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Stefano Maffezzoli Felis edited Energies.tex
over 8 years ago
Commit id: 65e267755112393658d3144cc2837ef04c80b00c
deletions | additions
diff --git a/Energies.tex b/Energies.tex
index 5ea1b40..2db206e 100644
--- a/Energies.tex
+++ b/Energies.tex
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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 $D(0)=\id$).
\begin{equation}
\left(\left(H_{2q}\right)\right)= \begin{bmatrix}
h \begin{table}
\begin{tabular}{ c c c c c }
_{--}_{--} & &
h &
h &
h \\
h
&
h &
h &
h & \\
h
&
h &
h &
h & \\
\epsilon
&
h &
h &
h & \\
& & & & \\
\end{bmatrix} \end{tabular}
\end{table}
\end{equation}