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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