import OAI.Geometry.IsometricImmersion.Metrics.LocalMetricQActive namespace OAI noncomputable section open Set Filter Function open scoped ContDiff Topology BigOperators Matrix namespace SmoothLocal.HighEquation open SmoothLocal.Geometry SmoothLocal.Weighted SmoothLocal.ODE SmoothLocal.Hyperbolic theorem qSpatialProjection_norm_le (w : DarbouxState) : ‖qSpatialProjection w‖ ≤ ‖w‖ := by apply (pi_norm_le_iff_of_nonneg (norm_nonneg w)).mpr intro i fin_cases i · exact norm_le_pi_norm w 0 · exact norm_le_pi_norm w 2 · exact norm_le_pi_norm w 3 · exact norm_le_pi_norm w 4 · exact norm_le_pi_norm w 5 theorem qSpatialCLM_projection_of_time_zero {w : DarbouxState} (hw : w 1 = 0) : qSpatialCLM (qSpatialProjection w) = w := by have he := qFixedTimeState_projection w simpa only [qFixedTimeState, hw, Pi.single_zero, add_zero] using he theorem coordPartial_qSolutionJet_xi_norm_bound {z : Coord → ℝ} {U S : Set Coord} {Z : ℝ} (hU : IsOpen U) (hz : ContDiffOn ℝ ∞ z U) (hSU : S ⊆ U) (hzB : CoordinateBound z S 3 Z) {p : Coord} (hp : p ∈ S) : ‖coordPartial 0 (qSolutionJet z) p‖ ≤ max 1 Z := by have he := coordinate_qSolutionJet_horizontal_positive hU hz (hSU hp) 1 (by norm_num) change coordPartial 0 (qSolutionJet z) p = _ at he rw [he] apply (pi_norm_le_iff_of_nonneg (zero_le_one.trans (le_max_left _ _))).mpr intro i rw [Real.norm_eq_abs] fin_cases i · simp · simp · exact (hzB [0, 0] (by norm_num) p hp).trans (le_max_right _ _) · exact (hzB [0, 1] (by norm_num) p hp).trans (le_max_right _ _) · exact (hzB [0, 0, 1] (by norm_num) p hp).trans (le_max_right _ _) · exact (hzB [0, 0, 0] (by norm_num) p hp).trans (le_max_right _ _) theorem heightQCoefficient_xi_eq_fixedTime_second {g : MetricField} {z : Coord → ℝ} {U : Set Coord} {p : Coord} (hg : SmoothPositiveOn g U) (hU : IsOpen U) (hz : ContDiffOn ℝ ∞ z U) (hp : p ∈ U) (hxx : covHessian g z p 0 0 ≠ 0) (i : Fin 6) (hi : i ≠ 1) : coordPartial 0 (heightQCoefficient g z i) p = iteratedFDeriv ℝ 2 (qFixedTimeQ g (p 1)) (qSpatialProjection (qSolutionJet z p)) ![qSpatialProjection (coordPartial 0 (qSolutionJet z) p), Pi.single (qSpatialIndex i) 1] := by have he : qFixedTimeState (p 1) (qSpatialProjection (qSolutionJet z p)) = qSolutionJet z p := qFixedTimeState_projection (qSolutionJet z p) have hv : qSpatialProjection (qSolutionJet z p) ∈ qFixedTimeDomain g U (p 1) := by change qFixedTimeState (p 1) (qSpatialProjection (qSolutionJet z p)) ∈ darbouxQStateDomain g U rw [he] exact qSolutionJet_mem_domain hp hxx have htime : coordPartial 0 (qSolutionJet z) p 1 = 0 := by have hh := congrArg (fun v : DarbouxState => v 1) (coordinate_qSolutionJet_horizontal_positive hU hz hp 1 (by norm_num)) exact hh rw [qFixedTimeQ_iteratedFDeriv hg hU hv 2, ContinuousMultilinearMap.compContinuousLinearMap_apply, he] have hvec : (fun j : Fin 2 => qSpatialCLM (![qSpatialProjection (coordPartial 0 (qSolutionJet z) p), Pi.single (qSpatialIndex i) 1] j)) = ![coordPartial 0 (qSolutionJet z) p, Pi.single i 1] := by funext j fin_cases j · exact qSpatialCLM_projection_of_time_zero htime · change qSpatialCLM (Pi.single (qSpatialIndex i) 1) = Pi.single i 1 rw [qSpatialCLM_single, qSpatialAxis_index hi] rw [hvec] exact (second_fderiv_comp_constant_direction_xi (sixVariableQ_contDiffAt_solutionJet hg hU hp hxx) (((qSolutionJet_contDiffOn hU hz).contDiffAt (hU.mem_nhds hp)).differentiableAt (by simp)) (Pi.single i 1)).symm theorem heightQCoefficient_xi_bound_of_fixedTime_second {g : MetricField} {z : Coord → ℝ} {U S : Set Coord} {Z C : ℝ} (hg : SmoothPositiveOn g U) (hU : IsOpen U) (hz : ContDiffOn ℝ ∞ z U) (hSU : S ⊆ U) (hzB : CoordinateBound z S 3 Z) (hC : 0 ≤ C) {p : Coord} (hp : p ∈ S) (hxx : covHessian g z p 0 0 ≠ 0) (hQ : ‖iteratedFDeriv ℝ 2 (qFixedTimeQ g (p 1)) (qSpatialProjection (qSolutionJet z p))‖ ≤ C) (i : Fin 6) (hi : i ≠ 1) : |coordPartial 0 (heightQCoefficient g z i) p| ≤ C * max 1 Z := by rw [heightQCoefficient_xi_eq_fixedTime_second hg hU hz (hSU hp) hxx i hi, ← Real.norm_eq_abs] have hd := (qSpatialProjection_norm_le (coordPartial 0 (qSolutionJet z) p)).trans (coordPartial_qSolutionJet_xi_norm_bound hU hz hSU hzB hp) have hb := (iteratedFDeriv ℝ 2 (qFixedTimeQ g (p 1)) (qSpatialProjection (qSolutionJet z p))).le_opNorm ![qSpatialProjection (coordPartial 0 (qSolutionJet z) p), Pi.single (qSpatialIndex i) (1 : ℝ)] simp only [Fin.prod_univ_two, Matrix.cons_val_zero, Matrix.cons_val_one, Pi.norm_single, norm_one, mul_one] at hb exact hb.trans (mul_le_mul hQ hd (norm_nonneg _) hC) theorem exists_same_region_Q_first_xi_bound (G R Z : ℝ) (hG : 0 ≤ G) (hR : 0 ≤ R) {d c : ℝ} (hd : 0 < d) (hc : 0 < c) : ∃ Cfirst : ℝ, 0 ≤ Cfirst ∧ ∀ (g : MetricField) (z : Coord → ℝ) (U S : Set Coord), SmoothPositiveOn g U → IsOpen U → ContDiffOn ℝ ∞ z U → S ⊆ U → (∀ p ∈ S, |p 0| ≤ R ∧ |p 1| ≤ R) → (∀ p ∈ S, HorizontalMetricTwoJetBound g p 2 G) → CoordinateBound z S 3 Z → (∀ p ∈ S, d ≤ |(g p).det|) → (∀ p ∈ S, c ≤ |covHessian g z p 0 0|) → ∀ i : Fin 6, i ≠ 1 → ∀ p ∈ S, |coordPartial 0 (heightQCoefficient g z i) p| ≤ Cfirst := by obtain ⟨C, hC, hQ⟩ := exists_local_fixedTime_Q_jet_bound G (max R Z) hG hd hc 2 refine ⟨C * max 1 Z, mul_nonneg hC (zero_le_one.trans (le_max_left _ _)), ?_⟩ intro g z U S hg hU hz hSU hcoords hgB hzB hdet hden i hi p hp have hxx : covHessian g z p 0 0 ≠ 0 := by intro he have hh := hden p hp rw [he, abs_zero] at hh linarith have he : qFixedTimeState (p 1) (qSpatialProjection (qSolutionJet z p)) = qSolutionJet z p := qFixedTimeState_projection (qSolutionJet z p) have hpoint : coordinatePoint (qSpatialProjection (qSolutionJet z p) 0) (p 1) = p := point_eta p have hz2 : CoordinateBound z S 2 Z := fun ds hds p hp => hzB ds (by omega) p hp have hbound := hQ g U hg hU (p 1) (qSpatialProjection (qSolutionJet z p)) (by simpa only [hpoint] using hSU hp) (by simpa only [hpoint] using hgB p hp) (by rw [he]; exact qSolutionJet_norm_bound_of_coordinateBound hR hz2 hcoords hp) (by simpa only [hpoint] using hdet p hp) (by rw [he, stateQDenominator_qSolutionJet]; exact hden p hp) 2 le_rfl exact heightQCoefficient_xi_bound_of_fixedTime_second hg hU hz hSU hzB hC hp hxx hbound i hi end SmoothLocal.HighEquation end end OAI