Measurement of the branching fractions of ψ ( 2 S ) → 3 ( π + π − ) and J / ψ → 2 ( π + π − )

Mei Wang,L S Wang,Kun Wang,J Z Wang, D Y Wang, G Varner, G L Tong, Y R Tian, N Tao,X Tang,Z J Sun,Y Z Sun,S S Sun,J F Sun,H S Sun,Xiaohong Shi,Feng Shi,H Y Sheng, X Y Shen, D L Shen,L Shang,L Y Shan,G Rong,Z Y Ren,J F Qiu, H Qin, C D Qian, N D Qi, H P Peng,S L Olsen,Z D Nie,Jun Nie, X H Mo, Z P Mao,X B Ma, Q M Ma, L L Ma, J M Ma, H L Ma, F C Ma, X L Luo, L X Luo, C L Luo, J G Lu,H J Lu, G R Lu,Feng Lu,Z X Liu,R G Liu,J B Liu, H H Liu, Fang Liu,C X Liu, H B Liao, Y F Liang, Y L Li,X Q Li, W D Li,S M Li, R Y Li,Q J Li, J C Li,H B Li,Guoyu Li, Feitao Li,Y F Lai,Yi Jin, S Jin, D P Jin, X S Jiang, C H Jiang,X B Ji,X T Huang, G S Huang,Tianjiang Hu,H M Hu,Y K Heng, Xihao He, M He, K L He,F A Harris, Z J Guo,Y N Guo,S D Gu, W X Gong,M Y Gong,Y N Gao, C S Gao, H Y Fu, C D Fu, S S Fang,Jianpei Fang,Z Z Du, S X Du,Q F Dong,L Y Dong,Z Y Deng,Y S Dai, H L Dai, X Z Cui, Y P Chu,S P Chi, Y B Chen, M L Chen, J C Chen, H X Chen,J F Chang,Xin Cai, J G Bian,Y Ban, J Z Bai, M Ablikim, C Z Yuan, G W Yu, C S Yu,Z Y Yi, L H Yi,Y X Ye, M H Ye,Y X Yang,Juan Yang,H X Yang,Feng Yang, M L Yan, S T Xue,Hong Xu, G F Xu,B Xin, X X Xie, X M Xia,Y M Wu,N Wu, D H Wei, C L Wei, Z Y Wang,Y F Wang, W F Wang,S Z Wang,P L Wang, B S Zou,X A Zhuang,B A Zhuang,Z A Zhu, Y S Zhu,Q M Zhu, K J Zhu,N F Zhou,Lei Zhou,G M Zhou,B Q Zhou, X C Zhong, Z P Zheng,L S Zheng, J P Zheng, H Q Zheng, Z G Zhao,Y B Zhao,X J Zhao,W R Zhao, P P Zhao, M G Zhao,J W Zhao,D X Zhao,Z Q Zhang,Y Y Zhang,X Y Zhang,S Q Zhang,Q J Zhang,J Y Zhang,H Y Zhang,Dong H Zhang, C C Zhang,B Y Zhang,Yu Zeng,S L Zang,Y Yuan, J M Yuan

Physical Review D(2005)

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摘要
Using data samples collected at {radical}(s)=3.686 GeV and 3.650 GeV by the BESII detector at the BEPC, the branching fraction of {psi}(2S){yields}3({pi}{sup +}{pi}{sup -}) is measured to be [5.45{+-}0.42(stat){+-}0.87(syst)]x10{sup -4}, and the relative branching fraction of J/{psi}{yields}2({pi}{sup +}{pi}{sup -}) to that of J/{psi}{yields}{mu}{sup +}{mu}{sup -} is measured to be [6.01{+-}0.20(stat){+-}0.48(syst)]% via {psi}(2S){yields}{pi}{sup +}{pi}{sup -}J/{psi},J/{psi}{yields}2({pi}{sup +}{pi}{sup -}). The electromagnetic form factor of 3({pi}{sup +}{pi}{sup -}) is determined to be 0.19{+-}0.02 and 0.24{+-}0.02 at {radical}(s)=3.650 GeV and 3.686 GeV, respectively.
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