JP2003098598A - Illumination system for projector - Google Patents

Illumination system for projector

Info

Publication number
JP2003098598A
JP2003098598A JP2001290441A JP2001290441A JP2003098598A JP 2003098598 A JP2003098598 A JP 2003098598A JP 2001290441 A JP2001290441 A JP 2001290441A JP 2001290441 A JP2001290441 A JP 2001290441A JP 2003098598 A JP2003098598 A JP 2003098598A
Authority
JP
Japan
Prior art keywords
light
lens array
conversion element
incident
polarization conversion
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.)
Granted
Application number
JP2001290441A
Other languages
Japanese (ja)
Other versions
JP3678353B2 (en
Inventor
Hideki Oshima
秀樹 大島
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.)
Sharp Corp
Original Assignee
Sharp 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 Sharp Corp filed Critical Sharp Corp
Priority to JP2001290441A priority Critical patent/JP3678353B2/en
Publication of JP2003098598A publication Critical patent/JP2003098598A/en
Application granted granted Critical
Publication of JP3678353B2 publication Critical patent/JP3678353B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To provide an illumination system for a projector system which can enhance the availability of light and screen quality. SOLUTION: The illumination system comprises, a light source for emitting white light, a 1st lens array constituted of several lenses for splitting/condensing the light emitted from the light source, a 2nd lens array arranged near the focal point of the 1st lens array and constituted of lenses corresponding to each lens of the 1st lens array, and a polarized light conversion element for converting the light emitted from the white light source in a single polarization direction, and the incident and exit surfaces of each polarized light conversion element corresponding to each lens of the 2nd lens array are provided with specified curvature, and then, almost the whole light made incident on the polarized light conversion element at an incident angle different according to an incident wavelength is made nearly parallel to a main optical axis.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は、投写光学系のプロ
ジェクタにおける光学系に関するものであり、特に、液
晶プロジェクタに好適に利用されうる偏光変換素子の設
計に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical system in a projection optical system projector, and more particularly to a design of a polarization conversion element that can be suitably used in a liquid crystal projector.

【0002】[0002]

【従来の技術】従来、液晶表示素子に表示された画像を
拡大投影する液晶プロジェクタには、白色光源からの光
をレンズアレイにより液晶画像表示素子を均一に照明す
る照明光学系が用いられる。この照明光学系には特開平
8−304739号公報等にて提案されるように、液晶
表示素子の偏光特性に合わせて照明光の偏光方向を揃え
る偏光変換素子が用いられる。
2. Description of the Related Art Conventionally, in a liquid crystal projector for enlarging and projecting an image displayed on a liquid crystal display element, an illumination optical system for uniformly illuminating light from a white light source on a liquid crystal image display element by a lens array is used. A polarization conversion element that aligns the polarization direction of the illumination light according to the polarization characteristics of the liquid crystal display element is used for this illumination optical system, as proposed in Japanese Patent Laid-Open No. 8-304739.

【0003】特開平8−304739号公報では、イン
テグレータ光学系と偏光変換光学系を組み合わせた光利
用効率の高い偏光照明装置を小型でコンパクトに構成す
るため、偏光照明装置は、偏光方向がランダムな光を出
射する光源部と、矩形状の外形を有する複数の矩形集光
レンズから構成され、前記光源からの出射光を集光し
て、複数の2次光源像を形成するための第1のレンズ板
と、前記複数の2次光源像が形成される位置の近傍に置
かれ、集光レンズアレイ、偏光分離プリズムアレイ、λ
/2位相差板、および出射側レンズを備えた第2のレン
ズ板とを有している。インテグレータ光学系を構成する
第1のレンズ板によって、微小な2次光源像を生成した
段階で、偏光光の分離が行なわれる。よって、偏光光の
分離に伴う光路の空間的な広がりを抑制できるので、偏
光変換光学系を備えているにもかかわらず、偏光照明装
置の小型化を達成できるものである。
In Japanese Unexamined Patent Publication No. 8-304739, a polarized illumination device having a high light utilization efficiency that is a combination of an integrator optical system and a polarization conversion optical system is constructed in a small size and compactly. Therefore, the polarized illumination device has random polarization directions. A first light source unit that emits light and a plurality of rectangular condenser lenses having a rectangular outer shape, collects light emitted from the light source, and forms a plurality of secondary light source images. The lens plate and the position where the plurality of secondary light source images are formed are placed in the vicinity of the lens plate, a condenser lens array, a polarization separation prism array, and λ.
It has a / 2 phase difference plate and a second lens plate having an exit side lens. The polarized light is separated at the stage when a minute secondary light source image is generated by the first lens plate that constitutes the integrator optical system. Therefore, it is possible to suppress the spatial expansion of the optical path due to the separation of the polarized light, so that it is possible to achieve the downsizing of the polarized illumination device, despite the provision of the polarization conversion optical system.

【0004】図5に、従来例として上記の照明光学系を
示す。2つのレンズアレイ401、402と偏光変換素
子403とを組み合わせる場合、偏光の分離は第2レン
ズアレイ402の近傍にできる第1のレンズアレイ40
1の集光位置でP偏光成分とS偏光成分に分離される。
FIG. 5 shows the above-mentioned illumination optical system as a conventional example. When the two lens arrays 401 and 402 and the polarization conversion element 403 are combined, the polarized light can be separated in the vicinity of the second lens array 402.
It is separated into a P-polarized light component and an S-polarized light component at the light collecting position of 1.

【0005】また、特開平10−333097号公報に
おいては、偏光方向の揃った光束を発する光源装置と、
この光源装置からの光束を入射させる位置に配置された
画像表示素子としての透過型の液晶パネル、そして液晶
パネルを透過した光束をスクリーン上に投影する投影レ
ンズとから構成される投射装置において、光源装置は、
偏光状態がランダムな光源と、光源からの光を集光する
凹面鏡と、光源から入射した光束の偏光方向を揃える偏
光変換素子と、偏光変換素子から射出した偏光方向が揃
った光束の強度分布を均一化するインテグレータとを備
え、投影画像に発生する色ムラを防止している。
Further, in Japanese Unexamined Patent Publication No. 10-333097, a light source device which emits a light beam having a uniform polarization direction,
In a projection device including a transmissive liquid crystal panel as an image display element arranged at a position where the light flux from the light source device is incident, and a projection lens that projects the light flux transmitted through the liquid crystal panel onto a screen, The device is
A light source with a random polarization state, a concave mirror that collects the light from the light source, a polarization conversion element that aligns the polarization direction of the light flux incident from the light source, and an intensity distribution of the light flux that is emitted from the polarization conversion element and has the same polarization direction. A uniformizing integrator is provided to prevent color unevenness that occurs in a projected image.

【0006】さらに、特開平11−295658号公報
においては、座標軸における一方の軸方向のみに偏芯し
たレンズを備えた第1マルチレンズアレイと、第1マル
チレンズアレイの各レンズによって前記一方の軸方向に
屈折された光を集光することができるレンズによって構
成されている第2マルチレンズアレイを備え、色分離/
合成や偏光分離を行なう光学薄膜に対する入射角度補正
を行っている。
Further, in Japanese Patent Application Laid-Open No. 11-295658, a first multi-lens array having a lens eccentric only in one axial direction of a coordinate axis, and each of the lenses of the first multi-lens array is provided with the one axis. The second multi-lens array including the lenses capable of collecting the light refracted in the direction,
Incident angle correction is performed on the optical thin film that performs synthesis and polarization separation.

【0007】[0007]

【発明が解決しようとする課題】ところで、液晶プロジ
ェクタの永遠のテーマともいえるスクリーン輝度競争は
年々激しくなってきている。スクリーン輝度を上げる手
段の1つとして、パネル照射領域に対してより大きな入
射角度、すなわちFナンバーの小さい照明光学系を作る
必要性がある。しいては偏光変換素子に、より大きな入
射角度の光を集める必要がある。しかし、偏光変換素子
の分離面は、一般に入射角度に依存して分光透過率、反
射率の分布が変化するので、入射角度が大きくなると偏
光変換素子から出射する光が変化し、パネル等の画像表
示素子を照射して、スクリーン上に色むらを発生させる
という課題がある。
By the way, the competition for screen brightness, which can be said as an eternal theme of liquid crystal projectors, is becoming more intense year by year. As one means for increasing the screen brightness, it is necessary to make an illumination optical system having a larger incident angle with respect to the panel irradiation area, that is, a smaller F number. Therefore, it is necessary to collect light having a larger incident angle on the polarization conversion element. However, on the separation surface of the polarization conversion element, the distribution of the spectral transmittance and the reflectance generally changes depending on the incident angle. Therefore, when the incident angle becomes large, the light emitted from the polarization conversion element changes, and the image of the panel or the like changes. There is a problem in that the display element is irradiated to cause color unevenness on the screen.

【0008】また、図6に示すように、従来例での偏光
変換素子502の分離面503により反射された光の出
射角度は変らないが、光路が長い分、光の広がりが大き
くなり、隣り合う偏光分離面での光のロスを発生させて
いた。
Further, as shown in FIG. 6, although the outgoing angle of the light reflected by the separation surface 503 of the polarization conversion element 502 in the conventional example does not change, the longer the optical path, the wider the light spreads, and the next. It caused a loss of light on the matching polarization splitting surface.

【0009】図3及び図4に、入射角度45°で入射す
る光を偏光方向が直交する2つの直線偏光成分に分離す
るように設計された偏光分離面の分光反射率、分光透過
率の分布を示す。図からS偏光成分については入射角度
が45°から変化すると長波長側で反射率が増減し、P
偏光成分については短波長側及び中間波長で透過率が減
少する事がわかる。
3 and 4, the distribution of the spectral reflectance and the spectral transmittance of the polarization splitting surface designed to split the light incident at an incident angle of 45 ° into two linearly polarized light components whose polarization directions are orthogonal to each other. Indicates. From the figure, for the S-polarized component, when the incident angle changes from 45 °, the reflectance increases and decreases on the long wavelength side, and P
It can be seen that the transmittance of the polarized component decreases on the short wavelength side and the intermediate wavelength.

【0010】また、このように偏光変換素子への入射角
度特性を補正する例として、特開平10−33309
7、特開平11−295658等があり、本発明とは違
う観点から提案されている。
Further, as an example of correcting the incident angle characteristic to the polarization conversion element as described above, Japanese Patent Application Laid-Open No. 10-33309.
7, JP-A-11-295658 and the like, which have been proposed from a viewpoint different from the present invention.

【0011】[0011]

【課題を解決するための手段】上記課題を解決する為
に、本発明によるプロジェクタの照明光学システムは、
白色光を発生する光源と、光源からの光を分割集光する
ための複数のレンズから構成されている第1のレンズア
レイと、第1のレンズアレイの焦点近傍に配置され、第
1のレンズアレイの各レンズに対応するレンズから構成
されている第2のレンズアレイと、前記白色光源からの
光を単一偏光方向に変換する偏光変換素子を配置し、前
記第2のレンズアレイの各レンズに対応する各偏光変換
素子入射面及び出射面が特定の曲率を有しており、入射
波長により異なる入射角度にて偏光変換素子へ入射され
るほぼ全ての光を、主光線軸に対しほぼ平行とすること
を特徴とする。
In order to solve the above-mentioned problems, the illumination optical system of the projector according to the present invention comprises:
A first lens array including a light source that emits white light, a plurality of lenses for dividing and condensing light from the light source, a first lens array that is disposed near a focal point of the first lens array, and a first lens Each lens of the second lens array includes a second lens array including lenses corresponding to each lens of the array and a polarization conversion element that converts light from the white light source into a single polarization direction. The incident surface and the exit surface of each polarization conversion element corresponding to are parallel to the principal ray axis, and almost all the light incident on the polarization conversion element at different incident angles depending on the incident wavelength is It is characterized by

【0012】さらに好ましくは、前記偏光変換素子入射
面及び出射面の特定の曲率がほぼ同じであることを特徴
とし、また、前記偏光変換素子入射面及び出射面の曲率
方向を同一もしくは反対にする事を特徴とする。
More preferably, the incident surface and the exit surface of the polarization conversion element have substantially the same specific curvature, and the directions of curvature of the incident surface and the exit surface of the polarization conversion element are the same or opposite. Characterize things.

【0013】[0013]

【発明の実施の形態】図1及び図2を用いて、本発明に
おける実施の形態を示す。図2は本願発明が好適に用い
られるプロジェクタ光学系配置図であり、図1は図2の
光学系配置図のうち、白色光源101からの光が、第1
のレンズアレイ102を通過し、第2のレンズアレイ1
03近傍に集光され、該集光位置近傍に配置される偏光
変換素子104の拡大図である。白色光源101からの
光は、スクリーン上の光均一化のため、第1のレンズア
レイ102のレンズ各々により、第2のレンズアレイ1
03近傍で集光されるが、その集光近傍位置の偏光変換
素子104の入射面及び出射面が特定の曲率を有するこ
とが本願発明では重要である。
DETAILED DESCRIPTION OF THE INVENTION An embodiment of the present invention will be described with reference to FIGS. 2 is a layout view of a projector optical system in which the present invention is preferably used. FIG. 1 is a layout view of the optical system of FIG.
Of the second lens array 1 after passing through the lens array 102 of
FIG. 3 is an enlarged view of the polarization conversion element 104 that is focused near 03 and is disposed near the focusing position. The light from the white light source 101 is supplied to the second lens array 1 by each of the lenses of the first lens array 102 in order to make the light on the screen uniform.
Although the light is condensed in the vicinity of 03, it is important in the present invention that the incident surface and the emission surface of the polarization conversion element 104 in the vicinity of the condensed light have a specific curvature.

【0014】図1を用いて、1つのレンズセルを通る3
つの光線の動きにて、詳細に説明する。図1に示す3つ
の光線A、B(主光線)、Cは、この曲率105により
偏光変換素子への入射角度は光線A,C共に、主光線で
あるBとほぼ平行になるように屈折され、偏光変換素子
内部の偏光分離面106にそれぞれ約45°で入射され
るような特定の曲率面を有する偏光変換素子である。偏
光分離面106によりP偏光とS偏光に分離され、光の
利用効率の向上を目的としている。光線を平行にする曲
率rを以下の近似式で示す。偏光変換素子に入射する光
線角度(AとBとの角度)をθ、A〜B間の距離高さをh、
偏光変換素子の屈折率をnとすると、次式が成立する。
Using FIG. 1, 3 passing through one lens cell
This will be explained in detail with reference to the movements of the two light rays. The three rays A, B (principal rays) and C shown in FIG. 1 are refracted by the curvature 105 so that the incident angles of the rays A and C are almost parallel to the principal ray B. The polarization conversion element has a specific curvature surface that is incident on the polarization separation surface 106 inside the polarization conversion element at about 45 °. The polarization splitting surface 106 splits the light into P-polarized light and S-polarized light for the purpose of improving the light utilization efficiency. The curvature r that makes the rays parallel is shown by the following approximate expression. The ray angle (angle between A and B) incident on the polarization conversion element is θ, the distance height between A and B is h,
When the refractive index of the polarization conversion element is n, the following equation holds.

【0015】r=−h*(n−1)/θ このように設計することにより、レンズアレイへの光線
入射位置による入射角度の違いをなくす(キャンセルす
る)ことができるため、最終的に画像が投影されたスク
リーン上での色むらの原因となる、入射角度の違う各光
線による分光特性の変化を無くす、若しくは低減するこ
とが可能となる。図3より、40度と50度に比べ45
度の分光特性が600nm以上の赤色において、反射率の
低下もしくは急な落ち込みが抑えられており、赤の明る
さによる色むらを低減できる事がわかる。
R = -h * (n-1) / θ By designing in this way, it is possible to eliminate (cancel) the difference in the incident angle depending on the incident position of the light beam on the lens array, so that the image is finally obtained. It is possible to eliminate or reduce the change in the spectral characteristics due to the light rays having different incident angles, which causes the color unevenness on the projected screen. From Figure 3, 45 degrees compared to 40 degrees and 50 degrees
It can be seen that in a red color with a spectral characteristic of 600 nm or more, a decrease in reflectance or a sharp drop is suppressed, and color unevenness due to the brightness of red can be reduced.

【0016】さらに、偏光分離面での高い透過率、反射
率特性も維持できるため、光の利用効率を高めることが
可能となる。この事は図4から、40度と50度に比べ
45度の分光特性が400〜700nmの可視光全域にお
いて、反射率の低下がしていない事から読み取ることが
できる。また、各々の光線の入射角度を、ほぼ45°近
傍にできるので、偏光変換素子内での光線の広がりが無
くなり、隣の偏光分離面での干渉ロスを少なくするこ
と、さらに、偏光分離面内での輝度むらの影響を抑える
ことが可能となる。言いかえると、前述のように光線の
広がりを抑える事ができるので、偏光分離面内のコート
むらの影響を受け難いものとできる。
Furthermore, since high transmittance and reflectance characteristics at the polarization splitting surface can be maintained, it is possible to improve the light utilization efficiency. This can be read from FIG. 4 because the reflectance is not lowered in the entire visible light range of 400 to 700 nm where the spectral characteristics at 45 degrees are higher than those at 40 degrees and 50 degrees. Further, since the incident angle of each light beam can be set to about 45 °, the spread of the light beam in the polarization conversion element is eliminated, interference loss at the adjacent polarization separation surface is reduced, and further, in the polarization separation surface. It is possible to suppress the influence of uneven brightness on the display. In other words, since the spread of light rays can be suppressed as described above, it is possible to make it less susceptible to uneven coating on the polarization splitting surface.

【0017】次に、偏光分離面106を反射した光線は
偏光変換素子の出射面の曲率107により、入射状態の
光線角度にそれぞれ戻され出射される。また、偏光分離
面106を透過した光線は偏光変換素子の出射面の曲率
107により、入射状態の光線角度に戻され出射する。
この時、入射面と出射面の曲率105、107をほぼ同
じにする事により、出射光線は入射光線の角度を維持
し、その後の第1、第2のコンデンサーレンズ109、
110のレンズ作用により、設計通りの光線が液晶パネ
ル112に到達可能となる。
Next, the light rays reflected by the polarization splitting surface 106 are returned to the light ray angle of the incident state by the curvature 107 of the exit surface of the polarization conversion element and are emitted. Further, the light ray transmitted through the polarization splitting surface 106 is returned to the light ray angle of the incident state by the curvature 107 of the exit surface of the polarization conversion element, and is emitted.
At this time, by making the curvatures 105 and 107 of the entrance surface and the exit surface approximately the same, the outgoing light beam maintains the angle of the incoming light beam, and then the first and second condenser lenses 109,
Due to the lens action of 110, light rays as designed can reach the liquid crystal panel 112.

【0018】図1の場合、入射面と出射面の曲率10
5、107は負の曲率である凹レンズで同一曲率方向に
なっているが、別の光線設計を行った場合、正の曲率で
ある凸レンズで入射し、凹レンズで出射する反対曲率方
向になる光学設計でも本発明が適用可能なことは言うま
でも無い。
In the case of FIG. 1, the curvatures of the entrance and exit surfaces are 10
Reference numerals 5 and 107 are concave lenses having a negative curvature and have the same curvature direction. However, when another ray design is performed, an optical design in which the convex lens having a positive curvature enters and the concave lens emits light has the opposite curvature direction. However, it goes without saying that the present invention is applicable.

【0019】偏光分離面106を反射した光は波長板1
08により、偏光分離面を透過した光と同一偏光方向に
回転合成され、第1、第2のコンデンサーレンズ10
9、110と色分離手段111と液晶パネル112及び
投影レンズ113により、スクリーン114上、明るく
色むらの無い映像が得られる事となる。
The light reflected by the polarization splitting surface 106 is the wave plate 1
08, the light transmitted through the polarization splitting surface is rotationally combined in the same polarization direction, and the first and second condenser lenses 10
By using 9, 110, the color separation means 111, the liquid crystal panel 112, and the projection lens 113, a bright image with no color unevenness can be obtained on the screen 114.

【0020】[0020]

【発明の効果】以上説明したように、本発明によれば、
偏光変換素子の入出射面に曲率を有する事によって、光
の利用効率ロス及びスクリーン上の色むらを抑える事が
可能となり、結果的にスクリーン投影時の明るさと品位
の向上が図れる。
As described above, according to the present invention,
Since the input / output surface of the polarization conversion element has a curvature, it is possible to suppress the loss of light use efficiency and color unevenness on the screen, and as a result, it is possible to improve the brightness and quality at the time of screen projection.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明にかかる偏光変換素子の光学設計図であ
る。
FIG. 1 is an optical design diagram of a polarization conversion element according to the present invention.

【図2】本発明の投射型プロジェクタの偏光変換光学系
の概略図である。
FIG. 2 is a schematic diagram of a polarization conversion optical system of the projection type projector of the present invention.

【図3】入射角度45°近傍における偏光分離面の分光
反射率の分布図である。
FIG. 3 is a distribution diagram of the spectral reflectance of the polarization splitting surface in the vicinity of an incident angle of 45 °.

【図4】入射角度45°近傍における偏光分離面の分光
透過率の分布図である。
FIG. 4 is a distribution diagram of a spectral transmittance of a polarization splitting surface in the vicinity of an incident angle of 45 °.

【図5】従来の照明光学系構成図である。FIG. 5 is a configuration diagram of a conventional illumination optical system.

【図6】図5に示す偏光変換素子において行われる偏光
変換の概略図である。
6 is a schematic diagram of polarization conversion performed in the polarization conversion element shown in FIG.

【符号の説明】[Explanation of symbols]

101 白色光源 102 第1のレンズアレイ 103 第2のレンズアレイ 104 偏光変換素子 105 偏光変換素子の入射曲率面 106 偏光分離面 107 偏光変換素子の出射曲率面 108 波長板 109 第1のコンデンサーレンズ 110 第2のコンデンサーレンズ 111 色分離手段 112 液晶パネル 113 投影レンズ 114 スクリーン 401 第1のレンズアレイ 402 第2のレンズアレイ 403 偏光変換素子 404 第1のコンデンサーレンズ 501 第2のレンズアレイ 502 偏光変換素子 503 偏光分離面 504 波長板 101 white light source 102 first lens array 103 Second lens array 104 Polarization conversion element 105 Incident curvature surface of polarization conversion element 106 polarized light separation plane 107 exit curvature surface of polarization conversion element 108 Wave plate 109 First condenser lens 110 Second condenser lens 111 color separation means 112 LCD panel 113 Projection lens 114 screen 401 First lens array 402 Second lens array 403 Polarization conversion element 404 First condenser lens 501 Second lens array 502 Polarization conversion element 503 Polarization separation plane 504 Wave plate

───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.7 識別記号 FI テーマコート゛(参考) G02F 1/1335 G02F 1/1335 510 510 1/13357 1/13357 G03B 21/00 G03B 21/00 E H04N 5/74 H04N 5/74 A Fターム(参考) 2H049 BA05 BA07 BB62 BC22 2H088 EA14 EA15 HA13 HA17 HA20 HA25 HA28 MA06 2H091 FA05X FA05Z FA10Z FA11Z FA29Z FA41Z FD06 LA30 MA07 2H099 AA12 BA09 CA02 CA08 DA05 5C058 AA06 AB03 AB06 BA05 BA23 EA02 EA11 EA26 EA51 ─────────────────────────────────────────────────── ─── Continuation of front page (51) Int.Cl. 7 Identification code FI theme code (reference) G02F 1/1335 G02F 1/1335 510 510 1/13357 1/13357 G03B 21/00 G03B 21/00 E H04N 5 / 74 H04N 5/74 A F-term (reference) 2H049 BA05 BA07 BB62 BC22 2H088 EA14 EA15 HA13 HA17 HA20 HA25 HA28 MA06 2H091 FA05X FA05Z FA10Z FA11Z FA29Z FA41Z FD06 LA30 MA07 2H099 AA12 BA09 CA02 CA08 DA05 5C058 AA06 AB03 AB06 BA05 BA23 EA02 EA11 EA26 EA51

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 白色光を発生する光源と、光源からの光
を分割集光するための複数のレンズから構成されている
第1のレンズアレイと、第1のレンズアレイの焦点近傍
に配置され、第1のレンズアレイの各レンズに対応する
レンズから構成されている第2のレンズアレイと、前記
白色光源からの光を単一偏光方向に変換する偏光変換素
子を配置し、前記第2のレンズアレイの各レンズに対応
する各偏光変換素子入射面及び出射面が特定の曲率を有
しており、入射波長により異なる入射角度にて偏光変換
素子へ入射されるほぼ全ての光を、主光線軸に対しほぼ
平行とすることを特徴とするプロジェクタの照明光学シ
ステム。
1. A first lens array composed of a light source that emits white light, a plurality of lenses for dividing and condensing light from the light source, and a first lens array that is disposed near a focal point of the first lens array. , A second lens array composed of lenses corresponding to the respective lenses of the first lens array, and a polarization conversion element for converting light from the white light source into a single polarization direction are arranged. Each polarization conversion element corresponding to each lens of the lens array has an entrance surface and an exit surface with a specific curvature, and almost all the light incident on the polarization conversion element at an incident angle different depending on the incident wavelength is converted into a chief ray. An illumination optical system for a projector, which is substantially parallel to the axis.
【請求項2】 請求項1において、前記偏光変換素子入
射面及び出射面の特定の曲率がほぼ同じであることを特
徴とするプロジェクタの照明光学システム。
2. The illumination optical system for a projector according to claim 1, wherein the incident surface and the exit surface of the polarization conversion element have substantially the same specific curvature.
【請求項3】 請求項1において、前記偏光変換素子入
射面及び出射面の曲率方向を同一もしくは反対にする事
を特徴とするプロジェクタの照明光学システム。
3. The illumination optical system for a projector according to claim 1, wherein the incident surface and the exit surface of the polarization conversion element have the same or opposite curvature directions.
JP2001290441A 2001-09-25 2001-09-25 Projector lighting system Expired - Fee Related JP3678353B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2001290441A JP3678353B2 (en) 2001-09-25 2001-09-25 Projector lighting system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2001290441A JP3678353B2 (en) 2001-09-25 2001-09-25 Projector lighting system

Publications (2)

Publication Number Publication Date
JP2003098598A true JP2003098598A (en) 2003-04-03
JP3678353B2 JP3678353B2 (en) 2005-08-03

Family

ID=19112744

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2001290441A Expired - Fee Related JP3678353B2 (en) 2001-09-25 2001-09-25 Projector lighting system

Country Status (1)

Country Link
JP (1) JP3678353B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010072136A (en) * 2008-09-17 2010-04-02 Nikon Corp Illumination optical system and projector device using the same

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010072136A (en) * 2008-09-17 2010-04-02 Nikon Corp Illumination optical system and projector device using the same

Also Published As

Publication number Publication date
JP3678353B2 (en) 2005-08-03

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