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Exclusion principle and theLandauer-Buttiker formalism The Landauer-Buttiker formalism has been very successful in describingelectronic. Landauer-Büttiker formalism. Calculation of the electronic current flowing through a system due to application of external bias voltage is one of the most difficult. Landauer-Büttiker formalism. Examples. Farkas Dániel Gergely. Msc physics student. 1. Contents. Difference of potencials; Difference of temperatures.

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Buhtiker is because there is an energy to be paid to extract the electron from the medium work function. Ballistic conduction differs from superconductivity due to the absence of the Meissner effect in the material.

Normally, transport of electrons or holes is dominated by scattering events, which relax the carrier momentum in an effort to bring the conducting material to equilibrium. Consider a coherent source of electrons connected to a conductor. For example, ballistic transport can be observed in a metal nanowire: Retrieved from ” https: A comparison with light provides an analogy between ballistic and non-ballistic conduction.

Therefore, even in the case of a perfect ballistic transport, there is a fundamental ballistic conductance which saturates the current of the device with a resistance of approximately For the 1D graphene nanoribbon field effect transistor GNR-FET on the right where the channel is assumed to be ballisticthe current from A to B, given by the Boltzmann transport equationis.

In terms of scattering mechanisms, optical phonon emission buttioer dominates, depending on the material and transport conditions. Their ballisticity is nearly 0. Like monochromatic light passing through milk, electrons undergo elastic interactions.


Phys. Rev. B 45, () – Exclusion principle and the Landauer-B\”uttiker formalism

Conversely, the quantum confinement in the 1D GNR channel constricts the number of modes to carrier degeneracy and restrictions from the energy dispersion relationship and the Brillouin zone. Ballistic conduction enables use of quantum mechanical properties of electron wave functions. There are also other scattering mechanisms which apply to different carriers that are not considered here e.

To get these characteristic scattering rates, one would need to derive a Hamiltonian and solve Fermi’s golden rule for the system in question. However it is still possible to observe ballistic conduction in Si nanowires at very low temperatures 2—3 K.

Ballistic conduction

Ballistic transport is observed when the mean free path of the electron is much longer than the dimension of the medium through which the electron travels. Ballistic conduction is typically observed in quasi-1D structures, such as carbon nanotubes or silicon nanowiresbecause of extreme size quantization effects in these materials. You still can deterministically predict its behavior and use it for computation theoretically.

From Wikipedia, the free encyclopedia. Heat conduction can experience ballistic thermal transport when heating size is larger than phonon mean free paths. Such a transport regime has been found to depend on the nanoribbon edge structure and the electron energy.

InRolf Landauer proposed that conduction in a 1D system could be viewed as a transmission problem.

Thus, ballistic transport in a material is determined by how ballistically conductive that material is. Isotopically pure diamond can have a significantly higher thermal conductivity. Nanoelectronics Charge carriers Mesoscopic physics. Ballistic electrons behave like light in a waveguide or a high-quality optical assembly.


Ballistic conduction – Wikipedia

Articles needing cleanup from March Dormalism pages needing cleanup Cleanup tagged articles with a reason field from March Wikipedia pages needing cleanup from March All articles with unsourced statements Articles with unsourced statements from July Articles with unsourced statements from June Articles with unsourced statements from February The mean free path can be increased by reducing the number of impurities in a crystal or by lowering its temperature.

See List of thermal conductivities. Ballistic transport is coherent in wave mechanics terms. The widely encountered phenomenon of electrical contact resistance or ECR, arises as an electric current flowing through a rough interface is restricted to a limited number of contact spots.

Transport becomes statistical and stochastic. Electrons can be scattered several ways in a conductor. Phenomena like double-slit interferencespatial resonance and other optical or microwave -like effects could be exploited in electronic systems at nanoscale in systems including nanowires and nanotubes.

Electrons which undergo inelastic interaction are then similar to non-monochromatic light.

As mentioned, nanostructures such as carbon nanotubes or graphene nanoribbons are often considered ballistic, but these devices only very closely resemble ballistic conduction. Some kinds of scattering can only cause a change in formwlism direction, others can cause energy loss.

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