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import OAI.MathematicalPhysics.Boltzmann.Branching.BoundedEntryPortion
import OAI.MathematicalPhysics.Boltzmann.Branching.DampedBoundedEndpointTransport
import OAI.MathematicalPhysics.Boltzmann.Branching.DampedLateBoxPhysicalBlock
import OAI.MathematicalPhysics.Boltzmann.Branching.LateBoxAccessMeasure
import OAI.MathematicalPhysics.Boltzmann.Compactness.LocalizedDampedBalance
namespace OAI
section
/-! # Retaining the actual open-left collision-time window in physical histories -/
noncomputable section
open MeasureTheory ProbabilityTheory Set
open scoped ENNReal NNReal ProbabilityTheory
namespace BoltzmannNonuniqueness.ReferenceGeometry
def physicalCollisionWindow (s T : ℝ) : Set PhysicalFlightState := {p | T-p.1 ∈ Ioc s T}
theorem physicalCollisionWindow_measurable (s T : ℝ) : MeasurableSet (physicalCollisionWindow s T) :=
(measurable_const.sub measurable_fst) measurableSet_Ioc
def localizedNormalWindowEvent (b : BeamCoefficients) (ρ C T a η l s : ℝ)
{Ω : Set (ℝ × WeakTime.Phase)} (hΩ : MeasurableSet Ω) :
Kernel PhysicalFlightState PhysicalFlightState :=
(localizedNormalPhysicalEvent b ρ C T a η l hΩ).restrict (physicalCollisionWindow_measurable s T)
instance localizedNormalWindowEvent_sFinite (b : BeamCoefficients) (ρ C T a η l s : ℝ)
{Ω : Set (ℝ × WeakTime.Phase)} (hΩ : MeasurableSet Ω) :
IsSFiniteKernel (localizedNormalWindowEvent b ρ C T a η l s hΩ) := by
unfold localizedNormalWindowEvent
infer_instance
theorem localizedNormalWindowEvent_transport (b : BeamCoefficients) (ρ : ℝ)
(C : ℝ≥0) (T a η l s : ℝ) {Ω : Set (ℝ × WeakTime.Phase)} (hΩ : MeasurableSet Ω) :
localizedNormalWindowEvent b ρ C T a η l s hΩ =
transportedKernel (flightCharacteristicEquiv T)
(((localizedNormalBeamKernel b ρ C a η l hΩ).restrict
(measurable_fst measurableSet_Ioc : MeasurableSet (Prod.fst ⁻¹' Ioc s T))) ∘ₖ
WeakTime.residenceKernel C T) := by
rw [transportedKernel_compKernel,transportedKernel_restrict,
← physicalWaitingKernel_eq_transport,Kernel.comp_restrict]
simp only [localizedNormalWindowEvent,localizedNormalPhysicalEvent,localizedNormalCollision,
Real.toNNReal_coe]
rfl
theorem boundedHistory_le_localized_window {C : ℝ≥0} (hC : referenceClock ≤ C)
(b : BeamCoefficients) (ρ : ℝ≥0) (T a η l : ℝ)
{Ω : Set (ℝ × WeakTime.Phase)} (hΩ : MeasurableSet Ω)
(p : PhysicalFlightState) (ht : 0 ≤ p.1) (hv : ‖p.2.2‖ ≤ 6)
(hΩcone : ∀ q, boundedFlightCone p q → flightCharacteristicEquiv T q ∈ Ω)
(hlocal : ∀ q, boundedFlightCone p q →
flightCharacteristicEquiv T q ∈ coldCharacteristicDomain a η l ∧
0 ≤ b.plusDensity (characteristicBeamPoint (flightCharacteristicEquiv T q)) ∧
0 ≤ b.minusDensity (characteristicBeamPoint (flightCharacteristicEquiv T q)) ∧
characteristicBeamFrequency b (flightCharacteristicEquiv T q) ≤ (referenceClock:ℝ))
(n : ℕ) :
((dampedBoundedDensityScaledEvent C b T ρ)^n) p ≤
((localizedNormalWindowEvent b ρ (ρ*C) T a η l (T-p.1) hΩ)^n) p := by
apply kernel_pow_le_on_invariant _ _ {q | boundedFlightCone p q} _ _ n p
(boundedFlightCone_refl ht hv)
· intro q hq
filter_upwards [dampedBoundedDensityScaledEvent_ae_cone C b T ρ q hq.2.2.1] with r hr
exact boundedFlightCone_trans hq hr
· intro q hq
have he : dampedBoundedDensityScaledEvent C b T ρ q ≤
localizedNormalPhysicalEvent b ρ (ρ*C) T a η l hΩ q := by
simpa only [pow_one] using boundedHistory_le_localized hC b ρ T a η l hΩ q hq.1 hq.2.2.1
(fun r hr => hΩcone r (boundedFlightCone_trans hq hr))
(fun r hr => hlocal r (boundedFlightCone_trans hq hr)) 1
have htwin : ∀ᵐ r ∂dampedBoundedDensityScaledEvent C b T ρ q,
r ∈ physicalCollisionWindow (T-p.1) T :=
dampedBoundedDensityScaledEvent_ae_time_window C b T ρ hq
calc
_ = (dampedBoundedDensityScaledEvent C b T ρ q).restrict
(physicalCollisionWindow (T-p.1) T) := (Measure.restrict_eq_self_of_ae_mem htwin).symm
_ ≤ _ := Measure.restrict_mono_measure he _
end BoltzmannNonuniqueness.ReferenceGeometry
end
end
section
/-! # Physical normal-angle histories end at the hot trace's characteristic endpoint -/
noncomputable section
open MeasureTheory ProbabilityTheory
open scoped ENNReal NNReal ProbabilityTheory
namespace BoltzmannNonuniqueness.ReferenceGeometry
theorem localizedNormalWindowEvent_pow_transport (b : BeamCoefficients) (ρ : ℝ)
(C : ℝ≥0) (T a η l s : ℝ) {Ω : Set (ℝ × WeakTime.Phase)} (hΩ : MeasurableSet Ω) (n : ℕ) :
(localizedNormalWindowEvent b ρ C T a η l s hΩ)^n =
transportedKernel (flightCharacteristicEquiv T)
((((localizedNormalBeamKernel b ρ C a η l hΩ).restrict
(measurable_fst measurableSet_Ioc : MeasurableSet (Prod.fst ⁻¹' Set.Ioc s T))) ∘ₖ
WeakTime.residenceKernel C T)^n) := by
rw [transportedKernel_pow,← localizedNormalWindowEvent_transport]
theorem localizedNormal_endpoint_characteristic (b : BeamCoefficients) (ρ : ℝ)
(C : ℝ≥0) (T a η l s : ℝ) {Ω : Set (ℝ × WeakTime.Phase)} (hΩ : MeasurableSet Ω)
(n : ℕ) (p : PhysicalFlightState) {f : V × V → ℝ≥0∞} (hf : Measurable f) :
(∫⁻ q, clockSurvival C q.1*f (finishMediumFlight q)
∂((localizedNormalWindowEvent b ρ C T a η l s hΩ)^n) p) =
∫⁻ q, f (EuclideanFlight.flight T q)
∂(WeakTime.phaseEndpointKernel C T ∘ₖ
((((localizedNormalBeamKernel b ρ C a η l hΩ).restrict
(measurable_fst measurableSet_Ioc : MeasurableSet (Prod.fst ⁻¹' Set.Ioc s T))) ∘ₖ
WeakTime.residenceKernel C T)^n)) (flightCharacteristicEquiv T p) := by
have hg : Measurable (fun z => f (EuclideanFlight.flight T z)) :=
hf.comp (EuclideanFlight.flight_measurePreserving T).measurable
have hw : Measurable (fun q : PhysicalFlightState => clockSurvival C q.1*f (finishMediumFlight q)) :=
(show Measurable (fun q : PhysicalFlightState => clockSurvival C q.1) by
unfold clockSurvival; fun_prop).mul (hf.comp finishMediumFlight_measurable)
rw [localizedNormalWindowEvent_pow_transport,transportedKernel_lintegral _ _ _ hw,
Kernel.lintegral_comp _ _ _ hg]
apply lintegral_congr
intro z
rw [WeakTime.phaseEndpointKernel_lintegral _ _ _ hg,physical_terminal_characteristic T C f]
simp only [MeasurableEquiv.apply_symm_apply]
end BoltzmannNonuniqueness.ReferenceGeometry
end
end
section
/-! # The finite physical branching block lies below the actual angular endpoint histories -/
noncomputable section
open MeasureTheory ProbabilityTheory Set
open scoped ENNReal NNReal ProbabilityTheory
namespace BoltzmannNonuniqueness.ReferenceGeometry
def localizedHistoryBlockMass (b : BeamCoefficients) (ρ C T a η l s : ℝ)
{Ω : Set (ℝ × WeakTime.Phase)} (hΩ : MeasurableSet Ω) (A : Set (V × V))
(N : ℕ) (z : ℝ × WeakTime.Phase) : ℝ≥0∞ :=
∑ n ∈ Finset.range N, ∫⁻ q, A.indicator 1 (EuclideanFlight.flight T q)
∂(WeakTime.phaseEndpointKernel C T ∘ₖ
((((localizedNormalBeamKernel b ρ C a η l hΩ).restrict
(measurable_fst measurableSet_Ioc : MeasurableSet (Prod.fst ⁻¹' Ioc s T))) ∘ₖ
WeakTime.residenceKernel C T)^n)) z
theorem physicalBlock_le_localized {C : ℝ≥0} (hC : referenceClock ≤ C)
(b : BeamCoefficients) (ρ : ℝ≥0) (s Δ a η l κ d : ℝ)
{Ω : Set (ℝ × WeakTime.Phase)} (hΩ : MeasurableSet Ω) (x : V) (v : RetainedState)
(hΔ : 0 ≤ Δ) (hv : ‖(v:V)‖ ≤ 6) (hp : (x,(v:V)) ∈ lateBox κ d s)
(hΩcone : ∀ q, boundedFlightCone (Δ,(x,(v:V))) q → flightCharacteristicEquiv (s+Δ) q ∈ Ω)
(hlocal : ∀ q, boundedFlightCone (Δ,(x,(v:V))) q →
flightCharacteristicEquiv (s+Δ) q ∈ coldCharacteristicDomain a η l ∧
0 ≤ b.plusDensity (characteristicBeamPoint (flightCharacteristicEquiv (s+Δ) q)) ∧
0 ≤ b.minusDensity (characteristicBeamPoint (flightCharacteristicEquiv (s+Δ) q)) ∧
characteristicBeamFrequency b (flightCharacteristicEquiv (s+Δ) q) ≤ (referenceClock:ℝ))
(N : ℕ) :
dampedDensityScaledBlockMass C b (s+Δ) ρ x Δ v κ d N ≤
localizedHistoryBlockMass b ρ (ρ*C) (s+Δ) a η l s hΩ (lateBox κ d (s+Δ)) N
(flightCharacteristicEquiv (s+Δ) (Δ,(x,(v:V)))) := by
let A := lateBox κ d (s+Δ)
have hA : MeasurableSet A := lateBox_measurable _ _ _
have hf : Measurable (A.indicator (1 : V × V → ℝ≥0∞)) := measurable_const.indicator hA
unfold dampedDensityScaledBlockMass localizedHistoryBlockMass
simp only [Real.toNNReal_coe]
apply Finset.sum_le_sum
intro n _hn
have hle := boundedHistory_le_localized_window hC b ρ (s+Δ) a η l hΩ
(Δ,(x,(v:V))) hΔ hv hΩcone hlocal n
have htime : (s+Δ)-Δ = s := by ring
rw [htime] at hle
calc
_ ≤ ∫⁻ q, clockSurvival (ρ*C) q.1*A.indicator 1 (finishMediumFlight q)
∂((dampedBoundedDensityScaledEvent C b (s+Δ) ρ)^n) (Δ,(x,(v:V))) := by
apply lintegral_mono
intro q
dsimp only
gcongr
exact fun _ hy => physicalBlockTarget_subset_lateBox hp hy
_ ≤ ∫⁻ q, clockSurvival (ρ*C) q.1*A.indicator 1 (finishMediumFlight q)
∂((localizedNormalWindowEvent b ρ (ρ*C) (s+Δ) a η l s hΩ)^n) (Δ,(x,(v:V))) :=
lintegral_mono' hle le_rfl
_ = _ := by
simpa only [NNReal.coe_mul] using
localizedNormal_endpoint_characteristic b ρ (ρ*C) (s+Δ) a η l s hΩ n (Δ,(x,(v:V))) hf
end BoltzmannNonuniqueness.ReferenceGeometry
end
end
end OAI