Electric-field distribution in a quantum superlattice with an injecting contact: Exact solution
- Autores: Maksimenko V.A.1,2, Makarov V.V.1, Koronovskii A.A.2, Hramov A.E.1,2, Venckevičius R.3, Valušis G.3, Balanov A.G.1,4, Kusmartsev F.V.4, Alekseev K.N.4
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							Afiliações: 
							- Yuri Gagarin State Technical University of Saratov
- National Research Saratov State University
- Terahertz Photonics Laboratory
- Department of Physics
 
- Edição: Volume 103, Nº 7 (2016)
- Páginas: 465-470
- Seção: Condensed Matter
- URL: https://journals.rcsi.science/0021-3640/article/view/159210
- DOI: https://doi.org/10.1134/S0021364016070080
- ID: 159210
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Resumo
A very simple model describing steady-state electron transport along a quantum superlattice of a finite length taking into account an arbitrary electrical characteristic of the injecting contact is considered. In the singleminiband approximation, exact formulas for the spatial distribution of the electric field in the superlattice are derived for different types of contact. Conditions under which the field is uniform are identified. Analytical expressions for the current–voltage characteristics are obtained. In the context of the developed theory, the possibility of attaining uniform-field conditions in a diode structure with a natural silicon-carbide superlattice is discussed.
Sobre autores
V. Maksimenko
Yuri Gagarin State Technical University of Saratov; National Research Saratov State University
														Email: K.Alekseev2@lboro.ac.uk
				                					                																			                												                	Rússia, 							ul. Politekhnicheskaya 77, Saratov, 410054; ul. Astrakhanskaya 83, Saratov, 410012						
V. Makarov
Yuri Gagarin State Technical University of Saratov
														Email: K.Alekseev2@lboro.ac.uk
				                					                																			                												                	Rússia, 							ul. Politekhnicheskaya 77, Saratov, 410054						
A. Koronovskii
National Research Saratov State University
														Email: K.Alekseev2@lboro.ac.uk
				                					                																			                												                	Rússia, 							ul. Astrakhanskaya 83, Saratov, 410012						
A. Hramov
Yuri Gagarin State Technical University of Saratov; National Research Saratov State University
														Email: K.Alekseev2@lboro.ac.uk
				                					                																			                												                	Rússia, 							ul. Politekhnicheskaya 77, Saratov, 410054; ul. Astrakhanskaya 83, Saratov, 410012						
R. Venckevičius
Terahertz Photonics Laboratory
														Email: K.Alekseev2@lboro.ac.uk
				                					                																			                												                	Lituânia, 							Vilnius, LT-01108						
G. Valušis
Terahertz Photonics Laboratory
														Email: K.Alekseev2@lboro.ac.uk
				                					                																			                												                	Lituânia, 							Vilnius, LT-01108						
A. Balanov
Yuri Gagarin State Technical University of Saratov; Department of Physics
														Email: K.Alekseev2@lboro.ac.uk
				                					                																			                												                	Rússia, 							ul. Politekhnicheskaya 77, Saratov, 410054; Loughborough, LE11 3TU						
F. Kusmartsev
Department of Physics
														Email: K.Alekseev2@lboro.ac.uk
				                					                																			                												                	Reino Unido da Grã-Bretanha e Irlanda do Norte, 							Loughborough, LE11 3TU						
K. Alekseev
Department of Physics
							Autor responsável pela correspondência
							Email: K.Alekseev2@lboro.ac.uk
				                					                																			                												                	Reino Unido da Grã-Bretanha e Irlanda do Norte, 							Loughborough, LE11 3TU						
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