Math 2.0

Statistical mechanics, structure of matter Disordered systems Example

Edwards–Anderson model

Builds on Ising model

Example

Let d≥1d \ge 1 and L≥2L \ge 2 be integers, and let ΛL={1,…,L}d⊂ℤd\Lambda_L = \set{1, \dots, L}^d \subset \Z^d. Let ELE_L be the set of pairs {x,y}\set{x, y} of points of ΛL\Lambda_L at distance 11. Let (Jxy){x,y}∈EL(J_{xy})_{\set{x,y} \in E_L} be independent random variables with a common law that is symmetric about 00, for example standard Gaussian or uniform on {−1,+1}\set{-1, +1}. The Edwards–Anderson model is the random Hamiltonian HL(σ)=−∑{x,y}∈ELJxyσxσy,σ∈{−1,+1}ΛL,H_L(\sigma) = -\sum_{\set{x, y} \in E_L} J_{xy} \sigma_x \sigma_y, \qquad \sigma \in \set{-1, +1}^{\Lambda_L}, with the Gibbs measure proportional to e−βHL(σ)e^{-\beta H_L(\sigma)} for each sample of the couplings.

Check: the couplings are independent, and a symmetric law that is not concentrated at 00 gives both signs with positive probability. So the model is a spin glass, with couplings supported on the nearest-neighbour edges of ℤd\Z^d.

Remarks

It is the Ising model on ℤd\Z^d with each coupling replaced by an independent random sign or Gaussian. Frustration is present: around a unit square of ℤ2\Z^2, the product of the four couplings is negative with probability 1/21/2, and then no configuration satisfies all four bonds. Edwards and Anderson introduced the quantity q=lim⁡1∣ΛL∣∑x⟨σx⟩2q = \lim \frac{1}{\abs{\Lambda_L}} \sum_x \langle \sigma_x \rangle^2 as an order parameter for the frozen phase. The nature of the low-temperature phase in finite dimension is still not settled mathematically.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Spin_glass
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MSC82B44, 82D30, 82B20
Instance ofSpin glass
UsesIsing model
Changed3 November 2026

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