Resonance Raman Scattering of Topological Insulators Bi<sub>2</sub>Te<sub>3</sub> and Bi<sub>2 − x</sub>Sb<sub>x</sub>Te<sub>3 − y</sub>Se<sub>y</sub> Thin Films

Abstract Phonon occupation is temperature ( T ) dependent; it may participate in scattering with electronic states of topological insulators (TIs). Longitudinal optical (LO) phonons and in Bi 2 − x Sb x Te 3 − y Se y (BSTS) was resonantly excited by a photon energy (E p ) 2.33 eV due to electronic transition of unoccupied conduction band. The intensity of these modes was enhanced in Bi 2 Te 3 film at E p 1.87 eV, which is close to the electronic transition of unoccupied Dirac states. Fröhlich coupling strength was the main mechanism for higher intensity of and modes. At 300 K, the intensity of the mode was significantly decayed in both the BSTS and Bi 2 Te 3 at E p 2.33 and 1.87 eV due to the anharmonic coupling. However, at similar value of T , spectral profile of and modes was not affected because of the lower probability of decay rate of these phonons. In resonant condition, well‐resolved Raman forbidden surface modes were observed at T of 50 K. At 300 K, more asymmetric Fano profile of surface phonon was observed due to the anharmonic coupling. The study indicated that at high T , mode and anharmonic coupling may become primary cause for scattering with electronic states of the TIs. However, at low T , primarily, both the LO phonons participated in the scattering.

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Publication Details

Journal
Journal of Raman Spectroscopy
Published
2024-11-26
DOI
https://doi.org/10.1002/jrs.6751
Citations
1
Primary Topic
Topological Materials and Phenomena
Type
article
Field-Weighted Citation Impact
0.34

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article

Resonance Raman Scattering of Topological Insulators Bi2Te3 and Bi2 − xSbxTe3 − ySey Thin Films

Н. В. Суровцев, P. A. Yunin, A. G. Milekhin, Oleg Evgenievich Tereshchenko et al.
1 citations
Journal of Raman Spectroscopy
Topological Materials and Phenomena
0.34
article

Resonance Raman Scattering of Topological Insulators Bi2Te3 and Bi2 − xSbxTe3 − ySey Thin Films

Н. В. Суровцев, P. A. Yunin, A. G. Milekhin, Oleg Evgenievich Tereshchenko, Ilya Milekhin, Д. В. Ищенко, N. Kumar
article en
1 citations

Abstract

Abstract Phonon occupation is temperature ( T ) dependent; it may participate in scattering with electronic states of topological insulators (TIs). Longitudinal optical (LO) phonons and in Bi 2 − x Sb x Te 3 − y Se y (BSTS) was resonantly excited by a photon energy (E p ) 2.33 eV due to electronic transition of unoccupied conduction band. The intensity of these modes was enhanced in Bi 2 Te 3 film at E p 1.87 eV, which is close to the electronic transition of unoccupied Dirac states. Fröhlich coupling strength was the main mechanism for higher intensity of and modes. At 300 K, the intensity of the mode was significantly decayed in both the BSTS and Bi 2 Te 3 at E p 2.33 and 1.87 eV due to the anharmonic coupling. However, at similar value of T , spectral profile of and modes was not affected because of the lower probability of decay rate of these phonons. In resonant condition, well‐resolved Raman forbidden surface modes were observed at T of 50 K. At 300 K, more asymmetric Fano profile of surface phonon was observed due to the anharmonic coupling. The study indicated that at high T , mode and anharmonic coupling may become primary cause for scattering with electronic states of the TIs. However, at low T , primarily, both the LO phonons participated in the scattering.

Journal of Raman SpectroscopyVol. 56(3)
Novosibirsk State University (RU), National Research Tomsk State University (RU), Boreskov Institute of Catalysis (RU), Siberian Branch of the Russian Academy of Sciences (RU), Institute of Semiconductor Physics (RU), Institute for Physics of Microstructures (RU), Institute of Automation and Electrometry (RU), N. I. Lobachevsky State University of Nizhny Novgorod (RU)
Russian Science Foundation, Ministry of Science and Higher Education of the Russian Federation
Affordable and clean energy
Openalex Percentile: Top 38%
Topological Materials and Phenomena
0.34
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