Definitions/Def_LanglandsTunnell_CubicInduction_CellBumps.lean
Cell bumps for local Whittaker functions of cubic induction forms
Throughout, v runs over the finite places of \mathbb{Q} (height-one primes of \mathcal{O}_{\mathbb{Q}}), and K is a number field whose ring of integers is an integral \mathcal{O}_{\mathbb{Q}}-algebra.
IsCellBumpAt v ψv 𝔡 t₀ W is a predicate on a function W on \mathrm{GL}_3(\mathbb{Q}_v), given an additive character \psi_v of \mathbb{Q}_v, an ideal \mathfrak{d} of \mathcal{O}_{\mathbb{Q}} and an element t_0 \in \mathrm{GL}_2(\mathbb{Q}_v). It is the conjunction of four clauses: W is a \psi_v-Whittaker function, i.e. W(u(x,y,z)g) = \psi_v(x+y)W(g) for the upper unipotent u(x,y,z) and all g; W(\iota(x)) = 0 for every x \in \mathrm{GL}_2(\mathbb{Q}_v) admitting no factorisation x = n\,t_0\,k with n in the range of the one-parameter upper unipotent homomorphism of \mathrm{GL}_2 and k in AdelicDock.localLevelOne (𝓞 ℚ) ℚ v 𝔡 (the pullback along the local-to-finite-adelic embedding at v of the finite-adelic level-one group of \mathfrak{d}); W(\iota(t_0 k)) = W(\iota(t_0)) for all such k; and W(\iota(t_0)) = 1. Here \iota is the block embedding g \mapsto \mathrm{diag}(g,1) of \mathrm{GL}_2 into \mathrm{GL}_3. Thus, restricted along \mathrm{GL}_2, W is supported on the single cell N t_0 K_1(\mathfrak{d}), is constant on it, and is normalised to 1 there.
IsNormalizedOffRamified K pins ψ μ D, for a CubicInductionForm D, asserts that D.form ≠ 0 and that at every v not ramified in K with addCharLevel (psiLoc ψ v) = 0 one has D.whittakerLoc v 1 = 1 together with HasSphericalTorusValuesAt (inducedCoeff K μ) v (D.whittakerLoc v). Since this is verbatim the condition appearing in HasCubicInductionForm, the theorem hasCubicInductionForm_iff_exists_isNormalizedOffRamified records the equivalence of HasCubicInductionForm K pins ψ μ with the existence of a cubic induction form satisfying IsNormalizedOffRamified, the two being the same by unfolding.
HasCellBumpsOn K pins ψ μ T π hπ m₀ is itself a Prop-valued implication, for a finite set T of finite places, a family of non-zero \pi_v \in \mathbb{Q}_v and integers m_0(v): under the hypotheses that each v \in T is ramified in K, that psiLoc ψ v is trivial on \mathcal{O}_v yet non-trivial, that |\pi_v| = \exp(-1) (so \pi_v is a uniformiser) and that m_0(v) \ge 0, it asserts the existence of a cubic induction form D and a family of ideals \mathfrak{d}_v such that D satisfies IsNormalizedOffRamified, \mathfrak{d}_v \neq \bot for v \in T, and for each v \in T the local Whittaker function D.whittakerLoc v is a cell bump at v for \psi_v, \mathfrak{d}_v and the torus element \mathrm{diag}(\pi_v^{m_0(v)},1).
Relation to Mathlib
Mathlib has no notion of Whittaker functions, of adelic level structures on \mathrm{GL}_2 or \mathrm{GL}_3, or of automorphic induction from a cubic field; the predicates here, and the level-one and maximal-compact subgroups they refer to, are the project's own.
Where it is used
These predicates belong to the Langlands–Tunnell input of the argument: the cubic induction forms are the automorphic objects on \mathrm{GL}_3 attached to a character of a cubic extension, and the cell-bump conditions pin down their local Whittaker functions at the places ramified in K, where no spherical normalisation is available, so that local integrals there can be computed explicitly when the form is compared with a \mathrm{GL}_2 object.
References
- 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
- H. Jacquet, I. I. Piatetski-Shapiro and J. A. Shalika, Automorphic forms on GL(3), I, Annals of Mathematics 109 (1979), 169–212
References are suggested automatically and have not been individually verified.
English text generated automatically from the Lean source; the Lean statement is authoritative.
- 60 lines
- 4 declarations
- used in the statements of 145 theorems and imported by 140 proofs
- imports 2 definition modules
Source file: Definitions/Def_LanglandsTunnell_CubicInduction_CellBumps.lean
Imported by
- no other definition module
Declarations
- def
LanglandsTunnell.CubicInduction.IsCellBumpAt - def
LanglandsTunnell.CubicInduction.IsNormalizedOffRamified - theorem
LanglandsTunnell.CubicInduction.hasCubicInductionForm_iff_exists_isNormalizedOffRamified - def
LanglandsTunnell.CubicInduction.HasCellBumpsOn
Source
import Definitions.Def_LanglandsTunnell_CubicInduction_Structure import Definitions.Def_UnramifiedWhittaker_HeckeRecursion set_option autoImplicit false open IsDedekindDomain NumberField AutomorphicForm noncomputable section namespace LanglandsTunnell.CubicInduction section CellBump variable (v : HeightOneSpectrum (𝓞 ℚ)) def IsCellBumpAt (ψv : AddChar (v.adicCompletion ℚ) ℂ) (𝔡 : Ideal (𝓞 ℚ)) (t₀ : GL (Fin 2) (v.adicCompletion ℚ)) (W : LocalGL3 v → ℂ) : Prop := IsGL3PsiWhittakerFn ψv W ∧ (∀ x : GL (Fin 2) (v.adicCompletion ℚ), (¬ ∃ n ∈ (AutomorphicForm.unipotentGL2Hom (R := v.adicCompletion ℚ)).range, ∃ k ∈ AdelicDock.localLevelOne (𝓞 ℚ) ℚ v 𝔡, x = n * t₀ * k) → W (iotaGL x) = 0) ∧ (∀ k ∈ AdelicDock.localLevelOne (𝓞 ℚ) ℚ v 𝔡, W (iotaGL (t₀ * k)) = W (iotaGL t₀)) ∧ W (iotaGL t₀) = 1 end CellBump section Existence variable (K : Type) [Field K] [NumberField K] [Algebra (𝓞 ℚ) (𝓞 K)] [Algebra.IsIntegral (𝓞 ℚ) (𝓞 K)] def IsNormalizedOffRamified (pins : CarrierPins ℚ) (ψ : AddChar (AdeleRing (𝓞 ℚ) ℚ) ℂ) (μ : (AdeleRing (𝓞 K) K)ˣ →* ℂˣ) (D : CubicInductionForm K pins ψ μ) : Prop := D.form ≠ 0 ∧ ∀ v, ¬ IsRamifiedIn K v → LanglandsTunnell.TateLocal.addCharLevel (psiLoc ψ v) = 0 → D.whittakerLoc v 1 = 1 ∧ HasSphericalTorusValuesAt (inducedCoeff K μ) v (D.whittakerLoc v) theorem hasCubicInductionForm_iff_exists_isNormalizedOffRamified (pins : CarrierPins ℚ) (ψ : AddChar (AdeleRing (𝓞 ℚ) ℚ) ℂ) (μ : (AdeleRing (𝓞 K) K)ˣ →* ℂˣ) : HasCubicInductionForm K pins ψ μ ↔ ∃ D : CubicInductionForm K pins ψ μ, IsNormalizedOffRamified K pins ψ μ D := Iff.rfl def HasCellBumpsOn (pins : CarrierPins ℚ) (ψ : AddChar (AdeleRing (𝓞 ℚ) ℚ) ℂ) (μ : (AdeleRing (𝓞 K) K)ˣ →* ℂˣ) (T : Finset (HeightOneSpectrum (𝓞 ℚ))) (π : (v : HeightOneSpectrum (𝓞 ℚ)) → v.adicCompletion ℚ) (hπ : ∀ v, π v ≠ 0) (m₀ : HeightOneSpectrum (𝓞 ℚ) → ℤ) : Prop := (∀ v ∈ T, IsRamifiedIn K v) → (∀ v ∈ T, ∀ r : v.adicCompletionIntegers ℚ, psiLoc ψ v (algebraMap (v.adicCompletionIntegers ℚ) (v.adicCompletion ℚ) r) = 1) → (∀ v ∈ T, psiLoc ψ v ≠ 1) → (∀ v ∈ T, Valued.v (π v) = WithZero.exp (-1 : ℤ)) → (∀ v ∈ T, 0 ≤ m₀ v) → ∃ (D : CubicInductionForm K pins ψ μ) (𝔡 : HeightOneSpectrum (𝓞 ℚ) → Ideal (𝓞 ℚ)), IsNormalizedOffRamified K pins ψ μ D ∧ (∀ v ∈ T, 𝔡 v ≠ ⊥) ∧ ∀ v ∈ T, IsCellBumpAt v (psiLoc ψ v) (𝔡 v) (UnramifiedWhittaker.diagZ (π v) (hπ v) (m₀ v)) (D.whittakerLoc v) end Existence end LanglandsTunnell.CubicInduction end
Statements phrased using this module (145)
- 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 - 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 - Normalised K₁(p^ℓ)-invariant vector with mirabolic bump support
LanglandsTunnell.RankinSelberg.exists_mem_gl3CyclicSubspace_congruenceK1_invariant_iotaGL_eq_bump_of_localZeta31_fe_one107 below · depth 19 - Torus finiteness for the cyclic space of a deep twist
LanglandsTunnell.RankinSelberg.forall_mem_gl3CyclicSubspace_twist_det_torusFinite_of_principalLevel_of_admissible_of_deepTwist12 below · depth 19 - Value form of the local GL₂timesGL₃ functional equation at p
LanglandsTunnell.RankinSelberg.forall_mem_span_rsLocalIntegral_dual_eq_stdRootNumber_mul_of_localZeta31_identified_of_torusFinite_of_centralChar_of_gauge_of_admissible_of_principalNormPin_adm_gamma_bump_levelShift_global514 below · depth 19 - Determinant twists cancel in the local GL₃× GL₂ Rankin–Selberg data
LanglandsTunnell.RankinSelberg.gl3CyclicSubspace_detTwist_and_rsIntegrand_detTwist_eq0 below · depth 19 - Deep-twist product law for priced local root numbers above p
LanglandsTunnell.Converse.finprod_stdRootNumberAt_twist_mul_twist_eq_sq_of_le_floor22 below · depth 20 - Pinned conductor exponent unchanged by a shallow norm twist
LanglandsTunnell.Converse.pinnedExp_comp_idelicNorm_mul_eq_pinnedExp_of_hasConductorExponentAt_le_of_depth_floor3 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 - Local GL₃× GL₂ gamma factor from a global realisation
LanglandsTunnell.RankinSelberg.exists_forall_mem_span_rsLocalIntegral_dual_mul_eq_mul_of_rsGlobalIntegral_realisation6 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 - Pair stability of the GL₃timesGL₂ local functional equation
LanglandsTunnell.RankinSelberg.forall_mem_span_rsLocalIntegral_dual_eq_mul_of_forall_localZeta31_fe_of_deepTwist_of_principalLevel_of_admissible_of_gammaFactor_of_forall_localZeta31_fe_of_bump_levelShift_global489 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 - 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 - Local Rankin–Selberg integrals evaluating a finite Whittaker family
LanglandsTunnell.RankinSelberg.exists_mem_gl3CyclicSubspace_forall_rsLocalIntegral_eq_mul_apply_of_finite11 below · depth 21 - Level 3B bump vector in a twisted principal-series Whittaker model
LanglandsTunnell.RankinSelberg.exists_mem_gl3CyclicSubspace_twist_coefficientFn_principalSeries3_congruenceK1_invariant_iotaGL_bump_of_pos_of_level157 below · depth 21 - Non-degenerate test pair for the local GL₃× GL₂ integral
LanglandsTunnell.RankinSelberg.exists_mem_span_forall_rsLocalIntegral_eq_const_ne_zero_of_isGL3PsiWhittakerFn13 below · depth 21 - A principal-series GL₃ Whittaker model with prescribed central character
LanglandsTunnell.RankinSelberg.exists_principalSeries3_whittaker_deepTwist_centralChar_of_higherUnitsAt_unitary_shallow12 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 - Rationality of local Rankin–Selberg integrals for GL₃ principal series
LanglandsTunnell.RankinSelberg.exists_rational_rsLocalIntegral_and_dual_of_principalSeries363 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 - Multiplicativity of the GL₃timesGL₂ local γ-factor in principal series
LanglandsTunnell.RankinSelberg.forall_mem_span_rsLocalIntegral_dual_eq_mul_of_forall_localZeta31_fe_of_principalSeries273 below · depth 21 - Deep twist: GL₃timesGL₂ local integrals are Laurent polynomials
LanglandsTunnell.RankinSelberg.forall_mem_span_rsLocalIntegral_eq_laurent_of_deepTwist_of_principalLevel_of_admissible20 below · depth 21 - Pair stability at (3,2): transfer of the cleared functional equation
LanglandsTunnell.RankinSelberg.forall_rsLocalIntegral_clearedFE_of_forall_rsLocalIntegral_clearedFE_of_centralChar_eq_of_deepTwist_pairStability32_of_bump59 below · depth 21 - Multiplicativity of the local GL₃× GL₂ functional equation
LanglandsTunnell.RankinSelberg.forall_rsLocalIntegral_clearedFE_prod_of_principalSeries3_of_forall_torusZeta_fe_multiplicativity3_ed3305 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 - Gauge majorant for cyclic translates of principal-series Whittaker coefficients
LanglandsTunnell.CubicInduction.exists_gauge_of_mem_gl3CyclicSubspace_coefficientFn_principalSeries323 below · depth 22 - Level-pᵈ Whittaker vector in a unitary principal series of GL₃
LanglandsTunnell.CubicInduction.exists_isWhittakerFunctional3_coefficientFn_ne_zero_forall_deepTwist_eq_of_forall_higherUnitsAt_of_pos11 below · depth 22 - Unramified twist shifts the local (3,1) functional equation
LanglandsTunnell.CubicInduction.forall_localZeta31_fe_of_twist_modulus_cpow0 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 - Local GL₃× GL₁ functional equation for deeply twisted principal series
LanglandsTunnell.RankinSelberg.exists_forall_localZeta31_fe_one_twist_coefficientFn_principalSeries3_of_exactConductor59 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 - Bump test vector for the local GL₃× GL₂ Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.exists_mem_gl3CyclicSubspace_forall_rsLocalIntegral_eq_mul_setIntegral_translate9 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 - Rationality of principal-series Rankin–Selberg local integrals at p
LanglandsTunnell.RankinSelberg.exists_rational_rsLocalIntegral_and_dual_of_jacquetWhittaker3_ed257 below · depth 22 - Non-degenerate local datum realising pair 2's cleared functional equation
LanglandsTunnell.RankinSelberg.exists_rsLocalIntegral_clearedFE_datum_of_centralChar_eq_of_deepTwist_pairStability32_of_bump56 below · depth 22 - Local GL₃timesGL₂ functional equation for a Jacquet-integral section
LanglandsTunnell.RankinSelberg.exists_rsLocalIntegral_jacquetIntegral_dual_eq_mul_of_forall_localZeta31_fe_of_integrable_setIntegral_localLevelOne_of_torusShell49 below · depth 22 - Cleared Rankin–Selberg functional equation for one Jacquet–Whittaker vector
LanglandsTunnell.RankinSelberg.forall_rsLocalIntegral_clearedFE_prod_of_jacquetWhittaker3_of_forall_torusZeta_fe301 below · depth 22 - Twisted translated Jacquet–Whittaker function: admissible, unitary central, gauged
LanglandsTunnell.CubicInduction.exists_detTwist_jacquetWhittaker3_translate_whittaker_smooth_central_admissible_gauge23 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 - Non-vanishing of a local GL₃× GL₂ Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.exists_mem_gl3CyclicSubspace_forall_rsLocalIntegral_ne_zero_of_ne_zero13 below · depth 23 - Test vectors with equal local integrals, one constant
LanglandsTunnell.RankinSelberg.exists_testVectors_rsLocalIntegral_eq_and_eq_const_of_centralChar_eq_of_deepTwist_of_bump55 below · depth 23 - Local GL₃× GL₂ cleared functional equation from torus equations
LanglandsTunnell.RankinSelberg.forall_rsLocalIntegral_clearedFE_prod_of_jacquetWhittaker3_of_forall_torusZeta_fe_core287 below · depth 23 - Cleared local Rankin–Selberg functional equation at the family centre
LanglandsTunnell.RankinSelberg.exists_cleared_rsLocalIntegral_fe_of_forall_lt_cleared_fe_finsum_cpow_of_isGL3PsiWhittakerFn14 below · depth 24 - Cleared local GL₃× GL₂ integrals along a flat twist family
LanglandsTunnell.RankinSelberg.exists_forall_lt_rsLocalIntegral_jacquetWhittaker3_twistFamily_mul_centralTate_eq_cpow_mul_eval144 below · depth 24 - Jacquet–Shalika test vectors with non-vanishing unit-shell pairing
LanglandsTunnell.RankinSelberg.exists_mem_span_schwartzBruhat_fourier_unitShell_pairing_ne_zero_of_deepTwist_of_conductor_le40 below · depth 24 - Dual Rankin–Selberg integral of a smoothed GL₃ bump vector
LanglandsTunnell.RankinSelberg.exists_pos_forall_rsLocalIntegral_dual_longWeyl3_smoothedBump_eq_mul_setIntegral_unitShell12 below · depth 24 - Cleared GL₃× GL₂ functional equation in the positive chamber
LanglandsTunnell.RankinSelberg.forall_rsLocalIntegral_clearedFE_prod_of_jacquetWhittaker3_of_forall_torusZeta_fe_core_of_chamber270 below · depth 24 - Equal smoothed Whittaker integrals along ι(GL₂)w₃ at level K₁(p^f)
LanglandsTunnell.RankinSelberg.integral_integral_iotaGL_mul_longWeyl3_mul_upperUnipotent3_eq_of_congruenceK1_of_centralChar_of_iotaGL_bump1 below · depth 24 - Unipotent smoothing of a K₁(p^f)-invariant function on GL₃
LanglandsTunnell.RankinSelberg.integral_integral_upperUnipotent3_translate_mem_gl3CyclicSubspace_of_congruenceK1_invariant0 below · depth 24 - Kirillov bump in a twisted Whittaker translate span
LanglandsTunnell.RankinSelberg.exists_mem_span_twist_det_kirillov_eq_indicator_shell_of_localLevelOne8 below · depth 25 - Rationality of the dual GL₂× GL₂ Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.exists_rsLocalIntegral22_dual_mul_one_sub_eq_cpow_mul_eval_of_principalSeries2_of_forall_torusZeta_polynomial40 below · depth 25 - Rationality of the local GL₂timesGL₂ Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.exists_rsLocalIntegral22_mul_one_sub_eq_cpow_mul_eval_of_principalSeries2_of_forall_torusZeta_polynomial39 below · depth 25 - Unfolded GL₃× GL₂ Rankin–Selberg integrals, primal and dual
LanglandsTunnell.RankinSelberg.exists_rsLocalIntegral_jacquetWhittaker3_iotaGL_eq_sum_and_dual_eq_mul_sum_of_chamber_ed2111 below · depth 25 - Cleared local GL₃× GL₂ Rankin–Selberg integrals in a chamber
LanglandsTunnell.RankinSelberg.exists_rsLocalIntegral_jacquetWhittaker3_mul_centralTate_eq_cpow_mul_eval_and_dual_of_chamber141 below · depth 25 - Whittaker functions agreeing on ι(GL₂) agree on ι(GL₂)N₃Z₃K₁
LanglandsTunnell.RankinSelberg.forall_apply_iotaGL_mul_upperUnipotent3_mul_scalar_mul_eq_of_forall_apply_iotaGL_eq0 below · depth 25 - Godement–Jacquet zeta integrals for GL₂: cleared functional equation
LanglandsTunnell.RankinSelberg.forall_godementZeta2_clearedFE_of_forall_torusZeta_fe167 below · depth 25 - Cleared GL₂× GL₂ local functional equation: principal series case
LanglandsTunnell.RankinSelberg.forall_rsLocalIntegral22_schwartz_clearedFE_of_principalSeries2_of_forall_torusZeta_fe_ed2219 below · depth 25 - Schwartz–Bruhat cut-off kernels with prescribed local Fourier transforms
LanglandsTunnell.RankinSelberg.isSchwartzBruhat_and_tateFourier_shellKernels_of_conductor_le15 below · depth 25 - Local dual Rankin–Selberg integrand of a smoothed bump vector
LanglandsTunnell.RankinSelberg.rsIntegrand_dual_longWeyl3_smoothedBump_invariant_support_bound_and_bigCell_eq3 below · depth 25 - Non-vanishing of a unit-shell Whittaker–Fourier pairing
LanglandsTunnell.RankinSelberg.setIntegral_unitShell_pairing_ne_zero_of_kirillov_shell_of_deepTwist_of_conductor_le34 below · depth 25 - Gauge bound for an admissible local Whittaker function on the torus
AutomorphicForm.WhittakerModel.exists_norm_diagUnits2_mul_le_and_eq_zero_of_admissible_of_centralChar4 below · depth 26 - Contragredient involution maps I(μ₀,μ₁) to I(μ₁⁻¹,μ₀⁻¹)
LanglandsTunnell.CubicInduction.conj_transposeInvN_mem_principalSeries20 below · depth 26 - Godement–Whittaker function of a pure tensor at ι(g)
LanglandsTunnell.CubicInduction.godementWhittaker3_iotaGL_eq_of_pureTensor0 below · depth 26 - Dual Jacquet integral of a principal-series vector
LanglandsTunnell.CubicInduction.integral_psiLocal_mul_transposeInvN_eq_mul_integral_psiLocal_mul_dual0 below · depth 26 - Godement-section realisation of the GL₃ Jacquet–Whittaker function
LanglandsTunnell.CubicInduction.jacquetWhittaker3_diagonal3_mul_eq_mul_godementWhittaker3_of_chamber27 below · depth 26 - Twisted contragredient of a Whittaker vector is again Whittaker
LanglandsTunnell.RankinSelberg.dualPartner_block_of_admissible2 below · depth 26 - Uniform radial profile of a Schwartz–Bruhat function on bottom rows
LanglandsTunnell.RankinSelberg.exists_forall_apply_row_localLevelOne_eq_zero_and_eq_apply_zero_of_isLocallyConstant_of_hasCompactSupport0 below · depth 26 - Convergence of the dual GL₂× GL₂ Rankin–Selberg integrand
LanglandsTunnell.RankinSelberg.exists_forall_integrable_dual_rsIntegrand22_withDensity_of_admissible_of_chamber33 below · depth 26 - Absolute convergence of the unfolded local Godement integrand
LanglandsTunnell.RankinSelberg.exists_forall_integrable_godementUnfold_of_principalSeries2_of_admissible_ed236 below · depth 26 - Integrability of the folded local Rankin–Selberg integrand in the chamber
LanglandsTunnell.RankinSelberg.exists_forall_integrable_jacquetIntegral_mul_whittaker_mul_row_mul_cpow_withDensity_of_principalSeries2_of_chamber28 below · depth 26 - Vanishing of deep dual torus shells over K₀
LanglandsTunnell.RankinSelberg.exists_forall_le_setIntegral_localLevelOne_dualJacquet_mul_partner_mul_eq_zero_of_dualTorusZeta_polynomial12 below · depth 26 - Rationality of the local (2,2) Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.exists_rsLocalIntegral22_mul_one_sub_eq_cpow_mul_eval_of_principalSeries2_of_forall_torusZeta_polynomial_core38 below · depth 26 - Open compact subgroup adapted to φ₁ and χ
LanglandsTunnell.RankinSelberg.exists_subgroup_isOpen_isCompact_forall_apply_mul_eq_and_det_eq_one_and_transposeInv_mem0 below · depth 26 - Half-plane integrability of local Godement–Jacquet integrals on GL₂
LanglandsTunnell.RankinSelberg.forall_exists_integrable_godementZeta2_coefficient36 below · depth 26 - Godement–Jacquet zeta integrals of GL₂ matrix coefficients
LanglandsTunnell.RankinSelberg.forall_exists_laurent_godementZeta2_coefficient_of_forall_torusZeta_fe47 below · depth 26 - Rationality of Whittaker Godement–Jacquet zeta integrals on GL₂
LanglandsTunnell.RankinSelberg.forall_exists_rational_godementZeta2_whittaker_of_forall_torusZeta_fe48 below · depth 26 - Cleared local Godement–Jacquet functional equation for Whittaker coefficients
LanglandsTunnell.RankinSelberg.forall_godementZeta2_whittaker_clearedFE_of_forall_torusZeta_fe166 below · depth 26 - Local GL₂× GL₂ functional equation for Laurent numerators
LanglandsTunnell.RankinSelberg.forall_rsLocalIntegral22_schwartz_centralCleared_laurentFE_of_principalSeries2_of_forall_torusZeta_fe206 below · depth 26 - Integrability of the local Rankin–Selberg integrand from its unfolding
LanglandsTunnell.RankinSelberg.integrable_rsIntegrand_godementSlot_of_integrable_unfold9 below · depth 26 - Unfolding of a Godement-section Rankin–Selberg local integral
LanglandsTunnell.RankinSelberg.rsLocalIntegral_godementWhittaker_iotaGL_eq_sum_rsLocalIntegral_mul_godementZeta9 below · depth 26 - Finiteness of |det|^t over norm balls in GL₂(ℚₚ)
AutomorphicForm.lintegral_indicator_norm_le_mul_norm_det_rpow_lt_top22 below · depth 27 - Big-cell GL₃ section as a GL₂ Godement integral
LanglandsTunnell.CubicInduction.cellSectionOf_antidiagonal3_mul_mul_eq_integral_godementDatum4 below · depth 27 - Finite pure-tensor decomposition of the local Godement datum
LanglandsTunnell.CubicInduction.exists_finset_pureTensor_godementDatum4 below · depth 27 - Godement slot vectors: principal series membership and support
LanglandsTunnell.CubicInduction.godementDatum_mem_principalSeries2_and_support2 below · depth 27 - Jacquet unfolding of a Godement section on GL₃
LanglandsTunnell.CubicInduction.integral_godementSection_upperUnipotent3_eq_godementWhittaker3_of_continuous4 below · depth 27 - Jacquet–Whittaker function at diag(1,-1,1)Y as a ψ-integral
LanglandsTunnell.CubicInduction.jacquetWhittaker3_diagonal3_mul_eq_mul_integral_psiLocal_cellSectionOf15 below · depth 27 - Measurability of the unfolded Godement double integrand
LanglandsTunnell.RankinSelberg.aestronglyMeasurable_godementUnfold_integrand3 below · depth 27 - Half-plane integrability of the local GL₂timesGL₂ integrand
LanglandsTunnell.RankinSelberg.exists_forall_integrable_jacquetIntegral_mul_whittaker_mul_row_withDensity_of_admissible_of_chamber25 below · depth 27 - Two-exponent asymptotics of chamber Jacquet integrals on small torus
LanglandsTunnell.RankinSelberg.exists_forall_jacquetIntegral_diagOne_mul_eq_sqrt_modulus_mul_add_of_mem_principalSeries2_of_chamber6 below · depth 27 - Inner bound for the local Rankin–Selberg N₂backslash GL₂ integral
LanglandsTunnell.RankinSelberg.exists_forall_lintegral_enorm_jacquetIntegral_mul_whittaker_mul_translate_mul_row_le_of_admissible_of_chamber23 below · depth 27 - Gauge bound and far-out vanishing for a GL₂ Jacquet integral
LanglandsTunnell.RankinSelberg.exists_forall_norm_jacquetIntegral_principalSeries2_diagUnits2_mul_le_and_eq_zero_of_chamber8 below · depth 27 - Torus-shell series of Jacquet and Whittaker integrals sums to q^{ms}P(q^{-s})
LanglandsTunnell.RankinSelberg.exists_hasSum_torusShells_jacquetIntegral_mul_whittaker_mul_row_eq_cpow_mul_eval_of_forall_torusZeta_polynomial_ed217 below · depth 27 - Iwasawa integration formula for Haar measure on GL₂(ℚₚ)
LanglandsTunnell.RankinSelberg.exists_pos_forall_lintegral_eq_mul_lintegral_prod_lintegral_unipotent_diagUnits220 below · depth 27 - Local integrability of a shifted Godement–Jacquet zeta integrand
LanglandsTunnell.RankinSelberg.forall_exists_integrable_godementZeta2_whittaker_shift29 below · depth 27 - Laurent Godement–Jacquet integrals of GL₂ Whittaker vectors
LanglandsTunnell.RankinSelberg.forall_exists_laurent_godementZeta2_whittaker_of_forall_torusZeta_fe42 below · depth 27 - Rationality in q^{-s} of local Godement zeta integrals
LanglandsTunnell.RankinSelberg.forall_exists_rational_godementZeta2_whittaker_shift44 below · depth 27 - Cleared Godement–Jacquet functional equation for a Whittaker coefficient
LanglandsTunnell.RankinSelberg.forall_godementZeta2_whittaker_clearedFE_of_forall_torusZeta_fe_of_borelEigenfunctional92 below · depth 27 - Godement–Jacquet functional equation for cuspidal Whittaker coefficients
LanglandsTunnell.RankinSelberg.forall_godementZeta2_whittaker_clearedFE_of_forall_torusZeta_fe_of_cuspidal121 below · depth 27 - Centre-cleared local GL₂× GL₂ functional equation, principal-series branch
LanglandsTunnell.RankinSelberg.forall_rsLocalIntegral22_schwartz_centralCleared_laurentFE_of_principalSeries2_of_forall_torusZeta_fe_of_borelEigenfunctional187 below · depth 27 - Centre-cleared local functional equation for GL₂× GL₂: cuspidal branch
LanglandsTunnell.RankinSelberg.forall_rsLocalIntegral22_schwartz_centralCleared_laurentFE_of_principalSeries2_of_forall_torusZeta_fe_of_cuspidal196 below · depth 27 - Transpose-inverse symmetry of the local GL₂ Godement zeta integral
LanglandsTunnell.RankinSelberg.godementZeta2_comp_transposeInvN_eq_godementZeta2_conj_of_central0 below · depth 27 - Torus-shell expansion of a local Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.hasSum_torusShells_rsLocalIntegral22_jacquetIntegral_schwartz_of_integrable9 below · depth 27 - Kirillov vanishing or Borel eigenfunctional dichotomy for GL₂(ℚₚ)
LanglandsTunnell.RankinSelberg.kirillov_vanish_near_zero_or_exists_borelEigenfunctional_of_irreducible_admissible4 below · depth 27 - Propagating a Whittaker gauge from the level-one subgroup to GL₂
AutomorphicForm.WhittakerModel.norm_diagUnits2_mul_le_of_forall_mem_localLevelOne_norm_diagUnits2_mul_le0 below · depth 28 - Principal series embedding when the Jacquet module is non-zero
LanglandsTunnell.CubicInduction.exists_linearMap_principalSeries2_of_jacquet_ne_top1 below · depth 28 - Product integrability of a local Rankin–Selberg kernel in the chamber
LanglandsTunnell.RankinSelberg.exists_forall_integrable_prod_row_mul_row_mul_cpow_mul_whittaker_diagOne_mul_cpow_of_admissible_of_chamber35 below · depth 28 - Product integrability of the local Rankin–Selberg kernel in a chamber
LanglandsTunnell.RankinSelberg.exists_forall_integrable_prod_row_mul_row_mul_cpow_mul_whittaker_diagOne_mul_cpow_of_chamber35 below · depth 28 - Vanishing of deep torus shells against a Whittaker vector
LanglandsTunnell.RankinSelberg.exists_forall_le_setIntegral_localLevelOne_mul_diagZ_mul_eq_zero_of_sqrt_modulus_tail_of_forall_torusZeta_polynomial7 below · depth 28 - Rationality and cleared functional equation for local GL₂ zeta integrals
LanglandsTunnell.RankinSelberg.exists_gamma_forall_rational_godementZeta2_principalSeries2_and_clearedFE66 below · depth 28 - Constant η-twisted local torus zeta integrals for Whittaker models
LanglandsTunnell.RankinSelberg.exists_mem_span_forall_torusZeta_twist_eq_const_and_dual_of_irreducible_admissible6 below · depth 28 - Local Godement zeta integral as a Rankin–Selberg row-slice integral
LanglandsTunnell.RankinSelberg.exists_pos_forall_godementZeta2_eq_mul_rsLocalIntegral_rowSlice0 below · depth 28 - Whittaker Godement zeta equals that of its principal-series image
LanglandsTunnell.RankinSelberg.exists_schwartz_godementZeta2_whittaker_eq_godementZeta2_section_and_dual_of_equivariant_embedding18 below · depth 28 - Local test function matching Godement–Jacquet and torus zeta integrals
LanglandsTunnell.RankinSelberg.exists_schwartz_godementZeta2_whittaker_eq_mul_torusZeta_and_dual_of_integrable22 below · depth 28 - One-shell Kirillov function under the Weyl element, cuspidal case
LanglandsTunnell.RankinSelberg.forall_apply_diagOne_mul_weylJ_eq_of_apply_diagOne_eq_inv_mul_indicator_shell_of_cuspidal36 below · depth 28 - Uniform abscissa for local Godement–Jacquet Whittaker integrals
LanglandsTunnell.RankinSelberg.forall_exists_forall_integrable_godementZeta2_whittaker_shift_of_isLocallyConstant30 below · depth 28 - Uniform integrability of dual local Godement–Jacquet integrals
LanglandsTunnell.RankinSelberg.forall_exists_forall_integrable_godementZeta2_whittaker_transposeInvN_shift_of_isLocallyConstant32 below · depth 28 - Integrability of the dual local Godement–Jacquet zeta integrand
LanglandsTunnell.RankinSelberg.forall_exists_integrable_godementZeta2_whittaker_transposeInvN_shift31 below · depth 28 - Laurent polynomiality of shifted Godement–Jacquet zeta integrals
LanglandsTunnell.RankinSelberg.forall_exists_laurent_godementZeta2_whittaker_shift_of_torusLaurent38 below · depth 28 - Fourier transform of cuspidal Kirillov matrix-coefficient functions on M₂
LanglandsTunnell.RankinSelberg.matFourier22_kirillov_det_mul_coefficient_eq_of_cuspidal75 below · depth 28 - Kirillov decomposition of cuspidal Whittaker vectors into shell–character vectors
LanglandsTunnell.RankinSelberg.exists_finset_eq_sum_smul_shell_character_kirillov_of_cuspidal15 below · depth 29 - Godement unfolding of a GL₂ principal-series zeta integral
LanglandsTunnell.RankinSelberg.exists_forall_integrable_and_godementZeta2_eq_mul_twoVarZeta_slice_of_mem_principalSeries26 below · depth 29 - Godement unfolding of the contragredient local GL₂ zeta integral
LanglandsTunnell.RankinSelberg.exists_forall_integrable_and_godementZeta2_transposeInv_matFourier22_eq_mul_twoVarZeta_fourierSlice_of_mem_principalSeries235 below · depth 29 - Local integrability of the unfolded Rankin–Selberg integrand
LanglandsTunnell.RankinSelberg.exists_forall_integrable_whittaker_mul_principalSeries2_antidiagonal2_mul_row_mul_cpow_of_admissible_of_chamber28 below · depth 29 - Vanishing of deep torus shells in the unfolded zeta integrand
LanglandsTunnell.RankinSelberg.exists_forall_setIntegral_localLevelOne_rowSlice_whittaker_shell_eq_zero_of_le17 below · depth 29 - Weyl element on shells: twisted local functional equation
LanglandsTunnell.RankinSelberg.exists_forall_setIntegral_units_apply_diagUnitGL2_mul_weylJ_eq_mul_setIntegral_of_cuspidal27 below · depth 29 - Godement zeta on a box as constant times torus zeta
LanglandsTunnell.RankinSelberg.godementZeta2_boxIndicator_eq_mul_torusZeta_of_isOpen_of_chart3 below · depth 29 - Dual Godement–Jacquet zeta of the Fourier-transformed torus box
LanglandsTunnell.RankinSelberg.godementZeta2_transposeInv_matFourier22_boxIndicator_eq_mul_torusZeta_dual_of_integrable_of_chart14 below · depth 29 - Two-variable local zeta integrals: rationality and cleared functional equation
LanglandsTunnell.TateLocal.exists_gamma_forall_twoVarZeta_rational_and_clearedFE36 below · depth 29 - Central transformation law extends to the span of right translates
LanglandsTunnell.RankinSelberg.apply_scalar_mul_eq_mul_of_mem_span_translate0 below · depth 30 - Vanishing of deep torus shell integrals
LanglandsTunnell.RankinSelberg.exists_forall_localLevelOne_setIntegral_units_whittaker_diagUnitGL2_eq_zero_of_le_of_torusLaurent10 below · depth 30 - Local functional equation with vector-independent γ-factor
LanglandsTunnell.RankinSelberg.exists_rational_forall_torusZeta_fe_twist_of_irreducible_admissible26 below · depth 30 - Bochner Iwasawa integration formula on GL₂(ℚₚ)
LanglandsTunnell.RankinSelberg.forall_integrable_prod_and_integral_eq_mul_setIntegral_unipotent_diagUnits2_of_forall_lintegral_eq2 below · depth 30 - Local Godement slice is locally constant with compact support
LanglandsTunnell.RankinSelberg.isLocallyConstant_and_hasCompactSupport_slice_of_mem_principalSeries21 below · depth 30 - Unit-torus average over the local level-one subgroup
LanglandsTunnell.RankinSelberg.setIntegral_localLevelOne_eq_setIntegral_setIntegral_units_diagUnitGL2_mul_of_isLocallyConstant3 below · depth 30 - Product of two local Tate zeta integrals: rationality and cleared functional equation
LanglandsTunnell.TateLocal.exists_gamma_forall_localZeta_mul_localZeta_rational_and_clearedFE31 below · depth 30 - Rationality of twisted torus zeta integrals over ℚₚ
LanglandsTunnell.RankinSelberg.forall_mem_span_exists_rational_torusZeta_twist_and_dual_of_irreducible_admissible9 below · depth 31 - Rational local Tate zeta integrals and cleared functional equation
LanglandsTunnell.TateLocal.exists_gamma_forall_localZeta_rational_and_clearedFE30 below · depth 31 - Tate's local functional equation with φ-uniform γ-factor
LanglandsTunnell.TateLocal.exists_gamma_forall_localZeta_tateFourier_mul_eq_of_strip23 below · depth 32 - Convergence and rationality of local Tate zeta integrals over ℚ
LanglandsTunnell.TateLocal.exists_rational_localZeta_of_isSchwartzBruhat_of_logb_lt_re7 below · depth 32