Searcharxiv⌕ Search

arXiv · 2611.08374

A Simple Approach to the Complexity of Mean Field Ising Spin Glasses

Abstract

The geometry of spherical spin glasses is relatively well understood, thanks in large part to the Kac-Rice formula. However, this formula does not directly apply to discrete spin systems, and much less is known mathematically about the geometry of Ising spin glasses. In this paper, we present a simple method for counting local optima and gapped states in a broad class of discrete spin glasses. To illustrate its scope, we compute the annealed complexities ("configurational entropies," in the physics language) of mixed Ising spin glasses with potentials, such as external fields, and of the Ghatak-Sherrington model. These computations recover several existing results in the mathematics and physics literature as special cases. We can also compute energy-constrained complexity, finding a critical energy threshold analogous to the spherical case, but for gapped states of pure Ising spin glasses. Finally, we use our method to establish a form of disorder persistence for gapped states, identifying a transition between $3$-spin and $4$-spin glasses.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Benjamin McKenna, Qiang Wu. 2026-11-05. A Simple Approach to the Complexity of Mean Field Ising Spin Glasses. https://arxiv.org/abs/2611.08374

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Line crossing problem for biased monotonic random walks in the plane

A $β$-biased monotonic random walk in the plane moves from $(x,y)$ to $(x+1,y)$ or $(x,y+1)$ with probabilities $1/(β+1)$ and $β/(β+1)$. We study $Φ_β(α,d)$, the probability that the walk started at the origin ever visits a lattice point strictly above the line $y=αx+d$, and $Ψ_β(α,d)$, the probability that it visits a lattice point \emph{on} the line after leaving the origin. For integer slopes $α=p$ we show $Φ_β(p,d)=ρ^{\lfloor d\rfloor+1}$, where $ρ$ is the smallest positive root of $y^{p+1}-(β+1)y+β=0$, give the Fuss--Catalan series for $ρ$, identify $ρ$ with the extinction probability of a Galton--Watson process, and compute the exact law and mean of the first crossing point. We prove that the return probability is $Ψ_β(p,0)=(p+1)(1-β/((β+1)ρ))$, which equals $(p+1)/(β+1)$ for $β\ge p$. For rational slopes $α=r/s$ we obtain $Φ_β$ in closed form from the $s$ large roots of the kernel $\tfracβ{β+1}z^{r+s}-z^r+\tfrac1{β+1}$, and $Ψ_β$ as a ratio of Green's functions. For arbitrary real $α$ we prove that the walk crosses every line $y=αx+d$ almost surely if and only if $β\geα$, and we establish the two-sided bound $e^{-θ(d+1)}\leΦ_β(α,d) β$.

math.PR↗

Commutation relations for two-sided radial SLE

We study the commutation relation for 2-radial SLE in the unit disc starting from two distinct boundary points. We follow the framework introduced by Dubédat~[12]. Under an additional requirement of the interchangeability of the two curves, we classify all locally commuting 2-radial SLE$_κ$ for $κ\in (0,8)$: it is either two-sided radial SLE$_κ$ with spiral of constant spiraling rate or chordal SLE$_κ$ weighted by a power of the conformal radius of its complement. Namely, for fixed $κ$ and starting points, we have exactly two one-parameter families of locally commuting 2-radial SLE curves. We also discuss the semiclassical limit of the commutation relation as $κ\to 0$. In particular, we show that the limit for the second family with an appropriately chosen power of the conformal radius is a chord that minimizes a modified chordal Loewner energy, which is unique only when the endpoints are not antipodal.

math.PR↗

Stochastic optimal transport for the Langevin dynamics and its zero-mass limit

We introduce a stochastic optimal transport for the Langevin dynamics with positive mass and study its zero--mass limit. The new aspect of this paper is that we only fix the initial and terminal probability distributions of the positions of particles under consideration, but not those of their velocities, with Heisenberg's uncertainty principle in mind. In the zero--mass limit, we show that the minimizers of our stochastic optimal transport is tight if and only if the initial momentum (=(mass)$\times$(velocity)) of a particle converges to zero. We also prove that the limit of minimizers of our stochastic optimal transport is a minimizer of a standard stochastic optimal transport for continuous semimartingales.

math.PR↗