Construction of the actual mean boundary operator by homogeneous-gradient completion and the Hilbert adjoint. No bounded inverse Laplacian on L² is assumed.
The only cutoff data: an actual compactly supported smooth scalar function.
- field : EulerSmoothLimit.Space → ℝ
Underlying field of
Cutoff, of typeSpace → ℝ. - compact : HasCompactSupport self.field
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Coordinate antisymmetrization of a genuine derivative.
Equations
- EulerMeanBoundary.curlMatrix A = WithLp.toLp 2 fun (i : Fin 3) => (A (EuclideanSpace.single (i + 1) 1)).ofLp (i + 2) - (A (EuclideanSpace.single (i + 2) 1)).ofLp (i + 1)
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The literal curl of the cutoff times a compact vector test, in ordinary L².
Equations
- EulerMeanBoundary.testCurl χ f = MeasureTheory.MemLp.toLp (EulerMeanCutoffCurl.vectorCurl fun (x : EulerSmoothLimit.Space) => χ.field x • ↑f x) ⋯
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The actual linear cutoff-curl operation on vector tests.
Equations
- EulerMeanBoundary.testCurlLinear χ = { toFun := EulerMeanBoundary.testCurl χ, map_add' := ⋯, map_smul' := ⋯ }
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The proved cutoff-dependent bound on the homogeneous space.
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- One or more equations did not get rendered due to their size.
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The bounded extension of actual cutoff-curl to the homogeneous Hilbert space.
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The Riesz/weak-Newtonian representation of the cutoff curl functional.
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The represented functional agrees exactly with the source's distributional pairing.
Compact vector tests determine the weak potential uniquely in the actual homogeneous space.
A genuine uniquely solvable weak Poisson/Riesz problem for the cutoff-curl functional.
The actual bounded positive mean boundary operator Tχ Tχ*.
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The actual test-level cutoff curl is solenoidal.
Closedness of the ordinary solenoidal space preserves the curl constraint under completion.
Fields supported in the cutoff's closed support, defined by actual L² restriction.
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Multiplication by the cutoff and then curl has no support outside the cutoff support.
Actual support is retained under homogeneous completion because L² restriction is continuous.
The constructed mean boundary output vanishes almost everywhere outside the cutoff support.
Symmetry follows from the actual Hilbert-adjoint construction.