Quantum spin Hall (QSH) insulators possess edge states that are topologically protected from backscattering. However, known QSH materials (e.g. HgTe/CdTe and InAs/GaSb quantum wells) exhibit very small energy gap and only work at low temperature, hindering their applications for room temperature devices. Based on the first-principles calculations, we predict a novel family of QSH insulators in monolayer tantalum carbide halide TaCX (X = Cl, Br, and I) with unique rectangular lattice and large direct energy gaps larger than 0.2 eV, accurately, 0.23−0.36 eV. The mechanism for 2D QSH effect in this system originates from a intrinsic d −d band inversion, different from conventional QSH systems with band inversion between s−p or p−p orbitals. Further, stain and intrinsic electric field can be used to tune the electronic structure and enhance the energy gap. TaCX nanoribbon, which has single-Dirac-cone edge states crossing the bulk band gap, exhibits a linear dispersion with a high Fermi velocity comparable to that of graphene. These 2D materials with considerable nontrivial gaps promise great application potential in the new generation of dissipationless electronics and spintronics.
KeywordsQuantum spin Hall insulator, Tantalum Carbide Halide, Gapless edge states, Band inversion, First-principles calculations Two-dimensional (2D) topological insulators (TIs), also known as Quantum spin Hall (QSH) insulators, characterized by an insulating bulk and fully spin-polarized gapless helical edge states without backscattering at the sample boundaries, are protected by timereversal symmetry and thus are promising for achieving dissipationless transport devices. 1,2Compared to three-dimensional (3D) TIs with the surface states only projected from exact 180 • C backscattering and suffering from other angles' scattering, the electrons with opposite