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Spin Glass


A spin glass is a spin model with disordered interactions, often with both positive and negative couplings. For binary spins on a graph, a typical energy is H(sigma)=-sum_({i,j})J_(ij)sigma_isigma_j, with random J_(ij). Conflicting interaction signs can prevent simultaneous minimization of every edge energy. Conditional on the disorder, the Gibbs measure is a probability law on spin configurations. Two independently sampled configurations from that conditional law are called replicas, and their overlap is

 R(sigma,tau)=1/Nsum_(i=1)^Nsigma_itau_i.

Overlap hierarchies enter variational descriptions of the limiting thermodynamic pressure. The Sherrington-Kirkpatrick model has interactions between every pair, whereas a diluted spin glass has a random number of interactions proportional to the number of spins. Orthogonally invariant spin glasses instead prescribe a limiting spectral law and random orthogonal eigenvectors.


See also

Diluted Spin Glass, Gibbs Measure, Orthogonally Invariant Spin Glass, Replica Symmetry Breaking, Sherrington-Kirkpatrick Model, Thermodynamic Pressure

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References

Fan, Z. and Wu, Y. "The Replica-Symmetric Free Energy for Ising Spin Glasses with Orthogonally Invariant Couplings." Probab. Th. Rel. Fields 190, 1-77, 2024. https://doi.org/10.1007/s00440-024-01309-w.Panchenko, D. "The Sherrington-Kirkpatrick Model: An Overview." J. Statist. Phys. 149, 362-383, 2012. https://doi.org/10.1007/s10955-012-0586-7.Panchenko, D. and Talagrand, M. "Bounds for Diluted Mean-Fields Spin Glass Models." Probab. Th. Rel. Fields 130, 319-336, 2004. https://doi.org/10.1007/s00440-004-0342-2.

Cite this as:

Weisstein, Eric W. "Spin Glass." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/SpinGlass.html

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