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Majorana parameters of the interacting boson model of nuclear structure and their implication for 0νββ decay
Here, the well-known spherical-deformed-transitional nucleus and potential 0$\textit{νββ}$ emitter 150Nd and its daughter 150Sm were investigated in nuclear resonance fluorescence experiments using quasimonoenergetic, linearly polarized γ-ray beams. For both nuclei transitions from the 1+ scissors m...
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Published in: | Physical review. C 2021-12, Vol.104 (6) |
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Main Authors: | , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | Here, the well-known spherical-deformed-transitional nucleus and potential 0$\textit{νββ}$ emitter 150Nd and its daughter 150Sm were investigated in nuclear resonance fluorescence experiments using quasimonoenergetic, linearly polarized γ-ray beams. For both nuclei transitions from the 1+ scissors mode to the $0^+_2$ and $2^+_2$ states were observed for the first time and their respective $\textit{M}$ 1 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 150Nd → 150Sm 0$\textit{νββ}$ decay in the IBM-2 with these improved representations results in $M^{(0νββ)}_{\text{IBM-2}}[0^+_1]$ = 3.35 for the NME for 0$\textit{νββ}$ decay into the ground state of 150Sm and $M^{(0νββ)}_{\text{IBM-2}}[0^+_2]$ = 1.30 for 0$\textit{νββ}$ decay to its $0^+_2$ state. |
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ISSN: | 2469-9985 2469-9993 |
DOI: | 10.1103/PhysRevC.104.L061302 |