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High-precision half-life measurements of the T=1/2 mirror β decays F17 and Cl33

J. Grinyer, G. F. Grinyer, M. Babo, H. Bouzomita, P. Chauveau, P. Delahaye, M. Dubois, R. Frigot, P. Jardin, C. Leboucher, L. Maunoury, C. Seiffert, J. C. Thomas, and E. Traykov
Phys. Rev. C 92, 045503 – Published 9 October 2015

Abstract

Background: Measurements of the ft values for T=1/2 mirror β+ decays offer a method to test the conserved vector current hypothesis and to determine Vud, the up-down matrix element of the Cabibbo-Kobayashi-Maskawa matrix. In most mirror decays used for these tests, uncertainties in the ft values are dominated by the uncertainties in the half-lives.

Purpose: Two precision half-life measurements were performed for the T=1/2β+ emitters, F17 and Cl33, in order to eliminate the half-life as the leading source of uncertainty in their ft values.

Method: Half-lives of F17 and Cl33 were determined using β counting of implanted radioactive ion beam samples on a moving tape transport system at the Système de Production d'Ions Radioactifs Accélérés en Ligne low-energy identification station at the Grand Accélérateur National d'Ions Lourds.

Results: The F17 half-life result, 64.347 (35) s, precise to ±0.05%, is a factor of 5 times more precise than the previous world average. The half-life of Cl33 was determined to be 2.5038 (22) s. The current precision of ±0.09% is nearly 2 times more precise compared to the previous world average.

Conclusions: The precision achieved during the present measurements implies that the half-life no longer dominates the uncertainty of the ft values for both T=1/2 mirror decays F17 and Cl33.

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  • Received 11 June 2015
  • Revised 27 August 2015

DOI:https://doi.org/10.1103/PhysRevC.92.045503

This article is available under the terms of the Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.

Published by the American Physical Society

Authors & Affiliations

J. Grinyer1,*, G. F. Grinyer1, M. Babo1, H. Bouzomita1, P. Chauveau1, P. Delahaye1, M. Dubois1, R. Frigot1, P. Jardin1, C. Leboucher1, L. Maunoury1, C. Seiffert2, J. C. Thomas1, and E. Traykov1,3

  • 1Grand Accélérateur National d'Ions Lourds (GANIL), CEA/DSM-CNRS/IN2P3, Bvd Henri Becquerel, 14076 Caen, France
  • 2ISOLDE, CERN, 1211 Geneva 23, Switzerland
  • 3IPHC, CNRS/IN2P3-Université de Strasbourg, 2 rue du Loess, 67037 Strasbourg, France

  • *joanna.grinyer@ganil.fr

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Vol. 92, Iss. 4 — October 2015

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