From c3c4d44881d1fc80b1d7cb18406a78d172bf19c7 Mon Sep 17 00:00:00 2001 From: "kurchan.jorge" Date: Wed, 9 Dec 2020 12:22:49 +0000 Subject: Update on Overleaf. --- bezout.tex | 5 ++++- 1 file changed, 4 insertions(+), 1 deletion(-) diff --git a/bezout.tex b/bezout.tex index 7d1335e..0a6efcb 100644 --- a/bezout.tex +++ b/bezout.tex @@ -39,12 +39,15 @@ different topological properties. Spin-glasses have long been considered the paradigm of `complex landscapes' of many variables, a subject that includes Neural Networks and optimization problems, most notably Constraint Satisfaction ones. -The most tractable family of these are the mean-field spherical p-spin models defined by the energy: +The most tractable family of these are the mean-field spherical p-spin models + +defined by the energy: \begin{equation} \label{eq:bare.hamiltonian} H_0 = \sum_p \frac{c_p}{p!}\sum_{i_1\cdots i_p}^NJ_{i_1\cdots i_p}z_{i_1}\cdots z_{i_p}, \end{equation} where the $J_{i_1\cdots i_p}$ are real Gaussian variables and the $z_i$ are real and constrained to a sphere $\sum_i z_i^2=N$. If there is a single term of a given $p$, this is known as the `pure $p$-spin' model, the case we shall study here. +Also in the algebra \cite{cartwright2013number} and probability literature \cite{auffinger2013complexity,auffinger2013random} This problem has been attacked from several angles: the replica trick to compute the Boltzmann--Gibbs distribution, a Kac--Rice \cite{Kac_1943_On, -- cgit v1.2.3-54-g00ecf