2018
DOI: 10.1103/physrevb.98.201201
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Magnetotransport phenomena in p -doped diamond from first principles

Abstract: We present a first-principles study of the magneto-transport phenomena in p-doped diamond via the exact solution of the linearized Boltzmann transport equation, in which the materials' parameters, including electron-phonon and phonon-phonon interactions, are obtained from density functional theory. This approach gives results in very good agreement with experimental data for Hall and drift mobilities, low-and high-field magnetoresistance and Seebeck coefficient, including the phonon drag effect, in a range of … Show more

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Cited by 41 publications
(40 citation statements)
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“…The mobility of diamond has mostly been measured in boron-doped samples and room-temperature values range from 1,450 to 3,700 cm 2 /Vs [148,151,157,150,325,158]. In this case the calculations yielded 1,830 cm 2 /Vs [152] and 2,500 cm 2 /Vs [65]. We could not find reports of electron mobility in n-type diamond.…”
Section: High-throughput Calculations Of Carrier Mobilitiesmentioning
confidence: 89%
See 1 more Smart Citation
“…The mobility of diamond has mostly been measured in boron-doped samples and room-temperature values range from 1,450 to 3,700 cm 2 /Vs [148,151,157,150,325,158]. In this case the calculations yielded 1,830 cm 2 /Vs [152] and 2,500 cm 2 /Vs [65]. We could not find reports of electron mobility in n-type diamond.…”
Section: High-throughput Calculations Of Carrier Mobilitiesmentioning
confidence: 89%
“…Inset: The corresponding Hall factor as a function of temperature; experimental data are from[158] ( ) and[159] ( ). Adapted from Ref [65]…”
mentioning
confidence: 99%
“…The theoretical data are in very good agreement with experiments, and the K-G formalism gives values that are very similar to the ones obtained with the BTE-CRT approach. The agreement between the exact and the approximate theoretical approaches is not novel (for instance, see the analysis done for simple semiconductors 39,40 ) and too surprising because, as we discussed above, a transport coefficient as the resistivity can be reproduced in a wide range of temperatures using the equilibrium band structure of the symmetric phase and a carrier relaxation time independent of temperature; the possibility to use a constant relaxation time τ justifies to a good extent the BTE-CRT approximation in which the Seebeck coefficient (as well as the Lorenz number discussed below) turns out to be independent of τ . It is important to notice that the values of the Seebeck coefficient are appreciably high in this pristine system.…”
Section: Thermoelectric Transport Coefficientsmentioning
confidence: 96%
“…through the linear response ∂ E β f nk of the electronic occupation function f nk to the electric field E and where V uc is the unit cell volume, Ω BZ the first Brillouin zone volume and, n c = (1/V uc ) n (d 3 k/Ω BZ )f nk is the carrier concentration. We solve the linearized Boltzmann transport equation (BTE) [63][64][65]:…”
Section: Carrier Mobilitymentioning
confidence: 99%