Manuscript VII-I@1 · VII-I.tex · theorem · 907e96ab

Theorem: Classical auxiliary-coordinate equivalence

Route B3: constrained auxiliary coordinates › Classical equivalence, not an independent coordinate field · lines 1563–1591 · proof included or linked

VII-I@1#thm:auxequivalence

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For every smooth metric jet , the constraints (eq:auxiliary-constraints) have exactly one solution. Projection from their solution graph to is bijective, and substituting that solution into

gives the original sharp .

The same statement holds for the prepared density equations, with their corresponding coefficients and zero data.

Proof. The first equation is a linear Cauchy problem with prescribed zero data. Its unique solution is . With that solution inserted, the second is another linear inhomogeneous Cauchy problem, whose unique solution is (eq:coordinate-coefficients). The observable equality is substitution into its formal inverse-map expansion. The prepared equations are handled in the same order.

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