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authorJaron Kent-Dobias <jaron@kent-dobias.com>2022-06-07 08:14:30 +0200
committerJaron Kent-Dobias <jaron@kent-dobias.com>2022-06-07 08:14:30 +0200
commit698f74a6f5abf481d860540850b202f6e66e01f3 (patch)
tree936dc38170b2145b585a01e7a08703340d2c002e /frsb_kac_new.tex
parent5bf3914c90c6c7d89f36746138b036d3ec121a29 (diff)
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Tiny fix.
Diffstat (limited to 'frsb_kac_new.tex')
-rw-r--r--frsb_kac_new.tex4
1 files changed, 2 insertions, 2 deletions
diff --git a/frsb_kac_new.tex b/frsb_kac_new.tex
index 99455de..f5e9422 100644
--- a/frsb_kac_new.tex
+++ b/frsb_kac_new.tex
@@ -400,9 +400,9 @@ Consider the extremum problem of \eqref{eq:diagonal.action} with respect to $R_d
=-\frac12f'(1)+\frac12\frac1{R_d^2}\lim_{n\to0}\frac1n\operatorname{Tr}((D_d/R_d^2)Q+I)^{-1}Q \label{eq:saddle.d}\\
0
&=\frac{\partial S}{\partial R_d}
- =-\mu+\hat\epsilon f'(1)+R_df''(1)+\frac1{R_d}+\frac{D_d}{R_d}\lim_{n\to0}\frac1n\operatorname{Tr}((D_d/R_d^2)Q+I)^{-1}Q \label{eq:saddle.r}
+ =-\mu+\hat\epsilon f'(1)+R_df''(1)+\frac1{R_d}-\frac{D_d}{R_d^3}\lim_{n\to0}\frac1n\operatorname{Tr}((D_d/R_d^2)Q+I)^{-1}Q \label{eq:saddle.r}
\end{align}
-Adding $2(D_d/R_d)$ of \eqref{eq:saddle.d} to \eqref{eq:saddle.r} and multiplying by $R_d$ gives
+Adding $2(D_d/R_d)$ times \eqref{eq:saddle.d} to \eqref{eq:saddle.r} and multiplying by $R_d$ gives
\begin{equation}
0=-R_d\mu+1+R_d^2f''(1)+f'(1)(R_d\hat\epsilon-D_d)
\end{equation}