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Parabolic group cohomology with MTT symmetric-power coefficients

Definition
MTT_ParabolicCohomology

by cbirkbeck · Sep 7, 2026 · Mathlib 0df444a (Lean v4.33.1)

group-cohomologymodular-formsperiods

Let Γ=Γ1(N)\Gamma=\Gamma_1(N)Γ=Γ1​(N) and let VnV_nVn​ be the complex vector space of homogeneous binary polynomials of degree nnn, with the left action ρ(γ)P(X,Y)=P((X,Y)γ)\rho(\gamma)P(X,Y)=P((X,Y)\gamma)ρ(γ)P(X,Y)=P((X,Y)γ). A one-cocycle is a function c:Γ→Vnc:\Gamma\to V_nc:Γ→Vn​ satisfying c(γδ)=ρ(γ)c(δ)+c(γ)c(\gamma\delta)=\rho(\gamma)c(\delta)+c(\gamma)c(γδ)=ρ(γ)c(δ)+c(γ).

A cocycle is parabolic if, for every rational cusp xxx and every γ∈Γ\gamma\in\Gammaγ∈Γ fixing xxx, its value belongs to (ρ(γ)−1)Vn(\rho(\gamma)-1)V_n(ρ(γ)−1)Vn​. Write Zpar1(Γ,Vn)Z^1_{\mathrm{par}}(\Gamma,V_n)Zpar1​(Γ,Vn​) for this subspace and B1(Γ,Vn)B^1(\Gamma,V_n)B1(Γ,Vn​) for the principal cocycles γ↦ρ(γ)P−P\gamma\mapsto\rho(\gamma)P-Pγ↦ρ(γ)P−P. The first parabolic cohomology is

Hpar1(Γ,Vn)=Zpar1(Γ,Vn)/B1(Γ,Vn).H^1_{\mathrm{par}}(\Gamma,V_n)=Z^1_{\mathrm{par}}(\Gamma,V_n)/B^1(\Gamma,V_n).Hpar1​(Γ,Vn​)=Zpar1​(Γ,Vn​)/B1(Γ,Vn​).

This supplies the coefficient representation and quotient space used in the MTT Eichler–Shimura dimension argument. Only the substitution action laws and the immediate cocycle membership interfaces are included; no dimension, injectivity, or surjectivity result is assumed.

Formalization Note The ordinary cocycles and coboundaries are mathlib's existing definitions. The parabolic condition is an intersection of inverse images of the subspaces (ρ(γ)−1)Vn(\rho(\gamma)-1)V_n(ρ(γ)−1)Vn​. The file also checks that all principal coboundaries lie in the parabolic subspace.

Definition code
import Definitions.Def_MTT_Cohomology
import Mathlib.RepresentationTheory.Rep.Basic
import Mathlib.Tactic.Module
import Mathlib.Tactic.FinCases
import Mathlib.Tactic.Ring
import Mathlib.RepresentationTheory.Homological.GroupCohomology.LowDegree

noncomputable section

/-!
# The MTT symmetric-power coefficient representation

The substitution calculations are adapted from allychan327's accepted Prove2Me
reflection-class proof b65c560e-ff07-4802-bc88-856b821148e6. No resource-limit
settings or unrelated parts of that submission are imported.
-/


namespace MTT.Cohomology

open MvPolynomial

variable {R : Type*} [CommRing R]

private lemma act_eq_bind (A : Matrix (Fin 2) (Fin 2) ℤ) (P : Binary R) :
    act A P = MvPolynomial.bind₁ (fun i : Fin 2 =>
      ∑ a : Fin 2, (A a i : R) • MvPolynomial.X a) P := rfl

@[simp] theorem act_one (P : Binary R) : act 1 P = P := by
  rw [act_eq_bind]
  have h : (fun i : Fin 2 => ∑ a : Fin 2,
      ((1 : Matrix (Fin 2) (Fin 2) ℤ) a i : R) • MvPolynomial.X a) =
      fun i : Fin 2 => (MvPolynomial.X i : Binary R) := by
    funext i
    rw [Fin.sum_univ_two]
    fin_cases i <;> simp [Matrix.one_apply]
  rw [h, MvPolynomial.bind₁_X_left, AlgHom.id_apply]

/-- Substituting linear forms respects multiplication of the coefficient matrices. -/
theorem act_matrix_mul (A B : Matrix (Fin 2) (Fin 2) ℤ) (P : Binary R) :
    act (A * B) P = act A (act B P) := by
  simp only [act_eq_bind]
  rw [MvPolynomial.bind₁_bind₁]
  congr 2
  funext i
  rw [map_sum]
  simp only [map_smul, MvPolynomial.bind₁_X_right, Fin.sum_univ_two, Matrix.mul_apply]
  match_scalars <;> ring

/-- A substitution by linear forms preserves the homogeneous degree. -/
theorem act_mem_sym (A : Matrix (Fin 2) (Fin 2) ℤ) {n : ℕ} {P : Binary R}
    (hP : P ∈ Sym R n) : act A P ∈ Sym R n := by
  have hg (i : Fin 2) :
      (∑ a : Fin 2, (A a i : R) • MvPolynomial.X a : Binary R).IsHomogeneous 1 := by
    change _ ∈ Sym R 1
    exact (Sym R 1).sum_mem fun a _ => (Sym R 1).smul_mem _ (isHomogeneous_X _ _)
  change (MvPolynomial.aeval (fun i : Fin 2 =>
    (∑ a : Fin 2, (A a i : R) • MvPolynomial.X a : Binary R)) P).IsHomogeneous n
  simpa only [one_mul] using hP.aeval
    (fun i : Fin 2 => ∑ a : Fin 2, (A a i : R) • MvPolynomial.X a) hg

/-- The MTT left action on homogeneous binary forms as a mathlib representation. -/
def symRepresentation (Γ : Subgroup (Matrix.SpecialLinearGroup (Fin 2) ℤ))
    (n : ℕ) (R : Type*) [CommRing R] : Rep R Γ :=
  Rep.of
    { toFun := fun γ =>
        { toFun := fun P : Sym R n => ⟨act γ.val.val P.val, act_mem_sym _ P.property⟩
          map_add' := fun P Q => Subtype.ext (map_add _ P.val Q.val)
          map_smul' := fun a P => Subtype.ext (map_smul _ a P.val) }
      map_one' := by
        apply LinearMap.ext
        intro P
        exact Subtype.ext (act_one P.val)
      map_mul' := by
        intro γ δ
        apply LinearMap.ext
        intro P
        exact Subtype.ext (act_matrix_mul γ.val.val δ.val.val P.val) }

end MTT.Cohomology


/-!
# Parabolic group cohomology for the MTT coefficient module

The one-cocycles and principal coboundaries are mathlib's existing definitions.
The parabolic subspace requires the value at every cusp-fixing element to lie
in the image of that element minus the identity. This is the definition in
Columbia's Spring 2021 Eichler–Shimura seminar notes, §1.1, specialized to the
rational cusps of Gamma1(N).
-/


namespace MTT.Cohomology

open groupCohomology

abbrev gammaOneRep (N n : ℕ) := symRepresentation (CongruenceSubgroup.Gamma1 N) n ℂ

/-- Cocycles whose restrictions to cyclic cusp stabilizers are principal. -/
def parabolicCocycles (N n : ℕ) :
    Submodule ℂ (CongruenceSubgroup.Gamma1 N → gammaOneRep N n) :=
  cocycles₁ (gammaOneRep N n) ⊓
    ⨅ (x : Cusp) (γ : CongruenceSubgroup.Gamma1 N) (_ : cuspAct γ.val x = x),
      (LinearMap.range ((gammaOneRep N n).ρ γ - LinearMap.id)).comap (LinearMap.proj γ)

/-- The principal coboundaries regarded as a submodule of parabolic cocycles. -/
def parabolicCoboundaries (N n : ℕ) : Submodule ℂ (parabolicCocycles N n) :=
  (coboundaries₁ (gammaOneRep N n)).comap (parabolicCocycles N n).subtype

/-- The first parabolic cohomology is the cocycle space modulo principal coboundaries. -/
abbrev ParabolicH1 (N n : ℕ) :=
  parabolicCocycles N n ⧸ parabolicCoboundaries N n

theorem mem_parabolicCocycles_iff {N n : ℕ}
    (c : CongruenceSubgroup.Gamma1 N → gammaOneRep N n) :
    c ∈ parabolicCocycles N n ↔
      (∀ γ δ, c (γ * δ) = (gammaOneRep N n).ρ γ (c δ) + c γ) ∧
      ∀ (x : Cusp) (γ : CongruenceSubgroup.Gamma1 N), cuspAct γ.val x = x →
        ∃ Q : gammaOneRep N n, c γ = (gammaOneRep N n).ρ γ Q - Q := by
  simp only [parabolicCocycles, Submodule.mem_inf, mem_cocycles₁_iff,
    Submodule.mem_iInf, Submodule.mem_comap, LinearMap.mem_range,
    LinearMap.sub_apply, LinearMap.id_apply, LinearMap.proj_apply, eq_comm]

theorem mem_parabolicCoboundaries_iff {N n : ℕ} (c : parabolicCocycles N n) :
    c ∈ parabolicCoboundaries N n ↔
      ∃ P : gammaOneRep N n, ∀ γ, c.val γ = (gammaOneRep N n).ρ γ P - P := by
  simp only [parabolicCoboundaries, Submodule.mem_comap, coboundaries₁,
    LinearMap.mem_range, Submodule.coe_subtype, funext_iff, d₀₁_hom_apply, eq_comm]

/-- Every principal cocycle satisfies all parabolic restrictions. -/
theorem coboundaries_le_parabolicCocycles (N n : ℕ) :
    coboundaries₁ (gammaOneRep N n) ≤ parabolicCocycles N n := by
  rintro c ⟨P, rfl⟩
  apply (mem_parabolicCocycles_iff _).mpr
  refine ⟨(mem_cocycles₁_iff _).mp (d₀₁_apply_mem_cocycles₁ P), ?_⟩
  intro x γ hx
  exact ⟨P, rfl⟩

end MTT.Cohomology
Source
Columbia Spring 2021 Eichler–Shimura seminar notes, https://www.math.columbia.edu/~dmarcil/Seminars/2021_Spring/Notes/Week4-5.pdf, §1.1 pp. 1–2 (Z^1, B^1, and the cyclic-restriction condition), Remark 1 p. 5; §1.2 pp. 7–9 for the symmetric-power coefficient module. Coefficient substitution calculations adapted with attribution from allychan327, accepted Prove2Me submission b65c560e-ff07-4802-bc88-856b821148e6 for MTT.Cohomology.reflection_class.

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