JPH01265228A - Liquid crystal display element - Google Patents

Liquid crystal display element

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Publication number
JPH01265228A
JPH01265228A JP63094119A JP9411988A JPH01265228A JP H01265228 A JPH01265228 A JP H01265228A JP 63094119 A JP63094119 A JP 63094119A JP 9411988 A JP9411988 A JP 9411988A JP H01265228 A JPH01265228 A JP H01265228A
Authority
JP
Japan
Prior art keywords
liquid crystal
light
layer
crystal display
display element
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP63094119A
Other languages
Japanese (ja)
Inventor
Yoshitaka Ito
嘉高 伊藤
Norihisa Okamoto
岡本 則久
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Seiko Epson Corp
Original Assignee
Seiko Epson Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP63094119A priority Critical patent/JPH01265228A/en
Publication of JPH01265228A publication Critical patent/JPH01265228A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To realize the extremely bright liquid crystal display element by providing a specific optical function layer consisting of three layers on a light- incidence side transparent substrate. CONSTITUTION:On one of a couple of transparent substrates, i.e. 109, the optical function layers consisting of three layers or a birefringent layer 102, a microlens layer 105, and a lambda/2 phase difference layer 107 is provided from the incidence side of light. The incident light is separated by the birefringent layer 102 into an ordinary light beam 103 and an extraordinary light beam 104, which are converged by the microlens layer 105 so that both light beams are put one over the other spatially. Then either of the ordinary light beam 103 and extraordinary light beam 104 is rotated by the lambda/2 phase difference layer 107 to the plane of polarization of the other and then the incident light beam is converted into luminous flux which has a specific polarizing direction without being absorbed, so an extremely bright display which is essentially free from light absorption is made.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は液晶表示素子に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a liquid crystal display element.

〔従来の技術〕[Conventional technology]

液晶表示素子の代表例であるツィステッド・ネマティッ
ク(TN)型液晶表示素子の構造を第2図に示す。透明
な電極被膜をもつ一対の透明基板間に液晶を保持して成
る液晶セルの前後に、各々の偏光方向が互いに90@異
なるように2枚の偏光子が置かれている。偏光子とは入
射光の偏光方向を揃えるもので、特定の偏光成分をもつ
光だけを選択的に透過させる機能をもつ。液晶は液晶分
子の配列の仕方によって、液晶層を通る光の偏光面を回
転させる作用を有するため、2つの偏光子と液晶層を組
み合わせることにより、光の透過光量を制御する事がで
きる。液晶表示素子についての詳細は、例えば佐々木編
「液晶エレクトロニクスの基礎と応用jオーム社(19
79)にて説明されている。
FIG. 2 shows the structure of a twisted nematic (TN) type liquid crystal display element, which is a typical example of a liquid crystal display element. Two polarizers are placed before and after a liquid crystal cell, which is made up of a liquid crystal cell held between a pair of transparent substrates having transparent electrode coatings, so that their polarization directions differ by 90@ from each other. A polarizer aligns the polarization direction of incident light, and has the function of selectively transmitting only light with a specific polarization component. Liquid crystals have the effect of rotating the plane of polarization of light passing through the liquid crystal layer depending on how the liquid crystal molecules are arranged, so by combining two polarizers and a liquid crystal layer, the amount of transmitted light can be controlled. For more information about liquid crystal display elements, see, for example, "Fundamentals and Applications of Liquid Crystal Electronics" edited by Sasaki, Ohmsha (1993).
79).

〔発明が解決しようとする課頭〕[The problem that the invention attempts to solve]

しかし、従来の液晶表示素子に用いられるシート状の偏
光子は有機重合体物質を一軸性延伸配向して作られるた
め、量産性に優れ安価である反面、光吸収の二色性を利
用しているため、偏光子自体が入射光の一部を吸収する
ことになり光透過率が悪く、さらに、強い光に対しては
光吸収に伴う発熱作用により、偏光子自身が熱破壊を生
じる場合があるなどの問題を有していた。そこで、本発
明は以上のような問題点を解決するもので、その目的と
するところは、本質的に光吸収がなく、光透過率が高い
明るい液晶表示素子を提供することにある。
However, sheet polarizers used in conventional liquid crystal display devices are made by uniaxially stretching and aligning organic polymer materials, so they are easy to mass produce and are inexpensive. As a result, the polarizer itself absorbs a portion of the incident light, resulting in poor light transmittance.Furthermore, the polarizer itself may be thermally destroyed due to the heat generation effect associated with light absorption when exposed to strong light. There were some problems. SUMMARY OF THE INVENTION The present invention is intended to solve the above-mentioned problems, and its purpose is to provide a bright liquid crystal display element that essentially does not absorb light and has high light transmittance.

〔課題を解決するための手段〕[Means to solve the problem]

上記課題を解決するために本発明の液晶表示素子は、一
対の透明基板間に液晶を保持し、該液晶の電気光学効果
により光の透過量を制御して画像情報を表示する液晶表
示素子において、光の入射側に位置する一方の前記透明
基板上に、入射光束を偏光面が互いに直交する2つの直
線偏光成分に分離する層と、該分離された2つの直線偏
光成分を各々空間的に異なる位置に集光する層と、該集
光する手段により得られた一方の直線偏光成分の偏光面
を旋回させる層を形成したことを特徴とする。
In order to solve the above problems, the liquid crystal display element of the present invention is a liquid crystal display element that holds a liquid crystal between a pair of transparent substrates and displays image information by controlling the amount of light transmitted through the electro-optic effect of the liquid crystal. , on one of the transparent substrates located on the light incident side, there is a layer that separates the incident light beam into two linearly polarized light components whose polarization planes are orthogonal to each other, and a layer that spatially separates the two separated linearly polarized light components. It is characterized by forming a layer that focuses light at different positions and a layer that rotates the plane of polarization of one linearly polarized light component obtained by the light focusing means.

〔作用〕[Effect]

方解石や一軸配向性高分子重合体などの光学的異方性媒
体に、通常の光源が発する自然光を入射すると、媒質中
の光学的異方軸に相応した振動面を有する2つの光束(
常光及び異常光)に分離される。この現象は媒質の屈折
能が2つの光線軸間で異なるために生じる。
When natural light emitted from a normal light source is incident on an optically anisotropic medium such as calcite or a uniaxially oriented polymer, two light beams (
It is separated into ordinary light and extraordinary light). This phenomenon occurs because the refractive power of the medium is different between the two beam axes.

第1図は本発明の液晶表示素子の構成断面図であり、こ
の第1図に基付いて本発明の詳細な説明する。従来の液
晶表示素子で、偏光子が置かれている位置、つまり、光
源側に位置する透明基板上に3層から成る光学的機能層
が構成されている。
FIG. 1 is a cross-sectional view of the structure of a liquid crystal display element according to the present invention, and the present invention will be explained in detail based on FIG. In a conventional liquid crystal display element, an optically functional layer consisting of three layers is formed on a transparent substrate located at a position where a polarizer is placed, that is, located on the light source side.

まず、光学的異方性材料で構成された複屈折層(102
)により、入射光は常光線(103)  と異常光線(
104)  に分離され、両光線が空間的に重なり合わ
ないように、−旦異なる位置にレンズ(105)を用い
て集光される。次に、常光線または異常光線のどちらか
一方の偏光面を回転させて(第1図では異常光)、他方
(第1図では常光)の偏光面と合わせてやれば、入射光
線は吸収される事なく、すべて特定の偏光方向(第1図
そ・は常光線と同じ振動方向)を有する光束に変換され
、液晶表示素子の透明開口部に到達する。
First, a birefringent layer (102
), the incident light is divided into an ordinary ray (103) and an extraordinary ray (
104) and are focused using lenses (105) at different positions so that the two light beams do not spatially overlap. Next, by rotating the plane of polarization of either the ordinary ray or the extraordinary ray (extraordinary ray in Figure 1) and aligning it with the plane of polarization of the other (ordinary ray in Figure 1), the incident ray will be absorbed. All of the light is converted into a light beam having a specific polarization direction (the vibration direction in FIG. 1 is the same as that of ordinary light), and reaches the transparent aperture of the liquid crystal display element.

従って、液晶表示素子の光源に対向しない側に従来と同
様の偏光子を構成することにより、通常の液晶表示素子
と同様の表示機能を有し、尚かつ光吸収が無いため光の
利用効率が高い、つまり非常に明るい液晶表示素子とな
る。
Therefore, by configuring a polarizer similar to the conventional one on the side of the liquid crystal display element that does not face the light source, it can have the same display function as a normal liquid crystal display element, and also improve the efficiency of light use because there is no light absorption. This results in an expensive, or extremely bright, liquid crystal display element.

〔実施例〕〔Example〕

以下、実施例に基づき本発明の詳細な説明する。 Hereinafter, the present invention will be explained in detail based on Examples.

但し、本発明は以下の実施例に限定されるものではない
。
However, the present invention is not limited to the following examples.

[実施例1] 第1図はTN型液晶表示素子の構成断面図である。透明
な共通電i (110)  が形成されている一対の透
明ガラス基板の第1の基板上(109)  にスペーサ
ーを介して^/2位相差層(107)  を形成した。
[Example 1] FIG. 1 is a cross-sectional view of the structure of a TN type liquid crystal display element. A ^/2 retardation layer (107) was formed on the first substrate (109) of a pair of transparent glass substrates on which a transparent common electrode i (110) was formed, with a spacer interposed therebetween.

この位相差層はストライプ状に幅100μmの位相差肩
部(107)  と、やはり幅100μmの空気層部(
106)  が交互に並んで配列している。
This retardation layer has a striped retardation shoulder part (107) with a width of 100 μm and an air layer part (107) with a width of 100 μm.
106) are arranged alternately.

その上に透明ガラス板をスペーサーとして介し、幅20
0μm、ピッチ200μmのレンチキュラー型レンズか
らなるマイクロレンズ層(105)  を形成した。こ
の時マイクロレンズの光軸が位相差肩部と空気層部の境
界上に位置するようにした。
A transparent glass plate is placed on top of it as a spacer, and the width is 20mm.
A microlens layer (105) consisting of lenticular lenses with a pitch of 0 μm and a pitch of 200 μm was formed. At this time, the optical axis of the microlens was positioned on the boundary between the phase difference shoulder and the air layer.

このマイクロレンズ層は、ガラス板上にメタクリレート
系のネガレジストをスピンコードし、写真製版技術を用
いて、露光、現像し、上記ネガレジストをオーバーエツ
チングする事によりレンチキュラー型レンズアレイを形
成した。さらにその上にやはりスペーサーを介して複屈
折層(102)  を形成した。複屈折層はシート状の
ポリイミド系重合体物質を一方向延伸した後、加圧成形
して得た。
For this microlens layer, a methacrylate negative resist was spin-coded on a glass plate, exposed and developed using photolithography, and the negative resist was over-etched to form a lenticular lens array. Furthermore, a birefringent layer (102) was formed thereon via a spacer. The birefringent layer was obtained by unidirectionally stretching a sheet-like polyimide polymer material and then press-molding it.

ここで、複屈折層により分離された常光線(103)と
異常光線(104)  が、先のマイクロレンズにより
位相基層部と空気層部それぞれ焦点を結ぶように位置合
わせを行なった。尚、本実施例の構成に於いては第1の
透明ガラス基板上にマイクロレンズ層(108)  が
形成されているが、このレンズは液晶層部に効果的に光
を導くために設けであるものであり、必ずしも必要なも
のではない。上記の構成により得た偏光素子は従来の光
吸収の二色性を利用した偏光板とは異なり、本質的に光
吸収を全くともなわずに、偏光面を一定方向に揃えるこ
とが可能である。
Here, the ordinary ray (103) and the extraordinary ray (104) separated by the birefringent layer were aligned using the aforementioned microlens so that they were focused on the phase base layer and the air layer, respectively. In the configuration of this embodiment, a microlens layer (108) is formed on the first transparent glass substrate, and this lens is provided to effectively guide light to the liquid crystal layer. It's a thing, but it's not necessarily a necessity. Unlike conventional polarizing plates that utilize dichroism of light absorption, the polarizing element obtained with the above configuration is capable of aligning the plane of polarization in a fixed direction without essentially absorbing light at all.

そして上記基板と第2の透明ガラス基板(112)を共
通電極が直交するように、スペーサー及びギャップ材を
介して液晶セルを組み、液晶を封入した。その後、第1
の基板上に形成した偏光素子により形成される偏光面と
直交するように、第2の基板の裏面に従来の偏光板(1
13)  を配置した。
Then, a liquid crystal cell was assembled between the above substrate and a second transparent glass substrate (112) via a spacer and a gap material so that the common electrodes were perpendicular to each other, and liquid crystal was sealed. Then the first
A conventional polarizing plate (1
13) was placed.

上記の構成により得られた偏光素子を備えたTN型液晶
表示素子は、従来のものと比較して明るさが約2倍に向
上していた。また、入射光の強度を大幅に増大させても
、第1の基板上に形成した偏光素子は光吸収作用を伴わ
ないため、熱破壊を生じず、長時間安定して機能するこ
とが確認された。
The brightness of the TN liquid crystal display element equipped with the polarizing element obtained with the above structure was approximately twice as high as that of the conventional one. In addition, even if the intensity of the incident light is significantly increased, the polarizing element formed on the first substrate does not have a light absorption effect, so it has been confirmed that it does not cause thermal damage and functions stably for a long time. Ta.

[実施例2] 第2図はTPT液晶表示素子の構成断面図である。透明
な石英基板上(204)  に液晶制御のためのスイッ
チング素子としてポリシリコン薄膜トランジスター(T
PT)  (203)  をマトリヅクス状に形成した
。一方、対向基板(2Q1)  には先の実施例1の場
合と同様の手段により、偏光素子及び透明な共通電極を
形成した。そして、上記一対の基板をスペーサー及びギ
ャップ材を介して液晶セルを組み液晶を封入した。さら
に、実施例1の場合と同様に石英基板の裏面に、従来の
偏光板(113)を配置しTPT液晶表示素子とした。
[Example 2] FIG. 2 is a cross-sectional view of the structure of a TPT liquid crystal display element. A polysilicon thin film transistor (T
PT) (203) was formed into a matrix. On the other hand, a polarizing element and a transparent common electrode were formed on the counter substrate (2Q1) by the same means as in Example 1 above. Then, a liquid crystal cell was assembled using the above-mentioned pair of substrates via a spacer and a gap material, and liquid crystal was sealed therein. Furthermore, as in Example 1, a conventional polarizing plate (113) was placed on the back surface of the quartz substrate to form a TPT liquid crystal display element.

本TPT液晶表示素子に於いても先のTN型液晶表示素
子の場合と同様に、大幅な明るさの改善が確認された。
In the present TPT liquid crystal display element, a significant improvement in brightness was confirmed as in the case of the above-mentioned TN type liquid crystal display element.

TPT液晶表示素子は透過光量を細かく多段階制御でき
るため、液晶テレビ、液晶プロジェクタ−などに使用さ
れ、映像及び画像処理分野に於いてその応用が急速に拡
大している。
Since TPT liquid crystal display elements can finely control the amount of transmitted light in multiple stages, they are used in liquid crystal televisions, liquid crystal projectors, etc., and their applications are rapidly expanding in the fields of video and image processing.

また、液晶制御のためのスイッチング素子に、金属−絶
縁体−金属構造のダイオード素子(MIM)を用いた液
晶表示素子が開発されているが、このMIM液晶表示素
子に於いても本発明の偏光素子を組み込み、表示素子の
明るさを大幅に改善することが可能である。
Furthermore, a liquid crystal display element using a metal-insulator-metal structure diode element (MIM) as a switching element for liquid crystal control has been developed, and this MIM liquid crystal display element also uses the polarized light of the present invention. It is possible to significantly improve the brightness of the display element by incorporating the display element.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明の液晶表示素子は、液晶表示
素子の光の入射側にくる従来の偏光板に変わって、光の
入射側に位置する一方の前記透明基板上に、入射光東香
偏光面が互いに直交する2つの直線偏光成分に分離する
層と、該分離された2つの直線偏光成分を各々空間的に
異なる位置に集光する層と、該集光する手段により得ら
れた一方の直線偏光成分の偏光面を旋回させる層を構成
することにより、本質的に光吸収が非常に少なく、はと
んど全ての光の偏光方向を一方向に揃えた状態で、液晶
画素部に導くことが可能であるため、従来にない非常に
明るい液晶表示素子とすることが可能である。また、液
晶表示素子の光の入射側に従来の偏光板を用いていない
ため、強い光を入射した場合にも、発熱による自己破壊
を招くことなく長時間安定的に機能する。液晶表示素子
は低電圧駆動、低消費電力を特徴として広く普及してい
るが、偏光成分を制御して情報を伝達するため光の利用
効率が低く、表示面が暗いのが欠点の一つであった。し
かし、本発明の液晶表示素子は従来のものと比較して、
表示面に於ける明るさが約2倍に向上しており、非常に
明るい表示素子である。従って、液晶テレビ、液晶グロ
ジェクターなどに最適な液晶表示素子であるといえる。
As explained above, in the liquid crystal display element of the present invention, instead of the conventional polarizing plate placed on the light incidence side of the liquid crystal display element, the incident light is placed on one of the transparent substrates located on the light incidence side. A layer that separates light into two linearly polarized light components whose planes of polarization are orthogonal to each other, a layer that focuses the two separated linearly polarized light components at spatially different positions, and a layer that is obtained by the light focusing means. By configuring a layer that rotates the polarization plane of the linearly polarized light component, light absorption is essentially very low, and the polarization direction of all light is aligned in one direction, and the liquid crystal pixel area is Therefore, it is possible to create an extremely bright liquid crystal display element that has never been seen before. Furthermore, since a conventional polarizing plate is not used on the light incident side of the liquid crystal display element, even when strong light is incident, the liquid crystal display element functions stably for a long time without causing self-destruction due to heat generation. Liquid crystal display elements are widely used due to their low voltage drive and low power consumption, but one of their drawbacks is that they have low light utilization efficiency and dark display surfaces because they transmit information by controlling polarization components. there were. However, compared to the conventional liquid crystal display element, the liquid crystal display element of the present invention has
The brightness on the display surface is approximately doubled, making it an extremely bright display element. Therefore, it can be said that it is an optimal liquid crystal display element for liquid crystal televisions, liquid crystal glow projectors, and the like.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明のTN型液晶表示素子の構成断面図。 第2図は本発明のTFT型液晶表示素子の構成断面図。 101・・・入射光 102・・・複屈折層 103・・・常光線 104・・・異常光線 105・・・マイクロレンズ層 106・・・空気層部 107・・・位相基層部 108・・・マイクロレンズ層 109・・・第1の透明ガラス基板 110・・・共通電極 111・・・液晶層部 112・・・第2の透明ガラス基板 113・・・偏光板 114・・・出射光 115・・・λ/2位相差層を通過した光の偏光方向(
紙面に平行) 116・・・偏光板113の偏光方向(紙面に垂直) 201・・・対向基板 20.2・・・画素電極 203・・・TFT素子 204・・・石英基板 以  上 出願人 セイコーエプソン 株式会社 代理人弁理士 鈴木喜三部(化1名) 0ノ01 第1図 0ν101 第2図
FIG. 1 is a cross-sectional view of the structure of a TN type liquid crystal display element of the present invention. FIG. 2 is a cross-sectional view of the structure of the TFT type liquid crystal display element of the present invention. 101... Incident light 102... Birefringent layer 103... Ordinary ray 104... Extraordinary ray 105... Microlens layer 106... Air layer portion 107... Phase base layer portion 108... Microlens layer 109...First transparent glass substrate 110...Common electrode 111...Liquid crystal layer portion 112...Second transparent glass substrate 113...Polarizing plate 114...Emitted light 115...・Polarization direction of light passing through the λ/2 retardation layer (
116...Polarization direction of the polarizing plate 113 (perpendicular to the page) 201...Counter substrate 20.2...Pixel electrode 203...TFT element 204...Quartz substrate or above Applicant: Seiko Epson Co., Ltd. Agent Patent Attorney Kizobe Suzuki (1 person) 0no01 Figure 1 0ν101 Figure 2

Claims (1)

【特許請求の範囲】[Claims] 一対の透明基板間に液晶を保持し、該液晶の電気光学効
果により光の透過量を制御して画像情報を表示する液晶
表示素子において、光の入射側に位置する一方の前記透
明基板上に、入射光束を偏光面が互いに直交する2つの
直線偏光成分に分離する層と、該分離された2つの直線
偏光成分を各々空間的に異なる位置に集光する層と、該
集光する手段により得られた一方の直線偏光成分の偏光
面を旋回させる層を形成したことを特徴とする液晶表示
素子。
In a liquid crystal display element that displays image information by holding a liquid crystal between a pair of transparent substrates and controlling the amount of light transmission through the electro-optical effect of the liquid crystal, one of the transparent substrates located on the light incident side is , a layer that separates an incident light beam into two linearly polarized light components whose polarization planes are orthogonal to each other, a layer that focuses the two separated linearly polarized light components at spatially different positions, and a means for focusing the light. A liquid crystal display element comprising a layer that rotates the plane of polarization of one of the obtained linearly polarized light components.
JP63094119A 1988-04-15 1988-04-15 Liquid crystal display element Pending JPH01265228A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63094119A JPH01265228A (en) 1988-04-15 1988-04-15 Liquid crystal display element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63094119A JPH01265228A (en) 1988-04-15 1988-04-15 Liquid crystal display element

Publications (1)

Publication Number Publication Date
JPH01265228A true JPH01265228A (en) 1989-10-23

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP63094119A Pending JPH01265228A (en) 1988-04-15 1988-04-15 Liquid crystal display element

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JP (1) JPH01265228A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5187599A (en) * 1990-02-01 1993-02-16 Sharp Kabushiki Kaisha Display including two microlens arrays with unequal focal lengths and congruent focal points
EP0753780A4 (en) * 1994-12-28 1997-12-29 Seiko Epson Corp POLARIZED LIGHT LIGHTING APPARATUS AND PROJECTION TYPE DISPLAY DEVICE
US5959704A (en) * 1996-02-08 1999-09-28 Fujitsu Limited Display device having diffraction grating

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5187599A (en) * 1990-02-01 1993-02-16 Sharp Kabushiki Kaisha Display including two microlens arrays with unequal focal lengths and congruent focal points
EP0753780A4 (en) * 1994-12-28 1997-12-29 Seiko Epson Corp POLARIZED LIGHT LIGHTING APPARATUS AND PROJECTION TYPE DISPLAY DEVICE
US6147802A (en) * 1994-12-28 2000-11-14 Seiko Epson Corporation Polarization luminaire and projection display
US6310723B1 (en) 1994-12-28 2001-10-30 Seiko Epson Corporation Polarization luminaire and projection display
US6344927B1 (en) 1994-12-28 2002-02-05 Seiko Epson Corporation Polarization luminaire and projection display
US6411438B1 (en) 1994-12-28 2002-06-25 Seiko Epson Corporation Polarization luminaire and projection display
US6445500B1 (en) 1994-12-28 2002-09-03 Seiko Epson Corporation Polarization luminaire and projection display
US6667834B2 (en) 1994-12-28 2003-12-23 Seiko Epson Corporation Polarization luminaire and projection display
US7119957B2 (en) 1994-12-28 2006-10-10 Seiko Epson Corporation Polarization luminaire and projection display
US5959704A (en) * 1996-02-08 1999-09-28 Fujitsu Limited Display device having diffraction grating
US6639642B1 (en) 1996-02-08 2003-10-28 Fujitsu Limited Display device having diffraction grating

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