2010
DOI: 10.1103/physrevb.81.125120
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Optical characterization ofBi2Se3in a magnetic field: Infrared evidence for magnetoelectric coupling in a topological insulator material

Abstract: We present an infrared magneto-optical study of the highly thermoelectric narrow-gap semiconductor Bi2Se3. Far-infrared and mid-infrared (IR) reflectance and transmission measurements have been performed in magnetic fields oriented both parallel and perpendicular to the trigonal c axis of this layered material, and supplemented with UV-visible ellipsometry to obtain the optical conductivity σ1(ω). With lowering of temperature we observe narrowing of the Drude conductivity due to reduced quasiparticle scatterin… Show more

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Cited by 243 publications
(244 citation statements)
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“…These modes transform as 2 + 2 1 + 2 + 2 1 , where 2 + 2 1 and 2 + 2 1 are, respectively, Raman and infrared-active representations [19]. We note that the bulk optical phonons of Bi2Se3 and Bi2Te3 have been previously measured using Raman [20,26,27,28] and neutron scattering [29], and infrared spectroscopy [19,20,30], Figure 1 shows Raman spectra of Bi2Se3 and Bi2Te3 at various temperatures in the ( ) ̅ ( + ) scattering configuration; note the logarithmic scale. Consistent with previous reports [20,27], the bulk Raman-active modes at 10 K are at 38.5 cm -1 ( 1 ), 75.5 cm -1 ( 1 1 ), 135.8 cm -1…”
Section: Resultsmentioning
confidence: 99%
“…These modes transform as 2 + 2 1 + 2 + 2 1 , where 2 + 2 1 and 2 + 2 1 are, respectively, Raman and infrared-active representations [19]. We note that the bulk optical phonons of Bi2Se3 and Bi2Te3 have been previously measured using Raman [20,26,27,28] and neutron scattering [29], and infrared spectroscopy [19,20,30], Figure 1 shows Raman spectra of Bi2Se3 and Bi2Te3 at various temperatures in the ( ) ̅ ( + ) scattering configuration; note the logarithmic scale. Consistent with previous reports [20,27], the bulk Raman-active modes at 10 K are at 38.5 cm -1 ( 1 ), 75.5 cm -1 ( 1 1 ), 135.8 cm -1…”
Section: Resultsmentioning
confidence: 99%
“…Bi 2 Se 3 electronic dielectric function at ambient pressure has been shown to be mainly determined [36,37] by a very intense optical transition at 2 eV, that would correspond to its Penn gap [38], according to the Phillips-van Vechten model [39][40][41] to the square of the plasma frequency. In Figure 6-b we plot (E g ) 3/2 versus (ħ PFC ) 2 .…”
Section: A Ftir Absorption and Reflection Resultsmentioning
confidence: 99%
“…Concerning the increase of the electronic dielectric constant, let's first try to identify the electronic transitions corresponding to the Penn gap (dielectric function peak at 2 eV) [36,37]. For optical transitions between the valence and conduction band, the only area of the band structure that could give rise to a high joint density of states at 2 eV seems to be around the -L direction.…”
Section: B Electronic Structure Under High Pressurementioning
confidence: 99%
“…54 58 and experiments have begun to investigate the transition between the three-and two-dimensional phases in this material. 59 Bi 2 Se 3 has also been studied in a magnetic field, revealing a magnetoelectric coupling 60 and an oscillatory angular dependence of the magnetoresistance. 61 Sample growth dynamics of Bi 2 Te 3 by means of MBE were monitored by reflection high-energy electron diffraction (RHEED).…”
Section: Introductionmentioning
confidence: 99%