Abstract

An innovative symmetry-guided approach and its applications to light and intermediate-mass nuclei is discussed. This approach, with Sp(3, R) the underpinning group, is based on our recent remarkable finding, namely, we have identified the symplectic Sp(3,R) as an approximate symmetry for low-energy nuclear dynamics. This study presents the results of two complementary studies, one that utilizes realistic nucleon-nucleon interactions and unveils symmetries inherent to nuclear dynamics from first principles (or ab initio), and another study, which selects important components of the nuclear interaction to explain the primary physics responsible for emergent phenomena, such as enhanced collectivity and alpha clusters. In particular, within this symmetry-guided framework, ab initio applications of the theory to light nuclei reveal the emergence of a simple orderly pattern from first principles. This provides a strategy for determining the nature of bound states of nuclei in terms of a relatively small fraction of the complete shell-model space, which, in turn, can be used to explore ultra-large model spaces for a description of alpha-cluster and highly deformed structures together with associated rotations. We find that by using only a fraction of the model space extended far beyond current no-core shell-model limits and a long-range interaction that respects the symmetries in play, the outcome reproduces characteristic features of the low-lying 0+ states in 12C (including the elusive Hoyle state of importance to astrophysics) and agrees with ab initio results in smaller spaces. For these states, we offer a novel perspective emerging out of no-core shell-model considerations, including a discussion of associated nuclear deformation, matter radii, and density distribution. The framework we find is also extensible beyond 12C, namely, to the low-lying 0+ states of 8Be as well as the ground-state rotational band of Ne, Mg, and Si isotopes.

Highlights

  • Approximate symmetries in atomic nuclei that favor large deformation along with monopole and quadrupole excitations thereof, associated with the SU(3) group and the symplectic Sp(3, R) group, have been long recognized in selected cases [1,2,3,4,5,6,7,8,9,10]

  • It divides the space in “horizontal” harmonic oscillator (HO) shells and is dictated by particle-hole excitations

  • The established no-core shell model (NCSM) methods are not able to reach the physics regime necessary for a description of largely deformed nuclear states, such as the 12C Hoyle state that was predicted based on observed abundances of heavy elements in the universe [22], and which has attracted much recent attention both in theory and experiment ( [25,26,27,28,29,30,31,32]). We address this problem, within a no-core shell-model framework, by utilizing a small subset of symplectic Sp(3, R) basis states [6, 7], an Sp(3, R)-preserving part of the long-range inter-nucleon interaction [12], and an important symmetry-breaking spin-orbit term

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Summary

Introduction

Approximate symmetries in atomic nuclei that favor large deformation along with monopole and quadrupole excitations thereof, associated with the SU(3) group and the symplectic Sp(3, R) group, have been long recognized in selected cases [1,2,3,4,5,6,7,8,9,10]. The Nmax cutoff is defined as the maximum number of HO quanta allowed in a many-body basis state above the minimum for a given nucleus It divides the space in “horizontal” HO shells and is dictated by particle-hole excitations (this is complementary to the NCSpM, which divides the space in vertical slices selected by collectivity-driven rules). We address this problem, within a no-core shell-model framework, by utilizing a small subset of symplectic Sp(3, R) basis states [6, 7] (with the complete set yielding results equivalent to those of the NCSM), an Sp(3, R)-preserving part of the long-range inter-nucleon interaction [12], and an important symmetry-breaking spin-orbit term.

Irreducible representations and many-body basis states
Reduced matrix elements of the symplectic generators

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