JPH02118935A - Magneto-optical disk - Google Patents
Magneto-optical diskInfo
- Publication number
- JPH02118935A JPH02118935A JP26829788A JP26829788A JPH02118935A JP H02118935 A JPH02118935 A JP H02118935A JP 26829788 A JP26829788 A JP 26829788A JP 26829788 A JP26829788 A JP 26829788A JP H02118935 A JPH02118935 A JP H02118935A
- Authority
- JP
- Japan
- Prior art keywords
- magneto
- optical disk
- reflectance
- layer
- tracking
- 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
- 230000000694 effects Effects 0.000 claims abstract description 16
- 238000002310 reflectometry Methods 0.000 claims abstract description 6
- 239000002223 garnet Substances 0.000 abstract description 8
- 239000000758 substrate Substances 0.000 abstract description 8
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 abstract description 7
- 229910052799 carbon Inorganic materials 0.000 abstract description 7
- 239000011521 glass Substances 0.000 abstract description 5
- 238000003486 chemical etching Methods 0.000 abstract description 2
- 239000000463 material Substances 0.000 description 8
- 239000000696 magnetic material Substances 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- VEXZGXHMUGYJMC-UHFFFAOYSA-N Hydrochloric acid Chemical compound Cl VEXZGXHMUGYJMC-UHFFFAOYSA-N 0.000 description 2
- 238000002425 crystallisation Methods 0.000 description 2
- 230000008025 crystallization Effects 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 239000011295 pitch Substances 0.000 description 2
- 229910052709 silver Inorganic materials 0.000 description 2
- 238000007740 vapor deposition Methods 0.000 description 2
- 230000005374 Kerr effect Effects 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 239000003960 organic solvent Substances 0.000 description 1
- 238000000206 photolithography Methods 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 229920000515 polycarbonate Polymers 0.000 description 1
- 239000004417 polycarbonate Substances 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
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
- G11B11/10582—Record carriers characterised by the selection of the material or by the structure or form
- G11B11/10584—Record carriers characterised by the selection of the material or by the structure or form characterised by the form, e.g. comprising mechanical protection elements
Abstract
Description
【発明の詳細な説明】
〔概 要〕
本発明は、ファラデー効果を用いる光磁気ディスクに関
し、
高密度記録に必要なトラッキングを行うことができる、
ファラデー効果を用いる光磁気ディスクを提供すること
を目的とし、
ファラデー効果を用いる光磁気ディスクにおいて、反射
膜の反射面に、必要な光磁気信号を得るのに十分な反射
率を有する高反射率領域と、トラッキングを行うのに十
分な差で上記高反射率領域の反射率よりも低い反射率を
有する低反射率領域とを、交互に同心円状またはスパイ
ラル状に形成して構成する。[Detailed Description of the Invention] [Summary] The present invention relates to a magneto-optical disk using the Faraday effect, which can perform tracking necessary for high-density recording.
The object of the present invention is to provide a magneto-optical disk using the Faraday effect, in which a high reflectance region having sufficient reflectance to obtain a necessary magneto-optical signal is provided on the reflective surface of the reflective film. and low reflectance regions having a reflectance lower than that of the high reflectance region by a sufficient difference for tracking are formed alternately in a concentric or spiral shape.
(産業上の利用分野]
本発明は、ファラデー効果を用いる光磁気ディスクに関
する。(Industrial Application Field) The present invention relates to a magneto-optical disk using the Faraday effect.
ファラデー効果を用いる光磁気ディスクは、透明な基板
(ガラス等)上にファラデー効果を有する磁性体(ガー
ネット等)の記録膜を形成し、その上に反射膜(A1等
)を形成して基本的に構成される。基板側から入射した
直線偏光は透明基板を透過し、次に記録膜を透過する際
に偏光面が記録膜の磁化の強さと厚さに比例する角度(
θ、)だけファラデー回転し、反射膜で反射して再び記
録膜中を透過する際に更に同じ角度(θf)だけ回転し
、最後に基板を透過して外部へ戻る。このように回転角
を2倍にできるので、偏光が記録膜面で反射する際に回
転するカー効果に比べて読取感度上有利なため、ファラ
デー効果を用いる光磁気ディスクは記録媒体として広範
な用途が期待されている。Magneto-optical disks that use the Faraday effect are made by forming a recording film of a magnetic material (garnet, etc.) that has a Faraday effect on a transparent substrate (glass, etc.), and then forming a reflective film (A1, etc.) on top of it. It is composed of Linearly polarized light incident from the substrate side passes through the transparent substrate, and then when it passes through the recording film, the plane of polarization changes at an angle proportional to the magnetization strength and thickness of the recording film.
The light undergoes a Faraday rotation by θ, ), is reflected by the reflective film, and when it passes through the recording film again, is further rotated by the same angle (θf), and finally passes through the substrate and returns to the outside. Since the rotation angle can be doubled in this way, it has an advantage in reading sensitivity compared to the Kerr effect, in which polarized light rotates when reflected on the recording film surface, so magneto-optical disks that use the Faraday effect have a wide range of applications as recording media. is expected.
しかし、ファラデー効果を有する磁性体は一般に結晶化
温度が高いため、高密度記録に必要なトラッキングを行
うためのガイドトラックを形成するごとができなかった
。すなわち、他の光ディスクでは、ガラス基板上のフォ
トポリマーやポリカーボネートにグループを形成してガ
イドトラックとしている。しかし、ファラデー効果を有
する磁性体では、高温結晶化によってこのグループが補
填してしまうため、この方法を適用することができず、
したがってトラッキングを必要とする高密度記録が行え
ないという問題があった。However, since magnetic materials having the Faraday effect generally have a high crystallization temperature, it has not been possible to form guide tracks for tracking required for high-density recording. That is, in other optical discs, groups are formed in photopolymer or polycarbonate on a glass substrate to serve as guide tracks. However, this method cannot be applied to magnetic materials that have the Faraday effect because this group is compensated for by high-temperature crystallization.
Therefore, there was a problem in that high-density recording requiring tracking could not be performed.
本発明は、高密度記録に必要なトラッキングを行うこと
ができる、ファラデー効果を用いる光磁気ディスクを提
供することを目的とする。An object of the present invention is to provide a magneto-optical disk using the Faraday effect that can perform the tracking required for high-density recording.
上記の目的は、本発明によれば、ファラデー効果を用い
る光磁気ディスクにおいて、反射膜の反射面に、必要な
光磁気信号を得るのに十分な反射率を有する高反射率領
域と、トラッキングを行うのに十分な差で上記高反射率
領域の反射率よりも低い反射率を有する低反射率領域と
を、交互に同心円状またはスパイラル状に形成したこと
を特徴とする光磁気ディスクによって達成される。According to the present invention, in a magneto-optical disk using the Faraday effect, the reflective surface of the reflective film has a high reflectance area having sufficient reflectance to obtain a necessary magneto-optical signal, and a tracking area. This is achieved by a magneto-optical disk characterized in that low reflectance regions having a reflectance lower than that of the high reflectance region are alternately formed in a concentric or spiral shape with a sufficient difference between the two regions. Ru.
必要な光磁気信号を得るために、従来約20%以上の反
射率の反射■々が用いられている。このような材料とし
てはAI、Ag等の金属が主として用いられている。本
発明の反射膜の高反射率領域を構成する材料は、このよ
うな従来ファラデー効果を用いる光磁気ディスクの反射
膜として用いられている材料でよい。In order to obtain the necessary magneto-optical signal, conventionally, a reflector having a reflectance of about 20% or more is used. Metals such as AI and Ag are mainly used as such materials. The material constituting the high reflectance region of the reflective film of the present invention may be a material that is conventionally used as a reflective film of such a magneto-optical disk using the Faraday effect.
低反射率領域は、高反射率領域に比べて、トラッキング
を行うのに十分な差で反射率が低いことが必′要である
。このための反射率の差は、従来、他の光ディスクでグ
ループによってトラッキングを行う場合に用いられてい
る反射率の差(グループの山の部分と谷の部分との差)
と原理的に同等である。従来のグループによる方式では
、通常10〜30%程度の反射率の差でトランキングし
ている。The low reflectance region needs to have a reflectance lower than the high reflectance region by a sufficient difference to enable tracking. The difference in reflectance for this purpose is the difference in reflectance (the difference between the peaks and valleys of the group) that is conventionally used when tracking by group on other optical discs.
is equivalent in principle. In the conventional group system, trunking is normally performed based on a difference in reflectance of about 10 to 30%.
低反射率9M域は、高反射率領域を構成する材料よりも
上記のように十分低い反射率の材料で形成することがで
きる。この場合に、高反射率領域の材料をH1低反射率
領域の材料をして表記すると、HとLの組み合わせH/
LとしてはたとえばArレーザを用いる場合Al/C、
八l/Au 、 Al/Cu 、 Ag/c 、Ag
/Cu等が用いられる。反射率の序列は用いるレーザの
波長によって決まるので、レーザ波長に応じて適宜組の
合、F)せる。The low reflectance 9M region can be formed of a material whose reflectance is sufficiently lower than that of the material forming the high reflectance region, as described above. In this case, if the material in the high reflectance region is expressed as H1, the material in the low reflectance region, the combination of H and L is H/
For example, when using an Ar laser, L may be Al/C,
8l/Au, Al/Cu, Ag/c, Ag
/Cu etc. are used. Since the order of reflectance is determined by the wavelength of the laser used, the combinations are set as appropriate depending on the laser wavelength.
高反射率領域と低反射率領域とを同一の材料で形成して
、反射面を適当な方法で同心円状またはスパイラル状に
処理して反射率が必要な差をもつよう二こすることもで
きる。It is also possible to form the high reflectance region and the low reflectance region with the same material, and process the reflective surface in a concentric or spiral shape using an appropriate method so that the reflectance has the required difference. .
〔作 用]
本発明のファラデー効果を用いる光磁気ディスクは、同
心円状またはスパイラル状に反射率の異なる領域を交互
に形成してガイドトラックとすること、によって、高、
密度記録に必要なトラッキングを行うことができる。[Function] The magneto-optical disk using the Faraday effect of the present invention has high reflectivity, by forming guide tracks by alternately forming regions with different reflectances in a concentric or spiral shape.
Tracking required for density recording can be performed.
このガイドトラックは、記録膜に従来のグループのガイ
ドトラックのような段差が存在しないため、記録膜の膜
質も向上する。Since this guide track does not have a step on the recording film unlike the guide tracks of the conventional group, the film quality of the recording film is also improved.
以下に、添付図面を参照し、実施例によって、本発明を
更に詳しく説明する。In the following, the invention will be explained in more detail by means of examples with reference to the accompanying drawings.
[実施例]
m1lF(a)〜(e)に示す工程によって、本発明に
したがったガーネット光磁気ディスクを製造した。[Example] A garnet magneto-optical disk according to the present invention was manufactured by the steps shown in m1IF(a) to (e).
厚さ1mのガラス基板1上に、スパフタリングによって
ガーネットの記録膜2(厚さ0.2 Jtm)を形成し
た(第1図(a))。この上に厚さ1如のAI層3を蒸
着によって形成した(第1図(b))。A garnet recording film 2 (thickness: 0.2 Jtm) was formed on a glass substrate 1 having a thickness of 1 m by sputtering (FIG. 1(a)). On top of this, an AI layer 3 having a thickness of 1 was formed by vapor deposition (FIG. 1(b)).
次に、AI層3上にフォトリソグラフィーによってピッ
チ2nの同心円状にレジストパターン5(厚さ100m
)を形成した(第1図(C))。この状態で塩酸による
化学エツチングを行った後、有機溶剤でレジスト5を除
去してA1層3の同心円状のパターンを得た(第1図(
d))。更に、この上に蒸着によって炭素の層4を厚さ
2卿に形成したく第1図(e))。このようにして得ら
れたガーネット光磁気ディスクは、A1の高反射率領域
(h)と炭素の低反射率61域(1)とがピッチ2趨で
交互に同心円状に反射面に形成された反射膜(3+4)
を有する。Next, a resist pattern 5 (thickness 100 m) is formed concentrically with a pitch of 2n on the AI layer 3 by photolithography.
) was formed (Fig. 1(C)). After chemical etching with hydrochloric acid in this state, the resist 5 was removed with an organic solvent to obtain a concentric pattern of the A1 layer 3 (see Fig. 1).
d)). Further, a carbon layer 4 is formed on this layer to a thickness of 2 mm by vapor deposition (FIG. 1(e)). In the thus obtained garnet magneto-optical disk, the high reflectance region (h) of A1 and the low reflectance region 61 (1) of carbon were formed alternately and concentrically at two pitches on the reflective surface. Reflective film (3+4)
has.
なお、この場合、3を炭素層、4をA(層として形成し
てもよい。In this case, 3 may be formed as a carbon layer and 4 may be formed as an A (layer).
本発明のファラデー効果を用いる光磁気ディスクは、ト
ランキングを可能としたことにより、高密度記録媒体と
して極めて有用である。The magneto-optical disk using the Faraday effect of the present invention enables trunking and is therefore extremely useful as a high-density recording medium.
第1図は本発明にしたがったガーネット光磁気ディスク
の製造工程を示す断面図である。
1・・・ガラス基板、 2・・・ガーネット記録膜、3
・・・A1層、 4・・・炭素層、5・・・レジス
ト層。FIG. 1 is a sectional view showing the manufacturing process of a garnet magneto-optical disk according to the present invention. 1... Glass substrate, 2... Garnet recording film, 3
...A1 layer, 4...carbon layer, 5...resist layer.
Claims (1)
反射膜の反射面に、必要な光磁気信号を得るのに十分な
反射率を有する高反射率領域と、トラッキングを行うの
に十分な差で上記高反射率領域の反射率よりも低い反射
率を有する低反射率領域とを、交互に同心円状またはス
パイラル状に形成したことを特徴とする光磁気ディスク
。1. In a magneto-optical disk using the Faraday effect,
On the reflective surface of the reflective film, there is a high reflectance area that has a reflectance sufficient to obtain the necessary magneto-optical signal, and a reflectance that is lower than the reflectance of the high reflectance area with a difference sufficient to perform tracking. 1. A magneto-optical disk characterized in that low reflectance areas having a low reflectivity are formed alternately in a concentric or spiral shape.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP26829788A JPH02118935A (en) | 1988-10-26 | 1988-10-26 | Magneto-optical disk |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP26829788A JPH02118935A (en) | 1988-10-26 | 1988-10-26 | Magneto-optical disk |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02118935A true JPH02118935A (en) | 1990-05-07 |
Family
ID=17456569
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP26829788A Pending JPH02118935A (en) | 1988-10-26 | 1988-10-26 | Magneto-optical disk |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02118935A (en) |
-
1988
- 1988-10-26 JP JP26829788A patent/JPH02118935A/en active Pending
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