Search forB0→pΛ¯π−γat Belle

Y.-T. Lai,M.-Z. Wang,I. Adachi, H. Aihara,D. M. Asner,V. Aulchenko,T. Aushev,A. M. Bakich,A. Bala,B. Bhuyan,A. Bobrov, A. Bozek, M. Bračko,T. E. Browder,P. Chang,V. Chekelian,A. Chen, P. Chen,B. G. Cheon,I.-S. Cho,K. Cho,V. Chobanova,S.-K. Choi, Y. Choi, D. Cinabro,J. Dalseno,Z. Doležal,A. Drutskoy,S. Eidelman,H. Farhat,J. E. Fast,T. Ferber,A. Frey,V. Gaur,S. Ganguly,R. Gillard,Y. M. Goh,B. Golob,J. Haba,H. Hayashii, Y. Hoshi,W.-S. Hou,Y. B. Hsiung, T. Iijima,A. Ishikawa, R. Itoh,Y. Iwasaki,T. Iwashita, I. Jaegle,T. Julius,J. H. Kang,E. Kato,T. Kawasaki,C. Kiesling,H. O. Kim,J. H. Kim,M. J. Kim,Y. J. Kim, J. Klucar,B. R. Ko,P. Kodyš,S. Korpar,P. Križan,P. Krokovny,T. Kuhr,T. Kumita,Y.-J. Kwon,J. S. Lange,S.-H. Lee,J. Li,J. Libby, Y. Liu,P. Lukin,D. Matvienko,H. Miyata,R. Mizuk,A. Moll,R. Mussa, E. Nakano, M. Nakao,H. Nakazawa,M. Nayak,C. Ng,N. K. Nisar,S. Nishida,O. Nitoh,S. Ogawa, Y. Onuki,H. Ozaki,G. Pakhlova,C. W. Park,H. Park,T. K. Pedlar, R. Pestotnik, M. Petrič,L. E. Piilonen,M. Ritter,M. Röhrken,A. Rostomyan,S. Ryu,H. Sahoo, T. Saito,Y. Sakai,S. Sandilya, D. Santel,L. Santelj,T. Sanuki,Y. Sato,O. Schneider,G. Schnell,C. Schwanda, D. Semmler,K. Senyo, M. Shapkin, C. P. Shen,T.-A. Shibata,J.-G. Shiu,B. Shwartz, A. Sibidanov,Y.-S. Sohn,E. Solovieva, S. Stanič, M. Starič, M. Steder,T. Sumiyoshi,U. Tamponi,K. Tanida,Y. Teramoto,M. Uchida, S. Uehara,T. Uglov, Y. Unno,S. Uno,P. Urquijo,S. E. Vahsen,C. Van Hulse, P. Vanhoefer, G. Varner,A. Vossen,M. N. Wagner,C. H. Wang,P. Wang, Y. Watanabe, K. M. Williams, E. Won,J. Yamaoka, Y. Yamashita,S. Yashchenko,Z. P. Zhang,V. Zhilich, V. Zhulanov, A. Zupanc

Physical review(2014)

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摘要
We search for the charmless ${B}^{0}$ decay with final state particles $p\overline{\mathrm{\ensuremath{\Lambda}}}{\ensuremath{\pi}}^{\ensuremath{-}}\ensuremath{\gamma}$ using the full data sample that contains $772\ifmmode\times\else\texttimes\fi{}1{0}^{6}B\overline{B}$ pairs collected at the $\mathrm{\ensuremath{\Upsilon}}(4S)$ resonance with the Belle detector at the KEKB asymmetric-energy ${e}^{+}{e}^{\ensuremath{-}}$ collider. This decay is predicted to proceed predominantly via the $b\ensuremath{\rightarrow}s\ensuremath{\gamma}$ radiative penguin process with a high energy photon. No significant signal is found. We set an upper limit of $6.5\ifmmode\times\else\texttimes\fi{}1{0}^{\ensuremath{-}7}$ for the branching fraction of ${B}^{0}\ensuremath{\rightarrow}p\overline{\mathrm{\ensuremath{\Lambda}}}{\ensuremath{\pi}}^{\ensuremath{-}}\ensuremath{\gamma}$ at the 90% confidence level.
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Particle physics,Physics
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