JP2013222188A - Ps converter alignment exposure equipment - Google Patents
Ps converter alignment exposure equipment Download PDFInfo
- Publication number
- JP2013222188A JP2013222188A JP2012104933A JP2012104933A JP2013222188A JP 2013222188 A JP2013222188 A JP 2013222188A JP 2012104933 A JP2012104933 A JP 2012104933A JP 2012104933 A JP2012104933 A JP 2012104933A JP 2013222188 A JP2013222188 A JP 2013222188A
- Authority
- JP
- Japan
- Prior art keywords
- wave
- exposure
- light
- angle
- polarization
- 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
Links
Images
Landscapes
- Polarising Elements (AREA)
- Liquid Crystal (AREA)
Abstract
Description
本発明は、液晶ディスプレイに関する配向膜を任意の方向へ連続的に配向を施すための、複屈折結晶位相差板を使った紫外線偏光露光装置に関する。The present invention relates to an ultraviolet polarized light exposure apparatus using a birefringent crystal phase difference plate for continuously aligning an alignment film in a liquid crystal display in an arbitrary direction.
液晶を整列させるため、液晶封じ込みパネルの液晶との接触面にラビング処理するかわりに、露光によって配向させる技術が普及してきた。紫外線域の直線偏光を露光して配向膜に偏光露光を行い、所望の方向に液晶層の配向制御をすることが出来る。In order to align the liquid crystal, a technique of aligning by exposure instead of rubbing the liquid crystal sealing panel contact surface with the liquid crystal has been widespread. It is possible to control the alignment of the liquid crystal layer in a desired direction by exposing the alignment film to polarized light by exposing to linearly polarized light in the ultraviolet region.
また近年、液晶ディスプレイの走査線を隔線ごとに右45度位相差、左45度位相差を起こすように配向して3D表示用する液晶ディスプレイも普及している。(有沢製作所Xポール)In recent years, a liquid crystal display for 3D display in which the scanning lines of the liquid crystal display are aligned so that a phase difference of 45 degrees to the right and a phase difference of 45 degrees to the left is generated for each separation line has become widespread. (Arisawa Plant X Pole)
光源のランダム光を単偏光に分離するためには、ブリュースター角の蛍石のプリズムを代表とする複屈折の結晶を用い、P波のみを露光に使いS波はプリズム内で反射して熱に変わる。In order to separate the random light of the light source into single polarized light, a birefringent crystal typified by a Brewster angle fluorite prism is used, and only the P wave is used for exposure, and the S wave is reflected in the prism and is heated. Changes to.
複屈折結晶プリズム分光方式はP波だけを使うため、露光機を任意の角度に回転する事によって配向膜に任意の配向を施すことが出来る。Since the birefringent crystal prism spectroscopic system uses only the P wave, the alignment film can be arbitrarily oriented by rotating the exposure device to an arbitrary angle.
任意の配向をロールされたフィルムに連続的に露光するためには、露光装置がフィルムの幅以上の長さが必要で、尚且つ任意の角度の配向露光照射がロールされたフィルムの進行方向に対してなされなければならない。In order to continuously expose an arbitrary orientation to a rolled film, the exposure apparatus needs to have a length longer than the width of the film, and the orientation exposure irradiation at an arbitrary angle in the traveling direction of the rolled film. Must be made against.
ワイヤーグリットはアルミのスリット蒸着がなされた素子で、任意の波長帯のP波を透過しS波を反射する機能があり、スリット光軸方向を回転する事によって直線偏光方向を任意に設定できる。The wire grit is an aluminum slit-deposited element, has a function of transmitting P waves in an arbitrary wavelength band and reflecting S waves, and the linear polarization direction can be arbitrarily set by rotating the slit optical axis direction.
任意の角度に回転したワイヤーグリットのスリット角を同じ角度にして横にならべることによって、フィルム幅方向に対して長尺の任意角の直線偏光板ができる。By aligning the slit angles of the wire grit rotated to an arbitrary angle with the same angle, the linear polarizing plate having an arbitrary angle that is long with respect to the film width direction can be obtained.
ロールされたフィルムはランダム偏光の露光光源を任意の角度に傾けた長尺のワイヤーグリットによって単偏光の露光光を連続的に照射することが出来るようになった。The rolled film can be continuously irradiated with single-polarized exposure light by a long wire grid in which a random-polarized exposure light source is inclined at an arbitrary angle.
しかし、ワイヤーグリッドを使った偏光露光装置はP波のみを露光に使い、S波は反射して光源側へ戻してしまうため、光量が半減する。そしてワイヤーグリッドの持つ光透過率80%とすると、実際に露光に使えるエネルギーは光源からの距離や拡散を無視しても40%(0.5×0.8=0.4)に満たない。However, since the polarization exposure apparatus using a wire grid uses only the P wave for exposure and reflects the S wave and returns it to the light source side, the amount of light is halved. If the light transmittance of the wire grid is 80%, the energy that can be actually used for exposure is less than 40% (0.5 × 0.8 = 0.4) even if the distance from the light source and the diffusion are ignored.
また[0004]に述べたように、光源のランダム光を単偏光に分離するためには、ブリュースター角の蛍石のプリズムを代表とする複屈折の結晶を用い、P波のみを露光に使う場合は透過率が95%有効の為47.5%(0.5×0.95=0.475)程度の単偏光を露光に使うことが出来るが、P波を任意の角度に回転させるためには露光光源と複屈折プリズムが一体であるため、装置そのものを任意の方向に傾けなくてはならない。しかしこの方法だとロールされたフィルムの進行方向に対して垂直である接線上に露光機を配置できないことになる。As described in [0004], in order to separate random light from a light source into single polarized light, a birefringent crystal typified by a Brewster angle fluorite prism is used, and only a P wave is used for exposure. In this case, since the transmittance is 95% effective, a single polarized light of about 47.5% (0.5 × 0.95 = 0.475) can be used for exposure, but the P wave is rotated to an arbitrary angle. Since the exposure light source and the birefringent prism are integral with each other, the apparatus itself must be tilted in an arbitrary direction. However, with this method, the exposure machine cannot be arranged on a tangent line perpendicular to the traveling direction of the rolled film.
ロールされたフィルムの進行方向に対して垂直である接線方向に任意の偏光光を照射させる露光機を提案するためには、P波を任意の角度だけ回転させ、S波を任意の角度だけ回転させるλ/2位相差板が必要になってくる。In order to propose an exposure machine that irradiates an arbitrary polarized light in a tangential direction perpendicular to the traveling direction of the rolled film, the P wave is rotated by an arbitrary angle and the S wave is rotated by an arbitrary angle. A λ / 2 retardation plate is required.
従来、露光光源の発する熱と紫外域の短波長は高エネルギーで、それに耐え、対応する位相差板を製作する事が無かった。
[特開2012−032730]露光装置 配向方向をスイッチにより切りかえる方式
[特開2012−018256]
[特開2011−027968]
[特開2011−203669]Conventionally, the heat generated by the exposure light source and the short wavelength in the ultraviolet region are high energy, withstood it, and no corresponding retardation plate has been manufactured.
[JP 2012-032730] Exposure apparatus Method of switching orientation direction by switch [JP 2012-018256]
[JP 2011-027968]
[JP 2011-203669]
本発明は、紫外域短波長露光用光源から発するランダム偏光の光を、ブリュースター角度に近い角度で分光する誘電体による多層膜の蒸着を施した透明なガラス状板によってP波を透過し、S波を反射する事によって分離し、P波は複数の水晶やサファイヤなどの複屈折を持つ結晶を任意の厚みまで研磨して組み合わせることで温度に依存しないλ/2の位相差板を製作し、該λ/2位相差板を装置した出射窓から偏光角を回転させて出射させることで、任意の偏光角を持った単偏光光を照射することが出来る。The present invention transmits P-waves by a transparent glass-like plate on which a multilayer film is deposited by a dielectric material that splits randomly polarized light emitted from a light source for ultraviolet short wavelength exposure at an angle close to the Brewster angle, The S wave is separated by reflecting, and the P wave is made by combining a plurality of crystals with birefringence, such as quartz and sapphire, to a desired thickness to produce a λ / 2 phase difference plate independent of temperature. By rotating the polarization angle from the exit window provided with the λ / 2 phase difference plate and emitting it, single polarized light having an arbitrary polarization angle can be irradiated.
前項で反射したS波も再び反射ミラーで反射されて、複数の水晶やサファイヤなどの副屈折を持つ結晶を任意の厚みまで研磨して組み合わせることで温度に依存しないλ/2の位相差板を製作し、該λ/2位相差板を装置した出射窓から偏光角を回転させて出射させることで、任意の偏光角を持った単偏光光を照射することが出来る。The S wave reflected in the previous section is also reflected again by the reflection mirror, and a temperature-dependent retardation plate of λ / 2 is obtained by polishing and combining a plurality of crystals having secondary refraction such as quartz and sapphire to an arbitrary thickness. The single polarized light having an arbitrary polarization angle can be irradiated by producing and rotating the polarization angle from the exit window provided with the λ / 2 phase difference plate.
直線偏光ビームを前項該1/2位相差板に入射した場合、直線偏光ビームとして出射される。しかしながら偏光面は入射偏光から回転し、該偏光面の回転角は入射偏光と該λ/2位相差板の軸で成す角度の2倍の値となる。When a linearly polarized beam is incident on the ½ phase difference plate described above, it is emitted as a linearly polarized beam. However, the polarization plane is rotated from the incident polarization, and the rotation angle of the polarization plane is twice the angle formed by the incident polarization and the axis of the λ / 2 retardation plate.
複屈折の結晶からなる位相差板は熱依存性の低い特性が必要であるため、複数の位相差板の遅送軸を直行させたゼロオーダータイプで無ければならない。A retardation plate made of a birefringent crystal needs to have a low thermal dependency, and therefore must be a zero order type in which the slow axes of a plurality of retardation plates are made to go straight.
ゼロオーダー波長板とはたとえば水晶板2枚の速軸を直角に交差し構成されます。
これら水晶板2枚の厚みの差が偏光の回転角を決定します。ゼロオーダタイプの波長板はマルチオーダー波長板と比べ温度や波長の変化による影響が少ないことが特徴である。A zero-order wave plate is formed by, for example, intersecting the fast axes of two quartz plates at right angles.
The difference in thickness between the two quartz plates determines the rotation angle of the polarized light. A zero-order type wave plate is characterized by being less affected by changes in temperature and wavelength than a multi-order wave plate.
本発明は紫外域短波長露光用光源から発するランダム偏光の光を、ブリュースター角度に近い角度で分光する誘電体による多層膜の蒸着を施した透明なガラス状板によってP波を透過し、S波を反射する事によって分離し、該透明なガラス状板を透過するP波の透過率は平行光であれば、光吸収が少なく、S波の反射率も高効率で反射する事が可能であり、かつS波を高反射率の誘電体コートによりミラーで反射して、P波の光進行方向と同方向にすることによって、今まで光源へ戻って行って熱に変換されていたS波を露光に使うことが出来る。The present invention transmits a P wave by a transparent glass-like plate on which a multilayer film is deposited by a dielectric material that splits randomly polarized light emitted from a light source for ultraviolet short wavelength exposure at an angle close to the Brewster angle. If the transmittance of the P wave that is separated by reflecting the wave and transmits through the transparent glass plate is parallel light, the light absorption is small and the reflectance of the S wave can be reflected with high efficiency. S wave that has been converted into heat by returning to the light source so far by reflecting the S wave with a mirror with a highly reflective dielectric coating and making it the same direction as the light traveling direction of the P wave Can be used for exposure.
複屈折率を持った結晶を研磨しゼロオーダータイプに直行させ、かつ露光する配向フィルムに任意の角度の配向をするように該λ/2位相差板を傾けて装置する光配向露光装置は長尺にしてフィルムの幅をロールされた円柱の接線上に露光光を出射する事によって連続的に露光をすることが出来る。A photo-alignment exposure apparatus that polishes a crystal having a birefringence and goes straight to a zero-order type and tilts the λ / 2 retardation plate so that the alignment film to be exposed is oriented at an arbitrary angle is long. The exposure can be continuously performed by emitting exposure light on the tangent of a cylinder whose scale is rolled to the width of the film.
3D表示用フラットパネルディスプレイの隔走査線ごとに右45度λ/4位相差板、左45度λ/4位相差板を露光配光する場合を例とすると、たとえば配向膜を塗布されたフィルムに走査線の幅のマスク窓を隔線毎に開けて(例偶数走査線のみ、あるいは奇数走査線のみに対して窓を開ける)光源から入射するランダム偏光はブリュースター角度に近い角度で分光する誘電体による多層膜の蒸着を施した透明なガラス状板によってP波が透過し、遅相軸67.5度に傾けたλ/2位相差板を通過する事によって45度の位置に直線偏光が傾いてマスク窓Aたどり着き、そこに空いている窓からフィルムに横一列に配向露光することが出来る。次に該ブリュースター角度に近い角度で分光する誘電体による多層膜の蒸着を施した透明なガラス状板によってS波が反射し、高反射率の誘電体コートによりミラーで反射して該P波の光進行方向と同方向にする。そして偏光S波の出射光に遅相軸−22.5度に傾けたλ/2位相差板を通過する事によって−45度の位置に直線偏光が傾いてマスク窓Bたどり着きそこに空いている窓からフィルムに横一列に配向露光することが出来る。
マスクAとマスクBは一体のものでもよく、ロールされたフィルムはマスクA及びマスクB間において同じ張力であるため、フィルムの伸縮による隔走査線の位置ズレ等の危険はなく、連続的に配向露光を続けることが出来る。For example, in the case where the right 45 degree λ / 4 phase difference plate and the left 45 degree λ / 4 phase difference plate are exposed and distributed for each scanning line of the flat panel display for 3D display, for example, a film coated with an alignment film A mask window with the width of the scanning line is opened for each separation line (for example, only the even scanning line or only the odd scanning line is opened). Random polarized light incident from the light source is split at an angle close to the Brewster angle. P-waves are transmitted through a transparent glass-like plate on which a multilayer film is deposited by a dielectric, and linearly polarized at a position of 45 degrees by passing through a λ / 2 phase difference plate inclined at a slow axis of 67.5 degrees. Is inclined to reach the mask window A, and the alignment exposure can be performed in a horizontal row on the film from the vacant window. Next, an S wave is reflected by a transparent glass-like plate on which a multilayer film is deposited by a dielectric material that splits at an angle close to the Brewster angle, and is reflected by a mirror by a high-reflectance dielectric coating, and the P wave is reflected. In the same direction as the light travel direction. Then, by passing through the λ / 2 phase difference plate inclined at the slow axis of −22.5 degrees to the outgoing light of the polarized S wave, the linearly polarized light is inclined at the position of −45 degrees and arrives at the mask window B and is freed there. Orientation exposure can be performed in a horizontal row from the window to the film.
The mask A and the mask B may be integrated, and the rolled film has the same tension between the mask A and the mask B. Therefore, there is no danger of misalignment of the scanning line due to expansion and contraction of the film, and the film is continuously oriented. Exposure can be continued.
前項においてマスクAとマスクBの開口部がフィルム幅で長方形である場合、かつマスクA及びマスクBにたどり着く偏光光がλ/2位相差板の遅相軸をAは67.5度、Bへの出射光へは22.5度とした場合はA,Bとも同じ直線偏光角45度となるため、液晶を封じ込める配向を従来の約2倍の光量で連続的に露光することが出来る。In the previous section, when the openings of the mask A and the mask B are rectangular with the film width, and the polarized light reaching the mask A and the mask B is the slow axis of the λ / 2 phase difference plate, A is 67.5 degrees, B In the case of 22.5 degrees, when A and B are set to 22.5 degrees, the same linear polarization angle is 45 degrees, so that the orientation for confining the liquid crystal can be continuously exposed with about twice the amount of light.
紫外線を含めた短波長域のP波S波コンバートメント配向装置であって、光源が高エネルギーであっても強い耐環境性能を持つため、レーザー光の合波などにも利用ができる。レーザー切断など2台のレーザー発振機光軸を合成することが出来る。A short-wavelength P-wave S-wave conversion orienting apparatus including ultraviolet rays, which has strong environmental resistance even when the light source has high energy, and can be used for combining laser beams. Two laser oscillator optical axes such as laser cutting can be synthesized.
1.露光用光源
2.集光用反射鏡
3.ランダム偏光
4.P波S波偏光分離透明ガラス
5.S波反射ミラー
6.λ/2位相差板A
7.λ/2位相差板B
8.マスクA
9.マスクB
10.ワイヤーグリッド
11.ワイヤーグリッドのスリット角
12.フィルム
13.フィルムの進行方向
14.ローラーの回転方向
15.ローラー
16.出射光方向
17出射光後方
18.P波S波偏光分離透明ガラスによって分離されたP波
19.λ/2位相差板遅相軸角
20.λ/2位相差板によって回転した出射光偏光角
21.P波S波偏光分離透明ガラスによって分離されたS波
22.マスク開口窓1. 1. Light source for
7. λ / 2 retardation plate B
8). Mask A
9. Mask B
10. 10.
Claims (3)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2012104933A JP2013222188A (en) | 2012-04-12 | 2012-04-12 | Ps converter alignment exposure equipment |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2012104933A JP2013222188A (en) | 2012-04-12 | 2012-04-12 | Ps converter alignment exposure equipment |
Publications (1)
Publication Number | Publication Date |
---|---|
JP2013222188A true JP2013222188A (en) | 2013-10-28 |
Family
ID=49593150
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2012104933A Pending JP2013222188A (en) | 2012-04-12 | 2012-04-12 | Ps converter alignment exposure equipment |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2013222188A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN106502034A (en) * | 2015-09-04 | 2017-03-15 | Lg伊诺特有限公司 | Light-emitting device and the luminaire including light-emitting device |
-
2012
- 2012-04-12 JP JP2012104933A patent/JP2013222188A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN106502034A (en) * | 2015-09-04 | 2017-03-15 | Lg伊诺特有限公司 | Light-emitting device and the luminaire including light-emitting device |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN113341569B (en) | Polarization multiplexing diffraction waveguide large-view-field angle imaging system and method | |
WO2019093228A1 (en) | Optical element | |
US20060092513A1 (en) | Polarizing beam splitter and display including the same | |
KR20170037884A (en) | Bragg liquid crystal polarization gratings | |
JP2001166227A (en) | Optical imaging assembly | |
TW201107791A (en) | Three-dimensional light modulation arrangement for modulating a wave field having complex information | |
JP2003035822A (en) | Polariscope and microlithography projection system provided with the same | |
JPH07230243A (en) | Production of hologram | |
JP2001502076A (en) | Display compensated by birefringent holographic film | |
JP3678120B2 (en) | Polarized light irradiation device | |
JP2003315552A (en) | Integrated optical element | |
JPH03156421A (en) | Polarized light source device | |
WO2020125569A1 (en) | Polarized light source for 3d printing of liquid crystal screen | |
US6577445B1 (en) | Composite birefringent crystal and filter | |
KR20010010649A (en) | Polarization Separating And Converting Glass Of Projection Display Unit | |
JP2020534569A5 (en) | ||
JP2013222188A (en) | Ps converter alignment exposure equipment | |
Nassiri et al. | High-order Laguerre-Gauss polychromatic beams from Bragg-Berry flat optics | |
JP5085127B2 (en) | Illumination device with polarization recycling in a double prism | |
CN208399807U (en) | A kind of light path system minimizing HUD | |
JP2007114375A (en) | Light irradiation device, liquid crystal display apparatus and liquid crystal projection apparatus | |
KR20040020411A (en) | Polarization conversion system | |
US20070236793A1 (en) | Polarization converter reflector | |
RU2321031C1 (en) | Reflecting prism for bringing plane of polarization in rotation | |
JPH03196015A (en) | Polarized light source device |