JPH10239518A - Phase difference plate, and polarizing element using it - Google Patents

Phase difference plate, and polarizing element using it

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Publication number
JPH10239518A
JPH10239518A JP9041192A JP4119297A JPH10239518A JP H10239518 A JPH10239518 A JP H10239518A JP 9041192 A JP9041192 A JP 9041192A JP 4119297 A JP4119297 A JP 4119297A JP H10239518 A JPH10239518 A JP H10239518A
Authority
JP
Japan
Prior art keywords
phase difference
wavelength
plate
light
dispersion value
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
JP9041192A
Other languages
Japanese (ja)
Inventor
Hisashi Ito
寿 伊東
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.)
Sumitomo Bakelite Co Ltd
Original Assignee
Sumitomo Bakelite Co Ltd
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 Sumitomo Bakelite Co Ltd filed Critical Sumitomo Bakelite Co Ltd
Priority to JP9041192A priority Critical patent/JPH10239518A/en
Publication of JPH10239518A publication Critical patent/JPH10239518A/en
Pending legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To generate a uniform phase difference regardless of wavelength in optical phase difference of all wavelength of visual light, by specifying the wavelength dispersion value of a phase difference plate of such structure that a plural kinds of double reflective media different in the wavelength dispersion value of a double refractive index are laminated in the orthogonally crossing state of respective lag axes. SOLUTION: In the phase difference plate formed by laminating double refractive media 10, 20 different in the wavelength dispersion value α [α=▵n (450nm)/▵n (650nm)] of a double refractive index ▵n, in the orthogonal state of lag axes 11, 21, the wavelength dispersion value α of this phase difference plate is made smaller than 1. When white linear polarized light enters this phase difference plate, optical phase difference generated from material with a characteristic of small wavelength dispersibility is cancelled by phase difference generated by material with a characteristic of large wavelength dispensability, and the cancelled phase difference quantity is larger in the phase difference generated in shorter wavelength. Longer the wavelength, phase difference amount shows the tendency of more monotoneous increase, and the polarized light incoming as white light also generates uniform phase difference in a visible light area so as to be obtained as white polarized light.

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】本発明は光学素子、偏光素
子、光分析装置、光計測装置や光学実験等で、直線偏
光、円偏光、楕円偏光を作り出す際に可視光波長域で一
様な位相差を発生させる広帯域波長板として有利な位相
差板に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical element, a polarizing element, an optical analyzer, an optical measuring apparatus, an optical experiment, and the like, for producing linearly polarized light, circularly polarized light, and elliptically polarized light in a uniform wavelength range in the visible light wavelength region. The present invention relates to a retardation plate that is advantageous as a broadband wave plate that generates a phase difference.

【0002】[0002]

【従来の技術】位相差板は、方解石、雲母、水晶などの
無機材料から構成される薄板や固有複屈折性の高いポリ
マーフィルムを延伸処理することにより得られる。この
位相差板の活用例として直線偏光を円偏光に変換する1
/4波長板(以下1/4λ板と略す)や直線偏光の偏光
振動面を90°変換する1/2波長板(以下1/2λ板
と略す)がある。
2. Description of the Related Art A retardation plate is obtained by stretching a thin plate made of an inorganic material such as calcite, mica, and quartz or a polymer film having a high intrinsic birefringence. Converting linearly polarized light to circularly polarized light 1
There are a 波長 wavelength plate (hereinafter abbreviated as a λλ plate) and a 波長 wavelength plate (hereinafter abbreviated as a 板 λ plate) that converts a polarization oscillation plane of linearly polarized light by 90 °.

【0003】これらの位相差板は単色光の場合は光線波
長の1/4λまたは1/2λの位相差に調整されるが、
可視光域の光線が混在している合成波である白色光の場
合は、位相差板を構成する材料の位相差の波長分散性か
ら各波長での偏光状態の分布が生じ有色の偏光に変換さ
れる。また、波長板の場合、材料の波長分散性から適用
される波長に合わせて調整した位相差板を用意する必要
があるので、波長ごとの波長板が必要になってくる。つ
まり、従来の位相差板では利用する光線波長ごとに波長
板を用意するためコスト高になることや、白色光への適
用が不適である等の問題が生じていた。
[0003] In the case of monochromatic light, these retardation plates are adjusted to a phase difference of 1 / 4λ or 1 / 2λ of the light wavelength.
In the case of white light, which is a composite wave in which light rays in the visible light region are mixed, the distribution of the polarization state at each wavelength occurs due to the wavelength dispersion of the phase difference of the material constituting the phase difference plate, and the light is converted into colored polarized light. Is done. Further, in the case of a wavelength plate, it is necessary to prepare a retardation plate adjusted according to the wavelength to be applied from the wavelength dispersibility of the material, so that a wavelength plate for each wavelength is required. That is, in the conventional retardation plate, there are problems that the cost is increased because a wavelength plate is prepared for each light beam wavelength to be used, and that application to white light is unsuitable.

【0004】[0004]

【発明が解決しようとする課題】本発明の目的は、可視
光の全ての波長における光学的位相差が、波長によらず
一様な位相差を発生するような波長分散性を有する位相
差板を提供することである。
SUMMARY OF THE INVENTION It is an object of the present invention to provide a retardation plate having a wavelength dispersibility such that an optical retardation at all wavelengths of visible light generates a uniform retardation regardless of the wavelength. It is to provide.

【0005】[0005]

【課題を解決するための手段】本発明の位相差板は、前
記の解決しようとする課題を達成するために、複屈折率
Δnの波長分散値α(α=Δn(450nm)/Δn
(650nm))の異なる2種類以上の複屈折媒体の各
遅相軸が直行した状態に積層した構造を有する位相差板
において、該位相差板の波長分散値αが1より小さいこ
とを特徴とする。
In order to achieve the above object, the retardation plate of the present invention has a wavelength dispersion value α (α = Δn (450 nm) / Δn) of the birefringence index Δn.
(650 nm)) in a retardation plate having a structure in which the slow axes of two or more types of birefringent media different in direction are perpendicular to each other, wherein the wavelength dispersion value α of the retardation plate is smaller than 1. I do.

【0006】また、波長分散値α(α=Δn(450n
m)/Δn(650nm))の異なる複屈折媒体が接着
層面内の位相差が5nm以下の1層以上の接着層を介し
て積層していることを特徴とする。
Further, a chromatic dispersion value α (α = Δn (450n
m) / Δn (650 nm)) are characterized by being laminated via one or more adhesive layers having a phase difference of 5 nm or less within the adhesive layer surface.

【0007】また、波長分散値α(α=Δn(450n
m)/Δn(650nm))の異なる複屈折媒体が液晶
組成物を少なくとも1種類以上有した接着層を介して積
層していることを特徴とする。
Further, a chromatic dispersion value α (α = Δn (450n
m) / Δn (650 nm)) are laminated via an adhesive layer having at least one liquid crystal composition.

【0008】また、位相差Rがλ/4に調整された1/
4λ板であることを特徴とする。
[0008] Also, 1 / when the phase difference R is adjusted to λ / 4.
It is a 4λ plate.

【0009】また、位相差Rがλ/2に調整された1/
2λ板であることを特徴とする。
[0009] Further, 1 / in which the phase difference R is adjusted to λ / 2,
It is a 2λ plate.

【0010】また、非偏光光の一部分を互いに偏光面が
直交する2つの偏光に分割する部分と、2つの偏光の内
1つの偏光面を変化させて偏光面の変化しない偏光の偏
光面と一致させる変調部を有している偏光素子におい
て、変調部として本発明の位相差板を用いると良い。
[0010] Further, a portion that divides a part of the unpolarized light into two polarized lights whose polarization planes are orthogonal to each other and coincides with the polarization plane of the polarized light whose polarization plane does not change by changing one of the two polarization planes. In a polarizing element having a modulating section to be used, it is preferable to use the retardation plate of the present invention as the modulating section.

【0011】また、非偏光光を偏光に変換する単位が、
連続的に加工されたシート状偏光素子であって、前記単
位が、前記非偏光光の一部分を互いに偏光面が直交する
反射光及び透過光に分割する部分と、前記反射光の偏光
面を変化させて透過光の偏光面と一致させる変調部を有
しているシート状偏光素子において、変調部として本発
明の位相差板を用いると良い。
A unit for converting non-polarized light into polarized light is
A sheet-shaped polarizing element that is continuously processed, wherein the unit changes a part of the unpolarized light into reflected light and transmitted light whose polarization planes are orthogonal to each other, and changes a polarization plane of the reflected light. In a sheet-like polarizing element having a modulation section that is made to coincide with the polarization plane of transmitted light, the retardation plate of the present invention may be used as the modulation section.

【0012】また、キューブ型偏光ビームスプリッター
と、該偏光ビームスプリッターの反射光側の出射面に1
/4波長板を挟むように組み合わせて張り合わせられた
光反射板と、反射板と該偏光ビームスプリッターを挟ん
で張り合わせられた少なくとも2つ以上の直角プリズム
からなる偏光素子において、1/4波長板として本発明
の位相差板を用いると良い。
[0012] Further, a cube-type polarizing beam splitter and a light exit surface on the reflected light side of the polarizing beam splitter are arranged on the same.
A 偏光 wavelength plate is used as a 反射 wavelength plate in a light reflecting plate bonded and bonded so as to sandwich a 波長 wavelength plate and at least two or more right angle prisms bonded together with the reflecting plate and the polarizing beam splitter therebetween. It is preferable to use the phase difference plate of the present invention.

【0013】[0013]

【発明の実施の形態】本発明の位相差板に白色光の直線
偏光が入射すると、複屈折率Δnの波長分散値α(α=
Δn(450nm)/Δn(650nm))の異なる複
屈折性媒体の遅相軸が直行するように積層されているた
めに、波長分散性の小さい特性を有する材料より生じる
光学的位位相差は、波長分散性の大きい特性を有する材
料により生じる位相差に打ち消される。この時、波長分
散性の大きい特性を有する材料により位相差が打ち消さ
れるために、短波長で生じる位相差ほど打ち消される位
相差量が大きい。
DESCRIPTION OF THE PREFERRED EMBODIMENTS When linearly polarized white light is incident on the retardation plate of the present invention, a wavelength dispersion value α (α =
Since the birefringent media having different Δn (450 nm) / Δn (650 nm) are laminated so that the slow axes are perpendicular to each other, an optical phase difference generated from a material having a small characteristic of wavelength dispersion is: It is canceled out by the phase difference caused by the material having the characteristic of large wavelength dispersion. At this time, since the phase difference is canceled by the material having the property of large wavelength dispersion, the phase difference generated at a shorter wavelength has a larger amount of the canceled phase difference.

【0014】つまり、本発明の位相差板によって、入射
する光線波長が短波長ほど小さな位相差を生じ、入射す
る光線波長が長波長ほど大きな位相差を生じる。よっ
て、本発明による位相差板の波長分散特性は長波長ほど
単調増加する傾向を示し、可視光の全ての波長における
光学的位相差が、波長によらず一様になるような波長分
散性を本発明の位相差板が有するので、白色光として入
射した偏光も可視光域で一様な位相差を生じ白色偏光と
して得ることができる。
That is, with the retardation plate of the present invention, the shorter the wavelength of the incident light beam, the smaller the phase difference, and the longer the wavelength of the incident light beam, the larger the phase difference. Therefore, the wavelength dispersion characteristic of the retardation plate according to the present invention tends to monotonously increase as the wavelength becomes longer, and the wavelength dispersion characteristic is such that the optical phase difference at all wavelengths of visible light becomes uniform regardless of the wavelength. Since the retardation plate of the present invention has the same, the polarized light incident as white light also has a uniform phase difference in the visible light region and can be obtained as white polarized light.

【0015】[0015]

【実施例】次に、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例に限定されるものでは
ない。
Next, the present invention will be described in detail with reference to examples. However, the present invention is not limited to the following examples.

【0016】本発明の位相差板は波長分散値αの異なる
材料が、各々の位相差の遅相軸を直行した状態に2層以
上積層された構造より成る。積層構造は積層される材料
同士の密着性または接着性が実用上問題ないレベルであ
れば2以上の層構造が好ましいが、密着性または接着性
に乏しい材料同士であれば接着層を介した構造の3層以
上の層構成であっても問題はない。
The retardation plate of the present invention has a structure in which two or more layers of materials having different wavelength dispersion values α are stacked in a state where the slow axes of the respective phase differences are perpendicular to each other. The laminated structure is preferably a two or more layered structure if the adhesion or adhesion between the materials to be laminated is practically no problem, but a structure via an adhesive layer if the materials have poor adhesion or adhesion. There is no problem even if the layer configuration has three or more layers.

【0017】より詳しく積層される材料の特性状態を説
明すると、波長分散値の小さな材料と波長分散値が大き
な材料を遅相軸を直行させ積層されている。また、波長
分散性の小さな材料の位相差は波長分散性の大きな材料
の位相差よりも大きいことが好ましい。
The characteristic state of the materials to be laminated will be described in more detail. A material having a small chromatic dispersion value and a material having a large chromatic dispersion value are laminated with their slow axes perpendicular to each other. Further, it is preferable that the phase difference of a material having a small wavelength dispersion is larger than the phase difference of a material having a large wavelength dispersion.

【0018】波長分散性の小さな材料の位相差が波長分
散性の大きな材料の位相差よりも小さい場合は、波長分
散性の大きな複屈折性媒体による位相差を波長分散性の
小さな複屈折性媒体による位相差で打ち消す際に、打ち
消される位相差量が小さいために積層構造による位相差
板の波長分散値は1より小さくならない場合がある。
When the phase difference of a material having a small wavelength dispersion is smaller than the phase difference of a material having a large wavelength dispersion, the phase difference due to the birefringent medium having a large wavelength dispersion is reduced by the birefringent medium having a small wavelength dispersion. When the phase difference is canceled by the phase difference, the wavelength dispersion value of the phase difference plate having the laminated structure may not be smaller than 1 because the amount of the canceled phase difference is small.

【0019】次に、本実施例の位相差板の動作について
説明する。
Next, the operation of the phase difference plate of this embodiment will be described.

【0020】本発明の位相差板に白色光の直線偏光が入
射すると、複屈折率Δnの波長分散値α(α=Δn(4
50nm)/Δn(650nm))の関係がαA<αB
あるA及びB複屈折性媒体の遅相軸が直行するように積
層されているために、波長分散性の小さいαAの特性を
有する材料より生じる光学的位位相差は、波長分散性の
大きいαBの特性を有する材料により生じる位相差に打
ち消される。この時、波長分散性の大きいαBの特性を
有する材料により位相差が打ち消されるために、短波長
で生じる位相差ほど打ち消される位相差量が大きい。
When linearly polarized white light is incident on the retardation plate of the present invention, the wavelength dispersion value α (α = Δn (4
Since the A and B birefringent media having a relationship of [alpha] A <[alpha] B with respect to [50 nm) / [Delta] n (650 nm)] are laminated so that the slow axes are perpendicular to each other, the characteristic of [alpha] A having a small wavelength dispersion is obtained. Is canceled out by the phase difference caused by the material having the property of α B having large wavelength dispersion. At this time, since the phase difference is canceled by the material having the characteristic of α B having large wavelength dispersion, the phase difference generated at a shorter wavelength has a larger amount of canceled phase difference.

【0021】また、各複屈折媒体の位相差(R)の関係
がRA>RBであるため、出射される位相差は短波長ほど
小さな位相差を有する偏光として出射される。つまり、
本発明の位相差板によって、入射する光線波長が短波長
ほど小さな位相差を生じ、入射する光線波長が長波長ほ
ど大きな位相差を生じる。よって、本発明による位相差
板の波長分散特性は長波長ほど単調増加する傾向を示
し、可視光の全ての波長における光学的位相差が、波長
によらず一様な位相差を有する波長分散性を示し、白色
光として入射した偏光も可視光域で一様な位相差を生じ
るために白色偏光として得ることができる。
Since the relationship of the phase difference (R) of each birefringent medium is R A > R B , the emitted phase difference is emitted as polarized light having a smaller phase difference as the wavelength becomes shorter. That is,
According to the retardation plate of the present invention, the shorter the wavelength of the incident light beam, the smaller the phase difference, and the longer the wavelength of the incident light beam, the larger the phase difference. Therefore, the wavelength dispersion characteristic of the retardation plate according to the present invention tends to monotonically increase as the wavelength increases, and the optical phase difference at all wavelengths of visible light has a uniform phase difference regardless of the wavelength. The polarized light incident as white light can also be obtained as white polarized light because a uniform phase difference occurs in the visible light region.

【0022】次に、本実施例の位相差板の各構成部の材
料について説明する。
Next, the material of each component of the phase difference plate of this embodiment will be described.

【0023】位相差板を構成する複屈折性媒体は、延伸
した高分子フィルム、一方向に分子長軸を配向させた低
分子液晶、光硬化型液晶の重合体、低分子液晶と光硬化
型液晶の複合重合体、熱硬化型液晶の重合体、低分子液
晶と熱硬化型液晶の複合重合体、側鎖型高分子液晶、主
鎖型高分子液晶の配向及び厚みを制御したもの、液晶組
成物を固体基板で狭持した液晶セル、無機酸化物、二色
性有機分子を斜方蒸着等のドライプロセスで製膜したも
の、雲母や水晶等の結晶性のものからなる群から選ばれ
る波長分散値αの異なる2種類以上の材料よりなる積層
構造位相差板であり、入射する光束に対して一様な位相
差を与えるもので構成されることが好ましく、更に、波
長分散値αの差が大きいものがより好ましい。
The birefringent medium constituting the retardation plate is a stretched polymer film, a low-molecular liquid crystal having a long molecular axis oriented in one direction, a polymer of a photocurable liquid crystal, a low-molecular liquid crystal and a photocurable liquid crystal. Liquid crystal composite polymer, thermosetting liquid crystal polymer, low molecular liquid crystal / thermosetting liquid crystal composite polymer, side-chain polymer liquid crystal, main-chain polymer liquid crystal with controlled orientation and thickness, liquid crystal It is selected from the group consisting of liquid crystal cells in which the composition is sandwiched between solid substrates, inorganic oxides, dichroic organic molecules formed by a dry process such as oblique evaporation, and crystalline materials such as mica and quartz. It is a laminated phase difference plate made of two or more kinds of materials having different wavelength dispersion values α, and is preferably configured to give a uniform phase difference to an incident light flux. Those having a large difference are more preferable.

【0024】[0024]

【発明の効果】以上説明したように、本発明の位相差板
を用いることにより、可視光域の全ての波長における光
学的位相差が光線波長によらずほぼ一様になるため、白
色偏光を容易に得られるばかりでなく、波長板を得る際
に適用光線波長ごとの波長板も必要にはならず、一枚の
波長板で全波長域に適用できる利点を備えた位相差板を
提供できる。本発明の位相差板は上記の特徴を活かし
て、偏光を必要とする各種表示素子、特に液晶表示素
子、光スイッチ、光学フィルターや、それを構成要素と
する各種光学測定機器など、広範囲の応用が可能であ
る。
As described above, by using the retardation plate of the present invention, the optical phase difference at all wavelengths in the visible light range becomes almost uniform irrespective of the light wavelength. In addition to being easily obtained, a wave plate for each applied light wavelength is not required when a wave plate is obtained, and a retardation plate having an advantage that one wave plate can be applied to the entire wavelength range can be provided. . The retardation plate of the present invention takes advantage of the above-mentioned characteristics, and can be applied to a wide range of applications such as various display elements requiring polarization, particularly liquid crystal display elements, optical switches, optical filters, and various optical measuring instruments including the same. Is possible.

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

【図1】 本発明の位相差板の構成図。FIG. 1 is a configuration diagram of a phase difference plate of the present invention.

【図2】 本発明の位相差板の構成図。FIG. 2 is a configuration diagram of a retardation plate of the present invention.

【図3】 本発明の位相差板の構成図。FIG. 3 is a configuration diagram of a phase difference plate of the present invention.

【符号の説明】[Explanation of symbols]

10 波長分散値が小さくかつ位相差の大きな複屈折性
媒体 11 複屈折性媒体10の遅相軸 20 複屈折性媒体10より波長分散値が大きくかつ位
相差の小さな複屈折性媒体 21 複屈折性媒体20の遅相軸 30 接着層 40 波長分散値が小さくかつ位相差の大きな複屈折性
媒体 41 複屈折性媒体40の遅相軸 50 波長分散値が大きくかつ複屈折性媒体40の2倍
の位相差より位相差の小さな複屈折性媒体 51 複屈折性媒体50の遅相軸
DESCRIPTION OF SYMBOLS 10 Birefringent medium with small wavelength dispersion value and large phase difference 11 Slow axis of birefringent medium 10 20 Birefringent medium with large wavelength dispersion value and small phase difference than birefringent medium 10 21 Birefringence Slow axis of medium 20 30 Adhesive layer 40 Birefringent medium with small wavelength dispersion value and large phase difference 41 Slow axis 50 of birefringent medium 40 Large wavelength dispersion value and twice as large as birefringent medium 40 Birefringent medium having smaller phase difference than phase difference 51 Slow axis of birefringent medium 50

Claims (8)

【特許請求の範囲】[Claims] 【請求項1】 複屈折率Δnの波長分散値α(α=Δn
(450nm)/Δn(650nm))の異なる2種類
以上の複屈折媒体を各遅相軸が直行した状態に積層した
構造を有する位相差板において、該位相差板の波長分散
値αが1より小さいことを特徴とする位相差板。
1. A wavelength dispersion value α (α = Δn) of a birefringence index Δn.
(450 nm) / Δn (650 nm)) in a retardation plate having a structure in which two or more types of birefringent media having different retardation axes are perpendicular to each other, have a wavelength dispersion value α of 1 or more. A phase difference plate characterized by being small.
【請求項2】 波長分散値α(α=Δn(450nm)
/Δn(650nm))の異なる複屈折媒体が接着層面
内の位相差が5nm以下の1層以上の接着層を介して積
層していることを特徴とする請求項1記載の位相差板。
2. A chromatic dispersion value α (α = Δn (450 nm)
2. The retardation plate according to claim 1, wherein birefringent media having different / Δn (650 nm) are laminated via one or more adhesive layers having a retardation in the plane of the adhesive layer of 5 nm or less.
【請求項3】 波長分散値α(α=Δn(450nm)
/Δn(650nm))の異なる複屈折媒体が液晶組成
物を少なくとも1種類以上有した接着層を介して積層し
ていることを特徴とする請求項1記載の位相差板。
3. A chromatic dispersion value α (α = Δn (450 nm)
2. The retardation plate according to claim 1, wherein birefringent media having different / Δn (650 nm) are laminated via an adhesive layer having at least one type of liquid crystal composition.
【請求項4】 位相差Rがλ/4に調整された1/4λ
板であることを特徴とする請求項1、2または3記載の
位相差板。
4. A quarter-wave having a phase difference R adjusted to λ / 4.
4. The phase difference plate according to claim 1, wherein the phase difference plate is a plate.
【請求項5】 位相差Rがλ/2に調整された1/2λ
板であることを特徴とする請求項1、2または3記載の
位相差板。
5. A half-wave having a phase difference R adjusted to λ / 2.
4. The phase difference plate according to claim 1, wherein the phase difference plate is a plate.
【請求項6】 非偏光光の一部分を互いに偏光面が直交
する2つの偏光に分割する部分と、2つの偏光の内1つ
の偏光面を変化させて偏光面の変化しない偏光の偏光面
と一致させる変調部を有している偏光素子において、変
調部として請求項5記載の位相差板を有していることを
特徴とする偏光素子。
6. A part that divides a part of the unpolarized light into two polarized lights whose polarization planes are orthogonal to each other, and matches a polarization plane of a polarized light whose polarization plane is not changed by changing one of the two polarization planes. A polarizing element having a modulating section for causing the phase difference plate according to claim 5 as a modulating section.
【請求項7】 非偏光光を偏光に変換する単位が、連続
的に加工されたシート状偏光素子であって、前記単位
が、前記非偏光光の一部分を互いに偏光面が直交する反
射光及び透過光に分割する部分と、前記反射光の偏光面
を変化させて透過光の偏光面と一致させる変調部を有し
ているシート状偏光素子において、変調部として請求項
5記載の位相差板を有していることを特徴とするシート
状偏光素子。
7. A unit for converting non-polarized light into polarized light, wherein the unit is a continuously processed sheet-like polarizing element, and the unit is configured to reflect a part of the non-polarized light as reflected light whose polarization plane is orthogonal to each other. 6. The retardation plate according to claim 5, wherein the retardation plate is a modulator in a sheet-shaped polarizing element having a portion that divides the transmitted light and a modulator that changes the polarization plane of the reflected light to match the polarization plane of the transmitted light. A sheet-like polarizing element comprising:
【請求項8】 キューブ型偏光ビームスプリッターと、
該偏光ビームスプリッターの反射光側の出射面に1/4
波長板を挟むように組み合わせて張り合わせられた光反
射板と、反射板と該偏光ビームスプリッターを挟んで張
り合わせられた少なくとも2つ以上の直角プリズムから
なる偏光素子において、1/4波長板として請求項4記
載の位相差板を有していることを特徴とする偏光素子。
8. A cube-type polarizing beam splitter,
The output surface on the reflected light side of the polarizing beam splitter is 1/4
Claims: In a polarizing element comprising a light reflecting plate bonded together so as to sandwich a wavelength plate, and at least two or more right-angle prisms bonded together across a reflecting plate and the polarizing beam splitter, a 1/4 wavelength plate is claimed. A polarizing element comprising the retardation plate according to 4.
JP9041192A 1997-02-25 1997-02-25 Phase difference plate, and polarizing element using it Pending JPH10239518A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9041192A JPH10239518A (en) 1997-02-25 1997-02-25 Phase difference plate, and polarizing element using it

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9041192A JPH10239518A (en) 1997-02-25 1997-02-25 Phase difference plate, and polarizing element using it

Publications (1)

Publication Number Publication Date
JPH10239518A true JPH10239518A (en) 1998-09-11

Family

ID=12601571

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9041192A Pending JPH10239518A (en) 1997-02-25 1997-02-25 Phase difference plate, and polarizing element using it

Country Status (1)

Country Link
JP (1) JPH10239518A (en)

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000310718A (en) * 1999-02-26 2000-11-07 Asahi Glass Co Ltd Phase shift element and optical element
JP2003139956A (en) * 1999-02-26 2003-05-14 Asahi Glass Co Ltd Phase retardation element, optical element and optical head device
US6667835B2 (en) 2001-04-05 2003-12-23 Nitto Denko Corporation Optical film, polarizer and display device
US6795246B2 (en) 2001-07-17 2004-09-21 Nitto Denko Corporation Optical film, polarizer and display device
US6917576B2 (en) 1999-08-26 2005-07-12 Asahi Glass Company, Limited Retarder and optical head device installing the same
WO2008001582A1 (en) 2006-06-28 2008-01-03 Sharp Kabushiki Kaisha Complex birefringent medium, polarizing plate, and liquid crystal device
JPWO2007129464A1 (en) * 2006-05-01 2009-09-17 三井化学株式会社 Method for correcting wavelength dependency of birefringence of optical component, optical component, and display device obtained using the same
US7738064B2 (en) 2002-08-30 2010-06-15 Fujifilm Corporation Retardation plate and its manufacturing method, circularly polarizing plate and 1/2 wave plate using same, and a reflective liquid crystal display
WO2016158298A1 (en) * 2015-03-30 2016-10-06 富士フイルム株式会社 Phase difference film, circularly polarizing film, and image display device

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03126910A (en) * 1989-10-13 1991-05-30 Mitsubishi Rayon Co Ltd Polarization light source device and polarization beam splitter
JPH0545520A (en) * 1991-08-14 1993-02-23 Nitto Denko Corp Polarizing plate and liquid crystal display device
JPH07225379A (en) * 1994-02-15 1995-08-22 Nec Corp Projection type liquid crystal display device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03126910A (en) * 1989-10-13 1991-05-30 Mitsubishi Rayon Co Ltd Polarization light source device and polarization beam splitter
JPH0545520A (en) * 1991-08-14 1993-02-23 Nitto Denko Corp Polarizing plate and liquid crystal display device
JPH07225379A (en) * 1994-02-15 1995-08-22 Nec Corp Projection type liquid crystal display device

Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000310718A (en) * 1999-02-26 2000-11-07 Asahi Glass Co Ltd Phase shift element and optical element
JP2003139956A (en) * 1999-02-26 2003-05-14 Asahi Glass Co Ltd Phase retardation element, optical element and optical head device
US6917576B2 (en) 1999-08-26 2005-07-12 Asahi Glass Company, Limited Retarder and optical head device installing the same
US6667835B2 (en) 2001-04-05 2003-12-23 Nitto Denko Corporation Optical film, polarizer and display device
US6795246B2 (en) 2001-07-17 2004-09-21 Nitto Denko Corporation Optical film, polarizer and display device
US7738064B2 (en) 2002-08-30 2010-06-15 Fujifilm Corporation Retardation plate and its manufacturing method, circularly polarizing plate and 1/2 wave plate using same, and a reflective liquid crystal display
JPWO2007129464A1 (en) * 2006-05-01 2009-09-17 三井化学株式会社 Method for correcting wavelength dependency of birefringence of optical component, optical component, and display device obtained using the same
WO2008001582A1 (en) 2006-06-28 2008-01-03 Sharp Kabushiki Kaisha Complex birefringent medium, polarizing plate, and liquid crystal device
EP2042896A2 (en) 2006-06-28 2009-04-01 Sharp Kabushiki Kaisha Complex birefringent medium polarizing plate, and liquid crystal device
US7999893B2 (en) 2006-06-28 2011-08-16 Sharp Kabushiki Kaisha Complex birefringent medium, polarizing plate, and liquid crystal device
WO2016158298A1 (en) * 2015-03-30 2016-10-06 富士フイルム株式会社 Phase difference film, circularly polarizing film, and image display device
US10564339B2 (en) 2015-03-30 2020-02-18 Fujifilm Corporation Phase difference film, circularly polarizing film, and image display device

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