TY - JOUR
T1 - Thermal-neutron capture by58Ni, 59Ni, and 60Ni
AU - Raman, S.
AU - Ouyang, Xiaoping
AU - Islam, M. A.
AU - Starner, J. W.
AU - Jurney, E. T.
AU - Lynn, J. E.
AU - Martínez-Pinedo, G.
PY - 2004/10
Y1 - 2004/10
N2 - We have studied the primary and secondary γ rays (414 in 59Ni, 390 in 60Ni, and 240 in 61Ni) following thermal-neutron capture by the stable 58Ni, radioactive 59Ni, and stable 60Ni isotopes. Most of these γ rays have been incorporated into the corresponding level schemes consisting of 65 levels in 59Ni, 88 levels in 60Ni, and 40 levels in 61Ni. The measured neutron separation energies (Sn in keV) for 59Ni, 60Ni, and 61Ni are, respectively, 8999.28±0.05, 11 387.73±0.05, and 7820.11 ±0.05. The measured thermal-neutron capture cross sections (in barns) for 58Ni, 59Ni, and 60Ni are, respectively, 4.13±0.05, 73.7±1.8, and 2.34±0.05. In all three cases, primary electric-dipole (E1) transitions account for the bulk of the total capture cross section. We have calculated these E1 partial cross sections (in 59Ni and 61Ni) using direct-capture theory and models of compound-nuclear capture. The agreement between theory and experiment is good. The experimental level schemes have been compared with the results from a large-basis shell-model calculation. The agreement was also found to be quite good.
AB - We have studied the primary and secondary γ rays (414 in 59Ni, 390 in 60Ni, and 240 in 61Ni) following thermal-neutron capture by the stable 58Ni, radioactive 59Ni, and stable 60Ni isotopes. Most of these γ rays have been incorporated into the corresponding level schemes consisting of 65 levels in 59Ni, 88 levels in 60Ni, and 40 levels in 61Ni. The measured neutron separation energies (Sn in keV) for 59Ni, 60Ni, and 61Ni are, respectively, 8999.28±0.05, 11 387.73±0.05, and 7820.11 ±0.05. The measured thermal-neutron capture cross sections (in barns) for 58Ni, 59Ni, and 60Ni are, respectively, 4.13±0.05, 73.7±1.8, and 2.34±0.05. In all three cases, primary electric-dipole (E1) transitions account for the bulk of the total capture cross section. We have calculated these E1 partial cross sections (in 59Ni and 61Ni) using direct-capture theory and models of compound-nuclear capture. The agreement between theory and experiment is good. The experimental level schemes have been compared with the results from a large-basis shell-model calculation. The agreement was also found to be quite good.
UR - https://www.scopus.com/pages/publications/11144252226
U2 - 10.1103/PhysRevC.70.044318
DO - 10.1103/PhysRevC.70.044318
M3 - 文章
AN - SCOPUS:11144252226
SN - 0556-2813
VL - 70
SP - 044318-1-044318-39
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 4
M1 - 044318
ER -