JPH02126403A - Magneto-optical recording and reproducing device - Google Patents

Magneto-optical recording and reproducing device

Info

Publication number
JPH02126403A
JPH02126403A JP28060288A JP28060288A JPH02126403A JP H02126403 A JPH02126403 A JP H02126403A JP 28060288 A JP28060288 A JP 28060288A JP 28060288 A JP28060288 A JP 28060288A JP H02126403 A JPH02126403 A JP H02126403A
Authority
JP
Japan
Prior art keywords
magnetic field
magneto
yoke
disk
information
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
JP28060288A
Other languages
Japanese (ja)
Inventor
Takeshi Terasawa
寺沢 毅
Koichi Takeuchi
浩一 竹内
Seio Watanabe
渡辺 勢夫
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP28060288A priority Critical patent/JPH02126403A/en
Publication of JPH02126403A publication Critical patent/JPH02126403A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing

Abstract

PURPOSE:To shorten the inversion time of magnetic field generated by an exciting element at the time of recording information by providing a repulsive magnetic field wiring which generates magnetic flux with which leakage flux from an actuator which flows in the exciting element should be cancelled in the exciting element. CONSTITUTION:A magneto-optical disk 4 is rotated and a current corresponding to a signal which should be recorded is inputted in the modulation coil 2 of the exciting element 1 to add the magnetic field to one surface of the disk 4, then a laser light which is projected by a semiconductor laser 13 and whose light intensity is constant is projected to the other surface of the disk 4 to record the information. By projecting only the laser light on the other surface of the disk 4, the variation of the reflected light is detected and recorded information in the disk 4 is reproduced. Meanwhile, the repulsive magnetic field wiring 21 generates the magnetic field of an opposite polarity so that the leakage flux which flows in a yoke 3 caused by the excitation may be cancelled. The magnetic flux PHI2 generated in the repulsive magnetic field circulates through a magnetic pole 3b in the center of the yoke 3 and the leakage flux PHI1 which flows in the yoke 3 is cancelled with the magnetic flux PHI2. The intensity of the magnetic field generated by the exciting element 1 is not changed and the information is recorded on the disk 4 with high accuracy.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は光磁気ディスクに光及び磁界を与えて情報の記
録再生を行う光磁気記録再生装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a magneto-optical recording and reproducing apparatus that records and reproduces information by applying light and a magnetic field to a magneto-optical disk.

〔従来の技術〕[Conventional technology]

第4図はこの種の従来の光磁気記録再生装置の模式的斜
視図である。ディスクモータ14により光磁気ディスク
4が回転するようになっている。励磁素子支持アーム1
5の先端側には、情報の記録。
FIG. 4 is a schematic perspective view of this type of conventional magneto-optical recording and reproducing apparatus. A magneto-optical disk 4 is rotated by a disk motor 14. Exciting element support arm 1
Information is recorded on the tip side of 5.

消去用のバイアス磁界を発生する励磁素子1が取り付け
られている。この励磁素子lは励磁素子支持アーム15
を矢符方向へ移動させることにより、光磁気ディスク4
の一面に接近した状態で光磁気ディスク4の径方向へ移
動するようになっている。
An excitation element 1 that generates a bias magnetic field for erasing is attached. This excitation element l is an excitation element support arm 15
by moving the magneto-optical disk 4 in the direction of the arrow.
It moves in the radial direction of the magneto-optical disk 4 while approaching one surface of the disk.

そして励磁素子lは3つの磁極3a、3b、3cを有す
るE字状をしたヨーク3の中央の磁極3bに変調コイル
2を巻回しており、磁極3a、3b、3cの並設方向を
光磁気ディスク4のトラック方向として、磁極3a。
The excitation element l has a modulation coil 2 wound around a central magnetic pole 3b of an E-shaped yoke 3 having three magnetic poles 3a, 3b, and 3c, and the direction in which the magnetic poles 3a, 3b, and 3c are arranged in parallel is magneto-optical. As the track direction of the disk 4, the magnetic pole 3a.

3b、3cを光磁気ディスク4と対向するように励磁素
子が位置決めされている。
The excitation element is positioned so that 3b and 3c face the magneto-optical disk 4.

一方、励磁素子1と対向しており、それと連動して同方
向へ移動し、光磁気ディスクの他面側に位置する光ピツ
クアップ6を設けている。この光ピツクアップ6には半
導体レーザ13を内蔵しており、光ビックアフブ6の励
磁素子1と対向する側には、半導体レーザ13のレーザ
光が通過する対物レンズ7を設けている。そしてこの光
ピツクアップ6の対物レンズ7が光磁気ディスク4の他
面に接近した状態で移動できるように設けている。
On the other hand, an optical pickup 6 is provided which faces the excitation element 1, moves in the same direction in conjunction with the excitation element 1, and is located on the other side of the magneto-optical disk. This optical pickup 6 has a built-in semiconductor laser 13, and an objective lens 7 through which the laser beam of the semiconductor laser 13 passes is provided on the side of the optical pickup 6 facing the excitation element 1. The objective lens 7 of the optical pickup 6 is provided so that it can move close to the other surface of the magneto-optical disk 4.

第5図は光磁気記録再生装置の要部の断面図である。光
ピツクアップ6内には前記半導体レーザ13とともに対
物レンズ7を光軸方向へ移動させるアクチエータ20を
内蔵している。アクチエータ20は、環状の永久磁石1
1と、その軸心位置に配設している柱状ヨーク12aと
、永久磁石11の一側端部に配設した環状ヨーク12b
と、柱状ヨーク12aに遊嵌しであるアクチエータコイ
ル10と、このアクチエータコイル10の一側軸端部が
取り付けられていて、柱状ヨーク12aに突設させた支
軸19が摺動自在に挿通されているレンズ支持体9とで
組み立てられている。レンズ支持体9の一側即ち半導体
レーザ13のレーザ光が投射される位置には前記対物レ
ンズ7を取り付けており、他側にはレンズ支持体9を水
平状態に安定させるレンズバランサ8を取り付けている
FIG. 5 is a sectional view of the main parts of the magneto-optical recording and reproducing apparatus. The optical pickup 6 includes an actuator 20 that moves the objective lens 7 along with the semiconductor laser 13 in the optical axis direction. The actuator 20 includes an annular permanent magnet 1
1, a columnar yoke 12a disposed at its axial center position, and an annular yoke 12b disposed at one end of the permanent magnet 11.
An actuator coil 10 is loosely fitted into the columnar yoke 12a, and one shaft end of this actuator coil 10 is attached, and a support shaft 19 protruding from the columnar yoke 12a is slidably provided. It is assembled with the lens support 9 inserted therethrough. The objective lens 7 is attached to one side of the lens support 9, that is, the position where the laser beam of the semiconductor laser 13 is projected, and the lens balancer 8 for stabilizing the lens support 9 in a horizontal state is attached to the other side. There is.

このアクチエータ20はアクチエータコイルlOを励磁
すると、それと柱状ヨーク12a及び環状ヨーク12b
との間に電磁力が作用してレンズ支持体9が支軸19の
軸方向に移動して対物レンズ7は光軸方向へ移動するよ
うになっている。そしてアクチエータコイル10の励磁
電流を、光磁気ディスク4の記録面に48に投射された
レーザ光の焦点ずれに関連して制御して、記録面4aに
常にレーザ光の合焦点を得るようにレンズ支持体9を移
動させるフォーカスサーボ動作を行わせ得るようになっ
ている。なお、レーザ光の合焦点位置は励磁素子1の中
央の磁極3bの中心を通る同一線上の記録面4aに位置
させている。
When the actuator coil 1O is excited, this actuator 20 connects it to the columnar yoke 12a and the annular yoke 12b.
An electromagnetic force acts between them, so that the lens support 9 moves in the axial direction of the support shaft 19, and the objective lens 7 moves in the optical axis direction. Then, the excitation current of the actuator coil 10 is controlled in relation to the focal shift of the laser beam projected onto the recording surface 48 of the magneto-optical disk 4, so that the laser beam is always focused on the recording surface 4a. A focus servo operation for moving the lens support 9 can be performed. Note that the focused position of the laser beam is located on the recording surface 4a on the same line passing through the center of the central magnetic pole 3b of the excitation element 1.

このような光磁気記録再生装置は、記録すべき信号に対
応した電流を励磁素子1の変調コイル2へ入力して光磁
気ディスクに磁界を与えるとともに、半導体レーザ13
が出射する光強度が一定のレーザ光を光磁気ディスクに
投射して情報を記録する。またレーザ光のみを光磁気デ
ィスク4の他面に投射してその反射光の変動を検知する
ことで記録情報を再生する。なお、情報の記録時は、光
磁気ディスクに情報が既に記録されている場合は、それ
が消去されて新たな情報を記録し得、所謂オーバライド
(重ね書き)ができる。
Such a magneto-optical recording/reproducing device inputs a current corresponding to a signal to be recorded into a modulation coil 2 of an excitation element 1 to apply a magnetic field to a magneto-optical disk, and also inputs a current corresponding to a signal to be recorded into a modulation coil 2 of an excitation element 1 to apply a magnetic field to a magneto-optical disk.
Information is recorded by projecting a laser beam of constant intensity onto a magneto-optical disk. Further, recorded information is reproduced by projecting only laser light onto the other surface of the magneto-optical disk 4 and detecting fluctuations in the reflected light. Note that when recording information, if information has already been recorded on the magneto-optical disk, it can be erased and new information can be recorded, so that so-called override (overwriting) can be performed.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

前述したように従来の光磁気記録再生装置は、レーザ光
のフォーカスサーボを行うためのアクチエータ20に永
久磁石11を用いているから、その漏洩磁束Φ1が第5
図に破線で示すように光磁気ディスク4を貫通して励磁
素子lのヨーク3内を通り永久磁石11に還流すること
になる。そのため、その漏洩磁束Φ工の方向とヨーク3
内に発生している磁界の方向とが一致している場合には
、光磁気ディスク4に与えられる磁界が強くなり、反対
に漏洩磁束とヨーク3内の磁界の方向とが不一致である
場合には光磁気ディスク4に与えられる磁界が弱くなる
。それにより、光磁気ディスク4に記録する情報に磁界
が対応せず記録精度が低下するという問題がある。その
ような問題を解決すべく漏洩磁束Φ1と相殺する電流を
変調コイル2に流すことも考えられるが、そうするとコ
イルの電流が過大になり励磁素子1が過熱するという問
題があり、また励磁素子1による磁界の極性を反転させ
る時間が長くなるという問題がある。
As mentioned above, since the conventional magneto-optical recording/reproducing device uses the permanent magnet 11 in the actuator 20 for focusing servo of the laser beam, the leakage magnetic flux Φ1 is
As shown by the broken line in the figure, the current passes through the magneto-optical disk 4, passes through the yoke 3 of the excitation element 1, and returns to the permanent magnet 11. Therefore, the direction of the leakage magnetic flux Φ and the yoke 3
If the direction of the magnetic field generated within the yoke matches, the magnetic field applied to the magneto-optical disk 4 will become stronger; on the other hand, if the leakage magnetic flux does not match the direction of the magnetic field within the yoke The magnetic field applied to the magneto-optical disk 4 becomes weaker. As a result, there is a problem that the magnetic field does not correspond to the information recorded on the magneto-optical disk 4, resulting in a decrease in recording accuracy. In order to solve such a problem, it is conceivable to flow a current through the modulation coil 2 to offset the leakage magnetic flux Φ1, but in this case, there is a problem that the current in the coil becomes excessive and the excitation element 1 overheats. There is a problem in that it takes a long time to reverse the polarity of the magnetic field.

本発明は斯かる問題に鑑み、アクチエータからの漏洩磁
束により情報の記録精度が損なわれず情報記録時の磁界
の極性反転時間が短い光磁気記録再生装置を提供するこ
とを目的とする。
In view of such problems, it is an object of the present invention to provide a magneto-optical recording/reproducing device in which the recording accuracy of information is not impaired by leakage magnetic flux from the actuator and the polarity reversal time of the magnetic field during information recording is short.

〔課題を解決するだめの手段〕[Failure to solve the problem]

本発明に係る光磁気記録再生装置は、記録すべき情報の
信号を入力する励磁素子に、その励磁素子に流入するア
クチエータからの漏洩磁束に反発する磁束を発生させる
反発磁界巻線を配設する。
In the magneto-optical recording and reproducing apparatus according to the present invention, a repulsion magnetic field winding that generates a magnetic flux repelling the leakage magnetic flux from the actuator flowing into the excitation element is disposed in the excitation element into which a signal of information to be recorded is input. .

〔作用〕[Effect]

励磁素子で発生した磁界は光磁気ディスクに与えられる
。反発磁界巻線はアクチエータから励磁素子に流入した
漏洩磁束を相殺する磁界を発生する。
The magnetic field generated by the excitation element is applied to the magneto-optical disk. The repulsion magnetic field winding generates a magnetic field that cancels leakage magnetic flux flowing into the excitation element from the actuator.

これにより、励磁素子に流入した漏洩磁束が相殺される
This cancels out the leakage magnetic flux that has flowed into the excitation element.

〔実施例〕〔Example〕

以下本発明をその実施例を示す図面によって詳述する。 The present invention will be described in detail below with reference to drawings showing embodiments thereof.

第1図は本発明に係る光磁気記録再生装置の模式的斜視
図である。ディスクモータ14により光磁気ディスク4
が回転するようになっている。励磁素子支持アーム15
の先端側下面には、情報の記録。
FIG. 1 is a schematic perspective view of a magneto-optical recording and reproducing apparatus according to the present invention. The magneto-optical disk 4 is driven by the disk motor 14.
is set to rotate. Exciting element support arm 15
Information is recorded on the lower surface of the tip.

消去用のバイアス磁界を発生する励磁素子1を取り付け
ている。励磁素子lは3つの磁極3a、3b、3cを有
するE字状のヨーク3の中央の磁極3bに、記録する信
号を入力する変調コイル2を巻回している。この励磁素
子1は磁極3a、3b、3cの並設方向を光磁気ディス
ク4のトラック方向とし、また磁極3a、3b、3(を
光磁気ディスクの一面と対向するように位置決めされて
いる。
An excitation element 1 that generates a bias magnetic field for erasing is attached. In the excitation element 1, a modulation coil 2 for inputting a signal to be recorded is wound around a central magnetic pole 3b of an E-shaped yoke 3 having three magnetic poles 3a, 3b, and 3c. In this excitation element 1, the direction in which the magnetic poles 3a, 3b, and 3c are arranged in parallel is the track direction of the magneto-optical disk 4, and the magnetic poles 3a, 3b, and 3 are positioned so as to face one surface of the magneto-optical disk.

またヨーク3の上部外周面には、ヨーク3を囲繞してい
る反発磁界巻線21を巻回している。この反発磁界巻線
21はヨーク3に流入した後述するアクチエータ20か
らの漏洩磁束を相殺すべき磁界を発生するように所要巻
回数で巻回され、所定の励磁電源に接続される。
Further, a repulsion magnetic field winding 21 surrounding the yoke 3 is wound around the upper outer peripheral surface of the yoke 3. This repulsion magnetic field winding 21 is wound with a required number of turns so as to generate a magnetic field that cancels leakage magnetic flux from an actuator 20, which will be described later, flowing into the yoke 3, and is connected to a predetermined excitation power source.

この励磁素子lは、励磁素子支持アーム15を、その長
寸方向と直交する矢符方向へ移動させることにより、光
磁気ディスク4の一面に接近した状態で光磁気ディスク
4の径方向へ移動するようになっている。
This excitation element l is moved in the radial direction of the magneto-optical disk 4 while approaching one surface of the magneto-optical disk 4 by moving the excitation element support arm 15 in the direction of the arrow perpendicular to the longitudinal direction of the excitation element l. It looks like this.

一方、励磁素子1と対向しており、それと連動して同方
向へ移動する光ピツクアップ6を設けている。この光ピ
ツクアップ6には半導体レーザ13を内蔵しており、光
ピンクアップ6の励磁素子lと対向する側には、半導体
レーザ13のレーザ光が通過する対物レンズ7を設けて
いる。そして、この光ピンクアップ6は対物レンズ7が
光磁気ディスク4の他面に接近した状態で移動するよう
に設けられている。
On the other hand, an optical pickup 6 is provided which faces the excitation element 1 and moves in the same direction in conjunction with it. This optical pickup 6 has a built-in semiconductor laser 13, and an objective lens 7 through which the laser light of the semiconductor laser 13 passes is provided on the side of the optical pickup 6 facing the excitation element 1. The optical pink-up 6 is provided so that the objective lens 7 moves close to the other surface of the magneto-optical disk 4.

第2図は発明要部の断面図である。光ピツクアップ6内
には前記半導体レーザ13とともに対物レンズを光軸方
向へ移動させるアクチエータ20を内蔵している。この
アクチエータ20は環状の永久磁石11と、その軸心位
置に配設している柱状ヨーク12aと、永久磁石11の
一側端部に配設した環状ヨーク12bと、柱状コーク1
2aに遊嵌しであるアクチエータコイル10と、このア
クチエータコイル10の一側軸端部が取り付けられてい
て、柱状ヨーク12aに突設された支軸19が摺動自在
に挿通されているレンズ支持体9とで組み立てられてい
る。レンズ支持体9の一例、即ち半導体レーザ13のレ
ーザ光が投射される位置には前記対物レンズ7を取り付
けており、他側にはレンズ支持体9を水平状態に安定さ
せるレンズバランサ8を取り付けている。
FIG. 2 is a sectional view of the main parts of the invention. The optical pickup 6 includes an actuator 20 that moves the objective lens along with the semiconductor laser 13 in the optical axis direction. This actuator 20 includes an annular permanent magnet 11, a columnar yoke 12a disposed at its axial center position, an annular yoke 12b disposed at one end of the permanent magnet 11, and a columnar cork 1.
An actuator coil 10 is loosely fitted to 2a, and one shaft end of this actuator coil 10 is attached, and a support shaft 19 protruding from the columnar yoke 12a is slidably inserted therein. It is assembled with a lens support 9. An example of the lens support 9 is that the objective lens 7 is attached to the position where the laser beam of the semiconductor laser 13 is projected, and a lens balancer 8 that stabilizes the lens support 9 in a horizontal state is attached to the other side. There is.

このアクチエータ20は、アクチエータコイル10を励
磁すると、それと柱状ヨーク12a及び環状ヨーク12
bとの間に電磁力が作用して、レンズ支持体9が支軸1
9の軸方向に移動して対物レンズ7を光軸方向へ移動さ
せるようになっている。そしてアクチエータコイル10
の励磁電流を、光磁気ディスク4の記録面4aに投射さ
れたレーザ光の焦点ずれに関連して制御して、記録面4
aにレーザ光の合焦点を常に得るようにレンズ支持体9
を移動させるフォーカスサーボ動作を行うようになって
いる。
When the actuator coil 10 is excited, this actuator 20 connects it to the columnar yoke 12a and the annular yoke 12.
An electromagnetic force acts between the lens support 9 and the support shaft 1.
9 to move the objective lens 7 in the optical axis direction. and actuator coil 10
The excitation current is controlled in relation to the focal shift of the laser beam projected onto the recording surface 4a of the magneto-optical disk 4.
Lens support 9 so that the laser beam is always focused at point a
A focus servo operation is performed to move the

なお、レーザ光の合焦点位置は励磁素子1の中央の磁極
3bの中心を通る同一線上の記録面4aに位置させてい
る。
Note that the focused position of the laser beam is located on the recording surface 4a on the same line passing through the center of the central magnetic pole 3b of the excitation element 1.

このように構成した光磁気記録再生装置は、光磁気ディ
スク4を回転させて、記録すべき信号に対応した電流を
励磁素子1の変調コイル2へ入力して光磁気ディスクの
一面に磁界を与えるとともに、半導体レーザ13が出射
する光強度が一定のレーザ光を光磁気ディスク4の他面
に投射して情報を記録する。またレーザ光のみを光磁気
ディスクの他面に投射し、その反射光の変動を検知する
ことにより光磁気ディスク4の記録情報を再生する。
The magneto-optical recording and reproducing apparatus configured in this manner rotates the magneto-optical disk 4, inputs a current corresponding to the signal to be recorded into the modulation coil 2 of the excitation element 1, and applies a magnetic field to one surface of the magneto-optical disk. At the same time, information is recorded by projecting a laser beam of constant light intensity emitted by the semiconductor laser 13 onto the other surface of the magneto-optical disk 4. Furthermore, only the laser beam is projected onto the other surface of the magneto-optical disk, and the recorded information on the magneto-optical disk 4 is reproduced by detecting fluctuations in the reflected light.

なお、情報の記録時に、既に光磁気ディスクに情報が記
録されている場合は、それが消去されて新たな情報が記
録され、所謂オーバライド(重ね書き)ができる。
Note that when information is recorded, if information has already been recorded on the magneto-optical disk, it is erased and new information is recorded, so that so-called override (overwriting) can be performed.

ところで、アクチエータ20の永久磁石11で生じた漏
洩磁束φ1は、光磁気ディスク4を貫通して、励磁素子
1のヨーク3の中央の磁極3bに流入して再び永久磁石
11に戻る破線で示す経路で還流することになる。
By the way, the leakage magnetic flux φ1 generated in the permanent magnet 11 of the actuator 20 passes through the magneto-optical disk 4, flows into the central magnetic pole 3b of the yoke 3 of the excitation element 1, and returns to the permanent magnet 11 again through the path shown by the broken line. This will result in reflux.

一方、反発磁界巻線21は、その励磁により、ヨーク3
内に流入した漏洩磁束を相殺すべき漏洩磁束は逆橿性の
磁゛界を発生する。そしてその反発磁界によって生じた
磁束Φ2は一点鎖線で示すようにヨーク3の中央の磁極
3bを通って還流することになる。それ故、ヨーク3内
に流入した漏洩磁束φ1は、反発磁界による磁束Φ2で
相殺されて、励磁素子1が発生する磁界の強さは漏洩磁
束Φ1の影響をうけて変化しない。
On the other hand, due to its excitation, the repulsion magnetic field winding 21 causes the yoke 3 to
The leakage magnetic flux that should cancel the leakage magnetic flux that has flowed into the inside generates a reverse radial magnetic field. The magnetic flux Φ2 generated by the repulsive magnetic field flows back through the magnetic pole 3b at the center of the yoke 3, as shown by the dashed line. Therefore, the leakage magnetic flux φ1 flowing into the yoke 3 is canceled out by the magnetic flux φ2 due to the repulsive magnetic field, and the strength of the magnetic field generated by the excitation element 1 does not change due to the influence of the leakage magnetic flux φ1.

したがって、変調コイル2に入力した信号による磁界の
みに関連して光磁気ディスク4に情報を高精度に記録す
ることができ、信転性が高い光磁気記録再生装置を提供
できることになる。また励磁素子1に流入した漏洩磁束
Φ1を相殺すべき磁束を、変調コイル2に電流を流して
発生させるものでないから、コイル電流が過大にならず
励磁素子1が温度上昇することもない。
Therefore, information can be recorded on the magneto-optical disk 4 with high precision only in relation to the magnetic field caused by the signal input to the modulation coil 2, and a magneto-optical recording/reproducing device with high reliability can be provided. Furthermore, since the magnetic flux that should offset the leakage magnetic flux Φ1 flowing into the excitation element 1 is not generated by passing current through the modulation coil 2, the coil current does not become excessive and the temperature of the excitation element 1 does not rise.

第3図は本発明の他の実施例を示す発明要部の斜視図で
ある。励磁素子1のヨーク3の中央の磁極3bに、その
基部側に反発磁界巻線21を位置させており、それとと
もに変調巻線2を巻回している。
FIG. 3 is a perspective view of the essential parts of another embodiment of the invention. A repulsion magnetic field winding 21 is located on the base side of the central magnetic pole 3b of the yoke 3 of the excitation element 1, and a modulation winding 2 is wound therewith.

このように同一磁極に、変調巻線2と反発磁界巻′Ia
21とを配設してもヨーク3に流入したアクチエータ2
0からの漏洩磁束を相殺でき、ヨーク3を囲繞するよう
に設けた場合と同様の効果が得られる。
In this way, the modulation winding 2 and the repulsion magnetic field winding 'Ia are connected to the same magnetic pole.
Actuator 2 flowing into yoke 3 even if 21 is arranged.
The leakage magnetic flux from the yoke 3 can be canceled out, and the same effect as when the yoke 3 is provided surrounding the yoke 3 can be obtained.

そして漏洩磁束が比較的少ない場合には効果的である。This is effective when the leakage magnetic flux is relatively small.

〔発明の効果〕〔Effect of the invention〕

以上詳述したように本発明は、アクチエータの永久磁石
から励磁素子に流入した漏洩磁束を相殺させ得るから、
情報記録時に励磁素子が発生する磁界の極性反転時間を
短縮できる。また、変調コイルに漏洩磁束を相殺させる
電流を流さないから、励磁素子が過熱しない。
As detailed above, the present invention can cancel out the leakage magnetic flux flowing into the excitation element from the permanent magnet of the actuator.
The polarity reversal time of the magnetic field generated by the excitation element during information recording can be shortened. Furthermore, since no current is passed through the modulation coil to offset the leakage magnetic flux, the excitation element does not overheat.

したがって、本発明によれば、光磁気ディスクに情報を
高精度に記録し得て、信頬性が高く、温度上昇が少ない
光磁気記録再生装置を提供できる優れた効果を奏する。
Therefore, according to the present invention, it is possible to provide a magneto-optical recording and reproducing device that can record information on a magneto-optical disk with high accuracy, has high reliability, and has a small temperature rise.

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

第1図は本発明に係る光磁気記録再生装置の模式的斜視
図、第2図はその発明要部の断面図、第3図は本発明の
他の実施例を示す発明要部の斜視図、第4図は従来の光
磁気記録再生装置の模式的斜視図、第5図はその装置要
部の断面図である。 1・・・励磁素子  2・・・変調コイル  3・・・
ヨーク  4・・・光磁気ディスク  6・・・光ピツ
クアップ  11・・・永久磁石  12b・・・環状
ヨーク  13・・・半導体レーザ  20・・・アク
チエータ  21・・・反発磁界巻線 なお、図中、同一符号は、同一、又は相当部分を示す。
FIG. 1 is a schematic perspective view of a magneto-optical recording and reproducing apparatus according to the present invention, FIG. 2 is a cross-sectional view of the main part of the invention, and FIG. 3 is a perspective view of the main part of the invention showing another embodiment of the invention. , FIG. 4 is a schematic perspective view of a conventional magneto-optical recording/reproducing device, and FIG. 5 is a sectional view of the main part of the device. 1... Excitation element 2... Modulation coil 3...
Yoke 4... Magneto-optical disk 6... Optical pickup 11... Permanent magnet 12b... Annular yoke 13... Semiconductor laser 20... Actuator 21... Repulsion magnetic field winding In the figure, The same reference numerals indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】 1、装着された光磁気ディスクの一面側に情報の記録、
消去用の磁界を発生する励磁素子を、他面側に前記光磁
気ディスクへの投射光の焦点を調整すべく磁力を用いて
なるアクチエータを夫々位置させて情報を記録、再生す
る光磁気記録再生装置において、 前記励磁素子に、該励磁素子に流入する前 記アクチエータからの漏洩磁束を相殺すべき磁束を発生
させる反発磁界巻線を設けたことを特徴とする光磁気記
録再生装置。
[Claims] 1. Recording information on one side of the mounted magneto-optical disk;
Magneto-optical recording and reproducing that records and reproduces information by positioning an excitation element that generates a magnetic field for erasure and an actuator that uses magnetic force to adjust the focus of the light projected onto the magneto-optical disk on the other side. A magneto-optical recording and reproducing apparatus, characterized in that the excitation element is provided with a repulsion magnetic field winding that generates a magnetic flux that should offset leakage magnetic flux from the actuator flowing into the excitation element.
JP28060288A 1988-11-07 1988-11-07 Magneto-optical recording and reproducing device Pending JPH02126403A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28060288A JPH02126403A (en) 1988-11-07 1988-11-07 Magneto-optical recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28060288A JPH02126403A (en) 1988-11-07 1988-11-07 Magneto-optical recording and reproducing device

Publications (1)

Publication Number Publication Date
JPH02126403A true JPH02126403A (en) 1990-05-15

Family

ID=17627320

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28060288A Pending JPH02126403A (en) 1988-11-07 1988-11-07 Magneto-optical recording and reproducing device

Country Status (1)

Country Link
JP (1) JPH02126403A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0604159A2 (en) * 1992-12-21 1994-06-29 Canon Kabushiki Kaisha Magneto-optical recording apparatus

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0604159A2 (en) * 1992-12-21 1994-06-29 Canon Kabushiki Kaisha Magneto-optical recording apparatus
EP0604159A3 (en) * 1992-12-21 1994-12-14 Canon Kk Magneto-optical recording apparatus.

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