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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-06-08 20:11:56 +0200 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-06-08 20:11:56 +0200 |
commit | 929067069100dbdeb78f3982fd3d1a5735183a3e (patch) | |
tree | b735f0648e15515aadb2bec444f8278ab5105371 | |
parent | cc283f06405bd4929479d34b961a8ee8c3d13dae (diff) | |
download | PRE_107_064111-929067069100dbdeb78f3982fd3d1a5735183a3e.tar.gz PRE_107_064111-929067069100dbdeb78f3982fd3d1a5735183a3e.tar.bz2 PRE_107_064111-929067069100dbdeb78f3982fd3d1a5735183a3e.zip |
Tweaked equilibrium section.
-rw-r--r-- | frsb_kac_new.tex | 11 |
1 files changed, 8 insertions, 3 deletions
diff --git a/frsb_kac_new.tex b/frsb_kac_new.tex index 34ca3c9..514fda9 100644 --- a/frsb_kac_new.tex +++ b/frsb_kac_new.tex @@ -162,7 +162,7 @@ carefully treating the $k$th term in each sum separately from the rest, we get \right\} \end{aligned} \end{equation} -$F$ is a $k-1$ RSB ansatz with all eigenvalues scaled by $\tilde\beta z^{-1}$ and shifted by +This is a $k-1$ RSB ansatz with all eigenvalues scaled by $\tilde\beta z^{-1}$ and shifted by 1, with effective temperature $\tilde\beta$, and an extra term. This can be seen more clearly by rewriting the result in terms of the matrix $\tilde Q$, a $(k-1)$-RSB Parisi matrix built from the $\tilde x_1,\ldots,\tilde x_{k-1}$ and @@ -174,8 +174,13 @@ $q_1,\ldots,q_{k-1}$, which gives \right) \end{equation} {\em We have lost one level of RSB because at zero temperature the states become points.} - -{\bf Jaron: should'nt we put here the continuum solution?} +In the continuum case, this is +\begin{equation} \label{eq:ground.state.free.energy} + \lim_{\beta\to\infty}\tilde\beta F + =-\frac12z\tilde\beta f'(1)-\frac12\int dq\left( + \tilde\beta^2f''(q)\tilde\chi(q)+\frac1{\tilde\chi(q)+\tilde\beta z^{-1}} + \right) +\end{equation} |