High-contrast homogenization: Provider.Regularity.CorrectorGlobalRepresentative #
Imported from the Apache-2.0 HighContrastHomogenization development at commit
7a13dbcd8d6609264a713373f5c69ceeac870472.
Global representatives of projective local correctors #
Compatible local value and gradient L² classes are glued along the disjoint
shells of the centered-cube exhaustion. The resulting raw fields are strongly
measurable and agree almost everywhere with every stored local component.
The disjoint shell added at the nth stage of the centered-cube
exhaustion.
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Every exhaustion shell is measurable.
The nth shell lies in the nth exhaustion cube.
Adding the successor shell to an exhaustion cube gives the next cube.
Distinct exhaustion shells are disjoint.
The shells exhaust the whole Euclidean space.
Glue arbitrary shellwise fields into a global field.
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The shell lift reads the supplied field on each shell.
Measurable shellwise fields have a measurable shell lift.
A strongly measurable representative of the local H¹ value component on exhaustion cube n.
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The local gradient component on exhaustion cube n, expressed in the algebraic vector L²
space.
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A strongly measurable representative of the vector L² gradient on exhaustion cube n.
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A global scalar representative of the projective local value classes.
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A global Euclidean representative of the projective local gradient classes.
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The global value representative is strongly measurable.
The global gradient representative is strongly measurable.
On every exhaustion cube, the global scalar representative agrees almost
everywhere with the stored scalar L² component.
On every exhaustion cube, the global Euclidean gradient representative agrees almost everywhere with the vector form of the stored gradient component.
The global scalar representative is square-integrable on every exhaustion cube.
The global gradient representative is square-integrable on every exhaustion cube.
On each exhaustion cube, the global scalar representative agrees almost
everywhere with the canonical recovered local H¹ function.
On each exhaustion cube, the global Euclidean gradient representative
agrees almost everywhere with the weak gradient of the canonical recovered
local H¹ function.