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Zero- and finite-temperature electromagnetic strength distributions in closed- and open-shell nuclei from first principles

Y. Beaujeault-Taudière1,2, M. Frosini3,4, J.-P. Ebran1,2, T. Duguet4,5, R. Roth6,7, and V. Somà4

  • 1CEA, DAM, DIF, 91297 Arpajon, France
  • 2Université Paris-Saclay, CEA, Laboratoire Matière en Conditions Extrêmes, 91680 Bruyères-le-Châtel, France
  • 3CEA, DEN, IRESNE, DER, SPRC, 13108 Saint-Paul-lès-Durance, France
  • 4IRFU, CEA, Université Paris-Saclay, 91191 Gif-sur-Yvette, France
  • 5KU Leuven, Department of Physics and Astronomy, Instituut voor Kern- en Stralingsfysica, 3001 Leuven, Belgium
  • 6Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
  • 7Helmholtz Forschungsakademie Hessen für FAIR, GSI Helmholtzzentrum, 64289 Darmstadt, Germany

Phys. Rev. C 107, L021302 – Published 10 February, 2023

DOI: https://doi.org/10.1103/PhysRevC.107.L021302

Abstract

Ab initio approaches to the nuclear many-body problem have seen their reach considerably extended over the past decade. However, collective excitations have been scarcely addressed so far due to the prohibitive cost of solving the corresponding equations of motion. Here, a numerically efficient method to compute electromagnetic response functions at zero- and finite-temperature in superfluid and deformed nuclei from an ab initio standpoint is presented and applied to O16, Si28, Ti46, and Fe56. This work opens the path to systematic ab initio calculations of nuclear responses to electroweak probes across a significant portion of the nuclear chart.

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