JPH0915534A - Polarization separation / synthesis device and liquid crystal display device - Google Patents
Polarization separation / synthesis device and liquid crystal display deviceInfo
- Publication number
- JPH0915534A JPH0915534A JP16398895A JP16398895A JPH0915534A JP H0915534 A JPH0915534 A JP H0915534A JP 16398895 A JP16398895 A JP 16398895A JP 16398895 A JP16398895 A JP 16398895A JP H0915534 A JPH0915534 A JP H0915534A
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- Prior art keywords
- light
- liquid crystal
- polarization
- crystal panel
- shape
- Prior art date
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Abstract
(57)【要約】
【目的】 液晶パネル部での光の有効利用効率の向上を
図る。
【構成】 偏光方向が混在する白色光を光源1とし、光
源1から発せられた光を偏光ビームスプリッタ3により
偏光方向が異なる2本の直線偏光成分P1、Sに分離
し、分離された片方の偏光成分光Sを1/2波長板4を
透過させることにより、その偏光方向を90°回転させ
他方の偏光方向と一致させた後(P2)、合成プリズム
6へこの2本の光を導いて合成させて取り出すにあた
り、偏光ビームスプリッタ3へ入射する光を光形状整形
手段9により楕円形状に整形し、その楕円形状の短軸方
向が合成プリズム6からの出射時の光7の合成方向と一
致せしめることによって、液晶パネル部における光有効
利用効率を向上させる。
(57) [Abstract] [Purpose] To improve the effective use efficiency of light in the liquid crystal panel. [Structure] White light having mixed polarization directions is used as a light source 1, and light emitted from the light source 1 is separated by a polarization beam splitter 3 into two linearly polarized light components P1 and S having different polarization directions. The polarized component light S is transmitted through the half-wave plate 4 to rotate its polarization direction by 90 ° to match the other polarization direction (P2), and then guide these two lights to the combining prism 6. In combining and taking out, the light incident on the polarization beam splitter 3 is shaped into an elliptical shape by the optical shape shaping means 9, and the minor axis direction of the elliptical shape coincides with the combining direction of the light 7 at the time of emission from the combining prism 6. As a result, the effective light utilization efficiency in the liquid crystal panel section is improved.
Description
【0001】[0001]
【産業上の利用分野】本発明は、偏光方向が混在する光
の偏光方向を揃えて取り出す偏光分離合成装置およびそ
の偏光分離合成装置を備えた液晶表示装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a polarization splitting / synthesizing device for extracting light with mixed polarization directions by aligning the polarization directions, and a liquid crystal display device equipped with the polarization splitting / synthesizing device.
【0002】[0002]
【従来の技術】液晶プロジェクターなどの液晶を利用し
た光学システムは、従来のCRTに変わるものとして近
年注目を浴びている。その光としては、偏光方向が一定
方向に直線偏光した光が用いられることが多い。このよ
うなある一定方向に直線偏光した光を得るために、メタ
ルハライドランプなど偏光方向が混在する光源と偏光板
とを組み合わせる方法が一般に用いられている。この場
合、偏光板に入射した光のうち、偏光板を透過する光に
対して垂直な偏光面を持つ偏光成分光が除去されるた
め、偏光板を透過して利用できる光の光量割合は元来の
半分以下に減少してしまうことになり、光量損失が大き
い。2. Description of the Related Art Optical systems using liquid crystals such as liquid crystal projectors have recently attracted attention as alternatives to conventional CRTs. As the light, light that is linearly polarized in a certain polarization direction is often used. In order to obtain such light linearly polarized in a certain direction, a method of combining a light source such as a metal halide lamp having a mixed polarization direction with a polarizing plate is generally used. In this case, of the light incident on the polarizing plate, the polarized component light having a polarization plane perpendicular to the light passing through the polarizing plate is removed. It will be reduced to less than half of what it was, resulting in a large loss of light.
【0003】そこで、光量損失を抑えたうえで一定方向
に直線偏光した光を得る方法が提案されている(例えば
特願平6−237587号)。この提案方法は、光源か
らの光を偏光ビームスプリッタにてP偏光及びS偏光の
2つの直線偏光成分に分離し、このうち片方の光を波長
板を透過させることにより、その偏光面を90゜回転さ
せてもう一方の光の偏光方向と一致させ、その後もう一
方の光と再度合成する方法である。Therefore, there has been proposed a method of obtaining light linearly polarized in a certain direction while suppressing the loss of light quantity (for example, Japanese Patent Application No. 6-237587). In this proposed method, a light beam from a light source is split into two linearly polarized light components, P-polarized light and S-polarized light, by a polarization beam splitter, and one of the light components is transmitted through a wave plate to make its polarization plane 90 °. This is a method in which the light is rotated to match the polarization direction of the other light and then combined with the other light again.
【0004】図10は、特願平6−237587号に開
示された装置を示す。光源1から発せられた光は曲面鏡
2にて反射された平行光となり、偏光ビームスプリッタ
3により、P偏光とS偏光とに分離される。偏光ビーム
スプリッタ3にて反射されたS偏光は、偏光方向回転手
段としての1/2波長板4を透過することで偏光面が9
0゜回転し、P偏光へと変換された後(P2)、合成プ
リズム6へ入射される。一方、偏光ビームスプリッタ3
を透過したP偏光は、ミラー5にて反射された後(P
1)、合成プリズム6へ入射される。合成プリズム6へ
入射された2本の光P1、P2は、合成プリズム6の働
きによって1本の光へと合成され、出射光7として取り
出される。FIG. 10 shows an apparatus disclosed in Japanese Patent Application No. 6-237587. The light emitted from the light source 1 becomes parallel light reflected by the curved mirror 2, and is split into P-polarized light and S-polarized light by the polarization beam splitter 3. The S-polarized light reflected by the polarization beam splitter 3 has a polarization plane of 9 by passing through the ½ wavelength plate 4 as a polarization direction rotating means.
After being rotated by 0 ° and converted into P-polarized light (P2), it is incident on the combining prism 6. On the other hand, the polarization beam splitter 3
The P-polarized light that has passed through is reflected by the mirror 5 (P
1), the light is incident on the combining prism 6. The two lights P1 and P2 incident on the combining prism 6 are combined into one light by the function of the combining prism 6, and are extracted as outgoing light 7.
【0005】以上のように、この従来技術では、P偏光
とS偏光との2つの偏光成分光が混在する光源より発せ
られた光から、S偏光をP偏光に変換してP偏光のみの
直線偏光成分光として取り出すことができる。As described above, in this conventional technique, the light emitted from the light source in which the two polarized component lights of P-polarized light and S-polarized light coexist is converted from S-polarized light to P-polarized light to obtain a straight line of only P-polarized light. It can be extracted as polarized component light.
【0006】[0006]
【発明が解決しようとする課題】ところで、光源1から
発せられた光は曲面鏡2にて反射され偏光ビームスプリ
ッタ3に入射するが、その際の光の形状は一般的に図1
1(a)に示すように円形状である。一方、合成プリズ
ム6から出射される光の形状は上述のごとく偏光ビーム
スプリッタ3にて分離されたP偏光(P1)、S偏光か
ら変換されたP偏光(P2)とが合成された出射光7と
なるため、図11(b)に示すように2本の光が合わさ
った、短径と長径の比が略1対2の楕円形状となる。By the way, the light emitted from the light source 1 is reflected by the curved mirror 2 and enters the polarization beam splitter 3, and the shape of the light at that time is generally as shown in FIG.
It has a circular shape as shown in FIG. On the other hand, the shape of the light emitted from the synthesizing prism 6 is the emitted light 7 obtained by synthesizing the P-polarized light (P1) separated by the polarization beam splitter 3 and the P-polarized light (P2) converted from the S-polarized light as described above. Therefore, as shown in FIG. 11B, the two light beams are combined into an elliptical shape having a ratio of the short diameter to the long diameter of approximately 1: 2.
【0007】上述した液晶プロジェクターなどの液晶表
示装置では、液晶パネルや偏光板から成る液晶ライトバ
ルブからの出射光をスクリーン上に投射して映像を表示
する。このとき、光の有効利用効率の点から見ると、全
体の光のうち液晶パネル内へ入射可能な光の割合が大き
いほど光の有効利用効率が高いことになる。In a liquid crystal display device such as the above-mentioned liquid crystal projector, light emitted from a liquid crystal light valve including a liquid crystal panel and a polarizing plate is projected on a screen to display an image. At this time, in terms of the effective use efficiency of light, the larger the ratio of the light that can enter the liquid crystal panel to the total light, the higher the effective use efficiency of light.
【0008】図12に液晶パネル16の外形と液晶パネ
ル16へ照射される出射光7の形状を示す。この図は、
短径と長径の比が略1対2の楕円形状の光7が、一般に
多く用いられている横方向長さと縦方向長さの比が4対
3である液晶パネル16へ接するような大きさで照射し
ている場合である。光7を実際に液晶パネル16へ取り
込んで利用している割合は、光7が照射されている領域
に対する液晶パネル16の占める領域の割合であり、こ
こでは、約59%の光しか利用していないことになる。FIG. 12 shows the outer shape of the liquid crystal panel 16 and the shape of the emitted light 7 with which the liquid crystal panel 16 is irradiated. This figure is
The size is such that the elliptical light 7 having a ratio of the minor axis to the major axis of about 1 to 2 comes into contact with the liquid crystal panel 16 having a ratio of the length in the horizontal direction to the length in the longitudinal direction of 4 which is commonly used. This is the case when irradiation is performed at. The ratio of actually taking in and using the light 7 in the liquid crystal panel 16 is the ratio of the area occupied by the liquid crystal panel 16 to the area irradiated with the light 7, and here only about 59% of the light is used. There will be no.
【0009】また、液晶パネルを透過した光は投射レン
ズを経てスクリーン上に映像を映し出すが、スクリーン
上での映像の明るさは、明るければ明るいほど、その映
像が見やすくなる。例えば、スクリーン照度が高けれ
ば、室内を暗くしなくても充分明るく映像を見ることが
できる。スクリーン上での映像の明るさは、液晶パネル
内へどれだけ多くの光を取り込むことができるかに大き
く係わっており、液晶パネル部での光の利用効率の向上
が求められている。Further, the light transmitted through the liquid crystal panel projects an image on the screen through the projection lens. The brighter the image on the screen, the easier it is to see the image. For example, if the screen illuminance is high, a sufficiently bright image can be viewed without darkening the room. The brightness of the image on the screen is largely related to how much light can be taken into the liquid crystal panel, and improvement of the light utilization efficiency in the liquid crystal panel is required.
【0010】しかしながら、液晶パネル部での光の有効
利用効率を単なる液晶パネルへの光の入射光面積と液晶
パネルの占有面積との面積比として考えた場合、偏光ビ
ームスプリッタ3へ入射される光が円形状の場合、上述
のごとくその利用効率はたかだか約59%と光利用効率
の低さからスクリーン上での明るさが不足するという問
題点があった。However, when the effective utilization efficiency of light in the liquid crystal panel portion is considered simply as the area ratio of the incident light area of the light to the liquid crystal panel and the occupied area of the liquid crystal panel, the light incident on the polarization beam splitter 3 is considered. In the case of a circular shape, there is a problem that the brightness on the screen is insufficient due to the low light utilization efficiency of about 59% as described above.
【0011】本発明は、このような従来技術の課題を解
決すべくなされたものであって、液晶パネル部における
光有効利用効率を向上させ得る偏光分離合成装置および
液晶表示装置を提供することを目的とする。The present invention has been made to solve the problems of the prior art, and it is an object of the present invention to provide a polarization splitting / combining device and a liquid crystal display device capable of improving the effective light utilization efficiency in a liquid crystal panel section. To aim.
【0012】[0012]
【課題を解決するための手段】本発明の偏光分離合成装
置は、光源から発せられた白色光をP偏光成分とS偏光
成分に分離する偏光分離手段に入射させ、該偏光分離手
段にて分離された各偏光成分光の偏光方向を偏光方向回
転手段により一致させた後、光合成手段に入射させるこ
とにより合成して取り出す偏光分離合成装置において、
該光源から発せられた白色光を光形状整形手段によって
楕円形状に整形し、楕円形状の短軸方向を該偏光分離手
段からの出射時の光の合成方向と一致せしめるので、そ
のことにより上記目的が達成される。A polarization separation / combination device of the present invention allows white light emitted from a light source to enter a polarization separation means for separating a P polarization component and an S polarization component, and the polarization separation means separates the white light. In the polarization splitting / synthesizing device, in which the polarization directions of the respective polarized component lights thus obtained are matched by the polarization direction rotating means, and then the light is combined and extracted by being incident on the light combining means,
The white light emitted from the light source is shaped into an elliptical shape by the light shape shaping means, and the minor axis direction of the elliptical shape is made to coincide with the direction in which light is emitted from the polarization splitting means. Is achieved.
【0013】本発明の液晶表示装置は、液晶パネル形状
の横方向長さと縦方向長さの比がM対Nである液晶ライ
トバルブへ偏光分離合成装置からの出射光が入射される
液晶表示装置において、請求項1の偏光分離合成装置の
偏光分離手段へ入射する光が楕円形状であり、かつ、長
軸長さと短軸長さの比をN対M/2としているので、そ
のことにより上記目的が達成される。The liquid crystal display device of the present invention is a liquid crystal display device in which light emitted from a polarization splitting / combining device is incident on a liquid crystal light valve in which the ratio of the horizontal length to the vertical length of the liquid crystal panel is M: N. In claim 1, the light incident on the polarization splitting means of the polarization splitting / combining device according to claim 1 is elliptical, and the ratio of the major axis length to the minor axis length is N: M / 2. The purpose is achieved.
【0014】[0014]
【作用】本発明にあっては、偏光方向が混在する白色光
を光源とし、光源から発せられた光を偏光分離手段によ
り偏光方向が異なる2本の直線偏光成分に分離し、分離
された片方の偏光成分光を偏光板を透過させることによ
り、その偏光方向を90゜回転させ他方の偏光方向の光
と一致させる。その後、光合成手段へこの2本の光を導
いて合成させて取り出す。この過程において、偏光分離
手段へ入射する光を光形状整形手段が楕円形状に整形
し、その楕円形状の短軸方向が偏光分離手段からの出射
時の光の合成方向と一致せしめる。これによって、液晶
表示装置を構成する液晶パネル部における光有効利用効
率が向上する。According to the present invention, white light having mixed polarization directions is used as the light source, and the light emitted from the light source is separated into two linearly polarized light components having different polarization directions by the polarization separating means, and the separated one is separated. By passing the polarized component light of (1) through the polarizing plate, its polarization direction is rotated by 90 ° and matched with the light of the other polarization direction. After that, these two lights are guided to the photosynthesis means to be synthesized and taken out. In this process, the light shape shaping means shapes the light incident on the polarization splitting means into an elliptical shape, and the minor axis direction of the elliptical shape is made to coincide with the direction in which the light is emitted from the polarization splitting means. As a result, the efficiency of effective use of light in the liquid crystal panel portion of the liquid crystal display device is improved.
【0015】この場合において、液晶パネル形状の横方
向長さと縦方向長さの比がM対Nであると、偏光分離手
段へ入射する光を、長軸長さと短軸長さの比がN対M/
2の楕円形状とする。In this case, if the ratio of the length in the horizontal direction to the length in the vertical direction of the liquid crystal panel is M to N, the light incident on the polarized light separating means has a ratio of the major axis length to the minor axis length of N. Vs. M /
It has an elliptical shape of 2.
【0016】[0016]
【実施例】以下に、本発明の実施例を図面に基づき説明
する。Embodiments of the present invention will be described below with reference to the drawings.
【0017】(実施例1)図1に本実施例の偏光分離合
成装置を組み込んだ液晶プロジェクターの平面図を示
す。偏光分離合成装置は、メタルハライドランプ、ハロ
ゲンランプ、またはキセノンランプなど白色光を発する
光源1と、楕円鏡8と、シリンドリカルレンズ10及び
平凸レンズ11からなる光形状整形手段9と、偏光分離
手段としての偏光ビームスプリッタ3と、偏光方向回転
手段としての1/2波長板4と、ミラー5と、合成プリ
ズム6とからなる。この偏光分離合成装置にて得られた
出射光7は、液晶パネルや偏光板からなる液晶ライトバ
ルブ12、フィールドレンズ13および投影レンズ14
を経てスクリーン15上に照射される。(Embodiment 1) FIG. 1 is a plan view of a liquid crystal projector incorporating the polarization splitting / synthesizing device of this embodiment. The polarization splitting / combining device includes a light source 1 that emits white light such as a metal halide lamp, a halogen lamp, or a xenon lamp, an elliptical mirror 8, an optical shape shaping unit 9 including a cylindrical lens 10 and a plano-convex lens 11, and a polarization splitting unit. It comprises a polarization beam splitter 3, a half-wave plate 4 as a polarization direction rotating means, a mirror 5, and a combining prism 6. The emitted light 7 obtained by this polarization separation / combination device is a liquid crystal light valve 12 including a liquid crystal panel and a polarizing plate, a field lens 13 and a projection lens 14.
Then, the light is irradiated onto the screen 15 via the.
【0018】上記光源1から発せられた光は、楕円鏡8
にて反射することで光束形状が略円形の収束光とされた
後、光形状整形手段9を透過する際、光束形状が略楕円
形状の平行光へと変換される。The light emitted from the light source 1 is elliptic mirror 8
After being converted into convergent light having a substantially circular beam shape by being reflected by, the light beam shape is converted into parallel light having a substantially elliptical shape when passing through the light shape shaping unit 9.
【0019】光形状整形手段9は、光束のある一方向の
みを縮小させるシリンドリカルレンズ10と平凸レンズ
11にて構成されている。また、シリンドリカルレンズ
10は、合成プリズム6からの出射時の光の合成される
方向と同じ方向に光が整形されるように構成されてお
り、光形状整形手段9に入射した円形収束光は、シリン
ドリカルレンズ10にて一方向のみを縮小された楕円光
とされた後、平凸レンズ11にて平行光とされる。The optical shape shaping means 9 is composed of a cylindrical lens 10 and a plano-convex lens 11 for reducing only one direction of a light beam. Further, the cylindrical lens 10 is configured so that the light is shaped in the same direction as the direction in which the light is emitted from the synthesizing prism 6, and the circular convergent light incident on the light shape shaping means 9 is The cylindrical lens 10 converts the light into elliptical light in only one direction, and then the plano-convex lens 11 converts the light into parallel light.
【0020】光形状整形手段9から出射した光は、偏光
ビームスプリッタ3を通過する際、透過光としてのP偏
光(P1)と反射光としてのS偏光(S)とに偏光方向
によって分離される。分離されたS偏光(S)は、1/
2波長板4を通過することで偏光面が90゜回転しP偏
光(P2)へと変換され、合成プリズム6へ入射され
る。一方のP偏光(P1)はミラー5にて反射された
後、合成プリズム6へ入射される。合成プリズム6に入
射したこの2本の光は偏光方向が一致した出射光7とし
て取り出される。この出射光7は、液晶パネルや偏光板
から成る液晶ライトバルブ12へと導かれた後、フィー
ルドレンズ13、投射レンズ14を経て、スクリーン1
5上へ照射される。When the light emitted from the light shaping means 9 passes through the polarization beam splitter 3, it is divided into P-polarized light (P1) as transmitted light and S-polarized light (S) as reflected light according to the polarization direction. . The separated S-polarized light (S) is 1 /
By passing through the two-wave plate 4, the plane of polarization is rotated by 90 ° and converted into P-polarized light (P2), which is then incident on the combining prism 6. One P-polarized light (P1) is reflected by the mirror 5 and then is incident on the combining prism 6. The two lights that have entered the combining prism 6 are extracted as outgoing light 7 whose polarization directions match. The emitted light 7 is guided to a liquid crystal light valve 12 including a liquid crystal panel and a polarizing plate, and then passes through a field lens 13 and a projection lens 14 and then to the screen 1.
5 is illuminated.
【0021】図2(a)は、偏光ビームスプリッタ3へ
の入射光形状が短軸長さと長軸長さの比を1対2とする
楕円形状の場合を示している。ここで、上記光形状整形
手段9によって整形された楕円形状の短軸方向は、合成
プリズム6からの出射時の光の合成方向と一致する方向
である。よって、合成プリズム6からの出射光7は、図
2(b)に示すような略円形状となる。FIG. 2 (a) shows a case where the shape of the incident light on the polarization beam splitter 3 is an elliptical shape in which the ratio of the minor axis length to the major axis length is 1: 2. Here, the minor axis direction of the elliptical shape shaped by the light shape shaping means 9 is a direction that coincides with the direction in which light is emitted from the synthetic prism 6. Therefore, the light 7 emitted from the combining prism 6 has a substantially circular shape as shown in FIG.
【0022】図3に、合成プリズム6からの出射光7が
円形状の場合において、液晶パネル16の外形と液晶パ
ネル16へ照射される光7の形状を示す。この図3は、
円形状の光7が、一般に多く用いられている横方向長さ
と縦方向長さの比が4対3である液晶パネル16へ接す
るような大きさで照射している場合である。この液晶パ
ネル16における光有効利用効率を、光7が照射されて
いる領域に対する液晶パネル16の領域の割合でみる
と、約61%と、偏光ビームスプリッタ3への入射光を
光形状整形手段9によって整形しない場合と比較してわ
ずかであるが光有効利用効率は向上している。FIG. 3 shows the outer shape of the liquid crystal panel 16 and the shape of the light 7 irradiated on the liquid crystal panel 16 when the light 7 emitted from the synthesizing prism 6 is circular. This FIG.
This is a case where the circular light 7 is radiated in such a size that it comes into contact with the liquid crystal panel 16 having a ratio of the length in the horizontal direction to the length in the vertical direction which is generally 4/3. The effective light use efficiency of the liquid crystal panel 16 is about 61% when the ratio of the area of the liquid crystal panel 16 to the area irradiated with the light 7 is about 61%, and the incident light to the polarization beam splitter 3 is shaped by the optical shape shaping means 9. The effective light utilization efficiency is slightly improved compared to the case without shaping.
【0023】さらに、図4(a)は偏光ビームスプリッ
タ3への入射光形状を示し、短軸長さと長軸長さの比が
2対3の場合である。図4(b)は、液晶パネル16の
外形と液晶パネル16へ照射される光7の形状を示す。
すなわち、図4においては、液晶パネル形状の横方向長
さと縦方向長さの比がM対Nである液晶パネル16に対
して、偏光ビームスプリッタ3への入射光を長軸長さと
短軸長さの比がN対M/2である楕円形状とする場合で
ある。ここでは、M=4,N=3に相当する。光7が照
射されている領域に対する液晶パネル16の占める領域
の割合でみた光有効利用効率は約64%となり、偏光ビ
ームスプリッタ3への入射光楕円形状を最適化すること
によって光有効利用効率のさらなる向上を図ることがで
きる。Further, FIG. 4A shows the shape of the incident light on the polarization beam splitter 3, in which the ratio of the minor axis length to the major axis length is 2: 3. FIG. 4B shows the outer shape of the liquid crystal panel 16 and the shape of the light 7 with which the liquid crystal panel 16 is irradiated.
That is, in FIG. 4, with respect to the liquid crystal panel 16 in which the ratio of the horizontal length and the vertical length of the liquid crystal panel is M: N, the incident light to the polarization beam splitter 3 is changed to the long axis length and the short axis length. This is a case of an elliptical shape having a height ratio of N to M / 2. Here, it corresponds to M = 4 and N = 3. The effective light utilization efficiency in terms of the ratio of the area occupied by the liquid crystal panel 16 to the area irradiated with the light 7 is about 64%. By optimizing the elliptical shape of the incident light to the polarization beam splitter 3, the effective light utilization efficiency is improved. Further improvement can be achieved.
【0024】ところで、上記光有効利用効率をさらに向
上させるためには、液晶パネルの領域外の光を液晶パネ
ルの領域内へ移動させる方法が考えられる。例えば、図
4に示すような液晶パネル領域外Aの光を液晶パネル領
域Bへ移動して利用する場合である。このとき問題とな
るのは液晶パネル16への光7の入射角度である。液晶
パネル16を透過する光の角度には制限があり、液晶パ
ネル16の特性に応じた許容入射角度が設けられてい
る。入射角度の悪い光を用いると、スクリーン15上で
色の滲みや、混色といった問題が発生する。このため、
液晶パネル16の光入射面には光入射角度制限手段(図
示せず)が設けられており、許容入射角度を超える光が
液晶パネル16へ入射しないよう入射光を制限してい
る。許容入射角度を超える光、すなわち、平行度の悪い
光を多く含んだ入射光を用いた場合、この光入射角度制
限手段によって蹴られる光の量が増加することで光有効
利用効率は向上しない。液晶パネル領域外Aの光を液晶
パネル領域Bへ移動させるということは、合成プリズム
6からの出射光7が元々平行光として液晶パネル16へ
入射していたのに対して、移動された光の部分は、その
移動量に応じた角度をもって液晶パネル16へ入射する
ことになる。上記移動量が大きい光ほど液晶パネル16
への入射角が大きくなり、液晶パネル16の特性に応じ
た許容入射角度を超えて液晶パネル16内へ取り込めな
い可能性が出てくる。従って、液晶パネル16内へ光を
確実に取り込むために上記移動量を少なくすることが求
められる。一般に多く用いられている横方向長さと縦方
向長さの比が4対3である液晶パネル16の場合、図1
2、及び図4に示すように、液晶パネル領域外Aの光を
液晶パネル領域Bへ移動させるための移動量は、それぞ
れMとLとになる。このとき、Lの長さがMの長さの約
0.5倍であることから、偏光ビームスプリッタ3への
入射光を長軸長さと短軸長さの比が2対3である楕円形
状とした場合の方が、偏光ビームスプリッタ3への入射
光を円形状とする場合と比較して、移動した光の液晶パ
ネルに対する入射角度が小さくてすみ液晶パネル内へ取
り込まれる可能性が大きいことになる。By the way, in order to further improve the light effective use efficiency, a method of moving light outside the region of the liquid crystal panel into the region of the liquid crystal panel can be considered. For example, there is a case where light outside the liquid crystal panel area A as shown in FIG. 4 is moved to the liquid crystal panel area B and used. At this time, the problem is the incident angle of the light 7 on the liquid crystal panel 16. There is a limit to the angle of light that passes through the liquid crystal panel 16, and an allowable incident angle according to the characteristics of the liquid crystal panel 16 is provided. If light with a poor incident angle is used, problems such as color bleeding and color mixing occur on the screen 15. For this reason,
A light incident angle limiting means (not shown) is provided on the light incident surface of the liquid crystal panel 16, and limits the incident light so that light exceeding the allowable incident angle does not enter the liquid crystal panel 16. When the light exceeding the allowable incident angle, that is, the incident light containing a large amount of light with poor parallelism is used, the amount of light kicked by the light incident angle limiting means is increased and the light effective utilization efficiency is not improved. Moving the light outside the liquid crystal panel area A to the liquid crystal panel area B means that the outgoing light 7 from the combining prism 6 originally entered the liquid crystal panel 16 as parallel light, whereas The part is incident on the liquid crystal panel 16 at an angle according to the amount of movement. The larger the amount of movement, the more the liquid crystal panel 16
The incident angle to the liquid crystal panel 16 becomes large, and there is a possibility that it cannot be taken into the liquid crystal panel 16 beyond the allowable incident angle according to the characteristics of the liquid crystal panel 16. Therefore, it is required to reduce the movement amount in order to reliably take in light into the liquid crystal panel 16. In the case of the liquid crystal panel 16 which has a ratio of the length in the horizontal direction to the length in the vertical direction of 4: 3, which is commonly used, FIG.
2 and 4, the movement amounts for moving the light outside the liquid crystal panel area A to the liquid crystal panel area B are M and L, respectively. At this time, since the length of L is about 0.5 times the length of M, the incident light on the polarization beam splitter 3 has an elliptical shape in which the ratio of the major axis length to the minor axis length is 2: 3. Compared with the case where the incident light to the polarization beam splitter 3 has a circular shape, the incident angle of the moved light with respect to the liquid crystal panel is smaller and the possibility of being taken into the liquid crystal panel is higher. become.
【0025】(実施例2)図5は、本発明の他の実施例
にかかる偏光分離合成装置の一部を示す図である。この
実施例2では、実施例1の楕円鏡8に代えてパラボラ曲
面鏡17を用い、また、実施例1の平凸レンズ11に代
えて凹柱レンズ18を用いている。白色光を発する光源
1から発せられた光は、パラボラ曲面鏡17にて反射す
ることで光束形状が略円形の略平行光とされる。その
後、光束のある一方向のみを縮小させるシリンドリカル
レンズ10にて、一方向のみが収束光となることで略楕
円形状に変換される。シリンドリカルレンズ10の方向
は、この楕円形状の短軸方向が合成プリズム6からの出
射時の光の合成方向と一致する方向に構成されている。
凹柱レンズ18にて収束する光の方向を再度平行光に戻
して楕円形状の平行光とした後、偏光ビームスプリッタ
3へ入射させる。(Embodiment 2) FIG. 5 is a diagram showing a part of a polarization splitting / combining apparatus according to another embodiment of the present invention. In the second embodiment, a parabolic curved mirror 17 is used instead of the elliptical mirror 8 of the first embodiment, and a concave column lens 18 is used instead of the plano-convex lens 11 of the first embodiment. The light emitted from the light source 1 that emits white light is reflected by the parabolic curved mirror 17 to be substantially parallel light having a substantially circular light flux shape. Then, in the cylindrical lens 10 that reduces only one direction of the light flux, the light is converged in only one direction, so that the light is converted into a substantially elliptical shape. The direction of the cylindrical lens 10 is configured such that the minor axis direction of this elliptical shape coincides with the direction in which light is emitted from the combining prism 6.
The direction of light converged by the concave lens 18 is returned to parallel light again to be elliptical parallel light, which is then incident on the polarization beam splitter 3.
【0026】(実施例3)図6は、本発明の更に他の偏
光分離合成装置の一部を示す図である。この実施例3で
は、実施例1の場合とは、光形状整形手段9を構成する
部材を代えている。つまり、平凹レンズ19と整形プリ
ズム20とを用いている。白色光を発する光源1から発
せられた光は、楕円鏡8にて反射することで光束形状が
略円形の収束光とされた後、平凹レンズ19にて所定の
大きさの平行光とされる。その後、光束のある一方向の
みを縮小させる整形プリズム20にて、光束形状が楕円
形状へ整形された後、偏光ビームスプリッタ3へ入射さ
れる。整形プリズム20による整形方向は、整形後の楕
円形状の短軸方向が合成プリズム6からの出射時の光の
合成方向と一致する方向に構成されている。(Third Embodiment) FIG. 6 is a diagram showing a part of still another polarization separation / combination device of the present invention. In the third embodiment, the members forming the optical shape shaping means 9 are replaced with those in the first embodiment. That is, the plano-concave lens 19 and the shaping prism 20 are used. The light emitted from the light source 1 that emits white light is reflected by the elliptical mirror 8 to be converged light having a substantially circular luminous flux shape, and then is converted into parallel light of a predetermined size by the plano-concave lens 19. . Then, the light beam is shaped into an elliptical shape by the shaping prism 20 that reduces only one direction of the light beam, and then enters the polarization beam splitter 3. The shaping direction by the shaping prism 20 is such that the minor axis direction of the shaped elliptical shape coincides with the synthesis direction of the light emitted from the synthesis prism 6.
【0027】(実施例4)図7(a)は、プリズム型偏
光ビームスプリッタ21を用いた偏光分離合成装置を組
み込んだ液晶プロジェクターの平面図を示す。図7
(b)は、そのプリズム型偏光ビームスプリッタ21を
拡大して示す平面図である。プリズム型偏光ビームスプ
リッタ21は以下のように構成されている。光源1から
発せられ、光形状整形手段9を透過した平行光束は、4
つの入射光B25,B26,B27,B28に分かれて
ミラー25,26,偏光ビームスプリッタ27,28に
入射する。この中で偏光ビームスプリッタ27,28に
入射した光B27,B28は透過するP偏光光Bp2
7,Bp28と反射するS偏光光Bs27,Bs28と
に分離される。透過したP偏光光Bp27,Bp28は
λ/2板33によってS偏光光Bs27’,Bs28’
に変換され紙面右方向に出射する。反射したS偏光光B
s27,Bs28はミラー29,30により紙面右方向
に向きを変える。次にミラー25,26に入射した光B
25,B26は偏光ビームスプリッタ31,32へ入射
し、透過するP偏光光Bp25,Bp26と反射するS
偏光光Bs25,Bs26とに分離される。反射したS
偏光光Bs25,Bs26はそのまま紙面右方向に出射
し、透過したP偏光光Bp25,Bp26はミラー2
3,23’により紙面右方向に向きを変えられλ/2板
24,24’によってS偏光光BS25’,Bs26’
に変換され出射する構成となっている。(Embodiment 4) FIG. 7A is a plan view of a liquid crystal projector incorporating a polarization splitting / combining device using a prism type polarization beam splitter 21. FIG.
(B) is an enlarged plan view showing the prism type polarization beam splitter 21. The prism type polarization beam splitter 21 is configured as follows. The parallel light flux emitted from the light source 1 and transmitted through the light shape shaping means 9 is 4
The two incident lights B25, B26, B27, B28 are split and incident on the mirrors 25, 26 and the polarization beam splitters 27, 28. Among them, the lights B27 and B28 incident on the polarization beam splitters 27 and 28 are P-polarized lights Bp2 which are transmitted.
7, Bp28 and the reflected S polarized light Bs27, Bs28 are separated. The transmitted P-polarized light Bp27, Bp28 is converted into S-polarized light Bs27 ', Bs28' by the λ / 2 plate 33.
And is emitted to the right on the paper surface. Reflected S-polarized light B
The mirrors 29 and 30 change the directions of s27 and Bs28 to the right on the paper surface. Next, the light B incident on the mirrors 25 and 26
25 and B26 are incident on the polarization beam splitters 31 and 32, and S which is reflected by the P-polarized light Bp25 and Bp26 that is transmitted therethrough is reflected.
It is separated into polarized lights Bs25 and Bs26. S reflected
The polarized lights Bs25 and Bs26 are emitted as they are toward the right side of the drawing, and the transmitted P-polarized lights Bp25 and Bp26 are reflected by the mirror 2
3, 23 'can be turned to the right in the plane of the drawing, and the λ / 2 plates 24, 24' can be used for S-polarized light BS25 ', Bs26'.
It is configured to be converted into and output.
【0028】図8(a)は、プリズム型偏光ビームスプ
リッタ21への入射光束形状を示し、円形状の場合であ
る。図8(b)はプリズム型偏光ビームスプリッタ21
の出射光束形状を示す。出射光束形状は、破線Tで示す
長軸長さと短軸長さの比が2対1の略楕円形状と見なす
ことができる。FIG. 8A shows the shape of a light beam incident on the prism type polarization beam splitter 21, which is a circular shape. FIG. 8B shows a prism type polarization beam splitter 21.
3 shows the shape of the outgoing light flux of. The shape of the emitted light beam can be regarded as a substantially elliptical shape in which the ratio of the major axis length to the minor axis length indicated by the broken line T is 2: 1.
【0029】図9(a)は、プリズム型偏光ビームスプ
リッタ21への入射光束形状を示し、略1対2の楕円形
状の場合である。図9(b)はプリズム型偏光ビームス
プリッタ21の出射光束形状を示している。ここで、光
形状整形手段9によって整形された楕円形状の短軸方向
は、プリズム型偏光ビームスプリッタ21からの出射時
の光の合成方向と一致する方向であって、この時、この
出射光7は、破線Qにて示すように略円形状となる。FIG. 9A shows the shape of an incident light beam to the prism type polarization beam splitter 21, which is an elliptical shape of approximately 1: 2. FIG. 9B shows the shape of the light flux emitted from the prism type polarization beam splitter 21. Here, the minor axis direction of the elliptical shape shaped by the light shape shaping means 9 is a direction that coincides with the combined direction of the light when it is emitted from the prism type polarization beam splitter 21, and at this time, the emitted light 7 Has a substantially circular shape as indicated by a broken line Q.
【0030】このように、偏光分離合成手段を変更した
場合においても、その入射光束形状と出射光束形状との
関係はほぼ同一と見なすことができるため、入射光束形
状を液晶パネル形状に適応した楕円形状とすることによ
る光有効利用効率向上の効果に関しても同様である。上
記プリズム型偏光ビームスプリッタ21の代わりに、図
13に示すプリズム型偏光ビームスプリッタ40や図1
4に示すプレート型偏光ビームスプリッタ50を用いる
ことができる。As described above, even when the polarization splitting / combining means is changed, the relationship between the incident light flux shape and the outgoing light flux shape can be regarded as almost the same, and therefore, the incident light flux shape is an ellipse adapted to the liquid crystal panel shape. The same applies to the effect of improving the effective use efficiency of light due to the shape. Instead of the prism type polarization beam splitter 21, the prism type polarization beam splitter 40 shown in FIG.
The plate type polarization beam splitter 50 shown in FIG. 4 can be used.
【0031】図13に示したプリズム型偏光ビームスプ
リッタ40は、2種類の複合プリズム45,46を採用
し、図7(b)で示すミラー23,23’,25,2
6,29,30のかわりにプリズム面47,47’,4
8,48’,49,49’の全反射面を使う(このとき
面47,48,47’,48’を全反射面にするためこ
の間に薄い空気層ができるように若干離して配置するこ
とが望ましい)ことでこれらの面での反射率をほぼ10
0%にした構成である。なお、43,44,44’はλ
/2板である。The prism type polarization beam splitter 40 shown in FIG. 13 employs two types of compound prisms 45 and 46, and mirrors 23, 23 ', 25 and 2 shown in FIG. 7B.
Instead of 6, 29, 30 prism surfaces 47, 47 ', 4
Use 8, 48 ', 49, 49' total reflection surfaces (at this time, since the surfaces 47, 48, 47 ', 48' are to be total reflection surfaces, they should be placed slightly apart so that a thin air layer can be formed between them. It is desirable that the reflectance on these surfaces be approximately 10
It is a structure with 0%. In addition, 43,44,44 'is λ
/ 2 plate.
【0032】図14に示したプレート型偏光ビームスプ
リッタ50は、偏光ビームスプリッタ52と、ミラー5
3と、λ/2板54とを組み合わせて、図7(b)又は
図13と同様の光の偏光変換を行い得る構成とされてい
る。The plate type polarization beam splitter 50 shown in FIG. 14 includes a polarization beam splitter 52 and a mirror 5.
3 and a λ / 2 plate 54 are combined to perform polarization conversion of light similar to that of FIG. 7B or 13.
【0033】なお、上記各実施例においては、光形状整
形手段として楕円鏡、シリンドリカルレンズ、平凸レン
ズの組み合わせ、またはパラボラ曲面鏡、シリンドリカ
ルレンズ、凹柱レンズの組み合わせ、または楕円鏡、平
凹レンズ、整形プリズムの組み合わせの場合を示した
が、本発明はこれに限らず、光形状を円形状から楕円形
状へ変換する手段であればどのような手段であってもか
まわない。また、偏光方向回転手段として1/2波長板
を用いたが、90°ツイストのTN型液晶素子などを用
いることも可能である。さらに、出射光はP偏光に一致
させてもS偏光に一致させても得られる効果は同様であ
る。In each of the above embodiments, as the optical shape shaping means, a combination of an elliptical mirror, a cylindrical lens and a plano-convex lens, or a combination of a parabolic curved mirror, a cylindrical lens and a concave column lens, or an elliptical mirror, a plano-concave lens and a shaping lens. Although the case of the combination of prisms is shown, the present invention is not limited to this, and any means may be used as long as it is a means for converting a light shape from a circular shape to an elliptical shape. Further, although the half-wave plate is used as the polarization direction rotating means, it is also possible to use a 90 ° twist TN type liquid crystal element or the like. Further, the same effect can be obtained whether the emitted light is matched with P-polarized light or S-polarized light.
【0034】[0034]
【発明の効果】本発明の偏光分離合成装置では、偏光方
向が混在する白色光を光源とし、光源から発せられた光
を光形状整形手段によって楕円形状に整形する際、その
楕円形状の短軸方向を偏光分離合成手段からの出射時の
光の合成方向と一致させる。さらに、液晶パネル形状の
横方向長さと縦方向長さの比がM対Nである時、楕円形
状の長軸長さと短軸長さの比をN対M/2とする。そし
て、整形後の光の偏光方向をP偏光成分とS偏光成分の
2本の直線偏光成分に分離する偏光分離手段に入射さ
せ、偏光方向回転手段により、分離された各偏光成分光
の偏光方向を一致させた出射光として取り出す構成とし
ている。その結果、その出射光を液晶ライトバルブへ照
射させる際、液晶パネル形状及び、液晶パネルへの光の
入射角を考慮した光束形状へ入射光を整形しているた
め、液晶パネル部における光有効利用効率を向上させる
ことができる。In the polarization splitting / synthesizing device of the present invention, when white light having mixed polarization directions is used as a light source and the light emitted from the light source is shaped into an elliptical shape by the optical shape shaping means, the minor axis of the elliptical shape is used. The direction is made to coincide with the direction in which light is emitted from the polarized light separating / combining means. Furthermore, when the ratio of the horizontal length to the vertical length of the liquid crystal panel is M to N, the ratio of the major axis length to the minor axis length of the elliptical shape is N to M / 2. Then, the polarization direction of the shaped light is made incident on the polarization separation means for separating the two linear polarization components of the P polarization component and the S polarization component, and the polarization direction rotation means divides the polarization direction of each polarization component light. Are output as matched emission light. As a result, when the emitted light is applied to the liquid crystal light valve, the incident light is shaped into a light flux shape that takes into account the shape of the liquid crystal panel and the angle of incidence of the light on the liquid crystal panel. The efficiency can be improved.
【図1】本実施例の偏光分離合成装置を組み込んだ液晶
プロジェクターの平面図。FIG. 1 is a plan view of a liquid crystal projector incorporating a polarization splitting / synthesizing device according to an embodiment.
【図2】(a)は偏光ビームスプリッタへの入射光形状
を示し、(b)は合成プリズムからの出射光形状を示す
図。FIG. 2A is a diagram showing a shape of light incident on a polarization beam splitter, and FIG. 2B is a diagram showing a shape of light emitted from a combining prism.
【図3】液晶パネル外形と液晶パネルへ照射される光の
形状とを示す図。FIG. 3 is a diagram showing an outer shape of a liquid crystal panel and a shape of light applied to the liquid crystal panel.
【図4】(a)は偏光ビームスプリッタへの入射光形状
を示し、(b)は液晶パネル外形と液晶パネルへ照射さ
れる光の形状とを示す図。FIG. 4A is a diagram showing an incident light shape on a polarization beam splitter, and FIG. 4B is a diagram showing an outer shape of a liquid crystal panel and a shape of light irradiated on the liquid crystal panel.
【図5】本発明の他の実施例にかかる偏光分離合成装置
の一部を示す図。FIG. 5 is a diagram showing a part of a polarization splitting / synthesizing device according to another embodiment of the present invention.
【図6】本発明の更に他の実施例にかかる偏光分離合成
装置の一部を示す図。FIG. 6 is a diagram showing a part of a polarization splitting / synthesizing device according to still another embodiment of the present invention.
【図7】(a)はプリズム型偏光ビームスプリッタを用
いた偏光分離合成装置を組み込んだ液晶プロジェクター
の平面図、(b)はそのプリズム型偏光ビームスプリッ
タを示す拡大図。7A is a plan view of a liquid crystal projector incorporating a polarization splitting / combining device using a prismatic polarization beam splitter, and FIG. 7B is an enlarged view showing the prismatic polarization beam splitter.
【図8】(a)はプリズム型偏光ビームスプリッタへの
入射光形状を示し、(b)はプリズム型偏光ビームスプ
リッタの出射光形状を示す図。FIG. 8A is a diagram showing an incident light shape of a prism type polarization beam splitter, and FIG. 8B is a diagram showing an emission light shape of the prism type polarization beam splitter.
【図9】(a)はプリズム型偏光ビームスプリッタへの
入射光形状を示し、(b)はプリズム型偏光ビームスプ
リッタの出射光形状を示す図。9A is a diagram showing the shape of incident light on a prism type polarization beam splitter, and FIG. 9B is a diagram showing the shape of light emitted from a prism type polarization beam splitter.
【図10】従来の偏光分離合成装置の平面図。FIG. 10 is a plan view of a conventional polarization splitting / synthesizing device.
【図11】(a)は偏光ビームスプリッタへの入射光形
状を示し、(b)は合成プリズムからの出射光形状を示
す図。FIG. 11A is a diagram showing the shape of light incident on the polarization beam splitter, and FIG. 11B is a diagram showing the shape of light emitted from the combining prism.
【図12】従来の液晶パネル外形と液晶パネルへ照射さ
れる光の形状とを示す図。FIG. 12 is a diagram showing an outer shape of a conventional liquid crystal panel and a shape of light applied to the liquid crystal panel.
【図13】本発明の偏光分離合成装置に用いられる他の
構成のプリズム型偏光ビームスプリッタを示す図。FIG. 13 is a view showing a prism type polarization beam splitter having another configuration used in the polarization splitting / combining device of the present invention.
【図14】本発明の偏光分離合成装置に用いられるプレ
ート型偏光ビームスプリッタを示す図。FIG. 14 is a diagram showing a plate-type polarization beam splitter used in the polarization splitting / combining device of the present invention.
1 光源 2 曲面鏡 3 偏光ビームスプリッタ 4 1/2波長板 5 ミラー 6 合成プリズム 7 偏光分離合成装置からの出射光 8 楕円鏡 9 光形状整形手段 10 シリンドリカルレンズ 11 平凸レンズ 12 液晶ライトバルブ 13 フィールドレンズ 14 投射レンズ 15 スクリーン 16 液晶パネル 17 パラボラ曲面鏡 18 凹柱レンズ 19 平凸レンズ 20 整形プリズム 21 プリズム型偏光ビームスプリッタ 1 Light Source 2 Curved Mirror 3 Polarizing Beam Splitter 4 1/2 Wave Plate 5 Mirror 6 Synthetic Prism 7 Emitted Light from Polarization Separation / Synthesis Device 8 Elliptical Mirror 9 Optical Shape Shaping Device 10 Cylindrical Lens 11 Plano-Convex Lens 12 Liquid Crystal Light Valve 13 Field Lens 14 Projection Lens 15 Screen 16 Liquid Crystal Panel 17 Parabolic Curved Mirror 18 Concave Column Lens 19 Plano-Convex Lens 20 Shaping Prism 21 Prism Type Polarizing Beam Splitter
Claims (2)
とS偏光成分に分離する偏光分離手段に入射させ、該偏
光分離手段にて分離された各偏光成分光の偏光方向を偏
光方向回転手段により一致させた後、光合成手段に入射
させることにより合成して取り出す偏光分離合成装置に
おいて、 該光源から発せられた白色光を光形状整形手段によって
楕円形状に整形し、楕円形状の短軸方向を該偏光分離手
段からの出射時の光の合成方向と一致せしめる偏光分離
合成装置。1. The white light emitted from a light source is made incident on a polarization separation means for separating a P polarization component and an S polarization component, and the polarization direction of each polarization component light separated by the polarization separation means is rotated. In the polarization splitting / combining device that is combined by the means and then is incident on the light combining means to extract the white light emitted from the light source, the white light emitted from the light source is shaped into an elliptical shape by the optical axis shaping means. A polarization splitting / combining device that matches the direction of light emitted from the polarization splitting means.
さの比がM対Nである液晶ライトバルブへ偏光分離合成
装置からの出射光が入射される液晶表示装置において、
請求項1の偏光分離合成装置の偏光分離手段へ入射する
光が楕円形状であり、かつ、長軸長さと短軸長さの比を
N対M/2としている液晶表示装置。2. A liquid crystal display device in which light emitted from a polarization splitting / combining device is incident on a liquid crystal light valve in which the ratio of the horizontal length to the vertical length of a liquid crystal panel is M: N.
A liquid crystal display device in which the light incident on the polarization separation means of the polarization separation / combination device according to claim 1 is elliptical, and the ratio of the major axis length to the minor axis length is N: M / 2.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16398895A JPH0915534A (en) | 1995-06-29 | 1995-06-29 | Polarization separation / synthesis device and liquid crystal display device |
| US08/536,779 US5729306A (en) | 1994-09-30 | 1995-09-29 | Light splitting and synthesizing device and liquid crystal display apparatus including the same |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16398895A JPH0915534A (en) | 1995-06-29 | 1995-06-29 | Polarization separation / synthesis device and liquid crystal display device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0915534A true JPH0915534A (en) | 1997-01-17 |
Family
ID=15784633
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP16398895A Pending JPH0915534A (en) | 1994-09-30 | 1995-06-29 | Polarization separation / synthesis device and liquid crystal display device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0915534A (en) |
Cited By (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 |
| JP2002514778A (en) * | 1998-05-14 | 2002-05-21 | モックステク | Polarizer device for producing a generally polarized light beam |
| US8422132B2 (en) | 2008-12-02 | 2013-04-16 | Shanghai Lexvu Opto Microelectronics Technology Co., Ltd. | Integrated planar polarizing device |
-
1995
- 1995-06-29 JP JP16398895A patent/JPH0915534A/en active Pending
Cited By (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 |
| JP2002514778A (en) * | 1998-05-14 | 2002-05-21 | モックステク | Polarizer device for producing a generally polarized light beam |
| US8422132B2 (en) | 2008-12-02 | 2013-04-16 | Shanghai Lexvu Opto Microelectronics Technology Co., Ltd. | Integrated planar polarizing device |
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