The Born approximation bremsstrahlung (and pair production) cross sections, valid at all energies and angles, are given for all possible states of longitudinal polarization of the particles involved.When the photon-incoming electron angle (θ₀) and the photon-outgoing electron angle (θ) are both zero, a cancellation of Feynman diagrams causes all cross sections to vanish in Born approximation. Further, if both θ₀ and θ are small compared to m²E₀², the "spin-flip" cross sections are small (of order θ²) relative to the "non-spin-flip" ones. When account is taken of the above cancellation, angular momentum conservation is sufficient to determine this small-angle behavior, but it explains neither the sign nor the magnitude of the bremsstrahlung circular polarization.
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K.W. McVoy (1958) studied this question.
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