Abstract

Magnetic moments of charged and neutral mesons are calculated with the use of the relativistic Hamiltonian derived from the path integral form of the q1qˉ2q_1\bar q_2 Green's function. The magnetic moments are shown to be expressed via the average quark energies which are defined by the fundamental quantities: the string tension σσ, the current quark masses, and the strong coupling constant αsα_s. Resulting values for vector, axial, and tensor light and KK mesons agree well with all available lattice data.

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