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Electronic Structure and Transport Properties of Bi2Te3 and Bi2Se3 Single Crystals
The electrical resistivity and the Hall effect of topological insulator Bi2Te3 and Bi2Se3 single crystals were studied in the temperature range from 4.2 to 300 K and in magnetic fields up to 10 T. Theoretical calculations of the electronic structure of these compounds were carried out in density fun...
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Published in: | Micromachines (Basel) 2023-09, Vol.14 (10), p.1888 |
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creator | Marchenkov, Vyacheslav V. Lukoyanov, Alexey V. Baidak, Semyon T. Perevalova, Alexandra N. Fominykh, Bogdan M. Naumov, Sergey V. Marchenkova, Elena B. |
description | The electrical resistivity and the Hall effect of topological insulator Bi2Te3 and Bi2Se3 single crystals were studied in the temperature range from 4.2 to 300 K and in magnetic fields up to 10 T. Theoretical calculations of the electronic structure of these compounds were carried out in density functional approach, taking into account spin–orbit coupling and crystal structure data for temperatures of 5, 50 and 300 K. A clear correlation was found between the density of electronic states at the Fermi level and the current carrier concentration. In the case of Bi2Te3, the density of states at the Fermi level and the current carrier concentration increase with increasing temperature, from 0.296 states eV−1 cell−1 (5 K) to 0.307 states eV−1 cell−1 (300 K) and from 0.9 × 1019 cm−3 (5 K) to 2.6 × 1019 cm−3 (300 K), respectively. On the contrary, in the case of Bi2Se3, the density of states decreases with increasing temperature, from 0.201 states eV−1 cell−1 (5 K) to 0.198 states eV−1 cell−1 (300 K), and, as a consequence, the charge carrier concentration also decreases from 2.94 × 1019 cm−3 (5 K) to 2.81 × 1019 cm−3 (300 K). |
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Theoretical calculations of the electronic structure of these compounds were carried out in density functional approach, taking into account spin–orbit coupling and crystal structure data for temperatures of 5, 50 and 300 K. A clear correlation was found between the density of electronic states at the Fermi level and the current carrier concentration. In the case of Bi2Te3, the density of states at the Fermi level and the current carrier concentration increase with increasing temperature, from 0.296 states eV−1 cell−1 (5 K) to 0.307 states eV−1 cell−1 (300 K) and from 0.9 × 1019 cm−3 (5 K) to 2.6 × 1019 cm−3 (300 K), respectively. On the contrary, in the case of Bi2Se3, the density of states decreases with increasing temperature, from 0.201 states eV−1 cell−1 (5 K) to 0.198 states eV−1 cell−1 (300 K), and, as a consequence, the charge carrier concentration also decreases from 2.94 × 1019 cm−3 (5 K) to 2.81 × 1019 cm−3 (300 K).</description><identifier>ISSN: 2072-666X</identifier><identifier>EISSN: 2072-666X</identifier><identifier>DOI: 10.3390/mi14101888</identifier><language>eng</language><publisher>Basel: MDPI AG</publisher><subject>2D materials ; Bi2Se3 ; Bi2Te3 ; Bismuth tellurides ; Carrier density ; Collaboration ; Crystal structure ; Current carriers ; Density of states ; DFT ; Electromagnetism ; Electron states ; Electronic structure ; Energy ; Fermi level ; Hall effect ; Magnetic fields ; Scanning electron microscopy ; Single crystals ; Spin-orbit interactions ; Symmetry ; topological insulator ; Topological insulators ; Transport properties</subject><ispartof>Micromachines (Basel), 2023-09, Vol.14 (10), p.1888</ispartof><rights>2023 by the authors. 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Theoretical calculations of the electronic structure of these compounds were carried out in density functional approach, taking into account spin–orbit coupling and crystal structure data for temperatures of 5, 50 and 300 K. A clear correlation was found between the density of electronic states at the Fermi level and the current carrier concentration. In the case of Bi2Te3, the density of states at the Fermi level and the current carrier concentration increase with increasing temperature, from 0.296 states eV−1 cell−1 (5 K) to 0.307 states eV−1 cell−1 (300 K) and from 0.9 × 1019 cm−3 (5 K) to 2.6 × 1019 cm−3 (300 K), respectively. On the contrary, in the case of Bi2Se3, the density of states decreases with increasing temperature, from 0.201 states eV−1 cell−1 (5 K) to 0.198 states eV−1 cell−1 (300 K), and, as a consequence, the charge carrier concentration also decreases from 2.94 × 1019 cm−3 (5 K) to 2.81 × 1019 cm−3 (300 K).</abstract><cop>Basel</cop><pub>MDPI AG</pub><doi>10.3390/mi14101888</doi><orcidid>https://orcid.org/0000-0003-2044-1789</orcidid><orcidid>https://orcid.org/0000-0003-4459-0893</orcidid><orcidid>https://orcid.org/0000-0002-4755-3839</orcidid><orcidid>https://orcid.org/0000-0002-8540-8720</orcidid><orcidid>https://orcid.org/0009-0001-1618-6773</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | 2D materials Bi2Se3 Bi2Te3 Bismuth tellurides Carrier density Collaboration Crystal structure Current carriers Density of states DFT Electromagnetism Electron states Electronic structure Energy Fermi level Hall effect Magnetic fields Scanning electron microscopy Single crystals Spin-orbit interactions Symmetry topological insulator Topological insulators Transport properties |
title | Electronic Structure and Transport Properties of Bi2Te3 and Bi2Se3 Single Crystals |
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