Manuscript XIX-B@1 · XIX-B.tex · proposition · b5670709
Proposition: The finite-time smooth inverse
Lemma C: uniqueness and the scope of an extension › A local solution operator for all smooth sources · lines 882–940 · proof included or linked
XIX-B@1#prop:local-inverse, XIX-B@1#eq:Kirchhoff, XIX-B@1#eq:homogeneous-inverse
For every smooth source , define
Then is the unique smooth zero-data solution of . It requires no spatial decay and agrees with the local compact-cutoff construction. Moreover,
is the corresponding zero-data inverse of . For spatially homogeneous ,
Proof. Let denote the normalized spherical mean. For smooth , the spherical-mean identity is
It follows by the divergence theorem, equivalently from , with its smooth value at .
Differentiate
The first endpoint term vanishes. The second derivative has endpoint term , because . The spherical-mean identity gives
The position and first time derivative vanish at . Smoothness follows by differentiation on the compact spheres and bounded time intervals. Lemma lem:C proves uniqueness.
For a compact observation set, the integration points in (eq:Kirchhoff) lie in a compact truncated causal past. Multiplication of by a smooth spatial cutoff equal to one on that region leaves the answer unchanged there. This proves the local-cutoff statement. The sign relation follows from . A homogeneous source has spherical mean , which proves (eq:homogeneous-inverse).
Displayed formulas in this passage
XIX-B@1#eq:Kirchhoff · line 885
XIX-B@1#eq:homogeneous-inverse · line 901
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