Definitions/Def_LocalNewvector_PrincipalSeriesCarrier.lean
Principal series of GL₂(ℚ_p): function model and carrier
Fix a prime p and write G=\mathrm{GL}_2(\mathbb{Q}_p). For units a_1,a_2\in\mathbb{Q}_p^\times and x\in\mathbb{Q}_p, borelElem p a₁ a₂ x is the upper triangular element \begin{pmatrix} a_1 & x\\ 0 & a_2\end{pmatrix} of G, given together with its explicit inverse; the accompanying lemmas record the product rule (a_1,a_2,x)\cdot(b_1,b_2,y)=(a_1b_1,a_2b_2,a_1y+xb_2), the inverse, and that (1,1,0) is the identity. halfModulus p a₁ a₂ is the complex number \sqrt{\lVert a_1\rVert/\lVert a_2\rVert}, obtained from the real square root of the ratio of p-adic norms; it depends only on the two norms, equals 1 when both are 1, and is multiplicative in (a_1,a_2).
Given monoid homomorphisms \mu_1,\mu_2:\mathbb{Q}_p^\times\to\mathbb{C}^\times, principalSeries p μ₁ μ₂ is the \mathbb{C}-submodule of all functions f:G\to\mathbb{C} that are locally constant and satisfy f(b\,g)=\mu_1(a_1)\mu_2(a_2)\sqrt{\lVert a_1\rVert/\lVert a_2\rVert}\,f(g) for every Borel element b= borelElem p a₁ a₂ x and every g\in G: a concrete model of the normalised induced representation, with no further support or growth condition. Membership is characterised, and the space is stable under right translation f\mapsto f(\cdot\,g). For a subgroup U\le G, rightInvariantFunctions p U is the submodule of f with f(xu)=f(x) for all u\in U, x\in G (local constancy is not required here).
PSCarrier p μ₁ μ₂ is the underlying type of principalSeries p μ₁ μ₂, equipped with its complex vector space structure and with the G-action (g\bullet f)(y)=f(yg), commuting with scalars, plus a small interface (mk, toSub, toFn, ext, toSubEquiv). Finally PSCarrier.fixedEquiv U is the \mathbb{C}-linear isomorphism between fixedSubmodule U (PSCarrier p μ₁ μ₂), the vectors fixed by every element of U, and the intersection principalSeries p μ₁ μ₂ ⊓ rightInvariantFunctions p U inside the function space, and finrank_fixed_eq transports complex dimensions across it.
Relation to Mathlib
Local constancy is Mathlib's IsLocallyConstant; Mathlib has no principal series or normalised induction for p-adic groups, so the function-space model, its carrier type and the fixed-space identification are the project's own.
Where it is used
These definitions give the working model of the principal series of \mathrm{GL}_2(\mathbb{Q}_p) used in the project's local newvector theory, where conductors are defined through the fixed spaces of the congruence subgroups K_1(p^n); fixedEquiv and finrank_fixed_eq let such fixed spaces be computed inside the space of functions on the group.
References
- H. Jacquet and R. P. Langlands, Automorphic Forms on GL(2), Lecture Notes in Mathematics 114, Springer, 1970
- W. Casselman, On some results of Atkin and Lehner, Mathematische Annalen 201 (1973), 301–314
References are suggested automatically and have not been individually verified.
English text generated automatically from the Lean source; the Lean statement is authoritative.
- 256 lines
- 33 declarations
- used in the statements of 48 theorems and imported by 55 proofs
- imports 1 definition modules
Source file: Definitions/Def_LocalNewvector_PrincipalSeriesCarrier.lean
Imported by
- no other definition module
Declarations
- def
LocalNewvector.borelElem - lemma
LocalNewvector.coe_borelElem - lemma
LocalNewvector.coe_borelElem_inv - theorem
LocalNewvector.borelElem_mul - theorem
LocalNewvector.borelElem_inv - theorem
LocalNewvector.borelElem_one - def
LocalNewvector.halfModulus - theorem
LocalNewvector.halfModulus_eq_one_of_norm_eq_one - theorem
LocalNewvector.halfModulus_one - theorem
LocalNewvector.halfModulus_congr - theorem
LocalNewvector.halfModulus_mul - def
LocalNewvector.principalSeries - theorem
LocalNewvector.mem_principalSeries_iff - theorem
LocalNewvector.isLocallyConstant_of_mem_principalSeries - theorem
LocalNewvector.apply_borelElem_mul_of_mem_principalSeries - theorem
LocalNewvector.rightTranslate_mem_principalSeries - def
LocalNewvector.rightInvariantFunctions - theorem
LocalNewvector.mem_rightInvariantFunctions_iff - def
LocalNewvector.PSCarrier - def
LocalNewvector.PSCarrier.mk - def
LocalNewvector.PSCarrier.toSub - def
LocalNewvector.PSCarrier.toFn - theorem
LocalNewvector.PSCarrier.toFn_mem - theorem
LocalNewvector.PSCarrier.ext - def
LocalNewvector.PSCarrier.toSubEquiv - theorem
LocalNewvector.PSCarrier.toFn_smul - theorem
LocalNewvector.PSCarrier.toFn_csmul - def
LocalNewvector.PSCarrier.fixedEquiv - theorem
LocalNewvector.PSCarrier.finrank_fixed_eq
Source
import Definitions.Def_LocalNewvector_ConductorDatum set_option autoImplicit false noncomputable section namespace LocalNewvector variable (p : ℕ) [Fact p.Prime] section BorelElements def borelElem (a₁ a₂ : ℚ_[p]ˣ) (x : ℚ_[p]) : GL (Fin 2) ℚ_[p] := ⟨!![(a₁ : ℚ_[p]), x; 0, (a₂ : ℚ_[p])], !![((a₁⁻¹ : ℚ_[p]ˣ) : ℚ_[p]), -(((a₁⁻¹ : ℚ_[p]ˣ) : ℚ_[p]) * x * ((a₂⁻¹ : ℚ_[p]ˣ) : ℚ_[p])); 0, ((a₂⁻¹ : ℚ_[p]ˣ) : ℚ_[p])], by have h1 : (a₁ : ℚ_[p]) ≠ 0 := a₁.ne_zero have h2 : (a₂ : ℚ_[p]) ≠ 0 := a₂.ne_zero ext i j fin_cases i <;> fin_cases j <;> simp [Matrix.mul_apply, Fin.sum_univ_two, Units.val_inv_eq_inv_val, mul_assoc, h1, h2], by have h1 : (a₁ : ℚ_[p]) ≠ 0 := a₁.ne_zero have h2 : (a₂ : ℚ_[p]) ≠ 0 := a₂.ne_zero ext i j fin_cases i <;> fin_cases j <;> simp [Matrix.mul_apply, Fin.sum_univ_two, Units.val_inv_eq_inv_val, mul_assoc, h1, h2]⟩ @[simp] lemma coe_borelElem (a₁ a₂ : ℚ_[p]ˣ) (x : ℚ_[p]) : (borelElem p a₁ a₂ x : Matrix (Fin 2) (Fin 2) ℚ_[p]) = !![(a₁ : ℚ_[p]), x; 0, (a₂ : ℚ_[p])] := rfl @[simp] lemma coe_borelElem_inv (a₁ a₂ : ℚ_[p]ˣ) (x : ℚ_[p]) : (((borelElem p a₁ a₂ x)⁻¹ : GL (Fin 2) ℚ_[p]) : Matrix (Fin 2) (Fin 2) ℚ_[p]) = !![((a₁⁻¹ : ℚ_[p]ˣ) : ℚ_[p]), -(((a₁⁻¹ : ℚ_[p]ˣ) : ℚ_[p]) * x * ((a₂⁻¹ : ℚ_[p]ˣ) : ℚ_[p])); 0, ((a₂⁻¹ : ℚ_[p]ˣ) : ℚ_[p])] := rfl theorem borelElem_mul (a₁ a₂ b₁ b₂ : ℚ_[p]ˣ) (x y : ℚ_[p]) : borelElem p a₁ a₂ x * borelElem p b₁ b₂ y = borelElem p (a₁ * b₁) (a₂ * b₂) ((a₁ : ℚ_[p]) * y + x * (b₂ : ℚ_[p])) := by apply Units.ext show (borelElem p a₁ a₂ x : Matrix (Fin 2) (Fin 2) ℚ_[p]) * (borelElem p b₁ b₂ y : Matrix (Fin 2) (Fin 2) ℚ_[p]) = _ ext i j fin_cases i <;> fin_cases j <;> simp [Matrix.mul_apply, Fin.sum_univ_two] theorem borelElem_inv (a₁ a₂ : ℚ_[p]ˣ) (x : ℚ_[p]) : (borelElem p a₁ a₂ x)⁻¹ = borelElem p a₁⁻¹ a₂⁻¹ (-(((a₁⁻¹ : ℚ_[p]ˣ) : ℚ_[p]) * x * ((a₂⁻¹ : ℚ_[p]ˣ) : ℚ_[p]))) := Units.ext rfl @[simp] theorem borelElem_one : borelElem p 1 1 0 = 1 := by apply Units.ext show (borelElem p 1 1 0 : Matrix (Fin 2) (Fin 2) ℚ_[p]) = 1 ext i j fin_cases i <;> fin_cases j <;> simp end BorelElements section HalfModulus def halfModulus (a₁ a₂ : ℚ_[p]ˣ) : ℂ := (Real.sqrt (‖(a₁ : ℚ_[p])‖ / ‖(a₂ : ℚ_[p])‖) : ℝ) theorem halfModulus_eq_one_of_norm_eq_one {a₁ a₂ : ℚ_[p]ˣ} (h₁ : ‖(a₁ : ℚ_[p])‖ = 1) (h₂ : ‖(a₂ : ℚ_[p])‖ = 1) : halfModulus p a₁ a₂ = 1 := by simp only [halfModulus, h₁, h₂, div_one, Real.sqrt_one, Complex.ofReal_one] @[simp] theorem halfModulus_one : halfModulus p 1 1 = 1 := halfModulus_eq_one_of_norm_eq_one p (by simp) (by simp) theorem halfModulus_congr {a₁ a₂ b₁ b₂ : ℚ_[p]ˣ} (h₁ : ‖(a₁ : ℚ_[p])‖ = ‖(b₁ : ℚ_[p])‖) (h₂ : ‖(a₂ : ℚ_[p])‖ = ‖(b₂ : ℚ_[p])‖) : halfModulus p a₁ a₂ = halfModulus p b₁ b₂ := by simp only [halfModulus, h₁, h₂] theorem halfModulus_mul (a₁ a₂ b₁ b₂ : ℚ_[p]ˣ) : halfModulus p (a₁ * b₁) (a₂ * b₂) = halfModulus p a₁ a₂ * halfModulus p b₁ b₂ := by have hquot : ‖((a₁ * b₁ : ℚ_[p]ˣ) : ℚ_[p])‖ / ‖((a₂ * b₂ : ℚ_[p]ˣ) : ℚ_[p])‖ = (‖(a₁ : ℚ_[p])‖ / ‖(a₂ : ℚ_[p])‖) * (‖(b₁ : ℚ_[p])‖ / ‖(b₂ : ℚ_[p])‖) := by rw [Units.val_mul, Units.val_mul, norm_mul, norm_mul, div_mul_div_comm] simp only [halfModulus, hquot] rw [Real.sqrt_mul (by positivity), Complex.ofReal_mul] end HalfModulus section PrincipalSeries def principalSeries (μ₁ μ₂ : ℚ_[p]ˣ →* ℂˣ) : Submodule ℂ (GL (Fin 2) ℚ_[p] → ℂ) where carrier := {f | IsLocallyConstant f ∧ ∀ (a₁ a₂ : ℚ_[p]ˣ) (x : ℚ_[p]) (g : GL (Fin 2) ℚ_[p]), f (borelElem p a₁ a₂ x * g) = (μ₁ a₁ : ℂ) * (μ₂ a₂ : ℂ) * halfModulus p a₁ a₂ * f g} zero_mem' := ⟨IsLocallyConstant.const 0, fun a₁ a₂ x g => by simp⟩ add_mem' := by intro f g hf hg obtain ⟨hf_lc, hf_tr⟩ := hf obtain ⟨hg_lc, hg_tr⟩ := hg refine ⟨hf_lc.comp₂ hg_lc (· + ·), fun a₁ a₂ x g₀ => ?_⟩ show f _ + g _ = _ * (f g₀ + g g₀) rw [hf_tr, hg_tr] ring smul_mem' := by intro c f hf obtain ⟨hf_lc, hf_tr⟩ := hf refine ⟨hf_lc.comp (c * ·), fun a₁ a₂ x g₀ => ?_⟩ show c * f _ = _ * (c * f g₀) rw [hf_tr] ring theorem mem_principalSeries_iff {μ₁ μ₂ : ℚ_[p]ˣ →* ℂˣ} {f : GL (Fin 2) ℚ_[p] → ℂ} : f ∈ principalSeries p μ₁ μ₂ ↔ IsLocallyConstant f ∧ ∀ (a₁ a₂ : ℚ_[p]ˣ) (x : ℚ_[p]) (g : GL (Fin 2) ℚ_[p]), f (borelElem p a₁ a₂ x * g) = (μ₁ a₁ : ℂ) * (μ₂ a₂ : ℂ) * halfModulus p a₁ a₂ * f g := Iff.rfl theorem isLocallyConstant_of_mem_principalSeries {μ₁ μ₂ : ℚ_[p]ˣ →* ℂˣ} {f : GL (Fin 2) ℚ_[p] → ℂ} (hf : f ∈ principalSeries p μ₁ μ₂) : IsLocallyConstant f := ((mem_principalSeries_iff p).mp hf).1 theorem apply_borelElem_mul_of_mem_principalSeries {μ₁ μ₂ : ℚ_[p]ˣ →* ℂˣ} {f : GL (Fin 2) ℚ_[p] → ℂ} (hf : f ∈ principalSeries p μ₁ μ₂) (a₁ a₂ : ℚ_[p]ˣ) (x : ℚ_[p]) (g : GL (Fin 2) ℚ_[p]) : f (borelElem p a₁ a₂ x * g) = (μ₁ a₁ : ℂ) * (μ₂ a₂ : ℂ) * halfModulus p a₁ a₂ * f g := ((mem_principalSeries_iff p).mp hf).2 a₁ a₂ x g theorem rightTranslate_mem_principalSeries {μ₁ μ₂ : ℚ_[p]ˣ →* ℂˣ} {f : GL (Fin 2) ℚ_[p] → ℂ} (hf : f ∈ principalSeries p μ₁ μ₂) (g : GL (Fin 2) ℚ_[p]) : (fun y => f (y * g)) ∈ principalSeries p μ₁ μ₂ := by obtain ⟨hlc, htr⟩ := (mem_principalSeries_iff p).mp hf refine (mem_principalSeries_iff p).mpr ⟨hlc.comp_continuous (continuous_id.mul continuous_const), fun a₁ a₂ x g₀ => ?_⟩ show f (borelElem p a₁ a₂ x * g₀ * g) = _ * f (g₀ * g) rw [mul_assoc, htr] end PrincipalSeries section RightInvariant def rightInvariantFunctions (U : Subgroup (GL (Fin 2) ℚ_[p])) : Submodule ℂ (GL (Fin 2) ℚ_[p] → ℂ) where carrier := {f | ∀ u ∈ U, ∀ x, f (x * u) = f x} zero_mem' := fun _ _ _ => rfl add_mem' := by intro f g hf hg u hu x show f (x * u) + g (x * u) = f x + g x rw [hf u hu x, hg u hu x] smul_mem' := by intro c f hf u hu x show c * f (x * u) = c * f x rw [hf u hu x] theorem mem_rightInvariantFunctions_iff {U : Subgroup (GL (Fin 2) ℚ_[p])} {f : GL (Fin 2) ℚ_[p] → ℂ} : f ∈ rightInvariantFunctions p U ↔ ∀ u ∈ U, ∀ x, f (x * u) = f x := Iff.rfl end RightInvariant section PrincipalSeriesCarrier variable (p : ℕ) [Fact p.Prime] (μ₁ μ₂ : ℚ_[p]ˣ →* ℂˣ) def PSCarrier : Type := ↥(principalSeries p μ₁ μ₂) namespace PSCarrier def mk (f : ↥(principalSeries p μ₁ μ₂)) : PSCarrier p μ₁ μ₂ := f def toSub (f : PSCarrier p μ₁ μ₂) : ↥(principalSeries p μ₁ μ₂) := f def toFn (f : PSCarrier p μ₁ μ₂) : GL (Fin 2) ℚ_[p] → ℂ := (toSub p μ₁ μ₂ f : GL (Fin 2) ℚ_[p] → ℂ) theorem toFn_mem (f : PSCarrier p μ₁ μ₂) : toFn p μ₁ μ₂ f ∈ principalSeries p μ₁ μ₂ := (toSub p μ₁ μ₂ f).property theorem ext {f g : PSCarrier p μ₁ μ₂} (h : ∀ y, toFn p μ₁ μ₂ f y = toFn p μ₁ μ₂ g y) : f = g := Subtype.ext (funext h) instance : AddCommGroup (PSCarrier p μ₁ μ₂) := inferInstanceAs (AddCommGroup ↥(principalSeries p μ₁ μ₂)) instance : Module ℂ (PSCarrier p μ₁ μ₂) := inferInstanceAs (Module ℂ ↥(principalSeries p μ₁ μ₂)) def toSubEquiv : PSCarrier p μ₁ μ₂ ≃ₗ[ℂ] ↥(principalSeries p μ₁ μ₂) where toFun := toSub p μ₁ μ₂ map_add' _ _ := rfl map_smul' _ _ := rfl invFun := mk p μ₁ μ₂ left_inv _ := rfl right_inv _ := rfl instance : DistribMulAction (GL (Fin 2) ℚ_[p]) (PSCarrier p μ₁ μ₂) where smul g f := mk p μ₁ μ₂ ⟨fun y => toFn p μ₁ μ₂ f (y * g), rightTranslate_mem_principalSeries p (toFn_mem p μ₁ μ₂ f) g⟩ one_smul f := ext p μ₁ μ₂ fun y => congrArg (toFn p μ₁ μ₂ f) (mul_one y) mul_smul g h f := ext p μ₁ μ₂ fun y => congrArg (toFn p μ₁ μ₂ f) (mul_assoc y g h).symm smul_zero _ := ext p μ₁ μ₂ fun _ => rfl smul_add _ _ _ := ext p μ₁ μ₂ fun _ => rfl @[simp] theorem toFn_smul (g : GL (Fin 2) ℚ_[p]) (f : PSCarrier p μ₁ μ₂) (y : GL (Fin 2) ℚ_[p]) : toFn p μ₁ μ₂ (g • f) y = toFn p μ₁ μ₂ f (y * g) := rfl @[simp] theorem toFn_csmul (c : ℂ) (f : PSCarrier p μ₁ μ₂) (y : GL (Fin 2) ℚ_[p]) : toFn p μ₁ μ₂ (c • f) y = c * toFn p μ₁ μ₂ f y := rfl instance : SMulCommClass (GL (Fin 2) ℚ_[p]) ℂ (PSCarrier p μ₁ μ₂) where smul_comm _ _ _ := ext p μ₁ μ₂ fun _ => rfl def fixedEquiv (U : Subgroup (GL (Fin 2) ℚ_[p])) : ↥(LocalNewvector.fixedSubmodule U (PSCarrier p μ₁ μ₂)) ≃ₗ[ℂ] ↥(principalSeries p μ₁ μ₂ ⊓ rightInvariantFunctions p U) where toFun v := ⟨toFn p μ₁ μ₂ v.val, Submodule.mem_inf.mpr ⟨toFn_mem p μ₁ μ₂ v.val, by rw [mem_rightInvariantFunctions_iff] intro u hu y exact congrArg (fun z => toFn p μ₁ μ₂ z y) ((LocalNewvector.mem_fixedSubmodule_iff.mp v.property) u hu)⟩⟩ map_add' _ _ := Subtype.ext rfl map_smul' _ _ := Subtype.ext rfl invFun w := ⟨mk p μ₁ μ₂ ⟨w.val, (Submodule.mem_inf.mp w.property).1⟩, by rw [LocalNewvector.mem_fixedSubmodule_iff] intro u hu refine ext p μ₁ μ₂ fun y => ?_ exact (mem_rightInvariantFunctions_iff p).mp (Submodule.mem_inf.mp w.property).2 u hu y⟩ left_inv _ := Subtype.ext (Subtype.ext rfl) right_inv _ := Subtype.ext rfl theorem finrank_fixed_eq (U : Subgroup (GL (Fin 2) ℚ_[p])) : Module.finrank ℂ ↥(LocalNewvector.fixedSubmodule U (PSCarrier p μ₁ μ₂)) = Module.finrank ℂ ↥(principalSeries p μ₁ μ₂ ⊓ rightInvariantFunctions p U) := (fixedEquiv p μ₁ μ₂ U).finrank_eq end PSCarrier end PrincipalSeriesCarrier end LocalNewvector end
Statements phrased using this module (48)
- Inertia at q with q² ‖ M: principal series versus supercuspidal
CuspForm.IsNewform.exists_charpoly_inertia_eq_principalSeries_supercuspidal_of_galoisRepAdic_of_two_laws_of_irreducible_odd_of_ne_two_of_factorization_eq_two10,725 below · depth 11 - Ramified first character in a principal series at q² ∣ M
CuspForm.IsNewform.exists_mem_higherUnits_apply_ne_one_of_linearMap_psCarrier_ne_zero_of_sq_dvd57 below · depth 11 - Unramifiedness of the central character μ₁μ₂
CuspForm.IsAdelicLiftOf.isUnramified_mul_of_linearMap_psCarrier_ne_zero6 below · depth 12 - Inertia at a principal-series prime q with v_q(M)=2
CuspForm.IsNewform.exists_charpoly_inertia_eq_and_pow_eq_one_iff_of_linearMap_psCarrier_ne_zero_of_factorization_eq_two7,035 below · depth 12 - Inertia at q is split with a^{q-1}≠ 1
CuspForm.IsNewform.exists_charpoly_inertia_eq_and_pow_sub_one_ne_one_of_forall_linearMap_psCarrier_eq_zero_of_factorization_eq_two_of_irreducible_odd_of_ne_two6,863 below · depth 12 - Newvector with Iwahori values 1 and -p⁻¹
LocalNewvector.PSCarrier.existsUnique_mem_inf_fixedSubmodule_padicK1_one_of_stable5 below · depth 12 - Dimension of K₁(p^m)-fixed vectors in principal series
LocalNewvector.PSCarrier.finrank_fixedSubmodule_padicK13 below · depth 12 - Spherical vectors lie in every nonzero stable subspace
LocalNewvector.PSCarrier.fixedSubmodule_padicK1_zero_le_of_stable4 below · depth 12 - Irreducibility of unramified principal series for GL₂(ℚₚ)
LocalNewvector.PSCarrier.isIrreducibleGLRep_of_isUnramified0 below · depth 12 - Lifting a K₁(qᵃ)-fixed vector through an equivariant map
LocalNewvector.exists_mem_fixedSubmodule_and_map_eq_of_map_mem_fixedSubmodule0 below · depth 12 - Twisting a ramified-ratio principal series to K₁(qᵇ)-fixed vectors
CuspForm.IsAdelicLiftOf.exists_mem_span_fnTwist_fixed_padicK1_of_principalSeries_of_not_isUnramified_ratio11 below · depth 13 - Inertia at q≠λ: principal series with unramified ratio
CuspForm.IsNewform.exists_charpoly_inertia_eq_and_pow_eq_one_iff_of_linearMap_psCarrier_ne_zero_of_isUnramified_ratio3,781 below · depth 13 - Inertial charpolys at a ramified principal-series prime, v_q(M)=2
CuspForm.IsNewform.exists_galoisRepAdic_charpoly_inertia_eq_cyclotomicCharacter_of_linearMap_psCarrier_ne_zero_of_not_isUnramified_ratio_of_factorization_eq_two6,229 below · depth 13 - Principal-series map from split tame inertia labels at q
CuspForm.IsNewform.exists_linearMap_psCarrier_ne_zero_of_charpoly_inertia_eq_of_pow_sub_one_eq_one_of_factorization_eq_two_of_irreducible_odd_of_ne_two6,836 below · depth 13 - Local type at a prime exactly squared in the level
CuspForm.IsNewform.psCarrier_lam_dvd_sub_one_or_no_psCarrier_lam_dvd_add_one_of_factorization_eq_two_of_residual_isUnipotent_of_irreducible_odd_of_absIrred_odd10,753 below · depth 13 - Oldform dimension count for a principal series
LocalNewvector.PSCarrier.finrank_fixedSubmodule_padicK1_of_add_le1 below · depth 13 - Casselman's conductor formula for the principal series
LocalNewvector.PSCarrier.hasNewvectorConductor_add1 below · depth 13 - Irreducibility of the principal series of GL₂(ℚₚ)
LocalNewvector.PSCarrier.isIrreducibleGLRep_of_hasCharConductor_of_ratio0 below · depth 13 - Level lowering at q with q² ∥ L, q≡-1, supercuspidal case
WeierstrassCurve.exists_isNormalizedEigenform_level_div_of_forall_linearMap_psCarrier_eq_zero_of_cast_eq_neg_one10,757 below · depth 13 - Both characters ramified at q forces q² ∣ M
CuspForm.IsAdelicLiftOf.sq_dvd_of_linearMap_psCarrier_ne_zero_of_not_isUnramified_of_not_isUnramified1 below · depth 14 - Ramified principal series at q with v_q(M)=2: twist of level exactly q
CuspForm.IsNewform.exists_isPrimitiveForm_adelicLiftGamma1_psCarrier_isUnramified_of_not_isUnramified_ratio_of_factorization_eq_two473 below · depth 14 - Quadratic twist lowering the q-exponent of a newform
CuspForm.IsNewform.exists_quadraticTwistToExponentOne_of_sq_dvd_of_adelicLift_principalSeries_isUnramified_ratio67 below · depth 14 - Depth zero at q when v_q(M)≤ 2
CuspForm.IsNewform.fixedSubmodule_gl2CongruenceSubgroup_one_adelicSpan_ne_bot_of_factorization_le_two47 below · depth 14 - Unipotent-fixed vectors vanish when no map to a principal series exists
CuspForm.IsNewform.gl2ReductionRep_unipotent_fixed_eq_zero_of_forall_linearMap_psCarrier_eq_zero16 below · depth 14 - Nonzero inertia invariants at q when v_q(M)=1
CuspForm.IsPrimitiveForm.exists_ne_zero_forall_inertiaSubgroupIn_apply_eq_self_of_linearMap_psCarrier_isUnramified_of_factorization_eq_one5,713 below · depth 14 - Characters of a nonzero principal series are smooth
LocalNewvector.PSCarrier.exists_forall_mem_higherUnits_apply_eq_one_of_ne_zero0 below · depth 14 - Integral mod-p parabolic eigenclass at level L/q
WeierstrassCurve.exists_H1_parabolic_not_dvd_diamondRaw_heckeT_congr_apOfModel_level_div_of_forall_linearMap_psCarrier_eq_zero10,743 below · depth 14 - Quadratic twist produces a K₁(q)-fixed vector with trivial central action
CuspForm.IsAdelicLiftOf.exists_mem_span_fnTwist_fixed_padicK1_one_of_principalSeries15 below · depth 15 - Principal-series characters trivial on 1+qℤ_q when v_q(M)=2
CuspForm.IsNewform.apply_eq_one_of_mem_higherUnits_one_of_factorization_eq_two_of_linearMap_psCarrier_ne_zero10 below · depth 15 - Twisting a newform to unramified principal-series character at q
CuspForm.IsNewform.exists_isPrimitiveForm_adelicLiftGamma1_psCarrier_isUnramified_of_not_isUnramified_ratio457 below · depth 15 - Unipotent-fixed vector gives a map to a principal series
CuspForm.IsNewform.exists_linearMap_psCarrier_of_gl2ReductionRep_unipotent_fixed_ne_zero15 below · depth 15 - Inertia invariants at q for v_q(M)=1, unramified principal series
CuspForm.IsPrimitiveForm.exists_galoisRepAdic_forall_inertiaSubgroupIn_apply_eq_self_of_linearMap_psCarrier_isUnramified_of_factorization_eq_one5,712 below · depth 15 - Principal series with unramified character: v_q(M) versus v_q(cond ε)
CuspForm.IsPrimitiveForm.factorization_eq_conductor_factorization_or_of_linearMap_psCarrier_isUnramified33 below · depth 15 - Ramified principal series has no GL₂(ℤₚ)-fixed vector
LocalNewvector.PSCarrier.fixedSubmodule_padicK1_zero_eq_bot0 below · depth 15 - Mod p eigensystem of W on H¹ with Steinberg-quotient coefficients
WeierstrassCurve.exists_charP_rep_steinberg_quotient_isEigensystemH1_apOfModel_of_isSemistableModel_of_qCoeff_congr10,659 below · depth 15 - Twisting away ramification of μ₁ in a principal series
LocalNewvector.AdelicSpan.exists_psCarrier_fnTwist_isUnramified_fixed_padicK1_of_not_isUnramified_ratio7 below · depth 16 - Invariant subspaces of the principal series B(μ₁,μ₁|·|)
LocalNewvector.PSCarrier.exists_forall_stable_iff_of_hasCharConductor_of_ratio_eq_natCast3 below · depth 16 - Casselman's level count for the special subrepresentation at K₁(p^m)
LocalNewvector.PSCarrier.finrank_inf_fixedSubmodule_padicK1_of_stable5 below · depth 16 - Level lowering at q² with Steinberg-quotient coefficients
WeierstrassCurve.isEigensystemH1_comp_apOfModel_of_isSemistableModel_of_qCoeff_congr_of_steinberg_quotient10,658 below · depth 16 - Inertia at q with v_q(M)=2 is non-tame of order ∤ q-1
CuspForm.IsNewform.exists_charpoly_inertia_eq_and_pow_sub_one_ne_one_of_forall_linearMap_psCarrier_eq_zero_of_factorization_eq_two_of_irreducible_odd_of_ne_two_of_cast_eq_neg_one6,598 below · depth 17 - Smooth B-invariant functions generated by one non-constant vector
LocalNewvector.mem_of_isLocallyConstant_of_borelInvariant_of_rightTranslate_stable2 below · depth 17 - Residual irreducibility, oddness and inertial unipotence for a congruent newform
WeierstrassCurve.exists_galoisRepAdic_residual_irreducible_odd_unipotent_of_isSemistableModel_of_qCoeff_congr1,487 below · depth 17 - Principal series map from tame split inertia at q
CuspForm.IsNewform.exists_linearMap_psCarrier_ne_zero_of_charpoly_inertia_eq_of_pow_sub_one_eq_one_of_factorization_eq_two_of_irreducible_odd_of_ne_two_of_cast_eq_neg_one6,571 below · depth 18 - Irreducibility of the K(q)-fixed reduction representation
CuspForm.IsNewform.gl2ReductionRep_toSubmodule_eq_top_of_ne_bot_of_forall_linearMap_psCarrier_eq_zero533 below · depth 18 - No equivariant map to a principal series at q when q² ‖ M
CuspForm.IsNewform.linearMap_psCarrier_eq_zero_of_charpoly_inertia_eq_mul_of_eq_pow_of_pow_sub_one_ne_one_exponent_two7,036 below · depth 18 - Indicator of B· K(p^M) lies in a translation-stable space
LocalNewvector.indicator_borelCell_mem_of_integralBorelInvariant_of_rightTranslate_stable0 below · depth 18 - Irreducibility of the local representation realised in the adelic span
CuspForm.IsNewform.isIrreducibleGLRep_of_linearMap_range_eq_span_padic_smul_self496 below · depth 19 - Admissibility of the principal series B(μ₁,μ₂)
LocalNewvector.finiteDimensional_principalSeries_inf_rightInvariantFunctions0 below · depth 22