JPS59121314A - Faraday rotor - Google Patents

Faraday rotor

Info

Publication number
JPS59121314A
JPS59121314A JP22866582A JP22866582A JPS59121314A JP S59121314 A JPS59121314 A JP S59121314A JP 22866582 A JP22866582 A JP 22866582A JP 22866582 A JP22866582 A JP 22866582A JP S59121314 A JPS59121314 A JP S59121314A
Authority
JP
Japan
Prior art keywords
magnetic field
faraday
rotation angle
stage
changing
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
JP22866582A
Other languages
Japanese (ja)
Inventor
Masataka Shirasaki
白崎 正孝
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP22866582A priority Critical patent/JPS59121314A/en
Publication of JPS59121314A publication Critical patent/JPS59121314A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/09Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on magneto-optical elements, e.g. exhibiting Faraday effect

Landscapes

  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)

Abstract

PURPOSE:To obviate the generation of an abnormal fluctuation in light level in the stage of changing over a Faraday's rotation angle by providing a closed electric path having about 45 deg. angle relative with the transmission direction of light so as to enclose a Faraday rotor. CONSTITUTION:A magnetic field in the direction opposite from the magnetic field that has been impressed till then by a means for changing the rotation angle in order to induce the effect of the Farady rotation in the opposite direction in a Faraday rotor 1 is impressed on said Faraday rotor which consists of a thin YIG plate, a means for impressing the magnetic field for changing the Farady's rotation angle and a closed electric circuit 3 and acts the effect of Faraday rotation in a certain direction. Induced current flows in the circuit 3 on account of a change in the magnetic flux generated in the stage of said changing over by which a magnetic field in the horizontal direction for the purpose of maintaining the magnetization in a satd. state is generated. The irregular fluctuation in the magnetic domain generated until the magnetic field attains the satd. state in the opposite direction through an unsatd. state is eliminated in the stage of changing over the rotation angle and the abnormal fluctuation in the light level in said stage is eliminated.

Description

【発明の詳細な説明】 (1)発明の技術分野 本発明は巻−冬インチ等に用いるファラデー回転子に係
り、特にファラデー回転方向切換え時の素子内磁区の不
規則な変動を防止しろる手段を備えたファラデー回転子
に関する。
DETAILED DESCRIPTION OF THE INVENTION (1) Technical Field of the Invention The present invention relates to a Faraday rotator used for winding, wintering, etc., and particularly to a means for preventing irregular fluctuations of magnetic domains within an element when switching the direction of Faraday rotation. Regarding a Faraday rotator with.

(2)技術の背景 ファラデー回転子はその回転角を逆転するために、光の
透過方向にかかる磁場の向きを逆転している。
(2) Background of the technology In order to reverse the rotation angle of the Faraday rotator, the direction of the magnetic field applied to the direction of light transmission is reversed.

しかしながら、従来のこの種磁場変更手段に問題があっ
てその変更時にファラデー回転角が不安定となり、スイ
ッチ出力の光レベルが異常に変動してしまうという望ま
しくない現象が現われてしまうので、これを解決しうる
技術手段の開発が要望されている。
However, there is a problem with conventional magnetic field changing means of this type, and when changing it, the Faraday rotation angle becomes unstable, resulting in an undesirable phenomenon in which the optical level of the switch output fluctuates abnormally. There is a need for the development of technological means that can do this.

(3)従来技術と問題点 従来、ファラデー回転子(Y I G)は光スィッチ等
に用いられているが、そのファラデー回転角を逆転する
場合ファラデー回転子にかかっている磁場の向きを逆転
している。その逆転の際に、磁化が飽和状態から零にな
り、逆向きの飽和状態になる。このような磁化の不飽和
状態における変化中2ファラデー回転子内の磁区が不規
則に変動し。
(3) Conventional technology and problems Conventionally, a Faraday rotator (YIG) has been used in optical switches, etc., but in order to reverse the Faraday rotation angle, it is necessary to reverse the direction of the magnetic field applied to the Faraday rotator. ing. During the reversal, the magnetization goes from a saturated state to zero, and then goes to a saturated state in the opposite direction. During such changes in the unsaturated state of magnetization, the magnetic domains within the two Faraday rotators fluctuate irregularly.

光に散乱を生じさせて光レベルに異當な変動が生じて来
るという不具合がある。
There is a problem in that the light is scattered, causing abnormal fluctuations in the light level.

(4)発明の目的 本発明は上述したような従来ファラデー回転子の有する
欠点に鑑みて創案されたもので、その目的はファラデー
回転角の切換え時に光レベルか異常な変動を生しないフ
ァラデー回転子を提供することにある。
(4) Purpose of the Invention The present invention was devised in view of the drawbacks of conventional Faraday rotators as described above, and its purpose is to provide a Faraday rotator that does not cause abnormal fluctuations in light level when switching the Faraday rotation angle. Our goal is to provide the following.

(5)発明の構成 そして、この目的はファラデー回転方向を逆転する際に
光の透過方向に印加されている磁場の向きを逆転するフ
ァラデー回転子であって、上記光の透過方向に列し45
度又はその近傍の角度をなす閉電路を上記ファラデー回
転子を囲繞されて設けるごとによって、達成される。
(5) Structure of the invention And, this object is a Faraday rotator that reverses the direction of the magnetic field applied in the light transmission direction when reversing the Faraday rotation direction, and the Faraday rotator is aligned in the light transmission direction.
This is achieved by surrounding the Faraday rotator with a closed circuit having an angle of at least 100 degrees or close to it.

(6)発明の実施例 以上、添付図面を参照して本発明の詳細な説明する。(6) Examples of the invention The present invention will now be described in detail with reference to the accompanying drawings.

添付図面は本発明の一実施例をボす。この図において、
1は本発明のファラデー回転子で、これはYIGii板
2と、この薄板2の1図面に対して水平な光透過方向に
可逆的に磁場を印加するファラデー回転角変更用磁場印
加手段(図面には明示せず)と、上記光の透過方向に対
し45度又はその近傍の角度でYIG薄板2を囲繞して
設&Jられた閉電路3とから成る。ファラデー回転角変
更用磁場印加手段は2例えば半硬質磁性体をコアに有す
る電磁石である。
The accompanying drawings illustrate one embodiment of the invention. In this diagram,
1 is a Faraday rotator of the present invention, which consists of a YIGii plate 2 and a Faraday rotation angle changing magnetic field applying means for reversibly applying a magnetic field in a horizontal light transmission direction with respect to one drawing of this thin plate 2 (see the drawing). (not shown) and a closed circuit 3 surrounding the YIG thin plate 2 at an angle of 45 degrees or in the vicinity of the direction of transmission of the light. The magnetic field applying means for changing the Faraday rotation angle is, for example, an electromagnet having a semi-hard magnetic material in its core.

次に2本発明ファラデー回転子の作用を説明する。Next, the operation of the two Faraday rotators of the present invention will be explained.

ファラデー回転子1に成る方向のファラデー回転作用を
生ぜしめるべく、ファラデー回転角変更用磁場印加手段
に光透過方向における成る向きの磁場がファラデー回転
子1に印加しておくか、ファラデー回転角変更用磁場印
加手段が2例えば半硬質磁性体をコアに有する電磁石で
ある場合には。
In order to produce a Faraday rotation effect in the direction of the Faraday rotator 1, a magnetic field in the direction of the light transmission direction is applied to the Faraday rotation angle changing magnetic field applying means to the Faraday rotator 1. For example, when the magnetic field applying means is an electromagnet having a semi-hard magnetic material in its core.

磁場の逆転時のみ電磁石に切換え用パルス電力か供給さ
れ、その切換え後は電磁石の有する自己保持機能による
磁場が回転子1に印加されている。
Pulse power for switching is supplied to the electromagnet only when the magnetic field is reversed, and after the switching, a magnetic field is applied to the rotor 1 due to the self-holding function of the electromagnet.

このようにして成る方向のファラデー回転作用が呈せし
められているファラデー回転子1に、逆゛ 向きのファ
ラデー回転作用を生ぜしめるべく、ファラデー回転角変
更用磁場印加手段によって、それまで印加されていた磁
場とは逆向きの磁場がファラデー回転子】内に生ぜしめ
られる。
In order to produce a Faraday rotation effect in the opposite direction, the Faraday rotation angle changing magnetic field applying means applies a magnetic field to the Faraday rotator 1, which is thus subjected to a Faraday rotation effect in the opposite direction. A magnetic field in the opposite direction to the magnetic field is generated within the Faraday rotator.

この切換え時に生ずる磁束変化によって閉電路3内に誘
導電流が流れ、これによって上記磁場に対し横方向の磁
場が発生される。この磁場は切換えられつつある磁化を
飽和に近い状態に保つためのものである。
An induced current flows in the closed circuit 3 due to the change in magnetic flux that occurs during this switching, thereby generating a magnetic field in a direction transverse to the above-mentioned magnetic field. This magnetic field is intended to keep the magnetization being switched close to saturation.

従って、ファラデー回転角を切換える際の、磁場が不飽
和状態を経て逆向きの飽和状態へ至るまでに生ずる磁区
の不規則な変動はなくなる。イ乃って、その際の光レヘ
ルの異常な変動を除去しうる。
Therefore, when the Faraday rotation angle is switched, irregular fluctuations in the magnetic domain that occur when the magnetic field passes through an unsaturated state and reaches a saturated state in the opposite direction are eliminated. In addition, abnormal fluctuations in the optical level at that time can be removed.

このような関係は上述の逆向きのファラデー回転作用か
ら上述の成る方向のファラデー回転作用への切換え時に
も維持される。
Such a relationship is maintained even when switching from the above-mentioned opposite Faraday rotation action to the above-mentioned directional Faraday rotation action.

(7)発明の効果 以上述べたように2本発明によれば、ファラデー回転角
変更用磁場の切換え時にその磁場に対し横方向をなす誘
導磁場が発生されて素子内磁区の不規則な変動を防止し
うるから、光レヘルの異常な変動を除去しうる。
(7) Effects of the invention As described above, according to the second invention, when the magnetic field for changing the Faraday rotation angle is switched, an induced magnetic field is generated in a direction transverse to the magnetic field, thereby suppressing irregular fluctuations of the magnetic domains within the element. Since it can be prevented, abnormal fluctuations in optical level can be eliminated.

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

添付図面は本発明の一実施例を示す。 図中、1はファラデー回転子、2はy+c薄板。 3ば閉電路である。 The accompanying drawings illustrate one embodiment of the invention. In the figure, 1 is a Faraday rotator and 2 is a y+c thin plate. 3. It is a closed circuit.

Claims (1)

【特許請求の範囲】 +11フアラデ一回転方向を逆転する際に光の透過力向
に印加されている磁場の向きを逆転するファラデー回転
子であって、上記光の透過方向に対し45度又はその近
傍の角度をなす閉電路を上記ファラデー回転子に囲繞さ
せて設けたことを特徴とするファラデー回転子。 (2)上記光の透過方向に磁場を印加する手段を、半硬
質磁性体をコアとする電磁石により構成したことを特徴
とする特許請求の範囲第1項記載のファラデー回転子。
[Scope of Claims] +11 Faraday A Faraday rotator that reverses the direction of a magnetic field applied to the light transmission direction when reversing the direction of rotation, the Faraday rotator at 45 degrees or less with respect to the light transmission direction. A Faraday rotator characterized in that a closed current path forming an angle in the vicinity is provided surrounding the Faraday rotator. (2) The Faraday rotator according to claim 1, wherein the means for applying a magnetic field in the direction of transmission of the light is constituted by an electromagnet having a core of a semi-hard magnetic material.
JP22866582A 1982-12-28 1982-12-28 Faraday rotor Pending JPS59121314A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22866582A JPS59121314A (en) 1982-12-28 1982-12-28 Faraday rotor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22866582A JPS59121314A (en) 1982-12-28 1982-12-28 Faraday rotor

Publications (1)

Publication Number Publication Date
JPS59121314A true JPS59121314A (en) 1984-07-13

Family

ID=16879890

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22866582A Pending JPS59121314A (en) 1982-12-28 1982-12-28 Faraday rotor

Country Status (1)

Country Link
JP (1) JPS59121314A (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0651255A (en) * 1992-07-31 1994-02-25 Fujitsu Ltd Optical attenuator
US5812304A (en) * 1995-08-29 1998-09-22 Fujitsu Limited Faraday rotator which generates a uniform magnetic field in a magnetic optical element
US5844710A (en) * 1996-09-18 1998-12-01 Fujitsu Limited Faraday rotator and optical device employing the same
US5867300A (en) * 1996-03-01 1999-02-02 Fujitsu Limited Variable optical attenuator which applies a magnetic field to a faraday element to rotate the polarization of a light signal
US5889609A (en) * 1992-07-31 1999-03-30 Fujitsu Limited Optical attenuator
US6018411A (en) * 1996-11-29 2000-01-25 Fujitsu Limited Optical device utilizing magneto-optical effect
US6441955B1 (en) 1998-02-27 2002-08-27 Fujitsu Limited Light wavelength-multiplexing systems
US6496300B2 (en) 1998-02-27 2002-12-17 Fujitsu Limited Optical amplifier

Cited By (16)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2815509B2 (en) * 1992-07-31 1998-10-27 富士通株式会社 Optical attenuator
US5889609A (en) * 1992-07-31 1999-03-30 Fujitsu Limited Optical attenuator
US6018412A (en) * 1992-07-31 2000-01-25 Fujitsu Limited Optical attenuator
JPH0651255A (en) * 1992-07-31 1994-02-25 Fujitsu Ltd Optical attenuator
US6275323B1 (en) 1992-07-31 2001-08-14 Fujitsu Limited Optical attenuator
US5812304A (en) * 1995-08-29 1998-09-22 Fujitsu Limited Faraday rotator which generates a uniform magnetic field in a magnetic optical element
US6570699B2 (en) 1996-03-01 2003-05-27 Fujitsu Limited Variable optical attenuator which applies a magnetic field to a Faraday element to rotate the polarization of a light signal
US5867300A (en) * 1996-03-01 1999-02-02 Fujitsu Limited Variable optical attenuator which applies a magnetic field to a faraday element to rotate the polarization of a light signal
US5973821A (en) * 1996-03-01 1999-10-26 Fujitsu Limited Variable optical attenuator which applies a magnetic field to a faraday element to rotate the polarization of light signal
US6333806B1 (en) 1996-03-01 2001-12-25 Fujitsu Limited Variable optical attenuator which applies a magnetic field to a Faraday element to rotate the polarization of a light signal
US6717713B2 (en) 1996-03-01 2004-04-06 Fujitsu Limited Variable optical attenuator which applies a magnetic field to a faraday element to rotate the polarization of a light signal
US5844710A (en) * 1996-09-18 1998-12-01 Fujitsu Limited Faraday rotator and optical device employing the same
US6018411A (en) * 1996-11-29 2000-01-25 Fujitsu Limited Optical device utilizing magneto-optical effect
US6496300B2 (en) 1998-02-27 2002-12-17 Fujitsu Limited Optical amplifier
US6441955B1 (en) 1998-02-27 2002-08-27 Fujitsu Limited Light wavelength-multiplexing systems
US6919987B2 (en) 1998-02-27 2005-07-19 Fujitsu Limited Light wavelength-multiplexing systems

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