ENTRY D5045 20110204 D076D504500000001 SUBENT D5045001 20110204 D076D504500100001 BIB 11 30 D504500100002 TITLE Radiative Strength Functions for Dipole Transitions in D504500100003 57,59Co D504500100004 AUTHOR (S.S.Ratkevich, I.D.Fedorets, B.A.Nemashkalo, D504500100005 V.E.Storizhko) D504500100006 INSTITUTE (4UKRKFT,4UKRKHU,4UKRUKR) D504500100007 REFERENCE (J,YF,63,1581,2000) D504500100008 (J,PAN,63,1497,2000) D504500100009 #doi:10.1134/1.1312882 D504500100010 #NSR 2000RA27 D504500100011 FACILITY (VDG,4UKRKFT) D504500100012 METHOD (SITA,EXTB) D504500100013 DETECTOR (GELI,NAICR) The spectra of gamma rays corresponding toD504500100014 primary transitions were measured by a pair D504500100015 spectrometer arranged at an angle of 55 degrees to the D504500100016 proton-beam direction. The yields of gamma rays D504500100017 corresponding to direct transitions to the ground D504500100018 states of 57Co and 59Co were also measured with the aidD504500100019 of a NaI(Tl) detector of dimensions 200x200 mm2. D504500100020 SAMPLE Targets were manufactured by electrolytically D504500100021 precipitating,onto a gold substrate, 56Fe (enrichment D504500100022 was 99.9%) in order to obtain 849 mg/cm2-and D504500100023 1.729 mg/cm2-thick samples or 58Fe (enrichment was D504500100024 90.7%) in order to obtain 849 mg/cm2 -thick samples. D504500100025 ADD-RES (COMP)Compared with the results of calculations that D504500100026 rely on the statistical approach and which take into D504500100027 account the temperature of the nucleus and its shell D504500100028 structure. D504500100029 ERR-ANALYS (DATA-ERR)Any additional information is absent. D504500100030 HISTORY (20090108C)UKRNDC D504500100031 (20110203U) VS. DOI identifier corrected D504500100032 ENDBIB 30 0 D504500100033 NOCOMMON 0 0 D504500100034 ENDSUBENT 33 0 D504500199999 SUBENT D5045002 20090108 D065D504500200001 BIB 3 3 D504500200002 REACTION (26-FE-56(P,G)27-CO-57,PAR,SIG) D504500200003 EN-SEC (E-LVL,27-CO-57) D504500200004 STATUS (TABLE) Table 1 from text D504500200005 ENDBIB 3 0 D504500200006 COMMON 2 3 D504500200007 EN EN-RSL D504500200008 MEV MEV D504500200009 2.84 0.18 D504500200010 ENDCOMMON 3 0 D504500200011 DATA 3 15 D504500200012 E-LVL DATA DATA-ERR D504500200013 MEV MICRO-B MICRO-B D504500200014 0.0 23.0 4.4 D504500200015 1.224 5.6 1.5 D504500200016 1.378 24.9 4.7 D504500200017 1.505 16.4 6.3 D504500200018 1.690 1.1 0.5 D504500200019 1.758 18.5 4.2 D504500200020 1.897 7.2 1.8 D504500200021 1.920 11.3 3.1 D504500200022 2.133 14.4 4.4 D504500200023 2.479 4.9 2.0 D504500200024 2.523 3.0 1.5 D504500200025 2.611 3.3 1.6 D504500200026 2.731 12.0 4.1 D504500200027 2.804 9.2 3.5 D504500200028 2.981 8.0 3.0 D504500200029 ENDDATA 17 0 D504500200030 ENDSUBENT 29 0 D504500299999 SUBENT D5045003 20090108 D065D504500300001 BIB 3 3 D504500300002 REACTION (26-FE-58(P,G)27-CO-59,PAR,SIG) D504500300003 EN-SEC (E-LVL,27-CO-59) D504500300004 STATUS (TABLE) Table 2 from text D504500300005 ENDBIB 3 0 D504500300006 COMMON 2 3 D504500300007 EN EN-RSL D504500300008 MEV MEV D504500300009 2.8 0.220 D504500300010 ENDCOMMON 3 0 D504500300011 DATA 3 21 D504500300012 E-LVL DATA DATA-ERR D504500300013 MEV MICRO-B MICRO-B D504500300014 0.0 49.0 3.9 D504500300015 1.099 68.6 6.4 D504500300016 1.190 8.5 5.0 D504500300017 1.292 64.3 9.7 D504500300018 1.460 65.8 15. D504500300019 1.745 19.5 4.3 D504500300020 2.087 29.5 8.3 D504500300021 2.154 9.5 2.3 D504500300022 2.205 23.7 7.4 D504500300023 2.395 4.4 2.0 D504500300024 2.479 19.3 4.4 D504500300025 2.582 68.1 17. D504500300026 2.770 99.9 25. D504500300027 2.817 32.9 8.7 D504500300028 2.958 30.6 17. D504500300029 3.015 4.7 2.2 D504500300030 3.082 16.7 6.4 D504500300031 3.141 4.2 1.8 D504500300032 3.160 23.4 12. D504500300033 3.220 38.4 8.6 D504500300034 3.323 4.8 1.4 D504500300035 ENDDATA 23 0 D504500300036 ENDSUBENT 35 0 D504500399999 ENDENTRY 3 0 D504599999999