Experimental $\gamma$-decay strength in $^{59, 60}$Ni compared with microscopic calculations
/ Authors
T. Renstrøm, D. Takenaka, J. E. Midtbø, D. Symochko, Yiu-Wing Lui, M. Guttormsen, B. V. Kheswa, A. Avdeenkov, S. Siem, S. Katayama
and 13 more authors
S. Grimes, V. W. Ingeberg, T. Hagen, H. Nyhus, B. A. Brown, S. Kamerdzhiev, A. Larsen, A. Görgen, H. Utsunomiya, A. Voinov, G. Tveten, T. Ari-izumi, O. Achakovskiy
/ Abstract
Nuclear level densities and $\gamma$-ray strength functions have been extracted for $^{59, 60}\rm{Ni}$, using the Oslo method on data sets from the $^{60}$Ni($^{3}$He,$^{3}$He$^{\prime}\gamma$)$^{60}$Ni and $^{60}$Ni($^{3}$He,$\alpha\gamma$)$^{59}$Ni reactions. Above the neutron separation energy, S$_n$, we have measured the $\gamma$-ray strength functions for $^{61}$Ni and $^{60}$Ni in photoneutron experiments. The low-energy part of the $^{59,60}$Ni $\gamma$-ray strength functions show an increase for decreasing $\gamma$ energies. The experimental $\gamma$-ray strength functions are compared with $M1$ $\gamma$-ray strength functions calculated within the shell model. The $E1$ $\gamma$-ray strength function of $^{60}$Ni has been calculated using the QTBA framework. The QTBA calculations describe the data above $E_{\gamma}\approx$ 7 MeV, while the shell-model calculations agree qualitatively with the low energy part of the $\gamma$-ray strength function. Hence, we give a plausible explanation of the observed shape of the $\gamma$-decay strength.
Journal: arXiv: Nuclear Experiment