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| author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2023-10-07 15:29:08 +0200 |
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| committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2023-10-07 15:29:08 +0200 |
| commit | ac27d79183ce80993bc332d6e09e0e12cb967fc3 (patch) | |
| tree | 308bea4755ee0d536335f270a26121e4d97c6e44 | |
| parent | f9a34f391dbae4e41d13b4ddde4bde6a8af8d93e (diff) | |
| download | marginal-ac27d79183ce80993bc332d6e09e0e12cb967fc3.tar.gz marginal-ac27d79183ce80993bc332d6e09e0e12cb967fc3.tar.bz2 marginal-ac27d79183ce80993bc332d6e09e0e12cb967fc3.zip | |
Some work.
| -rw-r--r-- | marginal.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/marginal.tex b/marginal.tex index 96c2a99..b840699 100644 --- a/marginal.tex +++ b/marginal.tex @@ -141,7 +141,7 @@ we expect no $b$-dependence of this matrix. $A^{aa}$ is the usual replica-symmetric overlap matrix of the spherical two-spin problem. $A^{ab}$ describes overlaps between eigenvectors at different stationary points and should be a constant $m_a\times m_b$ matrix. -We will discuss at the end of this paper when these order parameters can be expected to be nonzero, but in this problem all of the $X$s, $\hat X$s, and $A^{ab}$ for $a\neq b$ are zero. +We will discuss at the end of this paper when these order parameters can be expected to be nonzero, but in this and most isotropic problems all of the $X$s, $\hat X$s, and $A^{ab}$ for $a\neq b$ are zero. \begin{equation} \begin{aligned} |