Liquid crystal device using ferroelectric liquid crystal twisted in two stable states

Claim 2

A liquid crystal device comprising a first base plate, a second base plate and a ferroelectric liquid crystal disposed between the first and second base plates and placed under bistability condition comprising a first state and a second state; said ferroelectric liquid crystal being placed under the bistability condition in the presence of a surface which has been subjected to a uniaxial orientation treatment in an axial direction O, the liquid crystal molecules in the first state being arranged so as to be successively twisted from an axis A to an axis Aa, and the liquid crystal molecules in the second state being arranged so as to be successively twisted from an axis B to an axis Ba; wherein the axis A denotes the projection of a liquid crystal molecular axis in the vicinity of the first base plate face onto the first base plate face in the first state, the axis Aa denotes the projection of a liquid crystal molecular axis in the vicinity of the second base plate face onto the second base plate face, in the first state, the axis B denotes the projection of a liquid crystal molecular axis in the vicinity of the first base plate face onto the first base plate face in the second state, and the axis Ba denotes the projection of a liquid crystal molecular axis in the vicinity of the second base plate face onto the second base plate face in the second state.

Claim 3

The liquid crystal device according to claim 1, wherein the angle between the axes O and A is substantially equal to the angle between the axes O and Ba.

Claim 4

The liquid crystal device according to claim 1, wherein the angle between the axes O and Aa is substantially equal to the angle between the axes O and B.

Claim 5

The liquid crystal device according to claim 1, wherein the axis A substantially coincides with the transmission (or absorption) axis of the polarizer and, when the angle between the axes A and Aa is denoted by θ 1 , the transmission (or absorption) axis of the analyzer is disposed so that it will form an angle of 90°±θ 1 with the transmission (or absorption) axis of the polarizer.

Claim 6

The liquid crystal device according to claim 1, wherein the axis A substantially coincides the transmission (or absorption) axis of the polarizer and the axis Aa substantially coincides with the transmission (or absorption) axis of the analyzer.

Claim 7

The liquid crystal device according to claim 1, wherein said uniaxial orientation treatment is a rubbing treatment.

Claim 8

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

Claim 9

The liquid crystal device according to claim 7, wherein said chiral smectic liquid crystal is in chiral smectic C phase, H phase, F phase, I phase, J phase, G phase or K phase.

Claim 10

The liquid crystal device according to claim 1, wherein said ferroelectric liquid crystal is in a phase formed by phase transition from smectic A phase on temperature decrease.

Claim 11

The liquid crystal device according to claim 1, wherein said ferroelectric liquid crystal is in a phase formed by a successive phase transition through cholesteric phase and smectic A phase in the order named.

Claim 12

A liquid crystal device comprising a ferroelectric liquid crystal placed under bistability condition comprising two stable states, said ferroelectric liquid crystal being placed under the bistability condition in the presence of a surface which has been subjected to a uniaxial orientation treatment, the molecules of the ferroelectric liquid crystal aligning so as to be twisted in the direction of the liquid crystal layer thickness in either of the two stable states, the average electric dipole moments of the liquid crystal molecules in the two stable states being in mutually opposite polarities.

Claim 13

A liquid crystal device comprising a ferroelectric liquid crystal placed under bistability condition comprising two stable states, said ferroelectric liquid crystal being placed under the bistability condition in the presence of a surface which has been subjected to a uniaxial orientation treatment, the molecules of the ferroelectric liquid crystal aligning so as to be twisted in the direction of the liquid crystal layer thickness in either of the two stable states, the average electric dipole moments of the liquid crystal molecules in the two stable states being in mutually opposite polarities.

Claim 14

The liquid crystal device according to claim 11, wherein said uniaxial orientation treatment is a rubbing treatment.

Claim 15

The liquid crystal device according to claim 11, wherein said ferroelectric liquid crystal is a chiral smectic liquid crystal.

Claim 16

The liquid crystal device according to claim 13, wherein said chiral smectic liquid crystal is in chiral smectic C phase, H phase, F phase, I phase, J phase, G phase or K phase.

Claim 17

The liquid crystal device according to claim 11, wherein said ferroelectric liquid crystal is in a phase formed by phase transition from smectic A phase on temperature decrease.

Claim 18

The liquid crystal device according to claim 11, wherein said ferroelectric liquid crystal is in a phase formed by a successive phase transition through cholesteric phase and smectic A phase in the order named.

Claim 19

A liquid crystal device comprising first and second base plates having mutually opposite electrodes, a ferroelectric smectic liquid crystal sandwiched between the first and second base plates, a polarizer disposed in the neighborhood of the first base plate, and an analyzer disposed in the neighborhood of the second base plate, said polarizer and analyzer are so disposed that their transmission (or absorption) axes do not cross at right angles.

Claim 20

A liquid crystal device comprising first and second base plates having mutually opposite electrodes, a ferroelectric smectic liquid crystal sandwiched between the first and second base plates, a polarizer disposed in the neighborhood of the first base plate, and an analyzer disposed in the neighborhood of the second base plate, said polarizer and analyzer are so disposed that their transmission (or absorption) axes do not cross at right angles.

Claim 21

The liquid crystal device according to claim 17, wherein the transmission (or absorption) axes of the polarizer and the analyzer form an angle of 90°±(2.5° to 25°).

Claim 22

The liquid crystal device according to claim 17, wherein said ferroelectric smectic liquid crystal is placed under bistability condition comprising two stable states of molecular arrangement so that the two stable states of molecular arrangement are switched to each other to cause optical switching by applying mutually opposite polarities of voltages to the opposite electrodes.

Claim 23

The liquid crystal device according to claim 19, wherein the molecules of the ferroelectric liquid crystal align so as to be twisted in the direction of the liquid crystal layer thickness in either of the two stable states.

Claim 24

The liquid crystal device according to claim 17, wherein said ferroelectric smectic liquid crystal is a chiral smectic liquid crystal.

Claim 25

The liquid crystal device according to claim 21, wherein said chiral smectic liquid crystal is in chiral smectic C phase, H phase, F phase, I phase, J phase, G phase or K phase.

Claim 26

A switching device for electrooptically switching light rays from a light source, comprising: a. switching means comprising a pair of oppositely spaced electrodes and a ferroelectric liquid crystal disposed between the opposite electrodes and placed under bistability condition comprising two stable states in the presence of a surface which has been subjected to a uniaxial orientation treatment, the molecules of the ferroelectric liquid crystal aligning so as to be twisted in either of the two stable states, b. means for applying a first voltage signal for orienting the liquid crystal molecules to one stable state and a second voltage signal for orienting the liquid crystal molecules to the other stable state, and c. means for detecting an optical difference between a light ray having passed through ferroelectric liquid crystal molecules oriented to said one stable state and a light ray having passed through ferroelectric liquid crystal molecules oriented to said other stable state.

Claim 27

A switching device for electrooptically switching light rays from a light source, comprising: a. switching means comprising a pair of oppositely spaced electrodes and a ferroelectric liquid crystal disposed between the opposite electrodes and placed under bistability condition comprising two stable states in the presence of a surface which has been subjected to a uniaxial orientation treatment, the molecules of the ferroelectric liquid crystal aligning so as to be twisted in either of the two stable states, b. means for applying a first voltage signal for orienting the liquid crystal molecules to one stable state and a second voltage signal for orienting the liquid crystal molecules to the other stable state, and c. means for detecting an optical difference between a light ray having passed through ferroelectric liquid crystal molecules oriented to said one stable state and a light ray having passed through ferroelectric liquid crystal molecules oriented to said other stable state.

Claim 28

The switching device according to claim 23, wherein the electric fields of said first and second voltage signals are mutually opposite in direction.

Claim 29

The switching device according to claim 23, wherein said first and second voltage signals are mutually opposite polarities of voltages.

Claim 30

The switching device according to claim 23, wherein said means for detecting an optical difference comprises a polarizer and an analyzer arranged in cross nicols.

Claim 31

The switching device according to claim 26, wherein the transmission (or absorption) axes of the polarizer and the analyzer do not cross at right angles.

Claim 32

The switching device according to claim 27, wherein the transmission (or absorption) axes of the polarizer and the analyzer form an angle of 90°±(2.5° to 25°).

Claim 33

A switching device for electrooptically switching light rays from a light source, comprising: a. switching means comprising a pair of oppositely spaced electrodes and a ferroelectric liquid crystal disposed between the opposite electrodes and placed under bistability condition comprising two stable states in the presence of a surface which has been subjected to a uniaxial orientation treatment in an axial direction O, the liquid crystal molecules in the first state being arranged so as to be successively twisted from an axis A to an axis Aa, and the liquid crystal molecules in the second state being arranged so as to be successively twisted from an axis B to an axis Ba, wherein the axis A denotes the projection of a liquid crystal molecular axis on the vicinity of the first base plate face onto the first base plate face in the first state, the axis Aa denotes the projection of a liquid crystal molecular axis in the vicinity of the second base plate face onto the second base plate face, in the first state, the axis B denotes the projection of a liquid crystal molecular axis in the vicinity of the first base plate face onto the first base plate face in the second state, and the axis Ba denotes the projection of a liquid crystal molecular axis in the vicinity of the second base plate face onto the second base plate face in the second state, b. means for selectively applying first and second voltage signals of which the electric fields are in mutually opposite directions between the opposite electrodes, and c. optical detecting means comprising a polarizer so arranged that the transmission (or absorption) axis substantially coincides with any one axis of said axes A, Aa, B, and Ba.

Claim 34

A switching device for electrooptically switching light rays from a light source, comprising: a. switching means comprising a pair of oppositely spaced electrodes and a ferroelectric liquid crystal disposed between the opposite electrodes and placed under bistability condition comprising two stable states in the presence of a surface which has been subjected to a uniaxial orientation treatment in an axial direction O, the liquid crystal molecules in the first state being arranged so as to be successively twisted from an axis A to an axis Aa, and the liquid crystal molecules in the second state being arranged so as to be successively twisted from an axis B to an axis Ba, wherein the axis A denotes the projection of a liquid crystal molecular axis on the vicinity of the first base plate face onto the first base plate face in the first state, the axis Aa denotes the projection of a liquid crystal molecular axis in the vicinity of the second base plate face onto the second base plate face, in the first state, the axis B denotes the projection of a liquid crystal molecular axis in the vicinity of the first base plate face onto the first base plate face in the second state, and the axis Ba denotes the projection of a liquid crystal molecular axis in the vicinity of the second base plate face onto the second base plate face in the second state, b. means for selectively applying first and second voltage signals of which the electric fields are in mutually opposite directions between the opposite electrodes, and c. optical detecting means comprising a polarizer so arranged that the transmission (or absorption) axis substantially coincides with any one axis of said axes A, Aa, B, and Ba.

Claim 35

The switching device according to claim 29, wherein said optical detecting means further comprises an analyzer, the transmission (or absorption) axis substantially coincides with the axis A and, when the angle between the axes A and Aa is denoted by θ 1 , the transmission (or absorption) axis of the analyzer is disposed so that it will form an angle of 90°±θ 1 with the transmission (or absorption) axis of the polarizer.

Claim 36

The switching device according to claim 29, wherein said optical detecting means further comprises an analyzer, the transmission (or absorption) axis substantially coincides with the axis A, and the transmission (or absorption) axis of the analyzer substantially coincides with the axis Aa.

Claim 37

The switching device according to claim 29, wherein said first and second voltage signals have mutually opposite polarities.

Claim 38

The liquid crystal device according to claim 29, wherein the angle between the axes O and A is substantially equal to the angle between the axes O and Ba.

Claim 39

The liquid crystal device according to claim 29, wherein the angle between the axes O and Aa is substantially equal to the angle between the axes O and B.

Claim 42

The method according to claim 35, wherein the molecules of the ferroelectric liquid crystal align so as to be twisted in the direction of the liquid crystal layer thickness in either of the two states, and the average electric dipole moments of the liquid crystal molecules in the two states being in mutually opposite polarities.

Claim 43

The method according to claim 35, wherein said ferroelectric liquid crystal is a chiral smectic liquid crystal.

Claim 44

The method according to claim 37, wherein said chiral smectic liquid crystal is in chiral smectic C phase, H phase, F phase, I phase, J phase, G phase or K phase.