JPS60209944A - Device for optomagnetic recording, reproducing and erasing - Google Patents
Device for optomagnetic recording, reproducing and erasingInfo
- Publication number
- JPS60209944A JPS60209944A JP6554984A JP6554984A JPS60209944A JP S60209944 A JPS60209944 A JP S60209944A JP 6554984 A JP6554984 A JP 6554984A JP 6554984 A JP6554984 A JP 6554984A JP S60209944 A JPS60209944 A JP S60209944A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- recording
- medium
- reproducing
- erasing
- 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.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording 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
- G11B11/10—Recording 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
- G11B11/105—Recording 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
Landscapes
- Recording Or Reproducing By Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明はある特定の波長の光を用いて情報の記録再生消
去をおこなう光磁気記録再生消去装置に関する。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a magneto-optical recording, reproducing and erasing device that records, reproduces and erases information using light of a specific wavelength.
(従来技術とその問題点)
光磁気記録方式は書き替えのできる光デイスクメモリの
一方式である。光デイスクメモリは高密度大容量高速ア
クセスが可能であるということから現在の磁気ディスク
メモリに代わる新しいメモリと考えられ、中でも光磁気
記録方式は書き替え性を有することから最も注目されて
いる。(Prior art and its problems) Magneto-optical recording is a type of rewritable optical disk memory. Optical disk memory is considered a new memory to replace the current magnetic disk memory because it is capable of high-density, large-capacity, and high-speed access, and magneto-optical recording is attracting the most attention because of its rewritability.
従来より知られている光磁気記録再生消去装置の構成は
第1図に示したように、垂直磁化膜を記録層とする記録
媒体1.レーザー光によって情報の記録再生消去をおこ
なうヘッド部2.前記記録媒体1に磁界を印加するため
の磁界発生部3よ構成る。光磁気記録においては、情報
の記録時と消去時には、前記記録媒体1に印加する磁界
の方向を変える必要がある。そのために従来よシ前記磁
界発生部3には電磁石、永久磁石、空心コイルが用いら
れる。空心コイル以外の磁界発生部は前記記録媒体1に
関して前記ヘッド部2と互いに反対側になるように配置
される。通常用いられる記録媒体1は、ガラスあるいは
プラスチックディスク上に希土類遷移金属アモルファス
合金膜すなわち(Gd、 Tb、 Dy、 Ho )と
(li’e、Co、Ni)の合金膜を形成したものであ
る。記録消去にはそれぞれ100〜200への印加磁界
を必要とする。さらに高速での記録消去を実現するには
1μ式以下の速度での磁界のスイッチングをおこなう必
要がある。As shown in FIG. 1, the configuration of a conventionally known magneto-optical recording/reproducing/erasing device includes a recording medium 1. A head section that records, reproduces, and erases information using laser light 2. It consists of a magnetic field generating section 3 for applying a magnetic field to the recording medium 1. In magneto-optical recording, it is necessary to change the direction of the magnetic field applied to the recording medium 1 when recording and erasing information. For this purpose, conventionally, an electromagnet, a permanent magnet, or an air-core coil is used for the magnetic field generating section 3. The magnetic field generating section other than the air-core coil is arranged on the opposite side of the head section 2 with respect to the recording medium 1. A commonly used recording medium 1 is a rare earth transition metal amorphous alloy film, that is, an alloy film of (Gd, Tb, Dy, Ho) and (li'e, Co, Ni) formed on a glass or plastic disk. Recording and erasing each requires an applied magnetic field of 100-200°C. In order to realize recording and erasing at even higher speeds, it is necessary to switch the magnetic field at a speed of 1 μm or less.
磁界発生部3として電磁石を用いる場合、100〜20
0αの印加磁界を得ることは容易であるが、応答運車に
は限界があり、1μ(6)以下での磁界スイッチングは
できないという欠点がある。同様に、磁界発生部3とし
て永久磁石を用いる場合、100〜200ムの印加磁界
を得ることは容易であるが、磁界のスイッチングは機械
的手段に頼ることになるため、1μ(8)以下での磁界
スイッチングはできないという欠点がある。When using an electromagnet as the magnetic field generating section 3, 100 to 20
Although it is easy to obtain an applied magnetic field of 0α, there is a limit to responsive operation, and there is a drawback that magnetic field switching cannot be performed at 1 μ(6) or less. Similarly, if a permanent magnet is used as the magnetic field generator 3, it is easy to obtain an applied magnetic field of 100 to 200 µm, but since the switching of the magnetic field relies on mechanical means, the applied magnetic field is less than 1 µ(8). The disadvantage is that magnetic field switching is not possible.
磁界の高速スイッチングを可能にする一方法は空心コイ
ルを用いる方法である。を心コイルを用いる場合、10
0〜200αの磁界を鵬速でスイ。One way to enable fast switching of the magnetic field is to use air-core coils. When using a heart coil, 10
Swipe the magnetic field from 0 to 200α at high speed.
チングするためにはコイルの形状は小屋化してしまうの
で、記録媒体の回転に伴う面振れにより、空心コイルを
記録媒体近傍に固定しておくだけの方法では、コイルと
記録媒体間の距離の変動が生じ、一定の磁界を印加する
のは困難であるという欠点がある。Because the shape of the coil has to be shaped like a hut in order to change the shape of the coil, a method that only fixes the air-core coil near the recording medium will cause fluctuations in the distance between the coil and the recording medium due to surface run-out due to the rotation of the recording medium. This has the disadvantage that it is difficult to apply a constant magnetic field.
(発明の目的)
本発明の目的はこのような従来の欠点を除去せしめて、
記録媒体に印加する磁界を高速でスイ。(Object of the invention) The object of the present invention is to eliminate such conventional drawbacks,
Sweeps the magnetic field applied to the recording medium at high speed.
チングすることを可能ならしめる新規な光磁気記録再生
消去装置を提供することにある。It is an object of the present invention to provide a novel magneto-optical recording/reproducing/erasing device which enables the recording and erasing of data.
(発明の構成)
本発明によれば、反射光を光学的に検出し再生する光磁
気記録再生消去装置において、磁界発生部と記録再生消
去用光収束レンズとを記録媒体を介して互いに反対側に
配置し、前記磁界発生部と前記記録媒体との距離を所定
の間隔に保つ駆動手段を前記磁界発生部に設けるととも
に、前記磁界発生部として空心コイルを用いることを特
徴とする光磁気記録再生消去装置が得られる。(Structure of the Invention) According to the present invention, in a magneto-optical recording, reproducing and erasing device that optically detects and reproduces reflected light, a magnetic field generating section and a recording, reproducing and erasing optical converging lens are arranged on opposite sides of each other with a recording medium in between. magneto-optical recording and reproducing, characterized in that the magnetic field generating section is provided with a driving means for keeping the distance between the magnetic field generating section and the recording medium at a predetermined interval, and an air-core coil is used as the magnetic field generating section. An erasing device is obtained.
(構成の詳細な説明)
本発明は上述の構成をとることによシ従来技術の問題点
を解決した。まず、記録媒体への磁界印加手段として空
心コイルを用いることによシ、100〜200・)の磁
界を1μ(6)以下の高速でスイ、チングすることがで
きる。同時に記録媒体と空心コイルの距離を空心コイル
可動型の駆動手段によシ一定に保つことによって、所望
値の磁界を媒体に印加することができる。(Detailed Description of Configuration) The present invention solves the problems of the prior art by adopting the above-mentioned configuration. First, by using an air-core coil as a means for applying a magnetic field to a recording medium, a magnetic field of 100 to 200 mm can be switched at a high speed of 1 μ(6) or less. At the same time, by keeping the distance between the recording medium and the air-core coil constant using the air-core coil movable driving means, a magnetic field of a desired value can be applied to the medium.
磁界発生部と空心コイルの位置駆動手段及び制御部は一
体化されるとともに、記録再生消去用レーザー光源と光
収束レンズの半径方向の動きに合わせて半径方向に動く
構造を有する。The magnetic field generating section, the air-core coil position driving means, and the control section are integrated and have a structure that moves in the radial direction in accordance with the radial movement of the recording/reproducing/erasing laser light source and the light converging lens.
(実施例) 以下1本発明の実施例について図面に従って説明する。(Example) An embodiment of the present invention will be described below with reference to the drawings.
第2図は本発明の実施例を示したもので、光磁気記録用
磁性薄膜を有する記録媒体5の上方に記録再生消去用の
レーザー光源6と光収束レンズ7を設け、記録媒体を介
した反対側に磁界発生用空心コイル8と前記空心コイル
の位置駆動手段9ならびに記録媒体50面揚れを検出し
、空心コイルの位置駆動用の信号を発生する制御部10
を設けた構成である。記録媒体は回転用モーター11に
よ多回転する。FIG. 2 shows an embodiment of the present invention, in which a laser light source 6 for recording, reproducing and erasing and a light converging lens 7 are provided above a recording medium 5 having a magnetic thin film for magneto-optical recording. On the opposite side are an air-core coil 8 for generating a magnetic field, a position driving means 9 for the air-core coil, and a control unit 10 that detects the leveling up of the recording medium 50 and generates a signal for driving the position of the air-core coil.
This is a configuration with a The recording medium is rotated many times by a rotation motor 11.
制御部10は記録媒体5の面振れを検出するとともに空
心コイルの位置駆動手段9に制御信号を送シ、常に空心
コイル8と記録媒体5との間の距離を一定に保つように
働く。制御部10としては既知の光ヘッドの収束レンズ
合焦点制御部と同様の構成が利用される。レンズ12は
空心コイルと同一架体に取シ付けられた記録媒体間距離
の変動を検出するために用いられる。The control unit 10 detects the surface runout of the recording medium 5 and sends a control signal to the air-core coil position driving means 9, so as to always keep the distance between the air-core coil 8 and the recording medium 5 constant. As the control section 10, a configuration similar to that of a converging lens focusing point control section of a known optical head is used. The lens 12 is used to detect variations in the distance between recording media attached to the same frame as the air-core coil.
このように構成された実施例において、使用した空心コ
イルの形状とその磁気特性について説明する。使用した
空心コイルは、線径0.11mφの被覆銅線を用い、外
径3.1nφ、内径0.1wφ、コイル長0.2111
11m巻数30ターンとした。インピーダンスメーター
で測定した空心コイルのインダクタンスは1.1μHで
あった。第3図はコイル発生磁界をコイル先端からの距
離を変えてめた結果である。コイル電流IAのときコイ
ル先端から0.2゜のところで2000の磁界が得られ
る。また、負荷抵抗50Ωの電流パルサーを用いて空心
コイルにパルス電流を供給することによシ、1μm□□
以下での磁界スイッチングが可能であった1、記録媒体
と空心コイル間距離は、記録媒体の回転時の面振れが±
50μm程度であることから0.2 、、程度は必要で
ある。空心コイルと媒体との距離は本実施例で採用した
制御部と位置駆動手段によシ±1μm以下の変動におさ
えられているので、記録媒体に一定強度の磁界を安定し
て印加することができる。In the embodiment configured as described above, the shape of the air-core coil used and its magnetic properties will be explained. The air-core coil used was a coated copper wire with a wire diameter of 0.11 mφ, an outer diameter of 3.1 nφ, an inner diameter of 0.1 wφ, and a coil length of 0.2111 mm.
The number of turns was 11 m and 30 turns. The inductance of the air-core coil measured with an impedance meter was 1.1 μH. Figure 3 shows the results of the coil-generated magnetic field by varying the distance from the tip of the coil. When the coil current is IA, a magnetic field of 2000 is obtained at 0.2° from the tip of the coil. In addition, by supplying pulsed current to the air-core coil using a current pulser with a load resistance of 50Ω,
It was possible to perform magnetic field switching under
Since the thickness is about 50 μm, a thickness of about 0.2 μm is necessary. Since the distance between the air-core coil and the medium is suppressed to fluctuations of ±1 μm or less by the control unit and position driving means employed in this embodiment, it is possible to stably apply a magnetic field of constant strength to the recording medium. can.
(発明の効果)
以上説明したように本発明によれば、従来例と比較して
次のような効果がある。(Effects of the Invention) As explained above, the present invention has the following effects compared to the conventional example.
■“磁界発生部として空心コイルを用い、かつ空心コイ
ルと記録媒体との距離を一定に保つ機構を採用すること
によシ1μ就以下の高速で磁界のスイッチングが可能で
ある。■By using an air-core coil as the magnetic field generator and employing a mechanism that maintains a constant distance between the air-core coil and the recording medium, it is possible to switch the magnetic field at a high speed of less than 1 μm.
■ 磁界発生部が記録媒体の裏面に配置されるため、記
録再生消去用へ、ドの妨げとならず、ヘッド構成に制約
を与えない。(2) Since the magnetic field generating section is placed on the back surface of the recording medium, it does not interfere with recording, reproducing, or erasing operations, and does not impose restrictions on the head configuration.
■ 高速の磁界スイッチングを用いることによシ、1ト
ラック一括消去をおこなわずに、既記録トラックを書き
直す形で新しいデータを記録することができ、「消去モ
ード」を省略できる。(2) By using high-speed magnetic field switching, new data can be recorded by rewriting the already recorded track without erasing one track at a time, and the "erase mode" can be omitted.
■ 空心コイルからの発生磁界はコイル先端からの距離
が大きくなると急峻に低下するので光収束レンズ合焦駆
動制御手段及び空心コイル位置駆動手段への磁気的干渉
が生じない。(2) Since the magnetic field generated by the air-core coil decreases sharply as the distance from the tip of the coil increases, magnetic interference with the light converging lens focusing drive control means and the air-core coil position drive means does not occur.
第1図は従来の光磁気記録再生消去装置の構成図、第2
図は本発明の一実施例を示す構成図、第3図は本発明に
用いるを心コイルの発生磁界特性を示した図である。Figure 1 is a block diagram of a conventional magneto-optical recording/erasing device;
The figure is a block diagram showing one embodiment of the present invention, and FIG. 3 is a diagram showing the generated magnetic field characteristics of the core coil used in the present invention.
Claims (1)
置において、磁界発生部と記録再生消去用光収束レンズ
とを記録媒体金倉して互いに反対側に配置し、前記磁界
発生部と前記記録媒体との距離を所定の間隔に保つ駆動
手段を前記磁界発生部に設けるとともに、前記磁界発生
部として空心コイルを用いることを特徴とする光磁気記
録再生消去装置。In a magneto-optical recording, reproducing and erasing device that optically detects and reproduces reflected light, a magnetic field generating section and an optical converging lens for recording, reproducing and erasing are arranged on opposite sides of the recording medium, and the magnetic field generating section and the recording A magneto-optical recording/reproducing/erasing device characterized in that the magnetic field generating section is provided with a driving means for maintaining a distance from the medium at a predetermined interval, and an air-core coil is used as the magnetic field generating section.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59065549A JPH0719403B2 (en) | 1984-04-02 | 1984-04-02 | Magneto-optical recording / reproducing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59065549A JPH0719403B2 (en) | 1984-04-02 | 1984-04-02 | Magneto-optical recording / reproducing device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS60209944A true JPS60209944A (en) | 1985-10-22 |
JPH0719403B2 JPH0719403B2 (en) | 1995-03-06 |
Family
ID=13290201
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP59065549A Expired - Lifetime JPH0719403B2 (en) | 1984-04-02 | 1984-04-02 | Magneto-optical recording / reproducing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0719403B2 (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6455766A (en) * | 1987-08-26 | 1989-03-02 | Nec Corp | Magneto-optical recording, reproducing and erasing device |
EP0341778A2 (en) * | 1988-05-09 | 1989-11-15 | Koninklijke Philips Electronics N.V. | Magneto-optical recording method and magneto-optical recording apparatus |
US4937801A (en) * | 1986-10-17 | 1990-06-26 | Hitachi, Ltd. | Magneto-optical recording and reproducing apparatus with magnetic field controller |
US5163032A (en) * | 1988-06-07 | 1992-11-10 | U.S. Philips Corp. | Magneto-optical recorder with servo control system for a magnetic-field modulation system |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5625470A (en) * | 1979-08-09 | 1981-03-11 | Mitsubishi Electric Corp | Photo beam thermomagnetic recording apparatus |
JPS57133503A (en) * | 1981-02-10 | 1982-08-18 | Sharp Corp | Optical and magnetic recorder and reproducer |
JPS58115655A (en) * | 1981-12-28 | 1983-07-09 | Seiko Epson Corp | Magnetic storage device |
-
1984
- 1984-04-02 JP JP59065549A patent/JPH0719403B2/en not_active Expired - Lifetime
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5625470A (en) * | 1979-08-09 | 1981-03-11 | Mitsubishi Electric Corp | Photo beam thermomagnetic recording apparatus |
JPS57133503A (en) * | 1981-02-10 | 1982-08-18 | Sharp Corp | Optical and magnetic recorder and reproducer |
JPS58115655A (en) * | 1981-12-28 | 1983-07-09 | Seiko Epson Corp | Magnetic storage device |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4937801A (en) * | 1986-10-17 | 1990-06-26 | Hitachi, Ltd. | Magneto-optical recording and reproducing apparatus with magnetic field controller |
JPS6455766A (en) * | 1987-08-26 | 1989-03-02 | Nec Corp | Magneto-optical recording, reproducing and erasing device |
EP0341778A2 (en) * | 1988-05-09 | 1989-11-15 | Koninklijke Philips Electronics N.V. | Magneto-optical recording method and magneto-optical recording apparatus |
US5163032A (en) * | 1988-06-07 | 1992-11-10 | U.S. Philips Corp. | Magneto-optical recorder with servo control system for a magnetic-field modulation system |
Also Published As
Publication number | Publication date |
---|---|
JPH0719403B2 (en) | 1995-03-06 |
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