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An event excess observed in the deeply bound region of the C-12(K-,p) missing-mass spectrum

Authors
Ichikawa, YudaiYamagata-Sekihara, JunkoAhn, Jung KeunAkazawa, YuyaAoki, KanaeBotta, ElenaEkawa, HiroyukiEvtoukhovitch, PetrFeliciello, AlessandroFujita, ManamiGogami, ToshiyukiHasegawa, ShoichiHasegawa, TomoyukiHayakawa, ShuheiHayakawa, TomonoriHirenzaki, SatoruHonda, RyotaroHosomi, KenjiImai, Ken'ichiJung, WooseungKanatsuki, ShunsukeKim, Shin HyungKinbara, ShinjiKobayashi, KazuyaLee, JaeyongMarcello, SimonettaMiwa, KojiMoon, TaejinNagae, TomofumiNakada, YoshiyukiNakagawa, ManamiNanamura, TakuyaNaruki, MegumiSakaguchi, AtsushiSako, HiroyukiSato, SusumuSasaki, YukiShirotori, KotaroSugimura, HitoshiTakahashi, ToshiyukiTamura, HirokazuTanida, KiyoshiTsamalaidze, ZviadiUkai, MifuyuYamamoto, Takeshi O.
Issue Date
12월-2020
Publisher
OXFORD UNIV PRESS INC
Citation
PROGRESS OF THEORETICAL AND EXPERIMENTAL PHYSICS, v.2020, no.12
Indexed
SCIE
SCOPUS
Journal Title
PROGRESS OF THEORETICAL AND EXPERIMENTAL PHYSICS
Volume
2020
Number
12
URI
https://scholar.korea.ac.kr/handle/2021.sw.korea/130345
DOI
10.1093/ptep/ptaa139
ISSN
2050-3911
Abstract
We have measured, for the first time, the inclusive missing-mass spectrum of the C-12(K-,p) reaction at an incident kaon momentum of 1.8 GeV/c at the J-PARC K1.8 beamline. We observed a prominent quasi-elastic peak (K- p -> 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 (K) over bar -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 similar to 100 MeV, where the major decay channel of K- NN -> pi Sigma N is energetically closed, and the non-mesonic decay modes (K- NN -> 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 Y*-nucleus system.
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