JPH0386954A - Magneto-optical recorder - Google Patents
Magneto-optical recorderInfo
- Publication number
- JPH0386954A JPH0386954A JP22342389A JP22342389A JPH0386954A JP H0386954 A JPH0386954 A JP H0386954A JP 22342389 A JP22342389 A JP 22342389A JP 22342389 A JP22342389 A JP 22342389A JP H0386954 A JPH0386954 A JP H0386954A
- Authority
- JP
- Japan
- Prior art keywords
- recording
- magnetic field
- layer
- magnetic
- reference layer
- 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
Links
- 230000005291 magnetic effect Effects 0.000 claims abstract description 88
- 230000005415 magnetization Effects 0.000 claims abstract description 62
- 230000001678 irradiating effect Effects 0.000 claims description 3
- BGPVFRJUHWVFKM-UHFFFAOYSA-N N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] Chemical compound N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] BGPVFRJUHWVFKM-UHFFFAOYSA-N 0.000 abstract description 9
- 229910052723 transition metal Inorganic materials 0.000 description 11
- 150000003624 transition metals Chemical class 0.000 description 10
- 238000010586 diagram Methods 0.000 description 8
- 229910052761 rare earth metal Inorganic materials 0.000 description 4
- 150000002910 rare earth metals Chemical class 0.000 description 4
- 230000006866 deterioration Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000000696 magnetic material Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000008034 disappearance Effects 0.000 description 1
- 239000002902 ferrimagnetic material Substances 0.000 description 1
- 230000006870 function Effects 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 230000008929 regeneration Effects 0.000 description 1
- 238000011069 regeneration method Methods 0.000 description 1
- 239000004575 stone Substances 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明は、記録層と参照層とを含む多層の磁性層に局
部的に光を照射することにより、記録層に対して情報の
記録・消去を行なう光磁気記録装置に関するものであり
、特に、記録を安定に保持した高信頼性を有する光磁気
記録媒体を与えるように改良された光磁気記録装置に関
するものである。Detailed Description of the Invention [Industrial Field of Application] The present invention enables recording and recording of information on a recording layer by locally irradiating light onto a multilayer magnetic layer including a recording layer and a reference layer. The present invention relates to a magneto-optical recording device that performs erasing, and more particularly to a magneto-optical recording device that has been improved to provide a highly reliable magneto-optical recording medium that stably retains records.
[従来の技術]
磁気記録媒体に局部的に光を照射し、その熱エネルギに
よって媒体を磁化反転温度付近まで加熱すると抗磁力が
低下する。この状態で弱い外部磁界を加えることにより
光照射領域のみに残留磁化を与える記録方式を光磁気記
録という。光源としてレーザビームを使用するので高密
度記録が可能である。[Prior Art] When a magnetic recording medium is locally irradiated with light and its thermal energy is used to heat the medium to near the magnetization reversal temperature, the coercive force decreases. A recording method that applies a weak external magnetic field in this state to produce residual magnetization only in the light irradiated area is called magneto-optical recording. Since a laser beam is used as a light source, high-density recording is possible.
第7図は、たとえば刊行物(Internationa
l Symposium on 0ptical
Memory ’ 87 TECHNICAL
DIGEST)に示された従来の光磁気記録装置の
概略構成図を示し、第8図にその要部を断面図で示す。FIG. 7 shows, for example, a publication (International
Symposium on 0ptical
Memory '87 TECHNICAL
A schematic configuration diagram of a conventional magneto-optical recording device shown in ``DIGEST'' is shown, and FIG. 8 shows a cross-sectional view of the main part thereof.
これらの図を参照して、光磁気記録装置は、記録層3と
参照層4とを含む記録媒体1に情報を記録したり、記録
媒体1から情報を再生するものであり、基本的に記録系
と再生系とからなる。Referring to these figures, the magneto-optical recording device records information on a recording medium 1 including a recording layer 3 and a reference layer 4, and reproduces information from the recording medium 1, and basically records information. It consists of a system and a regeneration system.
記録系は、レーザ光源13と偏光子11と偏光ビームス
プリッタ10aと集光レンズ9と、記録消去時のレーザ
ビーム強度でのみ、磁性層の磁化方向に変化を与える磁
界を発生する第1外部磁石5と、記録層3の磁化方向に
かかわらず、参照層4の磁化方向が一様になるように、
該参照層4を磁化する磁界を発生する第2外部磁石6と
を備える。一方、再生系は、1対の光検出器14と、1
対の検光子12と、偏光ビームスプリッタ10bとから
なる。The recording system includes a laser light source 13, a polarizer 11, a polarizing beam splitter 10a, a condenser lens 9, and a first external magnet that generates a magnetic field that changes the magnetization direction of the magnetic layer only with the laser beam intensity during recording erasure. 5, so that the magnetization direction of the reference layer 4 is uniform regardless of the magnetization direction of the recording layer 3.
and a second external magnet 6 that generates a magnetic field that magnetizes the reference layer 4. On the other hand, the reproduction system includes a pair of photodetectors 14 and a
It consists of a pair of analyzers 12 and a polarizing beam splitter 10b.
レーザ光源13は、記録消去/読出用レーザビーム7の
出力を3段階に制御できるようにしである。図中、15
は記録媒体1に書込まれたビットを示す。The laser light source 13 is configured so that the output of the recording/erasing/reading laser beam 7 can be controlled in three stages. In the figure, 15
indicates bits written on recording medium 1.
記録媒体1は、第8図を参照して、透光性の基板2と、
記録層3と、参照層4とから構成される。Referring to FIG. 8, the recording medium 1 includes a transparent substrate 2,
It is composed of a recording layer 3 and a reference layer 4.
記録層3と参照層4は希土類−遷移金属合金で形成され
、希土類金属および遷移金属はそれぞれ副格子を形成し
ている。各副格子の磁性を担う磁気モーメントの総和と
して副格子磁化が与えられ、副格子磁化の総和として磁
化が与えられる。また、フェリ磁性体の場合、希土類金
属副格子磁化と遷移金属副格子磁化の方向は反対向きに
なっていて、磁化方向とたとえば遷移金属副格子磁化の
方向の関係は、磁性層の組成と温度により変化するが、
各磁性層の間には磁性層間でたとえば遷移金属間の互い
の副格子磁化を揃えるように働く交換結合力が働いてい
る。この従来例では、室温にて、遷移金属副格子磁化が
希土類金属副格子磁化より優勢で、室温以上では、磁化
とたとえば遷移金属副格子磁化の方向が一致する磁性体
が用いられている。The recording layer 3 and the reference layer 4 are formed of a rare earth-transition metal alloy, and the rare earth metal and the transition metal each form a sublattice. Sublattice magnetization is given as the sum of the magnetic moments responsible for the magnetism of each sublattice, and magnetization is given as the sum of the sublattice magnetizations. In addition, in the case of ferrimagnetic materials, the directions of rare earth metal sublattice magnetization and transition metal sublattice magnetization are opposite, and the relationship between the magnetization direction and the direction of transition metal sublattice magnetization, for example, depends on the composition of the magnetic layer and the temperature. Although it varies depending on
Between each magnetic layer, an exchange coupling force acts to align the sublattice magnetizations of transition metals, for example, between the magnetic layers. In this conventional example, a magnetic material is used in which the transition metal sublattice magnetization is more dominant than the rare earth metal sublattice magnetization at room temperature, and the direction of the magnetization and, for example, the transition metal sublattice magnetization coincide with each other above room temperature.
記録層3は情報を保持するための層で、参照層4はダイ
レクトオーバライドを可能にするための記録担体の役割
を持たない補助層である。第1外部磁石5は記録消去時
のレーザビーム強度でのみ磁性層の磁化方向に変化を与
える磁界を発生する。The recording layer 3 is a layer for holding information, and the reference layer 4 is an auxiliary layer that does not have the role of a record carrier to enable direct override. The first external magnet 5 generates a magnetic field that changes the magnetization direction of the magnetic layer only with the laser beam intensity during recording and erasing.
第2外部磁石6は、記録層3の磁化方向(副格子磁化方
向)にかかわらず、参照層4の磁化方向を一様に磁化す
る磁界を発生する。このとき記録層3の磁化方向(副格
子磁化方向)は、外部磁石および参照層4から働く交換
力によって影響を受けず、そのままの方向を保持する。The second external magnet 6 generates a magnetic field that uniformly magnetizes the reference layer 4 in the magnetization direction regardless of the magnetization direction (sublattice magnetization direction) of the recording layer 3 . At this time, the magnetization direction (sublattice magnetization direction) of the recording layer 3 is not affected by the exchange force acting from the external magnet and the reference layer 4, and maintains the same direction.
次に動作について説明する。Next, the operation will be explained.
レーザビーム7の出力を上げて、記録層3の各副格子磁
化方向が交換力により、参照層4の副格子磁化方向に揃
い、参照層4の副格子磁化が第1外部磁石5により反転
しないとき、参照層4の副格子磁化方向が記録層3に転
写され、記録層3の副格子磁化方向は上向きになる。参
照層4の磁化が第1外部磁石5からの磁界により磁化反
転を起こす温度(磁化反転温度)に達するときは、第1
外部磁石5により参照層4の磁化方向は下向きになり、
さらに参照層4の磁化方向が記録層3に転写され、記録
層3の磁化方向は下向き(副格子磁化も下向き)になる
。このようにレーザビーム7の出力を変えるだけで、記
録層3の磁化方向(副格子磁化方向)を変えられ、直接
オーバライドが可能になる。しかし、第9図を参照して
、記録消去後には、第2外部磁石6により参照層4の磁
化方向はすべて上向きに磁化されるため、参照層4の磁
化反転温度を越えるレーザビーム7の出力で記録を行な
った部分では、磁性層間に、磁壁Aが生じた状態になる
。By increasing the output of the laser beam 7, each sublattice magnetization direction of the recording layer 3 is aligned with the sublattice magnetization direction of the reference layer 4 due to the exchange force, and the sublattice magnetization of the reference layer 4 is not reversed by the first external magnet 5. At this time, the sublattice magnetization direction of the reference layer 4 is transferred to the recording layer 3, and the sublattice magnetization direction of the recording layer 3 becomes upward. When the magnetization of the reference layer 4 reaches a temperature at which magnetization reversal occurs due to the magnetic field from the first external magnet 5 (magnetization reversal temperature), the first
The magnetization direction of the reference layer 4 is directed downward by the external magnet 5,
Further, the magnetization direction of the reference layer 4 is transferred to the recording layer 3, and the magnetization direction of the recording layer 3 becomes downward (the sublattice magnetization also becomes downward). In this way, by simply changing the output of the laser beam 7, the magnetization direction (sublattice magnetization direction) of the recording layer 3 can be changed, making direct override possible. However, referring to FIG. 9, after erasure, the reference layer 4 is magnetized upward by the second external magnet 6, so the output of the laser beam 7 exceeds the magnetization reversal temperature of the reference layer 4. In the portion where recording was performed, a domain wall A is generated between the magnetic layers.
[発明が解決しようとする課題]
従来の光磁気記録装置は以上のように構成されているの
で、第9図を参照して、記録消去後に各磁性層間に磁壁
Aが生じて準安定状態にあり、高温にさらされると記録
担体の記録層3の磁化方向は参照層4に影響され、記録
が劣化・消失し、記録媒体としての信頼性を欠くなどの
問題があった。[Problems to be Solved by the Invention] Since the conventional magneto-optical recording device is configured as described above, referring to FIG. However, when exposed to high temperatures, the magnetization direction of the recording layer 3 of the record carrier is influenced by the reference layer 4, causing problems such as deterioration and disappearance of recording, and a lack of reliability as a recording medium.
この発明は上記のような問題点を解決するためになされ
たもので、記録を安定に保持し、高信頼性を有する光磁
気記録媒体を与える光磁気記録装置を提供することを目
的とする。The present invention has been made to solve the above-mentioned problems, and an object of the present invention is to provide a magneto-optical recording device that stably retains recording and provides a highly reliable magneto-optical recording medium.
[課題を解決するための手段]
この発明は、記録層と参照層とを含む多層の磁性層に局
部的に光を照射することにより、上記記録層に対して情
報の記録・消去を行なう光磁気記録装置に係るものであ
る。当該光磁気記録装置は情報記録・消去時の光強度で
のみ、上記磁性層の磁化方向に変化を与える磁界を発生
する第1磁界発生手段と・、上記記録層の磁化方向にか
かわらず上記参照層の磁化方向が一様になるように、該
参照層を磁化する磁界を発生する第2磁界発生手段と、
を備えている。さらに、当該光磁気記録装置は、上記問
題点を解決するために、上記第2磁界発生手段と逆方向
の磁界を発生し、情報の記録・消去後に、上記記録層と
上記参照層との間に生じた磁壁を消失させる第3磁界発
生手段を備えている。[Means for Solving the Problems] The present invention provides a method of recording and erasing information on the recording layer by locally irradiating light onto a multilayer magnetic layer including a recording layer and a reference layer. This relates to a magnetic recording device. The magneto-optical recording device includes a first magnetic field generating means that generates a magnetic field that changes the magnetization direction of the magnetic layer only at the light intensity during information recording/erasing, and a first magnetic field generating means that generates a magnetic field that changes the magnetization direction of the above-mentioned magnetic layer regardless of the magnetization direction of the above-mentioned recording layer. a second magnetic field generating means for generating a magnetic field that magnetizes the reference layer so that the magnetization direction of the layer is uniform;
It is equipped with Furthermore, in order to solve the above problem, the magneto-optical recording device generates a magnetic field in the opposite direction to the second magnetic field generating means, and after recording/erasing information, the magnetic field is generated between the recording layer and the reference layer. The magnetic field generating means is provided with a third magnetic field generating means for eliminating the domain wall generated in the magnetic field.
[作用コ
この発明に係る光磁気記録装置は、情報の記録・消去後
に記録層と参照層との間に生じた磁壁を消失させる第3
磁界発生手段を備えているので、光磁気記録媒体の磁性
層間に残存する磁壁を消失させることができる。[Function] The magneto-optical recording device according to the present invention includes a third layer that eliminates the domain wall generated between the recording layer and the reference layer after recording and erasing information.
Since the magnetic field generating means is provided, it is possible to eliminate domain walls remaining between the magnetic layers of the magneto-optical recording medium.
[実施例コ
第1図は、この発明の一実施例に係る光磁気記録装置の
記B峙の概略構成図を示しており、第2図はその要部の
断面図である。第3図は、上記光磁気記録装置の記録終
了■、1?の概略構成図を示しており、第4図はその要
部の断面図である。Embodiment FIG. 1 shows a schematic diagram of a magneto-optical recording apparatus according to an embodiment of the present invention, and FIG. 2 is a sectional view of the main parts thereof. FIG. 3 shows the completion of recording of the above-mentioned magneto-optical recording device (■, 1?). FIG. 4 is a sectional view of the main parts thereof.
第1図〜第4図に示す実施例は、以下の点を除いて、第
7図および第8図に示す従来例と同様であり、相当する
部分には同一の参照番号を付し、その説明を省略する。The embodiment shown in FIGS. 1 to 4 is similar to the conventional example shown in FIGS. 7 and 8 except for the following points, and corresponding parts are given the same reference numerals. The explanation will be omitted.
第1図〜第4図に示す実施例が、第7図および第8図に
示す従来例と異なる点は、第2外部磁石6と逆方向の磁
界を発生し、情報の記録・消去後に、記録層3と参照層
4との間に生じた磁壁Aを消失させる第3外部磁石8を
備えている点である。The embodiment shown in FIGS. 1 to 4 differs from the conventional example shown in FIGS. 7 and 8 in that a magnetic field is generated in the opposite direction to that of the second external magnet 6, and after recording/erasing information, The third external magnet 8 is provided to eliminate the domain wall A generated between the recording layer 3 and the reference layer 4.
記録層3および参照層4は、室温にて、遷移金属副格子
磁化が希土類金属副格子磁化より優勢で、室温以上では
、磁化とたとえば遷移金属副格子磁化の方向が一致する
磁性体を用いている。このとき、各磁性層が交換力で結
合しているので、参照層4のヒステリシス曲線は、記録
層の磁化が上向き(遷移金属副格子磁化は上向き)のと
きは、第5図(a)のように下向き磁界方向にシフトし
たものになり、記録層3の磁化が下向き(遷移金属副格
子磁化は下向き)のときは、第5図(b、)のように上
向き磁界方向にシフトしたものになる。The recording layer 3 and the reference layer 4 are made of a magnetic material in which the transition metal sublattice magnetization is more dominant than the rare earth metal sublattice magnetization at room temperature, and the direction of the magnetization and, for example, the transition metal sublattice magnetization match at room temperature or higher. There is. At this time, since each magnetic layer is coupled by exchange force, the hysteresis curve of the reference layer 4 is as shown in FIG. 5(a) when the magnetization of the recording layer is upward (transition metal sublattice magnetization is upward). When the magnetization of the recording layer 3 is downward (transition metal sublattice magnetization is downward), the magnetic field is shifted upward in the direction of the magnetic field as shown in Figure 5(b). Become.
この非対称なヒステリシス曲線において、絶対値が大き
い反転磁界をH2+、小さい反転磁界をH2−とする。In this asymmetric hysteresis curve, a switching magnetic field with a large absolute value is defined as H2+, and a switching magnetic field with a small absolute value is defined as H2-.
第3外部磁石8は、参照層4の室温での反転磁界H2−
+ ”2+の中間の大きさで、第2外部磁石6と逆方向
の磁界を発生し、通常の記録動作のときは、第1図およ
び第2図を参照して、記録媒体1から離されている。記
録媒体1を記録装置から取出すときに、第3図および第
4図のように、外部磁石6が記録媒体1から離された後
に、記録媒体1が1周回転する以上の時間だけ、磁界が
記録媒体1にかかるように、第3外部磁石8は記録媒体
1に向かって移動する。The third external magnet 8 has a reversal magnetic field H2- of the reference layer 4 at room temperature.
It generates a magnetic field in the opposite direction to the second external magnet 6, with a magnitude intermediate between ``2+'', and is separated from the recording medium 1 during normal recording operation, as shown in FIGS. 1 and 2. When taking out the recording medium 1 from the recording apparatus, as shown in FIGS. 3 and 4, after the external magnet 6 is separated from the recording medium 1, the rotation time is longer than the time for the recording medium 1 to rotate once. , the third external magnet 8 moves toward the recording medium 1 such that a magnetic field is applied to the recording medium 1 .
次に動作について説明する。Next, the operation will be explained.
記録媒体1を記録装置から取出すときに、第3外部磁石
8が記録媒体1に作用したとき、第2図中A部のように
記録・消去後、磁性層間に磁壁が残存している領域は、
反転磁界H2−、H2+の中間で、第2外部磁石6と逆
方向の磁界をかけることにより、記録層3は変化せず、
゛参照層4の磁化が反転し、磁性層間の磁壁が消失する
(第4図のC部分参照)。B部のように磁壁が残存しな
い領域は、第3外部磁石8により、磁性層の磁化方向は
変化しない。When the third external magnet 8 acts on the recording medium 1 when the recording medium 1 is taken out from the recording device, the area where domain walls remain between the magnetic layers after recording and erasing, as shown in part A in FIG. ,
By applying a magnetic field in the opposite direction to the second external magnet 6 between the reversal magnetic fields H2- and H2+, the recording layer 3 remains unchanged;
``The magnetization of the reference layer 4 is reversed, and the domain wall between the magnetic layers disappears (see section C in FIG. 4). In a region where no domain wall remains, such as part B, the magnetization direction of the magnetic layer does not change due to the third external magnet 8.
このように構成することにより、記録消去後に磁性層間
に磁壁が残存しても、第3外部磁石8により、参照層4
は、記録層3の磁化方向に反転するので、第3外部磁石
8通過後は、磁性層間に磁壁が残存しなくなる。その結
果、記録媒体を保存するときに、各磁性層間に磁壁がな
く、磁気的安定状態にあるので、高温に曝されても、記
録は安定で、記録媒体としての信頼性が向上する。With this configuration, even if a domain wall remains between the magnetic layers after recording and erasing, the third external magnet 8 can move the reference layer 4
is reversed in the magnetization direction of the recording layer 3, so that no domain wall remains between the magnetic layers after passing through the third external magnet 8. As a result, when the recording medium is stored, there are no domain walls between the magnetic layers and the recording medium is in a magnetically stable state, so even if exposed to high temperatures, recording is stable and reliability as a recording medium is improved.
第6図に、予め情報を記録した記録媒体を磁界中で高温
下に曝したときの誤り率を示す。従来の光磁気記録装置
で記録した記録媒体では、磁界6006e、温度60℃
あるいは零磁界・温度80℃で記録の劣化が起こったが
、本実施例の光磁気記録装置で記録した記録媒体では、
磁界600″C3e、温度100℃でも記録信号に変化
は現われなかった。FIG. 6 shows the error rate when a recording medium on which information has been previously recorded is exposed to high temperature in a magnetic field. A recording medium recorded with a conventional magneto-optical recording device has a magnetic field of 6006e and a temperature of 60°C.
Alternatively, recording deterioration occurred at zero magnetic field and temperature of 80°C, but in the recording medium recorded by the magneto-optical recording device of this example,
Even at a magnetic field of 600″C3e and a temperature of 100°C, no change appeared in the recorded signal.
なお、上記実施例では、第1外部磁石5と第3外部磁石
8とを別個のものとして構成した。しかし、第1外部磁
石5を電磁石にして、この電磁石で参照層4の室温での
反転磁界H2−1H2+の中間の大きさで、第2外部磁
石6と逆方向の磁界を、記録媒体1を記録装置から取出
すとき、すなわち、第2外部磁石6が記録媒体1から離
された後に、記録媒体1が1周回転する以上の時間だけ
、記録媒体にかかるようにしてもよい。この場合、光磁
気記録媒体1は、H2” #4 k’c5 e、 H2
#0.8に6eのものであり、上記磁界は1にづe〜2
k ’Cj e程度印加する必要がある。第1外部磁
石5は消去・記録時に200〜6006e程度の磁界を
発生するものであり、このような現在用いられている電
磁石でも11c ’Cj e以上の磁界を、記録媒体1
が1周回転する時間の数10ミリ秒は十分発生させるこ
とができる。このような装置を用いても、上記実施例と
同様に、苛酷な保17環境下でも、記録情報の消失もな
く、高い信頼性を有する光磁気記録媒体が得られる。こ
の場合、第3外部磁石8を別個独立に設置する必要がな
いので、装置の煩雑化が避けられるという効果も奏する
。In the above embodiment, the first external magnet 5 and the third external magnet 8 are configured as separate magnets. However, by using an electromagnet as the first external magnet 5, this electromagnet applies a magnetic field to the recording medium 1 with a magnitude intermediate between the reversal magnetic field H2-1H2+ of the reference layer 4 at room temperature and in the opposite direction to the second external magnet 6. When taking out the recording medium from the recording apparatus, that is, after the second external magnet 6 is separated from the recording medium 1, the recording medium may be subjected to a time longer than that for the recording medium 1 to rotate once. In this case, the magneto-optical recording medium 1 is H2''#4k'c5 e, H2
#0.8 to 6e, and the above magnetic field is 1 to 2
It is necessary to apply approximately k'Cj e. The first external magnet 5 generates a magnetic field of about 200 to 6006 e during erasing and recording, and even such electromagnets currently used cannot generate a magnetic field of more than 11 c'Cj e on the recording medium 1.
It is sufficient to generate several tens of milliseconds, which is the time required for one rotation of the rotor. Even when such an apparatus is used, a highly reliable magneto-optical recording medium can be obtained without loss of recorded information even under harsh storage environments, as in the above embodiments. In this case, there is no need to separately and independently install the third external magnet 8, so there is also the effect that the device can be prevented from becoming complicated.
また、第3外部磁石8は、第1外部磁石5または第2外
部磁石6を機械的に極性および媒体面での磁界強度を変
えるようにして兼用してもよく、記録再生装置以外で備
えてもよい。さらに、記録媒体に薄膜磁石等を直接設け
てもよい。また、記録媒体は、tIt板ディスクを貼り
合わせた両面媒体であってもよい。Further, the third external magnet 8 may also be used as the first external magnet 5 or the second external magnet 6 by mechanically changing the polarity and magnetic field strength on the medium surface, and may be provided in a device other than the recording/reproducing device. Good too. Furthermore, a thin film magnet or the like may be provided directly on the recording medium. Furthermore, the recording medium may be a double-sided medium in which TIt board disks are bonded together.
[発明の効果]
以上説明したとおり、この発明によれば、情報の記録・
消去後に記録層と参照層との間に生じた磁壁を消失させ
る第3磁界発生手段を備えているので、光磁気記録媒体
の磁性層間に残7jする磁壁を消失させることができる
。その結果、長期保存に耐えられる高信頼性を有する光
磁気記録媒体が得られるという効果を奏する。[Effect of the invention] As explained above, according to this invention, information recording and
Since the third magnetic field generating means is provided to eliminate the domain wall generated between the recording layer and the reference layer after erasing, the domain wall remaining between the magnetic layers of the magneto-optical recording medium can be eliminated. As a result, it is possible to obtain a highly reliable magneto-optical recording medium that can withstand long-term storage.
第1図は、この発明の一実施例に係る光磁気記録装置の
、記録時の概略構成図を示しており、第2図はその要部
の断面図である。第3図は、この発明の一実施例に係る
光磁気記録装置の、記録終了間の概略構成図を示してお
り、第4図はその要部の断面図である。第5図は、参照
層のヒステリシス特性図であり、(a)は記録層の磁化
が上向きのときの図であり、(b)は記録層の磁化が下
向きのときの図である。第6図は、従来例と本実施例で
得た記録媒体の、投入温度と磁界に対する誤り率特性図
である。第7図は、従来の光磁気記録装置の構成図であ
り、第8図はその要部の断面図である。第9図は、従来
の光磁気記録装置で作成した光磁気記録媒体の、記録消
去後の状態を示す断面図である。
図において、1は記録媒体、3は記録層、4は参照層、
5は第1外部は石、6は第2外部磁石、7はレーザビー
ム、8は第3外部磁石、Aは磁壁である。
なお、各図中、同一符号は同一または相当部分を示す。FIG. 1 shows a schematic configuration diagram of a magneto-optical recording device according to an embodiment of the present invention during recording, and FIG. 2 is a sectional view of the main parts thereof. FIG. 3 shows a schematic configuration diagram of a magneto-optical recording device according to an embodiment of the present invention during the end of recording, and FIG. 4 is a sectional view of the main part thereof. FIG. 5 is a hysteresis characteristic diagram of the reference layer, in which (a) is a diagram when the magnetization of the recording layer is upward, and (b) is a diagram when the magnetization of the recording layer is downward. FIG. 6 is a graph showing the error rate characteristics of the recording media obtained in the conventional example and the present example with respect to input temperature and magnetic field. FIG. 7 is a block diagram of a conventional magneto-optical recording device, and FIG. 8 is a sectional view of its main parts. FIG. 9 is a cross-sectional view showing the state of a magneto-optical recording medium produced by a conventional magneto-optical recording device after recording and erasure. In the figure, 1 is a recording medium, 3 is a recording layer, 4 is a reference layer,
5 is a first external stone, 6 is a second external magnet, 7 is a laser beam, 8 is a third external magnet, and A is a domain wall. In each figure, the same reference numerals indicate the same or corresponding parts.
Claims (1)
照射することにより、前記記録層に対して情報の記録・
消去を行なう光磁気記録装置であって、 情報の記録・消去時の光強度でのみ、前記磁性層の磁化
方向に変化を与える磁界を発生する第1磁界発生手段と
、 前記記録層の磁化方向にかかわらず、前記参照層の磁化
方向が一様になるように、該参照層を磁化する磁界を発
生する第2磁界発生手段と、前記第2磁界発生手段と逆
方向の磁界を発生し、情報の記録・消去後に、前記記録
層と前記参照層との間に生じた磁壁を消失させる第3磁
界発生手段と、 を備えた光磁気記録装置。[Claims] By locally irradiating light onto a multilayer magnetic layer including a recording layer and a reference layer, information can be recorded and recorded on the recording layer.
A magneto-optical recording device that performs erasing, comprising: a first magnetic field generating means that generates a magnetic field that changes the magnetization direction of the magnetic layer only with the light intensity when recording and erasing information; and the magnetization direction of the recording layer. Regardless, a second magnetic field generation means for generating a magnetic field that magnetizes the reference layer so that the magnetization direction of the reference layer is uniform, and a magnetic field generated in the opposite direction to the second magnetic field generation means, A magneto-optical recording device comprising: third magnetic field generating means for eliminating a domain wall generated between the recording layer and the reference layer after recording/erasing information.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP22342389A JPH0386954A (en) | 1989-08-30 | 1989-08-30 | Magneto-optical recorder |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP22342389A JPH0386954A (en) | 1989-08-30 | 1989-08-30 | Magneto-optical recorder |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0386954A true JPH0386954A (en) | 1991-04-11 |
Family
ID=16797911
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP22342389A Pending JPH0386954A (en) | 1989-08-30 | 1989-08-30 | Magneto-optical recorder |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0386954A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0472377A2 (en) * | 1990-08-17 | 1992-02-26 | Seiko Epson Corporation | Magneto-optical method and apparatus for recording/reproducing data |
KR100868104B1 (en) * | 2008-02-18 | 2008-11-10 | 부산교통공사 | Device for dectecting and indicating the exchanging time of air filter in a high-tension thyristor converter |
-
1989
- 1989-08-30 JP JP22342389A patent/JPH0386954A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0472377A2 (en) * | 1990-08-17 | 1992-02-26 | Seiko Epson Corporation | Magneto-optical method and apparatus for recording/reproducing data |
US5325345A (en) * | 1990-08-17 | 1994-06-28 | Seiko Epson Corporation | Magneto-optical method and apparatus for recording/reproducing data |
KR100868104B1 (en) * | 2008-02-18 | 2008-11-10 | 부산교통공사 | Device for dectecting and indicating the exchanging time of air filter in a high-tension thyristor converter |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JP2938284B2 (en) | Magneto-optical recording medium and recording / reproducing method using the same | |
US4771347A (en) | Magneto-optical recording system | |
EP0225141B1 (en) | Magneto-optical recording media | |
JPS60236137A (en) | Simultaneously erasing-recording type photomagnetic recording system and recording device and medium used for this system | |
JPH0785516A (en) | Magneto-optical disk and magneto-optical disk reproducing device | |
JPH087350A (en) | Magneto-optical recording medium and magneto-optical recording and reproducing apparatus | |
US5309427A (en) | Overwrite-capable magnetooptical recording medium allowing enlarged margin of high level beam intensity | |
US5164926A (en) | Over-write capable magnetooptical recording medium with four magnetic layered structure dispensing with external initializing field | |
KR930008148B1 (en) | Optical magnetic recording device | |
JP3538727B2 (en) | Magneto-optical recording medium | |
US5206844A (en) | Magnetooptic recording medium cartridge for two-sided overwriting | |
US5353171A (en) | Magneto-optical recording apparatus | |
JPH0386954A (en) | Magneto-optical recorder | |
JPH09212927A (en) | Magneto-optic recording medium and method for recording and reproducing by using the medium | |
JPH11353725A (en) | Magneto-optical recording medium and magneto-optical recorder | |
JPS5841451A (en) | Vertical magnetic recording medium | |
JPH04255941A (en) | Magneto-optical recording medium | |
JPS61214258A (en) | Write and reproducing integrated magnetic head | |
JPS59168954A (en) | Optical magnetic recording medium | |
JPH11185312A (en) | Magneto-optical recording medium | |
JPS63304448A (en) | Magneto-optical recording medium | |
JPH1125529A (en) | Information recording medium and reproducing method therefor | |
JP3542155B2 (en) | Magneto-optical recording medium and magneto-optical recording / reproducing device | |
JP2002298325A (en) | Magnetic recording medium and magnetic recorder having the same | |
JPS5819753A (en) | Vertical magnetic recording medium and reproducing method of vertical magnetizing signal using said recording medium |