From 5a903b3dca614142434a51054157e1f6642a63ae Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Thu, 18 Mar 2021 21:49:13 +0100
Subject: Missing word added.

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

(limited to 'bezout.tex')

diff --git a/bezout.tex b/bezout.tex
index 4b3bd19..902818c 100644
--- a/bezout.tex
+++ b/bezout.tex
@@ -101,7 +101,7 @@ One might balk at the constraint $z^Tz=N$---which could appropriately be called
 a \emph{hyperbolic} constraint---by comparison with $z^\dagger z=N$. The reasoning
 behind the choice is twofold.
 
-First, we seek draw conclusions from our model that are applicable to generic
+First, we seek to draw conclusions from our model that are applicable to generic
 holomorphic functions without any symmetry. Samples of $H_0$ nearly provide
 this, save for a single anomaly: the value of the energy and its gradient at
 any point $z$ correlate along the $z$ direction, with $\overline{H_0\partial
-- 
cgit v1.2.3-54-g00ecf

