Method for controlling an optical characteristic of a material and an analog imager for carrying out said method

Claim 3

A method according to claim 1 for a sequential control of an optical characteristic of a material constituting a plurality of zones arranged in a matrix and intercalated between a first family of p parallel control lines and a second family of q parallel control columns, the lines and the columns being in crossed relation, a zone x i y j being defined by that region of the material which is covered by the column x i where i is an integer 1≦j≦q and by the line y j where j is an integer 1≦j≦p, said lines and columns being employed to carry suitable signals for producing excitation of the material, wherein said method consists for the purpose of controlling said optical characteristic of the material of the zone x i y j at a value C in applying a signal A x to the column x i and a zero signal to the other columns and in applying to the line y j a signal A.sub. y having twice the duration and the same frequency equal to that of signal A x and wherein said phase shift is modified in order to adjust said optical characteristic of the material within the zone x i y j to said value C.

Claim 4

A method according to claim 2, wherein said characteristic is an even-numbered function of the excitation.

Claim 5

A method according to claim 2, wherein said method consists in controlling simultaneously the value of the optical characteristic of all the zones of a given column x i by applying simultaneously to each line the signal A y which corresponds thereto.

Claim 6

A method according to claim 2, wherein the signals A x and A y are rectangular signals having a zero mean value.

Claim 7

A method according to claim 2, wherein the signals A x and A y are sinusoidal signals having a zero mean value.

Claim 8

A method according claim 1, wherein said material is a liquid crystal film in which one optical characteristic is dependent on an electric field applied thereto, said excitation signals being voltages.

Claim 9

A method according to claim 7, wherein said liquid crystal has a birefringence induced by an effect of collective orientation of its molecules and wherein said optical characteristic is said birefringence.

Claim 10

A method for controlling an analog imager of the crossbar type comprising a matrix of zones in which one optical characteristic is controlled in accordance with the method of claim 2, said characteristic C being related to said phase shift φ by a law C (φ) wherein, in order to ensure that the characteristic C displayed in zone x i y j is an analog function of a value G of an input quantity assuming an amplitude which has a maximum, the following operations are performed: dividing the maximum amplitude which can be assumed by the input quantity into n quantization levels, taking account of said law C (φ) which relates the value of the characteristic C of the material to the phase shift φ between the excitation signals, forming n discrete values of the phase shift φ between 0 and π corresponding to the n quantization levels, forming by means of a periodic reference signal A x , n phase-shifted signals A y of said n discrete values of φ, causing to correspond to each value of the input quantity a signal A y which is phase-shifted with respect to A x by the appropriate value φ, said signal being applied to the line y j , applying said reference signal A x to the column x i .

Claim 11

A method according to claim 2 for controlling an analog imager of a crossbar type comprising a matrix of zones said material having an optical characteristic which is related to the phase shift φ between the excitation signals by the law C (φ) wherein, in order to ensure that said optical characteristic C displayed in a zone x i y j covered by column x i and line y i is an analog function of the value G of an input quantity, the following operations are performed: generating a periodic reference signal A x , generating in respect of each value of the input quantity a signal A y (φ) which is phase-shifted with respect to the signal A x by a value φ which is determined by said known law C (φ), applying said reference signal A x to the column x i , applying said signal A y (φ) to the line y j .

Claim 12

An analog imager for controlling an optical characteristic of a material comprising a display cell constituted by said material intercalated between two electrodes driven by periodic excitation signals, said material being such as to have an optical characteristic which is dependent on said excitation, and comprising means for delivering said excitation signals to said electrodes, wherein said means comprise means for delivering excitation signals having equal recurrence frequency and equal duration but having a phase shift φ with respect to each other and means for modifying said phase shift to any values between 0 and π in order to adjust said characteristic to correspond to any value G of an input quantity to be displayed.

Claim 13

An analog imager for controlling an optical characteristic of a material comprising a display cell constituted by said material intercalated between two electrodes driven by periodic excitation signals, said material being such as to have an optical characteristic which is dependent on said excitation, and comprising means for delivering said excitation signals to said electrodes, wherein said means comprise means for delivering excitation signals having equal recurrence frequency and equal duration but having a phase shift φ with respect to each other and means for modifying said phase shift to any values between 0 and π in order to adjust said characteristic to correspond to any value G of an input quantity to be displayed.

Claim 14

An analog imager according to claim 11, of the type comprising a plurality of zones arranged in a matrix and intercalated between a first family of p parallel control lines and a second family of q parallel control columns, the lines and the columns being in crossed relation, and overlapping a zone x i y j being defined by the overlapping of a column x i where i is an integer between 1 and q and of a line y j where j is an integer between 1 and p, said lines and columns being connected to suitable sequential excitation means, wherein said excitation means comprise: means for delivering a periodic signal A x of predetermined duration and applied sequentially to the lines, means for generating a periodic signal A x having a same duration as A x but having a phase shift φ with respect to A x , said signal A y being applied to the line y j , and means for causing a value of said phase shift φ to correspond to any value G of an input quantity to be displayed.

Claim 15

An imager according to claim 12, wherein the means for generating the signal A y comprise means for simultaneously generating p signals which excite in parallel p zones of any one column x i .

Claim 16

An imager according to claim 13, wherein said excitation means comprise: an oscillator for delivering a reference signal, a clock for defining sequences of application of the excitation signals, a sequence-generating circuit controlled by said clock to which the reference signal is applied and which delivers sequentially to q outputs a signal A x having a predetermined amplitude and duration, each of the q outputs being connected to one of the q columns of the imager, a circuit for quantizing the input quantity having n quantization levels and receiving in parallel groups of p values of the input quantity to be displayed simultaneously on the p zones of any one column and comprising p groups in parallel each having n outputs, the group of outputs having the index j being intended to carry the quantized value of the input quantity to be displayed on the line y j of the column x i , n phase shifters for receiving said reference signal and delivering n signals which are phase-shifted with respect to the reference signal by n discrete values between 0 and π, said phase-shift values being related to the n quantization levels by the law C (φ) which relates the value of the characteristic C of the material to the phase shift φ between the excitation signals, a chopper circuit to which the n phase-shifted signals are applied in parallel, which is controlled by said sequence generator and delivers simultaneously at n parallel outputs signals A y having a duration equal to that of the signal A x , a switching circuit having n parallel inputs, p groups of n control lines and p parallel outputs, the n inputs being such as to receive the n values of A y carried by the n outputs of the chopper circuit, the p groups of n control lines being connected to the p groups of n lines of the circuit for quantization of the input quantity, each of the p outputs being connected to one of the p lines of the imager.

Claim 17

An imager according to claim 13, wherein said excitation means comprise: an oscillator for delivering a reference signal, a clock for defining the sequences of application of the excitation signals, a sequence-generating circuit controlled by said clock to which the reference signal is applied and which delivers sequentially at q outputs a signal A x having a predetermined amplitude and duration, each of the q outputs being connected to one of the q columns of the imager, p analog phase-shifting circuits for receiving the reference signal and delivering p phase-shifted signals by suitable quantities determined by the law C (φ), p chopper circuits in parallel synchronized by the sequence generator which each receive one of the p phase-shifted signals and deliver at p outputs p signals A y having a duration equal to that of the signal A x each of the p outputs being connected to one of the p lines of the imager.

Claim 18

An imager according to claim 11 wherein said material is a nematic liquid crystal.