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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2020-12-07 15:10:36 +0100 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2020-12-07 15:10:36 +0100 |
commit | adef14da06a25d47befb5bf64f8fc1883665d08c (patch) | |
tree | b2da8c2dc6f48ae805ce26b1148656d268f678fb | |
parent | ebd7dd5bfbada4a66f18e27a18ae1fddb2daf0bc (diff) | |
download | PRR_3_023064-adef14da06a25d47befb5bf64f8fc1883665d08c.tar.gz PRR_3_023064-adef14da06a25d47befb5bf64f8fc1883665d08c.tar.bz2 PRR_3_023064-adef14da06a25d47befb5bf64f8fc1883665d08c.zip |
Slightly nicer notation.
-rw-r--r-- | bezout.tex | 2 |
1 files changed, 1 insertions, 1 deletions
@@ -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 |