6533b829fe1ef96bd128ac42

RESEARCH PRODUCT

Half-life, branching-ratio, andQ-value measurement for the superallowed0+→0+β+emitterTi42

Antti SaastamoinenT. KesslerPasi KarvonenUlrike HagerHeikki PenttiläJuha ÄYstöSami Rinta-antilaB. BlankSaidur RahamanT. SonodaJuho RissanenJ. GiovinazzoTommi EronenL. AudiracV.-v. ElomaaAri JokinenM. ReponenIain MooreAnu KankainenJ. SouinT. Kurtukian NietoJani HakalaChristine Weber

subject

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsQ valueBranching fraction0103 physical sciencesHalf-lifeAtomic physics010306 general physics01 natural sciencesCommon emitter

description

The half-life, the branching ratio, and the decay $Q$ value of the superallowed $\ensuremath{\beta}$ emitter $^{42}\mathrm{Ti}$ were measured in an experiment performed at the JYFLTRAP facility of the Accelerator Laboratory of the University of Jyv\"askyl\"a. $^{42}\mathrm{Ti}$ is the heaviest ${T}_{z}=\ensuremath{-}1$ nucleus for which high-precision measurements of these quantities have been tried. The half-life (${T}_{1/2}=208.14\ifmmode\pm\else\textpm\fi{}0.45$ ms) and the $Q$ value [${Q}_{\mathrm{EC}}=7016.83(25)$ keV] are close to or reach the required precision of about 0.1%. The branching ratio for the superallowed decay branch [$\mathrm{BR}=47.7(12)%$], a by-product of the half-life measurement, does not reach the necessary precision yet. Nonetheless, these results allow one to determine the experimental $\mathit{ft}$ value and the corrected $\mathcal{F}t$ value to be 3114(79) and 3122(79) s, respectively.

https://doi.org/10.1103/physrevc.80.035502