Definitions/Def_AutomorphicForm_UnipotentQuotient.lean
Adelic unipotent subgroup, its Haar measure, quotient measure
Throughout, K is a number field, \mathbb{A}_K its adele ring and \mathrm{GL}_2(\mathbb{A}_K) the adelic general linear group, both carrying the Borel \sigma-algebras of their adelic topologies. Four objects are introduced. First, adelicUnipotent K is the range of the homomorphism unipotentGL2Hom over \mathbb{A}_K, i.e. the subgroup N(\mathbb{A}_K)=\{\,n(x)=\begin{pmatrix}1&x\\0&1\end{pmatrix} : x\in\mathbb{A}_K\,\} of \mathrm{GL}_2(\mathbb{A}_K), obtained from the additive group \mathbb{A}_K viewed multiplicatively via n(x+y)=n(x)n(y). Second, UnipotentQuotient K is the orbit space of the left multiplication action of that subgroup on \mathrm{GL}_2(\mathbb{A}_K), that is the coset space N(\mathbb{A}_K)\backslash\mathrm{GL}_2(\mathbb{A}_K), with the quotient measurable structure. Third, toAdelicUnipotent K is the surjection x\mapsto n(x) from \mathbb{A}_K onto N(\mathbb{A}_K), the homomorphism n restricted to its range. Fourth, unipotentHaar K is the image under this surjection of the additive Haar measure adelicAddHaar of \mathbb{A}_K rescaled by the factor \bigl(\mathrm{vol}(\mathtt{adelicBox}\,K)\bigr)^{-1}, where adelicBox K consists of the adeles whose infinite component lies in the preimage of the fundamental domain of the lattice basis of K in the mixed space and whose finite component is integral at every finite place; thus the scaling is the one making that box have total mass one.
Finally, unipotentQuotientMeasure K is the measure on N(\mathbb{A}_K)\backslash\mathrm{GL}_2(\mathbb{A}_K) given by HaarQuotient.measure applied to the Haar measure adelicGLHaar of \mathrm{GL}_2(\mathbb{A}_K), the subgroup N(\mathbb{A}_K) and the measure unipotentHaar K: the pushforward along the quotient map of adelicGLHaar weighted by the density g\mapsto w(g)\big/\int_{N(\mathbb{A}_K)} w(xg)\,d\,\mathtt{unipotentHaar}(x), with w the weight function built from a compact exhaustion of the group.
Relation to Mathlib
The underlying Haar measures are Mathlib's Measure.addHaar and Measure.haar for the adelic topologies; the coset space is Mathlib's orbit-space quotient. The density-and-pushforward construction HaarQuotient.measure used for the quotient measure is the project's own, rather than Mathlib's quotient-Haar machinery for discrete subgroups with a fundamental domain.
Where it is used
These objects provide the adelic unipotent group and the measures in which the constant term of an adelic automorphic form on \mathrm{GL}_2 (integration over N(\mathbb{A}_K), normalised as here) and the L^2 condition on N(\mathbb{A}_K)\backslash\mathrm{GL}_2(\mathbb{A}_K) are formulated, on the automorphic side of the modularity argument.
References
- A. Weil, Basic Number Theory, Grundlehren der mathematischen Wissenschaften 144, Springer, 1974
- S. Gelbart, Automorphic Forms on Adele Groups, Annals of Mathematics Studies 83, Princeton University Press, 1975
References are suggested automatically and have not been individually verified.
English text generated automatically from the Lean source; the Lean statement is authoritative.
- 37 lines
- 5 declarations
- used in the statements of 68 theorems and imported by 77 proofs
- imports 5 definition modules
Source file: Definitions/Def_AutomorphicForm_UnipotentQuotient.lean
Imports
Declarations
- abbrev
AutomorphicForm.adelicUnipotent - abbrev
AutomorphicForm.UnipotentQuotient - def
AutomorphicForm.toAdelicUnipotent - def
AutomorphicForm.unipotentHaar - def
AutomorphicForm.unipotentQuotientMeasure
Source
import Definitions.Def_AutomorphicForm_ConstantTerm import Definitions.Def_AutomorphicForm_AdelicLsXi import Definitions.Def_NumberField_AdelicHaar import Definitions.Def_NumberField_AdelicBox import Definitions.Def_HaarQuotient open MeasureTheory NumberField NumberField.AdelicHaar NumberField.AdelicBox noncomputable section namespace AutomorphicForm attribute [local instance] NumberField.AdelicHaar.glBorel NumberField.AdelicHaar.borelSpace_glBorel NumberField.AdelicHaar.adeleBorel NumberField.AdelicHaar.borelSpace_adeleBorel variable (K : Type*) [Field K] [NumberField K] abbrev adelicUnipotent : Subgroup (AdelicGL2 (𝓞 K) K) := (unipotentGL2Hom (R := AdeleRing (𝓞 K) K)).range abbrev UnipotentQuotient : Type _ := MulAction.orbitRel.Quotient (adelicUnipotent K) (AdelicGL2 (𝓞 K) K) def toAdelicUnipotent (x : AdeleRing (𝓞 K) K) : adelicUnipotent K := (unipotentGL2Hom (R := AdeleRing (𝓞 K) K)).rangeRestrict (Multiplicative.ofAdd x) def unipotentHaar : Measure (adelicUnipotent K) := Measure.map (toAdelicUnipotent K) (((adelicAddHaar (𝓞 K) K) (adelicBox K))⁻¹ • adelicAddHaar (𝓞 K) K) def unipotentQuotientMeasure : Measure (UnipotentQuotient K) := HaarQuotient.measure (adelicGLHaar (Fin 2) (𝓞 K) K) (adelicUnipotent K) (unipotentHaar K) end AutomorphicForm end
Statements phrased using this module (68)
- Central translation invariance of the unipotent-quotient integral
AutomorphicForm.integral_unipotentQuotient_out_mul_of_central3 below · depth 18 - The adelic unipotent subgroup is closed in GL₂(A_K)
AutomorphicForm.isClosed_adelicUnipotent0 below · depth 18 - Normalised unipotent adelic measure is a bi-invariant Haar measure
AutomorphicForm.isHaarMeasure_and_isMulRightInvariant_unipotentHaar0 below · depth 18 - Unfolding the Haar integral on GL₂(A_K) along N(A_K)
AutomorphicForm.lintegral_adelicGLHaar_eq_mul_lintegral_unipotentQuotientMeasure2 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 - 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 - 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 - Two-sided unfolding of the GL₂timesGL₃ Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.exists_ne_zero_forall_rsGlobalIntegral_eq_mul_integral_unipotentQuotient_whittakerCoefficient_mul_of_hasSum_mirabolicTranslate_and_dual13 below · depth 18 - Integrability of the unfolded GL₂timesGL₃ Rankin–Selberg integrand
LanglandsTunnell.RankinSelberg.integrable_unipotentQuotient_whittakerCoefficient_mul_of_hasSum_mirabolicTranslate_and_dual13 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 - Measurability of unipotent integrals on N(A_K)backslashGL₂(A_K)
AutomorphicForm.measurable_lintegral_unipotentGL2_mul_out2 below · depth 19 - Unfolding along the unipotent subgroup of adelic GL₂
AutomorphicForm.setLIntegral_adelicGLHaar_eq_lintegral_unipotentQuotientMeasure2 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 - 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 - 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 - 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 - Unfolding the global GL₂timesGL₃ Rankin–Selberg integral, primal and dual
LanglandsTunnell.RankinSelberg.exists_ne_zero_forall_rsGlobalIntegral_eq_mul_integral_unipotentQuotient_whittakerCoefficient_mul_of_hasSum_mirabolicTranslate_and_dual_rpow13 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 - Integrability of the unfolded Rankin–Selberg integrand, primal and dual
LanglandsTunnell.RankinSelberg.integrable_unipotentQuotient_whittakerCoefficient_mul_of_hasSum_mirabolicTranslate_and_dual_rpow13 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 - Uncountable non-vanishing of the cut finite Rankin–Selberg factor
LanglandsTunnell.RankinSelberg.exists_finTranslate_not_countable_rsFinIntegral_indicator_ne_zero_of_purifier_of_finiteFamily_arch93 below · depth 22 - Frozen complements: explicit p-slot splitting of GL₃ Whittaker functions
LanglandsTunnell.RankinSelberg.exists_frozen_forall_sum_translate_whittaker_iota_eq_mul_pSlot_of_finiteFamily_arch_explicit42 below · depth 22 - Factorisation of the purified reference Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.exists_ne_zero_forall_rsGlobalIntegral_reference_eq_mul_rsArchIntegral_mul_rsFinIntegral_indicator_mul_of_finiteFamily_arch410 below · depth 22 - A p-adic purifier with pure-tensor Whittaker coefficient
LanglandsTunnell.RankinSelberg.exists_purifier_whittakerCoefficient_eq_mul_pSlot_of_finiteFamily_arch25 below · depth 22 - Independent tensor splitting of the finite Whittaker factor
AutomorphicForm.exists_finWhittaker_eq_sum_prod_mul_linearIndependent_levelOne_invariant_of_isIsotypicCuspFormAt_of_localSpaceAt15 below · depth 23 - Local integrability of the Rankin–Selberg integrand at p
LanglandsTunnell.RankinSelberg.exists_forall_integrable_iotaGL_mul_of_mem_span_localSpaceAt_of_mem_gl3CyclicSubspace_twist_of_finiteFamily_arch40 below · depth 23 - Euler factorisation of the cut finite Rankin–Selberg integral
LanglandsTunnell.RankinSelberg.exists_ne_zero_forall_rsFinIntegral_indicator_purified_eq_mul_sum_prod_rsLocalIntegral36 below · depth 23 - Rankin–Selberg side conditions for GL₂timesGL₂ over ℚ
LanglandsTunnell.RankinSelberg.exists_forall_summable_integrable_rs22_sideConditions_of_measurable_rat129 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 - Factorisation of the unipotent-quotient integral into archimedean and finite Rankin–Selberg factors
LanglandsTunnell.Converse.integral_unipotentQuotient_eq_rsArchIntegral_mul_rsFinIntegral4 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 - 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 - 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