JPS62166301A - Polygonal prism - Google Patents
Polygonal prismInfo
- Publication number
- JPS62166301A JPS62166301A JP800086A JP800086A JPS62166301A JP S62166301 A JPS62166301 A JP S62166301A JP 800086 A JP800086 A JP 800086A JP 800086 A JP800086 A JP 800086A JP S62166301 A JPS62166301 A JP S62166301A
- Authority
- JP
- Japan
- Prior art keywords
- optical interference
- light
- refractive index
- interference filter
- wavelength
- 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
- 230000003287 optical effect Effects 0.000 claims abstract description 50
- 239000000463 material Substances 0.000 claims abstract description 27
- 239000005304 optical glass Substances 0.000 claims description 18
- 239000013078 crystal Substances 0.000 claims description 3
- 238000000151 deposition Methods 0.000 abstract 1
- 230000003449 preventive effect Effects 0.000 abstract 1
- 239000000758 substrate Substances 0.000 description 14
- 239000000853 adhesive Substances 0.000 description 8
- 230000001070 adhesive effect Effects 0.000 description 8
- 238000007740 vapor deposition Methods 0.000 description 6
- 238000000034 method Methods 0.000 description 3
- 230000003667 anti-reflective effect Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000010365 information processing Effects 0.000 description 1
- 238000005498 polishing Methods 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 238000001771 vacuum deposition Methods 0.000 description 1
Landscapes
- Optical Elements Other Than Lenses (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、波長多重光通信および光情報処理等に利用さ
れる光合分波器に用いられる多角柱プリズムに関するも
のである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a polygonal prism used in an optical multiplexer/demultiplexer used in wavelength multiplexing optical communications, optical information processing, and the like.
低屈折率物質の層と高屈折率物質の層および屈折率1と
高屈折率物質の持つ屈折率との間の屈折率を持つ物質の
層のうち、少なくとも2種類の層が交互に重なって構成
された光干渉フィルタを、光学ガラスあるいは光学結晶
からなる多角柱プリズムの側面に形成する場合、従来は
、光学ガラス基板上に真空蒸着された光干渉フィルタを
多角柱プリズムの側面に屈折率整合用接着剤で接着する
ようにしていた。At least two types of layers are alternately overlapped among a layer of a low refractive index material, a layer of a high refractive index material, and a layer of a material having a refractive index between 1 and the refractive index of the high refractive index material. When forming a structured optical interference filter on the side surface of a polygonal prism made of optical glass or optical crystal, conventionally, the optical interference filter vacuum-deposited on an optical glass substrate is index-matched on the side surface of the polygonal prism. I tried to attach it with adhesive.
今、第4図、第5図に従来の五角柱プリズムの例を示す
。この五角柱プリズムにおいては、光学ガラス基板1上
に真空蒸着により形成された光干渉フィルタ2.3およ
び反射防止膜4が、屈折率整合用接着剤5で五角柱プリ
ズム6に接着された構造となっている。Now, FIGS. 4 and 5 show examples of conventional pentagonal prisms. This pentagonal prism has a structure in which an optical interference filter 2.3 and an antireflection film 4 formed by vacuum deposition on an optical glass substrate 1 are bonded to a pentagonal prism 6 with a refractive index matching adhesive 5. It has become.
ここで、光干渉フィルタ2は、波長λ1の光を透過し、
波長λ2の光を反射する特性を有する。Here, the optical interference filter 2 transmits light of wavelength λ1,
It has a characteristic of reflecting light of wavelength λ2.
一方、光干渉フィルタ3は、波長λ1 の光を反射し、
波長λ2の光を透過する特性を有する。反射防止膜4は
波長λ、および波長λ2の両波長に対して透過する特性
を有している。On the other hand, the optical interference filter 3 reflects the light of wavelength λ1,
It has a characteristic of transmitting light with wavelength λ2. The antireflection film 4 has a characteristic of transmitting both the wavelength λ and the wavelength λ2.
第5図に示すように、中心波長λ1の光と中心波長λ2
の光が光学ガラス基板1、反射防止膜4、屈折率整合用
接着剤5を通過して、五角柱プリズム6内に入射すると
、中心波長λ1の光は屈折率整合用接着剤5、光干渉フ
ィルタ2、光学ガラス基板1を通過して出射する。一方
、中心波長λ2の光は屈折率接合用接着剤5を通過して
光干渉フィルタ2で反射された後、屈折率整合用接着剤
5、光干渉フィルタ3、光学ガラス基板1より出射する
ことになる。これにより、中心波長λ1の光と中心波長
λ2の光とが分離されるようになっている。As shown in Figure 5, light with center wavelength λ1 and light with center wavelength λ2
When the light passes through the optical glass substrate 1, the antireflection film 4, and the refractive index matching adhesive 5 and enters the pentagonal prism 6, the light with the center wavelength λ1 passes through the refractive index matching adhesive 5 and the optical interference. The light passes through a filter 2 and an optical glass substrate 1 and is emitted. On the other hand, the light with the center wavelength λ2 passes through the refractive index bonding adhesive 5 and is reflected by the optical interference filter 2, and then exits from the refractive index matching adhesive 5, the optical interference filter 3, and the optical glass substrate 1. become. Thereby, the light with the center wavelength λ1 and the light with the center wavelength λ2 are separated.
しかし、上述した従来の光干渉フィルタ基板を多角柱プ
リズムの側面に接着する構造では、光学ガラス基板1に
光干渉フィルタ2.3を蒸着により形成し、その基板1
を直接もしくは切断等の加工を施した後、屈折率整合用
接着剤5で多角柱プリズム6の側面に接着するという作
業を必要とする。そのため、光干渉フィルタ機能を有す
る多角柱プリズムは高価なものとなっていた。また、光
干渉フィルタ2.3が蒸着により形成される光学ガラス
基板1の厚さが、0.5〜1mm程度ある。However, in the above-described conventional structure in which the optical interference filter substrate is bonded to the side surface of the polygonal prism, the optical interference filter 2.3 is formed on the optical glass substrate 1 by vapor deposition.
It is necessary to bond the polygonal prism 6 directly or after processing such as cutting, to the side surface of the polygonal prism 6 with the refractive index matching adhesive 5. Therefore, polygonal prisms having an optical interference filter function have become expensive. Further, the thickness of the optical glass substrate 1 on which the optical interference filter 2.3 is formed by vapor deposition is about 0.5 to 1 mm.
このため、光干渉フィルタ2.3が蒸着により形成され
た光学ガラス基板1を多角柱プリズム6の側面に接着し
て使用する場合、光学ガラス基板1での、光の屈折によ
る出射光の位置ずれを考慮しなければならない。そのた
め、光学ガラス基板1での出射光の位置ずれ量を低減す
る方法として、光学ガラス基板1を薄く光学研暦する方
法が採用されていた。しかし、この構造では研暦工程が
加わることで、光干渉フィルタ機能を有する多角柱プリ
ズムは、さらに高価なものになってしまうという欠点が
あった。Therefore, when the optical interference filter 2.3 is used by adhering the optical glass substrate 1 formed by vapor deposition to the side surface of the polygonal prism 6, the positional shift of the emitted light due to the refraction of the light on the optical glass substrate 1 will occur. must be taken into consideration. Therefore, as a method of reducing the amount of positional deviation of the emitted light on the optical glass substrate 1, a method of optically polishing the optical glass substrate 1 to make it thinner has been adopted. However, this structure has the disadvantage that the polygonal prism having an optical interference filter function becomes even more expensive due to the addition of a research process.
本発明の目的は上述した欠点に鑑みなされたもので、光
干渉フィルタ機能を有する安価な多角柱プリズムを提供
するにある。The object of the present invention was made in view of the above-mentioned drawbacks, and is to provide an inexpensive polygonal prism having an optical interference filter function.
本発明に係わる多角柱プリズムは、低屈折率物質の層と
高屈折率物質の層および屈折率と前記高屈折率物質の持
つ屈折率との間の屈折率を持つ物質の層のうち、少なく
とも2種類の層が交互に重なって構成された光干渉フィ
ルタを、プリズム側面に直接蒸着した構成とし、もって
上述した目的を達成せんとするものである。The polygonal prism according to the present invention includes at least a layer of a low refractive index material, a layer of a high refractive index material, and a layer of a material having a refractive index between the refractive index and the refractive index of the high refractive index material. The optical interference filter, which is composed of two types of layers that are alternately stacked, is deposited directly on the side surface of a prism, thereby achieving the above-mentioned purpose.
以下、図に示す実施例を用いて本発明の詳細な説明する
。Hereinafter, the present invention will be explained in detail using embodiments shown in the drawings.
第1図は本発明に係わる多角柱プリズムの一実施例を示
す概略斜視図、第2図は同多角柱プリズムの平面図であ
る。多角柱プリズムとしては光学ガラス製の五角柱プリ
ズム7が用いられ、その側面のうち2面に光干渉フィル
タ8.9が直接蒸着により形成されている。この光干渉
フィルタ8.9は、低屈折率物質の層と高屈折率物質の
層および屈折率1と高屈折率物質の持つ屈折率との間の
屈折率をもつ物質の層のうち、少なくとも2種類の層0
重なって構成されている。光干渉フィルタ8は、波長λ
、の光を透過し、波長λ2の光を反射する特性を有する
。一方、光干渉フィルタ9は、波長λ1 の光を反射し
、波長λ2の光を透過する特性を有する。さらに、五角
柱プリズム7の入射面には、波長λ、および波長λ2の
両波長に対して反射防止となる反射防止膜10が直接蒸
着により形成されている。FIG. 1 is a schematic perspective view showing an embodiment of a polygonal prism according to the present invention, and FIG. 2 is a plan view of the same polygonal prism. A pentagonal prism 7 made of optical glass is used as the polygonal prism, and optical interference filters 8.9 are formed on two of its side surfaces by direct vapor deposition. This optical interference filter 8.9 includes at least one of a layer of a low refractive index material, a layer of a high refractive index material, and a layer of a material having a refractive index between 1 and the refractive index of the high refractive index material. 2 types of layer 0
It is composed of overlapping parts. The optical interference filter 8 has a wavelength λ
It has a characteristic of transmitting light of wavelength λ2 and reflecting light of wavelength λ2. On the other hand, the optical interference filter 9 has a characteristic of reflecting light of wavelength λ1 and transmitting light of wavelength λ2. Further, on the entrance surface of the pentagonal prism 7, an antireflection film 10 is formed by direct vapor deposition to prevent reflections at both wavelengths λ and λ2.
第2図は、第1図に示した五角柱プリズムの機能を説明
する図である。中心波長λ1の光と中心波長λ2の光が
五角柱プリズム7に反射防止膜10を通って入射すると
、中心波長λ1 の光は光干渉フィルタ8を通って出射
する。一方、中心波長λ2の光は、光干渉フィルタ8で
反射された後、光干渉フィルタ9を通って出射すること
になる。FIG. 2 is a diagram illustrating the function of the pentagonal prism shown in FIG. 1. When the light with the center wavelength λ1 and the light with the center wavelength λ2 enter the pentagonal prism 7 through the antireflection film 10, the light with the center wavelength λ1 passes through the optical interference filter 8 and exits. On the other hand, the light having the center wavelength λ2 is reflected by the optical interference filter 8 and then passes through the optical interference filter 9 and exits.
これにより、中心波長λ、の光と中心波長λ2の光とを
分離することができる。Thereby, the light having the center wavelength λ and the light having the center wavelength λ2 can be separated.
第3図は、本考案に係わる多角柱プリズムの池の実施例
を示す平面図である。多角柱プリズムとしては光学ガラ
ス製の四角柱プリズム11が用いられ、その側面の相対
する2面の一部に光干渉フィルタ12.13が直接蒸着
により形成されている。光干渉フィルタ12.13は、
低屈折率物質の層と高屈折率物質の層および屈折率1と
高屈折率物質の持つ屈折率との間の屈折率をもつ物質の
層のうち、少なくとも2種類の層が重なって構成されて
いる。光干渉フィルタ12は、波長λ3の光を透過し、
波長λ、の光を反射する特性を有する。一方、光干渉フ
ィルタ13は波長λ3の光を反射し、波長λ4の光を透
過する特性を有する。FIG. 3 is a plan view showing an embodiment of a polygonal prism pond according to the present invention. A quadrangular prism 11 made of optical glass is used as the polygonal prism, and optical interference filters 12 and 13 are formed by direct vapor deposition on parts of two opposing sides of the prism. The optical interference filter 12.13 is
At least two types of layers are overlapped among a layer of a low refractive index material, a layer of a high refractive index material, and a layer of a material having a refractive index between 1 and the refractive index of the high refractive index material. ing. The optical interference filter 12 transmits light of wavelength λ3,
It has the property of reflecting light of wavelength λ. On the other hand, the optical interference filter 13 has a characteristic of reflecting light of wavelength λ3 and transmitting light of wavelength λ4.
さらに光干渉フィルタ13が形成されている四角柱プリ
ズム11の側面と同一面には、光の入射部分だけに波長
λ3および波長λ4の両波長に対して反射防止となる反
射防止膜14が直接蒸着により形成されている。Furthermore, on the same surface as the side surface of the square prism 11 on which the optical interference filter 13 is formed, an antireflection film 14 that prevents reflection against both wavelengths λ3 and λ4 is directly deposited only on the light incident part. It is formed by
ここで、中心波長λ3の光と中心波長λ4の光が四角柱
プリズム11に反射防止膜14を通って入射すると、中
心波長λ3の光は光干渉フィルタ12を通って出射する
。一方、中心波長λ4の光は、光干渉フィルタ12で反
射された後、光干渉フィルタ13を通って出射すること
になる。これにより、中心波長λ3の光の中心波長λ、
の光とを分離することができる。Here, when the light with the center wavelength λ3 and the light with the center wavelength λ4 enter the square prism 11 through the antireflection film 14, the light with the center wavelength λ3 passes through the optical interference filter 12 and exits. On the other hand, the light having the center wavelength λ4 is reflected by the optical interference filter 12 and then passes through the optical interference filter 13 and exits. As a result, the center wavelength λ of the light with the center wavelength λ3,
can be separated from the light.
以上説明したように本発明によれば、光学ガラスもしく
は光学結晶からなる多角柱プリズムの側面に、低屈折率
物質の層と高屈折率物質の層および屈折率1と前記高屈
折率物質の持つ屈折率との間の屈折率を持つ物質の層の
うち、少なくとも2種類の層が交互に重なって構成され
た光干渉フィルタを直接蒸着した構成としたので、従来
のように光干渉フィルタを蒸着した光学ガラス基板を切
断、研磨し、プリズムの側面に屈折率整合用接着剤で接
着するという作業を不要にできるのみならず、光学ガラ
ス基板での光の屈折による出射光の位置ずれをほとんど
考慮する必要がないので、従来に比べて安価な光干渉フ
ィルタ機能を有する多角柱プリズムを提供できるという
効果を存する。As explained above, according to the present invention, a layer of a low refractive index material and a layer of a high refractive index material are provided on the side surfaces of a polygonal prism made of optical glass or optical crystal, and The optical interference filter, which is composed of alternating layers of at least two types of layers of substances with refractive indexes between the two, is directly deposited, so it is not possible to deposit the optical interference filter as in the conventional method. This not only eliminates the need to cut, polish, and bond the optical glass substrate to the side surface of the prism with a refractive index matching adhesive, but also almost eliminates the positional shift of the emitted light due to the refraction of the light on the optical glass substrate. Since there is no need to do so, it is possible to provide a polygonal prism having an optical interference filter function at a lower cost than in the past.
加えて、本発明に係わる多角柱プリズムを用いることに
より、安価な光合分波器も提供できるという効果を有す
る。In addition, by using the polygonal prism according to the present invention, it is possible to provide an inexpensive optical multiplexer/demultiplexer.
第1図は本発明に係わる多角柱プリズムの一実施例を示
す概略斜視図、第2図は同多角柱プリズムの平面図、第
3図は本発明に係わる多角柱プリズムの他の実施例を示
す平面図、第4図は従来の多角柱プリズムの一例を示す
概略斜視図、第5図は同多角柱プリズムの平面図である
。
7・・・・・・五角柱プリズム、
8.9・・・・・・光干渉フィルタ、
10・・・・・・反射防止膜、
11・・・・・・四角柱プリズム、
12.13・・・・・・光干渉フィルタ、14・・・・
・・反射防止膜。
出 願 人
日本電気株式会社FIG. 1 is a schematic perspective view showing one embodiment of the polygonal prism according to the present invention, FIG. 2 is a plan view of the polygonal prism, and FIG. 3 is a schematic perspective view showing another embodiment of the polygonal prism according to the present invention. 4 is a schematic perspective view showing an example of a conventional polygonal prism, and FIG. 5 is a plan view of the same polygonal prism. 7... Pentagonal prism, 8.9... Optical interference filter, 10... Anti-reflection film, 11... Quadrilateral prism, 12.13. ...Optical interference filter, 14...
...Anti-reflective film. Applicant: NEC Corporation
Claims (1)
おいて、低屈折率物質の層と高屈折率物質の層および屈
折率1と前記高屈折率物質の持つ屈折率との間の屈折率
をもつ物質の層のうち、少なくとも2種類の層が交互に
重なって構成された光干渉フィルタを、プリズム側面に
直接蒸着したことを特徴とする多角柱プリズム。In a polygonal prism made of optical glass or optical crystal, a layer of a low refractive index material, a layer of a high refractive index material, and a layer of a material having a refractive index between 1 and the refractive index of the high refractive index material. A polygonal prism characterized in that an optical interference filter composed of at least two types of layers alternately stacked is directly deposited on a side surface of the prism.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP800086A JPS62166301A (en) | 1986-01-20 | 1986-01-20 | Polygonal prism |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP800086A JPS62166301A (en) | 1986-01-20 | 1986-01-20 | Polygonal prism |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS62166301A true JPS62166301A (en) | 1987-07-22 |
Family
ID=11681114
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP800086A Pending JPS62166301A (en) | 1986-01-20 | 1986-01-20 | Polygonal prism |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62166301A (en) |
-
1986
- 1986-01-20 JP JP800086A patent/JPS62166301A/en active Pending
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