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Cooling-Rate Dependence for the Spin-Glass Ground-State Energy: Implications for Optimization by Simulated Annealing
120
Citations
21
References
1986
Year
EngineeringGlass-forming LiquidSpin SystemsMagnetic ResonanceSpin DynamicSpin PhenomenonSpin-glass ModelsGlass TransitionSimulated AnnealingNumerical SimulationQuantum MaterialsThermodynamicsMonte Carlo StepsMaterials ScienceQuantum SciencePhysicsZero-temperature Ground-state PropertiesSpin-glass Ground-state EnergySpintronicsCooling-rate DependenceApplied PhysicsCondensed Matter PhysicsCritical Phenomenon
The zero-temperature ground-state properties of five spin-glass models have been studied as a function of the cooling rate $r=\frac{\ensuremath{-}\ensuremath{\Delta}T}{t}$. Here $\ensuremath{\Delta}T$ is the temperature decrement and $t$ is the time (in Monte Carlo steps) at each temperature $T$. For the 2D $\ifmmode\pm\else\textpm\fi{}J$ and Gaussian models, $E(r)={E}_{0}+{C}_{1}{r}^{x}$, where $x\ensuremath{\cong}0.25$, while for the 3D $\ifmmode\pm\else\textpm\fi{}J$, a two-layer $\ifmmode\pm\else\textpm\fi{}J$, and infinite-range models, $E(r)={E}_{0}\ensuremath{-}{C}_{2}{(\mathrm{inr})}^{\ensuremath{-}1}$. We speculate that this difference is related to the fact that the 2D models are not $\mathrm{NP}$-complete while the other three models are.
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