Definitions/Def_LanglandsTunnell_CubicInduction_MirabolicMajorant.lean
Root sizes and gauge majorants for adelic
Over a normed field L, six sizes are attached to k \in \mathrm{GL}_3(L) (rows and columns indexed by \{0,1,2\}): lastRowSup is the maximum of \|k_{2j}\| for j=0,1,2; bottomMinor k j j' is the 2\times 2 minor k_{1j}k_{2j'}-k_{1j'}k_{2j} formed from the last two rows and the columns j,j'; minorSup is the maximum of the norms of the three minors with (j,j')=(0,1),(0,2),(1,2); lastRowEucl and minorEucl are the corresponding Euclidean (\ell^2) sizes, i.e. the square roots of the sums of the squares of the same three norms; and detSize is \|\det k\|. For a number field F and g \in \mathrm{GL}_3(\mathbf{A}_F), two root sizes are formed at each place from the local component of g: at a finite place v, \mathrm{finRoot}_1 = d\cdot r/m^2 and \mathrm{finRoot}_2 = m/r^2 with d,r,m the determinant size, last-row sup-size and minor sup-size of the component at v; at an infinite place w the same formulas with the Euclidean sizes of the component at w. Division here follows the Lean convention (quotients by 0 are 0); no nondegeneracy is imposed. rootSizeProd multiplies the finprod over all finite places of \mathrm{finRoot}_1\cdot\mathrm{finRoot}_2 by the finite product of \mathrm{archRoot}_1\cdot\mathrm{archRoot}_2 over infinite places, and archRootSum sums \mathrm{archRoot}_1+\mathrm{archRoot}_2 over infinite places. InRootLevel T B g asks that both finite root sizes be \le 1 at every finite place outside a finite set T and \le B at places of T. Finally IsGaugeMajorised3 W, for W : \mathrm{GL}_3(\mathbf{A}_F) \to \mathbb{C}, asserts the existence of t \in \mathbb{N}, a finite set T of finite places and B \in \mathbb{R} such that for every N \in \mathbb{N} there is C \in \mathbb{R} with: W(g)=0 whenever InRootLevel fails, and \|W(g)\| \le C/(\mathrm{rootSizeProd}(g)^t (1+\mathrm{archRootSum}(g))^N) whenever it holds. The accompanying lemma records that the zero function is gauge-majorised (with t=0, T=\emptyset, B=1, C=0).
Relation to Mathlib
Mathlib supplies the ambient objects (the adele ring, the height-one spectrum, infinite places and their completions, and finprod) but has no notion of these root sizes or of gauge majorisation; both are the project's own.
Where it is used
These sizes implement the two simple roots of \mathrm{GL}_3 in matrix terms, and the majorisation predicate is the decay condition imposed on Whittaker-type functions in the \mathrm{GL}_3 induction step used for the Langlands–Tunnell theorem, which supplies modularity of the mod 3 representation in the Fermat argument.
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. Darmon, F. Diamond and R. Taylor, Fermat's Last Theorem, in: Current Developments in Mathematics 1995, International Press, 1995, 1–154, §3
References are suggested automatically and have not been individually verified.
English text generated automatically from the Lean source; the Lean statement is authoritative.
- 79 lines
- 15 declarations
- used in the statements of 361 theorems and imported by 382 proofs
- imports 1 definition modules
Source file: Definitions/Def_LanglandsTunnell_CubicInduction_MirabolicMajorant.lean
Imported by
- no other definition module
Declarations
- def
LanglandsTunnell.CubicInduction.lastRowSup - def
LanglandsTunnell.CubicInduction.bottomMinor - def
LanglandsTunnell.CubicInduction.minorSup - def
LanglandsTunnell.CubicInduction.lastRowEucl - def
LanglandsTunnell.CubicInduction.minorEucl - def
LanglandsTunnell.CubicInduction.detSize - def
LanglandsTunnell.CubicInduction.finRoot₁ - def
LanglandsTunnell.CubicInduction.finRoot₂ - def
LanglandsTunnell.CubicInduction.archRoot₁ - def
LanglandsTunnell.CubicInduction.archRoot₂ - def
LanglandsTunnell.CubicInduction.rootSizeProd - def
LanglandsTunnell.CubicInduction.archRootSum - def
LanglandsTunnell.CubicInduction.InRootLevel - def
LanglandsTunnell.CubicInduction.IsGaugeMajorised3 - theorem
LanglandsTunnell.CubicInduction.isGaugeMajorised3_zero
Source
import Definitions.Def_LanglandsTunnell_CubicInduction_Growth set_option autoImplicit false open IsDedekindDomain NumberField Matrix noncomputable section namespace LanglandsTunnell.CubicInduction section Sizes variable {L : Type*} [NormedField L] def lastRowSup (k : GL (Fin 3) L) : ℝ := max (max ‖(k : Matrix (Fin 3) (Fin 3) L) 2 0‖ ‖(k : Matrix (Fin 3) (Fin 3) L) 2 1‖) ‖(k : Matrix (Fin 3) (Fin 3) L) 2 2‖ def bottomMinor (k : GL (Fin 3) L) (j j' : Fin 3) : L := (k : Matrix (Fin 3) (Fin 3) L) 1 j * (k : Matrix (Fin 3) (Fin 3) L) 2 j' - (k : Matrix (Fin 3) (Fin 3) L) 1 j' * (k : Matrix (Fin 3) (Fin 3) L) 2 j def minorSup (k : GL (Fin 3) L) : ℝ := max (max ‖bottomMinor k 0 1‖ ‖bottomMinor k 0 2‖) ‖bottomMinor k 1 2‖ def lastRowEucl (k : GL (Fin 3) L) : ℝ := Real.sqrt (‖(k : Matrix (Fin 3) (Fin 3) L) 2 0‖ ^ 2 + ‖(k : Matrix (Fin 3) (Fin 3) L) 2 1‖ ^ 2 + ‖(k : Matrix (Fin 3) (Fin 3) L) 2 2‖ ^ 2) def minorEucl (k : GL (Fin 3) L) : ℝ := Real.sqrt (‖bottomMinor k 0 1‖ ^ 2 + ‖bottomMinor k 0 2‖ ^ 2 + ‖bottomMinor k 1 2‖ ^ 2) def detSize (k : GL (Fin 3) L) : ℝ := ‖(k : Matrix (Fin 3) (Fin 3) L).det‖ end Sizes section Roots variable (F : Type) [Field F] [NumberField F] def finRoot₁ (v : HeightOneSpectrum (𝓞 F)) (g : AdelicGL 3 (𝓞 F) F) : ℝ := detSize (componentAt3 (𝓞 F) F v g) * lastRowSup (componentAt3 (𝓞 F) F v g) / minorSup (componentAt3 (𝓞 F) F v g) ^ 2 def finRoot₂ (v : HeightOneSpectrum (𝓞 F)) (g : AdelicGL 3 (𝓞 F) F) : ℝ := minorSup (componentAt3 (𝓞 F) F v g) / lastRowSup (componentAt3 (𝓞 F) F v g) ^ 2 def archRoot₁ (w : InfinitePlace F) (g : AdelicGL 3 (𝓞 F) F) : ℝ := detSize (archPlaceComponent3 F w g) * lastRowEucl (archPlaceComponent3 F w g) / minorEucl (archPlaceComponent3 F w g) ^ 2 def archRoot₂ (w : InfinitePlace F) (g : AdelicGL 3 (𝓞 F) F) : ℝ := minorEucl (archPlaceComponent3 F w g) / lastRowEucl (archPlaceComponent3 F w g) ^ 2 def rootSizeProd (g : AdelicGL 3 (𝓞 F) F) : ℝ := (∏ᶠ v : HeightOneSpectrum (𝓞 F), finRoot₁ F v g * finRoot₂ F v g) * ∏ w : InfinitePlace F, archRoot₁ F w g * archRoot₂ F w g def archRootSum (g : AdelicGL 3 (𝓞 F) F) : ℝ := ∑ w : InfinitePlace F, (archRoot₁ F w g + archRoot₂ F w g) def InRootLevel (T : Finset (HeightOneSpectrum (𝓞 F))) (B : ℝ) (g : AdelicGL 3 (𝓞 F) F) : Prop := (∀ v, v ∉ T → finRoot₁ F v g ≤ 1 ∧ finRoot₂ F v g ≤ 1) ∧ ∀ v ∈ T, finRoot₁ F v g ≤ B ∧ finRoot₂ F v g ≤ B def IsGaugeMajorised3 (W : AdelicGL 3 (𝓞 F) F → ℂ) : Prop := ∃ (t : ℕ) (T : Finset (HeightOneSpectrum (𝓞 F))) (B : ℝ), ∀ N : ℕ, ∃ C : ℝ, ∀ g : AdelicGL 3 (𝓞 F) F, (¬ InRootLevel F T B g → W g = 0) ∧ (InRootLevel F T B g → ‖W g‖ ≤ C / (rootSizeProd F g ^ t * (1 + archRootSum F g) ^ N)) theorem isGaugeMajorised3_zero : IsGaugeMajorised3 F (fun _ => (0 : ℂ)) := ⟨0, ∅, 1, fun N => ⟨0, fun g => ⟨fun _ => rfl, fun _ => by simp⟩⟩⟩ end Roots end LanglandsTunnell.CubicInduction
Statements phrased using this module (361)
- Twisting a cubic induction form by a character of the determinant
LanglandsTunnell.CubicInduction.CubicInductionForm.twist_det_package2 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 - Gauge majorant descends to the local Whittaker function at v
LanglandsTunnell.CubicInduction.exists_gauge_whittakerLoc_of_isGaugeMajorised3_of_form_ne_zero0 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 - Local GL₃timesGL₂ functional equation on the cyclic space
LanglandsTunnell.CubicInduction.forall_mem_gl3CyclicSubspace_rsLocalIntegral_fe32_of_forall_localZeta31_fe_of_gauge87 below · depth 18 - Finiteness of torus coefficients in the twisted local cyclic space
LanglandsTunnell.CubicInduction.forall_mem_gl3CyclicSubspace_torusFinite_of_cubicInductionForm_twisted_noFE32_level19 below · depth 18 - Cubic automorphic induction: existence of a cubic induction form
LanglandsTunnell.CubicInduction.hasCubicInductionForm_arch_torusValues_localPackage_bad1,687 below · depth 18 - Right translation stability of cubic-induction Whittaker data
LanglandsTunnell.CubicInduction.isGaugeMajorised3_hasIotaMoments_hasWhittakerHalfPlane_comp_mul_right28 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 - 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 - Archimedean root sizes of a GL₂ block image and its dual
LanglandsTunnell.CubicInduction.archRoot_iota_archRealGLAt_and_dual0 below · depth 19 - Local GL₃timesGL₁ constants of a cubic induction at one bad place
LanglandsTunnell.CubicInduction.exists_forall_mem_gl3CyclicSubspace_localZetaDual31_eq_mul_of_isCubicInductionDataOn_deepAt539 below · depth 19 - Span-wide local constants for deep cubic induction data
LanglandsTunnell.CubicInduction.exists_forall_mem_gl3CyclicSubspace_localZetaDual31_eq_mul_of_isCubicInductionDataOn_deep_badPlaces550 below · depth 19 - Existence of a cubic-induction datum: archimedean and bad-place package
LanglandsTunnell.CubicInduction.exists_isCubicInductionDataOn_arch_torusValues_localPackage_bad1,686 below · depth 19 - Re-choosing one local Whittaker factor within its cyclic span
LanglandsTunnell.CubicInduction.exists_isCubicInductionDataOn_whittakerLoc_eq_of_mem_gl3CyclicSubspace28 below · depth 19 - Normalising cubic induction data at bad places
LanglandsTunnell.CubicInduction.exists_isCubicInductionDataOn_whittakerLoc_one_eq_one_of_isBadPlace31 below · depth 19 - Gauge majorisation passes to cyclic translates and duals on GL₃
LanglandsTunnell.CubicInduction.forall_mem_gl3CyclicSubspace_exists_gauge_and_exists_gauge_dualWhittakerFn30 below · depth 19 - Two-sided determinant moments from gauge-majorised mirabolic expansions
LanglandsTunnell.CubicInduction.hasIotaMoments_of_hasSum_mirabolicTranslate_of_isGaugeMajorised326 below · depth 19 - Gauge majorisation passes to spans of right translates
LanglandsTunnell.CubicInduction.isGaugeMajorised3_of_mem_gl3CyclicSubspace0 below · depth 19 - Archimedean zeta package for an explicit GL₃ Whittaker vector
LanglandsTunnell.CubicInduction.jacquetVector3_archZeta_package32 below · depth 19 - Multiplicativity of the local GL₃timesGL₂ functional equation, unramified partner
LanglandsTunnell.CubicInduction.rsLocalIntegral_fe32_of_forall_localZeta31_fe_of_gauge86 below · depth 19 - Mirabolic series and integrals of a gauge-majorised function on GL₃
LanglandsTunnell.CubicInduction.summable_growth_continuous_halfPlane_integrable_of_isGaugeMajorised325 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 - 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 - 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 - 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 - Modulus of a real Whittaker function on torus times O(2)
LanglandsTunnell.RankinSelberg.norm_archWhittaker_upperUnit_mul_rowIsometry0 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 - Archimedean functional equation for the induced GL₃ zeta integrals
LanglandsTunnell.CubicInduction.archZetaDual31_jacquetVector3_mul_archFactor_eq12 below · depth 20 - Continuity and gauge majorisation of factorisable functions on adelic GL₃
LanglandsTunnell.CubicInduction.continuous_and_isGaugeMajorised3_of_eq_mul_prod0 below · depth 20 - Explicit root number in the GL₃ functional equation at v
LanglandsTunnell.CubicInduction.eval_mul_eq_finprod_rootNumber_mul_eval_of_forall_localZeta31_fe_one_of_isCubicInductionDataOn_of_addCharLevel493 below · depth 20 - Local rationality and functional equation at a bad place
LanglandsTunnell.CubicInduction.exists_forall_exists_mul_eval_eq_of_isCubicInductionDataOn_of_forall_mem_bad_of_addCharLevel514 below · depth 20 - Local Whittaker data at bad places of a saturated cubic induction
LanglandsTunnell.CubicInduction.exists_forall_le_exists_localWhittaker_saturated_and_laurent_fe_of_mem_bad65 below · depth 20 - Uniform root-size bound for induced spherical Whittaker functions
LanglandsTunnell.CubicInduction.exists_forall_rootSize_bound_of_isInducedSphericalAt_of_isUnitaryChar3 below · depth 20 - Conductor bound for the local central character at unramified v
LanglandsTunnell.CubicInduction.exists_hasConductorExponentAt_localChar_centralChar_le_inducedLevelAt_of_isCubicInductionDataOn278 below · depth 20 - Odd admissible twist with non-vanishing archimedean GL₃ × GL₁ zeta
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_ne_zero_odd_of_isCubicInductionDataOn6 below · depth 20 - Archimedean zeta non-vanishing far right for a suitable translate
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_archZeta30_ne_zero_of_isCubicInductionDataOn1 below · depth 20 - Re-choosing one local Whittaker factor within its cyclic span
LanglandsTunnell.CubicInduction.exists_isCubicInductionDataOn_whittakerLoc_eq_of_mem_gl3CyclicSubspace_of_isOpen29 below · depth 20 - Local newvector of level K₁(ℓᵥ) at twist-ramified primes
LanglandsTunnell.CubicInduction.exists_mem_gl3CyclicSubspace_congruenceK1_torusValues_of_isCubicInductionDataOn615 below · depth 20 - Congruence-invariant vector in the local cyclic space at a ramified bad place
LanglandsTunnell.CubicInduction.exists_mem_gl3CyclicSubspace_principalLevel_le_of_isRamifiedIn_of_isCubicInductionDataOn_of_conductorBound615 below · depth 20 - A twist-independent constant in the deep-place GL₃× GL₁ functional equation
LanglandsTunnell.CubicInduction.exists_ne_zero_forall_eval_mul_eq_mul_rootNumber_mul_eval_of_forall_localZeta31_fe_twist_of_isCubicInductionDataOn_of_deep_of_archPackage_of_inv_eq_psiQ_of_whittakerLoc_one502 below · depth 20 - Root-size support and growth bound for local GL₃ Whittaker functions
LanglandsTunnell.CubicInduction.exists_rootSize_bound_of_isGL3PsiWhittakerFn1 below · depth 20 - Convergence and rationality of local GL₃× GL₂ Rankin–Selberg integrals
LanglandsTunnell.CubicInduction.exists_rsLocalIntegral_and_dual_integrable_and_eq_rational_sphericalWhittaker_of_forall_localZeta31_fe_of_gauge13 below · depth 20 - Converse-theorem input for the cubic induction from an archimedean Whittaker vector
LanglandsTunnell.CubicInduction.exists_whittaker_zeta_fe_of_forall_not_mem_isInducedSphericalAt_of_arch145 below · depth 20 - Product formula (prodᵥλᵥ²) λ_∞²=1 for a cubic induction
LanglandsTunnell.CubicInduction.finprod_sq_mul_lamSqArch_eq_one_of_forall_ne_zero_localZeta31_fe_rootNumber_of_isCubicInductionDataOn_of_archPackage_of_inv_eq_psiQ538 below · depth 20 - Twisting a cubic idelic character by χ ∘ N
LanglandsTunnell.CubicInduction.inducedCoeff_mul_comp_idelicNorm_and_isBadPlace_iff_of_conductorExponentAt_le24 below · depth 20 - Rapid decay of the GL₃ Jacquet–Whittaker vector
LanglandsTunnell.CubicInduction.jacquetVector3_norm_archComponent3_le6 below · depth 20 - Identified local functional equation passes to the cyclic span
LanglandsTunnell.CubicInduction.localZeta31_identified_of_mem_gl3CyclicSubspace1 below · depth 20 - Non-norm condition is stable under twisting by base-changed characters
LanglandsTunnell.CubicInduction.not_exists_eq_pow_inertiaDeg_mul_comp_idelicNorm_of_not_exists12 below · depth 20 - Local γ-factor identity for GL₃× GL₂ with gauge majorant
LanglandsTunnell.CubicInduction.rsLocalIntegral_fe32_of_eq_rational_of_forall_localZeta31_fe_of_gauge85 below · depth 20 - S-part integrability of the GL₃ zeta and dual integrands
LanglandsTunnell.CubicInduction.sPart_integrable_and_dual_of_isCubicInductionDataOn_of_isGaugeMajorised353 below · depth 20 - Central character law for the archimedean Whittaker function
LanglandsTunnell.CubicInduction.whittakerArch_scalar_mul_eq_centralChar_mul_of_isCubicInductionDataOn0 below · depth 20 - Global realisation of local Rankin–Selberg pairs at p
LanglandsTunnell.RankinSelberg.exists_factor_fundamentalDomain_forall_rsGlobalIntegral_realisation_member_twisted_of_finiteFamily_arch_of_archNonvanishing467 below · depth 20 - Cut-off remainder integrands of the dual finite cell are integrable
LanglandsTunnell.RankinSelberg.exists_forall_integrable_cutoff_remainder_mul_finprod_away113 below · depth 20 - Half-plane integrability of primal and dual finite cell integrands
LanglandsTunnell.RankinSelberg.exists_forall_integrable_rsFinCellIntegrand_translate_and_dual104 below · depth 20 - 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 - 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 - Normalised K₁(mathfrak pᵥ^ℓ)-newvector from a trivial-Euler functional equation
LanglandsTunnell.RankinSelberg.exists_normalisedNewvector_of_isLocalWhittakerDatum_of_localFE32_spherical_of_eulerPoly_eq_one21 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 - Spherical Rankin–Selberg periods determine torus values
LanglandsTunnell.RankinSelberg.forall_apply_diagZ_mul_scalarPi_pow_eq_ite_of_forall_rsLocalIntegral_spherical_eq_measure6 below · depth 20 - Vanishing of K₁-invariant GL₃ Whittaker values off the dominant cone
LanglandsTunnell.RankinSelberg.forall_apply_iotaGL_diagZ_mul_scalarPi_zpow_eq_zero_of_isGL3PsiWhittakerFn_of_congruenceK16 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 - Convergence and rationality of local GL₃timesGL₂ Rankin–Selberg integrals
LanglandsTunnell.RankinSelberg.forall_rsLocalIntegral_integrable_and_eq_laurent_of_torusFinite_of_centralChar_of_shellGrowth20 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 - Smoothness, admissibility and inverse Whittaker law for the dual function
LanglandsTunnell.CubicInduction.admissible_gl3CyclicSubspace_dualWhittakerFn3_rightTranslate1 below · depth 21 - Entire continuation and functional equation of GL₃ zeta integrals
LanglandsTunnell.CubicInduction.exists_entire_eq_globalZeta30_eq_mul_globalZetaDual31_of_isCubicInductionDataOn42 below · depth 21 - Convergence of the local GL₃timesGL₂ Rankin–Selberg integral
LanglandsTunnell.CubicInduction.exists_forall_integrable_rsLocalIntegrand_of_gauge8 below · depth 21 - Vanishing of GL₃ cell-section Whittaker functions outside a cone
LanglandsTunnell.CubicInduction.exists_forall_jacquetWhittaker3_eq_zero_of_rootSize_gt14 below · depth 21 - Local gauge bound for the cubic Whittaker function
LanglandsTunnell.CubicInduction.exists_gauge_whittakerLoc_of_isGaugeMajorised3_of_form_ne_zero_of_isCubicInductionDataOn0 below · depth 21 - Non-vanishing of the local GL₃× GL₁ zeta integral
LanglandsTunnell.CubicInduction.exists_isLocalZeta30ConvergentAbove_and_forall_exists_localZeta30_ne_zero_of_admissible_of_ne_zero13 below · depth 21 - Local zeta functional equation at a ramified place
LanglandsTunnell.CubicInduction.exists_localZeta31_fe_one_inducedEulerPoly_rational_of_isCubicInductionDataOn_of_isRamifiedIn527 below · depth 21 - Local functional equation at a bad place unramified in K
LanglandsTunnell.CubicInduction.exists_localZeta31_fe_one_inducedEulerPoly_rational_of_isCubicInductionDataOn_of_not_isRamifiedIn527 below · depth 21 - K-invariant vector in the cyclic span with unchanged local integrals
LanglandsTunnell.CubicInduction.exists_mem_gl3CyclicSubspace_iotaGL_invariant_rsLocalIntegral_eq9 below · depth 21 - Unfolded (3,2) functional equation for deformed spherical vectors
LanglandsTunnell.CubicInduction.exists_mvPolynomial_forall_dominant_rsLocalIntegral_deformedSpherical_eq_and_fe_of_forall_localZeta31_fe_of_gauge80 below · depth 21 - Rationality of the local GL₃timesGL₂ Rankin–Selberg integral
LanglandsTunnell.CubicInduction.exists_mvPolynomial_forall_rsLocalIntegral_mul_eq_eval_of_iotaGL_invariant14 below · depth 21 - Gauge bound for GL₃ Jacquet–Whittaker cell functions
LanglandsTunnell.CubicInduction.exists_norm_jacquetWhittaker3_le_of_rootSize_le14 below · depth 21 - Normalised K₁(v^ℓ)-newvector with prescribed Rankin–Selberg integral
LanglandsTunnell.CubicInduction.exists_normalisedNewvector_of_isLocalWhittakerDatum_of_localFE32_of_inducedE3_eq_zero42 below · depth 21 - Newvector in the cyclic span from local GL₃timesGL₂ functional equations
LanglandsTunnell.CubicInduction.exists_normalisedNewvector_of_isLocalWhittakerDatum_of_localFE32_of_ne_zero42 below · depth 21 - Three local characters at a bad prime of cubic induction
LanglandsTunnell.CubicInduction.exists_prod_eq_localChar_and_prod_stdRootNumberAt_eq_of_saturated21 below · depth 21 - Spherical torus values from Rankin–Selberg local integrals
LanglandsTunnell.CubicInduction.hasSphericalTorusValuesAt_inducedCoeff_of_rsLocalIntegral_eq_cellVolume17 below · depth 21 - No cubic term at primes ramified in a cubic field
LanglandsTunnell.CubicInduction.inducedE3_eq_zero_of_isRamifiedIn_of_finrank_eq_three0 below · depth 21 - Jacquet vector at a real diagonal torus element, unfolded
LanglandsTunnell.CubicInduction.jacquetVector3_iota_upperUnit_eq_integral_godementInner3_mulShift0 below · depth 21 - Sign-flip transport of the local GL₃ package, gauge edition
LanglandsTunnell.CubicInduction.localPackage_psiLocal_inv_comp_mul_diagonal_of_localPackage_psiLocal_of_gauge2 below · depth 21 - Place separation for local zeta quotients at a bad place
LanglandsTunnell.CubicInduction.mul_eq_mul_localZeta30_localZetaDual31_polynomial_of_isCubicInductionDataOn_of_forall_mem_bad512 below · depth 21 - Integrability of the dual S-part zeta integrand on GL₃
LanglandsTunnell.CubicInduction.sPartDual_integrable_of_isCubicInductionDataOn_of_isGaugeMajorised329 below · depth 21 - Convergence of the S-part zeta integral for cubic induction data
LanglandsTunnell.CubicInduction.sPart_integrable_of_isCubicInductionDataOn_of_isGaugeMajorised325 below · depth 21 - Convergence of finite-adelic big-cell Rankin–Selberg integrals under a gauge bound
LanglandsTunnell.RankinSelberg.exists_forall_integrable_bigCell_indicator_mul_finprod_iotaGL_of_gauge18 below · depth 21 - Convergence of the dual local GL₃timesGL₂ Rankin–Selberg integrand
LanglandsTunnell.RankinSelberg.exists_forall_integrable_dual_rsLocalIntegrand_of_gauge9 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 - 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 - 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-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 - 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 - 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 - 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 - Iwasawa bound for W_D(diag(at,1)e⁻¹)
LanglandsTunnell.Converse.ArchDatumR.norm_W_diagOne_mul_inv_le_of_iwasawa0 below · depth 22 - Measurability of the dual S-part zeta integrands
LanglandsTunnell.CubicInduction.aestronglyMeasurable_sPartDual_integrand_of_isCubicInductionDataOn2 below · depth 22 - Entire norm-≥ 1 part of a GL₃× GL₁ zeta integral
LanglandsTunnell.CubicInduction.exists_differentiable_boundedOnStrips_globalZeta30_eq_add_of_integrable26 below · depth 22 - Entire norm-≥ 1 part of the GL(3)× GL(1) zeta integral
LanglandsTunnell.CubicInduction.exists_differentiable_boundedOnStrips_globalZeta31_eq_add_of_integrable26 below · depth 22 - Local functional equation at v matches induced Euler polynomials
LanglandsTunnell.CubicInduction.exists_eval_mul_eq_mul_eval_of_forall_localZeta31_fe_one_of_isCubicInductionDataOn_of_addCharLevel493 below · depth 22 - Ramified place: local functional-equation datum matches induced Euler polynomials
LanglandsTunnell.CubicInduction.exists_eval_mul_eq_mul_eval_of_forall_localZeta31_fe_one_of_isCubicInductionDataOn_of_isRamifiedIn493 below · depth 22 - Deep-torus vanishing of unipotent coboundaries of Whittaker functions
LanglandsTunnell.CubicInduction.exists_forall_apply_iotaGL_torus_eq_zero_of_mem_span_radical_of_isGL3PsiWhittakerFn0 below · depth 22 - Gauge majorant for cyclic translates of principal-series Whittaker coefficients
LanglandsTunnell.CubicInduction.exists_gauge_of_mem_gl3CyclicSubspace_coefficientFn_principalSeries323 below · depth 22 - Two-point global-to-local zeta factorisation at a bad place
LanglandsTunnell.CubicInduction.exists_globalZeta30_eq_mul_localZeta30_and_globalZetaDual31_eq_mul_of_isCubicInductionDataOn508 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 - Admissible idele class character of ℚ with prescribed component at v and parity
LanglandsTunnell.CubicInduction.exists_isAdmissibleTwist_isUnramifiedCharAt_localChar_eq_isArchCompAt_of_hasConductorExponentAt8 below · depth 22 - Convergence of the dual archimedean GL₃ zeta integral at the trivial twist
LanglandsTunnell.CubicInduction.exists_isArchZeta31ConvergentAbove_dualWhittakerFn3_whittakerArch_of_isCubicInductionDataOn0 below · depth 22 - 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 - Jacquet's lemma in polynomial recurrence form for GL₃
LanglandsTunnell.CubicInduction.exists_polynomial_sum_coeff_smul_rightTranslate_pow_mem_span_radical_of_admissible1 below · depth 22 - Common middle of the local GL₃timesGL₂ functional equation
LanglandsTunnell.CubicInduction.exists_rsLocalIntegral_mul_eq_and_dual_mul_eq_middle_of_dominant_of_forall_localZeta31_fe_of_gauge76 below · depth 22 - Unramified twist shifts the local (3,1) functional equation
LanglandsTunnell.CubicInduction.forall_localZeta31_fe_of_twist_modulus_cpow0 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 - Haar scaling on the unipotent subgroup: dilating the integral ball
LanglandsTunnell.CubicInduction.measure_unipotentEntry_preimage_mul_eq0 below · depth 22 - Unipotent invariance of the dual Rankin–Selberg integrand
LanglandsTunnell.CubicInduction.mul_dual_eq_of_isGL3PsiWhittakerFn_inv_of_unipotent0 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 - Convergence of two intermediate GL₃timesGL₂ local integrals
LanglandsTunnell.RankinSelberg.exists_forall_integrable_flatSection_mul_whittaker_iotaGL_diagUnits2_longWeyl3_of_gauge1 below · depth 22
… and 211 more statements (search for the module name to find them).