Induced robust topological order on an ordinary insulator hetero-structured with a strong topological insulator
arXiv:1611.04688
Abstract
Topological states of matter originate from distinct topological electronic structures of materials. As for strong topological insulators (STIs), the topological surface (interface) is a direct consequence of electronic structure transition between materials categorized to different topological genus. Therefore, it is fundamentally interesting if such topological character can be manipulated. Besides tuning the crystal field and the strength of spin-orbital coupling (e.g., by external strain, or chemical doping), there is currently rare report on topological state induced in ordinary insulators (OIs) by the heterostructure of OI/STI. Here we report the observation of a Dirac cone topological surface state (TSS) induced on the Sb2Se3 layer up to 15 nm thick in the OI/STI heterostructure, in sharp contrast with the OI/OI heterostructure where no sign of TSS can be observed. This is evident for an induced topological state in an OI by heterostructure.
References in corpus (11)
- Topological Insulators
- Quantum Spin Hall Effect in Graphene
- Superconducting proximity effect and Majorana fermions at the surface of a topological insulator
- Experimental Observation of the Quantum Anomalous Hall Effect in a Magnetic Topological Insulator
- Discovery (theoretical prediction and experimental observation) of a large-gap topological-insulator class with spin-polarized single-Dirac-cone on the surface
- Quantum Spin Hall Effect
- Topological Phase Transition and Texture Inversion in a Tunable Topological Insulator
- Theoretical investigation of the evolution of the topological phase of BiSe under mechanical strain
- Sharp Raman Anomalies and Broken Adiabaticity at a Pressure Induced Transition from Band to Topological Insulator in Sb2Se3
- Pressure induced topological quantum phase transition in Sb_2Se_3
- The rhombohedral Sb2Se3 is also an intrinsic topological insulator