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LeanPool.EscauriazaSereginSverak.Endpoint.LocalHeatGainTrace

Zero initial trace for solutions vanishing near the initial time #

A square-integrable distributional solution of ∂ₜ u - Δ u = div H + f on ℝ³ × (a, b) that vanishes for t < a + δ has, for every spatial test ψ, a spatial pairing t ↦ ∫ u(x, t) ψ(x) dx with a continuous version on [a, b] vanishing at a: the pairing has an integrable distributional time derivative. This is the zero initial trace used with the energy estimate of lem:localized-vorticity-energy in the proof of lem:local-heat-gain.

The time derivative of a separated test ψ(x) θ(t).

The spatial derivative of a separated test ψ(x) θ(t).

The second spatial derivative of a separated test ψ(x) θ(t).

(x, t) ↦ g(x) is square integrable on a slab for square integrable g.

Continuous compactly supported spatial functions are square integrable on slabs.

theorem ESS.exists_continuous_version_zero_trace {a b δ : ℝ} (hab : a < b) (hδ : 0 < δ) {P Q : ℝ → ℝ} (hPint : MeasureTheory.Integrable P (MeasureTheory.volume.restrict (Set.Ioo a b))) (hQint : MeasureTheory.Integrable Q (MeasureTheory.volume.restrict (Set.Ioo a b))) (hweakP : CKN.HasWeakDerivOn (Set.Ioo a b) P Q) (hP0 : ∀ t < a + δ, P t = 0) :
∃ (c : ℝ → ℝ), ContinuousOn c (Set.Icc a b) ∧ c a = 0 ∧ ∀ᵐ (t : ℝ) ∂MeasureTheory.volume.restrict (Set.Ioo a b), c t = P t

A function on (a, b) with an integrable distributional derivative that vanishes near a has a continuous version on [a, b] vanishing at a.

A distributional solution on a slab vanishing near the initial time has a zero initial trace.