Period pairing as Euclidean integrals over arbitrary coset tiles
ProvedMTT.Cohomology.periodPairing_eq_sum_tilesmeasure-theorymodular-formsperiods
Let with , and let be a finite set of representatives for the right cosets . Let agree on the upper half-plane with the determinant-contraction density
For the standard modular domain , the period pairing is
The left side uses hyperbolic measure and the fixed quotient representatives in the definition of the period pairing; the right side uses Euclidean area and the arbitrary representatives . The equality retains the same central multiplicity on both sides. This is the change-of-measure interface needed to apply Stokes' theorem to the MTT period pairing.
Preamble
import Definitions.Def_MTT_PeriodPairing import Mathlib.NumberTheory.ModularForms.Bounds import Mathlib.GroupTheory.Complement set_option autoImplicit false noncomputable section open UpperHalfPlane MeasureTheory open scoped MatrixGroups Modular ComplexConjugate open MTT.Cohomology
Formal statement
theorem MTT.Cohomology.periodPairing_eq_sum_tiles {N k : ℕ} (hk : 2 ≤ k)
(f q : CuspForm (MTT.GammaOne N) (k : ℤ))
(R : Finset SL(2, ℤ))
(hR : Subgroup.IsComplement (CongruenceSubgroup.Gamma1 N : Set SL(2, ℤ))
(R : Set SL(2, ℤ)))
(D : ℂ → ℂ)
(hD : ∀ z : ℍ, D z = periodContraction (k - 2)
(f z • periodPower (k - 2) z)
(conj (q z) • periodPower (k - 2) (conj (z : ℂ)))) :
periodPairing N (k - 2) f q =
∑ σ ∈ R, ∫ z in (fun τ : ℍ => ((σ • τ : ℍ) : ℂ)) '' ModularGroup.fd,
D z := by sorrySource
Columbia Spring 2021 modular-forms seminar notes, Week 4–5, §1.2, pp. 8–10, proof of Theorem 1, especially the invariant quotient pairing on p. 9; https://www.math.columbia.edu/~dmarcil/Seminars/2021_Spring/Notes/Week4-5.pdf. This is the explicit finite-coset/change-of-measure identity underlying that quotient integral, with the source hypothesis k >= 2 retained. The contraction calculation is adapted from accepted Prove2Me proof 777707bf-f8aa-4fd9-8d82-71afe645b027, Part A, by cbirkbeck.