“…Among the existing representations of S F (X) in this field, we accept the so-called Fock-Schwinger one [4,5] in which the fermion propagator has an explicitly Lorentz-covariant form. Correlations, being under an influence of the magnetic field, among the scalar, pseudoscalar, vector and axial-vector currents in the Fock-Schwinger formalism were already studied [1,2] but correlators with the tensor current j µν (x) ≡ f (x)σ µν f (x) and other currents j A (x) were not considered in this approach, except the pseudoscalar-tensor correlator calculated by us earlier [6].…”