Canonical axis jets without a negative squared-radius extension #
The squared-radius jets are the iterates of the integral Hadamard operator on the signed radial variable. They are genuine right derivatives at the axis and genuine ordinary derivatives at positive squared radius.
Radial jet, given by EvenSmoothDescent.radialIterate (fun s => F (s, z)) k r.
Equations
- NavierStokes.BoundaryAxisJets.radialJet F k r z = NavierStokes.EvenSmoothDescent.radialIterate (fun (s : ℝ) => F (s, z)) k r
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Axis jet, given by radialJet F k (Real.sqrt p.1) p.2.
Equations
- NavierStokes.BoundaryAxisJets.axisJet F k p = NavierStokes.BoundaryAxisJets.radialJet F k (√p.1) p.2
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Locality of the genuine Hadamard iterates #
Localized, given by EvenSmoothDescent.localized R (fun r => F (r, p.2)) p.1.
Equations
- NavierStokes.BoundaryAxisJets.localized R F p = NavierStokes.EvenSmoothDescent.localized R (fun (r : ℝ) => F (r, p.2)) p.1
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Genuine joint smoothness of the signed radial pullbacks #
Radial partial, given by deriv (fun r => F (r, p.2)) p.1.
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Reduce family, given by EvenSmoothDescent.radialDerivative (fun r => F (r, p.2)) p.1.
Equations
- NavierStokes.BoundaryAxisJets.reduceFamily F p = NavierStokes.EvenSmoothDescent.radialDerivative (fun (r : ℝ) => F (r, p.2)) p.1
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The input needed by positive-order lower sources: every canonical squared-radius jet has a genuinely smooth, even signed radial pullback.
Holomorphy is preserved by the actual radial derivative #
The radial difference quotients converge in the supremum norm on every compact parameter disk. The holomorphic limit theorem therefore applies to the genuine radial derivative.
Segment: an abbreviation for ↥(Icc (0 : ℝ) 1).
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Segment extend, given by f (projIcc 0 1 zero_le_one t).
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Integration of a compact continuous family is complex linear.
Equations
- One or more equations did not get rendered due to their size.
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Every canonical right jet has holomorphic parameter slices, including at the axis, under the actual joint-smooth and holomorphic input hypotheses.
Actual mixed parameter jets #
Complex partial, given by deriv (fun z => F (p.1, z)) p.2.
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Complex jet, given by iteratedDeriv m (fun z => F (p.1, z)) p.2.
Equations
- NavierStokes.BoundaryAxisJets.complexJet F m p = iteratedDeriv m (fun (z : ℂ) => F (p.1, z)) p.2
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Mixed axis jet, given by iteratedDeriv m (fun z => axisJet F k (p.1, z)) p.2.
Equations
- NavierStokes.BoundaryAxisJets.mixedAxisJet F k m p = iteratedDeriv m (fun (z : ℂ) => NavierStokes.BoundaryAxisJets.axisJet F k (p.1, z)) p.2
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Every fixed mixed jet has the genuine joint regularity required of a
lower-order source, without any negative-X extension.
Interior localization retaining the full radial domain #
Interior bump, bundling rIn, rOut, rIn_pos, rIn_lt_rOut.
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Interior cutoff, given by interiorBump hS hSR r * interiorBump hS hSR (-r).
Equations
- NavierStokes.BoundaryAxisJets.interiorCutoff hS hSR r = ↑(NavierStokes.BoundaryAxisJets.interiorBump hS hSR) r * ↑(NavierStokes.BoundaryAxisJets.interiorBump hS hSR) (-r)
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Interior localized, given by interiorCutoff hS hSR p.1 • F p.
Equations
- NavierStokes.BoundaryAxisJets.interiorLocalized hS hSR F p = NavierStokes.BoundaryAxisJets.interiorCutoff hS hSR p.1 • F p
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No radial radius is lost: localization is chosen around each interior point while the canonical jet itself remains unchanged.