An exact Maxwell field for an accelerated light-like charge is constructed, combining a Coulomb-like part and a radiative part, and reducing to the known Coulomb analogue when the acceleration vanishes.
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Models of light-like charges with non-geodesic world lines
An exact Maxwell field for an accelerated light-like charge is constructed, combining a Coulomb-like part and a radiative part, and reducing to the known Coulomb analogue when the acceleration vanishes.