JPH0434205B2 - - Google Patents

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Publication number
JPH0434205B2
JPH0434205B2 JP59170592A JP17059284A JPH0434205B2 JP H0434205 B2 JPH0434205 B2 JP H0434205B2 JP 59170592 A JP59170592 A JP 59170592A JP 17059284 A JP17059284 A JP 17059284A JP H0434205 B2 JPH0434205 B2 JP H0434205B2
Authority
JP
Japan
Prior art keywords
thin film
gas
magnetic
metal thin
ferromagnetic metal
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
Application number
JP59170592A
Other languages
Japanese (ja)
Other versions
JPS6150218A (en
Inventor
Tadashi Yasunaga
Ryuji Shirahata
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.)
Fujifilm Holdings Corp
Original Assignee
Fuji Photo Film 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 Fuji Photo Film Co Ltd filed Critical Fuji Photo Film Co Ltd
Priority to JP17059284A priority Critical patent/JPS6150218A/en
Publication of JPS6150218A publication Critical patent/JPS6150218A/en
Publication of JPH0434205B2 publication Critical patent/JPH0434205B2/ja
Granted legal-status Critical Current

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  • Manufacturing Of Magnetic Record Carriers (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

〔産業上の利用分野〕 本発明は、基体上に磁気記録層として強磁性薄
膜を設けてなる磁気記録媒体の製造方法に関し、
とくに磁気特性にすぐれる金属薄膜型磁気記録媒
体の製造方法に関する。 〔従来技術〕 従来磁気記録媒体としては、非磁性支持体上に
γ−Fe2O3、Coをドープしたγ−Fe2O3、Fe3O4
CoをドープしたFe3O4、γ−Fe2O3とFe3O4のベ
ルトライド化合物、CrO2等の磁性粉末あるいは
強磁性合金粉末等を粉末磁性材料を塩化ビニル−
酢酸ビニル共重合体、スチレン−ブタジエン共重
合体、エポキシ樹脂、ポリウレタン樹脂等の有機
バインダー中に分散せしめたものを塗布し乾燥さ
せる塗布型のものが広く使用されてきている。近
年高密度記録への要求の高まりと共に真空蒸着、
スパツタリング、イオンプレーテイング等のペー
パーデポジシヨン法あるいは電気メツキ、無電解
メツキ等のメツキ法により形成される強磁性金属
薄膜を磁気記録層とする、バインダーを使用しな
い、いわゆる非バインダー型磁気記録媒体が注目
を浴びており実用化への努力が種々行なわれてい
る。 従来の塗布型の磁気記録媒体では主として強磁
性金属より飽和磁化の小さい金属酸化物を磁性材
料として使用しているため、高密度記録に必要な
磁性層薄層化が信号出力の低下をもたらすため限
界にきており、かつその製造工程も複雑で、溶剤
回収あるいは公害防止のための大きな附帯設備を
要するという欠点を有している。非バインダー型
の磁気記録媒体では上記酸化物より大きな飽和磁
化を有する強磁性金属をバインダーの如き非磁性
物質を含有しない状態で薄膜として形成せしめる
ため、高密度記録化のために超薄層化できるとい
う利点を有し、しかもその製造工程はより簡略化
される。 高密度記録用の磁気記録媒体に要求される条件
の一つとして、高抗磁力化、薄形化が理論的にも
実験的にも提唱されており、塗布型の磁気記録媒
体よりも一桁小さい薄層化が容易で、飽和磁束密
度の大きい非バインダー型磁気記録媒体への期待
は大きい。 とくに真空蒸着による方法は、メツキの場合の
ような排液処理を必要とせず製造工程も簡単で膜
の析出速度も大きくできるため非常にメリツトが
大きい。真空蒸着によつて磁気記録媒体に望まし
い抗磁力および角型性を有する磁性膜を製造する
方法としては、米国特許3342632号、同3342633号
等に述べられている斜め蒸着法が知られている。 実際にテープ状基体に斜め蒸着法により強磁性
金属薄膜を設け磁気記録媒体を製造するに際して
は、テープ状基体を冷却キヤンに沿つて搬送せし
め、蒸発源より蒸発せしめられた磁性金属材料の
蒸気流を、移動するテープ状基体に斜めに入射蒸
着せしめる方法が行なわれる。 その際、基体に対し入射する蒸気流の入射角が
大きいほど高抗磁力の磁性薄膜が得られるが入射
角が大きいと蒸着効率が低下する傾向があり製造
上好ましくない。比較的低入射角にて抗磁力の高
い磁性薄膜を形成させる方法として斜め蒸着の際
に酸素ガスを導入させる方法が提案されている。
例えば特開昭58−41443号には、テープ状移動基
体に対する蒸気流の入射角(θ)が高入射角
(θmax)から低入射角(θmin)へと連続的に変
化するように前記基体を移動せしめると共に、低
入射角(θmin)近傍に酸化性ガスを導入する方
法が開示されている。この方法によれば高抗磁力
の膜は得られるが、角型性が劣化するという欠点
を有していた。 〔発明の目的〕 本発明は、高密度記録に適した高抗磁力と高角
型比とを有す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。 〔発明の構成〕 本発明は、非磁性基体上に斜め蒸着法により強
磁性金属薄膜を形成してなる磁気記録媒体の製造
方法において、斜め蒸着による強磁性金属薄膜形
成後、同一真空系内において該強磁性金属薄膜表
面に該薄膜を加熱しつつO2ガスを主成分とする
気流を吹きつける、あるいはまた加熱したO2
スを主成分とする気流を吹きつけることによる磁
気記録媒体の製造方法に関する。 ここで基体としてはポリエチレンテレフタレー
ト、ポリイミド、ポリ塩化ビニル、三酢酸セルロ
ース、ポリカボネート、ポリエチレンナフタレー
ト等のプラスチツクベース、またAl、Ti、ステ
ンレス鋼等を使用することができる。 また、磁性層材料となる強磁性金属・合金とし
てはFe、Co、Ni等の強磁性金属、また、Fe−
Co、Fe−Ni、Co−Ni、Fe−Co−Ni、Fe−Rh、
Fe−Cu、Co−Cu、Co−Au、Co−Y、Co−La、
Co−Pr、Co−Gd、Co−Sm、Co−Pt、Ni−Cu、
Mn−Bi、Mn−Sb、Mn−Al、Fe−Cr、Co−
Cr、Ni−Cr、Fe−Co−Ni、Fe−Co−Cr、Ni−
Co−Cr等の強磁性合金が挙げられる。 これらのうち特に好ましいのはCo、あるいは
Coを50重量%以上含有する合金である。蒸着の
際強磁性金属の蒸気流にO2ガス、N2ガス等を導
入せしめても良い。 本発明において斜め蒸着法とは、米国特許
3342632号、同3342633号等に開示されている蒸着
法である。さらに本発明において同一真空系内と
は真空中において斜め蒸着法により形成された強
磁性金属薄膜を大気中に戻すことなく蒸着時の真
空系と同じ真空系内にて気流吹きつけを実施する
ものである。気流吹きつけは蒸着真空室と同一真
空室内にて行なうのが好ましいが、蒸着真空室と
分離された別個の真空室で実施しても良い。この
際、気流吹きつけの真空室の真空度は蒸着真空室
の10-2〜102倍とすることができる。 本発明において用いられる製造装置の一例が第
1図に示されている。真空槽1の内部には回転キ
ヤン2、蒸発源3が設けられており、蒸発源3か
らの蒸気流はマスク4により所望の蒸気流成分の
みが回転キヤン2に到達するように設計されてい
る。真空槽1内には強磁性金属薄膜表面に気流を
吹きつけるためのノズル5が設けられている。ノ
ズル5にはヒーター6が巻回されている。 送り出しロール7より供給された基体8は回転
キヤン2に沿つて走行し、巻き取りロール9に巻
き取られる。この走行途中において蒸発源3内の
強磁性金属・合金は基体8上に真空蒸着され、ひ
き続きヒーター5で加熱されたガス気流がノズル
5により基体8上の強磁性薄膜表面に吹きつけら
れる。強磁性金属薄膜の形成の際には回転キヤン
1の内部に冷媒を循環せしめて回転キヤン表面を
15℃以下に保持せしめることが好ましい。 第2図には本発明において用いられる製造装置
の他の一例が示されている。真空槽21の内部に
は回転キヤン22,23が設けられており、基体
24は送り出しロール25から回転キヤン22お
よび回転キヤン23に沿つて搬送された後、巻き
取りロール26に巻き取られる。回転キヤン22
の下方には蒸発源27が配設されており、蒸発源
27からの蒸気流はマスク28により所望の蒸気
流成分のみが回転キヤン22上の基体24表面に
達するようになつている。真空槽21は排気口2
9を介して真空排気される一方、ガス供給管30
によりO2ガスを主成分とするガスが供給される
ようになつている。ガス供給管30の先端にはノ
ズル31が設けられていて、回転キヤン23に沿
つて移動する基体24上に形成された蒸着磁性金
属薄膜表面にO2ガスを主成分とするガスを吹き
つける。回転キヤン22の内部には冷媒を循環せ
しめて回転キヤン表面を15℃以下に保持せしめる
と共に回転キヤン23の内部には温媒を循環せし
め蒸着磁性金属薄膜を加熱せしめる機構になつて
いる。 強磁性金属薄膜の形成後にO2ガス、N2ガス等
を吹きつけ、しわの発生を防止する方法(特開昭
55−14569号)、強磁性金属薄膜の形成後に磁性膜
を酸化性雰囲気にさらし耐蝕性を改良する方法
(特開昭57−198543号)、強磁性金属薄膜の形成後
に磁性膜を酸化性ガスを用いたグロー放電雰囲気
にさらし耐蝕性を改良する方法(特開昭58−
17544号)、さらには、強磁性金属薄膜を形成した
後、磁性膜を加熱した状態にてオゾン雰囲気にさ
らし、繰返し走行、高温高湿中での耐久性を改良
する方法(特開昭59−63031)などが知られてい
るが、本発明は、強磁性金属薄膜を斜め蒸着法に
より形成した後、磁性金属薄膜を加熱した状態に
てO2ガスを主成分とするガスを磁性金属薄膜表
面に吹き付けることにより、きわめて良好な磁気
特性を有する磁気記録媒体を得るものであつて、
上記公知の技術では予想できない新規な磁気記録
媒体の製造方法に関する。さらに、本発明では強
磁性金属薄膜を斜め蒸着による形成した後、加熱
したO2ガスを主成分とする気流を磁性金属薄膜
面に吹き付けることによりきわめて良好な磁気特
性を有する磁気記録媒体の得られることを見出し
たもので、従来技術では予想できぬ新規な技術で
ある。 本発明によりテープ状磁気記録媒体を製造する
場合には、強磁性金属薄膜表面にO2を主体とす
るガス気流を吹き付ける際テープ状基体を回転キ
ヤンに沿つて搬送させつつ実施するのが好まし
い。しかもこの際回転キヤンの中心からガス導入
部迄の距離(R)と回転キヤンの半径(r)との
比R/rが1.01から1.20の範囲となるようにガス
吹き付け部を配設するのが好ましい。 以下実施例に即して本発明の説明を行なう。本
実施例が本発明の適用範囲を限定するものではな
い。 実施例 1 第1図に示す製造装置を用いて12.5μm厚のポ
リエチレンテレフタレートフイルム上に膜厚1500
Åのコバルト蒸着磁性薄膜をO2ガスを導入しな
がら斜め蒸着法により形成し、磁気テープを作製
した。得られた磁気テープの磁気特性を振動型磁
束計(VSM)にて測定した。この結果を下表に
示す。
[Industrial Application Field] The present invention relates to a method for manufacturing a magnetic recording medium in which a ferromagnetic thin film is provided as a magnetic recording layer on a substrate.
In particular, it relates to a method of manufacturing a metal thin film magnetic recording medium with excellent magnetic properties. [Prior art] Conventional magnetic recording media include γ-Fe 2 O 3 , Co-doped γ-Fe 2 O 3 , Fe 3 O 4 ,
Co-doped Fe 3 O 4 , γ-Fe 2 O 3 and Fe 3 O 4 bertolide compounds, magnetic powders such as CrO 2 or ferromagnetic alloy powders, etc. are used as powder magnetic materials such as vinyl chloride.
Coating type materials have been widely used, in which a material dispersed in an organic binder such as vinyl acetate copolymer, styrene-butadiene copolymer, epoxy resin, or polyurethane resin is coated and dried. In recent years, with the increasing demand for high-density recording, vacuum deposition,
A so-called non-binder type magnetic recording medium that does not use a binder has a magnetic recording layer that is a ferromagnetic metal thin film formed by a paper deposition method such as sputtering or ion plating, or a plating method such as electroplating or electroless plating. It is attracting attention and various efforts are being made to put it into practical use. Conventional coating-type magnetic recording media mainly use metal oxides, which have lower saturation magnetization than ferromagnetic metals, as magnetic materials, so the thinning of the magnetic layer required for high-density recording results in a reduction in signal output. It has reached its limit, and its manufacturing process is complicated, and it has the drawback of requiring large auxiliary equipment for solvent recovery and pollution prevention. In non-binder type magnetic recording media, a ferromagnetic metal having a saturation magnetization higher than that of the above-mentioned oxides is formed as a thin film without containing a non-magnetic substance such as a binder, so it can be made into an ultra-thin layer for high-density recording. This has the advantage that the manufacturing process is further simplified. As one of the requirements for magnetic recording media for high-density recording, high coercive force and thinness have been proposed both theoretically and experimentally. There are great expectations for non-binder type magnetic recording media that can be easily made into small and thin layers and have a high saturation magnetic flux density. In particular, the vacuum deposition method is very advantageous because it does not require drainage treatment as is the case with plating, the manufacturing process is simple, and the deposition rate of the film can be increased. As a method for manufacturing a magnetic film having coercive force and squareness desirable for magnetic recording media by vacuum deposition, the oblique deposition method described in US Pat. Nos. 3,342,632 and 3,342,633 is known. In practice, when manufacturing a magnetic recording medium by forming a ferromagnetic metal thin film on a tape-shaped substrate by oblique vapor deposition, the tape-shaped substrate is conveyed along a cooling can, and the vapor of the magnetic metal material evaporated from an evaporation source flows. is deposited obliquely onto a moving tape-like substrate. At this time, a magnetic thin film with a high coercive force can be obtained as the incident angle of the vapor flow that is incident on the substrate is large, but a large incident angle tends to lower the vapor deposition efficiency, which is not preferable in terms of manufacturing. A method of introducing oxygen gas during oblique deposition has been proposed as a method for forming a magnetic thin film with high coercive force at a relatively low incident angle.
For example, Japanese Patent Application Laid-open No. 58-41443 discloses that a tape-shaped moving base is arranged so that the incident angle (θ) of the vapor flow on the base changes continuously from a high incidence angle (θmax) to a low incidence angle (θmin). A method is disclosed in which the oxidizing gas is introduced into the vicinity of a low incident angle (θmin). According to this method, a film with high coercive force can be obtained, but it has the disadvantage that the squareness deteriorates. [Object of the Invention] An object of the present invention is to provide a method for manufacturing a magnetic recording medium having a high coercive force and a high squareness ratio suitable for high-density recording. [Structure of the Invention] The present invention provides a method for manufacturing a magnetic recording medium in which a ferromagnetic metal thin film is formed on a non-magnetic substrate by an oblique evaporation method. A method for manufacturing a magnetic recording medium by blowing an air current mainly composed of O 2 gas onto the surface of the ferromagnetic metal thin film while heating the thin film, or by blowing an air current mainly composed of heated O 2 gas. Regarding. Here, as the substrate, plastic bases such as polyethylene terephthalate, polyimide, polyvinyl chloride, cellulose triacetate, polycarbonate, polyethylene naphthalate, etc., Al, Ti, stainless steel, etc. can be used. In addition, ferromagnetic metals and alloys that can be used as magnetic layer materials include ferromagnetic metals such as Fe, Co, and Ni, and Fe-
Co, Fe−Ni, Co−Ni, Fe−Co−Ni, Fe−Rh,
Fe-Cu, Co-Cu, Co-Au, Co-Y, Co-La,
Co-Pr, Co-Gd, Co-Sm, Co-Pt, Ni-Cu,
Mn-Bi, Mn-Sb, Mn-Al, Fe-Cr, Co-
Cr, Ni−Cr, Fe−Co−Ni, Fe−Co−Cr, Ni−
Examples include ferromagnetic alloys such as Co-Cr. Among these, Co or
It is an alloy containing 50% by weight or more of Co. O 2 gas, N 2 gas, etc. may be introduced into the vapor flow of the ferromagnetic metal during vapor deposition. In the present invention, the oblique evaporation method refers to the U.S. patent
This is a vapor deposition method disclosed in No. 3342632, No. 3342633, etc. Furthermore, in the present invention, "within the same vacuum system" means that the ferromagnetic metal thin film formed by the oblique evaporation method in vacuum is subjected to air flow blowing in the same vacuum system as that used during evaporation without returning it to the atmosphere. It is. Although it is preferable to perform the air flow blowing in the same vacuum chamber as the deposition vacuum chamber, it may be performed in a separate vacuum chamber separated from the deposition vacuum chamber. At this time, the degree of vacuum in the vacuum chamber for airflow blowing can be 10 -2 to 10 2 times that in the vapor deposition vacuum chamber. An example of the manufacturing apparatus used in the present invention is shown in FIG. A rotary can 2 and an evaporation source 3 are provided inside the vacuum chamber 1, and the vapor flow from the evaporation source 3 is designed so that only desired vapor flow components reach the rotary can 2 through a mask 4. . A nozzle 5 is provided in the vacuum chamber 1 for blowing an air flow onto the surface of the ferromagnetic metal thin film. A heater 6 is wound around the nozzle 5. The substrate 8 fed from the delivery roll 7 travels along the rotating can 2 and is wound up on a take-up roll 9. During this travel, the ferromagnetic metal/alloy in the evaporation source 3 is vacuum-deposited onto the base 8, and subsequently a gas stream heated by the heater 5 is blown onto the surface of the ferromagnetic thin film on the base 8 by the nozzle 5. When forming a ferromagnetic metal thin film, a coolant is circulated inside the rotating can 1 to coat the surface of the rotating can.
It is preferable to maintain the temperature at 15°C or lower. FIG. 2 shows another example of the manufacturing apparatus used in the present invention. Rotary cans 22 and 23 are provided inside the vacuum chamber 21, and the substrate 24 is conveyed from a delivery roll 25 along the rotary cans 22 and 23, and then wound onto a take-up roll 26. Rotating can 22
An evaporation source 27 is disposed below the evaporation source 27, and the vapor flow from the evaporation source 27 is masked by a mask 28 so that only desired vapor flow components reach the surface of the substrate 24 on the rotary can 22. Vacuum chamber 21 is exhaust port 2
9, while the gas supply pipe 30
A gas whose main component is O 2 gas is now supplied. A nozzle 31 is provided at the tip of the gas supply pipe 30 and sprays a gas containing O 2 gas as a main component onto the surface of the deposited magnetic metal thin film formed on the substrate 24 moving along the rotating can 23 . A mechanism is provided in which a coolant is circulated inside the rotary can 22 to maintain the surface of the rotary can at 15° C. or less, and a hot medium is circulated inside the rotary can 23 to heat the deposited magnetic metal thin film. A method for preventing wrinkles by spraying O 2 gas, N 2 gas, etc. after forming a ferromagnetic metal thin film (Japanese Patent Laid-Open No.
55-14569), a method for improving corrosion resistance by exposing a magnetic film to an oxidizing atmosphere after forming a ferromagnetic metal thin film (Japanese Patent Application Laid-open No. 57-198543), exposing a magnetic film to an oxidizing atmosphere after forming a ferromagnetic metal thin film A method for improving corrosion resistance by exposing to a glow discharge atmosphere using
17544), and a method of forming a ferromagnetic metal thin film and then exposing the magnetic film to an ozone atmosphere in a heated state to improve its durability under repeated running and high temperature and high humidity conditions (Japanese Unexamined Patent Publication No. 1759- 63031), etc., but in the present invention, after forming a ferromagnetic metal thin film by an oblique evaporation method, a gas mainly composed of O 2 gas is applied to the surface of the magnetic metal thin film while the magnetic metal thin film is heated. A magnetic recording medium having extremely good magnetic properties is obtained by spraying
The present invention relates to a method for manufacturing a novel magnetic recording medium that cannot be predicted using the above-mentioned known techniques. Furthermore, in the present invention, after forming a ferromagnetic metal thin film by oblique vapor deposition, a magnetic recording medium having extremely good magnetic properties can be obtained by blowing an air current mainly composed of heated O 2 gas onto the surface of the magnetic metal thin film. This is a new technology that could not be predicted using conventional technology. When manufacturing a tape-shaped magnetic recording medium according to the present invention, it is preferable to blow a gas flow mainly composed of O 2 onto the surface of a ferromagnetic metal thin film while conveying the tape-shaped substrate along a rotating can. Moreover, in this case, the gas blowing section should be arranged so that the ratio R/r of the distance (R) from the center of the rotation can to the gas introduction section and the radius (r) of the rotation can is in the range of 1.01 to 1.20. preferable. The present invention will be explained below based on Examples. This example does not limit the scope of application of the present invention. Example 1 Using the manufacturing equipment shown in Figure 1, a film with a thickness of 1500 mm was deposited on a 12.5 μm thick polyethylene terephthalate film.
A magnetic tape was fabricated by forming a cobalt-deposited magnetic thin film with a thickness of 1.5 Å using an oblique evaporation method while introducing O 2 gas. The magnetic properties of the obtained magnetic tape were measured using a vibrating magnetometer (VSM). The results are shown in the table below.

【表】 表からみてとれるように、従来の製造方法によ
る試料Aに対して斜め蒸着直後に磁性膜を加熱し
つつO2ガス気流をさし向けた試料D,Eにおい
ては角型比SQの大巾な良化が認められる。ここ
で、単に気流を吹きつけた場合(B)、あるいは
単に磁性膜を加熱した場合(C)では磁気特性の
変化が現われないことに注意すべきである。 上記において蒸着膜形成后、O2ガスのかわり
にオゾンガスを使用した場合には磁気特性の改良
は得られなかつた。 実施例 2 第2図に示す製造装置を用いて9.5μm厚ポリエ
チレンテレフタレーフイルム上に膜厚1300Åの
CoNi合金(Ni25重量%)蒸着磁性薄膜をO2ガス
を導入しながら斜め蒸着法により形成し、磁気テ
ープを作成した。得られた磁気テープの磁気特性
は下記のとおりであつた。 下記の表において、試料Fと試料G及び試料H
と試料Iとを比較することにより以下のことが分
かる。 回転キヤンの温度が低い場合には、強磁性金属
薄膜の表面にO2ガスを吹き付けても角型比の向
上が認められないこと、回転キヤンが75℃になる
ように強磁性薄膜表面を加熱しつゝO2ガスを強
磁性薄膜表面に吹き付けると角型比の向上が認め
られることである。 更に回転キヤンの温度を85℃にした試料Jにお
いても良好な結果が得られている。
[Table] As can be seen from the table, the squareness ratio SQ is larger in Samples D and E, in which the O 2 gas stream is directed while heating the magnetic film immediately after oblique evaporation, compared to Sample A produced by the conventional manufacturing method. Widespread improvement was observed. It should be noted here that no change in magnetic properties appears when simply blowing an air current (B) or when simply heating the magnetic film (C). In the above case, when ozone gas was used instead of O 2 gas after forming the deposited film, no improvement in magnetic properties could be obtained. Example 2 A film with a thickness of 1300 Å was deposited on a 9.5 μm thick polyethylene terephthalate film using the manufacturing equipment shown in Figure 2.
A CoNi alloy (Ni 25% by weight) vapor-deposited magnetic thin film was formed by oblique vapor deposition while introducing O 2 gas to create a magnetic tape. The magnetic properties of the obtained magnetic tape were as follows. In the table below, sample F, sample G and sample H
By comparing Sample I and Sample I, the following can be found. When the temperature of the rotating can is low, no improvement in the squareness ratio is observed even if O 2 gas is sprayed onto the surface of the ferromagnetic metal thin film, and the surface of the ferromagnetic thin film is heated so that the rotating can reaches 75°C. However, when O 2 gas is blown onto the surface of a ferromagnetic thin film, an improvement in the squareness ratio is observed. Furthermore, good results were also obtained for sample J in which the temperature of the rotating can was 85°C.

【表】 表から明らかなように本発明により製造された
磁気テープはすぐれた角型性を有する。 実施例 3 実施例1において、9.5μm厚のポリエチレンテ
レフタレートフイルム上に膜厚1300Aのコバルト
蒸着磁性薄膜をO2ガス導入口の配設位置を変え
てO2ガスを強磁性薄膜の表面に吹き付けた。 前記O2ガス導入口の配設位置は回転キヤンの
中心からの距離(R)と回転キヤンの半径(r)
との比R/rが1.015から1.25の範囲となるよう
に変えた。 得られた磁気テープの特性は下表の通りであつ
た。
[Table] As is clear from the table, the magnetic tape manufactured according to the present invention has excellent squareness. Example 3 In Example 1, a cobalt evaporated magnetic thin film with a film thickness of 1300 A was formed on a 9.5 μm thick polyethylene terephthalate film, and O 2 gas was blown onto the surface of the ferromagnetic thin film by changing the position of the O 2 gas inlet. . The location of the O 2 gas inlet is determined by the distance from the center of the rotation can (R) and the radius of the rotation can (r).
The ratio R/r was changed so that it was in the range of 1.015 to 1.25. The properties of the magnetic tape obtained were as shown in the table below.

〔発明の効果〕〔Effect of the invention〕

以上のように本発明によれば高密度記録に適し
たきわめて良好なる磁気特性を有する磁気記録媒
体を簡便なる工程により得られる。
As described above, according to the present invention, a magnetic recording medium having extremely good magnetic properties suitable for high-density recording can be obtained through a simple process.

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

第1図に本発明に用いられる製造装置の概略図
を示す。 1……真空槽、2……回転キヤン、3……蒸発
源、4……マスク、5……ガス気流吹きつけノズ
ル、6……加熱用ヒーター、7……送り出しロー
ル、8……基体、9……巻取りロール。 第2図は本発明による製造装置の他の一例を示
す。 21……真空槽、22,23……回転キヤン、
24……基体、25……送り出しロール、26…
…巻取りロール、27……蒸発源、28……マス
ク、29……排気孔、30……ガス供給管、31
……ガス気流吹きつけノズル。
FIG. 1 shows a schematic diagram of a manufacturing apparatus used in the present invention. DESCRIPTION OF SYMBOLS 1... Vacuum chamber, 2... Rotating can, 3... Evaporation source, 4... Mask, 5... Gas stream blowing nozzle, 6... Heater, 7... Delivery roll, 8... Substrate, 9... Winding roll. FIG. 2 shows another example of the manufacturing apparatus according to the present invention. 21... Vacuum chamber, 22, 23... Rotating can,
24...base body, 25...feeding roll, 26...
... Winding roll, 27 ... Evaporation source, 28 ... Mask, 29 ... Exhaust hole, 30 ... Gas supply pipe, 31
...Gas airflow spray nozzle.

Claims (1)

【特許請求の範囲】 1 非磁性支持体上に斜め蒸着法により、強磁性
金属薄膜を形成して磁気記録媒体を製造する方法
において、斜め蒸着法により強磁性金属薄膜を形
成した後、同一真空系内において該強磁性金属薄
膜を回転キヤンの温度が75℃以上となるように加
熱しつゝ該強磁性金属薄膜の表面にO2ガスを主
成分とする気流を、回転キヤンの中心からの距離
(R)と回転キヤンの半径(r)との比R/rが
1.01から1.20の範囲となるように配設したガス吹
き付け部より吹き付けることを特徴とする磁気記
録媒体の製造方法。 2 非磁性支持体上に斜め蒸着法により強磁性金
属薄膜を形成した後、同一真空系内において該強
磁性金属薄膜表面に加熱したO2ガスを主成分と
する気流を、回転キヤンの中心からの距離(R)
と回転キヤンの半径(r)との比R/rが1.01か
ら1.20の範囲となるように配設したガス吹き付け
部より吹き付けることを特徴とする磁気記録媒体
の製造方法。
[Claims] 1. In a method for manufacturing a magnetic recording medium by forming a ferromagnetic metal thin film on a non-magnetic support by an oblique evaporation method, after forming the ferromagnetic metal thin film by an oblique evaporation method, The ferromagnetic metal thin film is heated in the system so that the temperature of the rotating can becomes 75°C or higher, and an air flow containing O 2 gas as a main component is applied to the surface of the ferromagnetic metal thin film from the center of the rotating can. The ratio R/r between the distance (R) and the radius (r) of the rotating can is
A method for manufacturing a magnetic recording medium, characterized in that the gas is sprayed from a gas spraying section arranged so that the gas is in the range of 1.01 to 1.20. 2. After forming a ferromagnetic metal thin film on a non-magnetic support by oblique vapor deposition, an air flow mainly composed of heated O 2 gas is applied to the surface of the ferromagnetic metal thin film in the same vacuum system from the center of the rotating can. distance (R)
A method for manufacturing a magnetic recording medium, characterized in that the gas is sprayed from a gas spraying section arranged such that the ratio R/r of the radius (r) of the magnetic recording medium and the radius (r) of the rotating can is in the range of 1.01 to 1.20.
JP17059284A 1984-08-16 1984-08-16 Production of magnetic recording medium Granted JPS6150218A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17059284A JPS6150218A (en) 1984-08-16 1984-08-16 Production of magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17059284A JPS6150218A (en) 1984-08-16 1984-08-16 Production of magnetic recording medium

Publications (2)

Publication Number Publication Date
JPS6150218A JPS6150218A (en) 1986-03-12
JPH0434205B2 true JPH0434205B2 (en) 1992-06-05

Family

ID=15907692

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17059284A Granted JPS6150218A (en) 1984-08-16 1984-08-16 Production of magnetic recording medium

Country Status (1)

Country Link
JP (1) JPS6150218A (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57164421A (en) * 1981-04-01 1982-10-09 Matsushita Electric Ind Co Ltd Magnetic recording medium
JPS57198543A (en) * 1981-05-28 1982-12-06 Matsushita Electric Ind Co Ltd Manufacture of magnetic recording medium

Also Published As

Publication number Publication date
JPS6150218A (en) 1986-03-12

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