涉及 $D\bar{D}^*$、$πJ/ψ$ 和 $ρη_c $ 的 $Z_c(3900)$ 的三耦合通道分析

Kang Yu, Guang-Juan Wang, Jia-Jun Wu, Zhi Yang
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引用次数: 0

摘要

在这项工作中,我们基于单玻色子交换模型,对$Z_c(3900)$结构进行了三耦合信道分析,重点分析了$D\bar{D}^*$、$J/\psi \pi$和$\rho \eta_c$信道。借鉴之前对奇异态$T_{cc}$的研究,我们只利用多一个参数来构建通道之间的相互作用。我们的模型成功地再现了三个信道在$\sqrt{s} =4.23$和$4.26$ GeV时不变质量分布的实验线形。详细分析表明,$\pi J/\psi$ 和$\rho \eta_c$ 分布中的$Z_c(3900)$峰值主要来自涉及$D_1 \bar{D} 的三角环。D^*$ 中间系统。在$D\bar{D}^*$分布中,阈值峰是由三角图增强的级联衰变机制产生的。此外,我们还发现了一个远离阈值的虚拟极点,表明 $Z_c(3900)$ 峰与物理极点无关。我们得出结论,$Z_c(3900)$ 峰主要是由阈值尖顶引起的。
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A Three-Coupled-Channel Analysis of $Z_c(3900)$ Involving $D\bar{D}^*$, $πJ/ψ$, and $ρη_c $
In this work, we conduct a three-coupled-channel analysis of the $Z_c(3900)$ structure, focusing on the $D\bar{D}^*$, $J/\psi \pi$, and $\rho \eta_c$ channels, based on the one-boson exchange model. Drawing from previous study on the exotic state $T_{cc}$, we only utilize one more parameter to construct the interactions between the channels. Our model successfully reproduces the experimental line shapes of the invariant mass distribution at $\sqrt{s} = 4.23$ and $4.26$ GeV for the three channels. Additionally, the finite-volume energy levels in our model show agreement with current LQCD conclusion. Detailed analysis suggests that the $Z_c(3900)$ peaks in the $\pi J/\psi$ and $\rho \eta_c$ distributions primarily arise from the triangle loop involving the $D_1 \bar{D} D^*$ intermediate system. In the $D\bar{D}^*$ distribution, the threshold peak is generated by the cascade decay mechanism enhanced by a triangle diagram. Moreover, we find a virtual pole located far from the threshold, indicating that $Z_c(3900)$ peaks are not associated with physical pole. We conclude that the $Z_c(3900)$ peaks are predominantly caused by the threshold cusp.
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