00 -0.030 0.047 0.029

20.0000 1 .390E+00 1 .794E+00 3. 183E+00 1 .005E+01 3.543E-01 3.023E+00 -0.028 0.045 0.026

25.0000 1 .412E+00 2.293E+00 3.705E+00 1 . 151E+01 4.019E-01 3.352E+00 -0.024 0.040 0.021 30.0000 1 . 429E+00 2.800E+00 4.230E+00 1 .277E+0I 4.418E-01 3.632E+00 -0.022 0.037 0.018

35.0000 1 .444E+00 3.313E+00 4.757E+00 1 .388E+01 4.758E-01 3.874E+00 -0.020 0.035 0.016

40.0000 1 .456E+00 3.831 E+00 5.287E+00 1 .488E+01 5.052E-01 4.089E+00 -0.018 0.033 0.014

45.0000 1 .467E+00 4.352E+00 5.818E+00 1 .578E+01 5.309E-01 4.282E+00 -0.017 0.031 0.013

50.0000 1 .476E+00 4.876E+00 6.352E+00 1 .660E+01 5.536E-01 4.457E+00 -0.015 0.030 0.011 55.0000 1 .484E+00 5.403E+00 6 .887E+00 1 .736E+01 5.739E-01 4.618E+00 -0.014 0.029 0.010

60.0000 1 .492E+00 5.932E+00 7.424E+00 1 .806E+01 5.921E-01 4.767E+00 -0.013 0.028 0.010

70.0000 1 .505E+00 6.995E+00 8.500E+00 1 .932E+01 6.234E-01 5.035E+00 -0.012 0.026 0.008

80.0000 1 .516E+00 8.065E+00 9.580E+00 2.042E+01 6.496E-01 5.271E+00 -0.010 0.025 0.007

90.0000 1 .525E+00 9.1 39E+00 1 .066E+01 2.141E+01 6.718E-01 5.482E+00 -0.009 0.024 0.006 100.0000 1 .533E+00 1 .022E+01 1 .175E+01 2.230E+01 6.910E-01 5.672E+00 -0.008 0.023 0.006 125.0000 1 .551E+00 1 .293E+01 1 .448E+01 2.422E+01 7.292E-01 6.082E+00 -0.007 0.021 0.005

150.0000 1 .565E+00 1 .565E+01 1 .721E+01 2.580E+01 7.579E-01 6.422E+00 -0.006 0.020 0.004

175.0000 1 .576E+00 1 .838E+01 1 .995E+01 2.715E+01 7.804E-01 6 .712E+00 -0.005 0.019 0.003

200.0000 1 .586E+00 2.1 12E+01 2.270E+01 2.832E+01 7.985E-01 6 . 965E+00 -0.005 0.018 0.003

250 .0000 1 .602E+00 2.661E+01 2.821E+01 3.029E+01 8.263E-01 7.391E+00 -0.004 0.017 0.002

300 .0000 1 .615E+00 3.21 1E+01 3.373E+01 3.191E+01 8.465E-01 7.741E+00 -0.003 0.016 0.002

350.0000 1 .626E+00 3.763E+01 3.926E+01 3.329E+01 8.621E-01 8.039E+00 -0.003 0.015 0.002

400.0000 1 .636E+00 4.316E+01 4.479E+01 3.448E+01 8.745E-01 8.299E+00 -0.002 0.015 0.001 450.0000 1 .644E+00 4.869E+01 5.033E+01 3.553E+01 8.846E-01 8.528E+00 -0.002 0.014 0.001 500.0000 1 .651 E + 00 5.422E+01 5.588E+01 3.647E+01 8.930E-01 8.735E+00 -0.002 0.014 0.001 550.0000 1 .658E+00 5.976E+01 6. 142E+01 3.732E+01 9.002E-01 8. 922E+00 -0.002 0.014 0.001 600.0000 1 .664E+00 6.531E+01 6 .697E+01 3.81 OE+01 9.063E-01 9.093E+00 -0.001 0.013 0.001 700.0000 1 .675E+00 7.641E+01 7.808E+01 3. 949E+01 9.164E-01 9.397E+00 -0.001 0.013 0.001 800.0000 1 .684E+00 8.751E+01 8.920E+01 4.068E+01 9.244E-01 9.661E+00 -0.001 0.013 0.001 900.0000 1 .692E+00 9.863E+01 1 .003E+02 4. 174E+01 9.308E-01 9.894E+00 -0.001 0.012 0.001 1000.0000 1 .699E+00 1 .098E+02 1 . 114E+02 4.269E+01 9.361E-01 1 .010E+01 -0.001 0.012 0.001

158
POSITRONS IN LEAD

I = 823.0 eV DENSITY = 1 .135E+01 g/cm^

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 cm^/g MeV cm^/g MeV cm^/g g/cm ^

0.0100 1 .005E+01 2.0A5E-02 1 .007E+01 6.238E-0A 9. A33E-0A 0.0 -0.318 0 . A32 0 . 387 0.0125 8.6A1E+00 2.251E-02 8.66AE+00 8.925E-0A 1 .217E-03 0.0 -0.298 0.39A 0.356

0.0150 7.623E+00 2.A21E-02 7.6A7E+00 1 .200E-03 1 . A95E-03 0.0 -0.28A 0.367 0.335

0.0175 6.8A7E+00 2.566E-02 6.873E+00 1 .5A6E-03 1 .77AE-03 0.0 -0.273 0.3A7 0.319

0.0200 6.236E+00 2.693E-02 6.263E+00 1 .927E-03 2.055E-03 0.0 -0.26A 0.331 0.306

0.0250 5.329E+00 2.908E-02 5.358E+00 2.79AE-03 2.617E-03 0.0 -0.250 0.308 0.287

0.0300 A.685E+00 3.086E-02 A.716E+00 3.791E-03 3.178E-03 0.0 -0.2A1 0.291 0.273

0.0350 A.203E+00 3.2AOE-02 A.235E+00 A.912E-03 3.738E-03 0.0 -0.233 0.278 0.263

O.OAOO 3.827E+00 3.376E-02 3.861E+00 6.150E-03 A.296E-03 0.0 -0.227 0.268 0.255

0.0A50 3.526E+00 3.500E-02 3.561E+00 7.500E-03 A.850E-03 0.0 -0.222 0.260 0.2A8

0.0500 3.278E+00 3.61 3E-02 3.31AE+00 8.957E-03 5. A02E-03 0.0 -0.218 0.253 0 .2A2 0.0550 3.071E+00 3.718E-02 3.108E+00 1 .052E-02 5.950E-03 0.0 -0.21A 0.2A7 0.237

0.0600 2.895E+00 3.817E-02 2.933E+00 1 .217E-02 6.A95E-03 0.0 -0.211 0.2A2 0.233

0.0700 2.61 1E+00 3.998E-02 2.651E+00 1 .577E-02 7.57AE-03 0.0 -0.206 0.23A 0.225

0.0800 2.393E+00 A. 162E-02 2. A35E+00 1 . 971E-02 8.639E-03 0.0 -0.201 0.227 0.219

0.0900 2.220E+00 A.313E-02 2.263E+00 2.397E-02 9.688E-03 0.0 -0.198 0.221 0.215

0.1000 2.079E+00 A.A5AE-02 2. 123E+00 2.85AE-02 1 .072E-02 0.0 -0.195 0.217 0.210

0.1250 1 .820E+00 A.772E-02 1 .867E+00 A.11AE-02 1 .32AE-02 0.0 -0.189 0.208 0.202

0.1500 1 .6AAE+00 5.05AE-02 1 .69AE+00 5.523E-02 1 .565E-02 0.0 -0. 18A 0.201 0.196

0.1750 1 .517E+00 5.312E-02 1 .570E+00 7.059E-02 1 .796E-02 0.0 -0.180 0.195 0.191 0.2000 1 . A21E+00 5.555E-02 1 .A76E+00 8.703E-02 2.01 9E-02 7.387E-0A -0.173 0.191 0.186

0.2500 1 .287E+00 6.015E-02 1 .3A7E+00 1 .226E-01 2.A39E-02 8. A66E-03 -0.166 0.182 0.178

0 . 3000 1 .200E+00 6.A60E-02 1 .265E+00 1 .610E-01 2.831E-02 1 .693E-02 -0.160 0.176 0.172

0.3500 1 . 1 AOE+00 6.900E-02 1 .209E+00 2.015E-01 3.1 99E-02 2.596E-02 -0.155 0.171 0.166

O.AOOO 1 .097E+00 7.3A0E-02 1 . 170E+00 2.A35E-01 3.5A9E-02 3.5A5E-02 -0.151 0.166 0.161 O.A500 1 .065E+00 7.781E-02 1 .1 A2E+00 2.868E-01 3.881E-02 A.530E-02 -0.1A7 0.162 0.157

0.5000 1 .OAlE+00 8.228E-02 1 .123E+00 3.310E-01 A.200E-02 5.5A3E-02 -0.1 AA 0.158 0.1 5A 0.5500 1 .022E+00 8.677E-02 1 . 109E+00 3.758E-01 A.507E-02 6.577E-02 -O.lAl 0.155 0.150

0.6000 1 .008E+00 9.132E-02 1 .099E+00 A.21 lE-01 A.80AE-02 7.627E-02 -0.138 0.152 0.1A7

0.7000 9.887E-01 1 .005E-01 1 .089E+00 5.126E-01 5.371E-02 9.756E-02 -0.133 0.1 A7 0.1A2

0.8000 9.772E-01 1 .098E-01 1 .087E+00 6.0A5E-01 5.908E-02 1 .19IE-01 -0.128 0.1A3 0.137

0.9000 9.707E-01 1 . 1 93E-01 1 .090E+00 6.96AE-01 6.A21E-02 1 .A06E-01 -0.125 0.139 0.132

1 .0000 9.675E-01 1 .290E-01 1 .096E+00 7.879E-01 6.915E-02 1 .621E-01 -0.121 0.135 0.129

1.2500 9.676E-01 1 .537E-01 1 . 121E+00 1 .01 AE+00 8.081E-02 2.153E-01 -O.llA 0.128 0.120

1 .5000 9.737E-01 1 .792E-01 1 .153E+00 1 .233E+00 9. 173E-02 2.673E-01 -0.108 0.122 0.113

1 .7500 9.822E-01 2.053E-01 1 .187E+00 1 .AA7E+00 1 .021E-01 3. 183E-01 -0.103 0.117 0.108

2.0000 9.916E-01 2.31 9E-01 1 .22AE+00 1 .655E+00 1 . 120E-01 3.683E-01 -0.098 0.113 0.102

2.5000 1 .01 lE+00 2.866E-01 1 .297E+00 2.051E+00 1 .307E-01 A.653E-01 -0.090 0.105 0.09A

3.0000 1 .028E+00 3.A27E-01 1 .371E+00 2.A26E+00 1 .A82E-01 5.586E-01 -0.08A 0.099 0.086

3.5000 1 .OAAE+00 3.999E-01 1 .AAAE+00 2.782E+00 1 .6A7E-01 6.A81E-01 -0.078 0.09A 0.080

A. 0000 1 .059E+00 A.582E-01 1 .517E+00 3.119E+00 1 .803E-01 7.335E-01 -0.07A 0.090 0.075

A. 5000 1 .072E+00 5. 17AE-01 1 .589E+00 3.AA1E+00 1 .951E-01 8.1A9E-01 -0.070 0.086 0.070

5.0000 1 .08AE+00 5.773E-01 1 .661E+00 3.7A9E+00 2.093E-01 8.926E-01 -0.067 0.083 0.067

5.5000 1 .095E+00 6.379E-01 1 .733E+00 A.OAAE+00 2.228E-01 9.667E-01 -0.065 0.080 0.063

6.0000 1 .105E+00 6.991E-01 1 .80AE+00 A.326E+00 2.357E-01 1 .038E+00 -0.062 0.077 0.060

7.0000 1 .123E+00 8.233E-01 1 .9A6E+00 A.860E+00 2.600E-01 1 .170E+00 -0.058 0.073 0.05A

8.0000 1 . 1 38E+00 9.A95E-01 2.087E+00 5.356E+00 2.82AE-01 1 .293E+00 -0.055 0.069 0.050

9.0000 1 .151E+00 1 .077E+00 2.228E+00 5.820E+00 3.032E-01 1 .A06E+00 -0.052 0.066 0.0A6

10.0000 1 . 163E+00 1 .206E+00 2.369E+00 6.255E+00 3.225E-01 1 .512E+00 -0.050 0.063 O.OA3

12.5000 1 . 188E+00 1 .535E+00 2.723E+00 7.238E+00 3.655E-01 1 .7A9E+00 -0.0A5 0.057 0.037

15.0000 1 .208E+00 1 .870E+00 3.077E+00 8. lOlE+00 A.023E-01 1 .955E+00 -O.OAl 0.053 0.032

17.5000 1 .22AE+00 2.210E+00 3.A3AE+00 8.870E+00 A.3A3E-01 2.138E+00 -0.038 0.050 0.029

20.0000 1 .238E+00 2.55AE+00 3.792E+00 9.563E+00 A.62AE-01 2.302E+00 -0.036 0.0A7 0.026

25.0000 1 .261E+00 3.252E+00 A.513E+00 1 .077E+01 5.096E-01 2.589E+00 -0.032 0.0A3 0.022

30.0000 1 .279E+00 3.961E+00 5.2A0E+00 1 . 180E+01 5. A78E-01 2.83AE+00 -0.029 O.OAO 0.019

35.0000 1 .293E+00 A.678E+00 5.972E+00 1 .269E+01 5.796E-01 3.0A8E+00 -0.027 0.038 0.016

AO. 0000 1 .306E+00 5.A02E+00 6.708E+00 1 .3A8E+01 6.065E-01 3.2A1E+00 -0.025 0.036 0.015

A5.0000 1 .317E+00 6.132E+00 7.AA8E+00 1 .A1 9E+01 6.296E-01 3. A1 AE+00 -0.023 0.03A 0.013

50.0000 1 .326E+00 6 .865E+00 8.1 92E+00 1 .A83E+01 6.A97E-01 3.57AE+00 -0.022 0.033 0.012

55.0000 1 .335E+00 7.603E+00 8. 938E+00 1 .5A1E+01 6.67AE-01 3.720E+00 -0.020 0.032 0.01 1 60.0000 1 .3A2E+00 8.3A5E+00 9.687E+00 1 .595E+01 6.832E-01 3.857E+00 -0.019 0.031 0.010

70.0000 1 .355E+00 9.836E+00 1.11 9E+01 1 .691E+01 7.099E-01 A.103E+00 -0.017 0.029 0.009

80.0000 1 .366E+00 1 .13AE+01 1 .270E+01 1 .775E+01 7.31 9E-01 A.322E+00 -0.015 0.028 0.008

90.0000 1 .376E+00 1 .28AE+01 1 .A22E+01 1 .8A9E+01 7.50AE-01 A.518E+00 -O.OIA 0.027 0.007

100.0000 1 .38AE+00 1 . A36E+01 1 .57AE+01 1 .916E+01 7.661E-01 A.696E+00 -0.013 0.026 0.006

125.0000 1 .AOlE+00 1 .816E+01 1 .956E+01 2.058E+01 7.971E-01 5.080E+00 -0.011 0.02A 0.005

150.0000 1 . A1 5E+00 2.1 98E+01 2.3A0E+01 2.175E+01 8.199E-01 5. AOlE+00 -0.010 0.023 O.OOA

175.0000 1 .A26E+00 2.582E+01 2.725E+01 2.27AE+01 8.376E-01 5.677E+00 -0.009 0.022 O.OOA 200.0000 1 .A36E+00 2.966E+01 3.110E+01 2.359E+01 8.518E-01 5.919E+00 -0.008 0.021 0.003

250.0000 1 .A52E+00 3.737E+01 3.882E+01 2.503E+01 8.731E-01 6.329E+00 -0.006 0.020 0.003

300.0000 1 .A6AE+00 A.509E+01 A.656E+01 2.621E+01 8.886E-01 6 .668E+00 -0.005 0.019 0.002

350.0000 1 .A75E+00 5.283E+01 5.A31 E+01 2.720E+01 9.003E-01 6.959E+00 -0.005 0.018 0.002

AOO .0000 1 .A8AE+00 6.058E+01 6 .206E+01 2.806E+01 9.096E-01 7.212E+00 -0 .OOA 0.018 0.002

A50 .0000 1 .A91E+00 6 .833E+01 6 . 982E+01 2.882E+01 9.171E-01 7.A37E+00 -O.OOA 0.017 0.001 500.0000 1 . A98E+00 7.609E+01 7.759E+01 2.950E+01 9.23AE-01 7 .639E+00 -0.003 0.017 0.001 550.0000 1 .505E+00 8.386E+01 8.536E+01 3.01 lE+01 9.287E-01 7.823E+00 -0.003 0.017 0.001 600.0000 1 .510E+00 9. 163E+01 9.31AE+01 3.067E+01 9.332E-01 7.991E+00 -0.003 0.016 0.001 700.0000 1 .520E+00 1 .072E+02 1 .087E+02 3. 167E+01 9. A06E-01 8.290E+00 -0.002 0.016 0.001 800.0000 1 .529E+00 1 .227E+02 1 .2A3E+02 3.253E+01 9. A6AE-01 8.550E+00 -0.002 0.015 0.001 900.0000 1 .536E+00 1 .383E+02 1 .398E+02 3.328E+01 9.51 lE-01 8.780E+00 -0.002 0.015 0.001 1000.0000 1 .5A3E+00 1 .539E+02 1 .55AE+02 3.396E+01 9.5A9E-01 8.986E+00 -0.002 0.015 0.001

159
POSITRONS IN AIR, DRY (NEAR SEA LEVEL)

I = 85.7 eV DENSITY = 1.205E-03 g/cm^ (20<> C)

ENERGY STOPPING POWER CSDA RADIATION DENS.EFF. ddog1 )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm^/g g/cm ^ 0.0100 2. 180E+01 3.897E-03 2.180E+01 2.571E-09 9.658E-05 0.0 -0.185 0.208 0.207

0.0125 1 .825E+01 3.921E-03 1 .825E + 01 3.830E-09 1 .167E-09 0.0 -0.178 0.199 0.198

0.0150 1 .578E+01 3. 937E-03 1 .579E+01 5.307E-09 1 .359E-09 0.0 -0.173 0.193 0.192

0.0175 1 . 396E+01 3 . 996E-03 1 .397E+01 6.995E-09 1 .595E-09 0.0 -0.169 0.187 0.186 0.0200 1 .256E+01 3. 959E-03 1 .256E+01 8.885E-09 1 .725E-09 0.0 -0.165 0.183 0.182

0.0250 1 .053E+01 3.966E-03 1 .053E+01 1 .325E-03 2.072E-09 0.0 -0.160 0.176 0.176

0.0300 9.126E+00 3.976E-03 9.130E+00 1 .837E-03 2.909E-09 0.0 -0.156 0.171 0.171 0.0350 8.096E+00 3.986E-03 8. 100E+00 2.91 9E-03 2.723E-09 0.0 -0.153 0.167 0.167

O.OAOO 7.306E+00 3. 998E-03 7.310E+00 3.070E-03 3.032E-09 0.0 -0.150 0.169 0.163

0 .0A50 6 .680E+00 9.01 lE-03 6.689E+00 3.787E-03 3.333E-09 0.0 -0.198 0.161 0.160

0.0500 6.171E+00 9.025E-03 6 . 175E+00 9.566E-03 3.626E-09 0.0 -0.196 0.158 0.158

0.0550 5.799E+00 9.090E-03 5.753E+00 5.905E-03 3.912E-09 0.0 -0.199 0.156 0.156

0.0600 5.393E+00 9.057E-03 5.397E+00 6.303E-03 9.192E-09 0.0 -0.193 0.159 0.159

0.0700 9.826E+00 9.093E-03 9.830E+00 8.266E-03 9.735E-09 0.0 -0.190 0.151 0.151 0.0800 9.393E+00 9.133E-03 9.397E+00 1 .099E-02 5.261E-09 0.0 -0.138 0.199 0.199

0.0900 9.052E+00 9. 175E-03 9.056E+00 1 .281E-02 5.771E-09 0.0 -0.137 0.197 0.196

0.1000 3.776E+00 9.222E-03 3.780E+00 1 .537E-02 6.267E-09 0.0 -0.135 0.195 0.195

0.1250 3.279E+00 9.398E-03 3.278E+00 2.250E-02 7.958E-09 0.0 -0.132 0.191 0.191

0 . 1 500 2.935E+00 9.985E-03 2.990E+00 3.057E-02 8.593E-09 0.0 -0.130 0.138 0.138

0.1750 2.692E+00 9.633E-03 2.697E+00 3.997E-02 9.683E-09 0.0 -0.128 0.136 0.136

0.2000 2.510E+00 9.789E-03 2.515E+00 9. 908E-02 1 .079E-03 0.0 -0.126 0.139 0.139

0.2500 2.257E+00 5. 126E-03 2.262E+00 7.013E-02 1 .276E-03 0.0 -0.129 0.132 0.131 0.3000 2.091E+00 5.995E-03 2.097E+00 9.319E-02 1 .971E-03 0.0 -0.122 0.129 0.129

0.3500 1 .976E+00 5.890E-03 1 .982E+00 1 . 177E-01 1 .660E-03 0.0 -0.120 0.127 0.127

O.AOOO 1 .893E+00 6.31 IE-03 1 .899E+00 1 .935E-01 1 .896E-03 0.0 -0.118 0.126 0.125

0.9500 1 .831E+00 6.757E-03 1 .838E+00 1 .703E-01 2.030E-03 0.0 -0.117 0.129 0.123

0.5000 1 .789E+00 7.223E-03 1 .791E+00 1 .978E-01 2.212E-03 0.0 -0.116 0.123 0.122

0.5500 1 .798E+00 7.708E-03 1 .755E+00 2.261E-01 2.399E-03 0.0 -0.119 0.122 0.121 0.6000 1 .71 9E+00 8.210E-03 1 .727E+00 2.598E-01 2.575E-03 0.0 -0.113 0.121 0.120

0.7000 1 .678E+00 9.258E-03 1 .687E+00 3. 139E-01 2.939E-03 0.0 -0.111 0.119 0.118

0.8000 1 .652E+00 1 .036E-02 1 .663E+00 3.731E-01 3.309E-03 0.0 -0.109 0.118 0.116

0 . 9000 1 .636E+00 1 .151E-02 1 .698E+00 9.336E-01 3.671E-03 0.0 -0.108 0.116 0.119

1 .0000 1 .626E+00 1 .271E-02 1 .639E+00 9.995E-01 9.091E-03 0.0 -0.107 0.115 0.113

1 .2500 1 .617E+00 1 .588E-02 1 .633E+00 6.979E-01 9.980E-03 0.0 -0.109 0.113 0.110

1 .5000 1 .621E+00 1 .927E-02 1 .690E+00 8.002E-01 5.939E-03 0.0 -0.101 0.110 0.107

1 .7500 1 .630E+00 2.289E-02 1 .653E+00 9.521E-01 6 .916E-03 0.0 -0.099 0.109 0.105

2.0000 1 .692E+00 2.656E-02 1 .669E+00 1 . 103E+00 7.910E-03 0.0 -0.097 0.107 0.103

2.5000 1 .668E+00 3.937E-02 1 .703E+00 1 .399E+00 9.936E-03 0.0 -0.095 0.109 0.100

3.0000 1 .695E+00 9.260E-02 1 .738E+00 1 .690E+00 1 .200E-02 0.0 -0.092 0.102 0.097

3.5000 1 .720E+00 5.115E-02 1 .772E+00 1 .975E+00 1 .910E-02 0.0 -0.091 0.100 0.095

9.0000 1 .799E+00 5. 999E-02 1 .809E+00 2.255E+00 1 .622E-02 0.0 -0.089 0.099 0.093

9 . 5000 1 .766E+00 6 . 908E-02 1 .835E+00 2.529E+00 1 .836E-02 0.0 -0.088 0.097 0.091 5.0000 1 .786E+00 7.838E-02 1 .865E+00 2.800E+00 2.051E-02 0.0 -0.087 0.096 0.090

5.5000 1 .805E+00 8.787E-02 1 .893E+00 3.066E+00 2.266E-02 0.0 -0.086 0.095 0.089

6.0000 1 .823E+00 9.759E-02 1 .920E+00 3.328E+00 2.983E-02 0.0 -0.085 0.099 0.087

7.0000 1 .859E+00 1 .173E-01 1 .972E+00 3.892E+00 2.916E-02 0.0 -0.083 0.092 0.085

8.0000 1 .883E+00 1 .376E-01 2.020E+00 9.393E+00 3.399E-02 0.0 -0.082 0.090 0.083

9.0000 1 .908E+00 1 .589E-01 2.066E+00 9.832E+00 3.782E-02 0.0 -0.081 0.089 0.082

10.0000 1 . 931E+00 1 .795E-01 2.110E+00 5.31 lE+00 9.212E-02 0.0 -0.080 0.087 0.080

12.5000 1 . 980E+00 2.337E-01 2.219E+00 6.967E+00 5.278E-02 0.0 -0.078 0.089 0.077

15.0000 2.020E+00 2.895E-01 2.310E+00 7.573E+00 6.323E-02 0.0 -0.076 0.082 0.079

17.5000 2.055E+00 3.969E-01 2.901E+00 8.639E+00 7.396E-02 0.0 -0.075 0.080 0.072

20.0000 2.085E+00 9.092E-01 2.989E+00 9.656E+00 8.395E-02 0.0 -0.079 0.078 0.070

25.0000 2. 136E+00 5.21 9E-01 2.657E+00 1 .160E+01 1 .027E-01 0.0 -0.072 0.075 0.066

30.0000 2. 176E+00 6.917E-01 2.818E+00 1 .393E+01 1 .210E-01 7.636E-03 -0.069 0.072 0.063

35.0000 2.208E+00 7.630E-01 2.971E+00 1 .515E+01 1 .383E-01 5.989E-02 -0.053 0.069 0.058

90.0000 2.232E+00 8.855E-01 3.1 18E+00 1 .680E+01 1 .598E-01 1 .378E-01 -0.095 0.066 0.053

95.0000 2.252E+00 1 .009E+00 3.261E+00 1 .836E+01 1 .706E-01 2.266E-01 -0.090 0.063 0.099

50.0000 2.269E+00 1 . 1 33E+00 3.903E+00 1 .986E+01 1 .857E-01 3.192E-01 -0.036 0.060 0.095

55.0000 2.289E+00 1 .258E+00 3.592E+00 2.130E+01 2.001E-01 9.120E-01 -0.033 0.057 0.091 60.0000 2.297E+00 1 .389E+00 3.681 E+00 2.269E+01 2.139E-01 5.029E-01 -0.031 0.055 0.038

70.0000 2.31 9E+00 1 .637E+00 3.956E+00 2.531E+01 2.398E-01 6.762E-01 -0.027 0.051 0.033

80.0000 2.337E+00 1 .892E+00 9.229E+00 2.775E+01 2.637E-01 8.365E-01 -0.025 0.098 0.030

90.0000 2.353E+00 2.198E+00 9.501E+00 3.005E+01 2.858E-01 9.892E-01 -0.023 0.095 0.027

100.0000 2.367E+00 2.905E+00 9.772E+00 3.220E+01 3.063E-01 1 . 120E+00 -0.022 0.093 0.029

1 25.0000 2.395E+00 3.053E+00 5.998E+00 3.710E+01 3.517E-01 1 .91 9E+00 -0.020 0.039 0.020

1 50 .0000 2.918E+00 3.705E+00 6.122E+00 9.193E+01 3.909E-01 1 .670E+00 -0.019 0.036 0.017

175.0000 2.936E+00 9.360E+00 6 .796E+00 9.530E+01 9.237E-01 1 .887E+00 -0.018 0.033 0.015

200 .0000 2.952E+00 5.018E+00 7.970E+00 9.881E+01 9.529E-01 2.078E+00 -0.017 0.031 0.013

250.0000 2.979E+00 6.390E+00 8.818E+00 5.996E+01 5.016E-01 2.903E+00 -0.016 0.028 0.011 300.0000 2.500E+00 7.667E+00 1 .017E+01 6.029E+01 5.909E-01 2.675E+00 -0.015 0.026 0.009

350.0000 2.517E+00 8. 998E+00 1 .152E+01 6.986E+01 5.739E-01 2.909E+00 -0.019 0.025 0.008

900.0000 2.532E+00 1 .033E+01 1 .286E+01 6.896E+01 6.008E-01 3.116E+00 -0.013 0.023 0.007

950.0000 2.595E+00 1 . 1 67E+01 1 .922E+01 7.266E+01 6.293E-01 3.302E+00 -0.012 0.022 0.007

500.0000 2.556E+00 1 .301E+01 1 .557E+01 7.602E+01 6.997E-01 3.972E+00 -0.011 0.021 0.006

550.0000 2.566E+00 1 .935E+01 1 .692E+01 7.910E+01 6.627E-01 3.628E+00 -0.011 0.021 0.006

600.0000 2.575E+00 1 .569E+01 1 .827E+01 8.1 99E+01 6.786E-01 3.772E+00 -0.010 0.020 0.005

700.0000 2.590E+00 1 .838E+01 2.097E+01 8.705E+01 7.057E-01 9.039E+00 -0.008 0.019 0.005

800.0000 2.603E+00 2.107E+01 2.367E+01 9. 153E+01 7.279E-01 9.267E+00 -0.007 0.018 0.009

900.0000 2.619E+00 2.376E+01 2.638E+01 9.553E+01 7.966E-01 9.977E+00 -0.006 0.017 0.009

1000.0000 2.629E+00 2.696E+01 2.908E+01 9.919E+01 7.625E-01 9.668E+00 -0.005 0.017 0.003

160
POSITRONS IN POLYMETHYL METHACRYLATE, "LUCITE PERSPEX", "PLEXIGLAS

ENERGY

MeV

0.0100

0.0125

0.0150

0.0175

0.0200

0.0250

0.0300

0.0350

0 .OAOO 0.0A50

0.0500

0.0550

0.0500

0.0700

0.0800

0.0900

0.1000

0.1250

0.1500

0.1750

0.2000

0.2500

0.3000

0.3500

0. AOOO 0.A500

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

STOPPING POWER

COLLISION RADIATIVE

MeV cm^/g MoV cm^/g

A5

5

678 . 9.

10 . 12 . 15. 17. 20 . 25.

30.

35. AO.

A5.

50.

55.

60.

70. 80.

90. 100 . 125,

150.

175. 200 . 250.

300.

350. AOO,

A50.

500,

550, 600 , 700, 800 , 900

,0000

,5000 0000

,5000

,0000

,0000

,0000

,0000

,0000

,5000

,0000

,5000

,0000

,0000

,0000

.0000 ,0000

.0000

.0000

.0000

.0000

.0000

,0000 .0000

.0000 0000

0000

0000

0000

0000

0000 0000

0000 0000

0000 0000

0000

0000

0000

0000

2. A1 9E+01 2.023E+01

1 .7A9E+01

1 .5A6E+01

1 .390E+01

1 . 16AE+01

1 .009E+01 8.9A3E+00

8.068E+00

7.37AE+00

6.810E+00

6.3A3E+00

5. 9A9E+00

5.321E+00

A.8A2E+00

A.A65E+00

A.161E+00

3.606E+00

3.232E+00

2.963E+00

2.762E+00

2. A82E+00

2.300E+00

2.173E+00

2.081E+00

2.01 lE+00

1 .956E+00

1 .912E+00

1 .877E+00

1 .826E+00

1 .791E+00

1 .767E+00

1 .750E+00

1 .726E+00

1 .716E+00

1 .71 AE + 00

1 .716E+00

1 .72AE+00

1 .736E+00

1 .7A8E+00

1 .759E+00

1 .770E+00

1 .781E+00

1 .791E+00

1 .800E+00

1 .816E+00

1 .831E+00

1 .8AAE+00

1 .855E+00

1 .880E+00

1 .899E+00

1 .915E+00

1 .929E+00

1 .951E+00

1 .968E+00

1 .983E+00

1 .995E+00

2.005E+00

2.015E+00

2.023E+00

2.031 E+00 2.0AAE+00

2.055E+00

2.065E+00

2.07AE+00

2.093E+00

2. 108E+00

2. 121E+00

2.1 33E+00

2. 151E+00

2. 166E+00

2.179E+00

2.1 90E+00 2.200E+00

2.209E+00

2.217E+00

2.22AE+00

2.237E+00

2.2A8E+00

2.257E+00

3.332E-03

3.3A9E-03

3.359E-03

3.366E-03

3. 372E-03

3.382E-03

3.391E-03

3.A01E-03

3.A1 3E-03

3. A25E-03

3. A38E-03

3. A53E-03

3.A68E-03

3.502E-03

3.538E-03

3.577E-03

3.61 9E-03

3.732E-03

3.855E-03

3.987E-03

A.126E-03

A.A25E-03

A.751E-03

5.101E-03

5. A7AE-03

5.867E-03

6 .278E-03

6.707E-03

7.1A9E-03

8.076E-03

9.050E-03

1 .007E-02

1 .1 13E-02

1 .393E-02

1 -693E-02

2.009E-02

2.338E-02

3.031E-02

3.761E-02

A.521E-02

5.307E-02

6.115E-02

6.9A3E-02

7.788E-02

8.6A8E-02

1 .OAlE-01

1 .222E-01

1 . A07E-01

596E-01

079E-01

577E-01 086E-01

603E-01

656E-01

728E-01

815E-01

7.912E-01

9.020E-01

1 .01 3E + 00

1 . 126E+00

1 .238E+00

1 . A65E+00

1 .69AE+00

1 .92AE+00

2.155E+00

2.737E+00

3.323E+00

3.912E+00

A.503E+00

5.692E+00

6 .887E+00 8.085E+00

9.286E+00

1 .0A9E+01

1 . 170E+01

1 .290E+01

1 .A1 lE+01

1 .653E+01

1 .896E+01 2.139E+01

1000.0000 2.266E+00 2.382E+01

7A.0 eV DENSITY = 1 .190E+001 g/cm^

CSDA RADIATION DENS. EPF. dClog )/d(logI)

TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MoV cmVg g/cm^

2. A1 9E+01 2.309E-0A 7.A61E-05 0.0 -0.180 0.202 0.201 2.02AE+01 3. AAAE-OA 9.003E-05 0.0 -0.17A 0. 1 9A 0.193

1 .7A9E+01 A.777E-0A 1 .0A8E-0A 0.0 -0.169 0.187 0.186

1 .5A6E+01 6.301E-OA 1 .191E-0A 0.0 -0.165 0.182 0.182

1 .390E+01 8.009E-0A 1 .330E-0A 0.0 -0.161 0.178 0.177

1 . 16AE+01 1 . 1 96E-03 1 .598E-0A 0.0 -0.156 0.172 0.171

1 .009E+01 1 .659E-03 1 .85AE-0A 0.0 -0.152 0.167 0.166

8.9A7E+00 2. 186E-03 2.101E-0A 0.0 -0.1A9 0.163 0.163

8.071E+00 2.775E-03 2.3AOE-OA 0.0 -0.1A7 0.160 0.159

7.377E+00 3.A2AE-03 2.573E-0A 0.0 -0. 1 A5 0.157 0.157

6.81AE+00 A.130E-03 2.800E-0A 0.0 -0.1A3 0.155 0.155

6.3A7E+00 A.891E-03 3.022E-0A 0.0 -0.1A1 0.153 0.153

5. 953E+00 5.705E-03 3.2A0E-0A 0.0 -0.1 AO 0.151 0.151 5.325E+00 7.A85E-03 3.66AE-0A 0.0 -0.138 0. 1 A8 0.1 A8 A.8A6E+00 9.A57E-03 A.073E-0A 0.0 -0.136 0.1 A6 0.1 A5

A. A69E+00 1 .161E-02 A.A71E-0A 0.0 -0.1 3A O.IAA 0 . 1 A3

A. 16AE+00 1 .393E-02 A.859E-0A 0.0 -0.133 0.1 A2 0.1A2

3.609E+00 2.0A0E-02 5.791E-0A 0.0 -0.130 0.138 0.138

3.235E+00 2.77AE-02 6.682E-0A 0.0 -0.127 0.136 0.135

2. 967E+00 3.582E-02 7.538E-0A 0.0 -0.126 0.1 3A 0.133

2.766E+00 A. A56E-02 8.368E-0A 0.0 -0.1 2A 0.132 0.131 2.A87E+00 6.370E-02 9.967E-0A 0.0 -0.122 0.129 0.129

2.30AE+00 8.A63E-02 1 .151E-03 0.0 -0.120 0.127 0.126

2.178E+00 1 .070E-01 1 .301E-03 0.0 -0.118 0.125 0.12A

2.086E+00 1 .305E-01 1 . AA9E-03 0.0 -0.118 0.1 2A 0.123

2.017E+00 1 .5A9E-01 1 .595E-03 1 . A66E-02 -0.093 0.120 0.119

1 .962E+00 1 .800E-01 1 .7A1E-03 A.112E-02 -0.087 0.116 0.1 1A

1 .919E+00 2.058E-01 1 .887E-03 6.992E-02 -0.082 0.112 0.109

1 .885E+00 2.321E-01 2.033E-03 1 .005E-01 -0.077 0.108 0.10A

1 .83AE+00 2.859E-01 2.328E-03 1 .650E-01 -0.069 0.102 0.096

1 .800E+00 3.A10E-01 2.626E-03 2.321E-01 -0.063 0.096 0.090

1 .777E+00 3.969E-01 2.928E-03 3.001E-01 -0.058 0.091 0.08A

1 .761E+00 A.535E-01 3.235E-03 3.679E-01 -0.05A 0.086 0.078

1 .7A0E+00 5.96AE-01 A.019E-03 5.330E-01 -0.0A7 0.078 0.068

1 .733E+00 7.A05E-01 A.830E-03 6.887E-01 -0.0A2 0.071 0.061

1 .73AE+00 8.8A7E-01 5.66AE-03 8.339E-01 -0.039 0.066 0.055

1 .739E+00 1 .029E+00 6.520E-03 9.689E-01 -0.036 0.062 0.051

1 .755E+00 1 .315E+00 8.286E-03 1 .212E+00 -0.033 0.056 0.0A5

1 .773E+00 1 .598E+00 1 .01 IE-02 1 .A25E+00 -0.030 0.051 O.OAO

1 .793E+00 1 .879E+00 1 .198E-02 1 .613E+00 -0.029 O.OA8 0.037

1 .812E+00 2. 156E+00 1 .389E-02 1 .783E+00 -0.027 0.0A5 0.035

1 .832E+00 2.A31E+00 1 .583E-02 1 .936E+00 -0.026 0.0A3 0.033

1 .850E+00 2.702E+00 1 .779E-02 2.077E+00 -0.025 0.0A1 0.031

1 .869E+00 2.971E+00 1 .977E-02 2.207E+00 -0.02A O.OAO 0.030

1 .886E+00 3.237E+00 2. 177E-02 2.327E+00 -0.02A 0.038 0.029

1 .920E+00 3.763E+00 2.581E-02 2.5A5E+00 -0.022 0.036 0.027

1 .953E+00 A.279E+00 2.988E-02 2.739E+00 -0.021 0.03A 0.025

1 .985E+00 A.787E+00 3.398E-02 2.91AE+00 -0.020 0.033 0.02A

2.015E+00 5.287E+00 3.809E-02 3.073E+00 -0.019 0.031 0.023

2.088E+00 6.506E+00 A.836E-02 3. A21E+00 -0.016 0.028 0.020

2. 157E+00 7.68AE+00 5.856E-02 3.716E+00 -0.01 A 0.026 0.018

2.22AE+00 8.825E+00 6.865E-02 3.97AE+00 -0.012 0.02A 0.016

2.289E+00 9. 933E+00 7.859E-02 A.202E+00 -0.010 0.022 O.OIA 2.A17E+00 1 .206E+01 9.792E-02 A.596E+00 -0.008 0.020 0.012

2.5A1E+00 1 .A08E+01 1 . 165E-01 A.927E+00 -0.006 0.018 0.010

2.66AE+00 1 .600E+01 1 .3A2E-01 5.212E+00 -0.005 0.016 0.008

2.786E+00 1 .783E+01 1 .512E-01 5.A63E+00 -O.OOA 0.015 0.007

2.907E+00 1 .959E+01 1 .67AE-01 5.687E+00 -0.003 O.OIA 0.006

3.028E+00 2.127E+01 1 .830E-01 5.889E+00 -0.003 0.013 0.006

3. 1 A9E+00 2.289E+01 1 . 978E-01 6.072E+00 -0.002 0.012 0.005

3.269E+00 2. AA5E+01 2.120E-01 6.2A1E+00 -0.002 0.011 O.OOA 3.509E+00 2.7A0E+01 2.387E-01 6.5A1E+00 -0.001 0.010 O.OOA 3.750E+00 3.016E+01 2.632E-01 6.803E+00 -0.001 0.009 0.003

3.990E+00 3.27AE+01 2.859E-01 7.03AE+00 -0.001 0.009 0.003

A.230E+00 3.518E+01 3.069E-01 7.2A2E+00 -0.001 0.008 0.002

A .830E+00 A.070E+01 3.53AE-01 7.683E+00 -0.001 0.007 0.002

5.A31E+00 A.558E+01 3. 928E-01 8.0A5E+00 -0.000 0.006 0.001

6 .033E+00 A.995E+01 A.268E-01 8.351E+00 -0.000 0.006 0.001

6 .636E+00 5.390E+01 A.565E-01 8.617E+00 -0.000 0.005 0.001 7.8A3E+00 6 .082E+01 5.059E-01 9.061E+00 -0.000 0.005 0.001 9.053E+00 6.675E+01 5. A56E-01 9.A25E+00 -0.000 O.OOA 0.001

1 .026E+01 7.193E+01 5.783E-01 9.733E+00 -0.000 O.OOA 0.000

1 . 1 A8E+01 7.65AE+01 6.059E-01 9.999E+00 -0.000 O.OOA 0.000

1 .269E+01 8.068E+01 6.295E-01 1 .023E+01 -0.000 O.OOA 0.000

1 .391E+01 8. AAAE+01 6.A99E-01 1 .OAAE+01 -0.000 0.003 0.000

1 .512E+01 8.789E+01 6.679E-01 1 .06AE+01 -0.000 0.003 0.000

1 .63AE+01 9. 107E+01 6.838E-01 1 .081E+01 -0.000 0.003 0.000

1 .877E+01 9.678E+01 7.108E-01 1 .112E+01 -0.000 0.003 0.000

2. 1 21 E+01 1 .018E+02 7.329E-01 1 .138E+01 -0.000 0.003 0.000

2.36AE+01 1 .062E+02 7.51AE-01 1 .162E+01 -0.000 0.003 0.000

2.608E+01 1 . 103E+02 7.672E-01 1 . 183E+01 -0.000 0.003 0.000

161
POSITRONS IN WATER. LIQUID

I = 75.0 eV DENSITY = 1 .OOOE+001 g/cm

ENERGY STOPPING POWER CSDA RADIATION DEHS.EFF. dClog )/d(logI) COLLISION RADIATIVE TOTAL RANGE YIELD CORR. COLL CSDA RAD

(DELTA) LOSS RANGE YIELD

MeV MeV cm^/g MeV cm^/g MeV cm7/g g/cm ^ 0.0100 2.983E+01 3.89SE-03 2.989E+01 2.250E-09 8.925E-05 0.0 -0.181 0.202 0.201 0.0125 2.077E+01 3. 927E-03 2.078E+01 3.356E-09 1 .020E-09 0.0 -0.179 0.199 0.193

0.0150 1 .795E+01 3. 999E-03 1 .796E+01 9.659E-09 1 .191E-09 0.0 -0.169 0.188 0.187

0.0175 1 .587E+01 3.955E-03 1 .588E+01 6. 138E-09 1 .356E-09 0.0 -0.165 0.183 0.182

0 .0200 1 .927E+01 3. 963E-03 1 .927E+01 7.801 E-09 1 .515E-09 0.0 -0.162 0.179 0.178

0.0250 1 . 1 96E+01 3 . 979E-03 1 . 1 96E+01 1 .165E-03 1 .823E-09 0.0 -0.157 0.172 0.171 0.0300 1 .036E+01 3.989E-03 1 .036E+01 1 .615E-03 2.117E-09 0.0 -0.153 0.167 0.167

0.0350 9. 185E+00 3. 999E-03 9. 189E + 00 2.129E-03 2.900E-09 0.0 -0.150 0.163 0.163

O.OAOO 8.286E+00 9.005E-03 8.290E+00 2.703E-03 2.673E-09 0.0 -0.197 0.160 0.160

0.0A50 7.579E+00 9.018E-03 7.578E+00 3.339E-03 2. 939E-09 0.0 -0.195 0.157 0.157

0.0500 6.995E+00 9.031E-03 6 . 999E+00 9.021E-03 3.1 99E-09 0.0 -0.193 0.155 0.155

0.0550 6.516E+00 9.096E-03 6.520E+00 9.762E-03 3.952E-09 0.0 -0.192 0.153 0.153

0 .0600 6.111 E+00 9.062E-03 6. 1 15E+00 5.555E-03 3.700E-09 0.0 -0.190 0.151 0.151 0.0700 5.966E+00 9.098E-03 5.970E+00 7.287E-03 9.181E-09 0.0 -0.138 0.198 0.198

0 . 0800 9.979E+00 9. 1 38E-03 9. 979E+00 9.207E-03 9.696E-09 0.0 -0.136 0.196 0.196

0.0900 9.587E+00 9. 181E-03 9.591E+00 1 . 1 30E-02 5.098E-09 0.0 -0.139 0.199 0.199

0.1000 9.279E+00 9.228E-03 9.279E+00 1 .356E-02 5.538E-09 0.0 -0.133 0.192 0.192

0.1250 3 . 709E+00 9.355E-03 3.709E+00 1 .986E-02 6 .599E-09 0.0 -0.130 0.139 0.138

0.1500 3. 320E+00 9.999E-03 3. 325E+00 2.700E-02 7.601E-09 0.0 -0.128 0.136 0.136

0.1750 3.099E+00 9.693E-03 3.099E+00 3.987E-02 8.569E-09 0.0 -0.126 0.139 0.133

0.2000 2.838E+00 9.801E-03 2.893E+00 9.337E-02 9.506E-09 0.0 -0.129 0.132 0.132

0 . 2500 2.551E+00 5. 1 91 E-03 2.556E+00 6.199E-02 1 .131E-03 0.0 -0.122 0.129 0.129

0.3000 2. 363E+00 5.519E-03 2.368E+00 8.236E-02 1 .309E-03 0.0 -0.120 0.127 0.126

0.3500 2.233E+00 5. 91 3E-03 2.238E+00 1 .091E-01 1 .973E-03 0.0 -0.118 0.125 0.125

0.9000 2.138E+00 6 . 339E-03 2.195E+00 1 .270E-01 1 .638E-03 0.0 -0.116 0.129 0.123

0.9500 2 . 068E+00 6.787E-03 2.075E+00 1 .507E-01 1 .802E-03 0.0 -0.115 0.122 0.121

0 . 5000 2.019E+00 7.257E-03 2.021E+00 1 .751E-01 1 .965E-03 0.0 -0.113 0.121 0.120

0.5500 1 . 971 E+00 7.797E-03 1 .979E+00 2.001E-01 2.128E-03 1 . 103E-02 -0.095 0.119 0.117

0 .6000 1 . 937E+00 8.259E-03 1 .995E+00 2.256E-01 2.290E-03 2. 938E-02 -0.090 0.116 0.113

0.7000 1 .886E+00 9.312E-03 1 .895E+00 2.777E-01 2.617E-03 7.935E-02 -0.080 0.110 0.106

0.8000 1 .851E+00 1 .093E-02 1 .862E+00 3.310E-01 2.997E-03 1 .267E-01 -0.072 0.109 0.099

0 . 9000 1 .827E+00 1 . 1 59E-02 1 .839E+00 3.851E-01 3.280E-03 1 .835E-01 -0.065 0.099 0.093

1 .0000 1 .810E+00 1 .280E-02 1 .823E+00 9.397E-01 3.618E-03 2.928E-01 -0.060 0.095 0.087

1 .2500 1 .786E+00 1 .600E-02 1 .802E+00 5.777E-01 9.983E-03 3.999E-01 -0.050 0.085 0.076

1 .5000 1 .777E+00 1 . 992E-02 1 .796E+00 7.167E-01 5.375E-03 5.937E-01 -0.099 0.078 0.067

1.7500 1 .775E+00 2.303E-02 1 .798E+00 8.559E-01 6.299E-03 6.866E-01 -0.039 0.072 0.060

2.0000 1 .776E+00 2.678E-02 1 .803E+00 9.997E-01 7.235E-03 8.218E-01 -0.036 0.067 0.059

2.5000 1 .785E+00 3.968E-02 1 .820E+00 1 .271E+00 9. 177E-03 1 .069E+00 -0.031 0.059 0.096

3.0000 1 .796E+00 9.299E-02 1 .839E+00 1 .599E+00 1 . 1 18E-02 1 .288E+00 -0.028 0.059 0.091 3.5000 1 .808E+00 5.169E-02 1 .859E+00 1 .815E+00 1 .329E-02 1 .989E+00 -0.026 0.050 0.037

9.0000 1 .819E+00 6.058E-02 1 .879E+00 2.082E+00 1 .533E-02 1 .660E+00 -0.029 0.097 0.039

9.5000 1 .830E+00 6.976E-02 1 .899E+00 2.397E+00 1 .796E-02 1 .821E+00 -0.023 0.099 0.031 5.0000 1 .890E+00 7.917E-02 1 .919E+00 2.609E+00 1 .961E-02 1 .967E+00 -0.022 0.092 0.030

5.5000 1 .899E+00 8.876E-02 1 .938E+00 2.868E+00 2. 179E-02 2.102E+00 -0.022 0.090 0.028

6 .0000 1 .858E+00 9.859E-02 1 . 957E+00 3. 125E+00 2.398E-02 2.227E+00 -0.021 0.038 0.027

7.0000 1 .875E+00 1 . 185E-0I 1 .993E+00 3.631E+00 2.890E-02 2.953E+00 -0.020 0.036 0.025

8.0000 1 .889E+00 1 .391E-01 2.028E+00 9.128E+00 3.285E-02 2.652E+00 -0.019 0.039 0.023

9 .0000 1 .902E+00 1 .601E-01 2.062E+00 9.617E+00 3.732E-02 2.831E+00 -0.019 0.032 0.022

10.0000 1 . 91 9E+00 1 .819E-01 2.095E+00 5.098E+00 9. 180E-02 2.992E+00 -0.018 0.030 0.021 12.5000 1 . 939E+00 2.362E-01 2.175E+00 6.269E+00 5.297E-02 3.391E+00 -0.017 0.028 0.019

15.0000 1 . 959E+00 2.926E-01 2.252E+00 7.398E+00 6.903E-02 3.633E+00 -0.015 0.026 0.017

1 7 . 5000 1 .976E+00 3.501E-01 2.327E+00 8.990E+00 7.992E-02 3.885E+00 -0.019 0.029 0.016

20.0000 1 .991E+00 9.086E-01 2.900E+00 9.598E+00 8.561E-02 9.107E+00 -0.013 0.023 0.015

25.0000 2.015E+00 5.277E-01 2.592E+00 1 . 157E+01 1 .063E-01 9.987E+00 -0.011 0.020 0.013

30.0000 2.039E+00 6.989E-01 2.683E+00 1 .399E+01 1 .261E-01 9.806E+00 -0.009 0.018 0.011 35.0000 2.099E+00 7.716E-01 2.821E+00 1 .530E+01 1 .999E-01 5.082E+00 -0.007 0.017 0.010

90.0000 2.062E+00 8. 955E-01 2. 958E+00 1 .703E+01 1 .629E-01 5.326E+00 -0.006 0.016 0.009

95.0000 2.079E+00 1 .021E+00 3.099E+00 1 .869E+01 1 .799E-01 5.599E+00 -0.005 0.015 0.008

50.0000 2.089E+00 1 . 1 96E+00 3.230E+00 2.027E+01 1 .962E-01 5.791E+00 -0.009 0.019 0.007

55.0000 2. 093E+00 1 .273E+00 3.366E+00 2. 178E+01 2.117E-01 5.921E+00 -0.009 0.013 0.006

60.0000 2.101E+00 1 .900E+00 3.501E+00 2.329E+01 2.265E-01 6.087E+00 -0.003 0.012 0.006

70.0000 2.115E+00 1 .656E+00 3.771E+00 2.599E+01 2.591E-01 6 .383E + 00 -0.003 0.011 0.005

80.0000 2.1 27E+00 1 . 91 9E+00 9.091E+00 2.855E+01 2.795E-01 6.691E+00 -0.002 0.010 0.009

90.0000 2.137E+00 2. 173E+00 9.31 1E+00 3.095E+01 3.028E-01 6.871E+00 -0.002 0.010 0.009

100.0000 2. 197E+00 2.939E+00 9.580E+00 3.320E+01 3.293E-01 7.077E+00 -0.001 0.009 0.003

125.0000 2. 166E+00 3.089E+00 5.255E+00 3.829E+01 3.716E-01 7.516E+00 -0.001 0.008 0.002

150.0000 2. 182E+00 3.799E+00 5. 931 E+00 9.277E+01 9. 1 15E-01 7.876E+00 -0.001 0.007 0.002

175.0000 2.195E+00 9.912E+00 6.608E+00 9.676E+01 9.956E-01 8. 182E+00 -0.001 0.007 0.002

200 .0000 2.207E+00 5 . 078E+00 7.285E+00 5.036E+01 9.753E-01 8.997E+00 -0.000 0.006 0.001 250.0000 2.226E+00 6.916E+00 8.692E+00 5.665E+01 5.299E-01 8.891E+00 -0.000 0.005 0.001 300.0000 2.292E+00 7.760E+00 1 .OOOE+01 6.203E+01 5.637E-01 9.259E+00 -0.000 0.005 0.001 350.0000 2.255E+00 9 . 1 07E+00 1 , 1 36E+01 6.671E+01 5.959E-01 9.561E+00 -0.000 0.005 0.001 900.0000 2.266E+00 1 .096E+01 1 .273E+01 7.087E+01 6.229E-01 9.827E+00 -0.000 0.009 0.001 950.0000 2.276E+00 1 . 181E+01 1 .909E+01 7.960E+01 6.960E-01 1 .006E+01 -0.000 0.009 0.001 500.0000 2.285E+00 1 .317E+01 1 .595E+01 7.799E+01 6.659E-01 1 .027E+01 -0.000 0.009 0.000 550.0000 2.299E+00 1 .953E+01 1 .682E+01 8.109E+01 6.839E-01 1 .096E+01 -0.000 0.009 0.000

600.0000 2.301E+00 1 . 589E+01 1 .81 9E+01 8.395E+01 6.988E-01 1 .069E+01 -0.000 0.009 0.000

700.0000 2.319E+00 1 .861E+01 2.092E+01 8. 907E+01 7.250E-01 1 .099E+01 -0.000 0.003 0.000

800.0000 2.326E+00 2. 1 33E+01 2.366E+01 9.356E+01 7.963E-01 1 .121E+01 -0.000 0.003 0.000

900.0000 2.336E+00 2.906E+01 2.690E+01 9.756E+01 7.691E-01 1 .195E+01 -0.000 0.003 0.000 1000.0000 2.395E+00 2.679E+01 2.919E+01 1 .012E+02 7.793E-01 1 . 166E+01 -0.000 0.003 0.000

162
NBS>114A :ncv. s-7«i

U.S. DEPT. OF COMM.

BIBLIOGRAPHIC DATA

SHEET

1. PUBLICATION OR REPORT NO. NBSIR 82-2550

4. TITLE AND SUBTITLE

STOPPING POWERS AND RANGES OF ELECTRONS AND POSITRONS

7. AUTHORiS)

Martin J. Berger and Stephen M. Seltzer

9. PERFORMING ORGANIZATION NAME AND ADDRESS

NATIONAL BUREAU OF STANDARDS

DEPARTMENT OF COMMERCE

WASHINGTON. DC 20234

12. SPONSORING ORGANIZATION NAME AND COMPLETE ADDRESS rs/re«<, aiy. ziP)

'f. iSBcIpjwt's Accession No.

5. Public.ition Dntc August 1982

I. Performing Organization Code

Performing Organ. Report No.

I®. Pfoject/Task/Work Unit No.

11. Contract/Grant No,

13. Type of Report & Period Covered U.S. Dep. of Energy

Washington, D.C.

15. SUPPLEMENTARY NOTES

Office of Naval Research

Arlington, VA 22217

14. Sponsoring Agency Code

1

. Document describes a computer program; SF-185, FIPS Software Summary, is attached.

IS. ABSTRACT (A 200^word or factuetl ^umnuiry o( moat aiftnificant iritormatioT\. If document ir^eludes a significant bihliogrophy or

Jtteruture stirvay, mention it here.)

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

37 elements and 60 compounds, and for positrons in 8 materials. The tables

include (1) collision stopping powers (2) radiative stopping powers,

(3) total stopping powers, ‘{4) ranges (computed in the continuous-slowingdown approximation), (5) radiation yields (fraction of electron energy

converted into bremsstrahlung) , and (6) the logarithmic derivatives of all

these quantities with respect to the mean excitation energy of the medium.

These results are given at 81 energies between 1000 MeV and 10 keV.

Restricted collision stopping powers are tabulated for selected materials,

with cut-off energies of 1 , 10 and 100 keV. The principal new ingredients

in the preparation of these tables were: (1) a revision and updating of the mean excitation energies which enter into the Bethe stopping-power formula,

on the basis of the best available data from stopping-power measurements and

analyses of experimental oscillator-strength distributions and dielectricresponse functions; (2) use of the general formulation of Sternheimer and

Peierls for the density-effect correction to the collision stopping power;

and (3) use of theoretical bremsstrahlung cross sections of Tseng and Pratt.

1/. KF-Y WORD'V's/v to fi'.olve entries; /i]j}hni^eficnl order' capitalize or.Iy the first letter of the first key wori/ unlas n pr-ypet home;

1 »/»'.. / /;v n )f: t

Collision stopping power, electrons, positrons,

yield, radiative stopping power, range.

radiation

18. AVAiLABIUTY X Unlimited 19. SECURITY CLASS

(THIS REPORT)

21. NO. OF

PRINTED PAGES

1

. For Official DistriCi.tion. Do Not Release to NTlS

UNCLASSIFIED 164

Order From Sup. of Doc., U.S. Government Printing Office, Washington, DC

20402, SD Stock No. SN003-003-

20. SECURITY CLASS

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2?. Price $15.00

j Order From National Technical Information Service (NTIS), Springfield,

1, VA. 221 "'1 UNCLASSIFIED
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