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LeanPool.HighContrastHomogenization.Annealed.Measurability

High-contrast homogenization: Annealed.Measurability #

Imported from the Apache-2.0 HighContrastHomogenization development at commit 7a13dbcd8d6609264a713373f5c69ceeac870472.

Measurability of the coarse response over the coefficient space #

Every entry of the variational coarse block ๐€(โ–ก_m; ยท) of s.introduction is measurable for the canonical measurable structure of the coefficient space, which is the global sigma-field F = F(โ„^d) generated by the smooth linear statistics. Measurability is therefore a fact about the coefficient space alone: it holds for every law at once, and the well-formedness predicate HasMeasurableCoarseBlock that e.Theta.m presupposes never has to be assumed.

The entries reduce to the variational quantity Mu at the four doubled vectors built from a pair of basis directions, so the whole statement is the measurability of a โ†ฆ Mu (โ–ก_m) Q a. That is obtained by transporting the coarse-grained energy along a representative map into CoarseGraining's exact coarse-source carrier, whose own local sigma-fields are generated by exactly the same bilinear test integrals: the representative map pulls the generators back to the generators, and Mu only sees the almost everywhere class of the field, so the value is unchanged.

A representative in the exact coarse-source carrier #

theorem HCPolySupport.HighContrast.exists_sourceCarrier_ae_eq {d : โ„•} (a : CoeffSpace d) :
โˆƒ (b : Source.Coarse.Carrier d), โ†‘โ†‘a =แต[MeasureTheory.volume] โ†‘b

Every point of the coefficient space is represented, up to a null set, by a field of the exact coarse-source carrier: a measurable field that is uniformly elliptic on every ball with reciprocal constants. The sample's ellipticity constants on that ball supply the reciprocal constant, once normalized to lie in (0, 1].

The chosen coarse-source representative of a point of the coefficient space.

Equations
Instances For

    The coarse-source representative carries the sample's field.

    The bilinear test integrals of the coarse-source carrier pull back along the representative map to the generating linear statistics of F(U): both are the same integral, and the two integrands agree almost everywhere.

    The representative map is measurable for the global sigma-fields: it pulls each generator of the coarse-source carrier back to a generator of F(โ„^d), the test functions of the two families being the same.

    The variational quantity is measurable #

    The variational quantity does not distinguish the open realization โ–ก_m of the centered triadic cube from the half-open realization used internally.

    theorem HCPolySupport.HighContrast.measurable_Mu_centeredCube {d : โ„•} (m : โ„ค) (Q : BlockVec d) :
    Measurable fun (a : CoeffSpace d) => Mu (centeredCube d m) Q โ†‘โ†‘a

    The coarse-grained energy of a centered cube is measurable on the coefficient space, for the global sigma-field F(โ„^d). The coarse-source energy is local for the bilinear test sigma-field of the cube, hence measurable for the global one, and the representative map is measurable and leaves the energy unchanged.

    The coarse response is measurable #

    Every entry of the coarse block response on a centered cube is measurable for the canonical measurable structure of the coefficient space: the entries are the variational quantities at the four doubled vectors built from a pair of basis directions.

    The coarse response is measurable over every law: the well-formedness predicate that e.Theta.m presupposes is a theorem of the coefficient space, not an assumption on the law.