Co-ordinate addressing of smectic display cells

• US 4,419,664 A
• Filed: 12/23/1980
• Issued: 12/06/1983
• Est. Priority Date: 01/16/1980
• Status: Expired due to Term

• Current Assignee: Nortel Networks Limited (Nortel Networks Corporation)
• Original Assignee: International Standard Electric Corporation (ITT, Inc.)
• Inventors: Coates, David, Crossland, William A., Ayliffe, Peter J.
• Primary Examiner(s): Curtis, Marshall M.
• Application Number:
  US06/219,559
• Time in Patent Office: 1,078 Days
• Field of Search: 340/784, 340/765, 340/805, 350/333, 350/350 S, 350/330
• US Class Current: 345/94
• CPC Class Codes: G02F 1/13306 Circuit arrangements or driving methods for the control of single liquid crystal cells G02F1/132, G02F1/133382 take precedence
• CPC Class Codes: G02F 1/13781 using smectic liquid crystals G02F1/141 takes precedence
• CPC Class Codes: G09G 2300/0486 Cholesteric liquid crystals, including chiral-nematic liquid crystals, with transitions between focal conic, planar, and homeotropic states
• CPC Class Codes: G09G 2310/06 Details of flat display driving waveforms
• CPC Class Codes: G09G 3/2018 by time modulation using two or more time intervals
• CPC Class Codes: G09G 3/3629 using liquid crystals having memory effects, e.g. ferroelectric liquid crystals

Abstract

A co-ordinate matrix addressing system is used to address a liquid crystal display cell containing a positive dielectric anisotropy smectic material. For this purpose one or more direct voltage pulses are applied across selected elemental volumes of the display to convert them from a focal-conic scattering state to a homeotropically aligned state. Prior to this all elements are electrically driven into the turbulent scattering state which relaxes into the focal-conic scattering state upon removal of the driving field. The driving field may also take the form of direct voltage pulses.

Claims

1. A method of co-ordinate matrix addressing in internally electroded liquid crystal display cell which has a layer of smectic material sandwiched between two electroded plates crossing over a second array on the other plate defining therebetween a set of elemental volumes of liquid crystal each element of which is defined by the thickness of the liquid crystal layer and the area of overlap where a member of the first array crosses over a member of the second, wherein the smectic material exhibits positive dielectric anisotropy and has an electrical conductivity large enough for dynamic scattering to be capable of being produced by the application of an electric field across the layer, and wherein at least one of the plates is transparent and its surface in contact with the liquid crystal layer is such that, when the layer is taken into a smectic phase from less-ordered non-smectic phase by cooling in the absence of an applied field, those molecules of the layer adjacent said surface are caused to assume substantially homeotropic alignment, which method includes the steps of applying an electric potential between the members of the first array and those of the second in such a way as to cause dynamic scattering in said set of elemental volumes, converting the dynamic scattering in the set of elemental volumes into static focal-conic scattering by removal of said potential, and selectively restoring individual elemental volumes to non-scattering substantially homeotropically aligned state by the concurrent application of direct voltage signals of predetermined durations and magnitudes to selected electrodes in said arrays such that not more than ten direct voltage resultant switching pulses are applied between the two electrodes defining any elemental volume.

2. A method as claimed in claim 1 wherein each said selective restoration of an individual elemental volume to a non-scattering state is effected using a plurality of switching pulses providing a potential difference across the elemental volume that is not in the same direction for all of said switching pulses.

3. A method as claimed in claim 2 wherein said plurality of switching pulses is such as to alternate the direction of the potential difference.

4. A method as claimed in claim 2 wherein after a switching pulse is applied to a selected elemental volume the scan is completed before the next switching pulse is applied to that elemental volume.

5. A method as claimed in claim 3 wherein in any scan of the matrix switching pulses are applied in pairs to the selected elemental volumes such that each is subjected to a bipolar pulse potential difference waveform.

6. A method as claimed in claim 2, 3, 4 or 5 wherein a grey-scale is provided by applying fewer switching pulses to some of the selected elemental volumes than are applied to others.

7. A method as claimed in claim 1, 2, 3, 4 or 5 wherein the step of selectively restoring individual elemental volumes to a non-scattering state is effected by holding all the members of the first array of electrodes at a particular first direct voltage level except while they are being strobed in turn with a second direct voltage level V_S from the first level, while at the same time the members of the second array are individually and selectively switched between third and fourth direct voltage levels respectively +V_D and -V_D from the first voltage level, and wherein V_S ≧

2V_D.

8. A method as claimed in claim 7 wherein V_S <

3 V_D.

9. A method as claimed in claim 7 wherein V_S =2 V_D.

10. A method as claimed in claim 7 wherein V_S =3 V_D.

11. A method as claimed in claim 1, 2, 3, 4 or 5 wherein the electric potential applied between the members of the first array of electrodes and those of the second to cause dynamic scattering takes the form of a single direct voltage pulse.

12. A method as claimed in claim 1, 2, 3, 4 or 5 wherein the electric potential applied between the members of the first array of electrodes and those of the second to cause dynamic scattering takes the form of a bipolar pulse.

13. A method as claimed in claim 11 wherein the step of selectively restoring individual elemental volumes to a non-scattering state is interrupted one or more times by the insertion of a refresh pulse of shorter duration than said pulse used to cause dynamic scattering which refresh pulse is long enough to restore the unselected elemental volumes to substantially the same scattering state they possessed prior to commencement of the selective restoration step, but is not so long as to restore the selected elemental volumes.

14. A method as claimed in claim 1 wherein the smectic material is a smectic A material.