The propagator for a charged particle in a time‐dependent electric field is calculated following Hida and Streit's framework [1] where the propagator is the T‐transform of Feynman functional. However, we have to regard the potential V = −qE(τ)x≡mξ̇x following C. C. Bernido and M. V. Carpio‐Bernido's [2] prescription of time‐dependent potentials. The result agrees with the limiting form of Eqn. (16) of N. Morgenstern Horing, H. L. Cui, and G. Fiorenza [3], when the magnetic field is switched off, and Eqn. (17) of [3] when the electric field is constant in time.

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