Uniform primary weights and curl estimates #
A single enumeration of the joint band/label index transfers the existing weighted analysis without losing any inverse-edge factors. The reindexed strip retains the same domain, edge distance, and vanishing weight. Every constant is chosen before both the original band and the label.
Only the discrete scales are reindexed. The spatial edge geometry and its possibly vanishing weight are exactly the original ones.
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Surjectivity is the reason the constants also control every original label. It is never replaced by a separate bound for each label.
Enumeration, given by Classical.choose (exists_surjective_nat (ℕ × ι)).
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The actual slow scale on the joint index, in the (band,label) order
used by the phase and ODE constructions.
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Restrict genuine joint phase/ODE jets to the common strip, allowing a uniform polynomial change of slow scale.
This version retains the full inverse-edge polynomial in the majorant; it is not a polynomial-in-S replacement of the weight.
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Positivity is pointwise on the open strip. There is no positive minimum of the weight, even when it vanishes at the boundary.
Uniform band bound, given by `∃ C : ℝ, 0 ≤ C ∧ ∃ p : ℕ, ∀ l n, ‖a l n‖ ≤ C * s.epsilon n ^ β
- s.slow n ^ p`.
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The inverse matrix is differentiated after reindexing the genuine integrated entries. The determinant gap and entry bound are common to all labels; the target retains its full vanishing weight.
The exact normalization used by the primary covariance.
The normal inverse is computed from the actual jointly bounded normal, not supplied as a separately bounded potential coefficient.
This version permits radius and direction fields to vary with both band and label. All cylindrical connection terms are retained.
The half-power frequency gain is uniform even when the nonzero integer harmonic varies with the label.
The same actual integrated pulse matrix, now indexed jointly by band and label. Its entries are not independent input functions.
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Phase fundamental, defined pointwise by normalizedPulse ((A j).frame (n, l)) ((A j).lam (n, l)) ((A j).u (n, l)) ((A j).L (n, l)) (χ (n, l) x).
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Phase envelope, defined pointwise by referenceP ((A j).lam (n, l)) ((A j).u (n, l)) ((A j).L (n, l)) ((A j).L (n, l) * (χ (n, l) x).2).
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Phase cutoff fundamental, defined pointwise by cutoffPulse ((A j).frame (n, l)) ((A j).lam (n, l)) ((A j).u (n, l)) ((A j).L (n, l)) (χ (n, l) x).
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Phase slot envelope, defined pointwise by GaussianTailFlat.referenceSlotEnvelope ((A j).lam (n, l)) ((A j).u (n, l)) ((A j).L (n, l)) (χ (n, l) x).2.
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The matrix jets come from the actual parameter-dependent ODE and its actual middle-cutoff covariance integral, uniformly in both indices.
The actual smooth cutoff extension is controlled by the original Gaussian slot envelope, including its zero region.
Normal derivatives and the separated range are derived from the same joint phase data. The phase chart uses its actual unnormalized slot variable.
Uniform primary class from the actual joint phase/ODE construction. Only order-zero covariance separation and target data remain explicit.
Direct binding to the actual externally-cut LinearWaveBounds
coefficient. The cutoff occurs exactly once and every geometric class is
uniform in the label.
The Gaussian profile appears once in the actual coefficient.
Global slot-cutoff primary estimate: the actual cutoff extension and
its Gaussian envelope both vanish outside the slot. The edge weight is
still exactly sqrt zeta.
Apply this directly to a.withCutoff when the stronger Gaussian
slot-envelope bound has already been derived for its actual amplitude.
The primary half-power yields the advertised 1-kappa curl bound.