OAI/Analysis/LipschitzHilbert/Phase/ImprovedFourthMoment.lean
7 declarations, 0 contain sorry, 0 declared as axioms
The improved fourth moment: assembly of the quantitative gap and the dominant-coefficient alternative from §7.
- def
OAI.LipschitzHilbert.PhaseCombinatorics.phaseParameterline 20 - def
OAI.LipschitzHilbert.PhaseCombinatorics.fourthExponentline 22 - theorem
OAI.LipschitzHilbert.PhaseCombinatorics.nondominant_fourth_moment_boundline 24 - theorem
OAI.LipschitzHilbert.PhaseCombinatorics.mass_cube_le_two_sequenceNorm_fourthline 51 - theorem
OAI.LipschitzHilbert.PhaseCombinatorics.small_remainder_fourth_moment_boundline 69 - theorem
OAI.LipschitzHilbert.PhaseCombinatorics.finite_fourth_moment_gainline 96Source documentation
The constant-one fourth-moment estimate with the improved coefficient exponent, for arbitrary complex coefficients. This is the
p = 4endpoint of the manuscript's finite Fourier gain proposition.theorem finite_fourth_moment_gain (ν : Measure ℝ) [IsProbabilityMeasure ν] (frequency : ι → ℝ) (a : ι → ℂ) {gap D : ℝ} (hgap : 0 < gap) (hsep : Separated frequency gap) (hν : FourierGap ν gap) (hD : 1 ≤ D) (hcard : (Fintype.card ι : ℝ) ≤ D) : (∫ t, ‖finiteFourierSum frequency a t‖ ^ 4 ∂ν) ≤ (∑ i, ‖a i‖ ^ fourthExponent D) ^ (4 / fourthExponent D) := by …Mentions: OAI.LipschitzHilbert.PhaseCombinatorics.Separated, OAI.LipschitzHilbert.PhaseCombinatorics.FourierGap, OAI.LipschitzHilbert.PhaseCombinatorics.finiteFourierSum, OAI.LipschitzHilbert.PhaseCombinatorics.fourthExponent
- theorem
OAI.LipschitzHilbert.PhaseCombinatorics.finite_fourier_l4_gainline 131