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Application of the Covariant Spectator Theory to the Study of Heavy and Heavy-Light Mesons

机译:协方差理论在重介子和重介子研究中的应用

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摘要

As an application of the Covariant Spectator Theory (CST) we calculate the spectrum of heavy-light and heavy-heavy mesons using covariant versions of a linear confining potential, a one-gluon exchange, and a constant interaction. The CST equations possess the correct one-body limit and are therefore well-suited to describe mesons in which one quark is much heavier than the other. We find a good fit to the mass spectrum of heavy-light and heavy-heavy mesons with just three parameters (apart from the quark masses). Remarkably, the fit parameters are nearly unchanged when we fit to experimental pseudoscalar states only or to the whole spectrum. Because pseudoscalar states are insensitive to spin-orbit interactions and do not determine spin-spin interactions separately from central interactions, this result suggests that it is the covariance of the kernel that correctly predicts the spin-dependent quark-antiquark interactions.
机译:作为协变旁观者理论(CST)的一种应用,我们使用线性约束势,单胶子交换和恒定相互作用的协变形式来计算重轻介子和重介子的频谱。 CST方程具有正确的单体极限,因此非常适合描述其中一个夸克比另一个夸克重的介子。我们发现只有三个参数(除了夸克质量外)非常适合重轻介子和重介子的质谱。值得注意的是,当我们仅拟合实验伪标量状态或整个光谱时,拟合参数几乎不变。因为伪标量状态对自旋-轨道相互作用不敏感,并且不能独立于中心相互作用确定自旋-自旋相互作用,所以该结果表明正是内核的协方差正确地预测了自旋相关的夸克-反夸克相互作用。

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