Few-Body Systems

, Volume 54, Issue 1–4, pp 103–110 | Cite as

Three-Body ΛNN → nNN Nonmesonic Weak Decay Process of Λ Hypernuclei

  • 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
  • T. Takahashi
  • H. Tamura
  • K. Tanida
  • A. Toyoda
  • K. Tshoo
  • K. Tsukada
  • T. Watanabe
  • H. J. Yim
Article

Abstract

The fundamental motivation to study the non-mesonic weak decay (NMWD) of Λ hypernuclei is that it provides the unique channel for the information of the baryon–baryon weak interaction in SU3 f group. The relative strength of the two main channels of NMWD whose decay processes are the Λp → np and Λn → nn has been the long standing puzzle during last several decades. The puzzling status has been settled down recently with the Γ n / Γ p value converging to \({\sim 0.5}\) . The large experimental values of Γ n / Γ p of the previous measurements turned out to be due to the surprisingly large contribution of the competing three-body NMWD, ΛNN → nNN process. This paper discusses about the first measurement of the branching ratio of the three-body NMWD process and the renormalized intra-nuclear cascade method adopted to disentangle the contribution of the three-body process out of those due to final state interaction. And the prospects of the more accurate measurement of the three-body process also are presented.

Keywords

Weak Decay Coincidence Measurement Nucleon Pair Proton Energy Spectrum Nucleon Spectrum 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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Copyright information

© Springer-Verlag 2012

Authors and Affiliations

  • H. Bhang
    • 1
  • S. Ajimura
    • 2
  • K. Aoki
    • 3
  • A. Banu
    • 4
  • T. Fukuda
    • 5
  • O. Hashimoto
    • 6
  • J. I. Hwang
    • 7
  • S. Kameoka
    • 6
  • B. H. Kang
    • 1
    • 15
  • E. Kim
    • 1
  • J. H. Kim
    • 1
    • 8
  • M. Kim
    • 1
  • T. Maruta
    • 9
  • Y. Miura
    • 6
  • Y. Miyake
    • 2
  • T. Nagae
    • 3
    • 12
  • M. Nakamura
    • 9
  • S. N. Nakamura
    • 6
  • H. Noumi
    • 2
    • 3
  • S. Okada
    • 10
    • 14
  • Y. Okayasu
    • 6
  • H. Outa
    • 3
    • 11
  • H. Park
    • 8
  • P. K. Saha
    • 3
    • 13
  • Y. Sato
    • 3
  • M. Sekimoto
    • 3
  • T. Takahashi
    • 3
  • H. Tamura
    • 6
  • K. Tanida
    • 1
    • 11
  • A. Toyoda
    • 3
  • K. Tshoo
    • 1
  • K. Tsukada
    • 6
  • T. Watanabe
    • 6
  • H. J. Yim
    • 1
  1. 1.Department of Physics and AstronomySeoul National UniversitySeoulKorea
  2. 2.Department of PhysicsOsaka UniversityToyonagaJapan
  3. 3.High Energy Accelerator Research Organization (KEK)TsukubaJapan
  4. 4.Gesellschaft fur Schwerionenforschung mbH (GSI)DarmstadtGermany
  5. 5.Laboratory of PhysicsOsaka Electro Communication UniversityNeyagawaJapan
  6. 6.Department of PhysicsTohoku UniversitySendaiJapan
  7. 7.Department of PhysicsEwha Womans UniversitySeoulKorea
  8. 8.Korea Research Institute of Standards and Science (KRISS)DaejeonKorea
  9. 9.Department of PhysicsUniversity of TokyoTokyoJapan
  10. 10.Department of PhysicsTokyo Institute of TechnologyOkayamaJapan
  11. 11.Riken Nishina CenterWakoJapan
  12. 12.Department of PhysicsKyoto UniversityKyotoJapan
  13. 13.Japan Atomic Energy Research InstituteTokaiJapan
  14. 14.INFN-LNFFrascatiItaly
  15. 15.Department of Nuclear EngineeringHanyang UniversitySeoulKorea

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