Quantum Oscillations of Interlayer Conductivity in a Multilayer Topological Insulator
- Autores: Alisultanov Z.Z1,2, Abdullaev G.O2, Grigor'ev P.D3,4, Demirov N.A5
- 
							Afiliações: 
							- Abrikosov Center for Theoretical Physics, Moscow Institute of Physics and Technology
- Amirkhanov Institute of Physics, Dagestan Federal Research Center, Russian Academy of Sciences
- Landau Institute for Theoretical Physics, Russian Academy of Sciences
- National University of Science and Technology MISIS
- Joint Institute for High Temperatures, Russian Academy of Sciences
 
- Edição: Volume 163, Nº 3 (2023)
- Páginas: 401-416
- Seção: Articles
- URL: https://cardiosomatics.ru/0044-4510/article/view/653554
- DOI: https://doi.org/10.31857/S0044451023030124
- EDN: https://elibrary.ru/QFAGYG
- ID: 653554
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		                                					Resumo
Quantum and difference oscillations of interlayer conductivity in a multilayer system of thin films of topological insulators (TIs) are investigated. Due to the linearity of the carrier spectrum in such a system, new features of quantum oscillations arise. In particular, the frequencies of de Haas–van Alfvén and Shubnikov–de Haas oscillations depend quadratically on the chemical potential, rather than linearly as in systems with parabolic carrier spectrum. For the same reason, the temperature damping factor of oscillations contains the chemical potential. This is due to the nonequidistant character of the Landau levels: the higher the chemical potential, the smaller the distance between Landau levels. However, the beat frequencies, as well as the frequencies of slow oscillations, do not depend on the chemical potential; in this sense, the behavior of these systems is similar to that of conventional non-Dirac systems. Finally, in the Born approximation (in the second order cross-diagram technique), we considered the general case when the interlayer conductivity takes into account both intra- and interband transitions. We have shown that the contribution of intraband transitions is insignificant for the conductivity oscillations in the absence of magnetic impurities. However, in the presence of a Dirac point in the spectrum, a linear (in magnetic field) intraband contribution to conductivity arises from the zero Landau level. At low temperatures, this contribution is exponentially small compared to the intraband contribution and vanishes at zero temperature.
Sobre autores
Z. Alisultanov
Abrikosov Center for Theoretical Physics, Moscow Institute of Physics and Technology; Amirkhanov Institute of Physics, Dagestan Federal Research Center, Russian Academy of Sciences
														Email: zaur0102@gmail.com
				                					                																			                												                								141701, Dolgoprudny, Moscow oblast, Russia; 367015, Makhachkala, Russia						
G. Abdullaev
Amirkhanov Institute of Physics, Dagestan Federal Research Center, Russian Academy of Sciences
														Email: zaur0102@gmail.com
				                					                																			                												                								367015, Makhachkala, Russia						
P. Grigor'ev
Landau Institute for Theoretical Physics, Russian Academy of Sciences; National University of Science and Technology MISIS
														Email: zaur0102@gmail.com
				                					                																			                												                								142432, Chernogolovka, Moscow oblast, Russia;  119049, Moscow, Russia						
N. Demirov
Joint Institute for High Temperatures, Russian Academy of Sciences
							Autor responsável pela correspondência
							Email: zaur0102@gmail.com
				                					                																			                												                								125412, Moscow, Russia						
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