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import OAI.MathematicalPhysics.Boltzmann.Approximation.CapActualLossDensity
import OAI.MathematicalPhysics.Boltzmann.Approximation.CapHotUndamped
import OAI.MathematicalPhysics.Boltzmann.Approximation.CapLabelFreeLimit
import OAI.MathematicalPhysics.Boltzmann.Approximation.CapColdBounds
import OAI.MathematicalPhysics.Boltzmann.Approximation.CapNonlinearHotLimit
import OAI.MathematicalPhysics.Boltzmann.Approximation.PositiveNonlinearLimit
import OAI.MathematicalPhysics.Boltzmann.Branching.BackgroundBeamCloseness
import OAI.MathematicalPhysics.Boltzmann.Branching.HotCollisionDecomposition
import OAI.MathematicalPhysics.Boltzmann.Branching.IncomingLossRate
import OAI.MathematicalPhysics.Boltzmann.Branching.MixedPhysicalMeasures
import OAI.MathematicalPhysics.Boltzmann.Branching.RelativeCutoffConvergence
import OAI.MathematicalPhysics.Boltzmann.Branching.WeightedThermalChain
import OAI.MathematicalPhysics.Boltzmann.Collision.CollisionWeakMarginals
import OAI.MathematicalPhysics.Boltzmann.Collision.GaussianWeightedConvergence
import OAI.MathematicalPhysics.Boltzmann.Compactness.PhysicalEvolution
import OAI.MathematicalPhysics.Boltzmann.Compactness.WeakL1ToWeakStar
import OAI.MathematicalPhysics.Boltzmann.Jets.ColdCentralVanishing
namespace OAI
section
/-! # The actual cap family has a positive limit with its full collision terms -/
noncomputable section
open MeasureTheory
namespace BoltzmannNonuniqueness.JetCopyDatum
theorem TightCapFamily.exists_collision_limit
(hcarleman : Published.GPV2009CarlemanInput) (hGLPS : Published.GLPS1988Proposition3)
(hDP : Published.DunfordPettis1940Theorem321)
{s₀ η K α γ d₀ q : ℝ} (F : TightCapFamily s₀ η K α γ d₀ q)
(hq₁ : 1 < q) (hq₂ : q < 2) :
∃ (φ : ℕ → ℕ) (g : (ℝ × Position) × Velocity → ℝ), StrictMono φ ∧
Published.WeakL1Converges ((AnnularEnvelope.timePositionVolume F.time).prod volume)
(fun n => torusPhysical q (F.approximation (φ n)).solution.value) g ∧
Published.WeakL1Converges ((AnnularEnvelope.timePositionVolume F.time).prod volume)
(fun n => CollisionCompactness.gainDensity
(torusPhysical q (F.approximation (φ n)).solution.value))
(CollisionCompactness.gainDensity g) ∧
Published.WeakL1Converges ((AnnularEnvelope.timePositionVolume F.time).prod volume)
(fun n => CollisionCompactness.lossDensity
(torusPhysical q (F.approximation (φ n)).solution.value))
(CollisionCompactness.lossDensity g) ∧
Integrable (CollisionCompactness.pairDensity g)
((AnnularEnvelope.timePositionVolume F.time).prod volume) ∧ (∀ z, 0 ≤ g z) := by
obtain ⟨φ,g,hφ,hg,hpair,hgn⟩ := F.exists_positive_nonlinear_limit hcarleman hGLPS hDP hq₁ hq₂
have hfm n := torusPhysical_measurable (F.approximation (φ n)).solution.measurable_value q
have hfn n := torusPhysical_nonneg
(fun z => ((F.approximation (φ n)).solution.value_bounds z).1) q
have hf n := memLp_one_iff_integrable.mp (F.pairs_ui.memLp (φ n))
have hterms := CollisionCompactness.weak_gainLoss hfm hfn hg.1 hpair hf
exact ⟨φ,g,hφ,hg,hterms.1,hterms.2,hpair.2.1,hgn⟩
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # Full cold velocity averages converge weak-star to the atomic background -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.VelocityMoment
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.cold_spacetime_weakStar_limit (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 ≤ 1/4) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq : q < 2) {a A R : ℝ} (ha : 0 < a) (hA : ENNReal.ofReal A < E.horizon) (hR : 0 ≤ R)
{B : ℝ} {ψ : Velocity → ℝ} (hψ : Continuous ψ) (hψB : ∀ v, |ψ v| ≤ B) :
Compactness.WeakStarLInfConverges (coldCylinderVolume a A R)
(fun n => S.coldAverage (E.indices n) ψ)
(fun z => ∫ v, ψ v ∂E.background (max 0 z.1) z.2) := by
let ρ := coldCylinderVolume a A R
let M := escapedConstant s₀ η K α d₀*hotConstant q+JetEnvelopeGain.momentConstant K α γ/a
let N := 2*((1/4)*((K*max 1 (α*γ)⁻¹)/a))
let C := |B*M|+|N*B|
have hC : 0 ≤ C := add_nonneg (abs_nonneg _) (abs_nonneg _)
have hB : 0 ≤ B := (abs_nonneg (ψ 0)).trans (hψB 0)
have ham (n) : Measurable (S.coldAverage (E.indices n) ψ) :=
S.coldAverage_measurable hs₀ hsmax hη hηmax hK hd₀.le hq _ hψ.measurable
have hbm : Measurable (fun z : ℝ × JetPrototype.Space => ∫ v, ψ v ∂E.background (max 0 z.1) z.2) :=
GeometricBackground.clamped_background_test_measurable (zero_lt_one.trans_le E.phase_mem.1)
hK hα.le hγ.le η E.fraction hψ.measurable
have htime : ∀ᵐ z ∂ρ, z.1 ∈ Icc a A :=
Measure.quasiMeasurePreserving_fst.ae (ae_restrict_mem measurableSet_Icc)
have hab : ∀ᶠ n in atTop, ∀ᵐ z ∂ρ, |S.coldAverage (E.indices n) ψ z| ≤ C := by
filter_upwards [E.eventually_coldAverage_bound hs₀ hsmax hη hηmax hK hα
(hαmax.trans (by norm_num)) hγ hd₀ hd₀max hsmall hq ha hA hB hψB] with n hn
filter_upwards [htime] with z hz
exact (hn z.1 hz z.2).trans ((le_abs_self (B*M)).trans (le_add_of_nonneg_right (abs_nonneg _)))
have hbb : ∀ᵐ z ∂ρ, |∫ v, ψ v ∂E.background (max 0 z.1) z.2| ≤ C := by
filter_upwards [htime] with z hz
have ht : a ≤ max 0 z.1 := hz.1.trans (le_max_right _ _)
exact (E.background_average_slab_bound hK hα hγ ha ht hψB z.2).trans
((le_abs_self (N*B)).trans (le_add_of_nonneg_left (abs_nonneg _)))
apply Compactness.weakStar_of_exhaustion ham hbm hab hbb coldAxisCutoff coldAxisCutoff_measurable
(coldAxisCutoff_exhausts a A R)
intro m
have hw : Published.WeakL1Converges (ρ.restrict (coldAxisCutoff m))
(fun n => S.coldAverage (E.indices n) ψ)
(fun z => ∫ v, ψ v ∂E.background (max 0 z.1) z.2) := by
change Published.WeakL1Converges ((coldCylinderVolume a A R).restrict (coldAxisCutoff m)) _ _
rw [coldCylinderVolume_restrict_axis]
apply E.cold_away_axis_weak_limit hs₀ hsmax hη hηmax hK hα hαmax hγ hd₀ hd₀max
hsmall hq ha hA (by positivity) hR (coldTransverseAnnulus R m) (coldTransverseAnnulus_compact R m)
(fun _ hx => hx.2) (fun y hy => ?_) (Icc (-R) R) isCompact_Icc
(fun z hz => abs_le.mpr ⟨hz.1,hz.2⟩) hψ hψB
simpa only [Metric.mem_closedBall,dist_zero_right] using hy.1
exact hw.weakStar ham hC (hab.mono (fun _ hn => ae_restrict_of_ae hn)) (ae_restrict_of_ae hbb)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The actual collision error vanishes on the physical cold cylinders -/
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}
def physicalCollisionError (S : AttainedCapSequence F) (a A : ℝ) (n : ℕ)
(z : HotKineticPhase) : ℝ :=
(S.radius n)^2*CollisionCompactness.collisionSource (F.indices n+1) (S.physicalHotDensity n) z+
S.coldSourceDensity a A n z
theorem physicalCollisionError_measurable (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) (a A : ℝ) (n : ℕ) :
Measurable (S.physicalCollisionError a A n) :=
((CollisionCompactness.collisionSource_measurable
(S.physicalHotDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq n) _).const_mul _).add
(S.coldSourceDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq a A n)
theorem HotPairExtraction.vanishing_physical_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 (S.physicalCollisionError a A (E.indices (φ n))) 1
((coldCylinderVolume a A R).prod volume)) atTop (𝓝 0) := by
obtain ⟨φ,hφ,herr⟩ := E.vanishing_collision_error 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 hw : Tendsto (fun n => eLpNorm (S.physicalCollisionError a A (E.indices (φ n))) 1
(hotWindowVolume A R)) atTop (𝓝 0) := by
apply (herr a A R ha haA hA).congr'
filter_upwards [] with n
have he : (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)) =
S.physicalCollisionError a A (E.indices (φ n)) ∘ EuclideanFlight.hotChart := by
funext z
rw [euclideanHot_eq_chart]
rfl
rw [he]
exact eLpNorm_comp_measurePreserving
(S.physicalCollisionError_measurable hs₀ hsmax hη hηmax hK hd₀.le hq₂ a A _).aestronglyMeasurable
(EuclideanFlight.hotChart_measurePreserving A R)
refine tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds hw
(fun _ => bot_le) (fun n => ?_)
exact eLpNorm_mono_measure _ (Measure.prod_mono
(coldCylinderVolume_le_hotBaseWindowVolume ha.le) le_rfl)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The actual cold-hot pair density on finite positive-time cylinders -/
noncomputable section
open MeasureTheory Set
open scoped ENNReal
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}
def mixedDensity (S : AttainedCapSequence F) (n : ℕ) (z : HotPairPhase) : ℝ :=
S.rescaledColdDensity n (z.1,z.2.1)*S.hotDensity n (z.1,z.2.2)
theorem mixedDensity_measurable (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) :
Measurable (S.mixedDensity n) :=
((S.rescaledColdDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq n).comp
(measurable_fst.prodMk measurable_snd.fst)).mul
((S.hotDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq n).comp
(measurable_fst.prodMk measurable_snd.snd))
theorem mixedDensity_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 : HotPairPhase) :
0 ≤ S.mixedDensity n z :=
mul_nonneg (S.rescaledColdDensity_bounds hs₀ hsmax hη hηmax hK hd₀ hq n _).1
(S.hotDensity_nonneg hs₀ hsmax hη hηmax hK hd₀ hq n _)
theorem mixedDensity_integrable (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 A R : ℝ} (ha : 0 ≤ a) :
Integrable (S.mixedDensity n) ((coldCylinderVolume a A R).prod volume) := by
let ρ := coldCylinderVolume a A R
let C := (S.radius n*(2*(F.approximation n).amplitude))*(A+1)
have hi : Integrable (fun z : HotPairPhase => C*(H q z.2.1*H q z.2.2)) (ρ.prod volume) := by
have hv := (integrable_H hq).mul_prod (integrable_H hq)
rw [← Measure.volume_eq_prod] at hv
exact (hv.comp_snd ρ).const_mul C
have hb : ∀ᵐ z ∂ρ.prod (volume : Measure Velocity), S.hotDensity n z ≤ (A+1)*H q z.2 :=
(S.hotDensity_bound hs₀ hsmax hη hηmax hK hd₀ hq n A R).filter_mono
(ae_mono (Measure.prod_mono (coldCylinderVolume_le_hotBaseWindowVolume ha) le_rfl))
apply hi.mono' (S.mixedDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq n).aestronglyMeasurable
apply (Measure.ae_prod_iff_ae_ae (measurableSet_le
((S.mixedDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq n).norm)
((((ChartKernel.measurable_H q).comp measurable_snd.fst).mul
((ChartKernel.measurable_H q).comp measurable_snd.snd)).const_mul C))).mpr
filter_upwards [Measure.ae_ae_of_ae_prod hb] with x hx
have hw : ∀ᵐ p : Velocity × Velocity ∂(volume : Measure Velocity).prod volume,
S.hotDensity n (x,p.2) ≤ (A+1)*H q p.2 := Measure.quasiMeasurePreserving_snd.ae hx
rw [Measure.volume_eq_prod]
filter_upwards [hw] with p hp
rw [Real.norm_of_nonneg (S.mixedDensity_nonneg hs₀ hsmax hη hηmax hK hd₀ hq n _)]
exact (mul_le_mul (S.rescaledColdDensity_bounds hs₀ hsmax hη hηmax hK hd₀ hq n _).2 hp
(S.hotDensity_nonneg hs₀ hsmax hη hηmax hK hd₀ hq n _) (by
exact mul_nonneg (mul_nonneg (S.radius_pos hs₀ n).le (mul_nonneg (by norm_num)
(F.approximation n).amplitude_pos.le)) (H_nonneg q p.1))).trans_eq (by dsimp only [C,Function.comp_apply,Pi.mul_apply]; ring)
def mixedPrelimitMeasure (S : AttainedCapSequence F) (n : ℕ)
(ρ : Measure (ℝ × JetPrototype.Space)) : Measure HotPairPhase :=
(ρ.prod volume).withDensity (fun z => ENNReal.ofReal (S.mixedDensity n z))
theorem mixedPrelimitMeasure_finite (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 A R : ℝ} (ha : 0 ≤ a) :
IsFiniteMeasure (S.mixedPrelimitMeasure n (coldCylinderVolume a A R)) := by
apply isFiniteMeasure_withDensity
have hi := S.mixedDensity_integrable hs₀ hsmax hη hηmax hK hd₀ hq n (A := A) (R := R) ha
exact ((hasFiniteIntegral_iff_ofReal (ae_of_all _
(S.mixedDensity_nonneg hs₀ hsmax hη hηmax hK hd₀ hq n))).mp hi.hasFiniteIntegral).ne
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Mixed cold-hot velocity moments converge along the actual common sequence -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.VelocityMoment
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.mixed_average_weak_limit
(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 ≤ 1/4) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {a A R : ℝ}
(ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < E.horizon) (hR : 0 ≤ R)
{B D : ℝ} {ψ χ : Velocity → ℝ}
(hψ : Continuous ψ) (hψB : ∀ v, |ψ v| ≤ B) (hχ : Measurable χ) (hχD : ∀ v, |χ v| ≤ D) :
Published.WeakL1Converges (coldCylinderVolume a A R)
(fun n x => S.coldAverage (E.indices n) ψ x*(∫ v, χ v*S.hotDensity (E.indices n) (x,v)))
(fun x => (∫ v, ψ v ∂E.toHotLimitExtraction.background (max 0 x.1) x.2)*
(∫ v, χ v*E.toHotLimitExtraction.cappedHot (x,v))) := by
let ρ := coldCylinderVolume a A R
let M := escapedConstant s₀ η K α d₀*hotConstant q+JetEnvelopeGain.momentConstant K α γ/a
let N := 2*((1/4)*((K*max 1 (α*γ)⁻¹)/a))
let C := |B*M|+|N*B|
have hC : 0 ≤ C := add_nonneg (abs_nonneg _) (abs_nonneg _)
have hα1 : α ≤ 1 := hαmax.trans (by norm_num)
have hB : 0 ≤ B := (abs_nonneg (ψ 0)).trans (hψB 0)
have hρ : ρ ≤ hotBaseWindowVolume A R := coldCylinderVolume_le_hotBaseWindowVolume ha.le
have hcold := E.toHotLimitExtraction.cold_spacetime_weakStar_limit hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₂ ha hA hR hψ hψB
have hstrong := E.strong_all_hot_averages hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hα1 hγ
hd₀ hd₀max hsmall hq₁ hq₂ (ha.le.trans haA) hA R hχ hχD
have hstrongρ : Tendsto (fun n => eLpNorm (fun x =>
(∫ v, χ v*S.hotDensity (E.indices n) (x,v))-
(∫ v, χ v*E.toHotLimitExtraction.cappedHot (x,v))) 1 ρ) atTop (𝓝 0) :=
tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds hstrong
(fun _ => zero_le) (fun _ => eLpNorm_mono_measure _ hρ)
have hhm (n) : Measurable (fun x => ∫ v, χ v*S.hotDensity (E.indices n) (x,v)) :=
((hχ.comp measurable_snd).mul
(S.hotDensity_measurable hs₀ hsmax hη hηmax hK hd₀.le hq₂ _)).stronglyMeasurable.integral_prod_right'.measurable
have hgm : Measurable (fun x => ∫ v, χ v*E.toHotLimitExtraction.cappedHot (x,v)) :=
((hχ.comp measurable_snd).mul E.toHotLimitExtraction.cappedHot_measurable).stronglyMeasurable.integral_prod_right'.measurable
have hgi : Integrable (fun x => ∫ v, χ v*E.toHotLimitExtraction.cappedHot (x,v)) ρ := by
have hw := (E.toHotLimitExtraction.hotLimit_weak A R).congr_limit
E.toHotLimitExtraction.cappedHot_measurable (E.toHotLimitExtraction.cappedHot_eq A R).symm
have hi (n) := memLp_one_iff_integrable.mp
((S.hotDensity_uniformIntegrable hs₀ hsmax hη hηmax hK hd₀.le hq₂ A R).memLp (E.indices n))
exact ((hw.marginal hi (hχ.comp measurable_snd) D (fun z => hχD z.2)).2.1).mono_measure hρ
have htime : ∀ᵐ x ∂ρ, x.1 ∈ Icc a A :=
Measure.quasiMeasurePreserving_fst.ae (ae_restrict_mem measurableSet_Icc)
have hac : ∀ᶠ n in atTop, ∀ᵐ x ∂ρ, |S.coldAverage (E.indices n) ψ x| ≤ C := by
filter_upwards [E.toHotLimitExtraction.eventually_coldAverage_bound hs₀ hsmax hη hηmax hK hα hα1 hγ
hd₀ hd₀max hsmall hq₂ ha hA hB hψB] with n hn
filter_upwards [htime] with x hx
exact (hn x.1 hx x.2).trans ((le_abs_self (B*M)).trans (le_add_of_nonneg_right (abs_nonneg _)))
have hbc : ∀ᵐ x ∂ρ, |∫ v, ψ v ∂E.toHotLimitExtraction.background (max 0 x.1) x.2| ≤ C := by
filter_upwards [htime] with x hx
exact (E.toHotLimitExtraction.background_average_slab_bound hK hα hγ ha
(hx.1.trans (le_max_right _ _)) hψB x.2).trans
((le_abs_self (N*B)).trans (le_add_of_nonneg_left (abs_nonneg _)))
exact hcold.strong_product
(fun n => S.coldAverage_measurable hs₀ hsmax hη hηmax hK hd₀.le hq₂ _ hψ.measurable)
hhm hgm hgi hstrongρ hC hac hbc
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Uniform product Gaussian moments for the actual mixed measures -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.VelocityMoment
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 mixedPrelimitMeasure_gaussian_moment (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)
(ρ : Measure (ℝ × JetPrototype.Space)) [SFinite ρ] :
(∫⁻ z, ENNReal.ofReal (weight z.2.1*weight z.2.2) ∂S.mixedPrelimitMeasure n ρ) =
∫⁻ x, moment (fun v => S.rescaledColdDensity n (x,v))*moment (fun v => S.hotDensity n (x,v)) ∂ρ := by
have hc := S.rescaledColdDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq n
have hh := S.hotDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq n
have hw : Measurable (fun v : Velocity => weight v) := by unfold weight; fun_prop
have hwp : Measurable (fun z : HotPairPhase => ENNReal.ofReal (weight z.2.1*weight z.2.2)) :=
((hw.comp measurable_snd.fst).mul (hw.comp measurable_snd.snd)).ennreal_ofReal
rw [mixedPrelimitMeasure,lintegral_withDensity_eq_lintegral_mul _
(S.mixedDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq n).ennreal_ofReal hwp]
have he (z : HotPairPhase) :
ENNReal.ofReal (S.mixedDensity n z)*ENNReal.ofReal (weight z.2.1*weight z.2.2) =
ENNReal.ofReal (weight z.2.1*S.rescaledColdDensity n (z.1,z.2.1))*
ENNReal.ofReal (weight z.2.2*S.hotDensity n (z.1,z.2.2)) := by
rw [← ENNReal.ofReal_mul (S.mixedDensity_nonneg hs₀ hsmax hη hηmax hK hd₀ hq n z),
← ENNReal.ofReal_mul (mul_nonneg (weight_pos _).le
(S.rescaledColdDensity_bounds hs₀ hsmax hη hηmax hK hd₀ hq n _).1)]
congr 1
dsimp only [mixedDensity]
ring
simp_rw [Pi.mul_apply,he]
have hm : Measurable (fun z : HotPairPhase =>
ENNReal.ofReal (weight z.2.1*S.rescaledColdDensity n (z.1,z.2.1))*
ENNReal.ofReal (weight z.2.2*S.hotDensity n (z.1,z.2.2))) :=
(((hw.comp measurable_snd.fst).mul (hc.comp (measurable_fst.prodMk measurable_snd.fst))).ennreal_ofReal).mul
(((hw.comp measurable_snd.snd).mul (hh.comp (measurable_fst.prodMk measurable_snd.snd))).ennreal_ofReal)
rw [lintegral_prod _ hm.aemeasurable]
apply lintegral_congr
intro x
change (∫⁻ y : Velocity × Velocity,
ENNReal.ofReal (weight y.1*S.rescaledColdDensity n (x,y.1))*
ENNReal.ofReal (weight y.2*S.hotDensity n (x,y.2))) = _
rw [Measure.volume_eq_prod]
exact lintegral_prod_mul
(f := fun v => ENNReal.ofReal (weight v*S.rescaledColdDensity n (x,v)))
(g := fun v => ENNReal.ofReal (weight v*S.hotDensity n (x,v)))
((hw.mul (hc.comp (measurable_const.prodMk measurable_id))).ennreal_ofReal.aemeasurable)
((hw.mul (hh.comp (measurable_const.prodMk measurable_id))).ennreal_ofReal.aemeasurable)
theorem eventually_mixedPrelimitMeasure_gaussian_bound (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)
(hq : 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 : ℝ} (ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < U) :
∀ᶠ n in atTop,
(∫⁻ z, ENNReal.ofReal (weight z.2.1*weight z.2.2)
∂S.mixedPrelimitMeasure (κ n) (coldCylinderVolume a A R)) ≤
ENNReal.ofReal ((escapedConstant s₀ η K α d₀*hotConstant q+
JetEnvelopeGain.momentConstant K α γ/a)*((A+1)*hotConstant q))*
coldCylinderVolume a A R univ := by
have hc := S.eventually_rescaledColdDensity_moment hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq hκ hU ha hA
filter_upwards [hc] with n hn
rw [S.mixedPrelimitMeasure_gaussian_moment hs₀ hsmax hη hηmax hK hd₀.le hq]
have hb : ∀ᵐ z ∂(coldCylinderVolume a A R).prod (volume : Measure Velocity),
S.hotDensity (κ n) z ≤ (A+1)*VelocityWeight.H q z.2 :=
(S.hotDensity_bound hs₀ hsmax hη hηmax hK hd₀.le hq (κ n) A R).filter_mono
(ae_mono (Measure.prod_mono (coldCylinderVolume_le_hotBaseWindowVolume ha.le) le_rfl))
have ht : ∀ᵐ x ∂coldCylinderVolume a A R, x.1 ∈ Icc a A :=
Measure.quasiMeasurePreserving_fst.ae (ae_restrict_mem measurableSet_Icc)
calc
_ ≤ ∫⁻ _x : ℝ × JetPrototype.Space,
ENNReal.ofReal (escapedConstant s₀ η K α d₀*hotConstant q+
JetEnvelopeGain.momentConstant K α γ/a)*ENNReal.ofReal ((A+1)*hotConstant q) ∂coldCylinderVolume a A R := by
apply lintegral_mono_ae
filter_upwards [ht,Measure.ae_ae_of_ae_prod hb] with x hx hxb
exact mul_le_mul' (hn x.1 hx x.2)
((moment_mono_ae hxb).trans_eq (hot_moment hq (by linarith)))
_ = _ := by
rw [lintegral_const,← ENNReal.ofReal_mul]
exact add_nonneg
(mul_nonneg (JetEscapedEnvelope.constant_nonneg hs₀ hK hd₀ η α _) (hotConstant_nonneg q))
(div_nonneg (JetEnvelopeGain.momentConstant_nonneg hK α γ) ha.le)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Tensor integrals of the actual mixed prelimit measure -/
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}
theorem mixedPrelimitMeasure_integral (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)
(ρ : Measure (ℝ × JetPrototype.Space)) (f : HotPairPhase → ℝ) :
(∫ z, f z ∂S.mixedPrelimitMeasure n ρ) = ∫ z, S.mixedDensity n z*f z ∂ρ.prod volume := by
rw [mixedPrelimitMeasure,integral_withDensity_eq_integral_toReal_smul]
· simp_rw [ENNReal.toReal_ofReal (S.mixedDensity_nonneg hs₀ hsmax hη hηmax hK hd₀ hq n _),smul_eq_mul]
· exact (S.mixedDensity_measurable hs₀ hsmax hη hηmax hK hd₀ hq n).ennreal_ofReal
· exact ae_of_all _ (fun _ => ENNReal.ofReal_lt_top)
theorem mixedPrelimitMeasure_tensor (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)
(ρ : Measure (ℝ × JetPrototype.Space)) [SFinite ρ]
(θ : ℝ × JetPrototype.Space → ℝ) (ψ χ : Velocity → ℝ)
(hi : Integrable (fun z => S.mixedDensity n z*(θ z.1*(ψ z.2.1*χ z.2.2))) (ρ.prod volume)) :
(∫ z, θ z.1*(ψ z.2.1*χ z.2.2) ∂S.mixedPrelimitMeasure n ρ) =
∫ x, θ x*(S.coldAverage n ψ x*(∫ v, χ v*S.hotDensity n (x,v))) ∂ρ := by
rw [S.mixedPrelimitMeasure_integral hs₀ hsmax hη hηmax hK hd₀ hq n ρ,
integral_prod _ hi]
apply integral_congr_ae
filter_upwards [] with x
have he : (fun p : Velocity × Velocity => S.mixedDensity n (x,p)*(θ x*(ψ p.1*χ p.2))) =
(fun p => θ x*((ψ p.1*S.rescaledColdDensity n (x,p.1))*(χ p.2*S.hotDensity n (x,p.2)))) := by
funext p
dsimp only [mixedDensity]
ring
rw [he,integral_const_mul,Measure.volume_eq_prod,
integral_prod_mul (fun v => ψ v*S.rescaledColdDensity n (x,v))
(fun v => χ v*S.hotDensity n (x,v))]
rfl
theorem mixed_tensor_integrable (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 A R : ℝ} (ha : 0 ≤ a)
{θ : ℝ × JetPrototype.Space → ℝ} {ψ χ : Velocity → ℝ}
(hθ : Measurable θ) (hψ : Measurable ψ) (hχ : Measurable χ)
{B C D : ℝ} (hθB : ∀ x, |θ x| ≤ B) (hψC : ∀ v, |ψ v| ≤ C) (hχD : ∀ v, |χ v| ≤ D) :
Integrable (fun z => S.mixedDensity n z*(θ z.1*(ψ z.2.1*χ z.2.2)))
((coldCylinderVolume a A R).prod volume) := by
have hm : Measurable (fun z : HotPairPhase => θ z.1*(ψ z.2.1*χ z.2.2)) :=
(hθ.comp measurable_fst).mul ((hψ.comp measurable_snd.fst).mul (hχ.comp measurable_snd.snd))
have hb (z : HotPairPhase) : |θ z.1*(ψ z.2.1*χ z.2.2)| ≤ |B| *(|C| *|D|) := by
simp only [abs_mul]
exact mul_le_mul ((hθB _).trans (le_abs_self B))
(mul_le_mul ((hψC _).trans (le_abs_self C)) ((hχD _).trans (le_abs_self D))
(abs_nonneg _) (abs_nonneg _)) (mul_nonneg (abs_nonneg _) (abs_nonneg _)) (abs_nonneg _)
exact ((S.mixedDensity_integrable hs₀ hsmax hη hηmax hK hd₀ hq n ha).bdd_mul
hm.aestronglyMeasurable (ae_of_all _ hb)).congr (ae_of_all _ (fun z => mul_comm _ _))
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Actual mixed measures converge on separated space-time and velocity tests -/
noncomputable section
open MeasureTheory Set 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.mixed_measure_tensor_limit
(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 ≤ 1/4) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {a A R : ℝ}
(ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < E.horizon) (hR : 0 ≤ R)
{B C D : ℝ} {θ : ℝ × JetPrototype.Space → ℝ} {ψ χ : Velocity → ℝ}
(hθ : Measurable θ) (hθB : ∀ x, |θ x| ≤ B)
(hψ : Continuous ψ) (hψC : ∀ v, |ψ v| ≤ C) (hχ : Measurable χ) (hχD : ∀ v, |χ v| ≤ D) :
Tendsto (fun n => ∫ z, θ z.1*(ψ z.2.1*χ z.2.2)
∂S.mixedPrelimitMeasure (E.indices n) (coldCylinderVolume a A R)) atTop
(𝓝 (∫ z, θ z.1*(ψ z.2.1*χ z.2.2)
∂E.toHotLimitExtraction.mixedMeasure ha hK hα hγ (coldCylinderVolume a A R))) := by
let ρ := coldCylinderVolume a A R
have htime : ∀ᵐ x ∂ρ, a ≤ x.1 := (Measure.quasiMeasurePreserving_fst.ae
(ae_restrict_mem measurableSet_Icc)).mono (fun _ hx => hx.1)
let _ : IsFiniteMeasure (E.toHotLimitExtraction.mixedMeasure ha hK hα hγ ρ) :=
E.toHotLimitExtraction.mixedMeasure_finite ha (ha.le.trans haA) hK hα hγ hq₂ ρ
((Measure.quasiMeasurePreserving_fst.ae (ae_restrict_mem measurableSet_Icc)).mono (fun _ hx => hx.2))
have htestm : Measurable (fun z : HotPairPhase => θ z.1*(ψ z.2.1*χ z.2.2)) :=
(hθ.comp measurable_fst).mul ((hψ.measurable.comp measurable_snd.fst).mul (hχ.comp measurable_snd.snd))
have hb (z : HotPairPhase) : |θ z.1*(ψ z.2.1*χ z.2.2)| ≤ |B| *(|C| *|D|) := by
simp only [abs_mul]
exact mul_le_mul ((hθB _).trans (le_abs_self B))
(mul_le_mul ((hψC _).trans (le_abs_self C)) ((hχD _).trans (le_abs_self D))
(abs_nonneg _) (abs_nonneg _)) (mul_nonneg (abs_nonneg _) (abs_nonneg _)) (abs_nonneg _)
have htesti := Integrable.of_bound (μ := E.toHotLimitExtraction.mixedMeasure ha hK hα hγ ρ)
htestm.aestronglyMeasurable _ (ae_of_all _ hb)
have hleft (n) : (∫ z, θ z.1*(ψ z.2.1*χ z.2.2) ∂S.mixedPrelimitMeasure (E.indices n) ρ) =
∫ x, θ x*(S.coldAverage (E.indices n) ψ x*(∫ v, χ v*S.hotDensity (E.indices n) (x,v))) ∂ρ :=
S.mixedPrelimitMeasure_tensor hs₀ hsmax hη hηmax hK hd₀.le hq₂ _ ρ θ ψ χ
(S.mixed_tensor_integrable hs₀ hsmax hη hηmax hK hd₀.le hq₂ _ ha.le hθ hψ.measurable hχ hθB hψC hχD)
have hright : (∫ z, θ z.1*(ψ z.2.1*χ z.2.2)
∂E.toHotLimitExtraction.mixedMeasure ha hK hα hγ ρ) =
∫ x, θ x*((∫ v, ψ v ∂E.toHotLimitExtraction.background (max 0 x.1) x.2)*
(∫ v, χ v*E.toHotLimitExtraction.cappedHot (x,v))) ∂ρ := by
rw [E.toHotLimitExtraction.mixedMeasure_tensor_on_slab ha hK hα hγ ρ htime θ ψ χ htesti]
apply integral_congr_ae
filter_upwards [htime] with x hx
rw [max_eq_right (ha.le.trans hx)]
congr 2
apply integral_congr_ae
exact ae_of_all _ (fun v => mul_comm _ _)
dsimp only [ρ] at hleft hright
simp_rw [hleft]
rw [hright]
exact (E.mixed_average_weak_limit hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ ha haA hA hR hψ hψC hχ hχD).2.2 θ hθ ⟨B,hθB⟩
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Actual mixed measures converge for compact continuous velocity-pair tests -/
noncomputable section
open MeasureTheory Set 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.mixed_measure_compact_limit
(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 ≤ 1/4) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {a A R : ℝ}
(ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < E.horizon) (hR : 0 ≤ R)
{B : ℝ} {θ : ℝ × JetPrototype.Space → ℝ} (hθ : Measurable θ) (hθB : ∀ x, |θ x| ≤ B)
(k : C(Velocity × Velocity, ℝ)) (hk : HasCompactSupport k) :
Tendsto (fun n => ∫ z, θ z.1*k z.2
∂S.mixedPrelimitMeasure (E.indices n) (coldCylinderVolume a A R)) atTop
(𝓝 (∫ z, θ z.1*k z.2
∂E.toHotLimitExtraction.mixedMeasure ha hK hα hγ (coldCylinderVolume a A R))) := by
let ρ := coldCylinderVolume a A R
let μ : ℕ → Measure HotPairPhase := fun n => S.mixedPrelimitMeasure (E.indices n) ρ
let ν := E.toHotLimitExtraction.mixedMeasure ha hK hα hγ ρ
let _ (n) : IsFiniteMeasure (μ n) := S.mixedPrelimitMeasure_finite
hs₀ hsmax hη hηmax hK hd₀.le hq₂ _ ha.le
let _ : IsFiniteMeasure ν := E.toHotLimitExtraction.mixedMeasure_finite
ha (ha.le.trans haA) hK hα hγ hq₂ ρ
((Measure.quasiMeasurePreserving_fst.ae (ae_restrict_mem measurableSet_Icc)).mono (fun _ hx => hx.2))
have hm : Tendsto (fun n => (μ n).real univ) atTop (𝓝 (ν.real univ)) := by
have ht := E.mixed_measure_tensor_limit hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ ha haA hA hR
(θ := fun _ => 1) (ψ := fun _ => 1) (χ := fun _ => 1)
measurable_const (B := 1) (fun _ => by norm_num) continuous_const (C := 1)
(fun _ => by norm_num) measurable_const (D := 1) (fun _ => by norm_num)
simpa only [one_mul,integral_const,smul_eq_mul,mul_one,μ,ν,ρ] using ht
have hμ : ∀ᶠ n in atTop, (μ n).real univ ≤ ν.real univ+1 :=
(hm.eventually (gt_mem_nhds (lt_add_one (ν.real univ)))).mono (fun _ hn => hn.le)
apply Compactness.weighted_supported_integral_tendsto_of_tensor_tests
hθ hθB (C := ν.real univ+1) (by positivity) hμ _ k hk
intro f g hf hg
obtain ⟨C,hC⟩ := f.continuous.bounded_above_of_compact_support hf
obtain ⟨D,hD⟩ := g.continuous.bounded_above_of_compact_support hg
exact E.mixed_measure_tensor_limit hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ ha haA hA hR hθ hθB f.continuous hC g.continuous.measurable hD
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Actual mixed-measure convergence for the full hard-sphere growth class -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.VelocityMoment
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.mixed_measure_linear_growth_limit
(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 ≤ 1/4) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {a A R : ℝ}
(ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < E.horizon) (hR : 0 ≤ R)
{B : ℝ} {θ : ℝ × JetPrototype.Space → ℝ} (hθ : Measurable θ) (hθB : ∀ x, |θ x| ≤ B)
(k : C(Velocity × Velocity, ℝ)) {L : ℝ} (hL : 0 ≤ L)
(hk : ∀ p, |k p| ≤ L*(1+‖p.1‖+‖p.2‖)) :
Tendsto (fun n => ∫ z, θ z.1*k z.2
∂S.mixedPrelimitMeasure (E.indices n) (coldCylinderVolume a A R)) atTop
(𝓝 (∫ z, θ z.1*k z.2
∂E.toHotLimitExtraction.mixedMeasure ha hK hα hγ (coldCylinderVolume a A R))) := by
let ρ := coldCylinderVolume a A R
let C : ℝ≥0∞ := ENNReal.ofReal ((escapedConstant s₀ η K α d₀*hotConstant q+
JetEnvelopeGain.momentConstant K α γ/a)*((A+1)*hotConstant q))*ρ univ
let D : ℝ≥0∞ := ENNReal.ofReal ((2*((1/4)*((K*max 1 (α*γ)⁻¹)/a))*
Real.exp ((1+α)^2/2))*((A+1)*hotConstant q))*ρ univ
have hC : C ≠ ⊤ := ENNReal.mul_ne_top ENNReal.ofReal_ne_top (measure_ne_top ρ univ)
have hD : D ≠ ⊤ := ENNReal.mul_ne_top ENNReal.ofReal_ne_top (measure_ne_top ρ univ)
have hm := S.eventually_mixedPrelimitMeasure_gaussian_bound hs₀ hsmax hη hηmax hK hα
(hαmax.trans (by norm_num)) hγ hd₀ hd₀max hsmall hq₂ E.indices_strict E.horizon_limit (R := R) ha haA hA
have hn := E.toHotLimitExtraction.mixedMeasure_gaussian_bound ha (ha.le.trans haA)
hK hα hγ hq₂ ρ
((Measure.quasiMeasurePreserving_fst.ae (ae_restrict_mem measurableSet_Icc)).mono
(fun _ hx => hx.2))
apply Compactness.gaussian_weighted_integral_tendsto
(C := C.toReal) (D := D.toReal) ENNReal.toReal_nonneg ENNReal.toReal_nonneg
(by simpa only [ENNReal.ofReal_toReal hC] using hm)
(by simpa only [ENNReal.ofReal_toReal hD] using hn) hθ hθB _ k hL hk
intro g hg
exact E.mixed_measure_compact_limit hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ ha haA hA hR hθ hθB g hg
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Removal of the actual finite-cap relative-velocity cutoff -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.VelocityMoment
open BoltzmannNonuniqueness.CollisionCompactness
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}
def collisionCutoff (_S : AttainedCapSequence F) (n : ℕ) : ℝ := F.indices n+1
theorem collisionCutoff_tendsto (S : AttainedCapSequence F) :
Tendsto S.collisionCutoff atTop atTop := by
exact tendsto_atTop_add_const_right atTop (1 : ℝ)
(tendsto_natCast_atTop_atTop.comp F.indices_tendsto)
theorem HotPairExtraction.mixed_relative_cutoff_limit
(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 ≤ 1/4) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {a A R : ℝ}
(ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < E.horizon) (hR : 0 ≤ R)
{B : ℝ} {θ : ℝ × JetPrototype.Space → ℝ} (hθ : Measurable θ) (hθB : ∀ x, |θ x| ≤ B)
(k : C(Velocity × Velocity, ℝ)) {L : ℝ} (hL : 0 ≤ L)
(hk : ∀ p, |k p| ≤ L*(1+‖p.1‖+‖p.2‖)) :
Tendsto (fun n => ∫ z, θ z.1*relativeCutoff (S.collisionCutoff (E.indices n)) k z.2
∂S.mixedPrelimitMeasure (E.indices n) (coldCylinderVolume a A R)) atTop
(𝓝 (∫ z, θ z.1*k z.2
∂E.toHotLimitExtraction.mixedMeasure ha hK hα hγ (coldCylinderVolume a A R))) := by
let ρ := coldCylinderVolume a A R
let C : ℝ≥0∞ := ENNReal.ofReal ((escapedConstant s₀ η K α d₀*hotConstant q+
JetEnvelopeGain.momentConstant K α γ/a)*((A+1)*hotConstant q))*ρ univ
have hC : C ≠ ⊤ := ENNReal.mul_ne_top ENNReal.ofReal_ne_top (measure_ne_top ρ univ)
have hm := S.eventually_mixedPrelimitMeasure_gaussian_bound hs₀ hsmax hη hηmax hK hα
(hαmax.trans (by norm_num)) hγ hd₀ hd₀max hsmall hq₂ E.indices_strict E.horizon_limit
(R := R) ha haA hA
apply relative_cutoff_integral_tendsto (M := C.toReal) ENNReal.toReal_nonneg
(by simpa only [ENNReal.ofReal_toReal hC] using hm)
(S.collisionCutoff_tendsto.comp E.indices_strict.tendsto_atTop) hθ hθB
k.continuous.measurable hL hk
exact E.mixed_measure_linear_growth_limit hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ ha haA hA hR hθ hθB k hL hk
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Gain and loss tests pass to the actual cold--hot limit without velocity cutoffs -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.CollisionCompactness
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.mixed_incoming_collision_limit
(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 ≤ 1/4) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {a A R : ℝ}
(ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < E.horizon) (hR : 0 ≤ R)
{B : ℝ} {θ : ℝ × JetPrototype.Space → ℝ} (hθ : Measurable θ) (hθB : ∀ x, |θ x| ≤ B)
{φ : Velocity → ℝ} (hφ : Continuous φ) {C : ℝ} (hφC : ∀ v, |φ v| ≤ C) :
Tendsto (fun n => ∫ z, θ z.1*incomingGainTest φ z.2
∂S.mixedPrelimitMeasure (E.indices n) (coldCylinderVolume a A R)) atTop
(𝓝 (∫ z, θ z.1*incomingGainTest φ z.2
∂E.toHotLimitExtraction.mixedMeasure ha hK hα hγ (coldCylinderVolume a A R))) ∧
Tendsto (fun n => ∫ z, θ z.1*incomingLossTest φ z.2
∂S.mixedPrelimitMeasure (E.indices n) (coldCylinderVolume a A R)) atTop
(𝓝 (∫ z, θ z.1*incomingLossTest φ z.2
∂E.toHotLimitExtraction.mixedMeasure ha hK hα hγ (coldCylinderVolume a A R))) := by
have hC : 0 ≤ C := (abs_nonneg (φ 0)).trans (hφC 0)
have hL : 0 ≤ 2*Real.pi*C := mul_nonneg (by positivity) hC
constructor
· exact E.mixed_measure_linear_growth_limit hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ ha haA hA hR hθ hθB
⟨incomingGainTest φ,incomingGainTest_continuous hφ⟩ hL
(fun p => (incomingTests_linear_growth hφC p).1)
· exact E.mixed_measure_linear_growth_limit hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ ha haA hA hR hθ hθB
⟨incomingLossTest φ,incomingLossTest_continuous hφ⟩ hL
(fun p => (incomingTests_linear_growth hφC p).2)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Actual cold--hot collision rates are integrable on every positive-time cylinder -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.CollisionCompactness
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
theorem eventually_mixedPreRate_integrable (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)
(hq : 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 : ℝ} (ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < U) :
∀ᶠ n in atTop, ∀ b : ℝ,
Integrable (mixedPreRate b (S.rescaledColdDensity (κ n)) (S.hotDensity (κ n)))
(((coldCylinderVolume a A R).prod (volume : Measure (Velocity × Velocity))).prod sphereArea) := by
filter_upwards [S.eventually_mixedPrelimitMeasure_gaussian_bound hs₀ hsmax hη hηmax hK hα
hαmax hγ hd₀ hd₀max hsmall hq hκ hU (R := R) ha haA hA] with n hn
have hm := hn.trans_lt (ENNReal.mul_lt_top ENNReal.ofReal_lt_top
(measure_lt_top (coldCylinderVolume a A R) Set.univ))
have hc := S.rescaledColdDensity_measurable hs₀ hsmax hη hηmax hK hd₀.le hq (κ n)
have hh := S.hotDensity_measurable hs₀ hsmax hη hηmax hK hd₀.le hq (κ n)
have hcn := fun p => (S.rescaledColdDensity_bounds hs₀ hsmax hη hηmax hK hd₀.le hq (κ n) p).1
have hhn := S.hotDensity_nonneg hs₀ hsmax hη hηmax hK hd₀.le hq (κ n)
have hp := mixed_pair_rate_integrable_of_gaussian hc hh hcn hhn hm
exact fun b => mixedPreRate_integrable hc hh hcn hhn hp b
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # The physical hot collision equation for the actual finite cap solution -/
noncomputable section
open MeasureTheory
open BoltzmannNonuniqueness.CollisionCompactness BoltzmannNonuniqueness.WeightedLocal
namespace BoltzmannNonuniqueness.JetCopyDatum
def CapApproximation.physicalCold {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N) : (ℝ × JetPrototype.Space) × Velocity → ℝ :=
HotRepresentative.density q (GaussianLocal.state F.coldTotal)
def CapApproximation.physicalHot {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N) : (ℝ × JetPrototype.Space) × Velocity → ℝ :=
HotRepresentative.density q (GaussianLocal.state F.hot)
theorem CapApproximation.physical_hot_collision {s₀ η K α γ d₀ q T : ℝ} {N : ℕ}
(F : CapApproximation s₀ η K α γ d₀ q T N)
(hs₀ : 0 < s₀) (hsmax : s₀ ≤ 1/8) (hη : 0 < η) (hηmax : η ≤ Real.log 2)
(hK : 0 ≤ K) (hd₀ : 0 ≤ d₀) (hq : q < 2) (hT : 0 ≤ T)
(z : (ℝ × JetPrototype.Space) × Velocity) (hz : z.2 ∈ HotRepresentative.good q) :
VelocityWeight.H q z.2*F.hotNetSource (z.1.1,(z.1.2,z.2)) =
2*mixedGainDensity (N+1) F.physicalCold F.physicalHot z-
F.physicalHot z*KineticCollisionNullSets.frequency (N+1) F.physicalCold z+
collisionSource (N+1) F.physicalHot z+
VelocityWeight.H q z.2*F.coldSource (z.1.1,(z.1.2,z.2)) := by
have hc := F.cold_properties hs₀ hsmax hη hηmax hK hd₀ hq hT
have hcb (i : JetLattice.Label) (p : (ℝ × JetPrototype.Space) × Velocity) :
0 ≤ GaussianLocal.state (F.cold i) p ∧
GaussianLocal.state (F.cold i) p ≤ 2*F.amplitude := by
refine ⟨hc.2.1 i _,?_⟩
have hs := hc.2.2.1 {i} (p.1.1,(p.1.2,p.2))
simp only [Finset.sum_singleton] at hs
exact hs.trans (F.solution.value_bounds _).2
exact HotRepresentative.physical_hot_collision_decomposition hq (by positivity)
(WeightedLocalControl.damping q (N+1) F.amplitude)
(fun i => GaussianLocal.measurable_state (hc.1 i))
(GaussianLocal.measurable_state F.solution.measurable_value) hcb
(fun p => F.solution.value_bounds (p.1.1,(p.1.2,p.2)))
(fun s p => hc.2.2.1 s (p.1.1,(p.1.2,p.2))) z hz
end BoltzmannNonuniqueness.JetCopyDatum
end
end
section
/-! # Positive finite measures for the physical cap approximants' collision terms -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.CollisionCompactness
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
def physicalGainMeasure (S : AttainedCapSequence F) (a A R : ℝ) (n : ℕ) :
Measure HotKineticPhase :=
mixedGainMeasure (coldCylinderVolume a A R) (S.collisionCutoff n)
(S.rescaledColdDensity n) (S.hotDensity n)
def physicalLossMeasure (S : AttainedCapSequence F) (a A R : ℝ) (n : ℕ) :
Measure HotKineticPhase :=
mixedLossMeasure (coldCylinderVolume a A R) (S.collisionCutoff n)
(S.rescaledColdDensity n) (S.hotDensity n)
theorem eventually_physicalCollisionMeasures_finite (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)
(hq : 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 : ℝ} (ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < U) :
∀ᶠ n in atTop, IsFiniteMeasure (S.physicalGainMeasure a A R (κ n)) ∧
IsFiniteMeasure (S.physicalLossMeasure a A R (κ n)) := by
filter_upwards [S.eventually_mixedPreRate_integrable hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq hκ hU (R := R) ha haA hA] with n hn
have hc := fun p => (S.rescaledColdDensity_bounds hs₀ hsmax hη hηmax hK hd₀.le hq (κ n) p).1
have hh := S.hotDensity_nonneg hs₀ hsmax hη hηmax hK hd₀.le hq (κ n)
exact ⟨mixedGainMeasure_finite hc hh (hn _),mixedLossMeasure_finite hc hh (hn _)⟩
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Weak limit of the actual hot density times the cold collision frequency -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.CollisionCompactness
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.mixed_physical_loss_limit
(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 ≤ 1/4) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {a A R : ℝ}
(ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < E.horizon) (hR : 0 ≤ R)
{B : ℝ} {θ : ℝ × JetPrototype.Space → ℝ} (hθ : Measurable θ) (hθB : ∀ x, |θ x| ≤ B)
{φ : Velocity → ℝ} (hφ : Continuous φ) {C : ℝ} (hφC : ∀ v, |φ v| ≤ C) :
Tendsto (fun n => ∫ p, (θ p.1*φ p.2)*
(S.hotDensity (E.indices n) p*KineticCollisionNullSets.frequency
(S.collisionCutoff (E.indices n)) (S.rescaledColdDensity (E.indices n)) p)
∂(coldCylinderVolume a A R).prod volume) atTop
(𝓝 (∫ z, θ z.1*incomingLossTest φ z.2
∂E.toHotLimitExtraction.mixedMeasure ha hK hα hγ (coldCylinderVolume a A R))) := by
have hC : 0 ≤ C := (abs_nonneg (φ 0)).trans (hφC 0)
have hB : 0 ≤ B := (abs_nonneg (θ (0,0))).trans (hθB (0,0))
have hψ : Measurable (fun p : (ℝ × JetPrototype.Space) × Velocity => θ p.1*φ p.2) :=
(hθ.comp measurable_fst).mul (hφ.measurable.comp measurable_snd)
have hψB (p : (ℝ × JetPrototype.Space) × Velocity) : |θ p.1*φ p.2| ≤ B*C := by
rw [abs_mul]
exact mul_le_mul (hθB _) (hφC _) (abs_nonneg _) hB
have hc := E.mixed_relative_cutoff_limit hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ ha haA hA hR hθ hθB
⟨incomingLossTest φ,incomingLossTest_continuous hφ⟩
(mul_nonneg (by positivity : 0 ≤ 2*Real.pi) hC)
(fun p => (incomingTests_linear_growth hφC p).2)
apply hc.congr'
filter_upwards [S.eventually_mixedPreRate_integrable hs₀ hsmax hη hηmax hK hα
(hαmax.trans (by norm_num)) hγ hd₀ hd₀max hsmall hq₂ E.indices_strict E.horizon_limit
(R := R) ha haA hA] with n hn
have hr := hn (S.collisionCutoff (E.indices n))
have hsp := mixedPreRate_swapped_integrable hr
have hi : Integrable (fun z => (θ z.1.1*φ z.1.2.1)*
mixedPreRate (S.collisionCutoff (E.indices n)) (S.hotDensity (E.indices n))
(S.rescaledColdDensity (E.indices n)) z)
(((coldCylinderVolume a A R).prod (volume : Measure (Velocity × Velocity))).prod sphereArea) := by
apply hsp.bdd_mul
(hψ.comp (measurable_fst.fst.prodMk measurable_fst.snd.fst)).aestronglyMeasurable
exact ae_of_all _ (fun z => by
change ‖θ z.1.1*φ z.1.2.1‖ ≤ B*C
simpa only [Real.norm_eq_abs] using hψB (z.1.1,z.1.2.1))
have he := mixedLoss_test_incoming (S.collisionCutoff (E.indices n))
(S.rescaledColdDensity (E.indices n)) (S.hotDensity (E.indices n)) θ φ hi
have hphysical : (∫ p, (θ p.1*φ p.2)*mixedLossDensity (S.collisionCutoff (E.indices n))
(S.rescaledColdDensity (E.indices n)) (S.hotDensity (E.indices n)) p
∂(coldCylinderVolume a A R).prod volume) =
∫ p, (θ p.1*φ p.2)*(S.hotDensity (E.indices n) p*KineticCollisionNullSets.frequency
(S.collisionCutoff (E.indices n)) (S.rescaledColdDensity (E.indices n)) p)
∂(coldCylinderVolume a A R).prod volume := by
apply integral_congr_ae
filter_upwards [mixed_loss_ae_eq_frequency hr] with p hp
rw [hp]
rw [← hphysical,he,S.mixedPrelimitMeasure_integral hs₀ hsmax hη hηmax hK hd₀.le hq₂]
apply integral_congr_ae
exact ae_of_all _ (fun z => by
dsimp only [mixedDensity,relativeCutoff]
simp only [ContinuousMap.coe_mk]
ring)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Weak limit of the actual symmetric mixed gain density -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.CollisionCompactness
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.mixed_physical_gain_limit
(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 ≤ 1/4) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {a A R : ℝ}
(ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < E.horizon) (hR : 0 ≤ R)
{B : ℝ} {θ : ℝ × JetPrototype.Space → ℝ} (hθ : Measurable θ) (hθB : ∀ x, |θ x| ≤ B)
{φ : Velocity → ℝ} (hφ : Continuous φ) {C : ℝ} (hφC : ∀ v, |φ v| ≤ C) :
Tendsto (fun n => ∫ p, (θ p.1*φ p.2)*
mixedGainDensity (S.collisionCutoff (E.indices n))
(S.rescaledColdDensity (E.indices n)) (S.hotDensity (E.indices n)) p
∂(coldCylinderVolume a A R).prod volume) atTop
(𝓝 (∫ z, θ z.1*incomingGainTest φ z.2
∂E.toHotLimitExtraction.mixedMeasure ha hK hα hγ (coldCylinderVolume a A R))) := by
have hC : 0 ≤ C := (abs_nonneg (φ 0)).trans (hφC 0)
have hB : 0 ≤ B := (abs_nonneg (θ (0,0))).trans (hθB (0,0))
have hψ : Measurable (fun p : (ℝ × JetPrototype.Space) × Velocity => θ p.1*φ p.2) :=
(hθ.comp measurable_fst).mul (hφ.measurable.comp measurable_snd)
have hψB (p : (ℝ × JetPrototype.Space) × Velocity) : |θ p.1*φ p.2| ≤ B*C := by
rw [abs_mul]
exact mul_le_mul (hθB _) (hφC _) (abs_nonneg _) hB
have hc := E.mixed_relative_cutoff_limit hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax hγ
hd₀ hd₀max hsmall hq₁ hq₂ ha haA hA hR hθ hθB
⟨incomingGainTest φ,incomingGainTest_continuous hφ⟩
(mul_nonneg (by positivity : 0 ≤ 2*Real.pi) hC)
(fun p => (incomingTests_linear_growth hφC p).1)
apply hc.congr'
filter_upwards [S.eventually_mixedPreRate_integrable hs₀ hsmax hη hηmax hK hα
(hαmax.trans (by norm_num)) hγ hd₀ hd₀max hsmall hq₂ E.indices_strict E.horizon_limit
(R := R) ha haA hA] with n hn
have hr := hn (S.collisionCutoff (E.indices n))
have he := mixedGain_test_incoming (S.collisionCutoff (E.indices n))
(S.rescaledColdDensity (E.indices n)) (S.hotDensity (E.indices n)) θ φ
(mixedPostRate_test_integrable hr hψ hψB)
(mixedPostRate_test_integrable (mixedPreRate_swapped_integrable hr) hψ hψB)
(mixedPreRate_sum_test_integrable hr hψ hψB)
rw [he,S.mixedPrelimitMeasure_integral hs₀ hsmax hη hηmax hK hd₀.le hq₂]
apply integral_congr_ae
exact ae_of_all _ (fun z => by
dsimp only [mixedDensity,relativeCutoff]
simp only [ContinuousMap.coe_mk]
ring)
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Exact mixed collision equation under the attained cap dilation -/
noncomputable section
open MeasureTheory
open BoltzmannNonuniqueness.VelocityWeight BoltzmannNonuniqueness.CollisionCompactness
namespace BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
variable {s₀ η K α γ d₀ q : ℝ} {F : ShrinkingCapFamily s₀ η K α γ d₀ q}
def collisionDilation (S : AttainedCapSequence F) (n : ℕ)
(x : ℝ × JetPrototype.Space) : ℝ × JetPrototype.Space :=
(S.radius n*x.1,S.radius n • x.2)
theorem rescaledColdDensity_eq_physical (S : AttainedCapSequence F) (n : ℕ) :
S.rescaledColdDensity n = fun z => S.radius n*
(F.approximation n).physicalCold (S.collisionDilation n z.1,z.2) := by
funext z
unfold rescaledColdDensity CapApproximation.physicalCold HotRepresentative.density
GaussianLocal.state collisionDilation
ring
theorem physicalHotDensity_eq_physical (S : AttainedCapSequence F) (n : ℕ) :
S.physicalHotDensity n = fun z => (S.radius n)⁻¹*
(F.approximation n).physicalHot (S.collisionDilation n z.1,z.2) := by
funext z
unfold physicalHotDensity rescaledHot CapApproximation.physicalHot HotRepresentative.density
GaussianLocal.state collisionDilation
ring
theorem rescaled_hot_collision (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 : HotKineticPhase) (hz : z.2 ∈ HotRepresentative.good q) :
H q z.2*S.rescaledHotSource n (z.1.1,(z.1.2,z.2)) =
2*mixedGainDensity (F.indices n+1) (S.rescaledColdDensity n) (S.physicalHotDensity n) z-
S.physicalHotDensity n z*KineticCollisionNullSets.frequency (F.indices n+1) (S.rescaledColdDensity n) z+
(S.radius n)^2*collisionSource (F.indices n+1) (S.physicalHotDensity n) z+
H q z.2*S.rescaledColdSource n (z.1.1,(z.1.2,z.2)) := by
have hs :
2*mixedGainDensity (F.indices n+1) (S.rescaledColdDensity n) (S.physicalHotDensity n) z-
S.physicalHotDensity n z*KineticCollisionNullSets.frequency (F.indices n+1) (S.rescaledColdDensity n) z+
(S.radius n)^2*collisionSource (F.indices n+1) (S.physicalHotDensity n) z =
2*mixedGainDensity (F.indices n+1) (F.approximation n).physicalCold (F.approximation n).physicalHot
(S.collisionDilation n z.1,z.2)-
(F.approximation n).physicalHot (S.collisionDilation n z.1,z.2)*
KineticCollisionNullSets.frequency (F.indices n+1) (F.approximation n).physicalCold
(S.collisionDilation n z.1,z.2)+
collisionSource (F.indices n+1) (F.approximation n).physicalHot (S.collisionDilation n z.1,z.2) := by
rw [S.rescaledColdDensity_eq_physical,S.physicalHotDensity_eq_physical]
simpa only [mixedGain_base_comp,cutoffFrequency_base_comp,collisionSource_base_comp] using
mixed_source_rescale (F.indices n+1) (S.radius n) (S.radius_pos hs₀ n).ne'
(fun p => (F.approximation n).physicalCold (S.collisionDilation n p.1,p.2))
(fun p => (F.approximation n).physicalHot (S.collisionDilation n p.1,p.2)) z
rw [hs]
exact (F.approximation n).physical_hot_collision hs₀ hsmax hη hηmax hK hd₀ hq
(shrinkingHorizon_pos F.horizonScale_pos n).le (S.collisionDilation n z.1,z.2) hz
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
section
/-! # Separated-test convergence of the actual physical loss measures -/
noncomputable section
open MeasureTheory Set Filter
open scoped ENNReal Topology
open BoltzmannNonuniqueness.CollisionCompactness
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.loss_measure_separated_limit
(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 ≤ 1/4) (hγ : 0 < γ)
(hd₀ : 0 < d₀) (hd₀max : d₀ ≤ 1)
(hsmall : JetComparisonCoefficient.coefficient K*d₀*s₀^9 ≤ 1)
(hq₁ : 1 < q) (hq₂ : q < 2) {a A R : ℝ}
(ha : 0 < a) (haA : a ≤ A) (hA : ENNReal.ofReal A < E.horizon) (hR : 0 ≤ R)
{B : ℝ} {θ : ℝ × JetPrototype.Space → ℝ} (hθ : Measurable θ) (hθB : ∀ x, |θ x| ≤ B)
{φ : Velocity → ℝ} (hφ : Continuous φ) {C : ℝ} (hφC : ∀ v, |φ v| ≤ C) :
Tendsto (fun n => ∫ z, θ z.1*φ z.2 ∂S.physicalLossMeasure a A R (E.indices n)) atTop
(𝓝 (∫ z, θ z.1*φ z.2 ∂incomingLossMeasure
(E.toHotLimitExtraction.mixedMeasure ha hK hα hγ (coldCylinderVolume a A R)))) := by
let μ := E.toHotLimitExtraction.mixedMeasure ha hK hα hγ (coldCylinderVolume a A R)
let _ : SFinite μ := by dsimp [μ,HotLimitExtraction.mixedMeasure]; infer_instance
have hi : Integrable incomingRate μ :=
E.toHotLimitExtraction.incomingRate_integrable ha (ha.le.trans haA) hK hα hγ hq₂
have hB : 0 ≤ B := (abs_nonneg (θ (0,0))).trans (hθB _)
have ht := E.mixed_physical_loss_limit hcarleman hGLPS hs₀ hsmax hη hηmax hK hα hαmax
hγ hd₀ hd₀max hsmall hq₁ hq₂ ha haA hA hR hθ hθB hφ hφC
rw [← incomingLossMeasure_separated hi hθ hB hθB hφ.measurable hφC] at ht
apply ht.congr'
filter_upwards [S.eventually_mixedPreRate_integrable hs₀ hsmax hη hηmax hK hα
(hαmax.trans (by norm_num)) hγ hd₀ hd₀max hsmall hq₂ E.indices_strict E.horizon_limit
(R := R) ha haA hA] with n hn
have hc := fun p => (S.rescaledColdDensity_bounds hs₀ hsmax hη hηmax hK hd₀.le hq₂ (E.indices n) p).1
have hh := S.hotDensity_nonneg hs₀ hsmax hη hηmax hK hd₀.le hq₂ (E.indices n)
dsimp only [physicalLossMeasure]
rw [mixedLossMeasure_integral hc hh (hn (S.collisionCutoff (E.indices n))) (fun z => θ z.1*φ z.2)]
apply integral_congr_ae
filter_upwards [mixed_loss_ae_eq_frequency (hn (S.collisionCutoff (E.indices n)))] with z hz
rw [hz]
end BoltzmannNonuniqueness.JetCopyDatum.AttainedCapSequence
end
end
end OAI