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Exotic open-flavor bcqˉqˉbc\bar{q}\bar{q}, bcsˉsˉbc\bar{s}\bar{s} and qcqˉbˉqc\bar{q}\bar{b}, scsˉbˉsc\bar{s}\bar{b} tetraquark states

Abstract

We study the exotic bcqˉqˉbc\bar{q}\bar{q}, bcsˉsˉbc\bar{s}\bar{s} and qcqˉbˉqc\bar{q}\bar{b}, scsˉbˉsc\bar{s}\bar{b} systems by constructing the corresponding tetraquark currents with JP=0+J^P=0^+ and 1+1^+. After investigating the two-point correlation functions and the spectral densities, we perform QCD sum rule analysis and extract the masses of these open-flavor tetraquark states. Our results indicate that the masses of both the scalar and axial vector tetraquark states are about 7.17.27.1-7.2 GeV for the bcqˉqˉbc\bar{q}\bar{q} system and 7.27.37.2-7.3 GeV for the bcsˉsˉbc\bar{s}\bar{s} system. For the qcqˉbˉqc\bar{q}\bar{b} tetraquark states with JP=0+J^P=0^+ and 1+1^+, their masses are extracted to be around 7.17.1 GeV. The masses for the scalar and axial vector scsˉbˉsc\bar{s}\bar{b} states are 7.17.1 GeV and 6.97.16.9-7.1 GeV, respectively. The tetraquark states qcqˉbˉqc\bar{q}\bar{b} and scsˉbˉsc\bar{s}\bar{b} lie below the thresholds of D()B()D^{(\ast)}B^{(\ast)} and Ds()Bs()D_s^{(\ast)}B_s^{(\ast)} respectively, but they can decay into BcB_c plus a light meson. However, the tetraquark states bcqˉqˉbc\bar{q}\bar{q} and bcsˉsˉbc\bar{s}\bar{s} lie below the D()Bˉ()D^{(\ast)}\bar B^{(\ast)} and Ds()Bˉs()D_s^{(\ast)}\bar B_s^{(\ast)} thresholds, suggesting dominantly weak decay mechanisms.Comment: 18 pages, 7 figures, 4 table

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