content_image/371565.jpg content_image/371566.jpg content_image/371567.jpg content_image/371568.jpg content_image/371569.jpg content_image/371570.jpg content_image/371571.jpg content_image/371572.jpg content_image/371573.jpg
Motion equations for free electromagnetic field [compare with (6), (17)] 

and 

<img src='content_image/371565.jpg'>

<img src='content_image/371566.jpg'>

have the same form, that in the usual electrodynamics. Thus, having stipulated on the potentials A$_{e}$ and B$_{µ}$ the Lorentz condition 

<img src='content_image/371567.jpg'>

usual expression for chronological coupling of operators of electromagnetic field, generated by electrical charges, may be derived 

<img src='content_image/371568.jpg'>

and analogical expression for chronological coupling of operators of electromagnetic field, generated by magnetic charges, 

<img src='content_image/371569.jpg'>

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 

<img src='content_image/371570.jpg'>

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. 

<img src='content_image/371571.jpg'>

<img src='content_image/371572.jpg'>

<img src='content_image/371573.jpg'>

