GB2023864A - Liquid crystal display device - Google Patents
Liquid crystal display device Download PDFInfo
- Publication number
- GB2023864A GB2023864A GB7921265A GB7921265A GB2023864A GB 2023864 A GB2023864 A GB 2023864A GB 7921265 A GB7921265 A GB 7921265A GB 7921265 A GB7921265 A GB 7921265A GB 2023864 A GB2023864 A GB 2023864A
- Authority
- GB
- United Kingdom
- Prior art keywords
- alignment
- liquid crystal
- plates
- display
- zones
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
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Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/137—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering
- G02F1/139—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering based on orientation effects in which the liquid crystal remains transparent
- G02F1/1396—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering based on orientation effects in which the liquid crystal remains transparent the liquid crystal being selectively controlled between a twisted state and a non-twisted state, e.g. TN-LC cell
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- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- Chemical & Material Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Liquid Crystal (AREA)
- Devices For Indicating Variable Information By Combining Individual Elements (AREA)
Abstract
Between polarizers (1,2) an electro- optic display cell (3, 4, 5, 6) comprises a positive dielectric anisotropy nematic liquid crystal layer 6 having display zones (11) which in the unexecuted state differ from, and thus contrast with, other areas in having 90 DEG optical rotatory power. A field E between associated electrodes 7,8 produces homotropic alignment in zones 11 and destoys the contrast, but some zones 11 may have no electrodes for a permanent display. At zones 11 both cell plates 3, 4 have parallel homogeneous alignment layers (by rubbing or vapour deposition) with mutually orthogonal alignment directions. In the other areas, such directions would be mutually parallel, as shown, or one or both homogeneous alignment layers may be overlaid by homotropic alignment layers (e.g. cathodic sputtering, vapour deposition, or a surfactant). The liquid crystal may contain an optically active additive. <IMAGE>
Description
SPECIFICATION
Passive electro-optic display device
The present invention relates to a passive electrooptic display device comprising two polarizers between which is arranged a display cell comprising two transparent plates between which is imprisoned a liquid crystal having a positive dielectric anisotropy and a nematic order, at least locally, the inner faces of the said plates carrying control electrodes and alignment layers of the molecules of the said liquid crystal.
It is to be noted that one knows display cells, called twisted nematic, disclosed for instance in the U.S.
Patent No. 3.918.796, the principle of operation of which is the following : one takes into account the fact that a layer of nematic liquid crystal the molecules of which are orientated along an axis on one of the plates and along an axis which is perpendicular to the first one on the other plate rotates the plane of polarization of the light through 90 . If crossed polarizers are placed before and behind the cell, only one of the components of the light is absorbed and the cell is transparent. When a tension is applied to the electrodes of the cell, a field is produced which induces a homeotropous structure of the molecules of the liquid crystal. Hence, the plane of polarization does not rotate in the zones where the said field exists, so that the second component of the light is thus absorbed and the said zones are then absorbent.While placing the polarizers so as to be parallel to each other, one obtains a cell having a display which is complementary to that disclosed hereabove, that is to say which is absorbent in the non-activated zones and transparent in the activated zones.
The purpose of the invention is to realize a display device having characteristics which are equivalent to those previously disclosed but permitting, moreover, to simplify the determination of the topology of the electrodes of the cell, to reduce the consumption of energy and to realize zones in which permanent information is displayed, in the same plane as the display segments, without any supplementary operation and without increasing the consumption of the cell.
This purpose is reached owing to the means as claimed.
The drawing shows, by way of example, three embodiments of the invention.
Figures 1 to 3 are partial sectional views of three embodiments of passive electro-optic display devices.
It is to be noted that, in all these figures, the thicknesses of the represented elements have been exaggerated so as to increase the understanding of the drawing.
The passive electro-optic display device represented in Figure 1 comprises two polarizers 1 and 2, the axes of passage al and a2 of which are parallel, between which is arranged a display cell comprising two transparent plates 3 and 4, for instance made of glass, maintained at a distance from each other by a frame 5 to which the said plates are tightly assem
bled, thus providing a room in which a nematic
liquid crystal 6 is imprisoned, having a positive
dielectric anisotropy.
The front plate 3 carries, on its inner face, transpa
rent control electrodes 7, made of SnO2 for instance,
while the rear plate 4 carries, on its inner face, a
control electrode 8, also made of SnO2. The plate 3 is
innerly coated with a homogeneous planar align
ment layer 9, which is itself coated with a homeotro
pous alignment layer 10. This layer 10 is interrupted
opposite the display zones, at places designated by
11 in the drawing, which constitute segments. The
plate 4 is entirely innerly coated with a
homogeneous planar alignment layer 12 the align
ment direction of which is perpendicular to the
alignment direction of the layer 9. A diffuser 13 is
located behind the rear polarizer 2.
In the area of the cell situated outside the display
zones 11, the molecules of the liquid crystal are in
contact on the one hand with the homeotropous
alignment layer 10 of the plate 3 and on the other
hand with the homogeneous planar alignment layer
12 of the plate 4. As is shown by the drawing, the
layer 10 produces a homeotropous alignment of the
molecules of the liquid crystal while the layer 12
produces a homogeneous planar alignment of the
said molecules which are both parallel to the plane
of the cell and perpendicular to the plane of the
drawing. This arrangement does not rotate the
orientation of the plane of polarization of the light that the polarizer 1 allows to pass through.Conse
quently, and since the polarizer 2 is orientated in a
parallel direction to the polarizer 1, only one of the
components of the light is absorbed in the said area which, nevertheless, remains clear,
In the display zones (segments) 11, the molecules of the liquid crystal are in contact with the
homogeneous planar alignment layers 9 and 12.
Since the alignment directions of these two layers are substantially perpendicular to each other, they induce into the liquid crystal a helicoidal structure which rotates the plane of polarization of the light coming from the polarizer 1 through an angle of about 90 . The polarizers 1 and 2 being parallel to each other, it results therefrom that the two components of the light are absorbed, so that the nonactivated zones 11 are completely absorbent and appear in dark.
In the activated display zones, such as the zone 11 situated at the right side of Figure 1, the electric field induces into the liquid crystal a homeotropous structure, that is to say a structure perpendicular to the plane of the cell. Consequently, the plane of
polarization of the light is no more modified in its orientation. Therefore, the activated zones 11 become transparent and are then confused with the surrounding area, also transparent.
The embodiment of Figure 2 differs from that of
Figure 1 by the fact that, outside the display zones
11, the rear plate 4 is also covered with a homeotro
pous alignment layer, designated by 14.
It results from the arrangement as disclosed
hereabove that, in the area situated outside the display zones, the liquid crystal has a homeotropous structure. Consequently, the plane of polarization of the light is not modified and the said area is thus transparent, as in the case of Figure 1. As concerns the operation of the display zones 11, it is identical to that of Figure 1.
The embodiment of Figure 3 differs from that of
Figure 1 by the fact that, on the one hand, the device operates in the transmission mode, the diffuser 13 having been suppressed, and that, on the other hand, the axes of passage a1 and a2 of the polarizers 1 and 2, respectively, are perpendicular to each other. Moreover, in the area situated outside the display zones, the layer of the liquid crystal has a planar homogeneous structure and, hence, does not modify the plane of polarizatin of the component of the light which has passed through the polarizer 1.
Consequently, this component is absorbed by thel polarizer 2. The area situated outside the display zones will thus appear as dark. Opposite the display zones 11, and in the absence of any electric field the alignment layers 9 and 12 induce into the layer of the liquid crystal a helicoidal structure having the property of rotating through about 90 the plane of polarization of the component of the light which has passed through the polarizer 1. Consequently, this component will not be absorbed by the polarizer 2.
The area situated opposite the display zones will thus appear as transparent in the absence of the field
Thus, in the two first embodiments, the display appears in dark on a clear area, which is generally appreciated for the displays which work in the reflection mode while, in the third embodiment, which works in transmission mode, the display appears in clear on a dark area. In these three cases, the control is reversed, the application of the electric field having the effect of "cancelling" or "effacing" the display zones which have to be not visible.
A display in dark on a clear ground is obtained with a device the polarizers of which are parallel to each other while, for a display in clear on a dark ground, the polarizers are perpendicular to each other. The device will operate whatever the relative orientation of the polarizers and of the alignment layers may be. However, if the axes of the polarizers are perpendicular to the alignment direction of one or the other of the planar alignment layers, one will prevent the appearing of interference colors.
It is to be noted that the present device eliminates the usual constraints to which is submitted the determination of the topology of the electrodes. As a matter of fact, where the projection of the pattern of an electrode of the front plate on the rear plate crosses the pattern of an electrode of this rear plate, an electric field is created which tends to orientate the molecules of the liquid crystal according to a homeotropous structure, which structure does not modify the plane of polarization of the light. All the structures disclosed for the area situated outside the display zones having such a behavior, the crossing points do not risk, consequently, to be untimely visible. The realization of the pattern of the nets of the electrodes carried by the two plates is thereby greatly facilitated. Thus, one of the plates could be entirely covered with a conductive layer.This improvement can be considered as an important simplification.
The alignment layers used can be realized diversely:
The homeotropous alignment can be obtained by means of alumina, of magnesium fluoride (see
German Patent Application No. 2330 909 of the firm
SIEMENS) or still of magnesium oxide, which can be deposited in any known way, for instance by cathodic sputtering, by deposition in vapor phase or by evaporation under vacuum, according to an incidence substantially perpendicular to the substrate.
One can also use a surfactant such as, for instance, the lecithin.
As concerns the homogeneous planar alignment, it can be obtained by means of silicium oxide or other, especially according to the techniques exposed by J.L. JANNING in Applied Physics Letters,
Vol.21,1972, pages 173 and following. The planar alignment layers can also be realized by a mere rubbing of the substrate, the direction of this rubbing defining the alignment direction.
It must be understood that "planar" does not mean that the axes of the molecules are exactly parallel to the plane of the cell; likewise, "homeotropous" does not mean that these axes are exactly perpendicular to this plane. The parallelism and the perpendicularity are only limit cases.
It is to be noted that, for instance, for impelling a sense of rotation to the helix such as represented in the display zones 11 at the left side of the several figures of the drawing, one can add to the nematic liquid crystal an optically active compound having the effect of inducing, in the absence of outer constraints, a helicoidal structure. Such a mixture has a local nematic order (See E.B. Priestey, R C A
Review, Vol. 35, March 1974, p. 84 and followings).
At last, it is to be noted that one can provide, in the present device, permanent display zones, that is to say zones of the same construction as the display zones, but without control electrodes, which, consequently, will remain permanently contrasted. Such zones can, for instance, constitute a frame surrounding the whole display zones.
Likewise, the present arrangement can easily be combined with the conventional arrangement in which the segments which have to be displayed must be activated. One could, as a matter of fact, imagine a display cell comprising, in the same space, two display zones, one realized according to the present arrangement and the other one of the twisted nematic type.
Claims (8)
1. Passive electro-optic display device comprising two polarizers between which is arranged a display cell comprising two transparent plates between which is imprisoned a liquid crystal having a positive dielectric anisotropy and a nematic order, at least locally, the inner faces of the said plates carrying control electrodes and alignment layers of the molecules of the said liquid crystal, characterized by the fact that, opposite the display zones, the plates are covered with substantially homogeneous planar alignment layers, such that the alignment direction defined by the alignment layer of the front plate is substantially perpendicular to the alignment direction defined by the alignment layer of the rear plate, thus inducing into the layer of the liquid crystal, in the absence of any electric field, a helicoidal structure, while, in the area situated outside the display zones, the alignment layers of the two plates define alignment directions of the molecules of the liquid crystal such that there exists a plane, perpendicular to the plane of the cell, in which are inscribed the great axes of the molecules of the liquid crystal in the whole thickness of the layer.
2. Device as claimed in claim 1, characterized by the fact that the axes of the two polarizers are perpendicular to the alignment direction induced by one of the alignment layers in the display zones.
3. Device as clamed in claim 2, characterized by the fact that the polarizers are parallel to each other, being both perpendicular to the aligriment direction induced by the same alignment layer.
4. Device as claimed in claim 2, characterized by the fact that the polarizers are perpendicular to each other, being respectively perpendicular to the alignment direction induced by the alignment layers of each ofthe plates.
5. Device as claimed in claim 1, characterized by the fact that, in the area situated outside the display zones, the alignment layer of one of the plates induces a substantially homogeneous planar alignment while the alignment layer of the other plate induces a homeotropous alignment.
6. Device as claimed in claim 1, characterized by the fact that, in the area situated outside the display zones, the alignment layers deposited on the plates induce homogeneous planar alignments, the alignment directions being parallel to each other and to the direction of the alignment layer with which is coated one of the plates in the display zones.
7. Device as claimed in claim 1, characterized by the fact that, in the area situated outside the display zones, the alignment layers deposited on the plates induce homeotropous alignments.
8. A passive electro-optic display device constructed and arranged substantially as herein particularly described with reference to and as illustrated in Figure 1, Figure 2 or Figure 3 of the accompanying drawings.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CH679478A CH620774A5 (en) | 1978-06-22 | 1978-06-22 |
Publications (2)
Publication Number | Publication Date |
---|---|
GB2023864A true GB2023864A (en) | 1980-01-03 |
GB2023864B GB2023864B (en) | 1983-03-16 |
Family
ID=4315129
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB7921265A Expired GB2023864B (en) | 1978-06-22 | 1979-06-19 | Liquid crystal display device |
Country Status (3)
Country | Link |
---|---|
CH (1) | CH620774A5 (en) |
DE (1) | DE2855668A1 (en) |
GB (1) | GB2023864B (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2119110A (en) * | 1979-05-29 | 1983-11-09 | Texas Instruments Inc | Liquid crystal display cell |
GB2121226A (en) * | 1982-04-13 | 1983-12-14 | Canon Kk | Liquid crystal display |
EP0235634A1 (en) * | 1986-02-27 | 1987-09-09 | Asulab S.A. | Display cell |
EP0485017A2 (en) * | 1990-11-07 | 1992-05-13 | Koninklijke Philips Electronics N.V. | Active matrix liquid crystal display device with dark matrix interpixel areas |
EP0795774A2 (en) * | 1996-03-11 | 1997-09-17 | Canon Kabushiki Kaisha | Liquid crystal device and process for production thereof |
US6897915B1 (en) * | 2000-09-27 | 2005-05-24 | Kent State University | Non-lithographic photo-induced patterning of polymers from liquid crystal solvents with spatially modulated director fields |
-
1978
- 1978-06-22 CH CH679478A patent/CH620774A5/fr not_active IP Right Cessation
- 1978-12-20 DE DE19782855668 patent/DE2855668A1/en not_active Withdrawn
-
1979
- 1979-06-19 GB GB7921265A patent/GB2023864B/en not_active Expired
Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2119110A (en) * | 1979-05-29 | 1983-11-09 | Texas Instruments Inc | Liquid crystal display cell |
GB2121226A (en) * | 1982-04-13 | 1983-12-14 | Canon Kk | Liquid crystal display |
EP0235634A1 (en) * | 1986-02-27 | 1987-09-09 | Asulab S.A. | Display cell |
EP0485017A2 (en) * | 1990-11-07 | 1992-05-13 | Koninklijke Philips Electronics N.V. | Active matrix liquid crystal display device with dark matrix interpixel areas |
EP0485017A3 (en) * | 1990-11-07 | 1992-10-21 | N.V. Philips' Gloeilampenfabrieken | Active matrix liquid crystal display device with dark matrix interpixel areas |
EP0795774A2 (en) * | 1996-03-11 | 1997-09-17 | Canon Kabushiki Kaisha | Liquid crystal device and process for production thereof |
EP0795774A3 (en) * | 1996-03-11 | 1998-03-25 | Canon Kabushiki Kaisha | Liquid crystal device and process for production thereof |
US6320639B1 (en) | 1996-03-11 | 2001-11-20 | Canon Kabushiki Kaisha | Liquid crystal device and process for production thereof |
US6897915B1 (en) * | 2000-09-27 | 2005-05-24 | Kent State University | Non-lithographic photo-induced patterning of polymers from liquid crystal solvents with spatially modulated director fields |
US7372480B1 (en) | 2000-09-27 | 2008-05-13 | Kent State University | Non-lithographic photo-induced patterning of polymers from liquid crystal solvents with spatially modulated director fields |
Also Published As
Publication number | Publication date |
---|---|
GB2023864B (en) | 1983-03-16 |
DE2855668A1 (en) | 1980-01-10 |
CH620774A5 (en) | 1980-12-15 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
PCNP | Patent ceased through non-payment of renewal fee |