Detailed Information on Publication Record
2017
Interband absorption edge in the topological insulators Bi-2(Te1-xSex)(3)
DUBROKA, Adam, Ondřej CAHA, Miloš HRONČEK, Pavel FRIŠ, Milan ORLITA et. al.Basic information
Original name
Interband absorption edge in the topological insulators Bi-2(Te1-xSex)(3)
Authors
DUBROKA, Adam (203 Czech Republic, guarantor, belonging to the institution), Ondřej CAHA (203 Czech Republic, belonging to the institution), Miloš HRONČEK (703 Slovakia, belonging to the institution), Pavel FRIŠ (203 Czech Republic, belonging to the institution), Milan ORLITA (203 Czech Republic), Václav HOLÝ (203 Czech Republic, belonging to the institution), H. STEINER (40 Austria), Günther BAUER (40 Austria), Günter SPRINGHOLZ (40 Austria) and Josef HUMLÍČEK (203 Czech Republic, belonging to the institution)
Edition
Physical Review B, College PK, MD USA, AMER PHYSICAL SOC, 2017, 2469-9950
Other information
Language
English
Type of outcome
Článek v odborném periodiku
Field of Study
10302 Condensed matter physics
Country of publisher
United States of America
Confidentiality degree
není předmětem státního či obchodního tajemství
Impact factor
Impact factor: 3.813
RIV identification code
RIV/00216224:14310/17:00099464
Organization unit
Faculty of Science
UT WoS
000417757200005
Keywords in English
BISMUTH TELLURIDE; BI2SE3; SURFACE; BI2TE3; CRYSTALS; N-BI2SE3; SELENIDE; ALLOYS; STATES
Tags
Tags
International impact, Reviewed
Změněno: 25/2/2019 16:46, Mgr. Pavla Foltynová, Ph.D.
Abstract
V originále
We have investigated the optical properties of thin films of topological insulators Bi2Te3, Bi2Se3, and their alloys Bi-2(Te1-x Se-x)(3) on BaF2 substrates by a combination of infrared ellipsometry and reflectivity in the energy range from 0.06 to 6.5 eV. For the onset of interband absorption in Bi2Se3, after the correction for the Burstein-Moss effect, we find the value of the direct band gap of 215 +/- 10 meV at 10 K. Our data support the picture that Bi2Se3 has a direct band gap located at the Gamma point in the Brillouin zone and that the valence band reaches up to the Dirac point and has the shape of a downward-oriented paraboloid, i.e., without a camel-back structure. In Bi2Te3, the onset of strong direct interband absorption at 10 K is at a similar energy of about 200 meV, with a weaker additional feature at about 170 meV. Our data support the recent GW band-structure calculations suggesting that the direct interband transition does not occur at the Gamma point but near the Z-F line of the Brillouin zone. In the Bi-2(Te1-x Se-x)(3) alloy, the energy of the onset of direct interband transitions exhibits a maximum near x = 0.3 (i.e., the composition of Bi2Te2Se), suggesting that the crossover of the direct interband transitions between the two points in the Brillouin zone occurs close to this composition.
Links
LM2015041, research and development project |
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692034, interní kód MU |
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