A static background permits a Fourier transform of time difference, but a spatially varying coefficient generally prevents dependence on position difference alone. A momentum-space Green function then carries an incoming and an outgoing momentum, or equivalently one momentum together with the source position. Multiplication by a background field becomes a convolution, with a source-position phase when the Fourier basis is written as . A diagonal single-momentum representation is justified only with additional spatial translation symmetry or an explicitly fixed source origin.
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