JPH03135512A - Faraday rotator - Google Patents
Faraday rotatorInfo
- Publication number
- JPH03135512A JPH03135512A JP27416489A JP27416489A JPH03135512A JP H03135512 A JPH03135512 A JP H03135512A JP 27416489 A JP27416489 A JP 27416489A JP 27416489 A JP27416489 A JP 27416489A JP H03135512 A JPH03135512 A JP H03135512A
- Authority
- JP
- Japan
- Prior art keywords
- optical axis
- optical
- degrees
- incidence
- optical isolator
- 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 41
- 230000010287 polarization Effects 0.000 claims abstract description 16
- 238000000926 separation method Methods 0.000 claims description 9
- 239000004065 semiconductor Substances 0.000 description 8
- 230000000694 effects Effects 0.000 description 4
- GWEVSGVZZGPLCZ-UHFFFAOYSA-N Titan oxide Chemical compound O=[Ti]=O GWEVSGVZZGPLCZ-UHFFFAOYSA-N 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 2
- BGPVFRJUHWVFKM-UHFFFAOYSA-N N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] Chemical compound N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] BGPVFRJUHWVFKM-UHFFFAOYSA-N 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 239000013307 optical fiber Substances 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 230000008054 signal transmission Effects 0.000 description 1
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、光アイソレータ等に使用されるファラデー回
転子に関するものである。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a Faraday rotator used in optical isolators and the like.
従来の技術
半導体レーザを光通信等の光信号伝達系の光源として用
いる場合、半導体レーザからの出射光の一部が、伝送路
あるいは伝送用光学部品の各接続部で反射して、半導体
レーザの発振特性の不安定化や雑音増加を引き起こす原
因となる。この反射戻り光が半導体レーザに帰還するの
を防止するために、一般的に光アイソレータが使用され
ている。ファラデー回転子はファラデー効果を利用した
旋光素子であり、非相反性を持つことから光アイソレー
タに使用されている。Conventional Technology When a semiconductor laser is used as a light source in an optical signal transmission system such as optical communication, a portion of the light emitted from the semiconductor laser is reflected at the transmission line or at each connection of the transmission optical components, causing the semiconductor laser to emit light. This causes oscillation characteristics to become unstable and noise to increase. An optical isolator is generally used to prevent this reflected return light from returning to the semiconductor laser. A Faraday rotator is an optical rotation element that utilizes the Faraday effect, and is used in optical isolators because it has non-reciprocity.
従来の光アイソレータは、例えば第3図に示すように、
偏光子1.磁気光学素子2.検光子3および磁石4を備
えた構成をとる。光アイソレータの原理は、第4図(a
lに示すように、半導体レーザからの出射光5aは、ま
ず偏光子1を通過して直線偏光5bとなる。続いて飽和
磁界H中の磁気光学素子2を通過する際に、その偏光方
向は45度回転され、その直線偏光5Cは偏光子1と4
5度の角度に配置した検光子3を通過して直線偏光5d
となる。逆に、第4図(b)に示すように、反射戻り光
6aはまず、検光子3を通過して直線偏光6bとなる。A conventional optical isolator, for example, as shown in FIG.
Polarizer 1. Magneto-optical element 2. The configuration includes an analyzer 3 and a magnet 4. The principle of an optical isolator is shown in Figure 4 (a
As shown in FIG. 1, the emitted light 5a from the semiconductor laser first passes through the polarizer 1 and becomes linearly polarized light 5b. Subsequently, when passing through the magneto-optical element 2 in the saturation magnetic field H, its polarization direction is rotated by 45 degrees, and the linearly polarized light 5C is transmitted through the polarizers 1 and 4.
The linearly polarized light 5d passes through the analyzer 3 placed at an angle of 5 degrees.
becomes. Conversely, as shown in FIG. 4(b), the reflected return light 6a first passes through the analyzer 3 and becomes linearly polarized light 6b.
続いて飽和磁界H中の磁気光学素子2を通過する際に、
ファラデー効果の持つ非相反性により、偏光方向はさら
に45度回転され、直線偏光6Cとなり偏光子1と直交
するために通過できなくなる。以上のような原理で、反
射戻り光が半導体レーザに帰還するのを防止することが
できる。Subsequently, when passing through the magneto-optical element 2 in the saturation magnetic field H,
Due to the non-reciprocity of the Faraday effect, the polarization direction is further rotated by 45 degrees to become linearly polarized light 6C, which is perpendicular to the polarizer 1 and cannot pass through. Based on the principle described above, reflected return light can be prevented from returning to the semiconductor laser.
発明が解決しようとする課題
このような従来の光アイソレータの構成では、偏光子お
よび検光子が必要となるため、ケースに収納する際に内
部に余分な空間が生じて、光アイソレータの小型化には
限界があった。さらに、組み立ての際に、光の偏光方向
の微調整が必要になるという欠点があった。Problems to be Solved by the Invention In such a conventional optical isolator configuration, a polarizer and an analyzer are required, which creates extra space inside the case and makes it difficult to downsize the optical isolator. had its limits. Furthermore, there is a drawback that fine adjustment of the polarization direction of the light is required during assembly.
本発明はこのような課題を解決するもので、小型で組み
立てが容易な光アイソレータの提供を目的とするもので
ある。The present invention solves these problems and aims to provide an optical isolator that is small and easy to assemble.
課題を解決するための手段
本発明は前記課題を解決するために、光の入射面を光軸
に対して45度傾けかつ出射面を光軸と入射面の両方に
対して45度傾けた磁気光学素子の入出射面に、偏光分
離膜を形成したファラデー回転子を提供するものである
。Means for Solving the Problems In order to solve the above-mentioned problems, the present invention provides a magnetic sensor in which the light incident surface is tilted at 45 degrees with respect to the optical axis, and the light exit surface is tilted at 45 degrees with respect to both the optical axis and the incident surface. The present invention provides a Faraday rotator in which a polarization separation film is formed on the entrance/exit surface of an optical element.
作用
本発明のファラデー回転子によれば、偏光分離膜が直接
磁気光学素子に形成されており、しかも光の入射面と出
射面が45度傾いた構造となっているので、直線偏光を
得るための偏光子および検光子を除くことができ、小型
で組み立てが容易な光アイソレータを得ることができる
。Function: According to the Faraday rotator of the present invention, the polarization separation film is formed directly on the magneto-optical element, and the light entrance and exit surfaces are tilted at 45 degrees, so that linearly polarized light can be obtained. The polarizer and analyzer can be removed, resulting in an optical isolator that is compact and easy to assemble.
実施例
以下、本発明の実施例を第1図および第2図に基づき説
明する。EXAMPLE Hereinafter, an example of the present invention will be explained based on FIGS. 1 and 2.
第1図に本発明によるファラデー回転子の構造を示す。FIG. 1 shows the structure of a Faraday rotator according to the present invention.
まず、磁気光学素子7(例えばYIG)を円筒状とした
後、光軸8に対して45度となるように入射面9を光学
研磨する。次に、光軸に対して45度でかつ入射面9に
対しても45度となるように出射面10を光学研磨する
。その際、光軸上での入出射面間の距離が偏光方向を4
5度回転させる長さとなるようにしておく。続いて、入
射面9および出射面10に偏光分離膜(例えば5iO=
とTiO2の多層膜)を形成しファラデー回転子とする
。さらに、第2図に示すように、このファラデー回転子
を磁石11中に固定し光アイソレータとする。First, the magneto-optical element 7 (for example, YIG) is formed into a cylindrical shape, and then the entrance surface 9 is optically polished so as to form an angle of 45 degrees with respect to the optical axis 8 . Next, the output surface 10 is optically polished so that the angle is 45 degrees with respect to the optical axis and 45 degrees with respect to the input surface 9. At that time, the distance between the input and output planes on the optical axis changes the polarization direction by 4
Make the length so that it rotates 5 degrees. Next, a polarization separation film (for example, 5iO=
and TiO2) to form a Faraday rotator. Furthermore, as shown in FIG. 2, this Faraday rotator is fixed in a magnet 11 to form an optical isolator.
ここで、半導体レーザからの出射光12aは、まず偏光
分離膜が形成された入射面9を通過して直線偏光12b
となる。続いて磁気光学素子7を通過する際に、その偏
光方向は45度回転され、その直線偏光12cは入射面
9と45度の角度を持つ出射面10に形成された偏光分
離膜を通過して直線偏光12dとなる。逆に、反射戻り
光13aはまず、偏光分離膜を形成された出射面10を
通過して直線偏光13bとなる。続いて磁気光学素子7
を通過する際に、その偏光方向はファラデー効果の持つ
非相反性により、さらに45度回転されるので、直線偏
光13cは入射面9に形成された偏光分離膜を通過でき
ない。Here, the emitted light 12a from the semiconductor laser first passes through the incident surface 9 on which the polarized light separation film is formed, and then the linearly polarized light 12b
becomes. Subsequently, when passing through the magneto-optical element 7, its polarization direction is rotated by 45 degrees, and the linearly polarized light 12c passes through a polarization separation film formed on the output surface 10, which has an angle of 45 degrees with the input surface 9. It becomes linearly polarized light 12d. Conversely, the reflected return light 13a first passes through the output surface 10 on which the polarization separation film is formed, and becomes linearly polarized light 13b. Next, magneto-optical element 7
When passing through, the polarization direction is further rotated by 45 degrees due to the non-reciprocity of the Faraday effect, so that the linearly polarized light 13c cannot pass through the polarization separation film formed on the incident surface 9.
このような構成とすることによって、偏光子および検光
子を除くことができ、小型で組み立てが容易な光アイソ
レータが実現できる。With such a configuration, a polarizer and an analyzer can be omitted, and an optical isolator that is small and easy to assemble can be realized.
なお、前記実施例の光アイソレータにレンズおよび光フ
ァイバーを加え、光アイソレータ付き半導体レーザモジ
ニールとすることもできる。Note that a lens and an optical fiber may be added to the optical isolator of the above embodiment to form a semiconductor laser module with an optical isolator.
発明の効果
以上のように本発明によれば、光の入射面を光軸に対し
て45度傾け、かつ出射面を光軸と入射面の両方に対し
て45度傾けた磁気光学素子の入出射面に、偏光分離膜
を形成したことによって偏光子および検光子のない小型
で組み立てが容易な光アイソレータが得られることとな
る。Effects of the Invention As described above, according to the present invention, the input surface of the magneto-optical element is tilted at 45 degrees with respect to the optical axis, and the output surface is tilted at 45 degrees with respect to both the optical axis and the incidence surface. By forming a polarized light separation film on the output surface, it is possible to obtain an optical isolator that is small and easy to assemble without a polarizer or analyzer.
第1図は本発明によるファラデー回転子の側面図、第2
図は本発明による光アイソレータを説明するための説明
図、第3図は従来の光アイソレータの分解斜視図、第4
図は光アイソレータの原理図である。
7・・・・・・磁気光学素子、8・・・・・・光軸、9
・・・・・・入射面、10・・・・・・出射面、11・
・・・・・磁石、H・・・・・・飽和磁界。FIG. 1 is a side view of a Faraday rotator according to the present invention, FIG.
The figures are explanatory diagrams for explaining the optical isolator according to the present invention, Figure 3 is an exploded perspective view of a conventional optical isolator, and Figure 4 is an exploded perspective view of a conventional optical isolator.
The figure shows the principle of an optical isolator. 7...Magneto-optical element, 8...Optical axis, 9
...Incidence surface, 10...Output surface, 11.
...Magnet, H...Saturation magnetic field.
Claims (1)
と入射面の両方に対して45度傾けた磁気光学素子の入
出射面に、偏光分離膜を形成したことを特徴とするファ
ラデー回転子。A polarization separation film is formed on the input and output surfaces of a magneto-optical element whose light input surface is tilted at 45 degrees with respect to the optical axis and whose output surface is tilted at 45 degrees with respect to both the optical axis and the input surface. Faraday rotator.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP27416489A JPH03135512A (en) | 1989-10-20 | 1989-10-20 | Faraday rotator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP27416489A JPH03135512A (en) | 1989-10-20 | 1989-10-20 | Faraday rotator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH03135512A true JPH03135512A (en) | 1991-06-10 |
Family
ID=17537928
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP27416489A Pending JPH03135512A (en) | 1989-10-20 | 1989-10-20 | Faraday rotator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH03135512A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5278853A (en) * | 1991-05-28 | 1994-01-11 | Mitsubishi Gas Chemical Co., Ltd. | Optical isolator |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61279806A (en) * | 1985-06-05 | 1986-12-10 | Mitsubishi Electric Corp | Thin film type optical isolator |
-
1989
- 1989-10-20 JP JP27416489A patent/JPH03135512A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61279806A (en) * | 1985-06-05 | 1986-12-10 | Mitsubishi Electric Corp | Thin film type optical isolator |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5278853A (en) * | 1991-05-28 | 1994-01-11 | Mitsubishi Gas Chemical Co., Ltd. | Optical isolator |
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