OAI/NumberTheory/Ostmann/Tree/PairSquareMoment.lean
7 declarations, 0 contain sorry, 0 declared as axioms
Square-coordinate estimates for one moving bottom pair
- def
OAI.Ostmann.fieldPairCoefficientMomentline 14 - theorem
OAI.Ostmann.fieldPairCoefficientMoment_zeroline 18 - theorem
OAI.Ostmann.sum_fieldPairCoefficientMomentline 23 - theorem
OAI.Ostmann.mellinCoefficient_mul_constline 29 - theorem
OAI.Ostmann.fieldPair_scaled_square_coefficient_leline 40Source documentation
Multiplication by the difference can be absorbed into the fixed square coset; the zero difference is handled by the zero extension.
theorem fieldPair_scaled_square_coefficient_le {p : ℕ} [Fact p.Prime] (g : ZMod p → ℂ) (d : ZMod p) (K : (ZMod p)ˣ) (ρ : MulChar (ZMod p) ℂ) : ‖mellinCoefficient (fun r : (ZMod p)ˣ => fieldBottomPairValue g d ((K : ZMod p) * d * (r : ZMod p) ^ 2)) ρ‖ ^ 2 ≤ 2 * squareCharacterMass (fun χ => fieldPairCoefficientMoment g χ d) ρ := by …Mentions: OAI.Ostmann.mellinCoefficient, OAI.Ostmann.fieldBottomPairValue, OAI.Ostmann.squareCharacterMass, OAI.Ostmann.fieldPairCoefficientMoment
- theorem
OAI.Ostmann.fieldPair_scaled_square_mean_leline 56 - theorem
OAI.Ostmann.samePair_fixed_arguments_leline 73Source documentation
First average the held pair's split, while the two pair differences remain fixed. This costs two square fibers and the moving-pair coefficient.
theorem samePair_fixed_arguments_le {p : ℕ} [Fact p.Prime] (g h : ZMod p → ℂ) (d e : ZMod p) (K L : (ZMod p)ˣ) (ρ : MulChar (ZMod p) ℂ) : (Fintype.card (ZMod p)ˣ : ℝ)⁻¹ * (∑ b : (ZMod p)ˣ, ‖mellinCoefficient (fun r : (ZMod p)ˣ => fieldBottomPairValue g d ((K : ZMod p) * d * (r : ZMod p) ^ 2) * fieldBottomPairValue h e ((L : ZMod p) * e * (b : ZMod p) ^ 2)) ρ‖ ^ 2) ≤ 4 * squareCharacterMass (fun χ => fieldPairCoefficientMoment g χ d) ρ * fieldPairMoment h e := by …Mentions: OAI.Ostmann.mellinCoefficient, OAI.Ostmann.fieldBottomPairValue, OAI.Ostmann.squareCharacterMass, OAI.Ostmann.fieldPairCoefficientMoment, OAI.Ostmann.fieldPairMoment