ENTRY D5059 20100303 D072D505900000001 SUBENT D5059001 20100303 D072D505900100001 BIB 11 40 D505900100002 TITLE Analog resonances with Jpi= 3/2- in the 40-Ar(p,g)41-K D505900100003 reaction D505900100004 AUTHOR (A.N.Vodin, I.V.Ushakov, G.E.Tuller, L.P.Korda, D505900100005 V.T.Bykov, A.O.Rastrepina) D505900100006 INSTITUTE (4UKRKFT) D505900100007 REFERENCE (J,IZV,72,(3),413,2008) D505900100008 (J,BAS,72,385,2008) D505900100009 #NSR:2008VO03 D505900100010 #doi:10.3103/s11954-008-3024-x D505900100011 FACILITY (VDG,4UKRUFT)Electrostatic accelerator with maximum D505900100012 energy 4 MeV and energy dispersion of beam 400 eV. D505900100013 A beam current was 10-15 microA. D505900100014 SAMPLE The isotopic target of 40Ar is produced by hammering D505900100015 of 40Ar+ ions in tantalum backing directly in D505900100016 electromagnetic separator. The target thickness was D505900100017 about 4 keV at proton energy at Ep=2.0 MeV. D505900100018 DETECTOR (GELI) A germanium- lithium detector is used with an D505900100019 active volume of 63 cm**3 and a resolution of 3.0 keV D505900100020 at Eg=1.33 MeV. The detector was calibrated with D505900100021 standard sources and using gamma-rays from reaction D505900100022 27Al(p,gamma)28Si at Ep=991.86 keV. For reduction of D505900100023 the background from low energy gamma-rays the detector D505900100024 was shielded with Pb and Cu. The gamma-rays were D505900100025 detected at angles of 0, 30, 45, 60, 90 degrees D505900100026 concerning proton beam direction. D505900100027 (NAICR) NaI(Tl) detector was used for excitation D505900100028 function measurements and as monitor of gamma D505900100029 radiation. The dimensions of the crystal was D505900100030 diameter 15 x 10 cm. D505900100031 METHOD (GSPEC) D505900100032 ANALYSIS In REACTIONs FCT=1/(2Jp+1)(2Jt+1), D505900100033 where is Jp = spin of incident projectile and D505900100034 Jt = spin of target nucleus. D505900100035 In the formula of resonance strength: D505900100036 g*Gamma(i)Gamma(j)/Gamma(tot) D505900100037 instead of usual statistical weight: D505900100038 g=(2J+1)/(2Jp+1)(2Jt+1), the authors used g=(2J+1) D505900100039 ERR-ANALYS No information. D505900100040 HISTORY (20081020C)UKRNDC D505900100041 (20100303A) SD: ref.of DOI of publ. corrected D505900100042 ENDBIB 40 0 D505900100043 NOCOMMON 0 0 D505900100044 ENDSUBENT 43 0 D505900199999 SUBENT D5059002 20081020 D064D505900200001 BIB 5 8 D505900200002 REACTION 1(18-AR-40(P,0),,WID/STR,,RG)See ANALYSIS in SUB 001 D505900200003 2(18-AR-40(P,G),,WID) D505900200004 3(18-AR-40(P,0),,J) D505900200005 4(18-AR-40(P,0),,PTY) D505900200006 MONITOR (18-AR-40(P,0),,WID/STR) D505900200007 MONIT-REF (,J.J.Smit+,J,SAP,12,74,1989) D505900200008 ADD-RES (STRUC) D505900200009 STATUS (TABLE) tbl.1 D505900200010 ENDBIB 8 0 D505900200011 COMMON 4 3 D505900200012 EN-RES-ERR EN-RES-NRM MONIT MONIT-ERR D505900200013 KEV KEV EV EV D505900200014 1.0 1102. 8.0 0.5 D505900200015 ENDCOMMON 3 0 D505900200016 DATA 6 10 D505900200017 EN-RES DATA 1DATA-ERR 1DATA 2DATA 3DATA 4D505900200018 KEV EV EV EV NO-DIM NO-DIM D505900200019 1087. 2.4 0.4 1.7 D505900200020 1096. 0.4 0.2 D505900200021 1102. 8.0 0.5 3.4 1.5 -1. D505900200022 1109. 2.0 0.3 1.1 D505900200023 1118. 2.2 0.3 D505900200024 1839. 3.9 0.4 1.0 1.5 -1. D505900200025 1842. 3.3 0.3 0.8 1.5 -1. D505900200026 1859. 0.8 0.2 0.2 1.5 -1. D505900200027 1875. 2.8 0.3 0.7 1.5 -1. D505900200028 1896. 4.1 0.4 1.0 1.5 -1. D505900200029 ENDDATA 12 0 D505900200030 ENDSUBENT 29 0 D505900299999 SUBENT D5059003 20081020 D064D505900300001 BIB 2 2 D505900300002 REACTION (18-AR-40(P,G)19-K-41,PAR,DA,,LEG/RS) D505900300003 STATUS (TABLE) Tbl.3 D505900300004 ENDBIB 2 0 D505900300005 NOCOMMON 0 0 D505900300006 DATA 6 22 D505900300007 EN E-LVL-INI E-LVL-FIN NUMBER DATA DATA-ERR D505900300008 KEV MEV MEV NO-DIM NO-DIM NO-DIM D505900300009 1839. 9.610 0.0000 2.0000 0.08 0.13 D505900300010 1839. 9.610 0.0000 4.0000 0.03 0.12 D505900300011 1839. 9.610 0.98 2.0000 -0.72 0.23 D505900300012 1839. 9.610 0.98 4.0000 0.60 0.28 D505900300013 1839. 9.610 1.29 2.0000 0.16 0.26 D505900300014 1839. 9.610 1.29 4.0000 0.15 0.30 D505900300015 1839. 9.610 1.56 2.0000 -0.42 0.67 D505900300016 1839. 9.610 1.56 4.0000 0.28 0.80 D505900300017 1842. 9.613 0.98 2.0000 -0.72 0.23 D505900300018 1842. 9.613 0.98 4.0000 0.60 0.26 D505900300019 1842. 9.613 1.56 2.0000 0.36 0.51 D505900300020 1842. 9.613 1.56 4.0000 -0.56 0.50 D505900300021 1875. 9.646 0.0000 2.0000 0.04 0.20 D505900300022 1875. 9.646 0.0000 4.0000 -0.32 0.29 D505900300023 1875. 9.646 0.98 2.0000 -0.49 2.46 D505900300024 1875. 9.646 0.98 4.0000 0.24 0.24 D505900300025 1896. 9.667 0.0000 2.0000 0.36 0.19 D505900300026 1896. 9.667 0.0000 4.0000 0.16 0.19 D505900300027 1896. 9.667 0.98 2.0000 -0.22 0.75 D505900300028 1896. 9.667 0.98 4.0000 -0.09 0.90 D505900300029 1896. 9.667 1.58 2.0000 0.16 0.43 D505900300030 1896. 9.667 1.58 4.0000 0.01 0.54 D505900300031 ENDDATA 24 0 D505900300032 ENDSUBENT 31 0 D505900399999 ENDENTRY 3 0 D505999999999