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Mechanisms of the nonmesonic weak decay of Λ hypernuclei and the three-body process

  • H. Bhang
  • , S. Ajimura
  • , K. Aoki
  • , A. Banu
  • , T. Fukuda
  • , O. Hashimoto
  • , J. I. Hwang
  • , S. Kameoka
  • , B. H. Kang
  • , E. Kim
  • , J. H. Kim
  • , M. Kim
  • , T. Maruta
  • , Y. Miura
  • , Y. Miyake
  • , T. Nagae
  • , M. Nakamura
  • , S. N. Nakamura
  • , H. Noumi
  • , S. Okada
  • Y. Okayasu, H. Outa, H. Park, P. K. Saha, Y. Sato, M. Sekimoto, S. Shin, T. Takahashi, H. Tamura, K. Tanida, A. Toyata, K. Tsukada, T. Watanabe, H. J. Yim
  • Seoul National University
  • The University of Osaka
  • High Energy Accelerator Research Organization, Tsukuba
  • GSI Helmholtz Centre for Heavy Ion Research
  • Osaka Electro-Communication University
  • Tohoku University
  • Ewha Womans University
  • Korea Research Institute of Standards and Science
  • The University of Tokyo
  • Kyoto University
  • Institute of Science Tokyo
  • RIKEN
  • Japan Atomic Energy Agency

Research output: Contribution to journalArticlepeer-review

Abstract

The long standing Γnp puzzle of NMWD has finally been solved recently. It appears that the reason behind the puzzle was the universal quenching of nucleon yields from the prediction of one-nucleon induced (1N-) NMWD. We have shown that the quenching of nucleon yields can be explained only when we include a fairly large contribution of the three-body process (Γ2N) in Γnm.

Original languageEnglish
Pages (from-to)1023-1026
Number of pages4
JournalModern Physics Letters A
Volume24
Issue number11-13
DOIs
StatePublished - 30 Apr 2009

Keywords

  • Hypernuclei; Γ/Γ ratio
  • Nonmesonic weak decay
  • Three-body interaction

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