JPH0317846A - Magneto-optical recorder - Google Patents

Magneto-optical recorder

Info

Publication number
JPH0317846A
JPH0317846A JP15084389A JP15084389A JPH0317846A JP H0317846 A JPH0317846 A JP H0317846A JP 15084389 A JP15084389 A JP 15084389A JP 15084389 A JP15084389 A JP 15084389A JP H0317846 A JPH0317846 A JP H0317846A
Authority
JP
Japan
Prior art keywords
magnetic field
magneto
optical recording
recording medium
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.)
Pending
Application number
JP15084389A
Other languages
Japanese (ja)
Inventor
Takashi Akahori
赤堀 隆司
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.)
Ricoh Co Ltd
Original Assignee
Ricoh 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP15084389A priority Critical patent/JPH0317846A/en
Publication of JPH0317846A publication Critical patent/JPH0317846A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To make it possible to perform overwriting by one directional pulse magnetic field by making the direction of the component of a leakage magnetic field from an objective lens driving means which is orthogonally crossed with a magneto-optical recording medium opposite to the initial magnetizing direction of the magneto-optical recording medium. CONSTITUTION:It is possible to erase only by the leakage magnetic field 5 from a lens actuator 3 and a diamagnetic field from the peripheral part of the heating part of a perpendicularly magnetized film 4 without using the magnetic field generated by an external magnetic field generating device 1. But, in this case, very large magnetic field is necessary for the magnetic field 5. Then, the leakage magnetic field 5 of the actuator 3 which is made to be in the direction of performing recording (the direction opposite to the initial magnetization direction at the time of overwriting) can be more effectively used. And by making the magnetic field 5 and the diamagnetic field 6 from the peripheral part of the recording part act in the same direction, the magnetic field necessary for the inversion of magnetization can be given to the recording part, so that the magnetic recording can be performed without using the magnetic field from the device 1. And then, at the time of erasing the recorded information (the initial magnetization direction at the time of overwriting), the magnetic field is impressed on the erasing direction by the device 1.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、光磁気記録媒体にレーザ光ビームを照射し、
光ビームの光強度若しくは印加磁界の何れか一方若しく
は両方を記録信号に応じて変調することによって情報の
記録を行う光磁気記録装置に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention provides a method for irradiating a magneto-optical recording medium with a laser beam,
The present invention relates to a magneto-optical recording device that records information by modulating either the intensity of a light beam or an applied magnetic field, or both, according to a recording signal.

〔従来の技術〕[Conventional technology]

基板上に垂直磁化膜を積層形成された光磁気記録媒体に
、対物レンズによってレーザ光ビームを照射すると共に
その光ビームの照射部に電磁石等の磁界発生手段によっ
て磁界を印加し、上記光ビームの光強度若しくは印加磁
界の何れか一方若しくは両方を記録信号に応じて変調す
ることによって情報の記録を行う光磁気記録装置が知ら
れている. このような光磁気記録装置において、上記光磁気記録媒
体(例えば光磁気ディスク)は、光透過性の基板上に垂
直磁化膜を積層形威してなり、この垂直磁化膜4の磁化
方向は,未記録状態,あるいは消去状態では、第1図に
模式的に示すように垂直磁化膜の全領域においてその厚
さ方向の一方向{1!(例えば、図中矢印方向)に向く
ように配列されている. また,情報の記録時においては、垂直磁化膜4の記録部
にレーザ光ビームを照射してこの照射部において磁化膜
をそのキューリー点(強磁性キューリー点)付近の温度
に加熱すると共に、磁界発生装置により記録部に外部磁
界を印加し、外部磁界と加熱部周辺の磁化による反磁界
との作用により、その加熱部分の磁化方向を記録情報に
応じて反転して情報を記録する.第5図はこの記録を行
った後の磁化状態を模式的に示したものであり、記録領
域4Aにおいて磁化の反転がなされている状態を示して
いる. 尚、上述のようにして光磁気記録媒体に記録された2値
化情報(磁化の方向によってllPjj″011を表す
)の再生は,力一効果やファラディー効果等の磁気光学
効果を利用して磁化の方向を検出することによって行わ
れる。
A magneto-optical recording medium in which a perpendicularly magnetized film is laminated on a substrate is irradiated with a laser beam using an objective lens, and a magnetic field is applied to the irradiated portion of the light beam by a magnetic field generating means such as an electromagnet. Magneto-optical recording devices are known that record information by modulating either the optical intensity or the applied magnetic field, or both, according to the recording signal. In such a magneto-optical recording device, the magneto-optical recording medium (for example, a magneto-optical disk) is formed by laminating a perpendicular magnetization film on a light-transmitting substrate, and the magnetization direction of the perpendicular magnetization film 4 is as follows. In an unrecorded state or an erased state, as schematically shown in FIG. 1, the entire region of the perpendicularly magnetized film has one direction {1! (for example, in the direction of the arrow in the figure). In addition, when recording information, a laser beam is irradiated onto the recording part of the perpendicularly magnetized film 4, and the irradiated part heats the magnetized film to a temperature near its Curie point (ferromagnetic Curie point), and also generates a magnetic field. The device applies an external magnetic field to the recording section, and by the interaction of the external magnetic field and the demagnetizing field created by the magnetization around the heated section, the direction of magnetization of the heated section is reversed according to the recorded information, and information is recorded. FIG. 5 schematically shows the magnetization state after this recording, and shows a state in which the magnetization has been reversed in the recording area 4A. Note that the reproduction of the binary information (representing llPjj''011 depending on the direction of magnetization) recorded on the magneto-optical recording medium as described above is performed using magneto-optic effects such as the Rikichi effect and the Faraday effect. This is done by detecting the direction of magnetization.

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

ところで、上述の光磁気記録装置において、重ね書きに
よって磁化方向を記録状態に書き換える,所謂オーバー
ライトを行う場合は、消去のための特別な時間を必要と
しないことから、その書き換えを能率的に行うことがで
きるという利点がある.そして、このようなオーバーラ
イトを行う方法としては、磁界変調法がよく知られてい
る.しかるに、実際には種々の問題から実用化されるに
到ってない. その1つの問題は、一般的に考えられる磁界変調法によ
るオーバーライト法では、例えば、先の第5図に示した
第1の記録状態から、第6図に示す第2の記録状態を得
るのに,先の第5図における記録領域4Aの磁化状態を
反転消去し.一方、領域4B, 4Cでは新しい磁化反
転を生じさせているというように、磁化膜4の厚さ方向
に関し、互いに逆向き,すなわち、正負両極性の記録及
び消去磁界を記録情報信号に応じて発生させる必要があ
るということである. ところが、このような反転を高い周波数で可能にするに
は、この磁界発生手段の電磁石のコイルの巻回数を少な
くしてインダクタンスを小さくする必要があるが、この
場合は、その分だけ通電電流を大電流とする必要が生じ
る. しかしながら、このように通電電流を大電流とした場合
には、ジュール熱による発熱の問題が生じてくるのみな
らず、このような大電流を高い周波数で且つ正負両極性
をもって反転して振らせるような酩動電源は、電力消費
が大きく大型と或らざるを得なくなるものであり、更に
、この場合において、周波数特性に優れたものを得るこ
とは極めて困難である.また,前述した記録及び消去の
ためのオーバーライトの正負両極性の磁界のレベルは比
較的大きくすることが望まれ、この外部磁界を得るため
の磁界発生手段としては大出力のものが必要とされ、電
力消費の問題が大きくなる.ところで、光磁気記録装置
のピックアップ系には,光磁気記録媒体に光ビームを集
光する対物レンズと、永久磁石と電磁コイルとを備え上
記対物レンズを少なくとも光軸方向に駆動する対物レン
ズ駆動手段(以下、レンズアクチュエータと称する)と
が備えられており,少なくとも,レンズアクチュエータ
によってフォーカシング調整を行うようになっている. ここで、上記レンズアクチュエータは、実際上光磁気記
録媒体の面に対し直交する方向の直流磁界を発生する磁
石、例えば永久磁石を有しており、この磁石を含む磁気
回路内にフォー力シングサーボ電流を通ずる可動コイル
が配置され、サーボ電流に応じて可動コイルが光軸方向
に移動するようになされているものである.このような
レンズアクチュエータでは、通常、磁気シールドがなさ
れており,できるだけアクチュエータからの漏洩磁界を
小さくするような考慮がなされているが、少なくとも対
物レンズの配置部から記録媒体に対する磁界の漏洩を免
れることはできないという問題がある. ところで、レンズアクチュエータの漏洩磁界が記録媒体
にかかっていない場合,記録及び消去(オーバーライト
では初期磁化方向)に必要な外部磁界の強さは媒体の材
質やレーザ光のパワーによって異なるが,一般に、記録
時よりも消去時の方が強い磁界を必要とする.この理由
は、記録時に加熱された磁化膜にその周囲の磁化膜から
の反磁界(漏れ磁界)が作用し、その反磁界が磁化の反
転を助けるためである. 従来、レンズアクチュエータから光磁気記録媒体に与え
る漏洩磁界の方向と光磁気記録媒体の初期磁化(消去〉
方向との関係は規定されていなかったが、例えば、特開
昭63−66747号公報には、消去時に外部磁界の方
向とレンズアクチュエータの漏洩磁界の方向とを同一と
させ、漏洩磁界を消去磁界の補助として利用した構成の
光磁気記録装置が提案されており、これは、第7図及び
第8図に示すように、光磁気記録媒体の垂直磁化膜4の
初期磁化(消去)方向と、レンズアクチュエータ3から
の漏洩磁界5の方向とを同一としたものと考えてよい. しかるに、これは、磁界発生手段1からの印加磁界によ
って正負両極性を持って磁化方向を反転させているため
、磁界発生手段1としては前述した漏洩磁界を利用しな
いものと同様に,大出力のものが必要とされ、電力消費
等の問題は解消されない. 本発明は上記事情に鑑みてなされたものであって、上述
の諸問題を解消し、且つ一方向のみのパルス磁界発生に
よってオーバーライトを可能とした光磁気記録装置を提
供することを目的とする.〔課題を解決するための手段
〕 上記目的を達成するため、本発明では、光磁気記録媒体
に光ビームを集光する対物レンズと、永久磁石と電磁コ
イルとを備え上記対物レンズを少なくとも光軸方向に罠
動する対物レンズ駆動手段と、上記光磁気記録媒体へ磁
界を印加する磁界発生手段とを備え、上記光ビームの光
強度若しくは印加磁界の何れか一方若しくは両方を記録
信号に応じて変調することによって情報の記録を行う光
磁気記録装置において,上記対物レンズ廃動手段からの
漏洩磁界の上記記録媒体に対して直交する成分の方向と
光磁気記録媒体の初期磁化方向とが逆方向となるように
構威されていることを特徴とする. 〔作   用〕 本発明によれば、対物レンズ駆動手段からの漏洩磁界の
光磁気記録媒体に対する直交戊分の方向と光磁気記録媒
体の初期磁化方向とを逆方向となるように構成したこと
により、上記漏洩磁界を光磁気記録媒体の記録時の外部
磁界として作用させることができる。
By the way, in the above-mentioned magneto-optical recording device, when performing so-called overwriting, in which the magnetization direction is rewritten to the recorded state by overwriting, the rewriting can be performed efficiently since no special time is required for erasing. It has the advantage of being able to The magnetic field modulation method is well known as a method for performing such overwriting. However, it has not been put into practical use due to various problems. One problem is that with the generally considered overwriting method using the magnetic field modulation method, for example, it is difficult to obtain the second recording state shown in FIG. 6 from the first recording state shown in FIG. Next, the magnetization state of the recording area 4A in FIG. 5 is reversed and erased. On the other hand, in regions 4B and 4C, recording and erasing magnetic fields are generated in opposite directions in the thickness direction of the magnetized film 4, that is, with both positive and negative polarities, in response to the recorded information signal, causing new magnetization reversal. This means that it is necessary to do so. However, in order to make such reversal possible at a high frequency, it is necessary to reduce the number of turns of the electromagnet coil of this magnetic field generating means to reduce the inductance. It becomes necessary to use a large current. However, when the current is made to be a large current in this way, not only does the problem of heat generation due to Joule heat occur, but also it is necessary to make such a large current swing at a high frequency and with both positive and negative polarities reversed. Such an inductive power supply consumes a large amount of power and must be large in size, and furthermore, in this case, it is extremely difficult to obtain one with excellent frequency characteristics. In addition, it is desirable that the level of the magnetic field of both positive and negative polarities for overwriting for recording and erasing described above be relatively large, and a magnetic field generating means for obtaining this external magnetic field is required to have a large output. , the problem of power consumption increases. By the way, a pickup system of a magneto-optical recording device includes an objective lens that focuses a light beam on a magneto-optical recording medium, a permanent magnet, and an electromagnetic coil, and an objective lens driving means that drives the objective lens at least in the optical axis direction. (hereinafter referred to as a lens actuator), and at least focusing adjustment is performed by the lens actuator. Here, the lens actuator has a magnet, such as a permanent magnet, that actually generates a DC magnetic field in a direction perpendicular to the surface of the magneto-optical recording medium, and a forcing servo is installed in the magnetic circuit including this magnet. A moving coil that conducts current is arranged, and the moving coil moves in the optical axis direction in response to the servo current. Such lens actuators are usually magnetically shielded, and consideration is given to reducing the leakage magnetic field from the actuator as much as possible. The problem is that it is not possible. By the way, when the leakage magnetic field of the lens actuator is not applied to the recording medium, the strength of the external magnetic field required for recording and erasing (initial magnetization direction in overwriting) varies depending on the material of the medium and the power of the laser beam, but in general, Erasing requires a stronger magnetic field than recording. The reason for this is that the demagnetizing field (leakage field) from the surrounding magnetized film acts on the magnetized film that is heated during recording, and that demagnetizing field helps reverse the magnetization. Conventionally, the direction of the leakage magnetic field applied from the lens actuator to the magneto-optical recording medium and the initial magnetization (erasing) of the magneto-optical recording medium have been investigated.
Although the relationship with the direction was not specified, for example, in Japanese Patent Application Laid-Open No. 63-66747, the direction of the external magnetic field and the direction of the leakage magnetic field of the lens actuator are made to be the same during erasing, and the leakage magnetic field is used as the erase magnetic field. As shown in FIGS. 7 and 8, a magneto-optical recording device has been proposed in which the initial magnetization (erasing) direction of the perpendicular magnetization film 4 of the magneto-optical recording medium is It can be considered that the direction of the leakage magnetic field 5 from the lens actuator 3 is the same. However, since the magnetization direction is reversed with both positive and negative polarity by the applied magnetic field from the magnetic field generating means 1, the magnetic field generating means 1 has a high output power, similar to the above-mentioned one that does not utilize the leakage magnetic field. However, problems such as power consumption remain unsolved. The present invention has been made in view of the above circumstances, and aims to provide a magneto-optical recording device which solves the above-mentioned problems and enables overwriting by generating a pulsed magnetic field in only one direction. .. [Means for Solving the Problems] In order to achieve the above object, the present invention includes an objective lens for condensing a light beam on a magneto-optical recording medium, a permanent magnet, and an electromagnetic coil, and the objective lens is arranged at least along the optical axis. an objective lens driving means for moving the objective lens in a direction; and a magnetic field generating means for applying a magnetic field to the magneto-optical recording medium, and modulating either the optical intensity of the light beam or the applied magnetic field, or both, according to the recording signal. In a magneto-optical recording device that records information by It is characterized by being structured so that [Function] According to the present invention, the direction of the orthogonal component of the leakage magnetic field from the objective lens driving means with respect to the magneto-optical recording medium is configured to be opposite to the initial magnetization direction of the magneto-optical recording medium. , the leakage magnetic field can be made to act as an external magnetic field during recording on a magneto-optical recording medium.

〔実 施 例〕〔Example〕

以下、本発明を図面を参照して詳細に説明する.第l図
及び第2図は本発明の一実施例を示す光磁気記録装置の
概略的要部構成図であって、第1図は、記録時、第2図
は消去時の状態を夫々示す図であり、図中符号lは電磁
石等からなる外部磁界発生装置、符号2はレーザ光ビー
ムを光磁気記録媒体に集光するための対物レンズ、符号
3は永久磁石とコイルとを備え上記対物レンズ2をその
先軸方向に馳動してフォーカシング制御を行うためのレ
ンズアクチュエータ、符号4は光磁気記録媒体の垂直磁
化膜,符号5はレンズアクチュエータ3からの漏洩磁界
を夫々示している.第1図、第2図において、光磁気記
録媒体は初期状態,すなわち消去時の状態では全領域に
おいて図中下向きに初期磁化されている.また、レンズ
アクチュエータ3からの漏洩磁界5が光磁気記録媒体の
垂直磁化膜4にかかる方向は、垂直磁化膜4の初期磁化
方向とは逆向きとなっている.ここで、レンズアクチュ
エータ3の漏洩磁界5とは、光磁気記録媒体の垂直磁化
膜4に対して直交する磁界或分のことである.尚、第1
図及び第2図に示す例では,光磁気記録媒体の初期磁化
方向を図に対して下向き、レンズアクチュエータ3の漏
洩磁界5は図に対して上向きとしているが、夫々逆向き
としてもよい. さて,本発明は、第1図、第2図に示すような構成の光
磁気記録装置において、レーザー光ビームによって加熱
された垂直磁化膜の記録部周囲の磁化膜からの反磁界6
と、レンズアクチュエータ3からの漏洩磁界5とを記録
用磁界として有効に利用したものである. ここで,対物レンズ2によって集光されたレーザ光ビー
ムによって加熱された磁化膜の周辺からの反磁界6は,
記録方向(オーバーライトでは初期磁化方向の逆)にか
かるため、レンズアクチュエータ3からの漏洩磁界5を
記録磁界として利用するためには漏洩磁界5の磁界方向
を記録方向にする必要があり、この漏洩磁界5と反磁界
6とを同方向とすることにより外部磁界発生装置1によ
る磁界を利用せずに記録(磁化の反転)を行うことが可
能となる. ところで、レンズアクチュエータ3からの漏洩磁界5と
、垂直磁化膜4の加熱部周辺からの反磁界6の向きとが
従来装置のように逆向きとなる場合に、レンズアクチュ
エータ3からの漏洩磁界Sと加熱部周辺からの反磁界6
のみで外部磁界発生装置1による磁界を利用せずに消去
(オーバーライトでは初期磁化方向記録)を行うことが
可能であるが、この場合,漏洩磁界5として非常に大き
な磁界が必要となる.しかるに,漏洩磁界を大きくした
場合、レンズアクチュエータ3の構造が複雑化し、且つ
重量が増大してしまうため、アクセスタイムが遅くなる
等の欠点が生じる.このため、レンズアクチュエータの
漏洩磁界は、本発明のように記録させる方向(オーバー
ライト時では初期磁化方向の逆方向)にした方が有効に
利用できるわけである.そして、この漏洩磁界5と記録
部周辺からの反磁界とを同方向に作用させることにより
、磁化反転に必要な磁界を記録部に与えることができ,
外部磁界発生装置1からの磁界を利用せずに磁気記録を
行えるわけである.次に、記録された情報の消去時(オ
ーバーライトの場合は初期磁化方向)は、外部磁界発生
装置1により磁界を消去方向に印加することで行う.こ
こで、記録/消去、あるいはオーバーライト時の磁界の
印加状態を第3図に示す。ここで,第3図(A)は光磁
気記録媒体を加熱させた時に、レンズアクチュエータの
漏洩磁界aと加熱磁化膜(記録部)周辺の反磁界bとが
加熱磁化膜にかかっていることを示す図である.尚,第
3図において、磁界のl#+rlは記録方向(オーバー
ライトでは初期磁化方向と逆方向)を示し、磁界の71
 −Itは消去方向(オーバーライトでは初期磁化方向
と同方向)を示す. ここで、第3図(A)に示すようにレンズアクチュエー
タの漏洩磁界aと加熱磁化膜周辺の反磁界bとが加熱磁
化膜にかかっている状態時に、第3図(B)に示すよう
な消去方向のみの一方向のパルス磁界を外部磁界発生装
i!!1によって印加した場合,第3図(C)に示すよ
うに情報の記録/消去(または、オーバーライト)を行
うことができる. 尚、光磁気記録媒体にかかるレンズアクチュエータ3か
らの漏洩磁界は、アクチュエータ内の永久磁石の大きさ
や配置を変えることによって調整することができる. さて、以上において説明したように,本発明においては
、レンズアクチュエータ3から漏洩する磁界の記録媒体
と直交する方向の磁界或分を記録磁界として利用し、こ
の漏洩磁界の磁界方向と記録媒体の初期磁化方向(消去
時の磁化方向)とを逆方向にさせたことで、外部磁界発
生装置による磁界を用いずに情報の記録を行うことがで
きる.すなわち,レンズアクチュエータからの漏洩磁界
を消去方向ではなく記録方向とすることで、レンズアク
チュエータの構造の複雑化、重量の増大を抑えることが
でき、アクセスタイムへの影響を防止することができる
. また、外部磁界発生装置1は、記録と消去とで磁界の反
転を行う必要がなく、消去時のみ片チャンネル(一方向
)のパルス磁界を発生するのみで記録媒体に磁化の向き
が反転した消去部と記録部との磁化パターンの形成を行
うことができ、所謂オーバーライトを容易に行うことが
できるので,磁界印加手段の電気的,機械的構或、周波
数特性の向上、更には、その1!源部の構成の簡易化を
図ることができる. 〔発明の効果〕 以上、図面を参照して説明したように、本発明によれば
、対物レンズ駆動手段からの漏洩磁界の光磁気記録媒体
に対する直交威分の方向と光磁気記録媒体の初期磁化方
向(または消去時の磁化方向)とを逆方向となるように
構成したことにより、上記漏洩磁界を光磁気記録媒体の
記録時の外部磁界として作用させることができる. したがって、本発明による光磁気記録装置においては、
外部磁界発生装置による磁界の発生は消去時のみでよく
、一方向のみのパルス磁界発生によってオーバーライト
を行うことが可能なり、従来装置における諸問題、すな
わち、外部磁界発生手段の電気的、機構的問題や、周波
数特性の問題等が解消される.
Hereinafter, the present invention will be explained in detail with reference to the drawings. FIG. 1 and FIG. 2 are schematic diagrams of the main parts of a magneto-optical recording device showing an embodiment of the present invention, with FIG. 1 showing the state during recording and FIG. 2 showing the state during erasing, respectively. In the figure, reference numeral 1 denotes an external magnetic field generator including an electromagnet, 2 an objective lens for condensing a laser beam onto a magneto-optical recording medium, and 3 a permanent magnet and a coil. A lens actuator is used to perform focusing control by moving the lens 2 in the direction of its front axis. Reference numeral 4 indicates a perpendicular magnetization film of a magneto-optical recording medium, and reference numeral 5 indicates a leakage magnetic field from the lens actuator 3. In FIGS. 1 and 2, the magneto-optical recording medium is initially magnetized downward in the figure in its initial state, that is, in the state at the time of erasing. Further, the direction in which the leakage magnetic field 5 from the lens actuator 3 is applied to the perpendicular magnetization film 4 of the magneto-optical recording medium is opposite to the initial magnetization direction of the perpendicular magnetization film 4. Here, the leakage magnetic field 5 of the lens actuator 3 is a magnetic field perpendicular to the perpendicular magnetization film 4 of the magneto-optical recording medium. Furthermore, the first
In the example shown in the figure and FIG. 2, the initial magnetization direction of the magneto-optical recording medium is directed downward with respect to the figure, and the leakage magnetic field 5 of the lens actuator 3 is directed upward with respect to the figure, but the directions may be reversed. Now, the present invention provides a magneto-optical recording device having the configuration shown in FIGS.
The leakage magnetic field 5 from the lens actuator 3 is effectively used as a recording magnetic field. Here, the demagnetizing field 6 from the periphery of the magnetized film heated by the laser beam focused by the objective lens 2 is:
In order to use the leakage magnetic field 5 from the lens actuator 3 as a recording magnetic field, it is necessary to set the magnetic field direction of the leakage magnetic field 5 in the recording direction. By setting the magnetic field 5 and the demagnetizing field 6 in the same direction, it becomes possible to perform recording (reversal of magnetization) without using the magnetic field from the external magnetic field generator 1. By the way, when the leakage magnetic field 5 from the lens actuator 3 and the direction of the demagnetizing field 6 from around the heating part of the perpendicularly magnetized film 4 are opposite as in the conventional device, the leakage magnetic field S from the lens actuator 3 and Demagnetizing field from around the heating part 6
However, in this case, a very large magnetic field is required as the leakage magnetic field 5. However, when the leakage magnetic field is increased, the structure of the lens actuator 3 becomes complicated and the weight increases, resulting in drawbacks such as slow access time. Therefore, the leakage magnetic field of the lens actuator can be used more effectively if it is directed in the recording direction (in the direction opposite to the initial magnetization direction during overwriting) as in the present invention. By causing this leakage magnetic field 5 and the demagnetizing field from around the recording section to act in the same direction, the magnetic field necessary for magnetization reversal can be applied to the recording section.
This means that magnetic recording can be performed without using the magnetic field from the external magnetic field generator 1. Next, when erasing the recorded information (in the initial magnetization direction in the case of overwriting), the external magnetic field generator 1 applies a magnetic field in the erasing direction. Here, FIG. 3 shows the application state of the magnetic field during recording/erasing or overwriting. Here, Figure 3 (A) shows that when the magneto-optical recording medium is heated, the leakage magnetic field a of the lens actuator and the demagnetizing field b around the heated magnetized film (recording section) are applied to the heated magnetized film. This is a diagram showing In Fig. 3, l#+rl of the magnetic field indicates the recording direction (in overwriting, the direction opposite to the initial magnetization direction), and 71 of the magnetic field
-It indicates the erasing direction (in overwriting, the same direction as the initial magnetization direction). Here, when the leakage magnetic field a of the lens actuator and the demagnetizing field b around the heated magnetized film are applied to the heated magnetized film as shown in FIG. 3(A), the magnetic field shown in FIG. 3(B) An external magnetic field generator i! generates a unidirectional pulsed magnetic field in the erase direction only! ! 1, information can be recorded/erased (or overwritten) as shown in FIG. 3(C). Note that the leakage magnetic field from the lens actuator 3 applied to the magneto-optical recording medium can be adjusted by changing the size and arrangement of the permanent magnet in the actuator. Now, as explained above, in the present invention, a portion of the magnetic field leaking from the lens actuator 3 in a direction perpendicular to the recording medium is used as a recording magnetic field, and the magnetic field direction of this leaking magnetic field and the initial state of the recording medium are By making the magnetization direction (magnetization direction during erasing) opposite, information can be recorded without using a magnetic field from an external magnetic field generator. In other words, by directing the leakage magnetic field from the lens actuator in the recording direction rather than in the erasing direction, it is possible to suppress the complexity of the structure and increase in weight of the lens actuator, and prevent the impact on access time. In addition, the external magnetic field generator 1 does not need to reverse the magnetic field between recording and erasing, and only generates a pulsed magnetic field in one channel (one direction) during erasing, so that the direction of magnetization of the recording medium is reversed. It is possible to form a magnetization pattern between the recording part and the recording part, and it is possible to easily perform so-called overwriting. ! The configuration of the source section can be simplified. [Effects of the Invention] As described above with reference to the drawings, according to the present invention, the direction of the orthogonal force of the leakage magnetic field from the objective lens driving means with respect to the magneto-optical recording medium and the initial magnetization of the magneto-optical recording medium can be adjusted. By configuring the magnetization direction (or magnetization direction during erasing) to be opposite, the leakage magnetic field can be made to act as an external magnetic field during recording on the magneto-optical recording medium. Therefore, in the magneto-optical recording device according to the present invention,
The external magnetic field generator only needs to generate a magnetic field during erasing, and overwriting can be performed by generating a pulsed magnetic field in only one direction. problems and problems with frequency characteristics are resolved.

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

第l図及び第2図は本発明の一実施例を示す光磁気記録
装置の概略的要部構威図であって,第1図は記録時、第
2図は消去時の状態を夫々示す図である.第3図は第l
図及び第2図に示す光磁気記録装置による記録/消去若
しくはオーバーライト時の磁界の印加状態を説明するた
めの図、第4図乃至第6図は光磁気記録媒体の記録状態
を説明するための図、第7図及び第8図は従来技術の一
例を示す光磁気記録装置の概略的要部構成図であって、
第7図は記録時,第8図は消去時の状態を夫々示す図で
ある. 1・・・・外部磁界発生装置、2・・・・対物レンズ、
3・・・・対物レンズ駆動手段、4・・・・光磁気記録
媒体の垂直磁化膜、5・・・・対物レンズ駆動手段から
の漏洩磁界、6・・・・反転磁界、7・・・・外部磁界
発生装置による印加磁界.
FIG. 1 and FIG. 2 are schematic diagrams of the main parts of a magneto-optical recording device showing an embodiment of the present invention, with FIG. 1 showing the state during recording and FIG. 2 showing the state during erasing, respectively. This is a diagram. Figure 3 is
Figures 4 to 6 are diagrams for explaining the state of application of a magnetic field during recording/erasing or overwriting by the magneto-optical recording device shown in Figures 2 and 2, and Figures 4 to 6 are diagrams for explaining the recording state of the magneto-optical recording medium. , FIG. 7, and FIG. 8 are schematic main part configuration diagrams of a magneto-optical recording device showing an example of the prior art,
Fig. 7 shows the state during recording, and Fig. 8 shows the state during erasing. 1...External magnetic field generator, 2...Objective lens,
3... Objective lens driving means, 4... Perpendicular magnetization film of magneto-optical recording medium, 5... Leakage magnetic field from the objective lens driving means, 6... Reversal magnetic field, 7...・Magnetic field applied by an external magnetic field generator.

Claims (1)

【特許請求の範囲】[Claims] 光磁気記録媒体に光ビームを集光する対物レンズと、永
久磁石と電磁コイルとを備え上記対物レンズを少なくと
も光軸方向に駆動する対物レンズ駆動手段と、上記光磁
気記録媒体へ磁界を印加する磁界発生手段とを備え、上
記光ビームの光強度若しくは印加磁界の何れか一方若し
くは両方を記録信号に応じて変調することにより情報の
記録を行う光磁気記録装置において、上記対物レンズ駆
動手段からの漏洩磁界の上記記録媒体に対して直交する
成分の方向と光磁気記録媒体の初期磁化方向とが逆方向
となるように構成されていることを特徴とする光磁気記
録装置。
an objective lens that focuses a light beam on a magneto-optical recording medium; an objective lens driving means that includes a permanent magnet and an electromagnetic coil and drives the objective lens at least in the optical axis direction; and a magnetic field that applies a magnetic field to the magneto-optical recording medium. In the magneto-optical recording device, which records information by modulating either the light intensity of the light beam or the applied magnetic field, or both, according to a recording signal, the magnetic field generating means is provided with a magnetic field generating means. A magneto-optical recording device characterized in that the direction of the component of the leakage magnetic field orthogonal to the recording medium and the initial magnetization direction of the magneto-optical recording medium are opposite directions.
JP15084389A 1989-06-14 1989-06-14 Magneto-optical recorder Pending JPH0317846A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15084389A JPH0317846A (en) 1989-06-14 1989-06-14 Magneto-optical recorder

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15084389A JPH0317846A (en) 1989-06-14 1989-06-14 Magneto-optical recorder

Publications (1)

Publication Number Publication Date
JPH0317846A true JPH0317846A (en) 1991-01-25

Family

ID=15505592

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15084389A Pending JPH0317846A (en) 1989-06-14 1989-06-14 Magneto-optical recorder

Country Status (1)

Country Link
JP (1) JPH0317846A (en)

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