Liquid crystal devices

Claim 2

A liquid crystal device, comprising: a ferroelectric smectic phase liquid crystal enclosed between two plates, said plates having internal surfaces such that the directors of said liquid crystal adjacent said internal surfaces are not parallel to the internal surfaces; said directors adjacent one of said internal surfaces being not parallel to the directors adjacent the other of said internal surfaces; said directors having a direction which varies across the liquid crystal in the direction between said plates; said plates having a spacing therebetween and the liquid crystal having a cone angle θ s such that an electric field applied between said plates causes switching of said liquid crystal uniquely between two different states, the respective polarizations of which averaged across said liquid crystal are in different directions, said different directions not being parallel to either of said plates; and said liquid crystal cone angle θ s being substantially equal to half the angle 2θ o between a pair of directors, each adjacent a different one of said internal surfaces.

Claim 3

A device according to claim 1, wherein said directors adjacent one of said internal surfaces makes angles θ s with respect to said one surface, and said directors adjacent the other internal surface make angles of 2θ s with respect to said directors adjacent said one surface.

Claim 4

A device according to claim 1, wherein the liquid crystal has a phase sequence ferroelectric smectic→cholesteric→isotropic in order of increasing temperature.

Claim 5

A device according to claim 1, wherein an anisotropic dye is dissolved into the liquid crystal material.

Claim 6

A liquid crystal device, comprising: a ferroelectric smectic phase liquid crystal enclosed between two plates, said plates having internal surfaces such that the directors of said liquid crystal adjacent said internal surfaces are not parallel to the internal surfaces; said directors adjacent one of said internal surfaces being not parallel to the directors adjacent the other of said internal surfaces; said directors having a direction which varies across the liquid crystal in the direction between said plates; said plates having a spacing therebetween and said liquid crystal having a cone angle θ s such that an electric field applied between said plates causes switching of said liquid crystal uniquely between two different states, the respective polarizations of which averaged across said liquid crystal are in different directions, said different directions not being parallel to either of said plates; said liquid crystal cone angle θ s being substantially equal to half the angle 2θ o between a pair of directors, each adjacent a different one of said internal surfaces; said angle θ o being not greater than θ s ; and said directors having projections onto the internal surfaces of the directors adjacent said internal surfaces, said projections making an angle with each other substantially equal to 2θ t , where cos θ.sub.t =cos θ.sub.s sec θ.sub.o.

Claim 7

A liquid crystal device, comprising: a ferroelectric smectic phase liquid crystal enclosed between two plates, said plates having internal surfaces such that the directors of said liquid crystal adjacent said internal surfaces are not parallel to the internal surfaces; said directors adjacent one of said internal surfaces being not parallel to the directors adjacent the other of said internal surfaces; said directors having a direction which varies across the liquid crystal in the direction between said plates; said plates having a spacing therebetween and said liquid crystal having a cone angle θ s such that an electric field applied between said plates causes switching of said liquid crystal uniquely between two different states, the respective polarizations of which averaged across said liquid crystal are in different directions, said different directions not being parallel to either of said plates; said liquid crystal cone angle θ s being substantially equal to half the angle 2θ o between a pair of directors, each adjacent a different one of said internal surfaces; said angle θ o being not greater than θ s ; and said directors having projections onto the internal surfaces of the directors adjacent said internal surfaces, said projections making an angle with each other substantially equal to 2θ t , where cos θ.sub.t =cos θ.sub.s sec θ.sub.o.