ENTRY O0602 20230406 O095O0602 0 1 SUBENT O0602001 20230406 O095O0602 1 1 BIB 13 40 O0602 1 2 TITLE The binary and ternary fission of thorium, O0602 1 3 lead and platinum induced by 12.2 GeV protons O0602 1 4 AUTHOR (Z.Todorovic,R.Antanasijevic,M.Juric) O0602 1 5 INSTITUTE (3SRBBKB) O0602 1 6 FACILITY (SYNCY,1USAANL) O0602 1 7 REFERENCE (J,ZP,261,329,1973) O0602 1 8 SAMPLE Natural Th,Pb and Pt were evaporated in vacuum O0602 1 9 onto the detector surface. Target thickness was O0602 1 10 300-800 Angstrom. The surface of the sample was O0602 1 11 parallel to the proton beam. O0602 1 12 METHOD (FISCT) O0602 1 13 DETECTOR (TRD) Makrofol polycarbonate detectors consisted of O0602 1 14 two sheets of a size of 3*4*0.02 cm forming a sandwich.O0602 1 15 Detector was sensitive to fragments with A>=16. O0602 1 16 Heavy reaction fragments were stopped inside the O0602 1 17 Makrofol sheets and could thus be detected in O0602 1 18 a 4Pi geometry. O0602 1 19 CORRECTION Performed: Loss of events of about 2% due to removal O0602 1 20 of the detector material in the course of chemical O0602 1 21 treatment. O0602 1 22 Negligible: Casual coincidences between two individualO0602 1 23 tracks and an individual track with binary events. O0602 1 24 ERR-ANALYS (ERR-1,,10.) The errors in determinations of the O0602 1 25 target thicknesses O0602 1 26 (ERR-2,,10.) the uncertainty in the proton flux O0602 1 27 ADD-RES (RANGE) O0602 1 28 The range ratio distributions for two-prong events. O0602 1 29 the distributions of the space angle between two O0602 1 30 tracks for three-prong events. O0602 1 31 COMMENT - By Authors - The binary and ternary fission induced O0602 1 32 by high-energy particles is defined as a decay of the O0602 1 33 nucleus into two resp. three fragments of approximatelyO0602 1 34 equal masses. O0602 1 35 HISTORY (19971206C) AP: By Khlopin's Institute. O0602 1 36 (19971212A) Reactions and Data-Sections are corrected. O0602 1 37 (19980424A) AP: REL-REF for Pb data are added. O0602 1 38 (20000420U) Last checking has been done. O0602 1 39 (20000424A) DATE is corrected O0602 1 40 (20230406A) SD: Corrections in all Subents. Subent 003 O0602 1 41 was split in two. O0602 1 42 ENDBIB 40 0 O0602 1 43 NOCOMMON 0 0 O0602 1 44 ENDSUBENT 43 0 O0602 199999 SUBENT O0602002 20230406 O095O0602 2 1 BIB 4 9 O0602 2 2 REACTION 1(90-TH-232(P,F),,SIG) O0602 2 3 2(90-TH-232(P,F),TER,SIG) O0602 2 4 3(90-TH-232(P,F),TER/BIN,SIG/RAT) O0602 2 5 ERR-ANALYS (ERR-T) Statistics of the fission events, the O0602 2 6 uncertainties in the target thickness and the flux O0602 2 7 determinations. O0602 2 8 (ERR-S) Statistics of the fission events. O0602 2 9 STATUS (TABLE) Table 1 from Z.Physik,261(1973)329 O0602 2 10 HISTORY (20230406A) SD: SD: SF9=EXP deleted from REACTION code.O0602 2 11 ENDBIB 9 0 O0602 2 12 NOCOMMON 0 0 O0602 2 13 DATA 7 1 O0602 2 14 EN DATA 1ERR-T 1DATA 2ERR-T 2DATA 3O0602 2 15 ERR-S 3 O0602 2 16 GEV MB MB MB MB NO-DIM O0602 2 17 NO-DIM O0602 2 18 12.2 420. 63. 8.4 1.7 0.02O0602 2 19 0.003 O0602 2 20 ENDDATA 6 0 O0602 2 21 ENDSUBENT 20 0 O0602 299999 SUBENT O0602003 20230406 O095O0602 3 1 BIB 5 11 O0602 3 2 REACTION 1(82-PB-0(P,F),,SIG) O0602 3 3 2(82-PB-0(P,F),TER,SIG) O0602 3 4 REL-REF (A,O0221003,G.Remy+,J,NP/A,163,583,1971) O0602 3 5 (A,O0605006,R.Brandt+,J,RPA,7,243,1972) A more recent O0602 3 6 reference than given by authors. O0602 3 7 ERR-ANALYS (ERR-T) Statistics of the fission events, the O0602 3 8 uncertainties in the target thickness and the flux O0602 3 9 determinations. O0602 3 10 STATUS (TABLE) Text on pp.334, 335 of Z.Physik,261(1973)329 O0602 3 11 HISTORY (20230406A) SD: SD: SF9=EXP deleted from REACTION code.O0602 3 12 Part of data moved to Subent 005. O0602 3 13 ENDBIB 11 0 O0602 3 14 NOCOMMON 0 0 O0602 3 15 DATA 5 1 O0602 3 16 EN DATA 1ERR-T 1DATA 2ERR-T 2 O0602 3 17 GEV MB MB MB MB O0602 3 18 12.2 123. 18. 3.4 1. O0602 3 19 ENDDATA 3 0 O0602 3 20 ENDSUBENT 19 0 O0602 399999 SUBENT O0602004 20230406 O095O0602 4 1 BIB 4 9 O0602 4 2 REACTION 1(78-PT-0(P,F),,SIG) O0602 4 3 2(78-PT-0(P,F),TER,SIG) O0602 4 4 3(78-PT-0(P,F),TER/BIN,SIG/RAT) O0602 4 5 ERR-ANALYS (ERR-T) Statistics of the fission events, the O0602 4 6 uncertainties in the target thickness and the flux O0602 4 7 determinations. O0602 4 8 (ERR-S) Statistics of the fission events. O0602 4 9 STATUS (TABLE) Table 1 from Z.Physik,261(1973)329 O0602 4 10 HISTORY (20230406A) SD: SD: SF9=EXP deleted from REACTION code.O0602 4 11 ENDBIB 9 0 O0602 4 12 NOCOMMON 0 0 O0602 4 13 DATA 7 1 O0602 4 14 EN DATA 1ERR-T 1DATA 2ERR-T 2DATA 3O0602 4 15 ERR-S 3 O0602 4 16 GEV MB MB MB MB NO-DIM O0602 4 17 NO-DIM O0602 4 18 12.2 64. 10. 2. 0.4 0.031O0602 4 19 0.003 O0602 4 20 ENDDATA 6 0 O0602 4 21 ENDSUBENT 20 0 O0602 499999 SUBENT O0602005 20230406 O095O0602 5 1 BIB 4 5 O0602 5 2 REACTION (82-PB-0(P,F),TER/BIN,SIG/RAT) O0602 5 3 ERR-ANALYS (ERR-S) Statistics of the fission events. O0602 5 4 STATUS (CURVE) Fig.4 from Z.Physik,261(1973)329 O0602 5 5 HISTORY (20230406A) SD: SD: SF9=EXP deleted from REACTION code.O0602 5 6 Part of data moved to Subent 003. O0602 5 7 ENDBIB 5 0 O0602 5 8 NOCOMMON 0 0 O0602 5 9 DATA 3 1 O0602 5 10 EN DATA ERR-S O0602 5 11 GEV NO-DIM NO-DIM O0602 5 12 12.2 0.028 0.004 O0602 5 13 ENDDATA 3 0 O0602 5 14 ENDSUBENT 13 0 O0602 599999 ENDENTRY 5 0 O060299999999