Slice agreement for pressure extensions #
The spatial extensions are independent of exponent on every tensor that is integrable at two exponents. The proof reads them as time slices of extensions of a tensor supported on a finite time interval.
noncomputable def
CKN.Leray.rieszPressurePackageTimeTensor
(F : Fin 3 → Fin 3 → Foundation.Parabolic.Vec3 → ℝ)
(i j : Fin 3)
(z : Foundation.Parabolic.Vec3 × ℝ)
:
The space-time tensor component restricted to the time interval (0,1) and extended by zero
elsewhere.
Equations
Instances For
theorem
CKN.Leray.rieszPressureSlice_ae_eq_of_memLp_common
(r : ℝ)
(hr : 1 < r)
(s : ℝ)
(hs : 1 < s)
(F : Fin 3 → Fin 3 → Foundation.Parabolic.Vec3 → ℝ)
(hFr : ∀ (i j : Fin 3), MeasureTheory.MemLp (F i j) (ENNReal.ofReal r) MeasureTheory.volume)
(hFs : ∀ (i j : Fin 3), MeasureTheory.MemLp (F i j) (ENNReal.ofReal s) MeasureTheory.volume)
:
↑↑(rieszPressureSlice r hr fun (i j : Fin 3) => MeasureTheory.MemLp.toLp (F i j) ⋯) =ᵐ[MeasureTheory.volume]
↑↑(rieszPressureSlice s hs fun (i j : Fin 3) => MeasureTheory.MemLp.toLp (F i j) ⋯)
theorem
CKN.Leray.rieszPressureSpaceTime_slice_exponent_agreement
(r : ℝ)
(hr : 1 < r)
(s : ℝ)
(hs : 1 < s)
(F : Fin 3 → Fin 3 → Foundation.Parabolic.Vec3 × ℝ → ℝ)
(hFr : ∀ (i j : Fin 3), MeasureTheory.MemLp (F i j) (ENNReal.ofReal r) MeasureTheory.volume)
(hFs : ∀ (i j : Fin 3), MeasureTheory.MemLp (F i j) (ENNReal.ofReal s) MeasureTheory.volume)
:
∀ᵐ (t : ℝ), ∃ (hFrt :
∀ (i j : Fin 3),
MeasureTheory.MemLp (fun (x : Foundation.Parabolic.Vec3) => F i j (x, t)) (ENNReal.ofReal r) MeasureTheory.volume)
(hFst :
∀ (i j : Fin 3),
MeasureTheory.MemLp (fun (x : Foundation.Parabolic.Vec3) => F i j (x, t)) (ENNReal.ofReal s)
MeasureTheory.volume),
↑↑(rieszPressureSlice r hr fun (i j : Fin 3) =>
MeasureTheory.MemLp.toLp (fun (x : Foundation.Parabolic.Vec3) => F i j (x, t)) ⋯) =ᵐ[MeasureTheory.volume]
↑↑(rieszPressureSlice s hs fun (i j : Fin 3) =>
MeasureTheory.MemLp.toLp (fun (x : Foundation.Parabolic.Vec3) => F i j (x, t)) ⋯)