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(โก_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 โฆ Mu (โก_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 #
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 โก_m of
the centered triadic cube from the half-open realization used internally.
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.