JPH02304751A - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- Publication number
- JPH02304751A JPH02304751A JP12421089A JP12421089A JPH02304751A JP H02304751 A JPH02304751 A JP H02304751A JP 12421089 A JP12421089 A JP 12421089A JP 12421089 A JP12421089 A JP 12421089A JP H02304751 A JPH02304751 A JP H02304751A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- recording
- magneto
- read
- medium
- 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
- 230000035945 sensitivity Effects 0.000 abstract description 21
- 239000000463 material Substances 0.000 abstract description 2
- 230000003993 interaction Effects 0.000 abstract 1
- 239000010410 layer Substances 0.000 description 61
- 230000005415 magnetization Effects 0.000 description 12
- 239000000203 mixture Substances 0.000 description 6
- 238000010586 diagram Methods 0.000 description 5
- 238000000034 method Methods 0.000 description 5
- 230000007423 decrease Effects 0.000 description 4
- 230000015654 memory Effects 0.000 description 4
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 239000011241 protective layer Substances 0.000 description 3
- 229910052581 Si3N4 Inorganic materials 0.000 description 2
- MCMNRKCIXSYSNV-UHFFFAOYSA-N Zirconium dioxide Chemical compound O=[Zr]=O MCMNRKCIXSYSNV-UHFFFAOYSA-N 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000010408 film Substances 0.000 description 2
- 230000006870 function Effects 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- 229910052723 transition metal Inorganic materials 0.000 description 2
- 229910052692 Dysprosium Inorganic materials 0.000 description 1
- 229910052688 Gadolinium Inorganic materials 0.000 description 1
- 229910052779 Neodymium Inorganic materials 0.000 description 1
- 229910052771 Terbium Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000003384 imaging method Methods 0.000 description 1
- XEEYBQQBJWHFJM-UHFFFAOYSA-N iron Substances [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 1
- -1 iron group transition metals Chemical class 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 229910052761 rare earth metal Inorganic materials 0.000 description 1
- 150000002910 rare earth metals Chemical class 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
- 238000004544 sputter deposition Methods 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]
本発明は、レーザ光を用いて情報の記録・再生を行う光
磁気記録媒体に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a magneto-optical recording medium that records and reproduces information using laser light.
し従来の技術]
光デイスクメモリは、高密度、大容量、高速アクセスが
可能であるということから、現在の磁気ディスクメモリ
に代わる新規なメモリとして考えられている。中でも光
磁気記録媒体を用いた光磁気ディスクは、書き換え性を
有していることから最も注目され、近年活発に研究開発
が行われている。BACKGROUND OF THE INVENTION Optical disk memories are considered as a new memory to replace current magnetic disk memories because they are capable of high density, large capacity, and high-speed access. Among them, magneto-optical disks using magneto-optical recording media have attracted the most attention because of their rewritability, and have been actively researched and developed in recent years.
第4図は従来の光磁気記録媒体の一例を示す断面図であ
る。この光磁気記録媒体は、ガラスまたは有機物樹脂よ
りなる支持基板1の上に中間層2、光磁気記録層7、保
護層6を順次堆積することにより作製される。中間層2
および保護層6には、S i3N4 、AJ! N、S
i02 、ZrO2、A2203などが用いられ、光
磁気記録層7には、Tb、Gd、Dy、Ndなどの希土
類金属と、Fe、Goなどの鉄族遷移金属との組み合わ
せによって作製される非晶質合金薄膜が主に用いられる
。FIG. 4 is a sectional view showing an example of a conventional magneto-optical recording medium. This magneto-optical recording medium is manufactured by sequentially depositing an intermediate layer 2, a magneto-optical recording layer 7, and a protective layer 6 on a support substrate 1 made of glass or organic resin. middle layer 2
And the protective layer 6 contains Si3N4, AJ! N,S
i02, ZrO2, A2203, etc. are used, and the magneto-optical recording layer 7 is an amorphous material made by a combination of rare earth metals such as Tb, Gd, Dy, and Nd and iron group transition metals such as Fe and Go. Alloy thin films are mainly used.
近年、情報の処理速度の高速化が進行し、情報の転送速
度の速いメモリシステムが必要となってきた。これに伴
い、光磁気ディスクにおいても転送速度を高速化するた
めに、ディスクの回転数の高速化を促進する必要が生じ
てきた。このような状況の中で、光磁気記録媒体の記録
感度を向上させることが求められている。In recent years, the processing speed of information has been increasing, and a memory system with a high information transfer speed has become necessary. Along with this, in order to increase the transfer speed of magneto-optical disks as well, it has become necessary to increase the number of rotations of the disk. Under these circumstances, there is a need to improve the recording sensitivity of magneto-optical recording media.
記録感度向上の方法の一つとして、高いキュリー温度を
持ち、カー回転角の大きな読み出し層と、低いキュリー
温度を持つ記録層とを組み合わせた2層膜を用いる方法
がある。One method for improving recording sensitivity is to use a two-layer film that combines a readout layer with a high Curie temperature and a large Kerr rotation angle and a recording layer with a low Curie temperature.
[発明が解決しようとする課題]
非晶質希土類−遷移金属を単層記録媒体として使用した
場合、記録感度の向上を図るためには媒体の磁気キュリ
ー温度Tcを低下させる必要がある。一方、読み出し信
号の撮幅を決定する媒体のカー回転角θには、磁気キュ
リー温度の低下とともに小さくなる。従って、媒体の磁
気キュリー温度を低下させる方法で感度向上を図ると、
読み出し信号の撮幅が減少し、信号品質が劣化する。[Problems to be Solved by the Invention] When an amorphous rare earth-transition metal is used as a single-layer recording medium, it is necessary to lower the magnetic Curie temperature Tc of the medium in order to improve recording sensitivity. On the other hand, the Kerr rotation angle θ of the medium, which determines the width of the read signal, decreases as the magnetic Curie temperature decreases. Therefore, if you try to improve sensitivity by lowering the magnetic Curie temperature of the medium,
The imaging width of the readout signal decreases, and the signal quality deteriorates.
また2層膜方式における問題として、記録過程において
、記録層は磁化を失い読み出し層に最初にビットが形成
されるが、このビット形状が乱れやすいために記録ノイ
ズの上昇が起こり、信号品質が低下するという点がある
。Another problem with the two-layer film method is that during the recording process, the recording layer loses its magnetization and bits are first formed on the readout layer, but this bit shape is easily distorted, resulting in an increase in recording noise and a decrease in signal quality. There is a point.
本発明の目的は、媒体の記録感度と信号品質をそれぞれ
独立に制御し、高記録感度で信号品質の高い光磁気記録
媒体を提供することにある。An object of the present invention is to provide a magneto-optical recording medium with high recording sensitivity and high signal quality by independently controlling the recording sensitivity and signal quality of the medium.
[課題を解決するための手段]
本発明は、光磁気記録層が、相対的に大きなカー回転角
と高い磁気キュリー温度を有する読み出し層と、該読み
出し層よりも磁気キュリー温度が低い記録層と、前記読
み出し層よりも磁気キュリー温度が低いスイッチング層
とからなり、かつスイッチング層が読み出し層と記録層
の層間に位置する膜構成を有することを特徴とする光磁
気記録媒体である。[Means for Solving the Problems] The present invention provides a magneto-optical recording layer including a readout layer having a relatively large Kerr rotation angle and a high magnetic Curie temperature, and a recording layer having a lower magnetic Curie temperature than the readout layer. and a switching layer having a magnetic Curie temperature lower than that of the readout layer, and the switching layer is located between the readout layer and the recording layer.
[作用]
本発明の光磁気記録媒体の作用を第5図に基づいて説明
する。[Function] The function of the magneto-optical recording medium of the present invention will be explained based on FIG. 5.
第5図(a)は初期化された状態であり、各層の磁化8
は上向きに揃っている。第5図(b)は、レーザ光を照
射することにより、媒体温度を記録層のキュリー温度ま
で上昇させたときの図でおり、レーザ照射部分の記録層
5とスイッチング層4は磁化を消失している。第5図(
C)は、レーザ光の照射が停止され、媒体温度が徐々に
降下している状態の図である。媒体温度が記録層5の磁
気キュリー温度以下になると、外部磁場1−1exの方
向に向いた磁化が現われる。この時、スイッチング層4
はまだ磁化を消失した状態であるため、記録層5と読み
出し層3の交換的な磁気結合はなく、記録層5には読み
出し層3の磁気的影響を受けることなくきれいなビット
が形成される。ざらに媒体温度が低下した第5図(d)
ではスイッチング層4に磁化が現われ、この磁化は外部
磁場Hexならびに記録層5の磁化の方向に揃う。これ
と同時に、読み出し層3の磁化はスイッチング層4の磁
化との交換結合により、スイッチング層4の磁化の方向
に揃う。FIG. 5(a) shows the initialized state, and the magnetization of each layer is 8.
are aligned upward. FIG. 5(b) is a diagram when the medium temperature is raised to the Curie temperature of the recording layer by irradiating the laser beam, and the recording layer 5 and switching layer 4 in the laser irradiated area lose their magnetization. ing. Figure 5 (
C) is a diagram showing a state in which the laser beam irradiation is stopped and the medium temperature is gradually decreasing. When the medium temperature becomes lower than the magnetic Curie temperature of the recording layer 5, magnetization appears in the direction of the external magnetic field 1-1ex. At this time, switching layer 4
is still in a state where magnetization has disappeared, so there is no exchange magnetic coupling between the recording layer 5 and the readout layer 3, and a clean bit is formed in the recording layer 5 without being affected by the magnetic influence of the readout layer 3. Figure 5(d), where the medium temperature has decreased drastically.
Then, magnetization appears in the switching layer 4, and this magnetization is aligned in the direction of the external magnetic field Hex and the magnetization of the recording layer 5. At the same time, the magnetization of the readout layer 3 is aligned in the direction of the magnetization of the switching layer 4 due to exchange coupling with the magnetization of the switching layer 4.
このような記録過程においては、記録に必要な媒体温度
は記録層の磁気キュリー温度付近でおるため、記録層の
磁気キュリー温度を低くすることにより記録感度を向上
させることが可能である。In such a recording process, the medium temperature required for recording is around the magnetic Curie temperature of the recording layer, so it is possible to improve the recording sensitivity by lowering the magnetic Curie temperature of the recording layer.
また、記録図にビットが形成される時点においては、ス
イッチング層の磁化が消失しており、記録層と読み出し
層の磁気交換結合がないので、読み出し層の磁気特性に
は影響を受けることなく記録層にビットが形成される。In addition, at the time when bits are formed in the recording diagram, the magnetization of the switching layer has disappeared and there is no magnetic exchange coupling between the recording layer and the readout layer, so the magnetic properties of the readout layer are not affected. Bits are formed in the layer.
従って、読み出し層に磁気キュリー温度が高く、カー回
転角の大きな媒体を使用することにより、記録感度を低
下させることなく信号品質を向上させることが可能であ
る。Therefore, by using a medium with a high magnetic Curie temperature and a large Kerr rotation angle in the readout layer, it is possible to improve signal quality without reducing recording sensitivity.
以上のように、本発明の光磁気記録媒体においては、記
録感度と信号品質を独立に制御することができるので、
高感度でかつ信号品質の高い光磁気記録媒体を提供する
ことができる。As described above, in the magneto-optical recording medium of the present invention, recording sensitivity and signal quality can be controlled independently.
A magneto-optical recording medium with high sensitivity and high signal quality can be provided.
[実施例]
次に本発明の実施例について、図面を参照して詳細に説
明する。[Example] Next, an example of the present invention will be described in detail with reference to the drawings.
第1図は、本発明の一実施例の概略断面図である。支持
基板1上にSiN中間層2、GdFeC0読み出し層3
、DyFeC○スイッチング層4、TbD”y’FeC
0記録@5、Si3N4保護層6を順次スパッタリング
法により成膜した。FIG. 1 is a schematic cross-sectional view of one embodiment of the present invention. SiN intermediate layer 2 and GdFeC0 readout layer 3 on support substrate 1
, DyFeC○ switching layer 4, TbD"y'FeC
0 recording@5 and a Si3N4 protective layer 6 were sequentially formed by sputtering.
第2図はそれぞれの磁性層の保磁力HCの温度特性を示
す。GdFeCo@(読み出し層)は、カー回転角を大
きくする目的で磁気キュリー温度が高< (TC= 4
00’C)なるような組成を選んだ。FIG. 2 shows the temperature characteristics of the coercive force HC of each magnetic layer. GdFeCo@ (readout layer) has a magnetic Curie temperature of high < (TC= 4) for the purpose of increasing the Kerr rotation angle.
00'C) was selected.
TbDVFeCo層(記録層)は、記録感度向上を目的
としてキュリー温度の低い組成を選び、磁気キュリー温
度が160’Cのもの(TbDyFeCo(a))と1
20℃(TbDyFeCo(b))の2種類の組成で作
製した。DyFeCo層(スイッチング層)は、磁気キ
ュリー温度90 ’Cの組成で作製した。For the TbDVFeCo layer (recording layer), a composition with a low Curie temperature was selected for the purpose of improving recording sensitivity, and a composition with a magnetic Curie temperature of 160'C (TbDyFeCo(a)) and 1
Two types of compositions were prepared at 20°C (TbDyFeCo(b)). The DyFeCo layer (switching layer) was fabricated with a composition having a magnetic Curie temperature of 90'C.
このようにして作製した光磁気記録媒体の記録再生特性
を第3図に示す。ディスク(a)は磁気キュリー温度が
160’Cの組成のTbD’y’FeC0層を用い、デ
ィスク(b)は磁気キュリー温度が120°Cの組成の
TbDVFeCo層を用いた試料である一0測定条件は
、ディスクの回転数360Orpm 。FIG. 3 shows the recording and reproducing characteristics of the magneto-optical recording medium thus produced. Disk (a) is a sample using a TbD'y'FeC0 layer with a composition with a magnetic Curie temperature of 160'C, and disk (b) is a sample with a TbDVFeCo layer with a composition with a magnetic Curie temperature of 120°C.10 measurements. The conditions were a disc rotation speed of 360 rpm.
半径r=iaommで行った。ディスク(b)はディス
ク(a)に比較して、記録しきい値パワーが2m1Il
小さく、感度が向上している。信号品質に相当するC/
Nは両ディスクとも60 dBであった。このように本
発明の光磁気記録媒体では、信号品質を損なうことなし
に記録感度を向上させることができる。The radius was set to r=iaomm. Disk (b) has a recording threshold power of 2m1Il compared to disk (a).
Smaller size and improved sensitivity. C/corresponding to signal quality
N was 60 dB for both disks. As described above, in the magneto-optical recording medium of the present invention, recording sensitivity can be improved without impairing signal quality.
本実施例においては、記録層の磁気キュリー温度を変化
させることにより記録感度を制御した例を示したが、読
み出し層のカー回転角を大きくすることにより記録感度
を低下させることなしに信号品質の向上を図ることも可
能である。In this example, an example was shown in which the recording sensitivity was controlled by changing the magnetic Curie temperature of the recording layer, but by increasing the Kerr rotation angle of the readout layer, the signal quality could be improved without reducing the recording sensitivity. It is also possible to improve this.
[発明の効果1
以上説明したように、本発明の光磁気記録媒体は、その
磁気記録層を記録層、読み出し1、スイッチング層の3
層構造とすることにより記録感度と信号品質を独立に制
御することが可能になった。[Effect of the invention 1 As explained above, the magneto-optical recording medium of the present invention has a magnetic recording layer composed of three layers: a recording layer, a readout layer, and a switching layer.
The layered structure makes it possible to independently control recording sensitivity and signal quality.
このことにより信号品質を損なうことなしに記録感度を
向上させること、ならびに記録感度を低下させることな
しに信号品質を向上させることができるという効果を有
する。This has the effect that recording sensitivity can be improved without impairing signal quality, and signal quality can be improved without reducing recording sensitivity.
第1図は本発明の一実施例の概略断面図、第2図は本発
明の一実施例における磁気記録層の保磁力の温度依存性
を示す特性図、第3図は本発明の一実施例の記録再生特
性を示す特性図、第4図は従来の光磁気ディスクの一例
の概略断面図、第5図は本発明の光磁気記録媒体の記録
方式を説明するための説明図でおる。FIG. 1 is a schematic cross-sectional view of one embodiment of the present invention, FIG. 2 is a characteristic diagram showing the temperature dependence of the coercive force of the magnetic recording layer in one embodiment of the present invention, and FIG. 3 is an embodiment of the present invention. FIG. 4 is a schematic cross-sectional view of an example of a conventional magneto-optical disk, and FIG. 5 is an explanatory diagram for explaining the recording method of the magneto-optical recording medium of the present invention.
Claims (1)
い磁気キュリー温度を有する読み出し層と、該読み出し
層よりも磁気キュリー温度が低い記録層と、前記読み出
し層よりも磁気キュリー温度が低いスイッチング層とか
らなり、かつスイッチング層が読み出し層と記録層の層
間に位置する膜構成を有することを特徴とする光磁気記
録媒体。(1) The magneto-optical recording layer includes a readout layer having a relatively large Kerr rotation angle and a high magnetic Curie temperature, a recording layer having a magnetic Curie temperature lower than that of the readout layer, and a magnetic Curie temperature lower than that of the readout layer. 1. A magneto-optical recording medium comprising a low switching layer, and having a film structure in which the switching layer is located between a readout layer and a recording layer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12421089A JPH02304751A (en) | 1989-05-19 | 1989-05-19 | Magneto-optical recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12421089A JPH02304751A (en) | 1989-05-19 | 1989-05-19 | Magneto-optical recording medium |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02304751A true JPH02304751A (en) | 1990-12-18 |
Family
ID=14879721
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12421089A Pending JPH02304751A (en) | 1989-05-19 | 1989-05-19 | Magneto-optical recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02304751A (en) |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63195845A (en) * | 1987-02-10 | 1988-08-12 | Canon Inc | Magneto-optical recording medium and magneto-optical recording method |
| JPS63205835A (en) * | 1987-02-23 | 1988-08-25 | Canon Inc | Magneto-optical recording medium and magneto-optical recording method |
-
1989
- 1989-05-19 JP JP12421089A patent/JPH02304751A/en active Pending
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63195845A (en) * | 1987-02-10 | 1988-08-12 | Canon Inc | Magneto-optical recording medium and magneto-optical recording method |
| JPS63205835A (en) * | 1987-02-23 | 1988-08-25 | Canon Inc | Magneto-optical recording medium and magneto-optical recording method |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CA2073311C (en) | Magneto-optical recording medium whereon recording is carried out with an overwriting function | |
| JP2910250B2 (en) | Magneto-optical recording medium | |
| JP3072812B2 (en) | Magneto-optical recording medium and method of reproducing information from the medium | |
| US5204193A (en) | Recording magnetooptical recording medium | |
| JPH0235371B2 (en) | ||
| JPH05159387A (en) | Magneto-optical disk | |
| EP0782135A2 (en) | Magneto-optical recording medium and method for reproducing therefrom | |
| JPH06124500A (en) | Magneto-optical recording medium and reproducing method of the medium | |
| US4923765A (en) | Magneto-optical recording medium | |
| JPH056588A (en) | Magneto-optical recording medium and magneto-optical recording method | |
| JP3093340B2 (en) | Magneto-optical recording medium | |
| JP3184272B2 (en) | Magneto-optical recording method | |
| KR20010078359A (en) | Magneto-optical recording medium | |
| JPH04219642A (en) | Magneto-optical recording medium and method thereof | |
| JP2796602B2 (en) | Magneto-optical recording method | |
| JP2893089B2 (en) | Magneto-optical recording method | |
| JP2658512B2 (en) | Magneto-optical recording medium and magneto-optical recording method | |
| JP3538718B2 (en) | Magneto-optical recording medium | |
| JP3184273B2 (en) | Magneto-optical recording method | |
| JP2959646B2 (en) | Magneto-optical recording medium and magneto-optical recording method | |
| KR970010942B1 (en) | Optical recording medium | |
| JP3381960B2 (en) | Magneto-optical recording medium | |
| JP3000385B2 (en) | Magneto-optical recording method | |
| JP2565884B2 (en) | Magneto-optical storage element | |
| JP3071246B2 (en) | Magneto-optical recording method |