JPH0660448A - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- Publication number
- JPH0660448A JPH0660448A JP25864091A JP25864091A JPH0660448A JP H0660448 A JPH0660448 A JP H0660448A JP 25864091 A JP25864091 A JP 25864091A JP 25864091 A JP25864091 A JP 25864091A JP H0660448 A JPH0660448 A JP H0660448A
- Authority
- JP
- Japan
- Prior art keywords
- film
- artificial lattice
- layer
- magneto
- period
- 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
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は光磁気記録媒体に関す
る、更に詳しくは短波長対応の光磁気記録媒体に関す
る。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magneto-optical recording medium, and more particularly to a short wavelength compatible magneto-optical recording medium.
【0002】[0002]
【従来の技術】高密度光磁気記録媒体として、基板上に
Co層とPt層および/またはPd層とを交互に積層し
た人工格子膜を記録層とする光磁気記録媒体が提案され
ている(特開平2−56752公報)。このような光磁
気記録媒体は特に500nm以下の波長の光に対して大
きな磁気光学効果を示し、記録層に希土類金属等の酸化
されやすい金属を含まないため、耐蝕性に優れていると
されている。2. Description of the Related Art As a high-density magneto-optical recording medium, a magneto-optical recording medium having an artificial lattice film in which Co layers and Pt layers and / or Pd layers are alternately laminated on a substrate has been proposed ( JP-A-2-56752). Such a magneto-optical recording medium exhibits a large magneto-optical effect particularly for light having a wavelength of 500 nm or less, and since the recording layer does not contain a metal such as a rare earth metal that is easily oxidized, it is said to have excellent corrosion resistance. There is.
【0003】このようなCoとPtおよび/またはPd
とを積層した光磁気記録媒体に於いて再生性能を支配す
る磁気光学効果(カー回転角)の大きさは媒体中のCo
組成比と正の相関があるが、Coの組成比を高めるとキ
ュリー温度が上昇し、高い記録パワーが求められ、記録
感度が低下する。すなわち、媒体中のCo組成比は記録
システムの構成および記録再生に用いる光源に合わせ、
所望の記録特性が得られるCo組成比が選ばれる。Such Co and Pt and / or Pd
The magnitude of the magneto-optical effect (Kerr rotation angle) that governs the reproducing performance in a magneto-optical recording medium in which
Although there is a positive correlation with the composition ratio, when the Co composition ratio is increased, the Curie temperature rises, high recording power is required, and the recording sensitivity decreases. That is, the Co composition ratio in the medium is adjusted to the configuration of the recording system and the light source used for recording and reproduction,
A Co composition ratio that gives desired recording characteristics is selected.
【0004】[0004]
【発明が解決しようとする課題】一般に光磁気記録にお
いて、安定した状態で記録・再生を実施するには、磁性
体層の持つ特性であるカー回転角と保磁力がともに十分
に大きい材料が好ましい。Generally, in magneto-optical recording, a material having both a Kerr rotation angle and a coercive force, which are characteristics of a magnetic layer, are sufficiently large for stable recording and reproduction. .
【0005】しかしながら、所望の記録特性が得られる
組成比でPtとCoとを交互に積層した記録媒体におい
ては、均一な積層周期からなる媒体では大きな保磁力
と、大きなカー回転角を両立させる事は困難であった。However, in a recording medium in which Pt and Co are alternately laminated at a composition ratio that can obtain desired recording characteristics, a medium having a uniform lamination period should have a large coercive force and a large Kerr rotation angle. Was difficult.
【0006】本発明の目的は、保磁力、カー回転角がと
もに高い値を持つ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 having high values of both coercive force and Kerr rotation angle.
【0007】[0007]
【課題を解決するための手段】本発明者らは、上記目的
の達成のため種々の研究を重ねた結果、磁性層において
基板に近い部分とそれ以外の部分とで、PtとCo及び
/又はPdとの積層周期を変化させることにより保磁
力、カー回転角共に大きく、記録特性にも優れた光磁気
記録媒体が得られることを見出だし本発明を完成した。As a result of various studies to achieve the above object, the present inventors have found that Pt, Co and / or Pt and Co and / or The present invention has been completed by finding that a magneto-optical recording medium having a large coercive force and Kerr rotation angle and excellent recording characteristics can be obtained by changing the stacking period with Pd.
【0008】即ち本発明は、基板上に、Co層と、Pt
層及び/又はPd層とが交互に積層した人工格子膜を記
録層とする光磁気記録媒体において、前記人工格子膜
の、基板側の部分(1)が他の部分(2)より積層周期
が短い人工格子膜であり、(1)の部分が総膜厚の10
%以上80%以下の厚みであることを特徴とする光磁気
記録媒体に関するものである。次に本発明を更に詳細に
説明する。That is, according to the present invention, a Co layer and a Pt layer are formed on a substrate.
In a magneto-optical recording medium having a recording layer of an artificial lattice film in which layers and / or Pd layers are alternately laminated, a portion of the artificial lattice film on the substrate side (1) has a lamination cycle longer than that of the other portion (2). It is a short artificial lattice film, and the part (1) is 10 of the total film thickness.
The present invention relates to a magneto-optical recording medium having a thickness of 80% to 80%. Next, the present invention will be described in more detail.
【0009】図1は、CoとPtを用いて積層した本発
明の光磁気記録媒体の一実施態様を示す図である。図中
1は基板で、通常ガラスまたは高分子基板が用いられ
る。図中2は人工格子膜のうち積層周期の短い部分
(1)、3は人工格子膜のうち積層周期の長い部分
(2)である。FIG. 1 is a diagram showing an embodiment of a magneto-optical recording medium of the present invention laminated using Co and Pt. In the figure, 1 is a substrate, and a glass or polymer substrate is usually used. In the figure, 2 is a portion of the artificial lattice film having a short stacking period (1), and 3 is a portion of the artificial lattice film having a long stacking period (2).
【0010】本発明において、前記した積層周期を異に
する部分は、人工格子膜のうち基板側の部分(1)と、
それ以外の部分(2)であり、基板に近接し、総膜厚の
10%以上80%以下の厚さの部分(図1における
(1)の部分)においては、Co/Pt(及び/または
Pd)の積層周期を短くし、それ以外の部分(同(2)
の部分)ではこれより長くしたことが特徴である。In the present invention, the portion having a different stacking period is the portion (1) on the substrate side of the artificial lattice film,
In the other portion (2), which is close to the substrate and has a thickness of 10% or more and 80% or less of the total film thickness (portion (1) in FIG. 1), Co / Pt (and / or Pd) stacking period is shortened, and other parts (Same as (2)
Part) is characterized by making it longer than this.
【0011】上記した積層周期の変化する部分(1)の
厚みを、上記した範囲以外において変化させても、例え
ば10%より少なければ磁気光学効果の大きい部分によ
る全体への寄与が少なく、また、80%より多ければ保
磁力の大きな部分による全体への寄与が少なくなり、本
発明の効果が得られなくなる。Even if the thickness of the portion (1) in which the stacking period is changed is changed outside the above range, if the thickness is less than 10%, the contribution of the portion having a large magneto-optical effect to the whole is small, and If it is more than 80%, the contribution of the part having a large coercive force to the whole becomes small, and the effect of the present invention cannot be obtained.
【0012】本発明における前記した積層周期の好まし
い具体例は、前記(1)の部分においては、Coが0.
5〜1.5原子層、Pt(及び/またはPd)が1〜6
原子層の人工格子となることであり、又、前記(2)の
部分においては、(1)の部分の値より大で、かつ、C
oが1〜2.5原子層、Pt(及び/またはPd)が2
〜8原子層の人工格子となることである。前記した範囲
外では本発明の効果が充分得られない。A preferred specific example of the above-mentioned stacking period in the present invention is that Co is less than 0.
5 to 1.5 atomic layer, Pt (and / or Pd) 1 to 6
It is to be an artificial lattice of atomic layers, and in the part (2), the value is larger than the value in the part (1) and C
o is 1 to 2.5 atomic layer and Pt (and / or Pd) is 2
It is to be an artificial lattice of 8 atomic layers. Outside of the above range, the effect of the present invention cannot be sufficiently obtained.
【0013】本発明の光磁気記録媒体の製造は、基板面
に例えばスパッタリング法によりこれら金属を積層する
方法を用いることができ、スパッタリングの条件を適宜
設定することにより、積層周期の異なった人工格子膜を
形成することができる。In the manufacture of the magneto-optical recording medium of the present invention, a method of laminating these metals on the surface of the substrate by, for example, a sputtering method can be used. By appropriately setting the sputtering conditions, artificial lattices having different laminating periods can be used. A film can be formed.
【0014】即ち、その製法の一例としては、スパッタ
された原子が互いに混じらないように仕切り板で仕切ら
れた金属、例えばCoとPt(及び/またはPd)のタ
ーゲットを同時にスパッタしながら、基板がこれらのタ
ーゲット上を交互に通過するようにした基板ホルダーを
回転させ、この際に基板ホルダーの回転数を人工格子膜
の形成中に変化させることにより周期の異なる人工格子
を形成するような方法である。That is, as an example of the manufacturing method, while simultaneously sputtering a target of a metal, such as Co and Pt (and / or Pd), which is partitioned by a partition plate so that the sputtered atoms do not mix with each other, the substrate is By rotating the substrate holder that alternately passes over these targets, and changing the number of rotations of the substrate holder at this time during the formation of the artificial lattice film, a method of forming artificial lattices with different periods is used. is there.
【0015】スパッタリングにより成膜されたCo/P
t(及び/またはPd)人工格子において、保磁力は一
定のCo層厚において最大値を示すが、CoとPtの組
成比が同じ場合、積層周期が短いほど大きな磁気カー回
転角を示す。この場合、より大きな磁気カー回転角を得
るためにはより周期の短い人工格子の持つ性質をこれに
寄与させることである。Co / P formed by sputtering
In the t (and / or Pd) artificial lattice, the coercive force has the maximum value at a constant Co layer thickness, but when the composition ratio of Co and Pt is the same, the shorter the stacking period, the larger the magnetic Kerr rotation angle. In this case, in order to obtain a larger magnetic Kerr rotation angle, the property of the artificial lattice having a shorter period is to contribute to this.
【0016】本発明は、保磁力が大きい値を示す人工格
子構造の部分と磁気カー回転角が大きい値を示す人工格
子構造の部分を合せ持つ構成とすることにより、双方の
長所を兼ね備えたことが特徴である。本発明者の見出だ
したところによれば基板に近い部分すなわち人工格子膜
の初期形成層は膜の保磁力に余り影響しない。即ち、記
録層たる人工格子膜の記録の読みだし側である基板側の
部分には大きい磁気カー回転角を示す周期の短い人工格
子(図1の(1)層)を形成し、残りの部分には大きな
保磁力を示す人工格子(図1の(2)層)を形成するこ
とによって全体として大きな磁気カー回転角と保磁力を
得ることができる。(1)層と(2)層との人工格子膜
中における比率は、(1)層が10%より小では(1)
層の大きなカー回転角の特徴を示さなくなり、また
(2)層は20%より小では(2)層の大きな保磁力を
膜が示さなくなるため、人工格子膜中に占める(1)層
の割合を10%から80%の範囲にすることが必要であ
る。The present invention has both advantages by having a structure having both an artificial lattice structure having a large coercive force and an artificial lattice structure having a large magnetic Kerr rotation angle. Is a feature. According to the finding of the present inventor, the portion close to the substrate, that is, the initial formation layer of the artificial lattice film has little influence on the coercive force of the film. That is, an artificial lattice (layer (1) in FIG. 1) having a short period showing a large magnetic Kerr rotation angle is formed on the portion of the artificial lattice film, which is the recording layer, on the side of the substrate that is the recording read side, and the remaining portion is formed. A large magnetic Kerr rotation angle and a large coercive force can be obtained as a whole by forming an artificial lattice (layer (2) in FIG. 1) having a large coercive force. The ratio of the (1) layer to the (2) layer in the artificial lattice film is (1) when the (1) layer is less than 10%.
The ratio of the (1) layer occupying in the artificial lattice film does not show the characteristic of the large Kerr rotation angle of the layer, and when the (2) layer is smaller than 20%, the film does not show the large coercive force of the (2) layer. Should be in the range of 10% to 80%.
【0017】[0017]
【実施例1】スパッタガスにXeを用い、高周波マグネ
トロンスパッタ法で水冷したガラス基板上に人工格子膜
を形成した。スパッタ時のガス圧は約5mmTorrと
し、成膜速度は約1〜5A毎秒とした。Example 1 Xe was used as a sputtering gas, and an artificial lattice film was formed on a water-cooled glass substrate by a high frequency magnetron sputtering method. The gas pressure during sputtering was about 5 mmTorr, and the film formation rate was about 1 to 5 A / sec.
【0018】まず積層周期の短い部分(1)としてPt
層を4.5A,Co層を1.5Aとなるように、交互に
16回繰り返し(約100オングストローム)成膜した
のち、積層周期の長い部分(2)としてPt層を12
A,Co層を4Aとなるように、交互に7回繰り返し
(約100オングストローム)積層した。同様にして、
第1表に示したように、積層周期の短い部分(1)とし
て周期の異なる人工格子膜を形成し、それぞれについて
基板側から磁気光学効果および保磁力を測定した。測定
結果を第1表に示した。尚、これらの測定は400nm
の波長の光を用い、カーループトレーサーにより行っ
た。First, Pt is used as a portion (1) having a short stacking period.
The layers were alternately repeated 16 times (about 100 angstroms) so that the layers were 4.5 A and the Co layers were 1.5 A, and then 12 Pt layers were formed as a portion (2) having a long stacking period.
The A and Co layers were alternately laminated 7 times (about 100 Å) so as to have a thickness of 4 A. Similarly,
As shown in Table 1, artificial lattice films having different periods were formed as a portion (1) having a short stacking period, and the magneto-optical effect and the coercive force of each of the artificial lattice films were measured from the substrate side. The measurement results are shown in Table 1. In addition, these measurements are 400 nm
Was carried out by a Kerr loop tracer using light of the wavelength.
【0019】 第1表 (1)層 (2)層 試料 Co厚 Pt厚 Co厚 Pt厚 カー回転角 保磁力 (A) (A) (A) (A) (度) (Oe) a 1.5 4.5 4 12 0.53 650 b 2 6 4 12 0.53 700 c 2.5 7.5 4 12 0.51 720 d 3 9 4 12 0.49 750Table 1 (1) layer (2) layer Sample Co thickness Pt thickness Co thickness Pt thickness Kerr rotation angle Coercive force (A) (A) (A) (A) (degree) (Oe) a 1.5 4.5 4 12 0.53 650 b 2 6 4 12 0.53 700 c c 2.5 7.5 4 12 0.51 720 d 3 9 4 12 0.49 750
【0020】[0020]
【実施例2】実施例と同条件でガラス基板上に成膜を行
った。まず積層周期の短い部分(1)をPt7.5A/
Co2.5Aの積層周期で約50オングストロームから
150オングストロームの範囲で成膜したのち、積層周
期の長い部分(2)をPt12A/Co4Aの周期で連
続して積層し、総膜厚は約200Aとした。実施例1と
同様に行った磁気光学効果及び保磁力の測定結果を第2
表に示した。Example 2 A film was formed on a glass substrate under the same conditions as in Example. First, Pt 7.5A /
After forming a film in the range of about 50 angstroms to 150 angstroms at a stacking cycle of Co 2.5 A, the portion (2) having a long stacking cycle was continuously stacked at a cycle of Pt12A / Co4A, and the total film thickness was about 200 A. . The measurement results of the magneto-optical effect and the coercive force performed in the same manner as in Example 1 are
Shown in the table.
【0021】 第2表 試料 (1)層厚(A) (2)層厚(A) カー回転角(度) 保磁力(Oe) e 50 150 0.48 740 f 100 100 0.51 720 g 150 50 0.54 620Table 2 Sample (1) Layer thickness (A) (2) Layer thickness (A) Kerr rotation angle (degree) Coercive force (Oe) e 50 150 0.48 740 f 100 100 0.51 720 g 150 50 0.54 620
【0022】[0022]
【比較例】実施例と同条件でガラス基板上に均一な積層
周期を持つ膜を約200A成膜し、同条件で磁気光学効
果及び保磁力の測定を行った。測定結果を第3表に示
す。[Comparative Example] About 200 A of a film having a uniform stacking period was formed on a glass substrate under the same conditions as in the example, and the magneto-optical effect and coercive force were measured under the same conditions. The measurement results are shown in Table 3.
【0023】 第3表 試料 Co層厚 Pt層厚(A) カー回転角(度) 保磁力(Oe) h 2.0 6.0 0.56 450 i 3.0 9.0 0.51 640 j 4.0 12.0 0.44 760 k 5.0 15.0 0.39 650 実施例1の結果から、本発明による、積層周期を異にす
る2つの部分(1)、(2)からなる複合型人工格子膜
は、比較例に示した均一な積層周期からなる単純型人工
格子膜では得られなかった、磁気カー回転角0.5度以
上、保磁力700Oe以上の両立という優れた特性が得
られていることが分かる。Table 3 Sample Co layer thickness Pt layer thickness (A) Kerr rotation angle (degree) Coercive force (Oe) h 2.0 6.0 0.56 450 i 3.0 9.0 9.0 0.51 640 j 4.0 12.0 0.44 760 k 5.0 15.0 0.39 650 From the results of Example 1, the present invention comprises two parts (1) and (2) having different stacking periods. The composite type artificial lattice film has excellent characteristics that both the magnetic Kerr rotation angle of 0.5 degree or more and the coercive force of 700 Oe or more, which cannot be obtained by the simple type artificial lattice film having the uniform lamination period shown in the comparative example. You can see that it has been obtained.
【0024】さらに、実施例2の結果から明らかなよう
に積層周期の短い部分(1)と積層周期の長い部分
(2)の比を変化させることにより媒体の特性を連続的
に変化させることが可能であり、、採用する媒体構造、
記録再生に用いる光源の波長などに合わせ、人工格子膜
中で積層周期の短い部分(1)の占める割合は前記した
範囲内で所望の値を選べば良い。Further, as is clear from the results of Example 2, the characteristics of the medium can be continuously changed by changing the ratio of the portion (1) having a short lamination period and the portion (2) having a long lamination period. Possible and adopted media structure,
According to the wavelength of the light source used for recording / reproduction, etc., the proportion of the portion (1) having a short stacking period in the artificial lattice film may be selected within the above range.
【0025】これらの人工格子膜を光磁気記録媒体とし
て利用する際、すでに実用化されている希土類−遷移金
属アモルファス合金を用いた光磁気記録媒体において用
いられているように、磁性体層と誘電体層を組み合わせ
て積層することが、記録再生特性を向上させるのに有効
である。When these artificial lattice films are used as a magneto-optical recording medium, a magnetic material layer and a dielectric layer are used as in a magneto-optical recording medium using a rare earth-transition metal amorphous alloy which has already been put into practical use. It is effective to combine and stack body layers to improve recording / reproducing characteristics.
【0026】例えば、基板上に誘電体層、磁性体層、誘
電体層、反射層の順に積層した4層膜型を採用し、基板
側から記録再生を行なう形式の場合の該人工格子からな
る磁性体層の厚さは50〜300Aが適当である。For example, a 4-layer film type in which a dielectric layer, a magnetic layer, a dielectric layer, and a reflection layer are laminated in this order on a substrate is adopted, and the artificial lattice is used in the case of recording and reproducing from the substrate side. A suitable thickness of the magnetic layer is 50 to 300A.
【0027】また、成膜途中で積層周期を変化させるに
あたり、本実施例のように基板の回転数を変化させる手
法によらず、スパッタレートを変化させることでも同じ
効果が得られ、その場合、積層周期の短い部分(1)と
積層周期の長い部分(2)との間でPtとCoの組成比
に多少のずれが生じる場合でも本発明の範囲から除外さ
れるものではない。Further, when changing the stacking period during film formation, the same effect can be obtained by changing the sputter rate instead of the method of changing the rotation speed of the substrate as in this embodiment. In that case, Even if the composition ratio of Pt and Co is slightly different between the part (1) having a short stacking period and the part (2) having a long stacking period, it is not excluded from the scope of the present invention.
【0028】さらに、実施例および比較例にはPtとC
oの組成比が3:1(体積比)の場合を示したが、本発
明はこれに限定されるものではなく、用いる記録再生シ
ステムにより、所望の記録感度が得られるようにPtと
Coの組成比を変化させれば良い。Further, Pt and C are used in Examples and Comparative Examples.
Although the case where the composition ratio of o is 3: 1 (volume ratio) is shown, the present invention is not limited to this, and Pt and Co may be selected so as to obtain a desired recording sensitivity depending on the recording / reproducing system used. The composition ratio may be changed.
【0029】また成膜装置の都合上、実施例のように積
層周期を急峻に変化させ得ず、積層周期が連続的に変化
する場合も実施例とほぼ同等の効果が得られる。Further, due to the convenience of the film forming apparatus, it is possible to obtain substantially the same effect as the embodiment even when the lamination period cannot be changed sharply as in the embodiment and the lamination period is continuously changed.
【0030】[0030]
【発明の効果】以上の説明からも明らかなように本発明
によればキュリー温度を上げることなく磁気光学効果お
よび保磁力の大きな記録媒体が得られるため、短波長光
源および周辺光学系と組み合わせることにより高記録密
度、高CN比の光磁気記録を可能とするものである。As is apparent from the above description, according to the present invention, a recording medium having a large magneto-optical effect and coercive force can be obtained without raising the Curie temperature, and therefore, it is preferably combined with a short wavelength light source and a peripheral optical system. This enables magneto-optical recording with high recording density and high CN ratio.
【図1】本発明の光磁気記録媒体の一実施態様を示す図FIG. 1 is a diagram showing an embodiment of a magneto-optical recording medium of the present invention.
1:基板 2:人工格子膜のうち積層周期の短い部分(1) 3:人工格子膜のうち積層周期の長い部分(2) 1: Substrate 2: Part of artificial lattice film with short stacking period (1) 3: Part of artificial lattice film with long stacking period (2)
─────────────────────────────────────────────────────
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【手続補正書】[Procedure amendment]
【提出日】平成3年10月7日[Submission date] October 7, 1991
【手続補正1】[Procedure Amendment 1]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】請求項1[Name of item to be corrected] Claim 1
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【手続補正2】[Procedure Amendment 2]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】0008[Correction target item name] 0008
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【0008】 即ち本発明は、基板上に、Co層と、P
t層及び/又はPd層とが交互に積層した人工格子膜を
記録層とする光磁気記録媒体において、前記人工格子膜
の、基板側の部分(1)が他の部分(2)より積層周期
が短い人工格子膜であり、(1)の部分が人工格子膜の
総膜厚の10%以上80%以下の厚みであることを特徴
とする光磁気記録媒体に関するものである。次に本発明
を更に詳細に説明する。That is, according to the present invention, a Co layer and a P layer are formed on a substrate.
In a magneto-optical recording medium having an artificial lattice film in which t layers and / or Pd layers are alternately laminated as a recording layer, a portion (1) on the substrate side of the artificial lattice film has a lamination cycle longer than that of the other portion (2). Is a short artificial lattice film, and the portion (1) has a thickness of 10% or more and 80% or less of the total film thickness of the artificial lattice film . Next, the present invention will be described in more detail.
【手続補正3】[Procedure 3]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】0010[Correction target item name] 0010
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【0010】 本発明において、前記した積層周期を異
にする部分は、人工格子膜のうち基板側の部分(1)
と、それ以外の部分(2)であり、基板に近接し、人工
格子膜の総膜厚の10%以上80%以下の厚さの部分
(図1における(1)の部分)においては、Co/Pt
(及び/またはPd)の積層周期を短くし、それ以外の
部分(同(2)の部分)ではこれより長くしたことが特
徴である。In the present invention, the portion having a different stacking period is the portion (1) on the substrate side of the artificial lattice film.
When a remaining portion (2), close to the substrate, artificial
In the portion having a thickness of 10% to 80% of the total thickness of the lattice film (portion (1) in FIG. 1), Co / Pt
The stacking period of (and / or Pd) is shortened, and the other portion (portion (2)) is longer than this.
Claims (3)
d層とが交互に積層した人工格子膜を記録層とする光磁
気記録媒体において、前記人工格子膜の、基板側の部分
(1)が他の部分(2)より積層周期が短い人工格子膜
であり、(1)の部分が総膜厚の10%以上80%以下
の厚みであることを特徴とする光磁気記録媒体。1. A Co layer, a Pt layer and / or a P layer on a substrate.
In a magneto-optical recording medium having an artificial lattice film in which d layers are alternately laminated as a recording layer, a portion (1) of the artificial lattice film on the substrate side has a shorter lamination period than other portions (2). And a portion (1) has a thickness of 10% or more and 80% or less of the total film thickness.
子層、Pt:1〜6原子層の人工格子からなる請求項1
記載の光磁気記録媒体。2. The portion (1) comprises an artificial lattice of Co: 0.5 to 1.5 atomic layers and Pt: 1 to 6 atomic layers.
The magneto-optical recording medium described.
〜2.5原子層、Pt:2〜8原子層の人工格子からな
り、かつ(1)の部分のそれより大きい値を採る請求項
1又は2記載の光磁気記録媒体。3. The artificial lattice film, part (2) is Co: 1.
3. The magneto-optical recording medium according to claim 1, comprising an artificial lattice of .about.2.5 atomic layer, Pt: 2 to 8 atomic layer, and having a value larger than that of the portion (1).
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP25864091A JPH0660448A (en) | 1991-09-11 | 1991-09-11 | Magneto-optical recording medium |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP25864091A JPH0660448A (en) | 1991-09-11 | 1991-09-11 | Magneto-optical recording medium |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0660448A true JPH0660448A (en) | 1994-03-04 |
Family
ID=17323081
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP25864091A Pending JPH0660448A (en) | 1991-09-11 | 1991-09-11 | Magneto-optical recording medium |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0660448A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006039225A (en) * | 2004-07-27 | 2006-02-09 | Kyoto Univ | Recording medium, recording method and reproducing method |
-
1991
- 1991-09-11 JP JP25864091A patent/JPH0660448A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006039225A (en) * | 2004-07-27 | 2006-02-09 | Kyoto Univ | Recording medium, recording method and reproducing method |
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