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import OAI.MathematicalPhysics.Boltzmann.Approximation.CapHotSourceIntegrability
import OAI.MathematicalPhysics.Boltzmann.Approximation.CapDilationCompactness
import OAI.MathematicalPhysics.Boltzmann.Approximation.CapHotTransportBalance
import OAI.MathematicalPhysics.Boltzmann.Approximation.CapHotUndamped
import OAI.MathematicalPhysics.Boltzmann.Approximation.CapPairMoments
import OAI.MathematicalPhysics.Boltzmann.Approximation.PositiveNonlinearLimit
import OAI.MathematicalPhysics.Boltzmann.Branching.BoundedAverageProducts
import OAI.MathematicalPhysics.Boltzmann.Branching.EuclideanBackwardMap
import OAI.MathematicalPhysics.Boltzmann.Branching.HotChartHomeomorph
import OAI.MathematicalPhysics.Boltzmann.Branching.HotPositiveRegion
import OAI.MathematicalPhysics.Boltzmann.Branching.ProductKineticCutoff
import OAI.MathematicalPhysics.Boltzmann.Branching.VanishingCutoffCollision
import OAI.MathematicalPhysics.Boltzmann.Branching.VaryingBoundedMultiplier
import OAI.MathematicalPhysics.Boltzmann.Branching.WeightedJetStability
import OAI.MathematicalPhysics.Boltzmann.Collision.WeightLocalL1
import OAI.MathematicalPhysics.Boltzmann.Compactness.LocalMomentIntegrability
import OAI.MathematicalPhysics.Boltzmann.Compactness.PairPatchIdentity
import OAI.MathematicalPhysics.Boltzmann.Compactness.PairRepresentative
import OAI.MathematicalPhysics.Boltzmann.Compactness.StrongMassClip
import OAI.MathematicalPhysics.Boltzmann.Compactness.WeakConservedMarginal
import OAI.MathematicalPhysics.Boltzmann.Compactness.WeakL1Operations
import OAI.MathematicalPhysics.Boltzmann.Jets.ColdCentralVanishing
namespace OAI
section
/-! # Global L¹ convergence for every chosen compact interior hot average -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology ENNReal
open BoltzmannNonuniqueness.Published BoltzmannNonuniqueness.TransportCutoff
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
theorem HotLimitExtraction.global_strong_averages
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(S : AttainedCapSequence F) (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2)
(χ : ℕ → Published.KineticPhase → ℝ) (hχ : ∀ j, ContDiff ℝ (⊤ : ℕ∞) (χ j))
(hc : ∀ j, HasCompactSupport (χ j))
(hs : ∀ j, tsupport (χ j) ⊆ {z | 0 < z.1.1 ∧ ENNReal.ofReal z.1.1 < E.horizon})
(ψ : ℕ → Velocity → ℝ) (hψ : ∀ j, ContDiff ℝ (⊤ : ℕ∞) (ψ j))
(hψc : ∀ j, HasCompactSupport (ψ j)) :
∃ φ : ℕ → ℕ, StrictMono φ ∧ ∀ j,
Tendsto (fun n => eLpNorm (fun z =>
(∫ v, ψ j v*(χ j (z,v)*S.euclideanHot (E.indices (φ n)) (z,v)))-
(∫ v, ψ j v*(χ j (z,v)*E.hotLimit (EuclideanFlight.hotChart (z,v))))) 1 volume)
atTop (𝓝 0) := by
choose a A R ha haA hA hwin using fun j =>
exists_positive_cutoff_window E.horizon_ge (hc j) (hs j)
obtain ⟨φ,hφ,hconv⟩ := E.strong_averages hcarleman hGLPS S hs₀ hsmax hη hηmax hK hα
hαmax hγ hd₀ hd₀max hsmall hq₁ hq₂ a A R ha haA hA χ hχ hc hwin ψ hψ hψc
refine ⟨φ,hφ,fun j => ?_⟩
let D := Prod.fst '' tsupport (χ j)
have hD : IsCompact D := (hc j).image continuous_fst
have hspace : Continuous (fun z : Published.SpaceTime => EuclideanFlight.spaceEquiv z.2) :=
EuclideanFlight.spaceEquiv_continuous.comp continuous_snd
obtain ⟨B,_hB,hball⟩ := (hD.image hspace).isBounded.subset_ball_lt 0
(0 : JetPrototype.Space)
have hDw : D ⊆ EuclideanFlight.hotBaseSet (A j) B := by
rintro z ⟨u,hu,rfl⟩
refine ⟨⟨(ha j).le.trans (hwin j hu).1.1.1,(hwin j hu).1.1.2⟩,?_⟩
exact Metric.ball_subset_closedBall (hball (mem_image_of_mem _ (mem_image_of_mem Prod.fst hu)))
have ht := hconv j B D hD hDw
apply ht.congr
intro n
exact (EuclideanFlight.average_difference_norm_restrict (hc j) (ψ j)
(S.euclideanHot (E.indices (φ n))) (E.hotLimit ∘ EuclideanFlight.hotChart)).symm
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Strong local convergence of products of actual hot velocity averages -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology ENNReal
open BoltzmannNonuniqueness.Published BoltzmannNonuniqueness.TransportCutoff
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
theorem HotLimitExtraction.strong_average_products
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(S : AttainedCapSequence F) (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2)
(χ : ℕ → Published.KineticPhase → ℝ) (hχ : ∀ j, ContDiff ℝ (⊤ : ℕ∞) (χ j))
(hc : ∀ j, HasCompactSupport (χ j))
(hs : ∀ j, tsupport (χ j) ⊆ {z | 0 < z.1.1 ∧ ENNReal.ofReal z.1.1 < E.horizon})
(ψ : ℕ → Velocity → ℝ) (hψ : ∀ j, ContDiff ℝ (⊤ : ℕ∞) (ψ j))
(hψc : ∀ j, HasCompactSupport (ψ j)) :
∃ φ : ℕ → ℕ, StrictMono φ ∧ ∀ i j (D : Set Published.SpaceTime), IsCompact D →
Tendsto (fun n => eLpNorm (fun z =>
(∫ v, ψ i v*(χ i (z,v)*S.euclideanHot (E.indices (φ n)) (z,v)))*
(∫ v, ψ j v*(χ j (z,v)*S.euclideanHot (E.indices (φ n)) (z,v)))-
(∫ v, ψ i v*(χ i (z,v)*E.hotLimit (EuclideanFlight.hotChart (z,v))))*
(∫ v, ψ j v*(χ j (z,v)*E.hotLimit (EuclideanFlight.hotChart (z,v))))) 1
(volume.restrict D)) atTop (𝓝 0) := by
obtain ⟨φ,hφ,hconv⟩ := E.global_strong_averages hcarleman hGLPS S hs₀ hsmax hη hηmax
hK hα hαmax hγ hd₀ hd₀max hsmall hq₁ hq₂ χ hχ hc hs ψ hψ hψc
choose a A R ha haA hA hwin using fun j =>
exists_positive_cutoff_window E.horizon_ge (hc j) (hs j)
have hbound j := S.eventually_hot_average_bounded hs₀ hsmax hη hηmax hK hd₀.le hq₂
E.horizon_limit (ha j).le (haA j) (hA j) (hχ j).continuous (hc j) (hwin j)
(hψ j).continuous (hψc j)
choose B hB hb using hbound
let f : ℕ → ℕ → Published.SpaceTime → ℝ := fun j n z =>
∫ v, ψ j v*(χ j (z,v)*S.euclideanHot (E.indices (φ n)) (z,v))
let g : ℕ → Published.SpaceTime → ℝ := fun j z =>
∫ v, ψ j v*(χ j (z,v)*E.hotLimit (EuclideanFlight.hotChart (z,v)))
have hfm j n : Measurable (f j n) := by
have hm : Measurable (fun z : Published.KineticPhase =>
ψ j z.2*(χ j z*S.euclideanHot (E.indices (φ n)) z)) :=
((hψ j).continuous.measurable.comp measurable_snd).mul
((hχ j).continuous.measurable.mul
(S.euclideanHot_measurable hs₀ hsmax hη hηmax hK hd₀.le hq₂ _))
exact hm.stronglyMeasurable.integral_prod_right'.measurable
refine ⟨φ,hφ,fun i j D hD => ?_⟩
have : IsFiniteMeasure ((volume : Measure Published.SpaceTime).restrict D) :=
isFiniteMeasure_restrict.mpr hD.measure_lt_top.ne
have hlocal k : Tendsto (fun n => eLpNorm (fun z => f k n z-g k z) 1 (volume.restrict D))
atTop (𝓝 0) :=
tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds (hconv k)
(fun _ => zero_le) (fun _ => eLpNorm_mono_measure _ Measure.restrict_le_self)
have hlocalBound k : ∀ᶠ n in atTop, ∀ᵐ z ∂volume.restrict D, |f k n z| ≤ B k := by
filter_upwards [hφ.tendsto_atTop.eventually (hb k)] with n hn
exact ae_restrict_of_ae hn
exact Compactness.tendsto_L1_product_of_eventually_bounded
(fun n => (hfm i n).aestronglyMeasurable) (fun n => (hfm j n).aestronglyMeasurable)
(hlocal i) (hlocal j) (hB i) (hlocalBound i) (hlocalBound j)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The actual hot pair limit has the factorized tensor moments -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology ENNReal
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotPairExtraction.factorized_moments
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(E : HotPairExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2)
(χ : ℕ → Published.KineticPhase → ℝ) (hχ : ∀ j, ContDiff ℝ (⊤ : ℕ∞) (χ j))
(hc : ∀ j, HasCompactSupport (χ j))
(hs : ∀ j, tsupport (χ j) ⊆ {z | 0 < z.1.1 ∧ ENNReal.ofReal z.1.1 < E.horizon})
(ψ : ℕ → Velocity → ℝ) (hψ : ∀ j, ContDiff ℝ (⊤ : ℕ∞) (ψ j))
(hψc : ∀ j, HasCompactSupport (ψ j)) :
∀ i j (A R : ℝ), 0 ≤ A → ENNReal.ofReal A < E.horizon →
∀ D : Set Published.SpaceTime, IsCompact D → D ⊆ EuclideanFlight.hotBaseSet A R →
(fun z => ∫ y : Velocity × Velocity,
((ψ i y.1*χ i (z,y.1))*(ψ j y.2*χ j (z,y.2)))*
E.pairLimit (EuclideanFlight.hotPairChart (z,y))) =ᵐ[volume.restrict D]
(fun z => (∫ v, ψ i v*(χ i (z,v)*E.toHotLimitExtraction.hotLimit
(EuclideanFlight.hotChart (z,v))))*(∫ w, ψ j w*(χ j (z,w)*
E.toHotLimitExtraction.hotLimit (EuclideanFlight.hotChart (z,w))))) := by
obtain ⟨φ,hφ,hconv⟩ := E.toHotLimitExtraction.strong_average_products hcarleman hGLPS S
hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max hsmall hq₁ hq₂ χ hχ hc hs ψ hψ hψc
let E' := E.subsequence φ hφ
have hhot : E'.toHotLimitExtraction.hotLimit = E.toHotLimitExtraction.hotLimit := rfl
have hpair : E'.pairLimit = E.pairLimit := rfl
have hind : E'.indices = E.indices ∘ φ := rfl
let k : ℕ → Published.KineticPhase → ℝ := fun i z => ψ i z.2*χ i z
have hk i : Continuous (k i) :=
((hψ i).continuous.comp continuous_snd).mul (hχ i).continuous
have hkc i : HasCompactSupport (k i) := (hc i).mul_left
intro i j A R hA0 hA D hD hDw
have ht : Tendsto (fun n => eLpNorm (fun z =>
(∫ v, k i (z,v)*S.euclideanHot (E'.indices n) (z,v))*
(∫ w, k j (z,w)*S.euclideanHot (E'.indices n) (z,w))-
(∫ v, k i (z,v)*E'.toHotLimitExtraction.hotLimit (EuclideanFlight.hotChart (z,v)))*
(∫ w, k j (z,w)*E'.toHotLimitExtraction.hotLimit (EuclideanFlight.hotChart (z,w)))) 1
(volume.restrict D)) atTop (𝓝 0) := by
simpa only [hind,hhot,Function.comp_apply,k,mul_assoc] using hconv i j D hD
have he := E'.pair_moment_of_strong hs₀ hsmax hη hηmax hK hd₀.le hq₂ hA0 hA
(hk i) (hk j) (hkc i) (hkc j) hD hDw ht
simpa only [hpair,hhot,k,mul_assoc] using he
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The actual weak hot pair limit is the pair product of the hot density -/
noncomputable section
open MeasureTheory Set
open scoped ENNReal
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotPairExtraction.pairLimit_eq_product
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(E : HotPairExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {A : ℝ} (hA0 : 0 ≤ A)
(hA : ENNReal.ofReal A < E.horizon) (R : ℝ) :
(E.pairLimit ∘ EuclideanFlight.hotPairChart) =ᵐ[(EuclideanFlight.hotBaseVolume A R).prod volume]
CollisionCompactness.pairProduct (E.toHotLimitExtraction.hotLimit ∘ EuclideanFlight.hotChart) := by
have : SFinite (EuclideanFlight.hotBaseVolume A R) := by
unfold EuclideanFlight.hotBaseVolume
infer_instance
obtain ⟨ψ,hψ,hψc,hdet⟩ := Compactness.exists_countable_smooth_determining_tests
choose β hβ hβc _hβn hβtest using fun i => Compactness.exists_velocity_cutoff (hψc i)
obtain ⟨χ,hχ,hχc,hχs,hcover⟩ := Compactness.exists_spacetime_cutoff_cover
(EuclideanFlight.hotRegion_open E.horizon) (EuclideanFlight.hotRegion_nonempty E.horizon_ge)
let cuts : ℕ → Published.KineticPhase → ℝ := fun n =>
Compactness.productCutoff (χ (Nat.unpair n).1) (β (Nat.unpair n).2)
let tests : ℕ → Velocity → ℝ := fun n => ψ (Nat.unpair n).2
have hcuts n : ContDiff ℝ (⊤ : ℕ∞) (cuts n) :=
Compactness.productCutoff_smooth (hχ _) (hβ _)
have hcutsc n : HasCompactSupport (cuts n) :=
Compactness.productCutoff_compact (hχc _) (hβc _)
have hcutss n : tsupport (cuts n) ⊆
{z | 0 < z.1.1 ∧ ENNReal.ofReal z.1.1 < E.horizon} := by
intro z hz
exact hχs _ (Compactness.productCutoff_tsupport _ _ hz).1
have hfmom := E.factorized_moments hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ cuts hcuts hcutsc hcutss tests
(fun n => hψ _) (fun n => hψc _)
have hw (s i : ℕ) (z : Published.KineticPhase) :
tests (Nat.pair s i) z.2*cuts (Nat.pair s i) z = χ s z.1*ψ i z.2 := by
dsimp only [cuts,tests]
rw [Nat.unpair_pair]
change ψ i z.2*(χ s z.1*β i z.2) = χ s z.1*ψ i z.2
calc
_ = χ s z.1*(ψ i z.2*β i z.2) := by ring
_ = _ := by rw [hβtest]
have hwf (s i : ℕ) (z : Published.KineticPhase) (u : ℝ) :
tests (Nat.pair s i) z.2*(cuts (Nat.pair s i) z*u) = (χ s z.1*ψ i z.2)*u := by
rw [← mul_assoc,hw]
have hwv (s i : ℕ) (x : Published.SpaceTime) (v : Velocity) :
tests (Nat.pair s i) v*cuts (Nat.pair s i) (x,v) = χ s x*ψ i v := hw s i (x,v)
have hwfv (s i : ℕ) (x : Published.SpaceTime) (v : Velocity) (u : ℝ) :
tests (Nat.pair s i) v*(cuts (Nat.pair s i) (x,v)*u) = (χ s x*ψ i v)*u := hwf s i (x,v) u
let g := E.toHotLimitExtraction.hotLimit ∘ EuclideanFlight.hotChart
let W := E.pairLimit ∘ EuclideanFlight.hotPairChart
have hg := E.toHotLimitExtraction.euclidean_weak S hs₀ hsmax hη hηmax hK hd₀.le hq₂ hA R
have hW := E.euclidean_pair_weak hs₀ hsmax hη hηmax hK hd₀.le hq₂ hA R
have hscaled (s i j : ℕ) : ∀ᵐ x ∂EuclideanFlight.hotBaseVolume A R,
(∫ y : Velocity × Velocity, ((χ s x*ψ i y.1)*(χ s x*ψ j y.2))*W (x,y)) =
(∫ v, (χ s x*ψ i v)*g (x,v))*(∫ w, (χ s x*ψ j w)*g (x,w)) := by
apply Compactness.ae_of_all_compact_restrict
intro D hD
have hDc : IsCompact (D ∩ EuclideanFlight.hotBaseSet A R) :=
hD.inter_right (EuclideanFlight.hotBaseSet_closed A R)
have ht := hfmom (Nat.pair s i) (Nat.pair s j) A R hA0 hA
(D ∩ EuclideanFlight.hotBaseSet A R) hDc inter_subset_right
rw [EuclideanFlight.hotBaseVolume_eq,Measure.restrict_restrict hD.measurableSet]
filter_upwards [ht] with x hx
simpa only [hwv,hwfv,g,W,Function.comp_apply] using hx
have hpatch s : ∀ᵐ x ∂EuclideanFlight.hotBaseVolume A R, χ s x ≠ 0 →
(fun y => W (x,y)) =ᵐ[volume] (fun y : Velocity × Velocity => g (x,y.1)*g (x,y.2)) := by
apply Compactness.pair_identity_on_patch hψ hψc hdet hW.1 hg.1 hW.2.1 hg.2.1 (χ s)
exact fun i j => (hscaled s i j).mono (fun _ h _ => h)
have hfib : ∀ᵐ x ∂EuclideanFlight.hotBaseVolume A R,
(fun y => W (x,y)) =ᵐ[volume] (fun y : Velocity × Velocity => g (x,y.1)*g (x,y.2)) := by
filter_upwards [ae_all_iff.mpr hpatch,EuclideanFlight.hotRegion_ae hA R] with x hx hxin
obtain ⟨s,hs⟩ := hcover x hxin
exact hx s hs
exact (Measure.ae_prod_iff_ae_ae
(measurableSet_eq_fun hW.1 (CollisionCompactness.pairProduct_measurable hg.1))).mpr hfib
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The actual normalized hot cap bound on each time trace -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.Published BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
theorem normalizedHot_cap_at (S : AttainedCapSequence F)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (n : ℕ) {t : ℝ}
(ht : S.radius n*t ∈ Icc 0 (shrinkingHorizon F.horizonScale n)) :
∀ᵐ p : Velocity × Velocity, S.euclideanHot n ((t,p.1),p.2)/H q p.2 ≤ t+S.coldFraction n := by
have hp := EuclideanFlight.phaseEquiv_measurePreserving.quasiMeasurePreserving.ae
(S.rescaledHot_bound_at hs₀ hsmax hη hηmax hK hd₀ hq n ht)
filter_upwards [hp] with p hp
rw [S.euclideanHot_eq_rescaledHot]
apply (div_le_iff₀ (H_pos q p.2)).mpr
exact hp
theorem normalizedHot_cap_backward (S : AttainedCapSequence F)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (n : ℕ) {a : ℝ}
(ha : S.radius n*a ∈ Icc 0 (shrinkingHorizon F.horizonScale n)) (t : ℝ) :
∀ᵐ p : Velocity × Velocity,
S.euclideanHot n (PositiveIteration.flight ((t,p.1),p.2) a)/H q p.2 ≤ a+S.coldFraction n := by
have hp := (EuclideanFlight.flight_measurePreserving (a-t)).quasiMeasurePreserving.ae
(S.normalizedHot_cap_at hs₀ hsmax hη hηmax hK hd₀ hq n ha)
filter_upwards [hp] with p hp
convert hp using 1
unfold PositiveIteration.flight EuclideanFlight.flight
congr 4
module
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # An actual nonlinear weak hot limit on every bounded interior window -/
noncomputable section
open MeasureTheory Set
open scoped ENNReal
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotPairExtraction.nonlinear_weak
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(E : HotPairExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {A : ℝ} (hA0 : 0 ≤ A)
(hA : ENNReal.ofReal A < E.horizon) (R : ℝ) :
Published.WeakL1Converges ((EuclideanFlight.hotBaseVolume A R).prod volume)
(fun n => CollisionCompactness.pairProduct (S.euclideanHot (E.indices n)))
(CollisionCompactness.pairProduct
(E.toHotLimitExtraction.hotLimit ∘ EuclideanFlight.hotChart)) := by
exact (E.euclidean_pair_weak hs₀ hsmax hη hηmax hK hd₀.le hq₂ hA R).congr_limit
(CollisionCompactness.pairProduct_measurable
(E.toHotLimitExtraction.hotLimit_measurable.comp EuclideanFlight.hotChart.measurable))
(E.pairLimit_eq_product hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ hA0 hA R)
theorem exists_hot_nonlinear_limit
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(hDP : Published.DunfordPettis1940HotWindows)
(hDPpair : Published.DunfordPettis1940HotPairWindows) (S : AttainedCapSequence F)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) :
∃ E : HotPairExtraction S, ∀ A R : ℝ, 0 ≤ A → ENNReal.ofReal A < E.horizon →
Published.WeakL1Converges ((EuclideanFlight.hotBaseVolume A R).prod volume)
(fun n => CollisionCompactness.pairProduct (S.euclideanHot (E.indices n)))
(CollisionCompactness.pairProduct
(E.toHotLimitExtraction.hotLimit ∘ EuclideanFlight.hotChart)) := by
obtain ⟨E⟩ := S.exists_hot_limit_extraction hDP hs₀ hsmax hη hηmax hK hd₀.le hq₂
obtain ⟨P⟩ := S.exists_hot_pair_limit hDPpair E hs₀ hsmax hη hηmax hK hd₀.le hq₂
exact ⟨P,fun A R hA0 hA => P.nonlinear_weak hcarleman hGLPS hs₀ hsmax hη hηmax
hK hα hαmax hγ hd₀ hd₀max hsmall hq₁ hq₂ hA0 hA R⟩
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The hard-sphere weighted hot pair converges to the nonlinear limit -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology ENNReal
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotPairExtraction.weighted_nonlinear_subsequence
(hDP : Published.DunfordPettis1940HotPairWindows)
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(E : HotPairExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) :
∃ φ : ℕ → ℕ, StrictMono φ ∧ ∀ A R : ℝ, 0 ≤ A → ENNReal.ofReal A < E.horizon →
Published.WeakL1Converges ((EuclideanFlight.hotBaseVolume A R).prod volume)
(fun n => CollisionCompactness.pairDensity (S.euclideanHot (E.indices (φ n))))
(CollisionCompactness.pairDensity
(E.toHotLimitExtraction.hotLimit ∘ EuclideanFlight.hotChart)) := by
have hm n := CollisionCompactness.pairDensity_measurable
(S.hotDensity_measurable hs₀ hsmax hη hηmax hK hd₀.le hq₂ (E.indices n))
have hb (j : ℕ) := S.hotWeightedPair_bounds hs₀ hsmax hη hηmax hK hd₀.le hq₂
(show 0 ≤ (j:ℝ)+1 by positivity) ((j:ℝ)+1)
obtain ⟨φ,G,hφ,hG⟩ := Published.L1WeakCompactnessInput.countable
(fun j : ℕ => hotPairWindowVolume (j+1) (j+1))
(fun j => hDP (j+1) (j+1) (by positivity) (by positivity)) hm
(fun j => Compactness.uniformIntegrable_comp (hb j).1 E.indices)
(fun j => (hb j).2.comp E.indices)
refine ⟨φ,hφ,fun A R hA0 hA => ?_⟩
obtain ⟨j,hj⟩ := exists_nat_gt (max A R)
have hAj : A ≤ (j:ℝ)+1 := by have := (le_max_left A R).trans_lt hj; linarith
have hRj : R ≤ (j:ℝ)+1 := by have := (le_max_right A R).trans_lt hj; linarith
have hGj := (hG j).restrict (hotPairWindowSet_measurable A R)
rw [hotPairWindowVolume_restrict hAj hRj] at hGj
have hweighted := S.weighted_pair_physical_weak hs₀ hsmax hη hηmax hK hd₀.le hq₂
(E.horizon_limit.comp hφ.tendsto_atTop) hA hGj
have hraw := (E.nonlinear_weak hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ hA0 hA R).comp hφ.tendsto_atTop
let w : Published.SpaceTime × (Velocity × Velocity) → ℝ :=
fun z => 1+‖z.2.1‖+‖z.2.2‖
have hw : Measurable w := by dsimp [w]; fun_prop
have hw1 (z) : 1 ≤ w z := by
dsimp [w]
linarith [norm_nonneg z.2.1,norm_nonneg z.2.2]
have heq (u : Published.KineticPhase → ℝ) :
(fun z => w z*CollisionCompactness.pairProduct u z) =
CollisionCompactness.pairDensity u := by
funext z
simp only [w,CollisionCompactness.pairProduct,CollisionCompactness.pairDensity,mul_assoc]
have hw' : Published.WeakL1Converges ((EuclideanFlight.hotBaseVolume A R).prod volume)
(fun n z => w z*CollisionCompactness.pairProduct
(S.euclideanHot (E.indices (φ n))) z) (G j ∘ EuclideanFlight.hotPairChart) := by
have hs : (fun n z => w z*CollisionCompactness.pairProduct
(S.euclideanHot (E.indices (φ n))) z) =
(fun n => CollisionCompactness.pairDensity (S.euclideanHot (E.indices (φ n)))) :=
funext (fun n => heq _)
rw [hs]
exact hweighted
have hlim := Published.identify_weighted_weak_limit hraw hw' hw hw1
rw [heq] at hlim
exact hweighted.congr_limit
(CollisionCompactness.pairDensity_measurable
(E.toHotLimitExtraction.hotLimit_measurable.comp EuclideanFlight.hotChart.measurable)) hlim
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The identified hot pair in the physical capped representative -/
noncomputable section
open MeasureTheory
open scoped ENNReal
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotPairExtraction.pairLimit_eq_capped_product
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(E : HotPairExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {A : ℝ} (hA0 : 0 ≤ A)
(hA : ENNReal.ofReal A < E.horizon) (R : ℝ) :
E.pairLimit =ᵐ[hotPairWindowVolume A R]
CollisionCompactness.pairProduct E.toHotLimitExtraction.cappedHot := by
have he := E.pairLimit_eq_product hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ hA0 hA R
have hp := (MeasurePreserving.symm EuclideanFlight.hotPairChart
(EuclideanFlight.hotPairChart_measurePreserving A R)).quasiMeasurePreserving.ae he
have hraw : E.pairLimit =ᵐ[hotPairWindowVolume A R]
CollisionCompactness.pairProduct E.toHotLimitExtraction.hotLimit := by
filter_upwards [hp] with z hz
simp only [Function.comp_apply,MeasurableEquiv.apply_symm_apply] at hz
change E.pairLimit z = E.toHotLimitExtraction.hotLimit
((z.1.1,EuclideanFlight.spaceEquiv (EuclideanFlight.spaceEquiv.symm z.1.2)),z.2.1)*
E.toHotLimitExtraction.hotLimit
((z.1.1,EuclideanFlight.spaceEquiv (EuclideanFlight.spaceEquiv.symm z.1.2)),z.2.2) at hz
simpa only [MeasurableEquiv.apply_symm_apply,CollisionCompactness.pairProduct,Prod.mk.eta] using hz
have : SFinite (hotBaseWindowVolume A R) := by unfold hotBaseWindowVolume; infer_instance
exact hraw.trans (CollisionCompactness.pairProduct_congr
E.toHotLimitExtraction.hotLimit_measurable E.toHotLimitExtraction.cappedHot_measurable
(E.toHotLimitExtraction.cappedHot_eq A R).symm)
theorem HotPairExtraction.capped_pair_weak
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(E : HotPairExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {A : ℝ} (hA0 : 0 ≤ A)
(hA : ENNReal.ofReal A < E.horizon) (R : ℝ) :
Published.WeakL1Converges (hotPairWindowVolume A R)
(fun n => CollisionCompactness.pairProduct (S.hotDensity (E.indices n)))
(CollisionCompactness.pairProduct E.toHotLimitExtraction.cappedHot) :=
(E.pairLimit_weak A R).congr_limit
(CollisionCompactness.pairProduct_measurable E.toHotLimitExtraction.cappedHot_measurable)
(E.pairLimit_eq_capped_product hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ hA0 hA R)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Every bounded measurable hot average converges strongly on the same sequence -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotPairExtraction.strong_all_hot_averages
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(E : HotPairExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {A : ℝ} (hA0 : 0 ≤ A)
(hA : ENNReal.ofReal A < E.horizon) (R : ℝ)
{B : ℝ} {ψ : Velocity → ℝ} (hψ : Measurable ψ) (hψB : ∀ v, |ψ v| ≤ B) :
Tendsto (fun n => eLpNorm (fun x =>
(∫ v, ψ v*S.hotDensity (E.indices n) (x,v))-
(∫ v, ψ v*E.toHotLimitExtraction.cappedHot (x,v))) 1 (hotBaseWindowVolume A R))
atTop (𝓝 0) := by
let μ := hotBaseWindowVolume A R
let _ : IsFiniteMeasure ((volume : Measure JetPrototype.Space).restrict (Metric.closedBall 0 R)) :=
isFiniteMeasure_restrict.mpr (isCompact_closedBall (0 : JetPrototype.Space) R).measure_lt_top.ne
have : IsFiniteMeasure μ := by dsimp [μ,hotBaseWindowVolume]; infer_instance
have hB : 0 ≤ B := (abs_nonneg (ψ 0)).trans (hψB 0)
let C := (B*(A+1))*(∫ v, H q v)
have hC : 0 ≤ C := mul_nonneg (mul_nonneg hB (by linarith)) (integral_nonneg (H_nonneg q))
have hw := (E.toHotLimitExtraction.hotLimit_weak A R).congr_limit
E.toHotLimitExtraction.cappedHot_measurable (E.toHotLimitExtraction.cappedHot_eq A R).symm
have hp := E.capped_pair_weak hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ hA0 hA R
have hi (n) : Integrable (S.hotDensity (E.indices n)) (μ.prod volume) :=
memLp_one_iff_integrable.mp ((S.hotDensity_uniformIntegrable hs₀ hsmax hη hηmax hK hd₀.le hq₂ A R).memLp _)
have hpi (n) : Integrable (CollisionCompactness.pairProduct (S.hotDensity (E.indices n)))
(μ.prod (volume : Measure (Velocity × Velocity))) :=
memLp_one_iff_integrable.mp ((S.hotPair_bounds hs₀ hsmax hη hηmax hK hd₀.le hq₂ hA0 R).1.memLp _)
have havg (n) : ∀ᵐ x ∂μ, |∫ v, ψ v*S.hotDensity (E.indices n) (x,v)| ≤ C := by
filter_upwards [Measure.ae_ae_of_ae_prod
(S.hotDensity_bound hs₀ hsmax hη hηmax hK hd₀.le hq₂ (E.indices n) A R)] with x hx
have hb := norm_integral_le_of_norm_le
(f := fun v => ψ v*S.hotDensity (E.indices n) (x,v))
((integrable_H hq₂).const_mul (B*(A+1))) ?_
· simpa only [Real.norm_eq_abs,integral_const_mul,C] using hb
· filter_upwards [hx] with v hv
rw [Real.norm_eq_abs,abs_mul,abs_of_nonneg
(S.hotDensity_nonneg hs₀ hsmax hη hηmax hK hd₀.le hq₂ _ _)]
exact (mul_le_mul (hψB v) hv
(S.hotDensity_nonneg hs₀ hsmax hη hηmax hK hd₀.le hq₂ _ _) hB).trans_eq (by ring)
have hlim : ∀ᵐ x ∂μ, |∫ v, ψ v*E.toHotLimitExtraction.cappedHot (x,v)| ≤ C := by
filter_upwards [Measure.quasiMeasurePreserving_fst.ae (ae_restrict_mem measurableSet_Icc)] with x hx
have hb := norm_integral_le_of_norm_le
(f := fun v => ψ v*E.toHotLimitExtraction.cappedHot (x,v))
((integrable_H hq₂).const_mul (B*(A+1))) ?_
· simpa only [Real.norm_eq_abs,integral_const_mul,C] using hb
· filter_upwards [] with v
rw [Real.norm_eq_abs,abs_mul,abs_of_nonneg (E.toHotLimitExtraction.cappedHot_nonneg _)]
have htx : x.1+E.fraction ≤ A+1 := by linarith [hx.2,E.fraction_mem.2]
have hc := (E.toHotLimitExtraction.cappedHot_le hx.1 x.2 v).trans
(mul_le_mul_of_nonneg_right htx (H_nonneg q v))
exact (mul_le_mul (hψB v) hc (E.toHotLimitExtraction.cappedHot_nonneg _) hB).trans_eq (by ring)
change Published.WeakL1Converges (μ.prod (volume : Measure (Velocity × Velocity))) _ _ at hp
rw [Measure.volume_eq_prod Velocity Velocity] at hp hpi
exact Compactness.strong_average_of_weak_pairs hw hp
(fun n => S.hotDensity_measurable hs₀ hsmax hη hηmax hK hd₀.le hq₂ _)
(Eventually.of_forall hi) (Eventually.of_forall hpi) hψ hψB hC
(Eventually.of_forall havg) hlim
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Weak gain and loss limits for the actual rescaled hot density -/
noncomputable section
open MeasureTheory Set
open scoped ENNReal
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem euclideanHot_nonneg (S : AttainedCapSequence F)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (n : ℕ) (z : Published.KineticPhase) :
0 ≤ S.euclideanHot n z := by
rw [euclideanHot_eq_chart]
exact S.rescaledHot_nonneg hs₀ hsmax hη hηmax hK hd₀ hq n _
theorem HotPairExtraction.collision_subsequence
(hDP : Published.DunfordPettis1940HotPairWindows)
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(E : HotPairExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) :
∃ φ : ℕ → ℕ, StrictMono φ ∧ ∀ A R : ℝ, 0 ≤ A → ENNReal.ofReal A < E.horizon →
Published.WeakL1Converges ((EuclideanFlight.hotBaseVolume A R).prod volume)
(fun n => CollisionCompactness.gainDensity (S.euclideanHot (E.indices (φ n))))
(CollisionCompactness.gainDensity
(E.toHotLimitExtraction.hotLimit ∘ EuclideanFlight.hotChart)) ∧
Published.WeakL1Converges ((EuclideanFlight.hotBaseVolume A R).prod volume)
(fun n => CollisionCompactness.lossDensity (S.euclideanHot (E.indices (φ n))))
(CollisionCompactness.lossDensity
(E.toHotLimitExtraction.hotLimit ∘ EuclideanFlight.hotChart)) := by
obtain ⟨φ,hφ,hweighted⟩ := E.weighted_nonlinear_subsequence hDP hcarleman hGLPS
hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max hsmall hq₁ hq₂
refine ⟨φ,hφ,fun A R hA0 hA => ?_⟩
have : SFinite (EuclideanFlight.hotBaseVolume A R) := by
unfold EuclideanFlight.hotBaseVolume
infer_instance
have hi := (E.toHotLimitExtraction.subsequence φ hφ).eventually_weighted_pair_integrable
hs₀ hsmax hη hηmax hK hd₀.le hq₂ hA0 hA R
exact CollisionCompactness.weak_gainLoss_eventually
(fun n => S.euclideanHot_measurable hs₀ hsmax hη hηmax hK hd₀.le hq₂ _)
(fun n => S.euclideanHot_nonneg hs₀ hsmax hη hηmax hK hd₀.le hq₂ _)
(E.toHotLimitExtraction.hotLimit_measurable.comp EuclideanFlight.hotChart.measurable)
(hweighted A R hA0 hA) hi
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The actual rescaled hot-hot error vanishes on each interior window -/
noncomputable section
open MeasureTheory Filter
open scoped ENNReal Topology
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotPairExtraction.vanishing_quadratic_subsequence
(hDP : Published.DunfordPettis1940HotPairWindows)
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(E : HotPairExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) :
∃ φ : ℕ → ℕ, StrictMono φ ∧ ∀ A R : ℝ, 0 ≤ A → ENNReal.ofReal A < E.horizon →
Tendsto (fun n => eLpNorm (fun z => (S.radius (E.indices (φ n)))^2 *
CollisionCompactness.collisionSource (F.indices (E.indices (φ n))+1)
(S.euclideanHot (E.indices (φ n))) z) 1
((EuclideanFlight.hotBaseVolume A R).prod volume)) atTop (𝓝 0) := by
obtain ⟨φ,hφ,hcollision⟩ := E.collision_subsequence hDP hcarleman hGLPS hs₀ hsmax
hη hηmax hK hα hαmax hγ hd₀ hd₀max hsmall hq₁ hq₂
refine ⟨φ,hφ,fun A R hA0 hA => ?_⟩
have : SFinite (EuclideanFlight.hotBaseVolume A R) := by
unfold EuclideanFlight.hotBaseVolume
infer_instance
have hi := (E.toHotLimitExtraction.subsequence φ hφ).eventually_weighted_pair_integrable
hs₀ hsmax hη hηmax hK hd₀.le hq₂ hA0 hA R
have hr : Tendsto (fun n => (S.radius (E.indices (φ n)))^2) atTop (𝓝 0) := by
simpa only [Function.comp_def,zero_pow (by norm_num : (2:ℕ) ≠ 0)] using
((S.radius_tendsto_zero hs₀).comp (E.indices_strict.comp hφ).tendsto_atTop).pow 2
exact CollisionCompactness.vanishing_cutoff_collision
(fun n => S.euclideanHot_measurable hs₀ hsmax hη hηmax hK hd₀.le hq₂ _)
(fun n => S.euclideanHot_nonneg hs₀ hsmax hη hηmax hK hd₀.le hq₂ _)
hi (hcollision A R hA0 hA).1 (hcollision A R hA0 hA).2 _ hr
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Integrability of the actual hot density and source on physical cylinders -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology ENNReal
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
theorem eventually_physicalHot_cylinder_integrable (S : AttainedCapSequence F)
(E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) {a A : ℝ} (ha : 0 ≤ a)
(hA : ENNReal.ofReal A < E.horizon) (R : ℝ) :
∀ᶠ n in atTop, Integrable (S.physicalHotDensity (E.indices n))
((coldCylinderVolume a A R).prod volume) := by
have hui := S.hotDensity_uniformIntegrable hs₀ hsmax hη hηmax hK hd₀ hq A R
filter_upwards [S.eventually_extendedHot_eq hs₀ E.horizon_limit hA] with n hn
have hi : Integrable (S.hotDensity (E.indices n)) (hotWindowVolume A R) :=
memLp_one_iff_integrable.mp (hui.memLp (E.indices n))
have he : S.hotDensity (E.indices n) =ᵐ[hotWindowVolume A R]
S.physicalHotDensity (E.indices n) := by
filter_upwards [hotWindow_time_mem A R] with z hz
exact hn z.1.1 hz (z.1.2,z.2)
rw [coldCylinderVolume_eq_hot_restrict ha]
exact (hi.congr he).mono_measure Measure.restrict_le_self
theorem eventually_hotSource_cylinder_integrable (hcarleman : Published.GPV2009CarlemanInput)
(S : AttainedCapSequence F)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {κ : ℕ → ℕ} (hκ : StrictMono κ) {U : ℝ≥0∞}
(hU : Tendsto (fun n => S.normalizedHorizon (κ n)) atTop (𝓝 U))
{a A : ℝ} (ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < U) (R : ℝ) :
∀ᶠ n in atTop, Integrable (S.hotSourceDensity a A (κ n))
((coldCylinderVolume a A R).prod volume) := by
filter_upwards [S.eventually_hotSourceDensity_bound hcarleman hs₀ hsmax hη hηmax hK
hα hαmax hγ hd₀ hd₀max hsmall hq₁ hq₂ hκ hU ha haA hA R] with n hn
have hi : Integrable (S.hotSourceDensity a A (κ n)) (hotWindowVolume A R) := by
apply (sourceEnvelope_window_integrable hq₂ s₀ η K α γ d₀ a A R).mono'
(S.hotSourceDensity_measurable hs₀ hsmax hη hηmax hK hd₀.le hq₂ a A _).aestronglyMeasurable
simpa only [Real.norm_eq_abs] using hn
rw [coldCylinderVolume_eq_hot_restrict ha.le]
exact hi.mono_measure Measure.restrict_le_self
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Both error terms in the dilated hot equation vanish locally -/
noncomputable section
open MeasureTheory Filter
open scoped ENNReal Topology
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotPairExtraction.vanishing_collision_error
(hDP : Published.DunfordPettis1940HotPairWindows)
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(E : HotPairExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hα : 0 < α) (hαmax : α ≤ 1) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) :
∃ φ : ℕ → ℕ, StrictMono φ ∧ ∀ a A R : ℝ, 0 < a → a ≤ A →
ENNReal.ofReal A < E.horizon →
Tendsto (fun n => eLpNorm (fun z => (S.radius (E.indices (φ n)))^2 *
CollisionCompactness.collisionSource (F.indices (E.indices (φ n))+1)
(S.euclideanHot (E.indices (φ n))) z+
S.coldSourceDensity a A (E.indices (φ n)) (EuclideanFlight.hotChart z)) 1
((EuclideanFlight.hotBaseVolume A R).prod volume)) atTop (𝓝 0) := by
obtain ⟨φ,hφ,hquad⟩ := E.vanishing_quadratic_subsequence hDP hcarleman hGLPS hs₀ hsmax
hη hηmax hK hα hαmax hγ hd₀ hd₀max hsmall hq₁ hq₂
refine ⟨φ,hφ,fun a A R ha haA hA => ?_⟩
have hc := S.coldSourceDensity_tendsto_zero hcarleman hs₀ hsmax hη hηmax hK hα hαmax
hγ hd₀ hd₀max hsmall hq₁ hq₂ (E.indices_strict.comp hφ)
(E.horizon_limit.comp hφ.tendsto_atTop) ha haA hA R
have he (n) : eLpNorm (fun z =>
S.coldSourceDensity a A (E.indices (φ n)) (EuclideanFlight.hotChart z)) 1
((EuclideanFlight.hotBaseVolume A R).prod volume) =
eLpNorm (S.coldSourceDensity a A (E.indices (φ n))) 1 (hotWindowVolume A R) := by
exact eLpNorm_comp_measurePreserving
(S.coldSourceDensity_measurable hs₀ hsmax hη hηmax hK hd₀.le hq₂ a A _).aestronglyMeasurable
(EuclideanFlight.hotChart_measurePreserving A R)
have hc' : Tendsto (fun n => eLpNorm (fun z =>
S.coldSourceDensity a A (E.indices (φ n)) (EuclideanFlight.hotChart z)) 1
((EuclideanFlight.hotBaseVolume A R).prod volume)) atTop (𝓝 0) := by
simpa only [he,Function.comp_def] using hc
refine tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds
(by simpa only [zero_add] using (hquad A R (ha.le.trans haA) hA).add hc')
(fun _ => bot_le) (fun _ => ?_)
exact eLpNorm_add_le (by norm_num)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # A zero cap limit makes the actual bounded iteration input locally small -/
noncomputable section
open MeasureTheory Filter Set
open scoped ENNReal Topology
open BoltzmannNonuniqueness.Published BoltzmannNonuniqueness.VelocityWeight
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotLimitExtraction.zero_euclidean_L1 (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) {A R : ℝ}
(hA : ENNReal.ofReal A < E.horizon)
(hz : (E.hotLimit ∘ EuclideanFlight.hotChart) =ᵐ[(EuclideanFlight.hotBaseVolume A R).prod volume] 0) :
Tendsto (fun n => eLpNorm (S.euclideanHot (E.indices n)) 1
((EuclideanFlight.hotBaseVolume A R).prod volume)) atTop (𝓝 0) := by
apply (E.euclidean_weak S hs₀ hsmax hη hηmax hK hd₀ hq hA R).nonnegative_zero_L1 hz
(S.eventually_euclideanHot_integrable E hs₀ hsmax hη hηmax hK hd₀ hq hA R)
exact Eventually.of_forall (fun n => ae_of_all _
(S.euclideanHot_nonneg hs₀ hsmax hη hηmax hK hd₀ hq (E.indices n)))
theorem HotLimitExtraction.zero_boundedHotRatio_L1 (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) {A R V : ℝ}
(hA : ENNReal.ofReal A < E.horizon) (hV : 0 ≤ V)
(hz : (E.hotLimit ∘ EuclideanFlight.hotChart) =ᵐ[(EuclideanFlight.hotBaseVolume A R).prod volume] 0) :
Tendsto (fun n => eLpNorm (S.boundedHotRatio (E.indices n)) 1
(((EuclideanFlight.hotBaseVolume A R).prod volume).restrict {z | ‖z.2‖ ≤ V})) atTop (𝓝 0) := by
have hratio := Compactness.tendsto_L1_div_H_on_velocity_ball
(fun n => S.euclideanHot_measurable hs₀ hsmax hη hηmax hK hd₀ hq (E.indices n))
(E.zero_euclidean_L1 hs₀ hsmax hη hηmax hK hd₀ hq hA hz) q hV
apply tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds hratio
(fun _ => bot_le)
intro n
apply eLpNorm_mono_ae
(S.boundedHotRatio_measurable hs₀ hsmax hη hηmax hK hd₀ hq
(E.indices n)).aestronglyMeasurable
apply ae_of_all
intro z
have hn := div_nonneg (S.euclideanHot_nonneg hs₀ hsmax hη hηmax hK hd₀ hq (E.indices n) z)
(H_nonneg q z.2)
rw [Real.norm_eq_abs,Real.norm_eq_abs,
abs_of_nonneg (S.boundedHotRatio_bounds (E.indices n) z).1,abs_of_nonneg hn]
exact max_le hn (min_le_right _ _)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # A zero cap limit forces local L1 smallness of the actual hot solutions -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology ENNReal
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotLimitExtraction.zero_physical_L1 (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) {a A R : ℝ} (ha : 0 ≤ a)
(hA : ENNReal.ofReal A < E.horizon)
(hz : E.hotLimit =ᵐ[(coldCylinderVolume a A R).prod volume] 0) :
Tendsto (fun n => eLpNorm (S.physicalHotDensity (E.indices n)) 1
((coldCylinderVolume a A R).prod volume)) atTop (𝓝 0) := by
apply (E.physical_weak_cylinder S hs₀ ha hA R).nonnegative_zero_L1 hz
(S.eventually_physicalHot_cylinder_integrable E hs₀ hsmax hη hηmax hK hd₀ hq ha hA R)
exact Eventually.of_forall (fun n => ae_of_all _ (fun z =>
S.rescaledHot_nonneg hs₀ hsmax hη hηmax hK hd₀ hq (E.indices n) (z.1.1,(z.1.2,z.2))))
theorem HotLimitExtraction.zero_physical_inMeasure (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) {a A R : ℝ} (ha : 0 ≤ a)
(hA : ENNReal.ofReal A < E.horizon)
(hz : E.hotLimit =ᵐ[(coldCylinderVolume a A R).prod volume] 0) :
TendstoInMeasure ((coldCylinderVolume a A R).prod volume)
(fun n => S.physicalHotDensity (E.indices n)) atTop 0 := by
apply tendstoInMeasure_of_tendsto_eLpNorm (by norm_num : (1 : ℝ≥0∞) ≠ 0)
simpa only [sub_zero] using E.zero_physical_L1 hs₀ hsmax hη hηmax hK hd₀ hq ha hA hz
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Local vanishing of the normalized hot ratio under a zero cap limit -/
noncomputable section
open MeasureTheory Filter Set
open scoped Topology ENNReal
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
{S : AttainedCapSequence F}
theorem HotLimitExtraction.zero_ratio_L1 (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) {a A R V : ℝ} (ha : 0 ≤ a)
(hA : ENNReal.ofReal A < E.horizon) (hV : 0 ≤ V)
(hz : E.hotLimit =ᵐ[(coldCylinderVolume a A R).prod volume] 0) :
Tendsto (fun n => eLpNorm
(fun z => S.physicalHotDensity (E.indices n) z / VelocityWeight.H q z.2) 1
(((coldCylinderVolume a A R).prod volume).restrict {z | ‖z.2‖ ≤ V})) atTop (𝓝 0) :=
Compactness.tendsto_L1_div_H_on_velocity_ball
(fun _ => S.physicalHotDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq _)
(E.zero_physical_L1 hs₀ hsmax hη hηmax hK hd₀ hq ha hA hz) q hV
theorem HotLimitExtraction.zero_ratio_inMeasure (E : HotLimitExtraction S)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) {a A R V : ℝ} (ha : 0 ≤ a)
(hA : ENNReal.ofReal A < E.horizon) (hV : 0 ≤ V)
(hz : E.hotLimit =ᵐ[(coldCylinderVolume a A R).prod volume] 0) :
TendstoInMeasure (((coldCylinderVolume a A R).prod volume).restrict {z | ‖z.2‖ ≤ V})
(fun n z => S.physicalHotDensity (E.indices n) z / VelocityWeight.H q z.2) atTop 0 := by
apply tendstoInMeasure_of_tendsto_eLpNorm (by norm_num : (1 : ℝ≥0∞) ≠ 0)
simpa only [sub_zero] using E.zero_ratio_L1 hs₀ hsmax hη hηmax hK hd₀ hq ha hA hV hz
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
end OAI