ENTRY A0383 20220802 A101A038300000001 SUBENT A0383001 20220802 A101A038300100001 BIB 8 15 A038300100002 TITLE Radiative capture of protons by the deformed nuclide A038300100003 Th-232 A038300100004 AUTHOR (J.Szerypo,B.Szweryn,P.Hornshoj,H.Loft Nielsen, A038300100005 M.Luontama) A038300100006 INSTITUTE (3POLWWA,2DENAAU,2SF JYV) A038300100007 REFERENCE (J,ZP/A,323,97,1986) A038300100008 REL-REF (N,,J.Szerypo+,J,ZP/A,324,439,1986) Theory. A038300100009 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A038300100010 ADD-RES The results are compared with the excitation function A038300100011 for Yb-176(p,gamma)Lu-177 and the prediction of the A038300100012 CN-model. A038300100013 HISTORY (19880525C) A038300100014 (19880705U) A038300100015 (20220802A) SD:Updated to new date formats, lower case.A038300100016 Corrections in all Subents. A038300100017 ENDBIB 15 0 A038300100018 NOCOMMON 0 0 A038300100019 ENDSUBENT 18 0 A038300199999 SUBENT A0383002 20220802 A101A038300200001 BIB 12 31 A038300200002 REACTION (90-TH-232(P,G)91-PA-233,,SIG) A038300200003 FACILITY (VDG,2DENAAU) For protons energies 7-13 MeV. A038300200004 (CYCLO,3POLWWA) For protons energies 13-18 MeV. A038300200005 (CYCLO,2SF JYV) For protons energies 20 MeV. A038300200006 METHOD (ACTIV,BCINT,SITA) A038300200007 DECAY-DATA (91-PA-233,27.D,DG) A038300200008 MONITOR (90-TH-232(P,N)91-PA-232,,SIG) A038300200009 MONIT-REF (,A.Celler+,J,PS,24,930,1981) A038300200010 DETECTOR (GELI) Coaxial Ge(Li) spectrometers. A038300200011 SAMPLE Self-supporting metallic Th-foils,15 or 32 mg/cm**2 A038300200012 thickness was used. A038300200013 FLAG (1.).Measurements performed in Aarhus. A038300200014 (2.).Measurements performed in Turku. A038300200015 (3.).Measurements performed in Jyvaskyla. A038300200016 COMMENT /By authors/ In the Aarhus and Jyvaskyla measurements A038300200017 the irradiations were performed in vacuum and the A038300200018 beam was dumped away from the target. In the Turku A038300200019 measurements the target was mounted directly on a A038300200020 graphite beam-stop just after a thin steel window whichA038300200021 terminated the beam line. A038300200022 /By authors/ The results Th-232(p,gamma)Pa-233 still A038300200023 had to be corrected for the effects of neutron capture A038300200024 in the target of neutrons produced inside the target A038300200025 volume. The contributing processes are the (p,n), A038300200026 (p,2n), (p,3n) and (p,f) reactions on Th-232. A038300200027 A correction for the influence of the (p,xn) reactionsA038300200028 was calculated with the assumption of a compound A038300200029 nucleus energy spectrum of the neutrons and with the A038300200030 cross sections given in Celler et al.(see MONIT-REF). A038300200031 STATUS (TABLE) Tbl.2 from Zeitschr.Phys.,A323(1986)97 A038300200032 HISTORY (20220802A) SD: SF9=EXP deleted from REACTION code. A038300200033 ENDBIB 31 0 A038300200034 NOCOMMON 0 0 A038300200035 DATA 4 14 A038300200036 EN DATA DATA-ERR FLAG A038300200037 MEV MICRO-B MICRO-B NO-DIM A038300200038 6.85 1.17 0.18 1. A038300200039 7.86 4.82 0.86 1. A038300200040 8.86 17.5 2.4 1. A038300200041 9.86 51.1 7.2 1. A038300200042 10.89 120. 17. 1. A038300200043 11.89 191. 27. 1. A038300200044 12.7 239. 36. 1. A038300200045 12.89 236. 34. 1. A038300200046 13.6 282. 44. 2. A038300200047 14.7 275. 48. 2. A038300200048 15.9 275. 54. 2. A038300200049 16.7 276. 61. 2. A038300200050 17.4 256. 64. 2. A038300200051 19.7 269. 85. 3. A038300200052 ENDDATA 16 0 A038300200053 ENDSUBENT 52 0 A038300299999 SUBENT A0383003 20220802 A101A038300300001 BIB 11 19 A038300300002 REACTION (90-TH-232(P,F),,SIG) A038300300003 FACILITY (CYCLO,2SF JYV) A038300300004 METHOD (SITA) The details of method see REL-REF. A038300300005 SAMPLE Self-supporting 1 mg/cm**2 metallic Th foils were used.A038300300006 MONITOR (90-TH-232(P,INL)90-TH-232,,SIG) A038300300007 MONIT-REF (,A.Celler+,J,PS,24,930,1981) A038300300008 DECAY-MON (90-TH-232,,XR) A038300300009 COMMENT /By authors/ The relative fission cross sections were A038300300010 obtained via a normalization to the K-shell ionization A038300300011 cross sections used also by Celler et.al (see A038300300012 MONIT-REF). The resulting relative fission yield A038300300013 curve was transformed into an absolute excitation A038300300014 function by normalization to the excitation function A038300300015 of Kurcewicz et al., see REL-REF. A038300300016 REL-REF (A,,W.Kurcewicz+,J,ZP/A,306,99,1982) A038300300017 (A,,H.Kudo+,J,PR/C,25,3011,1982) A038300300018 (M,,W.Kurcewicz+,J,ZP/A,306,99,1982) A038300300019 STATUS (TABLE) Tbl.1 from Zeitschr.Phys.,A323(1986)97 A038300300020 HISTORY (20220802A) SD: SF9=EXP deleted from REACTION code. A038300300021 ENDBIB 19 0 A038300300022 NOCOMMON 0 0 A038300300023 DATA 3 13 A038300300024 EN DATA DATA-ERR A038300300025 MEV MB MB A038300300026 9.0 21.0 3.2 A038300300027 10.0 63.2 9.5 A038300300028 11.0 122. 18. A038300300029 12.0 242. 36. A038300300030 12.8 259. 39. A038300300031 14.0 447. 67. A038300300032 15.0 740. 110. A038300300033 16.0 900. 140. A038300300034 16.2 1140. 170. A038300300035 17.0 1200. 180. A038300300036 18.0 1420. 210. A038300300037 18.8 1410. 210. A038300300038 19.8 1470. 220. A038300300039 ENDDATA 15 0 A038300300040 ENDSUBENT 39 0 A038300399999 ENDENTRY 3 0 A038399999999