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  • Letter

Majorana parameters of the interacting boson model of nuclear structure and their implication for 0νββ decay

J. Kleemann1,*, T. Beck1,†, U. Friman-Gayer1,‡, N. Pietralla1, V. Werner1, S. W. Finch2, J. Kotila3,4,   Krishichayan2, B. Löher1 et al.

H. Pai1,§, O. Papst1, W. Tornow2, M. Weinert5, and A. Zilges5

  • 1Institut für Kernphysik, Technische Universität Darmstadt, Schlossgartenstrasse 9, 64289 Darmstadt, Germany
  • 2Department of Physics, Duke University and Triangle Universities Nuclear Laboratory, Durham, North Carolina 27708-0308, USA
  • 3Finnish Institute for Educational Research, University of Jyväskylä, P.O. Box 35, 40014 Jyväskylä, Finland
  • 4Center for Theoretical Physics, Sloane Physics Laboratory, Yale University, New Haven, Connecticut 06520-8120, USA
  • 5Institut für Kernphysik, University of Cologne, Zülpicher Strasse 77, 50937 Cologne, Germany

  • *jkleemann@ikp.tu-darmstadt.de
  • †Present address: Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA.
  • ‡Present address: Department of Physics, Duke University and Triangle Universities Nuclear Laboratory, Durham, North Carolina 27708-0308, USA.
  • §Present address: Nuclear Physics Division, Saha Institute of Nuclear Physics, 1/AF Bidhan Nagar, Kolkata 700064, India.

Phys. Rev. C 104, L061302 – Published 10 December, 2021

DOI: https://doi.org/10.1103/PhysRevC.104.L061302

Abstract

The well-known spherical-deformed-transitional nucleus and potential 0νββemitter Nd150and its daughter Sm150were investigated in nuclear resonance fluorescence experiments using quasimonoenergetic, linearly polarized γ-ray beams. For both nuclei transitions from the 1+ scissors mode to the 02+ and 22+ states were observed for the first time and their respective M1 transition strengths were determined. Through a systematic investigation, a sensitivity of these transition strengths to the three Majorana parameters of the interacting boson model-2 (IBM-2) was established. In combination with the novel experimental data, this poses strong constraints to the Majorana parameters in improved IBM-2 representations of both nuclei. A subsequent recalculation of the nuclear matrix elements (NMEs) for the Nd150→Sm150 0νββdecay in the IBM-2 with these improved representations results in MIBM-2(0νββ)[01+]=3.35 for the NME for 0νββdecay into the ground state of Sm150and MIBM-2(0νββ)[02+]=1.30 for 0νββdecay to its 02+ state.

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