Manuscript XI-D@1 · XI-D.tex · theorem · 994a5c1b
Theorem: The bare insertion is not generally free-closed
A necessary free-order closure condition › An explicit free-shell witness · lines 729–793 · proof included or linked
XI-D@1#thm:freewitness, XI-D@1#eq:S, XI-D@1#eq:witness
For every and every , there are admissible nonnegative observation tests and a smooth free multiplet configuration for which
In particular, this variation is not generally a functional vanishing on all free configurations.
Proof. Work over the Grassmann algebra with odd and nonzero. Set
Every equation in (eq:freeshell) holds. The ghost is an affine wave solution, and no ghost initial-data restriction in XI-B excludes it.
Here
so
The spatially constant zero-data wave response is therefore
The spatial components vanish. Ramp symmetry gives
It follows that
where when .
Choose with , and a small time interval on which it has a fixed nonzero sign. Choose , nonzero, compactly supported in that interval and in a spatial ball. Since there, the ordinary coefficient of in (eq:witness) is nonzero.
The switch and plateau may be chosen to contain this observation region while satisfying the frozen support requirements. They do not enter (eq:witness).
Displayed formulas in this passage
XI-D@1#eq:S · line 771
XI-D@1#eq:witness · line 776
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