The actual initialized correction state #
This consumer uses the single primary family selected by
CorrectionInitialization.ActualPrimary, retaining its exact pressure,
Gaussian errors and common-cover chart representations.
Primary piece, given by ActualPrimary.piece ActualPrimary.standardRegion l.2 l.1.
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Angular mode, constructed using PrimaryGeometryAssembly.angularMode.
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Primary block, given by (primaryPiece l).harmonicBlock (phase l) (angularMode l).
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Tangent block, given by (primaryPiece l).tangentBlock (phase l) (angularMode l).
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Curl block, given by (primaryPiece l).differenceBlock (phase l) (angularMode l).
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Gaussian block, given by (primaryPiece l).excludedBlock (phase l) (angularMode l).
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Coefficients, bundling labels, blocks, gaussian, aliasCoefficients and the required
compatibility proofs.
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Base error, given by ActualBaseResidual.baseError ActualPrimary.certificate ActualPrimary.modulation ActualPrimary.upper B.
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Source state, given by bandSeed (coefficients B N0).labels primaryPiece (baseError B).
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Primary state, given by VariableGaugeMean.reconstructState ActualPrimary.commonGauge (ActualPrimary.commonContext B) (sourceState B N0).
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Axial, given by ((0, 1), 0).
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Temporal state, constructed using VariableGaugeMean.temporalStageState.
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Rank state, constructed using VariableGaugeMean.rankStageState.
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Initial state, given by GaugeInitialization.retainPressureAlias ActualPrimary.commonGauge (ActualPrimary.commonContext B) (rankState B N0).
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Initial alias as an element of CorrectionStep.AxisymmetricAlias.
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The initial state and its actual harmonic data are constructed together; all later iterations retain these physical labels.
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The actual nonconstant residual coefficients supplied to the first particular solve. The separate axisymmetric alias is removed only by the angular nonconstant projection.
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The actual nonlinear coefficient of a mean-zero state is its linear coefficient plus the solenoidal self-transport. Constants remain uniform before the spatial label.
Strip, given by BaseContextAssembly.nativeStrip ActualPrimary.nominal ActualPrimary.standardRegion.
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Slow strip, constructed using PhysicalMeanDomain.localSlowStripData.
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Envelope, given by ActualPrimaryBounds.meanEnvelope (l.2,l.1).
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The exact curl construction retains the same pressure coefficient.
Good block, constructed using SignedWaveUpdate.coefficientBlock.
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The real harmonic operator is the operator of the literal corrected coefficient. Only regularity of those actual fields is used here.
The actual initialized mean changes the primary residual by a term of order at least nine tenths. The retained axisymmetric aliases do not enter the nonzero harmonic coefficients.
Zero block, given by { primaryBlock l with velocity := 0, pressure := 0 }.
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Extract the actual linear-good coefficient from the proved primary field identity, retaining its literal Gaussian coefficient.
The signed request uses the same active annulus and reserved mean patch.
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All stages use one moving strip, common index, and pressure gauge.
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The remaining radial mean is controlled by the actual measured pressure debt.
Harmonic solenoidality is extracted from the actual corrected curl.
All assumptions of local harmonic extraction follow from the actual initial state and the proved support separation of its primary pieces.
Restriction to zero angle and a union of actual copy cells preserve the constants chosen before labels and copies.
Full normal, given by (primaryPiece l).coefficients.normal (primaryPiece l).strip (primaryPiece l).directions n.
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Mean control cell, given by {x | ∃ k : TorusInverse.Frequency, (x,0) ∈ ActualPrimaryBounds.controlCell n ((l.2,l.1), k)}.
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Label carrier, given by ActualInitialExcluded.labelCarrier (l.2, l.1) n.
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The literal same-choice initialized state satisfies every analytic, support, regularity, and representation field used by the correction cycle.
The radial component is included: all three actual good mean residuals have exponent six fifths.
Exact decomposition of the actual differentiated PDE, with both the mean and every stored excluded error retained.
All derivatives of the complete stored excluded error satisfy estimates for every power on the full angular and auxiliary lift.