NMR studies of single crystals of the topological insulator Bi2Te3 at low temperatures
- Autores: Naumov S.V.1, Perevozchikova Y.A.1, Chistyakov V.V.1, Marchenkova E.B.1, Weber H.W.2, Huang J.C.3, Marchenkov V.V.1,4, Antonenko A.O.5, Charnaya E.V.5, Nefedov D.Y.5, Podorozhkin D.Y.5, Uskov A.V.5, Bugaev A.S.6, Lee M.K.3, Chang L.J.3
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Afiliações:
- Mikheev Institute of Metal Physics, Ural Branch
- Atominstitut—Institute of Atomic and Subatomic Physics
- National Cheng Kung University
- Ural Federal University
- St. Petersburg State University
- Moscow Institute of Physics and Technology (State University)
- Edição: Volume 59, Nº 5 (2017)
- Páginas: 855-859
- Seção: Semiconductors
- URL: https://ogarev-online.ru/1063-7834/article/view/200135
- DOI: https://doi.org/10.1134/S1063783417050031
- ID: 200135
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Resumo
A powder sample and single-crystal plates of the topological insulator Bi2Te3 have been investigated using the 125Te NMR method at room temperature and at low temperatures in the range from 12.5 to 16.5 K. The NMR spectra of the single-crystal plates have been studied in the orientation where the crystallographic axis c is directed parallel or perpendicular to the magnetic field. The spectra have been obtained by means of recording spin-echo signals and plotting their envelopes. It has been shown that the NMR spectra for the bismuth telluride powder and plates with the orientation c ⊥ B consist of two lines, which are presumably attributed to tellurium nuclei in two crystallographic positions in the bulk of the sample. The position and shape of the lines are determined by the chemical shift and the Knight shift. For the orientation of the plates c || B, the spectrum contains an additional component in the high-frequency region, which cannot appear due to the angular dependence of the line shifts caused by tellurium nuclei in the bulk of the topological insulator. At a low temperature, the additional line dominates in the spectrum.
Sobre autores
S. Naumov
Mikheev Institute of Metal Physics, Ural Branch
Email: charnaya@mail.ru
Rússia, ul. Sofii Kovalevskoi 18, Yekaterinburg, 620990
Yu. Perevozchikova
Mikheev Institute of Metal Physics, Ural Branch
Email: charnaya@mail.ru
Rússia, ul. Sofii Kovalevskoi 18, Yekaterinburg, 620990
V. Chistyakov
Mikheev Institute of Metal Physics, Ural Branch
Email: charnaya@mail.ru
Rússia, ul. Sofii Kovalevskoi 18, Yekaterinburg, 620990
E. Marchenkova
Mikheev Institute of Metal Physics, Ural Branch
Email: charnaya@mail.ru
Rússia, ul. Sofii Kovalevskoi 18, Yekaterinburg, 620990
H. Weber
Atominstitut—Institute of Atomic and Subatomic Physics
Email: charnaya@mail.ru
Áustria , Stadionallee 2, Vienna, 1020
J. Huang
National Cheng Kung University
Email: charnaya@mail.ru
República da China, 1 University Road, Tainan City 701
V. Marchenkov
Mikheev Institute of Metal Physics, Ural Branch; Ural Federal University
Email: charnaya@mail.ru
Rússia, ul. Sofii Kovalevskoi 18, Yekaterinburg, 620990; ul. Mira 19, Yekaterinburg, 620002
A. Antonenko
St. Petersburg State University
Email: charnaya@mail.ru
Rússia, Universitetskaya nab. 7–9, St. Petersburg, 199034
E. Charnaya
St. Petersburg State University
Autor responsável pela correspondência
Email: charnaya@mail.ru
Rússia, Universitetskaya nab. 7–9, St. Petersburg, 199034
D. Nefedov
St. Petersburg State University
Email: charnaya@mail.ru
Rússia, Universitetskaya nab. 7–9, St. Petersburg, 199034
D. Podorozhkin
St. Petersburg State University
Email: charnaya@mail.ru
Rússia, Universitetskaya nab. 7–9, St. Petersburg, 199034
A. Uskov
St. Petersburg State University
Email: charnaya@mail.ru
Rússia, Universitetskaya nab. 7–9, St. Petersburg, 199034
A. Bugaev
Moscow Institute of Physics and Technology (State University)
Email: charnaya@mail.ru
Rússia, Institutskii per. 9, Dolgoprudnyi, Moscow oblast, 141700
M. Lee
National Cheng Kung University
Email: charnaya@mail.ru
República da China, 1 University Road, Tainan City 701
L. Chang
National Cheng Kung University
Email: charnaya@mail.ru
República da China, 1 University Road, Tainan City 701
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