OAI/NumberTheory/CubicMoment/Estimates/NoncubeExponents.lean
9 declarations, 0 contain sorry, 0 declared as axioms
Strict exponent gaps away from the two exceptional conductor shapes. These are the normalized exponents of the two cubic-sieve bounds and of the ordinary character large sieve, respectively.
- def
OAI.CubicFirstMoment.pSieveExponentline 13 - def
OAI.CubicFirstMoment.qSieveExponentline 16 - def
OAI.CubicFirstMoment.ordinarySieveExponentline 19 - def
OAI.CubicFirstMoment.noncubeSieveExponentline 22 - lemma
OAI.CubicFirstMoment.pSieveExponent_negline 25 - lemma
OAI.CubicFirstMoment.qSieveExponent_negline 38 - lemma
OAI.CubicFirstMoment.ordinarySieveExponent_diag_negline 43 - theorem
OAI.CubicFirstMoment.noncubeSieveExponent_negline 50Source documentation
The only nonnegative-gap possibilities in the large-conductor region are precisely the two shapes treated by the structured moment argument.
theorem noncubeSieveExponent_neg {p q : ℝ} (hp : 0 ≤ p) (hq : 0 ≤ q) (hsize : p+2*q ≤ 1) (hlarge : 0 < p+2*q) (hfirst : p ≠ 1 ∨ q ≠ 0) (hbalanced : p ≠ 1/3 ∨ q ≠ 1/3) : noncubeSieveExponent p q < 0 := by … - lemma
OAI.CubicFirstMoment.continuous_noncubeSieveExponentline 65