transform of the magnetic susceptibility tensor which is written in terms the coupling tensor $\underline{g}$ as $$\label{c37}
\underline{\chi}^m(\vec{k},\vec{q}, t)=\left\{
\begin{array}{cc}
  \mu_0\int_0^\infty d\omega \frac{\sin \omega t}{\omega}\int d^3p \ \underline{g}(\omega , \vec{k} , \vec{p}) \cdot
  \underline{g}^\dag(\omega , \vec{q} , \vec{p}) & t> 0 \\
  \\
  0 & t\leq 0
\end{array}\right.$$ and $$\label{c38}
\underline{\vec{M}}_N(\vec{k},t)=\int_0^\infty d\omega\int d^3p \
\underline{g}( \omega ,
\vec{k},\vec{p})\cdot\left(\underline{\vec{\Pi}}_\omega(\vec{p},0)\frac{\sin
\omega t }{\omega}+ \underline{\vec{Y}}_\omega(\vec{p},0)\cos \omega
t\right)$$ is the noise magnetic polarization density. Therefore modeling an anisotropic magnetodielectric medium with two independent collections of harmonic oscillators, that is, the $E$ and $M$ field, we successfully have constructed a fully canonical quantization of electromagnetic field in the presence of such a medium, so that the Maxwell equations together with the constitutive equations of the medium have been obtained from the Heisenberg equations of the total system. In this method the susceptibility tenors of the medium are concluded in terms of the coupling tensors which are the key parameters of this theory and are describing the coupling of the electromagnetic field with the medium.\
The Equations (\[c32\]) and (\[c37\]) relate the parameters of this theory, that is the coupling tensors $f$ and $g$, to the physical quantities $\underline{\chi}^e$ and $\underline{\chi}^m$ . If the coupling tensors 