JPH0442730B2 - - Google Patents

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Publication number
JPH0442730B2
JPH0442730B2 JP4984183A JP4984183A JPH0442730B2 JP H0442730 B2 JPH0442730 B2 JP H0442730B2 JP 4984183 A JP4984183 A JP 4984183A JP 4984183 A JP4984183 A JP 4984183A JP H0442730 B2 JPH0442730 B2 JP H0442730B2
Authority
JP
Japan
Prior art keywords
substrate
present
film
magnetic
alloy
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
Application number
JP4984183A
Other languages
Japanese (ja)
Other versions
JPS59175034A (en
Inventor
Koichi Shinohara
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 JP58049841A priority Critical patent/JPS59175034A/en
Publication of JPS59175034A publication Critical patent/JPS59175034A/en
Publication of JPH0442730B2 publication Critical patent/JPH0442730B2/ja
Granted legal-status Critical Current

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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

Landscapes

  • Manufacturing Of Magnetic Record Carriers (AREA)
  • Thin Magnetic Films (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 本発明は短波長記録特性の優れた垂直記録方式
に利用される磁気記録媒体の製造方法に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a method for manufacturing a magnetic recording medium used in a perpendicular recording system with excellent short wavelength recording characteristics.

従来例の構成とその問題点 短波長記録特性の優れた記録方式として垂直記
録方式が開発され、それに伴い記録媒体の製造が
前記方式の実用化にとつて重要な課題となつてき
ている。
Conventional configurations and their problems A perpendicular recording system has been developed as a recording system with excellent short wavelength recording characteristics, and with this, the production of recording media has become an important issue for the practical application of the system.

前記記録方式の原理的検討の階段で用いられた
記録媒体は、基板にスパツタリング蒸着して得た
Co−Cr合金膜を配したものか、パーマロイを介
して、Co−Cr合金膜を配したものが主であつた。
記録媒体を量産するには、スパツタリング蒸着で
は成膜速度的に不満定であり、新しい垂直磁化膜
の成膜法として真空蒸着法を基礎にした条件検討
が一部で進められているが、満足する磁気特性を
得るには成膜時の基板温度を200℃以上に保持す
る必要があるため、基板として最も優れているポ
リエチレンテレフタレートが使えない難点があつ
た。
The recording medium used in the step of theoretical investigation of the recording method was obtained by sputtering deposition on the substrate.
The main types were those with a Co-Cr alloy film or those with a Co-Cr alloy film interposed through permalloy.
For mass production of recording media, sputtering evaporation is unsatisfactory in terms of film formation speed, and some studies are progressing on conditions based on vacuum evaporation as a new method for forming perpendicularly magnetized films; In order to obtain the desired magnetic properties, it is necessary to maintain the substrate temperature at 200°C or higher during film formation, making it impossible to use polyethylene terephthalate, which is the most excellent substrate.

発明の目的 本発明は基板としてポリエチレンテレフタレー
ト等の低融点の高分子材料を用いた場合でも、磁
化膜として垂直記録方式の磁化特性を満足できる
磁化膜を作ることができる磁気記録媒体の製造方
法を提供することを目的とする。
Purpose of the Invention The present invention provides a method for manufacturing a magnetic recording medium that can produce a magnetic film that satisfies the magnetization characteristics of a perpendicular recording method even when a low melting point polymer material such as polyethylene terephthalate is used as a substrate. The purpose is to provide.

発明の構成 本発明の磁気記録媒体の製造方法は、基板に
Co又はCo−Ni合金の何れかを電子ビーム蒸着す
ると同時に、Cr,Mo,V,w,Ru,Smのうち
より選ばれた1つの元素を含む非磁性Co系合金
をスパツタリング蒸着して、基板面に対して垂直
方向に磁化容易軸を有するCo系合金薄膜を形成
することを特徴とする。
Structure of the Invention The method for manufacturing a magnetic recording medium of the present invention provides a method for manufacturing a magnetic recording medium according to the present invention.
At the same time as Co or Co-Ni alloy is deposited by electron beam, a non-magnetic Co-based alloy containing one element selected from Cr, Mo, V, w, Ru, or Sm is sputter deposited on the substrate. It is characterized by forming a Co-based alloy thin film having an axis of easy magnetization perpendicular to the plane.

実施例の説明 以下、本発明の製造方法を具体例に基づいて説
明する。
Description of Examples Hereinafter, the manufacturing method of the present invention will be explained based on specific examples.

第1図は本発明は実施するために用いた巻取り
蒸着装置の主要構成図である。基板1は、送り出
し軸2より回転冷却支持体3に沿つて巻取り軸4
で巻きとられて移動する。基板1が巻取り軸4に
巻き取られるまでの間に、回転冷却支持体3にに
沿つた状態で冷却された基板1にCo又はCo−Ni
合金の蒸気流5がマスク6により入射角規制を受
けて差し向けられるよう、第1の蒸発源()が
配設されている。第1図においてこの第1の蒸発
源()は電子ビーム加熱方式が代表例として模
式的に図示されている。すなわち、蒸発源容器7
に蒸発材料8を入れ、電子線発生装置9より放射
される電子を加速して蒸発材料8の一部を衝撃し
て加熱し、前記蒸気流5が作されている。また、
第1図においては第2の蒸発源()としてスパ
ツタ源が設けられており、スパツタカソード10
としては、パツキングプレートにボンデイングし
た、Sm,Cr,Mo,W,V,Ruのうちより選ば
れた1種の元素を含む非磁性Co系合金の材料が
用いられている。このスパツタカソード10の配
置については、条件の最適化のための2〜3の実
験が必要であるが第1図に示したように、スパツ
タ原子が、ほぼ垂直に入射する蒸気流5にさらさ
れる基板の領域全体に行き渡るように、カソード
サイズと幾何学的配置は、作図で求めたものに近
い近い条件で選ばれている。
FIG. 1 is a main configuration diagram of a winding vapor deposition apparatus used to carry out the present invention. The substrate 1 is moved from the feed shaft 2 to the winding shaft 4 along the rotary cooling support 3.
It is rolled up and moved. Before the substrate 1 is wound up on the winding shaft 4, Co or Co-Ni is applied to the cooled substrate 1 along the rotating cooling support 3.
A first evaporation source ( ) is arranged such that a vapor stream 5 of the alloy is directed with angle of incidence regulation by a mask 6 . In FIG. 1, the first evaporation source ( ) is schematically shown as an electron beam heating method as a representative example. That is, the evaporation source container 7
An evaporative material 8 is placed in the evaporative material 8, and electrons emitted from an electron beam generator 9 are accelerated to impact and heat a part of the evaporative material 8, thereby creating the vapor flow 5. Also,
In FIG. 1, a sputter source is provided as a second evaporation source (), and a sputter cathode 10
As the material, a non-magnetic Co-based alloy material containing one element selected from among Sm, Cr, Mo, W, V, and Ru is used, which is bonded to the packing plate. Regarding the arrangement of the sputter cathode 10, a few experiments are required to optimize the conditions, but as shown in FIG. The cathode size and geometry are chosen to closely approximate what was determined in the drawing, so that the entire area of the substrate covered is covered.

真空容器11内部は、マスク6によつて巻取り
室12と蒸発源室13に分割されており、巻取り
室12は、巻取り系とスパツタ蒸着系を内蔵して
いる。また、蒸発源室13は電子ビーム蒸発系を
内蔵している。両者の空間12,13は、夫々排
気系14,15により排気され、通常、スパツタ
蒸着系には、パリアブリーク弁16の調節により
放電維持のために、外部より強制的に放電ガスが
ノズル17より導入されている。なお、真空容器
11を巻取り室12と蒸発源室13に分割した
が、これは必須要件でない。また、スパツタ蒸着
系に用られる方式としては、DCマグネトロン方
式か、高周波マグネトロン方式のいずれかが適し
ている。
The inside of the vacuum container 11 is divided by the mask 6 into a winding chamber 12 and an evaporation source chamber 13, and the winding chamber 12 contains a winding system and a sputter deposition system. Further, the evaporation source chamber 13 incorporates an electron beam evaporation system. Both spaces 12 and 13 are exhausted by exhaust systems 14 and 15, respectively, and normally discharge gas is forcibly introduced from the outside through a nozzle 17 in order to maintain the discharge by adjusting a barrier break valve 16 in the sputter deposition system. has been done. Although the vacuum container 11 is divided into the winding chamber 12 and the evaporation source chamber 13, this is not an essential requirement. Further, as a method for use in the sputter deposition system, either a DC magnetron method or a high frequency magnetron method is suitable.

第1図では垂直磁化膜の形成に用いる系のみ示
したが、本発明は基板上にあらかじめ下地として
パーマロイ、Cr,Ti等を所定厚み形成したもの
を基板として同様にこの装置で垂直磁化膜を形成
できる。
Although FIG. 1 only shows the system used to form a perpendicularly magnetized film, the present invention also uses this apparatus to form a perpendicularly magnetized film using a substrate on which a predetermined thickness of permalloy, Cr, Ti, etc. has been formed in advance as an underlayer. Can be formed.

前記基板1は、ポリエチレンテレフタレート、
ポリイミド、ポリアミド、ポリエチレンナフサタ
レート、ポリ塩化ビニル等であるが後述するよう
に、ポリエチレンテレフタレートを用いても、基
板は何ら熱劣化を受けることなく磁気特性として
満足できる垂直磁化膜を得ることができるのは、
スパツタ原子の有する運動エネルギーの大きな面
と、活性原子、イオン、電子の基板表面の衝撃効
果が、CoまたはCo−Niの高速蒸着と混合しても
維持されることによるものと考えられる。
The substrate 1 is made of polyethylene terephthalate,
Polyimide, polyamide, polyethylene naphthalate, polyvinyl chloride, etc. are used, but as described later, even if polyethylene terephthalate is used, a perpendicularly magnetized film with satisfactory magnetic properties can be obtained without any thermal deterioration of the substrate. The thing is,
This is thought to be due to the large kinetic energy of sputtering atoms and the impact effects of active atoms, ions, and electrons on the substrate surface, which are maintained even when mixed with high-speed deposition of Co or Co--Ni.

次に第1図の装置を用いて実施した各実験例を
説明する。
Next, various experimental examples carried out using the apparatus shown in FIG. 1 will be explained.

〔実施例 1〕 25μmのポリエチレンテレフタレートフイルム
に対して、入射角が0°から16°までの範囲でCo
(99.99%)を0.76μm/minの蒸着速度で蒸着する
と同時に、Coに対しVを40%含むCo−V合金を
ターゲツトとしてCo−V(99.98%)を入射角が平
均して45°に近い状態で0.2μm/minの蒸着速度で
蒸着した。この時、Arを0.03/min導入し真空
度1×10-4Torrとし、スパツタカソード10に
13.56MHzの高周波を印加した。そして回転キヤ
ンの表面温度を変化させて、Co−V膜のC軸分
散を調べた。
[Example 1] Co
At the same time, Co-V (99.98%) was deposited at a deposition rate of 0.76 μm/min, and the average incident angle was close to 45°. Vapor deposition was performed at a deposition rate of 0.2 μm/min. At this time, Ar was introduced at 0.03/min to make the vacuum level 1×10 -4 Torr, and the spatter cathode 10 was
A high frequency of 13.56MHz was applied. Then, the C-axis dispersion of the Co-V film was investigated by changing the surface temperature of the rotating can.

Co−V膜の形成は0.06μmから0.46μmの範囲で
実施した。またVの値は原子%で13%から28%の
範囲で実施した。
The Co-V film was formed in a range of 0.06 μm to 0.46 μm. Further, the value of V was carried out in the range of 13% to 28% in atomic %.

第2図は、0.15μmのV18.5at%のCo−V膜の垂
直方向の磁化曲線であり、極めて良好な垂直磁化
膜が得られていることがわかる。
FIG. 2 shows the vertical magnetization curve of a 0.15 μm V18.5 at% Co-V film, and it can be seen that an extremely good perpendicular magnetization film was obtained.

第3図は、横軸に基板1の表面温度に関連する
量である回転キヤンの表面温度をとり、(002)面
からのX線回転強度の角度分布をあらわすロツキ
ングカーブの半値幅(△θ50)の変化を、従来例
との比較で示したものである。第3図における比
較例()は、Co−V合金を電子ビーム蒸着し
た場合で、Vの成分比が一定に保持できないの
で、Vの値として17.5at%〜19at%までの間のサ
ンブルを抽出して測定した結果である。()は
本発明の製造方法によりものである。この第3図
より、極めて微小量の△θ50の値の改良が、基板
温度をあげることで、行われる様子が伺えるが、
絶対値が従来例に比較して、極めて小さい領域で
の変化であり、本発明の製造方法による媒体は、
いずれの△θ50値でも満足できるものである。
In Figure 3, the horizontal axis represents the surface temperature of the rotating can, which is a quantity related to the surface temperature of the substrate 1, and the half-width (△ The change in θ 50 ) is shown in comparison with the conventional example. The comparative example () in Figure 3 is a case where a Co-V alloy is deposited by electron beam, and since the component ratio of V cannot be kept constant, samples with V values between 17.5 at% and 19 at% are extracted. This is the result of measurement. () is obtained by the manufacturing method of the present invention. From this Figure 3, it can be seen that an extremely small amount of improvement in the value of △θ 50 is achieved by increasing the substrate temperature.
The absolute value changes in an extremely small area compared to the conventional example, and the medium produced by the manufacturing method of the present invention has
Any Δθ 50 value is satisfactory.

〔実施例 2〕 10.5μmのポリエチレンテレフタレートフイル
ムに対し、入射角が0°から16°までの範囲でCo85
%Ni15%(合金の純度、99.98%)を2.2μm/
minの蒸着速度で蒸着すると同時にCr(99.99%)
を34%含むCo−Cr合金をターゲツトとして第1
図に示したカソードと同じカソードを対称位置に
配し一対のカソードとし、夫々よりのCo−Ni−
Cr原子の平均的入射角が27°に近い状態で、
0.48μm/minのスパツタ蒸着速度で蒸着した。こ
の時のAr導入量は0.03/minで、真空度は1.8
×10-4Torrで、スパツターカソードに13.56MHz
の高周波を印加した。回転キヤンの表面温度は10
℃から120℃の範囲で実施したが、垂直方向の保
磁力は1300〔Oe〕で△θ50は4.5°〜4.7°であつた。
Co−Ni−Crの成分比については、Co−Ni−Cr
のスパツタ蒸着速度を固定してCo−Niの蒸着速
度を変えた場合と、Co−Niの蒸着速度を固定し
てCo−Ni−Crのスパツタ速度を可変する両者の
場合についてCo−Niに対して、原子%でCrが16
%〜29%までの範囲についても実施して、垂直方
向の保磁力は1200〔O¨〕〜1600〔O¨e〕、△θ50は3.9
°
〜5.6°の範囲の膜を得た。他に、Co100%に対し
てW,Cr,Sm,Mo,Ruを夫々Coに対して16−
33at%の範囲で可変しCo80%Ni20%の合金に対
して、Cr,V,W,Sm,Mo,RuをCo−Ni合金
に対して16〜33at%の範囲で可変して、本発明を
実施した。この場合、いずれの場合も、基板は熱
劣化なしに、0.03μmから0.6μmの垂直磁化膜を、
平均蒸着速度1.5μm/min〜9,9m/minの高
速で得ることができた。
[Example 2] Co85 was applied to a 10.5 μm polyethylene terephthalate film at an incident angle of 0° to 16°.
%Ni15% (alloy purity, 99.98%) 2.2μm/
Cr (99.99%) simultaneously deposited at a deposition rate of min
The first target was a Co-Cr alloy containing 34%
Co-Ni-
When the average angle of incidence of Cr atoms is close to 27°,
The deposition was performed at a sputter deposition rate of 0.48 μm/min. At this time, the amount of Ar introduced was 0.03/min, and the degree of vacuum was 1.8.
×10 -4 Torr, 13.56MHz to sputter cathode
high frequency was applied. The surface temperature of the rotating can is 10
The experiment was carried out at a temperature ranging from °C to 120 °C, and the vertical coercive force was 1300 [Oe] and Δθ 50 was 4.5° to 4.7°.
Regarding the component ratio of Co−Ni−Cr, Co−Ni−Cr
For Co-Ni, the sputtering speed is fixed and the sputtering speed of Co-Ni is varied, and the sputtering speed of Co-Ni is fixed and the sputtering speed of Co-Ni-Cr is varied. Cr is 16 atomic%
% to 29%, the vertical coercive force was 1200 [O¨] to 1600 [O¨e], and △θ 50 was 3.9
°
A membrane with a range of ~5.6° was obtained. In addition, for Co100%, W, Cr, Sm, Mo, and Ru are each 16− for Co.
The present invention was carried out by varying Cr, V, W, Sm, Mo, and Ru in the range of 16 to 33 at% with respect to the Co-Ni alloy for an alloy of 80% Co and 20% Ni with a range of 33 at%. carried out. In both cases, the substrate can hold a perpendicularly magnetized film of 0.03 μm to 0.6 μm without thermal deterioration.
It was possible to obtain high-speed deposition with an average deposition rate of 1.5 μm/min to 9.9 m/min.

また、ポリエチレンテレフタレート10.5μmの
上にあらかじめパーマロイ薄膜を0.1μm、電子ビ
ーム蒸着した上で前記条件で垂直磁化膜の作成を
試みたが、ポリエチレンテレフタレートに直接本
発明を実施した場合に得られた性能と磁気特性は
同一であつたか、若干改良されていた。
In addition, we attempted to create a perpendicularly magnetized film under the above conditions by electron beam evaporation of a 0.1 μm permalloy thin film on 10.5 μm polyethylene terephthalate, but the performance obtained when the present invention was applied directly to polyethylene terephthalate was The magnetic properties were either the same or slightly improved.

また、Coの飽和磁化量をうすめるために用い
られると同時に、C軸の配向性の改良のために用
いられるCr,Mo,V,W,Ru,Smは、Coと合
金状態にして蒸着した場合、蒸気圧がCoと大き
く異なるために一定の成分比を保持できないが、
本発明では、長時間に渡つて安定に成分比を制御
できその結果、磁気特性の均一性を確保できる利
点ある。
In addition, Cr, Mo, V, W, Ru, and Sm, which are used to dilute the saturation magnetization of Co and improve the C-axis orientation, are deposited in an alloyed state with Co. , it is not possible to maintain a constant component ratio because the vapor pressure is significantly different from that of Co, but
The present invention has the advantage that the component ratio can be stably controlled over a long period of time, and as a result, uniformity of magnetic properties can be ensured.

前記回転冷却支持体3は第1図に示したいわゆ
る回転キヤンに限らず、回転ベルトであつても良
い。
The rotary cooling support 3 is not limited to the so-called rotary can shown in FIG. 1, but may also be a rotary belt.

本発明は、広幅の基板で、ロール状に巻いてあ
る長尺物上に垂直磁化膜を得る上で、有用であつ
て、磁気記録媒体として、テープ、デイスク、シ
ート、カード等の形態については何ら制約される
ものではない。
INDUSTRIAL APPLICABILITY The present invention is useful for obtaining a perpendicularly magnetized film on a long, wide substrate wound into a roll, and is suitable for magnetic recording media such as tapes, disks, sheets, cards, etc. There are no restrictions whatsoever.

尚、本発明は、耐熱基板に適用することも当然
できるもので、例えば基板温度250℃に保持して
ポリイミド25μm上に本発明を実施したものは
Co80at%Cr20at%、0.15μmの垂直方向保磁力
1900〔Oe〕,△θ50=2.6°であり、本発明によらず
電子ビーム蒸着のみで同一構成の垂直磁化膜が保
磁力1300〔O¨e〕,△θ50=4.9°であつたのに比べて

極めて優れた磁気特性をもたらすものであつた。
Note that the present invention can naturally be applied to heat-resistant substrates; for example, the present invention can be applied to a 25 μm polyimide substrate while maintaining the substrate temperature at 250°C.
Co80at% Cr20at%, 0.15μm vertical coercive force
1900 [Oe], △θ 50 = 2.6°, and a perpendicularly magnetized film with the same configuration obtained only by electron beam evaporation without using the present invention had a coercive force of 1300 [O¨e], △θ 50 = 4.9°. Compared to
This resulted in extremely excellent magnetic properties.

発明の効果 以上説明のように本発明の磁気記録媒体の製造
方法によると、おきい保持力でC軸配向性の良好
な、垂直記録方式に適したCo又はCoNi系の合金
系薄膜を、耐熱基板のみならず低融点基板上に
も、高い生産性と、長尺での特性の均一性を確保
して実用規模で得ることができるものである。
Effects of the Invention As explained above, according to the method of manufacturing a magnetic recording medium of the present invention, a heat-resistant Co or CoNi alloy thin film suitable for perpendicular recording, which has a large coercive force and good C-axis orientation, is produced. It can be obtained on a practical scale not only on a substrate but also on a low melting point substrate while ensuring high productivity and uniformity of properties over a long length.

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

第1図は本発明の製造方法の具体的な一実施例
に使用される巻取り蒸着装置の要部概要構成図、
第2図は本発明により得られた媒体の代表例の磁
気特性図、第3図はC軸配向性の支持体温度依存
性について本発明の製造方法による媒体と従来の
媒体との比較説明図である。 1……基板、3……回転冷却支持体、8……蒸
発材料、10……スパツタカソード。
FIG. 1 is a schematic configuration diagram of main parts of a winding vapor deposition apparatus used in a specific embodiment of the manufacturing method of the present invention;
FIG. 2 is a magnetic characteristic diagram of a typical example of a medium obtained by the present invention, and FIG. 3 is a comparative illustration of the dependence of C-axis orientation on support temperature between a medium produced by the manufacturing method of the present invention and a conventional medium. It is. DESCRIPTION OF SYMBOLS 1... Substrate, 3... Rotating cooling support, 8... Evaporation material, 10... Sputter cathode.

Claims (1)

【特許請求の範囲】[Claims] 1 基板にCoまたはCo−Ni合金のいずれかを電
子ビーム蒸着すると同時に、Cr,Mo,V,W,
Ru,Smのうちより選ばれた1つの元素を含む非
磁性Co系合金をスパツタリング蒸着して基板面
に対して垂直方向に磁化容易軸を有するCo系合
金薄膜を形成する磁気記録媒体の製造方法。
1 At the same time as electron beam evaporation of either Co or Co-Ni alloy onto the substrate, Cr, Mo, V, W,
A method for producing a magnetic recording medium, comprising sputtering deposition of a non-magnetic Co-based alloy containing one element selected from Ru and Sm to form a Co-based alloy thin film having an axis of easy magnetization perpendicular to the substrate surface. .
JP58049841A 1983-03-24 1983-03-24 Production of magnetic recording medium Granted JPS59175034A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58049841A JPS59175034A (en) 1983-03-24 1983-03-24 Production of magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58049841A JPS59175034A (en) 1983-03-24 1983-03-24 Production of magnetic recording medium

Publications (2)

Publication Number Publication Date
JPS59175034A JPS59175034A (en) 1984-10-03
JPH0442730B2 true JPH0442730B2 (en) 1992-07-14

Family

ID=12842297

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58049841A Granted JPS59175034A (en) 1983-03-24 1983-03-24 Production of magnetic recording medium

Country Status (1)

Country Link
JP (1) JPS59175034A (en)

Also Published As

Publication number Publication date
JPS59175034A (en) 1984-10-03

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