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
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
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