It appears you don't have support to open PDFs in this web browser. To view this file, Open with your PDF reader
Abstract
Topological surface-states can acquire an energy gap when time-reversal symmetry is broken by interfacing with a magnetic insulator. This gap has yet to be measured. Such topological-magnetic insulator heterostructures can host a quantized anomalous Hall effect and can allow the control of the magnetic state of the insulator in a spintronic device. In this work, we observe the energy gap of topological surface-states in proximity to a magnetic insulator using magnetooptical Landau level spectroscopy. We measure Pb1-xSnxSe–EuSe heterostructures grown by molecular beam epitaxy exhibiting a record mobility and low Fermi energy. Through temperature dependent measurements and theoretical calculations, we show this gap is likely due to quantum confinement and conclude that the magnetic proximity effect is weak in this system. This weakness is disadvantageous for the realization of the quantum anomalous Hall effect, but favorable for spintronic devices which require the preservation of spin-momentum locking at the Fermi level.
The proximity coupling of topological insulators with magnetic materials can give rise to exotic phenomenon such as the quantum anomalous Hall effect. Here, the authors use magneto-optical Landau level spectroscopy to investigate Pb1-xSnxSe-EuSe heterostructures finding evidence of a quantum confinement induced energy gaps in the topological surface states, that overshadow the magnetic proximity effects.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer
Details






1 University of Notre Dame, Department of Physics and Astronomy, Notre Dame, USA (GRID:grid.131063.6) (ISNI:0000 0001 2168 0066)
2 Florida State University, National High Magnetic Fields Laboratory, Tallahassee, USA (GRID:grid.255986.5) (ISNI:0000 0004 0472 0419)
3 Argonne National Lab, X-ray Science Division, Advanced Photon Source, Lemont, USA (GRID:grid.187073.a) (ISNI:0000 0001 1939 4845)
4 Université PSL, CNRS, Sorbonne Université, Laboratoire de Physique de l’Ecole normale supérieure, ENS, Paris, France (GRID:grid.462608.e) (ISNI:0000 0004 0384 7821)
5 University of Notre Dame, Notre Dame Integrated Imaging Facility, Notre Dame, USA (GRID:grid.131063.6) (ISNI:0000 0001 2168 0066)
6 Oak Ridge National Laboratory, Neutron Scattering Division, Neutron Sciences Directorate, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659)
7 Oak Ridge National Laboratory, Neutron Scattering Division, Neutron Sciences Directorate, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659); Oak Ridge National Laboratory, Center for Nanophase Materials Sciences, Physical Science Directorate, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659)