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JPH0443326B2 - - Google Patents
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JPH0443326B2 - - Google Patents

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Publication number
JPH0443326B2
JPH0443326B2 JP25170183A JP25170183A JPH0443326B2 JP H0443326 B2 JPH0443326 B2 JP H0443326B2 JP 25170183 A JP25170183 A JP 25170183A JP 25170183 A JP25170183 A JP 25170183A JP H0443326 B2 JPH0443326 B2 JP H0443326B2
Authority
JP
Japan
Prior art keywords
magnetic
electron beam
thin film
layer
magnetic layer
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
JP25170183A
Other languages
Japanese (ja)
Other versions
JPS60143435A (en
Inventor
Koichi Shinohara
Takashi Fujita
Akio Hogo
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 JP58251701A priority Critical patent/JPS60143435A/en
Publication of JPS60143435A publication Critical patent/JPS60143435A/en
Publication of JPH0443326B2 publication Critical patent/JPH0443326B2/ja
Granted legal-status Critical Current

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Description

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

[産業上の利用分野] 本発明は広帯域の信号記録・再生に適した磁気
記録媒体の製造方法に関する。 [従来例の構成とその問題点] 回転磁気ヘツドによるヘリカル走査方式の音声
画像の記録再生を行なう技術は磁気記録の中でも
最も高密度記録化が進んでいる。この技術の延長
上で更に記録密度を高めていくには、単に記録波
長の最小値が小さくなるだけでなく、帯域の広い
波長特性を有する磁気記録媒体が望まれている。 一方、従来の磁気記録媒体は、記録波長が短か
くなる程、媒体内部の自己減磁界が増大し、更に
媒体内部のエネルギーが最小になるよう磁化ベク
トルの回転が生じ、それらが急激な再生出力低下
として現われるので、自己減磁界の影響をできる
限り小さくするため、自己減磁界に打ち勝つよう
に媒体の保磁力を大きくしてきた。しかしこの方
法は媒体厚さ方向への磁化浸透を減ずるように働
くため長波長出力の低下を招くので、磁化量を増
さなければならないが、実用に供されているフエ
ライトヘツドでは磁気的に飽和現象が起るので、
合金系のヘツドを開発する必要がある。 そこで支持体上に比較的低保磁力の第1磁性
層、例えばγ−Fe2O3針状粒子を結合剤と共に塗
布配向乾燥した層を形成し、その上に第2磁性
層、例えばγ−Fe2O3針状粒子をCrO2に置き換え
た層を形成する二層構造の磁気記録媒体が考案さ
れ、既に実用に供されている。 他にも二層構造として、塗布磁性層上に金属薄
膜型に強磁性層を配したものも提案されており、
例えば、支持体上にγ−Fe2O3、Coをドープした
γ−Fe2O3、Fe3O4、CrO2等の酸化物磁性粉末あ
るいは強磁性合金粉末等の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、ポリウレタン樹脂等の有機結合剤中
に分散せしめ塗布、乾燥させて得た第1磁性層上
に真空蒸着、スパツタリング、無電解めつき等の
方法で、Co、Co−Ni、Co−Mo、Co−Cr、Co
−Ni−Mg等の強磁性金属薄膜を形成して第2磁
性層となした媒体がある。この構成は広帯域の信
号の記録再生に適しているが、市販のビデオテー
プレコーダ(以下、V.T.R.と記す)を改造した
機構で記録再生を繰り返した時、信号対雑音比
(以下S/Nで表わす)の低下が急激に起る。 このS/N低下現象は、主として第2磁性層の
亀裂及び部分剥離によるもので、構成材料による
差はあるが、30パスから60パスの間で起り、実用
上は各種の環境でも200パスは安定な性能が必要
で改良が望まれていた。 [発明の目的] 本発明はこのような事情に鑑みてなされたもの
で塗布磁性層の改良により広帯域の信号の記録再
生に適した磁気記録媒体の製造方法を提供するの
が目的である。 [発明の構成] 本発明の磁気記録媒体の製造方法は、支持体上
に電子線照射によつて重合が可能な不飽和結合を
有する化合物を結合剤とする磁気塗料を塗布して
塗布磁性層を形成した後、該塗布磁性層上に強磁
性金属薄膜を真空蒸着法により形成し引き続き真
空中で前記強磁性金属薄膜を通して電子線照射を
行ない、前記不飽和結合を有する化合物を重合さ
せることを特徴とする。 [実施例の説明] 第1図は、本発明の製造方法により得られる磁
性記録媒体の拡大断面図である。即ち、支持体1
上に電子線照射によつて重合されたポリマーを結
合剤2aとして粉末磁性材料2aを固定する塗布
磁性層2を配し、その上に強磁性金属薄膜層3と
滑剤層4を配して成るもので、2cは本発明の製
造方法によつて強磁性金属薄膜層3と塗布磁性層
の間にできる中間層である。 本発明に用いることのできる電子線照射によつ
て重合が可能な不飽和結合を有する化合物として
は、代表的にはアクリロイル基、アクリルアミド
基、アリル基、ビニルチオエーテル基等を含む化
合物及び不飽和ポリエステル類等である。重合し
たポリマーの分子量は1000〜20000の範囲が好ま
しい。 本発明に用いられる磁性粉末はγ−Fe2O3、Co
を含有したγ−Fe2O3、Fe3O4、CrO2、バリウム
フエライト等の酸化物磁性粉末、Co、Fe、Co−
Fe、Co−Ni等の金属磁性粉末等で、添加剤は適
宜選択して用いることができる。 本発明に用いることのできる強磁性金属薄膜は
Fe、Co、Fe−Co、Co−Ni、Co−P、Co−B、
Co−Si、Co−V、Co−Ru、Co−Cr、Co−Cu、
Co−Ti、Co−Mo、Co−W、Co−Ni−Cr、Co
−Fe−Cr、Co−Si−Sm、Co−Ni−Mg、及びそ
れらの部分酸化膜、部分窒化膜等が挙げられる。 本発明に用いられる支持体はポリエチレンテレ
フタレート等のポリエステル類、ポリプロピレン
等のポリオレフイン類、セルロースジアセテー
ト、ニトロセルロース等のセルロース誘導体、ポ
リ塩化ビニル、芳香族ポリアミド、ポリイミド等
である。 上記した構成材料から成る磁気記録媒体を製造
する本発明の製造方法は、電子線照射により重合
可能な化合物を結合剤とし、磁性粉末、有機溶剤
等から成る磁気塗料を調製し、この磁気塗料をエ
アドクターコート、エアナイフコート、スクイズ
コート、含浸コート、リバースロールコート、グ
ラビアコート、キスコート、スプレイコート、ス
ピンコート等から選んだ塗布方法で支持体に予め
塗布し、乾燥して巻きあげる。 巻きあげたロールを後述する巻取蒸着機を改造
した本発明の磁気記録媒体製造方法を実施するた
めの装置に装着し、強磁性金属薄膜を前記塗布磁
性層の上に形成する。その方法は電子ビーム蒸着
法、イオンプレーテイング法、スパツタリング法
等の薄膜形成法は用いれば良い。 次に前記強磁性金属薄膜の表面側から電子線を
照射して巻きあげるのであるが、電子線照射に用
いられる電子線加速器は、一段加速のカーテンビ
ーム型の加速器が良い。勿論他の型の加速器でも
良いが、真空中で照射することと、強磁性金属薄
膜層から制動X線を有効に放射させることと、塗
布磁性層の厚みとを考慮し、塗布磁性層全体が重
合硬化するようにエネルギーを最適化する必要が
ある。 本発明の製造方法は、塗布磁性層の重合硬化後
に強磁性金属薄膜を形成するのではなく、塗布磁
性層が未硬化状態で強磁性金属薄膜を形成するこ
とで、蒸着された原子が一部、塗布磁性層に拡散
し、その原子を核にした中間層が形成される。 また、これらの原子は活性で重合の触媒作用を
行なうことができるのと、強磁性金属薄膜中を電
子線が通過する間に一部のエネルギーが失われ、
いわゆる制動X線を放射するので、X線源が塗布
磁性層に密着していること同一になり、電子線照
射単独よりも重合度が増し、塗布磁性層がより硬
くなることになり、より耐久性の向上が図れるも
のである。 本発明を実施例により更に詳しく説明するが、
本発明は下記の実施例に限定されるものではな
い。 実施例の説明に先立ち、第2図で、本発明の媒
体の製造方法の実施に用いた巻取蒸着装置につい
て概説する。 予め電子線照射によつて重合が可能な化合物に
磁性粉末を分散させたいわゆる磁気塗料を支持体
上に塗布したウエブ(以下これを単にウエブと呼
ぶ)5は、クーリングキヤン6の周側面に沿つ
て、送り出し軸7から巻取り軸8へ移動するよう
構成される。 まず、クーリングキヤン6に沿つた状態でウエ
ブ5の塗布面側に、限定された蒸気流11によ
り、強磁性金属薄膜を形成する。次いで、クーリ
ングキヤン6にやはり沿つた状態で結合剤を重合
させるために電子線照射を行なう。この状況はフ
イラメント9と電子線10で模式的に示してあ
る。 限定された蒸気流11は、例えば、蒸発源容器
12内にチヤージされた蒸発材料13が、加熱電
子源14より放射される電子ビーム15により加
熱された蒸発温度に達して放射され生成される蒸
気流を、この場合は、斜め蒸着の最小入射角を決
めるマスク16により限定を受けて形成されたも
のである。 上記の構成は、排気系17で真空に保持された
真空容器18内に配設される。19はフリーロー
ラーであり、20は電子線の遮へい板である。 実施例 1 CrO280重量部(以下「部」で表わす)、ウレタ
ンアクリレート14部、ジエチレングリコールジア
クリレート6部、メチルエチルケトン100部から
なる塗料成分をボールミル中で72時間混合分散さ
せ磁気塗料を調製した。この磁気塗料を厚さ8.5μ
mのポリエチレンテレフタレートフイルム上に溶
剤を蒸発させた後の膜厚が2.5μmになるようリバ
ースロールコータで塗布し、乾燥した。 このフイルムを第2図の装置に装着して、電子
ビーム蒸着によりCo−Ni−Cr(Co70、Ni15、
Cr15%)を斜め蒸着し、Co−Ni−Cr薄膜を0.13μ
m形成した。真空度は2×10-6Torr、最小入射
角40゜で、直径1mのクーリングキヤンを用いて
30m/minで移動させながら処理した。次に同一
クーリングキヤンに沿つた状態で、加速電圧
110KVの電子線を20μA/cm2の電流密度で照射
し、巻きあげた。 この状態のフイルムを大気中に取り出し、メチ
ルイソブチルケトンに溶かしたミリスチン酸
200ppmの溶液を同じくリバースロールコータで
塗布し、乾燥厚み約40〓の滑剤層を形成し、8mm
幅の磁気テープAを製造した。 実施例 2 Co−Ni(Ni20部)合金微粉末80部、ウレタン
アクリレート14部、ペンタエリスリトールテトラ
アクリレート6部、シクロヘキサノン100部から
成る塗料成分をボールミル中で72時間混合分散さ
せ磁気塗料を調製した。 この磁気塗料を厚さ7μmのポリエチレンテレ
フタレートフイルム上に溶剤を蒸発させた後の膜
圧が2μmになるようにリバースロールコータで
塗布した。こうして得られたフイルムを第2図の
装置により、60m/minで移動させながら、2×
10-5Torrの酸素中で、Co−Ni(Ni20部)薄膜を
電子ビーム蒸着により0.14μm形成した。最小入
射角37゜でクーリングキヤンの直径は1mのもの
を用いた。次に同一クーリングキヤンに沿つた状
態で、加速電圧130KVの電子線を30μA/cm2の電
流密度で照射し巻きあげた。 この状態のフイルムを大気中に取り出し、実施
例1の要領でミリスチン酸を塗布し、8mm幅の磁
気テープBを製造した。 比較例 1 CrO280部、塩化ビニル−酢酸ビニル−ビニル
アルコール共重合体12部、アクリロニトリル−ブ
タジエン共重合体8部、メチルイソブチルケトン
100部からなる塗料成分をボールミル中で72時間
混合分散させて磁気塗料を調製した。これを用い
て、電子線照射を行なわない以外は実施例1と同
じ手順で、磁気テープCを製造した。 比較例 2 電子線照射とCo−Ni薄膜形成の順序を逆にし
た以外は実施例2と同じ要領で、磁気テープDを
製造した。 磁気テープAからDまでを試作した評価用V.
T.R.にて繰り返し使用でのS/Nの変化を調べ
た。 測定は、5℃80%RH、25℃55%RH、30℃80
%RH、40℃80%RHで行なつたが、最も条件の
悪かつた40℃80%RHでの結果を次表にまとめて
示した。 S/Nは輝度信号の信号出力と雑音出力の比
で、中心周波数5.5MHzの信号をアモルフアスヘ
ツド(トラツク幅20μm、ギヤツプ長0.3μm)を
用い、磁気ヘツド・テープ相対速度3.5m/secで
初期値を0dBとして相対比較した値である。S/
Nが3dB低下したパス回数と、繰り返し走行での
実績を示してある。また、S/Nの低下原因と最
終テスト後の表面観察結果も併記した。
[Industrial Application Field] The present invention relates to a method of manufacturing a magnetic recording medium suitable for wideband signal recording and reproduction. [Constitution of Conventional Example and Problems thereof] The technique of recording and reproducing audio images using a helical scanning method using a rotating magnetic head is one of the most advanced types of magnetic recording in terms of high-density recording. In order to further increase the recording density as an extension of this technology, a magnetic recording medium that not only has a smaller minimum recording wavelength but also has wavelength characteristics with a wide band is desired. On the other hand, in conventional magnetic recording media, as the recording wavelength becomes shorter, the self-demagnetizing field inside the medium increases, and the magnetization vector rotates to minimize the energy inside the medium, which causes a rapid reproduction output. In order to minimize the effect of the self-demagnetizing field, the coercive force of the medium has been increased to overcome the self-demagnetizing field. However, this method works to reduce the penetration of magnetization in the direction of the medium thickness, resulting in a decrease in long wavelength output, so the amount of magnetization must be increased, but the ferrite head in practical use is not magnetically saturated. Because a phenomenon occurs,
It is necessary to develop an alloy head. Therefore, a first magnetic layer having a relatively low coercive force, such as a layer in which acicular particles of γ-Fe 2 O 3 are coated and oriented and dried together with a binder, is formed on the support, and a second magnetic layer, such as γ- A two-layer magnetic recording medium in which Fe 2 O 3 acicular particles are replaced with CrO 2 has been devised and is already in practical use. Another two-layer structure has been proposed, in which a ferromagnetic layer is arranged in the form of a metal thin film on a coated magnetic layer.
For example, powder magnetic materials such as oxide magnetic powders such as γ-Fe 2 O 3 , Co-doped γ-Fe 2 O 3 , Fe 3 O 4 , CrO 2 or ferromagnetic alloy powders are coated on a support with vinyl chloride. - Vacuum deposition, sputtering, electroless plating, etc. on the first magnetic layer obtained by dispersing and coating in an organic binder such as vinyl acetate copolymer, styrene-butadiene copolymer, or polyurethane resin, and drying. So, Co, Co−Ni, Co−Mo, Co−Cr, Co
There is a medium in which a second magnetic layer is formed by forming a ferromagnetic metal thin film such as -Ni-Mg. This configuration is suitable for recording and reproducing wideband signals, but when recording and reproducing are repeated using a mechanism modified from a commercially available video tape recorder (hereinafter referred to as VTR), the signal-to-noise ratio (hereinafter expressed as S/N) ) occurs rapidly. This S/N reduction phenomenon is mainly due to cracks and partial peeling of the second magnetic layer, and although there are differences depending on the constituent materials, it occurs between 30 and 60 passes, and in practice, 200 passes are required under various environments. Stable performance was required and improvements were desired. [Object of the Invention] The present invention has been made in view of the above circumstances, and an object thereof is to provide a method for manufacturing a magnetic recording medium suitable for recording and reproducing broadband signals by improving the coated magnetic layer. [Structure of the Invention] The method for producing a magnetic recording medium of the present invention involves coating a support with a magnetic paint containing as a binder a compound having an unsaturated bond that can be polymerized by electron beam irradiation, and forming a coated magnetic layer. After forming, a ferromagnetic metal thin film is formed on the coated magnetic layer by a vacuum evaporation method, and then electron beam irradiation is performed through the ferromagnetic metal thin film in a vacuum to polymerize the compound having the unsaturated bond. Features. [Description of Examples] FIG. 1 is an enlarged sectional view of a magnetic recording medium obtained by the manufacturing method of the present invention. That is, support 1
A coated magnetic layer 2 for fixing a powder magnetic material 2a using a polymer polymerized by electron beam irradiation as a binder 2a is disposed thereon, and a ferromagnetic metal thin film layer 3 and a lubricant layer 4 are disposed thereon. 2c is an intermediate layer formed between the ferromagnetic metal thin film layer 3 and the coated magnetic layer by the manufacturing method of the present invention. Examples of compounds having unsaturated bonds that can be polymerized by electron beam irradiation that can be used in the present invention include compounds containing acryloyl groups, acrylamide groups, allyl groups, vinyl thioether groups, etc., and unsaturated polyesters. etc. The molecular weight of the polymerized polymer is preferably in the range of 1,000 to 20,000. The magnetic powder used in the present invention is γ-Fe 2 O 3 , Co
γ- Fe2O3 , Fe3O4 , CrO2 , barium ferrite and other oxide magnetic powders containing
Additives such as metal magnetic powders such as Fe and Co-Ni can be appropriately selected and used. The ferromagnetic metal thin film that can be used in the present invention is
Fe, Co, Fe-Co, Co-Ni, Co-P, Co-B,
Co-Si, Co-V, Co-Ru, Co-Cr, Co-Cu,
Co-Ti, Co-Mo, Co-W, Co-Ni-Cr, Co
Examples include -Fe-Cr, Co-Si-Sm, Co-Ni-Mg, and partial oxide films and partial nitride films thereof. Supports used in the present invention include polyesters such as polyethylene terephthalate, polyolefins such as polypropylene, cellulose derivatives such as cellulose diacetate and nitrocellulose, polyvinyl chloride, aromatic polyamides, polyimides, and the like. The manufacturing method of the present invention for manufacturing a magnetic recording medium made of the above-mentioned constituent materials involves preparing a magnetic paint made of magnetic powder, an organic solvent, etc. using a compound that can be polymerized by electron beam irradiation as a binder, and applying the magnetic paint to the magnetic recording medium. It is coated on the support in advance by a coating method selected from air doctor coat, air knife coat, squeeze coat, impregnation coat, reverse roll coat, gravure coat, kiss coat, spray coat, spin coat, etc., dried and rolled up. The wound roll is attached to an apparatus for carrying out the method of manufacturing a magnetic recording medium of the present invention, which is a modified take-up vapor deposition machine described later, and a ferromagnetic metal thin film is formed on the coated magnetic layer. For this purpose, a thin film forming method such as an electron beam evaporation method, an ion plating method, or a sputtering method may be used. Next, an electron beam is irradiated from the surface side of the ferromagnetic metal thin film to wind it up. The electron beam accelerator used for electron beam irradiation is preferably a single-stage acceleration curtain beam type accelerator. Of course, other types of accelerators may be used, but considering the irradiation in a vacuum, the effective emission of bremsstrahlung X-rays from the ferromagnetic metal thin film layer, and the thickness of the coated magnetic layer, it is necessary to It is necessary to optimize the energy for polymerization and curing. The manufacturing method of the present invention does not form a ferromagnetic metal thin film after polymerizing and hardening the coated magnetic layer, but forms a ferromagnetic metal thin film with the coated magnetic layer in an uncured state, so that some of the deposited atoms are removed. , diffuse into the coated magnetic layer, and form an intermediate layer with the atoms as nuclei. In addition, these atoms are active and can catalyze polymerization, and some energy is lost while the electron beam passes through the ferromagnetic metal thin film.
Since it emits so-called bremsstrahlung X-rays, the X-ray source is in close contact with the coated magnetic layer, which increases the degree of polymerization and makes the coated magnetic layer harder than with electron beam irradiation alone, making it more durable. This is something that can improve sexual performance. The present invention will be explained in more detail by examples.
The present invention is not limited to the following examples. Prior to describing the embodiments, a winding vapor deposition apparatus used to carry out the method for producing a medium of the present invention will be outlined with reference to FIG. A web (hereinafter simply referred to as a web) 5 is coated on a support with so-called magnetic paint in which magnetic powder is dispersed in a compound that can be polymerized by electron beam irradiation. Then, it is configured to move from the sending shaft 7 to the winding shaft 8. First, a ferromagnetic metal thin film is formed on the coating surface side of the web 5 along the cooling can 6 using a limited vapor flow 11 . Next, electron beam irradiation is performed along the cooling can 6 in order to polymerize the binder. This situation is schematically illustrated by filament 9 and electron beam 10. The limited vapor flow 11 is, for example, vapor generated when the evaporation material 13 charged in the evaporation source container 12 reaches the evaporation temperature heated by the electron beam 15 emitted from the heating electron source 14 and is emitted. In this case, the flow is limited by a mask 16 that determines the minimum angle of incidence for oblique deposition. The above configuration is arranged in a vacuum container 18 that is maintained in a vacuum by an exhaust system 17. 19 is a free roller, and 20 is an electron beam shielding plate. Example 1 A magnetic paint was prepared by mixing and dispersing paint components consisting of 80 parts by weight (hereinafter expressed as "parts") of CrO 2 , 14 parts of urethane acrylate, 6 parts of diethylene glycol diacrylate, and 100 parts of methyl ethyl ketone in a ball mill for 72 hours. This magnetic paint has a thickness of 8.5μ
After the solvent was evaporated, the film was coated on a polyethylene terephthalate film with a reverse roll coater to a film thickness of 2.5 μm, and then dried. This film was mounted on the apparatus shown in Fig. 2, and Co-Ni-Cr (Co70, Ni15,
Co-Ni-Cr thin film with a thickness of 0.13μ
m was formed. The degree of vacuum was 2 × 10 -6 Torr, the minimum angle of incidence was 40°, and a cooling canister with a diameter of 1 m was used.
The treatment was carried out while moving at 30 m/min. Next, in a state along the same cooling can, the accelerating voltage
It was irradiated with a 110 KV electron beam at a current density of 20 μA/cm 2 and wound up. The film in this state was taken out into the atmosphere, and myristic acid was dissolved in methyl isobutyl ketone.
A 200ppm solution was applied using the same reverse roll coater to form a lubricant layer with a dry thickness of approximately 40 mm.
A magnetic tape A having a width of 1.5 mm was manufactured. Example 2 A magnetic paint was prepared by mixing and dispersing paint components consisting of 80 parts of Co--Ni (20 parts of Ni) alloy fine powder, 14 parts of urethane acrylate, 6 parts of pentaerythritol tetraacrylate, and 100 parts of cyclohexanone in a ball mill for 72 hours. This magnetic paint was applied onto a 7 μm thick polyethylene terephthalate film using a reverse roll coater so that the film thickness after evaporating the solvent was 2 μm. The film thus obtained was moved at a speed of 60 m/min using the device shown in Figure 2, and was
A Co--Ni (20 parts Ni) thin film was formed to a thickness of 0.14 μm by electron beam evaporation in oxygen at 10 −5 Torr. A cooling can with a minimum incident angle of 37° and a diameter of 1 m was used. Next, along the same cooling cann, it was irradiated with an electron beam at an accelerating voltage of 130 KV at a current density of 30 μA/cm 2 and wound up. The film in this state was taken out into the atmosphere, and myristic acid was applied in the same manner as in Example 1 to produce a magnetic tape B having a width of 8 mm. Comparative Example 1 80 parts of CrO 2 , 12 parts of vinyl chloride-vinyl acetate-vinyl alcohol copolymer, 8 parts of acrylonitrile-butadiene copolymer, methyl isobutyl ketone
A magnetic paint was prepared by mixing and dispersing 100 parts of paint components in a ball mill for 72 hours. Using this, magnetic tape C was manufactured in the same manner as in Example 1 except that electron beam irradiation was not performed. Comparative Example 2 Magnetic tape D was manufactured in the same manner as in Example 2 except that the order of electron beam irradiation and Co--Ni thin film formation was reversed. Evaluation V. which prototyped magnetic tapes A to D.
Changes in S/N with repeated use of TR were investigated. Measurement is 5℃80%RH, 25℃55%RH, 30℃80
%RH and 40°C and 80%RH, but the results at 40°C and 80%RH, which was the worst condition, are summarized in the following table. S/N is the ratio of the signal output of the luminance signal to the noise output. A signal with a center frequency of 5.5 MHz is measured using an amorphous head (track width 20 μm, gap length 0.3 μm) at a magnetic head/tape relative speed of 3.5 m/sec. This is a relative comparison value with the initial value as 0dB. S/
The number of passes where N decreased by 3 dB and the results of repeated running are shown. In addition, the cause of the decrease in S/N and the surface observation results after the final test are also listed.

【表】 上表より明らかなように本発明の製造方法によ
り得た磁気記録媒体の耐久性は実用水準にある。 [発明の効果] 本発明は支持体上に電子線照射によつて重合が
可能な不飽和結合を有する化合物を結合剤とする
磁気塗料を塗布して塗布磁性層を形成後、該塗布
磁性層上に強磁性金属膜を形成してから電子線照
射を真空中で行なうことで、広帯域の信号の記録
再生に適する二層構成の媒体のうち、塗布磁性
層、強磁性金属薄膜層の積層型の製造において、
実用水準の耐久性を保有する媒体を量産し得るも
のである。
[Table] As is clear from the above table, the durability of the magnetic recording medium obtained by the manufacturing method of the present invention is at a practical level. [Effects of the Invention] The present invention provides a method for forming a coated magnetic layer by coating a magnetic coating containing a compound having an unsaturated bond as a binder that can be polymerized by electron beam irradiation on a support. Among two-layered media suitable for recording and reproducing broadband signals, a laminated type with a coated magnetic layer and a ferromagnetic metal thin film layer is produced by forming a ferromagnetic metal film on top and then performing electron beam irradiation in a vacuum. In the production of
It is possible to mass-produce media with durability at a practical level.

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

第1図は本発明の製造方法によつて製造された
磁気記録媒体の拡大断面図、第2図は本発明の製
造方法を実施するための装置の要部構成図の一例
である。 1……支持体、2……塗布磁性層、2a……結
合剤、2b……粉末磁性材料、2c……中間層、
3……強磁性金属薄膜層、10……電子線、11
……金属蒸気流。
FIG. 1 is an enlarged sectional view of a magnetic recording medium manufactured by the manufacturing method of the present invention, and FIG. 2 is an example of a configuration diagram of a main part of an apparatus for carrying out the manufacturing method of the present invention. DESCRIPTION OF SYMBOLS 1... Support, 2... Coated magnetic layer, 2a... Binder, 2b... Powdered magnetic material, 2c... Intermediate layer,
3...Ferromagnetic metal thin film layer, 10...Electron beam, 11
...Metal vapor flow.

Claims (1)

【特許請求の範囲】[Claims] 1 支持体上に電子線照射によつて重合が可能な
不飽和結合を有する化合物を結合剤とする磁気塗
料を塗布して塗布磁性層を形成した後、該塗布磁
性層上に強磁性金属薄膜を形成し引き続き電子線
照射を真空中で行なつて上記不飽和結合を有する
化合物を重合させることを特徴とする磁気記録媒
体の製造方法。
1. After forming a coated magnetic layer by coating a magnetic paint containing a compound having an unsaturated bond as a binder that can be polymerized by electron beam irradiation on a support, a ferromagnetic metal thin film is formed on the coated magnetic layer. 1. A method for manufacturing a magnetic recording medium, which comprises forming a compound having an unsaturated bond, and subsequently irradiating the compound with an unsaturated bond in a vacuum to polymerize the compound having an unsaturated bond.
JP58251701A 1983-12-28 1983-12-28 Method for manufacturing magnetic recording media Granted JPS60143435A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58251701A JPS60143435A (en) 1983-12-28 1983-12-28 Method for manufacturing magnetic recording media

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58251701A JPS60143435A (en) 1983-12-28 1983-12-28 Method for manufacturing magnetic recording media

Publications (2)

Publication Number Publication Date
JPS60143435A JPS60143435A (en) 1985-07-29
JPH0443326B2 true JPH0443326B2 (en) 1992-07-16

Family

ID=17226713

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58251701A Granted JPS60143435A (en) 1983-12-28 1983-12-28 Method for manufacturing magnetic recording media

Country Status (1)

Country Link
JP (1) JPS60143435A (en)

Also Published As

Publication number Publication date
JPS60143435A (en) 1985-07-29

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