OAI/Probability/InvariantIsing/Magnetic/RestrictedFieldPublishedInput.lean
4 declarations, 0 contain sorry, 0 declared as axioms
Panchenko--Talagrand (2007), Lemma 3.1 (8), p.655 and Corollary 3.2 (9), p.656, specialized to the actual finite constrained terminal. The hypothesis concerns only the marked endpoint law; no pressure, spin expectation, or limiting assertion is an input.
- def
OAI.InvariantIsing.restrictedFieldTiltedPairMeanline 17 - def
OAI.InvariantIsing.RestrictedFieldAncestorPairLawline 27 - def
OAI.InvariantIsing.PanchenkoTalagrandRestrictedFieldPairInputline 43Source documentation
The same published marking theorem, with a nonempty finite spin constraint retained inside the terminal log partition.
def PanchenkoTalagrandRestrictedFieldPairInput : Prop := …
- theorem
OAI.InvariantIsing.restrictedFieldFinitePath_exp_integrableline 49Source documentation
The constrained terminal satisfies the published exponential-moment condition on every finite Gaussian path, also for zero variances.
theorem restrictedFieldFinitePath_exp_integrable {N : ℕ} (hN : 0 < N) (S : Finset (Spin N)) (hS : S.Nonempty) (n : ℕ) (v : ℕ → ℝ≥0) (z : Fin N → ℝ) : Integrable (fun w : Fin n → Fin N → ℝ => Real.exp (restrictedFieldTerminal S (z + ∑ i, w i))) (Measure.pi (fun i : Fin n => (vectorGaussianLaw N (v i) : Measure (Fin N → ℝ)))) := by …Mentions: OAI.InvariantIsing.Spin, OAI.InvariantIsing.restrictedFieldTerminal, OAI.InvariantIsing.vectorGaussianLaw