QRPA and PQRPA treatments of Ordinary Muon Capture: the case of 136Ba

The proton-neutron quasiparticle random-phase approximation (QRPA) and its particle-number projected version (PQRPA) are used to calculate the ordinary muon capture (OMC) on the ground state of $^{136}$Ba. Both the neutrinoless double beta decay ($0\nu\beta\beta$) and OMC populate the ground and excited states of $^{136}$Cs. This offers, for the case of the OMC, a valuable source of information about the still unobserved lepton number violating $0\nu\beta\beta$ process. We have computed OMC rates to nuclear states in $^{136}$Cs, in a region accessible to present-day OMC experiments. It turns out that the OMC rates computed in the PQRPA framework are larger than those computed using the QRPA.

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Publication Details

Published
2025-09-19
DOI
https://doi.org/10.22323/1.495.0003
Primary Topic
Muon and positron interactions and applications
Type
article
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article

QRPA and PQRPA treatments of Ordinary Muon Capture: the case of 136Ba

J. Kotila, J. Suhonen, O. Civitarese
Muon and positron interactions and applications
article

QRPA and PQRPA treatments of Ordinary Muon Capture: the case of 136Ba

J. Kotila, J. Suhonen, O. Civitarese
article en

Abstract

The proton-neutron quasiparticle random-phase approximation (QRPA) and its particle-number projected version (PQRPA) are used to calculate the ordinary muon capture (OMC) on the ground state of $^{136}$Ba. Both the neutrinoless double beta decay ($0\nu\beta\beta$) and OMC populate the ground and excited states of $^{136}$Cs. This offers, for the case of the OMC, a valuable source of information about the still unobserved lepton number violating $0\nu\beta\beta$ process. We have computed OMC rates to nuclear states in $^{136}$Cs, in a region accessible to present-day OMC experiments. It turns out that the OMC rates computed in the PQRPA framework are larger than those computed using the QRPA.

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Muon and positron interactions and applications
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