From 1eab2f16d7957745ba26ab051e91f0241f5ed79f Mon Sep 17 00:00:00 2001
From: Ian Jauslin <ian.jauslin@roma1.infn.it>
Date: Sun, 26 Jul 2015 19:56:08 +0000
Subject: Fix typos

---
 Jauslin_Como_2015.tex | 4 ++--
 1 file changed, 2 insertions(+), 2 deletions(-)

(limited to 'Jauslin_Como_2015.tex')

diff --git a/Jauslin_Como_2015.tex b/Jauslin_Como_2015.tex
index 89fe387..08c9e30 100644
--- a/Jauslin_Como_2015.tex
+++ b/Jauslin_Como_2015.tex
@@ -109,7 +109,7 @@ $$
 $$
 \lim_{\beta\to\infty}\chi^{(\lambda_0)}(0,\beta)=\infty.
 $$
-\item Anti-ferromagnetic interaction ($\lambda_0>0$):
+\item Anti-ferromagnetic interaction ($\lambda_0<0$):
 $$
 \lim_{\beta\to\infty}\chi^{(\lambda_0)}(0,\beta)<\infty.
 $$
@@ -137,7 +137,7 @@ $$
 \item Hierarchical Kondo model: idealization of the Kondo model that has the same scaling properties.
 \item It is {\it exactly solvable}: the map relating the effective theories at different scales is {\it explicit} (no perturbative expansions).
 \item With $\lambda_0<0$, the flow tends to a non-trivial fixed point, and $\chi^{(\lambda_0)}<\infty$ in the $\beta\to\infty$ limit (Kondo effect).
-\item{\tt Remark}: [Andrei, 1980]: the Kondo model (suitably linearized) is exactly solvable via Bethe Ansatz.
+\item{\tt Remark}: [N.~Andrei, 1980]: the Kondo model (suitably linearized) is exactly solvable via Bethe Ansatz.
 \end{itemize}
 \eject
 
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