Abstract

In liquid crystal (LC) displays, deriving an optimum resistance level of an LC alignment polyimide (PI) layer is important because of the trade-off between the voltage holding and surface-discharging properties. In particular, to apply a power-saving low-frequency operation scheme to fringe-field switching (FFS) LC modes with negative dielectric LC (n-LC), delicate material engineering is required to avoid surface-charge-dependent image flickering and sticking problems, which severely degrade with lowering operation frequency. Therefore, this paper proposes a photocontrolled variable-resistivity PI layer in order to systematically investigate the voltage holding and discharging properties of the FFS n-LC modes, according to the PI resistivity (ρ) levels. By doping fullerene into the high-ρ PI as the photoexcited charge-generating nanoparticles, the ρ levels of the PI were continuously controllable with a wide tunable range (0.95 × 1015 Ω∙cm to 5.36 × 1013 Ω∙cm) through Ar laser irradiation under the same LC and LC alignment conditions. The frequency-dependent voltage holding and discharge behaviors were analyzed with photocontrolled ρ variation. Thus, the proposed experimental scheme is a feasible approach in PI engineering for a power-saving low-frequency FFS n-LC mode without the image flickering and image sticking issues.

Highlights

  • This paper presents an optical ρ-variable PI layer, achieved by doping photoinduced charge generation fullerenes into a high-ρ liquid crystal (LC) alignment PI, in order to systematically investigate the trade-off between the voltage holding and discharging properties in the low-frequency-driven fringe-field switching (FFS) negative dielectric LC (n-LC) modes

  • With the photocontrolled ρvariable LC alignment PI layer, the frequency-dependent voltage holding ratios (VHRs) and discharging coefficients of the FFS n-LC cell were analyzed through a quantitative comparison according to the PI

  • The photocontrolled discharging coefficient showed a tunable range from α = 0.003 s−1 without Ar irradiation to α = 0.039 s−1 with Ar irradiation (50 mW·cm−2 intensity)

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Summary

Introduction

Fringe-field switching (FFS) liquid crystal (LC) modes are widely applied to mobile display applications as the most competitive LC operation scheme, owing to their high optical efficiency and low power consumption [1,2,3]. With increasing pixel density, the mobile display panels suffer from power consumption issues. Because the power consumption level in driving circuits is proportional to the operation frequency [6,7], extensive efforts have been made to reduce the operation frequency level of FFS LC modes without degrading the image quality [8,9,10,11,12,13,14,15,16]

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