Construction of the initial correction fields #
The operations in this file use the actual shifted pressure primitive, torus inverse, stream potential, and five-row inverse. The covariance identity is also differentiated as an identity of functions, retaining all derivatives of the squared partition. Quantitative initialization is assembled below from the estimates on these same operations.
The actual leading covariance, including all physical partition factors.
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In particular every derivative of every squared mask is included. No commutation of a derivative with an infinite sum is assumed.
The primitive data of one primary label. Its velocity below is the actual cutoff curl, and its pressure is the actual cutoff pressure mode.
- strip : WeightedClasses.StripData X
Strip of
PrimaryPiece, of typeStripData X. - directions : LinearWaveBounds.GraphDirections X
Directions of
PrimaryPiece, of typeGraphDirections X. - coefficients : LinearWaveBounds.WaveCoefficients X
Coefficients of
PrimaryPiece, of typeWaveCoefficients X. Cutoff of
PrimaryPiece, of typeℕ → X → ℝ.
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Exact coefficients, given by p.coefficients.corrected p.strip p.directions p.cutoff.
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- p.exactCoefficients = p.coefficients.corrected p.strip p.directions p.cutoff
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Velocity, defined pointwise by (vectorMode (p.coefficients.frequency n) (p.coefficients.phase n) (p.exactCoefficients.amplitude n) x i).re.
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- p.velocity n x i = (NavierStokes.HarmonicCalculus.vectorMode (p.coefficients.frequency n) (p.coefficients.phase n) (p.exactCoefficients.amplitude n) x i).re
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Tangent velocity, defined pointwise by (vectorMode (p.coefficients.frequency n) (p.coefficients.phase n) ((p.coefficients.withCutoff p.cutoff).amplitude n) x i).re.
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- p.tangentVelocity n x i = (NavierStokes.HarmonicCalculus.vectorMode (p.coefficients.frequency n) (p.coefficients.phase n) ((p.coefficients.withCutoff p.cutoff).amplitude n) x i).re
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Pressure, defined pointwise by (mode (p.coefficients.frequency n) (p.coefficients.phase n) (p.exactCoefficients.pressure n) x).re.
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- p.pressure n x = (NavierStokes.HarmonicCalculus.mode (p.coefficients.frequency n) (p.coefficients.phase n) (p.exactCoefficients.pressure n) x).re
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Excluded as an element of ℕ → X → Fin 3 → ℝ.
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Linear good, given by p.coefficients.constructedGood p.strip p.directions p.cutoff.
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- p.linearGood = p.coefficients.constructedGood p.strip p.directions p.cutoff
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Linear good field, defined pointwise by (vectorMode (p.coefficients.frequency n) (p.coefficients.phase n) (p.linearGood n) x i).re.
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- p.linearGoodField n x i = (NavierStokes.HarmonicCalculus.vectorMode (p.coefficients.frequency n) (p.coefficients.phase n) (p.linearGood n) x i).re
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Linear residual, defined pointwise by (p.exactCoefficients.harmonicResidual p.strip p.directions n x i).re.
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- p.linearResidual n x i = (p.exactCoefficients.harmonicResidual p.strip p.directions n x i).re
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Primary linear residuals are evaluated on the same constructed curl
used by velocity; the Gaussian cutoff derivative remains explicit.
These are the cumulative primary bounds, proved from the tangent coefficient and the actual curl remainder.
Taking the actual curl correction does not enlarge the closed support of its amplitude. This also includes every derivative at a slot boundary.
The signed inverse quotient at twice the primary target is exactly the positive primary square root; this identifies the two actual constructions.
Coefficients, given by SignedWaveUpdate.coefficients a s d H T (fun n x => (2 : ℝ) • T n x) mask v Ndot A j.
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Piece, given by ⟨s, d, coefficients a s d H T mask v Ndot A j, cutoff⟩.
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The primary pressure and amplitude estimates come from their formulas; the input record supplies only the fixed background geometry.
The only ODE used here is the constructed normalized primary fundamental. In particular no principal equation for the output coefficient is assumed.
The physical shear operator is built from the actual radial derivatives of the two background profiles.
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The physical action has order zero because the fixed background is independent of the radial fast variable.
A raw background record with zero wave and pressure is verified from the actual phase, base jets and chart. Its material defect and phase-normal bounds are derived here, not supplied as output estimates.
Pulse coordinates, defined pointwise by ((χ n x).1, (χ n x).2.2 / P.L n).
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Native coefficients as an element of WaveCoefficients X.
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The native coefficient has its actual primary pressure and satisfies the principal equation by the constructed ODE. All matching assumptions concern the chart, the scalar viscosity and the primitive slow inputs.
All primary coefficient and pressure estimates are derived from the same native ODE and matrix. The background record has zero amplitude and zero pressure, so no primary output estimate is an input.
The canonical coefficient and the covariance pulse contain the same Gaussian cutoff, applied exactly once.
Angular symmetry is derived from the coordinate translation and the primitive slow data, including the actual reconstructed primary pressure.
Both physical columns are constructed from the same native primary frames used above; continuity and kinematics are proved rather than stored as fresh assumptions.
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Excluded block, given by ErrorHarmonics.gaussianBlock p.directions p.cutoff p.coefficients.amplitude 0 1 p.coefficients.frequency Φ kp.
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- p.excludedBlock Φ kp = NavierStokes.ErrorHarmonics.gaussianBlock p.directions p.cutoff p.coefficients.amplitude 0 1 p.coefficients.frequency Φ kp
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The retained primary Gaussian error is a genuine nonzero angular harmonic, so its actual angular mean vanishes exactly.
Initial mean velocities vanish; the primary fields are actual finite label sums of cutoff curls and their homogeneous pressure modes.
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The active labels may depend on the chart band. No bound on their total cardinality is inserted into the construction or its class estimates.
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Primary stage, given by reconstructPressure p c (seed labels pieces baseError).
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After temporal, given by temporalStage p h axial c (primaryStage p c labels pieces baseError).
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After rank, given by rankStage p r axial c (afterTemporal p h axial c labels pieces baseError).
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The current pressure alias is retained once, after the final pressure reconstruction. Earlier obsolete pressure aliases are not accumulated.
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Initialized, given by retainPressureAlias p c (afterRank p r h axial c labels pieces baseError).
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The two actual integrated masses remain zero through both updates.
The actual current pressure reconstruction controls the radial residual by the computed pressure defect, with its exact alias retained.
The physical-gauge pipeline uses the actual slow-variable-dependent cutoff endpoints and an explicit common torus index at every step.
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After temporal, given by temporalStageState g h index axial c (primaryStage g c labels pieces baseError).
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After rank, given by rankStageState g r axial c (afterTemporal g h index axial c labels pieces baseError).
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Retain pressure alias, given by { u with errors := ⟨u.errors.base, u.errors.gaussian, u.errors.aliasError + pressureAliasState g c u⟩ }.
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Initialized, given by retainPressureAlias g c (afterRank g r h index axial c labels pieces baseError).
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Primary bands, given by reconstructState g c (bandSeed labels pieces baseError).
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Temporal bands, given by temporalStageState g h index axial c (primaryBands g c labels pieces baseError).
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Rank bands, given by rankStageState g r axial c (temporalBands g h index axial c labels pieces baseError).
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Initialized bands, given by retainPressureAlias g c (rankBands g r h index axial c labels pieces baseError).
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The stored base error cancels once. The primary Gaussian means vanish, and the two literal alias fields remain with their actual signs.
The band-dependent physical-gauge construction retains exactly the two current aliases. The base error cancels once and each primary Gaussian has zero actual angular mean.
Bookkeeping for the two tangential estimates after the actual rank stage: no class estimate on either excluded alias is inserted.
Insert, given by (ContinuousLinearMap.id ℝ D).prod 0.
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The actual coefficient domain on the angular slice.
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Restriction is a genuine linear pullback of every jet, with norm one.
A primary mode and its pressure, with the actual conjugate negative mode.
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Harmonic block, given by PrimaryHarmonics.block p.exactCoefficients Φ kp.
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Tangent block, given by PrimaryHarmonics.block (p.coefficients.withCutoff p.cutoff) Φ kp.
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Difference coefficients as an element of WaveCoefficients (D × ℝ).
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Difference block, given by PrimaryHarmonics.block p.differenceCoefficients Φ kp.
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The cumulative bounds belong to the actual finite harmonic blocks representing the cutoff curl and its difference from the primary tangent.
Before the temporal update, the pressure is the actual compact primitive of the radial equation. Its class is derived from the covariance.
All three incoming debts are actual radial moments. No defect bound is an input to this initial estimate.
The actual torus average preserves the flat mean class.
Exact leading covariance cancellation transfers the curl-product and higher-virtual-flux orders to the actual averaged radial flux.
The initial bar exponent 1.49 follows from the actual averaged
flux balance, a curl covariance error, and the axial derivative gain.
The literal radial source retains the moving support of the actual covariance, including every differentiated term.
Smoothness on the full valid slow domain follows from a containing annulus and the actual covariance support; no smooth extension of a positive-time totalization is used.
Actual moving-gauge initial pressure and raw tangential residuals, derived from the covariance and virtual stresses.
All three incoming debts are measured from the same initial fields. There is no assumed debt bound and no change to the moving edge weight.
Parameter differentiation of the actual torus average on the open slow domain. The localization equals the original source on a whole fiber germ, so its derivatives introduce no cutoff term.
Exact leading covariance cancellation combines with the actual curl covariance error and the higher virtual stress on the moving profile strip.
The actual zero-mean state has both improved bar residuals, once the two leading covariance identities have been applied.
Piece, bundling strip, directions, coefficients, cutoff.
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Envelope, defined pointwise by SignedWaveUpdate.phaseEnvelope F (pulseCoordinates (F j) χ) j n (x, 0).
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Native geometric and coefficient data. The principal equation, wave amplitude bounds, homogeneous pressure bounds and nonlinear residual bound are derived below rather than stored in this record.
- operators : MeanIncrementBounds.OperatorBounds s c.operators ChartScales.kappa
- matching : PrimaryResidualClass.Matches s c (PrimaryMaterialDefect.coefficients (F j) b χ 0 0 frequency)
- native_jets : PhaseJetBounds.PolynomialJets (PrimaryPulseBounds.phaseDomain (HarmonicWaveInteraction.productStrip s)) fun (n : ℕ) (x : D × ℝ) => ((χ n x).1, (χ n x).2.2)
- normalized_jets : PhaseJetBounds.PolynomialJets (PrimaryPulseBounds.phaseDomain (HarmonicWaveInteraction.productStrip s)) (PrimaryConstruction.pulseCoordinates (F j) χ)
- chart_smooth (n : ℕ) : ContDiffOn ℝ (↑⊤) (χ n) (HarmonicWaveInteraction.productStrip s).domain
- radial_base : WeightedClasses.UnweightedClass (HarmonicWaveInteraction.productStrip s) 1 fun (n : ℕ) (x : D × ℝ) => b n (χ n x).1
- radial_base_smooth (n : ℕ) : ContDiffOn ℝ (↑⊤) (b n) (U.carrier n)
- frequency_bound : WeightedClasses.BandBound s (-(1 / 2)) frequency
- inverse_frequency : WeightedClasses.BandBound s (1 / 2) fun (n : ℕ) => 1 / frequency n
- covariance : SignedWaveUpdate.CovarianceControl (HarmonicWaveInteraction.productStrip s) (SignedWaveUpdate.phaseMatrix F pref (PrimaryConstruction.pulseCoordinates (F j) χ)) T
Covariance supplied by
Control. - mask_bound : WeightedClasses.UnweightedClass (HarmonicWaveInteraction.productStrip s) 0 mask
- cutoff_bound : WeightedClasses.UnweightedClass (HarmonicWaveInteraction.productStrip s) 0 cutoff
- target_angle : SignedWaveUpdate.FrozenAlong (0, 1) T
- mask_angle : SignedWaveUpdate.FrozenAlong (0, 1) mask
- cutoff_angle : SignedWaveUpdate.FrozenAlong (0, 1) cutoff
- target_frozen : SignedWaveUpdate.FrozenAlong (PrimaryResidualClass.directions c).fast T
- mask_frozen : SignedWaveUpdate.FrozenAlong (PrimaryResidualClass.directions c).fast mask
- geometry (n : ℕ) : CurlClassBounds.CylindricalGeometry (HarmonicWaveInteraction.productStrip s).domain (fun (x : D × ℝ) => (χ n x).1.1) ((PrimaryResidualClass.directions c).radialField n) (fun (x : D × ℝ) => (0, 1)) ((PrimaryResidualClass.directions c).axialField (HarmonicWaveInteraction.productStrip s) n)
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The nonlinear good residual belongs to the actual primary cutoff curl, with its actual Gaussian error and any retained zero-mode alias.
The actual sum covariance and its tangent-to-curl error. The finite active label set may grow; only the proved slot/window overlap enters the estimate. The support input concerns the explicitly cut amplitude.
The first temporal increment is bounded by applying the actual moving torus inverse and stream to the residual of the constructed primary state.
The measured debt after a mean update is controlled by actual source and flux bounds. Its smoothness and support follow from the primitive mean and covariance fields.
The literal source of the updated state, including the leading radial term. No source estimate for the output state is an input.
The first rank correction is obtained from the measured debt of the actual temporal stage. Its velocity bound is derived through the five-row inverse and the moving-support stream estimate.
Data of the base, actual primary covariance, and virtual stress. No bound on the pressure, residual, temporal increment, or rank output is a field.
- operators : MeanIncrementBounds.OperatorBounds (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) c.operators ChartScales.kappa
- base : MeanIncrementBounds.BaseBounds (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) c.base
- localOperators : LocalRankDefect.LocalOperators U.carrier c.operators
- base_smooth : MeanIncrementBounds.SmoothTriple (LocalRankDefect.positiveDomain U.carrier) c.base
- profile (R : ℝ) (s : LocalSignedRequest.Plane) : s ∈ U.carrier → ∀ (Y : PressureStream.Plane), c.operators.radialProfile (R, s, Y) = c.operators.radialProfile (R, s, 0)
- covariance (i j : Fin 3) : WeightedClasses.MeanClass (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) 1 (u.covariance i j)
- covariance_smooth (i j : Fin 3) : MeanIncrementBounds.SmoothOn (PhysicalMeanDomain.slowDomain U.carrier) (u.covariance i j)
- covariance_periodic (i j : Fin 3) (n : ℕ) : PhysicalMeanDomain.PeriodicOn U.carrier (u.covariance i j n)
- covariance_support (i j : Fin 3) : CorrectionStep.GaugeSupported g.radial.inner g.radial.outer (VariableGaugeMean.qLength coord) U.carrier (u.covariance i j)
- theta : WeightedClasses.MeanClass (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) 1 c.virtualTheta
- axial : WeightedClasses.MeanClass (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) 1 c.virtualAxial
- theta_smooth : MeanIncrementBounds.SmoothOn (PhysicalMeanDomain.slowDomain U.carrier) c.virtualTheta
- axial_smooth : MeanIncrementBounds.SmoothOn (PhysicalMeanDomain.slowDomain U.carrier) c.virtualAxial
- theta_periodic (n : ℕ) : PhysicalMeanDomain.PeriodicOn U.carrier (c.virtualTheta n)
- axial_periodic (n : ℕ) : PhysicalMeanDomain.PeriodicOn U.carrier (c.virtualAxial n)
- theta_support : CorrectionStep.GaugeSupported g.radial.inner g.radial.outer (VariableGaugeMean.qLength coord) U.carrier c.virtualTheta
- axial_support : CorrectionStep.GaugeSupported g.radial.inner g.radial.outer (VariableGaugeMean.qLength coord) U.carrier c.virtualAxial
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All fields are properties of the literal first temporal stage.
- increment : MeanIncrementBounds.IncrementBounds (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) (1 - ChartScales.kappa) (VariableGaugeMean.temporalIncrementState g h index axial c (VariableGaugeMean.reconstructState g c u))
- increment_smooth : MeanIncrementBounds.SmoothTriple (PhysicalMeanDomain.slowDomain U.carrier) (VariableGaugeMean.temporalIncrementState g h index axial c (VariableGaugeMean.reconstructState g c u))
- increment_support : CorrectionStep.GaugeSupportedTriple g.radial.inner g.radial.outer (VariableGaugeMean.qLength coord) U.carrier (VariableGaugeMean.temporalIncrementState g h index axial c (VariableGaugeMean.reconstructState g c u))
- pressure_change : WeightedClasses.MeanClass (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) (1 - ChartScales.kappa) (CorrectionStep.gaugeTemporalPressureChange g h index axial c (VariableGaugeMean.reconstructState g c u))
- cumulative : CorrectionState.CumulativeBounds (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) (VariableGaugeMean.temporalStageState g h index axial c (VariableGaugeMean.reconstructState g c u))
- theta : WeightedClasses.MeanClass (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) (149 / 100) ((VariableGaugeMean.temporalStageState g h index axial c (VariableGaugeMean.reconstructState g c u)).thetaResidual c)
- axial : WeightedClasses.MeanClass (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) (149 / 100) fun (n : ℕ) (x : LocalSignedRequest.Point) => (VariableGaugeMean.temporalStageState g h index axial c (VariableGaugeMean.reconstructState g c u)).axialResidual c n x - VariableGaugeMean.temporalAliasState g h index c (VariableGaugeMean.reconstructState g c u) n (x, 0) 2
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The estimates refer to the actual rank inverse and recomputed pressure. The defect estimate is obtained after the five-row cancellation.
- increment : MeanIncrementBounds.IncrementBounds (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) (1 - ChartScales.kappa) (VariableGaugeMean.rankIncrementState g r axial c (VariableGaugeMean.temporalStageState g h index axial c (VariableGaugeMean.reconstructState g c u)))
- pressure_change : WeightedClasses.MeanClass (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) (1 - ChartScales.kappa) (CorrectionStep.gaugeRankPressureChange g r axial c (VariableGaugeMean.temporalStageState g h index axial c (VariableGaugeMean.reconstructState g c u)))
- cumulative : CorrectionState.CumulativeBounds (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) (VariableGaugeMean.rankStageState g r axial c (VariableGaugeMean.temporalStageState g h index axial c (VariableGaugeMean.reconstructState g c u)))
- mean_smooth : MeanIncrementBounds.SmoothTriple (PhysicalMeanDomain.slowDomain U.carrier) (VariableGaugeMean.rankStageState g r axial c (VariableGaugeMean.temporalStageState g h index axial c (VariableGaugeMean.reconstructState g c u))).mean
- mean_support : CorrectionStep.GaugeSupportedTriple g.radial.inner g.radial.outer (VariableGaugeMean.qLength coord) U.carrier (VariableGaugeMean.rankStageState g r axial c (VariableGaugeMean.temporalStageState g h index axial c (VariableGaugeMean.reconstructState g c u))).mean
- theta : WeightedClasses.MeanClass (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) (149 / 100) ((VariableGaugeMean.rankStageState g r axial c (VariableGaugeMean.temporalStageState g h index axial c (VariableGaugeMean.reconstructState g c u))).thetaResidual c)
- axial_residual : WeightedClasses.MeanClass (LocalSignedRequest.movingStripData U g.radial.inner g.radial.outer cL cR ha hcL hcR ε L hε hεone hL) (149 / 100) fun (n : ℕ) (x : LocalSignedRequest.Point) => (VariableGaugeMean.rankStageState g r axial c (VariableGaugeMean.temporalStageState g h index axial c (VariableGaugeMean.reconstructState g c u))).axialResidual c n x - VariableGaugeMean.temporalAliasState g h index c (VariableGaugeMean.reconstructState g c u) n (x, 0) 2
- defects : CorrectionState.DefectBounds (PhysicalMeanDomain.localSlowStripData U.carrier ⋯ ε L hε hεone hL) (1 / 5) c (VariableGaugeMean.rankStageState g r axial c (VariableGaugeMean.temporalStageState g h index axial c (VariableGaugeMean.reconstructState g c u)))
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The actual pressure, temporal, rank, and alias-retention stages meet all mean and defect bounds at sigma=1/5, from primitive primary mean data.
Levels, given by insert n (Finset.Icc (max 1 (n - 2)) (n + 2)).
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- NavierStokes.CorrectionInitialization.CommonWindow.levels n = insert n (Finset.Icc (max 1 (n - 2)) (n + 2))
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Index, given by ((levels n).image (ChartScales.nativeIndex h)).min' ((levels_nonempty n).image _).
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The same finite level window contains every actual closed dyadic support meeting the standard chart range. Endpoints are retained.
Grid radius, given by ⌈M / SlotColoring.width D j m + 2⌉.
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Grids, given by Fintype.piFinset (fun j => Finset.Icc (-gridRadius D M m j) (gridRadius D M m j)).
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Labels, given by (levels n).biUnion (fun m => (grids D M m).image (fun k => (m, k))).
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Every actual label whose closed mask support meets the bounded chart is in the explicit finite family. This is separate from the overlap bound.
Profile: an abbreviation for FinalSlowBase.actualProfile.
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Outgoing: an abbreviation for profile.outgoing.
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Nominal: an abbreviation for profile.nominal.
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Certificate: an abbreviation for profile.certificate.
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Modulation: an abbreviation for profile.modulation.
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Radial vector, given by TorusInverse.vector .radial.
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Temporal vector, given by TorusInverse.vector .temporal.
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Slots, given by PartitionedCovariance.constructedSlotSystem (CoordinateAlgebra.D h) h outgoing.data.h_pos.le radialVector temporalVector.
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These are selected outputs of the actual same-profile geometry and covariance construction. No matrix or phase estimate is a constructor input.
- prepared : PrimaryGeometryAssembly.Prepared certificate modulation upper B slots.radius N0
Prepared of
Choice, of typePrimaryGeometryAssembly.Prepared certificate modulation upper B slots.radius N0. - detGap : ℝ
Det gap of
Choice, of typeℝ. - entryBound : ℝ
Entry bound of
Choice, of typeℝ. - inverseLower : ℝ
Inverse lower of
Choice, of typeℝ. - covariance (L : PrimaryGeometryAssembly.Index nominal self.prepared.N) (p : PhaseCalculus.Slow) : p ∈ PositiveRepresentatives.positivePart (PrimaryGeometryAssembly.referenceSet nominal) → p ∈ (PrimaryGeometryAssembly.domain nominal self.prepared.N).carrier L → PrimaryCovarianceBounds.ZeroOrderBounds (√(ChartScales.S (BaseChartJets.cellBand L))) self.detGap self.entryBound self.inverseLower (PrimaryTargetBounds.movingWeight nominal p) (PrimaryTargetBounds.preparedCovariance certificate modulation self.prepared radialVector temporalVector L p) fun (j : Fin 2) => (PrimaryTargetBounds.actualTarget modulation p).ofLp j
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Choice, given by Classical.choice (choice_nonempty B N0).
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Phases, given by PrimaryGeometryAssembly.construction certificate modulation (choice B N0).prepared slots.radius_pos.
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Covariance, given by PrimaryTargetBounds.preparedCovariance certificate modulation (choice B N0).prepared radialVector temporalVector.
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Native context, given by BaseContextAssembly.nativeContext certificate modulation upper B.
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Gauge, bundling radial, length.
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The physical source and every primary phase use exactly the same profile, repaired coefficients, and Borel scale sequence.
Position as an element of SlotColoring.Position.
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Similarity scale, given by ChartScales.Q (BaseChartJets.cellBand L) * SimilarityCoordinates.coordinateQ (2 * h) (p.2.2, p.2.1).
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Spatial mask, given by PartitionedCovariance.mask (CoordinateAlgebra.D h) (PrimaryGeometryAssembly.label nominal L) (similarityScale L p) (position L p).
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Pulse coordinates, given by (x.1, x.2.2 / (phases B N0 0).L L).
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Raw velocity, constructed using PartitionedCovariance.amplitude.
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Gaussian, given by GaussianTailFlat.profile (pulseCoordinates L x).2.
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Cut velocity, given by gaussian L x • rawVelocity j L x.
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Phase point, given by (x.1, x.2.2).
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Raw pressure, constructed using ParticularWaveBounds.projectedPressure.
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Cut pressure, given by gaussian L x • rawPressure j L x.
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Geometry, bundling gap, basis, center.
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Clock window, bundling lower, upper, padding, padding_pos.
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Periodic phase as an element of ℝ.
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Common velocity, given by ∑' k : TorusInverse.Frequency, cutVelocity j L (p, (geometry j L).coordinates k Y).
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Common pressure, given by ∑' k : TorusInverse.Frequency, cutPressure j L (p, (geometry j L).coordinates k Y).
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The Gaussian cutoff is present exactly once in the common coefficient.
Source pair, bundling domain, point, point_mem, frame and the required compatibility
proofs.
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The pair used by the physical partition is the same primary ODE pair whose actual integral matrix was bounded above.
Unstretched coordinates as an element of TorusInverse.Plane.
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Common amplitude, given by ∑' k : TorusInverse.Frequency, CurlClassBounds.complexify (cutVelocity j L (p, (geometry j L).coordinates k Y)).
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Common context, given by CommonBaseContext.context certificate modulation upper B (CommonWindow.index h).
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Common gauge, bundling radial, length.
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Rank inner, given by ReservedPatches.radialSupportLeft outgoing nominal.controls.radius .mean.
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Rank outer, given by ReservedPatches.radialSupportRight outgoing nominal.controls.radius .mean.
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Rank amplitude, given by ReservedPatches.radialAmplitude outgoing nominal.controls.radius 0.
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Rank data, given by RankStateBounds.normalizedData (2 * h) (CoordinateAlgebra.A h) rankAmplitude outgoing.data.core.lam rankInner rankOuter.
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Native chart, given by ActualSignedGeometry.preparedChart certificate modulation (choice B N0).prepared slots.radius_pos.
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Native reference bounds used in correction initialization.
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Native base velocity, constructed using PrimaryCopyBounds.primaryVelocity.
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Native envelope, defined pointwise by Real.sqrt ((nativeChart B N0).weight L x) * PrimaryCopyBounds.pulseEnvelope (phases B N0) (nativeChart B N0).coordinate j L x.
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Native factors as an element of Label B N0 → ActualSignedGeometry.Native → ℝ.
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Tangent mode as an element of Fin 3 → ℝ.
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Physical tangent mode, given by ChartScales.Q (BaseChartJets.cellBand L) ^ (-CoordinateAlgebra.A h) • tangentMode j L p Y theta.
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Absolute point: an abbreviation for PhaseCalculus.Slow × TorusInverse.Plane.
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To absolute as an element of AbsolutePoint.
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From absolute as an element of LocalSignedRequest.Point.
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Chart geometry, given by { geometry j L with gap := ChartScales.nativeIndex h (BaseChartJets.cellBand L) - CommonWindow.index h n }.
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Outer raw velocity, given by PrimaryCopyBounds.outerCutoff (pulseCoordinates L x).2 • rawVelocity j L x.
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Attached raw velocity, given by WaveEdgeExtension.nativeExtension nominal (outerRawVelocity j L).
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Uncut amplitude, given by ∑' k : TorusInverse.Frequency, CurlClassBounds.complexify (attachedRawVelocity j L (p, (geometry j L).coordinates k Y)).
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Periodic gaussian, given by GaussianTailFlat.profile (PeriodicPhaseAssembly.periodicClock (geometry j L) (clockWindow L).cutoff Y / (phases B N0 0).L L).
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Outer raw pressure, given by PrimaryCopyBounds.outerCutoff (pulseCoordinates L x).2 • rawPressure j L x.
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Attached raw pressure, given by WaveEdgeExtension.nativeExtension nominal (outerRawPressure j L).
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Uncut pressure, given by ∑' k : TorusInverse.Frequency, attachedRawPressure j L (p, (geometry j L).coordinates k Y).
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Closed margins, bundling gap, entry, lower, gap_pos and the required compatibility
proofs.
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Copy cells, constructed using PeriodizedWaveBounds.nativeCells.
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Standard region, given by ActualSignedGeometry.standardSlowRegion outgoing.data.h_pos outgoing.data.h_lt_half.
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Physical position, given by ![Real.sqrt (ChartScales.Q n) * x.1, ChartScales.Q n ^ CoordinateAlgebra.D h * x.2.1.2, ChartScales.Q n * x.2.1.1].
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Physical scale, given by ChartScales.Q n * SimilarityCoordinates.coordinateQ (2 * h) x.2.1.
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Active labels as an element of Finset (Label B N0 × Fin 2).
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Full point: an abbreviation for LocalSignedRequest.Point × ℝ.
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Native slow as an element of PhaseCalculus.Slow.
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Absolute amplitude, given by ChartScales.Q (BaseChartJets.cellBand L) ^ (-CoordinateAlgebra.A h) • uncutAmplitude j L (nativeSlow L x) x.2.
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Absolute pressure, given by ChartScales.Q (BaseChartJets.cellBand L) ^ (-(2 * CoordinateAlgebra.A h)) • uncutPressure j L (nativeSlow L x) x.2.
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Absolute phase as an element of ℝ.
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Chart coefficients, bundling radius, radialBase, frequencyBase, axialBase and the
required compatibility proofs.
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Chart cutoff, given by periodicGaussian j L (toAbsolute n x.1).2.
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Piece, bundling strip, directions, coefficients, cutoff.
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Absolute tangent, defined pointwise by (HarmonicCalculus.vectorMode 1 (absolutePhase j L) (fun z => periodicGaussian j L z.1.2 • absoluteAmplitude j L z.1) x i).re.
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Absolute pressure mode, given by (HarmonicCalculus.mode 1 (absolutePhase j L) (fun z => periodicGaussian j L z.1.2 • absolutePressure j L z.1) x).re.
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The same periodic cutoff identity applies to a primary or signed native coefficient; only the actual native support is used.
A shared signed scalar stays outside the genuine lattice sum. It may be the current-state request evaluated at the common chart point.