JPH0845126A - Film forming method - Google Patents

Film forming method

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Publication number
JPH0845126A
JPH0845126A JP20273894A JP20273894A JPH0845126A JP H0845126 A JPH0845126 A JP H0845126A JP 20273894 A JP20273894 A JP 20273894A JP 20273894 A JP20273894 A JP 20273894A JP H0845126 A JPH0845126 A JP H0845126A
Authority
JP
Japan
Prior art keywords
dielectric layer
layer
target
electric field
high frequency
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
JP20273894A
Other languages
Japanese (ja)
Inventor
Atsushi Yamaguchi
山口  淳
Yoshihisa Suzuki
誉久 鈴木
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 JP20273894A priority Critical patent/JPH0845126A/en
Publication of JPH0845126A publication Critical patent/JPH0845126A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To decrease the time for film forming by etching a base dielectric layer simultaneously with forming a film. CONSTITUTION:A base dielectric layer (S layer) is formed on the surface of a substrate attached to a turntable T2 by impressing a high frequency electric field produced by 600W power between a SiN target ST4 and a chamber C1 for 20min to produce plasma discharge of the ST4 while the turntable T2 is rotated. While T2 is rotated, a high frequency electric field produced by 600W power is impressed for 15min to produce plasma discharge of the ST4 to from a S layer. At the same time, a high frequency electric field produced by 200W power is impressed between C1 and T2 for 15min to produce plasma discharge near T2 to etch the S layer. Then, while T2 is rotated, a high frequency electric field produced by 100W power is impressed between a Pt target 6 and C1 and between a Co target 5 and C1 to produce plasma discharge of the targets 6, 5 to alternately form Pt layers and Co layers to total 15 layers on the S layer. Thus, the required time to form films for a magneto-optical disk is decreased.

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、スパッタリング法によ
り、基板上に下地誘電体層を成膜し、その上に記録磁性
層を成膜する方法に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method of forming a base dielectric layer on a substrate by a sputtering method and forming a recording magnetic layer on the base dielectric layer.

【0002】[0002]

【従来の技術】レーザ光を用いて記録・再生を行う光磁
気記録方式は、磁気ヘッドを用いた磁気記録方式と比較
して記録密度が高く、また、記録・再生時に於いてヘッ
ドと記録媒体とが非接触であるために信頼性が高いとい
うメリットを有している。このため、盛んに研究された
結果、現在では実用化レベルに達している。
2. Description of the Related Art A magneto-optical recording method for recording / reproducing by using a laser beam has a higher recording density than a magnetic recording method using a magnetic head, and a head and a recording medium at the time of recording / reproducing. Since and are not in contact with each other, they have an advantage of high reliability. Therefore, as a result of vigorous research, it has reached the level of practical use at present.

【0003】現在使用されている光磁気記録用レーザ光
の波長は、780nmの赤外光が主流である。また、記
録磁性層としては、赤外光波長付近での磁気光学効果
(カー効果)の大きいTbFeCo膜に代表される希土
類−遷移金属合金が多く用いられている。将来的な高密
度化の要求に対しては、レーザ光源が短波長になるほど
光束を絞り込むことができ、したがって、より微小なピ
ットの書き込みが可能となるため、室温で安定して発振
する短波長の高出力青色レーザ光源の研究が盛んに行わ
れている。また、上述の希土類−遷移金属合金系の材料
では、レーザ光が短波長になると磁気光学効果が低下し
てしまうため、青〜緑色の短波長領域で磁気光学効果が
大きいPt/Co積層膜が、将来的な高密度光磁気記録
用の記録磁性層として研究されている。
The wavelength of the currently used laser beam for magneto-optical recording is mainly 780 nm infrared light. Further, a rare earth-transition metal alloy represented by a TbFeCo film, which has a large magneto-optical effect (Kerr effect) near the infrared wavelength, is often used for the recording magnetic layer. In order to meet the demand for higher density in the future, the shorter the wavelength of the laser light source, the more the light flux can be narrowed down. Therefore, it becomes possible to write smaller pits. Research on high-power blue laser light source of AK has been actively conducted. Further, in the above rare earth-transition metal alloy-based material, the magneto-optical effect is deteriorated when the laser light has a short wavelength. Therefore, a Pt / Co laminated film having a large magneto-optical effect in the blue to green short wavelength region is formed. , Is being studied as a recording magnetic layer for future high-density magneto-optical recording.

【0004】希土類系の記録磁性層や、Pt/Co積層
膜の記録磁性層では、いずれの場合も、基板と記録磁性
層の間に下地誘電体層を設けて、キャリアレベルを向上
させたり、光の干渉効果を利用して或る特定波長での磁
気光学効果を増大させたりしている。従来、この下地誘
電体層の成膜後であって記録磁性層の成膜前に、下地誘
電体層表面を逆スパッタして、表面を平滑化している。
これを、エッチング処理という。特に、Pt/Co積層
膜では、エッチング処理を施した場合と、施さない場合
とで、垂直磁気異方性や、磁化特性に、大きな変化が生
じている。例えば、光磁気記録媒体では、膜面垂直方向
が磁化容易軸となる垂直磁化膜になっていることが要求
されるのであるが、エッチング処理を施さなかった場合
には完全な垂直磁化膜にならなかったものでも、エッチ
ング処理を施すことで100%の角形比を持つ完全な垂
直磁化膜となることが判っている。
In either case of the rare earth-based recording magnetic layer or the Pt / Co laminated film recording magnetic layer, a base dielectric layer is provided between the substrate and the recording magnetic layer to improve the carrier level. The magneto-optical effect at a certain specific wavelength is increased by utilizing the interference effect of light. Conventionally, after the underlying dielectric layer is formed and before the recording magnetic layer is formed, the underlying dielectric layer surface is reverse-sputtered to smooth the surface.
This is called an etching process. In particular, in the Pt / Co laminated film, there is a large change in the perpendicular magnetic anisotropy and the magnetization characteristic between when the etching process is performed and when it is not performed. For example, in a magneto-optical recording medium, it is required that the perpendicular direction to the film surface is a perpendicular magnetization film whose easy axis is the axis of magnetization. It has been found that even if there is no such film, a completely perpendicular magnetization film having a squareness ratio of 100% can be obtained by performing the etching process.

【0005】スパッタリング法による従来の成膜方法を
図2に基づいて説明する。図2において、1はRFマグ
ネトロンスパッタ装置のチャンバー、2は不図示の基板
を下面側に取り付けるターンテーブル、3はターンテー
ブル2を回転させる回転軸、4は下地誘電体層用のSi
Nターゲット、5はCoターゲット、6はPtターゲッ
ト、7は放電プラズマである。まず、ターンテーブル2
を回転させながら、図2の(a)の如くSiNターゲッ
ト4とチャンバー1の間に高周波電界を印加してSiN
ターゲット4をプラズマ放電させてターンテーブル2の
下面側の基板表面にSiN層(下地誘電体層)を成膜
し、次に、図2の(b)の如くチャンバー1とターンテ
ーブル(=基板)2との間に高周波電界を印加してター
ンテーブル2の付近でプラズマ放電を行って上記SiN
層にエッチング処理を施し、その後、図2の(c)の如
くPtターゲット6とチャンバー1及びCoターゲット
5とチャンバー1の間に高周波電界を印加してPtター
ゲット6とCoターゲット5をプラズマ放電させて上記
SiN層の上に交互にPt層とCo層を積層する。この
ようにして、下地誘電体層と記録磁性層が成膜される。
A conventional film forming method by sputtering will be described with reference to FIG. In FIG. 2, 1 is a chamber of an RF magnetron sputtering apparatus, 2 is a turntable for mounting a substrate (not shown) on the lower surface side, 3 is a rotary shaft for rotating the turntable 2, and 4 is Si for an underlying dielectric layer.
N target, 5 Co target, 6 Pt target, and 7 discharge plasma. First, turntable 2
While rotating the SiN, a high frequency electric field is applied between the SiN target 4 and the chamber 1 as shown in FIG.
The target 4 is plasma-discharged to form a SiN layer (base dielectric layer) on the substrate surface on the lower surface side of the turntable 2, and then the chamber 1 and the turntable (= substrate) as shown in FIG. 2B. A high-frequency electric field is applied between the SiN and
The layer is subjected to an etching treatment, and then a high frequency electric field is applied between the Pt target 6 and the chamber 1 and the Co target 5 and the chamber 1 as shown in FIG. 2C to plasma discharge the Pt target 6 and the Co target 5. Then, Pt layers and Co layers are alternately laminated on the SiN layer. In this way, the underlying dielectric layer and the recording magnetic layer are formed.

【0006】[0006]

【発明が解決しようとする課題】上述の従来の成膜方法
では、下地誘電体層の成膜工程と記録磁性層の成膜工程
との間に、エッチング処理のための時間が必要であるた
め、成膜時間が長時間化し、コストダウンの障害になっ
ていた。本発明は、スパッタリング法による磁気記録媒
体の成膜方法において、成膜時間を短縮して製造コスト
を低減することを目的とする。
In the above-mentioned conventional film forming method, it takes time for the etching process between the step of forming the underlying dielectric layer and the step of forming the recording magnetic layer. However, the film formation time is prolonged, which is an obstacle to cost reduction. It is an object of the present invention to shorten the film forming time and reduce the manufacturing cost in the film forming method of a magnetic recording medium by the sputtering method.

【0007】[0007]

【課題を解決するための手段】本発明は、スパッタリン
グ法により基板表面に下地誘電体層を成膜した後、該下
地誘電体層の上に記録磁性層を成膜する成膜方法に於い
て、前記下地誘電体層の成膜時にエッチング処理を施す
ことを特徴とする成膜方法である。また、本発明は、チ
ャンバー内に基板とターゲットを対向させて配置し、前
記チャンバーと前記ターゲットの間に高周波電界を印加
するスパッタリング法により、前記基板表面に下地誘電
体層を成膜した後、該下地誘電体層の上に記録磁性層を
成膜する成膜方法に於いて、前記下地誘電体層の成膜時
に、前記ターンテーブルと前記チャンバーの間に高周波
電界を印加することにより前記下地誘電体層にエッチン
グ処理を施すことを特徴とする成膜方法である。上記エ
ッチング処理を、前記下地誘電体層の成膜開始後、所定
時間経過後に開始するようにしてもよい。また、上記基
板と上記チャンバーの間に印加する高周波電界を、所定
の周期でオン/オフさせるようにしてもよい。
The present invention relates to a film forming method for forming a base dielectric layer on a surface of a substrate by a sputtering method and then forming a recording magnetic layer on the base dielectric layer. The film forming method is characterized in that an etching process is performed at the time of forming the underlying dielectric layer. Further, the present invention, the substrate and the target are arranged in the chamber so as to face each other, by a sputtering method of applying a high frequency electric field between the chamber and the target, after forming a base dielectric layer on the substrate surface, In a film forming method for forming a recording magnetic layer on the underlying dielectric layer, the underlying layer is formed by applying a high frequency electric field between the turntable and the chamber when forming the underlying dielectric layer. The film forming method is characterized in that the dielectric layer is subjected to etching treatment. The etching process may be started after a lapse of a predetermined time from the start of forming the underlying dielectric layer. Further, the high frequency electric field applied between the substrate and the chamber may be turned on / off at a predetermined cycle.

【0008】[0008]

【作用】チャンバーと誘電体ターゲットの間に高周波電
界を印加するスパッタリング法により基板上に下地誘電
体層が成膜され、同時に、ターンテーブル(=基板)と
チャンバーの間に高周波電界を印加するエッチング処理
が成膜中の下地誘電体層に施される。その後、チャンバ
ーと記録磁性体ターゲットの間に高周波電界を印加する
スパッタリング法により下地誘電体層の上に記録磁性層
が成膜される。
Function: An underlying dielectric layer is formed on a substrate by a sputtering method in which a high frequency electric field is applied between a chamber and a dielectric target, and at the same time, an etching is performed in which a high frequency electric field is applied between the turntable (= substrate) and the chamber. Treatment is applied to the underlying dielectric layer being deposited. After that, a recording magnetic layer is formed on the underlying dielectric layer by a sputtering method in which a high frequency electric field is applied between the chamber and the recording magnetic target.

【0009】[0009]

【実施例】以下、本発明の一実施例を説明する。図1は
実施例の成膜方法を示す説明図、図3は実施例方法で成
膜された光磁気ディスクの断面構造を示す模式図、図4
は実施例の成膜方法を用いて作製した光磁気ディスクの
カーループを示す特性図、図5は従来の成膜方法を用い
て作製した光磁気ディスクのカーループを示す特性図で
ある。
EXAMPLE An example of the present invention will be described below. FIG. 1 is an explanatory view showing a film forming method of the embodiment, FIG. 3 is a schematic view showing a sectional structure of a magneto-optical disk formed by the embodiment method, and FIG.
5 is a characteristic diagram showing a Kerr loop of a magneto-optical disk manufactured by using the film forming method of the embodiment, and FIG. 5 is a characteristic diagram showing a Kerr loop of a magneto-optical disk manufactured by using a conventional film forming method.

【0010】図1において、1はRF2極マグネトロン
スパッタ装置のチャンバー、2は基板を下面側に取り付
けるためのターンテーブル、3はターンテーブル2を回
転させる回転軸、4は下地誘電体層用のSiNターゲッ
ト、5はCoターゲット、6はPtターゲット、7は放
電プラズマである。ここで、SiNターゲット4とCo
ターゲット5とPtターゲット6は、直径5インチであ
る。また、チャンバー1の到達真空度は1×10-6To
rr以下、成膜中のArガス流量は56SCCM、Ar
圧は7.5mTorrである。また、図3において、1
8は基板、17は基板18上に形成されたSiN層(下
地誘電体層)、15はPt層、16はCo層であり、S
iN層の膜厚は800Å、Pt層15とCo層16の各
膜厚は各々7Åと4Åである。
In FIG. 1, 1 is a chamber of an RF bipolar magnetron sputtering apparatus, 2 is a turntable for mounting a substrate on the lower surface side, 3 is a rotary shaft for rotating the turntable 2, and 4 is SiN for an underlying dielectric layer. Target 5 is a Co target, 6 is a Pt target, and 7 is discharge plasma. Here, SiN target 4 and Co
The target 5 and the Pt target 6 have a diameter of 5 inches. The ultimate vacuum of the chamber 1 is 1 × 10 -6 To
rr or less, the Ar gas flow rate during film formation is 56 SCCM, Ar
The pressure is 7.5 mTorr. In addition, in FIG.
8 is a substrate, 17 is a SiN layer (underlying dielectric layer) formed on the substrate 18, 15 is a Pt layer, 16 is a Co layer, S
The film thickness of the iN layer is 800Å, and the film thicknesses of the Pt layer 15 and the Co layer 16 are 7Å and 4Å, respectively.

【0011】*実施例試料の製造 次のようにして成膜処理とエッチング処理を行った。ま
ず、基板を取り付けたターンテーブル2を回転させなが
ら、図1の(a)の如くSiNターゲット4とチャンバ
ー1の間に投入電力600Wで高周波電界を20分間印
加してSiNターゲット4をプラズマ放電させてターン
テーブル2の下面側の基板表面にSiN層(下地誘電体
層)を成膜した。
* Manufacture of Example Samples A film forming process and an etching process were performed as follows. First, while rotating the turntable 2 having the substrate attached thereto, a high frequency electric field was applied between the SiN target 4 and the chamber 1 at an applied power of 600 W for 20 minutes as shown in FIG. Then, a SiN layer (underlying dielectric layer) was formed on the substrate surface on the lower surface side of the turntable 2.

【0012】次に、基板を取り付けたターンテーブル2
を回転させながら、図1の(b)の如くSiNターゲッ
ト4とチャンバー1の間に投入電力600Wで高周波電
界を15分間印加してSiNターゲット4をプラズマ放
電させてターンテーブル2の下面側の基板表面にSiN
層(下地誘電体層)を成膜しつつ、同時に、チャンバー
1とターンテーブル(=基板)2との間に投入電力20
0Wで高周波電界を15分間印加してターンテーブル2
の付近でプラズマ放電を行って上記SiN層にエッチン
グ処理を施した。
Next, the turntable 2 with the substrate attached
As shown in FIG. 1B, a high frequency electric field is applied between the SiN target 4 and the chamber 1 at a power of 600 W for 15 minutes while rotating the SiN target 4 to plasma-discharge the SiN target 4 and the substrate on the lower surface of the turntable 2. SiN on the surface
While depositing a layer (underlying dielectric layer), an electric power of 20 is applied between the chamber 1 and the turntable (= substrate) 2 at the same time.
Apply high frequency electric field for 15 minutes at 0 W and turntable 2
Plasma discharge was performed in the vicinity of to etch the SiN layer.

【0013】次に、基板を取り付けたターンテーブル2
を回転させながら、図1の(c)の如くPtターゲット
6とチャンバー1及びCoターゲット5とチャンバー1
の間に投入電力100Wで高周波電界を印加してPtタ
ーゲット6とCoターゲット5をプラズマ放電させて上
記SiN層の上にPt層とCo層を交互に15層積層し
て記録磁性層を成膜した。このようにして、図3の構造
の光磁気ディスクを得た。
Next, the turntable 2 with the substrate attached
While rotating, the Pt target 6 and the chamber 1 and the Co target 5 and the chamber 1 as shown in FIG.
A high frequency electric field is applied with an applied power of 100 W between them to plasma discharge the Pt target 6 and the Co target 5 to alternately form 15 layers of Pt layers and Co layers on the SiN layer to form a recording magnetic layer. did. In this way, a magneto-optical disk having the structure shown in FIG. 3 was obtained.

【0014】*実施例試料と従来例試料の特性比較 上述の方法で製造した実施例試料と、従来の方法で製造
した従来例試料の特性を下記のように比較した。ここ
で、従来例試料とは、投入電力600WでのSiN層
(下地誘電体層)の成膜のみを35分間行った後、投入
電力200Wでのエッチング処理のみを15分間行うこ
とで製造した光磁気ディスクであり、記録磁性層の成膜
は上述の実施例試料と同じ方法で行った試料である。
* Comparison of Characteristics between Example Sample and Conventional Example Sample The characteristics of the example sample manufactured by the above method and the conventional example sample manufactured by the conventional method were compared as follows. Here, the conventional sample is a light produced by performing only film formation of the SiN layer (underlying dielectric layer) at an applied power of 600 W for 35 minutes and then performing only an etching process at an applied power of 200 W for 15 minutes. This is a magnetic disk, and the recording magnetic layer is formed by the same method as the above-described example samples.

【0015】図4は波長780nmのレーザ光で測定し
た実施例試料のカーループ、図5は実施例試料と同じ条
件で測定した従来例試料のカーループである。カールー
プの大きさや、ループの保磁力、角形性等の特性は、光
磁気ディスクの記録・再生特性に大きく影響するもので
あるが、図4と図5の比較から明らかなように、両者の
カー回転角は0.84deg、保磁力は1.2kOe程
度であり、略同じ特性を示している。また角形性も良好
である。
FIG. 4 shows the Kerr loop of the example sample measured with a laser beam having a wavelength of 780 nm, and FIG. 5 shows the Kerr loop of the conventional example sample measured under the same conditions as the example sample. The characteristics such as the size of the Kerr loop, the coercive force of the loop, and the squareness have a great influence on the recording / reproducing characteristics of the magneto-optical disk, but as is clear from the comparison between FIG. 4 and FIG. The rotation angle is 0.84 deg and the coercive force is about 1.2 kOe, showing almost the same characteristics. It also has good squareness.

【0016】次に、実施例試料と従来例試料の各光磁気
ディスクについて、各々光変調記録方式での書き込みレ
ーザパワー対CNR(carrier to noise ratio)特性を
測定した。光磁気ディスクの回転数を1800rpmと
し、ディスク半径40mmの位置に波長830nmのレ
ーザ光を用いてデューティ比50%で1MHzの周波数
信号を記録した。記録ピット長は約3.7μmである。
記録時の外部印加磁界は200Oeとし、レーザパワー
は2mWから10mWまで2mW刻みで変化させた。こ
のように記録した信号を、レーザパワー1mWで読み出
したところ、CNRは、実施例試料と従来例試料の各光
磁気ディスクとも、略同等の特性を示した。例えば、書
き込みレーザパワー6mWのとき、実施例試料の光磁気
ディスクで50.6dB、従来例試料の光磁気ディスク
で50.4dBであった。以上の結果から、実施例試料
の光磁気ディスクと従来例試料の光磁気ディスクは、同
等の特性を有していることが判る。
Next, the write laser power vs. CNR (carrier to noise ratio) characteristics in the optical modulation recording method were measured for each of the magneto-optical disks of the example sample and the conventional example sample. A rotation frequency of the magneto-optical disk was set to 1800 rpm, and a frequency signal of 1 MHz was recorded at a disk radius of 40 mm using a laser beam having a wavelength of 830 nm and a duty ratio of 50%. The recording pit length is about 3.7 μm.
The externally applied magnetic field at the time of recording was 200 Oe, and the laser power was changed from 2 mW to 10 mW in steps of 2 mW. When the signal thus recorded was read out with a laser power of 1 mW, the CNR exhibited substantially the same characteristics in each of the magneto-optical disks of the example sample and the conventional example sample. For example, when the writing laser power was 6 mW, the magneto-optical disk of the example sample had a gain of 50.6 dB, and the magneto-optical disk of the conventional sample had a gain of 50.4 dB. From the above results, it can be seen that the magneto-optical disk of the example sample and the magneto-optical disk of the conventional sample have the same characteristics.

【0017】上記実施例では、下地誘電体層の35分間
の成膜処理の中の最終部分の15分間に、エッチング処
理を並行して行っているが、エッチング処理を同時に行
う時間は上記実施例に限定されない。また、並行して行
うエッチング処理及び/又は下地誘電体層の成膜処理を
周期的にオン/オフさせてもよい。また、例えば、ター
ンテーブルに複数の基板が取り付けられており、下地誘
電体層を成膜中である基板と、成膜中でない基板とが、
周期的(ターンテーブルの1回転ごと)に存在している
場合には、成膜中でない基板のみに周期的に繰り返して
エッチング処理を施すようにしてもよい。また、本発明
は、光磁気ディスクばかりでなく、スパッタリング法に
よる磁気記録媒体の成膜方法に適用可能である。
In the above embodiment, the etching process is performed in parallel during the final 15 minutes of the film formation process of the base dielectric layer for 35 minutes. Not limited to. Further, the etching process and / or the film forming process of the underlying dielectric layer performed in parallel may be periodically turned on / off. Further, for example, a plurality of substrates are attached to the turntable, and a substrate on which the underlying dielectric layer is being formed and a substrate on which the underlying dielectric layer is not being formed are
When they exist periodically (every time the turntable rotates), the etching treatment may be repeated cyclically only on the substrate that is not being film-formed. Further, the present invention can be applied not only to a magneto-optical disk but also to a film forming method for a magnetic recording medium by a sputtering method.

【0018】[0018]

【発明の効果】本発明では、下地誘電体層のエッチング
処理が下地誘電体層の成膜と同時に並行して行われるた
め、成膜所要時間を短縮化でき、したがって、記録媒体
の製造コストを低減できる。また、このようにして成膜
した記録媒体の特性は、従来の方法で成膜した記録媒体
の特性と比較して、遜色が無い。
According to the present invention, since the etching process of the underlying dielectric layer is performed concurrently with the film formation of the underlying dielectric layer, the time required for the film formation can be shortened, and therefore the manufacturing cost of the recording medium can be reduced. It can be reduced. Further, the characteristics of the recording medium thus formed are comparable to those of the recording medium formed by the conventional method.

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

【図1】実施例の成膜方法を示す説明図。FIG. 1 is an explanatory view showing a film forming method of an example.

【図2】従来の成膜方法を示す説明図。FIG. 2 is an explanatory view showing a conventional film forming method.

【図3】実施例方法で成膜された光磁気ディスクの断面
構造を示す模式図。
FIG. 3 is a schematic diagram showing a cross-sectional structure of a magneto-optical disk formed by an example method.

【図4】実施例方法を用いて作製した光磁気ディスクの
カーループを示す特性図。
FIG. 4 is a characteristic diagram showing a Kerr loop of a magneto-optical disk manufactured by using an example method.

【図5】従来の方法を用いて作製した光磁気ディスクの
カーループを示す特性図。
FIG. 5 is a characteristic diagram showing a Kerr loop of a magneto-optical disk manufactured by a conventional method.

【符号の説明】[Explanation of symbols]

1 チャンバー 2 ターンテーブル 3 回転軸 4 SiNターゲット 5 Coターゲット 6 Ptターゲット 7 放電プラズマ 1 chamber 2 turntable 3 rotating shaft 4 SiN target 5 Co target 6 Pt target 7 discharge plasma

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 スパッタリング法により基板表面に下地
誘電体層を成膜した後、該下地誘電体層の上に記録磁性
層を成膜する成膜方法に於いて、 前記下地誘電体層の成膜時に該下地誘電体層にエッチン
グ処理を施すことを特徴とする成膜方法。
1. A method for forming a base magnetic layer on a surface of a substrate by a sputtering method, and then forming a recording magnetic layer on the base dielectric layer, the method comprising forming the base dielectric layer. A film forming method, characterized in that the underlying dielectric layer is subjected to etching treatment during film formation.
【請求項2】 チャンバー内に基板とターゲットを対向
させて配置し、前記チャンバーと前記ターゲットの間に
高周波電界を印加するスパッタリング法により、前記基
板表面に下地誘電体層を成膜した後、該下地誘電体層の
上に記録磁性層を成膜する成膜方法に於いて、 前記下地誘電体層の成膜時に、前記基板と前記チャンバ
ーの間に高周波電界を印加するエッチング処理を施すこ
とを特徴とする成膜方法。
2. A substrate and a target are arranged to face each other in a chamber, and a base dielectric layer is formed on the surface of the substrate by a sputtering method in which a high frequency electric field is applied between the chamber and the target, In a film forming method for forming a recording magnetic layer on a base dielectric layer, an etching process for applying a high frequency electric field between the substrate and the chamber is performed at the time of forming the base dielectric layer. Characteristic film forming method.
【請求項3】 請求項2に於いて、 前記エッチング処理を、前記下地誘電体層の成膜開始
後、所定時間経過後に開始することを特徴とする成膜方
法。
3. The film forming method according to claim 2, wherein the etching process is started after a lapse of a predetermined time after the film formation of the underlying dielectric layer is started.
【請求項4】 請求項2、又は、請求項3に於いて、 前記基板と前記チャンバーの間に印加する高周波電界
を、所定の周期でオン/オフさせることを特徴とする成
膜方法。
4. The film forming method according to claim 2, wherein the high frequency electric field applied between the substrate and the chamber is turned on / off at a predetermined cycle.
JP20273894A 1994-08-03 1994-08-03 Film forming method Pending JPH0845126A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20273894A JPH0845126A (en) 1994-08-03 1994-08-03 Film forming method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20273894A JPH0845126A (en) 1994-08-03 1994-08-03 Film forming method

Publications (1)

Publication Number Publication Date
JPH0845126A true JPH0845126A (en) 1996-02-16

Family

ID=16462351

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20273894A Pending JPH0845126A (en) 1994-08-03 1994-08-03 Film forming method

Country Status (1)

Country Link
JP (1) JPH0845126A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5875169A (en) * 1997-06-12 1999-02-23 Eastman Kodak Company Magneto-optic data storage device having multiple data storage levels

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5875169A (en) * 1997-06-12 1999-02-23 Eastman Kodak Company Magneto-optic data storage device having multiple data storage levels

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