Actual primary covariance and the flat target #
The two columns use the two signs of the same representative and the actual Volterra primary. Target smallness at the attachment points is retained as a scalar factor throughout the finite matrix solve.
Primary phase geometry for the constructed slow base #
The representatives are chosen in the actual positive-time mask support. The phase carrier is an open two-mesh cell; the larger three-mesh cell is used for the local base estimates. Compact constants use the genuine stable inverse branch, including its regular zero-time boundary.
Plane: an abbreviation for MovingFrameODE.Plane /-! ## The actual positive support cells -/.
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The actual positive support cells #
Two meshes leave an open neighborhood of the closed one-mesh mask
support. They also give the precise 3/S³ representative distance used
by the phase comparison theorem.
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Cell domain, bundling scale, carrier, isOpen, one_le_scale.
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Restrict labels after the constants have been chosen. The actual label and its chosen positive representative are unchanged.
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- NavierStokes.PrimaryGeometryAssembly.earlierIndex hNM L = ⟨↑L, ⋯⟩
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The fixed profile, schedule, and joint label family #
Reference set, given by PrimaryRepresentatives.referenceCompact F.data.h (NominalConeAssembly.activeLeft W) (NominalConeAssembly.activeRight W).
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Index: an abbreviation for BaseChartJets.CellIndex F.data.h (NominalConeAssembly.activeLeft W) (NominalConeAssembly.activeRight W) N.
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Label, given by L.val.val.
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Domain, given by cellDomain F.data.h (NominalConeAssembly.activeLeft W) (NominalConeAssembly.activeRight W) N.
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Representative, given by PositiveRepresentatives.representative (referenceSet W) L.val.
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Base domain, given by PositiveRepresentatives.positiveCell L.val.val.1 L.val.val.2.
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Every genuinely nonzero physical mask has one of the joint positive labels used here. The implicit inverse is never evaluated at zero time.
Mean-flow charts use (T,Z), while the phase chart uses (R,(Z,T)).
This explicit map prevents their equal product types hiding a swap.
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The chart field of the very same FinalSlowBase schedule.
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Axial, given by BaseChartJets.axial (FinalSlowBase.scales H v upper B) F.data.h (FinalSlowBase.coefficients H v) (ChartScales.Q n).
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Leading frequency, given by BaseChartJets.leadingFrequency F.data.h W.axis.normalization (FinalSlowBase.coefficients H v).
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Leading axial, given by BaseChartJets.leadingAxial F.data.h (FinalSlowBase.coefficients H v).
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Shear, given by PhaseEstimates.shearVector (leadingFrequency H v) (leadingAxial H v).
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This record is an output of the concrete construction below. None of its analytic bounds are assumptions of the exported constructor.
- N : ℕ
Truncation order of
Prepared, of typeℕ. - M : ℝ
M of
Prepared, of typeℝ. - u : ℝ
U of
Prepared, of typeℝ. - eta : ℝ
Eta of
Prepared, of typeℝ. - base (L : Index W self.N) : PhaseEstimates.LocalBaseBounds (frequency H v upper B (BaseChartJets.cellBand L)) (axial H v upper B (BaseChartJets.cellBand L)) (leadingFrequency H v) (leadingAxial H v) (baseDomain W L) self.M (ChartScales.epsilon F.data.h (BaseChartJets.cellBand L))
- frequency_jets : PhaseJetBounds.PolynomialJets (domain W self.N) fun (L : Index W self.N) => frequency H v upper B (BaseChartJets.cellBand L)
- axial_jets : PhaseJetBounds.PolynomialJets (domain W self.N) fun (L : Index W self.N) => axial H v upper B (BaseChartJets.cellBand L)
- parameters (L : Index W self.N) : PrimaryRepresentatives.ParameterBounds self.M (representative W L).1 (leadingFrequency H v (representative W L)) (shear H v (representative W L))
- cone (L : Index W self.N) : PrimaryRepresentatives.ReferenceCone (leadingFrequency H v (representative W L)) (shear H v (representative W L))
- target_continuous : ContinuousOn self.target (referenceSet W)
- target_actual (p : Slow) : p ∈ referenceSet W → (PositiveRepresentatives.stableInner F.data.h p).1 ∈ Set.Ioo (NominalConeAssembly.activeLeft W) (NominalConeAssembly.activeRight W) → self.target p = PrimaryRepresentatives.normalDirection (ProfileSpectralCone.stressVector v.profiles F.data.h (PositiveRepresentatives.stableInner F.data.h p))
- target_margin (L : Index W self.N) (p : Slow) : p ∈ PositiveRepresentatives.positivePart (referenceSet W) → p ∈ (domain W self.N).carrier L → inner ℝ (self.target p) (PrimaryRepresentatives.normalDirection (shear H v (representative W L))) ≤ -self.eta ∧ |PrimaryRepresentatives.c0 (leadingFrequency H v (representative W L)) (shear H v (representative W L)) * inner ℝ (self.target p) (PrimaryRepresentatives.transverseDirection (shear H v (representative W L))) / inner ℝ (self.target p) (PrimaryRepresentatives.normalDirection (shear H v (representative W L)))| + self.eta ≤ PrimaryRepresentatives.slopeRatio self.u
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Phase sign, with branches according to c = 0.
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The actual positive representatives instantiate every entry of the phase data, including the unstable eigenpair and the nonzero rounding.
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Both signs have one joint domain and the same constants, which were
fixed before its band threshold. All phase comparison outputs are proved
by FamilyData.construction.
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- NavierStokes.PrimaryGeometryAssembly.construction H v a hr0 c = (NavierStokes.PrimaryGeometryAssembly.family H v a c).construction ⋯ hr0 ⋯ ⋯ ⋯ ⋯ ⋯ ⋯
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Every fixed chart, radial, and slot constant is enlarged before any phase band is selected.
The smooth summed base, its positive mask representatives, and the
actual strict cone supply every datum used by the phase theorem. The
last threshold is chosen only after u, the target margin, and M.
The same threshold applies to every active label and to both signs.
A selected, fully constructed datum. The caller supplies no local base bound, eigenpair estimate, or phase comparison.
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- NavierStokes.PrimaryGeometryAssembly.prepared H v hcone upper B r0 hbox N0 = Classical.choice ⋯
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Phases, given by construction H v (prepared H v hcone upper B r0 hbox N0) hr0.
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A canonical box large enough for every enlarged chart of the active
annulus. This uses exactly FinalSlowBase.scales H v (2*activeRight) B.
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- NavierStokes.PrimaryGeometryAssembly.canonicalPrepared H v hcone B r0 N0 = NavierStokes.PrimaryGeometryAssembly.prepared H v hcone (2 * NavierStokes.NominalConeAssembly.activeRight W) B r0 ⋯ N0
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Canonical phases, given by construction H v (canonicalPrepared H v hcone B r0 N0) hr0.
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The actual integer angular mode is retained; zero-floor rounding is not replaced by an unproved assertion that a real frequency is integral.
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A later common cutoff preserves the already selected geometry #
Restriction changes only the set of admissible labels. It does not reselect a target direction, parameter constant, representative, or Fourier mode. A final consumer can therefore take the maximum of its covariance cutoff and this geometry cutoff.
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Phase sign, with branches according to j = 0.
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The normal and transverse columns in the fixed physical tangent plane.
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- NavierStokes.PrimaryTargetBounds.basisMatrix K i j = if j = 0 then (NavierStokes.MovingFrameODE.quarterTurn K).ofLp i else K.ofLp i
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Model normal, given by -⟪T, MovingFrameODE.quarterTurn K⟫_ℝ.
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Model transverse, given by ⟪T, K⟫_ℝ.
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Model point: an abbreviation for ℝ × (Plane × Plane).
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Model set as an element of Set ModelPoint.
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Model vector, given by (-s) • K + (c * Real.sqrt (1 + s ^ 2)) • MovingFrameODE.quarterTurn K.
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Pulse ratio as an element of Plane.
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Geometric ratio constant as an element of ℝ.
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Ratio constant, constructed using geometricRatioConstant.
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The actual uncut primary is compared with the central signed model.
The two errors have the concentration-compatible orders 1/L and
|v-L/2|/L; no covariance convergence is a hypothesis.
The two signs share the same actual representative.
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The native finite covariance with the original joint label.
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Uniform finite-matrix bounds follow from the actual constructed phases and their ODEs. The model point only records the common representative and a unit target direction.
The mixed target margin is supplied by the actual closed profile direction and its actual positive representative.
Prepared covariance, given by familyCovariance vr vt (family H v a).
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One later cutoff, with all representatives, targets and phases kept fixed, supplies the actual normalized determinant and inverse bounds.
Left radius, given by Real.sqrt (2 * NominalConeAssembly.activeLeft W).
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Right radius, given by Real.sqrt (2 * NominalConeAssembly.activeRight W).
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These are the radial-log coefficients of the very same product weight, not a replacement weight with a faster decay.
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Profile radius, given by p.1 / Real.sqrt (BaseChartJets.normalizedCoordinates h p).1.
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Moving weight, given by stripWeight W (profileRadius F.data.h p).
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The mean-variable ordering (R,((T,Z),Y)) uses exactly the same
normalized point (R,(Z,T)).
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Exact equality with the strip used for the signed correction.
The literal leading covariance target in its own normalized band.
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Target amplitude as an element of ℝ.
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The chart target at its own band is exactly the actual leading stress times the residual scalar coordinate.
The actual primary covariance and the actual leading target satisfy all order-zero hypotheses used for positive square-root weights, with the same moving flat weight through both closed attachment edges.
A single final band threshold suffices. Restriction retains the original representative, carrier and phase on each surviving label.
The source profile supplies the whole geometry. There is no extra target orientation, determinant, inverse-weight or ODE-error input.