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The Zb(10610) and Zb(10650) as axial-vector tetraquark states in the QCD sum rules

2013/12/31 by Zhi-Gang Wang, Tao Huang · 2 citations
Physics and Astronomy · #hep-ph #hep-ex

paper · pdf · doi:10.1016/j.nuclphysa.2014.08.084

published as Nucl.Phys.A930(2014)63-85 · 21 pages, 15 figures. arXiv admin note: substantial text overlap with arXiv:1312.1537, arXiv:1311.1046

arxiv created 2014/09/19 · arxiv updated 2014/09/22

Abstract

In this article, we study the axial-vector mesons Zb(10610) and Zb(10650) with the Cγμ-Cγ5 type and Cγμ-Cγν type interpolating currents respectively by carrying out the operator product expansion to the vacuum condensates up to dimension-10. In calculations, we explore the energy scale dependence of the QCD spectral densities of the hidden bottom tetraquark states in details for the first time, and suggest a formula μ=√M2X/Y/Z-(2\mathbbMb)2 with the effective mass \mathbbMb=5.13 \rmGeV to determine the energy scales. The numerical results favor assigning the Zb(10610) and Zb(10650) as the Cγμ-Cγ5 type and Cγμ-Cγν type hidden bottom tetraquark states, respectively. We obtain the mass of the JPC=1++ hidden bottom tetraquark state as a byproduct, which can be compared to the experimental data in the futures. Furthermore, we study the strong decays Zb^±(10610)→Υπ± , ηbρ± with the three-point QCD sum rules, the decay widths also support assigning the Zb(10610) as the Cγμ-Cγ5 type hidden bottom tetraquark state.

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