Abstract
The quantum electrons dynamics in a thin metal film is studied numerically using the self-consistent Wigner-Poisson equations. The initial equilibrium is computed from the Kohn-Sham equations at finite temperature, and then mapped into the phase-space Wigner function. The time-dependent results are compared systematically with those obtained previously with a classical approach (Vlasov-Poisson equations). It is found that, for large excitations, the quantum and classical dynamics display the same low-frequency oscillations due to ballistic electrons bouncing back and forth on the film surfaces. However, below a certain excitation energy (roughly corresponding to one quantum of plasmon energy haωp), the quantum and classical results diverge, and the ballistic oscillations are no longer observed. These results provide an example of a quantum-classical transition that may be observed with current pump-probe experiments on thin metal films. ©IOP Publishing Ltd and Deutsche Physikalische Gesellschaft.
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CITATION STYLE
Jasiak, R., Manfredi, G., Hervieux, P. A., & Haefele, M. (2009). Quantum-classical transition in the electron dynamics of thin metal films. New Journal of Physics, 11. https://doi.org/10.1088/1367-2630/11/6/063042
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