• Photonics Research
  • Vol. 12, Issue 4, 865 (2024)
Zhenghao Guo1、2、†, Mengjun Liu3、4、†, Zijia Chen1、2, Ruizhi Yang3、4, Peiyun Li1、2, Haixia Da5、6, Dong Yuan1、2, Guofu Zhou1、2, Lingling Shui3、4、7, and Huapeng Ye1、2、*
Author Affiliations
  • 1Guangdong Provincial Key Laboratory of Optical Information Materials and Technology & Institute of Electronic Paper Displays, South China Academy of Advanced Optoelectronics, South China Normal University, Guangzhou 510006, China
  • 2SCNU-TUE Joint Lab of Device Integrated Responsive Materials (DIRM), National Center for International Research on Green Optoelectronics, South China Normal University, Guangzhou 510006, China
  • 3Guangdong Provincial Key Laboratory of Nanophotonic Functional Materials and Devices, School of Information and Optoelectronic Science and Engineering, South China Normal University, Guangzhou 510006, China
  • 4Joint Laboratory of Optofluidic Technology and Systems, National Center for International Research on Green Optoelectronics, South China Academy of Advanced Optoelectronics, South China Normal University, Guangzhou 510006, China
  • 5College of Electronic and Optical Engineering & College of Microelectronics, Nanjing University of Posts and Telecommunications, Nanjing 210046, China
  • 6Key Laboratory of Radio Frequency and Micro-Nano Electronics of Jiangsu Province, Nanjing 210023, China
  • 7e-mail: shuill@m.scnu.edu.cn
  • show less
    DOI: 10.1364/PRJ.516364 Cite this Article Set citation alerts
    Zhenghao Guo, Mengjun Liu, Zijia Chen, Ruizhi Yang, Peiyun Li, Haixia Da, Dong Yuan, Guofu Zhou, Lingling Shui, Huapeng Ye. Highly efficient nonuniform finite difference method for three-dimensional electrically stimulated liquid crystal photonic devices[J]. Photonics Research, 2024, 12(4): 865 Copy Citation Text show less
    (a) Schematic diagram of electrically stimulated LC photonic device. (b), (c) Grids of patterned electrode meshing in similar number of model grids. (b) Uniform grids and (c) nonuniform grids. The scale bars in (b), (c) are 10 μm.
    Fig. 1. (a) Schematic diagram of electrically stimulated LC photonic device. (b), (c) Grids of patterned electrode meshing in similar number of model grids. (b) Uniform grids and (c) nonuniform grids. The scale bars in (b), (c) are 10 μm.
    (a) Schematic diagram of calculation relation. (b) Calculation sequence of SOR. (c), (d) Schematic diagram of (c) periodic and (d) symmetric boundary conditions. (e) Boundary conditions at different p values.
    Fig. 2. (a) Schematic diagram of calculation relation. (b) Calculation sequence of SOR. (c), (d) Schematic diagram of (c) periodic and (d) symmetric boundary conditions. (e) Boundary conditions at different p values.
    (a) Schematic illustration of the unit cell of the LC photonic device. (b)–(j) Slice diagrams of the calculated tilt angle of the directors. (b)–(d) FEM, (e)–(g) uniform FDM, and (h)–(j) nonuniform FDM. (b), (e), (h) Along x direction where x is sampled at 50, 55, 60, 65, 70, 75, 80, and 85 μm. (c), (f), (i) Along z direction where z is sampled at 30, 35, 40, 45, and 49.5 μm. (d), (g), (j) Zoomed-in image of tilt angle diagrams of the directors.
    Fig. 3. (a) Schematic illustration of the unit cell of the LC photonic device. (b)–(j) Slice diagrams of the calculated tilt angle of the directors. (b)–(d) FEM, (e)–(g) uniform FDM, and (h)–(j) nonuniform FDM. (b), (e), (h) Along x direction where x is sampled at 50, 55, 60, 65, 70, 75, 80, and 85 μm. (c), (f), (i) Along z direction where z is sampled at 30, 35, 40, 45, and 49.5 μm. (d), (g), (j) Zoomed-in image of tilt angle diagrams of the directors.
    Comparison of mesh grid distribution between nonuniform and uniform methods. (a)–(c) Grid of nonuniform method (a) in xz plane, (b) in xy plane, and (c) inside the LC layer in xz plane. (d), (e) Grid size comparison between the uniform and nonuniform methods. (d) Along x or y direction. (e) Along z direction.
    Fig. 4. Comparison of mesh grid distribution between nonuniform and uniform methods. (a)–(c) Grid of nonuniform method (a) in xz plane, (b) in xy plane, and (c) inside the LC layer in xz plane. (d), (e) Grid size comparison between the uniform and nonuniform methods. (d) Along x or y direction. (e) Along z direction.
    (a) Schematic illustration of the experimental setup to characterize the LC devices. (b), (f) Experimentally recorded light field intensity distributions at the LC layer surface of (b) array and (f) one unit. (c), (d), (e) Light field simulation results of the LC layer in the transverse plane with (c) FEM, (d) uniform FDM, and (e) nonuniform FDM. (g) Light field intensity distribution of the outermost ring of the LC layer surface in polar coordinate. (h) Simulated light field intensity distribution along the longitudinal plane. (i) Experimentally recorded light field intensity distribution along the longitudinal plane. The scale bar in (b) is 50 μm; the scale bars in (c)–(f) are 10 μm.
    Fig. 5. (a) Schematic illustration of the experimental setup to characterize the LC devices. (b), (f) Experimentally recorded light field intensity distributions at the LC layer surface of (b) array and (f) one unit. (c), (d), (e) Light field simulation results of the LC layer in the transverse plane with (c) FEM, (d) uniform FDM, and (e) nonuniform FDM. (g) Light field intensity distribution of the outermost ring of the LC layer surface in polar coordinate. (h) Simulated light field intensity distribution along the longitudinal plane. (i) Experimentally recorded light field intensity distribution along the longitudinal plane. The scale bar in (b) is 50 μm; the scale bars in (c)–(f) are 10 μm.
    MethodsMinimum Element Size (μm)Number of Domain Elements (LC Region)Computational Resources (Gb)Number of IterationsSimulation Time (min)Total Energy Fg (J)
    FEM (COMSOL)1105,84713.61153.36.22×1010
    Uniform FDM0.69×0.69×0.482,198,0163.112537.46.33×1010
    Nonuniform FDM0.29×0.29×0.32,164,0323.1155110.26.36×1010
    Uniform FDM (fine)0.3×0.3×0.3118,063,3604.2195545.16.36×1010
    Table 1. Calculation Information of Three Methods
    Zhenghao Guo, Mengjun Liu, Zijia Chen, Ruizhi Yang, Peiyun Li, Haixia Da, Dong Yuan, Guofu Zhou, Lingling Shui, Huapeng Ye. Highly efficient nonuniform finite difference method for three-dimensional electrically stimulated liquid crystal photonic devices[J]. Photonics Research, 2024, 12(4): 865
    Download Citation