Experimental $\gamma$-decay strength in $^{59, 60}$Ni compared with microscopic calculations
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...
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Zusammenfassung: | 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. |
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DOI: | 10.48550/arxiv.1804.08086 |