JPS6190348A - Photomagnetic recording medium - Google Patents

Photomagnetic recording medium

Info

Publication number
JPS6190348A
JPS6190348A JP21132084A JP21132084A JPS6190348A JP S6190348 A JPS6190348 A JP S6190348A JP 21132084 A JP21132084 A JP 21132084A JP 21132084 A JP21132084 A JP 21132084A JP S6190348 A JPS6190348 A JP S6190348A
Authority
JP
Japan
Prior art keywords
film
recording medium
temp
amorphous
compensation
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
JP21132084A
Other languages
Japanese (ja)
Inventor
Shinji Takayama
高山 新司
Toshio Niihara
敏夫 新原
Katsuhiro Kaneko
金子 克弘
Ken Sugita
杉田 愃
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
Original Assignee
Hitachi 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 filed Critical Hitachi Ltd
Priority to JP21132084A priority Critical patent/JPS6190348A/en
Priority to DE19853536210 priority patent/DE3536210A1/en
Publication of JPS6190348A publication Critical patent/JPS6190348A/en
Priority to US07/294,941 priority patent/US4923765A/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
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03GELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
    • G03G5/00Recording members for original recording by exposure, e.g. to light, to heat, to electrons; Manufacture thereof; Selection of materials therefor
    • G03G5/16Layers for recording by changing the magnetic properties, e.g. for Curie-point-writing
    • 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
    • G11B11/10589Details
    • G11B11/10591Details for improving write-in properties, e.g. Curie-point temperature

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Thin Magnetic Films (AREA)

Abstract

PURPOSE:To decrease modulation noise and to increase a C/N value by specifying the Curie temp. and compensation temp. of an amorphous rare earth-ferrous photomagnetic recording medium having the axis of easy magnetization in the direction perpendicular to the film plane. CONSTITUTION:The amorphous ally film is manufactured by a sputtering method using a composite target disposed with a rare earth element and transition metallic element such as iron element so as to attain a prescribed compsn. in area ratio on a Co disk. The Curie temp. of the photomagnetic recording medium is specified to <=250 deg.C and the compensation temp. thereof <=0 deg.C. The following film characteristics are exhibited when, for example, the amorphous vertically magnetizable film consisting of Tb20Fe70.5Co9.5 compsn. is formed as the recording film: Curie temp. Tc=190-230 deg.C, compensation temp. Tcomp<=-50 deg.C, coercive force Hc=1-3kOe, satd. magnetization Ms=120-195 emu/cc, Kerr rotating angle thetaK(lambda=633nm)=0.31-0.35 deg.. The modulation noise is substantially eliminated and the high C/N value is obtd. even if the Kerr rotating angle is not apparently increased by multiple reflections in the interfer ence structure.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明はレーザ光を用いて情報の記録、再生。[Detailed description of the invention] [Field of application of the invention] The present invention uses laser light to record and reproduce information.

消去を行なう光磁気記録に係り、特に記B感度大で、再
生時の信号と雑音の比C/Nを向上するのに好適な、磁
気光学効果大の光磁気記録媒体に関する。
The present invention relates to magneto-optical recording for erasing, and particularly relates to a magneto-optical recording medium with high sensitivity and a large magneto-optic effect suitable for improving the signal-to-noise ratio C/N during reproduction.

〔発明の背景〕[Background of the invention]

最近、書き換え可能な光記録方式である光磁気記録の記
録材料として、比較的大きなカー回転角が得られる希土
類−鉄族系非晶質膜が注目を浴びている。これらの非晶
質膜の中でも、特に、カー回転角Okの大きい値が得ら
れるTb−Fe−G。
Recently, rare earth-iron group amorphous films have been attracting attention as recording materials for magneto-optical recording, which is a rewritable optical recording system, and can obtain a relatively large Kerr rotation angle. Among these amorphous films, Tb-Fe-G provides a particularly large Kerr rotation angle Ok.

非晶質膜の研究開発が活発化している。例えば、特開昭
58−73746等がその代表的なものである。しかし
これら合金系の非晶質膜も含めて。
Research and development of amorphous films is becoming more active. For example, Japanese Patent Laid-Open No. 58-73746 is a typical example. However, including these alloy-based amorphous films.

従来の非晶質膜では次の如き問題があった。Conventional amorphous films have the following problems.

(1)磁化が飽和した時のカー回転角は大きいが、残留
磁化でのカー回転角が小さいため再生信号が十分とれな
い。
(1) Although the Kerr rotation angle when magnetization is saturated is large, the Kerr rotation angle at residual magnetization is small, so a sufficient reproduction signal cannot be obtained.

(2)残留磁化でのカー回転角は比較的大きいが、キュ
リー温度が高すぎるため記録感度が悪く、そのため再生
信号が十分得られない。
(2) Although the Kerr rotation angle due to residual magnetization is relatively large, the Curie temperature is too high, so the recording sensitivity is poor, and therefore a sufficient reproduction signal cannot be obtained.

(3)残留磁化でのカー回転角は比較的大きく、キュリ
ー温度も比較的低いが、記録に際して、記録ドメインの
中心に書けない部分が生じるため変調ノイズが大き(な
ってしまい、その結果十分な再生時の信号と雑音の比C
/Nがとれない。
(3) Although the Kerr rotation angle for residual magnetization is relatively large and the Curie temperature is relatively low, during recording, there is a portion that cannot be written in the center of the recording domain, resulting in large modulation noise (as a result, sufficient Signal to noise ratio during playback C
/I can't get N.

〔発明の目的〕[Purpose of the invention]

本発明の目的は磁気光学効果が十分に大きく、高い再生
C/N比(あるいはS、/N比)が得られ、実用に好適
な非晶質光磁気記録材料を提供することにある。
An object of the present invention is to provide an amorphous magneto-optical recording material which has a sufficiently large magneto-optic effect, can obtain a high reproduction C/N ratio (or S,/N ratio), and is suitable for practical use.

〔発明の概要〕[Summary of the invention]

非晶質垂直磁化膜を実際に光磁気記録材料として用いる
場合、次の如きことが要請されるとみなされていた。
When an amorphous perpendicularly magnetized film is actually used as a magneto-optical recording material, the following requirements were considered to be required.

(1)  キュリー温度(Tc)は半導体レーザ光のパ
ワーの制限や、記録感度及び膜寿命の点で約250 ℃
以下であるのが望ましい。
(1) The Curie temperature (Tc) is approximately 250 °C due to limitations on the power of semiconductor laser light, recording sensitivity, and film life.
The following is desirable.

(2)  また保磁力(He)も記録情報の熱安定性の
点から約1koe以上であるのが望ましい。しかし本発
明者等は以上の要請のみではなく、キュリー温度以外に
補償温度(Tcomp)も、Tcとのかねあいで記録感
度、再生ノイズ等に大きく影響を及ぼすことを見い出し
た。
(2) It is also desirable that the coercive force (He) is about 1 koe or more in view of the thermal stability of recorded information. However, the present inventors have discovered that not only the above requirements but also the compensation temperature (Tcomp), in addition to the Curie temperature, has a great effect on recording sensitivity, reproduction noise, etc. due to the balance with Tc.

本発明の光磁気記録媒体は次の如き構成を有する。即ち
The magneto-optical recording medium of the present invention has the following configuration. That is.

膜面に垂直な方向に磁化容易軸を有し、実質的に非晶質
である希土類−鉄族系光磁気記録媒体において、当該非
晶質希土類−鉄族系光磁気媒体のキュリー温度が250
℃以下、補償温度が0℃以下になることを特徴とする。
In a rare earth-iron magneto-optical recording medium that has an axis of easy magnetization in a direction perpendicular to the film surface and is substantially amorphous, the Curie temperature of the amorphous rare earth-iron magneto-optical medium is 250.
℃ or less, the compensation temperature is 0℃ or less.

上記希土類−鉄族系光磁気記録媒体の二元系。A binary system of the rare earth metal-iron group magneto-optical recording medium.

三元系、或いは四元系材料の例としてはTb−Fe−C
o、 Tb −Fe、 Tb  Gd −Fe、 Tb
 −Sm −Go等が揚げられる。
Examples of ternary or quaternary materials include Tb-Fe-C
o, Tb-Fe, Tb Gd-Fe, Tb
-Sm-Go etc. are fried.

又、記録された情報が安定に存在するためにはごく一般
にはキュリー温度は100℃以上(より好ましくは15
0℃以上)となしている。
In addition, in order for recorded information to exist stably, the Curie temperature is generally 100°C or higher (more preferably 15°C).
0℃ or higher).

しかし、上記光磁気記録媒体のTcが250℃以下であ
っても、’I’compが室温附近にあると記録時に形
状均一な記録ドメインが形成されず、そのために高い変
調ノイズが生じ、再生時のC/ Nが低下してしまうこ
とがわかった。このことは記録時の飽和磁化の大きさと
その温度変化に大きく依存する。
However, even if the Tc of the above-mentioned magneto-optical recording medium is 250 degrees Celsius or lower, if 'I' comp is near room temperature, a recording domain with a uniform shape will not be formed during recording, resulting in high modulation noise, and during reproduction. It was found that the C/N of This greatly depends on the magnitude of saturation magnetization during recording and its temperature change.

変調ノイズが低く、高C/Nを得るために、記録膜の補
償温度は0℃以下、より好ましくは一50℃以下である
ことが好ましい。一般に、希土類−鉄族系元気記録媒体
においては、これらの温度範囲を満足する組成範囲は、
補償組成よりも鉄族系元素に富んだ組成に限られている
ことがわかった。その代表例として、第1図にTb−F
e−C。
In order to obtain low modulation noise and high C/N, the compensation temperature of the recording film is preferably 0° C. or lower, more preferably -50° C. or lower. In general, for rare earth-iron group energy recording media, the composition range that satisfies these temperature ranges is:
It was found that this is limited to compositions that are richer in iron group elements than the compensation composition. As a typical example, Fig. 1 shows Tb-F
e-C.

非晶質垂直磁化膜(TbxFel。。−〇−アCo、)
のキュリー温度Tcと補償温度T compの各Co濃
度に対するTbfi度依存性を示す。図に矢印で示した
のは補償組成のTb濃度を示す。図において、1の曲線
はy=30.4のTc、2はy=17.5のTc、3は
y=l lのTc、4はy=10.3のTc、5はy=
5のTc、6はy=30.4のT camp 、 7は
y=17.5のTcomp、 8はy:11のT co
mp 、 9はy=10.3のTcomp、 10はy
=5のT compを各々示している。図から、Co量
が増すに従い、Tcは上昇し、TcとTcompが一致
するTb濃度が高濃度側に移行していることがわかる。
Amorphous perpendicular magnetization film (TbxFel.-〇-A-Co,)
The Tbfi degree dependence of the Curie temperature Tc and the compensation temperature T comp on each Co concentration is shown. The arrow in the figure indicates the Tb concentration of the compensation composition. In the figure, curve 1 is Tc at y=30.4, curve 2 is Tc at y=17.5, curve 3 is Tc at y=l l, curve 4 is Tc at y=10.3, and curve 5 is Tc at y=17.5.
Tc of 5, 6 T camp of y=30.4, 7 Tcomp of y=17.5, 8 T co of y:11
mp, 9 is Tcomp of y=10.3, 10 is y
=5 T comp is shown in each case. The figure shows that as the amount of Co increases, Tc increases, and the Tb concentration, where Tc and Tcomp match, shifts to the high concentration side.

さて、上記でTcompが室温よりも低い組成は低Tb
′a度側組成(すなわち補償組成よりも鉄族元素に富ん
だ組成)であることがわかる。
Now, in the above composition where Tcomp is lower than room temperature, the composition is low Tb.
It can be seen that the composition is on the 'a degree side (that is, the composition is richer in iron group elements than the compensation composition).

従って、第1図の結果から、Tb  Fe  Co非晶
質垂直磁化膜の最適組成は、補償組成よりも鉄族元素に
富んだTb18〜21.5原子%、コバルト8〜tOE
C子%、残部が鉄元素から成る極めて狭い組成範囲であ
る必要がある。ここでカー回転角θ□が0.3°(λ”
633nm)以上の高い値を得るためにCo量の下限は
877X子%である。勿論、これら三元系に他の希土類
元素や遷移金属元素等の不純物元素を少量添加すること
により、さらに特性向上の最適化が可能であることは言
うまでもない。
Therefore, from the results shown in FIG. 1, the optimal composition of the Tb Fe Co amorphous perpendicularly magnetized film is 18 to 21.5 atomic % of Tb and 8 to tOE of Co, which are richer in iron group elements than the compensation composition.
It is necessary that the composition be within an extremely narrow composition range of % carbon and the balance consisting of iron element. Here, the Kerr rotation angle θ□ is 0.3° (λ”
In order to obtain a high value of 633 nm or higher, the lower limit of the Co content is 877X%. Of course, it is possible to further optimize the properties by adding small amounts of impurity elements such as other rare earth elements and transition metal elements to these ternary systems.

〔発明の実施例〕[Embodiments of the invention]

以下、本発明を実施例を用いて説明する。 The present invention will be explained below using examples.

本発明の非晶質合金膜は直径8インチのGo円板上にl
X1cnfの希土類元素と鉄元素等の遷移金属元素を面
積化で所定の組成になるように配置した複合ターゲット
を用いて、周知のマグネ1−ロンスパッタ法で作製した
。また記録・再生評価用ディスクとして、5“φガラス
ディスク上にUVtll脂でトラッキング用の溝を形成
し、その上にTb−Fe−Co膜(膜厚約1000人)
、5in2膜(膜厚約700人)の順に被膜したものを
用いた。
The amorphous alloy film of the present invention was placed on a Go disk with a diameter of 8 inches.
It was produced by the well-known Magne-1-ron sputtering method using a composite target in which a rare earth element of X1cnf and a transition metal element such as an iron element were arranged so as to have a predetermined composition by area calculation. In addition, as a disk for recording/playback evaluation, a tracking groove was formed on a 5"φ glass disk using UV tll resin, and a Tb-Fe-Co film (film thickness of about 1000 mm) was formed on top of it.
, 5in2 film (film thickness: about 700 layers) were used.

本発明の1実施例として、補償組成よりも鉄族元素に富
んだ組成の代表例として、Tb20  Fe70.5 
 Co9.5.Tb21  Fe70.5  G。
As an example of the present invention, Tb20 Fe70.5 is a representative example of a composition richer in iron group elements than the compensation composition.
Co9.5. Tb21 Fe70.5 G.

8.5.Tb21.5  Fe71.5.Co7等の組
成の非晶質垂直磁化膜を記録膜とした。以下にそれらの
膜特性を示す。キュリー温度Tc=190〜230’C
,補償温度T comp≦−50℃9保磁力Hc = 
1−3 koe、飽和磁化M s = 120−195
emu/cc、カー回転角θk(λ=633nm)=0
.31−0.35゜ これらの膜を用いて、上記した5“φ多層膜ディスクを
作製した。記録・再生特性評価で、記録時のレーザ光パ
ワーを9 m W 、読み出しレーザ光パワーを2.5
mWにすると、記録時の外部磁場が2000 e以上で
再生時の変調ノイズが零となった。外部磁場3000e
のもとで記録した時の再生出力とノイズの比C/Nは上
記膜で52〜55 d B (1k l−1y、 、Δ
f=30kHz、  トラックピッチ1.6μm)と窩
い値を示した。
8.5. Tb21.5 Fe71.5. An amorphous perpendicular magnetization film having a composition such as Co7 was used as a recording film. The properties of those films are shown below. Curie temperature Tc = 190-230'C
, Compensation temperature T comp≦-50℃9 Coercive force Hc =
1-3 koe, saturation magnetization M s = 120-195
emu/cc, Kerr rotation angle θk (λ=633nm)=0
.. 31-0.35° Using these films, the above-mentioned 5"φ multilayer film disk was fabricated. In the evaluation of recording/reproducing characteristics, the laser light power during recording was 9 mW, and the read laser light power was 2.5 mW. 5
mW, the modulation noise during reproduction became zero when the external magnetic field during recording was 2000 e or more. External magnetic field 3000e
The reproduction output to noise ratio C/N when recorded under
f = 30kHz, track pitch 1.6μm).

上述の実施例においては希土類−鉄族系光磁気体におい
て同様の効果を奏する。
In the above-described embodiments, similar effects can be achieved in rare earth-iron group magneto-optical materials.

以上の実施例から明らかなように2本発明の非晶質垂直
磁化膜は、変調ノイズがほとんど無く、干渉構造で多重
反射によりカー回転角を見かけ上あげなくても高いCl
N値が得られることがわかった。勿論、これらの膜と屈
折率の比較的高いZnS、AQN、Si、N4.BN、
Si○等の干渉膜とを組み合せた干渉多層膜ディスクで
は、さらに高い56dB以上の高C/Nが得られる。
As is clear from the above examples, the amorphous perpendicularly magnetized film of the present invention has almost no modulation noise, has an interference structure, and has high Cl without increasing the apparent Kerr rotation angle due to multiple reflections.
It was found that the N value was obtained. Of course, these films and ZnS, AQN, Si, N4. BN,
In the case of an interference multilayer film disk in which an interference film such as Si○ is combined, an even higher C/N of 56 dB or more can be obtained.

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

第1図はTb−Fe−Co非晶質垂直磁化膜のキュリー
温度Tcと補償温度Tcompの各CO濃度、yに対す
るTb濃度、X依存性を示す図である。 葛1圀
FIG. 1 is a diagram showing the dependence of the Curie temperature Tc and the compensation temperature Tcomp of the Tb-Fe-Co amorphous perpendicularly magnetized film on the CO concentration and y, the Tb concentration, and X. Kuzu 1 area

Claims (1)

【特許請求の範囲】 1、膜面に垂直な方向に磁化容易軸を有し、実質的に非
晶質である希土類−鉄族系光磁気記録媒体において、当
該光磁気記録媒体のキュリー温度が250℃以下、補償
温度が0℃以下であることを特徴とする光磁気記録媒体
。 2、前記光磁気記録媒体は原子比率でテルビウム18〜
21.5%、コバルト8〜10%、残部実質的に鉄より
成る補償組成よりも鉄族元素に富み、実質的に非晶質で
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。
[Claims] 1. A substantially amorphous rare earth-iron magneto-optical recording medium having an axis of easy magnetization in a direction perpendicular to the film surface, the Curie temperature of the magneto-optical recording medium being A magneto-optical recording medium characterized in that the compensation temperature is 250°C or less and the compensation temperature is 0°C or less. 2. The magneto-optical recording medium has an atomic ratio of terbium 18~
21.5% cobalt, 8-10% cobalt, and the balance substantially iron, and is substantially amorphous and richer in iron group elements than the compensating composition, which is substantially amorphous. Magneto-optical recording medium.
JP21132084A 1984-10-11 1984-10-11 Photomagnetic recording medium Pending JPS6190348A (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP21132084A JPS6190348A (en) 1984-10-11 1984-10-11 Photomagnetic recording medium
DE19853536210 DE3536210A1 (en) 1984-10-11 1985-10-10 Magneto-optical recording medium
US07/294,941 US4923765A (en) 1984-10-11 1989-01-06 Magneto-optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21132084A JPS6190348A (en) 1984-10-11 1984-10-11 Photomagnetic recording medium

Publications (1)

Publication Number Publication Date
JPS6190348A true JPS6190348A (en) 1986-05-08

Family

ID=16603993

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21132084A Pending JPS6190348A (en) 1984-10-11 1984-10-11 Photomagnetic recording medium

Country Status (1)

Country Link
JP (1) JPS6190348A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5642343A (en) * 1990-06-29 1997-06-24 Hitachi, Ltd. Magnetooptic disc apparatus and recording medium

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58159252A (en) * 1982-03-17 1983-09-21 Canon Inc Magnetooptic recording medium

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58159252A (en) * 1982-03-17 1983-09-21 Canon Inc Magnetooptic recording medium

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5642343A (en) * 1990-06-29 1997-06-24 Hitachi, Ltd. Magnetooptic disc apparatus and recording medium

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