Nonmesonic weak decay of the hypertriton

J. Golak, K. Miyagawa, H. Kamada, H. Witała, W. Glöckle, A. Parreño, A. Ramos, and C. Bennhold
Phys. Rev. C 55, 2196 – Published 1 May 1997; Erratum Phys. Rev. C 56, 2892 (1997)
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Abstract

The nonmesonic decay of the hypertriton is calculated based on a hypertriton wave function and 3N scattering states, which are rigorous solutions of three-body Faddeev equations using realistic NN and hyperon-nucleon interactions. The pion exchange together with heavier meson exchanges for the ΛNNN transition is considered. The total nonmesonic decay rate is found to be 0.5% of the free Λ decay rate. Integrated as well as differential decay rates are given. The p- and n-induced decays are discussed thoroughly and it is shown that the corresponding total rates cannot be measured individually.

  • Received 4 December 1996

DOI:https://doi.org/10.1103/PhysRevC.55.2196

©1997 American Physical Society

Erratum

Erratum: Nonmesonic weak decay of the hypertriton [Phys. Rev. C 55, 2196 (1997)]

J. Golak, K. Miyagawa, H. Kamada, H. Witała, W. Glöckle, A. Parreño, A. Ramos, and C. Bennhold
Phys. Rev. C 56, 2892 (1997)

Authors & Affiliations

J. Golak2, K. Miyagawa3, H. Kamada4, H. Witała2, W. Glöckle1, A. Parreño5, A. Ramos5, and C. Bennhold6

  • 1Institut für Theoretische Physik II, Ruhr Universität Bochum, D-44780 Bochum, Germany
  • 2Institut of Physics, Jagellonian University, PL 30059 Cracow, Poland
  • 3Department of Applied Physics, Okayama University of Science, Ridai-cho Okayama 700, Japan
  • 4Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
  • 5Departament d’Estructura i Constituents de la Matèria, Facultat de Física, Diagonal 647, E-08028, Spain
  • 6Center for Nuclear Studies, The George Washington University, Washington, D.C., 20052

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Issue

Vol. 55, Iss. 5 — May 1997

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