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Liquid crystal device, liquid crystal device driving method, and electronic apparatus

專利號
US10867567B2
公開日期
2020-12-15
申請人
SEIKO EPSON CORPORATION(JP Tokyo)
發(fā)明人
Satoshi Yatabe; Naoki Tomikawa
IPC分類
G09G3/36; G02F1/1343
技術(shù)領(lǐng)域
potential,electrode,signal,driving,crystal,com,in,ac,liquid,polarity
地域: Tokyo

摘要

A liquid crystal device includes, peripheral electrodes including three electrodes for ion trapping, and a transistor coupled to each of the three electrodes. A common signal (COM signal) that varies between a first potential and a second potential in a first period is applied to a counter electrode. A driving signal that varies between a third potential and a fourth potential is input to the transistor. The driving signal is coupled to or uncoupled from the peripheral electrodes by the transistor in a unit of a duration equal to or less than ? of the first period. AC signals varying between a positive-polarity potential and a negative-polarity potential, with a potential of the common signal being a reference, in a second period longer than the first period, are applied to the three electrodes of the peripheral electrodes, in a state where phases of the AC signals are shifted mutually.

說明書

where n is the number of the electrodes configured for ion trapping.

When the difference Δt in phase between the AC signals applied to adjacent electrodes configured for ion trapping is ? period as described in Examples 1, 2, 3, 4, and 5 above, when the AC signals having rectangular waves transition between +5 V and ?5 V, taking the COM potential as a reference, the potential difference Vn between adjacent electrodes configured for ion trapping is 10 V. Furthermore, when the arrangement pitch p of the electrodes configured for ion trapping is, for example, 8 μm and the mobility μ of the ionic impurities is 2.2×10?10 (m2/V·s), a preferable frequency f is approximately 12 Hz according to equation (6).

Note that the value of the mobility μ of ionic impurities is described in, for example, A. Sawada, A. Manabe and S. Naemura, “A Comparative Study on the Attributes of Ions in Nematic and Isotropic Phases”, Jpn. J. Appl Phys Vol. 40, p 220-p 224 (2001). It is also confirmed that ionic impurities having mobility μ that is approximately three orders of magnitude smaller may exist depending on the liquid crystal material or the configuration of the liquid crystal panel.

When the mobility μ of the ionic impurities contained in the liquid crystal layer 50 has a value of 2.2×10?10 (m2/V·s) as described above, a frequency f of the AC signals of higher than 12 Hz causes the ionic impurities not to keep up with the scrolling of electric field, and thus the frequency f is preferably smaller than 12 Hz.

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