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The Potts critical temperature and the FK critical parameter

6 fully proved

A. The FK parametrization

DefinitionPotts inverse temperature of an FK edge parameter#✓fully proved

The Potts inverse temperature -((q - 1)/q) log (1 - p) corresponding to the FK edge parameter p.

noncomputable def pToBeta (q p : ℝ) : ℝ := -((q - 1) / q) * Real.log (1 - p)
Used by 4

DefinitionFK edge parameter of a Potts inverse temperature#✓fully proved

The FK edge parameter 1 - e^{-qβ/(q-1)} of the q-state Potts model at inverse temperature β.

noncomputable def betaToP (q β : ℝ) : ℝ := 1 - Real.exp (-(q / (q - 1)) * β)
Used by 1

LemmaInverse-temperature map of the Potts model at \(q = 2\) is the Ising map#✓fully proved

At q = 2 the general parametrization pToBeta is betaOfP.

lemma pToBeta_two_eq_betaOfP (p : ℝ) : pToBeta 2 p = betaOfP p
Uses 2

LemmaFK edge-parameter map of the Potts model at \(q = 2\) is the Ising map#✓fully proved

At q = 2 the general parametrization betaToP is pOfBeta.

lemma betaToP_two_eq_pOfBeta (β : ℝ) : betaToP 2 β = pOfBeta β
Uses 2

B. Critical inverse temperatures

DefinitionCritical inverse temperature of a magnetization curve#✓fully proved

The critical inverse temperature sup {β > 0 : m*(β) = 0} of a spontaneous-magnetization curve m*. See also Ising.betaC, the infimum of the inverse temperatures with positive magnetization.

noncomputable def betaC (mStar : ℝ → ℝ) : ℝ :=
  sSup {β : ℝ | 0 < β ∧ mStar β = 0}
Used by 4

DefinitionCritical inverse temperature of the \(d\)-dimensional Ising model#✓fully proved

The critical inverse temperature of the d-dimensional Ising model, sup {β > 0 : m*(β) = 0}.

noncomputable def isingBetaC (d : ℕ) : ℝ :=
  betaC (Ising.magnetization d)
Uses 2

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