Chinese Optics Letters, Volume. 21, Issue 1, 010501(2023)
Electrically switchable structural patterns and diffractions in a dual frequency nematic liquid crystal
Fig. 1. (a) Frequency dependence of dielectric constants (ε∥ and ε⊥) of the DFNLC DP002-026 at various temperatures: 26°C (blue filled circle), 28°C (orange open square), 30°C (green filled rhombus), 32°C (red open triangle), 34°C (purple filled inverted triangle), 36°C (brown open circle), and 38°C (blue filled square). (b) Schematic illustration of the experimental setup for diffraction characterization. A cell is equipped in the hot stage and probed with a linearly polarized laser beam.
Fig. 2. POM images and the corresponding phase diagram of pattern formation for the DFNLC DP002-026. (a) Pattern generation as the field frequency varies from 28 kHz to 40 kHz at the voltage U = 16.1 V, the cell thickness d = 8 µm, and T = 30°C. (b) Pattern generation as the field frequency varies from 25 V to 0 V at the frequency f = 40 kHz, the cell thickness d = 8 µm, 0 V, and T = 30°C. (c) The corresponding phase diagram of pattern formation during voltage decrease for the DFNLC DP002-026 in the cell of thickness d = 8 µm and T = 30°C. The patterns are recorded using crossed polarizers and a quarter waveplate placed at 45° with respect to P. The initial nematic director aligns horizontally.
Fig. 3. Dependences of lateral rolls on the voltage and the dielectric anisotropy of the DFNLC DP002-026. Lateral rolls and corresponding diffraction phenomena at the voltages of amplitude (a) U = 7.5 V, (b) U = 11 V, (c) U = 15 V, and (d) transmitted light intensity versus x. (e) The voltage dependence of the lattice period Px. (f) Px (blue filled circles) and Lx (red open circles) as a function of the voltage frequency. (g) Px as a function of Δε. T = 30°C, d = 8.0 µm, and the initial direction of the director is horizontal.
Fig. 4. Dependences of longitudinal rolls on the voltage and the dielectric anisotropy of the DFNLC DP002-026. Longitudinal rolls and corresponding diffraction phenomena at the voltage of amplitudes (a) U = 14 V, (b) U = 17 V, (c) U = 20.5 V, and (d) transmitted light intensity versus y. (e) The voltage dependence of the lattice period Py. (f) Py (orange filled circles) and Ly (green open circles) as a function of the voltage frequency. (g) Py as a function of Δε. T = 30°C, d = 8.0 µm, and the initial direction of the director is horizontal.
Fig. 5. Dependences of square-grid patterns on the voltage and the dielectric anisotropy of the DFNLC DP002-026. The patterns and corresponding diffraction at the voltages of amplitude (a) U = 17 V, (b) U = 20 V, (c) U = 25 V, and (d) transmitted light intensity versus y. (e) The voltage dependence of the lattice period Px and Py. (f) Px, Py, and Lx, Ly as functions of the voltage frequency. (g) Py as a function of Δε. T = 30°C, d = 8.0 µm, and the initial direction of the director is horizontal.
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Zhenpeng Song, Ziyang Li, Xiaohu Shang, Chaoyi Li, Lingling Ma, Yanqing Lu, Bingxiang Li, "Electrically switchable structural patterns and diffractions in a dual frequency nematic liquid crystal," Chin. Opt. Lett. 21, 010501 (2023)
Category: Diffraction, Gratings, and Holography
Received: May. 17, 2022
Accepted: Aug. 10, 2022
Posted: Aug. 11, 2022
Published Online: Sep. 8, 2022
The Author Email: Lingling Ma (malingling@nju.edu.cn), Bingxiang Li (bxli@njupt.edu.cn)