import Mathlib import OAI.Analysis.Conductivity.Geometry.PhysicalBoxCorrection import OAI.Analysis.Conductivity.Variational.PhysicalOverlapMoments namespace OAI noncomputable section namespace ScalarConductivity open Set MeasureTheory Filter Topology Matrix open scoped Matrix.Norms.Elementwise lemma localPiolaSource_tsupport_image (X : OpenPartialHomeomorph Coord3 Coord3) (r : Coord3 → ℝ) (hc : HasCompactSupport r) (hs : tsupport r⊆X.source) : tsupport (localPiolaSource X r)⊆X '' tsupport r := by exact closure_minimal ((localPiolaSource_support X r).trans (image_mono (fun _ hx => subset_closure hx.1))) (hc.image_of_continuousOn (X.continuousOn.mono hs)).isClosed lemma localPiolaSource_inverse (X : OpenPartialHomeomorph Coord3 Coord3) (hX : DifferentiableOn ℝ X X.source) (hXi : DifferentiableOn ℝ X.symm X.target) (r : Coord3 → ℝ) (hs : Function.support r⊆X.target) : localPiolaSource X (localPiolaSource X.symm r)=r := by funext y by_cases hy : y∈X.target · have he := congrArg (fun D : Coord3 →L[ℝ] Coord3 => D.det) (local_fderiv_symm_comp X.symm hXi hX hy) simp only [OpenPartialHomeomorph.symm_symm,ContinuousLinearMap.det, ContinuousLinearMap.toLinearMap_comp,ContinuousLinearMap.coe_id, LinearMap.det_comp,LinearMap.det_id] at he have habs : |(fderiv ℝ X (X.symm y)).det| * |(fderiv ℝ X.symm y).det|=1 := by rw [←abs_mul] exact congrArg abs he |>.trans abs_one classical change (if y∈X.target then |(fderiv ℝ X (X.symm y)).det|⁻¹ * (if X.symm y∈X.source then |(fderiv ℝ X.symm (X (X.symm y))).det|⁻¹ * r (X (X.symm y)) else 0) else 0) = r y rw [ite_eq_left hy,ite_eq_left (X.map_target hy),X.right_inv hy] rw [←mul_assoc,←mul_inv,habs,inv_one,one_mul] · rw [localPiolaSource,ite_eq_right hy,Function.notMem_support.mp (fun h => hy (hs h))] def correctionBox (a b : Fin 3 → ℝ) : Set Coord3 := boxCoordinates ⁻¹' ((Ioo (a 0) (b 0) ×ˢ Ioo (a 1) (b 1)) ×ˢ Ioo (a 2) (b 2)) lemma localPiolaSource_inverse_support (X : OpenPartialHomeomorph Coord3 Coord3) (r : Coord3 → ℝ) (hc : HasCompactSupport r) {V : Set Coord3} (hV : V⊆X.source) (hs : tsupport r⊆X '' V) : tsupport (localPiolaSource X.symm r)⊆V := by have ht : tsupport r⊆X.target := hs.trans (by rintro y ⟨x,hx,rfl⟩; exact X.map_source (hV hx)) intro x hx obtain ⟨y,hy,rfl⟩ := localPiolaSource_tsupport_image X.symm r hc ht hx obtain ⟨z,hz,rfl⟩ := hs hy simpa only [X.left_inv (hV hz)] using hz theorem local_physical_symmetric_correction (X : OpenPartialHomeomorph Coord3 Coord3) (hX : ContDiffOn ℝ (↑(⊤:ℕ∞)) X X.source) (hXi : ContDiffOn ℝ (↑(⊤:ℕ∞)) X.symm X.target) {a b : Fin 3 → ℝ} (hab : ∀ i,a i localPiolaSource X.symm (r j) have hst (j) : tsupport (r j)⊆X.target := (hs j).trans (by rintro y ⟨x,hx,rfl⟩; exact X.map_source (hbox hx)) have hp (j) : ContDiff ℝ (↑(⊤:ℕ∞)) (p j) := localPiolaSource_smooth X.symm hXi hX (r j) (hr j) (hc j) (hst j) have hpc (j) : HasCompactSupport (p j) := (localPiolaSource_compact X.symm (r j) (hc j) (hst j)).1 have hps (j) : tsupport (p j)⊆correctionBox a b := localPiolaSource_inverse_support X (r j) (hc j) hbox (hs j) let q : Fin 2 → Box3 → ℝ := fun j => p j∘boxCoordinates.symm have hq (j) : ContDiff ℝ (↑(⊤:ℕ∞)) (q j) := (hp j).comp boxCoordinates.symm.contDiff have hqc (j) : HasCompactSupport (q j) := (hpc j).comp_homeomorph boxCoordinates.symm.toHomeomorph have hqs (j) : tsupport (q j)⊆ (Ioo (a 0) (b 0) ×ˢ Ioo (a 1) (b 1)) ×ˢ Ioo (a 2) (b 2) := by intro z hz have h := hps j ((tsupport_comp_subset_preimage (p j) boxCoordinates.symm.continuous) hz) simpa only [correctionBox,mem_preimage,boxCoordinates.apply_symm_apply] using h have hd := hX.differentiableOn (by simp) have hdi := hXi.differentiableOn (by simp) have hback (j) : localPiolaSource X (p j)=r j := localPiolaSource_inverse X hd hdi (r j) ((subset_tsupport _).trans (hst j)) have hqz (j) : (∫ z,q j z)=0 := by rw [←boxCoordinates_integral (q j)] simp only [q,Function.comp_apply,boxCoordinates.symm_apply_apply] have he := localPiolaSource_pairing volume X.symm hdi (fun _ hy => local_fderiv_det_ne_zero X.symm hdi hd hy) (r j) ((subset_tsupport _).trans (hst j)) (fun _ => 1) simpa only [one_mul] using he.trans (by simpa only [one_mul] using hz j) have hqt : (∫ z : Box3,z.1.2*q 0 z-z.1.1*q 1 z)=0 := by rw [←boxCoordinates_integral (fun z : Box3 => z.1.2*q 0 z-z.1.1*q 1 z)] have he := localPiolaSource_torque X hd hdi (p 0) (p 1) ((subset_tsupport _).trans ((hps 0).trans hbox)) ((subset_tsupport _).trans ((hps 1).trans hbox)) rw [hback 0,hback 1] at he simp only [q,Function.comp_apply,boxCoordinates.symm_apply_apply] change (∫ x,x 1*p 0 x-x 0*p 1 x)=0 rw [←he] refine (integral_congr_ae ?_).trans ht filter_upwards [] with y by_cases hy : y∈X.target · rw [hu hy]; rfl · rw [image_eq_zero_of_notMem_tsupport (fun h => hy (hst 0 h)), image_eq_zero_of_notMem_tsupport (fun h => hy (hst 1 h)),mul_zero,mul_zero,mul_zero,mul_zero] obtain ⟨H,hH,hHc,hHs,hsy,hweak⟩ := physical_box_symmetric_correction X hX hXi hab hbox (hq 0) (hq 1) (hqc 0) (hqc 1) (hqs 0) (hqs 1) (hqz 0) (hqz 1) hqt refine ⟨H,hH,hHc,hHs,hsy,?_⟩ intro j ψ hψ have he := hweak j ψ hψ have hpsource : (fun x => ![q 0 (boxCoordinates x),q 1 (boxCoordinates x)] j)=p j := by funext x fin_cases j <;> simp [q] rw [hpsource,hback j] at he refine (integral_congr_ae ?_).trans he filter_upwards [] with y by_cases hy : y∈X.target · have hf : u =ᶠ[𝓝 y] coordinatePair∘X.symm := Filter.eventuallyEq_of_mem (X.open_target.mem_nhds hy) (fun z hz => hu hz) rw [hf.fderiv_eq] · rw [image_eq_zero_of_notMem_tsupport (fun h => hy (hHs h)),Matrix.zero_mul,Matrix.zero_mul] end ScalarConductivity end end OAI