Documentation

LeanPool.Feige.TwoPointBoundary

Removing strict positivity from the finite two-point bound #

noncomputable def Feige.boundaryEpsilon (n : ℕ) :

A positive perturbation parameter tending to zero.

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    noncomputable def Feige.strictGammaApprox {m : ℕ} (γ : Fin m → ℝ) (n : ℕ) (i : Fin m) :

    A strictly positive approximation to a nonnegative lower displacement.

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      theorem Feige.strictGammaApprox_pos {m : ℕ} {γ : Fin m → ℝ} (hγ : ∀ (i : Fin m), 0 ≤ γ i) (n : ℕ) (i : Fin m) :
      theorem Feige.strictGammaApprox_le_one {m : ℕ} {γ : Fin m → ℝ} (hγ1 : ∀ (i : Fin m), γ i ≤ 1) (n : ℕ) (i : Fin m) :
      theorem Feige.tendsto_twoPointHighProbability_strictGammaApprox {m : ℕ} (γ β : Fin m → ℝ) (hγ : ∀ (i : Fin m), 0 ≤ γ i) (hβ : ∀ (i : Fin m), 0 < β i) (i : Fin m) :
      theorem Feige.tendsto_highSetMass_strictGammaApprox {m : ℕ} (γ β : Fin m → ℝ) (hγ : ∀ (i : Fin m), 0 ≤ γ i) (hβ : ∀ (i : Fin m), 0 < β i) (S : Finset (Fin m)) :
      theorem Feige.eventually_rejectionFinset_subset_strictApprox {m : ℕ} (γ β : Fin m → ℝ) (α δ : ℝ) (hδ : 0 < δ) :
      ∀ᶠ (n : ℕ) in Filter.atTop, ∀ S ∈ {S : Finset (Fin m) | twoPointKFinset γ β S ≤ α}, twoPointKFinset (strictGammaApprox γ n) β S ≤ α + δ

      Every state rejected at the limiting parameter is, uniformly over the finite Boolean state space, eventually rejected at threshold α + δ by the strict approximants.

      theorem Feige.twoPointRejectionMass_le_add_delta {m : ℕ} (γ β : Fin m → ℝ) (hγ0 : ∀ (i : Fin m), 0 ≤ γ i) (hγ1 : ∀ (i : Fin m), γ i ≤ 1) (hβ : ∀ (i : Fin m), 0 < β i) {α δ : ℝ} (hα : 0 ≤ α) (hδ : 0 < δ) :
      twoPointRejectionMass γ β α ≤ α + δ
      theorem Feige.twoPointRejectionMass_le_alpha {m : ℕ} (γ β : Fin m → ℝ) (hγ0 : ∀ (i : Fin m), 0 ≤ γ i) (hγ1 : ∀ (i : Fin m), γ i ≤ 1) (hβ : ∀ (i : Fin m), 0 < β i) {α : ℝ} (hα : 0 ≤ α) :

      Closed-boundary two-point rejection estimate.

      The fully discharged finite two-point rejection hypothesis used by the conditional-mixture calibration theorem.