Engineering three-dimensional topological insulators in Rashba-type spin-orbit coupled heterostructures [electronic resource]
Topological insulators represent a new class of quantum phase defined by invariant symmetries and spin-orbit coupling that guarantees metallic Dirac excitations at its surface. The discoveries of these states have sparked the hope of realizing non-trivial excitations and novel effects such as a magn...
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Format: | Government Document Electronic eBook |
Language: | English |
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Washington, D.C. : Oak Ridge, Tenn. :
United States. Department of Energy. Office of Science ; Distributed by the Office of Scientific and Technical Information, U.S. Department of Energy,
2013.
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245 | 0 | 0 | |a Engineering three-dimensional topological insulators in Rashba-type spin-orbit coupled heterostructures |h [electronic resource] |
260 | |a Washington, D.C. : |b United States. Department of Energy. Office of Science ; |a Oak Ridge, Tenn. : |b Distributed by the Office of Scientific and Technical Information, U.S. Department of Energy, |c 2013. | ||
300 | |a Size: Article No. 1972 : |b digital, PDF file. | ||
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500 | |a Published through Scitech Connect. | ||
500 | |a 06/06/2013. | ||
500 | |a "Journal ID: ISSN 2041-1723." | ||
500 | |a "Other: PII: BFncomms2972." | ||
500 | |a Das, Tanmoy ; Balatsky, A. V. ; | ||
520 | 3 | |a Topological insulators represent a new class of quantum phase defined by invariant symmetries and spin-orbit coupling that guarantees metallic Dirac excitations at its surface. The discoveries of these states have sparked the hope of realizing non-trivial excitations and novel effects such as a magnetoelectric effect and topological Majorana excitations. Here we develop a theoretical formalism to show that a three-dimensional topological insulator can be designed artificially via stacking bilayers of two-dimensional Fermi gases with opposite Rashba-type spin-orbit coupling on adjacent layers, and with interlayer quantum tunneling. We demonstrate that in the stack of bilayers grown along a (001)-direction, a non-trivial topological phase transition occurs above a critical number of Rashba bilayers. In the topological phase, we find the formation of a single spin-polarized Dirac cone at the G-point. This approach offers an accessible way to design artificial topological insulators in a set up that takes full advantage of the atomic layer deposition approach. This design principle is tunable and also allows us to bypass limitations imposed by bulk crystal geometry. | |
536 | |b AC52-06NA25396. | ||
650 | 7 | |a 77 nanoscience and nanotechnology |2 local. | |
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650 | 7 | |a Nanoscience and nanotechnology |2 local. | |
650 | 7 | |a Science & technology - other topics |2 local. | |
710 | 2 | |a Los Alamos National Laboratory. |4 res. | |
710 | 1 | |a United States. |b Department of Energy. |b Office of Science. |4 spn. | |
710 | 1 | |a United States. |b Department of Energy. |4 spn. | |
710 | 1 | |a United States. |b Department of Energy. |b Office of Scientific and Technical Information |4 dst. | |
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