Liang G Q, Chong Y D
Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, 637371 Singapore.
Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, 637371 Singapore and Centre for Disruptive Photonic Technologies, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, 637371 Singapore.
Phys Rev Lett. 2013 May 17;110(20):203904. doi: 10.1103/PhysRevLett.110.203904. Epub 2013 May 14.
A lattice of optical ring resonators can exhibit a topological insulator phase, with the role of spin played by the direction of propagation of light within each ring. Unlike the system studied by Hafezi et al., [Nat. Phys. 7, 907 (2011).] topological protection is achieved without fine-tuning the interresonator couplings, which are given the same periodicity as the underlying lattice. The topological insulator phase occurs for strong couplings, when the tight-binding method is inapplicable. Using the transfer matrix method, we derive the band structure and phase diagram, and demonstrate the existence of robust edge states. When gain and loss are introduced, the system functions as a diode for coupled resonator modes.
光学环形谐振器晶格可以呈现拓扑绝缘体相,其中每个环内光的传播方向扮演了自旋的角色。与哈菲齐等人研究的系统[《自然·物理》7, 907 (2011年)]不同,这里无需微调谐振器间的耦合就能实现拓扑保护,这些耦合具有与基础晶格相同的周期性。当紧束缚方法不适用时,强耦合情况下会出现拓扑绝缘体相。我们使用转移矩阵方法推导了能带结构和相图,并证明了稳健边缘态的存在。当引入增益和损耗时,该系统可作为耦合谐振器模式的二极管。