GB2208559A

GB2208559A - Liquid crystal devices

Info

Publication number: GB2208559A
Application number: GB8719078A
Authority: GB
Inventors: Carolyn Bowry
Original assignee: General Electric Co PLC
Current assignee: General Electric Co PLC
Priority date: 1987-08-12
Filing date: 1987-08-12
Publication date: 1989-04-05
Anticipated expiration: 2007-08-12
Also published as: DE3886192D1; EP0327627B1; GB8719078D0; WO1989001680A1; JPH02500936A; GB2208559B; DE3886192T2; EP0327627A1

Abstract

In a method of driving a matrix of ferroelectric liquid crystal devices in a TDM mode, each strobing signal comprises first and second pulses (20, 21) of opposite polarities and of different amplitudes, together with a dc voltage (26) which is applied from the end of the second pulse to the beginning of the first pulse of the next strobing signal on the same strobe line to cancel the dc level which would be caused by the unequal pulses. Data ON signals applied selectively to data lines of the matrix comprise two consecutive pulses (22, 23) of opposite polarities. Data OFF signals (24, 25) may be the inverse of the data ON signals or may comprise a constant dc level. The combination of the two pulses with a dc level to form each strobing signal means that only two strobe pulse time slots per frame are required for addressing each strobe line, as compared with the conventional systems in which four time slots per frame are required.

Description

Ferroelectnc Liquid Crystal Devices This invention relates to ferroelectric liquid crystal (FLC) devices, and particularly to a method and apparatus for driving the liquid crystal elements of such devices.

A ferroelectric liquid crystal has a permanent electric dipole which interacts with the applied electric field. Hence, ferroelectric liquid crystals exhibit fast response times, which make them suitable for use in display, switching and information processing applications. An example of an FLC device is described in a paper by N. A. Clarke et al, entitled "Submicrosecond bistable electro-optic switching in liquid crystals" in Appl. Phys. Lett. Volume 36, 1980, pp 899-901.

The stimulus to which an FLC device responds is a dc field, and its response is a function of the applied voltage (V) and the length of time (t) for which it is applied. The response is not a linear function of V x t, and there may be a voltage level at which, irrespective of the length of time for which the voltage is applied, switching of the device will not occur. There may also be a length of time of application of the voltage which will be too shot for switching to occur, irrespective of the magnitude of the voltage.

An FLC device which can be multiplexed needs to have at least two different states (called latched states) which the liquid crystal can adopt in the absence of an applied field. These can be the same states as the states (called switched states) obtained when a field of either polarity is applied, or they can be different states.

The liquid crystal can change from one switched state to another switched state when a field is applied thereto, without necessarily going to a latched state when the field is removed.

For a given time interval, the voltage at which the liquid crystal switches from one state to the other by 10% is called the switching threshold at 10 % switching (Tsio). The voltage at which the liquid crystal switches fully from one state to the other state is called the switching threshold at 100% switching (T5100). The voltage at which the liquid crystal will go fully into one of the latched states when the field is removed is called the latching threshold at 100% latching (TL1oo). The voltage at which the liquid crystal no longer goes into either of two different states when the field is removed is called the latching threshold at 0% latching (TLo).

A ferroelectric liquid crystal element is switched to one state by the application of a voltage of a given polarity across its electrodes, and is switched to the other state by the application thereto of a voltage of the opposite polarity. It is essential that an overall dc voltage shall not be applied across such an element for an appreciable period, so that the elements remain charge-balanced, thereby avoiding decomposition of the liquid crystal material.

Pulsed operation of such elements has therefore been effected, with a pulse of one polarity being immediately followed by a pulse of the other polarity, so that there is no resultant dc polarisation.

The liquid crystal elements are commonly arranged in matrix formation and are operated selectively by energising relevant row and column lines. Time-division multiplexing is effected by applying pulses cyclically to the row (strobe) lines in sequence and by applying pulses, in synchronism therewith, to selected column (data) lines.

An example of an FLC display driving system is disclosed in an article by T. Harada, M. Taguchi, K. Iwasa and M. Kai in SID 85 Digest, p 131 et seq. This system uses four pulses per refresh cdc , and can therefore be classified as a 4 time slot system. For a 625-line display at video frame rates this would require a 16yus response of the crystal elements.

It is an object of the present invention to provide a method and apparatus for driving the elements of an FLC device matrix, in which only two strobe pulse time slots per frame are required.

According to one aspect of the invention there is provided a method of driving a ferroelectric liquid crystal device matrix in a time-division multiplex mode, comprising applying strobing signals cyclically to strobe lines coupled to two-state liquid crystal elements of the display and applying data signals selectively to data lines coupled to the elements, wherein each strobing signal comprises a first pulse of one polarity followed by a second pulse of the opposite polarity and of different amplitude from the first pulse, and a dc voltage which is effective during a period between the end of the second pulse of a strobing signal and the beginning of the first pulse

of the next strobing sighalLto substantially cancel a dc voltage level resulting from the difference between the amplitudes of the first and second pulses and which will not switch the liquid crystal elements during this period, wherein the data signals comprise a first data signal operative in combination with the strobing signal to set a selected liquid crystal element in a first one of its states, and a second data signal operative in combination with the strobing signal to set the selected liquid crystal element in the other of its states, and wherein one or each of the first and second data signals comprises at least two consecutive pulses of opposite polarities and of substantially equal amplitudes.

According to another aspect of the invention there is provided apparatus for driving a ferroelectric liquid crystal device matrix in a time-division multiplex mode, comprising means to apply strobing signals cyclically to strobe lines coupled to two-state liquid crystal elements of the display; and means to apply data signals selectively to data lines coupled to the elements, wherein each strobing signal comprises a first pulse of one polarity followed by a second pulse of the opposite polarity and of different amplitude from the first pulse, and a dc voltage which is effective during a Deriod between the end of the second pulse of a said strobina sianal

and the beginning ot tne tirst pulse of the next strobing signalLto substantialb cancel a dc voltage level resulting from the difference between the amplitudes of the first and second pulses, which dc voltage will not switch the liquid crystal elements during said period, wherein the data signals comprise a first data signal operative in combination with the sot robing signal to set a selected liquid crystal element in a first one of its states, and a second data signal operative in combination with the strobing signal to set the selected liquid crystal element in the other of its states, and wherein one or each of the first and second data signals comprises at least two consecutive pulses of opposite polarities and of substantially equal amplitudes.

Embodiments of the invention will now be described, by way of example, with reference to the accompanying drawings, wherein Figure 1 is a block schematic diagram of an FLC device drive system; Figure 2 illustrates strobing and data pulses occurring in a known 4-slot drive system; Figure 3 illustrates strobing and data pulses occurring in one embodiment of a 2-slot drive system according to the present invention; and Figures 4 to 10 illustrate strobing and data pulses occurring in second to eighth embodiments, respectively, of the invention.

Referring to Figure 1, a ferroelectric liquid crystal device, such as display, comprises a matrix of ferroelectric liquid crystal elements 1 coupled to row (strobe) and column (data) lines 2 and 3, respectively. For the sake of example, nine of such elements coupled to three strobe lines and three data lines are shown, but there may be any desired number of elements and corresponding lines. A strobe pulse generator 4 is coupled to the strobe lines, and a data pulse generator 5 is coupled to the data lines. The strobe pulse generator continuously applies strobing signals to the strobe lines 2 in sequence, and the data pulse generator applies data signals to the data lines 3, in synchronism with the pulsing of the strobe lines, to set the corresponding element 1 in the required state.

Figure 2 shows waveforms which would be applied to the lines 2 and 3 in a known 4-slot drive system. In Figure 2(a), a strobing signal comprises a positive pulse 6 followed by a negative pulse 7 and, later during the same frame period, a negative pulse 8 followed by a positive pulse 9. All of these pulses are of the same amplitude VR, and there is therefore no residual dc level. The data signal may comprise a pulse train 10 (Figure 2(b)) for setting the addressed element in the ON state or a pulse train 11 (Figure 2(c)) for setting it in the OFF state, where ON and OFF merely indicate two different states. The pulse train 10 comprises positive and negative pulses 12 and 13, respectively, coincident with the pulses 6 and 7, and positive and negative pulses 14 and 15, respectively, coincident with the pulses 8 and 9. The pulses 12, 13, 14 and 15 are all of amplitude Vd.The pulse train 11 comprises pulses 16, 17, 18 and 19 of the same amplitude as the pulses 12, 13, 14 and 15 but of opposite polarity thereto.

The data pulses are also applied via the lines 3 to those liquid crystal elements 1 which are not being addressed by the strobing signal. This leads to crosstalk, which is inherent in any multiplexing scheme. In order to reduce visible crosstalk effects there are certain conditions which a multiplexing scheme must satisfy, as follows 1. The data voltage Vd must not be large enough to switch the liquid crystal. Switching the liquid crystal will reduce the contrast of the device.

i.e. Vd c Tio dTSo 2. The strobe voltage plus the data voltage (Vs + Vd) must be large enough to switch and latch the liquid crystal so that the cerecct spite (Ft cr OFF) of tk Wernent is i.e. V5 + Vd ATL100 3. The strobe voltage minus the data voltage (Vs - Vd) can switch the liquid crystal since it occcurs only once in every frame scan. However, it must not latch the liquid crystal, since this will reverse the data required, nor must it unlatch the liquid crystal from the original state.

i.e. VS - VdTLo Figure 3 shows waveforms provided in a first embodiment of the present invention. The strobing signal (Figure 3(a)) comprises a positive pulse 20 of amplitude V1, followed by a negative pulse 21 of amplitude V2, which is less than V1. This is the only pair of strobe pulses occurring during a frame period. The data signal comprises either a positive pulse 22 followed by a negative pulse 23 (Figure 3(b)) or a negative pulse 24 followed by a positive pulse 25, depending upon the data to be written. The pulses 22-25 are all of amplitude Vd (not necessarily equal to Vd of Figure 2).

Since the strobe pulses 20 and 21 are of different amplitudes, there would be a residual dc level applied to the addressed liquid crystal elements and, as stated above, this is undesirable. In the present invention, therefore, a small dc voltage 26 is applied to the strobe line between the end of the pulse 21 and the beginning of the pulse 20 of the next frame period.

Figure 3(d) shows the voltage appearing across the addressed liquid crystal element as a result of the strobe signal and the data signal of Figure 3(b), whilst Figure 3(e) similarly shows the resultant, but for the data signal of Figure 3(c). For the system to operate correctly, the following conditions should be satisfied as nearly as possible. The system can operate without their being satisfied, but there is then a loss of contrast.

V1 - VdTL1O0 V2 - VdTLo V2 + Vd7TL100 Vd ÇTio It will be seen that each strobe and data signal comprises only two pulses, so that the liquid crytal elements are addressed in only two time slots during a frame period, as compared to four time slots for the known system. This halves the requirement as regards the speed of switching of the liquid crystal elements.

Figure 4 shows an alternative arrangement of data pulses.

The strobe pulses (Figure 4 (a)) are similar to those in Figure 3(a), and the data OFF pulses (Figure 4 (c)) are similar to those in Figure 3(c). In this case, however, the data ON signal (Figure 3(b)) comprises merely a zero voltage level. The various voltages must then satisfy the following conditions.

V1 > To100 V24 TLo V2 + Vd?TL100 Vd < TSLo Figure 5 shows another alternative arrangement of data pulses. In this case the data ON pulses (Figures 5(b)) are similar to the data ON pulses of Figure 3(b), but the data OFF signal (Figure (c)) is merely a zero voltage level. The voltages must then satisfy the following conditions.

V1 - Vd?TL100 V2 - Vd < TLo V2 > TL100 VdT5o In each of the drive arrangements described above, the duration of the element-addressing time can be shortened by reducing the period (t) of either of the strobe pulses and by increasing the voltage (V) of each reduced-length pulse, taking into account the criteria mentioned hereinbefore.

Figure 6 shows one such configuration of strobe and data pulses. In Figure 6(a), a first strobe pulse 27 has an amplitude V1 and a period t1, whereas a second strobe pulse 28 has a period t2 which is shorter than tl, and an amplitude V2 which is larger than V1.

It will be apparent that V1xtl+V2xt2+Vdcxt3 must be substantially zero, where t3 is the length of the period between the end of the pulse 28 and the beginning of the next pulse 27.

The data ON signal, shown in Figure 6(b), comprises a positive-going pulse 29 of amplitude Yd1 and duration t1, and a negative-going pulse 30 of amplitude Vd2 and duration t2. The data OFF signal, shown in Figure 6(c), is the inverse of Figure 6(b). In order to avoid subjecting the liquid crystal elements to an overall dc level due to the application of the data pulses, Vd1xtl must be equal to Vd2xt2 for each data signal.

The voltages and periods of the strobe and data pulses are preferably selected to obtain optimum working of the liquid crystal elements. The optimum arrangement for the strobe pulses is achieved when V1 = V2 and t1 and t2 are adjusted to suit the liquid crystal elements. Any discrepancy between V1xtl and V2xt2 is then accounted for by selecting the correct value of the dc voltage 26.

Figure 7 shows an alternative pulse configuration in which the strobe pulses are the same as in Figure 6, but the first data pulse 31 is of different period from the first strobe pulse 27. The pulse 31 begins later than the beginning of the strobe pulse 27, but the pulses end simultaneously. Again, the data OFF signal of Figure 7(c) is the inverse of the data ON signal of Figure 7(b). In this case Vd3xt4 must equal Vd2xt2, where Vd3 and t4 are the amplitude and the period, respectively, of the pulse 31.

Figure 8 shows another pulse configuration in which the strobe pulses are the same as in Figure 6. In this case, however, the first data pulse 32 is the same width as the first strobe pulse 27, but the second data pulse 33 is longer than the second strobe pulse 28. The pulse 33 may alternatively be shorter than the pulse 28.

For dc cancellation, Vd4xt5 must equal Vdlxtl, where Vd4 and t5 are the voltage and period, respectively, of the pulse 33.

Figure 9 shows another alternative configuration, in which the first data pulse 34 begins simultaneously with the first strobe pulse, but the data pulse is shorter than the strobe pulse. The second data pulse 35 is the same length as the second strobe pulse.

In each of the drive arrangements described herein, the performance of the FLC device may be improved by including a period of zero voltage between the positive and negative strobe and/or data pulses and/or before and/or after any of those pulses. The zero voltage period can be of any suitable length and should be selected to suit the particular liquid crystal elements. Such a zero voltage level may be as shown at 36 in the data signal in Figure 9 or as shown in Figure 10, wherein the first and second strobe pulses 37 and 38, respectively, are separated by a period 39 of zero voltage.

In every case, the pulse voltages and lengths will be adjusted to suit the particular type of liquid crystal elements and the particular combination of strobing and data signals. In any of the configurations described above, the polarity of both the strobe pulses and the data pulses may be reversed.

In each of the drive arrangements of the present invention a further improvement may be effected by superimposing an ac voltage at, say, 10-100kHz on the pulses. This helps to sharpen the switching thresholds and may also improve the contrast ratio of the data ON and OFF states during multiplexing.

Claims

1. A method of driving a ferroelectric liquid crystal device matrix in a time-division multiplex mode, comprising applying strobing signals cyclically to strobe lines coupled to two-state liquid crystal elements of the display and applying data signals selectively to data lines coupled to the elements, wherein each strobing signal comprises a first pulse of one polarity followed by a second pulse of the opposite polarity and of different amplitude from the first pulse, and a dc voltage which is effective during a period between the end of the second pulse of a said strobing siqnal and the beginning of the first

pulse of the next sot robing signallto substantially cancel a dc voltage level resulting from the difference between the amplitudes of the first and second pulses and which dc voltage will not switch the liquid crystal elements during said period, wherein the data signals comprise a first data signal operative in combination with the strobing signal to set a selected liquid crystal element in a first one of its states, and a second data signal operative in combination with the strobing signal to set the selected liquid crystal element in the other of its states, and wherein one or each of the first and second data signals comprises two consecutive pulses of opposite polarities.

2. A method as claimed in Claim 1, wherein said first data signal comprises two consecutive pulses of mutually opposite polarities and of subtantially equal amplitudes, and said second data signal comprises two consecutive pulses of opposite polarities to the pulses of said first data signal and of substantially equal amplitudes.

3. A method as claimed in Claim 1, wherein said first data signal comprises a constant dc level, and said second data signal comprises two consecutive pulses of polarities opposite to those of the pulses of the strobing signal.

4. A method as claimed in Claim 1, wherein said first data signal comprises two consecutive pulses of the same polarities as the pulses of the strobing signal, and said second data signal comprises a constant dc level.

5. A method as claimed in Claim 1, wherein said first and second pulses of the strobing signal are of mutually different time durations.

6. A method as claimed in Claim 1, wherein each first and second data signal comprises two pulses of mutually opposite polarities and of mutually different time durations.

7. A method as claimed in Claim 1, wherein the strobe pulse and/or each first and second data signal comprises two pulses of mutually opposite polarities separated by a period of zero voltage.

8. A method as claimed in any preceding claim, wherein a relatively high-frequency ac voltage is superimposed on the strobing signals and/or the data signals.

9. A method of driving a ferroelectric liquid display matrix, substantially as hereinbefore described with reference to Figures 1 and 3-10 of the accompanying drawings.

10. Apparatus for driving a ferroelectric liquid crystal device matrix in a time-division multiplex mode, comprising means to apply strobing signals cyclically to strobe lines coupled to two-state liquid crystal elements of the display; and means to apply data signals selectively to data lines coupled to the elements, wherein each strobing signal comprises a first pulse of one polarity followed by a second pulse of the opposite polarity and of different amplitude from the first pulse, and a dc voltage which is effective during a Deriod between the end of the second Dulse of a said strobine sianal

and the beginning of the first pulse of the next strobing signalLto substantially cancel a dc voltage level resulting from the difference between the amplitudes of the first and second pulses which dc voltage will not switch the liquid crystal elements during said period, wherein the data signals comprise a first data signal operative in combination with the strobing signal to set a selected liquid crystal element in a first one of its states, and a second signal operative in combination with the strobing signal to set the selected liquid crystal element in the other of its states, and wherein one or each of the first and second data signals comprises at least two consecutive pulses of opposite polarities and of substantially equal amplitudes.