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| author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2021-03-09 16:09:55 +0100 |
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| committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2021-03-09 16:09:55 +0100 |
| commit | 823e1cb5e7ab98f7ebda8b8517e427241ec427ce (patch) | |
| tree | 0fe4eb6ae4fdb669d6376145fd512a45a5457583 | |
| parent | 55409dc28d44271a915e9197a423531a06a17d4a (diff) | |
| download | PRR_3_023064-823e1cb5e7ab98f7ebda8b8517e427241ec427ce.tar.gz PRR_3_023064-823e1cb5e7ab98f7ebda8b8517e427241ec427ce.tar.bz2 PRR_3_023064-823e1cb5e7ab98f7ebda8b8517e427241ec427ce.zip | |
Spelling mistake.
| -rw-r--r-- | bezout.tex | 2 |
1 files changed, 1 insertions, 1 deletions
@@ -103,7 +103,7 @@ a \emph{hyperbolic} constraint---by comparison with $|z|^2=N$. The reasoning is twofold. First, at every point $z$ the energy \eqref{eq:bare.hamiltonian} has a `radial' gradient of magnitude proportional to the energy, since $z\cdot\partial H_0=pH_0$. This anomalous direction must be neglected if critical -points are to exist a any nonzero energy, and the constraint surface $z^2=N$ is +points are to exist at any nonzero energy, and the constraint surface $z^2=N$ is the unique surface whose normal is parallel to $z$ and which contains the configuration space of the real $p$-spin model as a subspace. Second, taking the constraint to be the level set of a holomorphic function means the |