JPS6378341A - Production of magnetic recording medium - Google Patents

Production of magnetic recording medium

Info

Publication number
JPS6378341A
JPS6378341A JP22311086A JP22311086A JPS6378341A JP S6378341 A JPS6378341 A JP S6378341A JP 22311086 A JP22311086 A JP 22311086A JP 22311086 A JP22311086 A JP 22311086A JP S6378341 A JPS6378341 A JP S6378341A
Authority
JP
Japan
Prior art keywords
magnetic recording
magnetron
recording medium
oxygen
magnetic
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
JP22311086A
Other languages
Japanese (ja)
Inventor
Koichi Shinohara
紘一 篠原
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP22311086A priority Critical patent/JPS6378341A/en
Publication of JPS6378341A publication Critical patent/JPS6378341A/en
Pending legal-status Critical Current

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  • Manufacturing Of Magnetic Record Carriers (AREA)

Abstract

PURPOSE:To obtain a magnetic recording medium having good S/N by incorporating oxygen into an electric discharge gas at the time of disposing plural targets oppositely to a moving substrate and forming a thin ferromagnetic metallic film by sputtering vapor deposition using the magnetron discharge. CONSTITUTION:The oxygen is incorporated into the electric discharge gas at the time of disposing the plural targets 10, 11 oppositely to the moving substrate 7 and forming the thin ferromagnetic metallic film by the magnetron vapor deposition using the magnetron discharge. The space distribution of the evaporating particles generated by the magnetron discharge is thereby improved and the coercive force and noise are improved by the relieved magnetostatic coupling of the gaseous oxygen with the fine magnetic particles according to the compounding ratio thereof. The effect thereof is higher as the number of the plural targets is increased and the moving speed (productivity) is increased.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は高密度磁気記録に適する強磁性金属薄膜を磁気
記録層とする磁気記録媒体に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a magnetic recording medium whose magnetic recording layer is a ferromagnetic metal thin film suitable for high-density magnetic recording.

従来の技術 近年、磁気記録の高密度化の進歩は目覚しく、波長は1
μm以下、トラック幅は10μm近くにまで発展してき
たために、高い飽和磁束密度をもった薄膜により減磁作
用を少なくした磁気記録媒体が注目され実用化が一部は
じまっている。磁気記録層としては、Co−Cr垂直磁
化膜、Co−Ni面内磁化膜等が有望視されている。
Conventional technology In recent years, there has been remarkable progress in increasing the density of magnetic recording, and the wavelength
Since track widths have been developed to be less than .mu.m and track widths are close to 10 .mu.m, magnetic recording media in which the demagnetization effect is reduced by thin films with high saturation magnetic flux density have attracted attention, and some of them have begun to be put into practical use. As a magnetic recording layer, a Co--Cr perpendicular magnetization film, a Co--Ni in-plane magnetization film, etc. are considered promising.

Co−Cr膜、 Co −N i膜はA r r A 
r 十N2雰囲気中でスパッタすることによシ磁気記録
層を形成したシ、これらの膜を熱処理することによシ磁
気特性を制御することなどが良く知られている。(特開
昭57−72,307号公報、ジャーナルオブ アプラ
イド フィジックス (Tournal of Applied Physi
cs)第63巻第10号、6941〜6945(198
2)。
Co-Cr film and Co-Ni film are A r r A
It is well known that a magnetic recording layer is formed by sputtering in a N2 atmosphere, and that the magnetic properties are controlled by heat treating these films. (Unexamined Japanese Patent Publication No. 57-72,307, Journal of Applied Phys.
cs) Volume 63 No. 10, 6941-6945 (198
2).

特開昭61−153,827号公報) 例えば磁気ディスクを製造するのは、アルミ合金基板上
に平板マグネトロンスパッタにより、N2 :A r 
=1 : 1で全圧力を16mTorrにし、投入電力
1Kwで、 C0−30at%Niをターゲットにして
膜厚1000人形成し、340’CI時間熱処理するこ
とが一例として挙げられる。
(Japanese Unexamined Patent Publication No. 61-153,827) For example, magnetic disks are manufactured by flat plate magnetron sputtering on an aluminum alloy substrate using N2:Ar
An example of this is to set the total pressure to 16 mTorr with the ratio 1:1, to form a film with a thickness of 1000 on C0-30 at%Ni as a target, and to heat treat it for 340' CI time with an input power of 1 Kw.

発明が解決しようとする問題点 しかしながら上記した構成では、短波長出力は大きくで
きても、ノイズが太きいため、十分な信号対雑音比(以
下Sハと記す)を持った磁気記録媒体が得られないのと
、熱処理温度が高いだめ、ポリエステル等のフレキシブ
ル基板が用いられないため改良が望まれていた。
Problems to be Solved by the Invention However, with the above configuration, although the short wavelength output can be increased, the noise is large, so it is difficult to obtain a magnetic recording medium with a sufficient signal-to-noise ratio (hereinafter referred to as S). Improvements have been desired since flexible substrates such as polyester cannot be used due to the high heat treatment temperature.

本発明は上記事情に鑑みなされたもので、S/Nの良好
な磁気ディスクや磁気テープ等の磁気記録媒体を製造す
る方法を提供するものである。
The present invention has been made in view of the above circumstances, and provides a method for manufacturing magnetic recording media such as magnetic disks and magnetic tapes with good S/N.

問題点を解決するための手段 上記した問題点を解決するため、本発明の磁気記録媒体
の製造方法は、移動する基板に対して複数のターゲット
を配し、マグネトロン放電によ9強磁性金属薄膜をスパ
ッタリング蒸着する際、放電ガスに酸素を含めるように
したものである。
Means for Solving the Problems In order to solve the above-mentioned problems, the method for manufacturing a magnetic recording medium of the present invention involves disposing a plurality of targets on a moving substrate, and depositing nine ferromagnetic metal thin films by magnetron discharge. When depositing by sputtering, oxygen is included in the discharge gas.

作  用 上記した構成によシ、マグネトロン放電により生じる蒸
発原子の空間分布と酸素ガスの配合化による磁気微粒子
の静磁結合のかん和による保磁力向上とノイズの改良が
なされるものと考えられる。
It is believed that the above-described structure improves the coercive force and noise due to the spatial distribution of evaporated atoms generated by magnetron discharge and the fusion of the magnetostatic coupling of the magnetic fine particles due to the blending of oxygen gas.

ターゲットを複数化し、移動速度(生産性)を大きくす
る程その作用効果も強まる。
The more targets you have and the faster your movement speed (productivity), the stronger the effect will be.

実施例 以下、図面を参照しながら本発明の実施例について説明
する。
Embodiments Hereinafter, embodiments of the present invention will be described with reference to the drawings.

第1図は、本発明により得られる磁気記録媒体の一例・
の拡大断面である。第1図で1は高分子フィルム又はA
l−Mq金合金の非磁性基板2は、スパッタリングによ
り形成される磁気記録層3は保護膜である。
FIG. 1 shows an example of a magnetic recording medium obtained by the present invention.
This is an enlarged cross section of. In Figure 1, 1 is a polymer film or A
The magnetic recording layer 3 of the nonmagnetic substrate 2 made of l-Mq gold alloy is formed by sputtering and is a protective film.

第2図は本発明を実施するのに用いるスパッタリング装
置の一例の要部構成図である。同図において、4は真空
容器、5は真空排気系、6は冷却支持板、7は基板、8
は巻出しロール、9は巻き取りロール、10.11はタ
ーゲット、12.13は磁界発生器、14.15は高周
波電源、16はガス導入ボート、17は可変リーク弁、
18は絶縁導入端子である。磁界発生器は、基板の進行
方向に対して直交する磁界を形成するようになっている
FIG. 2 is a diagram showing a main part of an example of a sputtering apparatus used to carry out the present invention. In the figure, 4 is a vacuum container, 5 is a vacuum exhaust system, 6 is a cooling support plate, 7 is a substrate, and 8
is an unwinding roll, 9 is a take-up roll, 10.11 is a target, 12.13 is a magnetic field generator, 14.15 is a high frequency power supply, 16 is a gas introduction boat, 17 is a variable leak valve,
18 is an insulation introduction terminal. The magnetic field generator is configured to generate a magnetic field perpendicular to the traveling direction of the substrate.

これによりいわゆるマグネトロン放電を発生することが
でき、スパンタレイトが空間分布をもつようになり、導
入ガスとの比率をかえることができるようになるのであ
る。
This makes it possible to generate a so-called magnetron discharge, and the spantalate has a spatial distribution, making it possible to change the ratio to the introduced gas.

厚み26μmのポリエチレンテレフタレートフィ/I/
 A上にCo−N1(Co  80wt%)をターゲッ
トとし、表面磁界120(Oe)で13.56 (MH
z )の高周波グロー放電によりスパッタ蒸着した。そ
ノ時、 Ar I X1O−3(”rr)024X10
  (Torr)。
26μm thick polyethylene terephthalate fiber/I/
Co-N1 (Co 80wt%) was targeted on A, and 13.56 (MH
Sputter deposition was performed by high frequency glow discharge of z). At that time, Ar I X1O-3(”rr)024X10
(Torr).

ターゲットを2個とし、(1ケのターゲットは幅27.
5 cm 長さ12.61とした。)膜厚が0.1濁μ
mとなるような条件で成膜した。
There are two targets (one target has a width of 27 mm).
5 cm, length 12.61. ) Film thickness is 0.1 turbidity μ
The film was formed under conditions such that m.

移動速度は12m/m i nで、長さs 60m (
幅19cTL)の成膜を終えたのち、パーフロロオクタ
ン酸を厚み65人真空蒸着し、5.25インチのディス
クを作製し、(長手方向の任意抽出で1e枚選んだ)、
ギャップ長0.14μmのフェライトヘッドで、ビット
長0.3μmの矩形波を記録再生した。
The moving speed is 12 m/min, and the length s is 60 m (
After completing the film formation with a width of 19 cTL), perfluorooctanoic acid was vacuum-deposited to a thickness of 65 cm to produce a 5.25-inch disk (1e disks were selected by random selection in the longitudinal direction),
A rectangular wave with a bit length of 0.3 μm was recorded and reproduced using a ferrite head with a gap length of 0.14 μm.

比較例として、厚み20μmのポリアミドイミドフィル
ム上に厚み400人のクロムをスパッタ形成しその上に
0.07μmのCo−Ni (Co 80wt%)をA
r中で高周波マグネトロンスパッタし、次にOrを23
0人スパッタし、更に0.0了μmCo−Niをスパッ
タしその上にパーフロロオクタン酸を真空蒸着した磁気
ディスクを準備した。この製造条件を選んだのは、実施
例で得られた保磁力aso(Oe)。
As a comparative example, a chromium film with a thickness of 400 μm was sputtered on a polyamide-imide film with a thickness of 20 μm, and Co-Ni (Co 80 wt%) with a thickness of 0.07 μm was formed on it by sputtering.
High frequency magnetron sputtering in r, then Or 23
A magnetic disk was prepared by sputtering 0.0 μm Co--Ni and then vacuum-depositing perfluorooctanoic acid thereon. This manufacturing condition was chosen because of the coercive force aso (Oe) obtained in the example.

角形比0.83とほぼ同一の磁気特性とするためで、こ
の両者比較をS/Nについて行ったところ、実施例の方
がs、9(dB)優れていて、全帯域にノイズが改良さ
れていることが主な改善要素である。
This is to achieve almost the same magnetic characteristics with a squareness ratio of 0.83. When comparing the two in terms of S/N, the example was superior by s, 9 (dB), and the noise was improved in the entire band. The main improvement factor is that

以上述べた例に限定されないことは勿論テ、ハードディ
スク、磁気テープの形態であってもよい。
Of course, the present invention is not limited to the examples described above, and may take the form of a hard disk, magnetic tape, or the like.

ターゲットの枚数についても必要に応じて増せばよい。The number of targets may also be increased as necessary.

強磁性金属薄膜材料についてもCo −N i 、Co
−F e 。
Regarding ferromagnetic metal thin film materials, Co -N i , Co
-Fe.

Co−Cr、Co−Pr、Co−Ni−Pr等適宜選べ
ばよい。
Co-Cr, Co-Pr, Co-Ni-Pr, etc. may be selected as appropriate.

発明の効果 以上のように本発明によれば、低温で磁気特性が確保で
きるので、ポリエチレンテレフタレート等の汎用のプラ
スチックを基板として磁気記録媒体が得られるのと、S
/Nが良好な磁気記録層を高い生産性で得られるといっ
たすぐれた効果が得られる。
Effects of the Invention As described above, according to the present invention, magnetic properties can be ensured at low temperatures, so a magnetic recording medium can be obtained using a general-purpose plastic such as polyethylene terephthalate as a substrate, and S
An excellent effect can be obtained in that a magnetic recording layer having a good /N ratio can be obtained with high productivity.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明で製造する磁気記録媒体の一例の拡大断
面図、第2図は本発明の実施に用いたスパッタリング装
置の一例の概要図である。 1・・・・・・基板、2・・・・・・磁気記録層、7・
・・・・・基板、10.11・・・・・・ターゲット、
16・・・・・・ガス導入ボート。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名2−
・喪民記針層
FIG. 1 is an enlarged sectional view of an example of a magnetic recording medium manufactured according to the present invention, and FIG. 2 is a schematic diagram of an example of a sputtering apparatus used in carrying out the present invention. 1...Substrate, 2...Magnetic recording layer, 7.
...Substrate, 10.11 ...Target,
16... Gas introduction boat. Name of agent: Patent attorney Toshio Nakao and 1 other person2-
・Mourning record layer

Claims (1)

【特許請求の範囲】[Claims] 移動する基板に対向して複数のターゲットを配し、マグ
ネトロン放電により強磁性金属薄膜をスパッタリング蒸
着する際、放電ガスに酸素を含めたことを特徴とする磁
気記録媒体の製造方法。
A method for manufacturing a magnetic recording medium, characterized in that a plurality of targets are arranged facing a moving substrate, and oxygen is included in the discharge gas when a ferromagnetic metal thin film is sputter-deposited by magnetron discharge.
JP22311086A 1986-09-19 1986-09-19 Production of magnetic recording medium Pending JPS6378341A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22311086A JPS6378341A (en) 1986-09-19 1986-09-19 Production of magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22311086A JPS6378341A (en) 1986-09-19 1986-09-19 Production of magnetic recording medium

Publications (1)

Publication Number Publication Date
JPS6378341A true JPS6378341A (en) 1988-04-08

Family

ID=16792980

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22311086A Pending JPS6378341A (en) 1986-09-19 1986-09-19 Production of magnetic recording medium

Country Status (1)

Country Link
JP (1) JPS6378341A (en)

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