ENTRY T0406 20050406 T020T040600000001 SUBENT T0406001 20050406 T020T040600100001 BIB 10 23 T040600100002 INSTITUTE (1CANMON,1CANMCG) T040600100003 REFERENCE (J,PR/C,25,2534,1982) T040600100004 AUTHOR (B.P.Pathak,L.Lessard,L.Nikkinen,J.K.P.Lee) T040600100005 TITLE Proton-induced fission of iridium T040600100006 FACILITY (SYNCY,1CANMCG) T040600100007 (SPECM) T040600100008 SAMPLE Natural iridium metal powder deposited on graphite T040600100009 disks with upper segment removed to make flat plat- T040600100010 form for ionizer foil. Average target thickness 8 T040600100011 mg/cm2. Stacks of 25 disks, separated by 0.3 mm T040600100012 graphite washers inserted into target-oven heated to T040600100013 1600 C. T040600100014 METHOD (ASEP) Samples irradiated for 0.4 sec; data accumulatedT040600100015 in four groups of 1 sec. T040600100016 Fission fragments stopped in graphite disks and alkali T040600100017 elements come out by the thermal diffusion process. T040600100018 The isotopes of Rb are selectively ionized at T040600100019 temperatures of about 1000 C. T040600100020 CORRECTION Corrected for background and mass discrimination T040600100021 response of spectrometer. T040600100022 Proton energies corrected for attenuation in target. T040600100023 STATUS Data translated from NRDF file data set 746. T040600100024 HISTORY (20050406C) VM T040600100025 ENDBIB 23 0 T040600100026 NOCOMMON 0 0 T040600100027 ENDSUBENT 26 0 T040600199999 SUBENT T0406002 20050406 T020T040600200001 BIB 3 4 T040600200002 REACTION (77-IR-0(P,F)ELEM/MASS,IND,FY,,REL) T040600200003 ERR-ANALYS (DATA-ERR) No information given on source of T040600200004 uncertainty. T040600200005 STATUS (CURVE) Data scanned from Fig. 3 at JCPRG. T040600200006 ENDBIB 4 0 T040600200007 COMMON 1 3 T040600200008 ELEMENT T040600200009 NO-DIM T040600200010 37. T040600200011 ENDCOMMON 3 0 T040600200012 DATA 4 24 T040600200013 EN MASS DATA DATA-ERR T040600200014 MEV NO-DIM ARB-UNITS ARB-UNITS T040600200015 62. 86. 39.8 19.0 T040600200016 62. 87. 96.8 16.4 T040600200017 62. 88. 135.3 16.1 T040600200018 62. 89. 109.5 12.0 T040600200019 62. 90. 53.5 12.4 T040600200020 62. 91. 16.5 6.1 T040600200021 80. 84. 13.6 8.1 T040600200022 80. 85. 104.5 17.7 T040600200023 80. 86. 278.7 T040600200024 80. 87. 489.2 T040600200025 80. 88. 590.3 T040600200026 80. 89. 370.7 T040600200027 80. 90. 155.9 11.3 T040600200028 80. 91. 38.5 3.9 T040600200029 80. 92. 5.9 1.4 T040600200030 95. 84. 71.8 18.3 T040600200031 95. 85. 350.0 48.9 T040600200032 95. 86. 772.3 T040600200033 95. 87. 1102.0 132.0 T040600200034 95. 88. 877.5 T040600200035 95. 89. 547.4 T040600200036 95. 90. 269.9 T040600200037 95. 91. 118.8 T040600200038 95. 92. 52.8 4.3 T040600200039 ENDDATA 26 0 T040600200040 ENDSUBENT 39 0 T040600299999 SUBENT T0406003 20050406 T020T040600300001 BIB 5 9 T040600300002 REACTION (77-IR-0(P,F),,SIG,,REL) T040600300003 MONITOR (90-TH-232(P,F)ELEM/MASS,IND,FY) T040600300004 Relative to known yields of Rb isotopes in 232Th T040600300005 fission. T040600300006 ANALYSIS Calculated assuming that the total Rb cross sections T040600300007 are a constant fraction of the total fission cross T040600300008 section over the range of incident proton energies. T040600300009 ERR-ANALYS No information given on uncertainties. T040600300010 STATUS (CURVE) Data scanned from Fig. 4 at JCPRG. T040600300011 ENDBIB 9 0 T040600300012 NOCOMMON 0 0 T040600300013 DATA 2 3 T040600300014 EN DATA T040600300015 MEV ARB-UNITS T040600300016 62. 3.786E-01 T040600300017 80. 1.152E+00 T040600300018 95. 2.907E+00 T040600300019 ENDDATA 5 0 T040600300020 ENDSUBENT 19 0 T040600399999 ENDENTRY 3 0 T040699999999