Local Energy L4 #
Supporting estimates for the Navier–Stokes development.
theorem
CKN.scalarH1L4_bound
{x₀ : Foundation.Parabolic.Vec3}
{r : ℝ}
(hr : 0 < r)
(v : H1Function (euclideanBall x₀ r))
(h3 : MeasureTheory.MemLp v.toFun 3 (MeasureTheory.volume.restrict (euclideanBall x₀ r)))
:
MeasureTheory.MemLp v.toFun 4 (MeasureTheory.volume.restrict (euclideanBall x₀ r)) ∧ MeasureTheory.eLpNorm v.toFun 4 (MeasureTheory.volume.restrict (euclideanBall x₀ r)) ^ 4 ≤ MeasureTheory.eLpNorm v.toFun 3 (MeasureTheory.volume.restrict (euclideanBall x₀ r)) ^ 2 * (ENNReal.ofReal sobolevPoincareFaithfulC5 * (MeasureTheory.eLpNorm v.grad 2 (MeasureTheory.volume.restrict (euclideanBall x₀ r)) + (ENNReal.ofReal r)⁻¹ * MeasureTheory.eLpNorm v.toFun 2 (MeasureTheory.volume.restrict (euclideanBall x₀ r)))) ^ 2
The spatial interpolation step used for manuscript label lem:lei-L4 of the
Escauriaza–Seregin–Šverák manuscript:
an H¹ slice in L³ belongs to L⁴, with a bound that retains the L³
factor and the Sobolev L⁶ factor for later time integration.