ENTRY O0499 19991117 0000O049900000001 SUBENT O0499001 19991117 0000O049900100001 BIB 12 28 O049900100002 TITLE Isotopic Product Distributions in the Near Symmetric O049900100003 Mass Region in Proton Induced Fission of U-238. O049900100004 AUTHOR (P.P.JAUHO,A.JOKINEN,M.LEINO,J.M.PARMONEN,H.PENTTILA, O049900100005 J.AYSTO,K.ESKOLA,V.A.RUBCHENYA) O049900100006 INSTITUTE (2SF JYV) O049900100007 (2SF HLS) O049900100008 (4RUSRI ) O049900100009 REFERENCE (J,PR/C,49,2036,1994) O049900100010 HISTORY (19990119C) O049900100011 (19990511U) Last checking has been done. O049900100012 (19991117A) DATE is corrected O049900100013 SAMPLE The 10.0 mg/cm**2 Natural Uranium Target Which is O049900100014 Basically Composed of U-238 was Used. O049900100015 The Uranium Target was Covered with a 0.2 mg/cm**2 O049900100016 Aluminum Foil on Both Sides. O049900100017 ADD-RES (COMP).Theoretical Model For Calculating Mass and O049900100018 Independent Yields. O049900100019 COMMENT /by Authors/. Due to the Large Initial Energy Only a O049900100020 Small Fraction of Fission Fragments, I.E., About 1%,areO049900100021 Stopped in Helium in Our Set Up. O049900100022 DETECTOR (TELES,SOLST,SOLST,SOLST,SOLST). The Counting Setup O049900100023 Composed of a 50% Ge Detector,a Planar 10 mm Thick Ge O049900100024 X-Ray Detector,a 1 mm Thick Plastic Delta E Detector O049900100025 Positioned in Front of the Large Ge Detector. O049900100026 FACILITY (CYCLO,2SF JYV) The New Heavy Ion Cyclotron, Jyvaskyla.O049900100027 METHOD (OLMS) The on-Line Mass Separator Igisol. O049900100028 (BCINT) O049900100029 STATUS (TABLE) O049900100030 ENDBIB 28 0 O049900100031 NOCOMMON 0 0 O049900100032 ENDSUBENT 31 0 O049900199999 SUBENT O0499002 19991117 0000O049900200001 BIB 4 9 O049900200002 REACTION (92-U-238(P,X)ELEM/MASS,,PY) O049900200003 ERR-ANALYS (ERR-T).The Uncertainty is Reported by Authors. O049900200004 The Errors Include 10% Uncertainty in the Efficiency O049900200005 Calibration and the Statistical Error. O049900200006 FLAG (1.).The Values are Lowest Limits Only Due to the O049900200007 Uncertainty in the Branching Ratio. O049900200008 MISC-COL (MISC).The Author'S (ATOMS/MUC)Data were Recalculated O049900200009 By Compiler in Unit Nuc/Part. O049900200010 (MISC-ERR).'Misc' Uncertainty. O049900200011 ENDBIB 9 0 O049900200012 COMMON 1 3 O049900200013 EN O049900200014 MEV O049900200015 19.8 O049900200016 ENDCOMMON 3 0 O049900200017 DATA 7 47 O049900200018 ELEMENT MASS DATA ERR-T MISC MISC-ERR O049900200019 FLAG O049900200020 NO-DIM NO-DIM PRD/INC PRD/INC SEE TEXT SEE TEXT O049900200021 NO-DIM O049900200022 39. 96. 322.E-13 201. O049900200023 O049900200024 39. 97. 584.73E-13 365. O049900200025 O049900200026 40. 99. 619.97E-13 67.28E-13 387. 42.O049900200027 O049900200028 40. 100. 773.77E-13 84.91E-13 483. 53.O049900200029 O049900200030 40. 101. 422.93E-13 56.07E-13 264. 35.O049900200031 O049900200032 40. 102. 317.2E-13 36.85E-13 198. 23.O049900200033 O049900200034 40. 103. 29.16E-13 3.68E-13 18.2 2.3O049900200035 1. O049900200036 40. 104. 56.07E-13 11.21E-13 35. 7.O049900200037 O049900200038 41. 99. 898.72E-13 561. O049900200039 O049900200040 41. 100. 1119.8E-13 699. O049900200041 O049900200042 42. 104. 277.15E-13 38.45E-13 173. 24.O049900200043 O049900200044 42. 105. 259.52E-13 40.05E-13 162. 25.O049900200045 O049900200046 42. 106. 184.23E-13 22.43E-13 115. 14.O049900200047 O049900200048 42. 107. 42.61E-13 5.13E-13 26.6 3.2O049900200049 O049900200050 43. 104. 349.24E-13 38.45E-13 218. 24.O049900200051 O049900200052 43. 105. 429.34E-13 48.06E-13 268. 30.O049900200053 O049900200054 43. 106. 438.95E-13 49.66E-13 274. 31.O049900200055 O049900200056 43. 107. 352.44E-13 40.05E-13 220. 25.O049900200057 O049900200058 43. 108. 261.13E-13 30.44E-13 163. 19.O049900200059 O049900200060 43. 109. 145.78E-13 17.62E-13 91. 11.O049900200061 O049900200062 43. 110. 55.27E-13 7.21E-13 34.5 4.2O049900200063 O049900200064 43. 111. 2.66E-13 0.47E-13 1.66 0.29O049900200065 1. O049900200066 43. 112. 4.93E-13 0.83E-13 3.08 0.52O049900200067 O049900200068 44. 107. 352.44E-13 41.65E-13 220. 26.O049900200069 O049900200070 44. 108. 283.55E-13 32.04E-13 177. 20.O049900200071 O049900200072 44. 109. 89.55E-13 10.73E-13 55.9 6.7O049900200073 1. O049900200074 44. 110. 166.61E-13 20.83E-13 104. 13.O049900200075 O049900200076 44. 111. 150.59E-13 19.24E-13 94. 12.O049900200077 O049900200078 44. 112. 160.2E-13 19.24E-13 100. 12.O049900200079 O049900200080 44. 113. 31.88E-13 4.17E-13 19.9 2.6O049900200081 O049900200082 45. 108. 408.51E-13 46.46E-13 255. 29.O049900200083 O049900200084 45. 109. 485.41E-13 56.07E-13 303. 35.O049900200085 O049900200086 45. 110. 273.94E-13 41.65E-13 171. 26.O049900200087 O049900200088 45. 111. 355.64E-13 40.05E-13 222. 25.O049900200089 O049900200090 45. 112. 511.04E-13 72.09E-13 319. 45.O049900200091 O049900200092 45. 113. 211.46E-13 25.63E-13 132. 16.O049900200093 O049900200094 45. 114. 190.64E-13 24.03E-13 119. 15.O049900200095 O049900200096 45. 115. 38.61E-13 6.25E-13 24.1 3.9O049900200097 O049900200098 45. 116. 32.52E-13 4.97E-13 20.3 3.1O049900200099 O049900200100 47. 113. 477.4E-13 57.67E-13 298. 36.O049900200101 1. O049900200102 47. 114. 740.12E-13 91.31E-13 462. 57.O049900200103 1. O049900200104 47. 115. 341.23E-13 40.05E-13 213. 25.O049900200105 O049900200106 47. 116. 336.42E-13 40.05E-13 210. 25.O049900200107 O049900200108 47. 117. 427.73E-13 48.06E-13 267. 30.O049900200109 O049900200110 47. 118. 339.62E-13 49.66E-13 212. 31.O049900200111 O049900200112 47. 119. 185.83E-13 25.63E-13 116. 16.O049900200113 O049900200114 47. 120. 124.96E-13 17.62E-13 78. 11.O049900200115 O049900200116 ENDDATA 98 0 O049900200117 ENDSUBENT 116 0 O049900299999 ENDENTRY 2 0 O049999999999