JPH02216636A - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- Publication number
- JPH02216636A JPH02216636A JP3539589A JP3539589A JPH02216636A JP H02216636 A JPH02216636 A JP H02216636A JP 3539589 A JP3539589 A JP 3539589A JP 3539589 A JP3539589 A JP 3539589A JP H02216636 A JPH02216636 A JP H02216636A
- Authority
- JP
- Japan
- Prior art keywords
- magneto
- recording medium
- recording
- film
- optical 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
- 239000000203 mixture Substances 0.000 claims abstract description 14
- 229910052777 Praseodymium Inorganic materials 0.000 claims abstract description 6
- 239000010408 film Substances 0.000 claims abstract 5
- 239000010409 thin film Substances 0.000 claims abstract 2
- 229910000808 amorphous metal alloy Inorganic materials 0.000 claims description 2
- 230000005415 magnetization Effects 0.000 claims description 2
- 229910052761 rare earth metal Inorganic materials 0.000 abstract description 5
- 229910052742 iron Inorganic materials 0.000 abstract description 3
- 229910052759 nickel Inorganic materials 0.000 abstract description 3
- 230000000704 physical effect Effects 0.000 abstract description 2
- 239000005300 metallic glass Substances 0.000 abstract 1
- 239000000463 material Substances 0.000 description 9
- 230000000052 comparative effect Effects 0.000 description 6
- 230000000694 effects Effects 0.000 description 6
- 230000003287 optical effect Effects 0.000 description 6
- 229910052779 Neodymium Inorganic materials 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 230000007423 decrease Effects 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 229910052692 Dysprosium Inorganic materials 0.000 description 2
- 229910052688 Gadolinium Inorganic materials 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- 229910000640 Fe alloy Inorganic materials 0.000 description 1
- 230000005374 Kerr effect Effects 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 239000002178 crystalline material Substances 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- XEEYBQQBJWHFJM-UHFFFAOYSA-N iron Substances [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 1
- 229920000515 polycarbonate Polymers 0.000 description 1
- 239000004417 polycarbonate Substances 0.000 description 1
- 150000002910 rare earth metals Chemical class 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 229920006395 saturated elastomer 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J
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する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application J] The present invention relates to a magneto-optical recording medium used for magneto-optical recording, 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Iit!i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、TbF
eCo、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100〜200℃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、
MnB1等結晶材料の欠点である粒界ノイズがなく光m
黒記録材料としては望ましい特性を備久ている。[Prior Art] Conventionally known optical Iit! The i-recording medium consists of a disk-shaped substrate made of glass or resin having guide grooves and a recording layer formed thereon.
An amorphous alloy film of an amorphous heavy rare earth such as eCo or GdFeCo and a transition metal is used. These films have a Curie temperature of 100 to 200°C, making them suitable for recording and erasing using focused light from a semiconductor laser, and since they are amorphous,
There is no grain boundary noise, which is a drawback of crystalline materials such as MnB1, and light m
It has desirable properties as a black recording material.
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を
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、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, the magneto-optic effect can be increased by increasing the Curie temperature of the recording film. However, as the Curie temperature rises, the laser power required for recording and erasing increases. Therefore, in order to improve such drawbacks, a material in which a light rare earth element Sm is added to a heavy rare earth-iron alloy has been proposed. (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]
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。[Problems to be Solved by the Invention] However, this material still has the following problems that should be improved.
光6R気記録においては清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、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。In optical 6R recording, a bias magnetic field is required to record the 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 magnetic field modulation recording method has been proposed as a method for realizing overwriting in magneto-optical recording, but even in this method, it is desirable to use a recording medium with high m-field sensitivity. 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1if1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。The present invention is intended to solve the problems of the conventional optical 1if1 recording medium, and its purpose is to:
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 object of the present invention is to provide a magneto-optical recording medium that can perform good recording and erasing even with a low bias magnetic field.
[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、
fNd、Pr)x fsm*fDyGdl+−!ly
fFe、Go、Ni)100−++−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。[Means for Solving the Problems 1] The magneto-optical recording medium of the present invention is such that the recording layer is an amorphous film having an axis of easy magnetization in a direction perpendicular to the film surface, and has a composition in atomic ratio of fNd, Pr. )x fsm*fDyGdl+-! ly
fFe, Go, Ni) When expressed as 100-++-y, 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印化
膿であるためには、(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 achieve the perpendicular impurity, 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] 以下実施例に基づいて本発明の詳細な説明する。〔Example] The present invention will be described in detail below based on Examples.
(実施例1)
fNdo、 5Pro、 sl m、 o fs、ma
、 l ! fDyGdl O,ssl *s 。(Example 1) fNdo, 5Pro, sl m, o fs, ma
, l! fDyGdl O,ssl *s.
IFeo、 ascOo、 +8171. oなる組成
の非晶質膜を記BN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製した。IFeo, ascOo, +8171. A magneto-optical recording medium having an amorphous film with a composition of BN and a thickness of 1.6 μm
Diameter 120mm with pitch spiral guide groove
It was made using a polycarbonate substrate.
また、比較例としてfsmo、 Ill (DyGdl
0.88123゜fFeo、 ascOa、 +sl
??、 (lの組成の記録膜を有する光6n気記録媒
体を作製した。In addition, as a comparative example, fsmo, Ill (DyGdl
0.88123゜fFeo, ascOa, +sl
? ? An optical recording medium having a recording film having a composition of , (l) was prepared.
第1図は、本実施例のNdPrSmDyGdF e C
o (O)と比較例のSmDyGdFeC。FIG. 1 shows the NdPrSmDyGdF e C of this example.
o (O) and SmDyGdFeC as a comparative example.
(×)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。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、Prを含有しない光磁気記録媒体
は飽和するのに約3000e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(再生特性も優れて
いる。(x) indicates the dependence of the reproduction CN ratio on the recording bias magnetic field of a magneto-optical recording medium with a recording film. It can be seen that the CN ratio of the magneto-optical recording medium of this example is saturated at about 7000e, whereas the magneto-optical recording medium of the comparative example that does not contain Nd or Pr requires a bias magnetic field of about 3000e to reach saturation. . Furthermore, the reproduction CN ratio of the magneto-optical recording medium according to the embodiment of the present invention is about 2 dB higher (the reproduction characteristics are also superior).
(実施例2)
(Nda、 5Pro、 41 It (Smo、1o
(DyGdl O,sol z*、 o fFeo、
a。(Example 2) (Nda, 5Pro, 41 It (Smo, 1o
(DyGdl O, sol z*, o fFeo,
a.
Coo、 20) qa、 o−++なる組成において
、N d P r Nxを変化させて光磁気記録媒体を
作製した。第2図はNdPrMx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NdPrfix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
CN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。Coo, 20) Magneto-optical recording media were fabricated by changing NdPrNx in the composition qa, o-++. FIG. 2 is a plot of the magnitude of the recording bias magnetic field required for saturation of the CN ratio with respect to NdPrMx. The saturation bias magnetic field decreases as NdPrfix increases, reaches a minimum at x=6 (at%), and then increases. On the other hand, as shown in FIG. 3, the reproduction CN ratio of the magneto-optical recording medium gradually increases to about 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)
(NdPr添加−Ill S、 o (Smo、 +o
fDyGdl O,sol *z、 o fFeo、
a。(Example 3) (NdPr addition-Ill S, o (Smo, +o
fDyGdl O,sol *z, o fFeo,
a.
Coo、 z。)フ、。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。Coo, z. )centre,. In the composition, Nd and Pr
Magneto-optical recording media were fabricated by changing the amount ratio a.
第4図はN d @ aに対して、CN比の飽和に必要
な記録バイアス6fl界の大きさを表したものである。FIG. 4 shows the magnitude of the recording bias 6fl field necessary for saturation of the CN ratio with respect to N d @a.
飽和バイアス磁界は全域にわたってNdのみの場合やP
r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m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。The saturation bias magnetic field is applied over the entire area in the case of only Nd or in the case of P.
It can be seen that by mixing both Nd and Pr elements, recording and erasing with a smaller applied m field and a larger magneto-optic effect can be obtained than when using each element alone. .
(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1ift界とCN比を第3
表に示した。The recording bias 1if field and CN ratio required for saturation of the CN ratio of the magneto-optical recording media of these examples and comparative examples are
Shown in the table.
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P
r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、Sm
と(DyGd)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 number 6, and the CN ratio is also
A value equal to or higher than that of Comparative Example Sample No. 6 without r is obtained. Furthermore, the ratio of total rare earths is 15 (
at%) or more than 40 (at%), Sm
Although an improvement in the saturation bias magnetic field is observed in both cases where the ratio of (DyGd) and (DyGd) 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 involves a decrease in the CN ratio.
尚、重希土類元素であるDyとGdの比率の相違が、光
磁気記録媒体の特性に影響を及ぼさない。従って1本実
施例においては、DyとGdの比率は同等限定されるも
のではない。Note that the difference in the ratio of heavy rare earth elements Dy and Gd does not affect the characteristics of the magneto-optical recording medium. Therefore, in this embodiment, the ratio of Dy and Gd is not limited to the same 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.
第1図は、本発明の実施例におけるNdPrSmDyG
dFeCo膜と従来例のSmDyGdFeCo膿を記録
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1本発明の(Ndo、 aPro、 al *
fsmafDyGdl o、 sol it、 o
(Feo、 aocOo、 sol ts−++を用い
た光ui気記録媒体の(NdPr)量Xと飽和バイアス
611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、(NdaPr+−at s、 o fsmo
、 l o foycdl O,5atzz、 o f
Feo、 aacOo、 aol ts、 aなる組成
式においてNd量aとCN比の関係を示す図。
1− ・NdPrSmDyGdFeCo組成のバイアス
磁界(Oe)
第1図
記録膜。
SmDyGdFeCo組成の記録膜。
出願人 セイコーエプソン株式会社
代理人 弁理士 上 m 雅 誉(他1名)NdPr量
、X(at%)
第2図
NdPr量、X(at%)
Nd量比、aFIG. 1 shows NdPrSmDyG in an embodiment of the present invention.
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 dFeCo film and a conventional SmDyGdFeCo film as a recording film. FIG. 2 shows one of the present invention (Ndo, aPro, al*
fsmafDyGdl o, sol it, o
(A diagram showing the relationship between the (NdPr) amount A diagram showing the relationship.
, l o foycdl O,5azz, of
A diagram showing the relationship between the Nd amount a and the CN ratio in the composition formula Feo, aacOo, aol ts, a. 1- Bias magnetic field (Oe) of NdPrSmDyGdFeCo composition Figure 1 Recording film. Recording film with SmDyGdFeCo composition. Applicant Seiko Epson Co., Ltd. Agent Patent Attorney 1. Masa Homare (1 other person) NdPr amount, X (at%) Figure 2 NdPr amount, X (at%) Nd amount ratio, a
Claims (1)
であって、組成を原子比で、 (Nd,Pr)x(Smz(DyGd)1−z)y(F
e,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(Smz(DyGd)1-z)y(in atomic ratio) F
A magneto-optical recording medium characterized in that, when expressed as _1_0_0_-_x_-_y, 0<x≦10 15≦x+y≦40 0<z≦0.3.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3539589A JPH02216636A (en) | 1989-02-15 | 1989-02-15 | Magneto-optical recording medium |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3539589A JPH02216636A (en) | 1989-02-15 | 1989-02-15 | Magneto-optical recording medium |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02216636A true JPH02216636A (en) | 1990-08-29 |
Family
ID=12440733
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3539589A Pending JPH02216636A (en) | 1989-02-15 | 1989-02-15 | Magneto-optical recording medium |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02216636A (en) |
-
1989
- 1989-02-15 JP JP3539589A patent/JPH02216636A/en active Pending
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