Magnetic dipole γ-ray strength functions of heavy nuclei in the configuration-interaction shell model

¹ Center for Theoretical Physics, Sloane Physics Laboratory, Yale University, New Haven, Connecticut 06520, USA
² Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA

^* e-mail: yoram.alhassid@yale.edu
^** e-mail: paul.fanto@yale.edu
^*** e-mail: amercenne@lsu.edu

Published online: 14 March 2024

Abstract

A low-energy enhancement (LEE) has been observed in the deexcitation γ-ray strength function (γSF) of compound nuclei. The LEE has been a subject of intense experimental and theoretical interest since its discovery, and, if the LEE persists in heavy neutron-rich nuclei, it would have significant effects on calculations of r-process nucleosynthesis. Standard configuration-interaction (CI) shell-model calculations in medium-mass nuclei have attributed the LEE to the magnetic dipole γSF but such calculations are computationally intractable in heavy nuclei. We review a combination of beyond-mean-field many-body methods within the framework of the CI shell model that enables the calculation of γSF in heavy nuclei, and discuss the recent theoretical identification of a LEE in the magnetic dipole γSF of lanthanide isotopes.