Merge branch 'master' of https://git.overleaf.com/5fcce4736e7f601ffb7e1484

1 files changed, 2 insertions, 2 deletions

diff --git a/bezout.tex b/bezout.tex
index 5090de9..67d7602 100644
--- a/bezout.tex
+++ b/bezout.tex
@@ -336,7 +336,7 @@ values of $\kappa$ and $\epsilon$. Taking this saddle gives
   \log\overline{\mathcal N}(\kappa,\epsilon)
   =N\log(p-1).
 \end{equation}
-This is precisely the Bézout bound, the maximum number of solutions that $N$
+This is, to this order,  precisely the Bézout bound, the maximum number of solutions that $N$
 equations of degree $p-1$ may have \cite{Bezout_1779_Theorie}. More insight is
 gained by looking at the count as a function of $a$, defined by $\overline{\mathcal
 N}(\kappa,\epsilon,a)=e^{Nf(a)}$.  In the large-$N$ limit, this is the
@@ -364,7 +364,7 @@ Notice that the limit of this expression as $a\to\infty$ corresponds with
 several values of $\kappa$ in Fig.~\ref{fig:complexity}. For any $|\kappa|<1$,
 the complexity goes to negative infinity as $a\to1$, i.e., as the spins are
 restricted to the reals.  This is natural, given that the $y$ contribution to
-the volume shrinks to zero as that of an $N$-dimensional sphere with volume
+the volume shrinks to zero as that of an $N$-dimensional sphere $\sum_i y_i^2=N(a-1)$ with volume
 $\sim(a-1)^N$.  However, when the result is analytically continued to
 $\kappa=1$ (which corresponds to real $J$) something novel occurs: the
 complexity has a finite value at $a=1$. Since the $a$-dependence gives a