From eabaacdec785dd3d02c9147d2b635d6e1564a28d Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Fri, 10 Jun 2022 11:39:36 +0200
Subject: Killed extra space.

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

(limited to 'frsb_kac_new.tex')

diff --git a/frsb_kac_new.tex b/frsb_kac_new.tex
index 4d938da..44fce5b 100644
--- a/frsb_kac_new.tex
+++ b/frsb_kac_new.tex
@@ -376,7 +376,7 @@ We shall make the following ansatz for the saddle point:
   D_{ab}= D_d \delta_{ab}
 \end{align}
 From what we have seen above, this means that replica $a$ is insensitive to
-a small field applied to replica $b$ if $a \neq b$, a property related to ultrametricity. A similar situation happens in quantum replicated systems, 
+a small field applied to replica $b$ if $a \neq b$, a property related to ultrametricity. A similar situation happens in quantum replicated systems,
 with time appearing only on the diagonal terms: see Appendix C for details.
 
 From its very definition, it is easy to see just perturbing the equations
-- 
cgit v1.2.3-70-g09d2

