A geometrical picture for finite dimensional spin glasses
J. Houdayer, O. C. Martin

TL;DR
This paper proposes a geometric framework for understanding finite-dimensional spin glasses, suggesting a coexistence of droplet-like behavior at small scales and mean field characteristics at the system size, based on low energy sponge-like excitations.
Contribution
It introduces a geometric perspective that reconciles droplet models with mean field theory in finite-dimensional spin glasses through system-size excitations.
Findings
Existence of sponge-like low energy excitations at system size
Coexistence of droplet behavior and mean field features
System-size excitations can have constant energy without destroying the spin glass phase
Abstract
A controversial issue in spin glass theory is whether mean field correctly describes 3-dimensional spin glasses. If it does, how can replica symmetry breaking arise in terms of spin clusters in Euclidean space? Here we argue that there exist system-size low energy excitations that are sponge-like, generating multiple valleys separated by diverging energy barriers. The droplet model should be valid for length scales smaller than the size of the system (theta > 0), but nevertheless there can be system-size excitations of constant energy without destroying the spin glass phase. The picture we propose then combines droplet-like behavior at finite length scales with a potentially mean field behavior at the system-size scale.
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