ENTRY C2562 20200729 C198C256200000001 SUBENT C2562001 20200729 C198C256200100001 BIB 10 28 C256200100002 TITLE Nonequilibrium fission and heavy residue production C256200100003 in the interaction of 12-16 MeV/nucleon 32S with 165Ho C256200100004 AUTHOR (C.Casey,W.Loveland,Z.Xu,L.Sihver,K.Aleklett, C256200100005 G.T.Seaborg) C256200100006 REFERENCE (J,PR/C,40,1244,1989) C256200100007 #doi:10.1103/PhysRevC.40.1244 C256200100008 REL-REF (M,,D.J.Morrissey+,J,NIM,158,499,1979) Activation C256200100009 technique. C256200100010 INSTITUTE (1USAORU,2SWDSWR,1USABRK) C256200100011 FACILITY (CYCLO,1USABRK) The Lawrence Berkeley Laboratory (LBL) C256200100012 88-inch cyclotron. C256200100013 INC-SPECT Two irradiations, of duration 1.25 and 6.53 h, C256200100014 respectively, were performed to determine the target C256200100015 fragment yields (total fluences 2.4x10**15 and C256200100016 6.7x10**16 ions, respectively). C256200100017 SAMPLE The targets for these irradiations were 90 mg/cm2 C256200100018 thick, giving a center-of-target energy of 380 MeV C256200100019 or 12 MeV/nucleon. C256200100020 METHOD (CHSEP,ACTIV,GSPEC) Radiochemical techniques. These C256200100021 pieces were assayed by gamma-ray spectroscopy C256200100022 beginning a few minutes after the end of irradiation C256200100023 and continuing for periods up to two months in C256200100024 laboratories at LBL and Oregon State University. C256200100025 After identifying the activities present in each foil C256200100026 and the amount of each radionuclide present, C256200100027 differential cross sections for each angular interval C256200100028 were calculated. C256200100029 HISTORY (20200729C) BP C256200100030 ENDBIB 28 0 C256200100031 NOCOMMON 0 0 C256200100032 ENDSUBENT 31 0 C256200199999 SUBENT C2562002 20200729 C198C256200200001 BIB 4 15 C256200200002 REACTION (67-HO-165(16-S-32,X)ELEM/MASS,CUM,SIG) C256200200003 REL-REF (M,C2539001,D.J.Morrissey+,J,PR/C,21,1783,1980) Error C256200200004 analysis insights. C256200200005 ERR-ANALYS (DATA-ERR) The error bars on the integrated data C256200200006 points reflect the uncertainties due to counting C256200200007 statistics and those introduced in the charge C256200200008 distribution fitting process. Morrissey et al. have C256200200009 suggested that individual isobaric yields may have C256200200010 systematic uncertainties, due to the fitting process, C256200200011 of approximately 25%. Uncertainties due to lack of C256200200012 knowledge of the absolute beam intensity (estimated C256200200013 to be approximately 15%), and contributions due to C256200200014 secondary reactions (possibly as large as 10%) have C256200200015 been neglected. C256200200016 STATUS (TABLE) Table I, page 1246. C256200200017 ENDBIB 15 0 C256200200018 COMMON 1 3 C256200200019 EN C256200200020 MEV/A C256200200021 12.0 C256200200022 ENDCOMMON 3 0 C256200200023 DATA 5 66 C256200200024 ELEMENT MASS ISOMER DATA DATA-ERR C256200200025 NO-DIM NO-DIM NO-DIM MB MB C256200200026 19.0 42.0 9.8 0.5 C256200200027 19.0 43.0 11.2 0.3 C256200200028 20.0 47.0 1.6 0.06 C256200200029 23.0 48.0 2.26 0.03 C256200200030 25.0 52.0 1.5 0.01 C256200200031 25.0 56.0 18.0 2.0 C256200200032 26.0 59.0 10.0 0.3 C256200200033 30.0 65.0 15.0 1.0 C256200200034 32.0 69.0 11.2 0.9 C256200200035 33.0 74.0 30.0 2.0 C256200200036 34.0 73.0 4.2 0.1 C256200200037 34.0 75.0 29.4 0.9 C256200200038 35.0 75.0 2.5 0.2 C256200200039 35.0 76.0 14.0 6.0 C256200200040 35.0 77.0 32.0 2.0 C256200200041 36.0 79.0 21.0 10.0 C256200200042 37.0 81.0 18.1 0.9 C256200200043 37.0 82.0 1.0 28.0 4.0 C256200200044 37.0 83.0 56.0 4.0 C256200200045 39.0 86.0 28.0 2.0 C256200200046 39.0 87.0 62.3 0.9 C256200200047 39.0 88.0 40.0 2.0 C256200200048 40.0 88.0 36.0 2.0 C256200200049 40.0 89.0 51.0 1.0 C256200200050 41.0 90.0 25.0 2.0 C256200200051 43.0 93.0 3.3 0.3 C256200200052 43.0 94.0 10.0 2.0 C256200200053 43.0 95.0 18.0 3.0 C256200200054 44.0 95.0 3.1 0.2 C256200200055 44.0 97.0 18.1 0.7 C256200200056 45.0 100.0 23.6 0.4 C256200200057 45.0 101.0 1.0 33.0 1.0 C256200200058 47.0 105.0 33.0 5.0 C256200200059 49.0 111.0 30.6 0.7 C256200200060 53.0 123.0 36.0 1.0 C256200200061 53.0 124.0 3.8 0.2 C256200200062 54.0 123.0 15.9 0.8 C256200200063 54.0 127.0 15.0 6.0 C256200200064 55.0 127.0 14.3 0.54 C256200200065 55.0 129.0 20.2 0.8 C256200200066 56.0 126.0 7.7 0.9 C256200200067 56.0 128.0 25.0 8.0 C256200200068 58.0 132.0 10.0 0.6 C256200200069 58.0 135.0 16.0 2.0 C256200200070 58.0 139.0 6.0 1.0 C256200200071 63.0 145.0 11.2 0.3 C256200200072 63.0 146.0 7.4 0.4 C256200200073 64.0 149.0 24.0 1.0 C256200200074 65.0 151.0 18.0 3.0 C256200200075 65.0 152.0 15.0 2.0 C256200200076 65.0 153.0 27.0 2.0 C256200200077 65.0 155.0 37.0 11.0 C256200200078 66.0 155.0 31.3 0.7 C256200200079 66.0 157.0 48.7 0.9 C256200200080 68.0 160.0 94.0 6.0 C256200200081 68.0 161.0 82.0 3.0 C256200200082 69.0 163.0 94.0 22.0 C256200200083 69.0 165.0 156.0 23.0 C256200200084 69.0 167.0 76.0 4.0 C256200200085 70.0 166.0 54.0 5.0 C256200200086 71.0 169.0 29.0 1.0 C256200200087 72.0 170.0 16.9 0.8 C256200200088 72.0 171.0 14.0 1.0 C256200200089 72.0 173.0 12.7 0.4 C256200200090 72.0 175.0 22.0 1.0 C256200200091 73.0 173.0 4.0 2.0 C256200200092 ENDDATA 68 0 C256200200093 ENDSUBENT 92 0 C256200299999 SUBENT C2562003 20200729 C198C256200300001 BIB 5 19 C256200300002 REACTION (67-HO-165(16-S-32,X)ELEM/MASS,,SIG) C256200300003 REL-REF (M,C2539001,D.J.Morrissey+,J,PR/C,21,1783,1980) Error C256200300004 analysis insights. C256200300005 ANALYSIS By the term "independent yield" we refer to the C256200300006 yields of shielded nuclides, quasishielded nuclides, C256200300007 and nuclides whose production by precursor decay is C256200300008 not significant. C256200300009 ERR-ANALYS (DATA-ERR) The error bars on the integrated data C256200300010 points reflect the uncertainties due to counting C256200300011 statistics and those introduced in the charge C256200300012 distribution fitting process. Morrissey et al. have C256200300013 suggested that individual isobaric yields may have C256200300014 systematic uncertainties, due to the fitting process, C256200300015 of approximately 25%. Uncertainties due to lack of C256200300016 knowledge of the absolute beam intensity (estimated C256200300017 to be approximately 15%), and contributions due to C256200300018 secondary reactions (possibly as large as 10%) have C256200300019 been neglected. C256200300020 STATUS (TABLE) Table I, page 1246. C256200300021 ENDBIB 19 0 C256200300022 COMMON 1 3 C256200300023 EN C256200300024 MEV/A C256200300025 12.0 C256200300026 ENDCOMMON 3 0 C256200300027 DATA 5 7 C256200300028 ELEMENT MASS ISOMER DATA DATA-ERR C256200300029 NO-DIM NO-DIM NO-DIM MB MB C256200300030 21.0 46.0 11.5 0.5 C256200300031 21.0 48.0 5.2 0.6 C256200300032 35.0 82.0 5.8 0.4 C256200300033 37.0 84.0 39.0 1.0 C256200300034 41.0 92.0 1.0 1.6 0.5 C256200300035 43.0 96.0 30.6 0.2 C256200300036 65.0 156.0 5.5 0.2 C256200300037 ENDDATA 9 0 C256200300038 ENDSUBENT 37 0 C256200399999 SUBENT C2562004 20200729 C198C256200400001 BIB 3 3 C256200400002 REACTION (67-HO-165(16-S-32,X)21-SC-48,,DA,,REL) C256200400003 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C256200400004 STATUS (CURVE) Fig. 4, page 1249. C256200400005 ENDBIB 3 0 C256200400006 COMMON 1 3 C256200400007 EN C256200400008 MEV/A C256200400009 16.0 C256200400010 ENDCOMMON 3 0 C256200400011 DATA 3 10 C256200400012 ANG DATA DATA-ERR C256200400013 ADEG ARB-UNITS ARB-UNITS C256200400014 8.431 4.720E+00 C256200400015 14.155 2.303E+00 C256200400016 22.068 7.973E-01 1.752E-01 C256200400017 29.206 5.295E-01 C256200400018 39.002 2.738E-01 C256200400019 53.869 2.461E-01 C256200400020 72.650 1.048E-01 C256200400021 108.290 1.046E-01 C256200400022 132.105 6.429E-02 C256200400023 145.692 8.391E-02 C256200400024 ENDDATA 12 0 C256200400025 ENDSUBENT 24 0 C256200499999 SUBENT C2562005 20200729 C198C256200500001 BIB 2 2 C256200500002 REACTION (67-HO-165(16-S-32,X)33-AS-74,,DA,,REL) C256200500003 STATUS (CURVE) Fig. 4, page 1249. C256200500004 ENDBIB 2 0 C256200500005 COMMON 1 3 C256200500006 EN C256200500007 MEV/A C256200500008 16.0 C256200500009 ENDCOMMON 3 0 C256200500010 DATA 2 10 C256200500011 ANG DATA C256200500012 ADEG ARB-UNITS C256200500013 6.677 1.115E+01 C256200500014 12.390 5.715E+00 C256200500015 20.374 4.824E+00 C256200500016 27.868 2.541E+00 C256200500017 38.084 2.395E+00 C256200500018 53.149 1.486E+00 C256200500019 72.230 1.087E+00 C256200500020 108.201 8.129E-01 C256200500021 131.309 7.838E-01 C256200500022 145.530 7.796E-01 C256200500023 ENDDATA 12 0 C256200500024 ENDSUBENT 23 0 C256200599999 SUBENT C2562006 20200730 C198C256200600001 BIB 2 2 C256200600002 REACTION (67-HO-165(16-S-32,X)40-ZR-89,,DA,,REL) C256200600003 STATUS (CURVE) Fig. 4, page 1249. C256200600004 ENDBIB 2 0 C256200600005 COMMON 1 3 C256200600006 EN C256200600007 MEV/A C256200600008 16.0 C256200600009 ENDCOMMON 3 0 C256200600010 DATA 2 10 C256200600011 ANG DATA C256200600012 ADEG ARB-UNITS C256200600013 6.293 2.200E+01 C256200600014 11.612 8.234E+00 C256200600015 20.164 8.439E+00 C256200600016 28.217 4.750E+00 C256200600017 37.653 4.022E+00 C256200600018 52.907 2.322E+00 C256200600019 72.243 1.960E+00 C256200600020 107.732 9.290E-01 C256200600021 131.124 8.501E-01 C256200600022 145.499 6.272E-01 C256200600023 ENDDATA 12 0 C256200600024 ENDSUBENT 23 0 C256200699999 SUBENT C2562007 20200730 C198C256200700001 BIB 2 2 C256200700002 REACTION (67-HO-165(16-S-32,X)49-IN-111,,DA,,REL) C256200700003 STATUS (CURVE) Fig. 4, page 1249. C256200700004 ENDBIB 2 0 C256200700005 COMMON 1 3 C256200700006 EN C256200700007 MEV/A C256200700008 16.0 C256200700009 ENDCOMMON 3 0 C256200700010 DATA 2 10 C256200700011 ANG DATA C256200700012 ADEG ARB-UNITS C256200700013 5.480 9.392E+00 C256200700014 11.667 5.976E+00 C256200700015 19.644 4.033E+00 C256200700016 27.623 2.805E+00 C256200700017 37.395 2.132E+00 C256200700018 52.081 1.822E+00 C256200700019 71.597 8.287E-01 C256200700020 107.994 2.385E-01 C256200700021 131.551 1.417E-01 C256200700022 145.794 1.248E-01 C256200700023 ENDDATA 12 0 C256200700024 ENDSUBENT 23 0 C256200799999 SUBENT C2562008 20200730 C198C256200800001 BIB 3 3 C256200800002 REACTION (67-HO-165(16-S-32,X)56-BA-131,,DA,,REL) C256200800003 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C256200800004 STATUS (CURVE) Fig. 4, page 1249. C256200800005 ENDBIB 3 0 C256200800006 COMMON 1 3 C256200800007 EN C256200800008 MEV/A C256200800009 16.0 C256200800010 ENDCOMMON 3 0 C256200800011 DATA 3 7 C256200800012 ANG DATA DATA-ERR C256200800013 ADEG ARB-UNITS ARB-UNITS C256200800014 6.609 9.243E+00 3.478E+00 C256200800015 11.663 5.056E+00 C256200800016 20.216 3.411E+00 9.856E-01 C256200800017 27.991 2.766E+00 C256200800018 37.711 2.128E+00 6.920E-01 C256200800019 52.873 1.513E+00 C256200800020 71.922 2.116E-01 C256200800021 ENDDATA 9 0 C256200800022 ENDSUBENT 21 0 C256200899999 SUBENT C2562009 20200730 C198C256200900001 BIB 3 3 C256200900002 REACTION (67-HO-165(16-S-32,X)64-GD-146,,DA,,REL) C256200900003 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C256200900004 STATUS (CURVE) Fig. 4, page 1249. C256200900005 ENDBIB 3 0 C256200900006 COMMON 1 3 C256200900007 EN C256200900008 MEV/A C256200900009 16.0 C256200900010 ENDCOMMON 3 0 C256200900011 DATA 3 9 C256200900012 ANG DATA DATA-ERR C256200900013 ADEG ARB-UNITS ARB-UNITS C256200900014 6.524 1.061E+01 C256200900015 11.514 9.237E+00 1.812E+00 C256200900016 19.957 6.210E+00 C256200900017 27.633 5.092E+00 1.600E+00 C256200900018 37.612 2.863E+00 C256200900019 52.579 8.703E-01 2.615E-01 C256200900020 71.769 3.100E-01 1.806E-01 C256200900021 107.846 3.039E-01 C256200900022 145.457 4.432E-01 C256200900023 ENDDATA 11 0 C256200900024 ENDSUBENT 23 0 C256200999999 SUBENT C2562010 20200730 C198C256201000001 BIB 2 2 C256201000002 REACTION (67-HO-165(16-S-32,X)64-GD-149,,DA,,REL) C256201000003 STATUS (CURVE) Fig. 4, page 1249. C256201000004 ENDBIB 2 0 C256201000005 COMMON 1 3 C256201000006 EN C256201000007 MEV/A C256201000008 16.0 C256201000009 ENDCOMMON 3 0 C256201000010 DATA 2 7 C256201000011 ANG DATA C256201000012 ADEG ARB-UNITS C256201000013 6.323 1.587E+01 C256201000014 12.159 1.132E+01 C256201000015 20.669 1.027E+01 C256201000016 28.437 7.325E+00 C256201000017 37.402 3.795E+00 C256201000018 52.618 1.125E+00 C256201000019 72.204 1.252E-01 C256201000020 ENDDATA 9 0 C256201000021 ENDSUBENT 20 0 C256201099999 SUBENT C2562011 20200730 C198C256201100001 BIB 3 3 C256201100002 REACTION (67-HO-165(16-S-32,X)68-ER-160,,DA,,REL) C256201100003 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C256201100004 STATUS (CURVE) Fig. 4, page 1249. C256201100005 ENDBIB 3 0 C256201100006 COMMON 1 3 C256201100007 EN C256201100008 MEV/A C256201100009 16.0 C256201100010 ENDCOMMON 3 0 C256201100011 DATA 3 8 C256201100012 ANG DATA DATA-ERR C256201100013 ADEG ARB-UNITS ARB-UNITS C256201100014 7.100 6.087E+01 C256201100015 12.012 3.343E+01 8.306E+00 C256201100016 20.405 2.850E+01 C256201100017 27.992 1.563E+01 C256201100018 37.879 9.260E+00 C256201100019 53.099 4.563E+00 C256201100020 72.044 7.943E-01 C256201100021 128.914 3.650E-01 9.772E-02 C256201100022 ENDDATA 10 0 C256201100023 ENDSUBENT 22 0 C256201199999 SUBENT C2562012 20200730 C198C256201200001 BIB 3 3 C256201200002 REACTION (67-HO-165(16-S-32,X)70-YB-169,,DA,,REL) C256201200003 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C256201200004 STATUS (CURVE) Fig. 4, page 1249. C256201200005 ENDBIB 3 0 C256201200006 COMMON 1 3 C256201200007 EN C256201200008 MEV/A C256201200009 16.0 C256201200010 ENDCOMMON 3 0 C256201200011 DATA 3 4 C256201200012 ANG DATA DATA-ERR C256201200013 ADEG ARB-UNITS ARB-UNITS C256201200014 5.774 5.300E+01 C256201200015 11.735 1.861E+01 C256201200016 19.970 2.689E+00 C256201200017 37.903 4.404E-01 1.834E-01 C256201200018 ENDDATA 6 0 C256201200019 ENDSUBENT 18 0 C256201299999 ENDENTRY 12 0 C256299999999