Coarse-graining support: Support.Sobolev.Fractional.EuclideanWspSmoothDualFieldPairing #
Imported from the Apache-2.0 CoarseGraining development at commit
c7ddd76c08ade64fed1b8d2ca51be14dfee8deb4.
Smooth-dual pairing with actual fractional Sobolev fields #
This module closes the smooth-test dual pairing against an actual fractional
Sobolev field which also has the required L² representative.
noncomputable def
HCPolySupport.cubeEuclideanWspGraphPointOfField
{d : ℕ}
{Q : TriadicCube d}
{s : ↑FractionalOrder}
{p : FiniteLpExponent}
(F : CubeEuclideanWspField Q s p)
:
The ambient full-norm graph point of an actual fractional field.
Equations
- One or more equations did not get rendered due to their size.
Instances For
theorem
HCPolySupport.cubeEuclideanWspKernel_sub
{d : ℕ}
(s : ↑FractionalOrder)
(p : FiniteLpExponent)
(F G : Vec d → Vec d)
:
(cubeEuclideanWspKernel s p fun (x : Vec d) => F x - G x) = fun (z : Vec d × Vec d) =>
cubeEuclideanWspKernel s p F z - cubeEuclideanWspKernel s p G z
noncomputable def
HCPolySupport.cubeEuclideanWspFieldSub
{d : ℕ}
{Q : TriadicCube d}
{s : ↑FractionalOrder}
{p : FiniteLpExponent}
(F G : CubeEuclideanWspField Q s p)
:
CubeEuclideanWspField Q s p
Subtract fractional cube fields pointwise, retaining Euclidean L^p membership
and L^p membership of the Gagliardo difference kernel.
Equations
- HCPolySupport.cubeEuclideanWspFieldSub F G = { toField := fun (x : HCPolySupport.Vec d) => F.toField x - G.toField x, euclideanMemLp := ⋯, euclideanMemWsp := ⋯ }
Instances For
noncomputable def
HCPolySupport.cubeEuclideanNormalizedFieldPairing
{d : ℕ}
{Q : TriadicCube d}
{s : ↑FractionalOrder}
{p : FiniteLpExponent}
(F : CubeEuclideanLpField Q FiniteLpExponent.two)
(G : CubeEuclideanWspL2Field Q s p)
:
The literal normalized-cube pairing of an L² field with an actual
fractional Sobolev field.
Equations
Instances For
theorem
HCPolySupport.ennreal_ofReal_abs_cubeEuclideanNormalizedFieldPairing_le
{d : ℕ}
{Q : TriadicCube d}
{s : ↑FractionalOrder}
{p : FiniteLpExponent}
(F : CubeEuclideanLpField Q FiniteLpExponent.two)
(G : CubeEuclideanWspL2Field Q s p.conjugate)
:
The literal normalized-cube pairing is controlled by the smooth negative fractional-Sobolev dual norm.