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正反重强子对构成的强子分子态能谱
引用本文:董相坤,郭奉坤,邹冰松.正反重强子对构成的强子分子态能谱[J].物理学进展,2021,41(2):65-93.
作者姓名:董相坤  郭奉坤  邹冰松
作者单位:中国科学院理论物理研究所;中国科学院大学物理科学学院;中南大学物理学院
基金项目:supported in part by the Chinese Academy of Sciences(CAS)under Grant No.XDB34030000 and No.QYZDBSSW-SYS013;the National Natural Science Foundation of China(NSFC)under Grant No.11835015,No.12047503 and No.11961141012;the NSFC and the Deutsche Forschungsgemeinschaft(DFG,German Research Foundation)through the funds provided to the Sino-German Collaborative Research Center TRR110"Symmetries and the Emergence of Structure in QCD"(NSFC Grant No.12070131001,DFG Project-ID 196253076);the CAS Center for Excellence in Particle Physics(CCEPP).
摘    要:近二十年来,世界上众多高能物理实验发现了大量超出传统夸克模型的共振结构。为了理解 这些性质奇特的共振结构,科学家们提出了很多方法和模型。其中,因为实验上发现的这些奇特态 大多处在一对强子阈值附近,强子分子态的观点得到了很多关注。本文我们将以粲{反粲强子对为例 来探究哪些系统可以形成分子态,进而给出粲{反粲强子分子态的能谱。我们考虑了所有由 S 波粲 介子、粲重子以及窄的 P 波粲介子构成的粲{反粲强子对。我们假定它们之间的相互作用由介子交 换主导,在最低阶近似下可简化为常数。通过求解常数相互作用的 Bethe---Salpeter 方程,我们可以 找到振幅的极点进而确定该系统分子态的质量。最终我们发现,那些通过轻矢量介子交换在阈值附 近产生吸引力的系统,会存在一个靠近阈值的极点。不同的系统,由于其相互作用强度不同,极点 可能会处于能量复平面的第一黎曼面或者第二黎曼面,分别对应于束缚态或者虚态。我们总共发现 了 229 个强子分子态。很多实验上发现的那些位于粲---反粲强子对阈值附近的共振结构可以很好地 与我们的结果吻合。另外,我们需要强调所预言的一个 ΛcΛc  分子态,这个态可以很好地解释北京正负电子谱仪 (BESIII) 上测量的数据。

关 键 词:强子分子态    奇特强子态    隐粲系统    极点

A survey of heavy-antiheavy hadronic molecules
Dong Xiang-Kun,Guo Feng-Kun,Zou Bing-Song.A survey of heavy-antiheavy hadronic molecules[J].Progress In Physics,2021,41(2):65-93.
Authors:Dong Xiang-Kun  Guo Feng-Kun  Zou Bing-Song
Institution:(CAS Key Laboratory of Theoretical Physics,Institute of Theoretical Physics,Chinese Academy of Sciences,Beijing 100190;School of Physical Sciences,University of Chinese Academy of Sciences,Beijing 100049;School of Physics,Central South University,Changsha 410083)
Abstract:Many efforts have been made to reveal the nature of the overabundant resonant structures observed by the worldwide experiments in the last two decades.Haxdronic molecules attract special a>ttention 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 st reng th of interaction and the cutoff.In total,229 molecular st ates are predicted.The observed near-threshold structures with hidden-charm,like the famous X(3872)and Pc states,fit into the spectrum we obtain.We also highlight a ΛcˉΛc bound state that has a pole consistent with the cross section of the e+e-→ΛcˉΛc precisely measured by the BESIII Collaboration.
Keywords:Hadronic molecules  exotic hadrons  hidden-charm systems  poles
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