From 68b444280c77b9f7863350b091836112d7482e6c Mon Sep 17 00:00:00 2001
From: "kurchan.jorge" <kurchan.jorge@gmail.com>
Date: Mon, 7 Dec 2020 15:01:09 +0000
Subject: Update on Overleaf.

---
 bezout.tex | 2 +-
 1 file changed, 1 insertion(+), 1 deletion(-)

(limited to 'bezout.tex')

diff --git a/bezout.tex b/bezout.tex
index 92d3e41..4ef9f1a 100644
--- a/bezout.tex
+++ b/bezout.tex
@@ -47,7 +47,7 @@ where the $J_{i_1\cdots i_p}$ are real Gaussian variables and the $z_i$ are real
 to a sphere $\sum_i z_i^2=N$.
 
 This problem has been attacked from several angles: the replica trick to compute the Boltzmann-Gibbs distribution,
-a Kac-Rice \cite{Kac,Fyodorov} procedure (similar to the Fadeev-Popov integral to compute the number of saddle-points of the energy function, and the gradient-descent -- or more generally Langevin -- dynamics staring from a high-energy configuration.
+a Kac-Rice \cite{Kac,Fyodorov} procedure (similar to the Fadeev-Popov integral)  to compute the number of saddle-points of the energy function, and the gradient-descent -- or more generally Langevin -- dynamics staring from a high-energy configuration.
 Thanks to the relative simplicity of the energy, all these approaches are possible analytically in the large $N$ limit.
 
 In th
-- 
cgit v1.2.3-54-g00ecf

