CutoffHomogenizationError #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The cutoff homogenization error #
This file exposes the measurable Section 3 observable
\mathcal E_{s,\infty,2}(\square_m; a_m, \bar\sigma_r\operatorname{Id}) on its
source domain 0 < s. The auxiliary comparator scale r remains explicit;
the paper's state variable is the specialization r = m.
The public definitions use the genuine coefficient cutoff, genuine running diffusivity, and the verified measurable representative. Their almost-everywhere characterizations retain the separate coefficient, domain, and comparator scale roles and identify the observable with CoarseGraining's literal homogenization error.
Main definitions #
cutoffHomogenizationErrorAtComparatorScale: coefficient and cube scalem, with running-diffusivity comparator taken at a separately specified scale.cutoffHomogenizationError: the manuscript specialization whose three scales are allm.
References #
- ABK26, definition
d.mathcal.E, (2.28). - ABK26, definition
d.mathcalS.def, Section 3.1.
The measurable cutoff homogenization error with coefficient and cube scale
m and running-diffusivity comparator taken at comparatorScale:
\mathcal E_{s,\infty,2}(\square_m; a_m, \bar\sigma_{\mathit{comparatorScale}}\operatorname{Id}).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The cutoff homogenization error with a separate comparator scale is measurable under the genuine cutoff-sample law.
The actual Section 3 cutoff homogenization error is measurable.
The public observable with a separate comparator scale is almost everywhere the verified raw manuscript expression.
The public observable with a separate comparator scale is almost everywhere
CoarseGraining's literal p = ∞, q = 2 homogenization error for a_m on
\square_m, normalized by \bar\sigma_{\mathit{comparatorScale}}.
The actual Section 3 observable is almost everywhere its raw manuscript
expression with coefficient, cube, and comparator scales all equal to m.
The actual Section 3 observable is almost everywhere exactly \mathcal E_{s,\infty,2}(\square_m; a_m, \bar\sigma_m\operatorname{Id}) in
CoarseGraining's literal source semantics.