Actual particular-wave data on the active label-band pairs #
The reference phase and native slot are those of the existing initializer choice. The forced fields use the literal current harmonic residual. Active pair estimates do not impose polynomial clock bounds on inactive bands. The actual source support and transported cutoff then globalize the native estimates. The final theorems give uniform bounds for the literal common and finite-harmonic fields from the current analytic invariant.
Actual particular background on the full retained carrier #
The retained source mask gives the padded native scale interval (1/4,4).
The cells below use its phase carrier and closed clock core without adding
the narrower dyadic mask of the original primary coefficient support.
Local background bounds for the actual particular harmonics #
The fixed harmonic changes the frequency. Its phase is the same primary phase, including the free angular variable. All primitive bounds are pulled from the actual primary inputs on the same closed support cells.
The same jet constants work after the native coordinate isometry.
Reindex family, given by WaveFamily.ofCoefficients (fun i => ParticularWaveBounds.reindexCoefficients e (a.coefficients i)).
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This operation changes only the harmonic frequency and sets the two unknown coefficients to zero. In particular its actual normal and defect are unchanged.
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The same primary choice in native/free-angle coordinates #
Label: an abbreviation for ActualPrimaryBounds.SignedLabel B N0.
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Parameter: an abbreviation for CorrectionStep.CycleSlow.
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Native: an abbreviation for (Parameter × ℝ) × TorusInverse.Plane.
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Native to full, given by ParticularWaveAssembly.angleShuffle.symm.trans (StateReindex.cylinder cycleAssoc.symm).
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Native strip, given by ParticularWaveBounds.reindexStrip nativeToFull ActualPrimaryBounds.fullStrip.
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Cells, given by nativeToFull ⁻¹' ActualPrimaryBounds.controlCell n i.
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Directions, given by ParticularWaveBounds.reindexDirections nativeToFull (ActualPrimaryBounds.directions B).
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Primary block as an element of HarmonicBlock CyclePoint.
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Carrier, constructed using ParticularWaveAssembly.actualCarrier.
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Background family, given by WaveFamily.ofCoefficients (fun i => ParticularWaveBounds.zeroAmplitudes (carrier b j i.1)).
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All order-zero background classes, at every derivative order, are derived from the primary inputs. The envelope can be any nonnegative one because the velocity and pressure slots are zero. Constants remain uniform in the spatial label and lattice copy.
Padded cell as an element of Set ActualPrimary.FullPoint.
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Cells, given by ActualParticularBackground.nativeToFull ⁻¹' paddedCell n i.
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The actual normal and material defect on the larger cells #
Zero input slots and the unchanged native carrier #
The literal actualCarrier, now controlled on every retained padded
cell. No dyadic mask or additional support hypothesis is imposed.
Geometric jets for the actual scaled particular inverse #
The normal, its native time derivative, and the action operator are computed from the selected transported frame. Their native-copy jets follow from the selected phase construction and the polynomial coordinate cost, without estimates on a solved velocity or pressure as hypotheses.
The translation may depend on the lattice copy; its size never enters a derivative bound.
Argument, given by (χ x.1, (g.coordinates k x.2).2).
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- NavierStokes.ScaledParticularFrameJets.argument χ g k x = (χ x.1, (g.coordinates k x.2).2)
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Argument linear as an element of (P × Plane) →L[ℝ] (Slow × ℝ).
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Tangent, given by PrimaryCopyBridge.frameTangentData (nativeFrame (ScaledActualParticularControl.frame F φ clock normal (l,n)) χ) j (source l n).
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These are the three actual geometric inputs needed by the pressure
estimate in ParticularCopyBounds.uniform_coefficients_jets.
The frame reconstructed from the selected actual phase has exactly that phase's normal; the nonzero transverse normal follows from its proved reference comparison.
Both range constants precede every label, band, native copy and evaluation point. There is no inverse dependence on the clock rate.
The actual broad carrier in the canonical particular coordinates #
Only the selected geometry and its closed source support occur here. No property of a solved particular or signed field is assumed.
Parameter: an abbreviation for CorrectionStep.CycleSlow.
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Label carrier, given by ActualInitialExcluded.labelCarrier (l.2,l.1) n.
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Associated point, given by CorrectionStep.cycleAssoc.symm (p, Y).
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Parameter domain, given by {p | p.2 ∈ standardRegion.carrier}.
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Slow map, given by nativeSlow l.1 (toAbsolute n (associatedPoint p 0)).
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Slow core, given by slowMap l n ⁻¹' ActualGaussianCoverage.actualSlowCore certificate modulation (choice B N0).prepared l.1.
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Reference length, given by (phases B N0 l.2).L l.1.
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Clock, given by PhysicalParticularWave.clockWeight h (ChartScales.Q n) (ChartScales.Q (BaseChartJets.cellBand l.1)).
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Spatial label, given by PartitionedCovariance.signedLabel (PrimaryGeometryAssembly.label nominal l.1) l.2.
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Reference geometry, given by ActualSignedGeometry.slotGeometry slots vectors_det (spatialLabel l) 0.
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Geometry, given by CopySolveCompatibility.transportGeometry (referenceGeometry l) (gap l n) 0 (clock l n) (clock_pos l n).ne'.
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Source region, given by ActualGaussianCoverage.sourceRegion (slowCore l n) (geometry l n) slots.radius (referenceLength l) (clock l n).
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The common-band logarithmic range holds on the full slow domain, without any restriction on the radial variable.
Broad carrier support forces the same finite band distance on the entire slow domain, including radii outside the analytic strip.
The canonical geometry rescales time after the same native refinement.
The unordered branch is empty. This makes the same source-region description valid on the full slow domain for every band.
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Canonical source region, given by ActualGaussianCoverage.sourceRegion (activeSlowCore l n) (geometry l n) slots.radius (referenceLength l) (clock l n).
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Scalar-clock support of the actual particular solve #
This support argument uses the literal complex Volterra solve and the Gaussian-times-padding cutoff. Clock factors only need to be positive at each band; no uniform range for the complete clock family is assumed.
The literal complex Volterra solve and its separately transported Gaussian/outer cutoff, without uniform bounds on the clock scalars.
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Scalar cells, constructed using nativeCells.
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Outside the source carrier, each padded native cell has a zero cutoff or a zero whole-path Volterra solve.
Jets of the literal transported native cutoff #
The product consists of the padded reference window and the separate Gaussian slot cutoff. On the analytic patch the window equals one on an ambient neighborhood, including at the closed transverse endpoints. Its exact germ therefore transfers the Gaussian clock estimates without assumptions about a source, correction state, or modal-control output.
The literal cutoff, before placing it in any particular-solve record.
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Patch membership supplies the actual closed-core hypothesis of the reference window's neighborhood theorem.
This is an ambient germ, obtained from the padded window's exact cutoff_germ theorem rather than from its value at the boundary point.
All finite jets are uniform in the label, band, and lifted copy. The only quantitative input beyond the primitive phase and clock is the polynomial bound for the actual affine geometry.
Parameter: an abbreviation for PhysicalParticularWave.Parameter.
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AP: an abbreviation for CorrectionInitialization.ActualPrimary.FullPoint.
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Reindexing retains the selected phase, its frame, and all uniform constants.
Reindex domain, bundling scale, carrier, isOpen, one_le_scale.
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Reindex phase, bundling epsilon, p, pz, x0 and the required compatibility proofs.
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Reindex construction, bundling phase, V, openV, lam and the required compatibility
proofs.
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The original physical slot, Gaussian cutoff, and actual current-state data.
Spatial label, given by PartitionedCovariance.signedLabel (PrimaryGeometryAssembly.label nominal l.2) l.1.
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Reference geometry, given by ActualSignedGeometry.slotGeometry slots vectors_det (spatialLabel l) 0.
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Reference cutoff, given by (clockWindow l.2).cutoff z * GaussianTailFlat.slotCutoff ((phases B N0 l.1).L l.2) z.2.
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Reference, bundling band, geometry, length, length_pos and the required
compatibility proofs.
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Background, given by ParticularWaveBounds.reindexCoefficients nativeToFull (chartCoefficients l.1 l.2).
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Directions, given by ParticularWaveBounds.reindexDirections nativeToFull (PrimaryResidualClass.directions (commonContext B)).
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Associated context, given by StateReindex.context cycleAssoc.symm (commonContext B).
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Associated strip, given by ParticularWaveBounds.reindexStrip cycleAssoc.symm (BaseContextAssembly.nativeStrip nominal standardRegion).
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Assembly, bundling reference, charts, parameter, gap and the required compatibility
proofs.
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Parameters, given by ParticularParameters.fromReference (assembly x l) h (gap l).
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Fixed primitive data for all iterations of the same labeled construction.
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The sign combination is proved before specializing the constructed profile.
Signed phase, bundling epsilon, p, pz, x0 and the required compatibility proofs.
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Signed construction, bundling phase, V, openV, lam and the required compatibility
proofs.
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Joint domain, given by reindexDomain (PrimaryGeometryAssembly.domain nominal (choice B N0).prepared.N) Prod.snd.
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Joint phase, given by signedPhase (phases B N0).
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Joint construction, constructed using signedConstruction.
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Changing the native clock preserves the same grouped Gaussian exactly.
The slow/fast association keeps the full moving weight unchanged.
Slow insert, bundling toFun, map_add, map_smul, cont.
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Slow strip, given by HarmonicWaveInteraction.pullbackStrip (BaseContextAssembly.nativeStrip nominal standardRegion) slowInsert.
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Pulse envelope, given by PrimaryPulseBounds.referenceP ((phases B N0 l.1).lam l.2) ((phases B N0 l.1).u l.2) ((phases B N0 l.1).L l.2).
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Envelope, given by WaveEnvelopeTransport.copyEnvelope (chartGeometry n l.1 l.2) slots.radius ((phases B N0 l.1).L l.2) (pulseEnvelope l) z.2.
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Mean envelope, given by envelope l n (cycleAssoc z).
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Active, given by 1 ≤ n ∧ BaseChartJets.cellBand l.2 ∈ CommonWindow.levels n.
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Selected label, given by (e n).val.1.
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Selected band, given by (e n).val.2.
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Selected construction, given by reindexConstruction (jointConstruction (B := B) (N0 := N0)) (fun i : Unit × ℕ => selectedLabel e i.2).
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Selected strip, given by UniformPrimaryWeights.reindexedStrip slowStrip (fun n => (selectedBand e n, ())).
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Selected slot, given by spatialLabel (selectedLabel e n).
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Selected clock, given by ActualSignedGeometry.clockScale (selectedBand e) (fun u n => (selectedSlot e u n).1) (selected_near e) h.
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Selected normal, given by ActualSignedGeometry.normalScale (selectedBand e) (fun u n => (selectedSlot e u n).1) (selected_near e) outgoing.data.h_pos.le.
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Selected gap, given by gap (selectedLabel e n) (selectedBand e n).
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Selected geometry, constructed using ScaledActualParticularControl.geometry.
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Selected length, given by ScaledActualParticularControl.length (selectedConstruction e) (selectedClock e).
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Selected pulse envelope, given by ScaledActualParticularControl.envelope (selectedConstruction e) (selectedClock e).
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The input class is exactly the residual component of the cycle invariant.
Current source, constructed using ParticularWaveAssembly.sourceFamily.
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Selected phi, given by ScaledActualParticularControl.physicalPhi h (selectedBand e) (fun u n => (selectedSlot e u n).1).
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Selected chi, given by
ActualSignedGeometry.swapParameter.toContinuousLinearEquiv.toContinuousLinearMap.comp (ContinuousLinearMap.fst ℝ Parameter ℝ).
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Selected frame, constructed using ActualParticularControl.nativeFrame.
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Selected patch, constructed using ScaledActualParticularControl.patch.
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The real or imaginary control is constructed from the selected phase, the exact clock and slot geometry, and the current residual class.
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Selected source, given by currentSource x j (selectedLabel e n) (selectedBand e n).
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Selected tangent, given by (parameters x (selectedLabel e n)).nativeTangent j (selectedBand e n).
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Selected background, constructed using ParticularCopyBounds.reindexedBase.
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This is the control of the literal selected fromReference tangent,
after its source is overwritten by the corresponding part of the current HR source.
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The actual computed copy data, with the current residual as source.
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The active phase patch includes the transverse boundary. Its time coordinate is the actual transported clock.
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Selected weight, constructed using ActualParticularControl.groupedEnvelope.
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The selector is only an indexing device. Both actual raw fields have one bound before the original spatial label, active band, and lattice copy.
The support geometry is the same canonical scalar-clock geometry.
Support label, given by (l.2,l.1).
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Carrier cells, constructed using ScalarParticularSupport.scalarCells.
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Input support type used in actual particular stage controls.
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Actual incoming coefficient support supplies the source's zero germ on the full slow domain; no zero-germ conclusion about the solved field is assumed.
Actual source-carrier coverage of the analytic patch.
Every native cell is either controlled, killed by the actual cutoff, or has both a zero raw solve and a zero current forcing germ.
The literal transported window/Gaussian product has uniform jets.
Derived local background bounds and actual common-field estimates.
Preserves carriers: an abbreviation for ∀ l, SameCarrier (x.coefficients.blocks l) (ActualParticularBackground.primaryBlock l).
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The exact moving weight, finite harmonic assembly, and invariant interface.
Residual bounds type used in actual particular stage controls.
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Associated update as an element of HarmonicBlock (Parameter × Plane).
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Associated good as an element of HarmonicBlock (Parameter × Plane).
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Output block, given by StateReindex.block cycleAssoc (associatedUpdate x N l).
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Output good, given by StateReindex.block cycleAssoc (associatedGood x N l).
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The finite harmonic assembly and coordinate association retain constants chosen before the spatial label and band.
The quantitative inputs are precisely fields of the current analytic invariant. The geometric equalities identify its actual strip and carrier.