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We present an electromagnetic analog of gravitational wave memory. That is,we consider what change has occurred to a detector of electromagnetic radiationafter the wave has passed. Rather than a distortion in the detector, as occursin the gravitational wave case, we find a residual velocity (a "kick") to thecharges in the detector. In analogy with the two types of gravitational wavememory ("ordinary" and "nonlinear") we find two types of electromagnetic kick.

An electromagnetic analog of gravitational wave memory