JPH02216637A - Magneto-optical recording medium - Google Patents

Magneto-optical recording medium

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Publication number
JPH02216637A
JPH02216637A JP3539689A JP3539689A JPH02216637A JP H02216637 A JPH02216637 A JP H02216637A JP 3539689 A JP3539689 A JP 3539689A JP 3539689 A JP3539689 A JP 3539689A JP H02216637 A JPH02216637 A JP H02216637A
Authority
JP
Japan
Prior art keywords
magneto
recording medium
optical recording
film
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
Application number
JP3539689A
Other languages
Japanese (ja)
Inventor
Tadashi Mizutani
水谷 正
Satoshi Shimokawato
下川渡 聡
Masaya Ishida
方哉 石田
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.)
Seiko Epson Corp
Original Assignee
Seiko Epson Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP3539689A priority Critical patent/JPH02216637A/en
Publication of JPH02216637A publication Critical patent/JPH02216637A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain a magneto-optical recording medium which enables good recording/erasing even in a low bias magnetic field by constituting the recording layer of a specific amorphous metal thin film having the easily magnetizing axis perpendicular to the film surface. CONSTITUTION:The magneto-optical recording medium has the recording layer of an amorphous film having the easily magnetizing axis perpendicular to the surface thereof and the composition expressed by (Nd,Pr)x(SmzGd1-z)y(Fe, Co, Ni)100-x-y, wherein x, y and z satisfy the formula I. Proportions of the amounts of Fe, Co and Ni can be arbitrarily controlled according to the conditions of recording/erasing for the medium so as to obtain desired values of physical properties such as Curie temp. and compensation temp. However, to obtain a perpendicularly magnetized film, which is the requirement for the magneto- optical recording medium, from the composition above described, it is necessary to make the proportion of total rare earth elements (x+y) in the film in the range from 15at.% to 40at.%. Thus, the obtd. recording medium enables good recording/erasing even in a low bias magnetic field.

Description

【発明の詳細な説明】 〔産業上の利用分野1 本発明は、光m気配縁に用いられる光磁気記録媒体に関
するもので、特に、その光磁気記録層の材料に関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application 1] The present invention relates to a magneto-optical recording medium used for optical alignment, and in particular to a material for a magneto-optical recording layer thereof.

[従来の技術] 従来公知である光磁気記録媒体は、案内溝を有するガラ
ス、または樹脂製の円盤状基板と、その上に成膜した記
録層から成り、記録層としてはTbFe、TbFeCo
、GdFeCo等の非晶質の重希土類と遷移金属の非晶
質合金膜が用いられる。これらの膜はキュリー温度が1
00〜200℃と半導体レーザーの集束光による記録・
消去に適しており、また非晶質であることから、MnB
1等結晶材料の欠点である粒界ノイズがなく光磁気記録
材料としては望ましい特性を備えている。
[Prior Art] A conventionally known magneto-optical recording medium consists of a disk-shaped substrate made of glass or resin having a guide groove and a recording layer formed thereon.
, GdFeCo, or other amorphous heavy rare earth and transition metal amorphous alloy films are used. These films have a Curie temperature of 1
Recording at 00 to 200℃ and using focused light from a semiconductor laser.
MnB is suitable for erasing and is amorphous.
It has desirable characteristics as a magneto-optical recording material without grain boundary noise, which is a drawback of primary crystal materials.

しかしながら、これらの材料には次の様な欠点がある。However, these materials have the following drawbacks.

即ち、光磁気記録においては情報の再生はカー効果もし
くはファラデー効果を用いて行われるが、これらの材料
においてはこの磁気光学効果が非常に小さい、一方、磁
気光学効果は動作温度においては記録膜のキュリー温度
と正の相関が経験的に知られている。したがって、記録
膜のキュリー温度を高めることによって磁気光学効果な
大きくすることができる。ところが、キュリー温度が高
くなると記録・消去に必要なレーザーパワーが高くなる
。そこで2このような欠点を改善するために重希土−鉄
系合金に軽希土類元素のSmを添加した材料が提案され
ている。(特開昭59−178641)この材料によっ
て記録感度を低下せしめることなく、光再生特性を向上
させることができる。
That is, in magneto-optical recording, information is reproduced using the Kerr effect or the Faraday effect, but this magneto-optic effect is extremely small in these materials. It is empirically known that there is a positive correlation with the Curie temperature. Therefore, by increasing the Curie temperature of the recording film, the magneto-optic effect can be increased. However, as the Curie temperature rises, the laser power required for recording and erasing increases. Therefore, in order to improve these drawbacks, a material has been proposed in which a light rare earth element, Sm, is added to a heavy rare earth-iron alloy. (Japanese Unexamined Patent Publication No. 59-178641) With this material, optical reproduction characteristics can be improved without reducing recording sensitivity.

〔発明が解決しようとする課題1 しかしながら、この材料には次に示すような改善すべき
問題点が残されている。
[Problem to be Solved by the Invention 1] However, this material still has the following problems to be improved.

光磁気記録においては情報の記録のためにはバイアス磁
界を必要とする。このような材料を記録層に用いた場合
、最低3000e程度以上のバイアス磁界を記録ビット
周囲に印加させないと、良好な記録を行うことができな
い、また、記録・再生装置の小型化・低消費電力化を実
現するためには、低バイアス磁界での記録・消去が可能
な材料が要求されている。一方、光磁気記録における重
ね書きを実現する方法として1ga界変調記録法が提案
されているが、この方式においてもm場感度の高い記録
媒体が望ましい、即ち、従来の光磁気記録媒体を用いた
場合、大きな磁界を高速でスイッチングする必要からコ
イルに高電圧を印加することになる。さらに、高磁界を
高周波で得るためにコイルを媒体面より数μm程度まで
近づけると、光磁気記録の光メモリーとしての利点の大
半を失うことになる。
Magneto-optical recording requires a bias magnetic field to record information. When such a material is used for the recording layer, good recording cannot be performed unless a bias magnetic field of at least 3000e or more is applied around the recording bit.In addition, it is necessary to miniaturize and reduce power consumption of recording and reproducing devices. In order to achieve this, materials that can be recorded and erased in a low bias magnetic field are required. On the other hand, a 1 ga field modulation recording method has been proposed as a method for realizing overwriting in magneto-optical recording, but even in this method, a recording medium with high m-field sensitivity is desirable. In this case, a high voltage is applied to the coil because it is necessary to switch a large magnetic field at high speed. Furthermore, in order to obtain a high magnetic field at high frequency, if the coil is brought closer to the surface of the medium by several micrometers, most of the advantages of magneto-optical recording as an optical memory will be lost.

本発明はこのような従来の光…気記録媒体の課題を解決
するもので、その目的とするところは、低バイアス磁界
でも良好な記録・消去を行うことができる光磁気記録媒
体を提供するところにある。
The present invention is intended to solve the problems of conventional optical optical recording media, and its purpose is to provide a magneto-optical recording medium that can perform good recording and erasing even in a low bias magnetic field. It is in.

〔課題を解決するための手段1 本発明の光磁気記録媒体は、記録層が膜面と垂直な方向
に磁化容易軸を有する非晶質膜であって、組成を原子比
で。
[Means for Solving the Problems 1] In the magneto-optical recording medium of the present invention, the recording layer is an amorphous film having an axis of easy magnetization in a direction perpendicular to the film surface, and the composition is expressed in atomic ratio.

fNd、Pr1x fsmxcd+−5ly fFe、
Go、Nil 160−X−11と表した時、 0<x≦10 15≦x+y≦40 0<z≦0.3 である事を特徴とする。
fNd, Pr1x fsmxcd+-5ly fFe,
When expressed as Go, Nil 160-X-11, it is characterized by the following: 0<x≦10 15≦x+y≦40 0<z≦0.3.

ここで、Fe、Co、Niの比率は媒体の記録・再生条
件によって、キュリー温度及び補償温度等の物性、を所
望値にするため、任意に設定できる。但し、この組成系
においては光磁気記録媒体として必要条件である垂直磁
化膜であるためには、(x+y)即ち膜中の全希土類の
比率を15at%から40at%の範囲にする必要があ
る。
Here, the ratios of Fe, Co, and Ni can be arbitrarily set depending on the recording/reproducing conditions of the medium in order to set physical properties such as Curie temperature and compensation temperature to desired values. However, in this composition system, in order to obtain a perpendicularly magnetized film, which is a necessary condition for a magneto-optical recording medium, it is necessary that (x+y), that is, the ratio of the total rare earth elements in the film, be in the range of 15 at % to 40 at %.

〔実 施 例1 以下実施例に基づいて本発明の詳細な説明する。[Implementation example 1] The present invention will be described in detail below based on Examples.

(実施例1) (Ndo、 5Pro、 sl a、 o fsmoI
sGdo、 115123. OIFeo、 asc。
(Example 1) (Ndo, 5Pro, sla, o fsmoI
sGdo, 115123. OIFeo, asc.

。1slff1.oなる組成の非晶質膜を記録層とする
光磁気記録媒体を1.6μmピッチのスパイラル状の案
内溝な有する直径120mmのポリカーボネート基板を
用いて作製した。また、比較例としてfsmo、 +5
Gdo、 ss) 2s、 a fFeo、 ss(:
Oo、 +sl ??、 oの組成の記!!膜を有する
光磁気記録媒体を作製した。
. 1slff1. A magneto-optical recording medium having an amorphous film having a composition as a recording layer was fabricated using a polycarbonate substrate having a diameter of 120 mm and having spiral guide grooves with a pitch of 1.6 μm. Also, as a comparative example, fsmo, +5
Gdo, ss) 2s, a fFeo, ss(:
Oo, +sl? ? , A record of the composition of o! ! A magneto-optical recording medium having a film was fabricated.

第1図は1本実施例のNdPrSmGdFeCo(○)
と比較例のSmGdFeCo (x)を記録膜とした光
磁気記録媒体の再生CN比の記録バイアス磁界依存性を
示したものである6本実施例の光磁気記録媒体のCN比
が約7000eで飽和するのに対し、比較例のNd、P
rを含有しない光6t1気記録媒体は飽和するのに約3
000eのバイアス磁界が必要なことがわかる。また、
再生CN比も本発明の実施例における光磁気記録媒体の
方が約2dB高く再生特性も優れている6(実施例2) fNdo、 gPra、 41 X (Sn+o、 l
 oGdo、 eat 2□、 o (Feo、 so
c。
Figure 1 shows one example of NdPrSmGdFeCo (○).
The CN ratio of the magneto-optical recording medium of this example is saturated at about 7000e. In contrast, Nd, P in the comparative example
It takes about 3 to saturate a recording medium that does not contain r.
It can be seen that a bias magnetic field of 000e is required. Also,
The reproduction CN ratio is also about 2 dB higher in the magneto-optical recording medium in the example of the present invention, and the reproduction characteristics are also excellent6 (Example 2) fNdo, gPra, 41 X (Sn+o, l
oGdo, eat 2□, o (Feo, so
c.

。2ot ?a。□なる組成において、NdPr量Xを
変化させて光磁気記録媒体を作製した。
. 2ot? a. Magneto-optical recording media were fabricated with a composition of □ while varying the NdPr amount X.

第2図はN d P r @ xに対して、CN比の飽
和に要する記録バイアス磁界の大きさをプロットしたも
のである。飽和バイアス磁界はNdPr量Xの増加に伴
い減少し、x=6 (at%)で最小となった後、増大
する。一方、第3図に示す様に光磁気記録媒体の再生C
N比はx=8 (at%)程度まで漸増した後、急激に
低下する。この様なことを総合するとNdPr量として
は10(at%)以下であれば、NdPr添加の効果で
あるところの記録消去バイアス磁界の減少を再生信号の
劣化を伴わずに実現することができる。
FIG. 2 is a plot of the magnitude of the recording bias magnetic field required to saturate the CN ratio versus N d P r @x. The saturation bias magnetic field decreases as the NdPr amount X increases, reaches a minimum at x=6 (at%), and then increases. On the other hand, as shown in FIG.
The N ratio gradually increases to approximately x=8 (at%), and then rapidly decreases. Taking all of these things into account, if the amount of NdPr is 10 (at%) or less, the reduction in the recording/erasing bias magnetic field, which is the effect of adding NdPr, can be achieved without deteriorating the reproduced signal.

(実施例3) fNd、Pr 1−ale、 o (Srao、 + 
aGdo、 sol **、 o (FeI、、 so
c。
(Example 3) fNd, Pr 1-ale, o (Srao, +
aGdo, sol **, o (FeI,, so
c.

。2゜)2.。なる組成において、NdとPrの量比a
を変化させて光磁気記録媒体を作製した。
. 2゜)2. . In the composition, the amount ratio a of Nd and Pr is
Magneto-optical recording media were fabricated by varying the

第4図はN d Iaに対して、CN比の飽和に必要な
記録バイアス磁界の大きさを表したものである。飽和バ
イアス磁界は全域にわたってNdのみの場合やPrのみ
の場合よりも小さく、NdとPrの両方の元素を混合す
ることによって、各々を単独で用いるよりもより小さな
印加磁場での記録及び消去とより大きな磁気光学効果が
得られる事がわかる。
FIG. 4 shows the magnitude of the recording bias magnetic field necessary for saturation of the CN ratio with respect to N d Ia. The saturation bias magnetic field is smaller than that for Nd only or Pr only over the entire range, and by mixing both Nd and Pr elements, recording and erasing with smaller applied magnetic fields than using each element alone is possible. It can be seen that a large magneto-optical effect can be obtained.

(実施例4) 本発明の実施例として、第1表に示した組成の記録膜を
有する磁性膜を作製した。
(Example 4) As an example of the present invention, a magnetic film having a recording film having the composition shown in Table 1 was produced.

更に、比較のために第2表に示す組成の記録膜を有する
光磁気記録媒体を作製した。
Furthermore, for comparison, a magneto-optical recording medium having a recording film having the composition shown in Table 2 was prepared.

これらの実施例並びに比較例の光磁気記録媒体のCN比
の飽和に要する記録バイアス磁界とCN比を第3表に示
した。
Table 3 shows the recording bias magnetic field and CN ratio required for saturation of the CN ratio of the magneto-optical recording media of these Examples and Comparative Examples.

本発明の実施例の飽和記録バイアス磁界はいずれも比較
例試料番号6よりも小さい、また、CN°比もNd及び
Prの入らない比較例試料番号6と同等もしくは、それ
以上の値が得られている。更に、全希土類の比率が15
(at%)未満もしくは40(at%)を超えたり、S
mとGdの比率が3ニアを超えてSmが多く含有してい
る場合やNd、Pr量が10(at%)を超えたいずれ
の場合も飽和バイアス磁界の改善は認められるものの、
大幅なCN比の低下を伴うため好ましくないことがわか
る。
The saturation recording bias magnetic fields of the examples of the present invention are all smaller than that of Comparative Example Sample No. 6, and the CN° ratio is equal to or higher than that of Comparative Example Sample No. 6, which does not contain Nd and Pr. ing. Furthermore, the total rare earth ratio is 15
(at%) or more than 40 (at%), S
Although an improvement in the saturation bias magnetic field is observed in both cases where the ratio of m and Gd exceeds 3 nia and a large amount of Sm is contained, and when the amount of Nd and Pr exceeds 10 (at%),
It can be seen that this is not preferable because it is accompanied by a significant decrease in the CN ratio.

第1表 第  3  表 第2表 [発明の効果] 以上に述べた様に本発明によれば、光磁気記録媒体のC
N比の低下を伴うことなく、CN比の飽和バーイアス磁
界の低減を行うことができる。従って、低バイアス磁界
でも良好な記録及び、消去が可能な高性能な光磁気記録
媒体を供することができる。
Table 1 3 Table 2 [Effects of the invention] As described above, according to the present invention, the C
The saturation bias magnetic field of the CN ratio can be reduced without reducing the N ratio. Therefore, it is possible to provide a high-performance magneto-optical recording medium that can perform good recording and erasing even with a low bias magnetic field.

SmGdFeCo組成の記録膜。Recording film with SmGdFeCo composition.

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

第1図は、本発明の実施例におけるNdPrSmGdF
eCo膜と従来例のSmGdFeC。 模を記録膜とする光磁気記録媒体のCN比と記録バイア
ス磁界の関係を示す図。 第2図は、本発明の1Nda、 5Pro、 4)If
 [5IIC+、 +oGdo、 eo)as、 o 
(Fe0. aocOo、 sol ?a−xを用いた
光磁気記録媒体の(NdPrl量Xと飽和バイアス磁界
の関係を示す図。 第3図は、同じ< (NdPr)量XとCN比の関係を
示す図。 第4図は、fNdaPr+−ala。(smo、+oG
da、sol ax。 IFeo、 aacrQa、 xJ yi、 oなる組
成式においてN d l aとCN比の関係を示す図。
FIG. 1 shows NdPrSmGdF in an embodiment of the present invention.
eCo film and conventional SmGdFeC. FIG. 3 is a diagram showing the relationship between the CN ratio and the recording bias magnetic field of a magneto-optical recording medium using a mirror as a recording film. Figure 2 shows 1Nda, 5Pro, 4) If of the present invention.
[5IIC+, +oGdo, eo) as, o
A diagram showing the relationship between the (NdPrl amount X and the saturation bias magnetic field) of a magneto-optical recording medium using (Fe0. Figure 4 shows fNdaPr+-ala. (smo, +oG
da, sol ax. The figure which shows the relationship between Ndla and CN ratio in the composition formula of IFeo, aacrQa, xJ yi, o.

Claims (1)

【特許請求の範囲】 膜面と垂直な方向に磁化容易軸を有する非晶質合金薄膜
であって、組成を原子比で、 (Nd,Pr)x(SmzGd1−z)y(Fe,Co
,Ni)_1_0_0_−_x_−_yと表した時、 0<x≦10 15≦x+y≦40 0<z≦0.3 である事を特徴とする光磁気記録媒体。
[Claims] An amorphous alloy thin film having an axis of easy magnetization perpendicular to the film surface, the composition of which is (Nd,Pr)x(SmzGd1-z)y(Fe,Co) in atomic ratio.
, Ni)_1_0_0_-_x_-_y, a magneto-optical recording medium characterized in that, when expressed as 0<x≦10 15≦x+y≦40 0<z≦0.3.
JP3539689A 1989-02-15 1989-02-15 Magneto-optical recording medium Pending JPH02216637A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3539689A JPH02216637A (en) 1989-02-15 1989-02-15 Magneto-optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3539689A JPH02216637A (en) 1989-02-15 1989-02-15 Magneto-optical recording medium

Publications (1)

Publication Number Publication Date
JPH02216637A true JPH02216637A (en) 1990-08-29

Family

ID=12440763

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3539689A Pending JPH02216637A (en) 1989-02-15 1989-02-15 Magneto-optical recording medium

Country Status (1)

Country Link
JP (1) JPH02216637A (en)

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