JPS63218902A - Optical fiber decreased in ripple - Google Patents

Optical fiber decreased in ripple

Info

Publication number
JPS63218902A
JPS63218902A JP5253087A JP5253087A JPS63218902A JP S63218902 A JPS63218902 A JP S63218902A JP 5253087 A JP5253087 A JP 5253087A JP 5253087 A JP5253087 A JP 5253087A JP S63218902 A JPS63218902 A JP S63218902A
Authority
JP
Japan
Prior art keywords
layers
refractive index
layer
dielectric material
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.)
Pending
Application number
JP5253087A
Other languages
Japanese (ja)
Inventor
Shinji Uchida
真司 内田
Takaaki Tomita
孝明 富田
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP5253087A priority Critical patent/JPS63218902A/en
Publication of JPS63218902A publication Critical patent/JPS63218902A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain an optical filter which has fewer ripples and permits easy prepn. by using specific film configuration. CONSTITUTION:The number of the total layers is assumed to be N layers, then the odd layers counted from a substrate are dielectric material layers (TiO2 layers) having a high refractive index and the even layers are dielectric material layers (SiO2 layers) having a low refractive index. The alternate multi- layered films are formed by shifting the optical film thicknesses of the 1st layer, 3rd layer, (N-2)th layer and N-th layer which are the dielectric material layers having the high refractive index by about the same degrees from 1/3 of a design reference wavelength lambda0, and setting the optical film thicknesses of the other dielectric material layers having the refractive index at lambda0/3 and the optical film thicknesses of the dielectric material layers having the low refractive index at lambda0/6. The optical fiber having the fewer ripples in transmission band is thereby obtd.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、光学装置等に用いられる光学フィルターに関
する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to an optical filter used in optical devices and the like.

従来の技術 三板カメラ用三色分解プリズムには、色分離フィルター
等の光学多層膜が使用されている。例えば、赤反射フィ
ルター、青反射フィルター等がこれにあたる。
BACKGROUND OF THE INVENTION Optical multilayer films such as color separation filters are used in three-color separation prisms for three-panel cameras. For example, a red reflective filter, a blue reflective filter, etc. fall under this category.

三色分解プリズムは入射した光を青反射フィルターを用
いて青色光を反射させ、次に残りの光より赤色光を反射
させ青色光・赤色光・緑色光に分離する光学部品である
A three-color separation prism is an optical component that uses a blue reflection filter to reflect the blue light that enters the prism, and then reflects the red light from the remaining light to separate it into blue, red, and green light.

従ってその反射特性、透過特性が色特性に重要な影響を
与えるわけで、青赤反射フィルターの光学特性が悪けれ
ば、緑色特性にも悪影響を及ぼす。
Therefore, the reflection characteristics and transmission characteristics have an important influence on the color characteristics, and if the optical characteristics of the blue-red reflective filter are poor, the green characteristics will also be adversely affected.

従来よりこれら青反射フィルター、赤反射フィルターは
誘電体多層膜を用いて実現してきた。誘電体多層膜は高
屈折率物質と低屈折率物質を真空蒸着法を用いて交互に
蒸着し実現できる。
Conventionally, these blue reflection filters and red reflection filters have been realized using dielectric multilayer films. A dielectric multilayer film can be realized by alternately depositing a high refractive index material and a low refractive index material using a vacuum deposition method.

蒸着物質としてはTλ0□、 5i02等が主に用いら
れてきた。赤反射フィルターの一例を第9図に示す。膜
構成は、基板より数えて奇数層がT工02であり偶数層
が5IO2である。各層の光学的膜厚は設計波長をλ。
Tλ0□, 5i02, etc. have been mainly used as vapor deposition substances. An example of a red reflection filter is shown in FIG. Regarding the film structure, the odd numbered layers counting from the substrate are T-02 and the even numbered layers are 5IO2. The optical thickness of each layer is λ based on the design wavelength.

とすると、λ。/4であり、入射角度はθ=13°であ
る。
Then, λ. /4, and the incident angle is θ=13°.

発明が解決しようとする問題点 このような光学多層膜(光学フィルター)を三色分解プ
リズム等の色分解光学系に用いた際、問題となる点を説
明する。
Problems to be Solved by the Invention Problems that arise when such an optical multilayer film (optical filter) is used in a color separation optical system such as a three-color separation prism will be explained.

第9図中、λ= 580 n m以下の透過領域に大き
なリップルが生じている。これは、赤反射フィルター、
青反射フィルターを用いて、緑色光を取り出す場合に重
要な影響を与える。すなわち、赤色光は本フィルターに
て十分分離できるが、透過帯(緑色波長帯域)にリップ
ルがあるためこの光学特性が直接緑色の光学特性に悪影
響を与えてしまうのである。この膜構成は、高屈折率物
質Hと低屈折率物質りの光学的膜厚が1=1の場合であ
るが、H:L=3:1の場合も同様で、透過帯のリップ
ルを取り除くことはできなかった。
In FIG. 9, large ripples occur in the transmission region below λ=580 nm. This is a red reflective filter,
This has an important effect when extracting green light using a blue reflective filter. That is, although red light can be sufficiently separated by this filter, since there is a ripple in the transmission band (green wavelength band), this optical characteristic directly affects the optical characteristic of green color. This film configuration is for the case where the optical film thickness of the high refractive index material H and the low refractive index material is 1=1, but it is also the same when H:L=3:1, which removes ripples in the transmission band. I couldn't do that.

本発明は、かかる点に鑑みてなされたもので、透過帯の
リップルが少ない色分離フィルターを提供することを目
的としている。
The present invention has been made in view of this point, and an object of the present invention is to provide a color separation filter with less ripples in the transmission band.

問題点を解決するための手段 上記問題点を解決する本発明の技術的な手段は。Means to solve problems The technical means of the present invention to solve the above problems is as follows.

全層数をN層とすると基板から数えて奇数層は高屈折率
の誘電体物質層で、偶数層は低屈折率の誘電体層であり
、高屈折率の誘電体物質層である第1層、第3層、第N
−2層、第N層の光学的膜厚を設計基準波長λ。の狛よ
り同程度ずらし、前記以外の高屈折率の誘電体物質層の
光学的膜厚をλ。力任屈折率の誘電体物質層の光学的膜
厚をλ。/6とした交互多層膜とすることである。
Assuming that the total number of layers is N, the odd-numbered layers counting from the substrate are dielectric material layers with a high refractive index, the even-numbered layers are dielectric material layers with a low refractive index, and the first layer is a dielectric material layer with a high refractive index. layer, third layer, Nth layer
- The optical thickness of the second layer and the Nth layer is set to the design reference wavelength λ. The optical thickness of the dielectric material layer with a high refractive index other than the above is λ. The optical thickness of the dielectric material layer with power refractive index is λ. /6 and an alternating multilayer film.

作用 本発明は、上記薄膜系を用いることにより、透過帯にお
いてリップルの少ない光学フィルターが得られるもので
ある。
Function The present invention provides an optical filter with few ripples in the transmission band by using the above-mentioned thin film system.

実施例 全膜層数が19層で基板から数えて奇数層が高屈折率物
質のTiO2層であり、偶数層が低屈折率物質のsio
 2層である赤反射フィルターの透過率特性を第1図に
示す。
Example The total number of layers is 19, and the odd-numbered layers counting from the substrate are TiO2 layers of a high refractive index material, and the even-numbered layers are SIO layers of a low refractive index material.
Figure 1 shows the transmittance characteristics of a two-layer red reflective filter.

設計基準波長はλ。=esonmであり、入射角度は1
3°、 Ti02(7)屈折率nu = 2.3o 、
 5in2の屈折率はnL:1.46.基板の屈折率は
ng=1.61である。
The design standard wavelength is λ. = esonm, and the incident angle is 1
3°, Ti02(7) refractive index nu = 2.3o,
The refractive index of 5in2 is nL: 1.46. The refractive index of the substrate is ng=1.61.

縦軸が透過率(単位:チ)、横軸が波長(単位:nm)
である。
The vertical axis is transmittance (unit: h), the horizontal axis is wavelength (unit: nm)
It is.

本膜構成を第2図に示す。第1層、第3層、第緑色光領
域のリップルが大幅に低減化されていることかわかる。
The structure of this membrane is shown in Figure 2. It can be seen that the ripples in the first layer, third layer, and green light region are significantly reduced.

青領域に若干のリップルが生じているが、三色分角プリ
ズムでは、まず青反射フィルターにより青色光領域の光
を分離するので、リップルが生じていても特に問題はな
い。
Although some ripples occur in the blue region, the tricolor separation prism first separates the light in the blue light region using a blue reflection filter, so there is no particular problem even if the ripples occur.

第3図に基板の屈折率がng =+ 1.51  +第
4図にng=1.80の場合の透過率特性を示す。
FIG. 3 shows the transmittance characteristics when the refractive index of the substrate is ng=+1.51 and FIG. 4 shows the transmittance characteristics when ng=1.80.

緑色光領域のリップルが少ない良好な分光特性が実現で
きていることがわかる。本膜構成は、たとえ基板の屈折
率がかわったとしても良好な透過率特性を実現できるも
のであり非常に有用である。
It can be seen that good spectral characteristics with few ripples in the green light region have been achieved. This film configuration is very useful because it can achieve good transmittance characteristics even if the refractive index of the substrate changes.

第6図に全層数がB層の場合の透過率特性を示す。膜構
成は第1層、第3層、第11層、第13層の光学的膜厚
は、2.18X”、偶数層がある。形成物質としてTi
O2(nH= 2.30 )、SiO□(nL==1.
46)を用いている。設計波長はλo”680nm、入
射角度はθ=13°、基板の屈折率はng = 1.6
1である。
FIG. 6 shows the transmittance characteristics when the total number of layers is B layers. The optical thickness of the first, third, eleventh, and thirteenth layers is 2.18X'', and there are even layers.The forming material is Ti.
O2 (nH=2.30), SiO□ (nL==1.
46) is used. The design wavelength is λo” 680 nm, the incident angle is θ = 13°, and the refractive index of the substrate is ng = 1.6.
It is 1.

層数が13層の場合も同様に透過帯のリップルが大幅に
低減できる。
Similarly, when the number of layers is 13, ripples in the transmission band can be significantly reduced.

第6図に全層数が26層の場合の透過率特性を示す。第
1図の19層、第4図の13層の場合と同様、リップル
が大幅に改善されている。
FIG. 6 shows the transmittance characteristics when the total number of layers is 26. As in the case of the 19 layers in FIG. 1 and the 13 layers in FIG. 4, ripples are significantly improved.

従って、層数が変わったとしても、第1層、第3層、第
N−2層、第N層の光学的膜厚を2.00することがで
きる。
Therefore, even if the number of layers changes, the optical thicknesses of the first layer, the third layer, the N-2 layer, and the N-th layer can be set to 2.00.

一般に層数が変われば、反射帯の反射率、立上り特性が
変わる。層数が増す程反射率は増大するし、立上りはよ
り急峻になる。したがって所望の特性に応じた層数を決
定してやればよい。また反射帯の幅は使用する物質の屈
折率比1丁に応じて変化する。屈折率比11が増大すれ
ば、反射帯の幅も増大する。高屈折率物質としては他に
zro2 。
Generally, if the number of layers changes, the reflectance and rise characteristics of the reflection band will change. As the number of layers increases, the reflectance increases and the rise becomes steeper. Therefore, the number of layers may be determined depending on desired characteristics. Furthermore, the width of the reflection band varies depending on the refractive index ratio of the material used. As the refractive index ratio 11 increases, the width of the reflection band also increases. Another high refractive index material is zro2.

ZrTiO4,ZnS 、 0e02低屈折率物質とし
てMgF、、等がある。本発明は、これら物質でも有用
でリップルを低減化した色分離フィルターを実現できる
Examples of low refractive index materials include ZrTiO4, ZnS, and MgF. The present invention can realize a color separation filter that is useful even with these materials and has reduced ripples.

第7図に入射角度がθ=0の場合、第8図にθ=300
の場合を示す。膜層数は19層で高屈折率物質としてT
iO2、低屈折率物質として5102を用いている。
If the angle of incidence is θ = 0 in Figure 7, then θ = 300 in Figure 8.
The case is shown below. The number of layers is 19, and T is used as a high refractive index material.
iO2 and 5102 are used as the low refractive index material.

本発明の膜構成は、角度がかわっても有用であることが
わかる。
It can be seen that the membrane configuration of the present invention is useful even at different angles.

一般に設計波長の大小に応じて反射帯領域(本実施例の
場合は赤色光)がシフトする。
Generally, the reflection band region (red light in this example) shifts depending on the size of the design wavelength.

壕だ角度の増大とともに、反射帯域は短波長側にシフト
する。したがって所望の反射帯幅9反射領域、入射角度
に応じて成膜物質、設計波長1層数を決定し、第1層、
第3層、第N−2層、第N層の高屈折率物質の光学的膜
厚を2.OX−gλ0からずらすことにより、リップル
を低減化した良好な膜特性が実現できる。
As the trench angle increases, the reflection band shifts toward shorter wavelengths. Therefore, the film forming material and the number of layers per design wavelength are determined according to the desired reflection band width 9 reflection area and the incident angle, and the first layer,
The optical thickness of the high refractive index material of the third layer, the N-2 layer, and the N-th layer is 2. By shifting from OX-gλ0, good film characteristics with reduced ripples can be achieved.

この膜構成は、将来の大容量メモリとして注目されてい
る書換型光ディスク装置の光学ヘッド等に用いられる2
波長分離フィルターにも有用である。すなわち、波長λ
。中7801mの光を透過させ、波長λ0中830nm
の光を反射させるフィルターである。
This film structure is used in optical heads of rewritable optical disk devices, which are attracting attention as future large-capacity memories.
Also useful for wavelength separation filters. That is, the wavelength λ
. Transmits light of 7801 m in wavelength, 830 nm in wavelength λ0
It is a filter that reflects light.

光学ヘッドにおいては、λ。キ7801mの光の透過率
の高効率化、高安定性が要望されており、本発明のリッ
プルを低減した光学多層膜の膜構成は非常に有用である
In optical heads, λ. There is a demand for high efficiency and high stability in the light transmittance of Ki7801m, and the film structure of the optical multilayer film with reduced ripples of the present invention is very useful.

この膜構成を用いれば、高屈折率物質の光学的λ0 膜厚は2.0OXHと、これよりずらした第1層。If this film configuration is used, the optical λ0 of the high refractive index material The film thickness is 2.0OXH, and the first layer is shifted from this.

第3層、第H−2層、第N層の光学的膜厚と、低λ0 屈折率物質の1.00 X−1iとの計3つの光学的膜
厚の組み合わせで実現できることになる。
This can be achieved by combining a total of three optical thicknesses: the optical thicknesses of the third layer, H-2 layer, and Nth layer, and 1.00 X-1i of the low λ0 refractive index material.

このことは実際の薄膜形成時の膜厚設定の際に非常に有
用であり、膜厚設定のわずられしさを犬′幅に低限化で
きるものである。
This is very useful when setting the film thickness during actual thin film formation, and the difficulty in setting the film thickness can be reduced to within a dog's width.

発明の効果 以上述べてきたように、本発明の膜構成を用いることに
よりリップルが大幅に低減でき、また、製作の容易な光
学フィルターを実現できる。
Effects of the Invention As described above, by using the film structure of the present invention, ripples can be significantly reduced and an optical filter that is easy to manufacture can be realized.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、本発明の一実施例における光学フィルターの
透過率特性図、第2図は同フィルターの横型図、第3図
は基板の屈折率がngl、61の場合の透過率特性図、
第4図はng=1.80の透過率特性図、第5図は膜層
数が13層の時の透過率特性図、第6図は25層の時の
透過率特性図、第7図は入射角がθ=0 の時の透過率
特性図、第8図はθ=30のときの透過率特性図、第9
図は従来の光学フィルターの透過率特性図である。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 WAVELENCrTH(fL=r=)第2図 :jr、3図 レノ’AVELENcrTHtam) 第4図 WAVELENC7TH(a<) 第5図 WAVELENeTHmn−) 第6図 WAVELENGTH(fL傾p ;17図 WAVELEN(rTH(=cm) 第8図 WAVELENCrTH(?LfrL)第9図
FIG. 1 is a transmittance characteristic diagram of an optical filter according to an embodiment of the present invention, FIG. 2 is a horizontal view of the same filter, and FIG. 3 is a transmittance characteristic diagram when the refractive index of the substrate is ngl, 61.
Figure 4 is a transmittance characteristic diagram when ng=1.80, Figure 5 is a transmittance characteristic diagram when the number of film layers is 13, Figure 6 is a transmittance characteristic diagram when the number of film layers is 25, and Figure 7 is a transmittance characteristic diagram when the number of film layers is 13. is a transmittance characteristic diagram when the incident angle is θ = 0, Fig. 8 is a transmittance characteristic diagram when θ = 30, and Fig. 9 is a transmittance characteristic diagram when the incident angle is θ = 0.
The figure is a transmittance characteristic diagram of a conventional optical filter. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure WAVELENCrTH (fL=r=) Figure 2: jr, Figure 3 Reno'AVELENcrTHtam) Figure 4 WAVELENC7TH (a<) Figure 5 WAVELENeTHmn-) Figure 6 WAVELENGTH (fL slope p; Figure 17 WAVELEN (rTH (= cm) Fig. 8 WAVELENCrTH(?LfrL) Fig. 9

Claims (1)

【特許請求の範囲】[Claims] 基板とその基板上に成膜された誘電体多層膜と、その上
に接着された基板とを備え、全層数をN層とすると基板
から数えて奇数層は高屈折率の誘電体物質層であり、偶
数層は、低屈折率の誘電体層であり、高屈折率の誘電体
物質層である第1層、第3層、第N−2層、第N層の光
学的膜厚を設計基準波長λ_0の1/3から同程度ずら
し、前記以外の高屈折率の誘電体物質層の光学的膜厚を
λ_0/3、低屈折率の誘電体物質層の光学的膜厚をλ
_0/6としたリップルを低減したフィルター。
It is equipped with a substrate, a dielectric multilayer film formed on the substrate, and a substrate bonded thereon.If the total number of layers is N, odd-numbered layers counting from the substrate are dielectric material layers with a high refractive index. The even-numbered layers are dielectric layers with a low refractive index, and the optical thicknesses of the first layer, the third layer, the N-2 layer, and the N-th layer are dielectric layers with a high refractive index. Shift the same amount from 1/3 of the design standard wavelength λ_0, set the optical thickness of the dielectric material layer with a high refractive index other than the above to λ_0/3, and set the optical thickness of the dielectric material layer with a low refractive index to λ
A filter with reduced ripple of _0/6.
JP5253087A 1987-03-06 1987-03-06 Optical fiber decreased in ripple Pending JPS63218902A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5253087A JPS63218902A (en) 1987-03-06 1987-03-06 Optical fiber decreased in ripple

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5253087A JPS63218902A (en) 1987-03-06 1987-03-06 Optical fiber decreased in ripple

Publications (1)

Publication Number Publication Date
JPS63218902A true JPS63218902A (en) 1988-09-12

Family

ID=12917309

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5253087A Pending JPS63218902A (en) 1987-03-06 1987-03-06 Optical fiber decreased in ripple

Country Status (1)

Country Link
JP (1) JPS63218902A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5303319A (en) * 1992-12-28 1994-04-12 Honeywell Inc. Ion-beam deposited multilayer waveguides and resonators

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5303319A (en) * 1992-12-28 1994-04-12 Honeywell Inc. Ion-beam deposited multilayer waveguides and resonators

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