Polynomial uniform-time bounds and neighboring-label estimates for the
actual primary history. The terminal coordinate is the same at both labels.
historyVelocity_eq identifies the bounded path here with the genuine
coordinate velocity of the stationary endpoint solution.
Quantitative operator algebra for the actual fixed-space endpoint solve.
The input called R below is an inverse operator; the transverse specialization
constructs it by coercivity and discharges all of its norm bounds.
Taking adjoints preserves the norm of an operator difference.
The actual algebraic stationary correction in a fixed coordinate space.
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Endpoint operator, given by L - (correctionOperator D R A).comp L.
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The transported quadratic form used by the fixed-coordinate inverse.
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The neighboring-label estimate for the actual nonzero-terminal inverse. The inverse is the same coercive inverse as the packet construction. All constants below bound coefficients or their explicit frame-transport cost; no bound on an unknown inverse or on a supplied solution is assumed.
An abbreviation of the actual fixed-coordinate inverse, with its proved coercivity.
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- One or more equations did not get rendered due to their size.
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The literal coefficient distance for differentiating moving-frame paths.
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The polynomial sensitivity of an affine terminal-coordinate solve.
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A genuine neighboring-label bound on the physical endpoint solutions.
Polynomial size and coefficient sensitivity of the actual source (10) generator.
Only frame differences occur in the genuine generator difference.
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Uniform-time polynomial bounds from an actual L² value and generator derivative.
Reconstruct from the L² value and its prescribed generator derivative.
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History cost, given by q * traceCost T (2*c⁻¹*q*q₁) * slopeCost T d a r.
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- EulerTransverseHistoryBounds.historyCost T c q q₁ d a r = q * EulerTimeH1GeneratorBounds.traceCost T (2 * c⁻¹ * q * q₁) * EulerTransverseHistoryBounds.slopeCost T d a r
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History difference cost, constructed using δq.
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- One or more equations did not get rendered due to their size.
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The primary history has a polynomial, uniform-in-time coefficient sensitivity. In particular coefficient Lipschitz bounds give the source's physical-label Lipschitz bound with the same fixed terminal coordinate.