OAI/NumberTheory/JointDickman/Analysis/MultiscaleMellinEnergy.lean
11 declarations, 0 contain sorry, 0 declared as axioms
The actual multiscale prime partition in the Mellin convention
The costs below are the proved Ramaré extraction and amplified cofactor costs. The integral over the class with no small prime polynomial remains explicit; no estimate for that exceptional class is assumed here.
- structure
OAI.JointDickman.MellinPrimeBandsline 18 - def
OAI.JointDickman.MellinPrimeBands.polynomialline 28 - structure
OAI.JointDickman.MellinPrimeBands.Validline 33 - def
OAI.JointDickman.MellinPrimeBands.extractionCostline 45 - def
OAI.JointDickman.MellinPrimeBands.initialCostline 50 - def
OAI.JointDickman.MellinPrimeBands.laterCostline 54 - lemma
OAI.JointDickman.MellinPrimeBands.angular_eq_dyadicline 63 - lemma
OAI.JointDickman.MellinPrimeBands.polynomial_continuousline 66 - theorem
OAI.JointDickman.MellinPrimeBands.firstSmallBand_energy_leline 69 - theorem
OAI.JointDickman.MellinPrimeBands.laterSmallBand_energy_leline 85 - theorem
OAI.JointDickman.MellinPrimeBands.partition_energy_leline 119Source documentation
Every nonexceptional class is bounded by its actual small-prime or amplified cofactor estimate. Only the no-small-band integral is left.
theorem partition_energy_le (D : MellinPrimeBands) {J N : ℕ} (hD : D.Valid J N) (hN : 0 < N) (f : ℕ → ℂ) (hf : Multiplicative f) (hb : OneBounded f) {T : ℝ} (hT : 0 < T) {S : Set ℝ} (hSm : MeasurableSet S) (hS : S ⊆ Set.Ioc (-T) T) : (∫ t in S, ‖angularMellinPolynomial (Ioc N (2*N)) (mrtTypicalCoefficient (range J) D.primes f) t‖^2) ≤ (∫ t in S ∩ mrtNoSmallBand D.bins (D.polynomial f) D.threshold J, ‖angularMellinPolynomial (Ioc N (2*N)) (mrtTypicalCoefficient (range J) D.primes f) t‖^2) + ∑ j ∈ range J, (D.extractionCost j N T + if j = 0 then D.initialCost N T else D.laterCost j N T) := by …Mentions: OAI.JointDickman.MellinPrimeBands, OAI.JointDickman.angularMellinPolynomial