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在 e+ e- → πDD* 中观测到带电荷的 (DD*)± 质量峰,在 sqrt[s] = 4.26  GeV。

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

机构信息

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.

出版信息

Phys Rev Lett. 2014 Jan 17;112(2):022001. doi: 10.1103/PhysRevLett.112.022001. Epub 2014 Jan 15.

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.

摘要

我们报道了在 sqrt[s] = 4.26  GeV 下用 BESIII 探测器在 BEPCII 储存环上采集的 525 pb(-1) 数据样本中对 e+ e- → π± (DD*)∓过程的研究。在 (DD*)∓不变质量分布中观察到一个明显的带电结构。当用依赖质量的宽度 Breit-Wigner 线形状拟合时,极点质量和宽度确定为 Mpole = (3883.9±1.5(stat)±4.2(syst))  MeV/c2 和 Γpole = (24.8±3.3(stat)±11.0(syst))  MeV。我们称之为 Zc(3885)的结构的质量和宽度分别比 BESIII 和 Belle 在相同质心能量下产生的 π+ π- J/ψ 末态中观察到的 Zc(3900) → π± J/ψ 峰低 2σ 和 1σ。πZc(3885)系统的角分布有利于结构的 JP = 1+量子数赋值,并不利于 1-或 0-。测量 Zc(3885)的产生截面乘以 DD分支比 σ(e+ e- → π± Zc(3885)∓)×B(Zc(3885)∓ → (DD)∓) = (83.5±6.6(stat)±22.0(syst))   pb。假设这里报道的 Zc(3885) → DD信号和 Zc(3900) → πJ/ψ信号来自同一来源,则确定了部分宽度比 (Γ(Zc(3885) → DD)/Γ(Zc(3900) → πJ/ψ)) = 6.2±1.1(stat)±2.7(syst)。

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