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 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 , the current quark masses, and the strong coupling constant . Resulting values for vector, axial, and tensor light and mesons agree well with all available lattice data.
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