position vectors $ \vec{r}$ and $\vec{r'}$. The coupling tensors are the key parameters of this theory. As was mentioned above, it is not needed the electric and magnetic polarization fields of the medium explicitly to be appeared in the total Lagrangian (\[c1\])-(\[c4\]) as a part of degrees of freedom of the medium . As we will see, the electric polarization( magnetic polarization ) of the medium is obtained in terms of the coupling tensor $f$ ( $g$ ) and the dynamical variables $ \vec{X}_\omega $  ( $
\vec{Y}_\omega $). Also the electric susceptibility tensor ( magnetic susceptibility tensor) of the medium naturally will expressed in terms of the coupling tensor $f$ ( $g$ ). The coupling tensors $f$ and $g$ are appeared as common factors in both the noise polarization fields and the susceptibility tensors of the medium, so that for the free space the susceptibility tensors together with the noise polarizations become identically zero and this quantization scheme is reduced to the usual quantization of electromagnetic field in free space. Furthermore when the medium tends to a non-absorbing one, the coupling tensors and the noise polarizations tend also to zero and this quantization method is reduced to the quantization 