Stage estimates with the current-band particular fields #
The signed waves and mean increments retain their actual native inputs. The particular contribution is an independently constructed physical field, with no physical copy-family representation imposed on it.
The actual particular waves on valid physical charts #
The physical representative uses only the literal current-band solve. Its compatibility is obtained from the corresponding current-source transport laws. No value of a reference solve on an excluded face is used to define the physical representative.
Coherence of the actual current-band particular potential #
The common copy coefficient is retained, including its cutoffs. Its vector potential is transported before taking the physical curl. The derivative identity uses an invertible linear chart and does not require an additional smoothness assumption on the phase.
The phase scale cancels the inverse carrier in the literal potential. An invertible chart also handles the convention for a nonexistent derivative.
The physical potential has the scale exponent h, one half below the
velocity exponent.
Label: an abbreviation for ActualParticularStageControls.Label.
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The potential of the actual current common coefficient.
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The complete harmonic pressure, with the actual current common pressure coefficient and the same carrier.
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Only the phase needs a germ: the undifferentiated raw amplitude is evaluated at the point.
The pressure carrier is transported exactly together with its scalar coefficient.
Current-copy potential covariance is a consequence of actual source continuity, support/order, and incoming state/block coherence.
The full current harmonic pressure has the square velocity scale.
Equality holds as an ambient germ at every point of the open slow overlap, including all free radial, angular, and fast coordinates.
Removing the native scales from the current particular modes #
The native potential and pressure transformation laws imply equality of their actual physical modes. The angle and Cartesian rotation are the same at both bands, so the native scale cancels before applying either map.
Cancel a positive native scale before applying a physical coordinate map. No regularity or linearity of that later map is required.
The actual current-band vector potential becomes independent of the band once its native transformation law is supplied.
The pressure weight cancels the physical factor with exponent -2A.
The real part is taken only after cancelling the complex native modes.
The actual finite current-band potential, in the initializer's label order.
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Local pressure, given by ActualCurrentParticularPhysical.localPressure (ActualCycleParameters.particularState x) n.
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One representative of the actual current-band potential formulas.
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Pressure, given by ValidDyadicBandCover.field h N (localPressure x).
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Glued potential: an abbreviation for @potential.
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Glued pressure: an abbreviation for @pressure.
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The same physical polar angle is used in both bands. The comparison therefore retains the complete fast fiber instead of choosing new angles.
Physical jet bounds for the actual current particular label sum #
The closed label windows bound the number of contributing spatial labels. The two column choices are retained by the signed-label map and are already included in the 2250-color palette. The finite harmonic sum remains explicit.
Signed label, given by ActualPrimaryCovariance.signedLabelOf (l.2, l.1).
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Window position, given by ![AnnularEndpoint.radius w, w.2 2, 1 - w.1].
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Window, given by (SquaredPartition.logCoordinate (PhysicalWaveSum.physicalQ h w), windowPosition w).
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Chart point, constructed using ActualCarrierTransport.associatedPoint.
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The genuine one-mesh native support is contained in the two-mesh physical box. The column sign does not change the physical box.
Full refined support, including the native dyadic factor and the slow mask, puts a physical point in its actual signed label's closed window.
Finite harmonic sums with uniform spatial multiplicity #
The spatial factor is 2250, independently of the number of labels.
Different harmonics may retain different constants. All jet hypotheses
are pointwise at w; the open band is used only for support and germs.
The incoming actual invariant supplies all mode regularity #
Per-mode physical smoothness on the whole open valid band, including the axis. The invariant supplies source regularity and the actual raw boundary values; at the axis the retained support gives a zero germ.
Bound type used in glued stage estimates.
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These are the original native signed-wave data, without an unrelated particular copy-family field.
- potential : ℕ → PhysicalStageBounds.WaveData CorrectionInitialization.ActualPrimary.h D (Fin 3 × I) K (Fin 3)
Potential of
SignedInputs, of typeℕ → PhysicalStageBounds.WaveData h D (Fin 3 × I) K (Fin 3). - pressure : ℕ → PhysicalStageBounds.WaveData CorrectionInitialization.ActualPrimary.h D I K Unit
Pressure field of
SignedInputs, of typeℕ → PhysicalStageBounds.WaveData h D I K Unit. - potential_exponent (j : ℕ) : 1 / 2 + ActualIterationLedger.sigma j - ChartScales.kappa ≤ (self.potential j).alpha
- pressure_exponent (j : ℕ) : 1 + ActualIterationLedger.sigma j - ChartScales.kappa ≤ (self.pressure j).alpha
- pressure_shift (j : ℕ) : (self.pressure j).shift = -(2 * CoordinateAlgebra.A CorrectionInitialization.ActualPrimary.h)
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Signed mean potential as an element of VelocityField.
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Signed mean pressure, defined pointwise by (W.pressure j).pressure w + (ActualStageEstimates.pressureInput R M hN j).family.field w.
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- NavierStokes.GluedStageEstimates.signedMeanPressure R M hN W j w = (W.pressure j).pressure w + (NavierStokes.ActualStageEstimates.pressureInput R M hN j).family.field w
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Direct, given by (ActualStageEstimates.angularInput R M hN j).family.angularField.
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A physical particular contribution and the same mixed sequence #
Potential loss, given by max (L m) (PhysicalStageBounds.potentialLoss h h 0 m).
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Pressure loss, given by max (L m) (PhysicalStageBounds.pressureLoss h (2 * CoordinateAlgebra.A h) 0 m).
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The four literal contributions use the same order as the physical sequence construction.
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Pressure, defined pointwise by particularP j w + (W.pressure j).pressure w + (ActualStageEstimates.pressureInput R M hN j).family.field w.
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- NavierStokes.GluedStageEstimates.pressure R M hN W particularP j w = particularP j w + (W.pressure j).pressure w + (NavierStokes.ActualStageEstimates.pressureInput R M hN j).family.field w
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Six field identities on the common open sublevel. Their only content is identification of the actual sequence and its physical components.
- potential_zero : Set.EqOn (A 0) (ActualPhysicalStageBounds.initialPotential CorrectionInitialization.ActualPrimary.certificate CorrectionInitialization.ActualPrimary.modulation CorrectionInitialization.ActualPrimary.upper B WA (ActualPhysicalStageBounds.actualInitialTemporalInput B N0 N hN) (ActualPhysicalStageBounds.actualInitialRankInput B N0 N hN)) (CutStageEstimates.physicalSublevel CorrectionInitialization.ActualPrimary.h qbig)
- direct_zero : Set.EqOn (Bdirect 0) (ActualMeanPhysicalData.initialAngularFamily B N0 N).angularField (CutStageEstimates.physicalSublevel CorrectionInitialization.ActualPrimary.h qbig)
- pressure_zero : Set.EqOn (P 0) (fun (w : ProblemStatement.SpaceTime) => FinalSlowBase.pressure CorrectionInitialization.ActualPrimary.certificate CorrectionInitialization.ActualPrimary.modulation CorrectionInitialization.ActualPrimary.upper B w + ActualPhysicalStageBounds.initialPressureIncrement WP (ActualPhysicalStageBounds.actualInitialPressureInput B N0 N hN) w) (CutStageEstimates.physicalSublevel CorrectionInitialization.ActualPrimary.h qbig)
- potential_succ (j : ℕ) : Set.EqOn (potential R M hN W particularA j) (A (j + 1)) (CutStageEstimates.physicalSublevel CorrectionInitialization.ActualPrimary.h qbig)
- direct_succ (j : ℕ) : Set.EqOn (direct R M hN j) (Bdirect (j + 1)) (CutStageEstimates.physicalSublevel CorrectionInitialization.ActualPrimary.h qbig)
- pressure_succ (j : ℕ) : Set.EqOn (pressure R M hN W particularP j) (P (j + 1)) (CutStageEstimates.physicalSublevel CorrectionInitialization.ActualPrimary.h qbig)
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The algebraic consumer of the separate current-particular estimates. The fixed-run native inputs derive all signed and mean estimates here.
The residual floor is fixed to the next band. Only exact physical realizations of finite prefixes enter the residual part of the proof.
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The literal fields and native source data of the fixed run #
Current potential, given by ActualValidBandWaves.gluedPotential (ActualCyclePreservation.state B N0 j) N.
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Current pressure, given by ActualValidBandWaves.gluedPressure (ActualCyclePreservation.state B N0 j) N.
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Transfer a uniform estimate on comparable current bands to their actual glued representative. The bound has no factor counting charts.
The actual finite harmonic sum keeps the geometric factor 2250. The harmonic constants are summed before the band and point are chosen.
The source class is derived from the stored residual invariant and the actual label/coordinate reindexing.
The current-phase loss fits inside the original physical wave loss.
The inequality uses the fixed condition h < 1/2.
The representation record specialized to the exact glued particular fields and the constructed initial primary wave data.
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The actual glued current-band rates, native signed/mean data, and exact finite-prefix realizations supply the complete mixed-stage record. No physical derivative estimate is a premise of this constructor.
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