JPH02235231A - Magneto-optical recording medium, magneto-optical recording method, magneto-optical erasing method, and magneto-optical recording and reproducing device - Google Patents

Magneto-optical recording medium, magneto-optical recording method, magneto-optical erasing method, and magneto-optical recording and reproducing device

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Publication number
JPH02235231A
JPH02235231A JP5521689A JP5521689A JPH02235231A JP H02235231 A JPH02235231 A JP H02235231A JP 5521689 A JP5521689 A JP 5521689A JP 5521689 A JP5521689 A JP 5521689A JP H02235231 A JPH02235231 A JP H02235231A
Authority
JP
Japan
Prior art keywords
layer
magneto
magnetic field
magnetization
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
JP5521689A
Other languages
Japanese (ja)
Inventor
Yasuyuki Miyaoka
康之 宮岡
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP5521689A priority Critical patent/JPH02235231A/en
Publication of JPH02235231A publication Critical patent/JPH02235231A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To thin a device by laminating two magnetic layers respectively having a specific Curie point and room temperature coercive force, setting up the magnetization of both the magnetic layers in the stable direction of magnetization and using one of the magnetic layer as an auxiliary magnetic field forming layer and the other as a recording layer. CONSTITUTION:The recording layer 33 has a low Curie point and high coercive force at a room temperature and the auxiliary magnetic field forming layer 30 has a Curie point higher than that of the layer 33 and low coercive force at the room temperature. When magnetic field intensity Hb for inverting only the magnetization of the layer 30 by a bias magnetic field head 7 in an erasing state e.g. is impressed in the shown arrow direction, only the magnetization of the layer 30 is inverted and a recordably state is set up. When the surface of the layer 33 is irradiated with a laser beam modulated by an information signal and the laser beam is condensed thereon, only the laser 33 reaches the Curie point, and in a process reducing the temperature from the Curie point, the direction of the magnetization is reversed from that of the erasing state and recording can be executed. Consequently, it becomes unnecessary to arrange the bias magnetic field head 7 oppositely to the optical head 3 and the device can be thinned.

Description

【発明の詳細な説明】[Detailed description of the invention]

[産業上の利用分野】 本発明は光磁気記録方式を採用した光磁気記録媒体、該
媒体に情報を記録する方法、消去する方法、および光磁
気記録再生装置に関するものである.
[Field of Industrial Application] The present invention relates to a magneto-optical recording medium employing a magneto-optical recording method, a method for recording information on the medium, a method for erasing information, and a magneto-optical recording and reproducing apparatus.

【従来の技術】[Conventional technology]

従来,光磁.気による記録および再生を行なう光磁気記
録再生消去装置は第6図に示すような構成を取っている
のが普通であった. 同図において、光磁気ディスク1はガラス基板10等に
垂直磁化膿2を被着したものであり、この光磁気ディス
ク1をはさんで光ヘッド3、バイアス磁界ヘッド7を配
置した構成となっている.ここでバイアス磁界ヘッド7
はコイル8に電流を流すことによって成る電磁石で、コ
イル8に流す電流の向きを磁界駆動回路9により制御す
ることによって、バイアス磁界ヘッド7から発生する磁
界の向きを切り換えることができるようになっている.
この時、記録時又は消去時でそれぞれ、定磁界強度を発
生するようになっている.また、光ヘッド3は光磁気デ
ィスクlの半径方向に移動するようになっており,又光
磁気ディスクlに対してバイアス磁界ヘッド7に対向し
て配置される. 光ヘッド3は内蔵する半導体レーザより照射されるレー
ザ光を垂直磁化膜2上に焦点を結ぶようになっており、
端子5から入力される情報信号により光変調回路4が動
作して光ヘッド3を駆動する.また、光磁気ディスク1
はスピンドルモータ6により回転されるようになってい
る.以上の構成において、第7図に示すように記録信号
が入力されると、例えばここでは記録時の磁界強度をH
,とすると、記録信号によって変調されたレーザ光が垂
直磁化膜2上に照射され、照射された部分の垂直磁化膜
2がキエーリ点以上の温度になり、印加されたバイアス
磁界により、その部位の磁化が反転し、記録ビットが形
成される.[発明が解決しようとしている課題] しかしながら、上記従来例ではバイアス磁界ヘッド7を
光磁気ディスクlに対して、光ヘッド3に対向した位置
に配置する必要があり、光磁気記録再生消去装置の薄型
化を防げるという欠点があった。 [課題を解決するための手段】 本発明の目的は、上記欠点に鑑み、光磁気記録再生消去
装置を薄型化できる光磁気記録媒体、光磁気記録方法及
び光磁気消去方法、光磁気記録再生消去装置を提供する
ことある. 以上のような目的の達成のため、まず、低いキューリ点
TLと室温において高い保持力H.を有する第1の磁性
層と、この磁性層に比べて相対的に高いキューリ点TH
と室温において低い保持力HLを有する第2の磁性層を
少なくとも積層し、両磁性層の磁化を磁化の安定な向き
(平行で反平行でもよい)に設定し、前記第2の磁性層
を補助磁界形成層として、また前記第1の磁性層を記録
層として使用することを特徴とする光磁気記録媒体を提
供する. 次に、その光磁気記録媒体を使用し、外部磁界印加手段
により室温で前記補助磁界形成層の磁化の向きのみを逆
方向に磁化した後で,前記記録層を記録信号で強度変調
された光ビームで走査し、該逆方向の磁化の向きに対し
てエネルギー的に安定な方向に該記録層を磁化すること
により、情報を記録する光磁気記録方法を提供する.更
に上記の手順で記録された状態において、外部磁界印加
手段により室温で前記補助磁界形成層の磁化の向きを元
の方向に磁化した後で、前記記録層を連続光ビームで走
査し、該元方向の磁化の向きに対してエネルギー的に安
定な方向に該記録層を全て磁化することにより、情報を
消去する光磁気消去方法を提供する. 最後に本発明に係る光磁気記録媒体を使用し、前記外部
磁界印加手段と前記光ビームを発する光ヘッドとが共に
記録媒体の片側に設けられていることを特徴とする光磁
気記録再生装置を提供する. 上記のような目的は、上記4発明により達成される. [作用] 本発明によれば、光磁気ディスクの垂直磁化膿を2層膜
以上の多層膜とし、バイアス磁界ヘッドにより印加され
るバイアス磁界により1層の磁化の向きが決定され、他
層はバイアス磁界の影響を受けず、バイアス磁界が印加
された部位にレーザ光を照射した場合、バイアス磁界に
より磁化が決定された層に対して、他層がエネルギー的
に安定な方向に磁化されるような垂直磁化多層膜を使用
することにより、バイアス磁界ヘッドを光ヘッドに対向
して置く必要がなくなり、バイアス磁界ヘッドを光ヘッ
ドと同一面内に配置することが可能となり、光磁気記録
(消去も含む)再生装置の薄型化を可能とすることがで
きる. [実施例] 以下、本発明に係る光磁気記録媒体、光磁気記録方法、
光磁気消去方法及び光磁気記録再生装置を具体的な実施
例に基づき詳細に説明する.第1図は本発明の光磁気記
録再生装置の特徴を最もよ《表わす一実施例である. 同図において、1は多層膜垂直磁化膜2をガラス基板1
0に被着した光磁気ディスクである.光磁気ディスク1
はスピンドルモータ6により、中心軸0−0゜を中心と
して回転するようになっている.3は半導体レーザな基
本として成る光ヘッドであり、光ヘッド3は光変調回路
4により駆動され、光変調回路4は端子5から入力され
る情報信号により駆動される.光ヘッド3は半導体レー
ザから照射されたレーザ光を常に光磁気ディスク1の多
層膜垂直磁化膿2上に集光するように構成されている.
また、光ヘッド3は光磁気ディスク1の半径方向に移動
することができるよう構成されている.7は光ヘッド3
と同一面内に配置されたバイアス磁界ヘッドであり、コ
イル8を巻いた電磁石から構成されている.バイアス磁
界ヘッド7は磁界駆動回路9により、磁界を発生するよ
うに横成されている.この磁界ヘッド7は光磁気ディス
ク1の半径方向全域において、一定のバイアス磁界が印
加されるようになっている.以上説明したような構成に
おいて、第2図に記録動作原理、第3図に消去動作原理
を示す。 第2図において2は光磁気ディスク1の多層膜垂直磁化
膜であり、ここでは2層膜構成とする.そのうち、30
は補助磁界形成層(以下、補助層という)となる第2の
磁性層、33は記録層としての第1の磁性層である.第
1の磁性層33は低いキューリ点TLと室温において高
い保持力H.を有し、第2の磁性層30は該第1の磁性
層33に比べて相対的に高いキューリ点THと室温にお
いて低い保持力HLを有している.それらの特性の一例
を縦軸に保持力、横軸に温度をとり、第4図及び第5図
に示す.両図において40は第1の磁性層33の特性曲
線、44は第2の磁性層30の特性曲線である=また、
第4図においては第2の磁性層30の特性曲!144は
キューリ点の補償点を有しているが、本発明においては
第4図のみならず、第5図の構成も採用することができ
る.再び第2図において、各膜内の矢印は各層の磁化の
方向を示すものである.補助層30は室温において、バ
イアス磁界H.によって磁化の向きが決定されるのに対
し、記録層33は何ら影響を受けないように特性及びバ
イアス磁界HI,が決定される.また、記録層33に照
射するレーザ光の強度は、記録層33のみキューリ点T
Lに違し、補助層30のキューリ点THには達しない強
度が選ばれる. 上記特性を持つ構成において、(a)の状態がエネルギ
ー的に安定である2層膿垂直磁化膜とし、これを消去状
態とする.この状態においてバイアス磁界ヘッド7によ
って補助層30の磁化のみを反転させる磁界強度H.(
第4図及び第5図参照)を図中に示す方向に印加すると
補助層30のみの磁化が反転し、(b)のような磁化状
態となる.この状態を記録可能状態とする.記録可能状
態にある2層膜垂直磁化膿に、情報信号によって,変調
されたレーザ光(その強い光パワー範囲域は第4図及び
第5図参照)を記録層33上に照射、集光させると、前
記説明したように、記録層33の垂直磁化膜のみキエー
り点に達する.記録層33の垂直磁化膜の温度がキュー
リ点から下がる過程で記録層33の垂直磁化膜のm化の
向きは、交換結合力により、補助層30の磁化の向きに
対して、エネルギー的に安定な方向に磁化が向《ことに
なる.この磁化の向きは消去状態(a)の記録層33の
磁化向きと逆になり、結果として記録が行なえる. 第3図は消去動作原理を示すものである.第3図(a)
は第2図(c)に相当する記録した状態を示す.この記
録状態の2層膜垂直磁化膿にバイアス磁界ヘッド7によ
り記録時とは逆方向にバイアス磁界強度Hbを図中に示
すように印加する.バイアス磁界H.が印加されると、
高い保持力を有する記録層33の磁化の向きは変化せず
、補助層30の磁化のみがバイアス磁界H,を印加した
方向に向く.この状態を消去可能状態とする.消去可能
状態では記録層33に記録された記録情報は変化なく残
っている(第3図(b))。この消去可能状態にある2
眉膜垂直磁化膿に、記録層33のみがキューリ点に達す
るようなレーザ光強度で連続的に、レーザ光を照射する
ことにより、記録層33の垂直磁化膜はキエーり点に達
し、温度が低下する過程において、記録時と同様に交換
結合力により、補助層30の磁化の向きに対してエネル
ギー的に安定となるような方向に記録層33の磁化の向
きが決定される.したがって、磁化の向きが決定された
後は第2図に示す(a)の消去状態と同じになり消去さ
れる(第3図(c)). 本発明は上記実施例に限らず種々の実施例が可能である
。 例えば、第2図(a)における補助層30と記録層33
の磁化の安定な向きは平行でも反平行でもよい. また、第1図においては、光ヘッド3とバイアス磁界ヘ
ッド7が距離的に離れた構成を示しているが、光ヘッド
3のすぐ前に配置する構成でもよい。 〔発明の効果〕 以上説明したように、本発明の記録媒体,記録方法,消
去方法,および記録再生装置によれば、バイアス磁界ヘ
ッドを光ヘッドに対向して置く必要がなくなり、バイア
ス磁界ヘッドを光ヘッドと同一面内に配置することが可
能となり、光磁気記録再生消去装置が薄型化できる効果
がある。 また、本発明によれば、従来の構成に比べてレーザバワ
ーが少なくてすむという効果がある.
Conventionally, magneto-optical. Magneto-optical recording/erasing devices that perform recording and playback using air generally have the configuration shown in Figure 6. In the figure, a magneto-optical disk 1 is a glass substrate 10 or the like coated with perpendicular magnetism 2, and an optical head 3 and a bias magnetic field head 7 are arranged across the magneto-optical disk 1. There is. Here, bias magnetic field head 7
is an electromagnet formed by passing a current through a coil 8, and by controlling the direction of the current flowing through the coil 8 by a magnetic field drive circuit 9, the direction of the magnetic field generated from the bias magnetic field head 7 can be switched. There is.
At this time, a constant magnetic field strength is generated during recording or erasing, respectively. Further, the optical head 3 is adapted to move in the radial direction of the magneto-optical disk l, and is arranged opposite to the bias magnetic field head 7 with respect to the magneto-optical disk l. The optical head 3 focuses laser light emitted from a built-in semiconductor laser onto the perpendicularly magnetized film 2.
The optical modulation circuit 4 is operated by the information signal input from the terminal 5 to drive the optical head 3. Also, magneto-optical disk 1
is rotated by a spindle motor 6. In the above configuration, when a recording signal is input as shown in FIG.
, then the laser beam modulated by the recording signal is irradiated onto the perpendicularly magnetized film 2, the irradiated part of the perpendicularly magnetized film 2 reaches a temperature above the Chieri point, and the applied bias magnetic field causes the part of the perpendicularly magnetized film 2 to become heated. The magnetization is reversed and a recorded bit is formed. [Problems to be Solved by the Invention] However, in the conventional example described above, it is necessary to arrange the bias magnetic field head 7 at a position facing the optical head 3 with respect to the magneto-optical disk l, which makes the magneto-optical recording/reproducing/erasing device thin. The disadvantage was that it could prevent oxidation. [Means for Solving the Problems] In view of the above-mentioned drawbacks, an object of the present invention is to provide a magneto-optical recording medium, a magneto-optical recording method, a magneto-optical erasing method, and a magneto-optical recording method that can reduce the thickness of a magneto-optical recording/reproducing/erasing device. We may provide equipment. In order to achieve the above objectives, first of all, we need a low Curie point TL and a high holding power H. at room temperature. a first magnetic layer having a relatively high Curie point TH compared to this magnetic layer;
and a second magnetic layer having a low coercive force HL at room temperature, the magnetization of both magnetic layers is set in a stable magnetization direction (parallel or antiparallel may be used), and the second magnetic layer is auxiliary. A magneto-optical recording medium is provided, characterized in that the first magnetic layer is used as a magnetic field forming layer and as a recording layer. Next, using the magneto-optical recording medium, after magnetizing only the direction of magnetization of the auxiliary magnetic field forming layer in the opposite direction at room temperature using an external magnetic field applying means, the recording layer is exposed to light whose intensity is modulated by the recording signal. A magneto-optical recording method for recording information is provided by scanning with a beam and magnetizing the recording layer in a direction that is energetically stable with respect to the opposite direction of magnetization. Furthermore, in the state recorded in the above procedure, after the magnetization direction of the auxiliary magnetic field forming layer is magnetized in the original direction at room temperature by an external magnetic field applying means, the recording layer is scanned with a continuous light beam to record the original. Provided is a magneto-optical erasing method for erasing information by magnetizing all of the recording layer in a direction that is energetically stable with respect to the direction of magnetization. Finally, there is provided a magneto-optical recording and reproducing apparatus using the magneto-optical recording medium according to the present invention, wherein the external magnetic field applying means and the optical head for emitting the light beam are both provided on one side of the recording medium. provide. The above objects are achieved by the above four inventions. [Function] According to the present invention, the perpendicular magnetization of the magneto-optical disk is made into a multilayer film of two or more layers, and the direction of magnetization of one layer is determined by the bias magnetic field applied by the bias magnetic field head, and the direction of magnetization of the other layers is determined by the bias magnetic field applied by the bias magnetic field head. If a laser beam is applied to a region that is not affected by a magnetic field and a bias magnetic field is applied, the layer whose magnetization is determined by the bias magnetic field will be magnetized in a direction that is energetically stable. By using a perpendicular magnetization multilayer film, there is no need to place the bias magnetic field head opposite the optical head, and the bias magnetic field head can be placed in the same plane as the optical head. ) It is possible to make the playback device thinner. [Example] Hereinafter, a magneto-optical recording medium, a magneto-optical recording method according to the present invention,
The magneto-optical erasing method and magneto-optical recording/reproducing device will be explained in detail based on specific examples. FIG. 1 is an embodiment that best represents the features of the magneto-optical recording and reproducing apparatus of the present invention. In the same figure, 1 is a multilayer perpendicularly magnetized film 2 placed on a glass substrate 1.
This is a magneto-optical disk coated with 0. magneto-optical disk 1
is rotated by a spindle motor 6 around a central axis of 0-0°. Reference numeral 3 designates an optical head basically consisting of a semiconductor laser. The optical head 3 is driven by an optical modulation circuit 4, and the optical modulation circuit 4 is driven by an information signal inputted from a terminal 5. The optical head 3 is configured to always focus laser light emitted from a semiconductor laser onto the multilayer perpendicular magnetization layer 2 of the magneto-optical disk 1.
Further, the optical head 3 is configured to be able to move in the radial direction of the magneto-optical disk 1. 7 is optical head 3
This is a bias magnetic field head placed in the same plane as the . The bias magnetic field head 7 is horizontally configured to generate a magnetic field by a magnetic field drive circuit 9. This magnetic field head 7 is configured to apply a constant bias magnetic field to the entire radial area of the magneto-optical disk 1. In the configuration described above, FIG. 2 shows the principle of recording operation, and FIG. 3 shows the principle of erasing operation. In FIG. 2, numeral 2 denotes a multilayer perpendicular magnetization film of the magneto-optical disk 1, which here has a two-layer structure. Of these, 30
33 is a second magnetic layer serving as an auxiliary magnetic field forming layer (hereinafter referred to as an auxiliary layer), and 33 is a first magnetic layer serving as a recording layer. The first magnetic layer 33 has a low Curie point TL and a high coercive force H at room temperature. The second magnetic layer 30 has a relatively high Curie point TH and a low coercive force HL at room temperature compared to the first magnetic layer 33. An example of these characteristics is shown in Figures 4 and 5, with holding force on the vertical axis and temperature on the horizontal axis. In both figures, 40 is the characteristic curve of the first magnetic layer 33, and 44 is the characteristic curve of the second magnetic layer 30.
In FIG. 4, the characteristic curve of the second magnetic layer 30! 144 has a compensation point for the Curie point, but in the present invention, not only the configuration shown in FIG. 4 but also the configuration shown in FIG. 5 can be adopted. Referring again to FIG. 2, the arrows within each film indicate the direction of magnetization of each layer. The auxiliary layer 30 is exposed to a bias magnetic field H. On the other hand, the characteristics and bias magnetic field HI of the recording layer 33 are determined so as not to be affected in any way. In addition, the intensity of the laser beam irradiated to the recording layer 33 is such that only the recording layer 33 has a Curie point T.
Unlike L, an intensity that does not reach the Curie point TH of the auxiliary layer 30 is selected. In the configuration having the above characteristics, the state (a) is a two-layer perpendicular magnetization film that is energetically stable, and this is set as the erased state. In this state, the bias magnetic field head 7 is used to invert only the magnetization of the auxiliary layer 30 with a magnetic field strength H. (
4 and 5) in the direction shown in the figures, the magnetization of only the auxiliary layer 30 is reversed, resulting in a magnetization state as shown in (b). This state is the recordable state. A laser beam modulated by an information signal (see FIGS. 4 and 5 for the strong optical power range) is irradiated and focused onto the recording layer 33 of the double-layer film perpendicularly magnetized in a recordable state. As explained above, only the perpendicularly magnetized film of the recording layer 33 reaches the key point. As the temperature of the perpendicularly magnetized film of the recording layer 33 decreases from the Curie point, the direction of m-ization of the perpendicularly magnetized film of the recording layer 33 becomes energetically stable with respect to the magnetization direction of the auxiliary layer 30 due to exchange coupling force. The magnetization will be directed in the direction. The direction of this magnetization is opposite to the direction of magnetization of the recording layer 33 in the erased state (a), and as a result, recording can be performed. Figure 3 shows the principle of erasure operation. Figure 3(a)
shows the recorded state corresponding to Fig. 2(c). A bias magnetic field intensity Hb is applied to the perpendicular magnetization of the two-layer film in this recorded state by a bias magnetic field head 7 in a direction opposite to that during recording, as shown in the figure. Bias magnetic field H. is applied,
The direction of magnetization of the recording layer 33, which has a high coercive force, does not change, and only the magnetization of the auxiliary layer 30 is oriented in the direction to which the bias magnetic field H is applied. Let this state be the erasable state. In the erasable state, the recorded information recorded on the recording layer 33 remains unchanged (FIG. 3(b)). 2 in this erasable state
By continuously irradiating the perpendicular magnetization of the eyebrow membrane with laser light at a laser light intensity such that only the recording layer 33 reaches the Curie point, the perpendicular magnetization film of the recording layer 33 reaches the Curie point and the temperature decreases. In the process of decreasing, the direction of magnetization of the recording layer 33 is determined by the exchange coupling force in a direction that is energetically stable with respect to the direction of magnetization of the auxiliary layer 30, as in the case of recording. Therefore, after the direction of magnetization is determined, the data is erased in the same state as shown in FIG. 2(a) (FIG. 3(c)). The present invention is not limited to the embodiments described above, and various embodiments are possible. For example, the auxiliary layer 30 and the recording layer 33 in FIG.
The stable direction of magnetization of can be parallel or antiparallel. Further, although FIG. 1 shows a configuration in which the optical head 3 and the bias magnetic field head 7 are separated in distance, a configuration in which the optical head 3 and the bias magnetic field head 7 are disposed immediately in front of the optical head 3 may also be used. [Effects of the Invention] As explained above, according to the recording medium, recording method, erasing method, and recording/reproducing apparatus of the present invention, it is no longer necessary to place the bias magnetic field head opposite to the optical head, and the bias magnetic field head can be It can be placed in the same plane as the optical head, which has the effect of making the magneto-optical recording/reproducing/erasing device thinner. Further, according to the present invention, there is an effect that less laser power is required compared to the conventional configuration.

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

第1図は本発明の光磁気記録再生消去装置の一実施例を
示す構成図、第2図は第1図の記録プロセスを示す図、
第3図は第1図の消去プロセスを示す図、第4図及び第
5図はそれぞれ補助層と記録層の特性を示す図、第6図
は従来の光磁気記録再生消去装置の構成図、第7図は第
6図の記録プロセスを示す図である. l:光磁気ディスク、2:垂直磁化膜,、3o:補助層
、33二記録層、3:光ヘッド、4:光変調回路、5:
入力端子、6:スピンドルモータ,7;バイアス磁界ヘ
ッド、8:コイル、9:磁界駆動回路、10:ガラス基
板. 第1図 O 代理人 弁理士  山 下  穣 平 0−・−カ゛テ入暮状 《0》 :l4云仄.亀 第2図 (b) 言乙一k;rJと状勉 (C) tL課択1樫L 第 図 7・−−−ノ(イアス」早へ,ト” 9−−−・羞五界J!!勤口jト 第 図
FIG. 1 is a block diagram showing an embodiment of the magneto-optical recording/erasing device of the present invention, FIG. 2 is a diagram showing the recording process of FIG. 1,
FIG. 3 is a diagram showing the erasing process of FIG. 1, FIGS. 4 and 5 are diagrams showing the characteristics of the auxiliary layer and the recording layer, respectively, and FIG. 6 is a block diagram of a conventional magneto-optical recording/reproducing/erasing device. Figure 7 is a diagram showing the recording process of Figure 6. l: magneto-optical disk, 2: perpendicular magnetization film, 3o: auxiliary layer, 33 second recording layer, 3: optical head, 4: optical modulation circuit, 5:
Input terminal, 6: spindle motor, 7: bias magnetic field head, 8: coil, 9: magnetic field drive circuit, 10: glass substrate. Figure 1 O Agent Patent attorney Minoru Yamashita Hei 0--Category letter of entry《0》:l4 information. Tortoise Figure 2 (b) Kototsuichik;rJ and Shoben (C) tL Lesson Choice 1 KashiL Figure 7. !Attendance diagram

Claims (4)

【特許請求の範囲】[Claims] (1)低いキューリ点T_Lと室温において高い保持力
H_Hを有する第1の磁性層と、この磁性層に比べて相
対的に高いキューリ点T_Hと室温において低い保持力
H_Lを有する第2の磁性層を少なくとも積層し、両磁
性層の磁化を磁化の安定な向きに設定し、前記第2の磁
性層を補助磁界形成層として、また前記第1の磁性層を
記録層として使用することを特徴とする光磁気記録媒体
(1) A first magnetic layer that has a low Curie point T_L and a high coercive force H_H at room temperature, and a second magnetic layer that has a relatively high Curie point T_H and a low coercive force H_L at room temperature compared to this magnetic layer. are laminated at least, the magnetization of both magnetic layers is set in a stable magnetization direction, the second magnetic layer is used as an auxiliary magnetic field forming layer, and the first magnetic layer is used as a recording layer. magneto-optical recording medium.
(2)請求項1記載の光磁気記録媒体を使用し、外部磁
界印加手段により室温で前記補助磁界形成層の磁化の向
きのみを逆方向に磁化した後で、前記記録層を記録信号
で強度変調された光ビームで走査し、該逆方向の磁化の
向きに対してエネルギー的に安定な方向に該記録層を磁
化することにより、情報を記録する光磁気記録方法。
(2) Using the magneto-optical recording medium according to claim 1, after magnetizing only the magnetization direction of the auxiliary magnetic field forming layer in the opposite direction at room temperature by an external magnetic field applying means, the recording layer is intensified with a recording signal. A magneto-optical recording method for recording information by scanning with a modulated light beam and magnetizing the recording layer in a direction that is energetically stable with respect to the opposite direction of magnetization.
(3)請求項2記載の手順で記録された状態において、
外部磁界印加手段により室温で前記補助磁界形成層の磁
化の向きを元の方向に磁化した後で、前記記録層を連続
光ビームで走査し、該元方向の磁化の向きに対してエネ
ルギー的に安定な方向に該記録層を全て磁化することに
より、情報を消去する光磁気消去方法。
(3) In the state recorded by the procedure set forth in claim 2,
After the direction of magnetization of the auxiliary magnetic field forming layer is magnetized in the original direction at room temperature by an external magnetic field applying means, the recording layer is scanned with a continuous light beam, and the direction of magnetization in the original direction is changed energetically. A magneto-optical erasing method that erases information by magnetizing all of the recording layer in a stable direction.
(4)請求項1記載の光磁気記録媒体を使用し、前記外
部磁界印加手段と前記光ビームを発する光ヘッドとが共
に記録媒体の片面側に設けられていることを特徴とする
光磁気記録再生装置。
(4) Magneto-optical recording using the magneto-optical recording medium according to claim 1, wherein the external magnetic field applying means and the optical head for emitting the light beam are both provided on one side of the recording medium. playback device.
JP5521689A 1989-03-09 1989-03-09 Magneto-optical recording medium, magneto-optical recording method, magneto-optical erasing method, and magneto-optical recording and reproducing device Pending JPH02235231A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5521689A JPH02235231A (en) 1989-03-09 1989-03-09 Magneto-optical recording medium, magneto-optical recording method, magneto-optical erasing method, and magneto-optical recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5521689A JPH02235231A (en) 1989-03-09 1989-03-09 Magneto-optical recording medium, magneto-optical recording method, magneto-optical erasing method, and magneto-optical recording and reproducing device

Publications (1)

Publication Number Publication Date
JPH02235231A true JPH02235231A (en) 1990-09-18

Family

ID=12992425

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5521689A Pending JPH02235231A (en) 1989-03-09 1989-03-09 Magneto-optical recording medium, magneto-optical recording method, magneto-optical erasing method, and magneto-optical recording and reproducing device

Country Status (1)

Country Link
JP (1) JPH02235231A (en)

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