Lingling Ma, Chaoyi Li, Luyao Sun, Zhenpeng Song, Yanqing Lu, Bingxiang Li, "Submicrosecond electro-optical switching of one-dimensional soft photonic crystals," Photonics Res. 10, 786 (2022)

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- Photonics Research
- Vol. 10, Issue 3, 786 (2022)

Fig. 1. Optical characteristics of CLCs. (a) Schematic illustration of the 1D helical structure. Blue rods represent LC directors. White bidirectional arrow denotes the alignment direction. Green and pink arrows indicate the transmission and reflection of light. (b) POM images of planar CLCs at different c . They are taken under the reflection mode. Scale bar, 200 μm. (c) Reflection spectra of CLC mixtures with different c . The incident laser beam is linearly polarized. (d) Dependencies of λ 1 and λ 2 on c and 1 / c . The dashed line is a linear fitting. (e) Reflection spectra of the CLC mixture at different temperatures. (f) λ 1 , λ 2 , and P as functions of the temperature at c = 20.6 % .

Fig. 2. Electro-optic responses of CLC. (a) Dynamics of the transmitted light intensity of CLC under E 1 ≈ 62 V/μ m , E 2 ≈ 84 V/μ m , E 3 ≈ 107 V/μ m , E 4 ≈ 128 V/μ m , and E 5 ≈ 142 V/μ m . (b) Δ I as a function of E . The dashed line shows the linear fitting. (c) Dependency of τ max on E .

Fig. 3. Schematic illustration of field-induced effects. (a) Orientational order of LC molecules and ellipsoid optical tensor in the absence of an electric field. (b) Thermal fluctuation of the optical tensor. (c) Orientational order of LC molecules and elongated oblate optical tensor under an electric field. (d) Quenching of the optical tensor fluctuation.

Fig. 4. Three experimental geometries. (a) Geometry BU: n ^ orients parallel to the plane of incidence. (b) Geometry UF: n ^ is perpendicular to the plane of incidence. (c) Geometry FBU: the laser beam is normally incident to the cell. The polarization is 45º with respect to n ^ . Red bidirectional arrows indicate the incident polarizations. Black bidirectional arrows represent the alignment of LCs. In both BU and UF geometries, the incident angles are 45º, and the polarization of the incident light is 45º with respect to the plane of incidence.

Fig. 5. Submicrosecond electro-optic switching of the nematic LC host. (a) Field-induced δ n in three geometries. The duration of DC pulse is 400 ns; the amplitude is 142 V/μ m . (b) Dynamics of δ n at different E . (c) Dependency of δ n max on E . The dashed line is a parabola fitted curve. (d) Dependence of the τ max on the E . Data in (b)–(d) are obtained from experiments in geometry FBU.

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