Positive-time representatives and the genuine stable inverse branch #
The totalized coordinateQ is used only at positive time. A different,
constructed inverse extends the stable branch across its regular zero-time
face. The actual mask representatives stay at positive time.
Label: an abbreviation for PartitionedCovariance.UnsignedLabel.
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Positive time, given by {p | 0 < p.2.2}.
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Representative, given by PrimaryRepresentatives.representative (positivePart K) L.
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A smooth inverse on the stable branch, including its zero-time face #
Stable source, given by {p | 0 < p.1 ∧ 0 < scalarSlope a p.2 p.1}.
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Stable inverse, choosing the witness provided by hp.
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- NavierStokes.PositiveRepresentatives.stableInverse a p = if hp : p ∈ NavierStokes.PositiveRepresentatives.stableTarget a then Classical.choose hp else (1, p.2)
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The old closed reference set lies inside the regular stable target #
Source coordinates are (R,(Z,rho)), with rho independent of the
totalized inverse.
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- NavierStokes.PositiveRepresentatives.forwardSlow h p = (p.1, p.2.1, NavierStokes.SimilarityCoordinates.forwardScalar (2 * h) p.2.1 p.2.2)
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Lifted box, given by Icc (Real.sqrt a) (2 * Real.sqrt b) ×ˢ (Icc (-2 : ℝ) 2 ×ˢ Icc (1 / 2 : ℝ) 2).
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Lifted reference, given by liftedBox a b ∩ {p | 0 ≤ (forwardSlow h p).2.2 ∧ a * (2 * p.2.2) ≤ p.1 ^ 2 ∧ p.1 ^ 2 ≤ b * (2 * p.2.2)}.
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Stable domain, given by {p | 0 < p.1 ∧ (p.2.2, p.2.1) ∈ stableTarget (2 * h)}.
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Stable Q, given by (stableInverse (2 * h) (p.2.2, p.2.1)).1.
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- NavierStokes.PositiveRepresentatives.stableQ h p = (NavierStokes.PositiveRepresentatives.stableInverse (2 * h) (p.2.2, p.2.1)).1
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Stable X, given by p.1 ^ 2 / (2 * stableQ h p).
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- NavierStokes.PositiveRepresentatives.stableX h p = p.1 ^ 2 / (2 * NavierStokes.PositiveRepresentatives.stableQ h p)
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An open stable-branch neighborhood with fixed radial and similarity coordinate bounds. Its positive-time part is the physical domain.
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Three-mesh open box; the actual enlarged support uses two meshes.
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Positive cell, given by openGrid n k ∩ positiveTime.
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The positive cells eventually lie in any open neighborhood of the compact reference set. No lower bound for their positive time is used.
The same positive representative and a convex open domain work for every positive-time point in its enlarged two-mesh box. All coordinate range constants are uniform as time approaches zero.
Compact bounds use the genuine extension, with physical jet equality #
Stable pullback, given by stableQ h p ^ exponent * f (stableInner h p).
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- NavierStokes.PositiveRepresentatives.stablePullback h exponent f p = NavierStokes.PositiveRepresentatives.stableQ h p ^ exponent * f (NavierStokes.PositiveRepresentatives.stableInner h p)
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Physical pullback, given by SimilarityHomogeneity.chartQ h p ^ exponent * f (SimilarityHomogeneity.chartInner h p).
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- NavierStokes.PositiveRepresentatives.physicalPullback h exponent f p = NavierStokes.SimilarityHomogeneity.chartQ h p ^ exponent * f (NavierStokes.SimilarityHomogeneity.chartInner h p)
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Actual physical derivatives have one compact bound down to arbitrarily small positive time. The boundary values used in the proof are the genuine stable extension, not derivatives of a totalized inverse at zero time.
Compact reference data are transferred only at positive time #
To closed, given by ⟨L.val, L.property.1, representative K L, representative_mem K L, representative_mem_tsupport K L⟩.
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The reference functions on the compact closure are explicit extensions. Only their values at the positive representatives are identified with the physical data. No equality at zero time is assumed.
The target-direction margin is transferred from continuous extended reference data to the actual positive-time target and representative.