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

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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

  • XIX-B@1#eq:VI-normalized · line 593

  • XIX-B@1#eq:forcing-residual · line 600

  • XIX-B@1#eq:forcing-test · line 612

  • unlabeled · line 624

  • unlabeled · line 630

  • unlabeled · line 643

  • unlabeled · line 653

  • unlabeled · line 666

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