Large magnetic gap at the Dirac point in Bi2Te3/MnBi2Te4 heterostructures

E. D. L. Rienks, S. Wimmer, J. Sánchez-Barriga, O. Caha, P. S. Mandal, J. Růžička, A. Ney, H. Steiner, V. V. Volobuev, H. Groiss, M. Albu, G. Kothleitner, J. Michalička, S. A. Khan, J. Minár, H. Ebert, G. Bauer, F. Freyse, A. Varykhalov, O. Rader () and G. Springholz ()
Additional contact information
E. D. L. Rienks: Elektronenspeicherring BESSY II
S. Wimmer: Institut für Halbleiter- und Festkörperphysik, Johannes Kepler Universität
J. Sánchez-Barriga: Elektronenspeicherring BESSY II
O. Caha: Masaryk University
P. S. Mandal: Elektronenspeicherring BESSY II
J. Růžička: Masaryk University
A. Ney: Institut für Halbleiter- und Festkörperphysik, Johannes Kepler Universität
H. Steiner: Institut für Halbleiter- und Festkörperphysik, Johannes Kepler Universität
V. V. Volobuev: Institut für Halbleiter- und Festkörperphysik, Johannes Kepler Universität
H. Groiss: Zentrum für Oberflächen- und Nanoanalytik, Johannes Kepler Universität
M. Albu: Graz University of Technology
G. Kothleitner: Graz University of Technology
J. Michalička: Brno University of Technology
S. A. Khan: University of West Bohemia
J. Minár: University of West Bohemia
H. Ebert: Ludwig-Maximilians-Universität
G. Bauer: Institut für Halbleiter- und Festkörperphysik, Johannes Kepler Universität
F. Freyse: Elektronenspeicherring BESSY II
A. Varykhalov: Elektronenspeicherring BESSY II
O. Rader: Elektronenspeicherring BESSY II
G. Springholz: Institut für Halbleiter- und Festkörperphysik, Johannes Kepler Universität

Nature, 2019, vol. 576, issue 7787, 423-428

Abstract: Abstract Magnetically doped topological insulators enable the quantum anomalous Hall effect (QAHE), which provides quantized edge states for lossless charge-transport applications1–8. The edge states are hosted by a magnetic energy gap at the Dirac point2, but hitherto all attempts to observe this gap directly have been unsuccessful. Observing the gap is considered to be essential to overcoming the limitations of the QAHE, which so far occurs only at temperatures that are one to two orders of magnitude below the ferromagnetic Curie temperature, TC (ref. 8). Here we use low-temperature photoelectron spectroscopy to unambiguously reveal the magnetic gap of Mn-doped Bi2Te3, which displays ferromagnetic out-of-plane spin texture and opens up only below TC. Surprisingly, our analysis reveals large gap sizes at 1 kelvin of up to 90 millielectronvolts, which is five times larger than theoretically predicted9. Using multiscale analysis we show that this enhancement is due to a remarkable structure modification induced by Mn doping: instead of a disordered impurity system, a self-organized alternating sequence of MnBi2Te4 septuple and Bi2Te3 quintuple layers is formed. This enhances the wavefunction overlap and size of the magnetic gap10. Mn-doped Bi2Se3 (ref. 11) and Mn-doped Sb2Te3 form similar heterostructures, but for Bi2Se3 only a nonmagnetic gap is formed and the magnetization is in the surface plane. This is explained by the smaller spin–orbit interaction by comparison with Mn-doped Bi2Te3. Our findings provide insights that will be crucial in pushing lossless transport in topological insulators towards room-temperature applications.

Date: 2019
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DOI: 10.1038/s41586-019-1826-7

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