论文标题
关于$ d^*_ s \ bar d_ {s1} $在伯特 - 盐板框架内的可能分子状态的研究
Study on the possible molecular state composed of $D^*_s\bar D_{s1} $ within the Bethe-Salpeter framework
论文作者
论文摘要
最近,在$ d^+_ sd_ {s1}(2536)^ - $的门户中观察到了一个类似charmonium的状态$ y(4626)$。它引起了人们对共振结构的积极讨论,因为它具有明显的意义,可以更好地了解其具有适当的内部成分的望子结构。它确实涉及有关外来状态可能结构的一般理论框架。由于$ y(4626)$的质量略高于$ d^+_ s \ bar d_ {s1}(2536)^ - ^ - 而低于$ d^*_ s \ bar d_ s1} {s1}(2536)$的$ d^*_ s \ bar d^+d^+d^+d^s $ \ bar d_ s1 s11(2536)要猜想$ y(4626)$作为$ d^{*} _ s \ bar d_ {s1}(2536)$的分子状态,如文献中所建议。确认或否定这一指控将阐明我们所关注的目标。我们计算由向量介子和轴向向量组成的系统的质谱,即$ d^*_ s \ bar d_ {s1}(2536)$在Bethe-Salpeter方程的框架内。我们的数值结果表明,在现象学上引入每个顶点的尺寸中无量纲参数$λ$,远远超出了诱导甚至很小的绑定能$ΔE$的合理范围。这意味着$ d^*_ s \ bar d _ {s1}(2536)$ $系统在此模型中作为一种辐射分子在本质中不存在,因此我们可能不会认为是resonance $ y(4626)$作为$ d^*_ s \ bar d_ s \ bar d_ s1 {s1}(2536)$ and and andra,但某些东西,但
Recently a vector charmonium-like state $Y(4626)$ was observed in the portal of $D^+_sD_{s1}(2536)^-$. It intrigues an active discussion on the structure of the resonance because it has obvious significance for gaining a better understanding on its hadronic structure with suitable inner constituents. It indeed concerns the general theoretical framework about possible structures of exotic states. Since the mass of $Y(4626)$ is slightly above the production threshold of $D^+_s\bar D_{s1}(2536)^-$ whereas below that of $D^*_s\bar D_{s1}(2536)$ with the same quark contents as that of $D^+_s\bar D_{s1}(2536)^-$, it is natural to conjecture $Y(4626)$ to be a molecular state of $D^{*}_s\bar D_{s1}(2536)$, as suggested in literature. Confirming or negating this allegation would shed light on the goal we concern. We calculate the mass spectrum of a system composed of a vector meson and an axial vector i.e. $D^*_s\bar D_{s1}(2536)$ within the framework of the Bethe-Salpeter equations. Our numerical results show that the dimensionless parameter $λ$ in the form factor which is phenomenologically introduced to every vertex, is far beyond the reasonable range for inducing an even very small binding energy $ΔE$. It implies that the $D^*_s\bar D_{s1}(2536)$ system cannot exist in the nature as a hadronic molecule in this model, so that we may not think the resonance $Y(4626)$ to be a bound state of $D^*_s\bar D_{s1}(2536)$, but something else, for example a tetraquark and etc.