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Structure of low-lying states in Sm140 studied by Coulomb excitation

M. Klintefjord et al.
Phys. Rev. C 93, 054303 – Published 2 May 2016

Abstract

The electromagnetic structure of Sm140 was studied in a low-energy Coulomb excitation experiment with a radioactive ion beam from the REX-ISOLDE facility at CERN. The 2+ and 4+ states of the ground-state band and a second 2+ state were populated by multistep excitation. The analysis of the differential Coulomb excitation cross sections yielded reduced transition probabilities between all observed states and the spectroscopic quadrupole moment for the 21+ state. The experimental results are compared to large-scale shell model calculations and beyond-mean-field calculations based on the Gogny D1S interaction with a five-dimensional collective Hamiltonian formalism. Simpler geometric and algebraic models are also employed to interpret the experimental data. The results indicate that Sm140 shows considerable γ softness, but in contrast to earlier speculation no signs of shape coexistence at low excitation energy. This work sheds more light on the onset of deformation and collectivity in this mass region.

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  • Received 5 March 2016
  • Revised 6 April 2016

DOI:https://doi.org/10.1103/PhysRevC.93.054303

This article is available under the terms of the Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

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Vol. 93, Iss. 5 — May 2016

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Images

  • Figure 1
    Figure 1

    Partial level scheme showing low-lying states in Sm140. The spin assignments for the excited states at 990 and 1599 keV are taken from a recent angular correlation measurement [14].

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  • Figure 2
    Figure 2

    Particle-γ coincidence time spectrum. A normalized fraction of the random gate was used for background subtraction.

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  • Figure 3
    Figure 3

    Energy spectra of particles detected in the DSSSD as a function of the laboratory scattering angle. The cuts to select between detected Sm140 projectiles and recoiling Mo94 target nuclei are marked. Ring number 1 corresponds to laboratory angle 19.7 and ring 16 to laboratory angle 58.4.

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  • Figure 4
    Figure 4

    Background subtracted γ-ray spectrum in coincidence with a particle in the DSSSD, with Doppler correction for Sm140. The 21+01+ transition at 531 keV, the 41+21+ transition at 715 keV, and the 22+21+ transition at 460 keV are visible. The broad structure originates from the 871 keV 21+01+ transition in Mo94. The purple arrow marks the 21+01+ transition of the potential beam contaminant Nd140.

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  • Figure 5
    Figure 5

    Background subtracted γ-ray spectrum in coincidence with a particle in the DSSSD, with Doppler correction for the Mo94 recoils. The 21+01+ transition in Mo94 was observed at 871 keV. The inset shows an enlarged part of the same spectrum, where the 3/2+5/2gs+ transition in the target contaminant Mo95 is seen at 204 keV.

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  • Figure 6
    Figure 6

    Gamma-ray spectra obtained with and without RILIS laser ionization in a measurement during which the lasers were periodically switched on and off. The spectra are Doppler corrected for the Sm140 projectiles.

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  • Figure 7
    Figure 7

    Gamma-ray spectra for five separate ranges of center-of-mass scattering angles with Doppler correction for γ emission from the Sm140 projectiles.

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  • Figure 8
    Figure 8

    Illustration of the iterative procedure to fit the reduced matrix elements using the codes gosia and gosia2, with parts (a), (b), and (c) corresponding to steps 2, 3, and 4 as described in the text. The level schemes indicate which matrix elements were included in the fit as free parameters, as fixed values, or as free parameters with spectroscopic data to constrain the fit. Iterations between step 3 and step 4 were performed until the solution converged.

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  • Figure 9
    Figure 9

    Result of the χ2 minimization for the 01+E221+ and 21+E221+ matrix elements in Sm140 obtained after the last iteration of step 4 of the fitting procedure using target normalization. Note that the final uncertainties of all matrix elements were obtained after one more iteration of step 3.

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  • Figure 10
    Figure 10

    Comparison of the experimental excitation energies (in keV) of the low-lying states in Sm140 with predictions from beyond-mean-field calculations based on the Gogny D1S interaction, the shell model (SM), the interacting boson approximation (IBA), and expectations for a nucleus with E(5) critical point symmetry (see text for explanations).

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  • Figure 11
    Figure 11

    Potential energy surface for Sm140 from constrained deformed Hartree-Fock minimization in the shell-model basis.

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  • Figure 12
    Figure 12

    Potential energy surface for the ground state of Sm140 obtained in the CHFB calculations with the Gogny D1S interaction.

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