JPH01178107A - Magnetic field device for magneto-optical disk - Google Patents

Magnetic field device for magneto-optical disk

Info

Publication number
JPH01178107A
JPH01178107A JP192288A JP192288A JPH01178107A JP H01178107 A JPH01178107 A JP H01178107A JP 192288 A JP192288 A JP 192288A JP 192288 A JP192288 A JP 192288A JP H01178107 A JPH01178107 A JP H01178107A
Authority
JP
Japan
Prior art keywords
magnetic field
magneto
optical disk
coil
arm
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
JP192288A
Other languages
Japanese (ja)
Inventor
Hideo Tanaka
英男 田中
Fujio Suzuki
富士夫 鈴木
Nobuyoshi Oshida
大志田 信義
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
NEC 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 NEC Corp filed Critical NEC Corp
Priority to JP192288A priority Critical patent/JPH01178107A/en
Publication of JPH01178107A publication Critical patent/JPH01178107A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To attain high speed switching wit a large magnetic field by providing a 2nd coil generating the same direction of magnetic field to that of a 1st coil and passing a laser beam through the center via a hollow and the 1st coil to the arm of the U-shaped multi-layer thin strip high permeability magnetic substance formed through lamination of thin strip high permeability magnetic substances. CONSTITUTION:The hollow part 12 to irradiated a magneto-optical disk 5 with a laser beam L from the outer face of an arm 11A is provided to the tip of the 1st arm 11A of the multi-layer thin strip high permeability magnetic substance 1 and the coil 3 is provided in spiral to the inner circumference of the arm of the hollow 12. Moreover, the coil 2 is provided to the 2nd arm 11B of the multi-layer thin strip high permeability substance 1, the coils 2, 3 are excited by a magnetic field generating current modulation circuit 4 and connected to generate a magnetic field perpendicularly to the magneto-optical disk 5 and in the same direction at the same time. Thus, high speed switching with a large magnetic field is attained.

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装置に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a magnetic field applying device for a magneto-optical disk.

〔従来の技術〕[Conventional technology]

従来の光磁気ディスク用磁界印加装置においては、光磁
気ディスクの記録情報を消去する場合、外部磁界を、記
録時とは逆極性に印加し、レーザー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−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。
In conventional magnetic field application devices for magneto-optical disks, when erasing recorded information on a magneto-optical disk, an external magnetic field is applied with the opposite polarity to that during recording, and a laser beam is applied to the recording medium with the same intensity as during recording. Uniform 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.

ここで外部磁界印加手段としては、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, as the external magnetic field applying means, there are, for example, a method using an air-core coil, a method using an electromagnet, or a method using a permanent magnet.

こ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工ルステツ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。
In this magnetic field applying means, an applied magnetic field of several hundreds of steps or more is usually required during recording and erasing, so when an air-core coil is used, the coil becomes large.
Along with this, there is a drawback that the magnetic field switching speed becomes slow and the required applied magnetic field cannot be obtained unless the distance between the recording medium and the coil is made sufficiently close.

又電磁石を用いる場合にも、磁界印加手段は大型化し、
磁界切換速度が遅いという欠点を生じている。
Also, when using an electromagnet, the magnetic field applying means becomes larger,
The disadvantage is that the magnetic field switching speed is slow.

さらに、永久磁石を用いる場合には、機械的な駆動手段
を用いて磁界を切り変える為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た。
Furthermore, when permanent magnets are used, a complicated mechanism is required to switch the magnetic field using a mechanical drive means, and the magnetic field switching speed is also slow in this case.

以上の述べたように、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、又記録する時には、一定磁界
印加中にレーザーパワーを高速変調する方法が用いられ
ている。
As mentioned above, since the magnetic field switching speed is slow with any conventional external magnetic field applying means, the aforementioned batch erasing method is used for erasing, and when recording, laser power is applied while a constant magnetic field is applied. A method of high-speed modulation is used.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

上述した従来の光磁気ディスク用磁界印加装置は、磁界
切換速度が遅く一括消去方式となっているので、既に情
報が記録されている光磁気ディスクに新しい情報を高速
で重ね書きするといういわゆるオーバーライド機能を持
たせることが困難であるという問題点がある。
The above-mentioned conventional magnetic field applying device for magneto-optical disks has a slow magnetic field switching speed and uses a batch erasing method, so it has a so-called override function that overwrites new information at high speed on a magneto-optical disk on which information has already been recorded. The problem is that it is difficult to provide

本発明の目的は、大いき磁界を高速でスイッチングする
ことができ、オーバーライド機能を持たせることができ
る光磁気ディスク用磁界印加装置を提供することにある
An object of the present invention is to provide a magnetic field application device for a magneto-optical disk that can switch a large magnetic field at high speed and has an override function.

〔問題点を解決するための手段〕[Means for solving problems]

本発明の光磁気ディスク用磁界印加装置は、光磁気ディ
スクの周辺部外側で折返えされ、内面がこの光磁気ディ
スクの上下各面とそれぞれ対向する第1及び第2のアー
ム部を備え、複数の薄帯高透磁率磁性体を積層したU字
形状の多層薄帯高透磁率磁性体と、前記第1及び第2の
アーム部の少なくとも一方の先端部に設けられこのアー
ム部の外面側から前記光磁気ディスクにレーザービーム
を照射するための中空部と、前記第1及び第2のアーム
部の少なくとも一方に設けられ前記光磁気ディスクに対
して所定の磁界を発生する第1のコイルと、前記中空部
のアーム部内面周辺部に設けられ前記第1のコイルと同
時かつ同一方向に磁界を発生する第2のコイルとを有し
ている。
A magnetic field applying device for a magneto-optical disk according to the present invention includes first and second arm portions that are folded back outside the periphery of a magneto-optical disk, and whose inner surfaces face the upper and lower surfaces of the magneto-optical disk, respectively. A U-shaped multi-layer thin strip high permeability magnetic material laminated with a thin strip high permeability magnetic material, and a U-shaped multilayer thin strip high permeability magnetic material laminated, and a U-shaped multilayer thin strip high permeability magnetic material laminated, and a U-shaped multilayer thin strip high permeability magnetic material laminated, and a a hollow portion for irradiating the magneto-optical disk with a laser beam; a first coil provided in at least one of the first and second arm portions and generating a predetermined magnetic field toward the magneto-optical disk; A second coil is provided around the inner surface of the arm portion of the hollow portion and generates a magnetic field simultaneously and in the same direction as the first coil.

〔実施例〕〔Example〕

次に、本発明の実施例について図面を参照して説明する
Next, embodiments of the present invention will be described with reference to the drawings.

第1図は本発明の一実施例を示す斜視図である。FIG. 1 is a perspective view showing an embodiment of the present invention.

多層薄帯高透磁率磁性体1は、光磁気ディスク5の周辺
部外側で折返され、内面が光磁気ディスク5の上下各面
とそれぞれ対向する第1及び第2のアーム部114.1
1Bを備え、約30枚の薄帯高透磁率磁性体を積層接着
してU字形状に形成されている。
The multilayer ribbon high permeability magnetic material 1 is folded back outside the peripheral portion of the magneto-optical disk 5, and has first and second arm portions 114.1 whose inner surfaces face the upper and lower surfaces of the magneto-optical disk 5, respectively.
1B, and is formed into a U-shape by laminating and bonding about 30 thin strips of high permeability magnetic material.

ここで、薄帯高透磁率磁性体には、厚さ30μm、長さ
約20cmのフェライト(MnZn。
Here, the ribbon high permeability magnetic material is made of ferrite (MnZn) with a thickness of 30 μm and a length of about 20 cm.

NiZnなど)、パーマロイ(NiFu)、センダスト
、アモルファス(CoZr、FeCoZr、CoNb、
CoTa、CoHfなど)、鉄心などが用いられる。
NiZn, etc.), permalloy (NiFu), sendust, amorphous (CoZr, FeCoZr, CoNb,
CoTa, CoHf, etc.), iron core, etc. are used.

多層薄帯高透磁率磁性体1の第1のアーム部11Aの先
端部には、光磁気ディスク5にこのアーム部11Aの外
面側からレーザービームLを照射するための中空部12
が設けられており、この中空部12のアーム部内面周辺
部にはスパリラル状にコイル3が設けられている。これ
ら中空部12及びコイル3の内径は、レーザービームが
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ている。
A hollow portion 12 is provided at the tip of the first arm portion 11A of the multilayer ribbon high permeability magnetic material 1 for irradiating the laser beam L onto the magneto-optical disk 5 from the outer surface side of the arm portion 11A.
A spiral coil 3 is provided around the inner surface of the arm portion of the hollow portion 12. The inner diameters of the hollow portion 12 and the coil 3 are set to a size that allows the laser beam to pass therethrough and allows the lens to move in the track direction by tracking.

また、多層薄帯高透磁率磁性体1の第2のアーム部11
aにはコイル2が設けられており、これらコイル2.3
は磁界発生電流変調回路4で駆動され、光磁気ディスク
5に対し垂直に、同時にかつ同一方向に磁界を発生する
ように接続されている。
Further, the second arm portion 11 of the multilayer ribbon high permeability magnetic material 1
A is provided with a coil 2, and these coils 2.3
are driven by a magnetic field generation current modulation circuit 4 and are connected perpendicularly to the magneto-optical disk 5 so as to generate magnetic fields simultaneously and in the same direction.

これらコイル2.3の線径は例えば150μmのものが
用いられ、駆動電流は数10〜数100mAが妥当であ
る。
The wire diameter of these coils 2.3 is, for example, 150 μm, and the appropriate driving current is several 10 to several 100 mA.

このようにして構成された磁界印加手段では、磁界を集
束することができ、かつ巻き線のインダクタンスを1μ
H以下にすることが容易なため、多層薄帯高透磁率磁性
体lの内面から数mm離れた位置において、数100エ
ルステツドの磁界を数MHzの高速で容易に切換えるこ
とが出来る。
With the magnetic field applying means configured in this way, the magnetic field can be focused, and the inductance of the winding can be reduced to 1 μm.
Since it is easy to make the magnetic field less than H, a magnetic field of several hundred oersted can be easily switched at a high speed of several MHz at a position several mm away from the inner surface of the multilayer ribbon high permeability magnetic material l.

第2図は第1図の実施例が適用される光磁気記録再生装
置の周辺系のブロック図で、本実施例の効果を確認する
ためにこの装置により、光磁気ディスク5への記録再生
消去を行なった。
FIG. 2 is a block diagram of the peripheral system of a magneto-optical recording and reproducing apparatus to which the embodiment of FIG. I did it.

第1図、第2図において、磁界発生電流変調回路4の出
力電流■、がコイル2,3に流れ、光磁気ディスク5の
磁性媒体52に上向き及び下向きの磁界が交互に印加さ
れる。
In FIGS. 1 and 2, the output current (1) of the magnetic field generation current modulation circuit 4 flows through the coils 2 and 3, and upward and downward magnetic fields are alternately applied to the magnetic medium 52 of the magneto-optical disk 5.

光磁気用ヘッド7は従来と同等のものであり、次のよう
な構成を有する。
The magneto-optical head 7 is the same as the conventional one and has the following configuration.

71は直線偏光のレーザー光源であり、例えば半導体レ
ーザーが使用される。73A〜73cはビームスプリッ
タである。レーザービームLの集光用レンズ72はアク
チュエータ72A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のフォー
アスエラー信号検出用の受光素子75B、)ラッキング
エラー信号検出用の受光素子75cによってサーボ制御
回路8A 、8Bに入力され、サーボ信号となり、アク
チュエータ72 Bにフィードバックされる。
71 is a linearly polarized laser light source, for example, a semiconductor laser is used. 73A to 73c are beam splitters. A condensing lens 72 for the laser beam L is supported by an actuator 72A. The focus error and tracking error signals are input to the servo control circuits 8A and 8B by the respective light receiving elements 75B and 75c for detecting fourth error signals, respectively, and become servo signals, which are fed back to the actuator 72B. be done.

再生信号は偏光フィルタ74を通過後、再生信号用の受
光素子75Aによって検出され、再生信号の増幅回路9
によって増幅される。偏光フィル、り74としてはダラ
ムトムソンプリズムを用い、再生信号検出用の受光素子
75AとしてはPINフォトダイオードを用いた。
After passing through the polarizing filter 74, the reproduced signal is detected by the reproduced signal light receiving element 75A, and then sent to the reproduced signal amplification circuit 9.
is amplified by A Durham Thomson prism was used as the polarizing filter 74, and a PIN photodiode was used as the light receiving element 75A for detecting the reproduced signal.

レーザー光源71の変調にはレーザー光源変調回路6が
使用され、記録時、消去時、再生時に合わせてレーザー
光のパワーが変調される。
A laser light source modulation circuit 6 is used to modulate the laser light source 71, and the power of the laser light is modulated during recording, erasing, and reproduction.

光磁気ディスク5として120 mm径のプラスチック
の基板51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人厚に形成し、このT
bFeCo膜上にさらにSiNを形成“したディスクを
使用しな。この基板51に予めトラックピッチ1.6μ
m、深さ700人の溝を形成し、いわゆるプリグループ
基板として用いた。
As the magneto-optical disk 5, a TbFeCo film was further formed to a thickness of 800 mm on SiN formed by sputtering on a plastic substrate 51 with a diameter of 120 mm.
Do not use a disk in which SiN is further formed on the FeCo film.
A trench of 700 m and depth was formed and used as a so-called pre-group substrate.

第3図(a)〜(c)に、記録動作モード時の波形図を
示す。
FIGS. 3(a) to 3(c) show waveform diagrams in the recording operation mode.

記録媒体をキューリー温度以上に上昇できる一定強度P
wのレーザービームを照射しながら、外部磁界印加のた
めのコイル2,3に第3図(b)に示すような変調電流
IA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3図(c)に示すような記録
磁化状態が実現される。
Constant strength P that can raise the recording medium above the Curie temperature
By passing a modulation current IA as shown in FIG. 3(b) through the coils 2 and 3 for applying an external magnetic field while irradiating a laser beam of During the cooling process accompanying the running of the medium, a recording magnetization state as shown in FIG. 3(c) is realized in accordance with the direction of the applied magnetic field.

そして、まず線速9 m / s e cにて光磁気デ
ィスク5面上に4mWの一定強度し−ザービームLを照
射しながら、外部磁界印加手段のコイル2゜3にIMH
zで200mAの変調IA雷電流流したところ、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Q、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。
First, while irradiating the laser beam L with a constant intensity of 4 mW onto the 5 surface of the magneto-optical disk at a linear velocity of 9 m/sec, an IMH was applied to the coil 2°3 of the external magnetic field applying means.
When a modulated IA lightning current of 200 mA was applied at Z, good recording was achieved. When a recording magnetic field of Q and 5 MHz was newly applied to this recording track under the same conditions, recording corresponding to this recording magnetic field was possible, and no residual trace of the previously recorded signal was observed.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明は、内面が光磁気ディスクの
上下各面と対向する第1.第2のアームの備え薄帯高透
磁率磁性体を積層したU字形状の多層薄帯高透磁率磁性
体のアームに、第1のコイルと、中空部を介してレーザ
ービームが中心部を通過し第1のコイルと同一方向の磁
界を発生する第2のコイルを設ける構成とすることによ
り、磁束利用効率がよく、低インダクタンスにできるの
で、大きい磁界の高速スイッチングができ、かつオーバ
ーライド機能を持たせることができる効果がある。
As explained above, the present invention provides a first disk whose inner surface faces each of the upper and lower surfaces of the magneto-optical disk. The laser beam passes through the center of the arm of the second arm, which is made of a U-shaped multilayer thin ribbon high permeability magnetic material, through the first coil and the hollow part. However, by providing a second coil that generates a magnetic field in the same direction as the first coil, the magnetic flux utilization efficiency is high and the inductance can be reduced, allowing high-speed switching of large magnetic fields and an override function. There is an effect that can be used.

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

第1図は本発明の一実施例を示す斜視図、第2図は第1
図に示された実施例が適用される光磁気記録再生装置の
周辺系のブロック図、第3図は第1図に示された実施例
の記録動作モード時の波形図である。 1・・・多層薄帯高透磁率磁性体、2,3・・・コイル
、4・・・磁界発生電流変調回路、5・・・光磁気ディ
スフ、6・・・レーザー光源変調回路、7・・・光磁気
用ヘッド、8A 、8B・・・サーボ制御回路、9・・
・増幅回路、IIA、IIB・・・アーム部、12・・
・中空部、51・・・基板、52・・・磁性媒体、71
・・・レーザー光源、72・・・集光用レンズ、72A
・・・アクチュエータ、73A〜73c・・・ビームス
プリッタ、74・・・偏光フィルタ、75A〜75c・
・・受光素子。
FIG. 1 is a perspective view showing one embodiment of the present invention, and FIG. 2 is a perspective view showing one embodiment of the present invention.
FIG. 3 is a block diagram of a peripheral system of a magneto-optical recording/reproducing apparatus to which the embodiment shown in the figure is applied, and FIG. 3 is a waveform diagram in the recording operation mode of the embodiment shown in FIG. DESCRIPTION OF SYMBOLS 1... Multilayer thin ribbon high permeability magnetic material, 2, 3... Coil, 4... Magnetic field generation current modulation circuit, 5... Magneto-optical disc, 6... Laser light source modulation circuit, 7. ...Magneto-optical head, 8A, 8B... Servo control circuit, 9...
・Amplifier circuit, IIA, IIB...Arm section, 12...
- Hollow part, 51... Substrate, 52... Magnetic medium, 71
...Laser light source, 72...Condensing lens, 72A
... Actuator, 73A-73c... Beam splitter, 74... Polarizing filter, 75A-75c...
··Light receiving element.

Claims (1)

【特許請求の範囲】[Claims] 光磁気ディスクの周辺部外側で折返えされ、内面がこの
光磁気ディスクの上下各面とそれぞれ対向する第1及び
第2のアーム部を備え、複数の薄帯高透磁率磁性体を積
層したU字形状の多層薄帯高透磁率磁性体と、前記第1
及び第2のアーム部の少なくとも一方の先端部に設けら
れこのアーム部の外面側から前記光磁気ディスクにレー
ザービームを照射するための中空部と、前記第1及び第
2のアーム部の少なくとも一方に設けられ前記光磁気デ
ィスクに対して所定の磁界を発生する第1のコイルと、
前記中空部のアーム部内面周辺部に設けられ前記第1の
コイルと同時かつ同一方向に磁界を発生する第2のコイ
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
加装置。
A U that is folded back outside the periphery of a magneto-optical disk, has first and second arm portions whose inner surfaces face the upper and lower surfaces of the magneto-optical disk, respectively, and has a plurality of laminated thin strips of high permeability magnetic material. a multilayer ribbon high permeability magnetic material having a shape of
and a hollow portion provided at the tip of at least one of the second arm portions for irradiating the magneto-optical disk with a laser beam from the outer surface side of the arm portion, and at least one of the first and second arm portions. a first coil that is provided in the magneto-optical disk and generates a predetermined magnetic field with respect to the magneto-optical disk;
A magnetic field applying device for a magneto-optical disk, comprising a second coil that is provided around the inner surface of the arm portion of the hollow portion and generates a magnetic field simultaneously and in the same direction as the first coil.
JP192288A 1988-01-08 1988-01-08 Magnetic field device for magneto-optical disk Pending JPH01178107A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP192288A JPH01178107A (en) 1988-01-08 1988-01-08 Magnetic field device for magneto-optical disk

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP192288A JPH01178107A (en) 1988-01-08 1988-01-08 Magnetic field device for magneto-optical disk

Publications (1)

Publication Number Publication Date
JPH01178107A true JPH01178107A (en) 1989-07-14

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP192288A Pending JPH01178107A (en) 1988-01-08 1988-01-08 Magnetic field device for magneto-optical disk

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JP (1) JPH01178107A (en)

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5948803A (en) * 1982-09-14 1984-03-21 Nippon Kogaku Kk <Nikon> Auxiliary magnetic field generator for optical/magnetic disk devices
JPS59152503A (en) * 1983-02-19 1984-08-31 Canon Inc Optical pickup device
JPS61192001A (en) * 1985-02-20 1986-08-26 Fujitsu Ltd Bias magnetic field generator
JPS61217903A (en) * 1985-03-25 1986-09-27 Nippon Kogaku Kk <Nikon> External magnetic field application device for magneto-optical device

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5948803A (en) * 1982-09-14 1984-03-21 Nippon Kogaku Kk <Nikon> Auxiliary magnetic field generator for optical/magnetic disk devices
JPS59152503A (en) * 1983-02-19 1984-08-31 Canon Inc Optical pickup device
JPS61192001A (en) * 1985-02-20 1986-08-26 Fujitsu Ltd Bias magnetic field generator
JPS61217903A (en) * 1985-03-25 1986-09-27 Nippon Kogaku Kk <Nikon> External magnetic field application device for magneto-optical device

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