roseking's picture
Add lean source and binary files (part 85)
f18e7de verified
Raw History Blame Contribute Delete
24.5 kB
import OAI.MathematicalPhysics.Boltzmann.Approximation.PositiveIntegralPasting
import OAI.MathematicalPhysics.Boltzmann.Branching.AttenuationGap
import OAI.MathematicalPhysics.Boltzmann.Branching.DampedBranchingBlocks
import OAI.MathematicalPhysics.Boltzmann.Compactness.PeriodicMildApproximation
import OAI.MathematicalPhysics.Boltzmann.Jets.SpatialDilationAE
namespace OAI
section
/-! # The weak characteristic equation of the constructed mild states -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.WeightedLocal
namespace BoltzmannNonuniqueness.PositiveIntegral
theorem value_along_flight {T t : ℝ} (ht : t ∈ Icc 0 T) (L : ℝ)
(f₀ : JetPrototype.Phase → ℝ) (g : ℝ × JetPrototype.Phase → ℝ)
(p : JetPrototype.Phase) :
value T L JetBarrier.flight f₀ g (t,JetBarrier.flight t p) =
TransportPrimitive.damped L (f₀ p) (fun r => g (r,JetBarrier.flight r p)) t := by
rw [TransportPrimitive.damped_eq]
unfold value
rw [GaussianLocal.time_eq ht,JetFreeTransport.neg_flight]
congr 1
apply intervalIntegral.integral_congr
intro r _
dsimp only
rw [JetFreeTransport.flight_add,sub_add_cancel]
/-- The integral form of the transport equation, along almost every characteristic.
The source is only required to be measurable and bounded. -/
theorem weak_characteristic {T L S : ℝ} (hT : 0 ≤ T)
{f₀ : JetPrototype.Phase → ℝ} (hf₀ : Measurable f₀)
{F g : ℝ × JetPrototype.Phase → ℝ} (hFm : Measurable F) (hgm : Measurable g)
(hg : ∀ z, |g z| ≤ S)
(hmild : ∀ t ∈ Icc 0 T, (fun p => F (t,p)) =ᵐ[FlightMeasure.phaseVolume]
(fun p => value T L JetBarrier.flight f₀ g (t,p)))
{ψ ψ' : ℝ → ℝ} (hψ : ContinuousOn ψ (Icc 0 T))
(hψ' : ContinuousOn ψ' (Icc 0 T))
(hdψ : ∀ t ∈ Icc 0 T, HasDerivAt ψ (ψ' t) t) :
∀ᵐ p ∂FlightMeasure.phaseVolume,
(∫ t in 0..T, ψ' t*F (t,JetBarrier.flight t p) +
ψ t*(g (t,JetBarrier.flight t p)-L*F (t,JetBarrier.flight t p))) =
ψ T*F (T,JetBarrier.flight T p)-ψ 0*f₀ p := by
let A : ℝ × JetPrototype.Phase → ℝ := fun z => F (z.1,JetBarrier.flight z.1 z.2)
let B : ℝ × JetPrototype.Phase → ℝ := fun z =>
value T L JetBarrier.flight f₀ g (z.1,JetBarrier.flight z.1 z.2)
have hflow : Measurable (fun z : ℝ × JetPrototype.Phase =>
(z.1,JetBarrier.flight z.1 z.2)) :=
measurable_fst.prodMk GaussianLocal.measurable_flight
have hAm : Measurable A := hFm.comp hflow
have hBm : Measurable B :=
(measurable_value hT GaussianLocal.measurable_flight hf₀ hgm).comp hflow
have hslice (t : ℝ) (ht : t ∈ Icc 0 T) :
(fun p => A (t,p)) =ᵐ[FlightMeasure.phaseVolume] (fun p => B (t,p)) :=
(FlightMeasure.flight_measurePreserving t).quasiMeasurePreserving.ae (hmild t ht)
have hall : A =ᵐ[(volume.restrict (Icc 0 T)).prod FlightMeasure.phaseVolume] B := by
apply (Measure.ae_prod_iff_ae_ae (measurableSet_eq_fun hAm hBm)).mpr
filter_upwards [ae_restrict_mem measurableSet_Icc] with t ht
exact hslice t ht
have hp := Measure.ae_ae_of_ae_prod
((Measure.measurePreserving_swap (μ := FlightMeasure.phaseVolume)
(ν := volume.restrict (Icc 0 T))).quasiMeasurePreserving.ae hall)
filter_upwards [hp,hslice T ⟨hT,le_rfl⟩] with p hpe hpend
have hgi : IntervalIntegrable (fun t => g (t,JetBarrier.flight t p)) volume 0 T := by
apply (intervalIntegrable_const (c := S)).mono_fun'
· exact (hgm.comp (measurable_id.prodMk
(GaussianLocal.measurable_flight.comp (measurable_id.prodMk measurable_const)))).aestronglyMeasurable
· exact ae_of_all _ (fun t => by simpa only [Real.norm_eq_abs] using hg (t,JetBarrier.flight t p))
have H := TransportPrimitive.damped_integration_by_parts hT hgi hψ hψ' hdψ
(L := L) (c := f₀ p)
have he : (fun t => F (t,JetBarrier.flight t p)) =ᵐ[volume.restrict (Icc 0 T)]
(fun t => TransportPrimitive.damped L (f₀ p) (fun r => g (r,JetBarrier.flight r p)) t) := by
filter_upwards [hpe,ae_restrict_mem measurableSet_Icc] with t ht htm
exact ht.trans (value_along_flight htm L f₀ g p)
have hboundary : F (T,JetBarrier.flight T p) =
TransportPrimitive.damped L (f₀ p) (fun r => g (r,JetBarrier.flight r p)) T :=
hpend.trans (value_along_flight ⟨hT,le_rfl⟩ L f₀ g p)
rw [hboundary]
rw [← H]
rw [intervalIntegral.integral_of_le hT,intervalIntegral.integral_of_le hT]
apply integral_congr_ae
have he' := ae_restrict_of_ae_restrict_of_subset Ioc_subset_Icc_self he
filter_upwards [he'] with t ht
rw [ht]
end BoltzmannNonuniqueness.PositiveIntegral
end
end
section
/-! # Difference estimate for the positive mild iteration along a free path -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.JetPrototype
namespace BoltzmannNonuniqueness.MildStability
def value (f₀ : ℝ) (ν : ℝ → JetPrototype.Phase → ℝ) (g : ℝ → ℝ)
(t : ℝ) (p : JetPrototype.Phase) : ℝ :=
f₀ * JetPicardComparison.attenuation ν 0 t p +
∫ r in 0..t, JetPicardComparison.attenuation ν r t p * g r
private theorem product_difference {a b c d E M F : ℝ}
(ha : |a| ≤ 1) (hcd : |c - d| ≤ E) (hd : |d| ≤ M) (hab : |a - b| ≤ F)
(hF : 0 ≤ F) : |a * c - b * d| ≤ E + F * M := by
calc
_ = |a * (c - d) + (a - b) * d| := by congr 1; ring
_ ≤ |a| * |c - d| + |a - b| * |d| := by simpa only [abs_mul] using abs_add_le (a * (c - d)) ((a - b) * d)
_ ≤ 1 * E + F * M := add_le_add
(mul_le_mul ha hcd (abs_nonneg _) (by norm_num))
(mul_le_mul hab hd (abs_nonneg _) hF)
_ = _ := by ring
theorem difference {ν μ : ℝ → JetPrototype.Phase → ℝ} {g h : ℝ → ℝ}
{f₀ k₀ I A E M D t : ℝ} (ht : 0 ≤ t) (hD : 0 ≤ D)
(p : JetPrototype.Phase)
(hν : ∀ r ∈ Icc 0 t, 0 ≤ ν r (JetBarrier.flight r p))
(hμ : ∀ r ∈ Icc 0 t, 0 ≤ μ r (JetBarrier.flight r p))
(hνi : IntervalIntegrable (fun r => ν r (JetBarrier.flight r p)) volume 0 t)
(hμi : IntervalIntegrable (fun r => μ r (JetBarrier.flight r p)) volume 0 t)
(hνμ : ∀ r ∈ Icc 0 t, |ν r (JetBarrier.flight r p) - μ r (JetBarrier.flight r p)| ≤ D)
(hfk : |f₀ - k₀| ≤ I) (hk : |k₀| ≤ A)
(hgh : ∀ r ∈ Icc 0 t, |g r - h r| ≤ E) (hh : ∀ r ∈ Icc 0 t, |h r| ≤ M)
(hgi : IntervalIntegrable (fun r => JetPicardComparison.attenuation ν r t p * g r) volume 0 t)
(hhi : IntervalIntegrable (fun r => JetPicardComparison.attenuation μ r t p * h r) volume 0 t) :
|value f₀ ν g t p - value k₀ μ h t p| ≤ I + D * t * A + (E + D * t * M) * t := by
have hνsub (r : ℝ) (hr : r ∈ Icc 0 t) :
IntervalIntegrable (fun τ => ν τ (JetBarrier.flight τ p)) volume r t := by
apply hνi.mono_set
rw [uIcc_of_le hr.2, uIcc_of_le ht]
exact Icc_subset_Icc hr.1 le_rfl
have hμsub (r : ℝ) (hr : r ∈ Icc 0 t) :
IntervalIntegrable (fun τ => μ τ (JetBarrier.flight τ p)) volume r t := by
apply hμi.mono_set
rw [uIcc_of_le hr.2, uIcc_of_le ht]
exact Icc_subset_Icc hr.1 le_rfl
have had (r : ℝ) (hr : r ∈ Icc 0 t) :
|JetPicardComparison.attenuation ν r t p - JetPicardComparison.attenuation μ r t p| ≤ D * t := by
apply (AttenuationLipschitz.attenuation_difference_le hr.2 p
(fun τ hτ => hν τ ⟨hr.1.trans hτ.1, hτ.2⟩)
(fun τ hτ => hμ τ ⟨hr.1.trans hτ.1, hτ.2⟩)
(hνsub r hr) (hμsub r hr) (fun τ hτ => hνμ τ ⟨hr.1.trans hτ.1, hτ.2⟩)).trans
exact mul_le_mul_of_nonneg_left (sub_le_self t hr.1) hD
have han (r : ℝ) (hr : r ∈ Icc 0 t) : |JetPicardComparison.attenuation ν r t p| ≤ 1 := by
rw [abs_of_nonneg (JetPicardComparison.attenuation_nonneg _ _ _ _)]
exact JetPicardComparison.attenuation_le_one hr.2 (fun τ hτ => hν τ ⟨hr.1.trans hτ.1, hτ.2⟩)
have hinitial : |f₀ * JetPicardComparison.attenuation ν 0 t p -
k₀ * JetPicardComparison.attenuation μ 0 t p| ≤ I + D * t * A := by
simpa only [mul_comm f₀, mul_comm k₀] using product_difference (han 0 ⟨le_rfl, ht⟩)
hfk hk (had 0 ⟨le_rfl, ht⟩) (mul_nonneg hD ht)
have hpoint (r : ℝ) (hr : r ∈ Icc 0 t) :
|JetPicardComparison.attenuation ν r t p * g r -
JetPicardComparison.attenuation μ r t p * h r| ≤ E + D * t * M :=
product_difference (han r hr) (hgh r hr) (hh r hr) (had r hr) (mul_nonneg hD ht)
have hint : |(∫ r in 0..t, JetPicardComparison.attenuation ν r t p * g r) -
∫ r in 0..t, JetPicardComparison.attenuation μ r t p * h r| ≤ (E + D * t * M) * t := by
rw [← intervalIntegral.integral_sub hgi hhi]
apply (intervalIntegral.abs_integral_le_integral_abs ht).trans
calc
_ ≤ ∫ _r in 0..t, E + D * t * M :=
intervalIntegral.integral_mono_on ht (hgi.sub hhi).abs intervalIntegrable_const hpoint
_ = _ := by rw [intervalIntegral.integral_const]; simp only [sub_zero, smul_eq_mul]; ring
calc
_ = |(f₀ * JetPicardComparison.attenuation ν 0 t p - k₀ * JetPicardComparison.attenuation μ 0 t p) +
((∫ r in 0..t, JetPicardComparison.attenuation ν r t p * g r) -
∫ r in 0..t, JetPicardComparison.attenuation μ r t p * h r)| := by unfold value; congr 1; ring
_ ≤ _ := (abs_add_le _ _).trans (add_le_add hinitial hint)
end BoltzmannNonuniqueness.MildStability
end
end
section
/-! # Exact dilation of the damped characteristic integral -/
noncomputable section
open MeasureTheory Set
namespace BoltzmannNonuniqueness.PositiveIntegral
def scalePhase (r : ℝ) (p : JetPrototype.Phase) : JetPrototype.Phase := (r • p.1,p.2)
theorem scalePhase_flight (r t : ℝ) (p : JetPrototype.Phase) :
scalePhase r (JetBarrier.flight t p) = JetBarrier.flight (r*t) (scalePhase r p) := by
apply Prod.ext
· apply Prod.ext
· change r • (p.1.1+t • VelocityWeight.transverse p.2) =
r • p.1.1+(r*t) • VelocityWeight.transverse p.2
rw [smul_add,mul_smul]
· change r*(p.1.2+t*VelocityWeight.axial p.2) = r*p.1.2+(r*t)*VelocityWeight.axial p.2
ring
· rfl
theorem value_dilation {r T t : ℝ} (hr : 0 < r) (ht : t ∈ Icc 0 T)
(L : ℝ) (f₀ : JetPrototype.Phase → ℝ) (g : ℝ × JetPrototype.Phase → ℝ)
(p : JetPrototype.Phase) :
value (r*T) L JetBarrier.flight f₀ g (r*t,scalePhase r p)/r =
value T (r*L) JetBarrier.flight (fun p => f₀ (scalePhase r p)/r)
(fun u => g (r*u.1,scalePhase r u.2)) (t,p) := by
have hrt : r*t ∈ Icc 0 (r*T) :=
⟨mul_nonneg hr.le ht.1,mul_le_mul_of_nonneg_left ht.2 hr.le⟩
unfold value
rw [GaussianLocal.time_eq hrt,GaussianLocal.time_eq ht]
have hi := intervalIntegral.integral_comp_mul_left
(fun s => Real.exp (-L*(r*t-s))*g (s,JetBarrier.flight (s-r*t) (scalePhase r p))) hr.ne'
(a := 0) (b := t)
simp only [mul_zero,smul_eq_mul,← div_eq_inv_mul] at hi
rw [add_div,← hi]
have he : -L*(r*t) = -(r*L)*t := by ring
have hp : JetBarrier.flight (-(r*t)) (scalePhase r p) = scalePhase r (JetBarrier.flight (-t) p) := by
rw [scalePhase_flight]
congr 1
ring
rw [he,hp]
congr 1
· ring
· apply intervalIntegral.integral_congr
intro s _
have he : -L*(r*t-r*s) = -(r*L)*(t-s) := by ring
have hp : JetBarrier.flight (r*s-r*t) (scalePhase r p) = scalePhase r (JetBarrier.flight (s-t) p) := by
rw [scalePhase_flight]
congr 1
ring
dsimp only
rw [he,hp]
theorem mild_dilation {r U A L : ℝ} (hr : 0 < r) (hA : r*A ≤ U)
{f₀ : JetPrototype.Phase → ℝ} {F g : ℝ × JetPrototype.Phase → ℝ}
(hmild : ∀ t ∈ Icc 0 U, (fun p => F (t,p)) =ᵐ[FlightMeasure.phaseVolume]
(fun p => value U L JetBarrier.flight f₀ g (t,p))) :
∀ t ∈ Icc 0 A, (fun p => F (r*t,scalePhase r p)/r) =ᵐ[FlightMeasure.phaseVolume]
(fun p => value A (r*L) JetBarrier.flight (fun p => f₀ (scalePhase r p)/r)
(fun u => g (r*u.1,scalePhase r u.2)) (t,p)) := by
intro t ht
have hrt : r*t ∈ Icc 0 (r*A) :=
⟨mul_nonneg hr.le ht.1,mul_le_mul_of_nonneg_left ht.2 hr.le⟩
have htU : r*t ∈ Icc 0 U := ⟨hrt.1,hrt.2.trans hA⟩
have hae := (ColdDilationMeasure.spatial_dilation_quasiMeasurePreserving hr).ae (hmild (r*t) htU)
filter_upwards [hae] with p hp
calc
F (r*t,scalePhase r p)/r = value U L JetBarrier.flight f₀ g (r*t,scalePhase r p)/r :=
congrArg (fun z : ℝ => z/r) hp
_ = value (r*A) L JetBarrier.flight f₀ g (r*t,scalePhase r p)/r :=
congrArg (fun z : ℝ => z/r) (value_eq_at_time htU hrt.2 L f₀ (fun _ _ _ => rfl) _)
_ = _ := value_dilation hr ht L f₀ g p
end BoltzmannNonuniqueness.PositiveIntegral
end
end
section
/-! # Characteristic localization of bounded measurable mild solutions -/
noncomputable section
open MeasureTheory Set
namespace BoltzmannNonuniqueness.PositiveIntegral
theorem characteristic_ae {T L : ℝ} (hT : 0 ≤ T)
{f₀ : JetPrototype.Phase → ℝ} (hf₀ : Measurable f₀)
{F g : ℝ × JetPrototype.Phase → ℝ} (hFm : Measurable F) (hgm : Measurable g)
(hmild : ∀ t ∈ Icc 0 T, (fun p => F (t,p)) =ᵐ[FlightMeasure.phaseVolume]
(fun p => value T L JetBarrier.flight f₀ g (t,p))) :
∀ᵐ p ∂FlightMeasure.phaseVolume,
(fun t => F (t,JetBarrier.flight t p)) =ᵐ[volume.restrict (Icc 0 T)]
(fun t => TransportPrimitive.damped L (f₀ p)
(fun r => g (r,JetBarrier.flight r p)) t) := by
let A : ℝ × JetPrototype.Phase → ℝ := fun z => F (z.1,JetBarrier.flight z.1 z.2)
let B : ℝ × JetPrototype.Phase → ℝ := fun z =>
value T L JetBarrier.flight f₀ g (z.1,JetBarrier.flight z.1 z.2)
have hflow : Measurable (fun z : ℝ × JetPrototype.Phase =>
(z.1,JetBarrier.flight z.1 z.2)) :=
measurable_fst.prodMk GaussianLocal.measurable_flight
have hAm : Measurable A := hFm.comp hflow
have hBm : Measurable B :=
(measurable_value hT GaussianLocal.measurable_flight hf₀ hgm).comp hflow
have hall : A =ᵐ[(volume.restrict (Icc 0 T)).prod FlightMeasure.phaseVolume] B := by
apply (Measure.ae_prod_iff_ae_ae (measurableSet_eq_fun hAm hBm)).mpr
filter_upwards [ae_restrict_mem measurableSet_Icc] with t ht
exact (FlightMeasure.flight_measurePreserving t).quasiMeasurePreserving.ae (hmild t ht)
have hp := Measure.ae_ae_of_ae_prod
((Measure.measurePreserving_swap (μ := FlightMeasure.phaseVolume)
(ν := volume.restrict (Icc 0 T))).quasiMeasurePreserving.ae hall)
filter_upwards [hp] with p hpe
filter_upwards [hpe,ae_restrict_mem measurableSet_Icc] with t ht htm
exact ht.trans (value_along_flight htm L f₀ g p)
/-- The damping parameter of the iteration cancels, leaving the physical
source `g-L*F` plus the differentiated cutoff in a unit-damped formula. -/
theorem localized_characteristic {T L S : ℝ} (hT : 0 ≤ T)
{f₀ : JetPrototype.Phase → ℝ} (hf₀ : Measurable f₀)
{F g : ℝ × JetPrototype.Phase → ℝ} (hFm : Measurable F) (hgm : Measurable g)
(hg : ∀ z, |g z| ≤ S)
(hmild : ∀ t ∈ Icc 0 T, (fun p => F (t,p)) =ᵐ[FlightMeasure.phaseVolume]
(fun p => value T L JetBarrier.flight f₀ g (t,p)))
(χ χ' : JetPrototype.Phase → ℝ → ℝ)
(hχ : ∀ p, ContinuousOn (χ p) (Icc 0 T))
(hχ' : ∀ p, ContinuousOn (χ' p) (Icc 0 T))
(hdχ : ∀ p t, t ∈ Icc 0 T → HasDerivAt (χ p) (χ' p t) t) :
∀ᵐ p ∂FlightMeasure.phaseVolume,
χ p T*F (T,JetBarrier.flight T p) = Real.exp (-T)*χ p 0*f₀ p +
∫ t in 0..T, Real.exp (-(T-t)) *
(χ p t*(g (t,JetBarrier.flight t p)-L*F (t,JetBarrier.flight t p)) +
(χ' p t+χ p t)*F (t,JetBarrier.flight t p)) := by
have hp := characteristic_ae hT hf₀ hFm hgm hmild
have ht := (FlightMeasure.flight_measurePreserving T).quasiMeasurePreserving.ae
(hmild T ⟨hT,le_rfl⟩)
filter_upwards [hp,ht] with p hpe hpend
have hgi : IntervalIntegrable (fun t => g (t,JetBarrier.flight t p)) volume 0 T := by
apply (intervalIntegrable_const (c := S)).mono_fun'
· exact (hgm.comp (measurable_id.prodMk
(GaussianLocal.measurable_flight.comp (measurable_id.prodMk measurable_const)))).aestronglyMeasurable
· exact ae_of_all _ (fun t => by simpa only [Real.norm_eq_abs] using hg (t,JetBarrier.flight t p))
have H := TransportPrimitive.localized_damped hT hgi (hχ p) (hχ' p) (hdχ p)
(L := L) (c := f₀ p)
have hboundary := hpend.trans (value_along_flight ⟨hT,le_rfl⟩ L f₀ g p)
rw [hboundary,H]
congr 1
rw [intervalIntegral.integral_of_le hT,intervalIntegral.integral_of_le hT]
apply integral_congr_ae
have he := ae_restrict_of_ae_restrict_of_subset Ioc_subset_Icc_self hpe
filter_upwards [he] with t ht
rw [ht]
congr 1
ring
end BoltzmannNonuniqueness.PositiveIntegral
end
end
section
/-! # Undamped test identities along bounded mild characteristics -/
noncomputable section
open MeasureTheory Set
namespace BoltzmannNonuniqueness.PositiveIntegral
theorem tested_characteristic {T L S : ℝ} (hT : 0 ≤ T)
{f₀ : JetPrototype.Phase → ℝ} (hf₀ : Measurable f₀)
{F g : ℝ × JetPrototype.Phase → ℝ} (hFm : Measurable F) (hgm : Measurable g)
(hg : ∀ z, |g z| ≤ S)
(hmild : ∀ t ∈ Icc 0 T, (fun p => F (t,p)) =ᵐ[FlightMeasure.phaseVolume]
(fun p => value T L JetBarrier.flight f₀ g (t,p)))
(χ χ' : JetPrototype.Phase → ℝ → ℝ)
(hχ : ∀ p, ContinuousOn (χ p) (Icc 0 T))
(hχ' : ∀ p, ContinuousOn (χ' p) (Icc 0 T))
(hdχ : ∀ p t, t ∈ Icc 0 T → HasDerivAt (χ p) (χ' p t) t) :
∀ᵐ p ∂FlightMeasure.phaseVolume,
(∫ t in 0..T, χ' p t*F (t,JetBarrier.flight t p)+
χ p t*(g (t,JetBarrier.flight t p)-L*F (t,JetBarrier.flight t p))) =
χ p T*F (T,JetBarrier.flight T p)-χ p 0*f₀ p := by
have hp := characteristic_ae hT hf₀ hFm hgm hmild
have ht := (FlightMeasure.flight_measurePreserving T).quasiMeasurePreserving.ae
(hmild T ⟨hT,le_rfl⟩)
filter_upwards [hp,ht] with p hpe hpend
have hgi : IntervalIntegrable (fun t => g (t,JetBarrier.flight t p)) volume 0 T := by
apply (intervalIntegrable_const (c := S)).mono_fun'
· exact (hgm.comp (measurable_id.prodMk
(GaussianLocal.measurable_flight.comp (measurable_id.prodMk measurable_const)))).aestronglyMeasurable
· exact ae_of_all _ (fun t => by simpa only [Real.norm_eq_abs] using hg (t,JetBarrier.flight t p))
have H := TransportPrimitive.damped_integration_by_parts hT hgi (hχ p) (hχ' p) (hdχ p)
(L := L) (c := f₀ p)
have hb := hpend.trans (value_along_flight ⟨hT,le_rfl⟩ L f₀ g p)
rw [hb]
rw [← H]
rw [intervalIntegral.integral_of_le hT,intervalIntegral.integral_of_le hT]
apply integral_congr_ae
have he := ae_restrict_of_ae_restrict_of_subset Ioc_subset_Icc_self hpe
filter_upwards [he] with t ht
rw [ht]
end BoltzmannNonuniqueness.PositiveIntegral
end
end
section
/-! # Survival of a positive datum under a bounded loss rate -/
noncomputable section
open MeasureTheory Set
namespace BoltzmannNonuniqueness.PositiveIntegral
theorem survival_characteristic {T L B : ℝ} (hT : 0 ≤ T)
{f₀ : JetPrototype.Phase → ℝ} (hf₀ : Measurable f₀)
{F g : ℝ × JetPrototype.Phase → ℝ} (hFm : Measurable F) (hgm : Measurable g)
(hg : ∀ z, |g z| ≤ B)
(hmild : ∀ t ∈ Icc 0 T, (fun p => F (t,p)) =ᵐ[FlightMeasure.phaseVolume]
(fun p => value T L JetBarrier.flight f₀ g (t,p)))
(C : JetPrototype.Phase → ℝ)
(hlow : ∀ᵐ p ∂FlightMeasure.phaseVolume, ∀ᵐ t, t ∈ Ioc 0 T →
-C p*F (t,JetBarrier.flight t p) ≤
g (t,JetBarrier.flight t p)-L*F (t,JetBarrier.flight t p)) :
∀ᵐ p ∂FlightMeasure.phaseVolume,
Real.exp (-C p*T)*f₀ p ≤ F (T,JetBarrier.flight T p) := by
have ht := tested_characteristic hT hf₀ hFm hgm hg hmild
(fun p t => Real.exp (C p*t)) (fun p t => C p*Real.exp (C p*t))
(fun _ => (by fun_prop : Continuous _).continuousOn)
(fun _ => (by fun_prop : Continuous _).continuousOn)
(fun p t _ => by simpa [mul_comm] using ((hasDerivAt_id t).const_mul (C p)).exp)
filter_upwards [ht,hlow] with p hp hpl
have hi : 0 ≤ ∫ t in 0..T, C p*Real.exp (C p*t)*F (t,JetBarrier.flight t p)+
Real.exp (C p*t)*(g (t,JetBarrier.flight t p)-L*F (t,JetBarrier.flight t p)) := by
apply intervalIntegral.integral_nonneg_of_ae_restrict hT
rw [← Measure.restrict_congr_set (Ioc_ae_eq_Icc (μ := volume))]
filter_upwards [ae_restrict_of_ae hpl,ae_restrict_mem measurableSet_Ioc] with t ht htm
have h := mul_le_mul_of_nonneg_left (ht htm) (Real.exp_pos (C p*t)).le
change 0 ≤ C p*Real.exp (C p*t)*F (t,JetBarrier.flight t p)+
Real.exp (C p*t)*(g (t,JetBarrier.flight t p)-L*F (t,JetBarrier.flight t p))
nlinarith only [h]
rw [hp] at hi
simp only [mul_zero,Real.exp_zero,one_mul] at hi
have hm := mul_le_mul_of_nonneg_left (sub_nonneg.mp hi) (Real.exp_pos (-C p*T)).le
have he : Real.exp (-C p*T)*Real.exp (C p*T) = 1 := by
rw [← Real.exp_add]; ring_nf; simp
simpa only [← mul_assoc,he,one_mul] using hm
end BoltzmannNonuniqueness.PositiveIntegral
end
end
section
/-! # Removing the auxiliary damping from an actual mild solution -/
noncomputable section
open MeasureTheory Set
namespace BoltzmannNonuniqueness.PositiveIntegral
theorem undamped_characteristic {T L S : ℝ} (hT : 0 ≤ T)
{f₀ : JetPrototype.Phase → ℝ} (hf₀ : Measurable f₀)
{F g : ℝ × JetPrototype.Phase → ℝ} (hFm : Measurable F) (hgm : Measurable g)
(hg : ∀ z, |g z| ≤ S)
(hmild : ∀ t ∈ Icc 0 T, (fun p => F (t,p)) =ᵐ[FlightMeasure.phaseVolume]
(fun p => value T L JetBarrier.flight f₀ g (t,p))) :
∀ᵐ p ∂FlightMeasure.phaseVolume,
F (T,JetBarrier.flight T p) = f₀ p+
∫ t in 0..T, g (t,JetBarrier.flight t p)-L*F (t,JetBarrier.flight t p) := by
have h := tested_characteristic hT hf₀ hFm hgm hg hmild
(fun _ _ => 1) (fun _ _ => 0)
(fun _ => continuous_const.continuousOn) (fun _ => continuous_const.continuousOn)
(fun _ t _ => hasDerivAt_const t (1:ℝ))
filter_upwards [h] with p hp
simp only [zero_mul,one_mul,zero_add] at hp
linarith
end BoltzmannNonuniqueness.PositiveIntegral
end
end
section
/-! # The undamped source is integrable along almost every finite characteristic -/
noncomputable section
open MeasureTheory Set
namespace BoltzmannNonuniqueness.PositiveIntegral
theorem netSource_integrable_characteristic {T L S : ℝ} (hT : 0 ≤ T)
{f₀ : JetPrototype.Phase → ℝ} (hf₀ : Measurable f₀)
{F g : ℝ × JetPrototype.Phase → ℝ} (hFm : Measurable F) (hgm : Measurable g)
(hg : ∀ z, |g z| ≤ S)
(hmild : ∀ t ∈ Icc 0 T, (fun p => F (t,p)) =ᵐ[FlightMeasure.phaseVolume]
(fun p => value T L JetBarrier.flight f₀ g (t,p))) :
∀ᵐ p ∂FlightMeasure.phaseVolume,
IntervalIntegrable (fun t => g (t,JetBarrier.flight t p)-L*F (t,JetBarrier.flight t p))
volume 0 T := by
filter_upwards [characteristic_ae hT hf₀ hFm hgm hmild] with p hp
have hi : IntervalIntegrable (fun t => g (t,JetBarrier.flight t p)) volume 0 T := by
apply (intervalIntegrable_const (c := S)).mono_fun'
· exact (hgm.comp (measurable_id.prodMk
(GaussianLocal.measurable_flight.comp (measurable_id.prodMk measurable_const)))).aestronglyMeasurable
· exact ae_of_all _ (fun t => by simpa only [Real.norm_eq_abs] using hg (t,JetBarrier.flight t p))
have hd := TransportPrimitive.damped_continuousOn hT L (f₀ p) hi
have hfi : IntervalIntegrable
(TransportPrimitive.damped L (f₀ p) (fun t => g (t,JetBarrier.flight t p))) volume 0 T := by
apply ContinuousOn.intervalIntegrable
simpa only [uIcc_of_le hT] using hd
have he : (fun t => F (t,JetBarrier.flight t p)) =ᵐ[volume.restrict (Ioc 0 T)]
(TransportPrimitive.damped L (f₀ p) (fun t => g (t,JetBarrier.flight t p))) :=
ae_restrict_of_ae_restrict_of_subset Ioc_subset_Icc_self hp
have he' : (fun t => F (t,JetBarrier.flight t p)) =ᵐ[volume.restrict (uIoc 0 T)]
(TransportPrimitive.damped L (f₀ p) (fun t => g (t,JetBarrier.flight t p))) := by
simpa only [uIoc_of_le hT] using he
exact hi.sub ((hfi.congr_ae he'.symm).const_mul L)
end BoltzmannNonuniqueness.PositiveIntegral
end
end
end OAI