Antiferromagnetic Topological Superconductor and Electrically Controllable Majorana Fermions
arXiv:1409.6147 · doi:10.1103/PhysRevLett.114.056403
Abstract
We investigate the realization of a topological superconductor in a generic bucked honeycomb system equipped with four types of mass-generating terms, where the superconductor gap is introduced by attaching the honeycomb system to an -wave superconductor. Constructing the topological phase diagram, we show that Majorana modes are formed in the phase boundary. In particular, we analyze the honeycomb system with antiferromagnetic order in the presence of perpendicular electric field . It becomes topological for and trivial for , with a certain critical field. It is possible to create a topological spot in a trivial superconductor by controlling applied electric field. One Majorana zero-energy bound state appears at the phase boundary. We can arbitrarily control the position of the Majorana fermion by moving the spot of applied electric field, which will be made possible by a scanning tunneling microscope probe.
5 pages, 3 figures
References in corpus (9)
- Non-Abelian Anyons and Topological Quantum Computation
- Superconducting proximity effect and Majorana fermions at the surface of a topological insulator
- Classification of topological insulators and superconductors in three spatial dimensions
- Valley-Polarized Metals and Quantum Anomalous Hall Effect in Silicene
- Introduction to topological superconductivity and Majorana fermions
- Photo-Induced Topological Phase Transition and a Single Dirac-Cone State in Silicene
- Coupling the valley degree of freedom to antiferromagnetic order
- Spin-Valleytronics in Silicene: Quantum-Spin-Quantum-Anomalous Hall Insulators and Single-Valley Semimetals
- Topological Phase Transition and Electrically Tunable Diamagnetism in Silicene