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