JPH0673200B2 - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- Publication number
- JPH0673200B2 JPH0673200B2 JP30080086A JP30080086A JPH0673200B2 JP H0673200 B2 JPH0673200 B2 JP H0673200B2 JP 30080086 A JP30080086 A JP 30080086A JP 30080086 A JP30080086 A JP 30080086A JP H0673200 B2 JPH0673200 B2 JP H0673200B2
- Authority
- JP
- Japan
- Prior art keywords
- recording medium
- recording
- magneto
- layer
- magnetic
- 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
Links
- 239000010410 layer Substances 0.000 claims description 32
- 239000004020 conductor Substances 0.000 claims description 11
- 239000000758 substrate Substances 0.000 claims description 9
- 239000011241 protective layer Substances 0.000 claims description 5
- 230000003287 optical effect Effects 0.000 claims description 4
- 229910001004 magnetic alloy Inorganic materials 0.000 claims description 3
- 230000035699 permeability Effects 0.000 claims description 3
- 239000003989 dielectric material Substances 0.000 claims description 2
- 239000010408 film Substances 0.000 description 15
- 229910045601 alloy Inorganic materials 0.000 description 4
- 239000000956 alloy Substances 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 230000005415 magnetization Effects 0.000 description 4
- 230000015654 memory Effects 0.000 description 4
- 239000007789 gas Substances 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 229910001030 Iron–nickel alloy Inorganic materials 0.000 description 2
- 230000008901 benefit Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000006870 function Effects 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 239000012212 insulator Substances 0.000 description 2
- 230000001678 irradiating effect Effects 0.000 description 2
- 230000005381 magnetic domain Effects 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 229910002546 FeCo Inorganic materials 0.000 description 1
- 229910052688 Gadolinium Inorganic materials 0.000 description 1
- 229910052689 Holmium Inorganic materials 0.000 description 1
- 229910004298 SiO 2 Inorganic materials 0.000 description 1
- 229910052771 Terbium Inorganic materials 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 230000008034 disappearance Effects 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 238000001755 magnetron sputter deposition Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 229910052759 nickel Inorganic materials 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 229910000889 permalloy Inorganic materials 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 229910052761 rare earth metal Inorganic materials 0.000 description 1
- 150000002910 rare earth metals Chemical class 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 238000000992 sputter etching Methods 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- 229910052723 transition metal Inorganic materials 0.000 description 1
- 150000003624 transition metals Chemical class 0.000 description 1
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は光磁気メモリに用いられる記録媒体に関するも
のであり、更に詳しくは、膜面と垂直方向に磁化容易軸
を有する磁性膜を記録層とし、レーザなどの光ビームを
照射した領域に反転磁区を作ることにより情報を記録す
ることができ、磁気光学効果を利用して読み出すことの
でできる光磁気記録媒体に関するものである。Description: TECHNICAL FIELD The present invention relates to a recording medium used in a magneto-optical memory, and more specifically, a magnetic layer having a magnetic easy axis in a direction perpendicular to the film surface of the recording layer. Further, the present invention relates to a magneto-optical recording medium capable of recording information by forming a reversed magnetic domain in a region irradiated with a light beam such as a laser and capable of reading by utilizing a magneto-optical effect.
(従来の技術) 光メモリは大容量ファイルメモリの一つとして注目され
ている。中でも光磁気メモリは、記録情報の書き替えが
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。その記録媒体としては、Tb,Gd,D
y,Hoなどの希土類金属とFe,Co,Niなどの遷移金属との組
み合わせによって作製される非晶質磁性薄膜が、記録感
度が高い、粒界ノイズがない膜面に垂直方向の磁気異方
性を有する膜が容易に作れるなどの利点を有するため、
最も有望視されている。(Prior Art) An optical memory attracts attention as one of large-capacity file memories. Among them, the magneto-optical memory has the advantage that the recorded information can be rewritten, and is therefore actively studied in various places. The recording medium is Tb, Gd, D
Amorphous magnetic thin films prepared by combining rare earth metals such as y and Ho and transition metals such as Fe, Co and Ni are magnetically anisotropic in the perpendicular direction to the film surface with high recording sensitivity and no grain boundary noise. Since it has the advantage that a film with properties can be easily made,
Most promising.
従来、この様な記録媒体に対する情報の記録・消失は次
の様に行われる。記録は、一方向に着磁した記録媒体に
レーザ光ビームを照射して、媒体温度をキューリ温度Tc
もしくは補償温度Tcomp以上に上昇させ、外部印加磁界
と記録媒体の反磁界によって反転磁区を形成することに
より行われる。消失は、外部磁界を記録時とは逆極世に
印加し、レーザ光ビームを記録時と同等の強度で記録媒
体に一様に照射する。いわゆる一括消去により行われ
る。これにより記録媒体の磁化状態は、記録前の初期状
態に戻る。Conventionally, recording / erasing of information on such a recording medium is performed as follows. Recording is performed by irradiating a recording medium magnetized in one direction with a laser light beam to change the medium temperature to the Curie temperature Tc.
Alternatively, it is performed by increasing the temperature above the compensation temperature Tcomp and forming an inverted magnetic domain by an externally applied magnetic field and a demagnetizing field of the recording medium. For the disappearance, an external magnetic field is applied in the opposite pole to that at the time of recording, and the laser light beam is uniformly irradiated on the recording medium with the same intensity as that at the time of recording. This is done by so-called batch erase. As a result, the magnetization state of the recording medium returns to the initial state before recording.
(発明が解決しようとする問題点) この様に、従来の光磁気記録媒体に対して、記録を行う
場合には、レーザ光ビームを発生する光学系以外に、外
部磁界印加手段が必須であるため、光磁気記録・再生装
置の構成は、複雑になる傾向があった。また、外部磁界
印加手段として、従来は空心コイル、電磁石、永久磁石
等が用いられるが、これらを用いて、数百エルステッド
オーダの磁界を高速で切り替えることは困難である。従
って、消去には、上述した一括消去方式が用いられ、ま
た記録には、一定磁界中に、レーザパワーを高速変調す
る方法が用いられていた。(Problems to be Solved by the Invention) As described above, when recording is performed on the conventional magneto-optical recording medium, the external magnetic field applying means is indispensable in addition to the optical system for generating the laser light beam. Therefore, the structure of the magneto-optical recording / reproducing apparatus tends to be complicated. Further, conventionally, an air-core coil, an electromagnet, a permanent magnet, or the like has been used as the external magnetic field applying means, but it is difficult to switch a magnetic field of several hundred Oersted order at high speed using these. Therefore, the above-mentioned collective erasing method is used for erasing, and the method of modulating the laser power at high speed in a constant magnetic field is used for recording.
本発明の目的は、従来の外部磁界印加手段を必要とせず
に、記録ができる光磁気記録媒体を提供することにあ
る。It is an object of the present invention to provide a magneto-optical recording medium capable of recording without the conventional external magnetic field applying means.
(問題点を解決するための手段) 本発明の光磁気記録媒体は、光カード記録媒体であっ
て、カード状の基体上に、高透磁率磁性体層、絶縁体層
の順に形成され、このほぼ全面にわたり、導電体から成
り、一定の間隔を有し、基体の幅方向に下り返したジグ
サグ状パターンが形成され、次に膜面に垂直方向に、磁
気異方性を有し、非晶質磁性合金膜から成る記録層、誘
電体から成る保護層の順に形成されたことを特徴とす
る。(Means for Solving the Problems) The magneto-optical recording medium of the present invention is an optical card recording medium, in which a high magnetic permeability magnetic layer and an insulating layer are formed in this order on a card-shaped substrate. A zigzag pattern formed of conductors is formed over almost the entire surface at regular intervals and has a zigzag pattern that descends in the width direction of the substrate, and then has magnetic anisotropy in the direction perpendicular to the film surface and is amorphous. It is characterized in that a recording layer made of a magnetic alloy film and a protective layer made of a dielectric are formed in this order.
(作用) 基体上に、高透磁率磁性体層と絶縁体層を介して形成さ
れた、導電体から成り、一定間隔を有するジグサグ状パ
ターンに電流を流すことによって、前記パターンの間に
形成された記録層部分には垂直方向にバイアス磁界が印
加される。上記高磁率磁性体層は、記録層部分に、上記
バイアス磁界を効率良く導く働きをする。このバイアス
磁界印加方向は電流方向を切り替えることによって容易
に切り替えることができる。従って、一定のレーザパワ
ーを照射しながら、バイアス磁界を切り替えることによ
って所望の記録が行える。(Operation) A zigzag pattern made of a conductor, which is formed on the substrate via a high-permeability magnetic layer and an insulator layer, is formed between the patterns by passing a current in a zigsag pattern. A bias magnetic field is applied to the recording layer portion in the vertical direction. The high magnetic susceptibility magnetic layer functions to efficiently guide the bias magnetic field to the recording layer portion. The bias magnetic field application direction can be easily switched by switching the current direction. Therefore, desired recording can be performed by switching the bias magnetic field while irradiating a constant laser power.
(実施例) 次に本発明の実施例について図面を用いて詳細に説明す
る。第1図は、本発明に係る光磁気記録媒体の実施例を
示す。第2図は、断面構成図である。カード状ガラス基
板1上にパーマロイ等のNiFe合金から成る厚さ1000Åの
高透磁率磁性体層2、SiN膜から成る厚さ500Åの絶縁体
層3が形成され、この上のほぼ全面にわたり、その幅方
向に折返したAuやAl等の導電体から成るジグサグ状パタ
ーン4が、高さ約3000Å、幅約4000Å、ピッチ約1μm
で形成され、さらにこの上、膜面に垂直方向に磁気異方
性を有し、非晶質磁性合金膜から成る記録層5として、
厚さ3000ÅのTbFeCo合金膜(Tb0.22(Fe0.9C
o0.1)0.78)、さらに保護層6として、屈折率2.0厚さ8
00ÅのSiN膜の順に形成されている。(Example) Next, the Example of this invention is described in detail using drawing. FIG. 1 shows an embodiment of a magneto-optical recording medium according to the present invention. FIG. 2 is a sectional configuration diagram. A 1000 Å-thick high-permeability magnetic layer 2 made of a NiFe alloy such as permalloy and a 500 Å-thick insulator layer 3 made of a SiN film are formed on a card-shaped glass substrate 1, and almost all over the layer. The zigsag pattern 4 made of conductor such as Au or Al folded back in the width direction has a height of about 3000Å, a width of about 4000Å and a pitch of about 1 μm.
And further has a magnetic anisotropy in the direction perpendicular to the film surface, and as a recording layer 5 made of an amorphous magnetic alloy film,
3000 Å thick TbFeCo alloy film (Tb 0.22 (Fe 0.9 C
o 0.1 ) 0.78 ), and as a protective layer 6, a refractive index 2.0 thickness 8
It is formed in the order of 00Å SiN film.
各層は、マグネトロンスパッタにより成膜される。ま
ず、Au等の導電体から成るジグザグ状パターンは、次の
様にして形成される。カード状ガラス基板上に、厚さ10
00ÅのNiFe合金膜、厚さ500ÅのSiN膜、厚さ3000ÅのAu
膜の順に成膜した後、第3図(a)に示す様に、厚さ20
00Å、幅5000Åのレジストパターン7を、1μmピッチ
で形成し、Arを用いてガス圧2.6×10-2Paで4分間イオ
ンミリングする。さらに、酸素プラズマにより残ったレ
ジストを、はく離することによって、第3図(b)に示
す様に、Auの折り返し状パターン4が高さ3000Å、幅40
00Åピッチ約1μmで形成される。記録層を成すTbFeCo
合金膜は、FeCoターゲット上に、Tb片を配した複合ター
ゲットを用い、Arガス雰囲気で、パワー密度4W/cm2、ス
パッタガス圧3.5×10-1Paで作製される。Each layer is formed by magnetron sputtering. First, the zigzag pattern made of a conductor such as Au is formed as follows. On a card-shaped glass substrate, a thickness of 10
00Å NiFe alloy film, 500Å thickness SiN film, 3000Å thickness Au
After forming the film in order, as shown in FIG.
A resist pattern 7 having a width of 00 Å and a width of 5000 Å is formed at a pitch of 1 μm, and ion milling is performed using Ar for a gas pressure of 2.6 × 10 −2 Pa for 4 minutes. Further, by peeling off the resist remaining by the oxygen plasma, the folded pattern 4 of Au has a height of 3000 Å and a width of 40 mm as shown in FIG. 3 (b).
It is formed with a pitch of about 1 μm. TbFeCo forming the recording layer
The alloy film is produced by using a composite target in which Tb pieces are arranged on a FeCo target in an Ar gas atmosphere with a power density of 4 W / cm 2 and a sputtering gas pressure of 3.5 × 10 -1 Pa.
次に、本発明による光磁気記録媒体を用いた記録動作
を、第1図、第4図を用いて説明する。導電体端子A,B
間に電流を流すことによって、ジグサグ状パターンのま
わりに破線で示す磁界8を生じ、これらのパターンの間
に形成された記録層部分には、垂直方向にバイアス磁界
を印加することができる。そして、このバイアス磁界の
印加方向及び大きさは導電体端子A,B間に流す電流の方
向及び大きさにより、容易に選択できる。従って、第4
図に示す様に、レーザビーム10をカード状光磁気記録媒
体に対して相対運動させ、前記折り返し状パターンの間
にある所望の記録層部分に照射して、記録層の温度をキ
ュリー温度以上(220℃)に上昇させながら、着磁する
タイミングに同期して、導電体端子A,B間に流す電流を
スイッチングすることによって、記録層の冷却過程で所
望の記録磁化9を実現することができる。電流値は、記
録層の膜組成に応じて、数十〜数百ミリアンペアの範囲
で適宜選択される。Next, a recording operation using the magneto-optical recording medium according to the present invention will be described with reference to FIGS. Conductor terminals A, B
By passing a current between them, a magnetic field 8 shown by a broken line is generated around the zigzag pattern, and a bias magnetic field can be applied in the vertical direction to the recording layer portion formed between these patterns. The direction and magnitude of the bias magnetic field can be easily selected depending on the direction and magnitude of the current flowing between the conductor terminals A and B. Therefore, the fourth
As shown in the figure, the laser beam 10 is moved relative to the card-shaped magneto-optical recording medium, and the desired recording layer portion between the folded patterns is irradiated, and the temperature of the recording layer is equal to or higher than the Curie temperature ( The desired recording magnetization 9 can be realized during the cooling process of the recording layer by switching the current flowing between the conductor terminals A and B in synchronization with the magnetization timing while increasing the temperature to 220 ° C.). . The current value is appropriately selected within the range of several tens to several hundreds of milliamperes depending on the film composition of the recording layer.
ここで、導電体パターンの高さ及びピッチ等の形状及び
折り返し数並びに高透磁率磁性体層の厚さは、上述のも
のに限定されるものではなく、所望の記録媒体の記録感
度及びバイアス磁界の大きさに応じて、適宜選定され
る。パターンの高さとしては数千オングストローム、ピ
ッチとしては、1μm前後が好ましい。誘電体からなる
保護層及び絶縁層としては、SiNの他にAlN,SiO2,SiO等
を数百〜数千Åの厚さに形成したものが用いられる。Here, the shape such as the height and pitch of the conductor pattern, the number of turns, and the thickness of the high-permeability magnetic layer are not limited to those described above, but the recording sensitivity and the bias magnetic field of a desired recording medium are not limited. It is appropriately selected according to the size of. The height of the pattern is preferably several thousand angstroms, and the pitch is preferably around 1 μm. As the protective layer and the insulating layer made of a dielectric material, a layer in which AlN, SiO 2 , SiO or the like is formed in a thickness of several hundred to several thousand liters in addition to SiN is used.
(発明の効果) 以上述べた様に、本発明によれば、バイアス磁界を媒体
内に内蔵した折り返し状パターンに流す電流によって制
御できる新規なカード状光磁気記録媒体を提供できる。
又、基体と導電体パターンの間に絶縁層を介して設けた
高透磁率磁性体層は、上記バイアス磁界を記録領域に効
率良く導く働きがある。(Effects of the Invention) As described above, according to the present invention, it is possible to provide a novel card-shaped magneto-optical recording medium in which the bias magnetic field can be controlled by the current flowing in the folded pattern built in the medium.
Further, the high magnetic permeability magnetic layer provided between the substrate and the conductor pattern via the insulating layer has a function of efficiently guiding the bias magnetic field to the recording region.
第1図,第2図は、本発明の実施例を示す図、第3図
は、本発明の作製法を示す図、第4図は本発明の動作を
説明する図である。 図において、1……基板、2……高透磁率磁性層、3…
…絶縁層、4……導電体から成る折り返し状パターン、
5……記録層、6……保護層、7……レジストパター
ン、8……磁界、9……磁化、10……レーザビームであ
る。1 and 2 are diagrams showing an embodiment of the present invention, FIG. 3 is a diagram showing a manufacturing method of the present invention, and FIG. 4 is a diagram explaining an operation of the present invention. In the figure, 1 ... Substrate, 2 ... High-permeability magnetic layer, 3 ...
... Insulating layer, 4 ... Folded pattern made of conductor,
5 ... recording layer, 6 ... protective layer, 7 ... resist pattern, 8 ... magnetic field, 9 ... magnetization, 10 ... laser beam.
Claims (1)
体上に、高透磁率磁性体層、絶縁体層の順に形成され、
このほぼ全面にわたり、導電体から成り、一定の間隔を
有し、基体の幅方向に折り返したジグサグ状パターンが
形成され、次に膜面に垂直方向に、磁気異方性を有し、
非晶質磁性合金膜から成る記録層、誘電体から成る保護
層の順に形成されたことを特徴とする光磁気記録媒体。1. An optical card recording medium, wherein a high magnetic permeability magnetic layer and an insulating layer are formed in this order on a card-shaped substrate,
A zigsag-like pattern formed of a conductor and having a constant interval and folded back in the width direction of the substrate is formed over almost the entire surface, and then has a magnetic anisotropy in the direction perpendicular to the film surface.
A magneto-optical recording medium comprising a recording layer made of an amorphous magnetic alloy film and a protective layer made of a dielectric material in this order.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP30080086A JPH0673200B2 (en) | 1986-12-16 | 1986-12-16 | Magneto-optical recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP30080086A JPH0673200B2 (en) | 1986-12-16 | 1986-12-16 | Magneto-optical recording medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63152049A JPS63152049A (en) | 1988-06-24 |
| JPH0673200B2 true JPH0673200B2 (en) | 1994-09-14 |
Family
ID=17889249
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP30080086A Expired - Lifetime JPH0673200B2 (en) | 1986-12-16 | 1986-12-16 | Magneto-optical recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0673200B2 (en) |
-
1986
- 1986-12-16 JP JP30080086A patent/JPH0673200B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63152049A (en) | 1988-06-24 |
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