JPS59159510A - Magnetooptical recording medium - Google Patents
Magnetooptical recording mediumInfo
- Publication number
- JPS59159510A JPS59159510A JP3397383A JP3397383A JPS59159510A JP S59159510 A JPS59159510 A JP S59159510A JP 3397383 A JP3397383 A JP 3397383A JP 3397383 A JP3397383 A JP 3397383A JP S59159510 A JPS59159510 A JP S59159510A
- Authority
- JP
- Japan
- Prior art keywords
- recording medium
- composition
- coercive force
- magneto
- alloy
- 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.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03G—ELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
- G03G5/00—Recording members for original recording by exposure, e.g. to light, to heat, to electrons; Manufacture thereof; Selection of materials therefor
- G03G5/16—Layers for recording by changing the magnetic properties, e.g. for Curie-point-writing
-
- 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
Abstract
Description
【発明の詳細な説明】
本発明は光磁気メモIJ−1磁気記録、表示素子などに
用いられる磁気光学記録媒体に関するもので、特に磁気
カー効果若しくは7アラデー効果などの磁気光学効果を
用いて読出すことのできる磁性薄膜記録媒体に関するも
のである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magneto-optical recording medium used for magneto-optical memo IJ-1 magnetic recording, display elements, etc. In particular, the present invention relates to a magneto-optical recording medium used for magneto-optical memo IJ-1 magnetic recording, display elements, etc. This invention relates to a magnetic thin film recording medium that can be released.
従来、磁気光学記録媒体としてはMnB1 、MnCu
B1などの多結晶体薄膜、Gd、Co 、G4Fe 、
TbFe 、DyFe 。Conventionally, MnB1, MnCu are used as magneto-optical recording media.
Polycrystalline thin films such as B1, Gd, Co, G4Fe,
TbFe, DyFe.
GaTbFe 、 TbDyFeなどの非晶質薄膜、G
IGなどの単結晶薄膜などが知られている。これらの薄
膜のうち、大面積の薄膜を室温近傍の温度で製作する製
膜性、信号を小さな光熱エネルギ・−で書込むための書
込み効率、書込まれた信号をsZN比よく読出すための
読出し効率などを勘案し、最近では前記非晶質薄膜が磁
気光学記録媒体として優れていると考えられている。Amorphous thin films such as GaTbFe and TbDyFe, G
Single crystal thin films such as IG are known. Among these thin films, the film-forming ability to produce a large-area thin film at a temperature near room temperature, the writing efficiency to write signals with small photothermal energy, and the ability to read written signals better than sZN. In consideration of read efficiency and the like, the amorphous thin film has recently been considered to be excellent as a magneto-optical recording medium.
しかしながら、これ等の非晶質薄膜においては信号を読
出すだめの読出し効率に対応する性能指数がMnB1等
の多結晶質薄膜やGIGの単結晶質薄膜に比し小さく
、 S/N比が十分にとれないという難点がある。However, in these amorphous thin films, the figure of merit corresponding to the readout efficiency for reading signals is smaller than that of polycrystalline thin films such as MnB1 and single crystalline thin films such as GIG.
, there is a drawback that a sufficient S/N ratio cannot be obtained.
S/N比良く読出すために非晶質薄膜の磁気光学定数を
大きくするだめの提案としては特開昭56−12690
7号公報にGaTbFeよシなる非晶質3元系合金薄膜
が示されている。さらにAbstractθof Th
e 1Qth工nternational CCo11
oquis onMagnetic Films an
d 5urfaces (19B2.9.13〜16)
13a1に示されている如(TbFeCoよシなる非晶
質5元系合金薄膜がある。表1に従来の磁気光学薄膜の
磁気光学定数の1つであるカー回転角を示す。A proposal to increase the magneto-optical constant of an amorphous thin film in order to read out a good S/N ratio is disclosed in Japanese Patent Application Laid-Open No. 56-12690.
No. 7 discloses an amorphous ternary alloy thin film such as GaTbFe. Furthermore, Abstractθof Th
e 1Qth engineering international CCo11
oquis on Magnetic Films an
d 5 surfaces (19B2.9.13-16)
There is an amorphous quinary alloy thin film such as TbFeCo as shown in 13a1. Table 1 shows the Kerr rotation angle, which is one of the magneto-optic constants of the conventional magneto-optic thin film.
表 1
材 料 名 カー回転角(釦
DyFθ o、12TbFθ
0.18GdFe
O,24GdCo o、2Tb
DyFe o、2゜GdDyF’e
O,24GdTdFe
o、27TbO,21(FeOJ5 C00
,15)0,79 0.52(測定波長6628又
)
表1よシ分かる様に、カー回転角が最も大きいのはTb
0JI(”0,85 C00,15)0.79の0・5
2度である・87N比が良く読出せる為にはカー回転角
の如き磁気光学定数が大きければ大きい程良いことは言
うまでもない。Table 1 Material name Kerr rotation angle (button DyFθ o, 12TbFθ
0.18GdFe
O,24GdCo o,2Tb
DyFe o, 2゜GdDyF'e
O,24GdTdFe
o, 27TbO, 21(FeOJ5 C00
, 15) 0,79 0.52 (6628 measurement wavelengths) As can be seen from Table 1, the largest Kerr rotation angle is Tb.
0JI ("0,85 C00,15) 0.5 of 0.79
It goes without saying that the larger the magneto-optical constant, such as the Kerr rotation angle, the better in order to be able to read out the 87N ratio of 2 degrees.
一方、表1に示した如き合金はフェソ磁性を示すために
補償組成が存在する。この補償組成域近傍においては保
磁力は非常に大きな値を示す。On the other hand, since the alloys shown in Table 1 exhibit fesomagnetism, a compensating composition exists. Near this compensation composition region, the coercive force exhibits a very large value.
一般にS/N比に効くカー回転角と記録された磁ワの安
定性に効く保磁力とは合金組成に対して独立に変化する
ために、カー回転角の大きい組成が必ずしも適当な大き
さの保磁力を示すとはかぎらない。カー回転角が大きく
ても保磁力が非常に大きな合金組成であれば、記録媒体
としては着磁・消磁をするのに非常に大きな磁場を必要
とするために、実用上の点から不都合である。In general, the Kerr rotation angle, which has an effect on the S/N ratio, and the coercive force, which has an effect on the stability of the recorded magnetic flux, change independently depending on the alloy composition, so a composition with a large Kerr rotation angle does not necessarily have an appropriate size. It does not necessarily show coercive force. If the alloy composition has a very large coercive force even if the Kerr rotation angle is large, it is disadvantageous from a practical point of view as it requires a very large magnetic field to magnetize and demagnetize the recording medium. .
本発明の目的は、磁気光学定数が十分に大きく、S/N
比の良い読出しが可能で、かつ、取扱い易い保磁力をも
った磁気光学記録媒体を提供することにある。The object of the present invention is to have a sufficiently large magneto-optical constant and
It is an object of the present invention to provide a magneto-optical recording medium that can be read with a high ratio and has a coercive force that is easy to handle.
本発明は、テルビウム・鉄・コバルトの3元系非晶質磁
性合金よシ成シ、この合金の組成をTbY(F8.−x
COx)、−1と表わしたときに、XおよびYが条件、
0<X(,0,375かツ0.1 ≦Y< 0.16−
1−− X37.5
0.575 < X < 1かツ0.1 ≦Y ≦0.
2−0.0(S4(X−0,X175)O<X≦0.!
I かつ0.2十−≦Y≦0.40.3<X<1
かつ0.3≦Y≦0.4のいずれか1つを満足するよう
に形成された磁気光学記録媒体によって上記目的を達成
するものである。The present invention produces a ternary amorphous magnetic alloy of terbium, iron, and cobalt, and changes the composition of this alloy to TbY (F8.-x
COx), -1, then X and Y are the conditions, 0<
1-- X37.5 0.575 < X < 1 0.1 ≦Y ≦0.
2-0.0(S4(X-0,X175)O<X≦0.!
I and 0.20-≦Y≦0.40.3<X<1
The above object is achieved by a magneto-optical recording medium formed to satisfy any one of 0.3≦Y≦0.4.
以下、図面を用いて本発明の詳細な説明する。Hereinafter, the present invention will be explained in detail using the drawings.
礒
第1図は本発明に係る磁気光学定数準TbFeC0の3
元系非晶質磁性合金の組成と保磁力との関係を示したも
のである。図中1の曲線は補償組成を示し、2,2′は
保磁力4000エールステツドを、6,5′は保磁力3
000エールステツドを、4.4′は保磁力2000エ
ールステツドを、5,5′は保磁力1000エールステ
ツドを、6.6′は200エールステツドを示す。補償
組成近傍の組成につ゛
おいては補償組成に近ヂくにしたがって急激に保磁力が
大きくなっている。これら補償組成近傍の組成の媒体は
着磁・消磁の際に非常に太きな磁場を会費とし、また製
造の際の特性のバラツキ、再現性の面からも不都合であ
る。Figure 1 shows the magneto-optical constant quasi-TbFeC0 according to the present invention.
This figure shows the relationship between the composition and coercive force of an amorphous magnetic alloy. The curve 1 in the figure shows the compensation composition, 2, 2' indicates a coercive force of 4000 Oersted, and 6, 5' indicates a coercive force of 3.
000 Oersted, 4.4' indicates a coercive force of 2000 Oersted, 5,5' indicates a coercive force of 1000 Oersted, and 6.6' indicates a coercive force of 200 Oersted. For compositions near the compensation composition, the coercive force increases rapidly as the composition approaches the compensation composition. Media with compositions close to these compensation compositions require a very strong magnetic field during magnetization and demagnetization, and are also disadvantageous in terms of variation in characteristics and reproducibility during manufacture.
一般に取扱い易い磁気光学記録媒体を実現する為には保
磁力は400oエールステツド以下である必要がある。In general, in order to realize a magneto-optical recording medium that is easy to handle, the coercive force must be 400o Oersted or less.
又、膜面に垂直な方向に磁化容易軸を向けるのに十分な
磁気異方性を持だせる組成として、FθとCoとを合わ
せた原子比が/HQ atom%〜9 Q atom%
の範囲に存在するととが望ましい。In addition, as a composition that can provide sufficient magnetic anisotropy to orient the axis of easy magnetization in the direction perpendicular to the film surface, the atomic ratio of Fθ and Co is /HQ atom% to 9 Q atom%.
It is desirable that it exists in the range of .
従って、適当な保磁力を有する組成は第1図の斜線で示
される領域となる。曲a2,2’をそれぞれ近似すると
上記領域は、組成をTbY(鴨x cox)FTとして
、各々
0 <X< 0.375かッo、1≦Ys:o、t6+
−X (1)37.5
0.575 < X < 1かツ0.1≦Y≦0.2−
0.064(X−0,575) (2)0 <X< 0
.3 かつ0.2 十−<Y< 0.4
(3)0.5 <X< 1 かツ0.5 < Y<
0.4 (4)の式で示される4つの領域
で表わされる。Therefore, the composition having an appropriate coercive force is the area shown by diagonal lines in FIG. Approximating songs a2 and 2', the above regions have the following compositions: 0 < X < 0.375, 1 < Ys: o, t6 +
-X (1) 37.5 0.575 < X < 1 0.1≦Y≦0.2-
0.064(X-0,575) (2) 0 <X< 0
.. 3 and 0.2 10-<Y< 0.4
(3) 0.5 <X< 1 Katsu0.5 <Y<
0.4 It is expressed by four regions shown by the equation (4).
以下に、上記式を満足する組成で形成された本発明の実
施例を示す。Examples of the present invention formed with compositions satisfying the above formula will be shown below.
(実施例)
高周波スパッター装置において25 m X 76 y
mの大きさの白板ガラスを基板にし、ターゲットとして
直径12711IのFeの円板上に10正×10間厚さ
1Mの大きさのTb、、Coの薄板を夫々14枚、2枚
載せたものを使用した、基板とターゲットとの間隔が9
0朋となる様にセットした後3X10 Torr以下
になるまで真空排気した。この後、真空槽に99.99
9%純度のArガスを6×10 ”−5TOrrまで導
入した。この時のAr流量は608CCMであった。高
周波電源よジターゲットへ2W/cIrL2の割合で電
力を投入して#膜を行った。(Example) 25 m x 76 y in high frequency sputtering equipment
A white glass plate with a size of m is used as a substrate, and 14 thin plates of Tb, 2 thin plates of Co, each with a size of 10 square x 10 and a thickness of 1M are placed on a Fe disk with a diameter of 12711I as a target. The distance between the board and target was 9
After setting the pressure to 0 Torr, the vacuum was evacuated until the pressure became 3×10 Torr or less. After this, 99.99
Ar gas with a purity of 9% was introduced to 6 x 10''-5 TOrr.The Ar flow rate at this time was 608 CCM.Electric power was applied to the high frequency power source target at a rate of 2 W/cIrL2 to perform #filming. .
(サンダルAI)この様にしてできた膜厚1500Aの
膜は膜面に垂直な方向に磁化容易軸を有し、X線回析の
結果非晶質であることが分った。まCoが4.7μ%残
部Fθであることがわかった。この膜のカー回転角は0
.29°、保磁力は1500エールステツドあった。(Sandals AI) The film with a thickness of 1500 A thus formed had an axis of easy magnetization in the direction perpendicular to the film surface, and was found to be amorphous as a result of X-ray diffraction. It was found that Co had a balance Fθ of 4.7 μ%. The Kerr rotation angle of this film is 0
.. 29°, and the coercive force was 1500 oersted.
サンプルA1と、ターゲットのTl)およびC0薄板の
枚数を変え、同様の実験を行った結果を表2に示す。Table 2 shows the results of a similar experiment conducted using sample A1, the target Tl), and the number of C0 thin plates.
表 2
このように本発明においては、Tb−Fe−Go 5元
系非晶質磁性合金のTbの量を規制することによって取
扱い易い保磁力を有する磁気光学記録媒体が得られるが
、更に残シのFeおよびCOの原子比の比率を適当に選
択することによって、読出しのS/N比の高い磁気光学
記録媒体とすることが望ましい。Table 2 As described above, in the present invention, by regulating the amount of Tb in the Tb-Fe-Go 5-component amorphous magnetic alloy, a magneto-optical recording medium having a coercive force that is easy to handle can be obtained. It is desirable to obtain a magneto-optical recording medium with a high reading S/N ratio by appropriately selecting the atomic ratio of Fe and CO.
本発明のTb−Fe−Go 5元系非晶質磁性薄膜より
成る磁気光学記録媒体では、FeとCOとを合わせた原
子比を1Q Q atom%としたときに、COの原子
比が増大するにつれて、カー回転角が犬きくなシ、Co
の原子比が50 atom%で最大とな夛、更にCo量
を増すに従ってカー回転角は小さくなる。In the magneto-optical recording medium made of the Tb-Fe-Go quinary amorphous magnetic thin film of the present invention, when the combined atomic ratio of Fe and CO is 1Q Q atom%, the atomic ratio of CO increases. As the car rotation angle increases, Co
The Kerr rotation angle is maximum when the atomic ratio of Co is 50 atom%, and as the amount of Co is further increased, the Kerr rotation angle becomes smaller.
十分に高いS/N比の読出しを可能とする為には、Co
の原子比が5 Q atom%〜7 Q atom%の
範囲に存在しなくてはならない。従って本発明において
も、前記合金の組成を前記(1)〜(4)式の領域内で
、かつ、FeとCoとを合わせた原子比を100′at
om%としたときに、Coの原子比が3 Q atoI
r1%〜7 g Btom%の範囲に存在するように構
成することによって読出しのS/N比が高く、かつ、取
扱い易い保磁力を有する磁気光学記録媒体が得られるも
のである。更に前記磁気光学記録媒体において、Feと
COとを合わせた原子比を1100ato%とじたとき
に、Goの原子比を4 Q atom%〜6Q ILt
O!n%の範囲に存在するように構成すると、カー回転
角が最大値から約6%以内のずれしかなく、特性のバラ
ツキ、再現性等を問題にしなければならない製造面から
も取扱い易く、によっても全く同様の結果が得られた。In order to enable readout with a sufficiently high S/N ratio, Co
The atomic ratio of must be in the range of 5 Q atom% to 7 Q atom%. Therefore, in the present invention, the composition of the alloy is within the range of formulas (1) to (4), and the atomic ratio of Fe and Co is 100'at.
When expressed as om%, the atomic ratio of Co is 3 Q atoI
By configuring it so that it exists in the range of r1% to 7 g Btom%, a magneto-optical recording medium having a high reading S/N ratio and a coercive force that is easy to handle can be obtained. Further, in the magneto-optical recording medium, when the combined atomic ratio of Fe and CO is 1100 atom%, the atomic ratio of Go is 4Q atom% to 6Q ILt.
O! If the Kerr rotation angle is configured so that it exists within the range of n%, the deviation of the Kerr rotation angle from the maximum value is only within about 6%, and it is easy to handle from a manufacturing perspective, where variations in characteristics, reproducibility, etc. must be considered. Exactly similar results were obtained.
以上説明したように、本発明は従来の磁気光学記録媒体
において、この記録媒体の保磁力を取扱い易い大きさと
する効果を有するものである。As explained above, the present invention has the effect of increasing the coercive force of a conventional magneto-optical recording medium to a size that is easy to handle.
第1図は本発明に係る磁気光学記録媒体のTbFeCo
5元系非晶質磁性合金の組成と保磁力との関係を示す
図である。
1・・・補償組成
2.2′・・・保磁力4000エールスデツドを示す組
成6.6′・・・保磁力3000エールステツドを示す
組成4.4′・・・保磁力2000エールステツドを示
す組成5.5′・・・保磁力1000エールステツドを
示す組成6.6′・・・保磁力200エールステツドを
示す組成lll:e!FIG. 1 shows a TbFeCo magneto-optical recording medium according to the present invention.
FIG. 3 is a diagram showing the relationship between the composition and coercive force of a quinary amorphous magnetic alloy. 1... Compensation composition 2.2'... Composition showing a coercive force of 4000 Aersted 6.6'... Composition showing a coercive force of 3000 Aersted 4.4'... Composition showing a coercive force of 2000 Aersted 5. 5'...Composition exhibiting a coercive force of 1000 Oersted 6.6'...Composition exhibiting a coercive force of 200 Oerstedll:e!
Claims (1)
成す、該合金の組成をT1)Y(Fe、−xCoX)、
−エと表わしたときに、XおよびYが条件、1)o<x
≦0.375かつ0.1≦Y≦o−16+ −g−T、
s x(2) 0.575 <X<1かつ0.1<Y≦
0.2−0.064(X−0,375)’(5)O<X
≦0.5 かつ0.2+、−≦Y<:0.4(4)0
.3<X<l かつ0.5≦Y≦0.4のいずれか1
つを満足するように形成された磁気光学記録媒体。The composition of the ternary amorphous magnetic alloy of terbium, iron, and cobalt is T1) Y(Fe, -xCoX),
- When expressed as d, X and Y are conditions, 1) o<x
≦0.375 and 0.1≦Y≦o-16+ -g-T,
s x (2) 0.575 <X<1 and 0.1<Y≦
0.2-0.064(X-0,375)'(5)O<X
≦0.5 and 0.2+, -≦Y<:0.4(4)0
.. Any one of 3<X<l and 0.5≦Y≦0.4
A magneto-optical recording medium formed to satisfy two requirements.
Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3397383A JPS59159510A (en) | 1983-03-01 | 1983-03-01 | Magnetooptical recording medium |
DE19833309483 DE3309483C3 (en) | 1982-03-17 | 1983-03-16 | Magneto-optical recording material and its use |
DE3348424A DE3348424C2 (en) | 1982-03-17 | 1983-03-16 | Terbium:iron:cobalt alloy used as magneto:optic recording material |
US06/783,052 US4670353A (en) | 1982-03-17 | 1985-10-01 | Magnetooptical recording medium |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3397383A JPS59159510A (en) | 1983-03-01 | 1983-03-01 | Magnetooptical recording medium |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS59159510A true JPS59159510A (en) | 1984-09-10 |
JPH0570922B2 JPH0570922B2 (en) | 1993-10-06 |
Family
ID=12401424
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3397383A Granted JPS59159510A (en) | 1982-03-17 | 1983-03-01 | Magnetooptical recording medium |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59159510A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60189208A (en) * | 1984-03-09 | 1985-09-26 | Nippon Hoso Kyokai <Nhk> | Photomagnetic recording medium |
DE3536210A1 (en) * | 1984-10-11 | 1986-04-17 | Hitachi, Ltd., Tokio/Tokyo | Magneto-optical recording medium |
JPS6184004A (en) * | 1984-10-01 | 1986-04-28 | Sumitomo Metal Mining Co Ltd | Photo-magnetic recording medium |
JPS6190349A (en) * | 1984-10-11 | 1986-05-08 | Hitachi Ltd | Photomagnetic recording medium |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1249789C (en) | 2002-11-28 | 2006-04-05 | 东京毅力科创株式会社 | Plasma processing container internal parts |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5231703A (en) * | 1975-09-05 | 1977-03-10 | Kokusai Denshin Denwa Co Ltd <Kdd> | Magnetic thin film recording medium |
JPS5873746A (en) * | 1981-10-27 | 1983-05-04 | Kokusai Denshin Denwa Co Ltd <Kdd> | Photomagnetic recording medium |
JPS58159252A (en) * | 1982-03-17 | 1983-09-21 | Canon Inc | Magnetooptic recording medium |
JPS595450A (en) * | 1982-07-02 | 1984-01-12 | Ricoh Co Ltd | Optical magnetic recording medium |
JPS5988808A (en) * | 1982-11-15 | 1984-05-22 | Ricoh Co Ltd | Magnetic recording medium |
-
1983
- 1983-03-01 JP JP3397383A patent/JPS59159510A/en active Granted
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5231703A (en) * | 1975-09-05 | 1977-03-10 | Kokusai Denshin Denwa Co Ltd <Kdd> | Magnetic thin film recording medium |
JPS5873746A (en) * | 1981-10-27 | 1983-05-04 | Kokusai Denshin Denwa Co Ltd <Kdd> | Photomagnetic recording medium |
JPS58159252A (en) * | 1982-03-17 | 1983-09-21 | Canon Inc | Magnetooptic recording medium |
JPS595450A (en) * | 1982-07-02 | 1984-01-12 | Ricoh Co Ltd | Optical magnetic recording medium |
JPS5988808A (en) * | 1982-11-15 | 1984-05-22 | Ricoh Co Ltd | Magnetic recording medium |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60189208A (en) * | 1984-03-09 | 1985-09-26 | Nippon Hoso Kyokai <Nhk> | Photomagnetic recording medium |
JPS6184004A (en) * | 1984-10-01 | 1986-04-28 | Sumitomo Metal Mining Co Ltd | Photo-magnetic recording medium |
DE3536210A1 (en) * | 1984-10-11 | 1986-04-17 | Hitachi, Ltd., Tokio/Tokyo | Magneto-optical recording medium |
JPS6190349A (en) * | 1984-10-11 | 1986-05-08 | Hitachi Ltd | Photomagnetic recording medium |
Also Published As
Publication number | Publication date |
---|---|
JPH0570922B2 (en) | 1993-10-06 |
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