A retarded potential evaluates each source at the event on the source's past light cone. This accounts for propagation at the speed of light and enforces causality.
For a source point and field event , the retarded time solves
For and , the function has
It is strictly increasing, so the retarded-time equation has at most one solution.
The potentials of a point charge are
with every source quantity evaluated at the retarded time.

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