From 2836844fa30357e6de86296fe82f13d1a886fdef Mon Sep 17 00:00:00 2001
From: "kurchan.jorge" <kurchan.jorge@gmail.com>
Date: Wed, 9 Dec 2020 13:08:01 +0000
Subject: Update on Overleaf.

---
 bezout.tex | 3 ++-
 1 file changed, 2 insertions(+), 1 deletion(-)

(limited to 'bezout.tex')

diff --git a/bezout.tex b/bezout.tex
index c5f91cc..5fc340a 100644
--- a/bezout.tex
+++ b/bezout.tex
@@ -330,7 +330,8 @@ Consider for example the ground-state energy for given $a$, that is, the energy
 
 {\color{teal} {\bf somewhere} In Figure \ref{desert} we show that for $\kappa<1$ there is always a range of values of $a$ close to one for which there are no solutions: this is natural, given that the $y$ contribution to the volume shrinks to zero as that of an $N$-dimensional sphere $\sim(a-1)^N$.
 For the case $K=1$ -- i.e. the analytic continuation of the usual real computation -- the situation
-is more interesting. In the range of  values of $\Re$
+is more interesting. In the range of  values of $\Re H_0$ where there are real solutions there are solutions
+all the way down to $a=1$: this is only possible if the density of solutions diverges at this value: this is natural, since. 
 
 
 \begin{figure}[htpb]\label{desert}
-- 
cgit v1.2.3-54-g00ecf