Study of e(+)e(-)→ωχ(cJ) at center of mass energies from 4.21 to 4.42 GeV.

/ Authors

M. Ablikim, M. Achasov, X. Ai, O. Albayrak, M. Albrecht, D. Ambrose, A. Amoroso, F. An, Q. An, J. Bai

and 399 more authors

R. Ferroli, Y. Ban, D. Bennett, J. Bennett, M. Bertani, D. Bettoni, J. Bian, F. Bianchi, E. Boger, O. Bondarenko, I. Boyko, R. Briere, H. Cai, X. Cai, O. Cakir, A. Calcaterra, G. Cao, S. Cetin, J. Chang, G. Chelkov, G. Chen, H. Chen, H. Chen, J. Chen, M. Chen, S. Chen, X. Chen, X. Chen, Y. Chen, H. Cheng, X. Chu, Y. Chu, G. Cibinetto, D. Cronin-Hennessy, H. Dai, J. Dai, D. Dedovich, Z. Deng, A. Denig, I. Denysenko, M. Destefanis, F. De Mori, Y. Ding, C. Dong, J. Dong, L. Dong, M. Dong, S. Du, P. Duan, J. Fan, J. Fang, S. Fang, X. Fang, Y. Fang, L. Fava, F. Feldbauer, G. Felici, C. Feng, E. Fioravanti, C. Fu, Q. Gao, Y. Gao, I. Garzia, K. Goetzen, W. Gong, W. Gradl, M. Greco, M. Gu, Y. Gu, Y. Guan, A. Guo, L. Guo, T. Guo, Y. Guo, Y. Guo, Z. Haddadi, A. Hafner, S. Han, Y. Han, F. Harris, K. He, Z. He, T. Held, Y. Heng, Z. Hou, C. Hu, H. Hu, J. Hu, T. Hu, Y. Hu, G. Huang, G. Huang, H. Huang, J. Huang, X. Huang, Y. Huang, T. Hussain, Q. Ji, Q. Ji, X. Ji, X. Ji, L. Jiang, L. Jiang, X. Jiang, J. Jiao, Z. Jiao, D. Jin, S. Jin, T. Johansson, A. Julin, N. Kalantar-Nayestanaki, X. Kang, X. Kang, M. Kavatsyuk, B. Ke, R. Kliemt, B. Kloss, O. B. Kolcu, B. Kopf, M. Kornicer, W. Kuehn, A. Kupsc, W. Lai, J. Lange, M. Lara, P. Larin, Cheng Li, C. Li, D. Li, F. Li, G. Li, H. Li, J. Li, Jin Li, K. Li, K. Li, P. Li, T. Li, W. Li, W. Li, X. Li, X. Li, X. Li, X. Li, Z. Li, H. Liang, Y. Liang, Y. Liang, G. Liao, D. Lin, B. Liu, C. Liu, C. Liu, F. Liu, F. Liu, Feng. Liu, H. Liu, H. Liu, H. Liu, H. Liu, J. Liu, J. Liu, J. Liu, Li-Yu Daisy Liu, Li-Yu Daisy Liu, L. Liu, Q. Liu, S. Liu, X. Liu, X. Liu, Y. Liu, Z. Liu, Zhiqiang Liu, Zhiqing Liu, H. Loehner, X. Lou, H. Lu, J. Lu, R. Lu, Y. Lu, Y. Lu, C. Luo, M. Luo, T. Luo, X. Luo, M. Lv, X. Lyu, F. Ma, H. Ma, L. Ma, Q. Ma, S. Ma, T. Ma, X. Ma, X. Ma, F. Maas, M. Maggiora, Q. A. Malik, Y. Mao, Z. Mao, S. Marcello, J. Messchendorp, J. Min, T. Min, R. Mitchell, X. Mo, Y. Mo, H. Moeini, C. Morales, K. Moriya, N. Muchnoi, H. Muramatsu, Y. Nefedov, F. Nerling, I. Nikolaev, Z. Ning, S. Nisar, S. Niu, X. Niu, S. Olsen, Q. Ouyang, S. Pacetti, P. Patteri, M. Pelizaeus, H. Peng, K. Peters, J. Ping, R. Ping, R. Poling, Y. Pu, M. Qi, S. Qian, C. Qiao, L. Qin, N. Qin, X. Qin, Y. Qin, Z. Qin, J. Qiu, K. H. Rashid, C. Redmer, H. Ren, M. Ripka, G. Rong, X. Ruan, V. Santoro, A. Sarantsev, M. Savrié, K. Schoenning, S. Schumann, W. Shan, M. Shao, C. Shen, P. Shen, X. Shen, H. Sheng, M. Shepherd, W. Song, X. Song, S. Sosio, S. Spataro, B. Spruck, G. Sun, J. Sun, S. Sun, Y. Sun, Y. Sun, Z. Sun, Z. Sun, C. Tang, X. Tang, I. Tapan, E. Thorndike, M. Tiemens, D. Toth, M. Ullrich, I. Uman, G. Varner, B. Wang, B. Wang, D. Wang, D. Wang, K. Wang, L. Wang, L. Wang, M. Wang, P. Wang, P. Wang, Q. Wang, S. Wang, W. Wang, X. Wang, Y. Wang, Y. Wang, Y. Wang, Z. Wang, Z. Wang, Z. Wang, Z. Wang, D. Wei, J. Wei, P. Weidenkaff, S. Wen, U. Wiedner, M. Wolke, L. Wu, Z. Wu, L. Xia, Y. Xia, D. Xiao, Z. Xiao, Y. Xie, Q. L. Xiu, G. Xu, L. Xu, Q. Xu, Q. Xu, X. Xu, L. Yan, W. Yan, W. Yan, Y. Yan, H. Yang, L. Yang, Y. Yang, Y. Yang, H. Ye, M. Ye, M. Ye, J. Yin, B. Yu, C. Yu, H. Yu, J. Yu, C. Yuan, W. Yuan, Y. Yuan, A. Yuncu, A. Zafar, A. Zallo, Y. Zeng, B. Zhang, B. Zhang, C. Zhang, C. Zhang, D. Zhang, H. Zhang, H. Zhang, J. Zhang, J. Zhang, J. Zhang, J. Zhang, J. Zhang, J. Zhang, K. Zhang, L. Zhang, S. Zhang, X. Zhang, X. Zhang, Y. Zhang, Y. Zhang, Z. Zhang, Z. Zhang, Z. Zhang, G. Zhao, J. Zhao, J. Zhao, J. Zhao, Lei Zhao, Ling Zhao, M. Zhao, Q. Zhao, Q. Zhao, S. Zhao, T. Zhao, Y. Zhao, Z. Zhao, A. Zhemchugov, B. Zheng, J. Zheng, W. Zheng, Y. Zheng, B. Zhong, L. Zhou, Li Zhou, X. Zhou, X. Zhou, X. Zhou, X. Zhou, K. Zhu, K. Zhu, S. Zhu, X. Zhu, Y. Zhu, Y. Zhu, Z. Zhu, J. Zhuang, B. Zou, J. Zou

/ Abstract

Based on data samples collected with the BESIII detector at the BEPCII collider at nine center of mass energies from 4.21 to 4.42 GeV, we search for the production of e^{+}e^{-}→ωχ_{cJ} (J=0, 1, 2). The process e^{+}e^{-}→ωχ_{c0} is observed for the first time, and the Born cross sections at sqrt[s]=4.23 and 4.26 GeV are measured to be (55.4±6.0±5.9) and (23.7±5.3±3.5) pb, respectively, where the first uncertainties are statistical and the second are systematic. The ωχ_{c0} signals at the other seven energies and the e^{+}e^{-}→ωχ_{c1} and ωχ_{c2} signals are not significant, and the upper limits on the cross sections are determined. By examining the ωχ_{c0} cross section as a function of center of mass energy, we find that it is inconsistent with the line shape of the Y(4260) observed in e^{+}e^{-}→π^{+}π^{-}J/ψ. Assuming the ωχ_{c0} signals come from a single resonance, we extract the mass and width of the resonance to be (4230±8±6) MeV/c^{2} and (38±12±2) MeV, respectively, and the statistical significance is more than 9σ.

Journal: Physical review letters

DOI: 10.1103/PhysRevLett.114.092003