ENTRY O0606 20200227 O076O060600000001 SUBENT O0606001 20200227 O076O060600100001 BIB 8 23 O060600100002 TITLE Total and differential cross sections of 10 to 95 MeV O060600100003 proton-induced fission of actinide nuclei O060600100004 AUTHOR (A.N.Smirnov,I.Yu.Gorshkov,A.V.Prokofiev, V.P.Eismont) O060600100005 INSTITUTE (4RUSRI ) O060600100006 REFERENCE (C,91GAUSSG,,214,1991) In English. O060600100007 the article is not available -SD O060600100008 FACILITY (SYNCH,4RUSRI ) V.G.Khlopin Radium Institute's O060600100009 proton synchrotron. O060600100010 PART-DET (FF) O060600100011 ERR-ANALYS (ERR-1) Uncertainty of the target weight. O060600100012 (ERR-2) Inhomogeneity of the layer thickness. O060600100013 HISTORY (19980215C) by Khlopin's Institute - AP. O060600100014 (19980220A) ERR-ANALYS and COMMON sections are O060600100015 rewritten by AP. O060600100016 (19980309A) Angular distributions are included by AP. O060600100017 (19980424A) AUTHOR and MONITOR are corrected, REL-REF O060600100018 for U-238 data are included by AP. O060600100019 (20000420U) Last checking has been done. O060600100020 (20000424A) Date is corrected O060600100021 (20001116A) subentries O0606010-013 are corrected O060600100022 according to O.Schwerer remarks. O060600100023 (20001116U) Last checking has been done. O060600100024 (20200227U) SD: small corrections in all subents. O060600100025 ENDBIB 23 0 O060600100026 COMMON 2 3 O060600100027 ERR-1 ERR-2 O060600100028 PER-CENT PER-CENT O060600100029 3. 3. O060600100030 ENDCOMMON 3 0 O060600100031 ENDSUBENT 30 0 O060600199999 SUBENT O0606002 20200227 O076O060600200001 BIB 12 39 O060600200002 REACTION (92-U-238(P,F),,SIG) O060600200003 METHOD (FISCT,EXTB,SITA,MOSEP,ACTIV) O060600200004 SAMPLE Two 238-U targets, about 500 mu-g/cm**2, on the O060600200005 100-mu-m thick aluminum foils, were installed O060600200006 back-to-back at 45 deg. to the beam axis. Between the O060600200007 targets there was a 0.6-mm thick copper foil O060600200008 for monitoring. O060600200009 Target composition : O060600200010 U-238 - 99.999%, O060600200011 U-234 - 0.0003%, O060600200012 U-235 - 0.0003%, O060600200013 U-236 - 0.0003%. O060600200014 the targets had a small admixture of 252-Cf to provide O060600200015 calibration of the detectors simultaneously to the O060600200016 beam measurements O060600200017 DETECTOR (THRES) Thin-film breakdown counters of fission O060600200018 fragments, placed at 0,45,90,135 and 180 deg. to the O060600200019 beam direction O060600200020 MONITOR (29-CU-0(P,X)29-CU-61,CUM,SIG) O060600200021 MONIT-REF (A0178006,A.Grutter,J,NP/A,383,98,1982) O060600200022 DECAY-MON (29-CU-61,3.33HR,DG,683.,0.112) O060600200023 ANALYSIS (INTAD) O060600200024 CORRECTION Beam energy degradation in the targets, the O060600200025 detectors and the monitor foil. O060600200026 Negligible: fission induced by background neutrons O060600200027 ERR-ANALYS (ERR-T) The quoted errors include: O060600200028 * the uncertainty of the target weight; O060600200029 * the inhomogeneity of the layer thickness; O060600200030 * the uncertainty of measuring the proton O060600200031 beam current; O060600200032 * the statistics of fission events in the main and O060600200033 calibration measurements; O060600200034 * the uncertainty estimated from the spread of data O060600200035 obtained in different measurement series; O060600200036 (ERR-3) the uncertainty of measuring the proton beam O060600200037 current O060600200038 STATUS (TABLE) Data from the text of 91GAUSSG,214,1991 O060600200039 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060600200040 ERR-ANALYS updated. O060600200041 ENDBIB 39 0 O060600200042 NOCOMMON 0 0 O060600200043 DATA 5 1 O060600200044 EN EN-ERR DATA ERR-3 ERR-T O060600200045 MEV MEV MB PER-CENT MB O060600200046 62. 2. 1840. 5. 180. O060600200047 ENDDATA 3 0 O060600200048 ENDSUBENT 47 0 O060600299999 SUBENT O0606003 20200227 O076O060600300001 BIB 11 51 O060600300002 REACTION (92-U-238(P,F),,SIG) O060600300003 REL-REF (A,O0193001,S.Baba+,J,NP/A,175,177,1971) Total fission O060600300004 cross sections are not compiled in the given entry. O060600300005 (A,A0047002,O.E.Shigaev+,R,RI-17,1973) In Russian. O060600300006 (D,C0370008,P.C.Stevenson+,J,PR,111,886,1958) O060600300007 METHOD (FISCT,EXTB,STTA,EDEG) The range-energy tables were O060600300008 taken from: O.F.Nemets et al. Handbook on nuclear O060600300009 physics. Kiev, 1975 (in Russian). A few irradiations O060600300010 were done with different initial proton energies. O060600300011 SAMPLE A stack of 10 U-238 targets, each about 500 mu-gr/cm2, O060600300012 was installed perpendicularly to the beam axis. O060600300013 Copper filters were placed between the targets to O060600300014 provide the proton beam energy degradation. O060600300015 Target composition: O060600300016 U-238 - 99.999%, O060600300017 U-234 - 0.0003%, O060600300018 U-235 - 0.0003%, O060600300019 U-236 - 0.0003%. O060600300020 DETECTOR (THRES) Thin-film breakdown counters of fission O060600300021 fragments, placed close to the targets O060600300022 perpendicularly to the beam axis. Relative detector O060600300023 calibration was performed in the same geometry but O060600300024 without the copper filters, with the use of the O060600300025 proton beam with energy of about 100 MeV. O060600300026 COMMENT -By authors- O060600300027 segments of the relative fission cross section energy O060600300028 dependence obtained with different initial proton O060600300029 energies were sewed together with the use of the O060600300030 least-square method. O060600300031 The absolute fission cross sections were obtained with O060600300032 the use of the absolute measurement at 62 MeV (see O060600300033 subent O0606002). O060600300034 CORRECTION Performed: beam energy degradation in the targets O060600300035 and the detectors. O060600300036 Negligible: fission induced by background neutrons, O060600300037 energy dependence of the angular anisotropy of O060600300038 fission, the dependence of the detection efficiency O060600300039 on the energy and angular distributions of fission O060600300040 fragments. O060600300041 ERR-ANALYS (ERR-T). The quoted errors include the uncertainty of O060600300042 the target weight, the inhomogeneity of the layer O060600300043 thickness, the statistics of fission events in the O060600300044 main and calibration measurements and the uncertainty O060600300045 estimated from the spread of data obtained in O060600300046 different measurement series. O060600300047 The quoted errors do not include the uncertainty O060600300048 of the absolute fission cross section measurement. O060600300049 FLAG (1.) Absolute measurements. O060600300050 STATUS (TABLE) Data from the text of 91GAUSSG,214,1991 O060600300051 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060600300052 ERR-ANALYS updated. Vol. of ref. in REL-REF corrected. O060600300053 ENDBIB 51 0 O060600300054 NOCOMMON 0 0 O060600300055 DATA 5 14 O060600300056 EN EN-ERR DATA ERR-T FLAG O060600300057 MEV MEV MB MB NO-DIM O060600300058 11. 1. 18. 2. O060600300059 15. 1.5 660. 70. O060600300060 26. 2. 1130. 110. O060600300061 33. 2. 1550. 160. O060600300062 35. 2. 1650. 170. O060600300063 42. 2. 1720. 170. O060600300064 47. 2. 1870. 190. O060600300065 50. 2. 1710. 170. O060600300066 52. 2. 1870. 190. O060600300067 62. 2. 1840. 180. 1. O060600300068 65. 2. 2030. 200. O060600300069 76. 2. 1830. 180. O060600300070 83. 2. 1620. 160. O060600300071 95. 2. 1640. 160. O060600300072 ENDDATA 16 0 O060600300073 ENDSUBENT 72 0 O060600399999 SUBENT O0606004 20200227 O076O060600400001 BIB 8 30 O060600400002 REACTION ((90-TH-232(P,F),,SIG)/ O060600400003 (92-U-238(P,F),,SIG)) O060600400004 METHOD (FISCT,EXTB) O060600400005 SAMPLE Two pairs of back-to-back targets with layers O060600400006 of Th-232 and U-238, about 200 mu-g/cm**2, O060600400007 were installed at 45 deg. to the beam direction. O060600400008 Th-232 target composition: Th-232 - 100%. O060600400009 U-238 target composition: O060600400010 U-234 - 0.0003%, O060600400011 U-235 - 0.0003%, O060600400012 U-236 - 0.0003%, O060600400013 U-238 - 99.999%. O060600400014 DETECTOR (THRES) Thin-film breakdown counters of fission O060600400015 fragments, placed on both sides of the target pair in O060600400016 order to detect the fragments of each nuclide O060600400017 separately. The relative calibration of the detectors O060600400018 was performed with the use of double-sided U-238 O060600400019 targets irradiated by protons with the same energy as O060600400020 for the main measurements. O060600400021 CORRECTION Performed: beam energy degradation in the targets and O060600400022 the detectors, difference in angular O060600400023 anisotropy of fission for the nuclides under study. O060600400024 Negligible: fission induced by background neutrons. O060600400025 ERR-ANALYS (ERR-T) The quoted errors include the uncertainty of O060600400026 the weight of the main and calibration targets, O060600400027 the inhomogeneity of the layer thickness for the main O060600400028 and calibration targets, and the statistics of fission O060600400029 events in the main and calibration measurements. O060600400030 STATUS (TABLE) From tabl.1 of the 91GAUSSG,214,1991 O060600400031 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060600400032 ENDBIB 30 0 O060600400033 COMMON 2 3 O060600400034 EN-ERR ERR-T O060600400035 MEV PER-CENT O060600400036 2. 9. O060600400037 ENDCOMMON 3 0 O060600400038 DATA 2 11 O060600400039 EN DATA O060600400040 MEV NO-DIM O060600400041 24. 0.75 O060600400042 27. 0.74 O060600400043 29. 0.77 O060600400044 34. 0.84 O060600400045 37. 0.84 O060600400046 42. 0.83 O060600400047 49. 0.85 O060600400048 54. 0.84 O060600400049 59. 0.81 O060600400050 69. 0.85 O060600400051 78. 0.86 O060600400052 ENDDATA 13 0 O060600400053 ENDSUBENT 52 0 O060600499999 SUBENT O0606005 20200227 O076O060600500001 BIB 8 34 O060600500002 REACTION ((92-U-233(P,F),,SIG)/ O060600500003 (92-U-238(P,F),,SIG)) O060600500004 METHOD (FISCT,EXTB) O060600500005 SAMPLE Two pairs of back-to-back targets with layers O060600500006 of U-233 and U-238, about 200 mu-g/cm**2, O060600500007 were installed at 45 deg. To the beam direction. O060600500008 U-233 target composition: O060600500009 U-233 - 98.11%, O060600500010 U-234 - 0.41%, O060600500011 U-235 - 0.025%, O060600500012 U-238 - 1.45%. O060600500013 U-238 target composition: O060600500014 U-234 - 0.0003%, O060600500015 U-235 - 0.0003%, O060600500016 U-236 - 0.0003%, O060600500017 U-238 - 99.999%. O060600500018 DETECTOR (THRES) Thin-film breakdown counters of fission O060600500019 fragments, placed on both sides of the target pair in O060600500020 order to detect the fragments of each nuclide O060600500021 separately. The relative calibration of the detectors O060600500022 was performed with the use of double-sided U-238 O060600500023 targets irradiated by protons with the same energy as O060600500024 for the main measurements. O060600500025 CORRECTION Performed: beam energy degradation in the targets and O060600500026 the detectors, difference in angular O060600500027 anisotropy of fission for the nuclides under study. O060600500028 Negligible: fission induced by background neutrons. O060600500029 ERR-ANALYS (ERR-T) The quoted errors include the uncertainty of O060600500030 the weight of the main and calibration targets, O060600500031 the inhomogeneity of the layer thickness for the main O060600500032 and calibration targets, and the statistics of fission O060600500033 events in the main and calibration measurements. O060600500034 STATUS (TABLE) From tabl.1 of the 91GAUSSG,214,1991 O060600500035 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060600500036 ENDBIB 34 0 O060600500037 COMMON 2 3 O060600500038 EN-ERR ERR-T O060600500039 MEV PER-CENT O060600500040 2. 9. O060600500041 ENDCOMMON 3 0 O060600500042 DATA 2 11 O060600500043 EN DATA O060600500044 MEV NO-DIM O060600500045 24. 1.16 O060600500046 27. 1.14 O060600500047 29. 1.14 O060600500048 34. 1.08 O060600500049 37. 1.09 O060600500050 42. 1.1 O060600500051 49. 1.09 O060600500052 54. 1.08 O060600500053 59. 1.11 O060600500054 69. 1.06 O060600500055 78. 1.18 O060600500056 ENDDATA 13 0 O060600500057 ENDSUBENT 56 0 O060600599999 SUBENT O0606006 20200227 O076O060600600001 BIB 8 34 O060600600002 REACTION ((92-U-235(P,F),,SIG)/ O060600600003 (92-U-238(P,F),,SIG)) O060600600004 METHOD (FISCT,EXTB) O060600600005 SAMPLE Two pairs of back-to-back targets with layers O060600600006 of U-235 and U-238, about 200 mu-g/cm**2, O060600600007 were installed at 45 deg. to the beam direction. O060600600008 U-235 target composition: O060600600009 U-234 - 0.0020%, O060600600010 U-235 - 99.992%, O060600600011 U-236 - 0.0040%, O060600600012 U-238 - 0.0020%. O060600600013 U-238 target composition: O060600600014 U-234 - 0.0003%, O060600600015 U-235 - 0.0003%, O060600600016 U-236 - 0.0003%, O060600600017 U-238 - 99.999%. O060600600018 DETECTOR (THRES). Thin-film breakdown counters of fission O060600600019 fragments, placed on both sides of the target pair in O060600600020 order to detect the fragments of each nuclide O060600600021 separately. The relative calibration of the detectors O060600600022 was performed with the use of double-sided U-238 O060600600023 targets irradiated by protons with the same energy as O060600600024 for the main measurements. O060600600025 CORRECTION Performed: beam energy degradation in the targets and O060600600026 the detectors, difference in angular O060600600027 anisotropy of fission for the nuclides under study. O060600600028 Negligible: fission induced by background neutrons. O060600600029 ERR-ANALYS (ERR-T) The quoted errors include the uncertainty of O060600600030 the weight of the main and calibration targets, O060600600031 the inhomogeneity of the layer thickness for the main O060600600032 and calibration targets, and the statistics of fission O060600600033 events in the main and calibration measurements. O060600600034 STATUS (TABLE) From tabl.1 of the 91GAUSSG,214,1991 O060600600035 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060600600036 ENDBIB 34 0 O060600600037 COMMON 2 3 O060600600038 EN-ERR ERR-T O060600600039 MEV PER-CENT O060600600040 2. 9. O060600600041 ENDCOMMON 3 0 O060600600042 DATA 2 9 O060600600043 EN DATA O060600600044 MEV NO-DIM O060600600045 24. 1.08 O060600600046 27. 1.06 O060600600047 29. 1. O060600600048 34. 1.03 O060600600049 42. 0.95 O060600600050 49. 1.05 O060600600051 54. 0.97 O060600600052 59. 1.04 O060600600053 69. 1.01 O060600600054 ENDDATA 11 0 O060600600055 ENDSUBENT 54 0 O060600699999 SUBENT O0606007 20200227 O076O060600700001 BIB 8 34 O060600700002 REACTION ((93-NP-237(P,F),,SIG)/ O060600700003 (92-U-238(P,F),,SIG)) O060600700004 METHOD (FISCT,EXTB) O060600700005 SAMPLE Two pairs of back-to-back targets with layers O060600700006 of Np-237 and U-238, about 200 mu-g/cm**2, O060600700007 were installed at 45 deg. to the beam direction. O060600700008 Np-237 target composition: O060600700009 Np-237 - 99.834%, O060600700010 Pu-238 - 0.15%, O060600700011 Pu-239 - 0.016%. O060600700012 U-238 target composition: O060600700013 U-234 - 0.0003%, O060600700014 U-235 - 0.0003%, O060600700015 U-236 - 0.0003%, O060600700016 U-238 - 99.999%. O060600700017 DETECTOR (THRES). Thin-film breakdown counters of fission O060600700018 fragments, placed on both sides of the target pair in O060600700019 order to detect the fragments of each nuclide O060600700020 separately. The relative calibration of the detectors O060600700021 was performed with the use of double-sided U-238 O060600700022 targets irradiated by protons with the same energy as O060600700023 for the main measurements. O060600700024 CORRECTION Performed: beam energy degradation in the targets and O060600700025 the detectors, difference in angular O060600700026 anisotropy of fission for the nuclides under study. O060600700027 Negligible: fission induced by background neutrons. O060600700028 ERR-ANALYS (ERR-T) The quoted errors include the uncertainty of O060600700029 the weight of the main and calibration targets, O060600700030 the inhomogeneity of the layer thickness for the main O060600700031 and calibration targets, and the statistics of fission O060600700032 events in the main and calibration measurements. O060600700033 STATUS (TABLE) From tabl.1 of the 91GAUSSG,214,1991 O060600700034 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060600700035 Err-analys updated. O060600700036 ENDBIB 34 0 O060600700037 COMMON 2 3 O060600700038 EN-ERR ERR-T O060600700039 MEV PER-CENT O060600700040 2. 9. O060600700041 ENDCOMMON 3 0 O060600700042 DATA 2 10 O060600700043 EN DATA O060600700044 MEV NO-DIM O060600700045 24. 1.06 O060600700046 27. 1.12 O060600700047 29. 1.08 O060600700048 34. 1.05 O060600700049 37. 1.06 O060600700050 42. 0.98 O060600700051 49. 1.05 O060600700052 54. 1.04 O060600700053 59. 1.09 O060600700054 69. 0.99 O060600700055 ENDDATA 12 0 O060600700056 ENDSUBENT 55 0 O060600799999 SUBENT O0606008 20200227 O076O060600800001 BIB 8 35 O060600800002 REACTION ((94-PU-239(P,F),,SIG)/ O060600800003 (92-U-238(P,F),,SIG)) O060600800004 METHOD (FISCT,EXTB) O060600800005 SAMPLE Two pairs of back-to-back targets with layers O060600800006 of Pu-239 and U-238, about 200 mu-g/cm**2, O060600800007 were installed at 45 deg. to the beam direction. O060600800008 Pu-239 target composition: O060600800009 Pu-238 - 0.063%, O060600800010 Pu-239 - 99.764%, O060600800011 Pu-240 - 0.167%, O060600800012 Pu-241 - 0.003%, O060600800013 Pu-242 - 0.003%. O060600800014 U-238 target composition: O060600800015 U-234 - 0.0003%, O060600800016 U-235 - 0.0003%, O060600800017 U-236 - 0.0003%, O060600800018 U-238 - 99.999%. O060600800019 DETECTOR (THRES). Thin-film breakdown counters of fission O060600800020 fragments, placed on both sides of the target pair in O060600800021 order to detect the fragments of each nuclide O060600800022 separately. The relative calibration of the detectors O060600800023 was performed with the use of double-sided U-238 O060600800024 targets irradiated by protons with the same energy as O060600800025 for the main measurements. O060600800026 CORRECTION Performed: beam energy degradation in the targets and O060600800027 the detectors, difference in angular O060600800028 anisotropy of fission for the nuclides under study. O060600800029 Negligible: fission induced by background neutrons. O060600800030 ERR-ANALYS (ERR-T). The quoted errors include the uncertainty of O060600800031 the weight of the main and calibration targets, O060600800032 the inhomogeneity of the layer thickness for the main O060600800033 and calibration targets, and the statistics of fission O060600800034 events in the main and calibration measurements. O060600800035 STATUS (TABLE) From tabl.1 of the 91GAUSSG,214,1991 O060600800036 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060600800037 ENDBIB 35 0 O060600800038 COMMON 2 3 O060600800039 EN-ERR ERR-T O060600800040 MEV PER-CENT O060600800041 2. 9. O060600800042 ENDCOMMON 3 0 O060600800043 DATA 2 11 O060600800044 EN DATA O060600800045 MEV NO-DIM O060600800046 24. 1.13 O060600800047 27. 1.13 O060600800048 29. 1.1 O060600800049 34. 1.12 O060600800050 37. 1.17 O060600800051 42. 1.14 O060600800052 49. 1.16 O060600800053 54. 1.15 O060600800054 59. 1.16 O060600800055 69. 1.13 O060600800056 78. 1.09 O060600800057 ENDDATA 13 0 O060600800058 ENDSUBENT 57 0 O060600899999 SUBENT O0606009 20200227 O076O060600900001 BIB 8 34 O060600900002 REACTION ((95-AM-243(P,F),,SIG)/ O060600900003 (92-U-238(P,F),,SIG)) O060600900004 METHOD (FISCT,EXTB) O060600900005 SAMPLE Two pairs of back-to-back targets with layers O060600900006 of Am-243 and U-238, about 200 mu-g/cm**2, O060600900007 were installed at 45 deg. to the beam direction. O060600900008 Am-243 target composition: O060600900009 Am-243 - 97.4%, O060600900010 Am-241 - 2.6%, O060600900011 cm-244 - 0.01%, O060600900012 cm-242 - 0.00005%. O060600900013 U-238 target composition: O060600900014 U-234 - 0.0003%, O060600900015 U-235 - 0.0003%, O060600900016 U-236 - 0.0003%, O060600900017 U-238 - 99.999%. O060600900018 DETECTOR (THRES) Thin-film breakdown counters of fission O060600900019 fragments, placed on both sides of the target pair in O060600900020 order to detect the fragments of each nuclide O060600900021 separately. The relative calibration of the detectors O060600900022 was performed with the use of double-sided U-238 O060600900023 targets irradiated by protons with the same energy as O060600900024 for the main measurements. O060600900025 CORRECTION Performed: beam energy degradation in the targets and O060600900026 the detectors, difference in angular O060600900027 anisotropy of fission for the nuclides under study. O060600900028 Negligible: fission induced by background neutrons. O060600900029 ERR-ANALYS (ERR-T) The quoted errors include the uncertainty of O060600900030 the weight of the main and calibration targets, O060600900031 the inhomogeneity of the layer thickness for the main O060600900032 and calibration targets, and the statistics of fission O060600900033 events in the main and calibration measurements. O060600900034 STATUS (TABLE) From tabl.1 of the 91GAUSSG,214,1991 O060600900035 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060600900036 ENDBIB 34 0 O060600900037 COMMON 2 3 O060600900038 EN-ERR ERR-T O060600900039 MEV PER-CENT O060600900040 2. 9. O060600900041 ENDCOMMON 3 0 O060600900042 DATA 2 10 O060600900043 EN DATA O060600900044 MEV NO-DIM O060600900045 24. 1.16 O060600900046 27. 1.09 O060600900047 29. 1.1 O060600900048 34. 1.12 O060600900049 37. 1.09 O060600900050 42. 1.12 O060600900051 49. 1.12 O060600900052 54. 1.2 O060600900053 59. 1.2 O060600900054 69. 1.21 O060600900055 ENDDATA 12 0 O060600900056 ENDSUBENT 55 0 O060600999999 SUBENT O0606010 20200227 O076O060601000001 BIB 8 21 O060601000002 REACTION (92-U-238(P,F),,DA,FF,RSD) O060601000003 REL-REF (A,O0527001,J.R.Boyce+,J,PR/C,10,231,1974) O060601000004 (A,,J.W.Meadows,J,PR,110,1109,1958) O060601000005 (A,A0047001,O.E.Shigaev+,R,RI-17,1973) In Russian. O060601000006 METHOD (FISCT,EXTB,SITA). O060601000007 SAMPLE A U-238 layer of about 150-200 mu-g/cm**2 was O060601000008 obtained by vacuum evaporation to an aluminium oxide O060601000009 backing about 150 mu-g/cm2 thick. The target O060601000010 was installed at 45 degrees to the beam axis. O060601000011 The target had a small admixture of 252-Cf to provide O060601000012 calibration of the detectors simultaneously to the O060601000013 beam measurements. O060601000014 DETECTOR (THRES) Thin-film breakdown counters of fission O060601000015 fragments, placed at 0,30,60,90,90,120,150 and 180 deg.O060601000016 to the beam direction. O060601000017 ERR-ANALYS (ERR-T) The quoted uncertainties are obtained in O060601000018 fitting the angular distributions by the least-square O060601000019 method. O060601000020 STATUS (TABLE) Data from the authors. O060601000021 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060601000022 REL-REF updated. O060601000023 ENDBIB 21 0 O060601000024 COMMON 2 3 O060601000025 ANG-CM EN-ERR O060601000026 ADEG MEV O060601000027 0. 2. O060601000028 ENDCOMMON 3 0 O060601000029 DATA 3 6 O060601000030 EN DATA-CM ERR-T O060601000031 MEV NO-DIM NO-DIM O060601000032 23. 1.11 0.02 O060601000033 34. 1.13 0.04 O060601000034 45. 1.21 0.05 O060601000035 62. 1.16 0.04 O060601000036 75. 1.125 0.017 O060601000037 92. 1.088 0.014 O060601000038 ENDDATA 8 0 O060601000039 ENDSUBENT 38 0 O060601099999 SUBENT O0606011 20200227 O076O060601100001 BIB 7 17 O060601100002 REACTION (92-U-235(P,F),,DA,FF,RSD) O060601100003 METHOD (FISCT,EXTB,SITA). O060601100004 SAMPLE A U-235 layer of about 150-200 mu-g/cm**2 was O060601100005 obtained by vacuum evaporation to an aluminium oxide O060601100006 backing about 150 mu-g/cm**2 thick. The target O060601100007 was installed at 45 degrees to the beam axis. O060601100008 The target had a small admixture of 252-Cf to provide O060601100009 calibration of the detectors simultaneously to the O060601100010 beam measurements. O060601100011 DETECTOR (THRES) Thin-film breakdown counters of fission O060601100012 fragments, placed at 0,30,60,90,90,120,150 and 180 deg.O060601100013 to the beam direction. O060601100014 ERR-ANALYS (ERR-T) The quoted uncertainties are obtained in O060601100015 fitting the angular distributions by the least-square O060601100016 method. O060601100017 STATUS (TABLE) Data from the authors. O060601100018 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060601100019 ENDBIB 17 0 O060601100020 COMMON 2 3 O060601100021 ANG-CM EN-ERR O060601100022 ADEG MEV O060601100023 0. 2. O060601100024 ENDCOMMON 3 0 O060601100025 DATA 3 6 O060601100026 EN DATA-CM ERR-T O060601100027 MEV NO-DIM NO-DIM O060601100028 23. 1.05 0.03 O060601100029 34. 1.1 0.03 O060601100030 45. 1.11 0.03 O060601100031 62. 1.101 0.017 O060601100032 75. 1.09 0.03 O060601100033 92. 1.051 0.009 O060601100034 ENDDATA 8 0 O060601100035 ENDSUBENT 34 0 O060601199999 SUBENT O0606012 20200227 O076O060601200001 BIB 7 17 O060601200002 REACTION (92-U-233(P,F),,DA,FF,RSD) O060601200003 METHOD (FISCT,EXTB,SITA). O060601200004 SAMPLE A U-233 layer of about 150-200 mu-g/cm**2 was O060601200005 obtained by vacuum evaporation to an aluminium oxide O060601200006 backing about 150 mu-g/cm**2 thick. The target O060601200007 was installed at 45 degrees to the beam axis. O060601200008 The target had a small admixture of 252-Cf to provide O060601200009 calibration of the detectors simultaneously to the O060601200010 beam measurements. O060601200011 DETECTOR (THRES) Thin-film breakdown counters of fission O060601200012 fragments, placed at 0,30,60,90,90,120,150 and 180 deg.O060601200013 to the beam direction. O060601200014 ERR-ANALYS (ERR-T) The quoted uncertainties are obtained in O060601200015 fitting the angular distributions by the least-square O060601200016 method. O060601200017 STATUS (TABLE) Data from the authors. O060601200018 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060601200019 ENDBIB 17 0 O060601200020 COMMON 2 3 O060601200021 ANG-CM EN-ERR O060601200022 ADEG MEV O060601200023 0. 2. O060601200024 ENDCOMMON 3 0 O060601200025 DATA 3 6 O060601200026 EN DATA-CM ERR-T O060601200027 MEV NO-DIM NO-DIM O060601200028 23. 1.07 0.04 O060601200029 34. 1.09 0.04 O060601200030 45. 1.13 0.02 O060601200031 62. 1.08 0.03 O060601200032 75. 1.095 0.015 O060601200033 92. 1.065 0.005 O060601200034 ENDDATA 8 0 O060601200035 ENDSUBENT 34 0 O060601299999 SUBENT O0606013 20200227 O076O060601300001 BIB 7 17 O060601300002 REACTION (90-TH-232(P,F),,DA,FF,RSD) O060601300003 METHOD (FISCT,EXTB,SITA) O060601300004 SAMPLE A Th-232 layer of about 150-200 mu-g/cm**2 was O060601300005 obtained by vacuum evaporation to an aluminium oxide O060601300006 backing about 150 mu-g/cm**2 thick. The target O060601300007 was installed at 45 degrees to the beam axis. O060601300008 The target had a small admixture of 252-Cf to provide O060601300009 calibration of the detectors simultaneously to the O060601300010 beam measurements. O060601300011 DETECTOR (THRES) Thin-film breakdown counters of fission O060601300012 fragments, placed at 0,30,60,90,90,120,150 and 180 deg.O060601300013 to the beam direction. O060601300014 ERR-ANALYS (ERR-T) The quoted uncertainties are obtained in O060601300015 fitting the angular distributions by the least-square O060601300016 method. O060601300017 STATUS (TABLE) Data from the authors. O060601300018 HISTORY (20200227U) SD: SF9=EXP deleted from REACTION code. O060601300019 ENDBIB 17 0 O060601300020 COMMON 2 3 O060601300021 ANG-CM EN-ERR O060601300022 ADEG MEV O060601300023 0. 2. O060601300024 ENDCOMMON 3 0 O060601300025 DATA 3 6 O060601300026 EN DATA-CM ERR-T O060601300027 MEV NO-DIM NO-DIM O060601300028 23. 1.16 0.03 O060601300029 34. 1.25 0.04 O060601300030 45. 1.24 0.03 O060601300031 62. 1.175 0.018 O060601300032 75. 1.121 0.012 O060601300033 92. 1.16 0.04 O060601300034 ENDDATA 8 0 O060601300035 ENDSUBENT 34 0 O060601399999 ENDENTRY 13 0 O060699999999