JPH087361A - Magneto-optical recording medium, its manufacturing method and apparatus - Google Patents

Magneto-optical recording medium, its manufacturing method and apparatus

Info

Publication number
JPH087361A
JPH087361A JP13986094A JP13986094A JPH087361A JP H087361 A JPH087361 A JP H087361A JP 13986094 A JP13986094 A JP 13986094A JP 13986094 A JP13986094 A JP 13986094A JP H087361 A JPH087361 A JP H087361A
Authority
JP
Japan
Prior art keywords
magneto
recording medium
magnetic
optical recording
film
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
JP13986094A
Other languages
Japanese (ja)
Inventor
Jiichi Miyamoto
治一 宮本
Takeshi Maeda
武志 前田
Hiroyuki Awano
博之 粟野
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.)
Hitachi Ltd
Maxell Holdings Ltd
Original Assignee
Hitachi Ltd
Hitachi Maxell 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 Hitachi Ltd, Hitachi Maxell Ltd filed Critical Hitachi Ltd
Priority to JP13986094A priority Critical patent/JPH087361A/en
Publication of JPH087361A publication Critical patent/JPH087361A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To form magnetic domains whose sizes are smaller than a light spot diameter and facilitate high density recording by a method wherein regions whose magnetic characteristics, thermal characteristics and/or optical characteristics are different from those of the other regions are provided in the magnetic film of a magneto-optical recording medium. CONSTITUTION:At least a magnetic film 2 is provided on the disc-type substrate 1 of a magneto-optical recording medium. Regions 3 whose coercive forces are low are provided on the magnetic film 2. The regions 3 may be formed on the disc in various patterns. If they are formed in spiral patterns, they can be also used as tracks and accessed easily. At that time, the width of each region 3 is 0.4mum and the distance between the regions 3 is 0.3mum. The region whose coercive force is low has a higher sensitivity than the other region. Therefore, if a light beam having a proper intensity is applied to elevate a medium temperature, recording magnetic domains can be formed in the regions 3 only in the medium. With this constitution, the width of each magnetic domain is limited to the width (0.4mum) of each region 3 regardless of the wavelength of a laser beam, so that high density recording can be realized.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、光スポットよりも小さ
な磁区を安定に形成できる高密度光磁気記録媒体及びそ
の製造方法、それを用いた装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a high density magneto-optical recording medium capable of stably forming a magnetic domain smaller than a light spot, a method of manufacturing the same, and an apparatus using the same.

【0002】[0002]

【従来の技術】従来の光磁気記録媒体の断面構造は、例
えば、図2に示したような構造であった。トラッキング
のための案内溝を設けたガラス等の透明基板1上に、窒
化珪素等の誘電体層31を約90nm,TbFeCo等
の磁性層32を約100nm,窒化珪素等の保護層33
を約200nm順に積層して記録膜4としている。誘電
体層31は基板1側から入射したレーザ光をその内部で
多重反射させ、磁性層32で生じる偏光面の回転(カー
回転)を増大させる働きがある。保護層33は磁性層3
2を酸化等の腐食から保護する働きがある。
2. Description of the Related Art The cross-sectional structure of a conventional magneto-optical recording medium is, for example, the structure shown in FIG. On a transparent substrate 1 such as glass provided with a guide groove for tracking, a dielectric layer 31 of silicon nitride or the like is about 90 nm, a magnetic layer 32 of TbFeCo or the like is about 100 nm, and a protective layer 33 of silicon nitride or the like.
To form a recording film 4. The dielectric layer 31 has a function of multiply reflecting the laser light incident from the substrate 1 side therein, and increasing the rotation (Kerr rotation) of the polarization plane generated in the magnetic layer 32. The protective layer 33 is the magnetic layer 3
It has a function of protecting 2 from corrosion such as oxidation.

【0003】このような記録媒体の記録再生の原理につ
いて説明する。磁性層32の保磁力は、室温では大き
く、キュリー温度付近で小さくなる。そこで記録媒体に
記録磁界を印加しながら、レーザ光を収束して照射し記
録媒体の温度を上昇させると、記録温度に達したときに
保磁力Hc は記録磁界と等しくなるため、記録温度に達
した部分の磁性層32の磁化は記録磁界の方向に向き記
録磁区が形成される。再生時には、記録磁区に収束光を
照射し、その反射光の偏光面の回転を検出することによ
り記録磁区の有無,形状や大きさを検出する。
The principle of recording / reproducing on such a recording medium will be described. The coercive force of the magnetic layer 32 is large at room temperature and small near the Curie temperature. Therefore, when a recording magnetic field is applied to the recording medium and the laser light is converged and irradiated to raise the temperature of the recording medium, the coercive force Hc becomes equal to the recording magnetic field when the recording temperature is reached, so that the recording temperature is reached. The magnetization of the magnetic layer 32 in this portion is oriented in the direction of the recording magnetic field to form a recording magnetic domain. At the time of reproduction, the recording magnetic domain is irradiated with convergent light, and the rotation of the plane of polarization of the reflected light is detected to detect the presence, shape, and size of the recording magnetic domain.

【0004】この方法については、例えば,特開昭59−
210543号公報に記載されている。
This method is described, for example, in JP-A-59-
It is described in Japanese Patent Publication No. 210543.

【0005】[0005]

【発明が解決しようとする課題】しかし、従来例で光の
強度を制御することによって小さな磁区を記録しようと
すると、記録温度に達した部分の大きさを制御するのが
困難で、実質的には光スポット径の1/2よりも小さな
磁区は記録できないという問題があった。このため、高
密度な記録を行うのが困難であった。
However, when attempting to record a small magnetic domain by controlling the light intensity in the conventional example, it is difficult to control the size of the portion reaching the recording temperature, and it is substantially Had a problem that it was not possible to record magnetic domains smaller than 1/2 of the light spot diameter. Therefore, it is difficult to perform high density recording.

【0006】本発明の第1の目的は、光スポット径の1
/2よりも小さな磁区を形成して高密度記録を行うこと
の可能な光磁気記録媒体を提供することにある。
A first object of the present invention is to set the light spot diameter to 1
Another object of the present invention is to provide a magneto-optical recording medium capable of performing high density recording by forming magnetic domains smaller than / 2.

【0007】本発明の第2の目的は光スポット径の1/
2よりも小さな磁区を形成して高密度記録を行うことの
可能な光磁気記録媒体の製造方法を提供することにあ
る。
The second object of the present invention is to reduce the light spot diameter to 1 /
Another object of the present invention is to provide a method of manufacturing a magneto-optical recording medium capable of forming magnetic domains smaller than 2 and performing high density recording.

【0008】本発明の第3の目的は、光スポット径の1
/2よりも小さな磁区を形成して高密度記録を行うこと
の可能な光磁気記録装置を提供することにある。
A third object of the present invention is to set the light spot diameter to 1
It is an object of the present invention to provide a magneto-optical recording device capable of performing high density recording by forming magnetic domains smaller than / 2.

【0009】[0009]

【課題を解決するための手段】本発明では第1の目的を
解決するために次の手段を用いた。
The present invention uses the following means in order to solve the first object.

【0010】(1)少なくとも一層の磁性膜からなる光
磁気記録媒体で、前記光磁気記録媒体に一定磁界を印加
しながら温度を徐々に上げたとき、磁性膜内の一部の領
域にのみ反転磁区ができその他の領域にはできないよう
な温度が存在することを特徴とする光磁気記録媒体。
(1) In a magneto-optical recording medium composed of at least one magnetic film, when the temperature is gradually raised while applying a constant magnetic field to the magneto-optical recording medium, only a part of the magnetic film is inverted. A magneto-optical recording medium characterized in that there is a temperature such that a magnetic domain is formed and no other region is formed.

【0011】(2)少なくとも一層の磁性膜からなる光
磁気記録媒体で、前記光磁気記録媒体に一定温度で印加
する磁界を徐々に上げたとき、磁性膜内の一部の領域に
のみ反転磁区ができその他の領域にはできないような磁
界が存在することを特徴とする光磁気記録媒体。
(2) In a magneto-optical recording medium including at least one magnetic film, when the magnetic field applied to the magneto-optical recording medium at a constant temperature is gradually increased, the reversed magnetic domain is formed only in a part of the magnetic film. A magneto-optical recording medium characterized by the presence of a magnetic field that can be generated and cannot be generated in other areas.

【0012】(3)少なくとも一層の磁性膜からなる光
磁気記録媒体で、前記磁性膜内に記録感度の高い一部の
領域が存在することを特徴とする光磁気記録媒体。
(3) A magneto-optical recording medium comprising at least one magnetic film, wherein a part of the magnetic film having high recording sensitivity is present.

【0013】(4)少なくとも一層の磁性膜からなる光
磁気記録媒体で、前記磁性膜内に保磁力の低い一部の領
域が存在することを特徴とする光磁気記録媒体。
(4) A magneto-optical recording medium comprising at least one magnetic film, wherein a part of the region having a low coercive force is present in the magnetic film.

【0014】(5)前記の一部の領域の幅または長さの
少なくともいずれかが情報記録単位の幅または長さのい
ずれかよりも小さいことを特徴とする光磁気記録媒体。
(5) A magneto-optical recording medium characterized in that at least one of the width and the length of the partial area is smaller than the width or the length of the information recording unit.

【0015】これにより、温度上昇部のうち、上記の、
磁気特性,熱特性及び光学特性の少なくとも一つが他の
部分と異なる領域にのみ微小な記録磁区を形成すること
が容易になる。すなわち高密度記録が可能になる。
As a result, among the temperature rising parts,
It becomes easy to form a minute recording magnetic domain only in a region where at least one of magnetic property, thermal property and optical property is different from other parts. That is, high density recording becomes possible.

【0016】また、記録磁区の幅または長さを正確に制
御して記録することが容易になる。 (6)前記光磁気記録媒体が、前記磁性膜以外に融点が
200℃以上500℃以下の膜を少なくとも有すること
を特徴とする光磁気記録媒体。
Further, it becomes easy to record by controlling the width or length of the recording magnetic domain accurately. (6) A magneto-optical recording medium, wherein the magneto-optical recording medium has at least a film having a melting point of 200 ° C. or more and 500 ° C. or less in addition to the magnetic film.

【0017】(7)前記光磁気記録媒体が、前記磁性膜
以外に融点が300℃以上400℃以下の膜を少なくと
も有することを特徴とする光磁気記録媒体。
(7) A magneto-optical recording medium characterized in that the magneto-optical recording medium has at least a film having a melting point of 300 ° C. or higher and 400 ° C. or lower in addition to the magnetic film.

【0018】これにより、熱特性及び光学特性の少なく
とも一つが異なる領域を持った媒体を製造することが容
易になる。
This makes it easy to manufacture a medium having a region in which at least one of thermal characteristics and optical characteristics is different.

【0019】本発明では上記第2の目的を解決するため
に次の手段を用いた。
In the present invention, the following means are used in order to solve the second object.

【0020】(8)前記一部の領域を形成するにあた
り、記録媒体上に通常の記録時の光スポット径の0.8
倍以下の光スポット径の光を照射して行った。
(8) In forming the partial area, the diameter of the light spot at the time of normal recording is 0.8 on the recording medium.
It was performed by irradiating light with a light spot diameter not more than twice.

【0021】これにより、前記一部の領域を微小にする
のが容易になる。すなわち、高密度記録するのが容易に
なる。
As a result, it becomes easy to make the part of the area minute. That is, high density recording becomes easy.

【0022】(9)融点が200℃以上500℃以下の
膜を設けた後、光を照射して膜を融かし穴を開け、その
後、磁性膜を設ける光磁気記録媒体の製造方法。
(9) A method of manufacturing a magneto-optical recording medium in which a film having a melting point of 200 ° C. or more and 500 ° C. or less is provided, light is irradiated to melt the film, holes are formed, and then a magnetic film is provided.

【0023】これにより、磁性膜を熱劣化させずに、前
記の一部の領域を微小にするのが容易になる。
As a result, it becomes easy to miniaturize the above-mentioned part of the region without thermally deteriorating the magnetic film.

【0024】本発明では上記第3の目的を解決するため
に次の手段を用いた。
In the present invention, the following means are used to solve the third object.

【0025】(10)少なくとも前記磁性膜の温度を上昇
させるための光を照射する光ヘッドと、前記磁性膜上に
磁界を印加するための磁界印加手段と、所望の記録磁区
を形成するために前記光の強度をあるいは前記磁界の強
度あるいは向きを変化させるための変調手段と、前記光
を記録媒体上の所望の位置に照射するための自動位置制
御手段を有し、前記光磁気記録媒体を用いる光磁気記録
装置で、前記一部の領域とその他の部分との境界部に磁
壁が位置するよう記録磁区を形成するための記録制御手
段を少なくとも有することを特徴とする光磁気記録装
置。
(10) At least an optical head for irradiating light for raising the temperature of the magnetic film, a magnetic field applying means for applying a magnetic field on the magnetic film, and for forming a desired recording magnetic domain. The magneto-optical recording medium includes a modulator for changing the intensity of the light or the intensity or direction of the magnetic field, and an automatic position controller for irradiating the light to a desired position on the recording medium. The magneto-optical recording device to be used, comprising at least a recording control means for forming a recording magnetic domain so that a domain wall is located at a boundary between the partial area and the other portion.

【0026】(11)前記記録制御手段が、少なくとも、
前記光の強度を制御するための光強度制御部と前記光あ
るいは前記磁界の強度変化の時刻を制御するタイミング
制御部配した。
(11) The recording control means is at least
A light intensity control unit for controlling the intensity of the light and a timing control unit for controlling the time of the intensity change of the light or the magnetic field are arranged.

【0027】これらにより、記録磁区の幅または長さを
正確に制御して記録することが容易になる。すなわち、
高密度で、かつ、信号品質のよい記録を行うことが容易
になる。
As a result, it becomes easy to accurately control the width or length of the recording magnetic domain for recording. That is,
It becomes easy to perform recording with high density and good signal quality.

【0028】[0028]

【作用】本発明の記録媒体は、少なくとも一層の磁性膜
を有し、光を用いて磁性膜の温度を上昇させ、その温度
上昇部の磁化の向きを変化させて情報を記録する光磁気
記録媒体で、磁性膜内に磁気特性,熱特性及び光学特性
の少なくとも一つが他の部分と異なる領域を備えてい
る。
The recording medium of the present invention has at least one magnetic film, and the temperature of the magnetic film is raised by using light, and the direction of magnetization in the temperature rising portion is changed to record information. In the medium, the magnetic film has a region in which at least one of magnetic properties, thermal properties, and optical properties is different from other regions.

【0029】このため、例えば、磁性膜内の磁気特性,
熱特性及び光学特性の少なくとも一つが他の部分と異な
る領域のみを高感度(低い温度で記録できる)にするこ
とができ、適当な強度の(少し弱い)光を媒体に照射し
て記録を行えば、上高感度の領域にのみ記録磁区を形成
することができその他の領域に磁区が広がることはな
い。従って、磁気特性,熱特性及び光学特性の少なくと
も一つが他の部分と異なる領域と同程度の大きさの微小
な記録磁区を形成することが容易になる。
Therefore, for example, the magnetic characteristics in the magnetic film,
High sensitivity (recording at low temperature) can be achieved only in the area where at least one of thermal characteristics and optical characteristics is different from other areas. For example, the recording magnetic domain can be formed only in the upper high sensitivity region, and the magnetic domain does not spread to other regions. Therefore, it becomes easy to form a minute recording magnetic domain having the same size as a region where at least one of the magnetic characteristic, the thermal characteristic and the optical characteristic is different from the other portion.

【0030】そこで、この、磁気特性,熱特性及び光学
特性の少なくとも一つが他の部分と異なる微小領域を、
短波長の光などを用いてあらかじめ形成しておけば、高
密度記録が安定に行える。
Therefore, a minute region in which at least one of the magnetic characteristic, the thermal characteristic and the optical characteristic is different from other portions,
If it is formed in advance by using light with a short wavelength, high density recording can be stably performed.

【0031】また、その際、記録される磁区の形状や大
きさは、あらかじめ形成した磁気特性、熱特性及び光学
特性の少なくとも一つが他の部分と異なる微小領域の形
状や大きさによって決まるため、記録時のレーザ光強度
が変化したりしたとしても、一定の形状大きさの磁区が
形成でき、高S/Nな(低ノイズの)記録が可能とな
る。
Further, at this time, the shape and size of the recorded magnetic domain are determined by the shape and size of a minute region in which at least one of the magnetic property, the thermal property and the optical property which is formed in advance is different from other parts. Even if the laser light intensity during recording changes, magnetic domains having a constant shape and size can be formed, and high S / N (low noise) recording is possible.

【0032】このような手法で形成した媒体を用いて高
密度記録を行うには、例えば、磁性膜の温度を上昇させ
るための光を照射する光ヘッドと、磁性膜上に磁界を印
加するための磁界印加手段と、所望の記録磁区を形成す
るために光の強度をあるいは磁界の強度あるいは向きを
変化させるための変調手段と、光を記録媒体上の所望の
位置に照射するための自動位置制御手段を含み、光の強
度を制御する光強度制御部か、光あるいは磁化の強度変
化の時刻を制御するタイミング制御部を有する装置を用
い、記録磁区があらかじめ形成した磁気特性,熱特性及
び光学特性の少なくとも一つが他の部分と異なる微小領
域と一致して形成されるようにする。
In order to perform high density recording using the medium formed by such a method, for example, an optical head for irradiating light for raising the temperature of the magnetic film and a magnetic field applied on the magnetic film are applied. Magnetic field applying means, modulating means for changing the light intensity or the magnetic field strength or direction to form a desired recording magnetic domain, and an automatic position for irradiating light to a desired position on a recording medium. Using a device having a light intensity control unit for controlling the intensity of light or a timing control unit for controlling the time of intensity change of light or magnetization, including a control means, the magnetic characteristics, thermal characteristics and At least one of the characteristics is formed so as to coincide with a minute area different from other areas.

【0033】[0033]

【実施例】【Example】

《実施例1》図1に本発明の光磁気記録媒体の一実施例
の説明図を示す。光磁気記録媒体は、ディスク状の基板
1上に少なくとも磁性膜2を備えて成る。この例では磁
性膜2としてTbFeCoなどの光磁気記録膜を用いて
いる。TbFeCoなどの光磁気記録膜を用いる場合、
光磁気効果の増大と耐酸化性の向上のために、誘電体層
31(膜厚60nm)や保護層33(膜厚60nm)を
設け磁性層32(膜厚80nm)を挟んだ構成の磁性膜
を用いるのが望ましい。もちろん必要に応じて熱拡散層
や反射層などの金属層を設けても良い。磁性膜2上に
は、図1に示したように、保磁力の低い領域3が設けら
れている。この保磁力の低い領域3はディスク上にいろ
いろな形状に配置することが可能であるが図5に示した
ように同心円状または螺旋状に配置することによりトラ
ックを兼ねることができ、アクセスが容易になるため本
実施例では螺旋状に配置した。この時の保磁力の低い領
域3の幅は0.4μmとした。また、この保磁力の低い
領域3間の距離は0.3μmである。
<< Embodiment 1 >> FIG. 1 shows an explanatory view of an embodiment of the magneto-optical recording medium of the present invention. The magneto-optical recording medium comprises at least a magnetic film 2 on a disk-shaped substrate 1. In this example, a magneto-optical recording film such as TbFeCo is used as the magnetic film 2. When using a magneto-optical recording film such as TbFeCo,
A magnetic film having a structure in which a dielectric layer 31 (film thickness 60 nm) and a protective layer 33 (film thickness 60 nm) are provided to sandwich the magnetic layer 32 (film thickness 80 nm) in order to increase the magneto-optical effect and the oxidation resistance. It is preferable to use. Of course, a metal layer such as a heat diffusion layer or a reflection layer may be provided if necessary. A region 3 having a low coercive force is provided on the magnetic film 2 as shown in FIG. The region 3 having a low coercive force can be arranged in various shapes on the disk, but by arranging it in a concentric circle shape or a spiral shape as shown in FIG. Therefore, in this embodiment, they are arranged in a spiral shape. At this time, the width of the region 3 having a low coercive force was set to 0.4 μm. The distance between the regions 3 having low coercive force is 0.3 μm.

【0034】以下、この媒体が高密度化に有効であるこ
とを説明する。
Hereinafter, it will be explained that this medium is effective for increasing the density.

【0035】図3に示したように同じバイアス磁界で記
録するとき、保磁力の低い領域は、保磁力の高い領域と
比べて低い温度で記録できる。すなわち、保磁力の低い
領域は、他の部分と比べて、記録感度が高くなる。従っ
て、適当な強度で光を照射し媒体を昇温させることによ
り、図4に示したように媒体中の記録感度の高い領域、
すなわち、保磁力の低い領域3にのみ記録磁区を形成す
ることが可能となる。従って、記録磁区の幅は記録レー
ザ光の波長(スポット径)に依らず、保磁力の低い領域
3の幅(0.4μm)に限定される。すなわち、高密度
(狭トラック)記録が実現できる。この例では0.7μ
m ピッチの狭トラック記録が実現できるため、記録ビ
ットピッチ(線記録密度)を0.3μm とすれば1平方
インチあたり3GBの記録密度が達成できる。
When recording is performed with the same bias magnetic field as shown in FIG. 3, an area having a low coercive force can be recorded at a lower temperature than an area having a high coercive force. That is, the region having a low coercive force has a higher recording sensitivity than other regions. Therefore, by irradiating light with an appropriate intensity to raise the temperature of the medium, as shown in FIG. 4, a region with high recording sensitivity in the medium,
That is, the recording magnetic domain can be formed only in the region 3 having a low coercive force. Therefore, the width of the recording magnetic domain is limited to the width (0.4 μm) of the region 3 having a low coercive force, regardless of the wavelength (spot diameter) of the recording laser light. That is, high density (narrow track) recording can be realized. 0.7μ in this example
Since narrow track recording of m pitch can be realized, if the recording bit pitch (linear recording density) is 0.3 μm, a recording density of 3 GB per square inch can be achieved.

【0036】この例では、媒体上に保磁力の低い領域3
がある例を示したが、もちろんこの保磁力の低い領域の
変わりにその他の磁気特性または熱特性,光学特性の変
化した領域91を備えて成るものでも良い。
In this example, the region 3 having a low coercive force is formed on the medium.
However, it is of course possible to provide a region 91 in which other magnetic characteristics, thermal characteristics, or optical characteristics are changed in place of the low coercive force area.

【0037】また、この例では、この保磁力の低い領域
3、あるいは、磁気特性または熱特性,光学特性の変化
した領域91の形状が同心円状あるいは螺旋状である場
合を示したが、もちろんこの形状は別の形状、例えば、
図6に示す略円形の領域が数多く並ぶ形体でも良い。こ
の場合、狭トラック化のみならず線記録密度の高密度化
も実現できる。
In this example, the region 3 having a low coercive force, or the region 91 in which the magnetic characteristics, the thermal characteristics, and the optical characteristics are changed has a concentric or spiral shape. The shape is another shape, for example
A shape in which a large number of substantially circular regions shown in FIG. 6 are arranged may be used. In this case, not only a narrow track but also a high linear recording density can be realized.

【0038】また、磁性膜は、TbFeCo膜以外にも
PtCo膜やGdFeCo膜など光磁気記録膜として知
られたいずれの膜でも利用できる。本発明の効果は磁性
膜の種類に依らない。
The magnetic film may be any film known as a magneto-optical recording film such as a PtCo film or a GdFeCo film other than the TbFeCo film. The effect of the present invention does not depend on the type of magnetic film.

【0039】また、図1では光が基板と反対側から記録
膜に照射されているように図示されているが、これは、
図示の便宜上の問題で、記録のための光は基板側,基板
と反対側いずれでも問題なく本発明の効果がみられる。
Further, in FIG. 1, it is shown that light is applied to the recording film from the side opposite to the substrate.
For the sake of convenience of illustration, the effect of the present invention can be seen without any problem for the light for recording on either the substrate side or the side opposite to the substrate.

【0040】《実施例2》図7および図8に本発明の光
磁気記録媒体の1実施例の部分の断面図を示す。光磁気
記録媒体は、ディスク状の基板1上に小さな穴(溝)を有
するSnSbSe低融点膜41(膜厚50nm)と磁性
膜2を含む。この穴の径(溝の幅)は0.4μmであ
る。この例では磁性膜2としてTbFeCoなどの光磁
気記録膜を用い磁性層32(膜厚50nm)としてお
り、光磁気効果の増大と耐酸化性の向上のために、誘電
体層31(膜厚70nm)や保護層33(膜厚40n
m)を設け磁性層32を挟んだ構成にしてある。
<Embodiment 2> FIGS. 7 and 8 are sectional views showing a part of one embodiment of the magneto-optical recording medium of the present invention. The magneto-optical recording medium includes a SnSbSe low melting point film 41 (film thickness 50 nm) having a small hole (groove) on a disk-shaped substrate 1 and a magnetic film 2. The diameter of this hole (width of the groove) is 0.4 μm. In this example, a magneto-optical recording film such as TbFeCo is used as the magnetic film 2 to form the magnetic layer 32 (film thickness 50 nm). In order to increase the magneto-optical effect and the oxidation resistance, the dielectric layer 31 (film thickness 70 nm) is used. ) And the protective layer 33 (film thickness 40n
m) is provided to sandwich the magnetic layer 32.

【0041】この穴の部分では光学特性や熱特性が異な
るため、記録感度が異なっている、この例では穴の部分
で記録感度が高くなるように各層の膜厚を設計した。す
なわち、穴の部分では反射率が下がりかつ熱容量が減少
しているために、温度が上がりやすく実効的に記録感度
が上昇している。
Since the optical characteristics and the thermal characteristics are different in the hole portion, the recording sensitivity is different. In this example, the film thickness of each layer is designed so that the recording sensitivity is high in the hole portion. That is, since the reflectance is reduced and the heat capacity is reduced in the hole portion, the temperature easily rises and the recording sensitivity is effectively increased.

【0042】この例も、実施例1と同様に高密度化に有
効である。
This example is also effective for increasing the density as in the first embodiment.

【0043】《実施例3》実施例1に示した媒体の製造
方法の例を示す。
Example 3 An example of a method of manufacturing the medium shown in Example 1 will be described.

【0044】まず、ディスク状の基板1上に磁性膜2を
積層する。この例では磁性膜2としてTbFeCo光磁
気記録膜を用い、磁性層32とし、光磁気効果の増大と
耐酸化性の向上のために、誘電体層31(膜厚60nm)
や保護層33(膜厚60nm)を設け磁性層32(膜厚8
0nm)を挟んだ構成の磁性膜を用いる。これらの、誘
電体層31,磁性層32,保護層33はこの順に高周波
マグネトロンスパッタ法で製膜した。もちろん必要に応
じて熱拡散層や反射層などの金属層を設けても良い。
First, the magnetic film 2 is laminated on the disk-shaped substrate 1. In this example, a TbFeCo magneto-optical recording film is used as the magnetic film 2 and the magnetic layer 32 is used. The dielectric layer 31 (film thickness 60 nm) is used to increase the magneto-optical effect and the oxidation resistance.
And a protective layer 33 (film thickness 60 nm) is provided, and the magnetic layer 32 (film thickness 8
0 nm) is sandwiched between the magnetic films. The dielectric layer 31, the magnetic layer 32, and the protective layer 33 were formed in this order by a high frequency magnetron sputtering method. Of course, a metal layer such as a heat diffusion layer or a reflection layer may be provided if necessary.

【0045】次に、磁性膜上に保磁力の小さな領域3を
形成する。これには、記録光(4mW)よりも強度の強
い(6mW)の短波長(457nm)の光を開口比の大
きな(0.8)レンズで磁性膜2に照射して行う。この
時、内外周で特性が変わらないように線速度一定で行っ
た。この時の保磁力の低い領域3の幅は0.4μm とな
る。また、この保磁力の低い領域3間の距離は0.3μ
m(0.7μmピッチ)とした。
Next, the region 3 having a small coercive force is formed on the magnetic film. This is performed by irradiating the magnetic film 2 with light having a short wavelength (457 nm) having a higher intensity (6 mW) than the recording light (4 mW) with a lens having a large aperture ratio (0.8). At this time, the linear velocity was constant so that the characteristics did not change between the inner and outer circumferences. At this time, the width of the region 3 having a low coercive force is 0.4 μm. The distance between the regions 3 having low coercive force is 0.3 μm.
m (0.7 μm pitch).

【0046】上記の操作で、この保磁力の低い領域3が
形成される原理を図9を用いて説明する。一般にTbF
eCoなどの光磁気記録膜は、300℃以上に昇温する
と、保磁力が低下する(図9(a))。また、記録光よ
りも強度の強い短波長の光を開口比の大きなレンズで磁
性膜2に照射して、磁性膜の一部分の温度を昇温すると
その時の温度分布は図9(b)のようになる。従って、
この操作により、昇温した中心部の温度は、300℃を
超えるため、保磁力が低下し、保磁力の低い領域3とな
る。従って、この300℃を超える部分の幅が0.4μ
m となるように強度の強い光を制御して照射する。こ
の強度の強い光は短波長で開口数が大きいため、0.4
μm という狭い領域を制御するのは容易である。
The principle of forming the region 3 having a low coercive force by the above operation will be described with reference to FIG. Generally TbF
A magneto-optical recording film such as eCo has a lower coercive force when heated to 300 ° C. or higher (FIG. 9A). Further, when the magnetic film 2 is irradiated with light having a short wavelength, which is stronger than the recording light, with a lens having a large aperture ratio, and the temperature of a part of the magnetic film is raised, the temperature distribution at that time is as shown in FIG. 9B. become. Therefore,
By this operation, the temperature of the heated central portion exceeds 300 ° C., so that the coercive force is reduced and the region 3 having a low coercive force is formed. Therefore, the width of the part that exceeds 300 ℃ is 0.4μ.
Irradiation is performed by controlling light with high intensity so that m becomes m. This strong light has a short wavelength and a large numerical aperture, so 0.4
It is easy to control a small area of μm.

【0047】ここでは、保磁力が低下し始める領域の温
度が300℃であるとしたが、磁性膜の組成,膜厚,製
膜条件などによりこの温度はおよそ150℃から500
℃の間で変化する。
Although the temperature of the region where the coercive force starts to decrease is 300 ° C. here, this temperature is about 150 ° C. to 500 ° C. depending on the composition of the magnetic film, the film thickness, the film forming conditions and the like.
Varies between ° C.

【0048】《実施例4》実施例2の記録媒体の製造方
法を示す。
Example 4 A method of manufacturing the recording medium of Example 2 will be described.

【0049】実施例3では強度の強い光の照射による保
磁力の変化を利用したが、本実施例では、SnSbSe
などの低融点膜41(穴あけ型光記録膜)を積層しその
低融点膜41に実施例3と同様な強度の強い光により穴
をあけて、実施例2の穴の部分を形成する。この場合、
強度の強い光による昇温で基板などの変形が生じること
を防止するためには、低融点膜41の融点を500℃以
下とするのが良い。また、情報記録の際に上記低融点膜
41が変形するのを防ぐために、低融点膜41の融点は
記録温度よりも少なくとも高い方が良い。すなわち、低
融点膜41の融点は200℃以上とするのが良い。より
好ましくは、300℃以上とするのが良く、この場合、
繰返し記録や再生に対する信頼性が増す。
In the third embodiment, the change in the coercive force due to the irradiation of intense light is used, but in the present embodiment, SnSbSe is used.
A low melting point film 41 (perforation type optical recording film) is laminated and the low melting point film 41 is perforated with strong light similar to that of the third embodiment to form a hole portion of the second embodiment. in this case,
In order to prevent the substrate or the like from being deformed due to temperature rise due to light having high intensity, the melting point of the low melting point film 41 is preferably set to 500 ° C. or less. Further, in order to prevent the low melting point film 41 from being deformed at the time of recording information, the melting point of the low melting point film 41 is preferably at least higher than the recording temperature. That is, the melting point of the low melting point film 41 is preferably 200 ° C. or higher. More preferably, the temperature is preferably 300 ° C. or higher. In this case,
Increased reliability for repeated recording and playback.

【0050】図7の場合は、低融点膜41を積層後,強
度の強い光を照射し穴を形成する。その後、記録膜2を
実施例3と同様に積層する。
In the case of FIG. 7, after laminating the low melting point film 41, strong light is irradiated to form a hole. Then, the recording film 2 is laminated in the same manner as in Example 3.

【0051】図8の場合は、すべての膜を積層後に強度
の強い光を照射して、穴を形成する。その際、磁性膜が
極端な高温にさらされることを防ぐために、低融点膜の
融点を400℃以下とするのが望ましい。
In the case of FIG. 8, holes are formed by irradiating strong light after stacking all the films. At that time, in order to prevent the magnetic film from being exposed to an extremely high temperature, it is desirable that the melting point of the low melting point film is 400 ° C. or less.

【0052】《実施例5》実施例1に示した媒体の実施
例3とは別の製造方法の例を図10に示す。
<Embodiment 5> An example of a manufacturing method different from that of Embodiment 3 of the medium shown in Embodiment 1 is shown in FIG.

【0053】基板上に微小な凹凸部と平坦部を有する紫
外線硬化樹脂23を形成しておき、その上に、磁性膜2
を積層する。この例では磁性膜2としてTbFeCo光
磁気記録膜を用い、磁性層32とし、光磁気効果の増大
と耐酸化性の向上のために、誘電体層31(膜厚60n
m)や保護層33(膜厚60nm)を設け、磁性層32
(膜厚80nm)を挟んだ構成の磁性膜を用いた。基板
上に微小な凹凸部と平坦部を有する紫外線硬化樹脂23
を形成しておくには、微小な凹凸部と平坦部を有するス
タンパから転写して行うのが簡便である。この方法は、
従来の光ディスク基板の案内溝やピットを作成するのに
用いられている方法と同様である。従って、紫外線硬化
樹脂層23を用いる代わりに、射出成型法によりポリカ
ーボネートなどのプラスチック基板を形成する方法でも
良い。いずれにしても、基板の表面に微小な凹凸を有す
る部分と平坦な部分を設ければ良い。
An ultraviolet curable resin 23 having minute irregularities and flat portions is formed on a substrate, and the magnetic film 2 is formed on the ultraviolet curable resin 23.
Are laminated. In this example, a TbFeCo magneto-optical recording film is used as the magnetic film 2, and the magnetic layer 32 is used. In order to increase the magneto-optical effect and the oxidation resistance, the dielectric layer 31 (having a film thickness of 60 n) is used.
m) and a protective layer 33 (film thickness 60 nm) are provided, and the magnetic layer 32
A magnetic film having a structure sandwiching (thickness of 80 nm) was used. UV curable resin 23 having minute irregularities and flat portions on the substrate
In order to form the pattern, it is easy to transfer the pattern from a stamper having a minute uneven portion and a flat portion. This method
This is the same as the method used to create the guide groove or pit of the conventional optical disk substrate. Therefore, instead of using the ultraviolet curable resin layer 23, a method of forming a plastic substrate such as polycarbonate by an injection molding method may be used. In any case, it suffices to provide a portion having minute irregularities and a flat portion on the surface of the substrate.

【0054】このようにして、作成した媒体では、微小
な凹凸部と平坦部で磁性膜2の保磁力が異なるため、結
果として、保磁力の低い部分とそうでない部分を有する
媒体を得ることがでる。すなわち、実施例1の記録媒体
を得ることができる。
In the medium thus produced, the coercive force of the magnetic film 2 is different between the minute uneven portion and the flat portion, and as a result, a medium having a portion with low coercive force and a portion with no coercive force can be obtained. Out. That is, the recording medium of Example 1 can be obtained.

【0055】この場合、高密度化のため微小な凹凸部ま
たは平坦部の大きさは0.6μm 以下とするのが望まし
く。高S/N化(低ノイズ化)のためには、微小な凹凸
そのものの高さは2nm以上20nm以下、凹凸そのも
のの大きさは0.1μm 以下とするのが良い。
In this case, it is desirable that the size of the fine uneven portion or the flat portion be 0.6 μm or less in order to increase the density. In order to increase the S / N ratio (reduce noise), it is preferable that the height of the minute unevenness itself is 2 nm or more and 20 nm or less, and the size of the unevenness itself is 0.1 μm or less.

【0056】《実施例6》図11に本発明の光磁気記録
装置のブロック図を示す。
<Embodiment 6> FIG. 11 shows a block diagram of a magneto-optical recording apparatus of the present invention.

【0057】本発明の光磁気記録媒体12を用い、光磁
気記録媒体12に記録や再生のための光を照射する光ヘ
ッドを有し、その光ヘッドはオートフォーカスやトラッ
キングなどの位置制御手段によって、情報を記録/再生
すべき位置に位置決めされている。情報を記録する際に
は、記録すべき情報に応じて光の強度や磁界の強度を変
調手段を用いて変調する。その際、記録されて形成され
る磁区が、図6などに示した、磁気特性または熱特性,
光学特性の変化した領域91と概ね一致するように、再
生信号を元にクロック生成回路で作られたクロックに従
って、タイミング制御部によって、光や磁界の照射時刻
(タイミング)を制御する。磁気特性または熱特性,光
学特性の変化した領域91が図5に示したように同心円
あるいは螺旋上の形状を持つ場合にはタイミング制御回
路は不要である。
Using the magneto-optical recording medium 12 of the present invention, an optical head for irradiating the magneto-optical recording medium 12 with light for recording and reproduction is provided, and the optical head is controlled by position control means such as auto-focusing and tracking. , Is positioned at a position where information should be recorded / reproduced. When information is recorded, the intensity of light and the intensity of magnetic field are modulated by a modulation means according to the information to be recorded. At that time, the magnetic domains formed by recording have magnetic or thermal characteristics shown in FIG.
The timing control unit controls the irradiation time (timing) of light or magnetic field in accordance with the clock generated by the clock generation circuit based on the reproduction signal so as to approximately match the region 91 where the optical characteristics have changed. If the region 91 where the magnetic characteristic, the thermal characteristic, or the optical characteristic has changed has a concentric circle or spiral shape as shown in FIG. 5, the timing control circuit is not necessary.

【0058】本実施例では図6に示した構成の記録媒体
を用い、サンプルサーボ記録方式により、オートフォー
カスやトラッキングなどの位置制御をし、情報を記録す
る際には、記録すべき情報に応じて光の強度や磁界の強
度を変調手段を用いて変調する。その際、記録されて形
成される磁区が、図6などに示した、磁気特性または熱
特性,光学特性の変化した領域91と概ね一致するよう
に、再生信号を元にクロック生成回路で作られたクロッ
クに従って、タイミング制御部により、光や磁界の照射
時刻(タイミング)を制御する。
In this embodiment, the recording medium having the structure shown in FIG. 6 is used, and position control such as autofocusing and tracking is performed by the sample servo recording method, and when recording information, according to the information to be recorded. The intensity of light and the intensity of the magnetic field are modulated by the modulation means. At that time, a clock generation circuit is created based on the reproduction signal so that the recorded and formed magnetic domains substantially match the regions 91 in which the magnetic characteristics, the thermal characteristics, and the optical characteristics are changed as shown in FIG. The timing control unit controls the irradiation time (timing) of light or magnetic field according to the clock.

【0059】この方法で、1平方インチあたり3ギガバ
イト以上の高密度な記録が可能であった。
With this method, high density recording of 3 gigabytes or more per square inch was possible.

【0060】[0060]

【発明の効果】本発明では、光スポットよりも小さな記
録磁区を安定に形成することが可能となるため、1平方
インチあたり3ギガバイト以上の高密度な記録が可能で
ある。
According to the present invention, it is possible to stably form a recording magnetic domain smaller than the light spot, so that high density recording of 3 gigabytes or more per square inch is possible.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の光磁気記録媒体の一実施例を示す説明
図。
FIG. 1 is an explanatory view showing an embodiment of a magneto-optical recording medium of the present invention.

【図2】従来の光磁気記録媒体の一例を示す説明図。FIG. 2 is an explanatory diagram showing an example of a conventional magneto-optical recording medium.

【図3】本発明の一実施例の原理の説明図。FIG. 3 is an explanatory diagram of the principle of one embodiment of the present invention.

【図4】本発明の原理の説明図。FIG. 4 is an explanatory diagram of the principle of the present invention.

【図5】本発明の光磁気記録媒体の一実施例を示す斜視
図。
FIG. 5 is a perspective view showing an embodiment of the magneto-optical recording medium of the present invention.

【図6】本発明の光磁気記録媒体の第二実施例を示す斜
視図。
FIG. 6 is a perspective view showing a second embodiment of the magneto-optical recording medium of the present invention.

【図7】本発明の光磁気記録媒体の一実施例を示す説明
図。
FIG. 7 is an explanatory diagram showing an embodiment of a magneto-optical recording medium of the present invention.

【図8】本発明の光磁気記録媒体の一実施例を示す断面
図。
FIG. 8 is a sectional view showing an embodiment of the magneto-optical recording medium of the present invention.

【図9】本発明の光磁気記録媒体の製造方法の原理の説
明図。
FIG. 9 is an explanatory view of the principle of the method for manufacturing a magneto-optical recording medium of the present invention.

【図10】本発明の光磁気記録媒体の製造方法の一実施
例を示す断面図。
FIG. 10 is a cross-sectional view showing one embodiment of a method of manufacturing a magneto-optical recording medium of the present invention.

【図11】本発明の光磁気記録装置の一実施例を示すブ
ロック図。
FIG. 11 is a block diagram showing an embodiment of a magneto-optical recording apparatus of the present invention.

【符号の説明】[Explanation of symbols]

1…基板、2…磁性膜、3…保磁力の低い領域、4…記
録膜、5…記録磁区、6…光スポット、7…レンズ、8
…レーザ光、17…磁界、18…磁界印加手段。
1 ... Substrate, 2 ... Magnetic film, 3 ... Low coercive force region, 4 ... Recording film, 5 ... Recording magnetic domain, 6 ... Light spot, 7 ... Lens, 8
... laser light, 17 ... magnetic field, 18 ... magnetic field applying means.

───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.6 識別記号 庁内整理番号 FI 技術表示箇所 G11B 11/10 586 B 9296−5D (72)発明者 粟野 博之 東京都国分寺市東恋ケ窪1丁目280番地 株式会社日立製作所中央研究所内─────────────────────────────────────────────────── ─── Continuation of the front page (51) Int.Cl. 6 Identification number Internal reference number FI Technical indication location G11B 11/10 586 B 9296-5D (72) Inventor Hiroyuki Awano 1-280, Higashi Koikeku, Kokubunji, Tokyo Central Research Laboratory, Hitachi, Ltd.

Claims (11)

【特許請求の範囲】[Claims] 【請求項1】少なくとも一層の磁性膜からなる光磁気記
録媒体において、前記光磁気記録媒体に一定磁界を印加
しながら温度を徐々に上げたとき、前記磁性膜内の一部
の領域にのみ反転磁区ができ、その他の領域にはできな
いような温度が存在することを特徴とする光磁気記録媒
体。
1. In a magneto-optical recording medium comprising at least one magnetic film, when a temperature is gradually raised while applying a constant magnetic field to the magneto-optical recording medium, only a part of the magnetic film is inverted. A magneto-optical recording medium characterized in that there is a temperature that can form magnetic domains and cannot exist in other regions.
【請求項2】少なくとも一層の磁性膜からなる光磁気記
録媒体において、前記光磁気記録媒体に一定温度で印加
する磁界を徐々に上げたとき、前記磁性膜内の一部の領
域にのみ反転磁区ができその他の領域にはできないよう
な磁界が存在することを特徴とする光磁気記録媒体。
2. In a magneto-optical recording medium comprising at least one magnetic film, when a magnetic field applied to the magneto-optical recording medium at a constant temperature is gradually increased, a reversed magnetic domain is formed only in a part of the magnetic film. A magneto-optical recording medium characterized by the presence of a magnetic field that can be generated and cannot be generated in other areas.
【請求項3】少なくとも一層の磁性膜を有する光磁気記
録媒体において、該磁性膜内に記録感度の高い一部の領
域が存在することを特徴とする光磁気記録媒体。
3. A magneto-optical recording medium having a magnetic film of at least one layer, wherein a part of a region having high recording sensitivity is present in the magnetic film.
【請求項4】少なくとも一層の磁性膜からなる光磁気記
録媒体において、前記磁性膜内に保磁力の低い一部の領
域が存在することを特徴とする光磁気記録媒体。
4. A magneto-optical recording medium comprising at least one magnetic film, wherein the magnetic film has a part of a region having a low coercive force.
【請求項5】請求項1,2,3または4において、前記
一部の領域の幅およびまたは長さが情報記録単位の幅ま
たは長さのいずれかよりも小さい光磁気記録媒体。
5. The magneto-optical recording medium according to claim 1, 2, 3 or 4, wherein the width and / or the length of the partial area is smaller than either the width or the length of the information recording unit.
【請求項6】請求項1,2,3,4または5において、
前記光磁気記録媒体が、前記磁性膜以外に融点が200
℃以上500℃以下の膜を含む光磁気記録媒体。
6. The method according to claim 1, 2, 3, 4 or 5.
The magneto-optical recording medium has a melting point of 200 in addition to the magnetic film.
A magneto-optical recording medium including a film having a temperature of not less than 500 ° C. and not more than 500 ° C.
【請求項7】請求項1,2,3,4または5において、
前記光磁気記録媒体が、前記磁性膜以外に融点が300
℃以上400℃以下の膜を含む光磁気記録媒体。
7. The method according to claim 1, 2, 3, 4 or 5,
The magneto-optical recording medium has a melting point of 300 in addition to the magnetic film.
A magneto-optical recording medium including a film at a temperature of not less than 400 ° C. and not more than 400 ° C.
【請求項8】請求項1,2,3,4または5において、
前記一部の領域を形成するにあたり、記録媒体上に通常
の記録時の光スポット径の0.8 倍以下の光スポット径
の光を照射して行う光磁気記録媒体の製造方法。
8. The method according to claim 1, 2, 3, 4 or 5.
A method for manufacturing a magneto-optical recording medium, which comprises forming a part of the region by irradiating the recording medium with light having a light spot diameter not more than 0.8 times the light spot diameter at the time of normal recording.
【請求項9】融点が200℃以上500℃以下の膜を設
けた後、光を照射して膜を融かし穴を開け、その後、磁
性膜を設けることを特徴とする光磁気記録媒体の製造方
法。
9. A magneto-optical recording medium comprising a film having a melting point of 200 ° C. or more and 500 ° C. or less, irradiating light to melt the film to form a hole, and then providing a magnetic film. Production method.
【請求項10】少なくとも磁性膜の温度を上昇させるた
めの光を照射する光ヘッドと、前記磁性膜上に磁界を印
加するための磁界印加手段と、所望の記録磁区を形成す
るために前記光の強度をあるいは前記磁界の強度あるい
は向きを変化させるための変調手段と、前記光を記録媒
体上の所望の位置に照射するための自動位置制御手段と
を有し、前記光磁気記録媒体を用いる光磁気記録装置に
おいて、請求項1から5に記載の前記一部の領域と前記
その他の部分との境界部に磁壁が位置するよう記録磁区
を形成するための記録制御手段を含むことを特徴とする
光磁気記録装置。
10. An optical head for irradiating at least light for raising the temperature of a magnetic film, a magnetic field applying means for applying a magnetic field on the magnetic film, and the light for forming a desired recording magnetic domain. Using a magneto-optical recording medium having a modulation means for changing the intensity of the magnetic field or the intensity or direction of the magnetic field, and an automatic position control means for irradiating the light to a desired position on the recording medium. A magneto-optical recording apparatus comprising: a recording control unit for forming a recording magnetic domain so that a domain wall is located at a boundary between the partial region and the other portion according to claim 1. Magneto-optical recording device.
【請求項11】請求項9において、前記記録制御手段
が、前記光の強度を制御するための光強度制御部と、前
記光あるいは前記磁界の強度変化の時刻を制御するタイ
ミング制御部とを含む光磁気記録装置。
11. The recording control means according to claim 9, further comprising a light intensity control unit for controlling the intensity of the light, and a timing control unit for controlling the time of the intensity change of the light or the magnetic field. Magneto-optical recording device.
JP13986094A 1994-06-22 1994-06-22 Magneto-optical recording medium, its manufacturing method and apparatus Pending JPH087361A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13986094A JPH087361A (en) 1994-06-22 1994-06-22 Magneto-optical recording medium, its manufacturing method and apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13986094A JPH087361A (en) 1994-06-22 1994-06-22 Magneto-optical recording medium, its manufacturing method and apparatus

Publications (1)

Publication Number Publication Date
JPH087361A true JPH087361A (en) 1996-01-12

Family

ID=15255230

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13986094A Pending JPH087361A (en) 1994-06-22 1994-06-22 Magneto-optical recording medium, its manufacturing method and apparatus

Country Status (1)

Country Link
JP (1) JPH087361A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0848381A2 (en) * 1996-12-13 1998-06-17 Canon Kabushiki Kaisha Magneto-optical recording medium exclusively for reproduction, method of manufacturing the same and method of reproducing the medium

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0848381A2 (en) * 1996-12-13 1998-06-17 Canon Kabushiki Kaisha Magneto-optical recording medium exclusively for reproduction, method of manufacturing the same and method of reproducing the medium
EP0848381A3 (en) * 1996-12-13 1999-04-07 Canon Kabushiki Kaisha Magneto-optical recording medium exclusively for reproduction, method of manufacturing the same and method of reproducing the medium

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