Motion equations for free electromagnetic field [compare with (6), (17)] have the same form, that in the usual electrodynamics. Thus, having stipulated on the potentials A$_{e}$ and B$_{µ}$ the Lorentz condition usual expression for chronological coupling of operators of electromagnetic field, generated by electrical charges, may be derived and analogical expression for chronological coupling of operators of electromagnetic field, generated by magnetic charges, Because only vector potential A$_{e}$ enters in the equation (35), and only pseudovector- potential B$_{µ}$ enters in the equation(36), the chronological coupling of operators of these potentials, expressed via Green function of motion equations, is equal zero Hence, as accordingly to (27), (28) the effective potential A$_{µ}$ is a linear function of B$_{µ}$ , and the effective potential B$_{e}$ is a linear function of A$_{e}$ , chronological couplings are also equal zero. and 10 □ A k e + ∂ $^{k}$∂$_{l}$ A l e = 0 (35) □ B k µ + ∂ $^{k}$∂$_{l}$ B l µ = 0 (36) ∂$_{k}$A k e ≡ 0 , ∂$_{k}$B k µ ≡ 0 , (37) 〈 T { A k e ( x ) A l $_{e}$( y ) } 〉 = ig $^{kl}$Dc $_{0}$( x − y ) (38) 〈 T { B k $_{µ}$( x ) B l $_{µ}$( y ) } 〉 = ig $^{kl}$Dc $_{0}$( x − y ) . (39) 〈 T { A k e ( x ) B l $_{µ}$( y ) } 〉 = 0 . (40) 〈 T { A k e ( x ) A l $_{µ}$( y ) } 〉 = 0 , (41) 〈 T { A k $_{µ}$( x ) B l $_{e}$( y ) } 〉 = 0 , (42) 〈 T { B k e ( x ) B l $_{µ}$( y ) } 〉 = 0 (43)