JPS6083305A - Magneto-optic medium - Google Patents
Magneto-optic mediumInfo
- Publication number
- JPS6083305A JPS6083305A JP19074183A JP19074183A JPS6083305A JP S6083305 A JPS6083305 A JP S6083305A JP 19074183 A JP19074183 A JP 19074183A JP 19074183 A JP19074183 A JP 19074183A JP S6083305 A JPS6083305 A JP S6083305A
- Authority
- JP
- Japan
- Prior art keywords
- rare earth
- rotation angle
- earth element
- substituting
- increased
- 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
Landscapes
- Thin Magnetic Films (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明はレーザー光を用いて情報の記録・再生・消去を
行う光磁気記録に係シ、特にカー回転角を向上きせるこ
とにより性能指数を改善し、再生SZN比あるいはC/
N比を向上させた磁気光学媒体に関す木ものである。[Detailed Description of the Invention] [Field of Application of the Invention] The present invention relates to magneto-optical recording in which information is recorded, reproduced and erased using laser light, and in particular improves the figure of merit by improving the Kerr rotation angle. Then, the reproduction SZN ratio or C/
This is a story about a magneto-optical medium with improved N ratio.
最近高密度、大容量、情報の任意読み出し、書き換え等
が可能な光磁気記録が注目を浴びている。Recently, magneto-optical recording, which has high density, large capacity, and allows arbitrary reading and rewriting of information, has been attracting attention.
光磁気記録においては、膜面に垂直な方向に磁化容易軸
のある磁性薄膜(垂直磁化膜)が用いられ、光ビームに
よって任意の位置に反転磁区を作ることによって、それ
らの1お化の向きに対応して、61”、0”の2値情報
が6己録される。一方、かかる反転記録を行なった2値
信号の読み出しは、通常ポーラ−・カー効果あるいはフ
ァラデー効果を利用して行なう。In magneto-optical recording, a magnetic thin film (perpendicularly magnetized film) with an axis of easy magnetization perpendicular to the film surface is used, and by creating reversal magnetic domains at arbitrary positions with a light beam, the direction of one of them can be changed. Corresponding to this, binary information of 61" and 0" is recorded. On the other hand, the readout of binary signals subjected to such inversion recording is usually carried out using the Polar Kerr effect or the Faraday effect.
従来、仁れらlit、t 截光学媒体として、MnB1
系結晶質膜、希土類−遭移金属系非晶質薄膜、ガーネッ
トに代表される単結晶薄膜等の垂直磁化膜が提案されて
いる。中でも希土類−遷移金属系非晶質薄膜は、結晶粒
界がないので媒体ノイズが小さく、大面積作製が容易で
あることから現在量も有望視されている。これらの希土
類−遷移金属系非晶質薄膜として、Gd Co、G”r
b−cO。Conventionally, MnB1 was used as an optical medium.
Perpendicularly magnetized films have been proposed, such as crystalline films based on rare earth metals, amorphous thin films based on rare earth metals, and single crystal thin films typified by garnet. Among them, rare earth-transition metal-based amorphous thin films have no grain boundaries, have low media noise, and are easy to manufacture over large areas, so their current availability is considered promising. These rare earth-transition metal-based amorphous thin films include Gd Co, G”r
b-cO.
Gd Dy Co、Tb Fe、Tb Gd−Fe、T
b−1)y−Fe、Gd−Tb−Dy−p e 、 T
b −1i’ e −CO、D y−Ii’ e −
Co等の合金系が現在研兇開発され、膜自体のカー回転
角も0.4°と向上してきている。しかし実用化での再
生信号レベル(C/N、?50 d B )を得るには
、これらの合金系で得られるカー回転角では不十分であ
り、更にC/N向上のための膜自体のカー回□転角の向
上が要求されている。Gd Dy Co, Tb Fe, Tb Gd-Fe, T
b-1) y-Fe, Gd-Tb-Dy-pe, T
b -1i' e -CO, D y-Ii' e -
Alloy systems such as Co are currently being developed, and the Kerr rotation angle of the film itself has been improved to 0.4°. However, in order to obtain a reproduced signal level (C/N, -50 dB) for practical use, the Kerr rotation angle obtained with these alloy systems is insufficient, and the film itself must be improved to improve the C/N. There is a demand for improvement in car rotation angle.
本発明の目的はカー回転角が上記合金系よりさ□らに高
く、実用に十分適した再生C/N比が得ら1れる非晶質
磁気光学媒体を提供することにある。:〔発明の概要]
本発明者等は、Fe−希土@2元系非晶質垂直磁化膜に
おいて、カー回転角に評与するFe元素のモーメントを
、FeをCoで置換することによシ太きくシ、さらに1
tt4の構成元素である希土類元素を他種の希土類元素
で置換することにより、カー回転角をさらに改善し、同
時にキュリ一温度を最適化することによシ、再生出力レ
ベルに比例する性能指数v’Nθk (Rは反射率、θ
にはカー回転角)を向上させることを考え、本発明に至
った。An object of the present invention is to provide an amorphous magneto-optic medium which has a Kerr rotation angle higher than that of the above-mentioned alloy systems and which provides a reproduction C/N ratio sufficiently suitable for practical use. : [Summary of the Invention] The present inventors have determined that the moment of the Fe element, which contributes to the Kerr rotation angle, in an Fe-rare earth@binary amorphous perpendicularly magnetized film can be changed by replacing Fe with Co. Shitakikushi, 1 more
By replacing the rare earth element, which is a constituent element of tt4, with another kind of rare earth element, the Kerr rotation angle is further improved, and at the same time, by optimizing the Curie temperature, the figure of merit v, which is proportional to the reproduction output level, is improved. 'Nθk (R is reflectance, θ
The present invention was developed based on the idea of improving the Kerr rotation angle.
本発明の磁気光学媒体は、Tが強磁性体の希土類元素Q
d、Tb、Dyの群から選ばれる2元素。In the magneto-optical medium of the present invention, T is a ferromagnetic rare earth element Q
Two elements selected from the group of d, Tb, and Dy.
からなり、一般式が原子パーセント□で □(Fet−
ICOX)too−aTaで表わされる4元系非晶質垂
直−化膜である。、FeCo T b + FC−〇〇
−Gd三元系においてFeをCOで置換してリッタ時、
カー回転角がli’e : Co=1 : 1の組成附
近で極太を示すことは、Tsunashirna等(J
。The general formula is □(Fet-
It is a quaternary amorphous verticalized film represented by ICOX) too-aTa. , FeCo T b + FC-〇〇-Gd ternary system, when Fe is replaced with CO,
The fact that the Kerr rotation angle becomes extremely thick near the composition of li'e:Co=1:1 is explained by Tsunashirna et al.
.
AI)I)I 、 PhyS 53 (11) (19
82)I)、8175)あるいは辻本等(日本応用磁気
学会誌7 (2+ (1983)p、119)の実験結
果から明らかになっている。AI)I)I, PhyS 53 (11) (19
82) I), 8175) or from the experimental results of Tsujimoto et al. (Journal of the Japanese Society of Applied Magnetics 7 (2+ (1983) p. 119).
しかしこの」易合、カー回転角が大きいところでは保磁
力か小さくなって記録磁化の安定性が悪くなった弘キュ
リ一温度が高ずき゛て、半導体レーザー光では十分++
+2 録出来ない不都合が生じてくる。However, in this case, where the Kerr rotation angle is large, the coercive force decreases and the stability of recorded magnetization deteriorates.
+2 The inconvenience of not being able to record occurs.
そこで実用的には、用いるレーザー光あるいは記録再生
の装置に対して、非晶質垂直磁化膜自体の特性の最適化
が要求される。そこで本発明者等は上m13元系につい
て、先ず(Fet −xCOx)100−@DY”3元
系合金でも1・eをCOで置換することによりカー回転
角が増大することを確認した後、これら上記3元系の構
成元素である希土類元素を他稀希土類元素でさらに置換
する事により、さらにカー回転角を増大し、性能指数を
向上させ、記録ピット径の安定度の目安となる保磁力H
Cと飽和磁化MSの積)(c−MSを増大させ、実用に
適したキュリ一温度を有する非晶質垂直磁化膜を得るこ
とを試み完成した。本発明の4元系合金では、1−〇を
COで置換する量Xは0.1(x≦0.4にする必要が
ある。ここで、co置換によるカー回転角の増大の効果
をよシ顕著にする((はXが0.1よりも大きいことが
好ましく、またx = 0.4より多くなるとキュリ一
温度が230C以上と大きくなり、半導体レーザーによ
る情報書き込みが困難rこなることがらXは0.4以下
にする必要がある。次に希土類元素同志の置換において
は、Fe−C0−Dy系ではI)yの一部をTb9るい
はGdで置換することによシ、Fe−co−Tb系では
Tbの一部をGdあるいはDyで置換することにより、
Fe−Co−Gd系ではGdの一部をTbあるいはDy
で置換することにより、キュリ一温度を変化させ、性能
指数を同等以上にさせて、記録・再生感度を大幅に改善
することが出来る。しかしこれらの希土類同志の置換の
効果を得るためには置換量が1,113を子バー−1−
ント以上であることが望ましい。Therefore, in practice, it is required to optimize the characteristics of the amorphous perpendicularly magnetized film itself for the laser beam or recording/reproducing apparatus used. Therefore, the present inventors first confirmed that the Kerr rotation angle increases by replacing 1·e with CO even in the (Fet -xCOx)100-@DY'' ternary alloy for the m13 element system. By further substituting these rare earth elements, which are constituent elements of the above ternary system, with other rare earth elements, the Kerr rotation angle can be further increased, the figure of merit can be improved, and the coercive force can be used as a measure of the stability of the recording pit diameter. H
The product of C and saturation magnetization MS) (the product of c-MS) was attempted and completed in an attempt to obtain an amorphous perpendicular magnetization film having a Curie temperature suitable for practical use.In the quaternary alloy of the present invention, 1- The amount X by which 〇 is replaced with CO must be 0.1 (x≦0.4. Here, the effect of increasing the Kerr rotation angle due to co substitution becomes more pronounced (((=X is 0.1). It is preferable that it be larger than 1, and if x is larger than 0.4, the Curie temperature will increase to 230C or higher, making it difficult to write information with a semiconductor laser, so X needs to be 0.4 or less. Next, in the substitution of rare earth elements, in the Fe-C0-Dy system, part of I)y is replaced with Tb9 or Gd, and in the Fe-co-Tb system, part of Tb is replaced with Gd. Or by replacing with Dy,
In the Fe-Co-Gd system, part of Gd is replaced by Tb or Dy.
By replacing it with , it is possible to change the Curie temperature, make the figure of merit the same or higher, and greatly improve the recording/reproducing sensitivity. However, in order to obtain the effect of substitution between these rare earth elements, the amount of substitution must be 1,113.
It is desirable that the
また、給十類元素量を示すaの値は、17≦a≦32と
する。875Fこの範囲外の場合は、媒体の非晶質化を
阻害する傾向を生じ、好ましくない。Further, the value of a indicating the amount of the element in the 10th class is 17≦a≦32. 875F outside this range tends to inhibit the amorphization of the medium, which is not preferable.
〔発明の実施例〕 以下、本発り」の−実施ρりを第1図によシ説明する。[Embodiments of the invention] The implementation of this invention will be explained below with reference to FIG.
(Fex−bc oh)ysGdI9Tb6非晶質膜b
<0.4は、所定組成のJ・1 e Co合金、 G
dTb合金を真空中高周波加熱炉で作製し、これらの合
金を用いて、2ン一ス同時蒸着が可能な亀子ビーム蒸着
装置により、a X 10−7’l□rr以下0JK2
UT、膜成長速度3〜5A/5et3の条件で作製した
。第1図の曲線1は(Fe1−bcob)7sG’ts
Tbs非晶質合金のCO置換量に対するカー回転角θに
の変化を示す。(Fex-bc oh)ysGdI9Tb6 amorphous film b
<0.4 is a J・1e Co alloy with a predetermined composition, G
A dTb alloy is produced in a vacuum high-frequency heating furnace, and using a Kameko beam evaporation device capable of two-step simultaneous evaporation, a
It was produced under the conditions of UT and film growth rate of 3 to 5A/5et3. Curve 1 in Figure 1 is (Fe1-bcob)7sG'ts
2 shows the change in the Kerr rotation angle θ with respect to the CO substitution amount of the Tbs amorphous alloy.
図には比較のため(Ji’e1−bcob)rsTb2
5非晶質膜の結果も曲、1112に示しである。図から
明らかなようにXTbを(ンdで置換することによシ、
カー回転角θkをさらに増大出来ることがj:)かる。The figure shows (Ji'e1-bcob)rsTb2 for comparison.
The results for the 5 amorphous film are also shown in section 1112. As is clear from the figure, by replacing XTb with (d),
It can be seen that the Kerr rotation angle θk can be further increased.
一方、反射率几は第1図の実験結果の全組成範囲でほと
んど変わらず、几=52〜55%を示すことから、性能
指数fπ・θにはTbをQdで置換することにより増太
し、再生出力レベルの向上刃・得られる。On the other hand, the reflectance 几 remains almost unchanged over the entire composition range of the experimental results shown in Figure 1, showing 几=52 to 55%, so the figure of merit fπ・θ can be increased by replacing Tb with Qd. , improved playback output level can be obtained.
またキュリ一温度も160〜220Cの範囲で変化した
。壕だTbをJ)yで置換することによっても、性能指
数ff・θkを減少させずに、キュリ一温度を下げ、記
録再生感度を上げることが出来た。同様にしてFe−C
o−Gd、 、[i’e−Co−])yの各々の希土類
元素を他の希土類元素で置換することにより、三元系よ
りも優れた記録・再生特性を示した。The curri temperature also varied in the range of 160 to 220C. By replacing Tb with J)y, it was possible to lower the Curie temperature and increase the recording and reproducing sensitivity without reducing the figure of merit ff·θk. Similarly, Fe-C
By replacing each rare earth element of o-Gd, , [i'e-Co-])y with another rare earth element, recording/reproducing characteristics superior to those of the ternary system were exhibited.
以上の説明から明らかなように、本発明の4元系非晶質
#N、F e −Co T (’l’=Gd、’I’b
、 D>’から選ばれる三元素)において、従来報告さ
れている非晶質垂直磁化膜よりもより大きなカー回転角
θに1及び性能指数V1・θkを得ることが出来、性能
指数を低下させずに、キュリ一温度の最適化も容易で、
その結果、記録・再生感度の良い、優れた磁気光学媒体
が得られることがわかった。As is clear from the above explanation, the quaternary amorphous #N, Fe-CoT ('l'=Gd, 'I'b
, D>'), it is possible to obtain a larger Kerr rotation angle θ of 1 and a figure of merit V1・θk than the conventionally reported amorphous perpendicularly magnetized film, which reduces the figure of merit. It is easy to optimize the temperature of cucumbers without
As a result, it was found that an excellent magneto-optical medium with good recording and reproducing sensitivity could be obtained.
これらの非晶質膜を用いて、多層構造膜媒体の構成層と
することによっても、さらにカー回転角を増大させ、再
生情号レベルを向上させる効果が得られることは明らか
である。It is clear that by using these amorphous films as constituent layers of a multilayer film medium, it is possible to further increase the Kerr rotation angle and improve the reproduced information level.
第1図は(Ii’el−bcOb)75Tb6Gd19
1(Fel−bCob)7s’l’l:+25非晶質膜
におけるカー回転角θにのCO換度(b)依存性を示す
線図である。Figure 1 shows (Ii'el-bcOb)75Tb6Gd19
1(Fel-bCob)7s'l'l:+25 It is a diagram showing the dependence of CO exchange rate (b) on the Kerr rotation angle θ in an amorphous film.
Claims (1)
元素とするとき、一般式CF”1−zcOJloo−a
Taで示≦れる組成を有し、且つ17≦a≦32.0
(x≦0.4であることを特徴とする磁気光学媒体。1. Select T from the group consisting of Gd, Tb, ])y2.
When used as an element, the general formula CF"1-zcOJloo-a
It has a composition shown by Ta≦, and 17≦a≦32.0
(A magneto-optical medium characterized in that x≦0.4.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19074183A JPS6083305A (en) | 1983-10-14 | 1983-10-14 | Magneto-optic medium |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19074183A JPS6083305A (en) | 1983-10-14 | 1983-10-14 | Magneto-optic medium |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6083305A true JPS6083305A (en) | 1985-05-11 |
Family
ID=16262987
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19074183A Pending JPS6083305A (en) | 1983-10-14 | 1983-10-14 | Magneto-optic medium |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6083305A (en) |
Citations (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS508625A (en) * | 1973-05-31 | 1975-01-29 | ||
JPS5552535A (en) * | 1978-10-12 | 1980-04-17 | Nippon Hoso Kyokai <Nhk> | Magnetic recording medium |
JPS5727450A (en) * | 1980-07-23 | 1982-02-13 | Ricoh Co Ltd | Magnetic recording medium |
JPS5873746A (en) * | 1981-10-27 | 1983-05-04 | Kokusai Denshin Denwa Co Ltd <Kdd> | Photomagnetic recording medium |
JPS58159252A (en) * | 1982-03-17 | 1983-09-21 | Canon Inc | Magnetooptic recording medium |
JPS58165306A (en) * | 1982-03-26 | 1983-09-30 | Hitachi Ltd | Vertical magnetic recording medium |
JPS59217249A (en) * | 1983-05-25 | 1984-12-07 | Sony Corp | Photomagnetic recording medium |
JPS6068607A (en) * | 1983-09-14 | 1985-04-19 | Sumitomo Metal Mining Co Ltd | Magnetic thin film recording medium |
-
1983
- 1983-10-14 JP JP19074183A patent/JPS6083305A/en active Pending
Patent Citations (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS508625A (en) * | 1973-05-31 | 1975-01-29 | ||
JPS5552535A (en) * | 1978-10-12 | 1980-04-17 | Nippon Hoso Kyokai <Nhk> | Magnetic recording medium |
JPS5727450A (en) * | 1980-07-23 | 1982-02-13 | Ricoh Co Ltd | Magnetic recording medium |
JPS5873746A (en) * | 1981-10-27 | 1983-05-04 | Kokusai Denshin Denwa Co Ltd <Kdd> | Photomagnetic recording medium |
JPS58159252A (en) * | 1982-03-17 | 1983-09-21 | Canon Inc | Magnetooptic recording medium |
JPS58165306A (en) * | 1982-03-26 | 1983-09-30 | Hitachi Ltd | Vertical magnetic recording medium |
JPS59217249A (en) * | 1983-05-25 | 1984-12-07 | Sony Corp | Photomagnetic recording medium |
JPS6068607A (en) * | 1983-09-14 | 1985-04-19 | Sumitomo Metal Mining Co Ltd | Magnetic thin film recording medium |
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