Manuscript V-B@1 · V-B-v1.tex · section · 3fadc1ad

Operators and the fixed-time response

Operators and the fixed-time response · lines 372–430

V-B@1#eq:E, V-B@1#eq:B, V-B@1#eq:u, V-B@1#eq:adjoint

Back to manuscript

Let be the scalar Green operators for . Their spatial Fourier time kernels are

For componentwise massless waves write , where indicates tensor rank, and use

Its time kernel is .

These formulas define the inverses on compact distributions by transposition. Smooth Cauchy solutions follow from Fourier evolution. Finite propagation follows from the wave energy identity. On finite time intervals, all these maps are continuous in the relevant compact-data smooth topologies.

Fix a real smooth free scalar

with compact smooth Cauchy data, and fix . Define the response by

and

The scalar is held fixed in this metric functional.

Put

Then , and self-adjointness of the spatial sine propagator gives

The relevant source region is compact:

Displayed formulas in this passage

  • V-B@1#eq:E · line 383

  • V-B@1#eq:B · line 408

  • V-B@1#eq:u · line 415

  • V-B@1#eq:adjoint · line 421

  • unlabeled · line 376

  • unlabeled · line 397

  • unlabeled · line 403

  • unlabeled · line 426

Nearby in this section