The investigations of the PP-wave BsB_s states combining quark model and lattice QCD in the coupled channel framework

Abstract

Combining the quark model, the quark-pair-creation mechanism and B(βˆ—)KB^{(*)}K interaction, we have investigated the near-threshold PP-wave BsB_s states in the framework of the Hamiltonian effective field theory. With the heavy quark flavor symmetry, all the parameters are determined in the DsD_s sector by fitting the lattice data. The masses of the bottom-strange partners of the Ds0βˆ—(2317)D^{*}_{s0}(2317) and Ds1βˆ—(2460)D^{*}_{s1}(2460) are predicted to be MBs0βˆ—=5730.2βˆ’1.5+2.4M_{B^{*}_{s0}}=5730.2_{-1.5}^{+2.4} MeV and MBs1βˆ—=5769.6βˆ’1.6+2.4M_{B^{*}_{s1}}= 5769.6_{-1.6}^{+2.4} MeV, respectively, which are well consistent with the lattice QCD simulation. The two P-wave BsB_s states are the mixtures of the bare bsΛ‰b\bar s core and B(βˆ—)KB^{(*)}K component. Moreover, we find a crossing point between the energy levels with and without the interaction Hamiltonian in the finite volume spectrum in the 0+0^+ case, which corresponds to a CDD (Castillejo-Dalitz-Dyson) zero in the TT-matrix of the BKBK scattering. This CDD zero will help deepen the insights of the near-threshold states and can be examined by the future lattice calculation.Comment: 20 pages, 4 figure

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