Low-energy enhancement in the magnetic dipole $\gamma$-ray strength functions of heavy nuclei

TL;DR

This paper investigates the presence and characteristics of low-energy enhancement in magnetic dipole gamma-ray strength functions of heavy nuclei, using advanced many-body computational methods, revealing its persistence and evolution with neutron number.

Contribution

It demonstrates the existence of low-energy enhancement in heavy samarium nuclei's M1 gamma-ray strength functions using SPA+RPA and SMMC methods, extending prior findings from medium-mass nuclei.

Findings

Low-energy enhancement is present in heavy samarium nuclei.

The slope of the LEE is roughly independent of initial energy.

Strength transfers to a low-energy excitation as neutron number increases.

Abstract

A low-energy enhancement (LEE), observed experimentally in the $\gamma$-ray strength function ($\gamma$SF) describing the decay of compound nuclei, would have profound effects on $r$-process nucleosynthesis if it persists in heavy neutron-rich nuclei. The LEE was shown to be a feature of the magnetic dipole ($M1)$ strength function in configuration-interaction shell-model calculations in medium-mass nuclei. However, its existence in heavy nuclei and its evolution with neutron number remain open questions. Here, using a combination of many-body methods, we find the LEE in the $M1$ $\gamma$SFs of heavy samarium nuclei. In particular, we use the static-path plus random-phase approximation (SPA+RPA), which includes static and small-amplitude quantal fluctuations beyond the mean field. Using the SPA+RPA strength as a prior, we apply the maximum-entropy method (MEM) to obtain finite-temperature $M1$ $\gamma$SFs from exact imaginary-time response functions calculated with the shell model Monte Carlo (SMMC) method. We find that the slope of the LEE in samarium isotopes is roughly independent of the average initial energy over a wide range below the neutron separation energy. As the neutron number increases, strength transfers to a low-energy excitation, which we interpret as the scissors mode built on top of excited states.