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authorJaron Kent-Dobias <jaron@kent-dobias.com>2025-02-07 20:35:20 -0300
committerJaron Kent-Dobias <jaron@kent-dobias.com>2025-02-07 20:35:20 -0300
commit29b1b91c174103c1f6536ec4db72cbaef67f0576 (patch)
tree0d5436bfab3149c6c11cc207dd8a49dbace67835
parentd017d9982e121258b86d435a00eda55138a0e16b (diff)
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Fixed typo in relationship between V₀ and E.
The role of N in the relationship was inverted at the beginning of section 3.
-rw-r--r--topology.tex6
1 files changed, 3 insertions, 3 deletions
diff --git a/topology.tex b/topology.tex
index 965df01..9000b12 100644
--- a/topology.tex
+++ b/topology.tex
@@ -632,9 +632,9 @@ into the structure of solutions in this regime is merited.
\label{sec:ssg}
When $M=1$ the solution manifold corresponds to the energy
-level set of a spherical spin glass with energy density $E=\sqrt NV_0$. All the
+level set of a spherical spin glass with energy density $E=V_0/\sqrt N$. All the
results from the previous sections follow, and can be translated to the spin
-glasses by taking the limit $\alpha\to0$ while keeping $E=V_0\alpha^{-1/2}$ fixed. With a little algebra this procedure yields
+glasses by taking the limit $\alpha\to0$ while keeping $E=V_0\alpha^{1/2}$ fixed. With a little algebra this procedure yields
\begin{align}
E_\text{on}=\pm\sqrt{2f(1)}
&&
@@ -642,7 +642,7 @@ glasses by taking the limit $\alpha\to0$ while keeping $E=V_0\alpha^{-1/2}$ fixe
\label{eq:ssg.energies}
\end{align}
for the onset and shattering energies. The same limit taken for
-$V_\text{\textsc{sat}}\alpha^{-1/2}$ coincides with the ground state energy
+$V_\text{\textsc{sat}}\alpha^{1/2}$ coincides with the ground state energy
$E_\text{gs}$. In fact, for all energies below the threshold energy
$E_\text{th}$ (where minima become more numerous than saddle points in the
spin glass energy function) the logarithm of the average Euler characteristic