JP2543677B2 - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- Publication number
- JP2543677B2 JP2543677B2 JP61052841A JP5284186A JP2543677B2 JP 2543677 B2 JP2543677 B2 JP 2543677B2 JP 61052841 A JP61052841 A JP 61052841A JP 5284186 A JP5284186 A JP 5284186A JP 2543677 B2 JP2543677 B2 JP 2543677B2
- Authority
- JP
- Japan
- Prior art keywords
- magneto
- recording medium
- optical recording
- recording
- ratio
- 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.)
- Expired - Lifetime
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording 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
- G11B11/10—Recording 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
- G11B11/105—Recording 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
- G11B11/10582—Record carriers characterised by the selection of the material or by the structure or form
- G11B11/10586—Record carriers characterised by the selection of the material or by the structure or form characterised by the selection of the material
- G11B11/10589—Details
Landscapes
- Thin Magnetic Films (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、例えばレーザー光等の照射により、記録・
消去・再生が可能な光磁気記録媒体に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention is directed to recording / recording by irradiation with laser light or the like.
The present invention relates to an erasable / reproducible magneto-optical recording medium.
従来の光磁気記録媒体において、記録媒体として例え
ば、特開昭57−94948のように重希土類金属Tb,Dy,Gdの
うち1種類以上およびFeまたはCoのうち1種類以上で形
成された非晶質合金が用いられてきた。In a conventional magneto-optical recording medium, as a recording medium, for example, as disclosed in JP-A-57-94948, an amorphous material formed of one or more kinds of heavy rare earth metals Tb, Dy, Gd and one or more kinds of Fe or Co Quality alloys have been used.
レーザー光のスポツトで記録層を加熱しながら、外部
磁界を加え反転磁区を形成することにより記録し、記録
時より低パワーの直線偏光した上記レーザー光のスポツ
トを入射し、カー効果あるいはフアラデー効果を利用し
て再生を行なう、いわゆる光磁気記録方式に用いられる
記録媒体においては、少なくとも次の性質を満たすこと
が必要である。While heating the recording layer with laser light spots, an external magnetic field is applied to form inverted magnetic domains for recording, and the laser light spots of linearly polarized light with lower power than during recording are incident to produce the Kerr effect or Faraday effect. A recording medium used for so-called magneto-optical recording, which is reproduced by utilizing it, must satisfy at least the following properties.
1. 半導体レーザーで記録・消去を行なえる程度にキユ
リー温度が低く、通常の使用環境温度に比べて、キユリ
ー温度が充分高いこと。1. The Curie temperature is low enough to record and erase with a semiconductor laser, and the Curie temperature is sufficiently higher than the normal operating environment temperature.
2. 記録媒体が、多結晶であると生ずる粒界ノイズ、単
結晶であると生ずる製造の困難さを回避するため、記録
媒体が非晶質であること。この場合、結晶化温度がキユ
リー温度に比べて充分高いことが必要である。2. The recording medium should be amorphous in order to avoid grain boundary noise that occurs when the recording medium is polycrystalline and manufacturing difficulties that occur when the recording medium is single crystal. In this case, the crystallization temperature needs to be sufficiently higher than the Curie temperature.
3. 再生は、カー効果、ファラデー効果を利用するた
め、カー回転角、ファラデー回転角が大きいこと。3. Since the car effect and the Faraday effect are used for reproduction, the car rotation angle and the Faraday rotation angle are large.
4. 垂直磁化膜であること。4. Must be a perpendicular magnetic film.
そのため、上記のような重希土類金属−遷移金属非晶
質合金が記録層として用いられてきた。Therefore, the heavy rare earth metal-transition metal amorphous alloy as described above has been used as the recording layer.
しかし、光磁気記録媒体として用いられる重希土類−
遷移金属非晶質合金には、次のような欠点がある。However, heavy rare earths used as magneto-optical recording media
The transition metal amorphous alloy has the following drawbacks.
1. 室温でのみかけ上の磁化が消失する補償組成付近で
重希土類金属と遷移金属は金属間化合物を作りやすい。
これらの金属間化合物は割れやすいため、合金ターゲツ
トを作製するには、特殊な技術が必要である。1. Heavy rare earth metals and transition metals tend to form intermetallic compounds near the compensating composition where the apparent magnetization disappears at room temperature.
Since these intermetallic compounds are easily cracked, a special technique is required to produce an alloy target.
2. 補償組成より遷移金属が多い領域では、遷移金属中
のCoを増加することにより、カー回転角、フアラデー回
点角を増大することができる。しかし、FeをCoで置換す
ることにより、キユリー温度が高くなるため、記録・消
去時に必要な熱エネルギーが大きくなつてしまう。2. In the region where the amount of transition metal is larger than that of the compensating composition, the Kerr rotation angle and the Faraday turning point angle can be increased by increasing Co in the transition metal. However, replacing Fe with Co raises the Curie temperature, which increases the thermal energy required for recording and erasing.
3. 希土類−遷移金属非晶質合金は酸化されやすい。3. Rare earth-transition metal amorphous alloys are easily oxidized.
そこで、本発明はこのような問題点を解決するもの
で、その目的とするところは均一な組成の膜を作製しや
すくする合金ターゲツトの作製を可能にし、記録・消去
特性を向上させかつ、長期間にわたる光磁気特性の安定
性を向上させ、従来のものと比べて安価で高性能な光磁
気記録媒体を提供することにある。Therefore, the present invention solves such a problem, and its purpose is to enable the production of an alloy target that facilitates the production of a film having a uniform composition, improve the recording / erasing characteristics, and An object of the present invention is to provide a magneto-optical recording medium which improves the stability of magneto-optical characteristics over a period of time and is cheaper and has higher performance than conventional ones.
本発明の光磁気記録媒体は、 Nd、Sm、Pr、Ceより少なくとも1種選ばれた軽希土類
金属(LR)と、 Tb、Dy、Gdより少なくとも1種選ばれた重希土類金属
(HR)と、 Fe及びCo、もしくはFe及びCo及びNiからなる強磁性体
遷移金属(TM)と、 を含んでなる光磁気記録媒体において、 前記3元系金属に加え、さらにCr及びAl及びTiからな
る不動態形成金属(A)を添加してなることを特徴とす
る。The magneto-optical recording medium of the present invention comprises a light rare earth metal (LR) selected from at least one selected from Nd, Sm, Pr and Ce, and a heavy rare earth metal (HR) selected from at least one selected from Tb, Dy and Gd. In a magneto-optical recording medium containing a ferromagnetic transition metal (TM) consisting of Fe, Co and Fe, or Fe and Co and Ni, in addition to the ternary metal, a non-magnetic layer consisting of Cr, Al and Ti. It is characterized in that a kinetics forming metal (A) is added.
さらに、 前記LR対HRの比は、0.25対0.75であり、 前記TMのうち、Fe対CoまたはFe対Niの比は、0.55対0.
45であり、 前記(LR+HR)対TM対Aの比は、0.23対0.72対0.005
であることを特徴とする。Further, the ratio of LR to HR is 0.25 to 0.75, and the ratio of Fe to Co or Fe to Ni of the TM is 0.55 to 0.
45, and the ratio of (LR + HR) to TM to A was 0.23 to 0.72 to 0.005.
It is characterized by being.
以下、本発明の実施例について説明する。なお、本発
明の記録媒体は、低周波溶解炉で溶解し鋳造した後、直
径8インチ、厚さ4mmに成形したものをスパッタリング
用ターゲットとしたことにより、製造した。Examples of the present invention will be described below. The recording medium of the present invention was manufactured by melting and casting in a low-frequency melting furnace, and then forming a target having a diameter of 8 inches and a thickness of 4 mm as a sputtering target.
〔実施例1〕 本発明の実施例の合金ターゲット組成と試料番号の対
応表を表1に、記録層組成と試料番号の対応表を表2に
示す。なお、試料番号1が本発明の実施例であり、試料
番号2〜4は、比較例である。[Example 1] Table 1 shows a correspondence table of alloy target compositions and sample numbers of Examples of the present invention, and Table 2 shows a correspondence table of recording layer compositions and sample numbers. Sample number 1 is an example of the present invention, and sample numbers 2 to 4 are comparative examples.
表1、2からわかるように、合金ターゲツトからスパ
ツタリングで得られる光磁気記録媒体においては、希土
類金属が合金ターゲツトに含まれているよりも少なくな
るという傾向をもつ。但し、このような組成変化の程度
は、スパツタガスの種類、圧力、ターゲツトへの投入電
力、ターゲツト、基板間距離によつても変わる。表2に
示した記録層の作製条件は、到達真空度1×10-6Torr以
下、スパツタガスはArで、Arガス圧1m Torr,DCスパツタ
法を用い、ターゲツトへの投入電力は約400Wであつた。
また、ターゲツト基体間距離は基体中心とターゲツト中
心の距離ではかつて10cmであつた。 As can be seen from Tables 1 and 2, in the magneto-optical recording medium obtained by sputtering from the alloy target, there is a tendency that the rare earth metal is less than that contained in the alloy target. However, the degree of such composition change also changes depending on the type of the spatula gas, the pressure, the power applied to the target, the target, and the distance between the substrates. The recording layer shown in Table 2 was prepared under the conditions that the ultimate vacuum was 1 × 10 −6 Torr or less, the sputtering gas was Ar, the Ar gas pressure was 1 m Torr, the DC sputtering method was used, and the input power to the target was about 400 W. It was
Further, the distance between target substrates was 10 cm in the distance between the center of the substrate and the center of the target.
なお、本実施例1で作製した合金ターゲツトの酸素濃
度は重量比で0.05%以下であり、焼結体に比べてはるか
に小さい。The oxygen concentration of the alloy target produced in Example 1 is 0.05% or less by weight, which is far smaller than that of the sintered body.
第1図に、ガラス基体上に、(Nd0.25Dy0.75)0.28
(Fe0.55Co0.45)0.72−z(Cr,Ti,Al)zを約2000Å形
成し、その上に保護層としてAlを約1000Å形成したもの
について基体側から光を入射した場合のカー回転角とz
の関係を示す。入射光の波長は7800Åである。Fig. 1 shows that (Nd 0.25 Dy 0.75 ) 0.28 on a glass substrate.
(Fe0.55Co0.45) 0.72-z (Cr, Ti, Al) z about 2000Å formed and Al about 1000Å formed as a protective layer on it, Kerr rotation angle when light enters from the substrate side And z
Shows the relationship. The wavelength of incident light is 7800Å.
Ti,Alにおいてはzが0.05より小さければ、カー回転
角の低下はみられないが、Crにおいては低下してしま
う。In Ti and Al, if z is smaller than 0.05, the Kerr rotation angle does not decrease, but in Cr, it decreases.
〔実施例2〕 第2図は、実施例1表2に示した試料番号1,2,3をガ
ラス基体上に約500Åをそれぞれ形成したものと、Tb0.2
0(Fe0.90Co0.10)0.80を約500Å形成したものについ
て、60℃,90%RHに保つた時間とフアラデー回転角を初
期値で規格化したものとの関係を示したものである。保
護膜はつけていない。明らかに、Cr,Ti,Alの添加によ
り、耐食性が向上している。これらの元素は、原子比で
5%程度の添加で効果がある。比較実験で示したよう
に、この程度の添加では、カー回転角の大幅な低下はみ
られていない。従つて、これらの元素を原子比で5%程
度添加することにより光磁気特性を劣化させずに耐食性
をあげることができた。[Embodiment 2] FIG. 2 shows that the sample Nos. 1, 2, and 3 shown in Table 2 of Embodiment 1 were each formed on a glass substrate to a thickness of about 500 Å, and Tb0.2
About 0 (Fe0.90Co0.10) 0.80 formed about 500Å, the relationship between the time of keeping at 60 ℃ and 90% RH and the standardized Faraday rotation angle is shown. No protective film is attached. Apparently, the corrosion resistance is improved by adding Cr, Ti and Al. These elements are effective when added at an atomic ratio of about 5%. As shown in the comparative experiment, with this amount of addition, the Kerr rotation angle was not significantly reduced. Therefore, by adding these elements in an atomic ratio of about 5%, it was possible to improve the corrosion resistance without deteriorating the magneto-optical characteristics.
〔実施例3〕 表2に示した資料番号1、2、3の光磁気記録媒体の
記録・再生特性を調べるために、溝付きポリカーボネイ
ト基体上に約500Åそれぞれ形成し、その上に窒化アル
ミニウムを約1000Å形成し、その上に窒化アルミニウム
を約1000Å形成し、さらにその上にアルミニウムを約50
0Å形成した。第3図に記録・再生特性評価に用いた光
磁気記録媒体の構成を示す。再生信号は光磁気記録媒体
の反射光から得、次のような条件で記録・再生を行なつ
た。[Example 3] In order to investigate the recording / reproducing characteristics of the magneto-optical recording media of Material Nos. 1, 2, and 3 shown in Table 2, about 500 Å each was formed on a grooved polycarbonate substrate, and aluminum nitride was formed thereon. About 1000Å is formed, aluminum nitride is formed on it about 1000Å, and aluminum is further formed on it about 50Å
0 Å formed. FIG. 3 shows the structure of a magneto-optical recording medium used for recording / reproducing characteristic evaluation. The reproduction signal was obtained from the reflected light of the magneto-optical recording medium, and recording / reproduction was performed under the following conditions.
溝間記録、再生パワー1mW,記録磁界600Oe,線速毎秒4.
7m,記録周波数1MHz,バンド幅30KHzである。Groove recording, reproduction power 1 mW, recording magnetic field 600 Oe, linear velocity 4.
7m, recording frequency 1MHz, bandwidth 30KHz.
第4図に本発明の光磁気記録媒体の再生時のC/N比お
よび2次高調波抑圧比と記録レーザーパワーとの関係を
示す。記録層だけを厚さ約500ÅのTb0.20(Fe0.90Co0.1
0)0.80に変えた場合の第4図と同様の図が第5図であ
る。FIG. 4 shows the relationship between the recording laser power and the C / N ratio and the second harmonic suppression ratio during reproduction of the magneto-optical recording medium of the present invention. Tb0.20 (Fe0.90Co0.1) with a thickness of about 500Å
0) FIG. 5 is a view similar to FIG. 4 when changed to 0.80.
表3が本発明の光磁気記録媒体と前記Tb0.20(Fe0.90
Co0.10)0.80を用いた情報記録媒体を用いた光磁気記録
媒体における記録・再生特性評価の結果をまとめたもの
である。試料番号1〜3までは、表1,2と対応してい
る。試料番号4は前記Tb0.20(Fe0.90Co0.10)0.80を示
す。Table 3 shows the magneto-optical recording medium of the present invention and the Tb0.20 (Fe0.90).
This is a summary of the results of the recording / reproducing characteristic evaluation of the magneto-optical recording medium using the information recording medium using Co0.10) 0.80. Sample numbers 1 to 3 correspond to Tables 1 and 2. Sample No. 4 shows the above Tb0.20 (Fe0.90Co0.10) 0.80.
表3中の最適記録パワーは2次高調波抑圧比が最も小
さくなる記録パワーと定義し、C/N比は最適記録パワー
で記録したものを再生したときの値を示した。最適記録
パワーは、静的に測定したキユリー温度Tcとほぼ対応し
Tcの大きいものは記録パワーが大きい。 The optimum recording power in Table 3 is defined as the recording power at which the second harmonic suppression ratio is the smallest, and the C / N ratio is the value when the data recorded with the optimum recording power is reproduced. The optimum recording power corresponds roughly to the statically measured Kyuriy temperature Tc.
The recording power is large when the Tc is large.
このように本発明の光磁気記録媒体においては、むや
みに記録パワーをあげることなく、高いC/N比を得るこ
とができる。As described above, in the magneto-optical recording medium of the present invention, a high C / N ratio can be obtained without unnecessarily increasing the recording power.
以上述べてきたように、本発明の光磁気記録媒体によ
れば、割れにくい合金が作りやすくなるため、大面積の
合金ターゲツトを作れる。大面積の合金ターゲツトによ
れば、組成・膜厚の均一化をはかれるため量産に適する
という効果を有する。As described above, according to the magneto-optical recording medium of the present invention, it is easy to form an alloy that is not easily broken, and thus an alloy target having a large area can be formed. A large-area alloy target has an effect of being suitable for mass production because the composition and film thickness can be made uniform.
また、遷移金属中のCo濃度を増すことによりカー回転
角、フアラデー回転角を増大できるが、本発明の光磁気
記録媒体では、キユリー温度があまり高くならないた
め、最適記録・消去パワーがあまり大きくならないです
むという効果も有する。Further, the Kerr rotation angle and the Faraday rotation angle can be increased by increasing the Co concentration in the transition metal, but in the magneto-optical recording medium of the present invention, the Curie temperature does not become so high that the optimum recording / erasing power does not become too large. It also has the effect of
さらに、不動態形成金属Ti,Cr,Alも含むため耐食性も
向上できるという効果も有する。Further, since it also contains passivation forming metals Ti, Cr, and Al, it also has an effect that corrosion resistance can be improved.
第1図 (Nd0.25Dy0.75)0.30(Fe0.55Co0.45)
0.70−z(Cr、Ti、Al)zのカー回転角とzの関係を示
す図 第2図 本発明における光磁気記録媒体およびTb0.20
(Fe0.90Co0.10)0.80を60℃,90%RHに保つた時間と初
期値で規格化したフアラデー回転角の関係を示す図 第3図 記録・再生特性評価に用いた光磁気記録媒体の
構成を示す図 1……ポリカーボネイト 2……窒化アルミニウム 3……本発明の光磁気記録媒体またはTbFeCo 4……窒化アルミニウム 5……アルミニウム 第4図 本発明の(Nd0.25Dy0.75)0.23(Fe0.55Co0.4
5)0.72(Cr0.2Al0.4Ti0.4)0.05の記録パワーとC/N比
との関係を示す図 第5図 従来例のTb0.20(Fe0.80Co0.10)0.80の記録パ
ワーとC/N比との関係を示す図Fig. 1 (Nd 0.25 Dy 0.75 ) 0.30 (Fe 0.55 Co 0.45 )
0.70-z (Cr, Ti, Al) z magneto-optical recording medium shown in FIG. FIG. 2 the present invention showing the relationship between the Kerr rotation angle and z of and Tb0.20
Fig. 3 shows the relationship between the Faraday rotation angle standardized by the initial value and the time when (Fe0.90Co0.10) 0.80 was kept at 60 ° C, 90% RH. Fig. 3 The magneto-optical recording medium used for recording / reproducing characteristics evaluation FIG. 1 shows the structure 1 ... Polycarbonate 2 ... Aluminum nitride 3 ... Magneto-optical recording medium of the present invention or TbFeCo 4 ... Aluminum nitride 5 ... Aluminum FIG. 4 (Nd0.25Dy0.75) 0.23 (Fe0 of the present invention .55Co0.4
5) A graph showing the relationship between the recording power of 0.72 (Cr0.2Al0.4Ti0.4) 0.05 and the C / N ratio. Fig. 5 Recording power and C / N of Tb0.20 (Fe0.80Co0.10) 0.80 of the conventional example. Diagram showing the relationship with N ratio
───────────────────────────────────────────────────── フロントページの続き (72)発明者 根橋 聡 諏訪市大和3丁目3番5号 セイコーエ プソン株式会社内 (72)発明者 青山 明 諏訪市大和3丁目3番5号 セイコーエ プソン株式会社内 (72)発明者 杉本 守 諏訪市大和3丁目3番5号 セイコーエ プソン株式会社内 (56)参考文献 特開 昭61−22608(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Satoshi Nebashi 3-3-5 Yamato, Suwa-shi Seiko Epson Corporation (72) Inventor Akira Aoyama 3-3-5 Yamato, Suwa-shi Seiko Epson Corporation ( 72) Inventor Mamoru Sugimoto 3-3-5 Yamato, Suwa-shi, Seiko Epson Corporation (56) References JP 61-22608 (JP, A)
Claims (2)
た軽希土類金属(LR)と、 Tb、Dy、Gdより少なくとも1種選ばれた重希土類金属
(HR)と、 Fe及びCo、若しくはFe及びCo及びNiからなる強磁性体遷
移金属(TM)と、 を含んでなる光磁気記録媒体において、 前記3元系金属に加え、さらにCr及びAl及びTiからなる
不動態形成金属(A)を添加してなることを特徴とする
光磁気記録媒体。1. A light rare earth metal (LR) selected from at least one selected from Nd, Sm, Pr and Ce, a heavy rare earth metal (HR) selected from at least one selected from Tb, Dy and Gd, and Fe and Co. Or a ferromagnetic transition metal (TM) composed of Fe, Co and Ni, and a passivation forming metal (Cr), Al and Ti (in addition to the ternary metal). A magneto-optical recording medium containing A).
であり、 前記(LR+HR)対TM対Aの比は、0.23対0.72対0.005で
あることを特徴とする特許請求の範囲第1項記載の光磁
気記録媒体。2. The ratio of LR to HR is 0.25 to 0.75, and the ratio of Fe to Co or Fe to Ni of the TM is 0.55 to 0.45.
The magneto-optical recording medium according to claim 1, wherein the ratio of (LR + HR) to TM to A is 0.23: 0.72: 0.005.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61052841A JP2543677B2 (en) | 1986-03-11 | 1986-03-11 | Magneto-optical recording medium |
NL8602167A NL8602167A (en) | 1985-08-26 | 1986-08-26 | Magneto=optical recording medium - with layer alloy of light and heavy rare earth metals, transition metal and chromium, titanium, aluminium or copper |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61052841A JP2543677B2 (en) | 1986-03-11 | 1986-03-11 | Magneto-optical recording medium |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS62209748A JPS62209748A (en) | 1987-09-14 |
JP2543677B2 true JP2543677B2 (en) | 1996-10-16 |
Family
ID=12926071
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61052841A Expired - Lifetime JP2543677B2 (en) | 1985-08-26 | 1986-03-11 | Magneto-optical recording medium |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2543677B2 (en) |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6122608A (en) * | 1984-07-11 | 1986-01-31 | Hitachi Ltd | Photomagnetic recording material |
-
1986
- 1986-03-11 JP JP61052841A patent/JP2543677B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPS62209748A (en) | 1987-09-14 |
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