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| import OAI.AlgebraicGeometry.PlaneCurves.BasisNoncancellation | |
| import OAI.AlgebraicGeometry.PlaneCurves.MarkedDisplacements | |
| import OAI.AlgebraicGeometry.PlaneCurves.UniversalSections | |
| namespace OAI | |
| /-! | |
| # Collision for geometric section families and necessary sections | |
| -/ | |
| section | |
| /-! | |
| ## Source collision on the actual Wτ | |
| -/ | |
| noncomputable section | |
| namespace Nagata.W20 | |
| open scoped BigOperators Topology | |
| open Nagata.Workers.W12 Nagata.Workers.W10 Nagata.FiniteExponents | |
| open Nagata.CoefficientSpaces Nagata.W22 | |
| /-- The manuscript collision conclusion for the literal source section space | |
| and actual jet map. Finite basis and all analytic coefficient premises have been | |
| discharged. Only the universal necessary-W geometric input remains. -/ | |
| theorem source_collision_of_every_configuration | |
| {τ : ℝ} (hτ : 0 < τ) (hτone : τ < 1) | |
| (marks : Fin 9 → ℝ) (a delta x0 : ℝ) (d : ℤ) (m q : ℕ) | |
| (hs : (∑ i, marks i) = 9 * x0 - delta) | |
| (hd : 3 * (m : ℤ) < d) | |
| (hfirst : ∀ j : ℤ, 0 ≤ j → j ≤ (m : ℤ) → | |
| firstLower d (m : ℤ) j a delta ∉ Set.range (Int.cast : ℤ → ℝ)) | |
| (hsecond : ∀ j : ℤ, (m : ℤ) < j → j ≤ d / 3 → 0 < d - 3 * j → | |
| secondLower d j a delta ∉ Set.range (Int.cast : ℤ → ℝ)) | |
| {U : Set ℂ} (hU : IsOpen U) (h0 : (0 : ℂ) ∈ U) | |
| (hEvery : ∀ p : Fin q → ℂ, Function.Injective p → (∀ i, p i ∈ U) → | |
| ∃ F : genuineSourceSections hτ hτone marks a d m, F ≠ 0 ∧ | |
| ∀ i, Nagata.Workers.W28.HasAnalyticOrderAtLeast (𝕜 := ℂ) | |
| (fun x : ℂ × ℂ => localScalar F (tauPower τ x0) x.1 x.2) (p i, 0) m) : | |
| ∃ F₀ : genuineSourceSections hτ hτone marks a d m, | |
| F₀ ≠ 0 ∧ genuineSourceJetMap hτ hτone marks a x0 d m q F₀ = 0 := by | |
| exact actual_kernel_of_every_configuration | |
| (fun z hz => (rayMarkedSection_analyticOnNhd hτ hτone marks z hz).differentiableAt) | |
| (tauPower_ne_zero hτ x0) | |
| (genuineSourceBasis hτ hτone marks a delta x0 d m hs hd hfirst hsecond) | |
| hU h0 hEvery | |
| /-- The actual source jet rows are the manuscript's mixed derivatives in one | |
| fixed covering frame. Row first coordinate is b, second is ell. -/ | |
| theorem genuineSourceJetMap_eq_mixed_derivative | |
| {τ : ℝ} (hτ : 0 < τ) (hτone : τ < 1) | |
| (marks : Fin 9 → ℝ) (a x0 : ℝ) (d : ℤ) (m q : ℕ) | |
| (F : genuineSourceSections hτ hτone marks a d m) | |
| (row : Nagata.Workers.W30.JetIndex q m) : | |
| genuineSourceJetMap hτ hτone marks a x0 d m q F row = | |
| iteratedDeriv row.2.val | |
| (fun x => iteratedDeriv row.1.val | |
| (fun y => localScalar F (tauPower τ x0) x y) 0) 0 := by | |
| exact actualJetMap_apply_eq_mixed_derivative _ _ F row | |
| end Nagata.W20 | |
| end | |
| end | |
| section | |
| noncomputable section | |
| namespace Nagata.W20 | |
| open scoped BigOperators Topology | |
| open Nagata.Workers.W12 Nagata.Workers.W10 Nagata.CoefficientSpaces | |
| open Nagata.Workers.W17 Nagata.Workers.W28 Nagata.ProjectiveGeometry | |
| /-- Genuine universal-support specialization, transported to the exact Wτ used | |
| by the source basis and collision map, with all scalar identifications discharged. -/ | |
| theorem source_necessary_W_of_cubic_geometry {q d m : ℕ} {τ : ℝ} | |
| (hτ : 0 < τ) (hτone : τ < 1) | |
| (hUniversal : Nagata.W13.UniversalSupport (9 + q) d (fun _ => m)) | |
| (marks : Fin 9 → ℝ) (a x0 : ℝ) | |
| (hdisjoint : Pairwise (fun i j => ∀ k : ℤ, | |
| ((τ ^ marks i : ℝ) : ℂ) ≠ ((τ ^ marks j : ℝ) : ℂ) * (τ : ℂ) ^ k)) | |
| (ξ : Fin q → ℂ) | |
| (hpP : ∀ i, (Nagata.W22.rayMarkedSection hτ hτone marks).val | |
| (tauPower τ x0 * Complex.exp (ξ i)) ≠ 0) | |
| (C : MvPolynomial (Fin 3) ℂ) (hC : C.IsHomogeneous 3) | |
| (X : Fin 3 → Nagata.W08.automorphicSections (τ : ℂ) 3 | |
| (tauPower τ (((∑ i, marks i) + a) / 3))) | |
| (hrelations : Nagata.Workers.W25.polynomialRelationIdeal (fun i => (X i).val) = | |
| Ideal.span ({C} : Set _)) | |
| (chart : Fin (9 + q) → Fin 3) | |
| (hc : ∀ b, (X (chart b)).val | |
| (markedNormalBase (fun i => ((τ ^ marks i : ℝ) : ℂ)) | |
| (logarithmicPoints (tauPower τ x0) ξ) b) ≠ 0) | |
| (hbase : Function.Injective (fun b => chartPoint₂ (chart b) | |
| (planeCoordinate (normalizedCurvePoint (fun i => (X i).val) (chart b) | |
| (markedNormalBase (fun i => ((τ ^ marks i : ℝ) : ℂ)) | |
| (logarithmicPoints (tauPower τ x0) ξ) b))))) | |
| (hpartial : ∀ b, planePolynomialEval | |
| (MvPolynomial.pderiv 1 (Nagata.W27.directChartHom (chart b) C)) | |
| (normalizedCurvePoint (fun i => (X i).val) (chart b) | |
| (markedNormalBase (fun i => ((τ ^ marks i : ℝ) : ℂ)) | |
| (logarithmicPoints (tauPower τ x0) ξ) b)) ≠ 0) : | |
| ∃ F : genuineSourceSections hτ hτone marks a (d : ℤ) m, F ≠ 0 ∧ | |
| ∀ i, HasAnalyticOrderAtLeast (𝕜 := ℂ) | |
| (fun x : ℂ × ℂ => localScalar F (tauPower τ x0) x.1 x.2) (ξ i, 0) m := by | |
| have ht : ‖(τ : ℂ)‖ < 1 := by | |
| simpa only [Complex.norm_real, Real.norm_eq_abs, abs_of_pos hτ] using hτone | |
| have ht0 : (τ : ℂ) ≠ 0 := Complex.ofReal_ne_zero.mpr hτ.ne' | |
| have hm : ∀ i, ((τ ^ marks i : ℝ) : ℂ) ≠ 0 := | |
| fun i => Complex.ofReal_ne_zero.mpr (Real.rpow_pos_of_pos hτ (marks i)).ne' | |
| have heq := nineThetaSection_ray_eq hτ hτone ht ht0 marks hm | |
| have hp : ∀ i, (nineThetaSection ht ht0 (fun i => ((τ ^ marks i : ℝ) : ℂ)) hm).val | |
| ((logarithmicPoints (tauPower τ x0) ξ) i).1 ≠ 0 := by | |
| simpa only [heq, logarithmicPoints] using hpP | |
| have hW := universalSupport_necessary_W_local hUniversal ht ht0 | |
| (tauPower_ne_zero hτ (((∑ i, marks i) + a) / 3)) | |
| (fun i => ((τ ^ marks i : ℝ) : ℂ)) hm hdisjoint | |
| (tauPower τ x0) (tauPower_ne_zero hτ x0) ξ hp C hC X hrelations chart hc hbase hpartial | |
| change ∃ F : ActualSection (τ : ℂ) | |
| (tauPower τ (((∑ i, marks i) + a) / 3)) (∏ i, -((τ ^ marks i : ℝ) : ℂ)) | |
| (d : ℤ) m (Nagata.W22.rayMarkedSection hτ hτone marks).val, F ≠ 0 ∧ | |
| ∀ i, HasAnalyticOrderAtLeast (𝕜 := ℂ) | |
| (fun x : ℂ × ℂ => localScalar F (tauPower τ x0) x.1 x.2) (ξ i, 0) m at hW | |
| exact Eq.mp (congrArg (fun γ : ℂ => | |
| ∃ F : ActualSection (τ : ℂ) (tauPower τ (((∑ i, marks i) + a) / 3)) γ | |
| (d : ℤ) m (Nagata.W22.rayMarkedSection hτ hτone marks).val, F ≠ 0 ∧ | |
| ∀ i, HasAnalyticOrderAtLeast (𝕜 := ℂ) | |
| (fun x : ℂ × ℂ => localScalar F (tauPower τ x0) x.1 x.2) (ξ i, 0) m) | |
| (rayMarkedMultiplier hτ marks)) hW | |
| end Nagata.W20 | |
| end | |
| end | |
| section | |
| /-! Exact fixed-τ source collision from universal support and concrete cubic | |
| chart geometry. The common marked-point disk and Pi nonvanishing are supplied | |
| by the proved fixed-period configuration construction, not by caller assumptions. -/ | |
| noncomputable section | |
| namespace Nagata.W20 | |
| open scoped BigOperators Topology | |
| open Nagata.Workers.W12 Nagata.Workers.W10 Nagata.CoefficientSpaces | |
| open Nagata.Workers.W17 Nagata.Workers.W28 Nagata.ProjectiveGeometry | |
| open Nagata.FiniteExponents | |
| /-- Equality of the actual source marked section with the actual marked product | |
| on the common exponential chart. -/ | |
| theorem source_markedPi_cover_eq {τ : ℝ} (hτ : 0 < τ) (hτone : τ < 1) | |
| (marks : Fin 9 → ℝ) (x0 : ℝ) (x : ℂ) : | |
| (Nagata.W22.rayMarkedSection hτ hτone marks).val | |
| (tauPower τ x0 * Complex.exp x) = | |
| Nagata.W06.TorusConfiguration.markedPi τ marks | |
| (Nagata.Workers.W05.chartPoint τ x0 x : ℂ) := by | |
| have hz : tauPower τ x0 * Complex.exp x ≠ 0 := | |
| mul_ne_zero (tauPower_ne_zero hτ x0) (Complex.exp_ne_zero x) | |
| unfold Nagata.W22.rayMarkedSection | |
| rw [Nagata.W08.markedThetaSection_apply _ _ _ _ hz] | |
| unfold Nagata.W06.TorusConfiguration.markedPi | |
| simp only [Nagata.Workers.W05.chartPoint_eq_real_rpow hτ, | |
| Nagata.Workers.W05.rayPoint_eq_real_rpow hτ, tauPower] | |
| /-- The actual marked ray lifts occupy pairwise disjoint period orbits. -/ | |
| theorem source_marked_orbits_disjoint {τ : ℝ} (hτ : 0 < τ) (hτone : τ < 1) | |
| (marks : Fin 9 → ℝ) (hinj : Function.Injective marks) | |
| (hb : ∀ i, 0 < marks i ∧ marks i < 1 / 2) : | |
| Pairwise (fun i j => ∀ k : ℤ, | |
| ((τ ^ marks i : ℝ) : ℂ) ≠ ((τ ^ marks j : ℝ) : ℂ) * (τ : ℂ) ^ k) := by | |
| intro i j hij k he | |
| apply hij | |
| apply hinj | |
| have heq : Nagata.W21.torusPointMk (Nagata.Workers.W05.positivePeriod τ hτ) | |
| (Nagata.Workers.W05.rayPoint τ (marks j)) = | |
| Nagata.W21.torusPointMk (Nagata.Workers.W05.positivePeriod τ hτ) | |
| (Nagata.Workers.W05.rayPoint τ (marks i)) := by | |
| apply Quotient.sound | |
| apply (Nagata.W21.torusOrbitSetoid_iff_coe _ _ _).mpr | |
| refine ⟨k, ?_⟩ | |
| simpa only [Nagata.Workers.W05.rayPoint_eq_real_rpow hτ, | |
| Nagata.Workers.W05.positivePeriod, Units.val_mk0, mul_comm] using he | |
| have hj : marks j ∈ Set.Ioo (0 : ℝ) 1 := ⟨(hb j).1, by linarith [(hb j).2]⟩ | |
| have hi : marks i ∈ Set.Ioo (0 : ℝ) 1 := ⟨(hb i).1, by linarith [(hb i).2]⟩ | |
| exact (Nagata.W06.TorusConfiguration.rayTorusPoint_injective_on_unit_interval | |
| hτ hτone hj hi heq).symm | |
| /-- Fixed-period source collision from genuine universal support and concrete | |
| cubic chart geometry. No finite basis, analytic section, Pi-nonvanishing, local | |
| multiplicity, or moving-sequence hypothesis remains. -/ | |
| theorem source_collision_of_universalSupport_and_cubic_geometry | |
| {τ : ℝ} (hτ : 0 < τ) (hτone : τ < 1) | |
| (marks : Fin 9 → ℝ) (hmarks : Function.Injective marks) | |
| (hmbounds : ∀ i, 0 < marks i ∧ marks i < 1 / 2) | |
| (a delta : ℝ) (d m q : ℕ) | |
| (hs : (∑ i, marks i) = 9 * (1 / 2 : ℝ) - delta) | |
| (hd : 3 * (m : ℤ) < (d : ℤ)) | |
| (hfirst : ∀ j : ℤ, 0 ≤ j → j ≤ (m : ℤ) → | |
| firstLower (d : ℤ) (m : ℤ) j a delta ∉ Set.range (Int.cast : ℤ → ℝ)) | |
| (hsecond : ∀ j : ℤ, (m : ℤ) < j → j ≤ (d : ℤ) / 3 → 0 < (d : ℤ) - 3 * j → | |
| secondLower (d : ℤ) j a delta ∉ Set.range (Int.cast : ℤ → ℝ)) | |
| (hUniversal : Nagata.W13.UniversalSupport (9 + q) d (fun _ => m)) | |
| (C : MvPolynomial (Fin 3) ℂ) (hC : C.IsHomogeneous 3) | |
| (X : Fin 3 → Nagata.W08.automorphicSections (τ : ℂ) 3 | |
| (tauPower τ (((∑ i, marks i) + a) / 3))) | |
| (hrelations : Nagata.Workers.W25.polynomialRelationIdeal (fun i => (X i).val) = | |
| Ideal.span ({C} : Set _)) | |
| (hcharts : ∀ ξ : Fin q → ℂ, | |
| Function.Injective (Nagata.W06.TorusConfiguration.torusTuple τ hτ (1 / 2) marks ξ) → | |
| ∃ chart : Fin (9 + q) → Fin 3, | |
| (∀ b, (X (chart b)).val | |
| (markedNormalBase (fun i => ((τ ^ marks i : ℝ) : ℂ)) | |
| (logarithmicPoints (tauPower τ (1 / 2)) ξ) b) ≠ 0) ∧ | |
| Function.Injective (fun b => chartPoint₂ (chart b) | |
| (planeCoordinate (normalizedCurvePoint (fun i => (X i).val) (chart b) | |
| (markedNormalBase (fun i => ((τ ^ marks i : ℝ) : ℂ)) | |
| (logarithmicPoints (tauPower τ (1 / 2)) ξ) b)))) ∧ | |
| (∀ b, planePolynomialEval | |
| (MvPolynomial.pderiv 1 (Nagata.W27.directChartHom (chart b) C)) | |
| (normalizedCurvePoint (fun i => (X i).val) (chart b) | |
| (markedNormalBase (fun i => ((τ ^ marks i : ℝ) : ℂ)) | |
| (logarithmicPoints (tauPower τ (1 / 2)) ξ) b)) ≠ 0)) : | |
| ∃ F₀ : genuineSourceSections hτ hτone marks a (d : ℤ) m, | |
| F₀ ≠ 0 ∧ genuineSourceJetMap hτ hτone marks a (1 / 2) (d : ℤ) m q F₀ = 0 := by | |
| obtain ⟨R, hR, hcfg⟩ := Nagata.W06.TorusConfiguration.exists_disk_for_fixed_period | |
| hτ hτone marks hmarks hmbounds | |
| apply source_collision_of_every_configuration hτ hτone marks a delta (1 / 2) | |
| (d : ℤ) m q hs hd hfirst hsecond Metric.isOpen_ball (Metric.mem_ball_self hR) | |
| intro ξ hξ hξU | |
| have hnorm : ∀ i, ‖ξ i‖ < R := by | |
| intro i | |
| simpa only [Metric.mem_ball, dist_zero_right] using hξU i | |
| obtain ⟨hinj, hPi⟩ := hcfg q ξ hξ hnorm | |
| obtain ⟨chart, hc, hbase, hpartial⟩ := hcharts ξ hinj | |
| apply source_necessary_W_of_cubic_geometry hτ hτone hUniversal marks a (1 / 2) | |
| (source_marked_orbits_disjoint hτ hτone marks hmarks hmbounds) ξ ?_ | |
| C hC X hrelations chart hc hbase hpartial | |
| intro i | |
| rw [source_markedPi_cover_eq] | |
| exact hPi i | |
| end Nagata.W20 | |
| end | |
| end | |
| end OAI | |