ENTRY L0253 20190523 L042L025300000001 SUBENT L0253001 20190523 L042L025300100001 BIB 11 25 L025300100002 TITLE Independent yields from the photofission of 232Th, L025300100003 and the Z(p) and statistical-dynamic models L025300100004 AUTHOR (J.R.Smith,A.E.Richardson) L025300100005 INSTITUTE (1USANMS) L025300100006 REFERENCE (J,PR/C,44,1118,1991) L025300100007 #doi:10.1103/PhysRevC.44.1118 L025300100008 #NSR: 1991SM04 L025300100009 FACILITY (LINAC,1USAWSA) L025300100010 INC-SOURCE (BRST) Three irradiations were performed with 27-MeV L025300100011 peak bremsstrahlung, one with 15 MeV, one with 10 MeV. L025300100012 Fluctuations in peak bremsstrahlung energies during theL025300100013 irradiations were about +-1 MeV. L025300100014 METHOD (ACTIV) The duration of each irradiation was L025300100015 approximately 1 h. L025300100016 (CHSEP,GSPEC) L025300100017 DETECTOR (GELI,GE-IN) A Canberra Ge(Li) detector with a 2.3-MeV L025300100018 resolution for the 1.33-MeV gamma ray from Co and a 16%L025300100019 efficiency, two Ortec Ge(Li) detectors with a 2.1-keV L025300100020 resolution and a 15% efficiency, and an Ortec intrinsicL025300100021 Ge detector with a 1.75-keV resolution and 25% L025300100022 efficiency. L025300100023 SAMPLE 40-g samples of reagent-grade Th(NO3)4*4H20 in L025300100024 polyethylene ampoules L025300100025 ERR-ANALYS (DATA-ERR) No information on sources of uncertainties L025300100026 HISTORY (20190523C) OG. L025300100027 ENDBIB 25 0 L025300100028 NOCOMMON 0 0 L025300100029 ENDSUBENT 28 0 L025300199999 SUBENT L0253002 20190523 L042L025300200001 BIB 2 2 L025300200002 REACTION (90-TH-232(G,F)ELEM/MASS,IND,FY,,BRA) L025300200003 STATUS (TABLE) Table I from Phys.Rev.,C44,1118,1991 L025300200004 ENDBIB 2 0 L025300200005 NOCOMMON 0 0 L025300200006 DATA 6 9 L025300200007 EN-MAX MASS ELEMENT DATA-MAX DATA DATA-ERR L025300200008 MEV NO-DIM NO-DIM PC/FIS PC/FIS PC/FIS L025300200009 11. 136. 55. 1.06E-3 0.48E-3L025300200010 15. 136. 55. 3.37E-3 0.36E-3L025300200011 27. 82. 35. 8.91E-5 1.18E-5L025300200012 27. 86. 37. 5.84E-4 L025300200013 27. 96. 41. 2.40E-5 0.36E-5L025300200014 27. 124. 51. 1.26E-3 0.15E-3L025300200015 27. 126. 51. 2.41E-2 0.25E-2L025300200016 27. 134. 55. 1.42E-4 L025300200017 27. 136. 55. 1.13E-2 0.12E-2L025300200018 ENDDATA 11 0 L025300200019 ENDSUBENT 18 0 L025300299999 SUBENT L0253003 20190523 L042L025300300001 BIB 3 5 L025300300002 REACTION (90-TH-232(G,F)MASS,CHN,FY,,BRA) L025300300003 ANALYSIS The mass yields for masses 125 and 127 were based on L025300300004 the assumption that the cumulative chain yields of L025300300005 125Sb and 127Sb represented the mass yields. L025300300006 STATUS (TABLE) Table I from Phys.Rev.,C44,1118,1991 L025300300007 ENDBIB 5 0 L025300300008 COMMON 1 3 L025300300009 EN-MAX L025300300010 MEV L025300300011 27. L025300300012 ENDCOMMON 3 0 L025300300013 DATA 3 2 L025300300014 MASS DATA DATA-ERR L025300300015 NO-DIM PC/FIS PC/FIS L025300300016 125. 0.29 0.06 L025300300017 127. 0.44 0.05 L025300300018 ENDDATA 4 0 L025300300019 ENDSUBENT 18 0 L025300399999 ENDENTRY 3 0 L025399999999