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import OAI.MathematicalPhysics.Boltzmann.Branching.SmoothedPrePostIdentity
import OAI.MathematicalPhysics.Boltzmann.Branching.TransportCutoff
import OAI.MathematicalPhysics.Boltzmann.Branching.WeightedNormalizedGainTranslation
import OAI.MathematicalPhysics.Boltzmann.Collision.CollisionDissipation
import OAI.MathematicalPhysics.Boltzmann.Collision.CollisionMeasure
import OAI.MathematicalPhysics.Boltzmann.Collision.VelocityCutoffEntropyError
import OAI.MathematicalPhysics.Boltzmann.Compactness.NormalizedCollisionRates
import OAI.MathematicalPhysics.Boltzmann.Compactness.PairBoundedTruncation
namespace OAI
section
/-! # Incoming-velocity localization of the actual physical gain -/
noncomputable section
open MeasureTheory
namespace BoltzmannNonuniqueness.CollisionCompactness
open Compactness
variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [SFinite μ]
def localizedPostRate (η : C(Velocity,ℝ)) (f : X × Velocity → ℝ)
(z : (X × (Velocity × Velocity)) × Sphere) : ℝ :=
(η (scatterLeft z.1.2.1 z.1.2.2 z.2)*η (scatterRight z.1.2.1 z.1.2.2 z.2))*
massNormalizedPostRate f z
def localizedPhysicalGain (η : C(Velocity,ℝ)) (f : X × Velocity → ℝ) (p : X × Velocity) : ℝ :=
∫ q : Velocity × Sphere, localizedPostRate η f (collisionGrouping.symm (p,q))
∂(volume : Measure Velocity).prod sphereArea
theorem localizedPostRate_measurable (η : C(Velocity,ℝ))
{f : X × Velocity → ℝ} (hfm : Measurable f) : Measurable (localizedPostRate η f) := by
have hm : Measurable (fun z : (X × (Velocity × Velocity)) × Sphere =>
η (scatterLeft z.1.2.1 z.1.2.2 z.2)*η (scatterRight z.1.2.1 z.1.2.2 z.2)) := by
unfold scatterLeft scatterRight normalComponent
fun_prop
exact hm.mul (massNormalizedPostRate_measurable hfm)
theorem localizedPostRate_integrable (η : C(Velocity,ℝ)) (hη : HasCompactSupport η)
{f : X × Velocity → ℝ} (hfm : Measurable f)
(hi : Integrable (weightedNormalizedPair f) (μ.prod (volume : Measure (Velocity × Velocity)))) :
Integrable (localizedPostRate η f) ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) := by
obtain ⟨B,hB⟩ := η.continuous.bounded_above_of_compact_support hη
have hB0 : 0 ≤ B := (abs_nonneg (η 0)).trans (hB 0)
have hm : Measurable (fun z : (X × (Velocity × Velocity)) × Sphere =>
η (scatterLeft z.1.2.1 z.1.2.2 z.2)*η (scatterRight z.1.2.1 z.1.2.2 z.2)) := by
unfold scatterLeft scatterRight normalComponent
fun_prop
apply (massNormalizedPostRate_integrable hfm hi).bdd_mul hm.aestronglyMeasurable
filter_upwards [] with z
rw [Real.norm_eq_abs,abs_mul]
exact mul_le_mul (hB _) (hB _) (abs_nonneg _) hB0
theorem localizedPhysicalGain_integrable (η : C(Velocity,ℝ)) (hη : HasCompactSupport η)
{f : X × Velocity → ℝ} (hfm : Measurable f)
(hi : Integrable (weightedNormalizedPair f) (μ.prod (volume : Measure (Velocity × Velocity)))) :
Integrable (localizedPhysicalGain η f) (μ.prod volume) := by
have h := collision_test_marginal (localizedPostRate η f) (fun _ => (1:ℝ))
(by simpa only [one_mul] using localizedPostRate_integrable η hη hfm hi)
change Integrable (fun p => ∫ q : Velocity × Sphere,
localizedPostRate η f (collisionGrouping.symm (p,q)) ∂(volume : Measure Velocity).prod sphereArea)
(μ.prod volume)
simpa only [one_mul] using h.1
end BoltzmannNonuniqueness.CollisionCompactness
end
end
section
/-! # Identifying the localized physical gain with the linear pair operator -/
noncomputable section
open MeasureTheory
namespace BoltzmannNonuniqueness.CollisionCompactness.DoubleGain
open Compactness
variable {X : Type*}
def localizedPair (η : C(Velocity,ℝ)) (f : X × Velocity → ℝ)
(z : X × (Velocity × Velocity)) : ℝ :=
(η z.2.1*η z.2.2)*normalizedPair volume f z
theorem localizedPair_preRate (η : C(Velocity,ℝ)) (f : X × Velocity → ℝ)
(z : (X × (Velocity × Velocity)) × Sphere) :
pairPreRate (localizedPair η f) z =
(η z.1.2.1*η z.1.2.2)*massNormalizedPreRate f z := by
rw [massNormalizedPreRate_eq_pair]
unfold pairPreRate localizedPair
ring
theorem localizedPair_postRate (η : C(Velocity,ℝ)) (f : X × Velocity → ℝ)
(z : (X × (Velocity × Velocity)) × Sphere) :
pairPostRate (localizedPair η f) z = localizedPostRate η f z := by
rw [pairPostRate,localizedPair_preRate]
rfl
theorem localizedPhysicalGain_eq_pairGain [MeasurableSpace X] (η : C(Velocity,ℝ)) (f : X × Velocity → ℝ) :
localizedPhysicalGain η f = pairGain (localizedPair η f) := by
funext p
unfold localizedPhysicalGain pairGain
apply integral_congr_ae
exact ae_of_all _ (fun q => (localizedPair_postRate η f _).symm)
end BoltzmannNonuniqueness.CollisionCompactness.DoubleGain
end
end
section
/-! # The entropy velocity tail removes incoming localization of the gain -/
noncomputable section
open MeasureTheory Set
open scoped ENNReal
namespace BoltzmannNonuniqueness.CollisionCompactness.DoubleGain
open Compactness PeriodicApproximation
variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [SFinite μ]
theorem exists_velocity_unit_cutoff {R : ℝ} (hR : 0 < R) :
∃ η : C(Velocity,ℝ), HasCompactSupport η ∧
(∀ v, 0 ≤ η v) ∧ (∀ v, η v ≤ 1) ∧ (∀ v, ‖v‖ ≤ R → η v = 1) := by
let b : ContDiffBump (0 : Velocity) := ⟨R,R+1,hR,by linarith⟩
let η : C(Velocity,ℝ) := ⟨b,b.continuous⟩
refine ⟨η,b.hasCompactSupport,fun v => b.nonneg,fun v => b.le_one,?_⟩
intro v hv
apply b.one_of_mem_closedBall
simpa only [Metric.mem_closedBall,dist_zero_right] using hv
omit [MeasurableSpace X] in
theorem localizedPair_weight (η : C(Velocity,ℝ)) (f : X × Velocity → ℝ) :
momentPair (localizedPair η f) =
fun z => (η z.2.1*η z.2.2)*weightedNormalizedPair f z := by
funext z
unfold momentPair localizedPair weightedNormalizedPair pairVelocityWeight
ring
theorem localizedGain_tail_le {R C : ℝ} (hR : 0 < R)
(η : C(Velocity,ℝ)) (hη0 : ∀ v, 0 ≤ η v) (hη1 : ∀ v, η v ≤ 1)
(hone : ∀ v, ‖v‖ ≤ R → η v = 1)
{f : X × Velocity → ℝ} (hfm : Measurable f) (hf : ∀ p, 0 ≤ f p)
(hi : Integrable (entropyGauge f) (μ.prod volume))
(hb : (∫ p, entropyGauge f p ∂μ.prod volume) ≤ C) :
eLpNorm (fun p => pairGain (normalizedPair volume f) p-localizedPhysicalGain η f p)
1 (μ.prod volume) ≤ sphereArea univ*ENNReal.ofReal (8*C/R) := by
let w : X × (Velocity × Velocity) → ℝ := fun z => η z.2.1*η z.2.2
have hwm : Measurable w :=
(η.continuous.measurable.comp measurable_snd.fst).mul
(η.continuous.measurable.comp measurable_snd.snd)
have hw0 z : 0 ≤ w z := mul_nonneg (hη0 _) (hη0 _)
have hw1 z : w z ≤ 1 := by
dsimp only [w]
nlinarith [hη0 z.2.1,hη0 z.2.2,hη1 z.2.1,hη1 z.2.2]
have hpm : Measurable (normalizedPair volume f) :=
normalizedTensor_measurable (fiberMass_measurable hfm) hfm hfm
have hqm : Measurable (localizedPair η f) := hwm.mul hpm
have hwi : Integrable (weightedNormalizedPair f)
(μ.prod (volume : Measure (Velocity × Velocity))) := by
simpa only [Measure.volume_eq_prod] using weightedNormalizedPair_integrable hfm hf hi
have hqi : Integrable (momentPair (localizedPair η f))
(μ.prod (volume : Measure (Velocity × Velocity))) := by
rw [localizedPair_weight]
apply hwi.bdd_mul hwm.aestronglyMeasurable (c := 1)
exact ae_of_all _ (fun z => by rw [Real.norm_of_nonneg (hw0 z)]; exact hw1 z)
have hpn z : 0 ≤ weightedNormalizedPair f z := by
have hd : 0 ≤ 1+fiberMass volume f z.1 := by
have hm : 0 ≤ fiberMass volume f z.1 := integral_nonneg (fun v => hf (z.1,v))
linarith
exact mul_nonneg (by dsimp [pairVelocityWeight]; positivity)
(div_nonneg (mul_nonneg (hf _) (hf _)) hd)
have he : eLpNorm (momentPair (fun z => normalizedPair volume f z-localizedPair η f z))
1 (μ.prod (volume : Measure (Velocity × Velocity))) ≤
eLpNorm (fun z => weightedNormalizedPair f z-pairVelocityCut R f z)
1 (μ.prod (volume : Measure (Velocity × Velocity))) := by
apply eLpNorm_mono_ae (momentPair_measurable (hpm.sub hqm)).aestronglyMeasurable
filter_upwards [] with z
change ‖momentPair (fun y => normalizedPair volume f y-localizedPair η f y) z‖ ≤ _
have heq : momentPair (fun y => normalizedPair volume f y-localizedPair η f y) z =
(1-w z)*weightedNormalizedPair f z := by
dsimp only [momentPair,localizedPair,weightedNormalizedPair,pairVelocityWeight,w]
ring
rw [heq]
by_cases hv : ‖z.2.1‖ ≤ R ∧ ‖z.2.2‖ ≤ R
· have hw : w z = 1 := by simp only [w,hone _ hv.1,hone _ hv.2,one_mul]
simp only [hw,sub_self,zero_mul,norm_zero]
exact norm_nonneg _
· rw [pairVelocityCut,ite_eq_right hv,sub_zero,
Real.norm_of_nonneg (mul_nonneg (sub_nonneg.mpr (hw1 z)) (hpn z)),
Real.norm_of_nonneg (hpn z)]
nlinarith [mul_nonneg (hw0 z) (hpn z)]
rw [localizedPhysicalGain_eq_pairGain]
exact (pairGain_moment_difference_le hpm hqm hwi hqi).trans
(mul_le_mul' le_rfl (he.trans (pairVelocityCut_L1_error hR hfm hf hi hb)))
end BoltzmannNonuniqueness.CollisionCompactness.DoubleGain
end
end
section
/-! # Causal localized transport sources and their velocity support -/
noncomputable section
open MeasureTheory Set
open BoltzmannNonuniqueness.Published
namespace BoltzmannNonuniqueness.TransportCutoff
def localizedSource (U : ℝ) (χ f Q : KineticPhase → ℝ) (z : KineticPhase) : ℝ :=
if z.1.1 ∈ Icc 0 U then χ z*Q z+(transportDerivative χ z+χ z)*f z else 0
theorem localizedSource_causal (U : ℝ) (χ f Q : KineticPhase → ℝ)
(z : KineticPhase) (ht : z.1.1 < 0) : localizedSource U χ f Q z = 0 := by
apply ite_eq_right
exact fun h => not_le_of_gt ht h.1
theorem localizedSource_on {U : ℝ} (χ f Q : KineticPhase → ℝ)
(z : KineticPhase) (ht : z.1.1 ∈ Icc 0 U) :
localizedSource U χ f Q z = χ z*Q z+(transportDerivative χ z+χ z)*f z := ite_eq_left ht
theorem localizedSource_velocity_support {U R : ℝ} {χ : KineticPhase → ℝ}
(hχ : tsupport χ ⊆ {z | ‖z.2‖ ≤ R}) (f Q : KineticPhase → ℝ)
(z : KineticPhase) (hv : R < ‖z.2‖) : localizedSource U χ f Q z = 0 := by
have hz : z ∉ tsupport χ := fun h => not_le_of_gt hv (hχ h)
have hc : χ z = 0 := image_eq_zero_of_notMem_tsupport hz
have hd := transportDerivative_eq_zero hz
unfold localizedSource
split_ifs <;> simp only [hc,hd,zero_mul,add_zero]
theorem localizedSource_measurable {U : ℝ} {χ f Q : KineticPhase → ℝ}
(hχ : ContDiff ℝ (⊤ : ℕ∞) χ) (hf : Measurable f) (hQ : Measurable Q) :
Measurable (localizedSource U χ f Q) := by
apply Measurable.ite
· exact measurableSet_Icc.preimage measurable_fst.fst
· exact (hχ.continuous.measurable.mul hQ).add
(((transportDerivative_continuous hχ).measurable.add hχ.continuous.measurable).mul hf)
· exact measurable_const
end BoltzmannNonuniqueness.TransportCutoff
end
end
section
/-! # Velocity translations of the actual localized physical gains -/
noncomputable section
open MeasureTheory Filter
open scoped Topology NNReal
namespace BoltzmannNonuniqueness.CollisionCompactness.DoubleGain
open Compactness PeriodicApproximation
variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [IsFiniteMeasure μ]
theorem localizedGain_translation
{f : ℕ → X × Velocity → ℝ} {C : ℝ}
(hfm : ∀ n, Measurable (f n)) (hf : ∀ n p, 0 ≤ f n p)
(hi : ∀ n, Integrable (entropyGauge (f n)) (μ.prod volume))
(hb : ∀ n, (∫ p, entropyGauge (f n) p ∂μ.prod volume) ≤ C)
(η : C(Velocity,ℝ)) (hη : HasCompactSupport η)
{a : ℕ → Velocity} (ha : Tendsto a atTop (𝓝 0)) :
Tendsto (fun n => ∫ p,
|localizedPhysicalGain η (f n) (p.1,p.2+a n)-localizedPhysicalGain η (f n) p|
∂μ.prod volume) atTop (𝓝 0) := by
obtain ⟨B,hB⟩ := η.continuous.bounded_above_of_compact_support hη
have hB0 : 0 ≤ B := (abs_nonneg (η 0)).trans (hB 0)
let K : ℝ≥0 := ⟨B^2,sq_nonneg B⟩
have hw : Measurable (fun z : X × (Velocity × Velocity) => η z.2.1*η z.2.2) := by fun_prop
have hK (z : X × (Velocity × Velocity)) : |η z.2.1*η z.2.2| ≤ K := by
change |η z.2.1*η z.2.2| ≤ B^2
rw [abs_mul,pow_two]
exact mul_le_mul (hB _) (hB _) (abs_nonneg _) hB0
have ht := weighted_normalizedGain_translation (μ := μ) hfm hf hi hb hw K hK ha
simp_rw [localizedPhysicalGain_eq_pairGain]
change Tendsto (fun n => ∫ p,
|pairGain (fun z => η z.2.1*η z.2.2*normalizedPair volume (f n) z) (p.1,p.2+a n)-
pairGain (fun z => η z.2.1*η z.2.2*normalizedPair volume (f n) z) p|
∂μ.prod volume) atTop (𝓝 0)
exact ht
end BoltzmannNonuniqueness.CollisionCompactness.DoubleGain
end
end
section
/-! # Velocity smoothing of the genuine localized gain equals its incoming pair formula -/
noncomputable section
open MeasureTheory
namespace BoltzmannNonuniqueness.CollisionCompactness
open Compactness
variable {X : Type*} [MeasurableSpace X]
theorem localizedPhysicalGain_smoothing (η χ : C(Velocity,ℝ))
(hη : HasCompactSupport η) (hχ : HasCompactSupport χ)
(f : X × Velocity → ℝ) (x : X) (v : Velocity)
(hpre : Integrable (fun z : (Velocity × Velocity) × Sphere =>
massNormalizedPreRate f ((x,z.1),z.2)) ((volume : Measure (Velocity × Velocity)).prod sphereArea))
(hpost : Integrable (fun z : (Velocity × Velocity) × Sphere =>
localizedPostRate η f ((x,z.1),z.2)) ((volume : Measure (Velocity × Velocity)).prod sphereArea)) :
(∫ u : Velocity, χ (v-u)*localizedPhysicalGain η f (x,u)) =
∫ y : Velocity × Velocity, smoothedAngularKernel η χ (v,y)*normalizedPair volume f (x,y) := by
obtain ⟨B,hB⟩ := η.continuous.bounded_above_of_compact_support hη
obtain ⟨D,hD⟩ := χ.continuous.bounded_above_of_compact_support hχ
have hB0 : 0 ≤ B := (abs_nonneg (η 0)).trans (hB 0)
have hD0 : 0 ≤ D := (abs_nonneg (χ 0)).trans (hD 0)
have hm : Measurable (fun z : (Velocity × Velocity) × Sphere =>
(η z.1.1*η z.1.2)*χ (v-scatterLeft z.1.1 z.1.2 z.2)) := by
unfold scatterLeft normalComponent
fun_prop
have hi : Integrable (fun z : (Velocity × Velocity) × Sphere =>
(η z.1.1*η z.1.2)*χ (v-scatterLeft z.1.1 z.1.2 z.2)*
massNormalizedPreRate f ((x,z.1),z.2))
((volume : Measure (Velocity × Velocity)).prod sphereArea) := by
apply hpre.bdd_mul hm.aestronglyMeasurable (c := B*B*D)
filter_upwards [] with z
simp only [Real.norm_eq_abs,abs_mul]
exact mul_le_mul (mul_le_mul (hB _) (hB _) (abs_nonneg _) hB0) (hD _)
(abs_nonneg _) (mul_nonneg hB0 hB0)
have hposteq := collision_fiber_test_fubini hpost
(χ.continuous.measurable.comp (measurable_const.sub measurable_id)) D (fun u => hD (v-u))
calc
_ = ∫ ω : Sphere, (∫ y : Velocity × Velocity,
(η (scatterLeft y.1 y.2 ω)*η (scatterRight y.1 y.2 ω))*χ (v-y.1)*
massNormalizedPostRate f ((x,y),ω)) ∂sphereArea := by
change (∫ u : Velocity, χ (v-u)*localizedPhysicalGain η f (x,u)) = _ at hposteq
rw [hposteq]
apply integral_congr_ae
filter_upwards [] with ω
apply integral_congr_ae
filter_upwards [] with y
dsimp only [localizedPostRate,Function.comp_apply,Pi.sub_apply,Function.const_apply,id_eq]
ring
_ = ∫ ω : Sphere, (∫ y : Velocity × Velocity,
(η y.1*η y.2)*χ (v-scatterLeft y.1 y.2 ω)*massNormalizedPreRate f ((x,y),ω)) ∂sphereArea :=
(smoothed_pre_post_normals η χ f x v).symm
_ = ∫ y : Velocity × Velocity, ∫ ω : Sphere,
(η y.1*η y.2)*χ (v-scatterLeft y.1 y.2 ω)*massNormalizedPreRate f ((x,y),ω) ∂sphereArea :=
(integral_prod_symm _ hi).symm.trans (integral_prod _ hi)
_ = _ := smoothed_preRate_pair_identity η χ f x v
end BoltzmannNonuniqueness.CollisionCompactness
end
end
section
/-! # The physical gain convolution identity on a common full-measure base set -/
noncomputable section
open MeasureTheory
namespace BoltzmannNonuniqueness.CollisionCompactness
open Compactness
variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [SFinite μ]
local instance collisionRateFiberSFinite : SFinite ((volume : Measure (Velocity × Velocity)).prod sphereArea) :=
Measure.prod.instSFinite
theorem collision_rate_fibers {r : (X × (Velocity × Velocity)) × Sphere → ℝ}
(hi : Integrable r ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea)) :
∀ᵐ x ∂μ, Integrable (fun z : (Velocity × Velocity) × Sphere => r ((x,z.1),z.2))
((volume : Measure (Velocity × Velocity)).prod sphereArea) := by
have hmp := measurePreserving_prodAssoc μ (volume : Measure (Velocity × Velocity)) sphereArea
have hh := hmp.symm.integrable_comp_of_integrable hi
exact hh.prod_right_ae
theorem localizedPhysicalGain_smoothing_ae (η χ : C(Velocity,ℝ))
(hη : HasCompactSupport η) (hχ : HasCompactSupport χ)
{f : X × Velocity → ℝ} (hfm : Measurable f)
(hi : Integrable (weightedNormalizedPair f) (μ.prod (volume : Measure (Velocity × Velocity)))) :
∀ᵐ x ∂μ, ∀ v : Velocity,
(∫ u : Velocity, χ (v-u)*localizedPhysicalGain η f (x,u)) =
∫ y : Velocity × Velocity, smoothedAngularKernel η χ (v,y)*normalizedPair volume f (x,y) := by
filter_upwards [collision_rate_fibers (massNormalizedPreRate_integrable hfm hi),
collision_rate_fibers (localizedPostRate_integrable η hη hfm hi)] with x hx hy
intro v
exact localizedPhysicalGain_smoothing η χ hη hχ f x v hx hy
end BoltzmannNonuniqueness.CollisionCompactness
end
end
end OAI