Muon capture rates: Evaluation within the quasiparticle random phase approximation
- NázevTitle
- Muon capture rates: Evaluation within the quasiparticle random phase approximationMuon capture rates: Evaluation within the quasiparticle random phase approximation
- Druh výsledkuResult type
- Článek v časopiseJournal article
- AutořiAuthors
- F. Šimkovic, R. Dvornicky, P. Vogel
- DOIDOI
- 10.1103/PhysRevC.102.034301
- Časopis / citaceJournal / citation
- PHYSICAL REVIEW C. 2020, 102(3), ISSN 2469-9985.
- RokYear
- 2020
- JazykLanguage
- eng
- WoSWoS
- 000566919400002
- ScopusScopus
- 2-s2.0-85092745784
- RIVRIV
- RIV/68407700:21670/20:00346841!RIV21-MSM-21670___
- ProjektProject
- Inženýrské aplikace fyziky mikrosvětaEngineering applications of microworld physics
AbstraktAbstract
The quasiparticle random phase approximation is used in evaluation of the total muon capture rates for final nuclei participating in double-beta decay. Several variants of the method are used, depending on the size of the single-particle model space used, or treatment of the initial bound muon wave function. The resulting capture rates are all reasonably close to each other. In particular, the variant that appears to be most realistic results in rates that are in good agreement with the experimental values. There is no necessity for an empirical quenching of the axial current coupling constant g(A). Its standard value g(A) = 1.27 seems to be adequate.
The quasiparticle random phase approximation is used in evaluation of the total muon capture rates for final nuclei participating in double-beta decay. Several variants of the method are used, depending on the size of the single-particle model space used, or treatment of the initial bound muon wave function. The resulting capture rates are all reasonably close to each other. In particular, the variant that appears to be most realistic results in rates that are in good agreement with the experimental values. There is no necessity for an empirical quenching of the axial current coupling constant g(A). Its standard value g(A) = 1.27 seems to be adequate.