Amplitude Analysis of the Decays η^{'}→π^{+}π^{-}π^{0} and η^{'}→π^{0}π^{0}π^{0}.

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

PHYSICAL REVIEW LETTERS(2017)

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摘要
Based on a sample of 1.31 x 10(9) J/Psi events collected with the BESIII detector, an amplitude analysis of the isospin-violating decays eta' -> pi(+)pi(-)pi(0) and eta' -> pi(0)pi(0)pi(0) is performed. A significant P-wave contribution from eta' -> rho(+/-)eta(-/+) is observed for the first time in eta' -> pi(+)pi(-)pi(0). The branching fraction is determined to be B(eta' -> rho(+/-)pi(-/+)) = (7.44 +/- 0.60 +/- 1.26 +/- 1.84) x 10(-4), where the first uncertainty is statistical, the second systematic, and the third model dependent. In addition to the nonresonant S-wave component, there is a significant sigma meson component. The branching fractions of the combined S-wave components are determined to be B(eta' -> pi(+)pi(-)pi(0))(S) = (37.63 +/- 0.77 +/- 2.22 +/- 4.48) x 10(-4) and B(eta' -> pi(0)pi(0)pi(0)) = (35.22 +/- 0.82 +/- 2.54) x 10(-4), respectively. The latter one is consistent with previous BESIII measurements.
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