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