Manuscript XIX-B@1 · XIX-B.tex · lemma · b5670709
Lemma: Lemma B: witness forcing mismatch
Lemma B: the detecting forcing calculation · lines 588–680 · proof included or linked
XIX-B@1#lem:B, XIX-B@1#eq:VI-normalized, XIX-B@1#eq:forcing-residual, XIX-B@1#eq:forcing-test
On the same slab , with the transport (eq:htransport) and equal ordinary zero Cauchy data, VI's first coordinate equation becomes
The prepared candidate instead satisfies (eq:candidate-PDE). Their normalized forcing difference is
For every , its time component is nonzero as a smooth function. It is supported in the temporal preparation layer , but not in a compact spatial set.
There are a phase , , and a real nonnegative such that
Thus a real smooth witness detects the forcing mismatch.
Proof. Equation (eq:VI-first) and Lemma lem:transport give
Multiplying by gives (eq:VI-normalized). Subtracting its forcing from the candidate forcing gives
which proves (eq:forcing-residual). The sign normalization is essential: the native candidate has , not .
Suppose were identically zero. Then would be constant. Its value at is zero, so
Choose a nonempty open interval with . On , the last equality implies , hence . But the coefficient
in (eq:S00) has strictly nonzero real part on . The exponential never vanishes. This is a contradiction.
The residual vanishes for , because , and for , because . At a time where it is nonzero it is nonzero at every spatial point; its support is therefore not spatially compact.
Choose with , and choose
By continuity, on a sufficiently small interval about . Take a nonnegative nonzero time bump supported there and a nonnegative nonzero spatial bump . Then proves (eq:forcing-test). All operations are real linear after taking .
Displayed formulas in this passage
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XIX-B@1#eq:forcing-test · line 612
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