Abstract

The physical conditions for the emergence of the extremely low-lying nuclear isomer $^{229m}$Th at approximately 8 eV are investigated in the framework of our recently proposed nuclear structure model. Our theoretical approach explains the $^{229m}$Th-isomer phenomenon as the result of a very fine interplay between collective quadrupole-octupole and single-particle dynamics in the nucleus. We find that the isomeric state can only appear in a rather limited model space of quadrupole-octupole deformations in the single-particle potential, with the octupole deformation being of a crucial importance for its formation. Within this deformation space the model-described quantities exhibit a rather smooth behaviour close to the line of isomer-ground state quasi-degeneracy determined by the crossing of the corresponding single-particle orbitals. Our comprehensive analysis confirms the previous model predictions for reduced transition probabilities and the isomer magnetic moment, while showing a possibility for limited variation in the ground-state magnetic moment theoretical value. These findings prove the reliability of the model and suggest that the same dynamical mechanism could manifest in other actinide nuclei giving a general prescription for the search and exploration of similar isomer phenomena.

Highlights

  • Well supporting the current strong emphasis on interdisciplinary research, a unique extremely low-lying 229mTh isomer at approximately 8 eV [1,2,3,4] obviously disregards the recognized low-energy border of nuclear physics firmly stepping on atomic physics territory

  • In this work we have thoroughly examined the physical conditions for the formation of the 8 eV isomer of 229Th according to the model mechanism suggested by our QO

  • Woods-Saxon deformed shell model (DSM) quadrupole and octupole deformations, which allow the appearance of the ground state (GS) and isomeric state (IS) with the experimentally adopted K values and parities

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Summary

Introduction

Well supporting the current strong emphasis on interdisciplinary research, a unique extremely low-lying 229mTh isomer at approximately 8 eV [1,2,3,4] obviously disregards the recognized low-energy border of nuclear physics firmly stepping on atomic physics territory. Another low-lying nuclear excitation in 235U approaches this limit with an order of magnitude larger energy of 76 eV [5], currently 229mTh attracts much more interest since its energy lies in the range of accessibility of present vacuum ultraviolet (VUV) lasers capable to handle the wavelength of 150 nm (≈8 eV).

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