TWI362524B - An improved pi-cell liquid crystal display - Google Patents
An improved pi-cell liquid crystal display Download PDFInfo
- Publication number
- TWI362524B TWI362524B TW93132205A TW93132205A TWI362524B TW I362524 B TWI362524 B TW I362524B TW 93132205 A TW93132205 A TW 93132205A TW 93132205 A TW93132205 A TW 93132205A TW I362524 B TWI362524 B TW I362524B
- Authority
- TW
- Taiwan
- Prior art keywords
- liquid crystal
- alignment
- crystal device
- layer
- angle
- Prior art date
Links
- 239000004973 liquid crystal related substance Substances 0.000 title claims description 305
- 239000000463 material Substances 0.000 claims description 157
- 210000002858 crystal cell Anatomy 0.000 claims description 75
- 239000010408 film Substances 0.000 claims description 62
- 239000000758 substrate Substances 0.000 claims description 59
- 238000000034 method Methods 0.000 claims description 52
- 239000007787 solid Substances 0.000 claims description 30
- 239000011159 matrix material Substances 0.000 claims description 20
- 238000005452 bending Methods 0.000 claims description 17
- 239000000203 mixture Substances 0.000 claims description 15
- 238000012545 processing Methods 0.000 claims description 14
- 208000011823 Juvenile amyotrophic lateral sclerosis Diseases 0.000 claims description 13
- 238000002360 preparation method Methods 0.000 claims description 7
- 239000010409 thin film Substances 0.000 claims description 7
- 238000010884 ion-beam technique Methods 0.000 claims description 6
- 238000004519 manufacturing process Methods 0.000 claims description 6
- 239000004744 fabric Substances 0.000 claims description 5
- 239000002105 nanoparticle Substances 0.000 claims description 5
- 230000001678 irradiating effect Effects 0.000 claims description 4
- 230000003780 keratinization Effects 0.000 claims 1
- 210000004027 cell Anatomy 0.000 description 121
- 239000002904 solvent Substances 0.000 description 33
- 239000000243 solution Substances 0.000 description 27
- 230000005540 biological transmission Effects 0.000 description 17
- 230000008569 process Effects 0.000 description 17
- 239000007788 liquid Substances 0.000 description 15
- 239000011521 glass Substances 0.000 description 14
- 239000002086 nanomaterial Substances 0.000 description 13
- 230000003287 optical effect Effects 0.000 description 13
- 230000035484 reaction time Effects 0.000 description 11
- 238000004528 spin coating Methods 0.000 description 11
- 239000003795 chemical substances by application Substances 0.000 description 9
- 238000005516 engineering process Methods 0.000 description 8
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical group [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 8
- 229920000642 polymer Polymers 0.000 description 8
- 238000004873 anchoring Methods 0.000 description 7
- 238000000576 coating method Methods 0.000 description 7
- 238000007639 printing Methods 0.000 description 7
- 230000007704 transition Effects 0.000 description 7
- 238000006243 chemical reaction Methods 0.000 description 6
- 238000010276 construction Methods 0.000 description 5
- 239000013078 crystal Substances 0.000 description 5
- 239000003822 epoxy resin Substances 0.000 description 5
- 229920000647 polyepoxide Polymers 0.000 description 5
- 229920003051 synthetic elastomer Polymers 0.000 description 5
- 239000011248 coating agent Substances 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 229910052732 germanium Inorganic materials 0.000 description 4
- 238000002156 mixing Methods 0.000 description 4
- 239000000047 product Substances 0.000 description 4
- 125000006850 spacer group Chemical group 0.000 description 4
- 239000005061 synthetic rubber Substances 0.000 description 4
- ZMXDDKWLCZADIW-UHFFFAOYSA-N N,N-Dimethylformamide Chemical compound CN(C)C=O ZMXDDKWLCZADIW-UHFFFAOYSA-N 0.000 description 3
- 239000004642 Polyimide Substances 0.000 description 3
- DNIAPMSPPWPWGF-UHFFFAOYSA-N Propylene glycol Chemical compound CC(O)CO DNIAPMSPPWPWGF-UHFFFAOYSA-N 0.000 description 3
- 230000015572 biosynthetic process Effects 0.000 description 3
- 125000000484 butyl group Chemical group [H]C([*])([H])C([H])([H])C([H])([H])C([H])([H])[H] 0.000 description 3
- 239000001913 cellulose Substances 0.000 description 3
- 229920002678 cellulose Polymers 0.000 description 3
- 230000008859 change Effects 0.000 description 3
- 229920001721 polyimide Polymers 0.000 description 3
- 230000036632 reaction speed Effects 0.000 description 3
- 238000012546 transfer Methods 0.000 description 3
- WOQLPPITHNQPLR-UHFFFAOYSA-N 1-sulfanylpyrrolidin-2-one Chemical compound SN1CCCC1=O WOQLPPITHNQPLR-UHFFFAOYSA-N 0.000 description 2
- YEJRWHAVMIAJKC-UHFFFAOYSA-N 4-Butyrolactone Chemical compound O=C1CCCO1 YEJRWHAVMIAJKC-UHFFFAOYSA-N 0.000 description 2
- QIGBRXMKCJKVMJ-UHFFFAOYSA-N Hydroquinone Chemical compound OC1=CC=C(O)C=C1 QIGBRXMKCJKVMJ-UHFFFAOYSA-N 0.000 description 2
- 239000004988 Nematic liquid crystal Substances 0.000 description 2
- 239000004677 Nylon Substances 0.000 description 2
- 108010039918 Polylysine Proteins 0.000 description 2
- 239000004793 Polystyrene Substances 0.000 description 2
- 239000004372 Polyvinyl alcohol Substances 0.000 description 2
- 229920001577 copolymer Polymers 0.000 description 2
- 239000006185 dispersion Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000005489 elastic deformation Effects 0.000 description 2
- 229920001519 homopolymer Polymers 0.000 description 2
- AMGQUBHHOARCQH-UHFFFAOYSA-N indium;oxotin Chemical compound [In].[Sn]=O AMGQUBHHOARCQH-UHFFFAOYSA-N 0.000 description 2
- 238000007641 inkjet printing Methods 0.000 description 2
- 239000012528 membrane Substances 0.000 description 2
- 239000000178 monomer Substances 0.000 description 2
- 229920001778 nylon Polymers 0.000 description 2
- 230000000704 physical effect Effects 0.000 description 2
- 229920000515 polycarbonate Polymers 0.000 description 2
- 239000004417 polycarbonate Substances 0.000 description 2
- 229920000656 polylysine Polymers 0.000 description 2
- 229920002223 polystyrene Polymers 0.000 description 2
- 229920002451 polyvinyl alcohol Polymers 0.000 description 2
- 238000011160 research Methods 0.000 description 2
- 238000004088 simulation Methods 0.000 description 2
- 230000001052 transient effect Effects 0.000 description 2
- 101100008049 Caenorhabditis elegans cut-5 gene Proteins 0.000 description 1
- 244000025254 Cannabis sativa Species 0.000 description 1
- 239000004593 Epoxy Substances 0.000 description 1
- 206010061218 Inflammation Diseases 0.000 description 1
- WRQNANDWMGAFTP-UHFFFAOYSA-N Methylacetoacetic acid Chemical compound COC(=O)CC(C)=O WRQNANDWMGAFTP-UHFFFAOYSA-N 0.000 description 1
- 241000237509 Patinopecten sp. Species 0.000 description 1
- 239000004698 Polyethylene Substances 0.000 description 1
- KJTLSVCANCCWHF-UHFFFAOYSA-N Ruthenium Chemical compound [Ru] KJTLSVCANCCWHF-UHFFFAOYSA-N 0.000 description 1
- WYURNTSHIVDZCO-UHFFFAOYSA-N Tetrahydrofuran Chemical compound C1CCOC1 WYURNTSHIVDZCO-UHFFFAOYSA-N 0.000 description 1
- 150000001298 alcohols Chemical class 0.000 description 1
- 230000004075 alteration Effects 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 238000004630 atomic force microscopy Methods 0.000 description 1
- 239000000987 azo dye Substances 0.000 description 1
- 210000003719 b-lymphocyte Anatomy 0.000 description 1
- 239000012612 commercial material Substances 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 125000004122 cyclic group Chemical group 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000003618 dip coating Methods 0.000 description 1
- 238000009826 distribution Methods 0.000 description 1
- 238000007606 doctor blade method Methods 0.000 description 1
- 239000002019 doping agent Substances 0.000 description 1
- 238000001035 drying Methods 0.000 description 1
- 239000000428 dust Substances 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 230000008020 evaporation Effects 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 239000012456 homogeneous solution Substances 0.000 description 1
- 230000004054 inflammatory process Effects 0.000 description 1
- 230000005764 inhibitory process Effects 0.000 description 1
- 150000002500 ions Chemical class 0.000 description 1
- 239000004922 lacquer Substances 0.000 description 1
- 239000011259 mixed solution Substances 0.000 description 1
- 239000012046 mixed solvent Substances 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 239000012788 optical film Substances 0.000 description 1
- 230000000149 penetrating effect Effects 0.000 description 1
- 229920003229 poly(methyl methacrylate) Polymers 0.000 description 1
- -1 polyethylene Polymers 0.000 description 1
- 229920000573 polyethylene Polymers 0.000 description 1
- 229920002959 polymer blend Polymers 0.000 description 1
- 239000004926 polymethyl methacrylate Substances 0.000 description 1
- 239000002244 precipitate Substances 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 230000004044 response Effects 0.000 description 1
- 238000012552 review Methods 0.000 description 1
- 229910052707 ruthenium Inorganic materials 0.000 description 1
- 235000020637 scallop Nutrition 0.000 description 1
- 238000007650 screen-printing Methods 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 238000005507 spraying Methods 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- RWRDLPDLKQPQOW-UHFFFAOYSA-N tetrahydropyrrole Substances C1CCNC1 RWRDLPDLKQPQOW-UHFFFAOYSA-N 0.000 description 1
- 238000002834 transmittance Methods 0.000 description 1
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
- G02F1/1393—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 birefringence of the liquid crystal being electrically controlled, e.g. ECB-, DAP-, HAN-, PI-LC cells
- G02F1/1395—Optically compensated birefringence [OCB]- cells or PI- cells
Landscapes
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- Liquid Crystal (AREA)
- Chemical & Material Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
Description
1362524 931而两方7~| 九、發明說明: Γ:發明所属之技術領域3 發明領域 本發明涉及一種液晶顯示器(LCD)技術,特別地,涉及 5 通過提供一種改善的取向層來增加反應速度的LCD。 * C先前技術;1 發明背景 液晶顯示器(LCD)被用在很多應用中。液晶顯示器 (LCD)的光學設計是其應用的重要主題。理想地,一個好的 10 LCD模型應該具有卓越的對比度,寬闊的視角,高光學效 率和快轉換速度。 主要應用之一在於顯示視頻信號。這包括LCD電視 (LCD TV)。對於視頻速率信號顯示器,所述LCD的反應速 度必須快,否則會有運動圖像的模糊現象。同樣,所述LCD 15 τν的視角應該儘量寬,就像在傳統的陰極射線管一樣。通 常在水平方向的要求是160。,在垂直方向的要求是90。。對 於寬的視角’所述板内切換(IPS)模式和所述垂直取向 (vertical alignment)模式以及其很多的變型對於視頻應用很 有希望。然而,它們的切換速度需要從>10nls提高到2ms。 20這樣’需要LCD光學模式具有快的切換速度和寬的視角。 用於快速切換LCD的一種可能的候選者是π晶胞 (pi-cell)。一個π晶胞主要是一個彎曲變形的液晶晶胞。這 個π晶胞在1986年作為一種快速液晶切換被發明(p. Bos,美 國專利 No. 4566758: Rapid starting,high-speed liquid 5 1362524 號申請案修正f 101,01.12. crystal variable optical retarder)。在其被發明的原始形式 中,所述晶胞實際上是一種斜展變形晶胞,其需要一個偏 壓來轉換它成為一個彎曲晶胞或π晶胞。與所述二轴補償膜 一起,這個π晶胞後來被改進,也被稱作光學補償彎曲排列 5 (〇CB)液晶顯示器(H. Nakamura等人,美國第6069620號專 利:液晶顯示裝置之驅動方法)。所述π晶胞基本上在向列 液晶的多種彎曲變形之間工作。施加一個電壓改變所述液 晶晶胞指向矢(director)的彎曲角度’因此改變它的全部的 雙折射。這樣,所述π晶胞的光學性質基本上是一個電控雙 10 折射(electrically controlled birefringent,ECB)晶胞的光學 性質。這樣,它能夠容易地通過使用多種光學膜來補償以 獲得一個寬的視角。 一種傳統的π晶胞通過在所述液晶晶胞晶胞兩側的所 述取向層的平行摩擦形成。在所述液晶晶胞兩側的傾斜角 15 互相朝向對方傾斜,如第2圖放大示出。符合這些邊界條件 的可能的液晶指向矢取向是斜展變形(splay deformation, 以後稱為S-狀態),彎曲變形(bend deformation,以後稱為B-狀態),以及π-扭轉變形〇-twistdeformation,以後稱為τ-狀 態)。S-晶胞和B·晶胞分別在第8A和8B圖中示出。第1〇A和 20 10B圖顯示了在(A)零電壓和(B)高電壓的彎曲取向。當施加 一個高電壓時’所述B-狀態成為垂直取向(h〇me〇tn>pk alignment)。向所述的這種基本的結構引入π/4扭轉和π/8扭 轉,存在這種基本取向的變化。在研究的所有情況下,最 穩定的狀態是S-狀態。從更穩定的S-狀態到Β-狀態的變形 6 1362524 ,· · . 第93132205號申請案修正貢 101.01.12. 需要使用所述π晶胞。(參閱,例如E J Acosta等人,The role of surface tilt in the operation of pi-cell liquid crystal devices, Liquid crystals, vol 27,p 977,2000; S H Lee等人,BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a liquid crystal display (LCD) technology, and in particular to 5 to increase the reaction speed by providing an improved alignment layer. LCD. * C Prior Art; 1 Background of the Invention Liquid crystal displays (LCDs) are used in many applications. The optical design of liquid crystal displays (LCDs) is an important topic in their application. Ideally, a good 10 LCD model should have excellent contrast, wide viewing angle, high optical efficiency and fast switching speed. One of the main applications is to display video signals. This includes LCD TVs (LCD TVs). For a video rate signal display, the response speed of the LCD must be fast, otherwise there will be blurring of the moving image. Also, the angle of view of the LCD 15 τν should be as wide as possible, as in a conventional cathode ray tube. Usually the requirement in the horizontal direction is 160. The requirement in the vertical direction is 90. . The intra-panel switching (IPS) mode and the vertical alignment mode, as well as many variations thereof, for the wide viewing angle are promising for video applications. However, their switching speed needs to be increased from >10nls to 2ms. 20 such 'requires LCD optical mode with fast switching speed and wide viewing angle. One possible candidate for fast switching LCDs is the pi-cell. A π unit cell is mainly a bent liquid crystal cell. This π unit cell was invented in 1986 as a fast liquid crystal switching (p. Bos, U.S. Patent No. 4,566,758: Rapid starting, high-speed liquid 5 1362524, application f 101, 01.12. crystal variable optical retarder). In its original form of invention, the unit cell is actually a diagonally deformed unit cell that requires a bias to convert it into a curved unit cell or a π unit cell. Together with the biaxial compensation film, this π unit cell was later improved, also referred to as an optically compensated curved arrangement 5 (〇CB) liquid crystal display (H. Nakamura et al., US Patent No. 6069620: Driving of a liquid crystal display device) method). The π unit cell operates substantially between various bending deformations of the nematic liquid crystal. Applying a voltage changes the bending angle of the liquid crystal cell director' thus changing its overall birefringence. Thus, the optical properties of the π unit cell are essentially the optical properties of an electrically controlled birefringent (ECB) unit cell. Thus, it can be easily compensated by using a plurality of optical films to obtain a wide viewing angle. A conventional π unit cell is formed by parallel rubbing of the alignment layers on both sides of the liquid crystal cell unit cell. The inclination angles 15 on both sides of the liquid crystal cell are inclined toward each other as shown in Fig. 2 in an enlarged manner. Possible liquid crystal director orientations that conform to these boundary conditions are splay deformation (hereinafter referred to as S-state), bend deformation (hereinafter referred to as B-state), and π-torsional deformation 〇-twistdeformation, Hereinafter referred to as τ-state). The S-cell and the B-cell are shown in Figures 8A and 8B, respectively. Figures 1A and 20B show the bend orientation at (A) zero voltage and (B) high voltage. When a high voltage is applied, the B-state becomes a vertical orientation (h〇me〇tn>pk alignment). The introduction of π/4 twist and π/8 twist to the basic structure described has such a change in the basic orientation. In all cases studied, the most stable state is the S-state. From the more stable S-state to the Β-state deformation 6 1362524, · · The application of the 93132205 amendment 101.01.12. The use of the π unit cell. (See, for example, E J Acosta et al., The role of surface tilt in the operation of pi-cell liquid crystal devices, Liquid crystals, vol 27, p 977, 2000; S H Lee et al.
Chiral doped optically-compensated bend nematic liquid 5 crystal cell with continuous deformation from twist to twist-bend state, Japanese J of Applied Physics, vol 40,p L389,2001; S H Lee等人,Geometric structure for theChiral doped optically-compensated bend nematic liquid 5 crystal cell with integrated deformation from twist to twist-bend state, Japanese J of Applied Physics, vol 40, p L389, 2001; S H Lee et al., Geometric structure for the
uniform splay to bend transition in a pi-cell, Japanese JUniform splay to bend transition in a pi-cell, Japanese J
Applied Physics,vol 42, p L1148, 2003)。因為所述S和B變形 10不是拓撲等價的,需要發生有核的轉換。起初的S-狀態到 B-狀態的所述“條件”是研究的主要領域。已經提出了很多 方法’包括引入突起和添加手性分子換雜物。同樣,為了 所述π晶胞只在所述B-狀態正常工作’要維持一個偏壓。 本發明的一個目的是,提供一種改進的π晶胞。 15 【發明内容】 發明概要 在本發明的一個方面,提供用在液晶晶胞的一種液晶 取向層來取向液晶分子。所述取向層包括奈米結構: a· —種水平取向材料,能夠提供在與其接觸處的所述液 20 晶分子的—個第一預傾角; b·—種垂直取向材料’能夠提供在與其接觸處的所述 液晶分子的一個第二預傾角; 其中與所述取向層接觸的和在所述取向層附近的所述 液晶分子有效的預傾角能夠被控制以具有在所述第一預傾 7 丄的2524 角和第二預傾角之間的一個值。在一個優選實施例中,所 述第—預傾角在1〇-10。以及所述第二預傾角在8〇。-9〇。。在 一個更為優選的實施例中,所述第一預傾角在丨。_8。以及所 述第二預傾角在85。-90。。在另一個優選實施例中,所述取 5向層包括所述垂直取向材料或所述水平取向材料的奈米結 構。在另一個優選實施例中,所述奈米結構既包括所述水 平取向材料又包括所述垂直取向材料。在另一個實施例 中所述奈米結構是水平取向材料。在另一個實施例中, 所述奈米結構是垂直取向材料。在另一個優選實施例中, 10所述奈米結構大小是0-1微米的量級。 在一個優選實施例中,所述取向材料中的至少一種是 個t合體。在一個更為優選的實施例中,所述取向材料 中的至少一種是從包括聚醯亞胺,聚苯乙烯,聚甲基丙婦 酸甲酯,聚碳酸酯,聚醯胺酸和聚乙烯醇的一個組中選擇 15出來的。在一個更為優選的實施例中,所述取向材料中的 至少—種是聚醯亞胺。在一個最優選的實施例中,所述水 平取向材料是JALS9203,所述垂直取向材料是JALS2021, 其中 JALS9203與 JALS2021係來自 JSR公司(www. jsr. co. jp) 的商業產品,JALS9203與JALS2021例如其預傾角之特性可 20 在各自的產品說明單中找到。 在另一個優選的實施例中,所述重量:所述水平取向 材料相對於所述垂直取向材料的重量的比率是1 : 99到99 : 1。在一個更優選的實施例中,所述重量:所述水平取向材 料相對於所述垂直取向材料的重量的比率是1 : 4到4 : 1。 8Applied Physics, vol 42, p L1148, 2003). Since the S and B variants 10 are not topologically equivalent, a nucleus transition is required. The "conditions" of the initial S-state to B-state are the main areas of research. A number of methods have been proposed including the introduction of protrusions and the addition of chiral molecular alterations. Similarly, a bias voltage is maintained for the π cell to operate normally only in the B-state. It is an object of the invention to provide an improved π unit cell. SUMMARY OF THE INVENTION SUMMARY OF THE INVENTION In one aspect of the invention, a liquid crystal alignment layer for liquid crystal cells is used to orient liquid crystal molecules. The alignment layer comprises a nanostructure: a. a horizontally oriented material capable of providing a first pretilt angle of the liquid 20 molecule at the point of contact thereof; b. a vertical alignment material capable of providing a second pretilt angle of the liquid crystal molecules at the contact; wherein an effective pretilt angle of the liquid crystal molecules in contact with the alignment layer and in the vicinity of the alignment layer can be controlled to have the first pretilt 7 A value between the 2524 angle and the second pretilt angle. In a preferred embodiment, the first pretilt angle is between 1 and 10. And the second pretilt angle is 8 〇. -9 〇. . In a more preferred embodiment, the first pretilt angle is at 丨. _8. And the second pretilt angle is at 85. -90. . In another preferred embodiment, the unidirectional layer comprises a nanostructure of the vertical alignment material or the horizontal alignment material. In another preferred embodiment, the nanostructure comprises both the horizontally oriented material and the vertically oriented material. In another embodiment the nanostructure is a horizontally oriented material. In another embodiment, the nanostructure is a vertically oriented material. In another preferred embodiment, 10 the nanostructure size is on the order of 0-1 micron. In a preferred embodiment, at least one of the alignment materials is a t-complex. In a more preferred embodiment, at least one of the alignment materials is from the group consisting of polyimine, polystyrene, polymethyl methyl acetoacetate, polycarbonate, polylysine, and polyethylene. Select 15 out of a group of alcohols. In a more preferred embodiment, at least one of the oriented materials is a polyimide. In a most preferred embodiment, the horizontal alignment material is JALS9203, and the vertical alignment material is JALS2021, wherein JALS9203 and JALS2021 are commercial products from JSR Corporation (www.jsr.co.jp), for example JALS9203 and JALS2021 The characteristics of its pretilt angle can be found in the respective product description sheets. In another preferred embodiment, the weight: the ratio of the horizontally oriented material to the weight of the vertically oriented material is 1:99 to 99:1. In a more preferred embodiment, the weight: the ratio of the horizontally oriented material to the weight of the vertically oriented material is from 1: 4 to 4:1. 8
93132205號申請胃 在另—個優選的實施例中,在所述取向層上的所述極 角鳊疋能量在5 x 1 (T4J/cm2到2.5 X1 〇-3 J/cm2之間。 在本發明的另一方面,提供了在一個液晶晶胞中製造 一個取向層的方法,其包括: a) 在一個溶劑中溶解一種水肀取向材料和一種垂直取 向材料來形成_個均勻的溶液; b) 用這個溶液在基板上形成/層液體膜; c) 處理所述膜來形成一層變破的固體膜;以及 d)加工所述變硬的固體膜來得到一個統一的取向方 向。 在一個優選的實施例中,所述水平取向材料能夠在所 述取向層中提供一個第一預傾角,所述垂直取向材料能夠 在所述取向層中提供一個第二頓傾角。在整個說明書中使 用的“水平取向材料,,這個表達是指使液晶分子與其表面接 觸處取向0。的水平取向材料以及使液晶分子與其表面接觸 處取向大於0。的水平取向材料,例如,使液晶分子與其表 面接觸處取向一個大於0。的角的水平取向材料,可以到大 約12,11,1〇,9,8,7,6,5,4,3,2,1,〇_5或()‘1度°在整個說明書中使 用的“垂直取向材料,,這個表達是指使液晶分子與其表面接 觸處取向90。的垂直取向讨料以及使液晶分子與其表面接 觸處取向小於90。的垂直取雨材料’例如,使液晶分子與其 表面接觸處取向-個小於9G°的角的垂直取向材料’大約為 78,79,80,81,82,83,84,85,86,虬88,89,枞5,或89_9度。在-個 更為優選的實施例中,所述冑預傾角疋1 _1G並且第一預 …2524 1〇ΓδΠ2Γ] ggi^IggSlgrr 傾角是80°-90。。在一個進一步優選的實施例中所述第_ 預傾角是1。-8。並且第二預傾角是85。-90。。 所述水平取向材料可能全部地或至少部分地與所述垂 直取向材料溶混。 5 在另一個優選的實施例中,所述水平取向材料在混合 前被溶解到一個第一溶劑中《在另一個優選的實施例中, 所述垂直取向材料在混合前被溶解到一個第二溶劑中。 在另一個優選的實施例中,在步驟b)中形成的薄膜包 括所述垂直取向材料或所述水平取向材料的奈米結構。在 1〇另—個實施例中,所述奈米結構既包括所述水平取向材料 又包括垂直取向材料。所述奈米結構的大小是0-丨微米的量 級。 在另一個優選的實施例中,所述取向材料中的至少一 種义聚合體。在一個更為優選的實施例中,所述取向材料 15 中的至少一種是從包括聚醯亞胺,聚苯乙烯,聚甲基丙烯 酸甲酯,聚碳酸酯,聚醯胺酸和聚乙烯醇的/個組中選擇 出來的。在一個更為優選的實施例中,所述取向材料中的 至少—種是聚醯亞胺。在另一個實施例中,户斤述水平取向 材料和所述垂直取向材料都是聚醯亞胺。在/個最優選的 2〇 每t 實施例中,所述水平取向材料是JALS9203,所述垂直取向 材料是JALS202卜 在另一個優選的實施例令,所述第一和第二溶劑從包 括甲基-2-吡咯烷嗣I(NMP),二甲替甲醯胺(DlViF),丫-丁内酯 (YBL),丁基纖維素溶劑(BC)和THF(四氫呋喃)的一個組中 10 第93132205號申請案修正貝 101.01.12. 選出來。在一個更為優選的實施例中,所述第一溶劑包括 yBL ’ ;NMP和BC,所述第二溶劑包括丽j^BC。在一個最 優選的實施例中’所述第—和第二溶劑是包含在MLS92〇3 和JALS2021中的溶劑。 在另一個優選的實施例中,所述重量:所述水平取向 材料相對於所述垂直取向材料的重量的比率是丨:99到99 : 1。在一個更優選的實施例中,所述重量:所述水平取向材 料相對於所述垂直取向材料的重量的比率是丨:4到4 : j。 在另一個優選的實施例中,所述處理包括在80。-120。 的個第一供烤和在大約200。-250。的一個第二烘烤。在另 一個實施例中,所述處理是光處理。 在另一個實施例中’所述薄膜是通過旋塗法,絲網印 刷法,喷塗或喷墨印刷法形成。 在另一個實施例中’所述摩擦是通過一塊織物以一個 固定的方向的機械摩擦或通過用一個離子束在真空中以一 個固定的方向在一個固定的入射角照射所述表面來完成。 在另一個實施例中’所述基板是覆蓋銦錫氧化物的玻 璃。在一個優選的實施例中,所述銦錫氧化物在一個無源 矩陣顯示器中被排列成行和列的圖樣。在一個更為優選的 實施例中,所述基板包括用於有源矩陣驅動的一個薄膜電 晶體陣歹|J。 在本發明的另一個方面’提供為準備一個取向層而形 成—種溶液的處理,該取向層能夠提供在8。和85°之間的一 個第一預傾角。所述處理包括在一個溶劑中混合一個水平 1362524 號申請案漆iQi.oi 12~ 取向材料和一個垂直取向材料,其中所述水平取向材料能 夠在所述取向層中提供一個第一預傾角,並且所述垂直取 向材料能夠在所述取向層中提供一個第二預傾角。在一個 優選的實施例中,所述第一預傾角是〇°-1〇°,所述第二預傾 5角是80。-90。。在一個更為優選的實施例中’所述第一預傾 角是〇。-8。,所述第二預傾角是85。-90。。 在一個優選的實施例中,所述處理包括混合商業獲得 的水平和垂直取向材料。在一個更為優選的實施例中,所 述水平取向材料是JALS9203 ;並且所述垂直取向材料是 10 JALS-2021。 在另一個實施例中,所述溶劑能夠形成一個溶液,包 括奈米大小的液滴。在一個優選的實施例中,所述液滴或 者是水平的或者是垂直的取向材料。在另一個優選的實施 例中,所述液滴是垂直的還有水平的取向材料。 15 在本發明中,我們還公開了一種π晶胞,其不需要任何 偏壓並且總是處於彎曲變形,甚至於在零偏壓。沒有穩定 的斜展變形狀態。在後文中’這將被稱作“無偏壓彎曲,’晶 胞(no-bias bend, ΝΒΒ晶胞)。因此’這個新的π晶胞或ΝΒΒ 晶胞非常容易操作。由所述ΝΒΒ晶胞製造的液晶顯示器總 20的開啟_關閉切換時間不到2ms,開啟時間不到lms。所述光 學效率被優化到將近90%。這個NBB晶胞顯示器還能被光 學補償來具有類似于傳統冗晶胞的寬的視角。通過一個特殊 液晶取向層的發明,這個NBB晶胞有可能在液晶晶胞中生 成穩定的南預傾角。 12 1362524 y~^132205號申請案修正頁 ΙΟΙ.ΟΓΠ: 本發明的要點是所述ΝΒΒ晶胞❶這個ΝΒΒ晶胞通過取 向層的應用獲得’其可以為所述液晶分子提供大的預傾 角’在30°-70。範圍之内。 在本發明的另一方面,提供—個液晶晶胞,其包括: 5⑻互相面對的兩個基板;(b)密封在所述兩個基板之間的液 . 晶層,所述液晶層具有1微米到1〇微米的厚度;所述液晶層 . 包含具有正的介電異向性的液晶分子,即,f//>心;⑷提供 在所述基板内表面上的兩個取向層,朝向所述液晶層,為 了取向所述液晶層’所述取向層是固體薄膜的形式,厚度 10為lO-lOOnm。在所述液晶晶胞中,所述固體薄膜取向層包 含垂直取向材料和平行(水平)取向材料的混合物;所述固體 薄膜取向層能夠提供在與其接觸處的所述液晶分子的 30°-70°預傾角。 在本發明的另一個實施例中,提供一種液晶顯示器設 15備,包括⑷如上提到的所述NBB液晶晶胞;(b)設置在所述 第一基板後表面上的一個第一起偏器(p〇larizer)。在一個實 &例中所述第一起偏器是一個輸入起偏器。在另一個實 施例中’所述液晶設備包括設置在所述第二基板後表面上 的一個第二起偏器。在—個優選的實施例中,所述第二起 20偏器是-個輸出起偏器。在第3A圖中,所述第二起偏器也 被稱為檢偏器(analyzer)。 在另一個實施例中’如第3A圖所示的所述起偏角《和 γ ’與所述取向層的摩擦方向成正或負35。_55。角。在另一個 實施例中’所述液晶層的厚度在m米到雌米之間。在另 13 1362524 裏一93132205號申請案修正頁 101.01.12. 一個實施例中,所述液晶層包含具有正的介電異向性的液 晶分子,其中£7/ > Q。在另一個實施例中,所述取向層的厚 度為 10-200nm。 在另一個實施例中,與所述第一和第二取向層接觸的 * 5 所述液晶分子具有預傾角10°-80°。在一個優選實施例中, - 與所述第一和第二取向層接觸的所述液晶分子具有30°-70° 的預傾角。 在另一個實施例中,與所述第一和第二取向層接觸的 所述液晶分子的預傾角基本上相同。優選地,所述預傾角 10 在45°-90°範圍内。 在本發明的另一個實施例令,提供包括一個液晶晶胞 的一個彎曲狀態液晶顯示設備,包括: a. —個第一基板,其上具有一個第一取向層; b. —個第二基板,其上具有一個第二取向層; 15 C. —個液晶層,其夾心在所述第一和第二取向層之間, 所述第一取向層引出一個第一液晶預傾角A,其絕對值在 17°-60°,所述第二取向層引出一個第二液晶預傾角,其 絕對值在17°-60° ;所述(^和心定義在同一個坐標系中符號 相反,並且所述液晶層在零偏壓能夠維持一個穩定的彎曲 20 狀態。 在本發明的另一個方面,提供包括液晶晶胞的一個彎 曲狀態液晶設備,包括: a.—個第一基板,其上具有一個第一取向層,其被處理 來給出與所述第一取向層接觸的所述液晶分子的一個預傾 14 工 36252 第 93132205 號申 101.01.12 個方位角(azimuthal angle) A ; 声θι妒 衫〆個第一基板,其上具有·一個弟一"取向層,其被處 禮來修出與所述第二取向層接觸的所述液晶分子的一個預 個方位角心 1所述取向層的至少一個包括垂直取向材料和水平取 5 讨科的浪合物,所述垂直取向材料能夠提供85。-90。的預 所述水平取向材料能夠提供〇。-8。的預傾角; 0. η 丄〆個液晶層夾心在所述第一和第二取向層之間。 本發明的前兩個方面都包括一個實施例,其中所述液 晶設備的外和02滿足下述等式: (K3} -^.Xsin2^ +sin2^2) + 2(^-2^-2θ2Χκ33 +Κη) = 〇 - 在該等式中’ 是液晶的彎曲彈性常數,尺"是液晶的 斜展彈性常數。 在這兩個方面的一個優選實施例中,所述心和^基本上 15相同,並且在範圍30。-6〇。。在另一個優選的實施例中,當 時,所述仏和^是47±5。。在另—個實施例中, 當^/尤"=1.3時,心=17±5。以及仏=6〇±5。。 在這兩個方面的另一個實施例中,至少其中一個取向 層包括水平取向材料和垂直取向材料的混合物,所述水平 20取向材料能夠提供在與其接觸處的所述液晶分子的〇。_8。的 、員角料#絲向材料能夠提供在與其接觸處的所述 液晶分子的85。·90。的預傾角。在一個優選實施例中,所述 °曰的至夕個包括奈米大小的結構,大小為0-1微米。 在另-個優選實施例中,所述奈米大小結構包括所述水平 15 第93132205號申請案修正頁 101.01.12· 和垂直取向材料的至少一種。在一個更優選的實施例中, 所述取向層的水平取向材料是JALS92G3,並且所述取向層 的垂直取向材料是MLS-期。 &另個實施例中,包括液晶的所述液晶層具有一個 正的介電異向M . J。在一個優選實施例中,所述液晶層具有 在1_15微米之間的厚度。 在另一個實施例中,所述取向層是固體薄膜,具有厚 度 10-200nm。 10 在另一個實施例中’與所述第一和第二取向層接觸的 所述液晶分子鏡面對稱地傾斜。在另—個實施例中,在所 侧的所述預則以—種方式傾斜,使得當投射 到所述取向層的表面上時,所述預傾角的方向平行。 在另一個實施例中,所述基板中的至少一個是一個有 源矩陣底板,其包括以矩陣形式安排的薄膜電晶體。 在另一個實施例中’所述液晶層的處理是用一塊布機 械摩擦所述取向層。在另-個實施射,所述取向層的處 理疋光取向’通過暴露所述取向層到偏振光的-個紫外線 光束中進°在另—個實施例中所述取向層的處理是通 過個離子束在真空室中以一個角度照射所述取向層。 20 在另個實’中,所述液晶設備進一步包括一個輸 入和輸出起心。所述起偏轴被設置與所述液晶晶胞的取 向層的摩擦方向成正或負35。_55。角。在另一個實施例中 所述液晶設備進一 晶胞的外部。在另 步包括一個反射裝置,被置於所述液晶 —個實施例中,所述液晶設備進一步包 16 第93132205號申請 括-個反㈣置,其被置於所述液晶晶誠部的有源矩陣 底板上。在另一個實施例中,所述液晶設備進一步包括一 個補償延遲骐。 根據本發明的另一個方面,提供-個方法,用來在彎 曲狀態液W財生成—個敎的彎錄態。所述彎曲狀 態液晶設備包括—個第-基板,其上具有-個第-取向 曰^第〜基板,其上具有一個第二取向層。該方法包 括: 夾^有正的介電異向性的液晶在所述第一和第二 取向層之間; 弓 個第一液晶預傾角,在17。-60。的範圍内; c.引出個第二液晶預傾角在η。身的範圍内;以及 二向所述液晶在-個彎曲狀態,其在零偏壓電壓和 工作電壓保持穩定。 二 實%例令,所述預傾角通過提供取向層被引 出’该取⑽包括㈣提供在與其接财的所述液晶分子 on傾肖的水平取向射林關提供在與其接觸處的所 述液晶分子85°_%。龍角_直取向材料。 圖式簡單說明 第1A,1B和1C圖顯示了奸妨士& 一 了根據本發明一個方面的一個液 晶顯示設備的一部分的截面圖。 第2圖顯示了根據本發明 個方面的一個液晶晶胞 的一部分的截面圖。 第3圖顯示了在卡氏座標系中的液晶指向矢。 1362524 ιοΤόΓΤΙΓΊ I 第 93132205 號申语 第3Α圖顯示了根據本發明的另一個方面的起偏器,檢 偏器’光和觀察者相對於所述液晶晶胞的位置。 第4圖顯示了根據本發明的另一個方面的製作一個液 晶取向層的過程。 5 第5Α,5Β和5C圖是一組照片,顯示了根據本發明的另 一個方面’由液晶層作用劑形成的一層固體膜的奈米和微 米區域的例子。 第6Α圖顯示了根據本發明的另一個方面的’所述預傾 角和垂直取向材料(JALS2021)的濃度之間的關係。所述取 10 向膜由旋塗法形成。 第6Β圖顯示了根據本發明的另一個方面的’所述預傾 ;畜_ , 角和垂直取向材料(JALS2021)的濃度之間的關係° 所述取向膜由滾筒印刷法形成。 第7圖顯示了根據本發明的另一個方面的,所述極角& 15定能量和垂直取向材料(JALS2021)的濃度之間的關係 第8Α和8Β圖分別顯示了根據本發明的另〆方面的所 述液晶層的所述(Α)斜展和(Β)彎曲變形取向。 第9圖顯示了根據本發明的另一方面的一個浪晶層的 所述彎曲和斜展取向的所述彈性變形能量。 2〇 第1〇Α和10Β圖顯示了根據本發明的另一方面的在(Α) 零電壓和(Β)高電壓處的所述彎曲取向。 第11圖顯示了根據本發明的另一方面的由例4举備的 晶胞(1)的傳輸和電壓之間的關係。 第12Α和12Β圖是示波器描跡,顯示了根據本發明的另 18 1362524 ^93132205號申請索 一方面的由例4準備的晶胞⑴的切換動態特性。 第13圖是一個三維圖,顯示了根據本發明的另一方面 的反應時間(μδ) ’開始级別和結束級別的百分比之間的關 係’即’由例4準備的晶胞⑴從灰度(grey level)到灰度的切 5 換時間。 根據本發明的另一方面,第14圖顯示了根據例5準備的 晶胞(II)的傳輪和電壓之間的關係。 第15圖是一個三維圖,顯示了根據本發明的另一方面 的反應時間(μ8) ’開始級別和結束級別的百分比之間的關 10係,即’由例5準備的晶胞(Π)從灰度到灰度的切換時間。Application No. 93132205 In another preferred embodiment, the polar angle 鳊疋 energy on the orientation layer is between 5 x 1 (T4 J/cm 2 to 2.5 X1 〇 -3 J/cm 2 ). In another aspect of the invention, there is provided a method of fabricating an alignment layer in a liquid crystal cell comprising: a) dissolving a hydroquinone alignment material and a vertical alignment material in a solvent to form a uniform solution; Using this solution to form/layer a liquid film on the substrate; c) treating the film to form a layer of solid film that has broken; and d) processing the hardened solid film to obtain a uniform orientation. In a preferred embodiment, the horizontal alignment material is capable of providing a first pretilt angle in the alignment layer, the vertical alignment material being capable of providing a second dip in the alignment layer. As used throughout the specification, the term "horizontal orientation material" refers to a horizontal alignment material that orients liquid crystal molecules at a position where they are in contact with the surface thereof, and a horizontal alignment material that makes the alignment of the liquid crystal molecules in contact with the surface thereof greater than 0. For example, liquid crystal A horizontally oriented material that is oriented at a point where the molecule is in contact with its surface at an angle greater than 0. may be up to about 12, 11, 1 〇, 9, 8, 7, 6, 5, 4, 3, 2, 1, 〇 _5 or ( '1 degree ° "vertical alignment material used throughout the specification, this expression refers to the orientation 90 where the liquid crystal molecules are in contact with their surface. The vertical orientation of the material is such that the alignment of the liquid crystal molecules with their surface is less than 90. The vertical rain-receiving material 'for example, a vertical alignment material that makes the liquid crystal molecules in contact with the surface thereof - an angle of less than 9G°' is approximately 78, 79, 80, 81, 82, 83, 84, 85, 86, 虬 88 , 89, 枞 5, or 89_9 degrees. In a more preferred embodiment, the 胄 pretilt angle 疋 1 _1G and the first pre- 2524 1 〇Γ δ Π 2 Γ] ggi^IggSlgrr inclination angle is 80°-90. . In a further preferred embodiment the first pretilt angle is one. -8. And the second pretilt angle is 85. -90. . The horizontally oriented material may be miscible, either wholly or at least partially, with the vertical alignment material. In another preferred embodiment, the horizontally oriented material is dissolved into a first solvent prior to mixing. In another preferred embodiment, the vertically oriented material is dissolved to a second prior to mixing. In the solvent. In another preferred embodiment, the film formed in step b) comprises the nanostructure of the vertical alignment material or the horizontal alignment material. In another embodiment, the nanostructure includes both the horizontal alignment material and the vertical alignment material. The size of the nanostructure is on the order of 0-μm. In another preferred embodiment, at least one of the alignment materials is a polymer. In a more preferred embodiment, at least one of the alignment materials 15 is comprised of polyimine, polystyrene, polymethyl methacrylate, polycarbonate, polylysine, and polyvinyl alcohol. Selected in / group. In a more preferred embodiment, at least one of the oriented materials is a polyimide. In another embodiment, both the horizontally oriented material and the vertical alignment material are polyimine. In the most preferred embodiment, the horizontal alignment material is JALS 9203, and the vertical alignment material is JALS 202. In another preferred embodiment, the first and second solvents are from Base group of 2-pyrrolidine oxime I (NMP), dimethylformamide (DlViF), 丫-butyrolactone (YBL), butyl cellulose solvent (BC) and THF (tetrahydrofuran) The application for amendment No. 93132205 is selected from 101.01.12. In a more preferred embodiment, the first solvent comprises yBL '; NMP and BC, and the second solvent comprises 丽j^BC. In a most preferred embodiment, the first and second solvents are solvents contained in MLS92〇3 and JALS2021. In another preferred embodiment, the weight: the ratio of the horizontally oriented material to the weight of the vertically oriented material is 丨: 99 to 99:1. In a more preferred embodiment, the weight: the ratio of the horizontally oriented material to the weight of the vertical alignment material is 丨: 4 to 4: j. In another preferred embodiment, the processing is included at 80. -120. The first one is grilled and at about 200. -250. A second baking. In another embodiment, the process is light processing. In another embodiment, the film is formed by spin coating, screen printing, spray coating or ink jet printing. In another embodiment, the rubbing is accomplished by mechanical rubbing of a piece of fabric in a fixed direction or by illuminating the surface at a fixed angle of incidence with a beam of ions in a fixed direction in a vacuum. In another embodiment, the substrate is a glass covered with indium tin oxide. In a preferred embodiment, the indium tin oxide is arranged in a row and column pattern in a passive matrix display. In a more preferred embodiment, the substrate includes a thin film transistor array for active matrix driving. In another aspect of the invention, there is provided a process of forming a solution for preparing an alignment layer which can be provided at 8. A first pretilt angle between 85° and 85°. The treatment comprises mixing a level 1362524 application lacquer iQi.oi 12~ orientation material and a vertical alignment material in a solvent, wherein the horizontal alignment material is capable of providing a first pretilt angle in the alignment layer, and The vertical alignment material is capable of providing a second pretilt angle in the alignment layer. In a preferred embodiment, the first pretilt angle is 〇°-1〇° and the second pretilt 5 angle is 80. -90. . In a more preferred embodiment, the first pretilt angle is 〇. -8. The second pretilt angle is 85. -90. . In a preferred embodiment, the processing comprises mixing commercially available horizontal and vertical oriented materials. In a more preferred embodiment, the horizontal alignment material is JALS9203; and the vertical alignment material is 10 JALS-2021. In another embodiment, the solvent is capable of forming a solution comprising nanometer sized droplets. In a preferred embodiment, the droplets are either horizontal or vertical oriented materials. In another preferred embodiment, the droplets are vertical and horizontally oriented. In the present invention, we also disclose a π unit cell which does not require any bias and is always in bending deformation, even at zero bias. There is no stable oblique deformation state. In the following, this will be referred to as "unbiased bending," no-bias bend. Therefore, this new π unit cell or 晶 unit cell is very easy to operate. The cell-manufactured liquid crystal display has an on-off switching time of less than 2 ms and an on-time of less than 1 ms. The optical efficiency is optimized to nearly 90%. This NBB cell display can also be optically compensated to have a similar The wide viewing angle of the unit cell. Through the invention of a special liquid crystal alignment layer, this NBB unit cell may generate a stable south pretilt angle in the liquid crystal cell. 12 1362524 y~^132205 Application Revision Page ΟΓΠ.ΟΓΠ: Ben The gist of the invention is that the germanium unit cell, the germanium unit cell, obtains through the application of the alignment layer that it can provide a large pretilt angle for the liquid crystal molecules in the range of 30° to 70. In another aspect of the invention In one aspect, a liquid crystal cell is provided, comprising: 5 (8) two substrates facing each other; (b) a liquid crystal layer sealed between the two substrates, the liquid crystal layer having 1 micron to 1 micron Thickness; the liquid crystal layer Containing liquid crystal molecules having positive dielectric anisotropy, ie, f//>; (4) providing two alignment layers on the inner surface of the substrate toward the liquid crystal layer, in order to orient the liquid crystal layer The alignment layer is in the form of a solid film having a thickness of 10 to 100 nm. In the liquid crystal cell, the solid film alignment layer comprises a mixture of a vertical alignment material and a parallel (horizontal) alignment material; The alignment layer can provide a 30°-70° pretilt angle of the liquid crystal molecules in contact therewith. In another embodiment of the present invention, there is provided a liquid crystal display device comprising (4) the NBB liquid crystal as mentioned above a unit cell; (b) a first polarizer disposed on a rear surface of the first substrate. In a real case, the first polarizer is an input polarizer. In one embodiment, the liquid crystal device includes a second polarizer disposed on a rear surface of the second substrate. In a preferred embodiment, the second polarizer is an output a deflector. In Figure 3A, the second bias The device is also referred to as an analyzer. In another embodiment, the angles of "offsets" and "γ" as shown in Fig. 3A are positive or negative with respect to the rubbing direction of the alignment layer of 35. In another embodiment, the thickness of the liquid crystal layer is between m m and ym. In another 13 136 524, the application is amended on page 101.01.12. In one embodiment, the liquid crystal layer comprises A liquid crystal molecule having a positive dielectric anisotropy, wherein £7/> Q. In another embodiment, the alignment layer has a thickness of 10 to 200 nm. In another embodiment, the first The liquid crystal molecules which are in contact with the second alignment layer have a pretilt angle of 10° to 80°. In a preferred embodiment, - the liquid crystal molecules in contact with the first and second alignment layers have a pretilt angle of 30°-70°. In another embodiment, the pretilt angles of the liquid crystal molecules in contact with the first and second alignment layers are substantially the same. Preferably, the pretilt angle 10 is in the range of 45°-90°. In another embodiment of the present invention, a curved state liquid crystal display device including a liquid crystal cell is provided, comprising: a. a first substrate having a first alignment layer thereon; b. a second substrate Having a second alignment layer thereon; 15 C. a liquid crystal layer sandwiched between the first and second alignment layers, the first alignment layer extracting a first liquid crystal pretilt angle A, which is absolutely The value is between 17° and 60°, and the second orientation layer leads to a second liquid crystal pretilt angle, the absolute value of which is between 17° and 60°; the (^ and the heart are defined in opposite signs in the same coordinate system, and The liquid crystal layer can maintain a stable bend 20 state at zero bias. In another aspect of the invention, a curved state liquid crystal device including a liquid crystal cell is provided, comprising: a. a first substrate having a a first alignment layer processed to give a pretilt of the liquid crystal molecules in contact with the first alignment layer 36252 No. 93132205, 101.01.12 azimuthal angle A; sound θι妒a first substrate, Having a one-one orientation layer that is ritualized to modify a predetermined azimuth of the liquid crystal molecules in contact with the second alignment layer. At least one of the alignment layers includes a vertical alignment material and Level 5 is taken as a laminate, the vertical alignment material can provide 85-90. The pre-described horizontal alignment material can provide a pre-tilt angle of 〇. -8. η 丄〆 a liquid crystal layer sandwich The first two aspects of the present invention include an embodiment in which the outer sum 02 of the liquid crystal device satisfies the following equation: (K3} -^.Xsin2^ +sin2^ 2) + 2(^-2^-2θ2Χκ33 +Κη) = 〇 - In the equation ' is the bending elastic constant of the liquid crystal, and the ruler " is the oblique elastic constant of the liquid crystal. A preferred implementation in these two aspects In the example, the heart is substantially the same as 15 and is in the range of 30. -6. In another preferred embodiment, at the time, the 仏 and ^ are 47 ± 5. In another implementation In the example, when ^/尤 "=1.3, the heart = 17 ± 5 and 仏 = 6 〇 ± 5. In another implementation of these two aspects In an embodiment, at least one of the alignment layers comprises a mixture of a horizontal alignment material and a vertical alignment material capable of providing a ruthenium of the liquid crystal molecules at a position in contact therewith. A pretilt angle of 85.90 can be provided at the point of contact with the liquid crystal molecules. In a preferred embodiment, the 曰 个 包括 includes a nano-sized structure having a size of 0-1 micron. In another preferred embodiment, the nano-sized structure comprises at least one of the horizontally-edited page 101.01.12. In a more preferred embodiment, the horizontal alignment material of the alignment layer is JALS92G3, and the vertical alignment material of the alignment layer is MLS-phase. & In another embodiment, the liquid crystal layer including liquid crystal has a positive dielectric anisotropy M. J. In a preferred embodiment, the liquid crystal layer has a thickness of between 1 and 15 microns. In another embodiment, the alignment layer is a solid film having a thickness of 10-200 nm. In another embodiment, the liquid crystal molecules that are in contact with the first and second alignment layers are mirror-symmetrically inclined. In another embodiment, the pre-steps on the side are tilted in such a way that the directions of the pretilt angles are parallel when projected onto the surface of the orientation layer. In another embodiment, at least one of the substrates is an active matrix backplane comprising thin film transistors arranged in a matrix. In another embodiment, the treatment of the liquid crystal layer is to mechanically rub the alignment layer with a piece of cloth. In another embodiment, the alignment of the alignment layer is performed by exposing the alignment layer to the ultraviolet light beam of the polarized light. In another embodiment, the processing of the alignment layer is performed. The ion beam illuminates the alignment layer at an angle in a vacuum chamber. In another embodiment, the liquid crystal device further includes an input and output centering. The polarizing axis is set to be positive or negative 35 with respect to the rubbing direction of the alignment layer of the liquid crystal cell. _55. angle. In another embodiment the liquid crystal device is external to a unit cell. Further comprising a reflective device disposed in the liquid crystal embodiment, wherein the liquid crystal device further includes an anti-(four) arrangement, which is placed in the liquid crystal The source matrix is on the bottom plate. In another embodiment, the liquid crystal device further includes a compensation delay 骐. According to another aspect of the present invention, there is provided a method for generating a curved recording state in a curved state. The curved liquid crystal device includes a first substrate having a first-orientation substrate and a second alignment layer thereon. The method includes: sandwiching a liquid crystal having a positive dielectric anisotropy between the first and second alignment layers; and bowing a first liquid crystal pretilt angle at 17. -60. Within the range; c. Lead a second liquid crystal pretilt angle at η. Within the range of the body; and the two-way liquid crystal is in a bent state, which is stable at zero bias voltage and operating voltage. In the case of the second embodiment, the pretilt angle is extracted by providing an alignment layer, which includes (4) providing a horizontally-oriented liquid crystal on which the liquid crystal molecules that are converged are provided to provide the liquid crystal at a position in contact therewith. Molecular 85°_%. Long angle _ straight orientation material. BRIEF DESCRIPTION OF THE DRAWINGS Figs. 1A, 1B and 1C show a cross-sectional view of a portion of a liquid crystal display device in accordance with one aspect of the present invention. Fig. 2 is a cross-sectional view showing a portion of a liquid crystal cell according to aspects of the present invention. Figure 3 shows the liquid crystal director in the Cartesian coordinate system. 1362524 ιοΤόΓΤΙΓΊ I Patent No. 93132205 Figure 3 shows a polarizer according to another aspect of the invention, the position of the detector & the viewer relative to the liquid crystal cell. Fig. 4 shows a process of fabricating a liquid crystal alignment layer in accordance with another aspect of the present invention. 5 Figures 5, 5 and 5C are a set of photographs showing examples of nano and micro-regions of a solid film formed of a liquid crystal layering agent according to another aspect of the present invention. Fig. 6 is a view showing the relationship between the concentration of the pretilt angle and the vertical alignment material (JALS2021) according to another aspect of the present invention. The 10-way film is formed by spin coating. Fig. 6 is a view showing the relationship between the concentrations of the pretilt, the horn, and the vertical alignment material (JALS2021) according to another aspect of the present invention. The alignment film is formed by a roll printing method. Figure 7 is a view showing the relationship between the polar angle & 15 concentration of the energy and the vertical alignment material (JALS2021) according to another aspect of the present invention. Figs. 8 and 8 respectively show another according to the present invention. The (Α) oblique and (Β) bending deformation orientation of the liquid crystal layer of the aspect. Figure 9 is a graph showing the elastic deformation energy of the curved and oblique orientation of a wave layer according to another aspect of the present invention. 2〇 Figures 1 and 10 show the bending orientation at (Α) zero voltage and (Β) high voltage in accordance with another aspect of the present invention. Fig. 11 is a view showing the relationship between the transmission and the voltage of the unit cell (1) taught by Example 4 according to another aspect of the present invention. The 12th and 12th views are oscilloscope traces showing the switching dynamics of the unit cell (1) prepared by the example 4 on the one hand according to another aspect of the invention. Figure 13 is a three-dimensional diagram showing the relationship between the reaction time (μδ) 'the start level and the percentage of the end level' in accordance with another aspect of the present invention 'i' from the unit cell prepared by Example 4 (1) from gray scale (grey level) to grayscale cut 5 change time. According to another aspect of the present invention, Fig. 14 shows the relationship between the transfer wheel and the voltage of the unit cell (II) prepared according to Example 5. Figure 15 is a three-dimensional diagram showing the relationship between the start time and the percentage of the end level of the reaction time (μ8) according to another aspect of the present invention, that is, the unit cell prepared by the example 5 (Π) Switching time from grayscale to grayscale.
C實施方式;J 較佳實施例之詳細說明 兩個角“基本上相同”是指所述兩個角相差少於5。;優 選地’少於3。;最有選地,少於1。。這裏的“絕對值,,是指一 15 個實數的數值,而不考慮其符號。例如,-4的絕對值是4。 也叫作數值。 參考第1A圖’顯示了液晶顯示器的一部分,包括一個 液晶晶胞1和兩個起偏器2和3。所述箭頭指示通過所述液晶 晶胞的光徑。第1B圖顯示了具有兩個延遲膜13,14的穿透 2〇 式液晶晶胞,這兩個膜用來補償色散並改善所述液晶顯示 器的視角。所述箭頭指示通過所述液晶晶胞的光徑。第1C 圖顯示了一個反射液晶晶胞的一部分,其具有一個延遲膜 13,並且提供一個外部鏡面12。或者’第1C圖中的反射鏡 面能夠被形成在所述液晶晶胞内部作為無源和矩陣驅動顯 19 1362524 第93132205號申請案修IqOTT? 示器的象素結構的-部分°或者’提供延遲膜14而不是13。 所述兩個箭頭指示所述晶胞的光徑。 在第2圖中,顯米了沒有施加電壓時的一個液晶晶胞, 包括頂部基板4和底部基板5 ;兩個透明的導電電極6和7 ’ 5 —個頂部取向層8和/個底部取向層9 ’ 一個液晶層1〇。在 • 液晶分子10A的第一層和所述底部取向層9的表面之間形成 的角A被稱作第一預傾角。在液晶分子10B的第一層和所述 頂部取向層8的表面之間形成的角Θ2被稱作第二預傾角。0; 和^可以基本上相同或者不同。在這個液晶顯示器中,所 10 述基板4和5可以由玻璃製成。所述玻璃基板中的一個,如 5,可以是帶有薄膜電晶體陣列的一個有源矩陣底板。或 者’所述基板中的一個,如4,可以由玻璃製成,而另一個 基板5可以是不透明的材料,如矽。在這種情況下,可以在 所述矽基板上構造一個有源矩陣陣列。如果兩塊基板都是 15 由玻璃製成,所述液晶顯示器可以在穿透模式或透反射式 模式工作。如果所述基板中的一個是不透明的,所述液晶 顯示器只能在反射式模式工作,所述反射鏡被構造作為所 述液晶晶胞内部的所述有源矩陣結構的一部分。 第一優選實施例的其他要素之一是所述液晶層1〇,其 20央心在所述基板之間。通過所述液晶晶胞内部的間隔器(未 示出),所述液晶層的厚度被固定。所述液晶層的最重要的 參數是在邊界與所述取向層的所述預傾角。當不施加電壓 時’攻些預傾角<9/和<92決定所述液晶層1〇的⑽和㈣參閱 第3®)°這裏’為了簡便,我們假設所述角只依賴於一個 20 1362524 101.01.12. % 93132205^?glgT^ 變數Z ’其是到所述液晶晶胞的垂直方向上的距離,如第3 圖所示。一般地,Θ和#可以是(X ’ y,z)的函數。但是,在 廷裏,它不影響本發明的表達。 這個液晶層通過具有方向0和0的一個液晶指向矢表 5徵’ ^和炎分別是極角(polar angle)和方位角(azimuthal angle)在第3圖中示出。在本發明中,0還指傾斜角(仙 angle)。所述傾斜角在與所述取向層的邊界,和$⑷被 稱為預傾角。所述指向矢的取向,即,Θ⑻和〆以的值決定 所述液晶晶胞的光學特性。它基本上決定了所述液晶晶胞 10的穿透率和反射率。如第3圖所示,液晶分子η的所述指向 矢由一個預傾角(傾斜角)Ρ和一個預傾角方向(扭轉角決 疋,0對應於所述指向矢η的一個極角,$對應於它的一個方 位角液日a分子的所述指向矢η的所述Cartesian坐標系被定 義為: 15 n=(cos0cos^5 cos0sin0,sin0) 液晶的所述指向矢n可以被確定,通過在所述基板上進 行取向處理來控制所述預傾角辨σ所述預傾角方向彡。 由所述液晶晶胞進行的光的傳輸或反射通過所述起偏 器角α和所述檢偏器角γ決定,如第3Α圖所示,以及由所述 20的液晶層10的所述取向條件決定。所述電極ό,7和所述取 向層8,9被用來控制所述液晶層1〇的所述取向條件。所述 電極提供電壓來控制所述%ζ)和辦^值。所述取向層和它們 的處理決定和#Φ的值’其中d是所述液晶晶胞的厚 度。本質上,_是A而⑽是的,如前所述。它們是等價 21 1362524 百^132205號甲請案修正負 ΙΟΙ.ΟΤΤ^] 的符號。0(¾)和以及(9从)和多(¾)的所述值和所述彈性 Euler’s等式一起,決定%z;和多(¾)的解。所述液晶層的所述 取向的物理意義在現有技術中是公知的,在文獻中也有介 紹’如Springer在1994年出版的由Blinov和Chigrinov寫的專 5 論“Electrooptic Effects in Liquid Crystal Materials”。和 0(0)被認為是液晶取向的易取向軸。 應該注意的是,在所述表面上所述液晶的真實的取向 方向還依賴於取向表面的錨定能量。所述錨定能量是錫定 條件有多強的一個測量《如果所述錨定能量很大,就很難 10從這個條件偏離,而取向角是由易取向軸的方向給出。對 於弱錨定,在所述表面的液晶的真實角度可以偏離外和 Φ(〇)。 ' 顯而易見地,和#0)以及代4和的所述值或正 好在所述取向層附近的所述液晶分子的取向在設計所述液 15晶晶胞的光電特性中很重要。所述液晶分子的取向能夠通 過很多裝置得到,並且在液晶物理學和工程領域中是一個 被报好地研究的問題。所述預定的取向條件一般,例如, 通過摩擦取向層8、9得到。 八所述取向層被處理使得它們能夠取向在其附近的液晶 刀子所述處理大多由機械摩擦完成。有時也會採用其他 的技術,如,光取向或離子束取向。為了本發明的公開, 我們不限於任何-種取向技術。對於下面的討論,我們使 用摩擦作為所述取向層處理的一個例子。 在所述取向層上的摩擦方向決定蝴和_,而所述預 22 1362524 第9313乏2〇5號申請案修正頁 Γ^Γ^ΤΤΰ~~] 傾角(9(¾)和外Θ的值主要由所述取向層8、9的材料特性決 定。有平行取向材料,如,聚醯亞胺,其可以為生產扭曲 向列(TN)和超級扭曲向列(stn)液晶顯示器提供丨。_8。的預 傾角。這種材料還被稱作水平取向材料。還有材料能夠為 5生產向列型垂直取向(vertically aligned nematic, VAN)液晶 顯示器提供預傾角為85。-90。的垂直取向。這種材料還可稱 . 作垂直取向材料。這些平行和垂直材料可商業上獲得。报 多發明已經公開了不同種類的化學製品,它們可以提供水 平或垂直取向。但是應該注意的是,這些取向層只能提供 10 接近水平或接近垂直取向。不可能得到處於水平或垂直之 間的取向極角(alignment polar angles)。具體而言,在實踐 中,沒有已知的聚醯亞胺取向辞料可以提供接近45。的預傾 角’雖然過去有宣稱可以得到這種預傾角。這些聚醯亞胺 取向材料已經很好地服務於液晶顯示器工業。大量地用於 15製造實際的液晶顯示器(LCD)。 在這個第一優選實施例中,所述取向層8,9被特殊處 理,使所述液晶層10具有一個高預傾角。第3圖顯示了用來 視覺化不同角度的坐標系。這個坐標系用於描述整個液晶 晶胞中的η、必⑻、和0问。對於一個傳統的兀晶胞,戶列d), 20 並且與A相同)和與込相同)正負值相反。這可通過 平行摩擦所述頂部和底部取向層簡單地得到。在這個第一 優選實施例中,所述預傾角可造成一個穩定的π晶胞,即使 在沒有施加電壓的情況下。換而言之,必和込的值足夠大使 得所述晶胞的穩定結構是一個彎曲晶胞,即使沒有電壓施 23 1362524C. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT Two angles "substantially the same" mean that the two angles differ by less than five. ; preferably 'less than 3. Most preferred, less than 1. . Here, "absolute value, refers to a value of 15 real numbers, regardless of its sign. For example, the absolute value of -4 is 4. Also called a numerical value. Refer to Figure 1A' to show a part of the liquid crystal display, including a liquid crystal cell 1 and two polarizers 2 and 3. The arrows indicate the optical path through the liquid crystal cell. Figure 1B shows a penetrating 2 液晶 liquid crystal with two retardation films 13, 14. The two films are used to compensate for the dispersion and improve the viewing angle of the liquid crystal display. The arrows indicate the optical path through the liquid crystal cell. Figure 1C shows a portion of a reflective liquid crystal cell with a delay Membrane 13 and an external mirror 12 is provided. Or the mirror surface in Fig. 1C can be formed inside the liquid crystal cell as a passive and matrix driven display 19 1362524 No. 93132205 application IqOTT? The portion of the prime structure or 'provides a retardation film 14 instead of 13. The two arrows indicate the optical path of the unit cell. In Fig. 2, a liquid crystal cell is used when no voltage is applied, including Top substrate 4 and bottom Substrate 5; two transparent conductive electrodes 6 and 7' 5 - a top alignment layer 8 and / a bottom alignment layer 9 'a liquid crystal layer 1 〇. In the first layer of the liquid crystal molecules 10A and the bottom alignment layer 9 The angle A formed between the surfaces is referred to as a first pretilt angle. The corner 2 formed between the first layer of the liquid crystal molecules 10B and the surface of the top alignment layer 8 is referred to as a second pretilt angle. ^ can be substantially the same or different. In this liquid crystal display, the substrates 4 and 5 can be made of glass. One of the glass substrates, such as 5, can be an active with a thin film transistor array. a matrix backplane. Or one of the substrates, such as 4, may be made of glass, and the other substrate 5 may be an opaque material, such as germanium. In this case, a structure may be constructed on the germanium substrate. Active matrix array. If both substrates are made of glass, the liquid crystal display can operate in a transmissive mode or a transflective mode. If one of the substrates is opaque, the liquid crystal display can only In reflective mode The mirror is configured as part of the active matrix structure inside the liquid crystal cell. One of the other elements of the first preferred embodiment is the liquid crystal layer 1 〇 20 centered on the substrate The thickness of the liquid crystal layer is fixed by a spacer (not shown) inside the liquid crystal cell. The most important parameter of the liquid crystal layer is the pretilt angle at the boundary and the alignment layer. When no voltage is applied, 'spread some pretilt angles' 9/ and <92 determine the liquid crystal layer 1〇 (10) and (4) refer to the 3®)° Here, for the sake of simplicity, we assume that the angle depends only on one 20 1362524 101.01.12. % 93132205^?glgT^ The variable Z' is the distance in the vertical direction to the liquid crystal cell, as shown in Fig. 3. In general, Θ and # can be functions of (X y y, z). However, in the court, it does not affect the expression of the present invention. This liquid crystal layer is shown in Fig. 3 by a liquid crystal director having directions 0 and 0, and the inflammation is a polar angle and an azimuthal angle, respectively. In the present invention, 0 also refers to a tilt angle. The tilt angle is at the boundary with the orientation layer, and $(4) is referred to as the pretilt angle. The orientation of the directors, i.e., the values of Θ(8) and 〆, determine the optical properties of the liquid crystal cell. It basically determines the transmittance and reflectance of the liquid crystal cell 10. As shown in Fig. 3, the director of the liquid crystal molecule η is composed of a pretilt angle (inclination angle) Ρ and a pretilt angle (torsion angle 疋, 0 corresponds to a polar angle of the director η, $ corresponds The Cartesian coordinate system of the director η of one azimuth liquid a molecule is defined as: 15 n=(cos0cos^5 cos0sin0, sin0) The director n of the liquid crystal can be determined by An orientation treatment is performed on the substrate to control the pretilt angle σ. The pretilt direction 彡. The transmission or reflection of light by the liquid crystal unit passes through the polarizer angle α and the analyzer angle The γ is determined as shown in Fig. 3, and is determined by the orientation condition of the liquid crystal layer 10 of the 20. The electrode ό, 7 and the alignment layers 8, 9 are used to control the liquid crystal layer 1〇. The orientation condition. The electrode provides a voltage to control the % ζ) and the value. The alignment layers and their processing determine the value of #Φ' where d is the thickness of the liquid crystal cell. Essentially, _ is A and (10) is, as mentioned earlier. They are equivalent to 21 1362524 hundred ^ 132205 No. A request to correct the negative ΙΟΙ. ΟΤΤ ^] symbol. The values of 0 (3⁄4) and (9 from) and multiple (3⁄4), together with the elastic Euler's equation, determine %z; and multiple (3⁄4) solutions. The physical meaning of the orientation of the liquid crystal layer is well known in the prior art and is also described in the literature by "Electrooptic Effects in Liquid Crystal Materials" by Blinov and Chigrinov, published by Springer in 1994. And 0(0) is considered to be an easy orientation axis of liquid crystal orientation. It should be noted that the true orientation of the liquid crystal on the surface also depends on the anchoring energy of the oriented surface. The anchoring energy is a measure of how strong the tinning condition is. "If the anchoring energy is large, it is difficult to deviate from this condition, and the orientation angle is given by the direction of the easy orientation axis. For weak anchoring, the true angle of the liquid crystal on the surface can deviate from the outer sum Φ(〇). It is apparent that the value of the sum #0 and the sum of 4 and the orientation of the liquid crystal molecules just in the vicinity of the alignment layer are important in designing the photoelectric characteristics of the liquid crystal cell. The orientation of the liquid crystal molecules can be obtained by many devices and is a well-researched problem in the field of liquid crystal physics and engineering. The predetermined orientation conditions are generally obtained, for example, by rubbing the alignment layers 8, 9. Eight of the alignment layers are processed such that they can be oriented in the vicinity of the liquid crystal knives. The treatment is mostly done by mechanical friction. Other techniques, such as photo-orientation or ion beam orientation, are sometimes used. For the disclosure of the present invention, we are not limited to any of the orientation techniques. For the following discussion, we use friction as an example of the alignment layer treatment. The rubbing direction on the orientation layer determines the butterfly and _, and the pre-22 1362524 is the 9931 lacking the application number of the 〇^Γ^ΤΤΰ~~] dip angle (9 (3⁄4) and the value of the outer Θ Mainly determined by the material properties of the alignment layers 8, 9. There are parallel alignment materials, such as polyimides, which can provide germanium for the production of twisted nematic (TN) and super twisted nematic (stn) liquid crystal displays. The pretilt angle. This material is also referred to as a horizontally oriented material. Also, the material is capable of providing a vertical orientation of a pretilt angle of 85 to 90 for a vertically oriented nematic (VAN) liquid crystal display. Such materials can also be referred to as vertical alignment materials. These parallel and vertical materials are commercially available. Many inventions have disclosed different types of chemicals that can provide horizontal or vertical orientation. However, it should be noted that these orientations The layer can only provide 10 near horizontal or near vertical orientation. It is not possible to obtain alignment polar angles between horizontal or vertical. Specifically, in practice, there is no known polyimine extraction. The revelation can provide a pretilt angle close to 45. Although it has been claimed in the past to obtain such a pretilt angle, these polyimine orientation materials have been well served by the liquid crystal display industry. A large number of 15 are used to manufacture practical liquid crystal displays ( LCD). In this first preferred embodiment, the alignment layers 8, 9 are specially treated to provide the liquid crystal layer 10 with a high pretilt angle. Fig. 3 shows a coordinate system for visualizing different angles. This coordinate system is used to describe η, (8), and 0 in the entire liquid crystal cell. For a conventional germanium unit cell, the d), 20 and the same as A) and the same as the positive and negative values. This is simply obtained by rubbing the top and bottom alignment layers in parallel. In this first preferred embodiment, the pretilt angle can result in a stable π unit cell even when no voltage is applied. In other words, the value of must and 込 is large enough that the stable structure of the unit cell is a curved unit cell, even if there is no voltage applied 23 1362524
[£93132205 號申 101.01.12. I 加到所述液晶晶胞。這與一般的冗晶胞不同,其所述液晶晶 胞的零電壓取向是一個斜展晶胞,並且需要一個偏壓和轉 化方法來維持所述彎曲取向。 第4圖顯示了根據本發明一個方面的所述液晶取向層 5 的製作過程的一個實施例。在步驟1,一個垂直取向材料40 在溶劑A中稀釋,溶劑A能與所述垂直取向材料4〇完全溶 混,形成一個垂直材料溶液42。在步驟2,所述垂直溶液42 和一種水平取向材料44都溶解在一種溶劑c中,形成一個最 終的混合物46。或者在可選步驟2,中,所述水平取向材料 10 44首先溶解在一種溶劑B中,在與所述垂直材料溶液42在溶 劑C中混合之前,形成一個水平材料溶液45。在步驟3,所 述混合溶液46被塗到一塊基板上來形成一層固體膜48。所 - 述固體膜48就被熱處理,其包括步驟4中的預烤和最終的丈共 · 烤處理來$成一層硬的固體膜50。所述硬的固體膜具有 15 1〇ηΠ1 3〇〇nm的厚度。所述硬的固體膜50在步驟5中被摩 擦X生成所需的液晶取向層52 〇所述摩擦可以通過機械 摩擦進饤’其包括以—塊織物在—個固㈣方向上施力。 以上提到的處理只是本發明的實施例。存在很多其他 的方法來實施本發明,這些都是本領域技術人員公知的。 2〇例如’所述步驟4中的處理過程也可以用光處理進行 。所述 步驟5中的摩擦也可以通過一個離子束在真空中以一個固 疋方向在一個固定入射角照射所述取向層的表面來進行。 還可此在可選步驟3’中,從溶液46首先獲得一層液體膜 47 ’然後在步驟3”中’所述液體膜就被處理以得到固體膜 24 1362524 第9313^20^號申請案修正頁 48。乾燥所述液體膜來獲得所述固體膜的方法也會影響從 上述處理中得到的預傾角。 通過在所述液晶晶胞的兩側平行摩擦’形成一個傳統 的π晶胞。滿足這些邊界條件的巧*能的指向矢取向是所述斜 5展變形(S-狀態),所述彎曲變形(Β_狀態)’以及所述11扭轉 變形(Τ-狀態)。當施加一個高電塵時,所述Β-狀態變成所述 . 垂直取向(Η-狀態)。在一個傳統的π晶胞中’所述預傾角小 於10。。這樣’所述S-狀態具有較低的彈性變形能量,因此 更穩定。從這個更穩定的S-狀態到所述Β-狀態的轉化需要 10 使用所述π晶胞。(參閱’例如’ E J Acosta等人,The role surface tilt in the operation of pi-cell liquid crystal devices,[£93132205 application 101.01.12. I is added to the liquid crystal cell. This is in contrast to a general hard cell in which the zero voltage orientation of the liquid crystal cell is a diagonal cell and a biasing and conversion method is required to maintain the bend orientation. Fig. 4 shows an embodiment of a process of fabricating the liquid crystal alignment layer 5 according to an aspect of the present invention. In step 1, a vertical alignment material 40 is diluted in solvent A, and solvent A is completely miscible with the vertical alignment material 4, to form a vertical material solution 42. In step 2, both the vertical solution 42 and a horizontal alignment material 44 are dissolved in a solvent c to form a final mixture 46. Alternatively, in optional step 2, the horizontal alignment material 10 44 is first dissolved in a solvent B, and a horizontal material solution 45 is formed before being mixed with the vertical material solution 42 in the solvent C. In step 3, the mixed solution 46 is applied to a substrate to form a solid film 48. The solid film 48 is heat treated and includes a pre-bake in step 4 and a final co-bake treatment to form a hard solid film 50. The hard solid film has a thickness of 15 1 〇 Π 〇〇 13 〇〇 nm. The hard solid film 50 is rubbed in step 5 to form a desired liquid crystal alignment layer 52. The friction can be mechanically rubbed into the 饤' which includes applying a force in a solid (four) direction. The above mentioned processing is only an embodiment of the present invention. There are many other ways to implement the invention, which are well known to those skilled in the art. 2, for example, the processing in step 4 can also be carried out by light processing. The rubbing in the step 5 can also be carried out by irradiating an ion beam in a vacuum in a solid direction at a fixed incident angle to illuminate the surface of the alignment layer. It is also possible in this optional step 3' to first obtain a liquid film 47' from solution 46 and then in step 3" the liquid film is processed to obtain a solid film 24 1362524 No. 9313^20^ application amendment Page 48. The method of drying the liquid film to obtain the solid film also affects the pretilt angle obtained from the above treatment. A conventional π unit cell is formed by rubbing in parallel on both sides of the liquid crystal cell. The director orientation of these boundary conditions is the oblique deformation (S-state), the bending deformation (Β_state)', and the 11 torsional deformation (Τ-state). When a high is applied In the case of electric dust, the Β-state becomes the vertical orientation (Η-state). In a conventional π unit cell, the pretilt angle is less than 10. Thus the 'S-state has lower elasticity The deformation energy is therefore more stable. The conversion from this more stable S-state to the Β-state requires 10 to use the π unit cell (see 'eg 'EJ Acosta et al., The role surface tilt in the operation of Pi-cell liquid crystal devices,
Liquid crystals, vol 27,p 977,2000; S H Lee等人,Chiral doped optically-compensated bend nematic liquid crystal cell with continuous deformation from twist to twist-bend state, 15 Japanese J of Applied Physics, vol 40, p L389, 2001; S H Lee 等人,Geometric structure for the uniform splay to bend transition in a pi-cell, Japanese J Applied Physics, vol 42, p L1148, 2003)。因為所述s和B變形不是拓撲等價的,需要發 生有核的轉換。初始的S-狀態到B-狀態的所述“條件”是研 2〇 究的主要領域。已經提出了很多方法,包括引入突起和添 加手性分子摻雜物《同樣,為了所述π晶胞只在所述B-狀態 正常工作,要維持一個偏壓。 這樣,在傳統的π晶胞中,所述S-狀態變形比所述Β-狀 態變形更穩定,因為小的預傾角。在本發明中,我們公開 25 1362524 i〇r〇n^ 第 93132205 號辛胥 一種新方法來產生更加穩定的Β-狀態變形,即使在零偏壓β 眾所周知’無扭曲液晶晶胞的每單位面積的彈性能量 由下式給出Liquid crystals, vol 27, p 977, 2000; SH Lee et al, Chiral doped optically-compensated bend nematic liquid crystal cell with integrated deformation from twist to twist-bend state, 15 Japanese J of Applied Physics, vol 40, p L389, 2001; SH Lee et al., Geometric structure for the uniform splay to bend transition in a pi-cell, Japanese J Applied Physics, vol 42, p L1148, 2003). Since the s and B variants are not topologically equivalent, a nucleus transition is required. The "conditions" of the initial S-state to the B-state are the main areas of research. A number of methods have been proposed, including the introduction of protrusions and the addition of chiral molecular dopants. Similarly, a bias voltage is maintained for the π unit cell to operate normally only in the B-state. Thus, in the conventional π unit cell, the S-state deformation is more stable than the Β-state deformation because of the small pretilt angle. In the present invention, we disclose a new method of 25 1362524 i〇r〇n^ No. 93132205 to produce a more stable Β-state deformation, even at zero bias β known as 'no distortion liquid crystal cell per unit area The elastic energy is given by
cos2 0+KSisin2 Θ )承 dz 5 其中尺"和尺33分別是斜展和彎曲彈性常數。0是所述傾 斜角’其為所述晶胞内部的距離z的一個函數。在幾乎 是線性分佈的條件下(對於大多數液晶材料成立),所述3晶 胞和所述S晶胞的能量可以被計算。它們在第9圖中示出。 可以很清楚地看到,如果所述預傾角增加,將有助於B-變 10 形。然而,在傳統的LCD構造技術中,很難製造大於1〇。的 高預傾角。 我們可以很容易地估計形成所述B晶胞所需要的預傾 角。如果在所述液晶層兩側的所述預傾角分別是的和込,如 果滿足下述條件,所述斜展和彎曲晶胞將具有相同的彈性 15能量: iK33 -K„ \sin20, +sin292 ]+2(π-2θ, -2Θ2 \Κ33 +Κ„ )=〇 如果在所述晶胞兩側的所述預傾角相同並且等於θ,, 上述條件可以被簡化成: (K33 -K„ )sin2e, +(π-4θ, \Κ33 ^Κ„ )=〇 20 通過解這個等式,可以得到使得所述斜展和彎曲變形 能量相同的所述預傾角的條件。例如’對於 p-methyoxybenzylidene-p'-butylaniline (MBBA) * K32IKt]= 1.3,因此,込大約是47。。它也符合第9圖中顯示的圖表。 26 1362524 第93132205號申請案修正貢一 -ι〇丨.〇ι 12 一般地’可以看到,對於4/Λ:"的所有的值,的總是在45。 和58°之間。這樣’如果在所述液晶晶胞上的所述預傾角比 臨界角大’所述彎曲變形將比所述s_變形更穩定。換而言 之’所述液晶晶胞將總是處於所述B_狀態。這是沒有偏壓 5下的π晶胞。我們稱之為無偏壓彎曲(NBB)晶胞。對於不對 稱的液晶晶胞’在一側的所述預傾角可以比的小,並且在 另一側的所述預傾角必須比的大。例如,如果的是3〇。,則 根據上述等式,込須比67。大,如果尺//= 1.3。 構造這樣一個π晶胞的重要步驟是所述高預傾角取向 10層的準備。過去曾經介紹了很多技術,用來在一個液晶晶 胞中得到高預傾角。這包括Si〇x蒸鍍,離子束,光控取向 技術和反向機械摩擦。在本發明中,我們結合所述兀晶胞和 一種特殊技術,其可以生成我們發明的一個高預傾角。 本發明中得到這樣高預傾角的方法是摩擦一個經特殊 I5準備的取向層。液晶晶胞被取向層8和9取向。這些特殊取 向層的準備細節已經在上文中結合第4圖進行了描述。當一 個垂直取向材料和一個水平取向材料在溶液中以合適的比 例混合時,有可能形成一個取向層,其可以生成任何角度 的預傾角。第6A和6B圖顯示了針對這個實施例的實驗結 20果。在該圖中,顯示了通過將所述垂直取向材料,在這種 情況下,其是從Japan Synthetic Rubber公司得到的商業材 料,貨號為JALS2021,和一種水平取向材料混合,如 JALS9203,有可能得到1〇。-8〇。任何值的預傾角。 第6A和6B圖中指示的所述預傾角對於相同的溶液混 27 第93132205號申請案修正頁 口物不樣匕表明可得到的預傾角依賴於所述固體取向 層的準備方法在第6a圖中,使用—種旋塗技術來準備所 述固體取向層在第6B圖中,使用滾筒塗層以及隨後快速 加”’、的方..來準備所述固體膜。有很多其他方法來從所述 冷液形成所述取向層的—層薄膜。有可能,例如,使用絲 ,.同印刷法噴墨印刷法,浸人塗層或刮墨刀技術來形成所 述薄膜。為1本發明的公開,我們只使用㈣印刷和旋塗 的例子彳一疋所有其他的技術都包含在本發明的一部分 中。可以說,對於準備隨膜的每—種方法,存在可得到 的預傾角相對於溶液混合比率的唯—依賴心在初始準備 之後的所述固體膜的處理可以通過熱的裝置來執行,如, 放置所述基板在一個加熱的爐子内,或通過光處理照射強 紫外線光到所述液體臈上。 如果所述預傾角大於40。,將會得到所述彎曲結構,即 使在沒有電壓的情況下。如果所述取向層的摩擦取向條件 是平行的,就得到一個π晶胞或彎曲取向晶胞。如果所述輸 入起偏器和輸出起偏器2 ’ 3和所述液晶晶胞摩擦方向成45。 和-45°角,所述π晶胞的傳輸由下列等式給出 T=sin2~{An( z )dz Λο 其中λ是波長,d是所述液晶層的厚度並且Δη是所述液 晶層的雙折射,其依賴於所述取向條件如Cos2 0+KSisin2 Θ ) bearing dz 5 where the ruler " and the ruler 33 are the oblique and bending elastic constants, respectively. 0 is the tilt angle 'which is a function of the distance z inside the unit cell. Under conditions of almost linear distribution (established for most liquid crystal materials), the energy of the 3 cells and the S unit cells can be calculated. They are shown in Figure 9. It can be clearly seen that if the pretilt angle is increased, it will contribute to the B-shape. However, in the conventional LCD construction technology, it is difficult to manufacture more than 1 〇. High pretilt angle. We can easily estimate the pretilt angle required to form the B unit cell. If the pretilt angles on both sides of the liquid crystal layer are respectively 込, the diagonally and curved unit cells will have the same elasticity 15 energy if the following conditions are satisfied: iK33 -K„ \sin20, +sin292 ]+2(π-2θ, -2Θ2 \Κ33 +Κ„ )=〇 If the pretilt angles on both sides of the unit cell are the same and equal to θ, the above condition can be simplified as: (K33 -K„ ) Sin2e, +(π-4θ, \Κ33^Κ„)=〇20 By solving this equation, the condition of the pretilt angle that makes the oblique and bending deformation energies the same can be obtained. For example, 'for p-methyoxybenzylidene-p'-butylaniline (MBBA) * K32IKt] = 1.3, therefore, 込 is about 47. . It also conforms to the chart shown in Figure 9. 26 1362524 Application No. 93132205 Amendment Gongyi - ι〇丨.〇ι 12 Generally, you can see that for all values of 4/Λ:", it is always at 45. Between 58° and 58°. Thus, if the pretilt angle on the liquid crystal cell is greater than the critical angle, the bending deformation will be more stable than the s_deformation. In other words, the liquid crystal cell will always be in the B_ state. This is a π unit cell with no bias 5 . We call this the unbiased bend (NBB) unit cell. The pretilt angle on one side may be smaller for the asymmetrical liquid crystal cell ', and the pretilt angle on the other side must be larger than that. For example, if it is 3〇. According to the above equation, there is no need to compare 67. Large, if the ruler ///= 1.3. An important step in constructing such a π unit cell is the preparation of the high pretilt orientation of 10 layers. A number of techniques have been introduced in the past to achieve high pretilt angles in a liquid crystal cell. This includes Si〇x evaporation, ion beam, photo-alignment technology and reverse mechanical friction. In the present invention, we combine the germanium unit cell and a special technique which produces a high pretilt angle of our invention. The method of obtaining such a high pretilt angle in the present invention is to rub an orientation layer prepared by a special I5. The liquid crystal cell is oriented by the alignment layers 8 and 9. The details of the preparation of these special alignment layers have been described above in connection with Figure 4. When a vertical alignment material and a horizontal alignment material are mixed in a suitable ratio in a solution, it is possible to form an orientation layer which can generate a pretilt angle at any angle. Figures 6A and 6B show experimental results for this example. In the figure, it is shown that by the vertical alignment material, in this case it is a commercial material obtained from Japan Synthetic Rubber, article number JALS2021, and a horizontal alignment material such as JALS9203, it is possible to obtain 1〇. -8 〇. The pretilt angle of any value. The pretilt angle indicated in Figs. 6A and 6B is the same as the solution mixture. The modification of the page no. 93132205 indicates that the available pretilt angle depends on the preparation method of the solid alignment layer in Fig. 6a. The solid-state layer is prepared using a spin coating technique in Figure 6B, using a roll coating and then rapidly adding a square to prepare the solid film. There are many other ways to The cold liquid forms a film of the alignment layer. It is possible, for example, to form the film by using a silk, a printing inkjet printing method, a dip coating or a doctor blade technique. Disclosed, we only use (iv) examples of printing and spin coating. All other techniques are included in a part of the invention. It can be said that for each method of preparing the film, there is a pretilt angle that is available relative to the solution. The dependence of the ratio on the solid film after the initial preparation can be performed by a hot device, such as placing the substrate in a heated furnace or irradiating a strong ultraviolet light through light treatment. Light onto the liquid helium. If the pretilt angle is greater than 40, the curved structure will be obtained even in the absence of voltage. If the rubbing orientation conditions of the alignment layer are parallel, a π is obtained. a unit cell or a curved orientation unit cell. If the input polarizer and the output polarizer 2' 3 and the liquid crystal cell rub direction are 45. and -45°, the transmission of the π unit cell is as follows Let T = sin2~{An(z)dz Λο where λ is the wavelength, d is the thickness of the liquid crystal layer and Δη is the birefringence of the liquid crystal layer, depending on the orientation conditions such as
Jn(z)= ne (Θ(ζ))-η〇 (1~93132205 號^請案修正頁 Γ〇Γ〇ΓΤΓ~| 其中〜疋液晶材料的哥常折射率,%是液晶材料的非常 折射率。隨著0⑻的變形變化’所述液晶晶胞的傳輸也變 化。這是電控雙折射(ECB)晶胞的基礎。可以使用標準電腦 軟體模擬以此方式構造的所述兀晶胞的傳輸值,如第8Α圖和 8Β所示,針對於無電壓狀態和高電壓狀態。在高電壓,可 . 以得到所述液晶層的垂直取向。 _ 取向層通常用來獲得液晶層的取向來製造液晶顯示 器。文獻中提到很多用於此用途的取向材料。這些材料大 1部分是對於熱和光穩定的聚合體。例如’聚醯亞胺(ΡΙ),聚 10乙締醇(PVA),聚6旨和聚酿胺酸(ρΑ)。這些材料通常被旋塗 或絲網印刷到所述基板4和5上。需要預烤和最終烘烤步驟 來硬化和處理所述聚合的材料。這些聚合取向作用劑中的 一些能夠提供具有一定度數預傾角的平行取向條件。一些 特殊的取向作用劑能夠為具有將近9〇。預傾角的所述液& — 15提供垂直取向。兩種聚合體都能夠被塗到所述基板上,並 . 進行處理,用來在基板4,5上製造取向層,並且這都是本 領域内公知的。 20 在本發明的這個第—優選實施例中,對於所有工作電 磨’所述液晶層的取向保持,晶胞的取向。因此1 時間非常快。不像傳統的㈣胞那樣,不需要任何條件來轉與 化所边π晶胞從斜展到f曲變形。在所述液晶 預傾角可料目同或不同。在1的所述 是Π。,而在另—側的預傾角是預傾角 等的一個例子。第11圖顯f 極端不相 員不了所述實驗晶胞的傳輪相對於 29 1362524 第93132205號申請案修正頁 101.01.12. 電壓的特徵。第12A和12B圖顯示了我們構造的一個原型的 切換時間。因為所述切換可能非常快,即使對於暫態電壓, 我們繪製了 8個灰度的切換時間。第13圖中顯示了結果。可 以看出需要的最大時間為3ms,而最快的時間大大少於 • 5 1ms 〇在這個特別的例子中,不同參數的值在表I中標明。 表I:液晶晶胞參數 晶胞間隙 7微米 液晶材料 Merck MLC-6080 預傾角 17°和60° 垂直取向作用劑 JALS 2021 水平取向作用劑 JALS 9203 輸入起偏器角度 45° 輸出起偏器角度 -45° 在另一個例子中,在所述液晶層兩側的預傾角被製成 一樣。在這種情況下,需要53°的預傾角。第14圖顯示了這 樣一個樣本的傳輸相對於電壓的曲線。它和不對稱的情況 10 沒有太大不同。然而,由於較小的總的雙折射,這個樣本 的絕對傳輸比前一個樣本的低。第15圖總結了由這樣一個 樣本得到的所述切換時間。可以看到,所述反應時間更快, 並且通常少於2ms。表II顯示了這個實驗樣本的參數。 表II .液晶晶胞參數 晶胞間隙 7微米 液晶材料 Merck MLC-6080 預傾角 53° 垂直取向作用劑 JALS 2021 水平取向作用劑 JALS 9203 輸入起偏器角度 45° 輸出起偏器角度 -45° 15 在本發明的第二個優選實施例中,使用在第一個優選 30 1362524 第93132丽~號申請案修 實施例中描述的技術,所述液晶層的預傾角還是被製造的 較大。因此,所述液晶層的取向還是所述彎曲晶胞或所述π 晶胞的取向。然而,現在允許所述取向層的摩擦方向對於 所述頂部和底部取向層是不平行的。這樣,允許對於所述 5液晶晶胞存在一定的扭轉角度。這樣做的目的是使得所述 晶胞傳輸能夠被修正’成為所述扭曲向列晶胞的傳輸,而 不是所述電控雙折射晶胞的傳輸。這樣,所述晶胞間隙玎 以更小’並且反應時間可以更快。可以使用LCD仿真來優 化第二個實施例的光學特性。在這種情況下,所述晶胞間 10隙以及所述液晶晶胞的扭轉角度允許被改變。條件是對比 度應該好’並且所述亮狀態的亮度接近於一致(unity)。 在本發明的第三個優選實施例中,所述液晶顯示器是 —個反射顯示器。有一個輸入起偏器而沒有輸出起偏器。 如第1C圖所示,在所述液晶晶胞後面卻放置了一個鏡面 15 12。或者,對於反射式薄膜電晶體(TFT) LCD的情況,所述 鏡面可以是所述有源矩陣底板的一部分。所述液晶晶胞還 是和第一個優選實施例中的相同。然而,因為所述光束通 過所述液晶晶胞兩次,所需的雙折射會與第一個優選實施 例不同。這對於所述液晶晶胞的反應速度很重要。現在所 20述晶胞間隙可以被減半’速度可以快差不多4倍,因為通 吊’一個液晶晶胞的反應時間與所述晶胞間隙的平方成反 比。同樣’因為現在所述路徑長度變成兩倍於第一個優選 實施例中的長度,故所述液晶材料的雙折射Δη可以有更多 選擇。 31 1362524 第93132205號申請案修正頁 在所有優選實施例中,可能使用延遲膜13,14來補償 色散並改善所述液晶顯示器的視角。在一些情況下,只需 要一個膜。在另外一些情況下,為了精確的補償,在所述 液晶晶胞的兩側都需要一層膜。 5 例1 例1示出了準備一個取向層的過程,該取向層可以提供 44度的預傾角。 材料: •所述水平取向材料:從Japan Synthetic Rubber公司購 10 買(貨號:JALS9203),是溶液形式。(JSR Corporation,5-6-10 Tsukiji Chuo-ku,Tokyo, 104-8410, Japan)。JALS9203 中的所 述溶劑,包括γ-丁内酯(yBL),曱基-2-吡咯烧酮(NMP)和丁 基纖維素溶劑(BC)。 - •所述垂直取向材料:從Japan Synthetic Rubber公司蹲 15買(貨號:JALS2021) ’是溶液形式。JALS2021中的所述溶 劑,包括曱基-2-吡咯烷酮(NMP)和丁基纖維素溶劑(BC)。 •基板:帶有電極的一塊ITO玻璃,從中國深圳南玻公 司購買。 過程: 20 0.95克水平取向材料的溶液和0.05克垂直取向材料的 溶液混合在一起,並充分搜拌。所述混合物被塗到所述基 板上,使用旋塗法以得到一層軟的固體膜。所述旋塗法開 始時以800rmp的轉速梯作1 〇秒鐘,然後以35〇〇rmp的轉速操 作100秒。形成了包括所述水平和垂直取向材料的一層軟膜 32 T362524 降93132205號申請案i—頁 1〇1,〇ΠΣ 和剩餘的溶劑。 為了*去所有剩餘的溶劑,並加工聚合體,所述被塗 層的破璃被置於一個烤爐中。一開始,以1〇〇。〇烤1〇分鐘(軟 烤然後以230 C烤90分鐘(硬烤)。一層硬膜,即所述的取 向詹,就形成了。 所述取向層的表面要接受摩擦處理,使用 """'塊尼龍 #,與:次以一個方向摩擦所述層。 結采· 根據例1生成的所述取向層的預傾角是44度。 !〇 一山、 例2不出了準備一個取向層的過程,該取向層可以提供 度的預傾角。 . 讨科: •所述水平取向材料:從japan Synthetic Rubber公司購 15買(貨號:JALS9203) ’是溶液形式。 •所述垂直取向材料:從japan Synthetic Rubber公司購 買(貨號:JALS2021),是溶液形式。 •基板:帶有電極的一塊ITO玻璃,從中國深圳南玻公 司購買。 2〇 過程: 0.5克水平取向材料的溶液和0·5克垂直取向材料的溶 液混合在一起’並充分授拌。所述混合物被塗到所述基板 上,使用如下的印刷塗層法得到/層軟的固體膜: 一根直徑為2釐米,長為5英寸的不銹鋼棒被放置於所 33 ㊉力132205號申 ===r—,直到溶液沿 棒2或者沿所述基板的表面滑行,以形成-層液體膜。 、層的基板減置於—個1⑼。C的熱板上,10分鐘, 來去除所有的溶劑。鎌就放於—個烤爐内,在23〇Jn(z)= ne (Θ(ζ))-η〇(1~93132205^^Please correct the page |~| where ~ 疋 liquid crystal material has a constant refractive index, % is a very refraction of liquid crystal material Rate. The transmission of the liquid crystal cell changes as the deformation of 0(8) changes. This is the basis of the electronically controlled birefringence (ECB) unit cell. The standard cell computer can be used to simulate the germanium cell structure constructed in this way. The transmission values, as shown in Figures 8 and 8B, are for a no-voltage state and a high voltage state. At a high voltage, the vertical orientation of the liquid crystal layer can be obtained. _ The alignment layer is usually used to obtain the orientation of the liquid crystal layer. Manufacturing of liquid crystal displays. A number of oriented materials for this purpose are mentioned in the literature. A large part of these materials are heat and light stable polymers such as 'polyimine (ΡΙ), poly 10 propylene glycol (PVA), These materials are typically spin-coated or screen printed onto the substrates 4 and 5. Pre-bake and final baking steps are required to harden and process the polymeric material. Some of the polymeric orientation agents are capable of providing a pretilt angle with a certain degree Parallel orientation conditions. Some special orientation agents can provide a vertical orientation for the liquid & 15 having a pretilt angle of both. Both polymers can be applied to the substrate and processed. It is used to fabricate alignment layers on the substrates 4, 5, and this is well known in the art. 20 In this first preferred embodiment of the invention, the orientation of the liquid crystal layer is maintained for all working electromills, crystal The orientation of the cell. Therefore, the time is very fast. Unlike the traditional (four) cells, there is no need to change the π cell from the oblique to f-curve deformation. The liquid crystal pretilt angle can be expected to be the same or The difference between the ones in 1 is Π, and the pretilt angle on the other side is an example of the pretilt angle, etc. The eleventh figure shows that the transmission of the experimental unit cell is relatively inconsistent with respect to 29 1362524. 93132205 Application Revision Page 101.01.12. Characteristics of Voltage. Figures 12A and 12B show the switching time of a prototype we constructed. Because the switching can be very fast, even for transient voltages, we have drawn 8 grays. Degree switching time The results are shown in Figure 13. It can be seen that the maximum time required is 3ms, and the fastest time is much less than • 5 1ms. In this particular example, the values of the different parameters are indicated in Table I. : Liquid crystal cell parameters Cell gap 7 micron liquid crystal material Merck MLC-6080 Pretilt angle 17° and 60° Vertical alignment agent JALS 2021 Horizontal orientation agent JALS 9203 Input polarizer angle 45° Output polarizer angle -45° In another example, the pretilt angles on both sides of the liquid crystal layer are made the same. In this case, a pretilt angle of 53 is required. Figure 14 shows the plot of the transmission of such a sample versus voltage. It is not much different from the asymmetrical case 10. However, due to the smaller total birefringence, the absolute transmission of this sample is lower than that of the previous sample. Figure 15 summarizes the switching time obtained from such a sample. It can be seen that the reaction time is faster and is usually less than 2 ms. Table II shows the parameters of this experimental sample. Table II. Liquid crystal cell parameters Cell gap 7 micron liquid crystal material Merck MLC-6080 Pretilt angle 53° Vertical alignment agent JALS 2021 Horizontal orientation agent JALS 9203 Input polarizer angle 45° Output polarizer angle -45° 15 In a second preferred embodiment of the invention, the pretilt angle of the liquid crystal layer is still made larger, using the technique described in the first preferred embodiment of the preferred embodiment. Therefore, the orientation of the liquid crystal layer is also the orientation of the curved unit cell or the π unit cell. However, the rubbing direction of the alignment layer is now allowed to be non-parallel to the top and bottom alignment layers. Thus, a certain twist angle is allowed for the liquid crystal cell. The purpose of this is to enable the cell transfer to be corrected' into the transmission of the twisted nematic cell rather than the transmission of the electrically controlled birefringent cell. Thus, the cell gap 玎 is smaller and the reaction time can be faster. LCD simulation can be used to optimize the optical characteristics of the second embodiment. In this case, the inter-cell gap 10 and the twist angle of the liquid crystal cell are allowed to be changed. The condition is that the contrast should be good' and the brightness of the bright state is close to unity. In a third preferred embodiment of the invention, the liquid crystal display is a reflective display. There is one input polarizer and no output polarizer. As shown in Fig. 1C, a mirror surface 15 12 is placed behind the liquid crystal cell. Alternatively, in the case of a reflective thin film transistor (TFT) LCD, the mirror may be part of the active matrix backplane. The liquid crystal cell is also the same as in the first preferred embodiment. However, because the beam passes through the liquid crystal cell twice, the required birefringence will be different from the first preferred embodiment. This is important for the reaction rate of the liquid crystal cell. Now the cell gap can be halved' speed can be almost four times faster because the reaction time of a liquid crystal cell is inversely proportional to the square of the cell gap. Also, since the path length now becomes twice the length in the first preferred embodiment, the birefringence Δη of the liquid crystal material can be more selected. 31 1362524 Application No. 93132205 Amendment Page In all preferred embodiments, retardation films 13, 14 may be used to compensate for dispersion and improve the viewing angle of the liquid crystal display. In some cases, only one membrane is required. In other cases, a film is required on both sides of the liquid crystal cell for precise compensation. 5 Example 1 Example 1 shows a process of preparing an alignment layer which can provide a pretilt angle of 44 degrees. Materials: • The horizontally oriented material: purchased from Japan Synthetic Rubber Company 10 (Cat. No.: JALS9203), in the form of a solution. (JSR Corporation, 5-6-10 Tsukiji Chuo-ku, Tokyo, 104-8410, Japan). The solvents in JALS9203 include γ-butyrolactone (yBL), mercapto-2-pyrrolidone (NMP) and butyl cellulose solvent (BC). - • The vertical alignment material: purchased from Japan Synthetic Rubber Co., Ltd. (article number: JALS2021)' is in the form of a solution. The solvent in JALS 2021 includes mercapto-2-pyrrolidone (NMP) and butyl cellulose solvent (BC). • Substrate: An ITO glass with electrodes purchased from Shenzhen CSG. Procedure: 20 0.95 grams of a solution of the horizontally oriented material and 0.05 grams of a solution of the vertically oriented material were mixed together and thoroughly mixed. The mixture was applied to the substrate using spin coating to obtain a soft solid film. The spin coating method was started at 800 rpm for 1 , and then at 35 rpm for 100 seconds. A soft film comprising the horizontal and vertical alignment materials is formed. 32 T362524 pp 93,312,205, application i-page 1 〇 1, 〇ΠΣ and the remaining solvent. In order to remove all remaining solvent and process the polymer, the coated glass is placed in an oven. At the beginning, take 1 〇〇. Bake for 1 minute (soft bake and then bake at 230 C for 90 minutes (hard bake). A hard film, ie the orientation Zhan, is formed. The surface of the orientation layer is subjected to rubbing treatment, using "" ;"'Block nylon#, and: rubbing the layer in one direction. The picking effect · The pretilt angle of the orientation layer generated according to Example 1 is 44 degrees. 〇一山, Example 2 is not prepared for one The process of orienting the layer, which can provide a degree of pretilt angle. Discussion: • The horizontally oriented material: purchased from japan Synthetic Rubber Company 15 (Cat. No.: JALS 9203) 'is in solution. · The vertical alignment material : Purchased from japan Synthetic Rubber (article number: JALS2021), in solution. • Substrate: An ITO glass with electrodes, purchased from Shenzhen CSG, China. 2〇 Process: 0.5 g of horizontally oriented material solution and 0· A solution of 5 grams of the vertically oriented material was mixed together' and thoroughly mixed. The mixture was applied to the substrate and a soft solid film was obtained using the following printing coating method: a diameter of 2 cm, long 5 inches The inch stainless steel rod is placed on the 33rd force 132205 to ===r- until the solution slides along the rod 2 or along the surface of the substrate to form a liquid film of the layer. 1 (9). C on the hot plate, 10 minutes to remove all the solvent. 镰 placed in an oven, at 23 〇
_。就得到包括垂直和水平取向材料"硬膜J 述奴…始時以_rmp的轉速操作1〇秒鐘,然後以 350,的轉速操作卿。形成了包括所述水平和垂直取 向材料的一層軟膜和剩餘的溶劑。 為了除去所有剩餘的溶劑,並加工聚合體,所述被塗 層的玻璃被置於-㈣爐中。1始,以we烤1G分鐘(軟 烤)’然後以聰烤90分鐘(硬烤)…層硬膜,即,所迷的人 取向層,就形成了。所述取向層的表面要接受摩擦處理, 使用-塊尼龍布,每次以-個方向摩擦所述層。 結果: 根據例2生成的所述取向層的預傾角是”度。 在例1中,通過旋塗法,所述液體膜變成了軟的固體 膜。所述溶劑慢慢地蒸發,使得水平取向和垂直取向的區 域趨向於更大。而且,水平取向和垂直取向區域的表面積 的比率,將有助於在所述混合的溶劑中具有較高溶解性的 材料’因為具有較低溶解性的材料將先沉殿。 在例2中’由於在一塊熱的板子上加熱,所以凝固得後 快。這樣,所述區域傾向於更小。所述水平取向和垂直取 向區域面積的比率不會因為材料的不同溶解性而受到太大 1362524_. It is obtained by including the vertical and horizontal orientation materials "hard film J slave...starting at _rmp for 1 〇 second, then operating at 350 rpm. A soft film comprising the horizontal and vertical alignment materials and the remaining solvent are formed. In order to remove all remaining solvent and process the polymer, the coated glass is placed in a - (four) furnace. At the beginning, it was baked for 1G minutes (soft bake) and then baked for 90 minutes (hard baked)... a hard film, that is, a human orientation layer, was formed. The surface of the alignment layer was subjected to a rubbing treatment using a nylon cloth, and the layer was rubbed in one direction at a time. Results: The pretilt angle of the alignment layer produced according to Example 2 was "degree." In Example 1, the liquid film became a soft solid film by a spin coating method. The solvent was slowly evaporated to make a horizontal orientation. And the vertically oriented regions tend to be larger. Moreover, the ratio of the surface area of the horizontally oriented and vertically oriented regions will contribute to the material having higher solubility in the mixed solvent 'because of materials having lower solubility In the case 2, 'because it is heated on a hot plate, it solidifies quickly. Thus, the area tends to be smaller. The ratio of the area of the horizontal and vertical alignment areas is not due to the material. Different solubility and subject to too much 1362524
的影響。 由例1和例2的工藝過程得到的預傾角不同,即使對於 相同的水平取向和垂直取向取向作用劑的混合物。這是因 為使用不同的過程得到不同的區域結構。這裏有一個表 5格’列出了對於相同的混合物使用所述兩種不同的方法得 到的所述預傾角。 結果 與所述取向層接觸的液晶分子的預傾角是通過晶體旋 轉方法測量。 在所述取向層表面上的所述錫定能量通過Chigrinov 等人的公開中描述的方法進行測量Chigrinov,A Muravski,H S Kwok,H Takada,H Akiyama和 H Takatsu, Anchoring properties of photo-aligned azo-dyes materials,Impact. The pretilt angles obtained by the processes of Examples 1 and 2 were different, even for the same horizontal orientation and vertical orientation of the mixture of the orientation agents. This is because different processes are used to get different regional structures. There is a table 5 grid' which lists the pretilt angles obtained for the same mixture using the two different methods. As a result, the pretilt angle of the liquid crystal molecules in contact with the alignment layer was measured by a crystal rotation method. The tinning energy on the surface of the alignment layer is measured by the method described in the publication of Chigrinov et al. Chigrinov, A Muravski, HS Kwok, H Takada, H Akiyama and H Takatsu, Anchoring properties of photo-aligned azo- Dyes materials,
Physical Review E,vol 68 pp 61702-61702-5,2003)。 15 例3 除了例1和例2 ’本發明還可根據不同比例的垂直取向 層(JALS2021)和水平取向層(JALS9203)以及基本上與例1 和例2相同的過程來生成具有不同預傾角的取向層》通過旋 塗法生成的取向層的細節由表1顯示。通過印刷塗層法生成 20 的取向層的細節由表2顯示。 表1.通過旋塗法生成的取向層 JALS2021 的濃度(Wt%) JALS9203 的濃度(Wt%) 預傾角(度) 0 100 5 0.566 99.434 12.9 1.69 98.31 22.8 2.587 97.413 40.95 35 1362524 第93132205號申請案修正頁 101.01.12. 3.47 96.53 51.1 5.34 94.66 72.4 12.35 87.65 77 36 64 83.5 100 0 87 表2.通過印刷塗層法生成的取向層 JALS 2021 的濃度(wt%) JALS 9203 的濃度(wt%) 預傾角(度) 2.3 97.7 4.8 6 94 5.25 15.8 84.2 21.7 18.7 81.3 24.75 27.3 72.7 37.4 36 64 53.4 51 49 77 69 31 86 100 0 87 準備所述新的取向層中的關鍵步驟是在所述固體膜形 成過程中的奈米結構的形成。因為,所述兩種取向材料在 所述固體膜形成過程中的不同時間沉澱,就形成奈米-和微 5 結構。第5A-5C圖顯示了在標準原子力顯微鏡方法下觀察的 根據本發明形成的膜結構。在這些圖中,較亮的區域顯示 了所述垂直取向材料。從第5A到5C圖,垂直取向材料的百 分比在增加。這些樣本通過旋塗法生成,其中所述從液體 膜到固體膜的轉化相對較慢,並且允許有更多的時間用於 10 所述兩種取向材料的分離。在這些例子中,所述奈米結構 的特徵是幾分之一微米的量級的大小。在很多其他的情況 中,所述奈米結構可以小到幾個奈米。所述奈米結構通常 是以在所述平行取向材料的背景下的垂直取向材料的島狀 物的形式存在。這個結構由表面張力,表面能量,彈性和 所述兩種材料的其他物理性質以及所述普通溶劑的物理性 36 15 1362524 質決定。它們對於這個實施例都是有用的。 使用上述的取向層,一個液晶晶胞被準備,同時也獲 得完美的統一的取向。所述液晶分子的預傾角如第6圖a所 示。第6A圖顯示了在JALS2021的不同濃度測量的預傾角。 5 可以看出所述預傾角可以通過JALS2021的百分比來控制, 從大約5。到將近80。,同時JALS2021的濃度從0%到達大約 14% 〇 所述取向層表面的極角錨定能量也被測量,由第7圖示 出。可以看出,所述錨定能量根據JALS2021的百分比變化。 10 得到的所述預傾角和所述固體膜的準備的方法的相關 性可以概念地理解。就物理意義講,所述的兩種區域將與 所述液晶分子互相作用。它們的取向力將互相競爭,產生 一種取向,該取向介於垂直取向和水平取向之間。通過改 變所述垂直取向和平行取向材料的相對濃度,可以產生不 15 同值的預傾角。 根據本發明的描述產生的所述取向層可以有很多應 用。例如,它可以被用於一個液晶顯示器(LCD)設備的液晶 晶胞中。使用本發明的所述取向層的LCD設備具有很多優 點,如,提高的反應速度,寬的視角以及卓越的圖像無殘 20影現象性質。本領域技術人員能想到的其他應用,這裏就 不再詳述。 根據這裏公開的本發明的說明書和實踐,本發明的其 他實施例對於本領域技術人員是顯而易見的。雖然,本發 明的大部分實施例使用聚合體混合物混合兩種聚合體,其 37 1362524 gjii322Qsgggggg^—iQl0l 在形成取向層時分別提供垂直和水平取向能力,可以理解 也可以使用其他聚合體來準備取向層。例如,除了 JALS9203,可以使用其他的商業產品作為水平取向材料, 而且除了 JALS2021以外,可以使用其他的商業產品作為垂 5 直取向材料。 對於另一個例子,可以使用一種均聚合物,其具有提 供水平取向能力的一種側鏈結構和提供垂直取向能力的另 一種側鏈結構。所述均聚合物的側鏈可以被處理以得到理 想的預傾角。另一個例子,也可以使用一種共聚物,其包 10 括提供垂直取向能力的一種草體和提供水平取向能力的另 一種單體。所述共聚物中的組成單體也可以被控制來獲得 理想的預傾角。 雖然在il些例子中’商業構貝的所述取向材料已經溶 解在溶劑中,也有可能分別選擇取向材料和溶劑,如第4圖 15 所描述的。能夠使用的溶劑是那些既與水平取向材料又與 垂直取向材料易混合的溶劑。所述溶劑應該與兩種材料都 容易混合,使得當所述兩種材料溶解在所述溶劑中時,將 形成包括如奈米大小的液滴的一種均勻的溶液。當所述取 向層從這樣的溶液中形成’所述兩種材料的奈米大小的結 20構可以使用標準原子力顯微鏡方法進行觀察。Indratmoko Hari poerwant〇 和 Gudrun Schmidt-Naake (Telaah, Jilid ΧΧΠ,No. 1-2,2001)提供用於預測聚合體可混和性的一種 實際的方案。基於現有的知識,相信本領域技術人員應該 能夠根據本發明,以理想的可混和性來選擇合適的溶劑來 38 1362524 第93132205號申請案修正頁 101.01.12. 溶解所述垂直的和水平的取向材料。 例4 一種液晶晶胞1(晶胞I)通過下列方法製造: 成分: 5 •液晶:Merck MLC-6080 ;向列的;等方向性相轉變 溫度:95。; Δε(介電異向性):7,2 ; Δη(折射率異向性): 0.2024 ; Ku : 14.4 ; Κ33 : 19.1 •第一基板:從CSG Shenzhen Wellight Conductive Coating c〇.,Ltd 購買;貨號:STN<30Q ;大小: 10 14"χ 16"x l.imm •第二基板:同上 •取向層:下列例子1-3來準備能夠提供17。和60。預傾 角的取向層 •紫外線環氧樹脂(UV epoxy):從BOIS Technology Ltd 15 購買 •間隔器(spacer):從 BOIS Technology Ltd購買;貨號 PF70 過程: 標準LCD晶胞構造過程:所述玻璃基板被清洗it塗上 20 取向層。所述取向層被摩擦形成一個空的晶胞《所述晶胞 在真空室中被充滿液晶。所述晶胞的末端被環氧樹脂密 封°所述環氡樹脂被用紫外光處理。所述起偏器以合適角 度被層壓:輸入起偏器角度:45。;輸出起偏器角度:-45。。 晶胞I的構造: 39 1362524 •晶胞間隙:7微米 •預傾角:17。和60。 •液晶層的取向:在所有工作電壓處於彎曲狀態 所述第二個基板是一個有源矩陣底板,包括在一個基 5 板上的薄膜電晶體,如以一個矩陣形式排列的玻璃。 所述晶胞的狀態(彎曲或斜展)通過觀察所述晶胞的顏 色被確認’其相關於所述液晶晶胞的延遲。綠色代表所述 晶胞處於斜展狀態。白色代表所述晶胞處於彎曲狀態。當 施加電壓時,白色變成灰色然後黑色。 10 在晶胞1,與所述頂部取向層和所述底部取向層接觸的 所述液晶分子的預傾角分別是17。和60。。這是預傾角極端 不相等的情況。第11圖顯示了晶胞I的傳輸和電壓之間的關 係。第12圖顯示了我們構造的晶胞I的切換時間。因為所述 切換可能非常快,即使對於暫態電壓,我們繪製了 8個灰度 15的切換時間。第13圖中顯示了結果。可以看出需要的最大 時間為3ms ’而最快的時間大大少於lms。第11圖(以及第14 圖)中的傳輸相對於電壓的曲線通過使用Autr〇nics DMS5〇i 機器得到。第12A和12B圖是示波器描跡,顯示了晶胞⑴的 切換動態特性。第13圖中的反應時間通過使用紅色雷射器 20 (632nm) ’快速檢測器和示波器獲得〇 在這個晶胞I中,所述液晶取向層的取向對於所有工作 電壓保持B狀態,包括零電壓。因此所述切換時間非常快。 不像傳統的π晶胞那樣,從s狀態到B狀態轉換晶胞〗不需要 任何條件。 40 1362524 第93132205號申請案修正頁 ΓΟΠΓΊ 例5 第二種液晶晶胞11(晶胞Π)通過下列方法製造: 成分: .第一基板.從CSG Shenzhen Wellight Conductive 5 Coating Co_,Ltd 購買;貨號:STN<3〇n ;大小: 14"xl6"xl.lmm •第二基板:同上 •液晶:MerckMLC-6080 ;向列的;等方向性相轉變 溫度(isotropic phase transition temperature) : 95。; Αε(介電 10異向性):7·2 ; Δη(折射率各向異性):〇 2024 ; Κπ : 14.4 ; Κ33 · 19.1 •取向層:下列例子1-3來準備能夠提供大於53。預傾 角的取向層 •紫外線環氧樹脂:從B〇IS Techn〇1〇gy Ltd購買 15 •間隔器(sPacer):從BOIS Technology Ltd購買;貨號 PF50 過程: 標準LCD晶胞構造過程:所述玻璃基板被清洗並塗上 取向層。所述取向層被摩擦形成一個空的晶胞。所述晶胞 20在真空至中被充滿液晶。所述晶胞的末端被環氧樹脂密 封。所述環氧樹脂被用紫外光處理。所述起偏器以合適角 度被層壓:輸入起偏器角度45。;輸出起偏器角度:_45。。 晶胞(II)的構造: •晶胞間隙:5微米 41 1362524 「第 93132205 號頁 1〇1·〇ΐ·ΐ2· •兩個取向層的預傾角:53。;互相之間成45。角 •液晶層的取向:在所有工作電壓處於彎曲狀態 第14圖顯示了晶胞II的傳輸相對於電壓曲線。與晶胞工 的曲線沒有太大不同。然而’由於較小的總的雙折射,晶 5 胞Π的絕對傳輸比晶胞I的低。第15圖總結了由晶胞η獲得的 切換時間。可以看出’所述反應時間更快,一般少於2 ms。 使用一個標準的摩擦機器,所述取向層被摩擦,使得 所述頂部取向層和所述底部取向層的方向互相成45。角。這 樣’就允許對於所述液晶晶胞有一定量的扭轉角度。這樣 10 做的目的是使得所述晶胞傳輸能被修正並成為一個扭曲向 列晶胞的傳輸,而不是電控雙折射晶胞的傳輸。這樣,所 述晶胞間隙可以更小並且所述反應時間可以更快。可以使 用LCD模擬來優化這個第二實施例的光學特性。在這個模 擬中,所述液晶晶胞的晶胞間隙和扭轉角度允許被改變。 15 要求是所述對比度好並且所述亮狀態亮度接近於一。 例6 一個反射式液晶顯示器I(LCDI)通過下列方法製造: 成分: •第一基板:從CSG Shenzhen Wellight Conductive 20 Coating Co., Ltd 購買;貨號:STN<30Q ;大小: 14"xl6',xl.lmm •第二基板:帶有铭塗層的一塊玻璃 •液晶:MLC-6080 ;向列的;等方向性相轉變溫度: 95° ; Δε(介電異向性):7.2 ; Δη(折射率向異性):0.2024 ; 42 1362524 第93132205號申請案修正頁_101.01.12.Physical Review E, vol 68 pp 61702-61702-5, 2003). 15 Example 3 In addition to Examples 1 and 2, the present invention can also generate different pretilt angles according to different ratios of the vertical alignment layer (JALS2021) and the horizontal alignment layer (JALS9203) and substantially the same processes as in Examples 1 and 2. The details of the alignment layer produced by the spin coating method are shown in Table 1. The details of the orientation layer formed by the printing coating method 20 are shown in Table 2. Table 1. Concentration of orientation layer JALS2021 produced by spin coating (Wt%) Concentration of JALS9203 (Wt%) Pretilt angle (degrees) 0 100 5 0.566 99.434 12.9 1.69 98.31 22.8 2.587 97.413 40.95 35 1362524 Revision of application No. 93132205 Pages 101.01.12. 3.47 96.53 51.1 5.34 94.66 72.4 12.35 87.65 77 36 64 83.5 100 0 87 Table 2. Concentration of the orientation layer JALS 2021 produced by the printing coating method (wt%) Concentration of JALS 9203 (wt%) Pretilt angle (degrees) 2.3 97.7 4.8 6 94 5.25 15.8 84.2 21.7 18.7 81.3 24.75 27.3 72.7 37.4 36 64 53.4 51 49 77 69 31 86 100 0 87 The key step in preparing the new orientation layer is during the formation of the solid film The formation of the nanostructure. Since the two orientation materials precipitate at different times during the formation of the solid film, a nano- and micro-5 structure is formed. Figures 5A-5C show the structure of the film formed in accordance with the present invention as observed under standard atomic force microscopy. In these figures, the brighter areas show the vertically oriented material. From the 5A to 5C graph, the percentage of the vertically oriented material is increasing. These samples were produced by spin coating, wherein the conversion from the liquid film to the solid film was relatively slow and allowed more time for the separation of the two oriented materials. In these examples, the nanostructure is characterized by a size on the order of a fraction of a micron. In many other cases, the nanostructure can be as small as a few nanometers. The nanostructures are typically in the form of islands of vertically oriented material in the context of the parallel oriented material. This structure is determined by surface tension, surface energy, elasticity, and other physical properties of the two materials as well as the physical properties of the common solvent 36 15 1362524. They are all useful for this embodiment. Using the above alignment layer, a liquid crystal cell is prepared while achieving a perfect uniform orientation. The pretilt angle of the liquid crystal molecules is as shown in Fig. 6a. Figure 6A shows the pretilt angle measured at different concentrations of JALS2021. 5 It can be seen that the pretilt angle can be controlled by the percentage of JALS2021, from about 5. Nearly 80. At the same time, the concentration of JALS2021 reaches from about 0% to about 14%. The polar anchoring energy of the surface of the orientation layer is also measured, as shown by the seventh. It can be seen that the anchoring energy varies according to the percentage of JALS2021. The correlation between the obtained pretilt angle and the method of preparation of the solid film can be conceptually understood. In the physical sense, the two regions described will interact with the liquid crystal molecules. Their orientation forces will compete with one another to create an orientation between the vertical and horizontal orientations. By varying the relative concentrations of the vertically oriented and parallel oriented materials, a pretilt angle of not the same value can be produced. The alignment layer produced in accordance with the teachings of the present invention can have many applications. For example, it can be used in a liquid crystal cell of a liquid crystal display (LCD) device. The LCD device using the alignment layer of the present invention has many advantages such as an improved reaction speed, a wide viewing angle, and excellent image-free phenomenon. Other applications that will occur to those skilled in the art are not described in detail herein. Other embodiments of the invention will be apparent to those skilled in the <RTIgt; Although most of the embodiments of the present invention use a polymer mixture to mix two polymers, 37 1362524 gjii322Qsgggggg^-iQl0l provide vertical and horizontal orientation capabilities, respectively, when forming the alignment layer, it being understood that other polymers may be used to prepare the orientation. Floor. For example, in addition to JALS9203, other commercial products can be used as the horizontal alignment material, and other commercial products can be used as the vertical alignment material in addition to JALS2021. For another example, a homopolymer may be used having a side chain structure that provides horizontal orientation and another side chain structure that provides vertical orientation. The side chains of the homopolymer can be treated to achieve an ideal pretilt angle. As another example, a copolymer may be used which includes a grass body which provides vertical orientation ability and another monomer which provides horizontal orientation ability. The constituent monomers in the copolymer can also be controlled to achieve a desired pretilt angle. Although in the examples of il, the oriented material of the commercial scallop has been dissolved in a solvent, it is also possible to select the alignment material and the solvent, respectively, as described in Fig. 4 . Solvents which can be used are those which are easily miscible with both the horizontally oriented material and the vertically oriented material. The solvent should be easily miscible with both materials such that when the two materials are dissolved in the solvent, a homogeneous solution comprising droplets of a size such as nanometers will be formed. When the alignment layer is formed from such a solution, the nano-sized structure of the two materials can be observed using a standard atomic force microscope method. Indratmoko Hari poerwant〇 and Gudrun Schmidt-Naake (Telaah, Jilid ΧΧΠ, No. 1-2, 2001) provide a practical solution for predicting polymer miscibility. Based on the prior knowledge, it is believed that those skilled in the art will be able to select a suitable solvent in accordance with the present invention with an ideal blendability. 38 1362524 No. 93132205 Application Revision 101.01.12. Dissolving the vertical and horizontal orientations material. Example 4 A liquid crystal cell 1 (unit cell I) was produced by the following method: Composition: 5 • Liquid crystal: Merck MLC-6080; nematic; isotropic phase transition Temperature: 95. Δε (dielectric anisotropy): 7, 2; Δη (refractive index anisotropy): 0.2024; Ku: 14.4; Κ 33: 19.1 • First substrate: purchased from CSG Shenzhen Wellight Conductive Coating c〇., Ltd; Item No.: STN<30Q; Size: 10 14"χ 16"x l.imm • Second substrate: Same as above • Orientation layer: The following examples 1-3 are prepared to provide 17. And 60. Pre-tilt orientation layer • UV epoxy: purchased from BOIS Technology Ltd 15 • spacer: purchased from BOIS Technology Ltd; article number PF70 Procedure: Standard LCD cell construction process: the glass substrate was Wash it and apply a 20 orientation layer. The alignment layer is rubbed to form an empty unit cell "the unit cell is filled with liquid crystal in the vacuum chamber. The end of the unit cell is sealed with an epoxy resin. The cyclic resin is treated with ultraviolet light. The polarizer was laminated at a suitable angle: input polarizer angle: 45. ; output polarizer angle: -45. . Construction of unit cell I: 39 1362524 • Cell gap: 7 microns • Pretilt angle: 17. And 60. • Orientation of the liquid crystal layer: at all operating voltages in a bent state The second substrate is an active matrix substrate comprising thin film transistors on a substrate 5, such as glass arranged in a matrix. The state of the unit cell (bending or beveling) is confirmed by observing the color of the unit cell, which is related to the retardation of the liquid crystal cell. Green indicates that the unit cell is in an oblique state. White indicates that the unit cell is in a bent state. When a voltage is applied, the white color turns gray and then black. 10 In the unit cell 1, the liquid crystal molecules in contact with the top alignment layer and the bottom alignment layer have a pretilt angle of 17, respectively. And 60. . This is the case where the pretilt angles are extremely unequal. Figure 11 shows the relationship between the transmission of the unit cell I and the voltage. Figure 12 shows the switching time of the unit cell I constructed. Since the switching can be very fast, even for transient voltages, we plot 8 grayscale 15 switching times. The results are shown in Figure 13. It can be seen that the maximum time required is 3ms ’ and the fastest time is much less than lms. The transmission versus voltage curve in Figure 11 (and Figure 14) is obtained by using the Autr〇nics DMS5〇i machine. Figures 12A and 12B are oscilloscope traces showing the switching dynamics of the unit cell (1). The reaction time in Figure 13 was obtained by using a red laser 20 (632 nm) 'fast detector and oscilloscope in this cell I, the orientation of which is maintained in B state for all operating voltages, including zero voltage. . Therefore the switching time is very fast. Unlike the conventional π unit cell, the conversion of the unit cell from the s state to the B state does not require any conditions. 40 1362524 Application No. 93132205 Amendment Page 例 Example 5 The second liquid crystal cell 11 (cell Π) is manufactured by the following method: Composition: . First substrate. Purchased from CSG Shenzhen Wellight Conductive 5 Coating Co_, Ltd; STN<3〇n; Size: 14"xl6"xl.lmm • Second substrate: Same as above • Liquid crystal: MerckMLC-6080; Nematic; isotropic phase transition temperature: 95. Α ε (dielectric 10 anisotropy): 7·2 ; Δη (refractive index anisotropy): 〇 2024 ; Κ π : 14.4 ; Κ 33 · 19.1 • Orientation layer: The following examples 1-3 are prepared to provide greater than 53. Pretilt Orientation Layer • UV Epoxy Resin: Purchased from B〇IS Techn〇1〇gy Ltd 15 • Spacer (sPacer): purchased from BOIS Technology Ltd; Catalog No. PF50 Procedure: Standard LCD Cell Construction Process: The Glass The substrate is cleaned and coated with an alignment layer. The alignment layer is rubbed to form an empty unit cell. The unit cell 20 is filled with liquid crystal in a vacuum to medium. The ends of the unit cells are sealed with an epoxy resin. The epoxy resin is treated with ultraviolet light. The polarizer is laminated at a suitable angle: input polarizer angle 45. ; Output polarizer angle: _45. . Structure of unit cell (II): • Cell gap: 5 μm 41 1362524 “Page 93132205 Page 1〇1·〇ΐ·ΐ2· • Pretilt angle of two orientation layers: 53. 45 degrees to each other • Orientation of the liquid crystal layer: at all operating voltages in a bent state. Figure 14 shows the transmission versus cell voltage curve of cell II. The curve is not much different from that of the crystal cell. However, due to the smaller total birefringence, The absolute transmission of the crystal 5 cell is lower than that of the unit cell I. Figure 15 summarizes the switching time obtained by the unit cell η. It can be seen that the reaction time is faster, generally less than 2 ms. Using a standard friction The machine, the alignment layer is rubbed such that the directions of the top alignment layer and the bottom alignment layer are at an angle of 45. Thus, 'allows a certain amount of twist angle for the liquid crystal cell." Is such that the cell transfer energy can be corrected and transmitted as a twisted nematic cell, rather than the transmission of an electrically controlled birefringent cell. Thus, the cell gap can be smaller and the reaction time can be faster. Can use LCD mode The optical characteristics of this second embodiment are optimized. In this simulation, the cell gap and the twist angle of the liquid crystal cell are allowed to be changed. 15 The requirement is that the contrast is good and the brightness of the bright state is close to one. 6 A reflective liquid crystal display I (LCDI) is manufactured by the following methods: Composition: • First substrate: purchased from CSG Shenzhen Wellight Conductive 20 Coating Co., Ltd; article number: STN<30Q; size: 14"xl6', xl. Lmm • second substrate: a piece of glass with a coating of the name • liquid crystal: MLC-6080; nematic; isotropic phase transition temperature: 95°; Δε (dielectric anisotropy): 7.2; Δη (refractive index) To the opposite sex): 0.2024; 42 1362524 No. 93132205 application amendment page _101.01.12.
Kn : 14.4 ; Κ33 : 19.1 •取向層:根據例子1-3來準備能夠提供5〇。預傾角的 取向層 •鏡面:直接蒸鍍鋁膜到所述玻璃上。内部實施。 5 •紫外線環氧樹脂··從BOIS Technology Ltd購買 ' •間隔器:從BOIS Technology Ltd購買;貨號PF50 · 準備所述LCD晶胞的過程與例4和5中摇述的相同。另 外,如第1C圖(12)所示,一個鏡面被放置在所述液晶晶胞 的後面。在其他例子中,所述鏡面可以被放置於所述液晶 10晶胞内部和在所述基板的頂部作為所述有源矩陣底板的一 部分。所述起偏器是一個輸入起偏器,被置於如第1(:圖(2) 所示的一個位置。在這個例子中,沒有輸出起偏器。 構造: •晶胞間隙:3微米 15 •兩個取向層的預傾角:50。(正負號相反) •液晶層的取向:在所有工作電壓處於彎曲狀態 因為所述光束通過所述晶胞兩次,需要的雙折射比晶 胞1的例子所需的少。這對於所述液晶晶胞的反應速度很重 要。因為現在所述晶胞間隙可以被減半,速度可以快差不 多4倍。(通常,一個液晶晶胞的反應時間與所述晶胞間隙 的平方成反比。)並且,因為現在所述路徑長度變成兩倍於 胞1和aa胞II的長度,這裏對於所述液晶材料的雙折射 可能有更多選擇。 根據本發明的描述產生的取向層可以有很多應用。例 43 1362524 男"93132205號申請案修正頁 ΙΟΙ.ΟΟΙ 如,它可以被用於一個LCD設備的一個液晶晶胞中。使用 本發明的所述取向層的LCD設備具有很多優點,如,提高 的反應速度,寬的視角以及卓越的圖像無殘影現象性質。 本領域技術人員能想到的其他應用,這裏就不再詳述。 5 根據這裏公開的本發明的說明書和實踐,本發明的其 . 他實施例對於本領域技術人員是顯而易見的。希望本說明 書和例子只被當作是範例,本發明真正的範圍和精神將被 後面的權利要求指明。 【圖式簡單說明】 10 第ΙΑ,1B和1C圖顯示了根據本發明一個方面的一個液 晶顯示設備的一部分的截面圖。 第2圖顯示了根據本發明另一個方面的一個液晶晶胞 的一部分的截面圖。 第3圖顯不了在卡氏座標糸中的液晶指向矢。 15 第3A圖顯示了根據本發明的另一個方面的起偏器,檢 偏器,光和觀察者相對於所述液晶晶胞的位置。 第4圖顯示了根據本發明的另一個方面的製作一個液 晶取向層的過程。 第5A,5B和5C圖是一組照片,顯示了根據本發明的另 20 —個方面,由液晶層作用劑形成的一層固體膜的奈米和微 米區域的例子。 第6A圖顯示了根據本發明的另一個方面的,所述預傾 角和垂直取向材料(JALS2021)的濃度之間的關係。所述取 向膜由旋塗法形成。 44 1362524 \% 93132205 Ef I#f¥iTw— ~~~L__i2〇U2: 第6B圖顯示了根據本發明的另一個方面的,所述預傾 角和垂直取向材料(JALS2021)的濃度之間的關係。這裏, 所述取向膜由滾筒印刷法形成。 第7圖顯示了根據本發明的另一個方面的,所述極角錯 5定能量和垂直取向材料(JALS2021)的濃度之間的關係》 第8A和8B圖分別顯示了根據本發明的另一方面的所 述液晶層的所述(A)斜展和(B)彎曲變形取向。 第9圖顯示了根據本發明的另一方面的一個液晶層的 所述彎曲和斜展取向的所述彈性變形能量。 10 第10Α*1〇Β圖顯示了根據本發明的另一方面的在(A) 零電壓和(B)高電壓處的所述彎曲取向。 第11圖顯示了根據本發明的另一方面的由例4準備的 晶胞(1)的傳輸和電壓之間的關係。 第12A和12B圖是示波器描跡,顯示了根據本發明的另 15 一方面的由例4準備的晶胞(I)的切換動態特性。 第13圖是一個三維圖,顯示了根據本發明的另一方面 的反應時間(μ8),開始級別和結束級別的百分比之間的關 係’即’由例4準備的晶胞⑴從灰度(greylevel)到灰度的切 換時間。 2〇 根據本發明的另一方面’第14圖顯示了根據例5準備的 晶胞(II)的傳輸和電壓之間的關係。 第15圖是一個三維圖,顯示了根據本發明的另一方面 的反應時間(抑)’開始級別和結束級別的百分比之間的關 係’即’由例5準備的晶胞(11)從灰度到灰度的切換時間。 45 1362524 第93132205號申請案修正頁 101.01.12. 【主要元件符號說明】 1…液晶晶胞 40…垂直取向材料 2,3…起偏器 42…垂直材料溶液 4···頂部基板 44…水平取向材料 5…底部基板 46···混合物 6,7…導電電極 45…水平材料溶液 8···頂部取向層 46···混合溶液 9···底部取向層 47…液體膜 10…液晶層 48…固體膜 10B…液晶分子 50…固體膜 12…外部鏡面 52…液晶取向層 13,14…延遲膜 46Kn : 14.4 ; Κ 33 : 19.1 • Orientation layer: According to Examples 1-3, it is prepared to provide 5 〇. Pre-tilt orientation layer • Mirror: Directly vapor-deposited aluminum film onto the glass. Internal implementation. 5 • Ultraviolet epoxy resin··Buy from BOIS Technology Ltd' • Spacer: purchased from BOIS Technology Ltd; Catalog No. PF50 • The process of preparing the LCD unit cell is the same as that described in Examples 4 and 5. Further, as shown in Fig. 1C (12), a mirror surface is placed behind the liquid crystal cell. In other examples, the mirror may be placed inside the liquid crystal cell and at the top of the substrate as part of the active matrix substrate. The polarizer is an input polarizer placed in a position as shown in Figure 1 (Figure (2). In this example, there is no output polarizer. Construction: • Cell gap: 3 microns 15 • Pretilt angle of two orientation layers: 50. (opposite sign) • Orientation of the liquid crystal layer: at all operating voltages in a curved state because the beam passes through the unit cell twice, the required birefringence ratio is unit cell 1 The example is less required. This is important for the reaction rate of the liquid crystal cell. Because the cell gap can now be halved, the speed can be almost four times faster. (Normally, the reaction time of a liquid crystal cell is The square of the cell gap is inversely proportional.) And, since the path length now becomes twice the length of the cell 1 and the aa cell II, there may be more options for the birefringence of the liquid crystal material. The description of the resulting alignment layer can be used in many applications. Example 43 1362524 Male "93132205 Application Revision Page ΟΟΙ. For example, it can be used in a liquid crystal cell of an LCD device. The LCD device of the alignment layer has many advantages such as improved reaction speed, wide viewing angle, and excellent image without image sticking properties. Other applications that can be conceived by those skilled in the art will not be described in detail herein. The specification and the practice of the invention are disclosed herein. The embodiments of the invention will be apparent to those skilled in the art. BRIEF DESCRIPTION OF THE DRAWINGS [Brief Description] FIGS. 1A and 1C are cross-sectional views showing a part of a liquid crystal display device according to an aspect of the present invention. FIG. 2 is a view showing a liquid crystal crystal according to another aspect of the present invention. A cross-sectional view of a portion of the cell. Figure 3 shows the liquid crystal director in the Cartesian coordinate. 15 Figure 3A shows a polarizer, analyzer, light and observer relative to another aspect of the present invention. The position of the liquid crystal cell. Fig. 4 shows a process of fabricating a liquid crystal alignment layer according to another aspect of the present invention. 5A, 5B and 5C The figure is a set of photographs showing examples of nano and micro regions of a solid film formed of a liquid crystal layer agent according to another aspect of the present invention. Fig. 6A shows another aspect according to the present invention. The relationship between the pretilt angle and the concentration of the vertical alignment material (JALS2021). The alignment film is formed by spin coating. 44 1362524 \% 93132205 Ef I#f¥iTw — ~~~L__i2〇U2: 6B The figure shows the relationship between the pretilt angle and the concentration of the vertical alignment material (JALS2021) according to another aspect of the present invention. Here, the alignment film is formed by a roll printing method. Fig. 7 shows according to the present invention. In another aspect, the relationship between the polar error 5 constant energy and the concentration of the vertical alignment material (JALS2021), Figs. 8A and 8B respectively show the liquid crystal layer according to another aspect of the present invention. (A) oblique expansion and (B) bending deformation orientation. Fig. 9 is a view showing the elastic deformation energy of the curved and oblique orientation of a liquid crystal layer according to another aspect of the present invention. 10 Figure 10 shows a bend orientation at (A) zero voltage and (B) high voltage in accordance with another aspect of the present invention. Fig. 11 is a view showing the relationship between the transmission and the voltage of the unit cell (1) prepared by the example 4 according to another aspect of the present invention. Figures 12A and 12B are oscilloscope traces showing the switching dynamics of the unit cell (I) prepared by Example 4 in accordance with another aspect of the present invention. Figure 13 is a three-dimensional diagram showing the relationship between the reaction time (μ8), the percentage of the start level and the end level according to another aspect of the present invention 'i' from the unit cell prepared by Example 4 (1) from gray scale ( Greylevel) to grayscale switching time. 2〇 According to another aspect of the invention, Fig. 14 shows the relationship between the transmission and the voltage of the unit cell (II) prepared according to Example 5. Figure 15 is a three-dimensional diagram showing the relationship between the reaction time (inhibition) and the percentage of the end level in accordance with another aspect of the present invention 'i', the unit cell prepared by Example 5 (11) from the gray Degree to grayscale switching time. 45 1362524 Application No. 93132205 Amendment page 101.01.12. [Explanation of main component symbols] 1...Liquid crystal cell 40...Vertical alignment material 2,3...Polarizer 42...Vertical material solution 4···Top substrate 44...Horizontal Orienting material 5...bottom substrate 46··· mixture 6,7...conductive electrode 45...horizontal material solution 8···top alignment layer 46···mix solution 9··· bottom alignment layer 47...liquid film 10...liquid crystal layer 48...solid film 10B...liquid crystal molecule 50...solid film 12...external mirror 52...liquid crystal alignment layer 13,14...retardment film 46
Claims (1)
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US58293204P | 2004-06-26 | 2004-06-26 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| TW200600895A TW200600895A (en) | 2006-01-01 |
| TWI362524B true TWI362524B (en) | 2012-04-21 |
Family
ID=35781559
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| TW93132205A TWI362524B (en) | 2004-06-26 | 2004-10-22 | An improved pi-cell liquid crystal display |
Country Status (3)
| Country | Link |
|---|---|
| CN (1) | CN100520534C (en) |
| TW (1) | TWI362524B (en) |
| WO (1) | WO2006000133A1 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102169255A (en) | 2011-05-10 | 2011-08-31 | 深圳市华星光电技术有限公司 | OCB (Optically Compensated Birefringence) liquid crystal display panel and manufacturing method thereof as well as OCB liquid crystal display |
| US11822079B2 (en) | 2018-08-10 | 2023-11-21 | Apple Inc. | Waveguided display system with adjustable lenses |
| CN109828392A (en) * | 2019-03-06 | 2019-05-31 | 深圳市华星光电技术有限公司 | A kind of test method of liquid crystal display panel and its liquid crystal anchoring energy |
| CN114415401B (en) * | 2021-12-28 | 2023-07-25 | 昆山龙腾光电股份有限公司 | Display panel with switchable wide and narrow viewing angles, driving method and display device |
Family Cites Families (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2853629B2 (en) * | 1995-12-28 | 1999-02-03 | 日本電気株式会社 | Liquid crystal alignment film material and method of manufacturing liquid crystal display panel |
| GB2328290B (en) * | 1996-11-07 | 2000-08-09 | Lg Electronics Inc | Liquid crystal device |
| KR100526030B1 (en) * | 1998-09-03 | 2005-11-08 | 마쯔시다덴기산교 가부시키가이샤 | Liquid crystal display, method of manufacturing the same, method of driving liquid crystal display |
| JP3183654B2 (en) * | 1998-09-03 | 2001-07-09 | 松下電器産業株式会社 | Liquid crystal display device and driving method thereof |
| KR100448046B1 (en) * | 2000-12-05 | 2004-09-10 | 비오이 하이디스 테크놀로지 주식회사 | Reflective type fringe field swiching mode lcd |
-
2004
- 2004-10-22 TW TW93132205A patent/TWI362524B/en not_active IP Right Cessation
- 2004-10-25 WO PCT/CN2004/001207 patent/WO2006000133A1/en not_active Ceased
- 2004-10-25 CN CNB2004800438612A patent/CN100520534C/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| CN100520534C (en) | 2009-07-29 |
| WO2006000133A1 (en) | 2006-01-05 |
| TW200600895A (en) | 2006-01-01 |
| CN101023392A (en) | 2007-08-22 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| TWI310464B (en) | Compensation films for lcds | |
| TWI387816B (en) | Elliptical polarizer and vertical alignment type liquid crystal display device comprising the same | |
| KR101725997B1 (en) | Liquid crystal display device including alignment control layer containing polymerized mesogen, and method for fabricating the device | |
| JP5256714B2 (en) | Liquid crystal display element and manufacturing method thereof | |
| TWI360003B (en) | A liquid crystal alignment layer and methods of ma | |
| TWI361322B (en) | ||
| TW201219932A (en) | Liquid crystal display and method for preparation thereof | |
| JPH10232400A (en) | Photo-alignment composition, alignment film formed therefrom, and liquid crystal display device having the alignment film | |
| TW201627724A (en) | Polymer containing scattering type VA liquid crystal device | |
| TW200841290A (en) | Liquid crystal device | |
| Yoon et al. | Giant surfactants for the construction of automatic liquid crystal alignment layers | |
| JPH0764098A (en) | Ferroelectric liquid crystal element | |
| US20040070699A1 (en) | Liquid crystal optical element and method for fabricating the same | |
| TWI291986B (en) | Optically compensated birefringence alignment agent, liquid crystal device employing the same and fabrication method thereof | |
| TWI362524B (en) | An improved pi-cell liquid crystal display | |
| JP2556590B2 (en) | Liquid crystal element | |
| JP2007072213A (en) | Viewing angle compensation plate for vertical alignment type liquid crystal display device and vertical alignment type liquid crystal display device using the same | |
| US5973762A (en) | Ferroelectric liquid crystal cell with a monochevron structure of smectic layers | |
| JP3197392B2 (en) | Liquid crystal electro-optical device | |
| Lee et al. | Fast eight-domain patterned vertical alignment mode with reactive mesogen for a single-transistor-driving | |
| TWI376554B (en) | Liquid crystal display device | |
| JPH0720474A (en) | Liquid crystal alignment film for phase control element, method for forming the same, and phase control element | |
| TW200923445A (en) | Optical film, liquid crystal panels and liquid crystal displays | |
| JP3180171B2 (en) | Ferroelectric liquid crystal device | |
| JP2567128B2 (en) | Liquid crystal element |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| MK4A | Expiration of patent term of an invention patent |