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Diffstat (limited to 'marginal.tex')
| -rw-r--r-- | marginal.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/marginal.tex b/marginal.tex index 1f1143c..30d3dce 100644 --- a/marginal.tex +++ b/marginal.tex @@ -1394,7 +1394,7 @@ Unlike in the spherical and multispherical spin glasses, the value $\mu^*$ defined in \eqref{eq:mu.star} giving the typical value of $\frac1N\operatorname{Tr}\partial\partial H$ is not always zero. Instead $\mu^*=-f'(0)$, nonzero where there is a linear term in $V$. Fixing the trace -of the Hessian is therefore equivalent to setting $\omega=\mu+f'(0)$. +of the Hessian is therefore equivalent to constraining the value of the Lagrange multiplier $\omega=\mu+f'(0)$. The derivation of the marginal complexity for this model is complicated, but |