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import OAI.Dynamics.SmoothObstruction.TubeProjection
namespace OAI
section
open MeasureTheory Filter Topology TopologicalSpace Set Finset
open scoped ENNReal NNReal BoundedContinuousFunction
open Finset MeasureTheory Filter Topology
open scoped BigOperators
open Finset Matrix
open scoped Matrix.Norms.L2Operator
open Matrix
namespace SmoothObstruction.CanonicalRelation
open Set MeasureTheory Filter Topology
variable {X Y : Type*} [MeasurableSpace X] [MeasurableSpace Y]
[StandardBorelSpace X] [StandardBorelSpace Y]
/-- A Borel relation with exactly one output at every input has a genuine
measurable solution map. Its definition does not depend on any auxiliary
frame certificate used to obtain existence and uniqueness. -/
theorem measurable_solution (R : Set (X × Y)) (hR : MeasurableSet R)
(hex : ∀ x,∃! y,(x,y)∈R) :
∃ f : X → Y,Measurable f ∧ (∀ x,(x,f x)∈R) ∧
∀ x y,(x,y)∈R → y=f x := by
classical
let f : X → Y := fun x => (hex x).choose
have hf (x : X) : (x,f x)∈R := (hex x).choose_spec.1
have hu (x : X) (y : Y) (hy : (x,y)∈R) : y=f x :=
(hex x).choose_spec.2 y hy
let : StandardBorelSpace R := hR.standardBorel
let π : R → X := fun z => z.val.1
have hπ : Measurable π := measurable_fst.comp measurable_subtype_coe
have hsurj : Function.Surjective π := fun x => ⟨⟨(x,f x),hf x⟩,rfl⟩
have he : f ∘ π=(fun z : R => z.val.2) := by
funext z
exact (hu z.val.1 z.val.2 z.property).symm
have hm : Measurable (f ∘ π) := by
rw [he]
exact measurable_snd.comp measurable_subtype_coe
exact ⟨f,(Measurable.measurable_comp_iff_of_surjective hπ hsurj).mp hm,hf,hu⟩
/-- The retained set has its original Borel subspace, not a conditioned
probability space. The measurable total extension is only for convenient
pushforward notation; it is equal to the canonical solution on the carrier. -/
theorem retained_solution [Nonempty Y] (G : Set X) (hG : MeasurableSet G)
(R : X → Y → Prop) (hR : MeasurableSet {z : X×Y | z.1∈G ∧ R z.1 z.2})
(hex : ∀ x∈G,∃! y,R x y) :
∃ f : X → Y,Measurable f ∧ (∀ x∈G,R x (f x)) ∧
∀ x∈G,∀ y,R x y → y=f x := by
classical
let : StandardBorelSpace G := hG.standardBorel
let R' : Set (G×Y) := {z | R z.1.val z.2}
have hR' : MeasurableSet R' := by
have hm : Measurable (fun z : G×Y => (z.1.val,z.2)) :=
(measurable_subtype_coe.comp measurable_fst).prodMk measurable_snd
have he : R'= (fun z : G×Y => (z.1.val,z.2)) ⁻¹' {z : X×Y | z.1∈G ∧ R z.1 z.2} := by
ext z
simp only [R',mem_ofPred_eq,Set.mem_preimage]
exact ⟨fun h => ⟨z.1.property,h⟩,fun h => h.2⟩
rw [he]
exact hR.preimage hm
obtain ⟨f,hf,hfr,hfu⟩ := measurable_solution R' hR' (fun x => hex x x.property)
obtain ⟨F,hF,hFf⟩ := (MeasurableEmbedding.subtype_coe hG).exists_measurable_extend hf
(fun _ => inferInstance)
have he (x : G) : F x=f x := congrFun hFf x
refine ⟨F,hF,?_,?_⟩
· intro x hx
rw [he ⟨x,hx⟩]
exact hfr ⟨x,hx⟩
· intro x hx y hy
rw [he ⟨x,hx⟩]
exact hfu ⟨x,hx⟩ y hy
end SmoothObstruction.CanonicalRelation
namespace SmoothObstruction.CanonicalRelation
open Set Filter Topology
variable {E F : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E]
[NormedAddCommGroup F] [NormedSpace ℝ F]
/-- Local analytic branches agree with the canonical Borel solution merely
by satisfying its boundary relation inside the uniqueness tube. The frame
witnesses and chart codes need not be continuous functions of the inputs. -/
theorem local_derivative (G : Set E) (x : E) (hx : x∈G)
(R : E → F → Prop) (f g : E → F) (L : E →L[ℝ] F)
(hu : ∀ u∈G,∀ v,R u v → v=f u)
(hg : HasFDerivAt g L x) (hrel : ∀ᶠ u in 𝓝[G] x,R u (g u)) :
HasFDerivWithinAt f L G x := by
have he : g =ᶠ[𝓝[G] x] f := by
filter_upwards [hrel,self_mem_nhdsWithin] with u huR huG
exact hu u huG (g u) huR
exact hg.hasFDerivWithinAt.congr_of_eventuallyEq he.symm (he.eq_of_nhdsWithin hx).symm
end SmoothObstruction.CanonicalRelation
namespace SmoothObstruction.SelectedTube
open Set MeasureTheory
variable {X C E : Type*} [MeasurableSpace X] [Fintype C]
[MeasurableSpace C] [MeasurableSingletonClass C]
[NormedAddCommGroup E] [MeasurableSpace E] [BorelSpace E] [SecondCountableTopology E]
/-- The literal fixed-atlas coordinate tube, with chart sources checked.
Only the base point chooses the chart; the second point need not be good. -/
def tube (q : X → C) (U : C → Set X) (φ : C → X → E)
(f : ℕ → X → X) (n : ℕ) (δ : ℝ) (x z : X) : Prop :=
∀ t : Fin (n+1),f t z∈U (q (f t x)) ∧
‖φ (q (f t x)) (f t z)-φ (q (f t x)) (f t x)‖≤δ
omit [NormedAddCommGroup E] [BorelSpace E] [SecondCountableTopology E] in
lemma measurable_evaluate (φ : C → X → E) (hφ : ∀ c,Measurable (φ c)) :
Measurable (fun p : C×X => φ p.1 p.2) :=
measurable_from_prod_countable_right hφ
lemma measurable_tube (q : X → C) (hq : Measurable q)
(U : C → Set X) (hU : ∀ c,MeasurableSet (U c))
(φ : C → X → E) (hφ : ∀ c,Measurable (φ c))
(f : ℕ → X → X) (hf : ∀ t,Measurable (f t)) (n : ℕ) (δ : ℝ) :
MeasurableSet {p : X×X | tube q U φ f n δ p.1 p.2} := by
have hu : MeasurableSet {p : C×X | p.2∈U p.1} := by
have he : {p : C×X | p.2∈U p.1}=⋃ c,({c} ×ˢ U c) := by
ext p
simp only [mem_ofPred_eq,mem_iUnion,mem_prod,mem_singleton_iff]
exact ⟨fun h => ⟨p.1,rfl,h⟩,fun ⟨c,hc,h⟩ => hc ▸ h⟩
rw [he]
exact MeasurableSet.iUnion (fun c => (measurableSet_singleton c).prod (hU c))
simp only [tube,Set.ofPred_forall]
apply MeasurableSet.iInter
intro t
have hx : Measurable (fun p : X×X => f t p.1) := (hf t).comp measurable_fst
have hz : Measurable (fun p : X×X => f t p.2) := (hf t).comp measurable_snd
have hc := hq.comp hx
exact (hu.preimage (hc.prodMk hz)).inter
(measurableSet_le (((measurable_evaluate φ hφ).comp (hc.prodMk hz)).sub
((measurable_evaluate φ hφ).comp (hc.prodMk hx))).norm measurable_const)
end SmoothObstruction.SelectedTube
namespace SmoothObstruction.MeasurableSwitch
open Set MeasureTheory
variable {X C E : Type*} [MeasurableSpace X] [Fintype C]
[MeasurableSpace C] [MeasurableSingletonClass C]
[NormedAddCommGroup E] [MeasurableSpace E] [BorelSpace E] [SecondCountableTopology E]
/-- Fixed-bin future/past observations and the two old coordinate tubes.
All auxiliary frames have disappeared from this boundary relation. -/
def relation (F P : X → X → E) (TF TB : X → X → Prop) (u : X×X) (z : X) : Prop :=
F u.1 z=F u.1 u.1 ∧ P u.2 z=P u.2 u.2 ∧ TF u.1 z ∧ TB u.2 z
lemma measurable_relation (F P : X → X → E)
(hF : Measurable (Function.uncurry F)) (hP : Measurable (Function.uncurry P))
(TF TB : X → X → Prop) (hTF : MeasurableSet {p : X×X | TF p.1 p.2})
(hTB : MeasurableSet {p : X×X | TB p.1 p.2}) :
MeasurableSet {p : (X×X)×X | relation F P TF TB p.1 p.2} := by
have h₁ : Measurable (fun p : (X×X)×X => (p.1.1,p.2)) :=
(measurable_fst.comp measurable_fst).prodMk measurable_snd
have h₂ : Measurable (fun p : (X×X)×X => (p.1.2,p.2)) :=
(measurable_snd.comp measurable_fst).prodMk measurable_snd
have hx : Measurable (fun p : (X×X)×X => p.1.1) :=
measurable_fst.comp measurable_fst
have hy : Measurable (fun p : (X×X)×X => p.1.2) :=
measurable_snd.comp measurable_fst
exact (measurableSet_eq_fun (hF.comp h₁) (hF.comp (hx.prodMk hx))).inter
((measurableSet_eq_fun (hP.comp h₂) (hP.comp (hy.prodMk hy))).inter
((hTF.preimage h₁).inter (hTB.preimage h₂)))
/-- The original retained carrier gives one globally measurable pair map.
There is no measurable moving-frame selection and no conditioning of a law.
Existence and uniqueness are supplied by the actual finite-tube solve. -/
theorem canonical_pair [StandardBorelSpace X] [Nonempty X]
(G : Set (X×X)) (hG : MeasurableSet G)
(F P : X → X → E) (hF : Measurable (Function.uncurry F))
(hP : Measurable (Function.uncurry P))
(TF TB : X → X → Prop) (hTF : MeasurableSet {p : X×X | TF p.1 p.2})
(hTB : MeasurableSet {p : X×X | TB p.1 p.2})
(hex : ∀ u∈G,∃! z,relation F P TF TB u z)
(hex' : ∀ u∈G,∃! w,relation F P TF TB u.swap w) :
∃ Φ : X×X → X×X,Measurable Φ ∧
(∀ u∈G,relation F P TF TB u (Φ u).1 ∧ relation F P TF TB u.swap (Φ u).2) ∧
(∀ u∈G,∀ z,relation F P TF TB u z → z=(Φ u).1) ∧
(∀ u∈G,∀ w,relation F P TF TB u.swap w → w=(Φ u).2) := by
have hR := measurable_relation F P hF hP TF TB hTF hTB
have hRG : MeasurableSet {p : (X×X)×X | p.1∈G ∧ relation F P TF TB p.1 p.2} :=
(hG.preimage measurable_fst).inter hR
have hRG' : MeasurableSet {p : (X×X)×X | p.1∈G ∧ relation F P TF TB p.1.swap p.2} :=
(hG.preimage measurable_fst).inter (hR.preimage
((measurable_swap.comp measurable_fst).prodMk measurable_snd))
obtain ⟨z,hz,hzr,hzu⟩ := CanonicalRelation.retained_solution G hG
(relation F P TF TB) hRG hex
obtain ⟨w,hw,hwr,hwu⟩ := CanonicalRelation.retained_solution G hG
(fun u => relation F P TF TB u.swap) hRG' hex'
exact ⟨fun u => (z u,w u),hz.prodMk hw,fun u hu => ⟨hzr u hu,hwr u hu⟩,hzu,hwu⟩
end SmoothObstruction.MeasurableSwitch
namespace SmoothObstruction.EndpointObservation
open Set MeasureTheory
variable {X C B E : Type*} [MeasurableSpace X]
[Fintype C] [Fintype B] [MeasurableSpace C] [MeasurableSingletonClass C]
[MeasurableSpace B] [MeasurableSingletonClass B]
[NormedAddCommGroup E] [NormedSpace ℝ E] [MeasurableSpace E] [BorelSpace E]
/-- The source endpoint observation in the ambient coordinate space. Its
finite index consists ONLY of the starting coarse bin and endpoint coarse
bin; an internal frame witness is not part of this index. -/
def observation (c : X → C) (b : X → B) (f : X → X)
(φ : B → X → E) (P : C → B → E →L[ℝ] E) (x z : X) : E :=
P (c x) (b (f x)) (φ (b (f x)) (f z))
lemma measurable_observation (c : X → C) (hc : Measurable c)
(b : X → B) (hb : Measurable b) (f : X → X) (hf : Measurable f)
(φ : B → X → E) (hφ : ∀ j,Measurable (φ j)) (P : C → B → E →L[ℝ] E) :
Measurable (Function.uncurry (observation c b f φ P)) := by
have hh : Measurable (fun u : (C×B)×X => P u.1.1 u.1.2 (φ u.1.2 (f u.2))) := by
apply measurable_from_prod_countable_right
intro ij
exact (P ij.1 ij.2).continuous.measurable.comp ((hφ ij.2).comp hf)
exact hh.comp (((hc.comp measurable_fst).prodMk
(hb.comp (hf.comp measurable_fst))).prodMk measurable_snd)
omit [MeasurableSpace X] [Fintype C] [Fintype B]
[MeasurableSpace C] [MeasurableSingletonClass C]
[MeasurableSpace B] [MeasurableSingletonClass B] [MeasurableSpace E] [BorelSpace E]
/-- Positive bin margins turn the ambient observations into the actual fixed
smooth endpoint maps on a neighborhood; there is no differentiability claim
for the discontinuously selected observation itself. -/
lemma observation_fixed (c : X → C) (b : X → B) (f : X → X)
(φ : B → X → E) (P : C → B → E →L[ℝ] E)
(x y z : X) (hc : c x=c y) (hb : b (f x)=b (f y)) :
observation c b f φ P x z=observation c b f φ P y z := by
simp only [observation,hc,hb]
lemma observation_eq_iff (c : X → C) (b : X → B) (f : X → X)
(φ : B → X → E) (P : C → B → E →L[ℝ] E) (x y z : X) :
observation c b f φ P x z=observation c b f φ P x y ↔
P (c x) (b (f x)) (φ (b (f x)) (f z)-φ (b (f x)) (f y))=0 := by
simp only [observation,map_sub,sub_eq_zero]
end SmoothObstruction.EndpointObservation
namespace SmoothObstruction.ManifoldCoordinates
open Set MeasureTheory
open scoped Manifold ContDiff
variable {d : ℕ} {H : Type*} [TopologicalSpace H]
(I : ModelWithCorners ℝ (EuclideanSpace ℝ (Fin d)) H)
{M : Type*} [MetricSpace M] [ChartedSpace H M]
/-- A chart has no prescribed behaviour outside its source. This Borel
extension, used only to state global relations, agrees with it on the source. -/
noncomputable def borelChart (a : M) : M → EuclideanSpace ℝ (Fin d) := by
classical
exact (chartAt H a).source.piecewise (extChartAt I a) (fun _ => 0)
lemma borelChart_eq (a z : M) (hz : z∈(chartAt H a).source) :
borelChart I a z=(extChartAt I a) z := by
classical
exact Set.piecewise_eq_of_mem _ _ _ hz
variable [MeasurableSpace M] [BorelSpace M]
lemma measurable_borelChart (a : M) : Measurable (borelChart I a) := by
classical
apply ContinuousOn.measurable_piecewise _ continuousOn_const (chartAt H a).open_source.measurableSet
simpa only [extChartAt_source] using continuousOn_extChartAt (I:=I) a
variable {ι C : Type*} [Fintype ι] [MeasurableSpace ι] [MeasurableSingletonClass ι]
[Fintype C] [MeasurableSpace C] [MeasurableSingletonClass C]
(S : Diffeomorph I I M M ∞) (a : ι → M) (c : M → ι) (n : ℕ)
lemma measurable_originalTube (hc : Measurable c)
(hsource : ∀ z,z∈(chartAt H (a (c z))).source) (δ : ℝ) :
MeasurableSet {p : M×M | originalTube I S a c (n:=n) δ p.1 p.2} := by
have he : {p : M×M | originalTube I S a c (n:=n) δ p.1 p.2}=
{p | SelectedTube.tube c (fun j => (chartAt H (a j)).source)
(fun j => borelChart I (a j)) (fun t => S^[t]) n δ p.1 p.2} := by
ext p
constructor <;> intro hp t <;> obtain ⟨hs,ht⟩ := hp t
· exact ⟨hs,by simpa only [borelChart_eq I _ _ hs,
borelChart_eq I _ _ (hsource _)] using ht⟩
· exact ⟨hs,by simpa only [borelChart_eq I _ _ hs,
borelChart_eq I _ _ (hsource _)] using ht⟩
rw [he]
exact SelectedTube.measurable_tube c hc (fun j => (chartAt H (a j)).source)
(fun j => (chartAt H (a j)).open_source.measurableSet)
(fun j => borelChart I (a j)) (fun j => measurable_borelChart I (a j))
(fun t => S^[t]) (fun t => S.continuous.measurable.iterate t) n δ
noncomputable def originalObservation (P : M → C)
(W : C×C → Submodule ℝ (EuclideanSpace ℝ (Fin d))) (x z : M) :=
(W (P x,P (S^[n] x))).starProjection
(borelChart I (a (c (S^[n] x))) (S^[n] z))
lemma measurable_originalObservation (hc : Measurable c) (P : M → C) (hP : Measurable P)
(W : C×C → Submodule ℝ (EuclideanSpace ℝ (Fin d))) :
Measurable (Function.uncurry (originalObservation I S a c n P W)) := by
exact EndpointObservation.measurable_observation P hP (fun x => (P x,c x))
(hP.prodMk hc) (S^[n]) (S.continuous.measurable.iterate n)
(fun j : C×ι => borelChart I (a j.2)) (fun j => measurable_borelChart I (a j.2))
(fun q j => (W (q,j.1)).starProjection)
omit [MeasurableSpace M] [BorelSpace M]
[Fintype ι] [MeasurableSpace ι] [MeasurableSingletonClass ι]
[Fintype C] [MeasurableSpace C] [MeasurableSingletonClass C]
lemma originalObservation_eq_iff (P : M → C)
(W : C×C → Submodule ℝ (EuclideanSpace ℝ (Fin d))) (x z : M)
(hx : S^[n] x∈(chartAt H (a (c (S^[n] x)))).source)
(hz : S^[n] z∈(chartAt H (a (c (S^[n] x)))).source) :
originalObservation I S a c n P W x z=originalObservation I S a c n P W x x ↔
originalEndpoint I S a c (n:=n) (W (P x,P (S^[n] x))) x z := by
simp only [originalObservation,originalEndpoint,borelChart_eq I _ _ hx,borelChart_eq I _ _ hz]
lemma originalTube_mono {δ ε : ℝ} {x z : M} (h : δ≤ε)
(hx : originalTube I S a c (n:=n) δ x z) :
originalTube I S a c (n:=n) ε x z := fun t => ⟨(hx t).1,(hx t).2.trans h⟩
end SmoothObstruction.ManifoldCoordinates
namespace SmoothObstruction.ManifoldCoordinates
open Set Metric MeasureTheory
open scoped Manifold ContDiff Matrix.Norms.L2Operator
variable {d : ℕ} {H : Type*} [TopologicalSpace H]
(I : ModelWithCorners ℝ (EuclideanSpace ℝ (Fin d)) H)
{M : Type*} [MetricSpace M] [ChartedSpace H M] [IsManifold I ∞ M]
[MeasurableSpace M] [BorelSpace M] [StandardBorelSpace M] [Nonempty M]
{ι : Type*} [Fintype ι] [MeasurableSpace ι] [MeasurableSingletonClass ι]
open FiniteGreen ShortBin
/-- A measurable, witness-independent ORIGINAL pair switch. Its Borel relation
uses zero-extended charts, but all asserted equations and tube estimates are in
the original atlas. The retained set has not been normalized or repartitioned. -/
theorem canonical_original_switch (hclosed : IsClosed (range I))
(S : Diffeomorph I I M M ∞) (a : ι → M) (K : ι → Set M)
(hK : ∀ i,IsCompact (K i)) (hKU : ∀ i,K i⊆(chartAt H (a i)).source) :
∃ r₀ C₀ : ℝ,0<r₀ ∧ 1≤C₀ ∧
∀ (C J : Type*) [Fintype C] [MeasurableSpace C] [MeasurableSingletonClass C]
[Fintype J] [MeasurableSpace J] [MeasurableSingletonClass J]
(c : M → ι) (P : M → C) (L : M → J) (G R : Set M)
(n : ℕ) (B R₀ ε g α r δ : ℝ) (γ : C → ℝ)
(A : ∀ x:G,BilateralGauge I S a c n B R₀ x)
(T : G → Finset (Fin d)) (ref : G → G)
(Wf Wb : C×C → Submodule ℝ (EuclideanSpace ℝ (Fin d))),
Measurable c → Measurable P → Measurable L → MeasurableSet R → R⊆G →
(∀ v,v∈K (c v)) →
(∀ x y,L x=L y → P x=P y) →
(∀ x y,P x=P y → c x=c y) →
(∀ x∈R,I.IsInteriorPoint x) →
(∀ x:G,P (ref x)=P x) →
(∀ x y:G,P x=P y → (T x).card=(T y).card) →
(∀ x y:G,P x=P y → ref x=ref y) →
(∀ x:G,
‖((A (ref x)).forwardSpace I S a c 0 (T (ref x))ᶜ).starProjection-
((A x).forwardSpace I S a c 0 (T x)ᶜ).starProjection‖≤ε ∧
‖((A (ref x)).forwardSpace I S a c 0 (T (ref x))).starProjection-
((A x).forwardSpace I S a c 0 (T x)).starProjection‖≤ε) →
(∀ x:G,
Module.finrank ℝ ((A x).forwardSpace I S a c n (T x))=
Module.finrank ℝ (Wf (P x,P (S^[n] x))) ∧
Module.finrank ℝ ((A x).backwardSpace I S a c n (T x)ᶜ)=
Module.finrank ℝ (Wb (P x,P (S.symm^[n] x))) ∧
‖((A x).forwardSpace I S a c n (T x)).starProjection-
(Wf (P x,P (S^[n] x))).starProjection‖≤1/2 ∧
‖((A x).backwardSpace I S a c n (T x)ᶜ).starProjection-
(Wb (P x,P (S.symm^[n] x))).starProjection‖≤1/2) →
0≤ε → ε≤1/2 → Real.exp (2*B)*(2*ε)≤1/2 →
(∀ x:G,∀ j∈(T x)ᶜ,(A x).lam j≤γ (P x)-g) →
(∀ x:G,∀ j∈T x,γ (P x)+g≤(A x).lam j) →
(2*Real.exp (2*B))*(2*(2*Real.exp (2*B)^2*Real.exp (-2*g*n)))≤1/2 →
(∀ x:G,|γ (P x)|+|g|≤α) → 0≤r → 0<δ → δ≤r₀ →
(∀ x∈R,∀ t : Fin (n+1),
closedBall ((extChartAt I (a (c (S^[t.val] x)))) (S^[t.val] x)) δ⊆interior (range I) ∧
closedBall ((extChartAt I (a (c (S.symm^[t.val] x)))) (S.symm^[t.val] x)) δ⊆interior (range I)) →
(∀ x∈R,∀ y∈R,L x=L y →
‖(extChartAt I (a (c y))) y-(extChartAt I (a (c x))) x‖≤C₀*r) →
bvpInverseBound B α n*C₀*δ≤1/4 → bvpInverseBound B α n*C₀*r≤δ/4 →
∃ Φ : M×M → M×M,Measurable Φ ∧
(∀ x y:G,x.val∈R → y.val∈R → L x=L y →
let z := (Φ (x.val,y.val)).1
let w := (Φ (x.val,y.val)).2
originalTube I S a c (n:=n) (δ/2) x z ∧
originalTube I S.symm a c (n:=n) (δ/2) y z ∧
originalTube I S a c (n:=n) (δ/2) y w ∧
originalTube I S.symm a c (n:=n) (δ/2) x w ∧
originalEndpoint I S a c (n:=n) (Wf (P x,P (S^[n] x))) x z ∧
originalEndpoint I S.symm a c (n:=n) (Wb (P y,P (S.symm^[n] y))) y z ∧
originalEndpoint I S a c (n:=n) (Wf (P y,P (S^[n] y))) y w ∧
originalEndpoint I S.symm a c (n:=n) (Wb (P x,P (S.symm^[n] x))) x w ∧
originalTube I S a c (n:=n) (2*C₀*bvpInverseBound B α n*r) x z ∧
originalTube I S.symm a c (n:=n) (2*C₀*bvpInverseBound B α n*r) y z ∧
originalTube I S a c (n:=n) (2*C₀*bvpInverseBound B α n*r) y w ∧
originalTube I S.symm a c (n:=n) (2*C₀*bvpInverseBound B α n*r) x w ∧
‖(extChartAt I (a (c x))) z-(extChartAt I (a (c x))) x-
(((A (ref x)).forward I S a c).splitting (T (ref x))ᶜ).slow 0
((extChartAt I (a (c y))) y-(extChartAt I (a (c x))) x)‖≤
4*Real.exp (2*B)*(2*Real.exp (2*B))*(ε+2*Real.exp (2*B)^2*Real.exp (-2*g*n))*(C₀*r)+
bvpInverseBound B α n*C₀*(2*C₀*bvpInverseBound B α n*r)^2) ∧
∀ x∈R,∀ z,
originalTube I S a c (n:=n) δ x z → originalTube I S.symm a c (n:=n) δ x z →
originalEndpoint I S a c (n:=n) (Wf (P x,P (S^[n] x))) x z →
originalEndpoint I S.symm a c (n:=n) (Wb (P x,P (S.symm^[n] x))) x z → z=x := by
obtain ⟨r₀,C₀,hr₀,hC₀,hjoin⟩ := original_gauged_join I hclosed S a K hK hKU
refine ⟨r₀,C₀,hr₀,hC₀,?_⟩
intro C J _ _ _ _ _ _ c P L G R n B R₀ ε g α r δ γ A T ref Wf Wb
hc hP hL hR hRG hcover hLP hPc hint href hcard hrefeq hstart hend hε hεhalf
hsmall hslow hfast hgap hα hr hδ hδr hsafe hnear hcontract hdata
let F := originalObservation I S a c n P Wf
let V := originalObservation I S.symm a c n P Wb
let TF := originalTube I S a c (n:=n) δ
let TB := originalTube I S.symm a c (n:=n) δ
let Gpair : Set (M×M) := {u | u.1∈R ∧ u.2∈R ∧ L u.1=L u.2}
have hGpair : MeasurableSet Gpair :=
(hR.preimage measurable_fst).inter ((hR.preimage measurable_snd).inter
(measurableSet_eq_fun (hL.comp measurable_fst) (hL.comp measurable_snd)))
have hsrc (x : M) : x∈(chartAt H (a (c x))).source := hKU _ (hcover x)
have hspec (x y : G) (hx : x.val∈R) (hy : y.val∈R) (hxy : L x=L y) := by
have hp := hLP x y hxy
have hcst :
‖((A (ref x)).forwardSpace I S a c 0 (T (ref x))).starProjection-
((A y).forwardSpace I S a c 0 (T y)).starProjection‖≤ε := by
rw [hrefeq x y hp]
exact (hstart y).2
exact hjoin c n B R₀ ε (γ (P x)) g α r δ (ref x) x y
(A (ref x)) (A x) (A y) (T (ref x)) (T x) (T y)
(Wf (P x,P (S^[n] x))) (Wb (P y,P (S.symm^[n] y))) hcover (hPc x y hp)
(hint x hx) (hint y hy) (hend x).1 (hend y).2.1 (hend x).2.2.1 (hend y).2.2.2
hε hεhalf (hcard _ _ (href x)) (hcard _ _ ((href x).trans hp)) (hstart x).1 hcst hsmall
(hslow x) (hfast x) (by simpa only [hp] using hslow y) (by simpa only [hp] using hfast y)
hgap (hα x) hr hδ hδr (fun t => (hsafe x hx t).1) (fun t => (hsafe y hy t).2)
(hnear x hx y hy hxy) hcontract hdata
have hrel (x y : M) (z : M) :
MeasurableSwitch.relation F V TF TB (x,y) z ↔
originalEndpoint I S a c (n:=n) (Wf (P x,P (S^[n] x))) x z ∧
originalEndpoint I S.symm a c (n:=n) (Wb (P y,P (S.symm^[n] y))) y z ∧
TF x z ∧ TB y z := by
constructor
· rintro ⟨hf,hb,htf,htb⟩
exact ⟨(originalObservation_eq_iff I S a c n P Wf x z (hsrc _) (htf ⟨n,by omega⟩).1).mp hf,
(originalObservation_eq_iff I S.symm a c n P Wb y z (hsrc _) (htb ⟨n,by omega⟩).1).mp hb,htf,htb⟩
· rintro ⟨hf,hb,htf,htb⟩
exact ⟨(originalObservation_eq_iff I S a c n P Wf x z (hsrc _) (htf ⟨n,by omega⟩).1).mpr hf,
(originalObservation_eq_iff I S.symm a c n P Wb y z (hsrc _) (htb ⟨n,by omega⟩).1).mpr hb,htf,htb⟩
have hex (u : M×M) (hu : u∈Gpair) : ∃! z,MeasurableSwitch.relation F V TF TB u z := by
let x : G := ⟨u.1,hRG hu.1⟩
let y : G := ⟨u.2,hRG hu.2.1⟩
obtain ⟨z,hzf,hzb,hze,hze',hsharp,hsharp',hideal,hunique⟩ := hspec x y hu.1 hu.2.1 hu.2.2
refine ⟨z,(hrel _ _ _).mpr ⟨hze,hze',?_,?_⟩,?_⟩
· exact originalTube_mono I S a c n (by linarith) hzf
· exact originalTube_mono I S.symm a c n (by linarith) hzb
· intro z' hz'
obtain ⟨hf,hb,htf,htb⟩ := (hrel _ _ _).mp hz'
exact hunique z' htf htb hf hb
have hswap (u : M×M) (hu : u∈Gpair) : u.swap∈Gpair := ⟨hu.2.1,hu.1,hu.2.2.symm⟩
obtain ⟨Φ,hΦ,hΦr,hΦu,hΦu'⟩ := MeasurableSwitch.canonical_pair Gpair hGpair F V
(measurable_originalObservation I S a c n hc P hP Wf)
(measurable_originalObservation I S.symm a c n hc P hP Wb) TF TB
(measurable_originalTube I S a c n hc hsrc δ)
(measurable_originalTube I S.symm a c n hc hsrc δ) hex (fun u hu => hex u.swap (hswap u hu))
refine ⟨Φ,hΦ,?_,?_⟩
· intro x y hx hy hxy
obtain ⟨z,hzf,hzb,hze,hze',hsf,hsb,hideal,hunique⟩ := hspec x y hx hy hxy
obtain ⟨w,hwf,hwb,hwe,hwe',htf,htb,_,_⟩ := hspec y x hy hx hxy.symm
have hz : z=(Φ (x.val,y.val)).1 := hΦu _ ⟨hx,hy,hxy⟩ _ ((hrel _ _ _).mpr
⟨hze,hze',originalTube_mono I S a c n (by linarith) hzf,
originalTube_mono I S.symm a c n (by linarith) hzb⟩)
have hw : w=(Φ (x.val,y.val)).2 := hΦu' _ ⟨hx,hy,hxy⟩ _ ((hrel _ _ _).mpr
⟨hwe,hwe',originalTube_mono I S a c n (by linarith) hwf,
originalTube_mono I S.symm a c n (by linarith) hwb⟩)
dsimp only
rw [←hz,←hw]
exact ⟨hzf,hzb,hwf,hwb,hze,hze',hwe,hwe',hsf,hsb,htf,htb,hideal⟩
· intro x hx z htf htb hef heb
obtain ⟨w,_,_,_,_,_,_,_,hunique⟩ := hspec (⟨x,hRG hx⟩ : G) ⟨x,hRG hx⟩ hx hx rfl
have hselfF : originalTube I S a c (n:=n) δ x x := by
intro t
exact ⟨hsrc _,by simpa only [sub_self,norm_zero] using hδ.le⟩
have hselfB : originalTube I S.symm a c (n:=n) δ x x := by
intro t
exact ⟨hsrc _,by simpa only [sub_self,norm_zero] using hδ.le⟩
exact (hunique z htf htb hef heb).trans (hunique x hselfF hselfB rfl rfl).symm
end SmoothObstruction.ManifoldCoordinates
namespace SmoothObstruction.ManifoldCoordinates
open Set Metric MeasureTheory
open scoped Manifold ContDiff Matrix.Norms.L2Operator
variable {d : ℕ} {H : Type*} [TopologicalSpace H]
(I : ModelWithCorners ℝ (EuclideanSpace ℝ (Fin d)) H)
{M : Type*} [MetricSpace M] [ChartedSpace H M] [IsManifold I ∞ M]
[MeasurableSpace M] [BorelSpace M] [StandardBorelSpace M] [Nonempty M]
{ι : Type*} [Fintype ι] [MeasurableSpace ι] [MeasurableSingletonClass ι]
open FiniteGreen ShortBin
/-- A measurable, witness-independent ORIGINAL pair switch. Its Borel relation
uses zero-extended charts, but all asserted equations and tube estimates are in
the original atlas. The retained set has not been normalized or repartitioned. -/
theorem canonical_original_switch_unique (hclosed : IsClosed (range I))
(S : Diffeomorph I I M M ∞) (a : ι → M) (K : ι → Set M)
(hK : ∀ i,IsCompact (K i)) (hKU : ∀ i,K i⊆(chartAt H (a i)).source) :
∃ r₀ C₀ : ℝ,0<r₀ ∧ 1≤C₀ ∧
∀ (C J : Type*) [Fintype C] [MeasurableSpace C] [MeasurableSingletonClass C]
[Fintype J] [MeasurableSpace J] [MeasurableSingletonClass J]
(c : M → ι) (P : M → C) (L : M → J) (G R : Set M)
(n : ℕ) (B R₀ ε g α r δ : ℝ) (γ : C → ℝ)
(A : ∀ x:G,BilateralGauge I S a c n B R₀ x)
(T : G → Finset (Fin d)) (ref : G → G)
(Wf Wb : C×C → Submodule ℝ (EuclideanSpace ℝ (Fin d))),
Measurable c → Measurable P → Measurable L → MeasurableSet R → R⊆G →
(∀ v,v∈K (c v)) →
(∀ x y,L x=L y → P x=P y) →
(∀ x y,P x=P y → c x=c y) →
(∀ x∈R,I.IsInteriorPoint x) →
(∀ x:G,P (ref x)=P x) →
(∀ x y:G,P x=P y → (T x).card=(T y).card) →
(∀ x y:G,P x=P y → ref x=ref y) →
(∀ x:G,
‖((A (ref x)).forwardSpace I S a c 0 (T (ref x))ᶜ).starProjection-
((A x).forwardSpace I S a c 0 (T x)ᶜ).starProjection‖≤ε ∧
‖((A (ref x)).forwardSpace I S a c 0 (T (ref x))).starProjection-
((A x).forwardSpace I S a c 0 (T x)).starProjection‖≤ε) →
(∀ x:G,
Module.finrank ℝ ((A x).forwardSpace I S a c n (T x))=
Module.finrank ℝ (Wf (P x,P (S^[n] x))) ∧
Module.finrank ℝ ((A x).backwardSpace I S a c n (T x)ᶜ)=
Module.finrank ℝ (Wb (P x,P (S.symm^[n] x))) ∧
‖((A x).forwardSpace I S a c n (T x)).starProjection-
(Wf (P x,P (S^[n] x))).starProjection‖≤1/2 ∧
‖((A x).backwardSpace I S a c n (T x)ᶜ).starProjection-
(Wb (P x,P (S.symm^[n] x))).starProjection‖≤1/2) →
0≤ε → ε≤1/2 → Real.exp (2*B)*(2*ε)≤1/2 →
(∀ x:G,∀ j∈(T x)ᶜ,(A x).lam j≤γ (P x)-g) →
(∀ x:G,∀ j∈T x,γ (P x)+g≤(A x).lam j) →
(2*Real.exp (2*B))*(2*(2*Real.exp (2*B)^2*Real.exp (-2*g*n)))≤1/2 →
(∀ x:G,|γ (P x)|+|g|≤α) → 0≤r → 0<δ → δ≤r₀ →
(∀ x∈R,∀ t : Fin (n+1),
closedBall ((extChartAt I (a (c (S^[t.val] x)))) (S^[t.val] x)) δ⊆interior (range I) ∧
closedBall ((extChartAt I (a (c (S.symm^[t.val] x)))) (S.symm^[t.val] x)) δ⊆interior (range I)) →
(∀ x∈R,∀ y∈R,L x=L y →
‖(extChartAt I (a (c y))) y-(extChartAt I (a (c x))) x‖≤C₀*r) →
bvpInverseBound B α n*C₀*δ≤1/4 → bvpInverseBound B α n*C₀*r≤δ/4 →
∃ Φ : M×M → M×M,Measurable Φ ∧
(∀ x y:G,x.val∈R → y.val∈R → L x=L y →
let z := (Φ (x.val,y.val)).1
let w := (Φ (x.val,y.val)).2
originalTube I S a c (n:=n) (δ/2) x z ∧
originalTube I S.symm a c (n:=n) (δ/2) y z ∧
originalTube I S a c (n:=n) (δ/2) y w ∧
originalTube I S.symm a c (n:=n) (δ/2) x w ∧
originalEndpoint I S a c (n:=n) (Wf (P x,P (S^[n] x))) x z ∧
originalEndpoint I S.symm a c (n:=n) (Wb (P y,P (S.symm^[n] y))) y z ∧
originalEndpoint I S a c (n:=n) (Wf (P y,P (S^[n] y))) y w ∧
originalEndpoint I S.symm a c (n:=n) (Wb (P x,P (S.symm^[n] x))) x w ∧
originalTube I S a c (n:=n) (2*C₀*bvpInverseBound B α n*r) x z ∧
originalTube I S.symm a c (n:=n) (2*C₀*bvpInverseBound B α n*r) y z ∧
originalTube I S a c (n:=n) (2*C₀*bvpInverseBound B α n*r) y w ∧
originalTube I S.symm a c (n:=n) (2*C₀*bvpInverseBound B α n*r) x w ∧
‖(extChartAt I (a (c x))) z-(extChartAt I (a (c x))) x-
(((A (ref x)).forward I S a c).splitting (T (ref x))ᶜ).slow 0
((extChartAt I (a (c y))) y-(extChartAt I (a (c x))) x)‖≤
4*Real.exp (2*B)*(2*Real.exp (2*B))*(ε+2*Real.exp (2*B)^2*Real.exp (-2*g*n))*(C₀*r)+
bvpInverseBound B α n*C₀*(2*C₀*bvpInverseBound B α n*r)^2) ∧
(∀ x∈R,∀ z,
originalTube I S a c (n:=n) δ x z → originalTube I S.symm a c (n:=n) δ x z →
originalEndpoint I S a c (n:=n) (Wf (P x,P (S^[n] x))) x z →
originalEndpoint I S.symm a c (n:=n) (Wb (P x,P (S.symm^[n] x))) x z → z=x) ∧
∀ x∈R,∀ y∈R,L x=L y → ∀ z,
originalTube I S a c (n:=n) δ x z → originalTube I S.symm a c (n:=n) δ y z →
originalEndpoint I S a c (n:=n) (Wf (P x,P (S^[n] x))) x z →
originalEndpoint I S.symm a c (n:=n) (Wb (P y,P (S.symm^[n] y))) y z →
z=(Φ (x,y)).1 := by
obtain ⟨r₀,C₀,hr₀,hC₀,hjoin⟩ := original_gauged_join I hclosed S a K hK hKU
refine ⟨r₀,C₀,hr₀,hC₀,?_⟩
intro C J _ _ _ _ _ _ c P L G R n B R₀ ε g α r δ γ A T ref Wf Wb
hc hP hL hR hRG hcover hLP hPc hint href hcard hrefeq hstart hend hε hεhalf
hsmall hslow hfast hgap hα hr hδ hδr hsafe hnear hcontract hdata
let F := originalObservation I S a c n P Wf
let V := originalObservation I S.symm a c n P Wb
let TF := originalTube I S a c (n:=n) δ
let TB := originalTube I S.symm a c (n:=n) δ
let Gpair : Set (M×M) := {u | u.1∈R ∧ u.2∈R ∧ L u.1=L u.2}
have hGpair : MeasurableSet Gpair :=
(hR.preimage measurable_fst).inter ((hR.preimage measurable_snd).inter
(measurableSet_eq_fun (hL.comp measurable_fst) (hL.comp measurable_snd)))
have hsrc (x : M) : x∈(chartAt H (a (c x))).source := hKU _ (hcover x)
have hspec (x y : G) (hx : x.val∈R) (hy : y.val∈R) (hxy : L x=L y) := by
have hp := hLP x y hxy
have hcst :
‖((A (ref x)).forwardSpace I S a c 0 (T (ref x))).starProjection-
((A y).forwardSpace I S a c 0 (T y)).starProjection‖≤ε := by
rw [hrefeq x y hp]
exact (hstart y).2
exact hjoin c n B R₀ ε (γ (P x)) g α r δ (ref x) x y
(A (ref x)) (A x) (A y) (T (ref x)) (T x) (T y)
(Wf (P x,P (S^[n] x))) (Wb (P y,P (S.symm^[n] y))) hcover (hPc x y hp)
(hint x hx) (hint y hy) (hend x).1 (hend y).2.1 (hend x).2.2.1 (hend y).2.2.2
hε hεhalf (hcard _ _ (href x)) (hcard _ _ ((href x).trans hp)) (hstart x).1 hcst hsmall
(hslow x) (hfast x) (by simpa only [hp] using hslow y) (by simpa only [hp] using hfast y)
hgap (hα x) hr hδ hδr (fun t => (hsafe x hx t).1) (fun t => (hsafe y hy t).2)
(hnear x hx y hy hxy) hcontract hdata
have hrel (x y : M) (z : M) :
MeasurableSwitch.relation F V TF TB (x,y) z ↔
originalEndpoint I S a c (n:=n) (Wf (P x,P (S^[n] x))) x z ∧
originalEndpoint I S.symm a c (n:=n) (Wb (P y,P (S.symm^[n] y))) y z ∧
TF x z ∧ TB y z := by
constructor
· rintro ⟨hf,hb,htf,htb⟩
exact ⟨(originalObservation_eq_iff I S a c n P Wf x z (hsrc _) (htf ⟨n,by omega⟩).1).mp hf,
(originalObservation_eq_iff I S.symm a c n P Wb y z (hsrc _) (htb ⟨n,by omega⟩).1).mp hb,htf,htb⟩
· rintro ⟨hf,hb,htf,htb⟩
exact ⟨(originalObservation_eq_iff I S a c n P Wf x z (hsrc _) (htf ⟨n,by omega⟩).1).mpr hf,
(originalObservation_eq_iff I S.symm a c n P Wb y z (hsrc _) (htb ⟨n,by omega⟩).1).mpr hb,htf,htb⟩
have hex (u : M×M) (hu : u∈Gpair) : ∃! z,MeasurableSwitch.relation F V TF TB u z := by
let x : G := ⟨u.1,hRG hu.1⟩
let y : G := ⟨u.2,hRG hu.2.1⟩
obtain ⟨z,hzf,hzb,hze,hze',hsharp,hsharp',hideal,hunique⟩ := hspec x y hu.1 hu.2.1 hu.2.2
refine ⟨z,(hrel _ _ _).mpr ⟨hze,hze',?_,?_⟩,?_⟩
· exact originalTube_mono I S a c n (by linarith) hzf
· exact originalTube_mono I S.symm a c n (by linarith) hzb
· intro z' hz'
obtain ⟨hf,hb,htf,htb⟩ := (hrel _ _ _).mp hz'
exact hunique z' htf htb hf hb
have hswap (u : M×M) (hu : u∈Gpair) : u.swap∈Gpair := ⟨hu.2.1,hu.1,hu.2.2.symm⟩
obtain ⟨Φ,hΦ,hΦr,hΦu,hΦu'⟩ := MeasurableSwitch.canonical_pair Gpair hGpair F V
(measurable_originalObservation I S a c n hc P hP Wf)
(measurable_originalObservation I S.symm a c n hc P hP Wb) TF TB
(measurable_originalTube I S a c n hc hsrc δ)
(measurable_originalTube I S.symm a c n hc hsrc δ) hex (fun u hu => hex u.swap (hswap u hu))
refine ⟨Φ,hΦ,?_,?_,?_⟩
· intro x y hx hy hxy
obtain ⟨z,hzf,hzb,hze,hze',hsf,hsb,hideal,hunique⟩ := hspec x y hx hy hxy
obtain ⟨w,hwf,hwb,hwe,hwe',htf,htb,_,_⟩ := hspec y x hy hx hxy.symm
have hz : z=(Φ (x.val,y.val)).1 := hΦu _ ⟨hx,hy,hxy⟩ _ ((hrel _ _ _).mpr
⟨hze,hze',originalTube_mono I S a c n (by linarith) hzf,
originalTube_mono I S.symm a c n (by linarith) hzb⟩)
have hw : w=(Φ (x.val,y.val)).2 := hΦu' _ ⟨hx,hy,hxy⟩ _ ((hrel _ _ _).mpr
⟨hwe,hwe',originalTube_mono I S a c n (by linarith) hwf,
originalTube_mono I S.symm a c n (by linarith) hwb⟩)
dsimp only
rw [←hz,←hw]
exact ⟨hzf,hzb,hwf,hwb,hze,hze',hwe,hwe',hsf,hsb,htf,htb,hideal⟩
· intro x hx z htf htb hef heb
obtain ⟨w,_,_,_,_,_,_,_,hunique⟩ := hspec (⟨x,hRG hx⟩ : G) ⟨x,hRG hx⟩ hx hx rfl
have hselfF : originalTube I S a c (n:=n) δ x x := by
intro t
exact ⟨hsrc _,by simpa only [sub_self,norm_zero] using hδ.le⟩
have hselfB : originalTube I S.symm a c (n:=n) δ x x := by
intro t
exact ⟨hsrc _,by simpa only [sub_self,norm_zero] using hδ.le⟩
exact (hunique z htf htb hef heb).trans (hunique x hselfF hselfB rfl rfl).symm
· intro x hx y hy hxy z htf htb hef heb
exact hΦu _ ⟨hx,hy,hxy⟩ z ((hrel x y z).mpr ⟨hef,heb,htf,htb⟩)
end SmoothObstruction.ManifoldCoordinates
namespace SmoothObstruction.ManifoldCoordinates
open Set Metric MeasureTheory
open scoped Manifold ContDiff Matrix.Norms.L2Operator
variable {d : ℕ} {H : Type*} [TopologicalSpace H]
(I : ModelWithCorners ℝ (EuclideanSpace ℝ (Fin d)) H)
{M : Type*} [MetricSpace M] [ChartedSpace H M] [IsManifold I ∞ M]
[MeasurableSpace M] [BorelSpace M] [StandardBorelSpace M] [Nonempty M]
{ι : Type*} [Fintype ι] [MeasurableSpace ι] [MeasurableSingletonClass ι]
open FiniteGreen ShortBin
/-- A measurable, witness-independent ORIGINAL pair switch. Its Borel relation
uses zero-extended charts, but all asserted equations and tube estimates are in
the original atlas. The retained set has not been normalized or repartitioned. -/
theorem canonical_original_switch_complete (hclosed : IsClosed (range I))
(S : Diffeomorph I I M M ∞) (a : ι → M) (K : ι → Set M)
(hK : ∀ i,IsCompact (K i)) (hKU : ∀ i,K i⊆(chartAt H (a i)).source) :
∃ r₀ C₀ : ℝ,0<r₀ ∧ 1≤C₀ ∧
∀ (C J : Type*) [Fintype C] [MeasurableSpace C] [MeasurableSingletonClass C]
[Fintype J] [MeasurableSpace J] [MeasurableSingletonClass J]
(c : M → ι) (P : M → C) (L : M → J) (G R : Set M)
(n : ℕ) (B R₀ ε g α r δ : ℝ) (γ : C → ℝ)
(A : ∀ x:G,BilateralGauge I S a c n B R₀ x)
(T : G → Finset (Fin d)) (ref : G → G)
(Wf Wb : C×C → Submodule ℝ (EuclideanSpace ℝ (Fin d))),
Measurable c → Measurable P → Measurable L → MeasurableSet R → R⊆G →
(∀ v,v∈K (c v)) →
(∀ x y,L x=L y → P x=P y) →
(∀ x y,P x=P y → c x=c y) →
(∀ x∈R,I.IsInteriorPoint x) →
(∀ x:G,P (ref x)=P x) →
(∀ x y:G,P x=P y → (T x).card=(T y).card) →
(∀ x y:G,P x=P y → ref x=ref y) →
(∀ x:G,
‖((A (ref x)).forwardSpace I S a c 0 (T (ref x))ᶜ).starProjection-
((A x).forwardSpace I S a c 0 (T x)ᶜ).starProjection‖≤ε ∧
‖((A (ref x)).forwardSpace I S a c 0 (T (ref x))).starProjection-
((A x).forwardSpace I S a c 0 (T x)).starProjection‖≤ε) →
(∀ x:G,
Module.finrank ℝ ((A x).forwardSpace I S a c n (T x))=
Module.finrank ℝ (Wf (P x,P (S^[n] x))) ∧
Module.finrank ℝ ((A x).backwardSpace I S a c n (T x)ᶜ)=
Module.finrank ℝ (Wb (P x,P (S.symm^[n] x))) ∧
‖((A x).forwardSpace I S a c n (T x)).starProjection-
(Wf (P x,P (S^[n] x))).starProjection‖≤1/2 ∧
‖((A x).backwardSpace I S a c n (T x)ᶜ).starProjection-
(Wb (P x,P (S.symm^[n] x))).starProjection‖≤1/2) →
0≤ε → ε≤1/2 → Real.exp (2*B)*(2*ε)≤1/2 →
(∀ x:G,∀ j∈(T x)ᶜ,(A x).lam j≤γ (P x)-g) →
(∀ x:G,∀ j∈T x,γ (P x)+g≤(A x).lam j) →
(2*Real.exp (2*B))*(2*(2*Real.exp (2*B)^2*Real.exp (-2*g*n)))≤1/2 →
(∀ x:G,|γ (P x)|+|g|≤α) → 0≤r → 0<δ → δ≤r₀ →
(∀ x∈R,∀ t : Fin (n+1),
closedBall ((extChartAt I (a (c (S^[t.val] x)))) (S^[t.val] x)) δ⊆interior (range I) ∧
closedBall ((extChartAt I (a (c (S.symm^[t.val] x)))) (S.symm^[t.val] x)) δ⊆interior (range I)) →
(∀ x∈R,∀ y∈R,L x=L y →
‖(extChartAt I (a (c y))) y-(extChartAt I (a (c x))) x‖≤C₀*r) →
bvpInverseBound B α n*C₀*δ≤1/4 → bvpInverseBound B α n*C₀*r≤δ/4 →
∃ Φ : M×M → M×M,Measurable Φ ∧
(∀ x y:G,x.val∈R → y.val∈R → L x=L y →
let z := (Φ (x.val,y.val)).1
let w := (Φ (x.val,y.val)).2
originalTube I S a c (n:=n) (δ/2) x z ∧
originalTube I S.symm a c (n:=n) (δ/2) y z ∧
originalTube I S a c (n:=n) (δ/2) y w ∧
originalTube I S.symm a c (n:=n) (δ/2) x w ∧
originalEndpoint I S a c (n:=n) (Wf (P x,P (S^[n] x))) x z ∧
originalEndpoint I S.symm a c (n:=n) (Wb (P y,P (S.symm^[n] y))) y z ∧
originalEndpoint I S a c (n:=n) (Wf (P y,P (S^[n] y))) y w ∧
originalEndpoint I S.symm a c (n:=n) (Wb (P x,P (S.symm^[n] x))) x w ∧
originalTube I S a c (n:=n) (2*C₀*bvpInverseBound B α n*r) x z ∧
originalTube I S.symm a c (n:=n) (2*C₀*bvpInverseBound B α n*r) y z ∧
originalTube I S a c (n:=n) (2*C₀*bvpInverseBound B α n*r) y w ∧
originalTube I S.symm a c (n:=n) (2*C₀*bvpInverseBound B α n*r) x w ∧
‖(extChartAt I (a (c x))) z-(extChartAt I (a (c x))) x-
(((A (ref x)).forward I S a c).splitting (T (ref x))ᶜ).slow 0
((extChartAt I (a (c y))) y-(extChartAt I (a (c x))) x)‖≤
4*Real.exp (2*B)*(2*Real.exp (2*B))*(ε+2*Real.exp (2*B)^2*Real.exp (-2*g*n))*(C₀*r)+
bvpInverseBound B α n*C₀*(2*C₀*bvpInverseBound B α n*r)^2 ∧
‖(extChartAt I (a (c y))) w-(extChartAt I (a (c y))) y-
(((A (ref y)).forward I S a c).splitting (T (ref y))ᶜ).slow 0
((extChartAt I (a (c x))) x-(extChartAt I (a (c y))) y)‖≤
4*Real.exp (2*B)*(2*Real.exp (2*B))*(ε+2*Real.exp (2*B)^2*Real.exp (-2*g*n))*(C₀*r)+
bvpInverseBound B α n*C₀*(2*C₀*bvpInverseBound B α n*r)^2) ∧
(∀ x∈R,∀ z,
originalTube I S a c (n:=n) δ x z → originalTube I S.symm a c (n:=n) δ x z →
originalEndpoint I S a c (n:=n) (Wf (P x,P (S^[n] x))) x z →
originalEndpoint I S.symm a c (n:=n) (Wb (P x,P (S.symm^[n] x))) x z → z=x) ∧
∀ x∈R,∀ y∈R,L x=L y → ∀ z,
originalTube I S a c (n:=n) δ x z → originalTube I S.symm a c (n:=n) δ y z →
originalEndpoint I S a c (n:=n) (Wf (P x,P (S^[n] x))) x z →
originalEndpoint I S.symm a c (n:=n) (Wb (P y,P (S.symm^[n] y))) y z →
z=(Φ (x,y)).1 := by
obtain ⟨r₀,C₀,hr₀,hC₀,hjoin⟩ := original_gauged_join I hclosed S a K hK hKU
refine ⟨r₀,C₀,hr₀,hC₀,?_⟩
intro C J _ _ _ _ _ _ c P L G R n B R₀ ε g α r δ γ A T ref Wf Wb
hc hP hL hR hRG hcover hLP hPc hint href hcard hrefeq hstart hend hε hεhalf
hsmall hslow hfast hgap hα hr hδ hδr hsafe hnear hcontract hdata
let F := originalObservation I S a c n P Wf
let V := originalObservation I S.symm a c n P Wb
let TF := originalTube I S a c (n:=n) δ
let TB := originalTube I S.symm a c (n:=n) δ
let Gpair : Set (M×M) := {u | u.1∈R ∧ u.2∈R ∧ L u.1=L u.2}
have hGpair : MeasurableSet Gpair :=
(hR.preimage measurable_fst).inter ((hR.preimage measurable_snd).inter
(measurableSet_eq_fun (hL.comp measurable_fst) (hL.comp measurable_snd)))
have hsrc (x : M) : x∈(chartAt H (a (c x))).source := hKU _ (hcover x)
have hspec (x y : G) (hx : x.val∈R) (hy : y.val∈R) (hxy : L x=L y) := by
have hp := hLP x y hxy
have hcst :
‖((A (ref x)).forwardSpace I S a c 0 (T (ref x))).starProjection-
((A y).forwardSpace I S a c 0 (T y)).starProjection‖≤ε := by
rw [hrefeq x y hp]
exact (hstart y).2
exact hjoin c n B R₀ ε (γ (P x)) g α r δ (ref x) x y
(A (ref x)) (A x) (A y) (T (ref x)) (T x) (T y)
(Wf (P x,P (S^[n] x))) (Wb (P y,P (S.symm^[n] y))) hcover (hPc x y hp)
(hint x hx) (hint y hy) (hend x).1 (hend y).2.1 (hend x).2.2.1 (hend y).2.2.2
hε hεhalf (hcard _ _ (href x)) (hcard _ _ ((href x).trans hp)) (hstart x).1 hcst hsmall
(hslow x) (hfast x) (by simpa only [hp] using hslow y) (by simpa only [hp] using hfast y)
hgap (hα x) hr hδ hδr (fun t => (hsafe x hx t).1) (fun t => (hsafe y hy t).2)
(hnear x hx y hy hxy) hcontract hdata
have hrel (x y : M) (z : M) :
MeasurableSwitch.relation F V TF TB (x,y) z ↔
originalEndpoint I S a c (n:=n) (Wf (P x,P (S^[n] x))) x z ∧
originalEndpoint I S.symm a c (n:=n) (Wb (P y,P (S.symm^[n] y))) y z ∧
TF x z ∧ TB y z := by
constructor
· rintro ⟨hf,hb,htf,htb⟩
exact ⟨(originalObservation_eq_iff I S a c n P Wf x z (hsrc _) (htf ⟨n,by omega⟩).1).mp hf,
(originalObservation_eq_iff I S.symm a c n P Wb y z (hsrc _) (htb ⟨n,by omega⟩).1).mp hb,htf,htb⟩
· rintro ⟨hf,hb,htf,htb⟩
exact ⟨(originalObservation_eq_iff I S a c n P Wf x z (hsrc _) (htf ⟨n,by omega⟩).1).mpr hf,
(originalObservation_eq_iff I S.symm a c n P Wb y z (hsrc _) (htb ⟨n,by omega⟩).1).mpr hb,htf,htb⟩
have hex (u : M×M) (hu : u∈Gpair) : ∃! z,MeasurableSwitch.relation F V TF TB u z := by
let x : G := ⟨u.1,hRG hu.1⟩
let y : G := ⟨u.2,hRG hu.2.1⟩
obtain ⟨z,hzf,hzb,hze,hze',hsharp,hsharp',hideal,hunique⟩ := hspec x y hu.1 hu.2.1 hu.2.2
refine ⟨z,(hrel _ _ _).mpr ⟨hze,hze',?_,?_⟩,?_⟩
· exact originalTube_mono I S a c n (by linarith) hzf
· exact originalTube_mono I S.symm a c n (by linarith) hzb
· intro z' hz'
obtain ⟨hf,hb,htf,htb⟩ := (hrel _ _ _).mp hz'
exact hunique z' htf htb hf hb
have hswap (u : M×M) (hu : u∈Gpair) : u.swap∈Gpair := ⟨hu.2.1,hu.1,hu.2.2.symm⟩
obtain ⟨Φ,hΦ,hΦr,hΦu,hΦu'⟩ := MeasurableSwitch.canonical_pair Gpair hGpair F V
(measurable_originalObservation I S a c n hc P hP Wf)
(measurable_originalObservation I S.symm a c n hc P hP Wb) TF TB
(measurable_originalTube I S a c n hc hsrc δ)
(measurable_originalTube I S.symm a c n hc hsrc δ) hex (fun u hu => hex u.swap (hswap u hu))
refine ⟨Φ,hΦ,?_,?_,?_⟩
· intro x y hx hy hxy
obtain ⟨z,hzf,hzb,hze,hze',hsf,hsb,hideal,hunique⟩ := hspec x y hx hy hxy
obtain ⟨w,hwf,hwb,hwe,hwe',htf,htb,hideal',_⟩ := hspec y x hy hx hxy.symm
have hz : z=(Φ (x.val,y.val)).1 := hΦu _ ⟨hx,hy,hxy⟩ _ ((hrel _ _ _).mpr
⟨hze,hze',originalTube_mono I S a c n (by linarith) hzf,
originalTube_mono I S.symm a c n (by linarith) hzb⟩)
have hw : w=(Φ (x.val,y.val)).2 := hΦu' _ ⟨hx,hy,hxy⟩ _ ((hrel _ _ _).mpr
⟨hwe,hwe',originalTube_mono I S a c n (by linarith) hwf,
originalTube_mono I S.symm a c n (by linarith) hwb⟩)
dsimp only
rw [←hz,←hw]
exact ⟨hzf,hzb,hwf,hwb,hze,hze',hwe,hwe',hsf,hsb,htf,htb,hideal,hideal'⟩
· intro x hx z htf htb hef heb
obtain ⟨w,_,_,_,_,_,_,_,hunique⟩ := hspec (⟨x,hRG hx⟩ : G) ⟨x,hRG hx⟩ hx hx rfl
have hselfF : originalTube I S a c (n:=n) δ x x := by
intro t
exact ⟨hsrc _,by simpa only [sub_self,norm_zero] using hδ.le⟩
have hselfB : originalTube I S.symm a c (n:=n) δ x x := by
intro t
exact ⟨hsrc _,by simpa only [sub_self,norm_zero] using hδ.le⟩
exact (hunique z htf htb hef heb).trans (hunique x hselfF hselfB rfl rfl).symm
· intro x hx y hy hxy z htf htb hef heb
exact hΦu _ ⟨hx,hy,hxy⟩ z ((hrel x y z).mpr ⟨hef,heb,htf,htb⟩)
end SmoothObstruction.ManifoldCoordinates
end
end OAI