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First candidates for γ vibrational bands built on the [505]11/2 neutron orbital in odd-A Dy isotopes

S. N. T. Majola et al.
Phys. Rev. C 101, 044312 – Published 20 April 2020

Abstract

Rotational structures have been measured using the Jurogam II and GAMMASPHERE arrays at low spin following the Gd155(α,2n)Dy157 and Nd148(C12,5n)Dy155 reactions at 25 and 65 MeV, respectively. We report high-K bands, which are conjectured to be the first candidates of a Kπ=2+γ vibrational band, built on the [505]11/2 neutron orbital, in both odd-ADy155,157 isotopes. The coupling of the first excited K=0+ states or the so-called β vibrational bands at 661 and 676 keV in Dy154 and Dy156 to the [505]11/2 orbital, to produce a Kπ=11/2 band, was not observed in both Dy155 and Dy157, respectively. The implication of these findings on the interpretation of the first excited 0+ states in the core nuclei Dy154 and Dy156 are also discussed.

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  • Received 23 December 2019
  • Accepted 18 March 2020

DOI:https://doi.org/10.1103/PhysRevC.101.044312

©2020 American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

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Vol. 101, Iss. 4 — April 2020

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Images

  • Figure 1
    Figure 1

    Partial level scheme of Dy155 deduced from the current work. It shows band structures built on the [505]11/2 neutron orbital in Dy155. New rotational structures, established in this work that have been identified as the γ band built on [505]11/2 bands are labeled in red (and marked with asterisk symbols) while known bands, deduced from previous in-beam works, are labeled in black.

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  • Figure 2
    Figure 2

    Partial level scheme of Dy157 deduced from the current work. It shows band structures built on the [505]11/2 neutron orbital in Dy157. New rotational structures, established in this work that have been identified as the γ band built on [505]11/2 bands are labeled in red (and marked with asterisk symbols) while known bands, deduced from previous in-beam works, are labeled in black.

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  • Figure 3
    Figure 3

    (a) Double and (b) single gated coincidence spectra for the γ band built on the [505]11/2 neutron orbital in Dy155 and Dy157, respectively. Transitions corresponding to these newly found structures are labeled in red (and marked with asterisk symbols) while contaminants from other reaction channels and/or other bands of Dy155,157, not associated with the cascade of interest are denoted by hash (#) symbols. 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

    Neutron quasiparticle Routhians e, as a function of ω, calculated for Dy157 using CSM with parameters ɛ2=0.245,ɛ4=0.020, and γ=11.8. 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 1.

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  • Figure 5
    Figure 5

    Plots of excitation energy minus a rigid rotor energy for bands observed in (a) Dy155 and (b) Dy157. Open symbols have α=+1/2 while closed symbols have α=1/2.

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  • Figure 6
    Figure 6

    Plots of alignment ix and Routhians e for bands in Dy155 and Dy157. Harris parameters used are J0=322MeV1 and J1=344MeV3. Open symbols have α=+1/2 while closed symbols have α=1/2.

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  • Figure 7
    Figure 7

    Experimental B(M1;II1)/B(E2;II2) values for ΔI=1M1 intraband transitions pertaining to the [505]11/2 bands and newly established Kπ=15/2 bands in (a) Dy157 and (b) Dy155.

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  • Figure 8
    Figure 8

    The systematic review of band-head energies for γ bands in the even (with respect to the ground-state bands) and odd-N Gd and Dy isotopes (from N=88 to N=96, i.e., Gd152 [9], Gd153 [46], Gd154 [9, 42], Gd155 [17], Gd156 [39], Gd158 [47], Gd160 [48], Dy154 [8], Dy155 (current work), Dy156 [13], Dy157 (current work), Dy158 [9], Dy160 [49], Dy162 [49]). Note that the excitation energy given for the K=15/2 band heads (in the odd-N nuclei) has been subtracted relative to the excitation energy of the lowest lying state of the K=11/2 band. The discontinuity in the Gd isotopes can be attributed to the missing band head (yet to be observed) energy of the γ band in Gd155.

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  • Figure 9
    Figure 9

    A plot of excitation energy minus the rigid rotor energy, showing the systematics of γ bands with respect to their intrinsic states in even-even and odd-A isotopes of gadolinium and dysprosium (from N=88 to N=92, i.e., Gd152 [9], Gd153 [50], Gd154 [9, 42], Gd155 [17], Gd156 [39], Dy154 [8], Dy155 (current work), Dy156 [13], Dy157 (current work), and Dy158 [9]).

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