Quantitative bounds for the actual five-row matching debt #
The vanishing rescaled prefix and the drift of the held axial endpoint are estimated separately. All parameter derivatives below are actual derivatives of the constructed fields and their moment integrals.
Point: an abbreviation for ℝ × ℝ.
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Smooth extensions which preserve the entire parameter germ #
The incoming fields are smooth on their natural open strip. These explicit retractions allow the global smooth integral estimates to be used without assuming a global extension as additional data.
Parameter clamp, given by eta * (1 - OutgoingSchedule.sigma (20 * (eta ^ 2 - 1) - 1)).
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- NavierStokes.MatchingDebtBounds.parameterClamp eta = eta * (1 - NavierStokes.OutgoingSchedule.sigma (20 * (eta ^ 2 - 1) - 1))
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Radial clamp, given by X * OutgoingSchedule.sigma (scale * X + 2).
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- NavierStokes.MatchingDebtBounds.radialClamp scale X = X * NavierStokes.OutgoingSchedule.sigma (scale * X + 2)
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Strip, given by {p | -20 < scale * p.1 ∧ p.2 ∈ ReferencePath.parameterInterval}.
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- NavierStokes.MatchingDebtBounds.strip scale = {p : NavierStokes.MatchingDebtBounds.Point | -20 < scale * p.1 ∧ p.2 ∈ NavierStokes.ReferencePath.parameterInterval}
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Extend parameter, given by g (parameterClamp eta).
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Extend field, given by f (radialClamp scale p.1, parameterClamp p.2).
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The actual five-row vector and its jets #
Extended U, given by ShapeTransition.scaledFamily c.radius (extendField A.scale c.seedU).
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Extended F, constructed using ShapeTransition.scaledFamily.
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Extended debt, constructed using resetVector.
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Bounds on actual seed fields, before the shape modification or any
moment integration. They are supplied below by ordered_seed_bounds.
- logarithm (eta : ℝ) : eta ∈ Set.Icc (-1) 1 → ∀ n ≤ N, |iteratedDeriv n c.initialShape eta| ≤ BJ
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A finite-order budget, with separate vanishing and drift terms #
Vanishing sum, given by ∑ n ∈ Finset.range (N + 1), |ShapeTransition.vanishingDebtBound n B K L BG KA (ShapeTransition.separation T C P) C|.
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These constants depend only on the already fixed outgoing witness and
the requested finite order. In particular they precede j, Λ, and C.
- normalizer : ℝ
Normalizer of
FixedBounds, of typeℝ. - normalize (d : ℝ → Debt) : ContDiff ℝ (↑⊤) d → ∀ (D : ℝ), 0 ≤ D → JetBounds.FiniteJetBound N d (Set.Icc (-1) 1) D → JetBounds.FiniteJetBound N (NominalProfile.normalizedDebt F d) (Set.Icc (-1) 1) (self.normalizer * D)
- axial : ℝ
Axial of
FixedBounds, of typeℝ. - angular : ℝ
Angular of
FixedBounds, of typeℝ. - logarithm : ℝ
Logarithm of
FixedBounds, of typeℝ. - angular_jets (eta : ℝ) : eta ∈ Set.Icc (-1) 1 → ∀ n ≤ N, |iteratedDeriv n (NominalProfile.idealAmplitude F) eta| ≤ self.angular
- logarithm_jets (eta : ℝ) : eta ∈ Set.Icc (-1) 1 → ∀ n ≤ N, |iteratedDeriv n ShapeTransition.logShape eta| ≤ self.logarithm
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Fixed bounds, given by Classical.choice (fixedBounds_exists F N).
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Prefix budget, constructed using vanishingSum.
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Small control, given by c.reference.SmallLogControl (Icc (-1 : ℝ) 1) N eps c.activationTime c.kappa c.axialWidth c.angularWidth.
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- NavierStokes.MatchingDebtBounds.SmallControl c N eps = c.reference.SmallLogControl (Set.Icc (-1) 1) N eps c.activationTime c.kappa c.axialWidth c.angularWidth
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Drift budget, given by min 1 (rho / (4 * (q.normalizer * driftFactor N q.axial q.angular))).
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- NavierStokes.MatchingDebtBounds.driftBudget q rho = min 1 (rho / (4 * (q.normalizer * NavierStokes.MatchingDebtBounds.driftFactor N q.axial q.angular)))
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Matching bounds data, collecting separation, normalized_jets, shape_slope.
- normalized_jets (n : ℕ) : n ≤ N → ∀ eta ∈ Set.Icc (-1) 1, ‖iteratedFDeriv ℝ n (NominalProfile.normalizedDebt F c.debt) eta‖ < rho
- shape_slope (y eta : ℝ) : eta ∈ Set.Icc (-1) 1 → 11 / 20 ≤ 1 / 2 + deriv (fun (s : ℝ) => ShapeTransition.logProfile A.normalization c.shapeTime c.initialShape (s, eta)) y ∧ 1 / 2 + deriv (fun (s : ℝ) => ShapeTransition.logProfile A.normalization c.shapeTime c.initialShape (s, eta)) y ≤ 13 / 20
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Actual finite jets of the coefficients produced by the fixed nonlinear
inverse. The constant depends only on the requested order and that inverse.
The debt hypothesis is fulfilled by the ordered construction below, with the
target chosen to be tau^(N+1).
The thresholds hold for every incoming coefficient solution and every later control choice satisfying the displayed actual log-control estimate. Thus no new incoming profile is selected when a smaller control tolerance is required by another part of the construction.
Ordered existence with the exact entrance profile produced by the actual activation-continuation theorem. The profile is chosen before the final control order and tolerance. The same controls retain the continuation cone, the physical and logarithmic estimates, and the matching-debt bounds.
The late heat-completion radius is met by increasing the same C before
selecting the entrance profile. The assembled witness keeps that profile and
its exact continuation controls. No separation or final-debt hypothesis is
left as an input.
The analytic preparation and its cutoff margin are now chosen together. The assembled witness has the prescribed scale and normalization; both may be increased in their displayed order.
Actual nominal-profile existence from the fixed outgoing profile. The positive axial perturbation is chosen small enough for the fixed inverse, and all five moments are then repaired by its actual normalized solver.