Vector charmonium(-like) states in the energy range of 4.1-4.6 GeV
4.1-4.6 GeV 能量范围内的矢量粲偶素(类)态
Xiang-Kun Dong, Vadim Baru, Leon von Detten, Feng-Kun Guo, Christoph Hanhart, Teng Ji, Ulf-G. Meißner, Alexey Nefediev
AI总结 针对 4.1-4.6 GeV 能量区域矢量粲偶素(类)态谱的长期争议,本文发展了一个统一耦合道框架,通过同时拟合 BESIII 多个截面积数据,证明强耦合道效应和动力学产生极点可解释观测到的线形行为。
Comments 58 pages, 14 figures and 8 tables
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4.1-4.6 GeV 能量区域的矢量粲偶素(类)态谱存在长期争议。尽管包含性 $R$ 值表明只存在通常被解释为常规态的矢量粲偶素,但遍举 $e^+e^-$ 截面在采用 Breit-Wigner 函数拟合时揭示了额外的结构,其参数强烈依赖于观测的末态。这种令人困惑的模式表明耦合道和阈值效应起着关键作用。在本工作中,我们发展了一个适用于所考虑能量区域中 $1^{--}$ 共振态的统一耦合道框架。该框架包含了由重夸克自旋对称性约束的 $S$ 波开粧道 $D\bar{D}_1$、$D^*\bar{D}_1$ 和 $D^*\bar{D}_2^*$,可选的对应夸克模型态(可能与 $\psi(4160)$ 和 $\psi(4415)$ 相关)的裸极点,以及对于三体末态相关的 $Z_c$ 道中的末态相互作用。我们基于所构建的框架采用几个基准模型,对 BESIII 的 $e^+e^-\to J/\psi\pi^+\pi^-$、$h_c\pi^+\pi^-$、$D\bar{D}^*\pi$、$D^*\bar{D}^*\pi$、$J/\psi\eta$ 和 $\chi_{c0}\omega$ 截面数据,以及呈现 $Z_c(3900)$ 和 $Z_c(4020)$ 结构的可用不变质量分布进行同时拟合。这些模型在裸种子态数目和拟合策略上有所不同。我们表明,即使是纯动力学方案也能捕捉所有分析分布的主要特征。因此我们得出结论,所研究能量范围内测量线形的非平凡行为可以用强耦合道效应和动力学产生极点来理解。包含裸致密态会定量改善拟合质量,但不改变这一结论。
The spectrum of vector charmonium(-like) states in the 4.1-4.6 GeV energy region exhibits a long-standing tension. While the inclusive $R$-value indicates the presence of only vector charmonia that are usually interpreted as conventional states, exclusive $e^+e^-$ cross sections reveal additional structures whose parameters strongly depend on the observed final states when fitted with Breit-Wigner functions. This puzzling pattern suggests that coupled-channel and threshold effects play an essential role. In this work, we develop a unified coupled-channel framework relevant for the $1^{--}$ resonances in the considered energy region. The framework incorporates the $S$-wave open-charm channels $D\bar{D}_1$, $D^*\bar{D}_1$, and $D^*\bar{D}_2^*$, constrained by heavy-quark spin symmetry, optional bare poles corresponding to quark-model states which may be associated with the $ψ(4160)$ and the $ψ(4415)$, and final-state interaction in the $Z_c$ channels relevant for the three-body final states. We employ several benchmark models based on the constructed framework to perform simultaneous fits to the BESIII data for the cross sections of $e^+e^-\to J/ψπ^+π^-$, $h_cπ^+π^-$, $D\bar{D}^*π$, $D^*\bar{D}^*π$, $J/ψη$, and $χ_{c0}ω$, together with the available invariant-mass distributions that exhibit the $Z_c(3900)$ and $Z_c(4020)$ structures. The models differ in the number of bare seed states and the fitting strategy. We show that even the purely dynamical scheme captures the gross features of all the analyzed distributions. We therefore conclude that the nontrivial behavior of the measured line shapes in the studied energy range can be understood in terms of strong coupled-channel effects with dynamically generated poles. The inclusion of bare compact states leads to a quantitative improvement of the fit quality but does not alter this conclusion.