Abstract
The spectrum of the S-wave \(\bar{Q}Q\bar{q}q\) (where \(Q=c,b\) and \(q=u,d,s\)) system are studied within two constituent quark models. The bound states of \(B^*\bar{B}^*\) with \(I(J^{PC})=1(0^{++}),~1(1^{+-}),~0(2^{++})\) and \(B\bar{B}^*\) with isospin \(I=1\), or 0 are obtained in color-singlet-singlet channel. If considering the coupling of color channels, apart from the deep bound states appear in \([b\bar{q}]^{(*)}[q\bar{b}]^{(*)}\) scenario, a bound state \([c\bar{q}]^*[q\bar{c}]^*\) with \(I(J^{PC})=1(0^{++})\) is also formed. The \(B\bar{B}^*\) and the \(B^*\bar{B}^*\) with quantum number \(1(1^{+-})\) are good candidates for \(Z_b^{\pm }(10{,}610)\) and \(Z_b^{\pm }(10{,}650)\) reported by Belle Collaboration respectively, while the \(B\bar{B}^*\) with isospin 0 can be interpret as a candidate for \(Z_b^{0}(10{,}610)\). A bound state \([c\bar{q}]^*[q\bar{c}]^*\) with \(I(J^{PC})=1(0^{++})\) may be found in the \(e^+e^-\rightarrow D^*\bar{D}^*\pi \pi \) channel in the future by BES and other experimental collaborations.
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Acknowledgements
This work is supported partly by the National Science Foundation of China (under Contracts Nos. 11865019, 11675080, 11775118, 11535005, and 11690030), and the China Postdoctoral Science Foundation (under Grant No. 2015M571727), and by the Guizhou province outstanding youth science and technology talent cultivation object special funds (under Grant No. QKHRZ(2013)28).
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Yang, YC., Tan, ZY., Zong, HS. et al. Dynamical Study of S-Wave \(\bar{Q}Q\bar{q}q\) System. Few-Body Syst 60, 9 (2019). https://doi.org/10.1007/s00601-018-1477-5
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DOI: https://doi.org/10.1007/s00601-018-1477-5