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Structure of P43 and Si42 in a two-level shape-coexistence model

A. O. Macchiavelli, H. L. Crawford, C. M. Campbell, R. M. Clark, M. Cromaz, P. Fallon, I. Y. Lee, A. Gade, A. Poves, and E. Rice
Phys. Rev. C 105, 014309 – Published 11 January 2022

Abstract

Exclusive cross sections for the P43(1p)Si42 reaction to the lowest 0+ and 2+ states, measured at NSCL with GRETINA and the S800, are interpreted in terms of a two-level mixing (collective) model of oblate and prolate coexisting shapes. Using the formalism developed for deformed nuclei, we calculate the spectroscopic amplitudes and exclusive cross sections in the strong-coupling limit, where for P43 the schematic wave function includes the coupling of the Nilsson [211]12 proton orbit. Good agreement with the experimental data is obtained when the amplitude of the oblate configuration is 80%, suggesting that both nuclei are predominantly oblate, in line with theoretical expectations. Model predictions for excitation energies and electromagnetic observables, which could motivate further studies of both nuclei, are also presented.

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  • Received 16 August 2021
  • Accepted 10 December 2021

DOI:https://doi.org/10.1103/PhysRevC.105.014309

©2022 American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

Authors & Affiliations

A. O. Macchiavelli1, H. L. Crawford1, C. M. Campbell1, R. M. Clark1, M. Cromaz1, P. Fallon1, I. Y. Lee1, A. Gade2, A. Poves3, and E. Rice4,1

  • 1Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
  • 2National Superconducting Cyclotron Laboratory, East Lansing, Michigan 48824, USA
  • 3Departamento de Física Teórica and IFT-UAM/CSIC, Universidad Autónoma de Madrid, 28049 Madrid, Spain
  • 4Department of Physics and Astronomy, Ohio University, Athens, Ohio, USA

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Issue

Vol. 105, Iss. 1 — January 2022

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Images

  • Figure 1
    Figure 1

    Proton Nilsson orbitals originating from the sd shell and relevant for the structure of N=28 nuclei. Specifically for the case of P43, the [211]12 level is highlighted in blue, and the shaded yellow area indicates the anticipated regions of deformation (see text).

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  • Figure 2
    Figure 2

    Nilsson amplitudes for the [211]12 level as a function of deformation. The red line shows the estimated core overlap O|P.

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  • Figure 3
    Figure 3

    Results of the calculation (yellow bars) to reproduce the experimental cross sections (black data points) [9]. The reproduction is very good, with the asymmetric error bars for the calculation coming as a result of the constraint A, α[0,1].

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  • Figure 4
    Figure 4

    Excitation energies in Si42 predicted by the two-level model (open squares) fit to the experimental data (solid squares). The oblate and prolate amplitudes of the yrast band are shown in the inset. See text for discussion.

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  • Figure 5
    Figure 5

    Excitation energies in P43 predicted by the two-level model (open squares). The results are compared with some experimental data, which we assign to the [211]12 (black) and [202]32 (blue) Nilsson levels. We also include the results for the [202]52 (red) level. See text for discussion.

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