势夸克模型中的粲双重子共振

M. Oka, Saori Maeda, Yan-Rui Liu
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引用次数: 7

摘要

具有自旋宇称[公式:见文]和[公式:见文]的粲双重子态被预测为两体[公式:见文]([公式:见文],[公式:见文]或[公式:见文])系统。我们对耦合通道的哈密顿量采用了我们之前研究中提出的[公式:见文]-CTNN电位的复标度方法。我们在[公式:见文]和[公式:见文]阈值附近发现了四个尖锐的共振状态。通过对部分通道系统结合能的分析,我们得出这些共振态是费什巴赫共振。我们将结果与[公式:见文]重夸克极限下的共振态(其中[公式:见文]和[公式:见文]阈值是简并的)进行比较,发现它们形成了两对符合重夸克自旋对称的重夸克双重态。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Charmed dibaryon resonances in the potential quark model
Charmed dibaryon states with the spin-parity [Formula: see text], and [Formula: see text] are predicted for the two-body [Formula: see text] ([Formula: see text], [Formula: see text], or [Formula: see text]) systems. We employ the complex scaling method for the coupled channel Hamiltonian with the [Formula: see text]-CTNN potentials, which were proposed in our previous study. We find four sharp resonance states near the [Formula: see text] and [Formula: see text] thresholds. From the analysis of the binding energies of partial channel systems, we conclude that these resonance states are Feshbach resonances. We compare the results with the [Formula: see text] resonance states in the heavy quark limit, where the [Formula: see text] and [Formula: see text] thresholds are degenerate, and find that they form two pairs of the heavy-quark doublets in agreement with the heavy quark spin symmetry.
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