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The critical point of the square-lattice Ising model

4 fully proved

A. The Onsager integrand

DefinitionOnsager integrand of the square-lattice Ising model#✓fully proved

The Onsager integrand cosh² 2β - sinh 2β (cos k₁ + cos k₂) at inverse temperature β and momentum (k₁, k₂).

noncomputable def ons_gInt (β k₁ k₂ : ℝ) : ℝ :=
  Real.cosh (2*β)^2 - Real.sinh (2*β) * (Real.cos k₁ + Real.cos k₂)
Used by 4

DefinitionCritical inverse temperature ½ log(1 + √2) of the square lattice#✓fully proved

The critical inverse temperature β_c = ½ log (1 + √2) of the square-lattice Ising model with unit couplings.

noncomputable def ons_betaC : ℝ := (1/2) * Real.log (1 + Real.sqrt 2)
Used by 7

B. The critical inverse temperature

TheoremKramers-Wannier critical point#✓fully proved

sinh 2β_c = 1 (H. A. Kramers and G. H. Wannier, Statistics of the two-dimensional ferromagnet. Part I, 1941).

theorem ons_betaC_sinh : Real.sinh (2 * ons_betaC) = 1
Uses 1 · Used by 5

Lemmaβ_c is the unique positive solution of sinh 2β = 1#✓fully proved

β_c is the unique positive inverse temperature with sinh 2β = 1, the self-dual point of the Kramers-Wannier duality.

lemma ons_betaC_unique (β : ℝ) (_hβ : 0 < β) :
    Real.sinh (2*β) = 1 ↔ β = ons_betaC
Uses 2 · Used by 3

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