6533b7d3fe1ef96bd1261655
RESEARCH PRODUCT
Quenching of gA deduced from the β-spectrum shape of 113Cd measured with the COBRA experiment
E. RukhadzeJuliane VolkmerChristian NitschI. SteklJulia KüttlerYingjie ChuR. HodákKevin KröningerJ. TebrüggeR. TemminghoffThomas QuanteClaus GößlingS. ZatschlerKai ZuberD. GehreArne HeimboldJouni SuhonenChristian HerrmannJoel KostensaloLucas Bodenstein-dreslersubject
PhysicsNuclear and High Energy PhysicsQuenching (fluorescence)Coupling strength010308 nuclear & particles physicsSpectrum (functional analysis)Context (language use)01 natural sciencesSpectral linelcsh:QC1-999Semiconductor detector0103 physical sciencesAtomic physics010306 general physicsNuclear Experimentlcsh:Physicsdescription
A dedicated study of the quenching of the weak axial-vector coupling strength $g_{\rm A}$ in nuclear processes has been performed by the COBRA collaboration. This investigation is driven by nuclear model calculations which show that the $\beta$-spectrum shape of the fourfold forbidden non-unique decay of $^{113}$Cd strongly depends on the effective value of $g_{\rm A}$. Using an array of CdZnTe semiconductor detectors, 45 independent $^{113}$Cd spectra were obtained and interpreted in the context of three nuclear models. The resulting effective mean values are $\bar{g}_{\rm A}(\text{ISM}) = 0.915 \pm 0.007$, $\bar{g}_{\rm A}(\text{MQPM}) = 0.911 \pm 0.013$ and $\bar{g}_{\rm A}(\text{IBFM-2}) = 0.955 \pm 0.022$. These values agree well within the determined uncertainties and deviate significantly from the free value of $g_{\rm A}$. This can be seen as a first step towards answering the long-standing question regarding quenching effects related to $g_{\rm A}$ in low-energy nuclear processes.
year | journal | country | edition | language |
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2018-06-06 | Physics Letters B |