Zcs(3985)− as the U -spin partner of Zc(3900)− and implication of other states in the SU(3)F symmetry and heavy quark symmetry

L. Meng, Bo Wang, Shi-Lin Zhu
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引用次数: 18

Abstract

Recently, for the first time, the BESIII Collaboration reported the strange hidden charm tetraquark states $Z_{cs}(3985)^-$ in the $K^+$ recoil-mass spectrum near the $D_{s}^{-}D^{*0}/ D_{s}^{*-}D^{0}$ mass thresholds in the processes of $e^{+}e^{-}\to K^{+}(D_{s}^{-}D^{*0}+D_{s}^{*-}D^{0})$ at $\sqrt{s}=4.681$ GeV. The significance was estimated to be 5.3 $\sigma$. We show that the newly observed $Z_{cs}(3985)^-$ state is the $U$-spin partner of $Z_c(3900)^{-}$ as a resonance within coupled-channel calculation in the $\text{SU(3)}_F$ symmetry and heavy quark spin symmetry (HQSS). In the $\text{SU(3)}_F$ symmetry, we introduce the $G_{U/V}$ parity to construct the flavor wave functions of the $Z_{cs}$ states. In a unified framework, we consider the $J/\psi\pi(K)$, $\bar{D}_{(s)}{D}^*/\bar{D}_{(s)}^*{D}$ coupled-channel effect with the contact interaction. With the masses and widths of $Z_c(3900)$ and $Z_c(4020)$, we determine all the unknown coupling constants. We obtain mass and width of $Z_{cs}(3985)$ in good agreement with the experimental results, which strongly supports the $Z_{cs}$ states as the $U/V$-spin partner states of the charged $Z_c(3900)$. We also calculate the ratio of the partial decay widths of $Z_{cs}(3985)$, which implies that the $\bar{D}_sD^*/\bar{D}^*_s D$ decay modes are dominant. We also predict the $Z_{cs}^\prime$ states with a mass around $4130$ MeV and width around $30$ MeV, which are the $U/V$-spin partner states of the charged $Z_c(4020)$ and HQSS partner states of the $Z_{cs}(3985)$. In the hidden bottom sector, we predict the strange tetraquark states $Z_{bs}$ and $Z_{bs}^\prime$ with a mass around 10700 MeV and 10750 MeV, which are the $U/V$-spin partner states of $Z_{b}(10610)^{\pm}$ and $Z_b(10650)^{\pm}$, respectively.
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Zcs(3985)−作为Zc(3900)−的u自旋伙伴以及SU(3)F对称和重夸克对称中其他态的含义
最近,BESIII合作小组首次报道了在$\sqrt{s}=4.681$ GeV的$e^{+}e^{-}\to K^{+}(D_{s}^{-}D^{*0}+D_{s}^{*-}D^{0})$过程中,在$D_{s}^{-}D^{*0}/ D_{s}^{*-}D^{0}$质量阈值附近的$K^+$反冲-质量谱中发现了奇怪的隐藏粲四夸克态$Z_{cs}(3985)^-$。显著性估计为5.3 $\sigma$。在$\text{SU(3)}_F$对称和重夸克自旋对称(HQSS)的耦合通道计算中,我们证明了新观测到的$Z_{cs}(3985)^-$态是$Z_c(3900)^{-}$作为共振的$U$ -自旋伙伴。在$\text{SU(3)}_F$对称性中,我们引入$G_{U/V}$宇称来构造$Z_{cs}$状态的风味波函数。在统一的框架中,我们考虑了$J/\psi\pi(K)$, $\bar{D}_{(s)}{D}^*/\bar{D}_{(s)}^*{D}$与接触相互作用的耦合通道效应。利用$Z_c(3900)$和$Z_c(4020)$的质量和宽度,我们确定了所有未知的耦合常数。我们得到的$Z_{cs}(3985)$的质量和宽度与实验结果吻合较好,这有力地支持了$Z_{cs}$态是带电的$Z_c(3900)$的$U/V$自旋伙伴态。我们还计算了$Z_{cs}(3985)$的部分衰减宽度的比值,这意味着$\bar{D}_sD^*/\bar{D}^*_s D$的衰减模式占主导地位。我们还预测了质量在$4130$ MeV左右、宽度在$30$ MeV左右的$Z_{cs}^\prime$态,它们是带电粒子$Z_c(4020)$的$U/V$ -自旋伴态和$Z_{cs}(3985)$的HQSS伴态。在隐藏的底部扇区,我们预测了质量在10700 MeV和10750 MeV左右的奇异四夸克态$Z_{bs}$和$Z_{bs}^\prime$,它们分别是$Z_{b}(10610)^{\pm}$和$Z_b(10650)^{\pm}$的$U/V$自旋伙伴态。
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