Ablikim M, Achasov M N, Adlarson P, Ahmed S, Albrecht M, Alekseev M, Amoroso A, An F F, An Q, Bai Y, Bakina O, Ferroli R Baldini, Ban Y, Begzsuren K, Bennett J V, Berger N, Bertani M, Bettoni D, Bianchi F, Biernat J, Bloms J, Boyko I, Briere R A, Cai H, Cai X, Calcaterra A, Cao G F, Cao N, Cetin S A, Chai J, Chang J F, Chang W L, Chelkov G, Chen D Y, Chen G, Chen H S, Chen J C, Chen M L, Chen S J, Chen Y B, Cheng W, Cibinetto G, Cossio F, Cui X F, Dai H L, Dai J P, Dai X C, Dbeyssi A, Dedovich D, Deng Z Y, Denig A, Denysenko I, Destefanis M, De Mori F, Ding Y, Dong C, Dong J, Dong L Y, Dong M Y, Dou Z L, Du S X, Fan J Z, Fang J, Fang S S, Fang Y, Farinelli R, Fava L, Feldbauer F, Felici G, Feng C Q, Fritsch M, Fu C D, Fu Y, Gao Q, Gao X L, Gao Y, Gao Y, Gao Y G, Gao Z, Garillon B, Garzia I, Gersabeck E M, Gilman A, Goetzen K, Gong L, Gong W X, Gradl W, Greco M, Gu L M, Gu M H, Gu S, Gu Y T, Guo A Q, Guo L B, Guo R P, Guo Y P, Guskov A, Han S, Hao X Q, Harris F A, He K L, Heinsius F H, Held T, Heng Y K, Hou Y R, Hou Z L, Hu H M, Hu J F, Hu T, Hu Y, Huang G S, Huang J S, Huang X T, Huang X Z, Huesken N, Hussain T, Andersson W Ikegami, Imoehl W, Irshad M, Ji Q, Ji Q P, Ji X B, Ji X L, Jiang H L, Jiang X S, Jiang X Y, Jiao J B, Jiao Z, Jin D P, Jin S, Jin Y, Johansson T, Kalantar-Nayestanaki N, Kang X S, Kappert R, Kavatsyuk M, Ke B C, Keshk I K, Khan T, Khoukaz A, Kiese P, Kiuchi R, Kliemt R, Koch L, Kolcu O B, Kopf B, Kuemmel M, Kuessner M, Kupsc A, Kurth M, Kurth M G, Kühn W, Lange J S, Larin P, Lavezzi L, Leithoff H, Lenz T, Li C, Li Cheng, Li D M, Li F, Li F Y, Li G, Li H B, Li H J, Li J C, Li J W, Li Ke, Li L K, Li Lei, Li P L, Li P R, Li Q Y, Li W D, Li W G, Li X H, Li X L, Li X N, Li X Q, Li Z B, Liang H, Liang H, Liang Y F, Liang Y T, Liao G R, Liao L Z, Libby J, Lin C X, Lin D X, Lin Y J, Liu B, Liu B J, Liu C X, Liu D, Liu D Y, Liu F H, Liu Fang, Liu Feng, Liu H B, Liu H M, Liu Huanhuan, Liu Huihui, Liu J B, Liu J Y, Liu K Y, Liu Ke, Liu Q, Liu S B, Liu T, Liu X, Liu X Y, Liu Y B, Liu Z A, Liu Zhiqing, Long Y F, Lou X C, Lu H J, Lu J D, Lu J G, Lu Y, Lu Y P, Luo C L, Luo M X, Luo P W, Luo T, Luo X L, Lusso S, Lyu X R, Ma F C, Ma H L, Ma L L, Ma M M, Ma Q M, Ma X N, Ma X X, Ma X Y, Ma Y M, Maas F E, Maggiora M, Maldaner S, Malde S, Malik Q A, Mangoni A, Mao Y J, Mao Z P, Marcello S, Meng Z X, Messchendorp J G, Mezzadri G, Min J, Min T J, Mitchell R E, Mo X H, Mo Y J, Morales C Morales, Muchnoi N Yu, Muramatsu H, Mustafa A, Nakhoul S, Nefedov Y, Nerling F, Nikolaev I B, Ning Z, Nisar S, Niu S L, Olsen S L, Ouyang Q, Pacetti S, Pan Y, Papenbrock M, Patteri P, Pelizaeus M, Peng H P, Peters K, Pettersson J, Ping J L, Ping R G, Pitka A, Poling R, Prasad V, Qi M, Qi T Y, Qian S, Qiao C F, Qin N, Qin X P, Qin X S, Qin Z H, Qiu J F, Qu S Q, Rashid K H, Ravindran K, Redmer C F, Richter M, Ripka M, Rivetti A, Rodin V, Rolo M, Rong G, Rosner Ch, Rump M, Sarantsev A, Savri M, Schoenning K, Shan W, Shan X Y, Shao M, Shen C P, Shen P X, Shen X Y, Sheng H Y, Shi X, Shi X D, Song J J, Song Q Q, Song X Y, Sosio S, Sowa C, Spataro S, Sui F F, Sun G X, Sun J F, Sun L, Sun S S, Sun X H, Sun Y J, Sun Y K, Sun Y Z, Sun Z J, Sun Z T, Tan Y T, Tang C J, Tang G Y, Tang X, Thoren V, Tsednee B, Uman I, Wang B, Wang B L, Wang C W, Wang D Y, Wang H H, Wang K, Wang L L, Wang L S, Wang M, Wang M Z, Wang Meng, Wang P L, Wang R M, Wang W P, Wang X, Wang X F, Wang X L, Wang Y, Wang Y F, Wang Z, Wang Z G, Wang Z Y, Wang Zongyuan, Weber T, Wei D H, Weidenkaff P, Wen H W, Wen S P, Wiedner U, Wilkinson G, Wolke M, Wu L H, Wu L J, Wu Z, Xia L, Xia Y, Xiao S Y, Xiao Y J, Xiao Z J, Xie Y G, Xie Y H, Xing T Y, Xiong X A, Xiu Q L, Xu G F, Xu J J, Xu L, Xu Q J, Xu W, Xu X P, Yan F, Yan L, Yan W B, Yan W C, Yan Y H, Yang H J, Yang H X, Yang L, Yang R X, Yang S L, Yang Y H, Yang Y X, Yang Yifan, Yang Z Q, Ye M, Ye M H, Yin J H, You Z Y, Yu B X, Yu C X, Yu J S, Yuan C Z, Yuan X Q, Yuan Y, Yuncu A, Zafar A A, Zeng Y, Zhang B X, Zhang B Y, Zhang C C, Zhang D H, Zhang H H, Zhang H Y, Zhang J, Zhang J L, Zhang J Q, Zhang J W, Zhang J Y, Zhang J Z, Zhang K, Zhang L, Zhang S F, Zhang T J, Zhang X Y, Zhang Y, Zhang Y H, Zhang Y T, Zhang Yang, Zhang Yao, Zhang Yi, Zhang Yu, Zhang Z H, Zhang Z P, Zhang Z Y, Zhao G, Zhao J W, Zhao J Y, Zhao J Z, Zhao Lei, Zhao Ling, Zhao M G, Zhao Q, Zhao S J, Zhao T C, Zhao Y B, Zhao Z G, Zhemchugov A, Zheng B, Zheng J P, Zheng Y, Zheng Y H, Zhong B, Zhou L, Zhou L P, Zhou Q, Zhou X, Zhou X K, Zhou X R, Zhou Xiaoyu, Zhou Xu, Zhu A N, Zhu J, Zhu J, Zhu K, Zhu K J, Zhu S H, Zhu W J, Zhu X L, Zhu Y C, Zhu Y S, Zhu Z A, Zhuang J, Zou B S, Zou J H
Institute of High Energy Physics, Beijing 100049, People's Republic of China.
G.I. Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk 630090, Russia.
Phys Rev Lett. 2019 Jun 14;122(23):232002. doi: 10.1103/PhysRevLett.122.232002.
We study the e^{+}e^{-}→γωJ/ψ process using 11.6 fb^{-1} e^{+}e^{-} annihilation data taken at center-of-mass energies from sqrt[s]=4.008 GeV to 4.600 GeV with the BESIII detector at the BEPCII storage ring. The X(3872) resonance is observed for the first time in the ωJ/ψ system with a significance of more than 5σ. The relative decay ratio of X(3872)→ωJ/ψ and π^{+}π^{-}J/ψ is measured to be R=1.6_{-0.3}^{+0.4}±0.2, where the first uncertainty is statistical and the second systematic (the same hereafter). The sqrt[s]-dependent cross section of e^{+}e^{-}→γX(3872) is also measured and investigated, and it can be described by a single Breit-Wigner resonance, referred to as the Y(4200), with a mass of 4200.6_{-13.3}^{+7.9}±3.0 MeV/c^{2} and a width of 115_{-26}^{+38}±12 MeV. In addition, to describe the ωJ/ψ mass distribution above 3.9 GeV/c^{2}, we need at least one additional Breit-Wigner resonance, labeled as X(3915), in the fit. The mass and width of the X(3915) are determined. The resonant parameters of the X(3915) agree with those of the Y(3940) in B→KωJ/ψ and of the X(3915) in γγ→ωJ/ψ observed by the Belle and BABAR experiments within errors.
我们使用在北京正负电子对撞机(BEPCII)储存环上的北京谱仪III(BESIII)探测器,在质心能量从(\sqrt{s}=4.008) GeV到4.600 GeV范围内采集的(11.6,\text{fb}^{-1})正负电子湮灭数据,研究(e^{+}e^{-}\to\gamma\omega J/\psi)过程。首次在(\omega J/\psi)系统中观测到(X(3872))共振,显著性超过(5\sigma)。测量得到(X(3872)\to\omega J/\psi)与(\pi^{+}\pi^{-}J/\psi)的相对衰变率为(R = 1.6_{-0.3}^{+0.4}\pm0.2),其中第一个不确定度是统计性的,第二个是系统性的(此后相同)。还测量并研究了(e^{+}e^{-}\to\gamma X(3872))的(\sqrt{s})依赖的截面,它可以用一个单一的布赖特 - 维格纳共振来描述,称为(Y(4200)),其质量为(4200.6_{-13.3}^{+7.9}\pm3.0,\text{MeV}/c^{2}),宽度为(115_{-26}^{+38}\pm12,\text{MeV})。此外,为了描述高于(3.9,\text{GeV}/c^{2})的(\omega J/\psi)质量分布,在拟合中我们至少需要一个额外的布赖特 - 维格纳共振,标记为(X(3915))。确定了(X(3915))的质量和宽度。在误差范围内,(X(3915))的共振参数与在(B\to K\omega J/\psi)中观测到的(Y(3940))以及在(\gamma\gamma\to\omega J/\psi)中由Belle和BABAR实验观测到的(X(3915))的共振参数一致。