Method of control of a liquid-crystal display cell

Claim 1

A method of sequential control of a liquid-crystal display cell comprising a liquid-crystal film interposed between a first group of electrodes and a second group of electrodes, overlapping of one electrode of the first group by one electrode of the second group defining an excitable zone of the liquid-crystal film, said liquid crystal having dielectric anisotropy and a critical frequency at which said dielectric anisotropy undergoes a change of sign, the value of anisotropy being ε 1 below said critical frequency and ε 2 above said critical frequency, said liquid-crystal assuming a first optical state "0" corresponding to a first orientation of its molecules when subjected to an alternating electric field at a low frequency below said critical frequency and assuming a second optical state "1" corresponding to a second orientation of its molecules when subjected to an alternating electric field at a high frequency above said critical frequency, the steps of applying on the electrodes of the first group which controls the point at which it is desired to effect the display a voltage at said low frequency having an RMS values of V 1BF and a voltage at said high frequency having an RMS value of V 1HF and a zero voltage on the other electrodes of the first group, applying on the electrodes of the second group which controls the points at which it is desired to effect the display a voltage at said low frequency having an RMS value of V 2BF and a voltage at said high frequency having an RMS value of V 2HF , said RMS values being related by the inequality: ε.sub.1 (V.sub.1BF - V.sub.2BF).sup.2 < ε.sub.2 (V.sub.1HF + V.sub.2HF).sup.2 in the zones in which the state "0" is to be displayed and related by the contrary inequality in the zones in which the state "1" is to be displayed.

Claim 2

A method of sequential control of a liquid-crystal display cell comprising a liquid-crystal film interposed between a first group of electrodes and a second group of electrodes, overlapping of one electrode of the first group by one electrode of the second group defining an excitable zone of the liquid-crystal film, said liquid crystal having dielectric anisotropy and a critical frequency at which said dielectric anisotropy undergoes a change of sign, the value of anisotropy being ε 1 below said critical frequency and ε 2 above said critical frequency, said liquid-crystal assuming a first optical state "0" corresponding to a first orientation of its molecules when subjected to an alternating electric field at a low frequency below said critical frequency and assuming a second optical state "1" corresponding to a second orientation of its molecules when subjected to an alternating electric field at a high frequency above said critical frequency, the steps of applying on the electrodes of the first group which controls the point at which it is desired to effect the display a voltage at said low frequency having an RMS values of V 1BF and a voltage at said high frequency having an RMS value of V 1HF and a zero voltage on the other electrodes of the first group, applying on the electrodes of the second group which controls the points at which it is desired to effect the display a voltage at said low frequency having an RMS value of V 2BF and a voltage at said high frequency having an RMS value of V 2HF , said RMS values being related by the inequality: ε.sub.1 (V.sub.1BF - V.sub.2BF).sup.2 < ε.sub.2 (V.sub.1HF + V.sub.2HF).sup.2 in the zones in which the state "0" is to be displayed and related by the contrary inequality in the zones in which the state "1" is to be displayed.

Claim 3

A method of sequential control of a liquid-crystal display cell of the type consisting of a matrix of points defined by the overlapping of crossed strips disposed in k columns in crossed relation with lines, said liquid-crystal having dielectric anisotropy and a critical frequency at which said dielectric anisotropy undergoes a change of sign, the value of anisotropy being ε 1 below the critical frequency and ε 2 above said critical frequency, said liquid-crystal assuming a first optical state "0" corresponding to a first orientation of its molecules when subjected to an alternating electric field at a low frequency below said critical frequency and assuming a second optical state "1" corresponding to a second orientation of its molecules when subjected to an alternating electric field at high frequency above said critical frequency, the steps of applying sequentially to the columns a voltage at said low frequency having an RMS value of V 1BF and a voltage at said high frequency having an RMS value of V 1HF and a zero voltage is applied to the other columns, applying a low-frequency voltage having an RMS value of - V 2BF and a high-frequency voltage having an RMS value of V 2HF to the lines corresponding to those points of the column at which it is desired to produce the state "0", applying a low-frequency voltage having an RMS value of V 2BF and a high-frequency voltage having an RMS value of - V 2HF to the lines corresponding to those points of the column at which it is desired to produce the state "1", adjusting the RMS values of the voltages to provide that the quantity ε.sub.1 (V.sub.1BF - V.sub.2BF).sup.2 + (K - 1) ε.sub.1 (V.sub.2BF).sup.2 relating to the low-frequency signals is smaller than the quantity ε.sub.1 (V.sub.1HF + V.sub.2HF).sup.2 + (K - 1) ε.sub.2 (V.sub.2HF).sup.2 relating to the high-frequency signals in respect of all points of the cell at which the state "1" is produced and to provide that this inequality is reversed in the case of all points of the cell at which the state "0" is produced.

Claim 4

A method of sequential control of a liquid-crystal display cell of the type consisting of a matrix of points defined by the overlapping of crossed strips disposed in k columns in crossed relation with lines, said liquid-crystal having dielectric anisotropy and a critical frequency at which said dielectric anisotropy undergoes a change of sign, the value of anisotropy being ε 1 below the critical frequency and ε 2 above said critical frequency, said liquid-crystal assuming a first optical state "0" corresponding to a first orientation of its molecules when subjected to an alternating electric field at a low frequency below said critical frequency and assuming a second optical state "1" corresponding to a second orientation of its molecules when subjected to an alternating electric field at high frequency above said critical frequency, the steps of applying sequentially to the columns a voltage at said low frequency having an RMS value of V 1BF and a voltage at said high frequency having an RMS value of V 1HF and a zero voltage is applied to the other columns, applying a low-frequency voltage having an RMS value of - V 2BF and a high-frequency voltage having an RMS value of V 2HF to the lines corresponding to those points of the column at which it is desired to produce the state "0", applying a low-frequency voltage having an RMS value of V 2BF and a high-frequency voltage having an RMS value of - V 2HF to the lines corresponding to those points of the column at which it is desired to produce the state "1", adjusting the RMS values of the voltages to provide that the quantity ε.sub.1 (V.sub.1BF - V.sub.2BF).sup.2 + (K - 1) ε.sub.1 (V.sub.2BF).sup.2 relating to the low-frequency signals is smaller than the quantity ε.sub.1 (V.sub.1HF + V.sub.2HF).sup.2 + (K - 1) ε.sub.2 (V.sub.2HF).sup.2 relating to the high-frequency signals in respect of all points of the cell at which the state "1" is produced and to provide that this inequality is reversed in the case of all points of the cell at which the state "0" is produced.

Claim 7

A method of sequential control of a liquid crystal display cell of the type consisting of a matrix of points defined by the overlapping of crossed strips disposed in k columns in crossed relation with lines, said liquid crystal having dielectric anisotropy undergoes a change of sign, the value of anisotropy being ε 1 below the critical frequency and ε 2 above said critical frequency, said liquid crystal assuming a first optical state "0" corresponding to a first orientation of its molecules when subjected to an alternating electric field at a low frequency below said critical frequency and assuming a second optical state "1" corresponding to a second orientation of its molecules when subjected to an alternating electric field at a high frequency above said critical frequency, the steps of applying a low-frequency voltage having an RMS value of - V and a high-frequency voltage having an RMS value ##EQU9## to the lines corresponding to those points of the column at which it is desired to produce the state "0", and applying a low-frequency voltage having an RMS value of V and a high-frequency voltage having an RMS value ##EQU10## to the lines corresponding to those points of the column at which it is desired to produce the state "1".

Claim 8

A method of sequential control of a liquid crystal display cell of the type consisting of a matrix of points defined by the overlapping of crossed strips disposed in k columns in crossed relation with lines, said liquid crystal having dielectric anisotropy undergoes a change of sign, the value of anisotropy being ε 1 below the critical frequency and ε 2 above said critical frequency, said liquid crystal assuming a first optical state "0" corresponding to a first orientation of its molecules when subjected to an alternating electric field at a low frequency below said critical frequency and assuming a second optical state "1" corresponding to a second orientation of its molecules when subjected to an alternating electric field at a high frequency above said critical frequency, the steps of applying a low-frequency voltage having an RMS value of - V and a high-frequency voltage having an RMS value ##EQU9## to the lines corresponding to those points of the column at which it is desired to produce the state "0", and applying a low-frequency voltage having an RMS value of V and a high-frequency voltage having an RMS value ##EQU10## to the lines corresponding to those points of the column at which it is desired to produce the state "1".