JPH01124131A - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- Publication number
- JPH01124131A JPH01124131A JP28103487A JP28103487A JPH01124131A JP H01124131 A JPH01124131 A JP H01124131A JP 28103487 A JP28103487 A JP 28103487A JP 28103487 A JP28103487 A JP 28103487A JP H01124131 A JPH01124131 A JP H01124131A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic layer
- film
- magneto
- magnetic
- 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
Links
- 230000005291 magnetic effect Effects 0.000 claims abstract description 70
- 229910052688 Gadolinium Inorganic materials 0.000 claims abstract description 21
- 229910052779 Neodymium Inorganic materials 0.000 claims abstract description 21
- 229910052761 rare earth metal Inorganic materials 0.000 claims abstract description 14
- 229910052723 transition metal Inorganic materials 0.000 claims abstract description 9
- 150000003624 transition metals Chemical class 0.000 claims abstract description 9
- 239000000758 substrate Substances 0.000 claims description 8
- 239000000203 mixture Substances 0.000 claims description 6
- 238000009826 distribution Methods 0.000 claims description 5
- 239000000470 constituent Substances 0.000 claims 1
- 230000000694 effects Effects 0.000 abstract description 6
- 230000035945 sensitivity Effects 0.000 abstract description 4
- 239000010410 layer Substances 0.000 description 40
- 238000010586 diagram Methods 0.000 description 7
- 239000000956 alloy Substances 0.000 description 4
- 229910045601 alloy Inorganic materials 0.000 description 4
- 230000001681 protective effect Effects 0.000 description 4
- 238000000034 method Methods 0.000 description 3
- 238000004544 sputter deposition Methods 0.000 description 3
- 229910052581 Si3N4 Inorganic materials 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 238000001704 evaporation Methods 0.000 description 2
- 230000008020 evaporation Effects 0.000 description 2
- HQVNEWCFYHHQES-UHFFFAOYSA-N silicon nitride Chemical compound N12[Si]34N5[Si]62N3[Si]51N64 HQVNEWCFYHHQES-UHFFFAOYSA-N 0.000 description 2
- 229910002546 FeCo Inorganic materials 0.000 description 1
- 229910052771 Terbium Inorganic materials 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 229910052804 chromium Inorganic materials 0.000 description 1
- 238000005260 corrosion Methods 0.000 description 1
- 230000007797 corrosion Effects 0.000 description 1
- 229910052732 germanium Inorganic materials 0.000 description 1
- 150000002500 ions Chemical class 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 239000012528 membrane Substances 0.000 description 1
- 229910052758 niobium Inorganic materials 0.000 description 1
- 229910052697 platinum Inorganic materials 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
- 230000000087 stabilizing effect Effects 0.000 description 1
- 238000007738 vacuum evaporation Methods 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明はレーザ光の照射により、記録、再生と消去を行
なう光磁気記録媒体に係り、特に良好な記録再生特性を
得るのに好適な記録膜を有する光磁気記録媒体に関する
。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a magneto-optical recording medium in which recording, reproduction and erasing are performed by irradiation with laser light, and particularly relates to a recording medium suitable for obtaining good recording and reproduction characteristics. The present invention relates to a magneto-optical recording medium having a film.
希土類元素と遷移金属からなる非晶質磁性膜を記録膜と
して用いる光磁気記録媒体は、情報の書き換えが可能で
あり、かつ高密度の記録を行なうことができる。しかし
ながら、さらに大量の情報を高速に扱うためには、光磁
気記録媒体の記録再生特性をいっそう向上させることが
必要である。Magneto-optical recording media that use an amorphous magnetic film made of rare earth elements and transition metals as a recording film are capable of rewriting information and can perform high-density recording. However, in order to handle even larger amounts of information at higher speeds, it is necessary to further improve the recording and reproducing characteristics of magneto-optical recording media.
光磁気記録媒体の再生信号の大きさは、主にカー(Ke
rr)回転角の大きさによって決定される。The magnitude of the reproduction signal of a magneto-optical recording medium is mainly determined by Kerr (Ke
rr) Determined by the magnitude of the rotation angle.
近年、記録膜のカー回転角を増大させる方法として、希
土類元素であるNdあるいはGdを記録膜に添加する方
法が知られている。例えば、NdとGdの両者を含む記
録膜として、NdGdFe膜が特開昭60−11743
6号において提案されている。また。In recent years, a method of adding Nd or Gd, which is a rare earth element, to a recording film has been known as a method of increasing the Kerr rotation angle of the recording film. For example, as a recording film containing both Nd and Gd, a NdGdFe film is used in Japanese Patent Laid-Open No. 60-11743.
It is proposed in No. 6. Also.
日本応用磁気学会誌、第11巻、第193頁から第19
6頁には、Ndを含む記録膜のカー回転角がレーザ光の
短波長領域で増大する傾向があることが示されている。Journal of the Japanese Society of Applied Magnetics, Volume 11, Pages 193-19
Page 6 shows that the Kerr rotation angle of a recording film containing Nd tends to increase in the short wavelength region of laser light.
これは、特に短波長レーザ光を用いて微小ピットを書き
込み、高密度記録を行なう場合において有効である。This is particularly effective when writing minute pits using short wavelength laser light to perform high-density recording.
しかしながら、上記従来技術においては、 NdとGd
の添加によるカー回転角増大の効果を最大限に活用する
記録膜の構成についての配慮が全くなされておらず、従
来のT b F e Coなどの記録膜を用いた光磁気
記録媒体に比べて、実用的に優位な記録再生特性が得ら
れないという問題があった。However, in the above conventional technology, Nd and Gd
No consideration has been given to the structure of the recording film to maximize the effect of increasing the Kerr rotation angle due to the addition of However, there was a problem in that practically superior recording and reproducing characteristics could not be obtained.
すなわち、従来の記録膜を単層で用いる構成においては
、良好な記録感度が得られるようにキュリー温度を低温
に設定する必要があり、NdとGdの添加量は制限され
ていた。また、NdやGdを含むため垂直磁気異方性や
保磁力の大きさが十分でなく、記録ドメイン内の磁化が
記録膜面の垂直方向から傾いており、そのために大きな
再生出力が得られず、また記録した情報の安定性が悪い
という問題があった。That is, in a conventional configuration using a single layer recording film, it is necessary to set the Curie temperature to a low temperature so as to obtain good recording sensitivity, and the amounts of Nd and Gd added are limited. Also, since it contains Nd and Gd, the perpendicular magnetic anisotropy and coercive force are not large enough, and the magnetization within the recording domain is tilted from the perpendicular direction of the recording film surface, making it impossible to obtain a large reproduction output. There was also the problem that the recorded information was unstable.
本発明の目的は、希土類元素であるNdとGdを含む磁
性層を記録膜の一部分として用いた構成とすることによ
り、記録再生特性の優れた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 with excellent recording and reproducing characteristics by using a magnetic layer containing rare earth elements Nd and Gd as part of a recording film.
上記目的は、少なくともNdとGdを含む第1の磁性層
と、NdとGdを含まない第2の磁性層で構成された二
層構造の記録膜を用いることにより。The above object is achieved by using a recording film having a two-layer structure consisting of a first magnetic layer containing at least Nd and Gd and a second magnetic layer not containing Nd and Gd.
達成される。achieved.
記録膜は必ずしも二層構造である必要はなく。The recording film does not necessarily have to have a two-layer structure.
第1の磁性層と第2の磁性層を多数積層した構成であっ
ても良い。A structure in which a large number of first magnetic layers and second magnetic layers are laminated may be used.
レーザ光の入射面に、第1の磁性層が配置されることが
望ましく、第1の磁性層の最適の膜厚は50Å以上、3
00Å以下である。It is desirable that the first magnetic layer is placed on the laser beam incidence plane, and the optimal film thickness of the first magnetic layer is 50 Å or more, 3
00 Å or less.
最も望ましい記録膜の構成は、レーザ光の入射する基板
面に、第1の磁性層を50〜150人積層し。The most desirable configuration of the recording film is to laminate 50 to 150 first magnetic layers on the substrate surface onto which the laser beam is incident.
さらにその上に第2の磁性層を700〜1000人積層
した構成である。もちろん、記録膜の膜面側からレーザ
光を入射させて再生を行なう場合には、上記と逆の積層
順となる。Furthermore, a second magnetic layer is stacked on top of this by 700 to 1000 layers. Of course, when reproducing is performed by inputting a laser beam from the film surface side of the recording film, the stacking order is reversed to the above.
また、上記の積層構造は必ずしも膜厚方向の組成分布が
不連続に変化する必要はなく2組成分布が連続的に変化
する構造であっても良い。Moreover, the above-described laminated structure does not necessarily have to have a composition distribution in the film thickness direction that changes discontinuously, but may have a structure in which the two composition distributions change continuously.
NdとGdを含みカー回転角の大きい第1の磁性層をレ
ーザ光照射による情報読み出し層として用いるので、大
きな再生出力が得られる。一方、第2の磁性層として、
キュリー温度が低く、十分な大きさの垂直磁気異方性と
保磁力を持つ磁性層を選択することにより、記録感度の
低下やノイズレベルの上昇を防ぐことができる。Since the first magnetic layer containing Nd and Gd and having a large Kerr rotation angle is used as an information readout layer by laser beam irradiation, a large reproduction output can be obtained. On the other hand, as the second magnetic layer,
By selecting a magnetic layer with a low Curie temperature and sufficient perpendicular magnetic anisotropy and coercive force, it is possible to prevent a decrease in recording sensitivity and an increase in noise level.
記録膜を構成する両者の磁性層は磁気的に結合されてお
り、レーザ光照射による記録再生時には。Both magnetic layers constituting the recording film are magnetically coupled, and during recording and reproduction by laser beam irradiation.
−層の記録膜のようにふるまうため、良好な記録再生特
性が得られる。- Since the layer behaves like a recording film, good recording and reproducing characteristics can be obtained.
以下2本発明の一実施例を挙げ図面を参照しながらさら
に詳細に説明する。Hereinafter, two embodiments of the present invention will be described in more detail with reference to the drawings.
(実施例1)
第1図に示す構成の光磁気ディスクを以下に示す手順で
作製した。直径13c■の透明樹脂基板1上に、マグネ
トロン式高周波スパッタ法により窒化シリコン膜(誘電
体膜2)を850人積層した0次に記録膜として同じく
マグネトロン式高周波スパッタ法により、100人のN
d1. Gd!2Fe、。Co、、膜(第1の磁性膜3
)と900人のTb、、Fe、□Co7膜(第2の磁性
層4)を順に積層した。スパッタガスとしては純Arガ
スを用い、高周波出力は1.5kWであった。さらに保
護膜として、窒化シリコン膜(保護膜4)を1500人
積層した。作製した光磁気ディスクの基板側から測定し
たカー回転角は0.9度、保磁力は6.0kOeであっ
た。(Example 1) A magneto-optical disk having the configuration shown in FIG. 1 was manufactured according to the procedure shown below. A silicon nitride film (dielectric film 2) of 850 layers was laminated on a transparent resin substrate 1 with a diameter of 13cm by magnetron high frequency sputtering.
d1. Gd! 2Fe,. Co, , film (first magnetic film 3
) and 900 Tb, Fe, and □Co films (second magnetic layer 4) were laminated in this order. Pure Ar gas was used as the sputtering gas, and the high frequency output was 1.5 kW. Furthermore, 1,500 silicon nitride films (protective film 4) were laminated as a protective film. The Kerr rotation angle measured from the substrate side of the produced magneto-optical disk was 0.9 degrees, and the coercive force was 6.0 kOe.
第2図に本実施例において作製した光磁気ディスクの記
録再生特性を示す、情報の記録再生は。FIG. 2 shows the recording and reproducing characteristics of the magneto-optical disk manufactured in this example.
半導体レーザを用いて基板側から行なった。記録再生条
件は、記録レーザ出力8mW、記録磁界4000s、デ
ィスク回転数240Orpm 、再生レーザ出力2、O
aWである。第2図に示すように、記録周波数10MH
zにおいても、45dBのC/N (搬送波対雑音比)
が得られ、良好な記録再生特性を示すことがわかった。This was performed from the substrate side using a semiconductor laser. The recording and reproduction conditions were: recording laser output 8mW, recording magnetic field 4000s, disk rotation speed 240Orpm, reproduction laser output 2,0
It is aW. As shown in Figure 2, the recording frequency is 10MH
C/N (carrier-to-noise ratio) of 45 dB even at z
was obtained, and it was found that good recording and reproducing characteristics were obtained.
なお、上述の光磁気ディスクと同じ構成で、第1の磁性
層として、 Nd、、 Gd□、 Tb、、 Fe4.
Co、。Note that it has the same configuration as the magneto-optical disk described above, and the first magnetic layer includes Nd, Gd□, Tb, Fe4.
Co.
膜、 Nd、。Gd0. D31t Fe、、 Go、
、膜を用いた場合にも、それぞれIOM Hzの記録周
波数で、45dBと43dBのC/Nが得られた。Membrane, Nd. Gd0. D31t Fe,, Go,
, C/N of 45 dB and 43 dB were obtained at the recording frequency of IOM Hz, respectively, when using the film.
ここで、上述のNdGdFeCo膜を1000人積層し
。Here, 1000 people stacked the above-mentioned NdGdFeCo films.
これを記録膜として用いた光磁気ディスクにおいては、
良好な記録再生特性が得られなかった。これは第3図(
b)に示すように、カーヒステリシス曲線の角形性が不
良であるためである。すなわち、垂直磁気異方性と保磁
力の大きさが、光磁気記録膜として十分な大きさでない
ことがわかる。In magneto-optical disks using this as a recording film,
Good recording and reproducing characteristics could not be obtained. This is shown in Figure 3 (
This is because, as shown in b), the squareness of the Kerr hysteresis curve is poor. That is, it can be seen that the perpendicular magnetic anisotropy and coercive force are not large enough to be used as a magneto-optical recording film.
一方、第3図(a)に示すように2本発明による光磁気
ディスクの構成では、角形性の良好なカーヒステリシス
曲線が得られた。On the other hand, as shown in FIG. 3(a), in the structure of the two magneto-optical disks according to the present invention, a Kerr hysteresis curve with good squareness was obtained.
さらに、第4図に示すように、60人の膜厚のNdGd
FeCo膜と190人の膜厚のTbFeCo膜を合計8
層積層した記録膜を用いた光磁気ディスクを作製した。Furthermore, as shown in Figure 4, 60 people's thickness of NdGd
A total of 8 FeCo films and a TbFeCo film with a thickness of 190
A magneto-optical disk using a layered recording film was fabricated.
NdGdFeCo合金とTbFeCo合金の2個の蒸発
源を持つ真空蒸着装置を用い、ディスク基板がそれぞれ
の蒸発源の上を通過するように公転させた。このように
して作製した光磁気ディスクにおいても、lOMHzの
記録周波数で43dB以上のC/Nが得られた。A vacuum evaporation apparatus having two evaporation sources of NdGdFeCo alloy and TbFeCo alloy was used, and the disk substrate was rotated so as to pass over each evaporation source. Also in the magneto-optical disk produced in this way, a C/N of 43 dB or more was obtained at a recording frequency of 1OMHz.
(実施例2)
次に、第1の磁性層としてNdGdFeCo膜を用い、
第2の磁性層としてT b F a Co膜を用いた光
磁気ディスクを作製した。ディスクの作製手順は。(Example 2) Next, using an NdGdFeCo film as the first magnetic layer,
A magneto-optical disk was fabricated using a T b F a Co film as the second magnetic layer. What are the steps to make the disc?
実施例1と同様である。ただし、記録膜用のスパッタタ
ーゲットとしてNdGdFeCo合金ターゲット(第1
のターゲット)と’l’bFeco合金ターゲット(第
2のターゲット)を用い、まず2両者のターゲットを同
時に放電させ2次に、ディスク基板を第1のターゲット
上と第2のターゲット上を順次通過させた。第1の磁性
層と第2の磁性層を合せた記録膜の膜厚は1000人で
あった。この場合。This is the same as in Example 1. However, the NdGdFeCo alloy target (first
target) and 'l'b Feco alloy target (second target), first discharge both targets at the same time, and then pass the disk substrate over the first target and the second target in sequence. Ta. The thickness of the recording film including the first magnetic layer and the second magnetic layer was 1000 mm. in this case.
第1の磁性層と第2の磁性層の界面は明確でなく。The interface between the first magnetic layer and the second magnetic layer is not clear.
組成が連続的に変化したものとなった。The composition changed continuously.
第5図はオージェ分析法による。記録膜の希土類元素の
濃度分布を示す図である。保護膜4側から、Arイオン
でスパッタリングを行ない、記録膜の深さ方向の分析を
行なった。第1の磁性層の組成はNd、Gd、Tb4F
e7.Cot (原子%)であり。Figure 5 is based on Auger analysis. FIG. 3 is a diagram showing the concentration distribution of rare earth elements in a recording film. Sputtering was performed with Ar ions from the protective film 4 side, and the recording film was analyzed in the depth direction. The composition of the first magnetic layer is Nd, Gd, Tb4F
e7. Cot (atomic %).
第2の磁性層の組成はTb2!Fe@4CO□。であっ
た。The composition of the second magnetic layer is Tb2! Fe@4CO□. Met.
このディスクにおいて、実施例1に示した記録再生条件
で、46dBのC/Nが得られた。In this disc, a C/N of 46 dB was obtained under the recording and reproducing conditions shown in Example 1.
なお9以上の実施例において、第1の磁性層にGoを添
加したものを用いたが、これは、第1の磁性層のキュリ
ー温度を上げ、情報再生時の記録膜温度の上昇によるカ
ー回転角の減少を押えるためである。したがって、Go
の添加は必ずしも必要ではなく、第1の磁性層としてN
dGdFe膜やN d G d T b F e膜を用
いても、上記実施例と同様の効果がある。また第2の磁
性層として、TbFeC0膜以外に、TbFa、DyF
e、DyFeCo膜などを用いても良く、第1表に示す
光磁気記録膜の構成においても良好な記録再生特性(C
/N)が得られた。In Examples 9 and above, Go was added to the first magnetic layer. This is to suppress the decrease in the angle. Therefore, Go
The addition of N is not necessarily necessary, and as the first magnetic layer, N
Even if a dGdFe film or a N d G d T b Fe film is used, the same effect as in the above embodiment can be obtained. In addition, as the second magnetic layer, in addition to the TbFeC0 film, TbFa, DyF
e, DyFeCo film, etc. may be used, and the structure of the magneto-optical recording film shown in Table 1 also has good recording and reproducing characteristics (C
/N) was obtained.
第1表
さらに、第1の磁性層と第2磁性層に、耐食性の向上や
非晶質膜の安定化の目的で、 All、 Ti。Table 1 In addition, All and Ti are added to the first magnetic layer and the second magnetic layer for the purpose of improving corrosion resistance and stabilizing the amorphous film.
Cr、Pt、Nb、B、C,Si、Geなどの元素を添
加しても、同様の効果がある。Similar effects can be obtained by adding elements such as Cr, Pt, Nb, B, C, Si, and Ge.
以上詳細に説明したごとく2本発明によるNdとGdの
うちの少なくとも1種の希土類元素と遷移金属からなる
第1の磁性層と、NdとGdを除く希土類元素のうちの
少なくとも1種の希土類元素と遷移金属からなる第2の
磁性層によって構成される二層構造の磁性膜を記録膜と
して用いた光磁気記録媒体は、たとえNdやGdを含み
カー回転角が大きい磁性層を記録膜とする媒体であって
も。As explained in detail above, two first magnetic layers according to the present invention are made of at least one rare earth element among Nd and Gd and a transition metal, and at least one rare earth element among rare earth elements other than Nd and Gd. A magneto-optical recording medium that uses a two-layered magnetic film as a recording film consisting of a second magnetic layer made of a transition metal and a second magnetic layer, even if it contains Nd or Gd and has a large Kerr rotation angle, is used as a recording film. Even if it's a medium.
記録感度の低下やノイズレベルの上昇を押えることがで
き、極めて良好な記録再生特性を有する光磁気記録媒体
を得ることができる。It is possible to suppress a decrease in recording sensitivity and an increase in noise level, and it is possible to obtain a magneto-optical recording medium having extremely good recording and reproducing characteristics.
第1図は本発明の実施例1において作製した光磁気ディ
スクの断面構造を示す模式図、第2図は実施例1の光磁
気ディスクのC/Nの記録周波数依存性を示す図、第3
図(a)は実施例1の光磁気ディスクのカーヒステリシ
ス曲線を示す図、第3図(b)は従来の記録膜を用いた
光磁気ディスクのカーヒステリシス曲線を示す図、第4
図は本発明の実施例1において作製した多層に積層した
構造の記録膜を有する光磁気ディスクの断面構造を示す
模式図、第5図は本発明の実施例2において作製した光
磁気ディスクの記録膜における膜厚方向の希土類元素の
濃度分布を示す図である。
1・・・透明基板 2・・・誘電体膜3=・N
dGdFeCo膜(第1の磁性層)4・・・TbFeC
o膜(第2の磁性層)5・・・保護膜
代理人弁理士 中 村 純之助
第1図
第2図
1しどイト3≧8り)ヲ万乏づ社【 (−〆IHz)第
3図
(a) (b)
第4図
4−rbvecagl(−fzqrAfz層2第5図FIG. 1 is a schematic diagram showing the cross-sectional structure of the magneto-optical disk manufactured in Example 1 of the present invention, FIG. 2 is a diagram showing the recording frequency dependence of C/N of the magneto-optical disk of Example 1, and FIG.
FIG. 3(a) is a diagram showing the Kerr hysteresis curve of the magneto-optical disk of Example 1, FIG. 3(b) is a diagram showing the Kerr hysteresis curve of the magneto-optical disk using a conventional recording film, and FIG.
The figure is a schematic diagram showing the cross-sectional structure of a magneto-optical disk having a recording film with a multi-layered structure manufactured in Example 1 of the present invention, and FIG. 5 is the recording of the magneto-optical disk manufactured in Example 2 of the present invention. FIG. 2 is a diagram showing the concentration distribution of rare earth elements in the film thickness direction in a film. 1...Transparent substrate 2...Dielectric film 3=・N
dGdFeCo film (first magnetic layer) 4...TbFeC
O film (second magnetic layer) 5...Protective film Patent attorney Junnosuke Nakamura Figure 1 Figure 2 Figure (a) (b) Figure 4-rbvecagl (-fzqrAfz layer 2 Figure 5
Claims (1)
希土類元素と遷移金属を主成分とする非晶質磁性膜を記
録膜として用いる光磁気記録媒体において、上記記録膜
は、NdとGdのうちより選ばれる少なくとも1種の元
素を含む希土類元素と少なくとも1種の遷移金属からな
る第1の磁性層と、NdとGdを除く希土類元素のうち
より選ばれる少なくとも1種の希土類元素と少なくとも
1種の遷移金属からなる第2の磁性層とによって構成さ
れ、上記第1の磁性層と第2の磁性層を積層した二層構
造の磁性膜であることを特徴とする光磁気記録媒体。 2、記録膜を構成する一組の二層構造の磁性膜が複数組
設けられていることを特徴とする特許請求の範囲第1項
に記載の光磁気記録媒体。 3、記録膜を構成する二層構造の磁性膜は、レーザ光の
入射側の面に第1の磁性層を配置し、他面に第2の磁性
層を配置した構造とすることを特徴とする特許請求の範
囲第1項または第2項に記載の光磁気記録媒体。 4、記録膜を構成する二層構造の磁性膜の構成元素の組
成分布が、第1の磁性層と第2の磁性層との界面もしく
は第2の磁性層と第1の磁性層との界面において、不連
続的に変化するかもしくは連続的に変化する構造の記録
膜であることを特徴とする特許請求の範囲第1項ないし
第3項のいずれか1項に記載の光磁気記録媒体。 5、二層構造の磁性膜を構成する第1の磁性層がNdG
dFe、NdGdFeCo、NdGdTbFeCo、N
dGdDyFeCoのうちより選ばれる少なくとも1種
からなり、第2の磁性層がTbFeCoであることを特
徴とする特許請求の範囲第1項ないし第4項のいずれか
1項に記載の光磁気記録媒体。[Scope of Claims] 1. In a magneto-optical recording medium using as a recording film an amorphous magnetic film mainly composed of rare earth elements and transition metals formed directly or through an underlayer on a substrate, The film includes a first magnetic layer made of a rare earth element containing at least one element selected from Nd and Gd and at least one transition metal, and a first magnetic layer made of at least one transition metal selected from Nd and Gd. The magnetic film is composed of a second magnetic layer made of a rare earth element and at least one transition metal, and has a two-layer structure in which the first magnetic layer and the second magnetic layer are laminated. magneto-optical recording medium. 2. The magneto-optical recording medium according to claim 1, characterized in that a plurality of sets of two-layered magnetic films constituting the recording film are provided. 3. The two-layered magnetic film constituting the recording film is characterized in that the first magnetic layer is arranged on the surface on the laser beam incidence side, and the second magnetic layer is arranged on the other surface. A magneto-optical recording medium according to claim 1 or 2. 4. The composition distribution of the constituent elements of the two-layered magnetic film constituting the recording film is at the interface between the first magnetic layer and the second magnetic layer or at the interface between the second magnetic layer and the first magnetic layer. The magneto-optical recording medium according to any one of claims 1 to 3, wherein the recording film has a structure that changes discontinuously or continuously. 5. The first magnetic layer constituting the two-layer magnetic film is NdG.
dFe, NdGdFeCo, NdGdTbFeCo, N
The magneto-optical recording medium according to any one of claims 1 to 4, characterized in that the second magnetic layer is made of at least one kind selected from dGdDyFeCo, and the second magnetic layer is TbFeCo.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28103487A JPH01124131A (en) | 1987-11-09 | 1987-11-09 | Magneto-optical recording medium |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28103487A JPH01124131A (en) | 1987-11-09 | 1987-11-09 | Magneto-optical recording medium |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01124131A true JPH01124131A (en) | 1989-05-17 |
Family
ID=17633369
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP28103487A Pending JPH01124131A (en) | 1987-11-09 | 1987-11-09 | Magneto-optical recording medium |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01124131A (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01229443A (en) * | 1988-03-10 | 1989-09-13 | Canon Inc | Magneto-optical recording medium |
JPH01237945A (en) * | 1988-03-18 | 1989-09-22 | Canon Inc | Magneto-optical recording medium |
JPH03108144A (en) * | 1989-09-20 | 1991-05-08 | Internatl Business Mach Corp <Ibm> | Photomagnetic recording medium |
JPH03212838A (en) * | 1990-01-09 | 1991-09-18 | Internatl Business Mach Corp <Ibm> | Method and apparatus for photo-electromagnetic record and readout of high density digital data |
WO1993010530A1 (en) * | 1991-11-22 | 1993-05-27 | Seiko Epson Corporation | Magnetooptical recording media |
JPH0935345A (en) * | 1995-07-12 | 1997-02-07 | Samsung Electron Co Ltd | Magneto-optical recording medium for short wavelength |
-
1987
- 1987-11-09 JP JP28103487A patent/JPH01124131A/en active Pending
Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01229443A (en) * | 1988-03-10 | 1989-09-13 | Canon Inc | Magneto-optical recording medium |
JPH01237945A (en) * | 1988-03-18 | 1989-09-22 | Canon Inc | Magneto-optical recording medium |
JPH03108144A (en) * | 1989-09-20 | 1991-05-08 | Internatl Business Mach Corp <Ibm> | Photomagnetic recording medium |
JPH03212838A (en) * | 1990-01-09 | 1991-09-18 | Internatl Business Mach Corp <Ibm> | Method and apparatus for photo-electromagnetic record and readout of high density digital data |
JP2728103B2 (en) * | 1990-01-09 | 1998-03-18 | インターナショナル・ビジネス・マシーンズ・コーポレーション | Method and apparatus for magneto-optical recording and reading of high-density digital data |
WO1993010530A1 (en) * | 1991-11-22 | 1993-05-27 | Seiko Epson Corporation | Magnetooptical recording media |
US5648161A (en) * | 1991-11-22 | 1997-07-15 | Seiko Epson Corporation | Magneto-optical recording medium having large kerr rotational angle in short wavelength range |
US5792571A (en) * | 1991-11-22 | 1998-08-11 | Seiko Epson Corporation | Magneto-optical recording medium having large kerr rotational angle in short wavelength range |
US5843570A (en) * | 1991-11-22 | 1998-12-01 | Seiko Epson Corporation | Magneto-optical recording medium having large kerr rotational angle in short wavelength range |
JPH0935345A (en) * | 1995-07-12 | 1997-02-07 | Samsung Electron Co Ltd | Magneto-optical recording medium for short wavelength |
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