On the calculation and use of effective single-particle energies: the example of the neutron 1d 3/2 –1d 5/2 splitting along N = 20 isotones

Author:

Somà V.1ORCID,Duguet T.12

Affiliation:

1. IRFU, CEA, Université Paris-Saclay , 91191 Gif-sur-Yvette, France

2. KU Leuven, Instituut voor Kern- en Stralingsfysica , 3001 Leuven, Belgium

Abstract

The rich phenomenology of quantum many-body systems such as atomic nuclei is complex to interpret. Often, the behaviour (e.g. evolution with the number of constituents) of measurable/observable quantities such as binding or excitation energies can be best understood based on a simplified picture involving auxiliary quantities that are not observable, i.e. whose values vary with parameters that are internal to the theoretical construction (contrarily to measurable/observable quantities). While being useful, the simplified interpretation is thus theoretical-scheme dependent. This applies, in particular, to the so-called single-nucleon shell structure based on auxiliary effective single-particle energies (ESPEs). In this context, the present work aims at (i) recalling the way to compute ESPEs out of solutions of many-body Schrödinger’s equation, (ii) illustrating the use of ESPEs within the frame of state-of-the-art ab initio calculations to interpret the outcome of a recent nuclear experiment, and (iii) demonstrating the impact of several alterations on the computation of ESPEs. While the chosen alterations constitute approximations within the ab initio scheme, they are built-in when employing other theoretical constructs at play in nuclear physics. The present considerations are thus meant to empirically illustrate variations that can be expected between ESPEs computed within different (equally valid) theoretical schemes. This article is part of the theme issue ‘The liminal position of Nuclear Physics: from hadrons to neutron stars’.

Publisher

The Royal Society

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