Concrete qualitative data for the actual correction waves #
All native data below use the initializer's existing choice. A common-band translation is interpreted on a native cover only when the common index is at most the native index. The inactive bands are handled using actual zero germs; no periodicity of an unused unmasked phase is imposed on those bands.
Qualitative regularity of the actual finite wave updates #
All regularity statements below use the full open slow domain. The quantitative strip is used only for its fixed differential operators. Native smoothness and genuine zero germs, rather than estimates on a smaller strip, supply the continuation away from the active phase patches.
A qualitative domain for the same operators. No quantitative bound is extended from the original strip.
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These are native, uncorrected data. In particular the smoothness of the common corrected velocity is a conclusion, not a field of this record.
- cells : PeriodizedWaveBounds.Cells D I
Cells of
NativeData, of typeCells D I. Patch of
NativeData, of typeℕ → I → Set D.- raw : LocalizedCurlRealization.RawData a (onDomain s Ω hΩ) d self.patch
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The actual normalized vector-potential coefficient has a smooth zero extension too; smoothness of the bare phase normal off support is not used.
Locally finite native zero germs give a zero germ for the common corrected amplitude, even if the phase or normal is singular at this point.
Discrete translations on an open domain #
Unlike global translation identities, these statements only require the actual fields on the physical slow domain. Derivatives are genuine Fréchet derivatives, transferred through an open neighborhood.
Translation on, given by ∀ x ∈ Ω, f (x + z) = f x.
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- NavierStokes.ActualWaveRegularity.TranslationOn Ω z f = ∀ x ∈ Ω, f (x + z) = f x
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Qualitative regularity of the literal native solves #
Primitive smooth coefficient, forcing, and synthesis columns on a neighborhood of each entire Volterra path. No solved field occurs here.
- frame : ℕ → PrimaryODE.FrameData (P × ℝ)
Frame of
ModalSmooth, of typeℕ → PrimaryODE.FrameData (P × ℝ). - neighborhood : ℕ → TorusInverse.Frequency → Set (P × TorusInverse.Plane)
Neighborhood of
ModalSmooth, of typeℕ → Frequency → Set (P × Plane). Interval of
ModalSmooth, of typeℕ → Set ℝ.- bridge (n : ℕ) (k : PrimaryCopyBridge.Frequency) : PrimaryCopyBridge.Inputs (self.frame n) (t n) harmonic (g n) k (self.neighborhood n k) 0 (L n)
- coefficient (n : ℕ) (k : PrimaryCopyBridge.Frequency) : ContDiffOn ℝ (↑⊤) ((PrimaryCopyBridge.copyFrame (self.frame n) (g n) k).coefficient harmonic) (self.neighborhood n k ×ˢ self.interval n)
- forcing (n : ℕ) (k : PrimaryCopyBridge.Frequency) : ContDiffOn ℝ (↑⊤) ((PrimaryCopyBridge.copyFrame (self.frame n) (g n) k).forcing (PrimaryCopyBridge.copySource (t n).source (g n) k)) (self.neighborhood n k ×ˢ self.interval n)
- columns (n : ℕ) (k : PrimaryCopyBridge.Frequency) (i : Fin 2) : ContDiffOn ℝ (↑⊤) (PrimaryPulseBounds.synthesisColumn (PrimaryCopyBridge.copyFrame (self.frame n) (g n) k) i) (self.neighborhood n k ×ˢ self.interval n)
- current_slot (n : ℕ) (k : TorusInverse.Frequency) (x : P × TorusInverse.Plane) : x ∈ self.neighborhood n k → ((g n).coordinates k x.2).2 ∈ Set.Ioo 0 (L n)
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The actual signed quotient is smooth from its matrix, target, request, mask and homogeneous fundamental, on the strict covariance cone.
One actual mode on the full physical slow domain #
Point: an abbreviation for CorrectionStep.CyclePoint.
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Full domain, given by HarmonicResidual.liftDomain (PhysicalMeanDomain.slowDomain U.carrier).
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Native domain, given by e.symm ⁻¹' fullDomain U.
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Deck shift, given by ((0, (0, ((k.1 : ℝ), (k.2 : ℝ)))), 0).
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Mode oscillation, defined pointwise by (vectorMode (a.background.frequency n) (a.background.phase n) ((a.commonCorrected s d).amplitude n) (e x) i).re.
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Primitive continuation and deck identities for one mode. All spatial smoothness is confined to the genuine native patches. Radial support is proved using localized raw-amplitude zero germs.
- native : NativeData a s d (nativeDomain e U) ⋯
Native of
ModeData, of typeNativeData a s d (nativeDomain e U) (nativeDomain_open e U). - reindex : ℕ → TorusInverse.Frequency → I ≃ I
Reindex of
ModeData, of typeℕ → TorusInverse.Frequency → I ≃ I. - cutoff_deck (n : ℕ) (k : TorusInverse.Frequency) (i : I) (x : D) : x ∈ nativeDomain e U → a.cutoff n ((self.reindex n k) i) (x + e (deckShift k)) = a.cutoff n i x
- amplitude_deck (n : ℕ) (k : TorusInverse.Frequency) (i : I) (x : D) : x ∈ nativeDomain e U → a.amplitude n ((self.reindex n k) i) (x + e (deckShift k)) = a.amplitude n i x
- radius_deck (n : ℕ) (k : TorusInverse.Frequency) : TranslationOn (nativeDomain e U) (e (deckShift k)) (a.background.radius n)
- radial_deck (n : ℕ) (k : TorusInverse.Frequency) : TranslationOn (nativeDomain e U) (e (deckShift k)) (d.radialField n)
- phase_deck (n : ℕ) (k : TorusInverse.Frequency) : TranslationOn (nativeDomain e U) (e (deckShift k)) (a.background.phase n)
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Finite sums retain the whole-domain conclusions #
The literal particular update of the cycle #
Particular space: an abbreviation for (CycleSlow × ℝ) × TorusInverse.Plane.
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Particular chart, given by (StateReindex.cylinder cycleAssoc).trans angleShuffle.
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Particular strip, given by ParticularParameters.nativeStrip (reindexStrip cycleAssoc.symm p.strip).
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Particular copy data as an element of CopyData ParticularSpace TorusInverse.Frequency.
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Deck covariance of the actual Volterra coefficient follows from periodicity of its incoming residual coefficient, with the same anchor.
This representation is derived from the actual angle-lifted Volterra solve and the original carrier. No equality of completed output fields is an assumption.
Full-domain native inputs for the same particular copies and the same
incoming residual data used by CycleParameters.particularBlock.
- mode (l : ι) (j : ℤ) : j ∈ ParticularWaveAssembly.modes v.residualBand → ModeData (particularCopyData p v c u l j) (particularStrip p) (p.particular l).directions particularChart U r₀ r₁
Mode supplied by
ParticularData. - radius_angular (l : ι) (n : ℕ) : CopyAngularInvariance.Invariant ((0, 1), 0) ((p.particular l).background.radius n)
- radial_angular (l : ι) (n : ℕ) : CopyAngularInvariance.Invariant ((0, 1), 0) ((p.particular l).directions.radialField n)
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The literal signed update, using the post-particular request #
The native signed coefficient inherits a deck identity from the literal matrix, targets, mask, and homogeneous fundamental.
Angular identities of the primitive signed inputs. No identity of the corrected field, and no regularity away from the native support, is assumed.
Slope of
SignedAngles, of typeℕ → ℝ.- radial (n : ℕ) : CopyAngularInvariance.Invariant (0, 1) (p.directions.radialField n)
- request (n : ℕ) : CopyAngularInvariance.Invariant (0, 1) (request n)
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The existing native angular inputs imply the smaller qualitative record. Their quantitative-domain smoothness field is not extended or used.
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All fields use the literal post-particular request. The old state, profile, and native data are not reselected.
- mode (l : ι) : ModeData ((p.signed l).copyData p.strip (p.signedRequest v c u)) (HarmonicWaveInteraction.productStrip p.strip) (p.signed l).directions (LinearIsometryEquiv.refl ℝ Cylinder) U r₀ r₁
Mode supplied by
SignedData. - angles (l : ι) : SignedAngles (p.signed l) p.strip (p.signedRequest v c u)
Angles of
SignedData, of type∀ l, SignedAngles (p.signed l) p.strip (p.signedRequest v c u).
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The qualitative oscillation fields of the actual next cycle state. The intervening temporal, rank, and pressure-refresh operations preserve the same oscillation by the literal recurrence.
Moving radial edges of the literal coefficients #
At a flat radial boundary the coefficient need not have a zero germ. Instead, its actual interior tensor bounds prove smoothness across that boundary. The conclusions concern the original coefficient, whose exterior zero values identify it with the constructed extension.
The original, totalized coefficient has all zero edge tensors, from its actual interior derivatives and its actual exterior values.
Apply the already proved native Gaussian derivative estimates to the same literal coefficient. The constants are those in the native estimates; no full-domain estimate or output smoothness is assumed.
Index: an abbreviation for ActualSignedStageControls.SignedLabel B N0.
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Ordered, given by CommonWindow.index ActualPrimary.h n ≤ ChartScales.nativeIndex ActualPrimary.h (BaseChartJets.cellBand l.1).
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Deck index, given by coverIndex ((ActualPrimary.chartGeometry n l.2 l.1).gap) m.
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Deck permutation, given by Equiv.addRight (deckIndex l n m).
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Signed angles, bundling slope, radius, radial, phase and the required compatibility
proofs.
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The actual slow mask selects an ordered native cover #
The actual three assembled fields vanish on inactive common bands. The proof uses raw zero germs before applying the curl and copy sum.
The actual full-domain phase patches #
Signed phase patch as an element of Set FullPoint.
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Every point of the full slow domain either lies in the genuine positive-radius, interior-clock patch, or has a zero localized raw germ.
Literal exterior values of the signed quotient #
Radius, given by x.1.1 / VariableGaugeMean.qLength (2 * ActualPrimary.h) x.1.2.1.
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Actual quantitative cells cover every nonzero localized copy on the whole open strip. Closed dyadic, transverse and temporal endpoints remain in the cell; only genuine zero neighborhoods are used in the alternatives.
The actual strip weight gives all zero edge tensors #
This uses the actual product weight and actual strip growth. There is no boundary-continuity premise and no change to the given function.
Whole-domain regularity of the literal signed fields #
Signed copies, given by (ActualSignedStageControls.parameters l).copyData ActualPrimaryBounds.strip request.
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Positive domain, given by ActualWaveRegularity.fullDomain ActualPrimary.standardRegion ∩ ActualPrimaryCoherence.positiveRadialChart.
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Signed normal, constructed using CurlClassBounds.coefficient.
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Signed corrected, given by (signedCopies l request).commonCorrected ActualSignedStageControls.fullStrip (ActualSignedStageControls.parameters l).directions.
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Signed field as an element of CorrectionState.Oscillation Point.
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The same edge continuation in the particular solver's coordinates #
Particular full strip, given by ParticularWaveBounds.reindexStrip ActualWaveRegularity.particularChart.symm ActualSignedStageControls.fullStrip.
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No new radial coordinate or flat weight is chosen for the particular solver. Reassociation preserves the actual derivative norms.
The particular phase below is the literal carrier of its incoming block. Its equality with the selected primary phase is a carrier invariant, not a smoothness assumption on an output.
Particular copies, given by (ActualParticularStageControls.canonicalParameters l).copyData c u b G A j.
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- NavierStokes.ActualWaveRegularityData.particularCopies l c u b G A j = (NavierStokes.ActualParticularStageControls.canonicalParameters l).copyData c u b G A j
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Particular positive, given by ActualWaveRegularity.particularChart.symm ⁻¹' positiveDomain.
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Particular normal, constructed using CurlClassBounds.coefficient.
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Closed support and actual source continuity, unlike an interior norm bound alone, determine the literal values on the radial faces.
Coefficient periods for the actual signed wave, before angular or finite-label assembly.
The source callback is a per-label, complete-fiber statement. It is not replaced by periodicity of the total real oscillation.