summaryrefslogtreecommitdiff
diff options
context:
space:
mode:
authorJaron Kent-Dobias <jaron@kent-dobias.com>2020-12-14 14:51:39 +0100
committerJaron Kent-Dobias <jaron@kent-dobias.com>2020-12-14 14:51:39 +0100
commit54273f814e454770f11a44f6b7ca97a3dcceb66a (patch)
treeac84ec6a27da51730956347a9a2e5e7ff274011a
parent574c5495fbc22ea52927b77b1a1b2b60f2189f85 (diff)
downloadPRR_3_023064-54273f814e454770f11a44f6b7ca97a3dcceb66a.tar.gz
PRR_3_023064-54273f814e454770f11a44f6b7ca97a3dcceb66a.tar.bz2
PRR_3_023064-54273f814e454770f11a44f6b7ca97a3dcceb66a.zip
Slightly more honest.
-rw-r--r--bezout.tex4
1 files changed, 2 insertions, 2 deletions
diff --git a/bezout.tex b/bezout.tex
index fd48abb..2095b7f 100644
--- a/bezout.tex
+++ b/bezout.tex
@@ -202,8 +202,8 @@ where the argument of the exponential is
\right\}.
\end{equation}
The integral of the distribution $\rho$ of eigenvalues of $\partial\partial
- H$ comes from the Hessian and is dependant on $a$ alone. This function has a
- maximum in $\hat a$, $b$, $\hat c$, and $d$ at which its value is
+ H$ comes from the Hessian and is dependant on $a$ alone. This function has an
+ extremum in $\hat a$, $b$, $\hat c$, and $d$ at which its value is
\begin{equation} \label{eq:free.energy.a}
f(a)=1+\frac12\log\left(\frac4{p^2}\frac{a^2-1}{a^{2(p-1)}-|\kappa|^2}\right)+\int d\lambda\,\rho(\lambda)\log|\lambda|^2
-2C_+[\operatorname{Re}(\epsilon e^{-i\theta})]^2-2C_-[\operatorname{Im}(\epsilon e^{-i\theta})]^2,