• Chinese Optics Letters
  • Vol. 18, Issue 8, 080002 (2020)
Qi Guo1、2、*, Tian Liu1、2, Xiaoqian Wang3、**, Zhigang Zheng3, Aleksey Kudreyko4, Huijie Zhao1、2, V. Chigrinov5、6、7, and Hoi-Sing Kwok6
Author Affiliations
  • 1School of Instrumentation and Optoelectronic Engineering, Beihang University, Beijing 100191, China
  • 2Beihang University Qingdao Research Institute, Qingdao 266101, China
  • 3Physics Department, East China University of Science and Technology, Shanghai 200237, China
  • 4Department of Medical Physics and Informatics, Bashkir State Medical University, Ufa 450008, Russia
  • 5School of Physics and Optoelectronic Engineering, Foshan University, Foshan 528000, China
  • 6State Key Laboratory on Advanced Displays and Optoelectronics Technologies, The Hong Kong University of Science and Technology, Hong Kong 999077, China
  • 7Department of Theoretical Physics, Moscow Region State University, Mytishi 141014, Russia
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    DOI: 10.3788/COL202018.080002 Cite this Article Set citation alerts
    Qi Guo, Tian Liu, Xiaoqian Wang, Zhigang Zheng, Aleksey Kudreyko, Huijie Zhao, V. Chigrinov, Hoi-Sing Kwok. Ferroelectric liquid crystals for fast switchable circular Dammann grating [Invited][J]. Chinese Optics Letters, 2020, 18(8): 080002 Copy Citation Text show less
    Schematic representation of the two-step exposure technique for the patterned alignment layer of the FLC CDG. (a) The exposure of polarized UV on the SD1 substrate; (b) the exposure of the SD1 substrate with the mask; (c) the FLC CDG cell with a single-side alignment; (d) the chemical formula of the SD1.
    Fig. 1. Schematic representation of the two-step exposure technique for the patterned alignment layer of the FLC CDG. (a) The exposure of polarized UV on the SD1 substrate; (b) the exposure of the SD1 substrate with the mask; (c) the FLC CDG cell with a single-side alignment; (d) the chemical formula of the SD1.
    (a) Microscopic photo of the FLC CDG under the crossed polarizer and analyzer. The horizontal yellow bar shows the scale ratio of 200 μm. Red arrows indicate the alignment directions. (b) Illustration of the molecule directions and the helical orientation with respect to the polarizer and analyzer in the odd and even zones. (c) and (e) are the textures of the FLC CDG under the electric field of two polarities; (d) and (f) represent the orientation of the FLC molecules for textures (c) and (e), respectively.
    Fig. 2. (a) Microscopic photo of the FLC CDG under the crossed polarizer and analyzer. The horizontal yellow bar shows the scale ratio of 200 μm. Red arrows indicate the alignment directions. (b) Illustration of the molecule directions and the helical orientation with respect to the polarizer and analyzer in the odd and even zones. (c) and (e) are the textures of the FLC CDG under the electric field of two polarities; (d) and (f) represent the orientation of the FLC molecules for textures (c) and (e), respectively.
    For the eight-order FLC CDG, (a) the far-field diffraction patterns and (b) the corresponding light intensity profile.
    Fig. 3. For the eight-order FLC CDG, (a) the far-field diffraction patterns and (b) the corresponding light intensity profile.
    Switching time of the FLC CDG versus applied electric field. The magnitude of the driving frequency is set at 500 Hz. The inset figure shows the electro-optical response of the diffraction pattern.
    Fig. 4. Switching time of the FLC CDG versus applied electric field. The magnitude of the driving frequency is set at 500 Hz. The inset figure shows the electro-optical response of the diffraction pattern.
    Qi Guo, Tian Liu, Xiaoqian Wang, Zhigang Zheng, Aleksey Kudreyko, Huijie Zhao, V. Chigrinov, Hoi-Sing Kwok. Ferroelectric liquid crystals for fast switchable circular Dammann grating [Invited][J]. Chinese Optics Letters, 2020, 18(8): 080002
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