JP2808597B2 - Magnetic field applying electromagnet for magneto-optical disk - Google Patents

Magnetic field applying electromagnet for magneto-optical disk

Info

Publication number
JP2808597B2
JP2808597B2 JP3987088A JP3987088A JP2808597B2 JP 2808597 B2 JP2808597 B2 JP 2808597B2 JP 3987088 A JP3987088 A JP 3987088A JP 3987088 A JP3987088 A JP 3987088A JP 2808597 B2 JP2808597 B2 JP 2808597B2
Authority
JP
Japan
Prior art keywords
magnetic field
magneto
parallel
optical disk
recording
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 - Fee Related
Application number
JP3987088A
Other languages
Japanese (ja)
Other versions
JPH01213802A (en
Inventor
英男 田中
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.)
NEC Corp
Original Assignee
Nippon Electric Co 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP3987088A priority Critical patent/JP2808597B2/en
Publication of JPH01213802A publication Critical patent/JPH01213802A/en
Application granted granted Critical
Publication of JP2808597B2 publication Critical patent/JP2808597B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related 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
    • 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
    • G11B11/10532Heads
    • G11B11/10534Heads for recording by magnetising, demagnetising or transfer of magnetisation, by radiation, e.g. for thermomagnetic recording
    • G11B11/10536Heads for recording by magnetising, demagnetising or transfer of magnetisation, by radiation, e.g. for thermomagnetic recording using thermic beams, e.g. lasers

Landscapes

  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Recording Or Reproducing By Magnetic Means (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、光磁気ディスク用磁界印加電磁石に関す
る。
Description: TECHNICAL FIELD The present invention relates to a magnetic field applying electromagnet for a magneto-optical disk.

(従来の技術) 従来の光磁気記録において記録情報を消去する場合に
は、外部磁界を記録時とは逆極性に印加し、レーザ光ビ
ームを記録時と同等の強度で記録媒体に一様に照射す
る、いわゆる一括消去が行なわれている。即ち外部磁界
印加により記録媒体の磁化状態を記録前の初期状態に戻
している。
(Prior Art) When erasing recorded information in conventional magneto-optical recording, an external magnetic field is applied with a polarity opposite to that during recording, and a laser beam is uniformly applied to the recording medium at the same intensity as during recording. Irradiation, so-called batch erasure, is performed. That is, the magnetization state of the recording medium is returned to the initial state before recording by applying an external magnetic field.

ここで、公知の外部磁界印加手段は、例えば空心コイ
ルを用いる方法、電磁石を用いる方法、あるいは永久磁
石を用いる方法がある。
Here, the known external magnetic field applying means includes, for example, a method using an air-core coil, a method using an electromagnet, and a method using a permanent magnet.

(発明が解決しようとする課題) 前述の磁界印加手段において、記録時と消去時とでは
通常数100エルステッド以上の印加磁界が必要であるた
めに、空心コイルを用いる場合にはコイルが大型化し、
これに伴って磁界切換速度が遅くなるとともに、記録媒
体とコイルとの距離を充分に接近させないと所要の印加
磁界が得られないという欠点がある。また電磁石を用い
る場合にも、磁界印加手段は大型化し、コイルのインダ
クタンスが大きいために磁界切換速度が遅いという欠点
を生じている。さらに、永久磁石を用いる場合には、機
械的な駆動手段を用いて磁界を切換えるために複雑な機
構が必要であり、この場合も磁界切換速度は遅いものと
なっている。以上述べたように、従来のいずれの外部磁
界印加手段によっても磁界切換速度は遅いために、消去
には前述の一括消去方式が用いられ、また記録する時に
は一定磁界印加中にレーザパワーを高速変調する方法が
用いられている。即ち、従来の装置では既に記録された
情報に新しい情報を高速で重ね書きするいわゆるオーバ
ーライト機能を持たせることが困難であるという問題点
がある。
(Problems to be Solved by the Invention) In the above-described magnetic field applying means, an applied magnetic field of several hundred Oersted or more is usually required at the time of recording and erasing.
Accordingly, the switching speed of the magnetic field is reduced, and a required applied magnetic field cannot be obtained unless the distance between the recording medium and the coil is sufficiently reduced. Also, when an electromagnet is used, the size of the magnetic field applying means is increased and the inductance of the coil is large, so that the magnetic field switching speed is slow. Further, when a permanent magnet is used, a complicated mechanism is required for switching the magnetic field using a mechanical driving means, and the magnetic field switching speed is also slow in this case. As described above, since the magnetic field switching speed is slow by any of the conventional external magnetic field applying means, the above-described batch erasing method is used for erasing, and when recording, the laser power is rapidly modulated during application of a constant magnetic field. Is used. That is, the conventional apparatus has a problem that it is difficult to provide a so-called overwrite function for overwriting already recorded information with new information at a high speed.

本発明の目的は、このような従来の問題点を解決して
大きい磁界の高速スイッチングを可能にする新規な外部
磁界印加手段を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a new external magnetic field applying unit that solves the conventional problems and enables high-speed switching of a large magnetic field.

(課題を解決するための手段) 本発明の光磁気ディスク用磁界印加電磁石は、光磁気
ディスクの端面部で折り返してU字形とし、前記U字形
の二つの直線部が前記光磁気ディスクの両面のそれぞれ
に対面した高透磁率磁性体と、前記高透磁率磁性体の一
部に設けられ、n個のコイルが同一方向の磁界を発生す
るように並列に接続された第1の並列コイル群と、前記
第1の並列コイル群に一端が接続され、かつ前記第1の
並列コイル群が発生する磁界とは逆方向の磁界を発生す
るように並列に接続された第2の並列コイル群とにより
構成された前記n並列の3端子コイルとを有することに
より構成される。
(Means for Solving the Problems) A magnetic field applying electromagnet for a magneto-optical disk according to the present invention is folded back at the end surface of the magneto-optical disk into a U-shape, and the two linear portions of the U-shape are formed on both sides of the magneto-optical disk. A high-permeability magnetic body facing each other, and a first parallel coil group provided on a part of the high-permeability magnetic body and having n coils connected in parallel to generate a magnetic field in the same direction. A second parallel coil group having one end connected to the first parallel coil group and connected in parallel so as to generate a magnetic field in a direction opposite to a magnetic field generated by the first parallel coil group. And the above-described n-parallel three-terminal coil.

ここで高透磁率磁性体にはフェライト(MnZn,NiZnな
ど)、パーマロイ(NiFe)、センダスト、アモルファス
(CoZr,CoZr,FeCoZr,CoNb,CoTa,CoHfなど)、鉄心など
が考えられる。
Here, as the high magnetic permeability magnetic material, ferrite (MnZn, NiZn, etc.), permalloy (NiFe), sendust, amorphous (CoZr, CoZr, FeCoZr, CoNb, CoTa, CoHf, etc.), iron core, and the like can be considered.

また、U字形の高透磁率磁性体の同心円状の中空部は
レーザ集光用レンズと光磁気媒体との間に設定し、この
中空部の内径はレーザビームが通過でき、かつトラッキ
ングによりトラック方向にレンズが動かせる程度の大き
さに設定される。また第1及び第2のn個のコイルはそ
れぞれ電気的に並列に接続され、第1及び第2のコイル
群は一方の端子が接続され、全体として3端子の電磁石
を構成する。コイルのインダクタンスは並列に接続され
ているために大幅に減少する。従って、インダクタンス
が小さいことにより、記録電流の立ち上がり時間が小さ
くなるので、磁界の切換速度を大幅に早くすることがで
きる。
The concentric hollow portion of the U-shaped high magnetic permeability magnetic material is set between the laser condensing lens and the magneto-optical medium, and the inner diameter of the hollow portion allows a laser beam to pass therethrough and is tracked by tracking. The size is set so that the lens can be moved. The first and second n coils are electrically connected in parallel, respectively, and the first and second coil groups are connected to one terminal to form a three-terminal electromagnet as a whole. The inductance of the coil is greatly reduced due to the parallel connection. Therefore, since the rise time of the recording current is reduced due to the small inductance, the switching speed of the magnetic field can be greatly increased.

(実施例) 以下、本発明の実施例について図面を参照して説明す
る。
Hereinafter, embodiments of the present invention will be described with reference to the drawings.

第1図は本発明一実施例の構成図である。図において
光磁気ディスク用磁界印加電磁石は、光磁気ディスク5
の両面のそれぞれに対向し、光ディスクの端面部で折り
返してU字形とした高透磁率磁性体1と、この高透磁率
磁性体1の途中に設けられ、電気的に並列に接続された
第1の並列コイル群2と第2の並列コイル群3とにより
構成され、第1の並列コイル群2と第2の並列コイル群
3とは一方の端子が接続されている。これらの第1の並
列コイルと第2の並列コイルとに交互に電磁石駆動回路
4から記録電流が供給される。
FIG. 1 is a configuration diagram of one embodiment of the present invention. In the figure, the magnetic field applying electromagnet for the magneto-optical disk is a magneto-optical disk 5
A high-permeability magnetic body 1 which is opposed to both sides of the optical disk and is folded at the end surface of the optical disk to form a U-shape; a first magnetic-permeability magnetic body 1 provided in the middle of the high-permeability magnetic body 1 and electrically connected in parallel; , And one terminal is connected to the first parallel coil group 2 and the second parallel coil group 3. A recording current is supplied from the electromagnet drive circuit 4 to the first parallel coil and the second parallel coil alternately.

第2図は第1図の回路図で、それぞれn本の絶縁導体
によって作られた第1の並列コイル群2と第2の並列コ
イル群3と、これらの並列コイル群を駆動する電磁石駆
動回路4とが示されている。
FIG. 2 is a circuit diagram of FIG. 1, in which a first parallel coil group 2 and a second parallel coil group 3 each made of n insulated conductors, and an electromagnet drive circuit for driving these parallel coil groups 4 is shown.

電磁石駆動回路4により、第1及び第2の並列コイル
群2,3へ交互に電流を流すことによって記録媒体の垂直
方向への印加磁界が与えられる。また高透磁率磁性体1
は膜厚3mm,長さ約20cmのものが用いられ、また第1と第
2の並列コイル群としては線径150μmのものを用い
た。なお電流値としては数100mA〜1.0Aが適当である。
このようにして構成した磁界印加手段では、コイルを電
気的に並列に接続しているためにコイルのインダクタン
スLを、1μH以下にすることが容易なため、高透磁率
磁性体1の端面から数mm離れた位置において、数100エ
ルステッドの磁界を数MHzの高速で容易に切換ることが
出来る。
By applying an electric current alternately to the first and second parallel coil groups 2 and 3 by the electromagnet drive circuit 4, an applied magnetic field in the vertical direction of the recording medium is given. In addition, high permeability magnetic material 1
A 3 mm thick film having a length of about 20 cm was used, and a first and second parallel coil group having a wire diameter of 150 μm was used. A current value of several hundred mA to 1.0 A is appropriate.
In the magnetic field applying means configured in this manner, since the coil is electrically connected in parallel, it is easy to reduce the inductance L of the coil to 1 μH or less. At a distance of mm, a magnetic field of several hundred Oersteds can be easily switched at a high speed of several MHz.

第3図は第1図の実施例に周辺系を付加した光磁気記
録再生装置の構成図で、この装置により光磁気ディスク
5への記録再生消去を行った。第3図において電磁石駆
動回路4の出力電流が第1の並列コイル群2および第2
の並列コイル群3に流れ、光磁気ディスク5の磁性薄膜
6で構成された記録媒体に上向きおよび下向きの磁界が
交互に印加される。
FIG. 3 is a block diagram of a magneto-optical recording / reproducing apparatus in which a peripheral system is added to the embodiment of FIG. 1, and recording / reproducing / erasing on the magneto-optical disk 5 is performed by this apparatus. In FIG. 3, the output current of the electromagnet drive circuit 4 is the first parallel coil group 2 and the second parallel coil group 2.
, And upward and downward magnetic fields are alternately applied to the recording medium constituted by the magnetic thin film 6 of the magneto-optical disk 5.

光磁気記録用ヘッド31は従来と同等のものであり、次
のような構成を有する。32は直線偏光のレーザ光源であ
り、例えば半導体レーザが使用される。33,34,35はビー
ムスプリッタである。レーザ光ビーム集光用レンズ36は
アクチュエータ37により支持されている。フォーカスエ
ラーおよびトラッキングエラー信号はそれぞれフォーカ
スエラー信号検出用受光素子38,トラッキングエラー信
号検出用受光素子39によってサーボ制御回路40,41に入
力され、サーボ信号となりアクチュエータ37にフィード
バックされる。再生信号は偏光フィルタ42を通過後、再
生信号用受光素子43によって検出され、再生信号増幅回
路44によって増幅される。偏光フィルタ42としてはグラ
ムトムソンプリズムを用い、再生信号検出用受光素子43
としてはPINフォトダイオードを用いた。レーザ光源32
の変調にはレーザ光源変調回路45が使用され、記録時,
消去時,再生時に合わせてレーザ光のパワーが変調され
る。
The magneto-optical recording head 31 is equivalent to a conventional one, and has the following configuration. Reference numeral 32 denotes a linearly polarized laser light source, for example, a semiconductor laser. 33, 34 and 35 are beam splitters. The laser beam focusing lens 36 is supported by an actuator 37. The focus error and tracking error signals are input to the servo control circuits 40 and 41 by the focus error signal detecting light receiving element 38 and the tracking error signal detecting light receiving element 39, respectively, and are fed back to the actuator 37 as servo signals. After passing through the polarization filter 42, the reproduction signal is detected by the light-receiving element 43 for reproduction signal and amplified by the reproduction signal amplifier circuit 44. A Gram-Thompson prism is used as the polarization filter
Used a PIN photodiode. Laser light source 32
The laser light source modulation circuit 45 is used for the modulation of
The power of the laser beam is modulated at the time of erasure and reproduction.

光磁気ディスクとして120mm径のプラスチック基板上
にスパッタ法により形成されたSiN上に、さらにTbFeCo
膜を800オングストローム厚に形成し、このTbFeCo膜上
にさらにSiNを形成したディスクを使用した。基板とし
ては予めトラックピッチ1.6μm,深さ700オングストロー
ムの溝が形成されたいわゆるプリグループ基板を用い
た。
TbFeCo on SiN formed by sputtering on a 120 mm diameter plastic substrate as a magneto-optical disk
A disk having a thickness of 800 Å and a SiN layer formed on the TbFeCo film was used. The substrate used was a so-called pre-group substrate in which a groove having a track pitch of 1.6 μm and a depth of 700 Å was formed in advance.

第4図(a)〜(c)は記録の動作モード図である。
記録媒体をキュリー温度以上に上昇できる一定強度のレ
ーザビームを照射しながら、外部磁界印加のための第1
と第2との並列コイル群2,3に第4図(b)に示すよう
な変調電流を流すことによって、記録パターンに対応し
た外部磁界が印加され、記録媒体の走行に伴なう冷却過
程で印加磁界方向に対応して、第4図(c)に示すよう
な記録磁化状態が実現される。まず線速9m/secにてディ
スク面上10mWの一定強度レーザ光を照射しながら、外部
磁界印加手段の並列コイル2,3に1MHzで、800mAの変調電
流を流したところ、良好な記録ができた。この記録トラ
ック上に新たに同一条件で記録磁界を0.5MHzで印加した
ところ、この記録磁界に対応した記録ができ、前に記録
した信号の消え残りはみられなかった。
4A to 4C are operation mode diagrams of recording.
While irradiating the recording medium with a laser beam of a constant intensity capable of raising the temperature above the Curie temperature, a first
By applying a modulation current as shown in FIG. 4 (b) to the parallel coil groups 2 and 3 of the second and the third, an external magnetic field corresponding to the recording pattern is applied, and the cooling process accompanying the running of the recording medium is performed. Thus, a recording magnetization state as shown in FIG. 4 (c) is realized corresponding to the direction of the applied magnetic field. First, while irradiating a constant-intensity laser beam of 10 mW on the disk surface at a linear velocity of 9 m / sec, a modulation current of 800 mA was passed at 1 MHz to the parallel coils 2 and 3 of the external magnetic field applying means, and good recording was possible. Was. When a recording magnetic field was newly applied to this recording track under the same conditions at 0.5 MHz, recording corresponding to this recording magnetic field was performed, and the previously recorded signal remained unerased.

第5および第6図はそれぞれ本発明の別の実施例の構
成図および回路図である。本実施例では前記第一の実施
例の3端子の並列コイル群を高透磁率磁性体1上に並列
に第1,第2および第3の並列3端子コイル7,8および9
の3個構成とし、それぞれのコイルに第1,第2および第
3の電磁石駆動回路10,11および12を接続し、この3個
の電磁石駆動回路を同一の記録クロックで駆動するよう
にした。その後、前記第一の実施例と同じ構成の光ヘッ
ドにより、オーバーライト特性を測定した結果、第一の
実施例と同等のオーバーライト特性を得た。
FIGS. 5 and 6 are a configuration diagram and a circuit diagram, respectively, of another embodiment of the present invention. In this embodiment, the first, second and third parallel three-terminal coils 7, 8 and 9 are arranged in parallel with the three-terminal parallel coil group of the first embodiment on the high-permeability magnetic body 1.
The first, second and third electromagnet drive circuits 10, 11 and 12 are connected to the respective coils, and these three electromagnet drive circuits are driven by the same recording clock. Thereafter, the overwrite characteristics were measured using an optical head having the same configuration as that of the first embodiment. As a result, overwrite characteristics equivalent to those of the first embodiment were obtained.

(発明の効果) 以上述べたように、本発明によれば光磁気ディスクの
両側に対面するU字形の高透磁率磁性体を用い、且つn
個のコイルは電気的に並列に接続されているためにイン
ダクタンスを小さくできるので、大きい磁界の高速スイ
ッチングが可能であり、且つ磁束利用効率の良い光磁気
ディスク用磁界印加電磁石を提供できる。従って、光磁
気記録再生方式では従来の一括消去を必要とせずに直接
所望の記録が可能なオーバーライト性能が実現できると
いう効果がある。
(Effects of the Invention) As described above, according to the present invention, a U-shaped high magnetic permeability magnetic material facing both sides of a magneto-optical disk is used, and n
Since the coils are electrically connected in parallel, the inductance can be reduced, so that a high-speed switching of a large magnetic field is possible, and a magnetic field applying electromagnet for a magneto-optical disk with high magnetic flux utilization efficiency can be provided. Therefore, the magneto-optical recording / reproducing method has an effect that an overwrite performance capable of directly performing a desired recording can be realized without requiring the conventional batch erasing.

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

第1図は本発明の一実施例の構成図、第2図は第1図の
回路図、第3図は第1図の実施例を光磁気ディスク装置
に適用した場合の構成図、第4図は第3図の記録の動作
モード図、第5図は本発明の別の実施例の構成図、第6
図は第5図の回路図である。 1……高透磁率磁性体、2……第1の並列コイル群、3
……第2の並列コイル群、4……電磁石駆動回路、5…
…光ディスク、6……光ディスク磁性媒体、7,8,9……
第1,第2,第3の並列3端子コイル、10,11,12……第1,第
2,第3の電磁石駆動回路、13……フリップフロップ、21
……中空部、31……光磁気記録用ヘッド、32……レーザ
光源、33,34,35……ビームスプリッタ、36……レーザ光
ビーム集光レンズ、37……アクチュエータ、38……フォ
ーカスエラー信号検出用受光素子、39……トラッキング
エラー信号検出用受光素子、40,41……サーボ制御回
路、42……偏光フィルタ、43……再生信号検出用受光素
子、44……増幅回路、45……レーザ光源変調回路。
FIG. 1 is a block diagram of one embodiment of the present invention, FIG. 2 is a circuit diagram of FIG. 1, FIG. 3 is a block diagram of a case where the embodiment of FIG. 1 is applied to a magneto-optical disk drive, FIG. FIG. 3 is a diagram showing a recording operation mode in FIG. 3, FIG. 5 is a block diagram showing another embodiment of the present invention, and FIG.
The figure is the circuit diagram of FIG. 1. High magnetic permeability magnetic body 2. First parallel coil group 3,
... A second parallel coil group, 4... An electromagnet drive circuit, 5.
... optical disk, 6 ... optical disk magnetic medium, 7,8,9 ...
First, second, third parallel three-terminal coils, 10, 11, 12, ... first, first
2, a third electromagnet drive circuit, 13 ... flip-flop, 21
… Hollow part, 31… Head for magneto-optical recording, 32… Laser light source, 33, 34, 35… Beam splitter, 36… Laser beam focusing lens, 37… Actuator, 38… Focus error Light receiving element for signal detection, 39 ... Light receiving element for tracking error signal detection, 40, 41 ... Servo control circuit, 42 ... Polarizing filter, 43 ... Light receiving element for reproduction signal detection, 44 ... Amplifier circuit, 45 ... ... Laser light source modulation circuit.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】光磁気ディスクの端面部で折り返してU字
形とし、前記U字形の二つの直線部が前記光磁気ディス
クの両面のそれぞれに対面した高透磁率磁性体と、前記
高透磁率磁性体の一部に設けられ、n個のコイルが同一
方向の磁界を発生するように並列に接続された第1の並
列コイル群と、前記第1の並列コイル群に一端が接続さ
れ、かつ前記第1の並列コイル群が発生する磁界とは逆
方向の磁界を発生するように並列に接続された第2の並
列コイル群とにより構成された前記n並列の3端子コイ
ルとを有することを特徴とする光磁気ディスク用磁界印
加電磁石。
1. A high-permeability magnetic material which is folded at an end surface of a magneto-optical disk to form a U-shape, wherein two straight portions of the U-shape face each of both surfaces of the magneto-optical disk, and the high-permeability magnetic material. A first parallel coil group provided on a part of the body, wherein n coils are connected in parallel so as to generate a magnetic field in the same direction; one end connected to the first parallel coil group; A second parallel coil group connected in parallel so as to generate a magnetic field in a direction opposite to a magnetic field generated by the first parallel coil group, and the n-parallel three-terminal coil. A magnetic field applying electromagnet for a magneto-optical disk.
JP3987088A 1988-02-22 1988-02-22 Magnetic field applying electromagnet for magneto-optical disk Expired - Fee Related JP2808597B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3987088A JP2808597B2 (en) 1988-02-22 1988-02-22 Magnetic field applying electromagnet for magneto-optical disk

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3987088A JP2808597B2 (en) 1988-02-22 1988-02-22 Magnetic field applying electromagnet for magneto-optical disk

Publications (2)

Publication Number Publication Date
JPH01213802A JPH01213802A (en) 1989-08-28
JP2808597B2 true JP2808597B2 (en) 1998-10-08

Family

ID=12565012

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3987088A Expired - Fee Related JP2808597B2 (en) 1988-02-22 1988-02-22 Magnetic field applying electromagnet for magneto-optical disk

Country Status (1)

Country Link
JP (1) JP2808597B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3188339B2 (en) * 1992-03-06 2001-07-16 キヤノン株式会社 Magnetic head drive device and magneto-optical recording device

Also Published As

Publication number Publication date
JPH01213802A (en) 1989-08-28

Similar Documents

Publication Publication Date Title
US4340914A (en) Thermomagnetic recording and reproducing apparatus
JPH065585B2 (en) Magneto-optical storage device
US4518657A (en) Recording medium and recording-reproduction system provided with the recording medium
JPH0630183B2 (en) Magneto-optical recording / reproducing method and device
JP2811673B2 (en) Magnetic field applying electromagnet for magneto-optical disk
JP2808597B2 (en) Magnetic field applying electromagnet for magneto-optical disk
US4363052A (en) Thermomagnetic recording device
JPS6217282B2 (en)
JPH0568763B2 (en)
JPH01178104A (en) Magnetic field electromagnet for magneto-optical disk
JPS63144401A (en) Magnetic field impressing device for magneto-optical disk
JPH069082B2 (en) Magnetic field application device
JPH067401B2 (en) Magnetic field applying electromagnet for magneto-optical disk
JPH0325854B2 (en)
JPH0568762B2 (en)
JPS63217504A (en) Magnetic field impressing device for magneto-optical disk
JPH0568764B2 (en)
JPH01178106A (en) Magnetic field device for magneto-optical disk
JPH01178107A (en) Magnetic field device for magneto-optical disk
JP2604700B2 (en) Magneto-optical recording / reproduction / erasing method and apparatus
JP2604702B2 (en) Magneto-optical recording / reproduction / erasing method and apparatus
JPS61269204A (en) Magnetic field applying device
JPH0673201B2 (en) Magneto-optical recording / reproducing method and device
JP2834879B2 (en) Magneto-optical recording device
JPH03228201A (en) Externally applied magnetic field supply device for magneto-optical recording

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees