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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-06-07 08:14:30 +0200 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-06-07 08:14:30 +0200 |
commit | 698f74a6f5abf481d860540850b202f6e66e01f3 (patch) | |
tree | 936dc38170b2145b585a01e7a08703340d2c002e | |
parent | 5bf3914c90c6c7d89f36746138b036d3ec121a29 (diff) | |
download | PRE_107_064111-698f74a6f5abf481d860540850b202f6e66e01f3.tar.gz PRE_107_064111-698f74a6f5abf481d860540850b202f6e66e01f3.tar.bz2 PRE_107_064111-698f74a6f5abf481d860540850b202f6e66e01f3.zip |
Tiny fix.
-rw-r--r-- | frsb_kac_new.tex | 4 |
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} |