Abstract
The discovery of weak-localization effects in two-dimensional metallic systems [1] has given a new impetus to the study of transport properties of disordered conductors [2]. These effects are a direct consequence of the quantum interference between diffusively-scattered electron waves. Due to this interference, the back-scattering probability for the electron is modified during the time interval 0 < t < τφ with τφ the characteristic time, after which the phase of one of the interfering electron waves is changed.
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Van Haesendonck, C., Gijs, M., Bruynseraede, Y. (1985). Electron Scattering Times in Thin Metal Films Experimental Results. In: Kramer, B., Bergmann, G., Bruynseraede, Y. (eds) Localization, Interaction, and Transport Phenomena. Springer Series in Solid-State Sciences, vol 61. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-82516-3_22
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DOI: https://doi.org/10.1007/978-3-642-82516-3_22
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