JPH0429112A - Magneto-optical devices and optical isolators - Google Patents
Magneto-optical devices and optical isolatorsInfo
- Publication number
- JPH0429112A JPH0429112A JP2135064A JP13506490A JPH0429112A JP H0429112 A JPH0429112 A JP H0429112A JP 2135064 A JP2135064 A JP 2135064A JP 13506490 A JP13506490 A JP 13506490A JP H0429112 A JPH0429112 A JP H0429112A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- closed circuit
- value
- magneto
- external magnetic
- 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
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は光記録、光通信、光計測などに用いる磁気光学
装置および光アイソレータに関する物である。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a magneto-optical device and an optical isolator used in optical recording, optical communication, optical measurement, etc.
従来の技術
従来の技術として、Zn5eを磁気光学媒体として用い
た可視光用光アイソレータがアブライドオプティクス(
APPLIE[l 0PTIC5) V O1,16
、No6.1)p、1584−1587 (1977
)に報告されている。光アイソレータは光の透過偏波方
向を互いに46degに配した偏光子と検光子の間に4
5 degのファラデー回転角を有する磁気光学媒体を
置(構成をとり、偏光子を透過した順方向の光は磁気光
学媒体通過時に45degのファラブー回転を受は検光
子を通過するが、逆方向に検光子を通過した光は磁気光
学媒体のファラデー効果の持つ非相反性により磁気光学
媒体を通過時に一45degの回転を受け、偏光子の透
過偏波方向と直交し透過することはできないという機能
を有する物である。Conventional technology As a conventional technology, an optical isolator for visible light using Zn5e as a magneto-optic medium was developed by Abride Optics (
APPLIE [l 0PTIC5) V O1,16
, No.6.1) p., 1584-1587 (1977
) has been reported. An optical isolator is a 4-wire optical isolator between a polarizer and an analyzer whose transmission polarization directions of light are arranged at 46 degrees from each other.
A magneto-optical medium with a Faraday rotation angle of 5 deg was placed (configured), and the light in the forward direction that passed through the polarizer received a Farabou rotation of 45 deg when passing through the magneto-optic medium. The light that has passed through the analyzer is rotated by 145 degrees when passing through the magneto-optic medium due to the non-reciprocity of the Faraday effect of the magneto-optic medium, and the light is perpendicular to the transmitted polarization direction of the polarizer and cannot be transmitted. It is something that you have.
Zn5eのファラデー回転角θはθ=VBd1■はベル
デ定数、Bは光の伝搬方向の外部磁場、dは磁気光学媒
体中の光路長、で表される。本例においては使用光源の
波長λ=8328Aにおけるベルデ定数V=8. 7*
10−”deg/ (cm*G)、d=0.432c
mで42.35degのファラデー回転が得られる外部
磁場Bを印加しており、偏光子と検光子の透過偏波方向
を互いに42.35degとして用いている。The Faraday rotation angle θ of Zn5e is expressed as θ=VBd1 is the Verdet constant, B is the external magnetic field in the propagation direction of light, and d is the optical path length in the magneto-optic medium. In this example, the Verdet constant V=8 at the wavelength λ=8328A of the light source used. 7*
10-”deg/ (cm*G), d=0.432c
An external magnetic field B is applied to obtain a Faraday rotation of 42.35 deg in m, and the transmission polarization directions of the polarizer and analyzer are set to be 42.35 deg.
発明が解決しようとする課題
従来の技術で示したようにファラデー回転角θはθ=V
Bdで与えられるため、印加する外部磁場Bの値が変動
するとθが変化し、アイソレーション比の劣化を招く。Problem to be Solved by the Invention As shown in the prior art, the Faraday rotation angle θ is θ=V
Since it is given by Bd, when the value of the external magnetic field B to be applied changes, θ changes, leading to deterioration of the isolation ratio.
例えば、本従来の技術のV=6. 7* 100−3d
e / (cm*G)、 d=0゜432cmのZn5
eにおいて45degのファラデー回転角が得られる外
部磁場として15547Gを印加して用いた場合、外部
磁場が約2%変化しただけでファラデー回転角は46d
egとなる。For example, V=6. 7* 100-3d
e/(cm*G), Zn5 with d=0°432cm
When applying an external magnetic field of 15547G to obtain a Faraday rotation angle of 45 degrees at e, the Faraday rotation angle is 46 degrees with only a 2% change in the external magnetic field.
It becomes eg.
偏光子と検光子の透過偏波方向を互いに45degに配
して固定し、最初アイソレーション比として−35dB
得られたとき、磁気光学媒体のファラデー回転角が45
degからl degずれるとアイソレーション比は一
32dBに劣化した。本発明は磁気光学媒体へ印加する
外部磁場の変動による磁気光学装置の特性劣化を防ぐも
のである。また、光アイソレータにおいては磁気光学媒
体へ印加する外部磁場の変動によるアイソレーション比
の劣化を防ぐものである。The transmission polarization directions of the polarizer and analyzer are fixed at 45deg from each other, and the initial isolation ratio is -35dB.
When obtained, the Faraday rotation angle of the magneto-optic medium is 45
The isolation ratio deteriorated to -32 dB when the signal was shifted by 1 degree from 1 degree. The present invention prevents characteristic deterioration of a magneto-optical device due to fluctuations in an external magnetic field applied to a magneto-optic medium. Further, in the optical isolator, deterioration of the isolation ratio due to fluctuations in the external magnetic field applied to the magneto-optic medium is prevented.
課題を解決するための手段
本発明は磁気光学媒体へ印加する外部磁場の変動による
磁気光学装置の特性劣化を防くへく、光照射部および量
子細線よりなる閉回路部を構成する磁気光学媒体、前記
磁気光学媒体を磁化するための前記量子細線よりなる閉
回路部の閉回路に垂直に磁場を印加する手段、および前
記量子細線よりなる閉回路の磁気抵抗を測定する手段を
有し、前記磁気抵抗の値より前記量子細線よりなる閉回
路部の閉回路に垂直に印加した磁場の正確な値を得るこ
とにより前記磁場の値を所望の値に前記磁場を変化させ
ることが可能であることを特徴とする磁気光学装置を提
案するものである。また、本発明は光アイソレータにお
いては磁気光学媒体へ印加する外部磁場の変動によるア
イソレーション比の劣化を防くべく、偏光子、前記偏光
子と45degの偏波透過角度を有する検光子、光照射
部および量子細線よりなる閉回路部を構成する磁気光学
媒体、前記磁気光学体を磁化するための前記量子細線よ
りなる閉回路部の閉回路に垂直に磁場を印加する手段、
および前記量子細線よりなる閉回路の磁気抵抗を測定す
る手段ををし、前記磁気抵抗の値より前記量子細線より
なる閉回路部の閉回路に垂直に印加した磁場の正確な値
を得ることにより前記磁場の値を常に正確に45deg
のファラデー回転を与えることを特徴とする光アイソレ
ータを提案するものである。Means for Solving the Problems The present invention provides a magneto-optic medium that constitutes a closed circuit section consisting of a light irradiation section and a quantum wire, in order to prevent characteristic deterioration of a magneto-optical device due to fluctuations in an external magnetic field applied to the magneto-optic medium. , means for applying a magnetic field perpendicularly to a closed circuit of the closed circuit section made of the quantum wire for magnetizing the magneto-optic medium, and means for measuring the magnetic resistance of the closed circuit made of the quantum wire, It is possible to change the value of the magnetic field to a desired value by obtaining an accurate value of the magnetic field applied perpendicularly to the closed circuit of the closed circuit section made of the quantum wire from the value of magnetic resistance. This paper proposes a magneto-optical device characterized by: In addition, in the optical isolator, in order to prevent deterioration of the isolation ratio due to fluctuations in the external magnetic field applied to the magneto-optic medium, the present invention includes a polarizer, an analyzer having a polarization transmission angle of 45 degrees with respect to the polarizer, and a light irradiation device. a magneto-optical medium constituting a closed circuit section made of a quantum wire and a quantum wire, a means for applying a magnetic field perpendicularly to the closed circuit of the closed circuit section made of the quantum wire for magnetizing the magneto-optic body;
and a means for measuring the magnetic resistance of the closed circuit made of the quantum wire, and obtaining an accurate value of the magnetic field applied perpendicularly to the closed circuit of the closed circuit portion made of the quantum wire from the value of the magnetic resistance. The value of the magnetic field is always accurately 45 deg.
This paper proposes an optical isolator that is characterized by providing a Faraday rotation of .
作用
本発明の磁気光学装置は磁気光学媒体で作製した量子細
線よりなる閉回路部において、磁気光学媒体で作製した
量子細線よりなる閉回路部に垂直に印加する外部磁場の
値をアハラノフ−ボーム効果により振動する磁気抵抗値
として知ることができる。つまり、通常の磁気抵抗値変
化より微少な外部磁場変化に対して大きな磁気抵抗変化
として観測できる。この磁気抵抗変化から外部磁場の変
化をよみとり、外部磁場印加機構の制御ヘフィードバノ
クすることにより、本発明の磁気光学装置の光照射部に
印加する外部磁場を一定に保ち磁気光学装置の特性劣化
を防くものである。また、本発明の光アイソレータは本
発明の磁気光学装置と同様の作用により、光照射部への
印加外部磁場を一定に保ち、アイツレ−7ヨン比の劣化
を防くものである。Function: The magneto-optical device of the present invention changes the value of an external magnetic field applied perpendicularly to the closed circuit section made of quantum wires made of a magneto-optic medium using the Ahranov-Bohm effect. It can be known as the oscillating magnetic resistance value. In other words, a small change in the external magnetic field can be observed as a large change in magnetoresistance than a normal change in magnetoresistance value. By reading changes in the external magnetic field from this magnetoresistance change and feeding it back to the control of the external magnetic field application mechanism, the external magnetic field applied to the light irradiation part of the magneto-optical device of the present invention is kept constant and the characteristics of the magneto-optical device are prevented from deteriorating. It's a spider. Further, the optical isolator of the present invention has the same effect as the magneto-optical device of the present invention to keep the external magnetic field applied to the light irradiation part constant and prevent deterioration of the Eitz-Rayon ratio.
実施例
本発明の磁気光学装置の実施例の模式図を第1図に示す
。フッ化力ルンウム基板1上に磁気光学媒体としてZn
5e2をMOVPE法で成長し、イオンビーム加工によ
り、光照射部3と量子細線よりなる閉回路部4を形成す
る。磁気光学媒体の両側に磁気光学媒体に外部磁場を与
える手段の一例として電磁石5を配置する。量子細線よ
りなる閉回路部4の電流入出射端6.7に一定電流を流
し、電圧測定端8.9間の電圧を測定することにより、
量子細線よりなる閉回路部4の抵抗を測定する手段10
と得られた量子細線よりなる閉回路部4の抵抗の値から
磁気光学媒体に印加する外部磁場の値を求め、外部磁場
を与える電磁石5の電流を制御する手段11を有する。Embodiment A schematic diagram of an embodiment of the magneto-optical device of the present invention is shown in FIG. Zn is deposited as a magneto-optical medium on a fluorinated aluminum substrate 1.
5e2 is grown by the MOVPE method, and the closed circuit part 4 made of the light irradiation part 3 and the quantum wire is formed by ion beam processing. Electromagnets 5 are placed on both sides of the magneto-optic medium as an example of means for applying an external magnetic field to the magneto-optic medium. By passing a constant current through the current input and output ends 6.7 of the closed circuit section 4 made of quantum wire and measuring the voltage between the voltage measurement ends 8.9,
Means 10 for measuring the resistance of the closed circuit section 4 made of quantum wires
It has means 11 for determining the value of an external magnetic field to be applied to the magneto-optic medium from the resistance value of the closed circuit section 4 made of the quantum wire obtained and controlling the current of the electromagnet 5 that applies the external magnetic field.
磁気光学媒体に印加する外部磁場が変化すると量子細線
よりなる閉回路部4の抵抗値が振動するため、微少な外
部磁場の変化に対して大きな量子細線よりなる閉回路部
4の抵抗値の変化が得られ、量子細線よりなる閉回路部
4の抵抗の値から磁気光学媒体に印加する外部磁場の値
を求め、外部磁場を与える電磁石5の電流を制御する手
段11により容易に外部磁場を一定の値に制御すること
ができ、磁気光学装置の特性劣化を防ぐことができた。When the external magnetic field applied to the magneto-optic medium changes, the resistance value of the closed circuit section 4 made of quantum wires oscillates. Therefore, the resistance value of the closed circuit section 4 made of quantum wires changes in response to a small change in the external magnetic field. is obtained, the value of the external magnetic field to be applied to the magneto-optic medium is determined from the resistance value of the closed circuit section 4 made of quantum wires, and the external magnetic field is easily kept constant by the means 11 for controlling the current of the electromagnet 5 that applies the external magnetic field. It was possible to control the value to a value of , and prevent deterioration of the characteristics of the magneto-optical device.
なお、第1図に示した磁気光学装置の模式図に偏光子や
レンズ等の光学部品を組み合わせて、光スィッチ、光サ
ーキュレータ、光アイソレータ等を構成してもよく、磁
気光学媒体に外部磁場を与える手段が本例以外のもので
もよい。Note that optical switches, optical circulators, optical isolators, etc. may be constructed by combining optical components such as polarizers and lenses with the schematic diagram of the magneto-optical device shown in FIG. The means for providing may be other than this example.
第2図に本発明の光アイソレータの模式図を示す。偏光
子20と光の透過偏波方向を45degに配した検光子
21の間にフッ化力ルンウム基板1上に磁気光学媒体と
してZn5e2をMOVPE法で成長し、所望の外部磁
場で45degのファラデー回転角を有するだけの導波
路長を持つ光導波路22に加工した光照射部3と、イオ
ンビーム加工により形成したZn5e2の量子細線より
なる閉回路部4を設ける。磁気光学媒体の両側に磁気光
学媒体に外部磁場を与える手段の一例として電磁石5を
配置する。量子細線よりなる閉回路部4の電流入出射端
6.7に一定電流を流し、電圧測定端8.9間の電圧を
測定することにより、量子細線よりなる閉回路部4の抵
抗を測定する手段10と得られた量子細線よりなる閉回
路部4の抵抗の値から磁気光学媒体に印加する外部磁場
の値を求め、外部磁場を与える電磁石5の電流を制御す
る手段11を有する。磁気光学媒体に印加する外部磁場
が変化すると、光導波路22を導波する光のファラデー
回転角が45 degからそれることと同時に、量子細
線よりなる閉回路部4の抵抗値が変化する。量子細線よ
りなる閉回路部4の抵抗値は外部磁場の変化に対して振
動するため、微少な外部磁場の変化に対して大きな量子
細線よりなる閉回路部4の抵抗値の変化が得られ、量子
細線よりなる閉回路部4の抵抗の値から磁気光学媒体に
印加する外部磁場の値を求め、外部磁場を与える電磁石
5の電流を制御する手段11により容易に外部磁場を一
定の値に制御することができ、光アイソレータのアイソ
レーション比の劣化を防ぐことができた。FIG. 2 shows a schematic diagram of the optical isolator of the present invention. Between the polarizer 20 and the analyzer 21 with the transmission polarization direction of light set at 45 degrees, Zn5e2 is grown as a magneto-optical medium on the fluorinated substrate 1 by the MOVPE method, and Faraday rotation of 45 degrees is performed using a desired external magnetic field. A light irradiation section 3 processed into an optical waveguide 22 having a waveguide length corresponding to an angle, and a closed circuit section 4 made of a Zn5e2 quantum wire formed by ion beam processing are provided. Electromagnets 5 are placed on both sides of the magneto-optic medium as an example of means for applying an external magnetic field to the magneto-optic medium. The resistance of the closed circuit section 4 made of quantum wires is measured by passing a constant current through the current input/output ends 6.7 of the closed circuit section 4 made of quantum wires and measuring the voltage between the voltage measurement terminals 8.9. It has means 11 for determining the value of an external magnetic field to be applied to the magneto-optic medium from the resistance value of the means 10 and the closed circuit section 4 made of the obtained quantum wire, and controlling the current of the electromagnet 5 that applies the external magnetic field. When the external magnetic field applied to the magneto-optic medium changes, the Faraday rotation angle of the light guided through the optical waveguide 22 deviates from 45 degrees, and at the same time, the resistance value of the closed circuit section 4 made of quantum wire changes. Since the resistance value of the closed circuit section 4 made of quantum wires oscillates in response to changes in the external magnetic field, a large change in the resistance value of the closed circuit section 4 made of quantum wires can be obtained in response to a slight change in the external magnetic field. The value of the external magnetic field applied to the magneto-optical medium is determined from the resistance value of the closed circuit section 4 made of quantum wires, and the external magnetic field is easily controlled to a constant value by means 11 for controlling the current of the electromagnet 5 that applies the external magnetic field. This made it possible to prevent deterioration of the isolation ratio of the optical isolator.
発明の効果
本発明の磁気光学装置により磁気光学媒体に印加する外
部磁場の変動による特性劣化のない磁気光学装置が得ら
れた。本発明の光アイソレータにより磁気光学媒体に印
加する外部磁場の変動によるアイツレ−/ヨ/比の劣化
のない光アイソレータが得られた。Effects of the Invention By the magneto-optical device of the present invention, a magneto-optical device was obtained that does not suffer from characteristic deterioration due to fluctuations in the external magnetic field applied to the magneto-optic medium. By using the optical isolator of the present invention, an optical isolator which does not suffer from deterioration of the Eysle/yaw/ratio due to fluctuations in the external magnetic field applied to the magneto-optic medium was obtained.
第1図は本発明の実施例の磁気光学装置の模式図、第2
図は本発明の実施例の光アイソレータの模式図である。
2・・・Zn5e、3・・・光照射部、4・・の閉回路
部、6・・・電流入射端、7・・・電流出射端、8,9
・・・電圧測定端。FIG. 1 is a schematic diagram of a magneto-optical device according to an embodiment of the present invention, and FIG.
The figure is a schematic diagram of an optical isolator according to an embodiment of the present invention. 2... Zn5e, 3... Light irradiation part, 4... Closed circuit part, 6... Current input end, 7... Current output end, 8, 9
...Voltage measurement end.
Claims (2)
する磁気光学媒体、前記磁気光学媒体を磁化するための
前記量子細線よりなる閉回路部の閉回路に垂直に磁場を
印加する手段、および前記量子細線よりなる閉回路の磁
気抵抗を測定する手段を有し、前記磁気抵抗の値より前
記量子細線よりなる閉回路部の閉回路に垂直に印加した
磁場の正確な値を得ることにより前記磁場の値を所望の
値に前記磁場を変化させることが可能であることを特徴
とする磁気光学装置。(1) a magneto-optical medium constituting a closed circuit section made of a light irradiation section and a quantum wire, a means for applying a magnetic field perpendicularly to the closed circuit of the closed circuit section made of the quantum wire for magnetizing the magneto-optic medium; and means for measuring the magnetic resistance of the closed circuit made of the quantum wire, and obtaining an accurate value of the magnetic field applied perpendicularly to the closed circuit of the closed circuit portion made of the quantum wire from the value of the magnetic resistance. A magneto-optical device characterized in that the value of the magnetic field can be changed to a desired value.
を有する検光子、光照射部および量子細線よりなる閉回
路部を構成する磁気光学媒体、前記磁気光学体を磁化す
るための前記量子細線よりなる閉回路部の閉回路に垂直
に磁場を印加する手段、および前記量子細線よりなる閉
回路の磁気抵抗を測定する手段を有し、前記磁気抵抗の
値より前記量子細線よりなる閉回路部の閉回路に垂直に
印加した磁場の正確な値を得ることにより前記磁場の値
を常に正確に45degのファラデー回転を与えること
を特徴とする光アイソレータ。(2) a polarizer, an analyzer having a polarization transmission angle of 45 degrees with respect to the polarizer, a magneto-optic medium constituting a closed circuit section consisting of a light irradiation section and a quantum wire, and the quantum for magnetizing the magneto-optical body. means for applying a magnetic field perpendicularly to a closed circuit of a closed circuit portion made of a thin wire, and means for measuring magnetic resistance of the closed circuit made of the quantum wire, and the closed circuit made of the quantum wire is determined based on the value of the magnetic resistance. An optical isolator characterized in that the value of the magnetic field is always accurately given a Faraday rotation of 45 degrees by obtaining an accurate value of the magnetic field applied perpendicularly to the closed circuit of the optical isolator.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2135064A JPH0429112A (en) | 1990-05-24 | 1990-05-24 | Magneto-optical devices and optical isolators |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2135064A JPH0429112A (en) | 1990-05-24 | 1990-05-24 | Magneto-optical devices and optical isolators |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0429112A true JPH0429112A (en) | 1992-01-31 |
Family
ID=15143037
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2135064A Pending JPH0429112A (en) | 1990-05-24 | 1990-05-24 | Magneto-optical devices and optical isolators |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0429112A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7385361B2 (en) | 2003-05-14 | 2008-06-10 | Matsushita Electric Industrial Co., Ltd. | Ballast for high-pressure discharge lamp and method of operating the same |
-
1990
- 1990-05-24 JP JP2135064A patent/JPH0429112A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7385361B2 (en) | 2003-05-14 | 2008-06-10 | Matsushita Electric Industrial Co., Ltd. | Ballast for high-pressure discharge lamp and method of operating the same |
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