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| Hauptseite > Publikationsdatenbank > Two-Dimensional Topological Crystalline Insulator and Topological Phase Transition in TlSe and TlS Monolayers > print |
| Hauptseite > Publikationsdatenbank > Two-Dimensional Topological Crystalline Insulator and Topological Phase Transition in TlSe and TlS Monolayers > print |
| 001 | 276427 | ||
| 005 | 20210129220859.0 | ||
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| 100 | 1 | _ | |a Niu, Chengwang |0 P:(DE-Juel1)159381 |b 0 |e Corresponding author |u fzj |
| 245 | _ | _ | |a Two-Dimensional Topological Crystalline Insulator and Topological Phase Transition in TlSe and TlS Monolayers |
| 260 | _ | _ | |a Washington, DC |c 2015 |b ACS Publ. |
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| 520 | _ | _ | |a The properties that distinguish topological crystalline insulator (TCI) and topological insulator (TI) rely on crystalline symmetry and time-reversal symmetry, respectively, which encodes different bulk and surface/edge properties. Here, we predict theoretically that electron-doped TlM (M = S and Se) (110) monolayers realize a family of two-dimensional (2D) TCIs characterized by mirror Chern number CM = −2. Remarkably, under uniaxial strain (≈ 1%), a topological phase transition between 2D TCI and 2D TI is revealed with the calculated spin Chern number CS = −1 for the 2D TI. Using spin-resolved edge states analysis, we show different edge-state behaviors, especially at the time reversal invariant points. Finally, a TlBiSe2/NaCl quantum well is proposed to realize an undoped 2D TCI with inverted gap as large as 0.37 eV, indicating the high possibility for room-temperature observation. |
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