TY - JOUR
T1 - Energy levels and configurations in 94Nb
AU - Jurney, E. T.
AU - Motz, H. T.
AU - Sheline, R. K.
AU - Shera, E. B.
AU - Vervier, Jean
PY - 1968/4
Y1 - 1968/4
N2 - In the high-energy thermal neutron capture gamma-ray spectrum of 94Nb, 83 gamma rays were observed between 4500 keV, and the neutron binding energy determined here to be 7229.5 ± 1.5 keV. A total of 71 low-energy gamma rays was observed from 30 keV to 1500 keV. These and previous data were used to develop a decay scheme. The presence of states arising predominantly from the following configurations is proposed: πgfrac(9, 2) v (dfrac(5, 2))frac(5, 2)3, πgfrac(9, 2) v (dfrac(5, 2))frac(3, 2)3, π (pfrac(1, 2))- 1 (gfrac(9, 2))02 v (dfrac(5, 2))frac(5, 2)3 and, more tentatively, π (pfrac(1, 2))- 1 (gfrac(9, 2))02 v (dfrac(5, 2))frac(9, 2)3 and πgfrac(9, 2) v (dfrac(5, 2))02 Sfrac(1, 2). Some preliminary assignments of spins and parities to other states have also been attempted. Calculations based on 90Zr and 88Sr cores both agree well with energies, spectroscopic factors and reduced M1 transition probabilities. The generally close agreement between the calculations involving different cores is surprising in view of the considerable differences in the two sets of wave functions. This is probably to be understood in terms of the ability of the effective nucleon-nucleon interaction to absorb the effect of configuration mixing.
AB - In the high-energy thermal neutron capture gamma-ray spectrum of 94Nb, 83 gamma rays were observed between 4500 keV, and the neutron binding energy determined here to be 7229.5 ± 1.5 keV. A total of 71 low-energy gamma rays was observed from 30 keV to 1500 keV. These and previous data were used to develop a decay scheme. The presence of states arising predominantly from the following configurations is proposed: πgfrac(9, 2) v (dfrac(5, 2))frac(5, 2)3, πgfrac(9, 2) v (dfrac(5, 2))frac(3, 2)3, π (pfrac(1, 2))- 1 (gfrac(9, 2))02 v (dfrac(5, 2))frac(5, 2)3 and, more tentatively, π (pfrac(1, 2))- 1 (gfrac(9, 2))02 v (dfrac(5, 2))frac(9, 2)3 and πgfrac(9, 2) v (dfrac(5, 2))02 Sfrac(1, 2). Some preliminary assignments of spins and parities to other states have also been attempted. Calculations based on 90Zr and 88Sr cores both agree well with energies, spectroscopic factors and reduced M1 transition probabilities. The generally close agreement between the calculations involving different cores is surprising in view of the considerable differences in the two sets of wave functions. This is probably to be understood in terms of the ability of the effective nucleon-nucleon interaction to absorb the effect of configuration mixing.
KW - Nb(n,γ), E = th; measured E, I, Q
KW - Nb deduced levels
KW - Natural target, Ge(Li) detector
UR - http://www.scopus.com/inward/record.url?scp=4243834289&partnerID=8YFLogxK
U2 - 10.1016/S0375-9474(68)90504-6
DO - 10.1016/S0375-9474(68)90504-6
M3 - Article
AN - SCOPUS:4243834289
SN - 0375-9474
VL - 111
SP - 105
EP - 128
JO - Nuclear Physics, Section A
JF - Nuclear Physics, Section A
IS - 1
ER -