Definitions/Def_LanglandsTunnell_CubicInduction_AutomorphyDatum31.lean
Local-to-adelic embeddings, congruence sets, GL₃ automorphy datum
For a Dedekind domain R with fraction field K, a finite index type \iota and a finite place v of R, localMatN sends a matrix over the completion K_v to the matrix over the finite adeles whose v-component is the given matrix and whose component at every w \neq v is the identity matrix; localMatN_apply_self, localMatN_apply_of_ne, localMatN_one, localMatN_mul and the two extensionality lemmas matrixFin_ext, matrixAdele_ext (equality of adelic matrices is tested place by place, resp. on the archimedean and finite parts) give the multiplicativity used to upgrade it to a monoid homomorphism localEmbedN on general linear groups. Likewise finMatN puts the identity in the archimedean slot, giving finEmbedN, and localToAdelicN is their composite \mathrm{GL}_\iota(K_v) \to \mathrm{GL}_\iota(\mathbb{A}_K); localToAdelic3 is the case \iota = \mathrm{Fin}\,3, R = \mathcal{O}_{\mathbb{Q}}, K = \mathbb{Q}.
For a finite place v of \mathbb{Q} and a \in \mathbb{N}, converseCongruenceSet3 v a is the set of k in the local maximal compact subgroup of \mathrm{GL}_3(\mathbb{Q}_v) whose entries in positions (1,2) and (3,1) have valuation at most \exp(-a) and whose (3,2) entry has valuation at most \exp(-2a), i.e. lie in \mathfrak{p}_v^{a}, \mathfrak{p}_v^{a}, \mathfrak{p}_v^{2a}; the identity belongs to it. parabolicCongruenceSet3 v a consists of products p\,k with the (3,1) and (3,2) entries of p zero and k in the congruence set. IsCongruenceEquivariantAt/IsCongruenceEquivariantAlong assert W(gk) = \chi(u)\,W(g) for all g and all k in the congruence set, where u is a unit equal to the (3,3) entry of k (in the adelic version k is pushed forward by localToAdelic3). HasVanishingUnipotentIntegralAt/HasVanishingUnipotentIntegralAlong assert that for every g the integral, against the self-dual Haar measure of \mathbb{Q}_v over \{x : \mathrm{v}(x) \le \exp(1)\} = \mathfrak{p}_v^{-1}, of W(g \cdot n(x)) vanishes, n(x) being the unipotent with x in position (2,3).
AutomorphyDatum31 pins ψ S a ω W lam1 lam2 is a structure carrying a function form on \mathrm{GL}_3(\mathbb{A}_{\mathbb{Q}}) together with, as fields: continuity; left invariance under \mathrm{GL}_3(\mathbb{Q}); the central character law with \omega; moderate growth; congruence equivariance at each v \in S of level a(v) through the local component of \omega; the identity \mathrm{whittaker3}\,\psi\,(\mathrm{form})(g) = W(g) at every g whose components at the places of S lie in the congruence sets; vanishing of the double integral of form over the unipotent radical \mathrm{radicalP21} (against the measure carried by pins) at every g whose components at the places of S lie in the parabolic sets; and, at each p \notin S, right invariance under the image of the local maximal compact and the coset-eigenfunction property for the two Hecke generators with eigenvalues \mathrm{lam1}(p), \mathrm{lam2}(p). AutomorphyDatum31.zero exhibits such a datum with W = 0, given by the zero function.
Relation to Mathlib
Mathlib supplies the finite adele and adele rings, adic completions, general linear groups and Haar measure; the congruence sets, the equivariance and unipotent-integral predicates and the automorphy datum are the project's own. The matrix constructions repeat, for an arbitrary finite index type, the \mathrm{GL}_2 embeddings AdelicDock.localMat/AdelicDock.finMat.
Where it is used
These are the hypotheses of a converse theorem for \mathrm{GL}_3 in the form needed for Langlands–Tunnell: the datum records exactly the automorphy, growth, Hecke and local congruence properties of a candidate form on \mathrm{GL}_3(\mathbb{A}_{\mathbb{Q}}) attached to a cubic induction. Langlands–Tunnell in turn provides the modularity of the mod-3 representation with which the Wiles argument for Fermat's Last Theorem begins.
References
- H. Jacquet, I. I. Piatetski-Shapiro and J. A. Shalika, Automorphic forms on GL(3) I, II, Annals of Mathematics 109 (1979), 169–212 and 213–258
- R. P. Langlands, Base Change for GL(2), Annals of Mathematics Studies 96, Princeton University Press, 1980
- J. Tunnell, Artin's conjecture for representations of octahedral type, Bulletin of the American Mathematical Society (N.S.) 5 (1981), 173–175
References are suggested automatically and have not been individually verified.
English text generated automatically from the Lean source; the Lean statement is authoritative.
- 244 lines
- 45 declarations
- used in the statements of 185 theorems and imported by 213 proofs
- imports 2 definition modules
Source file: Definitions/Def_LanglandsTunnell_CubicInduction_AutomorphyDatum31.lean
Imported by
- no other definition module
Declarations
- theorem
LanglandsTunnell.CubicInduction.matrixFin_ext - theorem
LanglandsTunnell.CubicInduction.matrixAdele_ext - def
LanglandsTunnell.CubicInduction.localMatN - theorem
LanglandsTunnell.CubicInduction.localMatN_apply_self - theorem
LanglandsTunnell.CubicInduction.localMatN_apply_of_ne - theorem
LanglandsTunnell.CubicInduction.mapMatrix_localMatN_self - theorem
LanglandsTunnell.CubicInduction.mapMatrix_localMatN_of_ne - theorem
LanglandsTunnell.CubicInduction.localMatN_one - theorem
LanglandsTunnell.CubicInduction.localMatN_mul - def
LanglandsTunnell.CubicInduction.localEmbedN - def
LanglandsTunnell.CubicInduction.finMatN - theorem
LanglandsTunnell.CubicInduction.mapMatrix_arch_finMatN - theorem
LanglandsTunnell.CubicInduction.mapMatrix_fin_finMatN - theorem
LanglandsTunnell.CubicInduction.finMatN_one - theorem
LanglandsTunnell.CubicInduction.finMatN_mul - def
LanglandsTunnell.CubicInduction.finEmbedN - def
LanglandsTunnell.CubicInduction.localToAdelicN - abbrev
LanglandsTunnell.CubicInduction.localToAdelic3 - def
LanglandsTunnell.CubicInduction.converseCongruenceSet3 - theorem
LanglandsTunnell.CubicInduction.one_mem_converseCongruenceSet3 - def
LanglandsTunnell.CubicInduction.parabolicCongruenceSet3 - def
LanglandsTunnell.CubicInduction.IsCongruenceEquivariantAt - def
LanglandsTunnell.CubicInduction.HasVanishingUnipotentIntegralAt - def
LanglandsTunnell.CubicInduction.HasVanishingUnipotentIntegralAlong - def
LanglandsTunnell.CubicInduction.IsCongruenceEquivariantAlong - structure
LanglandsTunnell.CubicInduction.AutomorphyDatum31 - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.S - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.form - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.continuous - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.automorphic - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.form - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.central - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.form - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.moderateGrowth - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.equivariant - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.whittaker_eq - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.cuspidalP21 - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.letI - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.heckeInvariant - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.IsRightInvariant - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.hecke1 - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.IsCosetEigenfunction - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.hecke2 - field
LanglandsTunnell.CubicInduction.AutomorphyDatum31.IsCosetEigenfunction - def
LanglandsTunnell.CubicInduction.AutomorphyDatum31.zero
Source
import Definitions.Def_LanglandsTunnell_CubicInduction_GlobalZeta31 import Definitions.Def_AdelicDock_LocalEmbedding set_option autoImplicit false open Matrix IsDedekindDomain NumberField MeasureTheory AutomorphicForm noncomputable section namespace LanglandsTunnell.CubicInduction section Embeddings variable (ι : Type*) [Fintype ι] [DecidableEq ι] variable (R K : Type*) [CommRing R] [IsDedekindDomain R] [Field K] [Algebra R K] [IsFractionRing R K] theorem matrixFin_ext {M N : Matrix ι ι (FiniteAdeleRing R K)} (h : ∀ w : HeightOneSpectrum R, (AdelicLevel.finAdeleEval R K w).mapMatrix M = (AdelicLevel.finAdeleEval R K w).mapMatrix N) : M = N := by ext i j w : 2 have hw := congrFun (congrFun (h w) i) j simpa only [RingHom.mapMatrix_apply, Matrix.map_apply, AdelicLevel.finAdeleEval_apply] using hw theorem matrixAdele_ext {M N : Matrix ι ι (AdeleRing R K)} (h₁ : (AdelicLevel.adeleArch R K).mapMatrix M = (AdelicLevel.adeleArch R K).mapMatrix N) (h₂ : (AdelicLevel.adeleFin R K).mapMatrix M = (AdelicLevel.adeleFin R K).mapMatrix N) : M = N := by ext i j have hw₁ := congrFun (congrFun h₁ i) j have hw₂ := congrFun (congrFun h₂ i) j simp only [RingHom.mapMatrix_apply, Matrix.map_apply, AdelicLevel.adeleArch_apply, AdelicLevel.adeleFin_apply] at hw₁ hw₂ exact Prod.ext hw₁ hw₂ variable (v : HeightOneSpectrum R) def localMatN (g : Matrix ι ι (v.adicCompletion K)) : Matrix ι ι (FiniteAdeleRing R K) := Matrix.of fun i j => AdelicDock.splice R K v ((1 : Matrix ι ι (FiniteAdeleRing R K)) i j) (g i j) omit [Fintype ι] in theorem localMatN_apply_self (g : Matrix ι ι (v.adicCompletion K)) (i j : ι) : localMatN ι R K v g i j v = g i j := by simp [localMatN] omit [Fintype ι] in theorem localMatN_apply_of_ne (g : Matrix ι ι (v.adicCompletion K)) (i j : ι) {w : HeightOneSpectrum R} (hw : w ≠ v) : localMatN ι R K v g i j w = (1 : Matrix ι ι (w.adicCompletion K)) i j := by simp only [localMatN, Matrix.of_apply, AdelicDock.splice_apply_of_ne R K v _ _ hw] rw [Matrix.one_apply, Matrix.one_apply] split_ifs <;> rfl theorem mapMatrix_localMatN_self (g : Matrix ι ι (v.adicCompletion K)) : (AdelicLevel.finAdeleEval R K v).mapMatrix (localMatN ι R K v g) = g := by ext i j simp [RingHom.mapMatrix_apply, Matrix.map_apply, AdelicLevel.finAdeleEval_apply, localMatN_apply_self] theorem mapMatrix_localMatN_of_ne (g : Matrix ι ι (v.adicCompletion K)) {w : HeightOneSpectrum R} (hw : w ≠ v) : (AdelicLevel.finAdeleEval R K w).mapMatrix (localMatN ι R K v g) = 1 := by ext i j simp [RingHom.mapMatrix_apply, Matrix.map_apply, AdelicLevel.finAdeleEval_apply, localMatN_apply_of_ne ι R K v g i j hw] theorem localMatN_one : localMatN ι R K v 1 = 1 := by refine matrixFin_ext ι R K fun w => ?_ by_cases hw : w = v · subst hw; rw [mapMatrix_localMatN_self, map_one] · rw [mapMatrix_localMatN_of_ne ι R K v _ hw, map_one] theorem localMatN_mul (g h : Matrix ι ι (v.adicCompletion K)) : localMatN ι R K v (g * h) = localMatN ι R K v g * localMatN ι R K v h := by refine matrixFin_ext ι R K fun w => ?_ by_cases hw : w = v · subst hw rw [map_mul, mapMatrix_localMatN_self, mapMatrix_localMatN_self, mapMatrix_localMatN_self] · rw [map_mul, mapMatrix_localMatN_of_ne ι R K v _ hw, mapMatrix_localMatN_of_ne ι R K v _ hw, mapMatrix_localMatN_of_ne ι R K v _ hw, mul_one] def localEmbedN : GL ι (v.adicCompletion K) →* GL ι (FiniteAdeleRing R K) where toFun g := { val := localMatN ι R K v g inv := localMatN ι R K v ((g⁻¹ : GL ι (v.adicCompletion K)) : Matrix _ _ _) val_inv := by rw [← localMatN_mul, Units.mul_inv, localMatN_one] inv_val := by rw [← localMatN_mul, Units.inv_mul, localMatN_one] } map_one' := Units.ext (by simp only [Units.val_one]; exact localMatN_one ι R K v) map_mul' g h := Units.ext (by simp only [Units.val_mul]; exact localMatN_mul ι R K v _ _) def finMatN (g : Matrix ι ι (FiniteAdeleRing R K)) : Matrix ι ι (AdeleRing R K) := Matrix.of fun i j => (((1 : Matrix ι ι (InfiniteAdeleRing K)) i j, g i j) : AdeleRing R K) theorem mapMatrix_arch_finMatN (g : Matrix ι ι (FiniteAdeleRing R K)) : (AdelicLevel.adeleArch R K).mapMatrix (finMatN ι R K g) = 1 := by ext i j simp [finMatN, RingHom.mapMatrix_apply, Matrix.map_apply, AdelicLevel.adeleArch_apply] theorem mapMatrix_fin_finMatN (g : Matrix ι ι (FiniteAdeleRing R K)) : (AdelicLevel.adeleFin R K).mapMatrix (finMatN ι R K g) = g := by ext i j simp [finMatN, RingHom.mapMatrix_apply, Matrix.map_apply, AdelicLevel.adeleFin_apply] theorem finMatN_one : finMatN ι R K 1 = 1 := matrixAdele_ext ι R K (by rw [mapMatrix_arch_finMatN, map_one]) (by rw [mapMatrix_fin_finMatN, map_one]) theorem finMatN_mul (g h : Matrix ι ι (FiniteAdeleRing R K)) : finMatN ι R K (g * h) = finMatN ι R K g * finMatN ι R K h := matrixAdele_ext ι R K (by rw [map_mul, mapMatrix_arch_finMatN, mapMatrix_arch_finMatN, mapMatrix_arch_finMatN, mul_one]) (by rw [map_mul, mapMatrix_fin_finMatN, mapMatrix_fin_finMatN, mapMatrix_fin_finMatN]) def finEmbedN : GL ι (FiniteAdeleRing R K) →* GL ι (AdeleRing R K) where toFun g := { val := finMatN ι R K g inv := finMatN ι R K ((g⁻¹ : GL ι (FiniteAdeleRing R K)) : Matrix _ _ _) val_inv := by rw [← finMatN_mul, Units.mul_inv, finMatN_one] inv_val := by rw [← finMatN_mul, Units.inv_mul, finMatN_one] } map_one' := Units.ext (by simp only [Units.val_one]; exact finMatN_one ι R K) map_mul' g h := Units.ext (by simp only [Units.val_mul]; exact finMatN_mul ι R K _ _) def localToAdelicN : GL ι (v.adicCompletion K) →* GL ι (AdeleRing R K) := (finEmbedN ι R K).comp (localEmbedN ι R K v) end Embeddings section LocalThree variable (v : HeightOneSpectrum (𝓞 ℚ)) abbrev localToAdelic3 : LocalGL3 v →* AdelicGL 3 (𝓞 ℚ) ℚ := localToAdelicN (Fin 3) (𝓞 ℚ) ℚ v def converseCongruenceSet3 (a : ℕ) : Set (LocalGL3 v) := {k | k ∈ localMaximalCompact3 (𝓞 ℚ) ℚ v ∧ Valued.v ((k : Matrix (Fin 3) (Fin 3) (v.adicCompletion ℚ)) 0 1) ≤ WithZero.exp (-(a : ℤ)) ∧ Valued.v ((k : Matrix (Fin 3) (Fin 3) (v.adicCompletion ℚ)) 2 0) ≤ WithZero.exp (-(a : ℤ)) ∧ Valued.v ((k : Matrix (Fin 3) (Fin 3) (v.adicCompletion ℚ)) 2 1) ≤ WithZero.exp (-(2 * (a : ℤ)))} theorem one_mem_converseCongruenceSet3 (a : ℕ) : (1 : LocalGL3 v) ∈ converseCongruenceSet3 v a := by refine ⟨Subgroup.one_mem _, ?_, ?_, ?_⟩ · rw [Units.val_one, Matrix.one_apply_ne (by decide), map_zero] exact zero_le · rw [Units.val_one, Matrix.one_apply_ne (by decide), map_zero] exact zero_le · rw [Units.val_one, Matrix.one_apply_ne (by decide), map_zero] exact zero_le def parabolicCongruenceSet3 (a : ℕ) : Set (LocalGL3 v) := {g | ∃ p k : LocalGL3 v, (p : Matrix (Fin 3) (Fin 3) (v.adicCompletion ℚ)) 2 0 = 0 ∧ (p : Matrix (Fin 3) (Fin 3) (v.adicCompletion ℚ)) 2 1 = 0 ∧ k ∈ converseCongruenceSet3 v a ∧ g = p * k} def IsCongruenceEquivariantAt (a : ℕ) (χ : (v.adicCompletion ℚ)ˣ →* ℂˣ) (W : LocalGL3 v → ℂ) : Prop := ∀ k ∈ converseCongruenceSet3 v a, ∀ u : (v.adicCompletion ℚ)ˣ, (u : v.adicCompletion ℚ) = (k : Matrix (Fin 3) (Fin 3) (v.adicCompletion ℚ)) 2 2 → ∀ g, W (g * k) = ((χ u : ℂˣ) : ℂ) * W g def HasVanishingUnipotentIntegralAt (W : LocalGL3 v → ℂ) : Prop := letI := LanglandsTunnell.TateLocal.localBorel ℚ v ∀ g : LocalGL3 v, (∫ x in {x : v.adicCompletion ℚ | Valued.v x ≤ WithZero.exp (1 : ℤ)}, W (g * upperUnipotent3 0 x 0) ∂(LanglandsTunnell.TateLocal.selfDualHaarAt ℚ v)) = 0 def HasVanishingUnipotentIntegralAlong (W : AdelicGL 3 (𝓞 ℚ) ℚ → ℂ) : Prop := letI := LanglandsTunnell.TateLocal.localBorel ℚ v ∀ g : AdelicGL 3 (𝓞 ℚ) ℚ, (∫ x in {x : v.adicCompletion ℚ | Valued.v x ≤ WithZero.exp (1 : ℤ)}, W (g * localToAdelic3 v (upperUnipotent3 0 x 0)) ∂(LanglandsTunnell.TateLocal.selfDualHaarAt ℚ v)) = 0 def IsCongruenceEquivariantAlong (a : ℕ) (χ : (v.adicCompletion ℚ)ˣ →* ℂˣ) (W : AdelicGL 3 (𝓞 ℚ) ℚ → ℂ) : Prop := ∀ k ∈ converseCongruenceSet3 v a, ∀ u : (v.adicCompletion ℚ)ˣ, (u : v.adicCompletion ℚ) = (k : Matrix (Fin 3) (Fin 3) (v.adicCompletion ℚ)) 2 2 → ∀ g, W (g * localToAdelic3 v k) = ((χ u : ℂˣ) : ℂ) * W g end LocalThree section Global structure AutomorphyDatum31 (pins : CarrierPins ℚ) (ψ : AddChar (AdeleRing (𝓞 ℚ) ℚ) ℂ) (S : Finset (HeightOneSpectrum (𝓞 ℚ))) (a : HeightOneSpectrum (𝓞 ℚ) → ℕ) (ω : (AdeleRing (𝓞 ℚ) ℚ)ˣ →* ℂˣ) (W : AdelicGL 3 (𝓞 ℚ) ℚ → ℂ) (lam1 lam2 : HeightOneSpectrum (𝓞 ℚ) → ℂ) where form : AdelicGL 3 (𝓞 ℚ) ℚ → ℂ continuous : Continuous form automorphic : ∀ (γ : GL (Fin 3) ℚ) (g : AdelicGL 3 (𝓞 ℚ) ℚ), form (globalPointsGL 3 (𝓞 ℚ) ℚ γ * g) = form g central : ∀ (z : (AdeleRing (𝓞 ℚ) ℚ)ˣ) (g : AdelicGL 3 (𝓞 ℚ) ℚ), form (centralScalarGL 3 (𝓞 ℚ) ℚ z * g) = (ω z : ℂ) * form g moderateGrowth : IsModerateGrowth3 ℚ form equivariant : ∀ v ∈ S, IsCongruenceEquivariantAlong v (a v) (TateGlobal.localChar ω v) form whittaker_eq : ∀ g : AdelicGL 3 (𝓞 ℚ) ℚ, (∀ v ∈ S, componentAt3 (𝓞 ℚ) ℚ v g ∈ converseCongruenceSet3 v (a v)) → whittaker3 pins ψ form g = W g cuspidalP21 : ∀ g : AdelicGL 3 (𝓞 ℚ) ℚ, (∀ v ∈ S, componentAt3 (𝓞 ℚ) ℚ v g ∈ parabolicCongruenceSet3 v (a v)) → (letI := pins.nS; ∫ x, ∫ y, form (radicalP21 ![x, y] * g) ∂pins.ν ∂pins.ν) = 0 heckeInvariant : ∀ p, p ∉ S → IsRightInvariant ((localMaximalCompact3 (𝓞 ℚ) ℚ p).map (localToAdelic3 p)) form hecke1 : ∀ p, p ∉ S → IsCosetEigenfunction ((localMaximalCompact3 (𝓞 ℚ) ℚ p).map (localToAdelic3 p)) (localToAdelic3 p (heckeGen1 p)) form (lam1 p) hecke2 : ∀ p, p ∉ S → IsCosetEigenfunction ((localMaximalCompact3 (𝓞 ℚ) ℚ p).map (localToAdelic3 p)) (localToAdelic3 p (heckeGen2 p)) form (lam2 p) def AutomorphyDatum31.zero (pins : CarrierPins ℚ) (ψ : AddChar (AdeleRing (𝓞 ℚ) ℚ) ℂ) (S : Finset (HeightOneSpectrum (𝓞 ℚ))) (a : HeightOneSpectrum (𝓞 ℚ) → ℕ) (ω : (AdeleRing (𝓞 ℚ) ℚ)ˣ →* ℂˣ) (lam1 lam2 : HeightOneSpectrum (𝓞 ℚ) → ℂ) : AutomorphyDatum31 pins ψ S a ω 0 lam1 lam2 where form := 0 continuous := continuous_const automorphic := fun _ _ => rfl central := fun _ _ => by simp moderateGrowth := isModerateGrowth3_zero ℚ equivariant := fun _ _ _ _ _ _ _ => by simp whittaker_eq := fun _ _ => by simp only [whittaker3, Pi.zero_apply, zero_mul, MeasureTheory.integral_zero] cuspidalP21 := fun _ _ => by simp heckeInvariant := fun _ _ _ _ _ => rfl hecke1 := fun p _ => isCosetEigenfunction_zero _ _ (lam1 p) hecke2 := fun p _ => isCosetEigenfunction_zero _ _ (lam2 p) end Global end LanglandsTunnell.CubicInduction end #check @LanglandsTunnell.CubicInduction.localToAdelic3 #check @LanglandsTunnell.CubicInduction.converseCongruenceSet3 #check @LanglandsTunnell.CubicInduction.IsCongruenceEquivariantAt #check @LanglandsTunnell.CubicInduction.HasVanishingUnipotentIntegralAt #check @LanglandsTunnell.CubicInduction.AutomorphyDatum31 #check @LanglandsTunnell.CubicInduction.HasVanishingUnipotentIntegralAlong #check @LanglandsTunnell.CubicInduction.IsCongruenceEquivariantAlong #print axioms LanglandsTunnell.CubicInduction.localToAdelicN #print axioms LanglandsTunnell.CubicInduction.one_mem_converseCongruenceSet3 #print axioms LanglandsTunnell.CubicInduction.AutomorphyDatum31.zero
Statements phrased using this module (185)
- Local functional equation at one deeply twisted prime
LanglandsTunnell.CubicInduction.exists_forall_mem_gl3CyclicSubspace_localZeta31_fe_one_of_cubicInductionForm_twist_deepAt593 below · depth 18 - Local constants of twisted cubic induction on the cyclic span
LanglandsTunnell.CubicInduction.exists_forall_mem_gl3CyclicSubspace_localZetaDual31_eq_mul_of_cubicInductionForm_twisted_badPlaces_noFE32_adm598 below · depth 18 - Explicit K₁(p^{3B+Δ})-invariant bump vector for twisted cubic induction
LanglandsTunnell.CubicInduction.exists_mem_gl3CyclicSubspace_twist_whittakerLoc_congruenceK1_invariant_iotaGL_bump_of_conductor_le_ed3111 below · depth 18 - Finiteness of torus coefficients in the twisted local cyclic space
LanglandsTunnell.CubicInduction.forall_mem_gl3CyclicSubspace_torusFinite_of_cubicInductionForm_twisted_noFE32_level19 below · depth 18 - Cubic automorphic induction: existence of a cubic induction form
LanglandsTunnell.CubicInduction.hasCubicInductionForm_arch_torusValues_localPackage_bad1,687 below · depth 18 - Dual-side family identity in the GL₂timesGL₃ entire-pair assembly
LanglandsTunnell.RankinSelberg.EntirePairAssembly.dual_identity_family24 below · depth 18 - Archimedean holomorphy and non-vanishing from a torus Γ-factor identity
LanglandsTunnell.RankinSelberg.differentiableOn_and_rsArchIntegral_ne_zero_of_torusPair_eq_gammaFactor5 below · depth 18 - Local relations at p for the dual translate of W_f
LanglandsTunnell.RankinSelberg.dualTranslate_finWhittaker_local_relations3 below · depth 18 - Half-plane integrability of archimedean GL₂timesGL₃ Rankin–Selberg integrands
LanglandsTunnell.RankinSelberg.exists_forall_integrable_archWhittaker_torusPair_rpow_det7 below · depth 18 - Finite GL₃-translate family: constant integral and dual root number
LanglandsTunnell.RankinSelberg.exists_gl3Translates_sum_rsFinIntegral_cells_eq_const_and_dual_eq_rootNumberMonomial_of_finWhittaker_one_ne_zero_of_localSpaceAt_of_member_of_fe32_normPin_twisted_offSQ_archPsi_bump_levelShift_global982 below · depth 18 - Simultaneous splitting of the finite Whittaker factor over T
AutomorphicForm.exists_finWhittaker_eq_sum_prod_mul_of_isIsotypicCuspFormAt_placeEmbed_invariant_of_localSpaceAt14 below · depth 19 - Archimedean root sizes of a GL₂ block image and its dual
LanglandsTunnell.CubicInduction.archRoot_iota_archRealGLAt_and_dual0 below · depth 19 - Local GL₃timesGL₁ constants of a cubic induction at one bad place
LanglandsTunnell.CubicInduction.exists_forall_mem_gl3CyclicSubspace_localZetaDual31_eq_mul_of_isCubicInductionDataOn_deepAt539 below · depth 19 - Span-wide local constants for deep cubic induction data
LanglandsTunnell.CubicInduction.exists_forall_mem_gl3CyclicSubspace_localZetaDual31_eq_mul_of_isCubicInductionDataOn_deep_badPlaces550 below · depth 19 - Existence of a cubic-induction datum: archimedean and bad-place package
LanglandsTunnell.CubicInduction.exists_isCubicInductionDataOn_arch_torusValues_localPackage_bad1,686 below · depth 19 - Half-plane integrability of pure-tensor Rankin–Selberg cell integrands
LanglandsTunnell.RankinSelberg.exists_forall_integrable_rsFinCellIntegrand_pureTensorTerm_dual_and_hybrid_of_depth_twisted_torusFinite_central_growth_of_principalLevel_of_gammaHyp136 below · depth 19 - Integrability of the twisted Rankin–Selberg finite-cell integrands
LanglandsTunnell.RankinSelberg.exists_forall_integrable_rsFinCellIntegrand_translate_and_dual_twisted116 below · depth 19 - Half-plane integrability of an archimedean torus profile
LanglandsTunnell.RankinSelberg.exists_forall_lintegral_norm_torusProfile_mul_rpow_lt_top0 below · depth 19 - Rational local γ at a level prime, archimedean nonvanishing edition
LanglandsTunnell.RankinSelberg.exists_rational_gamma_rsLocalIntegral_member_twisted_of_finiteFamily_arch_deep_archPsi489 below · depth 19 - Modulus of a real Whittaker function on torus times O(2)
LanglandsTunnell.RankinSelberg.norm_archWhittaker_upperUnit_mul_rowIsometry0 below · depth 19 - Twisting a GL₃ cusp form by a character of the determinant
LanglandsTunnell.CubicInduction.continuous_and_isCuspidalAlong_and_whittaker3_fnTwist3_eq_chiDetGL_mul0 below · depth 20 - Local Whittaker data at bad places of a saturated cubic induction
LanglandsTunnell.CubicInduction.exists_forall_le_exists_localWhittaker_saturated_and_laurent_fe_of_mem_bad65 below · depth 20 - Conductor bound for the local central character at unramified v
LanglandsTunnell.CubicInduction.exists_hasConductorExponentAt_localChar_centralChar_le_inducedLevelAt_of_isCubicInductionDataOn278 below · depth 20 - Odd admissible twist with non-vanishing archimedean GL₃ × GL₁ zeta
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_ne_zero_odd_of_isCubicInductionDataOn6 below · depth 20 - Archimedean zeta non-vanishing far right for a suitable translate
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_ne_zero_of_isCubicInductionDataOn1 below · depth 20 - Local newvector of level K₁(ℓᵥ) at twist-ramified primes
LanglandsTunnell.CubicInduction.exists_mem_gl3CyclicSubspace_congruenceK1_torusValues_of_isCubicInductionDataOn615 below · depth 20 - Congruence-invariant vector in the local cyclic space at a ramified bad place
LanglandsTunnell.CubicInduction.exists_mem_gl3CyclicSubspace_principalLevel_le_of_isRamifiedIn_of_isCubicInductionDataOn_of_conductorBound615 below · depth 20 - A twist-independent constant in the deep-place GL₃× GL₁ functional equation
LanglandsTunnell.CubicInduction.exists_ne_zero_forall_eval_mul_eq_mul_rootNumber_mul_eval_of_forall_localZeta31_fe_twist_of_isCubicInductionDataOn_of_deep_of_archPackage_of_inv_eq_psiQ_of_whittakerLoc_one502 below · depth 20 - Pure tensor Whittaker vector with local multiplicity one at S
LanglandsTunnell.CubicInduction.exists_whittaker3_eq_mul_prod_hasWhittakerMultOne_of_isCuspidalAlong354 below · depth 20 - Converse-theorem input for the cubic induction from an archimedean Whittaker vector
LanglandsTunnell.CubicInduction.exists_whittaker_zeta_fe_of_forall_not_mem_isInducedSphericalAt_of_arch145 below · depth 20 - Product formula (prodᵥλᵥ²) λ_∞²=1 for a cubic induction
LanglandsTunnell.CubicInduction.finprod_sq_mul_lamSqArch_eq_one_of_forall_ne_zero_localZeta31_fe_rootNumber_of_isCubicInductionDataOn_of_archPackage_of_inv_eq_psiQ538 below · depth 20 - Twisting a cubic idelic character by χ ∘ N
LanglandsTunnell.CubicInduction.inducedCoeff_mul_comp_idelicNorm_and_isBadPlace_iff_of_conductorExponentAt_le24 below · depth 20 - Cuspidality of a GL₃ form from entire tempered Euler products
LanglandsTunnell.CubicInduction.isCuspidalAlong_form_of_tempered_of_entire_eulerTwists760 below · depth 20 - Identified local functional equation passes to the cyclic span
LanglandsTunnell.CubicInduction.localZeta31_identified_of_mem_gl3CyclicSubspace1 below · depth 20 - Converse theorem on GL₃/ℚ with finite exceptional set
LanglandsTunnell.CubicInduction.nonempty_automorphyDatum31_of_zeta_fe22 below · depth 20 - Non-norm condition is stable under twisting by base-changed characters
LanglandsTunnell.CubicInduction.not_exists_eq_pow_inertiaDeg_mul_comp_idelicNorm_of_not_exists12 below · depth 20 - S-part integrability of the GL₃ zeta and dual integrands
LanglandsTunnell.CubicInduction.sPart_integrable_and_dual_of_isCubicInductionDataOn_of_isGaugeMajorised353 below · depth 20 - Central character law for the archimedean Whittaker function
LanglandsTunnell.CubicInduction.whittakerArch_scalar_mul_eq_centralChar_mul_of_isCubicInductionDataOn0 below · depth 20 - Global realisation of local Rankin–Selberg pairs at p
LanglandsTunnell.RankinSelberg.exists_factor_fundamentalDomain_forall_rsGlobalIntegral_realisation_member_twisted_of_finiteFamily_arch_of_archNonvanishing467 below · depth 20 - Cut-off remainder integrands of the dual finite cell are integrable
LanglandsTunnell.RankinSelberg.exists_forall_integrable_cutoff_remainder_mul_finprod_away113 below · depth 20 - Half-plane integrability of primal and dual finite cell integrands
LanglandsTunnell.RankinSelberg.exists_forall_integrable_rsFinCellIntegrand_translate_and_dual104 below · depth 20 - A non-vanishing rational local Rankin–Selberg pair at a level prime
LanglandsTunnell.RankinSelberg.exists_mem_rsLocalIntegral_ne_zero_and_rational_member_twisted_of_finiteFamily_arch_deep58 below · depth 20 - Finiteness, continuity and unit phase of dual Whittaker products
LanglandsTunnell.RankinSelberg.finite_mulSupport_and_continuous_and_exists_phase_finprod_dualWhittakerFn3_away1 below · depth 20 - Swapping the S_Q-slots: dual and hybrid pure-tensor integrability
LanglandsTunnell.RankinSelberg.integrable_pureTensorTerm_dual_and_hybrid_of_integrable_cutoff_of_forall_lintegral_lt_top15 below · depth 20 - Radical Fourier coefficient of the dual mirabolic GL₃ series
LanglandsTunnell.CubicInduction.box_integral_dualSeries_radical_eq_ideleNorm_mul_tsum_integral_dual1 below · depth 21 - Local zeta functional equation at a ramified place
LanglandsTunnell.CubicInduction.exists_localZeta31_fe_one_inducedEulerPoly_rational_of_isCubicInductionDataOn_of_isRamifiedIn527 below · depth 21 - Local functional equation at a bad place unramified in K
LanglandsTunnell.CubicInduction.exists_localZeta31_fe_one_inducedEulerPoly_rational_of_isCubicInductionDataOn_of_not_isRamifiedIn527 below · depth 21 - Three local characters at a bad prime of cubic induction
LanglandsTunnell.CubicInduction.exists_prod_eq_localChar_and_prod_stdRootNumberAt_eq_of_saturated21 below · depth 21 - Rational representatives of polynomially bounded gauge on GL₃(A_ℚ)
LanglandsTunnell.CubicInduction.exists_rational_inv_mul_mem_converseCongruence_gauge3_le0 below · depth 21 - Local translates at v of a cuspidal GL₃ Hecke eigenform
LanglandsTunnell.CubicInduction.exists_sum_eq_span_translates_of_isCuspidalAlong_of_isCosetEigenfunction336 below · depth 21 - Mirabolic series equals its dual from radical coefficients
LanglandsTunnell.CubicInduction.mirabolicSeries_eq_dual_of_radicalCoefficient_eq7 below · depth 21 - Integrability of the dual S-part zeta integrand on GL₃
LanglandsTunnell.CubicInduction.sPartDual_integrable_of_isCubicInductionDataOn_of_isGaugeMajorised329 below · depth 21 - Convergence of the S-part zeta integral for cubic induction data
LanglandsTunnell.CubicInduction.sPart_integrable_of_isCubicInductionDataOn_of_isGaugeMajorised325 below · depth 21 - Integrability of the translated split dual finite cell integrand
LanglandsTunnell.RankinSelberg.exists_forall_integrable_translate_rsFinCellIntegrand_dual_split_of_dualFactor_phase109 below · depth 21 - Purified p-slot splitting of Whittaker coefficients of p-adic translates
LanglandsTunnell.RankinSelberg.exists_frozen_forall_sum_translate_purified_whittakerCoefficient_eq_mul_pSlot_of_finiteFamily_arch351 below · depth 21 - p-slot factorisation of GL₃ Whittaker functions along ι
LanglandsTunnell.RankinSelberg.exists_frozen_forall_sum_translate_whittaker_iota_eq_mul_pSlot_of_finiteFamily_arch42 below · depth 21 - Non-vanishing far right of a reference Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.exists_pureTranslates_combination_forall_rsGlobalIntegral_ne_zero_member_twisted_of_finiteFamily_arch_of_archNonvanishing463 below · depth 21 - Unisolvence points, reference points and cut-off subgroups at S_Q
LanglandsTunnell.RankinSelberg.exists_unisolvence_refPoint_cutoff_of_linearIndependent_slots1 below · depth 21 - Measurability and isolation identity for pure-tensor remainders
LanglandsTunnell.RankinSelberg.measurable_remainder_and_dualFactor_translate_mul_prod_eq_of_pureTensor_expansion2 below · depth 21 - Measurability of the dual S-part zeta integrands
LanglandsTunnell.CubicInduction.aestronglyMeasurable_sPartDual_integrand_of_isCubicInductionDataOn2 below · depth 22 - Annihilator of local translates of a cuspidal GL₃ eigenform
LanglandsTunnell.CubicInduction.exists_forall_sum_smul_translate_eq_zero_of_isCuspidalAlong335 below · depth 22 - Convergence of the dual archimedean GL₃ zeta integral at the trivial twist
LanglandsTunnell.CubicInduction.exists_isArchZeta31ConvergentAbove_dualWhittakerFn3_whittakerArch_of_isCubicInductionDataOn0 below · depth 22 - Uncountable non-vanishing of the cut finite Rankin–Selberg factor
LanglandsTunnell.RankinSelberg.exists_finTranslate_not_countable_rsFinIntegral_indicator_ne_zero_of_purifier_of_finiteFamily_arch93 below · depth 22 - Frozen complements: explicit p-slot splitting of GL₃ Whittaker functions
LanglandsTunnell.RankinSelberg.exists_frozen_forall_sum_translate_whittaker_iota_eq_mul_pSlot_of_finiteFamily_arch_explicit42 below · depth 22 - Factorisation of the purified reference Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.exists_ne_zero_forall_rsGlobalIntegral_reference_eq_mul_rsArchIntegral_mul_rsFinIntegral_indicator_mul_of_finiteFamily_arch410 below · depth 22 - A p-adic purifier with pure-tensor Whittaker coefficient
LanglandsTunnell.RankinSelberg.exists_purifier_whittakerCoefficient_eq_mul_pSlot_of_finiteFamily_arch25 below · depth 22 - Independent tensor splitting of the finite Whittaker factor
AutomorphicForm.exists_finWhittaker_eq_sum_prod_mul_linearIndependent_levelOne_invariant_of_isIsotypicCuspFormAt_of_localSpaceAt15 below · depth 23 - Non-orthogonality of GL₃ cusp forms with equal Hecke eigenvalues
LanglandsTunnell.CubicInduction.exists_inner_toL2_translateRight_ne_zero_of_isCosetEigenfunction331 below · depth 23 - Smoothing and translation preserve level and Hecke eigenvalues at p
LanglandsTunnell.CubicInduction.isRightInvariant_and_isCosetEigenfunction_translateRight_smoothingOperator1 below · depth 23 - Smoothing a cuspidal GL₃ function yields a slab cusp function
LanglandsTunnell.CubicInduction.smoothingOperator_mem_cuspFunctions_of_isCuspidalAlong10 below · depth 23 - Local integrability of the Rankin–Selberg integrand at p
LanglandsTunnell.RankinSelberg.exists_forall_integrable_iotaGL_mul_of_mem_span_localSpaceAt_of_mem_gl3CyclicSubspace_twist_of_finiteFamily_arch40 below · depth 23 - Euler factorisation of the cut finite Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.exists_ne_zero_forall_rsFinIntegral_indicator_purified_eq_mul_sum_prod_rsLocalIntegral36 below · depth 23 - Hecke-matched GL₃ cusp forms non-orthogonal after right translation
LanglandsTunnell.CubicInduction.exists_inner_toL2_translateRight_ne_zero_of_isCosetEigenfunction_of_isCentreFinite311 below · depth 24 - Hecke-eigen cusp function inside an invariant L² subspace
LanglandsTunnell.CubicInduction.exists_mem_cuspFunctions_toL2_mem_and_isCosetEigenfunction_of_forall_inner_eq_zero30 below · depth 24 - Level sets of level data are compact open in GL₃(A_ℚ^f)
LanglandsTunnell.CubicInduction.isOpen_and_isCompact_setOf_forall_componentAt3_finEmbedN_mem0 below · depth 24 - Universal torus table for GL₃ Whittaker coefficients
LanglandsTunnell.CubicInduction.exists_forall_whittaker3_mul_iotaGL_zpow_eq_mul5 below · depth 25 - Non-orthogonal right translates of two cuspidal GL₃ forms
LanglandsTunnell.CubicInduction.exists_inner_toL2_translateRight_ne_zero_of_forall_whittakerBlock_one_mul_eq60 below · depth 25 - Full Whittaker integral as a factor Λ(σ)≥ 1 times its block
LanglandsTunnell.CubicInduction.exists_one_le_and_lintegral_quotientMeasure_eq_mul_whittakerBlock9 below · depth 25 - Bounded Whittaker block for a centre-finite cusp form on GL₃
LanglandsTunnell.CubicInduction.exists_sum_translate_ne_zero_and_whittakerBlock_le_of_isCentreFinite310 below · depth 25 - Non-zero limit of (σ-1)Λ(σ) and blocks at σ=1
LanglandsTunnell.CubicInduction.exists_tendsto_sub_one_mul_and_whittakerBlock_one_mul_eq_of_whittakerBlock_le1 below · depth 25 - Smoothing operators as archimedean convolutions; level sets near 1
LanglandsTunnell.CubicInduction.SlabL2.smoothingOperator_eq_archConvN_and_exists_levelSet_subset2 below · depth 26 - Right mathfrakgl₃-derivatives at infinity: smoothness, linearity, commutators, translation
LanglandsTunnell.CubicInduction.WhittakerBlock.isArchSmooth3_archDeriv_and_archDeriv_add_smul_comm_translate0 below · depth 26 - Vanishing of a Whittaker product on GL₃ over ℚ
LanglandsTunnell.CubicInduction.conj_whittaker3_mul_whittaker3_eq_zero_of_forall_integral_conj_mul_eq_zero58 below · depth 26 - Translate combination with non-zero Whittaker coefficient and bounded block
LanglandsTunnell.CubicInduction.exists_sum_translate_whittaker_ne_zero_and_whittakerBlock_empty_le_of_isCentreFinite309 below · depth 26 - Fibration of the GL₃ Whittaker block over bottom rows
LanglandsTunnell.CubicInduction.exists_whittakerBlock_one_eq_lintegral_and_eq_smul_map_withDensity_haar7 below · depth 26 - Reproducing identity at the infinite place on GL₃
LanglandsTunnell.CubicInduction.exists_contDiff_hasCompactSupport_eq_integral_archRealLift30 below · depth 27 - Uniform exponent θ₀>1/2 for ray decay of GL₃ Whittaker integrals
LanglandsTunnell.CubicInduction.exists_one_half_lt_forall_rayOrder_whittaker3_of_isCentreFinite_of_isRightInvariant298 below · depth 27 - Whittaker decay on the full diagonal torus from ray bounds
LanglandsTunnell.CubicInduction.norm_whittaker3_sum_translate_diag_le_of_forall_rayOrder20 below · depth 27 - Automorphy conditions pass to iterated archimedean derivatives
LanglandsTunnell.CubicInduction.conditions_foldr_archDeriv0 below · depth 28 - Continuity and uniform moderate growth of archimedean derivatives
LanglandsTunnell.CubicInduction.continuous_and_norm_iterate_archDeriv_sum_translate_le_of_isCentreFinite1 below · depth 28 - Simple-root derivatives of the GL₃ Whittaker coefficient at a diagonal point
LanglandsTunnell.CubicInduction.exists_ne_zero_forall_mul_whittaker3_diag_eq_whittaker3_archDeriv2 below · depth 28 - Uniform ray exponent >1/2 for GL₃ Whittaker derivative words
LanglandsTunnell.CubicInduction.exists_one_half_lt_forall_foldr_archDeriv_rayOrder_whittaker3_of_casimir_relations_of_isRightInvariant290 below · depth 28 - Right translation of archimedean derivative words on GL₃
LanglandsTunnell.CubicInduction.foldr_archDeriv_mul_right_eq_sum0 below · depth 28 - Uniform two-variable torus bound for GL₃ Whittaker coefficients
LanglandsTunnell.CubicInduction.norm_whittaker3_diag_le_of_isCentreFinite_of_forall_rayOrder12 below · depth 28 - Transport of the GL₃ cusp package under g↦(g^{mathsf T})⁻¹
LanglandsTunnell.CubicInduction.rayOrder_transport_transposeInv3_of_isCentreFinite_of_isRightInvariant16 below · depth 28 - Transport of automorphy conditions under g↦^tg⁻¹
LanglandsTunnell.CubicInduction.archPackage_comp_transposeInv3_of_isCentreFinite4 below · depth 29 - Linear central element acts by a scalar
LanglandsTunnell.CubicInduction.exists_casimir1_eq_smul_of_isArchSmooth30 below · depth 29 - Whittaker expansion on GL₃ from two Casimir relations
LanglandsTunnell.CubicInduction.exists_exponents_whittaker3_diag_expansion_of_casimir_relations7 below · depth 29 - Two-variable Whittaker decay on GL₃ from regular-singular systems
LanglandsTunnell.CubicInduction.exists_forall_isCompact_orth3_norm_whittaker3_le_of_systems2 below · depth 29 - Simple-pole bound for torus mean squares of GL₃ Whittaker coefficients
LanglandsTunnell.CubicInduction.exists_lintegral_torus_whittaker3_sq_le_div_sub_one_of_isCuspidalAlong_of_isRightInvariant121 below · depth 29 - Regular-singular diagonal systems for GL₃ Whittaker coefficients
LanglandsTunnell.CubicInduction.exists_words_whittaker3_diag_hasDerivAt_systems_of_casimir_relations_natDegree_le2 below · depth 29 - Vanishing of the logarithm-free coefficient at exponent of real part 1/2
LanglandsTunnell.CubicInduction.expCoeff_eq_zero_of_re_eq_one_half_of_mem_span_archDeriv_translate272 below · depth 29 - Whittaker bound on orthogonal compacta extends to all compacta
LanglandsTunnell.CubicInduction.forall_isCompact_norm_whittaker3_le_of_forall_isCompact_orth30 below · depth 29 - Derivative words of translates stay cuspidal along both parabolics
LanglandsTunnell.CubicInduction.isCuspidalAlong_foldr_archDeriv_sum_translate3 below · depth 29 - Finite-adelic invariance of derivative words of translate combinations
LanglandsTunnell.CubicInduction.isRightInvariant_foldr_archDeriv_sum_translate0 below · depth 29 - Transpose–inverse involution exchanges the two GL₃ Whittaker rays
LanglandsTunnell.CubicInduction.norm_whittaker3_archRealLift3_diag_mul_eq_norm_whittaker3_comp_transposeInv35 below · depth 29 - Uniform moderate-growth bound for the GL₃ Whittaker coefficient on the diagonal
LanglandsTunnell.CubicInduction.norm_whittaker3_archRealLift3_diag_mul_le_of_isCompact1 below · depth 29 - Uniform simple-pole bound for the adelic Epstein pairing on a slab
LanglandsTunnell.CubicInduction.AdelicEpstein.exists_forall_sub_one_mul_lintegral_nnnorm_sq_mul_epsteinPlus_le_of_decay9 below · depth 30 - Bounded test function on A_ℚ³ positive on a third-row window
LanglandsTunnell.CubicInduction.exists_measurable_bounded_compactArch_integral_pos_on_thirdRow_window1 below · depth 30 - Smoothing submodule carrying the leading Whittaker coefficient at exponent 1/2
LanglandsTunnell.CubicInduction.exists_smoothingSubmodule_leadingCoeff_form_of_expCoeff_re_eq_one_half_centreFinite_mg146 below · depth 30 - Vanishing leading coefficient, or transition-stable harmonic families
LanglandsTunnell.CubicInduction.leadingCoeff_eq_zero_or_exists_transitionStable_family_ne_bot_of_smoothingSubmodule_re136 below · depth 30 - Cuspidal moderate-growth functions on GL₃ are slab cusp functions
LanglandsTunnell.CubicInduction.mem_cuspFunctions_of_isCuspidalAlong_of_archDeriv_growth109 below · depth 30 - Rapid decay on Siegel sets for GL₃ cusp forms
LanglandsTunnell.CubicInduction.norm_mul_gauge3_pow_le_of_siegel_of_isCuspidalAlong_of_archDeriv_growth107 below · depth 30 - Whittaker expansions on GL₃ persist under right smoothing
LanglandsTunnell.CubicInduction.SlabL2.exists_expansion_whittaker3_smoothingOperator99 below · depth 31 - Left O(3)-finite smoothing kernels concentrating at the identity
LanglandsTunnell.CubicInduction.SlabL2.exists_isSmoothingKernel_leftOrthFinite_setIntegral_compl_le99 below · depth 31 - Mass-concentration approximate identity for right smoothing on GL₃(A_ℚ)
LanglandsTunnell.CubicInduction.SlabL2.exists_nhds_one_forall_norm_smoothingOperator_sub_le_of_setIntegral_compl_le0 below · depth 31 - Reverse-cyclic cubic equals C₃+C₁²-3C₂
LanglandsTunnell.CubicInduction.WhittakerBlock.sum_archDeriv_rev_eq_casimir3_add_casimir1_casimir1_sub_three_smul_casimir21 below · depth 31 - Borel equivariance of the top-logarithmic double Whittaker coefficient
LanglandsTunnell.CubicInduction.doubleSlotCoeff_upperTriangular_equivariant_of_joint_expansion_top3 below · depth 31 - Joint two-variable Whittaker expansion with leading-slice non-triviality
LanglandsTunnell.CubicInduction.exists_exponents_whittaker3_diag_joint_expansion_nontrivial_of_casimir_relations40 below · depth 31 - Unipotent displacement on a Siegel set in GL₃(A_ℚ)
LanglandsTunnell.CubicInduction.exists_forall_norm_sub_radical_mul_le_div_archRoot_of_archDeriv_le_of_siegel12 below · depth 31 - Uniform gauge bound on a Siegel set determinant slab
LanglandsTunnell.CubicInduction.exists_gauge3_le_mul_archRoot_mul_archRoot_sq_of_siegel_of_ideleNorm_det_mem_Icc10 below · depth 31 - Joint Casimir eigenvector with non-vanishing coefficient functional
LanglandsTunnell.CubicInduction.exists_joint_casimir_eigenvector_apply_ne_zero_of_positive_skew_form3 below · depth 31 - Derivative words inherit automorphy, cuspidality and a common level
LanglandsTunnell.CubicInduction.exists_level_forall_foldr_archDeriv_invariant_cuspidal_archSmooth100 below · depth 31 - Induced-picture package from a top-slot double leading Whittaker coefficient
LanglandsTunnell.CubicInduction.exists_submodule_inducedPicture_package_of_doubleSlotCoeff_top27 below · depth 31 - Transition-stable harmonic families from an induced-picture package
LanglandsTunnell.CubicInduction.exists_transitionStable_families_ne_bot_of_inducedPicture_package_top82 below · depth 31 - Oscillation bound for cuspidal functions on GL₃(A_ℚ)
LanglandsTunnell.CubicInduction.norm_le_of_isCuspidalAlong_of_arch_oscillation_le10 below · depth 31 - Regularity package for derivative words of centre-finite translates
LanglandsTunnell.CubicInduction.seed_package_of_mem_span_archDeriv_translate9 below · depth 31 - Monic Casimir relations on the GL₃ smoothing module
LanglandsTunnell.CubicInduction.smoothingModule_casimir_relations111 below · depth 31 - Smoothing module on GL₃: leading-coefficient functional and its properties
LanglandsTunnell.CubicInduction.smoothingModule_expansion_leadingCoeff118 below · depth 31 - Orthogonal finiteness and derivative stability of the smoothing module
LanglandsTunnell.CubicInduction.smoothingModule_orthFinite_and_archDeriv_mem117 below · depth 31 - Regularity and gauge growth in the GL₃ smoothing module
LanglandsTunnell.CubicInduction.smoothingModule_regularity_and_growth116 below · depth 31 - The slab form on the GL₃ smoothing module
LanglandsTunnell.CubicInduction.smoothingModule_slabForm139 below · depth 31 - Archimedean derivatives of smoothed coefficients on GL₃(A_ℚ)
LanglandsTunnell.CubicInduction.SlabL2.hasDerivAt_integral_mul_comp_archRealLift3_smoothingKernel5 below · depth 32 - Skew-adjointness of archimedean derivatives on the slab
LanglandsTunnell.CubicInduction.SlabL2.integral_archDeriv_smoothingOperator_mul_conj_eq_neg122 below · depth 32 - Left orthogonal finiteness passes to archimedean derivative kernels
LanglandsTunnell.CubicInduction.SlabL2.leftOrthFinite_archDerivKernel99 below · depth 32 - Mean-value bound along a square-zero direction in GL₃(A_ℚ)
LanglandsTunnell.CubicInduction.WhittakerBlock.norm_sub_le_sum_abs_mul_of_mul_self_eq_zero_of_archDeriv_le0 below · depth 32 - Square-zero conjugate of a radical element past a Siegel point
LanglandsTunnell.CubicInduction.conj_radical_sub_one_mul_self_eq_zero_and_norm_le_div_archRoot_of_siegel10 below · depth 32 - No non-zero linear form is read in the split sign class
LanglandsTunnell.CubicInduction.eq_zero_of_isHomogeneous_one_of_read_signIsotypic_linear_of_inducedPicture_package47 below · depth 32 - Vanishing of degree-zero reads in a constant sign class
LanglandsTunnell.CubicInduction.eq_zero_of_isHomogeneous_zero_of_read_signIsotypic_const_of_inducedPicture_package47 below · depth 32 - Archimedean splitting of GL₃ of the adeles of ℚ
LanglandsTunnell.CubicInduction.exists_eq_archRealLift3_mul_of_archComponent3_eq_one0 below · depth 32 - Joint two-variable expansion of a GL₃ Whittaker coefficient
LanglandsTunnell.CubicInduction.exists_exponents_whittaker3_diag_joint_expansion_of_casimir_relations15 below · depth 32 - Existence of a congruence level for a smooth adelic function
LanglandsTunnell.CubicInduction.exists_level_forall_mul_finEmbedN_eq_of_isRightInvariant_of_isOpen99 below · depth 32 - Sign-isotypic splitting of a B⁺-equivariant adelic function space
LanglandsTunnell.CubicInduction.exists_signIsotypic_submodules_of_upperTriangular_equivariant_of_orthogonalRightStable0 below · depth 32 - Vanishing of a leading first-ratio Whittaker coefficient on GL₃
LanglandsTunnell.CubicInduction.exists_threshold_firstRatioCoeff_eq_zero_of_forall_secondRatioCoeff_eq_zero_of_casimir_relations34 below · depth 32 - Threshold vanishing of second-ratio Whittaker coefficients on GL₃
LanglandsTunnell.CubicInduction.exists_threshold_secondRatioCoeff_eq_zero_of_forall_firstRatioCoeff_eq_zero_of_casimir_relations34 below · depth 32 - Transition-stable family of harmonic polynomials read on O(3)
LanglandsTunnell.CubicInduction.exists_transitionStable_family_of_signIsotypic_submodule19 below · depth 32 - Odd sign classes: vanishing of sign-isotypic leading coefficients
LanglandsTunnell.CubicInduction.forall_apply_orthogonal_eq_zero_of_signIsotypic_odd_of_inducedPicture_package71 below · depth 32 - Double-slot coefficients intertwine the archimedean flow derivative
LanglandsTunnell.CubicInduction.hasDerivAt_doubleSlotCoeff_archFlow_of_joint_expansion_archDeriv12 below · depth 32 - Archimedean smoothness from Iwasawa equivariance and orthogonal finiteness
LanglandsTunnell.CubicInduction.isArchSmooth3_of_continuous_of_upperTriangular_equivariant_of_orthogonalFinite4 below · depth 32 - Vanishing Whittaker integral kills all joint-expansion coefficients
LanglandsTunnell.CubicInduction.joint_expansion_coeff_eq_zero_of_forall_whittaker3_diag_mul_eq_zero1 below · depth 32
… and 35 more statements (search for the module name to find them).