Partial wave analysis of ψ′→π+π−π0ψ′→π+π−π0 at BESII

M Ablikim,J Z Bai,Y Ban,J G Bian,Xu Cai,J F Chang,H X Chen,J C Chen,M L Chen,Y B Chen,S P Chi,Y P Chu,X Z Cui,H L Dai,Y S Dai,Z Y Deng,L Y Dong,S X Du,Z Z Du,Jianwen Fang,S S Fang,C D Fu,H Y Fu,C S Gao,Y N Gao,M Y Gong,W X Gong,S D Gu,Y Q Guo,Z J Guo,F A Harris,K L He, Mengchang He,Xinyi He,Y K Heng,H M Hu,Ting Hu,G S Huang,Likun Huang,X P Huang,X B Ji,Q Y Jia,C H Jiang,X S Jiang,D P Jin,S Jin, Yinlong Jin,Y F Lai,Fei Li,Guohong Li,H H Li,J C Li,Q J Li,R Y Li,S M Li,Wen Ge Li,X L Li,Y F Liang,H B Liao,Chun Xia Liu,Fengping Liu,H M Liu,J B Liu,R G Liu,Z X Liu,Feng Lu,G R Lu,J G Lu,C L Luo,X L Luo,F C Ma,J M Ma,L L Ma,Q M Ma,X Y Ma,Z P Mao,X H Mo,Jing Nie,Z D Nie,S L Olsen,H P Peng,N D Qi,C D Qian, Haiying Qin,J F Qiu,Z Y Ren,G Rong,L Y Shan,Li Shang,D L Shen,X Y Shen,H Y Sheng,Feng Shi,Xin Shi,H S Sun,S S Sun,Y Z Sun,Z J Sun,X Tang,N Tao,Y R Tian,G L Tong,G Varner,D Y Wang, J Z Wang,Kun Wang,L S Wang,Miao Wang,P L Wang,S Z Wang,W F Wang,Y F Wang,Z Y Wang,C L Wei,D H Wei,Ningning Wu,Y M Wu,X M Xia,X X Xie,B Xin,G F Xu,H Xu,Yingxin Xu,S T Xue,M L Yan,Fan Yang,Hong Xia Yang, Jerry Yang,S D Yang,Y X Yang,M H Ye,Y X Ye,L H Yi,Z Y Yi,C S Yu,G W Yu,C Z Yuan,J M Yuan,Yuan Yuan,Q Yue,S L Zang,Yan Zeng,B X Zhang,C C Zhang,D H Zhang,H Y Zhang,J W Zhang,L S Zhang,Q J Zhang,S Q Zhang,X Y Zhang,Y Y Zhang,Z Q Zhang,D X Zhao,J B Zhao,M G Zhao,P P Zhao,W R Zhao,X J Zhao,Y B Zhao,Z G Zhao,H Q Zheng,J P Zheng,L S Zheng,Z P Zheng,X C Zhong,B Q Zhou,G M Zhou,Liping Zhou,N F Zhou,K J Zhu,Q M Zhu,Y S Zhu,Z A Zhu,B A Zhuang,B S Zou

Physics Letters B(2005)

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摘要
The decay ψ′→π+π−π0 is analyzed using a sample of 14 million ψ′ events taken with the BESII detector at the BEPC, and the branching fraction is measured to be B(ψ′→π+π−π0)=(18.1±1.8±1.9)×10−5. A partial wave analysis is carried out using the helicity amplitude method. ψ′→ρ(770)π is observed, and the branching fraction is measured to be B(ψ′→ρ(770)π)=(5.1±0.7±1.1)×10−5, where the first error is statistical and the second one is systematic. A high mass enhancement with mass around 2.15 GeV/c2 is also observed. Attributing this enhancement to the ρ(2150) resonance, the branching fraction is measured to be B(ψ′→ρ(2150)π→π+π−π0)=(19.4±2.5−3.4+11.5)×10−5. The results will help in the understanding of the longstanding “ρπ puzzle” between J/ψ and ψ′ hadronic decays.
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