JPH01258249A - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- 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
Links
- 229910000808 amorphous metal alloy Inorganic materials 0.000 claims abstract description 5
- 230000005415 magnetization Effects 0.000 claims abstract description 4
- 239000010408 film Substances 0.000 claims description 13
- 239000000203 mixture Substances 0.000 claims description 7
- 239000010409 thin film Substances 0.000 claims description 2
- 230000003247 decreasing effect Effects 0.000 abstract 1
- 239000000463 material Substances 0.000 description 10
- 230000000694 effects Effects 0.000 description 6
- 230000000052 comparative effect Effects 0.000 description 5
- 229910052761 rare earth metal Inorganic materials 0.000 description 4
- 230000007423 decrease Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 150000002910 rare earth metals Chemical class 0.000 description 3
- 239000000758 substrate Substances 0.000 description 3
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 230000005374 Kerr effect Effects 0.000 description 1
- 229910052772 Samarium Inorganic materials 0.000 description 1
- 229910052771 Terbium Inorganic materials 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 230000000704 physical effect Effects 0.000 description 1
- 229920000515 polycarbonate Polymers 0.000 description 1
- 239000004417 polycarbonate Substances 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
- 229910052723 transition metal Inorganic materials 0.000 description 1
- 150000003624 transition metals Chemical class 0.000 description 1
Landscapes
- Thin Magnetic Films (AREA)
Abstract
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.
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.
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%.
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.
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)
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.
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) |
-
1988
- 1988-04-07 JP JP8582188A patent/JPH01258249A/en active Pending
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