Cargando…

The Most Accurate Determination of the $^{8}$B Half-life

Beta decay is a primary source of information of the structure of a nucleus. An accurate measurement of the half-life of a nucleus is essential for the proper determination of the reduced Gammow–Teller transition probability $B$(GT). In this work, we present an experiment using a compact set-up of S...

Descripción completa

Detalles Bibliográficos
Autores principales: Viñals, S, Nácher, E, Tengblad, O, Benito, J, Borge, M J G, Figuera, P, Fraile, L M, Fynbo, H O U, Gad, A, Jensen, J, Jonson, B, Lica, R, Marroquín, I, Munch, M, Nilsson, T, Ovejas, J D, Perea, A, Riisager, K, Smain, S, Sotty, C
Lenguaje:eng
Publicado: 2020
Materias:
Acceso en línea:https://dx.doi.org/10.5506/APhysPolB.51.717
http://cds.cern.ch/record/2800358
Descripción
Sumario:Beta decay is a primary source of information of the structure of a nucleus. An accurate measurement of the half-life of a nucleus is essential for the proper determination of the reduced Gammow–Teller transition probability $B$(GT). In this work, we present an experiment using a compact set-up of Si-telescope detectors to measure the half-life of the $^8$B nucleus. Three independent measurements have been analysed, obtaining the values 771.9(17) ms, 773.9(18) ms, and 770.9(27) ms. The value of the half-life obtained as the weighted averaged with the previous published measures is 771.17(94) ms which is a factor 3.2 of improvement in the uncertainty of the half-life