Spatial convolution with smooth compact kernels #
For a smooth compactly supported kernel k on ℝ³ and a spatial field h,
the convolution k ⋆ h is smooth, its partial derivatives are the
convolutions with the partial derivatives of k, it is bounded in L² by
‖k‖₁ ‖h‖₂, and it satisfies the whole-space integration by parts identity.
These are the spatial tools of the energy argument in
lem:localized-vorticity-energy of the Escauriaza–Seregin–Šverák manuscript.
Convolution of a spatial field h with a kernel k.
Equations
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The partial derivative of a kernel in the coordinate direction j.
Equations
- CKN.vlDeriv k j y = (fderiv ℝ k y) (CKN.basisVec j)
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Smooth compactly supported kernels.
Equations
- CKN.IsVlKernel k = (ContDiff ℝ (↑⊤) k ∧ HasCompactSupport k)
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The convolution of a locally integrable field with a smooth compact kernel is smooth.
Differentiating a convolution differentiates the kernel.
The convolution partial derivative, in CKN notation.
Young's inequality in L² for a smooth compact kernel of any sign.
Integration by parts for kernel convolutions of L² fields.
Convolution is linear in the kernel.