Definitions/Def_LanglandsTunnell_RSCarrierSplit.lean
Archimedean Haar measure and finite factor for adelic GL₂
Two concrete objects attached to \mathrm{GL}_2 over \mathbb{Q} are defined. First, RSCarrier.archMeasure is a measure on \mathrm{GL}_2(\mathbb{R}), taken with respect to the Borel \sigma-algebra of the group (supplied explicitly rather than through an instance). It is the push-back along the entrywise inclusion g \mapsto (g_{ij}) of \mathrm{GL}_2(\mathbb{R}) into the four-dimensional space \mathrm{Fin}\,2 \to \mathrm{Fin}\,2 \to \mathbb{R} of Lebesgue measure (volume), weighted by the density g \mapsto |\det g|^{-2} (converted into [0,\infty] by ENNReal.ofReal). Thus no normalising constant is built in; left and right invariance, regularity and positivity of this measure are assertions about it and form no part of the definition.
Second, RSCarrier.finFactor assigns to an adelic matrix g \in \mathrm{GL}_2(\mathbb{A}_\mathbb{Q}) an element of finiteAdelicGL2Subgroup ℚ, the kernel of the archimedean-component homomorphism AdelicLevel.glArch, i.e. the subgroup of adelic matrices whose archimedean part is the identity. Its underlying element is \big(\mathrm{archRealGLAt}\,(\mathrm{ratArchGL2}\,g)\big)^{-1} \cdot g, where LanglandsTunnell.ratArchGL2 reads off the real component of g at the default infinite place of \mathbb{Q} (which is real, \mathbb{Q} being totally real), transported through the identification of the completion at that place with \mathbb{R}, and archRealGLAt embeds \mathrm{GL}_2(\mathbb{R}) back into the adelic group at the same place. Membership in the subgroup is verified by an entrywise computation, using that \mathbb{Q} has a single infinite place. Consequently g factors as the image of its real component times finFactor g, and finFactor g has the same components as g at every finite place.
Relation to Mathlib
Mathlib supplies the ambient ingredients (Lebesgue measure on a finite product of copies of \mathbb{R}, Measure.comap, withDensity, and abstract Haar measures on locally compact groups); the explicit measure on \mathrm{GL}_2(\mathbb{R}) obtained here as Lebesgue measure on matrix entries with density |\det|^{-2}, and the splitting off of the real component of an adelic matrix, are the project's own.
Where it is used
These are the archimedean ingredients of the carrier on which Hecke eigensystems over \mathbb{Q} are realised by smooth cuspidal automorphic functions on adelic \mathrm{GL}_2: the measure is the archimedean factor used in integration over \mathrm{GL}_2(\mathbb{R}), and the finite factor lets a function on the adelic group be analysed in a real variable at the unique infinite place, as needed for the lift of the discriminant cusp form and the Casimir and weight conditions in the Langlands–Tunnell input to the modularity argument.
References
- H. Darmon, F. Diamond and R. Taylor, Fermat's Last Theorem, in: Current Developments in Mathematics 1995, International Press, 1995, 1–154
- S. Gelbart, Automorphic Forms on Adele Groups, Annals of Mathematics Studies 83, Princeton University Press, 1975
- D. Bump, Automorphic Forms and Representations, Cambridge Studies in Advanced Mathematics 55, Cambridge University Press, 1997
References are suggested automatically and have not been individually verified.
English text generated automatically from the Lean source; the Lean statement is authoritative.
- 36 lines
- 2 declarations
- used in the statements of 177 theorems and imported by 180 proofs
- imports 3 definition modules
Source file: Definitions/Def_LanglandsTunnell_RSCarrierSplit.lean
Imports
Imported by
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Declarations
Source
import Definitions.Def_AutomorphicForm_SmoothAutomorphicFnAt import Definitions.Def_AutomorphicForm_ArchDerivCasimir import Definitions.Def_LanglandsTunnell_DeltaLift open MeasureTheory NumberField AutomorphicForm noncomputable section namespace RSCarrier def archMeasure : @Measure (GL (Fin 2) ℝ) (borel (GL (Fin 2) ℝ)) := letI := borel (GL (Fin 2) ℝ) (Measure.comap (fun g : GL (Fin 2) ℝ => fun i j => (g : Matrix (Fin 2) (Fin 2) ℝ) i j) (volume : Measure (Fin 2 → Fin 2 → ℝ))).withDensity fun g => ENNReal.ofReal (|(Matrix.GeneralLinearGroup.det g : ℝ)| ^ 2)⁻¹ def finFactor (g : AdelicGL2 (𝓞 ℚ) ℚ) : finiteAdelicGL2Subgroup ℚ := ⟨(archRealGLAt (IsTotallyReal.isReal (default : InfinitePlace ℚ)) (LanglandsTunnell.ratArchGL2 g))⁻¹ * g, by rw [mem_finiteAdelicGL2Subgroup_iff, map_mul, map_inv, inv_mul_eq_one] rw [show AdelicLevel.glArch (𝓞 ℚ) ℚ (archRealGLAt (IsTotallyReal.isReal (default : InfinitePlace ℚ)) (LanglandsTunnell.ratArchGL2 g)) = archGLIncl ℚ default (glEquivOfRingEquiv (InfinitePlace.Completion.ringEquivRealOfIsReal (IsTotallyReal.isReal (default : InfinitePlace ℚ))).symm (LanglandsTunnell.ratArchGL2 g)) from glArch_adelicArchGLIncl ℚ _] refine Units.ext (Matrix.ext fun i j => funext fun v => ?_) obtain rfl : v = default := Subsingleton.elim v default refine (congrArg (fun u : GL (Fin 2) (default : InfinitePlace ℚ).Completion => (u : Matrix (Fin 2) (Fin 2) (default : InfinitePlace ℚ).Completion) i j) (archComponent_archGLIncl_self ℚ default _)).trans ?_ rw [glEquivOfRingEquiv_apply_entry] exact (InfinitePlace.Completion.ringEquivRealOfIsReal _).symm_apply_apply _⟩ end RSCarrier end
Statements phrased using this module (177)
- Assembling archimedean Rankin–Selberg integrals from diagonal torus identities
LanglandsTunnell.Converse.exists_const_sum_rsArchIntegral_eq_mul_of_torus_identities3 below · depth 18 - Haar measure on GL₂(A_ℚ) splits as a product
LanglandsTunnell.Converse.exists_isHaarMeasure_map_adelicGLHaar_eq_prod_archMeasure3 below · depth 18 - Haar splitting of the adelic unipotent group of GL₂/ℚ
LanglandsTunnell.Converse.exists_isHaarMeasure_map_unipotentHaar_eq_prod_map_val2 below · depth 18 - The measure |det g|⁻² dg is a bi-invariant Haar measure on GL₂(ℝ)
LanglandsTunnell.Converse.isHaarMeasure_and_isMulRightInvariant_archMeasure0 below · depth 18 - 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 - 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 - Archimedean GL₂timesGL₃ torus-pair identity for the cubic induction
LanglandsTunnell.RankinSelberg.exists_archWhittaker_torusPair_eq_gammaFactor_of_archWhittakerDatum324 below · depth 18 - Half-plane integrability of archimedean GL₂timesGL₃ Rankin–Selberg integrands
LanglandsTunnell.RankinSelberg.exists_forall_integrable_archWhittaker_torusPair_rpow_det7 below · depth 18 - Rankin–Selberg integral as archimedean times finite integral times partial L-function
LanglandsTunnell.RankinSelberg.exists_forall_rsGlobalIntegral_eq_mul_rsArchIntegral_mul_rsFinIntegral_mul_lFun24 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 - Pure-tensor factorisation of a Whittaker function over ℚ
LanglandsTunnell.exists_whittakerCoefficient_eq_archWhittaker_mul_finWhittaker_of_isIsotypicCuspFormAt3 below · depth 18 - Local Whittaker relations at a good place over ℚ
LanglandsTunnell.finWhittaker_unipotent_levelOne_hecke_centre_of_isIsotypicCuspFormAt1 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 - Iwasawa reduction of the archimedean Rankin–Selberg integral
LanglandsTunnell.Converse.exists_const_rsArchIntegral_eq_mul_integral_diagonal2 below · depth 19 - Iwasawa majorant for density-weighted integrals on GL₂(ℝ)
LanglandsTunnell.Converse.exists_lintegral_mul_density_archMeasure_le_lintegral_iwasawa3 below · depth 19 - Finite Rankin–Selberg integrand integrable, or archimedean integral vanishes
LanglandsTunnell.Converse.integrable_rsFinIntegrand_or_rsArchIntegral_eq_zero_of_integrable4 below · depth 19 - Archimedean–finite splitting of the unipotent-quotient Rankin–Selberg integral
LanglandsTunnell.Converse.integral_unipotentQuotient_eq_rsArchIntegral_mul_rsFinIntegral_of_integrable4 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 - 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 - Archimedean GL₂× GL₃ torus-pair Gamma identity, minimal type
LanglandsTunnell.RankinSelberg.exists_mem_polyGauss3_jacquetVector3_torusPair_eq_gammaFactor_of_archWhittakerDatum_of_isCasimirEigen_of_minimalType281 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 - Conductor bound for the local central character at unramified v
LanglandsTunnell.CubicInduction.exists_hasConductorExponentAt_localChar_centralChar_le_inducedLevelAt_of_isCubicInductionDataOn278 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 - 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 - Identified local functional equation passes to the cyclic span
LanglandsTunnell.CubicInduction.localZeta31_identified_of_mem_gl3CyclicSubspace1 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 - Unfolding the archimedean torus pairing of the GL₃ Jacquet vector
LanglandsTunnell.RankinSelberg.exists_forall_torusPair_jacquetVector3_eq_integral_quasiChar_mul_torusIntegral_mul_godementMellin6 below · depth 20 - Unfolded archimedean GL₂× GL₃ torus-pair identity at minimal type
LanglandsTunnell.RankinSelberg.exists_mem_polyGauss3_jacquetVector3_unfoldedTorusPair_eq_gammaFactor_of_archWhittakerDatum_of_isCasimirEigen_of_minimalType280 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 - Jacquet vector at a real diagonal torus element, unfolded
LanglandsTunnell.CubicInduction.jacquetVector3_iota_upperUnit_eq_integral_godementInner3_mulShift0 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 - Integrability of the unfolded archimedean torus-pair integrand
LanglandsTunnell.RankinSelberg.exists_forall_integrable_unfoldedTorusPairIntegrand_jacquetVector34 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 - Unfolded archimedean torus pair and its dual Γ-factors
LanglandsTunnell.RankinSelberg.exists_mem_polyGauss3_iotaWeight_archZeta30_ne_zero_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_archWhittakerDatum_of_isCasimirEigen272 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 - Iwasawa bound for W_D(diag(at,1)e⁻¹)
LanglandsTunnell.Converse.ArchDatumR.norm_W_diagOne_mul_inv_le_of_iwasawa0 below · depth 22 - Non-vanishing archimedean zeta of a block-harmonic Jacquet vector
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_jacquetVector3_ne_zero_of_blockHarmonicOne_colHarmonic_gaussian3_of_weightZero38 below · depth 22 - Non-vanishing archimedean zeta for the conjugate block-harmonic section
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_jacquetVector3_ne_zero_of_conjBlockHarmonicOne_colHarmonic_gaussian357 below · depth 22 - Non-vanishing of the weight-zero minor-section archimedean zeta integral
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_jacquetVector3_ne_zero_of_minorSection_gaussian337 below · depth 22 - Continuity and decay of the Godement inner integral
LanglandsTunnell.CubicInduction.godementInner3_mulShift_polyGauss3_continuousOn_and_decay0 below · depth 22 - Weight law for the Jacquet vector of a Gaussian section
LanglandsTunnell.CubicInduction.jacquetVector3_mul_iota_eq_archWeightChar_inv_mul_of_colHarmonic_gaussian30 below · depth 22 - Equivariance of the Jacquet vector under ι of row isometries
LanglandsTunnell.CubicInduction.jacquetVector3_mul_iota_eq_archWeightChar_inv_mul_of_conjBlockHarmonic_colHarmonic_gaussian30 below · depth 22 - Weight-one K-type of the minor-section Jacquet vector
LanglandsTunnell.CubicInduction.jacquetVector3_mul_iota_eq_archWeightOne_inv_mul_of_minorSection_gaussian30 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 - Integrability of a real Whittaker torus profile against |t|^{s-1/2}t⁻²
LanglandsTunnell.RankinSelberg.exists_forall_integrable_Wr_mul_abs_cpow_mul_inv_sq0 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 - Archimedean Rankin–Selberg pair outside weight-one GL₂ parameters
LanglandsTunnell.RankinSelberg.exists_mem_polyGauss3_iotaWeight_archZeta30_ne_zero_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_archWhittakerDatum_of_isCasimirEigen_of_not_weightOne206 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 - Weight-one unfolded torus-pair identities with Γ-factors
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_weightOne_of_blockHarmonicOne_colHarmonic_gaussian348 below · depth 22 - Weight-one torus-pair identities for the conjugate-block Gaussian section
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_weightOne_of_conjBlockHarmonicOne_colHarmonic_gaussian373 below · depth 22 - Weight-one minor-section torus-pair identities with archimedean Γ-factors
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_weightOne_of_minorSection_gaussian347 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 - Weight ≥ 1 real Whittaker profiles: both parity sheets non-vanishing
LanglandsTunnell.Converse.ArchDatumR.exists_W_diagOne_add_mul_W_diagOne_neg_ne_zero_of_one_le_weight32 below · depth 23 - Parity of the torus profile at weight zero
LanglandsTunnell.CubicInduction.archDatumR_W_diagOne_neg_eq_of_weightZero11 below · depth 23 - Weight-one torus profile as Gaussian multiplicative convolution
LanglandsTunnell.CubicInduction.exists_archDatumR_W_diagOne_add_eq_mul_mulConvGaussian_of_weightOne29 below · depth 23 - Discrete-series torus profile of a real archimedean Whittaker datum
LanglandsTunnell.CubicInduction.exists_archDatumR_W_diagOne_eq_mul_exp_and_eq_zero_of_discrete16 below · depth 23 - Weight-zero torus profile is a Gaussian multiplicative convolution
LanglandsTunnell.CubicInduction.exists_archDatumR_W_diagOne_eq_mul_mulConvGaussian_of_weightZero16 below · depth 23 - Non-vanishing archimedean zeta integral for the weight-zero quadratic section
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_jacquetVector3_ne_zero_of_detPow_blockQuadratic_colHarmonicTwo_gaussian3_of_weightZero38 below · depth 23 - An admissible twist with non-vanishing archimedean GL₃ zeta integral
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_jacquetVector3_ne_zero_of_detPow_colHarmonic_gaussian362 below · depth 23 - Weight zero of the block-quadratic Gaussian Jacquet vector
LanglandsTunnell.CubicInduction.jacquetVector3_mul_iota_eq_archWeightChar_inv_mul_of_detPow_blockQuadratic_gaussian30 below · depth 23 - Explicit dual archimedean torus pair: root number times π(-1)ᶜρ times Γ-factor
LanglandsTunnell.RankinSelberg.exists_dualTorusPair_eq_archRootNumber_mul_explicit_mul_gammaFactor_of_weightOne_of_blockHarmonicOne_colHarmonic_gaussian3_of_profile36 below · depth 23 - Folded dual torus pair on the discrete branch, explicit constant
LanglandsTunnell.RankinSelberg.exists_dualTorusPair_eq_archRootNumber_mul_explicit_mul_gammaFactor_of_weightOne_of_conjBlockHarmonicOne_colHarmonic_gaussian3_of_discrete_profile28 below · depth 23 - Folded dual torus pair: root number, explicit constant, dual Γ-factors
LanglandsTunnell.RankinSelberg.exists_dualTorusPair_eq_archRootNumber_mul_explicit_mul_gammaFactor_of_weightOne_of_conjBlockHarmonicOne_colHarmonic_gaussian3_of_weightOne_profile28 below · depth 23 - Dual minor-section archimedean torus pair equals ε_∞ times Γ-factors
LanglandsTunnell.RankinSelberg.exists_dualTorusPair_eq_archRootNumber_mul_explicit_mul_gammaFactor_of_weightOne_of_minorSection_gaussian3_of_profile37 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 Hecke-local Whittaker function at a point trivial outside S_Q
LanglandsTunnell.RankinSelberg.exists_forall_localAt_eq_one_and_ne_zero_of_heckeLocal_of_levelOne_invariant9 below · depth 23 - Archimedean GL₃× GL₂ pair identity: discrete-series case
LanglandsTunnell.RankinSelberg.exists_mem_polyGauss3_iotaWeight_archZeta30_ne_zero_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_archWhittakerDatum_of_isCasimirEigen_of_discreteSeries141 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 - Even principal parameter: primal and dual unfolded torus-pair identities
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_evenPrincipal_of_detPow_blockQuadratic_colHarmonicTwo_gaussian351 below · depth 23 - Even principal torus-pair identities for a weight-zero Gaussian section
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_evenPrincipal_of_detPow_colHarmonic_gaussian378 below · depth 23 - Explicit unfolded archimedean torus pair, weight one, block-harmonic section
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_eq_explicit_mul_gammaFactor_of_weightOne_of_blockHarmonicOne_colHarmonic_gaussian3_of_profile31 below · depth 23 - Discrete-branch unfolded torus pair equals explicit Gamma-factor product
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_eq_explicit_mul_gammaFactor_of_weightOne_of_conjBlockHarmonicOne_colHarmonic_gaussian3_of_discrete_profile24 below · depth 23 - Weight-one unfolded torus pair as explicit Γ-factor product
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_eq_explicit_mul_gammaFactor_of_weightOne_of_conjBlockHarmonicOne_colHarmonic_gaussian3_of_weightOne_profile25 below · depth 23 - Explicit primal torus pair for the minor-section Jacquet vector
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_eq_explicit_mul_gammaFactor_of_weightOne_of_minorSection_gaussian3_of_profile31 below · depth 23 - Rankin–Selberg test data over ℚ for a cusp-realizable eigensystem
AutomorphicForm.exists_rankinSelberg_testData_of_isArithGenuineCuspRealizable_rat554 below · depth 24 - Non-vanishing archimedean zeta of a flat-section Jacquet vector
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_jacquetVector3_ne_zero_of_conjBlockHarmonic_pow_colHarmonic_gaussian389 below · depth 24 - Dual torus pair unfolded for the block-harmonic section
LanglandsTunnell.RankinSelberg.dualTorusPair_eq_setIntegral_dualConfig_of_weightOne_of_blockHarmonicOne_colHarmonic_gaussian35 below · depth 24 - Unfolded dual torus pair for the conjugate-harmonic weight-one section
LanglandsTunnell.RankinSelberg.dualTorusPair_eq_setIntegral_dualConfig_of_weightOne_of_conjBlockHarmonicOne_colHarmonic_gaussian35 below · depth 24 - Dual torus pair of the minor-section Jacquet vector, unfolded
LanglandsTunnell.RankinSelberg.dualTorusPair_eq_setIntegral_dualConfig_of_weightOne_of_minorSection_gaussian35 below · depth 24 - Dual torus pair with explicit constant 2π(-1)ᵇρ
LanglandsTunnell.RankinSelberg.exists_dualTorusPair_eq_archRootNumber_mul_explicit_mul_gammaFactor_of_evenPrincipal_of_detPow_blockQuadratic_colHarmonicTwo_gaussian3_of_profile37 below · depth 24 - Dual torus pair identity, discrete Levi branch
LanglandsTunnell.RankinSelberg.exists_dualTorusPair_eq_archRootNumber_mul_explicit_mul_gammaFactor_of_evenPrincipal_of_detPow_colHarmonic_gaussian3_of_discrete_profile25 below · depth 24 - Dual archimedean torus pair, weight-one Levi branch
LanglandsTunnell.RankinSelberg.exists_dualTorusPair_eq_archRootNumber_mul_explicit_mul_gammaFactor_of_evenPrincipal_of_detPow_colHarmonic_gaussian3_of_weightOne_profile25 below · depth 24 - Dual torus pair, even principal type, weight-zero Levi branch
LanglandsTunnell.RankinSelberg.exists_dualTorusPair_eq_archRootNumber_mul_explicit_mul_gammaFactor_of_evenPrincipal_of_detPow_colHarmonic_gaussian3_of_weightZero_profile36 below · depth 24 - Archimedean Rankin–Selberg integral of a discrete-series torus profile
LanglandsTunnell.RankinSelberg.exists_forall_rsArchIntegral_gaussian_eq_mul_Gamma_mul_Gamma_of_discreteSeries_torusPair3 below · depth 24 - Archimedean Rankin–Selberg integral against the Gaussian for torus profiles
LanglandsTunnell.RankinSelberg.exists_forall_rsArchIntegral_gaussian_eq_mul_Gamma_mul_mellin_of_torusProfile4 below · depth 24 - Rankin–Selberg side conditions for GL₂timesGL₂ over ℚ
LanglandsTunnell.RankinSelberg.exists_forall_summable_integrable_rs22_sideConditions_of_measurable_rat129 below · depth 24 - Unfolded torus pair in Iwasawa coordinates, block-harmonic Gaussian section
LanglandsTunnell.RankinSelberg.exists_forall_unfoldedTorusPair_eq_setIntegral_iwasawa_tateM_of_blockHarmonic_colHarmonic_gaussian34 below · depth 24 - Iwasawa–Tate evaluation of an unfolded archimedean torus integral
LanglandsTunnell.RankinSelberg.exists_forall_unfoldedTorusPair_eq_setIntegral_iwasawa_tateM_of_conjBlockHarmonic_colHarmonic_gaussian34 below · depth 24 - Iwasawa and Tate–Mellin form of the minor-section torus pair
LanglandsTunnell.RankinSelberg.exists_forall_unfoldedTorusPair_eq_setIntegral_iwasawa_tateM_of_minorSection_gaussian34 below · depth 24 - Archimedean GL₃× GL₂ torus-pair identity: discrete series, flat section
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_discreteSeries_of_conjBlockHarmonic_colHarmonic_gaussian391 below · depth 24 - Unfolded torus pair equals 2π(-1)ᵇρ times Gamma factors
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_eq_explicit_mul_gammaFactor_of_evenPrincipal_of_detPow_blockQuadratic_colHarmonicTwo_gaussian3_of_profile32 below · depth 24 - Unfolded torus pair equals (-1)ᵇ(π/2)ρ times Γ-product
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_eq_explicit_mul_gammaFactor_of_evenPrincipal_of_detPow_colHarmonic_gaussian3_of_discrete_profile19 below · depth 24 - Explicit unfolded torus pair: (-1)ᵇ(π/2)ρ times the twisted Γ-product
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_eq_explicit_mul_gammaFactor_of_evenPrincipal_of_detPow_colHarmonic_gaussian3_of_weightOne_profile18 below · depth 24 - Unfolded archimedean torus pair in the weight-zero Levi branch
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_eq_explicit_mul_gammaFactor_of_evenPrincipal_of_detPow_colHarmonic_gaussian3_of_weightZero_profile29 below · depth 24 - Rankin–Selberg unfolded integral over ℚ factorises into carriers
LanglandsTunnell.RankinSelberg.rs22WhittakerIntegral_rat_eq_rsArchIntegral_mul_rsFinIntegral_of_eq_mul8 below · depth 24 - Shaped unitary cusp vector over ℚ with factorised Whittaker function
AutomorphicForm.exists_unitaryShapedVector_whittakerFactorization_torusProfile_of_isArithGenuineCuspRealizable_rat544 below · depth 25 - Non-vanishing scalar in the weight-one torus profile identity
LanglandsTunnell.Converse.exists_ne_zero_and_W_diagOne_add_eq_mul_mulConvGaussian_of_weightOneLevi33 below · depth 25 - Non-vanishing scalar in the discrete-series Whittaker profile
LanglandsTunnell.Converse.exists_ne_zero_and_W_diagOne_eq_mul_exp_and_eq_zero_of_discreteLevi33 below · depth 25 - Non-vanishing scalar in the weight-zero torus profile
LanglandsTunnell.Converse.exists_ne_zero_and_W_diagOne_eq_mul_mulConvGaussian_of_weightZeroLevi17 below · depth 25 - Factorisation of the unipotent-quotient integral into archimedean and finite Rankin–Selberg factors
LanglandsTunnell.Converse.integral_unipotentQuotient_eq_rsArchIntegral_mul_rsFinIntegral4 below · depth 25 - Admissible twist with non-vanishing archimedean zeta, discrete branch
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_jacquetVector3_ne_zero_of_conjBlockHarmonic_pow_colHarmonic_gaussian3_of_discreteLevi39 below · depth 25 - Weight-one Levi branch: non-vanishing archimedean zeta of a Jacquet vector
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_jacquetVector3_ne_zero_of_conjBlockHarmonic_pow_colHarmonic_gaussian3_of_weightOneLevi38 below · depth 25 - Non-vanishing archimedean zeta integral, weight-zero Levi branch
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_jacquetVector3_ne_zero_of_conjBlockHarmonic_pow_colHarmonic_gaussian3_of_weightZeroLevi54 below · depth 25 - Dual Jacquet vector at a Siegel upper-unit torus point
LanglandsTunnell.CubicInduction.jacquetVector3_longWeyl3_transposeInv3_iota_upperUnit_eq0 below · depth 25 - One-sided Whittaker profile for a discrete-series archimedean parameter
LanglandsTunnell.RankinSelberg.archWhittaker_profile_eq_zero_and_eq_two_mul_cpow_mul_exp_of_discrete2 below · depth 25 - Archimedean Whittaker value at a reflected dual torus point
LanglandsTunnell.RankinSelberg.archWhittaker_w0R_mul_transposeInv_upperUnit_eq_mul_archProfile0 below · depth 25 - Dual torus pair unfolded for a quadratic Schwartz section
LanglandsTunnell.RankinSelberg.dualTorusPair_eq_setIntegral_dualConfig_of_evenPrincipal_of_detPow_blockQuadratic_colHarmonicTwo_gaussian34 below · depth 25 - Dual unfolding of the even-type archimedean torus pair
LanglandsTunnell.RankinSelberg.dualTorusPair_eq_setIntegral_dualConfig_of_evenPrincipal_of_detPow_colHarmonic_gaussian35 below · depth 25 - Integrability of the folded Rankin–Selberg integrand over ℚ
LanglandsTunnell.RankinSelberg.exists_forall_integrableOn_norm_mul_godementSection_majorant_rat78 below · depth 25 - Integrability of the archimedean Rankin–Selberg integrand over ℚ
LanglandsTunnell.RankinSelberg.exists_forall_integrable_archWhittaker_gaussian_rpow_det_rat4 below · depth 25 - Integrability of the finite Rankin–Selberg integrand over ℚ
LanglandsTunnell.RankinSelberg.exists_forall_integrable_finWhittaker_rpow_ideleNorm_det_rat29 below · depth 25 - Integrability of the Rankin–Selberg integrand on NbackslashGL₂(A_ℚ)
LanglandsTunnell.RankinSelberg.exists_forall_integrable_norm_whittakerCoefficient_mul_rs22Kernel_unipotentQuotient_rat40 below · depth 25 - Integrability of the split Rankin–Selberg integrand over ℚ
LanglandsTunnell.RankinSelberg.exists_forall_integrable_prod_archWhittaker_finWhittaker_rpow_rat34 below · depth 25 - Absolute convergence of the Bruhat series of a Godement section
LanglandsTunnell.RankinSelberg.exists_forall_summable_norm_godementSection_bruhat_one_one_rat85 below · depth 25 - Unfolded torus pair in Iwasawa coordinates with Tate–Mellin evaluation
LanglandsTunnell.RankinSelberg.exists_forall_unfoldedTorusPair_eq_setIntegral_iwasawa_tateM_of_colHarmonic_gaussian34 below · depth 25 - Iwasawa form of the unfolded torus pair, quadratic-block Gaussian datum
LanglandsTunnell.RankinSelberg.exists_forall_unfoldedTorusPair_eq_setIntegral_iwasawa_tateM_of_detPow_blockQuadratic_colHarmonic_gaussian34 below · depth 25 - Finite Rankin–Selberg integral constant in s and positive
LanglandsTunnell.RankinSelberg.exists_pos_forall_rsFinIntegral_eq_const_of_ideleNorm_det_eq_one_of_nonneg0 below · depth 25 - One-place disintegration of a finite-adelic unipotent quotient integral
LanglandsTunnell.RankinSelberg.exists_sFinite_forall_lintegral_withDensity_density_eq_lintegral_lintegral_mul_finFactor_placeEmbed11 below · depth 25 - Primal and dual torus integrals, discrete Levi branch with one complex place
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_discreteSeries_of_conjBlockHarmonic_colHarmonic_gaussian3_of_oneComplex_discreteLevi71 below · depth 25 - Torus-pair unfolding equals twisted Γ-factors: one complex place, k_ℂ=0
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_discreteSeries_of_conjBlockHarmonic_colHarmonic_gaussian3_of_oneComplex_weightOneLevi74 below · depth 25 - Primal and dual torus pairs: three real places, opposite signs
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_discreteSeries_of_conjBlockHarmonic_colHarmonic_gaussian3_of_threeReal_oppSign74 below · depth 25 - Torus pairs for three real places with equal Levi signs
LanglandsTunnell.RankinSelberg.exists_unfoldedTorusPair_and_dualTorusPair_eq_gammaFactor_of_discreteSeries_of_conjBlockHarmonic_colHarmonic_gaussian3_of_threeReal_sameSign58 below · depth 25 - Measurability of the unfolded Rankin–Selberg integrand over ℚ
LanglandsTunnell.RankinSelberg.forall_measurable_whittakerCoefficient_mul_rs22Kernel_rat2 below · depth 25 - Unipotent invariance of a product of two Whittaker coefficients
LanglandsTunnell.RankinSelberg.whittakerCoefficient_mul_whittakerCoefficient_inv_unipotent_mul_rat0 below · depth 25 - Shaped raw cusp vector over ℚ with unit-shell support
AutomorphicForm.exists_shapedRawVector_finWhittaker_support_transl_rat135 below · depth 26 - Unitary twist transports the shaped Whittaker package over ℚ
AutomorphicForm.unitaryTwist_transport_shapedRawVector_transl_rat102 below · depth 26 - Closed form of the dual torus integral, discrete Levi branch
LanglandsTunnell.RankinSelberg.exists_forall_dualTorusPair_eq_closedForm_of_discreteSeries_of_conjBlockHarmonic_colHarmonic_gaussian3_of_discreteLevi29 below · depth 26 - Closed form of the dual torus pair, weight-one Levi branch
LanglandsTunnell.RankinSelberg.exists_forall_dualTorusPair_eq_closedForm_of_discreteSeries_of_conjBlockHarmonic_colHarmonic_gaussian3_of_weightOneLevi32 below · depth 26 - Closed form of the dual torus pair: weight-zero Levi branch
LanglandsTunnell.RankinSelberg.exists_forall_dualTorusPair_eq_closedForm_of_discreteSeries_of_conjBlockHarmonic_colHarmonic_gaussian3_of_weightZeroLevi32 below · depth 26 - Bruhat-series majorant for Godement sections on rational Siegel sets
LanglandsTunnell.RankinSelberg.exists_forall_norm_godementSection_add_tsum_le_mul_archHeight_pow_of_mem_integralWindowedSiegelSet_rat76 below · depth 26 - Closed form of the unfolded torus pair: discrete Levi branch
LanglandsTunnell.RankinSelberg.exists_forall_unfoldedTorusPair_eq_closedForm_of_discreteSeries_of_conjBlockHarmonic_colHarmonic_gaussian3_of_discreteLevi_ed224 below · depth 26
… and 27 more statements (search for the module name to find them).