import Mathlib import OAI.Analysis.Conductivity.Fourier.AngularPeriodization import OAI.Analysis.Conductivity.Fourier.SmoothAngularCutoff namespace OAI section noncomputable section namespace ScalarConductivity open Set Filter Topology Real MeasureTheory def angularCutoff (T : ℝ) (x : Coord3) : ℝ := periodCutoff T (x 1)*periodCutoff T (x 2) lemma angularCutoff_smooth (T : ℝ) : ContDiff ℝ (↑(⊤:ℕ∞)) (angularCutoff T) := ((periodCutoff_smooth T).comp (by fun_prop)).mul ((periodCutoff_smooth T).comp (by fun_prop)) lemma angularCutoff_support {T : ℝ} (hT : 0 hx (by simp [angularCutoff,h]) have hb : periodCutoff T (x 2)≠0 := fun h => hx (by simp [angularCutoff,h]) exact ⟨periodCutoff_support hT (subset_tsupport _ ha),periodCutoff_support hT (subset_tsupport _ hb)⟩ lemma angularCutoff_finsum {T : ℝ} (hT : 0 periodCutoff T (x 1+T*n) let b : ℤ → ℝ := fun n => periodCutoff T (x 2+T*n) have ha : (∑ᶠ n,a n)=1 := periodCutoff_finsum hT _ have hb : (∑ᶠ n,b n)=1 := periodCutoff_finsum hT _ have hf : Function.HasFiniteSupport (fun z : ℤ×ℤ => a z.1*b z.2) := by apply ((hasFiniteSupport_of_finsum_eq_one ha).prod (hasFiniteSupport_of_finsum_eq_one hb)).subset intro z hz exact ⟨fun h => hz (by simp [h]),fun h => hz (by simp [h])⟩ change (∑ᶠ n : Fin 2 → ℤ,a (n 0)*b (n 1))=1 have he := finsum_comp_equiv (MeasurableEquiv.finTwoArrow (α:=ℤ)).symm.toEquiv (f:=fun n : Fin 2 → ℤ => a (n 0)*b (n 1)) change (∑ᶠ z : ℤ×ℤ,a z.1*b z.2)=(∑ᶠ n : Fin 2 → ℤ,a (n 0)*b (n 1)) at he rw [←he,finsum_curry _ hf] simp_rw [←mul_finsum,hb,mul_one] exact ha lemma angularCutoff_periodize {T : ℝ} (hT : 0 angularCutoff T x*f x)=f := by funext x unfold angularPeriodize have he : (fun n : Fin 2 → ℤ => angularCutoff T (x+angularShift T n)*f (x+angularShift T n))= (fun n => angularCutoff T (x+angularShift T n)*f x) := by funext n; rw [hp n x] rw [he] rw [←finsum_mul,angularCutoff_finsum hT,one_mul] lemma angularCutoff_compact_support {T a b : ℝ} (hT : 0 angularCutoff T x*f x)⊆Icc ![a,-T,-T] ![b,T,T] := by intro x hx have h0 := hf ((tsupport_mul_subset_right (f:=angularCutoff T) (g:=f)) hx) have hθ := angularCutoff_support hT ((tsupport_mul_subset_left (f:=angularCutoff T) (g:=f)) hx) constructor <;> intro i <;> fin_cases i · exact h0.1 · exact hθ.1.1 · exact hθ.2.1 · exact h0.2 · exact hθ.1.2 · exact hθ.2.2 lemma angularCutoff_compact {T a b : ℝ} (hT : 0 angularCutoff T x*f x) := isCompact_Icc.of_isClosed_subset (isClosed_tsupport _) (angularCutoff_compact_support hT hf) lemma AngularPeriodic.coordinate_one {T : ℝ} {f : Coord3 → ℝ} (hp : AngularPeriodic T f) (t z : ℝ) : Function.Periodic (fun y => f ![t,y,z]) T := by intro y have hh := hp ![1,0] ![t,y,z] have he : ![t,y,z]+angularShift T ![1,0]=![t,y+T,z] := by ext i; fin_cases i <;> simp [angularShift] rw [he] at hh exact hh lemma AngularPeriodic.coordinate_two {T : ℝ} {f : Coord3 → ℝ} (hp : AngularPeriodic T f) (t y : ℝ) : Function.Periodic (fun z => f ![t,y,z]) T := by intro z have hh := hp ![0,1] ![t,y,z] have he : ![t,y,z]+angularShift T ![0,1]=![t,y,z+T] := by ext i; fin_cases i <;> simp [angularShift] rw [he] at hh exact hh end ScalarConductivity end end end OAI