Manuscript Em02-D@4 · Em02-D-v4.tex · theorem · fcf2fac7

Theorem: 5z leading expansion

The 5z coefficient and complete leading assembly › Explicit 5z coefficient · lines 1684–1761 · proof included or linked

Em02-D@4#thm:5z, Em02-D@4#eq:C5z

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Define

Then

and

There is no inverse-quartic leading term.

Proof. Since and on the retained patch,

Substitute Proposition prop:vertex-jets into (eq:5z-boundary). Its inverse-cubic terms are exactly (eq:C5z). The remaining boundary terms use , which is on the null boundary, including the required derivatives. The coefficient needs at most four -weight derivatives; the other terms need fewer. They are controlled by the stated common seminorm.

For the interior term, Lemma lem:regularity needs at most six -weight derivatives. On , the leading master estimates give

The -width of this layer is . Thus its contribution to (eq:5z-interior) is . On , the master and internal coefficient derivatives are uniformly bounded and all integration ranges are compact. This part is . Therefore the interior contribution is lower order than , with ample room in the claimed remainder.

For scale control, repeat the boundary and interior estimates with . The leading coefficients are multiplied by , so the boundary leading coefficient is , as required.

Finally, the exact decomposition contains no boundary term more singular than , and its nominal inverse-quartic coefficient vanishes by . The interior term is lower order. This proves the signed inverse-quartic cancellation.

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