Analytic infrastructure for the ε ↓ 0 limit of lem:aniso:comparison #
This module supplies the two analytic limits used in step 5b of the comparison lemma, where the
mollification parameter ε is sent to zero in the energy E of CIV.Comparison.EnergyInequality.
The spatial mollifier η_ε of CIV.Comparison.Mollifier has unit mass, so convolving a
bounded measurable function against it does not increase the squared L² mass on a ball, up
to enlarging the ball by ε; this is the quantitative form of the classical fact that an
approximate identity contracts on L² (integral_sq_mollifierKernel_convolution_le).
Combined with the uniform convergence of the mollification of a smooth compactly supported
approximant (from CIV.Comparison.CommutatorConvergence), this gives the
L²-of-every-ball convergence of the spatial mollification of a bounded a.e.-measurable time
slice to that slice as ε → 0 (tendsto_integral_sq_mollifySlice_sub).
The second limit concerns the DiPerna–Lions commutator. Its squared L² mass on a ball,
commutatorL2Sq, is a.e. strongly measurable in the time slice
(aestronglyMeasurable_commutatorL2Sq), and its time integral over a compact interval vanishes
as ε ↓ 0 (tendsto_integral_commutatorL2Sq), by dominated convergence from the per-slice
vanishing of CIV.Comparison.CommutatorConvergence.
The comparison proof uses both limits to pass to ε ↓ 0 in the integrated energy inequality
(CIV.ae_ae_le_barrier_of_referenceTime).
The mollifier is an L² contraction #
L² convergence of the spatial mollification #
L² convergence of mollifySlice #
Step 5b's core analytic fact: the spatial mollification of a bounded a.e.-measurable time
slice converges to it in L² of every ball as ε → 0.
Vanishing of the commutator, integrated over a compact time interval #
Joint measurability of the commutator's ball mass in the time slice #
Joint AEStronglyMeasurableness, in the pair (x, s) : Vec m × ℝ, of the DiPerna–Lions
commutator transported along a time-parametrized drift B, its divergence, and a time-parametrized
function q: from B and its divergence jointly measurable in space-time and q jointly
AEStronglyMeasurable on Vec m × ℝ against (volume : Measure (Vec m)).prod μs for any
SFinite measure μs on the time axis, the commutator itself — built at each fixed time slice
s from the space-time restrictions of B, its divergence, and q, and evaluated at the
spatial point x — is jointly AEStronglyMeasurable against the product measure. This is the
three-variable extension of
aestronglyMeasurable_diPernaLionsCommutator's two-variable argument: it bundles (x, s) into
one product factor and integrates the spatial variable y of the commutator's two defining
integrals out of it. It is the shared step behind aestronglyMeasurable_commutatorL2Sq, which
squares and ball-restricts this fact before integrating x out entirely.
Joint measurability of the DiPerna–Lions commutator's squared L² mass on a ball in the
time slice s: given B and its divergence jointly measurable in space-time and q a.e. strongly
measurable on ℝ^m × (τ₀, τ₊], the ball integral commutatorL2Sq is a.e. strongly measurable
as a function of s alone. This reduces to aestronglyMeasurable_diPernaLionsCommutator_prod
for the joint (x, s)-measurability of the commutator itself, then repeats a y-integration a
second time to remove x itself, over the ball, threading the ball restriction through an
indicator since AEStronglyMeasurable.integral_prod_right' integrates over the whole space.
The integrated vanishing of the commutator as ε ↓ 0 #
Step 5b's remaining analytic core: for an admissible drift and a locally bounded transported
function on a common domain I ⊇ [τ₀, τ₊], the commutator's squared L² mass, time-integrated
over (τ₀, τ₊], vanishes as ε ↓ 0. This combines the joint measurability just proved with the
per-slice ε → 0 vanishing tendsto_diPernaLionsCommutator_sq_integral and the per-slice L²
domination integral_sq_diPernaLionsCommutator_le via dominated convergence along the
countably-generated filter 𝓝[>] 0
(MeasureTheory.tendsto_integral_filter_of_dominated_convergence).