Electronic structure of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi mathvariant="normal">Bi</mml:mi> <mml:mn>2</mml:mn> </mml:msub> <mml:msub> <mml:mi mathvariant="normal">Te</mml:mi> <mml:mn>3</mml:mn> </mml:msub

The authors successfully prepare here a high-quality side surface of the layered topological insulator Bi_{2}Te_{3}. Using DFT calculations, they clearly demonstrate the reason behind the significant anisotropy of the Dirac state and its relationship with the projection of the bulk states onto the chosen crystallographic plane. Surface spectrum calculations enable them to determine the orientation of the facets on the prepared side surface, which is found to be $(10\overline{1})$, the spectrum of which aligns perfectly with the ARPES measurements.

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Publication Details

Journal
Physical review. B./Physical review. B
Published
2025-10-02
DOI
https://doi.org/10.1103/bd4p-zrmy
Primary Topic
Topological Materials and Phenomena
Type
article
Field-Weighted Citation Impact
0.00
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article

Electronic structure of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi mathvariant="normal">Bi</mml:mi> <mml:mn>2</mml:mn> </mml:msub> <mml:msub> <mml:mi mathvariant="normal">Te</mml:mi> <mml:mn>3</mml:mn> </mml:msub

N. Kumar, К. А. Кох, I. A. Shvets, О. Е. Терещенко et al.
Physical review. B./Physical review. B
Topological Materials and Phenomena
article

Electronic structure of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi mathvariant="normal">Bi</mml:mi> <mml:mn>2</mml:mn> </mml:msub> <mml:msub> <mml:mi mathvariant="normal">Te</mml:mi> <mml:mn>3</mml:mn> </mml:msub

N. Kumar, К. А. Кох, I. A. Shvets, О. Е. Терещенко, Sergey V. Eremeev, V. A. Golyashov, Andrey S. Tarasov
article en

Abstract

The authors successfully prepare here a high-quality side surface of the layered topological insulator Bi_{2}Te_{3}. Using DFT calculations, they clearly demonstrate the reason behind the significant anisotropy of the Dirac state and its relationship with the projection of the bulk states onto the chosen crystallographic plane. Surface spectrum calculations enable them to determine the orientation of the facets on the prepared side surface, which is found to be $(10\overline{1})$, the spectrum of which aligns perfectly with the ARPES measurements.

Physical review. B./Physical review. BVol. 112(15)
Institute of Strength Physics and Materials Science (RU), Russian Academy of Sciences (RU), St Petersburg University (RU), National Research Tomsk State University (RU), Boreskov Institute of Catalysis (RU), V.S. Sobolev Institute of Geology and Mineralogy (RU), Institute of Semiconductor Physics (RU)
Openalex Percentile: Top 75%
Topological Materials and Phenomena
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Electronic structure of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi mathvariant="normal">Bi</mml:mi> <mml:mn>2</mml:mn> </mml:msub> <mml:msub> <mml:mi mathvariant="normal">Te</mml:mi> <mml:mn>3</mml:mn> </mml:msub — N. Kumar, К. А. Кох, et al. · Physical review. B./Physical review. B (2025) | TGRS Research Map | TGRS