Abstract

Nuclear isomers are populated in the rapid neutron capture process (r process) of nucleosynthesis. The r process may cover a wide range of temperatures, potentially starting from several tens of GK (several MeV) and then cooling as material is ejected from the event. As the r-process environment cools, isomers can freeze out of thermal equilibrium or be directly populated as astrophysically metastable isomers (astromers). Astromers can undergo reactions and decays at rates very different from the ground state, so they may need to be treated independently in nucleosythesis simulations. Two key behaviors of astromers—ground state ↔ isomer transition rates and thermalization temperatures—are determined by direct transition rates between pairs of nuclear states. We perform a sensitivity study to constrain the effects of unknown transitions on astromer behavior. Detailed balance ensures that ground → isomer and isomer → ground transitions are symmetric, so unknown transitions are equally impactful in both directions. We also introduce a categorization of astromers that describes their potential effects in hot environments. We provide a table of neutron-rich isomers that includes the astromer type, thermalization temperature, and key unmeasured transition rates.

Highlights

  • Nuclear isomers are excited states of atomic nuclei with half-lives longer than the typical half-lives of picoseconds or femtoseconds [1]

  • We studied the sensitivity of effective thermal transition rates between nuclear isomers and ground states to unmeasured internal transitions

  • We categorized isomers as accelerants, batteries, or neutral according to the effects they could be expected to have in the r-process decay back to stability

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Summary

Introduction

Nuclear isomers are excited states of atomic nuclei with half-lives longer than the typical half-lives of picoseconds or femtoseconds [1]. These metastable states exhibit inhibited transitions to lower-lying levels due to structural dissimilarities between them; large differences in nuclear deformation, spin, and the projection of spin along the symmetry axis can each be responsible for nuclear isomerism [2,3,4]. Measurements of isomers and their properties continue to be a point of experimental interest for a variety of reasons, including as astrophysical model inputs, and for applications in industry, medicine, and tests of fundamental nuclear physics [7,8,9,10,11,12,13,14,15,16,17].

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