roseking's picture
Add lean source and binary files (part 9)
7f5fab8 verified
Raw History Blame Contribute Delete
12.3 kB
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