0000000000624574

AUTHOR

J. Souin

showing 2 related works from this author

Precise half-life measurement of the Si-26 ground state

2008

The beta-decay half-life of 26Si was measured with a relative precision of 1.4*10e3. The measurement yields a value of 2.2283(27) s which is in good agreement with previous measurements but has a precision that is better by a factor of 4. In the same experiment, we have also measured the non-analogue branching ratios and could determine the super-allowed one with a precision similar to the previously reported measurements. The experiment was done at the Accelerator Laboratory of the University of Jyvaskyla where we used the IGISOL technique with the JYFLTRAP facility to separate pure samples of 26Si.

PhysicsNuclear and High Energy PhysicsBranching fraction010308 nuclear & particles physicsFOS: Physical sciencesHalf-life01 natural sciencesNuclear physics0103 physical sciencesRelative precisionNuclear Experiment (nucl-ex)010306 general physicsGround stateNuclear ExperimentNuclear Physics
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Half-life, branching-ratio, andQ-value measurement for the superallowed0+→0+β+emitterTi42

2009

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-lif…

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