ENTRY C2398 20220130 C215C239800000001
SUBENT C2398001 20220130 C215C239800100001
BIB 9 25 C239800100002
TITLE The 136Xe + 198Pt reaction: A test of models of C239800100003
multi-nucleon transfer reactions C239800100004
AUTHOR (V.V.Desai,W.Loveland,K.McCaleb,R.Yanez,G.Lane, C239800100005
S.S.Hota,M.W.Reed,H.Watanabe,S.Zhu,K.Auranen, C239800100006
A.D.Ayangeakaa,M.P.Carpenter,J.P.Greene,F.G.Kondev, C239800100007
D.Seweryniak,R.V.F.Janssens,P.A.Copp) C239800100008
INSTITUTE (1USAORU,3AULCBR,1USAANL,1USANCA,1USATNL,1USADKE, C239800100009
1USALTI) C239800100010
REFERENCE (J,PR/C,99,044604,2019) C239800100011
FACILITY (LINAC,1USAANL) C239800100012
SAMPLE (78-PT-198,ENR=0.95) C239800100013
(78-PT-196,ENR=0.0284) C239800100014
(78-PT-195,ENR=0.0123) C239800100015
(78-PT-194,ENR=0.009) C239800100016
Sandwiched target consisting of C239800100017
-3.2 mg/cm2 198Pt foil C239800100018
-4.0 mg/cm2 198Pt foil C239800100019
-24 mg/cm2 197Au stopper foil. C239800100020
DETECTOR (HPGE) Well-calibrated Ge detector in the Center for C239800100021
Accelerator Target Science Counting Laboratory. C239800100022
METHOD (ACTIV) Activation method was used. The length of the C239800100023
irradiation was 28.3 h. The total observation period C239800100024
was 5 days, during which 19 measurements of target C239800100025
radioactivity were made. C239800100026
HISTORY (20220130C) Compiled by S.H. C239800100027
ENDBIB 25 0 C239800100028
NOCOMMON 0 0 C239800100029
ENDSUBENT 28 0 C239800199999
SUBENT C2398002 20220130 C215C239800200001
BIB 4 17 C239800200002
REACTION 1(78-PT-198(54-XE-136,F)ELEM/MASS,CUM,SIG) C239800200003
2(78-PT-198(54-XE-136,F)ELEM/MASS,,SIG) C239800200004
ANALYSIS The primary experimental data are cumulative yields, C239800200005
represented by cumulative cross sections. It was C239800200006
assumed that the charge distributions of neighboring C239800200007
isobaric chains are similar and radionuclide yields C239800200008
from a limited mass region can be used to determine a C239800200009
single charge distribution curve for that mass C239800200010
region. Then laws of radioactive decay was used to C239800200011
iteratively correct the measured cumulative formation C239800200012
cross sections for precursor decay to obtain C239800200013
independent cross sections. C239800200014
ERR-ANALYS (DATA-ERR) Origin of uncertainties not specified C239800200015
(ERR-SYS) Systematic uncertainty in calculation of C239800200016
independent yield C239800200017
STATUS (TABLE) Data taken from tab. 1,2 of the C239800200018
reference C239800200019
ENDBIB 17 0 C239800200020
COMMON 2 3 C239800200021
EN-CM ERR-SYS C239800200022
MEV PER-CENT C239800200023
451.0 30. C239800200024
ENDCOMMON 3 0 C239800200025
DATA 7 78 C239800200026
ELEMENT MASS ISOMER DATA 1DATA-ERR 1DATA 2C239800200027
DATA-ERR 2 C239800200028
NO-DIM NO-DIM NO-DIM MB MB MB C239800200029
MB C239800200030
19. 43. 0.535 0.106 0.452C239800200031
0.09 C239800200032
30. 69. 1. 0.0744 0.048 0.0744C239800200033
0.048 C239800200034
30. 72. 0.287 0.082 0.287C239800200035
0.082 C239800200036
31. 73. 2.22 0.28 2.22C239800200037
0.28 C239800200038
33. 72. 0.23 0.02 0.23C239800200039
0.02 C239800200040
40. 97. 0.36 0.03 0.36C239800200041
0.03 C239800200042
41. 96. 0.99 0.02 0.99C239800200043
0.02 C239800200044
42. 99. 0.81 0.04 0.81C239800200045
0.04 C239800200046
43. 99. 1. 0.71 0.26 0.56C239800200047
0.21 C239800200048
45. 105. 1.26 0.21 0.58C239800200049
0.1 C239800200050
46. 112. 1.11 0.11 1.11C239800200051
0.11 C239800200052
49. 110. 1.87 0.02 1.87C239800200053
0.02 C239800200054
49. 115. 1. 2.59 0.068 1.73C239800200055
0.45 C239800200056
51. 120. 1. 0.374 0.048 0.374C239800200057
0.048 C239800200058
51. 122. 1.652 0.033 1.652C239800200059
0.033 C239800200060
51. 126. 1.42 0.21 1.42C239800200061
0.21 C239800200062
51. 127. 2.15 0.28 1.83C239800200063
0.24 C239800200064
51. 128. 0.82 0.07 0.72C239800200065
0.07 C239800200066
52. 131. 1. 1.43 0.31 1.43C239800200067
0.31 C239800200068
53. 124. 1.2 0.05 1.2C239800200069
0.05 C239800200070
53. 130. 9.75 0.04 9.75C239800200071
0.04 C239800200072
53. 131. 18.2 0.5 15.3C239800200073
1.5 C239800200074
53. 132. 8.13 0.29 7.97C239800200075
0.8 C239800200076
53. 133. 16. 0.1 14.6C239800200077
1.4 C239800200078
53. 135. 4.63 0.42 4.63C239800200079
0.42 C239800200080
54. 125. 0.87 0.5 0.79C239800200081
0.46 C239800200082
54. 127. 2.61 0.43 2.24C239800200083
0.36 C239800200084
54. 133. 1. 23.2 0.4 21.9C239800200085
2.2 C239800200086
54. 135. 176. 1.4 164.5C239800200087
16.5 C239800200088
55. 127. 2.5 0.78 2.31C239800200089
0.72 C239800200090
55. 131. 1.1 0.2 0.96C239800200091
0.2 C239800200092
55. 132. 11.9 0.2 11.9C239800200093
1.2 C239800200094
55. 136. 15.5 0.4 15.5C239800200095
1.6 C239800200096
56. 135. 1. 12.5 0.2 12.5C239800200097
1.3 C239800200098
56. 140. 11.95 0.01 10.6C239800200099
1. C239800200100
57. 140. 2.29 0.06 2.28C239800200101
0.23 C239800200102
58. 143. 4.21 0.08 3.56C239800200103
0.36 C239800200104
59. 142. 7.9 2.2 7.9C239800200105
2.2 C239800200106
62. 153. 0.96 0.2 0.78C239800200107
0.16 C239800200108
65. 154. 1.92 0.11 1.25C239800200109
0.13 C239800200110
66. 157. 1.65 0.09 1.39C239800200111
0.14 C239800200112
71. 169. 1.7 1. 1.7C239800200113
1. C239800200114
72. 173. 0.72 0.02 0.63C239800200115
0.06 C239800200116
72. 175. 2.51 0.47 1.88C239800200117
0.35 C239800200118
72. 180. 1. 0.65 0.22 0.65C239800200119
0.22 C239800200120
73. 176. 1.35 1.18 1.2C239800200121
1.05 C239800200122
73. 177. 2.1 1.9 1.8C239800200123
1.6 C239800200124
73. 184. 0.82 0.02 0.73C239800200125
0.07 C239800200126
75. 181. 1.73 0.78 1.53C239800200127
0.69 C239800200128
75. 182. 8.26 2.38 8.19C239800200129
2.43 C239800200130
75. 188. 7.77 0.58 7.77C239800200131
0.58 C239800200132
75. 189. 17.5 0.9 14.8C239800200133
1.4 C239800200134
76. 182. 1.01 0.16 0.95C239800200135
0.15 C239800200136
76. 183. 0.83 0.04 0.47C239800200137
0.05 C239800200138
77. 188. 4.28 0.94 4.25C239800200139
0.93 C239800200140
77. 190. 3.11 0.03 1.67C239800200141
0.17 C239800200142
77. 194. 3.18 1.25 3.18C239800200143
1.25 C239800200144
77. 195. 1. 17.8 1.9 17.8C239800200145
1.9 C239800200146
77. 196. 1. 7.57 0.11 7.57C239800200147
0.76 C239800200148
78. 191. 5.6 0.01 4.5C239800200149
0.45 C239800200150
78. 195. 1. 26.5 5.7 20.C239800200151
4.3 C239800200152
79. 193. 15.4 9. 13.4C239800200153
7.8 C239800200154
79. 194. 6.4 0.1 6.4C239800200155
0.6 C239800200156
79. 196. 1. 115.3 0.5 115.3C239800200157
11.5 C239800200158
79. 198. 17.6 0.3 16.5C239800200159
1.5 C239800200160
79. 199. 205.6 0.6 168.8C239800200161
16.9 C239800200162
79. 200. 1. 1.79 0.08 1.79C239800200163
0.18 C239800200164
80. 195. 1. 3.4 0.1 2.9C239800200165
0.3 C239800200166
80. 197. 6.99 0.78 5.82C239800200167
0.65 C239800200168
80. 203. 19.9 0.8 17.5C239800200169
1.7 C239800200170
81. 200. 6.2 0.9 5.2C239800200171
0.8 C239800200172
81. 201. 6.8 0.5 5.C239800200173
0.5 C239800200174
81. 202. 1.4 0.03 1.4C239800200175
0.14 C239800200176
82. 200. 4.7 0.2 3.8C239800200177
0.4 C239800200178
82. 201. 4.4 0.2 3.3C239800200179
0.3 C239800200180
82. 202. 1. 6.2 0.3 6.2C239800200181
0.6 C239800200182
82. 203. 3.9 0.03 2.9C239800200183
0.3 C239800200184
83. 204. 0.88 0.02 0.66C239800200185
0.07 C239800200186
ENDDATA 160 0 C239800200187
ENDSUBENT 186 0 C239800299999
ENDENTRY 2 0 C239899999999