JPH0131601B2 - - Google Patents
Info
- Publication number
- JPH0131601B2 JPH0131601B2 JP55078090A JP7809080A JPH0131601B2 JP H0131601 B2 JPH0131601 B2 JP H0131601B2 JP 55078090 A JP55078090 A JP 55078090A JP 7809080 A JP7809080 A JP 7809080A JP H0131601 B2 JPH0131601 B2 JP H0131601B2
- Authority
- JP
- Japan
- Prior art keywords
- optical element
- radius
- present
- average distance
- optical
- 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.)
- Expired
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B5/00—Optical elements other than lenses
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B1/00—Optical elements characterised by the material of which they are made; Optical coatings for optical elements
- G02B1/10—Optical coatings produced by application to, or surface treatment of, optical elements
- G02B1/11—Anti-reflection coatings
- G02B1/118—Anti-reflection coatings having sub-optical wavelength surface structures designed to provide an enhanced transmittance, e.g. moth-eye structures
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Surface Treatment Of Optical Elements (AREA)
- Optical Elements Other Than Lenses (AREA)
Description
【発明の詳細な説明】
本発明は非反射特性を有する光学素子に関す
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical element having non-reflective properties.
一般に用いられる可視光を対象とした各種光学
機器(例えばテレビジヨン受像機、カメラ、オー
バーヘツドプロジエクターなど)の光学部品、又
はシヨーウインド、展示ケースなどの透明板、さ
らには計器類、表示部の前面板等の所謂光学素子
に於ては、その光学的性質(光透過性)を高める
ことが試られ、従来より種々の反射防止処置が提
案されいる。例えばガラス系の光学素子には所謂
干渉皮膜が用いられているが、しかしこの干渉皮
膜はプラスチツクに対して適用が難しく、均一な
特性を大面積にわたつて製造することが困難であ
つた。又、近年太陽電池等に対して用いられてき
た微細針状構造は、透過光の散乱を招き易く、製
造が困難で素子表面の耐久性にも難点があつた。 Optical components of various commonly used optical devices that target visible light (e.g. television receivers, cameras, overhead projectors, etc.), transparent panels such as window windows and display cases, and even instruments and displays. Attempts have been made to improve the optical properties (light transmittance) of so-called optical elements such as front plates, and various antireflection treatments have been proposed. For example, a so-called interference coating is used in glass-based optical elements, but this interference coating is difficult to apply to plastics, and it is difficult to manufacture uniform characteristics over a large area. Furthermore, the fine needle-like structures that have been used in solar cells and the like in recent years tend to cause scattering of transmitted light, are difficult to manufacture, and have drawbacks in the durability of the element surface.
本発明は、上記の欠点を解消し、新規な表面形
状とすることにより反射防止機能を有せしめ、主
としてプラスチツクの光学素子に適用して好適な
非反射性光学素子を提供するものである。 The present invention solves the above-mentioned drawbacks and provides a non-reflective optical element which has an anti-reflection function by providing a novel surface shape and is suitable for application mainly to plastic optical elements.
以下、図面を用いて本発明による非反射性光学
素子を説明する。 Hereinafter, a non-reflective optical element according to the present invention will be explained using the drawings.
第1図及び第2図は、共に本発明の基本的構成
を示す。第1図では例えば透明プラスチツクから
成り素体1の表面に、一定の深さD及び略一定の
半径Rを有する円柱形の複数の孔2を平均距離A
を隔てて不規則に配列形成して光学素子3Aを構
成する。又第2図の場合は同様の素体1の表面
に、これと一体に一定の高さD及び略一定の半径
Rを有する円柱形の複数の突起4を平均距離Aを
隔てて不規則に配列形成して光学素子3Bを構成
する。以後、便宜的に第1図の光学素子3Aを多
孔構造素子、第2図の光学素子3Bを多柱構造素
子と夫々呼ぶ。 1 and 2 both show the basic configuration of the present invention. In FIG. 1, a plurality of cylindrical holes 2 having a constant depth D and a substantially constant radius R are formed on the surface of an element body 1 made of transparent plastic, for example, at an average distance A.
The optical element 3A is formed by irregularly arranging and forming the optical element 3A. In the case of FIG. 2, a plurality of cylindrical projections 4 having a constant height D and a substantially constant radius R are irregularly spaced apart from each other by an average distance A on the surface of a similar element body 1. The optical element 3B is formed by forming an array. Hereinafter, for convenience, the optical element 3A in FIG. 1 will be referred to as a porous structure element, and the optical element 3B in FIG. 2 will be referred to as a multi-column structure element.
このような構成を有する夫々の素子3A及び3
Bは、その孔2又は突起4に関して特定条件を満
したとき、可視光に対して反射率が、未処理のも
のに対して1/5〜1/10に低下する。次にその条件
を示す。 Respective elements 3A and 3 having such a configuration
When B satisfies specific conditions regarding the holes 2 or protrusions 4, the reflectance for visible light decreases to 1/5 to 1/10 of that of the untreated material. The conditions are shown below.
上記素子3A及び3Bにおいて、今、空気の屈
折率をnp、素体1のプラスチツクの屈折率をnpと
する。プラスチツクが空間で占める割合をx(0
x1)とすれば、その部分の平均的屈折率n
は近似的に次の関係式で表わせる。 In the above elements 3A and 3B, let us now assume that the refractive index of air is n p and the refractive index of the plastic of the element body 1 is n p . Let the proportion of space occupied by plastic be x(0
x1), the average refractive index n of that part
can be approximately expressed by the following relational expression.
np・x+np(1−x)=n
∴ x=n−np/np−np ………(1)
完全反射防止の振巾条件は
n=√p・p ………(2)
簡単のため、np=1、np=1.5とおけば、n=
1.225、x=0.4495である。n p・x+n p (1−x)=n ∴ x=n−n p /n p −n p ………(1) The amplitude condition for complete anti-reflection is n=√ p・p ………(2 ) For simplicity, let n p = 1, n p = 1.5, then n =
1.225, x=0.4495.
半径Rと平均距離Aの比をr≡R/Aとおけば
多孔構造素子3Aの場合
1−πr2=x ………(3)
多柱構造素子3Bの場合
πr2=x ………(4)
であるから
R=0.418A(多孔構造素子)
R=0.378A(多柱構造素子)
が求める値となる。 If the ratio of the radius R and the average distance A is r≡R/A, then in the case of the porous structure element 3A, 1-πr 2 = x ......(3) In the case of the multi-column structure element 3B, πr 2 = x ......( 4) Therefore, R = 0.418A (porous structure element) and R = 0.378A (multi-column structure element) are the values to be obtained.
又、完全反射防止の位相条件は
nD=λ/4 ………(5)
(但しλは反射防止すべきの光の中心波長)であ
るから、可視光の中心波長λを5500Åとすれば、
D=1123Åとなる。 Also, the phase condition for complete anti-reflection is nD=λ/4 (5) (where λ is the center wavelength of the light to be prevented from reflecting), so if the center wavelength of visible light λ is 5500 Å,
D=1123 Å.
実験的にも略上記の値により、可視光全域にわ
たつて反射率を0.5%程度に減少することが確か
められている。 It has been experimentally confirmed that approximately the above value reduces the reflectance to about 0.5% over the entire visible light range.
斯くして、本発明においては、光学素子の表面
に略1/4λ(但しλは反射防止すべき光の中心波
長)の深さ又は高さDで且つ所定の平均的半径R
を有する複数の孔2又は突起4が2次元的に不規
則に配列形成して成る非反射性光学素子を提案す
るものである。ここで、平均距離Aの値は大きく
なるに従つて製造及び耐久性の為には良いが、短
波長である青色の方から透過光の散乱が増えてく
る。したがつて、この平均距離Aの値は光学素子
の用途に応じて選択すべきである。例えばレンズ
等の場合はA=600Å〜1000Å程度、プロジエク
ターのスクリーン又は文字表示の前面板の場合は
6000Å〜1μm程度が良好な結果が得られる。多
孔構造素子3Aにおいては、その孔2の深さDを
1100Å〜1150Åの範囲に、その半径Rと平均距離
Aの比R/Aを0.41〜0.43の範囲に夫々選定する
を可とする。又、多柱構造素子3Bにおいては、
その突起4の高さDを1100Å〜1150Åの範囲に、
その半径Rと平均距離Aの比R/Aを0.37〜0.39
の範囲に選定するを可とする。総合的にみて、可
視光を非反射にする条件としては、平均距離Aを
500Å〜2μmの範囲に、半径Rと平均距離Aの比
R/Aを0.3〜0.5の範囲に選ぶを可とするもので
ある。 Thus, in the present invention, the surface of the optical element has a depth or height D of approximately 1/4λ (where λ is the center wavelength of the light to be prevented from reflection) and a predetermined average radius R.
The present invention proposes a non-reflective optical element in which a plurality of holes 2 or protrusions 4 having a shape are irregularly arranged two-dimensionally. Here, as the value of the average distance A increases, it is good for manufacturing and durability, but the scattering of transmitted light increases from the blue side, which has a short wavelength. Therefore, the value of this average distance A should be selected depending on the use of the optical element. For example, in the case of a lens, etc., A = about 600Å to 1000Å, and in the case of a projector screen or character display front panel,
Good results can be obtained with a thickness of about 6000 Å to 1 μm. In the porous structure element 3A, the depth D of the hole 2 is
It is possible to select the ratio R/A of the radius R and the average distance A to be in the range of 0.41 to 0.43, respectively, in the range of 1100 Å to 1150 Å. Moreover, in the multi-column structural element 3B,
The height D of the protrusion 4 is in the range of 1100 Å to 1150 Å,
The ratio R/A of its radius R and average distance A is 0.37 to 0.39.
It is possible to select within the range of . Overall, as a condition for non-reflection of visible light, the average distance A is
It is possible to select the ratio R/A between the radius R and the average distance A to be in the range of 0.3 to 0.5 in the range of 500 Å to 2 μm.
尚、上記基本構造においては、孔2又は突起4
を円柱形としたが、例えば第3図に示す如く円錐
形の突起5又は孔(この例は図示せず)をもつて
形成することもできる。この場合には半径Rとし
てはその突起5の平均的半径R′(鎖線位置)を考
えればよい。 In addition, in the above basic structure, the hole 2 or the protrusion 4
Although it is assumed to have a cylindrical shape, it can also be formed with a conical protrusion 5 or hole (this example is not shown), for example, as shown in FIG. In this case, as the radius R, the average radius R' (position of the chain line) of the protrusion 5 may be considered.
上述せる本発明によれば、透明基体1表面に之
と一体に形成した上記条件を満す多数の孔2又は
突起4によつてその凹凸層が所謂単一の干渉膜と
して作用し、可視光全域にわたつて反射率の著し
く低減する非反射性光学素子が得られるものであ
る。この非反射性光学素子は、表面の各孔2又は
突起4の深さ(高さ)Dが小さく且つその半径R
が大きい多孔或いは多柱構造であり且つ一体物で
構成されるので、金型による製造が容易で且つ傷
つきにくい(耐久性がよい)特色を有し、しかも
実用上充分な反射防止作用と波長依存性をを有す
る。したがつて、主として透明プラスチツクの表
面を可視光に対して反射防止する場合に好適であ
る。なお、プラスチツク系の他ガラス系の光学素
子にも適用できること勿論である。依つて本発明
は、可視光を対象とした各種光学機器の光学部
品、シヨーウインド、展示ケース、計器、表示部
等の透明板又は前面板に適用して好適ならしめる
ものである。 According to the present invention described above, the uneven layer acts as a so-called single interference film due to the large number of holes 2 or protrusions 4 that are integrally formed on the surface of the transparent substrate 1 and satisfies the above conditions, and visible light A non-reflective optical element whose reflectance is significantly reduced over the entire area can be obtained. In this non-reflective optical element, the depth (height) D of each hole 2 or protrusion 4 on the surface is small and the radius R
Since it has a large porous or multi-column structure and is composed of a single piece, it is easy to manufacture with a mold and is scratch resistant (good durability), and has a practically sufficient antireflection effect and wavelength dependence. have sex. Therefore, it is suitable mainly for preventing the surface of transparent plastic from reflecting visible light. It goes without saying that the present invention can also be applied to glass-based optical elements in addition to plastic-based optical elements. Therefore, the present invention is suitable for application to transparent plates or front plates of optical components of various optical devices that use visible light, such as window windows, display cases, meters, display units, and the like.
第1図及び第2図は夫々本発明の非反射性光学
素子の基本構造の例を示す斜視図、第3図は本発
明の他の例を示す要部の斜視図である。
1は素体、2は孔、3A,3Bは光学素子、
4,5は突起である。
FIGS. 1 and 2 are perspective views showing an example of the basic structure of a non-reflective optical element according to the present invention, and FIG. 3 is a perspective view of essential parts showing another example of the present invention. 1 is the element body, 2 is the hole, 3A, 3B are the optical elements,
4 and 5 are protrusions.
Claims (1)
すべき光の中心波長)の深さ又は高さで且つ所定
の平均的半径を有する複数の孔又は突起が2次元
的に不規則に形成されて成る非反射性光学素子。1 A plurality of holes or projections having a depth or height of approximately 1/4λ (where λ is the center wavelength of the light to be prevented from reflection) and a predetermined average radius are two-dimensionally irregular on the surface of the optical element. A non-reflective optical element formed by
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7809080A JPS574001A (en) | 1980-06-10 | 1980-06-10 | Nonreflective optical element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7809080A JPS574001A (en) | 1980-06-10 | 1980-06-10 | Nonreflective optical element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS574001A JPS574001A (en) | 1982-01-09 |
| JPH0131601B2 true JPH0131601B2 (en) | 1989-06-27 |
Family
ID=13652144
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7809080A Granted JPS574001A (en) | 1980-06-10 | 1980-06-10 | Nonreflective optical element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS574001A (en) |
Families Citing this family (11)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61236060A (en) * | 1985-04-10 | 1986-10-21 | Sumitomo Light Metal Ind Ltd | Magnetic disk device |
| JP3206713B2 (en) * | 1995-10-27 | 2001-09-10 | 株式会社巴川製紙所 | Anti-glare material and polarizing film using the same |
| JP4792639B2 (en) * | 2001-02-14 | 2011-10-12 | 住友電気工業株式会社 | Window material, optical window, and manufacturing method of window material |
| JP2003107406A (en) * | 2001-09-28 | 2003-04-09 | Akihiro Fujimura | Image display system |
| US20050069678A1 (en) * | 2003-09-25 | 2005-03-31 | General Electric Company | Joined multi functional optical device |
| JP2007322572A (en) * | 2006-05-31 | 2007-12-13 | Omron Corp | Anti-reflection optical element |
| JP2009075539A (en) * | 2007-08-28 | 2009-04-09 | Nissan Motor Co Ltd | Antireflection structure and antireflection molded body |
| JP2009175481A (en) * | 2008-01-25 | 2009-08-06 | Sumitomo Electric Ind Ltd | Antireflection optical member and optical module |
| JP2009198626A (en) * | 2008-02-20 | 2009-09-03 | Nissan Motor Co Ltd | Anti-reflective structure and anti-reflective molded body |
| US8174769B2 (en) * | 2008-04-04 | 2012-05-08 | Hewlett-Packard Development Company, L.P. | Beamsplitters with offset compensation |
| JP2013088757A (en) * | 2011-10-21 | 2013-05-13 | Semiconductor Energy Lab Co Ltd | Antireflection structure |
-
1980
- 1980-06-10 JP JP7809080A patent/JPS574001A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS574001A (en) | 1982-01-09 |
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