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    First Measurement of the K− Escape Cross Section in the C12(K−,p) Reaction

    Fumiya Oura1,2,*, Yudai Ichikawa2,1, Junko Yamagata-Sekihara3, Jung Keun Ahn4, Sung Wook Choi4, Manami Fujita5, Takeshi Harada6, Shoichi Hasegawa1, Shuhei Hayakawa2 et al. (J-PARC E42 Collaboration)

    Shuhei Hayakawa2, Kenneth Hicks7, Satoru Hirenzaki8, Sang Hoon Hwang9, Ken’ichi Imai1,6, Yuji Ishikawa2, Woo Seung Jung1, Shunsuke Kajikawa2, Kento Kamada2, Byung Min Kang4, Shin Hyung Kim10, Tomomasa Kitaoka2, Jaeyong Lee11, Jong Won Lee12, Koji Miwa2,13, Taito Morino2, Tamao Sakao2, Hiroyuki Sako1, Masayoshi Saito2, Susumu Sato1, Toshiyuki Takahashi13, Kiyoshi Tanida1, Hirokazu Tamura2,1, Mifuyu Ukai13,2, Shunsuke Wada2, Takeshi O. Yamamoto1, and Seongbae Yang4 (J-PARC E42 Collaboration)

    • *Contact author: fumiya.oura@gmail.com

    Phys. Rev. Lett. 137, 132501 – Published 22 September, 2026

    DOI: https://doi.org/10.1103/y6wr-rqjp

    Abstract

    We investigated the K¯-nucleus interaction through the simultaneous measurement of the inclusive C12(K−,p) and exclusive K− escape C12(K−,pKesc−) reactions at 1.8  GeV/c at J-PARC. The present measurement explicitly focuses on the K− escape process for the first time, successfully accomplishing a direct experimental determination of the imaginary part of the K− optical potential. The differential cross section for the K− escape reaction was determined to be 436±6(stat.)±44(syst.)  μb/sr. A simultaneous likelihood fit yielded real and imaginary potential strengths of V0=−72−5+3(stat.)−8+0(syst.)  MeV and W0=−100−1+7(stat.)−16+0(syst.)  MeV at the nuclear center, respectively. The derived W0 is significantly stronger than that predicted by theoretical models based on one-nucleon processes, ssuggesting possible contributions from processes involving multiple nucleons.

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