openAI-math-dataset / lean /OAI /Analysis /HotSpots /ClosedSolution.lean
roseking's picture
Add lean source and binary files (part 19)
9eeb9c7 verified
Raw History Blame Contribute Delete
26.2 kB
import OAI.Analysis.HotSpots.Multiplier
namespace OAI
section ClosedChartTopology
noncomputable section
open Set Metric
open scoped Topology
namespace StrictHotSpots.Conformal.ClosedDiskChart
open DiskH10 PlaneGreen
variable {Ω : Set Plane} (c : ClosedDiskChart Ω)
lemma complex_maps_disk {z : ℂ} (hz : z ∈ ball 0 1) : c.F (complexIso z) ∈ Ω := by
have hx : complexIso z ∈ disk := by simpa only [disk,mem_ball_zero_iff,LinearIsometryEquiv.norm_map] using hz
rw [← c.diskMap_agrees hx]
exact c.diskMap.map_source hx
lemma complex_maps_closed {z : ℂ} (hz : z ∈ closedBall 0 1) : c.F (complexIso z) ∈ closure Ω := by
apply c.maps_closed
simpa only [disk,closure_ball (0:Plane) (by norm_num : (1:ℝ) ≠ 0),mem_closedBall_zero_iff,
LinearIsometryEquiv.norm_map] using hz
lemma complex_maps_boundary (s : Circle) : c.F (complexIso (s:ℂ)) ∈ frontier Ω := by
apply c.maps_boundary
simp only [disk,frontier_ball (0:Plane) (by norm_num : (1:ℝ) ≠ 0),mem_sphere_zero_iff_norm,
LinearIsometryEquiv.norm_map,Circle.norm_coe]
lemma complex_inverse_disk {x : Plane} (hx : x ∈ Ω) : complexIso.symm (c.G x) ∈ ball 0 1 := by
have hh := c.diskMap.map_target hx
change c.diskMap.symm x ∈ disk at hh
rw [c.diskMap_inverse_agrees hx] at hh
simpa only [disk,mem_ball_zero_iff,LinearIsometryEquiv.norm_map] using hh
lemma complex_inverse_boundary {x : Plane} (hx : x ∈ frontier Ω) : ‖complexIso.symm (c.G x)‖ = 1 := by
have hh := c.inverse_maps_boundary hx
simpa only [disk,frontier_ball (0:Plane) (by norm_num : (1:ℝ) ≠ 0),mem_sphere_zero_iff_norm,
LinearIsometryEquiv.norm_map] using hh
lemma complex_inverse_image (S : Set Plane) (hs : S ⊆ Ω) :
(fun x => complexIso.symm (c.G x)) '' S = ball 0 1 ∩ (fun z => c.F (complexIso z)) ⁻¹' S := by
ext z
constructor
· rintro ⟨x,hx,rfl⟩
refine ⟨c.complex_inverse_disk (hs hx),?_⟩
simpa only [mem_preimage,LinearIsometryEquiv.apply_symm_apply,c.right_inverse x (subset_closure (hs hx))] using hx
· rintro ⟨hz,hx⟩
refine ⟨c.F (complexIso z),hx,?_⟩
have hd : complexIso z ∈ closure disk := by
exact subset_closure (by simpa only [disk,mem_ball_zero_iff,LinearIsometryEquiv.norm_map] using hz)
change complexIso.symm (c.G (c.F (complexIso z))) = z
rw [c.left_inverse _ (c.source_eq.symm ▸ hd),LinearIsometryEquiv.symm_apply_apply]
lemma connected_complex_pull {v : Plane → ℝ} {P : Set ℝ}
(hcon : IsConnected (Ω ∩ v ⁻¹' P)) :
IsConnected (ball (0:ℂ) 1 ∩ (fun z => v (c.F (complexIso z))) ⁻¹' P) := by
have hh := hcon.image (fun x => complexIso.symm (c.G x))
(complexIso.symm.continuous.comp c.inverse_lipschitz.continuous).continuousOn
rw [c.complex_inverse_image _ inter_subset_left] at hh
convert hh using 1
ext z
constructor
· rintro ⟨hz,hv⟩
exact ⟨hz,c.complex_maps_disk hz,hv⟩
· rintro ⟨hz,_,hv⟩
exact ⟨hz,hv⟩
def circleBoundaryHomeomorph : Circle ≃ₜ frontier Ω := by
classical
let f : Circle → frontier Ω := fun s => ⟨c.F (complexIso (s:ℂ)),c.complex_maps_boundary s⟩
let g : frontier Ω → Circle := fun x => ⟨complexIso.symm (c.G x),
mem_sphere_zero_iff_norm.mpr (c.complex_inverse_boundary x.property)⟩
have hleft : Function.LeftInverse g f := by
intro s
apply Subtype.ext
have hd : complexIso (s:ℂ) ∈ closure disk := by
simp only [disk,closure_ball (0:Plane) (by norm_num : (1:ℝ) ≠ 0),mem_closedBall_zero_iff,
LinearIsometryEquiv.norm_map,Circle.norm_coe,le_refl]
change complexIso.symm (c.G (c.F (complexIso (s:ℂ)))) = (s:ℂ)
rw [c.left_inverse _ (c.source_eq.symm ▸ hd),LinearIsometryEquiv.symm_apply_apply]
have hright : Function.RightInverse g f := by
intro x
apply Subtype.ext
change c.F (complexIso (complexIso.symm (c.G x))) = x
rw [LinearIsometryEquiv.apply_symm_apply,c.right_inverse x x.property.1]
exact {
toFun := f
invFun := g
left_inv := hleft
right_inv := hright
continuous_toFun := (c.lipschitz.continuous.comp (complexIso.continuous.comp continuous_subtype_val)).subtype_mk _
continuous_invFun := (complexIso.symm.continuous.comp (c.inverse_lipschitz.continuous.comp continuous_subtype_val)).subtype_mk _ }
end StrictHotSpots.Conformal.ClosedDiskChart
end
end ClosedChartTopology
section BoundaryCoordinateExtension
noncomputable section
open Set MeasureTheory Filter Metric Function
open scoped NNReal Topology InnerProductSpace
namespace StrictHotSpots.Conformal.ClosedDiskChart
open PlaneGreen DiskH10
variable {Ω : Set Plane} (c : ClosedDiskChart Ω)
theorem boundary_scalar_extension {f : Boundary → ℝ} {B : ℝ≥0} (hf : LipschitzWith B f) :
∃ (g : Plane → ℝ) (A : ℝ≥0), LipschitzWith A g ∧ ∀ s : Boundary, g (c.F s) = f s := by
classical
let f' (x : Plane) := if h : ‖x‖ = 1 then f ⟨x,h⟩ else 0
have hl : LipschitzOnWith B f' {x : Plane | ‖x‖ = 1} := by
intro x hx y hy
change ‖x‖ = 1 at hx
change ‖y‖ = 1 at hy
simpa only [f',dite_eq_left hx,dite_eq_left hy,Subtype.edist_eq] using hf ⟨x,hx⟩ ⟨y,hy⟩
obtain ⟨g,hg,he⟩ := hl.extend_real
refine ⟨g ∘ c.G,B*c.InvLip,hg.comp c.inverse_lipschitz,?_⟩
intro s
change g (c.G (c.F s)) = f s
rw [c.left_inverse s (c.source_eq.symm ▸ (by simp only [disk,closure_ball (0:Plane) (by norm_num : (1:ℝ) ≠ 0),mem_closedBall_zero_iff,s.property,le_refl]))]
exact (he s.property).symm.trans (by simp only [f',dite_eq_left s.property])
end StrictHotSpots.Conformal.ClosedDiskChart
namespace StrictHotSpots.HilbertMultipliers
lemma coordinate_lipschitz {H S ι : Type*} [NormedAddCommGroup H] [InnerProductSpace ℝ H]
[PseudoMetricSpace S] (e : HilbertBasis ι ℝ H) {b : S → H} {B : ℝ≥0}
(hb : LipschitzWith B b) (i : ι) : LipschitzWith B (fun s => inner ℝ (e i) (b s)) := by
apply LipschitzWith.of_dist_le_mul
intro s t
rw [Real.dist_eq,← inner_sub_right]
calc
|inner ℝ (e i) (b s-b t)| ≤ ‖e i‖*‖b s-b t‖ := abs_real_inner_le_norm _ _
_ = ‖b s-b t‖ := by rw [e.orthonormal.1 i,one_mul]
_ ≤ B*dist s t := by simpa only [dist_eq_norm] using hb.dist_le_mul s t
end StrictHotSpots.HilbertMultipliers
end
end BoundaryCoordinateExtension
section GreenClosedContinuous
noncomputable section
open Set MeasureTheory Filter Metric
open scoped Topology InnerProductSpace ENNReal
namespace StrictHotSpots.PlaneGreen
open DiskH10
lemma norm_le_of_mem_closure_disk {x : Plane} (hx : x ∈ closure disk) : ‖x‖ ≤ 1 := by
simpa only [disk,closure_ball (0:Plane) (by norm_num : (1:ℝ) ≠ 0),
mem_closedBall_zero_iff] using hx
lemma mem_disk_of_norm_lt {x : Plane} (hx : ‖x‖ < 1) : x ∈ disk := by
simpa only [disk,mem_ball_zero_iff] using hx
lemma kernel_zero_left {x : Plane} (hx : ‖x‖ = 1) (y : Plane) : kernel x y = 0 := by
simp [kernel_plane_formula,hx]
lemma kernel_continuousAt_left_closed {x y : Plane} (hx : x ∈ closure disk)
(hy : y ∈ disk) (hxy : x ≠ y) : ContinuousAt (fun z => kernel z y) x := by
have hx1 := norm_le_of_mem_closure_disk hx
have hy1 : ‖y‖ < 1 := by simpa only [disk,mem_ball_zero_iff] using hy
have hx2 : 0 ≤ 1-‖x‖^2 := by nlinarith [norm_nonneg x]
have hy2 : 0 ≤ 1-‖y‖^2 := by nlinarith [norm_nonneg y]
have hn : ‖x-y‖^2 ≠ 0 := pow_ne_zero _ (norm_ne_zero_iff.mpr (sub_ne_zero.mpr hxy))
have ha : 1+(1-‖x‖^2)*(1-‖y‖^2)/‖x-y‖^2 ≠ 0 := by positivity
simp_rw [kernel_plane_formula]
fun_prop (disch := assumption)
variable {ν : Measure Plane} {C : ℝ≥0∞} (hC : C ≠ (∞ : ℝ≥0∞))
(hν : ν ≤ C • volume.restrict disk)
include hC hν in
lemma kernel_memLp_closed (x : Plane) (hx : x ∈ closure disk) : MemLp (kernel x) 2 ν := by
by_cases hi : ‖x‖ < 1
· exact kernel_memLp_weighted hC hν x (mem_disk_of_norm_lt hi)
· have hn : ‖x‖ = 1 := le_antisymm (norm_le_of_mem_closure_disk hx) (not_lt.mp hi)
have he : kernel x = 0 := funext (kernel_zero_left hn)
rw [he]
exact MemLp.zero
include hC hν in
lemma kernel_uniform_three_bound_closed : ∃ B : ℝ≥0∞, B ≠ ∞ ∧
∀ x ∈ closure disk, eLpNorm (kernel x) 3 ν ≤ B := by
obtain ⟨B,hB,h⟩ := kernel_uniform_three_bound_weighted hC hν
refine ⟨B,hB,fun x hx => ?_⟩
by_cases hi : ‖x‖ < 1
· exact h x (mem_disk_of_norm_lt hi)
· have hn : ‖x‖ = 1 := le_antisymm (norm_le_of_mem_closure_disk hx) (not_lt.mp hi)
have he : kernel x = 0 := funext (kernel_zero_left hn)
rw [he,eLpNorm_zero]
exact bot_le
def closedRow (x : closure disk) : Lp ℝ 2 ν :=
(kernel_memLp_closed hC hν x x.property).toLp (kernel x)
lemma closedRow_coe_ae (x : closure disk) : closedRow hC hν x =ᵐ[ν] kernel x :=
(kernel_memLp_closed hC hν x x.property).coeFn_toLp
lemma closedRow_continuous [IsFiniteMeasure ν] : Continuous (closedRow hC hν) := by
apply continuous_iff_seqContinuous.mpr
intro u x hu
simp only [Function.comp_def,closedRow]
apply (Lp.tendsto_Lp_iff_tendsto_eLpNorm'' (fun n => kernel (u n))
(fun n => kernel_memLp_closed hC hν _ (u n).property) (kernel x)
(kernel_memLp_closed hC hν _ x.property)).mpr
apply tendsto_Lp_finite_of_tendsto_ae (by norm_num) (by norm_num)
(fun n => (kernel_memLp_closed hC hν _ (u n).property).aestronglyMeasurable)
(kernel_memLp_closed hC hν _ x.property)
· obtain ⟨B,hB,h⟩ := kernel_uniform_three_bound_closed hC hν
exact L2Limits.unifIntegrable_two_of_three
(fun n => (kernel_memLp_closed hC hν _ (u n).property).aestronglyMeasurable)
hB (fun n => h _ (u n).property)
· have hne : ∀ᵐ y ∂ν, y ≠ (x:Plane) :=
((volume.restrict disk).ae_ne (x:Plane)).filter_mono
(Measure.absolutelyContinuous_of_le_smul hν).ae_le
filter_upwards [ae_mem_disk hν,hne] with y hyd hyx
exact (kernel_continuousAt_left_closed x.property hyd hyx.symm).tendsto.comp
((continuous_subtype_val.tendsto x).comp hu)
lemma green_integral_eq_closedInner (f : Lp ℝ 2 ν) (x : closure disk) :
(∫ y, kernel x y*f y ∂ν) = inner ℝ (closedRow hC hν x) f := by
rw [MeasurableL2Kernel.integral_mul_eq_inner
(kernel_memLp_closed hC hν x x.property) (Lp.memLp f),Lp.toLp_coeFn]
rfl
include hC hν in
lemma green_integral_continuousOn_closure [IsFiniteMeasure ν] (f : Lp ℝ 2 ν) :
ContinuousOn (fun x : Plane => ∫ y, kernel x y*f y ∂ν) (closure disk) := by
apply continuousOn_iff_continuous_domRestrict.mpr
change Continuous (fun x : closure disk => ∫ y, kernel x y*f y ∂ν)
simp_rw [green_integral_eq_closedInner hC hν]
exact (closedRow_continuous hC hν).inner continuous_const
lemma green_integral_boundary (f : Lp ℝ 2 ν) {x : Plane} (hx : x ∈ frontier disk) :
(∫ y, kernel x y*f y ∂ν) = 0 := by
have hn : ‖x‖ = 1 := by
simpa only [disk,frontier_ball (0:Plane) (by norm_num : (1:ℝ) ≠ 0),
mem_sphere_zero_iff_norm] using hx
simp only [kernel_zero_left hn,zero_mul,integral_zero]
end StrictHotSpots.PlaneGreen
end
end GreenClosedContinuous
section BoundaryClosedSolution
noncomputable section
open Set MeasureTheory Filter Metric AddCircle
open scoped Topology ContDiff InnerProductSpace ENNReal NNReal
namespace StrictHotSpots.PlaneGreen
open DiskH10
local instance : Fact (0 < 2*Real.pi) := ⟨by positivity⟩
local notation "τ" => (2*Real.pi)
def boundaryClosedPoisson (f : C(Boundary,ℝ)) : Plane → ℝ :=
Douglas.closedPlanePoisson (boundaryAngleData f)
lemma boundaryClosedPoisson_interior (f : C(Boundary,ℝ)) {x : Plane} (hx : x ∈ disk) :
boundaryClosedPoisson f x = poissonExtension f x :=
(Douglas.closedPlanePoisson_eqOn (boundaryAngleData f) hx).trans
(poissonExtension_eq_planePoisson f hx).symm
lemma boundaryClosedPoisson_trace (f : C(Boundary,ℝ)) (s : Boundary) :
boundaryClosedPoisson f s = f s := by
obtain ⟨t,rfl⟩ := angleBoundary.surjective s
rw [angleBoundary_coe]
exact Douglas.closedPlanePoisson_boundary (boundaryAngleData f) t
lemma boundaryClosedPoisson_continuousOn (f : C(Boundary,ℝ)) {A : ℝ≥0}
(hf : LipschitzWith A f) : ContinuousOn (boundaryClosedPoisson f) (closure disk) :=
Douglas.closedPlanePoisson_continuousOn (boundaryAngleData f) A.coe_nonneg
(boundaryAngleData_lipschitz f hf)
variable {ν : Measure Plane} [IsFiniteMeasure ν] {C : ℝ≥0∞}
(hC : C ≠ (∞ : ℝ≥0∞)) (hν : ν ≤ C • volume.restrict disk)
def boundaryClosedSolution (f : C(Boundary,ℝ)) {B : ℝ}
(hB : ∀ s, ‖f s‖ ≤ B) (x : Plane) : ℝ :=
boundaryClosedPoisson f x + ∫ y, kernel x y *
(BanachResolvent.resolvent (weightedIntegralOperator hC hν)
(poissonL2 hν f.continuous.measurable hB)) y ∂ν
lemma boundaryClosedSolution_interior (f : C(Boundary,ℝ)) {B : ℝ}
(hB : ∀ s, ‖f s‖ ≤ B) {x : Plane} (hx : x ∈ disk) :
boundaryClosedSolution hC hν f hB x = boundarySolutionValue hC hν f hB x := by
exact congrArg (fun a => a + ∫ y, kernel x y *
(BanachResolvent.resolvent (weightedIntegralOperator hC hν)
(poissonL2 hν f.continuous.measurable hB)) y ∂ν) (boundaryClosedPoisson_interior f hx)
lemma boundaryClosedSolution_continuousOn (f : C(Boundary,ℝ)) {A : ℝ≥0}
(hf : LipschitzWith A f) {B : ℝ} (hB : ∀ s, ‖f s‖ ≤ B) :
ContinuousOn (boundaryClosedSolution hC hν f hB) (closure disk) :=
(boundaryClosedPoisson_continuousOn f hf).add
(green_integral_continuousOn_closure hC hν _)
lemma boundaryClosedSolution_trace (f : C(Boundary,ℝ)) {B : ℝ}
(hB : ∀ s, ‖f s‖ ≤ B) (s : Boundary) :
boundaryClosedSolution hC hν f hB s = f s := by
have hs : (s:Plane) ∈ frontier disk := by
simpa only [disk,frontier_ball (0:Plane) (by norm_num : (1:ℝ) ≠ 0), mem_sphere, dist_zero_right] using s.property
rw [boundaryClosedSolution,green_integral_boundary _ hs,add_zero,boundaryClosedPoisson_trace]
lemma boundaryClosedSolution_value_ae (f : C(Boundary,ℝ)) {A : ℝ≥0}
(hf : LipschitzWith A f) {B : ℝ} (hB : ∀ s, ‖f s‖ ≤ B) :
(H1.value (boundarySolution hC hν f hf) : Plane → ℝ) =ᵐ[volume.restrict disk]
boundaryClosedSolution hC hν f hB := by
filter_upwards [boundarySolution_value_ae hC hν f hf hB,
ae_restrict_mem diskOpen.measurableSet] with x hx hxd
exact hx.trans (boundaryClosedSolution_interior hC hν f hB hxd).symm
lemma boundaryClosedSolution_hasH1Gradient (f : C(Boundary,ℝ)) {A : ℝ≥0}
(hf : LipschitzWith A f) {B : ℝ} (hB : ∀ s, ‖f s‖ ≤ B) :
HasH1Gradient disk (boundaryClosedSolution hC hν f hB)
(H1.grad (boundarySolution hC hν f hf)) :=
(H1.hasH1Gradient _).congr (boundaryClosedSolution_value_ae hC hν f hf hB)
Filter.EventuallyEq.rfl
lemma boundaryClosedSolution_K (hT : ‖weightedIntegralOperator hC hν‖ < 1)
(f : C(Boundary,ℝ)) {B : ℝ} (hB : ∀ s, ‖f s‖ ≤ B) (x : disk) :
boundaryClosedSolution hC hν f hB x =
∫ s, fullBoundaryK hC hν x s*f s ∂boundaryMeasure := by
rw [boundaryClosedSolution_interior hC hν f hB x.property]
exact boundarySolution_K hC hν hT f hB x
end StrictHotSpots.PlaneGreen
end
end BoundaryClosedSolution
section PhysicalClosedSolution
noncomputable section
open Set MeasureTheory Filter
open scoped ContDiff InnerProductSpace ENNReal NNReal Topology
namespace StrictHotSpots.Conformal.ClosedDiskChart
open DiskH10 PlaneGreen
variable {Ω : Set Plane} (c : ClosedDiskChart Ω)
lemma inverse_map_chartMeasure : (volume.restrict Ω).map c.G = chartMeasure c.diskMap c.d := by
have hm : (chartMeasure c.diskMap c.d).map c.diskMap = volume.restrict Ω :=
map_chartMeasure c.diskMap c.d c.diskMap_deriv
rw [← hm,
AEMeasurable.map_map_of_aemeasurable c.inverse_lipschitz.continuous.aemeasurable
(chart_aemeasurable c.diskMap c.d)]
have he : c.G ∘ c.diskMap =ᵐ[chartMeasure c.diskMap c.d] id := by
filter_upwards [ae_chart_source c.diskMap c.d] with x hx
change c.G (c.diskMap x)=x
rw [c.diskMap_agrees hx]
exact c.left_inverse x (c.source_eq.symm ▸ subset_closure hx)
rw [Measure.map_congr he,Measure.map_id]
lemma pull_ae_to_physical {f g : Plane → ℝ}
(h : f ∘ c.diskMap =ᵐ[chartMeasure c.diskMap c.d] g) :
f =ᵐ[volume.restrict Ω] (g ∘ c.G) := by
have hg : f ∘ c.diskMap =ᵐ[(volume.restrict Ω).map c.G] g :=
c.inverse_map_chartMeasure.symm ▸ h
have ha := ae_of_ae_map c.inverse_lipschitz.continuous.aemeasurable hg
filter_upwards [ha,ae_restrict_mem c.diskMap.open_target.measurableSet] with y hy hyΩ
have hi : c.diskMap (c.G y)=y := by
rw [← c.diskMap_inverse_agrees hyΩ]
exact c.diskMap.right_inv hyΩ
simpa only [Function.comp_apply,hi] using hy
lemma physicalSolution_pull_ae (hb : Bornology.IsBounded Ω) (hs : SmoothBoundary Ω)
(hμ : 0 ≤ firstPositiveNeumannValue Ω)
{w : Plane → ℝ} (hw : ContDiffOn ℝ ∞ w (closure Ω)) {B : ℝ≥0}
(hl : LipschitzWith B (c.datumTrace w hw.continuousOn)) :
(H1.value (c.physicalSolution hb hs hμ hw hl) : Plane → ℝ) ∘ c.diskMap
=ᵐ[chartMeasure c.diskMap c.d]
H1.value (boundarySolution c.densityBound_ne_top (c.density_bound hμ)
(c.datumTrace w hw.continuousOn) hl) := by
have h := affine_value_ae c.diskMap c.diskMap_inverse_smooth c.d c.diskMap_deriv hb
(smooth_closure_H1 (Ω:=Ω) (show IsOpen Ω from c.diskMap.open_target) hb hs hw)
(c.pullDatum_comp_H1 hb hs hw) (c.datumCorrection hb hs hμ hw hl)
have he : (c.pullDatum_comp_H1 hb hs hw).toH1+(c.datumCorrection hb hs hμ hw hl).val =
boundarySolution c.densityBound_ne_top (c.density_bound hμ)
(c.datumTrace w hw.continuousOn) hl :=
(congrArg (fun V : H1 disk => V+(c.datumCorrection hb hs hμ hw hl).val)
(c.pullDatum_comp_toH1 hb hs hw)).trans (c.datumCorrection_spec hb hs hμ hw hl).symm
exact (chartPull_ae c.diskMap c.d c.diskMap_deriv _).symm.trans
(h.trans (EventuallyEq.of_eq (congrArg (fun V : H1 disk => (H1.value V : Plane → ℝ)) he)))
lemma physicalSolution_closed_ae (hb : Bornology.IsBounded Ω) (hs : SmoothBoundary Ω)
(hμ : 0 ≤ firstPositiveNeumannValue Ω)
{w : Plane → ℝ} (hw : ContDiffOn ℝ ∞ w (closure Ω)) {B : ℝ≥0}
(hl : LipschitzWith B (c.datumTrace w hw.continuousOn)) {M : ℝ}
(hM : ∀ s : Boundary, ‖w (c.F s)‖ ≤ M) :
let _ : IsFiniteMeasure c.potential := c.potential_finite hb
(H1.value (c.physicalSolution hb hs hμ hw hl) : Plane → ℝ)
=ᵐ[volume.restrict Ω]
(boundaryClosedSolution c.densityBound_ne_top (c.density_bound hμ)
(c.datumTrace w hw.continuousOn) hM) ∘ c.G := by
let _ : IsFiniteMeasure c.potential := c.potential_finite hb
apply c.pull_ae_to_physical
exact (c.physicalSolution_pull_ae hb hs hμ hw hl).trans
((chartMeasure_ac c.diskMap c.d).ae_le
(boundaryClosedSolution_value_ae c.densityBound_ne_top (c.density_bound hμ)
(c.datumTrace w hw.continuousOn) hl hM))
end StrictHotSpots.Conformal.ClosedDiskChart
end
end PhysicalClosedSolution
section BoundaryClosedConvergence
noncomputable section
open Set MeasureTheory Filter
open scoped ContDiff InnerProductSpace ENNReal NNReal Topology
namespace StrictHotSpots.PlaneGreen
open DiskH10
variable {ν : Measure Plane} [IsFiniteMeasure ν] {C : ℝ≥0∞}
(hC : C ≠ (∞ : ℝ≥0∞)) (hν : ν ≤ C • volume.restrict disk)
lemma boundaryClosedSolution_tendsto (hT : ‖weightedIntegralOperator hC hν‖ < 1)
(fn : ℕ → C(Boundary,ℝ)) (f : C(Boundary,ℝ)) {M B : ℝ}
(hm : ∀ n s, ‖fn n s‖ ≤ M) (hb : ∀ s, ‖f s‖ ≤ B)
(ht : ∀ s, Tendsto (fun n => fn n s) atTop (𝓝 (f s))) (p : disk) :
Tendsto (fun n => boundaryClosedSolution hC hν (fn n) (hm n) p)
atTop (𝓝 (boundaryClosedSolution hC hν f hb p)) := by
obtain ⟨A,hA,hAb⟩ := fullBoundaryK_bounded hC hν p
have hn (s : Boundary) : ‖fullBoundaryK hC hν p s‖ ≤ A := by
rw [Real.norm_of_nonneg (fullBoundaryK_pos hC hν hT p s).le]
exact hAb s
simp only [boundaryClosedSolution_K hC hν hT]
apply tendsto_integral_of_dominated_convergence (fun _ : Boundary => A*M)
· intro n
exact ((fullBoundaryK_measurable hC hν p).mul (fn n).continuous.measurable).aestronglyMeasurable
· exact integrable_const _
· intro n
exact Eventually.of_forall fun s => (norm_mul _ _).trans_le
(mul_le_mul (hn s) (hm n s) (norm_nonneg _) hA)
· exact Eventually.of_forall fun s => (ht s).const_mul _
end StrictHotSpots.PlaneGreen
end
end BoundaryClosedConvergence
section PhysicalMultiplierClosed
noncomputable section
open Set MeasureTheory Filter
open scoped ContDiff InnerProductSpace ENNReal NNReal Topology
namespace StrictHotSpots.Conformal.ClosedDiskChart
open DiskH10 PlaneGreen Hodge
variable {Ω : Set Plane} (c : ClosedDiskChart Ω) (hΩ : AdmissibleDomain Ω)
variable (hμ : 0 < firstPositiveNeumannValue Ω)
variable {L : ℝ} (hl : firstPositiveNeumannValue Ω < L)
(hD : ∀ j : H10 hΩ.2.1, L*‖H10.value hΩ.2.1 j‖^2 ≤ ‖H10.grad hΩ.2.1 j‖^2)
lemma scalarSolution_closed_ae {w : Plane → ℝ} (hw : ContDiffOn ℝ ∞ w (closure Ω))
{M : ℝ} (hM : ∀ s : Boundary, ‖w (c.F s)‖ ≤ M) :
let _ : IsFiniteMeasure c.potential := c.potential_finite hΩ.2.2.1
(H1.value (c.scalarSolution hΩ.2.2.1 hΩ.2.2.2.2 hμ hw) : Plane → ℝ)
=ᵐ[volume.restrict Ω]
(boundaryClosedSolution c.densityBound_ne_top (c.density_bound hμ.le)
(c.datumTrace w hw.continuousOn) hM) ∘ c.G :=
c.physicalSolution_closed_ae hΩ.2.2.1 hΩ.2.2.2.2 hμ.le hw _ hM
lemma scalarSolution_mul_tendsto {w b : Plane → ℝ}
(hw : ContDiffOn ℝ ∞ w (closure Ω)) {B : ℝ≥0} (hb : LipschitzWith B b) :
Tendsto (fun n => c.scalarSolution hΩ.2.2.1 hΩ.2.2.2.2 hμ
((ambientSmooth_smooth (planeApproxBump n) hb).contDiffOn.mul hw)) atTop
(𝓝 (PhysicalHelmholtz.extension hΩ.2.1 hΩ.2.2.1 hμ.le hl hD
(H1.lipschitzMul hΩ.2.1 hΩ.2.2.1 hb (smooth_closure_H1 hΩ.2.1 hΩ.2.2.1 hΩ.2.2.2.2 hw).toH1))) := by
let U := (smooth_closure_H1 hΩ.2.1 hΩ.2.2.1 hΩ.2.2.2.2 hw).toH1
have ht := (PhysicalHelmholtz.extension hΩ.2.1 hΩ.2.2.1 hμ.le hl hD).continuous.continuousAt.tendsto.comp
(smoothMul_tendsto_lipschitzMul hΩ.2.1 hΩ.2.2.1 hb U)
apply ht.congr'
apply Eventually.of_forall
intro n
have hen := smoothMul_smooth_closure hΩ.2.1 hΩ.2.2.1 hΩ.2.2.2.2
(ambientSmooth_smooth (planeApproxBump n) hb)
(continuous_closure_memLp_top hΩ.2.1 hΩ.2.2.1
(ambientSmooth_lipschitz (planeApproxBump n) hb).continuous.continuousOn)
(lipschitz_gradient_memLp_top (ambientSmooth_lipschitz (planeApproxBump n) hb)) hw
exact ((c.scalarSolution_eq_extension hΩ hμ hl hD
((ambientSmooth_smooth (planeApproxBump n) hb).contDiffOn.mul hw)).trans
(congrArg (PhysicalHelmholtz.extension hΩ.2.1 hΩ.2.2.1 hμ.le hl hD) hen.symm)).symm
def multiplierTrace {b : Plane → ℝ} {B : ℝ≥0} (hb : LipschitzWith B b)
(w : Plane → ℝ) (hw : ContinuousOn w (closure Ω)) : C(Boundary,ℝ) where
toFun s := b (c.F s)*w (c.F s)
continuous_toFun := (c.physical_boundary_lipschitz hb).continuous.mul (c.datumTrace w hw).continuous
include hΩ in
lemma multiplierTrace_lipschitz {b w : Plane → ℝ} {B : ℝ≥0} (hb : LipschitzWith B b)
(hw : ContDiffOn ℝ ∞ w (closure Ω)) :
∃ A : ℝ≥0, LipschitzWith A (c.multiplierTrace hb w hw.continuousOn) := by
obtain ⟨D,hD⟩ := c.datumTrace_lipschitz hΩ.2.2.1 hΩ.2.2.2.2 hw
exact boundary_smul_lipschitz (c.physical_boundary_lipschitz hb) hD
lemma physical_lipschitzMul_closed_ae {w b : Plane → ℝ}
(hw : ContDiffOn ℝ ∞ w (closure Ω)) {B : ℝ≥0} (hb : LipschitzWith B b)
{A : ℝ} (hA : ∀ s, ‖c.multiplierTrace hb w hw.continuousOn s‖ ≤ A) :
let _ : IsFiniteMeasure c.potential := c.potential_finite hΩ.2.2.1
(H1.value (PhysicalHelmholtz.extension hΩ.2.1 hΩ.2.2.1 hμ.le hl hD
(H1.lipschitzMul hΩ.2.1 hΩ.2.2.1 hb (smooth_closure_H1 hΩ.2.1 hΩ.2.2.1 hΩ.2.2.2.2 hw).toH1)) : Plane → ℝ)
=ᵐ[volume.restrict Ω]
(boundaryClosedSolution c.densityBound_ne_top (c.density_bound hμ.le)
(c.multiplierTrace hb w hw.continuousOn) hA) ∘ c.G := by
let _ : IsFiniteMeasure c.potential := c.potential_finite hΩ.2.2.1
let hn (n : ℕ) := (ambientSmooth_smooth (planeApproxBump n) hb).contDiffOn.mul hw
let fn (n : ℕ) := c.datumTrace _ (hn n).continuousOn
obtain ⟨M,hM,hMb⟩ := c.smooth_physical_boundary_bound hΩ hb
obtain ⟨W,hW,hWb⟩ := boundary_continuous_bound (c.datumTrace w hw.continuousOn).continuous
have hMW (n : ℕ) (s : Boundary) : ‖fn n s‖ ≤ M*W := by
change ‖ambientSmooth (planeApproxBump n) b (c.F s)*w (c.F s)‖ ≤ M*W
rw [norm_mul]
exact mul_le_mul (hMb n s) (hWb s) (norm_nonneg _) hM
have ht (s : Boundary) : Tendsto (fun n => fn n s) atTop
(𝓝 (c.multiplierTrace hb w hw.continuousOn s)) :=
(ambientSmooth_tendsto planeApproxBump_rOut_tendsto hb (c.F s)).mul_const _
have he (n : ℕ) := c.scalarSolution_closed_ae hΩ hμ (hn n) (hMW n)
have hv := H1.value.continuous.continuousAt.tendsto.comp
(c.scalarSolution_mul_tendsto hΩ hμ hl hD hw hb)
obtain ⟨φ,hφ,hφae⟩ := (tendstoInMeasure_of_tendsto_Lp hv).exists_seq_tendsto_ae
filter_upwards [hφae,ae_all_iff.mpr he,ae_restrict_mem hΩ.2.1.measurableSet] with x hx hxe hxΩ
have hxD : c.G x ∈ disk := by
rw [← c.diskMap_inverse_agrees hxΩ]
exact c.diskMap.map_target hxΩ
have hk := boundaryClosedSolution_tendsto c.densityBound_ne_top (c.density_bound hμ.le)
(c.operator_norm_lt_one hΩ.2.2.1 hΩ.1 hμ) fn (c.multiplierTrace hb w hw.continuousOn)
hMW hA ht ⟨c.G x,hxD⟩
apply tendsto_nhds_unique hx
exact (hk.comp hφ.tendsto_atTop).congr' (Eventually.of_forall fun n => (hxe (φ n)).symm)
end StrictHotSpots.Conformal.ClosedDiskChart
end
end PhysicalMultiplierClosed
end OAI