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Stefano Maffezzoli Felis edited Energies.tex
over 8 years ago
Commit id: e7c0be96d01ca564113ce8e262841f192014a1d1
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\end{equation}
where $\alpha_{stnm}=\omega_0(\gamma_{st}-\gamma_{nm})$. Therefore, one can easily see that for $s=n$ and $t=m$ the matrix element becomes $=\delta_{MN}$ (since $D(0)=\id$).
As \textit{Rebolini} done in his thesis work \cite{ARebolini} I perform the \textit{adiabatic approximation} that consist in discarding the far-from diagonal matrix elements, i.e. for $M\neqN$.
\begin{comment} Adiabatic approximation consists in discarding the far-from diagonal matrix
elements (NM for N 6= M). This approximation can be legitimized
mathematically by inspecting the structure of Laguerre polynomials (2.2.3),