Cell estimates for spatially bounded pressure remainders #
A spatial supremum controlled in L^{3/2} in time gives the cell-radius
power needed for the harmonic part of the pressure gradient. The temporal
Hölder factor is retained explicitly before the Morrey normalization.
theorem
CKN.Core.Step4.pressure_remainder_time_power_bound
{H : ℝ → ENNReal}
(hH : AEMeasurable H MeasureTheory.volume)
{t r : ℝ}
(hr : 0 < r)
:
Temporal Hölder on a cell window produces the factor r^{2/5} for the
6/5 power integral of a function controlled in L^{3/2} in time.
theorem
CKN.Core.Step4.pressure_remainder_cylinder_power_bound
{F : Foundation.Parabolic.ParabolicPoint → ℝ}
{H : ℝ → ENNReal}
(hF : AEMeasurable F MeasureTheory.volume)
(hH : AEMeasurable H MeasureTheory.volume)
(hbound : ∀ᵐ (s : ℝ), ∀ (x : Foundation.Parabolic.Vec3), ‖F (x, s)‖ₑ ≤ H s)
{x : Foundation.Parabolic.Vec3}
{t r : ℝ}
(hr : 0 < r)
:
Foundation.Parabolic.Morrey.cylinderPowerIntegral (6 / 5) F (x, t) r ≤ MeasureTheory.volume (Foundation.Parabolic.vec3Ball x r) * (∫⁻ (s : ℝ), H s ^ (3 / 2)) ^ (4 / 5) * ENNReal.ofReal r ^ (2 / 5)
A spatial bound on almost every time slice gives a power-integral estimate on every cylinder, with its full spatial volume factor.
theorem
CKN.Core.Step4.pressure_remainder_morreyCell_bound
{κ : ℝ}
{F : Foundation.Parabolic.ParabolicPoint → ℝ}
{H : ℝ → ENNReal}
(hF : AEMeasurable F MeasureTheory.volume)
(hH : AEMeasurable H MeasureTheory.volume)
(hbound : ∀ᵐ (s : ℝ), ∀ (x : Foundation.Parabolic.Vec3), ‖F (x, s)‖ₑ ≤ H s)
{z : Foundation.Parabolic.ParabolicPoint}
{r : ℝ}
(hr : 0 < r)
:
The normalized cell estimate for a spatially bounded remainder. Its radius exponent is positive throughout the pressure-gradient bootstrap range.