JPS626450A - Photomagnetic disk - Google Patents
Photomagnetic diskInfo
- Publication number
- JPS626450A JPS626450A JP14509785A JP14509785A JPS626450A JP S626450 A JPS626450 A JP S626450A JP 14509785 A JP14509785 A JP 14509785A JP 14509785 A JP14509785 A JP 14509785A JP S626450 A JPS626450 A JP S626450A
- Authority
- JP
- Japan
- Prior art keywords
- film
- peripheral part
- recording
- magneto
- light
- 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
Abstract
Description
【発明の詳細な説明】
〔概要〕
回転する際の線速か異なる光磁気ディスクの内周部と外
周部とで同一のパワーで記録と消去とを行う方法として
、内周部より外周部に向かって膜厚が変化している光吸
収膜を備えた光磁気ディスク。[Detailed Description of the Invention] [Summary] As a method for recording and erasing with the same power on the inner and outer circumferential parts of a magneto-optical disk, which rotate at different linear velocities, the method uses A magneto-optical disk with a light-absorbing film whose thickness changes toward the other direction.
本発明はディスク全域にわたって均一なレーザパワーで
記録と消去を可能とする光磁気ディスクの構成に関する
。The present invention relates to a structure of a magneto-optical disk that enables recording and erasing with uniform laser power over the entire area of the disk.
光磁気ディスクはレーザ光を用いて高密度の情報記録を
行うメモリであり、光ディスクと同様に記録容量が大き
く、非接触で記録と再生を行うことができ、また塵埃の
影響を受けないなど優れた特徴をもつメモリである。A magneto-optical disk is a memory that uses laser light to record high-density information. Like an optical disk, it has a large storage capacity, can perform contactless recording and playback, and is unaffected by dust. It is a memory with unique characteristics.
すなわちレーザ光はレンズによって直径が1μm以下の
小さなスポットに絞り込むことが可能であり、従って1
ビツトの情報記録に要する面積が1μm2程度で足りる
。In other words, the laser beam can be narrowed down to a small spot with a diameter of 1 μm or less using a lens.
The area required for recording bit information is only about 1 μm2.
そのため磁気ディスク或いは磁気テープが1ビツトの情
報記録に数10〜数100μm2の面積が必要なのと較
べて溝かに少なくて済み、従って大容量記録が可能であ
る。Therefore, compared to the magnetic disk or magnetic tape, which requires an area of several tens to hundreds of micrometers to record one bit of information, only a few grooves are required, and therefore large-capacity recording is possible.
またレンズで絞り込む際に光磁気ディスクの基板面では
ビーム径は約1fl程度の広さになるので、基板面に大
きさが数10μII+2の塵埃が存在していても記録・
再生に殆ど影響を与えずに済ませることができる。In addition, when narrowing down with a lens, the beam diameter becomes about 1 fl on the substrate surface of the magneto-optical disk, so even if there is dust with a size of several tens of μII+2 on the substrate surface, recording and
This can be done with almost no effect on playback.
このように光源としてレーザ光を用いる光磁気ディスク
及び光ディスクは優れた特性を備えているが、この両者
を比較すると、光ディスクは記録媒体として低融点金属
を用い、情報の記録と再生を穴(ビット)の有無により
行う読出し専用メモリ(Read 0nly Memo
ry)が主であり、既に実用化されている。Magneto-optical disks and optical disks that use laser light as a light source have excellent properties, but when comparing the two, optical disks use a low-melting point metal as a recording medium, and information is recorded and reproduced using holes (bits). ) Read only memory (Read 0nly Memo)
ry) is the main one and has already been put into practical use.
一方、光磁気ディスクは書替え可能なメモリ(!!ra
sabl(Memory)として開発が進められている
もので、レーザ照射された磁化膜の温度上昇による磁化
反転が情報の記録と消去に用いられ、磁化膜からの反射
光或いは透過光の偏光面の回転が光続出しに使用されて
いる。On the other hand, magneto-optical disks are rewritable memory (!!ra
It is being developed as SABL (Memory), and magnetization reversal due to temperature rise of a magnetized film irradiated with a laser is used to record and erase information, and rotation of the polarization plane of reflected or transmitted light from the magnetized film is used. is used to produce a series of lights.
ここで磁化膜として垂直磁化膜が用いられているが、こ
れは1とOの記録ビーノドが隣接するときに垂直磁化膜
がより安定で高密度記録が可能なためである。Here, a perpendicular magnetization film is used as the magnetization film because the perpendicular magnetization film is more stable and enables high-density recording when the recording nodes of 1 and O are adjacent to each other.
光磁気ディスクは先に記したように1μm以下の直径に
まで絞・ったレーザ光を記録媒体である垂直磁化膜に投
射し、照射部が部分的に加熱されてキュリ一温度の近傍
或いはこれ以上の温度にまで上昇するのを利用して記録
や消去を行うものである。As mentioned earlier, a magneto-optical disk projects a laser beam focused to a diameter of 1 μm or less onto a perpendicularly magnetized film, which is a recording medium, and the irradiated area is partially heated to a temperature near or below the Curie temperature. Recording and erasing is performed by utilizing the temperature rising to the above temperature.
ここでディスクの回転数を一定とすると光磁気ディスク
の外周部と内周部とでは線速か異なるために同一のレー
ザパワーで照射を行っても被照射部の温度が異なると云
う問題がある。Here, if the rotational speed of the disk is constant, there is a problem that the temperature of the irradiated area will differ even if irradiated with the same laser power because the linear velocity is different between the outer and inner periphery of the magneto-optical disk. .
すなわち内周から外周に行くに従って線速か大きくなる
ので温度上昇が小さくなる。That is, as the linear velocity increases from the inner circumference to the outer circumference, the temperature rise becomes smaller.
従ってレーザパワーを一定とし、また回転数を一定とし
た状態で記録と消去を行うには工夫が必要である。Therefore, it is necessary to devise ways to perform recording and erasing while keeping the laser power constant and the rotational speed constant.
然し、光磁気ディスクの実用化が行われていない現在、
未だ明確な処理方法は決まっておらず、実験的には情報
の記録或いは消去位置により連続的にレーザパワーを変
化させる方法が採られている。However, at present, magneto-optical disks have not been put into practical use.
A clear processing method has not yet been determined, and experimentally a method has been adopted in which the laser power is continuously varied depending on the position where information is recorded or erased.
以上記したように光磁気ディスクはディスク基板の回転
中に内周部と外周部とでは線速か異なるためにディスク
基板の回転速度を一定とし、またレーザパワーを一定に
保持する場合に線速とどのようにして調和させるかが問
題である。As mentioned above, in a magneto-optical disk, the linear velocity differs between the inner and outer peripheries during rotation of the disk substrate, so when the rotational speed of the disk substrate is kept constant and the laser power is kept constant, The problem is how to harmonize it.
上記の問題は透明基板上に垂直磁化膜を形成し、該垂直
磁化膜にレーザビームを照射して情報の記録と再生およ
び消去を行う光磁気ディスクにおいて、該透明基板と垂
直磁化膜との間に光吸収膜を設け、該吸収膜の膜厚を内
周部より外周部に向かって変化させたことを特徴とする
光磁気ディスクにより解決することができる。The above problem occurs in magneto-optical disks in which a perpendicularly magnetized film is formed on a transparent substrate, and the perpendicularly magnetized film is irradiated with a laser beam to record, reproduce, and erase information. This problem can be solved by a magneto-optical disk characterized in that a light absorbing film is provided on the periphery, and the thickness of the absorbing film is changed from the inner periphery toward the outer periphery.
光磁気ディスクへの情報の記録と消去は垂直磁化膜に磁
場を加えた状態でレーザ照射してキュリ一温度にまで加
熱し、垂直磁化膜の磁化を磁場の方向に変えることによ
り行うものであるが、その際に垂直磁化膜の温度上昇は
レーザの照射強度を一定に保つ場合は照射時間に比例し
ている。Information is recorded and erased on a magneto-optical disk by irradiating a perpendicularly magnetized film with a laser while applying a magnetic field, heating it to a Curie temperature, and changing the magnetization of the perpendicularly magnetized film in the direction of the magnetic field. However, in this case, the temperature rise of the perpendicularly magnetized film is proportional to the irradiation time when the laser irradiation intensity is kept constant.
そのため内周部より外周部へ行くに従って単位面積当た
りの照射時間が少なく、従って垂直磁化膜の温度上昇が
低下するのを補償する方法として本発明は垂直磁化膜の
下に光吸収膜を設け、この膜厚を調節して内周部では光
吸収が少なく、外周部へ行くに従って光吸収が大きくな
るように形成することにより垂直磁化膜の温度上昇を線
速にマツチさせて一定値に保持させるものである。Therefore, the irradiation time per unit area decreases as you go from the inner circumference to the outer circumference.Therefore, as a method of compensating for the decrease in the temperature rise of the perpendicularly magnetized film, the present invention provides a light absorbing film under the perpendicularly magnetized film. By adjusting the thickness of this film so that light absorption is small in the inner circumference and increases toward the outer circumference, the temperature rise of the perpendicularly magnetized film can be matched to the linear velocity and maintained at a constant value. It is something.
すなわち成る平面に接して屈折率がnlなる薄膜を設け
、これに屈折率がn2なる媒質を通して光を入射させる
と、平面と薄膜との界面での反射光と薄膜と媒質との界
面での反射光とが干渉するが、この場合に光の吸収が最
大となる条件はn + t =1/4(2N+1) n
2 λ ・・・・・・(1)また光の吸収が最小とな
る条件は
n 2 t =1/4 ・2 N nz λ ・・
・・(2)但し Lは薄膜の厚さ
Nは正の整数
の関係がある。In other words, if a thin film with a refractive index of nl is provided in contact with a plane, and light is incident on it through a medium with a refractive index of n2, the light will be reflected at the interface between the plane and the thin film, and the light will be reflected at the interface between the thin film and the medium. In this case, the condition for maximum absorption of light is n + t = 1/4 (2N + 1) n
2 λ (1) The condition for minimizing light absorption is n 2 t = 1/4 ・2 N nz λ .
...(2) However, there is a relationship between L and the thickness of the thin film N, which are positive integers.
そこで本発明はレーザ光の照射線速に対応させて内周部
から外周部に行くに従って光吸収が大きくなるようにす
るものである。Therefore, the present invention is designed to increase light absorption from the inner circumferential portion to the outer circumferential portion in accordance with the irradiation linear velocity of the laser beam.
第1図は本発明を実施した光磁気ディスクの断面図で、
ポリメチル・メタクリエイト(PMMA)からなる透明
基板1の上に屈折率が2.4の硫化亜鉛(Zn S )
からなる光吸収膜2を設け、この上に例えば屈折率が3
.0のテルビウム・鉄・コバルト(Tb Fe Co)
垂直磁化膜3が設けられているが、光吸収M2は内周部
より外周部に互って厚さを変えて形成されている。FIG. 1 is a cross-sectional view of a magneto-optical disk embodying the present invention.
Zinc sulfide (ZnS) with a refractive index of 2.4 is placed on a transparent substrate 1 made of polymethyl methacrylate (PMMA).
A light absorbing film 2 consisting of
.. 0 terbium-iron-cobalt (Tb Fe Co)
A perpendicular magnetization film 3 is provided, and the light absorbing layer M2 is formed with a different thickness from the inner circumferential portion to the outer circumferential portion.
またこの垂直磁化膜3の上には更に酸化硅素(Sin)
などからなる保護膜4が設けられている。Moreover, silicon oxide (Sin) is further formed on this perpendicular magnetization film 3.
A protective film 4 made of, for example, is provided.
かかる透明基板1は図に示すように垂直磁化膜2の形成
部を内側とし、内周部と外周部にプラスチック或いは金
属からなるスペーサリング5を置き、上からPMMAな
どのディスク基板を張り合わせて光磁気ディスクが形成
される。As shown in the figure, such a transparent substrate 1 has the part where the perpendicularly magnetized film 2 is formed on the inside, spacer rings 5 made of plastic or metal are placed on the inner and outer peripheries, and a disk substrate such as PMMA is laminated from above. A magnetic disk is formed.
ここで本発明に使用しているZn Sからなる光吸収膜
は波長が830n+++のレーザ光に対して第2図に示
すような光吸収特性をもっている。The light absorption film made of ZnS used in the present invention has light absorption characteristics as shown in FIG. 2 for laser light having a wavelength of 830n++.
すなわちPMMAO上に厚さを変えてZn S膜を作り
、これについてPMMAを通してレーザを照射して光吸
収特性を調べたもので、光吸収量の目安として反射率の
逆数をとっである。That is, ZnS films with varying thicknesses were formed on PMMAO, and the light absorption characteristics of the films were investigated by irradiating a laser through the PMMA, and the reciprocal of the reflectance was used as a measure of the amount of light absorption.
すなわち膜厚が800人付近と1800人付近に吸収の
最大があるが、実施例の場合は前者の条件を使用し内周
部を310人にまた外周部が430人になるようにZn
Sの膜厚を調節した。In other words, the maximum absorption occurs when the film thickness is around 800 mm and around 1800 mm, but in the case of the example, using the former condition, Zn was
The film thickness of S was adjusted.
ここで膜厚の調節法としては真空蒸着法でディスク基板
上にZn Sを形成する場合に第3図に示すような開口
部6をもつマスク7を用い、これを蒸発源と被蒸着基板
との間に介在させ、被蒸着基板(この場合透明基板1)
を回転させて蒸着することにより形成した。Here, as a method for adjusting the film thickness, when forming ZnS on a disk substrate by vacuum evaporation, a mask 7 having an opening 6 as shown in FIG. The substrate to be deposited (transparent substrate 1 in this case)
It was formed by rotating and vapor depositing.
次にこのようにして形成したZn S光吸収膜2の上に
二部蒸着法によりTeとFe、Coを蒸着して厚さ約1
000人のTe Fe Coからなる垂直磁化膜3を形
成し、更にその上に厚さ約1000人のSiO保護膜4
を形成し、以下は従来の方法で外装を行い光磁気ディス
クをを形成した。Next, on the ZnS light absorption film 2 formed in this way, Te, Fe, and Co are deposited by a two-part deposition method to a thickness of approximately 1.
A perpendicularly magnetized film 3 made of Te Fe Co with a thickness of about 1,000 yen is formed thereon, and an SiO protective film 4 with a thickness of about 1,000 yen is further formed thereon.
A magneto-optical disk was then formed using a conventional method for packaging.
そして2m−のレーザパワーで情報の記録を行ったが均
一な条件で記録が行われており、読出し強度に差は認め
られなかった。Information was then recorded with a laser power of 2 m<->, but the recording was performed under uniform conditions, and no difference was observed in the readout intensity.
以上記したように本発明は厚さを調節した光吸収膜を設
けることにより、光磁気ディスク基板の内周部と外周部
とで線速が異なるにも拘わらず、同一のレーザパワーで
記録あるいは消去を可能とするもので、本発明の実施に
より光磁気ディスクの動作機構を簡単化することができ
る。As described above, by providing a light absorption film with an adjusted thickness, the present invention enables recording or recording with the same laser power even though the linear velocity differs between the inner and outer circumferential parts of the magneto-optical disk substrate. The operation mechanism of the magneto-optical disk can be simplified by implementing the present invention.
第1図は本発明を実施した光磁気ディスクの断面図・
第2図は光吸収膜の吸収特性、
第3図は蒸着マスクの平面図、
である。
図において、
1は透明基板、 2は光吸収膜、3は垂直磁化
膜、 6は開口部、7はマスク、
である。FIG. 1 is a cross-sectional view of a magneto-optical disk embodying the present invention, FIG. 2 is a diagram showing the absorption characteristics of a light-absorbing film, and FIG. 3 is a plan view of a vapor deposition mask. In the figure, 1 is a transparent substrate, 2 is a light absorption film, 3 is a perpendicular magnetization film, 6 is an opening, and 7 is a mask.
Claims (1)
磁化膜(3)にレーザビームを照射して情報の記録と再
生および消去を行う光磁気ディスクにおいて、該透明基
板(1)と垂直磁化膜(3)との間に光吸収膜(2)を
設け、該光吸収膜(2)の膜厚を内周部より外周部に向
かって変化させたことを特徴とする光磁気ディスク。In a magneto-optical disk, a perpendicularly magnetized film (3) is formed on a transparent substrate (1), and information is recorded, reproduced, and erased by irradiating the perpendicularly magnetized film (3) with a laser beam. ) and a perpendicularly magnetized film (3), a light absorption film (2) is provided between the light absorption film (2) and the thickness of the light absorption film (2) is changed from the inner circumference toward the outer circumference. magnetic disk.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14509785A JPS626450A (en) | 1985-07-02 | 1985-07-02 | Photomagnetic disk |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14509785A JPS626450A (en) | 1985-07-02 | 1985-07-02 | Photomagnetic disk |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS626450A true JPS626450A (en) | 1987-01-13 |
Family
ID=15377301
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14509785A Pending JPS626450A (en) | 1985-07-02 | 1985-07-02 | Photomagnetic disk |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS626450A (en) |
-
1985
- 1985-07-02 JP JP14509785A patent/JPS626450A/en active Pending
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