Uniform stripped jets on a common cover #
The input of the copy solve is evaluated on the common torus. The two actual argument maps below include the integration time as a variable. Their affine derivatives, the native time scale, and adjacent-band changes give estimates whose constants precede the band, copy, and source. No native periodicity of the source is used.
CCS: an abbreviation for CommonCoverSolve.Geometry.
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A point-dependent bound on a finite prefix of actual Fréchet jets.
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- NavierStokes.CommonCoverClass.EnvelopeJets m f envelope = ∀ j ≤ m, ∀ (x : X), ‖iteratedFDeriv ℝ j f x‖ ≤ envelope x
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The weight is evaluated at the same point in both factors; it need not be differentiated in this bound.
Joint slow/common-coordinate/integration-time space.
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Native argument, given by (w.1.1, ((g.coordinates k w.1.2).1, w.2)).
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- NavierStokes.CommonCoverClass.nativeArgument g k w = (w.1.1, (NavierStokes.CommonCoverSolve.Geometry.coordinates g k w.1.2).1, w.2)
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Source argument, given by (w.1.1, g.path k w.1.2 w.2).
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- NavierStokes.CommonCoverClass.sourceArgument g k w = (w.1.1, NavierStokes.CommonCoverSolve.Geometry.path g k w.1.2 w.2)
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Native linear as an element of Joint P →L[ℝ] P × Plane.
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Source linear as an element of Joint P →L[ℝ] P × Plane.
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One common affine cost for both maps. Its value is independent of the copy index and of the slow parameter space.
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The fixed native basis has columns v_r,v_t; only the second column is
multiplied by the actual time coefficient.
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- NavierStokes.CommonCoverClass.scaledBasis B ci hci = (NavierStokes.TorusAverages.transverseChart ci hci).trans B
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Band geometry, bundling gap, basis, center.
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Geometry cost, constructed using 1.
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This constant depends on the fixed native basis and the covering-gap budget, and is chosen before the band, center, copy, or source.
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Reinsert the actual current slot time after solving the joint equation.
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Current linear as an element of P × Plane →L[ℝ] Joint P.
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This is a bound on all joint input jets of the actual ODE coefficient.
Both factors are evaluated at their correct, generally different, arguments. In particular the source is not replaced by a native-periodic one.
Every radial and slow weight is unchanged by the source path. For each
requested jet prefix the only change is a fixed additional power of S.
This also applies with weight = sqrt(zeta) * P whenever P depends only
on the retained slow parameters.
The exact ratio (Q_n / Q_m)^a, written without a division.
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- NavierStokes.CommonCoverClass.bandRatio a n m = 2 ^ ((↑m - ↑n) * a)
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Slow point: an abbreviation for ℝ × (ℝ × ℝ).
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Normalized slow chart, given by (ChartScales.Q n ^ (-(1 / 2 : ℝ)) * x.1, (ChartScales.Q n ^ (-D) * x.2.1, ChartScales.Q n ^ (-1 : ℝ) * x.2.2)).
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Coarsest of a pair of simultaneously active levels.
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All hypotheses other than the source class concern the actual affine maps and the prescribed weights/scales. No derivative bound on the pulled-back source is a premise. Polynomial map and edge costs do not change the small-scale exponent.
A strip over a linear parameter projection. Its weights are the actual base weights, so retaining the parameter preserves them exactly.
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Source strip, given by parameterStrip s (ContinuousLinearMap.fst ℝ P Plane).
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Joint strip, given by parameterStrip s ((ContinuousLinearMap.fst ℝ P Plane).comp (ContinuousLinearMap.fst ℝ (P × Plane) ℝ)).
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Actual all-order class transport along the common-cover path. The
indexed band map allows a tail such as band n = n+4. Constants are uniform
in all choices of centers and lifted copies.
Either direction of a bounded covering change. The inverse is a map on the universal cover; no extra periodicity is imposed on its input.
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- NavierStokes.CommonCoverClass.coverChange forward d = if forward = true then ↑(NavierStokes.CommonCoverSolve.coverPower d) else ↑(NavierStokes.CommonCoverSolve.coverPower d).symm
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Band common chart, given by (bandChart D n m).prodMap (coverChange forward gap).
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- NavierStokes.CommonCoverClass.bandCommonChart D n m forward gap = (NavierStokes.CommonCoverClass.bandChart D n m).prodMap (NavierStokes.CommonCoverClass.coverChange forward gap)
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Class transport under the actual simultaneous slow-chart and bounded covering change. The weight/edge identities express the same physical profile in the two charts; they are geometric identities, not jet bounds.
A concrete strip with the physical profile weight and logarithmic distance. The independent index chooses the actual dyadic band.
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Here the domain and the edge identity are proved from actual profile homogeneity. Only the prescribed additional weight is transported.
The actual mean class is preserved, with exactly the same small-scale exponent, under all overlapping band/common-cover changes.
The wave envelope is transported at its actual point. The radial factor and edge distance are invariant; the slot profile is pulled back exactly and is not replaced by another label's profile.
Normalized small slow-box coordinates, using the actual widths from the coloring construction.
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- NavierStokes.CommonCoverClass.meshCoordinate D L x j = (x j - NavierStokes.SlotColoring.width D j L.1 * ↑(L.2.1 j)) / NavierStokes.SlotColoring.width D j L.1
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Mesh point, defined pointwise by SlotColoring.width D j L.1 * x j + SlotColoring.width D j L.1 * (L.2.1 j : ℝ).
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- NavierStokes.CommonCoverClass.meshPoint D L x j = NavierStokes.SlotColoring.width D j L.1 * x j + NavierStokes.SlotColoring.width D j L.1 * ↑(L.2.1 j)
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Mesh linear, constructed using ContinuousLinearMap.pi.
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Mesh offset, defined pointwise by (SlotColoring.width D j L.1 * (L.2.1 j : ℝ) - SlotColoring.width D j M.1 * (M.2.1 j : ℝ)) / SlotColoring.width D j M.1.
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Mesh transition, given by meshOffset D L M + meshLinear D L M x.
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Only physical-box adjacency is assumed; the normalized coordinate change is bounded uniformly over all box indices and levels.
The translation is controlled by genuine support overlap. It is not bounded by assuming the lattice copy indices themselves are bounded.
The covering budget used in the path estimate is now instantiated from the actual adjacent labels and their coarsest common native index.
The actual radial/time eigenvector basis, not an abstract invertible basis supplied as an assumption.
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The exact manuscript path, with the actual c_i and v_t.
Any finite collection of active levels with the geometric level-span bound has a genuine coarsest member and a uniform covering budget to it.