Study ofχcJradiative decays into a vector meson

M. Ablikim,M. N. Achasov, D. Alberto, L. An, Q. An, Z. H. An,J. Z. Bai,R. Baldini, Y. Ban,Jürgen Becker,Niklaus Berger, M. Bertani, J. M. Bian,O. Bondarenko,Igor Boyko,R. A. Briere, V. V. Bytev, X. Cai,G. F. Cao, X. X. Cao,J. F. Chang, G. A. Chelkov,Guo-Ming Chen, H. S. Chen, J. C. Chen,M. L. Chen, S. J. Chen,Yong Chen,Yuanbo Chen,H. P. Cheng,Y. P. Chu,D. Cronin-Hennessy,H. L. Dai,J. P. Dai, D. V. Dedovich,Z. Y. Deng, I. Denysenko,M. Destefanis, Y. Ding,L. Y. Dong,M. Y. Dong, S. X. Du,R. R. Fan, J. Fang,S. S. Fang,C. Q. Feng, C. D. Fu,J. L. Fu,Y.N. Gao, C. Geng, K. Goetzen,W. X. Gong,Michela Greco, S. Grishin, M. H. Gu,Y. T. Gu,Y. H. Guan,A. Q. Guo,L. B. Guo,Y. P. Guo, X. Q. Hao,F. A. Harris,K. L. He,Miao He,Z. Y. He,Y. K. Heng,Z. L. Hou,H. M. Hu,J. F. Hu, T. Hu, B. Huang,Guangming Huang,J. S. Huang,X. T. Huang,Yanping Huang,Talib Hussain,C. S. Ji,Q. P. Ji,X. B. Ji,X. L. Ji, L. K. Jia,L. L. Jiang,X. S. Jiang, J. B. Jiao,Z. Jiao, D. P. Jin, S. Jin, F. Jing,Nasser Kalantar-Nayestanaki,M. Kavatsyuk,Sachio Komamiya,W. Kuehn,J. S. Lange,J. K. C. Leung, Cheng Li, Cui Li,D. M. Li,F. Li,G. Li,H. B. Li,J. C. Li, Lei Li,N. B. Li,Q. J. Li,W. D. Li,W. G. Li,Xingguo Li,X. N. Li,Xiang Li,X. R. Li,Z. B. Li,H. Liang,Y. F. Liang,Y. T. Liang, G. R. Liao,X. T. Liao, Bing Liu,Chuan Liu,C. X. Liu,Chang Liu,Fu-Hu Liu,Fang Liu, Feng Liu,G. C. Liu,H. H. Liu,H. B. Liu,H. M. Liu,Hang Liu, J. P. Liu, K. Y. Liu,K. Y. Liu,Q. Liu, S. B. Liu,X. Liu,X. H. Liu, Y. B. Liu, Y. W. Liu, Yong Liu,Z. A. Liu,Zhiqing Liu,H. Loehner,G. R. Lu,H. J. Lu,J. G. Lu,Qi-Wen Lü,Xiao-Tong Lu, Y. P. Lu, C. L. Luo, M. X. Luo,Tao Luo, X. L. Luo,C. L. Ma,F. C. Ma,H. L. Ma, Q. M. Ma,T. Ma,X. B. Ma,X. Y. Ma, M. Maggiora,Q. A. Malik,H. Mao, Y. J. Mao,Z. P. Mao, J. G. Messchendorp, J. Min, R. E. Mitchell, X. H. Mo,N. Yu. Muchnoi,Y. Nefedov, Z. Ning,S. L. Olsen,Q. Ouyang, S. Pacetti, M. Pelizaeus,Krisztian Peters,Jialun Ping, R. G. Ping,R. Poling,Chun S. J. Pun, M. Qi,S. Qian,Cong-Feng Qiao,X. S. Qin, J. F. Qiu,K. H. Rashid,G. Rong,Xiangdong Ruan, A. Sarantsev, Julian Schulze,M. Shao,C. P. Shen, X. Y. Shen, H. Y. Sheng,M. R. Shepherd, X. Y. Song,S. Sonoda, S. Spataro,B. Spruck,D. H. Sun,G. X. Sun,J. F. Sun,S. S. Sun,X. Sun,Y. J. Sun,Yuhan Sun,Z. J. Sun,Zhe Sun, C. J. Tang, X. Tang, X. F. Tang,H. L. Tian,D. Toth,G. S. Varner,X. Wan,B. L. Wang,Ke Wang,L. L. Wang,L. S. Wang,Meng Wang,P. L. Wang,P. L. Wang, Qun-Yao Wang,Shan Wang,X. L. Wang, Yao Wang,Y. F. Wang, Y. Q. Wang,Zujian Wang, Z. G. Wang, Z. Y. Wang, D. H. Wei,Q. G. Wen,S. P. Wen,Ulrich Wiedner,L. H. Wu,N. Wu,Wei Wu,Z. Wu,Z. J. Xiao, Y. G. Xie, G. F. Xu, G. M. Xu, H.S. Xu, Y. Xu,Zhihao Xu,Z. Z. Xu,Z. Xue,Li Yan,W. B. Yan, Y. H. Yan, H. X. Yang,Mingming Yang,T. Yang,Youchang Yang, Y. X. Yang, M. H. Ye, M. H. Ye,B. X. Yu,C. X. Yu,L. Yu,C. Z. Yuan,W. L. Yuan,Ye Yuan,A. A. Zafar,A. Zallo, Y. Zeng,B. X. Zhang,B. Y. Zhang,C. C. Zhang,D. H. Zhang,H. H. Zhang,H. Y. Zhang, J. Zhang,J. Y. Zhang,J. Y. Zhang,J. Y. Zhang,L. Zhang,S. H. Zhang,T. R. Zhang,Xuantong Zhang,X. Y. Zhang,Y. Zhang, Y. Zhang, Zhenyu Zhang,Zhiyong Zhang,Gang Zhao,HongSheng Zhao,Jiawei Zhao,Jingwei Zhao,Lei Zhao,Ling Zhao,M. G. Zhao,Q. Zhao,Shujun Zhao, Ting Zhao,X. H. Zhao,Y. B. Zhao,Z. G. Zhao,Z. L. Zhao,A. Zhemchugov,B. Zheng,Jianping Zheng, Y. H. Zheng,Z. P. Zheng,B. Zhong, J. Zhong,L. Zhong, L. P. Zhou,X. K. Zhou,X. R. Zhou,Cheng Guang Zhu,K. J. Zhu,K. J. Zhu,Shou-hua Zhu,Xiaofeng Zhu,Xiaobo Zhu,Y. S. Zhu,Z. A. Zhu, J. Zhuang,B. S. Zou,J. H. Zou,J. X. Zuo,P. Zweber

user-5fe1a78c4c775e6ec07359f9(2011)

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摘要
The decays $\chi_{cJ}\to\gamma V$ ($V=\phi, \rho^0, \omega$) are studied with a sample of radiative $\psip\to\gamma\chi_{cJ}$ events in a sample of $(1.06\pm0.04)\times 10^{8} \psip$ events collected with the BESIII detector. The branching fractions are determined to be: ${\cal B}(\chi_{c1}\to \gamma\phi)=(25.8\pm 5.2\pm 2.3)\times 10^{-6}$, ${\cal B}(\chi_{c1}\to \gamma\rho^0)=(228\pm 13\pm 22)\times 10^{-6}$, and ${\cal B}(\chi_{c1}\to \gamma\omega)=(69.7\pm 7.2\pm 6.6)\times 10^{-6}$. The decay $\chi_{c1}\to \gamma\phi$ is observed for the first time. Upper limits at the 90% confidence level on the branching fractions for $\chi_{c0}$ and $\chict$ decays into these final states are determined. In addition, the fractions of the transverse polarization component of the vector meson in $\chi_{c1}\to \gamma V$ decays are measured to be $0.29_{-0.12-0.09}^{+0.13+0.10}$ for $\chi_{c1}\to \gamma\phi$, $0.158\pm 0.034^{+0.015}_{-0.014}$ for $\chi_{c1}\to \gamma\rho^0$, and $0.247_{-0.087-0.026}^{+0.090+0.044}$ for $\chi_{c1}\to \gamma\omega$, respectively. The first errors are statistical and the second ones are systematic.
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关键词
Vector meson,Electron–positron annihilation,Omega,Radiative transfer,Nuclear physics,Particle physics,Physics,Branching (version control)
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