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LeanPool.CaffarelliKohnNirenberg.Leray.ForcedRegLocalEnergyTime

The mollifier limit of the space-time energy identity #

For each velocity component of the forced regularized solution, the space-time energy identity of the mollified velocity passes to the limit as the mollifier radius tends to zero: on almost every time slice the mollified pairing converges to the unmollified pairing, dominated by an integrable product of slice L² norms. The result is ∫∫ u_k² ∂ₜψ = 2 ∫ L_k, where L_k is the limiting slice pairing. This is the limit step of eq:reg-local-energy-forced.

theorem CKN.Leray.memLp_toReal_of_lintegral_sq {N : ℝ → ENNReal} (hm : Measurable N) {T : ℝ} (hfin : ∫⁻ (t : ℝ) in Set.Ioo 0 T, N t ^ 2 ≠ ⊤) :
theorem CKN.Leray.exists_weight_bound {ψ : Foundation.Parabolic.Vec3 × ℝ → ℝ} (hψ : ContDiff ℝ (↑⊤) ψ) (hψc : HasCompactSupport ψ) :
∃ (M : ℝ), 0 ≤ M ∧ (∀ (z : Foundation.Parabolic.Vec3 × ℝ), |ψ z| ≤ M) ∧ ∀ (j : Fin 3) (x : Foundation.Parabolic.Vec3) (t : ℝ), |(fderiv ℝ (fun (y : Foundation.Parabolic.Vec3) => ψ (y, t)) x) (basisVec j)| ≤ M

A smooth compactly supported space-time weight and its spatial partial derivatives are uniformly bounded.

The mollified energy pairing of one component on a time slice.

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    The limiting energy pairing of one component on a time slice.

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      The dominating function of the mollified energy pairings.

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        theorem CKN.Leray.ae_leDelta (ρ : RegMollifierProfile) (ε : ℝ) (hε : 0 < ε) {a : Foundation.Parabolic.Vec3 → Foundation.Parabolic.Vec3} (ha : IsInJ a) {f : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3} (hf : IsLocallySquareIntegrableForce f) {T : ℝ} (hT : 0 < T) {ψ : Foundation.Parabolic.Vec3 × ℝ → ℝ} (hψ : ContDiff ℝ (↑⊤) ψ) (hψc : HasCompactSupport ψ) {M : ℝ} (hMψ : ∀ (z : Foundation.Parabolic.Vec3 × ℝ), |ψ z| ≤ M) (hMd : ∀ (j : Fin 3) (x : Foundation.Parabolic.Vec3) (t : ℝ), |(fderiv ℝ (fun (y : Foundation.Parabolic.Vec3) => ψ (y, t)) x) (basisVec j)| ≤ M) (k : Fin 3) :
        ∀ᵐ (t : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioo 0 T), (∀ (n : ℕ), |leDeltaT ρ ε hε ha hf ψ n k t| ≤ leTimeBound ρ ε hε ha hf M k t) ∧ Filter.Tendsto (fun (n : ℕ) => leDeltaT ρ ε hε ha hf ψ n k t) Filter.atTop (nhds (leLimitT ρ ε hε ha hf ψ k t)) ∧ ∀ (hft : MeasureTheory.MemLp (fun (x : Foundation.Parabolic.Vec3) => f (x, t)) 2 MeasureTheory.volume), leLimitT ρ ε hε ha hf ψ k t = leLimit (fun (y : Foundation.Parabolic.Vec3) => forcedRegRep ρ ε hε ha hf (y, t) k) (fun (j : Fin 3) (y : Foundation.Parabolic.Vec3) => forcedMollifiedGrad (forcedRegRep ρ ε hε ha hf) (y, t) k j) (fun (j : Fin 3) (y : Foundation.Parabolic.Vec3) => leTensor ρ ε hε ha hf j k (y, t)) (fun (y : Foundation.Parabolic.Vec3) => forcedQuadPressure ρ ε hε (forcedRegCurve ρ ε hε ha hf) (y, t)) (fun (y : Foundation.Parabolic.Vec3) => forcePressureGradientFunction (fun (x : Foundation.Parabolic.Vec3) => f (x, t)) hft y k) (fun (y : Foundation.Parabolic.Vec3) => forcedForceMod f hf (y, t) k) (fun (y : Foundation.Parabolic.Vec3) => ψ (y, t)) k

        On almost every time slice the mollified energy pairings are bounded by the dominating function and converge to the limiting pairing, which is the slice pairing of the unmollified fields.

        theorem CKN.Leray.integral_sq_timePartial_eq (ρ : RegMollifierProfile) (ε : ℝ) (hε : 0 < ε) {a : Foundation.Parabolic.Vec3 → Foundation.Parabolic.Vec3} (ha : IsInJ a) {f : Foundation.Parabolic.ParabolicPoint → Foundation.Parabolic.Vec3} (hf : IsLocallySquareIntegrableForce f) (k : Fin 3) {T : ℝ} (hT : 0 < T) {ψ : Foundation.Parabolic.Vec3 × ℝ → ℝ} (hψ : ContDiff ℝ (↑⊤) ψ) (hψc : HasCompactSupport ψ) {c d : ℝ} (hc : 0 < c) (hcd : c < d) (hdT : d < T) (hψs : ∀ z ∈ tsupport ψ, z.2 ∈ Set.Ioo c d) :
        ∫ (t : ℝ) in Set.Ioo 0 T, ∫ (x : Foundation.Parabolic.Vec3), forcedRegRep ρ ε hε ha hf (x, t) k * (forcedRegRep ρ ε hε ha hf (x, t) k * timePartial ψ (x, t)) = 2 * ∫ (t : ℝ) in Set.Ioo 0 T, leLimitT ρ ε hε ha hf ψ k t

        The mollifier limit of the space-time energy identity of one component.