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LeanPool.EscauriazaSereginSverak.LPS.CrossEndpointPairing

Endpoint cutoff pairings on the space-time slab #

The two endpoint pairings needed for the convection term of the cross density: an L²_t L∞_x velocity against an L²_t L¹_x convection, and an L∞_t L²_x velocity against an L¹_t L²_x convection (lem:lps-comparison).

theorem ESS.lps_lintegral_mul_ne_top_of_sq {μ : MeasureTheory.Measure ℝ} {a b : ℝ → ENNReal} (ha : AEMeasurable a μ) (hb : AEMeasurable b μ) (ha2 : ∫⁻ (t : ℝ), a t ^ 2 ∂μ < ⊤) (hb2 : ∫⁻ (t : ℝ), b t ^ 2 ∂μ < ⊤) :
∫⁻ (t : ℝ), a t * b t ∂μ ≠ ⊤

Cauchy–Schwarz in time for two profiles with finite square moments.

theorem ESS.lps_endpoint_cutoff_pairing_limit_linf_l1 {T t : ℝ} (ht : t ≤ T) {f g : CKN.Foundation.Parabolic.ParabolicPoint → ℝ} {β : ℝ → ℝ} (hf : MeasureTheory.AEStronglyMeasurable f (MeasureTheory.volume.restrict (CKN.spaceTimeSet Set.univ (Set.Ioo 0 T)))) (hg : MeasureTheory.AEStronglyMeasurable g (MeasureTheory.volume.restrict (CKN.spaceTimeSet Set.univ (Set.Ioo 0 T)))) (hβmeas : AEMeasurable (fun (τ : ℝ) => ENNReal.ofReal (β τ)) (MeasureTheory.volume.restrict (Set.Ioo 0 T))) (hβ : ∀ᵐ (τ : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioo 0 T), ∀ᵐ (x : CKN.Foundation.Parabolic.Vec3), |f (x, τ)| ≤ β τ) (hβint : ∫⁻ (τ : ℝ) in Set.Ioo 0 T, ENNReal.ofReal (β τ) ^ 2 < ⊤) (hgSlice : ∀ᵐ (τ : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioo 0 T), MeasureTheory.Integrable (fun (x : CKN.Foundation.Parabolic.Vec3) => g (x, τ)) MeasureTheory.volume) (hgMoment : ∫⁻ (τ : ℝ) in Set.Ioo 0 T, (∫⁻ (x : CKN.Foundation.Parabolic.Vec3), ‖g (x, τ)‖ₑ) ^ 2 < ⊤) :

Endpoint pairing of a velocity component with an essentially bounded L²_t spatial profile against an L²_t L¹_x convection component: the cutoff-weighted product of the spatial mollifications is integrable and its integral converges to that of the product.

theorem ESS.lps_endpoint_cutoff_pairing_limit_l2_l2 {T t : ℝ} (ht : t ≤ T) {f g : CKN.Foundation.Parabolic.ParabolicPoint → ℝ} {K : ENNReal} (hf : MeasureTheory.AEStronglyMeasurable f (MeasureTheory.volume.restrict (CKN.spaceTimeSet Set.univ (Set.Ioo 0 T)))) (hg : MeasureTheory.AEStronglyMeasurable g (MeasureTheory.volume.restrict (CKN.spaceTimeSet Set.univ (Set.Ioo 0 T)))) (hfSlice : ∀ᵐ (τ : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioo 0 T), MeasureTheory.MemLp (fun (x : CKN.Foundation.Parabolic.Vec3) => f (x, τ)) 2 MeasureTheory.volume) (hK : K ≠ ⊤) (hfBound : ∀ᵐ (τ : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioo 0 T), MeasureTheory.eLpNorm (fun (x : CKN.Foundation.Parabolic.Vec3) => f (x, τ)) 2 MeasureTheory.volume ≤ K) (hgSlice : ∀ᵐ (τ : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioo 0 T), MeasureTheory.MemLp (fun (x : CKN.Foundation.Parabolic.Vec3) => g (x, τ)) 2 MeasureTheory.volume) (hgMoment : ∫⁻ (τ : ℝ) in Set.Ioo 0 T, MeasureTheory.eLpNorm (fun (x : CKN.Foundation.Parabolic.Vec3) => g (x, τ)) 2 MeasureTheory.volume < ⊤) :

Endpoint pairing of an L∞_t L²_x velocity component against an L¹_t L²_x convection component.