OAI/NumberTheory/Ostmann/Construction/MaskedPhaseGiantMean.lean
5 declarations, 0 contain sorry, 0 declared as axioms
The favorable-prime mask in the initial giant
Nonfavorable primes remain in the prior. Their physical test is exactly zero.
- theorem
OAI.Ostmann.phaseGiantPhysical_zeroline 13 - def
OAI.Ostmann.favorablePhaseTransformline 17 - theorem
OAI.Ostmann.favorablePhaseTransform_realline 22 - theorem
OAI.Ostmann.favorablePhase_uniform_mean_lowerline 34Source documentation
The favorable Fourier L1 mass gives a positive uniform-support mean, while the other primes make zero contribution.
theorem favorablePhase_uniform_mean_lower {I : Type*} [Fintype I] (p : I → ℕ) [∀ i, Fact (p i).Prime] (S : ∀ i, Finset (ZMod (p i))) (F : Finset I) (w : I → ℝ) (hw : ∀ i, 0 ≤ w i) (γ : ℝ) (hS : ∀ i ∈ F, (S i).Nonempty) (hSp : ∀ i ∈ F, (S i).card < p i) (hσ : ∀ i ∈ F, residueDensity (S i) ≤ 2 / 3) (hγ : ∀ i ∈ F, γ ≤ (p i : ℝ)⁻¹ * ∑ b, ‖normalizedResidueTransform (S i) b‖) : (γ / 2) * (∑ i ∈ F, w i) ≤ ∑ i, w i * (((S i).card : ℝ)⁻¹ * ∑ x ∈ S i, (phaseGiantPhysical (favorablePhaseTransform p S F i) x).re) := by …Mentions: OAI.Ostmann.residueDensity, OAI.Ostmann.normalizedResidueTransform, OAI.Ostmann.phaseGiantPhysical, OAI.Ostmann.favorablePhaseTransform
- theorem
OAI.Ostmann.favorablePhase_empirical_mean_lowerline 59Source documentation
The initial empirical mean, with the genuine Fourier phase mask, pays only the square-root collision loss from Section 7.1.
theorem favorablePhase_empirical_mean_lower {I : Type*} [Fintype I] (p : I → ℕ) [∀ i, Fact (p i).Prime] (S : ∀ i, Finset (ZMod (p i))) (F : Finset I) (μ : ∀ i, ZMod (p i) → ℝ) (w : I → ℝ) (hw : ∀ i, 0 ≤ w i) (γ B : ℝ) (hS : ∀ i ∈ F, (S i).Nonempty) (hSp : ∀ i ∈ F, (S i).card < p i) (hσ : ∀ i ∈ F, residueDensity (S i) ≤ 2 / 3) (hγ : ∀ i ∈ F, γ ≤ (p i : ℝ)⁻¹ * ∑ b, ‖normalizedResidueTransform (S i) b‖) (hbudget : (∑ i, w i * ((p i : ℝ) * ∑ x ∈ S i, (μ i x - 1 / ((S i).card : ℝ)) ^ 2)) ≤ B) : (γ / 2) * (∑ i ∈ F, w i) - Real.sqrt (∑ i, w i) * Real.sqrt B ≤ ∑ i, w i * ∑ x ∈ S i, μ i x * (phaseGiantPhysical (favorablePhaseTransform p S F i) x).re := by …Mentions: OAI.Ostmann.residueDensity, OAI.Ostmann.normalizedResidueTransform, OAI.Ostmann.phaseGiantPhysical, OAI.Ostmann.favorablePhaseTransform