import OAI.Analysis.AncientFlat.Kernel.ClassicalBase namespace OAI noncomputable section open Set Filter MeasureTheory open scoped SchwartzMap Topology ZeroAtInfty BoundedContinuousFunction Laplacian ContDiff namespace FrozenParametrix open BiharmonicKernel variable {V : Type} [NormedAddCommGroup V] [InnerProductSpace ℝ V] [FiniteDimensional ℝ V] [MeasurableSpace V] [BorelSpace V] variable {α β : ℝ} lemma c0Time_eq_sourceValue (hα : 0 < α) (a : V →ᵇ Icc α β) (q : ℝ) (hq : 0 < q) (f : C₀(V,ℂ)) (x : V) : c0Time hα a q f x = SourceFrozenRows.value (heatKernel 1 zero_lt_one) (fun y => (a y).val) (q^(1/4 : ℝ)) f.toBCF x := by rw [c0Time_apply hα a q hq f, timeValue_eq_scaled hα a.toContinuousMap q hq f] unfold SourceFrozenRows.value have he : sourceScale a.toContinuousMap q = fun y => q^(1/4 : ℝ)*(a y).val^(1/4 : ℝ) := by funext y unfold sourceScale rw [Real.sqrt_eq_rpow,Real.sqrt_eq_rpow] change ((q*(a y).val)^(1/2 : ℝ))^(1/2 : ℝ) = _ rw [← Real.rpow_mul (mul_nonneg hq.le (hα.trans_le (a y).property.1).le)] norm_num exact Real.mul_rpow hq.le (hα.trans_le (a y).property.1).le rw [he] rfl end FrozenParametrix namespace ParametrixVolterra section ExtendedA open FrozenParametrix StrongWeightedVolterra BiharmonicKernel variable {V : Type} [NormedAddCommGroup V] variable {T α β : ℝ} variable (A : C(Slab T,V →ᵇ Icc α β)) (hT : 0 ≤ T) def extendedA (s : ℝ) (x : V) : ℝ := (A (projIcc 0 T hT s) x).val lemma continuous_extendedA : Continuous (Function.uncurry (extendedA A hT)) := by change Continuous (fun p : ℝ × V => (A (projIcc 0 T hT p.1) p.2).val) have h : Continuous (fun p : ℝ × V => A (projIcc 0 T hT p.1) p.2) := by fun_prop exact continuous_subtype_val.comp h lemma extendedA_range (s : ℝ) (x : V) : extendedA A hT s x ∈ Icc α β := (A (projIcc 0 T hT s) x).property lemma extendedA_lipschitz (L : ℝ) (hLip : ∀ s r : Slab T, ∀ x z : V, |(A s x).val-(A r z).val| ≤ L*(‖x-z‖+|s.val-r.val|)) : ∀ s x y, ‖extendedA A hT s x-extendedA A hT s y‖ ≤ L*‖x-y‖ := by intro s x y simpa only [extendedA,Real.norm_eq_abs,sub_self,abs_zero,add_zero] using hLip (projIcc 0 T hT s) (projIcc 0 T hT s) x y variable [InnerProductSpace ℝ V] [FiniteDimensional ℝ V] [MeasurableSpace V] [BorelSpace V] variable (hα : 0 < α) lemma duhamel_eq_sourceDuhamel (j : Time T →ᵇ C₀(V,ℂ)) (t : Time T) (x : V) : duhamel hα A j t.val x = SourceFrozenRows.duhamel (heatKernel 1 zero_lt_one) (extendedA A hT) (fun s => (unweighted j s).toBCF) t.val x := by unfold duhamel SourceFrozenRows.duhamel rw [HolderIntegral.intervalIntegral_apply _ (intervalIntegrable_sourceFrozen hα A j t.val t.val ⟨t.property.1.le,t.property.2⟩) x, intervalIntegral.integral_of_le t.property.1.le,integral_Ioc_eq_integral_Ioo] apply setIntegral_congr_fun measurableSet_Ioo intro s hs have hsT : s ∈ Ioc (0:ℝ) T := ⟨hs.1,hs.2.le.trans t.property.2⟩ dsimp only rw [VolterraIntegral.sourceExtend_apply _ _ _ hsT] dsimp [sourceFrozen] rw [c0Time_eq_sourceValue hα _ _ (sub_pos.mpr hs.2)] have he : projIcc 0 T hT s = now (⟨s,hsT⟩ : Time T) := projIcc_of_mem hT ⟨hs.1.le,hsT.2⟩ have heA : extendedA A hT s = fun y => (A (now (⟨s,hsT⟩ : Time T)) y).val := by funext y unfold extendedA rw [he] rw [heA] include hT in lemma contDiff_duhamel_of_holder (L : ℝ) (hL : 0 ≤ L) (hLip : ∀ s r : Slab T, ∀ x z : V, |(A s x).val-(A r z).val| ≤ L*(‖x-z‖+|s.val-r.val|)) (j : Time T →ᵇ C₀(V,ℂ)) (H : ℝ) (hH : 0 ≤ H) (hj : ∀ s : Time T, ∀ x y, ‖unweighted j s.val x-unweighted j s.val y‖ ≤ H*s.val^(-7/8 : ℝ)*‖x-y‖^(1/4 : ℝ)) (t : Time T) : ContDiff ℝ 4 (fun x => duhamel hα A j t.val x) := by have hf : StronglyMeasurable (fun s => (unweighted j s).toBCF) := ZeroAtInftyContinuousMap.isometry_toBCF.continuous.comp_stronglyMeasurable (stronglyMeasurable_unweighted j) have hn : ∀ s ∈ Ioo 0 t.val, ‖(unweighted j s).toBCF‖ ≤ ‖j‖*s^(-(3/4 : ℝ)) := by intro s hs rw [ZeroAtInftyContinuousMap.norm_toBCF_eq_norm] simpa only [neg_div,mul_comm] using norm_unweighted_le j s hs.1 have hh : ∀ s ∈ Ioo 0 t.val, ∀ x y : V, ‖(unweighted j s).toBCF x-(unweighted j s).toBCF y‖ ≤ (H*s^(-(7/8 : ℝ)))*‖x-y‖^(1/4 : ℝ) := by intro s hs x y change ‖unweighted j s x-unweighted j s y‖ ≤ _ simpa only [neg_div] using hj ⟨s,hs.1,hs.2.le.trans t.property.2⟩ x y have he := funext (duhamel_eq_sourceDuhamel A hT hα j t) rw [he] exact WeightedSourceFrozenRows.contDiff_duhamel (heatKernel 1 zero_lt_one) (extendedA A hT) (continuous_extendedA A hT) α β hα (extendedA_range A hT) L hL (extendedA_lipschitz A hT L hLip) (fun s => (unweighted j s).toBCF) hf (3/4) (7/8) ‖j‖ H (1/4) t.val (by norm_num) (by norm_num) (norm_nonneg j) hH t.property.1 (by norm_num) (by norm_num) hn hh end ExtendedA open FrozenParametrix StrongWeightedVolterra variable {V : Type} [NormedAddCommGroup V] [InnerProductSpace ℝ V] [FiniteDimensional ℝ V] [MeasurableSpace V] [BorelSpace V] variable {T α β : ℝ} (hα : 0 < α) (A : C(Slab T,V →ᵇ Icc α β)) (b : C(Slab T,V →ᵇ ℂ)) lemma contDiff_mildTime_of_correction (hT₀ : 0 ≤ T) (hT : T ≤ 1) (L B : ℝ) (hL : 0 ≤ L) (hB : 0 ≤ B) (hb : ∀ s, ‖b s‖ ≤ B) (hLip : ∀ s r : Slab T, ∀ x z : V, |(A s x).val-(A r z).val| ≤ L*(‖x-z‖+|s.val-r.val|)) (hLipb : ∀ s : Slab T, ∀ x z : V, ‖b s x-b s z‖ ≤ L*‖x-z‖) (d : C₀(V,ℂ)) (j : Time T →ᵇ C₀(V,ℂ)) (hi : ∀ t : Time T, IntervalIntegrable (fun r => residualKernel hα A b hT₀ t r (unweighted j r)) volume 0 t.val) (hj : ∀ t : Time T, unweighted j t.val + ∫ r in 0..t.val, residualKernel hα A b hT₀ t r (unweighted j r) = -actualResidual hα A b t (initial hT₀) d) (t : Time T) : ContDiff ℝ 4 (fun x => mildTime hα A hT₀ d j t.val x) := by obtain ⟨C,hC,hR⟩ := exists_actualResidual_holder_bound hα A b hT L B hL hB hb hLip hLipb (1/4) (by norm_num) (by norm_num) have hR' : ∀ (t : Time T) (s : Slab T), s.val c0Time hα (A (initial hT₀)) t.val d x) := by have he := funext (c0Time_apply hα (A (initial hT₀)) t.val t.property.1 d) rw [he] exact contDiff_infty.mp (contDiff_timeValue hα (A (initial hT₀)).toContinuousMap t.val t.property.1 d) 4 exact h0.add (contDiff_duhamel_of_holder A hT₀ hα L hL hLip j H hH hholder t) end ParametrixVolterra end end OAI