Observation of Z_{b}(10610) and Z_{b}(10650) Decaying to B Mesons.

A. Garmash,A. Abdesselam,I. Adachi,H. Aihara,D. Asner,T. Aushev,R. Ayad,T. Aziz,V. Babu,I. Badhrees,A. Bakich,P. Behera,V. Bhardwaj,B. Bhuyan,A. Bobrov,A. Bondar,G. Bonvicini,A. Bozek,M. Bračko,T. Browder,D. Červenkov,V. Chekelian,A. Chen,B. Cheon,K. Chilikin,K. Cho,V. Chobanova,Y. Choi,D. Cinabro,J. Dalseno,M. Danilov,N. Dash,Z. Doležal,A. Drutskoy,D. Dutta,S. Eidelman,D. Epifanov,H. Farhat,J. Fast,T. Ferber,B. G. Fulsom,V. Gaur,N. Gabyshev,R. Gillard, Y. Goh,P. Goldenzweig,B. Golob,T. Hara,K. Hayasaka,H. Hayashii,T. Iijima,A. Ishikawa,R. Itoh,Y. Iwasaki,I. Jaegle,D. Joffe,K. Joo,T. Julius, K. Kang,E. Kato,T. Kawasaki,D. Kim,J. Kim,K. Kim,M. Kim,S. Kim,Y. Kim,K. Kinoshita,S. Korpar,P. Križan,P. Krokovny,T. Kuhr,A. Kuzmin,Y. Kwon,J. Lange, I. Lee,C. Li,H. Li,L. Li,L. Li Gioi,J. Libby,D. Liventsev,P. Lukin,M. Masuda,D. Matvienko,K. Miyabayashi,H. Miyata,R. Mizuk,G. Mohanty,A. Moll,Takashi Mori,R. Mussa,E. Nakano,M. Nakao,T. Nanut,Z. Natkaniec,S. Nishida,S. Olsen,P. Pakhlov,G. Pakhlova,B. Pal,H. Park, T. Pedlar,R. Pestotnik,M. Petrić,L. Piilonen, C. Pulvermacher,E. Ribežl,M. Ritter,A. Rostomyan,H. Sahoo,Y. Sakai,S. Sandilya,T. Sanuki,V. Savinov,O. Schneider,G. Schnell,C. Schwanda,Y. Seino,D. Semmler,K. Senyo, I. Seong,M. Sevior,V. Shebalin,C. Shen,T. Shibata,J. Shiu,B. Shwartz,F. Simon, Y. Sohn,E. Solovieva,M. Starič,T. Sumiyoshi,U. Tamponi,K. Tanida,Y. Teramoto,K. Trabelsi,M. Uchida,S. Uehara,T. Uglov,S. Uno,C. Van Hulse,P. Vanhoefer,G. Varner,V. Vorobyev, M. Wagner,C. Wang,M. Wang,P. Wang,Y. Watanabe,K. M. Williams,E. Won,H. Yamamoto,J. Yamaoka,S. Yashchenko,J. Yelton,Y. Yook,C. Yuan,Z. Zhang,V. Zhilich,V. Zhulanov,A. Zupanc

Physical Review Letters(2015)

引用 0|浏览0
暂无评分
摘要
We report the analysis of the three-body e^{+}e^{-}→BB[over ¯]π^{±}, BB[over ¯]^{*}π^{±}, and B^{*}B[over ¯]^{*}π^{±} processes, including the first observations of the Z_{b}^{±}(10610)→[BB[over ¯]^{*}+c.c.]^{±} and Z_{b}^{±}(10650)→[B^{*}B[over ¯]^{*}]^{±} transitions that are found to dominate the corresponding final states. We measure Born cross sections for the three-body production of σ(e^{+}e^{-}→[BB[over ¯]^{*}+c.c.]^{±}π^{∓})=[17.4±1.6(stat)±1.9(syst)]  pb and σ(e^{+}e^{-}→[B^{*}B[over ¯]^{*}]^{±}π^{∓})=[8.75±1.15(stat)±1.04(syst)]  pb and set a 90% C.L. upper limit of σ(e^{+}e^{-}→[BB[over ¯]]^{±}π^{∓})<2.9  pb. The results are based on a 121.4  fb^{-1} data sample collected with the Belle detector at a center-of-mass energy near the ϒ(10860) peak.
更多
查看译文
AI 理解论文
溯源树
样例
生成溯源树,研究论文发展脉络
Chat Paper
正在生成论文摘要