Indexed weighted classes of actual stripped derivatives #
The index is a band, not a differentiable variable. Every derivative below is
Mathlib's iteratedFDeriv of the actual coefficient on an open domain.
Constants and polynomial degrees are chosen before the band and point.
The statements hold on real normed spaces, in particular on the Euclidean strips used by the construction. Radiality of the prescribed smooth weight is not needed for these closure results.
Geometry and positive indexed scales for a stripped coefficient family.
epsilon may in particular be Q n ^ h.
- domain : Set D
Epsilon of
StripData, of typeℕ → ℝ.Slow of
StripData, of typeℕ → ℝ.- delta : D → ℝ
- zeta : D → ℝ
- zeta_smooth : ContDiffOn ℝ (↑⊤) self.zeta self.domain
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Euclidean strip data: an abbreviation for StripData (EuclideanSpace ℝ (Fin d)).
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A common polynomial degree in S and the inverse edge distance is enough:
separate finite degrees can always be increased to their sum. The maximum
permits arbitrary positive delta, agreeing with delta⁻¹ when delta ≤ 1.
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Majorant, given by C * s.epsilon n ^ α * s.growth n x ^ p * w n x.
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Actual all-order bounds, uniform in band and point. The finite prefix in the last quantifier is useful for the higher Leibniz inequality.
- smooth (n : ℕ) : ContDiffOn ℝ (↑⊤) (f n) s.domain
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Mean class: an abbreviation for MemClass s (fun _ x => s.zeta x) α f.
Equations
- NavierStokes.WeightedClasses.MeanClass s α f = NavierStokes.WeightedClasses.MemClass s (fun (x : ℕ) (x_1 : D) => s.zeta x_1) α f
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Wave class: an abbreviation for MemClass s (fun n x => Real.sqrt (s.zeta x) * P n x) α f.
Equations
- NavierStokes.WeightedClasses.WaveClass s P α f = NavierStokes.WeightedClasses.MemClass s (fun (n : ℕ) (x : D) => √(s.zeta x) * P n x) α f
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Unweighted class: an abbreviation for MemClass s (fun _ _ => 1) α f.
Equations
- NavierStokes.WeightedClasses.UnweightedClass s α f = NavierStokes.WeightedClasses.MemClass s (fun (x : ℕ) (x_1 : D) => 1) α f
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Stage constants are deliberately not uniform in the stage index.
Equations
- NavierStokes.WeightedClasses.StageClasses s w α f = ∀ (stage : ℕ), NavierStokes.WeightedClasses.MemClass s w (α stage) (f stage)
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A bound on a band-dependent scalar. There is no spatial derivative of the discrete band index.
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The common-degree definition accepts the manuscript's separate logarithmic and inverse-edge polynomial degrees.
Actual higher Leibniz estimates add the two decay exponents.
Constant coefficients give nonzero examples of the unweighted class.
A fixed coefficient with uniform finite jet bounds is an order-zero
unweighted coefficient. This connects the class directly to JetBounds.
Wave products have the mean weight. This uses the actual Leibniz estimate
on coefficients, followed by (sqrt ζ * P)^2 ≤ ζ; no derivative identity for
the envelope P is postulated.
A normalized bounded radial weight makes the mean class an algebra.
An explicit radial graph operator with a band coefficient M and a
spatial coefficient a. The two directions can be radial and auxiliary.
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The expanded operator really is differentiation along its graph vector.
One explicit graph derivative loses at most κ in the band exponent.
The coefficient hypothesis is an actual all-jet bound on a, not a claim
about the desired output.
Graph iterate as an element of ℕ → ℕ → D → E | 0 => f | j + 1 => graphDerivative M a e v (graphIterate M a e v f j).
Equations
- NavierStokes.WeightedClasses.graphIterate M a e v f 0 = f
- NavierStokes.WeightedClasses.graphIterate M a e v f j.succ = NavierStokes.WeightedClasses.graphDerivative M a e v (NavierStokes.WeightedClasses.graphIterate M a e v f j)
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Every finite number of explicit graph derivatives has its finite loss.
Arbitrarily high additional stripped jets are still controlled at the same
resulting exponent, as recorded by MemClass.