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Spectroscopy of low-spin states in Dy157: Search for evidence of enhanced octupole correlations

S. N. T. Majola et al.
Phys. Rev. C 100, 034322 – Published 23 September 2019

Abstract

Low-spin states of Dy157 have been studied using the JUROGAM II array, following the Gd155 (α, 2n) reaction at a beam energy of 25 MeV. The level scheme of Dy157 has been expanded with four new bands. Rotational structures built on the [523]5/2 and [402]3/2+ neutron orbitals constitute new additions to the level scheme as do many of the inter- and intraband transitions. This manuscript also reports the observation of cross I+(I1) and I(I1)+ E1 dipole transitions interlinking structures built on the [523]5/2 (band 5) and [402]3/2+ (band 7) neutron orbitals. These interlacing band structures are interpreted as the bands of parity doublets with simplex quantum number s=i related to possible octupole correlations.

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  • Received 19 April 2019
  • Revised 10 May 2019

DOI:https://doi.org/10.1103/PhysRevC.100.034322

©2019 American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

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Vol. 100, Iss. 3 — September 2019

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Images

  • Figure 1
    Figure 1

    Partial level scheme of Dy157 deduced from the current work. It shows new rotational structures, bands 5 and 6, which decay predominantly to the ground and yrast bands. New findings from the current work are labeled in red (and marked with asterisk symbols) while previously known bands, deduced from previous in-beam works, are labeled in black. Proposed configurations for each band structure are given below the bands Quantities within parenthesis are quoted as tentative.

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  • Figure 2
    Figure 2

    Partial level scheme of Dy157 deduced from the current work. It shows all the new rotational structures (bands 5, 6, 7, and 8) built on the yrast and ground bands. New findings from the current work are labeled in red (and marked with asterisk symbols) while previously known bands, deduced from previous in-beam works, are labeled in black. Inter-leaving transitions linking bands 5 and 7 are marked with a dollar symbol ($). Proposed configurations for each band structure are given below the bands. Quantities within parenthesis are quoted as tentative.

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  • Figure 3
    Figure 3

    Gated coincidence spectra for bands 5, 6, 7, and 8 are shown in panels (a)–(d), respectively. Note that there is an overlap in the single gates set on doublets in (a) and (b) Transitions corresponding to new structures are labeled in red (and marked with asterisk symbols) while contaminant reaction channels and/or other bands of Dy157, not associated with the cascade of interest are denoted by a colored in blue and marked with hash (#) symbols. The transition marked with a dollar symbol ($) in (c) is associated with interleaving E1 transition connecting bands 5 and 7. Previously known transitions in the nucleus and/or decay path of interest are also highlighted in blue but are unmarked.

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  • Figure 4
    Figure 4

    Plot of neutron quasiparticle Routhian e, as a function of ω, calculated for Dy157 using the CSM with parameters ɛ2=0.19, ɛ4=0.020, and γ=0. The solid and dotted lines colored in red represent positive-parity states with signatures α=+1/2 and 1/2, respectively. The dot-dashed and dashed lines colored in blue represent negative-parity states with α=+1/2 and 1/2, respectively. The corresponding quasineutron labeling is given in Table 2.

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  • Figure 5
    Figure 5

    Plots of excitation energy minus a rigid rotor reference for the bands observed in Dy157. Open and closed symbols represent signatures α=+1/2 and α=1/2, respectively.

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  • Figure 6
    Figure 6

    Plots of the experimental (a) alignment ix and (b) Routhians e for the bands in Dy157, deduced using Harris parameters of J0=322MeV1 and J1=344MeV3. Open and closed symbols represent signatures α=+1/2 and α=1/2, respectively.

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  • Figure 7
    Figure 7

    Plot of the energy displacement δE(I) of bands 5 and 7 forming a reflection asymmetric structure (with simplex s=i) in Dy157. This structure is compared to similar structures identified in nuclei with considerable octupole deformation in the (a) rare-earth region (Ba143 [62] and Nd146 [47]) and (b) actinide region (Ra220 [35] and Th223 [96]). The energy displacement δE(I) is expected to approach 0 for structures exhibiting permanent octupole deformation. Open and closed symbols correspond to s=+i and s=i simplex structures, respectively.

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  • Figure 8
    Figure 8

    Rotational frequency ratio ω(I)/ω+(I) of bands 5 and 7 forming a reflection asymmetric structure (with simplex s=i) in Dy157. This structure is compared to similar structures identified in nuclei with considerable octupole deformation in the (a) rare-earth region (Ba143 [62] and Nd146 [47]) and (b) in the actinide region (Ra220 [35] and Th223 [96]). This ratio is expected to approach 1 for structures exhibiting stable octupole deformation. Open and closed symbols correspond to s=+i and s=i simplex structures, respectively.

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