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Hidden-charm and bottom meson-baryon molecules coupled with five-quark states

机译:隐藏的魅力和底部介子 - 重子分子加上五夸克   状态

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摘要

In this paper, we investigate the hidden-charm pentaquarks as$\bar{D}^{(\ast)}\Lambda_{\rm c}$ and $\bar{D}^{(\ast)}\Sigma^{(\ast)}_{\rm c}$molecules coupled to the five-quark states. Furthermore, we extend ourcalculations to the hidden-bottom sector. The coupling to the five-quark statesis treated as the short range potential, where the relative strength for themeson-baryon channels is determined by the structure of the five-quark states.We found that resonant and/or bound states appear in both the charm and bottomsectors. The five-quark state potential turned out to be attractive and, forthis reason, it plays an important role to produce these states. In the charmsector, we need the five-quark potential in addition to the pion exchangepotential in producing bound and resonant states, whereas, in the bottomsector, the pion exchange interaction is strong enough to produce states. Thus,from this investigation, it emerges that the hidden-bottom pentaquarks are morelikely to form than their hidden-charm counterparts; for this reason, wesuggest that the experimentalists should look for states in the bottom sector.
机译:在本文中,我们以$ \ bar {D} ^ {(\ ast)} \ Lambda _ {\ rm c} $和$ \ bar {D} ^ {(\ ast)} \ Sigma ^ {(\ ast)} _ {\ rm c} $个分子耦合到五夸克状态。此外,我们将计算范围扩展到隐藏的底端部分。与五夸克状态的耦合被视为短距离电势,themeson-baryon通道的相对强度由五夸克状态的结构决定。我们发现共振态和/或束缚态都出现在魅力中和底端部门。五夸克态势极具吸引力,因此,它在产生这些态中起着重要作用。在魅惑区,除了产生介导态和共振态的介子交换电位外,我们还需要五夸克电位,而在底层界,介子交换相互作用足以产生态。因此,从这项调查中可以看出,与之相比,隐身五夸克更容易形成。因此,我们建议实验者应在最底层寻找状态。

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