JPH01258249A - Magneto-optical recording medium - Google Patents

Magneto-optical recording medium

Info

Publication number
JPH01258249A
JPH01258249A JP8582188A JP8582188A JPH01258249A JP H01258249 A JPH01258249 A JP H01258249A JP 8582188 A JP8582188 A JP 8582188A JP 8582188 A JP8582188 A JP 8582188A JP H01258249 A JPH01258249 A JP H01258249A
Authority
JP
Japan
Prior art keywords
magneto
magnetic field
recording
optical recording
bias 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.)
Pending
Application number
JP8582188A
Other languages
Japanese (ja)
Inventor
Satoshi Shimokawato
下川渡 聡
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 JP8582188A priority Critical patent/JPH01258249A/en
Publication of JPH01258249A publication Critical patent/JPH01258249A/en
Pending legal-status Critical Current

Links

Landscapes

  • Thin Magnetic Films (AREA)

Abstract

PURPOSE:To enable the execution of recording and erasing at a low bias magnetic field by limiting the ratios of the total rear earths in a thin amorphous alloy film which has the compsn. expressed by the prescribed formula and has the axis of easy magnetization perpendicular to the film plane to a prescribed range. CONSTITUTION:The recording layer is formed of the thin amorphous alloy film having the axis of easy magnetization perpendicular to the film plane and the compsn. ratios of the thin amorphous alloy film are specified to 0<x<=10, 15<=x+y<=40, 0<z<=0.3 by atomic ratios when expressed by the formula I. The saturation bias magnetic field of the C/N is thereby decreased without lowering the C/N and the good recording and erasing are enabled even at the low bias magnetic field.

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わる。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a magneto-optical recording medium used for magneto-optical recording, and in particular to the material of the magneto-optical recording layer.

〔従来の技術〕[Conventional technology]

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、又は樹脂製の円盤状基板と、その上に製膜した記録
層からなり、記録層としてはTbWeJpTbFeoo
、GdTbFe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。これらの膜はキエリー温度が1
00〜200℃と半導体レーザーの収束光による記録、
消去に適しており、又、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。
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 on the substrate.
, GdTbFe, or other amorphous heavy rare earth metal and transition metal amorphous alloy film is used. These films have a Chierie temperature of 1
Recording at 00-200℃ and convergent 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ような欠点がある
。即ち、光磁気記録においては情報の再生はカー効果や
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エリー温度と正
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を大き
くすることができる。ところがキエ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ってしま
うるそこで、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59−1781542)。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。
However, these materials have the following drawbacks. That is, in magneto-optical recording, information is reproduced using the Kerr effect or the Faraday effect, but the magneto-optic effect is very small in these materials. On the other hand, it is empirically known that the magneto-optic effect has a positive correlation with the Chierly temperature of the recording film at the operating temperature. Therefore, the magneto-optic effect can be increased by increasing the Curie temperature of the recording film. However, as the Chierie temperature increases, the laser power required for recording and erasing increases. Therefore, in order to improve this drawback, heavy rare earth
A material in which Sm, a light rare earth element, is added to an iron-based alloy has been proposed (Japanese Unexamined Patent Publication No. 1781542/1983). 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頂〕[The problem that the invention attempts to solve]

しかしながらこの材料には次に示すよ5 jx改善すべ
き問題点が残されている。
However, this material still has some problems that need to be improved as shown below.

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5000e 程度以上のバイアス磁界を記録ピッ
ト周囲に発生させないと、良好な記録を行うことができ
ない。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
料が待望されている。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、磁界変調記録法が提案されて
いるが、この方式においても磁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ソゲする必要からコイルに
高電圧をかけることになる。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程度まで近付けると
、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 about 5000 e is generated around the recording pits. In order to realize smaller size and lower power consumption of recording and reproducing devices, there is a long-awaited material that can record and erase data in a low bias magnetic field. On the other hand, a magnetic 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 magnetic field sensitivity is desirable. That is, when using a conventional magneto-optical recording medium,
High voltage is applied to the coil because it is necessary to switch a large magnetic field at high speed. Furthermore, if the coil is brought closer to the medium surface by several micrometers in order to obtain a high magnetic field at high frequency, 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磁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本光磁気記録媒
体を提供することにある。
The present invention is intended to solve the problems of conventional magneto-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〕[Means to solve the problem]

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薄膜であって、組成を原
子比で、 Nd、z(SmzTbl−2)y(Fe、OO,N1)
10(1−,2;−yと表わしたとき、口<x<10 
y 15<、、x + yり40 、 O(z<:(L
 50であることを特徴とする。
In the magneto-optical recording medium of the present invention, the recording layer is an amorphous thin film having an axis of easy magnetization in a direction perpendicular to the film surface, and has a composition in atomic ratio of Nd, z(SmzTbl-2)y(Fe ,OO,N1)
When expressed as 10(1-,2;-y, mouth<x<10
y15<,,x+yri40,O(z<:(L
It is characterized by being 50.

ここで、IFe、Oo、Niの比率は媒体の記録、再生
条件によってキエリー温度、補償温度等の物性を所望の
値にするため、任意に設定できる。
Here, the ratios of IFe, Oo, and Ni can be arbitrarily set in order to set the physical properties such as Chierly temperature and compensation temperature to desired values depending on the recording and reproducing conditions of the medium.

ただし、この組成系において、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、’ + ’J
 e即ち、膜中の全希土類の比率を15αt%から40
αt%の範囲にする必要がある。
However, in this composition system, '+'J
e, that is, the ratio of the total rare earth in the film is increased from 15αt% to 40%.
It is necessary to keep it within the range of αt%.

〔実施例〕〔Example〕

以下実施例に基づいて本発明の詳細な説明する(実施例
1) Ndao(Smo、1sTbo、as)zs、o(?e
o、asOoo、ts)7t、o  なる組成の非晶質
膜な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を有する直径120mmのポリ
カーボネート基板を用いて作成した。また比較例として
(Smo、zsTba、5s)23.o(’Peo、5
s000.15)77.0の組成の記録膜を有する光磁
気記録媒体を作成した。
The present invention will be described in detail below based on Examples (Example 1) Ndao(Smo, 1sTbo, as)zs,o(?e
A magneto-optical recording medium having an amorphous recording layer having the following composition was fabricated using a polycarbonate substrate with a diameter of 120 mm and having spiral guide grooves with a pitch of 1.6 μm. Also, as a comparative example (Smo, zsTba, 5s) 23. o('Peo, 5
A magneto-optical recording medium having a recording film having a composition of s000.15)77.0 was prepared.

第1図は本実施例のNdSmTb1FeOo(・)と比
較例のSmTbIFθ0o(−)を記録膜とした光磁気
記録媒体の再生a / N比の記録バイアス磁界依存性
を示したものである。本実施例の媒体のo / N比が
約10000で飽和するのに対し、比較例のNdを含有
しない媒体は飽和するのに約300 oe のバイアス
磁界が必要なことがわかる、また、再生a / N比の
値も本発明の実施例の方が約2dB高く再生特性も優れ
ている。
FIG. 1 shows the dependence of the reproduction a/N ratio on the recording bias magnetic field of a magneto-optical recording medium in which the recording film was made of NdSmTb1FeOo(·) of the present example and SmTbIFθ0o(-) of the comparative example. It can be seen that the O/N ratio of the medium of this example saturates at about 10,000, whereas the medium that does not contain Nd of the comparative example requires a bias magnetic field of about 300 oe to saturate. The value of the /N ratio is also approximately 2 dB higher in the example of the present invention, and the reproduction characteristics are also excellent.

(実施例2) Nd、(SmoloTbo、5o)22.o (reo
、aoo□1lL2o)ys、o−x  なる組成にお
いて、Nd量Xを変化させて光磁気記録媒体を作成した
(Example 2) Nd, (SmoloTbo, 5o)22. o (reo
, aoo□1lL2o)ys,ox, magneto-optical recording media were prepared by varying the Nd amount X.

第2図はNd量Xに対して、O/ N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。
FIG. 2 is a plot of the magnitude of the recording bias magnetic field required to saturate the O/N ratio against the Nd amount X.

飽和バイアス磁界はNdiの増加に伴い減少し、x;6
(06%)で最少となった後、増大する。一方、第3図
に示すように光磁気記録媒体の再生0 / N比はx=
8(06%)程度まで斬増した後、急激に低下する。こ
のようなことを総合すると%Ndiとしては10αt%
以下であれば、Nd添加の効果であるところの記録バイ
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。
The saturation bias magnetic field decreases with increasing Ndi, x;6
After reaching the minimum at (06%), it increases. On the other hand, as shown in Figure 3, the reproduction 0/N ratio of the magneto-optical recording medium is x=
After increasing to about 8 (06%), it suddenly decreases. Taking all these things together, %Ndi is 10αt%
If it is below, the reduction in the recording bias magnetic field, which is the effect of Nd addition, can be achieved without deteriorating the reproduced signal.

(実施例3) 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
する光磁気記録媒体を作成した。
(Example 3) As an example of the present invention, a magneto-optical recording medium having a recording film having the composition shown in Table 1 was prepared.

さらに比較のために第2表に示す組成の記録膜を有する
光磁気記録媒体を作成した。
Further, for comparison, magneto-optical recording media having recording films having the compositions shown in Table 2 were prepared.

これらの実施例並びに比較例の記録媒体の0/N比の飽
和に要する記録バイアス磁界とo / N比を第3表に
示す。
Table 3 shows the recording bias magnetic field and O/N ratio required for saturation of the O/N ratio of the recording media of these Examples and Comparative Examples.

第  1  表 第  2  表 第  3  表 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Nα11よりも小さい。またo / N比もNdの
入らないNα11の試料と同等か、それ以上の値が得ら
れる。さらに、希土類の比率が15αt%未満であった
り40αt%を越えると、或いはSmとTbの比率が3
=7を越えた場合やNd#Lが10αt%を越えたとき
、いずれの場合も飽和バイアス磁界の改善は認められる
が、大幅な0/N比の低下を伴うため好ましくないこと
がわかる〔発明の効果〕 以上に述べたように本発明によれば、光磁気記録媒体の
o / N比の低下を伴うことなく、O/N比の飽和バ
イアス磁界の低減を行うことができる。従っ【、低バイ
アス磁界でも良好な記録、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 Table 2 Table 3 The saturation recording bias magnetic fields of the examples of the present invention are all smaller than that of the comparative example Nα11. Moreover, the o/N ratio is equal to or higher than that of the Nα11 sample containing no Nd. Furthermore, if the ratio of rare earths is less than 15αt% or exceeds 40αt%, or the ratio of Sm and Tb is 3
When Nd#L exceeds 7 or when Nd#L exceeds 10αt%, an improvement in the saturation bias magnetic field is recognized in both cases, but it is found that this is not preferable because it is accompanied by a significant decrease in the 0/N ratio [Invention Effects] As described above, according to the present invention, the saturation bias magnetic field of the O/N ratio can be reduced without reducing the O/N ratio of the magneto-optical recording medium. 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.

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

第1図は本発明のNdSmTb”Fe0OIJ(・)と
従来例のSmTbFe0o膜(論)を記録膜とする光磁
気記録媒体のa / N比と記録バイアス磁界の関係を
示す図である。 第2図は本発明のNdr(SmO,10TM、90)2
2.0 (Feo、a。 00G、20)78.0−□を用いた光磁気記録媒体の
N d 量”と飽和バイアス磁界の関係を表わす図であ
る。 第3図は同じ< Hd量:tとG / N比の関係を表
わす図である。 以上 出願人 セイコーエプソン株式会社 代理人 弁理士 上柳雅誉(他1名) 第1図 0    ダ   lO害 Nd量 x(,2矛−/、) 第2図
FIG. 1 is a diagram showing the relationship between the a/N ratio and the recording bias magnetic field of magneto-optical recording media in which the recording film is the NdSmTb"Fe0OIJ (•) of the present invention and the conventional SmTbFe0o film (theory). The figure shows the Ndr(SmO, 10TM, 90)2 of the present invention.
2.0 (Feo, a. 00G, 20) 78.0-□ is a diagram showing the relationship between the amount of N d and the saturation bias magnetic field of the magneto-optical recording medium. This is a diagram showing the relationship between t and G/N ratio. Applicant Seiko Epson Co., Ltd. Agent Patent attorney Masayoshi Kamiyanagi (and one other person) Figure 2

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_x(Sm_zTb_1_−_z)_y(Fe,C
o,Ni)_1_0_0_−_x_−_yと表わしたと
き 0<x≦10 15<x+y≦40 0<z≦0.3 であること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_x(Sm_zTb_1_-_z)_y(Fe,C
o, Ni)_1_0_0_-_x_-_y A magneto-optical recording medium characterized in that 0<x≦10 15<x+y≦40 0<z≦0.3.
JP8582188A 1988-04-07 1988-04-07 Magneto-optical recording medium Pending JPH01258249A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8582188A JPH01258249A (en) 1988-04-07 1988-04-07 Magneto-optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8582188A JPH01258249A (en) 1988-04-07 1988-04-07 Magneto-optical recording medium

Publications (1)

Publication Number Publication Date
JPH01258249A true JPH01258249A (en) 1989-10-16

Family

ID=13869520

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8582188A Pending JPH01258249A (en) 1988-04-07 1988-04-07 Magneto-optical recording medium

Country Status (1)

Country Link
JP (1) JPH01258249A (en)

Similar Documents

Publication Publication Date Title
JPH0123927B2 (en)
JPS59178641A (en) Photomagnetic recording medium
JPS60117436A (en) Magnetooptic storage element
JPH07244876A (en) Magneto-optic recording medium and magneto-optically recording/reproducing method
JPS6131533B2 (en)
JPH01258249A (en) Magneto-optical recording medium
JPS61246946A (en) Photomagnetic recording medium
JPH0316049A (en) Magneto-optical recording medium
JPH01258250A (en) Magneto-optical recording medium
JPH02265048A (en) Magneto-optical recording medium
JPH02265046A (en) Magnetic-optical recording medium
JPH02265047A (en) Magneto-optical recording medium
JPH02216635A (en) Magneto-optical recording medium
JP2921794B2 (en) Magneto-optical disk
JPS6243848A (en) Photomagnetic recording medium
JPH02216637A (en) Magneto-optical recording medium
JPH02216640A (en) Magneto-optical recording medium
JPH02265045A (en) Magneto-optical recording medium
JPH02265049A (en) Magneto-optical recording medium
JPH02216639A (en) Magneto-optical recording medium
JPH02265044A (en) Magneto-optical recording medium
JPH02216636A (en) Magneto-optical recording medium
JPH02265050A (en) Magneto-optical recording medium
JPH01140446A (en) Magneto-optical memory medium
JPH02216638A (en) Magneto-optical recording medium