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| author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2024-10-25 16:11:21 +0200 |
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| committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2024-10-25 16:11:21 +0200 |
| commit | 157b8b12bdad4646773d1c596f99af6a1b4d9c9d (patch) | |
| tree | adfd6840a54694e5e43a266bcd34bf61f2d0acc8 | |
| parent | 6aad3c973dd44c6e21022e1193f5d6c623d4e23b (diff) | |
| download | marginal-157b8b12bdad4646773d1c596f99af6a1b4d9c9d.tar.gz marginal-157b8b12bdad4646773d1c596f99af6a1b4d9c9d.tar.bz2 marginal-157b8b12bdad4646773d1c596f99af6a1b4d9c9d.zip | |
Fixed grammatically bad sentence.
| -rw-r--r-- | marginal.tex | 4 |
1 files changed, 2 insertions, 2 deletions
diff --git a/marginal.tex b/marginal.tex index fac7c48..acd3d4a 100644 --- a/marginal.tex +++ b/marginal.tex @@ -1288,8 +1288,8 @@ $\epsilon$ is increased, the most common type of marginal minimum drifts toward points with $\omega_1>\omega_2$. Multispherical spin glasses may be an interesting platform for testing ideas -about which among the possible marginal minima can dynamics, -and cannot. In the limit where $\epsilon=0$ and the configurations of the +about which among the possible marginal minima can attract dynamics +and which cannot. In the limit where $\epsilon=0$ and the configurations of the two spheres are independent, the minima found dynamically should be marginal on both subspaces. Just because technically on the expanded configuration space the Cartesian product of a deep stable minimum on one sphere and a marginal minimum on the other is |