MANDAL, P. S., G. SPRINGHOLZ, V. V. VOLOBUEV, Ondřej CAHA, A. VARYKHALOV, E. GOLIAS, G. BAUER, O. RADER and J. SANCHEZ-BARRIGA. Topological quantum phase transition from mirror to time reversal symmetry protected topological insulator. Nature Communications. London: Nature Publishing Group, 2017, vol. 8, October, p. "968-1"-"968-7", 7 pp. ISSN 2041-1723. Available from: https://dx.doi.org/10.1038/s41467-017-01204-0.
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Basic information
Original name Topological quantum phase transition from mirror to time reversal symmetry protected topological insulator
Authors MANDAL, P. S. (356 India), G. SPRINGHOLZ (40 Austria), V. V. VOLOBUEV (804 Ukraine), Ondřej CAHA (203 Czech Republic, guarantor, belonging to the institution), A. VARYKHALOV (643 Russian Federation), E. GOLIAS (300 Greece), G. BAUER (40 Austria), O. RADER (276 Germany) and J. SANCHEZ-BARRIGA (724 Spain).
Edition Nature Communications, London, Nature Publishing Group, 2017, 2041-1723.
Other information
Original language English
Type of outcome Article in a journal
Field of Study 10302 Condensed matter physics
Country of publisher United Kingdom of Great Britain and Northern Ireland
Confidentiality degree is not subject to a state or trade secret
Impact factor Impact factor: 12.353
RIV identification code RIV/00216224:14310/17:00099461
Organization unit Faculty of Science
Doi http://dx.doi.org/10.1038/s41467-017-01204-0
UT WoS 000413117400002
Keywords in English IV-VI COMPOUNDS; CRYSTALLINE INSULATOR; CARRIER DENSITY; SNTE; PB1-XSNXSE; INVERSION; GETE; GAP
Tags NZ, rivok
Tags International impact, Reviewed
Changed by Changed by: Ing. Nicole Zrilić, učo 240776. Changed: 12/4/2018 15:45.
Abstract
Topological insulators constitute a new phase of matter protected by symmetries. Time-reversal symmetry protects strong topological insulators of the Z(2) class, which possess an odd number of metallic surface states with dispersion of a Dirac cone. Topological crystalline insulators are merely protected by individual crystal symmetries and exist for an even number of Dirac cones. Here, we demonstrate that Bi-doping of Pb1-xSnxSe (111) epilayers induces a quantum phase transition from a topological crystalline insulator to a Z(2) topological insulator. This occurs because Bi-doping lifts the fourfold valley degeneracy and induces a gap at (Gamma) over bar, while the three Dirac cones at the (M) over bar points of the surface Brillouin zone remain intact. We interpret this new phase transition as caused by a lattice distortion. Our findings extend the topological phase diagram enormously and make strong topological insulators switchable by distortions or electric fields.
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