Multi-ion scattering of charged carriers by ionized impurities in heavily doped semiconductors: From bulk to nanowires

Analytical expressions for the low-field mobility in heavily doped 3D, 2D, and 1D semiconductor structures are obtained using the quantum-kinetic approach. The study takes into account the multi-ion (M-ion) scattering of charge carriers by ionized impurities. The calculated dependences of the carrie...

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Bibliographic Details
Main Authors: Kovalenko, K.L (Author), Kozlovskiy, S.I (Author), Sharan, N.N (Author), Venger, E.F (Author)
Format: Article
Language:English
Published: American Institute of Physics Inc. 2022
Subjects:
Online Access:View Fulltext in Publisher
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020 |a 00218979 (ISSN) 
245 1 0 |a Multi-ion scattering of charged carriers by ionized impurities in heavily doped semiconductors: From bulk to nanowires 
260 0 |b American Institute of Physics Inc.  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1063/5.0081033 
520 3 |a Analytical expressions for the low-field mobility in heavily doped 3D, 2D, and 1D semiconductor structures are obtained using the quantum-kinetic approach. The study takes into account the multi-ion (M-ion) scattering of charge carriers by ionized impurities. The calculated dependences of the carrier mobility on doping concentration are compared with experiment in the heavily doped bulk materials (3D) Si, InP, GaAs, n-In0.49Ga0.51P, in heavily doped In0.15Ga0.85As quantum wells and InN nanowires, respectively. When calculating mobility in n-Si, the anisotropic effective masses of electrons in the valleys are taken into account. We explain the difference in the electron mobility of n-Si bulk crystals heavily doped by phosphorus and arsenic in the framework of the M-ion scattering model, which considers the scattering of electrons by interaction potentials with two characteristic lengths: the screening length and the effective radius of the doping ion. The number of ions M participating in the scattering process depends on the effective masses of charge carriers. For the light carriers with effective masses m < 0.1 m 0 (m 0 is the free electron mass), the two-ion (M = 2) scattering is more probable. For carriers with higher effective masses, three- and four-ion scattering is relevant. © 2022 Author(s). 
650 0 4 |a Analytical expressions 
650 0 4 |a Carrier concentration 
650 0 4 |a Carrier mobility 
650 0 4 |a Charged carriers 
650 0 4 |a Doped semiconductors 
650 0 4 |a Effective mass 
650 0 4 |a Electrons 
650 0 4 |a Gallium arsenide 
650 0 4 |a Heavily doped 
650 0 4 |a III-V semiconductors 
650 0 4 |a Impurities in 
650 0 4 |a Indium phosphide 
650 0 4 |a Ion scattering 
650 0 4 |a Ionization 
650 0 4 |a Ionized impurities 
650 0 4 |a Ions 
650 0 4 |a Low field mobility 
650 0 4 |a Nanowires 
650 0 4 |a Semiconducting indium phosphide 
650 0 4 |a Semiconductor alloys 
650 0 4 |a Semiconductor doping 
650 0 4 |a Semiconductor structure 
700 1 |a Kovalenko, K.L.  |e author 
700 1 |a Kozlovskiy, S.I.  |e author 
700 1 |a Sharan, N.N.  |e author 
700 1 |a Venger, E.F.  |e author 
773 |t Journal of Applied Physics