2015
DOI: 10.1103/physrevb.91.235123
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Ab initioelectronic transport model with explicit solution to the linearized Boltzmann transport equation

Abstract: Accurate models of carrier transport are essential for describing the electronic properties of semiconductor materials. To the best of our knowledge, the current models following the framework of the Boltzmann transport equation (BTE) either rely heavily on experimental data (i.e., semi-empirical), or utilize simplifying assumptions, such as the constant relaxation time approximation (BTE-cRTA). While these models offer valuable physical insights and accurate calculations of transport properties in some cases,… Show more

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Cited by 71 publications
(95 citation statements)
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“…Furthermore, we also have calculated the resistivity using the AMSET model which takes into account various scattering mechanisms, such as optical phonon scattering and ionized impurity scattering rather than assuming a constant relaxation time. 94 Taking these scattering mechanisms into account we calculated resistivity in the range of 0.60-0.74 mO cm, still considerably lower than the measured resistivity, reinforcing the hypothesis that the low measured mobility is due to nanosized pores and scattering from small grains. Because of the low effective mass, small E g , and the high n (410 21 cm…”
Section: à2supporting
confidence: 69%
“…Furthermore, we also have calculated the resistivity using the AMSET model which takes into account various scattering mechanisms, such as optical phonon scattering and ionized impurity scattering rather than assuming a constant relaxation time. 94 Taking these scattering mechanisms into account we calculated resistivity in the range of 0.60-0.74 mO cm, still considerably lower than the measured resistivity, reinforcing the hypothesis that the low measured mobility is due to nanosized pores and scattering from small grains. Because of the low effective mass, small E g , and the high n (410 21 cm…”
Section: à2supporting
confidence: 69%
“…Some of the historically significant models to investigate these effects include the theory of ionized-impurity scattering by Conwell, Brooks, Norton, and others [27,28,29,30,31,32], and the theory of electron-electron scattering by Matulionis, Požela, and Reklaitis [33]. Recent work aimed at recasting these earlier models for defect-induced scattering and carrier-carrier scattering in the framework of k · p perturbation theory [34] and ab initio calculations [35]. Among the scattering mechanisms described above, only the scattering theory of charged carriers by phonons has been developed far enough that predictive calculations are now possible.…”
Section: Introductionmentioning
confidence: 99%
“…To determine the transport properties, we use the rigid band approximation, in which the electronic structure is unchanged with doping and only the Fermi level is shifted appropriately. For impurity doping, ionized impurities become scatterer centers and their concentration can be calculated at a given carrier concentration by iteratively solving the charge balance equation 54 . Once µ is calculated, the electrical conductivity can be obtained at a given carrier concentration (assuming that the carrier concentration remains constant at different temperatures).…”
mentioning
confidence: 99%