WO1995009379A1 - Retardation layer having a dispersion adapted to the active liquid-crystalline cell - Google Patents
Retardation layer having a dispersion adapted to the active liquid-crystalline cell Download PDFInfo
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- WO1995009379A1 WO1995009379A1 PCT/EP1994/003246 EP9403246W WO9509379A1 WO 1995009379 A1 WO1995009379 A1 WO 1995009379A1 EP 9403246 W EP9403246 W EP 9403246W WO 9509379 A1 WO9509379 A1 WO 9509379A1
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- C07D303/00—Compounds containing three-membered rings having one oxygen atom as the only ring hetero atom
- C07D303/02—Compounds containing oxirane rings
- C07D303/12—Compounds containing oxirane rings with hydrocarbon radicals, substituted by singly or doubly bound oxygen atoms
- C07D303/18—Compounds containing oxirane rings with hydrocarbon radicals, substituted by singly or doubly bound oxygen atoms by etherified hydroxyl radicals
- C07D303/20—Ethers with hydroxy compounds containing no oxirane rings
- C07D303/22—Ethers with hydroxy compounds containing no oxirane rings with monohydroxy compounds
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- 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
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1347—Arrangement of liquid crystal layers or cells in which the final condition of one light beam is achieved by the addition of the effects of two or more layers or cells
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- C07C225/22—Compounds containing amino groups and doubly—bound oxygen atoms bound to the same carbon skeleton, at least one of the doubly—bound oxygen atoms not being part of a —CHO group, e.g. amino ketones having amino groups bound to carbon atoms of six-membered aromatic rings of the carbon skeleton
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- C08G59/00—Polycondensates containing more than one epoxy group per molecule; Macromolecules obtained by polymerising compounds containing more than one epoxy group per molecule using curing agents or catalysts which react with the epoxy groups
- C08G59/18—Macromolecules obtained by polymerising compounds containing more than one epoxy group per molecule using curing agents or catalysts which react with the epoxy groups ; e.g. general methods of curing
- C08G59/20—Macromolecules obtained by polymerising compounds containing more than one epoxy group per molecule using curing agents or catalysts which react with the epoxy groups ; e.g. general methods of curing characterised by the epoxy compounds used
- C08G59/22—Di-epoxy compounds
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- C09K19/00—Liquid crystal materials
- C09K19/04—Liquid crystal materials characterised by the chemical structure of the liquid crystal components, e.g. by a specific unit
- C09K19/06—Non-steroidal liquid crystal compounds
- C09K19/08—Non-steroidal liquid crystal compounds containing at least two non-condensed rings
- C09K19/10—Non-steroidal liquid crystal compounds containing at least two non-condensed rings containing at least two benzene rings
- C09K19/22—Non-steroidal liquid crystal compounds containing at least two non-condensed rings containing at least two benzene rings linked by a chain containing carbon and nitrogen atoms as chain links, e.g. Schiff bases
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- C09K19/00—Liquid crystal materials
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- C09K19/06—Non-steroidal liquid crystal compounds
- C09K19/08—Non-steroidal liquid crystal compounds containing at least two non-condensed rings
- C09K19/10—Non-steroidal liquid crystal compounds containing at least two non-condensed rings containing at least two benzene rings
- C09K19/28—Non-steroidal liquid crystal compounds containing at least two non-condensed rings containing at least two benzene rings linked by a chain containing carbon and sulfur atoms as chain links, e.g. thioesters
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- C09K19/00—Liquid crystal materials
- C09K19/04—Liquid crystal materials characterised by the chemical structure of the liquid crystal components, e.g. by a specific unit
- C09K19/06—Non-steroidal liquid crystal compounds
- C09K19/08—Non-steroidal liquid crystal compounds containing at least two non-condensed rings
- C09K19/30—Non-steroidal liquid crystal compounds containing at least two non-condensed rings containing saturated or unsaturated non-aromatic rings, e.g. cyclohexane rings
- C09K19/3001—Cyclohexane rings
- C09K19/3086—Cyclohexane rings in which at least two rings are linked by a chain containing nitrogen atoms
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- C09K19/38—Polymers
- C09K19/3833—Polymers with mesogenic groups in the side chain
- C09K19/3876—Polyoxyalkylene polymers
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- C09K19/00—Liquid crystal materials
- C09K19/52—Liquid crystal materials characterised by components which are not liquid crystals, e.g. additives with special physical aspect: solvents, solid particles
- C09K19/60—Pleochroic dyes
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B5/00—Optical elements other than lenses
- G02B5/30—Polarising elements
- G02B5/3016—Polarising elements involving passive liquid crystal elements
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- 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
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1335—Structural association of cells with optical devices, e.g. polarisers or reflectors
- G02F1/13363—Birefringent elements, e.g. for optical compensation
- G02F1/133636—Birefringent elements, e.g. for optical compensation with twisted orientation, e.g. comprising helically oriented LC-molecules or a plurality of twisted birefringent sublayers
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- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/24—Record carriers characterised by shape, structure or physical properties, or by the selection of the material
- G11B7/241—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material
- G11B7/242—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers
- G11B7/244—Record carriers characterised by shape, structure or physical properties, or by the selection of the material characterised by the selection of the material of recording layers comprising organic materials only
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- C07C2601/00—Systems containing only non-condensed rings
- C07C2601/06—Systems containing only non-condensed rings with a five-membered ring
- C07C2601/10—Systems containing only non-condensed rings with a five-membered ring the ring being unsaturated
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- C09K2323/00—Functional layers of liquid crystal optical display excluding electroactive liquid crystal layer characterised by chemical composition
- C09K2323/06—Substrate layer characterised by chemical composition
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- 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
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1335—Structural association of cells with optical devices, e.g. polarisers or reflectors
- G02F1/13363—Birefringent elements, e.g. for optical compensation
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- 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
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1335—Structural association of cells with optical devices, e.g. polarisers or reflectors
- G02F1/13363—Birefringent elements, e.g. for optical compensation
- G02F1/133637—Birefringent elements, e.g. for optical compensation characterised by the wavelength dispersion
Definitions
- the invention is in the field of retardation layers comprising high- molecular weight liquid-crystalline material. Such retardation layers are used in displays.
- Figure 1 is a schematic depiction of the construction of a display.
- Figure 1 shows a cross-section of a display comprising an active twisted layer (4), the active cell, which can be switched on and off by means of transparent electrodes (6), and a retardation layer (3), with substrates (2) disposed on either side of the two layers (3) and (4).
- substrates (2) disposed on either side of the two layers (3) and (4).
- polarisers (1) At the outer sides of the two outermost substrates there are polarisers (1), and underneath the polariser situated under the active twisted layer is positioned a mirror (5).
- the mirror can be omitted in some displays.
- the invention is directed in particular to the retardation layer (3) of a display.
- Retardation layers serve to compensate for the undesirable birefringence effect that occurs in the active cell in the display.
- the retardation layer use may be made of a twisted nematic layer composed of low-molecular weight liquid-crystalline material such as is described in, e.g., Kirk Othmer's Encyclopedia of Technology, 3rd ed. (New York: Wiley & Sons) Vol. 7, p. 728.
- low-molecular weight liquid-crystalline material gives good compensation when used, it is attended with the drawback of being low- viscous. For that reason, the low-molecular weight material is sealed between inflexible substrates by means of spacers in order to attain a twisted, form-retaining structure. In other words, a closed, rigid cell has to be made.
- birefringent films e.g., a film of drawn polymer such as a birefringent polycarbonate film.
- a birefringent polycarbonate film is described in Jap. J. Appl . Physics, Vol. 30, No. 4 (April 1991), 682-686.
- birefringent polycarbonate films By using birefringent polycarbonate films a liquid-crystalline display of reduced thickness and weight may be obtained.
- said birefringent polycarbonate films fail to provide optimum contrast. The reason for this poor contrast is as follows:
- retardation layers serve to compensate for the undesirable birefringence effect that occurs in the active cell of a display.
- This birefringence effect depends on the retardation value, the angle of twist, and the direction of twist of the layer of liquid- crystalline molecules in the active cell of the display.
- the retardation of a birefringent layer is defined as the product of the birefringence value ( ⁇ ) and the layer thickness.
- ⁇ the birefringence value
- the birefringence effect of the active cell of the display can be completely compensated for by using a retardation layer that has equal retardation, and an equal as well as an opposite angle of rotation compared with the active cell. For full compensation these conditions should apply for the entire visible part of the wavelength spectrum. This requirement can only be realised if the dependence of the birefringence on the wavelength, also known as the dispersion, of the material of the retardation layer is equal to that of the LC material used in the active cell of the display.
- birefringent polycarbonate films This is not the case for birefringent polycarbonate films.
- the dispersion of birefringent polycarbonate films is lower than liquid crystalline active cells which are co rnercially used. Therefore, their retardation can only be set (by setting the layer thickness) to match the retardation of the active cell at 550 nm. As a consequence, over the rest of the visible wavelength area the retardation fails to match that of the active cell of the display, especially in the wavelength area of 400-550 nm the dispersion appears to be too low. This results in a less than optimal contrast.
- a retardation layer of high-molecular material which has a retardation virtually matching that of the active cell over the whole visible wavelength area.
- the invention is directed to a retardation layer for a liquid-crystalline display comprising high-molecular weight liquid- crystalline material, wherein the dispersion has been adapted to that of the active liquid-crystalline cell by varying the mesogenic groups of the high-molecular weight liquid-crystalline material, so that the difference in dispersion between the active cell and the retardation layer in the wavelength area of 400-800 nm is not more than 0.1, preferrabley not more than 0.03.
- high-molecular weight liquid-crystalline material are meant: relatively low-molecular weight liquid-crystalline polymers, oligomers, and liquid-crystalline glasses.
- the molecular weight for liquid-crystalline glasses and oligomers varies from 1000 to 4000, for liquid-crystalline polymers it varies 1000 to 20000.
- High-molecular weight liquid-crystalline material has a higher mechanical strength than low-molecular weight liquid-crystalline material. Therefore, it is not necessary to seal the liquid-crystalline material in a rigid cell. Because liquid-crystalline material is used, and the mesogenic groups of liquid-crystalline material can easily be varied, it is possible to obtain a retardation layer which has approximately the same dispersion as that of the active cell.
- the dispersion is defined here as the retardation (or the birefringence) at a certain wavelength divided by the retardation (or the birefringence) at 550 nm.
- mesogenic groups By using mesogenic groups with large conjugated systems the dispersion of liquid-crystalline material is increased, whereas smaller conjugated systems lower the dispersity, especially in the wavelength area of 400-550 nm.
- mesogenic groups have the following general formula: - (CH 2 ) m - 0 - ⁇ .- (Q) n ⁇ 2 -Ri
- the mesogenic group has a large conjugated system.
- the conjugation is decreased.
- the conjugation can be further decreased by using -0-R* or R* for the R ⁇ end group of the mesogenic group.
- the dispersity will be lower than when aromatic compounds are used.
- mesogenic groups with polar moieties the dispersion of the liquid-crystalline material is increased. For instance, if mesogenic groups according to formula 1 are used with -N0 as Ri instead of 0-R* or R* , the dispersion is increased. Halogenation of the mesogenic group also gives an increase of dispersion.
- the artisan can easily adjust the dispersion of the retardation layer via the measures described above.
- the birefringence at a certain wavelength can easily be measured with a refractometer, and from birefringences at various wavelengths the dispersion can be calculated.
- the retardation of a commercially available cell can be measured with various optical techniques known to the artisan. From the retardation at a certain wavelength and the retardation at 550 nm the dispersion at a certain wavelength can be calculated.
- liquid- crystalline material For accurate matching of the dispersion of an active cell, liquid- crystalline material may be used wherein both mesogenic groups having a large conjugated system and mesogenic groups having a small conjugated system are present. By varying the ratio of the two kinds of mesogenic groups the dispersion can be accurately matched with the active cell .
- cyclic or aromatic compounds ⁇ I and ⁇ * examples include:
- R* stands for an alkyl group having 1-5 carbon atoms.
- R groups examples include:
- R* groups contain an asymmetrical carbon atom.
- the use of chiral (exclusively laevorotatory or dextrorotatory) R* groups may be advantageous in LCD retardation layers, as will be explained below. It was found that the dispersion of high-molecular weight liquid- crystalline material is mainly dependent on the mesogenic group. A specific mesogenic group gives the virtually same dispersion irrespective of the liquid-crystalline polymer, oligomer or glass into which it is incorporated.
- high-molecular weight material has a higher mechanical strength than low-molecular weight material. This makes it possible to place the liquid-crystalline material between glass substrates having a thickness of 20-500 micrometers instead of thick glass substrates.
- the liquid-crystalline material may even be placed between or coated on flexible plastic substrates such as PET and polycarbonate.
- the retardation layer To obtain full compensation for the birefringence effect of the active cell, it is also necessary for the retardation layer to have an equal as well as an opposite angle of rotation compared with the active cell.
- a twisted structure is obtained by placing the liquid- crystalline material between two orienting substrates, giving one of the substrates a different orientation direction from that of the other substrate.
- the substrate itself may be rubbed in a single direction.
- the substrate in that case may be made of, e.g., polyimide, polyvinyl alcohol, glass, etc.
- the substrate may be provided with a thin orienting layer.
- This. may be a thin polymer layer which can be rubbed, e.g., polyimide, polyvinyl alcohol, etc.
- this thin orienting layer may be a SiO x layer evaporated at an angle of less than 90°, usually of 60° or 86°.
- a substrate of poor flexibility, such as glass or quartz is used for SiO x evaporation.
- the liquid-crystalline material is frequently mixed with a chiral material: the so-called chiral dopant.
- chiral dopant any optically active compound may be used to this end.
- cholesterol derivatives and 4-(4-hexyloxy-benzoyloxy) benzene acid 2-octyl -ester.
- up to 5 wt.% of chiral dopant is employed in relation to the total amount of liquid-crystalline material.
- the liquid crystalline material itself may be provided with chiral centres.
- this is done by providing the mesogenic group with a chiral chain (group R*) or spacer, since in this way the transition temperatures will hardly if at all be adversely affected.
- group R* chiral chain
- Examples of mesogenic groups with chiral chains have been described above.
- the angle of rotation of an STN display cell typically is 240° but may be any other appropriate value.
- the film In the case of an angle of rotation of 90° (or -90°), the film is generally called "twisted nematic.”
- an angle of rotation of 90° (or -90°) is required. If the angle of rotation is greater, the film is called “supertwisted nematic.”
- this invention also concerns retardation layers with a smaller angle of rotation, from 0° (no twist) to 90° (or -90°). For convenience these layers are also called “twisted nematic" here. In the case of an angle of rotation of 0°, the arrangement of the liquid-crystalline layer will be uniform planar.
- the invention is also directed to retardation layers having more than one pitch (even more than 5 pitches) .
- the high molecular-weight liquid-crystalline film can be placed between the substrate of the display cell and another substrate.
- the LC polymer film is placed between the polariser and a substrate.
- a second substrate is not necessary and the thickness and weight of the retardation layer are reduced further.
- the invention is further directed to a liquid-crystalline display comprising an active liquid-crystalline cell and a retardation layer of high-molecular weight liquid-crystalline material, wherein the difference in dispersion between the active cell and the retardation layer in the wavelength area of 400-800 nm is not more than 0.1.
- Liquid-crystalline glasses were prepared from mesogenic group- containing epoxides and diamines.
- a mixture of 1 eq. of diamine and 4 eq. of epoxy was heated for 5 hours under a nitrogen atmosphere at a temperature of 130°C.
- the melt was cooled down and dissolved in THF, and the solution of approximately 20% (m/M) was precipitated in a 10-fold excess of ethanol .
- the yields were in the range of 75 to 90%.
- LC 1 The epoxide of cyanobiphenyl was used to prepare an LC glass (LC 1) by the general method for the synthesis of LC glasses specified above, using m-xylylene diamine (m-XDA), ex Fluka ® .
- m-XDA m-xylylene diamine
- the molecualar weight was found to be 1140 , Tg: 64/70°C, Tc: 127°C.
- a liquid-crystalline glass (LC 2) was prepared by the general method for the synthesis of LC glasses specified above using methylene diamine, ex Fluka®. The molecular weight turned out to be 1398, Tg: 66/72°C, Tc: 127°C.
- Liquid-crystal l ine polyethers were prepared from mesogenic group- containing epoxides and mesogeni c group-containing diol s.
- the epoxide of methoxyphenyl benzoate was used, to prepare a liquid- crystalline polyether (LC 3) by the general method for the synthesis of LC polyethers specified above, using methoxyphenyl-(2,3 dihydroxypropyloxy)benzoate with an epoxy/OH ratio of 5:1.
- the diol was prepared in the same manner as the hexyloxy analogon in EP-A2-0550 105.
- the molecular weight turned out to be 2984, Tg: 46/52°C, Tc: 146°C.
- This product was recrystallised from 250 ml of glacial acetic acid.
- 32 g (0.18 mole) of the dried 4(allyloxy)benzoic acid were dissolved in 150 ml of thionyl chloride, whereupon 2 drops of dimethyl formamide were added and the whole was boiled with refluxing.
- Thionyl chloride was distilled off, and after being cooled the residue was incorporated into 100 ml of dry dichloromethane. After filtration the dichloromethane solution was added, with vigorous stirring, over 1 hour and at a temperature of 5-10°C, to a solution of 23 g of nitrophenol (0.166 mole) in a mixture of 135 ml of dichloromethane and 34.2 ml of pyridine.
- LC 4 liquid- crystalline polyether
- LC 4 liquid- crystalline polyether
- the diol was prepared in the same manner as the hexyloxy analogon in EP-A2-0550 105.
- the molecular weight turned out to be 3173, Tg: 58/63°C, Tc: 130°C.
- the epoxide of methoxycyclohexyl benzoate was used together with the epoxide of methoxyphenyl benzoate to prepare a liquid crystalline polyether (LC 5) by using the general method for the synthesis of liquid crystalline polyethers specified above, using methoxy phenyl-(2,3 dihydroxypropyloxy) benzoate with an epoxy/OH ratio of 5:1. It appeared that the cyclohexyl group containing epoxide was present for 16 mole % in the polyether.
- the layer thickness obtained was 4 micrometers.
- the two films of LC material 3 were dried in a vacuum oven for 16 hours at 20°C. They were then placed one on top of the other under a 60° difference in orientation direction and moulded at a temperature of 160°C. Next, the sample was cooled to 115°C, and after 5 minutes to room temperature. The quality of the resulting retardation film was determined with the aid of various optical techniques based on the theory described in E.P. Raynes, "Molecular Crystals,” Liquid Crystals Letters 4(3-4) (1987), 69-75.
- the dispersion of the high-molecular weight liquid-crystalline material was measured by fitting transmission spectra of the retardation layers between two polarisers to the formulae given in Raynes.
- the dispersion (defined as the retardation at a certain wavelength divided by the retardation at 550 nm) was given for LC 3, a birefingent polycarbonate film such as described in Jap. J. Appl Physics,VOl.30, No.4 (APril 1991), 682-686, and a commercially available low-molecular weight liquid-crystalline active cell as used in the Sharp wordprocessor WD A 330®, and an active cell containing a commercially available liquid crystal mixture ZLI 4544, ex Merck ® .
- the dispersion of LC 4 according to the invention is nearly the same as that of a commercially available active cell (a difference in dispersion of less than 0.1) over the whole wavelength area of 400-800 nm, whereas the dispersion of the birefringent polycarbonate film only matches that of the commercially available active cell at 550 nm , by definition, and shows large deviations, especially in the shorter wavelength area of 400-550 nm.
- the dispersion of LC 5 is nearly the same as that of the active cell containing ZLI 4544 over the whole wavelength area of 400-800 nm.
Abstract
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Application Number | Priority Date | Filing Date | Title |
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EP94929500A EP0721602B1 (en) | 1993-09-29 | 1994-09-29 | Retardation layer having a dispersion adapted to the active liquid-crystalline cell |
KR1019960701692A KR100314320B1 (en) | 1993-09-29 | 1994-09-29 | Is it suitable for active liquid crystal cell? |
JP7510117A JPH09504382A (en) | 1993-09-29 | 1994-09-29 | Phase delay layer with dispersion compatible with active liquid crystal cells |
DE69421407T DE69421407T2 (en) | 1993-09-29 | 1994-09-29 | DELAY LAYER WITH A DISPERSION ADAPTED TO THE ACTIVE LIQUID CRYSTAL CELL |
US08/619,613 US5760859A (en) | 1993-09-29 | 1994-09-29 | Retardation layer having a dispersion adapted to the active liquid-crystalline cell |
Applications Claiming Priority (6)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP93202788.1 | 1993-09-29 | ||
EP93202788 | 1993-09-29 | ||
NL9401217 | 1994-07-26 | ||
NL9401217 | 1994-07-26 | ||
NL9401342 | 1994-08-19 | ||
NL9401342 | 1995-03-14 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO1995009379A1 true WO1995009379A1 (en) | 1995-04-06 |
Family
ID=27235333
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/EP1994/003246 WO1995009379A1 (en) | 1993-09-29 | 1994-09-29 | Retardation layer having a dispersion adapted to the active liquid-crystalline cell |
Country Status (9)
Country | Link |
---|---|
US (1) | US5760859A (en) |
EP (1) | EP0721602B1 (en) |
JP (1) | JPH09504382A (en) |
KR (1) | KR100314320B1 (en) |
CN (1) | CN1047003C (en) |
AT (1) | ATE186125T1 (en) |
CA (1) | CA2172973A1 (en) |
DE (1) | DE69421407T2 (en) |
WO (1) | WO1995009379A1 (en) |
Cited By (6)
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WO1997023805A1 (en) * | 1995-12-22 | 1997-07-03 | Akzo Nobel N.V. | Temperature matched retardation layer |
WO1998004651A1 (en) * | 1996-07-26 | 1998-02-05 | Merck Patent Gmbh | Combination of optical elements |
EP0851269A1 (en) * | 1996-12-24 | 1998-07-01 | Sharp Kabushiki Kaisha | Liquid crystal display device |
EP0871059A3 (en) * | 1997-04-07 | 1999-09-15 | Sharp Kabushiki Kaisha | Liquid crystal display device |
US6084651A (en) * | 1997-03-05 | 2000-07-04 | Sharp Kabushiki Kaisha | Liquid crystal display device having liquid crystal layer divided at different ratios in each pixel |
USRE41281E1 (en) | 1996-07-01 | 2010-04-27 | Merck Patent Gesellschaft Mit Beschrankter Haftung | Liquid crystal display device |
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US6351299B2 (en) * | 1996-04-15 | 2002-02-26 | Ricoh Company, Ltd. | Liquid crystal display device |
JPH11509650A (en) * | 1996-05-17 | 1999-08-24 | フィリップス エレクトロニクス ネムローゼ フェンノートシャップ | Compensation layer, liquid crystal display and retardation foil |
TW515925B (en) * | 1996-12-25 | 2003-01-01 | Sharp Kk | Liquid crystal display device |
GB9713981D0 (en) * | 1997-07-03 | 1997-09-10 | Sharp Kk | Optical device |
US6606143B1 (en) * | 1998-03-13 | 2003-08-12 | Sharp Kabushiki Kaisha | Liquid crystal display device with phase element |
US6400433B1 (en) * | 1998-11-06 | 2002-06-04 | Fuji Photo Film Co., Ltd. | Circularly polarizing plate comprising linearly polarizing membrane and quarter wave plate |
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- 1994-09-29 CN CN94193572A patent/CN1047003C/en not_active Expired - Fee Related
- 1994-09-29 AT AT94929500T patent/ATE186125T1/en not_active IP Right Cessation
- 1994-09-29 US US08/619,613 patent/US5760859A/en not_active Expired - Fee Related
- 1994-09-29 DE DE69421407T patent/DE69421407T2/en not_active Expired - Fee Related
- 1994-09-29 KR KR1019960701692A patent/KR100314320B1/en not_active IP Right Cessation
- 1994-09-29 JP JP7510117A patent/JPH09504382A/en not_active Ceased
- 1994-09-29 WO PCT/EP1994/003246 patent/WO1995009379A1/en active IP Right Grant
- 1994-09-29 EP EP94929500A patent/EP0721602B1/en not_active Expired - Lifetime
- 1994-09-29 CA CA002172973A patent/CA2172973A1/en not_active Abandoned
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EP0382460A2 (en) * | 1989-02-06 | 1990-08-16 | Sharp Kabushiki Kaisha | Liquid crystal display device |
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EP0524028A1 (en) * | 1991-07-19 | 1993-01-20 | Nippon Oil Co. Ltd. | Viewing angle compensator for liquid crystal display |
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US6088077A (en) * | 1995-12-22 | 2000-07-11 | Akzo Nobel Nv | Temperature matched retardation layer |
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JP2000512768A (en) * | 1995-12-22 | 2000-09-26 | アクゾ ノーベル ナムローゼ フェンノートシャップ | Temperature matching retardation layer |
EA000614B1 (en) * | 1995-12-22 | 1999-12-29 | Акцо Нобель Н.В. | Temperature matched retardation layer |
USRE41281E1 (en) | 1996-07-01 | 2010-04-27 | Merck Patent Gesellschaft Mit Beschrankter Haftung | Liquid crystal display device |
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WO1998004651A1 (en) * | 1996-07-26 | 1998-02-05 | Merck Patent Gmbh | Combination of optical elements |
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US6163354A (en) * | 1996-12-24 | 2000-12-19 | Sharp Kabushiki Kaisha | Liquid crystal display device including liquid crystal display material preventing generation of viewing-angle-dependent coloration of display screen |
EP0851269A1 (en) * | 1996-12-24 | 1998-07-01 | Sharp Kabushiki Kaisha | Liquid crystal display device |
US6084651A (en) * | 1997-03-05 | 2000-07-04 | Sharp Kabushiki Kaisha | Liquid crystal display device having liquid crystal layer divided at different ratios in each pixel |
US6535258B1 (en) | 1997-04-07 | 2003-03-18 | Sharp Kabushiki Kaisha | Liquid crystal display device with low dispersion LC and high dispersion compensator |
US6137556A (en) * | 1997-04-07 | 2000-10-24 | Sharp Kabushiki Kaisha | Liquid crystal display device |
US6937309B2 (en) | 1997-04-07 | 2005-08-30 | Sharp Kabushiki Kaisha | Liquid crystal display/optical retardation compensator combination in which variations in the dispersion of light in the liquid crystal and/or in the compensator materials minimize undesired screen coloration |
EP0871059A3 (en) * | 1997-04-07 | 1999-09-15 | Sharp Kabushiki Kaisha | Liquid crystal display device |
US7245340B2 (en) | 1997-04-07 | 2007-07-17 | Sharp Kabushiki Kaisha | Liquid crystal display device having controlled refractive index anisotropy of the liquid crystal layer and the retardation compensator plate |
Also Published As
Publication number | Publication date |
---|---|
DE69421407D1 (en) | 1999-12-02 |
CN1132557A (en) | 1996-10-02 |
CA2172973A1 (en) | 1995-04-06 |
EP0721602B1 (en) | 1999-10-27 |
ATE186125T1 (en) | 1999-11-15 |
JPH09504382A (en) | 1997-04-28 |
KR960705254A (en) | 1996-10-09 |
KR100314320B1 (en) | 2001-12-28 |
US5760859A (en) | 1998-06-02 |
DE69421407T2 (en) | 2000-05-04 |
CN1047003C (en) | 1999-12-01 |
EP0721602A1 (en) | 1996-07-17 |
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