The physical-label estimate (21) supplies the multiplier inputs in (H1). The displacement, velocity and acceleration are the actual L² fields. The identity part of the deformation is never asserted to lie in L².
Source (21) controls actual ordered physical-label derivatives in a fixed Sobolev norm. This file converts those genuine L² blocks to uniform spatial coefficient bounds. The embedding constant is independent of the external order; only the one derivative from displacement to deformation enlarges the coefficient radius.
Embedding cost, given by sobolevEmbeddingConstant 1 3.
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Fixed H³ evaluation is applied after each external word, without a tensor-coordinate norm equivalence depending on the word length.
The bound applies to the actual continuous representative, not merely to a field chosen by the Sobolev reconstruction.
Differentiating the parent particle map once costs a fixed coefficient radius factor four and a single polynomial amplitude factor R.
Label normalization by a contraction does not enlarge positive spatial derivatives. This applies to the source scaling a=ℓ y.
The actual deformation is identity plus the derivative of the L² displacement. The identity is kept out of the spatial L² datum.
Coefficient radius, given by max 1024 (4*K).
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- EulerPacketParentLabelBounds.coefficientRadius K = max 1024 (4 * K)
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Gradient amplitude, given by embeddingCost*K^2.
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Frame amplitude, given by 1+gradientAmplitude K.
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An actual scalar label scaling with 0≤ℓ≤1 is a linear contraction.
A velocity or acceleration in the literal physical-label H⁶ word norm gives its actual spatial Jacobian at one polynomial coefficient radius.
The parent displacement bound gives the full deformation, including its constant identity, without making the identity an L² datum.