Quantum spin Hall phase in 2D trigonal lattice

Wang, Z. F.; Jin, Kyung -Hwan; Liu, Feng

doi:10.1038/ncomms12746

Title: Quantum spin Hall phase in 2D trigonal lattice

Journal Article · Wed Sep 07 00:00:00 EDT 2016 · Nature Communications

DOI:https://doi.org/10.1038/ncomms12746· OSTI ID:1361410

Wang, Z. F. ^[1]; Jin, Kyung -Hwan ^[2]; Liu, Feng ^[3]

Univ. of Science and Technology of China, Anhui (China); Univ. of Utah, Salt Lake City, UT (United States)
Univ. of Utah, Salt Lake City, UT (United States)
Univ. of Utah, Salt Lake City, UT (United States); Collaborative Innovation Center of Quantum Matter, Beijing (China)

The quantum spin Hall (QSH) phase is an exotic phenomena in condensed-matter physics. Here we show that a minimal basis of three orbitals (s, p_x, p_y) is required to produce a QSH phase via nearest-neighbour hopping in a two-dimensional trigonal lattice. Tight-binding model analyses and calculations show that the QSH phase arises from a spin–orbit coupling (SOC)-induced s–p band inversion or p–p bandgap opening at Brillouin zone centre (Γ point), whose topological phase diagram is mapped out in the parameter space of orbital energy and SOC. Remarkably, based on first-principles calculations, this exact model of QSH phase is shown to be realizable in an experimental system of Au/GaAs(111) surface with an SOC gap of ~73 meV, facilitating the possible room-temperature measurement. Finally, our results will extend the search for substrate supported QSH materials to new lattice and orbital types.

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Research Organization:: Univ. of Utah, Salt Lake City, UT (United States)

Sponsoring Organization:: USDOE

Grant/Contract Number:: FG02-04ER46148

OSTI ID:: 1361410

Journal Information:: Nature Communications, Vol. 7; ISSN 2041-1723

Publisher:: Nature Publishing GroupCopyright Statement

Country of Publication:: United States

Language:: English

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Cited by: 34 works

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