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authorJaron Kent-Dobias <jaron@kent-dobias.com>2020-12-07 15:10:36 +0100
committerJaron Kent-Dobias <jaron@kent-dobias.com>2020-12-07 15:10:36 +0100
commitadef14da06a25d47befb5bf64f8fc1883665d08c (patch)
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parentebd7dd5bfbada4a66f18e27a18ae1fddb2daf0bc (diff)
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Slightly nicer notation.
-rw-r--r--bezout.tex2
1 files changed, 1 insertions, 1 deletions
diff --git a/bezout.tex b/bezout.tex
index 897e79d..7d1378a 100644
--- a/bezout.tex
+++ b/bezout.tex
@@ -44,7 +44,7 @@ At any critical point $\epsilon=H/N$, the average energy.
When compared with $z^*z=N$, the constraint $z^2=N$ may seem an unnatural
extension of the real $p$-spin spherical model. However, a model with this
nonholomorphic spherical constraint has a disturbing lack of critical points
-nearly everywhere, since $0=\partial H/\partial z^*=-p\epsilon z$ is only
+nearly everywhere, since $0=\partial^* H=-p\epsilon z$ is only
satisfied for $\epsilon=0$, as $z=0$ is forbidden by the constraint.
Since $H$ is holomorphic, a point is a critical point of its real part if and