Coherence of the actual correction recurrence #
The incoming chart comparisons retain every radial, free auxiliary and angular variable. The actual initialized state and labeled coefficients start the induction together. The two literal wave constructions supply the transport used by the mean, pressure, and alias operations.
Full-fiber coherence of the actual signed Gaussian error #
The differentiated native cutoff is transported before the copy sum is taken. The source complement is retained, and the same copy index is used throughout. The final field is the actual conjugate-pair Gaussian block, with its full angular variable.
The invertible chart transports the actual directional derivative, including the totalized derivative at a nonsmooth point.
Exact transport of the computed Gaussian error. Only copies with a nonzero differentiated reference cutoff require an amplitude comparison.
Exchanging the two bands inverts the physical Gaussian weight.
Expansion of the literal Gaussian block at an arbitrary angle. The coefficient is the actual periodized error on the zero-angle section.
The signed request is the only coefficient input to this comparison. The same literal native copy and cutoff occur on both sides.
Full-fiber covariance derived from the actual incoming state and primitive identities. No covariance of a signed output is assumed.
Reverse transport of the actual complex Gaussian coefficient on the image of the same overlap, with the reciprocal physical weight.
The Gaussian component of WaveOn, for the actual signed Fourier
block, on all radial and free auxiliary fibers and at every angle.
The same field comparison in the reverse common-chart direction. Its domain is the exact image of the forward overlap.
Geometry: an abbreviation for ActualMeanPhysicalData.initialGeometry.
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Every comparison is on the intersection of the two actual normalized slow charts; the radial and torus fibers are unrestricted.
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Individual input fields are compared, including the Gaussian and nonzero harmonic alias inputs used by the next particular solve.
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Axis coherent, given by ∀ n m k, CommonWindow.index h n + k = CommonWindow.index h m → CycleStateCoherence.AxisBand geometry (overlap n m) n m k a.
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The geometric induction invariant, separate from all quantitative residual estimates. The label set is the initializer's fixed choice.
- state : StateCoherent x.state
- blocks : BlocksCoherent x.coefficients
- axis : AxisCoherent x.axisymmetricAlias
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Omitted labels vanish by their primitive support and zero modes #
The actual source on every fast-variable fiber #
Particular source, constructed using ParticularWaveAssembly.residualSource.
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All three fields of the actual signed insertion transform on the same overlap. The Gaussian term is the differentiated-cutoff error.
Particular point, given by ParticularWaveAssembly.angleShuffle (cycleAssoc z, 0).
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Algebraic propagation after the two actual wave laws are derived #
The two literal wave insertions have the required transport law. Every source and coefficient comparison is derived from the incoming state, its support, and the actual solver primitives.
Simultaneous propagation of the actual state, stored blocks, Gaussian/alias data, and the initializer's finite label choice.
The fixed actual recurrence and the mean atlas input #
State, constructed using CycleState.iterate.
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Collection of the already proved actual transport laws into precisely the input used by the physical mean atlas. Its covariance fields are derived from the same stage data as the analytic induction.
The geometric induction uses the same fixed recurrence and supplied analytic stage data; no sequence of coherent states is assumed.
The actual mean-atlas input is derived from the same analytic recurrence; its wave and covariance transports are conclusions.