MTT interpolation at positive conductor from disk moments
ProvedMTT.interpolation_positive_conductor_of_momentsmodular-formsnumber-theoryp-adic-l-functions
Let be prime, let and , and let be a normalized algebraic cuspidal Hecke eigenform of level and weight . Fix compatible complex and -adic embeddings, a period system , an ordinary root , and two signed bounded measures and on . Assume each signed measure realizes the prescribed critical polynomial moment on every positive-depth residue disk.
For every positive integer , every primitive algebraic Dirichlet character modulo , and every , there are a continuous function and an algebraic number such that
and
where is the MTT Euler multiplier. This isolates the positive-conductor part of the interpolation argument, obtained by summing the disk-moment identities against and selecting the sign prescribed by parity.
Preamble
import Definitions.Def_MTT_Measures set_option autoImplicit false noncomputable section open scoped BigOperators
Formal statement
open MTT in
theorem MTT.interpolation_positive_conductor_of_moments
{p N k : ℕ} [Fact p.Prime] (hN : 0 < N) (hk : 2 ≤ k)
(ι : Qbar →+* ℂ) (ιp : Qbar →+* ℂ_[p]) (f : Eigenform N k ι)
(P : Periods k ι f.form) (α : ℂ_[p]) (hα : IsOrdinaryRoot f ιp α)
(μ : Bool → UnitMeasure p)
(hμ : ∀ s, RealizesMoments f ιp P α s (μ s))
(n : ℕ) (hn : 0 < n) (χ : DirichletCharacter Qbar (p ^ n))
(hχ : χ.IsPrimitive) (j : ℕ) (hj : j ≤ k - 2) :
∃ (g : C((ℤ_[p])ˣ, ℂ_[p])) (v : Qbar),
(∀ x, g x = specialFunction ιp n χ j x) ∧
ι v = normalizedCriticalValue f P.omega n χ j ∧
(μ true + μ false) g = eulerMultiplier f ιp α n χ j * ιp v := by sorrySource
Mazur–Tate–Teitelbaum, On p-adic analogues of the conjectures of Birch and Swinnerton-Dyer, Invent. Math. 84 (1986), https://doi.org/10.1007/BF01388731; Chapter I, §14 Proposition, pp. 20–21, positive-conductor case, using (8.6) and (10.2).