JPS60130806A - Amorphous magnetooptical layer - Google Patents

Amorphous magnetooptical layer

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Publication number
JPS60130806A
JPS60130806A JP23898283A JP23898283A JPS60130806A JP S60130806 A JPS60130806 A JP S60130806A JP 23898283 A JP23898283 A JP 23898283A JP 23898283 A JP23898283 A JP 23898283A JP S60130806 A JPS60130806 A JP S60130806A
Authority
JP
Japan
Prior art keywords
film
rotation angle
kerr rotation
amorphous
coercive force
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
JP23898283A
Other languages
Japanese (ja)
Inventor
Motoharu Tanaka
元治 田中
Atsuyuki Watada
篤行 和多田
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.)
Ricoh Co Ltd
Original Assignee
Ricoh Co Ltd
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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP23898283A priority Critical patent/JPS60130806A/en
Publication of JPS60130806A publication Critical patent/JPS60130806A/en
Pending legal-status Critical Current

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  • Thin Magnetic Films (AREA)

Abstract

PURPOSE:To obtain an amorphous magnetooptical layer having the large Kerr rotation angle thetak, and moreover having large coercive force Hc by a method wherein copper or chromium of the specified quantity is contained in a Dy-Fe film having the direction of easy magnetization in the direction perpendicular to the film surface. CONSTITUTION:A Dy-Fe-Cu film or a Dy-Fe-Cr film containing Cu or Cr of at least 0.5atom% is formed according to the sputtering method, etc. on a non-magnetic substance consisting of glass, plastics, ceramics, etc. A Dy chip and a Cu or Cr chip are put on an Fe disk to construct a target using the composite method, for example, and composition is controlled according to the ratio of the surface area of the target. Because sufficient Kerr rotation angle can not be obtained when content of Cu or Cr is less than 0.5atom%, while coercive force Hc and the Kerr rotation angle thetak become small when content is enlarged too much, the range of 0.5-5atom% is desirable.

Description

【発明の詳細な説明】 〔技術分野〕 本発明は光磁気記録媒体に用いられる非晶質磁気光学層
に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to an amorphous magneto-optic layer used in a magneto-optical recording medium.

〔従来技術〕[Prior art]

従来、磁気光学ディスク、磁気バブルメモリーなどに用
いられる膜面と垂直な方向に磁化容易軸を有する強磁性
薄膜としてはMnB1に代表される多結晶金属薄膜、G
a−00%Gd−Feの非晶質金属薄膜、 GIGに代
表される化合物単結晶薄膜が知られている。これらの薄
膜は種々の利点を有するが、MnB1はキューリ一点が
高いために薄膜の作製が技術的に困難であり、また磁気
光学ディスクに利用した場合書き込みに大きなエネルギ
ーを必要とするという欠点がある。また、Gd−Co 
、 Gd−Feの非晶質金属薄膜は室温における保磁力
が小さく (300〜5000e)記録された情報が不
安定であるという欠点を有している。
Conventionally, polycrystalline metal thin films such as MnB1 and G
Amorphous metal thin films of a-00% Gd-Fe and compound single crystal thin films typified by GIG are known. Although these thin films have various advantages, MnB1 has the disadvantage that it is technically difficult to fabricate thin films due to its high Curie point, and that it requires a large amount of energy to write when used in magneto-optical disks. . Also, Gd-Co
The amorphous metal thin film of Gd-Fe has the disadvantage that the coercive force at room temperature is small (300 to 5000 e) and recorded information is unstable.

そこで、上記のような従来の磁性薄膜記録媒体の欠点を
除去する新しい磁性薄膜記録媒体として膜面と垂直方向
に磁化容易軸を有し18〜28 atom俤のB7を含
む非晶質Dy−Fe系合金膜を備えた磁気光学記憶媒体
が提案されている(特公昭57−20692号公報参照
)。しかしながら、上記の合金膜はキュリ一温度Tcが
70℃前後で低いがカー回転角θkがO,15deg前
後で小さく十分な再生出力を得ることができないという
問題がちった。
Therefore, as a new magnetic thin film recording medium that eliminates the drawbacks of the conventional magnetic thin film recording media as described above, an amorphous Dy-Fe material having an axis of easy magnetization perpendicular to the film surface and containing 18 to 28 atoms of B7 has been developed. A magneto-optical storage medium comprising a alloy film has been proposed (see Japanese Patent Publication No. 57-20692). However, the above-mentioned alloy film has a problem in that although the Curie temperature Tc is low at around 70° C., the Kerr rotation angle θk is small at around 0.15 degrees, making it impossible to obtain a sufficient reproduction output.

〔目 的〕〔the purpose〕

本発明は上記現状に鑑みてなされたものであって、その
目的はカー回転角θkが大きくかつ保磁力Haが大きい
非晶質磁気光学Iv1を提供することである。
The present invention has been made in view of the above-mentioned current situation, and its purpose is to provide an amorphous magneto-optic Iv1 having a large Kerr rotation angle θk and a large coercive force Ha.

〔構 成〕〔composition〕

本発明の非晶質磁気光学層は膜面と垂直な方向に磁化容
易軸を有するDy−Fe膜に少なくとも0.5原子−の
銅またはクロムを含むものである。
The amorphous magneto-optical layer of the present invention contains at least 0.5 atoms of copper or chromium in a Dy--Fe film having an axis of easy magnetization perpendicular to the film surface.

本発明において銅およびクロムの含有量をそれぞれ少な
くとも0.5原子チと限定するのは、大きなカー回転角
を得るためであり、一方0.5原子チ未満では充分なカ
ー回転角が得られず本発明の効果が達成されない。一方
、銅およびクロムの含有量をあまり大きくすると保磁力
Haが小さくなりかつカー回転角θにも小さくなるから
それぞれ0.5〜5原子−の範囲が好ましい。
In the present invention, the content of copper and chromium is limited to at least 0.5 atomic atoms each in order to obtain a large Kerr rotation angle, whereas if it is less than 0.5 atomic atoms, a sufficient Kerr rotation angle cannot be obtained. The effects of the present invention are not achieved. On the other hand, if the content of copper and chromium is too large, the coercive force Ha becomes small and the Kerr rotation angle θ also becomes small, so a range of 0.5 to 5 atoms each is preferable.

本発明の磁気光学層はガラス、プラスチック、セラミッ
クなどからなる非磁性基板上にスパッタ法、蒸着法、イ
オンブレーティング法などにより、少なくとも0.5原
子−のOuを含むDy−Fe−Cu膜または少なくとも
0.5原子−のOrを含むDy−Fe−Or膜を形成さ
せることにより作製することができる。膜の作製はスパ
ッタ法によって行うのが望ましい。ターゲットは例えば
コンポジット法を用い、28円板の上K DyおよびO
uチップまたはOrチップをのせて溝成しそして組成は
ターゲット表面の面積比でコントロールする。
The magneto-optic layer of the present invention is formed by sputtering, vapor deposition, ion blating, etc. on a non-magnetic substrate made of glass, plastic, ceramic, etc. It can be produced by forming a Dy-Fe-Or film containing at least 0.5 atoms of Or. Preferably, the film is formed by sputtering. The target is, for example, a composite method, with K Dy and O
A groove is formed by placing a U chip or an Or chip, and the composition is controlled by the area ratio of the target surface.

また、本発明の磁気光学層を光磁気記録媒体に使用する
場合はそれを単独で用いてもよいしちるいは他の膜と一
緒に用いてもよい。例えば保護膜例えば5102.5i
O1Si3N4などからなる膜をDy−Fe−0u膜ま
たはDy−Fe−0r膜の上または下にスパッタ法、蒸
着法、イオンブレーティング法などにより設けることが
できる。
Further, when the magneto-optic layer of the present invention is used in a magneto-optical recording medium, it may be used alone or together with a film or other film. For example, a protective film such as 5102.5i
A film made of O1Si3N4 or the like can be provided on or below the Dy-Fe-0u film or the Dy-Fe-0r film by sputtering, vapor deposition, ion blating, or the like.

〔実施例〕〔Example〕

以下に実施例をあげ、て本発明を具体的に説明するが、
これに限定されるものではない。
The present invention will be specifically explained with reference to Examples below.
It is not limited to this.

実施例 1 本実施例では以下のスパッタ条件下でスライドガラス基
板上に約2000λの膜厚のDy−Fe−0u膜を、D
y−Fe膜のD7の一部をOuで置換するという形でF
e0.78 (Dy1−XOux)0.22の中のXを
変化して作製した。なお、Dy−Fe膜の場合18〜2
8原子チのDyのとき垂直磁気異方性を示し補償組成は
およそ22原子チのDy付近にある。
Example 1 In this example, a Dy-Fe-0u film with a thickness of about 2000λ was deposited on a slide glass substrate under the following sputtering conditions.
F by replacing a part of D7 of the y-Fe film with O.
It was produced by changing X in e0.78 (Dy1-XOux)0.22. In addition, in the case of Dy-Fe film, 18-2
When Dy is 8 atoms, perpendicular magnetic anisotropy is exhibited, and the compensation composition is around Dy of about 22 atoms.

くスパッタ条件〉 残留ガス圧 ニア×10TOrr Arガス圧 : 2X10 ’rorr放電電力 : 
400W プレスパツタ時間 : 60分 メインスパッタ時間 : 10分 上述のようにして作製した記録媒体について基板側から
Hθ−Meレーザ(λ= 655 nm )を照射して
カー効果によりカー回転角θにおよび保磁力Hcをめた
。その結果0uの添加量に対するカー回転角θにおよび
保磁力Hcの変化は第1図のようになった。この図から
Ouの添加量を増していくとHcは小さくなるがθには
大きくなることがわかる。
Sputtering conditions> Residual gas pressure Near x 10 TOrr Ar gas pressure: 2 x 10 'rorr Discharge power:
400W Press sputtering time: 60 minutes Main sputtering time: 10 minutes The recording medium produced as described above was irradiated with an Hθ-Me laser (λ = 655 nm) from the substrate side to change the Kerr rotation angle θ and coercivity due to the Kerr effect. I met Hc. As a result, the changes in Kerr rotation angle θ and coercive force Hc with respect to the addition amount of 0 u were as shown in FIG. It can be seen from this figure that as the amount of O added increases, Hc decreases, but θ increases.

本実施例ではD7を0uで置換していったためOuを増
すと異方性に寄与しているD7が減りHaは急激に小さ
くなることからOuの添加量を七11はど上げられなか
ったがDyとFeとの比を一定にしてOuを添加するよ
うにすればHaの急激な減少はなくなりOuの添加量を
多くできる。実際にθにの比較を行ったところ、 ?”0.78D70..22のときθに−0,15de
gFeo、7s(D7o、960uo、o4)o、22
のときθに= 0.22 degとなり、θkがcuを
添加することくよシ47ダ大きくなることが明ら、がで
あった。
In this example, D7 was replaced with 0u, so when Ou was increased, D7, which contributes to anisotropy, decreased and Ha suddenly decreased, so it was not possible to increase the amount of Ou added by 711. If O is added while keeping the ratio of Dy and Fe constant, a rapid decrease in Ha can be prevented and the amount of O added can be increased. When we actually compared θ, ? "When 0.78D70..22, -0.15de to θ
gFeo, 7s (D7o, 960uo, o4) o, 22
When θ=0.22 deg, it is clear that θk increases by 47 degrees by adding cu.

実施例 2 本実施例では以下のスパッタ条件下でスライドガラス基
板上に約2000λの膜厚のDy−Fe −Or膜を、
Dy−Fe膜のDyの一部をOrで置換するという形で
78C1,78(D71−xcrx)0−22 の中の
Xを変化して作製した。なお、Dy7Pe膜の場合18
〜28原子チのDyのとき垂直磁気異方性を示し補償組
成はおよそ22原子優のD7付近にある。
Example 2 In this example, a Dy-Fe-Or film with a thickness of about 2000λ was deposited on a slide glass substrate under the following sputtering conditions.
It was produced by changing X in 78C1,78(D71-xcrx)0-22 by replacing a part of Dy in the Dy-Fe film with Or. In addition, in the case of Dy7Pe film, 18
When Dy is ~28 atoms, it exhibits perpendicular magnetic anisotropy, and the compensation composition is around D7, which is about 22 atoms.

〈スパッタ条件〉 残留ガス圧 : 7 X 10−’TorrArガス圧
 : 2X10 Torr 放電電力 + 400W プレスノリタ時間 : 6s分 メインスパッタ時1′!1: 1s分 上述のようにして作製した記録媒体について基板側から
He−Neレーザ(λ=636tun・)を照射してカ
ー効果によりカー回転角θにおよび保磁力Hcをめた。
<Sputtering conditions> Residual gas pressure: 7 x 10-'Torr Ar gas pressure: 2 x 10 Torr Discharge power + 400W Press Norita time: 6s minutes 1' for main sputtering! 1: The recording medium produced as described above was irradiated with a He-Ne laser (λ=636 tun·) from the substrate side for 1 s to set the Kerr rotation angle θ and the coercive force Hc due to the Kerr effect.

その結果Orの添加量に対するカー回転角θにおよび保
磁力Hcの変化は第2図のようKなった。この図からO
rの添加量を増していくとHaは小さくなるがθには大
きくなることがわかる。
As a result, the changes in Kerr rotation angle θ and coercive force Hc with respect to the amount of Or added were as shown in FIG. 2. From this figure, O
It can be seen that as the amount of r added increases, Ha decreases, but θ increases.

本実施例ではD7をOrで置換していったためOrを増
すと異方性に寄与しているDyが減りHaは急激に小さ
くなることからOrの添加量をそれを1と上げられなか
ったがD7とFeとの比を一定にしてOrを添加するよ
うにすればHaの急激な減少はなくなりOrの添加量を
多くできる。実際にθにの比較を行ったところ、 Fen、78D70.22のときθに±0.15deg
F′80.78(D70.94Or0.06)0.22
のときθに−0,18deqとなり、θkがOrを添加
することによ#)20%大きくなることが明らかであっ
た。
In this example, D7 was replaced with Or, so if Or was increased, Dy, which contributes to anisotropy, would decrease and Ha would rapidly decrease, so the amount of Or added could not be increased to 1. By adding Or while keeping the ratio of D7 and Fe constant, a rapid decrease in Ha can be prevented and the amount of Or added can be increased. When actually comparing θ, when Fen, 78D70.22, θ was ±0.15deg.
F'80.78 (D70.94Or0.06)0.22
When θ was -0.18 deq, it was clear that θk increased by 20% by adding Or.

〔効 果〕〔effect〕

本発明の非晶質磁気光学層はカー回転角θにの大きいか
っ保磁力Haの大きい光磁気記碌媒体を提供できる。
The amorphous magneto-optic layer of the present invention can provide a magneto-optical recording medium with a large Kerr rotation angle θ and a large coercive force Ha.

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

第1図および第2図は本発明の磁気光学層の最適条件を
決定するにあたっての組成変化に対するカー回転角と保
磁力との関係を示す図である。 特許出願人 株式会社 リ コ − 第1図 Fe0.78 CDy+−x C(Lx )o、22中
の工第2図
FIGS. 1 and 2 are diagrams showing the relationship between Kerr rotation angle and coercive force with respect to changes in composition in determining the optimum conditions for the magneto-optic layer of the present invention. Patent applicant Rico Co., Ltd. - Fig. 1 Fe0.78 CDy+-x C(Lx)o, Fig. 2 of 22

Claims (1)

【特許請求の範囲】[Claims] 膜面と垂直な方向に磁化容易軸を有するDr−Fe膜に
少なくとも0.5原子−の銅またはクロムを含むことを
特徴とする、非晶質磁気光学層。
An amorphous magneto-optical layer comprising at least 0.5 atoms of copper or chromium in a Dr-Fe film having an axis of easy magnetization perpendicular to the film surface.
JP23898283A 1983-12-20 1983-12-20 Amorphous magnetooptical layer Pending JPS60130806A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23898283A JPS60130806A (en) 1983-12-20 1983-12-20 Amorphous magnetooptical layer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23898283A JPS60130806A (en) 1983-12-20 1983-12-20 Amorphous magnetooptical layer

Publications (1)

Publication Number Publication Date
JPS60130806A true JPS60130806A (en) 1985-07-12

Family

ID=17038168

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23898283A Pending JPS60130806A (en) 1983-12-20 1983-12-20 Amorphous magnetooptical layer

Country Status (1)

Country Link
JP (1) JPS60130806A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4625585A (en) * 1985-01-09 1986-12-02 Tractech, Inc. Torque-proportioning differential with sectional housing
JPS62132254A (en) * 1985-12-05 1987-06-15 Hitachi Maxell Ltd Photomagnetic recording medium

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4625585A (en) * 1985-01-09 1986-12-02 Tractech, Inc. Torque-proportioning differential with sectional housing
JPS62132254A (en) * 1985-12-05 1987-06-15 Hitachi Maxell Ltd Photomagnetic recording medium

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