CubeFieldData #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The frozen perturbation restricted to a sub-cube #
The p = 0 descendant-cube D_h bound applies the splitting identity, the weak
integration by parts and the Besov product estimate on a sub-cube R of the
frozen unit-cube carrier. Every analytic datum needed there is the restriction
of a datum of the frozen UnitCubeSkewW2Infinity structure:
- the weak first-derivative data
unitCubeDerivData his a single global function ofx; itsL^∞memberships restrict by measure monotonicity and its weak-derivative property restricts byHasWeakPartialDerivOn.restrict; - the entrywise Lipschitz representatives supplied by
Provider.DhBound.Lipschitz.UnitCubeare globally Lipschitz functions onVec d, so the Lipschitz hypothesis of the Besov product estimate holds on every sub-cube verbatim; - the frozen
L^∞boundgradientW1Infinityis an a.e. bound on the whole carrier, hence on every sub-cube.
Every declaration is an internal helper for the Section 2.4 sensitivity providers.
Restriction of the frozen weak-derivative data #
The L^∞ memberships of the frozen first derivative restrict to any
sub-carrier.
The frozen weak-derivative identity restricts to any open sub-carrier.
Globally Lipschitz representatives of the first derivative #
The entrywise globally Lipschitz representative of the frozen first-derivative field.
Equations
Instances For
The globally Lipschitz representative of the weak divergence ∇·h.
Equations
Instances For
Transfer to a sub-cube #
The Lipschitz representative of ∇·h agrees a.e. with the weak divergence
on every sub-cube of the frozen carrier.