LocalizedAssembly #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The localized quantities are measurable functions of the sample #
The two localized quantities of Section 5.1 are suprema over the whole normalized forcing class, which is not countable, of quantities attached to almost-everywhere classes of Sobolev functions. They are nevertheless measurable, with no regularity hypothesis at all.
Both inner quantities are countable suprema of ball averages: the L^∞ norm of
a difference by the essential-supremum identification, and the Hölder seminorm
of the continuous representative by the identification that also reads ⊤ where
no continuous representative exists. A ball average of the solution is a
measurable function of the sample, and it is continuous in the forcing field —
by the energy estimate, the zero-trace Poincaré inequality and Cauchy-Schwarz,
none of which sees any regularity — so each inner quantity is lower
semicontinuous in the datum and its supremum over the normalized class is
attained on the countable subclass that approximates that class uniformly.
Main results #
measurable_localizedRegularity,measurable_localizedError— unconditional.measurable_percolationScaleTotal— the resulting measurability of the percolation scale.
References #
- ABK26, the localized error and regularity quantities and the chains of good cubes of Section 5.1.
1. The inner quantities as ball-average gauges #
The infimum over the continuous representatives is the ball-average Hölder
gauge, including the value ⊤ where no continuous representative exists.
The L^∞ norm of the difference of two solutions is the ball-average
supremum gauge.
2. The localized regularity #
The localized regularity is a measurable function of the sample.
3. The localized error #
The localized error is a measurable function of the sample.
4. The chain to the percolation scale #
The percolation scale is a measurable function of the sample, with no
hypothesis beyond the model: the two localized quantities are measurable, hence
so are the good cube event, the event Q, and the least scale beyond which no
light crossing occurs.