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Examination of the low-energy enhancement of the γ-ray strength function of Fe56

M. D. Jones et al.
Phys. Rev. C 97, 024327 – Published 22 February 2018

Abstract

A model-independent technique was used to determine the γ-ray strength function (γSF) of Fe56 down to γ-ray energies less than 1 MeV for the first time with GRETINA using the (p,p) reaction at 16 MeV. No difference was observed in the energy dependence of the γSF built on 2+ and 4+ final states, supporting the Brink hypothesis. In addition, angular distribution and polarization measurements were performed. The angular distributions are consistent with dipole radiation. The polarization results show a small bias towards magnetic character in the region of the enhancement.

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  • Received 13 November 2017

DOI:https://doi.org/10.1103/PhysRevC.97.024327

©2018 American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

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Vol. 97, Iss. 2 — February 2018

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Images

  • Figure 1
    Figure 1

    The ratio R=f(Ei)/f(Ej) as a function of excitation energy Ex, for several pairs of 2+ and 4+ states in Fe56. The red-dashed line denotes R=1, while the solid red-curve shows the expected ratios from the polynomial fit in Fig. 2. The final states used to construct the ratio are denoted by the fraction in the upper left or right with energies in keV.

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  • Figure 2
    Figure 2

    γ-ray strength function for Fe56 from the present work (colored squares) in comparison to previous measurements, Refs. [21] (black circles) and [33] (green triangles). The polynomial fit to Voinov et al. [21] is shown by the red-solid curve.

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  • Figure 3
    Figure 3

    (a) Angular distribution for the 847 keV 2+ state in Fe56. (b) The relative angular distribution for quasicontinuum γ rays between 1.0 and 6.0 MeV. The dashed line shows 1/W(θ)847. The bottom panels show the polarization asymmetry A for an electric (c) and magnetic (d) transition in Fe56 and Fe55, respectively, with fits in solid red.

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  • Figure 4
    Figure 4

    Polarization asymmetry A0 as a function of primary γ-ray energy. In blue (circles) are the extracted asymmetries from the best-fits in Fig. 3 for electric and magnetic transitions in Fe55 and Fe56. The red-solid curves denote the expected asymmetry given a linear polarization of P=0.30, and the red band (dashed) shows the range of asymmetries given the uncertainty in P. The grey band denotes the statistical uncertainty of measuring a uniform distribution.

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