import OAI.MathematicalPhysics.Boltzmann.Branching.AveragingTailSources import OAI.MathematicalPhysics.Boltzmann.Branching.CompactCapFamily import OAI.MathematicalPhysics.Boltzmann.Branching.ComplexWeakL2Diagonal import OAI.MathematicalPhysics.Boltzmann.Branching.RationalUniformApproximation import OAI.MathematicalPhysics.Boltzmann.Compactness.PeriodicRenormalizedCompactness import OAI.MathematicalPhysics.Boltzmann.Compactness.RenormalizedIntegrability import OAI.MathematicalPhysics.Boltzmann.Compactness.WeakL1ToWeakStar import OAI.MathematicalPhysics.Boltzmann.Compactness.WeakL1Operations namespace OAI section /-! # The actual gain divided by one plus density is uniformly integrable locally -/ noncomputable section open MeasureTheory Set namespace BoltzmannNonuniqueness.PeriodicApproximation open Compactness variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [SFinite μ] theorem gain_unit_uniformIntegrable_local {f : ℕ → X × Velocity → ℝ} {N : ℕ → ℝ} {R : ℝ} (hR : 0 ≤ R) (hfm : ∀ n, Measurable (f n)) (hf : ∀ n p, 0 ≤ f n p) (hN : ∀ n, 0 < N n) (hi : UniformIntegrable (fun n p => gain (N n) (f n) p/normalizer (f n) p) 1 (μ.prod volume)) : UniformIntegrable (fun n p => gain (N n) (f n) p/(1+f n p)) 1 (μ.prod ((volume : Measure Velocity).restrict (Metric.closedBall 0 R))) := by have hres := uniformIntegrable_restrict hi (univ ×ˢ Metric.closedBall (0:Velocity) R) rw [← Measure.prod_restrict,Measure.restrict_univ] at hres have hvel : ∀ᵐ p ∂μ.prod ((volume : Measure Velocity).restrict (Metric.closedBall 0 R)), p.2 ∈ Metric.closedBall (0:Velocity) R := Measure.quasiMeasurePreserving_snd.ae (ae_restrict_mem measurableSet_closedBall) apply uniformIntegrable_change_normalizer (fun n => gain_measurable (N n) (hfm n)) hfm (fun n p => (gain_bounds (hN n) (hfm n) (hf n) p).1) hf (maxwellianLower_pos R) _ hres filter_upwards [hvel] with p hp exact maxwellianLower_le hR (by simpa only [Metric.mem_closedBall,dist_zero_right] using hp) theorem approximatingSolution_gain_unit_uniformIntegrable_local (f : Density) (hfm : Measurable f) (hf : ∀ p, 0 ≤ f p) (hi : Integrable (entropyMoment f)) {T R : ℝ} (hT : 0 ≤ T) (hR : 0 ≤ R) : let F := fun n => (approximatingSolution f hfm (n+Nat.ceil T)).kineticProfile let N := fun n : ℕ => ((n+Nat.ceil T:ℕ):ℝ)+1 UniformIntegrable (fun n p => gain (N n) (F n) p/(1+F n p)) 1 (((volume.restrict (Icc 0 T)).prod (volume : Measure Position)).prod ((volume : Measure Velocity).restrict (Metric.closedBall 0 R))) := by apply gain_unit_uniformIntegrable_local hR (fun n => (approximatingSolution f hfm (n+Nat.ceil T)).kineticProfile_measurable) (fun n p => (approximatingSolution f hfm (n+Nat.ceil T)).nonnegative _) (fun n => by positivity) exact (approximatingSolution_normalizedSources_uniformIntegrable f hfm hf hi hT).1 end BoltzmannNonuniqueness.PeriodicApproximation end end section /-! # Local strong L2 convergence controls the local L1 seminorm -/ noncomputable section open MeasureTheory Filter Set open scoped Topology ENNReal namespace BoltzmannNonuniqueness.Published theorem localL2_L1_bound (K : Set FourierSpace) (a : Lp ℂ 2 (volume : Measure FourierSpace)) : eLpNorm (a : FourierSpace → ℂ) 1 (volume.restrict K) ≤ ENNReal.ofReal ‖complexL2Restriction K a‖ * volume K ^ (1/2 : ℝ) := by have h := eLpNorm_le_eLpNorm_mul_rpow_measure_univ (μ := volume.restrict K) (f := (a : FourierSpace → ℂ)) (p := 1) (q := 2) (by norm_num) (Lp.aestronglyMeasurable a).restrict have he : eLpNorm (a : FourierSpace → ℂ) 2 (volume.restrict K) = ENNReal.ofReal ‖complexL2Restriction K a‖ := by rw [ofReal_norm,complexL2Restriction,Lp.enorm_toLp] rw [he] at h convert h using 1; norm_num theorem localL2_L1_tendsto {u : ℕ → Lp ℂ 2 (volume : Measure FourierSpace)} (K : Set FourierSpace) (hK : volume K < ⊤) (hu : Tendsto (fun n => ‖complexL2Restriction K (u n)‖) atTop (𝓝 0)) : Tendsto (fun n => eLpNorm (u n : FourierSpace → ℂ) 1 (volume.restrict K)) atTop (𝓝 0) := by have h := ENNReal.continuous_ofReal.continuousAt.tendsto.comp hu have hb := ENNReal.Tendsto.mul_const h (Or.inr (ENNReal.rpow_ne_top_of_nonneg (by positivity : (0:ℝ) ≤ 1/2) hK.ne)) have hb' : Tendsto (fun n => ENNReal.ofReal ‖complexL2Restriction K (u n)‖ * volume K ^ (1/2 : ℝ)) atTop (𝓝 0) := by simpa only [Function.comp_apply,ENNReal.ofReal_zero,zero_mul] using hb exact tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds hb' (fun _ => bot_le) (fun n => localL2_L1_bound K (u n)) end BoltzmannNonuniqueness.Published end end section /-! # Uniform integrability of the physical loss with a unit density normalizer -/ noncomputable section open MeasureTheory Set namespace BoltzmannNonuniqueness.CollisionCompactness open Compactness PeriodicApproximation variable {X : Type*} [MeasurableSpace X] {μ : Measure X} [IsFiniteMeasure μ] theorem physicalLoss_unit_uniformIntegrable_local {f : ℕ → X × Velocity → ℝ} {R C : 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) : UniformIntegrable (fun n p => lossDensity (f n) p/(1+f n p)) 1 (μ.prod ((volume : Measure Velocity).restrict (Metric.closedBall 0 R))) := by have hres := uniformIntegrable_restrict (renormalized_loss_uniformIntegrable hfm hf hi hb) (univ ×ˢ Metric.closedBall (0:Velocity) R) rw [← Measure.prod_restrict,Measure.restrict_univ] at hres have hvel : ∀ᵐ p ∂μ.prod ((volume : Measure Velocity).restrict (Metric.closedBall 0 R)), p.2 ∈ Metric.closedBall (0:Velocity) R := Measure.quasiMeasurePreserving_snd.ae (ae_restrict_mem measurableSet_closedBall) apply uniformIntegrable_change_normalizer (fun n => lossDensity_measurable (hfm n)) hfm (fun n p => lossDensity_nonneg (hf n) p) hf (maxwellianLower_pos R) _ hres filter_upwards [hvel] with p hp exact maxwellianLower_le hR (by simpa only [Metric.mem_closedBall,dist_zero_right] using hp) end BoltzmannNonuniqueness.CollisionCompactness end end section /-! # Local factorization of pair moments along the actual averaging subsequence -/ noncomputable section open MeasureTheory Filter Set open scoped ENNReal Topology namespace BoltzmannNonuniqueness.Published theorem local_pair_moment_factorization {T : ℝ} {μ : Measure SpaceTime} [SFinite μ] (hμ : μ ≤ timeSpaceVolume T) {f : ℕ → KineticPhase → ℝ} {g : KineticPhase → ℝ} {W : SpaceTime × (Velocity × Velocity) → ℝ} (hfm : ∀ n, Measurable (f n)) (hfi : ∀ n, Integrable (f n) (μ.prod volume)) (hpUI : UniformIntegrable (fun (n : ℕ) (z : SpaceTime × (Velocity × Velocity)) => f n (z.1,z.2.1)*f n (z.1,z.2.2)) 1 (μ.prod volume)) (hg : WeakL1Converges (μ.prod volume) f g) (hW : WeakL1Converges (μ.prod volume) (fun n z => f n (z.1,z.2.1)*f n (z.1,z.2.2)) W) {k l : KineticPhase → ℝ} (hk : Continuous k) (hl : Continuous l) (hkc : HasCompactSupport k) (hlc : HasCompactSupport l) {A B : SpaceTime → ℝ} (hA : TimeLocalL1Converges T (fun n x => ∫ v, k (x,v)*f n (x,v)) A) (hB : TimeLocalL1Converges T (fun n x => ∫ v, l (x,v)*f n (x,v)) B) {K : Set SpaceTime} (hK : IsCompact K) [IsFiniteMeasure (μ.restrict K)] : (fun x => ∫ y : Velocity × Velocity, (k (x,y.1)*l (x,y.2))*W (x,y)) =ᵐ[μ.restrict K] (fun x => (∫ v, k (x,v)*g (x,v))*(∫ w, l (x,w)*g (x,w))) := by have hμv : μ ≤ (volume : Measure SpaceTime) := hμ.trans (Measure.prod_mono Measure.restrict_le_self le_rfl) have hmK := Measure.restrict_mono_measure hμ K have hAi := (hA.1.integrableOn_isCompact hK).mono_measure hμv have hBi := (hB.1.integrableOn_isCompact hK).mono_measure hμv have hA' : Tendsto (fun n => eLpNorm (fun x => (∫ v, k (x,v)*f n (x,v))-A x) 1 (μ.restrict K)) atTop (𝓝 0) := tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds (hA.2 K hK) (fun _ => zero_le) (fun _ => eLpNorm_mono_measure _ hmK) have hB' : Tendsto (fun n => eLpNorm (fun x => (∫ v, l (x,v)*f n (x,v))-B x) 1 (μ.restrict K)) atTop (𝓝 0) := tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds (hB.2 K hK) (fun _ => zero_le) (fun _ => eLpNorm_mono_measure _ hmK) have hfK (n) : Integrable (f n) ((μ.restrict K).prod volume) := by exact (hfi n).mono_measure (Measure.prod_mono Measure.restrict_le_self le_rfl) have hpK (n) : Integrable (fun z : SpaceTime × (Velocity × Velocity) => f n (z.1,z.2.1)*f n (z.1,z.2.2)) ((μ.restrict K).prod (volume.prod volume)) := by have hi : Integrable (fun z : SpaceTime × (Velocity × Velocity) => f n (z.1,z.2.1)*f n (z.1,z.2.2)) ((μ.restrict K).prod (volume : Measure (Velocity × Velocity))) := (memLp_one_iff_integrable.mp (hpUI.memLp n)).mono_measure (Measure.prod_mono Measure.restrict_le_self le_rfl) simpa only [Measure.volume_eq_prod] using hi have hgK := hg.restrict_base hK.measurableSet have hWK := hW.restrict_base hK.measurableSet rw [Measure.volume_eq_prod] at hWK obtain ⟨C,hC⟩ := hk.bounded_above_of_compact_support hkc obtain ⟨D,hD⟩ := hl.bounded_above_of_compact_support hlc have hui := Compactness.uniformIntegrable_restrict (Compactness.uniformIntegrable_compact_average_product hfm hpUI hk hl hkc hlc) K have he := weak_pair_moment_factorization hfm hfK hpK hgK hWK hk.measurable hl.measurable C D hC hD hAi hBi hA' hB' hui simpa only [← Measure.volume_eq_prod] using he end BoltzmannNonuniqueness.Published end end section /-! # Uniform integral bounds on finite balls give a global integral bound -/ noncomputable section open MeasureTheory Set open scoped ENNReal namespace BoltzmannNonuniqueness.Published theorem lintegral_le_of_closedBall_bounds (f : FourierSpace → ℝ≥0∞) (B : ℝ≥0∞) (h : ∀ n : ℕ, (∫⁻ x in Metric.closedBall (0 : FourierSpace) n, f x) ≤ B) : (∫⁻ x, f x) ≤ B := by let μ := (volume : Measure FourierSpace).withDensity f have hm : Monotone (fun n : ℕ => Metric.closedBall (0 : FourierSpace) n) := by intro n m hnm exact Metric.closedBall_subset_closedBall (by exact_mod_cast hnm) have he : (∫⁻ x, f x) = μ (Set.univ : Set FourierSpace) := by rw [withDensity_apply _ MeasurableSet.univ,Measure.restrict_univ] rw [he,← Metric.iUnion_closedBall_nat (0 : FourierSpace),hm.measure_iUnion] exact iSup_le (fun n => by simpa only [μ,withDensity_apply _ measurableSet_closedBall] using h n) end BoltzmannNonuniqueness.Published end end section /-! # Global L1 bounds pass through local L1 convergence -/ noncomputable section open MeasureTheory Filter Set open scoped Topology ENNReal namespace BoltzmannNonuniqueness.Published theorem localL1_global_bound {u : ℕ → FourierSpace → ℂ} {g : FourierSpace → ℂ} (hg : AEStronglyMeasurable g volume) (B : ℝ≥0∞) (hu : ∀ n, eLpNorm (u n) 1 volume ≤ B) (hc : ∀ K : Set FourierSpace, volume K < ⊤ → Tendsto (fun n => eLpNorm (u n-g) 1 (volume.restrict K)) atTop (𝓝 0)) : eLpNorm g 1 volume ≤ B := by rw [eLpNorm_one_eq_lintegral_enorm hg] apply lintegral_le_of_closedBall_bounds intro m let K := Metric.closedBall (0 : FourierSpace) (m : ℝ) have hK : volume K < ⊤ := measure_closedBall_lt_top have he n : eLpNorm g 1 (volume.restrict K) ≤ eLpNorm (u n-g) 1 (volume.restrict K)+B := by have hid : g = (g-u n)+u n := by funext x; simp calc _ = eLpNorm ((g-u n)+u n) 1 (volume.restrict K) := by rw [← hid] _ ≤ eLpNorm (g-u n) 1 (volume.restrict K)+eLpNorm (u n) 1 (volume.restrict K) := eLpNorm_add_le (by norm_num) _ ≤ eLpNorm (u n-g) 1 (volume.restrict K)+B := by rw [eLpNorm_sub_comm] exact add_le_add_right ((eLpNorm_mono_measure _ Measure.restrict_le_self).trans (hu n)) _ have ht : Tendsto (fun n => eLpNorm (u n-g) 1 (volume.restrict K)+B) atTop (𝓝 B) := by simpa using (hc K hK).add_const B have h := ge_of_tendsto ht (Eventually.of_forall he) simpa only [eLpNorm_one_eq_lintegral_enorm hg.restrict] using h theorem localL2_global_L1_bound {u : ℕ → Lp ℂ 2 (volume : Measure FourierSpace)} {g : Lp ℂ 2 (volume : Measure FourierSpace)} (B : ℝ≥0∞) (hu : ∀ n, eLpNorm (u n : FourierSpace → ℂ) 1 volume ≤ B) (hc : ∀ K : Set FourierSpace, volume K < ⊤ → Tendsto (fun n => ‖complexL2Restriction K (u n-g)‖) atTop (𝓝 0)) : eLpNorm (g : FourierSpace → ℂ) 1 volume ≤ B := by apply localL1_global_bound (Lp.aestronglyMeasurable g) B hu intro K hK have h := localL2_L1_tendsto K hK (hc K hK) have he n : eLpNorm (u n-g : Lp ℂ 2 volume) 1 (volume.restrict K) = eLpNorm ((u n : FourierSpace → ℂ)-(g : FourierSpace → ℂ)) 1 (volume.restrict K) := eLpNorm_congr_ae (ae_restrict_of_ae (Lp.coeFn_sub _ _)) simpa only [he] using h end BoltzmannNonuniqueness.Published end end section /-! # Local L1 convergence is stable under differences -/ noncomputable section open MeasureTheory Filter Set open scoped Topology ENNReal namespace BoltzmannNonuniqueness.Published theorem eLpNorm_sub_triangle {X : Type*} [MeasurableSpace X] (μ : Measure X) (f g h : X → ℂ) : eLpNorm (f-h) 1 μ ≤ eLpNorm (f-g) 1 μ+eLpNorm (g-h) 1 μ := by have he : f-h = (f-g)+(g-h) := by ext x; simp rw [he] exact eLpNorm_add_le (by norm_num) theorem localL1_difference_tendsto {u v : ℕ → FourierSpace → ℂ} {g h : FourierSpace → ℂ} (K : Set FourierSpace) (hu : Tendsto (fun n => eLpNorm (u n-g) 1 (volume.restrict K)) atTop (𝓝 0)) (hv : Tendsto (fun n => eLpNorm (v n-h) 1 (volume.restrict K)) atTop (𝓝 0)) : Tendsto (fun n => eLpNorm ((u n-v n)-(g-h)) 1 (volume.restrict K)) atTop (𝓝 0) := by have he n : (u n-v n)-(g-h) = (u n-g)-(v n-h) := by ext x; simp only [Pi.sub_apply]; ring have hb n : eLpNorm ((u n-v n)-(g-h)) 1 (volume.restrict K) ≤ eLpNorm (u n-g) 1 (volume.restrict K)+eLpNorm (v n-h) 1 (volume.restrict K) := by rw [he] exact eLpNorm_sub_le (by norm_num) have ht : Tendsto (fun n => eLpNorm (u n-g) 1 (volume.restrict K)+ eLpNorm (v n-h) 1 (volume.restrict K)) atTop (𝓝 0) := by simpa using hu.add hv exact tendsto_of_tendsto_of_tendsto_of_le_of_le tendsto_const_nhds ht (fun _ => bot_le) hb end BoltzmannNonuniqueness.Published end end section /-! # Limits of uniform L1 approximations are Cauchy in global L1 -/ noncomputable section open MeasureTheory Filter Set open scoped Topology ENNReal namespace BoltzmannNonuniqueness.Published theorem localL1_approximation_difference_bound (f : ℕ → FourierSpace → ℂ) (u : ℕ → ℕ → FourierSpace → ℂ) (g : ℕ → FourierSpace → ℂ) (hg : ∀ m, Integrable (g m)) (δ : ℕ → ℝ) (hδ : ∀ m, 0 ≤ δ m) (he : ∀ m n, eLpNorm (f n-u m n) 1 volume ≤ ENNReal.ofReal (δ m)) (hc : ∀ m (K : Set FourierSpace), volume K < ⊤ → Tendsto (fun n => eLpNorm (u m n-g m) 1 (volume.restrict K)) atTop (𝓝 0)) (m k : ℕ) : eLpNorm (g m-g k) 1 volume ≤ ENNReal.ofReal (δ m+δ k) := by apply localL1_global_bound ((hg m).sub (hg k)).aestronglyMeasurable · intro n have h := eLpNorm_sub_triangle volume (u m n) (f n) (u k n) rw [eLpNorm_sub_comm (u m n) (f n)] at h apply h.trans simpa only [ENNReal.ofReal_add (hδ m) (hδ k)] using add_le_add (he m n) (he k n) · intro K hK exact localL1_difference_tendsto K (hc m K hK) (hc k K hK) theorem localL1_approximation_cauchy (f : ℕ → FourierSpace → ℂ) (u : ℕ → ℕ → FourierSpace → ℂ) (g : ℕ → FourierSpace → ℂ) (hg : ∀ m, Integrable (g m)) (δ : ℕ → ℝ) (hδ : ∀ m, 0 ≤ δ m) (hδ0 : Tendsto δ atTop (𝓝 0)) (he : ∀ m n, eLpNorm (f n-u m n) 1 volume ≤ ENNReal.ofReal (δ m)) (hc : ∀ m (K : Set FourierSpace), volume K < ⊤ → Tendsto (fun n => eLpNorm (u m n-g m) 1 (volume.restrict K)) atTop (𝓝 0)) : CauchySeq (fun m => (hg m).toL1 (g m)) := by have hb m k := localL1_approximation_difference_bound f u g hg δ hδ he hc m k have hd m k : dist ((hg m).toL1 (g m)) ((hg k).toL1 (g k)) ≤ δ m+δ k := by apply (ENNReal.ofReal_le_ofReal_iff (add_nonneg (hδ m) (hδ k))).mp rw [dist_eq_norm,L1.ofReal_norm_sub_eq_lintegral] have hae : (fun x => ‖(hg m).toL1 (g m) x-(hg k).toL1 (g k) x‖ₑ) =ᵐ[volume] (fun x => ‖(g m-g k) x‖ₑ) := by filter_upwards [(hg m).coeFn_toL1,(hg k).coeFn_toL1] with x hm hk simp only [hm,hk,Pi.sub_apply] rw [lintegral_congr_ae hae] simpa only [eLpNorm_one_eq_lintegral_enorm ((hg m).sub (hg k)).aestronglyMeasurable] using hb m k rw [Metric.cauchySeq_iff] intro ε hε obtain ⟨N,hN⟩ := eventually_atTop.mp (hδ0.eventually (gt_mem_nhds (half_pos hε))) exact ⟨N,fun m hm k hk => (hd m k).trans_lt (by linarith [hN m hm,hN k hk])⟩ end BoltzmannNonuniqueness.Published end end section /-! # Identification on compact subsets of a local weak-convergence window -/ noncomputable section open MeasureTheory Filter Set open scoped ENNReal Topology namespace BoltzmannNonuniqueness.Published theorem WeakL1Converges.eq_of_local_strong {X : Type*} [NormedAddCommGroup X] [MeasurableSpace X] [BorelSpace X] {μ : Measure X} {Ω E : Set X} {f : ℕ → X → ℝ} {g A : X → ℝ} (h : WeakL1Converges (μ.restrict Ω) f g) (hf : ∀ᶠ n in atTop, Integrable (f n) (μ.restrict Ω)) (hA : LocallyIntegrable A μ) (hE : IsCompact E) (hEΩ : E ⊆ Ω) (hstrong : Tendsto (fun n => eLpNorm (fun x => f n x-A x) 1 (μ.restrict E)) atTop (𝓝 0)) : A =ᵐ[μ.restrict E] g := by have hr := h.restrict hE.measurableSet rw [Measure.restrict_restrict_of_subset hEΩ] at hr apply hr.eq_of_strong_eventually _ (hA.integrableOn_isCompact hE) hstrong filter_upwards [hf] with n hn exact hn.mono_measure (Measure.restrict_mono hEΩ le_rfl) end BoltzmannNonuniqueness.Published end end section /-! # Transfer of local strong convergence through eventual equality on a window -/ noncomputable section open MeasureTheory Filter Set open scoped Topology ENNReal namespace BoltzmannNonuniqueness.Published theorem LocalL1Converges.congr_on_window {f h : ℕ → SpaceTime → ℝ} {g : SpaceTime → ℝ} (hf : LocalL1Converges f g) {Ω : Set SpaceTime} (he : ∀ᶠ n in atTop, h n =ᵐ[volume.restrict Ω] f n) : ∀ K : Set SpaceTime, IsCompact K → K ⊆ Ω → Tendsto (fun n => eLpNorm (fun z => h n z-g z) 1 (volume.restrict K)) atTop (𝓝 0) := by intro K hK hKΩ apply (hf.2 K hK).congr' filter_upwards [he] with n hn apply eLpNorm_congr_ae have hkn := hn.filter_mono (ae_mono (Measure.restrict_mono hKΩ le_rfl)) filter_upwards [hkn] with z hz rw [hz] end BoltzmannNonuniqueness.Published end end section /-! # Completing a sequence uniformly approximated by locally compact families -/ noncomputable section open MeasureTheory Filter Set open scoped Topology ENNReal namespace BoltzmannNonuniqueness.Published theorem localL1_approximation_limit (f : ℕ → FourierSpace → ℂ) (u : ℕ → ℕ → FourierSpace → ℂ) (g : ℕ → FourierSpace → ℂ) (hg : ∀ m, Integrable (g m)) (δ : ℕ → ℝ) (hδ : ∀ m, 0 ≤ δ m) (hδ0 : Tendsto δ atTop (𝓝 0)) (he : ∀ m n, eLpNorm (f n-u m n) 1 volume ≤ ENNReal.ofReal (δ m)) (hc : ∀ m (K : Set FourierSpace), volume K < ⊤ → Tendsto (fun n => eLpNorm (u m n-g m) 1 (volume.restrict K)) atTop (𝓝 0)) : ∃ q : Lp ℂ 1 (volume : Measure FourierSpace), ∀ K : Set FourierSpace, volume K < ⊤ → Tendsto (fun n => eLpNorm (f n-(q : FourierSpace → ℂ)) 1 (volume.restrict K)) atTop (𝓝 0) := by obtain ⟨q,hq⟩ := cauchySeq_tendsto_of_complete (localL1_approximation_cauchy f u g hg δ hδ hδ0 he hc) have hq0 : Tendsto (fun m => eLpNorm (g m-(q : FourierSpace → ℂ)) 1 volume) atTop (𝓝 0) := by have ht := ENNReal.continuous_ofReal.continuousAt.tendsto.comp ((hq.sub_const q).norm) have heq m : ENNReal.ofReal ‖(hg m).toL1 (g m)-q‖ = eLpNorm (g m-(q : FourierSpace → ℂ)) 1 volume := by rw [L1.ofReal_norm_sub_eq_lintegral, eLpNorm_one_eq_lintegral_enorm ((hg m).sub (L1.integrable_coeFn q)).aestronglyMeasurable] apply lintegral_congr_ae filter_upwards [(hg m).coeFn_toL1] with x hx simp only [hx,Pi.sub_apply] simpa only [Function.comp_def,sub_self,norm_zero,ENNReal.ofReal_zero,heq] using ht have herror : Tendsto (fun m => ENNReal.ofReal (δ m)+eLpNorm (g m-(q : FourierSpace → ℂ)) 1 volume) atTop (𝓝 0) := by simpa only [Function.comp_def,ENNReal.ofReal_zero,zero_add] using (ENNReal.continuous_ofReal.continuousAt.tendsto.comp hδ0).add hq0 refine ⟨q,fun K hK => ?_⟩ apply ENNReal.tendsto_nhds_zero.mpr intro ε hε have hh : 0 < ε/2 := ENNReal.div_pos hε.ne' (by norm_num) obtain ⟨m,hm⟩ := (ENNReal.tendsto_nhds_zero.mp herror (ε/2) hh).exists filter_upwards [ENNReal.tendsto_nhds_zero.mp (hc m K hK) (ε/2) hh] with n hn calc eLpNorm (f n-(q : FourierSpace → ℂ)) 1 (volume.restrict K) ≤ eLpNorm (f n-u m n) 1 (volume.restrict K)+eLpNorm (u m n-(q : FourierSpace → ℂ)) 1 (volume.restrict K) := eLpNorm_sub_triangle _ _ _ _ _ ≤ ENNReal.ofReal (δ m)+(eLpNorm (u m n-g m) 1 (volume.restrict K)+eLpNorm (g m-(q : FourierSpace → ℂ)) 1 volume) := by apply add_le_add ((eLpNorm_mono_measure _ Measure.restrict_le_self).trans (he m n)) exact (eLpNorm_sub_triangle _ _ _ _).trans (add_le_add le_rfl (eLpNorm_mono_measure _ Measure.restrict_le_self)) _ = (ENNReal.ofReal (δ m)+eLpNorm (g m-(q : FourierSpace → ℂ)) 1 volume)+eLpNorm (u m n-g m) 1 (volume.restrict K) := by ac_rfl _ ≤ ε/2+ε/2 := add_le_add hm hn _ = ε := ENNReal.add_halves ε end BoltzmannNonuniqueness.Published end end end OAI