JPH034980Y2 - - Google Patents

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Publication number
JPH034980Y2
JPH034980Y2 JP1983016566U JP1656683U JPH034980Y2 JP H034980 Y2 JPH034980 Y2 JP H034980Y2 JP 1983016566 U JP1983016566 U JP 1983016566U JP 1656683 U JP1656683 U JP 1656683U JP H034980 Y2 JPH034980 Y2 JP H034980Y2
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JP
Japan
Prior art keywords
magnetic field
signal
thin film
coil
laser beam
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.)
Expired
Application number
JP1983016566U
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Japanese (ja)
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JPS59125728U (en
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Priority to JP1656683U priority Critical patent/JPS59125728U/en
Publication of JPS59125728U publication Critical patent/JPS59125728U/en
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Description

【考案の詳細な説明】 本考案は垂直磁化薄膜にレーザ光と磁場を印加
して信号を記録するようにした光磁気記録装置に
関する。
[Detailed Description of the Invention] The present invention relates to a magneto-optical recording device that records signals by applying a laser beam and a magnetic field to a perpendicularly magnetized thin film.

従来の、この種磁場変調型光磁気記録用ヘツド
装置として第1図に示すものがあつた。図面にお
いて、Aは表面に垂直磁化薄膜が形成されたデイ
スクで、駆動体により円周方向に回転する。Bは
レーザ光Baを常に垂直磁化薄膜上に集光するた
めのフオーカスアクチユエータで、該アクチユエ
ータCはレーザ光Baを集光するレンズ系Dと、
該レンズ系Dを収納する非磁性体の鏡筒Eと、該
鏡筒Eに巻装されたフオーカスコイルFと、該フ
オーカスコイルFを駆動する磁気回路Gとで構成
されている。Hは信号磁場発生用コイルで、該コ
イルHは連結具IによりデイスクAを介してフオ
ーカスアクチユエータCに対向して配置される。
尚、発振器B、フオーカスアクチユエータC、信
号磁場発生用コイルHは信号記録再生時、一体と
なつてデイスクAの系方向に移動する。
A conventional magnetic field modulation type magneto-optical recording head device of this type is shown in FIG. In the drawings, A is a disk having a perpendicularly magnetized thin film formed on its surface, and is rotated in the circumferential direction by a driver. B is a focus actuator for always focusing the laser beam Ba on the perpendicularly magnetized thin film, and the actuator C includes a lens system D for focusing the laser beam Ba;
It consists of a non-magnetic lens barrel E that houses the lens system D, a focus coil F wound around the lens barrel E, and a magnetic circuit G that drives the focus coil F. Reference numeral H denotes a signal magnetic field generating coil, and the coil H is arranged by a connector I to face the focus actuator C via the disk A.
The oscillator B, the focus actuator C, and the signal magnetic field generating coil H move together in the direction of the disk A during signal recording and reproduction.

次に上記の動作について説明すると、発振器B
から射出されたレーザ光Baはレンズ系Dによつ
てデイスクAの垂直磁化薄膜上に収束され微小な
スポツトを結ばせる。この際、デイスクAの面ぶ
れ等があるとフオーカスコイルFに流れる制御信
号と磁気回路Gの磁束とによつてレンズ系Dを上
下方向(レーザ光Baの光軸方向)に移動してデ
イスクA上に常にスポツトが結ばれるように制御
する。このようにしてスポツトの結ばれた集光点
はレーザ光Baの光エネルギーによつて温度が上
昇し、磁性膜の性質によつて保磁力HCが減少す
る。このとき外部の信号磁場発生用コイルHから
当該集光点に保磁力HCを超える磁場HBを印加す
ると、垂直磁化薄膜内の自発磁化MSの向きが磁
場HBの方向となる。そしてスポツト通過後の垂
直磁化薄膜の冷却に伴つてスポツト通過部分の保
磁力HCが再び増加し自発磁化MSの向きが磁場HB
の方向に固定されるので磁場HBの方向に信号
(ピツト)が記録される。従つて、磁場HBの向き
は信号磁場発生用コイルHに印加される信号電流
の向きにより決定されるので、スポツト通過部分
の自発磁化MSの向きは、上記の信号電流の向き
により決定されることになる。このようにして垂
直磁化薄膜に記録された信号(ピツト)は、反射
光偏向面の回転角の差(カー効果)によつて読み
とることができる。
Next, to explain the above operation, oscillator B
The laser beam Ba emitted from the lens system D is focused onto the perpendicularly magnetized thin film of the disk A to form a minute spot. At this time, if there is surface wobbling of the disk A, the control signal flowing to the focus coil F and the magnetic flux of the magnetic circuit G move the lens system D in the vertical direction (in the direction of the optical axis of the laser beam Ba), and the disk Control is performed so that the spot is always connected on A. The temperature of the focused point where the spots are connected increases due to the optical energy of the laser beam Ba, and the coercive force H C decreases depending on the properties of the magnetic film. At this time, when a magnetic field H B exceeding a coercive force H C is applied to the focal point from an external signal magnetic field generating coil H, the direction of the spontaneous magnetization M S in the perpendicularly magnetized thin film becomes the direction of the magnetic field H B. Then, as the perpendicularly magnetized thin film cools after passing through the spot, the coercive force H C of the part passing through the spot increases again, and the direction of the spontaneous magnetization M S changes according to the magnetic field H B
Since it is fixed in the direction of the magnetic field H B , a signal (pit) is recorded in the direction of the magnetic field H B. Therefore, since the direction of the magnetic field H B is determined by the direction of the signal current applied to the signal magnetic field generating coil H, the direction of the spontaneous magnetization M S of the spot passing portion is determined by the direction of the above signal current. That will happen. The signals (pits) recorded in the perpendicularly magnetized thin film in this manner can be read by the difference in rotation angle of the reflected light deflection plane (Kerr effect).

しかしながら従来の光磁気記録装置は上記のよ
うに、レーザ光Baを集光するフオーカスアクチ
ユエータCと、記録信号を印加する信号磁場発生
用コイルHとがデイスクAを介して両側に対設し
ているので、両者を相互に固定しなければならな
い。また、信号磁場発生用コイルHがデイスクA
に対して上下方向に移動不可能なるように配置さ
れているので、デイスクAの面ぶれ(上下動)に
対して追従することができず、垂直磁化薄膜面で
の磁場強度が大きく変動し記録ビツトの大きさが
変化してしまうことがある。斯かる事態を避ける
ため信号磁場発生用コイルHをデイスクAに近づ
けすぎるとデイスクAが面振れにより衝突するお
それがある。更にフオーカスアクチユエータCと
信号磁場発生用コイルHとをデイスクAの両側に
配置するので、ヘツド全体が大型化し重くなると
いう欠点があつた。
However, in the conventional magneto-optical recording device, as described above, the focus actuator C that focuses the laser beam Ba and the signal magnetic field generating coil H that applies the recording signal are arranged oppositely on both sides with the disk A interposed between them. Therefore, both must be fixed to each other. In addition, the signal magnetic field generation coil H is connected to the disk A.
Since it is arranged so that it cannot move vertically relative to the disk A, it is unable to follow the surface wobbling (vertical movement) of disk A, and the magnetic field strength on the perpendicularly magnetized thin film surface fluctuates greatly, causing recording. The size of the bit may change. In order to avoid such a situation, if the signal magnetic field generating coil H is brought too close to the disk A, there is a risk that the disk A will collide due to surface runout. Furthermore, since the focus actuator C and the signal magnetic field generating coil H are arranged on both sides of the disk A, there is a drawback that the entire head becomes large and heavy.

そこで、このような欠点を解消するものとし
て、従来、信号磁場発生用コイルをフオーカスア
クチユエータのレンズ系の近傍である同一側に配
置することにより、デイスクの面ぶれに対して磁
場発生用コイルも同時に追従させるようにし、垂
直磁化薄膜面での磁場強度の変動を小さくするよ
うにしたものが存在した。
Therefore, in order to solve this problem, conventionally, the coil for generating the signal magnetic field is placed on the same side near the lens system of the focus actuator. There was one in which the coil was made to follow the magnetic field at the same time, thereby reducing fluctuations in the magnetic field strength on the perpendicularly magnetized thin film surface.

しかしながら、上記の従来技術によれば、信号
磁場発生用コイルとレンズ系を駆動するためのフ
オーカスアクチユエータとが近接して設けられて
いるため、磁気的に悪影響を及ぼすという問題を
有していた。そのために信号磁場発生用コイルで
発生した磁束を、レーザ光の集光点に有効に集中
させることができないという問題を有していた。
However, according to the above-mentioned conventional technology, since the signal magnetic field generation coil and the focus actuator for driving the lens system are provided in close proximity, there is a problem that there is an adverse magnetic effect. was. Therefore, there was a problem in that the magnetic flux generated by the signal magnetic field generating coil could not be effectively concentrated at the focal point of the laser beam.

そこで、本考案は上記のような欠点を解消する
ためになされたもので、レーザ光を垂直磁化薄膜
に集光するレンズ系と、該レンズ系を収納する非
磁性体の鏡筒と、該鏡筒の上端に巻装されたフオ
ーカスコイルとよりなる可動部と、該コイルを上
下方向に駆動するための磁界を与える固定部とし
ての磁気回路とから構成されるアクチユエータ
と、前記鏡筒の下端に巻装された信号磁場発生用
コイルとからなり、この垂直磁化薄膜にレーザ光
と磁場とを印加し、該レーザ光または磁場のうち
の一方を記録信号に対応して変化するようにし、
該薄膜に反射された該レーザ光よりフオーカスエ
ラー信号を抽出し、該フオーカスエラー信号に対
応して該レーザ光を該薄膜上に集光するレンズの
位置を制御するようにすると共に、該磁場を発生
する磁場発生手段の位置をも制御するようにした
光磁気記録装置において、前記鏡筒の外側部下端
に高透磁率材料により形成されたコアを設け、該
コアに信号磁場発生用コイルを巻装すると共に、
該コアの先端をレーザ光の集光点に集中させるよ
うに設けることにより、信号磁場発生用コイルと
レンズ系を駆動するためのアクチユエータとを同
一側に配置しながら、互いに影響を及ぼすことな
く、信号磁場発生用コイルで発生した磁束を、レ
ーザ光の集光点に集中させて、磁束の有効性を高
めることができる光磁気記録装置を提供すること
を目的とするものである。
Therefore, the present invention was devised to eliminate the above-mentioned drawbacks, and consists of a lens system that focuses laser light on a perpendicularly magnetized thin film, a non-magnetic lens barrel that houses the lens system, and a lens barrel made of a non-magnetic material that houses the lens system. An actuator consisting of a movable part consisting of a focus coil wound around the upper end of the tube, a magnetic circuit as a fixed part that provides a magnetic field to drive the coil in the vertical direction, and the lower end of the lens barrel. a signal magnetic field generating coil wound around the perpendicularly magnetized thin film, applying a laser beam and a magnetic field to the perpendicularly magnetized thin film so that either the laser beam or the magnetic field changes in accordance with the recording signal,
A focus error signal is extracted from the laser beam reflected by the thin film, and the position of a lens that focuses the laser beam on the thin film is controlled in accordance with the focus error signal. In a magneto-optical recording device that also controls the position of a magnetic field generating means that generates a magnetic field, a core formed of a high magnetic permeability material is provided at the outer lower end of the lens barrel, and a signal magnetic field generating coil is attached to the core. In addition to wrapping the
By arranging the tip of the core so as to concentrate the laser beam on the focal point of the laser beam, the signal magnetic field generating coil and the actuator for driving the lens system can be placed on the same side without affecting each other. It is an object of the present invention to provide a magneto-optical recording device that can increase the effectiveness of the magnetic flux by concentrating the magnetic flux generated by a signal magnetic field generating coil on the focal point of a laser beam.

以下、本考案を図面の実施例に基づいて説明す
ると、第2図は本考案に係る光磁気記録装置の概
略図で、図中、1は厚み方向、即ち垂直方向に磁
化される垂直磁化薄膜が表面に形成されたデイス
クで、図示しない駆動体により円周方向に回転す
る。2はレーザ光2aを射出する発振器、3はレ
ーザ光2aを垂直磁化薄膜上に集光するためのフ
オーカスアクチユエータで、該アクチユエータ3
はレーザ光2aを集光するレンズ系4と、該レン
ズ系4を収納する非磁性体の鏡筒5と、該鏡筒5
の上端に巻装されたフオーカスコイル6とよりな
る可動部と、該コイル6を上下方向に駆動するた
めの磁界を与える固定部としての磁気回路7とで
構成されてい。8は記録信号を印加する信号磁場
発生用コイルであり、9は高透磁率材料によつて
作られた中空なコアで、該コア9の外周に導線を
数回〜数十回巻装した構造で、軽量化されてい
る。そして、信号磁場発生用コイル8は中空なコ
ア9を前記鏡筒5の下端に被嵌して固定されてお
り、この場合、鏡筒5はフオーカスコイル6と信
号磁場発生用コイル8とが互いに磁気的に影響を
およぼさないような充分な長さに形成されてい
る。また、鏡筒5の下端に固定されている中空な
コア9の先端部分は、垂直磁化薄膜の方向に向か
つて先細りとなるように形成され、これによつて
信号磁場発生用コイル8で発生した磁束を、レー
ザ光2aの集光点に集中させている。
Hereinafter, the present invention will be explained based on the embodiments shown in the drawings. Fig. 2 is a schematic diagram of a magneto-optical recording device according to the present invention, in which 1 is a perpendicularly magnetized thin film magnetized in the thickness direction, that is, in the perpendicular direction. is formed on the surface, and is rotated in the circumferential direction by a driving body (not shown). 2 is an oscillator that emits a laser beam 2a; 3 is a focus actuator that focuses the laser beam 2a onto a perpendicularly magnetized thin film;
A lens system 4 that condenses the laser beam 2a, a lens barrel 5 made of a non-magnetic material that houses the lens system 4, and a lens barrel 5 that is made of a non-magnetic material.
It is composed of a movable part consisting of a focus coil 6 wound around the upper end, and a magnetic circuit 7 as a fixed part that provides a magnetic field to drive the coil 6 in the vertical direction. 8 is a signal magnetic field generation coil for applying a recording signal, and 9 is a hollow core made of a high magnetic permeability material, and has a structure in which a conducting wire is wound several times to several tens of times around the outer periphery of the core 9. And it's lighter. The signal magnetic field generating coil 8 is fixed by fitting a hollow core 9 into the lower end of the lens barrel 5. In this case, the lens barrel 5 has a focus coil 6 and a signal magnetic field generating coil 8. They are formed to have a sufficient length so that they do not influence each other magnetically. Further, the tip of the hollow core 9 fixed to the lower end of the lens barrel 5 is formed to be tapered toward the direction of the perpendicular magnetization thin film. The magnetic flux is concentrated at the focal point of the laser beam 2a.

次に上記の作用について説明すると、発振器2
から射出されたレーザ光2aはレンズ系4によつ
て集光され垂直磁化薄膜1の集光点にスポツトを
結ばせる。垂直磁化薄膜にて反射されたレーザ光
2aは図示しないフオーカスエラー信号検出装置
に案内され、そこで抽出されたフオーカスエラー
信号がフオーカスコイル6に供給される。従つ
て、フオーカスアクチユエータ3の可動部はレー
ザ光2aの光軸方向に運動し、垂直磁化薄膜とレ
ンズ系4との距離が常に一定になるようにフオー
カスサーボ装置が動作する。スポツトの結ばれた
集光点の温度はレーザ光2aの光エネルギにより
上昇し、当該集光点の保磁力が低下する。一方、
信号磁場発生用コイル8に記録信号に対応して変
化する電流を加えて上記の集光点に保磁力を超え
る磁場を印加して集光点の自発磁化の向きを磁場
の向きにし、前述したようにこの磁場の向きに従
つて信号(ビツト)を記録する。この際、信号磁
場発生用コイル8はフオーカスアクチユエータ3
の可動部と一体化されているので、デイスク1の
面ぶれがあつた場合でも、信号磁場発生用コイル
8と垂直磁化薄膜との距離は常に一定に保たれ、
上記のコイル8で発生する磁場の大きさは垂直磁
化薄膜上で一定となる。従つて、垂直磁化薄膜の
面ぶれがあつても記録されるピツトの大きさは一
定に保たれる。また、中空なコア9の先端は垂直
磁化薄膜の方向に向かつて先細りとなるように形
成されているため、これによつて信号磁場発生用
コイル8で発生した磁束を、レーザ光2aの集光
点に集中させることができるので、磁場の収束が
有効となる。
Next, to explain the above operation, the oscillator 2
The laser beam 2a emitted from the perpendicularly magnetized thin film 1 is focused by a lens system 4 to form a spot on the focused point of the perpendicularly magnetized thin film 1. The laser beam 2a reflected by the perpendicularly magnetized thin film is guided to a focus error signal detection device (not shown), and the focus error signal extracted there is supplied to the focus coil 6. Therefore, the movable part of the focus actuator 3 moves in the optical axis direction of the laser beam 2a, and the focus servo device operates so that the distance between the perpendicularly magnetized thin film and the lens system 4 is always constant. The temperature of the condensing point where the spots are connected rises due to the optical energy of the laser beam 2a, and the coercive force of the condensing point decreases. on the other hand,
A current that changes in accordance with the recording signal is applied to the signal magnetic field generating coil 8, and a magnetic field exceeding the coercive force is applied to the above-mentioned focal point to change the direction of the spontaneous magnetization of the focal point to the direction of the magnetic field, as described above. Signals (bits) are recorded according to the direction of this magnetic field. At this time, the signal magnetic field generation coil 8 is connected to the focus actuator 3.
Since it is integrated with the movable part of the disk 1, the distance between the signal magnetic field generating coil 8 and the perpendicular magnetization thin film is always kept constant even if the surface of the disk 1 is shaken.
The magnitude of the magnetic field generated by the coil 8 is constant on the perpendicularly magnetized thin film. Therefore, even if there is surface wobbling of the perpendicularly magnetized thin film, the size of the recorded pits remains constant. In addition, since the tip of the hollow core 9 is tapered toward the direction of the perpendicularly magnetized thin film, the magnetic flux generated by the signal magnetic field generating coil 8 is focused into the laser beam 2a. Since it can be concentrated at a point, convergence of the magnetic field is effective.

第3図は本考案の他実施例で、上記の実施例で
は信号磁場発生用コイル8はフオーカスアクチユ
エータ3の鏡筒5に対して同軸上に固定している
が、本実施例では鏡筒5の側方下端に所定の角度
をもつて固定すると共に、信号磁場発生用コイル
8は棒状のコア9に導線を巻装した構造となつて
いる。その他の点については前記の実施例と同様
である。
FIG. 3 shows another embodiment of the present invention. In the above embodiment, the signal magnetic field generating coil 8 is coaxially fixed to the lens barrel 5 of the focus actuator 3, but in this embodiment, The signal magnetic field generating coil 8 is fixed to the lower side end of the lens barrel 5 at a predetermined angle, and has a structure in which a conducting wire is wound around a rod-shaped core 9. The other points are the same as those of the previous embodiment.

尚、上記の実施例においては、レーザ光2aを
照射したままの状態とし、信号磁場発生用コイル
8に流れる電流を記録信号によつて変化させる磁
場変調方式としたが、逆に該コイル8に流れる電
流を変化させず、レーザ光2aの照射を記録信号
に対応して変化させる光変調方式としても本考案
は応用可能である。この場合、コイル8にかえて
永久磁石を磁場発生手段としてもよい。更に磁場
発生手段を駆動するアクチユエータをレンズ系4
を駆動するフオーカスアクチユエータ3と独立し
たものでもよい。
In the above embodiment, the laser beam 2a remains irradiated and the magnetic field modulation method is used in which the current flowing through the signal magnetic field generating coil 8 is changed according to the recording signal. The present invention can also be applied to an optical modulation method that changes the irradiation of the laser beam 2a in accordance with the recording signal without changing the flowing current. In this case, instead of the coil 8, a permanent magnet may be used as the magnetic field generating means. Further, an actuator for driving the magnetic field generating means is connected to the lens system 4.
The focus actuator 3 may be independent from the focus actuator 3 that drives the focus actuator 3.

本考案は叙上のように、レーザ光を垂直磁化薄
膜に集光するレンズ系と、該レンズ系を収納する
非磁性体の鏡筒と、該鏡筒の上端に巻装されたフ
オーカスコイルとよりなる可動部と、該コイルを
上下方向に駆動するための磁界を与える固定部と
しての磁気回路とから構成されるアクチユエータ
と、前記鏡筒の下端に巻装された信号磁場発生用
コイルとからなり、この垂直磁化薄膜にレーザ光
と磁場とを印加し、該レーザ光または磁場のうち
の一方を記録信号に対応して変化するようにし、
該薄膜に反射された該レーザ光よりフオーカスエ
ラー信号を抽出し、該フオーカスエラー信号に対
応して該レーザ光を該薄膜上に集光するレンズの
位置を制御するようにすると共に、該磁場を発生
する磁場発生手段の位置をも制御するようにした
光磁気記録装置において、前記鏡筒の外側部下端
に高透磁率材料により形成されたコアを設け、該
コアに信号磁場発生用コイルを巻装すると共に、
該コアの先端をレーザ光の集光点に集中させるよ
うに設けたものである。
As mentioned above, the present invention consists of a lens system that focuses laser light onto a perpendicularly magnetized thin film, a non-magnetic lens barrel that houses the lens system, and a focus coil that is wound around the upper end of the lens barrel. an actuator consisting of a movable part, a magnetic circuit as a fixed part that applies a magnetic field to drive the coil in the vertical direction; and a signal magnetic field generating coil wound around the lower end of the lens barrel. A laser beam and a magnetic field are applied to the perpendicularly magnetized thin film, and either the laser beam or the magnetic field is changed in accordance with the recording signal,
A focus error signal is extracted from the laser beam reflected by the thin film, and the position of a lens that focuses the laser beam on the thin film is controlled in accordance with the focus error signal. In a magneto-optical recording device that also controls the position of a magnetic field generating means that generates a magnetic field, a core formed of a high magnetic permeability material is provided at the outer lower end of the lens barrel, and a signal magnetic field generating coil is attached to the core. In addition to wrapping the
The tip of the core is provided so as to concentrate the laser beam at the focal point.

従つて、信号磁場発生用コイル8とレンズ系4
を駆動するためのアクチユエータ3とを同一側に
配置して、装置全体の小型軽量化を図りながら、
互いに影響を及ぼすことなく磁場発生用コイル8
で発生した磁束を、レーザ光2aの集光点に集中
させることができるので、磁場の収束が有効とな
る。また、デイスクに面ぶれがあつても印加され
る磁場の強さは一定となり、記録される信号の
S/Nが向上する。
Therefore, the signal magnetic field generating coil 8 and the lens system 4
By placing the actuator 3 for driving on the same side, the entire device is made smaller and lighter.
Coil 8 for generating magnetic field without affecting each other
Since the magnetic flux generated can be concentrated at the focal point of the laser beam 2a, the convergence of the magnetic field becomes effective. Furthermore, even if the disk surface is shaken, the strength of the applied magnetic field remains constant, improving the S/N ratio of the recorded signal.

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

第1図は従来例の光磁気記録装置の概略図、第
2図、第3図は各々本考案に係る光磁気記録装置
の異なる実施例を示す概略図である。 1……デイスク、2a……レーザ光、3……フ
オーカスアクチユエータ、8……信号磁場発生用
コイル、9……コア。
FIG. 1 is a schematic diagram of a conventional magneto-optical recording device, and FIGS. 2 and 3 are schematic diagrams showing different embodiments of the magneto-optical recording device according to the present invention. DESCRIPTION OF SYMBOLS 1... Disk, 2a... Laser light, 3... Focus actuator, 8... Signal magnetic field generation coil, 9... Core.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] レーザ光を垂直磁化薄膜に集光するレンズ系
と、該レンズ系を収納する非磁性体の鏡筒と、該
鏡筒の上端に巻装されたフオーカスコイルとより
なる可動部と、該コイルを上下方向に駆動するた
めの磁界を与える固定部としての磁気回路とから
構成されるアクチユエータと、前記鏡筒の下端に
巻装された信号磁場発生用コイルとからなり、こ
の垂直磁化薄膜にレーザ光と磁場とを印加し、該
レーザ光または磁場のうちの一方を記録信号に対
応して変化するようにし、該薄膜に反射された該
レーザ光よりフオーカスエラー信号を抽出し、該
フオーカスエラー信号に対応して該レーザ光を該
薄膜上に集光するレンズの位置を制御するように
すると共に、該磁場を発生する磁場発生手段の位
置をも制御するようにした光磁気記録装置におい
て、前記鏡筒の外側部下端に高透磁率材料により
形成されたコアを設け、該コアに信号磁場発生用
コイルを巻装すると共に、該コアの先端をレーザ
光の集光点に集中させるように設けたことを特徴
とする光磁気記録装置。
A movable part consisting of a lens system that focuses laser light on a perpendicularly magnetized thin film, a non-magnetic lens barrel that houses the lens system, a focus coil wound around the upper end of the lens barrel, and the coil. The actuator consists of a magnetic circuit as a fixed part that provides a magnetic field to drive the lens vertically, and a signal magnetic field generating coil wound around the lower end of the lens barrel. Applying light and a magnetic field, causing either the laser light or the magnetic field to change in accordance with the recording signal, extracting a focus error signal from the laser light reflected on the thin film, and detecting the focus error signal. In a magneto-optical recording device, the position of a lens that focuses the laser beam on the thin film is controlled in response to an error signal, and the position of a magnetic field generating means that generates the magnetic field is also controlled. , a core made of a high magnetic permeability material is provided at the outer lower end of the lens barrel, a signal magnetic field generating coil is wound around the core, and the tip of the core is configured to focus the laser beam at a focal point. A magneto-optical recording device characterized by being provided with.
JP1656683U 1983-02-07 1983-02-07 magneto-optical recording device Granted JPS59125728U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1656683U JPS59125728U (en) 1983-02-07 1983-02-07 magneto-optical recording device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1656683U JPS59125728U (en) 1983-02-07 1983-02-07 magneto-optical recording device

Publications (2)

Publication Number Publication Date
JPS59125728U JPS59125728U (en) 1984-08-24
JPH034980Y2 true JPH034980Y2 (en) 1991-02-08

Family

ID=30147843

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1656683U Granted JPS59125728U (en) 1983-02-07 1983-02-07 magneto-optical recording device

Country Status (1)

Country Link
JP (1) JPS59125728U (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2503402Y2 (en) * 1985-02-28 1996-07-03 ソニー株式会社 Magneto-optical recording device
JPH0775086B2 (en) * 1986-11-12 1995-08-09 株式会社日立製作所 Magneto-optical recording / reproducing device

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57133503A (en) * 1981-02-10 1982-08-18 Sharp Corp Optical and magnetic recorder and reproducer

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57133503A (en) * 1981-02-10 1982-08-18 Sharp Corp Optical and magnetic recorder and reproducer

Also Published As

Publication number Publication date
JPS59125728U (en) 1984-08-24

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