Smooth zero extension across both moving radial edges #
The raw coefficient is used only inside the annulus. Gaussian bounds on its actual full derivative tensors prove that its literal zero extension has all derivatives zero on both moving boundary hypersurfaces.
Extension as an element of E.
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- NavierStokes.WaveEdgeExtension.extension ρ a b f x = if x ∈ NavierStokes.WaveEdgeExtension.window ρ a b then f x else 0
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A local bound on actual tensors from the interior side of an edge.
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A smooth defining function may replace the straight edge coordinate. Its actual derivative controls its distance by ambient distance.
Log coordinate, given by WeightedRadialPrimitive.logPosition a (ρ x).
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Boundary controls as an element of Prop.
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Extended jets, defined pointwise by extension ρ a b (iteratedFDeriv ℝ n f) x.
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- NavierStokes.WaveEdgeExtension.extendedJets ρ a b f x n = NavierStokes.WaveEdgeExtension.extension ρ a b (iteratedFDeriv ℝ n f) x
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Explicit two-edge Gaussian bounds #
Flat weight, given by WeightedRadialPrimitive.zeta cL cR (WeightedRadialPrimitive.logLength a b) (logCoordinate ρ a x).
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Edge growth, given by max 1 (WeightedRadialPrimitive.delta (WeightedRadialPrimitive.logLength a b) (logCoordinate ρ a x))⁻¹.
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The actual square-root two-edge weight supplies both boundary controls. The envelope only needs to be continuous near the boundary, where its local bound is absorbed into the constant.
Reduce the actual native class estimate without differentiating the weight or discarding any of its flat-edge factor.
Smooth zero extension of an actual native coefficient. No smoothness of the raw coefficient is assumed outside the open moving annulus.
The actual moving radial profile in native coordinates #
Native point: an abbreviation for PhaseCalculus.Slow × TorusInverse.Plane.
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Native slow domain, given by {x | 0 < x.1.2.2}.
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Native radius, given by PrimaryTargetBounds.profileRadius h x.1.
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Native extension, given by extension (nativeRadius F.data.h) (PrimaryTargetBounds.leftRadius W) (PrimaryTargetBounds.rightRadius W) f.
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The literal extension is zero on all nonpositive physical radii.
Direct adapter for the exact moving weight used by the primary and
signed constructions, in the native (R,Z,T,u,v) variable ordering.
Exact comparison with the inner-coordinate edge distance #
The inverse edge factor in the actual inner-coordinate estimates is bounded by the radial logarithmic factor, with constant exactly one.
Regularity of the literal native extension, including its exact full-tensor values at both moving edges.
- smooth : ContDiffOn ℝ (↑⊤) (nativeExtension W f) nativeSlowDomain
- jets (n : ℕ) (x : NativePoint) : x ∈ nativeSlowDomain → iteratedFDeriv ℝ n (nativeExtension W f) x = nativeExtension W (iteratedFDeriv ℝ n f) x
- edge (n : ℕ) (x : NativePoint) : x ∈ nativeSlowDomain → nativeRadius F.data.h x = PrimaryTargetBounds.leftRadius W ∨ nativeRadius F.data.h x = PrimaryTargetBounds.rightRadius W → iteratedFDeriv ℝ n (nativeExtension W f) x = 0
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The constructed primary pulse and its actual envelope #
Apply the extension construction directly to the actual Cramer-scaled homogeneous pulse. The only raw regularity premise is its already-derived native interior jet estimate.
Localization before radial extension #
Enlarge only the domain of an already localized coefficient. The same constants bound every derivative; outside the native chart its actual zero germ supplies all zero tensors.
A domain for the literal localized field over the full open native annulus. Its growth allows the source chart scale and the given slow factor.
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The source chart need only cover points where the actual localized formula has a nonzero germ. This permits slow-cell and outer-slot localization before taking the radial zero extension.
Extending by zero does not enlarge an interior tensor bound. This pointwise form keeps any constants already uniform in the external labels.
Every pre-existing uniform native constant and polynomial degree is unchanged by the literal extension. The regularity at the new radial boundary is supplied by the construction above.
The same extension in the mean-field variable ordering #
The actual permutation from (R,((T,Z),Y)) to ((R,(Z,T)),Y).
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Mean extension, given by nativeExtension W f (meanNative x).
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Reordering the coordinates preserves the norm of every full tensor.