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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2024-06-28 18:07:14 +0200 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2024-06-28 18:07:14 +0200 |
commit | d7ca4fca253e7e71ff19e48dbf9fe4cbef6efe60 (patch) | |
tree | fa6135892cac86d64398bd9a5b112f71db3a6867 | |
parent | 8e73e832988f02816bc1ca85b7a7b1f6a3a02cc0 (diff) | |
download | marginal-d7ca4fca253e7e71ff19e48dbf9fe4cbef6efe60.tar.gz marginal-d7ca4fca253e7e71ff19e48dbf9fe4cbef6efe60.tar.bz2 marginal-d7ca4fca253e7e71ff19e48dbf9fe4cbef6efe60.zip |
Small tweak.
-rw-r--r-- | marginal.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/marginal.tex b/marginal.tex index dd7bf68..b95872b 100644 --- a/marginal.tex +++ b/marginal.tex @@ -109,7 +109,7 @@ further looking for a sign that the zero eigenvalue lies at the edge of a continuous spectrum, we enforce the condition that the spectrum has a pseudogap, and is therefore marginal. We demonstrate the method on the spherical spin glasses, where it is unnecessary but instructive, and on extensions of -the spherical models with non-GOE Hessians where the technique is more useful. +the spherical models where the technique is more useful. In a companion paper, we compare the marginal complexity with the performance of gradient descent and approximate message passing algorithms \cite{Kent-Dobias_2024_Algorithm-independent}. |