JPH0675305B2 - Magneto-optical recording medium - Google Patents
Magneto-optical recording mediumInfo
- Publication number
- JPH0675305B2 JPH0675305B2 JP5367885A JP5367885A JPH0675305B2 JP H0675305 B2 JPH0675305 B2 JP H0675305B2 JP 5367885 A JP5367885 A JP 5367885A JP 5367885 A JP5367885 A JP 5367885A JP H0675305 B2 JPH0675305 B2 JP H0675305B2
- Authority
- JP
- Japan
- Prior art keywords
- magneto
- optical recording
- power
- recording medium
- optimum
- 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
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Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は、レーザ光を用いて情報の記録再生消去をおこ
なう光磁気記録媒体に関する。The present invention relates to a magneto-optical recording medium for recording / reproducing / erasing information by using a laser 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・高速アクセスが可
能であるということから、現在の磁気デイスクメモリに
代わる新規なメモリとして考えられている。中でも光磁
気記録媒体を用いた光磁気デイスクは書き替え性を有し
ていることから最も注目され、近年活発に研究開発がお
こなわれている。従来より知られている光磁気記録媒体
の構成は、第6図に示したように支持基板1としてガラ
スあるいは有機物樹脂を用い、支持基板1上に基板に対
して垂直方向に磁化を有する垂直磁化膜から成る光磁気
記録層3を形成したものである。光磁気記録層としては
MnBi,MnCuBi,MnTiBi,MnAlGe,PtCoなどの結晶体磁性薄
膜、あるいはGd,Tb,Dy,Hoなどの希土類とFe,Co,Niなど
の遷移金属との合金として得られるアモルフアス磁性薄
膜が知られている。(Prior Art and Its Problems) Optical disk memories are considered as a new memory to replace the current magnetic disk memories because they can be accessed with high density, large capacity and high speed. Among them, a magneto-optical disk using a magneto-optical recording medium has received the most attention because it has rewritability, and has been actively researched and developed in recent years. The configuration of a conventionally known magneto-optical recording medium is as shown in FIG. 6, in which glass or an organic resin is used as the supporting substrate 1, and the perpendicular magnetization having the magnetization in the direction perpendicular to the substrate is provided on the supporting substrate 1. The magneto-optical recording layer 3 made of a film is formed. As a magneto-optical recording layer
Known crystalline magnetic thin films such as MnBi, MnCuBi, MnTiBi, MnAlGe, and PtCo, or amorphous magnetic thin films obtained as alloys of rare earths such as Gd, Tb, Dy, and Ho with transition metals such as Fe, Co, and Ni. There is.
また、第7図に示したように、支持基板1に深さ600〜1
000Å周期1.6〜2.5μmの溝11を同心円状もしくはうず
巻き状に形成し、前記支持基板1上に光磁気記録層3を
形成した媒体構成も知られている。ここで形成されてい
る溝11は、記録媒体への情報の記録、あるいは再生・消
去に用いるレーザー集光ビームのトラツキングアクセス
に用いられるものである。In addition, as shown in FIG.
There is also known a medium structure in which a groove 11 having a 000Å period of 1.6 to 2.5 μm is formed in a concentric circle shape or a spiral shape, and the magneto-optical recording layer 3 is formed on the support substrate 1. The groove 11 formed here is used for tracking access of the laser condensed beam used for recording or reproducing / erasing information on the recording medium.
また、従来より知られている光磁気記録媒体として第8
図に示したように保護層2上の光磁気記録層3の上に反
射層4を形成し、基板側から入射したレーザ光20の光磁
気記録層3表面からの反射光21と光磁気記録層3を通り
反射層4で反射された反射光22を利用し、光磁気記録層
3の磁気光学効果を大きくしたものがある。この構成の
媒体においても第9図のように第7図と同様同心円状も
しくはうず巻き状の溝11を持つ支持基板1を用いた媒体
が知られている。しかしながら、従来より知られている
前述の光磁気記録媒体では光磁気記録層3及び反射層4
の膜厚は半径方向に対して一定となるように形成されて
いるために、等角速度で媒体を回転して情報の記録・再
生・消去をおこなう場合、半径位置に応じて記録パワ
ー、再生パワー、消去パワーを変えなければならないと
いう欠点があつた。(たとえば、川久保ら電子通信学会
技術研究報告MR84-39)この原因は、一定膜厚の媒体の
最適記録パワー、最適再生パワー、最適消去パワーが媒
体の線速度に大きく依存しているためである。In addition, as a conventionally known magneto-optical recording medium,
As shown in the figure, the reflection layer 4 is formed on the magneto-optical recording layer 3 on the protective layer 2, and the laser light 20 incident from the substrate side is reflected from the surface 21 of the magneto-optical recording layer 3 and the magneto-optical recording. There is one in which the magneto-optical effect of the magneto-optical recording layer 3 is enhanced by utilizing the reflected light 22 that has passed through the layer 3 and is reflected by the reflective layer 4. Also in the medium having this structure, as shown in FIG. 9, there is known a medium using the support substrate 1 having the concentric or spiral groove 11 as in FIG. However, in the previously known magneto-optical recording medium, the magneto-optical recording layer 3 and the reflective layer 4 are used.
Since the film thickness is constant in the radial direction, when recording / reproducing / erasing information by rotating the medium at a constant angular velocity, the recording power and the reproducing power are changed according to the radial position. However, there was a drawback that the erase power had to be changed. (For example, Kawakubo et al. IEICE Technical Report MR84-39) This is because the optimum recording power, optimum reproducing power, and optimum erasing power of a medium with a certain thickness greatly depend on the linear velocity of the medium. .
(発明の目的) 本発明の目的は、前記の従来の光磁気記録媒体の欠点を
解決し、簡単な媒体構成により、線速に依存することな
く半径方向に対して一定の最適記録パワー、最適再生パ
ワー、最適消去パワーを有し、良好な記録再生消去性能
を持つ新規な光磁気記録媒体を提供することにある。(Object of the Invention) An object of the present invention is to solve the above-mentioned drawbacks of the conventional magneto-optical recording medium and to provide a constant optimum recording power and an optimum recording power in the radial direction without depending on the linear velocity by a simple medium structure. An object of the present invention is to provide a novel magneto-optical recording medium having a reproducing power and an optimum erasing power, and having a good recording / reproducing / erasing performance.
(発明の構成) 上記目的を達成するために、本発明は、レーザ光を用い
て情報の記録再生消去をおこなう光磁気記録媒体におい
て、円板状支持基板と前記円板状支持基板上に形成され
た保護層と前記保護層上に形成された光磁気記録層と前
記光磁気記録層上に形成された反射層とを備え、前記反
射層の膜厚が光磁気記録媒体の外周ほど薄くなるように
したものである。(Structure of the Invention) In order to achieve the above object, the present invention is a magneto-optical recording medium for recording / reproducing / erasing information by using a laser beam, which is formed on a disk-shaped support substrate and the disk-shaped support substrate. Protective layer, a magneto-optical recording layer formed on the protective layer, and a reflective layer formed on the magneto-optical recording layer, and the thickness of the reflective layer becomes thinner toward the outer periphery of the magneto-optical recording medium. It was done like this.
(構成の詳細な説明) 本発明は上述の構成をとることにより、従来技術の問題
点を解決した。以下、本発明の詳細について図面を用い
て説明する。第1図は本発明にかかる光磁気記録媒体の
一例を示す断面図である。支持基板1上に保護層2が形
成され、さらに前記保護層2上に光磁気記録層3が形成
され、さらに前記光磁気記録層3上に反射層4が形成さ
れた構成である。支持基板1としてはポリメチルメタク
リレート、ポリカーボネート、エポキシなどの有機物樹
脂材料あるいはガラスが使用され、第2図のようにレー
ザビームトラツキング用の溝11があらかじめ形成された
タイプのものも使用される。保護層2としては基板側か
らの水分の浸透を防ぎ使用するレーザ波長において吸収
のないものが用いられ、たとえばSiO,SiO2,CeO2,ZrO2,T
iO2,Bi2O3,WO2,SnO2,Sb2O3,Al2O3,MgO,ThO2,La2O3,In2O
3,Nd2O3などの酸化物、AlN,Si3N4などの窒化物、ZnS,Sb
2S3,CdSなどの硫化物ThF4,MgF2,LaF3,NdF3,CeF3,PbF2な
どのフツ化物、Si,Geなどの半導体が使用される。光磁
気記録層3としてはGd,Tb,Dy,Hoなどの希土類金属と、F
e,Co,Niなどの遷移金属との合金から成るアモルフアス
磁性薄膜が用いられる。たとえば、GdCo,GdTbCo,GdTbFe
Co,TbFe,TbFeCo,TbDyFeCo,GdTbFe,GdTbDyFe,TbCo,TbDyC
o,TbFeNiなどである。反射層4としてはAl,Cu,Ti,Ag,A
u,Ptなどのメタルが用いられる。反射層4は媒体の内周
から外周に向けて膜厚を変えて作成され、外周ほど膜厚
が薄くなつている。これが、本発明にかかる光磁気記録
媒体の特徴である。(Detailed Description of Configuration) The present invention has solved the problems of the prior art by adopting the above configuration. Hereinafter, details of the present invention will be described with reference to the drawings. FIG. 1 is a sectional view showing an example of a magneto-optical recording medium according to the present invention. The protective layer 2 is formed on the supporting substrate 1, the magneto-optical recording layer 3 is further formed on the protective layer 2, and the reflective layer 4 is further formed on the magneto-optical recording layer 3. As the supporting substrate 1, an organic resin material such as polymethylmethacrylate, polycarbonate, epoxy or glass is used, and a type in which a groove 11 for laser beam tracking is formed in advance as shown in FIG. 2 is also used. As the protective layer 2, a layer that prevents water from penetrating from the substrate side and does not absorb at the laser wavelength used is used. For example, SiO, SiO 2 , CeO 2 , ZrO 2 , T
iO 2 , Bi 2 O 3 , WO 2 , SnO 2 , Sb 2 O 3 , Al 2 O 3 , MgO, ThO 2 , La 2 O 3 , In 2 O
3 , Oxides such as Nd 2 O 3 , nitrides such as AlN, Si 3 N 4 , ZnS, Sb
Sulfides such as 2 S 3 and CdS, fluorides such as ThF 4 , MgF 2 , LaF 3 , NdF 3 , CeF 3 and PbF 2, and semiconductors such as Si and Ge are used. As the magneto-optical recording layer 3, rare earth metals such as Gd, Tb, Dy and Ho, and F
Amorphous magnetic thin films made of alloys with transition metals such as e, Co and Ni are used. For example, GdCo, GdTbCo, GdTbFe
Co, TbFe, TbFeCo, TbDyFeCo, GdTbFe, GdTbDyFe, TbCo, TbDyC
o, TbFeNi, etc. Al, Cu, Ti, Ag, A as the reflective layer 4
Metals such as u and Pt are used. The reflective layer 4 is formed by changing the film thickness from the inner circumference to the outer circumference of the medium, and the film thickness decreases toward the outer circumference. This is a feature of the magneto-optical recording medium according to the present invention.
保護層2、光磁気記録層3、反射層4は真空蒸着法、ス
パツタリング法などの成膜方法により作成される。反射
層4の膜厚を外周に向けて薄くなるように形成するに
は、第3図に示したようにデイスク5の回転中心に対し
て偏心した位置に蒸着源あるいはスパツタソース6を有
する成膜装置を用いる。9は排気系、10は導入ガスであ
る。デスク5をモータ8により回転させながら成膜する
ことにより半径方向に所望の膜厚分布を持つ光磁気記録
媒体が容易に得られる。第4図(a)(b)(c)はそ
れぞれ光磁気記録媒体の最適記録パワー、最適再生パワ
ー,最適消去パワーと線速度との関係を示した図であ
る。パラメータとして第1図及び第2図の構成の媒体の
反射層4の膜厚をとつている。ここで言う最適記録パワ
ーとは、記録信号に最も忠実に記録ビツトが形成できる
記録パワーである。The protective layer 2, the magneto-optical recording layer 3, and the reflective layer 4 are formed by a film forming method such as a vacuum evaporation method and a sputtering method. In order to form the reflective layer 4 so that the film thickness becomes thinner toward the outer periphery, as shown in FIG. 3, a film forming apparatus having an evaporation source or a sputtering source 6 at a position eccentric to the rotation center of the disk 5 is formed. To use. Reference numeral 9 is an exhaust system, and 10 is an introduced gas. By forming the film while rotating the desk 5 by the motor 8, a magneto-optical recording medium having a desired film thickness distribution in the radial direction can be easily obtained. FIGS. 4 (a), (b) and (c) are diagrams showing the relationships between the optimum recording power, the optimum reproducing power, the optimum erasing power and the linear velocity of the magneto-optical recording medium. As a parameter, the film thickness of the reflective layer 4 of the medium having the configuration shown in FIGS. 1 and 2 is taken. The optimum recording power mentioned here is a recording power that can form a recording bit most faithfully to a recording signal.
また、最適再生パワーとは再生信号のC/Nすなわち再生
信号レベルと雑音信号レベルの比が最も大きくなる再生
パワーを言う。さらに最適消去パワーとは最適記録され
たビツトを完全に消去できる消去パワーを言う。最適記
録パワー、最適再生パワー、最適消去パワーはいずれも
線速が増すと高いパワー側にシフトする。また、反射層
の膜厚が厚くなると同じ線速であつても最適となる各パ
ワーは大きくなる。逆に、線速に対して最適パワーを一
定にするためには反射層の膜厚を変える必要がある。The optimum reproduction power is the reproduction power that maximizes the C / N of the reproduction signal, that is, the ratio of the reproduction signal level and the noise signal level. Furthermore, the optimum erasing power is the erasing power that can completely erase the optimum recorded bit. The optimum recording power, the optimum reproducing power, and the optimum erasing power all shift to the higher power side as the linear velocity increases. Further, as the film thickness of the reflective layer becomes thicker, each optimum power becomes larger even at the same linear velocity. On the contrary, in order to keep the optimum power constant with respect to the linear velocity, it is necessary to change the film thickness of the reflective layer.
反射層の膜厚が半径方向に一様であると、第4図からわ
かるように、最適な記録パワー、再生パワー、消去パワ
ーを半径位置に応じて変化させなければならないが、本
発明にかかる光磁気記録媒体のごとく反射層の膜厚を第
5図に示すように半径方向に変化させ、外周部ほど膜厚
が減少するように作成すると、最適パワーを半径位置に
対して一定にできる。If the thickness of the reflective layer is uniform in the radial direction, the optimum recording power, reproducing power, and erasing power must be changed according to the radial position, as can be seen from FIG. The optimum power can be made constant with respect to the radial position by changing the film thickness of the reflective layer in the radial direction as in the magneto-optical recording medium as shown in FIG. 5 so that the film thickness decreases toward the outer peripheral portion.
(実施例) 深さ700Å、幅0.8μm、ピツチ2.5μmのうず巻き状の
溝を有するポリメチルメタクリレート基板(120mm直
径、厚さ1.2mm)上にSi3N4から成る保護膜、GdTbFe膜、
Cuの反射膜を順次真空を破ることなくスパツタリング法
によりデイスクを回転しながら成膜した。Si3N4の成膜
にはSiをターゲツトとし、Ar+N2混合ガスによる反応性
スパツタリング法を採用した。膜厚は700Åとし半径方
向に均一になるようにデイスクとターゲツト間に置いた
シールド板で調節した。GdTbFe膜はGd,Tb,Feから成る複
合型ターゲツトを用いたスパツタリング法によつて作成
された。膜厚は500Å、半径方向に均一になるようにSi3
N4と同様シールド板で調節した。Cuの反射膜は半径29mm
で膜厚1500Å、半径58mmで500Åとなるようスパツタリ
ングにより成膜された。ここでデイスクはCuのスパツタ
ソースに対して偏心回転させた。(Example) A protective film made of Si 3 N 4 , a GdTbFe film, on a polymethylmethacrylate substrate (120 mm diameter, 1.2 mm thickness) having a spiral wound groove with a depth of 700 Å, a width of 0.8 μm and a pitch of 2.5 μm,
Cu reflective films were sequentially formed by rotating the disk by the sputtering method without breaking the vacuum. For the deposition of Si 3 N 4, the target was Si and the reactive sputtering method using Ar + N 2 mixed gas was adopted. The film thickness was 700Å and was adjusted with a shield plate placed between the disk and the target so that it would be uniform in the radial direction. The GdTbFe film was prepared by the sputtering method using a composite target composed of Gd, Tb, and Fe. The film thickness is 500Å, and Si 3 is made uniform in the radial direction.
It was adjusted with a shield plate like N 4 . Cu reflective film has a radius of 29 mm
The film thickness was 1500 Å and the film was sputtered to a radius of 58 mm to 500 Å. Here, the disk was eccentrically rotated with respect to the Cu sputter source.
次に、作成した光磁気記録媒体を用いて情報の記録・再
生・消去をおこなつた。媒体を毎秒30回転で回転し、記
録・再生・消去をおこなつた。半径29mmから58mmにおい
て、最適な記録パワー、再生パワー、消去パワーはそれ
ぞれ一定であり、良好な記録再生消去ができた。Next, information was recorded / reproduced / erased using the prepared magneto-optical recording medium. The medium was rotated at 30 revolutions per second to record, reproduce, and erase. The optimum recording power, reproducing power, and erasing power were constant at a radius of 29 mm to 58 mm, and good recording / reproducing / erasing could be performed.
(発明の効果) 以上、説明したように本発意によれば従来例と比較して
次のような効果がある。(Effects of the Invention) As described above, the present invention has the following effects as compared with the conventional example.
等角速度回転での使用において、光磁気記録媒体の
半径方向に対して最適記録パワー、最適再生パワー、最
適消去パワーが一定となるように媒体設計されているの
で、従来例のように半径位置に応じて各パワーを変える
必要がなく、装置構成を簡略化できる。Since the medium is designed so that the optimum recording power, optimum reproducing power, and optimum erasing power are constant in the radial direction of the magneto-optical recording medium when used at a constant angular velocity, the radial position is set to the same as in the conventional example. Accordingly, it is not necessary to change each power, and the device configuration can be simplified.
蒸着源あるいはスパツタソースの位置に対してデイ
スク回転中心を偏心させることにより、容易に半径方向
に所望の膜厚分布を持つ媒体が作成できる。By eccentricizing the disk rotation center with respect to the position of the vapor deposition source or the sputtering source, it is possible to easily create a medium having a desired film thickness distribution in the radial direction.
本発明は等角速度回転で用いる光磁気記録媒体すべ
てに適用できる。すなわち、本発明の実施例に限らず、
種々の保護層材料、光磁気記録材料、反射層材料を用い
た種々の膜構成の光磁気記録媒体に適用できる。The present invention can be applied to all magneto-optical recording media used at a constant angular velocity rotation. That is, not limited to the embodiment of the present invention,
It can be applied to magneto-optical recording media having various film structures using various protective layer materials, magneto-optical recording materials, and reflective layer materials.
第1図及び第2図は本発明の適用された光磁気記録媒体
の構成例を示す断面図、第3図は本発明にかかる光磁気
記録媒体の作成に用いる成膜装置の概略図、第4図
(a)(b)(c)は光磁気記録媒体の最適記録パワ
ー、最適再生パワー、最適消去パワーと線速度との関係
を示した図、第5図は本発明にかかる光磁気記録媒体の
反射層の半径方向の膜厚分布を示す図、第6図、第7
図、第8図及び第9図は従来の光磁気記録媒体の構成を
示す断面図である。 図中1……支持基板、2……保護層、3……光磁気記録
層、4……反射層、5……デイスク、6……蒸着源ある
いはスパツタソース、7……真空室、8……モーター、
9……排気系、10……導入ガス、11……溝、20、21、22
……レーザ光である。1 and 2 are cross-sectional views showing an example of the structure of a magneto-optical recording medium to which the present invention is applied, and FIG. 3 is a schematic view of a film forming apparatus used for producing the magneto-optical recording medium according to the present invention. 4 (a), (b) and (c) show the relationship between the optimum recording power, the optimum reproducing power, the optimum erasing power and the linear velocity of the magneto-optical recording medium, and FIG. 5 is the magneto-optical recording according to the present invention. FIG. 6, FIG. 6 and FIG. 7 showing the radial thickness distribution of the reflective layer of the medium.
FIGS. 8, 8 and 9 are sectional views showing the structure of a conventional magneto-optical recording medium. In the figure, 1 ... Support substrate, 2 ... Protective layer, 3 ... Magneto-optical recording layer, 4 ... Reflective layer, 5 ... Disk, 6 ... Deposition source or sputter source, 7 ... Vacuum chamber, 8 ... motor,
9 ... Exhaust system, 10 ... Introduced gas, 11 ... Groove, 20, 21, 22
...... It is laser light.
Claims (1)
こなう光磁気記録媒体において、円板状支持基板と前記
円板状支持基板上に形成された保護層と前記保護層上に
形成された光磁気記録層と前記光磁気記録層上に形成さ
れた反射層とを備え、前記反射層の膜厚が光磁気記録媒
体の外周ほど薄くなっていることを特徴とする光磁気記
録媒体。1. A magneto-optical recording medium in which information is recorded / reproduced / erased by using a laser beam, a disc-shaped supporting substrate, a protective layer formed on the disc-shaped supporting substrate, and a protective layer formed on the protective layer. A magneto-optical recording medium comprising a magneto-optical recording layer and a reflective layer formed on the magneto-optical recording layer, wherein the thickness of the reflective layer is thinner toward the outer periphery of the magneto-optical recording medium.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5367885A JPH0675305B2 (en) | 1985-03-18 | 1985-03-18 | Magneto-optical recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5367885A JPH0675305B2 (en) | 1985-03-18 | 1985-03-18 | Magneto-optical recording medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61211852A JPS61211852A (en) | 1986-09-19 |
| JPH0675305B2 true JPH0675305B2 (en) | 1994-09-21 |
Family
ID=12949477
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5367885A Expired - Lifetime JPH0675305B2 (en) | 1985-03-18 | 1985-03-18 | Magneto-optical recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0675305B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2806274B2 (en) * | 1994-10-19 | 1998-09-30 | 日本電気株式会社 | Optical information recording medium |
-
1985
- 1985-03-18 JP JP5367885A patent/JPH0675305B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61211852A (en) | 1986-09-19 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |