Abstract
Landauer derived the relation between the conductance of a one-dimensional (1D) wire and the transmission and reflection probabilities at the Fermi level [1]. Let us consider the system schematically illustrated in Fig. 1.3.1. A wire is connected at both ends to an ideal wire which is infinitely long and eventually connected to an electron reservoir. The ideal reservoir satisfies the following two conditions:
-
(1)
All incident electrons are absorbed by the reservoir irrespective of their energy and phase.
-
(2)
It constantly provides electrons with energy below chemical potential µ. The energy and phase of these electrons are independent of those of absorbed electrons.
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Ando, T. (1998). Landauer’s Formula. In: Ando, T., Arakawa, Y., Furuya, K., Komiyama, S., Nakashima, H. (eds) Mesoscopic Physics and Electronics. NanoScience and Technology. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-71976-9_3
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