JPH0572014B2 - - Google Patents
Info
- Publication number
- JPH0572014B2 JPH0572014B2 JP57233620A JP23362082A JPH0572014B2 JP H0572014 B2 JPH0572014 B2 JP H0572014B2 JP 57233620 A JP57233620 A JP 57233620A JP 23362082 A JP23362082 A JP 23362082A JP H0572014 B2 JPH0572014 B2 JP H0572014B2
- Authority
- JP
- Japan
- Prior art keywords
- electron beam
- gas
- ferromagnetic
- ferromagnetic material
- inert gas
- 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 - Lifetime
Links
Classifications
-
- 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
- Manufacturing Of Magnetic Record Carriers (AREA)
Description
産業上の利用分野
本発明は金属薄膜型磁気記録媒体の製造方法に
関し、特に短波長域での優れたC/N特性を有す
る媒体を再現よく生産する方法に関するものであ
る。
従来例の構成とその問題点
近年、高密度記録に適する媒体として、強磁性
薄膜を磁気記録層とする媒体が注目され、一部で
はオーデイオ用途で実用に供されている。
金属薄膜型磁気記録媒体をビデオ用途に実用化
する努力を各方面で続けられているものの、公知
の斜め蒸着法による蒸着テープでは、磁性の不均
一性からくるノイズが大きく、感度が高いにもか
かわらず、結果的にC/Nが低いという課題があ
り、本発明者等は、既に酸素を真空雰囲気に導入
することと、変形した斜め蒸着の組み合わせによ
る、前記課題を改良する方法を既に提案した。
(特公昭57−29770号公報)
この方法により、生産性の面と、C/N面での
改良は見込めるものの、長尺での安定性、ロツト
間の再現性は充分ではなかつた。
発明の目的
金属薄膜型磁気記録媒体の製造法で、長尺での
安定性、ロツト間の再現性の改良された方法を提
供する。
発明の構成
回転支持体に沿つて移動する基材に、酸化性気
体を最大分圧とする真空雰囲気で、強磁性層を蒸
着法により形成する際、前記強磁性材料の蒸発を
集束電子ビームの衝撃加熱にて行うと共に、前記
電子ビームの走査部分及び基材が強磁性体の蒸着
を受ける部分の近傍より主として排気することを
要旨とするものである。
強磁性材料の加熱蒸発に用いる集束電子ビーム
が、大電流の電子ビームであると、電子同志の反
発力により、ビームが発散する傾向を持つ。しか
し、大電流の電子ビームに不活性ガスを導入し、
不活性ガスと電子との相互作用で発生する不活性
ガスのイオンが電子を引きつけ、電子同志の反発
力を小さくするガス集束法を用いると、大電流の
電子ビームの発散を防止し、電子ビームを集束さ
せることができる。従つて、大電流の電子ビーム
の集束には、ガス集束法が最も適しており、その
結果、投入電力密度が大きくとれ、Co等の高融
点材料の大量蒸発を実現することができる。
熱電子の発生源が、工業的には、高温のタング
ステンで構成されるため、酸素をガス集束のため
に用いると、前記タングステンが急速に酸化され
破損することが多く実用にならないからである。
しかしこの不活性気体は、強磁性薄膜形成雰囲
気に流入し、酸素効果を妨害する。
即ち酸素効果により極微細化した磁区が、局所
的にアルゴン等の不活性気体の影響により、大き
な磁区が発生し、その結果短波長域でのノイズを
大きくすると共に、かつロツト間の再現性を悪く
するもとになるのである。
この原因を排除する最も優れた実用的な方法は
電子ビームの走査部分(これは、広幅の基材に均
一な膜厚、磁気特性を得る上で不可欠の構成要素
である。)近傍より、主排気を行うことである。
ここでいう主排気の意味は、巻取り蒸着では一
般に蒸着部分と巻取部分とに2分して別々に排気
したり、グロー処理するために、補助的な排気系
を準備することが多いのであるが、蒸着雰囲気を
最大の排気速度で排気する排気系を指しており、
蒸着室に2系統排気系が配設されても、いずれか
のうち大きな排気速度を有する排気系による排気
を主排気と呼んでいるのである。
前記した主排気法の他の作用は、酸素等の酸化
性気体を真空槽内に導入することで、強磁性金属
粒子の表面を部分酸化する際、基材が蒸着時に受
ける熱で基材の温度があがり、基材より放出され
る水蒸気等の気体が酸素を妨害する不都合を無視
できる程度に排気してしまう作用である。
そのため、前記した主排気は、電子ビームの走
査部分及び基材が強磁性体の蒸着を受ける部分の
近傍より行われるような構成が最も優れていると
いえる。
実施例の説明
第1図は本発明を実施するのに用いた装置の要
部構成図である。
基材1は、回転キヤン2の周側面に沿つて送り
出し軸3より、巻き取り軸4へ移動するよう構成
される。巻取り系の公知要素で、巻取り蒸着には
不可欠ではあつても、本発明に直接関連のないも
のは、簡略化して省いてある。
蒸発源容器5に、保持された強磁性材料6の加
熱は、加速された電子ビーム7により行われる。
電子発生源8はピアス型電子銃が用いられ、バ
リアブルリークバルブ9の調節により、ガス集束
のためのガスを外部より導入する。
ガス集束された電子ビーム7は、走査コイル1
0の発生する走査磁界により、基材の幅方向に走
査され、強磁性材料6の蒸発分布を制御し、膜厚
をはじめ、所要の磁気特性が基材の幅方向に均一
になるよう調整される。
主排気系11は真空槽12内部を排気するので
あるが、基材が強磁性体の蒸着を受ける部分の近
傍で、構造的に許される限り、前記電子ビームの
走査部分の近傍で構成されるのが望ましい。
その結果、模式的に示したように、ガス集束用
のガス13、基材等からでる不要のガス14が有
効に排気され、バイアブルリークバルブ15の調
節により真空槽内に導入される、例えば酸素等の
酸化性気体の、強磁性蒸着膜に与える効果が再現
よく得られることになる。16は、磁気特性の調
節のために、入射角を限定するマスクである。
比較の例として、真空槽の基板の幅方向の中心
位置で、回転支持体直下に、排気系17を配設し
た場合(破線で示した。)を取りあげた。
〔実施例 1〕
図に要部構成を示した装置により、第1表の条
件で、50cm幅、長さ4000m、厚み10μmのポリエ
チレンテレフタレート基材上に蒸着を実施し、磁
気記録媒体を得た。
比較例は、前記した排気系位置を用いた場合で
ある。
入射角は45°一度とし、回転支持体の表面温度
は5±0.5℃に制御した。
他にポリエチレンテレフタレートの厚みを8μm
から25μmまで変化させ、他の条件はサンプル2
の条件で、磁気記録媒体を得た。
基材の種類については、ポリエチレンテレフタ
レートの他に、ポリアミド、ポリイミドについて
も前記同様に本発明を実施した。
磁性材料については、Co,CoNi系合金、
CoNiCr系合金を中心に検討し、CoAg,CoFe,
CoSi,CoPt等についても実施した。
〔実施例 2〕
実施例1の系で、基材長さを3倍の12000mと
した場合について本発明と比較例を検討した。
INDUSTRIAL APPLICATION FIELD The present invention relates to a method for manufacturing a metal thin film type magnetic recording medium, and particularly to a method for reproducibly producing a medium having excellent C/N characteristics in a short wavelength region. Structures of Conventional Examples and Their Problems In recent years, media with a ferromagnetic thin film as a magnetic recording layer have attracted attention as media suitable for high-density recording, and some have been put to practical use in audio applications. Efforts are being made in various fields to put metal thin film magnetic recording media into practical use for video applications, but tapes made using the known oblique evaporation method produce large noise due to non-uniformity of magnetism, and although they have high sensitivity, However, as a result, there is a problem that the C/N is low, and the present inventors have already proposed a method to improve the problem by a combination of introducing oxygen into a vacuum atmosphere and modified oblique evaporation. did.
(Japanese Patent Publication No. 57-29770) Although improvements in productivity and C/N can be expected with this method, stability in long lengths and reproducibility between lots were not sufficient. OBJECTS OF THE INVENTION It is to provide a method for manufacturing a metal thin film type magnetic recording medium with improved long-length stability and lot-to-lot reproducibility. Structure of the Invention When a ferromagnetic layer is formed by vapor deposition on a substrate moving along a rotating support in a vacuum atmosphere with a maximum partial pressure of oxidizing gas, the evaporation of the ferromagnetic material is caused by a focused electron beam. The gist of this method is to carry out impact heating and to exhaust air mainly from the vicinity of the scanning part of the electron beam and the part where the ferromagnetic material is deposited on the base material. If the focused electron beam used to heat and evaporate a ferromagnetic material is an electron beam with a large current, the beam tends to diverge due to the repulsive force between the electrons. However, by introducing an inert gas into the high-current electron beam,
Using the gas focusing method, in which inert gas ions generated by the interaction between inert gas and electrons attract electrons and reduce the repulsive force between electrons, it is possible to prevent the divergence of large current electron beams and can be focused. Therefore, the gas focusing method is most suitable for focusing a large current electron beam, and as a result, the input power density can be increased and large amounts of high melting point materials such as Co can be evaporated. This is because, industrially, the source of thermionic electrons is composed of high-temperature tungsten, so if oxygen is used for gas focusing, the tungsten is often rapidly oxidized and damaged, making it impractical. However, this inert gas flows into the ferromagnetic thin film formation atmosphere and interferes with the oxygen effect. In other words, the magnetic domains that have become extremely fine due to the oxygen effect are locally generated into large magnetic domains due to the influence of inert gas such as argon, which increases noise in the short wavelength range and reduces the reproducibility between lots. It becomes a source of deterioration. The best practical way to eliminate this cause is to focus the scanning part of the electron beam (this is an essential component in obtaining uniform film thickness and magnetic properties on a wide substrate) from the vicinity. It is to exhaust the air. The meaning of main exhaust here is that in winding deposition, the deposition area and the winding area are generally separated into two parts and evacuated separately, or an auxiliary exhaust system is often prepared for glow treatment. However, it refers to an exhaust system that exhausts the deposition atmosphere at the maximum exhaust speed.
Even if two exhaust systems are provided in the deposition chamber, the exhaust system that has the higher exhaust speed is called the main exhaust system. Another effect of the main evacuation method described above is that when the surface of the ferromagnetic metal particles is partially oxidized by introducing an oxidizing gas such as oxygen into the vacuum chamber, the heat that the base material receives during vapor deposition is used to oxidize the base material. This is an effect in which the temperature rises and gases such as water vapor released from the base material are exhausted to such an extent that the inconvenience of interfering with oxygen can be ignored. Therefore, it can be said that a configuration in which the above-mentioned main exhaust is performed from near the scanning part of the electron beam and the part where the substrate receives the ferromagnetic material deposition is most excellent. DESCRIPTION OF EMBODIMENTS FIG. 1 is a block diagram of the main parts of an apparatus used to carry out the present invention. The base material 1 is configured to move from the feed shaft 3 to the wind-up shaft 4 along the circumferential surface of the rotary can 2. Known elements of the winding system that are essential for winding deposition but are not directly related to the present invention are simplified and omitted. The ferromagnetic material 6 held in the evaporation source container 5 is heated by an accelerated electron beam 7. A piercing type electron gun is used as the electron source 8, and a variable leak valve 9 is adjusted to introduce gas from the outside for gas focusing. The gas-focused electron beam 7 passes through the scanning coil 1
The scanning magnetic field generated by the ferromagnetic material 6 is scanned in the width direction of the base material, and the evaporation distribution of the ferromagnetic material 6 is controlled, and the required magnetic properties including the film thickness are adjusted to be uniform in the width direction of the base material. Ru. The main exhaust system 11 exhausts the inside of the vacuum chamber 12, and is configured near the part of the substrate where the ferromagnetic material is deposited, and as close to the part where the electron beam is scanned as structurally permitted. is desirable. As a result, as schematically shown, the gas 13 for gas focusing, the unnecessary gas 14 coming from the base material, etc. are effectively exhausted, and are introduced into the vacuum chamber by adjusting the viaable leak valve 15, e.g. The effect of oxidizing gas such as oxygen on the ferromagnetic deposited film can be obtained with good reproducibility. 16 is a mask that limits the angle of incidence in order to adjust the magnetic properties. As a comparative example, a case was taken up in which the exhaust system 17 was disposed directly below the rotating support at the center position in the width direction of the substrate of the vacuum chamber (indicated by a broken line). [Example 1] Vapor deposition was carried out on a polyethylene terephthalate base material with a width of 50 cm, a length of 4000 m, and a thickness of 10 μm under the conditions shown in Table 1 using the apparatus whose main part configuration is shown in the figure to obtain a magnetic recording medium. . The comparative example is a case where the above-mentioned exhaust system position is used. The angle of incidence was 45°, and the surface temperature of the rotating support was controlled at 5±0.5°C. In addition, the thickness of polyethylene terephthalate was 8 μm.
to 25 μm, and the other conditions were Sample 2.
A magnetic recording medium was obtained under these conditions. Regarding the type of base material, in addition to polyethylene terephthalate, the present invention was also carried out using polyamide and polyimide in the same manner as described above. For magnetic materials, Co, CoNi alloys,
Focusing on CoNiCr alloys, CoAg, CoFe,
Tests were also conducted for CoSi, CoPt, etc. [Example 2] In the system of Example 1, the present invention and a comparative example were examined in the case where the length of the base material was tripled to 12000 m.
【表】
発明の効果
第1表にC/Nの値と再現性について示した。
C/Nの値については、キヤリアの中心周波数
を5.5MHzにとり、キヤリア近傍のノイズが、磁
気特性の不均一性を反映していると考えられるこ
とから、5MHzのノイズを測定して算出した。
基準のテープは、改良されたγ−Fe2O3の塗布
型テープで市販されてるものの中で、最もC/N
の優れたものを用いた。
テープとヘツドの相対速度は2m/secとした。
また、再現性については、同一条件設定で5ロ
ツトの間のC/Nのバラツキで比較した。
第1表より明らかなように、C/N、再現性共
に本発明品が優れている。
これらの効果は、第1表に示さなかつた、前記
の多くの実施例でも確認された。
又実施例2についても得られたC/Nについて
は殆んど実施例1と同じであつたが、再現性につ
いてみると、従来例と本発明の差は更に開き実施
例−1の1から5の条件相当では±1.5dBであつ
たのに対し、比較例(6,7相当条件)では夫々
±4.6dB±5.9dBであつた。
本発明は前記実施例に限定されるものではない
のは勿論で、使用される装置条件も、回転キヤン
によらない、例えばエンドレスベルトで構成され
た回転支持体でも良いし、排気系の基本要件を満
たせば、種類は問わないものである。
近年より短波長化の進む磁気記録分野に、優れ
た媒体の大量供給を可能にする本発明の有価値性
は極めて大きい。[Table] Effects of the invention Table 1 shows the C/N values and reproducibility. The C/N value was calculated by setting the center frequency of the carrier to 5.5 MHz and measuring the noise at 5 MHz, since it is thought that the noise near the carrier reflects the non-uniformity of the magnetic properties. The standard tape has the highest C/N among the improved γ-Fe 2 O 3 coated tapes commercially available.
The best one was used. The relative speed between the tape and the head was 2 m/sec. Regarding reproducibility, the variation in C/N between 5 lots was compared under the same conditions. As is clear from Table 1, the product of the present invention is superior in both C/N and reproducibility. These effects were also confirmed in many of the above examples not shown in Table 1. In addition, the C/N obtained in Example 2 was almost the same as in Example 1, but when looking at reproducibility, the difference between the conventional example and the present invention was even wider, from 1 of Example-1. In the case corresponding to condition No. 5, it was ±1.5 dB, whereas in the comparative example (conditions equivalent to No. 6 and 7), it was ±4.6 dB and ±5.9 dB, respectively. It goes without saying that the present invention is not limited to the above-mentioned embodiments, and the equipment conditions used may be independent of the rotation can, for example, a rotating support made of an endless belt, and the basic requirements of the exhaust system. As long as it satisfies the following, the type does not matter. The present invention is extremely valuable in that it enables the supply of excellent media in large quantities to the field of magnetic recording, where wavelengths are increasingly becoming shorter in recent years.
図は本発明の製造方法の実施に用いられる巻取
蒸着装置の一例の要部構成図である。
1……基材、2……回転キヤン、5……蒸発源
容器、6……蒸着材料、7……電子ビーム、8…
…電子発生源、11……排気系。
The figure is a diagram illustrating the main part of an example of a winding vapor deposition apparatus used to carry out the manufacturing method of the present invention. DESCRIPTION OF SYMBOLS 1... Base material, 2... Rotation can, 5... Evaporation source container, 6... Vapor deposition material, 7... Electron beam, 8...
...Electron source, 11...Exhaust system.
Claims (1)
気体を最大分圧とする真空雰囲気で、強磁性層を
蒸着させる方法において、集束電子ビームを走査
する手段より手前であつて、電子ビームが通過す
る通路に、不活性ガスを導入する不活性ガス導入
手段を備えたガス集束型ビアス電子銃が放射する
前記集束電子ビームによる衝撃加熱にて、強磁性
材料の蒸発を行うと共に、前記集束電子ビームの
走査部分及び前記基材が前記強磁性層の蒸着を受
ける部分の近傍より主として排気することを特徴
とする金属薄膜型磁気記録媒体の製造方法。1. In a method of depositing a ferromagnetic layer on a substrate moving along a rotating support in a vacuum atmosphere with maximum partial pressure of an oxidizing gas, The ferromagnetic material is evaporated by impact heating by the focused electron beam emitted by a gas focusing type bias electron gun equipped with an inert gas introducing means for introducing an inert gas into the passage through which the ferromagnetic material passes, and the focused electron beam A method for manufacturing a metal thin film type magnetic recording medium, characterized in that exhaust is mainly carried out from the vicinity of a scanning portion of an electron beam and a portion of the substrate where the ferromagnetic layer is deposited.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57233620A JPS59124037A (en) | 1982-12-29 | 1982-12-29 | Manufacture of metallic thin-film type magnetic recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57233620A JPS59124037A (en) | 1982-12-29 | 1982-12-29 | Manufacture of metallic thin-film type magnetic recording medium |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59124037A JPS59124037A (en) | 1984-07-18 |
| JPH0572014B2 true JPH0572014B2 (en) | 1993-10-08 |
Family
ID=16957896
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57233620A Granted JPS59124037A (en) | 1982-12-29 | 1982-12-29 | Manufacture of metallic thin-film type magnetic recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59124037A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS59210539A (en) * | 1983-05-16 | 1984-11-29 | Hitachi Condenser Co Ltd | Producer of magnetic recording medium |
-
1982
- 1982-12-29 JP JP57233620A patent/JPS59124037A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59124037A (en) | 1984-07-18 |
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