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LeanPool.EscauriazaSereginSverak.PartV.ForcedHeatCriticalFinal

The critical L⁵ and L^∞ L³ bounds for the smooth forced heat response #

Letting the regularization vanish in the window estimates and applying Hölder's inequality to Y = ∫∫ |Z| |g|² gives, with B = ∫∫ |g|^{5/2},

∫∫ |Z|⁵ ≤ C B² and ∫ |Z(t)|³ ≤ C B^{6/5} for 0 ≤ t ≤ τ,

the smooth-data form of eq:pv-stokes-l5 in lem:pv-stokes, with an absolute constant C.

The space-time L⁵ integral of the response is bounded by C Y^{5/3}.

theorem ESS.response_rpow_three_le {g : Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ} (hg : ∀ (i j : Fin 3), ContDiff ℝ (↑⊤) (g i j)) (hgc : ∀ (i j : Fin 3), HasCompactSupport (g i j)) (hgpos : ∀ (i j : Fin 3), tsupport (g i j) ⊆ {p : CKN.Foundation.Parabolic.Vec3 × ℝ | 0 < p.2}) {τ : ℝ} (hτ : 0 ≤ τ) {t : ℝ} (ht : t ∈ Set.Icc 0 τ) :

For every time in the window, the spatial L³ integral of the response is bounded by 3 Y.

theorem ESS.response_forcing_holder {g : Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ} (hg : ∀ (i j : Fin 3), ContDiff ℝ (↑⊤) (g i j)) (hgc : ∀ (i j : Fin 3), HasCompactSupport (g i j)) (hgpos : ∀ (i j : Fin 3), tsupport (g i j) ⊆ {p : CKN.Foundation.Parabolic.Vec3 × ℝ | 0 < p.2}) {τ : ℝ} (hτ : 0 ≤ τ) :

Hölder's inequality for Y = ∫∫ |Z| |g|² with exponents 5 and 5/4.

The absolute constant of the smooth-data critical estimate.

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    theorem ESS.response_critical_estimate {g : Fin 3 → Fin 3 → CKN.Foundation.Parabolic.Vec3 × ℝ → ℝ} (hg : ∀ (i j : Fin 3), ContDiff ℝ (↑⊤) (g i j)) (hgc : ∀ (i j : Fin 3), HasCompactSupport (g i j)) (hgpos : ∀ (i j : Fin 3), tsupport (g i j) ⊆ {p : CKN.Foundation.Parabolic.Vec3 × ℝ | 0 < p.2}) {τ : ℝ} (hτ : 0 ≤ τ) :

    The critical estimate for the smooth forced heat response: with B = ∫∫_{(0,τ]} |g|^{5/2}, ∫∫_{(0,τ]} |Z|⁵ ≤ C B² and ∫ |Z(t)|³ ≤ C B^{6/5} for 0 ≤ t ≤ τ, with an absolute constant C.