词条 | Landauer formula |
释义 |
The Landauer formula—named after Rolf Landauer, who first suggested its prototype in 1957[1]—is a formula relating the electrical resistance of a quantum conductor to the scattering properties of the conductor.[2] In the simplest case where the system only has two terminals, and the scattering matrix of the conductor does not depend on energy, the formula reads where is the electrical conductance, is the conductance quantum, are the transmission eigenvalues of the channels, and the sum runs over all transport channels in the conductor. This formula is very simple and physically sensible: The conductance of a nanoscale conductor is given by the sum of all the transmission possibilities that an electron has when propagating with an energy equal to the chemical potential, . A generalization of the Landauer formula for multiple probes is the Landauer-Büttiker formula,[3] proposed by Landauer and {{Interlanguage link|Markus Büttiker|de||WD=}}. If probe has voltage (that is, its chemical potential is ), and is the sum of transmission probabilities from probe to probe (note that may or may not equal ), the net current leaving probe is See also
References1. ^{{cite journal|last1=Landauer|first1=R. |title=Spatial Variation of Currents and Fields Due to Localized Scatterers in Metallic Conduction|year=1957|journal=IBM Journal of Research and Development|volume=1|pages=223–231|doi=10.1147/rd.13.0223}} 2. ^{{cite book|last1=Nazarov|first1=Y. V.|last2=Blanter|first2=Ya. M. |title=Quantum transport: Introduction to Nanoscience|year=2009|publisher=Cambridge University Press|isbn=978-0521832465|pages=29–41}} 3. ^{{cite thesis |last=Bestwick|first=Andrew J. |date=2015|title=Quantum Edge Transport in Topological Insulators |publisher=Stanford University}} 3 : Mesoscopic physics|Quantum mechanics|Nanoelectronics |
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