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

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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

  • unlabeled · line 276

  • unlabeled · line 283

  • VII-B@1#eq:C-definition · line 288

  • unlabeled · line 299