JP2604475B2 - Magneto-optical recording medium - Google Patents

Magneto-optical recording medium

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Publication number
JP2604475B2
JP2604475B2 JP25597989A JP25597989A JP2604475B2 JP 2604475 B2 JP2604475 B2 JP 2604475B2 JP 25597989 A JP25597989 A JP 25597989A JP 25597989 A JP25597989 A JP 25597989A JP 2604475 B2 JP2604475 B2 JP 2604475B2
Authority
JP
Japan
Prior art keywords
film
magneto
recording medium
optical recording
magnetic
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 - Fee Related
Application number
JP25597989A
Other languages
Japanese (ja)
Other versions
JPH03119540A (en
Inventor
浩司 小野
洋一 橋本
紘一郎 堀野
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.)
Kuraray Co Ltd
Original Assignee
Kuraray Co Ltd
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Publication of JPH03119540A publication Critical patent/JPH03119540A/en
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Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は光磁気記録媒体に関する。Description: TECHNICAL FIELD The present invention relates to a magneto-optical recording medium.

[従来の技術] 記録された情報の有無にかかわらず新たな情報を重ね
て記録すること(オーバーライト(over write))が可
能な光磁気記録媒体における記録方式には、磁界変調記
録方式と光変調記録方式とがある。
[Related Art] Magneto-optical recording media capable of recording new information in a superimposed manner regardless of the presence or absence of recorded information (overwrite) include a magnetic field modulation recording method and an optical recording medium. There is a modulation recording method.

磁界変調記録方式は通常の磁気記録方式と同様に光磁
気記録媒体に一定強度のレーザ光照射下に記録する情報
に対応して光磁気記録媒体に印加する磁界を変調するこ
とによつて該光磁気記録媒体にオーバーライトを行うも
のである。磁界変調記録方式によつてオーバーライトを
行うには、光磁気記録媒体の磁性膜と記録ヘツドとの間
隔が小さくなければならないので、使用する光磁気記録
媒体が磁性膜が片面のみにある単板構造である必要があ
る。また記録のために印加する磁界の強度が低くなるよ
うな磁性膜の組成にする必要がある。
The magnetic field modulation recording system modulates the magnetic field applied to the magneto-optical recording medium by modulating the magnetic field applied to the magneto-optical recording medium in accordance with the information to be recorded under irradiation of a laser beam of constant intensity, similarly to the ordinary magnetic recording system. This is for overwriting the magnetic recording medium. In order to perform overwriting by the magnetic field modulation recording method, the distance between the magnetic film of the magneto-optical recording medium and the recording head must be small, so that the magneto-optical recording medium to be used is a single plate having the magnetic film on only one side. Must be a structure. Further, the composition of the magnetic film needs to be such that the intensity of the magnetic field applied for recording is low.

光変調記録方式は透明基板上に保護膜、磁気特性の異
なる2層の磁性膜および保護膜が順次積層されてなり、
上層の磁性膜(以下、これを補助層と称する)を形成す
る材料が下層の磁性膜(以下、これを記録層と称する)
を形成する材料よりも室温で低い保磁力と高いキユリー
温度とを有している光磁気記録媒体に初期化用の補助磁
界とこれとは反対方向の記録用磁界とを印加し、記録す
る情報に対応して照射するレーザ光の強度を変調するこ
とによつてオーバーライトを行うものである(特開昭62
−175948号公報参照)。これを具体的に説明すると、ま
ず初期化用の補助磁界を印加することによつて、補助層
の磁化の向きを消去方向にそろえる。この状態で消去レ
ベルの強度のレーザ光を照射すれば、補助層が有する磁
界が記録層に熱転写され、記録層の磁化は消去方向に向
く。ここで、書込レベルの高強度の光を記録する情報に
対応して照射すれば、補助層および記録層の磁化が消失
する。磁化が消失した磁性膜に記憶用磁界を印加すれ
ば、記録層の磁化の向きは消去方向とは逆の記録方向に
なるので、新たな情報が記録される。
The light modulation recording method is such that a protective film, two magnetic films having different magnetic properties and a protective film are sequentially laminated on a transparent substrate,
The material forming the upper magnetic film (hereinafter, referred to as an auxiliary layer) is a lower magnetic film (hereinafter, referred to as a recording layer).
Information to be recorded by applying an auxiliary magnetic field for initialization and a recording magnetic field in the opposite direction to a magneto-optical recording medium having a lower coercive force and a higher Curie temperature at room temperature than the material forming The overwriting is performed by modulating the intensity of the laser light to be irradiated in accordance with the method described in
-175948). More specifically, the direction of magnetization of the auxiliary layer is aligned with the erasing direction by applying an auxiliary magnetic field for initialization. When a laser beam having an erasing level is irradiated in this state, the magnetic field of the auxiliary layer is thermally transferred to the recording layer, and the magnetization of the recording layer is directed to the erasing direction. Here, if the high-intensity light at the writing level is irradiated in accordance with the information to be recorded, the magnetizations of the auxiliary layer and the recording layer disappear. If a storage magnetic field is applied to the magnetic film from which the magnetization has disappeared, the direction of the magnetization of the recording layer will be the recording direction opposite to the erasing direction, and thus new information will be recorded.

また特開昭63−64651号公報には、透明基板上に保護
膜、磁気特性の異なる3層の磁性膜および保護膜とが順
次積層されてなり、上層の磁性膜(補助膜)を形成する
材料が中間層の磁性膜(記録膜)を形成する材料よりも
室温で低い保磁力と高いキユリー温度とを有し、下層の
磁性膜(転写層)を形成する材料が上層の磁性膜を形成
する材料よりも室温で低い保磁力と高いキユリー温度と
を有している光磁気記録媒体を用いて光変調記録方式に
よつてオーバーライトを行うことが示されている。
JP-A-63-64651 discloses that a protective film, a three-layer magnetic film having different magnetic properties and a protective film are sequentially laminated on a transparent substrate to form an upper magnetic film (auxiliary film). The material has a lower coercive force and a higher Kyrie temperature at room temperature than the material forming the magnetic film (recording film) of the intermediate layer, and the material forming the lower magnetic film (transfer layer) forms the upper magnetic film It is disclosed that overwriting is performed by a light modulation recording method using a magneto-optical recording medium having a lower coercive force and a higher Curie temperature at room temperature than the material to be used.

[発明が解決しようとする課題] 上記の磁界変調記録方式には、磁界を高速で変調する
ことが困難であるために高速でオーバーライトを行うこ
とができない点、使用する光磁気記録媒体が単板構造の
ものに限られ、貼り合わせ構造にすることができないこ
とから、記録する情報量を多くできない点などの欠点が
ある。また上記の光変調記録方式には、消去むらが生じ
易いために高密度の情報を記録することが困難である点
などの欠点がある。
[Problems to be Solved by the Invention] The above-mentioned magnetic field modulation recording method cannot perform overwriting at high speed because it is difficult to modulate a magnetic field at high speed. Since it is limited to a plate structure and cannot be a laminated structure, there is a disadvantage that the amount of information to be recorded cannot be increased. In addition, the above-mentioned optical modulation recording method has a drawback that it is difficult to record high-density information because erasure unevenness is likely to occur.

本発明の目的は高密度のオーバーライトを高速で行う
ことができる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 capable of performing high-density overwriting at high speed.

[課題を解決するための手段] 本発明によれば、上記の目的は、基板上に保護膜、磁
気特性の異なる2層の磁性膜、保護膜および該保護膜の
熱伝導率よりも高い熱伝導率を有する熱吸収膜とが順次
積層されてなり、上層の磁性膜を形成する材料が下層の
磁性膜を形成する材料よりも室温で低い保磁力と高いキ
ユリー温度とを有していることを特徴とする光磁気記録
媒体を提供することによつて達成され、また基板上に保
護膜、磁気特性の異なる3層の磁性膜、保護膜および該
保護膜の熱伝導率よりも高い熱伝導率を有する熱吸収膜
とが順次積層されてなり、上層の磁性膜を形成する材料
が中間層の磁性膜を形成する材料よりも室温で低い保磁
力と高いキユリー温度とを有し、下層の磁性膜を形成す
る材料が上層の磁性膜を形成する材料よりも室温で低い
保磁力と高いキユリー温度とを有していることを特徴と
する光磁気記録媒体を提供することによつて達成され
る。
[Means for Solving the Problems] According to the present invention, the above object is achieved by providing a protective film on a substrate, two magnetic films having different magnetic properties, a protective film, and a heat higher than the thermal conductivity of the protective film. A heat absorbing film having conductivity is sequentially laminated, and a material forming an upper magnetic film has lower coercive force and a higher Kyrie temperature at room temperature than a material forming a lower magnetic film. And a protective film, a three-layer magnetic film having different magnetic properties, a protective film, and a thermal conductivity higher than the thermal conductivity of the protective film. And a heat absorbing film having a high coercivity at room temperature and a higher Kyrie temperature at room temperature than the material forming the magnetic film of the intermediate layer. The material that forms the magnetic film is higher than the material that forms the upper magnetic film. This is achieved by providing a magneto-optical recording medium characterized by having a low coercive force and a high Curie temperature at room temperature.

[実施例] 以下、実施例により本発明を具体的に説明するが、本
発明はこれらの実施例によつて何ら限定されるものでは
ない。
[Examples] Hereinafter, the present invention will be described specifically with reference to Examples, but the present invention is not limited to these Examples.

実施例1 本発明の光磁気記録媒体の1例の概略部分断面図を第
1図に示す。この光磁気記録媒体はポリカーボネート樹
脂基板1の上にSi51N49(原子数比)からなる保護膜2
と、Gd4Tb19Fe77(原子数比)からなる磁性膜(以下こ
れを記録層と称する)3と、Tb29Fe61Co10(原子数比)
からなる磁性膜(以下、これを補助層と称する)4と、
Si51N49(原子数比)からなる保護膜5と、Al97Ti3(原
子数比)からなる熱吸収膜6とが、それぞれ膜厚が下層
の保護膜1100Å、記録層1100Å、補助層500Å、上層の
保護膜350Åおよび熱吸収膜500Åになるように積載され
てなる。上記の補助層を形成する材料の保磁力は3KOe、
キユリー温度は220℃であり、記録層を形成する材料の
保持力は7KOe、キユリー温度は150℃である。
Embodiment 1 FIG. 1 shows a schematic partial cross-sectional view of one example of the magneto-optical recording medium of the present invention. This magneto-optical recording medium has a protective film 2 made of Si 51 N 49 (atomic ratio) on a polycarbonate resin substrate 1.
, A magnetic film 3 composed of Gd 4 Tb 19 Fe 77 (atomic ratio) (hereinafter referred to as a recording layer), and Tb 29 Fe 61 Co 10 (atomic ratio)
A magnetic film (hereinafter referred to as an auxiliary layer) 4 comprising
A protective film 5 made of Si 51 N 49 (atomic ratio) and a heat absorbing film 6 made of Al 97 Ti 3 (atomic ratio) are each composed of a protective film 1100 Å, a recording layer 1100 補助, and an auxiliary layer having lower film thicknesses. 500 mm, the upper protective film 350 mm, and the heat absorbing film 500 mm. The coercive force of the material forming the above auxiliary layer is 3KOe,
The Curie temperature is 220 ° C., the holding power of the material forming the recording layer is 7 KOe, and the Curie temperature is 150 ° C.

この光磁気記録媒体を用い、基板側から照射するレー
ザ光の消去レベルの出力が8mW、書込レベルの出力が12m
Wであり、記録用磁界が0.3KOe、初期化用磁界が5KOeで
あり、かつ回転数が1800rpmである条件で光変調記録方
式のオーバーライトを行うことにより情報を記録した。
この情報を再生して得られた信号における周波数とC/N
との関係を第2図に実線で示す。
Using this magneto-optical recording medium, the erasing level output of the laser beam irradiated from the substrate side is 8 mW, and the writing level output is 12 mW.
W, the recording magnetic field was 0.3 KOe, the initialization magnetic field was 5 KOe, and the information was recorded by performing the overwriting of the light modulation recording method under the condition that the rotation speed was 1800 rpm.
Frequency and C / N in the signal obtained by reproducing this information
Is shown by a solid line in FIG.

また、この光磁気記録媒体を用い、照射するレーザ光
の消去レベルの出力が8mW、記録用磁界が0.3KOe、初期
化用磁界が5KOe、回転数が1800rpmである条件で、照射
するレーザ光の書込レベルの出力を7〜15mWの範囲で変
えて光変調記録方式のオーバーライトを行うことにより
情報を記録した。この情報を再生して得られた信号にお
ける書込レベルのレーザ光の出力とC/Nとの関係を第3
図に実線で示す。
Further, using this magneto-optical recording medium, the output of the erasing level of the irradiated laser beam is 8 mW, the recording magnetic field is 0.3 KOe, the initialization magnetic field is 5 KOe, and the rotation speed is 1800 rpm. The information was recorded by changing the output of the writing level in the range of 7 to 15 mW and performing overwriting of the light modulation recording method. The relationship between the output of the laser light at the write level and the C / N in the signal obtained by reproducing this information is shown in FIG.
This is shown by a solid line in the figure.

比較例1 実施例1において熱吸収膜を備えていない以外は同一
の構造を有する光磁気記録媒体を用い、同じ条件で測定
した周波数とC/Nとの関係を第2図に、書込レベルのレ
ーザ光の出力とC/Nとの関係を第3図にそれぞれ破線で
示す。
Comparative Example 1 The relationship between the frequency and C / N measured under the same conditions using a magneto-optical recording medium having the same structure as in Example 1 except that the heat absorbing film was not provided is shown in FIG. The relationship between the laser light output and C / N is shown by broken lines in FIG.

第2図から明らかなように、実施例1の光磁気記録媒
体は比較例1の光磁気記録媒体に比べて高い周波数にお
いて高いC/Nを有しており、オーバーライトを高速で行
うことができる。また第3図から明らかなように、実施
例1の光磁気記録媒体は比較例1の光磁気記録媒体に比
べて記録のために照射するレーザ光の出力の許容範囲が
広く、情報の記録時に照射するレーザ光により発生する
熱が磁性膜内に残留し難いことを示している。したがっ
て、実施例1の光磁気記録媒体は比較例1の光磁気記録
媒体に比べて情報を高い密度で記録することができる。
As is clear from FIG. 2, the magneto-optical recording medium of Example 1 has a higher C / N at a higher frequency than the magneto-optical recording medium of Comparative Example 1, so that overwriting can be performed at high speed. it can. As is clear from FIG. 3, the magneto-optical recording medium of Example 1 has a wider allowable range of the output of the laser beam irradiated for recording than the magneto-optical recording medium of Comparative Example 1, so that the information recording time can be reduced. This indicates that the heat generated by the irradiating laser light hardly remains in the magnetic film. Therefore, the magneto-optical recording medium of Example 1 can record information at a higher density than the magneto-optical recording medium of Comparative Example 1.

実施例2 本発明の光磁気記録媒体の他の1例の部分概略断面図
を第4図に示す。この光磁気記録媒体はポリカーボネー
ト樹脂基板1の上に、Si48N52(原子数比)からなる保
護膜2(膜厚1000Å)、Gd22Fe55Co23(原子数比)から
なる磁性膜(以下、これを転写層と称する)7(膜厚50
0Å)、Gd23Tb3Fe74(原子数比)からなる磁性膜(以
下、これを記録層と称する)8(膜厚500Å)、Tb28Fe
65Co7(原子数比)からなる磁性膜(以下、これを補助
層と称する)9(膜厚500Å)、Si48N52(原子数比)か
らなる保護膜5(膜厚:300Å)およびAl90Ti10(原子数
比)からなる熱吸収膜6(膜厚:450Å)が順次積層され
てなる。上記の転写層を形成する材料の保磁力は0.1KO
e、キユリー温度は380℃であり、記録層を形成する材料
の保磁力は8kOe、キユリー温度は150℃であり、補助層
を形成する材料の保磁力は3KOe、キユリー温度は200℃
である。
Embodiment 2 FIG. 4 is a partial schematic sectional view of another example of the magneto-optical recording medium of the present invention. In this magneto-optical recording medium, a protective film 2 (thickness: 1000 mm) made of Si 48 N 52 (atomic ratio) and a magnetic film (thickness: Gd 22 Fe 55 Co 23 (atomic ratio)) are formed on a polycarbonate resin substrate 1. Hereinafter, this is referred to as a transfer layer.
0Å), a magnetic film made of Gd 23 Tb 3 Fe 74 (atomic ratio) (hereinafter referred to as a recording layer) 8 (500Å in thickness), Tb 28 Fe
A magnetic film made of 65 Co 7 (atomic ratio) (hereinafter referred to as an auxiliary layer) 9 (500 Å in thickness), a protective film 5 made of Si 48 N 52 (atomic ratio) (thickness: 300 お よ び) and A heat absorbing film 6 (thickness: 450 °) made of Al 90 Ti 10 (atomic ratio) is sequentially laminated. The coercive force of the material forming the transfer layer is 0.1 KO
e, the Kyuri temperature is 380 ° C, the coercive force of the material forming the recording layer is 8 kOe, the Kyuri temperature is 150 ° C, the coercive force of the material forming the auxiliary layer is 3KOe, and the Kyuri temperature is 200 ° C
It is.

この光磁気記録媒体も高い周波数において高いC/Nを
有しており、また記録のために照射するレーザ光の出力
の許容範囲が広い特徴を有する。
This magneto-optical recording medium also has a high C / N at a high frequency, and has a feature that the allowable range of the output of the laser beam irradiated for recording is wide.

本発明における熱吸収膜はAl、Au、Ag、PtおよびCUか
らなる群から選ばれる1つの元素からなるか、上記の群
から選ばれる1つの元素と、Cr、Ti、GeおよびSiからな
る群から選ばれる少なくとも1つの元素との合金からな
ることが好ましく、保護膜およぶ磁性膜の熱特性に応じ
て組成および膜厚を適宜設定すればよい。
The heat absorbing film of the present invention is made of one element selected from the group consisting of Al, Au, Ag, Pt and CU, or one element selected from the above group and a group consisting of Cr, Ti, Ge and Si. It is preferable that the composition and the film thickness be appropriately set in accordance with the thermal characteristics of the protective film and the magnetic film, which is an alloy with at least one element selected from the group consisting of:

上記の基板としてはポリカーボネート樹脂の他にポリ
メチルメタクリレート樹脂、エポキシ樹脂、ガラスなど
を用いることができる。また磁性膜は2層構造または3
層構造を有しており、その2層構造を形成する磁性膜の
材料としてはGdDyFe−GdTbFe、TbFe−GdTbFe、TbDyFe−
GdDyFeなどの組合わせを用いることができ、磁性膜が3
層を有する場合、その3層構造を形成する磁性膜の材料
としてはGdFeCo−GdDyFe−GdTbFe、GdFeCo−TbFe−GdTb
Fe、TbDyFe−GdDYFe−GdFeCoなどの組合わせを用いるこ
とができる。保護膜を形成する材料としては、SiNの他
にAlN、AlSiNなどを用いることができる。
As the above substrate, a polymethyl methacrylate resin, an epoxy resin, glass, or the like can be used in addition to the polycarbonate resin. The magnetic film has a two-layer structure or a three-layer structure.
It has a layer structure, and as a material of the magnetic film forming the two-layer structure, GdDyFe-GdTbFe, TbFe-GdTbFe, TbDyFe-
A combination such as GdDyFe can be used, and the magnetic film is 3
In the case of having a layer, the material of the magnetic film forming the three-layer structure is GdFeCo-GdDyFe-GdTbFe, GdFeCo-TbFe-GdTb
A combination such as Fe, TbDyFe-GdDYFe-GdFeCo can be used. As a material for forming the protective film, AlN, AlSiN, or the like can be used in addition to SiN.

保護膜、磁性膜などの膜厚はこれらの光学的特性およ
び熱伝導率に応じて決めることができるが、通常それぞ
れの膜厚は下層の保護膜400〜1200Å、磁性膜(記録層
+補助層または転写層+記録層+補助層)を合わせた膜
厚が600〜2300Å、上層の保護膜300〜1200Å、熱吸収率
200〜1500Åの範囲であることが好ましい。上記の各膜
はスパツタリング法によつて形成することができる。
The thickness of the protective film, the magnetic film, etc. can be determined according to their optical characteristics and thermal conductivity. Usually, each film thickness is 400 to 1200 mm of the lower protective film and the magnetic film (recording layer + auxiliary layer). Or the total thickness of transfer layer + recording layer + auxiliary layer) is 600 ~ 2300mm, upper protective film is 300 ~ 1200mm, heat absorption rate
Preferably it is in the range of 200 to 1500 °. Each of the above films can be formed by a sputtering method.

[発明の効果] 本発明によれば、高密度の情報のオーバーライトを高
速で行うことができる光磁気記録媒体が提供される。
[Effect of the Invention] According to the present invention, a magneto-optical recording medium capable of performing high-density information overwriting at high speed is provided.

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

第1図は本発明の光磁気記録媒体の1例の概略部分断面
図、第2図は光磁気記録媒体の周波数とC/Nとの関係を
示す特性図、第3図は光磁気記録媒体の書込レベルのレ
ーザ光の出力とC/Nとの関係を示す特性図、第4図は本
発明の光磁気記録媒体の他の1例の概略部分断面図であ
る。 1……基板、 2……保護膜、 3……磁性膜(記録膜)、 4……磁性膜(補助層)、 5……保護膜、 6……熱吸収膜、 7……磁性膜(転写層)、 8……磁性膜(記録層)、 9……磁性膜(補助層)。
FIG. 1 is a schematic partial cross-sectional view of one example of a magneto-optical recording medium of the present invention, FIG. 2 is a characteristic diagram showing the relationship between the frequency and C / N of the magneto-optical recording medium, and FIG. FIG. 4 is a characteristic diagram showing the relationship between the output of the laser light at the write level and the C / N ratio, and FIG. 4 is a schematic partial sectional view of another example of the magneto-optical recording medium of the present invention. DESCRIPTION OF SYMBOLS 1 ... board | substrate, 2 ... protective film, 3 ... magnetic film (recording film), 4 ... magnetic film (auxiliary layer), 5 ... protective film, 6 ... heat absorption film, 7 ... magnetic film ( Transfer layer), 8 ... magnetic film (recording layer), 9 ... magnetic film (auxiliary layer).

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】基板上に保護膜、磁気特性の異なる2層の
磁性膜、保護膜および該保護膜の熱伝導率よりも高い熱
伝導率を有する熱吸収膜とが順次積層されてなり、上層
の磁性膜を形成する材料が下層の磁性膜を形成する材料
よりも室温で低い保磁力と高いキユリー温度とを有して
いることを特徴とする光磁気記録媒体。
A protective film, a two-layer magnetic film having different magnetic properties, a protective film, and a heat absorbing film having a thermal conductivity higher than the thermal conductivity of the protective film are sequentially laminated on a substrate; A magneto-optical recording medium, characterized in that the material forming the upper magnetic film has lower coercive force and higher Curie temperature at room temperature than the material forming the lower magnetic film.
【請求項2】基板上に保護膜、磁気特性の異なる3層の
磁性膜、保護膜および該保護膜の熱伝導率よりも高い熱
伝導率を有する熱吸収膜とが順次積層されてなり、上層
の磁性膜を形成する材料が中間層の磁性膜を形成する材
料よりも室温で低い保磁力と高いキユリー温度とを有
し、下層の磁性膜を形成する材料が上層の磁性膜を形成
する材料よりも室温で低い保磁力と高いキユリー温度と
を有していることを特徴とする光磁気記録媒体。
2. A protective film, a magnetic film of three layers having different magnetic properties, a protective film, and a heat absorbing film having a thermal conductivity higher than that of the protective film are sequentially laminated on a substrate, The material forming the upper magnetic film has a lower coercive force and a higher temperature at room temperature than the material forming the magnetic film of the intermediate layer, and the material forming the lower magnetic film forms the upper magnetic film. A magneto-optical recording medium having a lower coercive force and a higher Curie temperature at room temperature than a material.
JP25597989A 1989-09-29 1989-09-29 Magneto-optical recording medium Expired - Fee Related JP2604475B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25597989A JP2604475B2 (en) 1989-09-29 1989-09-29 Magneto-optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25597989A JP2604475B2 (en) 1989-09-29 1989-09-29 Magneto-optical recording medium

Publications (2)

Publication Number Publication Date
JPH03119540A JPH03119540A (en) 1991-05-21
JP2604475B2 true JP2604475B2 (en) 1997-04-30

Family

ID=17286223

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25597989A Expired - Fee Related JP2604475B2 (en) 1989-09-29 1989-09-29 Magneto-optical recording medium

Country Status (1)

Country Link
JP (1) JP2604475B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3057644B2 (en) * 1989-11-10 2000-07-04 三菱化学株式会社 Magneto-optical recording medium
JP2008161963A (en) * 2006-12-27 2008-07-17 Sdi Corp Labor-saving type hole punch

Also Published As

Publication number Publication date
JPH03119540A (en) 1991-05-21

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