Bounds for the forced mild equation in frequency variables #
Pointwise bounds for the Duhamel integrands of eq:reg-mild-forced, the Abel
kernel integral, and the resulting bound on the frequency form of the right
hand side, uniform on bounded time intervals.
theorem
CKN.Leray.integral_norm_sq_eq_norm_sq_Lp
{α : Type u_1}
{E : Type u_2}
[MeasurableSpace α]
{μ : MeasureTheory.Measure α}
[NormedAddCommGroup E]
[InnerProductSpace ℂ E]
(f : ↥(MeasureTheory.Lp E 2 μ))
:
The squared L² norm is the integral of the squared pointwise norm.
theorem
CKN.Leray.ae_leraySymbol_fourier_of_mildJData
(b : ↥RealVectorL2)
(hb : RegularizedMildJData b)
:
A datum in J has transform fixed by the Leray symbol almost everywhere.
The pointwise bound for the frequency force integrand.
theorem
CKN.Leray.norm_forcedFourierMild_le
(b : ↥ComplexVectorL2)
{F : ℝ → ↥ComplexTensorL2}
{H : ℝ → ↥ComplexVectorL2}
{t T C : ℝ}
(ht : 0 ≤ t)
(htT : t ≤ T)
(hFC : ∀ s ∈ Set.Ioc 0 T, ‖F s‖ ≤ C)
(hH : MeasureTheory.IntegrableOn (fun (s : ℝ) => ‖H s‖) (Set.Ioc 0 T) MeasureTheory.volume)
(hC : 0 ≤ C)
:
The frequency form of the right-hand side of eq:reg-mild-forced is
bounded on [0, T] uniformly in time.