High-temperature expansion of the Ising partition function
DefinitionZero-field Ising partition function with unit couplings#✓fully proved
The zero-field Ising partition function of G with unit couplings at inverse temperature β.
noncomputable def ons_Z (β : ℝ) : ℝ := isingZ G β 0
noncomputable def isingZ (β h : ℝ) : ℝ := ∑ s : ConfigSpace V, isingWeight G β h s
PhyslibExt/CondensedMatter/IsingModel/Gibbs.lean:126
Uses 1 · Used by 7
DefinitionEven-subgraph generating function of a graph#✓fully proved
The even-subgraph generating function ∑_F x^|F| of G, over edge sets F in which every
vertex has even degree.
noncomputable def ons_X (x : ℝ) : ℝ :=
∑ F ∈ G.edgeFinset.powerset.filter IsEvenSubgraph, x ^ F.card
def IsEvenSubgraph (F : Finset (Sym2 V)) : Prop := ∀ v : V, Even (incCount F v)
PhyslibExt/CondensedMatter/IsingModel/KWSelfDuality.lean:114
Uses 2 · Used by 7
TheoremHigh-temperature expansion#✓fully proved
High-temperature expansion (van der Waerden 1941). Z(β) = 2^|V| (cosh β)^|E| X(tanh β) for
the zero-field Ising model on a finite graph (B. L. van der Waerden, Die lange Reichweite der
regelmässigen Atomanordnung in Mischkristallen, 1941).
theorem ons_hte (β : ℝ) :
ons_Z G β
= (2 : ℝ) ^ Fintype.card V * (Real.cosh β) ^ G.edgeFinset.card
* ons_X G (Real.tanh β)
noncomputable def ons_Z (β : ℝ) : ℝ := isingZ G β 0
PhyslibExt/CondensedMatter/IsingModel/Onsager/HighTemp.lean:64
noncomputable def ons_X (x : ℝ) : ℝ :=
∑ F ∈ G.edgeFinset.powerset.filter IsEvenSubgraph, x ^ F.card
PhyslibExt/CondensedMatter/IsingModel/Onsager/HighTemp.lean:68
Uses 4 · Used by 5
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