JPH06274951A - Magneto-optical recording medium - Google Patents

Magneto-optical recording medium

Info

Publication number
JPH06274951A
JPH06274951A JP5061779A JP6177993A JPH06274951A JP H06274951 A JPH06274951 A JP H06274951A JP 5061779 A JP5061779 A JP 5061779A JP 6177993 A JP6177993 A JP 6177993A JP H06274951 A JPH06274951 A JP H06274951A
Authority
JP
Japan
Prior art keywords
layer
magneto
reproducing
recording medium
optical recording
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.)
Granted
Application number
JP5061779A
Other languages
Japanese (ja)
Other versions
JP3328988B2 (en
Inventor
Koyata Takahashi
小弥太 高橋
Toshio Inao
俊雄 稲生
Akio Kondo
昭夫 近藤
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.)
Tosoh Corp
Original Assignee
Tosoh Corp
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 Tosoh Corp filed Critical Tosoh Corp
Priority to JP06177993A priority Critical patent/JP3328988B2/en
Publication of JPH06274951A publication Critical patent/JPH06274951A/en
Application granted granted Critical
Publication of JP3328988B2 publication Critical patent/JP3328988B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To obtain a MSR medium which can be formed in films with small number of targets. CONSTITUTION:This magneto-optical recording medium (MSR medium) consists of a transparent substrate, dielectric material layer, and an exchange coupling multilayer film consisting of at least a reproducing layer, intermediate layer and recording holding layer. Recorded signals in the medium are read by changing the magnetized state of the reproducing layer. Among the films of the exchange coupling multilayer film, the layer having the lower Curie temp. consists of (Tb, Fe, Co)1-xSix (x<=0.18). Thereby, the number of targets necessary for formation of the multilayer film can be decreased, and by only controlling the Si density, the margin for the Curie temp. of the intermediate layer can be increased.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は書き換えが可能な光磁気
記録媒体のなかで、再生層の磁化状態を変化させながら
記録信号を読み取る光磁気記録媒体に係わる。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a rewritable magneto-optical recording medium for reading a recording signal while changing the magnetization state of a reproducing layer.

【0002】[0002]

【従来の技術】光磁気記録媒体は書き換え可能な光記録
媒体であり、相変化型光記録媒体などと比較して繰り返
し消去/書き込み耐久性や消去比率に優れ、可搬型大容
量の記録媒体として注目されている。
2. Description of the Related Art A magneto-optical recording medium is a rewritable optical recording medium, and is excellent in repeated erasing / writing durability and erasing ratio as compared with a phase change type optical recording medium and is a portable large capacity recording medium. Attention has been paid.

【0003】光磁気記録媒体は、レ−ザ−光照射による
局所加熱によって記録ビットを形成し、これをカ−効果
により読み出す記録再生方法が取られる。記録ビットの
間隔はレ−ザ−光照射パワ−、記録磁界の強度などの調
整でレ−ザ−スポット径よりもかなり小さくすることが
可能であるが、読みだしは再生時のレ−ザ波長、レンズ
の開口率などによって制約を受ける。
The magneto-optical recording medium employs a recording / reproducing method in which a recording bit is formed by local heating by laser light irradiation, and the recording bit is read by the curling effect. The recording bit interval can be made considerably smaller than the laser spot diameter by adjusting the laser light irradiation power, the recording magnetic field strength, etc., but the reading is the laser wavelength during reproduction. , It is limited by the aperture ratio of the lens.

【0004】このような再生時の制約から決まる記録密
度を越えて、読み出すための改善の試みとして、少なく
とも再生層と記録保持層を有し再生層の磁化状態を変化
させながら記録信号を読み取る方法がMSR(Magn
etically induced Super Re
solution)と呼ばれて近年注目されている。例
えば、消滅型MSRあるいはFAD(Front Ap
erture Detection)とよばれる方式は
特開平1−143041号公報や特開平1−14304
2号公報に開示され、記録ビットを再生時に拡大、縮小
させながら再生することにより再生分解能が向上する技
術である。この方式は、記録磁性層を再生層、中間層、
記録保持層からなる交換結合多層膜とし、再生光照射に
よる温度上昇を利用し、中間層のキュリ−温度以上の高
温領域で再生層を再生磁界の方向に常に向けることによ
り、ビ−ムスポットを部分的にいわばマスクするもの
で、再生時の符号間干渉を減少させ、光の回折限界以下
の周期の信号を再生可能とするものである。
As an attempt to improve the reading beyond the recording density determined by such a restriction at the time of reproduction, a method of reading a recording signal while at least having a reproduction layer and a recording holding layer and changing the magnetization state of the reproduction layer. Is MSR (Magn
physically induced Super Re
In recent years, it has been drawing attention as a solution. For example, extinction type MSR or FAD (Front Ap)
A method called "entry detection" is disclosed in Japanese Laid-Open Patent Publication No. 1-143041 and Japanese Laid-Open Patent Publication No. 1-14304.
This is a technique disclosed in Japanese Patent Laid-Open No. 2 (1994), in which the reproduction resolution is improved by reproducing the recorded bits while enlarging or reducing the recorded bits. In this method, the recording magnetic layer is a reproducing layer, an intermediate layer,
A beam spot is formed by using an exchange-coupling multilayer film composed of a recording holding layer, and utilizing the temperature rise due to the irradiation of reproducing light, and always orienting the reproducing layer in the direction of the reproducing magnetic field in a high temperature region above the Curie temperature of the intermediate layer. It is a so-called mask partly, which reduces the intersymbol interference at the time of reproduction and makes it possible to reproduce a signal having a period less than the diffraction limit of light.

【0005】また、浮き出し型MSRあるいはRAD
(Rear Aperture Detection)
とよばれる方式は特開平3−93058号公報に開示さ
れ、記録磁性層を再生層、再生補助層、中間層、記録保
持層からなる交換結合多層膜とし、再生前に初期化磁石
で再生層の磁化の向きを揃えた後、記録保持層の記録ビ
ットを再生層に転写しながら、再生することにより再生
分解能が向上する技術である。
In addition, a raised MSR or RAD
(Rear Aperture Detection)
A method called "a" is disclosed in Japanese Patent Laid-Open No. 3-93058, and the recording magnetic layer is an exchange coupling multilayer film including a reproducing layer, a reproducing auxiliary layer, an intermediate layer and a recording holding layer, and a reproducing layer is formed by an initialization magnet before reproducing. Is a technique for improving the reproduction resolution by reproducing the recording bits of the recording holding layer while transferring the recording bits of the recording holding layer to the reproducing layer after aligning the magnetization directions.

【0006】多層膜の各層で最もキュリ−温度が低いの
はFAD方式においては中間層、RAD方式においては
再生補助層である。これらの材料は、例えば特開平1−
143041号公報ではTbFe、TbFeCo、Dy
FeCo、特開平4−255937号公報ではTbFe
CoAlなどが示されている。
The lowest Curie temperature in each layer of the multilayer film is the intermediate layer in the FAD system and the regeneration assisting layer in the RAD system. These materials are disclosed, for example, in JP-A-1-
No. 143041 discloses TbFe, TbFeCo, Dy.
FeCo, TbFe in JP-A-4-255937
CoAl and the like are shown.

【0007】[0007]

【発明が解決しようとする課題】これらの複雑な多層膜
は通常スパッタ法で成膜されるが、合金タ−ゲットで成
膜したとしても最低膜の数だけのタ−ゲットが必要で、
さらに各層の最適の組み合わせを決める為には同時スパ
ッタを行う必要がありタ−ゲットの数はさらに多くな
る。
These complicated multi-layered films are usually formed by a sputtering method, but even if they are formed by an alloy target, it is necessary to have as many targets as the number of films.
Further, in order to determine the optimum combination of each layer, it is necessary to carry out simultaneous sputtering, and the number of targets is further increased.

【0008】本発明が解決しようとする課題は、できる
だけ少ない数のタ−ゲットで成膜が可能なMSR媒体を
得ることを可能とするものである。
[0008] The problem to be solved by the present invention is to make it possible to obtain an MSR medium capable of forming a film with as few targets as possible.

【0009】[0009]

【課題を解決するための手段】本発明者らは、誘電体成
膜に必要なSiに注目して、中間層あるいは再生補助層
をTbFeCoSiとすることでタ−ゲットの数を少な
くすることを可能とし、本発明を完成するに至った。
DISCLOSURE OF THE INVENTION The inventors of the present invention pay attention to Si necessary for dielectric film formation and reduce the number of targets by using TbFeCoSi as an intermediate layer or a reproduction assisting layer. It was made possible, and the present invention was completed.

【0010】即ち本発明は、透明基板上に誘電体層を介
して、少なくとも再生層、記録保持層及び再生層と記録
保持層との間に中間層を設けてなる交換結合多層膜を形
成し、再生層の磁化状態を変化させながら記録信号を読
み出す光磁気記録媒体において、交換結合多層膜を形成
する膜中で最も低いキュリー温度をもつべき層(以下、
特定層と称する)が、少なくとも(Tb、Fe)1-x
x(但し、x≦0.18)に示される元素より構成さ
れていることを特徴とする光磁気記録媒体に関する。
That is, according to the present invention, an exchange-coupling multilayer film is formed on a transparent substrate through a dielectric layer, at least a reproducing layer, a recording holding layer, and an intermediate layer provided between the reproducing layer and the recording holding layer. , In a magneto-optical recording medium that reads a recording signal while changing the magnetization state of the reproducing layer, a layer that should have the lowest Curie temperature in the film forming the exchange coupling multilayer film (hereinafter,
The specific layer) is at least (Tb, Fe) 1-x S
The present invention relates to a magneto-optical recording medium characterized by comprising an element represented by i x (where x ≦ 0.18).

【0011】本発明において、特定層とは、FAD方式
においては中間層、RAD方式においては再生補助層に
相当する。特定層としてTbFeCoにSiを含有させ
た場合、Si濃度xを高くすることでキュリ−温度が下
がり、x=0.18でSiを含有しないとき(TbFe
Coのみ)と比べて約150℃下がる。x>0.18に
なってもさらにキュリ−温度は下がるが、垂直磁気異方
性の下がり方が著しくなり良好なMSR特性が得られな
くなる。
In the present invention, the specific layer corresponds to the intermediate layer in the FAD system and the reproduction auxiliary layer in the RAD system. When Si is contained in TbFeCo as the specific layer, the Curie temperature is lowered by increasing the Si concentration x, and when Si is not contained at x = 0.18 (TbFeCo
It is about 150 ° C lower than that of Co only). Even if x> 0.18, the Curie temperature is further lowered, but the perpendicular magnetic anisotropy is significantly lowered, and good MSR characteristics cannot be obtained.

【0012】キュリ−温度、垂直磁気異方性の関係から
特定層は、 (Tby(Fe1-zCoz))1-xSix (但し、x≦0.18、0.14≦y≦0.30、0≦
z≦0.20)なる構成をとることが好ましい。
[0012] Curie - temperature, the specific layer from the relationship between the perpendicular magnetic anisotropy, (Tb y (Fe 1- z Co z)) 1-x Si x ( where, x ≦ 0.18,0.14 ≦ y ≦ 0.30, 0 ≦
z ≦ 0.20) is preferable.

【0013】また、本発明の光磁気記録媒体の特定層に
は、耐久性を高める為にCr、Ti、Ta等を0.1〜
15atm%含んでいてもよい。
Further, in the specific layer of the magneto-optical recording medium of the present invention, Cr, Ti, Ta, etc. are added in an amount of 0.1 to 0.1% in order to improve durability.
It may be contained at 15 atm%.

【0014】本発明の光磁気記録媒体の製造方法として
は、例えばGd、Tb、FeCo、Siをタ−ゲットと
してそれらの任意の同時スパッタの組み合わせで成膜す
ることが可能である。より具体的にはFADの場合、誘
電体層を窒化ケイ素、再生層をGdFeCo、中間層を
TbFeCoSi、記録保持層をTbFeCoとして成
膜することができ、RADの場合、誘電体層を窒化ケイ
素、再生層をGdFeCo、再生補助層をTbFeCo
Si、中間層をGdFeCoまたはGdFeCoSi、
記録保持層をTbFeCoとして成膜することができ
る。従来、中間層にAlを添加したり、記録保持層と中
間層とでCoとFeの組成比を変えたりする方法が取ら
れていたが、このような方法ではさらに1〜2個のタ−
ゲットを追加して、スパッタチャンバ−の個数も増加せ
ざるを得なかった。
In the method of manufacturing the magneto-optical recording medium of the present invention, it is possible to form a film by using Gd, Tb, FeCo, and Si as targets and combining them by any desired simultaneous sputtering. More specifically, in the case of FAD, the dielectric layer can be formed of silicon nitride, the reproducing layer can be formed of GdFeCo, the intermediate layer can be formed of TbFeCoSi, and the recording holding layer can be formed of TbFeCo. In the case of RAD, the dielectric layer can be formed of silicon nitride, The reproducing layer is GdFeCo, and the reproducing auxiliary layer is TbFeCo.
Si, the intermediate layer is GdFeCo or GdFeCoSi,
The recording holding layer can be formed as TbFeCo. Conventionally, a method of adding Al to the intermediate layer or changing the composition ratio of Co and Fe between the recording holding layer and the intermediate layer has been taken.
The number of sputter chambers had to be increased by adding a get.

【0015】本発明の光磁気記録媒体で、記録保持層が
TbFeCo、特定層がTbFeCoSiからなる場
合、CoとFeの組成比が同一となるため、特定層と記
録保持層とのキュリ−温度の差により顕著なMSR効果
を得るためには、Si濃度xを0.07<xとすること
が好ましい。
In the magneto-optical recording medium of the present invention, when the recording holding layer is made of TbFeCo and the specific layer is made of TbFeCoSi, the composition ratios of Co and Fe are the same, so that the Curie temperatures of the specific layer and the recording holding layer are the same. In order to obtain a remarkable MSR effect due to the difference, the Si concentration x is preferably 0.07 <x.

【0016】[0016]

【実施例】【Example】

実施例1 Gd、Tb、Fe0.87Co0.13およびSiの各タ−ゲッ
トをそれぞれ単独あるいは同時スパッタの組合せとして
用い、図1に示すようなFAD方式の光磁気記録媒体を
製造した。ポリカ−ボネ−ト基板1上に、窒化ケイ素か
らなる誘電体層2(膜厚:800オングストローム)、
GdFeCoからなる再生層3(膜厚:300オングス
トローム、磁化:20emu/cc(室温)、キュリー
温度:340℃)、TbFeCoSiからなる中間層4
(膜厚:100オングストローム、補償組成、キュリー
温度:80〜200℃)、TbFeCoからなる記録保
持層5(膜厚:400オングストローム、保磁力:>1
2kOe、キュリー温度:260℃)、さらに窒化ケイ
素層6(膜厚:800オングストローム)を成膜した。
Example 1 An FAD type magneto-optical recording medium as shown in FIG. 1 was manufactured by using each target of Gd, Tb, Fe 0.87 Co 0.13 and Si individually or as a combination of co-sputtering. A dielectric layer 2 made of silicon nitride (film thickness: 800 angstrom) is formed on a polycarbonate substrate 1.
Reproducing layer 3 made of GdFeCo (film thickness: 300 Å, magnetization: 20 emu / cc (room temperature), Curie temperature: 340 ° C.), intermediate layer 4 made of TbFeCoSi
(Film thickness: 100 Å, compensation composition, Curie temperature: 80 to 200 ° C.), TbFeCo recording holding layer 5 (film thickness: 400 Å, coercive force:> 1)
2 kOe, Curie temperature: 260 ° C.), and a silicon nitride layer 6 (film thickness: 800 Å) was further formed.

【0017】中間層のキュリ−温度を80〜200℃で
変化させるためにTbFeCoSi中のSi濃度はx=
0.08〜0.19で変化させた。補償組成とするため
にTb濃度も同時に変化させた。図2にSi濃度xに対
してキュリ−温度、補償組成のTb濃度yを示す。
In order to change the Curie temperature of the intermediate layer at 80 to 200 ° C., the Si concentration in TbFeCoSi is x =
The value varied from 0.08 to 0.19. The Tb concentration was also changed at the same time to obtain a compensation composition. FIG. 2 shows the Curie temperature with respect to the Si concentration x and the Tb concentration y of the compensation composition.

【0018】次に、この光磁気記録媒体を記録再生装置
にセットして、線速度5.5m/secで回転させなが
ら780nmの波長のレ−ザ−ビ−ムを33%のデュ−
ティ−において7.1MHzで変調させながら5.4m
Wのレ−ザ−パワ−で記録を行なった。記録時のバイア
ス磁界は250Oeであった。
Next, this magneto-optical recording medium was set in a recording / reproducing apparatus, and while being rotated at a linear velocity of 5.5 m / sec, a laser beam having a wavelength of 780 nm and a duty ratio of 33% were used.
5.4m while modulating at 7.1MHz on the tee
Recording was performed with a W laser power. The bias magnetic field during recording was 250 Oe.

【0019】消去方向に300Oeのバイアス磁界(H
r)をかけながらレ−ザ−パワ−を1〜2.5mWで調
整して再生し、得られた最大のC/Nの値をSi濃度と
比較して図3に示す。Si濃度が0.18以下で40d
B以上の良好なC/Nが、特にx<0.15では45d
B以上の更に良好なC/Nが得られた。
A bias magnetic field of 300 Oe (H
The laser power was adjusted to 1 to 2.5 mW and regenerated while applying r), and the maximum C / N value obtained is shown in FIG. 3 in comparison with the Si concentration. 40d when Si concentration is 0.18 or less
Good C / N of B or more, especially 45d when x <0.15
An even better C / N of B or higher was obtained.

【0020】[0020]

【発明の効果】本発明の光磁気記録媒体では、MSR媒
体の特定層を少なくともTb、Fe及びSiから構成す
ることで、誘電体成膜に必要なSiタ−ゲットとタ−ゲ
ットを共通化して多層膜成膜に必要なのタ−ゲットの数
を少なくすることを可能とした。また、Si添加による
垂直磁気異方性の低下が緩やかなので、Si濃度の調整
だけで特定層のキュリ−温度の選択の幅を150℃程度
取ることができ、マ−ジンを考慮したMSR媒体の設計
が可能である。
In the magneto-optical recording medium of the present invention, the specific layer of the MSR medium is composed of at least Tb, Fe and Si, so that the Si target and the target required for the dielectric film formation are made common. It is possible to reduce the number of targets necessary for forming a multilayer film. Further, since the perpendicular magnetic anisotropy is gradually decreased by adding Si, the range of selection of the Curie temperature of the specific layer can be set to about 150 ° C. only by adjusting the Si concentration, and the MSR medium considering the margin can be obtained. Design is possible.

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

【図1】 本発明の光磁気記録媒体の構造の一例を示す
断面図である。
FIG. 1 is a sectional view showing an example of a structure of a magneto-optical recording medium of the present invention.

【図2】 TbFeCoSi中間層のSi濃度を変化さ
せたときのキュリ−温度または補償組成との関係を示す
図である。
FIG. 2 is a diagram showing a relationship with a Curie temperature or a compensation composition when the Si concentration of a TbFeCoSi intermediate layer is changed.

【図3】 実施例1の光磁気記録媒体をFAD再生した
ときのSi濃度とC/Nとの関係を示す図である。
FIG. 3 is a diagram showing a relationship between Si concentration and C / N when FAD reproduction is performed on the magneto-optical recording medium of Example 1.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 透明基板上に誘電体層を介して、少なく
とも再生層、記録保持層及び再生層と記録保持層との間
に中間層を設けてなる交換結合多層膜を形成し、再生層
の磁化状態を変化させながら記録信号を読み出す光磁気
記録媒体において、交換結合多層膜を形成する膜中で最
も低いキュリー温度をもつべき層が、少なくとも(T
b、Fe)1-xSix(但し、x≦0.18)に示される
元素より構成されていることを特徴とする光磁気記録媒
体。
1. A reproducing layer is formed on a transparent substrate by forming at least a reproducing layer, a recording holding layer and an intermediate layer between the reproducing layer and the recording holding layer with a dielectric layer interposed therebetween. In a magneto-optical recording medium for reading out a recording signal while changing the magnetization state of, the layer that should have the lowest Curie temperature in the film forming the exchange-coupling multilayer film is at least (T
b, Fe) 1-x Si x (provided that x ≦ 0.18), a magneto-optical recording medium.
JP06177993A 1993-03-22 1993-03-22 Magneto-optical recording medium Expired - Fee Related JP3328988B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP06177993A JP3328988B2 (en) 1993-03-22 1993-03-22 Magneto-optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP06177993A JP3328988B2 (en) 1993-03-22 1993-03-22 Magneto-optical recording medium

Publications (2)

Publication Number Publication Date
JPH06274951A true JPH06274951A (en) 1994-09-30
JP3328988B2 JP3328988B2 (en) 2002-09-30

Family

ID=13180926

Family Applications (1)

Application Number Title Priority Date Filing Date
JP06177993A Expired - Fee Related JP3328988B2 (en) 1993-03-22 1993-03-22 Magneto-optical recording medium

Country Status (1)

Country Link
JP (1) JP3328988B2 (en)

Also Published As

Publication number Publication date
JP3328988B2 (en) 2002-09-30

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