Chinese Journal of Liquid Crystals and Displays, Volume. 37, Issue 12, 1507(2022)
Recent progress in oblique heliconical cholesteric liquid crystal materials
Fig. 1. Structural diagram of(a)ordinary cholesteric phase and(b)ChOH
Fig. 2. Field induced behavior of cholesterics structures.(a)Right-angle helicoidal cholesteric in a planar cell;(b)Sufficiently strong vertical electric field E realigns the cholesteric axis perpendicularly to itself,causing light-scattering fingerprint texture;(c)Heliconical structure in a cholesteric stabilized by the vertical electric field E1;(d)Pitch P and tilt angle θ of the field-induced heliconical state decrease as the electric field increases,E2>E1;(e)As the field increases further,to some E3>E2,it unwinds the helical structure completely and forms a homeotropic nematic state[16].
Fig. 3. Electric field-controlled structural colors of a ChOH cell.(a)Polarizing optical microscope textures;(b)Reflection spectra,incident light is unpolarized[17].
Fig. 4. Absorbance and fluorescence spectra of laser dyes in CLC mixtures.(a)DCM;(b)LD688[14].
Fig. 5. Electric field dependence of the lasing wavelength λ for DCM and LD688 dye-doped CLCOH samples[14]
Fig. 6. Spectra of heliconical cholesteric liquid crystals modulated by electricfiled with different mass fraction of chiral photosensitive materials(a)2.0%,(b)1.5%,(c)1.0%[19].
Fig. 7. Electrically tunable selective reflection of red,green and blue colours for different temperatures.(a)16.5 ℃;(b)18.5 ℃;(c)21.5 ℃;(d)25.5 ℃[18].
Fig. 8. Temperature dependence of the bend elastic constant K33[24]
Fig. 9. (a)Selective light reflection of mixture at different temperatures;(b)Reflection color image in reflection mode of polarized light microscope[25].
Fig. 10. Effect of(a)5CB,(b)R811 and(c)COC concentration on the phase transition temperatures between isotropic(Iso),nematic(N)and twist-bend nematic(Ntb)phases in the mixture[25].
Fig. 11. Reflection spectra recorded from the mixture for different values of the magnetic fields at temperatures of 32 ℃(bottom),35 ℃(middle)and 38 ℃(top),all are within the N∗ range[15].
Fig. 12. Helix transformation based on a photo responsive cholesteric LC system by dual stimulation with electric field and light[31]
Fig. 13. Performance of soft superstructure transformation with electrical and optical stimuli as driving modes[31]
Fig. 14. Sample appearance in reflection mode under the action of an increasing static electric field in the absence(left column)and in the presence(right column)of an optical field[32].
Fig. 15. Evolution of optical intensity dependent central wavelength of the reflection band under various electric field intensities[19]
Fig. 17. Transmission spectra of polymer stabilized samples as a functionof electric field[37]
Fig. 19. Spectra of samples stabilized by different chiral doped polymers(a)R811 and(b)S811 under different detection light polarization conditions[37]
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Xiang-hui TIAN, Hao SUN, Shuang-shuang ZENG, Hai-yi LIN, Jin-bao GUO. Recent progress in oblique heliconical cholesteric liquid crystal materials[J]. Chinese Journal of Liquid Crystals and Displays, 2022, 37(12): 1507
Category: Research Articles
Received: Jul. 22, 2022
Accepted: --
Published Online: Nov. 30, 2022
The Author Email: Jin-bao GUO (guojb@mail.buct.edu.cn)