JPH04321001A - Polarized light separating element - Google Patents

Polarized light separating element

Info

Publication number
JPH04321001A
JPH04321001A JP3090266A JP9026691A JPH04321001A JP H04321001 A JPH04321001 A JP H04321001A JP 3090266 A JP3090266 A JP 3090266A JP 9026691 A JP9026691 A JP 9026691A JP H04321001 A JPH04321001 A JP H04321001A
Authority
JP
Japan
Prior art keywords
polarized light
prism
polarization separation
film
light separating
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP3090266A
Other languages
Japanese (ja)
Inventor
Yoshio Yokogawa
美穂 横川
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Seiko Epson Corp
Original Assignee
Seiko Epson Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP3090266A priority Critical patent/JPH04321001A/en
Publication of JPH04321001A publication Critical patent/JPH04321001A/en
Pending legal-status Critical Current

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  • Optical Elements Other Than Lenses (AREA)
  • Polarising Elements (AREA)
  • Surface Treatment Of Optical Elements (AREA)

Abstract

PURPOSE:To inexpensively attain the improvement of polarized light separating efficiency. CONSTITUTION:This polarized light separating element consists of a square prism 4 in which angles formed between a pair of side faces and a bottom face are equal and a triangular prism 3 arranged so as to be stuck to the bottom face the prism 4 through a polarized light separating film, one of angles formed between the bottom face of the prism 3 contacting with the separating film and side faces is equal to the angle formed between each side face and the bottom face of the prism 4 and the face of the prism 3 which is opposed to the stuck face through the separating film is parallel with one of inclined faces of the prism 4. Since the polarized light separating efficiency of the polarized light separating element is high, dielectric multi-layer films can be reduced.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明は、自然偏光を直行する2
つの直線偏光に分離し、かつ、互いの直線偏光の出射方
向が直角である偏光分離素子の構造に関する。
[Industrial Application Field] The present invention is directed to orthogonal natural polarized light.
The present invention relates to a structure of a polarization separation element that separates light into two linearly polarized lights, and the emission directions of the linearly polarized lights are perpendicular to each other.

【0002】0002

【従来の技術】従来の偏光分離素子は図5に示すように
一対の直角プリズムの斜面どうしを接着した構造をとっ
ていた。この偏光分離素子の外表面に0°で、かつ、接
着面に存在する偏光分離膜に対して45°で入射された
自然偏光は、偏光分離膜によって、偏光面が互いに直行
する2つの直線偏光であるS偏光とP偏光に分けられ(
S偏光の大部分は反射され、P偏光の大部分はそのまま
透過する)、90°の分離角を持って、偏光分離素子の
隣接する2つの外表面から出射される。
2. Description of the Related Art A conventional polarization separation element has a structure in which the slopes of a pair of right-angled prisms are glued together, as shown in FIG. Naturally polarized light incident on the outer surface of this polarization separation element at 0° and at 45° to the polarization separation film present on the adhesive surface is divided into two linearly polarized lights whose polarization planes are perpendicular to each other by the polarization separation film. It is divided into S polarized light and P polarized light (
Most of the S-polarized light is reflected, and most of the P-polarized light is transmitted unchanged), and is emitted from two adjacent outer surfaces of the polarization splitting element with a separation angle of 90°.

【0003】0003

【発明が解決しようとする課題】しかし、前述の偏光分
離素子においては、偏光分離素子への自然偏光の入射角
が45°であるために、分離効率に限界があった。分離
効率をあげるには、偏光分離膜の層数を増やす方法があ
るが、層数の増加はコストを上昇させ、かつ膜が暑くな
るほど収差が大きくなってしまう。また、偏光分離素子
を複数使用する、同一素子内に複数箇所偏光分離膜を設
ける等の方法でも上記同様、コストダウンと分離効率の
向上の両方を実現することはできなかった。
However, in the above-mentioned polarized light splitting element, the incident angle of naturally polarized light to the polarized light splitting element is 45 degrees, so that there is a limit to the separation efficiency. One way to increase separation efficiency is to increase the number of layers in the polarization separation film, but increasing the number of layers increases cost, and the hotter the film, the greater the aberrations. Furthermore, even with methods such as using a plurality of polarization separation elements or providing polarization separation films at a plurality of locations within the same element, it has not been possible to achieve both cost reduction and improvement in separation efficiency, as described above.

【0004】そこで本発明では、このような問題点を低
価格で、かつ、簡単な構造によって解決するもので、そ
の目的とするところは高い偏光分離効率が得られる偏光
分離素子を提供するところにある。
The present invention aims to solve these problems at low cost and with a simple structure, and the object thereof is to provide a polarization separation element that can obtain high polarization separation efficiency. be.

【0005】[0005]

【課題を解決するための手段】本発明は、2つのプリズ
ムを偏光分離膜を介して密着配置した偏光分離素子にお
いて、少なくとも1対の側面と底面との角度が等しい四
角柱プリズムと、該四角柱の底面に該偏光分離膜を介し
て密着配置した三角プリズムとからなり、該三角プリズ
ムの該偏光分離膜に接する底面と側面との角度のうち少
なくとも1つが、該四角柱プリズムの少なくとも1対の
側面と底面との角度と等しく、かつ、該三角プリズムの
該偏光分離膜を介して密着配置した面の対向面と、該四
角柱プリズムの一方の斜面とが平行であり、該四角柱プ
リズムの少なくとも1対の側面と底面との角度は、45
°より大きく90°未満であり、該偏光分離膜への偏光
光源からの偏光の入射角は45°より大きく90°より
小さく、該2つのプリズムは、その光入出射面に反射防
止膜を被着させてあり、該偏光分離膜は、誘電多層膜か
らなるので、高い偏光分離効率が得られる。
Means for Solving the Problems The present invention provides a polarization separation element in which two prisms are arranged in close contact with each other through a polarization separation film, including at least one pair of square prisms whose side faces and bottom faces are at equal angles; a triangular prism disposed in close contact with the bottom surface of a prism through the polarization separation film, and at least one of the angles between the bottom surface and the side surface of the triangular prism in contact with the polarization separation film is at least one pair of the square prism. is equal to the angle between the side surface and the bottom surface of the triangular prism, and the opposing surface of the surface of the triangular prism that is closely arranged through the polarization separation film is parallel to one slope of the quadrangular prism, and the quadrangular prism The angle between at least one pair of side faces and the bottom face is 45
The angle of incidence of polarized light from the polarized light source on the polarized light separation film is greater than 45° and less than 90°, and the two prisms are coated with an antireflection film on their light input and output surfaces. Since the polarization separation film is made of a dielectric multilayer film, high polarization separation efficiency can be obtained.

【0006】[0006]

【作用】屈折率の異なる2つの媒質の境界面に光を入射
するとき、境界面での入射光に対する反射光の反射率と
位相との関係はフレネルの反射の法則によって説明され
、次式のように表される。
[Operation] When light is incident on the interface between two media with different refractive indexes, the relationship between the reflectance and phase of the reflected light relative to the incident light at the interface is explained by Fresnel's law of reflection, and is expressed by the following equation. It is expressed as follows.

【0007】[0007]

【数1】 rs={sin(θ1−θ2)/sin(θ1+θ2)
}2
[Formula 1] rs={sin(θ1-θ2)/sin(θ1+θ2)
}2

【0008】[0008]

【数2】 rp={tan(θ1−θ2)/tan(θ1+θ2)
}2ここでrSはS偏光の反射率、rpはP偏光の反射
率を、θ1は入射角、θ2は屈折角である。
[Formula 2] rp={tan(θ1-θ2)/tan(θ1+θ2)
}2 Here, rS is the reflectance of S-polarized light, rp is the reflectance of P-polarized light, θ1 is the incident angle, and θ2 is the refraction angle.

【0009】rpは、入射角がブリュースター角におい
て0%となり、この角度においてP偏光とS偏光の分離
効率が最大となる。ブリュースター角は次式で求められ
る。
The incident angle of rp is 0% at the Brewster angle, and the separation efficiency of P-polarized light and S-polarized light is maximum at this angle. Brewster's angle is determined by the following formula.

【0010】0010

【数3】 θ1=arctan(n1/n2) n1、n2は、2つの媒体のそれぞれの屈折率である。[Math 3] θ1=arctan(n1/n2) n1 and n2 are the respective refractive indices of the two media.

【0011】つまり、本発明において、偏光分離膜にブ
リュースター角で入射した偏光は、フレネルの反射の法
則によりP偏光と、S偏光に分離される。P偏光は、偏
光分離膜で反射されずに直進し、S偏光は、偏光分離膜
によりほぼ100%反射される。
That is, in the present invention, polarized light incident on the polarization separation film at Brewster's angle is separated into P-polarized light and S-polarized light according to Fresnel's law of reflection. P-polarized light travels straight without being reflected by the polarization separation film, and almost 100% of S-polarized light is reflected by the polarization separation film.

【0012】0012

【実施例】図1は、本発明の実施例における立体図であ
り、図2は、断面図である。
Embodiment FIG. 1 is a three-dimensional view of an embodiment of the present invention, and FIG. 2 is a sectional view.

【0013】偏光光源からの光は、図2におけるabか
ら偏光分離素子に入射する。abへの偏光の入射角度は
0°から80°にする。
Light from the polarized light source enters the polarization separation element from ab to ab in FIG. The angle of incidence of polarized light on ab is set from 0° to 80°.

【0014】入射された偏光はbd面上でP偏光とS偏
光に分離される。bd面上の偏光分離膜への入射角度は
45°より大きく90°未満が良い。
The incident polarized light is separated into P polarized light and S polarized light on the bd plane. The angle of incidence on the polarization separation film on the bd plane is preferably greater than 45° and less than 90°.

【0015】また、角abdと、角bdeと、角bdc
の角度は50°から90°にするのが良い。
[0015] Also, the angle abd, the angle bde, and the angle bdc
The angle should preferably be between 50° and 90°.

【0016】P偏光は偏光分離膜で反射されずに偏光分
離膜を通過し、三角プリズムの側面dcから出射される
。ab面とdc面とは平行であるので、入射光と出射光
とは平行である。
The P-polarized light passes through the polarization separation film without being reflected by the polarization separation film, and is emitted from the side surface dc of the triangular prism. Since the AB plane and the DC plane are parallel, the incident light and the outgoing light are parallel.

【0017】偏光分離膜への偏光の入射角がブリュース
ター角である場合の入射角度とS偏光の反射率の関係は
図3に示した。これによると、入射角度が大きくなるほ
どS偏光の反射率が大きくなっている。
FIG. 3 shows the relationship between the incident angle and the reflectance of S-polarized light when the incident angle of polarized light on the polarization separation film is the Brewster angle. According to this, the reflectance of S-polarized light increases as the incident angle increases.

【0018】図4は、本発明の偏光分離素子と、偏光方
向変換手段からなる光学系の構造の1実施例である。偏
光分離素子によって分離されたP偏光の光路上に、偏光
方向変換手段としてλ/2板を設置することにより、偏
光面が90°回転し、S偏光となって直進する。一方S
偏光は、反射鏡によって進行方向を変換されて、両偏光
は、同一方向の偏光方向に変換され、並列に出射される
FIG. 4 shows one embodiment of the structure of an optical system comprising the polarization separation element of the present invention and polarization direction conversion means. By installing a λ/2 plate as a polarization direction converting means on the optical path of the P-polarized light separated by the polarization separation element, the plane of polarization is rotated by 90 degrees, and the P-polarized light travels straight as S-polarized light. On the other hand, S
The traveling direction of the polarized light is changed by a reflecting mirror, and both polarized lights are converted into the same polarization direction and emitted in parallel.

【0019】偏光成分としてP偏光を用いる場合には、
λ/2板をS偏光の光路上に設置し、P偏光の光路上に
は反射鏡を設置する。
When using P-polarized light as the polarized light component,
A λ/2 plate is installed on the optical path of S-polarized light, and a reflecting mirror is installed on the optical path of P-polarized light.

【0020】S偏光とP偏光の分離角度が小さすぎると
、偏光方向変換を行うのに装置が大きくなってしまう。 分離角度が大きすぎると、並列に出射された同一方向の
偏光間の収差が大きくなってしまう。これらを考慮する
と、S偏光とP偏光の分離角度は0°より大きく、13
0°以下が良い。より好ましくは、10°から110°
である。
[0020] If the separation angle between the S-polarized light and the P-polarized light is too small, the size of the apparatus required to convert the polarization direction will become large. If the separation angle is too large, aberrations between polarized lights in the same direction emitted in parallel will become large. Considering these, the separation angle between S-polarized light and P-polarized light is larger than 0°, and 13
0° or less is good. More preferably from 10° to 110°
It is.

【0021】以上、偏光分離膜への入射角と、偏光分離
膜の角abd、及び角bde、角bcdの角度と、偏光
分離素子への入射角と、S偏光とP偏光との分離角度は
、それぞれ、最適値をとるように設定する。
As described above, the angle of incidence on the polarization separation film, the angles abd, bde, and bcd of the polarization separation film, the angle of incidence on the polarization separation element, and the separation angle of S-polarized light and P-polarized light are , are each set to take the optimum value.

【0022】さらに、偏光光源から偏光分離素子への偏
光の入射面と、S偏光、P偏光の出射面には、それぞれ
、反射防止膜を設けた。なお、誘電多層膜からなる偏光
分離膜の層数及び材質は偏光分離効率が最大になるよう
に設定する。
Furthermore, anti-reflection films were provided on the incident surface of polarized light from the polarized light source to the polarized light splitting element and on the exit surfaces of S-polarized light and P-polarized light, respectively. Note that the number of layers and the material of the polarization separation film made of a dielectric multilayer film are set so that the polarization separation efficiency is maximized.

【0023】[0023]

【発明の効果】本発明は、以上説明したように偏光分離
膜への偏光の入射角度が大きくなる構成であるので、分
離効率をあげるために、偏光分離膜の層数を増やす必要
がなく、収差を最小限にすることができる。また、複数
の偏光分離素子を用いる必要がないので、低価格で、か
つ、簡単な構造によって、高い偏光分離効率が得られる
偏光分離素子を提供することができる。
[Effects of the Invention] As explained above, the present invention has a structure in which the angle of incidence of polarized light on the polarized light separation film is increased, so there is no need to increase the number of layers of the polarized light separation film in order to increase separation efficiency. Aberrations can be minimized. Furthermore, since it is not necessary to use a plurality of polarization separation elements, it is possible to provide a polarization separation element that is inexpensive, has a simple structure, and can obtain high polarization separation efficiency.

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

【図1】本発明の偏光分離素子の立体図。FIG. 1 is a three-dimensional diagram of a polarization separation element of the present invention.

【図2】本発明の偏光分離素子の断面図。FIG. 2 is a cross-sectional view of the polarization splitting element of the present invention.

【図3】偏光分離膜への偏光の入射角がブリュースター
角である場合の入射角度とS偏光の反射率の関係を示す
図。
FIG. 3 is a diagram showing the relationship between the incident angle and the reflectance of S-polarized light when the incident angle of polarized light to the polarization separation film is the Brewster angle.

【図4】本発明の偏光分離素子と、偏光方向変換手段か
らなる光学系の構造を示す図。
FIG. 4 is a diagram showing the structure of an optical system including a polarization separation element of the present invention and polarization direction conversion means.

【図5】従来の偏光分離素子の断面図。FIG. 5 is a cross-sectional view of a conventional polarization splitting element.

【符号の説明】[Explanation of symbols]

1  偏光分離素子 2  反射防止膜 3  三角プリズム 4  四角柱プリズム 5  S偏光 6  P偏光 7  偏光光源 8  λ/2板 9  入射光 1 Polarization separation element 2 Anti-reflection film 3 Triangular prism 4 Square prism 5 S polarized light 6 P polarized light 7 Polarized light source 8 λ/2 plate 9 Incident light

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】  2つのプリズムを偏光分離膜を介して
密着配置した偏光分離素子において、少なくとも1対の
側面と底面との角度が等しい四角柱プリズムと、該四角
柱の底面に該偏光分離膜を介して密着配置した三角プリ
ズムとからなり、該三角プリズムの該偏光分離膜に接す
る底面と側面との角度のうち少なくとも1つが、該四角
柱プリズムの少なくとも1対の側面と底面との角度と等
しく、かつ、該三角プリズムの該偏光分離膜を介して密
着配置した面の対向面と、該四角柱プリズムの一方の斜
面とが平行であることを特徴とする偏光分離素子。
1. A polarization separation element in which two prisms are arranged in close contact with each other with a polarization separation film interposed therebetween, comprising: a square prism having at least one pair of side surfaces and a bottom surface having equal angles; and a polarization separation film on the bottom surface of the square prism. and a triangular prism arranged in close contact with each other through a prism, and at least one of the angles between the bottom surface and the side surface of the triangular prism in contact with the polarization separation film is the angle between at least one pair of side surfaces and the bottom surface of the quadrangular prism. 1. A polarized light separating element characterized in that opposing surfaces of the triangular prism which are arranged in close contact with each other via the polarized light separating film are parallel to one slope of the quadrangular prism.
【請求項2】  該四角柱プリズムの少なくとも1対の
側面と底面との角度は、45°より大きく90°未満で
あることを特徴とする請求項1記載の偏光分離素子。
2. The polarization separation element according to claim 1, wherein the angle between the at least one pair of side surfaces and the bottom surface of the quadrangular prism is greater than 45 degrees and less than 90 degrees.
【請求項3】  該偏光分離膜への偏光光源からの偏光
の入射角は45°より大きく90°より小さいことを特
徴とする請求項1記載の偏光分離素子。
3. The polarized light separating element according to claim 1, wherein the incident angle of the polarized light from the polarized light source onto the polarized light separating film is greater than 45° and smaller than 90°.
【請求項4】  該2つのプリズムは、その光入出射面
に反射防止膜を被着させてあることを特徴をする請求項
1記載の偏光分離素子。
4. The polarized light separation element according to claim 1, wherein the two prisms have an antireflection film coated on their light input/output surfaces.
【請求項5】  該偏光分離膜は、誘電多層膜からなる
ことを特徴とする請求項1、請求項2、請求項3、請求
項4記載の偏光分離素子。
5. The polarized light separating element according to claim 1, wherein the polarized light separating film is made of a dielectric multilayer film.
JP3090266A 1991-04-22 1991-04-22 Polarized light separating element Pending JPH04321001A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3090266A JPH04321001A (en) 1991-04-22 1991-04-22 Polarized light separating element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3090266A JPH04321001A (en) 1991-04-22 1991-04-22 Polarized light separating element

Publications (1)

Publication Number Publication Date
JPH04321001A true JPH04321001A (en) 1992-11-11

Family

ID=13993705

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3090266A Pending JPH04321001A (en) 1991-04-22 1991-04-22 Polarized light separating element

Country Status (1)

Country Link
JP (1) JPH04321001A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2015108767A (en) * 2013-12-05 2015-06-11 コニカミノルタ株式会社 Prism for projection optical system, and optical system using the same

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2015108767A (en) * 2013-12-05 2015-06-11 コニカミノルタ株式会社 Prism for projection optical system, and optical system using the same
US9651790B2 (en) 2013-12-05 2017-05-16 Konica Minolta, Inc. Prism for projection optical system and optical system having same

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