import OAI.MathematicalPhysics.Boltzmann.Branching.MarginalUniformIntegrability import OAI.MathematicalPhysics.Boltzmann.Branching.RealL1ApproximationLimit import OAI.MathematicalPhysics.Boltzmann.Collision.CollisionSources import OAI.MathematicalPhysics.Boltzmann.Collision.CollisionConservation import OAI.MathematicalPhysics.Boltzmann.Compactness.NormalizedCollisionRates import OAI.MathematicalPhysics.Boltzmann.Compactness.NormalizedGainCompactness import OAI.MathematicalPhysics.Boltzmann.Compactness.NormalizedKernelAction import OAI.MathematicalPhysics.Boltzmann.Compactness.NormalizedPairCompactness import OAI.MathematicalPhysics.Boltzmann.Compactness.PeriodicMildApproximation import OAI.MathematicalPhysics.Boltzmann.Compactness.PeriodicRenormalizedCompactness import OAI.MathematicalPhysics.Boltzmann.Compactness.StrongMassClip import OAI.MathematicalPhysics.Boltzmann.Compactness.UniformIntegrability import OAI.MathematicalPhysics.Boltzmann.Compactness.WeakL1Operations import OAI.MathematicalPhysics.Boltzmann.Jets.TorusTransport namespace OAI section /-! # Strong spatial masses remove gain normalization in measure -/ noncomputable section open MeasureTheory Filter open scoped ENNReal Topology namespace BoltzmannNonuniqueness.Compactness variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [IsFiniteMeasure μ] theorem tendstoInMeasure_of_strong_massNormalized {f r : ℕ → X → ℝ} {g s : X → ℝ} (hfm : ∀ n, Measurable (f n)) (hrm : ∀ n, Measurable (r n)) (hr0 : ∀ n x, 0 ≤ r n x) (hs0 : ∀ x, 0 ≤ s x) (hr : Tendsto (fun n => eLpNorm (fun x => r n x-s x) 1 μ) atTop (𝓝 0)) (hf : Tendsto (fun n => eLpNorm (fun x => f n x/(1+r n x)-g x/(1+s x)) 1 μ) atTop (𝓝 0)) : TendstoInMeasure μ f atTop g := by have hri := tendstoInMeasure_of_tendsto_eLpNorm (by norm_num : (1:ℝ≥0∞) ≠ 0) hr have hfi := tendstoInMeasure_of_tendsto_eLpNorm (by norm_num : (1:ℝ≥0∞) ≠ 0) hf have hrc := tendstoInMeasure_continuous_comp (fun n => (hrm n).aestronglyMeasurable) hri (P := fun x : ℝ => 1+x) (continuous_const.add continuous_id) have h := tendstoInMeasure_mul (fun n => ((hfm n).div (measurable_const.add (hrm n))).aestronglyMeasurable) (fun n => (measurable_const.add (hrm n)).aestronglyMeasurable) hfi hrc have he n x : f n x/(1+r n x)*(1+r n x) = f n x := div_mul_cancel₀ _ (by linarith [hr0 n x]) have heg x : g x/(1+s x)*(1+s x) = g x := div_mul_cancel₀ _ (by linarith [hs0 x]) change TendstoInMeasure μ (fun n x => f n x/(1+r n x)*(1+r n x)) atTop (fun x => g x/(1+s x)*(1+s x)) at h simpa only [he,heg] using h end BoltzmannNonuniqueness.Compactness end end section /-! # Compact temporal support of the complete local-mass integrand -/ noncomputable section open Set namespace BoltzmannNonuniqueness theorem MassTest.exists_time_cutoff (φ : MassTest) : ∃ T : ℝ, 0 < T ∧ (∀ x, φ.toFun T x = 0) ∧ ∀ t, T < t → ∀ p : Phase, φ.transportDerivative t p = 0 := by obtain ⟨R,hR,hzero⟩ := φ.compact_time let L : ℝ × Velocity → ℝ := fun z => φ.toFun z.1 (torusProjection z.2) have hs : tsupport L ⊆ {z : ℝ × Velocity | z.1 ≤ R} := by apply closure_minimal · intro z hz by_contra hn exact hz (hzero z.1 (torusProjection z.2) ((lt_of_not_ge hn).trans_le (le_abs_self _))) · exact isClosed_le continuous_fst continuous_const refine ⟨R+1,by linarith,?_,?_⟩ · intro x exact hzero (R+1) x (by rw [abs_of_pos (by linarith : 0 < R+1)]; linarith) · intro t ht p have hn : (t,torusRepresentative p.1) ∉ tsupport L := by intro hp have := hs hp change t ≤ R at this linarith have hd : fderiv ℝ L (t,torusRepresentative p.1) = 0 := fderiv_of_notMem_tsupport ℝ hn exact congrArg (fun A : (ℝ × Velocity) →L[ℝ] ℝ => A (1,p.2)) hd end BoltzmannNonuniqueness end end section /-! # The actual finite collision rates divided by the same spatial mass -/ noncomputable section open MeasureTheory namespace BoltzmannNonuniqueness.PeriodicApproximation open CollisionCompactness Compactness variable {X : Type*} [MeasurableSpace X] def massRegularizedPreRate (N : ℝ) (f : X × Velocity → ℝ) (z : (X × (Velocity × Velocity)) × Sphere) : ℝ := regularizedPreRate N f z/(1+fiberMass volume f z.1.1) def massRegularizedPostRate (N : ℝ) (f : X × Velocity → ℝ) (z : (X × (Velocity × Velocity)) × Sphere) : ℝ := regularizedPostRate N f z/(1+fiberMass volume f z.1.1) theorem massRegularizedPreRate_measurable (N : ℝ) {f : X × Velocity → ℝ} (hfm : Measurable f) : Measurable (massRegularizedPreRate N f) := by exact (regularizedPreRate_measurable N hfm).div (measurable_const.add ((fiberMass_measurable hfm).comp measurable_fst.fst)) omit [MeasurableSpace X] in theorem massRegularizedPostRate_eq (N : ℝ) (f : X × Velocity → ℝ) : massRegularizedPostRate N f = massRegularizedPreRate N f ∘ scatterTriple := rfl theorem massRegularizedPostRate_measurable (N : ℝ) {f : X × Velocity → ℝ} (hfm : Measurable f) : Measurable (massRegularizedPostRate N f) := (massRegularizedPreRate_measurable N hfm).comp scatterTriple_measurable omit [MeasurableSpace X] in theorem massRegularizedPreRate_bounds {N : ℝ} (hN : 0 < N) {f : X × Velocity → ℝ} (hf : ∀ p, 0 ≤ f p) (z : (X × (Velocity × Velocity)) × Sphere) : 0 ≤ massRegularizedPreRate N f z ∧ massRegularizedPreRate N f z ≤ massNormalizedPreRate f z := by have hd : 0 ≤ 1+fiberMass volume f z.1.1 := by have h : 0 ≤ fiberMass volume f z.1.1 := integral_nonneg (fun v => hf (z.1.1,v)) linarith exact ⟨div_nonneg (regularizedPreRate_bounds hN hf z).1 hd, div_le_div_of_nonneg_right (regularizedPreRate_le_physical hN hf z) hd⟩ variable {μ : Measure X} [SFinite μ] omit [SFinite μ] in theorem massRegularizedPreRate_integrable {N : ℝ} (hN : 0 < N) {f : X × Velocity → ℝ} (hfm : Measurable f) (hf : ∀ p, 0 ≤ f p) (hi : Integrable (weightedNormalizedPair f) (μ.prod (volume : Measure (Velocity × Velocity)))) : Integrable (massRegularizedPreRate N f) ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) := by apply (massNormalizedPreRate_integrable hfm hi).mono' (massRegularizedPreRate_measurable N hfm).aestronglyMeasurable filter_upwards [] with z rw [Real.norm_of_nonneg (massRegularizedPreRate_bounds hN hf z).1] exact (massRegularizedPreRate_bounds hN hf z).2 theorem massRegularizedPostRate_integrable {N : ℝ} (hN : 0 < N) {f : X × Velocity → ℝ} (hfm : Measurable f) (hf : ∀ p, 0 ≤ f p) (hi : Integrable (weightedNormalizedPair f) (μ.prod (volume : Measure (Velocity × Velocity)))) : Integrable (massRegularizedPostRate N f) ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) := (scatterTriple_measurePreserving μ).integrable_comp_of_integrable (massRegularizedPreRate_integrable hN hfm hf hi) end BoltzmannNonuniqueness.PeriodicApproximation end end section /-! # Entropy controls the mass-normalized collision rate outside velocity windows -/ noncomputable section open MeasureTheory Set open scoped ENNReal namespace BoltzmannNonuniqueness.PeriodicApproximation open CollisionCompactness Compactness variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [SFinite μ] theorem massPreRate_velocity_tail {R C : ℝ} (hR : 0 < R) {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 ((collisionWindow R)ᶜ.indicator (massNormalizedPreRate f)) 1 ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) ≤ ENNReal.ofReal (16*C/R)*eLpNorm (fun _ : Sphere => (1:ℝ)) 1 sphereArea := by let u : X × (Velocity × Velocity) → ℝ := fun z => weightedNormalizedPair f z-pairVelocityCut (R/2) f z have hum : Measurable u := (weightedNormalizedPair_measurable hfm).sub (pairVelocityCut_measurable (R/2) hfm) have hdom (z : (X × (Velocity × Velocity)) × Sphere) : ‖((collisionWindow R)ᶜ.indicator (massNormalizedPreRate f)) z‖ ≤ ‖u z.1‖ := by by_cases hz : z ∈ collisionWindow R · rw [indicator_of_notMem (notMem_compl_iff.mpr hz),norm_zero] exact norm_nonneg _ · have hbox : ¬(‖z.1.2.1‖ ≤ R/2 ∧ ‖z.1.2.2‖ ≤ R/2) := by intro h have hv : ‖z.1.2.1‖^2 ≤ (R/2)^2 := (sq_le_sq₀ (norm_nonneg _) (by positivity)).mpr h.1 have hw : ‖z.1.2.2‖^2 ≤ (R/2)^2 := (sq_le_sq₀ (norm_nonneg _) (by positivity)).mpr h.2 apply hz change ‖z.1.2.1‖^2+‖z.1.2.2‖^2 ≤ R^2 nlinarith [sq_nonneg R] rw [indicator_of_mem (mem_compl hz),massNormalizedPreRate_eq] change ‖normalizedKernel z*weightedNormalizedPair f z.1‖ ≤ ‖weightedNormalizedPair f z.1-pairVelocityCut (R/2) f z.1‖ simp only [pairVelocityCut,hbox,ite_false,sub_zero,norm_mul] exact (mul_le_mul_of_nonneg_right (normalizedKernel_bound z) (norm_nonneg _)).trans_eq (one_mul _) have hm := (massNormalizedPreRate_measurable hfm).indicator (collisionWindow_measurable R).compl have hn := eLpNorm_mono (p := 1) (μ := (μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) hm.aestronglyMeasurable hdom have hp := eLpNorm_mul_prod_one (μ := μ.prod (volume.prod volume)) (ν := sphereArea) hum (g := fun _ : Sphere => (1:ℝ)) measurable_const simp only [mul_one] at hp rw [Measure.volume_eq_prod] at hn rw [hp] at hn apply hn.trans have he := pairVelocityCut_L1_error (half_pos hR) hfm hf hi hb have hc : 8*C/(R/2) = 16*C/R := by ring rw [hc] at he exact mul_le_mul' he le_rfl end BoltzmannNonuniqueness.PeriodicApproximation end end section /-! # Strong mass coefficients on bounded collision windows -/ noncomputable section open MeasureTheory Set Filter open scoped ENNReal Topology namespace BoltzmannNonuniqueness.PeriodicApproximation open Compactness CollisionCompactness variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [IsFiniteMeasure μ] def collisionMassClip (K : ℝ) (f : X × Velocity → ℝ) (z : (X × (Velocity × Velocity)) × Sphere) : ℝ := massClip K (fiberMass volume f z.1.1) theorem collisionMassClip_measurable (K : ℝ) {f : X × Velocity → ℝ} (hf : Measurable f) : Measurable (collisionMassClip K f) := (massClip_measurable K (fiberMass_measurable hf)).comp measurable_fst.fst theorem collisionMassClip_strong_on_box {f : ℕ → X × Velocity → ℝ} {g : X × Velocity → ℝ} (hfm : ∀ n, Measurable (f n)) (hgm : Measurable g) (hm : Tendsto (fun n => eLpNorm (fun x => fiberMass volume (f n) x-fiberMass volume g x) 1 μ) atTop (𝓝 0)) (K R : ℝ) : Tendsto (fun n => eLpNorm (fun z => collisionMassClip K (f n) z-collisionMassClip K g z) 1 (((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea).restrict (angularPairBox R))) atTop (𝓝 0) := by let B : Set (Velocity × Velocity) := Metric.closedBall 0 R ×ˢ Metric.closedBall 0 R let ν : Measure (Velocity × Velocity) := volume.restrict B have : IsFiniteMeasure ν := by constructor dsimp only [ν] rw [Measure.restrict_apply_univ,Measure.volume_eq_prod,Measure.prod_prod] exact ENNReal.mul_lt_top (isCompact_closedBall (0:Velocity) R).measure_lt_top (isCompact_closedBall (0:Velocity) R).measure_lt_top let a n x := massClip K (fiberMass volume (f n) x)-massClip K (fiberMass volume g x) have ham n : Measurable (a n) := (massClip_measurable K (fiberMass_measurable (hfm n))).sub (massClip_measurable K (fiberMass_measurable hgm)) have ha := strong_massClip (fun n => fiberMass_measurable (hfm n)) (fiberMass_measurable hgm) K hm have ht := strongL1_comp_fst (ν := sphereArea) (fun n => (ham n).comp measurable_fst) (strongL1_comp_fst (ν := ν) ham ha) have he : (μ.prod ν).prod sphereArea = ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea).restrict (angularPairBox R) := by dsimp only [ν,angularPairBox,velocityPairBox,B] rw [← Measure.restrict_prod_eq_prod_univ,← Measure.prod_restrict,Measure.restrict_univ] rw [he] at ht exact ht omit [MeasurableSpace X] in theorem collisionWindow_subset_angularPairBox {R : ℝ} (hR : 0 ≤ R) : collisionWindow (X := X) R ⊆ angularPairBox R := by intro z hz have h := collisionWindow_bounds hR hz exact ⟨⟨mem_univ _,by simpa only [Set.mem_prod,Metric.mem_closedBall,dist_zero_right] using h⟩,mem_univ _⟩ theorem collisionMassClip_strong_on_window {f : ℕ → X × Velocity → ℝ} {g : X × Velocity → ℝ} (hfm : ∀ n, Measurable (f n)) (hgm : Measurable g) (hm : Tendsto (fun n => eLpNorm (fun x => fiberMass volume (f n) x-fiberMass volume g x) 1 μ) atTop (𝓝 0)) (K : ℝ) {R : ℝ} (hR : 0 ≤ R) : Tendsto (fun n => eLpNorm (fun z => collisionMassClip K (f n) z-collisionMassClip K g z) 1 (((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea).restrict (collisionWindow R))) atTop (𝓝 0) := by apply tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds (collisionMassClip_strong_on_box hfm hgm hm K R) (fun _ => zero_le) exact fun n => eLpNorm_mono_measure _ (Measure.restrict_mono (collisionWindow_subset_angularPairBox hR) le_rfl) end BoltzmannNonuniqueness.PeriodicApproximation end end section /-! # Actual finite pre-rates converge to physical pre-rates on each collision window -/ noncomputable section open MeasureTheory Set Filter open scoped ENNReal NNReal Topology namespace BoltzmannNonuniqueness.PeriodicApproximation open CollisionCompactness Compactness variable {X : Type*} [MeasurableSpace X] omit [MeasurableSpace X] in theorem collisionWindow_mono {R N : ℝ} (hR : 0 ≤ R) (hRN : R ≤ N) : collisionWindow (X := X) R ⊆ collisionWindow N := by intro z hz exact hz.trans ((sq_le_sq₀ hR (hR.trans hRN)).mpr hRN) omit [MeasurableSpace X] in theorem massRegularizedPreRate_on_window {R N : ℝ} (hR : 0 ≤ R) (hRN : R ≤ N) (f : X × Velocity → ℝ) (z : (X × (Velocity × Velocity)) × Sphere) (hz : z ∈ collisionWindow R) : massRegularizedPreRate N f z = rateMultiplier N f z*massNormalizedPreRate f z := by unfold massRegularizedPreRate massNormalizedPreRate rw [regularizedPreRate_factor,windowKernel,indicator_of_mem (collisionWindow_mono hR hRN hz)] unfold preRate ring omit [MeasurableSpace X] in theorem massRegularizedPreRate_window_difference {R N : ℝ} (hR : 0 ≤ R) (hRN : R ≤ N) (f : X × Velocity → ℝ) : (collisionWindow R).indicator (fun z => massRegularizedPreRate N f z-massNormalizedPreRate f z) = fun z => -((collisionWindow R).indicator (fun z => 1-rateMultiplier N f z) z * massNormalizedPreRate f z) := by funext z by_cases hz : z ∈ collisionWindow R · rw [indicator_of_mem hz,indicator_of_mem hz,massRegularizedPreRate_on_window hR hRN f z hz] ring · simp only [indicator_of_notMem hz,zero_mul,neg_zero] variable {μ : Measure X} [IsFiniteMeasure μ] theorem massRegularizedPreRate_window_L1 {f : ℕ → X × Velocity → ℝ} {N : ℕ → ℝ} {C : ℝ} (R : ℝ) (hR : 0 ≤ 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) (hN : ∀ n, 0 < N n) (hNt : Tendsto N atTop atTop) (B : ℝ≥0) (hB : ∀ n, eLpNorm (f n) 1 (μ.prod volume) ≤ B) : Tendsto (fun n => eLpNorm ((collisionWindow R).indicator (fun z => massRegularizedPreRate (N n) (f n) z-massNormalizedPreRate (f n) z)) 1 ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea)) atTop (𝓝 0) := by have ht := collisionAttenuation_preRate_L1 R hR hfm hf hi hb hN hNt B hB have he : (fun n => eLpNorm ((collisionWindow R).indicator (fun z => massRegularizedPreRate (N n) (f n) z-massNormalizedPreRate (f n) z)) 1 ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea)) =ᶠ[atTop] (fun n => eLpNorm (fun z => (collisionWindow R).indicator (fun z => 1-rateMultiplier (N n) (f n) z) z*massNormalizedPreRate (f n) z) 1 ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea)) := by filter_upwards [hNt.eventually (eventually_ge_atTop R)] with n hn rw [massRegularizedPreRate_window_difference hR hn] exact eLpNorm_neg _ _ _ exact (tendsto_congr' he).mpr ht end BoltzmannNonuniqueness.PeriodicApproximation end end section /-! # Removing every collision cutoff from the mass-normalized actual rates -/ noncomputable section open MeasureTheory Set Filter open scoped ENNReal NNReal Topology namespace BoltzmannNonuniqueness.PeriodicApproximation open CollisionCompactness Compactness variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [IsFiniteMeasure μ] omit [MeasurableSpace X] [IsFiniteMeasure μ] in private theorem massRegularizedPreRate_difference_bound {N : ℝ} (hN : 0 < N) {f : X × Velocity → ℝ} (hf : ∀ p, 0 ≤ f p) (z : (X × (Velocity × Velocity)) × Sphere) : |massRegularizedPreRate N f z-massNormalizedPreRate f z| ≤ |massNormalizedPreRate f z| := by have h := massRegularizedPreRate_bounds hN hf z rw [abs_of_nonpos (sub_nonpos.mpr h.2),abs_of_nonneg (h.1.trans h.2)] linarith theorem massRegularizedPreRate_L1 {f : ℕ → X × Velocity → ℝ} {N : ℕ → 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) (hN : ∀ n, 0 < N n) (hNt : Tendsto N atTop atTop) (B : ℝ≥0) (hB : ∀ n, eLpNorm (f n) 1 (μ.prod volume) ≤ B) : Tendsto (fun n => eLpNorm (fun z => massRegularizedPreRate (N n) (f n) z- massNormalizedPreRate (f n) z) 1 ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea)) atTop (𝓝 0) := by let ν := (μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea let d n := fun z => massRegularizedPreRate (N n) (f n) z-massNormalizedPreRate (f n) z let P := eLpNorm (fun _ : Sphere => (1:ℝ)) 1 sphereArea have hP : P ≠ ⊤ := (memLp_one_iff_integrable.mpr (integrable_const (1:ℝ))).eLpNorm_ne_top have hdm n : Measurable (d n) := (massRegularizedPreRate_measurable (N n) (hfm n)).sub (massNormalizedPreRate_measurable (hfm n)) have htail (R : ℝ) (hR : 0 < R) (n : ℕ) : eLpNorm ((collisionWindow R)ᶜ.indicator (d n)) 1 ν ≤ ENNReal.ofReal (16*C/R)*P := by apply le_trans (b := eLpNorm ((collisionWindow R)ᶜ.indicator (massNormalizedPreRate (f n))) 1 ν) · apply eLpNorm_mono ((hdm n).indicator (collisionWindow_measurable R).compl).aestronglyMeasurable intro z by_cases hz : z ∈ collisionWindow R · simp only [indicator_of_notMem (notMem_compl_iff.mpr hz),norm_zero,le_refl] · simp only [indicator_of_mem (mem_compl hz),Real.norm_eq_abs] exact massRegularizedPreRate_difference_bound (hN n) (hf n) z · exact massPreRate_velocity_tail hR (hfm n) (hf n) (hi n) (hb n) have hsplit (R : ℝ) (n : ℕ) : eLpNorm (d n) 1 ν ≤ eLpNorm ((collisionWindow R).indicator (d n)) 1 ν+ eLpNorm ((collisionWindow R)ᶜ.indicator (d n)) 1 ν := by have he : d n = (collisionWindow R).indicator (d n)+(collisionWindow R)ᶜ.indicator (d n) := by funext z by_cases hz : z ∈ collisionWindow R <;> simp [hz] conv_lhs => rw [he] exact eLpNorm_add_le (by norm_num) have hδ : Tendsto (fun j : ℕ => ENNReal.ofReal (16*C/((j:ℝ)+1))*P) atTop (𝓝 0) := by have ht := ENNReal.tendsto_ofReal (tendsto_const_nhds.div_atTop (tendsto_natCast_atTop_atTop.atTop_add tendsto_const_nhds) : Tendsto (fun j : ℕ => 16*C/((j:ℝ)+1)) atTop (𝓝 0)) simpa only [ENNReal.ofReal_zero,zero_mul] using ENNReal.Tendsto.mul_const ht (Or.inr hP) apply ENNReal.tendsto_nhds_zero.mpr intro ε hε have hε2 : 0 < ε/2 := ENNReal.div_pos hε.ne' (by norm_num) obtain ⟨j,hj⟩ := (ENNReal.tendsto_nhds_zero.mp hδ (ε/2) hε2).exists have hR : 0 < (j:ℝ)+1 := by positivity have hw := massRegularizedPreRate_window_L1 ((j:ℝ)+1) hR.le hfm hf hi hb hN hNt B hB filter_upwards [ENNReal.tendsto_nhds_zero.mp hw (ε/2) hε2] with n hn exact (hsplit ((j:ℝ)+1) n).trans ((add_le_add hn ((htail _ hR n).trans hj)).trans_eq ε.add_halves) theorem massRegularizedPostRate_L1 {f : ℕ → X × Velocity → ℝ} {N : ℕ → 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) (hN : ∀ n, 0 < N n) (hNt : Tendsto N atTop atTop) (B : ℝ≥0) (hB : ∀ n, eLpNorm (f n) 1 (μ.prod volume) ≤ B) : Tendsto (fun n => eLpNorm (fun z => massRegularizedPostRate (N n) (f n) z- massNormalizedPostRate (f n) z) 1 ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea)) atTop (𝓝 0) := by have he n : eLpNorm (fun z => massRegularizedPostRate (N n) (f n) z- massNormalizedPostRate (f n) z) 1 ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) = eLpNorm (fun z => massRegularizedPreRate (N n) (f n) z- massNormalizedPreRate (f n) z) 1 ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) := by exact eLpNorm_comp_measurePreserving ((massRegularizedPreRate_measurable (N n) (hfm n)).sub (massNormalizedPreRate_measurable (hfm n))).aestronglyMeasurable (scatterTriple_measurePreserving μ) simpa only [he] using massRegularizedPreRate_L1 hfm hf hi hb hN hNt B hB end BoltzmannNonuniqueness.PeriodicApproximation end end section /-! # Removing velocity cutoffs from strong mass averages -/ noncomputable section open MeasureTheory Filter open scoped ENNReal Topology namespace BoltzmannNonuniqueness.Compactness variable {X Y : Type*} [MeasurableSpace X] [MeasurableSpace Y] variable {μ : Measure X} {ν : Measure Y} [SFinite μ] [SFinite ν] theorem strong_mass_of_velocity_averages {f : ℕ → X × Y → ℝ} {g : X × Y → ℝ} (hfm : ∀ n, Measurable (f n)) (hfi : ∀ n, Integrable (f n) (μ.prod ν)) (hw : Published.WeakL1Converges (μ.prod ν) f g) {k : ℕ → Y → ℝ} (hkm : ∀ j, Measurable (k j)) (hkb : ∀ j y, |k j y| ≤ 1) {δ : ℕ → ℝ≥0∞} (hδ : Tendsto δ atTop (𝓝 0)) (he : ∀ j n, eLpNorm (fun p => f n p-k j p.2*f n p) 1 (μ.prod ν) ≤ δ j) (hc : ∀ j, Tendsto (fun n => eLpNorm (fun x => (∫ v, k j v*f n (x,v) ∂ν)-(∫ v, k j v*g (x,v) ∂ν)) 1 μ) atTop (𝓝 0)) : Tendsto (fun n => eLpNorm (fun x => (∫ v, f n (x,v) ∂ν)-(∫ v, g (x,v) ∂ν)) 1 μ) atTop (𝓝 0) := by let U := fun j n x => ∫ v, k j v*f n (x,v) ∂ν have hu j n : Integrable (fun p : X × Y => k j p.2*f n p) (μ.prod ν) := (hfi n).bdd_mul ((hkm j).comp measurable_snd).aestronglyMeasurable (ae_of_all _ (fun p => hkb j p.2)) have herr j n : eLpNorm ((fun x => ∫ v, f n (x,v) ∂ν)-U j n) 1 μ ≤ δ j := by have hae : ((fun x => ∫ v, f n (x,v) ∂ν)-U j n) =ᵐ[μ] (fun x => ∫ v, f n (x,v)-k j v*f n (x,v) ∂ν) := by filter_upwards [(hfi n).prod_right_ae,(hu j n).prod_right_ae] with x hfx hux exact (integral_sub hfx hux).symm rw [eLpNorm_congr_ae hae] exact (eLpNorm_integral_le ((hfm n).sub (((hkm j).comp measurable_snd).mul (hfm n)))).trans (he j n) obtain ⟨q,hqi,hq⟩ := l1_limit_of_uniform_approximation (fun n => (hfi n).integral_prod_left) hδ herr hc have hwm := hw.marginal hfi (measurable_const : Measurable (fun _ : X × Y => (1:ℝ))) 1 (fun _ => by norm_num) simp only [one_mul] at hwm have hq' : Tendsto (fun n => eLpNorm (fun x => (∫ v, f n (x,v) ∂ν)-q x) 1 μ) atTop (𝓝 0) := hq have hqe := hwm.eq_of_strong (fun n => (hfi n).integral_prod_left) hqi hq' have hn n : eLpNorm (fun x => (∫ v, f n (x,v) ∂ν)-q x) 1 μ = eLpNorm (fun x => (∫ v, f n (x,v) ∂ν)-(∫ v, g (x,v) ∂ν)) 1 μ := by apply eLpNorm_congr_ae filter_upwards [hqe] with x hx rw [hx] simpa only [hn] using hq' end BoltzmannNonuniqueness.Compactness end end section /-! # The actual finite collision rates have the same mass-normalized weak limit -/ noncomputable section open MeasureTheory Filter open scoped ENNReal NNReal Topology namespace BoltzmannNonuniqueness.PeriodicApproximation open CollisionCompactness Compactness variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [IsFiniteMeasure μ] theorem weak_massRegularizedPreRate {f : ℕ → X × Velocity → ℝ} {g : X × Velocity → ℝ} {N : ℕ → 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) (hN : ∀ n, 0 < N n) (hNt : Tendsto N atTop atTop) (B : ℝ≥0) (hB : ∀ n, eLpNorm (f n) 1 (μ.prod volume) ≤ B) (hw : Published.WeakL1Converges ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) (fun n => massNormalizedPreRate (f n)) (massNormalizedPreRate g)) : Published.WeakL1Converges ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) (fun n => massRegularizedPreRate (N n) (f n)) (massNormalizedPreRate g) := by have hwi n : Integrable (weightedNormalizedPair (f n)) (μ.prod (volume : Measure (Velocity × Velocity))) := by rw [Measure.volume_eq_prod] exact weightedNormalizedPair_integrable (hfm n) (hf n) (hi n) exact hw.of_eLpNorm_sub (fun n => massNormalizedPreRate_integrable (hfm n) (hwi n)) (fun n => massRegularizedPreRate_integrable (hN n) (hfm n) (hf n) (hwi n)) (massRegularizedPreRate_L1 hfm hf hi hb hN hNt B hB) theorem weak_massRegularizedPostRate {f : ℕ → X × Velocity → ℝ} {g : X × Velocity → ℝ} {N : ℕ → 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) (hN : ∀ n, 0 < N n) (hNt : Tendsto N atTop atTop) (B : ℝ≥0) (hB : ∀ n, eLpNorm (f n) 1 (μ.prod volume) ≤ B) (hw : Published.WeakL1Converges ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) (fun n => massNormalizedPostRate (f n)) (massNormalizedPostRate g)) : Published.WeakL1Converges ((μ.prod (volume : Measure (Velocity × Velocity))).prod sphereArea) (fun n => massRegularizedPostRate (N n) (f n)) (massNormalizedPostRate g) := by have hwi n : Integrable (weightedNormalizedPair (f n)) (μ.prod (volume : Measure (Velocity × Velocity))) := by rw [Measure.volume_eq_prod] exact weightedNormalizedPair_integrable (hfm n) (hf n) (hi n) exact hw.of_eLpNorm_sub (fun n => massNormalizedPostRate_integrable (hfm n) (hwi n)) (fun n => massRegularizedPostRate_integrable (hN n) (hfm n) (hf n) (hwi n)) (massRegularizedPostRate_L1 hfm hf hi hb hN hNt B hB) end BoltzmannNonuniqueness.PeriodicApproximation end end section /-! # Removing finite collision attenuation from the mass-normalized gain -/ noncomputable section open MeasureTheory Filter open scoped ENNReal NNReal Topology namespace BoltzmannNonuniqueness.PeriodicApproximation open Compactness CollisionCompactness CollisionCompactness.DoubleGain variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [IsFiniteMeasure μ] theorem massRegularized_gain {N : ℝ} (hN : 0 ≤ N) (f : X × Velocity → ℝ) (p : X × Velocity) : collisionMarginal (massRegularizedPostRate N f) p = gain N f p/(1+fiberMass volume f p.1) := by change (∫ q : Velocity × Sphere, regularizedPostRate N f (collisionGrouping.symm (p,q))/(1+fiberMass volume f p.1) ∂(volume : Measure Velocity).prod sphereArea) = _ rw [integral_div,← gain_eq_full_integral hN] theorem massNormalized_gain (f : X × Velocity → ℝ) (p : X × Velocity) : collisionMarginal (massNormalizedPostRate f) p = gainDensity f p/(1+fiberMass volume f p.1) := by change (∫ q : Velocity × Sphere, postRate f (collisionGrouping.symm (p,q))/(1+fiberMass volume f p.1) ∂(volume : Measure Velocity).prod sphereArea) = _ rw [integral_div] rfl theorem massRegularizedGain_L1 {f : ℕ → X × Velocity → ℝ} {N : ℕ → 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) (hN : ∀ n, 0 < N n) (hNt : Tendsto N atTop atTop) (B : ℝ≥0) (hB : ∀ n, eLpNorm (f n) 1 (μ.prod volume) ≤ B) : Tendsto (fun n => eLpNorm (fun p => gain (N n) (f n) p/(1+fiberMass volume (f n) p.1)- gainDensity (f n) p/(1+fiberMass volume (f n) p.1)) 1 (μ.prod volume)) atTop (𝓝 0) := by have herr := massRegularizedPostRate_L1 hfm hf hi hb hN hNt B hB apply tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds herr (fun _ => zero_le) intro n have hwi : Integrable (weightedNormalizedPair (f n)) (μ.prod (volume : Measure (Velocity × Velocity))) := by simpa only [Measure.volume_eq_prod] using weightedNormalizedPair_integrable (hfm n) (hf n) (hi n) have hm := massRegularizedPostRate_measurable (N n) (hfm n) have km := massNormalizedPostRate_measurable (hfm n) have hri := massRegularizedPostRate_integrable (hN n) (hfm n) (hf n) hwi have hpi := massNormalizedPostRate_integrable (hfm n) hwi have h := collisionMarginal_difference_le hm km hri hpi have he : collisionMarginal (massRegularizedPostRate (N n) (f n))- collisionMarginal (massNormalizedPostRate (f n)) = (fun p => gain (N n) (f n) p/(1+fiberMass volume (f n) p.1)- gainDensity (f n) p/(1+fiberMass volume (f n) p.1)) := by funext p exact congrArg₂ (fun a b : ℝ => a-b) (massRegularized_gain (hN n).le (f n) p) (massNormalized_gain (f n) p) rw [he] at h exact h end BoltzmannNonuniqueness.PeriodicApproximation end end section /-! # Removing finite collision attenuation from the mass-normalized loss -/ noncomputable section open MeasureTheory Filter open scoped ENNReal NNReal Topology namespace BoltzmannNonuniqueness.PeriodicApproximation open Compactness CollisionCompactness CollisionCompactness.DoubleGain variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [IsFiniteMeasure μ] theorem massRegularized_loss {N : ℝ} (hN : 0 ≤ N) (f : X × Velocity → ℝ) (p : X × Velocity) : collisionMarginal (massRegularizedPreRate N f) p = loss N f p/(1+fiberMass volume f p.1) := by change (∫ q : Velocity × Sphere, regularizedPreRate N f (collisionGrouping.symm (p,q))/(1+fiberMass volume f p.1) ∂(volume : Measure Velocity).prod sphereArea) = _ rw [integral_div,← loss_eq_full_integral hN] theorem massNormalized_loss (f : X × Velocity → ℝ) (p : X × Velocity) : collisionMarginal (massNormalizedPreRate f) p = lossDensity f p/(1+fiberMass volume f p.1) := by change (∫ q : Velocity × Sphere, preRate f (collisionGrouping.symm (p,q))/(1+fiberMass volume f p.1) ∂(volume : Measure Velocity).prod sphereArea) = _ rw [integral_div] rfl theorem massRegularizedLoss_L1 {f : ℕ → X × Velocity → ℝ} {N : ℕ → 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) (hN : ∀ n, 0 < N n) (hNt : Tendsto N atTop atTop) (B : ℝ≥0) (hB : ∀ n, eLpNorm (f n) 1 (μ.prod volume) ≤ B) : Tendsto (fun n => eLpNorm (fun p => loss (N n) (f n) p/(1+fiberMass volume (f n) p.1)- lossDensity (f n) p/(1+fiberMass volume (f n) p.1)) 1 (μ.prod volume)) atTop (𝓝 0) := by have herr := massRegularizedPreRate_L1 hfm hf hi hb hN hNt B hB apply tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds herr (fun _ => zero_le) intro n have hwi : Integrable (weightedNormalizedPair (f n)) (μ.prod (volume : Measure (Velocity × Velocity))) := by simpa only [Measure.volume_eq_prod] using weightedNormalizedPair_integrable (hfm n) (hf n) (hi n) have hm := massRegularizedPreRate_measurable (N n) (hfm n) have km := massNormalizedPreRate_measurable (hfm n) have hri := massRegularizedPreRate_integrable (hN n) (hfm n) (hf n) hwi have hpi := massNormalizedPreRate_integrable (hfm n) hwi have h := collisionMarginal_difference_le hm km hri hpi have he : collisionMarginal (massRegularizedPreRate (N n) (f n))- collisionMarginal (massNormalizedPreRate (f n)) = (fun p => loss (N n) (f n) p/(1+fiberMass volume (f n) p.1)- lossDensity (f n) p/(1+fiberMass volume (f n) p.1)) := by funext p exact congrArg₂ (fun a b : ℝ => a-b) (massRegularized_loss (hN n).le (f n) p) (massNormalized_loss (f n) p) rw [he] at h exact h end BoltzmannNonuniqueness.PeriodicApproximation end end end OAI