Manuscript VII-B@1 · VII-B.tex · section · be632835
Spacetime, fields, and zero-Cauchy response
Classical input and geometric bookkeeping › Spacetime, fields, and zero-Cauchy response · lines 273–341
VII-B@1#eq:C-definition, VII-B@1#eq:cauchy-operator, VII-B@1#eq:cauchy-retarded, VII-B@1#eq:L-definition, VII-B@1#eq:DK
Let
Indices are raised and lowered with , and
The metric perturbation is a smooth symmetric covariant tensor. Write
The symbol without indices denotes the trace only where no confusion can arise.
Let and denote the retarded and advanced Green operators for , respectively:
The zero-Cauchy solution operator is defined by
For smooth , it can be realized for as
The right-hand side is understood as the retarded solution of the past-compact distributional source . Its restriction to has the prescribed zero Cauchy data.
The first coordinate response is
This operator is not switched.
For a compact set , set
In Minkowski spacetime this is compact. Finite propagation speed implies that depends only on in , including its trace on the initial surface.
Displayed formulas in this passage
VII-B@1#eq:cauchy-operator · line 305
VII-B@1#eq:cauchy-retarded · line 312
VII-B@1#eq:L-definition · line 327
VII-B@1#eq:DK · line 334
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VII-B@1#eq:C-definition · line 288
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