1996arXiv (Cornell University)Open access

Double beta decay of $^{48}$Ca

A. Balysh, De Silva, A., V. I. Lebedev, K. Lou, M. K. Moe, Nelson, M. A., A. Piepke, A. Pronskiy, Vient, M. A., P. Vogel

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Abstract

$^{48}$Ca, the lightest double beta decay candidate, is the only one simple enough to be treated exactly in the nuclear shell model. Thus, the $ββ(2ν)$ half-life measurement, reported here, provides a unique test of the nuclear physics involved in the $ββ$ matrix element calculation. Enriched $^{48}$Ca sources of two different thicknesses have been exposed in a time projection chamber, and yield T$_{1/2}^{2ν} = (4.3^{+2.4}_{-1.1} [{\rm stat.}] \pm 1.4 [{\rm syst.}]) \times 10^{19}$ years, compatible with the shell model calculations.

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What this paper is about

$^{48}$Ca, the lightest double beta decay candidate, is the only one simple enough to be treated exactly in the nuclear shell model. Thus, the $ββ(2ν)$ half-life measurement, reported here, provides a unique test of the nuclear physics involved in the $ββ$ matrix element calculation. Enriched $^{48}$Ca sources of two different thicknesses have been exposed in a time projection chamber, and yield T$_{1/2}^{2ν} = (4.3^{+2.4}_{-1.1} [{\rm stat.}] \pm 1.4 [{\rm syst.}]) \times 10^{19}$ years, compatible with the shell model calculations.

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Available abstract

$^{48}$Ca, the lightest double beta decay candidate, is the only one simple enough to be treated exactly in the nuclear shell model. Thus, the $ββ(2ν)$ half-life measurement, reported here, provides a unique test of the nuclear physics involved in the $ββ$ matrix element calculation. Enriched $^{48}$Ca sources of two different thicknesses have been exposed in a time projection chamber, and yield T$_{1/2}^{2ν} = (4.3^{+2.4}_{-1.1} [{\rm stat.}] \pm 1.4 [{\rm syst.}]) \times 10^{19}$ years, compatible with the shell model calculations.

Key concepts: Double beta decay, Physics, Nuclear physics, Neutrino

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