Multipole tomography of atomic nuclei with conserved symmetries

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Main Authors: Sun, X., Dobaczewski, J., Nazarewicz, W., Wibowo, H.
Format: Preprint
Published: 2026
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author Sun, X.
Dobaczewski, J.
Nazarewicz, W.
Wibowo, H.
author_facet Sun, X.
Dobaczewski, J.
Nazarewicz, W.
Wibowo, H.
contents We introduce two-body nuclear conditional probabilities that allow the definition of an intrinsic reference frame and the multipole moments of angular-momentum-$J$-conserving states. This enables the characterization of quadrupole deformations of states with $J\leq1/2$, which are not accessible via spectroscopic one-body quadrupole moments. We illustrate the method with nuclear density functional theory (DFT) calculations for $J=0$ states of $^{16}$O and $^{20}$Ne, the latter obtained by restoring rotational symmetry of prolate or oblate intrinsic configurations. We show that the two-body quadrupole shape characterizations are not equal to the one-body moments obtained from broken-symmetry states, mainly because of Pauli repulsion effects. Calculations of two-body multipole moments can be performed within various theoretical frameworks, but their experimental determination requires measuring two-body correlations.
format Preprint
id arxiv_https___arxiv_org_abs_2605_26088
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Multipole tomography of atomic nuclei with conserved symmetries
Sun, X.
Dobaczewski, J.
Nazarewicz, W.
Wibowo, H.
Nuclear Theory
High Energy Physics - Phenomenology
Nuclear Experiment
We introduce two-body nuclear conditional probabilities that allow the definition of an intrinsic reference frame and the multipole moments of angular-momentum-$J$-conserving states. This enables the characterization of quadrupole deformations of states with $J\leq1/2$, which are not accessible via spectroscopic one-body quadrupole moments. We illustrate the method with nuclear density functional theory (DFT) calculations for $J=0$ states of $^{16}$O and $^{20}$Ne, the latter obtained by restoring rotational symmetry of prolate or oblate intrinsic configurations. We show that the two-body quadrupole shape characterizations are not equal to the one-body moments obtained from broken-symmetry states, mainly because of Pauli repulsion effects. Calculations of two-body multipole moments can be performed within various theoretical frameworks, but their experimental determination requires measuring two-body correlations.
title Multipole tomography of atomic nuclei with conserved symmetries
topic Nuclear Theory
High Energy Physics - Phenomenology
Nuclear Experiment
url https://arxiv.org/abs/2605.26088