From 1eab2f16d7957745ba26ab051e91f0241f5ed79f Mon Sep 17 00:00:00 2001 From: Ian Jauslin Date: Sun, 26 Jul 2015 19:56:08 +0000 Subject: Fix typos --- Jauslin_Como_2015.tex | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) 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 -- cgit v1.2.3-54-g00ecf