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Approximate analytic solutions for the athermal relaxation and diffusion of carriers in free-electron metals excited by ultrashort optical pulses are derived. The energy-loss time of the electrons is shown to be ~τ₀1/3τS2/3, where τ₀ and τS are characteristic electron-electron and electron-phonon scattering times. By evaluating the average excess energy per excitation we are able to establish an approximate criterion for the time of transition from an athermal electron distribution to a thermalized distribution. We thus demonstrate how one can calculate the evolution of the total energy and number densities of the nonequilibrium electrons at a given point in the metal, linking the athermal to the thermalized regime by interpolation. Quantitative agreement of the theory with some recent experiments on hot electrons in metals is good.
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Gusev et al. (1998) studied this question.
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