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First Observation of a Three-Resonance Structure in e^{+}e^{-}→Nonopen Charm Hadrons.

Authors :
Ablikim M
Achasov MN
Adlarson P
Ai XC
Aliberti R
Amoroso A
An MR
An Q
Bai Y
Bakina O
Balossino I
Ban Y
Batozskaya V
Begzsuren K
Berger N
Berlowski M
Bertani M
Bettoni D
Bianchi F
Bianco E
Bortone A
Boyko I
Briere RA
Brueggemann A
Cai H
Cai X
Calcaterra A
Cao GF
Cao N
Cetin SA
Chang JF
Chang TT
Chang WL
Che GR
Chelkov G
Chen C
Chen C
Chen G
Chen HS
Chen ML
Chen SJ
Chen SM
Chen T
Chen XR
Chen XT
Chen YB
Chen YQ
Chen ZJ
Cheng WS
Choi SK
Chu X
Cibinetto G
Coen SC
Cossio F
Cui JJ
Dai HL
Dai JP
Dbeyssi A
de Boer RE
Dedovich D
Deng ZY
Denig A
Denysenko I
Destefanis M
De Mori F
Ding B
Ding XX
Ding Y
Ding Y
Dong J
Dong LY
Dong MY
Dong X
Du MC
Du SX
Duan ZH
Egorov P
Fan YL
Fang J
Fang SS
Fang WX
Fang Y
Farinelli R
Fava L
Feldbauer F
Felici G
Feng CQ
Feng JH
Fischer K
Fritsch M
Fritzsch C
Fu CD
Fu JL
Fu YW
Gao H
Gao YN
Gao Y
Garbolino S
Garzia I
Ge PT
Ge ZW
Geng C
Gersabeck EM
Gilman A
Goetzen K
Gong L
Gong WX
Gradl W
Gramigna S
Greco M
Gu MH
Gu YT
Guan CY
Guan ZL
Guo AQ
Guo LB
Guo MJ
Guo RP
Guo YP
Guskov A
Han TT
Han WY
Hao XQ
Harris FA
He KK
He KL
Heinsius FHH
Heinz CH
Heng YK
Herold C
Holtmann T
Hong PC
Hou GY
Hou XT
Hou YR
Hou ZL
Hu HM
Hu JF
Hu T
Hu Y
Huang GS
Huang KX
Huang LQ
Huang XT
Huang YP
Hussain T
Hüsken N
Imoehl W
Irshad M
Jackson J
Jaeger S
Janchiv S
Jeong JH
Ji Q
Ji QP
Ji XB
Ji XL
Ji YY
Jia XQ
Jia ZK
Jiang HJ
Jiang LL
Jiang PC
Jiang SS
Jiang TJ
Jiang XS
Jiang Y
Jiao JB
Jiao Z
Jin S
Jin Y
Jing MQ
Johansson T
Kui X
Kabana S
Kalantar-Nayestanaki N
Kang XL
Kang XS
Kappert R
Kavatsyuk M
Ke BC
Khoukaz A
Kiuchi R
Kliemt R
Kolcu OB
Kopf B
Kuessner MK
Kupsc A
Kühn W
Lane JJ
Larin P
Lavania A
Lavezzi L
Lei TT
Lei ZH
Leithoff H
Lellmann M
Lenz T
Li C
Li C
Li CH
Li C
Li DM
Li F
Li G
Li H
Li HB
Li HJ
Li HN
Li H
Li JR
Li JS
Li JW
Li KL
Li K
Li LJ
Li LK
Li L
Li MH
Li PR
Li QX
Li SX
Li T
Li WD
Li WG
Li XH
Li XL
Li X
Li YG
Li ZJ
Li ZX
Liang C
Liang H
Liang H
Liang H
Liang YF
Liang YT
Liao GR
Liao LZ
Liao YP
Libby J
Limphirat A
Lin DX
Lin T
Liu BJ
Liu BX
Liu C
Liu CX
Liu FH
Liu F
Liu F
Liu GM
Liu H
Liu HB
Liu HM
Liu H
Liu H
Liu JB
Liu JL
Liu JY
Liu K
Liu KY
Liu K
Liu L
Liu LC
Liu L
Liu MH
Liu PL
Liu Q
Liu SB
Liu T
Liu WK
Liu WM
Liu X
Liu Y
Liu Y
Liu YB
Liu ZA
Liu ZQ
Lou XC
Lu FX
Lu HJ
Lu JG
Lu XL
Lu Y
Lu YP
Lu ZH
Luo CL
Luo MX
Luo T
Luo XL
Lyu XR
Lyu YF
Ma FC
Ma HL
Ma JL
Ma LL
Ma MM
Ma QM
Ma RQ
Ma RT
Ma XY
Ma Y
Ma YM
Maas FE
Maggiora M
Malde S
Malik QA
Mangoni A
Mao YJ
Mao ZP
Marcello S
Meng ZX
Messchendorp JG
Mezzadri G
Miao H
Min TJ
Mitchell RE
Mo XH
Muchnoi NY
Nefedov Y
Nerling F
Nikolaev IB
Ning Z
Nisar S
Niu Y
Olsen SL
Ouyang Q
Pacetti S
Pan X
Pan Y
Pathak A
Patteri P
Pei YP
Pelizaeus M
Peng HP
Peters K
Ping JL
Ping RG
Plura S
Pogodin S
Prasad V
Qi FZ
Qi H
Qi HR
Qi M
Qi TY
Qian S
Qian WB
Qiao CF
Qin JJ
Qin LQ
Qin XP
Qin XS
Qin ZH
Qiu JF
Qu SQ
Redmer CF
Ren KJ
Rivetti A
Rodin V
Rolo M
Rong G
Rosner C
Ruan SN
Salone N
Sarantsev A
Schelhaas Y
Schoenning K
Scodeggio M
Shan KY
Shan W
Shan XY
Shangguan JF
Shao LG
Shao M
Shen CP
Shen HF
Shen WH
Shen XY
Shi BA
Shi HC
Shi JL
Shi JY
Shi QQ
Shi RS
Shi X
Song JJ
Song TZ
Song WM
Song YJ
Song YX
Sosio S
Spataro S
Stieler F
Su YJ
Sun GB
Sun GX
Sun H
Sun HK
Sun JF
Sun K
Sun L
Sun SS
Sun T
Sun WY
Sun Y
Sun YJ
Sun YZ
Sun ZT
Tan YX
Tang CJ
Tang GY
Tang J
Tang YA
Tao LY
Tao QT
Tat M
Teng JX
Thoren V
Tian WH
Tian WH
Tian Y
Tian ZF
Uman I
Wang SJ
Wang B
Wang BL
Wang B
Wang CW
Wang DY
Wang F
Wang HJ
Wang HP
Wang JP
Wang K
Wang LL
Wang M
Wang M
Wang S
Wang S
Wang T
Wang TJ
Wang W
Wang W
Wang WP
Wang X
Wang XF
Wang XJ
Wang XL
Wang Y
Wang YD
Wang YF
Wang YH
Wang YN
Wang YQ
Wang Y
Wang Y
Wang Z
Wang ZL
Wang ZY
Wang Z
Wei D
Wei DH
Weidner F
Wen SP
Wenzel CW
Wiedner UW
Wilkinson G
Wolke M
Wollenberg L
Wu C
Wu JF
Wu LH
Wu LJ
Wu X
Wu XH
Wu Y
Wu YJ
Wu Z
Xia L
Xian XM
Xiang T
Xiao D
Xiao GY
Xiao H
Xiao SY
Xiao YL
Xiao ZJ
Xie C
Xie XH
Xie Y
Xie YG
Xie YH
Xie ZP
Xing TY
Xu CF
Xu CJ
Xu GF
Xu HY
Xu QJ
Xu QN
Xu W
Xu WL
Xu XP
Xu YC
Xu ZP
Xu ZS
Yan F
Yan L
Yan WB
Yan WC
Yan XQ
Yang HJ
Yang HL
Yang HX
Yang T
Yang Y
Yang YF
Yang YX
Yang Y
Yang ZW
Yao ZP
Ye M
Ye MH
Yin JH
You ZY
Yu BX
Yu CX
Yu G
Yu JS
Yu T
Yu XD
Yuan CZ
Yuan L
Yuan SC
Yuan XQ
Yuan Y
Yuan ZY
Yue CX
Zafar AA
Zeng FR
Zeng X
Zeng Y
Zeng YJ
Zhai XY
Zhai YC
Zhan YH
Zhang AQ
Zhang BL
Zhang BX
Zhang DH
Zhang GY
Zhang H
Zhang HH
Zhang HH
Zhang HQ
Zhang HY
Zhang JJ
Zhang JL
Zhang JQ
Zhang JW
Zhang JX
Zhang JY
Zhang JZ
Zhang J
Zhang J
Zhang LM
Zhang LQ
Zhang L
Zhang P
Zhang QY
Zhang S
Zhang S
Zhang XD
Zhang XM
Zhang XY
Zhang X
Zhang Y
Zhang Y
Zhang YT
Zhang YH
Zhang Y
Zhang Y
Zhang ZH
Zhang ZL
Zhang ZY
Zhang ZY
Zhao G
Zhao J
Zhao JY
Zhao JZ
Zhao L
Zhao L
Zhao MG
Zhao SJ
Zhao YB
Zhao YX
Zhao ZG
Zhemchugov A
Zheng B
Zheng JP
Zheng WJ
Zheng YH
Zhong B
Zhong X
Zhou H
Zhou LP
Zhou X
Zhou XK
Zhou XR
Zhou XY
Zhou YZ
Zhu J
Zhu K
Zhu KJ
Zhu L
Zhu LX
Zhu SH
Zhu SQ
Zhu TJ
Zhu WJ
Zhu YC
Zhu ZA
Zou JH
Zu J
Source :
Physical review letters [Phys Rev Lett] 2024 May 10; Vol. 132 (19), pp. 191902.
Publication Year :
2024

Abstract

We report the measurement of the inclusive cross sections for e^{+}e^{-}→nOCH (where nOCH denotes non-open charm hadrons) with improved precision at center-of-mass (c.m.) energies from 3.645 to 3.871 GeV. We observe three resonances: R(3760), R(3780), and R(3810) with significances of 8.1σ, 13.7σ, and 8.8σ, respectively. The R(3810) state is observed for the first time, while the R(3760) and R(3780) states are observed for the first time in the nOCH cross sections. Two sets of resonance parameters describe the energy-dependent line shape of the cross sections well. In set I [set II], the R(3810) state has mass (3805.7±1.1±2.7) [(3805.7±1.1±2.7)]  MeV/c^{2}, total width (11.6±2.9±1.9) [(11.5±2.8±1.9)]  MeV, and an electronic width multiplied by the nOCH decay branching fraction of (10.9±3.8±2.5) [(11.0±3.4±2.5)]  eV. In addition, we measure the branching fractions B[R(3760)→nOCH]=(25.2±16.1±30.4)%[(6.4±4.8±7.7)%] and B[R(3780)→nOCH]=(12.3±6.6±8.3)%[(10.4±4.8±7.0)%] for the first time. The R(3760) state can be interpreted as an open-charm (OC) molecular state, but containing a simple four-quark state component. The R(3810) state can be interpreted as a hadrocharmonium state.

Details

Language :
English
ISSN :
1079-7114
Volume :
132
Issue :
19
Database :
MEDLINE
Journal :
Physical review letters
Publication Type :
Academic Journal
Accession number :
38804946
Full Text :
https://doi.org/10.1103/PhysRevLett.132.191902