Electronic Transport In Mesoscopic Systems

By D. Adler. 2016

2,477 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/2d52fe7c5d8c11eb9ff06979623c57edfccd2251

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Citations in the corpus

Anisotropic electrical conductivity of polymer composites with aligned carbon nanotubes (2015, background): “It can be described by the one-dimensional Landauer-Büttiker formula of electron transport theory [39], due to the CNTeCNT contact region involves only a few atoms [48], such that.”
The hot pick-up technique for batch assembly of van der Waals heterostructures (2016, unknown): “Furthermore 16% of the measurements are strictly quasiballistic with the estimated mean-free paths exceeding the device width 27,28 .”
Tunable spin–orbit coupling and symmetry-protected edge states in graphene/WS2 (2016, background): “Our device length (∼ 20μm × 2μm) greatly exceeds the coherence length (∼ 1μm); hence the conductivity self-averages resulting in suppressed universal conductance fluctuations (UCF) [29].”
Anomalous Josephson effect induced by spin-orbit interaction and Zeeman effect in semiconductor nanowires (2014, methodology): “To obtain the scattering matrix Ŝ, we describe the normal region by a tight-binding model of square lattice model in twodimensional space (xy plane) [62], as schematically shown in Fig.”
Frequency-dependent phonon mean free path in carbon nanotubes from nonequilibrium molecular dynamics (2014, background): “It can be derived by treating the phonon-phonon scattering events as resistance sources and combining the resistances incoherently [44] or from the Boltzmann transport equation under the frequency-dependent relaxation time approximation [47].”
First-principles Green's-function method for surface calculations: A pseudopotential localized basis set approach (2017, unknown): “[24–26].”
Ab initio study of electron-phonon interaction in phosphorene (2014, methodology): “The factor (1 − vk′ ·vk |vk′ ||vk| ) takes into account the momentum loss in the scattering processes, and the thus defined relaxation time is usually named “the momentum relaxation time” and used for calculating transport properties [58,59].”
Homogeneous nonequilibrium molecular dynamics method for heat transport and spectral decomposition with many-body potentials (2018, unknown): “At the nanoscale, however, the conventional concept of the conductivity can become invalid [64] and the conductivity as defined in Eq.”
Fundamental aspects of steady-state conversion of heat to work at the nanoscale (2016, methodology): “5 below, one must have S (−B) = S (B) for any non-interacting two-terminal system as a consequence of the symmetry properties of the scattering matrix [85, 86].”
The role of contact resistance in graphene field-effect devices (2017, methodology): “graphene MG and of the total carrier transport probability T following the Landauer approach [48] as G = 4q(2)TMGh , with MG in the graphene channel and under the contact depending on the difference between the Fermi level and the Dirac point in the channel or under the contact respectively.”