JPH0673198B2 - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- Publication number
- JPH0673198B2 JPH0673198B2 JP30079586A JP30079586A JPH0673198B2 JP H0673198 B2 JPH0673198 B2 JP H0673198B2 JP 30079586 A JP30079586 A JP 30079586A JP 30079586 A JP30079586 A JP 30079586A JP H0673198 B2 JPH0673198 B2 JP H0673198B2
- Authority
- JP
- Japan
- Prior art keywords
- recording medium
- magneto
- recording
- magnetic field
- optical recording
- 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 13
- 239000004020 conductor Substances 0.000 claims description 11
- 239000000758 substrate Substances 0.000 claims description 7
- 239000011241 protective layer Substances 0.000 claims description 6
- 230000003287 optical effect Effects 0.000 claims description 4
- 239000003989 dielectric material Substances 0.000 claims description 3
- 229910001004 magnetic alloy Inorganic materials 0.000 claims description 2
- 239000010408 film Substances 0.000 description 14
- 239000007789 gas Substances 0.000 description 6
- 230000005415 magnetization Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 230000015654 memory Effects 0.000 description 4
- 238000000034 method Methods 0.000 description 3
- 238000004544 sputter deposition Methods 0.000 description 3
- 229910045601 alloy Inorganic materials 0.000 description 2
- 239000000956 alloy Substances 0.000 description 2
- 230000008901 benefit Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 229910052742 iron Inorganic materials 0.000 description 2
- 230000001678 irradiating effect Effects 0.000 description 2
- 230000005381 magnetic domain Effects 0.000 description 2
- 238000004519 manufacturing process Methods 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
- 230000006870 function Effects 0.000 description 1
- 238000001755 magnetron sputter deposition Methods 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 229910052759 nickel Inorganic materials 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 239000001301 oxygen Substances 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
- 238000005546 reactive sputtering Methods 0.000 description 1
- 230000035945 sensitivity Effects 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
きる光磁気記録媒体に関するものである。TECHNICAL FIELD The present invention relates to a recording medium used in a magneto-optical memory, and more specifically, a magnetic film having an easy axis of magnetization in a direction perpendicular to the film surface as a recording layer. The present invention relates to a magneto-optical recording medium in which information can be recorded by forming a reversed magnetic domain in a region irradiated with a light beam such as a laser and which can be read by utilizing a magneto-optical effect.
(従来技術) 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 direction perpendicular to the film surface with high recording sensitivity and no grain boundary noise. It is the most promising because it has advantages such as easy production of a film having properties.
従来、この様な記録媒体に対する情報の記録・消去は次
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。消去は、外部磁界を記録時とは逆極性に
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. The erasing is performed by so-called batch erasing, in which an external magnetic field is applied with a polarity opposite to that used during recording, and a laser light beam is uniformly irradiated onto the recording medium at the same intensity as during recording.
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式が用いら
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 unit is essential in addition to the optical system for generating the laser light beam. The structure of the magneto-optical recording / reproducing device tends to be complicated. Further, air core coils, electromagnets, permanent magnets and the like have been conventionally used as the external magnetic field applying means, but it is difficult to use these to switch a magnetic field of several hundred Oersted order at high speed. Therefore, the above-mentioned batch erasing method is used for erasing, and recording is
A method of modulating the laser power at high speed in a constant magnetic field has been used.
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
グザ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, which is made of a conductor and has a constant interval over almost the entire surface of a card-shaped substrate. Zigzag pattern is formed by folding back in the width direction of, and then in the direction perpendicular to the film surface,
A recording layer having magnetic anisotropy and made of an amorphous magnetic alloy film,
It is characterized in that a protective layer made of a dielectric material is formed in this order.
(作用) 基体上に形成された導電体から成り、一定間隔を有する
ジグザ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。このバイアス磁界印加方向は
電流を流す方向を切り替えることによって、容易に切り
替えることがでぎる。従って一定のレーザパワーを照射
しながら、バイアス磁界の切り替えによって所望の記録
が行える。(Function) A bias magnetic field is applied in a vertical direction to the recording layer portion formed between the patterns by applying a current to a zigzag pattern formed of a conductor formed on a substrate and having a constant interval. It The bias magnetic field application direction can be easily switched by switching the direction of current flow. 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上のほぼ全面にわたり、その幅方向に折り返したAuや
Al等の導電体から成るジグザグ状パターン2が、高さ約
3000Å、幅約4000、Åピッチ約1μmで形成され、この
上に、膜面に垂直方向に磁気異方性を有し、非晶質磁性
合成膜から成る記録層3として、厚さ3000ÅのTb,Fe,Co
合金膜(Tb0.22(Fe0.9Co0.01)0.78)、さらに保護層
4として屈折率2.0厚さ800ÅのSi3N4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. Over almost the entire surface of the card-shaped glass substrate 1, Au folded in the width direction and
The zigzag pattern 2 made of a conductor such as Al has a height of about
It is formed with 3000 Å, width of about 4000, Å pitch of about 1 μm, and has a magnetic anisotropy in the direction perpendicular to the film surface, and a recording layer 3 made of an amorphous magnetic synthetic film with a thickness of 3000 Å Tb. , Fe, Co
An alloy film (Tb 0.22 (Fe 0.9 Co 0.01 ) 0.78 ) and a Si 3 N 4 film having a refractive index of 2.0 and a thickness of 800 Å are formed in this order as the protective layer 4.
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折り返し状パターン2は次の様に
して形成される。カード状ガラス基板1上に、Au膜を30
00Åの厚さに、スパッした後、第3図(a)に示す様
に、厚さ2000Å、幅5000Åのレジストパターン5を1μ
m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2が、高さ3000
Å、幅4000Å、ピッチ約1μmで形成される。Each layer is formed by magnetron sputtering. First,
The folded pattern 2 made of a conductor such as Au is formed as follows. 30 Au film on card-shaped glass substrate 1
After spattering to a thickness of 00Å, as shown in Fig. 3 (a), a resist pattern 5 having a thickness of 2000Å and a width of 5000Å is set to 1 µm.
Formed at m pitch, and using Ar, gas pressure 2.6 × 10 -2 Pa 4
Ion mill for minutes. Further, by removing the remaining resist by oxygen plasma, FIG.
As shown in, the Au folded pattern 2 has a height of 3000
Å, width 4000 Å, pitch about 1 μm.
記録層3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。The TbFeCo alloy film forming the recording layer 3 is formed on the FeCo target,
Using a composite target with Tb pieces arranged, in an Ar gas atmosphere,
It is manufactured with a power density of 4 w / cm 2 and a sputtering gas pressure of 3.5 × 10 -1 Pa.
保護層4を成すSi3N4膜は、Siターゲットを用い、ArとN
2の混合ガス(45.5%N2)を、スパッタガスとた反応性
スパッタによりパワー密度8w/cm2、スパッタガス圧2.5
×10-1Paで作製される。The Si 3 N 4 film forming the protective layer 4 uses a Si target and Ar and N
The power density was 8 w / cm 2 and the sputtering gas pressure was 2.5 by reactive sputtering using a mixed gas of 2 (45.5% N 2 ) as the sputtering gas.
Manufactured at × 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、折り返し状パターン2のまわ
りに破線で示す磁界6を生じ、これらのパターン間に形
成された記録層部分には、垂直方向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8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2の間にあ
る所望の記録層部分に照射して記録層3の温度をキュリ
温度以上(220℃)に上昇させながら、着磁するタイミ
ングにあわせて導電体端子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3の冷却過程で所望の記
録磁化7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, the recording operation using the magneto-optical recording medium according to the present invention will be described.
This will be described with reference to FIGS. 1 and 4. By passing a current between the conductor terminals A and B, a magnetic field 6 shown by a broken line is generated around the folded pattern 2, and a vertical bias magnetic field is applied to the recording layer portion formed between these patterns. be able to. The application direction and magnitude of this 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, as shown in FIG. 4, the laser beam 8 is moved relative to the card-shaped magneto-optical recording medium to irradiate a desired recording layer portion between the folded patterns 2 and the temperature of the recording layer 3 is changed. The desired recording magnetization 7 is realized in the cooling process of the recording layer 3 by switching the current flowing between the conductor terminals A and B in synchronization with the magnetization timing while increasing the temperature above the Curie temperature (220 ° C). can do. 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
り返し数等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密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
万オングストローム、ピッチとしては1μm前後が好ま
しい。誘電体から成る保護層としては、Si3N4の他にAI
N,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 like are not limited to those described above, and are appropriately selected according to the desired recording density of the recording medium and the magnitude of the bias magnetic field. . The height of the pattern is preferably tens of millions of angstroms, and the pitch is preferably around 1 μm. As a protective layer made of a dielectric material, in addition to Si 3 N 4 , AI
N, which was formed SiO 2, SiO or the like to a thickness of several hundred to several thousand Å 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導電体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。(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 conductor pattern built in the medium.
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……導電体から成る折り返
し状パターン、3……記録層、4……保護層、5……レ
ジストパターン、6……磁界、7……磁化、8……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 ... Folded pattern made of conductor, 3 ... Recording layer, 4 ... Protective layer, 5 ... Resist pattern, 6 ... Magnetic field, 7 ... Magnetization, 8 ... It is a laser beam.
Claims (1)
体上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ザグ状パターン
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 zigzag pattern, which is made of a conductor and has a constant interval and is folded back in the width direction of the substrate, is formed over substantially the entire surface of a card-shaped substrate. A magneto-optical recording medium having a magnetic anisotropy in the direction perpendicular to the film surface, and a recording layer made of an amorphous magnetic alloy film and a protective layer made of a dielectric material are formed in this order.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP30079586A JPH0673198B2 (en) | 1986-12-16 | 1986-12-16 | Magneto-optical recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP30079586A JPH0673198B2 (en) | 1986-12-16 | 1986-12-16 | Magneto-optical recording medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63152044A JPS63152044A (en) | 1988-06-24 |
| JPH0673198B2 true JPH0673198B2 (en) | 1994-09-14 |
Family
ID=17889188
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP30079586A Expired - Lifetime JPH0673198B2 (en) | 1986-12-16 | 1986-12-16 | Magneto-optical recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0673198B2 (en) |
-
1986
- 1986-12-16 JP JP30079586A patent/JPH0673198B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63152044A (en) | 1988-06-24 |
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