JPH10239519A - Phase difference plate, and polarizing element using it - Google Patents

Phase difference plate, and polarizing element using it

Info

Publication number
JPH10239519A
JPH10239519A JP9041193A JP4119397A JPH10239519A JP H10239519 A JPH10239519 A JP H10239519A JP 9041193 A JP9041193 A JP 9041193A JP 4119397 A JP4119397 A JP 4119397A JP H10239519 A JPH10239519 A JP H10239519A
Authority
JP
Japan
Prior art keywords
retardation plate
phase difference
wavelength
polymer
light
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
JP9041193A
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 JP9041193A priority Critical patent/JPH10239519A/en
Publication of JPH10239519A publication Critical patent/JPH10239519A/en
Pending legal-status Critical Current

Links

Landscapes

  • Polarising Elements (AREA)

Abstract

PROBLEM TO BE SOLVED: To generate almost uniform phase difference corresponding to all wavelength in visual light area, by laminating films or sheets specified in the relation of the wavelength dispersion value of a double refractive index and in the relation of phase difference, in the mutually orthogonal direction of lag axes, and specifying the wavelength dispersion value. SOLUTION: In the phase difference plate formed by laminating films or sheets formed of A- and B-polymers which are Α<Β in the relation of the wavelength dispersion value α[α=Δn(450nm)/Δn(650nm)] of a double refractive index Δn, the relation of phase difference R of the respective polymers is RA>RB, the films or sheets are laminated in the orthogonal directions of lag axes of the respective polymers, and the wavelength dispersion value α is made smaller than 1. The A-polymer is selected from a group formed of polypropylene, polymethyl methacrylate, an ethylene-vinyl alcohol copolymer, amorphous polyolefine, and the like, and the B-polymer is selected from the group formed of polystyrene, polyarylate, polycarbonate, polysulfone, polyethersulfone, and the like.

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))の関係がαA<αBであるA及びBポリ
マーからなるフィルムまたはシートを積層した位相差板
において、各ポリマーの位相差Rの関係がRA>RBであ
り、各ポリマーの遅相軸が直行する方位に積層してお
り、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 in which films or sheets made of A and B polymers having a relationship of α AB are laminated, the relationship of the retardation R of each polymer is R A > R B , and each polymer is Are stacked in a direction in which the slow axis is perpendicular to the axis, and the chromatic dispersion value α is smaller than 1.

【0006】また、各ポリマーよりなるフィルムまたは
シートを接着層面内の位相差が5nm以下の接着層を介
して積層していることを特徴とする。
Further, a film or a sheet made of each polymer is laminated via an adhesive layer having an in-plane retardation of 5 nm or less.

【0007】また、各ポリマーよりなるフィルムまたは
シートを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。
[0007] A film or sheet made of each polymer is laminated via an adhesive layer having at least one kind of liquid crystal composition.

【0008】また、複屈折率Δnの波長分散値α(α=
Δn(450nm)/Δn(650nm))の関係がα
A<αBであるA及びBポリマーからなるフィルムまたは
シートを積層した位相差板において、Aポリマーがポリ
プロピレン、ポリメタクリル酸メチル、エチレン−ビニ
ルアルコール共重合体、アモルファスポリオレフィン、
トリアセテート、ジアセテート、ポリビニルアルコール
からなる群から選ばれる少なくとも1種類であることを
特徴とする。
Further, the wavelength dispersion value α (α = α) of the birefringence index Δn
Δn (450 nm) / Δn (650 nm)) is α
In A <alpha consisting in which A and B polymer B film or the retardation plate obtained by laminating a sheet, A polymer polypropylene, polymethyl methacrylate, ethylene - vinyl alcohol copolymer, amorphous polyolefin,
It is characterized by being at least one selected from the group consisting of triacetate, diacetate and polyvinyl alcohol.

【0009】また、複屈折率Δnの波長分散値α(α=
Δn(450nm)/Δn(650nm))の関係がα
A<αBであるA及びBポリマーからなるフィルムまたは
シートを積層した位相差板において、Bポリマーがポリ
スチレン、ポリアリレート、ポリカーボネート、ポリサ
ルホン、ポリエーテルサルホン、ポリエーテルイミド、
ポリイミド、ポリフッ化ビニリデンからなる群から選ば
れる少なくとも1種類であることを特徴とする。
Further, the wavelength dispersion value α of the birefringence index Δn (α =
Δn (450 nm) / Δn (650 nm)) is α
In a retardation plate obtained by laminating films or sheets comprising A and B polymers in which AB , the B polymer is composed of polystyrene, polyarylate, polycarbonate, polysulfone, polyethersulfone, polyetherimide,
It is characterized in that it is at least one selected from the group consisting of polyimide and polyvinylidene fluoride.

【0010】また、位相差Rが(RA−RB)=λ/4に
調整された1/4λ板であることを特徴とする。
Further, characterized in that the phase difference R is (R A -R B) = 1 / 4λ plate which is adjusted to lambda / 4.

【0011】また、位相差Rが(RA−RB)=λ/2に
調整された1/2λ板であることを特徴とする。
Further, the present invention is characterized in that the phase difference R is a half λ plate adjusted to (R A -R B ) = λ / 2.

【0012】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。
Also, a part that divides a part of the unpolarized light into two polarized lights whose polarization planes are orthogonal to each other, and that one of the two polarized lights is changed to match the polarization plane of the polarized light whose polarization plane is not changed. 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.

【0013】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.

【0014】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。
[0014] Further, a cube-type polarizing beam splitter and a light exiting surface on the reflected light side of the polarizing beam splitter are provided on the surface.
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.

【0015】[0015]

【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))の関係がα
A<αBであるA及びBポリマーからなるフィルムまたは
シート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。
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 =
Δn (450 nm) / Δn (650 nm)) is α
AB The film or sheet composed of the polymers A and B is laminated so that the slow axes are perpendicular to each other, so that the optical retardation caused by the material having the characteristic of α A having small wavelength dispersion is obtained. Is canceled 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.

【0016】また、各ポリマーから成るフィルムまたは
シートの位相差の関係が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。
Further, since the relation of the retardation of the film or sheet made of each polymer is RA> RB, the outputted retardation is outputted as polarized light having a smaller phase difference as the wavelength becomes shorter. In other words, the retardation plate of the present invention produces a smaller phase difference as the wavelength of the incident light is shorter, and produces a larger phase difference as the wavelength of the incident light is longer. 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.

【0017】[0017]

【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。本発明の位相差板の光学的物性は次の方法により
測定した。 (1)位相差及び遅相軸 オリンパス光学(株)製偏光顕微鏡BH2とベレックコ
ンペンセーターを用い、波長550nmでの光学的位相
差及び遅相軸を測定した。 (2)波長分散値 大塚電子(株)製RETS−6000を用いて400nm
から780nmの波長範囲の光学的位相差を測定した。
Next, the present invention will be described in detail with reference to examples. However, the present invention is not limited to the following examples. The optical properties of the retardation plate of the present invention were measured by the following methods. (1) Phase difference and slow axis The optical phase difference and the slow axis at a wavelength of 550 nm were measured using a polarizing microscope BH2 manufactured by Olympus Optical Co., Ltd. and a Berek compensator. (2) Wavelength dispersion value 400 nm using RETS-6000 manufactured by Otsuka Electronics Co., Ltd.
The optical phase difference in the wavelength range from to 780 nm was measured.

【0018】(実施例) ポリエチレン−ビニルアルコ
ール共重合体(クラレ社製EF-F、以下、EVOHと略
す)を熱変形温度以上の雰囲気温度の180℃で一軸延
伸し、550nmの光線に対し550nmの位相差に調
整した。延伸EVOHフィルムは遅相軸が延伸方向に一
致し、波長分散値αは1.004であった。
(Example) A polyethylene-vinyl alcohol copolymer (EF-F manufactured by Kuraray Co., Ltd .; hereinafter abbreviated as EVOH) was uniaxially stretched at 180 ° C. at an atmosphere temperature not lower than the thermal deformation temperature, and 550 nm for a light beam of 550 nm. The phase difference was adjusted to In the stretched EVOH film, the slow axis coincided with the stretching direction, and the wavelength dispersion value α was 1.004.

【0019】ポリエーテルスルホン(住友ヘ゛―クライト社製
FS-1300、以下、PESと略す)をガラス転移点以上の
雰囲気温度の240℃で一軸延伸し、550nmの光線
に対し275nmの位相差に調整した。延伸PESフィ
ルムは遅相軸が延伸方向に一致し、波長分散値αは1.
230であった。
Polyether sulfone (manufactured by Sumitomo Heclite Co.)
FS-1300 (hereinafter abbreviated as PES) was uniaxially stretched at 240 ° C. at an atmosphere temperature equal to or higher than the glass transition point, and adjusted to a 275 nm phase difference with respect to a 550 nm light beam. In the stretched PES film, the slow axis coincides with the stretching direction, and the wavelength dispersion value α is 1.
230.

【0020】延伸処理したEVOHフィルムとPESフ
ィルムの遅相軸を互いに直行させて積層貼り合わせした
位相差板を作製した。積層位相差板の位相差は550n
mの光線に対し275nmであり、波長分散値は0.8
09であった。
A retardation plate was prepared by laminating the stretched EVOH film and the PES film with their slow axes perpendicular to each other. The retardation of the laminated retardation plate is 550n
m is 275 nm, and the chromatic dispersion value is 0.8.
09.

【0021】400nmから780nmの波長範囲の光
学的位相差を測定した結果、本発明によるEVOH/P
ES積層型の位相差板から作製した1/2λ板の光学的
機能は、450nmから650nmの波長範囲において
10%以下の位相差ずれであり、良好な1/2λ機能を
示した。
As a result of measuring the optical phase difference in the wavelength range of 400 nm to 780 nm, the EVOH / P according to the present invention was measured.
The optical function of the λλ plate manufactured from the ES laminated type retardation plate had a phase difference shift of 10% or less in a wavelength range of 450 nm to 650 nm, and showed a good λλ function.

【0022】偏光子と検光子の間に本発明の位相差板を
挿入して、偏光子と検光子が平行ニコルに配列された場
合の透過光強度と偏光子と検光子がクロスニコルに配列
された場合の透過高強度を測定することで、本発明によ
り1/2波長に調整されるように作製した位相差板の偏
光変換機能を400nmから780nmの波長範囲で測
定した。直線偏光の偏光面が1/2λ板により90°変
換された直線偏光に変換される効率は、本発明による位
相差板により450nmから650nmの波長範囲で9
8%以上であり、良好な1/2λ機能を示した。
The phase difference plate of the present invention is inserted between the polarizer and the analyzer, and the transmitted light intensity when the polarizer and the analyzer are arranged in parallel Nicols and the polarizer and the analyzer are arranged in crossed Nicols. By measuring the transmission high intensity in the case of the above, the polarization conversion function of the retardation plate manufactured so as to be adjusted to 波長 wavelength according to the present invention was measured in a wavelength range of 400 nm to 780 nm. The efficiency with which the plane of polarization of linearly polarized light is converted into linearly polarized light that has been converted by 90 ° by the λλ plate is 9 in the wavelength range of 450 nm to 650 nm by the retardation plate according to the present invention.
8% or more, indicating a good 1 / 2λ function.

【0023】(比較例) ポリカーボネート(ロンザ社
製Pokalon、以下、PCと略す)を熱変形温度以上の雰
囲気温度の175℃で一軸延伸し、550nmの光線に
対し275nmの位相差に調整した。延伸PCフィルム
は遅相軸が延伸方向に一致し、波長分散値αは1.09
8であった。
(Comparative Example) Polycarbonate (Pokalon manufactured by Lonza, hereinafter abbreviated as PC) was uniaxially stretched at 175 ° C., which is an atmosphere temperature higher than the thermal deformation temperature, and adjusted to a 275 nm phase difference with respect to a 550 nm light beam. In the stretched PC film, the slow axis coincides with the stretching direction, and the wavelength dispersion value α is 1.09.
It was 8.

【0024】400nmから780nmの波長範囲の光
学的位相差を測定した結果、延伸PCフィルムの位相差
板から作製した1/2λ板の光学的機能は、450nm
から650nmの波長範囲において28%の位相差ずれ
であり、1/2λ機能が大きく低下した。
As a result of measuring the optical retardation in the wavelength range from 400 nm to 780 nm, the optical function of the 1 / 2λ plate produced from the retardation plate of the stretched PC film was 450 nm.
In the wavelength range from 650 nm to 650 nm, the phase difference was 28%, and the 1 / 2λ function was greatly reduced.

【0025】偏光子と検光子の間にPC位相差板を挿入
して、偏光子と検光子が平行ニコルに配列された場合の
透過光強度と偏光子と検光子がクロスニコルに配列され
た場合の透過高強度を測定することで、1/2波長に調
整されるように作製した位相差板の偏光変換機能を40
0nmから780nmの波長範囲で測定した。直線偏光
の偏光面が1/2λ板により90°変換された直線偏光
に変換される効率は、PC位相差板により450nmか
ら650nmの波長範囲で84%から99.9%の分布
が確認され、1/2λ機能の低下を示した。
When a PC retardation plate is inserted between the polarizer and the analyzer, the transmitted light intensity when the polarizer and the analyzer are arranged in parallel Nicols, and the polarizer and the analyzer are arranged in crossed Nicols. By measuring the transmission high intensity in the case, the polarization conversion function of the retardation plate manufactured so as to be adjusted to a half wavelength can be improved.
The measurement was performed in a wavelength range from 0 nm to 780 nm. As for the efficiency with which the plane of polarization of linearly polarized light is converted into linearly polarized light that has been converted by 90 ° by the λλ plate, a distribution of 84% to 99.9% is confirmed by a PC retardation plate in a wavelength range of 450 nm to 650 nm, A decrease in 1 / 2λ function was indicated.

【0026】[0026]

【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】 可視光域における位相差板の波長分散特性FIG. 1 Wavelength dispersion characteristics of a retardation plate in the visible light region

【図2】 本発明の位相差板により作製した1/2波長
板の可視光域における位相差特性
FIG. 2 shows a retardation characteristic in a visible light region of a half-wave plate produced by the retardation plate of the present invention.

【図3】 本発明の位相差板により作製した1/2波長
板の可視光域における偏光変換特性
FIG. 3 shows a polarization conversion characteristic in a visible light region of a half-wave plate manufactured using the retardation plate of the present invention.

Claims (10)

【特許請求の範囲】[Claims] 【請求項1】 複屈折率 nの波長分散値α(α=Δn
(450nm)/Δn(650nm))の関係がαA
αBであるA及びBポリマーからなるフィルムまたはシ
ートを積層した位相差板において、各ポリマーの位相差
Rの関係がRA>RBであり、各ポリマーの遅相軸が直行
する方位に積層しており、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 n.
(450 nm) / Δn (650 nm)) is α A <
In the retardation plate obtained by laminating a film or sheet consisting of A and B polymer is alpha B, the relationship of the phase difference R of the polymer is R A> R B, laminated to the orientation slow axis of each polymer is perpendicular And a chromatic dispersion value α is smaller than 1.
【請求項2】 各ポリマーよりなるフィルムまたはシー
トを接着層面内の位相差が5nm以下の接着層を介して
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. The retardation plate according to claim 1, wherein a film or a sheet made of each polymer is laminated via an adhesive layer having an in-plane retardation of 5 nm or less.
【請求項3】 各ポリマーよりなるフィルムまたはシー
トを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. The retardation plate according to claim 1, wherein a film or a sheet made of each polymer is laminated via an adhesive layer having at least one kind of liquid crystal composition.
【請求項4】 複屈折率Δnの波長分散値α(α=Δn
(450nm)/Δn(650nm))の関係がαA
αBであるA及びBポリマーからなるフィルムまたはシ
ートを積層した位相差板において、Aポリマーがポリプ
ロピレン、ポリメタクリル酸メチル、エチレン−ビニル
アルコール共重合体、アモルファスポリオレフィン、ト
リアセテート、ジアセテート、ポリビニルアルコールか
らなる群から選ばれる少なくとも1種類であることを特
徴とする請求項1、2または3記載の位相差板。
4. A wavelength dispersion value α (α = Δn) of a birefringence index Δn.
(450 nm) / Δn (650 nm)) is α A <
In alpha B retardation plate obtained by laminating a film or sheet consisting of A and B polymers is, polypropylene A polymer, polymethyl methacrylate, ethylene - vinyl alcohol copolymer, amorphous polyolefins, triacetate, diacetate, polyvinyl alcohol 4. The retardation plate according to claim 1, wherein the retardation plate is at least one selected from the group consisting of:
【請求項5】 複屈折率Δnの波長分散値α(α=Δn
(450nm)/Δn(650nm))の関係がαA
αBであるA及びBポリマーからなるフィルムまたはシ
ートを積層した位相差板において、Bポリマーがポリス
チレン、ポリアリレート、ポリカーボネート、ポリサル
ホン、ポリエーテルサルホン、ポリエーテルイミド、ポ
リイミド、ポリフッ化ビニリデンからなる群から選ばれ
る少なくとも1種類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 wavelength dispersion value α (α = Δn) of a birefringence index Δn.
(450 nm) / Δn (650 nm)) is α A <
In the retardation plate obtained by laminating a film or sheet consisting of A and B polymer is alpha B, the group B polymer is polystyrene, polyarylate, polycarbonate, polysulfone, polyether sulfone, polyetherimide, polyimide, polyvinylidene fluoride Claim 1 characterized by being at least one kind selected from
4. The retardation plate according to 2 or 3.
【請求項6】 位相差Rが(RA−RB)=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、3、4または5記載の位相差板。
6. The method of claim 1, wherein the phase difference R is (R A -R B) = λ / 4 1 / 4λ plate, adjusted to
The retardation plate according to 2, 3, 4 or 5.
【請求項7】 位相差Rが(RA−RB)=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、3、4または5記載の位相差板。
7. The method of claim 1, wherein the phase difference R is (R A -R B) = λ / 2 1 / 2λ plate, adjusted to
The retardation plate according to 2, 3, 4 or 5.
【請求項8】 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7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 part that divides a part of the unpolarized light into two polarized lights whose polarization planes are orthogonal to each other, and matches the polarization plane of the polarized light whose polarization plane does not change by changing one of the two polarization planes. A polarizing element comprising a modulating section for causing the phase difference plate according to claim 7 as a modulating section.
【請求項9】 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
7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。
9. A unit for converting non-polarized light into polarized light, wherein the unit is a sheet-like polarizing element that is continuously processed, and the unit is configured to reflect a part of the non-polarized light and reflected light whose polarization planes are orthogonal to each other. The retardation plate according to claim 7, wherein the sheet-like polarizing element has 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10】 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
6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。
10. A cube-type polarization beam splitter, and one light exit surface on the reflected light side of the polarization beam splitter is provided.
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. A polarizing element comprising the retardation plate according to claim 6.
JP9041193A 1997-02-25 1997-02-25 Phase difference plate, and polarizing element using it Pending JPH10239519A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9041193A JPH10239519A (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
JP9041193A JPH10239519A (en) 1997-02-25 1997-02-25 Phase difference plate, and polarizing element using it

Publications (1)

Publication Number Publication Date
JPH10239519A true JPH10239519A (en) 1998-09-11

Family

ID=12601597

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9041193A Pending JPH10239519A (en) 1997-02-25 1997-02-25 Phase difference plate, and polarizing element using it

Country Status (1)

Country Link
JP (1) JPH10239519A (en)

Cited By (7)

* 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
JP2002071956A (en) * 2000-09-05 2002-03-12 Teijin Ltd Lamianted phase difference film and lamianted polarizing film using the same
JP2003139956A (en) * 1999-02-26 2003-05-14 Asahi Glass Co Ltd Phase retardation element, optical element and optical head device
JP2003207640A (en) * 2001-05-10 2003-07-25 Sumitomo Chem Co Ltd Optical retardation plate
JP2003279987A (en) * 2002-03-26 2003-10-02 Seiko Epson Corp Liquid crystal display device and electronic appliance
US6917576B2 (en) 1999-08-26 2005-07-12 Asahi Glass Company, Limited Retarder and optical head device installing the same
KR100901672B1 (en) * 2001-05-10 2009-06-08 스미또모 가가꾸 가부시끼가이샤 Phase retarder

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 (7)

* 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
JP2002071956A (en) * 2000-09-05 2002-03-12 Teijin Ltd Lamianted phase difference film and lamianted polarizing film using the same
JP2003207640A (en) * 2001-05-10 2003-07-25 Sumitomo Chem Co Ltd Optical retardation plate
KR100901672B1 (en) * 2001-05-10 2009-06-08 스미또모 가가꾸 가부시끼가이샤 Phase retarder
JP2003279987A (en) * 2002-03-26 2003-10-02 Seiko Epson Corp Liquid crystal display device and electronic appliance

Similar Documents

Publication Publication Date Title
US7999893B2 (en) Complex birefringent medium, polarizing plate, and liquid crystal device
US7079202B2 (en) Multi-layer diffraction type polarizer and liquid crystal element
JPH1152131A (en) Phase difference plate and polarizing element using the same
JP3174367B2 (en) Laminated wave plate and circularly polarizing plate
JPH1090521A (en) Laminated phase difference plate which rotates polarization axis and projection type liquid crystal display device using the same
JPH1068816A (en) Phase difference plate and circularly polarizing plate
JP2009507256A (en) Polarizing beam splitter and combiner
WO2000025176A1 (en) Liquid crystal display
JP2002303723A (en) Optical film, polarizing plate and display device
JP2020528159A (en) Wide-angle compensation for uniaxial retarder stack
JP3719374B2 (en) Manufacturing method of polarizing element
KR100277325B1 (en) Reflective Liquid Crystal Device_
JP3331150B2 (en) Display element illumination method and liquid crystal display device
JPH10239519A (en) Phase difference plate, and polarizing element using it
JPH10239518A (en) Phase difference plate, and polarizing element using it
JP2002277633A (en) Optical film, polarizing plate and liquid crystal display
JP2005316511A (en) Liquid crystal display
JP2000284127A (en) Bidirectional dichroic circular polarization plate and reflection-transmission type liquid crystal display device
JPH11326896A (en) Liquid crystal display
JPH0313917A (en) Phase difference plate and liquid crystal electrooptical device using this plate
JP2667716B2 (en) Liquid crystal display
JP2013011850A (en) Wavelength plate
JPH09297213A (en) Polarizer
JP2001235624A (en) Polarizing transforming element and projection device for liquid crystal projector
JPH10239525A (en) Phase difference plate, and polarizing element using it

Legal Events

Date Code Title Description
A977 Report on retrieval

Free format text: JAPANESE INTERMEDIATE CODE: A971007

Effective date: 20051116

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20051219

A02 Decision of refusal

Free format text: JAPANESE INTERMEDIATE CODE: A02

Effective date: 20060418