A UNITED STATES DEPARTMENT OF COMMERCE

PUBLICATION

AlllDQ TfiMflTfl

NATL INST OF STANDARDS & TECH R.I.C

A1 11 00984898

United States. Natlo/Photonuclear reacti QC100 .U57 V380;1973 C.I NBS-PUB-C 1973

PUBLICATIONS

REFERENCE

NBS SPECIAL PUBLICATION 380

U.S.

DEPARTMENT

OF

COMMERCE

National

)au

of

I O O ds

ho. 380

[^n3

Photonuclear Reaction Data,

1973
NATIONAL BUREAU OF STANDARDS

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APR 9 19?3

Photonuclear Reaction Data, 1973

,u5n ^ —

E. G. Fuller, H. M. Gerstenberg,

H. Vander Molen, and T. C. Dunn

Center for Radiation Research

Institute for Basic Standards

%i National Bureau of Standards

Washington, D.C. 20234 » e

no- ^ '^0 ^

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

NATIONAL BUREAU OF STANDARDS, Richard W. Roberts, D/recfor

Issued March 1973
Library of Congress Catalog Card Number: 72-600057

National Bureau of Standards Special Publication 380

Nat. Bur. Stand. (U.S.), Spec. Publ. 380, 131 pages (Mar. 1973)

CODEN: XNBSAV

(This publication supersedes NBS Miscellaneous Publication 277 and NBS Special

Publication 322 which also embraced Supplement 1 to Misc Publ. 277. All

information contained in these publications has been combined and merged with new

data to form the Photonuclear Data Index and Bibliography contained in this

publication.)

For sale by the Superintendent of Documents, U.S. Government Printing Office, Washington, D.C. 20402.

Price $2.10 domestic postpaid or $1.75 G.P.O. Bookstore.
Foreword

The National Standard Reference Data System was established in 1963 for the purpose of promoting the critical evaluation and dissemination of numerical data of the physical sciences. The program is coordinated by the Office of Standard Reference Data of the National Bureau of Standards

but involves the efforts of many groups in universities, government laboratories, and private industry. The primary aim of the program is to provide compilations of critically evaluated physical and

chemical property data. These tables are published in the Journal of Physical and Chemical Ref- erence Data, in the NSRDS-NBS series of the National Bureau of Standards, and through other

appropriate channels.

The task of critical evaluation is carried out in various data centers, each with a well-defined

technical scope. A necessary preliminary step to the critical evaluation process is the retrieval from

the world scientific literature of all papers falling within the scope of the center. Each center, therefore,

builds up a comprehensive well-indexed bibliographical file which forms the base for the evaluation

task. Bibliographies derived from these files are published when they appear to be of value to research

workers and others interested in the particular technical area.

Further information on NSRDS and the publications which form the primary output of the

program may be obtained by writing to the Office of Standard Reference Data, National Bureau of

Standards, Washington, DC 20234.

David R. Lide, Jr., Chief

Office of Standard Reference Data
Contents

Page

Foreword ------------------------------------- iii

1. Introduction --------------------------------- 1

2. Gross Features of the Giant Resonance -------------------- 3

2.1. General Description ------------------------- 3

2.2. Experimental Data -------------------------- 4

2.3. Estimating Yield --------------------------- 10

3. Description of the Photonuclear Data Index and Bibliography --------- 12

3.1. Introduction ----------------------------- 12

3.2. Scope of the Data Index ----------------------- 12

3.3. Description of the Index ----------------------- 12

3.4. Description of Column Headings -------------------- 13

4. Photonuclear Data Index (1955-1972) --------------------- 15

5. Photonuclear Reaction Data Bibliography (1955-1972) ------------- 55

6. Definitions of Abbreviations and Sjnnbols ------------------- 122

6.1. Symbols Used to Define Incoming Beam and Reaction Products ------ 122

6.2. Symbols and Abbreviations ---------------------- 122

7. References ---------------------------------- 125

iv
Photonuclear Reaction Data, 1973

E. G. Fuller, H. M. Gerstenberg, H. Vander Molen, and T. Co Dunn

A brief summary is given of the available data on the gross

features of the photonuclear giant resonance. Data are presented

in tabular form for all nuclei where measurements have been made.

In addition, a comprehensive, annotated data index and bibliography

are given which cover experimental data for the field of photonuclear

reactions published in scientific and technical journals in the

period from 1955 through 1972. Organized by element and isotope,

each entry in the index is for a specific reaction reported in a given reference. Information is given on the type of measurement,

excitation energies studied, source type and energies, detector type

and angular ranges covered for each reaction entry.

Key words: Bibliography; data index; data summary; elements;

isotopes; nuclear physics; photonuclear giant resonance; photonuclear

reaction.

1. Introduction

The field of Photonuclear Reactions is concerned with the interaction of electromagnetic radiation with nuclei. The interactions can take place through the intermediary of

either "real" or "virtual" photons. The field was first opened for study forty years ago

when Chadwick and Goldhaber [l] observed protons in an ionization chamber containing

deuterium gas that was bombarded with the 2.61 MeV y-rays from ^°®Tl. This most elementary

photonuclear reaction is still the subject of considerable study both experimentally as well as theoretically.

During the first ten years of its history, the study of the field was limited to the use of real photons obtained from radioactive sources or from the y-decay of highly ex- cited states formed in nuclear reactions. The range of photon energies at which studies

could be made was of necessity very limited. Only after the development of the

betatron [2] was it possible to study the photonuclear interaction as a function of photon

energy. In the late forties, Baldwin and Klaiber [3] were able to obtain the first evidence for the existence of the photonuclear giant resonance in spite of the fact that the

bremsstrahlung beam produced by the betatron was a continuous energy spectrum of photons

with only a well-defined upper energy limit. This phenomenon, i.e., the concentration of

most of the strength of the photonuclear reaction over a relatively narrow energy band, has

been studied extensively over the last 25 years. During the decade of the fifties,

improvements in accelerator technology, data analysis techniques, and radiation detectors

resulted in a number of significant measurements being made of the cross sections for total

photon absorption, quasi-elastic photon scattering, and specific reaction yields. These

experiments established the systematics of the photonuclear interaction and showed the

dependence of the general features of the giant resonance on nuclear structure, e.g., the

ground-state deformation and the tensor polarizability of the nucleus. Further developments in accelerator and detector technologies in the decade of the sixties provided data

that confirmed the general features indicated by the earlier bremsstrahlung data and also

permitted measurements to be made in greater detail and with higher precision. To a large

extent, the improved data resulted from the development of "quasi-monoenergetic" photon

beams using the annihilation- in-flight of positrons generated by electron beams from linear

accelerators [4]. Up through the sixties the great majority of data obtained on the photonuclear interaction was "one-dimensional", i.e., a particular reaction was studied as a

A Nuclear Information Research Associate (NIRA) at the National Bureau of Standards.

^Figures in brackets indicate the literature references at the end of this publication.

1
function of excitation energy only. It had long been realized that studies of inelastic

electron scattering could lead to "two-dimensional" data Csl. These experiments could give

information not only as a function of excitation energy but also for a fixed excitation

energy, as a function of the momentum transferred to the nucleus, i.e., the wavelength of

the probe used to study the interaction could be made arbitrarily shorter than that associated with the energy transfer. Only during the last few years have developments in accelerator facilities, detection systems, and data analysis techniques permitted reliable data

of this type to be obtained. Measurements in this area should have a considerable impact

on the field of photonuclear reactions during the decade of the seventies.

The objective of this report is twofold. First, to present a brief stramary of what is

known about the gross features of the giant resonance in such a form that the data may be

useful both for individuals interested in the basic interaction as well as those interested

in obtaining the yield of a particular reaction under specified conditions; second, to

present a cumulative, comprehensive, annotated index and bibliography covering the data on photonuclear reactioas that have been published in the world's scientific and technical

literature in the period from 1955 through 1972. The report is organized as follows:

Section 2 discusses the gross features of the giant resonance and presents data in both

graphical as well as tabular form; Section 3 gives a description of the annotated index and

bibliography; Section A consists of the data index; Section 5, the bibliography; and

Section 6 lists the abbreviations used in the various tables and their definitions. the

final section, 7, is a reference list to citations made in the textual parts of this report

which are not included in the bibliography given in Section 5.

Figure 1. Giant resonance summary. The energy scale for each nucleus

has been normalized so that the giant resonance is at one. The width of the giant resonance on this scale is indicated

by the shaded regions. Separation energies are indicated by

circles, open for protons and closed for neutrons. See text

for complete description.

2
2. Gross Features of the Giant Resonance

2.1. General Description

The giant resonance of the photonuclear interaction is an empirical phenomenon exhibited by all nuclei. It is the large peak seen in the plot of the nuclear photon absorption

cross section as a function of photon energy. The area under this peak is always found to

be approximately that given by the dipole sum- rule result CgI:

J, (J(E)dE =

^ ^ = 0.06 NZ/A (MeV-bams) (1)

o Mc A

Figure 1 gives a rough "bird's-eye" picture of the giant resonance for nuclei ranging

from oxygen to lead. In this figure the energy scale for each nucleus has been normalized

so that the mean energy for photon absorption below 30 MeV has been set equal to one. The

actual mean energies for the specific nuclei are given in MeV by the figures in the center

of the shaded region indicated for each nucleus. These shaded regions indicate the extent

of the giant resonance, i.e., they indicate roughly the region between the half maximum

points on the absorption cross section curve. Note that in this figure the overall widths

of the giant resonance vary by about a factor of two. The narrowest resonances are for

those nuclei with closed shells while the broadest are for those (e.g., ^^^Ho) having large

permanent deformations. The overall extent of the giant resonance for the deformed nuclei

is determined to a large extent by the splitting of the giant resonance resulting from the

deformation. In this respect, the large width indicated for ''^^As is interesting in that it can probably be associated with a dynamic deformation of this nucleus resulting from the

zero-point vibrations of the nuclear surface.

The black dots and open circles shown in Figure 1 represent, respectively, the neutron

and proton separation energies. The lines designated by the letter "B" in each diagram

indicate the top of the Coulomb barrier for protons. In the light nuclei this barrier com- pensates for the difference in the separation energy for neutrons and protons. The total

iy,p) yield might then be expected to equal the total (y,n) yield were it not for the fact

that the high neutron separation energy results in there being a paucity of states available for neutron decay. In the heavy nuclei the top of the Coulomb barrier comes well

above the giant resonance and the decay is predominantly by neutron emission. The two

black dots indicate the threshold for the (y,2n) reaction. In the light nuclei this

threshold is well above the giant resonance while in the heavier ones it comes at about its

center. For these nuclei the (')',2n) reaction can contribute appreciably to the total

absorption cross section.

The numbers given across the top of Figure 1 give the energies, in units of the giant resonance energy, at which the ratio of the nuclear radius to the photon wavelength divided

by 2n is equal to one. This is the energy at which retardation effects might be expected

to set in and where the usual multipole expansion of the electromagnetic operator might be

expected to lead to difficulties.

Good resolution experiments have shown that for the light nuclei, atomic number A<40,

the giant resonance has considerable fine structure. While some such structure has been

sho\m to exist for the heavier nuclei, this is in general not a significant feature of the

shape of the absorption curve for nuclei with A>100. In any event, all such structure is

going to be smoothed over in this discussion. The only structure that will be Indicated

is that associated with nuclei having permanently deformed nuclear ground states. The

giant resonance for these nuclei is very well described by the superposition of two Lorentz

shape resoiiance curves in which the area under the higher energy peak is twice that under

the lower energy peak, i.e.,

6 {T E) (J (r E)

C,(E) = ±^ + L_b ^2)

(E^-E + (r E)^ (E^-E^)^ + (r E)2

3
and (SyyV-^ = 2 c^a^a* Except for the normalizations used to present the data in some of the

figures, little or no attempt will be made to correlate any of the data presented with

theory. This aspect of the field is covered in a number of recent reviews L?].

2.2. Experimental Data

The gross features of the giant resonance are summarized in Table 1 and Figures 2 and

3. Table 1 presents data for all nuclei for which measurements have been made. No attempt

has been made to indicate the fine structure often observed in the giant resonance for the

lighter nuclei. The data presented for a given nucleus and reaction are the energy at

which the giant resonance peaks, Ej the magnitude of the cross section at E, SIG; and the

full width of the cross section curve at half maximum, DEL.

Where authors have fit a cross section curve by either one or the superposition of

two Lorentz lines, the resulting parameters are listed and a letter L is entered under

REMARKS. Also listed are the integrated cross section up to some upper energy limit

(Jo (Ea ) , SIG-0, and the bremss trahlung weighted cross section cJ.^ (En ),SIG-1. These quantities are defined by

E

CJ (E ) = (J(E)dE

o m y

(3)

When these integrals have been evaluated from the Lorentz line parameters used to fit the cross section, Ej, is given as L. For the lighter nuclei these quantities are given where

possible both for the total cross section as well as for one or more of the partial reaction cross sections which make a major contribution to the total. For the heavier nuclei

the data pertain almost exclusively to neutron-producing cross sections « The various

reactions listed are indicated by the symbols given in the second column of the table,

(INT). These symbols are defined as follows:

TOT the total nuclear absorption cross section

for photons

N the (y,n) cross section

XN the neutron yield cross section cJ(xn)

cJ(xn) = (J(y,n) + (J(y,np) + 2(J(7,2n) + T7CJ(y,f)

SN the sum of the neutron-producing cross sections

(J(SN); (J(SN) = (J(y,n) + cJ(y,np) + (J((J,2n) + . . .

P the (y,p) cross section

T the (y, t) cross section (t = triton)

D the (y,d) cross section (d = deuteron)

F the photofission cross section

N+P cf(y,n) + cJ(y,p)

SNF CJ(SN) + cJ(y,f)

Where a number of measurements of a particular cross section are available in the

literature, the parameters given in Table 1 are taken from a single measurement which has

been selected as being the most representative of the data for a particular nucleus. This

measurement is identified by the bibliographic reference given for each entry in the table.

The notes referred to in the final column (REMARKS) are listed at the end of the table.

These are used to expand on the information given in the table, to indicate the need for

4
possible renormalizatlons of the values quoted, and to give the source of data listed where

no bibliographic reference number Is available.

The general trends with mass number A of the integrated absorption cross section and

the bremss trahlung weighted cross section are indicated in Figures 2 and 3, respectively.

On these figures the data for nuclei having mass numbers less than 70 all come from direct

measurements of the total photon absorption cross section. For the lightest nuclei two

values are given, one where the upper limit to the integration is 140 MeV (i.e., approximately the meson production threshold) and a second value where the limit is 30 MeV for 0^ and 35 MeV for C-i . The data for the heavier nuclei are all taken from measurements of the

neutron-producting cross sectioii, cf(SN), that have been fit with Lorentz shape resonance

curves. In general, the measurements have extended up to about 25 MeV. The values listed

all result from carrying out the appropriate analytical integrations (0 < E < °=) over the resonance curves. None of the data presented in these figures were derived from (J(SN) curves that had been obtained by making statistical model corrections to measurements of

cJ(XN) . The integrated cross section values have been normalized in terms of the value

given by the classical dipole sum rule (see Equation (1)). The bremss trahlung weighted

cross section values have been normalized by dividing by A*/ the mass number dependence

given by most elementary models of the nuclear photoeffec t [85.

80 120 160

MASS NUMBER,

A

Figure 2. Integrated absorption cross sections normalized to the classical dipole sum rule value. All points are from data selected

from those listed in Table 1. Solid dots were obtained from

integrating Lorentz line fits to cf(SN) data. Open circles and

squares are from total absorption cross section measurements.

For open circles integration is taken to 30 MeV, for the squares

it goes to 140 MeV.

5
Except for some fluctuations associated with the lightest nuclei, the normalized

values of both do and C-i are relatively independent of the mass number. Note that for the

light nuclei (A < 40), where data are available, that there is a rather large contribution

to (Jo (140) coming from energies above 30 MeV. The contribution of the cross section at

these ranges to c!'-i(140), however, is relatively small. The total cross section for these

nuclei indicates that (Jo (140) is about twice the classical sum-rule result. Unfortunately,

only very sketchy data are available to give an indication of what this limit might be for

the heavier nuclei. The data which do exist are not inconsistent with Co(140) being twice

the dipole suni-rule value for these nuclei also (see Equation (1)).

80 120 160

MASS NUMBER, A

Figure 3. Normalized bremss trahlung weighted cross sections. Solid dots

obtained from integrating Lorentz line fits to tf(SN) data.

Open circles and squares from total absorption cross section

measurements. For open circles integration is to 35 MeV,

while for squares it goes to 140 MeV.

6
Table 1, Gross Features of tvie Giant Resomance

J. U ^ L. Q U O I N T S 1 G DEL S I G-0 S 1 G1

REF REMARKS NUCLEUS I NT E S I G DEL S I G-C SIG-1 REF REMARKS

Z A MEV MB MEV MEV-MB ( MEV

)

MB { M E V

)

2 A MEV MB MEV niEV-HB ( MEV

)

M b ( K E V )

IH 2 TOT 4.48 2.5 18. 1 40 ( 140

)

3.7( 140) «1,»2

29(30) 3.6(30) 24CR XN 18.5 97 1628(80) 62(80) 54C02

IH 3 D 12. .72 12. 12(33) .78(33) 58PF1 24CR A = 5U, 52, 53 , 54 NO DATA

25MN55 TOT 17.5 100 7 . 5 816(29) 69001

2HE3 D 12.5 .75 18. 15(40) 1.1(40) 65ST 1 2HE 3 N 15. .90 13. 13(30) . 77 ( 30

)

70BE6 26FE TOT 17.5 90 9.0 735(27) 59D02

2HE4 P 26.5 1 . 7 14 . 40(170) 1.1(170) 58G05 »2 25FE54 N 19.2 38 6.9 290 ( 31

)

57CA2

2HE* N 25.5 1.7 14. 42(170) 1 . 1 ( 170 ) 58G06 '2 25FE A = 55, 57, 58 NO UATA

3LI6 T 18.5 .59 1 1 . 5.6(35) .22(35) 71VE1 58SH2 27C059 TOT 18.6 92 9.3 1030 ( 35

)

50(35) 66WY1

3L 16 SN 12 . 1.7 15. 27(32) 1.9(32) 658E1 »3

3L I 7 T 17. 0,2 20

.

4.9(35) 570E1 55MI1

3 L I 7 XN 16 + 3.0 13 + 50(29) 55HA1 2 8N I TOT 16.7 89 7.5 9 20(35) 44(35) 65WY1

2BN I 58 N + P 19.5 125 4.8 840(32) 59CA4

2 SN 160 N+ P 19.0 90 5.5 940 ( 3 0) 59G02 70IS4

4BE 9 TOT 24. 5.2 2 8. 2 2 8 { 140) 7 . 4 ( 140) 7 1 AH 1 * 4 2 6N I *" 6 1, 52

,

64 NO DATA 4BE9 75(30) 5.1(35) 71AH1 »4 4BE9 XN 28 . 4.7 2 6. 220(70) 7.6(70) 55C04 2 9C U TOT 17.5 94 11.5 10 3 6(35) 51(35) 55WY1 29CU53 SN 16.5 53 5.0 754(26) 3 8 { L ) 54FU1 L 21.3 22 7 . 1 64FU1 L 56 10 XN 24. 6.5 10. 5 67(29) 65HA1 29CU65 SN 15.8 88 5.0 765 ( 28

)

63 ( L ) 54FU1 L 58 11 XN 25. 7.5 1 1 . 59(29) 65HA1 20.5 36 6 . 0 64FU1 L 58 11 p 2 5. 15. 10. 98(31) 69S02

302N XN 15.7 9 1 4.6 1507 ( 80

)

56 ( 80

)

57C01 54C02 30ZN54 N 17.2 48 7.0 330(23) 60R04

6C 12 TOT 23. 20. 5. 2 288 ( 140

)

7.7( 140) 71AH1 30ZN A = 66 , 67

,

68

,

7 0 NO DATA

108(30) 5.1(35) 71AH1

6C 12 SN 23. 7. 4 . 8 35(30) 56FU1 *5 3 IGA XN 16.5 115 1

8

947 ( 28

)

9 4(80) 65BA3 64C02

31GA A = 59, 71 NO DATA

7N 14 TOT 2 2.5 27

.

7. 0 195(30) 8.4(30) 59BE2 32GE XN 17.5 158 2495 ( 80

)

102(80) 64C02

7N 1

4

SN 23.2 14. 5

.

1 98 ( 30

)

70BEe 32GE70 N 17.5 158 8.6 50FE1 32GE76 N 18.9 243 7 + 1500(21) 65B01 32GE A = 72 , 73 . 74 NO DATA

80 16 TOT 23.5 30

.

5. 5 280 ( 140

)

14( ItO

)

71AH1 215(30) 10(35) 71AH1 33AS75 SN 15.0 39 3.63 910( 30) 51 ( 30] 598E1 L 80 15 SN 23. 7. 5. 5 46(30) 54BR1 S 17.5 78 7.41 59BE1 L

34SE XN 15.6 118 5.2 67C02

9F 19 TOT 24 . 18. 14 + 271(30) 59BE2 34SE82 N 16.0 190 4.5 870 ( 22

)

56S I 2 34SE A = 74, 76, 77, 78 , 80 NO DATA

1 ONE NO DATA

35BR NO DATA

1 1NA23 TOT 2 3. 15. 16. 200 ( 30

)

11(35) 6 5WY 1

1 1NA23 SN 2 3. 10. 15 + 119(27) 71AL1 35)CR NO DATA

37RB SN 16.8 192 4.1 1140(24) 67 ( 24

)

71LE1 L

1 2MG TOT 19. 24. 1 3 . 225(30) 12(35) 65WY1 37RB A = 85, 87 NO DATA 12MG24 SN 19.5 7.5 1 1 . 50( 28) 2.8(28) 71FU2

12MG2 5 SN 23. 28. 9 249 ( 29

)

12(29) 71AL1 3BSR SN 15.7 207 4.2 1420 ( 27

)

80 ( 27

)

71LE1 L

1 2MG26 SN 17.5 20. 7

,

294(28) 12(28) 7 1 F(J2 3 8 S R 8 4 NO OAT A 38SR85 XN 15.9 150 5.0 920(23) 55YE2

38SR87 XN 15.8 146 5.3 loco ( 23

)

55YE2

13AL27 TOT 21 . 40. 10. 408 ( 140

)

25 ( 140

)

71AH1 38SR88 XN 15.3 20 1 4.0 1050 ( 23

)

56YE2

384 ( 30 ) 20(35) 71AH1

1 3AL27 £M 21. 1 5 . 1 1 . 172(37) 65FU1

39Y 89 SN 16.7 225 4.1 1360( 27) 77(27) 71LE1 L

14S I TOT 20.2 52. 5. 882 ( 140

)

26 ( 140

)

71AH1 378(30] 20(35) 71AH1 40ZR90 SN 16.7 2 1 1 4.0 1260(26) 71(25) 71LE1 L 14S I 23 N 2 1

.

15. 5. 93(31) 7 0WE1 40ZR9

1

SN 16.5 184 4.23 1080(30) 66(30) 67BE2 L 40ZR92 SN 15.3 155 4.73 1 100 ( 28

)

65(28) 67BE2 L 40ZR94 SN 15.2 151 5.20 1010(30) 59( 31 ) 57BE2 L 15P 31 XN 22 . 1 3 . 1 1 • 5 127(28) 63801 »5 40ZR95 NO DATA

1 5P 31 XP 21. 43

.

9 , 350 ( 32 ) 64 I S

1

4 1N893 SN 16.5 202 4.70 1330(24) 79(24) 7 1 L F 1 L 16S TOT 20

.

50. 7 . 400 ( 30

)

22(35) 55WY1

16S 32 XN 21 . 16. 1 1 . 137(32) 70AN3 42M092 XN 16.4 170 5.0 1290( 30

)

701S1 42M098 XN 16.8 280 5 .0 2000 ( 30

)

701S1 17CL35 N 20. 14. 6. 5 93(27) 62KU1 42M0100 N+P 15.0 180 5 .

6

1110(20) 64GE1

42M0 A = 94 » 95 , 96

,

9 7 NO DATA

ieAR40 TOT 19. 42. 10. 4 5 0(32) 6 5EH1 18AR40 N 19. 37. 5, 200 ( 32

)

65EH1 44RU NO DATA

19IC 39 N 20

.

16 . 7 . 102(30) 7 1 W E 1 * 6

4 5 RH 1 0 3 SN 14.3 150 3.0 2 1 3 0 ( L ) 1 2 3 { L ) 62601 7L

20CA TOT 20. 92 . 4 . 8 1 140 ( 140

)

42(140) 71AH1 17.5 240 3.8 52B01 7L

650 ( 30

)

3 8 ( 3 5 ) 71Ahl 20CA SN 20. 15. 3

,

g 7 3 ( 2 5 ) 66M 1

2

4 6PD 1 0 8 SN 15.7 210 5.0 1725(25) 10 4(25) 69DE5

NO DATA PD 102i, 104, 105, 106, 110

2 1 SC45 NO DATA 47AG TOT 15.8 218 7.5 2 568(35) 130(35) 55WY1 47AG107 SN 15.0 62 4.81 1350(30) 79 ( 30

)

59BE1 L 15.5 99 7.01 59BE1 L 22T 1 XN 17.0 60 7 + 6 7C0

1

47AG1C9 XN 15.9 175 5.5 12 10(29) 69IS2

22T I 46 SN 20.5 31 8 . 5 259( 31

)

52SH5

22T I A = 47 , 48 , 49, 50 NO DATA 48CD XN 15.5 253 5.1 1760 ( 27

)

111(27) 56GA1 48CD A = 106- 108, 110, 111 , 112, 113 , 114, 116 NO DATA

23V 51 SN 17.5 41 3.60 580 ( 28 ) 33(L ) 62FU1 L 20.3 46 6.5 52FU1 L 49IN SN 15.6 265 5.24 1901 ( 31

)

113(31) 69FU1 L 49 INU3 NO DATA 49IN115 SN 14.0 116 3.0 22 10 ( L

)

1 19 ( L) 52601 -»7L 15.3 240 3.8 62B01 »7L

7
NUCLEUS INT E Z A MEV

SIG

MB DEL SIG-0 SIG-1 REF REMARKS

MEV MEV-MB(MEV) MBIMEVI NUCLEUS INT E SIS DEL SIG-0 SIG-1 REF REMARKS

Z A MEV Md MEV MEV-MU ( MtV I Mb (MEV)

50SN XN 16.0 300 5.0 1540 ( 40

1

-134 ( L ) 58FU1 67H0165 SN 12.1 250 2.70 2790(25) 194 ( 25

)

68BE5 L 50SN112 N 16.0 340 5.0 1820 121) 1 52 ( L ) 61KU1 15.6 285 4.80 58BE5 L 5DSN115 SN 15.7 266 4.19 1 667 ( 29

)

94(29) 69FU1 L 50SN1 17 5N 15.7 254 5.02 1939( 31 ) 114(31) 69FU1 L 50SN1 16 SN 15.6 255 4.76 1898 ( 30

)

110(30) 59FU1 L 68ER SN 12.1 225 2.90 270u( 25) 186(25) 69BE6 L 50SN1 19 SN 15.5 253 4.81 2078131

)

119131) 69FU1 L 15.5 260 5 .0 69BE6 L 50SN120 SN 15.4 280 4.88 2090(30) 124( 30

)

69FU1 L 68ER A = 166.167.1 168 11 170 NO DATA

50SN12'i SN 15.2 283 4.81 2077( 31) 123(31) 69FU1 L 50SN A = 114, 115. 122 NO DATA 69TM159 SN 13.8 235 6.3 1480 ( 22

)

148(L) 58KA1

51SB NO DATA 70YB NO DATA

52TE NO DATA 71LU175 SN 12.4 230 2.70 2650(25) 182125) 69BE6

531 127 SN 14.5 255 3.78 2020 ( 25

)

129(25) 69BE6 L 16.8 130 3.87 69BE6 L 72HA NO DATA

54XE NO DATA 73TA181 SN 12.4 270 2.57 2900 ( 25 ) 205 ( 25

)

68BE5 L 15.3 330 4.47 68BE5 L

7 3T A 18 1 p 60(40) 60BA5

* 5.05 ^ (J U U I 3 U ) 1 24 ( 30

)

69BE1 L

74W 186 SN 12.6 211 2.29 3975 129) 222 1 L

)

69eE8 L 56BA SN 15.3 356 4.70 2600 1 L

)

1 57 1 L ) 71BE4 L 14.9 334 5.18 69BE8 L 56BA138 SN 15.3 327 4.51 2040 127) 131127) 70BE8 74W A = 182 , 183. 184 NO DATA

56BA A = 134.135 . 136 ,

i 137 NO DATA

75RE NO DATA

5 7LA1 39 SN 15.2 340 4.45 2 320128) 146 ( 28

)

71bE458Bc5 L

760S NO DATA

58CE SN "15.0 360 4.35 21301 25

)

140 ( 25

)

71BE469BE6 L 58CE A = 140. 142 NO DATA

77IR NO DATA

59PR141 SN 15.2 320 4.49 2100( 30) 135(L) 566R1 L 78PT NO DATA

60ND142 SN 14.9 359 4.43 2500( L

)

153( L

)

71CA1 L 50ND143 SN 15.0 360 4.5 2540 ( L

)

1551L) 71CA1 L 79AU197 SN 13.7 540 4.75 3480 1 25

)

238(25) 70VE1 60ND144 SN 15.1 317 5.3 2500(L) 15e(L) 71CA1 L 60ND145 SN 15.0 297 6.5 300O ( L

)

178(L) 71CA1 L 60ND146 SN 14.8 308 5.U 2900 ( L

)

174( L ) 71CA1 L 80HG NO DATA 60N0143 SN 14.7 263 7.2 3000 ( L

)

176 ( L

)

71CA1 L 60ND15O SN 12.3 174 3.3 2700(L) 171 IL ) 71CA1 L 16.0 223 5.2 71CA1 L 81TL TOT 14.0 548 4.6 3770 1 27

)

266 ( 27

)

55GA1 81TL203 SN 14.2 490 3.7 2610 1 20

)

185 69AN10

81TL205 SN 14.1 490 3.7 2780 1 2u

]

187(L) 59AN10

6 2SM SN 12.8 155 4.25 2480 ( 25

)

157(25) 59BE5 L 81TL205 P 20. . 1 57EL2

15.5 260 4.6 69BE6 L YIELD OF A/P/N =1/100/10000

62SM14e SN 14.1 335 4 . u 2080(22) 137 ( L

]

71VA2 »7L 62SM150 SN 13.6 360 5.50 2213(23) 203 ( L

)

59VA3 S-7L 62SK152 SN 11.5 40 0 2.4 3079( 23) 254(L) 59VA3 *7L 82P6205 SN 13.7 525 3.76 2780 1 281 208 ( L

)

54HA2 »5L

14.7 420 3.4 69VA3 7L 82PB207 SN 13.6 485 3. 87 2650128) 199(L) 54HA2 »5L 52SM154 SN 11.0 204 3.0 2478(23) 2021L) 59VA3 *7L 82PB208 SN 13.4 640 4.05 3480 ( 25

)

251125) 70VE1 L 15.3 320 4.0 59VA3 «7L 82PB208 P 27(33) 71DA1 62SM A=:144.147..149 NO DATA

83BI209 SN 13.5 520 3.83 2930 ( 28

)

213 1 L

)

64HA2 »5 L 63EU151 SN 14.0 285 4.5 2020122) 131 1 L

)

71VA2 »7L 53EU153 SN 12.3 155 2.75 2310 129) 1551 L

)

59bE8 L 15.8 222 5.83 69BEe L 88RA NO DATA

54GD152 SN 12.0 147 3.0 1990 1 22

)

135 ( L

)

71VA2 »7L 90TH232 SNF 11.1 268 3.37 2500 115) 198 115) *8L

15. 259 3.2 71VA2 7L 14.1 349 4.52 »BL 64GD154 SN 1 1.9 161 2.4 200U 122) 133 ( L

)

7 1VA2 »7L 90TH A= 228. 230 NO DATA

15.0 250 3.5 71VA2 7L

64GD155 SN 11.9 180 2.5 2 110(22) 142 1 L

)

71VA2 »7L

15.2 243 3.5 71VA2 *7L 91PA231 NO DATA 64GD158 SN 11.7 165 2.5 2160(22) 146 ( L

)

71VA2 »7L 14.9 249 3.8 71VA2 »7L 54GD150 SN 12.2 57KA1 58KA2 215 2.77 2560( 29

)

181(L) 59BE8 L 92U 233 XN 14.0 1570 6.0 11200122)

15.0 233 5.28 69BE8 L 92U 235 SNF 10.9 354 2.45 3560 1 19

)

3031L) 64Bu3 L 64GD A = 155.157 NO DATA 14.1 446 4.00 54B03 L 92U 238 SNF 11.0 301 2.90 2980 118) 235118) »8L 14.0 369 4.53 «eL 65TB159 SN 12.1 205 3.25 2500 1 27

)

1721 27) 68BE6 L 92U A = 234. 236 NO DATA

15.0 240 4.87 58BE6 L 93NP237 SNF 11.1 251 3.15 2500 ( 16 • 8L

)

2041 15) 14.2 380 5.12 »8L 66DY NO DATA

94PU239 XN 1396 1580 5.3 11500(22) 57KA1 58KA2

8
Notes for Table 1

*1 E. G. Fuller and Evans Hayward, "The Giant Resonance of the Nuclear Photoeffect"

in Nuclear Reactions II, Eds. P. M. Endt and P. B. Smith (North-Holland Publishing

Co., Amsterdam, 1962)? F. Partovi, Ann. Phys. 27, 79 (1964).

*2 See also - J. S. O'Connell, "Electromagnetic Interactions of the Few-Nucleon Systems,"

to be published in the Proceedings of the International Conference on Electromagnetic

Interactions of Nuclei at Low and Medium Energies , Moscow, December 1972.

*3 Cross section given^is total neutron yield. This includes all reaction cross sections

except the ^Li(y,t) He. Lowest threshold for 2-neutron emissions is 24o2 MeV. Other

data indicate cross section magnitudes may be 1.2 X those quoted. (66Ge3)

*4 Measurement does not extend below 16 MeV. The Cg and cJ-i values quoted have been

corrected to include (5(y,n) in energy region from 1.6-16 MeV.

*5 Cross sections may be low by 20-307o. See 66Ge2, 70Vel, and other measurements of

n-production cross sections.

*6 Cross section for production of .95 isomer. This represents about 0.6 of total (7,n) cross section (see &2Go3, 65Go3).

*7 Statistical model used to correct for neutron multiplicity.

*8 R. Bergere, H. Beil, P. Carlos, A. Veyssiere, A. Leprete, Nuclear Structure Studies

Using Electron Scattering and Photoreaction , Eds. K. Shoda and H. Vi, p. 273

(Tohoku University, Sendai, Japan, 1972).

9
2.3. Estimating Yield

Figures 4 and 5, when used in conjunction with the data listed in Table 1 can be used

to estimate bremsstrahlung-induced photonuclear reaction yields. The estimate is based on

the assumption that the cross sections can be described by Lorentz resonance curves. This

is a very good approximation for the heavier nuclei (A > 100). It is not a good approximation for light nuclei, particularly those for A ^ 16. For these nuclei, (A < 40) if

yields are required with an accuracy better than a factor of three, detailed calculations

should be carried out making use of the best available cross-section data. For the heavier

nuclei, yields can usually be estimated to within - 307„ by making use of the Lorentz-line

approximation.

It can be readily shown that for a Lorentz-shaped resonance curve

(j.(E r.)

(J (L) = / dE = ^ (J.r

f

(E r ) (L) -i i ° J (E=-E.^)= + (E T.f 2 1

1

•'o ^ 1 1 (4)

CO /N f '^i^^ dE 7t ^i^i 1 fi ^ 1 . -1. . (1 -2(2a)-^)

I

(E^-E.= )= + (E r.)= ^ ^ h a -(2a)-=)^ L (1 -(2a)"^)^

where a = Ei/Fi. Note that only for a » 1 does cIi(L) nCS^Ti/(2E^) . For values of a typical of most giant resonance curves O'-i (L) is approximately 0.8 to 0.9 times the sharp resonance limit. The quantities plotted in Figures 4 and 5 are (Jg (x)/cJg (L) and

(Xi (x)/(J.i (L) as a function of x = E/Ej for various values of a.

If N(E,E^ ) = l(E,E5,)/E represents the bremsstrahlung spectrum (number of photons per

MeV), cf(E) the cross section for a reaction, and n the effective number of nuclei per cm^

in the bremsstrahlung beam, then, Y(Eu), the reaction yield per MeV in the bremsstrahlung

beam, is given by

"m I(E,E ) cr(E) / /"m

Y(Bj=n( ^ dE/ / I(E,EjdE. (5)

For estimating yields the thin target bremsstrahlung spectrum can be approximated by as- suming that I(E,E„ ) is independent of E so that

E

m . .

m / m

^o

For any particular cross section, values of 6-i{'E^) can be obtained by making use of Fig. 5 and the data listed in Table 1. With the approximations indicated here, thick target

bremsstrahlung spectra can be assumed to be an appropriately weighted superposition of thin

target spectra. Note that the "cross section per equivalent quantum" (Jq(Ej|) is equal to

C-i when I(E,Ej|) is assumed to be constant, i.e..

E )dE o m

E Y(E ) E I(E,E ) cr(E) a (E) = -i^^^ = 2 / E dE ^ a ,(E ). (7)

q m' n _E__ J

E

^ m

^

10
11
3. Description of the Photonuclear Data Index and Bibliography

3.1. Introduction

This Photonuclear Data Index is the fourth one published by the Photonuclear Data

Center. It is a cumulative index and as such supersedes all previous publications of the

Center [9]. It is an index to all the experimental data published in the field of photonuclear reactions and entered into the Center's files in the period from January 1, 1955

through January 15, 1973. All of these data are published in regular journals or as rather

complete reports as contributions to various international conferences. Nine journals are searched regularly for data. These are listed below along with an indication of the last

issue searched for data included in this index. These are the issues that had been re- ceived in the National Bureau of Standards Library by January 15, 1973. Nuclear Science

Abstracts is used to find papers published in those journals not regularly searched.

Journal Last Issue

Physical Review, The Vol. 6, #6

Physical Review Letters Vol, 30, #2

Nuclear Physics Vol. A198

Physics Letters Vol. 42B, #3

Soviet J. of Nuclear Physics Vol. 15, #4

11 Nuovo Cimento Vol. 12B, #1

11 Nuovo Cimento Letters Vol. 5, #2

J. Physical Society Japan Vol. 33, #5

Zeitschrift fur Physik Vol. 255

Nuclear Science Abstracts Vol. 26, #23

3.2. Scope of the Data Index

The function of this data index is to furnish a means of readily locating experimental

data in the field of photonuclear reactions. This index differs from a bibliography in

that it supplies quantitative information about the content of a paper. Each entry in the

index corresponds to the measurement of a specific photonuclear reaction for a specific

nuclide or group of nuclides. An attempt is made to give as complete a description of each

measurement as is possible in a single line. The type of measurement is indicated as well

as the range of excitation energies covered, the type of detector used and its energy

response, and the type of angular distribution data obtained. The object has been to give

a description of each measurement that is complete enough to permit an individual looking

for specific types of data in the field to locate the pertinent references without having

to go through a large number of irrelevant papers as might be the case if only the title

of the paper or the reaction studied were listed for each entry.

For the purposes of this index, the general criterion as to what constitutes a meas- urement of photonuclear data is that the measurement must give information on the electromagnetic matrix element between the ground state and excited states of some nucleus. The

most common type of reactions are: (e,e'), (y,y), (y,n), (y,p), and (p,yo)« Two reactions

which fit the matrix element criterion, but which were not included in the compilation

because of their rather special nature are heavy particle Coulomb excitation and the thermal neutron capture reaction (n,yo). While the energy region of particular interest

extends from 0 to 150 MeV, some papers are indexed which report measurements in the region

from 150 MeV to 1 GeV. Most of the experiments listed are concerned with the excitation

energy range 8 to 30 MeV, the region of the photonuclear giant resonance.

3.3. Description of the Index

The data index for each element begins with the isotopic abundances for that element

and a list of separation energies for each isotope. The abundances were taken from a com- pilation by Gladys Fuller TlOJ. This reference should be consulted for remarks concerning

the accuracy of these values and possible variations with the source of the sample. The

separation energies were taken from the tabulation of Wapstra and Gove [ill which were based on their 1971 Atomic Mass Evaluation. The values given in Ref. Cll] have been arbitrarily rounded off to the nearest 0.1 MeV except for those cases where the uncertainties

12
quoted are of the order of 1 MeV. In these cases, thresholds are given to the nearest MeV.

In the data index which follows, eight columns are used to describe a reaction re- ported in a specific paper. Where for clarification purposes a brief remark has been included in the index entry for a specific reaction, this remark is listed on the line

immediately below the line giving the main index entry. The purpose of this remark is to give additional information that will make the index entry more useful. For example,

pertinent energies are more exactly defined, additional information is given on polarization or alignment experiments, residual nuclei are identified, etc. The additional information is selected in a fairly unsystematic way and is limited by the available space. The

entries should not be regarded as exhaustive or consistent. The headings of the eight

principal columns used for an index entry are: REF (Bibliographic Reference Number),

NUCLIDE, REACTION, RES (Result), EXCIT (Excitation Energy), SOURCE, DETECTOR, and NUM

(Acquisition Number). These headings are described more completely in the following

section.

Under a given element, the index entries are grouped so that those listed "irst are for measurements made on the element, i.e., on samples with naturally occurring isotopic

abundances. Following this, measurements pertaining to the various isotopes of an element

are listed together. The entries for a given element or isotope are ordered by reaction

according to a priority listing of, first, the incoming particle, and second, the outgoing

particle. All entries for a given reaction are listed chronologically.

3.4. Description of Column Headings

An alphabetical list of the symbols used under the various columns of the data index

is given in Section 6 of this report. The purpose of this section is to describe the

meanings of the various column headings.

Co lumn 1 REF Bibliographic Reference Number. This number is made

up of the year and the first two letters of the first

author's name, plus an additional serial number.

Column_2 NUCLIDE The atomic number (Z), chemical symbol, and mass number (A) of the excited nucleus (not necessarily

the target nucleus) is given. The mass number is

listed only if the isotopic assignment is unambiguous.

In general, it was assumed that the mass number was unambiguous if in the target the abundance of a single

isotope was > 977..

Column _3 REACTION The notation used is the usual one. Where necessary,

a remark is often used to more fully define some of

the more esoteric reactions. The notation E,E/P means

the inelastically scattered electron and proton were

detected in coincidence in a reaction of the type:

A + e

"* (A - 1) + e' + p, while E,P means that only

the proton was detected. Where the measurement involved the polarization or alignment of either the

incoming beam, the target nucleus, or the outgoing

particle, a $ is listed to the left of the column.

Column 4 RES Result, i.e., the type of information given in the

paper.

Column 5 EXCIT Excitation Energy Range. The excitation energy range

of the nucleus involved in the ganma-ray transition

is given in MeV. For reactions initiated by gamma

rays, the excitation energy is taken as the gamma-ray

energy; for reactions initiated by particles, the

binding energy and kinematic corrections are made.

The abbreviation THR stands for threshold. Where the

13
Column 5 (continued)

EXCIT scale 1-999 MeV is inappropriate for a measurement,

999 is entered and the actual energy given under REMARKS.

Column 6 SOURCE Source Type and Energy Range. The source of incident

particles is characterized by the letter C or D indicating that the source was continuous or discrete in

energy. The source energy is indicated under MIN-MAX.

The usual source of photons is bremsstrahlung which

would be marked C. The range of endpoint energies is

given.

Column 7 DETECTOR Detector Type, Energy, and Angular Range. The symbols

used to indicate the detector used in measurement are defined in the list given in Section 6. The letter

D or I under TYPE means that the reaction product was detected differentially or integrally in energy. For

example, a scintillator (SCI) is usually used differentially (D) while a BFs detector (BF3) always integrates

over neutron energy (I). The range of detected particle

angular distribution is shown under ANG. A single

number in the column means the measurement was made at

this angle (given in degrees) only. DST means that the

measurement was made at two or more angles and 4PI

indicates that the detector used essentially integrated over all outgoing particle directions.

Column 8 NUM Acquisition Number. This is the number used to identify

cross section data that are available in digital form

from the Photonuclear Data Center's library. When an acquisition number is followed by a +, digitized data

from the paper in question are available for quantities

which are normally not indexed, e.g., a (y(SN) cross section curve.

14
^. Photonuclear Data Index

1955-1972

15
PHOTONUCLEAR DATA INDEX

HYDROGEN 2=1 NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF 2 A I N OUT TYPE ANG

ABUND. SEPARAT ION ENERGIES (MEV)

G G» , T G»HE3 G,A G»2N G,NP Gt2P 70 I T 1 1 H 2 G P I — RLX 6 0 0- 999 C60'^-999 SPK-I API 99.99 » « * 999=1700 MEV

. 5(-2 ) 2.2 2. * * 2.2 * 70SC2 1 H 2 (3 P I - ABX 600- 999 C600-999 MAG-0 DST

3 * 6 .3 8. » * 8.5 8.5 * 999=1.2 GEV. PI DET

P ABX 200 999 C200-999 MAG-0 180 999 = 1.2 GEV

NUCL IDE REACT ION RES EXC I T 7 2F U2 1

H

2 P I — NOX 260 — 800 C999 MAG-D DST

R EF Z . N OUT REL PI+.999=1.3 GEV

70 I T 1 IH 2 P 1 + RLX 60 0 — 999

7 2 T I ^ 1

H

E / SPC 3 5 0 999=1700 MEV 999=1.18 GEV 7 1 F U 3 1

H

2 ^ P I + ABX 2 0 0 — 999 LiUU Vyv NAb— U loU

60 W Y 1 1 H MU- T ABX C 90 NAI -D 4P

I

QQO — 1 7 r, F\/

5 50X

1

1 H 1 G ABX 20- 98 C 98 TEL-D DST 72 1

H

2 G P RLX * 8 00 rQQo ^777 TFl— ItL DL^UOI nm

580X

1

IH 1 6 G ABX L o f 1 t L — U Uo 1 999= 1.1 GEV 60G01 t- / D 1 t L- U Ub 1 66GR1 IH 2 N G SPC 2 D 1 SCD-D

61BA3 1 H 1 G G ABX 24 7 L <: O U 1 t L — U U b 1 BINDING ENERGY

63ST1

J ABX CqOCi TFl -n Qn 67TU1 IH 2 N ABX g D 14 TEL-D 0 70 I T

1

1 H P 1 + R L Y v-OU'-' 7 y 7 Oris— i I 7 1 BA3 1

H

2 N G DST 239- 378 D473-750 SPK-I DST 999=1700 MEV D AND C COINC

U 1

H

1 G P I + NOX 210- 27 0 njlO— ?7n TFl — n n^T 7 1 SC 1 1

H

2 N G NOX 3 00- 700 D300-720 SPK-D DST

lIMt — KtVtKoAL Itbl 72BA5 1

H

]^ P I 0 RLX 400 - 800 i^OQQ TCI _ Pi n C T BX D 1 56 MAG-D DST yyy- 1.1 uLv QUASI-FREE N

5 9 F R 1 2 SPC 9 5 6 6HU2 1

H

3 E E / FM F 0- 160 D250-370 MAG-D DST

1

H

E E / P 0 1

6

D550 MAG-D DST

6 1 K E 3 RLX 2 0 D204-300 MAG-D 143 6^602 1 H 3 N ABX y_ 9 nU 7—1 RF'^— DrJ I

i ADI Hr \ 6 1 PE2 IH ABX 6 5 BO 2 1

H

3 G N

c 6

— 1 1 0 6- 11 BF3-I DST 62BA1 1

H

2 ABX 0- 1 0 66K02 IH G ^ SPC THR- 33 C 33 TEL-D 90 uA o 1 A K b t 1 68PF 1 1 H 3 G P ABX 11- 33 C 33 TEL-D 90

6 2 P E 1 ABX 0 — 2 0 U H t 1^*1 M O U i O w 66K02 IH 3 G D ASX THR- 33 C 33 TEL-D 90 SOL 10 TARGET 68PF1 IH 3 6 .0 ABX 18- 31 C 33 TEL-D 90

6 3B A 1 1

H

2 SPC 0

— 1 4 0 42 MAG-D 18 0 6 1 C E 2 IH 3 N G ABX 16 0 14 TEL-D API 64YE2 1 H 2 E / 0- 40 riic,."! UIDU MA/" MAu r\i'ai; U 15_) 66G01 IH 2 E E/ ABX 0- 6 6* I M

1

1

H

N (3 ABY D 0- ACT-I 4P1 66GR2 IH 2 E / Q_ 60 D219— 447 MAG-D DST NO H4 FOUND

1

H

2 E / PMF Q- 7 0 D146-473 MAG-D DST 6 5 A J

1

1

H

N G ABX 1 1 D 14 SCO-D 0

6 7RA1 1

H

2 E / ABX Q- g

r>'^c.r\ — '3~7r\ MA/" r\ iq/> UPPER LIMIT ABX

68K. A2 IH 2 E E/ ABX 2- D "ift— on Mar, — n

T I O ABX 726A2 1 M A B X n~ Q 70-280 MAG-0 180

6 5 30

1

1

H

E E / P ABX 0~ 100 J> _J U l*IM\J L/ L/O 1 6 5 603 IH E /P ABX 5 0 — 100 HELIUM Z = 2 DK TW11"! /*riIM/" (^U 1 578A1 H AB Y C120-260 THR- I DST

DFi KtL VITLUo* nQ» n//" U/t_ A ABUND. ( 1

1

SEPARATION ENERGIES (MEV) 58BA 1 N ABX THR 2 3 5 ^-i/U*^Dlj inK — 1 UjI G • N G. P C , T G.HE3 G.A G.2N G.NP

60GE 3 IH 2 G NOX L 1 HK or J— 1 1 2 1 .51- 2 1 2 .2 2. 2 * ' 2.2

Tj-iDpcuni 1 nnc.jn^i-L'n 3 1 . A ( - 4 ) 7 . 7 5. 5 • 7.7

6 1 JO 1 1 H 2 G NOX 0 — 1 U i or i— 1 Uo 1 99. 99 20 .6 19. 8 19 .» 20.6 28.3 26.1 NEUTRONS PO

L

AR I 2 ED

6 1 T A 1 IH 2 G N RLX C 22 THR-I DST

6 3BE7 IH 2 $ G N NOX 12- 30 C 30 SCI-D DST NUCL I DE REACT I ON RES EXC I T SOURCE DETECTOR NEUTRONS POLARIZED REF Z A IN OUT TYPE ANG

6 3 BO^ IH 2 $ G N SPC 3- 9 C 3- SLI-UUbl

NEUTRONS POLARIZED 66 HU2 2HE3 E E/ ABX 0- 150 D250-670 SCI-D DST 63FR1 IH 2 $ G N NOX 11- 23 C 2A CCH-D 1*8 2HE3 E E/ ABX 0- 17 D200 MAG-D 60 NEUTRONS POLARIZED 6 9 CM 1 2HE3 E E/ ABX 5- 20 D 57 MAG-D 180 64BE 8 1

H

2 G N NOX THR 3 2 C 32 SCI-DDST 6 9CH2 2HE3 E E/ SPC 0- 14 0 56 MAG-D 180 NEUT POLARIZATION 64 JO 1 2HE3 E E/P ABX 0- 12 0550 MAG-D DST

p. 1

H

2 G N 2 — 3 u 3 t3r3-lDbl 7 1 KU3 2HE3 E D ABX 13- 45 D 86 MAG-D DST POL NEUT ASYMM 72S<1 2HE3 E D RLX 16- 27 D 43- 87 MAG-0 DST

6 7 BA 1 H NOX LWV 1 EL—

U

DETECTED D AND P 999=1 GEV 2HE3 G N ABX 5- 170 C170 CCH-D DST

6 9 501 M 3 30 /"Ten /CO crt^ r\ f^cT 6 5 F E 1 2HE3 G N ABX THR- 170 C170 CCH-D DST

1

H

2 G N 17- 30 C 23- 30 TOF-D DST 66GE 1 2HE3 6 N ABX THR- 30 CTHR- 30 BF3-I API 70SH3 1 H 2 G N wn 10 — 9 5 C125 TOF-D DST 66VA3 2HE3 G N ABX THR- 170 C170 CCH-D 4P1

7 2M A 1 1

H

2 G N ABX 5 - 9

n c n c 1 r /. Dt U ^— 9 br3— I *+rl 70 BE 6 2HE3 G N ABX 8- 30 D 3- 30 MOD- I 4PI

7 2 N A2 IH ^ N NO X ^~ 30 C O 5 1 Ul U Ui> 1 64BE5 2HE3 G 2P ABX 8 22 C 8- 22 SCI-D 90

N POLARIZATION FORM FACTOR

5 5 AL 1 1

H

2 G 20- 6 5 L liU— EMU— 1 1 2HE3 G 2P SPC 9- 40 C 40 SCD-D 90 56D I 1 IH ^ G ABX 1 3 6~ 29 3 L342 ItL— D Uil ASUA 1 2HE3 G 2P ABX THR- 170 C170 CCH-0 DST

5 6KE 1 1

H

2 G AbX 7 3- 4 30 C150-*30 TEL-D DST

£ ^C T 2HE3 G D ABX 8- 20 C 22 SCI-D 90

5 6WH

1

1

H

2 G 6 0- 2 5 0 C 60-250 EMU-D DST 6 3F I 2 2HE3 G D ABX 1 3- 27 C 31 SCI-D 90

5 7 AL

1

1

H

2 G ABX 30- 150 C170»264 TEL-D DST 6 3G02 2HE3 G D ABX 5- 90 C170 CCH-D API

IH 2 G P ABX 146- 238 C146-238 TEL-D DST ALSO G.N

58WH1 IH 2 G P ABX 9- 2 3 C 9- 23 NAI-I DST 2HE3 G D ABX THR- 30 C 34 SCD-D 90

60 FE 2 IH 2 S G »P ABX 130- 300 C15O-300 EiMU-0 SPECTRUM

PROTONS POLARIZED 2HE3 G D ABX THR- 120 C175 CCH-D DST

'IH 2 G P ABX 50- 90 C 9* TEL-D DST 6 5 S T

1

2HE3 G D ABX 9- 46 C 40, 55 SCD-D 90

a! IM 1 IH 2 G tP ABX 330- 900 C500-900 TEL-D DST 2HE3 G 0 ABX 6 . 7 D 6. 7 lON-D 4PI

1 IH 2 s G ,P NO X 2- 294 C294 SPK-D 58 A4RF5 2HE3 G D ABX 8- 22 C 8- 22 5CI-D 90

IH 2 $ G fP RLX 80- 140 C400-500 MAG-O 90 FORM FACTOR PHOTONS POLARIZED 64G04 2HE3 G 0 ABX 5- 170 C170 CCH-0 DST

IH 2 i G ,P NOX 75- 250 C 75-250 MAG-D DST 6 5 F E

1

2HE3 G .0 ABX THR- 170 C170 CCH-D DST POL PHOTON 6 5VA

1

2HE3 6 .D ABX THR- 170 C170 CCH-D DST

6 7 K.0 3 IH 2 G P ABX 100- 420 C500 TEL-D DST 2HE3 G .0 ABX THR- 170 C170 CCH-D API

N IN COINC 69P I 3 2HE3 G D ABX 200- 500 C999 TEL-D 90 67TU2 IH 2 G »P NOX 9 D 9 EMU-I DST 999=1 GEV 68BU2 IH 2 G ,P ABX 140- 400 CitOO MAG-D DST 70BO3 2HE3 G D NOX 16- 26 C 33 SPK-I DST 68SM1 IH 2 G ,P ABX 100- 320 C210-330 TEL-D DST 72FA3 2HE3 S G D NOX 170- 290 D170-290 TEL-D 90 69AN1 IH 2 G P ABX THR- 342 C222-342 MAG-D DST POL ASYM PARAM G. 71TI 1 IH 2 G .P ABX 20- 33 C 60 TEL-O 90 720F2 2HE3 G D ABX AO- 150 C250 TEL-D DST 71WE2 IH 2 G P ABX 25- 55 C 60 SCD-D DST P AND D COINC

69IC01 IH 2 G ,P NOX 282- 403 C500 TEL-D DST PROT POLARIZATION

16
NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN. OUT TYPE ANG NUM LITHIUM Z=3

A ABUND.dl SEPARATION ENERGIES (MEV)

5 5GR 1 2HE 3 »

6

5

- 8 D 0- ~y MAI r\CT G.N 6, P C ,T G»HE3 G.A G.2N GtNP

6 2 GR 1 2HE 3 • G ABX 5- 7 D 0- o MAT r\c;T 7.42 5.7 4. 6 1

5

.8 15. 3 1.5 27.2 3.7

6 3 GR 1 2 HE 3 G 5

- 6 C 0- iN A I — U I/O I 7 92.58 7.3 10.0 2 .5 26. U *J 11.

O

S AN

C

P WAVE PARTS

66BA2 2HE 3 P »

G

AB X 110 D155 SCI-D DST 66W01 2HE3 P .G ABX 7- li. D 2- 12 NAI-0 DST NUCLI OE REACT ION RES EXC I T 6 7GE

1

2HE 3 »

G

9 D 2- 4 NAI-0 90 REF Z A I N »OUT TYPE ANG 67W01 2HE3 P .G ABX 7- 14 D 2- 12 NAI-D DST 70BA2 2HE3 P »G ABX 5- 7 D 0- 2 NAI-D DST 64G03 3LI » E / ABX U hU— i \j rlAu U loU D155 MAG-D DST FMF

7 2 CH3 2HE 3 p » G ABX 12- ]^ 7 D 10- 18 NAI-D 90 69AN8 3L I P »

P

RLY T HR — v-VW I'IMO U UOI

7 2HA2 2HE 3 » G R L X 1 4 — 2 3 D 14- 26 NAI-D DST CORRECTS 71VA1 69AN8 3L I Q T HR — 999 C999 MAG-D DST

70 BE^ 2HE 3 * 12* 1 5 D 19, 29 MAG-D DST DEUT, BEAM 69 AN8 3L I RLY THR-999

L.3 GEV REL P/D.O/T

Q Q O MAI" ri t T

7 1 V A 1 2 HE 3 »

G

ABX 12 — D 20- 45 MAG-D DST

SEE 72HA2 60 K,U2 68K A 1 3L I 3L I

N ABX

ABX

T HR50 — 90

85

ooo-i r, pw» RFi n/T

r on TFi — n nt.T

61BU2 2HE^ ABX 325 D400. 500 MAG-D DST NEUT ENGY SPEC

65FR1 2HE^ E .E/ ABX 0- 30 0200 MAG-D DST 55HE1 3L I G .XN RLX 13- 32 c i ^— 3^ br J— I 4K

I

6 8 FR 1 2HE^ » E / 20" 30 D150- 400 MAG-D DST tlNKlCnLU Lw

T n I.I A z.

f U W M H 2HE^ 19- 31 D 56- 65 MAG-D DST 5 8R Y 1 3L I G XN ABX 5- 24 C 5- 24 BF3-I 4PI 20.1 MEV LEVEL G ABX 11 — 56 C 11- 57 BF3-I 4PI

7 OWA 5 2HE^ E / FMF 19- 31 D 55 MAG-D DST 63C03 3L I G XN ABX 8 — 75 C 8-100 BF3-I 4PI 72SK3 2HE4 E D ABX 35- 50 D 35- 50 MAG-D DST 64AL1 3L I 1 XN ABX THR — 19 C - 19 BF3-I 4PI

7 2D01 2HE^ E HE ABX 30- 52 D 90 MAG-D 90 63K I 1 3LI ABX 150 — 335 C335 TEL-D DST HE=HE3 . RATIO G»P/G»N 63KU2 3L I ABX 10 — 30 C 30 DST 72D01 2HEi^ E T ABX 30- 52 0 90 MAG-D 90 RATIO G,P/G,N 66M A 1 3 L I p SP C 1 0 — 28 G-WIDTH

C 32 TEL-D 90 58G01 2HE^ G N ABX 2 0- 160 C170 CCH-D DST 7 1 AN 1 3L I S PC 4 1- 999 C700.999 TEL-D DST

58L I 1 2HE^ (3 N AB I 40- 60 C 70 EMU-I DST 999=1.2 GEV, REL D/P DETECTED HE3 7 2 AN 3 3L I G p RLY 34 999 C999 MAG-D DST 66FE1 2HE^ G N ABX 20- 80 C 20- 80 BF3-I 4PI 999=1.1 GEV

68G02 2HE4 G N ABX THR- 260 C250 CCH-D DST 58 WH2 3L I G .XP ABX 40- 100 C 45-110 TEL-D DST 68G05 2HE^ G .N ABX 26- 150 C170. 260 CCH-D DST 6 1 M A 2 3L I G .XP NOX 10- 21 C 21 SCI-D OST

69 AR 3 2 HE 4 S G N NOX 2 2- 6 4 C300 CCH-D DST

POL OF HE3

6 26E 1 3L I G . D RLY THR- 260 C160-250 MAG-D DST YLD REL TO PROTONS

69 A R^ 2HE4 N ABX 21 — 120 C120 CCH-D DST 263 + 6 6M A 1 3L I G D SPC 10 — 28 C 32 TEL-D 90 70WA2 2HE4 G N ABX 50- 8 5 D 91 MAG-D DST 7 lANl 3L I ^ SPC 46 — 999 C700.999 TEL-D OST

7 1 6U

1

2 HE4 *p

V 2 5 — 80 C 80 CCH-D OST 339 999=1.2 GEV. REL D/P

G

w 3 2 C 35 TOF-D 90 7 2 AN 3 3 L I RLY 999 L9V9 MAG-D Deal 70BE9 2 HE 4 G xw 2 1 — 3 2 D 21- 32 BF3-I 4PI 3 38 999=1.1 GEV

7 IBE 3 2HE 4 ^ 1(N ARX 2 0- 3 1 D 20- 31 BF3-I DST 63ICU2 3L I Q T ABX 12- 2 7 C 3 0 DST

5 7G0

1

2HE4 G P A BX 2 0- 160 C170 CCH-D DST A — W I n T H

6 OM I 1 2H E 4 G P ABX 23- D 32 EMU-D 90 66M A

1

3 L 1 G T ABX 10- 28 C 32 TEL-D 90

2H E4 G NOX 2 3 — 33 C 70 EMU-D DST 72AN3 3L I G T RLY 83-999 C999 MAG-D DST

6 5 AR 1 2HE 4 p ABX THR — qQQ 9 C999 CCH-D 4PI 999=1 GEV 58BA3 3L I G NP RLX 150- 280

999 = 1. 1 GEV

V_^OVJ ILL L/L/OI 65CL 1 2HE 4 G P ABX 24- 56 C 40- 60 SCD-D 90 PAIR SPC.NP.COIN

67BU

1

2HE4 G p RL Y THR- 5 4 C 44. 5i* ACT-I 4PI 67DE3 2HE4 G P ABX 24- 50 C 52 TEL-D 90 64 IMl 3L I 4 p G ABY nU H—U INMI wAi_nU on7U

6 8G02 2HE4 p AB X THR — 260 C260 CCH-D DST M n 1 1 Zi F n 1 1 ^l ri INVJ Lit ruui\u 67G05 2HE4 G p ABX 20- 170 C170 CCH-D DST 68G05 2HE4 G P ABX 20- 200 C17C , 260 CCH-D DST 68BU1 3L 15 G 16- J 7 A RMI 1

1

2HE4 p 2 3 — 32 C 28. 33 SCI-D 90 68<R 1 3L I 5 D G AftX 16- 19 0 2-6 NAI-0 DST 69AR2 2HE4 p ARX 23- 32 C300 CCH-D 4PI J-PI. 3/2+

69 AR 3 2HE 4 i G NOX 2 2- 64 C30J CCH-D DST 6 8DE 2 3 L I 5 HE G ABX 17- 21 0 2- 12 NAI-D 90 POL OF P AND T HE=HE3

69P I 2 2 HE4 p ABX 18 0

— 480 C TEL-D 90

P AND D COINC

3 L I 5 HE G A BX 18- 21 D 4- 12 NAI-D DST HE=HE3

69SAI 2HE4 G P ABX 22- 30 C 32 EMU-O DST 72KI2 3L I 5 HE G ABX 17- 26 D 2- 26 NAI-D DST

70 AR2 2HE4 0, p ABX 2 0- 120 C 20- 120 CCH-D DST

SEE 71AR1 HE=HE3

70S A I 2HE 4 Q p ABX 2 3- 32 C 32 EMU-D DST 60BA4 3 L 1 6 £ £ / ABI 0 40 MAG-D DST 70WA2 2HE4 G P ABX 22- 70 D 91 MAG-D DST 63BA1 3L 16 E E / AB I 16 0 42 MAG-D 180

7 1 BU

1

2 HE4 p ABX 24- 80 C 80 CCH-0 DST 4 LEVELS

60RE2 2HE4 G XP NOX THR- 330 C330 CCH-D 4PI 63BE2 3L I 6 E / FMF 8 DlOl MAG-D DST

65 AS 1 2HE4 Q XP ABX 78 - 300 C250 . 300 TEL-D DST 5 LEVELS

69P I 3 2HE4 XP ABX 2 00- 500 C999 TEL-D 90 999=1 GEV

6 3B E 8 3L I 6 E E / FMF 0 — 7 0100-180 MAG-D DST J-PI. B(E21

7 1 A R 1 2HE 4 XP NOX 2 0- 50 C 20- 50 CCH-D DST 63B I 1 3L I 6 E E/ ABX 5 — 40 DlOl MAG-D 50 NEW ANAL OF 70AR2 6 6 AR2 3 L I 6 E c / L F T ^~ 4 D MAG-D DST

65 AR 1 2HE4 D AB Y T HR-999 C999 CCH-D 4PI 999=1 GEV 6 8E I 1 3 L I 6 E E / L F T 2 . 4

2 = 2. 18. 4=3.55 MEV

D 30- 58 MAG-D DST

6 5 AS 1 300 C250 . 300 TEL-D DST COINCIDENCE 68HU1 3 L I 6 E E / FMF 2=2.184, 4=3.562

D 53-127 MAG-0 DST

5 7G0 1 2HE4 p AR 20 160 C170 CCH-D 4PI 6 9 E I 1 3L I 6 E E / LET 2 — 5 0 30- 50 MAG-D OST 58BA3 2HE4 G MP 15 0- 280 C280 TEL-D DST 4 LEVELS 0 .2-.

6

PAIR SPC. NP COIN 3L I 6 E E/ FMF 0- 42 D 55-127 MAG-D OST

2HE 4 G NP ABX 2 5 — 170 C170 CCH-D 4PI AQNF 1 3L I 6 ^ E/ FMF 2 » 3 0109-282 MAG-D DST 69AR1 G 120 C120 CCH-D 4P1 2=2.184.3=3.562

69 AR 5 2HE4 NP ABX 2b~ 120 C120 EMU-D DST 2 8 3 7 OHU 1 3L I 6 £ / FMF D 5v-150 MAG-D DST 69AR 5 2HE4 2 p 2M ABX 2 8 — 120 C120 EMU-D 4PI 2 8 2 5.36 MEV LEVEL

6 9 GO 1 150 C170 CCH-D 4P

I

7 1 L I 1 3 L I 6 E E / FMF 2 0200.500 MAG-D DST 71G02 2HE4 G PI + RLY 150- 500 C500 CCH-0 DST 2=2.18 PI-/PI+ YIELD RATIO 7 IMO 3 3 L I 6 E E / ABX 0- 240 D500 MAG-D 60 63ZU 1 2 HE4 N ABX 2 ^ D 4 NAI DST 7 INE 1 3L I 6 E E/ FMF 5 0 80-190 MAG-D DST

5 5 P E2 2HE4 p 20 — 35 D 0- NAI-D DST 3=3.56. 5=5.35

6 2GA

1

2HE 4 p APX 2 27 D 6- 10 NAI-D DST 7 2 T I 4 3L I 6 E E/ SPC 0- 550 0999 MAG-D DST

G 2 3 — 28 D 4- 11 NAI-D DST 999=1.18 GEV

G APX 2 0 — 23 D 0- 4 NAI-0 0 64CH 1 3 L I 6 E P ABX THR- 999 D999 MAG-D DST

F G RLY 2 2 — 33 0 3- 18 NAI-D DST 440 999=1 GEV

5 F D G ABX 24 D 1 NAI 45 1=1,35 MEV

64E R2 59C04

3 L I 6 3L I 6G

G MU-TG ABX

LET

5-

4 40 C 5- 40 NAI-D 4P

I

C 6 NAI-D 130 69DE3 2HE4 0 G ABX 25- 30 D 4- 10 NAI-D 130 62B06 3L 16 G G LET C 4 NAI-D 110 69ME 1 2HE4 D G ABX 26- 34 D 5- 19 NAI-D 135 J-PI ANG DIST AT 10 MEV 62SE1 3L 16 G G NOX 4 C 17 NAI-D 90

63SIC1 3L 16 G G LET u C 4 NAI-D 105 63BU2 2HE5 D G RLY 17- 18 D 0- NAI-D 69RA3 3L 16 G G LFT 3 C 3 NAI-D DST 69BE10 2HE5 D G AEX 17 D999 NA I-D 3=3.56 MEV 999=25-100 KEV

70K01 2HE5 D G ABX 18 D 1 SCI-I 90 1=1025 KEV

17
NUCLIDE REACTION RES EXCIT

REF Z A IN OUT

56E02 3L 16 G N ABX 6 50PR1 3L 16 G N RL I 5

3L 16 G N ABX 5 66C05 3L I 6 G N ABX 5 66PA1 3LI6 G N SPC THR 59R01 3L I 6 G XN ABX 5 63C01 3L 1 6 G XN ABX 5 6A8A2 3L I 6 G XN ABX 5 65BA2 3L I 6 G XN ABX THR 65BE1 3L I 6 G XN ABX 6 55HA1 3H6 G XN ABX THR 60BA3 3L I 5 6 P ABY 30 60KO3 3L I 6 G P SPC 5

50KO5 3L I 6 G P SPC 5 60PR 1 3L I 6 G p SPC 5

62V01 3L I 6 G p ABY 1

1

64MA 3 3 L I 6 (3 p SPC THR 64S H2 3 L I 6 (3 p ABX s 65MA5 3L 16 G P SPC THR 66MA4 3L I 5 G P SPC THR 67DE2 3L 16 G P ABX 9 68MA1 3LI6 G P ABX 100 50CH1 3LI6 G XP RLY 20 62CH2 3L I 6 G XP RLY 20

65BA2 3LI6 G XP RLY THR 670D1 3L 16 G XP NOX 5

69S03 3LI6 G XP ABX 5 70W01 3LI6 G XP ABX 7 6 2 VO

1

3 L I 6 (3 ABY g 6^K04 3 L I 6 Q RLY THR

65DA1 3L I 6 G D ABY THR 65MA5 3LI6 G D SPC THR 66AL1 3LI6 G D ABY 100 67DE2 3L I 6 G D ABX 7 60CH1 3LI6 6 XD RLY 17

62CH2 3L I 6 G XD RLY 16

6 2 vol 3L I 6 G T ABY 2 3 54<04 3L I 6 G T SPC THR

55BA2 3L I 6 G T ABX 19 65MA5 3L I 6 G T SPC THR 55SH1 3LI6 G T ABX 19 67DE2 3L I 6 G T ABX 21 68MU2 3L I 6 G T ABX THR 58SH2 3LI6 G T ABX 24 70MU1 3LI6 G T ABX 18 70W01 3L 16 G T ABX 20 50CH1 3L 16 G XT RLY 31

60PR1 3L I 6 G NP RL I 7 58MU2 3LI6 G PD ABX THR 70MU1 3LI5 G PD ABX 22 64NE 1 3LI6 G H4 ABY 24

70W01 3LI6 G HE3 ABX 20 71VE1 3L I 6 T G ABX 20

66NU

I

3L 16 HE G ABX 1

6

68BH 3L I 6 HE G ABX 16

70Y01 3L 16 HE G ABX 16

63BA1 3L I 7 E E / AB I 7 63BE3 3L I 7 E E/ FMF 4 63BE8 3L I 7 E E/ FMF 0

64BI4 3LI7 E E/ ABX 1 65CH1 3L I 7 E E/ ABX 1 66AR2 3L I 7 E E/ LFT 11

69HU1 3L I 7 E E/ FMF 0 71VA3 3L 17 E E/ LFT 1

70W01 3L I 7 E p ABX 6 58BE3 3L I 7 G G LFT 1

59SW1 3LI7 G G LFT 1 60B03 3LI7 G G LFT 0 53M01 3L I 7 G G LFT 0 62M01 3L I 7 G G LFT 0 64801 3L I 7 G G LFT 1

54GR2 3L I 7 G N ABX THR

67BA2 3L 17 G N ABX THR 59R01 3L I 7 G XN ABX Q 65HA1 3L I 7 G XN ABX THR 65WA1 3L I 7 G XN SPC THR 59GA1 3L I 7 $ G XN SPC 2

69GA3 3L I 7 G XN SPC 8

9 97

30

20

50

6050

323080

23

DETECTOR

TYPE ANG NUM

MOO- I 4PI SCI-I 90

NUCLIDE REACTION RES

Z A IN. OUT

COINC WITH PROTONS

5- BF3-I 4PI

5- 97 BF3-I 4P1

30 EMU-D 90

4- 20 BF3-I 4PI

5- 50 BF3-I 4PI

5- 50 BF3-I 4PI

5- 50 BF3-I 4PI 5- 32 BF3-I 4PI

5- 30 BF3-I 4PI

5- 87 TEL-D DST

8 EMU-D 50 SEPARATED ISOTOPES

- 28

- 17

- 90

- 20

- 10

- 31 -102

- 55

- 90

- 90

- 30

- 15

- 12

- 19

- 90

- 35

- 31 -700

- 55

- 90

C 28

C 17 RLI ,

EMU-D 60 SCI-D 90 COINC WITH N

C 30- 90 TEL-D

C 20

C 10

C 31

C

C

EMU-D EMU-D SCD-0

95,102 TEL-D

30- 55 TEL-D

95-102 TEL-D

90 DST OST

90 DST

90 DST

9030- TEL-I DST

90 TEL-D DST

REL TO DEUTERONS

C 20. 28 EMU-D DST

C 16 EMU-D 45 15=15.7 MEV

C 32 EMU-D 4PI

C 22. 27 MAG-D 90

C 30- 90 TEL-D 90

C 35 EMU-D DST REL TO T C 4 SCD-D 90

C 31 SCD-0 90 C200-800 MAG-0 35

C 30- 55 TEL-D 90

C 90 TEL-0 OST

REL TO PROTONS. SPC

C 30- 90 TEL-D DST

REL TO PROTONS

- 90

- 35

- 25

- 31

- 24

- 55

- 32

- 35

- 28

- 52

- 90

- 17

- 32

- 32 -250

- 52

- 28

- 25

- 28

- 36

90 TEL-D 90 EMU-D OST

YLD REL TO D EMU-D DST

31 SCD-D

40 SCO-D

30- 55 TEL-D

32 EMU-D

40 MAG-D

32 EMU-D

90 MAG-D

90 TEL-I DST REL TO PROTONS

9090

90 DST

90 DST

90

17 SCI-I 90

32 EMU-D 4PI

32 EMU-D 4PI C250 ACT-I 4PI NO H4 FOUND

C 90 MAG-D 90

0 9- 25 NAI-D OST HE3 BEAM

D 5- 20 NAI-D OST HE=HE3

0 0- 11 NAI-D OST HE=HE3

0 0- 20 NAI-D DST HE=HE3. SEE 58BL1

14 D 42

8 DIOO7 0100-

6 0150

0 2- 0 30-

25 D 55-

D 25-

20 C

C

0

C0

C

3 C

MAG-D 180

180 MAG-D DST

180 MAG-D DST J-PI. B(E2) MAG-D DST

4 MAG-0 152 60 MAG-0 DST 11=11.28 MEV

127 MAG-D DST

90 MAG-0 OST 1=478 KEV

90 MAG-D 90 NAI-D 120 WIDTH

NAI-D OST NAI-D 100 NAI-D

NAI-D

NAI-D

11 DTHR135

130

100

ABI 4P I

5020

3025

85

5-

25

85

N 85

11 BF3-IWIDTH

50 BF3-I 4PI 288

20 BF3-D 4PI

30 BF3-I 4PI EMU-D 90 CCH-0 DST POLARI ZAT ION CCH-0 DST

626R2

62LI1

3L I 7 3LI 7

52SH1 3LI7

52V01

63<U1

670E1

6BMA1 69AN4

69AN6

70T02

63NE1

54SH1

60CH1 62CH2

3L 1 7 3LI7

3L I 7 3LI7

3L 17

3L I 7

3LI7

3L 17 3L I 7

3L I 7 3L I 7

G

S G

G

G

G

G

S G

70SA2 3L I 7 G XP ABX 50- 84 62V01 3L I 7 G 0 ABY 17- 90 570E1 3L I 7 G 0 ABX 15- 50 69AN5 3LI7' G 0 ABY 107-999

50CH1

62CH2

71AN2

55M 1

1

50MI2

51SH5

52V01

53KU1 65DA1

570E1 59S03

59DE7

50CH1

60ST1

67SM1

54NE1

3L 17

3L I 7

3LI7 3LI7

ABX

NOX

10- 155-

ABX 12- 15 C

ABY ABY

ABX ABX

RLY

ABY

NOX

ABY

ABX

ABX

RLY

17-

3- 14- 100 320

107-

550-

THR- THRDETECTOR

TYPE ANG NUM

30 C 10- 30 ACT-I 4P1 C355 TEL-D OST PLR P BY C SCT

12- 16 EMU-D DST G-WDTH

25- 90 TEL-D DST 20- 30 TEL-D OST 21- 52 TEL-D 90 95-102 TEL-D DST MAG-D 33

90

10

50

90

90

RLX

RLY

25-

25-

C0

C

C0320 COHERENT BREMS

999 C700.999 TEL-D DST 999=1.2 GEV

840 C700.810 MAG-D 41 P-POLAR I ZAT ION 320 C320 ACT-I 4P

I

210 C210 ACT-I 90

H5 LIMIT

999 DTHR-999 ACT-I 4PI NO H5. 999=1 GEV

C 90 TEL-I DST

C 25- 90 TEL-D DST REL TO DEUTERONS

999 C620.999 TEL-D OST 999=1115 MEV

D 50- 84 TEL-D 45

C 25- 90 TEL-0 OST

C 21- 52 TEL-D 90 C700,999 TEL-D DST 999=1.2 GEV

90 C 90 TEL-D DST

REL TO PROTONS. SPC

90 C 25- 90 TEL-D DST REL TO PROTONS

-D DST

-D 4PI

•D DST

J-P I -D OST

-0 OST

3L I 7 G XD ABX 100- 520 C520 MAG

3L I 7 G T ABX 5- 21 C 10, 21 EMU

3L I 7 G T ABX 5- 15 C 11- 20 EMU

3LI7 G T ABX 5- 9 C 10 EMU

3L 17 G T ABY 14- 90 C 25- 90 TEL 3LI7 G T ABY 14- 25 C 30 TEL

3L I 7 G T ABY THR- 4 C 4 SCO

3L I 7 G T ABX 8- 50 C 21- 52 TEL

3L I 7 G T ABX 5- 1

1

C 12 EMU

3L I 7 G TG/ ABX 23- 32 C 18- 32 TEL 3LI7 G XT RLX 19- 90 C 90 TEL

289

D 90

D 90 292

0 4PI

D 90

D DST

REL TO PROTONS. SPC

320 C320 TEL-D 75 293 REL TO h2 CROS SEC ABX 150- 250 C250 TOF- 0 OST

ABY 23- 250 C250 ACT- I 4P I NO H4 FOUND

RLY 150- 500 C50Q CCH- D DST PI-/PI+ YIELD RATIO

G.N

1 . 7

BERYLLIUM Z=4

SEPARATION ENERGIES IMEV) G.P G.T G.HE3 G.A G.2N G.NP

15.9 17.7 21.2 2.5 20.5 18.9 G.2P

29.3

REF

59NA2

59GE1 60MA2

51ME1 52CA3

63M I 1 53PE1

63RE1

63R I 1 64SC2

54TA1

578L2

67N I 1

508A4

62ED1

53NG1 63NG2

65NG1

NUCLIDE REACTION RES

Z A IN. OUT

4BE8

4BE8

4BE8

4BE8

4BE8

4BE8

4BE8

4BE8 4BE8

4BE8

4BE8 4BE8

4BE9

4BE9

4BE9

4BE9

4BE9

EXCIT SOURCE DETECTOR

TYPE ANG NUM

2 D 0- 1 NAI-D 90 SOURCE 164-245 KEV

p G ABX 21- 25 0 4- NAI -0 90

p G RLY 17- 18 0 C- NAI -0 DST

p G NOX 18 0 0 NAI -D DST

p G RLX 18- 20 D 0- NAI -0 DST

p G RLX 19- 26 0 2- NAI -D DST

P G RLX 18- 27 0 1- 1 1 NAI -0 OST

p G ABX 19- 25 D 4- NAI -0 OST

P G LFT 18 0 0- NAI -D 90

p G RLX 17- 19 D 0- NA I -D OST

J -PI

p G ABX 21- 25 0 4- NAI -0 90

p G RLX 17- 34 0 1- 18 NAI -0 90

p G RLY 18- 19 D 1- 3 NAI -D DST

E E/ ABI 2 D 42 MAG -0 160

E E/ SPC 0- 20 0 42 TEL -0 180

55AR2 48E9

55CL1 67BE1

68VA1 65AM3

48E9 48E9

4BE9

4BE9

E E/ LFT 1- 6

E E/ FMF 4- 47

E E/ FMF 2- 47

E E/ LFT 15

E E/ LFT 14- 17

E E/ FMF 2

E E/ ABX 0- 26

E E/P RLY 8- 50

G-WDTH, ABX

0 50-250 MAG-D DST

47 0100-180 MAG-D 135

D 50-250 MAG-D DST 2.47.6.4 MEV.CONT

0 MAG-D DST 16=15.97 MEV

0 40- 50 MAG-D DST 0340 MAG-0 DST 2=2.43 MEV

0 42- 58 MAG-D 180 0510-590 MAG-D 51 100 MEV P COINC

18
NUCLIDE REACTION RES EXC I T SOURCE DETECTOR NUCL I DE REACT I ON RES EXC I T SOURCE DETECTOR

REF Z A I N OUT TYPE ANG NUM REF Z A I N .OUT TYPE ANG

58BA2 'tBE9 E N ABX 2- 16 C 2- 16 BF3-I 4PI 66DE6 4BE9 G . J ABX T HR- 5 0 G 20— 50 TEL— 0 90 COMPAREC WITH G.N 56 VO

1

4BE9 ABX T HR — 8 1 G 71— fil TFI— n QH 59BA3 4BE9 E N ABY THR- 36 D lo- 36 BF3-I 4P I 6 8 AD 1 4BE9 ' ^ RLY 18 — 28 68B02 4BE9 E XXX RLY THR- 119 D119 MAG-D 76 XXX=MASS SPECTRUM 6 0 C H

1

4BE 9 .XT RLY 3 2 — G 62^4 4BE9 G MU- T ABX 16- 27 C 31 MGC-D 4P I REL TO DEUTERONS

5'iTEl 4BE9 G MU- T ABX 20- 21 D 20- 21 NAI-D 4PI 64BE 1 4BE9 G . A SPC THR- 34 c 34 SCD-D DST 55WY1 4BE9 G MU- T ABX 10- 35 C 90 SC I -D 4P I 54 J-PI 69D03 4BE9 G MU- T ABX 10- 30 C25J MGP-D 4PI 262 68AD1 4BE9 G .A RLY 3- 28 C 28 MAG-D 4P! 71AH1 4BE9 G MU- T ABX THR- 150 C 10-150 MGC-D 4P I FORWARD YIELDS

54L03 4BE9 G G ABX 10- 30 C 10- 30 NAI-D 140 64BE1 4BE9 G .2A SPC THR- 34 C 18- 34 SCD-D 90 67L01 4BE9 G G/ ABX 12- 30 C 34 NAI-D DST J-PI 55J01 4BE9 G N RLY 12- 65 C 55 SC I-D DST 50ST1 4BE9 G ,NP RLX 149- 320 C320 TEL-D 75 36ED1 4BE9 G N ABX 2- 8 D 2- MODI

4PI REL TO H2 CROS SEC 56FA1 46E9 G N NOX THR- 1 8 C 18 SCI-I DST 65LA1 4BE9 p .G ABX 160 D165 SCD-D DST 58AS1 4BE9 (-J N NOX 2- 1 7 C 17 SCII

OST 71SC2 4BE9 D .G SPC 17 D 0 NAI-D 135 58BA2 4BE9 N ABX 2- 1 6 C 2-16 BF3-I 4PI 17 = 16. 97.0=. 361 MEV COMPAREC W I TH E.N

59G I 1 48E9 N ABX 1 D 1 . BF3-I 4P I 59TH1 4BE9 G N ABX 6- 18 C 5-18 BF3-I 4P I 60KU2 4BE9 G N RLY 12- 90 C 90 TEL-I DST 61JA1 4BE9 G N ABX THR- 5 CTHR- BF3-I 4P I BORON Z = 5 62BO't 4BE9 s G N NOX 3 D 3 BF3- I DST NEUTRONS POLARIZED

62B07 4BE9 N NOX 5- 9 D 5- SCI-I DST A ABUND. 1 1

1

SEPARATION ENERGIES (MEV) 62CU1 48E9 G N ABX 4- 32 C 32 EMU-D OST G.N G. P C .T G.HE3 G.A G.2N G.NP

62J02 4BE9 Q N ABX l

- I D 1- MOD-I 4P I 10 19.51 8.4 6. 5 18.7 17. 8 4.5 27.0 8.3 63B04 4BE9 G N ABX 3- 9 D 5- SCI-D DST 1

1

80.39 11.5 11.2 11 .2 27. 2 8.7 19.9 18.0 NEUTRONS POLARIZED

4BE9 I G N NOX 3 D 3 DST NEUTRONS POLARIZED NUCLIDE REACTION RES EXC I T SOURCE DETECTOR

54K05 48E9 G N RLY 1 5- 32 C 35 MAG-D OST REF Z A IN OUT TYPE ANG

66C0it 48E9 G N AB I 6- 80 C 6- 80 BF3-I 4P I G N SPC 8 5 C 8 5 CCH-D 135 5B p RLY 30 C 30 MAG-0

66 T H

1

4BE9 SPC THR~ C 17 SCI-D 90 59C05 5B G . G AB I 5 , 7 C 5. NAI-D 130 67BE6 4BE9 G N ABX 2- 4 C 2- 4 TOF-D 135 60RE1 5B G 6 ABX 7 D 7 NAI-D 90 56<A1 4BE9 G N ABX 50- 85 C 55. 85 TOF-D 67 52SE1 5B G G RLY 0- 13 13 NAI-D 90 NEUT ENGY SPEC 64B01 5B G G LFT 1- 3 C 1- NAI-D 100 57L01 4BE9 G 2N ABY 20- 30 C 20- 30 ACT-I 4P I ABI 64AR2 4BE9 G 2N RLY 2 1- 57 C 44. 57 ACT-I 4PI 68KA1 5B G N ABX 50- 85 C 55. 85 TOF-D 57 REL TC C12 ( G.N

]

NEUT ENGY SPEC

67&A1 4BE9 G 2N ABY THR- 23 C 23 ACT-I 4P I 63C03 5B G XN ABX THR- 80 CTHR- 80 BF3-I 4P

I

55BA5 46E9 G XN ABY 30- 200 C150-250 THR- I DST 71C02 5B G XN AB I 35- 54 C 10- 54 BF3-I 4PI

5501 1 4BE9 G XN NOX 2- 70 C 70 SCI-I DST FAST N YIELD

59KU1 4BE9 G XN NOX 12- 88 C 88 TEL-I DST 60CH1 5B G XP RLY THR- 90 C 90 TEL-I 90 60BE1 4BE9 G XN ABX 2- 17 C 5- 17 TOF-D DST REL TO DEUTERONS

6'iAL5 4BE9 G XN NOX THR- 34 C 34 THR- I DST 63K. I 1 5B G XP ABX THR-355 C335 TEL-D OST 65C02 4BE9 G XN AB 1 6- 80 C 5- 80 BF3- I 4PI 50CH1 5B G XD RLY THR- 90 C 90 TEL-I 90 695A1 4BE9 $ G XN SPC 2- 85 C 85 CCH-D DST REL TO PROTONS

N POLARIZATION 50CH1 5B G XT RLY THR- 90 C 90 TEL-I 90 59GA3 4BE9 G XN SPC 3- 85 C 85 CCH-D DST REL TO DEUTERONS

72TH2 4BE9 G XN ABX 6- 28 C 7- 28 BF3-I 4P I 57GA1 5B G BE7 RLY THR- 23 C 23 ACT-I 4PI 56C01 4BE9 G P ABY 19- 24 C 24 EMU-D 90 58CH1 4BE9 G P SPC THR- 44 C 44 EMU-0 DST 56PA4 58 8 p G ABX 1 - 2 D 1- 2 SCO-D 2PI

6 ENERGY GROUPS

6 2CL 1 4BE9 G p ABX 16- 54 C 15- 54 ACT-I 4PI 62ED1 58 10 E E/ ABX 0- 20 D 42 MAG-D 180 62CU1 4BE9 G p ABX 16- 2 8 C 32 EMU-0 DST 6 5 F R 2 5 6 10 E E/ FMF 5 DlOO-220 MAG-D DST 62L I 1 4BE9 i G P NOX 190 C355 TEL-D DST 5=5.02 MEV PROTONS POLARIZED 55SP1 5B 10 E E/ FMF 7 0 55 MAG-D DST 62V02 4BE9 G P ABX 40- 90 C 40- 90 TEL-I 90 WIDTH. 7.48 MEV

53>; I 1 4BE9 G P NOX THR- 335 C335 TEL-D DST 65K01 5B 10 E E/ A6X 0- 18 D 50. 60 MAG-D 180

5't<06 4BE9 G P ABX 15- 32 C 35 MAG-D DST 8 LEVELS

55K.02 4BE9 G P ABX 18- 3 1 C 35 EMU-D DST 56SP 1 5B 10 E E/ ABX 6 . 7 D 32- 57 MAG-D DST 66DE6 4BE9 G p ABX THR- 50 C 2U- 50 ACT-I 4P I 6 .7=5.01.7.47 MEV

66DE6 4BE9 G p ABX THR- 50 C 20- 50 TEL-D 90 64L03 5B 10 G G ABX 10- 30 C 10- 30 NAI-D 140 66V01 4BE9 G P ABX THR- 81 C 21- 61 TEL-D 90 57L01 5B 10 G G/ ABX 12- 30 C 34 NAI-D DST 69AN6 4BE9 G P ABY 1 14- 999 C700 .999 TEL-D DST 64GR2 5B 10 G N ABX 9- 1 1 D 9- 11 8F3-I 4PI 999=1.2 GEV WIDTH

71AN1 4BE9 G P SPC 51- 999 C700 .999 TEL-D DST 65HA1 58 10 G XN ABX THR- 30 C 6- 30 BF3-I API 999=1.2 GEV . REL D/P 62V02 68 10 G P ABX 23- 90 C 90 . SCI-D 90 57CH1 4BE9 G XP SPC THR- 84 C 68. 84 EMU-D OST 68SH5 58 10 G P ABX 6- 13 C 13 EMU-D DST 5eWH2 4BE9 G XP ABX 40- 100 C 45-110 TEL-D 90 13=12.5 MEV

59CH1 4BE9 G XP RLY THR- 80 C 90 TEL-D DST 62CH2 58 10 G XP ABX 23- 90 c 30- 90 TEL-0 90 REL C TO P YLD 62V02 56 10 G D ABX 25- 90 c 90 SCI-D 90 60CH1 4BE9 G XP RLY 30- 90 C 90 TEL-I DST 62CH2 56 10 G XD ABX 22- 90 c 30- 90 TEL-D 90 REL TO DEUTERONS 62EL1 56 10 P G NOX 7- 8 D 1 NAI-D 90 62CH2 46E9 G XP ABX 40- 90 C 40- 90 MAG-D DST J-PI 68AD 1 4BE9 G XP RLY 17- 28 C 28 MAG-D 4P I 53FU3 56 10 P G ABX 7- 9 D 1- NAI-D DST FORWARD YIELDS G-WDTH. J-PI . T 71C01 4BE9 G XP ABY 17- 90 C 50- 90 TEL-D 60 7 IL I 3 58 10 T G LFT 18. 19 D 1- 2 SCD-D DST 62BA1 46E9 G D ABY 40- 60 C 45- 52 ACT- I 4PI J-PI . 18.4.19.3 MEV

64K:05 4BE9 G D RLY 1 5- 32 C 35 MAG-D DST 55PA1 56 10 HE G ABX 18- 19 0- 3 NAI-D DST 660E6 4BE9 G D ABX THR- 50 C 20- 50 TEL-D 90 HE=HE3

66V01 48E9 G D ABX THR- 81 C 21- 81 TEL-D 90 58L I 1 56 10 HE G ABX 21- 27 D 3- 6 NAI-D DST 59AN6 4BE9 G 0 ABY 1 1 4- 999 C70O.999 TEL-D DST HE=HE3

999=1.2 GEV 66F02 58 10 A G SPC 5- 7 D 1- 3 NAI-D 90

7 lANl 4BE9 G 0 SPC 55- 999 C700.999 TEL-D DST 999=1.2 GEV . REL D/P 52E01 58 11 E E/ ABX 0- 20 D 42 MAG-D 180 59CH1 4BE9 G xo RLY THR- 80 C 90 TEL-D DST 54BR2 56 11 E E/ SPC 8- 9 0 54 MAG-D 141 REL C TO P YLD 55AR2 58 11 E E/ LFT 4

.

5 0 30- 50 MAG-D DST 60CH1 4BE9 G XD RLY 19- 90 C 90 TEL-I OST 4 = 4.45. 5=5.04 MEV

REL TO PROTONS 66<01 58 11 E E/ ABX 0- 19 D 50. 60 MAG-D 180 62CH2 4BE9 G XD ABX 40- 90 C 40- 90 MAG-D DST 7 LEVELS

68AD1 4BE9 G XD RLY 17- 28 C 28 MAG-D 4PI 65R I 1 66 11 E E/ FMF 2 . 4 D MAG-D DST FORWARD YIELDS 2 .4=2.13.4.45 MEV 71AN2 4BE9 G XD ABX 107- 620 C520 MAG-D DST 66SP1 58 11 E E/ A6X 2- 9 D 32- 67 MAG-D DST

2. 12.8.56.8.93 MEV 57SP1 56 11 E. E/ FMF 4 . 5 D 35- 57 MAG-D DST

4 .5=4.45.5.04 MEV

71VL1 56 11 E . E/ FMF 0- 300 D592-999 MAG-D DST

19
NUCLIDE REACTION RES EXCIT SOURCE DETECTOR NUCLI OE REACT ION RES EXCIT SOURCE DETECTOR

REF 2 A I N OUT TYPE ANG NUM REF Z I N .GUI TYPE ANG

72N03 5B 11 E PI- RLY 150- 999 C150-999 ACT-1 4PI 67CR1 6C 1

2

.E / FMF 0- 1 0 DlOO-200 MAG-D OST 999=1.2 GEV RLY TO G 4. 43 . 7.66 .9 . 4 MEV

58ME1 5B 1 1 G LFT 2 n 0 MAT_ri on 6 7CR2 6C FMF 19 D400-800 MAG-O OST 58RA1 5B 1 1 G G LFT D 4 NA I -D DST 1Q— IQ S MF\/ 60BO3 5 B LFT 2 v_ 1 — INAI— U iiU 67PE1 1 2 E » E / LFT 1 5 D 40- 65 0 DST 62B06 5B 1 1 G G LFT 2 C 1 - NA I -D 110 15=1^-1 MF

V

J-P I 68BE6 » t / FMF ft D 63-128 MAG-D OST 63VA1 5B G NOX 0- 3 C 3 NAI-D 60 1 0 L. MFV 1 FUFI

5'tL03 5B 1 1 G G A6X 10- 30 C 10- 30 NAI— D 140 6 8 DE 3 6C 1

2

E . E / FMF 55 — 2 02 ri c, Q f 1 — Q 6. D M A n ri C T 65KE1 bQ \ 1 G LFT 2 C 5 NAI-D135 6 8 OR 1 6C 1

2

E » E/ FMF 1 9 U'lHU I'IMv? ij L'OI

C — c. * L D IIUV lO— lO U MFU

67L01 58 G / ABX 12- 3 0 C 34 NA I -0 OST 6 8 P R

1

6C 1 2 E » E / FMF 14- 2 1 69MU2 5B 1 1 G NG SPC 11- 35 C 24» 35 SCD-D UKN 6 LEVELS

GAMMA SPECTRUM 68R I 1 6 C 1 2 E . E / FMF 2 6 — 3 5 n AO- inn MAfi— n n^T 65HA1 58 1 1 G XN ABX THR- 30 C 6- 30 BF 3- 1 4P

I

2 15 + 698E 5 6C

^ FMF 180 0200-300 MAG-D 60 62LU 56 1 I $ G p NOX THR- 355 C355 TEL-D DST 690E6 6 C 1

2

E . E / ABX 30 0 0580-968 MAG-D DST POLARIZED PROTONS 6 9GU 2 1

2

ABX 62V01 5B 1 1 G P RLY THR- 40 C 40 TEL-D 90 69T I 2 6C 1 2 £ . E / ABX n~ 7nn 0999 MAG-D 25 69S02 5B 1 1 G P ABX 15- 32 C 15- 32 SCO-D 4P

1

216 999= 1.126 GEV

70S01 56 1 1 G p ABX 1 1- 1

9

C 17* 19 EMU-D DST 279 + 69 T02 E * FMF 1 1 D183.250 MAG-0 OST 69MU2 56 1 1 G PG SPC 11- 35 C 24» 35 SCD-D U<N 11=10.8 MEV GAMMA SPECTRUM 69T04 6C 1

2

* ABX D177.250 MAG-0 DST 56TA1 56 1 1 G 2P ABX THR- 3 2 0 69VA1 6C 12 r ABX D 5 0- 70 MAG— 0 180 DELAYED NEUTRONS 15.1.19.2 MEV 63NE2 56 1 1 G 3P A6Y THR- 320 C320 ACT-I 4P

I

70 AN 1 6C 1 2 E » c / ABX 16- 3 0 D 55 MAG-D 141 56NE1 56 1 I G 3P A6Y i+5- 2 5 0 C 2 5 0 AC T - I 4P I 70DE 1 6C 1

2

E » E / ABX 400 — 999 D690.999 MAG-D OST 62CH2 56 1 I G XP RLY 19- 40 C 40 TEL-D 90 999=1115 MEV

REL TO PROTONS 70L I 1 6C "1 2 E . E / FMF 2 2- 37 n ^7 — ^ r\7 mat-. — n n^^T

7 1 PA 1 56 1 1 G NG A6X 10- 35 C 20- 35 SCD-D 90 RFH MATPiy Fl FMNTC,

7 IPAl 58 I \ G PG A6X 10- 3 5 r 70— "^rn — n on 70L 12 6C 1

2

. E / AB I 7 D 52-102 MAG-0 OST 62V01 56 I 1 G RLY THR- 40 C 40 TEL-D 90 SEE 70LI1 62CH2 5B 1 1 G XD RLY 24- 40 70ST2 6C 1

2

. E / ABX 7 D 31- 59 MAG-0 DST REL TO PROTONS 7=7.55 0+ 62V01 56 1 1 G T RLY THR- 40 C 40 TEL-D 90 7 0 TO 1 6C 1 2 E . E / FMF 1 5- 30 68NY1 56 I I G P I - ABX 140- 700 ri/. ii_"7nn ai^t_i /iDt 7 16E2 E FMF D 77-106 MAG-D OST

C — 1 1 ACT 71 MO 3 6C 1

2

. E / ABX 0 - 240 0500 MAG-D 60

7 2N0 3 56 1 1 G PI — ABX 15 0- 999 C150-999 ACT-I 4Pl 71NA1 6C 1 2 » E / FMF 9

— 1 7 0250 MAG-D DST LEVELS 14. 1 ,4.43 70G02 ABX 12- 235 7 INAl 6C 1 2 » E / FMF 9 — 1 7 0250 MAG-D DST

j_p J ,G-W I DTH ERRATUM 71NA1 61KN1 56 \ I G ABX 16- 18 D 0- 2 THR-I 4P

I

7 1 Y A2 E ABX 100 D 88-250 MAG-D OST 62SU2 D G RLX 16 — J-PI , FMF, 10 LEVELS

63SU2 56 1 1 D G A8X 16- 20 D 1- NAI-DDST 64AM1 6C 1 2 . E /P RLX T HR - 150 D550 MAG-0 51

6i(SUl 58 1 1 D G ABX 18- 2 3 D 0- 5 NA I -0 DST 6 7 am: 6C 1

2

» E / P RLX 1 3 0 » 160 0635 MAG-D 51 66SU1 58 1 1 D G ABX 16- 2 1 D 1- 6 NAI-D DST 71BU2 6C 1 2 . E/P ABX 5- 85 D500 MAG-0 51 66Z 1 1 56 1 1 D G A6X 15- 18 D 1- 2 NAI-D OST PROT P=25 100 MEV/C

71BAi. 56 1

1

D A6X 16- 20 D 0- 4 NAI-D DST 58BA2 6C ]^ 2 E * N RLY 2 4

— 145 C 24-145 ACT-I 4PI 67PA3 56 1 1 A G A6X 9- 1 1 D 1- 4 NAI-D 90 COMPARED WITH G>N

59BA3 6C 1 2 N A6Y T H R — 36 D 10- 36 6F3-I 4PI 65HE 1 I 2 RLY 32 D 14- 32 ACT-I 4PI

7 1 VO 1 6C 1 2 ABX THR — 266 C150-265 TOF-0 90 72KU6 6C ^ ^ M ABX 19- 30 0 20- 30 ACT-I 4PI CAR60N Z = 5 E+/E- YIELD RATIO

65HE 1 6C 1 2 E + N RLY T HR- 32 D 14- 32 ACT-I 4PI

6 1 VAl 6C 1 2 p NOX 2 0 — 40 C 24. 40 MAG-D DST

A A6UND. ( 1

)

SEPARATION ENERGIES IMEV) 64CH 1 6C 1 2 E ABX 0999 MAG-0 DST

G .N G. P G ,T G.HE3 G.A G.2N G.NP G.2P 999=4 GEV

12 98. 39 18 . 7 16.0 27 .4 26.3 7,4 31.8 27.4 27.2 6 9 AN3 1

2

RLY T HR — 999 C400-999 MAG-D DST

13 1. 11 h , 9 17. 5 23.9 24.4 10.6 23.7 20.9 31.6 999=1 GEV, REL D/T 70AN5 6C 1 2 . P RLY 9 6- 999 C620,999 TEL-0 DST 999=1140 MEV NUCLIDE REACT I ON RES EXCI T SOURCE DETECTOR 62D01 6C 1

2

XP SPC 2 5- 30 C 25- 30 MAG-D DST

REF Z A I N OUT TYPE ANG NUM 70 V Y 1 xP ABX 200 0100-200 MAG-D DST

7 ISHl 6C 1 2 . XP SPC 16- 29 0 43 MAG-0 DST

6 IJ A2 6C 1 1 P G NOX 10 D 0- NAI-D 90 69AN6 6C 1

2

E . 0 RLY THR- 999 C400-999 MAG-D DST

J-PI » G-WIDTH 1.3 GEV REL P/0,0/T

620P2 5C 1 1 P G ABX 11- 14 D 2- NAI-D 0 72SK7 6C 1

2

. D ABX 40 - 60 0 40- 60 MAG-0 DST 70KU1 6C 1 1 P G ABX 11- 24 D 2- 17 NAI-D DST 255 69AN8 6C 1

2

E T RLY Tt- R- 999 C40--999 MAG-0 OST 999=1 GEV, REL 0/T 55FR1 6C 12 E E/ ABX 4- 10 D 80-187 MAG-D DST 68B02 6C 1 2 XXX RLY T H R - 110 DllO MAG-0 76 LEVELS 4.4*7.7. 9.

6

XXX=MASS SPECTRUM

56FR1 5C 12 E E/ ABX 0- 35 D187 MAG-D DST 56T22 6C 1 2 MU — J LFT 2 3 C 22- 23 ACT-I 4PI J-PI 59K-0

1

6 C 1 2 G T ABX 15 — 30 C 31 NAI-D 4PI 59BA1 6C 12 E E/ A6 I 0- 30 D 43 MAG-D 160 60 T A2 mm" ABX 32 C 11- 32 MAG-0 4PI

60BA<t 6C 12 E E/ SPC 0- 30 D 42 MAG-D DST 60WY 1 6C 1 2 y ABX 13 — 83 C 35- 90 NAI-D 4P1

ABI » MULT I POLAR i TY 60Z I 1 1

2

Ml! ABX 1 0 — 30 C 32 MGP-D 4PI 61604 5C 12 E E/ SPC 0- 164 D194 MAG-D 135 6 3BU 1 6 C 1 2 MU j ABX 1 3 — 27 C 13- 27 MGP-D 4PI 61Du: 6C 12 E E/ ABX 13- 18 D 46-154 MAG-D 135 6 3BU3 1

2

MU ABX 13 — 27 C220 MGP-D 4PI 52E01 6C 12 E E/ ABI 15 D 42 MAG-D 180 65vJYi 6C 1

2

MU— ABX 10- 35 C 90 SCI-D 4PI

G WIDTH. J-PI 69BE2 6C 1

2

y ABX 10 — 30 C 35 MGC-0 4PI

6 3 BO 3 6C 12 E E/ ABX 4- 25 D200 MAG-D 135 71AH1 6C 1

2

MU- J ABX THR - 150 C 10-150 MGC-0 4PI

53GO<t 6C 12 E E/ ABX 0- 30 D 42 MAG-D 180 57HA1 6C 1 2 (3 (5 ABX 0

- 19 C 19 NAI-D 120 63LE1 6C 12 E £/ FMF 0- 35 D 55 MAG-D 180 58RA1 6C 1

2

(3 LFT D 4 NAI-D OST Q-RANGE 0-1 59GA1 6C 1 2 (3 (3 LFT 1 5 C 19- 42 NAI-D DST

6'iBR2 6C 12 E E/ SPC 0- 20 D 54 MAG-D 141 15.1 MEV LEVEL

6'tCRl 6C 12 E E/ ABX 4- 10 D250 MAG-D OST 59PA3 G G ABX 0 15, 18 NAI-D 90

W I DTHS 59PE5 6C 1 C G G ABX 1 Q

1 ^ 61 C 19- 61 NAI-D 135 64G02 5C 12 E E/ ABX 10- 32 D 40- 70 MAG-D DST 60 BU3 6C 1 2 LFT C 23 NAI-D DST

FMF 15=15.1 MEV 6AG03 5C 12 E E/ A6X 15 0 40- 70 MAG-D 160 60HA2 6C 1 2 G G ABX 1 5 0 15, 17 NAI-D 90 FMF 60 JAl 6C 12 $ G NOX 0

— 15 C 25 NAI-D DST

6'tGUl 6C 12 E E/ FMF 15 D NAI-D DST J-P I . MULT I POLAR I TY 0=0.2-0.5. WIDTH 6 1 BU3 6C 1 2 G G ABX 19 — 36 C 32 NAI-D 140 66AR2 6C 12 E E/ LFT 4 0 MAG-D 4PI SEE 51BU4 4=4.43 MEV 6 1 W I 1 6C 1 2 ABX 120 C132 SCI-0 DST 66CR1 6C 12 E E/ FMF 4 > 10 D600-800 MAG-D DST 62SE 1 6 C 1 2 (3 SPC 0- 19 C 19 NAI-D 90 4.10=4.43.9.6 MEV 63SC3 6C 1 2 ABX 1 5 D 15, 18 NAI-D DST 66PR1 6C 12 E E/ NOX 14- 21 DlOO-200 MAG-D 180 6-WDTH

67AF 1 6C 12 E E/ RLX 0- 100 D846 MAG-D DST 67KU2 6C 12 G G LFT 15 0 16 NAI-D 135 67BE3 5C 12 E .E/ ABX 4 D113-390 MAG-D DST 15=15.1 MEV 4=4.43 MEV 70AH1 6C 12 G G ABX 15- 80 C108 NAI-D 135 67L01 6C 12 G G/ ABX 18- 34 C 34 NAI-D DST

52 + 105 +

20
NUCLIDE REACTION RES EXCIT SOURCE DETECTOR NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF z A I N »OUT TYPE ANG NUM REF Z A I N OUT TYPE ANG

55BA1 6C 12 G t N ABX 18- 36 C 18- 260 ACT-I 4P I 69CA3 6C 1 2 G P ABX 70- 27 D 32 TEL-D DST 55SP2 6C 1 2 G > N RLY THR- 20 C 17- 20 ACT-I 4P I GROUND STATE BREAKS 69MA3 6C 1 2 G P ABX 36- 80 C 50- 80 TfcL-D 45 56TZ 1 6C 12 G iN RLY 22- 24 C 22- 24 ACT-I 4PI 69TA1 5C 12 G P ABX 16- 60 C170 CCH-D DST

5 7BA

1

6C 1

2

G »N ABY 30- 260 C120- 250 THR- I DST XXX=CHRGD PARTCLES

57CA2 6C 1

2

(3 »

N

ABX 20- 3 1 C 20- 31 ACT-I 4P I 7UT02 6C 12 J G p NOX 680- 840 C700-930 MAG-D 41 58BA2 6C 1 2 »N RLY 24- 145 0 24- 145 ACT-I 4P I P-POLARI ZAT ION COMPARED WITH E.N 71AN1 6C 1 2 G P SPC 49-999 C700,999 TEL-D DST 59C01 6C 1

2

(3 N ABX 20- 2 1 ACT-I 4P I 999=1.2 GEV. REL D/P 59SA1 6C 12 G N NOX 19- 2 1 C 18- 21 MODI

4P I 71G01 6C 12 I G P NOX 15- 800 C550-800 MAG-D UKN BREAKS POLARIZED PROTONS

59SA1 6C 1 2 G N NOX THR- 19 C 18- 19 ACT-I 4PI 66MA2 6C 12 G PG/ RLX 21- 3 1 C 21- 31 NAI-D UKN BREAKS 70ME4 6C 1 2 G PG/ ABY 18- 42 C 24- 42 SCO-D 112 60EM2 6C 12 G N SPC 20- 30 C 30 EMU-D DST 67TA1 6C 12 G 2P AB I THR- 170 C170 CCH-I 4P I 5UGE2 6C 12 G N RLY 19- 20 C 19 20 ACT-I 4P I 58TA1 6C 12 G 3P ABX 100- 320 ClOO-320 ACT-I 4P I THRESHOLD LI-9 N BY BF3 60GE3 6C 12 G N NOX THR CTHR BF3-I 4P I 56C01 6C 12 G XP ABY THR- 24 C 24 EMU-D 90 THRESHOLD 57CH1 6C 1

2

G XP SPC THR- 84 C 64, 84 EMU-D DST

6 1R02 6C 1 2 G N ABX 19- 23 C 19- 23 ACT-I 4P I 57L I 1 6C 1 2 G XP SPC THR- 3 5 C 35 EMU-D DST

6 2 803 6C 1

2

(3 N ABX 18- 90 C 18- 90 ACT-I 4P I 58CH1 6C 12 G XP SPC THR- 44 C 30, 44 EMU-D DST 52DE 1 6C 12 G N ADX 20- 2 1 D 20- 21 ACT-I 4P I 59BA2 6C 12 G XP SPC THR- 89 C 82, 89 TEL-D 90 62FI2 6C 12 G N RLX 2 1- 29 C 25- 32 TOF-D UKN 59CH1 6C 12 G XP RLY THR- 80 C 80 TEL-D 90 62FU5 6C 12 G N ABX 21- 31 C 31 SCI-D 90 REL D TO P YLD 62MI2 6C 12 G N ABX 18- 26 D 18- 26 BF3-I 4P I 59PE4 6C 12 G XP ABX 22- 52 C 22- 90 SCI-D DST 64BE6 6C 12 I G N NOX THR- 32 C 32 SC I-D DST 60BA1 6C 12 G XP ABY THR- 90 C 30, 90 TEL-D 58 NEUT POLARIZATION 50CH1 6C 1 2 G XP RLY THR- 90 C 90 TEL-I DST 65VE1 6C 12 G N SPC THR- 33 C 34 TOF-0 DST REL TO DEUTERONS

66BA4 6C 12 G N ABX THR- 52 C 18- 52 BF3-I 4P I 61CE1 6C 1 2 G XP ABX THR- 342 D245-342 TEL-D 60 66C02 5C 12 G N ABX THR- 65 CTHR- 70 ACT-I 4PI 111 6 IVA 1 6C 12 G XP NOX 20- 40 C 24, 40 MAG-D DST 66F0

1

6C 1 2 N ABX 18- 70 C 18- 70 ACT-I 4P I 62CH2 6C 12 G XP RLY THR- 9 0 C 90 TEL-D DST 66FU1 6C 1 2 G N ax 18- 37 D 18- 37 BF3-I 4PI 112 REL TO DEUTERONS

56L01 6C 12 G N ABX 2 1- 27 0 21- 27 ACT- I 4PI 6 2HE

1

6C 1 2 G XP SPC 19- C 31 SCD-D UKN 66M I 2 6C 1 2 G N ABX 18- 26 D 18- 26 6F3-I 4PI 62L 1

1

6C 12 S G XP RLY THR- 33 5 C335 TEL-0 DST 67AN1 6C 1 2 G N RLY THR- 999 CTHR- 999 ACT-I 4P I PROTONS POLARIZED

67D I 2 6C 1 2 G N ADY 18- 999 C300- 999 ACT-I 4P I 62PA1 5C 1 2 G XP ABY THR- 150 C150 SCI-O 60 999=1 GEV 63FI4 6C 12 G XP SPC 19- 30 C 31 SCI-D 90 67DI 3 6C 1 2 G N ABX 300-999 C30U-999 ACT-I 4P I SPECTRUM

999=1 GEV 63KI1 6C 12 G XP ABY THR- 335 C335 TEL-D DST 67GE2 6C 1 2 (3 N ABY THR- 2 7 C 22. 27 BF3-I 4PI 63MU1 6C 12 G XP ABY THR- 24 C 24 SCD-D 120

67 JO 1 6C 1 2 N ABX 19- 20 D 19- 20 ACT-I 4P I 63WA2 6C 12 G XP RLY THR- 55 C 55 SCI-O DST 67TA1 6C 1 2 C3 N AB I THR- 170 C170 CCH-I 4P I 54SE1 6C 12 G XP SPC THR- 24 C 24 EMU-D DST 68KA1 6C 1

2

N ABX 50- 85 C 55, 85 TOF-D 67 68FR3 6C 1 2 G XP RLX 20- 38 C 38 TEL-D 90 NEUT ENGY SPEC 38=37.7 MEV

68WU 1 6C \ 2 N ABX THR- 4 0 C 20- 40 TOF-D 90 222 + 64K I 1 6C 1 2 G D ABY 80- 800 C400-800 TOF-D 57 69DE 1 6C 1

2

N ABY THR- 999 C 1- 6 ACT-I 4P I 65K I 2 6C 12 G 0 ABY 70-720 D400-720 MAG-D 57 999=5.5 GEV 69ANb 6C 12 G D ABY 219-999 C400,999 MAG-D 30 69DE4 6C 1 2 G NOX 19- 260 C260 ACT-I DST 999=1.4 GEV

Cll RECOIL DST 69AN6 6C 12 G 0 ABY 115- 999 C700,999 TEL-D DST 70HY1 6C 12 G N ABX 200-999 ClOO- 999 ACT-I 4PI 999=1.2 GEV 999=1050 MEV 71AN1 6C 12 G 0 SPC 55- 999 C700,999 TEL-D DST 70KA2 6C 12 G N ABX 18- 100 C 20. 140 ACT-I 4P 1 999=1.2 GEV. REL D/P 71IS3 6C 12 G N ABX 19- 25 C 19- 25 BF3-I 4P I 412 72AN3 5C 12 G 0 RLY 105- 999 C700,999 MAG-0 DST 71SA1 6C 12 G N ABY 18- 68 C 10- 68 ACT-I 4P I 999=1.2 GEV

56MA2 6C 12 G NG/ RLX 21- 31 C 21- 31 NAI-D UKN 59CH1 6C 12 G XD RLY TFR- 80 C 80 TEL-D 90

70ME'. 6C 12 G NG/ ABY 21- 42 C 24- 42 SCD-D 112 REL 0 T3 P YLD

590CL 6C 1 2 G 2N RL I THR- 100 CTHR- 100 ACT-I 4P 1 6 OC H

1

6C ^ 2 G XD RLX THR- 90 C 90 TEL-I DST REL TO G,N REL TO PROTONS

70KA2 6C 12 G 2N ABX 30- 556 C 35- 130 ACT-I 4P I 62CH2 6C 12 G XD RLY THR- 90 C 90 TEL-D DST 55BA5 6C 12 G XN ABY 30- 200 C150- 250 THR-I DST REL TO PROTONS

55DI 1 6C 12 G XN NOX THR- 70 C 70 SCI-I DST 71AN2 5C 12 G XD ABX 115- 999 C520,999 MAG-D DST 56FA1 6C 12 G XN NOX THR- 23 C 23 SCI-I DST 999=1.14 GEV

57C01 6C 12 G XN ABX 19- 41 C 19- 40 BF3-I 4P I 67KR2 6C 12 G T RLX THR- 55 C 30- 55 ACT-I 4P I SBBAl 6C 12 G XN ABY THR- 255 C170. 255 THR-I DST 72AN3 6C 1 2 G T SPC 107- 999 C700>999 MAG-0 DST 58BA5 6C 1 2 G XN RLY THR- 23 C 18- 23 BF3-I 4P I 999=1.2 GEV BREAKS 67TA1 6C 1

2

G HE3 AB I THR- 170 C170 CCH-I 4PI 59<U1 6C 1 2 G XN ABY THR- 88 C 88 TEL-D DST 55GL 1 6C 1 2 G A SPC 1 7 D 14, 17 EMU-D 4P I 61PR1 6C 12 G XN RLY 30- 85 C 30- 85 THR- I 4P I 70MU1 6C 12 G A ABX 1 2- 32 C 32 EMU-0 4P I 62M I 2 6C 1

2

G XN ABX 18- 26 D 18- 26 BF3-I 4P I 55CA2 6C 1

2

G 3A ABX 1 2- 18 D 16, 18 EMU-D 4P I 63C03 6C 1 2 G XN ABX THR- 80 CTHR- 80 BF3-I 4P I 55CA2 6C 12 G 3A ABX 1 2- 18 0 15, 18 ION-0 4PI 63FU1 6C 12 G XN ABX 20- 29 t 31 SCI-D 90 55G01 6C 1 2 G 3A SPC THR- 60 C 60 EMU-D DST SPECTRUM 55HA1 6C 12 G 3A RLY 9- 33 C 27, 33 EMU-D DST 64AL5 6C 1 2 G XN NOX THR- 34 C 34 THR-I OST 5 7MI,'l 6C 1 2 G 3A SPC 1 5 , 18 0 15, 18 EMU-D DST 65BA1 6C 12 G XN ABX THR- 52 C 16- 52 BF3- I 4PI 5 8MAI 6C 1 2 G 3A ABX 12- 40 C150,250 EMU-D 4P I 65M I 1 6C 1 2 G XN ABX THR- 30 CTHR- 30 BF3-I 4P I 60GA 2 6C 1 2 G 3A ABX 15, 18 D 15, 18 EMU-I UKN

66BI 1 6C 1 2 G XN ABX 20- 200 C 20- 200 BF3-I 4P I 61SE3 6C 12 G 3 A RLY 18 D 18 EMU-D API 66FI2 6C I 2 G XN SPC THR- 65 C 65 TOF-D 90 6 3SH2 6C 1 2 G 3A NOX 8- 70 C 70 EMU-D 4PI 67FE2 6C 12 G XN ABX 100- 150 C150 BF3-I 4P I Q-VALUE DISTRIB

68RA2 6C 1 2 G XN SPC THR- 103 C103 TOF-D DST 64GR1 6C 12 G 3A ABY 7- 24 C 17- 24 EMU-I 4P I 698A1 6C 12 G XN ABX 1 9- 25 C 19- 25 BF3-I 4P I 314 64T01 6C 1 2 G 3A ABX 9- 22 C 22 EMU-D DST 71C02 6C 1 2 G XN AB I 36- 64 C 10- 64 8F3-I 4P I SPECTRUM

FAST N YIELD 6 4 W A 1 6C 1 2 G 3 A ABX 1

8

D 17 SCI-D 4P 1 71M 11 6C 1 2 G XN ABX 70- 90 C 64- 128 TOF-D OST 18=17.5 MEV

72VA2 6C 12 G XN ABX 18- 32 C 18- 32 BF3-I 4P I 55R01 6C 12 G 3A ABX 12- 17 C 12- 17 EMU-D 4P I 55 JOl 6C 1 2 G p RLY THR- 65 C 65 SCI-D DST 58WH2 6C 12 G NP ABX THR- 110 C 40-110 TEL-D DST 56MA1 6C 12 G P ABX 1

8

D 18 EMU-D 4P I COINC WITH BF3 59BA2 6C 1 2 G P SPC 34- 89 C 82. 89 SCI-D 90 60ST1 6C 12 G NP RLX 157- 320 C320 TEL-D 75

61 THl 6C 1 2 G p AB I 18- 2 3 C 18- 23 ACT-I 4P I REL TO H2 CROS SEC

18 BREAKS 64TA3 6C 1 2 G NP SPC THR- 100 C170 CCH-D 4P I 64SH4 6C 1 2 G p ABX 2 0- 2 3 D 20- 23 SCI-D 4P I 67SM1 6C 1 2 G NP ABX 150- 250 C250 TOF-D DST WIDTHS 57TA1 6C 1 2 G NP AB I THR- 170 C170 CCH-I 4P I 64TA3 6C 1 2 G P SPC THR- 100 C170 CCH-D 4P I 68TA1 6C 12 G NP ABX THR- 170 C170 CCH-I OST 65< I 2 6C 12 G P ABY 88- 720 D400- 720 MAG-D 57 6 8 T A

1

6C 1 2 G NPA ABX THR- 170 C170 CCH-I OST 66<E1 6C 12 i G P ABX 21- 22 D 21- 22 EMU-D OST 67TA1 6C 1 2 G NHE3 AB I THR- 170 C170 CCH-I 4P I 66PA2 6C 12 G P SPC THR- 55 C 55 SCI-O DST 68TA1 6C 1 2 G NHE3 ABX THR- 170 C170 CCH-I DST 67TA1 6C 12 G p ABX THR- 170 C170 CCH-I DST 67TA1 6C 12 G NA AB I THR- 170 C170 CCH-I 4P I 6eFR2 6C 12 G P RLX THR- 32 C 30, 32 TEL-D DST 68TA1 6C 1 2 G NA ABX THR- 170 C170 CCH-I DST tSMAl 6C 12 G P ABX 100 C 95- 102 TEL-D DST 690W2 6C 12 G NA ABX 25- 31 C 25- 71 ACT-I 4P I 68WA2 6C 12 G P RLX 50- 80 C 50- 80 TEL-I 45 58MA1 6C 12 G PT ABX 27- 70 C150,250 EMU-D 4PI 69AN5 6C 12 G P ABY 113- 999 C400 999 MAG-D 30 68TA1 6C 12 G PT ABX THR- 170 C170 CCH-I DST 999= 1.4 GEV 69AN6 6C 12 G P ABY 114- 999 C700, 999 TEL-D DST

21
NUCL 1 OE REACT 1 ON RES EXCI T SOURCE DETECTOR NUCLI DE REACTION RES EXCIT SOURCE DETECTOR

REF Z A I N OUT TYPE ANG NUM REF Z A I N OUT TYPE ANG

55L I 1 6C 1 2 G PA A8X 30- 50 C 25- 70 EMU-I UKN 52ED1 7N 14 E E/ ABX 0- 1

0

D 42 TEL-D 180 58MA1 6C 12 G PA ABX 2 5- 80 Cl 50 . 250 EMU-D 4P

I

63BA1 7N 1 4 E E/ ABX 0- 18 D 42 MAG-0 180

6 2 MO 2 6C 1 2 G PA AB I 2 5- 120 C120 EMU-D 4P

I

G-WDTH

67TA1 6C 1 2 G PA AB I THR- 170 C170 CCH-I 4PI 64BI 1 7N 14 E E/ ABX 0- 8 D120 , 180 MAG-D DST 68TA1 6C 1

2

(3 PA ABX THR- 170 C 1 70 CCH-I DST FORM FACTORS

66AR I 6C 1 2 G BE7 ABX 30- 57 C 30- 57 ACT-I 4PI 66K01 7N 14 E E/ ABX 8- 14 D 50. 50 MAG-D 180 6701 2 6C 12 G BE7 ABY THR- 999 C300-999 ACT-I 4P

I

5 LEVELS

999=1 GEV 68CL1 7N 1 4 E E/ LFT 8- 1 2 0 35- 5 8 MAG-D DST

6 7D I 3 6C 1 2 (3 BE7 ABX 300- 999 C300- 999 ACT-I 4PI 9 , 17, 999=1 GEV 60CA1 7N 1 4 (3 MU-T ABX 7- 2 1 D 20- NAT— n ZiPT

6 7 T A

1

6C I 2 SPL AB I THR- 170 C170 CCH-I 4PI 6 2G0

1

7N 1 4 (3 MU-T AB I 0- 170 C 1 70 LCH— D 4K

1

6itMA4 6C 1

2

XXX ABY 150- 72 0 C150- 720 ACT-I 4PI 69BE2 7N ABX 10 — 3 0 C 3 5 MGL — U 4r

1

XXX=C11 FINAL 6 ISW

1

7N 1 4 G G LFT 2 0 2 NAI-D DST 69TA1 6C 12 G XXX ABX 1 6- 60 C170 CCH-D 4PI 64B0

1

7N 1 4 (3 G LFT \ ~ 3 C 1 - MAT ri 1 n N A 1 U i U U XXX=CHRGD PARTCLES

71GR2 6C 12 G PI- ABY 150- 560 C560 EMU-D DST 66SW1 7N 1

4

(3 G LFT 7 D 7 NAI-D DST PI-/PI+ YIELD RATIO 7-7.11 /— i.ii MFV 'lev 71002 6C 12 G p 1 + RLY 160- 500 C500 CCH-D DST 67L01 7 N 1 4 G/ ABX 18 — 3 2 C 3 4 NA 1 -0 DST

PI -/P I* YIELD RAT 10 70TH1 7N 1 4 (3 XG ABX T HR- 2 9 C 2 9 SCO— D 125 71GR2 6C 1 2 G p I + ABY 150- 560 C560 EMU-D DST 59 MU

1

7N 1 4 (3 N RLY 11 — ^ 7 C 11- 17 ACT-I 4PI PI-/PI+ YIELD RATIO 60FA1 7N 1 4 (3 N ABX 11- 6 1 C 13- 51 BF3-I 4PI 59GE1 6C 12 p G ABX 19- 23 C 4- NAI-0 90 60GE 1 7N 1 4 (3 N RLX 10- 1 2 C 10- 12 ACT-I 4PI 59G01 6C 12 P G RLX 19- 26 D 3- 11 NAI-D DST 60GE2 7N 1 4 G * N RLY 10- 1

1

C 10- 11 AC T- I 4P I 6 IGOl 6C 12 P G ABX 19- 27 0 3- 11 NAI-D DST E - THR E SHOLO

G.P ABI BY DT BAL 60K I 2 7N 1 4 6 • N ABX 10- 2 5 C 10- 25 ACT-I 4PI

6 1SE2 6C 12 p G RLY 16 D 0 NAI-I 90 60MU1 7N 1 4 (3 »N RLY THR- 20 C 15- 20 ACT-I 4P

I

G-WDTH, MULTIPOLAR RRFac w Krv oS 638E5 6C 12 P G RLY 2 1- 28 0 6- 13 NAI-I 90 1 4 N 10 — 1 3 C 10- 13 ACT— I 4PI 53RE1 6C 12 P G ABX 30- 39 D 15- 25 NAI-0 90 62G01 7N 14 G * N AB I 11- 170 C170 CCH-D 4P

I

AB I BY DETAIL BAL 6 2K02 7N 1 4 (3 »

N

ABX 11- 90 C 90 rru-n ^ ^ n \j nST \j ^ \ 64AL2 6C 12 P G ABX 19- 29 D 4- 14 NAI-0 DST 225 68KA1 7N 14 G )N ABX 50- 85 C 55. 85 TOF-D 67 64AL3 6C 12 P G NOX 20- 30 D 4- 14 NAI-D DST NEUT ENGY SPEC 64HA3 5C 12 P G ABX 17- 20 0 1- 4 NAI-I DST 71FR1 7N 14 G N ABY 10- 800 ClOO- 800 ACT-I 4P1 55SEI 6C 12 P G ABX 16- 20 D 0- 4 NAI-D DST 71SA1 7N 1 4 G N ABY 1 0- 68 C 10- 68 ACT-I 4PI 67FE1 6C 12 P G ABX 25- 30 D 10- 15 NAI-D 90 72&E3 7N 14 G N ABX 10- 30 C 15- 30 TOF-D 90 69KE1 6C 12 P 6 ABX 28- 37 D 13- 21 NAI-D DST 227 + 590C1 7N 1 4 G 2N RL I THR- 100 CTHR- 100 ACT-I 4P

I

72BR4 6C 12 P G ABX 29- 35 D 14- 24 NAI-D DST REL TO G.N

72611 6C 12 S P 6 ABX 16- 30 0 6- 14 NAI-0 DST 60BA7 7N 1 4 XN RLX THR- 200 C200 ^ ^ n— L> O 1 POLARIZED PROTONS 53FU2 7N 1 4 G XN SPC 10- 30 C 31 SC I -D 90 64BL1 6C 1 2 HE G ABX 28 D 2- NAI-D 90 70BE8 7N 1 4 G XN ABX 10- 30 0 10- 30 BF 3 — I 4P

I

HE=HE3 56WR1 7N 1 4 G p ABX 7- 23 C 19- 23 CCH-D 4P

I

72BL6 6C 1

2

(3 ABX 2 6- 32 D 1- 6 NAI-0 DST 57L I 1 7N 1 4 G p SPC T HR - 70 C 30 . 70 EMU-D

HE=HE3

.

G-WIDTH. J-P 58CQ2 7N 1 4 G P NOX 7- 30 C 18- 30 EMU-D 90 67PE1 6C 1 3 LFT 1 5 D 40- 65 MAG-D DST 58GR1 7N 1 4 G P LFT 8 0 8 lON-D 4P I 15=15.11 MEV 50BA7 7N 1 4 G p RLX THR- 200 C200 CCH-D DST 69CA1 6C 1 3 E E / SPC 0- 20 D140 MAG-D DST 6 0 KOI 7N 1 4 G p AB I THR- 90 C 90 CCH-D DST 69T01 6C 1 3 E / FMF 3 D 34- 65 MAG-D DST 60WA1 7N 1 4 G p SPC 8- 1

6

C 12, 16 EMU-O DST 3=3.08 MEV 62G01 7N 14 G P AB I 7- 1 70 C170 CCH-D 4PI 69W I 2 6C 1 3 E E/ LFT 3- 15 0 35- 55 MAG-D DST 5 7L I 1 7N 14 G XP SPC THR- 70 C 30 . 70 EMU-D DST

7 LEVELS 60RE2 7N 14 G XP C330 CCH-D 4PI 70W 1 1 6C 13 E E/ LFT 3- 15 D 35- 55 MA6-0 DST 63F 14 7N 14 G XP SPC 0- 3 1 C 31 SCI-D 90

9 LEVELS 64K01 7N 14 G XP SPC THR- 31 C 16- 31 SCI-D 90 71BE2 6C 13 E E/ FMF 8- 44 D 77- 106 MAG-D DST ABX 71YA1 6C 1 3 E E/ FMF 3- 20 D 40- 125 MAG-D DST 56WR1 7N 14 G A ABX 12- 2 3 C 19- 23 CCH-D 4PI

10 LEVELS 5 2 GO 1 AB I 12 — C170 CCH-D 4PI

7 1 SH

1

6C ^ 3 p SPC 18 — 31 D 43 MAG-D DST 6 4 T02 7N 14 ABX T HR — 2 2 C 22 EMU-D DST 69RA3 6C 1 3 G .G LFT 3 C 3 NAI-D DST 55WR1 7N 1 4 G 2A ABX 16- 23 C 19- 23 CCH-D 4PI 3=3.68 MEV 56W R 1 7N 1 4 G NP ABX 12- 2 3 C 19- 23 CCH-0 4PI 60ED1 6C 1 3 G .N ABX 6- 7 D 6- BF3-I 4PI 60BA7 7N 1 4 G NP RL I THR- 200 C200 CCH-D DST 640R2 6C 1 3 G • N ABX 6- 11 D 5- 11 BF3-I 4PI 60 KOI 7N 1 4 G NP SPC THR- 90 C 90 CCH-D DST 65BE2 6C 1 3 G *N ABX 6- 14 C 8- 14 TOF-D DST PROTON SPECTRUM

66FU3 6C 1 3 G »N RLY THR- 15 C 5- 15 BF3-I 4PI 6 2G01 7N 1 4 G NP AB I 12- 170 C170 CCH-D 4PI NSA 13943 BREAKS 62K02 7N 1 4 G NP ABX 15- 9 0 C 90 CCH-0 DST 70FU2 6C 1 3 Qi N ABX 5 - 14 C 5- 14 BF3-I 90 5 2 GO 1 12 AB I C170 CCH-D 4P1 70FU3 6C 1 3 (3 »N ABX 6- 14 C 5- 14 BF3-I DST 70 S H

1

7N Jf P N SPC 15 — 3 0 C 15- 30 TOF-D 90 71MU1 6C 1 3 Q »NG ABY 9- 28 C 21 . 28 SCD-D 90 DE -EXCIT. NEUTS

57C01 6C 1 3 G »XN ABX 6- 41 C 6- 40 BF3-I 4PI 297 56L I 1 7N 14 G PA ABX 2 5 — 50 C 25- 70 EMU-I UKN

6 1 SA2 6C 1 3 G » XN SPC 7- 14 C 14 TOF-D 79 55WR1 7N 1 4 G PA ABX 17- 2 3 C 19- 23 CCH-D 4PI 57C01 6C 1

3

(3 , p ABX 17- 45 C 17- 40 ACT-I 4P

I

62M02 7N 1 4 G PA AB I 18- 12 0 C120 EMU-D 4PI 64K02 6C 13 G .P SPC 20- 32 C 32 SCI-0 90 6 2 K02 7N 14 G NP3A RLY 20- 90 C 90 CCH-0 4PI SEPARATED ISOTOPES 60HE2 7N 14 P G ABX 8 D 0- NAI-0 DST 640E2 6C 1 3 G XP ABX 18- 50 C 18- 50 ACT-I 4PI 313 G-WDTH

50R01 7N 14 P G NOX 9 D 2 NAI-D DST

J-P I 60R02 7N 1 4 p G ABY 1

0

0 2- NAI-D DST

J-P I NITROGEN Z = 7 6 IHE 1 7N 1 4 p G ABX 8 D 0- NAI-0 0

6 ISE 1 7N 14 P G RLY 6 . 9 0 2 MGP-D DST

A ABUND. ( 1

)

SEPARATION ENERGIES (MEV) 63PR1 7N 1 4 p G NOX 9 D 2 J-PI NAI-D DST

G G. P G , T G.HE3 G. A G.2N G,NP G.2P G-WDTH, ^MPL RATIO

14 99. 53 10 .6 7. 6 22 . 7 20. 7 11. 6 30.6 12.5 25.1 55DE2 7N 14 P C LFT 9 D 2 NAI-D OST

15 0. 37 10.8 10.2 14 .8 28. 2 11. 0 21.4 18.4 31.0 71R I 1 7N 14 P G ABX 10- 24 D 3- 18 NAI-0 OST

51KN1 7N 1 4 G ABX 10- 1 2 0 0- 2 J-PI

THR-I 4PI NUCLIDE R EACTION RES EXCIT SOURCE DETECTOR 70BL1 7N 14 HE G ABX 21- 2 4 D 1- 3 NAI-D DST REF Z A IN .OUT TYPE ANG NUM HE=HE3

60HE2 7N 1 3 P .G ABX 2- 3 D 0- NAI-D DST 6 8 BE 1 7 N 1 5 £ / LFT D 50- 57 MAG-D DST 62PA2 7N 13 P .G ABX 8- 1 1 D 5- NAl-D 90 5=5.32 MEV

62WA1 7N 13 P .G ABX 15- 20 D 14- 20 NAI-0 90 70DA1 7 N I 5 £ / ABX 5 - 8 0250 , 400 MAG-0 DST 63F I 1 7N 1 3 P .6 ABX 11- 41 D 10- 49 NAI-D 90 266 + LEVELS 5 .3-7.56FMF

53Y02 7N 1 3 P .G ABX 2- 4 D 1- NAI-D DST 680 I 1 7N 13 P .G LFT 15 D 14- 15 NAI-D DST 15.07 MEV

68R 1 2 7N 13 P .G LFT 2 D 1 NAI-0 4PI 2=2.37 MEV

72HA1 7N 13 P .G ABX 10- 17 D 8- 17 NAI-D 90 5 46 72BE1 7N 1 3 HE .G ABX 25- 33 0 5- 15 NAI-D 90 HE=HE3

22
NUCLIDE REACTION RES EXCIT SOURCE DETECTOR NUCLIDE REACT I ON RES EXCI T SOURCE DETECTOR

REF A I N »0U T TYPE ANG NUM REF A I N .OUT TYPE ANG

58RH1 7N * P ABX 11- 2 5 C 19, 25 EMU-D DST 57SW1 80 1

6

G LFT 7 , j Q 7 , NAI-D DST 64K03 7N » P SPC 12- 3 1 C 19- 31 SCI-D 90 59P A3 80

It

G ASX ]_ -J 15, NAI-D 90 ABX 59PE 5 ABX 19- 61 Q 6 1 NA I -0 135

7 2DE4 7N 1 5 * P ABX 19- 39 C 19- 39 ThL-D 90 60RE 1 80 1 A G ABX D 7 NAI-D DST

63F I 3 7N 1 5 • XP SPC 13- 3 1 C 25, 31 SCI-D 90 6 2SE

1

80 1 6 G G NOX 7 C 16 NAI-D 90

AB I » SEP I SOTOPES 64L A5 60 RLX T HR — C 24 , 32 NAI-D DST 69S I 1 7N 1 3 p »C ABX 1 0 D 0- 1 NAl-D DST 64L03 80 1 A ABX 10 — c 10- 30 NAI-D 140 SOURCE 250-670 KEV 68EV 1 80 6 G LFT 6 »

fi D 6 , 8 SCD~D UKN

7 IKUl 7N 1 5 p * ABX 11" 1 3 D 1- 3 SCD-0 DST LEVELS 6.92* 7,12

72R A2 7 N p * RL Y 1 4 D 4 NAI-D 60 7 0 AH 1 80 1

6

G ABX 15 8 0 C108 NAI-D 135

-Pi, 13. 42 MEV LEVEL 5 9P E 5 80 1

6

G G / ABX 19 — 6 1 c 19- 61 NAI-D 135

7 2 WE 2 ABX 1 3 7 0 3- 8NAI-DDST 547 80 1 6 G G/ 19- 30 21- 31 j-p I 6 7LO

1

ABX 32 34 NAI — D DST

5 5CA

1

80 1 6 Q N ABX 1 7 Q 0 ACT-I 4PI 55PE1 60 1 6 (3 »

N

AB I 15- 2 3 c 1 6- 23 ACT-I 4P

I

57BA3 80 1 6 »

N

ABY 15- 1 8 c 1 5- 16 ACT-I 4PI BREAKS OXYGEN Z = 8 57CA2 60 1 6 ^ N ABX 16- 3 1 c 15- 30 ACT-I 4PI 57ER1 60 1 6 (3 N ABX 16- 3 2 c 16- 32 ACT-I 4PI

5 7SP2 RLX 2 5 G 14- 25 ACT-I 4PI

A ABUND, { 1

)

SEPARATION ENERGIES (MEV) 58BE

1

80 16 * RL Y 1 R~ 15- 17 ACT-I 4P! G.N G

»

P G ,T G»HE3 G,A G,2N G.NP G,2P THRESHOLD. BREAK

16 99. 76 15.7 12. 1 25.0 22. 3 7,2 28.9 23,0 22,3 59K t 1 80 1 6 . N AB I 15- 1 8 G 1 5- 19 ACT-I 4PI

17 3 .7 ( - 2 ) 4.1 13. 8 18 .6 18, 3 6.4 19.8 16.3 25.3 6RKS

18 0,20 8.0 15. 9 15 .8 25. D 6,2 12,2 21,8 29, 1 59M I 2 60 1 6 N NOX THR 30 c 30 EMU-D 90 59M 1 3 80 1

6

, N NOX 16- 3 1 c 31 EMU-D DST 59PE 3 80 16 G N NOX 16- c 16- 18 ACT-I 4PI

NUyCLIDE REACTION RES EXCI T SOURCE DE T ECTOR BRK5

REF A I N • OUT TYPE ANG NUM 59SA2 80 1 6 G N NOX THR- 22 c 15- 22 ACT-I 4PI BREAKS

59C02 80 1 b p »G ABX 19- 2 5 D 14- 20 NAI-O 90 60GE 1 G ABX 15 1 7 c 15- 17 ACT-I 4PI 61C01 80 1 ^? p »G ABX 19- 25 D 14- 20 NAI-D 90 60GE2 80 16 N NOX 15 — c 15- 17 ACT-I 4PI

6 3 BA 2 80 1 5 »G NOX D 1 NA I — D DST 60KU2 80 1 6 N RL Y THR — 90 c 90 TEL-I DST

6 3HE 1 80 1 5 p »

G

8 n 0— Nil—

n

60SA 1 80 16 G N NOX 15- 16 c 15- 16 ACT-I 4PI

80 1 5 p SPC 5 — D 1— 2 NAI-D DST BRKS

67EV1 80 1 5 p (3 LPT 9- 1 0 0 1- 3NAI-DDST 61 BRl 80 1 6 (3 N AB I 0 — 34 c 24 ACT-I 4PI 70KU 1 80 1 5 p »G ABX 11- 24 D 2- 19 NAI-D DST 246 + 6 IKE 1 80 16 G .N ABX 1 7- 18 D 17- 18 ACT-I 4PI 72PH1 80 1 5 p ABX 10- 1 3 D 3- 6 NAI-D 90 61R02 80 16 G N ABY 16- 22 c 22 ACT-I 4PI 626 14 80 1

6

N ABI 60- 150 c 60- 150 ACT-I 4PI

60 I SI 80 1 6 E/ RLX 2 0- 30 D 60-150 MAG-0 DST MULTIPOLARITY

611 SI 80 16 E / FMF 0- 115 D 90-215 MAG-D DST 6 2 BO 2 80 1 6 (3 N ABX 15, 30 c 15- 30 BF3-I 4PI 62BI 3 80 1 6 E E/ FMF 44 * 49 D150 MAG-D UK.N 6 2 BR 1 80 16 G N ABI THR- 32 c 32 ACT-I 4PI 62BI2 80 16 E E/ FMF 19 D14C-215 MAG-D DST 62DE 1 80 16 G .N ASX 20 D 20 ACT-I 4PI J-P I , MULT I POLE 6 2 F I 1 RLX c 31 TOF-D 90 62ED1 80 1

6

E E / NOX 0- 1

6

0 41 MAG-D 180 62F I 2 fin 1 A M RLX 2 9 c 26- 32 TOF-O UKN

63BA 1 80 1

6

ABX 1 9 D 41 M AG — D 18 0 6 2 F U5 an 1 A G

M ABX 21 — 3 1 c 31 SCI-D 90 63B 12 80 16 E E/ FMF 11- 1 4 D MAG-D DST 62G01 80 1 A N AB I C170 CCH-D 4PI

63 I SI 80 1 6 E E/ NOX 22- 26 ClOO-215 MAG-D DST 62G02 80 16 N ABX ^ 12~ ^75 C170 CCH-D DST 64BI2 80 1 6 E E/ ABX 0- 150 D 90-215 MAG-D DST 63AN

1

80 1 6 (3 N ASX 15- 60 C 1 5- 60 ACT-I 4PI SUM RULES 6 3C A

1

80 ABX 16 — 3 0 D 16- 30 8F3-I 4PI 64BI 3 80 1 6 E E/ ABX 6- 14 DlOO-218 MAG-D DST 63GE2 80 1 6 N ASX 15- 2 3 C 15- 23 ACT-I API FORM FACTORS 64BE8 80 1

6

J, (3 N NOX 17- 3 2 C 32 SCI-D DST 64G02 80 1 6 E £/ ABX 1 7- 32 D 40- 70 MAG-D 180 64BR1 80 1 6 (3 N ABX 15- 30 D 15- 30 BF3-I API FMF 64DE 3 80 ABX 0 17- 18 ACT-I 4PI 65VA4 80 1 6 E E / ABX 10- 30 D 43- 69 MAG-O 180 64T A4 80 1 6 N SPC 16- 2 6 D 34 TOF-D 90

66 AR2 80 1 6 ^ c/ L F T ^ * 1 2 D 30- 60 MAG— D DST 6 5GR

1

80 1 6 ABX C 10- 66 ACT-I 4PI 7=6.92, 12=11,52 6 5 V E

1

80 1

6

G N SPC THR~ 33 C 34 TOF-D DST 66CR 1 80 1 6 E E/ FMF 6 D600-800 MAG-D DST 66BA5 80 1 6 (J N ABX 15- 2 5 c 1 5- 25 ACT-I 4PI 6=6,1 MEV 66C0

1

80 1

6

N ABX THR- 6 5 CTHR- 70 ACT-I 4PI 66ST2 80 16 E E/ FMF 5- 14 KJ OU 1*1 MO U 11./ 66F I 1 80 16 i G N NOX THR- 70 C 10- 70 TOF-D DST 66M I 2 ASX 16 — 2 7 D 16- 27 BF3-I 4PI

66 V A 1 80 16 E E/ FMF 10- 30 <J H J 0 7 1*1 MU U lOU 67GE2 60 16 N ABY THR- 27 C 22. 27 BF3-I 4PI

6 7 DR 1 80 16 E £/ FMF 19- U 1 C. O 1*1 MO U UJl 68KA1 8 0 1 6 (3 N ABX 50- 8 5 C 55, 85 TOF-D 67 J-PI, 19,08 MEV NEUT EN6Y SPEC

68DR i 80 16 E E/ FMF 19, 20 DUO MAG-D DST 6 8 WU

1

6 0 16 N ABX T HR — 40 c 20- 40 TOF-O 90 19=19,1 ,20=20.5 69C03 60 1 6 $ G N NOX 20- 33 c 30 . 60 TOF-D DST 69S I 2 80 16 E E/ FMF 10- 30 DlOO-400 MAG-D DST N POLAR IZAT ION 69T02 80 16 E E/ FMF 7 D183.250 MAG-D DST 69 I VI 80 1 6 C3 N RLX 16- 2 2 c 16- 30 ACT-I 4PI 7=7.12 MEV 69KH1 80 1

6

N ABX 16- 3 3 c 22- 33 TOF-D 98 70BE 1 80 16 E E/ FMF 6- 8 D 51-105 MAG-D DST 69NA1 80 1 6 N ABX 3 5- 65 c 35- 65 TOF-D 68 6,05,6.13,6.91,7.1 70F I 1 80 ABX c 15- 120 ACT-I 4PI 70G01 80 16 E E/ LFT 19, 20 D 46. 54 MAG-0 DST 70 JU 1 80 1

6

N ABX 17~ 30 c 23- 30 TOF-D DST 19,04.20.36 MEV 7 IFRl 80 1

6

(3 N ABY 16- 300 cioo- 800 ACT-I 4PI 70GO4 80 16 E c/ FMF 21- 26 D 43- 58 MAG-D DST 7 1 S A 1 ABY 15 — c 10- 68 ACT-I 4PI 70KI 1 80 16 E E/ FMF 1 1- 14 D 40-105 MAG-D DST 57SV1 an 1 A6 Mr ABX 20 — c 16- 30 NAI-D 120 FMF 11,5-13.1 MEV INCL (G,P6) 70S T 1 80 16 E E/ LFT 14- 21 D 34- 58 MAG-0 DST 66FU2 80 1 6 (3 NG RL Y 20- 2 6 0 20- 26 BF3-I 4P! 62BI 4 80 16 E N ABY 60- 150 C 60-150 ACT-I 4PI COINC

MULT I POLAR I TY 660W 1 80 16 NG RL Y THR 29 c 20- 29 SCD-D 135 62D01 80 16 E P ABX 16- 27 C 30 MAG-D DST 249 + 660W2 60 1

6

(3 NG RLX T HR- 29 c 20- 29 SCD-D 135 58S I 3 80 16 G MU-T RLX 16- 25 C 15- 25 ACT-I 4P1 678A5 80 1

6

(3 NG SPC 2 1 — 26 c 26 SCD-D 135 59PE2 80 16 G MU-T ABX THR- 30 C 31 ACT-I 4PI 3-SPECTRUM

60CA1 80 16 G MU-T ABX 20- 21 D 20- 21 NAI-D 4PI 6 7MU 1 Nf SPC 21 — 3 0 c 28 , 30 SCD-D 90 60WY 1 80 16 G MU-T ABX 18- 35 C 90 NAI-D 4P

I

3-SPECTRUM

60Z I 1 80 16 G MU-T ABX 12- 26 C 30 MGP-D 4PI 69MU1 80 1

6

NG SPC 16 — 30 c 21- 30 SCD-D 90 62BU

1

80 16 G MU-T ABX 19- 27 C250 MGP-D 4PI 3~SPECTRUM

63BU 1 80 16 G MU-T ABX 12- 26 C250 MGP-D 4PI 69UL 1 80 16 NG ABY THR — 3 2 c 32 SCD-D 120 64TE L 80 16 G MU-T ABX 20- 22 D 20- 22 NAI-D 4P

1

70H0 1 80 1

6

^ NG RL Y 21- 2 7 c 27, 36 NAI-D DST WATER TARGET 7 1 ADl 60 1 6 G NG ABY 22- 800 cioo- 800 SCD-D 135

6 5 DO 3 80 16 G MU-T ABX 13- 22 C MGC-D 4PI 590C1 60 16 G 2N RL I THR- 100 CTHR- 100 ACT-I 4PI 65WY1 80 16 G MU-T ABX 10- 35 C 90 SCI-D 4P

I

50 + REL TO G.N

69BE2 80 16 G MU-T ABX 10- 30 C 35 MGC-O 4PI 108 62BR1 80 16 G 2N ABI THR- 32 C 32 ACT-I 4PI 71AH1 80 16 G MU-T ABX THR- 150 C 10-150 MGC-D 4PI 68ME4 80 16 G 2N ABX THR- 300 C 20- 300 ACT-I API 70FI 1 80 16 G 2N ABX 30- 115 30- 120 ACT-I API

23
REF NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

2 A IN. OUT TYPE ANG NUM NUCLIDE REACTION RES EXCIT SOURCE DETECTORREF 2 A IN. OUT TYPE ANG NUM

62M I 2 80 16 G XN ABX 15- 25 D 15- 25 BF3-I 4PI 55SC2 80 16 G NA ABY THR- 32 C 32 ACT- I 4P

I

6 3AU1 80 1

6

G XN SPC 20- 56 C 46. 55 TOF-D 90 6 2G0 1 80 1 6 G N A AB I THR- 170 C170 CCH-D 4P

I

63C03 80 16 G XN ABX 16- 75 C 16- 100 BF3-I 4PI 62K01 80 1 6 G PD RLY THR- 90 9 0 CCH- I 4P

I

6 3 FU

1

80 1 6 XN SPC THR- 3 I C 31 SCI-D 90 6 2K0 1 80 1 6 G ND RLY THR- 90 G 9 0 CCH- I 4P

I

64F I 1 80 1

6

XN SPC THR- 32 C 25- 32 TOF-O 70 65 AR3 80 1 6 G BE7 RLY 32- 57 (2 AC T- 1 4P

I

64Y E 1 80 1

6

XN SPC THR- 3 5 C 34 TOF-D 90 66 AR 1 80 1 6 G BE 7 ABX 3 0- 5 7 G 30 57 AC T — I 4P

I

BRANCHING RATIOS 6 7KR 2 80 1 6 G C 1

1

RLX THR- 5 5 G 30- 5 5 AC T- I 4P

I

64BA 3 80 1

6

G XN ABX 1 5- 2 8 C 15- 28 BF3-I 4PI 312 6 7ICR2 80 1 6 G N 1 3 RLX THR- 5 5 c 30- 55 AC T - I 4P

I

O/C YLD=1.7(22MEVI 59C02 80 1 6 p G ABX 21- 26 Q 14- 19 NA I - D 9 0 64BA 5 80 1 6 (3 XN ABX 15- 2 8 C 15- 28 BF3-I 4P

I

59 TA 1 80 1 6 p G ABX 16- 20 NA I -D 9 0

6 5C A 1 80 1 6 G XN ABX 17- 28 D 17- 2 8 BF 3- I 4P

I

38 + 60HE1 80 1 6 p G ABX 1 2 Q _ NA I -D UKN

6 1 COl 80 1 6 p G ABX 21- 26 Q 10- 1 5 N A I - D 9 0 65HA1 80 16 G XN ABX THR- 30 C 6- 30 8F3-I ^PI 61TA3 80 16 p G ABX 12- 2 6 0- 14 NA I -0 90 66F I 2 80 1 6 G XN SPC THR- 65 C 65 TOF-D 90 63G05 80 1 6 p G RLY 13- 1 7 D 1 - NAI-D UKN

67FE2 80 16 G XN ABX 100- 150 C150 BF3-I i*P\ 64EA 1 80 1 6 p G NOX 13- 2 5 D 1 - 1 3 NA I -D DST 67MI2 80 16 G XN SPC THR- 20 C 23- 27 TOF-0 100 64TA2 80 16 P G ABX 16- 26 D 4- 14 NAI-D DST 70IS5 80 16 G XN ABX 15- 25 C 15- 25 BF3-I 4PI 341 67BL2 80 1 6 P G RLX 21- 22 D 9- 12 NAI-D 45 72TH2 80 16 G XN ABX 15- 24 C 15- 24 BF3-I 4PI 67BL1 80 1 6 P G RLX 20- 30 Q 10- 18 NAI-D DST 55SP1 80 16 G P ABX lU- 18 c 19 EMU-0 DST 67EA1 80 16 P G ABX 13- 25 Q j — 14 NAI-D DST 55ST1 80 16 G P ABX 1*- 25 c 25 EMU-D DST 70BA 1 80 1 6 p G ABY 16- 24 Q 1 3 N A I - 0 9 0 55C01 80 16 G P ABX 18- 25 c 25 EMU-D 90 6 2SU2 80 1 6 0 G RLX 21- 2 5 I - NAI-D 90 56LI2 80 16 G P SPC 17- 70 c 30- 70 EMU-D DST 63SU2 80 1 6 D G ABX 21- 2 5 I - 1

1

NAI-D DST 57J01 80 16 G P ABX 12- 26 c 20- 26 EMU-D DST 6 3SU2 80 1 6 D G ABX 21- 2 5 D 1- it NAI-O DST 57SV1 80 16 G P ABX 20- 25 c 16- 30 NAI-D 120 64SU1 80 1 6 Q G ABX 24- 2 8

J

~ NAI-D DST G.PG 66SU 1 80 1 6 G ABX 2 1- 2 6 ^ NAI-D DST

58MI 1 80 16 G P ABX 15- 30 c 1 5- 30 EMU-D IOC 7 2WE 1 80 1 6 D G RLY 2 2- 2 4 D 2- 3 NAI-D 90 59BR2 80 16 G P NOX 2 3- 30 c 32 EMU-D DST 66PU1 80 16 HE RLX 23- 26 D 1 - 5 MAI r\ on 61F I 1 80 16 G P AB I THR- 35 c 35 SCI-D 90 HE=HE3

6 1 SH3 80 16 i G P SPC THR- 2 1 c 21 EMU-D DST 64LA2 80 1 6 A G ABX 10- 1 3 p 3 — NAI-D DST POLARIZED PHOTONS J- PI. WIDTHS

62G01 80 16 G P AB I THR- 170 C170 CCH-D 4PI 64M I 1 80 1 6 G RLX 1 3 0 7- NAI-D DST

6 2G02 80 16 G p ABX 12- 75 C 170 CCH-D DST J- PI. WIDTHS

6 3 SC

1

80 1 6 G 3

1

C 31 SCD-D UKN 67SU1 80 1 6 A G RLX 1 4- 25 0 8- 24 NAI-O DST 65M01 80 1 6 G p SPC ^15- 29 c 22 . 40 SCD-D 90 70 JA2 80 1 6 A G ABX 8- 1

1

D 1- 5 NAI-D UKN BRANCH RATIOS 70 J A 1 80 1 6 A G ABX 9- I I D 1- 4 NAI-D 84 65ST2 80 16 (3 p ABX 1 ^- 1 5 c 14- 16 SCD-D 90 70VO 1 go 1 6 A G NOX l 3 D 8 NAI-D DST 66DE4 80 1 6 G P AB I THR- 44 c 21- 44 TEL-D 90 13=13. 1 MEV 67K01 80 1 6 (3 p ABX THR- 5 5 c 21- 55 TEL-D 90 7 IKE 1 80 1 6 A G ABX 12- 1 4 D 7- 9 NAI-D DST

6 7 T HI 80 1

6

(3 p R L X 19- 26 c 20- 26 SCD-D DST 202

6 7TH2 80 1

6

(3 p R L X 20- 2 5 c 25 SCD-D 135 6 1 L Al 80 1 8 E E / FMF 2 - D150 MAG-D DST

6 7 TU3 80 1 6 (3 p SPC T HR- 2 2 D 22 EMU-D DST 6 5 VA2 80 1 8 E / ABX 2- 2 7 D 69 MAG-D 180

6 8 DE

1

go 1

6

(3 p ABX 16- 55 c 21- 55 TEL-D 90 7 1 GR

1

80 1 8 E / FMF 2 - D 92 . 106 MAG-D DST

6 8 S T

1

8 0 1

6

(3 p SPC 2 0- 2 6 c 26 SCD-D DST 7 LEVELS. eiEL) 26=25.6 MEV 64MU1 80 18 G N SPC 10- 20 C 20 EMU-D DST

6 8 TU

1

80 1 6 (3 p SPC 21. 2 2 D 21 . 22 EMU-D DST J ' P I . 2189 TRACKS

21=2 1.71.22=22.15 63FU2 80 I 8 G XN SPC 11- 3 1 C 31 SCI-D 90 69BA2 80 16 G P ABX 20- 30 C 25. 31 SCD-D DST 55RE1 80 1 8 G P ABI THR- 400 C 50- 400 ACT-I 4PI 69FR1 80 15 G P ABX 12- 33 C 12- 33 SCD-D DST 64K02 80 18 G P SPC 18- 32 c 32 SCI-D 90

69K.E3 80 15 G P SPC 16- 25 C 26 SCD-D 90 SEPARATED ISOTOPES

69SH3 80 15 G P RLX 12- 27 C 23. 27 EMU-0 DST 69H01 80 18 G XP ABY THR- 33 C 24- 33 SCD-D 90 69ST1 80 16 G P ABX 21- 33 C 33 SCD-D DST 194 56FU2 80 16 G PG RLY 20- 25 D 20- 26 BF3-I 4PI CO INC 560W 1 80 16 G PG RLY THR- 29 C 20- 29 SCD-D 135 560W2 80 16 G PG RLX THR- 29 C 20- 29 SCD-D 135 FLUORINE Z = 9 67BA5 80 16 G PG SPC 17- 26 C 25 SCD-D 135 G-SPECTRUM

67MU1 80 16 G PG SPC 17- 30 c 28. 30 SCD-D 90 A A8UN0 SEPARAT ION ENERGIES (MEV ) G-SPECTRUM G.N G.P G.T G.HE3 G.A G.2N G.NP G.2P

59MU1 80 15 G PG SPC 12- 30 C 21 - 30 SCD-D 90 19 100 .00 10.4 8. 0 11 .7 22. 1 4. 0 19.6 15.0

G -SPECTRUM

69UL1 80 15 G PG ABY THR- 32 C 32 SCD-D 120 70H01 80 15 G PG RLY 17- 27 C 27 . 35 NAI-D DST NUCLIDE REACT I UN RES EXCIT SOURCE DETECTOR

71AD1 80 16 G PG ABY 18- 800 ClOO -800 SCD-0 135 REF 2 A IN .OUT TYPE ANG

57BR1 80 16 G XP SPC 10- 19 C 28 EMU-D UKN

57MI 1 80 16 G XP NOX THR- 30 C 30 EMU-D DST 53SE1 9F 17 P .G RLY 4 D 3 NAI-D DST 51HE2 80 15 G- XP SPC 0- 35 C 35 SC I-D 90 J -PI. WIDTH

53FI4 80 16 G XP SPC 14- 30 C 31 SC I-D 90 55V01 80 16 G D ABX THR- 50 c 20 - 50 TEL-D 90 71C03 9F 18 A .G ABX 4- 5 D 0- 2 ACT-I 4PI 62BI4 80 16 G T ABY 50- 150 c 50 -150 ACT-I 4P 1 MULTIPOLARITY 63BA1 9F 19 E .E/ SPC 0- 15 0 42 MAG-D 180 65BU1 80 15 G T THR 50 c 50 ACT- I 4P I 70WA1 9F 19 E .E/ LFT 1- 2 D 30- 60 MAG-O DST 55SC2 80 15 G T ABY THR- 32 c 32 ACT-1 4P I 1 .56. 1 .35 MEV

56G02 80 16 G T ABX THR- 55 CTHR - 55 ACT-I 4P I 52D01 9F 19 E P SPC 10- 19 C 18- 30 MAG-D DST 57KR2 80 16 G T RLX THR- 55 C 30 - 55 ACT-I 4P I 66002 9F 19 G MU-T ABX 8- 30 C250 MGP-D 4PI 57J01 80 16 G A SPC 7- 19 C 19 EMU-D DST 54TE1 9F 19 G MU-T ABX 20- 21 D 20- 21 NAI-D 4PI 52G01 80 15 G A ABI THR- 170 C170 CCH-D 4P I 59BE2 9F 19 G MU-T ABX 10- 30 C 35 MGC-D 4PI 54GR1 80 15 G A ABY 7- 14 C 17 . 24 EMU-D 4PI SPC

5 0 BO 3 9F 19 G G LFT 1 C 0- NAI-D 100 J-PI 64T02 80 16 G A ABX THR- 22 c 22 EMU-D DST 50RE1 9F 19 G G ABX 7 D 7 NAI-D 90 64T03 80 16 G A ABX 9- 21 c 22 EMU-D DST 62B05 9F 19 G G LFT 0- 4 C 0- NAI-D DST 65R01 80 15 G A ABX 12- 1 7 c 12 - 17 EMU-O 4P 1 64B01 9F 19 G G LFT 1- 3 C 1 - NAI-D 100 65R02 80 16 G A RLY 17 c 17 EMU-D DST ABI 70V01 80 15 G A NOX 13 D 13 lON-D DST 64L03 9F 19 G G ABX 10- 30 C 10- 30 NAI-D 140

13 = 13.1 MEV 67L01 9F 19 G G/ ABX 14- 32 c 34 NAI-D DST 55HA1 80 15 G .4A NOX 20- 32 C 27 . 33 EMU-D DST 72SH2 9F 19 G G/ SPC 0- 14 c 14 SCD-D 87 56DA1 80 16 G 4A ABI 22- 25 C 70 EMU-D UKN 58BE1 9F 19 G N NOX 10- 1

1

c 10- 11 ACT-I 4PI 58MA1 80 16 G 4A ABX 20- 40 C150 .250 EMU-D 4PI THRESHOLD

64GR1 80 16 G 4A ABY 14- 24 C 24 EMUI4P I 50GE2 9F 19 G N NOX 10- 11 c 10- 11 ACT-I 4PI 54T02 80 16 G .4A ABX THR- 22 C 22 EMU-D DST THRESHOLD

64T03 80 15 G .4A ABX 9- 21 C 22 EMU-D DST 60KI4 9F 19 G N ABX 10- 23 c 10- 23 ACT-I 4PI 65R01 80 15 G .4A ABX 12- 17 C 12 - 17 EMU-D 4P I 60SA2 9F 19 G N RLY 10- 12 c 10- 12 ACT-I 4PI 550D1 80 15 G .NP RLX 140- 250 C340 TEL- 60WA2 9F 19 G N ABX 10- 240 C120- 240 ACT-I 4PI

D NP COINCIDENCE 62DE1 9F 19 G N ABX 20- 21 D 20- 21 ACT-I 4PI 60ST1 80 15 G .NP RLY 153- 320 C320 TEL-D 76 55DE5 9F 19 G N NOX THR- 260 C250 ACT-I DST REL TO H2 CROS SEC 57BA3 9F 19 G N ABX THR- 25 CTHR- 25 ACT-I 4PI 62G01 80 16 G .NP ABI THR- 170 C170 CCH-D 4P I NSA 35223 BREAKS

65GA1 80 16 G .NP ABX 250 C300 TEL-D DST 71BA2 9F 19 G N ABX 12- 15 C 15 TOF-D 135 58MA1 80 16 G • PA ABY 27- 80 C150 ,250 EMU-D 4P I 71FR1 9F 19 G N ABY 10- 800 ClOO- 300 ACT-I 4PI 62M02 80 16 G .PA ABI 23- 120 C120 EMU-D 4P I 590C1 9F 19 G 2N RL I THR- 100 CTHR- 100 ACT-I API REL TO G.N 72VA2 9F 19 G.XN ABX 10- 19 C 10- 19 BF3-I 4PI

24
NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN. OUT TYPE AN5 NUM SODIUM Z=ll

55LA1 9F 19 G P SPC 10 60F02 9F 1

9

G P RL X 10

62 BR3 9F 1 9 G P SPC 18 63MU1 9F 19 G P SPC 1

1

72SH2 9F 19 G PG SPC 0 55RE1 9F 19 G 2P ABI THR 64SE

1

9F 1 9 G XP SPC THR 58A61 9F 19 G XP SPC THR

6 5HA2 9F 19 G A SPC THR SSME* 9F 19 G 2NP ABX THR 72SH2 9F 19 G AG SPC 0 71W01 9F 19 P G ABI 10

72R03 9F 19 A G LFT 5

67BE7 9F 20 N G LET 6

- 17 C 17 EMU-D DST

18 C 16. 19 EMU-D DST

D 18 EMU-D DST

24 C 24 SCD-0 120

- 14 C 14 SCD-D 87 400 C 80-400 ACT-I 4PI

- 24 C 14- 24 EMU-D DST

22 C 22 SCD-D 90

31 C 31 EMU-D DST 300 C 20-300 ACT-I 4PI

14 C 14 SCD-D 87

D 2 SCO-D DST 10=10.129 MEV

7 0 1-3 SCD-D DST

J-P I . 4 LEVELS

- 7 D 0- 1 NAI-0 90 SOURCE 27.50 KEV

20

21

22

62G01

62G01

57<01 62SU1

63F 14 62G01

57k;oi 57K01

57K01 62G01

62G01

57K01 55RE1

71BE1

71 HOI

72MI4

59HA1

59HA1 60RE2

69H01

59HA1

59HA1

59HA1 60BR1 64AL3

64TA1 66PA3

67SE1 72AL4

90.92

0. 26 8.82

NEON Z=10

SEPARATION ENERGIES IMEV) G.N G.P G.T G.HE3 G.A G.2N G.NP G.2P

16.9 12.8 23.9 21.2 4.7 28.5 23.3 20.8

6.8 13.0 21 .6 19.9 7. 3 23.6 19.5 23.6

10.4 15.3 21.5 25.3 9.7 17.1 23.4 26.4

NUCLIDE REACTION RES EXCI

Z A IN. OUT

lONE lONE

57K;01 lONE

62G01 lONE

lONE lONE

lONE

lONE

lONE

lONE

lONE

lONE lONE

lONE

lONE

63BA1 10NE20

10NE20

10NE20

10NE20

62D01 10NE20

61CL1 10NE20

10NE20

10NE20

10NE20 10NE20

10NE20

10NE20

10NE20

10NE20

10NE20

10NE20

10NE20

10NE20

10NE20

G .MU-T G.N

ABI 0-170 C170

ABI THR-170 C170

E .E/

E .E/

E .E/

E .E/

E .P

G.G

G.N

G.P GiXP

G .XP G.A

G.2A G.PA

P .G P.G

P.G

P.G

P.G

A.G

CE DETECTOR

TYPE ANG NUM

CCH-D 4PI CCH-I 4PI INCLUDES G.2N

G P ABY THR- 80 C 80 CCH-D DST

A8I

G ,P ABI THR- 170 C170 CCH-I 4PI

1 NCLUDES G.D

G .2P ABY THR- 80 C 80 CCH-D 4PI

G .XP SPC 16- 23 C 23 EMU-D 90

G .XP SPC 15- 29 C 31 SCI-D 90

G .A ABI THR- 170 C 170 CCH-I

G .2A ABY THR- 80 C 80 CCH-D 4P I G .5A ABY THR- 80 C 80 CCH-D 4P I G .NP ABY THR- 80 C 80 CCH-D 4PI

G .NP ABI THR- 170 C170 CCH- I 4P I G .NA AB I THR- 170 C170 CCH-I 4PI

G .PA ABY THR- 80 C 80 CCH-D 4P 1 G .N17 ABI THR- 400 C 90- 400 ACT-I 4P I

SPC

ABX

FMF

FMF

SPC

LFT

ABX ABX

RLY

ABY

ABX

ABX

ABX

RLY

NOX ABX

NOX

ABX LFT

0-

11

1 •

6-

3-

1-

15.

15 . 100- THR16.

15,

15 . 17- 17-

17-

1815-

7-

18

18 240

33

18

181823

2224

25

9

D 42 J-PI

0 39.

1 1 D163.

D120-

.72-7.

C 18-

D 1- 1.63.

D 15,

D 15. C240

C 24-

0 15,

0 15.

D 15,

0 4-

D 4-

D 4-

D 5 D 3-

D

MAG-D 180

, WIDTHS. ABX

56 MAG-D 180 .23.11.58 MEV

250 MAG-D DST 1.63.4.25 MEV

250 MAG-D DST

84 MEV LEVELS

30 MAG-D DST

ABI

3 NAI-D 0 2.62 ,3.34 MEV

18 lON-D 4PI

18 lON-D 4PI CCH-D 4PI

33 SCI-D

18 lON-D

18 lON-D

18 lON-D

11 NAI-D UXN NAI-D DST

11 NAI-D 90 SCI-D DST

13 NAI-D DST SCD-D DST

4 LEVELS

90

4P I 4PI

4PI

G.N G. P

2 3 100.00 i.4 8. 8 1

NUCL I DE REACTION RES

REF 2 A I N OUT

61BE2 11NA21 P G SPC 708E3 1 1NA2

1

P G LFT

60KR1 1 1NA22 P G SPC 65TA1 1 1NA22 P G NOX

56WE1 1 1NA22 P G SPC

63BA1 1 1NA23 E E/ SPC

65BA4 1 1 NA2 3 E E/ ABX

69SA3 1 1NA2 3 E E/ FMF

68SA3 11NA23 E .E/ FMF

65WY1 1 1NA23 G MU-T ABX 72T03 1 1 NA2 3 G MU-T LFT

56FU1 1 1NA23 G G ABX 59RA1 11NA23 G G LFT 60M01 11NA23 G G NOX

61AM1 11NA23 G G LFT

62B06 11NA23 G G LFT 62M01 1 1NA23 G G LFT 64L03 11NA23 G G ABX 64ME1 11NA23 G G LFT

64ME2 11NA23 G G LFT

54SW1 1 1NA23 G G NOX

70SH2 1 1NA23 G G LFT

7 ISWl 11NA23 G G LFT

72FR4 1 1NA23 G G LFT

67L01 1 1 NA2 3 G G/ ABX 72SH2 11NA23 G G/ SPC 58CH2 1 1NA23 G N RLY

71AL1 1 1NA23 G N ABX

71SA1 1 1NA23 G N ABY 590C1 11NA23 G 2N RLI

71AL1 1 1NA23 G 2N ABX 63C03 1 1NA23 G XN ABX 53SA1 1 1NA23 G XN ABX

58KE1 11NA23 G P SPC

5e0Pl 11NA23 G P SPC

620D1 1 1NA23 G P SPC

68SH3 1 1NA23 G XP SPC 59H01 11NA23 G XP ABY 55RE1 1 1NA23 G N17 ABI 60WA2 1 1NA23 G 2N2P ABX 62BR2 1 1NA23 P G NOX

71PI2 1 1NA23 P G RLX

72VI 1 11NA23 P G NOX

67FE3 1 1NA23 0 G ABX

SEPARATION ENERGIES (MEV) G.T G,HE3 G,A G.2N G.NP G.2P

7.4 24.4 10.5 23.5 19.2 24.1

lURCE DETECTOR

TYPE ANG NUM

1 NAI-D DST

6- 8 SCD-D 90 8.973,9.215 MEV

0 10 D

9 D

D

10 D 1-

NAI-D IPI

1 NAI-O 90 LEVELS, J-PI

2 NAI-D DST

0- 20 D 42

2

2.

10-

9

4-

19

MAG-O 180 ABX

D 59 MAG-D 180 4=4.431 MEV

D 99-227 MAG-D DST BIEL12.08 MEV

D225 MAG-D DST

2 = 2.08 .7 = 6.27-i-7.10

0-

1 10-

7

7

7

3-

15-

0- THR

0-

1 10-

90 SCI-D 4PI

9 NAI-D 4PI 9.404, 9.700 MEV

4- 40 NAI-D 120

1 NAI-D DST

9 NAI-D DST WIDTH NAI-D 120 1=.438 MEV NAI-D 110 NAI-D 130

30 NAI-D 140 NAI-D DST J-PI, WIDTH NAI-D DST 4=4.431 MEV NAI-D DST

J-PI . WIDTH

SCD-D U<N 7=7.895 MEV

7 SCD-D DST

5 LEVELS

3- 6 NAI-D 130 LEVELS. G-WIDTH

NAI-D DST SCD-D 87 BF3-I 4PI THRESHOLD

27 BF3-I 4PI INCLUDES G.NP

68 C 10- 68 ACT-I 4PI 100 CTHR-100 ACT-I 4PI G.N

C 14

C 34

C 14 CTHR

12- 27 D 12-

12- THR23-

13-

12- 18

27

8024

REL TO

27 BF3-I 4PI

80 8F3-I API 24 BF3-I 4PI NAI-D

18 D 18

11- 18 C 18

20- THR- THR^

THR^

9^

9-

9-

23^

20. 24-

4PI ABX NAI-D 4PI ABX EMU-D DST

ABY

24 EMU-D DST

33 SCI-D 90 90-400 ACT-I 4PI 240 C120-240 ACT-I 4P

I

10 D u- NAI-D DST

J-PI

10 D 0- 2 SCD-D DST 9.61 MEV LEVEL J-PI

10 D 0- 1 SCD-D DST

4 LEVELS. J-PI

29 D 12- 31 NAI-D 90

L I 7-t-016

24

33 400

- 5

60KO2 10NE22

59H01

59HA1 50KO2

10NE22

10NE22

10NE22

68GR1 10NE22

G.P

G.XP

G ,A

G ,NP

A ,G

SPC THR- 90 C 90 CCH-D DST

ABY THR- 33 ABX 15, 18 SPC THR- 90

LFT 12, 13

SEPARATED ISOTOPES

C 24- 33 SCI-D 90

0 15, 18 lON-D 4PI

C 90 CCH-0 DST SEPARATED ISOTOPES

D 2, 3 NAI-D DST

12 , 13=11.89 , 12.28

MAGNESIUM Z=12

A ABUND. SEPARATION ENERGIES (MEV) G,N G,P G,T G.HE3 G.A G,2N G.NP G.2P

24 78.70 16.5 11.7 26.7 23.1 9.3 29.7 24.1 20.5

25 10.13 7.? 12.1 23.0 20.1 9.9 23.9 19.0 22.6

26 11.17 11.1 14.1 21.6 26.0 10.6 18.4 23.2 24.8

NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN, OUT TYPE ANG NUM

64G03 12MG E,E/ ABX 11 D 40- 70 MAG-D 180 FMF 68SA1 12MG E,E/ FMF 1- 8 DlOO-260 MAG-D UK.N

3 PEAKS 1.4-6.0 69SA2 12MG E.E/ FMF 1-8 0 99-229 MAG-D DST B(EL) 1-8 MEV

25
NUCLIDE REACTION RES EXCIT SOURCE DETECTOR NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

Z A IN. OUT TYPE ANG NUM REF Z A IN. OUT TYPE ANG NUM

6^D02 12MG G MU- T ABX 12- 30 C250 MGP-D 4P I 60ME 1 12MG25 G G NOX 2 0 2 NA I-D DST 65D02 1 2MG MU- J ABX 11- 30 C260 MGP-D 4P I j_p I , W I DTH

6 5WY 1 1 2MG MU- T ABX 10- 70 C 90 SC I-D 4P I 47+ 61RA1 12MG25 G G LFT 2 2 NAI-D DST 66D02 1 2MG MU- T ABX 8- 30 C260 MGP-0 4P I 323 J-P I 56FU1 1 2MG G G ABX 4- 40 C 4- 40 NAI-D 120 62B06 12MG25 G G LFT 0- 4 c 0- NAI-D DST ERRATUM PR 106 993 64B01 12MG25 G G LFT 1 - 3 c 1 - NAI-D 100 59LA 1 1 2MG G G LFT 1 0 C 13 NAI-D 135 AS I 10=10.3 MEV 70BE5 1 2MG2 5 G N ABX 7- 10 c 1 1 TOF-D 135

6 1BU4 1 2MG G G ABX 15- 30 C 27. 32 NAI-D 140 71AL1 1 2 M G 2 5 G N ABX 7- 29 D 7- 29 BF 3- I 4P

I

61SU1 12MG G G RLY 7- 1

4

C 7- 14 NAI-D 120 INCLUDES G.NP

62SE 1 1 2MG G G NOX 0- 16 C 16 NAI-D 90 7 1 B A2 1 2MG2 5 G N ABX 7- 1 1 8 . 1 1 TOF-D 135 63SU1 12MG G G ABX 4- 14 C 4- 14 NAI-D 120 7 1 AL

1

1 2MG2 5 G 2N ABX 23- 29 D 2 3- 29 BF3- I 4P

I

67L01 12MG G G/ ABX 16- 32 C 34 NAI-D DST 55NA1 12MG25 G XN ABX 7- 24 c 9- 24 BF3-I 4PI 58SP2 1 2MG G N ABX 8- 1 7 C 8- 17 BF3-I 4P I 328 680K3 12MG25 G p ABY THR- 20 C 20 AC T- I 4P I 54F I 2 12MG G N RLY 18- 26 C 27- 32 TOF-D UKN 67BE7 1 2MG2 5 N G LFT 7 D 1 NAI-D 90 70WE1 12MG G N ABX 17- 32 C 17- 32 ACT- I 4P I SOURCE 84 KEV

56YE1 12MG G XN ABY 7- 23 C 7- 23 BF3-I 4P I 63C03 12MG G XN ABX 10- 80 C 10- 80 BF3- I 4P I 327 65T I 1 12MG26 E E/ LFT 7- 15 D 51 MAG-D DST 65MI1 12MG G XN ABX THR- 30 CTHR- 30 BF3-1 4P 1 325 DST CONST Q 66FI2 12MG G XN SPC THR- 65 C 65 TOF-D 90 68BE2 12MG26 E E/ ABX 8- 14 D 39. 56 MAG-D 180 71FU2 12MG G XN ABX THR- 29 D 10- 29 BF3- I 4P I 342 70GO3 12MG26 E E/ ABX 15- 26 D 45- 55 MAG-D DST

14 LEVEL F I T 70KH1 12MG26 E E/ FMF 1 D225 MAG-0 DST 62SH1

1

12MG G P ABX 1 5- 24 CTHR- 24 SCI-D DST 1=1.81

6AF01 12MG G P SPC THR- 40 C 20- 40 EMU-0 DST 70T I 1 12MG26 E E/ SPC 12- 28 D 50- 54 MAG-D DST

71SA2 12MG G P ABX THR-250 C 20- 250 ACT- I 4P I 6 IRAl 12MG26 G G LFT 2 D 2 NAI-D DST 64IS1 12MG G XP ABX THR- 32 C 15- 32 SCI-0 UKN 326 64B01 12MG26 G G LFT 1- 3 C 1- NAI-D 100 65MA4 12MG G XP SPC THR- 31 C 31 SCD-D UKN ABI 66H03 12MG G A SPC THR- 31 c 31 SCD-D 130 67KU2 12MG26 G G LFT 10- D NAI-D 135 55RE1 12MG G Nl 7 AB I THR-400 c 80- 400 ACT-I 4PI 10=10.07 MEV

56HE3

63BA1

67T I 1 58FA1

69T I 1

70FA1

70G03

70KH1

70ST2

71H01

71M03

72NA1

12MG24

12MG24

66AR2 12MG24

66TI1 12MG24

12MG24 12MG24

12MG24

12MG24

12MG24 12MG24

12MG24

12MG24

12MG24 12MG24

353

320

CONST Q=.41 FM-1

FMF

SPC

LFT

LFT

SPC

LFT

FMF

LFT

ABX

FMF

ABX

FMF

ABX

LFT

1 5-

7-

1 5-

1

7 16

22

15

26

28

12

14

26

240

6

D187

D 42

D 52

D 51

MAG-D DST MAG-D 180

PI. WIDTHS MAG-D 141

5 LEVELS MAG-D DST

DST CONST 0

D 45- 54 MAG-0 DST

D 39. 56 MAG-D 180 DETAILS 9.9. 10.7

D 37- 51 MAG-D DST TABULAR DATA

D 39. 56 MAG-D 180 REANALYSIS 68FA11

D 45- 55 MAG-D OST D225 MAG-D DST 1=1.37

D 31- 59 MAG-D DST 6=6.44 0+ 0183,250 MAG-D DST 1.37.4.12 MEV

D500 MAG-D 50 D183-25D MAG-D DST 1.37.4.23.6.00 MEV

69BE3 12MG26

58BU1 12MG24 G G LFT 1 D 1 SCI-D 4P I 1=1.38 MEV

60BU2 12MG24 G G LFT 1 1 C NAI-D DST 60BU3 12MG24 G G LFT 10 C 23 NAI-0 DST 60ME1 12MG24 G G NOX 1 D 1 NAI-0 DST

J -PI . WIDTH

60T01 12MG24 G G NOX 9- 11 C 13 NAI-D 118 THRESHOLD

62B06 12MG24 6 G LFT 0- 4 C 0- NAI-D DST 64B01 12MG24 G G LFT 1- 3 c 1- NAI-O 100

ABI 67KU2 12MG24 G 6 LFT 9- 1 1 D 9- 1

1

NA I-D 135

9. 92. 10.66 MEV

71SW2 12MG24 G G LFT 1 0 1 SCD-D 127

1 .368MEV.2+ STATE

60K I 1 12MG24 G N ABX 15- 25 C 15- 25 ACT-I 4P I 66MI2 I2MG24 G N ABX 16- 27 D 16- 27 BF3- I 4PI 68C01 12MG24 G N RLX THR- 66 C 13- 55 ACT-I 4P I 580K2 12MG24 G N ABY THR- 20 C 20 ACT- I 4P I ISOMERIC YIELD

71BA2 12MG24 G N ABX 16- 20 C 17. 20 TOF-D 135 71FU2 12MG24 G N ABX 16- 29 D 16- 30 BF3- I 4PI

14 LEVEL FIT 55NA1 12MG24 G XN ABX 16- 24 C 9- 24 BF3-I 4P I 69AN2 12MG24 G XN ABX THR- 55 C 16- 54 ACT-I 4P I MEAS TOTAL ACT

72 I SI 1 2MG24 G XN ABX 16- 30 C 15- 30 BF3-I 4P I 63YA1 12MG24 G P SPC 15- 22 C 22 EMU-D DST RLY

65 I SI 12MG24 G P ABX THR- 34 C 15 30 EMU-0 DST 60WA2 12MG24 G 2N3P ABX THR- 240 C240 ACT-I 4P I 53SH3 12MG24 G C12 RLY THR- 70 C 7U EMU-O 4P 1 54SH6 12MG24 G F ABY THR- 100 ClOO ACT-I 4P I 61G01 12MG24 P G RLY 15- 23 0 3- 11 NAI-D 90 62GL1 12MG24 P G NOX 12 0 0- NA I-D 55 62PR1 12MG24 P G NOX 12 13 D 0- NAI-D 55 WIDTHS

63G03 12MG24 P G RLY 15- 23 D 4- 12 NA I-D 90 67LE1 12MG24 P G ABX 16- 25 D 5- 14 MGP-D 90 68BE3 12MG24 P • G ABX 16- 24 D 4- 13 NAI-D DST

68HI 1 12MG24 A .G RLX 1 1- 14 D 3- 6 NAI-D DST

J- PI .G-WIDTH

59FA2 12MG25 E .E/ ABX 0- 27 D 39. 56 MAG-D 180

71BA2

71FU2

12MG26

12MG26

71FU2 12MG25

70WU2

72IS1 12MG2512MG25

G.N

G.N

G.XN

G.XN

ABX

ABX

SPC

ABX

1 1- 10-

18- 29 0 18-

11- 11-

13 TOF-D 135 0=10 TO 1200 KEV

11. 14 TOF-D 135

10- 29 BF3-I 4PI

32 LEVEL FIT

29 BF3-I 4PI

32 LEVEL FIT

23 TOF-0 UKN

30 BF3-I 4PI

G.N

13.1

ALUMINUM z=13

SEPARATION ENERGIES (MEVl G.P G.T G.HE3 G.A G.2N G.NP

8.3 18.2 23.7 10.1 24.4 19.4 G.2P 22.4

53GA1 68M02

62NE2

63GA1

NUCLIDE REACTION RES

Z A IN. OUT

1 3AL25 13AL25

EXC I T

1 3AL25 13AL26

63BA1 13AL27

53G04

67L02

1 3AL27

1 3AL27

71VL1 13AL27

64AM1 59BA3

71V01

64CH1

62D01

70AN5

70FU1

13AL27

13AL27

1 3AL27

1 3AL27

1 3AL27

13AL27

1 3AL27

72N03 13AL27

58Z I 1 59DU1

59K01 59M I 1 50CA1 60TA2

60WY 1 50Z I 1 64D02

54TE1

65WY1 71AH1

56FU1 59PA3 60ME1

60RE1

50VA1 61BU3

51BU4

61T01 62B06

1 3AL27 13AL27 13AL27

13AL27

13AL27

13AL27

1 3AL27 13AL27

13AL27

13AL27

13AL27

13AL27 13AL27

1 3AL27 13AL27

13AL27

1 3AL27 13AL27

13AL27

13AL27

1 3AL27

p G LFT 1 p G LFT 8

p .G NOX 7- 8 p G LFT 1

E .E/ SPC 0- 18

E .E/ ABX

E .E/ FMF 0- 3

E .E/ FMF 0- 300

E .E/P RLX THR- 150

E .N ABY THR- 35

E .N ABX THR- 255

E .P ABX

E ,P SPC 17- 29

E .P RLY 88- 999

E F RLY 999

E P I + RLY 150- 999

G .MU- T ABX 17- 25

G MU- T ABX 13- 30

G MU- T ABX 13- 30

G MU- T ABX 13- 30

G MU- T ABX 13- 21

G MU- T ABX 7- 28

G MU- T ABX 13- 55

G MU- T ABX 13- 30

G MU- T ABX 9- 29

G MU- T ABX 20- 21

G MU- T ABX 10- 70

G MU- T ABX THR- 150

G G ABX 4- 40

G G ABX 17

G G NOX 1 . 2 G G ABX 7 G G LFT 1 G G ABX 14- 32

G G ABX 15- 30

G G ABX 3- 15

G G LFT 3

DETECTOR

TYPE ANG NUM

SCI-D UKN

SCD-I DST G-WIDTH

NAI-0 0 SCD-D UKN

D 42 MAG-D 180 ABX

D 41 MAG-0 180

D 90-190 MAG-O DST

5 LEVELS .84-3 MEV 0592-999 MAG-0 DST 999=1143 QUAELSCTG

D550 MAG-D 51

D 10- 36 BF3-I 4P1 C150-266 TOF-D 90 D999 MAG-D OST 999=8 GEV

C 18- 30 MAG-D DST VIRTUAL PHOTONS

C999 TEL-D DST 999=1140 MEV

D999 ACT-0 4P

I

999=1.5-16.0 GEV C150-999 ACT-1 4P

I

999=1.2 GEV

C 17- 30 MGP-D 4PI

30

C 30

0 20

29. 30 MGC-D 4P

I

D 4P I 0 4PI

D 4PI

NAIMGC21 NAI- MAG-D 4PI 35- 90 NAI- 10- 30 MGP50 MGP- 20- 21 NAI90 SCI- 10-150 MGC4- 40 NAI18 NAINAI15.

1 . 73 32

27.4-

0-

4P I 4P 1 4P I 96

4P I 4P I 120

90 DST

NA I- NAINAI32 NAI

15 NAI

NAI

D 90

D 120

D DST SEE 61BU4

0 140

D 120

0 DST

26
NUCL I DE REACTION RES EXCIT SOURCE DETECTOR NUCL I DE REACTION RES EXCIT SOURCE DETECTOR

REF 2 A I N OUT TYPE ANG NUM REF Z A I N .OUT TYPE ANG NUM

6 3VA3 1 3AL27 » G NOX 2 c 3 NAI-0 DST 57B01 13AL27 (3 . A SPC THR- 30 C 31 EMU-D DST WIDTH 58T02 13AL27 G . A ABY 10- 22 C 22 EMU-I 4P I 6 3 V A4 1 3AL27 NOX 3 c NAI-0 120 61MA1 13AL27 (3 . A RLY 19- 3 5 C 35 MGP-D OST WIDTH 62BE3 13AL27 G . A SPC 16- 30 C 30 SCO-0 DST 64B0

1

1 3 AL 2 7 tG L F T NA I D ASYMMETRY SPECTRUM

ab? 65HA2 13AL27 C3 . A SPC THR- 3 1 C 31 EMU-D DST 64ME 2 1 3AL 27 »

G

L F T D NA I -0 DST 66H03 13AL27 (3 . A SPC T H R- 3 1 C 31 SCD-D 130 MEV 66WE2 1 3AL2 7 (3 . A ABX 10- 3 3 C 33- SCD-D 90

6 5 KHl 1 3 AL 2 7 G LFT 2 , 3 D 2 , 3 NA I -D DST 60ST1 13AL27 G . NP RLX 149- 320 C320 TEL-D 7 6 2,3 = 2,21.2.98 MEV REL TO H2 CROS SEC 65ME3 1 3AL2 7 »

G

LET D NA I -D OST 60G02 13AL27 (3 .N2P ABX 30- 26 0 C 30-260 ACT-I 4P I 4=4.403 MEV 57AN 1 13AL27 (3 .N2P RLX THR- 99 9 CjHR-999 ACT-I 4P I 66H0 2 1 3AL27 »

G

LFT c NAI-D 117 60G02 13AL27 G . PO ABX 30- 260 C 30-260 ACT-I 4P I 1=1.01 MEV 68ME4 13AL27 G .2NP ABX THR- 300 C 20-300 ACT-I 4P I 66VA4 1 3AL27 f3 AB I 1

0

D 1

0

NAI-D 80 60WA2 13AL27 (3 . 4N4P ABX THR- 2 40 C120-240 ACT-I 4P I 10=10.1 MEV 55RE1 13AL27 G .N17 AB I THR- 400 C 80-400 ACT-I 4P I 68R01 1 3AL27 G G LFT 3 C 3 NAI-I 113 54MA4 13AL27 G .F18 ABY 150- 720 C150-720 ACT-I 4P I 2.21 .2.98.3.0 MEV 71DI3 13AL27 G .NA22 ABY THR- 999 C300-999 ACT-1 4P I 725H2 1 3AL27 Q, G/ SPC Q- 14 C 14 SCD-D 87 999= 1 GEV

55J01 1 3AL27 (3 N RLY 15- 6 5 C 65 SCI-D DST 54MA4 13AL27 G .NA24 ABY 150- 720 C150-720 ACT-I 4P1 57FE 1 1 3 AL2 7 (3 N RLY 22- 3 1 c 31 THR-I DST 69N01 13AL27 G . NA24 ABY 31- 999 ClOO-999 ACT-I 4P I 58AS1 1 3AL 2 7 N NOX 13- 1 7 c 17 SCI-I DST 999=1.2 GEV

5 QCH2 1 3AL27 (3 N RLY T HR CTHR BF3-I 4P I 71DI 3 13AL27 G . N A 2 4 ABY THR- 999 C300-999 ACT-I 4P I THRESHOLD 999= 1 GEV

SSFEl 13AL27 G N ABX 13- 30 C 13- 30 ACT-I 4PI 71SA2 13AL27 G . N A 2 4 ABX THR- 250 C 20-250 ACT-I 4P I 59KU1 13AL27 G N NOX 2 3- 88 C 88 SCI-I DST 69FU2 13AL27 G .SPL RLY THR- 999 0999 SCO-0 DST OUASI-DEUTERON 999 = 3 GEV

60CH2 1 3AL27 G N ABX 13- 2 1 D 12- 21 BF3-I 4P I 71FU4 13AL27 G SPL RLX THR- 999 D999 ACT-I 4PI 60GE3 1 3AL27 (3 N NOX T HR CTHR SF3-I 4P I 999 = 5 GEV THRESHOLD 71K.U2 13AL27 G SPL ABY THR- 999 C800-999 ACT-I 4P I 60K.U2 13AL27 G N RLY 23- 90 C 90 TEL-I DST 999 = 2.1 GEV

6 ISA 1 1 3AL2 7 (3 N ABX 13- 1

9

C 12- 19 BF3-I 4P I 71GR2 1 3AL27 G PI- ABY 150- 560 C56C EMU-D OST 61PR1 1 3AL27 G N RLX 13- 85 C 25- 65 THR-D PI-/PI+ YIELD RATIO

52B02 13AL27 G H ABX 13- 30 C 14- 30 BF3-I 4PI 64MA4 13AL27 G P 1 + ABY 1 50- 720 C150-720 ACT-I 4P I 62MU1 13AL27 G N ABX 13- 24 C 1 3- 24 8F3-I 4P I 68NY 1 1 3AL27 f3 P 1 + ABX 140- 700 C140-700 ACT-I 4P I 63M I 4 1 3AL27 G N SPC 15- 30 C 24. 30 EMU-0 90 MG-27 ACT 64TH1 13AL27 G N ABX 15- 24 c 15- 24 ACT-I 4P I 7 1GR2 1 3AL27 G P I + ABY 150- 560 C550 EMU-0 OST

65 TH2 1 3AL2 7 G N ABX 13- 2 4 r 13- 25 ACT-I 4P| 76 PI-/PI+ YIELD RATIO THRESHOLD 7 2 NO 3 13AL27 (3 P I + ABX 150- 999 C150-999 ACT-I 4PI 668 I 1 13AL27 G N ABX 20-200 C 20- 200 BF3-I 4P 1 999=1.2 GEV 66FU1 1 3AL27 G N ABX 1 3- 37 D 13- 37 6F3-I 4P I 115 61N01 13AL27 p (3 NOX 9 D 1 UKN 57GE2 13AL27 G N ABY THR- 2 7 C 22 . 27 8F3-I 4PI J-PI . WIDTH

58C01 13AL27 G N RLX T HR- 65 C 13- 65 ACT-I 4PI 62LA1 13AL27 p G NOX I I D 3 NAI-D DST 68KA1 1 3AL27 G N ABX 50- 8 5 c 55 . 85 TOF-D 67 -PI NEUT ENGY SPEC 520P 1 13AL27 p (3 NOX 9 0 0- NAI-D OST 66FU1 1 3AL2 7 G 2N ABX 25- 3 7 0 25- 37 8F3-I 4P I 115 -PI 55BA5 1 3AL27 (3 XN ABY 30- 20 0 C15U- 250 THR-I DST 63VA6 1 3AL27 p G RLY 9- 10 0 1- NAI-D OST 55D I 1 1 3AL 2 7 (3 XN NOX 13- 7 0 C 70 SCI-I DST SEPARATED ISOTOPES

5 8BA 5 1 3 AL2 7 (3 XN RLY T HR- 1 5 C 12- 15 BF3-I 4P I 54VA1 1 3AL27 P G NOX 10- 1 1 0 2- NAI-0 OST BREAKS -PI 58FE1 1 3AL27 G XN ABX 1 3- 30 c 13- 30 THR-I 54VA2 1 3AL27 P G NOX 10 0 2 NAI-D UKN FAST NEUTRONS J -PI 59C03 1 3AL27 G XN SPC 15- 30 c 24 . 30 EMU-D 90 55VA5 13AL27 P G SPC 10 D 2 NAI-D OST 63C03 1 3AL 2 7 (3 XN ABX 12- 80 c 80 BF3-I 4P I 67SH2 13AL27 P G LFT 8- 1

1

D 0- 3 SCD-0 DST 64AL5 1 3AL 2 7 XN NOX T HR- 34 c 34 THR-I DST 57VA1 13AL27 P G NOX 8- 1 1 0 0-3 SCO-D 45

66 F I 2 1 3AL 2 7 ^ SPC c 66 TOF-D 90

6 7AN2 1 3 AL 2 7 (3 XN ABX T HR— 2 6 c 1 3- 25 BF3-I 4P I 63CV1 1 3AL28 N (3 ABX 12- 22 0 14 TEL-D 4PI 69AN3 13AL27 G XN RLX 13- 65 c 13- 55 ACT-I 4P I 57BE7 1 3AL28 N G LFT 7- 8 D 0- 1 NAI-D 90 69C02 13AL27 G XN ABX 15- 35 D 15- 35 BF3-I 4P I SOURCE 35.89 KEV 69IS3 1 3AL27 G XN ABX 13- 30 C 5- 30 BF3-I 4P I 453 69VE I 13AL27 G XN SPC THR- 33 C 33 TOF-D OST 71C02 13AL27 G XN AB I 36- 64 C 10- 54 BF3-I 4P I FAST N YIELD

55J01 13AL27 G P RLY THR- 65 c 55 SCI-D OST SILICON Z = 14 598A2 1 3AL27 G P SPC 25- 52 c 18- 52 TEL-D 90 60CH2 1 3AL27 G P ABX 12- 21 c 12- 21 lON-I 4P I 61MA1 13AL27 G p RLY 11- 3 5 c 35 MGP-D U<N A ABUNO. ( 1

1

SEPARATION ENERGIES (MEVl 62BR3 13AL27 G p SPC 1 8 D 18 EMU-D OST G.N G.P G .T G.HE3 G.A G.2N G .NP G.2

G P ABX 1 5 * 1

8

D 15. 18 SCI-D 28 92.21 17,2 11.5 27.5 23.2 10.0' 30.5 24.6 19.

1 ^Ai"?-? G SPC 10- 2 4 C 24 EMU-D DST 29 4.70 3.5 12.3 24.6 20.

e

11.1 25.7 20.1 21.

G P 10- 2 4 c 24 SCI-I 4P I 30 3.09 10.6 13.5 22 .2 24.6 10.5 19.1 22.9 24 . 63001 1 3AL27 G ABY 10- 2 2 c 22 EMU-D DST 66L I 1 1 3AL27 (3 p SPC T HR- 3 2 c 32 SCI-D 90 69C04 G 8 — 8 5 c 85 CCH-D 180 NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

70CO2 1 3AL 2 7 (3 p RLY g - 34 c 85 TEL-0 OST REF 2 A IN OUT TYPE ANG NUM

720D1 13AL27 (3 p ABX 12- 2 2 c 15- 22 SCD-I 90 58AU1 1 3AL27 (3 2P ABX 2 0- 6 3 c 20- 63 ACT-I 4PI 64G03 14SI E E/ ABX 12 D 40- 70 MAG-0 180 560A2 1 3AL2 7 (3 XP SPC 11- 70 c 70 EMU-D DST FMF ABY 58SA2 14SI E E/ FMF 1- 13 0114-260 MAG-D DST 57BA2 1 3 AL2 7 G XP SPC T HR- 6 5 c 85 TEL-D DST 5 LEVELS 1.78-12.7

58BA6 13AL27 G XP SPC THR- 8 5 c 85 . 90 TEL-D OST 59DU1 14SI G MU-T ABX 15- 25 C 29. 30 MGC-0 4P I 60CH1 13AL27 G XP RLX 24- 90 c 90 TEL- I 90 65WY1 14SI G MU-T ABX 10- 35 C 90 SCI-D 4PI 61 + REL TO DEUTERONS 68BE4 14SI G MU-T ABX 10- 30 C 35 MGC-D 4P I 103 61MA2 13AL27 G XP NOX 8- 2 1 c 21 SC I-O DST 71AH1 14SI G MU-T ABX THR- 150 C 10-150 MGC-D 4P I 62CH2 13AL27 G XP RLY 2 3- 3 5 c 35 MAG-D OST 60RE1 14SI G G ABX 7 0 7 NAI-D 90 REL TO DEUTERONS 6 ISUl 14SI G G RLY 11 C 6- 13 NAI-D 120 63M I 5 13AL27 (3 XP ABY 12- 2 2 c 22 SCI-D DST 6 1 TOl 14SI G G ABX 4- 14 C 5- 14 NAl-D 120 64MA2 1 3AL27 (3 XP SPC T HR- 2 0 c 20 SCD-D 62SE1 14SI G G NOX 11 C 16 NAl-D 90 68A83 1 3AL27 (3 XP SPC THR- 2 7 c 22. 27 SCO-D 90 6 3 BO 1 14SI G N ABX 15- 25 C 10- 30 8F3-I 4PI 51MA1 13AL27 G RLY 20- 35 c 35 MGP-D DST 63SA1 14SI G N ABX 10- 24 C 10- 24 BF3-I 4PI 60CH1 13AL27 G xo RLX 32- 90 c 90 TEL-I 90 66G03 14SI G N ABX 17- 30 C 17- 30 BF3-I 4P I 74 REL TO PROTONS 70WU1 14SI G N ABX 18- 21 C 16- 22 TOF-0 90 62CH2 1 3AL27 G xo RLY 32- 35 c 35 MAG-D DST GROUND STATE

REL TO PROTONS 53C03 14SI G XN ABX 13- 80 C 13- 80 BF3-I 4P I 7 1AN2 13AL27 G XD ABX 107- 999 C999 MAG-D DST 66F I 2 14SI G XN SPC THR- 50 C 60 TOF-D 90 999=1 . 14 GEV 58G05 14S I G XN ABX 17- 30 C 17- 30 BF3-I 4P I 431 56HE1 13AL27 G T RLY THR- 31 c 31 ACT-I 4PI 59AN3 14SI G XN RLX THR- 65 C 15- 55 ACT-I 4P I 56WA1 13AL27 G T RLY THR- 31 c 31 ACT- I 4P I 59C01 14S I G XN ABX 14- 38 C 14- 38 BF3-I 4P I 70CU1 1 3AL27 G T ABY THR- 90 c 90 ACT-I 4PI 71C02 14S I G XN ABI 36- 64 C 10- 64 BF3-I 4P I 60GO2 13AL27 G HE3 ABX 30- 260 c 3u- 260 ACT-I 4P I FAST N YIELD

27
NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN. OUT TYPE ANG NUM REF NUCLIDE REACTION RES

Z A IN, OUT EXCIT SOURCE DETECTORTYPE ANG NUM

58EM1 14S 1 G P NOX THR- 30 C 30 EMU-D DST 60WA2 14SI28 G 4N5P ABX THR- 240 C240 ACT-1 4PI 62SH11 14SI G P ASX THR- 24 CTHR- 24 SCI-I DST 71G02 14SI28 G PI + RLY 150- 500 C500 CCH-D OST

e^iMAl 14SI G P ABX 17- 22 D 17- 22 SCD-D 4P

I

PI -/PI+ YIELD RATIO BRANCHING RATIOS 60KI3 14SI28 P G RLX 19- 26 0 8- 15 NAI-D 90 64UL1 14S I G P SPC 14- 20 C 17- 20 SCD-0 4PI 61GA1 14SI28 P C ABX 16- 25 0 5- 13 NAI-D 90 SCO TARGET 5 IGOl 14SI28 P G RLY 15- 22 0 3- 11 NAI-0 OST 65G01 14SI G P SPC THR- 27 C 23- 27 SCD-D 90 61K I 1 145128 P G ABX 7- 1 5 0 7- 15 NAI-O 90 66LI1 14S I G P SPC THR- 32 C 21, 32 SCI-D 90 63AN2 14S I 28 P G NOX 13 0 1- NAI-D 90 67G01 14S I G P ABX THR- 29 C 11- 29 SCD-D 4PI 63S 1 1 145 I 28 P G NOX 12 0 1 NAI-0 OST 71AN1 14SI G P SPC 45-999 C700,999 TEL-D DST J-P I 999=1.2 GEV. REL D/P 64AL3 145128 P G ABX 15- 24 0 4- 13 NAI-0 DST 71SA2 14SI G 2P ASX THR- 250 C 20-250 ACT-I 4P

I

64RA1 145I2B P G RLX 15- 18 0 5- NAI-0 90 60CH1 14S I G XP RLX THR- 90 C 90 TEL-I 90 FLUCTUAT I ONS

REL TO DEUTERONS 55PA2 14SI28 P G ABX 19- 22 D 8- 11 NAI-0 90

61SHi. 14SI G XP SPC THR- 24 C 24 EMU-D DST 65S 11 145128 P G ABX 16- 24 0 4- 13 NAI-0 90 104 ABSOLUTE YIELD 70ME1 145128 P G RLY 12- 1 3 D 1- 2 SCD-D 55 61SH5 14SI G XP SPC 14- 24 C 24 EMU-D UKN 710A2 14SI28 HE G ABX 27- 31 0 4- 8 NAI-D DST 64L02 14S I G XP SPC THR- 21 C 21 SCI-D 4PI HE = HE3

SCO TARGET 62SM1 14SI28 A G ABY 11- 13 D 1- NAI-D DST

6'.UL2 14SI G XP SPC THR- 30 C 15- 30 SCD-D 4PI J -PI . SEP ISOTOPES

7 lANl 14SI G D SPC 55- 999 C700,999 TEL-D DST 64WE1 14SI 28 A G NOX 12- 14 0 3- NAI-D DST 999=1.2 GEV, REL D/P W IDTHS 60CH1 14SI G XO RLX THR- 90 C 90 TEL-I 90 REL TO PROTONS 62806 145 129 G G LFT 1 . 2 C 0- NAI-D DST 50CH1 14SI G XT RLY THR- 90 C 90 TEL-I 90 J-PI, WIDTHS

REL TO DEUTERONS 54RE1 14SI29 G .G LFT 1 0 1 NAI-D 90 64MA1 14S I G A ABX 17- 22 0 17- 22 SCD-D 4PI 1=1.277 MEV BRANCHING RATIOS 61BE1 14SI29 G N RLY THR CTHR ACT-I 4PI S^ULl 14S I G A SPC 14- 20 C 17- 20 SCD-D 4PI SCO TARGET 660^3 14SI29 G P ABY THR- 20 C 20 ACT-I 4PI

6 5H A 2 1 4S I G A SPC TH R - 31 C 31 EMU-D DST 67AN1 14S I G NA24 RLX THR- 999 CTHR-999 ACT-I 4PI 61BE1 14SI30 G N RLY THR CTHR ACT-I 4PI 69N01 14S1 G NA24 ABY 43- 999 ClOO-999 ACT-I 4P

I

THRESHOLD

999=1.2 GEV 680K3 14S I 30 G P ABY THR- 20 C 20 ACT-I 4PI 71SA2 14SI G NA24 ASX THR- 250 C 20-250 ACT-I 4P

I

71FR1 14SI30 G P ABX 14- 800 ClOU-800 ACT-I 4PI 58ME1 14SI30 G A ABX 14- 22 0 4- 14 NAI-0 DST 56HE3 14SI28 E E/ FMF 1- 7 D187 MAG-D DST 72RU1 14SI30 A G ABY 13- 14 D 3- 4 NAI-D DST 60BA4 14SI28 E E/ SPC 0- 30 D 43 MAG-D 160 J-PI .LFT

52ED1 14SI28 E E/ ABI 0- 12 ABID 42 TEL-0 180 68ME1 14S I 32 A G ABX 13- 18 0 7- 12 NAI-0 DST G-WDTH

54BR2 14SI28 E E/ SPC 0- 12 D 41 MA6-D 152 66AR2 14SI28 E E/ LFT 5 D MAG-D DST 5=4.97 MEV 66LI2 14S 128 E E/ LET 2- 12 D 30- 56 MAG-D DST PHOSPHORUS Z = 15

4 LEVELS

67SA1 145 128 E E/ FMF 1- 10 DlOO-260 MAG-D DST

4 LEVELS A ABUNO. SEPARAT ION ENERGIES (MEVI SSAF 1 14S 128 E E/ FMF 10- 30 D150-225 MAG-D DST G.N G, P G . T G.HE3 G, A G.2N G.NP G, B(EL) 31 100.00 12.3 7. 3 17.9 22. 5 9. 7 23.6 17.9 20 680R1 14SI28 E .E/ FMF 11 D140 MAG-D DST 11=11.4 MEV

68GU1 14SI 28 E E/ ABX 10- 30 D150-225 MAG-D OST NUCLIDE REACTION RES EXC I T SOURCE DETECTOR

69FA1 14S I 28 E E/ ASX 9- 16 D 39, 55 MAG-D 180 REF Z A IN OUT TYPE ANG NUM

J-P I • B ( ML 1 700E1 14SI28 E E/ ABX 400-999 D690-999 MAG-D DST 69 I S3 15P G XN ABX 12- 30 C 5- 30 BF3-I 4PI 454

NO DATA, SEE C12 70D01 14S I 28 E E/ FMF 11- 24 0100-300 MAG-D 145 60NE1 15P 29 P ,G NOX 4- 5 D 1- NAI-D DST 70ST2 14SI28 E .E/ ABX 5 . 6 0 30- 58 MAG-D OST J-PI . WIDTH 5=4.98,6=6.69 0+ 6 1VA3 15P 29 P ,6 NOX 3- 5 0 0- NAI-D OST 71H01 14SI2e E .E/ FMF 2 . 5 0183,250 MAG-D DST J-PI, WIDTHS

1.78,4.61 MEV 66Y01 15P 29 P ,G SPC 8- 9 0 5- 6 ACT-I 4PI 71VL1 14SI28 E .E/ FMF 0- 300 D592-999 MAG-0 OST

999= 1143 MEV 61VA2 15P 30 P G NOX 7 0 1 NAI-D DST 72NA1 14SI28 E .E/ LFT 1- 1

0

D183-250 MAG-D OST J-PI

1 .78.4.6.6.9,9.7 MEV 62AN2 16P 30 P G NOX 7- 8 D 1- NAI-0 90 60T01 14SI28 G G RLY THR- 1 3 C 13 NAI-D 120 J-P I THRESHOLD 53VA2 15P 30 P G NOX 7 D 1 NAI-D UKN 61804 14S I 28 G .C ABX 1 1 C 11- 16 NAI-D UKN J-PI WIDTHS 64EJ1 15P 30 P G NOX 7 D 1 NAI-D OST 51BU4 14SI28 G .G ABX 15- 30 C 32 NAI-D 140 J-PI, WIDTHS

62B06 14SI28 G G LFT 2 C 0- NAI-D 110 69HA2 15P 30 P G LFT 6- 8 0 0- 2 SCO-D 45 J-PI. WIDTH J-PI 64B01 14SI28 G >S LFT 1- 3 C 1- NAI-D 100

ABI 63BA1 15P 31 E E/ SPC 0- 15 D 42 MAG-D 180 65SW1 14SI26 G G LFT 7 0 7 NAl-D DST ABX

J 7=6.88 MEV 53L02 15P 31 E E/ FMF 6 D130. 180 MAG-0 OST 67BE5 14SI28 G G LFT 2 D 2 NAI-D 120 65K01 15P 31 E E/ FMF 6 D130- 180 MAG-0 DST 2=1.78 MEV 8 LEVELS

67KU2 14SI28 G G LFT 12 D 11- 13 NAI-0 135 590U1 15P 31 G MU-T ABX 10- 30 C 29, 30 MGC-0 4PI 12=11.42 MEV 60BO3 15P 31 G G LFT C 0- NAI-D 100 57L01 14SI2e G G/ ABX 15- 32 C 34 NAI-D OST J-PI 61BE1 14SI28 G N RLY THR CTHR ACT-I 4PI 51B03 15P 31 G MU-T ABX 11- 20 C 11- 20 ACT-I 4PI THRESHOLD 61BU4 15P 31 6 G ABX 15- 30 C 32 NAI-D 140 63CA1 14SI28 G N ABX 17- 30 D 15- 30 BF3-I 4PI 72 62B06 15P 31 G G LFT C 0- NAI-D 110 68C01 14SI28 G N RLX THR- 65 C 13- 65 ACT-I 4PI J-PI. WIDTH

70WE1 14SI28 G ,N ABX 17- 32 C 17- 32 ACT-I 4PI 356 64801 15P 3 1 G G LFT 3 C 1- NAI-D 100 61SH1 14SI28 G P SPC 14- 24 C 24 EMU-D UKN ABI 62B1 1 14SI28 G P SPC 18 0 18 SCD-D OST 66H02 1 5P 31 G G LFT c 1 NAI-D 117 54UL3 14SI28 6 P SPC IS- 23 C 24 SCD-D 4P1 1=1.26 MEV

65BI 1 145128 G P RLX IS 0 18 SCO-D 4PI 68CR1 15P 31 G G LFT 3 c 3 ANI-D 135 65CA2 14SI28 G P ABX THR- 23 C 16- 23 SCD-D 4P1 3=3.13 MEV 65MA5 14SI28 G P ABX 17- 22 0 17- 22 SCD-D 4PI 68H01 15P 31 G G LFT 7- 8 0 7- 8 NAl-D 0 69AN6 14S I 28 G P ABY 109- 999 C700,999 TEL-0 OST 7 8 = 7 .90.8.201 MEV 999=1.2 GEV 58R01 15P 31 G G LFT 3 C 3 NAI-I 113 69AN6 14S I 28 G D ABY 120- 999 C700.999 TEL-D OST SELF-ABSORPT ION 999=1.2 GEV 69RA3 15P 31 G G LFT 3 C 3 NAI-D OST

52BI 1 14SI28 G A SPC 18 D 18 SCO-O DST 3=3.51 MEV 65BI1 14SI28 G A RLX 18 0 18 SCD-0 4PI 705H2 15P 31 G G LFT 6 c 14 SCO-D UKN 65CA2 14SI28 G A ASX THR- 23 C 16- 23 SCD-0 4PI 6=6.381 MEV 65MA5 145 I 28 G A ABX 17- 22 D 17- 22 SCD-0 4PI 72SH2 15P 31 G G/ SPC 0- 14 c 14 SCO-D 87 68ME1 145128 G A ABX 15- 22 D 5- 14 NAI-D OST 77+

28
NUCLIDE REACT ION RES exciT SOURCE DETECTOR NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

Rfc'F 2 A I N »OUT TYPE ANG NUM REF Z A I N .OUT TYPE ANG

55BA2 1 5P 3 1 G iN RLY 12- 1 3 C 12- 13 ACT-I 4PI 60CH1 15S G .XT RLY THR- 90 C 90 TEL-I 90 THRESHOLD REL TO DEUTERONS

57BA3 1 5P 3 1 G • N ABY 11- 1 4 C 11- 14 ACT-I 4PI 66H03 16S G .A SPC THR- 31 C 31 SCD-D 130 BREAKS 59N01 165 G .NA24 ABY 78- 999 ClOO-999 ACT-I 4P

I

58CH2 1 5P 3 1 G *N RLY THR CTHR BF3-I 4PI 999=1.2 GEV THRESHOLD 71SA2 16S G .NA24 ABX THR- 250 C 20-250 ACT-I 4P

I

60&E3 1 5P 3 1 G tN NOX THR CTHR ACT-I 4PI THRESHOLD 56HE3 16S 32 E . E/ FMF 1- 7 D187 MAG-D DST 51SA1 1 5P 3 1 G *N RLY 12- 14 C 12- 14 ACT-I 4PI 61BI 1 16S 32 E . E/ FMF 0- 4 D15U MAG-D 135 THRESHOLD MULT I POLAR I TY 62EM1 1 5P 3 1 G *N SPC 10- 30 C 30 EMU-D DST 63BA1 1 6 S 3 2 . E / SPC 0 — 22 D 42 MAG-D 180 63MC3 1 5P 3 1 G »N ABX 12- 24 C 12- 24 ACT-I 4PI G-WIDTH

67GE2 1 5P 3 1 G N ABY THR- 27 C 22 , 27 BF3-I 4PI 64L01 165 32 . E / FMF Q — 9 D120-180 MAG-D DST 71FR1 1 5P 31 G «N ABY 12- 800 ClOO-800 ACT-I 4PI J-P I 62MU2 I 5P 31 G tXN ABX 12- 24 c 24 8F3-I 4PI 69DE8 165 32 . E / ABX 0- 200 D999 MAG-D DST 63601 15P 31 G ,XN ABX 13- 28 c 10- 30 BF3-I 4PI QUASI-EL, 999=1.11 G 63C03 15P 31 G .XN ABX 13- 80 c 80 BF3-I 4PI 69GU3 16S 32 E .E/ FMF 1 3- 31 D120-200 MAG-D DST 67M12 15P 31 G .XN SPC THR- 20 c 23- 27 TOF-D 100 70ST2 165 32 . E / ABX 4 D 58. 59 MAG-0 105 623H12 15P 31 G ,P SPC 10- 19 c 19 EMU-D 4PI 4=3.78 0+ 66IS2 15P 31 G ,P SPC THR- 34 c 18 . 34 EMU-D 30 55AM2 165 32 E .E/P RLY 0- 120 D500-530 MAG-0 51 590C1 1 5P 31 G .2P RL 1 THR- 100 CTHR-100 ACT-I 4PI 100 MEV P COINC

REL TO G.N 62006 165 32 G .G LET 0- 4 c 0- NA I -D 1 1

0

70AN2 15P 31 G .2P ABX 23- 63 C 23- 63 ACT-I 4PI J-P I 71SA2 ISP 31 G .3P ABX THR- 250 C 20-250 ACT-I 4PI 67L01 165 32 G .G/ ABX 14- 32 C 34 NAI-D DST

51SH'» I 5P 3 1 G .XP SPC 9- 24 C 24 EMU-D DST 59FA1 165 32 G .N ABX 15- 30 C 30 ACT-I 4PI ABSOLUTE YIELD 60FE 1 165 32 G .N ABX 15- 30 C 31 ACT-I 4PI

6'* I SI 1 5P 3 1 G XP ABX T hR- 3 2 C 15- 32 SCI-D UKN 62F I 3 16S 32 G .N RLY 16- 28 C 32 TOF-D UKN

1 5P 3 1 G XP SPC THR- 2 7 C 22. 27 SCD-D 90 62<U1 165 32 G N ABX 1 5- 25 C 12- 27 ACT-I 4PI 68 SH 3 1 5P 3 1 G XP SPC THR- 1

9

D 19 EMU-D DST 6 2MI5 165 3 2 G . N SPC 15- 30 C 30 EMU-D DST SgOCl 1 5P 3 1 G N2P RL I THR- 100 CTHR-100 ACT-I 4PI 62MU2 165 32 G >N ABX 15- 22 C 12- 24 BF3-I 4PI REL TO G.N 65TH1 165 32 G N ABX THR- 22 C 15- 22 ACT-I 4PI 70AN2 1 5P 3 1 G 2PN ABX 2 3- 63 C 23- 63 ACT-I 4PI 66BI 1 165 32 G N ABX 20- 200 c 20-200 BF3-I 4PI 60WA2 15P 3 1 G 6N6P ABX THR- 240 C240 ACT-I 4PI 67WE1 155 32 G N ABX THR- 32 c 20- 32 ACT-I 4PI 60602 15P 31 G NA2<t ABX 30- 260 C 3J-260 ACT-I 4PI 67WE2 155 32 G N ABX 20- 32 c 20- 32 ACT-I 4P1 INCLUDES G.HE4N2P 68C01 155 32 G N RLX THR- 65 c 13- 55 ACT-I 4PI 69N01 15P 31 G NA24 ABY 69-999 ClOO-999 ACT-I 4P1 70IS2 16S 32 G NG SPC THR- 32 c 32 SCD-D 135 999=1.2 GEV LEVELS 1.26.2.23

71SA2 15P 31 G NA2'i ABX THR- 250 C 20-250 ACT-I 4PI 70TH1 165 32 G NG ABX THR- 29 c 29 SCD-D 125 62TU1 15P 31 P G NOX 8- 9 0 1- EMU-D DST 60FE1 165 32 G XN ABX 12- 31 c 31 MOD- I 4P I J-P I 52B03 165 32 G XN ABX 15- 90 c 30- 90 BF3-I 4P I 6*TU1 1 5P 3 1 t P G NOX 10 0 3 EMU-D 90 57AN2 165 32 G XN ABX THR- 26 c 13- 26 BF3-I 4PI J-P I . POL OF G 70AN3 16 5 3 2 G X N ABX 15- 62 c 16- 52 ACT-I 4PI 66VA2 15P 3 1 P G SPC 8- 10 D 1- 2 NAI-D DST (G.NI+(G.2N)

67B01 1 5P 3 1 p G NOX 9- 10 0 2- 3 NAI-D 55 6 1 FO

1

1 6 S Q p SPC 10- 30 c 30 EMU-D UKN

68W01 1 5P 3 1 p 6 SPC 0- 9 D 1- 2 SCO-D 90 70 I S2 16S 32 G PG SPC THR- 32 c 32 SCD-D 135 69W I 1 1 5P 3 1 P G LET 10- 1 1 D 3- 4 NAI-! 55 LEVELS 1.25.2.23

G-G CORRELATION 70TH1 165 32 G PG ABX THR- 29 c 29 SCD-D 125 68SH3 165 32 G XP SPC 17- 20 D 17. 20 EMU-D DST

55VI 1 15S 32 G D ABX 19- 22 c 17- 22 ACT-I 4PI INCLUDES G.NP

58G03 155 32 G D RLY 19- 22 c 16- 22 ACT-I 4PI SULFUR Z = 16 REACTION UNCERTAIN

55DE1 16S 32 G NP ABX 18- 22 C 18- 22 ACT-I 4PI 58G03 155 32 G NP RLY 21- 22 C 16- 22 ACT-I 4PI

A ABUND. ( 1

)

SEPARATION ENERGIES ( MEV 1 REACTION UNCERTAIN

G t N G

«

P G ,T G.HE3 GiA G.2N G.NP G.2P 59FA1 165 32 NP ABX 2 0- 30 C 30 THR-I

32 95. 30 15 , 1 8

.

9 24 . 0 19.1 6.9 28.1 21.2 16.2 59FA1 165 32 G NP ABX 21- 30 C 30 ACT-I 4PI

33 0. 76 8 .6 9, 6 21.3 17.1 7 . 1 23.7 17.5 18.2 60FE 1 16S 32 G NP ABX 21- 31 C 31 ACT-I 4PI

22 1 1 .4 10. 9 20 . 4 21.

S

7.9 20.1 21.0 20.4 62B03 165 32 G NP ABX 20- 90 C 30- 90 ACT-I 4PI

36 1 2 1 9 • 9 * 19 . 3 « 9.0 16.9 21.2 65VA3 165 32 G NP ABX 50- 300 c 50-300 ACT-I 4PI 71BR1 155 32 G NP ABX 19- 30 c 19- 30 ACT-I 4PI 60WA2 165 3 2 G 6N7P ABX THR- 240 C240 ACT-1 4PI NUCLIDE REACTION RES EXCIT SOURCE DETECTOR 7 100 2 165 32 G P I + RLY 150- 500 C500 CCH-D DST

RtF Z A IN OUT TYPE ANG NUM p; -/P1+ YIELD RATIO

62BE4 1 6S 3 2 p (3 ABY 9- 10 D 0- NAI-D DST

7 IFAl 16S E E/ ABX 8- 12 D 39 , 56 MAG-D 180 J-PI

5 LEVELS 62NE 1 165 32 P G RLY 9- 10 D 0- NAI-I 90 59<01 16S G MU-T ABX 12- 30 C 31 NAI-O 4P

I

J-PI 590U1 16S G MU-T ABX 11- 30 C 29. 30 MGC-D 4PI 63CH1 16S 32 P C SPC 9- 10 D 0- NAI-D DST 65WY1 16S G MU-T ABX 10- 35 C 90 SCI-D 4PI 43+ J-P I 68D01 16S G MU-T ABX 10- 30 C260 MGP-D 4PI 63KI2 165 32 P G ABX 17- 22 D 8- 14 NAI-I DST 56FU1 165 G G ABX 4- 40 C 4- 40 NAI-D 120 63SP1 165 32 P G NOX 9- 10 0 0- NAI-D DST 60RE1 16S G G ABX 7 D 7 NAI-D 90 J-PI. G-WDTH

61T01 16S G G ADX 4- 1 3 C 5- 13 NAI-D 120 64SM1 165 32 p G ABY 9- 10 D 0- NAI-D DST b^QQ 1 16S G G LET 1- 3 C 1- NAI-D 100 J-PI. WIDTHS

ABI 650E1 16S 32 p G ABX 10- 21 D 2- 12 NAI-D DST 63801 16S G N ABX 12- 28 C 10- 30 BF3-I 4PI 56H01 165 32 p C SPC 1 0 0 1 NAI-D 55 68KA1 16S G N ABX 50- 85 C 55 . 85 TOF-D 67 69MA5 165 32 p G ABX 18- 21 D 9- 12 NAI-O DST NEUT ENGY SPEC 69P I 1 165 32 P C LET 4- 1

1

0 1- 2 SCD-D DST 70WU1 16S G N ABX 16- 19 c 16- 22 TOF-D 90 72C02 165 32 p G LET 9- 1 1 D 0- 2 SCO-D 56 GROUND STATE J-PI 63C03 16S G XN ABX 14- 80 c 0- 80 BF3-I 4PI 72ES1 165 32 P G LFT 6- 8 D 3- 6 SCD-D UKN 63MU2 16S G XN ABX 15- 22 c 15- 22 SCI-D 90 LEVEL IS 5.550 MEV SPECTRUM 64SM1 16S 32 A G ABY 9- 10 D 2- NAI-D DST

6<*F I 1 16S G XN SPC THR- 25 c 23. 25 TOF-D 70 J-PI. WIDTHS

68G06 16S G XN ABX 14- 30 c 14- 30 6F3-I 4PI 432 7 ICHl 165 32 A G LFT 10- 12 D 4- 6 SCD-D DST 71C02 16S G XN AB I 36- 64 c 10- 64 BF3-I 4PI J-PI FAST N YIELD

62SH11 16S G p ABX 9- 24 c 9- 24 SCI-I DST 67BE7 165 3 3 N G LFT 8- 9 D 0- 1 NAI-D 90 66L 1 1 16S G P SPC THR- 32 c 32 SCI-D 90 SOURCE 30.111 KEV 671S1 16S G P ABX THR- 35 c 22- 35 EMU-D DST 71SA2 16S G 4P ABX THR- 250 c 20-250 ACT-I 4PI 62B06 16S 34 G G LFT 0- 4 C 0- NAI-D 110 60CH1 15S G XP RLX THR- 90 c 90 TEL-I 90 J-PI REL TO OEUTERONS 65MC2 165 34 A G RLY 11- 12 D 3- 4 NAI-D DST 61MA2 15S G XP NOX 9- 21 c 21 SCI-D DST 6 7W I 1 165 34 A G LFT 11- 12 D 4- 5 NAI-D DST

53SHi. 16S G XP SPC 11- 24 c 24 EMU-D U<N

16S G XP ABX THR- 32 c 15- 32 SCI-D U^N 66K04 165 35 P G NOX 10- 1

1

D 1- 2 NAI-I DST 58AB5 16S G XP SPC THR- 24 c 21- 24 SCD-D 90 SPINS

69AB1 15S G XP SPC THR- 26 c 26 SCD-D 90 55RI 1 15S G D RLY THR- 65 c 65 CCH-I 4PI RLY TO PROTONS

60CH1 16S G XD RLX THR- 90 c 90 TEL-I 90 REL TO PROTONS

29
CHLORINE Z=17 NUCLIDE REACTION RES

Z A IN. OUT DETECTOR

TYPE ANG NUM

SEPARATION ENERGIES (MEV) G.N G.P G. T G,HE3 G.A G.2N G.NP G.2P 57K02 18AR40 G XP NOX THR- 90 C 90 CCH-D

35 75.53 12.6 5.4 17. 9 19.5 7.0 24.2 17.8 17.3 SeiAl 18AR40 G XP ABI 12- 70 C 70 CCH-D

37 2*. 47 10.3 8.4 15. 8 21.9 7.8 18.9 18.3 69H01 18AR40 G XP ABY THR- 33 C 24- 33 SC I-D 59EM2 18AR40 G A ABX 5- 12 c 23- 30 EMU-D

61K01 18AR40 G A SPC 10- 17 c 70 lON-D

NUCL 1 DE REACTION RES EXC I T SOURCE DETECTOR 55RE1 18AR40 G A ABX 9 D 9 CCH-D

REF 2 A IN .OUT TYPE ANG NUM 55WE2 18AR40 G A ABX 7- 33 c 33 SCD-D

59BR1 18AR40 G NP ABI 21- 34 C 34 ACT-I 66BE3 17CL G.G RLX 5- 10 D 5- 10 NAI-D 135 59PE1 18AR40 G NP ABX 19- 40 C 14- 44 ACT-I 55ER1 17CL G.A ABY THR- 31 C 32 EMU-I 4P

I

69N01 17CL G.NA24 ABY 104-999 ClOO-999 ACT-I 4P I 999=1.2 GEV

6 0DO1 65EH1 leAR40 G. 18AR40 Gi ABI 21- 33 C ABY THR- 31 C

DST

DST

90

90

90

4PI90

SYNTHESI

S

34 ACT-I 4PI

31 ACT-I 4PI

59GR1 17CL34 7 D 1 SCD-D OST

5 LEVELS

52806 17CL35 G G LET 0- 4 C 0- NAI-D 110 POTASSIUM Z= 19

65H02 17CL35 G G LFT 1 C 1 J-PI NAI-D 117 1=1.22 MEV A ABUND. SEPARATION ENERGIES (MEV) 55BA3 17CL35 G N RLY 12- 22 C 22 ACT-I 4PI G.N G. P G.T G.HE3 G.A G.2N G.NP G,2P THRESHOLD 39 93.10 13. 1 6. 4 18.5 19.2 7.2 25.2 18.2 16.6 55B02 17CL35 G N ABX 13- 21 C 13- 21 ACT-I 4PI 40 .2 (-2

)

7.8 7. 5 17.5 16. 7 6.4 20.9 14.2 16.3 55DE1 17CL35 G N ABX 13- 21 C 13- 21 ACT-I 4PI 41 5. 88 10.1 7. 8 15.8 20. 7 6.2 17.9 17.7 20.3 THRESHOLD

57BA3 17CL35 G N RLY 12- 14 C 12- 14 ACT-I 4PI BREAKS NUCLIDE REACT ION RES EXCIT SOURCE DETECTOR

59FE1 17CL35 G N ABX 12- 31 C 31 ACT-1 4PI REF Z A . 1

N

OUT TYPE ANG NUM

59FE1 17CL35 G N ABX 16- 31 C 31 THR- I 4PI 61SA1 17CL35 G N RLY 12- 14 C 12- 14 ACT-I 4PI 59SA3 19K E E/ FMF 3. 7 D 99-227 MAG-D DST THRESHOLD B(EL) .3.5.6.5

62KU1 17CL35 G N ABX 12- 25 c 27 ACT-I 4PI 51T0I 19< G G ABX 5- 12 C 5- 12 NAI-D 120 67K02 17CL35 P G LFT 8 D 2 NAI-D DST 59EM1 19K G XN SPC 7- 31 C 31 EMU-D OST

J-PI 63C03 19K G XN ABX 12- 80 C 0- 80 BF3-I 4PI 67WA1 17CL35 P G LFT 8 D 2- SCD-D 4PI 59N01 19K G NA24 ABY 140-999 ClOO-999 ACT-1 4PI

59SE1

67BE7 17CL36

62B05

60GE3

57IE1

17CL37

17CL37

17CL37

N .G

G.G

G.N

P .G

SPC

LFT

LFT

NOX

LFT

0-

THR

9-

C

9 0

4 C

0 NAI-D 90 G-WIDTH

0- 1 NAI-D 90 SOURCE 25.50 <EV

57G02 19< 37

0- NAI-D 110 J-P I CTHR BF3-I 4PI THRESHOLD

10 D 1- 2 NAI-D 55

63BA1

70PE1

19K 39 19K 39

E .E/

E .E/ SPC ABX

0 42

D 60

52B05 19< 39

57L01 55B02

55DE1

50GE3 19K 39

999=1.2 GEV

5 SCO-D OST

J-P I

MAG-D 180 MAG-0 DST

7 LEVELS NAI-D 110

J-PI

19K 39 G G/ ABX 14- 32 C 34 NAI-D DST

19K 39 G N ASX 13- 21 C 13- 21 ACT- I 4P I 19K 39 G N ABX 13- 21 C 13- 21 ACT.-

I

4PI

ARGON Z=le

A ABUND. SEPARATION ENERGIES (MEV) G.N G.P G.T G.HE3 G.A G.2N G.NP G.2P

35 0.34 15.3 8.5 24.2 18.5 6.5 28.0 21.2 14.9

38 6.3(-2} 11.8 10.2 20.7 20.8 7.2 20.6 20.5 18.6

40 99.5 9.9 12.5 18.2 23.1 6.8 16.5 20.5 22.8

REF

72FA1

59H01

64ER1

NUCLIDE REACTION RES EXCIT

Z A IN. OUT

18AR36

18AR36

67ME3 18AR36 P .G RLX 12- 19 D 4- 70<E1 18AR3S P .0 RLX 14- 20 D 6- 64ER1 18AR36 A .G RLY 8- 10 D 2-

55EH1 18AR38 G N ABY THR- 31 c 18- 31 ACT-I 4PI 70KE1 18AR38 P G RLX 14- 22 D 4- 12 NAI-D 90 245 64ER1 leAR38 A G RLY 9- 10 0 2- NAI-D DST J-PI. WIDTHS

54PH1

72CH1

59PE1 18AR40

13 D 39

.

J-PI. G- ABY THR- RLY 8-

E DETECTOR

TYPE ANG NUM

56 MAG-D 180 WIDTH. 8 LEVS

33 C 24- 33 SCI-D 90

10 D 2- NAI-D DST J-PI. WIDTHS

12 NAI-D DST

12 NAI-D 90 244 NAI-D DST J-PI. WIDTHS

52G03

65C01

55C03

59WE1

70KA2

71WE1

58KE1

580P2 62SH9

69H01

60H01

19K 39

19IC 39

19K 39 19< 39

19K 39 19< 39

19K 39 19K 39 19K 39 19K 39 19K 39

G.N G.N

G.N

G.N

G.N

G.N

G.P

G.P

G.P

G .XP

G .D

ABX 14- ABX THRABX THR- RLX 13-

ABX

ABX

ABX 18 ABX 18 SPC 5- ABY THR- ABY 20-

120

30

C 14-

C 12-

THRESHOLD

ACT-I 4PI THRESHOLD

24 ACT-I 4PI

70 ACT-I API ISOMER RATIO

ACT-I API

29 ACT-I API

TO 123 KEV ISOMER

C 15-140 ACT-I API

C 13- 30 ACT-I API G.N TO ISOMER

18 SCI-D 4PI

18 SCI-0 4PI

24 EMU-D 4P! 24- 33 SCI-D 90 20- 25 ACT-I API REACTION UNCERTAIN

60H01 19K 39 G NP ABY 20- 25 C 20- 25 ACT-I API REACTION UNCERTAIN

55C03 19K 39 G NP ABX THR- 80 C 80 ACT-I API 55SC2 19K 39 G NA ABY THR- 32 C 32 ACT-I 4PI 57ER1 19K 39 G NA ABI 1 3- 32 C 32 ACT-I API

71BL1 19K 41 G P I + ABY 150- 700 C15J-700 ACT-I API SEE 68 NY 1 53K02 19K 41 P G RLY 9 D 0- NAI-D OST SEPARATED ISOTOPES

G RLY 99- 11 D 3-

G ABX 10- 12 D

NAI-D DST J-PI. WIDTHS

4- 5 NAI-D DST

12 LEVELS. J-PI CALCIUM Z=20

56HE3 18AR40 E E/ FMF 1- 7 0187 MAG-D OST 63BA1 18AR40 E E/ SPC 0- 24 0 42 MAG-0 180 A ABUND. SEPARATION ENERGIES (MEV) 62D01 18AR40 E P SPC 13- 30 C 30 MAG-D 75 G.N G.P G.T G.HE3 G.A G.2N G.NP G.2P SEPARATED ISOTOPE

10- 23 C 14-

50FA1 ISARAO G N ABX 1 3- 49 C 10 72L02 18AR40 G N ABX 10- 13 D 13 59PE1 leARAO G 2N ABX 17- 23 C 14

55SP3 18AR40 G P SPC THR- 23 C 23 55K01 18AR40 G P NOX 12- 90 C 90 58GU1 18AR40 G P SPC 13- 15 C 15 59BR1 18AR40 G P ABI 12- 34 C 34 59EM2 18AR40 G P SPC 10- 30 c 23 59PE1 1 8AR40 G P ABX 13- 33 c 14

60D01 18AR40 G P ABI 12- 33 c 30 51FI1 IBARAO G P RLY 0- 35 c 35 65RE1 18AR40 G P ABX 9 0 9

44 ACT-I API SYNTHESIS

50 BF3-I 4PI TOF-0 90

44 ACT-I API SYNTHESIS

EMU-D OST CCH-I CCH-D

ACT-I API

30 EMU-D 90

44 ACT-I API SYNTHESIS

34 ACT-I API SCI-D 90 CCH-D 4PI

40

4243

44

45

46

95.97 15.5 0.54

0.15

2.05 3.3(-3) 0.19

11.5

7.9

11.1

10.4 10.0

8.3

10.3

10.7 12.2

13.8

15.8

25.0 18.8 7.0 29.0 21.4 14.7

19.7

19.8 20.9

21.5

22.6

20.2

18.3 23.3

6.2

7.6

8 . 8 11.1

19.8 20.4

19.4 18.2

19.1 21.8

17.8 22.7

17.2 24.2

18.1 19.9 21.6

DST

DST NUCLIDE REACTION RES

Z A IN. OUT SOURCE DETECTORTYPE ANG NUM

61PE1 20CA40

628L1 20CA40

52E01 20CA40

E .E/ E.E/ ABX 11- FMF 0- 25 D120-180 MAG-D OST

9 0120-220 MAG-D DST

7 LEVELS

0 A2 TEL-D 150

NO EXCITATION OBS

30
REF NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

Z A IN. OUT TYPE AN& NUM NUCLIDE REACTION RES

REF Z A IN. OUT EXCIT SOURCE DETECTORTYPE AN& NJM

6 3BA

1

20C A40 E E/ SPC 0- 2 3 D 42 MAtj— U loU 6 1 PO

1

2 OC A40 P G RLY 9- 1

C

D 1— NAI-D U^N

J-P I 6 1 TA2 2 OC A40 P G RLY 18- 2 2 D 9— 15 NAl— D 100 63BL 1 20CAitO E E/ FMF 0- 1 1 D120- 220 MAG-D 100 6 2 R A

1

UL AA u G SPC ^~ 1

0

0 1 NAIU Uol 6^H0 1 2 0CA40 E E/ A3X 10- I 7 D 80- 200 MA6-D DST 1 DI l~ l^(I^^TLJ J — HI. b — WlUIn

65CR 1 20CAifO F E/ ABX 3- 5 D250 MAG-D DST 64HA

1

2 OC A40 P G ABX 14- 2 3 D 6- 15 SCI-0 90

sur It LEVELS DETAILED BALANCE

66AR2 20CA40 E E / L F T 7 D MAG-D DST 64S I 1 2 0 C A4 0 P G NOX 9 - 1

0

0 1 — NA I — D DST

7 =6.89 MEV J-PI 68Z I 2 20C A40 E E/ ABX 2- 2 5 0283 MAG-D 88 64TA1 20CA40 P G ABX D 9- 14 NAI-0 100 69E I 1 2 t-iC A40 E E / FMF 3 - 5 D 61 MAG-0 DST 66L E 1 2 OC A40 P G SPC 9- 1

1

D 1- 3 NAI-D 55 B(EL) .3.7-4.5 6 7F E

1

2 OC A40 P G ABX 18 — 2 3 0 10- 15 NAI-D 90 192 70GO3 2 OC A40 E E/ ABX 15- 26 D 55 MAG-D DST 68BA1 2 0CA40 P G R LX 11- 1 A D 3- 6 NAI-D 0 196

7 0 I T 2 2 OC A4 0 E E / FMF 0

— 25 0183* 250 MAG-D DST 3=2.88.6=6.03 MEV LEVELS 3-9 MEV c u L A A u G ABX 14 D 2- 6 NAI-D OST

7 S 2 i? nV r MA H nU E / ABX 3 D 54. 5 9 MA 0 U 14 1 3=3.35 0+ 7 1 HE 1 2 OC A42 £ / FMF l — 0198-300 MAG-D DST

7 1 F A 1 2 0 C A4 0 E / ABX 5- 1 1 D 39 . 56 MAG-D 180 3 LEVELS

4 LEVELS 66 2 0 2 NAI-D 90

7 1 HE 1 o n /" A A E E / FMF 4 D198- 300 MAG-D DST 2=1.52 MEV

3 LEVELS 42 D 1- NAI-D UKN

7 1 MO 3 if Ut. Am-U E E / 240 D500 MAG-D 60 SEPARATED ISOTOPES

6 6 AM 1 2 0 C A40 E E / P SPC 0- 120 D560- 760 MAG-D 51 71BU2 20CA40 E E/P ABX 5- 85 D500 MAG-D 51 71 HF 1 £ U I.W M H H D198-300 MAG-0 DST

PROT P = 25 . 100 MEV/C 5 LEVELS

59DU1 20CAifO G MU-T ABX 11- 30 C 29» 30 MGC-D *PI 58BR1 9 A A /i /. G * A B I C 31 ACT-I API 65D0

1

20CAi*0 G MU-T ABX 10- 28 C260 MGP-D iiP] 680k3 ^ U L Ahh G » P ABY T 2 0 C 20 ACT-I API 65WY

1

2 OC A40 G MU—

T

ABX 10- 70 C 90 SCI-D 4PI 66D02 2 0 CA4 0 G MU—

T

ABX 8- 30 C26 j MGP-D 4PI 68Z I 2 2 u C A 4 0 ABX 2^ D283 MAG-0 88 68BE4 20CA40 G MU-T ABX 10- 30 C 35 MGC-D 4PI 102 + 69E I 1 20CA48 E E/ FMF 3- 5 D 42 . 61 MAG-D OST

56FU1 20CA40 G G ASX 4- 40 c 4- 'tO NAI-D 120 BIEL) ,3.7-4.5

6 1 BU3 2 0 C A4 0 G G ABX 15 — 32 c 32 NAI-D DST 69 L A 3 2 0CA48 G N ABY 10- 5 5 C 39- 55 ACT-I API SEE 61BU4 A6Y UPPER LIMIT

6 1 BU4 0 nUL^ A /. A A'+U G G 30 c 27 , 32 NAI-D OST

6 lECl "5 n A /. n ^ U H*+ u G NOX n 0 10 NAI-D DST

J-PI , G-WIOTH

6 1 TO 1 2 OC A40 G G A B X 6

— 12 c 6- 12 NAI-D 120 62B06 i U L A4 U G LFT 0- if c 0- NAI-D 110 SCANDIUM Z = 21

6 8ME 2 £ U Ah- U G G FT D 7 J-PI SCD-D DST

J- PI 6.91 .6.95 MEV A ABUND

.

SEPARATION ENERGIES (MEVI

6 7L0 1 20C A40 G G/ ABX 14- 30 C 34 NAI-0 DST G • N G. P G .T G.HE3 6. A G.2N G.NP G

«

6 0 KU2 2 OC A40 G N R L Y 15 — 90 C 90 TEL-I DST 4 5 10 0.00 11 . 3 5. 9 17.5 21.0 7.9 21.0 18.0 1

9

6 2 F I 3 £. UL A4U G N RL Y 16 — 28 c 32 TOF-D UKN

6 2M I 2 20C A40 G N ABX 15- 23 0 15- 25 BF3-I 4PI

6 3M I 2 2 UCA4 0 G N ABX 15- 26 c 15- 30 BF3-I API NULL 1 Dt REACT I ON RES EXCIT SOURCE DETECTOR

64 BA

1

20 C A40 G N ABX 15 — 30 c 15- 30 ACT-I API REF Z A I N OUT TYPE ANG

AQU

' ?

"5 n r A n 26 D 15- 26 aF3-I 4PI

<; u i_ Mt u N ARX 17 — 24 D 15- 2* TOF-D 90 2 00+ 6 1 BU

1

2 1 SC 4 1 P G AB I 1- 3 D 0- ACT-I API

£ u L A U 1 8- 20 c 16- 22 TOF-D 90 GROUND STATE 66 T A

1

2 1 SC4 5 G N RLY THR- 48 C 24- 46 ACT-I API

fe9UL 1 2 OC A40 G NG AB Y T HR — 32 c 32 SCD-D 120 66WA1 2 1SC45 G N RLY THR- 300 c 50-300 ACT-I 4PI

59 EM 1 2 OC A40 G XN SPC 7 — 31 c 31 EMU-D 90 ISOMER RATIO SC44

60FE 1 20CA40 G XN ABX 12- 3 1 c 31 ACT-I API 2 1 SC45 G N ABY 1 1- 48 c 48 ACT-I API

60 L I 2 2 OC A40 G XN AB I THR- 34 c 34 NAI-I 4PI 67BEa 2 1 SC 4 5 G 2N ABY 21- 46 c 48 ACT-I 4PI

6 3C0 3 2 OC A40 G XN ABX 15- 80 c 0- 80 BF3-I 4PI 6 7BE 8 2 1 SC4 5 G 2P ABY 19- 48 c 48 ACT-I API 64F I 1 2 OC A40 G XN SPC T HR — 32 c 25 . 32 TOF-0 70

66 AN 1 <: OC Ah U G 16 — 62 c 16- 62 ACT-I 4PI 19 3 660U2 2 1 SC49 P G SPC 10- 1 1 0 1 NAI-D DST

66 BA 1 2 OC A4 0 G vw ABX 15 — 50 c 15- 50 BF3-I 4PI 67CH1 2 1 SC49 P G LFT 12 D 2 SCD-D 90 66F I 2 ^ U Ah U G SPC

1 Aft" 65 c 65 TOF-D 90 7 1 P A3 2 1 SC49 P G REL 13- 27 D 4- 18 NAl-D 105

6 7F E 2

~> f\ r \ I, f\

^: UL Ah U G XN AO Y 100 — 150 C150 BF3-I 4PI

? I'l A z. 1*1 ^ U M H U 27 c 22, 27 BF3-I 4PI

6 7G0 3 ^? nU

("

^_ HA £1H nU ^ XN A8X 15 — 30 c 15- 30 BF3-I 4PI 185 + 67M 1

2

^: U L AhU G SPC THR- 20 c 23- 27 TOF-D 100

6 8G06 U L A H U G XN ABX 15 — 30 c 15- 30 BF3-I 4PI TITANIUM Z = 22

7 1 I S

1

2 0 C A4 0 G XN ABX 15- 26 c 16- 26 BF3-I 4PI 414

5 9K.02 2 OC A4 0 G P SPC THR- 85 c 85 EMU-D DST

6 20R

1

"> A ^ A y. A ^ u 0. Ah u G SPC 8 — 22 c 22 EMU-D DST A ABUNO

.

SEPARATION ENERGIES (MEV)

6 2 JO 1 ^: U L A H U G SPC ^~ 21 c 20 . 21 EMU-D DST G .N G. P G ,T G.HE3 6. A G.2N G.NP G

»

6 25H 1

2

<: Ut- AHU G

D SPC 10 — 21 c 21 EMU-0 UKN 46 7.93 13 .2 10. 4 22 .9 20.7 6.0 22.7 21.7 1

7

64 I S2 ^ U L A H U G ABX 14- 32 c 14- 32 EMU-D DST 47 7.28 8 .9 10.5 22 . 1 18.4 9.0, 22.1 19.2 1

8

SPC 48 7 3.94 11 . 6 11. 4 22 , 4 22.6 9.4 20.5 22.1 1

9

64153 0 A /" A A UL AhU G ABX THR 34 c 18- EMU-D DST 49 5.51 8 . 1 11. 4 21 .7 20.4 10.2 19.6 19.6 20 64R A2 A ^ A A U L Ah U G AB X 14 — 27 c 30 SCl-I DST 5 0 5.34 10 .9 12. 2 22 . 1 24.0 10.7 19.1 22.3 2 1 INCLUDES G.NP

65 I SI ^ u L AH U G SPC 25 c 18- 25 EMU-D DST

6 7DR2 2 OC A^O G SPC T HR — 19 c 16- 19 EMU-D DST NUCLIDE REACT ION RES EXCIT SOURCE DETECTOR

6 7G04 2 0 C A^tO G ABX THR- 30 c 12- 30 SCD-D UKN REF Z A IN OUT TYPE ANG NUM

6 8G0

1

^ UC Ah U G ABX 30 c 12- 30 SCD-D 10 18 7

^ U AH U ^

r A^

17 24 D 15- 2* SCD-D 90 199+ 66BE 3 2 2 T I G G RLX 5- 10 D 5- 10 NAI-0 135

7 1 Sn5 A /" A A ^ U(_ Ah u G p SPC 12- 25 c 18- 26 EMU-D DST 70 AR

1

22T I G G ABX 12- 30 C 32 NAI-D OST 69U L 1 A A V. A ^ U L A H U G PG AB Y THR- 32 c 32 SCD-D 120 RATIO 6.G/T0 2+ 62CH2 ^ U L Ah U G XP RL Y 8 — 35 c 35 MAG-O DST 64AL5 22 T I G XN NOX THR- 34 C 34 THR-I DST REL TO OEUTERONS 67C01 22T I G XN ABX 12- 24 C 24 BF3-I 4PI 4 34 ^ ' ^

^ U L AH U G 22 c 22 SCI-I DST 7 1 C02 2 2 T I G XN AB I 36- 64 C 10- 64 BF3-I 4PI

A /" A /. A ^ U L A H U G YP SPC THR~ 20 D 20 EMU-D OST FAST N YIELD

6 2 Cn2 0 .'A ^ A /, A (1 AhU G X D R L Y 19 — 35 c 35 MAG-D DST 6 90K

1

2 2 T I G P RLY THR- 60 C 30- 60 NAI-D API REL TO PROTONS YLD REL 12c IG.N

)

5 8H0

1

2 OC A40 G » NP ABX 2 6 — 32 c 26- 32 ACT-I 4PI 6 3M I 5 22T 1 G XP ABY 8- 22 C 22 SCI-I DST THRESHOLD 64SC 1 22T I G A SPC THR- 33 C 33 SCD-0 90

A 1" A /. A ^ U t, AH U G 31 c 31 ACT-I API ABS YIELD

65VA3 7 n 1^ ft /. A il U >«. A H U G 'np Ab"! 50~ 300 c 50- 300 ACT-I API 7 2KE4 2 2 T I G A RLY 7- 32 C 32 SCD-0 DST 67SM1 20CA40 G »NP ABX 150- 250 C250 TOF-D DST 690M 22T I G SC44 RLY THR- 60 C 30- 60 NAI-D API 70KA2 20CA40 G .NP ABX 20- 140 C 20- 1*0 ACT-I 4PI YLD REL 12C(G.N)

71BR1 20CA40 G ,NP ABX 19- 30 c 19- 30 ACT-I API 690K1 22TI G T 145 RLY THR- 60 C 30- 60 NAI-D API 57SC1 20CA40 G .3N3P ABX 35- 70 c 35- 70 ACT-I API YLD REL 12CIG,N) 69N01 20CA40 G .NA24 ABY 140- 999 ClOU- 999 ACT-I API 690K1 22T 1 G CA47 RLY THR- 60 C 30- 60 NAI-D 4PI 999=1.2 GEV YLD REL 12C(G.N)

71G02 20CA^0 G PI + RLY 150- 500 C500 CCH-D DST

Pl- /PI+ YI ELD RAT 10 71SI 1 22T I 44 A G LFT 8- 9 D 4- 5 SCD-D DST

4 LEVELS

31
NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF L A IN. OUT TYPE ANG NUM REF NUCLIDE REACTION RES EXCIT SOURCE DETECTORZ A IN, OUT TYPE ANG NUM

7 IHE 1 22TIA6 E E/ FMF 1 . 2 0198-300 MAG-D DST 56HE2 23V 51 G 2P RLY THR- 31 C 31 ACT-I 4PI 1=0.885. 2=2.0 REL G.A 63KA1 22TI46 0 G A6X 1 D 1 NAI-D 108 67BE8 23V 51 G 2P ABY 20- 37 C 26- 37 ACT-I 4P

I

58SI4 22TI46 6 N RLX 13- 22 CTHR- 22 ACT-I 4PI 59AB2 23V 5 1 G XP SPC 8- 27 C 27 SCD-D 90 52SH5 22TI46 G N ABX 14- 3 1 (2 14 Mv.l l 4ri 58HA1 23V 51 G XP SPC THR- 30 C 30 EMU-D DST 69GA2 22TI46 G 2N ABX 30, 34 J 1 jy ACJ l 4rl 63M I 5 23V 51 G XP ABY 5- 22 C 22 SCI-I DST 62SH5 22TI45 G NP ABX 22- 31 Q 14— ^1 arT— I 4PI 55HE2 23V 51 G A RLY THR- 31 C 31 ACT-I 4P1 65TA1 22TI45 G NP RLY THR- 48 ^4 48 ALI— 1 4r| REL CU 53 696A2 22TI46 G NP ABX 30, 34 c 31- 39 ACT-I 4PI 57ER1 23V 51 G A ABI 8- 32 C 32 ACT-I 4PI 58T02 23V 51 G A ABY 8- 22 C 22 EMU-I DST 64B01 22TI47 G G LFT 1- 3 c 1- NAI-D 100 59DY1 23V 51 G A ABX 14- 25 C 25 ACT-I 4PI

ABI 5 1CA2 23V 5 1 G A ABX THR- 32 CTHR- 32 ACT-I 4P

I

62SH5 22T I 47 G P A6X 14- 31 c 14- 31 ACT-I 4PI 62KR1 23V 51 G A AB ! 10- 30 C 21. 30 SCD-D 90 67PA2 22T 147 G P RLY THR- 30 c 22. 30 ACT-I 4PI 53KR1 23V 51 G A RLY 8- 30 C 21. 30 SCD-I 90 580K3 22TI47 G P ABY THR- 20 c 20 ACT-I 4PI 57BE8 23V 5 1 G A ABY 10- 37 C 25- 37 ACT-I 4P

I

690K1 22T 147 G P RLY THR- 60 c 30- 60 NAI-D 4PI 68ME4 23V 51 G A ABX THR- 300 C 20-300 ACT-I 4PI YLD REL 12C(G.N) 680K1 23V 51 G A ABY THR- 20 C 20 ACT-I 4PI 62SH5 22T I 47 G 2P ABX 14- 3 1 c 14- 31 ACT-I 4P1 72KE4 23V 51 G A RLY 10- 32 C 32 SCD-D DST 67PA2 22TI47 G NP RLY THR- 30 c 22. 30 ACT-I 4PI 52FU1 23V 51 G NP ABX 20- 28 D 8- 28 BF3-I 4PI QUADRUPOLE MOMENT

71HE1 22TI48 E E/ FMF 1- 3 D198-300 MAG-D DST 67BE8 23V 51 G NA ABY 21- 37 C 25- 37 ACT-I 4P

I

3 LEVELS 68ME4 23V 51 G A3N ABX THR- 300 C 20-300 ACT-I 4PI 72L I 1 22TI48 E E/ FMF 0- 3 D 60-120 MAG-D DST 690<1 23V 51 G SC45 RLY THR- 60 C 30- 50 NAI-0 4PI .99,2.44 MEV YLD REL 12C(G.N) 63AK1 22T 148 G G LFT 2 D 2 NAI-D 150 690K1 23V 51 G SC47 RLY THR- 60 C 30- 60 NAI-D 4PI

SiiBOl 22T 148 G G LFT 1- 3 C 1- NAI-D 100 YLD REL 12C(G,NI

ABI 690K1 23V 51 G SC48 RLY THR- 50 C 30- 60 NAI-0 4PI 62SH5 22T 148 G P ABX 14- 31 C 14- 31 ACT-I 4PI YLD REL 12C(G.N) 580K3 22T 148 G P ABY THR- 20 C 20 ACT-I 4PI 71KU2 23V 51- G SPL ABY THR-999 C800-999 ACT-I 4P

I

6 7P A2 2 2 T 1 48 p RLY THR- 3 0 C 22, 30 ACT-I 4PI y y y — u 1. unv 690K1 22T 148 G P RLY THR- 60 C 30- 60 NAI-D 4PI 68NY1 23V 51 G PI + ABX 140- 700 C140-700 ACT-I 4PI YLD REL 12CIG.N) TI-51 ACT 60ST1 22T I 48 G NP RLX 152- 320 C320 TEL-D 76 68NY1 23V 51 G PI2N ABX 140- 700 C140-700 ACT-I 4PI REL TO H2 CROS SEC CR-49 ACT 62SH5 22T 148 G NP ABX 14- 31 C 14- 31 ACT-I 4PI 67PA2 22T I 48 G NP RLY THR- 30 C 22. 30 ACT-I 4PI

62SH5 22TI49 G P ABX 14- 31 C 14- 31 ACT-I 4PI 67PA2 22TI49 G P RLY THR- 30 C 22, 30 ACT-I 4PI CHROMIUM Z = 24 680<3 22TI49 6 P ABY THR- 20 C 20 ACT-I 4PI 690K1 22TI49 G P RLY THR- 50 C 30- 50 NAI-D 4PI YLD REL 12C(G,N) A ABUND SEPARATION ENERGIES (MEV) 62SH5 22TI49 G NP ABX 14- 31 C 14- 31 ACT-I 4PI G ,N G, P G . T G.HE3 G.A G,2N G.NP 6, 57PA2 22T I 49 G NP RLY THR- 30 C 22, 30 ACT-I 4PI 50 4.31 12 .9 9. 6 23 .2 20. 15 52 83. 75 12 . 0 10.5 22.4 21. a Q4 71^ 71A 18 71HE1 22T I 50 E E/ FMF 1- 5 D198-300 MAG-D DST 53 9.55 7 .9 U. 1 21 .0 18. 20

5 LEVELS 54 2. 38 9 .7 12.4 19 .7 22. 22 58S U 22TI 50 G P RLX 12- 22 CTHR- 22 ACT-I 4P

I

62SH6 22T I 50 G P A8X 14- 31 C 14- 31 ACT-I 4PI 67PA2 22T I 50 G P RLY THR- 30 C 22. 30 ACT-I 4PI NUCLIDE REACT I ON RES EXCIT SOURCE DETECTOR

62SH5 22TI50 G NP ABX 14- 31 C 14- 31 ACT-I 4PI REF Z A I N OUT TYPE ANG NUM 67PA2 22T I 50 G NP RLY THR- 30 C 22. 30 ACT-I 4PI 60RE1 24CR G G ABX 7 0 7 NAI-D 90 70AR1 24CR G G ABX 12- 30 C 32 NAI-D DST RATIO G,G/TO 2+ 57FE2 24CR G N ABY 15- 30 C 14- 30 THR-I 90 VANADIUM Z = 23 56C01 24CR G N SPC 5- 30 C 20, 30 EMU-D 90 THRESHOLD

54C03 24CR G N ABI THR- 80 C 10- 60 BF3-I 4PI

A ABUND. SEPARATION ENERGIES (MEVI 68 Jul 24CR G N NOX THR- 22 C 22 THR-I DST

G ,N G. P C .T G.HE3 G.A G,2N G,NP G,2P 6 1BA2 24CR G XN ABY THR- 22 C 22 THR-I DST

50 0.24 9 .3 7. 9 19 .2 19.8 9.9 20.9 16.1 19.3 54AL5 24CR G XN NOX THR- 34 C 34 THR-I DST

5 1 99. 76 11 . 1 8. 1 18.7 22. 5 10.3 20.4 19.0 20.2 64C02 24CR G XN ABY THR- 80 C 80 BF3-I 4PI 68MC1 24CR G XN SPC THR- 32 C 22- 32 THR-I DST

MIN 1U'.. f r 1L 1T nU Ft. REACTION RES EXC I T SOURCE DETECTOR 24CR50 G G ABX 9 D 9 SCD-D DST

REF I A IN OUT TYPE ANG NUM 9=8. 888, LFT 62DE 1 24CR50 G N ABX 20 D 20 ACT-I 4PI 71KU5 23V G .SPL ABY THR- 999 C 999 ACT-I 4PI 999=1.5 GEV 54BE3 24CR52 E E/ FMF 0- 9 0150,180 MAG-D OST 71KU5 2 3V G PI + ABY THR- 999 C200-999 ACT-I 4PI J-PI 999=2.2 GEV 64B01 24CR52 G G LFT 1- 3 C 1- NAI-D 100

ABI 68F01 23V 49 P ,G LFT 8 D 1 SCD-D DST 60GE3 24CR52 G N NOX THR CTHR BF3-I 4PI ANALOG STATES THRESHOLD

69LE1 23V 49 P G LFT 7- 8 D 1- 2 SCD-D DST 71BA2 24CR52 G N ABX 12- 14 C 12, 14 TOF-D 135

4 LEVELS 70WA3 24CR52 G 2N RLY THR- 305 C150-305 ACT-I 4P

I

59G03 24CR52 G XN ABX 12- 30 C 12- 30 BF3-I 4PI 449 62KE1 23V 51 E .E/ SPC 0- 17 D183-600 TEL-0 DST 70 1 S4 24CR52 G XP ABX 10- 30 C 10- 30 SCD-D UKN SOURCE 183.300,500 PROB 90 DEGREES

50RE1 23V 51 G .G ABX 7 D 7 NAI-D 90 70WA3 24CR52 G PN RLY THR- 305 C150-305 ACT-I 4P

I

70AR1 23V 51 G • G ABX 12- 30 C 32 NAI-D DST RATIO G.G/TO 2+ 64B01 24CR53 G G LFT 1- 3 C 1- NAI-D 100 58CH2 23V 51 G .N RLY THR CTHR BF3-I 4PI ABI THRESHOLD 60GE3 24CR53 G N NOX THR CTHR BF3-I 4PI 60GE3 23V 51 G • N NOX THR CTHR BF3-I 4PI THRESHOLD

THRESHOLD 71BA2 24CR53 G N ABX 9- 12 C 9, 12 TOF-D 135 62FU1 23V 51 G .N ABX 11- 28 D 8- 28 BF3-I 4PI 433 71JA1 24CR53 G N RLX 7- 9 C 7- 9 TOF-D DST QUADRUPOLE MOMENT 580K3 24CR53 G P ABY THR- 20 C 20 ACT-I 4PI 68JU1 23V 51 G ,N NOX THR- 32 C 32 THR-I DST 71RA1 24CR53 G P RLY 11- 14 C 11- 14 ACT-I 4PI 62FU1 23V 51 G .2N ABX 20- 28 D 8- 28 BF3-I 4PI 443 QUADRUPOLE MOMENT

67SE8 23V 51 G ,2N ABY 20- 37 C 25- 37 ACT-I 4PI 67BE8 23V 5 1 G ,3N 30- 37 C 37 ACT-I 4PI 690K1 23V 51 G ,3N RLY THR- 60 C 30- 60 NAI-D 4PI YLD REL 12C(G,N)

5eKAl 23V 51 G ,XN ABX 12- 22 C 12- 22 BF3-I 4PI 61BA2 23V 51 G .XN ABY THR- 22 C 22 THR-I DST eSGAl 23V 51 $ G .XN SPC THR- 85 C 85 CCH 135 NEUT POLARIZATION

69GA3 23V 51 G .XN SPC 12- 85 C 85 CCH-D 135 69603 23V 51 G ,XN ABX 1 1- 30 C 11- 30 BF3-I 4PI 448

32
MANGANESE Z=25 NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN. OUT TYPE ANG NUM

A ABUND. SEPARATION ENERGIES (MEV) G.N G, P Gi.T G.HE3 G, A G.2N G.NP &.2P 69FU2 25FE G 1 SPL RLY THR- 999 D999 SCD-D OST

55 100.00 10.2 8. 1 17.2 21.2 7. 9 19.2 17. e 20.4 999=3 GEV

7 1 FU4 25FE G 1. SPL RLX THR- 999 0999 ACT-I 4PI 999=5 GEV NUCLIDE REACT I ON RES EXC I T SOURCE DETECTOR 71KU2 26FE G t. SPL ABY THR- 999 C999 ACT-I 4PI REF Z A I N ,lOUT TYPE ANG NUM

71KU5 26FE Gi.SPL ABY THR- 999

999

C 999

= 1.5 GEV

ACT-I 4PI 67ER1 25MN51 P ..G NOX 6- 7 P 1- 2 SCO-D DST 999=1.5 GEV

67FU1 26FE G 1. F ABY THR- 999 0999 ACT-I 4PI 56VU1 26MN53 P ' G R L Y 7 — D 1 — 2

*> MAr_n INAI— u on?u

7 1KU5 26FE G 1. P I + ABY THR- 999 C200-999

999=3 GEV

ACT-I 4PI 69TH1 E ' E/ ABX 0- 4 D 51- 61 MAG— D DST 999=2.2 GEV

B ( E L ) 55BE1 25FE N 1.G SPC 1 5 D 7 NAI-D UKN

5 7H I 1 2 5MN 5 5 E '. 3N ABX 30- 60 0 64 * 82 ACT-I 4PI

6 9D0

1

G '1 MU- T ABX 10- 3 0 C 10- 2oU MAG U 4Pi 5 5DE 1 2 5F E 5 3 G \. N ABX 11 — 2 4 C 11- 24 ACT-I 4PI

56 FU

1

G

'

G ABX 4— 40 C 4— 40 NAJ— U 12U 60RE1 2 5MN 5 5 G'.G ABX 7 D 7 NAI-D 90 550ei 26FE54 G . N ABX 11- 2 4 C 11- 24 ACT-I 4PI 64B01 Z 5MN55 G .G LET 1- 3 C 1- NAI-D 100

AB I 57CA2

620E1 26FE5426FE54

G

G

>N.N ABX

ABX

12-

20

30 C 13- 30

D 20 ACT-I 4PI ACT-I 4PI

6 8 AL

1

^ C U M C C

2 DMN 5

3

G'iG LET 0- 3 C 4 SCD-D 130 70WA3 26FE54 G'.2N RLY THR- 305 C150-305 ACT-I 4PI

7 LEVELS 70WA3 25FE54 G'.PN RLY THR- 305 C150-305 ACT-I 4PI 67L01 25MN55 G .G/ ABX 14- 32 C 34 NAI-D DST 58003 25FE54 G'.D RLY 19- 22 C 16- 22 ACT-I 4PI 5eCH2 25MN55 G .N RLY THR CTHR BF3-I 4PI REACTION UNCERTAIN

THRESHOLD 58G03 25FE54 G .NP RLY 19- 22 C 16- 22 ACT-I 4PI 59PA2 25MN55 G • N ABX 10- 24 C 10- 24 BF3-I 4PI 439 REACTION UNCERTA I

N

60GE3 25MN55 6 .N NOX THR CTHR BF3-I 4PI THRESHOLD 70PE2 26FE56 E . E/ FMF 0- 5 D 60 MAG-0 DST

61 TAl 25klN55 G .N NOX 16- 22 C 22 THR-I 90 7 2+, 1 3- STATES

64C03 25MN55 G • N AB I THR- 80 C 10- 80 BF3-I 4PI 71HE1 26FE56 E .E/ FMF 1 D198-300 MAG-D DST 68JU1 25MN55 G • N NOX THR- 22 C 22 THR-I DST 1 = .880 69DE1 25MN55 G'iN ABY THR- 999 C 2- 6 ACT-I 4PI 999=5.5 GEV 5KE2 25FE56 G .G NOX 1 D 1 NAI-D 100 G-WIDTH

71SA1 25MN55 G->N ABY 10- 68 C 10- 58 ACT-I 4PI 57L01 25FE56 G . G/ ABX 14- 32 C 34 NAI-D DST 66WA1 25MN55 G'.3N RLY THR- 300 ClOO- 300 ACT-I 4P1 58T01 26FE56 G . N RLY 12- 22 C 22 BF3-I 4PI ISOMER RATIO MN52 THRESHOLD

690E 1 25MN55 G'.3N ABY THR- 999 C 2- 5 ACT-1 4PI 999=5.5 GEV

60GE3 26FE56 G .N NOX T MR CTHR BF3-I 4PI THRESHOLD

58KA1 25MN55 G .XN ABX 11- 22 C 11- 22 BF3-I 4PI 558E4 25FE56 G .N ABX 1

1

C 13 TOF-D 135 60FL1 25MN56 G .XN ABX 11- 27 C 12- 30 BF3-I 4PI 67B02 26FE56 G .N ABX 12. 13 C 12. 13 TOF-D 135 QUADRUPOLE MOMENT J-PI 61BA2 2 5MN5 5 G .XN ABY THR- 22 C 22 THR-I DST 71BA2 26FE55 G .N ABX 11- 1 3 C 11. 13 TOF-D 135 64C02 25MN55 G .XN ABY THR- 80 C 80 BF3-I 4PI 68SH3 26FE55 G .XP ABX THR- 23 C 13- 23 SCI-1 DST 68GA1 25MN55 I G .XN SPC THR- 85 C 85 CCH-O 135 SPECTRA ALSO GIVEN

NEUT POLARI ZAT ION 6B0K3 25FE55 G .NP ABY THR- 20 C 20 ACT-I 4PI 69GA3 2 5MN 5 5 G .XN SPC 11- 85 C 85 CCH-D 135 68SH3 25MN55 G'.XP ABX THR- 23 C 13- 23 SCI-I DST 58T01 26FE57 G • N RLY 12- 22 C 22 BF3-I 4PI SPECTRA ALSO GIVEN THRESHOLD

66WA1 25MN55 G..7N'.P RLY THR- 300 ClOO- 300 ACT-I 4PI 50GE3 25FE57 G .N NOX THR CTHR 6F3-I 4PI ISOMER RATIO SC44 THRESHOLD

71KU2 25MN55 G .SPL ABY THR- 999 C999 ACT-I 4PI 999 = 1.5 GEV 71BA2

71JA1 71JA2

25FE57

25FE57

25FE57

G

G

G

.N

.N

.N

ABX RLX

RLX

7-

7-8-

12

69

C 8- 12

C 7- 8 C 8

TOF-D 135 TOF-D DST TOF-D DST 51CA1 25MN56 D .G ABX 16- 18 0 3- ACT-I 4PI G--WIDTH, 7 .5-8.4 MEV

6aOK.3 26FE57 G.P ABY THR- 20 C 20 ACT-I 4PI

IRON Z=26 COBALT Z=27

A ABUND. SEPARATION ENERGIES (MEV) G.N G.P G.T G.HE3 G..A G.2N G.NP G.2P A ABUND. SEPARATION ENERGIES (MEV)

54 5.82 13.4 8.9 23.0 19.7 8 ..4 24. 1 20.9 15.4 G.N G.P G.T G.HE3 G.A G.2N G.NP G.2P

56 91.65 11.2 10.2 20.9 20.3 7,.5 20.5 20.4 18.3 59 100.00 10.5 7.4 15.5 20.3 7.0 19.0 17.4 19.2

57 2.19 7.6 10.6 19.6 18.2 7,. 3 18.8 17.8 19.5

56 0.33 10.0 11.8 19.4 22.0 7,.5 17.7 20.5 21.5 NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN. OUT TYPE ANG NUM NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN..OUT TYPE ANG NUM 72MA2 27C055 P ,.G LET 7 D 2 SCD-D DST

71FU1 25FE El.SPL ABI THR- 999 D 40-999 SCD-D 4P I J-PI

999= 15 GEV 70ER1 27C058 P ..G SPC 8- 9 D 1- 2 SCD-D 45 70FU1 25FE E ..F RLY 999 D999 ACT-D 4PI DETAILS 4 LEVELS

999=1. 5-15.0 GEV

59K.01 26FE G..MU-T ABX 10- 27 C 31 NAI-0 6 ICRl 27C059 E..E/ NOX 0- 4 D183 MAG- I DST 59002 25FE Gi.MU-T ABX 10- 27 CTHR-250 MGP-D 4PI G-WDTH , MULTIPOLES

60RE1 25FE Gi.G ABX 7 D 7 NAI-D DST 65WY1 27C059 G..MU-T ABX 10- 35 C 90 SC I-D 4P

I

63SU1 26FE G..G ABX 4- 14 C 4- 14 NAI-D 120 50RE1 27C059 G.iG ABX 7 D 7 NAI-D 90 64B01 25FE G ,.G LET 1- 3 C 1- NAI-D 100 64B01 27C059 G 1.G LET 1- 3 C 1- NAI-D 100

ABI ABI 64C03 25FE G ..N ABI THR- 80 C 10- 80 BF3-I 4P I 68AL1 27C059 G '.G LET 1 C 4 SCD-D 130 58KA1 25FE G .>N ABX 50- 85 C 55. 85 TOF-D 57 1=1.187 MEV

NEUT ENGY SPEC 71SW3 27C059 G .G LET 1- 5 C 5 SCD-D DST

55DI 1 25FE Gi.XN NOX THR- 70 C 70 SC I-I DST 15 LEVELS. J-PI 55HA1 26FE G..XN ABX 15 . 18 D 15, 18 BF3- I 4PI 57L01 27C059 G'.G/ ABX 14- 32 C 34 NAI-D DST 61BA2 26FE G..XN ABY THR- 22 C 22 THR-I DST 58CH2 27C059 G ..N RLY THR CTHR BF3-I 4PI 54C02 26FE G-.XN ABY THR- 80 c 80 BF3-I 4P I THRESHOLD

57C02 25FE G .XN ABX THR- 24 c 11- 24 BF3-I 4P I 435 50GE3 27C059 G -iN NOX THR CTHR BF3-I 4PI 71C02 26FE G .XN ABI 36- 54 c 10- 54 SF3- I 4P I THRESHOLD

FAST N YIELD 52CA1 27C059 G ..N NOX 11- 30 C 30 ACT-I 4PI 56WA1 26FE G .,XNP RLY THR- 250 ClOO-250 ACT-I 4PI ISOMER RATIO

ISOMER RAT 10 MN52 62FU1 27C059 G ..N ABX 11- 28 C 9- 28 BF3-I 4PI 65WA1 26FE G..XN5P RLY THR- 250 ClOO-250 ACT-I 4PI 54C03 27C059 G..N ABI THR- 80 C 10- 80 BF3-I 4PI

I SOMER RATIO SC44 57GE2 27C059 G '.N ABY THR- 27 C 22, 27 BF3-I 4PI 53MI5 25FE G..XP ABY 8- 22 C 22 SCI-I DST 57HU1 27C059 G .>N ABX 11 D 1 1 BF3-I 4PI 58702 25FE G..A ABY 7- 22 C 22 EMU-I DST 57L I 1 27C059 G .N RLY THR- 54 C 35, 64 ACT-1 4PI 53KR1 26FE G..A RLY 7- 30 C 21 , 30 SCD-I 90 REL Cll, ISM RATIO 72KE4 25FE G .A RLY 7- 32 C 32 SCO-D DST 71SA1 27C059 G-.N ABY 10- 58 C 10- 58 ACT-I 4PI

33
NUCL 1 DE REACTION RES EXCIT SOURCE DETECTOR NUCLIDE REACTION RES EXC I T SOURCE DETECTOR

REF Z A I N OUT TYPE ANG NUM REF Z A I N OUT TYPE ANG NUM

62FU1 27C059 G 2N A8X 19- 28 C 9- 28 BF3-I 4PI 444 56HA

1

28N I G XN ABX 1 5 . 16 D 15. 18 BF 3- I 4P

I

67L I 1 27C059 G 2N RLY THR- 54 C 35 . 54 ACT-I 4PI 6 1BA2 28N 1 G XN ABY THR- 22 C 22 THR-I DST

REL G.N 64BA4 28N I G XN ABX 10- 27 C 10- 27 BF3-I 4P1 67L I 1 27C059 G 3N RLY THR- 54 C 35 . 54 ACT-I 4PI 55BA3 SAME DATA

REL G.N 546A5 28N I G XN ABX 12- 28 C 12- 28 BF3-I 4P

I

67L 1

1

27C059 G 4N RLY THR- 54 C 35. 54 ACT-I API 54C02 28N I G XN ABY THR- 80 C 80 BF3-I 4PI REL (G.N) 65BA3 2 8N I G XN ABX THR- 28 c 10- 30 8F3-I 4PI 56HA1 27C059 G XN ABX 15 . 1 8 0 15. 18 BF3-I 4PI 68F I 1 28N I G XN ABX 11- 25 c 11- 25 BF3-I 4PI 27C059 G XN ABX 10- 22 C 10- 22 BF3-I 4PI 58GA1 28N I I G XN SPC THR- 85 c 85 CCH-I 135 60FL1 27C059 G XN ABX 11- 24 C 12- 30 BF3-I 4PI NEUT POLARIZATION

OUADRUPOLE MOMENT 59GA3 28N I G XN SPC 11- 85 c 85 CCH-D 135

6 1BA2 27C059 G XN ABY THR- 22 C 22 THR-I DST 55DL1 2eN I G P SPC 18 D 18 EMU-D 4PI 61EM1 27C059 G XN SPC 13- 30 C 30 EMU-D 90 55J01 28N I G P RLY THR- 65 C 55 SCI-D DST 64BA2 27C059 G XN ABX 10- 30 C 10- 30 BF3-I 4PI 55LE1 2SNI G P ABX 8- 28 C 21- 28 EMU-I DST

6'tBA'> 27C059 G XN ABX 10- 27 C 10- 27 BF3-I 4PI 57SP1 28NI G P SPC 9- 18 C 18 EMU-D OST 65BA3 SAME DATA 52SE2 28N I G P ABX 1 5 . 18 D 15 . 18 SC I- I 0 64C02 2 7C0 5 9 G XN ABY THR- 80 C 80 BF3-I 4PI 57BA2 28N I G XP SPC THR- 85 C 85 TEL-O DST 65BA3 27C059 G XN ABX THR- 28 C 10- 30 BF3-I 4PI 58BA6 28N I G XP SPC THR- 85 C 85 TEL-D DST 66F I 2 27C059 G XN SPC THR- 60 C 60 TOF-0 90 60CH1 28N I G XP RLX THR- 90 C 90 TEL-I 90 68GA1 27C059 t G XN SPC THR- 85 C 85 CCH-D 135 REL TO DEUTERONS

NEUT POLARIZATION 51MA2 28N I G XP NOX 8- 21 C 18 . 21 SCI-D DST 58RH1 27C059 G XN NOX THR- 48 C 48 ACT-I 4PI 63MI5 28NI G XP ABY 8- 22 C 22 SCI-I DST 59GA3 27C059 G XN SPC 11- 85 C 85 CCH-D 135 63YA2 28N I G D RLY 15- 25 C 25 EMU-D 90 69G03 27C059 G XN ABX 10- 30 C 10- 30 BF3-I 4PI 450 REL TO PROTONS

7 IBAl 27C059 G XN ABX 10- 22 C 10- 22 BF3-I 4PI 247 + 60CH1 2 8N I G xo RLX THR- 90 C 90 TEL-I 90 56F0 1 27C059 G P RLY 7- 30 C 30 EMU-D 90 REL TO PROTONS

YLO REL TO G.D 67KN1 2eN I G . T RLY THR- 49 c 36. 49 ACT-I 4PI 57R01 27C059 G P SPC 15. 18 D 15. 18 EMU-D DST 60CH1 28N ! G XT RLY THR- 90 c 90 TEL-I 90 60CH1 27C059 G XP RLX 22- 90 C 90 TEL-I 90 REL TO DEUTERONS

REL TO DEUTERONS 57B01 28N I G A SPC THR- 30 c 31 EMU-D DST

63MI 5 27C059 G XP ABY 7- 22 C 22 SCI-I DST 58T02 2 8N I G .A ABY 6- 22 c 22 EMU-I DST 56F01 27C039 G D RLY 15- 30 C 30 EMU-D 90 63KR1 28N I G A SPC 6- 30 c 21. 30 SCD-D 90 YLO REL TO G.P RELATIVE YIELDS

6 IFO

1

27C059 G D SPC 7- 30 C 30 EMU-D UKN 54SC1 28N I G A SPC THR- 33 c 33 SCO-D 90 61F01 27C059 G D RLY 1 5- 30 C 30 EMU-D DST ABS YIELD

NO DEUTERONS FOUND 65H03 28N I G A SPC THR- 31 c 31 SCO-D 130 60CH1 2 7C059 G XD RLX 30- 90 C 90 TEL-I 90 72KE4 28NI G .A RLY 5- 32 c 32 SCD-D OST

REL TO PROTONS 7 IMEl 28N I G F ABY THR- 900 C300-900 TRK-I 4P

I

56HE 1 27C059 G T RLY THR- 31 C 31 ACT-I 4PI 56BE 1 28N I N G SPC 16 D 7 NAI-D UKN

56WA1 27C059 G T RLY THR- 31 C 31 ACT-I 4P! 60CH1 27C059 G XT RLY 32- 90 C 90 TEL-I 90 6 ICRl 28N I 58 E E/ NOX 0- 8 D183 MAG-D DST REL TO DEUTERONS G -WDTH. MULTIPOLES

58T02 27C059 G A ABY 7- 22 C 22 EMU-I DST 66DU1 28N I 58 E E/ FMF 1 D 45- 55 MAG-0 DST 61F01 27C059 G A SPC 9- 30 C 30 EMU-D UKN 1=1.452

7 2 K E4 2 7C0 5 9 G A RLY 7- 32 C 32 SCD-D DST 57DU1 2 8N I 58 E E/ FM F 1- 5 D 45- 55 MAG-D DST 62FU1 27C059 G NP ABX 18- 28 C 9- 28 BF3-I 4PI 441 B ( EL ) . 4 LEVELS

60G02 27C059 G PD ABX 30- 260 C 30- 260 ACT-I 4PI 69AF 1 28N I 58 E E/ FMF 1 . 4 0150.225 MAG-D DST ALSO G.N2P. G.HE3 1,4=1.45.4.45 MEV

60G02 27C059 G HE3 ABX 30- 260 C 30- 250 ACT-I 4PI 69GU

1

2 8N I 5

8

E E / ABX 10- 3 0 D199 MAG-D 40 ALSQ G.N2P. G.PD FMF 60G02 27C039 G N2P ABX 30- 250 C 30- 250 ACT-I 4PI 64 BO 1 2 ON I 5 o G G L F T 1 3 C 1- NAI-D 100 ALSO G.PD. G.HE3 ABI 66W A 1 2 7C059 G 5N2P RLY THR- 150 C150 ACT-I 4PI 7 OME 3 2 ON 1 t) O G G L F T 1- 4 C 4 SCD-D DST ISOMER RATIO MN52 6 LEVELS

67L U 27C059 G MN56 RLY THR- 54 C 35. 54 ACT-I 4PI 59CA4 28N I 58 G N ABX 12- 32 C 12- 32 ACT-I 4PI REL (G.N) 59R02 28N I 58 G N ABX 12- 24 C 24 ACT-I API

7 1KU2 27C059 G SPL ABY THR- 999 C999 ACT-I 4PI 68M I 1 28N 158 G N ABX THR- 25 C 10- 25 BF3-I 4PI 17 999 = 1.5 GEV 68G04 28N I 58 G XN ABX THR- 30 C 7- 30 BF3-I 4PI 69G02 2eN I 58 G XN ABX 12- 30 C 12- 30 BF3-I 4PI 278 66WA2 27C060 N G RLY 7 D 0 SCD-D 45 690W1 28N I 58 G XN ABX 1 2- 25 C 12- 25 BF3-I 4PI 191 700W

1

28N I 58 G XN ABX 11- 24 C 10- 24 BF3-I 4PI 2 74 59CA4 2eN I 58 G P ABX 12- 32 C 12- 32 ACT-I API 64MA2 28N I 58 G XP SPC THR- 22 C 22 SCD-D UKN

70 I S4 28N I 58 G XP ABX 8- 30 C 8- 30 SCD-0 UKN NICKEL Z = 28 PROB 90 DEGREES

59CA4 28NI58 G NP ABX 12- 32 C 12- 32 ACT-I 4PI

7 1 AN2 28N I 58 6 XD ABX 107- 999 C999 MAG-D DST

A ABUND. 5EPARAT ION ENERGIES (MEV) 999=1.14 GEV

G .N G. P C . T G.HE3 G. A G.2N G.NP G.2P

58 67.88 12 .2 8. 2 21 .2 17. 7 6. 4 22.5 19.5 14.2 70AN5 28N I 59 E P RLY 90- 999 C999 TEL-D DST

60 26.23 1

1

.4 9. 5 20 . 1 19.2 6. 3 20.4 20.0 16.9 999= 1140 MEV

61 1.19 7 .8 9. 9 19 . 3 17. 0 6. 5 19.2 17.4 18.1

62 3.66 10 .6 1 1 . 1 19 . 5 21 . 0 7. 0 18.4 20.5 19.9 61CR1 28N I 60 E E/ NOX 0- 5 D183 MAG-D DST

64 1.08 9 .7 12.5 19 . 1 23. 0 8. 1 16.5 20.9 * G -WDTH. MULTIPOLES

66DU1 28N I 50 E E/ FMF 1 D 45- 65 MAG-D DST 1=1.332 MEV

NUCL I DE REACT ION RES EXCIT SOURCE DETECTOR 670U1 2eNI60 E E/ FMF 1 . 4 0 45- 65 MAG-0

REF Z. A I N .OUT TYPE ANG NUM B (EL)1.33.4.03 MEV

69AF1 28N I 50 E E/ FMF 1 . 4 D150.225 MAG-D DST

71 MO 3 28N I E .E/ ABX 0- 240 D500 MAG-D 60 1.4=1.33.4.04 MEV

65WY1 28N I G .MU-T ABX 10- 35 C 90 5CI-0 4PI 59 69GU1 2 8N I 50 E E/ ABX 10- 30 D199 MAG-D DST 56FU1 28N I G .G ABX 4- 40 C 4- 40 NAl-D 120 FMF 60RE 1 28N I G .G ABX 7 D 7 NAI-D 90 69T03 28N I 60 E E/ FMF 0- 8 D183.250 MAG-D DST

6 1 M I 1 28N I G .G ABX 8- 15 D 8- 15 NAI-r DST B ( EL ) . J-P

I

6 1 TO 1 2eN I G .G ABX 4- 14 C 4- 14 NAI-D 120 72L I 1 28NI60 E E/ FMF 1- 3 D 50-120 MAG-D DST 62BE2 28N I G .G ABX 5- 9 D 5- NAI-D 135 1.33.2.16 MEV

64AR1 28N I G .G ABX 8 D 8 NAI-0 DST 56ME2 28N I 50 G G LET 1 D 1 NAI-D DST

J. WIDTH J-P I 64G I 1 28N ! G .G NOX 8 D 8 NAI-D 135 67BE5 28N 160 G G LET 1 D 1 NAI-0 120 WIDTH 70ME3 28NI50 G G LFT 1- 4 C 4 SCO-0 DST 66BE3 28N I G .G RLX 5- 10 D 6- 10 NAI-D 135 5 LEVELS

69CE 1 28N I G .G NOX 6- 8 D 6- 8 SCD-D DST 68M I 1 28NI60 G N ABX THR- 25 C 10- 25 BF3-I API 2 1 55G I 1 28N I G .G/ RLY 8 D 8 NAI-D 135 58G04 28NI60 G XN ABX THR- 30 C 7- 30 BF3-I 4PI 64C03 28N I G .N ABI THR- 80 C 10- 80 BF3-I 4PI 69G02 28N I 60 G XN ABX 11- 30 C 11- 30 8F3-I 4PI 278 67HU2 28N I G .N ABY THR- 22 C 22 THR-I DST 690W1 28NI50 G XN ABX 12- 25 C 12- 25 BF3-I 4PI 190 700W1 28NI50 G XN ABX 11- 24 c 10- 24 BF3-I 4PI 275 70TI2 28NI60 G XN RLY 12- 30 c 12- 30 BF3-I 4PI

70 I S4 28N 1 50 G XP ABX 9- 30 c 9- 30 SCD-D UKN

PROB 90 DEGREES

71014 28N 160 P G ABX 13- 23 0 4- 14 NAI-D DST 2544

71JA1 28NI51 G N RLX 7- 9 c 7- 9 TOF-D DST

3H
NUCL I DE REACT I ON RES EXC I T SOURCE DETECTOR NUCL I DE REACTION RES EXCI T SOURCE DETECTOR

REF Z A I N OUT TYPE ANG NUM REF Z A I N ,OUT TYPE ANG

66DU1 28N 162 E/ FMF 1 D 45- 65 MAG-D OST 56DA2 29CU G XP SPC 6- 70 C 70 EMU-D DST

1 =1.172 MEV 50CH1 29CU G XP RLX THR- 90 C 90 TEL-I 90

6 70U

1

2 8N I 62 E FMF * D 45- 65 MAG-D DST REL TO DEUTERONS

B (EL)1.17,3.75 MEV 51MA2 29CU G XP NOX 6- 2 1 C 21 SCI-D DST

6 8M0

1

2 8N I 62 NOX -J 0 7 NAI-D 90 63M I 5 29CU G XP A6Y 7- 22 C 22 SCI-I DST POLARIMETER 7.646 55F01 29CU G D RLY THR- 30 c 30 EMU-D 90 67ST 1 28N I 62 (3 LET 7 0 7 NAI-D 135 YLO REL TO G,P

7 = 7 .64 MEV 60K04 29CU G D RLY 15- 35 c 7u EMU-D DST 70ES1 28N 162 NOX 7 0 7 SCD-D DST 61 HOI 29CU G Q RLY 11- 45 c 45 EMU-r DST

7 = 7.64 REL TO PROTONS

70MO2 28N 1 62 (3 ABX g D 8 SCD-D DST 62V01 29CU G Q RLY 11 — 90 c 34, 90 TtL-D 90

a =7.645 , LF T 63YA2 29CU G RLY 14- 26 c 25 EMU-D OST 67ES1 2 8N I 62 C3 G/ ABX g D 8 NA I -D DST YIELD REL TO PROTN

59CA4 2BN I 62 (3 p ABX 12- 3 2 C 12- 32 ACT- 1 4P I 64SH3 29CU G 0 RLY 15- 40 C 24- 40 MSP-I 4PI 66V01 29CU G 0 ABX THR- 52 C 23- 52 TtL-D 90 69AF1 28N I 6* E F/ FMF 1 , 4 D150 . 225 MAG-D DST 71AN1 29CU G D SPC 45- 999 C700 . 999 TEL-D DST 1,4=1.32.3.55 MEV 999 = 1.2 GEV, REL D/P 696U1 28N I 64 E / ABX 10- 30 0150 MAG-D 55 60CH1 29CU G XD RLX THR- 90 C 90 TEL-I 90 FMF REL TO PROTONS

7 1 R Al 2 8N I 64 (3 p RLY 12- \ 7 C 12- 17 ACT- I 4P I 56HE 1 29CU G T RLY THR- 31 C 31 ACT-I 4PI 55WA1 29CU G X RLY THR- 31 C 31 ACT-I 4PI 52V01 29CU G T RLY 15- 90 C 34, 90 TEL-D 90 50CH1 29CU G XT RLY THR- 90 C 90 TEL-I 90 REL TO DEUTERONS

COPPER Z = 29 57B01 29CU G A SPC THR- 30 C 31 EMU-D DST 58T02 29CU G A SPC 7- 22 c 22 EMU-O OST 61F01 29CU G A RLY 7- 22 c 30 EMU-I UKN

A ABUND SEPARAT ION ENERGIES (MEV) REL TO PROTONS

G • N G. ^ G » T G.HE3 G,A G,2N 3 ,NP G , 2P 63XR1 29CU G SPC g - 30 c 21 , 30 SCD-D 90

63 69.09 10 .9 6. 18.9 5.8 19.7 16.7 17.2 RELATIVE YIELD

65 30.91 1 .9 7. 4 15 , 5 20.7 6.8 17.8 17.1 20.0 64S C

1

2 9CU G , A SPC T HR — 33 c 33 SCD-D 90 ABS YIELD

65ME2 29CU G A SPC THR- 35 c 35 SCO-D 90 NUCLIDE REACT ION RES EXC I T SOURCE DETECTOR 72KE4 29CU G A RLY 5- 32 c 32 SCD-O DST

REF Z A IN OUT TYPE ANG NUM 60ST1 29CU G NP RLX 144- 320 C320 TtL-D 75 REL TO H2 CROS SEC 59BA3 29CU E N ABY THR- 36 D 10- 36 8F3- I 4P I 64MA4 29CU G CU62 ABY 150- 720 C150-720 ACT-I 4PI 71V01 29CU E N ABX THR- 266 C150-266 TOF-0 90 59U I 3 29CU G SPL RLY THR-600 C500 ACT-I 4PI

6<.CH1 29CU E P ABX D999 MAG-D DST 71ME1 29CU G F ABY THR-900 C300-900 TRK-I 4PI 999=1 GEV 71GR2 29CU G P 1 + ABY 1 50-560 C560 EMU-D DST

58Z [ 1 29CU G MU-T ABX 15- 2 1 C 15- 30 MGP-D 4P I PI -/PI + Y I ELD RAT 10 65WY 1 29CU G MU-f ABX 10- 35 C 90 SC I-D 4P I 58 71GR2 29CU G P I - ABY 150- 560 C55'J EMU-D DST 558U1 29CU G G R L X 0- 3 C 3 NAI-D 90 PI -/PI+ YIELD RATIO

56FU1 29CU G G 40 C 4- 40 NAI-D 120 57BE 1 29CU G G ABX 13 — 2 1 c 18- 22 ACT-I 90 61CA1 29CU60 0 ABX 14- 1

6

D 3- ACT-I 4PI 59PE5 29CU G G ABX 19 — 6

1

c 19- 61 NAI-D 135 60RE 1 29CU G G ABX 6 — 7 D 6- NAI-D DST 57HI1 29CU63 E N ABX 10- 82 D 30- 82 ACT-I 4PI

G- «DTH MULTIPOLARITIES

61 101 29CU G G ABX 3 - 1

6

c 3- 16 NAI-D 120 65HE1 29CU63 E N RLY THR- 32 D 14- 32 ACT-I 4PI 628E2 29CU G G ADX 5 . 9 D 5- NAI-D 135 72KU6 29CU63 E N ABX 11- 30 D 20- 30 ACT-I 4PI 53KA3 29CU G G ABX D I , NAI-0 120 E+/E - YIELD RAT 10 66BE3 29CU G S RL X 3 _ 1

0

D 5- 10 NAI-D 135 65HE1 29CU63 E + N RLY THR- 32 D 14- 32 ACT-I 4P| 67GI 1 29CU G G LET 6 . g 0 6- 8 NAI-D DST 60B03 29CU63 G G LFT 0- 2 C 0- NAI-D 100 6.8=6.07.8.50 MEV J 67TUit 29CU G

- D 5 NAI-D UKN 61R01 29CU6 3 G G ABX 0- 1 D 0- NAI-O DST

5 7FE 1 29CU G N 3 ^ C 15- 31 THR-I DST LIFETIMES

58AS1 29CU G N NOX ^ 7 C 17 SCI-I DST 62B06 29CU63 G G LFT 0- 4 C 0- NAI-D 110 60CH2 29CU G N R L X 8 - 2 1 C 8- 21 BF3-I 4P I J-PI REL TO PROTONS 63MC1 29CU63 G G LFT 1 0 1 NAI-D 90

fcOiCU2 29CU G N RLY 18 — 90 C 90 TEL-I DST 64B01 29CU63 G G LFT 1- 3 C 1- NAI-D 100 51TA1 29CU G N NOX 12- 22 c 22 THR- I DST ABI 62MI3 29CU G N ABX 10- 20 D 10- 20 8F3-! 4P 1 68AL1 29CU63 G G LFT 0- 2 C 4 SCD-D 130 64C03 29CU G N AB I THR- 80 C 10- 80 BF3-I 4PI 1 . 414 ,1.551 MEV

64FU1 29CU G N ABX 9- 28 D 9- 28 BF3-I 4P I 68TA2 29CU63 G G LFT \ D 1 NAl-D 90 67GE2 29CiJ G N ABY THR- 27 C 22 , 27 BF3-I 4P I U.953 MEV

68K.A1 29CU G N ABX 50- 85 c 55, 85 TOF-D 67 69BE7 29CU6 3 G G LFT 6 , 8 D 5 , 8 U<N-D DST NEUT ENGY SPEC 6 .07 , 8.60 MEV

6'tFUl 29CU G 2N ABX 18- 28 0 18- 28 BF3-I 4PI 55CA1 29CU63 G N RLY 18 D 18 ACT-I 4PI 55D U 29CU G XN GPC THR- 70 c 70 EMU-D DST 55SC1 29CU53 G N ABX 1 0- 20 C 12- 20 ACT-I 4PI USED SCI FOR DST 58BE1 29CU63 G N RLY 10- 1 1 C 10- 11 ACT-I 4PI 55L 1

1

29CU G XN SPC 8- 70 c 70 EMU-O U»,N THRESHOLD

55MC1 29CU G XN RLY THR- 22 c 22 NAI - I 90 59NA1 29CU53 G N ABX 1 8 D 18 BF3-I 4PI 56GA1 29CU G XN ABX 11- 27 c 18- 27 BF3-I 4P I 59PE3 29CU53 G N RLY 10- 11 C 1 J- 11 ACT-I 4PI 56HA1 29CU G XN ABX 15. 18 D 15, 18 BF3-I 4P I THRESHOLD

61BA2 29CU G XN ABY THR- 22 C 22 THR- I DST 60GE3 - 29CU63 G N NOX THR CTHR BF3-I 4PI 51M I 1 29CU G XN ABX 10- 20 0 10- 20 BF3-I 4P I THRESHOLD

e^iALS 29CU G XN NOX THR- 34 C 34 THR- I DST 61C02 29CU63 G N ABX 12- 16 D 12- 18 ACT-I 4PI

6'tBA'. 29CU G XN ABX 10- 27 C 10- 27 BF3-I 4P I 52DE1 29CU63 G N ABX 2 1 D 21 ACT-I 4PI 65BA3 SAME DATA 54FU1 29CU62 G N ABX 10- 28 D 10- 28 BF3-I 4PI

6'tC02 29CU G XN ABY THR- 80 c 80 BF3-I 4P I 65GR1 29CU63 G N ABX THR- 44 C 10- 65 ACT-I 4PI 65BA3 29CU G XN ABX THR- 28 c 10- 30 BF3-I 4PI 5 80K1 29CU63 G N RLX 12- 24 C 10- 24 ACT-I 4PI 58T01 29CU G XN ABX 10- 24 c 10- 24 BF3-I 4P I 58SU1 29CU63 G N ABX THR- 25 D 10- 25 ACT-I 4PI MONTR CALIBRATION 720R2 29CU53 G N ABX 11- 25 C 11- 26 ACT-I 4PI

70 1 S6 29CU G X.N ABX 10- 30 C 10- 30 BF3-I 4P I 487 54FU1 29CU53 G 2N ABX 1 9- 28 D 10- 28 BF3-I 4PI 550L1 29CU G P SPC 18 D 18 EMU-D 4PI 68SU1 29CU63 G 2N ABX THR- 25 D 10- 26 ACT-I 4PI 55CH1 29CU G P SPC 15. 18 D 15, 18 EMU-D UK,N 60YA1 29CU63 G p ABX 15, 18 D 15, 18 ACT-I 4PI 56F01 29CU G P RLY THR- 30 C 30 EMU-D 90 69AN6 29CU63 G

p ABY 103- 999 C700 , 999 TEL-D DST

YLD REL TO G,D 999=1.2 GEV

55LE1 29CU G P RLX 3- 31 C 19- 31 EMUI

DST 62CH2 29CU63 G XP RLY 6- 90 C 34- 90 TEL-D DST 60CH2 29CU G P ABX 9- 21 C 8- 21 lON-I 4P 1 REL TO DEUTERONS

61F01 29CU G P SPC 5- 30 C 30 EMU-D UK.N 54MA2 29CU63 G XP SPC THR- 17 C 17 SCD-D UKN YIELD REL TO ALPHA 6eAB2 29CU63 G XP SPC THR- 27 C 27 SCD-D 90 61H01 29CU G P RLY 3- 45 C 45 EMUI

DST 6 3 GO 6 29CU63 G D RLY 14- 22 C 22 EMU-I DST REL TO DEUTERONS REL TO PROTONS

62SE2 29CU G P ABX 15, 18 D 16, 18 SC I-I UKN 69AN6 29CU53 G D ABY 112- 999 C700 , 999 TEL-D DST 62V01 29CU G .P RLY 6- 90 C 34, 90 TEL-0 90 999=1.2 GEV 630D1 29CU G ,P ABY 5- 22 c 22 EMU- I DST 52CH2 29CU63 G XD RLY 1 1- 90 C 34- 90 TEL-D DST 64RA3 29CU G »

P

ABX THR- 27 c 30 SCI-I DST REL TO PROTONS

66V01 29CU G .P ABX THR- 52 c 23- 52 TEL-0 90 71AN1 29CU G ,P SPC 37- 999 C700,999 TEL-D DST 999=1.2 GEV, REL D/P

35
NUCLl DE REACT ION RES EXCI T SOURCE DETECTOR

REF 2 A I N ,OUT TYPE ANG

58T02 29CU63 G »A ABY 6- 22 C 22 EMU-I DST SEPARATED ISOTOPE 63G08 29CU63 G pA RLY THR- 22 c t" M 1 1— I n c. T R

_

1 \j n r\\J 1 VJ o 66H03 29CU63 G t A ABY THR- 31 c 31 680K1 29CU63 >A ABY THR- 20 c 20 ACT-I 4PI 68R I 3 29CU63 G >NA RLY THR- 50 c 30- 50 ACT-I ipPI RLY G.2N

5eR I 3 29CU63 G

'

.2NA RLY THR- 50 c 30- 50 ACT-I ipPI RLY G.2N

60B03 29CU55 G'.G LET 0- 2 c 0- NAl-D 100 53KA1 29CU65 G'pG LFT 1 0 1 NAI-D 108 MEAN ABS CROSS SEC 64BE6 29CU65 G .pG LET 1 D 1 NAI-D DST MIXING RATIO

64B01 29CU65 G ipG LFT 1- 3 C 1- NAI-D 100

ABI 68ME3 29CU65 Q<pG LFT 1 D 1 NAI-D DST

1 =1.116 MEV 69BE7 29CUfe5 G,pG LFT 6. 8 D 6 . 8 U<N-D DST

5 .07 . 8.50 MEV

58BE1 29CU65 G ,pN RLY 9- 1

1

C 9- 1

1

ACT-I ^tPI THRESHOLD

60GE3 29CU55 G ..N NOX THR CTHR BF3-I itPl THRESHOLD 6K02 29CU55 G 1iN RLX 1 5 . 1 8 D 15. 18 ACT-I itPl REL TO CU63

6<tFUl 29CU65 G I>N ABX 10- 28 D 10- 28 BF3-I 4PI 670E4 29CU65 G 1,H NOX THR- 260 C260 ACT-I DST 64FU1 29CU65 G \.2N ABX 1 6- 28 0 10- 28 BF3-I 4PI 50A I 1 29CU55 G <.3N AB I 29- 110 c 29- 110 ACT-1 4PI 50LI1 29CU53 G 1,P ABX 12- 28 c 12- 28 EMU-D DST SPECTRUM

62CH2 29CU65 G 1,XP RLY 7- 90 c S'l- 90 TEL-D DST REL TO OEUTERONS

68AB2 29CU65 GiiXP SPC THR- 27 c 27 SCD-0 90 62CH2 29CU65 G .,XD RLY 15- 90 c 3f- 90 TEL-D DST 57ER1 REL TO PROTONS

29CU65 G ,,A AB i 't- 32 c 32 ACT-I UPl 71BL1 29CU65 G,,PI + ABY 150- 700 C150- 700 ACT-I 4PI SEE 68NY1

Z I NC Z = 30

A ABUND. SEPARATION ENERGIES (MEVl G.N G.P G.T G.HE3 G.A G.2N G.NP G,2P

64 48. 89 11.9 7.7 19.0 16.7 4.0 21.0 18.6 13.8

66 27. 81 11.1 8.9 18.3 18.3 4.6 19.0 18.8 16.4

57 4. 11 7.1 8.9 17.4 15.7 4.8 18. 1 15.0 17.3

68 18. 57 10.2 10.0 17.7 19.8 5.3 17. 3 19.1 18.5

70 0. 62 9,2 10.9 17.2 21.3 5.9 15.7 19.5 >

NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN pOUT TYPE ANG

60RE1 3UZN G .G ABX 7 D 7 NAI-D 90 53SU1 30ZN G iG ABX 4- 14 C 4- 14 NAI-D 120 55aE3 302N G >G RLX 5- 10 D 5- 10 NAI-D 135 61TA1 30ZN G .N NOX 12- 22 C 22 THR-I DST 67HU2 30ZN G pN ABY THR- 22 C 22 THR-I DST 5eKAl 30ZN G P.N ABX 50- 85 C 55, 85 TOF-D 67 NEUT ENGY SPEC

70C01 30ZN G-pN RLX 12- 40 C 10- 40 ACT-I 4PI 70C01 30ZN G p2N RLX 21- 40 C 10- 40 ACT-I 4PI 55GA1 30ZN G pXN ABX 7- 27 C 9- 27 BF3-I 4PI 56HA1 30ZN G 'pXN ABX 1 5 . 18 D 15, 18 BF3-I 4PI 64C02 30ZN GipXN ABY THR- 80 C 80 BF3-I 4PI 57C01 30ZN G,pXN ABX 12- 24 C 24 BF3-I 4PI 71C02 30ZN G.pXN ABI 35- 64 c 10- 64 BF3-I 4PI FAST N YIELD

55DL1 30ZN G ,pp ABX 18 D 18 EMU-D 4PI 570S1 30ZN G ,pP ABX THR- 31 C 20- 31 EMU-D DST 53M I 5 30ZN G ,,XP ABY 10- 22 C 22 SCI-I DST 66AC1 30ZN G ,pD YLD 15- 22 C 22 MAG-D 4PI YIELD UPPER LIMIT

70CU1 30ZN G ,pT ABY THR- 90 C 90 ACT-I 4PI 58T02 30ZN G ,pA ABY 2- 22 C 22 EMU-I DST 66H03 30ZN G.pA SPC THR- 31 C 31 SCO-D 130 72<E4 30ZN G <pA RLY 4- 32 C 16- 32 SCO-D DST 70C01 30ZN G :pNP RLX 19- 40 c lo- 40 ACT-I 4PI 65VA3 30ZN GipCU64 AB I 50- 300 c 50- 300 ACT-I 4PI

70AF1 30ZN64 E ppE/ FMF 0- 3 D150 , 225 MAG-D DST

.'?9.3 .0 MEV. Bl EL

}

72LI1 30ZN54 EllE/ FMF 0- 2 D 60- 120 KAG-D DST

.99 ,1.80 MEV 69BE7 30ZN64 Gf.G LFT 7 D 7 UKN-D DST 7.38 MEV

72ME3 30ZN64 G .iG LFT 3- 5 C 5 SCD-D DST

J-PI

NUCL I 0£ REACT 1 ON RES EXCIT SOURCE DETECTOR

RlF Z A I N •(OUT TYPE ANG NUM

55DE1 30ZN6^ G !»N ABX 12- 2 3 12- 2 3 ACT-I ^PI 55V I 1 30ZN6^ G '»

N

ABX 12- 2 2 Q 12- 2 2 ACT-I -iPI 59NA1 30ZN64 G '1 N ABX 1 8 I 8 BF3-I 4PI 60RO^ G ',

fij ABX 12- 2 3 12- 2 3 ACT-I £^P I 6 1C02 30ZN6^ G ', N RLX 15* 1

8

Q l 5 » 1 8 AC T - I 4P I REL TO CU6 3 ( G » N

)

62DE1 30ZN6^ G '* N ABX 2 I Q 2 1 ACT-I 4P I 67CA1 30ZN6^ G ' N RLX 12- 2 2 Q 12 — 2 2 ACT-I i*P I 680W 1 30ZN64 G ', jSJ RLX 12- 2^ 10- 2^ AC T- I ^P I 109 55DE1 30ZN6A G •, 2N ABY 20- 2 3 c 20- 23 ACT-1 4PI THRESHOLD

55V I 1 ^ » 2 N ABY 15- 2 2 C 12- 22 ACT- I 4P I 57EL1 30ZN64 G

» 2 N RLY T H R- 30 C 32 ACT-I 4P

I

58HO

1

30ZN6^ G 1» 2 N AB I 20 — 28 C 28 ACT-I i*P I

5 8 GO 3 3UZN6^ G '1

D

ABX 16- 2 2 C 16- 22 ACT-1 4PI REACT ION UNCERTA I

N

58G03 30ZN64 G .MP ABX 16- 22 C 16- 22 ACT-I 4PI REACT ION UNCERTAIN

5 8H01 30ZN6^ G ') NP AB I 16- 2 8 C 28 ACT-1 i*Pl THRESHOLD

71PA3 30ZN64 p ,, (3 ABX 10- 26 D 2- 18 NAI-0 90

70AF1 30ZN66 E • E/ FMF 0- 3 D150. 225 MAG-D DST

1 ,0i* » 2.8 MEVtB{ EL

)

67BE5 30ZN66 G • G LFT 1 D 1 NAI-D 120

1:=1.064 MEV

68SH5 30ZN66 G '»

G

NOX 7 D 7 SCD-D DST

7^=7.368 MEV

69SH1 30ZN66 G »G LFT 7 D 7 SCD-D 135

7^-"7 9<^fl MC^ M 72ME3 3UZN66 G »G LFT 3- 5 C 5 SCD-D DST J-PI 64C03 30ZN66 G

'

1 N AB I THR- 80 C 10- 80 6F3-I 4PI 55V 1

1

30ZN66 G '1 D ABX 20- 2 2 c 20- 22 ACT-I 4PI INCLUDES G,NP

58G03 302N66 G '> P ABX 16- 2 2 c 16- 22 ACT-I 4PI REACT ION UNCERTAIN

55DE

1

3 0 Z N 6 6 G '» NP ABX 19- 2 3 C 19- 23 ACT-I 4PI 57EL1 3UZN66 G-.NP ABX 22- 30 C 32 ACT-I 4PI 58G03 30ZN66 G'.NP ABX 16- 22 C 16- 22 ACT-I 4PI REACT ION UNCERTAIN

58H01 30ZN66 G iNP ABX 21- 32 C 15- 32 ACT-I 4PI THRESHOLD

6 80 K, 3 30 Z N66 ABY THR C 20 ACT-I 4PI

66 I V 1 30ZN67 G t P ABX ThR- 28 C 12- 28 ACT-I 4PI

72ME3 3UZN68 G .G LFT 3- 5 C 5 SCD-D DST

J-P I 57EL1 30ZN68 G'»

P

ABX 13- 30 C 32 ACT-I 4PI 58H01 30ZN68 G .P RLY 10- 32 c 15- 32 ACT-I 4PI THRESHOLD

GALLIUM Z=31

A ABUND. SEPARATION ENERGIES (MEV) G,N G.P G.T G.HES G,A G,2N G,NP G,2P

69 60.4 10.3 6.6 15.4 18.0 4,5 13.6 16.8 16.5

71 39.6 9.3 7.9 15.1 19.7 5,3 17.0 17.1 18.8

NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN, OUT TYPE ANG NUM

54C03 31SA G !pN ABI THR- 80 C 10- 80 BF3-I 4PI 64BA4 31GA G.pXN ABX 10- 27 C 10- 27 BF3- I 4P I 55BA3 SAME DATA

64BA5 31GA G 1pXN ABX 11- 26 C 11- 26 BF3-I 4P I 54C02 3 IGA G.pXN ABY THR- 80 C 80 BF3-I 4P I 65BA3 31GA dipXN ABX THR- 28 c 10- 30 BF3- I 4P I

59CA1 31GA66 D,pG ABX 14- 15 D 3- ACT- I 4PI

58AL1 31GA59 GipG LFT 0- 1 C 4 SCO-D 130 0.872

,

1,107 MEV

68LA1 31GA69 G.pG LFT 0- 1 D 0- 1 NAI-D 130

4 LEVELS. TO 1 .337

60GE3 3 1GA7

1

G ppN NOX THR CTHR BF3-1 4PI THRESHOLD

580K1 31GA71 G ppA ABY THR- 20 C 20 ACT-I 4P I

36
GERMANIUM Z = 32 NUCL I DE REACT I ON RES EXC I T SOURCE DETECTOR

REF Z A I N .OUT TYPE ANG NUM

ABUND. SEPARATION ENERGIES (MEV) G.N G .P G ,T G.KE3 G.A G.2N G.NP G.2P 56SU1 33AS75 G '»N2P RLY THR- 320 C140.320 ACT-I 4P I 70 20*52 11.5 8 .5 18 .6 17.6 4.1 20.0 18.8 15.1 56SU1 33AS75 G '» 3 N 2 P RL Y T HR - 3 2 0 C14U . 320 ACT- I 4P I 72 2 7 • 4 3 10.7 9 .7 18 .2 19.1 5.0 18.2 19.0 17.6 56SU1 33AS75 G '1 3N4P RLY T HR- 320 C 1 40 . 320 ACT-I 4P I 73 7 76 6 . B 10.0 17 . 3 16.7 5.3 17.5 16.5 18.5 56SU1 33AS75 G »4N5P RLY THR- 320 C140 . 320 ACT-I 4P I 74 36 • 5 4 10.2 11 .0 13 .2 21.0 6.3 17.0 20.2 19.9 56SU1 33AS75 G '1 5N2P RLY THR- 320 C 140 » 320 ACT-I 4P 1 76 7.76 9.4 12 .0 18 . 4 « 7.5 15.9 20.7 • 56SU1 33AS75 G

'

.5N5P RLY THR- 3 2 0 C140 . 320 ACT-I 4P I 56SU1 33AS75 G '.7N2P RLY THR- 320 C140 . 320 ACT-I 4P I 56SU1 33AS75 ( 7N4P RLY T HR — 3 2 0 C140 . 320 ACT-I 4P I NUCLIDE REACTION RES EXCIT SOURCE DETECTOR 56SU1 3 3AS7 5 Gi,8N6P RLY THR- 320 C140.320 ACT- I 4P I RI£F Z A I N lOUT TYPE ANG NUM 56SU1 33AS75 G-.CU61 RLY THR- 320 C140 .320 ACT-I 4P I 56SU1 33AS75 RLY C140 .320 64C0 3 3 2GE G t N AS I THR- 80 C 10- 80 BF3-I 4PI 7 1 K U2 3 3 AS7 5 I SP

L

ABY THR~999 C900 ACT-I 4P \ 64C02 32GE G > XN AS Y T HR- 8 0 C 80 BF3-I 4P I 999 = 1.5 GEV

68KR2 32GE G lA ABX THR — 3 3 C 33 SCD-D 90

70M04 32GE70 G , (3 LET 6 SCD-D DST 6.018. J-PI .LET 55B01 32GE70 , ABX 12- 2 1 C 12- 21 ACT-I 4P I SELENIUM 2 = 34

5 5DE 1 32GE70 . N A 3X 9 — 21 C 9- 21 ACT-I 4PI THRESHOLD

60FE 1 32GE70 . N ABX Il- 31 C 31 ACT-I 4PI A ABUND. SEPARAT ION ENERGI ES 1 MEV ) 60FE1 32GE70 .NP ABX ls— 31 C 31 ACT-I 4P I G .N G.P G . T 6.HE3 G.A G . 2N G.NP G. 2P

74 0.87 12 . 1 8.5 19 .3 17.2 4.1 20.7 19.3 14 . 2 56ME 1 32GE72 G »

G

LET [) 1 NAI-D DST 76 9.02 11 .2 9.5 19 . 3 18.9 5.1 19.2 19.8 16 . 4 J 7 7 7.56 7 ,4 9.6 18.7 16.1 5.7 18.6 16.9 I 7 ^ 3 78 23.52 10.5 10.4 18.9 20.1 6.0 17.9 20.1 18 . 4 58T01 32GE73 G . N 7 — 22 C 22 BF3-I 4PI 8C 49.82 9 , 9 11.4 18 .8 21.5 7.0 16.9 20.4 2 0 . 6 THRESHOLD 82 9.19 9 .3 12.3 18 .8 23.1 8.2 15.0 21.2 » 56 HE 2 3 2GE 7 3 31 C 31 ACT-I 4P I REL CU 63

6 80K

1

32GE73 G 1* 20 20 ACT-I 4P I NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN,.OUT TYPE ANG NUM

5 6 M E

1

32GE74 G

'

. G LPT Q 1 NAI-D DST

J 65BE3 34SE 6,iG RLX 5- 10 0 5- 10 NAI-D 135 70MO2 32GE74 G !, (3 ABX 6 Q 6 SCD-D DST 70AR1 345E G,.G ABX 12- 30 C 32 NAI-D DST 6=6.018 .LET RATIO G.G/TO 2+

7 1M02 32GE74 G !, G/ LET 6 . 8 0 6. 8 SCD-D OST 63KA2 34SE G,.G/ RLY 1 C 5 ACT- I 4P I 6.018. 7.632 MEV 67HU2 34SE G.>N ABY THR- 22 C 22 THR-I DST 680K3 32GE74 G ., p ABY THR- 20 C 20 ACT-I 4P I 67C02 34SE G..XN ABX THR- 24 C 11- 24 BF3-I 4PI 437 71C02 34SE Gi.XN A8I 36- 64 C 10- 64 BF3-I 4P I 437

bSBOl 32GE76 G>N ABX 9- 21 C 9- 21 ACT-I 4P I FAST N YIELD

550E1 32GE /6 G..N ABX 9- 21 C 9- 21 ACT-I 4P I 66WE2 34SE G <.A ABX 6- 33 C 33 SCD-D 90 62CA1 32GE76 G,.N NOX 10- 30 C 30 ACT-I 4PI ISOMERIC RATIO 60DE2 34SE76 G,.G LET 1 D 1 NAI-D UKN 680K2 32GE76 G,.N ABY THR- 20 C 20 ACT-I 4PI 63PR2 34SE76 G..G LET 1 D 1 NAI-D DST ISOMERIC YIELD

69603 34SE77 G ..G ABX 0- 2 C 0- 2 ACT-I 4P I 63VE2 34SE77 G 1.G/ ABX 0- 1 D 1 ACT-I 4P I

I SOMERS 1=1.33 MEV 6eOK3 34SE77 G ,.P ABY THR- 20 C 20 ACT-I 4P I ARSENIC 2=33

680IC2 34SE78 G..N ABY THR- 20 C 20 ACT-I 4P I ISOMERIC YIELD

A ABUND. SEPARATION ENERGIES (MEV] G.N G .P G , T G .HE3 G.A G.2N G.NP G.2P 58H01 34SEeO G..NP RLY 20- 32 C 32 ACT-I 4PI

75 100.00 10.2 6 .9 15 . 4 19.4 5.3 18.2 17.1 17.9 THRESHOLD

56S 12 34SE82 G <.N ABX 9- 22 C 9- 22 ACT-I 4P I NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN. OUT TYPE ANG NUM

66AM2 33AS75 E.E/P SPC 105-365 D66U-880 MAG-D 62 ANGLE OF E/ IS 51 BROMINE Z=35 62ME2 33AS75 G .G LET 1 0 1 NAI-0 0 635U1 33AS75 G iG ABX 4- 14 C 4 - 14 NAI-D 120 64SH5 33AS75 G .G LET 1 D 1 NAI-D 122 A ABUND. SEPARATION ENERGIES IMEV 1

1 =.265 MEV G.N G. P G.T G.HE3 G.A G.2N G.NP

67LA1 33AS75 G .G LET 1 D 1 NAI-D DST 79 50.54 10.7 5. 3 15.8 13.7 5.5 19.0 16.8

1 = .265 . .280 MEV 81 49. 46 10.2 7. 5 15.9 20.2 6.5 18.0 17.4 68AL1 33AS75 G 'iG LET 0- 1 C 4 0.86 .1.07 SCD-0 DST .1.35 MEV

6 9 MO 3 33AS75 G .G ABX 8 D 3 SCD-D DST NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

J-PI .G-WIDTH.7.546 REF Z A IN..OUT TYPE ANG 70AR1 33AS75 G .G ABX 12- 30 C 32 GETS NAI-D DST G.G/TO 2+ 63KA2 35BR G'.0/ RLY 1 C 4 ACT-I 4PI 7CM02 33AS76 G ..G ASx 8 D 8

8 = SCD-D DST

7. 645. LET 58JU1 35BR >N NOX THR- 27 C 27 THR-I DST

56SU1 33AS75 G I.N RLY THR- 320 CI 40 .320 ACT-I 4PI 66LA1 35BR79 .G LFT 0- 1 D 0- 1 NAI-D 123 57FE2 33AS75 G .N ABY 14- 30 C 14 - 30 THR-I 4PI 1=.834 MEV 58CH2 33AS75 G >N RLY THR CTHR BF3-I 4PI THRESHOLD 57KI1 35BR61 >N RLY 10- 70 C 15- 70 BF3-I 4PI 60GE3 33AS75 G .N NOX THR CTHR BF3-I 4PI THRESHOLD

60GE3 35BR81 .N NOX THR CTHR BF3-I 4PI THRESHOLD

61TA1 33AS75 G'iN NOX 7- 22 C 22 THR-I DST 52CA1 358R81 G-.N NOX 10- 30 C 30 ACT-I 4PI 64C03 33AS75 G .N AB I THR- 80 c 10 - 80 aF3-I 4PI ISOMERIC RATIO

57HU1 33AS75 G .N ABX 1 1 0 1 1 BF3-I 4PI 55SC2 35BR81 G .A ABY THR- 32 C 32 ACT-I 4PI 71SA1 33AS75 G'iN ABY 10- 68 C 10 - 58 ACT-I 4PI 57ER1 35BR81 G 1.A AB I 5- 32 C 32 ACT-I 4PI 59BE1 33AS75 G .2N ABX THR- 30 D 18 - 30 BF3-I 4PI 680K1 35BRS1 G .A ABY TFR- 20 C 20 ACT-I 4PI 55SU1 33AS75 G'.3N RLY THR- 320 C140 .320 ACT-I 4PI 58<A1 33AS75 G ,XN ABX 10- 22 C 10 - 22 BF3-I 4PI 61BA2 33AS75 G,,XN ABY THR- 22 C 22 THR-I DST 64C02 33AS75 G,.XN ABY THR- 80 C 80 BF3-I 4PI 65F I 1 33AS75 G ,XN ABX 10- 25 C 10 - 25 BF3-I 4P! 69BE1 33AS75 G'.XN ABX THR- 30 D 10 - 30 BF3-I 4PI 144+ 56SU1 33AS75 G'.2P RLY THR- 320 C140 .320 ACT-I 4PI

37
K.RYPTON Z = 36 YTTRIUM Z=39

SEPARATION ENERGIES (MEVl G.T 6,HE3 G.A G.2N G.NP G,2P SEPARATION ENERGIES IMEV) G.T G.HE3 G.A G.2N G.NP

78 0.35 12.0 8. 2 19 .9 15.9 4.4 21.1 19.4 13.5 89 100.00 11.5 7. 1 18 . 1 19.9 8. 0 20.3 18.2 17. 80 2,27 1

1

.5 9. 1 19 .6 18.2 5.1 19.9 19.8 15,4

82 11.56 11 .0 9.9 19 . 5 19.6 6 .

0

18.8 20.1 17.4

83 11.55 7 .5 9. 8 19 . 1 17.2 5 . 5 18.5 17.4 18.2 NUCLIDE REACT ION RES EXCIT SOURCE DETECTOR

84 56.90 10 . 5 10. 7 19 . 21.0 7 . 1 16.0 20.3 19.4 REF I A I N OUT TYPE ANG NUM

86 17.37 9 .9 11.9 19 .2 22.8 8 . 1 17.0 20.9 21.9 67SH1 39Y 8 9 E E / FMF 2- 3 D225 MAG-D DST

2.5 MEV

NUCL I DE REACT ION RtS EXC I T SOURCE DETECTOR 68PE1 39Y 89 E E/ RLY 1- 3 0 65. 70 MAG-D DST

REF 2 A IN OUT TYPE ANG NUM 5 LEVELS

71M03 39Y 89 E / ABX 0- 240 0500 MAG-D 60 69H01 36K.R G XP ABY ThR- 33 C 24- 33 SCI-D 90 69SH6 39Y 89 E P SPC 10- 26 D 20 MAG-D UKN

68AL1 3 9 Y 8 9 G LFT 2 C 4 SCD-D 130 66BE2 36KR82 G .G LFT 1 C 1 NA I -D 113 2=1.51 MEV 1=.777 MEV 70AR1 39Y 89 G G ABX 12- 30 C 32 NAI-D DST RAT 10 G.G/TO 2+ 69H01 36K.R84 G .XP ABY ThR- 33 C 24- 33 SCI-D 90 58S I 1 39Y 89 G G/ ABY 2- 2 1 C 22 ACT- I 4P I 53KA2 39Y 89 G G/ RLY 1 C 5 ACT-I 4PI 63VE2 39Y 89 G/ ABX 0- 1 D 1 ACT-I 4P I

I SOMERS 1=1.33 MEV

58CH2 39Y 89 G N RLY THR CTHR 6F3-I 4P I RUBIDIUM Z = 37 THRESHOLD

60GE3 39Y 89 (3 N NOX T HR CTHR BF3-I 4P 1 THRESHOLD

ABUND. SEPARAT ION ENERGIES ( MEV ) 62 REl 39Y 89 N NOX fe- 5 5 C 55 THR-I DST

G .N G, P G . T G.HE3 G.A G.2N G.NP G . 2P 63GE 1 39Y 89 G N RLY ll - 1 2 C 11- 12 BF3-I 4PI

85 72.15 10 .5 7. 0 16.5 19.6 6.6 19.4 17.5 17.7 THRESHOLD

87 27.85 9 .9 8. 6 17 . 1 21.8 8.0 18.6 18.5 2 0.5 676E2 39Y 89 G N ABX THR- 28 DTHR- 28 BF3-I 4P I 69BE4 39Y 89 G N ABX 11- 2 5 D 11- 26 MODI

4P I 188

71 LEI 39Y 89 G N ABX 11- 2 7 D 11- 27 MOD- I 4P I 381 NUCLIDE REACTION RES EXCIT SOURCE DE TECTOR 7 1 SA

1

39Y 89 G N ABY 11- 68 C 10- 68 ACT- I 4P I REF 2 A IN OUT TYPE ANG NUM 66F U2 3 9 Y 8 9 2 N AB I THR — 28 DTHR- 28 BF3- I 4P I 66WA1 39Y 89 G 2N RLY THR- 280 C150 . 230 ACT-I 4P I 71LE1 37RB G N A8X 11- 24 D 11- 24 MOD- I 4PI 375 I SOMER RAT 10 Y 87 71LE1 37RB G 2N ABX 1 7- 24 D 11- 24 MOD- I 4P

I

376 57BE2 39Y 89 G 2N ABX THR- 28 DTHR- 28 BF3-I 4P I 1 + 61BA2 37RB G XN ABY THR- 22 C 22 THR-I DST 696E4 39Y 89 G 2N ABX 21- 27 D 19- 28 MOOI

4P I 189 70WA3 39Y 89 G 2N RLY THR- 305 C150- 305 ACT-I 4P I 58T01 37RB8 5 G N RLY 10- 11 C 22 ACT-I 4PI 7 1 LE

1

39Y 89 G 2N ABX 21- 27 D 11- 27 MODI

4P I 382 THRESHOLD 56YE2 39Y 89 G XN ABX 12- 23 C 24 BF3- I 4P I 60GE3 37RB85 G N NOX THR CTHR BF3-I 4PI 39Y 89 G XN ABX 12- 22 C 12- 22 BF3-I 4P I THRESHOLD 61BA2 39Y 89 G XN ABY THR- 22 C 22 THR-I OST 69KN1 37RBe5 G N RLY 10- 45 C 45 ACT-I 4PI 55FU2 39Y 89 G XN ABI ThR- 28 DTHR- 28 BF3-I 4PI ISOMER YIELD 59SH4 39Y 89 G P ABX 7- 24 C 17- 24 EMU-O DST 67TA2 39Y 89 6 XP SPC THR- 24 C 17. 24 EMU-D 4P I 58TOI 37RB87 G .N RLY 9- 11 C 22 BF3-I 4PI 70WA3 39Y 89 G PN RLY THR- 305 C150- 305 ACT- I 4P I THRESHOLD 68SH1 39Y 09 P G ABX 13- 15 D 5- 9 NAI-D DST 60GE3 37RB87 6 N NOX THR CTHR BF3-I 4PI 59R I 1 39Y 89 P G ABX 12 D 5 SCD-D 90 THRESHOLD 5 = 4.97-5.15 MEV

57ER1 37R887 G A ABI 8- 32 C 32 ACT-I 4PI 71UM1 39Y 89 P G ABX 10- 1

1

D 2- 3 NAI-D 0 57ER1 37RB87 G .NA AB I 17- 32 C 32 ACT-I 4PI

ZIRCONIUM Z=40 STRONTIUM Z=38

A ABUND. SEPARATION ENERGIES (MEV)

A ABUND. SEPARATION ENERGIES (MEV 1 G . N G .P G.T G.HE3 G . A G.2N G.NP G.2P

G .N G. P G.T G.HE3 G.A G.2N G .NP G.2P 90 51 46 12. 0 8 . 4 20.7 18.3 6. 7 21.3 19.8 15.4

84 0.55 12 .0 9. 0 20.2 17.9 5.2 21.2 19.8 14.6 91 1 1 23 7. 2 8 .7 18.5 14.9 5. 5 19.2 15.5 15.3

85 9.86 1

1

. 5 9. 5 20.5 19.5 6.3 20.0 20. 1 16.7 92 17 1

1

8. 6 9 . 4 15.7 17.2 3 . 0 15.8 17.3 17.1

87 7.02 8 . 4 9. 4 20.1 17.4 7.3 19.9 18.1 18.0 94 17 40 8. 2 10 .3 16.9 18.5 3. 8 14.9 17.8 18.9

88 82.56 1 1 . 1 10. 6 20.7 21.4 7.9 19.5 20.5 19.2 96 2 8C 7. 3 11 . 5 16. 1 20.4 4

.

9 14.3 18.5 21.3

NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A INiOUT TYPE ANG NUM

53KA2 38SR G G/ RLY 1 C 6 ACT-I 4P I 71LE1 3eSR G N ABX 11- 27 0 11- 27 MODI

4P I 378 71LE1 38SR G 2N ABX 19- 27 D 1 1- 27 MODI

4P I 379 51BA2 38SR G XN ABY THR- 22 C 22 THR- I DST 70HI 1 38SR G XN ABX 10- 27 C 10- 27 BF3- I 4P I 329

62CA1 38SR85 G N NOX 12- 30 C 30 ACT-I 4P I ISOMER RATIO

56YE2 38SR86 G XN ABX 11- 23 C 24 BF3- I 4P I

53VE2 38SR87 G G/ ABX 0- 1 D 1 ACT-I 4P I

I SOMERS 1=1.33 MEV

56YE2 38SRa7 G XN ABX 9- 23 C 24 BF3-I 4P I 580K3 38SR87 G P ABY THR- 20 C 20 ACT-I 4P I

66HE3 38SR88 E E/ FMF 1- 7 D187 MAG-D DST 58PE1 38SR88 E E/ RLY 1- 7 D 65 . 70 MAG-D DST B(ELI , 4 LEVELS

59SH5 38SR88 E P ABX 14- 25 D 16- 30 MAG-D UKN 59SH6 38SR88 E P SPC 14- 30 D 30 MAG-D UKN 54BE7 38SR88 G G LFT 2 D 2 UKN-D UKN 2=1.85 MEV

55YE2 38SR88 G XN ABX 11- 23 C 24 BF3- I 4P I 71BL1 38SR8e G PI + ABY 150- 700 C150- 700 ACT-I 4P I SEE 58NY1

59HA1 36SR88 P G RLX 15- 22 D 4- 12 NAI-D 90 207

NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN .OUT TYPE ANG NUM

50RE1 40ZR G G ABX 7 0 7 NAI-D 90 66BE3 40ZR G G RLX 5- 10 0 5- 10 NAI-D 135 70AX1 402R G G ABX 8- 1 3 0 8- 13 NAI-D 22 67HU2 40ZR G N ABY THR- 22 THR-I DST 64DU1 40ZR G P ABX THR- 34 C 22- 34 MAG-D DST ABX

65DU1 40ZR G P ABX 18- 25 D 17- 24 EMU-D DST 69SH4 40ZR G P ABX 8- 24 C 20. 24 EMU-D DST 63M15 40ZR G XP ABY 8- 22 C 22 SCI-I DST

59B02 40ZR90 E E/ FMF 2- 4 D 58 MAG-D DST

2. 18 TO 3.84 MEV

70BE2 40ZR90 E E/ ABX 0- 4 D 42- 51 MAG-D DST

2. 18. 2.74.3.84

68SH4 402R90 E P SPC 11- 20 D 20 MAG-D 90 ANALOG STATES

59SH5 40ZR90 E P ABX 12- 23 D 16- 24 MAG-D UKN 59SH6 40ZR90 E P SPC 12- 22 D 15- 23 MAG-D DST 53AX1 40ZR90 G G ABX 8- 13 D 8- 13 NAI-D 135 59RA1 40ZR90 G G LFT 9 D 9 NAI-D DST

9 = 8.496 MEV

56AX 1 40ZR90 G N RLX 12- 23 C 12- 23 ACT-I 4P I THRESHOLD

59MU2 40ZR90 G N RLX 12- 24 C 12- 25 ACT-1 4P I 52CA1 40ZR90 G N NOX 12- 30 C 30 ACT- I 4P I ISOMERIC RATIO

65C01 40ZR90 G N ABX THR- 70 C 12- 70 ACT- I 4P I 67BE2 40ZR90 G N ABX THR- 28 DTHR- 28 BF3- I 4PI 10 + 71LE1 40ZR90 G N ABX 12- 26 0 12- 25 MOD- I 4P I 384 56FU2 40ZR90 G 2N ABI THR- 28 DTHR- 28 BF3-I 4P I 67BE2 40ZR90 G 2N ABX THR- 28 DTHR- 28 BF3-I 4P I 10 + 71LE1 40ZR90 G 2N ABX 21- 25 D 12- 26 MOD- I 4P I 385

38
NUCLIDE REACTION RES tXC 1 T REF Z A I N OU T

56YE2 40ZR90 S .XN ABX 12- 23 59NA1 4UZR90 5 .XN ABX 12- 24

^+0 Z R 9 0 G .XN 69AN7 40ZR90 G-.XN ABX 12- 23 71IS2 4t'ZR90 G'.XN ABX 12- 28 4UZR90 p..G RLX 13- 17

660B1 40ZR90 P ..6 RLX 11- 14 67AX1 40ZR90 P '. G ABX 14- 25 670B1 40ZR9 0 P :iG ABX 12 — 1 3 69HA1 40ZR90 P iiG RLX 16- 22 59MA4 40ZR90 P .iG ABX 10- 27 71UK1 40ZR90 P ..G ABX 9- 10

6 7 BE 2 40Z R 9

1

G,.N 3 0 65FU2 40ZR9

1

G :,2N AB I THR- 30 578E2 40ZR91 G.,2N ABX THR- 30 55NA1 40ZR9 1 G !. XN ABX 7- 24

56YE2 40ZR91 G .,XN ABX 7- 23 66FU2 40ZR91 G..XN ABI THR- 30 69AN7 40ZR9

1

G 1,XN ABX 12- 23

67BE2 40ZR92 G 11 N ABX THR- 28 66FU2 40 ZR 92 G 1,2N A8 I 2 8 67BE2 40ZR92 G .,2N ABX THR- 28 56YE2 40ZR92 G .iXN ABX 9- 23 66FU2 40ZR92 G .iXN AB I TriR- 23

67^E2 4JZR94 G tiN ABX THR- 30 55FU2 40ZR94 G .,2N AB I THR- 30 67BE2 4UZR94 G .i2N ABX THR- 30 66FU2 4uZR94 G.iXN ABI THR- 30

DETECTOR

TYPE ANG NUH

C 24 BF3-1 4PI

C 5- 24 BF3-I 4PI THRESHOLD

DTHR- 28 BF3-I 4P

I

23 BF3-I 4PI

- 28 BF3-

NAI- ANALOGUE

2-

5-4-

7-

6 NAI

17 NAI

3 NAI

14 NAI

19 NAI

-I 4PI 413

-D OST

= 6 90

90

0 DST

DST

0

30 BF3-I 4PI

30 BF3-I 4PI

30 BF3-! 4P1

24 BF3-I 4PI THRESHOLD

aF3-I 4PI

30 BF3-I 4PI

23 BF3-I 4PI

28 BF3-I 4PI 10+

28 BF3-I 4PI

28 BF3-I 4PI 10+ 8F3-I 4PI

28 BF3-I 4PI

30 BF3-I 4PI

30 BF3-I 4P I 30 BF3-I 4PI 12+

30 8F3-I 4P I

NIOBIUM 2=41

SEPARATION ENERGIES IMEV) G,2N G.NP

16.7 14.7 G.N G. P G .T G.HE3 G 93 100.00 8.8 6. 0 1

3

. 4 15. 7 I

NUCLIDE REACT I ON RES EXC I T SOUi REF Z A IN..OUT

67SH1 41NB93 E .E/ FMF 2- 3 D225

58CH2 41NB93 G .N RLY THR CTHR

58SI2 41NB93 G..N ABX 8- 22 C 8- 50GE3 41NB93 G <H NOX THR CTHR

6 IWEl 41NB93 G .N ABX 9- 10 D 9- 67HU1 41NS93 G'.N ABX 9- 1 1 D 9

.

67HU2 4 1N393 G .N AB-' THR- 22 C 22 71LE1 41NB93 G'.N ABX 9- 24 D 9- 71SA1 41NB93 G .N ABY 8- 68 C 10- 71LE1 41NB93 G .2N ABX 16- 24 D 9- 58KA1 41NB9 3 G 'iXN ABX 9- 22 C 9- 60BA5 41NBP3 G..P ABX 14- 40 C 40

60BA6 41NB93 G',P SPC 17- 40 C 10- 630S1 41NB93 G:.P RLY 10- 28 C 19-

63MI5 41NB93 G :iXP ABY 10- 22 C 22 64SC3 41NB93 G:,XP SPC THR- 32 C 32

58T02 41NB93 G ilA ABY 2- 22 C 22 64SC1 41NB93 G,.A SPC THR- 33 c 33

67KR1 41Ne93 G '.A SPC 2- 31 c 31 68<R2 41NB93 G ..A ABX ThR- 33 c 33 65WA1 41NB93 G.,4N2P RLY THR- 280 C150

G,2P

15.4

71G02 41N893

CE DETECTOR

TYPE ANG NUM

MAG-D DST

2.2 MEV

BF3-I 4PI THRESHOLD

22 ACT-I 4PI 3F3-I 4PI THRESHOLD

11 ACT-I 4PI

11 8F3-I 4PI THR-I DST

24 MOD-I 4PI 369

68 ACT-I 4PI

24 .MOD-I 4PI 370

22 BF3-1 4P! MAG-D DST SPECTRUM

40 .Y.AG-D OST

28 EMU-O DST SPECTRUM

SCI-I DST SCI-D 90 ABY

EMU- I DST SCD-D 90 ABS YIELD SCD-D 90 SCD-O 90

ISOMER RATIO Y 87 RLY 150-500 C500 CCH-D DaT PI-/P I + YIELD RAT 10

MOLYBDENUM Z=42

SEPARATION ENERGIES IMEV) G.N G,P G.T G.HE3 G. A G.2N G.NP G,2P

92 15.84 12.7 7.5 20.8 16.9 5. 6 22.8 19.5 12.5

94 9.04 9.7 8.5 16.7 15.4 2. 1 17.7 17.3 14.5

95 1 5. 72 7.4 8.6 16.2 14.2 2. 2 17.0 15.9 15.1

96 16.53 9.2 9.3 16.5 15.6 2 . 8 15.5 17.8 16.1

97 9.46 6.8 9.2 16.1 15.2 2. 8 16.0 16. 1 16.5

98 23. 78 8.6 9.3 15.3 17.4 3. 3 15.5 17.9 17.3

100 9.63 8.3 10.6 15.5 18.2 3. 2 14.2 18.0 19.5

REF

50RE1 56BE3

57HU2

68 Jul 71C02

55J01

53M I 5

54GE1

68GE1

70IS1

7 1M02

64GE1

57FE3

54GE1

NUCLIDE REACTION RES

Z A IN. OUT DETECTOR

TYPE ANG NUM

42M0

42M0

42M0

42M0 42M0

42M0

42MO

G.G

G.G

G.N G.N

G .XN

G .P G.XP

ABX

RLX

75- 10 ABY THR- 22 NOX THR- 22 ABI 36- 64

RLY THR- ABY 10-

D 7 NAI- 0 90

D 5- 10 NAI- D 135

C 22 THR- I DST

C 22 THR- I DST

C 10- 64 BF3- I 4PI FAST N YIELD

C 65 sei- D DST

C 22 se I- I DST

69SH6 42M092 E .P SPC 11- 18 D 20 MAG-D UKN 59MU2 42M092 G .N ABX 13- 24 C 0 - 25 ACT-I 4PI 62CA1 42M092 G .N NOX 7- 30 C 30 ACT-I 4PI ISOMERIC RATIO

62DE1 42M092 G..N ABX 21 D 21 ACT-I 4PI 54GE1 42M092 G ..N ABX THR- 22 CTHR - 33 ACT-I 4PI 65C01 42M092 G..N RLX THR- 70 C 12 - 70 ACT-I 4PI 58GE1 42M092 G .N ABX 12- 26 CTHR - 26 ACT-I 4PI 680K2 42M092 G..N ABY THR- 20 C 20 ACT-I 4PI ISOMERIC YIELD

71HA2 42M092 G.>N RLY 13- 70 C 70 ACT-I 4PI ISOMER RATIO

64GE1 42M092 G .,2N ABX THR- 33 CTHR - 33 ACT-I 4PI MIXED WITH G.NP

70WA3 42M092 G i,2N RLY THR- 305 C150 -305 ACT-I 4PI 70IS1 42M092 G..XN ABX THR- 30 CTHR - 30 BF3-I 4P! 57EL1 42M092 G.,P RLY THR- 32 C 32 ACT-I 4PI 57EL1 42M092 G..NP RLY THR- 32 C 32 ACT-I 4PI 58H01 42M092 G..NP RLY 19- 32 C 32 ACT-I 4PI THRESHOLD

64GE1 42M092 G..NP ABX THR- 33 CTHR - 33 ACT-I 4PI MIXED WITH G,2N

70WA3 42M092 G.iPN RLY THR- 305 C150 -305 ACT-I 4PI

71HA2 42M094 G .,3N RLY 31- 70 C 70 ACT-I 4PI ISOMER RATIO

57LA3 42M095 G..G LFT 1 D 1 NAI-D DST

1

==0.755 MEV

69BE7 42M096 G ..G LFT 6 D 6 D OST 5.41 ., 5.44 MEV 69AN6 42M096 Gi,P ABY 106- 999 C700 .999 TEL-D DST

59AN6 42M095

52JA1 42M096

999=1.2 GEV 113-999 C701J,999 TEL-D DST 999=1.2 GEV

9 DO- NAI-D 90

42M097 42M097

42M098

G..P ABX THR- 26 CTHR- 33 ACT-I 4P I G..P ABX 13- 25 CTHR- 25 ACT-I 4PI

G..XN ABX THR- 30 CTHR- 30 BF3-I 4P1 445

54GE 1 42M098 G ..P ABX THR- 26 CTHR- 33 ACT-I 4P I 58GE1 42M098 G 1,P ABX 13- 25 CTHR- 25 ACT-I 4P I 64GE1 42M098 G,.NP ABX THR- 32 CTHR- 33 ACT-I 4P 1

42M0100 G.P 42MO100 G.P

58GE1 42M010U G.N+P ABX

6 D 5. 6 SCD-D DST 5.418 MEV

HR- 20 CTHR- 33 ACT-I 4PI MIXED WITH G.P

14- 31 C 14- 31 ACT-I 4PI

HR- 20 CTHR- 33 ACT-I 4P

I

MIXED WITH G,N

7- 26 CTHR- 25 ACT-I 4P

I

TECHNETIUM Z=43

SEPARATION ENERGIES (MEVl G.N G.P G.T G.HE3 G.A 6.2N G.NP G,2P

12.8 4.1 18.4 16.9 5.1 23.2 16.8 11.6

REF

69EJ2 43TC93

NUCLIDE REACTION RES EXCIT

Z A IN. OUT

10 D 6. 5.75-6

DETECTOR

TYPE ANG NUM

7 SCD-O DST ,05.6.5-5.63

39
RUTHENIUM Z=4't SILVER Z = ii7

SEPARATION ENERGIES IMEV] G.N G.P G.T G.HE3 G.A G>2N G .NP G,2P

95 5.51 10.7 7.4 17.4 14.2 1.7 19.5 17.3 12.2

98 1.87 10.3 8.3 17.2 15.4 2.2 18.3 17.7 14.0

99 12.72 7.5 8.4 16.7 13.8 2.3 17.7 15.8 14.7

100 12.62 9 . 7 9.2 17.0 16.5 2 .

9

17.1 18. 1 15.7

101 17.07 6.8 9.4 16.4 14.8 2.8 16.5 15,0 15.6

102 31.61 9.2 10.1 16.7 18.1 3.4 16.0 18.6 17.5

10* 18.58 8.9 10.5 16.7 19.5 4.3 15.1 18.9 19.1

NUCLI DE REACTION RES EXCIT SOURCE DE TECTOR

REE Z A IN OUT TYPE ANG NUM

68JU1 44RU G N NOX THR - 27 C 27 THR- DST

SEPARATION ENERGIES (MEVl G.T G.HE3 G.A G.2N G.NP

RHODIUM z=45

SEPARATION ENERGIES (MEV) G.P G.T G.HE3 G.A G.2N G.NP

5.3 14.5 13.3 2.2 18.6 12.7 G,2P13.7

REF

65<R1

NUCLIDE REACTION RES

Z A IN, OUT

59K1 45RH103 G 6/ ABX 1 50BO2 45RH103 G G/ ABX 5 63VE2 45RH103 G G/ ABX 0

EXC I T

65<R1

5eCH2

59PA2

6UGE3

45RH103

45RH103

45RH103

45RH103

G .G/

G.N

G.N

G.N

RLY 7-

RLY THR

ABX 9-

NOX THR

DETECTOR

TYPE ANG NUM

D 7- 18 ACT-I 4PI ISOMER YIELD

D 1 ACT-I 4PI

C 5- 26 ACT-I 4PI

D 1 ACT-I 4PI ISOMERS 1=1.33 MEV

C 7- 18 ACT-I 4PI ISOMER YIELD

CTHR BF3-I 4PI THRESHOLD

C 9- 24 BF3-I 4PI QUADRUPOLE MOMENT

CTHR BF3-I 4PI THRESHOLD

52B01 45RH103 G N ABX 10- 23 C 10- 23 BF3-I 4PI 428 57HU1 45RH103 G N ABX 10. 11 D 10 , 1

1

BF3-I 4PI 68JU1 46RH103 G N NOX THR- 27 C 27 THR-I DST 69DE1 45RH103 G N ABY THR- 999 C 1- 6 ACT-1 4PI 999=5.5 GEV 69DE1 45RH103 G 2N ABY THR- 999 C 1- 5 ACT-1 4PI 999=5.5 GEV

58KA1 45RH103 G XN ABX 9- 22 C 9- 22 BF3-I 4PI 52SH2 45RH103 G P ABY 9- 34 C 23 . 34 EMU-D DST SPECTRUM

62SH4 45RH103 G P ABY 9- 34 C 23 . 34 EMU-D DST SPECTRUM

55KR1 45RH103 G 2P ABX 15- 40 C 15- 40 ACT-I 4PI 56DA2 45RH103 G XP ABY 10- 70 C 70 EMU-D DST SPECTRUM

53 I S2 45RH103 G XP ABX 13- 32 C 14- 32 SCI-D DST 58T02 45RH103 G A ABY THR- 22 C 22 EMU-I DST

PALLADIUM Z=46

102 104

105

106 108 no

A8UND.

0.95

10.97 22.23

27.33

26.71

11.81

G.N

10.5

10.0

7. 1 9.5

9.2

G.P

7.8

9.3 10.0

SEPARATION ENERGIES (MEV) G.T G.HE3 G.A G,2N G,NP G,2P

17.3 17.0

16.6

15.8 15.6

.8 10.5 16.4 19.6

15.2 2.1 18.9

16.4 2.6 17.6

14.2 2.9 17.1 17.6 3.2 15.6 18.5 3.9 15.8 4.4 15.0

7.7 8.0

5.8

8.3

8.5 8.7

13.3 14.9

15.7

16.4 17.8

19.2

68 Jul 67KN1

NUCLIDE

Z A

46PD

46PD

REACTION RES EXCIT

IN. OUT SOURCE DETECTORTYPE ANG NUM

G.N

G.T

NOX THRRLY THR27 C 27 49 C 36. THR-I DST

49 ACT-I 4PI

107 51.35 9.6 5. 8 13 .9 16.4 2. 6 17.5 15.4

109 48.55 9.2 5. 5 13 .8 17.3 3. 3 16.5 15.7

NUCLIDE REACT I ON RES EXCIT SOURCE DETECTOR

REF Z A I N OUT TYPE ANG

65WY 1 47AG MU- T ABX 10- 3 5 c 90 SCI-D 4PI 60RE1 47AG (3 . G ABX 7 7 NAI-D DST G-WDTH

58B01 47AG (3 G/ ABX 5- 28 G 5 — 28 ACT-I 4PI ISOMER YIELD

63KA2 47AG G / RLY G 5 ACT-I 4P

1

57FE1 47AG (3 N RLY 17- 3 ^ G 15- 3 I THR-I DST 61TA1 47AG G N NOX 7- 2 2 c 22 THR-1 DST 67GE2 47AG G )N ABY THR- 27 C 22, 27 BF3-I 4P

I

57HU1 47AG G >N ABX 10 > 1 1 D 10 , 1

1

BF3-I 4P

1

56HA1 47AG G ,XN ABX 16. 18 D 1 5 . 18 BF3-I 4PI

5 1BA2 47AG G .XN ABY THR- 22 C 22 THR-I DST

58F I 1 47AG G • XN ABX 9- 25 C 9- 25 BF3-I 4P

I

59L01 47AG G ,p ABX 17- 3 1 c 16- 32 SCI-D DST SPECTRUM

62SE2 47AG G ,P ABX 1 5 , 18 D 15, 18 SCI-I 0 63M I 5 47AG G .XP ABY 4- 22 C 22 SCI-I DST 58T02 47AG G A ABY 2- 22 C 22 EMU-I DST 55ME2 47AG G A SPC THR- 35 C 35 SCD-D 90 56WE2 47AG G >A ABX 3- 33 C 33 SCD-D 90 72KE4 47AG G .A RLY 2- 32 C 32 SCD-D DST 55WA1 47AG G . T RLY THR- 3

1

C 31 ACT-I 4PI 540E4 47AG G F ABX 300- 999 C300- 999 EMU-D 4PI 999=1 GEV

71ME1 47AG G F ABY T HR- 900 C300- 900 TRK-l 4P

I

55HE1 47AG107 N RLY T HR - 3 2 D 14- 32 ACT-I 4PI 72KU5 47AG107 N ABX 10- 3 0 D 2 0- 30 ACT-I 4PI

(E + .N ) / ( E-.N

)

65HE1 47AG107 E + N RLY THR- 3 2 D 14- 32 ACT-I 4PI 63B I 3 47AG107 G G ABX 1 D 1 ACT-I 4PI MOSSBAUER

69B03 47AG1 07 G G ABX 0- 2 C 0- 2 ACT-I 4PI 63B05 47AG107 G G/ ABX 6- 26 C 5- 25 ACT-I 4PI SEPARATED ISOTOPES

53VE2 47AG107 G G/ ABX 0- 1 D 1 ACT-I 4PI

I SOMERS 1=1.33 MEV

56CA1 47AG107 G G/ AB I 0- 2 C 0- 2 ACT-I 4PI

5 LEVELS

58BE1 47AG107 G N RLY 9- 10 C 9- 10 ACT-I 4PI THRESHOLD

59MU2 47AG107 G N ABX 9- 21 C 9- 25 ACT-I 4PI 60GE3 47AG107 G N NOX THR CTHR BF3-I 4PI THRESHOLD

61WE1 47AG107 G N ABX 9- 1 1 D 9- 11 ACT-I 4PI THRESHOLD

52B01 47AG107 G N ABX 10- 22 C 10- 22 BF3-I 4PI 52CA1 47AG107 G N NOX g_ 3 0 C 30 ACT-I 4PI ISOMERIC RATIO

62FU5 47AG1 07 G N RLY 9 - 34 C 34 ACT-I 4PI YLO REL TO CU62 69BE1 47AG1 07 G N ABX THR- 3 0 0 9- 30 BF3-I 4PI SEP ISOTOPES

69BE 1 47AG1 07 G 2N ABX THR- 30 D 17- 30 BF3-I 4PI SEP ISOTOPES

69 I S2 47AG107 G X N ABX g _ 2 9 C 7- 30 BF3-I 4PI 66W I 1 47AG1 07 G J ABX THR — 5 6 C 31- 56 ACT-I 4PI

59B03 47AG109 G G ABX 0- 2 c 0- 2 ACT-I 4PI 70M02 47AG109 G G ABX Q D 8 SCD-D DST

8 =7. 632. LET 66CA1 47AG109 G G/ A8I 0- 2 C 0- 2 ACT-I 4PI

5 LEVELS

58BE1 47AG109 G N RLY 9- 10 C 9- 10 ACT-I 4PI THRESHOLD

59NA1 47AG109 G N ABX 18 D 18 BF3-I 4P

1

50GE3 47AG109 G N NOX THR CTHR BF3-I 4PI THRESHOLD

59IS2 47AG109 G XN ABX 9- 29 C 7- 30 BF3-I 4PI 55ER1 47AG1 09 G A ABY THR- 31 C 32 ACT-I 4PI 55SC2 47AG109 G A ABY THR- 32 C 32 ACT-I 4PI 57ER1 47AG109 G A ABI THR- 32 C 32 ACT-I API 59R03 47AG109 G A ABX 15- 25 C 15- 25 ACT-I 4PI 580K1 47AG109 G A ABY THR- 20 C 20 ACT-1 4P

I

6.2P

15.1 16.4

580K3

62ME1

71SH6

46PD104

45PD105

46PD105

G ,NP

G.G

G,G

ABY THR- 20 C 20 ACT-I 4PI

NOX

LET

D 1 NAI-D DST

J-PI .TRANS PROBABL

0 1 NAI-D UKN 1=.319 MEV

59DA1 46PD105 G.G ABY NAI-D 120 1=.5117 MEV

69DE2

69DE5

59DE2 59DE5

46P0108 45PD108

45PD108 45PD106

G.XN

G.XN

G.P

G.P

ABX ABX

ABX

ABX

25 C 26 C 26 C 28 C

25 BF3-I 4PI 184

25 BF3-I 4PI

25 ACT-I 4PI 183

28 ACT-I 4P1

69DE5 46P0110 G.N ABX : 8- 28 ACT-I 4P1 ISOMER YIELD ONLY

i)0
CADMIUM Z=48

A ABUND. SEPARAT ION ENERGIES (MEVl

G • N G. P C ,T G.HE3 G . A G.2N G.NP G. 2P 105 1.22 10 .9 7. 3 17 . 3 14. 6 1 . 6 19.3 17.2 12 . 3 108 0 . 88 10 . 3 8. 1 17 . 1 15. 8 2. 3 18.3 17.7 13 ,9 no 12.39 9 .9 8. 9 16 . 9 15. 9 2 . 9 17.2 18.1 15.4

111 12. 75 7 .0 9. 1 16 .5 14. 7 3. 3 15.9 15.9 16 .2 112 24.07 9 . 4 9. 5 15.8 17. 9 3. 5 15.4 18.5 16 .8

1 1 3 12.25 6 . 5 9. 8 16.5 15. 6 3. 9 15.9 15.2 1 7 .5

1 1-* 28.86 9 .0 10. 3 15 . 7 18. 9 4 . 1 15.6 18.8 18 .3 116 7.58 8 .7 11. 1 15 .5 15.6 4. 9 14,8 19.1 »

NUCL I DE REACTION RES EXCIT SOURCE DETECTOR

REF 2 A I N .OUT TYPE ANG NUM

71V01 48CD E >N ABX THR- 256 C150- 255 TOF-D 90 55BU1 48CD G >G RLX 0- 3 C 3 NAI-D 90 60RE1 48CD G .G ABX 7 0 7 NAI-D 90 61T01 48CD G .G ABX 4- 14 C 4- 14 NAI-D 120 635U1 48CD G .G ABX 4- 14 Q 4- 14 NAI-D 120 64611 48CD G .G NOX 8 Q 8 NAI-D 135 WIDTH

66 BE 3 48C0 . G RLX 5- 1

0

0 5- 10 NAI-D 135 69RA 1 48CD .G NOX D 7 NAI-D DST 7=6.485 MEV

70 AR 1 48 CD G . G ABX 12 — 30 C 32 NAI-D DST RATIO G.G/TO 2+

63K,A2 4ecD G G/ RLY 1 c 6 ACT-I 4PI 65C I 1 48C0 G G/ RLY 8 D 8 NAI-D 135 8=7.54 MEV

60KU2 48CD G N RLY 16- 90 c 90 TEL-I DST 67HU2 48CD G N ABY THR- 22 C 22 THR-I DST 55MC1 48CD G XN RLY THR- 22 C 22 NAI-I 90 56GA1 48CD G XN ABX 6- 27 c 6- 27 BP3-I 4PI 61BA2 48CD G XN ABY THR- 22 C 22 THR-I DST 60RO3 4eCD G P SPC 18 0 18 EMJ-D DST 63MI5 48C0 G XP ABY 11- 22 c 22 SCI-I DST 63KR1 48CD G A SPC 3- 21 c 21 SCD-D 90 RELATIVE YIELD

69M I 1 48CD11U G G SPC 5- 8 D 5- 8 SCD-D DST

65CH1 48C01 1

1

E E/ ABX 1 0 1- 2 ACT-I 4PI 1=1.34 MEV 69B03 48CD1 1

1

G G ABX 0- 2 C 0- 2 ACT-I 4PI 71SH6 48CD1 1

1

G G LPT 1 D 1 NAl-D U<N

1=.342 MEV

62HU2 48C01 1

1

G G/ ABX 7 D 7 ACT-I 4PI ISOMERIC RATIO

63VE 1 48CD1 1

1

G G / NOX 1 — 2 D 1- NAI-D 90 56CA1 48CD1 1

1

G G/ AB I 0- 2 c 0- 2 ACT-I 4PI

76 . 1.12. 1 . 3 MEV

66MI1 48CD1 12 G ABX 0 8 NAI-D DST 8=7.54 MEV

68M01 48CD1 12 I G G NOX 7 D NAI-D 90 POLARIMETER 7.53

69CE1 48CD1 12 G G NOX 5- 8 D 6- 8 SCD-D DST 69M I 1 48CD112 G G SPC 5- 6 D 6- 8 SCD-D DST 70ES1 48CD1 12 G G NOX 7 D 7 SCD-D DST 7=7,64

70MO2 48CD1 12 G G ABX 8 D 8 SCD-D DST 8=7.532.LFT

7 1M04 48CD1 12 G G LPT 7 D 7 SCD-D DST

J. PI .POL 7=7.632

71M02 48CD1 12 G G/ LP 7 6 . 8 D 6 . 8 SCD-D DST 6.018. 7.632 MEV

59KU2 48CD1 12 G P ABX TriR- 28 C 1 5- 28 ACT-I 4PI 60KU1 48C01 1

2

G P ABX 10- 30 C 10- 30 ACT-I 4PI

59<U2 48CD113 G P ABX THR- 28 C 15- 28 ACT-I 4PI 60KU1 48CD1 1

3

G P ABX 10- 30 C 10- 30 ACT-I 4PI 680K3 48C01 1

3

G P ABY THR- 20 C 20 ACT-I 4PI

67ST1 48CD 1 14 G G LPT 7 0 7 NAI-D 135 7=7.54 MEV

59<U2 48CD1 14 G P A13X THR- 28 C 15- 28 ACT-I 4PI 60KU1 48CD1 14 G P ABX 10- 30 C 10- 30 ACT-I 4PI

52CA1 48CD1 15 G N NOX 9- 30 C 3 0 ACT-I 4PI ISOMERIC RATIO

59KU2 48CD1 16 G P ABX THR- 28 c 15- 28 ACT-I 4PI 60HU1 48CD116 G P ABX 11- 30 c 1 1- 30 ACT-I 4PI

INDIUM Z=49

A ABUND. SEPARAT ION ENERGIES (MEV)

G ,N G. P G .T G.HE3 G.A G.2N G.NP G . 2P

1 13 4.28 9 .4 6. 1 13 .9 16,

e

3.0 17,1 15,5 15.7

1 15 95. 72 9.0 6. 8 1

3

.9 17.

?

3,7 16,3 15,9 17.1

NUCL I DE REACT ION RES EXC I T SOURCE DETECTOR

REF Z A I N OUT TYPE ANG NUM

55BU1 49IN G G RLX 0- 3 C 3 NAI-D 90 70AR1 49IN G G ABX 12- 30 C 32 NAI-D DST RATIO G.G/TO 2+ 55BU2 49IN G G/ ABX 0- 1 4 C 1- 14 ACT-I 4PI

53k;A2 49IN G .0/ RLY 1 C 6 ACT-I 4PI 6eKAl 49IN G N ABX 50- 85 C 56. 85 TOP-D 57 NEUT ENGY SPEC

69FU1 49IN G .N ABX 9- 31 D 9- 31 BF3-I 4PI 140 69FU1 49 I N G .2N ABX 15- 31 D 15- 31 BF3-I 4P1 141 59FU1 49 I N G .3N ABX 25- 31 D 25- 31 BF3-I 4PI 142 + 57R02 49IN G ,P SPC 15. 18 D 15. 18 EMU-D DST 60BA5 49IN G ,P ABX 16- 40 C 16- 40 MAG-D DST 60CH1 49IN G . XP RLX THR- 90 C OA TCI I o r\ 9U 1 t L— 1 9 U REL TO OEUTERONS

53M I 5 49 I N G XP ABY 8- 22 c 22 SCI-I DST 60CH1 49IN G .XD RLX THR- 90 c 90 TEL-I 90 REL TO PROTONS

50CH1 49IN G XT RLY THR- 90 c 90 TEL-I 90 REL TO DEUTERONS

5 8 T02 G A ABY 1- 22 c 22 EMU-I DST 55ME2 49IN G A SPC THR- 35 c 35 SCD-D 90

56VE1 49IN113 G G/ ABX 1 D 0- 1 ACT-I 4PI 1=,392 MEV

52CA1 49IN113 G N NOX 5- 30 C 30 ACT-I 4PI ISOMERIC RATIO

55CH1 49IN115 E E/ ABX 1 0 1- 2 ACT-I 4PI 1=1,07 MEV

55KR1 49IN115 E E/ RLY 7- 18 D 7- 18 ACT-I 4PI ISOMER YIELD

58B03 49IN115 G G AB I 1 . 1 C 0- 1 ACT-I 4PI 1.1=600.830 KEV 69AL1 49IN115 G .G SPC 0- 3 c 1- 3 SCD-D 70

10 LEVELS

59B03 49IN115 G G ABX 0- 2 c 0- 2 ACT-I 4PI 55B01 49IN115 G G/ ABX 5- 27 c 5- 27 ACT-I 4PI 52HU2 49IN115 G G/ NOX 7 0 7 ACT-1 4PI ISOMERIC RATIO

63VE1 49IN1 15 G G/ NOX 1- 2 D 1- NAI-D 90 65KR1 49 INI 15 G G/ RLY 7- 18 C 7- 18 ACT-I 4P

1

ISOMER YIELD

56VE1 49 ; Nl 1

5

G G/ ABX 1 D 0- 1 ACT-I 4PI 1=1.04 MEV

71B01 49IN115 G G/ ABX 0- 2 C 0- 2 ACT-I 4PI

9 LEVS..6-1,6 MEV

55B01 49 INI 15 G N ABX 9- 27 C 9- 27 eF3-I 4PI 5eBEl 49 I N 1 1 5 G N RLY 9- 10 C 9- 10 ACT-I 4PI THRESHOLD

60GE3 49IN115 G N NOX THR CTHR BF3-I 4PI THRESHOLD

52AN1 49IN115 G N SPC 9- 28 C 28 EMU-0 DST 62B01 49IN115 G N ABX 10- 23 C 10- 23 BF3-I 4PI 457 67HU1 49IN115 G N ABX 10. 11 0 10. 11 BP3-I 4PI 55HE2 49IN115 G 2P RLY THR- 31 C 31 ACT-I 4PI REL G.A

55HE2 49IN115 G A RLY THR- 31 C 31 ACT-I 4PI REL NEUTRONS

680K1 49IN115 G A ABY THR- 20 C 20 ACT-I 4PI

TIN 2 = 50

A ABUND. SEPARAT ION ENERGIES (MEV)

G .N G. P G . T G.HE3 G.A G.2N G.NP G.2P

112 0.96 10 .8 7. 5 17 . 1 15.0 1,8 19,0 17.6 12.9

1 14 0.55 10 .3 e. 5 17,1 16.2 2.5 18.1 17.9 14.6

115 0.35 7 , 5 8. 7 17 .0 14,4 J. 2 17.9 15.0 15,6

1 16 14.30 9 ,5 9. 3 17 , 1 17,4 3,4 17.1 18.3 15.1

117 7.61 5 .9 9. 4 15,8 15,3 3.8 15.5 15.2 16.9

118 24.03 9 . 3 10. 0 17 . 1 18.5 4.1 15.3 18.8 17.5

119 8.58 6 .5 9. 9 15 .8 15,3 4.4 15,8 15.5 18.2

120 32.85 9 . 1 10.7 17.1 19.5 4.8 15.5 19.0 19.0

122 4. 72 8 .8 11.4 17 ,2 20.7 5.7 15.0 19.8

124 5. 94 8 .5 12. 1 1 7 ,4 « * 14.4 20.4

NUCL I DE REACT ION RES EXCIT SOURCE DETECTOR

REF Z A I N OUT TYPE ANG NUM

71 MO 3 50SN E E/ ABX 0- 240 D500 MAG-D 60 55PU1 50SN G G ABX 4- 40 C 4- 40 NAI-D 120 60RE1 50SN G G ABX 7 D 7 NAI-D DST G-WDTH

61T01 50SN G G ABX 3- 15 C 3- 15 NAI-D 120 62BE2 50SN G G ABX 5- 9 D 5- NAI-D 135 53AX 1 50SN G G ABX 5- 10 0 6- 10 NAI-D 135 53KA3 50SN G G ABX 1 , 1 D 1. NAI-D 120 54AR1 50SN G G ABX 6. 7 D 6. NAI-D 135 65BE3 50SN G G RLX 5- 10 D 5- 10 NAI-0 135
NUCLIDE REACTION RES

Z A IN. OUT

70AX 1 50SN G G ABX 5- 10 0 53<A2 50SN G G/ RLY 1 C 57HU2 50SN G N ABY THR- 22 C 68KA1 50SN G N ABX 50- 85 C

55DI 1 50SN G XN NOX THR- 70 C 70 56HA1 50SN G XN ABX 15 . 18 0 15 58FU1 50SN G XN ABX 7- 40 C 7 64AL5 50SN G XN NOX THR- 34 C 34 60RO3 50SN G P SPC 18 D 18 63M I 5 50SN G XP ABY 10- 22 C 22 53YA2 50SN G D RLY 12- 24 C 24

50SN 50SN

51I^U1 50SN112 G N ABX 10- 21 c 10- 21 ACT- I 4P I 62DE1 51SB121 G N ABX 20 D 20 71S01 50SN112 G XP ABX 10- 29 c 8- 29 SCO-D 4P I 57ER1 51SB121 G D ABX 18- 32 C 18 55ER1 51SB121 G A ABY THR- 31 C 32 70BR1 50SN1 14 G P RLY 12- 22 c 1 4- 23 ACT-I 4PI 56HE2 51SB121 G A RLY THR- 31 C 31

67BA4 50SN116 E E/ FMF 1 • 2 D150 MAG-D DST 61W01 5156121- G A ABX 15- 24 C 15- 24 ACT-I 4PI

69CU1 50SN116 E E/ FMF 1- 12 D 55 , 1.27,2.24

60 MAG-D

MEV

DST 64SH5 51SB123 G G LFT 1 D 1 NAI-D 122 69SH7 50SN116 E P ABY 14- 19 D 19 MAG-D DST 1=0.161 MEV 72SU4 50SN116 E P ABI 13- 19 D 16- 21 MAG-D 4P I 50GE3 51SB123 G N NOX THR CTHR BF3-I 4PI 62KA1 50SN1 16 G G LFT 1 D 1 NAI-D UKN THRESHOLD

62LI2 538E6 50SN116

50SN115

G

G

6

G LFT

LFT

1

1

D

D

11 NAI-D

NAI-0

132 100 58H01 51SB123 G NP RLY 18- 32 C 32 ACT-I 4PI THRESHOLD 59FU1 50SN116 G N ABX 9- 29 D 9- 29 BF3-I 4P I 117 69FU1 50SN1 16 G 2N ABX 17- 29 D 17- 29 BF3-I 4PI 118 69FU1 50SN1 16 G 3N ABX 27- 29 D 27- 29 BF3-I 4P I 119

ABY

ABY

EXCIT SOURCE DETECTOR

TYPE ANG NUM

0 7 NAI-D DST 7=6.988 MEV

D 6. 7 SCD-D UKN 6=6.736.7=7.368

C 32 NAI-D DST RATIO G,G/TO 2+ 6- 10 NAI-D 45

6 ACT-I 4P

I

22 THR-I DST

55, 85 TOF-D 67 NEUT ENGY SPEC

SCI-I DST

, 18 BF3-I 4PI

- 40 BF3-I 4P! THR-I DST EMU-D DST SCI-I DST EMU-D DST SPC, YLD REL TO P

C 90 ACT-I 4PI D300-900 TRK-I 4P

I

THRTHR- 90 900

121 123

REF

50RE1

63SU1 56aE3

6 7HU1

68 JUl 63YA2

63ME1

60GE3

61C02

57.25

42. 75

ANTIMONY 2=51

SEPARATION ENERGIES IMEV) G,N G,P G,T G,HE3 G.A G,2N G.NP &,2P

9.2 5.8 12.9 17.1 3.1 16.3 14.9 16.5 9.0 6.6 13.1 18.7 3.9 15.8 15.4 18.0

NUCLIDE REACTION RES EXCIT

Z A IN, OUT

51SB

51SB

51SB

51SB

61SB

51SB

51SB121

51SB121

51S6121

SOURCE DETECTOR

TYPE ANG NUM

G G ABX 7 D 7 NAI-D 90

G G ABX 4- 14 C 4- 14 NAl-D 120

G G RLX 5- 10 D 5- 10 NAI-D 135

G N ABX 10, 11 0 10. 11 BF3-I 4PI

G N NOX THR- 27 C 27 THR-I DST

G D RLY 10- 24 C 24SPC EMU-0 126 YLD REL TO P

G ,G

G ,N

G ,N

LFT 1

NOX THR

RLX 15,

1

CTHR

NAI-D OST

J-PI BF3-I 4PI THRESHOLD

D 15, 18 ACT-I 4PI REL TO CU63 SIGMA

ACT-I 4PI

32 ACT-I 4PI ACT-I 4PI ACT-I 4PI REL NEUTRONS

72SU4 50SN117 E P ABI 9- 20 D 16- 21 MAG-D 90 50ME2 50SN117 G G LFT 1 D 1 NAI-D 125 67GI 1 50SN117 G G LFT 7 D 6- 7 NA I -D DST 7=7.01 MEV 69BE7 60SN117 G G LFT 7 D 7 D DST 7.01 MEV

69FU1 50SN117 G N ABX 6- 31 D 5- 31 BF3-I 4P I 120 70W I 2 50SN1 17 G N ABX 7- 9 C 7- 9 TOF-D 130 69FU1 50SN117 G 2N ABX 16- 31 D 16- 31 BF3-I 4PI 121 69FU1 50SN117 G 3N ABX 24- 31 D 24- 31 BF3-I 4P I 122 + 680<3 50SN117 G P ABY THR- 20 C 20 ACT-I 4P I

69CU1 50SN118 E E/ FMF 1- 4 D 55, 60 MAG-D DST 69SH7 50SN118 E P ABY 15- 20 D 20 MAG-D DST 72SU4 50SN118 E P ABI 14- 20 D 16- 21 MAG-D 4P I 66HR1 SOSNl 18 G G LFT 1 0 1 NAI-D 90 1=1.22 MEV

69CE 1 50SN118 G G NOX 6- 8 D 6- 8 SCD-D DST 69FU1 50SN118 G N ABX 9- 30 D 9- 30 BF3-I 4P I 124 69FU1 50SN118 G 2N ABX 16- 30 D 16- 30 BF3-I 4P I 125 69FU1 50SN118 G 3N ABX 25- 30 D 25- 30 BF3-I 4PI 126 + 51HU1 50SN1 18 G P RLY 6- 24 C 24 ACT-I 4P I THRESHOLD

69FU1 50SN1 19 G ,N ABX 6- 31 D 6- 31 BF3-I 4P I 128 70W I 2 50SN1 19 G ,N ABX 7- 9 C 6- 9 TOF-0 130 69FU1 50SN1 19 G ,2N ABX 15- 31 D 15- 31 BF3-I 4P I 129 69FU1 50SN119 G 3N ABX 22- 31 D 22- 31 BF3- I 4PI 130 + 60ST1 50SN119 G .NP RLX 146- 320 C320 TEL-D 76

TELLURIUM Z=52

SEPARATION ENERGIES (MEV) G,N G, P G, T G.HE3 G.A G,2N G,NP G,2P

120 t .9 1-2) 10 . 3 7.2 15.7 13.9 0.3 17.9 16.8 12.3

122 2.46 9.8 8. 0 15. 8 15.2 1.1 17.0 17.3 13.8

12? 0.87 6.9 8 . 1 15. 7 13.0 1.5 16.7 14.9 14.5

124 4.61 °.4 8. 6 15. 9 16.2 1.8 16.4 17.5 15.2

125 5.99 6.6 8. 7 15. 7 14.0 2.2 16.0 15.2 15.8

126 13.71 °.l 1 15. 8 17.2 2.6 15.7 17.8 16.4

128 31 . 79 8.8 °. 6 15. 7 18.0 3.2 15.1 18.0 17,6

130 34.48 8.4 10.0 15. 6 18.8 3.8 14.5 19.0 18.5

NUCLIDE REACT I ON RES EXCIT SOURCE DET£ CTOR

REF 2 A I N OUT TYPE ANG NUM

60RE1 52TE G G ABX 7 0 7 NAI- D DST 64PA1 52TE G G LFT 1 D 1 NAI- D 90 66BE3 52TE G G RLX 5- 10 0 5- 10 NAI- D 135 60HA1 52TE G A SPC 8- 33 C 33 EMU- D DST

63SH5 52TE122

61AIC1 65AK1 52TE124

52TE124

G ,G G,G

LFT

LFT

68SC1 52TE124

REL TO H2 CROS SEC

NAI-D 105

NAI-D 100 1=.603 MEV NAI-0 105 1=603 KEV

67BA4 50SN12O E E/ FMF 1 > 2 D150 MAG-D DST 66ME1 52TE125 G LFT 1 D 1 SCD-0 OST 1.18,2.40 MEV 1=.463 MEV

69CU1 50SN120 E E/ FMF 1- 4 D 55, 60 MAG-D DST 60GE3 52TE125 G N NOX THR CTHR BF3-I 4P

I

69SH7 50SN120 E P ABY 15- 20 D 21 MAG-D DST THRESHOLD

72SU4 50SN120 E P ABI 15- 21 D 17- 22 MAG-D 4PI 66HR1 50SN120 G G LFT 1 0 1 NAI-D 90 60GE3 52TE126 G N NOX THR CTHR BF3-I 4PI 1=1.18 MEV THRESHOLD

69FU1 50SN120 G N ABX 9- 29 D 9- 29 6F3-I 4P I 132 69FU1 50SN120 G 2N ABX 15- 29 0 15- 29 8F3-I 4P I 133 60GE3 52TE128 G N NOX THR CTHR BF3-I 4PI 69FU1 50SN120 G 3N ABX 24- 29 D 24- 29 BF3-I 4PI 13 4+ THRESHOLD, ALSO 130

60K.U1 50SN120 G P ABX 16- 27 C 15- 27 ACT-I 4P I 60KU1 50SN12n G NP ABX 23- 27 C 23- 27 ACT-I 4P I 60GE3 52TE130 G N NOX THR CTHR BF3-I 4PI THRESHOLD, ALSO 128 72SU4 50SN122 E P ABI 15- 21 D 1 7- 22 MAG-D 125

67BA4 50SN124 E E/ FMF 1 , 2 D150 MAG-D OST 1.13,2.59 MEV

69CU1 50SN124 E E/ FMF 1- 4 D 55, 60 MAG-D DST 59SH7 50SN124 E P ABY 16- 22 0 22 MAG-D 90 72SU4 50SN124 E P ABI 16- 22 D 19- 24 MAG-0 90 61KU1 50SN124 G N ABX 8- 20 C 8- 20 ACT-I 4PI 69FU1 50SN124 G N ABX 8- 31 D 8- 31 BF3-I 4P I 136 69FU1 50SN124 6 2N ABX 14- 31 D 14- 31 BF3-I 4P I 137 69FU1 50SN124 G 3N ABX 23- 31 D 23- 31 BF3-I 4P I 138 + 71S01 50SN124 G XP ABX 14- 29 C 12- 29 SCO-D 4P 1

12
IODINE 2=53 CESIUM Z=55

SEPARATION ENERGIES IMEV] A ABUND. SEPARATION ENERGIES C^EVl G,N G.P G.T G.HE3 G.A G.2N G.NP G,2P G.N G.P G.T G.HE3 G.A G,2N G»NP G.2P

9.1 5.2 13.* 16.3 2.2 16.2 15.3 15.3 133 loO.OO 9.0 6.1 13.2 16.1 2.0 16.2 15.0 15.2

NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF 2 A I N OUT TYPE ANG

56FU1 53 1 127 G G ABX itO C 4- 40 NAl-D 120 60RE1 531 127 G G ABX 7 D 7 NAI-D 90 55FR1 531 127 G G LFT 1 D 1 SCD-0 140 1=.203 MEV 59LA1 531 127 G G LFT 1 D 1 NAl-D 130

1 = 375 KEV 56ER1 531 127 G N ABX 15 . 18 D 1 5 . 18 ACT-I 4P I 57FE2 531 127 G N RLY 14- 30 C 14- 30 THR- 1 9U 58CH2 531 127 G N RLY THR CTHR BF3-I 4P 1 THRESHOLD

60GE3 53 1 127 G N NOX THR CTHR BF3-I 4P I THRESHOLD

60KU2 53 1 127 G N RLY 15- 90 C 90 TEL-1 DST 60RE1 531 127 G N ABX 7 D 7 NAI-I 90 61NA1 531 127 G N ABX 8- 22 C 10- 20 ACT-I 4P I 6 1 T A 1 531 127 G N NOX 12- 22 C 22 THR- I DST 66aR 1 531 127 G ,N ABX THR- 33 D 8- 33 BF3-I 4P I 57D I 1 53 1 127 G N ABX 300- 100 ClOO ACT- I 4P I 999= 1 GEV 67HU1 5 3 I 127 G N ABX 10. 1

1

0 10, 11 6F3-I 4P I 68J01 53 1 127 G N ABY THR- 300 C 50- 800 ACT-I 4P I 59BE6 531 127 G N ABX 9- 2 1 D 9- 31 MODI

4PI 690E 1 531 127 G N ABY THR- 999 C 1- 6 ACT- I 4P I 999=5.5 GEV 69VE2 531 127 G N ABX 9- 32 D 9- 32 MOD-1 4PI 71SA1 531 127 G N ABY 9- 68 C 10- 58 ACT-I 4P1 56ER1 531 127 G 2N ABX 15 , 18 0 15. 18 ACT- I 4P 1 51NA1 531 127 G 2N ABX 15- 22 C 10- 20 BF3-I 4P I ALSO ACT IVATION

66BR1 53 1 127 G 2N ABX THR- 33 D 8- 33 BF3-1 4P I 67D 1 1 531 127 G 2N ABX 300- 999 C999 ACT- I 4P I 999= 1 GEV

6eJ01 531 127 G 2N ABY THR- 800 C 50- 800 ACT-1 4P1 59BE5 531 127 G 2N ABX 16- 31 D 9- 31 MODI

4P1 59VE2 531 127 G 2N ABX 15- 32 D 16- 32 MOD- 1 4PI 670 I 1 531 127 G 3N ABX 300- 999 C999 ACT-I 4PI 999=1 GEV

68J01 531 127 (3 3N ABY THR- 800 C 50- 800 ACT-I 4P 1 69BE6 531 127 G 3N ABX 27- 31 D 9- 31 MOD- 1 4PI 69DE1 531 127 G 3N ABY THR- 999 C 2- 5 ACT-1 4P1 999=5.5 GEV

69VE2 531 127 G 3N ABX 25- 32 D 26- 32 MODI

4P 1 68J01 531 127 G UN ABY THR- 800 C 50- 800 ACT- I 4P 1 68J01 531 127 G 6N ABY THR- 800 C 50- 800 ACT-I 4PI 70J01 531 127 G 5N ABY THR- 900 C 75- 900 ACT-I 4PI 68J01 531 127 G 7N ABY THR- 800 C 60- 800 ACT- 1 4P 1 70 JOl 531 127 G 7N ABY THR- 900 C 75- 900 ACT- 1 4P I 70J01 531 127 G SN AOY THR- 900 c 75- 900 ACT-I 4PI

70 JOl 531 127 G 9N ABY THR- 900 c 75- 900 ACT-I 4P 1 56GA1 531 127 G XN ABX 9- 27 c 9- 27 BF3-I 4P I 58KU1 531 127 G XN ABX 7- 40 c 7- 40 BF3-I 4P I 58<A1 531 127 G XN ABX 9- 22 c 9- 22 BF3-1 4PI 61BA2 531 127 G XN ABY THR- 22 c 22 THR-I OST

68 J02 531 127 G XN ABX THR- 800 C150- 800 ACT-1 4P 1 58<E1 531 127 G P ABX 18 D 18 SC 1-0 0 SPECTRUM

59801 531 127 G P ABX 15. 18 D 15. 18 SC 1-D 4PI 50TA1 531 127 G p ABX 14- 32 C 14- 32 SC l-D 4P I SPC. CSI TARGET 61SE« 531 127 G p ABX 15. 18 D 15. 18 SC I-D 4PI

CSI TARGET. SPC THR-999 ClOO-999 ACT-I 4P

I

999=1 GEV

NUCL I OE REACT ION RES EXCIT SOURCE DETECTOR

REF I A I N OUT TYPE ANG NUM

58CH2 56CS133 G N RLY TriR CTHR BF3-I 4P1 THRESHOLD

50GE3 55CS133 G N NOX THR CTHR BF3-I 4PI THRESHOLD

57HU1 55CS133 G N ABX 10 . 1

1

D 10, 11 BF3-1 4PI 59BE1 55CS133 G N ABX THR- 30 0 9- 30 8F3-I 4P1 150 69BE1 55CS133 G 2N ABX THR- 30 0 16- 30 aF3-! 4PI 152 59BE1 55CS133 G .3N ABX THR- 30 0 26- 30 8F3-I 4P1 153 70<A3 55CS133 G 4N RLY THR- 250 C150- 250 ACT-I 4PI REL IG .N

)

70^A3 55CS1 33 G 5N RLY THR- 250 C150- 250 ACT-1 4PI REL (G.N

)

58^A1 55CS133 G XN ABX 9- 22 C 9- 22 SF3-! 4PI 58<E1 55CS133 G P ABX 18 D 18 SCI-0 0 SPECTRUM

59B01 55CS133 G P ABX 15. 18 D 15, 18 SCI-D 4P1 60TA1 55CS133 G P ABX 14- 32 C 14- 32 SCI-D 4PI SPC. CSI TARGET 61SE4 55CS1 33 G P ABX 15. 18 D 15. 18 SCI-D 4PI

70.<A3 55CS133

70KA3 55CS133

CSI TARGET, SPC

2P RLY ThR-250 C150-250 ACT-I 4P1 REL (G.N) 70KA3 55CS133 G.2PN RLY THR-250 C15O-250 ACT-1 4P1 RELIG.Nl

JN RLY THR-250 C160-250 ACT-I 4P

I

REL ( 5,N) . J=5 . 7,8 , 10

,

BARIUM Z=55

A ABUNO. SEPARATION E NERGIES (MEV 1 G,N G.P G.T 0.HE3 G.A 6.2N G.NP G,2P

130 0.10 10.2 7.0 15.0 13.9 0.6 18.2 16.7 12.0

132 9.71-21 9.8 7.7 15.3 14.7 1.0 17.3 17.0 13.1

134 2.42 9.5 8.2 15.9 15.5 1.5 16.7 17.1 14.3

135 5.59 7.0 3.3 15.5 13.5 1 .9 16.4 15.1 14.8

135 7.81 9.1 8.5 15.3 16.2 2.1 16. 1 17.4 15.4

137 11.32 6.9 8.7 15.8 14.5 2 . 5 15.0 15.4 15.8

133 71.65 B.6 9.0 15.6 16.7 2.6 15.5 17.3 15.4

REF

60RE1 63<A2

57FE1

71BE4 71BE4

61BA2 54AL5

59HA2

50GE3

680K,3

71SH3

71BL1

NUCLIDE REACTION RES

Z A IN, OUT

55BA 55BA

56BA

EXCIT SOURCE DETECTOR

TYPE ANG NUM

55BA

56BA 56BA

56BA

56BA

56BA137 G.N

568A137 G.P

G G ABX 7 D 7 NAI-D 90

G G/ RLY 1 C 5 ACT-I 4PI

G N RLY 17- 31 c 15- 31 THR-I DST SPECTRUM

G N ABX 9- 24 0 9- 24 MOOI

4P I 372

G 2N ABX 15- 24 0 15- 24 MOOI

4P I 373

G XN ADY THR- 22 c 22 THR- 1 DST

G XN NOX THR- 34 c 34 THR- I DST

G A SPC THR- 30 c 30 EMU-O DST

NOX THR

ABY THRCTHR20 C 20

BF3-I 4PI THRESHOLD

ACT-I 4PI

ABX 15- 22 D150 MAG-D 90 ISOBARIC ANALOGS

ABY 150-700 C15O-70O ACT-1 4PI SEE 58 NY 1 70BE8 55BA138 G N ABX 8- 28 D 3- 28 BF3- I 4P I 494 70BE8 56BA138 G 2N ABX 15- 28 0 15- 28 BF3- 1 4P I 426 XENON Z=54 70BE8 56BA1 33 G 3N ABX 25- 29 D 25- 29 BF3-I 4PI 459

A ABUND. SEPARATION ENERGIES (MEV) G.N G.P G.T G,HE3 G.A G.2N G.NP G.2P

124 J. 10 10.2 6.8 16.2 13.8 0.5 13.5 16.6 11.7

125 0.09 10. 1 7.5 15.2 14.9 1.3 17.9 17.2 13.2

123 1.92 9.6 3.2 15.9 15.8 1.8 IS. 8 17.3 14.4

129 25.44 6.9 8.2 15.7 13.6 2.1 16.5 15.1 15.0

130 4.08 9.3 8.7 15.8 16.5 2.2 15.2 17.5 15.5

131 21.18 6.6 3.8 15.5 14.4 2.5 15.9 15.3 15.0

132 25.39 3.9 9.1 15.7 17.2 2.7 15.5 17.8 15.5

134 10.44 3.5 9.5 15.6 17.9 3.2 15.0 17.8 17.5

136 8.87 8.0 9.9 15.5 18.5 3.7 14.4 17.8 18.4

REF

69H01

70<E2

NUCLIDE REACTION RES EXCIT

Z A IN. OUT

54XE

54XE130

SOURCE DETECTOR

TYPE ANG NUM

G.XP ABY THR- 33 C 24- 33 SCI-D 90

G.G ABX 1 D 1 SCD-D 45 LFT, .536 MEV LEVEL

70BE7 54XE131 G.G 1 0 0- J-PI ,

1 NAI-D DST

,637. .723 MEV

LANTHANUM Z=57

138

139

.9 ( -2

)

99.91

SEPARATION ENERGIES (MEV) G.N G.P G.T G.HE3 G.A G.2N G.NP G,2P

7.3 5.0 13.6 13.8 2.0 15.5 12.9 14.7 8.8 5.2 13.2 15.8 2.0 15.1 14.8 15.2

NUCLIDE REACTION RES

Z A IN. OUT DETECTOR

TYPE ANG NUM

71PI1 57LA139

69SH8 57LA139

55BE3 57LA139

69BE7

70MO2

7 0 MO 3

70SZ1

57LA1 39

57LA139

57LA139

57LA139

E.E/

E .P G.G

G.G

G.G

G.G

G.G

SPC

SPC 11- 22 0 30 4- 16 D 50, 65 MAG-D OST

RLX

LFT

ABX

LFT

LFT

MAG-D U<N

5- 10 D 5- 10 NAI-D 135

D

D

D

9 0

6 UKN-D OST 6.413 MEV

6 SCO-0 DST

5=5. 018, LFT

6 NAl-D DST

J-P I ,5.018,5.418

5- 9 SCD-D DST

5 LFVELS

43
REF NUCLIDE REACTION RES EXCIT SOURCE OETECTOR

Z A IN. OUT TYPE ANG NUM REF NUCLIOE REACTION RES EXCIT SOURCE DETECTOR

t A IN. OUT TYPE ANG NUM

5eCH2 67LA139 G'>N RLY THR CTHR BF3-I 4P I THRESHOLD

58SP 1 57LA 1 39 G \>N RLX 8- 18 C 8- 18 BF3-I 4P1 606E3 57LA 1 39 G 1>N NOX THR CTHR BF3-1 4P I THRESHOLD

61TA1 57LA1 39 G 'rN NOX 11- 22 (; 22 THR- I DS T 52M I 3 57LA1 39 G ',N ABX 10- 2 1 0 10- 2 1 BF 3- I 4P I 62RE 1 57LA 1 39 G 1»

N

NOX 11- 5 5 5 5 THR- I DST

6 7HU

1

57LA139 G 1

N

ABX 9- 1

1

D 9 - 1

1

BF 3- I 4P ! 68BE5 57LA1 39 G >N ABX THR- 30 D 7- 30 MOO- I 4P I 98 68 JU 1 57LA139 G \pN NOX THR- 27 C 27 THR- I DST 686E5 57LA139 G '1 2N ABX THR- 30 D 7- 30 MOD- I 4P I 99 58BE5 57LA139 G ..3N ABX THR- 30 D 7- 30 MOD- I 4PI 100 + 58FU1 57LA139 G .XN ABY 7- 40 C 7- 40 BF3- I 4P I 58KA1 57LA139 G 'pXN ABX 9- 22 C 9- 22 BF3-I 4P I 61BA2 67LA139 G..XN ABY THR- 22 C 22 THR- I DST 61M I 1 57LA139 G'.XN ABX 10- 22 D 10- 22 BF3-I 4P I 64R I 1 57LA139 G •.XN ABX 8- 30 C 8- 30 BF3-I 4P 1 72DE3 57LA139 G .XN ABX 9- 24 C 8- 24 BF3- I 4P I 559 72TH2 57LA139 G ,XN ABX 9- 17 C 8- 16 BF3-I 4P I 71BE4 57LA139 G .SN ABX 8- 18 D 8- 18 MODI

4P I 71ME1 57LA139 G .F ABY THR- 900 C300- 900 TRK-I 4P I

CERIUM Z=58

A ABUND. SEPARATION ENERGIES (MEVl

G .N G. P G , T G.HE3 G •A G.2N G.NP G, 2P 136 0.19 10.0 6. 9 15.7 13. 8 0 .4 17.9 15.5 12 . 1 138 0.25 9 .6 7. 5 15 .7 14. 6 1 .0 17.2 15.9 1 3 . 2 140 88.48 9 .2 8. 1 15.8 15.2 1 .6 15.7 15.9 14 .3 142 11.07 7 .2 8. 8 12 .3 14. 5 -1 .4 12.5 15.6 15 .8

NUCL I DE REACT ION RES EXC I T SOURCE DETECTOR

REF Z A I N .OUT TYPE ANG NUM

71P I 1 58CE EllE/ SPC 4- 18 D 50 . 55 MAG-D DST 54BE4 58CE G '.G LET 2 D 2 NAI-D 120 66BE3 58CE G I.G RLX 5- 10 D 5 - 10 NAI-D 135 62MI3 58CE G'.N ABX 10- 21 D 10 - 21 BF3-I 4P I 69BE6 58CE G .N ABX 8- 23 D 8 -30 MOOI

4PI 363 59BE6 58CE G'.2N ABX 12- 30 D 8 - 30 MODI

4P I 354 69BE6 58CE G .3N ABX 24- 30 D 8 - 30 MOD-I 4P I 58FU1 58CE G .XN ABY 7- 40 C 7 - 40 8F3-I 4P I 61BA2 58CE G .XN A6Y THR- 22 C 22 THR-I DST

6 IMI 1 58CE G ..XN ABX 8- 21 D 8 - 21 BF3-I 4P I 71BE4 58CE G'.SN ABX 9- 18 0 9 - 18 MOD-I 4P I 59HA2 58CE G .A SPC THR- 30 C 30 EMU-D DST

71HA2 58CE138 Gi.N RLY 10- 70 C ACT-I 4P I ISOMER RATIO

TOP I 1 58CE140 E ..E/ LFT 1- 4 D 50 50 MAG-D 141

5 LEVELS. J-PI 68SH4 58CE140 E ., p SPC 13- 30 D 30 MAG-D 90 ANALOG STATES

69SH8 58CE140 E i,P SPC 13- 22 D 20 . 22 MAG-D DST 71SH3 58CE140 E .P ABX 15- 22 D150 MAG-D 90 ISOBARIC ANALOGS

52CA1 58CE140 G .N NOX 5- 30 C 30 ACT-I 4P I ISOMERIC RATIO

62FU6 58CE140 G'.N RLY 5- 31 C 31 ACT- I 4P 1 680K2 58CE140 G ..N ABY THR- 20 C 20 ACT- I 4P I ISOMERIC YIELD

71HA2 58CE140 G . 3N RLY 26- 70 C 70 ACT- I 4P I ISOMER RATIO

60GE3 58CE142 G iN NOX THR CTHR BF3- I 4P I THRESHOLD

PRASEODYMIUM Z=59

A ABUND. SEPARATION ENERGIES (MEV) G.N G.P G.T G.HE3 G.A G,2N G.NP G.2P

141 100.00 9.4 5.2 13.4 14.4 1.2 17.3 14.4 13.4

NUCLI DE REACT I ON RES EXC I T SOURCE DETECTOR

REF Z A 1 N ,.OUT TYPE ANG

71P 1

1

59PR141 E .E/ SPC 4- 18 D 50, 65 MAG-D DST 69SH8 59PR141 E ,P SPC 10- 19 D 20 MAG-D DST 61B03 59PR141 G..MU-T ABX 11- 20 C 11- 20 ACT-I 4P I 71AH1 59PR141 G..MU-T ABX THR- 150 C 10-150 MGC-D 4P I 52BE2 59PR141 G :.G ABX 5- 9 0 5- NAI-D 135 54AR1 59PR141 G'.G ABX 6- 9 D 5- NAI-0 135 55BE3 59PR141 G .G RLX 5- 10 D 5- 10 NAI-D 135

6 8M01 59PR141 I G'.e NOX 7 D 7 NAI-D 90 POLARIMETER 7. 532 69M I 1 59PR141 G..G SPC 5- 8 D 6- 8 SCO-D DST 70MO2 59PR141 G..G ABX 85 D 8 SCD-D DST

8 = 7.632. LFT 71PA2 59PR141 G-.G LFT 5- 9 0 6-9 SCD-D OST

5 LEVELS

58CH2 59PR 1^1 G \1 N RLY T HR CTHR BF3-I 4P 1 THRESHOLD

5 9C A2 5 9PR 1 ^

1

G '»

N

ABX 10- 3 2 C 33 ACT- I 4P I 59C A3 5 9 p R 1 /+

1

G ABX 10- 32 C lU- 32 ACT- I 4P I 590 I 1 59PR 1^

1

G '(N RLY g- 30 c 30 ACT-I 4P I REL <:U53 (G.NI

59 FE 2 5 9 P R 141 G '»

N

ABX 9 — 30 c 30 ACT-I 4P I THRESHOLD

6 0 6E 3 5 9P R ]^ ]^ t N NOX THR CTHR ACT- I 4P I THRESHOLD

6 1 BO 1 5 9PR 1 4

1

G '• N ABX 9 — 29 C 10- 29 ACT-I 4P I 6 1 C02 5 9PR 1 4

1

G 1 5 * 1

8

D 15» 18 ACT-I 4P I 6 1 T A

1

5 9PR 141 , m NOX 12 — 2 2 C 22 THR- I DST

6 2DE 1 5 9 P R 14-1 Mn^2 0 D 21 ACT-I 4PI

5 9 p R 1 4

1

r

' C 55 THR- I DST

66 BR 1 5 9 P R 1 4 1 r N AHX T HR — -v\ D 8- 33 BF3-I 4P I 5 9 P R 141 r 'n ABX 65 CTHR- 70 ACT-I 4P I 1 14+

6 7C A

1

5 9 PR 1 4

1

r »

N

RLX 9_ 1 7 C 9- 1

7

ACT-I 4P I 5 9 P R 141 10* 1

1

6F3-I 4P I 6 8 C A 1 5 9 P R 141 G »

N

ABX C 9- 1

7

ACT-I 4PI

6 8 JU 1 5 9PR 1 4

1

G NOX T HR - 30 c 30- THR-I OST

7 CSU

1

5 9 P R 1 4 1 »

N

ABX 9 — 2 4 p 9 — 24 ACT-I 4P I 27 7

7 1 BE ^ 5 9PR 141 G N -J D 9- 1

7

MOD- I 4PI

7 2 0R2 5 9PR 1 4

1

G 1 N ABX 9- 20 c 9- 20 ACT-1 4P1 447

5 9CA2 59PR 141 G

'

» 2N ABX 18- 3 2 c 33 ACT- I 4P I THRESHOLD

59FE2 59PR 14

1

G ', 2N ABX 16- 30 c 30 ACT-I 4P 1 THRESHOLD

6 1 BO 1 5 9P R 1 4

1

\ 2N ABX 16 — 2 9 c 10- 29 ACT-I 4P I 66BR

1

5 9P R 141 G ', 2N Abx THR- 30 D 8- BF3-I 4P I 305

6 1 MO 1 5 qpp \ G •1 3 N AS I 2 7- 3 3 c 27- 33 ACT- I 4P I THRESHOLD

66BR 1 59PR 141 G \» 3N ABX THR- 30 D 8- 3 3 6F3-I 4P I 306 + 58KA1 59PR141 G '.XN ABX 10- 22 c 10- 22 BF3-I 4P I 60TH1 59PR141 G .XN ABX 9- 18 c 7- 18 BF3-I 4P I 6^R 1

1

5 9 P R I 4 1 G 1. XN ABX 9- 30 c 9- 30 BF3-I 4P I 70MC1 59PR141 G >.XN SPC 11- 28 c 28 TOF-D 98 72DE3 59PR141 G>.XN ABX 9- 22 c 9- 22 BF3- I 4P I 550

6 1 SH2 5 9PR 141 G \. P ABY 5- 34 c 23, 34 EMU-D OST

62GHit 59PR141 G>.P SPC 5- 34 c 23 , 34 EMU-D DST 69EJ1 59PR141 P 1.G ABX 15 0 9- 11 SCI-D OST

li'=14.95 MEV

NEODYMIUM Z = iso

A ABUND. SEPARATION ENERGIES (MEV)

G .N G .P G . T G.HE3 G. A G.2N G.NP G,2P

142 27. 11 9 .8 7 . 2 15 . 1 13. 9 0. 8 17.9 15.5 12.5

143 12.17 5 . 1 7 . 5 14 . 3 10.9 -0 . 5 15.9 13.4 13.1

144 23.85 7 . 8 8 .0 12 .7 13. 2 -1 . 9 13.9 15.3 13.8

145 8, 30 5 .8 8 .0 12.6 11. 8 -1. 5 13.5 13.7 14.4

146 17.22 7 .5 8 .5 12 .8 14. 2 -1.2 13.3 15.5 15.1

148 5.73 7 .3 9 .2 12 .7 16.2 -0. 6 12.6 15.9 16.2

150 5.62 7 .4 9 .5 13 .2 15.4 0 . 4 12.4 15.5 17.5

NUCL I DE REACTION RES EXCIT SOURCE DETECTOR

REF Z A I N .OUT TYPE ANG NUM

54AR1 60ND G .G ABX 7 D 7 NAI-D 135 55BE3 50ND G .G RLX 5- 10 D 5- 10 NAI-D 135 71BE4 50ND G . SN ABX 10- 18 D 9- 18 MOD-I 4PI 59HA2 60ND G .A SPC THR- 30 C 30 EMU-O DST 71ME1 6UND G .F ABY THR- 900 C300- 900 TRK-I 4PI

7 IMAl 50ND142 E .E/ FMF 1 . 2 D 50 MAG-D DST

1 =1.57. 2=2.09

71SH3 60ND142 E .P ABX 15- 22 0150 MAG-D 90 ISOBARIC ANALOGS

59CA3 50ND142 G .N ABX 10- 32 C 10- 32 ACT-I 4PI 5eOK2 60ND142 G'iN ABY THR- 20 C 20 ACT-1 4PI ISOMERIC YIELD

7 ICAl 60ND142 G .N ABX 10- 20 D 8- 20 MOD-I 4PI 391 71HA2 50ND142 GiiN RLY 10- 70 C 70 ACT-I 4PI ISOMER RATIO

71CA1 60ND142 G ..2N ABX 10- 20 D 8- 20 MOD-I 4PI 392 72HA3 60ND142 P ..G ABX 14- 24 0 6- 17 NAI-D DST

71CA1 60ND143 G iN ABX 9- 20 0 8- 20 MOD-I 4PI 394 71CA1 50ND143 G'.2N ABX 9- 20 D 8- 20 MOD-I 4PI 395

63BL2 60ND144 G ,iG ABX 2 D 2 UlCN-O U<N 63RI2 50ND144 Gi.G LFT 2 D 2 NAI-0 90

G--WDTH. SEP ISOTPS 59ME3 50ND144 Gi.G LFT 2 . 2 C 2 . 2 SCD-0 DST

B 1 EL > ,2.074, 2.186

71CA1 50ND144 G..N ABX 8- 20 D 8- 20 MOD-I 4PI 397 71CA1 50ND144 G 1.2N ABX 8- 20 D 8- 20 MOD-! 4PI 398 71HA2 50ND144 G., 3N RLY 24- 70 C 70 ACT-I 4PI ISOMER RATIO

60&E3 50ND145 G,.N NOX ThR CTHR BF3-I 4PI THRESHOLD

71CA1 5UND145 Gi.N ABX 10- 20 D 8- 20 MOD-I 4PI 4O0 71CA1 60ND145 G .i2N ABX 10- 20 D 8- 20 MOD-I 4PI 401
NUCLIDE REACTION RES

2 A IN. OUT

EXC I T SOURCE DETECTOR

TYPE ANG NUM EUROPIUM Z=53

SEPARATION ENERGIES (MEV] 71MA1 60ND146 E E/ FMF 0 D 41 MAG-D DST G.N G. P G ,T G.KE3 G . A G.2N G.NP G,2

0 = 0.45 151 47. 82 8.0 4. 9 10.3 12. 7 -2 . 0 14.4 12.9 13. 71CA1 bONDl'tb G N ABX 8- 20 D 8- 20 MOD- I 4PI 403 153 52.18 8.6 5. 9 11 . 3 14. 8 -0 . 3 14.9 14.2 14. 71CA1 60NDl't6 G 2N ABX 8- 20 D 8- 20 MOD-I 4P1 404 71VA2 60ND146 G XN ABX 7- 24 C 7- 24 BF3-I 4P1 NUCL I DE REACTION RES EXC IT SOURCE DETECTOR

71CA1 60N014e G N ABX 8- 20 D 8- 20 MOD-I 4PI 406 REF 2 A I N OUT TYPE ANG NOM

71CA1 eONDlftB G 2N ABX 8- 20 D 8- 20 MOD-I 4PI 407 69VA2 eONDlftS G XN ABX 8- 23 C 8- 23 BF3-I 4PI 208 67HU1 63EU G N A8X 9- 1 1 D 9- 11 BF3-I 4PI 69VA3 eONDlftS G XN ABX 8- 22 C 8- 22 BF3-I 4PI 238 SEE 69VA2 50GE3 63EU151 G N NOX THR CTHR BF3-I 4PI THRESHOLD

7 IMAl 60ND150 E E/ FMF 0 D 60 MAG-D DST 70SE1 63EU1 51 G XN ABX 8- 24 C 6- 24 8F3-I 4PI

0 = 0.13 70VA1 63EU151 G XN ABX 8- 22 C 8- 22 BF3-I 4PI 468 59CA3 60ND150 G N RLX 8- 32 C 8- 32 ACT-I 4PI 71VA2 63EU151 G XN ABX 7- 24 C 7- 24 BF3-I 4P1 71CA1 60ND150 G N ABX 10- 20 D 8- 20 MOD-I 4P1 409 71CA1 60N0150 G 2N ABX 10- 20 D 8- 20 MOD-I 4PI 410 66AT1 63EU153 G G LFT 1 D 1 SCD-O Uf;N 59VA2 60ND150 G XN ABX 8- 23 C 8- 23 BF3-1 4PI 209+ 1=97 <EV 69VA3 60ND1 50 G XN ABX 8- 22 C 8- 22 BF3-I 4PI 239+ 60GE3 63EU153 G .N NOX THR CTHR BF3-1 4PI SEE 69VA2 THRESHOLD

69BE8 63EU153 G N ABX 8- 29 D 8- 29 BF3-I 4PI 154+ INCLUDES NP 69BEe 63EU153 G 2N ABX 8- 29 D 8- 29 BF3-I 4PI 156 INCLUDES 2NP SAMARIUM Z = 62 69BE8 63EU153 G 3N ABX 8- 29 D 8- 29 8F3-I 4PI 157 70SE1 63EU153 G XN ABX 8- 24 C 8- 24 BF3-I 4PI 70VA1 63EU153 G XN ABX 8- 22 C 8- 22 SF3-I 4PI 489

A ABUND. SEPARATION ENERGIES (MEV ) 71VA2 63EU153 G XN ABX 8- 24 C 8- 24 BF3-I 4PI

66eE3

72AR1

55DE 1 56S I 1

59CA3

5901 1

65ME 1

7iyA2

60GE3

69VA2

72BE3

65ME1

67BE4

68TA2

69VA2

69VA3

62^03

69M01

G.T G.HE3 G.A G.2N G.NP G,2P

12.4

13.0

13.6

14.2 15.7 16.9

144 3.09 10 .6 6. 3 16.4 12.7 -0.1 19.0 16.2

147 14.97 6 . 4 7. 1 12 .9 10.5 -2.3 14.8 13.4

148 11.24 3 . 1 7. 5 13 . 0 12.8 -2.0 14.5 15.3

149 13.33 5 .9 7. 6 12.6 11.2 -1.9 14.0 13.5

150 7.44 8 .0 8. 3 13.0 13.8 -1.4 13.9 15.5

152 26.72 8 . 3 8. 7 13 . 7 15.3 -0.2 13.9 16.6 154 22.71 8 .0 9. 0 14.0 15.5 1.2 13.8 16.5

NUCL IDE REACT ION RES EXC I T SOURCE DETECT JR REF Z A IN OUT TYPE ANG

60RE1 62SM G G ABX 7 0 7 NAI- D 90 52BE2 52SM G G ABX 5- 9 D 5- NAI- D 135 64AR1 62SM G G ABX 9 0 9 NAI- D 135 69BE6 62SM G N ABX 7- 21 D 7- 27 MOD- I 4P I 69BE6 62SM G 2N ABX 13- 25 D 7- 27 MOD- I 4P I 69BE6 62SM G 3N ABX 23- 27 D 7- 27 MOD- I 4PI 58FU1 62SM G XN ABX 7- 40 (- 7- 40 BF3- I 4P I 59HA2 62SM G A SPC THR- 30 ( 30 EMU- D DST

693H8 52SM144 E p SPC 1 1- 20 D 20 MAG- 0 UlvN 71SH3 52SM144 E P ABX 15- 22 D150 MAG- D 90

62SM144

62SM144

62SM144 52SM144

62SM144 62SM144

62SM148

52SM146

62SM149

62SM150

62SM152

62SM152

62SM152

52SM152

62SM152

62SM152

59M01 62SM154

52SM1 54

62SM154

G

XN

N

XN

E/

G

G

G

XN

XN

RLX

LFT

ABX

ABX

ABX

RLY

10-

11-

ISOBARIC ANALOGS

D 5- 10 NAI-D 135

D 9 SCD-D 135 SEE 66BE3. 9=8.998

C 9- 23 ACT-! 4PI

C 22 ACT-I 4PI THRESHOLD

C 10- 32 ACT-I 4PI

C 22. 30 ACT-I 4PI REL CU53 (G.N)

LFT 1

ABX 8

NOX THR

ABX 8

ABX ABX

D 1 NAI-O DST 1=1.46 MEV

24 C 8- 24 BF3-I 4PI

CTHR 8F3-I 4P1 THRESHOLD

23 C 8- 23 BF3-I 4PI

1 D 50-105 MAG-D DST

.122. .367 MEV LEVELS

D 1 NAI-D 105 1=0.96 MEV

D ! NAI-O 120 1=0.963 MEV

D 1 NAl-D 90 1=0.963 MEV

23 C 8- 23 BF3-I 4PI 211

22 C 8- 22 BF3-I 4PI 24H

SEE 69VA2

ABX THR-999 D 60-999 TRK-I DST 999=1 GEV

59CA3 62SM164 G N ABX 8- 32 C 8- 32 59VA2 62SM154 G XN ABX 8- 23 C 8- 23 59VA3 62SM1 54 G XN ABX 8- 22 C 8- 22 212

RLX THR- 20 C 20

ABX THR-999 C

SEE 69VA2

ACT-I 4PI REL TO NEUTRONS

60-999 TRK-I DST 999=1 GEV

GADOLINIUM 2=64

SEPARATION ENERGIES (MEV) G.N G.P G.T G.HE3 G.A G.2N G.NP 6.2P

152 0.20 8.6 7.4 13.3 12.5 -2.2 15. 1 15.3 12.2

154 2.15 8.7 7.6 14.0 14.1 -0.9 15.1 16.2 13.5

155 14.73 6.4 7.6 14.2 12.2 -0.1 15.1 14. 1 14.1

156 20.47 8.5 8.0 14. 1 14.9 0.2 15.0 16.2 14.7

157 15.68 5.4 8.0 14.1 13.3 0.7 14.9 14.4 15.2

158 24.87 7.9 6.5 13.8 15.4 0.7 14. 3 16.0 15.9

160 21.90 7.5 9.3 13.4 1.0 13.4 16.0 *

NUCL I DE REACT ION RES EXCIT SOURCE DETECTOR

REF 2 A IN OUT TYPE ANG NUM

71ME1 64GD

70SE1

70VA1

71VA2

70SE1

70VA1 71VA2

500E1

55BA3

65ST1

70SE1 70VA1 71VA2

54G0152 64GD152

64G0152

64GD154

64GD1 54 54GD154

54GD155

64GD155

64GD1 55

64GD155

64G0156

54GD1 55

60GE3 54GD157

70VA1 71VA2

59CA3 59BE8

72DR5 59BEB

69BE8

72DR5

64GD158

54G0158

54GD160

64GD160

64GD160

64GD150

64GD160

64GD150

G.F

G.XN

G .XN

G .XN

G.XN

G .XN

G .XN

G.G

G.G

G.G

G.XN

G .XN G.XN

G.N

G .XN

G .XN

G.N

G.N

G.N G.2N

G.3N

G.XP

ABY THR-900 C300-900 TRK-I 4P

I

ABX

ABX

ABX

ABX ABX

ABX

LFT

LFT

LFT

ABX

ABX

ABX

ABX

ABX

ABX

A8X

ABX

ABX

3- 24 C 8- 24 BF3-I 4P

I

3- 22 C 8- 22 BF3-I 4PI 490

3- 24 C 8- 24 8F3-I 4P

I

3- 24 C 8- 24 BF3-I 4PI

3- 22 C 8- 22 BF3-I 4PI 491

3- 24 C 8- 24 6F3-I 4P

I

D 1 NAI-D 125 SEPARATED ISOTOPES

D 1 NAI-D UKN

60. 86.5 KEV

D 1 NAI-O UKN

1=60 KEV

24 C 22 C 24 C

22 C 24 C

3229

33

29

ABX 6- ABX 15- 29 D 33 C

8- 24 BF3-I 4PI

8- 22 BF3-I 4PI 492

8- 24 BF3-I 4PI

HR BF3-I 4PI THRESHOLD

8- 22 BF3-I 4PI 493

7- 24 BF3-I 4PI

8- 32 ACT-I 4PI

8- 29 BF3-I 4PI 156+ INCLUDES NP

6- 33 ACT-I 4PI 8- 29 BF3-I 4PI 160 INCLUDES 2NP

8- 29 BF3-I 4PI 161 14- 33 ACT-I 4PI XP=P+NP

45
TERBIUM Z = 65 NUCL I DE REACTION RES EXC I T SOURCE DETECTOR

REF Z A I N 1 OUT TYPE ANG NUM

A ABUND

.

SEPARATION ENERGIES (MEV)

G >N G < P G , T G.HE3 G.A G.2N G.NP G.2P 58FU1 67H0i65 G 1.XN ABX 7- 40 C 7- 40 BF3-I 4P1 156 5 . 2

( -2 ) 7 . 1 5. 5 12 . 1 11.8 -0.2 16.1 11.9 13.1 58KA1 67H0165 G 11 XN ABX 9- 22 C 9- 22 BF3-1 4P

I

159 99.95 8 . 1 6. I 11 .9 14.4 0.1 14.9 14.0 14.6 60TH1 67H0165 G ).XN ABX 8- 18 C 7- 18 ACT-I 4PI 62FU3 57H0165 G ). XN ABX 8- 24 C 8- 24 BF3-I 4PI QUADRUPOLE MOMENT

NUCL I DE REACTION RES EXC I T SOURCE DETECTOR 65AM1 67H0165 i G 11 XN ABY 10- 20 C 10- 20 BF3-I 4P

1

REF 2 A I N 'iOUT TYPE ANG NUM ORIENTED TARGET 69KE2 67H0165 i G

1

. XN ABX 10- 21 D 10- 21 8F3-I ^P

I

59ME 1 65TB 1 59 G '.6 LFT 1 D 1 NAI-D DST ORIENTED TARGET

MUL T I POLAR I T

Y

66SC1 67H0165 G 1

, p SPC THR- 70 C 70 TEL-0 DST

6'»LA1 65TB159 G '.G ABX 10- 25 C 30 NAI-D DST 66S C

1

67H0165 G !. D RLY THR- 70 C 70 TEL-D DST 66AT2 65TB159 G '.G LFT 1 D 1 SCD-D DST 66SC1 67H0165 G 1, J RLY THR- 70 C 70 TEL-D DST

1 = 58 t^EV 63BR1 67H0 16 5 G 11 NP ABX 13- 28 C 13- 28 BF3-I 4P

I

66RA1 65TB159 G 'pG LFT 1 D 1 NAI-D DST QUADRUPOLE MOMENT

1 = 363. 580 K.EV 7 1 ME 1 67H0165 G \, F ABY THR-900 C300-900 TRK-1 4P

I

5eCH2 65TB159 G ..N RLY THR CTHR BF3-I 4PI THRESHOLD

60GE3 65TB159 G > N NOX T H R CTHR BF3-I 4PI THRESHOLD

6 2B01 65TB159 G .N ABX 8- 21 CTHR- 21 6F3-I 4P

I

ERBIUM Z=68

6i*QRl 65TB159 G'.N ABX 8- 28 0 8- 28 BF3-I 4PI 68BE5 65TB159 G .N ABX THR- 30 D 7- 30 MOD-I 4PI 94 680K2 65TB159 G '.N ABY ThR- 20 C 20 ACT-I 4P

1

A ABUND

.

SEPARATION ENERGIES (MEV)

I SOMER I C YIELD G.N G

.

P G .T G.HE3 G.A G.2N G.NP G.2P 64BR1 65Tei59 G .2N ABX 14- 28 D 8- 28 BF3-I 4PI 162 0. 14 9.2 6. 4 13.8 12.1 -1.7 16.5 14.9 11.2 688E5 65TB159 G 1.2N ABX THR- 30 D 7- 30 MOD-I 4PI 95 164 1.56 8.9 6. 9 13.7 12.8 -1.3 15.8 15.3 12.3 6eBE5 65TB159 G .3N ABX THR- 30 D 7- 30 MOD-I 4PI 96 + 166 33.41 8.5 7 . 3 13 .5 13.5 -0.8 15.1 15.3 13.5

5 8 F U

1

6 5 T B 1 5 9 G '.XN ABY 7- 40 C 7- 40 BF3-I 4P I 167 2 2.94 6.4 7. 5 13 .3 12.3 -3.7 14.9 13.8 14.3 58FU2 65TB159 G ',XN ABX 8- 23 CTHR- 25 BF3-1 4P

1

168 27.07 7.8 8. 0 13 .0 14.3 -0.5 14.2 15.3 15.0 58KA1 65T6159 G '.XN ABX 9- 22 C 9- 22 BF3-I 4PI 170 14.88 7.3 8. 6 12 .7 • U.O 13.3 15.3 « 60TH1 65TB159 G ', XN ABX 8- 18 C 7- 18 BF3-1 4PI NUCL I DE REACTION RES EXC I T SOURCE DETECTOR

REF I A IN..OUT TYPE ANG NUM

DYSPROSIUM Z = 56 62FU3 68ER G .G ABX 8- 28 C 8- 28 NAI-D 90 TENSOR POLARIZABIL

63LA1 68ER G'.G ABX 9- 26 C 9- 27 NAI-0 DST

A ABUND. SEPARATION ENERGIES (MEV) 63KA2 68ER G'.G/ RLY 1 C 4 ACT-I 4PI

G .N G, P G , T G.HE3 G.A G,2N G.NP G.2P 64LA1 68ER G-.G ABX 10- 25 C 30 NAI-D DST

156 5.2(-2) 9 . 4 6. 6 14 . 1 12.3 -1.8 16.3 15.6 11.4 69BE6 68ER G .N ABX 7- 21 D 7- 28 MOD-I 4PI

15 8 9 9 . 1 6. 9 14 . 1 13.3 -0.9 16.0 15.5 12.4 59BE6 68ER G'.2N ABX 13- 27 D 7- 28 MOD-I 4PI 160 2.29 8 .6 7. 4 13.8 13.8 -0.5 15.4 15.6 13.5 69BE6 68ER G . 3N ABX 23- 28 D 7- 28 MOD-I 4PI

6 7. 5 13 12.3 -0.4 15.0 13.9 14.1 58FU1 68ER G .XN ABX 7- 40 C 7- 40 BF3-I 4PI

162 2 5.53 8 , 2 8. 0 13.6 14.5 -0.1 14.6 15.7 14.8 62FU3 68ER G .XN ABX 8- 24 C 8- 24 BF3-I 4PI

16 3 PR

* ?R

5 .3 8. 0 13 . 5 13.3 0.2 14.5 14.3 15.4 QUADRUPOLE MOMENT

1 64 8.18 7 .7 8. 5 13 .4 15.4 0.4 13.9 15.6 16.2 60GE3 68ER 167 G .N NOX THR CTHR BF3-I 4PI THRESHOLD

IN U L L 1 U c REACTION RES EXC I T SOURCE DETECTOR

REF Z A IN..OUT TYPE ANG NUM 63M I 3 68ER170 G .P NOX THR- 21 C 21 ACT-I 4PI

61BA2 66DY G..XN ABY THR- 22 C 22 THR-I DST

60GE3 66DY163 G .N NOX THR CTHR BF3-1 4PI THRESHOLD THULIUM Z=69

A ABUND. SEPARATION ENERGIES (MEV) G.N G. P G .T G.HE3 G.A G.2N G.NP G,2P

HOLMI UM Z = 67 159 100 .00 8. 1 5. 6 11 .3 13.1 -1.2 14.9 13.3 13.5

A ABUND. SEPARATION ENERGIES (MEV) N UC L I DE REACT I ON RES EXC I T SOURCE DETECTOR

G ,N • G, P G ,T G.HE3 G.A G,2N G.NP G , 2 P RE Z A I N .OUT TYPE ANG NUM

165 100.00 8 .0 6.2 11 .7 14. 1 -0.1 14.7 13.9 14.3 58CH2 69TM169 G .N RLY THR CTHR 6F3-I 4PI THRESHOLD

NUCL 1 DE REACT ION RES EXCI T SOURCE DETECTOR 60GE3 59TM169 G .N NOX THR CTHR BF3-I 4PI REF Z A I N ,.OUT TYPE ANG NUM THRESHOLD

58KA1 59TM169 G .XN ABX 8- 22 C 8- 22 BF3-I 4PI 62FU3 67H0165 Gi.G ABX 8- 28 C 8- 28 NAI-D 90 TENSOR POLARIZABIL

63LA1 67H0165 G,.G ABX 9- 26 C 9- 27 NAI-D DST 64LA1 67H0165 Gi.G ABX 10- 25 C 27 NAI-D DST 66AX1 67H0165 G 1.G ABX 13. 16 D 13, 16 NAI-D DST YTTERBIUM Z=70

63T I 1 67H0165 G ..G/ ABX 10- 19 D 10- 19 NAI-D 135 58CH2 67H0165 G ..N RLY THR CTHR BF3-I 4PI THRESHOLD A ABUND. SEPARATION ENERGIES (MEV) 60GE3 67H0165 G ..N NOX THR CTHR BF3-I 4PI G.N G. P G .T G.HE3 G.A G.2N G.NP G,2P THRESHOLD 168 0,14 9.1 6. 3 13 .6 12.0 -1 .9 16. 1 15.0 11.2 61WE1 67H0155 G .N ABX 8- 1 1 D 8- 11 ACT-I 4PI 1 70 3.03 8 . 5 6. 8 13 .2 12.4 -1.7 15.3 14.8 12.4 62RE1 67H0165 G'.N NOX 11- 55 C 55 THR-I DST 171 14.31 6.6 5. 8 13 .0 11.3 -1.6 15.1 13.4 13.0 63BR1 67H0165 G .N ABX 8- 28 C 8- 28 BF3-I 4PI 1 72 21.82 8.0 7. T 12 .9 13.3 -1.3 14.6 14.8 13.7 QUADRUPOLE MOMENT 173 16.13 6.4 7. 5 12 .7 12.4 -0.9 14.4 13.7 14.4 66AX 1 67H0165 G >N ABX 8- 20 D 8- 20 BF3-I 4PI 174 31.84 7 . 5 8. 0 12 .7 14.2 -0.7 13.8 14.9 15.0 67GE2 67H0165 G .N ABY THR- 27 C 22. 27 BF3-I 4P

I

1 76 12.73 6.9 8. 5 12 .2 15.0 -0.6 12.7 15.0 67HU1 67H0155 G .N ABX 9- 1

1

D 9- 11 BF3-I 4PI 68BE5 67H0165 G .N ABX THR- 30 D 7- 30 MOD-I 4PI 90 69BE8 67H0165 G-.N ABX 8- 29 D 8- 29 8F3-1 4PI 163 NUCL I DE REACT I ON RES EXC I T SOURCE DETECTOR

INCLUDES NP REF Z A i N .OUT TYPE ANG NUM 638R1 67H0165 G..2N ABX 14- 28 C 14- 28 BF3-I 4PI QUADRUPOLE MOMENT 58FU1 70YB G .XN ABY 7- 40 C 7- 40 BF3-I 4P1 66AX1 67H0165 G'.2N ABX 8- 20 D 8- 20 BF3-I 4P! 71ME1 70YB G .F ABY THR-900 C300-900 TRK-I 4P

I

67HA1 67H0165 G .2N RLX 14- 29 C 14- 29 ACT-I 4PI YIELD TO ISOMERE 60GE3 70YB173 G .N NOX THR CTHR BF3-I 4PI 68BE5 57H0165 G .2N ABX ThR- 30 D 7- 30 MOD-I 4PI 91 THRESHOLD

69BE8 67H0165 6 ,2N ABX 8- 29 D 8- 29 BF3-I 4P

I

164 INCLUDES 2NP 69M01 70YB174 E .F ABX THR-999 D 60-999 TRK-I DST 68BE5 67H0165 G . 3N ABX THR- 30 D 7- 30 MOD-I 4PI 92 + 999=1 GEV 69BE8 67H0165 G .3N ABX 8- 29 D 8- 29 BF3-I 4P

I

162 + 69M01 70YB174 G .F ABX THR-999 C 60-999 TR<-1 DST 999=1 GEV

46
175

176 97.41 2.59

G,N

7.7

6.3

LUTETIUM Z=71

SEPARATION ENERGIES (MEVI G.P G.T 6.HE3 G.A G.2N G.NP G,2P

5.5 10.9 12,7 -1.5 14,4 13,0 13.5 6.0 10,8 12,1 ^1.5 14.0 11.8 14.1

NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

NUCLIDE REACTION RES EXCIT

69BE6 71LU G N ABX 7- 24 D 7- 69BE6 71LU G 2N ABX 14- 28 D 7- 69BE6 71LU G 3N A3X 24- 28 D 7-

52DE2 71LU175

58KI1 71LU175

60GE3 71LU175

5e<Al 71LU175

G.G

G.N

G.N

G . XN

LET

ABX

NOX THR

ABX 8-

SOURCE DETECTOR

TYPE ANG NUM

28 MOD-I 4P

I

28 MOD-I 4PI

28 MOO- I 4PI

D 1 NAI-D DST J-PI. MULTIPOLARIT

23 C 8- 23 BF3-I 4P I THRESHOLD

BF3-I 4PI THRESHOLD

22 BF3-I 4PI

CTHR

22 C 8-

HAFNIUM Z=72

A ABUNO, SEPARATION ENERGIES (MEV 1 G.N G. P G.T G.HE3 G.A G.2N G.NP G.2P

174 0.18 8.5 6. 2 12.8 11,4 -2.5 15.6 14.4 11.1

1 76 5.20 8. 1 5, 7 12.7 12.0 -2.3 14.9 14.4 12.2

177 18.50 6.4 6, 3 12.3 10.9 -2.2 14. 5 13.1 12.8

178 27.14 7,6 7, 3 12,2 12.7 -2.1 14,0 14,4 13.5

179 13.75 6, 1 7, 5 12,0 11.9 -1,8 13,7 13,4 14. 1 180 35.24 7.4 8. 0 12,3 13,7 -1 , 3 13,5 15,0 14.9

NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN OUT TYPE ANG NUM

63KA2 72HF G G/ RLY 1 C 5 ACT-I 4PI 67MI1 72HF

67RA2

51 HA I

58T01

60GE3

70B04

53VE2

58T01

50GE3

72HF

72HF177

72HF1 77

72HF177

G.F

G.F

G.G

G.N

G.N

ABX 300-999 D30U-999 TR<-I DST 999=1600 MEV

ABX THR-260 C200-250 EMU-I 4P

I

LFT 0- 1 D

72HF179 G.G

72HF179 G.G/

72HF179 G.N

72HF179 G.N

60GE3 72HF18U

0- 1 NAI-0 110

113. 321 KEV

C 5- BF3-I 4PI THRESHOLD

CTHR BF3-I 4PI THRESHOLD

C 0- 2 ACT-I 4PI

6 LEVELS

D 1 ACT-I 4PI ISOMERS 1=1,33 MEV

C 6- BF3-I 4PI THRESHOLD

CTHR BF3-I 4PI THRESHOLD

CTHR BF3-I 4PI THRESHOLD

180

181 1,21-2) 99.99

G.N

5.5

7.5

TANTALUM Z=73

SEPARATION ENERGIES (MEV) G.P G.T G.HE3 G.A G.2N G.NP G.2P

5.7 10.9 11.4 -2,1 14,5 11.8 13.3

5.9 10,9 13,2 -1.5 14.2 13.3 13.9

NUCLIDE REACTION RES EXCIT

REF Z A I N OUT

71 MO 3 73TA181 E E/ ABX 59BA3 73TA181 E N ABY

65HE1 73TA181 E N RLY 59GR2 73TAiel E N RLY

50BA2 73TAI81 E 3N RLY

70BU2 73TA181 E XN SPC

69ANe 73TA181 E P RLY

70AN5 73TA181 E P RLY

69AN8 73TA181 E D RLY

69AN8 73TA181 E T RLY

65HE1 73TA181 E* N RLY 58B01 73TA181 E F ABI 58FU3 73TA181 G G ABX 61BU4 73TA181 G .G ABX 63LA1 73TA181 G .G NOX 63Y01 73TA181 G .G ABX 54LA1 73TA181 G .G ABX

URGE DETECTOR

TYPE ANG NUM

0-240 D500 MAG-D 60 THR- 36 D 10- 35 8F3-I 4P

I

THR- 32 D 14- 32 ACT-I 4P

I

THR-999 C 70-999 ACT-I 4P1 999=! GEV E-.N/E+.N

22- 42 D 22- 42 ACT-I 4P

I

REL TO G.3N

7-140 C140 TOF-D 165 THICK TARGET

THR-999 C999 MAG-D DST 999=1 GEV. REL D/T 86-999 C999 TEL-D DST 999=1140 MEV THR-999 C999 MAG-D DST 999=1.3 GEV THR-999 C999 MAG-D DST 999=1 GEV. REL 0/T THR- 32 D 14- 32 ACT-I 4PI D250.600 FMU-I 4P

I

5- 27 C 5- 27 NAI-D 120 10- 25 C 20 NAI-D DST

11- 22 C 27 NAI-D DST 6- 8 D 6- NAI-D 120 10- 25 C 32 NAI-0 OST

REF Z A IN .OUT TYPE ANG

57SH3 73TAiei G .G/ ABX 18 D 18 NAI-D 90 RAMAN SCATTERING

55J01 73TA181 G .N RLY THR- 55 C 65 SCI-D DST 55J01 73TA181 G .N RLY THR- 65 C 65 SCI-D DST 57CA1 73TA181 G .N RLX 8- 3 1 C 8- 31 ACT-I 4PI 57FE2 73TA181 G .N RLY 14- 30 C 14- 30 THR-I 90 5eBE2 73TA181 G .N SPC 8- 15 C 14. 15 TOF-0 120 58CA1 73TA181 G .N ABX 7- 32 C 7- 32 ACT-I 4PI THRESHOLD

58CH2 73TA181 G N RLY THR CTHR BF3-I 4PI THRESHOLD

58C01 73TA181 G >N SPC 9- 30 C 20. 30 EMU-D 90 THRESHOLD

58SP1 73TA181 G N ABX 8- 18 C 8- 18 BF3-I 4PI 59AU1 73TA181 G .N ABX 18- 55 c 18- 65 THR-I 4P

I

59CA3 73TA181 G .N ABX 8- 33 c 8- 33 ACT-I DST 59PA1 73TA131 G N ABX 8- 22 c 8- 22 BF3-I 4PI THRESHOLD

60BA2 73TA181 G .N RLX 8- 32 c 8- 32 ACT-I 4PI 60GE3 73TA181 G .N NOX THR CTHR ACT-I 4PI THRESHOLD

61WE1 73TA181 G .N ABX 7- 1 1 D 7- 11 ACT-I 4PI THRESHOLD

52B01 73TA181 G N ABX 9- 23 C 9- 23 BF3-I 4PI 52MI 3 73TA181 G N ABX 7- 22 D 7- 22 BF3-I 4PI 536R1 73TA181 G N ABX 8- 28 D 8- 28 BF3-I 4PI QUADRUPOLE MOMENT

53ZA1 73TAiel G N SPC 9- 19 C 14 . 19 EMU-D DST 64GR2 73TA181 G .N ABX THR- 11 DTHR- 1

1

BFS-I 4PI 67GE2 7 3 T A 1 8

1

N A By THR- 2 7 C 22, 27 BF3-I 4PI 67HU1 73TA181 .N ABX Q- \ \ 0 8- 11 BF3-I 4PI 58BE5 73TA181 G .N ABX THR- 30 D 7- 30 MOD-I 4PI 58XA1 73TA181 G N ABX 50- 85 C 55 . 85 TOF-D 67 NEUT ENGY SPEC

58VE1 73TA181 G N ABX THR- 35 D 7- 36 MOD-I 4PI 59TS1 73TA181 G N NOX 15- 26 C 26 SCI-D DST 57CA1 73TA181 G 2N RLX 14- 31 c 8- 31 MOD-I 4PI

MI XED WI TH G.3N

58CA1 73TA181 G 2N ABX 14- 32 c 7- 32 ACT-I 4PI THRESHOLD

63BR1 73TA181 G 2N ABX 13- 26 0 8- 28 BF3-I 4PI QUDRPL MOM. THRESH

68BE5 73TA181 G 2N ABX THR- 30 0 7- 30 MOD-I 4PI 58VE1 73TA181 6 2N ABX THR- 36 0 7- 35 MOD-I 4PI 57CA1 73TA181 G 3N RLX 14- 31 C 8- 31 MOD-I 4PI MIXED WITH G.2N

58CA1 73TA181 G 3N ABX 22- 32 C 7- 32 ACT-I 4PI THRESHOLD

60BA2 73TA181 G 3N RLX 22- 32 C 22- 32 ACT-I 4PI 68BE5 73TA181 G 3N ABX THR- 30 0 7- 30 MOD-I 4PI 58VE1 73TA181 6 3N ABX THR- 35 D 7- 36 MOD-I 4PI 68BE5 73TA181 G 4N ABX THR- 36 0 7- 36 MOD-I 4PI 68VE1 73TA181 G 4N ABX THR- 36 D 7- 36 MOD-I 4PI 56GA1 73TA181 G XN ABX 8- 27 C 8- 27 BF3-I 4PI 56HA1 73TA181 G XN ABX 15 . 18 D 15. 18 BF3-I 4PI 57CA1 73TA181 G XN RLX 8- 31 C 8- 31 MOD-I 4PI 58FU1 73TA181 G XN ABY 7- 40 c 7- 40 8F3-I 4PI 58FU2 73TA181 G XN ABX 8- 23 CTHR- 25 BF3-I 4PI 58KA1 73TA181 G XN ABX 9- 22 C 9- 22 BF3-I 4PI 51BA2 73TA1B1 G XN ABY THR- 22 C 22 THR-I DST 61BA2 73TA181 G XN ABY THR- 22 C 22 THR-I DST 61M I 1 73TA181 G XN ABX 8- 22 0 8- 22 BF3-I 4PI 54AL5 73TA181 G XN NOX THR- 34 C 34 THR-I DST 55FI2 73TA181 G XN SPC THR- 5C c 50 TOF-D 90 67AN2 73TA181 G XN ABX THR- 20 c 8- 20 BF3-I 4PI 69IS1 73TA181 G XN ABX 7- 30 c 7- 30 MOD-I 4PI 59SE2 73TA181 G P ABX 15. 18 0 15. 18 EMU-I 4PI 60BA5 73TA181 G P ABX 17- 39 c 17- 39 MAG-D DST SPECTRUM

60CA2 73TA181 G P ABX 15- 32 c 15- 32 ACT-I 4PI THRESHOLD

59AN5 73TA181 G P ABY 103- 999 C700 . 999 TEL-D DST 999=1.2 GEV

71AN1 73TA181 G P SPC 35- 999 C700 , 999 TEL-D DST

999 = 1.2 GEV . REL D/P 55T01 73TA181 G XP SPC 11- 23 C 23 EMU-D DST ABSOLUTE YIELD

50CH1 73TA181 G XP RLX 22- 90 C 90 TEL-I 90 REL TO DEUTERONS

69AN6 73TA181 G 0 ABY 109- 999 C700 . 999 TEL-D DST 999=1.2 GEV

71AN1 73TA181 G D SPC 43- 999 C700. 999 TEL-D DST

999 = 1.2 GEV . GEV D/P 50CH1 73TA181 G XD RLX 27- 90 C 90 TEL-I 90 REL TO PROTONS

71AN2 73TA181 G xo ABX 101- 999 C999 MAG-D DST

999 =1,14 GEV 60CH1 73TA181 G XT RLY 27- 90 C 90 TEL-I 90 REL TO DEUTERONS

57ER1 73TA181 G A ABI 1- 32 C 32 ACT-I 4PI 53BR1 73TA181 G NP ABX 14- 28 D 8- 28 BF3-I 4PI 71FU4 73TA181 G SPL RLY THR- 999 C999 ACT-I 4PI 999=5 GEV

72KA5 73TA181 G SPL RLY THR- 999 C600- 999 TRK-I DST 999=1,7 GEV

47
NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN, OUT TYPE ANG NUM OSMIUM Z-lb

57M I 1 73TA181 G .F ABX 300- 999 C300 -999 TRK.-I 999= 1600

DST MEV 67RA2 73TA181 G .F ABX THR- 260 C200 -260 EMU-I 4PI

7 IME 1 73TA181 G t,F ABY THR- 900 C300 -900 TRK-I 4P I 71VA4 73TA181 Gi.F ABX 100- 999 ClOO -999 TR(;-I 999= 5

4P I GEV

72>;A5 73TA181 G'iF RLY THR- 999 C600 -999 TR<-I 999=1.7DST GEV

72KR3 73TA181 G,,F ABY THR- 999 C350 -999 TRK-I 999= 1 DST GEV 72SK6 73TA181 G ,F LFT THR- 999 C999 TRK- I 999=1.45

DST GEV

A ABUND. SEPARATION ENERGIES IMEVl G.N G.P G.T G.HE3 G.A G.2N G.NP G,2P

184 0.02 8.9 5.7 12.7 10.9 -3.1 16.1 14.2 10.5

186 1.59 8.3 6.5 12.1 11.6 -2.8 14.9 14.3 11.9

187 1.64 6.3 6.6 12.1 10.4 -2.7 14.6 12.8 12.4

188 13.3 8.0 7.2 12.3 12.7 -2.1 14. 3 14.6 13.2

189 16.1 5.9 7.3 12.0 11.4 -2.0 13.9 13.1 13.7

190 26.4 7.8 8.0 12.4 13.7 -1.4 13.7 15.1 14.6

192 41.0 7.6 8.7 12.9 15.3 -0.4 13.3 15.7

NUCLIDE REACT ION RES EXCIT SOURCE DETECTOR

REF Z A IN..OUT TYPE ANG NUM

67MI1 760S G.F ABX 300-999 C300-999 TRK-I DST 999=1600 MEV

67RA2 760S G.F ABX THR-260 C200-260 EMU-I 4P

I

TUNGSTEN (WOLFRAMI Z=74

SEPARATION ENERGIES (MEV] G.N G.P G.T G.HE3 G.A G.2N G.NP G.2P IRIDIUM z=77

180 0.14 3.5 6.6 12.9 11.7 -2.5 15.4 14.5 11.8

182 26.41 8.1 7.1 12.8 12.7 -1.8 14.7 14.7 13.0

183 14.40 6.2 7.2 12.4 11.5 -1 . 7 14.2 13.3 13.5 A ABUND. SEPARATION ENERGIES (MEV) 184 30.64 7.4 7.7 12.2 13.2 -1.7 13.6 14.6 14.3 G.N Gi,P G.T G.HE3 G.A G.2N G.NP G.2P

186 28.41 7.2 8.4 12.2 14.2 -1.0 13.0 15.2 * 191 37.3 8.1 5,.3 10.5 12.6 -2.1 14.4 13.1 13.3

5.9 10.8 13.9 -1.0 14.0 13.5 14.6

NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN,.OUT TYPE ANG NUM NUCLI DE REACT ION RES EXCIT SOURCE DETECTOR

REF Z A IN .OUT TYPE ANG NUM 71MA2 74W E ,,F SPC THR- 999 D500 .999 TRK-I 4PI 999=1.3 GEV 63KA2 77 1 R G iG/ RLY 1 C 5 ACT-I 4P I 60RE1 7 4W G,iG ABX 7 D 7 NAI-D 90 66BE3 74W G 1>G RLX 5- 10 D 5 - 10 NAI-D 135 67SC1 77IR191 G .G LFT 0- 10 0 1 SCD-D 125 63KA2 7 4W G,.G/ RLY 1 C 5 ACT-I 4PI 539.588 <EV

56HA1 74W GiiXN ABX 15. 18 D 15 . 18 BF3-I 4PI 68DA1 77 I R191 S G ,iG NOX 1 D 1 NAI-D DST 61BA2 7 4W G.iXN ABY THR- 22 C 22 THR-1 DST MAG MOMENT. 129 ICEV 62SH4 74W G,,P SPC 7- 34 C 23 . 34 EMU-D DST 64LA4 77IR191 G iiG LFT 0- 1 D u NAI-D 125 ABSOLUTE YIELD 63VE2 771R191 G '.G/ ABX 0- 1 D 1 ACT-I 4P I 62SH6 7 4W G ,,P SPC 7- 34 C 23 . 34 EMU-D DST I SOMERS 1=1.33 MEV

63SH1 74W G ,,P ABX 15- 34 C 15 - 34 SCI-I DST MULT I POLAR I T I ES 67ME2 77IR193 G .G LFT 0- 1 0 0 1 SCD-D 105 64DE4 74W G iF ABX 300- 999 C300 -999 EMU-D 4PI 450. 557.559 KEV 999=1 GEV 70ME6 77IR193 G,iG LFT 0- 1 D 0 1 SCD-D 105 SEE 57ME2

66SH2 74W 183 G •.G LFT 1 D 1 NAI-D 4P

I

60GE3 77IR193 G .N NOX THR CTHR BF3-1 4PI

1 =46.48 KEV THRESHOLD

60GE3 74W 183 G .N NOX THR CTHR BF3-I 4PI THRESHOLD

62CA2 74W 184 G .P ABX 15- 32 C 32 ACT-I 4PI PLAT INUM Z = 78 71M02 74W 186 G .G/ LFT 6 D 6 . 8 SCD-D DST 6.418 MEV 60GE3 74W 186 G'>N NOX THR CTHR BF3-I 4PI A ABUND. SEPARATION ENERGIES (MEV) THRESHOLD G .N G. P G , T G.HE3 G .A G.2N G .NP G,2P 62CA2 74W 185 G .N ABX 9- 32 C 32 ACT-I 4PI 190 1.3(-2

1

8 .8 5. 1 12 .6 11.0 -3 .2 15.7 14.4 10.8 598E8 74W 186 6 .N ABX 8- 29 D 8 - 29 BF3-I 4PI 166 192 0.78 8 . 7 6. 9 12 .8 12.2 -2 .4 15. 1 15.0 12.2 INCLUDES NP 194 32.9 8 .4 7. 5 1

3

. 0 13.3 -1 . 6 14.6 15.3 13.5 69BE8 74W 186 G .2N ABX 8- 29 D 8 - 29 BF3-1 4PI 168 195 33.8 6 . 1 7. 6 12 . 9 11.9 -1 .2 14.5 13.6 14.0 INCLUDES 2NP 195 25.3 7 .9 8. 1 13 . 1 14.2 -J .8 14.0 15.5 14.8 69BE8 74W 186 G .3N ABX 8- 29 D 8 - 29 BF3-I 4PI 169 198 7.21 7 .6 8. 8 13.0 15.0 -0 . 1 13.4 15.8 » 62CA2 74W 186 G .P ABX 15- 32 C 32 ACT-I 4P1

NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

185

187

REF

57MI1

57RA2

67ME1

64LA3

64SH5

57LA2

60GE3

37.07 52.93

G.N

7.8

7.4

RHENIUM z=75

SEPARATION ENERGIES (MEV) G.P G.T G.HE3 G.A G.2N G.NP 6,2P

5.4 10.5 12.3 -2.2 14.1 12.8 13.1 6.0 10.5 13.5 -1.7 13.6 13.2 14.4

NUCLIDE REACTION RES EXCIT

Z A

75RE

75RE

75RE185

75RE187

75REie7

75RE187

75RE187

IN, OUT

G.F

G,F

G.G

G,G

G.G

G.G

G.N

SOURCE DETECTOR

TYPE ANG NUM

ABX 300-999 C300-999 TRK-I DST 999=1600 MEV

ABX THR-260 C200-260 EMU-1 4PI

LFT

LFT

LFT

LFT

1 D 0- 1 SCD-D DST 645.718.874 KEV

1 D

D

0-

1

1 D 0-

CTHR

1 NAI-D DST

5 LEVELS NAI-D 122 1=686 KEV

1 SCD-D 115

8 LEVELS

BF3-I 4PI THRESHOLD

REF Z A IN '.OUT TYPE ANG

66BE3 78PT &.G RLX 5- 10 D 5- 10 NAI-D 135 53KA2 78PT G .0/ RLY 1 C 5 ACT-I 4P I 64GL1 78PT G >N SPC 15 D 15 TOF-D 90 68JU1 78PT G .N NOX THR- 27 C 27 THR-I DST 62SH2 78PT G .P SPC 7- 34 C 23 . 34 EMU-D DST

52SH4

67M I 1

67RA2

63VE2

60GE3

60GE3

62CH1

78PT

78PT

78PT

78PT195

78PT195

G.P

G,N

ABSOLUTE YIELD

SPC 7- 34 C 23. 34 EMU-D DST ABSOLUTE YIELD

ABX 300-999 C300-999 TRK-I DST 999=1600 MEV

ABX THR-260 ClOU-250 EMU-I DST

ABX

NOX THR

78PT195 G.N NOX THR

78PT196 N.G NOX 8

1 D 1 ACT-I 4P I ISOMERS 1=1.33 MEV

CTHR BF3-I 4PI THRESHOLD

CTHR BF3-I 4PI THRESHOLD

D 0- NAI-D 90

REL TRANS PROBABIL

48
GOLD Z=79 NUCLIDE REACTION RES

Z A IN. OUT DETECTOR

TYPE ANG NUM

SEPARATION ENERGIES (MEV)

197 100.00 8.1 5. 3 1 . 4 13.

N 1 1 r 1 t n F REACT ION RES EXC I T REP Z A IN .OUT

60BA2 79AU197 E .N RL Y 14- 38

60BA2 79AU197 E .2N RLY 17- 38

58Z I 1 79AU197 G .MU-T ABX 9- 20 56FU1 79AU197 G .G ABX 4- 40 60RE1 79AU197 G .G ABX 7 620C1 79AU197 G .G ABX 11- 18 63LA1 79AU197 G .G ABX 9- 26

5'tLAl 79AU197 G .G ABX 10- 25 53KA2 79AU197 G .G/ RLY 1 63VE2 79AU197 G .G/ ABX 0- 1

57FE1 79AU 1 97 .N RLY 15- 3 1 58BE2 79AU197 G .N SPC 7- 16 58CA2 79AU197 (3 N SPC 10- 1

9

58CH2 79AU197 G N RLY THR

59 AU

1

79 AU 1 9 7 C3 N ABX 18- 65

60AS1 79AU197 G N SPC 6- 55

60 BA 2 7 9 AU 1 9 7 G N R LX 10- 20 60eA8 79AU197 G N ABX 14. 18 60GE3 79AU197 G N NOX THR

61NA1 79AU197 G N ABX 10- 22 51TA1 79AU197 G N NOX 12- 22 51WE1 79AU197 G N ABX 8- ID 62FU2 79AU197 G N ABX 8- 25

52MI3 79AU197 G N ABX 6- 22 62RE1 79AU197 G N NOX 1 1 - 55 63ZA1 79AU197 G N SPC 7- 19 67GE2 79AU197 G N ABY TriR- 27 57HU1 79AU197 G N ABX 9- 1

1

69DE1 79AU197 G N ABY T HR— 999

69DI 1 79AU197 G N ABY THR- 900 7QVE1 79AU197 N ABX g - 2 6

7 1 D I 1 7 9 AU 1 9 7 G N ABY 8- 999

7 1 L I 2 79 AU 1 9 7 G N ABY THR- 900

( V M U 1 ^ / G N 8- 68 60BA2 79AU 1 97 G 2N RLX 15- 26 61NA1 79AU197 2N ABX 15- 2 2 62FU2 79AU197 G 2N ABX 14- 2 5 70VE1 79AU197 (3 2 N ABX 14 — 2 7

7 1 D I 1 79 AU 1 9 7 G 2N ABY 15- 999

7 1 L I 2 79AU197 G 2N ABY THR- 900 70VE 1 79AU197 G 3N ABX 24- 27 71L 12 79AU197 G 3N ABY THR-900

7 1 L I 2 79AU197 G <.N ABY THR- 900

7 1 L I 2 79 AU 1 9 7 G 5N ABY THR- 90C

7 1 L I 2 7 9 A U 1 9 7 G 7N ABY THR- 900 71LI2 79AU197 G 9N ABY THR- 900 71LI2 79AU197 G 1 IN ABY THR- 900

71L 12 79AU197 G 1 3N ABY THR- 900 71LI2 79AU197 G 15N ABY THR- 900 55GA1 79AU197 G XN ABX 7- 27 56HA1 79AU197 G XN ABX 15. IS 58FU1 79AU197 G XN ABY 7- 40 58FU2 79AU197 G XN ABX 8- 23 5BKA1 79AU197 G XN ABX 8- 22 61MH 79AU197 G XN ABX 8- 20 59MA1 79AU197 G P RLY THR- 70

60BA5 79AU197 G P SPC 9- 40

60MA1 79AU197 p SPC 13- 2 ^

56DA2 79AU197 G XP SPC 1 1- 70

60CH1 79AU197 G XP RLX 21- 90

59MA1 79AU197 G D RLY THR- 70

60CH1 79AU197 G XD RLY 27- 90

60CH1 79AU197 G XT RLY 26- 90

65HA2 79AU197 G A SPC THR- 31 65ME2 79AU197 G A SPC THR- 35 62FU2 79AU197 G NP ABX 14- 25

HE3

6 G.A

-0.9 G.2N

14.8 G.NP13.7 G,2P

13.9 67MI1 79AU197

SOURCE DETECTOR

TYPE ANG NUM

D 14- 38 ACT-I 4PI REL TO G.N

D 17- 38 ACT-I 4PI REL TO G.2N

9- 30 MGP-D Ut^N 4- 40 NAI-D 120 NAI-D 90

18 NAI-D 135

32 NAI-D DST NAl-D DST ACT-I 4PI ACT-I 4PI ISOMERS 1=1.33 MEV

C 15- 31 THR-I DST

16 TOF-D 120 EMU-D 90 THRESHOLD

CTHR BF3-I 4PI THRESHOLD

C 18- 55 THR-I 4PI YLD REL TO CU53

14.

30

22

55 EMU-D 90 10- 38 ACT-I 4PI

14, 18 ACT-I 4PI HR BF3-I 4PI THRESHOLD

10- 22 ACT-I 4PI THR-I DST

6- 10 ACT-I 4PI

7- 25 BF3-I 4PI MIXED WITH G.NP

6- 22 BF3-I 4PI

5 THR-I DST

4. 19 EMU-D DST

2, 27 BF3-I 4PI 9- 11 BF3-I 4PI

1- 6 ACT-I 4PI 999=5.5 GEV C400-900 ACT-I 4PI

D 7- 35 BF3-I 4PI 334 C300-999 ACT-I 4PI 999= 1 GEV

C 75-900 ACT-I 4PI

C 10- 68 ACT-I 4PI

C 15- 38 ACT-I 4PI

C 10- 22 ACT-I 4PI

D 7- 25 BF3-I 4P

I

D 7- 26 BF3-I 4P I 335 C300-999 ACT-I 4PI 999= 1 GEV 75-900 ACT-I 4PI 7- 35 BF3-I 4PI 75-900 ACT-I 4PI 75-900 ACT-I 4PI 75-900 ACT-I 4PI 75-900 ACT-I 4PI

335 +

75-900 ACT-I 4PI 75-900 ACT-I 4PI 75- 900 ACT-I

76- 900 ACT-I

4P I 4P I 27 BF3-I 4PI 4P I 4P I 15. 18 BF3-I

7- 40 BF3-I CTHR- 25 BF3-I 4PI

C 8- 22 BF3-I 4PI

D 8- 20 BF3-I 4PI

C 70 EMU-D 90 IG.DI / (G.P

)

C 40 MAG-D DST ABS INTEG CROS SEC

C 23 EMU-D OST ABSOLUTE YIELD

C 70 EMU-D DST ABSOLUTE YIELD

C 90 TEL-I 90 REL TO DEUTERONS

C 70 EMU-D 90

( G.D) / (G .P

)

C 90 TEL-I 90 REL TO PROTONS

C 90 TEL-I 90 REL TO DEUTERONS

C 31 EMU-D DST

C 35 SCD-D 90

D 7- 25 BF3-I 4P

I

MIXED WITH G.N

67RA2

691^02 79AU19779AU197

71EM2 79AU197

71ME1 71VA4

72DA5

72KR3

79AU197

79AU197

79AU197

79AU197

G.F ABX 300-999 C300-999 TRI^-I 999=1600

G.F ABX THR-250 ClOO-260 EMUI

G.F SPC THR-999 C250-999 SCD-O 999=1000

G.F ABY THR-999 C300-999 TRI^-I 999=1000

G.F ABY THR-900 C30o-900 TR<-I G.F A6X 100-999 ClOO-999 TRK-I 999= 5 G.F ABY THR-999 C800-999 TRK-I 999=2.2

G.F ABY THR-999 C350-999 TRK-I 999= 1

MERCURY Z=80

SEPARATION ENERGIES (MEV)

OST MEV

DST DST MEV

4P I MEV

4PI 4P I GEV

DST GEV

DST GEV

G.N G.P G.T G.HE3 G.A G.2N G.NP G,2P

196 0.15 8.8 5.6 13.4 12.3 -2.0 15.8 15.0 11.7

198 10.02 8.3 7.1 13.4 13.1 -1.3 15.3 15.2 12.9

199 16. 84 5.6 7.2 13.3 11.8 -0.8 14.9 13.8 13.7 200 23.13 8.0 7.7 13.3 14.0 -0.7 14.7 15.3 14.2

201 13.22 6.2 7.6 13.0 12.7 -0.3 14.3 13.9 14.8 202 29.80 7.8 8.5 13.2 14.9 -n.i 14.0 15.4 15.3 204 6.85 7.5 9.2 13.5 15.1 0.5 13.5 15.2 »

REF

60RE1

52BE2

63FL1

53Y01

64AR1 55BE3

69RA1

63KA2

55MC1

55HA1 61BA2

71EM2

53FR2

52CA1

57KN1 69B03

63VE2

60GE3

580K3

59CA2

60GE3

52EU1

52CA2

55ME1 60GE3

NUCLIDE REACTION RES

2 A IN. OUT

80HG

80HG

80HG

80HG

80HG

80HG

80HG

BOHG 80HG

80HG 80HG

80HG198

80HG198

80HG199

80HG199 80HG199

80HG199

80HG199

80HG201

80HG201

80HG201

80HG201

80HG202

80HG202

G G ABX 7

G G ABX 5 G G LFT 2

G G ABX 6 G G ABX 5 G G RLX 5 G G NOX 5

G G/ RLY 1 G XN RLY THR

G XN ABX 15 G XN ABY THR

G F ABY THR

G G ABX 1

G N NOX THR

G G LFT 1 G G ABX 0 G 0/ ABX 0

G N NOX THR

G P ABY THR

G MU-T ABX 0

G N NOX THR

G N ABI 9

G P ABX 15

G G LFT 1 G N NOX THR

EXC I T

22

1822

5-2-

5-

55-

5

5 2215,

22

:E DETECTOR

TYPE ANG NUM

NAI-D DST G-WDTH

NAI-D 135 NAI-D 130 G-WIOTH NAI-D DST NAI-0 135

10 NAI-0 135 NAI-D DST 5=4.905 MEV

ACT-I 4PI NAI-I 90

18 BF3-I 4PI THR-I DST

999 TRK-I 4PI 999=1000 MEV

D 1 NAI-D OST LIFETIME. J-Pl

C 30 ACT-I 4P1 ISOMERIC RATIO

D 1 SCI-D 90

C 0- 2 ACT-I 4PI

D 1 ACT-I 4PI ISOMERS 1=1.33 MEV

CTHR BF3-I 4PI THRESHOLD

C 20 ACT-I 4PI

D 0 SCI-0 4PI 0=32.2 KEV. J-PI CTHR 8F3-I 4PI THRESHOLD

C 9- 23 ACT-I API RELATIVE YIELD

C 16- 32 ACT-I 4PI

D 1 CTHR

DST BF3-I API THRESHOLD

203

205

REF

29.5

70.5

G.N

7.7

7.5

THALLIUM Z=81

SEPARATION ENERGIES (MEVI G.P G.T G.HE3 G.A G,2N G.NP

5.7 11.2 13.4 -0.9 14.7 13.5 5.4 11.4 14.9 0.1 14.2 13.9

G,2P

14.2

15.6

NUCLIDE REACTION RES

Z A IN. OUT DETECTOR

TYPE ANG NUM

50RE1 81TL 66BE3 81TL

6eKAl 81TL

55GA1 81TL 65M02 81TL

71EM2 81TL

67MI1 81TL

G G ABX 7 D 7 NAI -D 90

G G RLX 5- 10 D 5- 10 NAI -0 135

G N ABX 50- 85 C 55. 85 TOF -D 67 NEUT ENGY SPEC G.XN ABX 7- 27 C 7- 27 BF3-I 4P

I

G.XN ABX 10-110 C 16-110 ACT-I 4P

I

G.F ABY THR-999 C300-999 TRK-I 4PI 999=1000 MEV

G.F ABX 300-999 C300-999 TRK-1 DST 999=1500 MEV

19
REF NUCLIDE REACTION RES

2 A IN. OUT EXCIT SOURCE DETECTOR

TYPE ANG NUM

61DE3 81TL203

57PA1 81TL203

70M01 81TL203

56HE2 81TL203

71SA1 81TL203

69AN10 81TL203

56HE2 81TL203

57ER1 81TL203

57ER1 81TL203

59H02 81TL205

69RA1 81TL205

70CE1 81TL205

70M02 81TL205

606E3 81TL205

69AN10 81TL205

57EI-2 81TL205

57ER1 81TL205

57ER1 81TL205

G.G

G.G

G.G

G.N

G.N G.XN

G .A

G .A

G.NA

G.G

G.G

G.G

G.G

G.N

G .XN

G .A G.A

G .NA

LET 1

LET 1

LET 6

RLY THR

ABY 7- ABX 7- RLY THRAB I 0-

ABI 11-

LFT 7

LET 8

SPC 8

ABX 8

NOX THR

ABX 7- ABX THRABX 18- ABX 29-

D 1 NAI-D DST

REL CROSS SECTION

0 1 NAI-D 1 10 1=279 KEV

D 6 SCD-D DST J=l/2. £=6.418 MEV

- 31 C 31

68

20

31

ACT-I 4PI REL CU63

C 10- 68 ACT-I 4PI

C 7- 30 BF3-I 4PI

C 31 ACT-I 4PI REL NEUTRONS

C 32 ACT-I 4PI

MI XED WITH G .NA

C 32 ACT-I 4PI

M 1 XED WITH G.A

0 7

SCD-D 145 8=7.646 MEV SCD-D DST

8=7. 646. LET BF3-I 4PI THRESHOLD

30 BF3-I 4PI 452 ACT-I 4PI

32 ACT-I 4PI 18- 32 ACT-I 4PI

ABUND. ( 1

)

LEAD Z=82

SEPARATION ENERGIES (.^lEV) G.N G.P G.T G.HE3 G.A G.2N G.NP G,2P

204 1.48 8.4 6.5 12.8 12.4 -2.0 15.2 14.4 12.3 206 23.6 8.1 7.3 13.0 13.4 -1.1 14.8 14.8 13.7

207 22.5 6.7 7.5 13.1 12.7 -0.4 14.8 14.0 14.7

208 52.3 7.4 8.0 12.9 14.4 -0.5 14.1 14.9 15.4

NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF I A I N OUT TYPE ANG NUM

59BA3 82PB E N ABY THR - 35 D 10- 36 BF3- 4P I 71V01

71MA2

558U1

55FU1 59C05

59PA3 60RE1

61MI1

51T01

52BE2 62FU4

53B02

63FL1

53Y01

54AR1

64GI 1

82PB

82PB

82PB 82PB

82PB

82PB 82Pa

82PB

82PB 82PB

82PB 82PB

82PB

82PB 82PB

82PB

E.N ABX THR-266 C150-266 TOF-D 90

E.F SPC THR-999 D500.999 TRK-I 4P I 999=1.3 GEV

65GI1 82PB

65DE1

55J01

55J01 58AS1

60GR1

61TA1 62BR4

62MI3 64AL4

64D01

64GL'l 67GE2

57HU2

58JU1

58KA1

82PB

82PB 82PB

82PB

82PB 82P8

82PB

82PB

82PB

82PB

82PB

82PB 82PB

82PB

82PB

69TS1 82PB

G G RLX 0- 3 C 3 NAI-D 90

G G ABX 4- 40 C 4- 40 NAI-D 120

G G ABX 6 . 7 D 6 . 7 NAI-D 30

G G ABX 17 D 15, 18 NAI-D 90

G G ABX 7 D 7 NAI-D DST G-WDTH

G G ABX 10- 22 D 10- 22 NAI-D DST

G G ABX 3- 16 C 3- 15 NAI-D 120

G G ABX 5- 9 D 5- NAI-D 135

G G ABX 4- 9 C 4- NAI-D 120

G G ABX 9 D 9 NAI-D DST

G G LET 2- 6 0 2- NAI-D 30 G-Wl DTH

G G ABX 5- 8 D 5- NAI-D DST

G G ABX 7 . 7 D 7 . NAI-D 135

G G NOX 7 . 8 D 7 . NAI-D 135 WIDTH

G G LFT 8 D 5- 8 NAI-D

i=7.28

135 MEV

G G RLX 12- 17 D 12- 17 NAI-D DST

G N RLY THR- 65 C 55 SCI-D DST

G N RLY THR- 55 C 55 SCI-D DST

G N NOX THR- 17 C 17 SCI-I DST

G N ABI 10- 21 C 10- 21 BF3- I 4P I G N NOX 10- 22 C 22 THR- I DST

G N SPC 8- 33 C 33 SCI-D 90

G N ABX 5- 22 D 6- 22 BF3- I 4PI

G N NOX THR- 18 C 18 SCI-I DST

G N ABX 8- 20 C 8- 20 BF3-I 4P I G N SPC 16 D 15 TOF-D 90

G N ABY THR- 27 C 22 . 27 BF3-I 4P I G N ABY THR- 22 C 22 THR-I DST

G N NOX THR- 22 C 22 THR-I DST

G N ABX 50- 85 C 55. 85 TOF-D 67 NEUT ENGY SPEC

G N NOX 14- 26 C 26 SCD-D DST

55BA5

55DI1

55MC1

56HA1

57T01

58FU1 51BA2

6 1BA2 51M I 1 54AL5

58MC1 68T01

69GA3

70KI2

NUCLIDE REACTION RES

Z A

82Pa

82PB

82PB 82PB

82PB

SOURCE DETECTOR

82PB

82P8

82PB

82PB

82PB 82PB

82PB

82PB 82PB

N OUT TYPE ANG

G XN ABY 30- 200 C150-250 THR- I DST

G XN SPC THR- 70 C 70 EMU-D DST

G XN RLY THR- 22 C 22 NA I - I 90

G XN ABX 1 5 » 18 D 1 5 * 18 BF 3- I 4P I G XN ABX 8- 22 C 8-22 BE 3- I 4P I SPECTRUM WITH EMUL

G XN RLX 7- 40 C 7- 40 BF3- I 4P I G XN ABY THR- 22 C 22 THR-I DST

G XN ABY THR- 22 C 22 THR- I DST

G XN ABX 8- 20 0 8- 20 BF3-I 4P I G XN NOX THR- 34 C 34 THR-I DST

G XN NOX THR- 32 C 22- 32 THR-I DST

G XN ABX 10- 24 C 10- 24 BF3-I 4P I

SCD-D DST 70MC1 82PB G XN SPC 8- 31 7=7.646 62SH2 82PB G P SPC 10- 34 NAI-D DST 62SH4 82PB 6 P SPC 9- 34 7.547 MEV 71AN1 82PB G P SPC 37-999

71AN1 82PB

67MI1 82P8

67RA2

71EM1

71ME1

72ICR3

71GR2

71GR2

66BE1

65Z I 2

58Z 1

1

50RE1

52FU4

63AX1 66BE3

71ME2

64HA2

57HU1

69B01

7 1BA2 54HA2 52FU4

69VE1

66Z 12

68Z I 1

71SH2 60GE3

63BE4

64HA2

65DE2

69B01

69B04

70801

71BA2 64HA2 62FU4

55DE1

52S01

60ST1

82PB

82P8

71EM2 82P8

82PB

82PB

82P8

82PB

82PB

82PB206

82PB206

82PB206

82PB206

82PB205

82PB206 82Pe206

60GE3 82PB205

82PB206

82PB206

82PB205

82PB206 82PB205

82PB205

82PB206

82PB207

82PB207

82PB207

82PB207

82P8207

82PB207

82P8207 82PB207

82P8207

82PB207

82PB207

e2PB207

82PB207 82PB207

82P3207

82PB207

MONTR CALIBRATION

SPC

SPC

85

18 CCH-D 13518 TOF-D DST THICK TARGETS TOF-0 98

34 EMU-D DST

34 EMU-D DST

PN

NN

N

N

N

N

N2N

XN

P

P

NP

SPC

ABX

ABY

ABY

ABY

ABY

ABY

SPC

RLX

FMF

ABX

ABX

ABX RLX

LFT

999=1.2 GEV, REL D/P 42-999 C700,999 TEL-D DST 999=1.2 GEV, REL D/P 300-999 C300-999 TRK-I DST 999=1600 MEV THR-260 ClOO-250 EMU- 1 DST THR-999 C30U-999 TRK-I 4P

I

999=1000 MEV THR-999 C300-999 TRK-I 4PI 999=1000 MEV THR-900 C300-900 TRK-I 4PI THR-999 C350-999 TSK-I DST 999= 1 GEV

150-550 C560 EMU-D DST PI-/PI+ YIELD RATIO

150-560 C560 EMU-0 DST PI-/PI+ YIELD RATIO

14 D 7 NAl-D U(CN

3 D 28- 70 MAG-D DST 8(EL) 3=2.5 MEV

2- 5 D 28- 73 MAG-D 100 B(EL) 3 LEVELS

6-

5-

2

D 7 G-WDTH

C 4-

D 6-

D

D

NAI-D DST RADIOLEAD

NAI-D 120 RADIOLEAD

NAI-D 135

10 NAI-D 135 SCD-D OST 1.704 MEV

BF3-I 4PI

2=1

THRESHOLD

G N ABX 6- 27 D 6- 25 BF3-I API

G N ABX 9- 1

1

D 9- 11 BF3-I API

G N SPC THR- 10 C 8- 10 TOF-D 135 G-WIDTh

G N ABX 8- 10 C 9 . 10 TOF-0 135

G 2N ABX 12- 27 D 12- 26 BF3-I 4PI

G XN ABX 8- 19 C 3- 19 BF3-I 4PI

G XN SPC THR- 33 C 33 TOF-D OST ENRICHED PB205

E E/ RLX 3 D 28- 70 MAG-D DST

ABX

NOX

SPC ABX

SPC SPC

ABX

ABX

ABX

ABX ABX

ABX

ABX

RLX

12- THR

7-6- thr- THRTHRTHR6- 12-

5-

11-

B(EL) 3=2.62.2.55

5 D 23- 73 MAG-D 100

5 LEVELS

14 D 19- 21 MAG-D 125 CTHR BF3-I API THRESHOLD

9 C 9 lOF-D U<N

27 D 6- 26 8F3-I 4PI

80 C 80 CCH-D 135

9 C 7- 9 TOF-D 135 G-WIDTH

8 C 9 TOF-D 135 25-350 <EV NEUTS

8 C 9 TOF-D 135 ERRATUM FOR 69B04

1027

19

21

-D 135

-I 4PI

15- ;

144-320 C320

7- 10 TOF12- 26 BF3-

6- 19 BF3-I 4PI 11- 21 ACT-I 4PI MIXED WITH PB208

15- 33 ACT-I API

173

MIXED WITH PB208 TEL-D 76 REL TO H2 CROS SEC

50
NUCL IDE REACT ION RES EXCI T SOURCE DETECTOR 81 SMUTH Z = 83 REF Z A I N OUT TYPE ANG NUM

A ABUND. SEPARAT ION ENERGIES { ME V ) 60 BA't 82PB2 08 ^ / SPC 0 - 2 3 D 4 3 MAG-D 160 G *N G» P G.T G.HE3 G. A G.2N G.NP

ABS INTLGR CROSSEC 209 100.00 7 .5 3. 8 9.4 10. 9 -3 . 1 14.4 11,2

0 ^ r D ^ U O E E / NOX 0~ 8 D183 MAG-D DST J-P I » TRANS RATE

C £ r D t U O E E / FMF 0 D 70 MAG-D 130 NUCL I DE REACT ION RES EXCIT SOURCE DETECTOR

66 Z 1 Z

Q -) D O 9 n fl 0 ^ r O ^ U 0 E E / RLX ^ 0 28- 70 MAG-D DST REF 2 A I N »0U T TYPE ANG

B (EL) 3=2.615 MEV

68Z I 1 8 2P 82 08 E / FMF 2 — 7 D 28- 73 MAG-D 100 6 1 CR 1 83B 1 2 09 » E / NOX Q — 5 C183 TEL-I DST

7 LEVELS J- P I » G-WDTH

70HE2 82PB208 E / 3 D248»502 MAG-D DST 6 3BA1 83B I 209 E » E / SPC 0- 2 3 D 42 MAG-D 180 3=2.6 MEV J-PI

7 1 MO 3 82PB2 08 E / ABX 0 — 240 D50U MAG-D 60 6 6 Z I 2 8 3 B I 2 09 E » E / RLX 2- 3 D 28- 70 MAG-D DST

7 1NA2 82PB208 E / LET 2- D183»248 MAG-D DST B ( EL ) 2.58. 2.73

6 LEVELS 6 8 Z I 1 ft ^ R I 7 nQ * FMF 2 D 28- 73 MAG-D 100 72F R5 82PB208 ABX 2 — D124,167 MAG-D DST B ( EL) 2.6 MEV

3 LEVELS TAB DATA 7 1 SH2 R ^ R T 7 riQ E p A8 X 10 — D 17- 21 MAG-D 125 69M01 82PB208 E F ABX THR- 999 0 6U-999 TRK-I DST 6 8BA2 838 I 209 ABX T H R — 099 D200- 999 TRK-I 4PI 999=1 GEV 999=1.5 GEV

68K.A3 82PB208 MU- T LET 7 D 7 NAI-D 4P

I

68B01 83B I 2 09 J p AB I T HR — 500 D250, 500 EMU- I 4PI 7=7.277 MEV 69M01 8 381209 , p ABX T HR- 999 D 60- 999 TRK-l DST

63 AX 1 82PB2 08 G G ABX 6- 8 D 6- NAI-D 135 999=1 GEV 63FL2 82PB208 LET 3 - g D 7 SCI-D 4PI 56FU1 8381209 G • G ABX 4 — 40 C 4- 40 NAI-D 120 G-WDTH 6 ORE 1 o Q R ! 9 n O G G ARX 7 D 7 NAI-D DST

6^ AR 1 g 2 PB208 ABX 7_ g 0 7- NAI-D 135

WI DTH 6 1 BU4 83B I 2 09 G ,G ABX 10- 2 5 C 22 NAI-D^B^¥

65''^Cl 82P B208 G G LF T 7 D 7 NAI-D DST 6 IM I 1 8381209 G »

G

ABX 10- 2 1 D 10- 21 NAI-D DST 7=7.28 MEV 61 TOl 8 3B I 2 09 G »G ABX 3- 1

6

C 3- 16 NAI-D 120

66 BE 3 8 2 P B2 0 8 G RLX D 5- 10 NAI-D 135 62FU4 83B I 209 G G ABX 4- 9 C 4- NAI-D 120 7=7.28 MEV 6 3AX1 838 I 209 G »

G

ABX 5- 8 D 5- NAI-D 135

66 ft ? D R ? n R G G LET D 7 NAI-D DST 635U1 838 I 209 G »G ABX 4

— 14 C 4- 14 NAl-D 120 7=7.297 MEV 63 YOl 83BI 209 G »

G

ABX 6- 8 D 6- NAI-D DST

ftO ^? Pr RD ^7 nw RO LET D 7 NAI-D DST 64AR1 83B I 2 09 G »

G

ABX 7 D 7 NAI-D 135 ERRATUM FOR 66001 66BE3 838 I 209 G G RLX 5- 10 D 5- 10 NAI-D 135

6 7G I 1 62PB208 LET 7 D 6- 8 NAI-D DST 660E 1 838 I 209 G G RLX 12- 17 D 12- 17 NAI-D DST 7=7.28 MEV 67G I 1 8381209 G G LFT 7 D 6- 8 NAI-D DST

6 7S T 1 82Pb206 (3 G LF T 7 D 7 NAI-D 135 7=7.15 MEV 7=7.28 MEV 69BE7 838 I 209 G G LFT 7 D 7 D DST 68M0 1 82P B208 $ G NOX 7 D 7 NAI-D 90 7.15 MEV POLARIMETER 7.28 69CE 1 8 381209 G G NOX 6- 8 D 6- 8 SCD-D DST

6 9R A 1 8 2PB2 08 G LET g D 8 NAI-0 DST 69ME 2 8 38 1 2 09 G G LFT 2- 3 C 3 SCO-D 127 8=7.277 MEV 2 .563 . 2.581.2.598

70MO2 82PB208 ABX 7 D 7 SCD-D DST 69R Al 8 38 I 2 09 G G LFT 8 • 8 D 8 . 8 NAI-D OST 7=7.279 .LET 8.8 = 7. 416. 7.149

56PR 1 Q2PB208 N RL Y 7 — 2 2 C 22 NAI-I 90 72 JA 1 8 38 I 2 09 G G RLX 1 0 0 10 SCD-D 90 SEPARATED ISOTOPES RAT 10- RAMAN/ELASTIC

58F A 1 82PB208 N ABX 11- 1 8 C 10- 20 ACT-I 4PI 56FE 1 838 I 209 G N RLX 7- 20 c 7- 30 THR-D DST

I SOMERIC PRODUCT 57DE 1 8381209 G N RLY 10- 30 c lu- 30 ACT-I 4PI 60GE 3 82P82 08 i3 N NOX T HR CTHR BF3-I 4PI I SOMER THRESHOLD 57FE 1 8381209 G N RLY 10- 30 c 20, 30 THR-I DST

6 3BE'* 82PB2 08 N SPC 7- 1 0 C 9. 10 TOF-D 5 72 Al 83812 09 G N SPC 8- 19 c 19 EMU-D DST

6i*HA2 82PB208 G N AbX 6- 27 D 6- 26 BF3-I 4PI 176 REL YIELD

67HU1 82PB208 G N ABX 9- 1

1

0 9- 11 BF3-I 4PI 58BE2 8381209 G N SPC 8- 16 c 14* 16 TOF-0 120 69B01 82Pb208 G N SPC T hR- 1 0 C 7- 10 TOF-D 135 60EM1 8 3B I 2 09 G N SPC 8- 30 c 30 EMU-D DST G-W I DTH 60GE3 8381 209 G N NOX THR CTHR 8F3-I 4PI 69B04 82PB208 G N ABX T HR - 8 C 9 TOF-0 135 THRESHOLD

25-350 KEV NEUTS Q 1 R r 7 n Q G RLY 90 c 90 TEL-I OST

7 0 BO 1 82PB208 ABX T HR — 8 C 9 TOF-D 135 6 1 T Al 0

o -aJ oO I

1 c

5 noU V 6

w NOX 22 c 22 THR-I DST ERRATUM FOR 69B04 62 BO 5 O

Q -aJ> ROr

1 ^7 0U 07 w ABX 22 D 8- 22 NAI-I OST 70B02 82P8208 G N ABX 7- 9 C 10 TOF-D DST 6 2M I 3 83812 09 N ABX 22 D 8- 22 BF3-I 4PI SEVEN 1+ LEVELS 62RE 1 838 I 209 N NOX 1 1 — 55 C 55 THR-I OST 70VE1 82PB208 G N ABX 7- 3 1 D 7- 36 BF3-I 4PI 330 632A1 838 I 209 G SPC 8 - 19 C 14 . 19 EMU-D OST 71BA2 82PB208 G N ABX 7- 1 0 C 7- 10 TOF-D 135 64A L4 8 38 I 2 09 NOX THR — 18 C 18 SCI-I OST 72T01 82PB208 G N LFT 7- 9 C 9 TOF-D DST 64DE 1 8 38 1 2 09 ^ N NOX THR- 80 C 80 CCH-D 135 G-WIDTH* J-PI NEUTRONS POLARIZED

64HA2 ABX 12 — 2 7 D 12- 26 8F3-I 4PI 17 7 + 64GL 1

ft R I 7 no G N SPC 1

6

D 16 TOF-D 90

7 OV E 1 8 2 P 32 08 2N ABX 14 — 3

1

D 7- 36 BF3-I 4PI 331 64HA2 8 3 B I 209 G ABX 27 D 6- 26 8F3-I 4PI 70VE 1 82PB208 3 N ABX 2 3- 3 1 D 7- 36 BF3-I 4PI 332 66BE4 8 3B I 2 09 G N ABX

7~

C 1 1 TOF-D 135

70 VE 1 8 2 P B 2 08 AB X 30- 36 0 7- 36 BF3-I 4PI 333 6 60E 2 8 3 B I 209 G M SPC THR 80 CTHR- 80 CCH-O 135

6 2 F U4 82PB208 G XN ABX 7_ 1 9 C 7- 19 BF3-I 4PI 6 7HU 1 8 38 1209 G N ABX 11 D 9- 11 8F3-1 4P1 68G03 82P3208 XN ABX T HR — 2 2 CTHR- 22 BF3-I 4P

I

67KU 1 8 38 I 2 09

^

N SPC 12 — 16 D 12- 16 TOF-D 115 698E 9 82 P 02 08 ABX D 7- 19 MOD-I 4P

I

2 34 68K A 1 8 38 I 2 09 N ABX 5 0 — 85 C 55. 85 TOF-D 67

6 9 V I- 1 R 7 P R 7 nfi 'xN SPC T HR — C 33 TOF-D OST NEUT ENGY SPEC ENRICHED Py208 68LE 1 838 1209 G N SPC 7- 20 C 2U EMU-D OST

70 I S3 O t r D t V O G AB X ft C 7- 18 8F3-1 4PI 264 69TS1 8 38 I 209 G N NOX 15- 26 c 26 SCI-D DST

5 5 DE 1 8 2P B2 08 G ABX - 7 1 C 11- 21 ACT-I 4P1 64H A2 838 I 209 G 2N ABX 12- 27 D 12- 26 BF3-I 4P1 MIXED WITH Pa207 6 7WY 1 8 38 1 209 G 3N RL I THR- 137 C137 ACT-I 4PI

ftO 7 P R 7 n fl

<: r D £ U O G .P ABX 15 — 3 3 C 15- 33 ACT-I 4PI 6 7WY 1 9 3 812 09 G 4N RL 1 THR- 137 C137 ACT-I 4PI MIXED WITH P3207 6 7WY 1 8 38 I 209 G 5N RL I THR- 137 C137 ACT-I 4PI

7 1 DA 1 8 2PB2 08 * ABX 15 — c 12- 33 ACT-I 4PI 67WY 1 838 I 209 G 6N RL I THR- 137 C137 ACT-I 4PI INCLUDES (G.PN) 6 7W Y

1

833 I 209 G 7N RL I THR- 137 C137 ACT-I 4PI 55T01 82P B2 08 G » XP SPC 13- 2 3 c 23 EMU-D DST 67WY1 8381209 G 6N RL I THR- 137 C137 ACT-I 4PI SEPARATED ISOTUPES 67WY1 838 I 209 G 9N RL I THR- 137 C137 ACT-I 4PI 62SC I 82PB208 G D ABX 1 5- 33 C 15- 33 ACT-I 4PI 56GA 1 838 I 2 09 G XN ABX 7 — 27 C 7- 27 8F3-I 4PI ALSO G.NP»PB207G.P 56HA1 8381209 G XN ABX 1 5 » 18 D 1 5 , 18 BF3-I 4PI 62SC1 B2PB208 G fNP ABX 15- 33 C 15- 33 ACT-I 4PI 58KA1 83BI 209 G XN ABX 8- 22 C 6- 22 8F3-I 4PI ALSOfG.D) »PB207G,P 6 1BA2 8331209 G XN ABY 10- 22 C 22 THR-I DST 69M01 82PB208 G , F ABX T HR- 999 C 60-999 TRK.-I DST 6 1BA2 838 1 2 09 G XN ABY 12- 22 C 22 THR-I DST 999=1 GEV 6 IM 1

1

838 I 209 G XN A 8X 8- 22 D 8- 22 BF3-I 4PI

6 1 W A

1

8 3 8 I 2 09 G XN SPC 10- 22 C 22 EMU-D DST 72BE7 82PB2G9 N • G ABX 10- 1 9 D 6- 15 NAI-D 90 6 2FU4 838 1 2 09 G XN ABX 7- 10 C 7- 10 BF3-I 4PI 63AN3 838 I 209 G XN ABY 9- 85 C 85 EMU-O DST 64AL5 833 I 2 09 G XN NOX THR- 34 c 34 THR-I DST 67AN2 83312 09 G XN ABX THR- 20 c 8- 20 BF3-I 4PI 69VE1 83BI209 G XN SPC THR- 33 c 33 TOF-0 DST 69GA3 83BI209 G XN SPC 8- 85 c 85 CCH-D 135 69LA2 8381209 G XN SPC 29 c 29 EMU-D DST 72TH2 8381 209 G XN ABX 7- 20 c 6- 19 BF3-I 4PI 70CU1 8381209 G T ABY THR- 90 c 90 ACT-I 4PI

51
NUCLIDE REACTION RES

Z A IN. OUT EXCIT DETECTORTYPE ANG NUM NUCLIDE REACTION RESZ A IN, OUT EXCIT DETECTORTYPE ANG NUM

67WY1

67WY1

67WY1

67WY1

6 7WY1 61DE2

6'(DE4

67RA2

68WA1

69K02

69M01

70SC1

71EM1

7 1VA4

71SN2

66BE1

83BI209

83BI209

83BI209

83BI 209 83BI209 83BI209

83BI209

67MI1 83BI209

83BI209

83BI 209

83B I 209

83BI209

8381209

83BI 209

83BI209

83BI209

83BI210

G .4NP G.5NP

G>fcNP G.7NP

G .8NP G.F

G.F

G.F

G.F

G.F

G.F

G.F

G.F

G.F

G.F

P .G

N .G

RL I RL 1 RLI

RL I RLI ABX ABX

THRTHRTHRTHRTHR300-

300-

ABX ABX

SPC

ABX

RLY

ABY

ABX

ABX

137

137

137

137 137 999

999

ABX 300-999

THR30-

THRTHRTHRThR100-

13-

250

40

999

999

700 999

999

22

C137 ACT-1 'tPl C137 ACT-I 4PI C137 ACT-I 4PI C137 ACT-I 4PI C137 ACT-I 4PI C300-999 EMU- I 4P

I

C300-999 EMU-D 4P 999=1 GEV C300-999 TRK-1 DST 999=1600 MEV ClOO-260 EMU-I DST

C 30- 40 ACT-I 4PI FRAGMENT YIELDS C250-999 SCD-D DST 999=1000 MEV

C 60-999 TRK-I DST 999=1 GEV

C700 ACT-I 4PI C300-999 TRK-I 4P

I

999=1000 MEV ClOO-999 TRK-I 4P

I

999= 5 GEV

D 9- 18 NAI-D 90

D 7 NAI-D UKN

70AU1 90TH232 RLY THR- 17 C 14

70ME5

70RA1

71 I Gl 71MA3

7 1VA4

72BR8

72KH1

72MA1 62MI1

90TH232

90TH232

70SC1 90TH232

90TH232

90TH232

90TH232

71WA1 90TH232

90TH232

90TH232 90TH232

90TH232

2 34 235

238

A6UND.

5.5 ( -3 I 0.72 99.27

G.F

G.F

5.3

6.1

ABY ABX

THRTHR- 900 C200

9 C 5

17 ACT-I 4PI ISOMER YIELDS

900 TRK-I 4PI

10 TRK-D DST SEE 68RA1. 69KA1

G F RLY THR- 999 C300 -999 ACT-I 4P I 999=1100 MEV

G F ABX 5- 7 C 5 - 7 TRK-I DST

G F NOX 5- 9 D 5 - 9 EMU-I OST

G F ABX 100-999 ClOO -999 TRK-I 4P I 999= 5 GEV

G F ABX THR- 999 C20U -999 SCD-I DST 999=1150 MEV

G F RLY THR- 1

1

C 5 - 11 TRK-I 4PI

G F ABX TKR- 9 0 5 - 9 I ONI4PI

G F A6X 5- 9 0 5 - 9 lON-I 4P I N G ABX D ACT-1 4P I

URANIUM Z=92

SEPARATION ENERGIES (MEV) G.P G.T G.HE3 G.A G.2N G.NP

6.6 10.2 10.6 -4.9 12.6 13.1 5.7 10.0 9.5 -4.7 12.1 11.9 7.7 10.0 » -4.3 U.3 13.5

G.2P

11.9 12.4

RADIUM Z =

SEPARATION ENERGIES (MEV) G.N G.P G.T G.HE3 G.A G.2N G.NP

5.4 6.9 9.7 -4.9 11.3 13.4

NUCLIDE REACTION RES EXCIT

NUCLIDE REACTION RES

2 A IN. OUT DETECTOR

TYPE ANG NUM

6eZHl

71ZH1 88RA226 G.F 88RA226 G.F

RLY ThR- 25 C 9- 25 TRK-I DST ABX 9- 20 C 9- 20 TRK-I 4P

1

N/F EMISSION WIDTH

THORIUM Z=90

SEPARATION ENERGIES (MEV) G.T G.HE3 G.A

232 100.00 6.4 7. 3 10.2 12. 2 -4

NUCL I DE REACTION RES EXC I T sou

REF Z A IN OUT

59WA1 90TH G F RLX 0- 999 C200

60RE1 90TH232 G G ABX 7 0 7 64LA1 90TH232 G G ABX 10- 25 C 30 71HA1 90TH232 G G ABX 8- 9 D 8 72JA1 90TH232 G G RLX 10 D 10 RATIO

56GI1 90TH232 G N ABX 8- 16 C 8 72MA1 90TH232 G N ABX 5- 9 D 5 55BA4 90TH232 G XN ABY 12 C 19 55GA1 90TH232 G XN ABX 5- 27 C 5 57KA1 90TH232 G XN ABX 6- 23 c 6 61BA2 90TH232 G XN ABY THR- 22 C 22 72BR8 90TH232 G XN RLY THR- 1

1

c 5 55BA4 90TH232 G F ABY 12 c 19 55LA2 90TH232 G F RLY THR- 19 c 19

G.2N

11.6 G.NP

13.7 G,2P

13.7

56G I 1 90TH232 G F ABX 8- 20 C 8- 56K02 90TH232 G F ABX 8- 24 C 8- 56K03 90TH232 G F SPC THR- 18 C 18 57SC2 90TH232 G F RLY THR- 15 C 4- 58FA2 90TH232 G F NOX THR- 15 C 16 58KA2 90TH232 G F ABX 5- 18 C 5- 59BA4 90TH232 G F RLY THR- 20 C 6- 60PR2 90TH232 G F NOX 6 D 5 61B02 90TH232 G F SPC THR- 70 c 70 61DE2 90TH232 G F ABX 300- 999 C300-

520E3 90TH232 G F ABX 7 D 7 62HU1 90TH232 G F ABX 5. 7 D 6 . 62M03 90TH232 G F ABY THR- 20 C 12 . DEL 63BA3 90TH232 G F RLY 0- 12 C 12 53DE1 90TH232 G F ABX 5 D 6 53K01 90TH232 G F SPC THR- 90 C 90 65AL1 90TH232 G F RLX 2- 7 D 5- 55CA3 90TH232 G F ABY 300- 100 C 1 55SA1 90TH232 G F SPC THR- 8 C 8 55S01 90TH232 G F RLX 5 . 7 D 5. 56N I 1 90TH232 G F RLY THR- 15 C 10-

DETECTOR

TYPE ANG NUM

999=1.2 GEV

NAI-D DST NAl-D DST

9 SCO-D 140 SCD-D 90 iAMAN/ELASTIC

20 ACT-I 4PI

9 BF3-I 4PI BF3-I 4PI

27 BF3-I 4PI

23 BF3-I 4PI THR-I DST

11 BF3-I 4PI

I ON- I 4PI BF3-I 4P

I

DELAYED NEUT

20 ACT-I 4PI

24 lON-I lON-D 4P

I

16 ACT-I 4PI EMU-I DST

18 lON-I DST

20 lON-I BF3-I EMU-D

)99 EMU-I EMU- I lON20 BF3-

DST

4P I

DST

-I 4P1

-I 4PI

68RA1 90TH232 G F NOX THR- 8 C 5- 69KA1 90TH232 G F ABX THR- 8 C 5- 69MA2 90TH232 G F ABX 5- 9 D 5-

EMU-I DST EMU-I DST lON-D DST

7 EMU-D DST EMU-I 4PI TOF-D DST

7 TRK-I DST

15 TRK-D 4PI DELAYED N YIELDS

8 TRK-I DST

8 TRK-I DST

9 EMU-I 4PI

REF Z A IN .OUT

7 1MA2 92U E .F SPC ThR71KI1 92U G ,XN SPC 5-

5 7KA

1

9 2U 233 G X N ABX 5- 58KA2 92U 233 G »F ABX 5- 59BA4 92U 233 G .F RLY THR52HU1 92U 233 G F ABX 5 . 70AU1 92U 233 G F RLY THR598A4 92U 234 G F RLY THR62HU1 92U 234 G F ABX 6 . 70AU1 92U 234 G F RLY THR64B03 92U 2 3 5 G .N ABX Q6 4 BO 3 92U 2 35 G 2 N ABX 3 - 64B03 92U 2 3 5 G TN ABX 8- 72BR8 92U 235 G XN RLY THR59BA4 92U 235 G F RLY THR52HU1 92U 235 G F ABX 5. 64B03 92U 235 G F ABX 6- 55K03 92U 235 G F RLY THR56N 1

1

92U 235 G F RLY ThR68PE2 92U 235 G F NOX THR59PE1 92U 235 G F SPC THR70KU2 92U 235 G F NOX 5-

70AU1 92U 235 G F RLY THR71VA4 92U 235 G F ABX 100-

72BR8 92U 235 G F RLY THR- 72KH1 92U 235 G F ABX THR59BA4 92U 236 G F RLY THR- 62HU1 92U 236 G F ABX 5. 70AU1 92U 236 G F RLY THR59BA3 92U 238 E N ABY ThR- 57RA3 92U 238 E F RLX THR58B01 92U 238 E F ABI THR- 69GR2 92U 238 E F RLY THR59M01 92U 238 E F ABX THR70KA1 92U 238 E F ABX THR55FU1 92U 238 G 0 ABX 4- 63B02 92U 238 G 6 A8X 9 71HA1 92U 238 G G ABX 8-

72 JAl 92U 238 G G RLX 10

56G I 1 92U 238 G N ABX 8- 51TA1 92U 238 G N NOX THR54GL1 92U 238 G N SPC 15 68KA1 92U 238 G N ABX 50-

69DE1 92U 238 G N ABY THR-<

71DI2 92U 238 G N ABY 7-

72MA1 92U 238 G N ABX 5- 72SC5 92U 238 G N ABY THRSOURCE DETECTOR

TYPE ANG NUM

999=1.3 GEV

6- 23 BF3-I 4PI 5- 18 lON-I DST

6- 20 lON-I DST

5. lON-I 4PI

14- 17 ACT-I API ISOMER YIELDS

21

2 1 21

1120

7 19

25

15

25

12

10

17

-999

1 19

6- 20 lON-I DST

5. lON-I 4PI 14- 17 ACT-I 4PI ISOMER YIELDS

8- 21 BF3-I 4PI 424

8- 21 BF3-! 4P I 442

8- 21 BF3-I 4PI 423

5- 11 BF3-I 4PI 6- 20 lON-I DST

5. lON-I 4PI 6- 19 lON-I 4PI 425

10- 25 ACT-I 4P1 10- 15 TRK-0 4PI DELAYED N YIELDS

C 25 lON-D API

C 12 lON-D 4PI MASS. ENERGY SPC

C 8. 10 BF3-I API DELAYED NEUT YLDS

C 14- 17 ACT-I API ISOMER YIELDS

ClOO-999 TRK-I API 999= 5 GEV

C 5- 11 TRK-I 4P1

D 5- 9 lON-I 4PI

5- 20 lON-I DST

6. lON-I 4PI

4- 17 ACT-I API ISOMER YIELDS

36 D 10 -250 D 25 40 0250

-999 C 70 RLY E- -999 D 50

-500 C 25 40 CD

9 D

D RATIO

15 C 8 22 C 22

0 16 85 C 55

-999 C 1

-999 C300

10

9 D 5 -700 C150

- 35 6F3-I 4P1 -250 EMU-I 4PI .500 EMU-I DST -999 ACT-I API /E+. 999= 1 GE -999 TRK-I DST 999=1 -500 TRK-D

- 40 NAl-D

NAI-0

- 9 SCD-D

SCD-D RAMAN/ELASTIC

20 ACT-I API THR-I DST TOF-D 90

85 TOF-D 57 NEUT ENGY SPEC

- 5 ACT-I API 999=5.5 GEV

999 ACT-I 4PI 999= 1 GEV

- 9 8F3-I 4PI -700 ACT-D API

GEV

4PI

120 DST

90

DST

52
NUCLIDE REACTION RES EXCIT SOURCE DETECTOR

REF Z A IN .OUT TYPE ANG

55844 92U 238 G .XN ABY 12 C 19 BF3-I 4P I 56GA1 92U 238 G .XN ABX 5- 27 C 5- 27 BF3-I 4P I 57<A1 92U 238 G'.XN A8X 5- 23 C 6- 23 6F3-I 4P I 618A2 92U 238 G..XN ABY ThR- 22 C 22 THR- I OST 72eRe 92U 238 G .XN RLY THR- 1

1

C 5- 1

1

BF3-I 4P I 55BA4 92U 238 G • F ABY 12 C 19 I ONI

4P I 55<A1 92U 238 G .F ABX THR- 26 C 12- 26 ACT- I 4P I 55LA2 92U 238 G'iF RLY THR- 19 C 19 BF3-I 4P I DELAYED NEUT

56GI 1 92U 238 G<.F ABX 8- 20 C 8- 20 ACT-I 4P I 55t;02 92U 238 Gi,F ABX 8- 24 C 8- 24 I ONI

4P I 56IC03 92U 238 G,.F SPC THR- 18 C 18 lON-D 4P I 57BA4 92U 238 G ..F NOX THR- 27 C 9- 27 EMU-D OST 57SC2 92U 238 G..F RLY THR- 15 C 4- 16 ACT-I 4P I 58BA7 92U 238 G , F NOX THR- 27 C 6- 27 EMU- I DST 58KA2 92U 238 G ..F ABX 5- 18 C 5- 18 lON-I DST 59BA4 92U 238 G ,.F RLY THR- 20 c 6- 20 ION- I DST 50B01 92U 238 G <iF SPC THR- 70 c 70 lON-D 4P I 50F01 92U 238 G .,F NOX 5- 20 c 5- 20 EMU- I DST 60PR2 92U 238 G .,F NOX 7 D 7 BF3-I 4P I

60TA3

61DE1 61DE2

62B08

520E3

52hUl 62K04

92U 238 92U 238 92U 238 92U 238

92U 238

92U 238 92U 238

62M03 92U 238

G.F

G.F

G.F G.F

G.F

G.F

G.F

G.F

SPC NOX ABX

SPC

ABX

ABX

NOX

6

6- 300-

THR76, THRD 20 C

SOURCE F19(P.AG|

6 EMU-D DST

6- 20 EMU-I DST

ABY THR- 20 C

63B06 92U 23 8 G .r NOX THR- 35 C 35 53DE1 92U 238 Gi.F ABX 7 D 7 63PE2 92U 238 G..F RLY THR- 14 C 14 65AL1 92U 238 G',F RLX 5- 7 D 6' 65CA3 92U 238 G '.F ABY 300- 999 C999

65H01 92U 238 G .iF RLY THR- 33 C 33

65ri02 92U 238 G 1.F NOX 7 D 7

65K11 92U 238 G-,F ABY 6- 7 C 65MA3 92U 238 G .F ABX 5- 8 D 65NI1 92U 238 G .F RLY THR- 1 5 C 65S01 92U 238 G'.F RLX 6 . 7 D 65S02 92U 238 G .,F NOX TFR- 9 C 66B01 92U 238 G iiF NOX ThR- 9 C 66MA3 92U 238 G :.F ABX 5- 9 D 56ME2 92U 238 G iiF ABY 17 0

66NI1 92U 238 RLY THR- 15 C

999 C300-999 EMU-I 4PI

50 C 17- 50 lON-D 90

D 7 EMU-I DST

7 0 5. lON-I 4PI

36 C 35 lON-D DST MASS DISTRIBUTION

12. 20 BF3-1 4P! DELAYED N YIELDS

lON-D DST EMU-I OST ACT-I 4PI EMU-D DST EMU-I 4PI 999=1 GEV SCD-D 90 MASS SPC

SCI-I 4PI SOURCE F19(P.A6)

5- 7 ACT-I 4PI

5- 8 EMU-D 4P

I

10- 15 6F3-I 4P1

5. 7 TRK-I DST

5- 9 EMU-I DST

5- 9 TRK-i DST

5- 9 EMU-I DST

17 ACT-I 4PI SOURCE LI7(P.GI

10- 15 TRK-D 4PI DELAYED N YIELDS

66SA1 92U 238 G .F RLY THR- 650 C650 ACT-I 4P I 67KA1 92U 238 G .F RLY THR- 7 C 5- 7 ACT-I 4P I 67RA3 92U 238 G .F RLX THR- 260 C 25- 260 EMU-I 4PI 58KU1 92U 238 G'.F ABY THR- 7 C 4- 7 ACT-I 4P I 68RA1 92U 238 G .F NOX THR- 8 t 5- 8 TRK-I DST 69<A1 92U 238 G ,F ABX THR- 8 C 5- 8 TRK-I DST 69K02 92U 238 G ',F SPC ThR- 999 C250- 999 SCO-D 999=1000

DST MEV

69MA1 92U 238 G^.F ABX 5- 9 0 5- 9 EMU-I N-CAPTURE

OST G'S 69M01 92U 238 G !iF ABX THR- 999 C 60-999 TRK-1 999=1

DST GEV

69WA1 92U 238 G <.F RLX 0- 999 C200-999 SCD-D

999= 1 . 2 DST GEV

70AU1 92U 238 G,,F RLY THR- 17 C 14- 17 ACT-I 4P I

70K.A1 70KU2

70ME5

70RA1

92U 238 92U 238

92U 238 92U 238

70SC1 92U 238

71001

71 IGl 71PE1

92U 238 92U 238 92U 238

G.F

G.F

G.F G.F

G.F

G.F G.F

G.F

71TA1 92U 238 G.F

ISOMER YIELDS

500 C 26-600 TRK-D 4P

1

10 C 8. 10 BF3-I 4PI DELAYED NEUT YLDS

-900 C200-900 TRK-I 4P

I

9 C 5-10 TRK-D DST SEE 68RA1. 69KA1

RLY THR-999 C300-999 ACT-I 4PI 999=1100 MEV

9 0 6-9 TRK-I DST

8 C 6- 8 TRK-I OST

25 C 15. 25 MSP-I 4P

I

XE 131-136 YIELDS

LFT ThR- 53 C 53 SCD-I 90 DELAYED FISSION

ABY

NOX

ABY ABX

NOX

ABX

RLY

THR6-

THRTHR5-

5- THR71VA4 92U 238 G .F ABX 100- 999 ClOO- 999 TRK-I 999= 5

4P I GEV

71WA1 92U 238 G-.F ABX THR- 999 C200- 999 SCO-I 999=1150

DST 461 MEV

72AN2 92U 238 G-.F RLX 5- 8 D 5- 8 SCD-I 4PI 72BR8 92U 238 G',F RLY THR- 11 C 5- 11 TRK-I 4P I 72DA6 92U 238 G -,F ABY THR-999 CBOO- 999 TRK-I 999=2.2

DST GEV 72KH1 92U 238 G,.F ABX ThR- 9 D 6- 9 lON-I 4P I 72MA1 92U 238 G,,F ABX 5- 9 D 6- 9 lON-I 4PI 72SC6 92U 238 G.,F ABY THR- 700 C150- 700 ACT-O 4PI

G.N

6.6

NEPTUNIUM Z = 93

SEPARATION ENERGIES IMEV)

.P G.T G.HE3 G.A G.2N G.NP

.9 8.2 10.4 -5.0 12.3 11.4 G.2P12.0

REF NUCLIDE REACTION RES

Z A IN. OUT SOURCE DETECTOR

TYPE ANG NUM

58KA2 93NP237 G.F 598A4 93NP237 G.F 62HU1 93NP237 G.F

ABX 5- 18 C RLY THR- 20 C ABX 6. 7 D

5- 18 lON-I DST

5- 20 lON-I DST

6. I ON- I 4PI

PLUTONIUM Z = 94

SEPARATION ENERGIES (MEV)

238 239

240

242

REF

69KA1 71SH4

70RA1

G.N G.P G,, T G.hE3 G.A G.2N G.NP G.2P

7.0 6.0 9., 8 9.7 -6.6 12.9 12.6 10.9

5.7 6.2 9 ,,8 8.8 -5.2 12.7 11.6 11.4

6.6 6.6 9., 7 10.2 -5.3 12.2 12.7 11.8 6.3 5.9 9., 5 10.8 -6.0 11.5 12.9 12.6

NUCLIDE REACTION RES

Z A IN. OUT

94PU238

94PU238 94PU238

EXCIT DETECTOR

TYPE ANG NUM

G-.F ABX THR- 8 C 5- 8 TRK- I DST

G-.F ABX 7- 11 C 4- 12 SPK- I 2P I G iF ABX THR- 9 C 5- 10 TRK- D OST

SEE 68RA1 . 69KA1

57KA1 94PU239 G ,.XN ABX 5- 23 C 6- 72BR8 94PU239 GiiXN RLY ThR- 1 1 c 5- 58KA2 94PU239 G ',F ABX 5- 18 c 5- 59BA4 94PU239 G .F RLY THR- 20 c 6- 66N I 1 94PU239 G'.F RLY THR- 1 5 c 10-

66RA2 94PU239 G <iF NOX 5- 7 C 58RA1 94PU239 G .F NOX THR- 8 C 70S02 94PU239 G '.F ABX 5- 8 C 71SH4 94PU239 G',F ABX 7- 1

1

C 71TA1 94PU239 G'iF LFT THR- 53 C

59BA4 94PU240 G .F RLY THR- 20 C 68RA1 94PU240 G .F NOX THR- 8 c 59KA1 94PU240 G •,F ABX ThR- 8 c 70RA1 94PU240 G .,F ABX THR- 9 c

68RA1 94PU242 G'.F NOX THR- 8 c 69KA1 94PU242 G'.F ABX THR- 8 c

23 6F3-

11 BF3-

18 lON20 lON15 TRK- DELAYEO N Y 5- 8 UKN8 TRK8 TRK12 SPKSCO5.5-

53DELAYED FI 20 lON8 TRK8 TRK10 TRKSEE 68RA1.

I 4PI

I 4PI

I DST

I DST

D 4PI lELDS

I OST

I DST

D DST

I 4PI

I 90 SSION

I DST

I DST

I DST

D DST 69KA1

8 TRK-I DST

8 TRK-I DST

AMERICIUM Z = 95

SEPARATION ENERGIES (MEV) G.P G.T G.HE3 G.A 6.2N G.NP

4.5 8.2 9.5 -5.6 12.6 11.0 G,2P

11.0

REF NUCLIDE REACTION RESZ A IN. OUT

58KA2 95AM241 59BA4 95AM241

70GA1 95AM241

70GA1 96AM243

G.F

G.F G.NF

ABX 6- RLY THRTHR THRIT SOURCE DETECTOR

TYPE ANG NUM

18 C 5- 18 lON-I DST

20 C 6- 20 lON-I DST

14 C 10- 13 SPK-D 4PI PROMPT-DELAYED F

THR THR- 14 C 10- 13 SPK-D 4PI PROMPT-DELAYED F

FISSION PRODUCTS

53

5. Photonuclear Reaction Data Bibliography

1955-1972

55
BIBLI6GRAPHY

In the following bibliography Conference Proceedings are

indicated as follows;

PICNS-60

PICNS

PICNS

-61

-62

PICNS-64

PICNS-66

PICNS-67

PICNS-69

Proceedings of the International Conference on

Nuclear Structure, Kingston, Ontario 1960 (Bromley,

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57Erl P, Erdos, P, Scherrer, P. Stoll; Helva. Phys. Acta 30, 639

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57Gol

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57Hi 1 57Jol

57Kal

57Ki 1 57Knl

57Kol

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57Li 1 57Lol

57Wil

57Mi2

57Mul

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57Sp2

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58Bul N. A. Burgov, Yu , V, Terekhov; J. Nucl. Energy 7, 247

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58Cal J. B, Carver, W. Turchinetz; Proc, Phys, Soc . 71, 613

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58Ca2 S. Cavallaro, V. Emma, C. Mllone, A. Rubbino; Nuovo

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58Ch2 B. G. Chidley, L. Katz, S. Kowalski; Can. J. Phys. 36, 407

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58Col G. Cortini, C. Milone, A. Rubbino, Nuovo Cimento 9, 85

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58Co2 G. Cortini, C. Milone, R. Rinzivillo, C. Tribuno; Nuovo

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58Eml V. Emma, C. Milone, A. Rubbino; Nuovo Cimento 9, 343

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58Fal U. Farinelli, F. Ferrero, R. Malvano, S. Menardi, E. Silva;

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58Go2 A. N. Gorbunov, V. M. Spiridonov; Zhur. Eksp. i Teoret.

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58Go3 J. Goldemberg, L. Marquez; Nuclear Phys. 7, 202 (1958)

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58Mil C. Milone, S. Mi lone -Tambur ino , R. Rinzivillo, A.

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586x1 C. L. Oxley, Phys. Rev. 110, 733 (1958)

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58Yal I. P. Yavor, Zhur. Eksp. i Teoret. Fiz, 34, 1420 (1958);

Soviet Phys. JETP 7, 983 (1958)

58Zil B. Ziegler, Z. Physik 152, 566 (1958)

59Aul L. B. Aull, P. C. Reinhardt, W. D. Whitehead; Nuclear

Phys. 1 3, 292 ( 1 959 ) 59Bal W. C. Barber, F. E. Gudden ; Phys. Rev. Letters 3, 219

( 1959

)

59Ba2 E. B. Bazhanov, Zhur. Eksp. i Teoret. Fiz. 37, 374 (1959);

Soviet Phys. JETP 10, 267 (1960)

62
59Ba3 W. C. Barber, W. D. George; Phys. Rev. 116, 1551 (1959)

59Ba4 A. P. Baerg, R. M. Bartholomew, F. Brown, L. Katz, S. B.

Kowaiski; Can. J. Phys. 37, 1418 (1959)

59Bol M. Bormann, H, Neuert; Z. Naturforsch. 14a, 922 (1959)

59Brl P. Brlx, A. Kording, K. H. Lindenberger ; Z. Physik 154,

56 9 ( 1959 ) 59Br2 P. Brlx, E. K. Maschke; Z. Physik 155, 109 (1959)

59Bul N. A. Burgov, G. V, Danilyan, B. S. Dolbilkin, L. E,

Lazareva, F. A. Nlkolaev; Zhur . Eksp. 1 Teoret. Fiz. 37

1811 (1959); Soviet Phys. JETP 10, 1278 (1960)

59Cal J. H. Carver, G, A. Jones; Nuclear Phys. 11, 400 (1959)

59Ca2 J. H. Carver, W. Turchinetz; Proc. Phys. Soc. 73, 110

( 19 59

)

59Ca3 J. H, Carver, W, Turchinetz; Proc. Phys. Soc. 73, 69

( 19 59 ) 59Ca4 J. H. Carver, W. Turchinetz; Proc. Phys. Soc, 73, 585

( 19 59

)

59Chl V. P. Chizhov, L. A. Kul chitskii; Zhur. Eksp. i Teoret.

Fiz. 36, 345 (1959); Soviet Phys. JETP 9, 239 (1959)

59Col L, D. Cohen, W. E, Stephens; Phys. Rev, Letters 2, 263

( 1959 ) 59Co2 S, G, Cohen, P. S, Fischer, E, K, Warburton; Phys. Rev,

Letters 3, 433 ( 1959)

59Co3 G, Cortini, C, Milone, T, Papa, R, Rinzivillo; Nuovo

Cimento 14, 54 (1959)

59Co4 L. Cohen, R. A. Tobin; Nuclear Phys. 14, 243 (1959)

59Co5 L. Cohen, R. A. Tobin, J. McElhinney; Phys. Rev. 114,

590 ( 1959)

59Co6 S. G. Cohen; Nuovo Cimento 14, 931 ( 1959 ) 59Del N. N. Delyagin; J. Exptl. Theoret, Phys, USSR 37, 1177

(1959); Sov. Phys. JETP 37, 837 (1960)

59Dil G. Di Caporiacco, M. Mando, F. Ferrero; Nuovo Cimento

13, 522 ( 1959)

59Dul J. Dular, G, Kernel, M, Kregar, M. V, Mihailovic, G.

Pregl, M, Rosina, C, Zupancic; Nuclear Phys, 14, 131

( 1959 ) 59Dyl P. Dyal, J. P, Hummel; Phys, Rev. 115, 1264 (1959)

59Eml V. Emma, C. Milone, R. Rinzivillo; Nuovo Cimento 14,

1149 ( 1 959 ) 59Em2 V. Emma, C. Milone, R, Rinzivillo, A, Rubbino; Nuovo

Cimento 14, 62 (1959)

59Fal U, Farinelli, F. Ferrero, S, Ferroni, R, Malvano, E, Silva;

Nuovo Cimento 12, 89 (1959)

59Fel F, Ferrero, S, Ferroni, R. Malvano, S. Menardi, E. Silva;

Nuovo Cimento 11, 410 (1959)

59Fe2 F, Ferrero, R. Malvano, E. Silva, J. Goldemberg, G.

Moscati ; Nuclear Phys, 10, 423 (1959)

59Frl J, I, Friedman; Phys, Rev, 116, 1257 (1959)

59Gal E, L, Garwin; Phys. Rev, 114, 143 (1959)

59Gel D, S, Gemmell, A. H, Morton, E, W, Titterton; Nuclear

Phys. 10, 33 ( 1959

)

63
59Gi 1

59Gol

59Hal

59Ha2

59Ikl

59Ki 1 59Kol

59Ko2

59Kul

59Ku2

59Lal

59Lol

59Mal

59Mel

59Mil

59M12

59Mi3

59Mul

59Mu2

59Nal

59ec 1

59Pal

59Pa2

59Pa3

59Pel

59Pe2

59Pe3

59Pe4

59Pe5

59Fal

59Fol

59Eo2

59Eo3

59Sal

J. H, Gibbons, R» L. Macklin,

Schmitt; Phys, Rev. 114, 1319

H. E. Gove, A. E. Lltherland,

Letters 3, 177 (1959)

H. J, Hay, J. B, Warren; Can.

I. Havlicek; Nuovo Cimento

J. B. Marion,

( 1959 ) H. W.

R. Batchelor; Phys. Rev,

J. Phys. 37, 1153 (1959)

F. I. Havlicek; Nuovo Cimento 13, 969 (1959)

N. Ikeda, K. Yoshihara; Radioisotopes (Tokyo) 8, 24 (1959)

H. King, L. Katz; Can. J. Phys. 37, 1357 (1959)

J. Kockum, N. Starfelt; Nuclear Instruments 5, 37 ( 1959 ) P. Komar, T. N. Dragnev; Dokl. Akad . Nauk SSSR

(1959); Soviet Phys. Dokiady 4, 653 (1959)

A.

126, 1234

L. A. Kul chitskii, V. Presperin; Zhur . Eksp. i Teoret.

37 1524 ( 1959); Soviet Phys. JETP 10, 1082 ( 1960)

Chi-Ti Kuo, B. S. Ratner; Dokl. Akad. Nauk SSSR 125,

761 (1959); Soviet Phys. Doklady 4, 369 (1959)

de Nercy; J. Phys. Radium 20,

Fiz,

Soc. 73, 697 ( 1 959

)

M. Langevin, A. Bussiere

831 ( 1959); (See 61Bu4)

K. H. Lokan; Proc. Phys.

E. D. Makhnovskii; Zhur. Eksp. i Teoret. Fiz. 36, 739

(1959); Soviet Phys. JETP 9, 519 (1959)

F. R, Metzger, W. D. Todd; Nuclear Phys. 13, 177 (1959)

M. V. Mihailovic, G. Pregl, G. Kernel, M. Kregar; Phys.

Rev. 1 14, 1621 ( 1959

)

C. Milone; Phys. Rev. Letters 3, 43 (1959)

C. Milone, A. Rubbino. Nuovo Cimento 13, 1035 (1959)

N. Mutsuro, Y. 6hnuki, K. Sato, K. Kageyama, M,

Kimura; J. Phys. Soc. Japan 14, 1457 (1959)

N, Mutsuro, Y. Ghnuki, K. Sato, M. Kimura; J. Phys.

Soc. Japan 14, 1649 (1959)

T. Nakamura, K. Takamatsu, K. Fukunaga, M. Yata, S.

Yasumi ; J. Phys. Soc. Japan 14, 693 (1959)

J. 6 Connell, P. Dyal, J. Goldemberg; Phys. Rev. 116, 173

( 1959 ) R. \*. Parsons, L. Katz; Can. J. Phys. 37, 809 ( 1959)

Parsons; Can. J, Phys. 37, 1344 (1959)

Paul, U. Stierlin; Nuclear Phys. 13, 576 (1959)

S. Penfold, E. L. Garwin; Phys. Rev. 114,

S. Penfold, E. L. Garwin; Phys. Rev. 114,

L. Garwin; Phys. Rev. 115,

Leiss; Phys. Rev. 114, 1101

L, Garwin; Phys. Rev. 116,

R. Metzger, C.

R.

P.

A.

A.

A.

S.

A.

S. Penfold, E

Penner, J. E.

S. Penfold, E

E. Rasmussen, F . 95 ( 1959

)

V.

Phys. 13,

T. A. Romanowski, V. W,

( 1959)

J. P. Roalsvig, R.N.H.

Phys. 37, 607 (1959)

J. P. Roalsvig, R. N. H. Haslam, L. D.

Buschke; Can. J. Phys. 37, 722 (1959)

D. Sadeh; Compt . Rend. 249, 531 (1959)

1 139 ( 1959 ) 1324 ( 1959 ) 420 ( 1 959 )

( 1959 ) 120 ( 1959

)

P. Swann; Nuc lear

Voelker; Phys, Rev. 113, 886

Haslam, D. J. McKenzie; Can. J.

Skarsgard, E. E.

64
59Sa2 D. Sadeh; Compt. Rend. 249, 2313 (1959)

59Sel R. E, Segcl ; Phys. Rev. 113, 844 (1959)

59Se2 W. Sebaoun, H, Gauvin; Compt. Rend. 248, 791 (1959)

59Swl C. P. Swann, V. K. Rasmussen, F, R, Metzger; Phys.

Rev. 1 14, 862 ( 1959

)

59Tal N. W. Tanner, G, C. Thomas, W. E. Meyerhof; Nuovo

Cimento 14, 257 (1959)

59Thl H. H. Thies, B. M. Splcer, J.E.E. Baglin; Australian J.

Phys. 12, 21 ( 1959)

60Ail M. J. Aitken, N. Middlemas; Phys. Rev. 117, 1111 (1960)

60AL1 Ya. Alksnis, U. Ulmanis; Latv. PSR Zinat. Akad. Vestis 3

( 152 ), 71 ( 1960 ) eOAsl R. F. Askew, A. P. Batson; Nuclear Phys. 20, 408 (1960)

60Bal E. B. Bazhanov; Zhur , Eksp. i Teoret. Fiz. 38, 267 (I960);

Soviet Phys. JETP 11, 193 (1960)

60Ba2 W. C. Barber, T. Wiedling; Nuclear Phys. 18, 575 (1960)

60Ba3 E. B. Bazhanov, L. A. Kul chitskii; Zhur. Eksp. i Teoret.

Fiz. 38, 1685 (I960); Soviet Phys. JETP 11, 1215 (1960)

60Ba4 W. C. Barber, F. Berthold, G. Fricke, F. E. Gudden;

Phys. Rev. 120, 2081 (1960)

60Ba5 W. C. Barber, V. J. Vanhuyse. Nuclear Phys. 16, 381

( 1960

)

60Ba6 W. C. Barber, V. J. Vanhuyse. J. Phys. Radium 21, 299

( 1960 ) 60Ba7 D. Balfour, D. C. Menzies; Proc. Phys. Soc . 75, 543 (1960)

60Ba8 M. A. Bak, K. A. Petrzhak, Tei-Mei Chen; Izv. Akad,

Nauk SSSR 24, 818 (1960)

60Bel W. Bertozzi, P. T. Demos, S. Kowalski, F. Paolini, C. P.

Sargent; PICNS 746, (1960)

6OB0I B. A, Bochagov, A. P. Komar, G. E. Solaykin; Zhur. Eksp.

i Teoret. Fiz. 38, 1374 (I960); Soviet Phys. JETP 11, 990

( 1960 ) 6CBo2 0. v. Bogdankevich, L. E. Lazareva, A. M. Maiseev;

Zhur. Eksp. i Teoret. Fiz. 39, 1224 (I960); Soviet Phys.

JETP 12, 853 ( 1961 ) 60Bo3 E. C. Booth; Nuclear Phys. 19, 426 (1960)

6CBrl C. Broude, H, E. Gove; PICNS 754 (1960)

60Bu2 A. Bussiere de Nercy; Compt. Rend. 250, 1252 (I960); (See

61Bu4

)

60Bu3 A. Bussiere de Nercy, M, Langevin; J. Phys. Radium 21,

293 (I960); (See 61Bu4)

60Cal E. E. Carroll, Jr., W. E. Stephens; Phys. Rev. 118, 1256

( 1960 ) 60Ca2 J. H. Carver, R. B. Taylor, W. Turchinetz; Aust . J. Phys.

13, 617 ( 1960

)

60Chl V. P. Chizhov; Zhur. Eksp. i Teoret. Fiz. 38, 809 (I960);

Soviet Phys. JETP 11, 587 (1960)

60Ch2 F. E. Chrien, A. H. Benade; Phys. Rev. 119, 748 (1960)

60Del B. I. Deutch, F. R. Metzger, F. J, Wilhelm; Nuclear Phys.

16, 81 ( 1960 ) 60De2 N. N. Delyagin; Zhur. Eksp. i Teoret. Fiz. 38, 1111 (I960);

Soviet Phys. JETP 11, 803 (1960)

65
60Dol H. G. Dosch, K, H, L indenberge r, P. Brix; Nuclear Phys

.

18, 615 ( 1960 ) 60Ecil R. D. Edge; Phys. Rev. 119, 1643 ( 1960 ) 60Enil V. Emma, C. Milone, A, Rubbino, A, Malvano; Nuovo

Cimento 17, 365 (1960)

60Em2 V. Emma, C. Milone, A. Rubbino, Phys. Rev. 118, 1297

( 1960 ) 60Fal R. Fast, P. A. Flournoy, R. S. Tickle, W. D,

Whitehead; Phys. Rev. 118, 535 (1960)

60Fel F. Ferrero, S. Ferroni, R. Malvano, S. Menardi, E, Silva;

Nuclear Phys. 15, 436 (1960)

60Fe2 B. T. Feld, B. C. Maglic, J. Parks; Nuovo Cimento 17,

Suppl. 2, 241 ( 1 960 ) 60F11 P. A. Flournoy, R. S. Tickle, W. D. Whitehead; Phys. Rev,

120 , 1424 ( 1960 ) 6OF0I B. Forkman, S.A.E. Johansson; Nuclear Phys. 20, 136

( 1960 ) 60Fo2 B. Forkman, I. Wahlstrom; Arkiv Fysik 18, 339 (1960)

60Gal J. A. Galey; Phys. Rev. 117, 763 (1960)

60Ga2 M. Garnier, H. Gauvin, W, Sebaoun; J. Phys. Radium 21,

893 ( 1960 ) 60Gel K. N. Geller; Phys. Rev. 120, 2147 (1960)

60Ge2 K. N, Geller, J. Halpern, E. G. Muirhead; Phys. Rev. 119,

716 (1 960 ) 60Ge3 K. N. Keller, J. Halpern, E. G. Muirhead; Phys. Rev. 118,

1302 ( 1 960 ) 6OG0I V. I. Gol danskii, 6. A. Karpukhin, A. V. Kutsenke, V. V.

Pavlovskaya; Zhur. Eksp. i Teoret. Fiz. 38, 1695 (I960);

Soviet Phys. JETP 11, 1223 (1960)

6OG02 A. N. Gorbunov, F. P. Denisov, V. A, Kolutkhin; Zhur.

Eksp. i Teoret. Fiz. 38, 1084 (I960); Soviet Phys. JETP 11,

783 ( 1960 ) 60Grl V. M. Grizhko, D, I. Sikora, V. A. Shkoda-Ul yanov, A.

D. Abramenkov, B. I. Shramenko , A. N. Fisun; Zhur.

Eksp. i Teoret. Fiz. 38, 1370 (I960); Soviet Phys. JETP 11,

987 ( 1960 ) 60Hal F. I. Havlicek; Nuovo Cimento 18, 65 (1960)

6CEa2 S. S. Hanna and R. E. Segel; Proc. Royal Soc . (London)

A259, 267 (1960)

60Hel D. F. Hebbard; Nuclear Phys. 15, 289 (1960)

60He2 D. F, Hebbard, J. L. Vogl; Nuclear Phys. 21, 652 (1960)

6OH0I P. Horvat, J. Pahor, M. Vakselj; Nuclear Phys. 16, 90

( 1960 )

60Isl D. Isabelle, G. Bishop; Compt. Rend. 251, 697 (1960)

60Jal D. Jamnik, D. Axel; Phys. Rev. 117, 194 (1960)

60Kil J. D. King, W. J. McDonald; Nuclear Phys. 19, 94 (1960)

60Ki2 J. D. King, R. N, H. Haslam, R, W. Parsons. Can. J.

Phys . 38, 231 ( 1 960 ) 60Ki3 M. Kimura, K. Shoda, N, Mutsuro, T. Tohei, K. Sato, K.

Kuroda, K. Kuriyama, T, Ariba; J. Phys. Soc. Japan 15,

1 128 ( 1960 ) 60Ki4 J. D. King, R. N. H. Haslam, W. J. McDonald; Can. J.

Phys. 38, 1069 (1960)

66
60Kol

60Ko2

6CKo3

6 0Ko4

6CKo5

60Krl

eOKul

60Ku2

60Lil

60Li2

60Mal

60Ma.2

60Mel

60Me2

60M1 1 60Wi2

eoMol

60Mul

6CNel

60Prl

60Pr2

60Eel

60Fe2

6OF0I

60Ro2

60Eo3

60Fo4

60Sal

60Sa2

60Stl

eOTal

A. P. Komar, Ya . Krzhemenek, I. P. Yavor; Dokl , Akad.

Nauk SSSR 131, 283 (I960); Soviet Phys . Doklady 5, 295

( 1 961 ) A. P. Komar, Ya , Krzhemenek, I. P. Yavor; Dokl. Akad.

Nauk SSSR 135, 291 (I960); Soviet Phys. Doklady 5, 1234

( 1961 ) A. P. Komar, E.

135, 52 ( 1960 ) ; A. P. Komar, E,

Akad. Nauk

824 ( 1961 ) SSSR

D. Makhnovskii; Dokl. Akad. Nauk SSSR

Soviet Phys. Doklady 5, 1229 (1961)

D. Makhnovskii, V. P. Puddubnov; Dokl.

133, 797 (I960); Soviet Phys. Doklady 5,

A.

R.

P. Komar

;

Krone,

Kuo Ch i-di,

1578 ( 1960 ) ;

1 562 ( 1 960

)

39,

PICNS-60, 494 (1960)

J. J. Singh; Phys. Rev. 117,

B. S. Ratner; Zhur. Eksp. i Teoret, Fiz.

Soviet Phys JETP 12, 1098 (1961)

L. A, Kul chitskii, V, Presperin; Zhur. Eksp. i Teoret. Fiz,

39, 1001 (I960); Soviet Phys. JETP 12, 696 (1961)

N. V. Linkova, R. M. 6sokina, B. S. Ratner, Sh. Amirov,

V. V. Akindinov; Zhur. Eksp. I Teoret. Fiz. 38, 780 (I960);

Soviet Phys. JETP 1 1 , 566 ( 1960 ) K. U. Lindenberger

,

( 1960 ) E. D. Makhnovskii; Zhur. Eksp

(I960); Soviet Phys. JETP 11,

B» Mainsbridge; Nuclear Phys.

J. A. Scheer; Z. Physik 158, 111

X Fiz. 38, 96

70

21

Swann, V, K.

Teoret

.

( 1 960 )

, 1 ( 1 96 0 ) Rasmussen

;

Nuclear

138 ( 1960

)

F. R. Metzger, C. P.

Phys. 16, 568 (1960)

F. R, Metzger; J. Franklin Institute 270,

C. Milone; Phys. Rev. 120, 1302 (1960)

M. Miwa, M. Yamanouchi ; J. Phys. Soc. Japan 15, 947

( 1960 ) W. L. Mouton, P. B, Smith; Nuclear Phys. 16, 206 (1960)

N, Mutsuro, K. Sato, M, Mishina; J. Phys. Soc, Japan 15,

358 ( 1 960 ) J, ©. Newton; Nuclear Phys. 21, 529 (1960)

D. G.

L. I

.

( 1960

)

K.

Proctor, W. H.

Prokhorova, G.

Voelker; Phys. Rev. 118, 217

N. Smirenkin; Atom. Energiya

Reibel

,

J. M. Reid,

( 1960 ) H. J. Rose;

H. J. Rose,

( 1960 )

M. Rozkos,

129 ( 1960 )

A. K. Mann; Phys. Rev. 118, 701 (1960)

B, Lalovic; Proc. Phys. Soc. (London)

Nuclear Phys

F. Riess, W.

19, 1 13 ( 1960 ) Trost; Nuclear Phys. 21,

( 1960 ) 8, 457

76, 6 5

367

M. Smrcka, 6. Jakxibcek; Czech. J. Phys. 10,

J. P. Roalsvig, R. N. H. Haslam, J. L. Bergste insson; Can.

J. Phys. 38, 320 (1960)

D. Sadeh; Phys. Rev. Letters 4, 75 (1960)

D. Sadeh; Compt. Rend. 250, 1632 (1960)

P. C. Stein, A. C. 0dian, A. Wattenberg, R

Phys. Rev. 119, 348 (1960)

R. B. Taylor; Nuclear Phys. 19, 453 (1960)

We i nste i n;

67
60Ta2 G. Tamas, J. Miller, C. G. Schuhl, C. Tzara; J. Phys

.

Radium 21, 532 (1960)

60Ta3 E, Takekoshi, J, Phys, Soc . Japan 15, 2129 (1960)

60Thl H. H. Thies, B, M. Spicer; Australian J. Phys. 13, 505

( 1960 ) 6OT0I R. A. Tobin; Phys. Rev. 120, 175 (1960)

60Val V. J. Vanhuyse, G. J. Vanpraet; J. Phys. Radium 21, 290

( 1960 ) 60Wal I. ¥/ahlstrom, B. Forkman; Arki v Fysik 18, 83 ( 1960 ) 60\*a2 T. G. Walker, W. T. Morton; Proc . Phys. Soc. 75, 4

( 1960 ) 60A«yl J. M, Wyckoff, H. W. Koch; Phys. Rev. 117, 126 1 ( 1960)

60Yal S. Yasumi, M. Yata, K. Takamatsu, A. Masaike, Y.

Masuda; J. Phys. Soc. Japan 15, 1913 (1960)

60Zil B. Ziegler; Nuclear Phys. 17, 238 (1960)

61Akl A. F. Akkerman, D. K. Kaipov, Yu. K. Shubnyi; Zhur.

Eksp. i Teoret. Fiz. 40, 1031 (1961); Soviet Phys. JETP 13,

725 ( 1961 ) 61Aml B. Ambrozy, A. Faudrowicz, A. Jasinski, J, Kownacki, H,

Lancman, J. Ludz ie Jewski ; PICNS-61 281 (1961)

61Bal J. E. E. Baglin, M. N. Thompson, B. M. Spicer; Nuclear

Phys. 22, 207 ( 1 96 1 ) 61Ba2 R. G. Baker, K. G. McNeill; Can. J. Phys. 39, 1158 (1961)

61Ba3 P. S. Baranov, L. I. Slovokhotov, G. A. Sokol, N.

Shtarkov; Zhur. Eksp. i Teoret. Fiz. 41, 1713 (1961); Soviet

Phys. JETP 14, 1219 (1962)

61Bel A, K. Berzin, R. P. Meshcheryakov; Zhur. Eksp. i Teoret.

Fiz. 41, 1013 (1961); Soviet Phys. JETP 14, 72 1 (1962)

61Be2 R. E. Benenson, L. J. Lidofsky; Phys. Rev. 123, 939 (1961)

61Bil G. R. Bishop, G. A. Proca; J. Phys. Radium 22, 541 (1961)

6IB0I 6. Borello, S. Costa, F. Ferrero; Nuclear Phys. 27, 25

( 1961 ) 61Bo2 B. A. Bochagov, A. P. Komar, G. E. Solyakin, V. I.

Fadeev; Atom. Energiya 11, 540 (1961)

61Bo3 6. A, Borello; Rev. Un . Mat. Argent. As. Fis. Argent. 19,

251 ( 1961 ) 61Bo4 P. Bounin, G. R. Bishop; J. Phys. Radium 22, 555 (1961)

61Brl P. Brix, H. Fuchs, K. H, Lindenberger, C. Salander; Z.

Physik 165, 485 (1961)

61Bul J. Butler; Phys. Rev. 123, 873 ( 1961 ) 61Bu2 G. R. Burleson; Phys. Rev. 121, 624 (1961)

61Bu3 A. B. DeNercy; J. Phys. Radium 22, 535 (1961) (see 61Bu4)

61Bu4 A. Bussiere de Nercy; Ann. Phys. (Paris) 3rd Series,

Vol . 6, 1 379 ( 1961 ) 61Cal J. H. Carver, G. A. Jones; Nuclear Phys. 24, 607 (1961)

61Ca2 J. H. Carver; Proc. Phys. Soc. 77, 417 (1961)

61Cel R. J. Cence, B. J. Moyer; Phys. Rev. 122, 1634 (1961)

( 1961 ) 61Ce2 M. Cerineo, K. Ilakovac, I. Slaus, P. Tomas; Phys. Rev.

124, 1947 ( 1961 ) 61C11 M. A. Clark, H. E. Gove, A. E. Litherland; PICNS-61 807

( 1961 )

68
61Col S, G, Cohen, P, S. Fisher, E. K, Warburton; Phys. Rev.

121 , 858 ( 1961 ) 61Co2 G, E, Coote, W, E . Turchinetz, I.F.Wright; Nuclear Phys.

23, 468 ( 1961 ) 61Crl H. Crannell, R. Helm, H. Kendall, J, 6eser, M. YearianJ

Phys. Rev. 123, 923 (1961)

61 Del H. G. DeCarvalho, A, G. DaSilva, J. Goldemberg; Nuovo

Cimento 19, 1131 (1961)

61De2 H. G. DeCarvalho, A. Celano, G. Cortini, R. Rinzivil[o, G.

Ghigo; Nuovo Cimento 19, 187 (1961)

61De3 B. I. Deutch, F. R. Metzger; Phys. Rev. 122, 848 (1961)

61Dul B. Dudelzak, R. E. Taylor; J. Phys. Radium 22, 544 (1961)

61Ecl A. C. Eckert, E. F. Shrader; Phys. Rev. 124, 1541 (1961)

61£ml V. Emma, C. Milone, A. Rubbino, S. Janelli, F.

Mezzanores; Nuovo Cimento 22, 135 (1961)

61Fil E. Finch, U. Hegel; Z. Physik 162, 154 (1961)

6IF0I B. Forkman; Nuclear Phys. 23, 269 (1961)

61Gal C. C. Gardner, P. C. Gugelot; PICNS-61, 263 (1961)

6IG0I H. E. Gove, A. E. Litherland, R. Batchelor; Nuclear Phys.

26, 480 ( 1 961 ) 61Hal W. D. Hamilton, B. S. Sood; Nuclear Phys. 27, 66 (1961)

61Hel R. E. Hester, W. A. S. Lamb; Phys. Rev. 121, 584 (1961)

61He2 U. Hegel, E. Finckli; Z. Physik 162, 142 ( 1961 ) 6IH0I C. P. Ho, E. L. Iloff; Nuclear Phys. 27, 234 (1961)

61Hul J. P. Hummel, Phys. Rev. 123, 950 (1961)

61Isl D. S. Isabelle, G. R. Bishop; J. Phys. Radium 22, 548

( 1961 ) 61Jal M. J. Jakobson; Phys. Rev. 123, 229 (1961)

61Ja2 A. N. James; Nuclear Phys. 24, 675 ( 1961 ) 6IJ0I W. John, F. V. Martin; Phys. Rev. 124, 830 (1961)

61Kel L. Keszthelyi, I. Berkes, I. Demeter, I. Fodor; Nuclear

Phys. 23, 513 ( 1 96 1 ) 61Ke2 W. H. Kelly, G. B. Beard; Nuclear Phys. 27, 188 (1961)

61Ke3 H. W. Kendall, J. I. Friedman, E. F. Erickson, P. A. M.

Gramm; Phys. Rev. 124, 1596 (1961)

61Kil M. Kimura, K. Shoda, N. Mutsuro, T. Tohei, K. Sato,

K.Kuroda, K.Kuriyaraa, T.Akiba; Nuclear Phys. 23, 338

( 1961 ) 61Knl H. H. Knitter, H. Waffler; PICNS-61, 823 (1961)

6IK0I A. P. Komar, B. A. Bochagov, G. E. Solyakin; Dokl.

Akad. Nauk SSSR 141, 1339 (1961); Soviet Phys. Doklady

6. 1088 ( 1962)

61Kul Kuo Ch i-di, B. S. Ratner, B. V. Sergeev; Zhur. Eksp. i

Teorct Fiz. 40, 85 (1961); Soviet Phys. JETP 13, 60 (1961)

61Lal F. Lacoste, G. R, Bishop; Nuclear Phys. 26, 511 (1961)

61Mal E. D. Makhnovskii; Zhur. Eksp. i Teoret. Fiz. 41, 1091

(1961); Soviet Phys. JETP 14, 779 (1962)

61Ma2 M. Masuda; J. Phys. Soc. Japan 16, 1801 (1961)

61Mel V. Meyer, H. Muller, H. H. Staub, R. Zurmuhle; Nuclear

Phys. 27, 284 ( 1 961

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69
61Mil J. Miller, C. Schuhl, C. Tzara; J. Phys. Radium 22, 529

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61Myl H, Myers, R. Gomes, D. Guinier, A, V, Tollestrup; Phys.

Rev. 121 , 630 ( 1961 )

i 61Nal I. C, Nascimento, G, Moscati, J. Goldemberg, Nuclear

Phys. 22, 484 (1961)

6IN0I R. Nordhagen; Nuclear Phys, 27, 112 (196 1)

61 Pel J. P. Perez y Jorba, H, Nguyen Ngoc; J, Phys, Radium 22,

551 (1 961 ) 61Pe2 G. A. Peterson, W. C. Barber; PICNS-61, 83 1 (1961)

6IP0I R. A, Pope, D, V. Freck, W, W, Evans; Nuclear Phys,

24, 657 ( 1 961 ) 61Prl V, Presperin, L, A, Kul chitskii; Zhur, Eksp. i Teoret . Fiz.

41, 60 (1961); Soviet Phys. JETP 14, 46 (1962)

6 1 Ra 1 V. K, Rasmussen, F, R, Metzger, C, P. Swann; Phys.

Rev , 123, 1386 ( 1 961 ) 6IF0I T. Rothem, F, R. Metzger, C, P. Swann; Nuclear Phys.

22, 505 ( 1961

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6IR02 J. P. Roalsvig, I. C. Gupta, R. N. H. Haslam; Can. J,

Phys. 39, 643 ( 196 1 ) 61Sal D. Sadeh; Phys. Rev, 123, 855 (1961)

61Sa2 C. P, Sargent, W. Bertozzi, P. T. Demos, W. Turchinetz;

Proceedings of the Symposium on Neutron Time -of -Fl ight Methods, p. 353 (1961)

61Sel R. E. Segel, J. W. Daughtry, J. W. Glness; Phys. Rev.

123, 194 ( 1961

)

61Se2 R. E. Segel, M. J. Bina; Phys, Rev, 124, 814 (1961)

61Se3 W, Sebaoun, H, Gauvin; J. Phys, Radium 22, 771 (1961)

61Se4 W. Sebaoun, J. Phys, Radium 22, 735 (1961)

61Shl K, Shoda, K, Kobayashi, S. Siina, K. Abe, M. Kimura; J,

Phys, Soc. Japan 16, 1031 (1961)

61Sh2 V. G. Shevchenko, B. A. Yur ev ; Zhur, Eksp, i Teoret,

Fiz. 41, 1421 (1961); Soviet Phys. JETP 14, 1015 (1962)

61Sh3 K. Shoda; J. Phys. Soc. Japan 16, 1841 (1961)

61Sh4 K. Shoda, S. Siina, K. Kobayashi, K. Abe, M. Kimura; J,

Phys. Soc. Japan 16, 1807 (1961)

61Sh5 K. Shoda, K. KobayShi, S. Siina, K. Abe, M. Kimura; J.

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61Sh6 V. G. Shevchenko, B. A. Yur ev; Izv. Akad Nauk SSSR

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61Sul M. Sugawara; J. Phys. Soc. Japan 16, 1857 (1961)

61Swl C. P. Swann, V. K. Rasmussen, F. R, Metzger; Phys,

Rev. 121, 242 ( 1961 ) 61Tal F. Tagliabue, J, Goldemberg, Nuclear Phys, 23, 144 (1961)

61Ta2 N. W, Tanner, G. C. Thomas, E. D. Earle; PICNS-61 297

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( 1961

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61Thl I. M. Thorson, L, Katz; Proc. Phys. Soc. 77, 166 (1961)

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70
61 Val

61 Va2

61 Va3

61 Wal

611*6 1 61 1

6 1 Wo 1 62Anl

62An2

62Bal

62Bel

62Be2

62Be3

62Be4

62Bi 1

62Bi2

62Bi3

62Bi4

62B11

62Bol

62Bo2

62Bo3

62Bo4

62Bo5

62Bo6

62Bo7

62Bo8

62Brl

V, J. Vanhuyse,

( 1961 ) W. C, Barber; Nuclear Phys 26, 233

Antuf ev, E, G, Kopane±s, A. N, L

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1 035 ( 1962

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Nuclear Phys. 25, 409 (1961)

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R. E.

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A. K. Val ter, Yu. P.

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Soviet Phys. JETP 14,

K. J. Van 6ostrum, N,

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Nuovo Cimento 19, 864 (1961)

Welsh, D. J. Donahue; Phys.

C. Williams, H. S. Caplan, D. T.

Soc. (London) 78, 1125 (1961)

Wolfe, J. P. Hummel; Phys. Rev. 123, 898 (1961)

Anashkina; Zhur. Eksp. i Teoret, Fiz. 43, 1197

(1962); Soviet Phys. JETP 16, 847

Yu, P. Antuf ev, A. K. Val

Kopanets, S, P. Tsytko; Zhur.

(1962); Soviet Phys. JETP 15,

V. V. Balashov, V. N

Fiz . 26, 1 188 ( 1 962 )

A. S. Belousov, S. V. Rusakov, E. I. Tamm; Zhur. Eksp.

Teoret. Fiz. 43, 813 (1962); Soviet Phys, JETP 16, 576

( 1963)

J,

E.

H.

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( 1963

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Eksp. i Teoret.

268 ( 1962

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E. G.

Fiz, 42, 386

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G, Ben-David (Davis),

87 ( 1962)

B. Huebschmann; Phys. Letters 3,

C. Becchi, L. Meneghetti, Meneghetti, S. Vitale; Vitale; Phys. Letters Letters 3, 89

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I. Berkes, I. Dezsi, I. Fodor, L. Keszthely; Nuclear Phys.

39, 631 ( 1962)

M. Bizzet i -Sona, M. Bocciolini, G.

Mando; Nuovo Cimento 26, 1412 (1962)

B. Isabelle; Phys. Letters 1, 323 (1962)

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Grossetete, J. C. Risset; J. Phys, Radium

D,

D.

B,

J. Bellicard; PICNS-62 761 (1962)

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DiCapol iacco , M.

G. R. Bishop,

G, R, Bishop,

G, R, Bishop,

23, 31 ( 1962 ) D, Blum, P, Barreau,

€(, V, Bogdankevich, B, I, Goryachev, V, A, Zapevalov;

Zhur, Eksp. i Teoret, Fiz, 42, 1502 (1962); Soviet Phys.

JETP 15, 1 044 ( 1 962 ) L, N. Bolen, W, D, Whitehead; Phys, Rev, Letters 9, 458

( 1962 ) G, Bonazzola, O, A, Borello, S, Costa, S, Ferroni; Nuclear

Phys, 34, 637 ( 1962 ) R, Bosch, J. Lang, R. Muller, W, Wolfli; Phys, Letters 1,

1 14 ( 1962 ) 6. Borello, F. Ferrero, R. Malvano, A. Molinari; Nxiclear

Phys. 3 1, 53 ( 1962 ) E. C. Booth, K. A. Wright; Nuclear Phys. 35, 472 (1962)

R. Bosch, J. Lang, R. Muller, W. Wolfli; Helv. Phys, Acta

35, 288 ( 1 962 ) B, A, Bochagov, A, P, Komar, G, E, Solyakin; Zhur. Eksp,

i Teoret, Fiz. 43, 1611 (1962); Soviet Phys. JETP 16, 1135

( 1963 ) H. Breuer, W. Pohlit; Nuclear Phys. 30, 417 (1962)

71
62Br2 D. W. Braben, L. L. Green, J. C. Willmott; Nuclear Phys

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62Br4 H. Breuer; Z. Naturforsh. 17A, 584 (1962)

62Bul N. A. Burgov, G. V, Danilyan, B. S. Dolbilkin, L, E.

Lazareva, F. A, Nikolaev; Zhur. Eksp. i Teoret. Fiz. 43, (1962); Soviet Phys. JETP 16, 50 (1963)

62Cal J, H. Carver,

37, 449 ( 1 962 ) G.

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62Ca2 J, H, Carver,

2198 ( 196 2

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R. B. Taylor; Phys. Rev. 127

62Ca3 S. Cavallaro,

597 ( 1962 ) R. Polrenza, A, Rubbino; Nuclear Phys. 36,

62Chl R. E. Chrien,

1680 ( 196 2 ) H. H. Boloirln, H. Palevsky; Phys. Rev. 127,

62Ch2 V. P. Chlzhov, A . P • Komar, L. A. Kul chitskii. A, V.

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126, 1 822 ( 1962 ) 62Cul B. Cujec; Nuclear Phys. 37, 396 (1962)

62Del W. E. Del Bianco, W. E.Stephens; Phys. Rev. 126, 709

( 1962 ) 62De2 B. I. Deutch; Nuclear Phys. 30, 191 (1962)

62De3 H. G. DeCarvalho, A . Man f r ed ini , M.Muchnik, M.Severi,

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25, 534 ( 1962)

62Dol W. R. Dodge, W. C. Barber; Phys. Rev. 127, 1746 (1962)

62Drl T. N. Dragnev, B, P. Konstantinov; Zhur. Eksp. i Teoret.

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62Edl R. D. Edge, G. H. Peterson; Phys. Rev. 128, 2750 (1962)

62E11 R. J. Ellison, B. Dickinson; Nuclear Phys. 35, 606 (1962)

62Einl V. Emma, C. Milone; S. Jannelli, F. Mezzanares; Nuovo

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62Eul P. Euthymiou, P. Axel; Phys. Rev. 128, 274 (1962)

62Fil F, W. K. Firk; Phys. Rev. Letters 8, 321 (1962)

62Fi2 F. W. K. Firk, K. H. Lokan, E. M. Bowey; PICNS-62 804

( 1962 ) 62Fi3 F. W. K. Firk, E. R. Rae; PICNS-62 807 (1962)

62Ful S.C.Fultz, R.L.Bramblett, J.T.Caldwell, N. E. Hansen C.

P. Jupiter; Phys. Rev. 128, 2345 (1962)

62Fu2 S. C. Fultz, R. L. Bramblett, J. T. Caldwell, N. A. Kerr;

Phys. Rev. 127, 1273 (1962)

62Fu3 E. G. Fuller, E. Hayward; Nuclear Phys. 30, 613 (1962)

62Fu4 E. G. Fuller, E. Hayward; Nuclear Phys. 33, 431 (1962)

62Fu5 H, Fuchs, D, Haag, K, H. Lindenber ger, U. MeyerBerkhout; Z. Naturforsch 17a, 439 (1962)

62Fu6 H. Fuchs, R. Kosiek, U. Meyer- Berkhout ; Z. Physik 166,

590 ( 1 962 ) 62Gal C. C. Gardner, J. D. Anderson; Phys. Rev. 125, 626 (1962)

62Gel D. S. Gemmell, G. A. Jones; Nuclear Phys. 33, 102 (1962)

72
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( 1962 ) 62Gol A. N, Gorbunov, V, A, Dubrovina, V, A, Osipova, V, S.

Silaeva, P. A. Cerenkov; Zhur. Eksp. i Teoret. Fiz, 42, 747

(1962); Soviet Phys. JETP 15, 520 (1962)

62Go2 A. N. Goi'bunov, V, A. 6sipova; Zhur. Eksp. i Teoret. Fiz.

43, 40 (1962); Soviet Phys. JETP 16, 27 (1963)

62Go3 D. Goldman, A. F. T. Piza, E. Silva; Nuovo Cimento 25,

41 ( 1962)

62Go4 A. N, Gorbunov, D. K. Kaipov, K. G. Kuvatov; Trudy Inst.

Yadernoi Fiz., Akad. Nauk Kazakh. 3SR 5, 135 (1962)

62Grl G. M. Griffiths, E. A. Larson, L. P. Robertson; Can. J. , Phys. 40, 402 (1962)

62Gr2 A. G. Greeory, T. R. Sherwood, E. W. Titterton; Nuclear

Phys. 32, 543 ( 1 962

)

62Hel K. 6. Hermann, J. A. Scheer; Z. Physik 170, 162 (1962)

62Hul J. R . Hui zenga, K.M.Clarke, J.E.Girdler; R. Vandenbosch;

Nuclear Phys. 34, 439 (1962)

62Hu2 J. R. Huizenga, R. Vandenbosch; Nuclear Phys. 34, 457

( 1962

)

62Jal H. E. Jackson; Phys. Rev. 127, 1687 (1962)

62Jol S. A .E.Johansson, B.Forkman; Nuclear Phys. 36, 141 (1962)

62Jo2 \». John, J. M. Prosser; Phys. Rev. 127, 23 1 ( 1962)

62Kal D. K. Kaipov, Yu . K. Shubnyi, R. B. Begzhanov, A. A.

Islamov, Zhur. Eksp. i Teoret. Fiz. 43, 808 (1962); Soviet

Phys. JETP 16, 572 (1963)

62Kel H. W. Kendall, I. Talmi ; Phys. Rev. 128, 792 (1962)

62Kol A. P. Komar, A. V. Kulikov, V. P. Chizhov, I. P. Yavor,

Yu. M. Volkov; Zhur. Eksp. i Teoret. Fiz. 43, 1657 (1962);

Soviet Phys. JETP 16, 1168 (1963)

62Ko2 A. P. Komar, Ya. Krzhemenek, I. P. Yavor; Nuclear Phys.

34, 55 1 ( 1962

)

62Ko3 K. Kotajina; Nuclear Phys. 39, 89 (1962)

62Ko4 A. P. Komar, B. A. Bochagov, V. I. Fadeev; Dokl. Akad.

Nauk SSSR 146, 1051 (1962); Soviet Phys. Doklady 7, 913

( 1963 ) 62Krl M. Kregar, B. Povh; Phys. Letters 2, 103 (1962)

62Kul K. Kuriyama; J. Phys. Soc. Japan 17, 1681 (1962)

62Lal B. T. Lawergren, T. R. 0phel; Phys. Letters 2, 265 (1962)

62Lil F. F. Liu, F. J. Loeffler, T. R. Palfrey, Y. S. Kim; Phys.

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62Li2 N. Lingappa, E. Kondaiah, C. Badrinathan, M. D.

Deshpande, M. Balakr is hnan ; Nuclear Phys. 38, 146 (1962)

62Mal I. G. Main; Nuovo Cimento 26, 884 (1962)

62Mel F. R. Metzger; Phys. Rev. 128, 2332 (1962)

62Me2 F. R. Metzger; Phys. Rev. 127, 220 (1962)

62Mil J. A. Miskel, K. V. Marsh, M. Lindner, R. J. Nagle; Phys.

Rev. 1 28, 27 17 ( 1962

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62Mi2 J. Miller, C. Schuhl, G. Tamas, C. Tzara; Phys. Letters 2,

76 (1962)

62Mi3 J. Miller, C. Schuhl, C. Tzara; Nuclear Phys. 32, 236

( 1962)

73
62M14 U. Miklavzic, N. Bezic, D. Jamnik, G. Kernel, Z. Milavc,

J, Snajder; Nuclear Phys. 31, 570 (1962)

62Mi5 C. Milone, S, Milone Tamburino, V. Emma, S, Femino, S.

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62Wol W. L. Mouton, J, P. F, Sellschop, R. J. Keddy; Phys.

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62Mo2 W. T. Morton, T. G. Walker; Phil. Mag. 7, 74 1 (1962)

62Wo3 G. Moscati, J. Goldemberg; Phys. Rev. 126, 1098 (1962)

62Mul N. Mutsuro , K. Kageyama, M. Mishina, T. Nakagawa, E.

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62Wu2 N, Mutsuro, K. Kageyama, M. Mishina, E. Tanaka, M.

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62Nel E, B. Nelson, R. R. Carlson, L. D. Schlenker; Nuclear

Phys. 31, 65 ( 1962 ) 62Ne2 D. R. Neher, F. W. Prosser, Jr., R. W. Krone; Nuclear

Phys. 3 1, 231 ( 1 962

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620C1 J. S. O Connell, P. A. Tipler, P. Axel; Phys. Rev. 126,

228 ( 1962 ) 620dl M. 6dera; J. Phys. Soc. Japan 17, 1675 (1962)

62epl T. R. €Jphel, B. T. Lawergren; Nuclear Phys. 30, 215

( 1962 ) 62Clp2 T. R. 6phel, R. N. Glover, E, W. Titterton; Nuclear Phys.

33, 198 ( 1962)

62Pal V. Parikh; Nuclear Phys. 38, 529 (1962)

62Pa2 A. W. Parker, G. G. Shute; Australian J. Phys. 15, 443

( 1962 ) 62Pel G. A. Peterson, W. C. Barber; Phys. Rev. 128, 812 (1962)

62Prl F. W, Prosser, Jr., W. P. Unruh, B. W. Wildenthal; R. W.

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62Ral L, K. Rangan, G. I. Harris, L. W. Seagondollar ; Phys.

Rev. 1 27, 21 80 ( 1962 ) 62Rel G. C. Reinhardt, W, D. Whitehead; Nuclear Phys. 30, 201

( 1962 ) 62Sel F. D. Seward; Phys. Rev. 125, 335 (1962)

62Se2 W. Sebaoun; J. Phys. Radium 23, 989 (1962)

62Shl A. K. Shardanov, V. G. Shevchenko, Zhur. Eksp. i Teoret.

Fiz. 42, 1438 (1962); Soviet Phys, JETP 15, 996 (1962)

62Sh2 V. G. Shevchenko, B. A, Yur ev ; Zhur. Eksp. i Teoret.

Fiz. 42, 707 (1962); Soviet Phys. JETP 15, 492 (1962)

62£h3 V. G. Shevchenko, B. A. Yur ev; Zhur. Eksp. i Teoret,

Fiz. 43, 860 (1962); Soviet Phys, JETP 16, 609 (1963)

62Sh4 V, G. Shevchenko, B. A. Yur ev ; Nuclear Phys. 37, 495

( 1962 ) 62Sh5 X. R. Sherwood, W. E. Turchinetz; Nuclear Phys. 29, 292

( 1962 ) 62Sh6 V. G. Shevchenko, B. A. Yur ev ; Vestn. Mosk. Univ., Ser.

Ill, No. 3, 90 ( 1962 ) 62Sh8 K. Shoda, T. Ishizuka, K. Shimizu, M. Akashi ; J. Phys,

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74
62ShlO K. Shoda,

Soc • Japan

62Shll K. Shoda,

Klmura; J.

62Shl2 K. Shoda,

Kimura; J.

62Sml P. J. M. Smulders, P

62Sol Yu. I. Sorokin, V. G

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I 7, 407 ( 1962 ) K, Abe, T, Ishizuka,

Phys. Soc, Japan 17,

T. Ishizuka, N. Kawamura, K. Abe,

Phys. Soc. Japan 17, 40 1 (1962)

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N, Kawamura,

73 5 ( 1 96 2

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M.

M.

( 1 962 )

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43, 1600 (1962); Soviet Phys. JETP 16,

62Sul

62Su2

62Tul

62 Vol

62Vo2

62Wal

63Akl

63Anl

63 An 2

63An3

63Aul

63Axl

63Bal

63Ba2

63Ba3

6 3 Bel

63Be2

63Be3

63Be4

63Be5

63Be6

63Be7

63Be8

63Bi 1

1127 ( 1 963 ) B. N. Sung; J. Phys. Soc. Japan 17, 1811 (1962) 842 (1962)

M. Suffert, G. Costa, D. Magnac-Vaiette; PICNS-62

P. M. Tutakin; Zhur. Eksp, i Teoret. Fiz. 43, 1140 (1962);

Soviet Phys, JETP 16, 80 5 (1963)

Yu. M. Volkov, L. A. Kul chitskii; Zhur. Eksp. i Teoret.

Fiz. 42, 108 (1962); Soviet Phys. JETP 15, 77 (1962)

Yu. M. Volkov, A. V. Kulikov, V. P. Chizov; Zhur. Eksp. i

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E. K. Warburton, H. 6. Funsten; Phys. Rev. 128, 1810

( 1962 ) A. F. Akkertnan, V. L. Kochetkov, V, N. Chekanov, V. V.

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D. W. Anderson, A. J. Bureau, B. C, Cook, J. E. Griffin,

J. R. McConnell, K. H. Nybo ; Phys, Rev. Letters 10, 250

( 1963 ) Y. P. Antoufiev, L. M. El-Nadi, D. A. E, Darwish, 0. E.

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E. S. Anashkina ; Zhur, Eksp, i Teoret, Fiz, 45, 404 (1963);

Soviet Phys, JETP 18, 279 (1964)

R, H, Augustson, N, N. Kaushal, W. R, Meyer, E. J.

Winhold, P. F. Yergin; Helv, Phys. Acta 36, 816 (1963)

P. Axel, K. Min, N. Stein, D. C. Sutton; Phys. Rev,

Letters 10, 299 (1963)

W. C. Barber, J. Goldemberg, G. A. Peterson, Y.

Torizuka; Nuclear Phys. 41, 46 1 (1963)

G. M. Bailey, D. R. Hebbard; Nuclear Phys. 46, 529 (1963)

M. V. Ballariny; Notes de Fisica 10(No. 12), 205 (1963)

B. L. Berman, L,

Letters 10, 527

M. Bernheim, G.

Bernheim, G.

Bertozzi, C.

M.

\».

6,

J,

G,

108 ( 1963

)

A, Becker, J,

B. Beard, W.

Bertozzi, P.

J. Koester, Jr., J. H. Smith; Phys. Rev.

( 1 963 ) R. Bishop; Phys, Letters 5, 270 (1963)

R, Bishop; Phys. Letters 5, 294 (1963)

P. Sargent, W. Turchinetz; Phys. Letters

D. Fox; Nuclear Phys. 42, 669 (1963)

H. Kelly; Nuclear Phys. 43, 523 (1963)

W, Bertozzi, P. T, Demos, S. Kowalski, C. P. Sargent, W.

Turchinetz, R. Fullwood, J. Russell; Phys. Rev. Letters

10, 106 ( 1963)

M. Bernheim, G. R. Bishop; J. de Physique 24, 970 (1963)

G. R. Bishop, M. Bernheim; Phys. Letters 5, 140 (1963)

75
63Bi2

63Bi3

63B11

63BI2

63Bo 1

63Bo2

63Bo3

63Bo4

63Bo5

63Bo6

63Brl

63Bul

63Bu2

63Bu3

63Cal

63Chl

63 Col

63Co3

63Cvl

63Dc3

63Del

63Fi 1

63Fi2

63Fi3

63Fi4

G. R, Bishop, C. Betourne, D, B, IsabelLc; J, de Physique

24, 973 ( 1963)

G, E, Bizina, A. G, Beda, N, A, Burgov, A. V, Davydov;

Zhur. Eksp, i Teoret. Fys. 45, 1408 (1963); Soviet Phys

.

JETP 18, 973 ( 1 964 ) D, Blum, P. Barreau, J, Bellicard; Phys. Letters 4, 109

( 1963 ) Blanc

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36, 820

J. P.

Acta

L, N, Bolen,

( 1963 ) R, Bosch, J.

Acta 36, 625

P. Bounin, G

M . Lambert

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( 1963 ) C, F, Perdrisat; Helva Phys.

W. D. Whitehead; Phys. Rev. 132, 2251

Lang, R. Muller, W, Wolfli; Helva. Phys.

( 1963

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R. 24, 974

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45, 882 ( 1963 );

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A. Nikolaev; Zhur. Eksp. i Teoret. Fiz,

Soviet Phys. JETP 18, 606 (1964)

B. A, Bochagov, A, P. Eomar, V, I, Fadeev; Atomnaya Energiya 15, 191 (1963); Soviet Atomic Energy 15, 891

( 1963)

R. L, Bramblett, J. T, Caldwell, G. F, Auchampaugh, S.

C. Fultz; Phys. Rev. 129, 2723 (1963)

N. A. Burgov, G. V. Danilyan, D, S. Dolbilkin, L. E.

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( 1963)

W. Buss, H. Waeffler, B, Ziegler; Phys. Letters 4, 198

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N. A. Burgov, G. V, Danilyan, B. S, Dolbilkin, L, E.

Lazareva, F. A, Nikolaev; Zhur. Eksp. i Teoret. Fiz.

1693 (1963); Soviet Phys. JETP 18, 1159 (1964)

J. T. Caldwell, R. R. Harvey, R. L. Bramblett, S. C.

Fultz. Phys. Letters 6, 213 (1963)

P. A. Treado; Nuclear Phys. 40, 195

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P. R. Chagnon,

( 1963

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S. Ferroni,

308 ( 1963 ) S, Costa, V. Wataghin, R. Malvano, Phys.

Letters 4_

S. Costa, F. Ferrero, S. Ferroni, B. Minetti, C. Molino, R.

Malvano; Phys. Letters 6, 226 (1963)

F. Cvelbar, A. Hudoklin, M. V. Mihailovic, M, Najzer, V.

Ramsak; Phys. Letters 3, 364 (1963)

H. Schmid, W. Scholz; Z. Physik 175, 430 (1963)

H. G, DeCarvalho, A. Manfredini, M. Muchnik, M. Severi,

R. Bosch, VI, Wolfli; Nuovo Cimento 29, 463 ( 1963)

P.

A.

S.

B.

Fisher, D. F. Measday,

Clegg;

Finckh, R,

Nuc lear

A. Nikolaev,

1 13 ( 1963 ) A, Kalmykov,

E.

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271 (1963)

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( 1963 )

Phys, 45,

Kosiek, K, H, Li ndenberger , U. MeyerNucker, K. Schlupmann; Phys, Letters 7,

Kosiek, K, Schlupmann; Naturwiss, 50, 326

E. Finckh, R

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174, 337 ( 1963

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Kosiek, K. H, Li ndenberger , K.

M. Schechter, J. Zimmerer; Z

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63F11 H. H, Fleischmann; Ann. Physik 12, 133 (1963)

63F12 H. H. Fleischmann, F. W, Stanek; Z, Physik 175, 172

( 1963 ) 63Frl D. E. Frederick. Phys. Rev. 130, 1131 (1963)

63Fr2 E. Friedland, H. R. Lemmer; Z. Physik 174, 507 (1963)

63Ful H. Fuchs, D. Haae; Z. Physik 171, 403 (1963)

63Fu2 H. Fuchs; Z. Physik 171, 416 (1963)

63Fu3 B. Furubayashi , E. Tcranishi, M. Kageyama; J. Phys. Soc

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Japan 18, 1235 (1963)

63Gal N. B. Gale, N. Tubbs, N. Nath, A. T. G. Ferguson; Phys.

Letters 5, 345 (1963)

63Gel K. N. Geller; Nuclear Phys. 40, 177 (1963)

63Ge2 K. N. Geller; Phys. Rev. Letters 11, 371 (1963)

63Go2 A. N. Gorbunov, A. T. Varfolomeev; Phys. Letters 5, 149

( 1963)

63Go3 H. E. Gove; Nuclear Phys. 49, 279 (1963)

63Go4 J. Goldemberg, Y. Torizuka, W, C. Barber, J. D. Walecka;

Nuclear Phys. 43, 242 (1963)

63Go5 S. Gorodetzky, W, Benenson, P. Chevallier, D. Disdier, F.

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63Go8 J. Goldemberg, E. W. Hamburger, A. Szi ly; An. Acad.

Brasil. Cienc. 35, 169 (1963)

63Grl G, M. Griffiths, M. Lai, C. D. Scarfe; Can. J. Phys. 41,

724 ( 1963

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63Hel D. F. Hebbard, G. M. Bailey; Nuclear Phys. 49, 666 (1963)

63Hol P. Horvat, P. Kump , B. Povh; Nuclear Phys. 45, 341

( 1963)

63Isl D. B. Isabelle, G. R. Bishop; Nuclear Phys. 45, 209 (1963)

63Is2 B. S. Ishkhanov, E, N, Kornienko, Yu. I. Sorokin, V. G,

Shevchenko, B. A. Yur ev; Zhur . Eksp. i Teoret. Fiz. 45,

38 (1963); Soviet Phys. JETP 18, 29 (1964)

63Kal D. K. Kaipov, R» B. Begzhanov, A. V. Kuz minov, Yu. K.

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Phys. JETP 17, 1217 (1963)

e3Ka2 T. Kaminishi, C. Kojima; Jap. J. Appl. Phys. 2, 399 (1963)

63Ka3 D. K. Kaipov, Yu . K. Shubnyi, Yu. G. Kosyak, R. B.

Begzhanov; Zhur. Eksp. i Teoret. Fiz. 45, 443 (1963); Soviet Phys. JETP 18, 305 (1964)

63Kel H. W. Kendall, J. 6eser; Phys. Rev. 130, 245 (1963)

63Kil Y. S. Kim, F, F. Liu, F. J. Loeffler, T. R. Palfrey; Phys,

Rev. 129, 1362 (1963)

63K12 M. Kimura, K. Shoda, N. Mutsuro, M. Sugawara, K. Abe,

K. Kageyama, M. Mishina, A. 6no, T. Ishizuka, S. Mori,

N. Kawamura, T. Nakagawa, E. Tanaka; J. Phys. Soc.

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63Kol A. P. Komar, B. A. Bochagov, V. I. Fadeev; Dokl. Akad.

Nauk SSSR 152, 858 (1963); Soviet Phys. Doklady 8, 978

( 1964)

63Ko2 I. Kohno; J. Phys. Soc. Japan 18, 1709 (1963)

63Krl M. Kregar, B. Povh; Nuclear Phys. 43, 170 (1963)

63Kul L. A. Kul chitskii, Yu, M. Volkov; Zhur. Eksp. i Teoret.

Fiz. 44, 1153 (1963); Soviet Phys, JETP 17, 780 (1963)

77
63Ku2 L. A. Kul chitskii, Yu , M. Volkov, V. P. Denisov, V. I,

6rgurtsov; Izv. Akad . Nauk. SSSR 27, 1412 (1963)

63Lal M. Langevln, J, M, Loiseaux; J, dc Physique 24, 1027

( 1963

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63Lel F. H. Lewis, Jx*, , J« D, Walecka, J, Goldemberg, W, C,

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63Lol F. J. Loeffler, T. R, Palfrey, Jr., T. 6. White, Jr., Phys.

Rev. 131, 1844 ( 1963

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63Lo2 R. Lombard, P. Kossanyi, G. R. Bishop; J. de Physique

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63Mcl J. A. Mclntyre, G. K. Tandon ; Phys, Letters 4, 117 (1963)

63Mc2 G. J. McCallum; Can. J. Phys. 41, 923 (1963)

63Wc3 W. J. McDonald, E. Buchholz, R. N, H. Hasiam; Can. J.

Phys. 41, 180 ( 1963

)

63Mel F. R. Metzger, H. Langhoff; Phys. Rev. 132, 1753 (1963)

63Mil I. V. Mitchell, R. B. Taylor; Nuclear Phys. 44, 664 (1963)

63Mi2 K. Min, L. N. Bolen, W. D. Whitehead; Phys. Rev. 132,

749 ( 1963

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63Wi3 K. Miyano, T. Kuroyanagi, Nuclear Phys. 49, 315 (1963)

63Mi4 C, Milone; Nuclear Phys. 47, 607 (1963)

63Mi5 0. M. M. Mitchell, K. G. McNeill; Can. J. Phys. 41, 871

( 1963)

63Mol W. L. Mouton, J. P. F. Sellschop, G. Wiechers; Phys.

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63Mul K. M, Murray, W. L. Bendel; Phys. Rev. 132, 1134 (1963)

63Mu2 N. Mutsuro, K. Rageyama, M. Mishina, E. Tanaka, T.

Aizawa, M. Kimura; J. Phys. Soc. Japan 18, 599 (1963)

63Nel B. M. K. Nefkens ; Phys. Rev. Letters 10, 55 (1963)

63Ne2 B. M, K. Nefkens; Phys. Rev, Letters 10, 243 (1963)

63Ngl H. Nguyen Ngoc , M. Hors, J. Perez y Jorba; Nuclear

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63Ng2 H. Nguygen Ngoc, J. Perez y Jorba; J. de Physique 24,

965 ( 1963

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63Gdl M. Gdera, N. Yamamuro, J. Phys. Soc. Japan 18, 325

( 1963)

63<3sl R. M. Osokina; Zhur Eksp . i Teoret. Fiz, 44, 444 ( 1963);

Soviet Phys, JETP 17, 303 (1963)

63Pel R, R, Perry, B, Mainsbridge, J, Richards; Nuclear Phys,

45, 586 ( 1963)

63Pe2 K, A, Petrzhak, R, V, Sedletskii; Atomnaya Energiya 15,

308(1963); Soviet Atomic Energy 15, 1025 (1963)

63Prl F, W. Prosser, Jr, , R, W. Krone, J. J. Singh; Phys. Rev.

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63Fel N, W, Reay, N, M, Hintz, L, L. Lee, Jr., Nuclear Phys.

44, 338 ( 1963)

63Ril V. Fiech; Phys. Letters 6, 267 (1963)

63Ri2 P. Rice-Evans; Proc. Phys, Soc, 82, 914 (1963)

63Sal K, Sato; J. Phys. Soc. Japan 18, 1353 (1963)

78
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Let'ters 7 269 ( 1963 ) 63Sc3 H. Schmid'and W. Scholz; Z. Physik 175, 430 (1963)

63Sel R, E. Segel, P. P. Singh, R, G. Alias, S. S, Hanna; Phys.

Rev. Leti:ers 10, 345 ( 1963 ) 63Shl V. G. Shevchenko, B. A. Yur ev , B. P. Levkin; Zhur.

Eksp. i Teoret. Fiz. 44, 808 (1963); Soviet Phys. JETP 17,

547 ( 1 963 ) 63Sh2 N. K. Sherman; Phys. Letters 4, 113 (1963)

63Sh3 N. K, Sherman; Phys. Letters 4, 138 (1963)

63£h4 K. Shoda, B, N. Sung, N. Kawamura, M. 6yamada, K. , Abe, T. Ishizuka, M. Kimura; J. Phys. Soc. Japan 18, 152

( 1963)

63Sh5 Yu. K, Shubnyi ; Zhur. Eksp. i Teoret. Fiz. 45, 460 (1963);

Soviet Phys. JETP 18, 316 (1964)

63511 L. Simons, K, E. Nysten, M. Koskelin, 6, Siltanen, E.

Spring, G. Wendt ; Phys. Letters 3, 306 (1963)

63512 L. Simons, K. E. Nysten, E. Spring, L. Kald; H. Junger, P.

Holmberg, I. Forsblom; Phys. Letters 7, 344 (1963)

63Skl S. J, Skorka, R. Hubner, T. W. Re tz "Sc hmid t , H. Wahl

Nuclear Phys. 47, 417 (1963)

63Spl E. Spring; Soc, Sci. Fennica, Commenta ti ones PhysMath. 28, I ( 1963

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63Stl R. F. Stiening, E. Loh, M. Deutsch; Phys. Rev. Letters 10,

536 (1963 ) 63Sul M. Sugawara, S. Mori, A. 6no, A. Hotta, M. Kimura; J.

Phys. Soc. Japan 18, 17 (1963)

63Su2 M. Suffert, G. Costa, D. Magnac-Valette; J. de Phys. 24,

1029 ( 1 963 ) 63Til P. A. Tipler, P. Axel, N. Stein, D. C. Sutton; Phys. Rev.

129, 2096 ( 1963 ) 63Val V. J . Vanhuyse, G . T. Vanpraet ; Nuclear Phys. 43, 344 (1963)

63Va2 A. K. Val ter, E. G. Kopanets, A. N, L vov, S. P. Tsytko;

Izv. Akad. Nauk. SSSR 27, 232 (1963)

63Va3 V. J. Vanhuyse, G. J. Vanpraet; Nuclear Phys. 45, 602

( 1963 ) 63Va4 V. J, Vanhuyse, G. J. Vanpraet, K. J. Van Camp; Phys.

Letters 5, 89 (1963)

63Va5 A. K. Val ter, E, G, Kopanets, A. N. L vov, A. Stegner, S.

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63Vel A. Veres; Int. J. Appl . Rad. Isotopes 14,123 (1963)

63Ve2 A. Veres; Acta Phys. Acad. Sci. Hung. 16, 261-273 (1963)

63^al J. B. Warren, K. L. Erdman, L. P. Robertson, D. A,

Axen, J. R. MacDonald; Phys. Rev. 132, 1691 (1963)

63Wa2 H. D. Warren, A. P. Batson; Nuclear Phys. 48, 361 (1963)

63Yal N. Yamamuro; J. Phys. Soc. Japan 18, 11 (1963)

63Ya2 M. Yamanouchi; J. Phys. Soc. Japan 18, 638 ( 1963)

63Yol C. S. Young, D. J. Donahue; Phys. Rev. 132, 1724 (1963)

63Yo2 F. C. Young, J. C. Armstrong, J. B. Marion; Nuclear

Phys. 44, 486 (1963) (Errata: Nuclear Phys. 49, 695 (1963))

63Zal G. N. Zatsepina, V. V, Igonin, L. E, Lazareva, A. I.

Lepestkin; Zhur. Eksp. i Teoret. Fiz. 44,1787 (1963); Soviet

Phys. JETP 17, 1200 (1963)

79
63Zul

64A11

64A12

64A13

64A14

64A15

64Aml

64Arl

64Ar2

64Bal

64Ba2

64Ba3

64Ba4

64Ba5

64Bel

64Be2

64Be3

64Be4

64Be5

64Be6

64Be7

64Be8

64 Bi 1

64Bi2

64Bi3

64Bi4

64BI 1

R. W. Zurmuhle, W, E. Stephens, H. H. Staub; Phys.

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51 177 ( 1964)

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( 1964

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W, Quirk, B, M, Spicer; Aust . J, Phys. 17,

W. Quirk, B. M. Spicer; Nucl, Phys, 53,

F. R. Allum, T.

420 ( 1964 ) F. R. Allum, T.

545 ( 1964

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B. Arad ( Huebschmann ), G. Ben- David( Davi s )

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112 ( 1964 ) Fricke,

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P . Komar , A

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Nuclear Phys. 54, 549 (1964)

V. Kulikov; Zhur. Eksp. Soviet Phys, JETP 19, 1014

E. B. Bazhanov, A.

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( 1964)

G. Baciu; Rev. Roum. Phys. 9, 783 (1964)

G. Baciu, A. Bonazzola, B. Minetti, C. Molino, L.

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G. Baciu

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C. Molino, B. Minetti, L. Pasqualini, G.

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J. Bellicard, P. Barreau, D.

( 1964 ) R. B. Begzhanov,

46, 1486 ( 1964 )

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B. L. Berraan, L.

133, Bl 17 ( 1964 )

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Soviet Phys, JETP 19, 1005 (1964)

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Fiz,

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G. R, Bishop,

Phys, 54, 353

D,

Fiz,

M, Bernheim,

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G, R, Bishop,

54, 97 ( 1964

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G, R, Bishop, C,

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G. R, Bishop, M,

J, L. Black, G.

689 ( 1 964

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P. Kossanyi Demay; Nuclear

B. Isabelle, C. Betourne; Nuclear Phys.

Betourne, D. B. Isabelle; Nuclear Phys.

Bernheim; Phys. Letters 8, 48 (1964)

A. Jones, P. B. Treacy; Nuclear Phys. 54,

80
64B12 J. L. Black, N. W. Tanner; Phys. Letters 11, 135 (1964)

64Bol E. C. Booth, B. Chasan, K. A. Wright; Nuclear Phys. 57,

403 (1964)

64Bo2 R. Bosch, J. Lang, R. Muller, W. Wolfli; Phys. Letters 8,

120 ( 1964

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64Bo3 C. D. Bowman, G. F. Auchampaugh, S. C, Fultz; Phys,

Bev. 133, B676 (1964)

64Brl R. L. Bramblett, J. T. Caldwell, R. R, Harvey, S. C, Fultz;

Phys. Rev. 133, B869 (1964)

64Br2 P. Brix, H. G. Clerc, R. Engfer, G. Fricke, F. Gudden, H,

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64Chl K, W. Chen, J, R, Dunning, Jr., J. R. Rees, W, Shlaer, J.

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64Col E. G. Corman, R. W, Jewell, W. John, J. E. Sherwood, D«

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64Co2 S. Costa, F. Ferroni, S. Ferroni, C. Molino, R. Malvano;

Phys. Letters 11, 324 (1964)

64Co3 S. Costa, F. Ferrero, S. Ferroni, R. Malvano; PICNS-64

1034 ( 1964 ) 64Crl H. L. Crannell, T. A. Griffy; Phys. Rev. 136, B1580 (1964)

64Del A. DeMarco, R, Gar±agnini, G. Piragino; Phys. Letters 10,

213 ( 1964 ) 64De2 V. P. Denisov, A. V. Kulikov, L. A. Kul chitskii; Zhur.

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1007 ( 1 964 ) 64rie3 W. Del Bianco, W. E. Stephens, J. Wiza; Phys. Rev. 136,

B418 ( 1964

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64De4 H. G. De Carvalho, G. Cortini, E. Del Giudice, G.

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( 1964)

64Dol M. M. Dorosh, A. M. Parlafe, V. A. Shkoda Ulyanov, L. A.

Shabalina; Zhur. Eksp. i Teoret. Fiz. 46, 1540 (1964); Soviet Phys. JETP 19, 1042 (1964)

64Do2 B. S, Dolbilkin, V. A. Zapevalov, V. I. Korin, L, E.

Lazareva, F. A, Nikolaev; PICNS-64 1060 (1964)

64Dul I. I. Dushkov, B. S. Ishkhanov, I. M. Kaitonov, B, A. Yur

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64Eal E. D, Earle, N. W. Tanner, G. C, Thomas; PICNS-64 385

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64Ejl H. EJiri, Y. Nakjima, K. Horie, S. Matsumoto, Y, No garni

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Nuclear Phys. 51, 470 (1964)

64Erl F. C. Erne, C. Van der Leun; Nuclear Phys. 52, 515 (1964)

64Er2 R. A. Eramzhyan; Izv, Akad. Nauk. SSSR, Ser. Fiz., 28,

1 1 81 -1 1 84 (1 964 ) 64Fil F. W. K. Firk; Nuclear Phys. 52, 437 (1964)

64Fi2 F. W. K. Firk, E. M. Bowey; PICNS-64 1013 (1964)

64Fol B. Forkman, W. Stiefler; Nuclear Phys. 56, 604 (1964)

64Ful S. C. Fultz, R. L. Bramblett, J. T. Caldwell, R. R,

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81
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1

64Gol

64Go2

64Go3

64Go4

64Grl

64Gr2

64Gul

64Hal

64Ha2

64Ha3

64Hol

64 Iml

64 Isl

64Is2

64 Is3

64Jol

64 Ki 1

64Kol

64Ko2

64Ko3

64Ko4

64Ko5

64Lal

64La2

64La3

64La4

64La5

Phys. Letters 11, 137

Yu. Ya, Glazunov, M, V. Savin, I. N, Safina, E. F,

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A. N. Gorbunov, A, T, Varfolomeev;

( 1964 ) J, Goldemberg, W. C, Barber; Phys. Rev. 134, B963 ( 1964 ) J. Goldemberg, W. C, Barber, F. H. Lewis, Jr., J, W,

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J. C, Hafele, F, W, Bingham, J. S. Allen;

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S. S. Hanna, S, E. Segel, R. G. Alias; PICNS-64 1022

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Shevchenko, B, A. Yur ev; Zhur. Eksp. i

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A. Johansson; Phys. Rev. 136, B1030 (1964)

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R, Kosiek, K, Schlupmann. H. W, Siebert, R

Z, Physik 179,

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M . L an g ev in, J . M .

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Makhnovsky; Nuc I . Phys

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Wendling;

Nauk SSSR

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Nuclear Phys,

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64Nel

64Pal

64 Phi

64fial

64Ra2

64Fa3

64Fel

64Ril

64Scl

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64Sc3

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64 Si 1

64Sml

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65Mc 1 65Mc2

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65Mi 1 65Wol

65Wo2

65Ngl

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65Fal

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65Kel

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65Ko2

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65Si 1

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66Be4

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66C11

66C0I

66C02

66Co3

66Co4

66Co5

66Crl

66Del

66De2

66De3

66De4

66De5

66De6

66D0I

66E02

66Dul

66Du2

66Evl

66Fel

66F1 1 66Fi2

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N, De Botton, J Schuhl, G, Teunas, C, Tzara;

Nucl, Phys. 75,

Miller, C,

396 ( 1 966 ) Garfagnini

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Gar f agn in i

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G, Piragino; Nuovo Cimento

G. Piragino; Nuovo Cimento

J, Nucl, Phys, (USSR)

2, 48 ( 1 966 ) Kosareva, P, A,

82 (1965) Sov. J. Nucl.

A. De Marco, R,

44B, 172 ( 1966)

A, De Marco, R,

42B, 355 ( 1966

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V. P, Denisov, L, A, Kul chitskii;

2, 70 ( 1965) ; Sov. J, Nucl. Phys.

v. P, Denisov, A, Duisebaev, K, V,

Cerenkov; J, Nucl, Phys. (USSR) 1,

Phys. 2, 58 ( 1966 ) V. P. Denisov, L, A. Kul chitskii;

3, 268 (1966); Sov. J. Nucl. Phys.

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B. S. Dolbilkin, V. A. Zapevalov, V. I. Korin, L. E

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M. A. Duguay, C, K, Bockelman, T, H, Curtis, R. A,

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192 ( 1966 ) Rev. 145,

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Cimento 45B, 273 (1966)

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K, Firk; PICNS-66, 352 (1967)

F, Ferrero, C.

G. Rama; Nuovo

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89
66Fol

66Fo2

66Frl

66Ful

66Fu2

66Fu3

66Ge 1

66G0I

66Go2

66Go3

66Grl

66Gr2

66H0I

66Ho2

66Ho3

66Hrl

66Hul

66Hu2

66Isl

66Is2

66 Ivl

66Kel

66 Ko 1

66K02

66Ko3

66Ko4

66Lal

Ricco, C, Manf redo tt i; Nuovo Cimento

T. Tu and W. F, Hornyak; Nucl. Phys.

W. Schott, H, Langhoff, A, F iammersfeld; Z,

248 ( 1 966

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G. M. Fossa, G*

43B, 347 ( 1966

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P. D. Forsyth, H.

82, 33 ( 1966 ) L, Frevert,

Physik 194,

S, C. Fultz, J. T. Caldwell, B, L. Berman, R, L,

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S. C. Fultz, R. L. Bramblett, B. L. Berman, J. T,

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K. Fukuda, S. 0kabe, Y. Sato; Ann. Rep. Radiat. Center

Osaka Prefect. 7, 38 (1966)

H. M. Gerstenberg, J. S, 6 Connell; Phys. Rev. 144, 834

( 1966

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J. Goldemberg, C. Schaerf; Phys. Letters 20, 193 (1966)

A. Goldroann, P. Kneisel, H. v. Buttlar; Z. Physik 192, 282

( 1966 ) B. I. Goryachev,

A. Yur ev; ZhETF

330 ( 1 966 )

B. S. Tshkhanov, V. G. Shevchenko, B.

Pisma 4, 491 (1966) ; JETP Letters 4,

R. C. Greenwood,

( 1 966

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B. Grossetete,

1435 ( 1966

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P. Holmberg;

31 , 1 ( 1966

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J. H. Hough,

W. W, Black; Phys. Letters 21, 702

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Comm. Phys. Math. Ed. Soc . Sc i . Fennica

H. Hoffmann,

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W. L. Mouton; Nucl. Phys. 76, 248 (1966)

B. Prowe, H, Ullrich; Nucl. Phys. 85, 631

V. Knapp, M. Vlatkovic; Nucl. Phys. 89, 412

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Sci. USSR-Phys. 30, 383 (1966)

B. S. Ishkhanov, I. M. Kapitonov, Zh. M. Sel iverst ova, V.

G, Shevchenko, B. A. Yur ev; Izv. Akad. Nauk. SSR Fiz.

30, 1385 (1966) ; Bull. Acad. Sci. USSR 30, 1446 (1966)

V. G. Ivanchenko, B. S. Ratner; ZhETF Pisma 3, 452

3, 296 ( 1 966 ) Stephens; Phys. Rev. 149, 798 (1966)

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Ivanchenko

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(1966); JETP Letters

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G

E. M. Kellogg, W,

P. Koss any i -Demay

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( 1 966 ) R. Kosiek, D. Muller, R

Letters 21, 199 (1966)

M. Ya. Kondrat ko, K. A

20, 514 ( 1 966 ); Atomic Energy 20,

A. A. Koval, E, G. Kopanets, Yu. S. Korda, L. N,

Sukhotin, S. P. Tsytko; Izv. Akad. Nauk Fiz. 30, 416

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H. Langhoff, L. Frevert, W. Schott, A. F Iammersfeld;

Nucl. Phys. 79, 145 (1966)

Pfeiffer, 6. Merwitz; Phys.

Petrzhak; Atomnaya Energiya

594 ( 1966 )

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66Lel H. P. Leenhouts, P, M. Endt; Physica 32, 322 (1966)

66Lil H. Lichtbiau, B. M. Spicer; Aust. J, Phys. 19, 297 (1966)

66Li2 H, Liesem; Z. Physik 196, 174 (1966)

66L0I W. A. Lochstet, W. E. Stephens; Phys. Rev. 141 1002

( 1966

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66Wal G« E, Manuzio, G. Ricco, M, Sanzone; Nuovo Cimento

42B, 348 ( 1966 ) 66Ma2 J. Id, Maison, M, Langevin, J. M. Loiseaux; J. Physique

Colloq. 1 , 36(1 966

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66Ma3 A, Manfredini, M, Muchnik, L, Fiore, C, Raiaorlno, H, G.

Dc Carvalho, R, Bosch, W, Wolfli; Nuovo Cimento 44B,

218 (1966)

66Ma4 J. L. Matthews, W, Bertozzi, S. Kowalski , C. P. Sargent,

W. Turchinetz; PICNS-66, 386 (1967)

66Wel F, R. Metzger, R, S. Raghavan; Phys. Rev. 145, 968

( 1966 ) 66Me2 J. L. Meason, P. K. Kuroda; Phys. Rev. 142, 691 (1966)

66Me3 F. R. Metzger, G. K. Tandon; Phys. Rev, 148, 1133 (1966)

66Wil K. Min; Phys, Rev, 152, 1062 (1966)

66Mi2 J, Miller, C, Schuhl, G, Tamas, C. Tzara; J. de Physique

27, 8 ( 1966 ) 66Nel B. M, K, Nefkens, D, C. Sutton, M. N. Thompson; NucI

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Phys , 88, 523 ( 1 966 ) 66Nil 0, P, Nikotin and K, A. Petrzhak; Atom. Energiya 20, 268

( 1966 ) 66Mul F, Nusslin, H, Werner, J, Zlmmerer; Z, Naturforschg,

21A, 1 195 ( 1966 ) 566bl E. Gbst, F. Rauch, E, Rossle; Phys. Letters 21, 50 (1966)

666wl R. e. Gwens, J. E, E. Baglin; Phys. Rev. Letters 17, 1268

( 1 966 ) 66ew2 R. 0. 6wens, J. E, E, Baglin; PICNS-66, 337 (1967)

66Pal G, Paoli, M, Scotto, A, Wataghin; Nuovo Cimento 43B,

189 ( 1966 ) 66Pa2 V, Parikh; Nucl. Phys. 77, 157 (1966)

66Pa3 A, ^, Parker, R, R. Whitehead, G, G, Shute; Aust, J,

Phys, 19, 147 ( 1966 )

66Pa4 P, D. Parker; Phys, Rev, 150, 851 (1966)

66Pel G, A, Peterson, J, F, Ziegler; Phys, Letters 21, 543 (1966)

66Prl G, Proca, D, Isabelle, J, Goldemberg; J, Physique Colloq,

1, 105 ( 1966 ) 66Pul N. G, Puttaswamy, D, Kohler; Phys, Letters 20, 288 (1966)

66Eal R. S. Raghavan; Phys. Rev. 143, B947 (1966)

66Fa2 N. S, Rabotnov, G, N, Smirenkin, A, S, Soldatov, L, N.

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77, 92 ( 1966 ) 66Eil R, Riskalla, D, Vinciguerra; J, Physique Colloq, 1, 106

( 1966 ) 66Sal K, Sakamtoto, P. J. Kuroda; J. Inorg. Nucl, Chem. 28, 679

( 1966 ) 66Scl P. J. Scanlon; Nucl, Phys, 88, 424 (1966)

66Shl N, K, Sherman, J, P, Stewart, R, C, Morrison; Phys, Rev,

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66Sh2 N, ShikazonOf H, Takekoshi, T. Shoji; J, Phys. Soc , Japan

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66Spl E. Spamer; Z. Physik, 191, 24 (1966)

66Stl R. R. Stevens, Jr., Y. K. Lee, J. C. Walker; Phys. Letters

21 , 401 ( 1 966 ) 66St2 M. Stroetzel, F. Guctden; Phys, Letters 2 2, 485 ( 1966)

66Sul M. Suffert; Nucl. Phys. 75, 226 (1966)

66£wl C, P. Swann; Phys, Rev. 148, 1119 (1966)

66Tal J, F. Tatarczuk, H. A, Medicus; Phys. Rev. 143, B818

( 1966 ) 66Thl M. N. Thompson, J. M. Taylor; Nucl. Phys. 76, 377 (1966)

66Til 6. Titze, E. Spamer; Z. Naturf orschg . 21A, 1504 (1966)

66Val G, J. Vanpraet, W. C. Barber; Nucl. Phys. 79, 550 (1966)

66Va2 H. A. Van Rinsvelt, P. M. Endt ; Physica 32, 513 (1966)

66Va3 A. T. Varfolomeev, A. N. Gorbunov, G. G. Taran; J. Nucl.

Phys. (USSR) 3, 647 (1966) ; Sov. J. Nucl. Phys. 3, 473

( 1 966 ) 66Va4 C. Van der Leun, N. C. Burhoven Jaspers; Nucl. Phys.

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66Vel A. Veres, I. Pavlicsek; Int. J. App. Rad. and Isotopes 17,

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66Vol Yu. M. Volkov, A. P. Komar, V. P. Chizhov; J. Nucl.

Phys. (USSR) 3, 277 (1966) ; Sov. J. Nucl. Phys. 3, 198

( 1 966 ) 66Vul P. H. Vulster; Nucl. Phys. 83, 593 (1966)

66\<al W. B. Walters, J. P. Hummel; Phys. Rev. 150, 867 ( 1966)

66Wa2 6. A. Wasson, M. R. Bhat, R. E. Chrien, M. A. Lone, M.

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66Wel E. Wernbom-Selin, S. E. Arnell ; Ark. Fysik 31, 113

( 1 966 ) 66We2 R. Wendline, R. Koslek; Z. Physik 192, 502 (1966)

66Wil BJorn Wiik; Z. Physik 189, 423 (1966)

66^»ol W. Wolfli, R. Bosch, J. Lang, R. Muller, P. Marmier;

Phys. Letters 22, 75 (1966)

66Y0I D. H. Youngblood, G. C. Morrison, R. E. Segel; Phys,

Letters 22, 625 (1966)

66Zil B. Ziegler, W. Buss, H. Waf±ler; Nucl. Phys. 83, 145 (1966)

66Zi2 J. F. Ziegler, G. A. Peterson; PICNS-66, 319 (1967)

67Afl N. G. A±anas ev, V. A. Gol dshtein, S. V. Dementii, V. G.

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67Aml U. Amaldi Jr. , G. Campos Venuti, G. Cortellessa, E. De

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Letters 25B, 24 ( 1967)

67Anl Yu. P. Antuf ev, I. I. Miroshnichenko, V. I. Noga, P. V,

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( 1 968 ) 67An2 G. P. Antropov, I. E. Mitrofanov, V. S. Russkikh; Izv.

Akad. Nauk SSR Fiz. 31, 336 (1967) ; Bull. Acad. Sci,

USSR 31 , 320 ( 1967 ) 67Axl P. Axel, D. M. Drake, S. Whetstone, S. S. Hanna; Phys.

Rev. Letters 19, 1343 (1967)

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67Bal G. Barbicllini, C. Bernardini, F. Fclicetti, G, P. Murtas;

Phys. Rev. 154, 988 (1967)

67Ba2 E, B, Bazhanov, A, P. Komar, A, V. Kulikov; Dokl . Akad.

Nauk. SSSR 171, 549 (1966) ; Sov. Phys. Doklady 11, 953

( 1967)

67Ba3 G. Baciu, D, Catana, C. Deberth, I, Raileanu; Rev. Roum.

Phys. 1 2, 385 ( 1 967 ) 67Ba4 P. Barreau, J, B, Bellicard; Phys. Rev. Letters 19, 1444

( 1967 ) 67Ba5 J. E. E. Baglin, M. N. Thompson; PICNS-67, 388 (1967)

67Bel M. Bernheim, T. Stovalt, D. Vinciguerra; Nucl. Phys. A97, 488 ( 1 967 ) 67Be2 B. L. Berman, J. T. Caldwell, R. R. Harvey, M. A. Kelly,

R. L. Bramblett, S. C. Fultz; Phys. Rev. 162, 1098 (1967)

67Be3 M. Bernheim, T. Stovall, D. Vinciguerra; Phys, Letters

25B, 461 (1967)

67Be4 R. B. Begzhanov, A. A. Islamov, S. V. Starodub t sev; J.

Nucl. Phys. (USSR) 5, 250 (1967); Sov. J. Nucl. Phys. 5, 176 ( 1967 ) 67Be5 R. B, Begzhanov, A. A. Islamov; J. Nucl. Phys. (USSR) 5, 483 (1967);Sov. J. Nucl. Phys. 5, 339 (1967)

67Bc6 B. L. Berman, R. L. Van Hemert , C. D. Bowman; Phys.

Rev. 1 63, 958 ( 1 967 ) 67Be7 I. Bergqvist, J. A. Biggerstaff, J. H. Gibbons, W. M. Good;

Phys. Rev. 158, 1049 (1967)

67Be8 H. Bernatowicz, H. A. Medicus; PICNS-67, 384 (1967)

67B11 J. L. Black, W. J. 6 Connell, S. S. Hanna, G. L. Latshaw;

Phys. Letters 25B, 405 (1967)

67B12 J. L. Black, F. Piess, P. Paul, W. J. 6 Connell, G. A.

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67Bol C« H. Bornman, M. A. Meyer, D, Reitmann; Nucl. Phys.

A99 , 337 ( 1967

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67Bo2 C. D. Bowman, G. S, Sidhu, B. L. Berman; Phys. Rev.

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67Bul H. V. Buttlar, F. Freund, G. Gammel; Z. Physik 200, 1

( 1967 ) 67Cal P. H, Cannington, D, G. Owen, R. J. J. Stewart, E. G.

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67Ca2 J. T. Caldwell, Ph.D. thesis. University of California, 1967;

UCRL-50287

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67Chl C. Chasman, K. W. Jones, R. A. Ristinen, J. T, Sample;

Phys. Rev. Letters 18, 219 (1967)

67Col S. Costa, F. Ferrero, C. Manfredotti, L. Pasqualini, G,

Piragino, H, Arenhovel ; Nuovo Cimento 48B, 460 (1967)

67Co2 S. Costa, F. Ferrero, C. Manfredotti, L, Pasqualini, G,

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67Crl H. Crannell, T. A. Griffy, L. R. Suelzle, M. R. Yearian;

Nucl. Phys, A90, 152 (1967)

67Cr2 H, Crannell, H. A. Dahl, F. H. Lewis, Jr.; Phys. Rev. 155,

1062 ( 1967 ) 67Del V, P. Denisov, L. A. Kul chitskii; J. Nucl. Phys. (USSR)

5, 490 (1967); Sov. J. Nucl. Phys. 5, 344 (1967)

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67De3 V. P. Denisov, L. A. Kul chitskii; J, Nucl. Phys, (USSR)

6, 437 (1967); Sov. J. Nucl. Phys. 6, 318 (1968)

67De4 F. P. Denisov, A. Duisebaev, P. A. Cerenkov; ZhETF

Pisna 5, 249 (1967) ; JETP Letters 5, 200 (1967)

67Dil V. Di Napoli, F. Dobici, F, Salvetti, H. G, De Carvalho;

Nuovo Cimento 48B, 1 (1967)

67Di2 V. Di Napoli, F. Dobici, F. Salvetti, 6, Forina, H. G. De

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67Di3 V. Di Napoli, F. Dobici, 6, Forina, F. Salvetti, H. G. de

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67Dol E. J. Dowdy, J. A. Mclntyre; Phys. Rev. 157, 1166 (1967)

67Drl T. E. Drake, R, M. Hutcheon, V. W. Stobie, G. A. Beer,

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67Dr2 T. N. Dragnev, A. P. Komar; J, Nucl. Phys. (USSR) 5,

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67Dul M. A. Duguay, C. K. Bockelman, T. H. Curtis, R. A.

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67Eal E. D. Earle, N. W, Tanner; Nucl. Phys. A95, 241 (1967)

67Erl B. Erlandsson; Arkiv Fysik 34, 285 (1967)

67Esl G. P. Estes, K. Min; Phys. Rev. 154, 1104 (1967)

67Evl A. E. Evans; Phys. Rev. 155, 1047 (1967)

67Fel L. Feldman, B. B, Baliga, M, Nessin; Phys. Rev. 157, 921

( 1967 ) 67Fe2 S. Ferroni, V. Gracco, D. B. Isabelle, R. Malvano, M.

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67Fe3 W. Feldman, D. W. Heikkinen, W. E. Meyerhof; Phys.

Letters 25B, 593 (1967)

67Frl R. F. Frosch, H. L. Crannell, J. S. McCarthy, R. E, Rand,

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67Ful C. B. Fulmer, I. Williams, T. H. Handley, G. F. Dell,

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67Gal ti, L, Garzon, G. G. Rocco; J, Inorg. Nucl. Chem. 29, 1

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A96, 397 ( 1967

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67Ge2 H. M. Gerstenberg, E. G. Fuller; NBS Technical Note 416,

Study of a Halpern-Type Neutron Detector; U.S.

Government Printing dffice, Washington, D.C., June 1967.

67Gi 1 M. Giannini, P. Oliva, D. Prosperi, G. Toumbev; Nucl.

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67Gol B. I. Goryachev, B. S. Ishkhanov, I. M. Kapitonov, Zh. M.

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Phys. (USSR) 4, 505 (1966) ; Soviet J. Nucl. Phys. 4, 359

( 1967

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67Go2 D. R. Goosman, R. W, Kavanagh; Phys, Rev, 161, 1156

( 1967)

67Go3 B, I, Goryachev, B. S. Ishkhanov, B. G. Shevchenko, B.

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Pisma 5, 225 (1967) ; JETP Letters 5, 180 (1967)

67Go5 A. N, Gorbunov; PICNS-67, 376 (1967)

67Hal J. R, Harrington, B. M. Spicer; PICNS-67, 380 (1967)

67Hul R. R. Hurst, D. J, Donahue; Nucl, Phys. A9 1, 365 (1967)

67Hu2 S. M. Hussain, K, G. Mc Neiil; Can, J. Phys. 45, 2851

( 1967 ) 67Iel Yu , P. Tevlev, A, A, Koval, E. G, Kopanets, Yu. S, Korda

L. N. Sukhotln, S. P. Tsytko; Uk. Fiz. Zhur. 12, 743 (1967)

67Isl B. S. Ishkhanov, I, M. Kapitonov, V. G. Shevchenko, B, A,

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Phys. 4, 544 ( 1 967 ) 67Jol S. A. E. Johansson, L. Nilsson; Arkiv Fysik 35, 403 (19 67)

67Kal S. P. Kapitsa, V, I. Novgorodt seva , V. A. Pchelin, G. N.

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Pisma 6, 495 (1967) ; JETP Letters 6, 27 (1967)

67Knl P. Kneisel, A. Golctmann, H. v. Buttlar; Z. Physik 199,

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67Kol A. P. Komar, V. P. Denisov, L. A. Kul chitskii; Dokl.

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67Ko3 R. Kose, W. Paul, K. Stockhorst, K. H. Kissler; Z. Physik

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67Kr2 K. Kramer, H. v. Buttlar, A, Goldmann, B. Huber; Z,

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67Ku2 H, W. Kuehne, P. Axel, D. C. Sutton; Phys. Rev. 163,

1278 ( 1 967 ) 67Lal H. Langhoff, M. Schumacher; Phys. Rev. 155, 1246 (1967)

67La2 H. Langhoff; Phys. Rev. 159, 1033 (1967)

67La3 H. Langhoff, R. Cesareo, A. Fl ammer sf eld ; Z. Physik 205,

1 ( 1967 ) 67Lel J. R. Leslie, I. G. Main; Nuovo Cimento 50B, 389 (1967)

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67Lol J. M. Loiseaux, J. M. Maison, M. Langevin; J. de

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67Lo2 R. M. Lombard, G. R. Bishop; Nucl. Phys. AlOl, 601

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67Mel F. R. Metzger; Phys. Rev. 157, 1060 (1967)

67Me2 F. R. Metzger; Phys. Rev. 161, 1249 (1967) (See F. R.

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67Mul K. M. Murray, J. C. Ritter; PICNS-67, 383 (1967)

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67ebl E. 6bst, F. Rauch, H. G. Wahsweiler; NucL, Phys. A103,

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67ectl Y. 0da, H. Hirabayasi, K, Fujioka; PICNS-67, 374 ( 1967 ) 67Pal J. C. Pala thingal, M. L. Wiedenbeck; Nucl. Phys. AlOl,

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Red. 9, 626 (1969) ; JETP Letters 9, 384 (1969)

69Ar4 Yu. M. Arkatov, P. I. Vatset, V. I. Voloshchuk, A. P.

Klyucharev, V. L, Marchenko, A. F. Khodyachikh; Yad.

Fiz. 9, 473 (1969); Sov. J. Nucl. Phys. 9, 271 (1969)

69Ar5 Yu. M. Arkatov, A. V. Bazareva, P. I. Vatset, V. I.

Voloshchuk, A. P. Klyucharev, A. F. Khodyachikh; Yad.

Fiz. 10, 1123 (1969); Sov. J. Nucl. Phys. 10, 639 (1970)

69Bal G, Baciu, D. Catana, C. Deberth, C. Iliescu, B. Cirstoiu;

Z. Physik 227, 336 (1969)

69Ba2 J. E. E. Baglin, M. N. Thompson; Nucl. Phys. A138, 73

( 1969 ) 69Bel B. L. Berman, R. L. Bramblett, J. T. Caldwell, H. S.

Davis, M. A. Kelly, S. C. Fultz; Phys. Rev. 177, 1745

( 1969 ) 69Be2 N. Bezic, D. Brajnik, D. Jamnik, G. Kernel; Nucl. Phys.

A128, 426 ( 1 969

)

69Be3 B. L. Berman, R. L. Van Hemert , C. D. Bowman; Phys.

Rev. Letters 23, 386 (1969)

69Be4 R. Bergere, P. Carlos, A. Veyssiere, H. Beil; PICNS-69

352 ( 1 969 ) 69Be5 J, Berthot, P. Y. Bertin, J. P. Gi r ardeau- Mont aut , D. B.

Isabelle; PICNS-69, 138 (1969)

102
69Be6 R. Bergere, H, Beil, P. Carlos, A. Veyssiere; Nucl . Phys. A133, 417 (1969)

69Be7 R. B, Begzhanov, S. M. Akhrarov; ZhETF Pis. Red. 10, 39

(1969); JETP Letters 10, 26 (1969)

69Be8 B. L. Berman, M. A. Kelly, R. L. Brambtett, J. T.

Caldwell, H. S. Davis, S. C. Fultz; Phys. Rev. 185, 1576

( 1969 ) 69Be9 H. Beil, R. Bergere, P. Carlos and A. Veyssiere; C.R.

Acad. Sci . Paris 269, 216 (1969)

69BelO V, M. Bezotosnyi, V. A. Zhmailo, L. M. Surov, and M. S.

Shvetsov; Yad. Fiz. 10, 225 (1969), Sov. J. Nucl. Phys. 10,

127 (1970)

69Bol C. D. Bowman, B. L. Berman, H. E. Jackson; Phys. Rev.

178, 1827 ( 1969 ) 69Bo2 C. K. Bockelman, T. H. Curtiss, R, A, Eisenstein, D. W.

Madsen; PICNS-69, 132 ( 1969)

69Bo3 M. Boivin, Y. Cauchois, Y. Heno; Nucl. Phys. A137, 520

( 1969 ) 69Bo4 C. D. Bowman, R. J. Baglan, B. L. Berman; Phys. Rev,

Letters 23, 796 ( 1969)

69Cal H. S, Caplan, R. K, Gupta, E. L. Tomusiak, C. S. Yang;

PICNS-69, 134 ( 1969)

69Ca2 D. E. Carlson, A. A. Temperley; Phys. Letters 30B, 322

( 1969 ) 69Ca3 P. H, Cannington and J . M. Dixon; Aust J. Phys. 22, 679

( 1969 ) 69Cel R. Cesareo, M. Giannini, P. 0liva, D. Prosperi, M, C.

Ramorino; Nucl. Phys. A132, 512 (1969)

69Chl B. T. Chertok, E, C. Jones, W. L. Bendel, L. W. Fagg;

Phys. Rev. Letters 23, 34 (1969)

69Ch2 B. T. Chertok, E. C. Jones, W. L. Bendel, L. W. Fagg, H.

F. Kaiser, S. K. Numrich; PICNS-69, 60 ( 1969)

69Col S. Costa, L. Ferrero, L. Pasqualini, F. Ferrero, C.

Manfredotti; Lettere al Nuovo Cimento 1, 346 (1969)

69Co2 S. Costa, L. Ferrero, L. Pasqualini, C. Manfredotti;

Lettere al Nuovo Cimento 2, 318 (1969)

69Co3 G. W. Cole Jr., F. W. K. Firk, T. W. Phillips; Phys.

Letters 30B, 91 (1969)

69Co4 S. Costa, L. Ferrero, R. Garfagnini, G. Piragino, and A.

Zanini; Lettere Al Nuovo Cimento 2, 336 (1969)

69Cul T. H. Curtis, R. A. Eisenstein, D. W. Madsen, C. K.

Bockelman; Phys. Rev. 184, 1162 (1969)

69Dal A. V. Davydov, G. R. Kartashov, I. N. Vishnevsky; Phys.

Letters 30B, 616 (1969)

69Del H. G, De Carvalho, V. Di Napoli, D. Margadonna, F.

Salvetti, K. Tesch; Nucl. Phys. A126, 505 (1969)

69De2 T. K. Deague, E. G. Muirhead, B. M, Spicer; PICNS-69,

350 (1969)

69De3 W. Del Bianco, J. M. Poutissou; Phys. Letters 29B, 299

( 1969

)

69De4 F. P. Denisov, A. Duisebaev, P. A. Cerenkov; Yad. Fiz. 9,

3 (1969); Sov. J. Nucl. Phys. 9, 1 (1969)

69De5 T. K. Deague, E. G. Muirhead, B. M. Spicer; Nucl. Phys.

A139, 501 (1969)

103
69De6 S. V, Dementii, N, G, Afanas ev, I. M, Arkatov, V. G,

vtasenko, V, A, Got dshtein, E. L, Kuplennikov; Yad. Fiz.

9, 241 (1969); Sov. J. Nucl. Phys. 9, 142 (1969)

69De7 V. P. Denisov, A. P. Komar, L. A. Kui chitskii, I. Ya.

Chubukov; Yad. Fiz. 10, 1116 (1969); Sov, J. Nucl. Phys.

10, 635 ( 1970)

69De8 S. V. Dementii, M. G. Afanas ev, - M. Arkatov, V, G,

Vlasenko, V. 0. Gol dshtcln, E. L. Kuplennikov, V, I,

Startsev; Ukr. Fiz. Zhur. 14, 1911 (1969)

69Dil V. Di Napoli, D. Mar^adonna, F. Salvetti, H. G. De

Carvalho, J. B. Martins; Lettere al Nuovo Cimento 1, 121

( 1969 ) 69Di2 J. P. Didelez, H. Langevin-Joi iot, G. Duhamel, L. Marcus,

P. Narboni; Nucl. Phys. A139, 69(1969)

69Di3 V. DiNapoli, D. Margadonna, F. Salvetti; Ricerca Sci. 39,

133 ( 1969 ) 69Dol B. S. Dolbilkin, A. I. Isakov, V. I. Korin, L. E. Lazareva

ZhETF Pis. Red, 10, 365 (1969); JETP Letters 10, 231

( 1969 ) 69Do2 B, S, Dolbilkin, A. I. Isakov, V. I. Korin, L. E. Lazareva

N. V, Lin kova, B. A, Tulupov; Yad, Fiz. 9, 675 (1969);

Sov. J. Nucl. Phys. 9, 391 (1969)

69Do3 B, S. Dolbilkin, A. I, Isakov, V, I. Korin, L. E. Lazareva

N. V. Lin kova, and F. A. Nikolaev; Yad. Fiz. 9, 914

(1969),; Sov. J. Nucl. Phys. 9, 534 (1969)

69Eil R. A. Eisenstein, D. W, Madsen, H. Theissen, -L. S,

Cardman, C, A, Bockelman; Phys. Rev. 188, 1815 (1969)

69Ei2 F. Eigenbrod; Z. Physik 228, 337 (1969)

69EJ1 H. EJiri, P. Richard, S. Ferguson, R. Heffner, D. Perry;

Nucl. Phys. A128, 388 (1969)

69EJ2 H. Ejiri, S. M. Ferguson, I. Halpern, R. Heffner; Phys.

Letters 29B, 111 (1969)

69Fal L. W. Fagg, W, L. Bendel, E. C. Jones, Jr., S. Numrich;

Phys. Rev. 187, 1378 (1969)

69Fa2 L. W. Fagg, W. L. Bendel, E. C. Jones, Jr., H. F. Kaiser,

T. F. Godlove; Phys. Rev. 187, 1384 (1969)

69Frl D. E. Frederick, R. J, J, Stewart, R, C. Morrison; Phys.

Rev. 186, 992 (1969)

69Ful S. C. Fultz, B. L. Berman, J. T. Caldwell, R. L.

Bramblett, M. A. Kelly; Phys. Rev. 186, 1255 (1969)

69Fu2 C. B. Fulmer, I. R. Williams, K. S. Toth, G. F. Dell;

Phys. Rev. 188, 1752 (1969)

69Gal R. Garfagnini, G. Piragino, A. Zanini; Nuovo Cimento 63B,

670 ( 1969 ) 69Ga2 D. B. Gayther, J. W, McMillan, H. A. Medicus; PICNS69 365 ( 1969 ) 69Ga3 R, Garfagnini, G, Piragino, A, Zanini; Atti Accad. Naz.

Lincei, Rend, Cl . Sci. Fis. Mat. Natur. 47, 33 (1969)

69Gol A. N. Gorbunov; Yad. Fiz. 10, 469 ( 1969) Sov. J. Nucl.

-Phys. 10, 268 (1969)

69Go2 B. I. Goryachev, B. S. Ishkhanov, I. M. Kapitonov, I. M.

Piskarev, V. G, Shevchenko, 6. P. Shevchenko; Yad. Fiz.

10, 252 (1969); Sov. J. Nucl. Phys. 11, 141 (1970)

104
69Go3 B. I. Goryachev, B. S. Ishkhanov, I, M, Kapi-tonov, I, M.

Plskarev, V, G, Stievchenko, €>, P. Shevchenko; Izv,

Akad. Nauk. Fiz. 33, 1736 (1969); Bull. Acad. Sci. USSRPhys. 33, 1588 (1969)

69Grl H. D. Graber and Gale I. Harris; Phys. Rev. 188, 1685

( 1969

)

69Gr2 I. A. Grishaev, V. P. Efimov, V. I, Kasilov, V. I. Noga

,

Yu. N. Ranyuk, P. V. Sorokin, A. N, Fisun; Ukr, Fiz.

Zhur. 14, 1818 (1969)

69Gul I. S, Gul karov, N. G. Afanas ev, V. M. Khvastunov, N,

G. Shevchenko, V. D. Afanas ev, G. A. Savitskii, A, A.

Khomich; Yad. Fiz. 9, 478 (1969); Sov. J. Nucl . Phys. 9, 274 ( 1969 ) 69Gu2 I, S. Gulkarov, N, G, Afanas ev. A, A. Khomich, V, D.

Afanas ev, V, M. Khvastunov, G. A. Savitskii, N. G,

Shevchenko; Yad, Fiz. 9, 1138 (1969), Sov, J, Nucl. Phys,

9, 666 ( 1969 ) 69Gu3 I. S, Gul karov, N. G. Afanas ev, A. A. Khomich, V, M,

Khvastunov, V, D. Afanas ev, G. A. Savitskii, N. G,

Shevchenko; Yad, Fiz, 10, 694 (1969); Sov. J. Nucl. Phys.

10, 400 ( 1970)

69Hal M, Hasinoff, G, A, Fisher, H. M, Kuan, S. S. Hanna;

Phys. Letters 30B, 337 (1969)

69Ha2 G. I. Harris, A. K. Hyder,Jr., J. Walinga; Phys, Rev, 187,

1413 ( 1969 ) 69Hol W. Hofmann, R. Kosiek, G, Kraft, R, Mundhenke; Z.

Physik 225, 303 (1969)

69Hul R. M. Eutcheon, H. S. Caplan; Nucl. Phys. A127, 417

( 1969)

69Isl B, S, Ishkhanov, I, M, Kapitonov, E. V. Lazutin, I. M,

Piskarev, 6, P. Shevchenko; ZhETF Pis, Red. 10, 80

(1969); JETP Letters 10, 51 (1969)

69 Is2 B, S, Ishkhanov, I, M. Kapitonov, E, V, Lazutin, I, M,

Piskarev, 6. P. Shevchenko; Izv. Akad, Nauk. Fiz. 33,

2074 (1969); Bull. Acad. Sci. USSR-Phys. 33, 1889 (1969)

69 Is3 B. S. Ishkhanov, I. M. Kapitonov, E. V. Lazutin, I. M,

Piskarev, V. G. Shevchenko; Izv. Akad. Nauk. Fiz. 33,

1742 (1969); Bull. Acad. Sci. USSR-Phys. 33, 1594 (1969)

69Ivl V. G. Ivanchenko and B, S, Ratner; Izv. Akad. Nauk. Fiz.

34, 175 (1969); Bull. Acad. Sci, USSR-Phys, 34, 159 (1970)

69Kal S, P. Kapitza, N. S. Rabotnov, G, N. Smirenkin, A. S,

Soldatov, L, N. Usachev, Yu, M. Ysipenyuk; ZhETF Pis,

Red, 9, 128 (1969) ; JETP Letters 9, 73 (1969)

69Kel G. Kernel, W. M. Mason; Nucl. Phys. A123, 205 (1969)

69Ke2 M. A. Kelly, B. L. Berman, R, L, Bramble tt, S, C, Fultz;

Phys. Rev, 179, 1194 (1969)

69Ke3 N, K. Keller, J, K, P. Lee, D, B, McConnell; Can. J.

Phys. 47, 61 1 ( 1969 ) 69Khl T. A. Khan, J. S, Hewitt, K. G. iMcNelll; Can. J, Phys. 47,

1037 ( 1969

)

69Knl U, Knelssl, fl. Schneider, R. Volpel, K. Wolcken; Nucl,

Phys, A135, 395 (1969)

69Fol R. Rose, B, Martin, R, Runkel, H. Wahlen, K, H. Kissler;

Z. Physik 220, 305 (1969)

105
69Ko2

69Lal

69La2

69La3

69Lel

69Mal

69Ma2

69Ma3

69Ma4

69Ma5

69Mel

69Me2

69Ale3

69Mil

6 9Mol

69Mo2

69Mo3

69Mul

69Wu2

69Nal

69Na2

69Nel

69Nol

69ekl

69ewl

696w2

69Pel

69Pi 1

A. P. Komar, B. A, Bochagov, A, A, Kotov, Yu, N.

Ranyuk, G. G, Semenchuk, G, E. Solyakin, and P. V, Sorokin; Yad. Fiz. 10, 51 (1969), Sov. J. Nucl. Phys . 10,

( 1970

)

H. Langhoff, D. Gfoller; Nucl. Phys. A127, 379 (1969)

L. E. Lazareva and A, I. Lepestkin; Yad, Fiz. 10, 266

(1969); Sov. J. Nucl. Phys. 11, 149 (1970)

R. E. Larson and C. M. Gordon; J. Geophys.

( 1969)

J. C, Legg, D. G

S. Hechtl; Phys.

A. Man±redini , L

W. Wolfli; Nucl.

A.

Megli, D, R. Abraham,

Rev. 186. 1138 (1969)

Fiore, C. Ramorino, H,

Phys. A123, 664 (1969)

Manfredini, L

Wolfli; Nucl.

Res. 74, 6023

L. D. Ellsworth,

G. De Carvalho,

Fiore, C. Ramorino, H. De Carvalho,

Phys. A127, 687 (1969)

G. Manuzio, G. Ricco, M. Sanzone, L, Ferrero; Nucl,

Phys. A133, 225 (1969)

W. M, Mason, G, Kernel, J. L. Black, N. W.

Nucl. Phys. A135, 193 (1969)

W. M, Mason, N, W. Tanner, G. Kernel; Nucl

Al 38, 253 ( 1969

)

W, E, Meyerhof, W, Feldman, S,

Nucl, Phys. A131, 489 (1969)

F. R. Metzger; Phys. Rev, 187,

F. R, Metzger; Phys, Rev, 187,

Michalk, J, A, Mclntyre;

Gilbert, W,

Tannner

;

Phys,

OConnell;

V. E.

( 1 969

)

L, G, Moretto, R,

J, H, Heisenberg, Hofstadter; Phys,

1630 ( 1969

)

1700 ( 1969)

Nucl, Phys, A137, 115

C.

L,

Gatti, S. G, Thompson, J, T, Routti,

M. Middleman, M, R. Yearian, R.

Rev. 179, 1176 (1969)

R. Moreh, A. Wolf; Phys. Rev. 182, 1236 (1969)

R. Moreh and 6. Shahal; Phys. Rev. 188, 1765 (1969)

, Ritter; Phys, Rev, 182, 1097 (1969)

Phys. Rev. Letters 23, 1461 (1969)

Winhold, P. F. Yergin, P. Stoler, S.

A127, 669 ( 1969 ) Dwarakanath, D. Ashery; Nucl. Phys.

K. M, Murray, J. C

Kenneth M, Murray;

P. C. Nagle, E, J,

Mecca; Nucl. Phys.

K. Nagatani, M. R.

Al 28, 325 ( 1969

)

Reiner Neuhausen; Z. Physik 220, 456 (1969)

V. I. Noga, Yu, N, Ranyuk, and P, V, Sorokin; Yad, Fiz.

9, 1152 (1969), Sov. J. Nucl. Phys. 9, 673 (1969)

N. Sato; Bull. Chem. Soc, Japan 42,

J.

387

M. Spicer; PICNS-69,

Y. eka, T. Kato,

( 1969

)

D. G. awen, E. G. Muirhead, B.

349 ( 1 969

)

D. G. 6wen, B. M. Spicer; Phys. Letters 30B, 242 (1969)

K. A. Petrzhak and G. A. Tutin; Yad. Fiz. 9, 949 (1969),

Sov, J. Nucl. Phys. 9, 556 (1969)

C. J. Piluso, G, C. Salzman, D. K.

181 , 1555 ( 1969

)

McDaniels; Phys. Rev.

106
69Fi2 P. Picozza, C. Schaerf, R. Scrimaglio, G. Goggi , A.

Piazzoli, D, Scannicchio; Lettere al Nuovo Cimento II, 445

( 1969)

69Pi3 P. Picozza, C. Schaerf, R, Scrimaglio, G. Goggi, A.

Piazzoli, D. Scannicchio; PICNS-69, 70 (1969)

69Fal S. Ramchandran, J. A. Mclntyre; Phys , Rev, 179, 1153

( 1969)

69Fa3 V. K, Rasmussen, C. P. Swann ; Phys , Rev, 183, 918

( 1969

)

69Fil P, Richard, F, Gabbard, A. C, Porter, F. F, Hopkins;

Phys, Letters 29B, 646 (1969)

69Sal J. Sanada, M, Yamanouchi , N, Sakai, S, Seki; J, Phys.

Soc. Japan 26, 850 (1969)

69Sa2 G, A, Savitskii, N. G. Asanas ev, I. V, Avdreeva, I. S. Gul

karov, L, M, Krugovaya, V« M, Khvastunov, A, A,

Khoojich, N. G, Shevchenko; Izv, Akad, Nauk. Fiz, 33, 53

(1969), Bull. Acad. Sci . USSR-Phys. 33, 50 (1969)

69Sa3 G. A, Savitskii, N. G. Afanas ev, I, S, Gul karov, V. D,

Kovalev, V. M, Khvastunov, N, G. Shevchenko, I. V.

Andreeva; Izv. Akad. Nauk. Fiz. 33, 60 (1969), Bull. Acad.

Sci. USSR-Phys. 33, 56 (1969)

69Shl N. Shikazono, Y. Kawarasaki; J. Phys. Soc. Japan 27, 273

( 1969

)

69Sh2 N. Shikazono, Y. Kawarasaki; J. Phys. Soc. Japan 26,

13 19 ( 1 969 ) 69Sh3 T. Shintomi,

( 1969

)

M. Masuda; J . Phys. Soc . Japan 26, 607

69Sh4 K. Shoda, H. Taneichi; J. Phys . Soc . J apan 26, 217 ( 1969 ) 69Sh5 K. Shoda, M.

Letters 23,

Sugawar a, 800 (1969)T. Sai t o

,

H. Miya se; Phys. Rev.

69Sh6 K. Shoda, M.

( As ilomar )

,

Sugawar a, 125(1 969

)

T. Saito, H. Mi yase

;

PICNS- 69

69Sh7 K. Shoda, M.

( As i lomar )

,

Sugawar a,

131 (1969)

T. Sait o. H. Miya se

;

PICNS-69

69Sh8 K. Shoda, M.

( As i lomar ) , Sugawara,137 ( 1969)

T. Saito, H, Mi yase

;

PICNS-69

69Si 1 H. E. Siefken, P. M. Cockburn, R . w. Krone

;

Nuc I . Phys

.

A128, 162 ( 1969)

69Si2 I. Sick, E. B. Hughes, T. W. Donnelly, J. D. Walecka and

G. E. Walker; Phys. Rev. Letters 23, 1117 (1969)

69501 D. I. Sober, D. G. Cassel, A. J. Sadoff, K, W. Chen, P. A.

Crean; Phys. Rev. Letters 22, 430 (1969)

69502 Yu. I. Sorokin, V, G. Shevchenko, B. A. Yur ev; Yad. Fiz.

9, 254 (1969); Sov . J. Nucl . Phys. 9, 149 (1969)

69503 Yu . I. Sorokin, A. Kh. Shardanov, V. G. Shevchenko and

B. A. Yur ev; Izv Akad. Nauk. Fiz. 33, 721 (1969), Bull.

Acad. Sci. USSR-Phys. 33, 663 (1969)

69Stl R. J. J. Stewart, R. C. Morrison, D. E. Frederick; Phys.

Rev. Letters 23, 323 ( 1969)

69Tal G. G. Taran; Yad. Fiz. 10, 211 (1969), Sov. J. Nucl. Phys.

10, 119 ( 1 970 ) 69Thl H, Theissen, R, J. Peterson, W. J. Alston, III, J. R.

Stewart; Phys. Rev. 186, 1119 (1969)

69Til 6tto Titze; Z. Physik 220, 66 (1969)

107
59X12 Yu. I. Tltov, E. V. Stcpula, R. V. Akhmerov, S, A.

Byvalin, N. F. Severin, E. M, Smelov and L, D,

Yaroshevskli ; Yad. Fiz, 9, 1326 (1969); Sov. J, Nucl . Phys

9, 772 ( 1969 ) 69Tol M. Tomaselli, L. Grunbaum, G. A. Beer, H. G. Clerc, G, Wittwer; Phys. Letters 29B, 579 (1969)

69To2 Y, Torizuka, M. Oyamacta, K, Nakahara, K, Sugiyama, Y«

Kojima, T, Terasawa, K, Itoh, A, Yamaguchi, M, Klmura;

Phys. Rev. Letters 22, 544 (1969)

69To3 Y. Torlzuka, Y. Kojima, M. Oyamada, K. Nakahara, K.

Su^iyama, T. Terasawa, K. Itoh, A. Yamaguchi, M.

Kimura; Phys. Rev. 185, 1499 (1969)

69To4 Y, Torizuka, A. Yamaguchi, K. Nakahara, N. 6yamada,

T, Terasawa, K. Itoh, Y, Kojima and M, Kimura; Phys,

Rev. 188, 1745 (1969)

69Tsl H. Tsubota, N. Fujiwara, H. Ishimaru, E. Tanaka , T.

Aizawa, M. Kanazawa, N. Mutsuro; J. Phys. Soc. Japan

26, 1 ( 1969)

69U11 H. Ullrich, H. Krauth; Nucl. Phys. A123, 641 (1969)

69Val G. J. Vanpraet, P. Kossanyi; Z. Physik 222, 455 (1969)

69Va2 0. V. Vasilijev, G. N. Zalesny, S, F. Semenko, V. A,

Semenov; Phys. Letters 30B, 97 (1969)

69Va3 0. V. Vasil ev, G. N. Zalesnyi, S. F. Semenko, and V. A.

Semenov; Yad. Fiz. 10, 46C (1969), Sov. J. Nucl. Phys. 10,

263 ( 1970 ) 69Vel V. V. Verbinski, W. R. Burrus; Phys. Rev. 177, 1671

( 1969

)

69Ve2 A. Veyssiere, H, Beil, R. Bergere, P. Carlos; C. R. Acad.

Sc. Paris 268, 981 (1969)

69Wal Y. Wakuta, M, Sonada, A. Katase, H. Tawara, M.

Hyakutake; J. Phys. Soc. Japan 26, 851 ( 1969)

69¥rel D. V. Webb, E. G. Muirhead, B. M. Spicer; PICNS-69,

351 ( 1969 ) 69\»i 1 G. Wiechers, W. R. McMurray, I. J. Van Heerden; Nucl.

Phys. A124, 165 (1969)

69Wi2 G. Wittwer, H. G. Clerc, G. A. Beer; Phys. Letters 30B,

634 ( 1969 ) 69\*ul C. P. Wu, J. E. E. Baglin, F. W. K. Firk, T. W. Phillips;

Phys. Letters 29B, 359 ( 1969)

70Afl V. D. Afanas ev, N. G. Afanas ev, A. Yu. Buki, G. A.

Savitskii, V. M. Khvastunov, N. G. Shevchenko; Yad. Fiz.

12, 885 (1970); Sov. J. Nucl. Phys. 12, 480 (1971)

7CAhl J. Ahrens, H. Borchert, K. H. Czock, D. Mehlig and B.

Ziegler; Phys. Letters 31B, 57 0 (1970)

70Anl P. Antony-Spies, P. P. Delsanto, E, Spamer, A,

Goldmann and 6. Titze; Phys. Letters 31B, 632 (1970)

70An2 D. W. Anderson and S. C. Swift; Nucl. Phys. A150, 625

( 1970 ) 70An3 D. W. Anderson, A. J. Bureau, B. C, Cook, T, J. Englert,

R. E. Schramm; Nucl. Phys. A156, 74 (1970)

70An4 Yu. P. Antuf ev, V. B. Ganenko, V. S. Kuz menko, V. L.

Agranovich, I, I. Mi roshnichenko , V. M. Sanin, and P. V.

Sorokin; Yad. Fiz. 11, 948 (1970) Sov. J. Nucl. Phys. 11,

527 ( 1970 )

108
70An5

70Arl

70Ar2

70Aul

70Axl

70Bal

70Ba2

70Bel

70Be2

70Be3

7CBe4

70Be5

7CBe6

70Ee7

70Be8

70Be9

70B11

70Bol

70Bo2

70Bo3

70Bo4

70Br 1

70Bul

70Bu2

70Cel

70Col

S.

F i z ,

Phys. A147, 305 (1970)

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70Co2

TOCul

70Dal

70Del

70Di 1

7CDol

70Erl

7CEsl

70Fal

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70Ful

70Fu2

70Fu3

70Gal

70Gol

7CGo2

70Go3

70Go4

70Bel

70Be2

70Hil

70Bol

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70Hy 1 70 Isl

70 Is2

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70It2 K. Itoh, M. eyamada, Y. Torizuka; Phys. Rev. C2 , 2181

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70Me4

70Me5

70Me6

70»dol

70Mo2

70Wo3

70Mo4

70Mul

70ewl

70ew2

70Pel

70Pe2

70Pi 1 7 0Fal

70Ki 1

70£al

70Sa2

70Scl

7 0Sc2

7CSc3

70Sel

7 0 Shi

70Sh2

70Sh3

7 0 Sol

70So2

70St 1 70St2

70£ul

7C Szl

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70T12

7CTol

70To2

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7CVel

70Vol

70Vyl

70 Wal

70T»a2

70\^a3

70\*a4

70TVa5

701Vel

70\Vil

701*12

70Wol

70\»ul

70Wu2

70Yol

71 Adl

71 Ahl

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71 Anl

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71Cal P. Carlos, H. Beil, R. Bergere, A. Lepretre, A. Veyssiere;

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71Co2 S. Costa, L. Ferrero, L. Pasqualini, E. Mancini; Lettere al

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71Dal H. Dahncen, F. Dreyer, J. Staude and H. H. Thies; Nucl,

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71Di2 V. DiNapoli, F. Salvetti, H. G. DeCarvalho, J. Benuzzi

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71Gol N. V. Goncharov, A. I. Der ebchinski i , A. A. Zybalov, 0.

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Khvorostyan; Yad. Fiz. 14, 673 (1971); Sov. J. Nucl, Phys.

14, 377 ( 1972)

71Go2 N. V, Goncharov, A. I. De rebchinski i , 0. P. Konovalov, S.

G. Tonapetyan, V. M. Khvorostyan; Yad. Fiz. 14, 31 (1971)

Sov. J. Nucl. Phys.; 14, 18 (1972)

71Grl J. L. Groh, R. P. Singhal, H. S. Caplan, B. S. Dolbilkin;

Can. J. Phys. 49, 2743 (1971)

71Gr2 I. A. Grishaev, A. N. Krinitsyn, N. I. Lapin, V. I.

Nikiforov, G. D, Pugachev, B. I. Shramenko; Yad, Fiz. 14,

35 (1971); Sov, J, Nucl. Phys. 14, 20 (1972)

71Hal M. Hass, R, Moreh, D, Salzmann; Phys. Letters 36B, 68

( 1971 ) 71Ha2 P, E, Haustein, A, F, Voigt; J. Inorg. Nucl. Chem. 33, 289

( 1971

)

7 1 He 1 J, Heisenberg, J, S, McCarthy and I, Sick; Nucl. Phys.

A164, 353 ( 1971

)

71Hol Y. Horikawa, Y. Torizuka, A. Nakada, S. Mitsunobu, Y.

Kojima, M. Kimura; Phys. Letters 36B, 9 (1971)

71Igl A. V, Ignatyuk, N, S. Rabotnov, G. N. Smirenkin, A. S.

Soldatov, Yu, M, Tsipenyuk; Zh, Eksp. Teor, Fiz, 61, 12 84

(1971); Sov. Phys. JETP 34, 684 (1972)

71Isl B. S, Ishkhanov, I, M, Piskarev, I, M, Kapitonov, E. V.

Lazutin, V. S. Sopov, V. G, Shevchenko; Yad. Fiz. 13,

1141 (1971); Sov, J. Nucl, Phys, 13, 655 (1971)

71Is2 B. S, Ishkhanov, I, M, Kapitonov, I, M, Piskarev, 6, P.

Shevchenko; Yad. Fiz. 14, 27 (1971); Sov. J. Nucl. Phys.

14, 16 ( 1972 )

71Is3 B. S, Ishkhanov, I, M, Kapitonov, I. M, Piskarev, V, G,

Shevchenko; Yad. Fiz, 14, 253 (1971); Sov, J, Nucl, Phys,

14, 142 ( 1972)

71Jal H, E. Jackson, E, N, Strait; Phys. Rev. C4, 1314 ( 1971 )

115
71Ja2 H, E. Jackson, E, N. Strait; Statistical Properties of

Nuclei, ed, J, B, Garg, Plenum Publishing Corporation,

New York (1971) p. 601.

71Kel G, Kernel, W, M, Mason, U, Von Wimmersperg; Nucl,

Phys. A167, 352 (1971)

71Kil I. Kimura, S. A. flayashi, K, Kobayashi, S. Yamamoto, T.

Shibata; J. Nucl. Sci, and Tech. 8, 173 (1971)

71Kul H. M, Kuan, C. J. Umbarger and D, G. Shirk; Nucl. Phys.

A160, 211 (1971)

71Ku2 G. J, Kumbartzki, Ung Kim and Ch. K, Kwan; Nucl. Phys,

A160, 237 ( 1971

)

71Ku3 S. K. Kundu, Y. M. Shin, G. D. Wait; Nucl. Phys. A171,

384 ( 1 971

)

71Ku4 V. M, Kuznetsov, 6. I. Stukov, E. V. Repenko, V. D.

Epaneshnikov, V. N. Zabaev, A. P. Potylitsyn; Yad. Fiz.

13, 1052 (1971); Sov. J. Nucl. Phys. 13, 603 (1971)

71Ku5 G. Kumbartzki, U, Kim; Nucl. Phys. A176, 23 (1971)

71Lel A, Lepretre, H. Beil, R. Bergere, P. Carlos, A. Veyssiere;

Nucl. Phys. A175, 609 (1971)

71Lil G. C. Li, I. Sick, R. R. Whitney and M. E, Yearian; Nucl.

Phys. A162, 583 (1971)

71Li2 K, Lindgren and G, G. Jonsson; Nucl. Phys. A166, 643

( 1971

)

71Li3 S. C. Ling, S. L. Blatt; Nucl. Phys. A174, 375 (1971)

71Mal D. W. Madsen, L. S. Cardman,J. R. Legg, C. K.

Bockelman; Nucl. Phys.A168, 97 (1971)

71Ma2 J. Maly; Phys. Letters 35B, 148 (1971)

71Ma3 A. Manfredini, L. Fiore, C. Ramorino, W. Wolfli; Nuovo

Cimento 4A , 421 (1971)

7 1 Me 1 T. Methasiri and S. A. E. Johansson; Nucl. Phys. A167,

97 ( 1971 ) 71Me2 F. R. Metzger; Ann. Phys, 66, 697 (1971)

71Mil H. G. Miller, W. Buss, and J, A. Rawlins; Nucl. Phys.

Al 63, 637 ( 1 971

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71Mo2 K. Moreh, A. Nof, €». Shahal, A. Wolf; Phys. Letters 36B,

71 ( 197 1 ) 71Mo3 E. J. Moniz, I. Sick, R. R. Whitney, J. R. Ficenec, R. D.

Kephart, W. P. Trower; Phys. Rev. Letters 26, 445 ( 1971 ) 71Mo4 R. Moreh, A. Nof; Phys. Rev. C4, 2265 (1971)

71Mul K, M. Murray and M, E. Toms; Lettere al Nuovo Cimento

1, 571 ( 1971 ) 71Nal A, Nakada, Y, Torizuka, Y, Horikawa; Phys, Rev, Letters

27, 745 (1971); See Erratum- Phys. Rev, Letters 27, 1102

( 1971 ) 71Na2 M. Nagao, Y. Torizuka; Phys. Letters 37B, 383 (1971)

71Ne!l R. Neuhausen and R. M. Hutcheon; Nucl. Phys. A164,

497 ( 1 971 ) 71Pal B. H. Patrick, H. A. Medicus, G. K, Mehta, E. M. Bowey,

and D. B, Gayther; Phys. Letters 34B, 488 (1971)

71Pa2 D, Pavel, G, Ben-David, Y, Schlesinger, H, Szichman;

Nucl. Phys. A160, 409 (1971)

71Pa3 P. Paul, J. F. Amann , K. A. Snover; Phys, Rev. Letters

27, 10 13 ( 1971 )

116
71Pel K, A. Petrzhak, V. F. Teplykh, M, G. Pan yan, V. A,

Demin; Yad . Fiz, 14, 950 (1971); Sov. J. Nucl. Phys . 14, 532 ( 1972 ) 71P11 K. Pitthan and Th. Walcher; Phys. Letters 36B, 563 (1971)

71Fi2 M. Piiparinen, A, Anttila, M, Viitasalo; Z. Physik 247, 400

( 1971 ) 71Fal B. S. Ratner; ZhETF Pis. Red. 13, 628 (1971); JETP

Letters 13, 447 (1971)

71i;il F. Riess, W. J, 6 Connell, P. Paul; Nucl, Phys. A175, 462

( 1971

)

71Sal Tatsuya Saito; Nippon Kagaku Zasshi 92, 164 (1971)

71Sa2 Tatsuya Saito; Bull, Chem, Soc, Japan 44, 1800 (1971)

7 1 Sc 1 B, L, Schrock, R, P, Haddock, J, A, Helland, M. J, Longo

S, S, Wilson, K, K, Young, D. Cheng, V, Perez-Mendez

;

Phys. Rev. Letters 26, 1659 (1971)

71Sc2 M. Schaeffer, M. Suff ert , D. Magnac-Vale tte; Nucl, Phys, A175, 217 ( 1971 ) 71Shl Y, M. Shin, C. F. Wong, H. S. Caplan; Nucl. Phys. A166,

162 ( 1971 ) 71Sh2 K. Shoda, A, Suzuki, M. Sugawara, T. Saito, H. Miyase

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71Sh3 K. Shoda, T. Saito, M, Sugawara, H. Miyase, S. 6ikawa,

A. Suzuki; Phys, Rev. C4 , 1842 (1971)

71Sh4 A. Shapiro, W. F. Stubbins; Nucl. Sci. and Engr. 45, 47

( 1971 ) 71 Sh5 T. Shintomi, C. Yamaguchi, M. Masuda; J. Phys. Soc.

Japan 3 1, 1297 ( 1971 ) 71Sh6 Yu. K. Shubnyi, Yu . A. Lysikov; Izv. Akad, Nauk SSSR

Fiz, 35, 1651 ( 1971

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71Sil J. J. Simpson, W. R. Dixon, R. S. Storey; Phys. Rev. C4,

443 ( 1971

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71Snl K. A, Snover, J. M, McDonald, D, B, Fossan; Phys, Rev,

C4, 398 ( 1 971

)

71Sn2 K, A, Snover, J. F. Amann, W. Bering, P, Paul; Phys,

Letters 37B, 29 (1971)

71Sol Yu, I, Sorokin, V, A, Khrushchev, B, A, Yur ev; Yad, Fiz,

14, 1118 (1971); Sov, J, Nucl, Phys, 14, 622 (1971)

71S»1 C, P, Swann; Nucl, Phys, A167, 201 (1971)

71Sw2 C, P, Swann; Phys. Rev. C4, 1489 ( 1971 ) 71Sw3 C. P. Swann; Nucl. Phys. A172, 569 (1971)

71Tal B. Tamain, B. Pfeiffer, H. Wollnik, E. konecny; Nucl.

Phys. A173, 465 (1971)

71111 K. Tietze, H. Riech and J. 6. Trier; Z, Physik 242, 328

( 1971 ) 71llml C. J. Umbarger, D, A, Close, W, L, Sievers, and R, C,

Bearse; Phys. Rev, C3, 199 ( 1971 )

71Val A. van der Woude , M, L. Halbert, C, R. Bingham, and B.

D. Belt; Phys. Rev. Letters 26, 909 (1971)

71Va2 6. V. Vasil ev, V. A. Semenov, S. f. Semenko; Yad. Fiz.

13, 463 (1971); Sov. J. Nucl. Phys. 13, 259 (1971)

71Va3 G. J. C. Van Niftrik, L. Lapikas, H, DeVries, G, Box;

Nucl, Phys, A174, 173 (1971)

117
71 Va4-

71 Vel

71 VI

1

7 1 Vol

71 Wal

71 \»el

71 We2

71 Wol

71 yal

71 Ya2

71 Zhl

72A14

72An2

72An3

72Arl

72Ba5

72Bel

72Be2

72Be3

72Bc7

72BV6

72Br8

72Br4

G, A, Vartapctyan, N, A, Demekhina, V, I, Kasilov, Yu,

N. Kanyuk, P. V, Sorokin, A, G. Khudaverdyan ; Yad, Fiz.

14, 65 (1971); Sov. J. Nucl. Phys. 14, 37 (1972)

E. Ventura, C. C. Chang, W, E, Meyerhof; Nucl, Phys.

A173, 1 ( 1971 ) V. G, Vlasenko, N. G. Afanas ev, V, a. Got dshtein, S.

Dementll, E. L. Kuplennikov; Yad. Fiz. 13, 259 (1971);

Sov. J. Nucl. Phys. 13, 144 (1971)

H. J. Von Eyss, H, Schier, B. Schoch; Elba-71,

Tagungsber icht Elektronen Besc hleuniger Arbeits

Gruppen ; (Sept. 1971) Justus L iebig-Univer si ta t Giessen.

Yoshihisa Wakuta; J. Phys. Soc , Japan 31, 12 (1971)

D. V, Webb, E. G. Muirhead, B. M, Spicer; Nucl. Phys.

A17 1, 324 ( 1971 ) B. Weissman and H. L. Schultz; Nucl. Phys. A174, 129

( 1971

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M. E. Wormald, I. F. Wright;

and Nuclei; 2, 168 (1971)

C. S. Yang, E. L. Tomusiak,

Nucl. Phys. A162, 71 (1971)

A. Yamaguchi, T. Terasawa, K. Nakahara, and

Torizuka; Phys. Rev. C3, 1750 ( 1971 ) E. A. Zhagrov, Yu. A. Nemilov, N, V.

Selitskii; Yad. Fiz. 13, 934 (1971);

537 ( 1971 ) T. K. Alexander, B. Y. Underwood, N.

A. Jelley, J. Szucs, S. P. Dolan, M.

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R. A. Anderl, J.

V. Yester, D. J,

10 1 ( 1972 )

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Reprinted from

R. K. Gupta, H,

Particles

S. Caplan;

Y.

Nikitina, Yu. A.

Sov. J. Nucl. Phys. 13,

Anyas-Weiss, N.

R. Wormald, K. W.

E. Hall, R. C. Morrison, R. G. Struss, M.

Zaffarano; Nucl. Instr. and Methods 102,

ev. V. L. Agranovich, V. B« Ganenko, V, S.

Miroshnichenko, P. V. Sorokin, S. V,

Fiz. 15, 643 (1972); Sov. J. Nucl. Phys

Yu. P. Antuf

Kuz menko, I . I

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Shalatskii; Yad.

357 ( 1972 ) B, Arad, G. Ben-David, Y. Schlesinger, M, Hass; Phys.

Rev. C6, 670 ( 1972

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C, Bacci, R. Baldi ni -Ce 1 io, B. Esposito, C. Mencuccini,

A. Reale, G. Sciacca, M. Spinetti, A. Zallo; Lettere al

Nuovo Cimento 4, 5 ( 1972

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G. Graham, J, V. Thompson; Nucl. Phys

15,

I. Bell, I

408 ( 1972 ) Berman, F.

791 ( 1972

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W. K. Firk, C, P. Wu; Nucl. Phys.

R. A.

A179,

B. L.

A179,

W. Bertozzi, T. Cooper, N. Ensslin, J. Heisenberg, S.

Kowalski, M. Mills, W. Turchinetz, C. Williamson, S. P.

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Letters 28, 1711 (1972)

I. Bergqvist, D. M. Drake, D. K, McDaniels; Nucl. Phys.

A19 1 , 641 ( 1 972 ) K. J. Moon, D.

3 S. L. Blatt,

( 1972

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R. L, Bramblett, T. Gozani,

Rundquist; Nucl, Technology

C. Brassard, H, D, Shay, J,

Bromley; Phys. Rev, C6, 53

Kohler; Phys. Rev. C6, 1536

R. 6. Ginaven, D, E.

13, 33 ( 1972 ) P. Coffin, W. scholz,

( 1972 ) D. A.

118
72Chl

7 2Ch3

72Co2

72Da6

72De3

72De4

72Dol

72Dr2

72Dr5

72Esl

72Fal

72Fa3

72Fr4

72Fr5

72Fu2

72Ga2

72Ge3

72G11

72Hal

72Ha2

72Ha3

72Isl

72Jal

72Ka5

72Ke4

72Khl

A, Chevallier, E, Bozek, J, Chevallier, A, Pape, R.

Armbruster; Nuc I . Phys. A191, 20 1 (1972)

C. C, Chang, E. M, Diener, E, Ventura; Phys. Pev,

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A, Meyer, D. Reitmann; Nucl. Phys.

Letters 29, 307 (1972)

Coetzee, M.

644 ( 1 972 ) W. F.Al 85,

P. David, J. Debrus, U . Kim, G. Kumbartzki, H.

Mommsen, W. Soyez, K, H, Speidel, G, Stein; Nucl.

A197, 163 ( 1972

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T. K, Deague, R. J. J. Stewart; Nucl. Phys. A191,

( 1972

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Phys.

305

Phys ,

Staude, H.

Staude, H

V. P. Denisov, L. A. Kul chitskii,

Fiz. 14, 889 (1971); Sov. J. Nucl.

W. F. Dodge, J, J, Murphy, II;

( 1972)

F. Dreyer, H. Dahmen, J.

Phys. A181, 477 (1972)

F. Dreyer, H, Dahmen, J.

Phys. A192, 433 (1972)

M. A. Eswaran, M. Ismail,

C5, 1270 ( 1972

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L. ^. Fagg, W, L. Bendel,

F. Kaiser; Phys. Rev, C5,

Rev . C5, 1 143 ( 1 972 ) F. L. Fabbri, P. Picozza, Cimento 3, 63 (1972)

D. L. Friesel, T, J. Lewis,

846 ( 1972

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J. Friedrich; Nucl.

T. Fujii, S. Homma,

Takasaki, T. Kondo,

I, Ya. Chubukov; Yad

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Phys. 14, 497 (1972)

Rev. Letters 28, 839

H, Thies; Nucl.

H. Thies; Nucl.

N, L. Ragoowansi; Phys. Rev.

E, C. Jones, Jr., L. Cohen, H.

120 (1972) See Erratum - Phys.

C, Schaerf; Lett ere al Nuovo

W. C. Miller; Phys. Rev, C6

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A191

Kato, H, 6kuno, F,

I. Endo, H. Fujii;

B. Isabelle; Nucl.

Phys

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Phys.

C.

Phys. A191, 118 (1972)

K, Huke, S

S. Yamada,

Rev. Letters 28, 1672 (1972)

D. Ganichot, B. Grossetete, D,

A178, 545 ( 1972

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R. Gellie, K. H. Lokan, N. K. Sherman, R. G.

Johnson, J. I. Lodge; Can. J. Phys. 50, 1689 (1972)

H. F. Glavish, S. S. Hanna, R. Avida, R. N. Boyd, C,

Chang, E. Diener; Phys. Rev, Letters 28, 766 (1972)

M. Hasinoff, D, Johnson, D, F, Measday; Phys, Letters

39B, 506 ( 1972 ) M, L, Halbert, E, K, Warburton; Proceedings of

International Conference on Few Particle Problems in the

Nuclear Interaction; UCLA (Aug, 28-Sept, 1, 1972)

M. Hasinoff, G. A. Fisher, P. Kurjan, S. S. Hanna; Nucl.

Phys. A195, 78 (1972)

B, S, Ishkhanov, I. M. Kapitonov, E. V. Lazutin, I. M,

Piskarev, V. G. Shevchenko; Nucl. Phys, A186, 438 (1972)

H, E, Jackson, K, J, Wetzel; Phys, Rev. Letters 28, 513

( 1972 ) V. I. Kasilov, A, V, Mi trof anova, Yu, N. Ranyuk, P. V.

Sorokin; Yad. Fiz. 15, 406 (1972); Sov. J. Nucl. Phys. 15

228 ( 1972 ) N, A, Keller and

( 1972

)

A. M. Khan, J, W

D, B. McConnell; Can. J. Phys, 50, 1554

Knowles; Nucl, Phys, A179, 333 (1972)

119
72K12 H. T. King, W. E. Meyerhof, R. G, Hirko; Nuci. Phys.

A178, 337 ( 1 972

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72Kr3 I. Kroon, B. Forkman; Nucl . Phys. A179, 141 (1972)

72Ku6 G. Kuhl, U. Kneissl; Nucl. Phys. A195, 559 (1972)

72Lil J. W. Lightbody Jr.; Phys. Letters 38B, 475 (1972)

72Lo2 K. H. Lokan, N. K. Sherman, R, W. Gellie, J. W. Jury, J.

I, Lodge, R. G. Johnson; Phys. Rev. Letters 28, 1526

( 1972 ) 72Mal 6. Y, Mafra, S. Kuniyoshi, J. Goldemberg; Nucl. Phys.

Al 86, 1 10 ( 1972

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72Ma2 D. J. Martin, J. R. Leslie, W. McLatchie, C. F. Monahan,

L. E. Carlson; Nucl. Phys. A187, 337 (1972)

72Me3 F. R. Metzger; Nucl. Phys. A189, 409 (1972)

72Wi4 S. Mitsunohu and Y. Torizuka; Phys, Rev. Letters 28, 920

( 1972)

72Nal A. Nakada and Y. Torizuka; J. Phys. Soc . Japan 32, 1

( 1972)

72Na2 R. Nath, F. W. K, Firk, H. L. Schultz; Nucl. Phys. A194,

49 ( 1972)

72No3 V. I. Noga, Yu. N. Ranyuk, P. V. Sorokin, V. A.

Tkachenko; Yad. Fiz. 14, 904 (1971); Sov. J. Nucl. Phys.

14, 506 ( 1 972

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72edl Y. 6da, M. Kondo, H. Hirabayashi; J. Phys, Soc, Japan

32, 869 ( 1972)

72ef2 N. M. 0 Fallon, L. J. Koester,Jr., J, H. Smith; Phys. Rev.

C5, 1926 ( 1972

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72Phl G. W. Phillips, P. Richard, D, 0, Elliott, F. F, Hopkins,

A. C. Porter; Phys. Rev. C5, 297 (1972)

72Ea2 J. J. Ramirez, R. A. Blue, H. R. Weller; Phys, Rev, C5

17, ( 1972 ) 721Ro3 D, e, Rogers, R, P, Beukens, W. T. Diamond; Can. J.

Phys. 50, 2428 (1972)

72Rul J. P. Russell, W. E. Taylor, F. E. Dunnam, H. A. Van

Rinsvelt; Nucl. Phys. A187, 449 (1972)

72Sc5 B. Schroder, B. Nordgren, A. Aim; Nucl. Phys. A193, 555

( 1972 ) 72Sh2 N. Shikazono and Y. Kawarasaki ; Nucl. Phys. A188, 46 1

( 1972

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72Skl D. M. Skopik, Y, M. Shin; Can. J. Phys. 50, 392 (1972)

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72£k6 N. A. Skakun, N. P. Dikii; Yad. Fiz. 15, 615 (1972); Sov.

J, Nucl, Phys. 15, 341 (1972)

72Sk7 D. M. Skopik, Y. M. Shin, J. W. Horniachek, S. K.

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72Su4 M. Sugawara, K. Shoda, T. Saito, H. Miyase, A, Suzuki,

S. eikawa, R. Bergere; Phys. Rev. C5, 1705 (1972)

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A196, 89 ( 1972

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J. Nucl. Phys. 15, 361 (1972)

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72To3 Z. B, du Toit, P, R, de Kock, J. H, Hough, W, L, Mouton

;

Z. Physik 255, 97 (1972)

120
72Va2 R. E. Van de Vyver, H. Ferdinande, G. Knuyt, R.

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72\il M, Viitasalo, M. Pilparinen, A. Anttila; Z. Physik 250, 387

( 1972

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( 1972

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72\ile2 H. R. Weller, R. A. Blue, E. M. Bernstein, J. J. Ramirez;

Nucl. Phys. A185, 284 (1972)

121
6. Definitions of Abbreviations and Symbols

6.1. Symbols Used to Define Incoming Beam and Reaction Products

A

D

E

E/

E+

F

G

G/

HE

MU-T

N

P

PI

SN

SPL

T

XN

XP

XXX

alpha particle

deuteron

electron

inelastically scattered electron

positron

fission

pho ton

inelastically scattered photon

3

He particle

used only in combination G,MU-T to indicate a total photon

absorption cross section measurement

neutron

proton

pi on

sum of neutron-producing reactions

spallation

triton

all neutrons, total neutron yield

all protons, total proton yield

reaction products defined in REMARKS

6.2. Symbols and Abbreviations (Table 1 and Data Index - Columns 4-7 and REMARKS

nuclear mass number

absolute integrated cross-section data /cdE

absolute cross-section data

absolute yield data

measurement of radioactivity of the target

A

ABI

ABX

ABY

ACT

ANG angle. Symbols listed under ANG indicate type of angular

distribution data available for a reaction.

BBL bubble chamber

B(EL) reduced radiative transition probability

BF3 BF3 neutron counter with moderator, e.g., Halpern detector,

long counter

BREAKS levels located by "breaks" in the yield curve

C continuous. Used to describe a photon source or a detector

response function. Contrast with D = discrete.

CCH cloud chamber

CF compared with

GOING coincidence

D deuteron

122
6.2. Symbols and Abbreviations (Continued)

D discrete. Used to describe a photoii source or a detector

response function. Contrast with C = continuous.

DEL delta, full width of cross-section curve at half maximum^ May

also be width of Lorentz line fit to crass-section curve. DST an angular distribution was measured

DT BAL detail balance

E energy. Usually energy at which cross-section curve peaks

or resonance energy of Lorentz line fit,

EMU emulsions (photographic plates)

EXCIT excitation. Usually the excitation energy of the nucleus

in which a gamma-ray transition is ^aade.

F fission

FMF form factor

G-WIDTH r , gamma-ray transition width

INT interaction or type of reaction

ION ionization chamber

J-PI spin and parity assignments of levels are made

LFT excited state lifetime

MAG magnetic spectrometer

MGC magnetic Compton spectrometer

MGP magnetic pair spectrometer

MOD moderated neutron detector not employing a BF3 gounter,

e,g,, rhodium foil, Szilard-Chalmers reaction. He, Li

reactions, Gd loaded liquid scintillator, etc.

MSP mass spectrometer

N neutron

N+P neutron plus proton. Usually means the sum of the (y,n)

and (y,p) reactions.

NAI Nal(Tl) spectrometer

NOX no cross-section data

NUM number. The acquisition number for data available in the

digitized cross-section library of the Photonuclear Data

Center.

P proton

PI pion

POL polarization

Q-SQUARE momentum transfer squared (q^)

REF reference. The bibliographic reference number assigned to a paper by the Photonuclear Data Center.

REL relative

RES result. Symbols listed under RES indicate type of measure- ment made for a given reaction.

RLI relative integrated cross-section data

RLX relative cross-section data

123
6.2. Symbols and Abbreviations (Continued)

RLY relative yield data

SCD semiconductor (solid state) detector

SCI scintillator detector other than Nal, e.g., Csl, KI,

organic (liquid or solid), stilbene, He

SEP ISOTP separated isotope used

SIG cross section. The maximum value of the cross section as

a function of photon energy.

SIG-0 (Sq

SIG-1 {y_j

SN used alone or as cr(SN)/cr(y, SN)

(J(SN) = cr(y,n) + cJ(y,np) + cy(y,2n) + (?(y,3n) + . . .

SNF used alone or as cf(SNF)/cr(y, SNF)

(J(SNF) = cy(SN) + <J(y,f)

SPC photon or particle energy spectrum

SPK spark chamber

T triton

TEL counter telescope

THR threshold detector, e.g., ^® Si(n,p)^® Al

TOF time-of-f light detector

TOT total nuclear absorption cross section for photons

TRK tracks of particles or fragments observed in solid

materials (glass, mylar, etc.)

XN all neutrons. Used alone or as <J(XN)/(?( y,XN)

cr(XN) = (J(y,n) + <j(y,np) + 2(J(y,n) . . . + r)Cl{y,f) + . . . XP all photons. Used alone or as tf(XP)/cr( y,XP)

(J(XP) = cf(y,p) + (J(y,np) + 2cJ(y,p) + . . »

Z atomic number (number of protons)

4PI a 4n geometry was used or a method like radioactivity

or a total absorption measurement

999 energy defined In REMARKS

$ indicates the measurement involved either beams or targets that were polarized/aligned, or that the polarization of the reaction

products was determined

124
7. References

[l] J. Chadwick and M. Goldhaber, Nature 134, 237 (1934).

[2] D. W. Kerst, Phys. Rev. 58_, 841 (1940).

[3] G. C. Baldwin and G. S. Klaiber, Phys. Rev. _71, 3 (1947); Phys. Rev. T^, 1136 (1948).

[4] C. Schuhl and C. Tzara, Nucl. Instr. & Methods 10, 217 (1961); C. P. Jupiter,

N. E. Hanson, R. E. Shafer, S. C. Fultz, Phys. Rev. 1_21, 866 (1961)«

[5] W. C. Barber, Ann. Rev. Mod. Sci. 12, I (1962).

[5] J. S. Levinger and H. A. Bethe, Phys. Rev. ]_&, 115 (1930).

[7] B. M. Spicer, The Giant Dipole Resonance , In Advances in Nuclear Physics, Vol. 2

(Plenum Press, 1969); Evans Hayward, Photonuclear Reactions , NBS Monograph 118 , August 1970; F. W. K. Firk, Low- Energy Photonuclear Reactions , in Ann. Rev. Nucl.

Sci., Vol. 20, 1970.

[8] J. S. Levinger, Nuclear Pho todisintegration, Oxford University Press (1960).

[9] N. V. Baggett, T. M. Collins, E. G. Fuller, J» C. Holland, J. H. Hubbell, and

J. S. O'Connell, Photonuclear Data Index , (1955-1965), NBS Misc. Publ. 277 , April 1966; T. M. Collins, Eo G. Fuller, J. D. Murphy, and J. S. O'Connell,

Photonuclear Data Index (January 1965 through April 1967), NBS Misc. Publ. 277 - Supplement 1, October 1967; E. G. Fuller, H. M. Gerstenberg, and T. M. Collins,

Photonuclear Data Index (1965-1970), NBS Spec. Publ. 322, May 1970.

[10] Gladys Fuller, 1959 Nuclear Data Tables (NUCLEAR DATA PROJECT) - National Academy

of Sciences, National Research Council, Washington, D. C.

[11] A. H. Wapstra and N. B. Gove, Nuclear Data Tables , 9_, 303 ( 1971).

'-• U. S. GOVERNMENT PRINTING OFFICE : 1 973 —51 1 -323

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Photonuclear Reaction Data, 1973.

5. Publication Date March 1973

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7. AUTHOR(S) E. G. Fuller, H. M. Gerstenberg, H. Vander Molen,

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A brief summary is given of the available data on the gross features of the

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17. KEY WORDS (Alphabetical order, separated by semicolons) Bibliography; data index; data Summary;

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