JPS60209946A - Optomagnetic recording medium - Google Patents

Optomagnetic recording medium

Info

Publication number
JPS60209946A
JPS60209946A JP59065552A JP6555284A JPS60209946A JP S60209946 A JPS60209946 A JP S60209946A JP 59065552 A JP59065552 A JP 59065552A JP 6555284 A JP6555284 A JP 6555284A JP S60209946 A JPS60209946 A JP S60209946A
Authority
JP
Japan
Prior art keywords
layer
refractive index
magneto
recording layer
optical recording
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP59065552A
Other languages
Japanese (ja)
Inventor
Mitsuya Okada
満哉 岡田
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.)
NEC Corp
Original Assignee
NEC Corp
Nippon Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP59065552A priority Critical patent/JPS60209946A/en
Publication of JPS60209946A publication Critical patent/JPS60209946A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10582Record carriers characterised by the selection of the material or by the structure or form
    • G11B11/10586Record carriers characterised by the selection of the material or by the structure or form characterised by the selection of the material
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing

Abstract

PURPOSE:To increase considerably the rotating angle of the plane of polarization of a recording layer and to improve the S/N ratio of a reproduction signal by using silicon as a high-refractive index interference layer. CONSTITUTION:A high-refractive index interference layer 3, an optomagnetic recording layer 2 and a reflecting layer 5 are provided on a transparent substrate 4. A glassy org. resin (polymethyl methacrylate, polycarbonate, polyvinyl chloride, etc.) is used as the substrate 4. Silicon (Si) (refractive index n=2.5) is used as the lyer 3. More specifically, the rotation of the plane of polarization is further increased by using Si in addition to the increase in the rotation of the plane of polarization with the structure of the reflected film.

Description

【発明の詳細な説明】 (座業上の利用分野) 本発明はレーザ光を用いて情報の記録・再生・消去をお
こなう光磁気記録媒体に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of sedentary use) The present invention relates to a magneto-optical recording medium that records, reproduces and erases information using laser light.

(従来技術とその問題点) 光磁気記録媒体は書き替えのできる光デイスクメモリ用
媒体である。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u−?−m −+ M
t’Ma d 、−t hJ −r−II Ifl−P
# 7&4ffl j Jモリと考えられている。中で
も光磁気記録媒体を用いた光磁気ディスクは書き替え性
を有することから最も注目され、近年活発に研究開発が
おこなわれて1.いる。
(Prior art and its problems) A magneto-optical recording medium is a rewritable optical disk memory medium. Does optical disk memory have high density, large capacity, and high speed access? −m −+ M
t'Ma d, -t hJ -r-II Ifl-P
#7&4ffl j It is considered to be J Mori. Among them, magneto-optical disks using magneto-optical recording media have attracted the most attention due to their rewritability, and have been actively researched and developed in recent years.1. There is.

従来よシ知られている光磁気記録媒体の構成は第1図に
示したように支持基板1としてガラス。
The configuration of a conventionally known magneto-optical recording medium is as shown in FIG. 1, in which a support substrate 1 is made of glass.

金属あるいは有機物樹脂を用い、支持基板1上に基板に
対して垂直方向に磁化を有する垂直磁化膜から成る光磁
気記録層2を形成したものである。。
A magneto-optical recording layer 2 made of a perpendicular magnetization film having magnetization in a direction perpendicular to the substrate is formed on a support substrate 1 using metal or organic resin. .

光磁気記録層としてはMnB1 、 MnCuB1 +
 PtCo 。
As the magneto-optical recording layer, MnB1, MnCuB1 +
PtCo.

MnAtGe等の結晶体+ Gds Tb、 Dy、 
Ho等希土類とFe、 Coo Ni等遷移金属とを種
々の組成で混合して作製したアモルファス磁性薄膜が知
られている。
Crystals such as MnAtGe + Gds Tb, Dy,
Amorphous magnetic thin films made by mixing rare earth elements such as Ho and transition metals such as Fe and Coo Ni in various compositions are known.

光磁気記録媒体は前記のとおシ磁気ディスクメモリに代
わる利点を有している反面、再生信号レベルすなわち8
7N比が低いという欠点がおる。特に光磁気記録媒体か
らの反射光を用いて再生をおこなうカー効果による再生
方式においては、媒体のカー同級角カニ/11愼込とシ
カE(丘S/N田の原田〒ありた。
Magneto-optical recording media have the above-mentioned advantages in place of magnetic disk memories, but on the other hand, the playback signal level, that is, 8.
It has the disadvantage of a low 7N ratio. In particular, in the reproduction method based on the Kerr effect, in which reproduction is performed using reflected light from a magneto-optical recording medium, there were two types of media: Kerr's class of Kani/11 and Shika E (Oka S/N's Harada).

従来より再生信号のS/N比を向上させる方法として、
記録層の改良すなわち光磁気記録層を多元系にするある
いは他元素を添加する方法や、記録媒体のレーザ光入射
面に高屈折率干渉層を形成しして反射光を減少させ、カ
ー回転角を増大させるカー回転増幅法が用いられている
As a conventional method of improving the S/N ratio of the reproduced signal,
Improving the recording layer, that is, making the magneto-optical recording layer multi-component or adding other elements, and forming a high refractive index interference layer on the laser beam incidence surface of the recording medium to reduce reflected light and improve the Kerr rotation angle. A Kerr rotation amplification method is used to increase the .

このうち後者のカー回転増幅法に関しては、第2図に示
したように支持基板lの上に光磁気記録層2を形成し、
さらに前記記録層2の上にSIOあるいはsio、の高
屈折率干渉層3を形成した媒体が知られている。しかし
ながらこの媒体においては、前記記録層2が酸化しやす
い場合には、前記高屈折率干渉層3に用いる5iO9S
iO,中の酸素が前記記録層2の表面で酸化物を形成し
、記録層のカー回転角が経時変化を受け低下するという
欠点がある。また前記高屈折率干渉層3上に付着する小
さなごみ、#1こり、汚れは記録層に集光されるレーザ
ー光の合焦点位置近傍に存在するため、信号・再生時の
雑音源になるという欠点がある。
Regarding the latter Kerr rotation amplification method, a magneto-optical recording layer 2 is formed on a support substrate l as shown in FIG.
Further, a medium is known in which a high refractive index interference layer 3 of SIO or sio is formed on the recording layer 2. However, in this medium, when the recording layer 2 is easily oxidized, the 5iO9S used for the high refractive index interference layer 3 is
The disadvantage is that the oxygen in iO forms an oxide on the surface of the recording layer 2, and the Kerr rotation angle of the recording layer decreases over time. In addition, small dust, #1 dust, and dirt that adhere to the high refractive index interference layer 3 are present near the focal point of the laser beam focused on the recording layer, so they become a source of noise during signal/reproduction. There are drawbacks.

(発明の目的) 本発明はこのような従来の欠点を除去せしめて、作製が
容易で記録層の耐蝕性・耐酸化性に優れ、かつ小さなご
みや汚れの影響を無視でき、さらにはカー回転角を増幅
できる機能を有し、優れた再生信号S/N比が得られる
新規な光磁気記録媒体を提供することにある。
(Objective of the Invention) The present invention eliminates these conventional drawbacks, provides a recording layer that is easy to produce, has excellent corrosion resistance and oxidation resistance, can ignore the effects of small dust and dirt, and further improves Kerr rotation. It is an object of the present invention to provide a novel magneto-optical recording medium which has a function of amplifying the angle and can obtain an excellent reproduced signal S/N ratio.

(発明の構成) 本発明によれば、透明基板上に高屈折率干渉層を設け、
前記高屈折率干渉層の上に光磁気記録層を設け、前記光
磁気記録層の上に反射層を設けた光磁気記録媒体におい
て、前記高屈折率干渉層としてケイ素を用いることを特
徴とする光磁気記録媒体が得られる。
(Structure of the Invention) According to the present invention, a high refractive index interference layer is provided on a transparent substrate,
A magneto-optical recording medium in which a magneto-optical recording layer is provided on the high refractive index interference layer and a reflective layer is provided on the magneto-optical recording layer, characterized in that silicon is used as the high refractive index interference layer. A magneto-optical recording medium is obtained.

(構成の詳細な説明) 本発明は上述の構成をとることにょ夛従来技術の問題点
を解決した。まず、媒体支持基板として透明基板を用い
ることにょシ、信号の記録再生消去用レーザー光を基板
側から記録層に入射させる方式が採用できる。この方式
によれば、表面基板表面ではレーザー光は未集光状態で
あるため、透明基板表面に付着する小さなごみ、はこシ
、汚れは記録・再生・消去性能にはとんど影響しない。
(Detailed Description of Configuration) The present invention solves the problems of the prior art by employing the above-mentioned configuration. First, when a transparent substrate is used as the medium support substrate, a method can be adopted in which laser light for recording, reproducing, and erasing signals is made incident on the recording layer from the substrate side. According to this method, since the laser beam is not focused on the surface of the front substrate, small dust, chips, and dirt that adhere to the surface of the transparent substrate have almost no effect on recording, reproducing, and erasing performance.

本発明の特徴は高屈折率干渉層としてケイ素(St)を
用いることである。StはSin、 5i02に比べて
屈折率が大きく、それ故にカー回転角増幅効果も大きい
。また、Stは半導体レーザー波長780〜830 n
mでは吸収がない。さらには、干渉層が酸化物でないた
めに、干渉層と光磁気記録層との界面に記録層物質の酸
化物が形成されることがない。酸化層の形成は記録!−
の特性特にカー回転角の低下につなが少記録媒体の性能
を劣化させる。
A feature of the present invention is the use of silicon (St) as a high refractive index interference layer. St has a larger refractive index than Sin and 5i02, and therefore has a larger Kerr rotation angle amplification effect. In addition, St is a semiconductor laser wavelength of 780 to 830 n
There is no absorption at m. Furthermore, since the interference layer is not an oxide, no oxide of the recording layer material is formed at the interface between the interference layer and the magneto-optical recording layer. Record the formation of oxide layer! −
This leads to a decrease in the characteristics, especially the Kerr rotation angle, which deteriorates the performance of the recording medium.

光磁気記録層は記録再生消去に用いるレーザー光の一部
が透過する厚さに設定される。これによシ、再生レーザ
ー光は記録層表面で受けるカー回転と、記録層の往復に
よって受けるファラデー回転によってよシ大きな偏光面
回転を持りて反射される。記録層上部に設けた反射層は
記録層を透過した光を反射させる役割とともに、記録層
上部側からの記録層劣化を防ぐ保護層の役割を持つ。
The magneto-optical recording layer is set to have a thickness that allows a portion of laser light used for recording, reproduction, and erasure to pass through. As a result, the reproduction laser beam is reflected with a large polarization plane rotation due to the Kerr rotation received on the surface of the recording layer and the Faraday rotation received as the recording layer moves back and forth. The reflective layer provided above the recording layer has the role of reflecting light that has passed through the recording layer, and also has the role of a protective layer that prevents the recording layer from deteriorating from the upper side of the recording layer.

(実施例) 第3図は本発明の適用された光磁気記録媒体の一実施例
の断面図であり透明基似4の上部に尚屈折率干渉層3さ
らに光磁気記録層2さらに反射層5を有する。透明基板
4としてはガラス有機物樹脂(ポリメチルメタクリレー
ト、ポリカーボネート、ポリ塩化ビニル等)が用いられ
る。高屈折率干渉層3としてケイ素(St)(屈折率n
=2.5)を用いる。SiはSiO,5iO1に比べて
萬屈折率である。光磁気記録層2としてはMnB1 、
 MnCuB1 +P tCo + MnAtGe等の
結晶体あるいはGd、 Tb 、 Dy 。
(Embodiment) FIG. 3 is a cross-sectional view of an embodiment of a magneto-optical recording medium to which the present invention is applied. On top of a transparent substrate 4, a refractive index interference layer 3, a magneto-optical recording layer 2, and a reflective layer 5 are provided. has. As the transparent substrate 4, a glass organic resin (polymethyl methacrylate, polycarbonate, polyvinyl chloride, etc.) is used. Silicon (St) (refractive index n
=2.5) is used. Si has a refractive index of 1,000,000 compared to SiO and 5iO1. As the magneto-optical recording layer 2, MnB1,
Crystals such as MnCuB1 + P tCo + MnAtGe or Gd, Tb, Dy.

Ho等の希土類とFe 、 Co r Ni等の遷移金
属の徨々の組成から成るアモルファス磁性薄膜が用いら
れる。反射層5としては、AI−+ Cu + Cr 
+ Ag + Au等の金属が用いられる。記録・再生
に用いるレーザ光6は透明基板4側から入射し、記録層
2に情報の記録をおこない、記録層2ならびに反射層5
からの反射光によってカー回転角ならびにファラデー回
転角に基づく偏光面の回転から情報を再生する。ここで
記録層2の膜厚を再生に用いるレーザ光波長に対して部
分的に透過を可能とする厚さに設定することによシ再生
時の偏光面回転を大きくすることができ、たとえば透明
基板上に光磁気記録層t−200人厚に形成上、さらに
その上部に反射層を形成した構成では、反射層のない構
成に比べて偏光面回転は2倍になる。
An amorphous magnetic thin film composed of various compositions of rare earth elements such as Ho and transition metals such as Fe and CorNi is used. As the reflective layer 5, AI−+Cu+Cr
A metal such as +Ag+Au is used. Laser light 6 used for recording and reproduction enters from the side of transparent substrate 4, records information on recording layer 2, and records information on recording layer 2 and reflective layer 5.
Information is reproduced from the rotation of the plane of polarization based on the Kerr rotation angle and the Faraday rotation angle using the reflected light. By setting the film thickness of the recording layer 2 to a thickness that allows partial transmission of the wavelength of the laser light used for reproduction, the rotation of the polarization plane during reproduction can be increased, for example, transparent In a configuration in which a magneto-optical recording layer is formed on a substrate to a thickness of t-200 mm and a reflective layer is further formed on top of the layer, the rotation of the plane of polarization is twice that of a configuration without a reflective layer.

本発明の一実施例である第3図に示した光磁気記録媒体
の特徴は、上記の反射膜構造による偏光面回転増大に加
えて、Slを用いることによってさらに偏光面回転を増
幅しようとすることである。
The feature of the magneto-optical recording medium shown in FIG. 3, which is an embodiment of the present invention, is that in addition to increasing the polarization plane rotation by the above-mentioned reflective film structure, the polarization plane rotation is further amplified by using Sl. That's true.

第3図に示した冒屈折率干渉層3の膜厚によって偏光面
回転増幅効果は変化し、また再生時に用いるレーザー光
の波長によっても異なる。しかしながら高屈折率干渉層
の屈折率が大きいものほど、偏光面回転の増幅率は大き
い。たとえば、高屈折率干渉層3として5i(n=2.
5)i用いた場合と5iO(n=1.9)t−用いた場
合では、Skの場合のほうが、偏光面回転の増幅率は大
きく、最大5倍に達する。
The polarization plane rotation amplification effect changes depending on the film thickness of the refractive index interference layer 3 shown in FIG. 3, and also changes depending on the wavelength of the laser beam used during reproduction. However, the higher the refractive index of the high refractive index interference layer, the higher the amplification factor of polarization plane rotation. For example, as the high refractive index interference layer 3, 5i (n=2.
5) In the case of using i and the case of using 5iO (n=1.9)t-, the amplification factor of the polarization plane rotation is larger in the case of Sk, reaching a maximum of 5 times.

透明基板としてガラスを用い、厚さ600^のSi。Glass is used as a transparent substrate, and Si is 600^ thick.

厚す200A(7)GdTbFs J[、厚す1000
AOAui[’i連続してスバ、り法によシ作成した本
発明に係る光磁気記録媒体においては、波長830 n
mでのカー回転角及びファラデー回転角に基づく偏光面
回転はGdTbF・膜のみの場合の10倍に達し、Si
を用いた高屈折率干渉層と、反射膜構造両者の効果によ
シ偏九面回転が大幅に増大される。
Thickness 200A (7) GdTbFs J[, Thickness 1000A
In the magneto-optical recording medium according to the present invention produced by the AOAui['i continuous process, the wavelength is 830 nm.
The polarization plane rotation based on the Kerr rotation angle and Faraday rotation angle at
The nine-plane rotation is greatly increased by the effects of both the high refractive index interference layer and the reflective film structure.

一般に光磁気記録においては、再生信号のS/N比は偏
光面回転角を09反射率をRとしたとき8/N oc 
θ・【− であることが知られている。前記本発明の一実施例にお
いては反射率RはGdTbFe膜のみの場合に比べて−
に低下しているにすぎず、S/N比は本発明によ93.
3倍改善されることがわかる。
In general, in magneto-optical recording, the S/N ratio of the reproduced signal is 8/Noc, where the polarization plane rotation angle is 09 and the reflectance is R.
It is known that θ・[−. In the embodiment of the present invention, the reflectance R is - compared to the case of using only the GdTbFe film.
However, the S/N ratio is only 93.
It can be seen that this is improved by 3 times.

次に、記録層の耐蝕性、耐酸化性については、記録層が
高屈折率干渉層と、反射層間に配置されているために、
完全に大気に対して遮蔽筋れていること、及び高屈折率
干渉層9反射層共に酸化物でないことさらには各層が高
真空中で連続して作製されるので各層の界面が大気にさ
らされないことから記録層が比較的薄いにもかかわらず
、記録層の経時変化、特性の劣化はみられない。
Next, regarding the corrosion resistance and oxidation resistance of the recording layer, since the recording layer is arranged between the high refractive index interference layer and the reflective layer,
It is completely shielded from the atmosphere, and both the high refractive index interference layer 9 and the reflective layer are not made of oxide.Furthermore, each layer is manufactured in succession in a high vacuum, so the interface between each layer is not exposed to the atmosphere. Therefore, although the recording layer is relatively thin, no change in the recording layer over time or deterioration of the characteristics is observed.

(発明の効果) 本発明は簡単な構成であシながら、記録層の偏光面回転
角を大幅に増大させて再生信号S/N比を改善すること
ができる。さらに記録層を高屈折率干渉層と反射層では
さみ込んだ構造にし、酸化物でないSii電体層と金属
反射膜を用いることによって耐蝕性、耐酸化性の向上が
可能である。St誘電体層は特に基板として浸水性のあ
る有機物樹脂を使用するときに基板と記録層間の保護層
となり、効果を発揮する。
(Effects of the Invention) Although the present invention has a simple configuration, it is possible to significantly increase the rotation angle of the polarization plane of the recording layer and improve the reproduced signal S/N ratio. Furthermore, corrosion resistance and oxidation resistance can be improved by forming a structure in which the recording layer is sandwiched between a high refractive index interference layer and a reflective layer, and by using a non-oxide Sii electric layer and a metal reflective film. The St dielectric layer serves as a protective layer between the substrate and the recording layer and is particularly effective when a water-permeable organic resin is used as the substrate.

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

第1図は従来の光磁気記録媒体の構成を示す断面図、第
2図は従来の高屈折率干渉層を有する光磁気記録媒体の
構成を示す断面図、第3図は本発明の一実施例の構成を
示す断面図である。 図中 1・・・支持基板、2・・・光磁気記録層、3・
・・高屈折率干渉層、4・・・透明基板、5・・・反射
層、6・・・レーザー光
FIG. 1 is a sectional view showing the structure of a conventional magneto-optical recording medium, FIG. 2 is a sectional view showing the structure of a conventional magneto-optical recording medium having a high refractive index interference layer, and FIG. 3 is an embodiment of the present invention. FIG. 3 is a cross-sectional view showing an example configuration. In the figure 1... Support substrate, 2... Magneto-optical recording layer, 3...
...High refractive index interference layer, 4...Transparent substrate, 5...Reflection layer, 6...Laser light

Claims (1)

【特許請求の範囲】[Claims] 透明基板上に高屈折率干渉層を設け、前記高屈折率干渉
層の上に光磁気記録層を設け、前記光磁気記録層の上に
反射層を設けた光磁気記録媒体において、前記高屈折率
干渉層としてケイ素を用いることを特徴とする光磁気記
録媒体。
In the magneto-optical recording medium, a high refractive index interference layer is provided on a transparent substrate, a magneto-optical recording layer is provided on the high refractive index interference layer, and a reflective layer is provided on the magneto-optical recording layer. 1. A magneto-optical recording medium characterized in that silicon is used as an index interference layer.
JP59065552A 1984-04-02 1984-04-02 Optomagnetic recording medium Pending JPS60209946A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59065552A JPS60209946A (en) 1984-04-02 1984-04-02 Optomagnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59065552A JPS60209946A (en) 1984-04-02 1984-04-02 Optomagnetic recording medium

Publications (1)

Publication Number Publication Date
JPS60209946A true JPS60209946A (en) 1985-10-22

Family

ID=13290282

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59065552A Pending JPS60209946A (en) 1984-04-02 1984-04-02 Optomagnetic recording medium

Country Status (1)

Country Link
JP (1) JPS60209946A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0296888A2 (en) * 1987-06-26 1988-12-28 Mitsubishi Kasei Corporation Magnetooptical recording media
JPS6466847A (en) * 1987-09-07 1989-03-13 Mitsubishi Chem Ind Magneto-optical recording medium

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60133558A (en) * 1983-12-21 1985-07-16 Nec Corp Photomagnetic recording medium
JPS60163247A (en) * 1984-02-06 1985-08-26 Ulvac Corp Photomagnetic recording medium

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60133558A (en) * 1983-12-21 1985-07-16 Nec Corp Photomagnetic recording medium
JPS60163247A (en) * 1984-02-06 1985-08-26 Ulvac Corp Photomagnetic recording medium

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0296888A2 (en) * 1987-06-26 1988-12-28 Mitsubishi Kasei Corporation Magnetooptical recording media
JPS6466847A (en) * 1987-09-07 1989-03-13 Mitsubishi Chem Ind Magneto-optical recording medium

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