ﻻ يوجد ملخص باللغة العربية
Two-dimensional quantum spin Hall (QSH) insulators are a promising material class for spintronic applications based on dissipationless topologically-protected spin currents in their edges. Yet, they have not lived up to their technological potential, as experimental realizations are scarce and limited to cryogenic temperatures. These constraints have also severely restricted the characterization of their dynamical properties, imperative for the design of QSH devices operating under nonequilibrium conditions. Here, we report on the electron dynamics of the novel room-temperature QSH candidate bismuthene after photoexcitation using time- and angle-resolved photoemission spectroscopy. We map the transiently occupied conduction band and observe a metallic dispersive feature within the bulk band gap - a signature of topological edge states. Our analysis of hot photocarrier lifetimes provides insight into the microscopic scattering processes and the key role of edge states. The demonstration of the large bulk band gap and stability of edge states at room temperature marks a critical step towards QSH applications.
We use the bulk Hamiltonian for a three-dimensional topological insulator such as $rm Bi_2 Se_3$ to study the states which appear on its various surfaces and along the edge between two surfaces. We use both analytical methods based on the surface Ham
We have performed angle-resolved photoemission spectroscopy on (PbSe)5(Bi2Se3)3m, which forms a natural multilayer heterostructure consisting of a topological insulator (TI) and an ordinary insulator. For m = 2, we observed a gapped Dirac-cone state
We present a microscopic theory of the chiral one-dimensional electron gas system localized on the sidewalls of magnetically-doped Bi$_2$Se$_3$-family topological insulator nanoribbons in the quantum anomalous Hall effect (QAHE) regime. Our theory is
Helical edge states of two-dimensional topological insulators show a gap in the Density of States (DOS) and suppressed conductance in the presence of ordered magnetic impurities. Here we will consider the dynamical effects on the DOS and transmission
The non-trivial topology of the three-dimensional (3D) topological insulator (TI) dictates the appearance of gapless Dirac surface states. Intriguingly, when a 3D TI is made into a nanowire, a gap opens at the Dirac point due to the quantum confineme