ENTRY O1386 20221224 O092O1386 0 1 SUBENT O1386001 20221224 O092O1386 1 1 BIB 14 44 O1386 1 2 TITLE Yield of near-target product interaction of 47 MeV/A O1386 1 3 12-C ions with bismuth targets O1386 1 4 AUTHOR (Zongwei Li, Zhizheng Zhao, Weifan Yang, Xianghua Zeng)O1386 1 5 INSTITUTE (3CPRIMP) O1386 1 6 REFERENCE (J,JRN/L,212,409,1996) O1386 1 7 (J,CST,44,513,2010) in Chinese lang. - same data of Au O1386 1 8 REL-REF (R,,D.Z.Molzahn,J,JRC,80,109,1983) The isotopic O1386 1 9 distributions of Po, Bi and the formation cross O1386 1 10 sections of At, Rn, with the reaction of 86 MeV/A O1386 1 11 12-C bombarding Bi and thin Pb targets. O1386 1 12 SAMPLE The targets were 1.28 g/cm2 Bi2-O3 powders. O1386 1 13 According to calculation of the authors, 12-C particlesO1386 1 14 were completely stopped in the target powders. O1386 1 15 The Al foils of 6.8 um thickness were installed in O1386 1 16 front of the targets. O1386 1 17 MONITOR (13-AL-27(6-C-12,X)11-NA-24,CUM,SIG) O1386 1 18 DETECTOR (HPGE) To measure the gamma-decay spectra of the O1386 1 19 separated sources and unseparated target powders. O1386 1 20 FACILITY (ACCEL,3CPRIMP) HIRFL O1386 1 21 METHOD (EXTB) The average beam current intensity of 47 MeV/A O1386 1 22 12-C was 8 nanoAmperes. The irradiation beam time was O1386 1 23 Separated for several sections in order to make mother O1386 1 24 - daughter decay modifications and to obtain the O1386 1 25 average production cross sections of residues. O1386 1 26 (BCINT) The beam current was monitored by a Faraday O1386 1 27 cup. Both methods of beam current measurements gave O1386 1 28 the same results within the limit of error. O1386 1 29 (ACTIV) The whole irradiation time was 6.8 hours. O1386 1 30 (GSPEC) Off-line gamma-spectroscopic method. O1386 1 31 (CHSEP) Reaction products from a part irradiated targetO1386 1 32 were separated by a standard radiochemical separation O1386 1 33 method. O1386 1 34 ANALYSIS (DECAY) O1386 1 35 CORRECTION Decay correction of the experimental values was O1386 1 36 provided by the measured yields of mother isotopes. O1386 1 37 Partial isotope cross-sections were obtained from the O1386 1 38 correction of mother decay effects, similar to the O1386 1 39 method of decay correction of mass distribution and O1386 1 40 charge distribution in order to get independent yields.O1386 1 41 STATUS (TABLE) Tbl.1 from O1386 1 42 J.Radioanal.Nucl.Chem.,Let.,212(1996)409 O1386 1 43 HISTORY (20060421C) By F.Ch O1386 1 44 (20060423U) Last checking has been done. O1386 1 45 (20221224A) SD: Ref. added. Correction in Subent 002. O1386 1 46 ENDBIB 44 0 O1386 1 47 NOCOMMON 0 0 O1386 1 48 ENDSUBENT 47 0 O1386 199999 SUBENT O1386002 20221224 O092O1386 2 1 BIB 5 8 O1386 2 2 REACTION (83-BI-209(6-C-12,X)ELEM/MASS,,SIG) O1386 2 3 MISC-COL (MISC) The measured cross section before needed O1386 2 4 correction mother decay were included. O1386 2 5 FLAG (1.) The cross section includes isomer state productionO1386 2 6 too. O1386 2 7 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1386 2 8 (MISC-ERR) No information about source of uncertainty O1386 2 9 HISTORY (20221224A) SD: SF5=IND deleted from REACTION code. O1386 2 10 ENDBIB 8 0 O1386 2 11 COMMON 1 3 O1386 2 12 EN O1386 2 13 MEV O1386 2 14 564. O1386 2 15 ENDCOMMON 3 0 O1386 2 16 DATA 8 21 O1386 2 17 ELEMENT MASS ISOMER DATA DATA-ERR MISC O1386 2 18 MISC-ERR FLAG O1386 2 19 NO-DIM NO-DIM NO-DIM MB MB MB O1386 2 20 MB NO-DIM O1386 2 21 78. 185. 2.2 0.8 2.3O1386 2 22 0.9 O1386 2 23 78. 186. 5.3 0.4 6.O1386 2 24 0.5 O1386 2 25 78. 187. 5.9 0.6 7.2O1386 2 26 0.4 O1386 2 27 78. 188. 4.2 0.4 5.7O1386 2 28 0.5 O1386 2 29 78. 189. 6.3 0.6 10.1O1386 2 30 0.7 O1386 2 31 78. 191. 3.6 0.4 6.8O1386 2 32 0.6 O1386 2 33 78. 197. 1. 0.27 0.04 0.27O1386 2 34 0.04 O1386 2 35 79. 191. 7.5 11.7O1386 2 36 2.4 O1386 2 37 79. 192. 7.1 1.9 9.7O1386 2 38 2.6 O1386 2 39 79. 193. 6.1 1.8 9.8O1386 2 40 2.8 O1386 2 41 79. 194. 0.49 0.1 0.49O1386 2 42 0.1 O1386 2 43 79. 195. 2.5 0.8 4.1O1386 2 44 0.7 O1386 2 45 79. 196. 0.26 0.08 0.26O1386 2 46 0.08 1. O1386 2 47 79. 198. 0.16 0.06 0.16O1386 2 48 0.06 1. O1386 2 49 79. 199. 0.18 0.02 0.19O1386 2 50 0.2 O1386 2 51 80. 191. 4.7 2. 6.7O1386 2 52 2.7 O1386 2 53 80. 192. 9.1 0.6 11.6O1386 2 54 0.8 O1386 2 55 80. 193. 8.4 0.7 8.5O1386 2 56 0.8 1. O1386 2 57 80. 195. 12.7 1.3 13.5O1386 2 58 1. 1. O1386 2 59 80. 197. 1. 0.78 0.1 0.78O1386 2 60 0.1 O1386 2 61 80. 203. 1.9 0.4 1.9O1386 2 62 0.4 O1386 2 63 ENDDATA 46 0 O1386 2 64 ENDSUBENT 63 0 O1386 299999 ENDENTRY 2 0 O138699999999