The zero-temperature ground-state properties of five spin-glass models have been studied as a function of the cooling rate r=-ΔTt. Here ΔT is the temperature decrement and t is the time (in Monte Carlo steps) at each temperature T. For the 2D ±J and Gaussian models, E(r)=E₀+C₁rˣ, where x0.25, while for the 3D ±J, a two-layer ±J, and infinite-range models, E(r)=E₀-C₂(inr)^-1. We speculate that this difference is related to the fact that the 2D models are not NP-complete while the other three models are.
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Grest et al. (1986) studied this question.
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