From 034be30931cea7a5870e33b925de49e19dd6d92a Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Wed, 9 Dec 2020 17:41:30 +0100
Subject: Updated reference.

---
 bezout.tex | 4 ++--
 1 file changed, 2 insertions(+), 2 deletions(-)

(limited to 'bezout.tex')

diff --git a/bezout.tex b/bezout.tex
index 21d8146..4202e9b 100644
--- a/bezout.tex
+++ b/bezout.tex
@@ -69,7 +69,7 @@ complex variables, and the roots are simple all the way (we shall confirm this),
 variables minima of functions appear and disappear, and this procedure is not possible. The same idea may be implemented by 
 performing diffusion in the $J$'s, and following the roots, in complete analogy with Dyson's stochastic dynamics.
 
-This study also provides a complement to the work on the distribution of zeroes of random polynomials \cite{bogomolny1992distribution}.
+This study also provides a complement to the work on the distribution of zeroes of random polynomials \cite{Bogomolny_1992_Distribution}.
 
 
 Let us go back to our model.
@@ -319,7 +319,7 @@ The number of critical points contained within is
   =(p-1)^{N/2},
 \end{equation}
 the square root of \eqref{eq:bezout} and precisely the number of critical
-points of the real pure spherical $p$-spin model. (note the role of conjugation symmetry, already underlined in Ref\cite{bogomolny1992distribution}). In fact, the full
+points of the real pure spherical $p$-spin model. (note the role of conjugation symmetry, already underlined in Ref\cite{Bogomolny_1992_Distribution}). In fact, the full
 $\epsilon$-dependence of the real pure spherical $p$-spin is recovered by this
 limit as $\epsilon$ is varied.
 
-- 
cgit v1.2.3-54-g00ecf

