JPS58141444A - Production of magnetic recording medium - Google Patents

Production of magnetic recording medium

Info

Publication number
JPS58141444A
JPS58141444A JP2471882A JP2471882A JPS58141444A JP S58141444 A JPS58141444 A JP S58141444A JP 2471882 A JP2471882 A JP 2471882A JP 2471882 A JP2471882 A JP 2471882A JP S58141444 A JPS58141444 A JP S58141444A
Authority
JP
Japan
Prior art keywords
plasma
gaseous
vapor
recording medium
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.)
Granted
Application number
JP2471882A
Other languages
Japanese (ja)
Other versions
JPH0334620B2 (en
Inventor
Koichi Shinohara
紘一 篠原
Toshiaki Kunieda
国枝 敏明
Ryuji Sugita
龍二 杉田
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 JP2471882A priority Critical patent/JPS58141444A/en
Publication of JPS58141444A publication Critical patent/JPS58141444A/en
Publication of JPH0334620B2 publication Critical patent/JPH0334620B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/84Processes or apparatus specially adapted for manufacturing record carriers
    • G11B5/85Coating a support with a magnetic layer by vapour deposition
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/0021Reactive sputtering or evaporation

Abstract

PURPOSE:To form a long-sized medium to be used for a vertical recording system with high productivity while maintaining the component ratio of Cr with which the control of the rate of vapor deposition is difficult, at a stable state, by directing vapor flow contg. Co to a substrate and passing the vapor flow through the inside of plasma formed by a gaseous Cr compd. as a discharge gas. CONSTITUTION:A tape-like sustrate 1 moves along the peripheral side surface of a cylindrical can 2 under temp. control and is vapor-deposited through the aperture part of a mask 5. Co or a Co alloy 6 is evaporated by heating with electron beams, and Cr is supplied from plasma. More specifically, a gaseous Cr compd. such as Cr(C9H12)2 is introduced as a discharge gas by each specified amt. into the system through an introducing nozzle 13, and high frequency plasma is formed by a coiled high frequency electrode 9.

Description

【発明の詳細な説明】 本発明は垂直記録方式に用いる記録媒体の製造力θ、に
関し、長尺の媒体を安定に製造できるようにすることを
目的とするものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to the manufacturing capacity θ of a recording medium used in a perpendicular recording system, and an object of the present invention is to enable stable manufacturing of long media.

垂直記録方式は、短波長記録に適する記録方式として注
目され、媒体の開発、記録方式の研究が各方面で盛んで
ある。
The perpendicular recording method has attracted attention as a recording method suitable for short wavelength recording, and research on media development and recording methods is active in various fields.

11(直方向に磁化容易軸を有する。いわゆ−る垂直磁
化膜は、 CoにOrを添加してMSを下け、かつり、
c、p構造の結晶のC軸を基板面の垂直方向に小さな分
散で配向させた膜が良く知られる。
11 (having an axis of easy magnetization in the perpendicular direction. The so-called perpendicular magnetization film is made by adding Or to Co to lower the MS, and
A film in which the C axis of a c,p structure crystal is oriented with small dispersion in the direction perpendicular to the substrate surface is well known.

この膜の製法は、高周波スパッタリング法、電子ビーム
蒸着法が知られる。高周波スパッタリング法は、成膜速
度が小さいため、実用に供する上では難点がある。
Known methods for manufacturing this film include high frequency sputtering and electron beam evaporation. Since the high-frequency sputtering method has a low film formation rate, it is difficult to put it into practical use.

m1電子ビーム蒸着法は、Orの成分比を一定に保持す
る上で困難を伴うため、成膜速度の大きさを生かす上で
工夫を必要とする。
Since the m1 electron beam evaporation method involves difficulties in keeping the Or component ratio constant, it requires some ingenuity to take advantage of the high film formation rate.

Or は昇華するため、蒸着速度の制御がむずかしいか
らである。
This is because Or sublimes, making it difficult to control the deposition rate.

本発明はかかる点に鑑みなされたもので蒸発源としてH
,co又はCoNi等のCo  kペースとし。
The present invention has been made in view of this point, and uses H as an evaporation source.
, co or CoNi.

蒸気圧の近い物質の組み合わせたものを用いCjrの添
加[、Orの気体プラズマからの析出により行い、成分
比を安定に保持するものである。以下に図面を用い本発
明の詳細な説明する。
The addition of Cjr and Or is performed by precipitation from gas plasma using a combination of substances with similar vapor pressures, and the component ratio is kept stable. The present invention will be described in detail below using the drawings.

図は本発明を実施するための装置の一例を示す。The figure shows an example of a device for implementing the invention.

図に示すように、高分子成形物等よりなるテーゾ状基体
1は、温度制御された円筒状キャン2の周側面にイイっ
て、送り出し軸3より1巻取軸4へ移動する。その間、
マスク6の開孔部を通し蒸着きれる。
As shown in the figure, a Tezo-shaped substrate 1 made of a polymer molded product or the like is moved from a feed-out shaft 3 to a take-up shaft 4 on the circumferential side of a cylindrical can 2 whose temperature is controlled. meanwhile,
The vapor deposition is completed through the opening of the mask 6.

CO又はCo合金6は、電子ビーム加熱により蒸気化さ
Lる。8は電子ビーム源を模式的に示す。
CO or Co alloy 6 is vaporized by electron beam heating. 8 schematically shows an electron beam source.

7tま蒸発源容器である。This is a 7 ton evaporation source container.

Or  の供給は、プラズマより行うよう構成する。The supply of Or is configured to be performed by plasma.

例えば、一端が開放されたコイル状の高周波電極9にマ
ツチングホックス10の調整によV、高周彼電諒11よ
り高周波電、力を効率良く供給し、高1、“、1彼プラ
ズマを生成するよう構成する。
For example, by adjusting the matching hook 10 to a coil-shaped high-frequency electrode 9 with one end open, high-frequency electricity and power can be efficiently supplied from the high-frequency electrode 11 to generate high-frequency plasma. Configure to generate.

放電気体としてOr(09H+ 2)2などのガス状C
r化合物をニードル升12を調節して、系内に導入する
。導入ノズル13は勿論、真空槽14の外部も。
Gaseous C such as Or(09H+ 2)2 as a discharge electric body
The r compound is introduced into the system by adjusting the needle size 12. Not only the introduction nozzle 13 but also the outside of the vacuum chamber 14.

180’(:程度に保持する必要がめる。それは、上、
11;気体の導入jt’(r一定に制御するためである
180' (: It is necessary to hold the
11; This is to control the introduction of gas jt'(r to be constant).

負空槽14は1巻取り機□構を配する上室16と。The negative empty tank 14 has an upper chamber 16 in which a single winding machine □ structure is arranged.

プラズマ室16と、蒸発室17に、かくへ@18゜19
で伺切られる。電子ビーム蒸発源は16’Torr以上
の高真空を必要とするため、ある程度の差圧をとる必要
もあり1個々に、真空排気系20.21゜22を具備さ
せるのが良い。
To the plasma chamber 16 and the evaporation chamber 17, there is @18°19
I was asked. Since the electron beam evaporation source requires a high vacuum of 16' Torr or more, it is also necessary to provide a certain degree of pressure difference, so it is preferable to provide each source with a vacuum evacuation system 20.21°22.

23はシャッタであり、’ 24ri高圧導入用の絶縁
端子である。
23 is a shutter, and 24 is an insulated terminal for introducing high voltage.

次に具体的に本発明の詳細な説明する。Next, the present invention will be specifically explained in detail.

〔実施例1〕 基体として、ポリエチレンテレフタレートフィルム(厚
さ12μ111.幅、16011m、長さ1.ooo 
m )を用いた。
[Example 1] As a substrate, a polyethylene terephthalate film (thickness: 12 μm, width: 16011 m, length: 1.ooo
m) was used.

高周波電極は4ターンに構成され、高周波電力ij、 
 13.6611に490Wに制御した。
The high frequency electrode is configured with 4 turns, and high frequency power ij,
It was controlled to 490W on 13.6611.

GO蒸発源は、aokV、最大4ムの電子ビーム加熱方
式を採用し、蒸発源容器はZrO2製で、C。
The GO evaporation source uses an electron beam heating method with aokV and maximum of 4 μm, and the evaporation source container is made of ZrO2 and C.

の供給は、蒸発源容器に直径16MMのロンドを上記電
子ビームの一部のパワーで溶解し補給する方法をとった
。実験結果を表1に示す。
was supplied by melting and replenishing the evaporation source container with a rond having a diameter of 16 mm using a part of the power of the electron beam. The experimental results are shown in Table 1.

く以 下 余 白〉 なお表1における本発明ムはキャン直径5Q(ff。Kui Shimo White The invention in Table 1 has a can diameter of 5Q (ff.

同温度70°Cとし厚さ0.2μmの磁性膜を形成した
場合を示し1本発明Bはキャン直径1100c。
This shows the case where a magnetic film with a thickness of 0.2 μm was formed at the same temperature of 70° C. 1 Invention B has a can diameter of 1100 cm.

同温度80’Cとし、厚さ0.2μmの磁性膜を形成し
た場合を示す。
The case where a magnetic film with a thickness of 0.2 μm was formed at the same temperature of 80'C is shown.

〔実施例2〕 ポリイミドフィルム(厚さ26μm )を用い。[Example 2] Using polyimide film (thickness 26 μm).

キャン温度200’Cで1本発明を実施した場合の生産
性と特性面を他の方法におけるのと比較した結果を表2
示す。
Table 2 shows the results of comparing the productivity and characteristics when implementing the present invention at a can temperature of 200'C with those using other methods.
show.

く以 下 余 白〉 以上の表19表2に示した結果から明らかなように、不
発明により製造したものは、長尺ものの長手方向におけ
る性状の変動が極めて小さなものとなってお9.しかも
生産性が鳥いものとなっている。
As is clear from the results shown in Table 19 and Table 2 above, the products manufactured by the non-inventive method have extremely small variations in properties in the longitudinal direction of the long products. Moreover, productivity is at an all-time high.

なお本発明は、基体上に非磁性下地を配した場合、或い
はパーマロイ薄膜を配した2層構成の場合は勿論、基体
の両面にかかる構成を得る場合も有効である。
Note that the present invention is effective not only when a nonmagnetic base is disposed on the substrate, or when a two-layer structure is provided with a permalloy thin film, but also when such a structure is obtained on both sides of the substrate.

又、基体の種類によらず有効で、さらに磁性膜としてC
o −Orに限定さnず他の垂直磁化膜でOrを含有す
るものについて共通に効果がある。
In addition, it is effective regardless of the type of substrate, and furthermore, as a magnetic film, C
This effect is not limited to o-Or, but is common to other perpendicular magnetization films containing Or.

以上の説明により明らかなように1本発明は。As is clear from the above description, one aspect of the present invention is as follows.

高い生産性と、高品質の垂直磁化膜の生産を両立させ得
るものであって、テープ、ディスクの形態によらず、長
尺の原反を得るのに最適であって。
It is capable of achieving both high productivity and production of high-quality perpendicularly magnetized films, and is ideal for obtaining long lengths of material regardless of the form of tape or disk.

その工業的有価値性は太きいものがある。Its industrial value is significant.

【図面の簡単な説明】 図は本発明を実施するために用いられる装置の一例を示
す図である。 1・・・・・・基体、2・・・・・円筒状キャン、6・
・・・・・00合3.9・・・・・・高周波電極、13
・・・・・・導入ノズル。
BRIEF DESCRIPTION OF THE DRAWINGS The figure is a diagram showing an example of an apparatus used to carry out the present invention. 1... Base body, 2... Cylindrical can, 6...
...00 go 3.9...High frequency electrode, 13
...Introduction nozzle.

Claims (2)

【特許請求の範囲】[Claims] (1)円筒状キャンの周側面に沿って移動する基体にG
o  2含む蒸気流を差し向けるとともに上記蒸気流を
ガス状Or 化合物を放電気体とするプラズマ中を通過
せしめることを特徴とする磁気記録媒体の製造方法。
(1) G on the base body moving along the circumferential side of the cylindrical can.
A method for producing a magnetic recording medium, which comprises directing a vapor flow containing O 2 and causing the vapor flow to pass through a plasma containing a gaseous Or 2 compound as a discharge material.
(2)  Or 化合物が0r(C9H+す2 で表さ
れる化合物であることを特徴とする特許請求の範囲第1
項記載の磁気記録媒体の製造方法。
(2) Claim 1, wherein the Or compound is a compound represented by 0r(C9H+S2)
A method for producing a magnetic recording medium as described in .
JP2471882A 1982-02-17 1982-02-17 Production of magnetic recording medium Granted JPS58141444A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2471882A JPS58141444A (en) 1982-02-17 1982-02-17 Production of magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2471882A JPS58141444A (en) 1982-02-17 1982-02-17 Production of magnetic recording medium

Publications (2)

Publication Number Publication Date
JPS58141444A true JPS58141444A (en) 1983-08-22
JPH0334620B2 JPH0334620B2 (en) 1991-05-23

Family

ID=12145935

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2471882A Granted JPS58141444A (en) 1982-02-17 1982-02-17 Production of magnetic recording medium

Country Status (1)

Country Link
JP (1) JPS58141444A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100731483B1 (en) 2005-04-15 2007-06-21 삼성에스디아이 주식회사 Plasma display panel manufacturing equipment

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100731483B1 (en) 2005-04-15 2007-06-21 삼성에스디아이 주식회사 Plasma display panel manufacturing equipment

Also Published As

Publication number Publication date
JPH0334620B2 (en) 1991-05-23

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