Observation and Spin-Parity Determination of the X(1835) in J/ψ→γK_{S}^{0}K_{S}^{0}η.

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 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,S X Du, P F Duan, E E Eren,J Z Fan,J Fang,S S Fang,X Fang,Y Fang, L Fava, F Feldbauer,G Felici, C Q Feng,E Fioravanti,M Fritsch, C D Fu,Q Gao,X Y Gao,Y Gao, Z Gao, I Garzia, C Geng,K Goetzen, W X Gong,W Gradl,M Greco,M H Gu,Y T Gu,Y H Guan,A Q Guo,L B Guo,Y Guo,Y P Guo,Z Haddadi,A Hafner,S Han,Y L Han, X Q Hao,F A Harris,K L He,Z Y He,T Held,Y K Heng,Z L Hou,C Hu,H M Hu, J F Hu, T Hu, Y Hu,G M Huang,G S Huang, H P Huang,J S Huang,X T Huang, Y Huang,T Hussain,Q Ji,Q P Ji,X B Ji,X L Ji,L L Jiang,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,W Kühn,A Kupsc, J S Lange,M Lara,P Larin,C Leng,C Li,C H Li,Cheng Li,D M Li, F Li,G Li, H B Li,J C Li,Jin Li,K Li,K Li,Lei Li,P R Li, T Li,W D Li,W G Li,X L Li,X M Li,X N Li,X Q Li,Z B Li,H Liang,Y F Liang,Y T Liang, G R Liao, D X Lin,B J Liu,C X 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 Liu,K Y Liu,L D Liu,P L Liu,Q Liu,S B Liu,X Liu,X X Liu,Y B Liu,Z A Liu,Zhiqiang Liu,Zhiqing Liu, H Loehner,X C Lou, H J Lu, J G Lu, R Q Lu,Y Lu,Y P Lu, C L Luo, M X Luo,T Luo, X L Luo,M Lv, X R Lyu, F C Ma,H L Ma,L L Ma, Q M Ma,T Ma,X N Ma,X Y 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,K Moriya,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,P Patteri,M Pelizaeus, H P Peng,K Peters,J Pettersson, J L Ping, R G Ping,R Poling,V Prasad,Y N Pu, M Qi, S Qian, C F Qiao,L Q Qin,N Qin,X S Qin,Y Qin, Z H Qin, J F Qiu, K H Rashid, C F Redmer,H L Ren, M Ripka, G Rong,Ch Rosner, X D Ruan,V Santoro, A Sarantsev,M Savrié,K Schoenning,S Schumann, W Shan,M Shao,C P Shen,P X Shen,X Y Shen,H Y Sheng,W M Song,X Y Song, S Sosio, S Spataro, G X Sun,J F Sun,S S 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, S G Wang,W Wang, X F Wang, Y D Wang, Y F Wang, Y Q Wang, Z Wang, Z G Wang, Z H Wang, Z Y Wang,T Weber, D H Wei, J B Wei, P Weidenkaff,S P Wen,U Wiedner, M Wolke,L H Wu,Z Wu, L G Xia,Y Xia, D Xiao,Z J Xiao,Y G Xie,Q L Xiu,G F 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 Yang,Y X Yang,H Ye,M Ye,M H Ye, J H Yin,B X Yu,C X Yu, H W Yu, J S Yu,C Z Yuan,W L Yuan,Y Yuan, A Yuncu,A A Zafar,A Zallo, Y Zeng, B X Zhang, B Y Zhang,C Zhang,C C Zhang, D H Zhang, H H Zhang, H Y Zhang, J J Zhang,J L Zhang, J Q Zhang, J W Zhang, J Y Zhang, J Z Zhang,K Zhang,L Zhang, S H Zhang, X Y Zhang, Y Zhang, Y N Zhang, Y H 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,Li Zhou,X Zhou,X K Zhou,X R Zhou,X Y Zhou,K Zhu,K J Zhu,S 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(2015)

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摘要
We report an observation of the process J/ψ→γX(1835)→γK_{S}^{0}K_{S}^{0}η at low K_{S}^{0}K_{S}^{0} mass with a statistical significance larger than 12.9σ using a data sample of 1.31×10^{9} J/ψ events collected with the BESIII detector. In this region of phase space the K_{S}^{0}K_{S}^{0} system is dominantly produced through the f_{0}(980). By performing a partial wave analysis, we determine the spin parity of the X(1835) to be J^{PC}=0^{-+}. The mass and width of the observed X(1835) are 1844±9(stat)_{-25}^{+16}(syst)  MeV/c^{2} and 192_{-17}^{+20}(stat)_{-43}^{+62}(syst)  MeV, respectively, which are consistent with the results obtained by BESIII in the channel J/ψ→γπ^{+}π^{-}η^{'}.
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BESIII,Spin-Parity,Determination,X(1835)
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