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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2024-06-07 17:38:49 +0200 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2024-06-07 17:38:49 +0200 |
commit | d02197918d759195dd1d863de28f352f70cbf14c (patch) | |
tree | a717649a0dfba93722fb128603f6a6713d539107 /marginal.tex | |
parent | 56a93b963c9f47a865678a272e85fc6708c3ccb4 (diff) | |
download | marginal-d02197918d759195dd1d863de28f352f70cbf14c.tar.gz marginal-d02197918d759195dd1d863de28f352f70cbf14c.tar.bz2 marginal-d02197918d759195dd1d863de28f352f70cbf14c.zip |
Small caption tweak.
Diffstat (limited to 'marginal.tex')
-rw-r--r-- | marginal.tex | 4 |
1 files changed, 2 insertions, 2 deletions
diff --git a/marginal.tex b/marginal.tex index e2bd24f..246bcaf 100644 --- a/marginal.tex +++ b/marginal.tex @@ -307,8 +307,8 @@ pseudogap. and the calculation breaks down, leading to the imaginary part. For $\mu>2\sigma$ the spectrum can satisfy the constraint on the smallest eigenvalue by isolating a single eigenvalue at zero at the cost of an - order-$N$ large deviation. At $\mu=2\sigma$, the transition point, the - spectrum is pseudogapped or marginal. + order-$N$ large deviation. At the transition point $\mu=2\sigma$ the + spectrum is pseudogapped. } \label{fig:large.dev} \end{figure} |