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JP3139181B2 - Manufacturing method of magnetic recording medium - Google Patents
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JP3139181B2 - Manufacturing method of magnetic recording medium - Google Patents

Manufacturing method of magnetic recording medium

Info

Publication number
JP3139181B2
JP3139181B2 JP04308550A JP30855092A JP3139181B2 JP 3139181 B2 JP3139181 B2 JP 3139181B2 JP 04308550 A JP04308550 A JP 04308550A JP 30855092 A JP30855092 A JP 30855092A JP 3139181 B2 JP3139181 B2 JP 3139181B2
Authority
JP
Japan
Prior art keywords
shielding plate
film
oxygen
cylindrical
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 - Fee Related
Application number
JP04308550A
Other languages
Japanese (ja)
Other versions
JPH06162502A (en
Inventor
龍二 杉田
清和 東間
達朗 石田
泰明 伴
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 Corp
Panasonic Holdings Corp
Original Assignee
Panasonic Corp
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 Panasonic Corp, Matsushita Electric Industrial Co Ltd filed Critical Panasonic Corp
Priority to JP04308550A priority Critical patent/JP3139181B2/en
Publication of JPH06162502A publication Critical patent/JPH06162502A/en
Application granted granted Critical
Publication of JP3139181B2 publication Critical patent/JP3139181B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Physical Vapour Deposition (AREA)
  • Manufacturing Of Magnetic Record Carriers (AREA)

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は高密度記録特性の優れた
磁気記録媒体の製造方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for manufacturing a magnetic recording medium having excellent high density recording characteristics.

【0002】[0002]

【従来の技術】磁気記録再生装置は年々高密度化してお
り、短波長記録再生特性の優れた磁気記録媒体が要望さ
れている。現在では基板上に磁性粉を塗布した塗布型磁
気記録媒体が主に使用されており、上記要望を満足すべ
く特性改善がなされているが、ほぼ限界に近づいてい
る。
2. Description of the Related Art Magnetic recording / reproducing apparatuses have been increasing in density year by year, and a magnetic recording medium having excellent short-wavelength recording / reproducing characteristics has been demanded. At present, a coating type magnetic recording medium in which a magnetic powder is coated on a substrate is mainly used, and the characteristics have been improved to satisfy the above-mentioned demands, but they have almost reached the limit.

【0003】この限界を越えるものとして薄膜型磁気記
録媒体が開発されている。薄膜型磁気記録媒体は真空蒸
着法、スパッタリング法、メッキ法等により作製され、
優れた短波長記録再生特性を有する。薄膜型磁気記録媒
体における磁性層としては、Co、Co−Ni、Co−
Ni−P、Co−O、Co−Ni−O、Co−Fe−
O、Co−Ni−Fe−O、Co−Cr、Co−Ni−
Cr等が検討されている。
[0003] Thin film magnetic recording media have been developed to exceed this limit. The thin-film magnetic recording medium is manufactured by a vacuum evaporation method, a sputtering method, a plating method, and the like.
Has excellent short-wavelength recording / reproducing characteristics. As the magnetic layer in the thin-film type magnetic recording medium, Co, Co-Ni, Co-
Ni-P, Co-O, Co-Ni-O, Co-Fe-
O, Co-Ni-Fe-O, Co-Cr, Co-Ni-
Cr and the like are being studied.

【0004】磁気テープへの応用の点からは、これらの
中で、部分酸化膜であるCo−O膜、Co−Ni−O膜
が最も適していると考えられており、Co−Ni−Oを
磁性層とした蒸着テープが既にHi8方式VTRテープ
として実用化されている。
[0004] From the viewpoint of application to a magnetic tape, it is considered that a Co-O film or a Co-Ni-O film which is a partial oxide film is most suitable among these, and a Co-Ni-O film is considered. Has already been put to practical use as a Hi8 type VTR tape.

【0005】蒸着テープ製造方法の一例を、(図2)を
用いて以下に説明する。(図2)は蒸着テープを作製す
るための真空蒸着装置内部の構成の一例である。高分子
フィルムから成る基板1は円筒状キャン2に沿って矢印
6の向きに走行する。蒸発源8から蒸発した蒸発原子9
が、基板1に付着することにより磁性層が形成される。
[0005] An example of a method for manufacturing a vapor deposition tape will be described below with reference to FIG. (FIG. 2) is an example of a configuration inside a vacuum evaporation apparatus for producing an evaporation tape. The substrate 1 made of a polymer film travels along the cylindrical can 2 in the direction of arrow 6. Evaporated atoms 9 evaporated from the evaporation source 8
Adhere to the substrate 1 to form a magnetic layer.

【0006】蒸発源8としては電子ビーム蒸発源が適し
ており、この中に蒸発物質7としてのCo基の合金を充
填する。なお、蒸発源として電子ビーム蒸発源を用いる
のは、Co等の高融点金属を高い蒸発速度で蒸発させる
ためである。3A、3Bは不用な蒸発原子が基板に付着
するのを防ぐために設けてある遮蔽板であり、前者は膜
形成開始部を規制する遮蔽板、後者は膜形成終了部を規
制する遮蔽板である。(図2)においては、いずれの遮
蔽板も1重、すなわち1枚の板から成っている。10は
蒸着時に真空槽内に酸素を導入するための酸素導入口で
ある。θi、θfは、それぞれ膜形成開始部及び膜形成終
了部における蒸発原子9の基板1への入射角である。現
在市販されているHi8方式VTR用蒸着テープは、以
上のような方法で製造されている。4、5はそれぞれ基
板1の供給ロールと巻き取りロールである。
As the evaporation source 8, an electron beam evaporation source is suitable, in which a Co-based alloy as the evaporating substance 7 is filled. The reason why an electron beam evaporation source is used as the evaporation source is to evaporate a high melting point metal such as Co at a high evaporation rate. Reference numerals 3A and 3B denote shielding plates provided to prevent unnecessary evaporated atoms from adhering to the substrate. The former is a shielding plate for regulating a film formation start portion, and the latter is a shielding plate for regulating a film formation end portion. . In FIG. 2, each of the shielding plates has a single layer, that is, a single plate. Reference numeral 10 denotes an oxygen inlet for introducing oxygen into the vacuum chamber during vapor deposition. θ i and θ f are incident angles of the evaporated atoms 9 on the substrate 1 at the film formation start portion and the film formation end portion, respectively. The currently commercially available evaporated tape for Hi8 type VTR is manufactured by the above method. Reference numerals 4 and 5 denote a supply roll and a take-up roll of the substrate 1, respectively.

【0007】このようにして作製されたCo−Oあるい
はCo−Ni−O磁性層は、磁化容易軸が膜面の法線に
対して傾斜している。すなわち、磁化容易軸が膜面内あ
るいは膜面の法線方向にあるのではなく、蒸発原子の基
板への入射方向を含む法面内において、法線に対して斜
めに傾斜した方向にある。
In the Co—O or Co—Ni—O magnetic layer thus manufactured, the axis of easy magnetization is inclined with respect to the normal to the film surface. That is, the axis of easy magnetization is not in the film plane or in the normal direction of the film surface, but in the normal plane including the incident direction of the evaporated atoms to the substrate, in the direction oblique to the normal line.

【0008】以上説明したような部分酸化膜から成る磁
性層は、蒸着時の酸素導入量及び酸素導入方法によって
記録再生特性が大きく変化する。
[0008] The recording / reproducing characteristics of the magnetic layer composed of the partial oxide film as described above greatly vary depending on the amount of oxygen introduced during vapor deposition and the method of introducing oxygen.

【0009】[0009]

【発明が解決しようとする課題】今後、磁気テープには
短波長領域における高出力、高S/Nの要求がますます
強くなる。この要求に応える方法としては、部分酸化膜
から成る磁性層において、その成膜時に酸素の導入方法
を改善することが有望と考えられる。
In the future, demands for high output and high S / N in a short wavelength region will be further increased for magnetic tapes. As a method for meeting this demand, it is considered promising to improve the method of introducing oxygen into the magnetic layer made of a partial oxide film during the film formation.

【0010】[0010]

【課題を解決するための手段】本発明は上記要望を実現
したものであって、円筒状キャンに沿って走行しつつあ
る基板上に、磁化容易軸が膜面の法線に対して傾斜して
いるCo基の磁性層を真空蒸着法により形成する際に、
膜形成終了部を規制する遮蔽板を2重以上の構造とし、
かつ前記遮蔽板間及び遮蔽板と前記円筒状キャンとの間
から酸素を蒸発原子に向かって吹き出すことを特徴とす
る。
SUMMARY OF THE INVENTION The present invention fulfills the above-mentioned demands. In the present invention, an axis of easy magnetization is inclined on a substrate running along a cylindrical can with respect to a normal to a film surface. When forming a Co-based magnetic layer by a vacuum evaporation method,
The shielding plate that regulates the film formation end portion has a structure of two or more layers,
Further, oxygen is blown out toward the evaporated atoms from between the shielding plates and between the shielding plate and the cylindrical can.

【0011】[0011]

【作用】本発明の方法によれば、磁性層の膜厚方向にお
ける酸素濃度分布の最適化及び膜形成終了部における蒸
発原子の回り込みの防止ができるので、短波長領域で高
出力、高S/Nを有する磁気テープを提供できる。
According to the method of the present invention, it is possible to optimize the oxygen concentration distribution in the thickness direction of the magnetic layer and to prevent the evaporation of evaporated atoms at the end of film formation. N can be provided.

【0012】[0012]

【実施例】本発明の実施例を(図1)に基づいて説明す
る。(図1)は本発明の方法を実施するための真空蒸着
装置内部の一例を示す。基本的には、(図2)に示した
従来のものと同様であるが、膜形成終了部を規制する遮
蔽板が異なる。本発明においては、膜形成終了部を規制
する遮蔽板は2重以上になっており、(図1)は2重の
場合の例である。すなわち(図1)に示す如く、膜形成
終了部を規制する遮蔽板は、3Bと3B’とから成って
おり、2重の構造となっている。また酸素導入口10
は、(図1)の如く配置されており、ここから出た酸素
は、遮蔽板3Bと3B’の間及び遮蔽板3B’と円筒状
キャン2の間を通って、蒸発原子9に向かって吹き出
す。遮蔽板3Bの左端と遮蔽板3B’との距離及び遮蔽
板3B’の左端と円筒状キャンとの距離は2cm以下にな
るように設定することが望ましい。また、酸素は各遮蔽
板間及び遮蔽板と円筒状キャンとの間のいずれからも吹
き出す必要がある。そうしないと本発明の効果は著しく
低下する。(図1)は2重の場合の例であるが、3重以
上にしても2重の場合と同様の効果がある。なお、3重
以上の場合は、遮蔽板間のすべてから酸素を吹き出す必
要はなく、少なくとも円筒状キャンに近い遮蔽板間の1
箇所から吹き出せばよい。また、(図1)では、酸素導
入口は1箇所であるが、遮蔽板3Bと3B’との間及び
遮蔽版3B’と円筒状キャン2との間に、それぞれ酸素
導入口を配置してもよい。
An embodiment of the present invention will be described with reference to FIG. FIG. 1 shows an example of the inside of a vacuum deposition apparatus for carrying out the method of the present invention. Basically, it is the same as the conventional one shown in FIG. 2 (FIG. 2), except that a shielding plate for regulating the film formation end portion is different. In the present invention, the shielding plate that regulates the film formation end portion is double or more, and FIG. 1 is an example of the case of double. That is, as shown in FIG. 1, the shielding plate that regulates the film formation end portion is composed of 3B and 3B ′, and has a double structure. In addition, oxygen inlet 10
Are arranged as shown in FIG. 1, and the oxygen coming out therefrom passes between the shielding plates 3B and 3B ′ and between the shielding plate 3B ′ and the cylindrical can 2 toward the evaporated atoms 9. Blow out. It is desirable that the distance between the left end of the shielding plate 3B and the shielding plate 3B 'and the distance between the left end of the shielding plate 3B' and the cylindrical can be set to 2 cm or less. Further, oxygen needs to be blown out from between each shielding plate and between the shielding plate and the cylindrical can. Otherwise, the effects of the present invention will be significantly reduced. FIG. 1 shows an example in the case of double, but the same effect as in the case of double is obtained even in the case of triple or more. In addition, triple
In the above case, oxygen must be blown out from everything between the shielding plates.
There is no need, at least one between the shielding plates close to the cylindrical can
You just need to blow it out of the place. In FIG. 1, there is one oxygen inlet, but between the shielding plates 3B and 3B ′ and between the shielding plate 3B ′ and the cylindrical can 2, oxygen inlets are respectively arranged. Is also good.

【0013】以上のような設定により、従来の製造方法
で作製した蒸着テープに比べて、磁性層膜厚方向におけ
る酸素濃度分布の最適化と蒸発原子の回り込み防止を同
時に実現できるので、短波長領域において高い再生出力
及び高S/Nを有する磁気テープを得ることが出来る。
With the above setting, the optimization of the oxygen concentration distribution in the thickness direction of the magnetic layer and the prevention of the wraparound of the evaporated atoms can be realized at the same time as compared with the evaporation tape manufactured by the conventional manufacturing method. Thus, a magnetic tape having a high reproduction output and a high S / N can be obtained.

【0014】蒸発原子の回り込みについて(図2)を用
いて説明する。(図2)に示される、膜形成終了部を規
制する遮蔽板3Bで規制された蒸発原子が、(図2)に
示す如く、そのまま直進してθfの入射角で基板に付着
するのであれば、蒸発原子の回り込みは全く無いことに
なる。ところが実際には、蒸発原子は主に拡散によって
移動しているので、遮蔽板3Bと円筒状キャン2の間の
蒸発原子は、(図2)に示されるよりも右側に広がる。
このことを回り込みと呼ぶ。回り込みがあると、蒸発原
子はθfよりも小さい入射角で基板に付着することにな
る。このような回り込みで付着した蒸発原子は、磁性層
の記録再生特性を著しく劣化させる。
The wraparound of the evaporated atoms will be described with reference to FIG. (Figure 2) shown in, evaporated atoms which is regulated by a shielding plate 3B for regulating the film forming completion portion, as shown in (FIG. 2), whether to adhere to the substrate as it incident angle of the rectilinear to theta f In other words, there is no wraparound of the evaporated atoms. However, in practice, the evaporated atoms move mainly by diffusion, so that the evaporated atoms between the shielding plate 3B and the cylindrical can 2 spread to the right side as shown in FIG. 2.
This is called wraparound. If there is wraparound, evaporated atoms would adhere to the substrate at a small angle of incidence than theta f. The evaporated atoms attached by such wraparound significantly deteriorate the recording / reproducing characteristics of the magnetic layer.

【0015】次に、(図1)に示す本発明の構成で高い
再生出力及び高S/Nを有する媒体が得られる理由を詳
しく説明する。
Next, the reason why a medium having a high reproduction output and a high S / N can be obtained with the structure of the present invention shown in FIG. 1 will be described in detail.

【0016】(図2)に示す構成の従来の真空蒸着装置
で、Co基の磁性層から成る蒸着テープを作製する際
に、(図2)における膜形成終了部を規制する遮蔽板3
Bの左端と円筒状キャン2との距離(以下この距離をX
とする)を変えると、θfを同一に設定しておいても記
録再生特性が変化する。Xを大きくすると酸素ガスが流
れ易くなるので、蒸発原子に向かう酸素量が増加する。
単に蒸発原子に向かう酸素量が増加するだけであれば、
再生出力の増加及びノイズの低下が期待できるが、Xを
大きくすると蒸発原子の回り込み量が増える。回り込み
は再生出力を低下させる。この低下量の方が、酸素量が
増えることによる再生出力の増加よりも大きいので、総
合すると、Xを大きくすると、再生出力は低下してしま
うことになる。従って、回り込みを増加させずに酸素量
を増やせれば、再生出力の増加及びノイズの低下が期待
できる。
When a conventional vacuum vapor deposition apparatus having the structure shown in FIG. 2 is used to produce a vapor deposition tape composed of a Co-based magnetic layer, a shielding plate 3 for regulating the end of film formation in FIG. 2 is used.
A distance between the left end of B and the cylindrical can 2 (hereinafter, this distance is X
), The recording / reproducing characteristics change even if θ f is set to be the same. When X is increased, the oxygen gas flows more easily, so that the amount of oxygen toward the evaporated atoms increases.
If the amount of oxygen going to the evaporated atoms simply increases,
An increase in reproduction output and a decrease in noise can be expected. However, when X is increased, the amount of wraparound of evaporated atoms increases. The wraparound reduces the reproduction output. Since the amount of decrease is greater than the increase in reproduction output due to an increase in the amount of oxygen, when X is increased, the reproduction output decreases. Therefore, if the amount of oxygen can be increased without increasing the wraparound, an increase in reproduction output and a decrease in noise can be expected.

【0017】本発明のように2重以上の遮蔽板を使用す
ると、回り込みにより基板に付着する蒸発原子の量を増
加させずに、蒸発原子に向かう酸素量を増加させること
ができる。その結果、再生出力の増加及びノイズの低減
を図ることができる。
When a double or more shield plate is used as in the present invention, the amount of oxygen toward the evaporated atoms can be increased without increasing the amount of evaporated atoms attached to the substrate due to wraparound. As a result, it is possible to increase the reproduction output and reduce noise.

【0018】以下に、本発明の具体的実施例について説
明する。まず、(図1)のような基本構成を有する真空
蒸着装置を用いて、蒸着テープを作製した。円筒状キャ
ン2の直径は1mとし、テープ厚10μmのポリエチレン
テレフタレートフィルムを基板1として使用した。蒸発
物質7としてはCoを用いた。遮蔽板3Bの左端と遮蔽
板3B’との距離及び遮蔽板3B’左端と円筒状キャン
2との距離は1cmに設定した。膜形成開始部の入射角θ
iは85゜、膜形成終了部の入射角θfは55゜に設定し
た。
Hereinafter, specific embodiments of the present invention will be described. First, an evaporation tape was produced using a vacuum evaporation apparatus having a basic configuration as shown in FIG. The diameter of the cylindrical can 2 was 1 m, and a polyethylene terephthalate film having a tape thickness of 10 μm was used as the substrate 1. Co was used as the evaporating substance 7. The distance between the left end of the shield plate 3B and the shield plate 3B 'and the distance between the left end of the shield plate 3B' and the cylindrical can 2 were set to 1 cm. Incident angle θ at the start of film formation
i was set at 85 °, and the incident angle θ f at the film formation end portion was set at 55 °.

【0019】以上のような構成で、平均の膜堆積速度を
0.3μm/sとして、膜厚0.1μmの磁性層を形成し
た。なお、酸素導入口10から真空槽内へは、0.8l/
minの割合で酸素を導入した。以上のようにして作製し
た媒体をサンプル(1)とする。
With the above configuration, a magnetic layer having a thickness of 0.1 μm was formed at an average film deposition rate of 0.3 μm / s. In addition, 0.8 l /
Oxygen was introduced at a rate of min. The medium manufactured as described above is referred to as a sample (1).

【0020】比較のために、遮蔽板3Bと3B’との間
に酸素の通過を阻止する板を配置して、酸素を遮蔽板3
B’と円筒状キャン2との間からのみ吹き出して、それ
以外の条件は、上記と同一にして媒体を作製した。これ
をサンプル(2)とする。また、遮蔽板3B’と円筒状
キャン2との間に酸素の通過を阻止する板を配置し、酸
素を遮蔽板3Bと3B’との間からのみ吹き出して、そ
れ以外の条件は上記と同一にして媒体を作製した。これ
をサンプル(3)とする。
For comparison, a plate for blocking the passage of oxygen is disposed between the shielding plates 3B and 3B ', so that oxygen is shielded from the shielding plate 3B.
A medium was produced by blowing out only from between B ′ and the cylindrical can 2 and the other conditions were the same as above. This is designated as sample (2). Further, a plate for blocking the passage of oxygen is disposed between the shielding plate 3B 'and the cylindrical can 2, and oxygen is blown only from between the shielding plates 3B and 3B'. Other conditions are the same as those described above. To produce a medium. This is designated as sample (3).

【0021】さらに、比較のために、(図2)のような
従来の基本構成を有する真空蒸着装置を用いて、蒸着テ
ープを作製した。膜形成終了部を規制する遮蔽板が3B
のみで1重であることを除いては、上記と全く同じ条件
で成膜した。ただし、遮蔽板3Bの左端と円筒状キャン
2との距離は変化させて、3種類の媒体を作製した。こ
の距離を1cmとして作製した媒体をサンプル(4)、2
cmとしたものをサンプル(5)、4cmとしたものをサン
プル(6)とする。
Further, for comparison, an evaporation tape was manufactured using a vacuum evaporation apparatus having a conventional basic structure as shown in FIG. 3B shielding plate that regulates the end of film formation
The film was formed under exactly the same conditions as described above, except that only one layer was used. However, the distance between the left end of the shielding plate 3B and the cylindrical can 2 was changed to produce three types of media. Samples (4) and 2 (2) were prepared by setting the distance to 1 cm.
The sample having a size of 4 cm was designated as sample (5), and the sample having a size of 4 cm was designated as sample (6).

【0022】以上のようにして作製したサンプル(1)
〜(6)をテープ状にスリットし、センダストから成る
ギャップ長0.15μmのリング形磁気ヘッドを用いて
記録再生特性の評価を行なった。この評価の際には、い
ずれのサンプルにも表面に10nm厚のカーボン保護層を
形成した。評価結果を(表1)に示す。
Sample (1) prepared as described above
(6) was slit into a tape shape, and the recording / reproducing characteristics were evaluated using a ring-type magnetic head made of Sendust and having a gap length of 0.15 μm. At the time of this evaluation, a carbon protective layer having a thickness of 10 nm was formed on the surface of each sample. The evaluation results are shown in (Table 1).

【0023】[0023]

【表1】 [Table 1]

【0024】(表1)には、波長0.5μmの信号を記
録再生した際の再生出力、波長0.5μmの信号を記録
再生した際の波長0.6μmに相当する周波数における
ノイズを、サンプル(1)の値を0dBとして、これに対
する相対値で示してある。
Table 1 shows the reproduction output when recording and reproducing a signal having a wavelength of 0.5 μm and the noise at a frequency corresponding to a wavelength of 0.6 μm when recording and reproducing a signal having a wavelength of 0.5 μm. Assuming that the value of (1) is 0 dB, it is shown as a relative value to this.

【0025】(表1)から、従来の方法で作製したサン
プル(4)〜(6)は、本発明の方法で得られたサンプ
ル(1)と比較して、いずれも再生出力が低く、(図
2)の遮蔽板3Bの左端と円筒状キャン2との距離が大
きくなるに従って、再生出力が低くなっている。これは
蒸発原子の回り込みによるものと考えられる。またノイ
ズは、サンプル(4)は本発明の方法で得られたサンプ
ル(1)よりも1dB高くなっており、サンプル(5)、
(6)は(1)と同等である。
From Table 1, it can be seen that all of the samples (4) to (6) produced by the conventional method had a lower reproduction output than the sample (1) obtained by the method of the present invention. As the distance between the left end of the shielding plate 3B in FIG. 2) and the cylindrical can 2 increases, the reproduction output decreases. This is thought to be due to the wraparound of the evaporated atoms. The noise of sample (4) was 1 dB higher than that of sample (1) obtained by the method of the present invention.
(6) is equivalent to (1).

【0026】本発明の方法と同様に、遮蔽板は2重にな
っているが、酸素を遮蔽板3B’と円筒状キャン2の間
からのみ吹き出して作製したサンプル(2)、及び酸素
を遮蔽板間からのみ吹き出して作製したサンプル(3)
は、いずれも(1)よりも再生出力は1dB低く、ノイズ
は1dB高い。
As in the method of the present invention, the shielding plate is doubled, but a sample (2) produced by blowing oxygen only from between the shielding plate 3B 'and the cylindrical can 2; Sample (3) produced by blowing out only from between the plates
Are 1 dB lower in reproduction output and 1 dB higher in noise than (1).

【0027】上記の如く、本発明の方法で作製した媒体
が最も高い再生出力及び最も低いノイズを有している。
As described above, the medium produced by the method of the present invention has the highest reproduction output and the lowest noise.

【0028】以上ではCo部分酸化膜の例についてのみ
説明したが、この組成以外の部分酸化膜についても全く
同様の本発明の効果が得られる。また、基板について
は、ポリエチレンテレフタレートフィルムについて説明
したが、ポリイミドフィルム、ポリアミドフィルム、ポ
リエーテルイミドフィルム、ポリエチレンナフタレート
フィルム等の高分子フィルムでも、全く同様であること
は言うまでもない。さらに、非磁性の下地層あるいは磁
性層の形成されている高分子フィルムを基板として使用
しても、本発明の方法の効果は上記の説明と同様であ
る。また、蒸発原子の基板への入射角、θi、θfについ
ても、上記の説明の値に限ったものではない。ただし高
い再生出力を得るためには、θi>θfかつθf>50゜
なる条件を満たす必要がある。また、以上では遮蔽板が
2重の場合についての例についてのみ説明したが、3重
以上であっても上記と同様の効果が得られる。ただし、
この際、遮蔽板関の少なくとも円筒状キャンに近い側の
1箇所、及び遮蔽板と円筒状キャンとの間から、酸素を
蒸発原子に向かって吹き出すことが必要である。
Although only an example of a Co partial oxide film has been described above, the same effect of the present invention can be obtained for a partial oxide film other than this composition. Further, as the substrate, a polyethylene terephthalate film has been described, but it goes without saying that the same applies to a polymer film such as a polyimide film, a polyamide film, a polyetherimide film, and a polyethylene naphthalate film. Further, the effect of the method of the present invention is the same as described above even when a polymer film having a nonmagnetic underlayer or a magnetic layer is used as a substrate. Further, the incident angles, θ i , and θ f of the evaporated atoms on the substrate are not limited to the values described above. However, in order to obtain a high reproduction output, it is necessary to satisfy the conditions of θ i > θ f and θ f > 50 °. In the above, only the example in which the shield plate is double has been described, but the same effect can be obtained even if the shield plate is triple or more. However,
At this time, at least the side near the cylindrical can of the shielding plate
Oxygen from one location and between the shielding plate and the cylindrical can
It is necessary to blow out toward the evaporating atoms.

【0029】[0029]

【発明の効果】本発明によれば、短波長領域において高
い再生出力及び高S/Nを有する薄膜型磁気テープを提
供できる。
According to the present invention, it is possible to provide a thin-film magnetic tape having a high reproduction output and a high S / N in a short wavelength region.

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

【図1】本発明の一実施例における真空蒸着装置内部の
概略を示す図
FIG. 1 is a diagram schematically illustrating the inside of a vacuum evaporation apparatus according to an embodiment of the present invention.

【図2】従来の真空蒸着装置内部の概略を示す図FIG. 2 is a diagram schematically showing the inside of a conventional vacuum deposition apparatus.

【符号の説明】[Explanation of symbols]

1 基板 2 円筒状キャン 3A 膜形成開始部を規制する遮蔽板 3B、3B’ 膜形成終了部を規制する遮蔽板 4 供給ロール 5 巻き取りロール 6 基板走行方向 7 蒸発物質 8 蒸発源 9 蒸発原子 10 酸素導入口 DESCRIPTION OF SYMBOLS 1 Substrate 2 Cylindrical can 3A Shield plate for regulating film formation start part 3B, 3B 'Shield plate for regulating film formation end part 4 Supply roll 5 Winding roll 6 Substrate running direction 7 Evaporated substance 8 Evaporation source 9 Evaporated atom 10 Oxygen inlet

───────────────────────────────────────────────────── フロントページの続き (72)発明者 伴 泰明 大阪府門真市大字門真1006番地 松下電 器産業株式会社内 (56)参考文献 特開 平2−282479(JP,A) 特開 昭57−198543(JP,A) 特開 平4−216320(JP,A) 特開 平4−222926(JP,A) 特開 昭63−310959(JP,A) (58)調査した分野(Int.Cl.7,DB名) G11B 5/85 ────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Yasuaki Ban 1006 Kazuma, Kadoma, Osaka Prefecture Matsushita Electric Industrial Co., Ltd. (56) References JP-A-2-282479 (JP, A) JP-A-57- 198543 (JP, A) JP-A-4-216320 (JP, A) JP-A-4-222926 (JP, A) JP-A-63-310959 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) G11B 5/85

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】円筒状キャンに沿って走行しつつある基板
上に、磁化容易軸が膜面の法線に対して傾斜しているC
o基の磁性層を真空蒸着法により形成する際に、膜形成
終了部を規制する遮蔽板を2重以上の構造とし、かつ前
記遮蔽板間及び遮蔽板と前記円筒状キャンとの間から酸
素を蒸発原子に向かって吹き出すことを特徴とする磁気
記録媒体の製造方法。
1. A substrate having an axis of easy magnetization inclined on a normal to a film surface on a substrate running along a cylindrical can.
When the o-based magnetic layer is formed by a vacuum deposition method, the shielding plate that regulates the film formation end portion has a double or more structure, and oxygen is interposed between the shielding plate and between the shielding plate and the cylindrical can. Is blown toward vaporized atoms.
JP04308550A 1992-11-18 1992-11-18 Manufacturing method of magnetic recording medium Expired - Fee Related JP3139181B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP04308550A JP3139181B2 (en) 1992-11-18 1992-11-18 Manufacturing method of magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP04308550A JP3139181B2 (en) 1992-11-18 1992-11-18 Manufacturing method of magnetic recording medium

Publications (2)

Publication Number Publication Date
JPH06162502A JPH06162502A (en) 1994-06-10
JP3139181B2 true JP3139181B2 (en) 2001-02-26

Family

ID=17982383

Family Applications (1)

Application Number Title Priority Date Filing Date
JP04308550A Expired - Fee Related JP3139181B2 (en) 1992-11-18 1992-11-18 Manufacturing method of magnetic recording medium

Country Status (1)

Country Link
JP (1) JP3139181B2 (en)

Also Published As

Publication number Publication date
JPH06162502A (en) 1994-06-10

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