Actual shifted transport primitives #
The source is integrated along a fixed translation direction. All integrals are Bochner integrals. Compact radial support is used to justify local fixed finite integration intervals, so ordinary derivatives pass under the integral without differentiating the translation parameter.
The translated radial integral and repeated integration by parts #
The integrals and derivatives in this file are actual Bochner integrals and Fréchet derivatives. The auxiliary variable may be the universal cover of a torus. A separately constructed directional primitive supplies the inverse identity; no decay estimate for the integral is assumed.
The actual line along which the auxiliary variable is translated.
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The translated integral over the radial support interval.
Equations
- NavierStokes.RadialAlias.aliasIntegral a b M v Y f = ∫ (u : ℝ) in a..b, f (NavierStokes.RadialAlias.shift M v Y u)
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The same integral over the whole radial line.
Equations
- NavierStokes.RadialAlias.wholeAlias M v Y f = ∫ (u : ℝ), f (NavierStokes.RadialAlias.shift M v Y u)
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Support in a fixed radial interval, uniformly in the auxiliary variable.
Equations
- NavierStokes.RadialAlias.RadiallySupported a b f = (Function.support f ⊆ Prod.fst ⁻¹' Set.Icc a b)
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The derivative in the slow radial coordinate, holding the auxiliary variable fixed.
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The actual auxiliary directional derivative.
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This is the chain rule d/du = ∂u + M L_v on the translated source.
Compact radial support makes the finite interval integral the whole-line integral.
One integration by parts, including the minus sign and the inverse factor.
Successive actual slow derivatives of directional primitives.
Equations
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When the inverse commutes with slow differentiation, these are literally
∂u^p (J^p f), as in the manuscript.
Arbitrarily many integrations by parts. The hypotheses concern actual directional derivatives, smoothness and support; no integral estimate is assumed.
The manuscript's literal ∂u^p J^p form, with the sign displayed.
The all-order gain has a constant uniform in the translation parameter Y and in M whenever the last source-jet bound is uniform.
Continuity gives a uniform bound near a parameter value on a compact interval. The parameter space need not be finite dimensional.
The parameter derivative of a jointly smooth integrand.
Equations
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Smoothness of a genuine integral over a fixed finite interval, with arbitrary normed parameter space and Banach-valued output.
A fixed translation along the transport direction.
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The past half-line primitive, in fixed integration coordinates.
Equations
- NavierStokes.TransportPrimitive.pastIntegral M v f z = ∫ (u : ℝ) in Set.Iic 0, f (NavierStokes.TransportPrimitive.shift M v z u)
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The complete translated radial integral.
Equations
- NavierStokes.TransportPrimitive.totalIntegral M v f z = ∫ (u : ℝ), f (NavierStokes.TransportPrimitive.shift M v z u)
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Compactification with a fixed radial cutoff.
Equations
- NavierStokes.TransportPrimitive.compactIntegral χ M v f z = NavierStokes.TransportPrimitive.pastIntegral M v f z - χ z.1 • NavierStokes.TransportPrimitive.totalIntegral M v f z
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The past integral is locally a finite interval integral with fixed endpoints.
All actual Fréchet derivatives retain radial support.
The entire Fréchet derivative commutes with the fixed-u past integral.
An ordinary derivative in any fixed direction, including a slow parameter.
Equations
- NavierStokes.TransportPrimitive.fixedDeriv w f z = (fderiv ℝ f z) w
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The exact transport identity, proved by the fundamental theorem of calculus.
The complete translated integral is constant along each transport line.
This derivative is exactly ∂U + M v·∂Y.
The cutoff product rule retains the actual ordinary radial derivative.
An explicit smooth transition with specified plateau thresholds.
Equations
- NavierStokes.TransportPrimitive.cutoff c d u = ((u - c) / (d - c)).smoothTransition
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The canonical cutoff has both plateaus strictly inside the support interval.
Equations
- NavierStokes.TransportPrimitive.interiorCutoff a b = NavierStokes.TransportPrimitive.cutoff ((2 * a + b) / 3) ((a + 2 * b) / 3)
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The complementary future integral used at the right support edge.
Equations
- NavierStokes.TransportPrimitive.futureIntegral M v f z = ∫ (u : ℝ) in Set.Ioi 0, f (NavierStokes.TransportPrimitive.shift M v z u)
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The alternative radial-coordinate formula is derived by translation.
Only the radial support length enters; there is no power of M in this bound.
Every order of the actual multilinear Fréchet derivative commutes with I.
Every order of the actual multilinear Fréchet derivative commutes with J.
Full binomial Leibniz bound. Every derivative of the cutoff is retained.
Uniform all-order operator-norm estimate from a finite list of genuine source and cutoff derivative bounds. The constant contains no translation parameter.
The future primitive has the same derivative commutation as the past primitive.
The total integral agrees with the separately formalized radial alias.