JPH0628724A - Magneto-optical recording medium - Google Patents

Magneto-optical recording medium

Info

Publication number
JPH0628724A
JPH0628724A JP4207290A JP20729092A JPH0628724A JP H0628724 A JPH0628724 A JP H0628724A JP 4207290 A JP4207290 A JP 4207290A JP 20729092 A JP20729092 A JP 20729092A JP H0628724 A JPH0628724 A JP H0628724A
Authority
JP
Japan
Prior art keywords
magneto
optical recording
recording medium
peripheral side
layer
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
Application number
JP4207290A
Other languages
Japanese (ja)
Inventor
Hiroyuki Okamoto
弘之 岡本
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Ricoh Co Ltd
Original Assignee
Ricoh Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP4207290A priority Critical patent/JPH0628724A/en
Publication of JPH0628724A publication Critical patent/JPH0628724A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To provide the magneto-optical recording medium which has excellent reliability and sensitivity and is less changed in the laser output necessary for recording from the inner peripheral part to the outer peripheral part by changing the film thickness of a first dielectric layer and the Al compsn. of an Al alloy reflection layer in a diametral direction. CONSTITUTION:This magneto-optical recording medium is constituted by laminating the first dielectric protective layer 2, a magneto-optical recording layer 3, the second dielectric protective layer 4, the Al alloy reflection layer 5a and a UV curing resin layer 6 in this order on a transparent disk substrate 1. The ratio of the At compsn. of the Al alloy reflection layer 5a is lower the nearer the outer periphery of the diameter of the recording medium. In addition, the film thickness of the first dielectric protective layer 2a changes likewise in the same diametral direction and the outer peripheral side is thinner than the inner peripheral side. The first dielectric protective layer 2a acts a heat reservoir in the case where the heat of the magneto-optical recording layer 3 diffuses. The magneto-optical recording layer 3 is more easily deprived of heat as the film thickness of this layer is larger. In addition, the thermal efficiency by the irradiation with the laser on the peripheral side is made better than on the inner peripheral side. The thermal efficiency of the Al alloy reflection layer is improved as well by increasing the ratio of the Ti compsn. on the outer peripheral side.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明はレーザー光を用いて情報
の記録、再生、消去を行なう光磁気記録媒体に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magneto-optical recording medium for recording, reproducing and erasing information by using laser light.

【0002】[0002]

【従来の技術】光磁気記録方式においては、光磁気記録
装置を簡単にするために光磁気ディスクを一定の回転数
で回転させながら用いる、いわゆるCAV方式が広く用
いられている。光磁気ディスクに記録を行うには記録を
行う部分を一定温度以上に加熱する必要があるが、CA
V方式においてはレーザー照射部におけるディスクの線
速度が内周より外周側の方が速くなり、熱効率が低下す
る。このためディスク全面に渡りレーザー照射部の温度
を均一化するためには、外周になるに従いより強いレー
ザー出力が必要となる。
2. Description of the Related Art As a magneto-optical recording method, a so-called CAV method is widely used in which a magneto-optical disk is used while rotating at a constant rotational speed in order to simplify a magneto-optical recording apparatus. In order to record on a magneto-optical disk, it is necessary to heat the part to be recorded above a certain temperature.
In the V method, the linear velocity of the disk in the laser irradiation portion is higher on the outer peripheral side than on the inner peripheral side, and the thermal efficiency is reduced. Therefore, in order to make the temperature of the laser irradiation portion uniform over the entire surface of the disk, a stronger laser output is required toward the outer circumference.

【0003】しかしながらCAV方式で光磁気ディスク
を駆動する場合、記録レーザー出力を内周から外周側に
向って段階的に大きくすることは半導体レーザーのパワ
ーマージンを大きくする必要があり、又、出力制御回路
等を複雑にし、ドライブ側にとって負担となっている。
However, when the magneto-optical disk is driven by the CAV method, it is necessary to increase the power margin of the semiconductor laser and increase the output control in order to increase the recording laser output stepwise from the inner circumference toward the outer circumference. It complicates the circuit, etc. and is a burden on the drive side.

【0004】特開昭57−152555号公報では、T
bFeの組成を内周から外周側に連続的に変化させた光
磁気記録層によりキュリー点を内周から外周側に連続的
に小さくなるようにしている。キュリー点を変えること
で、記録ビットのコントラストの均一化を図っている。
しかしディスクの内外周で記録層の組成を制御すること
は成膜技術的に複雑であり、特にスループット、歩留ま
りの点で優れたスパッタ法では困難である。
In Japanese Patent Application Laid-Open No. 57-152555, T
The Curie point is continuously reduced from the inner circumference to the outer circumference by the magneto-optical recording layer in which the composition of bFe is continuously changed from the inner circumference to the outer circumference. By changing the Curie point, the contrast of recorded bits is made uniform.
However, controlling the composition of the recording layer on the inner and outer peripheries of the disk is complicated in terms of film-forming technology, and it is particularly difficult for the sputtering method, which is excellent in terms of throughput and yield.

【0005】特開昭61−211852号公報では、支
持基板、保護層、光磁気記録層、反射層の構成の光磁気
記録媒体において反射層の膜厚を径方向に変化させてい
る。しかし、この構成では反射層が光磁気記録層に密着
しているために熱拡散率が大きく、第2誘電体保護層が
ある場合に比ベて、記録に必要なレーザー出力が大きく
なりパワーマージンの点で好ましくない。又、熱拡散率
の勾配を径方向に設定するのに大きな膜厚の変化を必要
とする。このことはディスクの信頼性を低下させるなど
の一因となる。
In Japanese Patent Laid-Open No. 61-211852, in a magneto-optical recording medium having a supporting substrate, a protective layer, a magneto-optical recording layer and a reflecting layer, the thickness of the reflecting layer is changed in the radial direction. However, in this structure, since the reflective layer is in close contact with the magneto-optical recording layer, the thermal diffusivity is large, and the laser output required for recording is large compared with the case where the second dielectric protective layer is provided, and the power margin is increased. Is not preferable. Further, a large change in film thickness is required to set the thermal diffusivity gradient in the radial direction. This is one of the causes of lowering the reliability of the disc.

【0006】特開平3−69039号公報では、透明な
円板状基板、誘電体、熱拡散膜、保護膜の構成の光磁気
記録媒体において熱拡散膜の膜厚を基板の中心部から外
周部にかけて連続的もしくは段階的に薄くしている。こ
の場合も特開昭61−211852号公報と同じ理由で
好ましくない。
In Japanese Patent Laid-Open No. 3-69039, in a magneto-optical recording medium having a transparent disk-shaped substrate, a dielectric, a heat diffusion film, and a protective film, the thickness of the heat diffusion film is changed from the central portion to the outer peripheral portion of the substrate. It is continuously or stepwise thinned over time. This case is also not preferable for the same reason as in JP-A-61-211852.

【0007】[0007]

【発明が解決しようとする課題】本発明の目的は、信頼
性及び感度に優れるとともに内周から外周部にかけての
記録に必要なレーザー出力の変化の少ない光磁気記録媒
体を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a magneto-optical recording medium which is excellent in reliability and sensitivity and has a small change in laser output required for recording from the inner circumference to the outer circumference.

【0008】[0008]

【課題を解決するための手段】上記本発明の目的は、透
明な円盤基板上に第1誘電体保護層、光磁気記録層、第
2誘電体保護層、Al合金反射層及び紫外線硬化型樹脂
層がこの順で積層された光磁気記録媒体の各層のうち第
1誘電体保護層、Al合金反射層、第2誘電体保護層、
光磁気記録層の膜厚を記録媒体の径方向に連続的あるい
は段階的に変化させることで、あるいは更にAl合金反
射層のAl組成を径方向に変化させることで達成され
る。
The above object of the present invention is to provide a first dielectric protective layer, a magneto-optical recording layer, a second dielectric protective layer, an Al alloy reflective layer and an ultraviolet curable resin on a transparent disk substrate. A first dielectric protective layer, an Al alloy reflective layer, a second dielectric protective layer among the layers of the magneto-optical recording medium in which the layers are laminated in this order,
This is achieved by continuously or stepwise changing the film thickness of the magneto-optical recording layer in the radial direction of the recording medium, or by further changing the Al composition of the Al alloy reflective layer in the radial direction.

【0009】即ち、Al合金反射層のAl組成が径方向
に変化し、Al組成の割合が径の外周ほど低くなり、か
つ第1誘電体保護層の膜厚が記録媒体の径方向に変化
し、その際外周側における膜厚が内周側よりも薄いこと
を特微とする光磁気記録媒体である。
That is, the Al composition of the Al alloy reflective layer changes in the radial direction, the proportion of the Al composition decreases toward the outer periphery of the diameter, and the film thickness of the first dielectric protective layer changes in the radial direction of the recording medium. In this case, the magneto-optical recording medium is characterized in that the film thickness on the outer peripheral side is thinner than that on the inner peripheral side.

【0010】又、第1誘電体保護層の膜厚が記録媒体の
径方向に変化し、その際外周側における膜厚が内周側よ
りも薄く、かつAl合金反射層の膜厚が記録媒体の径方
向に変化し、その際外周側における膜厚が内周側よりも
薄い光磁気記録媒体である。
Further, the film thickness of the first dielectric protective layer changes in the radial direction of the recording medium, in which case the film thickness on the outer peripheral side is thinner than that on the inner peripheral side and the film thickness of the Al alloy reflective layer is the recording medium. Of the magneto-optical recording medium in which the film thickness on the outer peripheral side is thinner than that on the inner peripheral side.

【0011】更に又、第1誘電体保護層の膜厚が記録媒
体の径方向に変化し、その際外周側における膜厚が内周
側よりも薄く、かつ第2誘電体保護層の膜厚が記録媒体
の径方向に変化し、その際外周側における膜厚が内周側
よりも厚い光磁気記録媒体である。
Furthermore, the film thickness of the first dielectric protective layer changes in the radial direction of the recording medium, the film thickness on the outer peripheral side is smaller than that on the inner peripheral side, and the film thickness of the second dielectric protective layer. Changes in the radial direction of the recording medium, and at that time, the film thickness on the outer peripheral side is thicker than that on the inner peripheral side.

【0012】又、第1誘電体保護層の膜厚が記録媒体の
径方向に変化し、その際外周側における膜厚が内周側よ
りも薄く、かつ光磁気記録層の膜厚が記録媒体の径方向
に変化し、その際外周側における膜厚が内周側よりも薄
い光磁気記録媒体である。
Further, the film thickness of the first dielectric protective layer changes in the radial direction of the recording medium, the film thickness on the outer peripheral side is smaller than that on the inner peripheral side, and the film thickness of the magneto-optical recording layer is smaller than that of the recording medium. Of the magneto-optical recording medium in which the film thickness on the outer peripheral side is thinner than that on the inner peripheral side.

【0013】以下、図面に基づいて本発明を説明する。
比較の便宜上、従来の光磁気記録媒体から述べる。
The present invention will be described below with reference to the drawings.
For convenience of comparison, the conventional magneto-optical recording medium will be described first.

【0014】図1は従来の光磁気記録媒体を示し、透明
な円盤基板1の上に第1誘電体保護層2、光磁気記録層
3、第2誘電体保護層4、Al合金反射層5及び紫外線
硬化型樹脂層6がこの順で積層されている。光磁気ディ
スクが1800回転/分で回転しているとき、半径24
mmでの線速度は4.5m/s、半径39.5mmでの線
速度は7.4m/sと異なるため、同一のレーザー出力
で記録媒体を加熱すると、外周になるほど単位面積当り
の受け取るエネルギーは小さくなり、ディスク全面にお
いて照射部を均一の温度に加熱するには外周側程レーザ
ー出力を強くする必要がある。つまりCAV方式では、
内周より外周側の方が記録に要するレーザー出力は高く
する必要がある。記録レーザーの出力が適正の時、適正
な記録ビットが光磁気記録層に形成されるが、適正以上
のレーザー出力をかけた場合は記録ビットが大きくなり
すぎCNR(Carrier to Noise Ratio)が低下する。ま
た適正以下のレーザー出力の場合もCNRは低下する。
FIG. 1 shows a conventional magneto-optical recording medium, in which a first dielectric protective layer 2, a magneto-optical recording layer 3, a second dielectric protective layer 4 and an Al alloy reflective layer 5 are provided on a transparent disk substrate 1. And the ultraviolet curable resin layer 6 are laminated in this order. When the magneto-optical disk is rotating at 1800 rpm, the radius is 24
Since the linear velocity in mm is 4.5 m / s and the linear velocity in a radius of 39.5 mm is 7.4 m / s, when the recording medium is heated with the same laser output, the energy received per unit area becomes closer to the outer circumference. Becomes smaller, and it is necessary to increase the laser output toward the outer peripheral side in order to heat the irradiation part to a uniform temperature over the entire surface of the disk. That is, in the CAV method,
It is necessary to increase the laser output required for recording on the outer circumference side than the inner circumference side. When the output of the recording laser is appropriate, an appropriate recording bit is formed in the magneto-optical recording layer, but when the laser output above the appropriate level is applied, the recording bit becomes too large and the CNR (Carrier to Noise Ratio) decreases. . The CNR is also reduced when the laser output is below the proper level.

【0015】図1の従来の場合、直径86mmのポリカ
ーボネート基板1上に第1誘電体保護層2としてシリコ
ン窒化膜を900Å、光磁気記録層3としてDy15T
b7Fe70Co8を200Å第2誘電体保護層4とし
てシリコン窒化膜を300Å、Al合金反射膜5として
アルミニウム・チタン合金を500Å、紫外線硬化型樹
脂1μmを積層した場合の光磁気ディスクのCNRの記
録レーザー出力依存性を図6に示す。半径24.1mm
と半径39.5mmでのCNRの不均一性が顕著にみら
れる。
In the conventional case of FIG. 1, a silicon nitride film as a first dielectric protection layer 2 is 900Å and a magneto-optical recording layer 3 is Dy15T on a polycarbonate substrate 1 having a diameter of 86 mm.
b7Fe70Co8 is 200 Å The second dielectric protection layer 4 is a silicon nitride film 300 Å, the Al alloy reflection film 5 is an aluminum / titanium alloy 500 Å, and the UV curable resin 1 μm is laminated. The sex is shown in FIG. Radius 24.1mm
And the non-uniformity of CNR at a radius of 39.5 mm is noticeable.

【0016】図2は本発明の光磁気記録媒体の実施例を
示すもので、第1誘電体保護層2aは屈折率2.15の
シリコン窒化膜を半径24mmで1000Å、半径3
9.5mmで900Åになるように成膜したものであ
る。又、Al合金反射層5aのAl組成は最内周に当た
るところで95%、最外周に当たるところで90%にな
るようにAl組成を連続的あるいは段階的に変化させて
いる。Alに添加する元素としてはTiを用いている。
他の各層の条件は図1の場合と同じである。
FIG. 2 shows an embodiment of the magneto-optical recording medium of the present invention. The first dielectric protective layer 2a is a silicon nitride film having a refractive index of 2.15, a radius of 24 mm, a length of 1000 Å, and a radius of 3.
The film was formed to have a thickness of 900 Å at 9.5 mm. Further, the Al composition of the Al alloy reflection layer 5a is changed continuously or stepwise so that the Al composition reaches 95% at the innermost circumference and 90% at the outermost circumference. Ti is used as an element added to Al.
The conditions for the other layers are the same as in FIG.

【0017】第1誘電体保護層はレーザーによって加熱
された光磁気記録層3の熱が拡散する場合の熱溜の働き
をし、第1誘電体保護層の膜厚が厚くなるほど光磁気記
録層から熱が奪われ易くなる。このため内周側に比ベ外
周側でのレーザー照射による熱効率が改善される。ま
た、Ti組成の割合の高いAl合金ほど熱伝導率が低く
なるため、外周側ほど熱が逃げにくく、熱効率が改善さ
れる。
The first dielectric protective layer acts as a heat reservoir when the heat of the magneto-optical recording layer 3 heated by the laser diffuses, and the thicker the first dielectric protective layer is, the magneto-optical recording layer. It becomes easy to take away heat from. For this reason, the thermal efficiency of the laser irradiation on the outer peripheral side relative to the inner peripheral side is improved. Further, since the Al alloy having a higher proportion of Ti has a lower thermal conductivity, the heat is less likely to escape toward the outer peripheral side, and the thermal efficiency is improved.

【0018】この構成での光磁気ディスクのCNRの記
録レーザー出力依存性を図7に示す。内周(半径24.
2mm)と外周(39.5mm)でのCNRの均一性が
改善されている。従ってディスクの内周と外周でレーザ
ー出力を変える必要がない。
FIG. 7 shows the dependence of the CNR of the magneto-optical disk having this structure on the recording laser output. Inner circumference (radius 24.
2 mm) and the outer circumference (39.5 mm) have improved CNR uniformity. Therefore, it is not necessary to change the laser output between the inner circumference and the outer circumference of the disk.

【0019】図3は本発明の光磁気記録媒体の別の実施
例を示す図で、第1誘電体保護層2aは屈折率2.15
のシリコン窒化膜を半径24mmで1000Å、半径3
9.5mmで900Åになるように、さらに光磁気記録
層3aはTbDyFeCo合金を半径24mmで200
Å、半径39.5mmで150Åになるように成膜した
ものである。他の各層の条件は図1の場合と同じであ
る。レーザーよって加熱された光磁気記録層3aの熱は
第2誘電体保護層4を介してAl反射層5に拡散放出さ
れ、又、光磁気記録層3aの熱は第1誘電体保護層2a
に拡散される。光磁気記録層3aの熱容量は膜厚が厚い
場所ほど大きくなる。又、外周側の第1誘電体保護層の
膜厚が薄いので内周側よりも外周側でのレーザー照射に
よる熱効率が改善される。
FIG. 3 is a diagram showing another embodiment of the magneto-optical recording medium of the present invention, in which the first dielectric protective layer 2a has a refractive index of 2.15.
The silicon nitride film of 1000 Å with a radius of 24 mm and a radius of 3
Further, the magneto-optical recording layer 3a is made of a TbDyFeCo alloy having a radius of 24 mm and a thickness of 200 mm so as to be 900 Å at 9.5 mm.
Å, a film having a radius of 39.5 mm and a thickness of 150 Å. The conditions for the other layers are the same as in FIG. The heat of the magneto-optical recording layer 3a heated by the laser is diffused and emitted to the Al reflection layer 5 through the second dielectric protection layer 4, and the heat of the magneto-optical recording layer 3a is also discharged to the first dielectric protection layer 2a.
Be spread to. The heat capacity of the magneto-optical recording layer 3a increases as the film thickness increases. Moreover, since the film thickness of the first dielectric protective layer on the outer peripheral side is thin, the thermal efficiency by laser irradiation on the outer peripheral side is improved rather than on the inner peripheral side.

【0020】図4は本発明の光磁気記録媒体の更に別の
実施例を示すもので、第1誘電体保護層2aは屈折率
2.15のシリコン窒化膜を半径24mmで1000
Å、半径39.5mmで900Åになるように、更に第
2誘電体保護体4aは屈折率2.15のシリコン窒化膜
を半径24mmで250Å、半径39.5mmで300
Åになるように成膜したものである。他の各層の条件は
図1の場合と同じである。第2誘電体保護層はレーザー
よって加熱された光磁気記録層3の熱がAl合金反射層
5まで拡散する場合の熱抵抗として働くため、第2誘電
体保護層の膜厚が厚くなるほど光磁気記録層から熱が逃
げにくくなる。また外周側の第1誘電体保護層の膜厚が
薄いので内周側よりも外周側でのレーザー照射による熱
効率が改善される。
FIG. 4 shows another embodiment of the magneto-optical recording medium of the present invention. The first dielectric protective layer 2a is a silicon nitride film having a refractive index of 2.15 and a radius of 24 mm of 1000.
Å, the second dielectric protector 4a is a silicon nitride film having a refractive index of 2.15 of 250 Å with a radius of 24 mm and 300 Å with a radius of 39.5 mm.
The film was formed so as to become Å. The conditions for the other layers are the same as in FIG. Since the second dielectric protection layer acts as a thermal resistance when the heat of the magneto-optical recording layer 3 heated by the laser diffuses to the Al alloy reflection layer 5, the thicker the second dielectric protection layer is, the more the magneto-optical property is increased. It becomes difficult for heat to escape from the recording layer. Further, since the thickness of the first dielectric protective layer on the outer peripheral side is thin, the thermal efficiency due to laser irradiation on the outer peripheral side is improved rather than on the inner peripheral side.

【0021】図5は本発明の光磁気記録媒体の更にまた
別の実施例を示すもので、第1誘電体保護層2aは屈折
率2.15のシリコン窒化膜を半径24mmで1000
Å、半径39.5mmで900Åになるように、更に金
属反射層5bはアルミニウム・チタン合金を半径24m
mで600Å、半径39.5mmで500Åになるよう
に成膜したものである。他の各層の条件は図1の場合と
同じである。レーザーによって加熱された光磁気記録層
3の熱は第2誘電体保護層4を介してAl合金反射層5
bに拡散放出される。Al合金反射層は熱の良導体であ
り、薄膜の膜厚が厚い場所ほど熱容量が大きくなり光磁
気記録層の熱を逃し安くなる。又、外周側の第1誘電体
保護層の膜厚が薄いので内周側よりも外周側でのレーザ
ー照射による熱効率が改善される。
FIG. 5 shows still another embodiment of the magneto-optical recording medium of the present invention. The first dielectric protective layer 2a is a silicon nitride film having a refractive index of 2.15 and a radius of 24 mm of 1000.
Å, the metal reflective layer 5b is made of aluminum / titanium alloy with a radius of 24 m so that the radius becomes 39.5 mm and 900Å.
The film was formed so as to have a thickness of 600Å in m and a radius of 39.5 mm in 500Å. The conditions for the other layers are the same as in FIG. The heat of the magneto-optical recording layer 3 heated by the laser is transmitted through the second dielectric protection layer 4 to the Al alloy reflection layer 5
It is diffused and emitted to b. The Al alloy reflection layer is a good conductor of heat, and the larger the thickness of the thin film, the larger the heat capacity, and the more the heat of the magneto-optical recording layer escapes, the cheaper it becomes. Moreover, since the film thickness of the first dielectric protective layer on the outer peripheral side is thin, the thermal efficiency by laser irradiation on the outer peripheral side is improved rather than on the inner peripheral side.

【0022】[0022]

【発明の効果】以上の如く本発明による各構成の光磁気
記録媒体はいずれも内周に対して外周側のレーザー照射
による熱効率が改善されるので、各々レーザー出力に対
してディスク全面にわたり均一なCNRが得られる。こ
のため半導体レーザーの出力制御回路等を簡略化でき
る。
As described above, in each of the magneto-optical recording media according to the present invention, the thermal efficiency of the laser irradiation on the outer circumference side with respect to the inner circumference is improved, so that the laser output is uniform over the entire disk surface. CNR is obtained. Therefore, the output control circuit of the semiconductor laser can be simplified.

【図面の簡単な説明】[Brief description of drawings]

【図1】従来の光磁気記録媒体の断面を示す模式図。FIG. 1 is a schematic view showing a cross section of a conventional magneto-optical recording medium.

【図2】[Fig. 2]

【図3】[Figure 3]

【図4】[Figure 4]

【図5】以上、本発明の光磁気記録媒体の断面を示す模
式図。
FIG. 5 is a schematic view showing a cross section of the magneto-optical recording medium of the present invention.

【図6】[Figure 6]

【図7】以上、光磁気記録媒体のCNRの記録レーザー
出力依存性を示す図で、図6は従来の、又、図7は本発
明の光磁気記録媒体のそれを示す。
7 is a diagram showing the recording laser output dependence of CNR of a magneto-optical recording medium, FIG. 6 showing that of a conventional magneto-optical recording medium, and FIG. 7 showing that of a magneto-optical recording medium of the present invention.

【符号の説明】[Explanation of symbols]

1 透明基板 2、2a 第1誘電体保護層 3、3a 光磁気記録層 4、4a 第2誘電体保護層 5、5a、5b Al合金反射膜 6 紫外線硬化型樹脂層 1 transparent substrate 2, 2a first dielectric protective layer 3, 3a magneto-optical recording layer 4, 4a second dielectric protective layer 5, 5a, 5b Al alloy reflective film 6 ultraviolet curable resin layer

Claims (8)

【特許請求の範囲】[Claims] 【請求項1】 透明な円盤基板上に第1誘電体保護層、
光磁気記録層、第2誘電体保護層、Al合金反射層及び
紫外線硬化樹脂がこの順で積層された光磁気記録媒体に
おいて、第1誘電体保護層の膜厚が記録媒体の径方向に
変化し、かつAl合金反射層の合金組成が記録媒体の径
方向に変化し、その際外周側におけるAlの組成の割合
が内周側よりも低いことを特徴とする光磁気記録媒体。
1. A first dielectric protective layer on a transparent disk substrate,
In a magneto-optical recording medium in which a magneto-optical recording layer, a second dielectric protective layer, an Al alloy reflective layer and an ultraviolet curable resin are laminated in this order, the film thickness of the first dielectric protective layer changes in the radial direction of the recording medium. In addition, the magneto-optical recording medium is characterized in that the alloy composition of the Al alloy reflective layer changes in the radial direction of the recording medium, and the proportion of Al composition on the outer peripheral side is lower than that on the inner peripheral side.
【請求項2】 第1誘電体保護層を屈折率が2.00〜
2.30のシリコン窒化膜とし、基板のグループの最外
周部から最内周部に位置する第1誘電体保護層の膜厚を
800〜1000Åの範囲とすることを特徴とする請求
項1記載の光磁気記録媒体。
2. The first dielectric protective layer has a refractive index of 2.00 to
2. The silicon nitride film of 2.30, wherein the film thickness of the first dielectric protective layer located from the outermost peripheral portion to the innermost peripheral portion of the group of substrates is in the range of 800 to 1000Å. Magneto-optical recording medium.
【請求項3】 第1誘電体保護層の外周側における膜厚
が内周側よりも薄く、かつ光磁気記録層の膜厚が記録媒
体の径方向に変化し、その際外周側における膜厚が内周
側よりも薄いことを特徴とする請求項2記載の光磁気記
録媒体。
3. The film thickness on the outer peripheral side of the first dielectric protective layer is thinner than that on the inner peripheral side, and the film thickness of the magneto-optical recording layer changes in the radial direction of the recording medium. 3. The magneto-optical recording medium according to claim 2, wherein is thinner than the inner peripheral side.
【請求項4】 光磁気記録層をTbDyFeCo合金と
し、基板のグループの最外周側から最内周部に位置する
光磁気記録層の膜厚を150〜300Åの範囲にするこ
とを特徴とする請求項3記載の光磁気記録媒体。
4. The magneto-optical recording layer is made of a TbDyFeCo alloy, and the film thickness of the magneto-optical recording layer located from the outermost peripheral side to the innermost peripheral portion of the substrate group is set in the range of 150 to 300Å. Item 3. A magneto-optical recording medium.
【請求項5】 第1誘電体保護層の外周側における膜厚
が内周側よりも薄く、かつ第2誘電体保護層の膜厚が記
録媒体の径方向に変化し、その際外周側における膜厚が
内周側よりも厚いことを特徴とする請求項2記載の光磁
気記録媒体。
5. The film thickness on the outer peripheral side of the first dielectric protective layer is thinner than that on the inner peripheral side, and the film thickness of the second dielectric protective layer changes in the radial direction of the recording medium. The magneto-optical recording medium according to claim 2, wherein the film thickness is thicker than the inner peripheral side.
【請求項6】 第2誘電体保護層を屈折率が2.00〜
2.30のシリコン窒化膜とし、基板のグループの最外
周部から最内周部に位置する第2誘電体保護層の膜厚を
250〜350Åの範囲とすることを特徴とする請求項
5記載の光磁気記録媒体。
6. The second dielectric protective layer has a refractive index of 2.00 to
6. The silicon nitride film of 2.30, wherein the film thickness of the second dielectric protection layer located from the outermost peripheral portion to the innermost peripheral portion of the substrate group is in the range of 250 to 350Å. Magneto-optical recording medium.
【請求項7】 第1誘電体保護層の外周側における膜厚
が内周側よりも薄く、かつAl合金反射層の膜厚が記録
媒体の径方向に変化し、その際外周側における膜厚が内
周側よりも薄いことを特徴とする請求項2記載の光磁気
記録媒体。
7. The film thickness on the outer peripheral side of the first dielectric protective layer is thinner than that on the inner peripheral side, and the film thickness of the Al alloy reflective layer changes in the radial direction of the recording medium, in which case the film thickness on the outer peripheral side. 3. The magneto-optical recording medium according to claim 2, wherein is thinner than the inner peripheral side.
【請求項8】 基板のグルーブの最外周部から最内周部
に位置するAl合金反射層の膜厚を400〜650Åの
範囲とすることを特徴とする請求項7記載の光磁気記録
媒体。
8. The magneto-optical recording medium according to claim 7, wherein the film thickness of the Al alloy reflective layer located from the outermost peripheral portion to the innermost peripheral portion of the groove of the substrate is in the range of 400 to 650Å.
JP4207290A 1992-07-10 1992-07-10 Magneto-optical recording medium Pending JPH0628724A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4207290A JPH0628724A (en) 1992-07-10 1992-07-10 Magneto-optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4207290A JPH0628724A (en) 1992-07-10 1992-07-10 Magneto-optical recording medium

Publications (1)

Publication Number Publication Date
JPH0628724A true JPH0628724A (en) 1994-02-04

Family

ID=16537350

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4207290A Pending JPH0628724A (en) 1992-07-10 1992-07-10 Magneto-optical recording medium

Country Status (1)

Country Link
JP (1) JPH0628724A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0751511A2 (en) * 1995-06-30 1997-01-02 Sony Corporation Magneto-optical disc
JP2007334141A (en) * 2006-06-16 2007-12-27 Sanyo Electric Co Ltd Culture observation system

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0751511A2 (en) * 1995-06-30 1997-01-02 Sony Corporation Magneto-optical disc
EP0751511A3 (en) * 1995-06-30 1997-06-25 Sony Corp Magneto-optical disc
US5751670A (en) * 1995-06-30 1998-05-12 Sony Corporation Magneto-optical disk having variable thickness recording layer but adequate uniform reflectance value
JP2007334141A (en) * 2006-06-16 2007-12-27 Sanyo Electric Co Ltd Culture observation system

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