• Acta Physica Sinica
  • Vol. 68, Issue 22, 224206-1 (2019)
Hong-Fei Wang1, Bi-Ye Xie1, Peng Zhan1、2、3, Ming-Hui Lu1、3、4、*, and Yan-Feng Chen1、3
Author Affiliations
  • 1National Laboratory of Solid State Microstructures, Department of Materials Science and Engineering, Nanjing University, Nanjing 210093, China
  • 2School of Physics, Nanjing University, Nanjing 210093, China
  • 3Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
  • 4Jiangsu Key Laboratory of Artificial Functional Materials, Nanjing 210093, China
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    DOI: 10.7498/aps.68.20191437 Cite this Article
    Hong-Fei Wang, Bi-Ye Xie, Peng Zhan, Ming-Hui Lu, Yan-Feng Chen. Research progress of topological photonics[J]. Acta Physica Sinica, 2019, 68(22): 224206-1 Copy Citation Text show less
    Schematic of the SSH model, there are two sites in each unit cell.SSH模型示意图, 每个元胞包含两个格点
    Fig. 1. Schematic of the SSH model, there are two sites in each unit cell.SSH模型示意图, 每个元胞包含两个格点
    (a) SEM image of the coupled micropillars; (b) Modes of single micropillars; (c) Different modes of the micropillar array and edge states; (d) SSH microring array.(a) 微纳加工(SSH 模型)的SEM图; (b) 单个柱子的模式; (c) 不同能带中的态及存在的边界态; (d) 利用波导环形阵列实现SSH模型
    Fig. 2. (a) SEM image of the coupled micropillars; (b) Modes of single micropillars; (c) Different modes of the micropillar array and edge states; (d) SSH microring array.(a) 微纳加工(SSH 模型)的SEM图; (b) 单个柱子的模式; (c) 不同能带中的态及存在的边界态; (d) 利用波导环形阵列实现SSH模型
    (a) Schematic of the gyromagnetic photonic crystal; (b) forward and backward spectra, and projected band structures with chiral edge states; (c) the diagram of large Chern number photonic crystals; (d) the band gap map and their Chern number.(a) 旋磁光子晶体的示意图; (b) 向前向后的传输谱以及具有手性边界态的投影能带; (c) 大陈数光子晶体结构图; (d) 能带的带隙及其陈数
    Fig. 3. (a) Schematic of the gyromagnetic photonic crystal; (b) forward and backward spectra, and projected band structures with chiral edge states; (c) the diagram of large Chern number photonic crystals; (d) the band gap map and their Chern number.(a) 旋磁光子晶体的示意图; (b) 向前向后的传输谱以及具有手性边界态的投影能带; (c) 大陈数光子晶体结构图; (d) 能带的带隙及其陈数
    (a) The polarization of LCP and RCP on the Poincaré sphere, and the photonic crystal consisting of PE and PM superlattices; (b) band structures without coupling between dseudospin states and with their coupling, and the projected band structures for the latter case; (c) photonic crystals consisting of metallic rods and collars at different positions, and their band strucutres.(a) Poincaré球上的LCP和RCP, 以及由PE和PM材料构成的光子晶体; (b) 没有赝自旋耦合以及具有赝自旋耦合的能带以及后者的投影能带; (c) 通过调节金属柱子实现赝自旋的耦合
    Fig. 4. (a) The polarization of LCP and RCP on the Poincaré sphere, and the photonic crystal consisting of PE and PM superlattices; (b) band structures without coupling between dseudospin states and with their coupling, and the projected band structures for the latter case; (c) photonic crystals consisting of metallic rods and collars at different positions, and their band strucutres.(a) Poincaré球上的LCP和RCP, 以及由PE和PM材料构成的光子晶体; (b) 没有赝自旋耦合以及具有赝自旋耦合的能带以及后者的投影能带; (c) 通过调节金属柱子实现赝自旋的耦合
    (a) Schematic of all-dielectric photonic crystals; (b) band structures of shrinking and expanding lattices; (c) visualization of pseudospin-dependent edge states.(a) 全介质光子晶体结构; (b) 收缩、高对称以及扩张晶格所对应的能带; (c) 赝自旋依赖的边界态的实验观测
    Fig. 5. (a) Schematic of all-dielectric photonic crystals; (b) band structures of shrinking and expanding lattices; (c) visualization of pseudospin-dependent edge states.(a) 全介质光子晶体结构; (b) 收缩、高对称以及扩张晶格所对应的能带; (c) 赝自旋依赖的边界态的实验观测
    (a) Two coupled resonators in one unit cell; (b) a periodic array arranged by unit cells.(a) 谐振腔耦合单元; (b) 周期排布形成的耦合阵列
    Fig. 6. (a) Two coupled resonators in one unit cell; (b) a periodic array arranged by unit cells.(a) 谐振腔耦合单元; (b) 周期排布形成的耦合阵列
    (a) The resonator lattice with dynamic modulation; (b) floquet topological insulators using the femtosecond laser writing method; (c) four different bonds with different coupling.(a) 光学谐振腔阵列的动态调制; (b) 激光直写波导系统的拓扑绝缘体构型; (c) 四种耦合组成的周期构型
    Fig. 7. (a) The resonator lattice with dynamic modulation; (b) floquet topological insulators using the femtosecond laser writing method; (c) four different bonds with different coupling.(a) 光学谐振腔阵列的动态调制; (b) 激光直写波导系统的拓扑绝缘体构型; (c) 四种耦合组成的周期构型
    (a) Photonic crystals with two gyroid structures in one unit cell, and their band structures with Weyl points or nodal-line; (b) schematic of photonic crystals with the saddle-shaped metallic inclusion, and their Weyl points.(a) 能够产生Weyl点以及节线的双螺旋光子晶体; (b) 具有Weyl点的金属夹杂的光子晶体
    Fig. 8. (a) Photonic crystals with two gyroid structures in one unit cell, and their band structures with Weyl points or nodal-line; (b) schematic of photonic crystals with the saddle-shaped metallic inclusion, and their Weyl points.(a) 能够产生Weyl点以及节线的双螺旋光子晶体; (b) 具有Weyl点的金属夹杂的光子晶体
    (a) 3 D all-dielectric and bianisotropic metacrystals; (b) band structures corresponding to two structures in (a); (c) photonic crystals with opened Dirac points when magnetization is applied on rods.(a) 三维全介质与双各向异性光子晶体; (b) 两种构型的光子晶体对应的能带; (c) 通过引入磁场破缺Dirac点的光子晶体构型
    Fig. 9. (a) 3 D all-dielectric and bianisotropic metacrystals; (b) band structures corresponding to two structures in (a); (c) photonic crystals with opened Dirac points when magnetization is applied on rods.(a) 三维全介质与双各向异性光子晶体; (b) 两种构型的光子晶体对应的能带; (c) 通过引入磁场破缺Dirac点的光子晶体构型
    (a) Exceptional points in momentum space, and the tight-binding model with gain and loss for αi and βi; (b) the waveguide array with gain and loss; (c) photonic crystal slabs with the ring of exceptional points.(a) 动量空间中的奇异点以及具有增益损耗的紧束缚模型; (b) 具有增益损耗的波导阵列; (c) 具有奇异环的光子晶体板结构
    Fig. 10. (a) Exceptional points in momentum space, and the tight-binding model with gain and loss for αi and βi; (b) the waveguide array with gain and loss; (c) photonic crystal slabs with the ring of exceptional points. (a) 动量空间中的奇异点以及具有增益损耗的紧束缚模型; (b) 具有增益损耗的波导阵列; (c) 具有奇异环的光子晶体板结构
    (a) The nonlinear SSH model; (b) the winding number (Berry phase) changed by intensity; (c) schematic diagram of qubits and their couplers in 2 D lattice; (d) the superconducting circuit including three qubits.(a) 非线性SSH模型; (b) 与光强度相关的环绕数(贝利相位); (c) 将量子比特与它们的耦合器铺成二维格子的示意图; (d) 包含三个超导量子比特的超导回路
    Fig. 11. (a) The nonlinear SSH model; (b) the winding number (Berry phase) changed by intensity; (c) schematic diagram of qubits and their couplers in 2 D lattice; (d) the superconducting circuit including three qubits.(a) 非线性SSH模型; (b) 与光强度相关的环绕数(贝利相位); (c) 将量子比特与它们的耦合器铺成二维格子的示意图; (d) 包含三个超导量子比特的超导回路
    (a) Photonic crystals of the 2D SSH model consisting of dielectric pillars; (b) band structures of shrinking, high symmetry and expending structures; (c) shrinking supercells contain expanding supercells, and the relationship between solution numbers and eigenfrequencies; (d) experimentally measured corner states when the source is placed at the corner.(a) 介质柱构成的二维SSH模型的光子晶体; (b) 收缩、高对称与扩张晶格构型的能带结构; (c) 由收缩区域包围扩张区域构成的整体结构, 解的序号与本征频率的关系; (d) 实验中放于一个角的源激发的拐角态
    Fig. 12. (a) Photonic crystals of the 2D SSH model consisting of dielectric pillars; (b) band structures of shrinking, high symmetry and expending structures; (c) shrinking supercells contain expanding supercells, and the relationship between solution numbers and eigenfrequencies; (d) experimentally measured corner states when the source is placed at the corner.(a) 介质柱构成的二维SSH模型的光子晶体; (b) 收缩、高对称与扩张晶格构型的能带结构; (c) 由收缩区域包围扩张区域构成的整体结构, 解的序号与本征频率的关系; (d) 实验中放于一个角的源激发的拐角态
    Hong-Fei Wang, Bi-Ye Xie, Peng Zhan, Ming-Hui Lu, Yan-Feng Chen. Research progress of topological photonics[J]. Acta Physica Sinica, 2019, 68(22): 224206-1
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