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Electronic Structure and Transport Properties of Bi2Te3 and Bi2Se3 Single Crystals. / Marchenkov, Vyacheslav V.; Lukoyanov, Alexey V.; Baidak, Semyon T. et al.
In: Micromachines, Vol. 14, No. 10, 1888, 2023.

Research output: Contribution to journalArticlepeer-review

Harvard

Marchenkov, VV, Lukoyanov, AV, Baidak, ST, Perevalova, AN, Fominykh, BM, Naumov, SV & Marchenkova, EB 2023, 'Electronic Structure and Transport Properties of Bi2Te3 and Bi2Se3 Single Crystals', Micromachines, vol. 14, no. 10, 1888. https://doi.org/10.3390/mi14101888

APA

Marchenkov, V. V., Lukoyanov, A. V., Baidak, S. T., Perevalova, A. N., Fominykh, B. M., Naumov, S. V., & Marchenkova, E. B. (2023). Electronic Structure and Transport Properties of Bi2Te3 and Bi2Se3 Single Crystals. Micromachines, 14(10), [1888]. https://doi.org/10.3390/mi14101888

Vancouver

Marchenkov VV, Lukoyanov AV, Baidak ST, Perevalova AN, Fominykh BM, Naumov SV et al. Electronic Structure and Transport Properties of Bi2Te3 and Bi2Se3 Single Crystals. Micromachines. 2023;14(10):1888. doi: 10.3390/mi14101888

Author

BibTeX

@article{daed0d68cae44cdd87ea173b60f6afca,
title = "Electronic Structure and Transport Properties of Bi2Te3 and Bi2Se3 Single Crystals",
abstract = "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).",
author = "Marchenkov, {Vyacheslav V.} and Lukoyanov, {Alexey V.} and Baidak, {Semyon T.} and Perevalova, {Alexandra N.} and Fominykh, {Bogdan M.} and Naumov, {Sergey V.} and Marchenkova, {Elena B.}",
note = "This research was supported by Russian Science Foundation (project No. 22-42-02021) for the experimental and theoretical studies in Section 1, Section 2, Section 3.1 and Section 3.2 ; the analysis of current carrier concentration (Section 3.3) was done within the state assignment of Ministry of Science and Higher Education of the Russian Federation (themes «Spin», № 122021000036-3 and «Electron», № 122021000039-4).",
year = "2023",
doi = "10.3390/mi14101888",
language = "English",
volume = "14",
journal = "Micromachines",
issn = "2072-666X",
publisher = "Multidisciplinary Digital Publishing Institute (MDPI)",
number = "10",

}

RIS

TY - JOUR

T1 - Electronic Structure and Transport Properties of Bi2Te3 and Bi2Se3 Single Crystals

AU - Marchenkov, Vyacheslav V.

AU - Lukoyanov, Alexey V.

AU - Baidak, Semyon T.

AU - Perevalova, Alexandra N.

AU - Fominykh, Bogdan M.

AU - Naumov, Sergey V.

AU - Marchenkova, Elena B.

N1 - This research was supported by Russian Science Foundation (project No. 22-42-02021) for the experimental and theoretical studies in Section 1, Section 2, Section 3.1 and Section 3.2 ; the analysis of current carrier concentration (Section 3.3) was done within the state assignment of Ministry of Science and Higher Education of the Russian Federation (themes «Spin», № 122021000036-3 and «Electron», № 122021000039-4).

PY - 2023

Y1 - 2023

N2 - 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).

AB - 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).

UR - http://www.scopus.com/inward/record.url?partnerID=8YFLogxK&scp=85175032415

UR - https://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcAuth=tsmetrics&SrcApp=tsm_test&DestApp=WOS_CPL&DestLinkType=FullRecord&KeyUT=001099343200001

U2 - 10.3390/mi14101888

DO - 10.3390/mi14101888

M3 - Article

VL - 14

JO - Micromachines

JF - Micromachines

SN - 2072-666X

IS - 10

M1 - 1888

ER -

ID: 47878926