JPH0572015B2 - - Google Patents
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- Publication number
- JPH0572015B2 JPH0572015B2 JP63308264A JP30826488A JPH0572015B2 JP H0572015 B2 JPH0572015 B2 JP H0572015B2 JP 63308264 A JP63308264 A JP 63308264A JP 30826488 A JP30826488 A JP 30826488A JP H0572015 B2 JPH0572015 B2 JP H0572015B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- thin film
- substrate
- sputtering
- coercive force
- Prior art date
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- Manufacturing Of Magnetic Record Carriers (AREA)
Description
[産業上の利用分野]
本発明は磁気記録媒体の製造法に係り、詳しく
は、高い保磁力を有する磁気記録媒体を製造する
方法に関するものである。
[従来の技術]
近年、コンピユータ等の情報処理技術の発達に
伴い、その外部記憶装置に用いられる磁気デイス
クなどの磁気記録媒体に対し、高密度記録化への
要求がますます高められている。
現在、長手記録用磁気デイスクに用いられる磁
気記録媒体の磁性層としては、スパツタリング等
によりCr下地薄膜上に、エピタキシヤル的に成
膜されたCo系合金薄膜が主流となつてきている。
しかして、このCo系合金薄膜磁性層についても、
高密度記録化への要求に対し、磁気特性としてよ
り高い保磁力を付与することが必要とされてお
り、従来より、その特性についての報告が、数多
くなされている。(例えば、“New longitudinal
recording media Cox Niy Crz from high
rate static magnetron sputter−ingsystem”
IEEE Trans.Magn.Mag−22,No5,(1986),
334;特開昭63−79233号公報;特開昭63−79968
号公報。)
[発明が解決しようとする課題]
従来報告されているように、Co系合金薄膜磁
性層の保磁力は、Cr下地薄膜の膜厚とともに増
大する。しかしながら、ある上限値を超えると飽
和特性を示し、それ以上の高保磁力化は困難であ
る。例えば、特開昭63−79968号公報には、Cr下
地層薄膜の膜厚が1500Å以上では磁性層の保磁力
がそれ以上上昇しない飽和傾向が認められ、それ
以下では磁性層の保磁力が著しく低下し、実用上
問題があることが示されている。
また、この保磁力は、Co系合金薄膜の膜厚の
低減により増加する。しかしながら、膜厚の低減
は再生出力値の低下につながるため、実用上、所
定の膜厚以下に薄くすることは困難である。更
に、磁性層の成膜時における成膜ガス圧力、基板
温度などのスパツタ条件の選択により、ある程度
の保磁力の向上は可能であるが、その向上効果は
小さいものである。
本発明は上記従来の問題点を解決し、著しく高
い保磁力を有する磁気記録媒体を製造する方法を
提供することを目的とする。
[課題を解決するための手段]
本発明の磁気記録媒体の製造方法は、基板上に
クロム下地層薄膜及びコバルト系合金磁性薄膜を
順次スパツタリングによつて形成する磁気記録媒
体の製造方法において、基板上にクロム下地層薄
膜を10〜1200Åの膜厚で形成させた後、基板側に
負のバイアス電圧を印加した状態でコバルト
(Co)を主成分とし、クロム(Cr)及びタンタル
(Ta)を含むコバルト系合金磁性薄膜を形成する
ことを特徴とする。
即ち、本発明者等は上記従来の状況に鑑み、
Cr下地層薄膜の膜厚が1200Å以下の薄膜におい
ても磁気記録媒体の保磁力を高いレベルに維持さ
せるべく鋭意検討を重ねた結果、基板上にCr下
地層薄膜を1200Å以下の膜厚で形成させ、次いで
Co,Cr及びTaからなる磁性層薄膜を特定の条件
下でスパツタリングさせて形成させることによ
り、磁気記録媒体の保磁力が高いレベルに維持さ
れることを見出し、本発明を完成するに至つた。
以下、本発明につき詳細に説明する。
本発明に用いられる基板としては、一般にアル
ミニウム又はアルミニウム合金のデイスク状基板
が用いられ、通常、アルミニウム基板を所定の厚
さに加工した後、その表面を鏡面加工したもの
に、第1次下地層として硬質非磁性金属、例えば
Ni−P合金を無電解メツキ或いは陽極酸化処理
により形成し、しかる後、第2次下地層として
Crをスパツタリングしたものが用いられる。基
板3としては、上記第1次下地層を形成せずに、
鏡面加工したアルミニウム基板上に直接下地層と
してCrをスパツタリングしたものを用いること
もできる。
本発明において、Cr下地層の膜厚は10〜1200
Å、好ましくは50〜1000Å、更に好ましくは100
〜400Åの範囲とする。上記膜厚が10Å未満では
磁性層の保磁力が著しく低下し、また1200Åより
厚くしても磁性層の保持力はそれ以上増加せず、
逆にコストアツプにつながるので好ましくない。
Cr下地層を形成するスパツタリング条件とし
ては特に制限はなく、通常のCr下地層を形成す
る際に採用されるスパツタリング条件及び後述す
る磁性層薄膜を形成するスパツタリング条件等を
採用することができる。
本発明においては、このような所定厚さのCr
下地層を基板上に形成させた後、Coを主成分と
し、Cr及びTaを含むCo系合金磁性薄膜を特定条
件にてスパツタリングにより形成させる。
以下にこの磁性薄膜の形成方法につき、図面を
参照して詳細に説明する。
第1図は本発明の実施に好適なスパツタリング
装置の一例を示す概略構成図である。図中、1は
ターゲツトであり、これに対向した位置に基板ホ
ルダー2が設けられており、基板ホルダー2には
基板3が装着されている。基板ホルダー2は基板
3を連続的に成膜できるように移動可能とされて
いる。4はターゲツト1に接続されるスパツタリ
ング用電源である。5は基板ホルダー2に負のバ
イアス電圧を印加させるためのバイアス電源であ
る。
これらスパツタリング用電源4及びバイアス電
源5としては直流電源が好ましいが、RF電源も
使用できる。スパツタ装置としては、通常のDC
マグネトロンスパツタ装置又はRFマグネトロン
スパツタ装置等が採用される。
ターゲツト1としては、Coを主成分とし、Cr
及びTaからなる合金が用いられる。このCo−Cr
−Ta合金としては、Co:70〜95原子%、Cr:
520原子%及びTa:0.1〜10原子%の組成のもの
が好適である。
第1図に示すスパツタリング装置を用いて、本
発明の方法に従つて、磁気記録媒体を製造するに
は、まず、前述のCr下地層を形成した基板3を
装置の基板ホルダー2に取り付け、前記Co−Cr
−Ta合金のターゲツト2を用いて、アルゴン等
の希ガスの存在下でスパツタリングを行なうが、
この際、基板ホルダー2には負のバイアス電圧を
印加した状態、即ち、バイアス電源5により基板
ホルダー2に例えば−1000V以上、好ましくは−
50〜−500V、更に好ましくは−100〜−400Vの
電圧を印加した状態でスパツタリングを行ない、
基板3上にCo,Cr及びTaからなる磁性薄膜を形
成する。
本発明において、スパツタリング条件として
は、通常、磁気記録媒体の磁性層を形成させる際
に採用される条件を採用することができる。例え
ば、真空排気したチヤンバー内圧力を1×10-6
Torr以下、Ar等の希ガス圧力を0.5×10-3〜2×
10-2Torr、望ましくは1×10-3〜5×10-3Torr
の範囲で、基板温度を150℃以上、望ましくは200
〜300℃の範囲の条件下でスパツタリングを実施
することができる。
このようなスパツタリングにより形成する磁性
薄膜層の膜厚は、残留磁性密度(Br)と磁性薄
膜層の膜厚(t)との積(Br・t)が300〜
700G・μmとなるような膜厚とするのが好まし
い。
[作用]
膜厚10〜1200Åの膜厚のCr下地層を介して、
基板側に負のバイアス電圧を印加した状態でスパ
ツタリングにより形成されたCo−Cr−Ta系1合
金磁性薄膜層により、高い保磁力を有する高特性
磁性層が形成される。
[実施例]
以下に実施例及び比較例を挙げて本発明をより
具体的に説明するが、本発明はその要旨を超えな
い限り、以下の実施例に限定されるものではな
い。
実施例 1〜4、参考例 1〜2、比較例 1〜
5
第1図に示す装置を用い、下地層として第1表
に示す膜厚のCr薄膜をスパツタリングにより形
成したアルミニウム基板3及び、Co−Cr−Ta合
金ターゲツト1を用いて、バイアス電源4に第1
表に示す電圧を印加した状態で、チヤンバー内到
達圧力1×10-6Torr以下、アルゴン圧力2×
10-3Torr、基板温度250℃の条件下でスパツタリ
ングを行ない、基板上に86原子%Co−12原子%
Cr−2原子%Ta磁性層(550G・μm)を形成し
た。
得られた磁気デイスクの保磁力を試料振動型磁
力計で測定し、結果を第1表に示した。
比較例 6〜14
実施例1において、Co−Cr−Ta合金ターゲツ
トに代えてCo−Ni−Cr合金ターゲツトを用い、
第1表に示す電圧にて基板上に70原子%Co−20
原子%Ni−10原子%Cr磁性層550G・μm)を形
成させたこと以外は同様にして磁気デイスクを
得、その保磁力測定結果を第1表に示した。
[Industrial Field of Application] The present invention relates to a method of manufacturing a magnetic recording medium, and more particularly, to a method of manufacturing a magnetic recording medium having a high coercive force. [Background Art] In recent years, with the development of information processing technology for computers and the like, there has been an increasing demand for high-density recording in magnetic recording media such as magnetic disks used in external storage devices. Currently, Co-based alloy thin films epitaxially formed on Cr underlayer thin films by sputtering or the like are becoming mainstream as magnetic layers of magnetic recording media used in longitudinal recording magnetic disks.
However, regarding this Co-based alloy thin film magnetic layer,
In response to the demand for high-density recording, it is necessary to provide magnetic properties with higher coercive force, and there have been many reports regarding this property. (For example, “New longitudinal
recording media Co x Ni y Cr z from high
rate static magnetron sputter−ing system”
IEEE Trans.Magn.Mag−22, No5, (1986),
334; JP-A-63-79233; JP-A-63-79968
Publication No. ) [Problems to be Solved by the Invention] As previously reported, the coercive force of a Co-based alloy thin film magnetic layer increases with the thickness of the Cr underlayer thin film. However, when a certain upper limit is exceeded, saturation characteristics are exhibited, and it is difficult to increase the coercive force further. For example, in Japanese Patent Application Laid-open No. 63-79968, it is recognized that when the thickness of the Cr underlayer thin film is 1500 Å or more, the coercive force of the magnetic layer tends to saturate and the coercive force of the magnetic layer does not increase any further. It has been shown that there is a problem in practical use. Moreover, this coercive force increases as the thickness of the Co-based alloy thin film is reduced. However, since reducing the film thickness leads to a decrease in the reproduction output value, it is practically difficult to reduce the film thickness to a predetermined thickness or less. Furthermore, although it is possible to improve the coercive force to some extent by selecting sputtering conditions such as the film forming gas pressure and substrate temperature during film formation of the magnetic layer, the improvement effect is small. SUMMARY OF THE INVENTION An object of the present invention is to solve the above-mentioned conventional problems and provide a method for manufacturing a magnetic recording medium having an extremely high coercive force. [Means for Solving the Problems] The method for manufacturing a magnetic recording medium of the present invention is a method for manufacturing a magnetic recording medium in which a chromium underlayer thin film and a cobalt-based alloy magnetic thin film are sequentially formed on a substrate by sputtering. After forming a thin film of chromium underlayer with a thickness of 10 to 1200 Å on top, a film containing cobalt (Co) as the main component, chromium (Cr) and tantalum (Ta) is coated with a negative bias voltage applied to the substrate side. It is characterized by forming a magnetic thin film containing a cobalt-based alloy. That is, in view of the above-mentioned conventional situation, the present inventors have
As a result of intensive studies to maintain the coercive force of the magnetic recording medium at a high level even when the thickness of the Cr underlayer is 1200 Å or less, we have developed a method to form a Cr underlayer thin film on the substrate with a thickness of 1200 Å or less. , then
The present inventors have discovered that the coercive force of a magnetic recording medium can be maintained at a high level by sputtering and forming a thin magnetic layer consisting of Co, Cr, and Ta under specific conditions, leading to the completion of the present invention. Hereinafter, the present invention will be explained in detail. The substrate used in the present invention is generally a disc-shaped substrate made of aluminum or an aluminum alloy. Usually, after processing the aluminum substrate to a predetermined thickness, the surface of the aluminum substrate is mirror-finished, and then a first base layer is applied. as hard non-magnetic metals, e.g.
Ni-P alloy is formed by electroless plating or anodic oxidation treatment, and then used as a second base layer.
Sputtered Cr is used. As the substrate 3, without forming the above-mentioned first base layer,
It is also possible to use a material in which Cr is sputtered directly onto a mirror-finished aluminum substrate as an underlayer. In the present invention, the film thickness of the Cr underlayer is 10 to 1200
Å, preferably 50 to 1000 Å, more preferably 100
~400Å range. If the film thickness is less than 10 Å, the coercive force of the magnetic layer will decrease significantly, and if it is thicker than 1200 Å, the coercive force of the magnetic layer will not increase any further.
On the contrary, this is not desirable because it leads to an increase in costs. There are no particular restrictions on the sputtering conditions for forming the Cr underlayer, and the sputtering conditions employed when forming a normal Cr underlayer, the sputtering conditions for forming a magnetic layer thin film, etc., which will be described later, can be adopted. In the present invention, such a predetermined thickness of Cr
After forming the underlayer on the substrate, a Co-based alloy magnetic thin film containing Co as a main component and Cr and Ta is formed by sputtering under specific conditions. The method for forming this magnetic thin film will be described in detail below with reference to the drawings. FIG. 1 is a schematic diagram showing an example of a sputtering apparatus suitable for implementing the present invention. In the figure, reference numeral 1 indicates a target, and a substrate holder 2 is provided at a position opposite to the target, and a substrate 3 is mounted on the substrate holder 2. The substrate holder 2 is movable so that the substrates 3 can be continuously deposited. 4 is a sputtering power source connected to the target 1. Reference numeral 5 denotes a bias power supply for applying a negative bias voltage to the substrate holder 2. As these sputtering power source 4 and bias power source 5, DC power sources are preferable, but RF power sources can also be used. As a sputtering device, ordinary DC
A magnetron sputter device or an RF magnetron sputter device is used. As target 1, the main component is Co, and Cr
An alloy consisting of Ta and Ta is used. This Co−Cr
-Ta alloy: Co: 70 to 95 atomic%, Cr:
A composition having a composition of 520 atomic % and Ta: 0.1 to 10 atomic % is preferable. In order to manufacture a magnetic recording medium according to the method of the present invention using the sputtering apparatus shown in FIG. Co−Cr
- Sputtering is performed using Ta alloy target 2 in the presence of a rare gas such as argon.
At this time, a negative bias voltage is applied to the substrate holder 2, that is, the bias power supply 5 applies a voltage of -1000 V or more to the substrate holder 2, preferably -
Perform sputtering while applying a voltage of 50 to -500V, more preferably -100 to -400V,
A magnetic thin film made of Co, Cr and Ta is formed on the substrate 3. In the present invention, as the sputtering conditions, conditions normally employed when forming a magnetic layer of a magnetic recording medium can be employed. For example, the pressure inside the evacuated chamber is 1×10 -6
Torr or less, rare gas pressure such as Ar is 0.5×10 -3 to 2×
10 -2 Torr, preferably 1×10 -3 to 5×10 -3 Torr
Keep the substrate temperature above 150°C, preferably 200°C.
Sputtering can be carried out under conditions ranging from ~300°C. The thickness of the magnetic thin film layer formed by such sputtering is such that the product (Br・t) of the residual magnetic density (Br) and the film thickness (t) of the magnetic thin film layer is 300 to 300.
It is preferable to set the film thickness to 700G·μm. [Function] Through a Cr underlayer with a thickness of 10 to 1200 Å,
A Co--Cr--Ta based 1 alloy magnetic thin film layer formed by sputtering with a negative bias voltage applied to the substrate side forms a high-performance magnetic layer having a high coercive force. [Examples] The present invention will be described in more detail with reference to Examples and Comparative Examples below, but the present invention is not limited to the following Examples unless it exceeds the gist thereof. Examples 1-4, Reference examples 1-2, Comparative examples 1-
5 Using the apparatus shown in FIG. 1, using the aluminum substrate 3 on which a Cr thin film with the thickness shown in Table 1 was formed by sputtering as an underlayer and the Co-Cr-Ta alloy target 1, a bias power source 4 was connected to the aluminum substrate 3. 1
With the voltage shown in the table applied, the ultimate pressure inside the chamber is 1 x 10 -6 Torr or less, and the argon pressure is 2 x
Sputtering was performed under conditions of 10 -3 Torr and a substrate temperature of 250°C, and 86 atomic% Co-12 atomic% was deposited on the substrate.
A Cr-2 atomic % Ta magnetic layer (550G·μm) was formed. The coercive force of the obtained magnetic disk was measured using a sample vibrating magnetometer, and the results are shown in Table 1. Comparative Examples 6 to 14 In Example 1, a Co-Ni-Cr alloy target was used instead of the Co-Cr-Ta alloy target,
70 atomic% Co-20 on the substrate at the voltage shown in Table 1.
A magnetic disk was obtained in the same manner except that a magnetic layer of 550 G.mu.m in atomic % Ni-10 atomic % Cr was formed, and the coercive force measurement results are shown in Table 1.
【表】【table】
【表】
[発明の効果]
以上詳述した通り、本発明の磁気記録媒体の製
造方法によれば、高い保磁力を有する高特性磁気
記録媒体を容易に製造することができ磁気記録媒
体のより一層の高密度記録化が可能とされる。[Table] [Effects of the Invention] As detailed above, according to the method for manufacturing a magnetic recording medium of the present invention, a high-performance magnetic recording medium having a high coercive force can be easily manufactured, and the magnetic recording medium can be improved. It is possible to achieve even higher density recording.
第1図は本発明の実施に好適なスパツタリング
装置の一例を示す概略構成図である。
1……ターゲツト、2……基板ホルダー、3…
…基板、4……スパツタリング用電源、5……バ
イアス電源。
FIG. 1 is a schematic diagram showing an example of a sputtering apparatus suitable for implementing the present invention. 1...Target, 2...Substrate holder, 3...
...Substrate, 4...Power supply for sputtering, 5...Bias power supply.
Claims (1)
金磁性薄膜を順次スパツタリングによつて形成す
る磁気記録媒体の製造方法において、基板上にク
ロム下地層薄膜を10〜1200Åの膜厚で形成させた
後、基板側に負のバイアス電圧を印加した状態で
コバルトを主成分とし、クロム及びタンタルを含
むコバルト系合金磁性薄膜を形成することを特徴
とする磁気記録媒体の製造方法。1. In a method for manufacturing a magnetic recording medium in which a chromium underlayer thin film and a cobalt-based alloy magnetic thin film are sequentially formed on a substrate by sputtering, after forming a chromium underlayer thin film on the substrate with a film thickness of 10 to 1200 Å, A method for manufacturing a magnetic recording medium, comprising forming a cobalt-based alloy magnetic thin film mainly composed of cobalt and containing chromium and tantalum while applying a negative bias voltage to a substrate side.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP30826488A JPH02154323A (en) | 1988-12-06 | 1988-12-06 | Method for manufacturing magnetic recording media |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP30826488A JPH02154323A (en) | 1988-12-06 | 1988-12-06 | Method for manufacturing magnetic recording media |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02154323A JPH02154323A (en) | 1990-06-13 |
| JPH0572015B2 true JPH0572015B2 (en) | 1993-10-08 |
Family
ID=17978919
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP30826488A Granted JPH02154323A (en) | 1988-12-06 | 1988-12-06 | Method for manufacturing magnetic recording media |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02154323A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04134718A (en) * | 1990-09-27 | 1992-05-08 | Mitsubishi Kasei Corp | Magnetic recording medium |
| JP2760906B2 (en) * | 1991-03-08 | 1998-06-04 | 日立金属株式会社 | Magnetic recording medium and method of manufacturing the same |
| JPH10228621A (en) * | 1997-02-17 | 1998-08-25 | Fujitsu Ltd | Magnetic recording medium and magnetic disk drive |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS61227231A (en) * | 1985-03-30 | 1986-10-09 | Unitika Ltd | Production of magnetic recording body |
| US4677032A (en) * | 1985-09-23 | 1987-06-30 | International Business Machines Corporation | Vertical magnetic recording media with multilayered magnetic film structure |
| JPH02161617A (en) * | 1988-03-15 | 1990-06-21 | Ulvac Corp | Production of magnetic recording medium |
-
1988
- 1988-12-06 JP JP30826488A patent/JPH02154323A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH02154323A (en) | 1990-06-13 |
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| Date | Code | Title | Description |
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| LAPS | Cancellation because of no payment of annual fees |