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Observation of a charged (DD*)± mass peak in e+ e- → πDD* at sqrt[s] = 4.26  GeV.

Authors :
Ablikim M
Achasov MN
Albayrak O
Ambrose DJ
An FF
An Q
Bai JZ
Baldini Ferroli R
Ban Y
Becker J
Bennett JV
Bertani M
Bian JM
Boger E
Bondarenko O
Boyko I
Braun S
Briere RA
Bytev V
Cai H
Cai X
Cakir O
Calcaterra A
Cao GF
Cetin SA
Chang JF
Chelkov G
Chen G
Chen HS
Chen JC
Chen ML
Chen SJ
Chen XR
Chen YB
Cheng HP
Chu XK
Chu YP
Cronin-Hennessy D
Dai HL
Dai JP
Dedovich D
Deng ZY
Denig A
Denysenko I
Destefanis M
Ding WM
Ding Y
Dong LY
Dong MY
Du SX
Fang J
Fang SS
Fava L
Feng CQ
Friedel P
Fu CD
Fu JL
Fuks O
Gao Y
Geng C
Goetzen K
Gong WX
Gradl W
Greco M
Gu MH
Gu YT
Guan YH
Guo AQ
Guo LB
Guo T
Guo YP
Han YL
Harris FA
He KL
He M
He ZY
Held T
Heng YK
Hou ZL
Hu C
Hu HM
Hu JF
Hu T
Huang GM
Huang GS
Huang JS
Huang L
Huang XT
Huang Y
Hussain T
Ji CS
Ji Q
Ji QP
Ji XB
Ji XL
Jiang LL
Jiang XS
Jiao JB
Jiao Z
Jin DP
Jin S
Jing FF
Kalantar-Nayestanaki N
Kavatsyuk M
Kloss B
Kopf B
Kornicer M
Kuehn W
Lai W
Lange JS
Lara M
Larin P
Leyhe M
Li CH
Li C
Li C
Li DL
Li DM
Li F
Li G
Li HB
Li JC
Li K
Li L
Li N
Li PR
Li QJ
Li WD
Li WG
Li XL
Li XN
Li XQ
Li XR
Li ZB
Liang H
Liang YF
Liang YT
Liao GR
Lin DX
Liu BJ
Liu CL
Liu CX
Liu FH
Liu F
Liu F
Liu HB
Liu HH
Liu HM
Liu JP
Liu K
Liu KY
Liu PL
Liu Q
Liu SB
Liu X
Liu YB
Liu ZA
Liu Z
Liu Z
Loehner H
Lou XC
Lu GR
Lu HJ
Lu JG
Lu XR
Lu YP
Luo CL
Luo MX
Luo T
Luo XL
Lv M
Ma FC
Ma HL
Ma QM
Ma S
Ma T
Ma XY
Maas FE
Maggiora M
Malik QA
Mao YJ
Mao ZP
Messchendorp JG
Min J
Min TJ
Mitchell RE
Mo XH
Moeini H
MoralesMorales C
Moriya K
Muchnoi NY
Muramatsu H
Nefedov Y
Nikolaev IB
Ning Z
Nisar S
Olsen SL
Ouyang Q
Pacetti S
Park JW
Pelizaeus M
Peng HP
Peters K
Ping JL
Ping RG
Poling R
Prencipe E
Qi M
Qian S
Qiao CF
Qin LQ
Qin XS
Qin Y
Qin ZH
Qiu JF
Rashid KH
Redmer CF
Ripka M
Rong G
Ruan XD
Sarantsev A
Schumann S
Shan W
Shao M
Shen CP
Shen XY
Sheng HY
Shepherd MR
Song WM
Song XY
Spataro S
Spruck B
Sun GX
Sun JF
Sun SS
Sun YJ
Sun YZ
Sun ZJ
Sun ZT
Tang CJ
Tang X
Tapan I
Thorndike EH
Toth D
Ullrich M
Uman I
Varner GS
Wang B
Wang D
Wang DY
Wang K
Wang LL
Wang LS
Wang M
Wang P
Wang PL
Wang QJ
Wang SG
Wang XF
Wang XL
Wang YD
Wang YF
Wang YQ
Wang Z
Wang ZG
Wang ZH
Wang ZY
Wei DH
Wei JB
Weidenkaff P
Wen QG
Wen SP
Werner M
Wiedner U
Wu LH
Wu N
Wu SX
Wu W
Wu Z
Xia LG
Xia YX
Xiao ZJ
Xie YG
Xiu QL
Xu GF
Xu QJ
Xu QN
Xu XP
Xue Z
Yan L
Yan WB
Yan WC
Yan YH
Yang HX
Yang Y
Yang YX
Yang YZ
Ye H
Ye M
Ye MH
Yu BX
Yu CX
Yu HW
Yu JS
Yu SP
Yuan CZ
Yuan WL
Yuan Y
Zafar AA
Zallo A
Zang SL
Zeng Y
Zhang BX
Zhang BY
Zhang C
Zhang CB
Zhang CC
Zhang DH
Zhang HH
Zhang HY
Zhang JL
Zhang JQ
Zhang JW
Zhang JY
Zhang JZ
Zhang L
Zhang SH
Zhang XJ
Zhang XY
Zhang Y
Zhang YH
Zhang ZP
Zhang ZY
Zhang Z
Zhao G
Zhao JW
Zhao L
Zhao L
Zhao MG
Zhao Q
Zhao SJ
Zhao TC
Zhao XH
Zhao YB
Zhao ZG
Zhemchugov A
Zheng B
Zheng JP
Zheng YH
Zhong B
Zhou L
Zhou X
Zhou XK
Zhou XR
Zhu K
Zhu KJ
Zhu XL
Zhu YC
Zhu YS
Zhu ZA
Zhuang J
Zou BS
Zou JH
Source :
Physical review letters [Phys Rev Lett] 2014 Jan 17; Vol. 112 (2), pp. 022001. Date of Electronic Publication: 2014 Jan 15.
Publication Year :
2014

Abstract

We report on a study of the process e+ e- → π± (DD*)∓ at sqrt[s] = 4.26  GeV using a 525 pb(-1) data sample collected with the BESIII detector at the BEPCII storage ring. A distinct charged structure is observed in the (DD*)∓ invariant mass distribution. When fitted to a mass-dependent-width Breit-Wigner line shape, the pole mass and width are determined to be Mpole = (3883.9±1.5(stat)±4.2(syst))  MeV/c2 and Γpole = (24.8±3.3(stat)±11.0(syst))  MeV. The mass and width of the structure, which we refer to as Zc(3885), are 2σ and 1σ, respectively, below those of the Zc(3900) → π± J/ψ peak observed by BESIII and Belle in π+ π- J/ψ final states produced at the same center-of-mass energy. The angular distribution of the πZc(3885) system favors a JP = 1+ quantum number assignment for the structure and disfavors 1- or 0-. The Born cross section times the DD* branching fraction of the Zc(3885) is measured to be σ(e+ e- → π± Zc(3885)∓)×B(Zc(3885)∓ → (DD*)∓) = (83.5±6.6(stat)±22.0(syst))   pb. Assuming the Zc(3885) → DD* signal reported here and the Zc(3900) → πJ/ψ signal are from the same source, the partial width ratio (Γ(Zc(3885) → DD*)/Γ(Zc(3900) → πJ/ψ)) = 6.2±1.1(stat)±2.7(syst) is determined.

Details

Language :
English
ISSN :
1079-7114
Volume :
112
Issue :
2
Database :
MEDLINE
Journal :
Physical review letters
Publication Type :
Academic Journal
Accession number :
24484002
Full Text :
https://doi.org/10.1103/PhysRevLett.112.022001