OAI/Probability/InvariantIsing/Gaussian/GaussianBaseComparison.lean

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3 declarations, 0 contain sorry, 0 declared as axioms

Stability of the actual Gaussian partition under bounded base-energy changes.

  1. theorem OAI.InvariantIsing.countable_cylinder_log_mean_cost line 17

    Source documentation

    An independent Gaussian perturbation changes the mean pressure by at most half its maximal variance, including after a fixed base-energy tilt.

    theorem countable_cylinder_log_mean_cost {X : Type*} [MeasurableSpace X] [Countable X]
        [MeasurableSingletonClass X] (ν : Measure X) [IsProbabilityMeasure ν]
        (H : X → ℝ) (hH : Integrable (fun x => Real.exp (H x)) ν)
        (A : X → ℕ →₀ ℝ) {B : ℝ} (hA : ∀ x, (A x).sum (fun _ c => c ^ 2) ≤ B) :
        let d := (∫ g : ℕ → ℝ, Real.log (∫ x, Real.exp (H x + cylinderField (A x) g) ∂ν)
    …
  2. lemma OAI.InvariantIsing.cylinder_partition_exp_integrable_ae line 29
  3. theorem OAI.InvariantIsing.countable_cylinder_log_mean_base_compare line 48

    Source documentation

    A uniform deterministic energy change bounds the mean logpartition change, for every countable prior and bounded-variance Gaussian field.

    theorem countable_cylinder_log_mean_base_compare {X : Type*} [MeasurableSpace X] [Countable X]
        [MeasurableSingletonClass X] (ν : Measure X) [IsProbabilityMeasure ν]
        (H J : X → ℝ) (hH : Integrable (fun x => Real.exp (H x)) ν)
        (hJ : Integrable (fun x => Real.exp (J x)) ν)
        (A : X → ℕ →₀ ℝ) {B K : ℝ} (hA : ∀ x, (A x).sum (fun _ c => c ^ 2) ≤ B)
        (hK : ∀ x, |H x - J x| ≤ K) :
        |(∫ g : ℕ → ℝ, Real.log (∫ x, Real.exp (H x + cylinderField (A x) g) ∂ν)
            ∂gaussianCoordinates) -
          ∫ g : ℕ → ℝ, Real.log (∫ x, Real.exp (J x + cylinderField (A x) g) ∂ν)
            ∂gaussianCoordinates| ≤ K := by
    …