JP2900896B2 - Polarizing element and lighting device - Google Patents
Polarizing element and lighting deviceInfo
- Publication number
- JP2900896B2 JP2900896B2 JP8278377A JP27837796A JP2900896B2 JP 2900896 B2 JP2900896 B2 JP 2900896B2 JP 8278377 A JP8278377 A JP 8278377A JP 27837796 A JP27837796 A JP 27837796A JP 2900896 B2 JP2900896 B2 JP 2900896B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- polarization
- phase difference
- difference layer
- layer
- 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.)
- Expired - Lifetime
Links
- 230000010287 polarization Effects 0.000 claims description 52
- 238000006243 chemical reaction Methods 0.000 claims description 6
- 238000000926 separation method Methods 0.000 claims description 5
- 238000005286 illumination Methods 0.000 claims 1
- 230000001678 irradiating effect Effects 0.000 claims 1
- 230000003287 optical effect Effects 0.000 description 9
- 239000000463 material Substances 0.000 description 8
- 230000031700 light absorption Effects 0.000 description 6
- 239000013078 crystal Substances 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 238000000465 moulding Methods 0.000 description 3
- 229920000620 organic polymer Polymers 0.000 description 3
- 229920000642 polymer Polymers 0.000 description 3
- 238000002834 transmittance Methods 0.000 description 3
- 229910021532 Calcite Inorganic materials 0.000 description 2
- 230000020169 heat generation Effects 0.000 description 2
- 239000004973 liquid crystal related substance Substances 0.000 description 2
- 239000002861 polymer material Substances 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- -1 (trifluoromethyl)- Chemical class 0.000 description 1
- 239000004642 Polyimide Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000000835 fiber Substances 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 238000001746 injection moulding Methods 0.000 description 1
- 238000004898 kneading Methods 0.000 description 1
- 239000006210 lotion Substances 0.000 description 1
- 238000003754 machining Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 229920001721 polyimide Polymers 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- 239000012780 transparent material Substances 0.000 description 1
Landscapes
- Polarising Elements (AREA)
- Liquid Crystal (AREA)
- Microscoopes, Condenser (AREA)
Description
【0001】[0001]
【発明の属する技術分野】本発明は各種表示体、光スイ
ッチ、光アイソレーレータ、光学フィルター、各種光測
定機等に有用な偏光素子、特に偏光分離合成素子に関す
るものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a polarizing element useful for various displays, optical switches, optical isolators, optical filters, various optical measuring devices, etc., and more particularly to a polarization separating / combining element.
【0002】[0002]
【従来の技術】従来、通常の光源が発する自然光から直
線偏光を得る場合には、ウオラストン形、ローション形
などの複屈折性プリズム、あるいは光吸収の二色性を利
用した一方向延伸配向フィルム等が利用されてきた。2. Description of the Related Art Conventionally, when linearly polarized light is obtained from natural light emitted from an ordinary light source, a birefringent prism such as a Wollaston type or a lotion type or a unidirectionally stretched oriented film utilizing dichroism of light absorption is used. Has been used.
【0003】[0003]
【発明が解決しようとする課題】しかし、複屈折性プリ
ズムは大きな単結晶体を精密加工して作る必要があるこ
とから非常に高価であるばかりか、特定の用途に要求さ
れる望ましい形状または配置に容易に形成できない。さ
らに、得られる単結晶体の大きさに限度があるため、そ
れがまた利用の範囲を著しく限定しているなどの問題を
有していた。一方、延伸配向フィルムは有機重合体物質
により形成されているため、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、フィルム自体
が入射光の一部を吸収することになり光透過率が低い。
さらに、強い光に対しては光吸収に伴う発熱作用によ
り、フィルム自身が自己破壊を生じる場合があるなどの
欠点を有していた。However, birefringent prisms are not only very expensive due to the necessity of precision machining of a large single crystal, but also have a desirable shape or arrangement required for a specific application. Cannot be easily formed. In addition, the size of the obtained single crystal body is limited, which also has a problem that the range of use is significantly limited. On the other hand, the stretch-oriented film is made of an organic polymer material, so it is excellent in mass productivity and inexpensive, but because it utilizes dichroism of light absorption, the film itself absorbs a part of incident light. That is, the light transmittance is low.
Further, the film has a drawback that the film itself may cause self-destruction with respect to strong light due to a heat generation effect accompanying light absorption.
【0004】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
収がなくコンパクトかつ安価な偏光素子を提供すること
にある。The present invention has been made to solve the above problems, and an object of the present invention is to provide a compact and inexpensive polarizing element having essentially no light absorption.
【0005】[0005]
【課題を解決するための手段】上記課題を解決するため
に本発明の偏光素子は、入射光を偏光面の揃った光に変
換して出射する偏光素子であって、前記入射光を、偏光
面が互いに直交する2種類の偏光成分の光に分離して、
互いに異なる方向へ出射する偏光分離手段と、偏光面を
旋回させる位相差層が、同一平面内の複数箇所に選択的
に形成された偏光変換手段と、前記偏光変換手段の出射
面側に配置された偏光板と、前記偏光分離手段から出射
された前記2種類の偏光成分の光のうち、一方の光を前
記位相差層の形成されている部分に導き、他方の光を前
記位相差層の形成されていない部分に導く集光手段とを
有し、前記集光手段は、各々、互いに異なる方向から入
射した前記2種類の偏光成分の光のうち、一方の光を前
記位相差層の形成されている部分に導き、他方の光を前
記位相差層の形成されていない部分に導く複数のレンズ
体を備え、前記一方の光は前記位相差層を経て出射さ
れ、前記他方の光は前記位相差層が形成されていない部
分を経て出射されることを特徴とする。また、本発明の
照明装置は、入射光を偏光面の揃った光に変換して照射
する照明装置であって、前記入射光を、偏光面が互いに
直交する2種類の偏光成分の光に分離して、互いに異な
る方向へ出射する偏光分離手段と、偏光面を旋回させる
位相差層が、同一平面内の複数箇所に選択的に形成され
た偏光変換手段と、前記偏光変換手段の出射面側に配置
された偏光板と、前記偏光分離手段から出射された前記
2種類の偏光成分の光のうち、一方の光を前記位相差層
の形成されている部分に導き、他方の光を前記位相差層
の形成されていない部分に導く集光手段とを有し、前記
集光手段は、各々、互いに異なる方向から入射した前記
2種類の偏光成分の光のうち、一方の光を前記位相差層
の形成されている部分に導き、他方の光を前記位相差層
の形成されていない部分に導く複数のレンズ体を備え、
前記一方の光は前記位相差層を経て出射され、前記他方
の光は前記位相差層が形成されていない部分を経て照射
されることを特徴とする。In order to solve the above-mentioned problems, a polarizing element according to the present invention is a polarizing element that converts incident light into light having a uniform polarization plane and emits the light. Separated into two types of polarized light components whose planes are orthogonal to each other,
Polarization separation means for emitting light in different directions, a phase difference layer for rotating the polarization plane, polarization conversion means selectively formed at a plurality of locations in the same plane, and an emission surface side of the polarization conversion means are arranged. Polarizing plate, and of the two types of polarized light components emitted from the polarization separating means, one light is guided to a portion where the phase difference layer is formed, and the other light is directed to the phase difference layer. Light-collecting means for guiding the light to the non-formed portion, wherein the light-collecting means forms one of the two types of polarized light components incident from different directions on the phase difference layer. A plurality of lens bodies that guide the other light to a portion where the phase difference layer is not formed, wherein the one light is emitted through the phase difference layer, and the other light is the other light. Emitted through the part where the retardation layer is not formed And wherein the door. Further, the lighting device of the present invention is a lighting device that converts incident light into light having a uniform polarization plane and irradiates the light, and separates the incident light into two kinds of polarization component lights whose polarization planes are orthogonal to each other. Then, polarization separating means for emitting light in different directions from each other, a phase difference layer for rotating the polarization plane, polarization converting means selectively formed at a plurality of locations in the same plane, and an emission surface side of the polarization converting means And one of the two kinds of polarized light components emitted from the polarization splitting means is guided to a portion where the retardation layer is formed, and the other light is directed to the polarized light component. Light condensing means for guiding the light to the portion where the retardation layer is not formed, wherein the light condensing means converts one of the two types of polarized light components incident from different directions from each other to the phase difference. To the portion where the layer is formed and direct the other light to the phase difference layer Comprising a plurality of lens body leading to made that is not part,
The one light is emitted through the phase difference layer, and the other light is emitted through a portion where the phase difference layer is not formed.
【0006】[0006]
【発明の実施の形態】以下、いくつかの実施形態(実施
例)に基づき本発明を詳細に説明する。但し、本発明は
以下の実施形態に限定されるものではない。DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, the present invention will be described in detail based on several embodiments (examples). However, the present invention is not limited to the following embodiments.
【0007】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、通常の光瀕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。[0007] When natural light, which emits light normally, is incident on an optically anisotropic medium such as calcite or uniaxially oriented polymer, it has a vibrating surface corresponding to the optically anisotropic axis in the medium.
It is split into two light beams (ordinary light and extraordinary light). This phenomenon occurs because the refractive power of the medium differs between the two light axes.
【0008】図1は本発明の偏光素子の一実施形態を示
す構成断面図であり、この図1に基付いて下記実施例の
作用を説明する。FIG. 1 is a sectional view showing the structure of an embodiment of the polarizing element of the present invention. The operation of the following embodiment will be described with reference to FIG.
【0009】まず、光学的異方性材料で構成された複屈
折層102により入射光線は常光線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、一旦
異なる位置にレンズ105を用いて集光される。この場
合、常光線の偏光方向は紙面と平行、異常光線の偏光方
向は紙面に対し垂直方向とする。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(図1では
異常光)、他方(図1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(図1では常光線と同じ紙面に平行な振動方向とな
る)を有する光束108に変換することが可能となる。First, an incident light beam is separated into an ordinary light beam 103 and an extraordinary light beam 104 by a birefringent layer 102 made of an optically anisotropic material, and the light beams are temporarily shifted to different positions so as not to spatially overlap each other. The light is condensed using the lens 105. In this case, the polarization direction of the ordinary ray is parallel to the page, and the polarization direction of the extraordinary ray is perpendicular to the page. Next, if the polarization plane of one of the ordinary ray and the extraordinary ray is rotated (the extraordinary ray in FIG. 1) and the polarization plane of the other ray (the ordinary ray in FIG. 1) is used, the incident ray is absorbed. Instead, the light beam can be converted into a light beam 108 having a specific polarization direction (in FIG. 1, the vibration direction is the same as the ordinary ray in the plane of the paper).
【0010】(実施例1) 光学的異方性材料から成る複屈折層102に入射した光は
互いに直交する偏光面を有する一対の直線偏光成分(常
光線103、異常光線104)に分離される。複屈折層による
2つの偏光成分の分離角は、複屈折層を形成する材料の
複屈折能と複屈折層の形状(層の下部に設けられたテー
パーの角度)により決定される。そのため材料の選択と
テーパーの角度の決定が重要となる。一例を挙げると常
光及び異常光に対する屈折率が各々1.5、2.0であ
る複屈折性材料で複屈折層を形成し、その場合のテーパ
ーの角度を10°とすると、複屈折層による常光線及び
異常光線の分離角は約5.2°となる。本実施例ではこ
の値を採用した。(Example 1) Light incident on a birefringent layer 102 made of an optically anisotropic material is separated into a pair of linearly polarized light components (ordinary ray 103 and extraordinary ray 104) having mutually orthogonal polarization planes. . The separation angle of the two polarization components by the birefringent layer is determined by the birefringence ability of the material forming the birefringent layer and the shape of the birefringent layer (the angle of the taper provided below the layer). Therefore, it is important to select a material and determine the taper angle. To give an example, the birefringent layer is formed of a birefringent material having a refractive index of 1.5 and 2.0 for ordinary light and extraordinary light, respectively. The separation angle between the ordinary ray and the extraordinary ray is about 5.2 °. In this embodiment, this value is adopted.
【0011】複屈折層を形成する材料は方解石、石英な
どの無機単結晶、あるいは一軸配向性の有機重合体など
透明で複屈折性を示す材料であれば使用可能であるが、
加工性を考えた場合、後者の方が優れている。有機重合
体物質はフィルム、シート、コーティング膜、繊維など
種々の形に形成または成形できる。このような重合体物
質の一例を挙げると、例えばポリイミド化合物の一種で
あるポリ〔2,2’−ビス(トリフルオロメチル)−
4,4’−ビフェニレン〕−2”,2”−ジメトキシ−
4,4”−ビフェニレンジカルボキシアミドが使用可能
である。As a material for forming the birefringent layer, any material can be used as long as it is a transparent material having birefringence such as an inorganic single crystal such as calcite or quartz, or a uniaxially oriented organic polymer.
When considering workability, the latter is superior. The organic polymer material can be formed or formed into various forms such as films, sheets, coatings, fibers and the like. An example of such a polymer substance is poly [2,2'-bis (trifluoromethyl)-, which is a kind of polyimide compound.
4,4'-biphenylene] -2 ", 2" -dimethoxy-
4,4 "-biphenylenedicarboxamide can be used.
【0012】複屈折層はシート状の重合体物質を一方向
延伸配向した後、加圧成形して得た。複屈折層により分
離された互いに偏光面が直交する常光及び異常光は、レ
ンズ体105により各々集光され、各々異なる位置に焦点
を形成する。このレンズ体は通常の光学的等方性材料を
用いて形成すればよい。その成形方法は種々あるが、加
圧成形法、射出成形法が代表例である。次に、異常光練
の焦点位置に(常光線の焦点位置でも良い)に入/2の
位相差層106を形成し、異常光線が位相差層を通過する
ことにより光線の偏光面が90°旋回するように構成し
た。つまり、偏光素子の出射端に於いてはすべての光線
の偏光方向は一方向に揃ったことになる。The birefringent layer was obtained by unidirectionally stretching and orienting a sheet-like polymer substance and then press-molding. The ordinary light and the extraordinary light, whose polarization planes are orthogonal to each other, separated by the birefringent layer are respectively condensed by the lens body 105 and form focal points at different positions. This lens body may be formed using a usual optically isotropic material. Although there are various molding methods, a pressure molding method and an injection molding method are typical examples. Next, at the focal position of the extraordinary light kneading (or the focal position of the ordinary ray), a phase difference layer 106 of 2 is formed, and the extraordinary ray passes through the retardation layer, so that the polarization plane of the ray becomes 90 °. It was configured to turn. That is, at the output end of the polarizing element, the polarization directions of all the light beams are aligned in one direction.
【0013】従来の偏光板を用いた方法では光透過率が
最大50%程度であったのに対して、本発明の偏光素子
を用いた方法ではほとんど100%近い光透過率が得ら
れる。焦点を通過した光は集光時と同じ角度を持って広
がるが、以上の構成をある程度微小なサイズ(本実施例
では集光レンズ径が100μm)で実現すれば、光線の
発散性はそれほど問題とはならず、光の吸収を伴わずに
入射光のほとんど全てを、偏光面の揃った出射光とする
ことが可能である。The light transmittance of the conventional method using a polarizing plate is about 50% at the maximum, whereas the light transmittance of the method using the polarizing element of the present invention is almost 100%. The light passing through the focal point spreads at the same angle as that at the time of focusing. However, if the above configuration is realized with a small size to some extent (in this embodiment, the diameter of the focusing lens is 100 μm), the divergence of the light ray is not so significant. Rather, almost all of the incident light can be converted into outgoing light with a uniform polarization plane without light absorption.
【0014】(実施例2) 第2図は実施例1の偏光素子の応用例を示したもので、
偏光素子と偏光板を組み合わせて構成した偏光素子を示
す構成断面図である。本発明の偏光素子を単独で使用し
ても、かなり偏光面の揃った光束を得ることができる
が、第2図に示すようにλ/2の位相差層106の後方
に、透過光の偏光方向に揃えて偏光板201を配置すれ
ば、極めて偏光方向の揃った出射光を得ることができ
る。本発明の偏光素子を光学測定機器などに組み込む場
合には上記のような構成とすることが望ましい。Embodiment 2 FIG. 2 shows an application example of the polarizing element of Embodiment 1.
FIG. 3 is a configuration sectional view illustrating a polarization element configured by combining a polarization element and a polarization plate. Even if the polarizing element of the present invention is used alone, a light beam having a considerably uniform polarization plane can be obtained. However, as shown in FIG. By arranging the polarizing plates 201 in the same direction, it is possible to obtain emitted light with a very uniform polarization direction. When the polarizing element of the present invention is incorporated in an optical measuring instrument or the like, it is desirable to adopt the above configuration.
【0015】(実施例3) 第3図は実施例2の偏光素子を入射光束に垂直な面内に
複数構成した場合の概略構成を示したものである。この
場合、実施例2と同様に円形レンズを平面上に並べてレ
ンズアレイとしたものを用いてもよいが、集光効率の高
さ及び製造の容易さから、レンチキュラーレンズを平面
状に並べてレンズアレイとしたものが使いやすい。偏光
素子を2次元の平面状に多数個並べる事により、大面積
の各種表示体(例えば液晶表示体)あるいは各種照明装
置などに応用することが可能となる。(Embodiment 3) FIG. 3 shows a schematic configuration in a case where a plurality of polarizing elements of Embodiment 2 are arranged in a plane perpendicular to the incident light beam. In this case, a lens array in which circular lenses are arranged on a plane in the same manner as in the second embodiment may be used. However, from the viewpoint of high light-collecting efficiency and ease of manufacture, lenticular lenses are arranged in a plane to form a lens array. Easy to use. By arranging a large number of polarizing elements in a two-dimensional plane, it can be applied to various displays having a large area (for example, a liquid crystal display) or various lighting devices.
【0016】[0016]
【発明の効果】以上説明したように本発明の偏光素子お
よび照明装置によれば、入射した光のほとんど全てを偏
光面が揃った出射光に、高効率で変換することが可能で
ある。同様の目的で使用される従来の偏光板とは異な
り、本発明の偏光素子は本質的に光吸収が無いため、強
い光線を入射させた場合にも、発熱による自己破壊を招
く事なく安定的に機能する。As described above, according to the polarizing element and the illuminating device of the present invention, almost all of the incident light can be converted into outgoing light having a uniform polarization plane with high efficiency. Unlike the conventional polarizing plate used for the same purpose, the polarizing element of the present invention has essentially no light absorption, so that even when a strong light is incident, it is stable without causing self-destruction due to heat generation. To work.
【0017】本発明の偏光素子および照明装置は上記の
特性を生かして、偏光を必要とする各種表示体、特に液
晶表示体、光アイソレータ、光スイッチ、光学フィルタ
や、それらを構成要素とする各種光学測定機器等、広範
囲の応用が可能である。The polarizing element and the illuminating device of the present invention make use of the above-mentioned characteristics to make use of various displays requiring polarization, in particular, liquid crystal displays, optical isolators, optical switches, optical filters, and various components comprising them. A wide range of applications such as optical measurement equipment is possible.
図1は実施例1の偏光素子の構成断面図。図2は実施例
2の偏光素子の構成断面図。図3は実施例3の偏光素子
の構成概略図。FIG. 1 is a configuration sectional view of a polarizing element according to a first embodiment. FIG. 2 is a cross-sectional view illustrating a configuration of a polarizing element according to a second embodiment. FIG. 3 is a schematic configuration diagram of a polarizing element according to a third embodiment.
101・・・入射光束 102・・・複屈折層 103・・・常光線 104・・・異常光線 105・・・レンズ層 106・・・λ/2位相差層 107・・・透明開口部 108・・・出射光束 109・・・常光線の偏光方向(紙面に対して平行) 110・・・異常光線の偏光方向(紙面に対して垂直) 111・・・λ/2位相差層を透過した後の光束の偏光方
向(紙面に対して平行) 201・・・偏光板 202・・・偏光板の偏光方向(紙面に対して平行) 301・・・複屈折層部 302・・・レンズアレイ層部 303・・・λ/2位相差層部 304・・・偏光子層部101 ... incident light beam 102 ... birefringent layer 103 ... ordinary ray 104 ... extraordinary ray 105 ... lens layer 106 ... λ / 2 retardation layer 107 ... transparent aperture 108 ..Outgoing light flux 109 ・ ・ ・ Polarization direction of ordinary ray (parallel to paper) 110 ・ ・ ・ Polarization direction of extraordinary ray (perpendicular to paper) 111 ・ ・ ・ After passing through λ / 2 retardation layer Polarization direction of the light beam (parallel to the paper surface) 201: polarizing plate 202: polarization direction of the polarization plate (parallel to the paper surface) 301: birefringent layer 302: lens array layer 303 ・ ・ ・ λ / 2 retardation layer section 304 ・ ・ ・ Polarizer layer section
フロントページの続き (56)参考文献 特開 平1−265206(JP,A) 特開 昭60−63503(JP,A) 特開 昭61−90584(JP,A) 実開 昭58−36707(JP,U) 特許2718057(JP,B2) (58)調査した分野(Int.Cl.6,DB名) G02B 5/30 G02B 19/00 G02B 27/28 Continuation of the front page (56) References JP-A-1-265206 (JP, A) JP-A-60-63503 (JP, A) JP-A-61-90584 (JP, A) JP-A-58-36707 (JP) , U) Patent 2718057 (JP, B2) (58) Fields investigated (Int. Cl. 6 , DB name) G02B 5/30 G02B 19/00 G02B 27/28
Claims (2)
射する偏光素子であって、 前記入射光を、偏光面が互いに直交する2種類の偏光成
分の光に分離して、互いに異なる方向へ出射する偏光分
離手段と、 偏光面を旋回させる位相差層が、同一平面内の複数箇所
に選択的に形成された偏光変換手段と、 前記偏光変換手段の出射面側に配置された偏光板と、 前記偏光分離手段から出射された前記2種類の偏光成分
の光のうち、一方の光を前記位相差層の形成されている
部分に導き、他方の光を前記位相差層の形成されていな
い部分に導く集光手段とを有し、 前記集光手段は、各々、互いに異なる方向から入射した
前記2種類の偏光成分の光のうち、一方の光を前記位相
差層の形成されている部分に導き、他方の光を前記位相
差層の形成されていない部分に導く複数のレンズ体を備
え、 前記一方の光は前記位相差層を経て出射され、前記他方
の光は前記位相差層が形成されていない部分を経て出射
されることを特徴とする偏光素子。1. A polarizing element that converts incident light into light having a uniform polarization plane and emits the light, wherein the incident light is separated into two types of polarization components whose polarization planes are orthogonal to each other. Polarization separation means for emitting light in different directions, a phase difference layer for rotating the polarization plane, polarization conversion means selectively formed at a plurality of locations in the same plane, and disposed on the emission surface side of the polarization conversion means A polarizing plate, of the two types of polarized light components emitted from the polarized light separating means, guides one light to a portion where the phase difference layer is formed, and directs the other light to the portion where the phase difference layer is formed. Light collecting means for guiding light to a portion that is not formed, wherein the light collecting means is configured such that one of the two types of polarized light components incident from different directions is formed on the phase difference layer. To the part where the other light is formed on the retardation layer A plurality of lens bodies for guiding to the non-existing portion, wherein the one light is emitted through the phase difference layer, and the other light is emitted through a portion where the phase difference layer is not formed. Polarizing element.
射する照明装置であって、 前記入射光を、偏光面が互いに直交する2種類の偏光成
分の光に分離して、互いに異なる方向へ出射する偏光分
離手段と、 偏光面を旋回させる位相差層が、同一平面内の複数箇所
に選択的に形成された偏光変換手段と、 前記偏光変換手段の出射面側に配置された偏光板と、 前記偏光分離手段から出射された前記2種類の偏光成分
の光のうち、一方の光を前記位相差層の形成されている
部分に導き、他方の光を前記位相差層の形成されていな
い部分に導く集光手段とを有し、 前記集光手段は、各々、互いに異なる方向から入射した
前記2種類の偏光成分の光のうち、一方の光を前記位相
差層の形成されている部分に導き、他方の光を前記位相
差層の形成されていない部分に導く複数のレンズ体を備
え、 前記一方の光は前記位相差層を経て出射され、前記他方
の光は前記位相差層が形成されていない部分を経て照射
されることを特徴とする照明装置。2. An illumination device for converting incident light into light having a uniform polarization plane and irradiating the light, wherein the incident light is separated into two kinds of polarization components of light whose polarization planes are orthogonal to each other. Polarization separation means for emitting light in different directions, a phase difference layer for rotating the polarization plane, polarization conversion means selectively formed at a plurality of locations in the same plane, and disposed on the emission surface side of the polarization conversion means A polarizing plate, of the two types of polarized light components emitted from the polarized light separating means, guides one light to a portion where the phase difference layer is formed, and directs the other light to the portion where the phase difference layer is formed. Light collecting means for guiding light to a portion that is not formed, wherein the light collecting means is configured such that one of the two types of polarized light components incident from different directions is formed on the phase difference layer. To the part where the other light is formed on the retardation layer A plurality of lens bodies for guiding to the non-existing portion, wherein the one light is emitted through the phase difference layer, and the other light is irradiated through a portion where the phase difference layer is not formed. Lighting equipment.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8278377A JP2900896B2 (en) | 1996-10-21 | 1996-10-21 | Polarizing element and lighting device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8278377A JP2900896B2 (en) | 1996-10-21 | 1996-10-21 | Polarizing element and lighting device |
Related Parent Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63094118A Division JP2718057B2 (en) | 1988-04-15 | 1988-04-15 | Polarizing element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH09145926A JPH09145926A (en) | 1997-06-06 |
| JP2900896B2 true JP2900896B2 (en) | 1999-06-02 |
Family
ID=17596496
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8278377A Expired - Lifetime JP2900896B2 (en) | 1996-10-21 | 1996-10-21 | Polarizing element and lighting device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2900896B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5940149A (en) * | 1997-12-11 | 1999-08-17 | Minnesota Mining And Manufacturing Company | Planar polarizer for LCD projectors |
| US8422132B2 (en) | 2008-12-02 | 2013-04-16 | Shanghai Lexvu Opto Microelectronics Technology Co., Ltd. | Integrated planar polarizing device |
| JP2015095546A (en) * | 2013-11-12 | 2015-05-18 | 株式会社リコー | Image pickup device package and image pickup apparatus |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2718057B2 (en) | 1988-04-15 | 1998-02-25 | セイコーエプソン株式会社 | Polarizing element |
-
1996
- 1996-10-21 JP JP8278377A patent/JP2900896B2/en not_active Expired - Lifetime
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2718057B2 (en) | 1988-04-15 | 1998-02-25 | セイコーエプソン株式会社 | Polarizing element |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH09145926A (en) | 1997-06-06 |
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