NBSIR 73-176 (/«)

Comparison of Photon Interaction Data

Sets. Yl. McGuire and Kaman

Pliotoeffect Data.

G. L. Simmons.* J. H. Hubbell

*Science Applications, Inc. Huntsville. Alabama 35805

Center for Radiation Researcti

Institute for Basic Standards

National Bureau of Standards

Washington, D. C. 20234

May 1973

Interim Report for Period January March 1973

Prepared for Defense Nuclear Agency

Washington, D C. 20234

NBSIR 73-176

COMPARISON OF PHOTON INTERACTION DATA

SETS. VI. MCGUIRE AND KAMAN

PHOTOEFFECT DATA.

G. L. Simmons,* J. H. Hubbell

*Science Applications, Inc. Huntsville, Alabama 35805

*Center for Radiation Research

Institute for Basic Standards

National Bureau of Standards

Washington, D. C. 20234

May 1973

Interim Report for Period January-March 1973

This report is to be superseded by a future publication which will receive

general distribution and should be cited as a reference. Please consult the NBS Office of Technical Information and Publications to obtain the proper

citation.

Prepared for Defense Nuclear Agency

Washington, D. C. 20234

a

U. S. DEPARTMENT OF COMMERCE, Frederick B. Dent, Secretary

IMATIOIMAL BUREAU OF STANDARDS, Richard W. Roberts. Director

Abs tract

Photoeffect cross sections calculated by McGuire, covering the energy

range 0„0062 to 62.0 keV for elements with Z = 2 to 54, are compared with

values interpolated from results calculated by Veigele et al (Kaman) which

cover the energy range 0.1 to between 1.0 and 8,0 keV. This comparison is

presented in the form of percent differences between these two data sets,

with the Kaman values taken as the reference set . The cross sections are listed and the differences are tabulated over the energy range 0.103 to

62„0 keV, At the higher energies (above between 1.0 and 8,0 keV) in this

region of overlap, the Kaman values were fitted to experimental data, rather

than calculated from theory. Discrepancies ranged from less than 3% up to as much as a factor of ten in the iodine Mjy - My edge region at 0„620 keV.

From this comparison, and from graphical comparison of both sets with experimental data for carbon, aluminum and tin, we estimate that for Z = 2 to 54

the envelope of uncertainty of present calculated values in the region 0.1

to 1.0 keV is of the order of ± 20% except in the presence of resonance

absorption features where the uncertainty can be an order of magnitude.

I. Intro duct ion

1/

In a previous report (IV. Kaman and ENDF/B) in this series, we presented a

comparison of the photon cross section data set (0„1 to 1000 keV, Z = I to 94)

2,3 / 4/

given by Veigele et al (Kaman Corp.) with the ENDF/B library data set (1 keV

to 100 MeV, 87 elements with Z = 1 to 94).

In that report we also included a comparison of the total attenuation coef8/

ficients in the Kaman set with the light-element, low-Z set by Henke and Elgin.

The Henke and Elgin set, extending over the range 0.03 to 6.0 keV for Z = 2 to

18, was fitted and interpolated from available experimental data.

The Kaman cross section set in the region 0.1 to 1.0 keV, on the other hand,

was calculated from theory for all elements. For elements with Z greater than

21 (Sc) these calculations were extended to energies higher than 1 keV, in one

case up to 8.0 keV (Pu, Z = 94), above which, except for hydrogen, the Kaman set

consists of values derived from experimental data.

In this low-energy region, particularly below 1 keV, the total attenuation

coefficient is comprised almost entirely of the photoeffect cross section as

indicated in Table I. The remaining portions of the total cross section, the

coherent and incoherent scattering contributions, were calculated by means of

the customary scattering-factor, impul se -approximation approach throughout the

0„1 to 1000. keV energy range of the Kaman set. These scattering cross section

contributions enter only as small or negligible corrections to the total cross

section in the range 0.1 to 1.0 keV. Hence in this low energy region an examination of the total attenuation coefficient reduces essentially to an examination

of the photoeffect cross section.

In addition to the Kaman calculation of the photoeffect cross sections

below 1 keV, there also exists an independent systematic calculation

9/

of photoeffect cross sections by McGuire extending over the region
0.0062 keV (200oX) to 62.0 keV (O.ll) for elements with Z = 2 to 54. In this

report we compare the McGuire and Kaman theoretical photoeffect values in

the region 0.103 keV (120X) to 62.0 keV (O.2X), Z = 2 to 54.

The theoretical basis and calculational procedure for the Kaman low-energy

photoeffect cross section computation were briefly described in report IV of this

y

series. We similarly describe briefly as follows the McGuire calculations and

indicate some of the similarities and differences with respect to the Kaman

calculation, ' v

II. McGuire Photoeffect Calculations

Both the Kaman and McGuire soft x-ray theoretical photoeffect cross sections

were calculated using the dipole central-field model discussed in detail by

10/

Co oper. In this model, the contribution t ^ o f the subshell to the total

photoionization cross section is

4 a , T = — Tra a N . hv

n-L 3 0 n-t '\2l+l)^-l + (z^+lK+l i

where a is the fine- structure constant, a is the Bohr radius, N , is the sub0 n-t shell occupation number, hv is the photon energy in Rydbergs, and ^ are the

radial matrix elements for the transition of the electron from the bound state

with orbital quantum number to continuum states with = t ±1.

For the evaluations of the radial matrix elements % +-|^

, both the Kaman and

McGuire calculations used the dipole-length expression.

%-l = J ^nt(^>^ 1. 1 dr (2)

o

'

in which r is the electron radial position in Bohr units, e is the continuum

(photo-ejected) electron energy, and P^^(r) and P^ ^^^(r) are the bound and

continuum radial wave functions, respectively, of the photoelectron. These wave

2
functions P(r) were determined by solving the radial Schrodinger equation

+ V(r) + E - ^^^^ i P(r) = 0 (3) ,2 n 2 J dr r.

in which E is the energy (E <0) in Rydbergs of an electron in the nth subshell.

n n Values of the potential V(r) were taken from the tables of Herman and Skillman

for both the Kaman and McGuire calculations.

The principal two points of difference between the Kaman and McGuire calculational procedures are in the treatments of V(r) and E in equation (3) for

n purposes of carrying out the necessary integrations for evaluating P (r) and

Pg ^^^(r) : (1) McGuire approximated the quantity rV(r) by a series of straight

lines, by means of which solutions to equation (3) could be expressed analytically in terms of Whittaker functions and evaluated without recourse to numerical

integration. In the Kaman calculation the tabulated Herman- Skillman V(r) values

were used directly, and numerical integration was used. (2) McGuire used theoretical E^ values in equation (3) corresponding to the initial bound- state

configuration, hence the frozen-orbital or unrelaxed-core approximation. In the

Kaman calculation, on the other hand, core-relaxation or fast-rearrangement was

taken into account to some extent by inserting experimental absorption-edge

energies for E^ in equation (3).

Use of experimental E^ values has some advantage in providing absorption

edges at the right energies, with no scaling of the calculated results required

to relate them to experimental cross sections. There is, however, some risk in

this procedure in that corrections may be inconsistently introduced, according

12/ 12/

to Pratt, Ron and Tseng. Pratt et al also suggest, on the basis of results of

13/

Rosen and Lindgren, that the relaxed-core (sudden rearrangement) approximation

is more suitable for inner shells, particularly for light and medium Z elements.

3
where binding energies calculated in this approximation agree best with experimental thresholds. However, for outer electron shells, binding energies calculated

using the unrelaxed core (slow rearrangement) approximation tend to agree better

with experimental thresholds.

III. Results

The McGuire energy grid is in integral values of angstroms rather than keV,

and the upper energy varies from 0.310 keV (40 X) for helium (Z=2) up to 62.0 keV

(OoZX) for silver (Z=47) through xenon (Z=54). Because of this varying upper

energy, and also because McGuire gives no cross section values at the absorption

edge energies, we interpolated (log-log linear interpolation) the Kaman photoeffect values to the McGuire energy grid for purposes of this comparison, rather

than vice-versa. These interpolated values are listed in barns/atom in the last

column in Table II following the McGuire values in the same units as taken from

reference (9)o

The results of the comparison are given in the second column of Table II.

For each element Z = 2 to 54, the percentage deviation of the McGuire photoeffect

cross sections from the Kaman values was calculated as

Percent Deviation = 100.0 (t^, ^ . - t )/t (4) McGuire Kaman Kaman

The resulting sign indicates that the McGuire cross section is greater (+) or less

(-) than the Kaman value. The percent deviations are rounded off to the nearest

one-tenth percent.

In Figures 1 and 2 we have indicated the combinations of energy and atomic

number for which the absolute deviation of the McGuire photoeffect cross section

from the Kaman value exceeds 3% and 207o, respectively. It is evident from

Figures 1 and 2 and an inspection of Table II that the majority of the deviations

are between 37o and 20?o. The only systematic trends appear to be that the McGuire

4
values are generally greater than the Kaman values below 0.5 keV and tend to be

less than the Kaman values in the region 1.0 to 10 keV.

In Figures 3, 4 and 5 we graphically compare the McGuire (dashed line) and

Kaman (solid line) calculated results, also the Kaman values above 1.0 keV fitted

to experimental data (dotted line) for carbon, aluminum and tin. Also included

in these graphs are experimental total cross section data points from the NBS

data-file indexed and documented in reference (14). In the regions shown, the

total cross section on this scale is indistinguishable from the photoeffect, as

was indicated in Table I. In Figure 4 the dip in the McGuire values at 2.07 keV

for aluminum we attribute to a typographical error.

In these saiiqjle graphical conparisons X'je see that both the McGuire and Kaman

results are for the most part consistent with the experimental data points within

the experimental spread of the order of ± 20% . An exception to the ± 10% consistency is seen in Figure 5 for tin below 0.3 keV where a pronounced resonancetype feature is shown by the experimental points. Similar peaks have been

observed between 0,1 and 1.0 keV for a number of other medium and high Z elements

(see, e.g.. Figs. 27-52 of reference (2), Vol. II). Although both the McGuire

and Kaman calculated results tend to suggest the presence of such features, these

cross section values may disagree with each other and/or with experiment by an

order of magnitude at the peak energy.

Some additional isolated large discrepancies between the McGuire and Kaman

values (1057% for nitrogen 0.103 keV and 64 07o fiDr palladium at 6.2 keV) we

attribute to misplaced decimal points in the McGuire tables. Other large discrepancies as listed in Table III we attribute to differences between the McGuire

theoretical (initial bound-state configuration E values as discussed in Section II) " 15_/

absorption-edge energies and the experimental values from Bearden and Burr

used in the Kaman calculations. All of these differences are positive, hence the

theoretical McGuire threshold energy in each case in less than the Bearden- Burr

value also listed in Table III.

References

1. G. L. Sitninons and J. H. Hubbell: "Comparisons of Photon Interaction Cross

Section Data Sets. I. Storm-Israel and ENDF/B; II. Biggs-Lighthill and

ENDF/B; III. NSRDS-NBS 29 and ENDF/B; IV. Kaman and ENDF/B; V. Photran and

ENDF/B," NBS Reports 10668, 10818, 10842, 10847 and 10848 (unpublished).

2. W. J. Veigele, E. Briggs, L. Bates, E. M. Henry and B. Bracewell (Kaman

Nuclear Corp., Colorado Springs): "X-Ray Cross Section Compilation from

0.1 keV to 1 MeV," Vols. 1 and 2, Rev. 1, KN-71-431 (R) (DASA 2433) July 3l,

1971.

3. E. M. Henry, C. L. Bates and W. J. Veigele: "Low-Energy Photoionization,

Physo Rev. A 6., 2131-2138 (1972).

4. The present ENDF/B photon interaction cross section library tape, also

designated as RSIC (Radiation Shielding Information Center, Oak Ridge

National Laboratory) tape DLC-7, became a part of the Evaluated Nuclear Data

File system as a result of action taken by the Shielding Subcommittee of

CSEWG (Cross Section Evaluation Working Group, AEC) at a meeting at Los

Alamos May 12-13, 1970. This library is documented in references 5, 6 and

7 as discussed in reference 1 (I)

5. E. F. Plechaty and J. R, Terrall (Lawrence Livermore Lab., Calif.): "Photon

Cross Sections 1 keV to 100 MeV", UCRL-50400, Vol. VI (1968).

6. W. H. McMaster, N. K. DelGrande and J. H. Mallett (Lawrence Livermore Lab.,

Calif.) and J. H. Hubbell (National Bureau of Standards): "Compilation of

X-Ray Cross Sections", UCRL-50174, Sec. I (1970), Sec. II, Rev. 1 (1969),

Sec. Ill (1969) and Sec. IV (1969), These reports are available from the

National Technical Information Service, Springfield, Virginia 22151.

7. Jo H. Hubbell: "Photon Cross Sections, Attenuation Coefficients, and Energy

Absorption Coefficients from 10 keV to 100 GeV", NSRDS-NBS 29 (1969).

8. B. L. Henke and R. L. Elgin: "X-Ray Absorption Tables for the 2-to-200 %

Region," Adv. in X-Ray Anal. 13, 639-665 (1970).

9. E. J. McGuire: "Photo-Ionization Cross Sections of the Elements Helium to

Xenon," Phys . Rev. 175^, 20-30 (1968).

10. J. W. Cooper: "Photoionization from Outer Atomic Subshells. A Model Study,"

Phys. Rev. 128, 681-693 (1962).

11. F. Herman and S. Skillman: Atomic Structure Calculations (Prentice-Hall, Inc.,

Englewood Cliffs, N. J., 1963).

12. R. H. Pratt, A. Ron and H. K. Tseng: "Atomic Photoeffect above 10 keV , " Rev.

Mod. Phys. (in press).

13. A. Ros^n and I. Lindgren: "Relativistic Calculations of Electron Binding

Energies by a Modified Hartree-Fock-Slater Method," Phys. Rev, 176 , 114-125

(1968).

14. J. H. Hubbell: "Survey of Photon-Attenuation-Coefficient Measurements 10 eV

to 100 GeV," Atomic Data 3, 241-297 (1971).
15. J. A. Bearden and A. F. Burr: "Reevaluation of X-Ray Atomic Energy Levels,"

Rev. Mod. Phys. 125-142 (1967); also in J. A„ Bearden: "X-Ray Wavelengths

and X-Ray Atomic Energy Levels," NSRDS-NBS 14 (1967).
Figure Captions

Figure 1. Elements and grid-energies (see Table II) for which the

McGuire calculated photoeffect cross section is at least

37o greater (+) or less (-) than the corresponding photoeffect cross section interpolated from the Kaman data set.

No McGuire values are given for higher energies or Z's

beyond the indicated boundary line in Figures 1 and 2.

Figure 2. Elements and grid-energies for which the McGuire calculated

photoeffect cross section is at least 207o greater (+) or less (-) than the corresponding photoeffect cross section

interpolated from the Kaman data set.

Figure 3. Photoeffect cross sections for carbon calculated by McGuire

( ) and Kaman ( ), also fitted by Kaman to experimental

data ( ). The circles are measured total-cross-section

data-points (see text)

Figure 4. Photoeffect cross sections for aluminum, with same notation

as Fig. 3. .

Figure 5. Photoeffect cross sections for tin, with same notation as Fig. 3.
Table Captions

Table I. Ratios of the photoeffect cross section to the t^^al cross

section, based on values from the Kaman data setT

Table II. Percent differences 100 x (Tj^^.^.^ - ^Kaman)/^Kainan the

McGuire grid energies. The photoeffect cross sections

^McGuire ^^'^ ^Kaman (ir^terpolated to the McGuire energies)

are listed in the last two columns in barns/atom.

Table III. Large percent differences in Table II attributable to discrepancies between the McGuire theoretical edge-energies

and the Kaman experimental edge-energies. The experimental

edge-energies or ranges of edge-energies,^in the last three

columns are taken from Bearden and Burr^-/
ATOMIC NUMBER, Z

o o O

I

I I

I 1

I -H-Hl-H ltt+ I I I I I 1 1 I

• H I I I I I I I I

l-H- + 1 1 I I I I I I I I

I I I I 1 1 1

I -H-l +

1+ -H4++1 -H-lH-l I

I 1 1 I l-H-f

1+ + t+l 4- I I I

-H-l- H-l + I I I

I I I

I I I I 1+ I I

I I *—1+4 +H-+ MM

H-H-l + M-l M

I M M M M M

4-H+-H-H-H-+

4-M + I M M

l-H I I I II I I

I-H-+ +f4l +

I I -H+ Hl-l-H-H I I -H

I I-HH-I4I

I I4-I-I 1 1 II

l-H 141 I I

++4-I-I ! I 14- HI M I I M I

I I I I M I l-H 14-H-f I I I I i M M

I I I I I I I 14-1 H- 4H- I I 1 8 4-HI

1 1 I

1 I 14-1 144-H- I I II 1 8 M

HUM -H4-I I I 8 M M H4H-4 -H-l-l-144- 4-I4-I + I4-H4-H

1 II I I -I-I44- 44- I 144-1-H-l-l

I III 144-144- I I I4-H4-H-S

H I 1 I I 144-144-

H-1 I I 14-

I I 114-1- -K44-

III 111

4+

1 1 14-fl-H-fl

l-H 14- 14-9-

I

I 14- I-H-I4-

I 1 14-1 S44-S
ATOMIC NUMBER. Z

O O

O

H

O _ ^

o

m

m

:x)

CD

-<

CD

<

in OP o

o

+ +1

+ +

+ + +

+

1

!+

IV

o

•H-H-4- +

+++++

1 +

+1 +

+

S I 1 +

I +

+ -H- +

! 4- + -H-

++ + ++

+ II I I IH I + I I N I + III I I

+ + + 4-HI +

111!

I !

I i

i 1

I 1 -H-l-f

+ 4+1 +

444- +

+ 11!

I ti

+ I

I I i

+ ! 1

o
MCGUIRE CALC

KAMAN CALC.

KAMAN EXP. F

10" 10

PHOTON ENERGY, keV
.4

10

• Q 6 O O

Al

MCGUIRE CALC.

KAMAN CALC.

KAMAN EXR FT

=

I I I I I 10' lo'

PHOTON ENERGY . ke

10

Fi
10

8

50 Sn

O

10

GD

-XXMCGUIRE CALC.

KAMAN CALC.

KAMAN EXP F

10'' 10

PHOTON ENERGY, keV

10

Fig. 5

<f

O on vO o vO (M ON (M 00 <t 1—1 (M <i-

<7N ON (JN ON ON 1^ ro

0^ On CJN C3N ON ON ON ON C7N 00 O

in o O 00 vO in (M o <^

00 ON 1—4 ON

O <r 1—4 oo ON CJN ON ON CJN 00 vO l-H

r\] OS ON OS CJN ON ON ON CJN CJN OS

00 oo vJ- o 1—1

O 1—1 in C3N C~) ON ON r-. o CO

On ON ON CJN ON 00m CO ro <t ON ON ON CJN ON ON ON ON 00 ON O c0 00 CO O ON ON 00 CJN <f 00

'H c 00 CO 00 ON in <f 1—1

O oo ro

JJ ON ON C3N ON C7N (3N 00 <t 1^ ON UN w * UN us 00

0) in w

O

COMo

S-j CJ ON 00 (M in ON vO 00 sD <f

c—

ON (3N ON ON <! in OO c-o CJ ON C7N ON CJN ON 00 C3N c^ oo

4J ON CJN CJN ON CTN C7N ON ON CO o (M

4-1 o co

•H

JJu 1—

o o vO o ro ON <f o in O]

0) < o o ON 00 ON <! in ON M o o ON (JN ON ON r~ O vO o 1—1 o o CJN ON (7N C3N CJN <!- 1—1 m • • • • • • CO I—

1—

ouu

4-1 u o o ON in

O 00 1—1 1—4 0) o o ON (7N o 00

14-1 o o ON C3N ON 00 in o 4-1 o o C3N ON ON C3N 00 O o

<U • • • • • a « 0 1—1 1—1 4Jo o o 1—1 O 00 0>

•H o o ON 00 •c in C3N 00 on o o o 0^ C3N 00 ro oo o o o o ON C3N ON 00 o o o • o o cn vO <l- 1^ o ON 1—1 (U o o ON o sO C3N in o o o o ON C7N <l- 1—4 1—1 1—4 o o

(M o o CJN C3N ON

m 1—1

O o o

1—1 I—

o 1^ (M cn o ON 1-4 1—1 o On <} sO ON o o o o ON C7N <r CM vO o o o o r—t o C3N C3N ON vO O o o o o

c—

V

V

1—4 oo in o o o • o o o 1-4 oo in or-H o

oo oin LOO
Table II

HEL lUM

ENERGY P F p r K T (KFV) DIFEEPEMCF M r r. Lj T P e K A A (^j .103 3.1 3 , ^ 0 E + 0 5 . 3 0 + 0 b

. 1 ?4 -I?.

1 . 8 n E + n 5 ^ . O-SF + OS

. 15S -1 ?.« I, 0 0 E + 0 1 . l^^' + O':) .?07 -11.7 4 . n E + 0 4 5 . P 1 e 04

.310 -7.

1 . 5 n E + 0 4 I . 6 P E * u 4

- I ITHIDM

ENER(iY PERPF MT

( t\ r v ) MCGU [ P|- K A 1-1 At N

.103 1 R.« 1 .'^PE + n^, 1 . ?HF + Oft

. 1?4 1 « .4 9 , « 0 E + 0 H H ,;^ 7 + 0 5

. ?0 . 1 5 , M 0 p. n S 4 , w 3F + ()-)

. ?n7 ^ . ^ E + 0 5 r-. 3?E >l.-> .310 13.0 8.Q0E+-04 7 , M^F + u<+ .413 7. ft 3 . M 0 E + 0 4 .1 , 5 + ij 4

. ,^?0 -Q.O 1 . 0 0 E + f) ^ 1 . 1 0 F u

H E R Y L L F n M

ENERr.Y P F P C E w T (KEV) DIFFEPENCF

.103 1 A. i . 3 0 E + n s 1 . 1 *'J5

. I r **• J 4 , ? ? . 1 fi E + n A 1 . H'Jp + 0 h

. iss 1?.7 1 . 1 T t + 0 6 1 , 1 M F + 0 b

.?n7 . 70E OS '5 , j M + 0 S

.310 1 ? . ? 0 E * ''; s .

'~ + 1) b

.413 11.4 1 . ) <^ E + 0 ^ 1 , O'Sf-" + (;b

.6?n ^ . 0 n t: + 0 3,47 h + u 4- .8?7 1 . 8 r E + (1 4 i « b t-^ • 0 H

1 .033 ?3,f^ 1 . 0 0 E + 0 4 >! . 0 + (; J

POPrjM

ENERGY PFPCf- NT

(KEV) DTFFFPi^NCf^ M r ij I p F

i .103 1 A . ? ? , V 0 E 0 + -J . 1 ?4 10.3 1 . H'^fc + 05 1 , f-KF + (-3

.155 ?.4 1 . 0 fc + 0 s 1 . 0 + (O

.?07 17.7 1 . ? ? E + 0 ^ 1 . 1 --(j6

.310 4 , H n E + 0 s 4 . 7 7 r HJ 3

.413 ? . ? 0 F + r, s P , 3 s F + 0 b

- , Q b , n OF + OA H . 0 7 t-~ + u 4

.8?7 '•! . ^ 0 F + 04 •^ , ^ 7 F ( ; 1.033 ^^7. 1 ? . 5 0 F + !) 4 1 . 7 F * (>
Table II. Continued

PFPrFMT

( K F V/ ) 0 T FFFIvPmCF

1 q. o S ,

f-*

It. + !

1 4 .

. 1 ^4 ? 1 . O 4 . riOt. + -IS ^ . + s

. l'^'^ ?n . 3 ? . ^4 n t + 0 s 1 . i- * i;8

. ?0 7 4 . 1 . 0 P + n ^ I . 0 '^f- * U 8

.310 ^ 3.7 -t . 1 n [•: 4- 0 7 . 1 ^ *C8

.411 8,3 4 . S 0 F + ("1 S . * L ->

- .^?Q 17.7 1 .p?r. 1 . + fio .flp7 1 7.q '-( . ci E t- n ^ r

? 1 - + IJ 4

1 .033 1 ^ , 7 0 F + 0 a 3

W t» ^' 04

1 .?40 ?n . 0 ? . Q 0 F + () ^4 r , 4 o t-" + (J 4

1 .SSO 1 Q.'^ 1 . n E 0 a 1 . > 8 r + 'J 4

^' I TPCM^ N

ENERGY P F P C f- T (KEV ) DIFFFPFmCF 'vi r r, 1 J

1 -? F

- A N

.103 1 nSA."^ 1 . n E w) 7 A '1 r

. 1?4 7 '-i . S n E + n 8 .

•) ^ c + U 8

. ISS ?.7 3 . Q 0 F * P .?07 7.? . n '-'E + ('^ 1 . lib .310 -4.8 7 , n n E + f) 4 7 . -(4 + U 4

.413 3.« h , H n E + ') c. 8 . K f' 1)8

.6?0 . P. + 0 ^ *

.B?7 - . 7 1 . ? E * n s <->

^'

«• 0

1 .033 7. n 7 . ^ n f n a 7 . - \J 4

1 . ?40 8 .

c) 4 . 7,^.h + .14 4n--- + 1/4

1 .SSO 11.7 ^ . 8 n h - n 4* < f- i) 4

?. 086 m . 0 1 . ? 0 r. * ^ i . I' 1 ^ > 04

0 X Y G t- \

ENERGY PFPfF^iT

(KFV) nTFFFPFN.'CF •A u tM .10 3 1 4 . Q 1 , 7 7 1 + 0 8 • 84 t- + U 8

. 1 ?4 « . 4 1 . 1 ? E 8 1 . -0 8

. 1 1 n . P 7 . 0 0 E + 0 8 . 3 - * i J b

. ?07 1 « . 1 ^ , 8 ^ E P 3 . .310 ^0 . ? i . 8 0 F + 0 1 . -'IE + 08

.413 8.7 8 . s 0 E n u 8 . 0

'"^ ^ + 4

. 'SPO .« ^.Q'-E + OS 3. + 08

. R?7 .4 1 . Q ^ E + 0 S 1 . U 4 8 + Ob

1 .033 A. 8 1 . ? 0 r. + (1

'-'-^ 1 . 1 1 ^ + (.) 8

1 . ?40 ?. 1 7 . ? 0 E 0 a 7. + ( M1 .SSO 7.8 4 . 1 n E 0 4 u 8 1

^" + 0 '* 2.086 1 P . ^ ? . n 0 E * (; <i 1

- ij4
Table II. Continued

p fT P (~ p K| J

( KE V ) M r 1 1 1 F" K' '1 fx .in? p 1 ^ ^ /. U .1. i 1 A,

. 1 ?4 4 Q 1 n F * n A 1 7 P i- 4. 1

. 1 S'=> 2 3,'^ 1 » ^ n !~ -f 0 ^ 1 ( 'i A P A. 1 1 ^-

• ? n 7 '"),'-* ^ F + ; ) '-5 .310 1 C1.4 . 4 h. + 0 ? , O'^-.K + (;i

.4 13 ?3.7 1 , 2 4 F + 0 S i , n 0 F <• 0 ^ A Q n . O IJ on Li s . n n t + 'J 4 ^ ^ u C + 1 J 14.

ft 7 "7 ~7

' . f ~i r» r' i_' . r\ r"

. "! . I ' S t + 0 n 2 . 3 + ' i

1 n "5 » < 1 . ' '1 t •• ') ^^

1 . A F + 1

,

1 p A n n , n 1 . 1 s t- 4- rm 1 , 0 '^ + 1; "-t

r> . »

(

' r + '

1 ti —\ ^ w A 4 ?c .. nV f%r) A "3 A A f J A .' . '1 >' ^ J-

( ; 4

' f 0 f^i F ,\j p c? r; Y P F" O f ^ M T

( K F V/

)

K A ' •' ^. f'i .10 3 a ri F 4- n A

"3 n >^ C; A k u. 7 t- J. . #-v

"3 '3

1 7 c; h" 4 I" 2-, 1 . f r +1-0

. ? 0 7 ? 7 7 . i1 1 C. ' ! ^ M , . r + ' J 'T .310 ^ . A n K. + n s i . 3 - ^ + .J D .413 4.4 1 . 7 0 F. + 0 s 1 . S It- * >)b ^ p n Q 7 "3 , 7 '4 F * i ( 4

ft ? 7 11 A I J . i • f ) n t" . + M ^

"J (i_ i t

' -r" . A '-^ r » u '4

1 n T — IT i~. J r. c L . M c. r '

' ^ r + t h , i 7 P * ;

— 1 1 P 1 C ^ LI 1 c. •

1 c; n f « M' ^ + n q. <j. fi ^- * 1 ; u p n A A 1 7 " J A tr . / ^ /

j • w M -f ; ) ^ J , . 1 F jj ^

F M F R Y p p p r fM T

( K F V ) n T F"FFPF^i^'^'

1 1 p ^ Q CI t" J, /"i 4^ A . S 4 1 J ^-) A n n h A f 1 ^-v '-r » 1 .' w c * w r>

1 1 • 2 « 1 *" • 0 r; , ? 0 7 — 7 A i • I n t + M r> 1 . 1 + U b

- 3 1 0 -PI A "7 J C , 1 1 u .413 -21.7 1 , M A f: 4 f) ^ 2 , F. + ( ; "3 .6?0 -I 2.

7 . 0 1. + n 4 1^ + (. 4

.8?7 -1 3.C) 3 . s 0 F + n 4 4 .

1 1 7 F' * u 1.033 -21.2 1 . FlOF + 1)4 2 . 2 " F * '

1 .240 P. 0 2.3?F*0'. 2 . 1 F + ,j w

1 .sso 1

c; , Q 1 . 3 P F + 0 i , 1 W P .UJ u, 2. 0^^^ 11.7 . 1 0 F + 0 4 5 , A F + f; i+
Table II „ Continued

A G N t- S I 1

' M

PFRrf- MT

(KEV) MrGUT'-^t-'

.103 17.1 'S . ^ f"- F 4- 0 ^ ^. f-. <

^" + ( ^ 'J .1^4 \P,P 4 . w 0 F + 0 4 .

.> ^-i t- + 1 ,j

. ISS 3.>^ \ i^f: *nh + F .?07 1 1 . F + () h 1

^, -1 f-' + 1) F

.310 -.A 6 , M 0 F + (1

. H 4 F + 1,1 .413 3 . n F + 0 3

4 7t- + U .6?n -1.4 I ,?^F + ns I .

^ + U

' .B?7 -1.0 (S . 0 n F + 0 4 b . n f- + (, 4 1.033 4. 3. 3f ^ •'(14

1 . ?4 0 1 . 4 ?,40E+04 2 , 0 H F + 04

1 .=^S0 1 . '^?F Ot^ 1 .

i-.. :-! h + 1! 2. Of.6 7.0 7 . <^ n t + 0 4 7. >• F + u ^ 3.100 1 r' , 7t=^F + Ou + 1:4 4 . 1 3 1 , "^4 t +04 i .

Pi ."I t^" f (; ^

ALljM 1 ENERGY PFPff- MT

(KEV) OIFFFt^f- ^'CP f/ifGU [PF K' ,:> ' iJ,

• .10 3 S , 4 F + ; 1 0 . + U5

. 1?4 A.q S . S 0 E

'"1 S 5 . 1 + U 0

. ISB 11.0 4 . 1 3 E + 0 f) 3 .

/" ? ^ + (J h

.?07 ? , F F_ + 0 A 1 + U F

.310 n.^ 1 . 0^.E + 0^ ? + l i -) .41 3 7.P S. loe 4 . 7 ^ f-' + ()-.? .6?0 4.7 1 . F F * 0 I . 7 /P + OF

f>. n ^ , 0 0 F + 0 4 "1 . 4 'v F + ;

) '+ 1.033 1 . 0 4 ,

>-* 0 F + f

' ^ 4 , 7

1 . ?40 -10.? ? , f. f-' + n 4 P . + 1/4

1 .SRO 1 . 7 0 F + 0 1 . '.(it- U H 2. Of>^ -40.4 5 .

fi 0 F + 0 4 -V , f 4f- + (.; 3.100 1 . 3 . ^ F + 0 4 3. i

'

1 F' + iy -4 4. 1 33 17.*^ 1 , ^"^F + 04 1, . a^>F + 1;, 4 SILK

tNEC?GY pppf (- ^;T (KEv/) OT FFFKEMft^ •'.:!.] .103 -R7.fi , K r + n t, •> u c; c- + (J f.

. 1?4 10.7 S . ^ 4 r + n ^ 4 , 7 ^ ^

. 15S ^.4 a . ^ P h ^ 4 . a 7r + i; b

.?07 10.1 -i . 1 " F + 0 A «• (

.310 11.? 1 , ^ F, * i^>^

I . .413 ^. 7 ^ ,

>J P t- + 0 V 7 P + 1

,^?0 ?. 1 P , 4 F + 0 4 1 ^ + L -.^ 1 . 1 -'F + OF j . 1 - u t- 1.033 -3.fi 6 . 1 0 e + n -, f + ' «4

1 .?40 -9.4 ^ . 7 t * n 4 1 u F + (!'*-

1 .5S0 r' . 1 :^ r. + 0 4 + :; 4 2. 0^(S -IS.M 1 . 0 r + (1 s 1 . P yi r + ii 3.100 3. ^ 4 . ^ 1- n 4 . .1

+ ',: 4

4.133 5.7 ? . F + ri +

'

; -4
Table II, Continued

fcNE«GY PFOf FMT

( K E V ) DTEFFPFMCf K- C'-A.) T -'F .103 1 S.4 '^ . 7 01^ + O'^ 4 , 4 - '

. 1 ?4 2S. 3 4 . 7nh + OS 3 . / S

=• u ^.-i

. ISS 21 . n s . 4 n e + n h .'+ ,

44. '-,1- + (1 (1 .?07 -3.4 3 . <^ F + 0 6

.310 3.1 . 7 n t + 0 6 1 . h4 +0 f .413 -1.2 >^ . s n f: + 0 ^ . ^ 0 ^ + 1 1 "-^

. 6 ? 0 -7.0 3 . fi 0 t 0 R W S5 7

1.033 -1 0 . n H . ') n t + f) b , '-''^^

1 .?40 -8.7 s . 1 0 F + n ^ , s'-

1 .5S0 U 0 F + 0 4 3 , n 7 <• 0 4 2.066 -12.? 1 . 2SF + Oh 1 , 4 i M: 4

3.100 . n -) . S 0 F + n 4 , Oh 4- IJ.V 4.133 7.Q 2 . 7 0 F + 0 ^ ? , S f"i F * i

SilLFLiw

ENERGY PFPCF MT

(KFV) DTfffpfmCF C U T r" .103 IP.P Fl . S 0 F + 0 5 7 . 1

- * 0 S

.124 2S. 1 7 . 0 0 F * n

. 1S5 2^=^.'^ S . 0 n F + n 3 . '•us .207 -1 ."^ 3 . F + n ^ , A S F + ij 6

.310 ',<^ ? . 0 F + n ^ 2 . n A p + u h

.413 1 1 . 1 ?F* 1 . 1 OF f iib .620 -7.7 3 . -^OF * O"^ 4 . 2 'J D

Q O 7 > 1 7 P » ' 1 ""1 L. m ' i ' ^ -J .J 1.033 -14.4 1 . n 0 F + f) s 1 . i 7 > D b

1 .240 -s.n 7 . p. n t + ') 4 . -i 7 + ( . 4

1 .S-^O -6.3 3 . ri F + P) 4 4 , ( ) f> F- + (J 4

2.06A -12.

1 , A 4 F + n 4 1 , ^ *-< ^"

! J 4

3.100 -2.Q 6 . 7 n F + n F , 9 fi F * 0 't 4.133 7. A 3 . 40F + fi4 3 , ) F + ; ) H

THLOF 1 MF

ENERGY PFPCF NIT (KEV) DIFFFOFN'CF ./ r r- u J ^1

.103 1 1 . 0 0 F + 0 6 ^ . 1 F + ) -)

. 1 24 . 2 n F + 0 ^ 7 ^ H O r .y I

. is-s h . n n F + 0 S , 7 4 F + i .207 1 2q, n 6 , 4 n F + i"! IS ? , M fi i

, h

.310 -1 .A 2 . 4 S F * 0 fs 2 . 4 *^ r + (1 K .413 1 I , 4 n E + 0 >^ i , 3 '-<F + {; t) .6?0 -16.1 4 . S f) F + 0 S S . 3 7 F 4. ; ) S

.R27 -1 ^^.7 2 . 2 0 F + 0 s . A 4 F - u S

1.033 - 1 « . 2 1 .23F + c,S i , S 0 F f u b

1 .240 -17.2 7 , 9 0 F • 0 4 9 , S4i^ +

I .5S0 -1 0 .Q 4 . 7 n F + n 4 ^ , ? 7 1 + (

)

2. 066 - 2 0 . A 1 . q F n 4 2 . 4 F + ( ; 4

3.100 -11.'^ 7 . n F * n 4 H . S ] f +1)4

4.133 3 . n F * 0 4 3 .

'-^ f +(14
Table II, Continued

tNERGY PfPQF MT

(KEV) DTFFFPFMCE < A

' ' A iv .101 4.7 1 . 3 E 4 n 6 ] . / r + 0 f.>

. 1 ?4 4.Q 1 . lOE + nfS 1 .

<' -y- + U h

. iss 7.Q >^ . '^i 0 E + 0 S 7 + 1

.?07 9."=i 5 . 5 0 E + n s S , (

+ (; ^ .310 -Q.4 2 . S?E + 0^ 2 . 7 p f- + (! h

.413 -S.Q 1 . ^ E 0 r, 1 . / ^. 1^

(.1 h

.f)?0 -10.4 6 . ? f1 E + 0 * Oh

.B?7 -1 4.q 2 . 9 n E + 0 5 . 4 1 + ( 1 "-I

1 .033 -17.4 1 . ^ 0 E + (1 1 . 4 * 1 ; V)

1 .?40 3 1 . 0 0 E -t- 0 ^ * '3

1 .sso - 1 0 .

ft ^ . n 0 E + r; ^ ^ . 7

^' + 1,1 -1^.3 ? . 0 E + 0 ^ . 1 1 + ' / H 3.100 -1ft. ft ft . 5 n E + 0 3 1 . OS'- + 0 H 4.133 -7.1 4 . 6 0 E + 0 4 4 , w ( + 0

POT ASS T tJM Pf^PCENT

(KEV) DTFFFPEMCF •-I A Cvl .103 9. ft 1 . 5 0 E + n 1 . ^ 7 r -t- i j h

. 1?4 13. ft 1 . 3nE + 0^ 1 . 1 4F + (1 6

.155 13.7 1 . 0^E> 0 6 9 , () t- .?07 13.4 A . H 0 E + 0 5 b . 4 Q F + D'o .310 -7.7 3 . 3 0 E 0 h 3 . ^

*" * () b

.413 -7.1 1 . 9 ? E * n 6 . 0 7 r + 1 ; h

.6?0 -1?.9 7 . 3 0 E 0 5 . ? r + l ! "^i .R?7 -4.4 4. onE + n'=> , 1 ^' + (!'-) 1.033 -ft.? 2 . 2 0 E + !) 2 , ^ n t- > (; h

1 .?40 -] 4.ft 1 . 3 n E f 0 5 1 .

-^ ^^^ + !; 3

1 .5S0 -7.4 7,ftOE-»-0/i H . ^+ p

^ > 04

2. 0^6 -13.? 3 . 4 0 £ * (1

3.9^H + ij ^ 3.100 -Q.9 1 . 2 n E -nVf 1 . 3'^^' + I I ii 4.133 -7.-^ S . 4 0 E * 0 a •-) , M 3 * U 4

6. 199 3.7 2 . 0 n E * 0 4 1 4 ( i •'+ 8.2^^5 5.7 9. inE + 03 ft . 1 ^' * \J .i
Table II. Continued

C AL C 1 i jM

EMFPGY P F P r F N.' T (KEV) DTFFFwFMCF MCGU T -^e .103 1 R , R 1 . ^>nF + 0 6 I . S i I- * U D

. 1?4 IP.? 1 .^3F + 06 1 . ? ^ * Uh

.15^ 10.1 .1.1 6E + Of^ J , 0 F + (J b

,?07 P.

7 . « 0 fc + 0 5 Z' . 1 7 + 0 b

.310 16.'=. 4 . 3 0 E 0 S 3 . h'^F *<)•-) .413 '=..? ? . ? 0 F +• 0 ^ ? . 0 F' * (J h

- .6?0 -7.7 9 . ? 0 E + 0 5 9 , 9 7 ^- + U 5

.R?7 -.^ 5 . 0 0 F + 0 5 5,0 ^ F + (J '^

1 .033 . 4 3 . 0 n E + n ^ ? , 9 0 F + u

1 .?40 -1.4 1 . H n E 0 s 1 . ^ ^ U b

1 . 5S 0 -4 . ? W , M 0 £ + 0 4 1 . 0?E* Ob

2. 066 -3.9 . 0 E + 0 M 4 , 7 4

3.100 1 . s n E + 0 <^ 1 . 6 4 F + ij 4

4.133 -1 ?. 0 6 , 1 0 E * n 4 O . >-J F + (J ^4. 6. 199 3. ? . 4 OF * 0-=+ . 3 ^ f-" + 04

H, ?65 ^.3 1 . 1 0 E + 0 4 i . 0 f-' + 0 4

10.33? 9.Q ^1 . 1 0 E 0 3 5 . K -t. I) J

S C N I"' II 1 ENERGY PFRCF MT

(KEV) DTFFFPFMCP ^ A '

'• A i J

. 103 1 .6 1 .gsE + o*^. 1 » w ? + 0 f-'

. 1?4 3.4 1 . 6 7 E + 0 h 1 ,

f-i r Ob

. ISS -3.3 1 . ?'^E + O'-. 1 .

i j h

.?07 -1 1 . n 7.80E +ns

.310 -4 .

ft 4 . 3 0 E + 0 ^ 4 ,

'-^ P F + !

.413 13.0 . R 0 F + 0 IK P , ? ] r + 0 f

.^?0 . 3 1 . ?OE-K)f 1 . ? 0 f; 6

.B?7 11.^ 6 , » 0 E + 0 6 , ] 1 r + 0 ^ 1.033 16.4 4 . 1 0 E + ') s 3 0 b

1 .?40 1?.4 ? . 0 E 0 ? . ^ E + 1.' 1 .SSO 11.7 1 . 4 n E 0 s 1 . ? ^ F' f 0 b a. 066 7.^ 6 . 3 0 E + 0 4

3.100 4.5 ? . 1 n F * 0 4 ? . 0 1 F +1)0. 4.133 7.4 1 . 0 0 E + 0 4 ^. 3],t-"f OJ

6. 199 -?.^ ? , 7 0 E + ( ) 4 ^ . 7 ?F + 04

8.?65 7.^ 1 . 3^E+ 04 ] . ? ^ ^ + 0 H 10.33? 10.5 7 . 4 n E + (1 3 b , 7 0 F + j 1 .-(
Table II. Continued

("HP f_) ,v 1 1 )

PFPfFNiT

(KEV) Mr r;u T Qf: .103 14.4 4 , 1 c h: + j . ^ -* * 1

.1?4 1?.9 3 . 3 n F + 0 ? , -'^ + .155 7.« P . 4 0 t + 0 h ? . ? ^= .?07 -.7 1 . 4 S F + n 1 .

'j ^ h + !.i h

.310 -?.^ 7 . ? 0 F + n 7. 3wt

.413 4.

4 . n E + 0 s ^ . 30f- + ;|K

.6?0 -PP . P ? . 0 0 t + 0 s i .

"/

! i ^- + ( , (

11.^ 1 . 1 n F + () K , ^ 11 n

1 . 033 IS.

n . 7 0 1 + 0 K S , R 1 {

1 .?40 8.1 4.nnE4.n=> i , 7 0 (- + 0 O

1 .SSO 9.4 ? . 3 0 £ + 0 ^ . 1 -3 2 . OS'S 3.4 1 , n ^ E + (

, 9 7 K 0 4 3.100 -3. n i . 3 n t + 0 ^ 3 . 4 0 -4 4.133 -4.S 1 . s ii t + n ^ 1 (; M- 6. 199 -n .

i+ . 0 oE + <! <4 , 4 • •' F + . ) 4 8. 1.4 ? . 1 n E + P . ')7t ^ 10.33? 1 .

1 ft E + 0 i « I ? F + ; ; a

1 ?. 398 7.4 7 . ? 0 E > (1 h ./IF* w 3

ENEPGY PFOCF MT

(KFV) DTFFFPFN'Cr

.103 37.^ b , 4 s E * 0 ^ •i , 9 *-> F + 0

. 1?4 37.^ 4 , 4 E * ' ^ 3 . P 1^ + U

. 1 5S 3?. 0 ^ . 3 0 1-; + 0 ^ ? , S 0 - «-Ub

. ?n7 ?3.« ?. nsE + Oh 1 . A ^, ^ + :^ N

.310 ] S.7 9 . 8 n E 0 ^ ^ . A / F + {) .413 ?0.'^ . 0 0 F * 0 ^ . 9 P + (j 'J .6?0 1 3.Q P . ^ 0 E 0 S ? . '5 F + I) b

.«?7 -.ft 1 . 1 0 E + 0 ^ 1 . ] 1 F + f j 1.03^ -Q.? ^ . n 0 E + 0 ^ '^ . 6 1 * * 0 b

1 .?40 4 . n n E + 0 ^ , ? F f-' + 0 n

1 ."^^sn -13.7 ? . 1 n E + 0 . 4 F + (i ?, OiS'^ -1 S. P 9 , P 0 E + '1 ^ 1 , 1 A F + U ti- J. 1 on -??. 3 . 1 n E + f - 4 . 0 p ^ . * u 4. 1 33 -?4 . ? 1 , ^- C' E + n 1 . F * 0 H

(S. 199 -?S .

*^ 6. , 0 F + (-i i 6 . 1 + ' ) .i 7.Q ? . E + T ^» P , 3 F + (

10.3 3? q.4 1 , '+ '"i F. +

'

' ^ i . P F + ) a 1?.39« S. ? H , 1 0 E + n 3 , ^ Wf^ + (J J

15.49P. 4 . 0 0 E + 0 3 4 , 0 F + (J 3
Table II. Continued

TlTAMiJ^^

t" M P D r V t INC. "^I? T D cr 0 L M T

V rS c. V / n T C r C." 0 (T K , F r i\ " !\ W

1 n 1 r , c ^ + ' J O

P T T 11 .

> [J (-3

1 " •

1 7 n F 4. n 1-^ 11 •

-< r + I ^ ? n 7 1 A I •

1

1 ) 1 r + u o

• J i _ Q /i 4 r + u AIT "3 U 3 P A 1-' X A U f ;

' -< f + ' j S

• ~ u

1 -3

1 • ^

1

1 • 0 0 7 3.1 7 A A A 7

1 n "a "3 1 • U .1 .1 n • ^ A /• A t-" -L A w 4 .

1 7 CT J. 11 Us

1 • r U

1 "3 A '3 A A 1-' J. A

<!? f-1 S + (.! b

1 .s-^o 1 . 0 b: + 0 1

.

0 r l> S

?. 0^f> 3.S 7 . 3 0 f- + 0 4 1 . n f^*^ + i)4

"3 Inn p 0 J CC A P 4. A A Jr • A '3 C J. i'\ /i

'i- i r 1.1 4

*f . 1 5

•( 1 1 C L 1 /'i / 1 , 1 "-^ C + 1 1 A 1 . ] P F +04

4- 1 O Q 1 p J P A P J. A /. JJ • P 4 P f ) 4

ii ? A c, o • r n ^

3 Q 1 . ^ C V' A 1 " ^ r U 4

- . U A A U" I 3r", .

1 \ a c L M ^

! ) 1^ " _ A C /, ^ A P _L /\ 4 , ^ P F 4- (

V M l\i A I

' 1 ' 1 C In L. " 'T T D P D P f ^ 1 T

V rv C V ^

1 n "3 . 7 A L" 1 I £^

1 J A PI 7 r 1 . ^ P P F + fj ^

• I T> ' 1 U "3 P A c; P J. A

1 . 7 3 P 1 I , P A 7 A C 1 « ? ? h 0 h 1 •

• -1 1 U - , K T , H 1) r. + n s i) 9 K + I

r ^

• 4 1 J

—) -7 3 . 0 . + u h

. o ? 0 1 P . 0 ) , t + 0 1 , s R h + 1 ) ^

. HP 7 -4.1 H . f1 0 E + 0 ^ •! 4 P + 1

)

1 T P . 1

' y 0 f- + ,j s

1 . ?40 - 3 . « 3 . 0 Oh + 0^ ^

.

i P F + 1 J ->

1 , 0 -4,1 1 , 7 n + 1 , 7

7^"" + b

^, 06^ 1 *i , ? 0 PI + 0 4 M . s P 1= + i^) a

3 , 1 0 n . 7 f-: + 0 ^ ^. i

''•1 F -» ' ) 4 4. 1 ?3 -^.9 1 . ? E + 0 h 1 . 3 1 + HH- 6. 199 -9.4 i . 4 '-^h + 1) 4 > . 1 F f 1; i+ -?. 1 . 7 0 F 0 4 ! . + U 4

10.3-^? -3.4 9 , ) 0 F + f1 3 9 .

^' + '

) .3 It'. 398 S . s n H + 0 u
Table II. Continued

T POM

PF»CI- iMT (KEV) DTFFFPPMrr 1^ C d u r ^ F

.103 ?8. 0 5 . 0 n F + 0 ^ /+ , K i- + 0 ^

. 1?4 1?. 3 . 0 ^ t: ••• 0 8

. ISS 31.7 3 . 9 0 F + f) h r' . 8 ^" * 0 6

.?07 ?7. ? ? . 0 E + 0 6 1 . 4 7 P •• 0 t> .310 9. c- 1 . 1 nF-^ Of- 1 . 0 0 r + (J b

.413 8 . 3 n E + n s S . H^-,(^ • Oh

.'^?0 1 .? 2 . 8 0 r. »• n S 2 . S 7'y O':^ .B?7 -.9 1 . 1 0 E + 0 1 . ] 1 F + ( 1 f-)

1 .033 1 . 3 7.70E-t-0'^ 7 . 'snF

1 .?40 1 ?. 0 5 . S 0 E + n S 4 . 9 1 P ( ! h

1 .5S0 -4.1 2 . 7 n E + n s ^ , S P i" + ij , -7.8 1 .?^E*n^ 1 . 3 F + (1 1 . 1 n 0 -(^ 7 4,^0E + ''^4 i* , 7 + 1 ) ^ 4. 133 -1.0 <e . ] 0 E • n 4 2 . 1 • > r j ^

f.. 19Q f. , A 7 . 7 0 E + 0 1 7 . P:^r + (j J 1.7 ?. 7SE + 04 , 7 n f +• 0 H1 0.33? 1 1 .

"^^ 0 E + 0 4 1 ,4^1'+ ( ) H 1^.39rt 3.0 ^ . ?()E + 0 3 H . 9 li- + J 15.4Q8 ?.^ 4 . 9 0 E + 0 ^ . 7 ^ F -v M 3

rOH AL T tNERr.Y p r w r f

\i T

( KEV ) 0 IFFF^FMCf^ N'CGU IPF

.103 ?Q, 1 6 . H 0 E + n f> s , F * u h

. 1?4 ?7. 7 t) .

'^^ F + f ) f- H ,

< -m " + U b

. ISS ?0 . 3 4 . 1 0 E + 0 3 . ^ 1 ^ > 0 b

.?07 11.^ . E * n 2 . 2"^*^ + 'JfD .310 7. 1 I 1.1 ^ F > u b

.413 -4 . H h . s n t + n s ^ E + u h

.6?0 ?0 3 , ^. (1 F + 0 s < , 9 'J E + ij r) .B?7 -3.« 1 . ? n E + f""^ 1 . 2 E + u E 1.033 -10.7 7 , 7 n E fi s , o ^ E ij b

1 .?40 -s.i S . 3 0 E + 0

f"- . ^OF +

1 .'SSO -4. 1 3 . 1 0 F + r; K 3 . 2 ^ F + (J b

2. 086 -4. 1 1 , s n h + 0 S 1 , S + U b

3. 100 -14.1 '+ . 7 n F fU S , 4 7 f-' + 0 u ^.133 -] 2.10 E + Ci a 2 , S>-> + 0^

6. 199 -1 S.7 7 . 1 f' E ^ n n . 4 ? - + ( J J 8.?>>5 -?.7 3 . 1 0 1- + r 1 ^ 3. l^^F VU4

10.33? 4. n 1 . M fi rl + (~i u 1 . 7 1 r + 0 4

12. 3Q« 3.7 1 . fi ^ E + 0 1 . ('I 4 1- + U 4

15.498 4.^ S , n E •• 0 1 b.SSF *03
Table II. Continued

^| I ' K t L t N t W fT Y n c" ri ^ £- ^ 1 T

( t\ t V ) U \ r h r r'Lh r ' ' M \|

1 A

• 1 0 i 1 R . 1 7 7 A C J. i.

' . r n r + ' I K ,

' 1 »- + 1 ; >~i

, ^

^ 7 c u" j_ r £ <+» ' -<'• (j h

•i^ 1 cc;

• inn J /. D 1 A- H T 1. 1- J. A K T » ^ C + ' 1 n 5 , 7 K + ij 0

O r\ ~T O "7 U J /, A P -i. < ^ <-

.3 . M- 1 1 r. + ' ) r;

• 5 1 U ^ • ^ 1 , i ' ^ + 1 ) r .i

• 4 1 3 7 f ^ 'J V. i '1

( » ' ^ 1 ^ 1 ' _>

1 f I , 4 "J Q A C . A UL i C-, "3 t- J. ; I U, O T ] .

1 A t J. A tZ 1 ,

*< ^' * ' i'zi

1 A '3 O -r , "-V S F + ij "D

1 • r 4 (J

*^ A A A A U l-» /I A f- J. : i-^

1 cr A -H.I '3 /. A U J. A 'i y f\ A. : t-* o r\ ^ ill - 1 1 • n

1 ^ A C _L A U. 1 ij /^ w L 1

J • i 0 0 - 1 / • 4 O A t" J. ( W. ? , '-^ (- + (J 4

4.131 -13.^

o • 1 94 - J 4 , T u 0 A C i A 0m ^ I ^ * [} i

kJ o ^ c M • r n T — < n ,

'-^ '3 CL A . A J 4 , 4 1

1" IJ 3

10.31? 9 .

?.07t+04 ] , '1 '-J 1- + u 4

1?. 39R P . 4 1 . ?^E + 04 1 . r- p + 1 1

15.49R 4. 1 6 . n E> 11 3

roppiENERGY P F P C FM T (KEV) niFf^FPFMC^ K H AN

.103 ?4 , 8. l-^^E ^ . Sa"- + 1)6

. 1?4 1 7. l-^.E ') . ^ 7 F * u h

. iss ?1 .'^ s . R n E + (1

8

4 , 7 7 r + 0 b

.?07 ?R.R 4 . n oE + n*^; 3. 1 OF + O'^ .310 A , n 1 . 7 0

+ Oh i . ^ 0 F + 0 6

.411 . ^ 9 . 0 e; + OS V . 4 ^ f- + u b

.6?0 ?.9 4 . 1 r) E + OS 4 . 1

>^ + ;j s

. 8?7 -7. 1 ^ . in E + OS r' . ?'^*- + Ob

1 .013 -.R 1 . n n h + n 1 . 0 I F + 0 b

1 .?40 - . 7 n E + n s 7 , 4 1 F + (J b

1 .5S0 -p . ^ X . ^ 0 E + ri<^ 4 , S F + 0 5

0fS6 -R.4 1 .<^n£ + ns ? . ORE* i)b

3.100 -R , R 6 . s n E + 11

7 . 1 1 F + 0 4

4.111 -1 0 ."^ 3 . 0 n E + 04 3 . 1 b F »',> 6. 1Q9 -10.7 1 . n 0 E + 0 4 1 . 1?F +0^

8 . ?hS -1 ?.'^ 4 , S 0 £ + f) 1 b , 1 4 F + IJ 3

10.13? 9. ? ^ . ^ E + (1 ^ . 1 F + 0 ^ 12. 39R 10.1 1 . 4 E + 0 ^ 1 . 3 * 0 4

lb.4QR . R 7 . ? n E + n 7 . ] 4K +1) J
Table II. Continued

7 INC

t N F R G Y pppf P MT

( KFv ) .10 3 1 . 1

. 1 ^4 1 S . «

. 1 5^^ 1 n , ^

. ?07 4 . 0 .310 -1.7

.413 -s . 1

. '^^O -M . q

. «?7 - 1 « , ?

1.031 1 oq . 1 1.240 -?0 . 7

1 , SRO - 1 1 - 0 2.0^6 - 1 7 , n 3.100 -fl . 1 4.133

6. IQQ -?'^ .q

8 . ? ^< •=> -?Q . 4

10.33? .• Q

J. t, • ' ' '

' ? 1

1 S . 498 1 1

1 • I ? 0 .

- 1 S

PFPCI- "MT

( KEV ) DT rFFPPK'Cr

• 1 0 3 ? 1 .

. 1 ?4 16.?

. I 17,1

. ?07 1 Q . ?

• 3 1 0 1 S . 0 .413 7.4

- 8P0 - 7 4

R ? 7 — A 4

- Q ^

1 ?4 n

1 - 0

? . 0 - 1 1

1 inn — 1 Q

4.133 -1 '^.o

6. 19C) -IP.n

8. P'S'S -?1 .

1 0 .33? ^34,4

l?.3Qft 1 lS.4qft ?.4

?0 .f.f^3 3.4

, 4 t.' + 0 ^ 7 . I '+ ^ u

7 , 0 t -t- ^ .

' + .ih

. 7st;-t-()K . ? 1 F + I) b

, w n E + 0 f> ] . f-, s i- * u ^.

1 , W C, p + ; ) ^ 1 .

^-^ ^- + 0 1)

1 . n7F + ^^- 1 . 1 ^ + \ , h

4 , 4 0 1 + 0 4 , ^ U O

? . 1 0 E + n s ?.-> 7^ * ( )

1 , 0 ^, t + 0 S . 0 7*=^ >• U •-.:)

fS , f^OF + ')S . ! P F + I

^ , ? 0 F * c. 4 . ^ ^ r- + F'

1 , Q q p + (

^. !j ^

7 , ^ n E + 0 ^ . 1 F + U 4 ? , + 04 .3 . 1 F U 4

, a 0 E + 0 3 1 . ^.-fh + !)4

4 . ? 0 h * f 1 3 s , q'^E + (J J

? , s n E + n 4 ? , a F u '+

1 , S E + f 4 1 . > + 04

^ 3 0 p + fj H ? 1 ^" + (/ 3 , ^ 0 F. + 0 1 +

ij

„1 a

-. J H . H F I'l ^. -S . -J f- + (J o

7 , r, f + l) F.

. 3'^.E n f-, S . '4 1 F + J t.5 4 , q 0 r. + 0 <^ 4 . M F > 1.) h

>

^

c, t f + r, f. c .'^ U b

1 , 4 0 E + ^' 1 . ^ 0 h + u*-'

, ? n F + ') h . f> P (- + U S

^ 0 p + P ,

^ y

'-^ 1-

1 , n t

+'!'-'

1 . / 7 F + (jt) 7 , H 0 F, + ,') R H .

1

.-^ P s , 1 0 E + '^ E S . 4 P F + ^)

, 1 n F + 0 P ,

f-^ F + Ob

7 . n F + 0 4 -) . P 4 r + (; 4

1 , F, 0 F * ! ) 4 4 . ^'^F + !j «+

1 . ?0L + (1^ 1 ,4'.F * 04

S . 3 n F + ) 3 h. 7

-^^ * 'J J

? , 7nE+ ;i4 1 , M r 'J 3

1 , 7 n E + " 1 . P 4- g ^

. 1 n p + n \ . 0>^F + i; J

4 , ? 0 F 4- r 1

a .

') it, c * ,1
Table II. Continued

P F R r F ^1

( KEV

)

DIFFFPFMCF c U T P F' KAMA r.j .10 3 1 7 .

"^^ H , 2 f ' t-' + 0

'^^ 6 . W'-i- + Oh

. 1 ?4 13.fi ! . B F 0 b 6 , V 0 I-' + ij b

.15S 1 .S 6 , R fl t •» 0 S . ^ F + u 6

. ?0

1 S , S 0 E + 0 6

.310 30 . 0 3 . n + 0 . 6 f + u 6

• 4 1 3 3Q, 7 2 . ] n F + 0 IS 1 . SuF f 06

. 6?0 -^.1 6 , 4 f") F + 0 S S 4 P" + u b

.8?7 -2 . 1 ^ , 4 n F + 0 3 .

'4 7 + 0 b

1.033 -3 . 0 2 .no F * n s 2 . 0 6 1- + 1 ) b

1 . ?40 on . ? , I n F + 0 ^ u. . 7'-F + Ob

1 .SSO -•^ . 0 , h Ti f; + 0 s b . 11'-' + b

<f . 066 -9.7 2 . 7 0 h n s r'. . H ^ t- + 0 b

3.100 -ic>. 1 ^ . 0 F 0 4 1

.

(JbF + Ot)

4. 1 33 -1 7. A 4 . 0 0 F -t- f ) 4 4 . « 7 F + (J 4

6 . 1 -17.7 1 , p + p 4 I . s 4 1-" + 04

8 . ^^'^^ 6 , 1 0 t. + 0 1 , S 1 F ij j

10.33? - 1 <P . 4 . 7 n F + 0 3 4 , 0

''-^ F * U 3

1 ? . 3Qft 4 . ^ 1 , Q 0 F + 0 4 1 . M ^ F + IJ 4

1 S . 49^ 6 . 4 1 , 0 F 0 4 .

'-y 7F ; ^ ?0 . 663 4.^ 4 . 7 0 F + f) 3 4 , 4'J(-' 4 0 J

A h> S F fv I ENERGY D F p C f- T (KEV ) OTFFFUf--MCF ^TGi) f PF K a A i-j .10 3 1 fi . 1 1 . (S P F + 0 ^ ^ . 1 b F * 1 1 6

.124 17.^ 1 , 4 It F + 0 ^ i 0 F f 0 1)

. 15"^ 1 ^.^ 7 . ] n F * ri 2 "< t- + tj b

.207 1 0 b , 7 0 F -t- r» ^ ^ . O'-'F + On

.310 11.7 3 . 2 t + 1) ^> 2 . P ^

^ + 0 b

.4 ] 3 9 . 1 1 , P t. + 0 f-, 1 . 7 2F + Ob

.620 - 1 n , n , M n F + f") s 7. S <^ f- 4 1 J 5

-7.7 3 . 7 0 F + 0 S 4 , 0 1 {)b

1.03^ -7 . Q 2 , 2 F * 0 ^ - * r--> P t ;

)

1.240 -6 . 7 I , 4 F + ' "i 1 .

t- + ( ; -,

1 . ^"=^0 -S. 3 ^, . 4 0 F + 0 ^ 7 -i F + 0 b

2.066 -4 . 3 , 2 0F + ^'^ F « (

, b

3.100 -7.1 1 , 1 n F + 0 s 1 . 1 i ! 4.133 -11.1 it , 0 t-_ + 0 4 1

1- n <+ 6. l^Q 1 , 7 0 F + n 4 1 .

- -1 r 1) U H.26S -1 0 .f 7 . 7 0 F + ri 1 . r, ) t- + ij 3 10.312 -17.2 3 , 0 F. + 0 3 + .

'

] F + 1 } J 12. 3c)R 1 n . 1 . 3 f ' F + 0 4 • 0 ^ y + U 4

15.4QB 3.4 1 , 1 " t. + 0 4 1 . 1 4 ^ > 0 <+ 20 .663 -2. s , 0 0 t + f) 3 s. 1. 4f- t 0 3
Table II. Continued

S t L K N 1 1 ) M

ENERGY P F P C f ^! T

( K E \y ) D T fffpfmcf Mr GU ] t-'t- •<' A A r^i .103 1 1 .s 6 , OOF + Oh F .

^ U 1- h

. 1 ?4 ?q

7 , S n t: + (1 h F .

. 1 "^^ 1 s .

7 . 1 r t: M ^^

1 1 i- 0 f---

. ?0 7 1 7 . n 6 , 2'=^ fc. + M A ") .

^ '+ u h

.310 , n 3 . S^^l- + O'S --t

;-' -t F b

.413 .

<= ? , 0 OPl + Oh 1 .

' t F + i f-,

. f>?0 -14,3 7 . 0 F -f n F .

t- »)-)

. 8?7 -1 3.« 4,ont + 0'^ 4 . h 4 f- + ;j F 1.033 -1 1 .'^ 2 , 4 S F + 0 b . 7 7 r + V) F

1 . ?40 - 1 . 3 1 . S 0 E + 0 S 1 . 7 0r * ,)-,

1 .sso -P. 7 6. OOt + OS h . F 7 F .1- ij

'- I 2. Of.^ 1 . 0 .) . "OE + O*^ 3 . 7 F- F + [1 b

3.100 - 1 3 . R 1 . 1 E + 0 S 1 . ^3E + ,)D

4.133 5 . ? n F + 0 4 F . ? '^

t

" + ; ( 4

6. 19Q -15.1 1 .MOE + 0^ ^ . ] 2 F 4- ( / H « . -1 3. o ^ . 4 0 t + 0 3 9 ,

,^ 4 - + 'J ,1 10.33? -1 3.'^ 4 . h n F 0 3 5

^. 3 F + 'j 3

1 2 . 39B - 1 7 . n 2 . 7 0 E + !1 3 3 . 2 F F 4 ; , 3

1 S . 4QR ^.9 1 . 3 7 F + n 4 1 . p i-i (-'

•». i,. 20 . 6*^3 . 1 S . R 0 E + 0 3 S. H n F !

' _i 30 . 9qS 3 . 4 1 . 0 F + 0 3 1 . 4 F 0 3

M Pf)|v 1 M?

ENERCtY PFPf H>iT

( K E V ) 0 T FF-FPFMCF '^Cr.u I ^F

. 1 03 -19,^ 3 . 0 t- * 0 F. 37 3 F 4-

. 1 ?4 36 . n . 4 0 L + 'I F ^ . 7 ] 4. n h

. 1 ss ^0.7 7,7=^ F •» " F , U -^l t- + (1 p. .20 7 "^1.6 7 . 3 F E 0 h F . F M F * ') h

.310 13.7 '+ , 1 n t f 0 h 3. F. 0 4-

;

! f-, .413 3. « . 3 0 r + 0 F 2 . P P 4 1 ) b

.6?0 -?1 .? 7 , M n t * r s 9. M O F + ; j i-j .H?7 -1 ?.M ^ . F n £ + (1 s F . F 1- 4- ,i 1.033 -9.9 2 , =^ E + S 3. ] ^ F 4 (;

1 .?40 -10,0 1 . H R F + 0 F 2, "FF + lib

1 .s=^o A 1 f,. ^ 6 . ? n E + 0 F i . > i) C 4 1 ^ 2 . O^f. -10.4 3 . 7 F E * ^ F ^ . 1 ^

^ f 4 / -) 3.100 -19.^ 1 , 2 0 E + n F 1 .

in. '•) F + 1 ; F 4. 133 -??. 7 F . 4 0 E. + ( I a F ,

^, ^ (" t (

6. 19Q -??. 1 1 . F c~ t + n 2 , 3 F' * u &»?(^'^ -?\ ,q . ^ 0 F + n 1 1 . 0 '-< F 4 0-^ 10.3 3? -?4.? , F n F 4-0 5 F, Q y 4- { , . i, 12.3QR -?^.4 2 , 7 0 1. + n 3.

15.49R 1 A. P 1 , F F F 4. n ^ 1 . a i 4 0 -4. 20.6^3 7 . 9 0 E * 0 3 F . ]

t- 4 J J

30.9qS -?. 1 2 , 0 0 E 0 ? 2 .

' ) 4 F + 1 ) j;
Table II. Continued

KPYPTO^i

ENERGY p p p p c M T

( KEV

)

DTFFFPFMfF */( r" c i 1 T D t"

f'1 A N

• 1 0 3 -^^n . 7f

1 5 n (-' a. n A 1 C\ \^ % i \

- I . ' .5 . 4 1' t + n '-v P » S M h >• 0 h

9 1 J.J 1 7 A 1 n C J. A A "3 "7 C J M w b . w r + U h

• ?.07 D , 4 ( I t •• u b

. 3 1 n A 7 .1 y. A U -i. /'i ^ 4, jPi^ +(7b

.413 J » r

P ^ C i- ^ A ^ <i , n t. + ! ' p P.n ^t. + Ub

• ^' cT V,/ - 1 7 A Q U A t ^ n L 1 . I ^ + U O

A P 7 — 1 r , <

CI / A C" A A £1 n, ISF + UtD

1X • 0V O -3 — 7 Q 3 /• A C. J. A w i.b'-'r + Ud

p , 4 0 1 +()::>

1 • ^ ~ V/ "7 A A C 1 A CI 1 , 4 n F + s

c • V' rj o 11 1 A LT j_ A *+ • 1 (1 L + (1 b b , P 0 F + ij 3 - 1 n n — 1 Q A 1 /. A C" J. A C

1 . 74h + Ob

4.133 -?3.5 6 , 1 n E + 0 ^. 7 , 9PF

6. 199 -?5 . n P . n n E + 0 4 P , 7F + u <+ O • f_ O 7> 1 , P P f- + l; 4 in T "3 o — ^ n , H 6,701-+ u 3

I C • J *7 n _ ? 1 Q

3 • ? 0 1 + (") 3 4 . 0 9 F' + ! ) J

1 zj • *T ^ n 1 r • /r^ • n t. + i • 4 1 . S F > (J it

c; u • •) n J 1 1 • r> r , n h + 0 ^ 7 . 0 ^. F + U J

3 f1 9 Q R r r n h + f) P . P 7 F + 1 j 3

FnjF Rr; y p F D r p M T ni-^ TI P^P ~ r l:JF^l^^ r I 1^

' I. K z': ^^ Kj _ A c: /L 4 , A n F + u

-) _ "3 1 c: 1 A A L . ri /' 1 , 4 A 1- -f ( ; h

4 . P'lF + I; h

? n 7 In A 4 , *^ 0 t. + 0 b , 3

"^'- + ;. )b r , ^ 4, "^OE + Oh 4 , 1

»•< + U b

_-T.I C 1 , ^1 S h + 0 h P . 7 9 f + (.1 h

A p n - 1 . ' 1 . P '-^ L + . 1 '^ 1 . P 7F + OF

P 7 1 O 1 ^ . 7 n t + 0

"-^ 'S . ^ 7 + f) f

1 n T J. • " _-5 ,1 ^ 1 .

•< ^ , 0 n h + 0 s 4 . 1 P ^" + U o

1 P Zi n 11 1

J 1 • 1 . 0 E •- 5 P . 7 0 + ! j

1 c; c, n

1 « 1 1 .

i'' 0 E + i'l c,. I . ^ 7 - + I ) - c % U ri n - 1 9 , S 4 .

<-) 0 t * 1

S .

<^ f-' + -

, 1 1 fi n o • 1 11 U - 1 H , 7 1 , ^ fi h + 0 1 . 7 f + i

, •-) — in p A r> A t i A S , M ^ '- + '., u 6. 199 -?.r> P . o F + n P . 9 ^, F" 4 i; H

H . ?f>5 ^.9 1 , 4 n F ri ^ 1 . 3 n F + , j 12.398 1 0 . P ^ . 'V n t + 0 3 4 . 4 ^ + I. i ? 15.4qP -5.9 1 . f 0 E * n ^ 1 . 7

•' ) H + i j 4

2 0.^^3 IP.

8

H , n F * 0 7 , M 0 ^ + 1) J 30.9qs 7. ^ P . 7 0 E + 0 3 P . b K + 1 J 3

41 . 3?7 4 . 0 1 . l^E + n

1 . ] 1 E 4 0 J
Table II. Continued

tNfc W(^Y

( K E V ) -.irr.ij 1 Of K A ' 1

i - j .103 -6 . 7 5 . 1 0 h * n n , U 7 F * 1 ,1 "5

. 1 ?4 -^.7 4 ,70 tr > 0 S 4 .

"•i -> i- + \i b

. 1 -83.3 3 , Q 0 fc 0 ? . 3 F + ij »-) .207 -14.3 <+ . 3 0 E + 0 h . 0 ^1 F + 0 6

.310 13.3 5 .on F + 0 h 4 , 4 1 F + 1 , b

.4 13 1 2. n 3 , 4 n t-^ 4- n ^ . 0 4 F + ij h

. 13.4 I , 6 Of + '.)(

I . 4 1 F * ()6

.«?7 17.3 . 0 0 t + 0 5 7 . 7 F + !]

1 .0 33 23.0 . 7 Ot + OS , ^ -3 F + r, ^

1 .?40 31 .7 , 0 n t. + 0 s 3 .

(') 4 * IJ

1 .5R0 49. 1 2 . 6 S E + 0

1^

1 . 7 -* r -f ( ) h

2. 066 -15.1 4 . 7 n t + n s 5 . s 4 f; 4 (

) s 3.100 -4.2 2 , 1 0 E + I) 2 . 1 W F' + 0 s 4 . 1 ? 3 5 . 1 1 , 0 E + n s , 9 ^ + 0 4

6. 199 33.6 4 , 4 0 h + 0 4 3. g F + ij 4

8 . ?(^5 ^3.4 ,^ , 3 0 E + 0 4 I . ^ i'! F + ;) 4

12. 3Qrt 1 nn . 0 u . 9 0 F + 0 3 4 , ^SF (J 3

15. 4Q« 1 0 ^ . ^ S , 6 r E + 0 2 .

5 F + ^,1 J

20 .663 36 . n I . 1 7 F + 4 0 + U .-5 30.99'=i 25.'^ 3 . s 0 F + n 7 Q F + u 3

4 1.327 22.2 1 . 0 E + 0 1 .

^' '-^ + !)

f.nepgy p c p r f-M T

( KEV )

1 r r; ij

J u t: K ^ " f\j .103 1 H. 3 7 , IS fi E * 0 s 4 P F + 0

. 1 24 16.7 6 ^ A (1 F + 0

«~ ->

. M F + F

. 155 4 A 4 . 8 p . A 0 E 0 1 4f + lib .20 7 50 . Q , q r E -n1 5 / F * 'j t) .310 -6 . 0 4 , 4 0 E + 0 6 n*- F

' * U C

.413 -3.0 3 3. .^St" 4 DO

.620 -^.0 1 . 5 n F + f) h 1 .

'=.'^1^ 4 ;;b .Q?7 -3.6 A . 3 0 E 0 S . ^^ I F f M -1 1.033 -4.1 5 . 0 0 E 0 s 5 . ^ ? F 4 ,j

1 .240 1 7. n 4 . 0 E + n s 3. '4 ? F 4 1 1

1 .550 17.3 ? , 3 C. F + ;', S 2. 0 n f-' 4 i.i s 2. 066 42.7 1 , 4 0 E » S M 1 f" 4.^4

3.100 -9.7 P , p 1) V + p, ^ 4 4 F 4-

(^) 4.133 3.7 I , 1 Q F + M S 1 . ] 1 F 4. i ;^ 6. 1 99 ?3 . n 4 , FOF + fW4 i . *^ F> I- 4 1 ) 4 8.265 ^4 . 1 2 , 4 n F 0 /•» 1 . 7 F 4 0 4

12. 3tJ8 ^2. 0 I . 0 0 E + 0 Ur'-^y 4 0 . < 15. 4Q8 104.'^ 6 , ] 0 1-

. + m 2 .

•1' -t E 4 (i ;5 20.663 2^ , « I . 2 0 E + 0 4 . 4 iS f

4- ; 1 J

30 .9q5 33 . 2 4 , 1 n e + 0 1 f i >-• F 4 i

, 41 .327 •=^8.3 2 . 1 s E 0 3 1 . 3 h + (; J
Table II. Continued

7 I hv r: 0 i\i T I ! M

ENERGY PFPCFMT

( K F \/

)

OTFFE^^F^'CF K A

^' M '1

. 1 0 3 .« 7 , 2 n r * n s 1 . 1 4 ^ V / "3

. 1 ?4 . 5 6 , 0 1:. + n s h . 7 r- * 1

' "5 -14.2 s , 2 n E * 0 h .

fj ^- - (

,

,?m -74 .S 7 , 0 0 fc + n s + ' ; 'J .310 1 Q.2 5 . ] h + 0 I.' .4] 3 14.8 J ^ g u, K + 0 :! , <* r (- i; o .'SPO 14.7 . 0 n F_ + n ^ I . 7 h * !J6 10.9 I , 0 f^ t * ri f w . ^ ^ f- * 1 1 S'-v 1.033 1 6.0 , « 0 y + r

i s s . -;'t- f 1

1 . ?40 2S. 7 4 .

' 0 + f

] ^\

1 \ u.

1 .sso 38.1 3 . 1 0 E + 0 S . 2 r + 1

i -1 2 . 06<S 1 . 7 1 . ^ 0 E + 0 1 . 1 1 - , 1 —

,

3.100 - . 2 . 7 n E + 0 . Mf-' • ) b

4.133 9.3 i . 3 E + f 1 ^ 1 . 4 V '.' 6.199 2"^ . 4 n . 0 r E + /) A a ,

11 1^ + U4

8

.

^(^ , ? 2 . 5 n E + 0 4 1 ,

.-i 4 i- -f ; ) 4

1 2 . 398 66.1 1 . 0 0 E + 0 4 6 . U

'

' f » ;

lb. 49ft ft 1 . 1

• 5 . 9 0 F + ri ^ . ^ 'J J 20 .6f,3 ?Q . 1 . 1 0 E + 0 ^4 1 . 0 0 f- + U 4 30.99'^ 2S . 1 4 ,

>^ 0 1, + 0 3 -s . s

•• ij J 41 .327 3 3.3 2 . 0 E + 0 1 . 0 f- + . 3

M 1 riH 1 u.-i ENERGY

{ KFV ) •irr-jiwi- K /\ •• • a '-i .10 3 -P . A 7 . 1 'i E + 0 K 7 . / 7 F + U 5

. 1 ?4 -14.^ , n ir + 0 7 .

t-" + ' /

. I ss -2^ . ? ^1 , 0 E + '1 '-I /' , -1

1

' ""i

. ?n 7 -^4 , -J , n p + 0

u, u ^

c. ;: 4. ' ) ^) .310 -10,0 4 , 1 - E + 0 6 4 ,

' 1 ^-i f- + i./ o .4 13 1 , n ^ . 3 2 E + 6 3 .

'-'^"^ + '. ) ''J .6?0 22.

/ . 4 0 1: + n 1 f- 4 ,) ^

. R?7 2?, ^ 1 . ^ ^ E + ' ' 6 1 .

'> ^ 1^'

t- 1.03 3 ?1 .Q - . 0 0 E + 0 s f ^ ^

-1 A f- + (J 5

1 . ?^o 23.1 "1. 3 0E + '>'^ 4 , n (- +

1 .S'^O 30 . ^ 3 . lOE + i*'^' 2 . -> + 2.066 40,4 1 . 7 5 E * n 5 1 .25 E + .! ^5 3.100 -1.2 < , 0 0 E * !") i . ' ; 4 + ' "7 4.133 - 1 . i . 3 E + n ; —

)

6. ] 99 1 0 . P . ' ' t + 0 4 a . 1 + ; 4 8.265 17.4 . 1 ' r. + '"! 4 2 ,

(

•) i> V +

1 2 . 3Qft 3?. ^ . 9 '"1 h_ ^ 0 1 ^ . 7 0 i^' -•• ; 3

lB.4Qq 4 0,1^ 5 , ] n h * 0 5 3 . ^ + .1 J 20 .6f^3 12,7 1 , ? ? E » 0 a 1 . 0 E 4 ! <+ 30 .Q95 14 , 4.20^ + 0-^ -! . 7 F + 41 .3?7 5.5 1,7^ E + 0 1 .

^' * i 3
Table II. Continued

EfvJEPGY PFRCI- ^'T (KFV) OT FFf-^vF ^Tc C (J I ^ K

.103 ] 0 . ? H , H n F + 0 s 7 . mF + 0 ^.

. 1?4 n .« w . 0 0 1 + n s H , 0 F + (J "0

. ISS 1^=^. 1 . ? 0 t + 7 . p * ^1 .?07 1^,7 8 . 0 n F -f fm ^ , ^ * + '0 .310 4 . 4 ? r + ( ' f-, 4 , h F F + .413 ?. Q 4 , 0 4 1 + 0 f^, 3 . M n + (J IS .6?0 -.1 ^'.13t: + ()^ ^^ + U h

1 . ISF + n^ 1 . ] (V F + 1.033 -3.0 7 . 0 0 t + 0 7 . X ? f- + ( : b

1 .?40 -3.? 4 , 0 t. + 0 S 4 ,

1 ."=^^0 -1 O.f, ? . 0 F + ( )

^'-^ 0 F' + (.i b

2.06^ -10.? 1 . ? '=« e + 0 s 1 . 3.100 -1 '^.f^ p . M n F + f' S i . .^r-F 1) J H . 1 1 1 - ! r 1 • r ^ L + 1

' T

1i • ^ J> r

J.+ /\

) w3

6. 19Q -17.) 4 ,

1 0 e: + 0 4 4 , -^4 F 4. D 8. -1 4 .Q 1 , 9 0 £ + ^ P. .-^ F + I ) H 1^. 3QH -9.4 , ^ n F + 0 3 7 . ? ^« f > U J

I5.4qp 3 . 7 0 F + n 3 P + U -1 ?0.^'^3 . 3 1 , ? n F + 0 a 1 . ? 0 F +,,)<+ 30.^4'^ 4.0 4 . ? 0 e. + . 1 6.

,

' i4F -t- 0 ^ 41 . 3?7 1 .'^ 1 .

.q c f. + f

1 , c :3 ^ , , J

T F f H ^. F T T 1

P r W r P T

( K F\M ni p'F-'Ff-*^ Mcr ,/irGu] ^vF A A. iSl .103 1 P . 0 1.04 1

!J ? F + ; S

. 1?4 7.7 'J . ^ n F * n -' • 1 P + !

/ ')

. iss 9 . ) 0 + fi "-^ h7F * - i^

.?07 9.7 H , ? 0 F + 0 7. '--,hF + i; "-1 .310 -15.0 3 . 7 0 F + 4 .

^•"-.f * ( , ^ .41? ?7.? 4 . s n f; + 0 ^, 3. -> 4 F + 0 F- .6?0 1 . 4 n F + n p

p Qf ^ i j .8?7 1 . ?<=.!-* 0 IS 1

^ F t 1 1 h

1.033 -4 / . S n F + 0 s 7. h t-" + ^; F)

1 . ?40 4 ^ 0 F + 0 ci + !

i ^

1 .sso -'=>.7 ? , onF 4- Oh ' «

( ) F * 'JO ?. 0^6 -?.4 1 . ^ b + 11 i . F- 4 F + 1 ) -J 3.100 -1 ft ,Q p ^ o c F + (1 s i

f-. 4 F 4 4.133 -^0.1 i , > t + 0 1 , F »- + 1 ; '1 6. 199 -17.0 4 . 0 F + .' ) A > • P P -I- 0 -1?.7 ? . 1

' F + n i }- + I i ^ 1?.39A -4 .

vJ 7 , 7 0 F + n. "I

; : o f -1-

; i .1

1 S . 4 9 P 4 , 0 F -t '1 3 4 ,

< ^ + ( i j

?0.^'^3 70 ? . S 1 . f . n F + 0 4 1 .

'"^ f-" + 0 30 .99S ^.>^ 4 . 7 0 F + f ) ^ 4 , a 4 t~ ».i J 41 .3?7 11.1 P . ? 0 r. 4 (1 3 .1 . q ^ P * ,
Table II. Continued

M- U T H t N r I

)

t'NF Rr;Y P F R r F ^' T

( K E vy ) DTFrFwRNjCF" Mr r;(j ] lv^ < A .'^ A fx; .10 3 ?f . 0 1 . 0 M t + 0

. 1?4 \^ 1 . C-'^F - 0^ w , ! ; -if I'l "-i

. 1 5S f>,7 1 . 0 2 f- - n f> q ,

'^'•< f- * '.)

. ?0 7 «.4 q , 0 1 0 s H . 7 ^' -nj

.310 -1^0 , 3 7 . 0 F + ' ; -1

1 . P ''-J F' + (J

. 4 ] 3 3 . 7 IF t- 0^ 3 + Oh

. 6?0 12.1 2 ,

'^ F + 0 f- , F 4 F + ! j h

. R?7 -.7 1 . 4 ;^ h * 1 , 4 "^ F * l .H 1.033 -1 . . 7 0 F + 0 s ^ . /^^

1 . ?40 8 . 0 0 F 0 ^ S , 7 r- +1)1".

1 .'=;sn -7.n 3 . 2 0 F + '1 s 3,44 f- + 'i t;. -9.1 1 . t •• n s 1.701- * V t> 3. 100 -'^ . 7 3 . 1 0 h + f »

5

u •( ^^

'f. 1 33 -22. 7 1 . 4 r; F + n 1 . H 1 ^ 4 :j b

6. 19Q -1 q. 4 4 . P 0 F -t- <

' 4 F . q + i ) 4 8 . ?fSS - 1 . 1 2 . '1 F * 0 4 2 , 701^ + (.4

1 2 . 3 q p -10.0 P . 0 0 F + 0 3 p . ^-J f- + ^1

1 5 . 49P 4 ,

fi F + 3 4 . P ?- 4- ( J J ?0 . ^^3 2 . 2 0 F + 0 2 , 1 -' F + (I j

30 . ^^'=> ' •• 5 . 1 0 F + 4 ,

>^ 4 ^ 4-

v.; j

4 1 . 3 ? 7 1 .7 2 , 2 0 F + 0 ? 2 . 1 + fj 3

^rinn 1 1 jM

DPPf f-'M J (kFv) D T F F F ilv F N! C f-" .10^ 1 . 0 1 . 0 3 F + 0 f--

. 1 ?4 1 S.P 1 . n F + n q .

''

' + v) s

. ISS 1.17F*n^, 1 . ''^ + '.i f-> .207 IP.

I . 1 F + 0 f-. q , f : - F + i

)

.310 ?f , 4 1 . 1 0 F + f- P , n : r + U "."i .41 ? q.«5 - 4 , ^ ? F + ' ^ 4.1 1 P 4 .J h

. f^?0 -2.3 2 . F + T! 2 . r-. ] t 4 I J r.

. «?7 1 . 4"^ F + 1^

I . 7 F 4 t; r, 1.033 -4.Q q . ? 0 F + "1 s , ' ^ 7 '-41; : -i

1 . ?40 b , n 0 F * n ^ M ,

! ^ 4- 0 >

1 .=^"^0 -1 « . 3 . 1 0 h + n 3 , 0 .- 4 u 2 , Of^f^ -17. ft

1 .

<=• f

" * n ^ 1 . ^--F 4 i) 3.100 U 2 .

•'^ F 4. r

P . P ^. F 4 0 4.13^ 1. . 7 2r_^.'i'^

6. 1 -10.7 S . P n F + 0 4 r . li 7 F 4 • ! .+ -P .4 p . 7 n F < i 4 P ^ Q ^'^ F 4- ; ) <+

1 2. 39« q . 2 n F + T < W . 7^+ 4 i / S lB.4gP S . 1 0 F + 0 . V' * ;j 3

20 .^^^3 -2.7 ^ , ^ F + I I ^ P . 4 ^ 1- + 0 i 30.9qs ^ .q "-I , ^OF + 'M P , '-^ I- 4- u _i 4 I . 327 ^.7 2 ,

''-^ r t + 3 p . 4 + 1
Table II. Continued

A L. L. 1 1

; f-' PFPTF ^iT (KFV) nTFFFKFMCF K AMAhj

.103 4 . 4 1 . 1 f' - ''1 »- 1 . 0 ^ F + 0 (-^

. 1?4 -3 1 . 0 0 h. '

1 1 . 0 4 f- + (; O

. iss -?.q 1 . n 0 h + 0 f-r 1 . 'j < ^ * f 1 .?07 -.9 1 . n 7 F + 0 h 1 . 0 ^ i + U n .310 10.2 -J , n t + '1

^ i- ( 1 : ~) .413 -4. 1 4 . 1 0 F + () ^ . 2

'•' > + 6

-9. ft 2 . r. 0 F + 0 6. ^ ^ M F 4 1 1 fj

. 8P7 -6.P 1 , f, ?F * 'i ^• 1 . 7 4 F + 0 o 1.033 1 . 1 n t -t- 0 *-

) . 0 7F 4 (je.

1 .?40 -.A 7 , 0 fc. + 0 7 , n^r +()'->

1 .'^SO -9.7 3 ^ u 0 F 0 ^ -4 , 2 1 F 4. (J ^ 2. Oi^^ -16.=^ 1 , 7 t + ' S 2 . 'J'-i- + u':-

.J • 1 WW P ft 7 ^ . 0 0 F + i") 7 , F I

i ^ 4.133 -22.'=^ 1 , 7 fi F » n ^ . 1

*• + L! 5

6. 199 6 4 0.1 . 3 n e. ^- 0 5 7 . 1 ^

' + ( ) '+ -?^, Q ,401: * 0 4 3 , 4 f- + (J 4 12. 390 40] .? , 10 F * 0 4 1 . 0'-'- + l;4 15.49f< -1 9.S 4 . (SOr 0 3 S . 7 [ F + (J 20.^*^3 - 1 4 . ft 2 . 2 0 F + 0 2 . 5 ^ F 4 J .1 30.995 S , Q fi t + 0 y. 5 , ^''1- + '..) .^ 41 . 327 2.4 2 , f. 0 fc. + 0

"< 2 , S ^ *" + ij .I

ENf PHY p r w r f: ^ T (KEV) 0 T F F F Lv P N, r t- .irr,.j T^vP

.103 34 . 1 ] . 3 7 L + 0 F i . 0 ? F !_) f;. .124 2S.= 1 . 32F + ''^

1 . O^F 4 (jb

. 15S 37.3 I . s n F + 1") fi 1 . 0 '-^^ 4 U r-

. 207 36.0 1 1 . i + Mf,

.310 23.1 1 . 1 0 F + 0 >-< , u f- + i j ^ .41 3 11 ft.

u. . 4 5 F + 0 t- 2 . S 0 f- 4 ( 1 r

.620 -1 4.'^ 2 , ^ 0 F n f~ 3 , 0 4 F + U h

.f^27 -24. 1 I . 4 2 F + 0 ^, 1 . r-. 7f + Oh

1.033 -IQ.? . 4 n F + ('i ^ 1 . 1 ^ 5^ 4. u 6

1 .240 -12.7 , 7 r> F 4. rm 7 ,

^- MF 4 1;'-.

1 .SSO -30.4 j , ? 0 F * '1 F 4 , F Of- + !»S 2. OAA -32.4 J ^ . ?'.-F 4. ( , 3.100 1 oq.ft 1 . 7 7 F * n K . ''F 4.133 - 1 9 . M 1 , g ri + (y . : < 7 f 4- 0 ^ 6. 199 -16.4 .

t, n F + 1 ^ 7 . 7 7f- 4- H.26S -1 4.Q ^ . 0 nh * 0 4 3 . S 1 f 4- ( 1 ^ 12.39ft -1 0 .Q 1 , 0 F * 1 . 1 M.u

15.49R -10. S . ^ n F + 0 3 6 , 2 ^ '• f (.1 ,.^ 20 . 6^3 -ft.

? , ^ n F> n i 2 , 4 4. (J , A 30.99S ^.3 h . 3 0t. 4- t i "<

••) ,

'-ii " (- 4-11:}

41 .327 5.7 2 , Q n f: +0 3 2 . 7 4 t- 4-

^ , J 61 .9q0 13.1 1 . 0 fi F + ') 3 h .

>^ a

»'' + c
Table II. Continued

C ADM I ijM

emergy P F R r 1- M T

( KEV ) niFFF^veMCF c n u I F .10 3 ] . 7 0 E + 0 h

. 1 ?4 1 3. 1.24t>0^> 1 . O'-'f- 4 ut,

. ISS 1 0 . « 1 . 2^^^ + 0^ i . J

^i- f 0 t:- . ?0 7 ^ . 4 I . + f)f- .310 1 O.Q l , (1 c K * 0 .'- '•( ( ^ (

' '-.« .4 13 -3.'=> 9 , 2nF + ,

'

-v 6. >^ + ; .1 s

. 6?0 '7.1 J , '^i S t + 0 !>• 2 . 7 I i- -t- uh

. 7 ^.4 2 . 2 0 t * n ^ , 0 < F 4 ,j 1.033 P.

9

I . 3 P t + (1 s

1 . P^O 1 , P 0 H + 0 t> ^, , '! ' i '- »•!' s

1 .'^'^O ^.3 , 0 ir> 0 ^ '4 , 't' 4 •-Ob

'^ . Of>fs 2 , ^^ n F + M ^ .

'"^ 0 b

3 . 1 ri 0 -16.7 / . 7 n E + 0 y . .-• "-i »- + i / 4 4.133 -23.0 2 , n r, f + 0 6.199 -'3.3 'V , n b + n a 1 , 'i 0. + i y 4

i . 0 0 E * 1) u .5 . + ;j 4 12. 3Q8 -2S.7 9 , 3 0 F + " ^

1 , •» • } H

1S.49R -'7.R 4 . 9 0 E + u ,3 , 7 ^ + ( ; 3

?0.6f,3 -31.3 2. 1 0F>n •( 3 , (X^.r- 0 ji 30.t)9S 3 . ] 6 . 7 0 E + r, f-. , S n - + , j j

41 . 327 2 . 9 ^ E + 0 3 2 . 7 f- 4- 3 61 .990 4.f. 1 . ^ E + 0 3 g ,

i^, + i

1 ^

I Nf' I I'M ENERGY p^P(-^-^!T

(KFV) n TFFFPFN.CP '1 r r- u r

t .103 SO . 7 1 . 8 n F -t- n 8 1 .

.'1 At^' + ; . 1 24 1 P. 3 1 . 2 ^ E + 0 8 1 . ' ) 1^ F +06

.155 P'^ , Q i . 4 F -.- 0 A 1 . 1 7 F 4 (J F, .207 ?? , H 1 . 8 E + fi 1 . P9F + Uh

.310 4.« l.l'E+08 1.07 P + (.) b

.413 27.4 1 . OOF + (/^^ 7 . H F + 1 ) b

, 6?0 ?4 , ^ U F + 0 ?,'---! f^' + u b

.P27 9. « 2 . 4 E + 0 A 2 . . •^ 0 s^ ' * u b

1.033 9.4 1 .snE + o^ I . 3 / F + (; b

1 .240 -. 1 9, not* OS 9 . (j ) F f 0 b

1 .SSO 2.2 b . S 0 h + . 1 ^ b . .-^PF + jjt-, 2. 066 -S. A 2 . 8 n f + /m 2 . ? 3.100 -14.2 . 7 n F + n 4 .1 . 1

1- -v 1 s 4.133 -1 .s 2 . 3 0 F + ^ , i 4 F + ( ) 7) 6. 19<3 - 2 1 . P / . 2nF 4 f)4 . 1 ' J M . P'SS -'1.0 3 . 30F + 04 '-+.]'- I" + l) M- 12. 39P - 1 o, p 1 . 1 0 F + 0 a ] , r^p- + ; lH 1S.49P -17.9 . 1 0 F * ^ 3 ^ , a 'J h 4 ( ; -j 20 . 68? -17.0 2 . P 0 F. + M 3 S .

' ! 7 t- + 0 J 30.99S . 3 7 . f! F + n , ^ 4 F + 1) J ^ 1 . 327 3.4 3 . 4 0 h + n 1 ? , 2 F ^ 0 A 6 1.990 1 . ) 0 E 4- n ^

I , 1.1 4 f- + 0 j
Table II. Continued

T I H

F N F w r 1

l_ l>( [_ 1 P p R f

t M T

( KEV ) n T pppppf^irr M r u I E K A M A N

-• 1i mV -J ? 1 4 . ? H . 2 0 t- + 0 6 1 , 3 4 F (j t,

. 1 ?4 ftft , 0 1 .ft^t + 0^ 4 , ft 4 F + u b

Q 1 . 2 2. lOF + 0^ 1 tPO^ + Uh

. ?0 7 - ^ • ' 2 . 1 n E + 0 6 1 . S F -UJ b

.310 1 ^ ft 1 . 3 ^ E + 0 6 1 . 1 ^ F 4 ;j b

.411 V - 2 0 E + 0 rs , A F + 0 t>

. ? 0 3,onF+06 3 . ] F ( I h

— 1 4 1 F + n A , < F + (J r,

1 • V» J J -7 ? 1 . IftE + OA 1 . 4 F +-0 6

1 . ?4 0 -ft , 0 9 , OOE + O"^ 9 , 7 y t-" + 'j b

1 . S^S 0 -7 ft S . u n F + 0 S b.MAJ^+y^

-ft , 2 . 7 E + 0 S 1 . n 1

t- + .;i b

3.100 - 1 7 .

"5 9 , 2 0 E + 0 A 1 . 1 1 F + I, <o 4.133 41.2 2 . 6 0 E + 0 S ] . ^uF + (jb

6. 199 -20 . ft ft . 0 0 E + n A 1 . 0 1 F 4 u b

8 . P'SS - 1 ^ , 3 . ft 0 E + 0 0^ 4 , b ^- F + (,n+

1 2 . 3 Q « - 1 . 1 1 , 2 ^ E + 0 ^ 1 , 4 F^ u ^ 15.49R -14,3 6,9 0E+ni A , ObF + i; .3 20 . (S^ 3 -12.0 3 . 2 0 E + n 1 3 , b4 F + 0 J 30 . 99R 10.7 3 . 2 n E + 0 3 7 . 0- 1 F + 0 J

41 . 3?7 4.4 3 . A 0 E + 0 3 3 , 4 F + J J

61 .990 7 . 1 1 , ? 0 E + 0 1 . ) P F^ ( i j

Nl T 1 M 0 N| Y ENERGY

f K F \/ ^ M r 1 1 T p F

- 1 n 1 p ^ 0 p + n A 1 , J r * D

. 1 ?4 ft 1 n 1 P ^ P' + ( J

• 1 ~ c; u 7 1 Q c; c" J. n A i m ^ .T ~ + w O

? n 7 AO ^ • 1 n c + n o 1 /i ^ P *. I'l A

' .1 • n 4 1 1 1 P c; p J. A

• " C? nV..'

, ? 7 14 ft ? 7 ? F 4. f 1 A

1 A 1 1 1 F + n A

1 . ?4 n 1 1 S 1 p n F' + 0 A

1 H 0

1 ft Q •« Q n F + fm < P M F + 1 } -1 3.100 7 4 1 1 0 F + 0 S 1 P 1 F + 1 1 -) A • ' 1 ' ^ V,' -J 4 111 PR p i • ^ J

• * U J 6. 19Q -?A . 0 7 . 9 0 F + r) A 1 .0 7F + ijb

-24.4 i . 7 0 E * n a 4 , « ^ F" + 0 1+ 12.39ft -23.3 1 . 2 ^ E 0 4 1 , A--<(^ + 0 4

15.49ft -?3.S e , p n t + 0 --s H , H -) (1 j< 20. ^A3 -23.

Q

3 . 1 0 1: ^ n T 4.0 '-* f-' * 0 J 30.9QS -1.7 . 1 n E 0 -i . ^ + Vi -3 41 .327 -.ft 3 . ft 0 e * 3 3 . 1 F + ( , J

61 .990 1 . 3 n L * 0 3 i . 2

i-' 'J 3
Table II. Continued

ENERTiY PFPCFNT

(KEV) DTf^FFPFMrF K A f

'' A i .103 flQ , Q 2 . 3 ^ E + a A I . 24F + (!b

. 1?4 7S.? 2 , mF + 0 h 1 , 1 6^ + i;*^

. ISS , n 1 . 6 F + 0 6 1 . i)2^ 00

.?07 47.<=> 2 . 1 8 E + n A 1 . 4 s F + I) h

.310 47. ? 1 . 9^E •»• OA 1 . 3 2 F 4. 1 ) h

.413 ?0 . 7 I . 2?E> OA 1 . fi 1 P. + ij6

.6?0 18.0 6,'-inE + ()6 S . 3 4 H + i.) 6

47,4 3 . 0 ^ E * 0 6 2 . n 7

1- + 0 b

1.033 ??,6 2 . 1 n E + 0 6 1 . 7 K + U h

1 .?40 =>.6 1 .20E + n6 1 , 1 4 F + U 6

1 ."=^50 7.7 7 , 4 n E + 0 s 6 . 8 7 F + (J ?. 066 6.4 3 , 8 0 E + 0 s 3.S7F + .)b

3.100 6.0 1 . 4 0 E + 0 S 1 . 3^F > l)b

4.133 T31 . 7 2 . 9 n E n ^ 6 , 7 ? F + (J 4

6. 199 -21.8 / 9 . 1 0 1 * n 4 1 . 1 At- * 0 b

8.?65 -19.4 4 . 5 n E + 0 ^* S . ^ "^f^ •• 0 4

12. 3C1B -21 1

. 4 ("t E + rt 4 1 . 7 I-. > 0 4

15.49R -20 . ^ 7 . 7nE + fi ? 9 . A 9 F + 0 3

20 .663 -21.1 i . S 0 E + 0 1 4 , /4 4 f-' > 0 30.9qS t^4

. 9.1-0^ + 0^ 1 . 4 8 1- -t- v) 3

41 .3?7 -1.2 4 . 1 n E + 0 ? 4 , ] ^ r + 0 3

61 .900 -2.7 1 . 3 0 E 0 1 . 3 ^ F * 0 3

IOOUjE

ENERGY D F P r F M T

( KEV

)

otfc-f^fmcf f^CGU T K A f

' A N

.103 ?64,Q 6 . 6 0 E + 0 1 . 8 1

f- 0 b

. 1 ?4 17 4.4 3 , 0 f^E '1^- 1 . 0 F + 0 A.

. iS'i A 1 . S 1 . 7nE + nA 1 . S t + 0 6

. ?07 18.1 1 . 8 n E + 't 6 i . '"i2*-! + 0 b

.310 ^8 . 1 I ^ g c, £ + 0 A 1 . 1 F + U b

.4 1? ?n . o 1 . 4 F +

' ") A 1 . 0

''^ F + (J 6

.620 1 mQ . ^ 7 . 2 OF 4 -1 6 . :3 ^ F (1 b

,f\?l 6 . 9 2 , 4 n P. + 0 ^ , /^4r Ub

1.033 . 4 1 . A ^ F + 0 A I . 7SI- + Ut:

1 .?40 -. 1 . 2 E ^ r, ^ 1 .2 ^ + I i ft

1 .S'=^0 -7. A ^^ , Q n t: ••• 0 S r, 1+ A F u F> 2.0^6 -7.1 < , A + ;

)

3 , >^ + (1 D 3.100 -1 8 ."^ 1 . 1 7f- +or. 1 , 4 4

' > ' ) b

4.133 -33.9 4 . Ti f- ( ) u. 7 , ?(^'<- + !

i H 6. 19Q -?A , 0 i , r) r- + 0 u 1 . 2Ar + (,b

8.P6S 4 . 1 r + 0 6 -1 . 7 4 + ! IM- 12. 398 - 1 0 . f^ 1 . 3 ^ +

'"^ ^ i .

' i + u 4

15.498 -31 .4 7 . 1 0 1- + r, 1 . 0 ^ + U M 20 .6A? -?8. 1 3 , -4 0 t, + 0 . 7

' i

>- + 1 ; 5 30 .9gS -29.8 1 . 1 0 F f 0 3 1 41 .327 4.^ 4 . s n t + ^' 3 4 , 4 r. - + u .j 61 .990 6.8 1 .

=^ n h > n 3 1 . ^ Ot- * u -5
Table II, Continued

X h M ( J K ENERGY PFPCFMT

(KEV) DTFFE^FMCF

.103 3 1 ? . 3 1 . 4 0 t- 4 f> 7 3 • 4 0 *-

. 1?4 PS . 3 . r, t. + ll <^ 1 •

1

\--

. ISS 1 + ;) H. 1 • 1 + ( 1 h; .?07 -?7.3 1 , 0 (1 K + 08 1 H !: ¥ '1 (-1 .310 1 + n 8 1 • + 0 ^ .413 -1 7.? 1 . 0 n h + 0 ]. 1 f (1 h

.6?0 - 1 n ^ . -^oe * OS 7 1- 0 '-s

. «?7 . 30(- + f-. <^ •

U, 1- 'r- + 'J8 1.033 1 . ^ f\ + n h 1 •

^> ) ^

+ hi-)

1 .?40 1 . 3 1 . ••t7F 1 • < ! 1 6

1 .s^o H .^OE. + nt> • 1 7^ ^. 086 - .

>^ U , ? n e: + 0 s • ^

^- 3.100 -3.7 1 .'••.OF + 1 • S<Si- + wS

4.133 -8.1 7 . WlF •t- 0/4 • 7 6. IQQ -1 7 . n 1 . 1 OF + OS 1 * O + (iS

S . ] r. + 0 h !1 7 r + U 'I 1?.3Q8 -1 S.R 1 , 7nF 114 / • 0 / (• + ..; 4

15.4Q8 -18.^ . 0 0 F + 0 1 • 1 OF + i.i 4

?0.6fS3 -^'O . 7 4 , nnF * 0 s • 0 u f- + U J 30 .QQi^^

1 .

"=> (1

* n ^ 1 *

*" >- + 0 .i 41 .3?? 4 . 6 f) r_ + D • 61 .Q90 .4 1 . SOF •f n ] • 6 -^f- + (i J
Table III

Element Energy

(keV)

Percent

Difference

M- edges

(keV)

L- edges

(keV)

K-edge

(keV)

Zn (30)

Ga (31)

Kr (36)

Y (39)

Tc (43)

Pd (46)

Te (52)

1,03

10.3

1.55

0.155

20.7

3.10

4.13

31.0

1097o

6347,

4017o

4457o

7047,

2847,

3327,

5437,

0.157-0.394

1.02-1.19

1.67-1.92

3.17-3.60

4.34-4.94

10.37

21.04

31.81

I (53) 0.620 10407, 0.619-1.072
. 4 A I . -

: . U.S. DEPT. OF COMM. BIBLIOGRAPHIC DATA

SHEET

!. Pi. iU.lCAl iO.\ UK Kt.i-'ORr NO. NBSIR 73-1762, Gov't Accession

No.

3. Recipient's Accession No.

4. TITLE AND SUBTITLE

Comparison of Photon Interaction Cross Data Sets.

VI. McGuire and Kaman Photoeffect Data.

5. Publication Date

6. Performing Organization Code

7. AUTHOR(S)

G. L. Simmons and J. H. Hubbell

8. Performing Organization

NBSIR 73-176

9. PERFORMING ORGANIZATION NAME AND ADDRESS

NATIONAL BUREAU OF STANDARDS

DEPARTMENT OF COMMERCE

WASHINGTON, D.C. 20234

10, Project/Task/Work Unit No. 2400432

2400105

11. Contract/Grant No. DNA-EO-72-804

Subtask No. PC-100-05

12. SpoQsoring Organization Name and Address

Defense Nuclear Agency

Washington, D. C. 20305

Support was also received from

NBS Office of Standard Reference Data

IJ. 1 ype or Report & Period Covered

Interim Report for

period Januarv-Mar . 197!

14. Sponsoring Agency Code

15. SUPPLEMENTARY NOTES

16» ABSTRACT (A 200-word or less factual summary of most significant information. If document includes a significant

bibliography or literature survey, mention it here.) Photoeffect cross sections calculated by McGuire, covering the energy range 0.0062 to

62,0 keV for elements with Z = 2 to 54, are compared with values interpolated from

results calculated by Veigele et al (Kaman) which cover the energy range 0.1 to

between 1.0 and 8.0 keV. This comparison is presented in the form of percent differences between these two data sets, with the Kaman values taken as the reference

set. The cross sections are listed and the differences are tabulated over the energy

range 0.103 to 62.0 keV, thus at the higher energies the comparison is with Kaman

values which were fitted to experimental data. Discrepancies ranged from less than

37c up to as much as a factor of ten in the iodine M^^ - edge region at 0.620 keV.

From this comparison, and from graphical comparison of both sets with experimental

data for carbon, aluminum and tin, we estimate that for Z = 2 to 54 the envelop of uncertainty

of the Kaman calculated values in the region 0.1 to 1.0 keV is of the order of ± 20?o except in the presence of resonance absorption features where the uncertainty can be an order of magnitude.

17. KEY WORDS (Alphabetical order, separated by semicolons)

Attenuation coefficients; comparison; cross sections; photoeffect; photons; x-rays

18. AVAILABILITY STATEMENT

SH UNLIMITED,

I I FOR OFFIQAL DISTRIBUTION. DO NiVi TO NTIS,

19, SECURITY CLASS

(THIS REPORT)

UNCL ASSIFIED

20. SECURITY CLASS

(THIS PAGE)

21. NO. OF PAGES

40

22. Pr

I

I

1
i

!

1