JPS61104446A - Photomagnetic recording medium - Google Patents
Photomagnetic recording mediumInfo
- Publication number
- JPS61104446A JPS61104446A JP22523884A JP22523884A JPS61104446A JP S61104446 A JPS61104446 A JP S61104446A JP 22523884 A JP22523884 A JP 22523884A JP 22523884 A JP22523884 A JP 22523884A JP S61104446 A JPS61104446 A JP S61104446A
- Authority
- JP
- Japan
- Prior art keywords
- target
- film
- compsn
- recording medium
- magnetic alloy
- 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
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
- G11B11/10582—Record carriers characterised by the selection of the material or by the structure or form
- G11B11/10586—Record carriers characterised by the selection of the material or by the structure or form characterised by the selection of the material
Landscapes
- Thin Magnetic Films (AREA)
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は光磁気ディスクメモリに用いられる磁性薄膜記
録媒体に関するもので、更に詳しくは、膜面と垂直方向
に磁化容易軸を有し、レーザーなどの元ビームを照射し
た領域に反転磁区全作ることにより、情報を記録するこ
とができ%磁気光学効果金利用して読み出、すことので
きる磁性薄膜記録媒体に関するものである。Detailed Description of the Invention (Field of Industrial Application) The present invention relates to a magnetic thin film recording medium used in magneto-optical disk memories, and more specifically, it has an axis of easy magnetization perpendicular to the film surface and This invention relates to a magnetic thin film recording medium in which information can be recorded and read by making use of the magneto-optical effect by completely creating inverted magnetic domains in the area irradiated with the original beam.
(従来技術とその問題点)
光デイスクメモリは、高密度−大容量記録が可能であ、
す、かつ非接触・高速アクセスもできるという点から、
大容量ファイルメモリの一つとして近年注目を集めてい
る。その中でも、光磁気ディスクメモリは、記録情報の
書き換えが可能であるという利点を持っていることから
、各所で盛ん、に研究されている。(Prior art and its problems) Optical disk memory is capable of high-density and large-capacity recording;
In addition, contactless and high-speed access is possible.
It has attracted attention in recent years as a type of large-capacity file memory. Among these, magneto-optical disk memories have the advantage that recorded information can be rewritten, and are therefore being actively researched in various places.
従来、その記録媒体としてはMnB1.MnCuB1な
どの多結晶体薄膜、Tb、 Gd、 l)yなどの希土
類金層と、Fee Coなどの鉄族遷移金属との組み合
わせによって作成される非晶質磁性合金薄膜、GIGな
どの単結晶薄膜などが知られている。これらの薄膜のう
ちで、非晶質磁性合金薄膜は、書き込み感度が高い、粒
界ノイズがない、膜面に垂直方向の母気異方性を有する
膜が容易に作れるなどの利点を有するため、記録媒体と
して、最も有望視されている。Conventionally, MnB1. Polycrystalline thin films such as MnCuB1, amorphous magnetic alloy thin films created by combining rare earth gold layers such as Tb, Gd, l)y, and iron group transition metals such as Fee Co, and single crystal thin films such as GIG. etc. are known. Among these thin films, amorphous magnetic alloy thin films have advantages such as high writing sensitivity, no grain boundary noise, and easy production of films with matrix anisotropy perpendicular to the film surface. , is considered the most promising as a recording medium.
しかし、この膜は一般に、カー回転角〜が小さいために
、これを記録層として用いた光磁気ディスクメモリの再
生−は、あまル高くできない・という欠点がある。光磁
気ディスクメモリの高性能化のためには、膜のカー回転
角θに金少しでも大きくする必要がある。このため、上
記膜に種々の元素を添加して、カー回転角θkを大きく
する研究が盛んに行われている。However, since this film generally has a small Kerr rotation angle, it has the disadvantage that the reproduction rate of a magneto-optical disk memory using this film as a recording layer cannot be very high. In order to improve the performance of magneto-optical disk memories, it is necessary to increase the Kerr rotation angle θ of the film as much as possible. For this reason, many studies are being conducted to increase the Kerr rotation angle θk by adding various elements to the film.
(発明の目的)
本発明は、かかる観点から成されたものでありカー回転
角θにの大きい非晶質磁性合金薄膜を記録層とした光磁
気記録媒体全提供することにある。(Objective of the Invention) The present invention has been made from this point of view, and it is an object of the present invention to provide a complete magneto-optical recording medium whose recording layer is an amorphous magnetic alloy thin film having a large Kerr rotation angle θ.
(発明の構成)
本発明にかかる光磁気記録媒体は、膜面と垂直方向に磁
化容易軸全方し、希土類元素と鉄族遷移元素とAgとN
i含む磁性合金全記録層とすることを特徴とする。(Structure of the Invention) The magneto-optical recording medium according to the present invention has an easy axis of magnetization in the direction perpendicular to the film surface, and contains a rare earth element, an iron group transition element, Ag and N.
It is characterized in that the entire recording layer is made of a magnetic alloy containing i.
(実施例) 以下、本発明の実施例について詳細に説明する。(Example) Examples of the present invention will be described in detail below.
膜の作製には、高周波スパッタ装置を用いた。ターゲッ
トとして、pe板上忙、TbチッグとAgチップを分散
配置した複合ターゲラトラ用いた。A high frequency sputtering device was used to prepare the film. As a target, a composite target rattler on which Tb chips and Ag chips were dispersed was used on a PE board.
組成はターゲットの面積比で、TbxsFes< XA
g xとなる様に調成した。又、雰囲気ガスとして、
純アルゴン及びアルゴンと窒素の混合ガスを用いた。x
= Qのターゲット組成で純アルゴン雰囲気で作製し
た膜の組成は、XMAによれば、Tb3Qat%であり
、補償組成に対してTb1Jツチであった。以下にスパ
ッタ条件全まζめて示す。The composition is the area ratio of the target, TbxsFes<XA
It was prepared so that g x. Also, as an atmospheric gas,
Pure argon and a mixed gas of argon and nitrogen were used. x
According to XMA, the composition of the film produced in a pure argon atmosphere with a target composition of =Q was Tb3Qat%, which was Tb1J with respect to the compensation composition. All sputtering conditions are shown below.
ターゲット Tb 5gFe s4−)(Agx基
板 ガラス
背 圧 2 X 10 Torr以下雰囲
気ガス圧 2 X 10 ’f’orrスパッタ
パワー 2W/7
電極間距離 5α
第1図に、この様にして作製された膜厚1500Aの膜
に対して、カーヒステリシス曲線から得られるカー回転
角θk及び抗磁力HCとターゲット組成との関係を、雰
囲気ガス中のNxi:を、パラメータとして示す。膜は
全て補償組成に対してTb1Jツチの特性を示し、膜面
に垂直方向の磁化容易軸を有し、さらにX線的に非晶質
であった。Target Tb 5gFe s4-) (Agx group
Plate glass back pressure 2 x 10 Torr or less Atmospheric gas pressure 2 x 10 'f'orr Sputtering power 2W/7 Interelectrode distance 5α Figure 1 shows that the car The relationship between the Kerr rotation angle θk and the coercive force HC obtained from the hysteresis curve and the target composition is shown using Nxi: in the atmospheric gas as a parameter. All of the films exhibited Tb1J characteristics with respect to the compensation composition, had easy magnetization axes perpendicular to the film plane, and were X-ray amorphous.
HX1図によると、純アルゴン雰囲気の場合、TbFe
へのAgの添加量が増大するにつれ、抗磁力HCは単調
に減少するが、カー回転角θには殆ど変わらなかった。According to the HX1 diagram, in the case of pure argon atmosphere, TbFe
As the amount of Ag added increases, the coercive force HC monotonically decreases, but the Kerr rotation angle θ hardly changes.
一方、N z 412モルチの混合ガス雰囲気で作製さ
れた膜では、純アルゴン雰囲気で作製されたものに比べ
て、膜の補償組成はTbグリッチ側へフトし、抗磁力H
cは、全体的に上昇した。そして、カー回転角θ、は、
ターゲット組成に対しては、殆ど変化しないが、純アル
ゴン雰囲気で作製されたものより、約9多大きくなった
。この様な傾向は、雰囲気ガス中のN2量が3〜4モル
チの場合に対しても、同様に見られたがN!量5モルチ
以上では、垂直磁化膜が得られなかった。On the other hand, in a film fabricated in a mixed gas atmosphere of Nz 412M, the compensation composition of the film shifts to the Tb glitch side, and the coercive force H
c increased overall. And the Kerr rotation angle θ is
Although there was almost no change in the target composition, it was about 9 times larger than that produced in a pure argon atmosphere. Similar trends were observed when the amount of N2 in the atmospheric gas was 3 to 4 molt, but N! A perpendicularly magnetized film could not be obtained when the amount was 5 molti or more.
以上述べた’pbpeへのAg及びN添加効果は上述の
組成に限定されるものではなく、’l’b yFe(1
oo−d −x Ag X Q8≦y≦35at%、0
くxく5)で示される全組成に対して、同様の効果が見
られた。しかし10<x<20の範囲になると特性が劣
化し、光磁気記録媒体としては不適自になる。The effect of adding Ag and N to 'pbpe as described above is not limited to the above-mentioned composition;
oo-d −x Ag X Q8≦y≦35at%, 0
Similar effects were observed for all compositions shown in 5). However, in the range of 10<x<20, the characteristics deteriorate, making it unsuitable as a magneto-optical recording medium.
上記効果は、他の希土類と鉄族遷移元素からなる磁性合
金、例えばTbFeCo、GctTbFe、GdTbF
eCo、TbPeNi、TbFeNiCo K対しても
同様に見られる。The above effect can be obtained by using magnetic alloys made of other rare earth elements and iron group transition elements, such as TbFeCo, GctTbFe, and GdTbF.
Similar results can be seen for eCo, TbPeNi, and TbFeNiCo K.
(発明の効果)
以上述べた様に、本発明によれば、カー回転角θ、の増
加した非晶質磁性合金薄Me記録層とした光磁気記録媒
体全提供できる。(Effects of the Invention) As described above, according to the present invention, it is possible to provide an entire magneto-optical recording medium having an amorphous magnetic alloy thin Me recording layer with an increased Kerr rotation angle θ.
第1図は、本発明の実施例を示す図である。 FIG. 1 is a diagram showing an embodiment of the present invention.
Claims (1)
と鉄族遷移元素とAgとNを含む磁性合金を記録層とす
ることを特徴とする光磁気記録媒体。(1) A magneto-optical recording medium characterized by having an axis of easy magnetization perpendicular to the film surface and having a recording layer made of a magnetic alloy containing a rare earth element, an iron group transition element, Ag, and N.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP22523884A JPS61104446A (en) | 1984-10-26 | 1984-10-26 | Photomagnetic recording medium |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP22523884A JPS61104446A (en) | 1984-10-26 | 1984-10-26 | Photomagnetic recording medium |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61104446A true JPS61104446A (en) | 1986-05-22 |
Family
ID=16826155
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP22523884A Pending JPS61104446A (en) | 1984-10-26 | 1984-10-26 | Photomagnetic recording medium |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61104446A (en) |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5860444A (en) * | 1981-10-06 | 1983-04-09 | Canon Inc | Manufacture of photothermomagnetic recording medium |
JPS5984358A (en) * | 1982-11-04 | 1984-05-16 | Seiko Instr & Electronics Ltd | Photomagnetic recording medium |
-
1984
- 1984-10-26 JP JP22523884A patent/JPS61104446A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5860444A (en) * | 1981-10-06 | 1983-04-09 | Canon Inc | Manufacture of photothermomagnetic recording medium |
JPS5984358A (en) * | 1982-11-04 | 1984-05-16 | Seiko Instr & Electronics Ltd | Photomagnetic recording medium |
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