Driving method for liquid crystal cell and liquid crystal apparatus

Claim 2

A driving method for a liquid crystal cell of the type constructed without a photoconductive layer comprising a pair of oppositely spaced electrodes forming a matrix electrode structure, a dielectric layer disposed on either one or both sides of the pair of electrodes, and a memory type ferroelectric liquid crystal disposed between the oppositely spaced electrodes, said driving method comprising the step of: applying to the liquid crystal cell a driving voltage having a rectangular waveform of a duration provided with an attenuation slope at the falling part thereof.

Claim 3

The driving method according to claim 1, wherein said attenuation slope is expressed by a linear or exponential function.

Claim 4

The driving method according to claim 1, wherein said ferroelectric liquid crystal is a chiral smectic liquid crystal.

Claim 5

The driving method according to claim 1, wherein said ferroelectric liquid crystal is a chiral smectic liquid crystal having at least two stable states.

Claim 6

The driving method according to claim 1, wherein said ferroelectric liquid crystal is a bistable chiral smectic liquid crystal.

Claim 7

The driving method according to claim 1, wherein said ferroelectric liquid crystal is a chiral smectic liquid crystal with a non-spiral structure.

Claim 8

The driving method according to claim 1, which further comprises a dielectric layer of an insulating material between the pair of oppositely spaced electrodes.

Claim 9

A liquid crystal apparatus, comprising: (a) a liquid crystal cell without a photoconductive layer comprising a pair of oppositely spaced electrodes forming a matrix electrode structure, a dielectric layer disposed on either one or both sides of the pair of electrodes, and a memory type ferroelectric liquid crystal disposed between the oppositely spaced electrodes; (b) means for applying a driving voltage between the pair of electrodes, said means comprising means for applying a scanning voltage signal having a rectangular waveform of a duration provided with an attenuation slope at the falling part thereof; and (c) means for detecting an optical change based on a change in orientation of the memory type ferroelectric liquid crystal.

Claim 10

A liquid crystal apparatus, comprising: (a) a liquid crystal cell without a photoconductive layer comprising a pair of oppositely spaced electrodes forming a matrix electrode structure, a dielectric layer disposed on either one or both sides of the pair of electrodes, and a memory type ferroelectric liquid crystal disposed between the oppositely spaced electrodes; (b) means for applying a driving voltage between the pair of electrodes, said means comprising means for applying a scanning voltage signal having a rectangular waveform of a duration provided with an attenuation slope at the falling part thereof; and (c) means for detecting an optical change based on a change in orientation of the memory type ferroelectric liquid crystal.

Claim 11

The liquid crystal apparatus according to claim 8, wherein said ferroelectric liquid crystal is a chiral smectic liquid crystal having at least two stable states.

Claim 12

The liquid crystal apparatus according to claim 8, wherein said attenuation slope is expressed by linear or exponential function.

Claim 13

The liquid crystal apparatus according to claim 8, wherein one of said pair of electrodes is connected to a scanning side driver circuit and is supplied with a pulse voltage waveform comprising a rectangular rising part followed by a constant amplitude and a attenuated falling slope.