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Quantum magic and multipartite entanglement in the structure of nuclei

Florian Brökemeier1, S. Momme Hengstenberg1, James W. T. Keeble1, Caroline E. P. Robin1,2,*, Federico Rocco1, and Martin J. Savage3,†

  • *Contact author: crobin@physik.uni-bielefeld.de
  • Contact author: mjs5@uw.edu; On leave from the Institute for Nuclear Theory.

Phys. Rev. C 111, 034317 – Published 11 March, 2025Erratum Phys. Rev. C 114, 039901 (2026)

DOI: https://doi.org/10.1103/PhysRevC.111.034317

Abstract

Motivated by the Gottesman-Knill theorem, we present a detailed study of the quantum complexity of p-shell and sd-shell nuclei. Valence-space nuclear shell-model wave functions generated by the bigstick code are mapped to qubit registers using the Jordan-Wigner mapping (12 qubits for the p shell and 24 qubits for the sd shell), from which measures of the many-body entanglement (n-tangles) and magic (nonstabilizerness) are determined. While exact evaluations of these measures are possible for nuclei with a modest number of active nucleons, Monte Carlo simulations are required for the more complex nuclei. The broadly applicable Pauli-string ÎẐ exact (PSIZe) Markov chain Monte Carlo (MCMC) technique is introduced to accelerate the evaluation of measures of magic in deformed nuclei (with hierarchical wave functions), by factors of 8 for some nuclei. Significant multinucleon entanglement is found in the sd shell, dominated by proton-neutron configurations, along with significant measures of magic. This is evident not only for the deformed states, but also for nuclei on the path to instability via regions of shape coexistence and level inversion. These results indicate that quantum-computing resources will accelerate precision simulations of such nuclei and beyond.

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Erratum

Erratum: Quantum magic and multipartite entanglement in the structure of nuclei [Phys. Rev. C 111, 034317 (2025)]

Florian Brökemeier, S. Momme Hengstenberg, James W. T. Keeble, Caroline E. P. Robin, Federico Rocco, and Martin J. Savage
Phys. Rev. C 114, 039901 (2026)

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