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JP3108126B2 - Magneto-optical recording medium - Google Patents
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JP3108126B2 - Magneto-optical recording medium - Google Patents

Magneto-optical recording medium

Info

Publication number
JP3108126B2
JP3108126B2 JP03126087A JP12608791A JP3108126B2 JP 3108126 B2 JP3108126 B2 JP 3108126B2 JP 03126087 A JP03126087 A JP 03126087A JP 12608791 A JP12608791 A JP 12608791A JP 3108126 B2 JP3108126 B2 JP 3108126B2
Authority
JP
Japan
Prior art keywords
layer
magneto
recording medium
optical recording
underlayer
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 - Fee Related
Application number
JP03126087A
Other languages
Japanese (ja)
Other versions
JPH04351733A (en
Inventor
靖子 寺垣
聡 鷲見
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.)
Sanyo Electric Co Ltd
Original Assignee
Sanyo Electric 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 Sanyo Electric Co Ltd filed Critical Sanyo Electric Co Ltd
Priority to JP03126087A priority Critical patent/JP3108126B2/en
Publication of JPH04351733A publication Critical patent/JPH04351733A/en
Application granted granted Critical
Publication of JP3108126B2 publication Critical patent/JP3108126B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

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、記録膜の基板側にPt
層を形成した構造の光磁気記録媒体に関するものであ
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention
The present invention relates to a magneto-optical recording medium having a structure in which a layer is formed.

【0002】[0002]

【従来の技術】従来技術によるPt/Co積層構造の光
磁気記録媒体の例を図2、図3に示す。図2は、ガラス
やPC(ポリカーボネート)の基板1上に、カー効果を
増大させるため下地層(Si34)4を成膜し、成膜し
た下地層4の表面を平滑にするため、エッチング5処理
を行い、更にその上にPtとCoをPt層、Co層、
…、Pt層の順に積層したものである(第14回 日本
応用磁気学会学術講演概要集(1990)65頁「Pt
/Co積層膜の微細構造」鷲見他)。このような光磁気
記録媒体では、Si34がアモルファスであり、Pt層
が[111]方向にきれいに積層されない。従って、垂
直磁気異方性が小さく、保磁力は1kOe程度しか得ら
れない。
2. Description of the Related Art FIGS. 2 and 3 show an example of a conventional magneto-optical recording medium having a Pt / Co laminated structure. FIG. 2 shows that an underlayer (Si 3 N 4 ) 4 is formed on a glass or PC (polycarbonate) substrate 1 in order to increase the Kerr effect, and the surface of the formed underlayer 4 is smoothed. Etching 5 treatment is performed, and Pt and Co are further deposited on the Pt layer, the Co layer,
…, Pt layers in this order (14th Annual Meeting of the Japan Society of Applied Magnetics (1990), p. 65, “Pt
/ Co microstructure of laminated film ”, Sumi et al.). In such a magneto-optical recording medium, the Si 3 N 4 is amorphous, and the Pt layer is not stacked clearly in the [111] direction. Therefore, the perpendicular magnetic anisotropy is small and the coercive force is only about 1 kOe.

【0003】また、図3に示すようなGaAs6やAg
を下地層として用いることによって、Pt/Co積層構
造の光磁気記録媒体の保磁力が4kOeまで増大したと
いう報告があるが(E−MRS spring’90
CVIII−7)、GaAs6やAgは不透明なため、その
ような下地層を設けると、信号の読み出しができない。
[0003], GaAs6 or Ag, as shown in FIG. 3
It has been reported that the coercive force of a magneto-optical recording medium having a Pt / Co laminated structure was increased to 4 kOe by using as an underlayer (E-MRS spring '90).
CVIII-7), GaAs6 and Ag are opaque, so if such an underlayer is provided, signals cannot be read.

【0004】[0004]

【発明が解決しようとする課題】本発明は、かかる問題
点を解決するためになされたものであり、記録膜の基板
側にPt層を形成した構造の光磁気記録媒体において、
保磁力を大きくするものである。
SUMMARY OF THE INVENTION The present invention has been made in order to solve such a problem, and a magneto-optical recording medium having a structure in which a Pt layer is formed on a substrate side of a recording film is provided.
This is to increase the coercive force.

【0005】[0005]

【課題を解決するための手段】Pt層と遷移金属層とか
ら成る交互積層膜、もしくはPt層と希土類遷移金属合
金層とから成る磁性層を記録膜とした光磁気記録媒体に
おいて、センアエン鉱型構造、ウルツ石型構造、ヒ化ニ
ッケル型構造、リン化チタン型構造、炭化タングステン
型構造の中のいずれかの構造である透明な化合物から成
る下地層を、交互積層膜、もしくは磁性層と、基板との
間に挿入し、Pt層と下地層とが接する構造とした。
SUMMARY OF THE INVENTION In a magneto-optical recording medium in which a recording film is composed of an alternately laminated film composed of a Pt layer and a transition metal layer, or a magnetic layer composed of a Pt layer and a rare earth transition metal alloy layer, a senaene mineral type is used. Structure, wurtzite type structure, nickel arsenide type structure, titanium phosphide type structure, an underlayer made of a transparent compound having any one of the tungsten carbide type structure, an alternately laminated film, or a magnetic layer, The structure was inserted between the substrate and the Pt layer so that the Pt layer was in contact with the underlayer.

【0006】[0006]

【作用】本発明による光磁気記録媒体では、記録膜を構
成するPt層が結晶構造を有する下地層に接しているた
め、記録膜を成膜する際に、Pt層を成膜するとPt層
も結晶が密な並び方をしている下地層と同じように密な
並び方をする。これによって、記録膜の保磁力が大きく
なり、高密度記録が可能になる。
In the magneto-optical recording medium according to the present invention, the Pt layer constituting the recording film is in contact with the underlayer having a crystalline structure. Crystals are densely arranged in the same manner as a base layer in which crystals are densely arranged. As a result, the coercive force of the recording film increases, and high-density recording becomes possible.

【0007】[0007]

【実施例】本発明による一実施例を図面に基づいて説明
する。
An embodiment according to the present invention will be described with reference to the drawings.

【0008】図1は、本発明によるPt/Co積層構造
の光磁気記録媒体の断面構造図であり、基板1上に下地
層2を成膜し、更に前記下地層2上にPt層、Co層、
…、Pt層の順にPt/Co積層膜3を形成したもので
ある。前記下地層2は、センアエン鉱型構造、ウルツ石
型構造、ヒ化ニッケル型構造、リン化チタン型構造、炭
化タングステン型構造の中のいずれかの構造である透明
な化合物を用いた。
FIG. 1 is a sectional view of a magneto-optical recording medium having a Pt / Co laminated structure according to the present invention, in which a base layer 2 is formed on a substrate 1, and a Pt layer and a Co layer are formed on the base layer 2. layer,
.., The Pt / Co laminated film 3 is formed in the order of the Pt layer. For the underlayer 2, a transparent compound having any one of a senaenite structure, a wurtzite structure, a nickel arsenide structure, a titanium phosphide structure, and a tungsten carbide structure was used.

【0009】Pt結晶は、図4に示すように面心立方格
子であり、[111]方向から見ると図5のように最密
な積み重ねをした構造である。格子定数は3.9Å、原
子間距離は2.8Åである。下地層表面の原子の並び方
が、Ptの[111]方向から見た面と類似していると
Ptの配向性が向上する。
The Pt crystal is a face-centered cubic lattice as shown in FIG. 4, and has a structure in which the Pt crystals are densely stacked as shown in FIG. 5 when viewed from the [111] direction. The lattice constant is 3.9 ° and the interatomic distance is 2.8 °. When the arrangement of atoms on the surface of the underlayer is similar to the plane of Pt viewed from the [111] direction, the orientation of Pt is improved.

【0010】結晶のある面がPtの[111]方向から
見た面と同じ並び方をするものを図6〜10に示す。図
6は立方晶のセンアエン鉱型構造で[111]方向から
見るとPtと同じように密な並び方をする。図7はウル
ツ石型構造、図8はヒ化ニッケル型構造、図9はリン化
チタン型構造、図10は炭化タングステン型構造で、い
ずれも六方晶であり、[111]方向から見ると、Pt
の[111]方向から見た面と同じ密な並び方をしてい
る。そこで、以上の結晶構造を持つもので、立方晶の格
子定数が3.9Å付近、六方晶の格子定数が2.8Å付
近のものを下地層として用い、その上にPtを成膜する
とPt層も最密な構造で成膜されることになる。図11
は、下地層の表面がPtの[111]方向から見た面と
大きく異なるときを、図12は類似しているときのPt
層と下地層の界面の状態を示したものである。ここで、
7はPt原子、8は下地層の原子である。図12はPt
が最密な並び方をしながら成膜されている。
FIGS. 6 to 10 show a case where a plane having a crystal is arranged in the same manner as a plane viewed from the [111] direction of Pt. FIG. 6 shows a cubic senaenite type structure, which is densely arranged like Pt when viewed from the [111] direction. 7 is a wurtzite structure, FIG. 8 is a nickel arsenide structure, FIG. 9 is a titanium phosphide structure, and FIG. 10 is a tungsten carbide structure, all of which are hexagonal and viewed from the [111] direction. Pt
In the same dense arrangement as the plane viewed from the [111] direction. Therefore, a substrate having the above crystal structure and having a cubic lattice constant of around 3.9 ° and a hexagonal lattice constant of around 2.8 ° is used as an underlayer. Is also formed with the closest structure. FIG.
FIG. 12 shows the case where the surface of the underlayer is significantly different from the surface of the Pt viewed from the [111] direction.
3 shows a state of an interface between a layer and an underlayer. here,
7 is a Pt atom, and 8 is an atom of the underlayer. FIG. 12 shows Pt
Are formed in the closest arrangement.

【0011】本発明によるPt/Co積層構造の光磁気
記録媒体の下地層に用いる化合物の例を表1に示す。
Table 1 shows examples of compounds used for the underlayer of the magneto-optical recording medium having a Pt / Co laminated structure according to the present invention.

【0012】[0012]

【表1】 [Table 1]

【0013】図13は、表1の化合物のうちAlNを下
地層として用いたPt/Co積層構造の光磁気記録媒体
9と従来技術よるPt/Co積層構造の光磁気記録媒体
(Si34を下地層として用いたもの)10の特性図で
ある。図13より、明らかに本発明によるPt/Co積
層構造の光磁気記録媒体は保磁力が増大していることが
分かる。
FIG. 13 shows a magneto-optical recording medium 9 having a Pt / Co laminated structure using AlN as an underlayer and a magneto-optical recording medium having a Pt / Co laminated structure (Si 3 N 4) according to the prior art. FIG. 10 is a characteristic diagram of No. 10 in which is used as an underlayer. FIG. 13 clearly shows that the coercive force of the magneto-optical recording medium having the Pt / Co laminated structure according to the present invention is increased.

【0014】また、表1のAlN以外の化合物を下地層
として用いた場合も同様の効果が得られる。
Similar effects can be obtained when a compound other than AlN shown in Table 1 is used as the underlayer.

【0015】光磁気記録媒体の記録膜は、Co以外の磁
性体(例えば、Fe)とPtの積層構造や、磁性膜(例
えば、希土類−遷移金属合金)の基板側にPt層を形成
した構造であってもよい。
The recording film of the magneto-optical recording medium has a laminated structure of a magnetic material other than Co (eg, Fe) and Pt, or a structure in which a Pt layer is formed on the substrate side of a magnetic film (eg, a rare earth-transition metal alloy). It may be.

【0016】[0016]

【発明の効果】本発明によれば、記録膜の基板側にPt
層を形成した構造の光磁気記録媒体において、Ptの配
向性が向上し、記録膜の保磁力が向上する。その結果、
高密度記録が可能になる。
According to the present invention, Pt is added to the substrate side of the recording film.
In a magneto-optical recording medium having a layered structure, the orientation of Pt is improved, and the coercive force of the recording film is improved. as a result,
High density recording becomes possible.

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

【図1】本発明によるPt/Co積層構造の光磁気記録
媒体の断面構造図である。
FIG. 1 is a sectional structural view of a magneto-optical recording medium having a Pt / Co laminated structure according to the present invention.

【図2】Si34を下地層に用いたPt/Co積層構造
の光磁気記録媒体の断面構造図である。
FIG. 2 is a sectional structural view of a magneto-optical recording medium having a Pt / Co laminated structure using Si 3 N 4 as an underlayer.

【図3】GaAsを下地層に用いたPt/Co積層構造
の光磁気記録媒体の断面構造図である。
FIG. 3 is a sectional structural view of a magneto-optical recording medium having a Pt / Co laminated structure using GaAs as an underlayer.

【図4】Ptの結晶構造(面心立方格子)を示す模式図
である。
FIG. 4 is a schematic diagram showing a crystal structure (face-centered cubic lattice) of Pt.

【図5】図4のPt結晶を[111]方向から見たPt
結晶の積み重ねの様子を示す図である。
FIG. 5 is a view showing the Pt crystal of FIG. 4 viewed from the [111] direction.
It is a figure which shows the mode of a stack of crystals.

【図6】センアエン鉱型構造の化合物の結晶構造を示す
模式図である。
FIG. 6 is a schematic view showing a crystal structure of a compound having a senaenite structure.

【図7】ウルツ石型構造の化合物の結晶構造を示す模式
図である。
FIG. 7 is a schematic diagram showing a crystal structure of a compound having a wurtzite structure.

【図8】ヒ化ニッケル型構造の化合物の結晶構造を示す
模式図である。
FIG. 8 is a schematic diagram showing a crystal structure of a compound having a nickel arsenide type structure.

【図9】リン化チタン型構造の化合物の結晶構造を示す
模式図である。
FIG. 9 is a schematic view showing a crystal structure of a compound having a titanium phosphide type structure.

【図10】炭化タングステン型構造の化合物の結晶構造
を示す模式図である。
FIG. 10 is a schematic view showing a crystal structure of a compound having a tungsten carbide type structure.

【図11】下地層の表面がPtの[111]方向から見
た面と大きく異なるときのPt層と下地層の界面の状態
を示す図である。
FIG. 11 is a diagram showing the state of the interface between the Pt layer and the underlayer when the surface of the underlayer is significantly different from the surface of the Pt viewed from the [111] direction.

【図12】下地層の表面がPtの[111]方向から見
た面と類似しているときのPt層と下地層の界面の状態
を示した図である。
FIG. 12 is a diagram showing a state of the interface between the Pt layer and the underlayer when the surface of the underlayer is similar to the surface of the Pt viewed from the [111] direction.

【図13】本発明によるPt/Co積層構造の光磁気記
録媒体(AlNを下地層として用いたもの)と従来技術
によるPt/Co積層構造の光磁気記録媒体(Si34
を下地層として用いたもの)の特性図である。
FIG. 13 shows a Pt / Co laminated magneto-optical recording medium (using AlN as an underlayer) according to the present invention and a conventional Pt / Co laminated magneto-optical recording medium (Si 3 N 4).
FIG. 4 is a characteristic diagram of a case where the underlayer is used as a base layer).

【符号の説明】[Explanation of symbols]

1 基板 2 下地層 3 Pt/Co積層膜 4 下地層(Si34) 5 エッチング 6 下地層(GaAs) 7 Pt原子 8 下地層の原子 9 本発明によるPt/Co積層構造の光磁気記録媒体
(AlNを下地層として用いたもの) 10 従来技術によるPt/Co積層構造の光磁気記録
媒体(Si34を下地層として用いたもの)
1 substrate 2 underlayer 3 Pt / Co multilayer film 4 underlayer (Si 3 N 4) 5 etched 6 underlayer (GaAs) 7 magneto-optical recording medium of the Pt / Co multilayer structure according atoms nine invention Pt atomic 8 underlayer (using AlN as an underlayer) 10 magneto-optical recording medium of the prior art Pt / Co multilayer structure (Si 3 N 4 that using as a base layer)

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 Pt層と遷移金属層とから成る交互積層
膜、もしくはPt層と希土類遷移金属合金層とから成る
磁性膜を記録膜とした光磁気記録媒体において、 センアエン鉱型構造、ウルツ石型構造、ヒ化ニッケル型
構造、リン化チタン型構造、炭化タングステン型構造の
中のいずれかの構造である透明な化合物から成る下地層
、前記交互積層膜、もしくは前記磁性膜と、基板との
間に挿入し、前記Pt層と前記下地層とが接する構造と
したことを特徴とする光磁気記録媒体。
1. An alternate lamination comprising a Pt layer and a transition metal layer.
Consisting of a film or a Pt layer and a rare earth transition metal alloy layer
In a magneto-optical recording medium using a magnetic film as a recording film , a transparent structure that is one of a senaenite structure, a wurtzite structure, a nickel arsenide structure, a titanium phosphide structure, and a tungsten carbide structure. A base layer made of a compound , the alternating laminated film, or the magnetic film, and a substrate
A structure in which the Pt layer and the underlayer are in contact with each other;
A magneto-optical recording medium characterized in that:
JP03126087A 1991-05-29 1991-05-29 Magneto-optical recording medium Expired - Fee Related JP3108126B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP03126087A JP3108126B2 (en) 1991-05-29 1991-05-29 Magneto-optical recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP03126087A JP3108126B2 (en) 1991-05-29 1991-05-29 Magneto-optical recording medium

Publications (2)

Publication Number Publication Date
JPH04351733A JPH04351733A (en) 1992-12-07
JP3108126B2 true JP3108126B2 (en) 2000-11-13

Family

ID=14926282

Family Applications (1)

Application Number Title Priority Date Filing Date
JP03126087A Expired - Fee Related JP3108126B2 (en) 1991-05-29 1991-05-29 Magneto-optical recording medium

Country Status (1)

Country Link
JP (1) JP3108126B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1866378B (en) * 1996-02-28 2010-09-29 松下电器产业株式会社 disc playback device

Also Published As

Publication number Publication date
JPH04351733A (en) 1992-12-07

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