The $\mathbf{\bar{q}q\bar{s}Q}$ $\mathbf{(q=u,\,d;\,Q=c,\,b)}$ tetraquark system in a chiral quark model

Gang Yang, Jia-Lun 平加伦 Ping, Jorge Segovia
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Abstract

The $S$-wave $\bar{q}q\bar{s}Q$ $(q=u,\,d;\,Q=c,\,b)$ tetraquarks, with spin-parity $J^P=0^+$, $1^+$ and $2^+$, in both isoscalar and isovector sectors are systematically studied in a chiral quark model. The meson-meson, diquark-antidiquark and K-type arrangements of quarks, along with all possible color wave functions, are comprehensively considered. The four-body system is solved by means of a highly efficient computational approach, the Gaussian expansion method, along with a complex-scaling formulation of the problem to disentangle bound, resonance and scattering states. This theoretical framework has already been successfully applied in various tetra- and penta-quark systems. In the complete coupled-channel case, and within the complex-range formulation, several narrow resonances of $\bar{q}q\bar{s}c$ and $\bar{q}q\bar{s}b$ systems are obtained, in each allowed $I(J^P)$-channels, within the energy regions $2.4-3.4$ GeV and $5.7-6.7$ GeV, respectively. The predicted exotic states, which are an indication of a richer color structure when going towards multiquark systems beyond mesons and baryons, are expected to be confirmed in future high-energy particle and nuclear experiments.Content from this work may be used under the terms of the Creative Commons Attribution 3.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI. Article funded by SCOAP3 and published under licence by Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Science and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd.
手性夸克模型中的 $mathbf{ (q=u,\,d;\,Q=c,\,b)}$ 四夸克系统
在手性夸克模型中系统地研究了自旋奇偶性为$J^P=0^+$、$1^+$和$2^+$的$S$波$\bar{q}q\bar{s}Q$$(q=u,\,d;\,Q=c,\,b)$四夸克,它们在等标量和等矢量部门都具有自旋奇偶性$J^P=0^+$、$1^+$和$2^+$。全面考虑了介子-介子、二夸克-反夸克和 K 型夸克排列,以及所有可能的颜色波函数。四体系统是通过一种高效的计算方法--高斯展开法--以及一种复杂的缩放问题表述来解决的,从而将束缚态、共振态和散射态区分开来。这一理论框架已成功应用于各种四夸克和五夸克系统。在完全耦合通道的情况下,在复范围公式中,分别在2.4-3.4 GeV和5.7-6.7 GeV的能量区域内,在每个允许的$I(J^P)$通道中,得到了$\bar{q}q\bar{s}c$和$\bar{q}q\bar{s}b$系统的若干窄共振。所预测的奇异状态表明,在介子和重子之外的多夸克系统中,还有更丰富的颜色结构,有望在未来的高能粒子和核实验中得到证实。对本作品的任何进一步传播都必须注明作者、作品名称、期刊引文和 DOI。文章由 SCOAP3 资助,由中国物理学会、中国科学院高能物理研究所、中国科学院近代物理研究所和 IOP Publishing Ltd. 授权出版。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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