Method of driving a liquid crystal matrix panel

• US 5,010,327 A
• Filed: 09/05/1986
• Issued: 04/23/1991
• Est. Priority Date: 09/06/1985
• Status: Expired due to Term

• Current Assignee: Matsushita Electric Industrial Company Limited (Panasonic Holdings Corporation)
• Original Assignee: Matsushita Electric Industrial Company Limited (Panasonic Holdings Corporation)
• Inventors: Fujita, Shingo, Ota, Isao, Uemura, Tsuyoshi, Wakita, Naohide, Ohnishi, Hiroyuki, Ohba, Noriko
• Primary Examiner(s): Oberley, Alvin E.
• Application Number:
  US06/903,773
• Time in Patent Office: 1,691 Days
• Field of Search: 340/784, 340/805, 350/330, 350/331 R, 350/331 T, 350/332, 350/333, 350/350 S, 350/347 R
• US Class Current: 345/89
• CPC Class Codes: G09G 2310/06 Details of flat display driving waveforms
• CPC Class Codes: G09G 3/2014 by modulation of the duration of a single pulse during which the logic level remains constant
• CPC Class Codes: G09G 3/3629 using liquid crystals having memory effects, e.g. ferroelectric liquid crystals
• CPC Class Codes: H04N 3/127 using liquid crystals

Abstract

An improved driving method capable of achieving high-quality display even in simple matrix addressing for a ferroelectric liquid crystal matrix panel at a high multiplex ratio applies pulses of a frequency higher than that of a scanning voltage in an addressed condition to a scanning electrode in a non-addressed condition to gain either a surface stabilizing effect or an AC field stabilizing effect, hence ensuring high-contrast display. And the panel is so driven that the temporal average of the voltage applied to each pixel becomes zero, thereby averting deterioration of the liquid crystal.

Claims

1. A method of driving a liquid crystal matrix panel where a ferroelectric liquid crystal having negative dielectric anisotropy is held between scanning electrodes and signal electrodes crossing the scanning electrodes to form a matrix of pixels at crossing positions of the scanning and signal electrodes, comprising the steps of:

applying signal voltage pulses to a signal electrode and addressing voltage pulses to a scanning electrode in an addressed condition so as to make an addressed pixel at the crossing position of the signal electrode and the scanning electrode to be a desired molecular orientation state; and

applying to the scanning electrode, in a non-addressed condition following the addressed condition, voltage pulses whose frequency is higher than that of the addressing voltage pulses and higher than a frequency in which spontaneous polarization of the ferroelectric liquid crystal can follow and whose average voltage is zero so that the effective value of voltage pulses applied to the pixel in the non-addressed condition becomes a substantially constant value greater than an effective threshold voltage at which a molecular orientation stabilizing effect begins to be produced by the dielectric anisotropy, whereby the state of the pixel made in the addressed condition is held in the non-addressed condition until a next addressed condition.

2. A method as claimed in claim 1, wherein a train of high-frequency voltage pulses equal in frequency to the voltage pulses applied to the scanning electrode in the non-addressed condition are applied to the signal electrode for a part of a time period H of the addressed condition in accordance with a grey level of the addressed pixel thereby changing the pulse width of a voltage pulse applied to the addressed pixel so as to allow the state of the addressed pixel to be the grey level.

3. A method as claimed in claim 2, wherein said train of high-frequency pulses applied to the signal electrode each have a fixed duration and a start time thereof is changed in accordance with the grey level.

4. A method as claimed in claim 3, wherein said train of high-frequency pulses applied to the signal electrode each have a duration of 1/2 H and the start time thereof is changed from 0 to 1/2 H in accordance with the grey level.

5. A method as claimed in claim 2, wherein each of said train of high-frequency pulses applied to the signal electrode has approximately double the amplitude of the pulse applied to the scanning electrode.

6. A method as claimed in claim 1, wherein first and second series of AC pulses mutually reverse in polarity sequence are applied to the pixel in one addressed condition, and either the voltage or the pulse duration of at least one series of said AC pulses in the latter half is changed in accordance with the grey level.

7. A method as claimed in claim 6, wherein a grey-scale signal complementary to a desired grey level is superposed on the first-half of the AC pulses.

8. A method as claimed in claim 6, wherein the sequence of any pulses other than the last pulse including the grey-scale signal is changed.

9. A method as claimed in claim 6, wherein said two series of AC pulses are applied through division for two scanning operations.