Random Field Ising Model — Imry-Ma
Quenched random magnetic fields compete with ferromagnetic coupling. Imry-Ma argument: in d≤2, arbitrarily weak random fields destroy long-range order by domain formation.
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Random Field Ising Model: H = −J Σ⟨ij⟩ sᵢsⱼ − Σᵢ hᵢsᵢ where hᵢ ~ N(0,h²). Imry-Ma (1975): domain wall energy ∝ R^(d-1), random field energy gain ∝ h R^(d/2). Balance gives optimal domain size R* ∝ (J/h)^(2/(4-d)) (d<4).