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Open charm-bottom axial-vector tetraquarks and their properties

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Table 1 Input parameters
Fig. 1 The perturbative and nonperturbative contributions to the sum rule as functions of M 2 at an average s
Fig. 3 The mass (left panel) and meson–current coupling (right panel) as functions of the Borel parameter M 2 at fixed values of the continuum threshold s 0
Fig. 4 The pole contribution in the g Z q B c ρ coupling sum rule calculations as a function of the Borel parameter M 2 at fixed s 0 (left panel), and as
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