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An Event excess observed in the deeply bound region of the $$^{12}$$C$$(K^-,p)$$ missing-mass spectrum

市川 裕大*   ; 藤田 真奈美; 長谷川 勝一   ; 早川 修平; 佐甲 博之   ; 佐藤 進  ; 田村 裕和; 谷田 聖   ; 山本 剛史  ; 他36名*

Ichikawa, Yudai*; Fujita, Manami; Hasegawa, Shoichi; Hayakawa, Shuhei; Sako, Hiroyuki; Sato, Susumu; Tamura, Hirokazu; Tanida, Kiyoshi; Yamamoto, Takeshi; 36 of others*

We have measured, for the first time, the inclusive missing-mass spectrum of the $$^{12}$$C$$(K^-,p)$$ reaction at an incident kaon momentum of 1.8 GeV/c at the J-PARCK 1.8 beamline. We observed a prominent quasi-elastic peak ($$K^-,p)$$ $$rightarrow$$ $$(K^-,p)$$ in this spectrum. In the quasi-elastic peak region, the effect of secondary interaction is apparently observed as a peak shift, and the peak exhibits a tail in the bound region. We compared the spectrum with a theoretical calculation based on the Green's function method by assuming different values of the parameters for the $$bar{K}$$-nucleus optical potential. We found that the spectrum shape in the binding-energy region -300 MeV $$<$$ $$B_{K}$$ $$<$$ 40 MeV is best reproduced with the potential depths $$V_{0}$$ = -80 MeV (real part) and $$W_{0}$$ = -40 MeV(imaginary part). On the other hand, we observed a significant event excess in the deeply bound region around $$B_{K}$$ $$sim$$ 100 MeV, where the major decay channel of $$K^{-}NN$$ $$rightarrow$$ $$pi Sigma$$$$N$$ is energetically closed, and the non-mesonic decay modes ($$K^{-}NN$$ $$rightarrow$$ $$Lambda$$$$N$$ and $$Sigma$$$$N$$) should mainly contribute. The enhancement is fitted well by a Breit-Wigner function with a kaon-binding energy of 90 MeV and width 100 MeV. A possible interpretation is a deeply bound state of a $$gamma*$$-nucleus system.

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パーセンタイル:51.48

分野:Physics, Multidisciplinary

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