JPS5960407A - Optical filter - Google Patents
Optical filterInfo
- Publication number
- JPS5960407A JPS5960407A JP17234682A JP17234682A JPS5960407A JP S5960407 A JPS5960407 A JP S5960407A JP 17234682 A JP17234682 A JP 17234682A JP 17234682 A JP17234682 A JP 17234682A JP S5960407 A JPS5960407 A JP S5960407A
- Authority
- JP
- Japan
- Prior art keywords
- film
- optical filter
- glass substrate
- refractive index
- tio2
- 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
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B5/00—Optical elements other than lenses
- G02B5/20—Filters
- G02B5/28—Interference filters
- G02B5/285—Interference filters comprising deposited thin solid films
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Surface Treatment Of Optical Elements (AREA)
- Optical Filters (AREA)
Abstract
Description
【発明の詳細な説明】
発明の技術分野
本発明は、光通信用分波器等の基本構成要素のTioz
、S 1()z系の誘電体多層膜を有する帯域通過型の
光学フィルタに関するものである。DETAILED DESCRIPTION OF THE INVENTION Technical Field of the Invention The present invention relates to Tioz
, S1()z-based dielectric multilayer film.
従来技術と問題点
TiO2,5i02系の誘電体多層膜を有する帯域通過
型の光学フィルタは、一般に、ガラス基板上に電子ビー
ム蒸着等の技術によりTiO2゜S i O2を交互に
積層して形成するものであった。例えば第1図に示すよ
うに、ガラス基板l上に′I’ + 02膜2を蒸着し
、ソノ上に5I02膜3を蒸着し、これを交互に繰り返
して多層膜を形成し、最外層は第1層と同様なTiO2
膜2とするものである。各膜の厚さは光の波長をλとす
ると、λ/4とするものである(但し、一部の5i02
脱はλ/2とする)。Prior Art and Problems A band-pass optical filter having a TiO2, 5i02-based dielectric multilayer film is generally formed by alternately stacking TiO2°S i O2 on a glass substrate using techniques such as electron beam evaporation. It was something. For example, as shown in FIG. 1, an 'I'+02 film 2 is deposited on a glass substrate l, a 5I02 film 3 is deposited on a glass substrate, and this process is repeated alternately to form a multilayer film, with the outermost layer being TiO2 similar to the first layer
This is the film 2. The thickness of each film is λ/4, where λ is the wavelength of light (However, for some 5i02
).
前記構成の光学フィルタをそのまま分波器用として用い
る場合は、光学的に非対称であることにより、分波器に
要求される高精度の特性を得ることができないものであ
る。そこで、従来は、第2図に示すように、最外層膜上
に接着剤4よりガラス基板5を設け、誘電体多層膜をガ
ラス基板1゜5で挾む構成とし、光学的な対称性を与え
て通過域の特性を改善するものであった。If the optical filter having the above configuration is used as it is for a demultiplexer, it will not be possible to obtain the highly accurate characteristics required for the demultiplexer due to the optical asymmetry. Therefore, conventionally, as shown in FIG. 2, a glass substrate 5 is provided on the outermost layer film using an adhesive 4, and the dielectric multilayer film is sandwiched between glass substrates 1.5 degrees to achieve optical symmetry. This was to improve the characteristics of the passband.
第3図は、前記第1図と第2図との構成による特性曲線
図であり、曲線Aは第り図の構成9曲線Bは第2図の構
成の場合の一例の特性を示し、第2図の構成のようにガ
ラス基板5を設けることにより、通過域の特性が改善さ
れることが判る。FIG. 3 is a characteristic curve diagram for the configuration shown in FIGS. 1 and 2. Curve A shows the characteristic of the configuration shown in FIG. It can be seen that by providing the glass substrate 5 as in the configuration shown in FIG. 2, the characteristics of the passband are improved.
しかし、接着剤4を使用する為、信頼性の問題が生じる
と共に、均一の厚さの接着剤4でガラス基板5を最外層
膜上に接着する作業が容易でない欠点があった。However, since the adhesive 4 is used, there are problems with reliability and it is not easy to bond the glass substrate 5 onto the outermost film with the adhesive 4 having a uniform thickness.
発明の目的
本発明り、ガラス基板を接着することなく、フィルタ特
性を改善し得るようにすることを目的とするものである
。以下実施例について詳細に説明する。OBJECTS OF THE INVENTION It is an object of the present invention to make it possible to improve filter characteristics without bonding glass substrates. Examples will be described in detail below.
発明の実施例
第4図は本発明の実施例の概略断面図であり、第1図と
同一部分は同一符号で示す。ガラス基板1上にT i
O2膜2と5iO2N!f!3とを交互に積層すること
は従来例と同様であるが、空気側の最外層となるSiO
2膜3上にs i3N、膜6を蒸着等により形成するも
のである。TiO2膜2の屈折率は2.3であり、5i
02膜3の屈折率は1.46であるから、それらの屈折
率の中間的な屈折率の1.8〜1.9の屈折率のS i
3N4膜6を形成するものである。それによりガラス
基板を最外層に接着した第2図の構成の光学フィルタと
同程度或いはそれ以上の特性の光学フィルタを得ること
ができることを、シュミレーションにより確認された。Embodiment of the Invention FIG. 4 is a schematic sectional view of an embodiment of the invention, and the same parts as in FIG. 1 are designated by the same reference numerals. Ti on the glass substrate 1
O2 membrane 2 and 5iO2N! f! 3 and 3 are stacked alternately as in the conventional example, but the outermost layer on the air side is SiO
A Si3N film 6 is formed on the second film 3 by vapor deposition or the like. The refractive index of the TiO2 film 2 is 2.3, and 5i
Since the refractive index of the 02 film 3 is 1.46, S i with a refractive index of 1.8 to 1.9, which is an intermediate refractive index between those refractive indexes.
A 3N4 film 6 is formed. It has been confirmed through simulations that it is possible to obtain an optical filter with characteristics comparable to or better than the optical filter having the configuration shown in FIG. 2 in which a glass substrate is bonded to the outermost layer.
第5図は光学フィルタの特性曲線図であり、曲線Bは第
2図の構成の従来例の光学フィルタの特性、曲線C,D
は第4図の構成の本発明の実施例の光学フィルタについ
て、Si3N4膜として屈折率が2及び1.8の場合の
特性を示すものである。通過域損失を改善する点のみを
考えると、誘電体多層膜の最外層に形成するS i 3
N 4膜の屈折率は1.46〜2.3の範囲内で選定
することができるが、帯域幅が狭くなるから、最適な屈
折率としては、1.8〜1.9程度が好適である。FIG. 5 is a characteristic curve diagram of the optical filter, curve B is the characteristic of the conventional optical filter having the configuration shown in FIG. 2, curves C and D are
4 shows the characteristics of the optical filter according to the embodiment of the present invention having the structure shown in FIG. 4 when the Si3N4 film has a refractive index of 2 and 1.8. Considering only the improvement of passband loss, Si 3 formed in the outermost layer of the dielectric multilayer film
The refractive index of the N4 film can be selected within the range of 1.46 to 2.3, but since the bandwidth becomes narrow, the optimal refractive index is preferably about 1.8 to 1.9. be.
又s 13N、膜6の厚さは、λ/4以上であれば良い
ので、製作も容易である。Further, since the thickness of the film 6 only needs to be λ/4 or more, manufacturing is easy.
発明の詳細
な説明したように、本発明は、T i O2膜2とS
i O2膜3とを交互にガラス基板1上に形成した誘電
体多層膜の最外層にS i 3 N 4膜6を形成した
ものであるから、誘電体多層膜の最外層にガラス基板を
接着する従来例に比較して、接着剤を用いないことによ
り信頼性を向上することができる利点があり、又誘電体
多層膜の形成と同様な手段で形成することができるから
、製作が容易となる利点がある。As described in detail, the present invention includes a TiO2 film 2 and an S
Since the Si 3 N 4 film 6 is formed on the outermost layer of the dielectric multilayer film in which the iO2 film 3 is alternately formed on the glass substrate 1, the glass substrate is bonded to the outermost layer of the dielectric multilayer film. Compared to conventional methods, this method has the advantage of improving reliability by not using adhesives, and is easy to manufacture because it can be formed using the same method as that used for forming dielectric multilayer films. There are some advantages.
第1図及び第2図は従来例の光学フィルタの概略断面図
、m3図は第1図及び第2図の構成の光学フィルタの特
性曲線図、第4図は本発明の実施例の概略断面図、第5
図は従来例の光学フィルりと本発明の実施例の光学フィ
ルタの一例の特性曲線図である。
lはガラス基板、2.3は誘電体多層膜を構成する”I
” + 02股及び3i02膜、6は3 i 3 N
4膜である。
特許出願人 富士通株式会社
代理人弁理士 玉蟲久五部 外3名
第 2 図
第4図Figures 1 and 2 are schematic cross-sectional views of conventional optical filters, Figure m3 is a characteristic curve diagram of the optical filter having the configuration shown in Figures 1 and 2, and Figure 4 is a schematic cross-sectional view of an embodiment of the present invention. Figure, 5th
The figure is a characteristic curve diagram of an example of an optical filter of a conventional example and an optical filter of an embodiment of the present invention. l is the glass substrate, 2.3 is "I" constituting the dielectric multilayer film.
” + 02 crotch and 3i02 membrane, 6 is 3 i 3 N
There are 4 membranes. Patent applicant Fujitsu Ltd. Representative Patent Attorney Gobe Tamamushi and 3 others Figure 2 Figure 4
Claims (1)
学フィルタに於て、空気側の最外層に、前記’r i
02と5102との欣の屈折率との間に相当する屈折率
のSi3N4膜を形成したことを特徴とする光学フィル
タ。In an optical filter having a TiO2, Si02-based dielectric optical multilayer film, the above-mentioned 'r i
1. An optical filter comprising a Si3N4 film having a refractive index between 02 and 5102.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17234682A JPS5960407A (en) | 1982-09-29 | 1982-09-29 | Optical filter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17234682A JPS5960407A (en) | 1982-09-29 | 1982-09-29 | Optical filter |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS5960407A true JPS5960407A (en) | 1984-04-06 |
Family
ID=15940201
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17234682A Pending JPS5960407A (en) | 1982-09-29 | 1982-09-29 | Optical filter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5960407A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0573163A3 (en) * | 1992-06-05 | 1995-08-23 | Optical Coating Laboratory Inc | Enhanced durability optical stack such as a mirror and a process for forming the stack. |
-
1982
- 1982-09-29 JP JP17234682A patent/JPS5960407A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0573163A3 (en) * | 1992-06-05 | 1995-08-23 | Optical Coating Laboratory Inc | Enhanced durability optical stack such as a mirror and a process for forming the stack. |
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