重-反-重强子分子的研究进展

Xiang-Kun Dong, F. Guo, B. Zou
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引用次数: 65

摘要

在过去的二十年里,人们做了许多努力来揭示世界范围内实验观察到的过多共振结构的性质。强子分子吸引了特别的注意,因为许多这些看似非常规的共振位于一对强子的阈值附近。为了给出由一对重-反重强子组成的强子分子光谱的总体特征,即哪对强子可能形成分子态,我们以粲强子为例,研究它们之间的相互作用,并通过求解Bethe-Salpeter方程寻找极点。我们考虑了$S$波单粲介子和重子以及狭窄的$P$波粲介子的强子对的所有可能组合。相互作用被假定为介子交换饱和,用恒定的接触项来描述,这些接触项被恢复为产生极点。结果表明,如果一个系统在阈值附近被光介子交换吸引,则根据相互作用的强度和截止,在阈值附近存在一个与束缚态或虚态相对应的极。总共预测了229种分子状态。观测到的具有隐藏魅力的近阈值结构,如著名的$X(3872)$和$P_c$状态,符合我们获得的光谱。我们还强调了一个$\Lambda_c\bar \Lambda_c$束缚态,它的极点与BESIII合作精确测量的$e^+e^-\to\Lambda_c\bar \Lambda_c$的横截面一致。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A survey of heavy-antiheavy hadronic molecules
Many efforts have been made to reveal the nature of the overabundant resonant structures observed by the worldwide experiments in the last two decades. Hadronic molecules attract special attention because many of these seemingly unconventional resonances are located close to the threshold of a pair of hadrons. To give an overall feature of the spectrum of hadronic molecules composed of a pair of heavy-antiheavy hadrons, namely, which pairs are possible to form molecular states, we take charmed hadrons for example to investigate the interaction between them and search for poles by solving the Bethe-Salpeter equation. We consider all possible combinations of hadron pairs of the $S$-wave singly-charmed mesons and baryons as well as the narrow $P$-wave charmed mesons. The interactions, which are assumed to be meson-exchange saturated, are described by constant contact terms which are resummed to generate poles. It turns out that if a system is attractive near threshold by the light meson exchange, there is a pole close to threshold corresponding to a bound state or a virtual state, depending on the strength of interaction and the cutoff. In total, 229 molecular states are predicted. The observed near-threshold structures with hidden-charm, like the famous $X(3872)$ and $P_c$ states, fit into the spectrum we obtain. We also highlight a $\Lambda_c\bar \Lambda_c$ bound state that has a pole consistent with the cross section of the $e^+e^-\to\Lambda_c\bar \Lambda_c$ precisely measured by the BESIII Collaboration.
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