JPH0154777B2 - - Google Patents
Info
- Publication number
- JPH0154777B2 JPH0154777B2 JP13117781A JP13117781A JPH0154777B2 JP H0154777 B2 JPH0154777 B2 JP H0154777B2 JP 13117781 A JP13117781 A JP 13117781A JP 13117781 A JP13117781 A JP 13117781A JP H0154777 B2 JPH0154777 B2 JP H0154777B2
- Authority
- JP
- Japan
- Prior art keywords
- coercive force
- present
- angle
- evaporation
- substrate
- 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
Links
- 230000005291 magnetic effect Effects 0.000 claims description 12
- 239000000758 substrate Substances 0.000 claims description 10
- 238000000034 method Methods 0.000 claims description 5
- 238000001816 cooling Methods 0.000 claims description 4
- 238000000151 deposition Methods 0.000 claims description 4
- 239000003302 ferromagnetic material Substances 0.000 claims description 4
- 238000004519 manufacturing process Methods 0.000 claims description 3
- 229920000642 polymer Polymers 0.000 claims 1
- 230000001105 regulatory effect Effects 0.000 claims 1
- 238000001704 evaporation Methods 0.000 description 13
- 230000008020 evaporation Effects 0.000 description 12
- 239000002184 metal Substances 0.000 description 9
- 229910052751 metal Inorganic materials 0.000 description 9
- 230000008859 change Effects 0.000 description 6
- 239000000463 material Substances 0.000 description 6
- 230000005294 ferromagnetic effect Effects 0.000 description 5
- 239000010408 film Substances 0.000 description 5
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 4
- 238000007796 conventional method Methods 0.000 description 4
- 230000007246 mechanism Effects 0.000 description 4
- 238000004804 winding Methods 0.000 description 4
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 3
- 230000008021 deposition Effects 0.000 description 3
- -1 polyethylene terephthalate Polymers 0.000 description 3
- 229920000139 polyethylene terephthalate Polymers 0.000 description 3
- 239000005020 polyethylene terephthalate Substances 0.000 description 3
- 239000010409 thin film Substances 0.000 description 3
- 238000007740 vapor deposition Methods 0.000 description 3
- UQSXHKLRYXJYBZ-UHFFFAOYSA-N Iron oxide Chemical compound [Fe]=O UQSXHKLRYXJYBZ-UHFFFAOYSA-N 0.000 description 2
- 239000011230 binding agent Substances 0.000 description 2
- 230000004907 flux Effects 0.000 description 2
- 229910052742 iron Inorganic materials 0.000 description 2
- 239000000696 magnetic material Substances 0.000 description 2
- 230000002265 prevention Effects 0.000 description 2
- 229910000531 Co alloy Inorganic materials 0.000 description 1
- 229910000990 Ni alloy Inorganic materials 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005566 electron beam evaporation Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000010419 fine particle Substances 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 230000006698 induction Effects 0.000 description 1
- 230000000873 masking effect Effects 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 229910052759 nickel Inorganic materials 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 238000012856 packing Methods 0.000 description 1
- 238000005192 partition Methods 0.000 description 1
- 230000004044 response Effects 0.000 description 1
- 238000007738 vacuum evaporation Methods 0.000 description 1
Classifications
-
- C—CHEMISTRY; METALLURGY
- C23—COATING 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
- C23C—COATING 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
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/04—Coating on selected surface areas, e.g. using masks
- C23C14/042—Coating on selected surface areas, e.g. using masks using masks
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/84—Processes or apparatus specially adapted for manufacturing record carriers
- G11B5/85—Coating a support with a magnetic layer by vapour deposition
Landscapes
- Chemical & Material Sciences (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Engineering & Computer Science (AREA)
- Materials Engineering (AREA)
- Mechanical Engineering (AREA)
- Metallurgy (AREA)
- Organic Chemistry (AREA)
- Manufacturing Of Magnetic Record Carriers (AREA)
- Thin Magnetic Films (AREA)
Description
本発明は、強磁性金属薄膜層を記録層とする磁
気記録媒体の製造方法に関し、特に斜方蒸着によ
り抗磁力制御を行う方法の改良を目的としてい
る。
磁気記録は高密度化の要求に対して、磁気記録
媒体の抗磁力を大きくすることで対応してきた
が、より短波長化が進むに従つて、磁化されるの
は、媒体の表面近くだけになるため、抗磁力の増
大の他に、飽和磁束密度の大きい磁性体の利用へ
と移行がはじまつている。
そのひとつは、従来の塗布形の延長上で、バイ
ンダ等の非磁性材料で稀釈されるものの、本質的
に飽和磁束密度の大きい、鉄系の強磁性金属又は
合金の微粒子を、酸化鉄の代わりに用いるもの
で、もう一方はバインダを用いない、強磁性金属
薄膜を磁気記録層とする媒体で、このタイプは薄
膜形成を真空蒸着で行うことから蒸着テープの名
で一部実用に供されるに至つている。
しかし蒸着テープは、まだ歴史も浅いので、工
業化に向けて、改良すべき課題もいくつか残つて
いる。
そのなかのひとつは抗磁力の安定な制御法の改
良であろう。
蒸着で安定に抗磁力を制御できる可能性のある
のは、特公昭41−19389号公報に開示されている
いわゆる斜方蒸着である。
しかしこの技術を工業化する上で解決すべき課
題が2つある。そのひとつは、蒸着効率が低いこ
とと、もうひとつは、本発明が解決しようとす
る、大きい抗磁力領域でのわずかな入射角変化に
対応して、抗磁力の変化が大きくなることであ
る。
この解決にとられるアプローチの方法には2つ
ある。そのひとつは材料に頼る方法特に雰囲気制
御との有効な組み合わせを利用する方法と、もう
ひとつは、入射角の制御を正確に行う方法であ
る。本発明は後者に主として係わるが、前者の実
施に於ても本発明の有効性は同じである。
以下に図面を用い本発明を説明する。
図は本発明を実施するための装置の一例を示
す。
これは二室構成の巻取式蒸着機と類似している
が、これによらずとも良く、非磁性層を配する場
合、キヤン等の冷却支持体を2ケ以上配設した方
が効果的である場合もあり、強磁性層を分割して
形成する場合に複数個の冷却支持体を配設する場
合も含めて、強磁性層形成に於ける制約に係わる
のが本発明である。
図では、回転キヤン4を冷却支持体として示し
たが、これによらず、例えばSUS304の薄い板を
接続してエンドレスベルトにして別の駆動機構で
駆動した回転ベルトを用い、それのひとつの面に
沿つて基板を移動するように構成することもでき
る。
回転キヤン4に沿つて基板1は送り出し軸11
より、捲き取り軸12へ移動する。なお捲き取り
に必要な他の公知の要素は略している。
真空槽5内は、基板1の捲き取り機構を主とし
て収納する上室6と、蒸発源とマスク機構等を収
納する下室7とに分けられ夫々独立した排気系1
0,9により所定の真空度に保持される。なお1
3は仕切板である。
蒸発源は、容器3と蒸着材料2で構式的に示し
たが、電子ビーム蒸発源、誘導加熱式蒸発源、等
公知の蒸発源の中より適宜選択される。
蒸発源より放射される蒸気流の一部限定された
入射角により成膜する場合で、基板にたてた法線
と該蒸気流とのなす角度で表わす入射角が45゜以
上になると鉄、コバルト、ニツケルそれらの合金
の一部は抗磁力が少しずつ増加をはじめ60゜あた
りより急激に増大し、75゜〜80゜あたりでは、入射
角が2〜3゜変化するだけで50〜100〔O¨e〕程度の
抗磁力変化がみられる。
それを防ぐため本発明では、入射角を限定する
マスクを金属ベルト8で構成し、このベルト8を
運動体とし(例えば矢印B方向に絶えず運動す
る)ドクターブレード16でこのベルト表面に蒸
着された強磁性材料をかき落し、例えば受皿18
(必要に応じて平面内に運動するようにし、回収
する強磁性材料のパツキングを有効に行えるよう
にする)に集める。14,15はフリーローラー
で冷却するか否かも自由である。19はニツプロ
ーラで、これによりベルトの移動を図つている。
固定マスク17は先端Tに付着した蒸着材により
θ1が変化しない位置に配設されなければならない
のは当然である。便宜的にSとPを結ぶ線と
とのなす角θ1を入射角と呼ぶが、実質的な蒸発位
置は点Sではなく、体積を有すると考えられてい
る蒸発源が存在していることはいうまでもない。
なお金属ベルトの蒸着される側は、極めて平滑
にすることが大切であることは、ブレードにより
有効に付着した蒸着材料をかき落すことの必要性
より相像される。
次に具体的に本発明の実施例について説明す
る。
〔実施例 1〕
キヤン直径100cm、キヤン幅65cm、金属ベルト
SUS304 65cm幅、長さ1.5m,=40cm、=
30cm。
50cm幅、長さ3000mのポリエチレンテレフタレ
ートフイルム9.5μを2本用意し、1本は本発明に
より入射角55゜で蒸着し、他の1本は比較として
従来法により、即ち防着板17をマスクとし初期
値が55゜となるようにずらして蒸着した。
その結果のうち抗磁力を長手方向にサンプリン
グして比較しまとめたものを下の表に示す。
The present invention relates to a method of manufacturing a magnetic recording medium having a ferromagnetic metal thin film layer as a recording layer, and particularly aims to improve a method of controlling coercive force by oblique evaporation. Magnetic recording has responded to demands for higher densities by increasing the coercive force of magnetic recording media, but as wavelengths continue to become shorter, only areas near the surface of the media are magnetized. Therefore, in addition to increasing coercive force, a shift has begun to the use of magnetic materials that have a large saturation magnetic flux density. One is an extension of the conventional coating method, in which fine particles of iron-based ferromagnetic metals or alloys, which are diluted with a non-magnetic material such as a binder but have essentially a high saturation magnetic flux density, are used instead of iron oxide. The other type is a medium that does not use a binder and has a ferromagnetic metal thin film as the magnetic recording layer.This type is used in some practical applications under the name evaporation tape because the thin film is formed by vacuum evaporation. It has reached this point. However, since vapor-deposited tape still has a short history, there are still some issues that need to be improved before it can be industrialized. One of these would be the improvement of a stable control method for coercive force. The so-called oblique evaporation method disclosed in Japanese Patent Publication No. 19389/1989 has the possibility of stably controlling the coercive force through evaporation. However, there are two issues that need to be resolved in order to commercialize this technology. One of these is that the deposition efficiency is low, and the other is that the change in coercive force becomes large in response to a slight change in the angle of incidence in the region of large coercive force, which is the problem that the present invention seeks to solve. There are two ways to approach this solution. One is a method that relies on materials, especially an effective combination with atmospheric control, and the other is a method that accurately controls the angle of incidence. Although the present invention mainly relates to the latter, the present invention is equally effective in implementing the former. The present invention will be explained below using the drawings. The figure shows an example of a device for implementing the invention. This is similar to a two-chamber roll-type vapor deposition machine, but it is not necessary to rely on this, and when disposing a non-magnetic layer, it is more effective to dispose two or more cooling supports such as cans. The present invention relates to restrictions in forming the ferromagnetic layer, including the case where a plurality of cooling supports are provided when the ferromagnetic layer is formed by dividing it. In the figure, the rotary can 4 is shown as a cooling support, but instead of using this, for example, a rotary belt connected with thin plates of SUS304 and made into an endless belt driven by a separate drive mechanism can be used. It is also possible to configure the substrate to move along. Along the rotation can 4, the substrate 1 is connected to the feed shaft 11.
Then, it moves to the winding shaft 12. Note that other known elements necessary for winding are omitted. The inside of the vacuum chamber 5 is divided into an upper chamber 6 which mainly houses a winding mechanism for the substrate 1, and a lower chamber 7 which houses an evaporation source, a mask mechanism, etc., and each has an independent exhaust system 1.
0.9 to maintain a predetermined degree of vacuum. Note 1
3 is a partition plate. Although the evaporation source is shown structurally as the container 3 and the evaporation material 2, it is appropriately selected from known evaporation sources such as an electron beam evaporation source, an induction heating type evaporation source, and the like. When forming a film using a partially limited incident angle of the vapor flow emitted from the evaporation source, if the angle of incidence expressed by the angle between the normal to the substrate and the vapor flow is 45° or more, iron, For some alloys of cobalt and nickel, the coercive force starts to increase little by little and increases sharply from around 60 degrees, and at around 75 degrees to 80 degrees, it increases by 50 to 100 with a change of only 2 to 3 degrees in the angle of incidence. A change in coercive force of about O¨e] is observed. In order to prevent this, in the present invention, a mask that limits the angle of incidence is constructed of a metal belt 8, and this belt 8 is used as a moving body (for example, it moves constantly in the direction of arrow B). Scrape off the ferromagnetic material, e.g.
(Move in a plane as necessary to enable effective packing of the ferromagnetic material to be collected). 14 and 15 may be cooled with free rollers or not. Reference numeral 19 is a nip roller, which is used to move the belt.
It goes without saying that the fixed mask 17 must be placed at a position where θ 1 does not change due to the vapor deposition material attached to the tip T. For convenience, the angle θ 1 formed by the line connecting S and P is called the incident angle, but the actual evaporation position is not the point S, but there is an evaporation source that is considered to have a volume. Needless to say. The fact that it is important to make the side of the metal belt on which the metal belt is deposited extremely smooth is consistent with the need to effectively scrape off the deposited material with the blade. Next, embodiments of the present invention will be specifically described. [Example 1] Can diameter 100cm, can width 65cm, metal belt
SUS304 65cm width, length 1.5m, = 40cm, =
30cm. Two 9.5μ polyethylene terephthalate films with a width of 50 cm and a length of 3000 m were prepared, one of which was deposited by the present invention at an incident angle of 55°, and the other film was deposited by the conventional method for comparison, that is, by masking the deposition prevention plate 17. The film was deposited at an angle of 55° to the initial value. Among the results, the coercive force was sampled in the longitudinal direction and compared and summarized in the table below.
実施例1と同一のキヤンで、=50cm、=
35cmで入射角72゜に設定し、表面マツトを形成し
たポリエチレンテレフタレート11.5μmを1500m
用意し、実施例1と同様の比較を行つた。ベルト
運動条件は5cm/secとし、キヤン温度は20℃一
定とした。
Co100%を0.1μmになるよう制御した磁性層の
抗磁力は初期から1450mまで10点調べたところ、
1060〜1070〔O¨e〕と極めて安定であつたのに対
し、従来法では0.1μmになるよう制御するのに、
基板の移動速度が初期値に比して30%低下し(本
発明の場合は一定速度である。)、抗磁力は1050
〔O¨e〕から1490〔O¨e〕まで増加した。
Co90% Cr10%について本発明により0.15μm
成膜したものについても同様の傾向を確かめた。
本発明では抗磁力1200〜1220〔O¨e〕、従来方式
では1200〜1590〔O¨e〕であつた。
〔実施例 3〕
回転キヤン径50cm、=34cm、=27cmと
し、下室雰囲気として外部より酸素を導入し
(0.1/min〜0.16/min)、2×10-5Torr〜4.5
×10-5TorrでCo100%、Co80%Ni20%、Co95%
W5%、Co98%Rh2%、を夫々、実施例2と同一
のポリエチレンテレフタレート基板に、0.15μm
蒸着した。
入射角35゜の場合と、入射角43゜の場合と、入射
角60゜の場合について、蒸着長2000mで従来方式
と比較した。
いずれの場合も本発明による媒体の抗磁力は安
定であつたのに対し、いずれの場合もおよそ
1000m過ぎるあたりから抗磁力の増加が従来例で
は目立つた。最も少いCo80%Ni20%の場合で初
期値に対して1950m位置で16%増、最大の変化率
は37%でCo95%W5%の入射角60゜の場合であつ
た。
〔実施例 4〕
防着板17をなくして、本発明におけるマスク
機構を入射角制御以外の目的に変形使用した。す
なわち図において破線で囲つた部分Kにもう一式
のベルトとブレードの組み合わせを配した。これ
により蒸着金属の回収が極めて効果的になされ
た。
これはCo95%Pt5%等の実施には極めて高い経
済効果をもたらすものであつた。
以上述べてきたように本発明の有効性は、基板
の種類、蒸着材料を選ばずに極めて高い。
又このマスクを二対として、垂直入射により、
垂直磁気記緑用媒体を得る場合にも有効であるな
ど、本発明の磁気記録媒体の製造に係わる有価値
性は長尺化がすすむ程大きい。
Same can as in Example 1, =50cm, =
The incident angle was set at 72° at 35cm, and the polyethylene terephthalate 11.5μm with a matt surface was exposed at 1500m.
A comparison was made in the same manner as in Example 1. The belt movement conditions were 5 cm/sec, and the can temperature was kept constant at 20°C. The coercive force of the magnetic layer with 100% Co controlled to 0.1 μm was investigated at 10 points from the initial stage to 1450 m.
It was extremely stable at 1060-1070〔O¨e〕, whereas with the conventional method, it was controlled to be 0.1μm, but
The moving speed of the substrate is reduced by 30% compared to the initial value (in the case of the present invention, it is a constant speed), and the coercive force is 1050.
It increased from [O¨e] to 1490 [O¨e]. 0.15 μm according to the present invention for Co90% Cr10%
A similar trend was confirmed for the film formed. In the present invention, the coercive force was 1200 to 1220 [O¨e], and in the conventional method, it was 1200 to 1590 [O¨e]. [Example 3] The rotation can diameters were 50 cm, = 34 cm, and = 27 cm, and oxygen was introduced from the outside as a lower chamber atmosphere (0.1/min to 0.16/min), and 2 × 10 -5 Torr to 4.5
×10 -5 Torr Co100%, Co80% Ni20%, Co95%
W5%, Co98% Rh2%, respectively, were placed on the same polyethylene terephthalate substrate as in Example 2 with a thickness of 0.15 μm.
Deposited. A comparison was made with the conventional method at a deposition length of 2000 m for the cases of an incident angle of 35°, 43°, and 60°. In all cases, the coercive force of the medium according to the present invention was stable;
In the conventional example, the increase in coercive force was noticeable after 1000m. In the case of 80% Co and 20% Ni, there was a 16% increase compared to the initial value at a position of 1950 m, and the maximum rate of change was 37% in the case of 95% Co, 5% W and an incident angle of 60°. [Example 4] The mask mechanism of the present invention was modified and used for purposes other than incident angle control by omitting the adhesion prevention plate 17. That is, in the figure, another belt and blade combination is arranged in a portion K surrounded by a broken line. This made it possible to recover the deposited metal very effectively. This brought extremely high economic effects to the implementation of Co95% Pt5%, etc. As described above, the effectiveness of the present invention is extremely high regardless of the type of substrate or vapor deposition material. Also, with two pairs of these masks, by vertical incidence,
The value of manufacturing the magnetic recording medium of the present invention increases as the length of the magnetic recording medium increases, as it is also effective in obtaining a medium for perpendicular magnetic recording.
図は本発明を実施するための装置の一例を示す
図である。
1…基板、2…蒸着材料、3…容器、4…回転
キヤン、5…真空槽、8…金属ベルト、11…捲
き取り軸、12…送り出し軸、16…ドクターブ
レード、17…固定マスク。
The figure is a diagram showing an example of an apparatus for implementing the present invention. DESCRIPTION OF SYMBOLS 1... Substrate, 2... Evaporation material, 3... Container, 4... Rotating can, 5... Vacuum chamber, 8... Metal belt, 11... Winding shaft, 12... Feeding shaft, 16... Doctor blade, 17... Fixed mask.
Claims (1)
板に強磁性材料を蒸着する際、該強磁性材料蒸気
の基板への入射角規制を、回転駆動された耐熱性
ベルトにより行なうことを特徴とする磁気記録媒
体の製造方法。1. When depositing a ferromagnetic material onto a polymer molded substrate moving along a cooling support, the angle of incidence of the ferromagnetic material vapor onto the substrate is regulated by a rotationally driven heat-resistant belt. A method for manufacturing a magnetic recording medium.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56131177A JPS5832235A (en) | 1981-08-20 | 1981-08-20 | Method for manufacturing magnetic recording media |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56131177A JPS5832235A (en) | 1981-08-20 | 1981-08-20 | Method for manufacturing magnetic recording media |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5832235A JPS5832235A (en) | 1983-02-25 |
| JPH0154777B2 true JPH0154777B2 (en) | 1989-11-21 |
Family
ID=15051801
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56131177A Granted JPS5832235A (en) | 1981-08-20 | 1981-08-20 | Method for manufacturing magnetic recording media |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5832235A (en) |
-
1981
- 1981-08-20 JP JP56131177A patent/JPS5832235A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5832235A (en) | 1983-02-25 |
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