Ablikim M, Achasov M N, Adlarson P, Ahmed S, Albrecht M, Amoroso A, An Q, Bai Y, Bakina O, Baldini Ferroli R, Balossino I, 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, Chang J F, Chang W L, Chelkov G, Chen D Y, Chen G, Chen H S, Chen M L, Chen S J, Chen X R, 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, Du S X, 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 X L, Gao Y, Gao Y, Gao Y G, 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, Guan C Y, Guo A Q, Guo L B, Guo R P, Guo Y P, Guo Y P, Guskov A, Han S, Han T T, Han T Z, Hao X Q, Harris F A, He K L, Heinsius F H, Held T, Heng Y K, Himmelreich M, Holtmann T, Hou Y R, Hou Z L, Hu H M, Hu J F, Hu T, Hu Y, Huang G S, Huang L Q, Huang X T, Huesken N, Hussain T, Ikegami Andersson W, Imoehl W, Irshad M, Jaeger S, Janchiv S, Ji Q, Ji Q P, Ji X B, Ji X L, Jiang H B, 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, Khoukaz A, Kiese P, Kiuchi R, Kliemt R, Koch L, Kolcu O B, Kopf B, Kuemmel M, Kuessner M, Kupsc A, Kurth M G, Kühn W, Lane J J, Lange J S, Larin P, Lavezzi L, Leithoff H, Lellmann M, Lenz T, Li C, Li C H, Li Cheng, Li D M, Li F, Li G, Li H B, Li H J, Li J C, Li J L, Li Ke, Li L K, Li Lei, Li P L, Li P R, Li S Y, Li W D, Li W G, Li X H, Li X L, Li X N, Li Z B, Li Z Y, Liang H, Liang H, Liang Y F, Liang Y T, Liao L Z, Libby J, Lin C X, Lin D X, 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, Liu K Y, Liu Ke, Liu L, Liu L Y, Liu Q, Liu S B, Liu Shuai, Liu T, Liu X, Liu X Y, Liu Y B, Liu Z A, Liu Z Q, Long Y F, Lou X C, Lu H J, Lu J D, Lu J G, Lu X L, 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 R Q, Ma R T, 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 Morales C, Muchnoi N Yu, Muramatsu H, Nakhoul S, Nefedov Y, Nerling F, Nikolaev I B, Ning Z, Nisar S, Olsen S L, Ouyang Q, Pacetti S, Pan X, Pan Y, Papenbrock M, Pathak A, Patteri P, Pelizaeus M, Peng H P, Peters K, Pettersson J, Ping J L, Ping R G, Pitka A, Poling R, Prasad V, Qi H, Qi H R, Qi M, Qi T Y, Qian S, Qiao C F, Qin L Q, 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, Rivetti A, Rodin V, Rolo M, Rong G, Rosner Ch, Rump M, Sarantsev A, Savrié M, Schelhaas Y, Schnier C, Schoenning K, Shan D C, Shan W, Shan X Y, Shao M, Shen C P, Shen P X, Shen X Y, Sheng H Y, Shi H C, Shi R S, Shi X, Shi X D, Song J J, Song Q Q, Song X Y, Song Y X, Sosio S, Sowa C, Spataro S, Sui F F, Sun G X, Sun J F, Sun L, Sun S S, Sun T, Sun W Y, Sun Y J, Sun Y K, Sun Y Z, Sun Z J, Sun Z T, Tan Y X, Tang C J, Tang G Y, Tang J, Tang X, Thoren V, Tsednee B, Uman I, Wang B, Wang B L, Wang C W, Wang D Y, Wang H P, Wang K, Wang L L, Wang L S, Wang M, Wang M Z, Wang Meng, Wang P L, Wang W P, Wang X, Wang X F, Wang X L, Wang Y, Wang Y, Wang Y D, Wang Y F, Wang Y Q, Wang Z, Wang Z G, Wang Z Y, Wang Ziyi, Wang Zongyuan, Weber T, Wei D H, Weidenkaff P, Weidner F, Wen H W, Wen S P, White D J, Wiedner U, Wilkinson G, Wolke M, Wollenberg L, Wu J F, Wu L H, Wu L J, Wu X, Wu Z, Xia L, Xiao H, Xiao S Y, Xiao Y J, Xiao Z J, Xie Y G, Xie Y H, Xing T Y, Xiong X A, Xu G F, Xu J J, Xu Q J, Xu W, Xu X P, Yan L, Yan L, Yan W B, Yan W C, Yan Xu, Yang H J, Yang H X, Yang L, Yang R X, Yang S L, Yang Y H, Yang Y X, Yang Yifan, Yang Zhi, Ye M, Ye M H, Yin J H, You Z Y, Yu B X, Yu C X, Yu G, Yu J S, Yu T, Yuan C Z, Yuan W, Yuan X Q, Yuan Y, Yue C X, Yuncu A, Zafar A A, Zeng Y, Zhang B X, Zhang B Y, Zhang C C, Zhang D H, Zhang Guangyi, Zhang H H, Zhang H Y, Zhang J L, Zhang J Q, Zhang J W, Zhang J Y, Zhang J Z, Zhang Jianyu, Zhang Jiawei, Zhang L, Zhang Lei, Zhang S, Zhang S F, Zhang T J, Zhang X Y, Zhang Y, Zhang Y H, Zhang Y T, Zhang Yan, Zhang Yao, Zhang Yi, Zhang Z H, Zhang Z Y, Zhao G, Zhao J, 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, Zhong C, Zhou L, Zhou L P, Zhou Q, Zhou X, Zhou X K, Zhou X R, Zhu A N, 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. 2020 Mar 20;124(11):112001. doi: 10.1103/PhysRevLett.124.112001.
A partial-wave analysis is performed for the process e^{+}e^{-}→K^{+}K^{-}π^{0}π^{0} at the center-of-mass energies ranging from 2.000 to 2.644 GeV. The data samples of e^{+}e^{-} collisions, collected by the BESIII detector at the BEPCII collider with a total integrated luminosity of 300 pb^{-1}, are analyzed. The total Born cross sections for the process e^{+}e^{-}→K^{+}K^{-}π^{0}π^{0}, as well as the Born cross sections for the subprocesses e^{+}e^{-}→ϕπ^{0}π^{0}, K^{+}(1460)K^{-}, K_{1}^{+}(1400)K^{-}, K_{1}^{+}(1270)K^{-}, and K^{+}(892)K^{-}(892), are measured versus the center-of-mass energy. The corresponding results for e^{+}e^{-}→K^{+}K^{-}π^{0}π^{0} and ϕπ^{0}π^{0} are consistent with those of BABAR with better precision. By analyzing the cross sections for the four subprocesses, K^{+}(1460)K^{-}, K_{1}^{+}(1400)K^{-}, K_{1}^{+}(1270)K^{-}, and K^{+}(892)K^{-}(892), a structure with mass M=(2126.5±16.8±12.4) MeV/c^{2} and width Γ=(106.9±32.1±28.1) MeV is observed with an overall statistical significance of 6.3σ, although with very limited significance in the subprocesses e^{+}e^{-}→K_{1}^{+}(1270)K^{-} and K^{+}(892)K^{-}(892). The resonant parameters of the observed structure suggest it can be identified with the ϕ(2170), thus the results provide valuable input to the internal nature of the ϕ(2170).
在质心能量范围为2.000至2.644 GeV的情况下,对过程(e^{+}e^{-}\to K^{+}K^{-}\pi^{0}\pi^{0})进行了分波分析。分析了由北京正负电子对撞机(BEPCII)上的北京谱仪III(BESIII)探测器收集的(e^{+}e^{-})碰撞数据样本,其总积分亮度为300 pb⁻¹。测量了过程(e^{+}e^{-}\to K^{+}K^{-}\pi^{0}\pi^{0})的总玻恩截面,以及子过程(e^{+}e^{-}\to\phi\pi^{0}\pi^{0})、(K^{+}(1460)K^{-})、(K_{1}^{+}(1400)K^{-})、(K_{1}^{+}(1270)K^{-})和(K^{+}(892)K^{-}(892))的玻恩截面随质心能量的变化情况。(e^{+}e^{-}\to K^{+}K^{-}\pi^{0}\pi^{0})和(\phi\pi^{0}\pi^{0})的相应结果与BABAR的结果一致,且精度更高。通过分析四个子过程(K^{+}(1460)K^{-})、(K_{1}^{+}(1400)K^{-})、(K_{1}^{+}(1270)K^{-})和(K^{+}(892)K^{-}(892))的截面,观察到一个质量(M=(2126.5\pm16.8\pm12.4)) MeV/c²、宽度(\Gamma=(106.9\pm32.1\pm28.1)) MeV的结构,其总体统计显著性为6.3σ,不过在子过程(e^{+}e^{-}\to K_{1}^{+}(1270)K^{-})和(K^{+}(892)K^{-}(892))中的显著性非常有限。所观察到的结构的共振参数表明它可以被认定为(\phi(2170)),因此这些结果为(\phi(2170))的内部性质提供了有价值的信息。