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author | kurchan.jorge <kurchan.jorge@gmail.com> | 2020-12-08 10:34:49 +0000 |
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committer | overleaf <overleaf@localhost> | 2020-12-08 10:34:50 +0000 |
commit | d1a667025fb04971f7e03aac4ac4f970bc7a6210 (patch) | |
tree | 92a92973ab48f323a4a78514c48b3cbb23281e34 | |
parent | 3bfcc79839e9311f9ca8d1ffac439922c542be86 (diff) | |
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Update on Overleaf.
-rw-r--r-- | bezout.tex | 2 |
1 files changed, 1 insertions, 1 deletions
@@ -216,7 +216,7 @@ Another instrument we have to study this problem is to compute the following par \begin{eqnarray} Z= \int \Pi_i dx_i dy_i \; e^{-\beta_{R} \Re H_0 -\beta_I \Im H_0} \delta(\sum_i z_i^2-N) \delta\left(\sum_i y_i^2 -N \frac{a-1}{2}\right) -\end{equation} +\end{eqnarray} The energy $\Re H_0, \Im H_0$ are in a one-to one relation with the temperatures $\beta_R,\beta_I$. The entropy $S(a,H_0) = \ln Z+ +\beta_{R} \langle \Re H_0 \rangle +\beta_I \langle \Im H_0\rangle$ is the logarithm of the number of configurations of a given $(a,H_0)$. |