JPH0782943B2 - Amorphous magneto-optical layer - Google Patents

Amorphous magneto-optical layer

Info

Publication number
JPH0782943B2
JPH0782943B2 JP59089619A JP8961984A JPH0782943B2 JP H0782943 B2 JPH0782943 B2 JP H0782943B2 JP 59089619 A JP59089619 A JP 59089619A JP 8961984 A JP8961984 A JP 8961984A JP H0782943 B2 JPH0782943 B2 JP H0782943B2
Authority
JP
Japan
Prior art keywords
magneto
amorphous
optical layer
film
optical
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.)
Expired - Lifetime
Application number
JP59089619A
Other languages
Japanese (ja)
Other versions
JPS60233810A (en
Inventor
元治 田中
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 JP59089619A priority Critical patent/JPH0782943B2/en
Publication of JPS60233810A publication Critical patent/JPS60233810A/en
Publication of JPH0782943B2 publication Critical patent/JPH0782943B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Thin Magnetic Films (AREA)

Description

【発明の詳細な説明】 技術分野 本発明はハードデイスク、フロツピーデイスク、ドキユ
メントフアイル等に使用される光磁気記録媒体に関する
ものであり、特に磁気光学的に優れた非晶質磁気光学層
に係るものである。
TECHNICAL FIELD The present invention relates to a magneto-optical recording medium used for a hard disk, a floppy disk, a document file, etc., and particularly to an amorphous magneto-optical layer excellent in magneto-optical properties. It is related.

従来技術 近年、半導体レーザー光により磁気記録を行う光磁気記
録媒体が高密度記録用として種々研究されている。特に
高密度記録用として使用されるためには磁性膜がその膜
面に垂直な方向に磁化容易軸を有することが必要とされ
る。従来、これら光磁気記録媒体に用いられる磁性膜と
してはGd−Co,Gd−Fe,Tb−Fe,Gd−Tb−Fe,Tb−Dy−Fe等
の非晶質合金を用いたもの等が知られているが、これら
非晶質合金磁性体を用いた光磁気記録媒体は記録感度が
高く半導体レーザー光によつて高速度(周波数、数MHz
において)で記録できるという利点はあるものの磁気光
学効果が十分満足できるものではない問題点を有するも
のである。かかることからTb−Dy−Fe−Coよりなる4元
系非晶質磁性膜を用いることによりカー回転角θkを大
きくして磁気光学効果を向上させることを本件出願人は
既に提案している。このような磁性膜を用いて光磁気記
録媒体を作るには一般にガラス板のような基板上に前記
磁性体を真空蒸着、スパツタリング等の方法で付着させ
て磁性膜を形成している。こうして得られる光磁気記録
媒体への記録、再生は次のようにして行われる。すなわ
ち、記録は磁性膜のキユリー温度または補償温度近傍に
おける温度変化に対応した保磁力の急激な変化特性を利
用して情報信号で変調されたレーザー光を磁性膜に照射
加熱して磁性膜表面磁化の向きを反転させることにより
行われる。また再生はこうして反転記録された磁性膜の
カー回転角を読出すことにより行われる。このような非
晶質合金磁性体のように光が透過しにくい場合の情報信
号の記録、再生はカー効果を利用するものである。カー
効果とは磁性体の表面で光が反射する際の偏光面の回転
現象であり、a)極(polar)効果、b)縦(longitudi
nal)効果、c)横(transverse)効果があり、特に非
晶質合金磁性体の場合にはaの極効果が用いられ、その
カー回転角θkを利用して再生が行われる。従つてカー
回転角θkが少しでも大きくなればそれだけ磁気光学効
果が増し、再生特性が向上することになる。
2. Description of the Related Art In recent years, various studies have been conducted on a high-density recording magneto-optical recording medium that performs magnetic recording with a semiconductor laser beam. In particular, in order to be used for high density recording, it is necessary that the magnetic film has an easy axis of magnetization in the direction perpendicular to the film surface. Conventionally, as magnetic films used in these magneto-optical recording media, those using amorphous alloys such as Gd-Co, Gd-Fe, Tb-Fe, Gd-Tb-Fe, and Tb-Dy-Fe are known. However, the magneto-optical recording medium using these amorphous alloy magnetic materials has a high recording sensitivity and a high speed (frequency, several MHz) by the semiconductor laser light.
However, there is a problem that the magneto-optical effect is not sufficiently satisfied, although there is an advantage that the recording can be performed in (1). Therefore, the applicant of the present application has already proposed to increase the Kerr rotation angle θk and improve the magneto-optical effect by using a quaternary amorphous magnetic film made of Tb-Dy-Fe-Co. In order to manufacture a magneto-optical recording medium using such a magnetic film, generally, the magnetic material is attached onto a substrate such as a glass plate by a method such as vacuum deposition and sputtering to form the magnetic film. Recording and reproduction on the thus obtained magneto-optical recording medium are performed as follows. That is, recording is performed by irradiating and heating the magnetic film with a laser beam modulated by an information signal by utilizing the rapid change characteristic of the coercive force corresponding to the temperature change near the Curie temperature or the compensation temperature of the magnetic film. This is done by reversing the direction of. Further, the reproduction is performed by reading the Kerr rotation angle of the magnetic film thus recorded in reverse. The Kerr effect is used for recording and reproducing an information signal when light is difficult to pass through as in such an amorphous alloy magnetic body. The Kerr effect is the rotation phenomenon of the plane of polarization when light is reflected on the surface of a magnetic material, and is a) polar effect, b) vertical (longitudi).
nal) effect and c) transverse effect. Especially, in the case of an amorphous alloy magnetic body, the pole effect of a is used, and the Kerr rotation angle θk is used to perform reproduction. Therefore, if the Kerr rotation angle θk is increased as much as possible, the magneto-optical effect is increased and the reproduction characteristic is improved.

しかしながら、前述のTb−Dy−Fe−Coよりなる4元系非
晶質合金磁性膜のカー回転角θkはその組成により0.29
deg、もしくは0.30deg程度であり、光再生特性の向上が
望まれている状況にある。
However, the Kerr rotation angle θk of the quaternary amorphous alloy magnetic film made of Tb-Dy-Fe-Co is 0.29 due to its composition.
It is about deg or about 0.30 deg, and there is a demand for improvement of the optical reproduction characteristic.

目的 本発明の目的は膜面に垂直な方向に磁化容易軸を有する
非晶質合金磁性膜におけるカー回転角θkをより増大せ
しめ、それにより光再生特性を向上させた非晶質磁気光
学層を提供することにある。
OBJECT The object of the present invention is to provide an amorphous magneto-optical layer having an increased Kerr rotation angle θk in an amorphous alloy magnetic film having an easy axis of magnetization in a direction perpendicular to the film surface, thereby improving the light reproduction characteristics. To provide.

構成 本発明は膜面に垂直な方向に磁化容易軸を有するTb−Dy
−Fe−Co−Cuの5元系非晶質合金磁性膜からなる非晶質
磁気光学層である。
Structure The present invention is a Tb-Dy having an easy axis of magnetization in a direction perpendicular to the film surface.
It is an amorphous magneto-optical layer composed of a quinary amorphous alloy magnetic film of -Fe-Co-Cu.

また本発明の非晶質磁気光学層は垂直磁気異方性を示
し、かつ高保磁力Hcを有する必要があり、そのために本
発明の磁性材料の組成式を、 {(Tb1-XDyX)Z(Fe1-YCOY)1-Z1-ACuA と表わした場合、0<X<1,0.01≦Y≦0.5,0.1≦Z≦
0.5,0.001≦A≦0.1であることが望ましい。
Further, the amorphous magneto-optical layer of the present invention is required to exhibit perpendicular magnetic anisotropy and have a high coercive force Hc. Therefore, the composition formula of the magnetic material of the present invention is represented by {(Tb 1-X Dy X ). When expressed as Z (Fe 1-Y CO Y ) 1-Z } 1-A Cu A , 0 <X <1,0.01 ≦ Y ≦ 0.5,0.1 ≦ Z ≦
It is desirable that 0.5, 0.001 ≦ A ≦ 0.1.

本発明の非晶質磁気光学層は適宜の支持体上に真空蒸
着、スパツタリング、イオンプレーテイング等の方法で
膜厚0.01〜1μm程度に形成する。これにより得られる
磁性膜は膜面に垂直磁化されたものとなる。
The amorphous magneto-optical layer of the present invention is formed on a suitable support by a method such as vacuum deposition, sputtering, ion plating and the like to have a film thickness of about 0.01 to 1 μm. The magnetic film thus obtained is one that is perpendicularly magnetized to the film surface.

スパツタリングにて磁性体の薄膜形成を行う場合には、
各材料成分を各個にあるいは組合わせてターゲツトと
し、磁性体組成はターゲツト表面の面積比でコントロー
ルするようにする。
When forming a magnetic thin film by sputtering,
Each material component is used individually or in combination to form a target, and the magnetic material composition is controlled by the area ratio of the target surface.

支持体としてはガラス、プラスチツク、セラミツク等が
使用できる。
As the support, glass, plastic, ceramic or the like can be used.

なお、本発明の磁気光学層を光磁気記録媒体に使用する
場合はそれを単独に用いてもよいし、あるいは他の膜と
一緒に用いてもよい。例えばTb−Dy−Fe−Co−Cu膜の上
面または上下面に保護膜としてアクリル樹脂、ポリウレ
タン樹脂、ポリカーボネート樹脂、ポリエーテルスルホ
ン樹脂、ポリアミド樹脂、エポキシ樹脂、TiN,Si3N4,Al
N,CrN,TaN,SiO2,SiO等を樹脂の場合は塗布法で、その他
の材料の場合は真空蒸着、スパツタリング、反応スパツ
タリング、CVD等の方法で膜厚0.1〜10μm程度に付着さ
せるようにしてもよい。
When the magneto-optical layer of the present invention is used in a magneto-optical recording medium, it may be used alone or in combination with other films. For example, an acrylic resin, a polyurethane resin, a polycarbonate resin, a polyethersulfone resin, a polyamide resin, an epoxy resin, TiN, Si 3 N 4 , Al as a protective film on the upper surface or the upper and lower surfaces of the Tb-Dy-Fe-Co-Cu film.
Apply N, CrN, TaN, SiO 2 , SiO, etc. to the film thickness of 0.1 to 10 μm by the coating method for resin and vacuum evaporation, sputtering, reactive sputtering, CVD etc. for other materials. May be.

効果 このようにして得られるTb−Dy−Fe−Co−Cuからなる非
晶質磁気光学層に情報信号で変調されたレーザー光を照
射加熱した場合、前記非晶質磁気光学層のカー回転角θ
kが従来のものに比べて大きいため、これをカー効果に
より再生する際の光再生特性が良好となり、S/N比が向
上するとともに記録ピツト数も増大し、高密度記録再生
可能な光磁気記録媒体が得られることになる。
Effect When the amorphous magneto-optical layer made of Tb-Dy-Fe-Co-Cu thus obtained is heated by irradiation with laser light modulated by an information signal, the Kerr rotation angle of the amorphous magneto-optical layer θ
Since k is larger than that of the conventional one, the optical reproduction characteristic when reproducing this by the Kerr effect is improved, the S / N ratio is improved, the number of recording dots is increased, and high-density recording / reproduction is possible. A recording medium will be obtained.

以下に実施例を示す。Examples will be shown below.

実施例 スライドガラス支持体上にスパツタリング法によりTb−
Dy−Fe−Co−Cuからなる非晶質磁気光学層を形成した。
ターゲツトはコンポジツト法を用い、Fe0.9Co0.1合金円
板上にTb0.5Dy0.5の合金チツプおよびCuチツプをのせて
構成し、各組成比をターゲツト表面の面積比でコントロ
ールしつつ膜を形成した。
Example Tb-on a slide glass support by the sputtering method
An amorphous magneto-optical layer made of Dy-Fe-Co-Cu was formed.
The target was formed by using a composite method by placing an alloy chip of Tb 0.5 Dy 0.5 and a Cu chip on a Fe 0.9 Co 0.1 alloy disk, and forming a film while controlling each composition ratio by the area ratio of the target surface.

非晶質磁気光学層の作成条件を次表に示す。The conditions for forming the amorphous magneto-optical layer are shown in the following table.

各非晶質磁気光学層は保磁力Hcの大きい補償組成付近の
(Fe0.9Co0.1)0.79(Tb0.5Dy0.5)0.21の組成において、(T
b0.5Dy0.5)の一部をCuで置換した形、すなわち(Fe0.9Co
0.1)0.79{(Tb0.5Dy0.5)1-XCuX0.21の組成となし、作
製した。
Each amorphous magneto-optical layer has a large coercive force Hc near the compensation composition.
In the composition of (Fe 0.9 Co 0.1 ) 0.79 (Tb 0.5 Dy 0.5 ) 0.21 , (T
b 0.5 Dy 0.5 ) partly replaced by Cu, that is, (Fe 0.9 Co
0.1 ) 0.79 {(Tb 0.5 Dy 0.5 ) 1-X Cu X } 0.21 was prepared.

膜の評価は基板側からHe−Neレーザー(λ=633nm)を
照射し、カー効果を用いてカー回転角θkおよび保磁力
Hcを求めた。
The film was evaluated by irradiating a He-Ne laser (λ = 633 nm) from the substrate side and using the Kerr effect, the Kerr rotation angle θk and the coercive force.
I asked for Hc.

それらの結果を第1図に示す。これらの図よりX、すな
わちCuの量を増加させることによりHcは小さくなるもの
のθkは大きくなることがわかる。本実施例では(Tb
0.5Dy0.5)の一部をCuで置換したため、Cu量を増大させ
ると異方性に寄与しているTbの量が減り、Hcは小さくな
るためCu量をそれ程増大できなかつたが、(Fe0.9C
o0.1)と(Tb0.5Dy0.5)の量の比を一定にしてCu量を増
すようにすればHcの低下は抑えられCu量を増大させるこ
とができる。
The results are shown in FIG. From these figures, it can be seen that by increasing X, that is, the amount of Cu, Hc decreases but θk increases. In this embodiment, (Tb
Since 0.5 Dy 0.5 ) was partially replaced by Cu, increasing the amount of Cu reduced the amount of Tb contributing to anisotropy and decreasing Hc, so the amount of Cu could not be increased so much. 0.9 C
If the ratio of (O 0.1 ) and (Tb 0.5 Dy 0.5 ) is kept constant and the amount of Cu is increased, the decrease in Hc can be suppressed and the amount of Cu can be increased.

ここで改めて各実施例における非晶質磁気光学層におい
て最もカー回転角が大きくなる場合のTb−Dy−Fe−Co−
Cu膜組成、カー回転角θkおよびCuを含有させない場合
と比べたθkの増加値を示す。
Here, Tb-Dy-Fe-Co- in the case where the Kerr rotation angle is maximized in the amorphous magneto-optical layer in each of the examples.
The Cu film composition, the Kerr rotation angle θk, and the increase value of θk compared with the case where Cu is not contained are shown.

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

第1図は実施例における各非晶質磁気光学層中のCuの量
を変えた場合のθkおよびHcの変化図である。
FIG. 1 is a change diagram of θk and Hc when the amount of Cu in each amorphous magneto-optical layer is changed in the examples.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】膜面に垂直な方向に磁化容易軸を有するTb
−Dy−Fe−Co−Cuの5元系非晶質合金磁性膜からなる非
晶質磁気光学層。
1. A Tb having an easy axis of magnetization in a direction perpendicular to a film surface.
An amorphous magneto-optical layer formed of a quinary amorphous alloy magnetic film of -Dy-Fe-Co-Cu.
JP59089619A 1984-05-04 1984-05-04 Amorphous magneto-optical layer Expired - Lifetime JPH0782943B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59089619A JPH0782943B2 (en) 1984-05-04 1984-05-04 Amorphous magneto-optical layer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59089619A JPH0782943B2 (en) 1984-05-04 1984-05-04 Amorphous magneto-optical layer

Publications (2)

Publication Number Publication Date
JPS60233810A JPS60233810A (en) 1985-11-20
JPH0782943B2 true JPH0782943B2 (en) 1995-09-06

Family

ID=13975767

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59089619A Expired - Lifetime JPH0782943B2 (en) 1984-05-04 1984-05-04 Amorphous magneto-optical layer

Country Status (1)

Country Link
JP (1) JPH0782943B2 (en)

Families Citing this family (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6140012A (en) * 1984-07-31 1986-02-26 Oki Electric Ind Co Ltd Material for photomagnetic recording
JPS61172237A (en) * 1985-01-28 1986-08-02 Kyocera Corp Photoelectromagnetic recording element
JP2601796B2 (en) * 1985-12-05 1997-04-16 日立マクセル株式会社 Magneto-optical recording medium
US4950556A (en) * 1987-10-26 1990-08-21 Minnesota Mining And Manufacturing Company Magneto-optic recording medium
JP2770027B2 (en) * 1988-07-22 1998-06-25 ティーディーケイ株式会社 Magneto-optical recording medium and magneto-optical recording method
JPH0233745A (en) * 1988-07-22 1990-02-02 Tdk Corp Magneto-optical recording medium and magneto-optical recording method
JP2918889B2 (en) * 1988-07-22 1999-07-12 ティーディーケイ株式会社 Magneto-optical recording medium and magneto-optical recording method
KR950005965B1 (en) * 1993-02-25 1995-06-07 주식회사금성사 Optical recording medium
US5858565A (en) * 1995-11-09 1999-01-12 Eastman Kodak Company Magneto-optic compositionally modulated structure
US6479169B1 (en) * 2000-03-16 2002-11-12 Trace Storage Technology Corp. Low noise magnetic recording media having a interlayer film
CN112466409B (en) * 2020-11-19 2023-09-22 江苏科技大学 Five-membered high-entropy amorphous alloy component design method based on combination of two quaternary amorphous alloy elements

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58165306A (en) * 1982-03-26 1983-09-30 Hitachi Ltd Vertical magnetic recording medium
JPS5961011A (en) * 1982-09-30 1984-04-07 Ricoh Co Ltd Optical magnetic recording medium

Also Published As

Publication number Publication date
JPS60233810A (en) 1985-11-20

Similar Documents

Publication Publication Date Title
US4753853A (en) Double-layered magnetooptical recording medium
US4838962A (en) Magneto-optical recording medium
JPH0782943B2 (en) Amorphous magneto-optical layer
JPH0630300B2 (en) Amorphous magneto-optical layer
US5639563A (en) Magneto-optical recording medium
JP2602425B2 (en) Amorphous magneto-optical layer
JPH05198029A (en) Photomagnetic recording medium
JPH0638370B2 (en) Amorphous magneto-optical layer
JP2550633B2 (en) Photothermal magnetic recording medium
JPH0690813B2 (en) Amorphous magneto-optical layer
JPS6122455A (en) Magnetooptic recording medium
JPH0664761B2 (en) Magneto-optical recording medium
JP2681199B2 (en) Magneto-optical recording element
US7235313B2 (en) Magneto-optical recording medium, method of manufacturing magneto-optical recording medium, method of recording on magneto-optical recording medium, and method of reproduction from magneto-optical recording medium
JPH0350343B2 (en)
JPH0328739B2 (en)
JPH0619859B2 (en) Magneto-optical recording medium
JP2604361B2 (en) Magneto-optical recording medium
JPH0660452A (en) Magneto-optical recording medium
JPS6029996A (en) Photomagnetic recording carrier
JP3446297B2 (en) Magneto-optical recording medium
JPS6189604A (en) Metal oxide magnetic substance and magnetic film
JPS5996714A (en) Magnetic recording medium
KR100209584B1 (en) Magneto-optical disk
JP3657667B2 (en) Magneto-optical recording medium

Legal Events

Date Code Title Description
EXPY Cancellation because of completion of term