JPH04121703A - Phase difference element - Google Patents
Phase difference elementInfo
- Publication number
- JPH04121703A JPH04121703A JP24109690A JP24109690A JPH04121703A JP H04121703 A JPH04121703 A JP H04121703A JP 24109690 A JP24109690 A JP 24109690A JP 24109690 A JP24109690 A JP 24109690A JP H04121703 A JPH04121703 A JP H04121703A
- Authority
- JP
- Japan
- Prior art keywords
- retardation
- plates
- phase difference
- wavelength
- wavelength dependence
- 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
- 238000010030 laminating Methods 0.000 abstract description 4
- 239000004973 liquid crystal related substance Substances 0.000 description 9
- 230000001419 dependent effect Effects 0.000 description 4
- 238000010586 diagram Methods 0.000 description 3
- 238000004040 coloring Methods 0.000 description 2
- 239000004925 Acrylic resin Substances 0.000 description 1
- 229920000178 Acrylic resin Polymers 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
Landscapes
- Polarising Elements (AREA)
Abstract
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は位相差素子に関するものである。[Detailed description of the invention] [Industrial application field] The present invention relates to a phase difference element.
位相差素子は、光学系における屈折率異方性の調整等に
使用されており、この位相差素子としては、従来、ジア
セテート樹脂板やアクリル樹脂板等からなる位相差板が
単独で用いられている。この位相差板は、その屈折率異
方性Δnが全ての波長光に対して一定ではなく、シたが
って、この位相差板のリタデーションΔnd(屈折率異
方性Δnと板厚dとの積)には波長依存性がある。Retardation elements are used to adjust refractive index anisotropy in optical systems, and conventionally, retardation plates made of diacetate resin plates, acrylic resin plates, etc. have been used alone. ing. In this retardation plate, its refractive index anisotropy Δn is not constant for all wavelengths of light, and therefore, the retardation Δnd (product of refractive index anisotropy Δn and plate thickness d) of this retardation plate is ) has wavelength dependence.
ところで、この位相差板は、例えば液晶表示素子(主に
STN型液晶表示素子)における透過光の色付きの補償
に使用されているが、この場合、液晶表示素子の透過光
の色付きを補償するには、位相差板のリタデーションΔ
ndを、液晶表示素子のリタデーションΔnd(液晶の
屈折率異方性Δnと液晶層厚dとの積)に応じた値にす
る必要がある。そしてこの場合、位相差板のリタデーシ
ョンΔndには波長依存性があり、また液晶表示素子の
リタデーションΔndにも波長依存性があるため、可視
光領域の全ての波長光についてその色付きを補償するに
は、位相差板として、液晶表示素子とほぼ同じ波長依存
性をもつものを使用する必要がある。By the way, this retardation plate is used, for example, to compensate for the coloring of transmitted light in a liquid crystal display element (mainly an STN type liquid crystal display element); is the retardation Δ of the retardation plate
It is necessary to set nd to a value corresponding to the retardation Δnd of the liquid crystal display element (the product of the refractive index anisotropy Δn of the liquid crystal and the liquid crystal layer thickness d). In this case, the retardation Δnd of the retardation plate has wavelength dependence, and the retardation Δnd of the liquid crystal display element also has wavelength dependence, so it is necessary to compensate for the coloring of light of all wavelengths in the visible light region. , it is necessary to use a retardation plate that has almost the same wavelength dependence as that of the liquid crystal display element.
しかしながら、上記位相差板は、その材質および製法等
によって決まる固有の波長依存性をもっているため、各
種位相差板のなかから所望の波長依存性をもつ位相差板
を探しても、該当するものがないことが多い。However, the above-mentioned retardation plate has a unique wavelength dependence determined by its material, manufacturing method, etc., so even if you search for a retardation plate with the desired wavelength dependence among various retardation plates, you will not be able to find the appropriate one. Often there isn't.
このため、従来は、所望の波長依存性にてきるだけ近い
波長依存性をもつ位相差板を選んで使用しており、例え
ば位相差板を液晶表示素子における透過光の色付きの補
償に使用する場合は、液晶表示素子の波長依存性にてき
るだけ近い波長依存性をもつ位相差板を選んで使用して
いるが、これては、位相差板のリタデーションΔndと
液晶表示素子のリタデーションΔndとが光の波長によ
ってずれるため、可視光領域の全ての波長光についてそ
の色付きを補償することができなかった。For this reason, conventionally, a retardation plate with a wavelength dependence as close as possible to the desired wavelength dependence is selected and used.For example, a retardation plate is used to compensate for colored transmitted light in a liquid crystal display element. In this case, a retardation plate with a wavelength dependence as close as possible to that of the liquid crystal display element is selected and used. Because the color shifts depending on the wavelength of the light, it has not been possible to compensate for the coloration of light of all wavelengths in the visible light region.
本発明は上記のような実情にかんがみてなされたもので
あって、その目的とするところは、波長依存性を任意の
特性にすることができる位相差素子を提供することにあ
る。The present invention has been made in view of the above-mentioned circumstances, and an object of the present invention is to provide a retardation element whose wavelength dependence can be made into an arbitrary characteristic.
本発明の位相差素子は、波長依存性をもちかつ各波長で
のリタデーションが互いに異なる2枚の位相差板を、そ
の進相軸を互いに直交させて積層したものである。The retardation element of the present invention is obtained by laminating two retardation plates having wavelength dependence and different retardations at each wavelength, with their fast axes orthogonal to each other.
〔作用〕
この位相差素子は、波長依存性をもちかつ各波長でのリ
タデーションが互いに異なる2枚の位相差板をその進相
軸を互いに直交させて積層したものであるため、この位
相差素子の特性は、そのリタデーションが2枚の位相差
板のリタデーションの差に相当し、波長依存性が2枚の
位相差板の波長依存性の差に相当する特性となるから、
位相差板の組合わせの選択により、波長依存性を任意の
特性にすることができる。[Operation] This retardation element is made by laminating two retardation plates with wavelength dependence and different retardations at each wavelength with their fast axes orthogonal to each other. The characteristic of is that the retardation corresponds to the difference in retardation of two retardation plates, and the wavelength dependence corresponds to the difference in wavelength dependence of two retardation plates.
By selecting a combination of retardation plates, the wavelength dependence can be made into an arbitrary characteristic.
以下、本発明の一実施例を図面を参照して説明する。 Hereinafter, one embodiment of the present invention will be described with reference to the drawings.
第1図は位相差素子の斜視図である。この実施例の位相
差素子は、リタデーションΔndに波長依存性があり、
かつ各波長でのリタデーションが互いに異なる2枚の位
相差板1,2を積層したもので、この2枚の位相差板1
,2は、その進相軸A 1. A 2を互いに直交させ
て積層されている。FIG. 1 is a perspective view of the phase difference element. In the retardation element of this example, the retardation Δnd has wavelength dependence,
It is a stack of two retardation plates 1 and 2 with different retardations at each wavelength, and these two retardation plates 1
, 2 is its fast axis A1. They are stacked with A2's perpendicular to each other.
なお、Bl、B2は各位相差板1,2の遅相軸であり、
この遅相軸Bl、B2 も互いに直交している。Note that Bl and B2 are slow axes of each retardation plate 1 and 2,
The slow axes Bl and B2 are also orthogonal to each other.
この位相差素子によれば、波長依存性をもちかつ各波長
でのリタデーションが互いに異なる2枚の位相差板1.
2をその進相軸A、、A2を互いに直交させて積層して
いるため、この位相差素子の特性は、そのリタデーショ
ンΔndが2枚の位相差板1,2のリタデーションΔn
、d。According to this retardation element, two retardation plates 1.
2 are stacked with their fast axes A, , A2 perpendicular to each other, so the characteristics of this retardation element are that its retardation Δnd is equal to the retardation Δn of the two retardation plates 1 and 2.
, d.
Δn2 d2の差(Δnd−Δn、d、−Δn2d2)
に相当し、波長依存性が2枚の位相差板1゜2の波長依
存性の差に相当する特性となる。したがって、位相差板
1,2の組合わせを選択すれば、位相差素子の波長依存
性を任意の特性にすることができる。Difference in Δn2 d2 (Δnd-Δn, d, -Δn2d2)
The wavelength dependence corresponds to the difference in the wavelength dependence of the two retardation plates 1°2. Therefore, by selecting a combination of the retardation plates 1 and 2, the wavelength dependence of the retardation element can be made to have arbitrary characteristics.
すなわち、第2図は上記2枚の位相差板1,2の特性を
示し、第3図は位相差素子の特性を示しており、例えば
第2図のように、2枚の位相差板1.2をいずれも、長
波長域側においてリタデーションΔn1dl+ Δn
2 d2が大きくなる波長依存性をもつものを選び、か
つ、一方の位相差板1として、40 Or+mでのΔn
、d、が20Or+m700n印でのΔn、d、が50
0n匝の波長依存性をもつものを用い、他方の位相差板
1として、400nmでのΔn、d、が100nm、
700nmでのΔn、d、が300nmの波長依存性
をもつものを用いた場合、位相差素子の特性は、第3図
のように、400nmでのΔn、d、が100 rv。That is, FIG. 2 shows the characteristics of the two retardation plates 1 and 2, and FIG. 3 shows the characteristics of the retardation element. For example, as shown in FIG. .2, the retardation Δn1dl+ Δn on the long wavelength region side
2 Select a plate with wavelength dependence that increases d2, and use one of the retardation plates 1 as Δn at 40 Or+m.
, d, is 20Or+m700n mark, d, is 50
A plate with a wavelength dependence of 0 nm was used, and as the other retardation plate 1, Δn,d at 400 nm was 100 nm,
When using a retardation element with a wavelength dependence of Δn, d of 300 nm at 700 nm, the characteristics of the retardation element are such that Δn, d at 400 nm is 100 rv, as shown in FIG.
700 nmでのΔn(dBが200 nmの波長依存
性をもつ特性となる。The characteristic is that Δn (dB) at 700 nm has a wavelength dependence of 200 nm.
また、この実施例において、一方の位相差板1の板厚d
1を他方の位相差板2の板厚d2より厚くすれば、位相
差素子の波長依存性は、第3図の特性よりも一方の位相
差板1の特性に近づいた特性となり、一方の位相差板1
の板厚d1を他方の位相差板2の板厚d2より薄くすれ
ば、位相差素子の波長依存性は、第3図の特性よりも他
方の位相差板2の特性に近づいた特性となる。この場合
、各位相差板1,2の板厚dl、d2を適当に選べば、
位相差素子の特性を、波長依存性がほとんどない、はぼ
水平な特性にすることも可能である。In addition, in this embodiment, the plate thickness d of one of the retardation plates 1
1 is made thicker than the plate thickness d2 of the other retardation plate 2, the wavelength dependence of the retardation element becomes a characteristic closer to that of one retardation plate 1 than the characteristics shown in FIG. Retardation plate 1
If the thickness d1 of the retardation plate 2 is made thinner than the thickness d2 of the other retardation plate 2, the wavelength dependence of the retardation element will become closer to the characteristics of the other retardation plate 2 than the characteristics shown in FIG. . In this case, if the plate thicknesses dl and d2 of each retardation plate 1 and 2 are appropriately selected,
It is also possible to make the characteristics of the retardation element substantially horizontal, with almost no wavelength dependence.
なお、上記実施例では、2枚の位相差板1.2として、
長波長域側においてリタデーションが大きくなる波長依
存性の位相差板同士を組合わせているが、この位相差板
1.2の組合わせは、長波長域側においてリタデーショ
ンが小さくなる波長依存性の位相差板同士の組合わせで
も、また、長波長域側においてリタデーションが大きく
なる波長依存性の位相差板と、長波長域側においてリタ
デーションが小さくなる波長依存性の位相差板との組合
わせでもよく(ただし両位相差板1.2の各波長でのリ
タデーションは互いに異なる)、その場合も、位相差素
子の特性は、そのリタデーションΔndが2枚の位相差
板1.2のリタデーションΔn1dl+ Δn2 d2
の差に相当し、また波長依存性が2枚の位相差板1.2
の波長依存性の差に相当する特性となる。In addition, in the above embodiment, as the two retardation plates 1.2,
A combination of wavelength-dependent retardation plates with large retardation on the long-wavelength side is used, but this combination of retardation plates 1 and 2 has a wavelength-dependent position with small retardation on the long-wavelength side. It may be a combination of two retardation plates, or a combination of a wavelength-dependent retardation plate that has a large retardation on the long wavelength side and a wavelength-dependent retardation plate that has a small retardation on the long wavelength side. (However, the retardations at each wavelength of both retardation plates 1.2 are different from each other.) In that case, the characteristics of the retardation element are such that the retardation Δnd is the retardation of the two retardation plates 1.2 Δn1dl+ Δn2 d2
The wavelength dependence corresponds to the difference between the two retardation plates 1.2
This characteristic corresponds to the difference in wavelength dependence of .
なお、本発明の位相差素子は、他の位相差板と組合わせ
て使用することも可能である。Note that the retardation element of the present invention can also be used in combination with other retardation plates.
本発明の位相差素子は、波長依存性をもちかつ各波長で
のリタデーションが互いに異なる2枚の位相差板を、そ
の進相軸を直交させて積層したものであるから、波長依
存性を任意の特性にすることができる。The retardation element of the present invention is made by laminating two retardation plates with wavelength dependence and different retardations at each wavelength, with their fast axes orthogonal, so that the wavelength dependence can be adjusted arbitrarily. can be made into a characteristic.
第1図〜第3図は本発明の一実施例を示したもので、第
1図は位相差素子の斜視図、第2図は各位相差板の特性
図、第3図は位相差素子の特性図である。
1.2・・・位相差板、AI、A2・・・進相軸、B1
B2・・・遅相軸。Figures 1 to 3 show an embodiment of the present invention. Figure 1 is a perspective view of a retardation element, Figure 2 is a characteristic diagram of each retardation plate, and Figure 3 is a diagram of the retardation element. It is a characteristic diagram. 1.2... Retardation plate, AI, A2... Fast axis, B1
B2...Slow axis.
Claims (1)
に異なる2枚の位相差板を、その進相軸を互いに直交さ
せて積層したことを特徴とする位相差素子。A retardation element characterized in that two retardation plates having wavelength dependence and different retardations at each wavelength are laminated with their fast axes orthogonal to each other.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24109690A JPH04121703A (en) | 1990-09-13 | 1990-09-13 | Phase difference element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24109690A JPH04121703A (en) | 1990-09-13 | 1990-09-13 | Phase difference element |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04121703A true JPH04121703A (en) | 1992-04-22 |
Family
ID=17069230
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP24109690A Pending JPH04121703A (en) | 1990-09-13 | 1990-09-13 | Phase difference element |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04121703A (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2002156523A (en) * | 2000-11-16 | 2002-05-31 | Fuji Photo Film Co Ltd | Optical retardation plate and method for producing the same |
JP2002156525A (en) * | 2000-11-21 | 2002-05-31 | Fuji Photo Film Co Ltd | Optical retardation plate and method for manufacturing the same |
US6812983B2 (en) * | 2000-05-17 | 2004-11-02 | Fuji Photo Film Co., Ltd. | Retardation plate and fabrication method thereof, and plate for circularly polarizing light, ½ wave plate and reflection-type liquid crystal display device utilizing the retardation plate |
EP1654585A1 (en) * | 2003-08-14 | 2006-05-10 | LG Chemical, Ltd. | Complex light-compensation c plate with two or more of c plates different in dispersion ratio value and liquid crystal display using the same |
WO2008001582A1 (en) | 2006-06-28 | 2008-01-03 | Sharp Kabushiki Kaisha | Complex birefringent medium, polarizing plate, and liquid crystal device |
JP2010002940A (en) * | 1999-12-16 | 2010-01-07 | Fujifilm Corp | Fabrication method of retardation plate |
-
1990
- 1990-09-13 JP JP24109690A patent/JPH04121703A/en active Pending
Cited By (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2010002940A (en) * | 1999-12-16 | 2010-01-07 | Fujifilm Corp | Fabrication method of retardation plate |
US6812983B2 (en) * | 2000-05-17 | 2004-11-02 | Fuji Photo Film Co., Ltd. | Retardation plate and fabrication method thereof, and plate for circularly polarizing light, ½ wave plate and reflection-type liquid crystal display device utilizing the retardation plate |
JP2002156523A (en) * | 2000-11-16 | 2002-05-31 | Fuji Photo Film Co Ltd | Optical retardation plate and method for producing the same |
JP2002156525A (en) * | 2000-11-21 | 2002-05-31 | Fuji Photo Film Co Ltd | Optical retardation plate and method for manufacturing the same |
EP1654585A1 (en) * | 2003-08-14 | 2006-05-10 | LG Chemical, Ltd. | Complex light-compensation c plate with two or more of c plates different in dispersion ratio value and liquid crystal display using the same |
JP2006527394A (en) * | 2003-08-14 | 2006-11-30 | エルジー・ケム・リミテッド | Compound optical compensation C plate including two or more C plates having different dispersion ratio values and liquid crystal display device using the same |
EP1654585A4 (en) * | 2003-08-14 | 2007-06-27 | Lg Chemical Ltd | Complex light-compensation c plate with two or more of c plates different in dispersion ratio value and liquid crystal display using the same |
US7326364B2 (en) | 2003-08-14 | 2008-02-05 | Lg Chem, Ltd. | Complex light-compensation C plate with two or more of C plates different in dispersion ratio value and liquid crystal display 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 |
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