JPH0622171B2 - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- Publication number
- JPH0622171B2 JPH0622171B2 JP58233907A JP23390783A JPH0622171B2 JP H0622171 B2 JPH0622171 B2 JP H0622171B2 JP 58233907 A JP58233907 A JP 58233907A JP 23390783 A JP23390783 A JP 23390783A JP H0622171 B2 JPH0622171 B2 JP H0622171B2
- Authority
- JP
- Japan
- Prior art keywords
- magneto
- magnetic
- optical recording
- recording medium
- film
- 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
Landscapes
- Compounds Of Iron (AREA)
- Hard Magnetic Materials (AREA)
- Thin Magnetic Films (AREA)
Description
【発明の詳細な説明】 技術分野 本発明は新規な金属酸化物磁性体よりなる磁性膜を有す
る光磁気記録媒体に関する。TECHNICAL FIELD The present invention relates to a magneto-optical recording medium having a magnetic film made of a novel metal oxide magnetic material.
従来技術 近年、半導体レーザー光により磁気記録を行なう光磁気
記録媒体が高密度記録用として研究開発されている。従
来、光磁気記録媒体に用いられる磁性体としては希土類
金属と遷移金属との非晶質合金からなるものが多い。こ
のような非晶質合金磁性体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、、
例えばTb−Fe合金を真空蒸着、スパッタリング等の方法
で厚さ0.1〜1μm程度に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
次のようにして行なわれる。即ち記録は磁性膜のキュリ
ー温度又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2値信号で変調された
レーザー光を磁性膜に照射加熱して磁化の向きを反転さ
せることにより行なわれる。また再生はこうして反転記
録された磁性膜の磁気光学効果の差を利用して読出すこ
とにより行なわれる。前述のような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いため、半導体レ
ーザー光によって高速度(周波数1MHzにおいて)で記録
できるという利点はあるが、非晶質合金磁性体、特に希
土類金属成分は酸化腐食を受け易いので、経時と共に磁
性膜の磁気光学特性が劣化するという大きな欠点があ
る。これを防止するため、非晶質磁性膜上にSiO,S
iO2等の保護膜を設ける(形成法は磁性膜の場合と同
様、真空蒸着、スパッタリング等による)ことも知られ
ているが、磁性膜或いは保護膜の形成時、真空中に残存
するO2、基板面に吸着されたO2,H2O等及び合金
磁性体のターゲット中に含まれるO2,H2O等により
経時と共に磁性膜が酸化腐食される上、記録時の光及び
熱により更にこの酸化腐食は促進される。また非結晶質
磁性体は熱によって結晶化され易く、そのために磁気特
性の劣化を来たし易いという欠点を有する。更に再生出
力を向上するための再生方式として磁性膜をできるだけ
厚くし、その上にCu,Al,Pt,Ag等の反射膜を
設け、レーザー光を磁性膜に照射透過させた後、反射膜
で反射させ、この反射光を検出する反射型ファラデー方
式は高S/Nの信号が得られるという点で有利である
が、従来の非晶質磁性膜は透光性に欠けるため、この方
式に用いることができないものであった。2. Description of the Related Art In recent years, a magneto-optical recording medium for performing magnetic recording with a semiconductor laser beam has been researched and developed for high density recording. Conventionally, most magnetic materials used in magneto-optical recording media are amorphous alloys of rare earth metals and transition metals. In order to manufacture a magneto-optical recording medium using such an amorphous alloy magnetic material, the magnetic material is generally provided on a substrate such as a glass plate,
For example, a magnetic film is formed by adhering a Tb-Fe alloy to a thickness of about 0.1 to 1 μm by a method such as vacuum deposition and sputtering. Recording and reproduction on the thus obtained magneto-optical recording medium are performed as follows. That is, the recording is performed by irradiating and heating the magnetic film with laser light modulated by a binary signal by utilizing the rapid change characteristic of the coercive force corresponding to the temperature change in the vicinity of the Curie temperature or the compensation temperature of the magnetic film to change the direction of magnetization. It is performed by reversing. In addition, reproduction is performed by reading by utilizing the difference in magneto-optical effect of the magnetic film thus recorded in reverse. Since the magneto-optical recording medium using the amorphous alloy magnetic material as described above has a high recording sensitivity, it has an advantage that it can be recorded at a high speed (at a frequency of 1 MHz) by a semiconductor laser light. In particular, since the rare earth metal component is susceptible to oxidative corrosion, there is a major drawback that the magneto-optical characteristics of the magnetic film deteriorate with time. In order to prevent this, SiO, S is formed on the amorphous magnetic film.
It is also known to provide a protective film such as iO 2 (the forming method is vacuum evaporation, sputtering, etc. as in the case of the magnetic film), but O 2 which remains in vacuum when the magnetic film or the protective film is formed , on the magnetic film is oxidized and corroded with time by O 2, H 2 O or the like contained in the target of the adsorbed O 2, H 2 O and the like and alloys magnetic surface of the substrate, the recording time of the light and heat Furthermore, this oxidative corrosion is accelerated. Further, the amorphous magnetic material has a drawback that it is easily crystallized by heat, which easily deteriorates the magnetic characteristics. As a reproducing method for further improving the reproducing output, the magnetic film is made as thick as possible, and a reflective film of Cu, Al, Pt, Ag, etc. is provided on the magnetic film, and after the laser light is irradiated and transmitted through the magnetic film, The reflection type Faraday method of reflecting and detecting the reflected light is advantageous in that a high S / N signal can be obtained, but since the conventional amorphous magnetic film lacks translucency, it is used for this method. It was impossible.
目 的 本発明の目的は新規な金属化物磁性体よりなる磁性膜を
有する記録感度が高く、しかも耐酸化腐食性及び透光性
に優れた光磁気記録媒体を提供することである。It is an object of the present invention to provide a magneto-optical recording medium which has a magnetic film made of a novel metallized magnetic material, has high recording sensitivity, and is excellent in oxidative corrosion resistance and translucency.
構 成 本発明の光磁気記録媒体に用いる金属酸化物磁性体は一
般式 CoMxFe2−xO4 (但しM=Mn,Ni,Ti,Zn,Al,Sn,Cr,Cu,Mg,Rh,V,Ga,In,Sb,S
c,Bi,Y,Sm,Eu,Tb及びGdからなる群の少なくとも1種,0.
4≦x≦1.4) で示されるものであり、また磁性膜は前記一般式の金属
化物磁性体よりなるものである。Structure The metal oxide magnetic material used in the magneto-optical recording medium of the present invention has the general formula CoM x Fe 2 -x O 4 (where M = Mn, Ni, Ti, Zn, Al, Sn, Cr, Cu, Mg, Rh). , V, Ga, In, Sb, S
at least one member of the group consisting of c, Bi, Y, Sm, Eu, Tb and Gd, 0.
4 ≦ x ≦ 1.4) and the magnetic film is made of the metallized magnetic material of the above general formula.
光磁気記録媒体に用いられる磁性体又は磁性膜には半導
体レーザー光によって記録、再生可能な磁気光学特性
(適正なキュリー温度、保磁力等)を備えていなければ
ならないが、特に高い記録感度を得るためにキュリー温
度Tcが低いこと及び記録したメモリーを安定に維持す
るために保磁力Hcが適度に高いことが必要である。一
般にこのTc及びHcの適正範囲はTcについては100
〜350℃、については300〜6000エルステッドと考えられ
る。これはTcが100℃以下では記録したメモリーが再
生時のレーザー光によって不安定になって再生特性の劣
化原因となり、また、350℃以上では半導体レーザー光
による記録が困難であり、一方、Hcが300エルステッド
以下ではメモリーが不安定となって消失する可能性があ
り、また6000エルステッド以上では記録時の磁化反転に
必要なレーザー出力や外部磁界が大きくなり、好ましく
ないからである。The magnetic substance or magnetic film used in the magneto-optical recording medium must have magneto-optical characteristics (appropriate Curie temperature, coercive force, etc.) that can be recorded and reproduced by semiconductor laser light, but particularly high recording sensitivity is obtained. Therefore, it is necessary that the Curie temperature Tc is low and that the coercive force Hc is appropriately high in order to stably maintain the recorded memory. Generally, the proper range of Tc and Hc is 100 for Tc.
For ~ 350 ° C, it is considered to be 300-6000 Oersted. This is because when the Tc is 100 ° C. or lower, the recorded memory becomes unstable due to the laser light during reproduction, which causes deterioration of the reproducing characteristics, and when the temperature is 350 ° C. or higher, recording by the semiconductor laser light is difficult. If it is less than 300 oersteds, the memory may become unstable and may disappear, and if it is more than 6000 oersteds, the laser output and the external magnetic field necessary for the magnetization reversal at the time of recording become large, which is not preferable.
一方、従来より磁気バルブ材料として六方晶糸及びスピ
ネル糸の金属酸化物磁性体が研究されている。このうち
スピネル糸のものでは例えばCoスピネル型鉄酸化物が
知られている。本発明者らはこの種の磁性体がそれ自
体、酸化物であるため、酸化劣化の恐れがなく、しかも
膜厚10μmとしても透光性を備えていることに注目し
た。しかしこれらはキュリー温度Tcが450℃以上と高
いため、前述のように半導体レーザー光による記録は困
難であり、そのままでは光磁気記録媒体用材料として適
用できない。そこで本発明者らは種々検討したところ、
Coスピネル型鉄酸化物の中のFe原子の一部を前記M
で示される金属(以下M金属という)原子で置換する
と、Tcが低下することを見出した。そこで本発明者ら
はこのようなM金属の置換効果に着目し、更に光磁気記
録媒体用の磁性体又は磁性膜に要求されるTc及びHc
の前記適正範囲を考慮してCoスピネル型鉄酸化物のF
eの一部をM金属で種々の割合で置換した結果、前記一
般式の金属酸化物磁性体が光磁気記録媒体として優れた
特性を与えることを見出し、本発明に到達した。On the other hand, as a magnetic valve material, a hexagonal crystal thread and a spinel thread metal oxide magnetic material have been studied. Among them, for spinel yarn, for example, Co spinel type iron oxide is known. The inventors of the present invention noted that this kind of magnetic substance is an oxide itself, so that there is no fear of oxidative deterioration and that it has translucency even when the film thickness is 10 μm. However, since the Curie temperature Tc of them is as high as 450 ° C. or higher, it is difficult to record with a semiconductor laser beam as described above, and they cannot be applied as they are as a material for a magneto-optical recording medium. Therefore, the present inventors have made various studies,
A part of the Fe atoms in the Co spinel type iron oxide is M
It was found that Tc is lowered by substituting with a metal atom represented by (hereinafter referred to as M metal) atom. Therefore, the present inventors have paid attention to such an effect of substituting M metal, and further, Tc and Hc required for a magnetic body or a magnetic film for a magneto-optical recording medium.
In consideration of the appropriate range of F of Co spinel type iron oxide
As a result of substituting a part of e with M metal at various ratios, it was found that the metal oxide magnetic material of the above general formula gave excellent characteristics as a magneto-optical recording medium, and the present invention was accomplished.
このように本発明は、特にキュリー温度が高いため、光
磁気記録媒体用材料として顧みられなかったCoスピネ
ル型鉄酸化物中のFe原子の一部をM金属原子で置換す
ることによって、メモリーに要求される適度に高い保磁
力を維持しながら、キュリー温度を低下せしめて半導体
レーザー光による記録、再生を可能にし、こうして光磁
気記録媒体用材料として適用できるようにしたものであ
る。As described above, according to the present invention, since the Curie temperature is particularly high, a part of Fe atoms in the Co spinel type iron oxide, which has not been neglected as a material for a magneto-optical recording medium, is replaced with M metal atoms, so that a memory can be obtained. While maintaining a required moderately high coercive force, the Curie temperature is lowered to enable recording / reproducing with a semiconductor laser beam, and thus it can be applied as a material for a magneto-optical recording medium.
以上の説明から判るように本発明の金属酸化物磁性体は
光磁気記録媒体用材料として要求される適正キュリー温
度範囲Tc及び適正保磁力範囲Hcを満足するものであ
る。これらのTc及びHc特性により本発明の金属酸化
物磁性体又は磁性膜は半導体レーザー光により記録、再
生を行なう光磁気記録媒体用材料として適用できること
は勿論、キュリー温度が低いため、記録感度が高い上、
耐酸化腐食性及び透光性を備えている等の特長を持って
いる。As can be seen from the above description, the metal oxide magnetic material of the present invention satisfies the appropriate Curie temperature range Tc and the appropriate coercive force range Hc required as a material for a magneto-optical recording medium. Due to these Tc and Hc characteristics, the metal oxide magnetic material or magnetic film of the present invention can be applied as a material for a magneto-optical recording medium for recording / reproducing with a semiconductor laser beam, and of course, because of its low Curie temperature, high recording sensitivity. Up,
It has features such as oxidation resistance and translucency.
本発明の金属酸化物磁性体を作るにはFe2O31モル
とCo2O30.5モルとM2O30.5モルとを混合粉砕
し、これを適当な形状の金型に入れて成型後、1200〜14
00℃の温度で焼結すればよい。In order to produce the metal oxide magnetic material of the present invention, 1 mol of Fe 2 O 3, 0.5 mol of Co 2 O 3 and 0.5 mol of M 2 O 3 are mixed and pulverized, and this is put into a mold having an appropriate shape and molded. After 1200 ~ 14
Sintering may be performed at a temperature of 00 ° C.
以上のようにして得られる本発明の金属酸化物磁性体の
具体例としては CoCr0.8 Fe1.2 O4,CoMn1.0 Fe
1.0 O4, CoCr0.75Fe1.25O4,CoCr1.2 Fe
0.8 O4, CoMn0.75Fe1.25O4,CoAl0.8 Fe
1.2 O4, CoAl1.0 Fe1.0 O4,CoZn0.75Fe
1.25O4, CoZn1.0 Fe1.0 O4,CoTi0.8 Fe
1.2 O4, CoSn1.2 Fe0.8 O4,CoCu1.0 Fe
1.0 O4, CoRh0.5 Fe0.5 O4,CoCr0.85Fe
1.15O4, CoCr1.0 Fe1.0 O4,CoMn0.4 Fe
1.0 O4, CoMn0.9 Fe1.1 O4,CoCr0.8 Bi0.2 Fe
1.0 O4 CoMn0.6 Bi0.2 Fe1.2 O4,CoAl0.8 Bi
0.1 Fe1.1 O4, CoCr0.8 V0.1 Fe1.1 O4,CoMn0.7 Sn
0.1 Fe1.2 O4, CoMn0.8 V0.1 Bi0.1 Fe1.0 O4 等が挙げられる。Specific examples of the metal oxide magnetic material of the present invention obtained as described above include CoCr 0.8 Fe 1.2 O 4 and CoMn 1.0 Fe.
1.0 O 4 , CoCr 0.75 Fe 1.25 O 4 , CoCr 1.2 Fe
0.8 O 4 , CoMn 0.75 Fe 1.25 O 4 , CoAl 0.8 Fe
1.2 O 4 , CoAl 1.0 Fe 1.0 O 4 , CoZn 0.75 Fe
1.25 O 4 , CoZn 1.0 Fe 1.0 O 4 , CoTi 0.8 Fe
1.2 O 4 , CoSn 1.2 Fe 0.8 O 4 , CoCu 1.0 Fe
1.0 O 4 , CoRh 0.5 Fe 0.5 O 4 , CoCr 0.85 Fe
1.15 O 4 , CoCr 1.0 Fe 1.0 O 4 , CoMn 0.4 Fe
1.0 O 4 , CoMn 0.9 Fe 1.1 O 4 , CoCr 0.8 Bi 0.2 Fe
1.0 O 4 CoMn 0.6 Bi 0.2 Fe 1.2 O 4 , CoAl 0.8 Bi
0.1 Fe 1.1 O 4 , CoCr 0.8 V 0.1 Fe 1.1 O 4 , CoMn 0.7 Sn
0.1 Fe 1.2 O 4, CoMn 0.8 V 0.1 Bi 0.1 Fe 1.0 O 4 and the like.
なお以上のような金属酸化物磁性体にはファラデー回転
角を更に増大して磁気光学特性を改善するためにLa,
Yb,Dy等の金属を添加することができる。In addition, in order to improve the magneto-optical characteristics by further increasing the Faraday rotation angle, the above metal oxide magnetic material has La,
Metals such as Yb and Dy can be added.
本発明の金属酸化物磁性体を用いて磁性膜を作るには、
基板の種類にもよるが、一般に基板上にこの磁性体をタ
ーゲットとして基板温度500〜700℃で真空蒸着、スパッ
タリング、イオンプレーティング等の方法で膜厚0.1〜1
0μm程度に付着させればよい。こうして第5図に示す
ように基板1上に、垂直磁化された磁性膜2を有する光
磁気記録媒体が得られる。なお場合によっては磁性膜の
形成は基板温度500℃未満で行なうこともできる。但し
この場合は磁性膜形成後、これに500〜800℃の熱処理
を、場合により磁界を印加しながら、行なって垂直磁化
させる必要がある。ここで基板の材料としては一般にア
ルミニウムのような耐熱性金属;石英ガラス;GGG;
サファイヤ;リチウムタンタレート;結晶化透明ガラ
ス;パイレックスガラス;表面を酸化処理し又は処理し
ない単結晶シリコン;Al2O3,Al2O3・Mg
O,MgO・LiF,Y2O3・LiF,BeO,Zr
O2・Y2O3,ThO2・CaO等の透明セラミック
材;無機シリコン材(例えば東芝シリコン社製トスガー
ド、住友化学社製スミセラムP)等の無機材料或いはア
クリル樹脂、ポリカーボネート樹脂、ポリエステル樹脂
等の有機材料が使用できる。To make a magnetic film using the metal oxide magnetic material of the present invention,
Depending on the type of substrate, this magnetic material is generally used as a target on the substrate at a substrate temperature of 500 to 700 ° C and the film thickness is 0.1 to 1 by a method such as vacuum deposition, sputtering, or ion plating.
It may be attached to a thickness of about 0 μm. Thus, as shown in FIG. 5, a magneto-optical recording medium having the magnetic film 2 which is perpendicularly magnetized on the substrate 1 is obtained. In some cases, the magnetic film can be formed at a substrate temperature lower than 500 ° C. However, in this case, after the magnetic film is formed, it is necessary to perform heat treatment at 500 to 800 ° C. on this, while applying a magnetic field in some cases, for perpendicular magnetization. Here, the substrate material is generally a heat-resistant metal such as aluminum; quartz glass; GGG;
Sapphire; Lithium tantalate; Crystallized transparent glass; Pyrex glass; Single crystal silicon with or without surface oxidation treatment; Al 2 O 3 , Al 2 O 3 .Mg
O, MgO · LiF, Y 2 O 3 · LiF, BeO, Zr
Transparent ceramic materials such as O 2 · Y 2 O 3 and ThO 2 · CaO; inorganic materials such as inorganic silicon materials (for example, Tosgard manufactured by Toshiba Silicon Co., Sumiceram P manufactured by Sumitomo Chemical Co., Ltd.), acrylic resins, polycarbonate resins, polyester resins, etc. Organic materials can be used.
本発明の磁性膜は第1図のような単層型光磁気記録媒体
に限らず、従来公知のすべての多層型光磁気記録媒体に
適用できる。この種の多層型の例としては第2〜4図に
示すような構成のものが挙げられる。図中、1′はガイ
ドトラック付き基板、3は反射膜、4はガイドトラック
層、5は保護膜、6は透明接着層、7は耐熱層である。
ここでガイドトラック付き基板1′は前述のような有機
材料を射出成型、押出成型、フォトエッチング法等によ
り加工して作られる。なお基板のガイドトラックは記
録、再生時のレーザー光を案内するものである。反射膜
3はCu,Al,Ag,Au,Pt,TeOx,Te
C,SeAs,TeAs,TiN,TaN,CrN,シ
アニン染料、フタロシアニン染料等を真空蒸着、スパッ
タリング、イオンプレーティング等の方法で対象面に膜
厚500〜10000Å程度に付着させることにより形成され
る。なおこの反射膜は、磁性膜を透過したレーザー光を
反射し、再び磁性膜を透過することによるファラデー効
果を増大させる目的で設けられる。ガイドトラック層4
は対象面に紫外線硬化性樹脂を塗布した後、ガイド溝を
有する金型を圧着しながら、紫外線を照射して前記樹脂
を硬化させることにより形成される。保護膜5はアクリ
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,TaN,SiO2,SiO等
を樹脂の場合は塗布法で、その他の場合は真空蒸着、ス
パッタリング、イオンプレーティング等の方法で対象面
に膜厚約0.1〜10μm程度に付着させることにより形成
される。なおこの保護膜は反射膜3を保護する目的で設
けられる。透明接着層6は、反射膜3を設けたガイドト
ラック付き基板1′の反射膜と磁性膜2を設けた耐熱層
7(この層は前記無機材料よりなるので、「磁性膜を設
けた耐熱層」とは前記単層型光磁気記録材料のことであ
る。)の磁性膜とをエポキシ樹脂、ポリウレタン、ポリ
アミド等の樹脂で約2〜100μm厚程度に接着すること
により形成される。即ちこの透明接着層は単に基板1′
上の反射膜3と単層型光磁気記録材料の磁性膜2とを接
合するための層である。なお耐熱層7は前述のような無
機材料よりなるので、基板1に相当するが、ここでは磁
性膜2の耐熱性向上の目的で設けられる。厚さは約10〜
500 μm程度が適当てある。The magnetic film of the present invention can be applied not only to the single-layer type magneto-optical recording medium as shown in FIG. 1 but also to all conventionally known multi-layer type magneto-optical recording media. Examples of this type of multi-layer type include those having the configurations shown in FIGS. In the figure, 1'is a substrate with a guide track, 3 is a reflective film, 4 is a guide track layer, 5 is a protective film, 6 is a transparent adhesive layer, and 7 is a heat resistant layer.
Here, the substrate 1'with a guide track is made by processing the above-mentioned organic material by injection molding, extrusion molding, photoetching or the like. The guide track on the substrate guides the laser beam during recording and reproduction. The reflective film 3 is made of Cu, Al, Ag, Au, Pt, TeOx, Te.
It is formed by depositing C, SeAs, TeAs, TiN, TaN, CrN, cyanine dye, phthalocyanine dye, etc. on the target surface to a film thickness of about 500 to 10000Å by a method such as vacuum deposition, sputtering, and ion plating. The reflective film is provided for the purpose of reflecting the laser beam transmitted through the magnetic film and increasing the Faraday effect by transmitting the laser beam through the magnetic film again. Guide track layer 4
Is formed by applying an ultraviolet curable resin to the target surface and then irradiating ultraviolet rays to cure the resin while pressing a mold having a guide groove. The protective film 5 is an acrylic resin, a polyurethane resin, a polycarbonate resin, a polyether sulfone resin, a polyamide resin, an epoxy resin, TiN, Si 3 N 4 , TaN, SiO 2 , SiO or the like, which is a coating method in the case of a resin, and other cases. Is formed by depositing a film having a thickness of about 0.1 to 10 μm on the target surface by a method such as vacuum deposition, sputtering, and ion plating. The protective film is provided for the purpose of protecting the reflective film 3. The transparent adhesive layer 6 is a heat-resistant layer 7 provided with the magnetic film 2 and the reflection film of the substrate 1 ′ having a guide track provided with the reflection film 3 (since this layer is made of the above-mentioned inorganic material, “heat-resistant layer provided with a magnetic film”). Is a single-layer type magneto-optical recording material) and is adhered with a resin such as epoxy resin, polyurethane or polyamide to a thickness of about 2 to 100 μm. That is, this transparent adhesive layer is simply the substrate 1 '.
It is a layer for joining the upper reflection film 3 and the magnetic film 2 of the single-layer type magneto-optical recording material. Since the heat-resistant layer 7 is made of the above-mentioned inorganic material and corresponds to the substrate 1, it is provided here for the purpose of improving the heat resistance of the magnetic film 2. Thickness is about 10 ~
About 500 μm is suitable.
本発明の磁性膜を用いた以上のような光磁気記録媒体へ
の記録、再生は従来と同じく磁性膜又は基板側から変調
又は偏向されたレーザー光を照射して行なわれる。Recording and reproduction on the above-described magneto-optical recording medium using the magnetic film of the present invention are performed by irradiating a laser beam modulated or deflected from the magnetic film or the substrate side as in the conventional case.
効 果 本発明の金属酸化物磁性体又は磁性膜は光磁気記録媒体
用材料として適正なTc及びHcを有し、記録感度が高
いにも拘わらず、従来品にはなかった耐酸化腐食性及び
透明性を備えているので、磁気光学特性の経時劣化がな
く、且つ再生時に透過光も利用でき、このため再生出力
の高いファラデー回転角を利用して再生することができ
る。The metal oxide magnetic material or magnetic film of the present invention has suitable Tc and Hc as a material for a magneto-optical recording medium, and has high recording sensitivity, but has an oxidation resistance and corrosion resistance which are not present in conventional products. Since it has transparency, the magneto-optical characteristics do not deteriorate with time, and transmitted light can be used during reproduction, and therefore reproduction can be performed using a Faraday rotation angle with high reproduction output.
以下に本発明の実施例を示す。Examples of the present invention will be shown below.
実施例1〜12 Fe2O31モルとCo2O30.5モルとM2O30.5モ
ルとをボールミルでよく混合分散し、これを内径120mm
深さ2mmの円板状金型に入れて圧力300kg/cm2、温度12
00℃で2時間焼結を行ない、表記の円板状ターゲットを
得た。次にこれらのターゲットを用いてArガス90%〜
O210%の混合ガス中、基板温度200℃、ガス圧3パス
カル、放電々力50Wの条件で石英基板上にRFスパッタ
リングを行ない、5000Å厚の磁性膜を設けた。これら磁
性膜のキュリー温度Tc及び保磁力Hcを測定した結果
を下表に示す。Example 1~12 Fe 2 O 3 1 mol of Co 2 O 3 0.5 moles of the M 2 O 3 0.5 mol well mixed and dispersed in a ball mill, the inner diameter 120mm this
Placed in a disc-shaped mold with a depth of 2 mm, pressure 300 kg / cm 2 , temperature 12
Sintering was carried out at 00 ° C. for 2 hours to obtain the disc-shaped target shown. Next, using these targets, Ar gas 90% ~
RF sputtering was performed on a quartz substrate under the conditions of a substrate temperature of 200 ° C., a gas pressure of 3 Pascal, and a discharge power of 50 W in a mixed gas of O 2 10% to form a magnetic film having a thickness of 5000 Å. The results of measuring the Curie temperature Tc and the coercive force Hc of these magnetic films are shown in the table below.
次に以上のようにして得られた各光磁気記録媒体を800
℃に加熱しながら外部より10Kエルステッドの磁界を印
加することにより垂直方向に磁化させ、この磁化の方向
とは逆の500エルステッドの磁界を印加しながら、出力2
0mWの半導体レーザー光を記録媒体表面での強度10mW及
び周波数1MHzのパルスで照射して磁気反転せしめ、記録
したところ、いずれもピット径約1.5μmの記録ピット
が形成された。 Next, each of the magneto-optical recording media obtained as described above is
Applying a magnetic field of 10K oersted from the outside while heating to ℃, magnetize in the perpendicular direction, and apply a magnetic field of 500 oersted opposite to the direction of this magnetization, and output 2
When recording was performed by irradiating 0 mW of semiconductor laser light with a pulse of intensity 10 mW and frequency 1 MHz on the surface of the recording medium for magnetic reversal and recording, a recording pit having a pit diameter of about 1.5 μm was formed in each case.
第1〜4図は夫々本発明の光磁気記録媒体の一例の構成
図である。 1……基板 1′……ガイドトラック付き基板 2……磁性膜、3……反射膜 4……ガイドトラック層、5……保護膜 6……透明接着層、7……耐熱層1 to 4 are block diagrams of examples of the magneto-optical recording medium of the present invention. 1 ... Substrate 1 '... Substrate with guide track 2 ... Magnetic film, 3 ... Reflective film 4 ... Guide track layer, 5 ... Protective film 6 ... Transparent adhesive layer, 7 ... Heat-resistant layer
───────────────────────────────────────────────────── フロントページの続き (72)発明者 田中 元治 東京都大田区中馬込1丁目3番6号 株式 会社リコー内 (72)発明者 和多田 篤行 東京都大田区中馬込1丁目3番6号 株式 会社リコー内 (72)発明者 近江 文也 東京都大田区中馬込1丁目3番6号 株式 会社リコー内 (56)参考文献 特開 昭51−119999(JP,A) 特開 昭55−55503(JP,A) 特開 昭58−145625(JP,A) 特公 昭41−547(JP,B1) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Motoharu Tanaka 1-3-6 Nakamagome, Ota-ku, Tokyo Within Ricoh Co., Ltd. (72) Inventor Atsuyuki Watada 1-3-6 Nakamagome, Ota-ku, Tokyo Stocks Within Ricoh Company (72) Inventor Fumiya Omi 1-3-6 Nakamagome, Ota-ku, Tokyo Within Ricoh Company Ltd. (56) Reference JP-A-51-119999 (JP, A) JP-A-55-55503 ( JP, A) JP 58-145625 (JP, A) JP 41-547 (JP, B1)
Claims (1)
h,V,Ga,In,Sb,Sc,Bi,Y,Sm,Eu,Tb及びGdから
なる群の少なくとも1種、0.4≦x≦1.4を表わす)で示
される金属酸化物磁性体よりなる磁性膜を有することを
特徴とする光磁気記録媒体。1. A substrate of the general formula CoM x Fe 2-x O 4 (where M is Mn, Ni, Ti, Zn, Al, Sn, Cr, Cu, Mg, R).
h, V, Ga, In, Sb, Sc, Bi, Y, Sm, Eu, Tb, and at least one of the group consisting of Gd, 0.4 ≦ x ≦ 1.4) A magneto-optical recording medium having a film.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58233907A JPH0622171B2 (en) | 1983-12-12 | 1983-12-12 | Magneto-optical recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58233907A JPH0622171B2 (en) | 1983-12-12 | 1983-12-12 | Magneto-optical recording medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60124901A JPS60124901A (en) | 1985-07-04 |
| JPH0622171B2 true JPH0622171B2 (en) | 1994-03-23 |
Family
ID=16962451
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58233907A Expired - Lifetime JPH0622171B2 (en) | 1983-12-12 | 1983-12-12 | Magneto-optical recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0622171B2 (en) |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60204691A (en) * | 1984-03-28 | 1985-10-16 | Nippon Sheet Glass Co Ltd | Production of perpendicularly magnetized co ferrite film |
| JPH0664762B2 (en) * | 1984-06-11 | 1994-08-22 | 株式会社リコー | Magneto-optical recording medium |
| JPH02165447A (en) * | 1988-12-16 | 1990-06-26 | Matsushita Electric Ind Co Ltd | Magneto-optical recording medium and its manufacturing method |
| JPH02166647A (en) * | 1988-12-20 | 1990-06-27 | Matsushita Electric Ind Co Ltd | Magneto-optical recording medium and its manufacturing method |
| US7326360B1 (en) | 2003-07-24 | 2008-02-05 | Iowa State University Research Foundation, Inc. | Cobalt ferrite based magnetostrictive materials for magnetic stress sensor and actuator applications |
| WO2005081667A2 (en) * | 2003-07-24 | 2005-09-09 | Iowa State University Research Foundation, Inc. | Cobalt ferrite based magnetostrictive materials for magnetic stress sensor and actuator applications |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS51119999A (en) * | 1976-01-24 | 1976-10-20 | Kyocera Corp | Magnetic thin film memory |
| JPS5555503A (en) * | 1978-10-18 | 1980-04-23 | Hitachi Ltd | Garnet film for magnetic bubble element |
| JPS58145625A (en) * | 1982-02-12 | 1983-08-30 | Tdk Corp | Magnetic carrier particle |
-
1983
- 1983-12-12 JP JP58233907A patent/JPH0622171B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60124901A (en) | 1985-07-04 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| EP0470546B1 (en) | Magneto-optical recording medium | |
| JPH0622171B2 (en) | Magneto-optical recording medium | |
| WO1988008192A1 (en) | Photomagnetic recording membrane | |
| JPH08180497A (en) | Reproducing method for magneto-optical recording medium and magneto-optical recording medium | |
| JPS6189607A (en) | Metal oxide magnetic materials and magnetic films | |
| JPS6189604A (en) | Metal oxide magnetic materials and magnetic films | |
| JPS60164303A (en) | Metal oxide magnetic materials and magnetic films | |
| JPS60164302A (en) | Metal oxide magnetic materials and magnetic films | |
| JPS6189605A (en) | Metal oxide magnetic materials and magnetic films | |
| JPS60211904A (en) | Metal oxide magnetic materials and magnetic films | |
| JPS60158604A (en) | Metal oxide magnetic materials and magnetic films | |
| JPH0677347B2 (en) | Information recording medium | |
| JPH0576763B2 (en) | ||
| JPS60115202A (en) | Metal oxide magnetic materials and magnetic films | |
| JPS60201603A (en) | Magnetic material and magnetic film of metal oxide | |
| JPH02206045A (en) | magneto-optical recording medium | |
| JPS60163406A (en) | Metallic oxide magnetic material and magnetic film | |
| JPS60124902A (en) | Metal oxide magnetic materials and magnetic films | |
| JPS60263357A (en) | magneto-optical recording medium | |
| JPS60120503A (en) | Metallic oxide magnetic material and magnetic film | |
| JPS60240106A (en) | Metal oxide magnetic material and magnetic film | |
| JPS60163408A (en) | Metallic oxide magnetic material and magnetic film | |
| JPS6177627A (en) | Metal oxide magnetic materials and magnetic films | |
| JPS60182108A (en) | Metal oxide magnetic materials and magnetic films | |
| JPS60163407A (en) | Metal oxide magnetic materials and magnetic films |