openAI-math-dataset / lean /OAI /Analysis /Conductivity /Geometry /LocalFamilyRegionCoordinates.lean
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Add lean source and binary files (part 15)
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import Mathlib
import OAI.Analysis.Conductivity.Geometry.ParametricCorrectionRegionPiola
namespace OAI
section
noncomputable section
namespace ScalarConductivity
open Set Filter Topology
open scoped Matrix.Norms.Elementwise
variable {P : Type} [NormedAddCommGroup P] [NormedSpace ℝ P] [FiniteDimensional ℝ P]
theorem exists_transported_vanishing_region
{u v : P×Coord3 → Fin 2 → ℝ}
(hu : ContDiff ℝ (↑(⊤:ℕ∞)) u) (hv : ContDiff ℝ (↑(⊤:ℕ∞)) v) (p : P)
(Y : OpenPartialHomeomorph (P×Coord3) (P×Coord3))
(hY : ∀ q x,(Y (q,x)).1=q)
(hsm : ContDiff ℝ (↑(⊤:ℕ∞)) Y)
(hinv : ContDiffOn ℝ (↑(⊤:ℕ∞)) Y.symm Y.target)
{U : Set Coord3} (hYU : Y.source⊆univ×ˢU)
{x : Coord3} (hx : (p,x)∈Y.source)
(hpot : ∀ z∈Y.source,v (z.1,(Y z).2)=u z)
(hlocal : ∀ A : Set Coord3,IsOpen A → (Y (p,x)).2∈A →
∃ B : VanishingCorrectionRegion v p A,(Y (p,x)).2∈B.region) :
∃ B : VanishingCorrectionRegion u p U,x∈B.region := by
let z := (Y (p,x)).2
have hpz : (p,z)∈Y.target := by
have he : (p,z)=Y (p,x) := Prod.ext (hY p x).symm rfl
rw [he]
exact Y.map_source hx
obtain ⟨V₀,A₀,hV₀,hA₀,hp₀,hz₀,hprod₀⟩ := exists_open_product_inside Y.open_target hpz
obtain ⟨δ,hδ,hδball⟩ := Metric.isOpen_iff.mp hV₀ p hp₀
obtain ⟨η,hη,hηball⟩ := Metric.isOpen_iff.mp hA₀ z hz₀
let Kp := Metric.closedBall p (δ/2)
let Ka := Metric.closedBall z (η/2)
let A := Metric.ball z (η/2)
have hpK : Kp⊆V₀ := fun q hq => hδball
(lt_of_le_of_lt hq (by linarith : δ/2<δ))
have haK : Ka⊆A₀ := fun y hy => hηball
(lt_of_le_of_lt hy (by linarith : η/2<η))
have hjoint : Kp×ˢKa⊆Y.target := fun q hq => hprod₀ ⟨hpK hq.1,haK hq.2⟩
obtain ⟨C,hC,hbound⟩ := parametric_chart_compact_bounds Y hY hsm hinv
((isCompact_closedBall _ _).prod (isCompact_closedBall _ _)) hjoint
obtain ⟨B,hzB⟩ := hlocal A Metric.isOpen_ball (Metric.mem_ball_self (by positivity))
obtain ⟨τ,hτ,hτball⟩ := Metric.isOpen_iff.mp B.region_open z hzB
let K := Metric.closedBall z (τ/2)
have hKB : K⊆B.region := fun y hy => hτball
(lt_of_le_of_lt hy (by linarith : τ/2<τ))
let O : Set (P×Coord3) := Y.source∩{q | (Y q).2∈Metric.ball z (τ/2)}
have hO : IsOpen O := Y.open_source.inter
(Metric.isOpen_ball.preimage (continuous_snd.comp hsm.continuous))
have hxO : (p,x)∈O := ⟨hx,Metric.mem_ball_self (by positivity)⟩
obtain ⟨V₁,W₁,hV₁,hW₁,hp₁,hx₁,hprod₁⟩ := exists_open_product_inside hO hxO
let V := Metric.ball p (δ/2)∩V₁
let W := W₁∩Metric.ball x 1
have hVp : p∈V := ⟨Metric.mem_ball_self (by positivity),hp₁⟩
have hWx : x∈W := ⟨hx₁,Metric.mem_ball_self zero_lt_one⟩
have hWU : W⊆U := fun y hy => (hYU (hprod₁ (show (p,y)∈V₁×ˢW₁ from ⟨hp₁,hy.1⟩)).1).2
have hVA : V×ˢA⊆Y.target := fun q hq => hjoint
⟨Metric.ball_subset_closedBall hq.1.1,Metric.ball_subset_closedBall hq.2⟩
have hW : ∀ q∈V,W⊆(fiberSlice Y hY q).symm '' K := by
intro q hq y hy
have hh := hprod₁ (show (q,y)∈V₁×ˢW₁ from ⟨hq.2,hy.1⟩)
exact ⟨(Y (q,y)).2,Metric.ball_subset_closedBall hh.2,(fiberSlice Y hY q).left_inv hh.1⟩
have himage : ∀ q∈V,(fiberSlice Y hY q).symm '' A⊆U := by
rintro q hq _ ⟨y,hy,rfl⟩
exact (hYU ((fiberSlice Y hY q).map_target (hVA ⟨hq,hy⟩))).2
have hpot' : ∀ q∈V,∀ y∈A,u (q,(fiberSlice Y hY q).symm y)=v (q,y) := by
intro q hq y hy
have hyt := hVA (show (q,y)∈V×ˢA from ⟨hq,hy⟩)
have hys := (fiberSlice Y hY q).map_target hyt
have hh := hpot (q,(fiberSlice Y hY q).symm y) hys
rw [show (Y (q,(fiberSlice Y hY q).symm y)).2=y from
(fiberSlice Y hY q).right_inv hyt] at hh
exact hh.symm
let D := VanishingCorrectionRegion.piola hu hv p Y hY hsm hinv
(Metric.isOpen_ball.inter hV₁) hVp (Metric.isBounded_ball.subset inter_subset_left)
Metric.isOpen_ball B (isCompact_closedBall _ _) hKB hVA hW
(hW₁.inter Metric.isOpen_ball) ⟨x,hWx⟩
(Metric.isBounded_ball.subset inter_subset_right) hWU himage hpot' hC
(fun q hq y hy => (hbound (q,y)
⟨Metric.ball_subset_closedBall hq.1,Metric.ball_subset_closedBall hy⟩).2.2.2)
exact ⟨D,hWx⟩
end ScalarConductivity
end
end
end OAI