JPH01258226A - Production of magnetic recording medium - Google Patents
Production of magnetic recording mediumInfo
- Publication number
- JPH01258226A JPH01258226A JP8566688A JP8566688A JPH01258226A JP H01258226 A JPH01258226 A JP H01258226A JP 8566688 A JP8566688 A JP 8566688A JP 8566688 A JP8566688 A JP 8566688A JP H01258226 A JPH01258226 A JP H01258226A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- columnar
- recording medium
- magnetic recording
- vapor
- 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.)
- Pending
Links
- 230000005291 magnetic effect Effects 0.000 title claims abstract description 58
- 238000004519 manufacturing process Methods 0.000 title claims description 11
- 239000000758 substrate Substances 0.000 claims abstract description 22
- 238000007740 vapor deposition Methods 0.000 claims abstract description 3
- 239000006249 magnetic particle Substances 0.000 claims description 19
- 238000000034 method Methods 0.000 claims description 8
- 238000005507 spraying Methods 0.000 claims description 7
- 239000002245 particle Substances 0.000 abstract description 5
- 238000007664 blowing Methods 0.000 abstract description 4
- 238000006243 chemical reaction Methods 0.000 abstract description 3
- 239000000696 magnetic material Substances 0.000 abstract description 3
- SGTNSNPWRIOYBX-UHFFFAOYSA-N 2-(3,4-dimethoxyphenyl)-5-{[2-(3,4-dimethoxyphenyl)ethyl](methyl)amino}-2-(propan-2-yl)pentanenitrile Chemical compound C1=C(OC)C(OC)=CC=C1CCN(C)CCCC(C#N)(C(C)C)C1=CC=C(OC)C(OC)=C1 SGTNSNPWRIOYBX-UHFFFAOYSA-N 0.000 abstract 1
- 230000003247 decreasing effect Effects 0.000 abstract 1
- 238000010438 heat treatment Methods 0.000 abstract 1
- 230000001681 protective effect Effects 0.000 abstract 1
- 239000007789 gas Substances 0.000 description 26
- 239000010408 film Substances 0.000 description 17
- 239000010410 layer Substances 0.000 description 16
- 238000001704 evaporation Methods 0.000 description 7
- 230000000694 effects Effects 0.000 description 6
- 230000008020 evaporation Effects 0.000 description 5
- 230000003746 surface roughness Effects 0.000 description 5
- 238000000151 deposition Methods 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 230000008021 deposition Effects 0.000 description 3
- 239000002985 plastic film Substances 0.000 description 3
- 229920006255 plastic film Polymers 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- 230000001590 oxidative effect Effects 0.000 description 2
- -1 polyethylene terephthalate Polymers 0.000 description 2
- 229920000139 polyethylene terephthalate Polymers 0.000 description 2
- 239000005020 polyethylene terephthalate Substances 0.000 description 2
- 239000010409 thin film Substances 0.000 description 2
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- 241001062872 Cleyera japonica Species 0.000 description 1
- 229910002441 CoNi Inorganic materials 0.000 description 1
- 229910020517 Co—Ti Inorganic materials 0.000 description 1
- 229910003271 Ni-Fe Inorganic materials 0.000 description 1
- 229910018487 Ni—Cr Inorganic materials 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 239000011230 binding agent Substances 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 238000005056 compaction Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 230000005294 ferromagnetic effect Effects 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 238000005240 physical vapour deposition Methods 0.000 description 1
- 239000011241 protective layer Substances 0.000 description 1
- 230000001105 regulatory effect Effects 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Landscapes
- Physical Vapour Deposition (AREA)
- Magnetic Record Carriers (AREA)
- Manufacturing Of Magnetic Record Carriers (AREA)
- Thin Magnetic Films (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分!PF1
本発明は磁気記録媒体の製造方法に関する。更に詳細に
は、本発明は連続斜めM打法により形成された柱状構造
の磁性層において、該柱状構造が斜め柱状部分と垂直柱
状部分とから構成されている磁気記録媒体の製造方法に
関する。[Detailed description of the invention] [Industrial use! PF1 The present invention relates to a method of manufacturing a magnetic recording medium. More specifically, the present invention relates to a method for manufacturing a magnetic recording medium in which a magnetic layer having a columnar structure is formed by a continuous oblique M-striking method, and the columnar structure is composed of an oblique columnar portion and a vertical columnar portion.
[従来の技術]
非磁性基体上に磁性体粒子を物理蒸着させることにより
磁性薄膜を形成させた、いわゆる非バインダー型磁気記
録媒体は、短波長領域における電磁変換特性に優れてい
るので、高密度記録用として好適である。[Prior Art] So-called non-binder type magnetic recording media, in which a magnetic thin film is formed by physical vapor deposition of magnetic particles on a non-magnetic substrate, have excellent electromagnetic conversion characteristics in the short wavelength region, so they can be used at high density. Suitable for recording purposes.
高密度記録用媒体としての機能を発揮するためには、媒
体表面の平滑性を高めてスペーシングロスを極力減少さ
せることが好ましい。しかし、媒体表面をあまり平坦化
させすぎると、磁気ヘッドのへラドタッチおよび走行性
が不良となる。In order to function as a high-density recording medium, it is preferable to increase the smoothness of the medium surface and reduce spacing loss as much as possible. However, if the medium surface is made too flat, the magnetic head will have poor contact and running performance.
この問題点を解決する手段として、特開昭59−924
28号公報には粒子杖突起を有する下地層を設けたプラ
スチックフィルム面上に強磁性薄膜を形成させた磁気記
録媒体が提案されている。As a means to solve this problem, Japanese Patent Laid-Open No. 59-924
No. 28 proposes a magnetic recording medium in which a ferromagnetic thin film is formed on a plastic film surface provided with an underlayer having particle projections.
この公報に開示された媒体では、粒子状突起を有するF
地層を設けたプラスチックフィルム面上に磁性体粒子を
重置蒸着させると、下地層の突起形状に対応した凸状部
が磁性層表面に形成される。In the medium disclosed in this publication, F having particulate protrusions is used.
When magnetic particles are superimposed and vapor-deposited on the surface of the plastic film provided with the base layer, convex portions corresponding to the protrusion shapes of the base layer are formed on the surface of the magnetic layer.
[発明が解決しようとする課題]
しかし、磁性体粒子を斜め蒸着させると、第6図に示さ
れるように、磁性層表面の凸状部の形状は下地層の突起
の形状に対応した形状とならず、緩斜面部分Aと急斜面
部分Bとを有する不規則な形状の凸状部が形成される。[Problems to be Solved by the Invention] However, when magnetic particles are obliquely deposited, as shown in FIG. Instead, an irregularly shaped convex portion having a gentle slope portion A and a steep slope portion B is formed.
磁気ヘッドが緩斜面方向から急斜面方向に向かって走行
する場合、下地層の突起の形状によって本来もたらされ
る走行性の改善効果はあまりみられなくなる。また、逆
に、急斜面方向から緩斜面方向にヘッドが走行する場合
、急斜面によりヘッドが引っ掛り、耐久性劣化の原因と
なる。When the magnetic head runs from a gentle slope direction to a steep slope direction, the effect of improving running performance originally brought about by the shape of the protrusions of the underlayer is not so noticeable. Conversely, when the head runs from a steep slope direction to a gentle slope direction, the head gets caught on the steep slope, causing deterioration of durability.
従って、粒子状突起を有する下地層を設けたプラスチッ
クフィルム面上に磁性体粒子を斜め蒸着させると、ヘッ
ドタッチおよび走行性は垂直蒸着させた時はど改占され
ない。Therefore, when magnetic particles are deposited obliquely on the surface of a plastic film provided with an underlayer having particulate protrusions, the head touch and runnability are not affected as much as when they are deposited vertically.
東向蒸着磁性膜に比べて、斜め蒸着磁性膜の方が高密度
記録がIIJ能な面内記録膜を形成するのに適している
。Compared to the eastward deposited magnetic film, the obliquely deposited magnetic film is more suitable for forming an in-plane recording film capable of high-density recording.
この発明は、−1ユ記従来技術が持っていた、斜め蒸着
法により磁性体粒子を蒸着させた場合に生じる磁性層表
面における突起形状の乱れという欠点を解決し、以て走
行性、耐久性および電磁変換特性に優れた磁気記録媒体
およびその製造方法を提供することを目的とする。This invention solves the drawback of the prior art described in -1 U, which is the disorder of the protrusion shape on the surface of the magnetic layer that occurs when magnetic particles are deposited by the oblique deposition method, and improves runnability and durability. Another object of the present invention is to provide a magnetic recording medium with excellent electromagnetic conversion characteristics and a method for manufacturing the same.
[課題を解決するための手段コ
本発明者が長年にわたり広範な研究と実験を続けた結果
、連続斜め蒸着法により非磁性基体i−に磁性体粒子の
柱状構造磁性層を形成する場合、前記磁性体粒子の蒸気
流の高入射側および/または低入射側にガスを吹付ける
ことにより、柱状構造中に斜め柱状部分と垂直柱状部分
とを形成させることにより前記の従来技術の欠点が解消
されることが発見された。本発明は斯かる知見に基づき
完成された。[Means for Solving the Problems] As a result of extensive research and experiments carried out by the present inventor over many years, it was found that when a columnar structure magnetic layer of magnetic particles is formed on a non-magnetic substrate i- by a continuous oblique evaporation method, the above-mentioned By blowing gas on the high incidence side and/or the low incidence side of the vapor flow of magnetic particles, the above-mentioned drawbacks of the prior art are overcome by forming oblique columnar portions and vertical columnar portions in the columnar structure. It was discovered that The present invention was completed based on this knowledge.
斜め柱状部分は柱状構造の基部寄りに形成され、垂直柱
状部分は頂部寄りに形成されることが好ましい。Preferably, the oblique columnar portion is formed closer to the base of the columnar structure, and the vertical columnar portion is formed closer to the top.
本発明の磁気記録媒体における基体は平滑基体でもよい
が、表面に、様々な形状の突起を有する基体が特に好ま
しい。Although the substrate in the magnetic recording medium of the present invention may be a smooth substrate, substrates having protrusions of various shapes on the surface are particularly preferred.
[作用]
このような突起を有する基体に、斜め柱状部分と垂直柱
状部分とからなる柱状構造の磁性体粒子の磁性膜を積層
させると、垂直柱状部分の頂点を結ぶと、下の突起の形
状と大体同じ形状の凸状部が形成される。[Function] When a magnetic film of magnetic particles having a columnar structure consisting of an oblique columnar portion and a vertical columnar portion is laminated on a substrate having such protrusions, when the vertices of the vertical columnar portions are connected, the shape of the protrusion below will change. A convex portion having approximately the same shape is formed.
かくして、斜め蒸着膜でありながら、垂直蒸着膜の場合
とほぼ同じ形状の凸状部を表面に有する磁性膜を形成す
ることができる。In this way, although it is an obliquely deposited film, it is possible to form a magnetic film that has convex portions on its surface that are approximately the same shape as those of a vertically deposited film.
また、基体の表面の突起の有無に拘わらず、柱状粒子の
頂部寄りを〜γ、ちあげ、斜め柱状部分を少なくすると
カラー信号S/Nが改善されることも期待できる。Furthermore, regardless of the presence or absence of protrusions on the surface of the substrate, it can be expected that the color signal S/N will be improved by raising the top portion of the columnar particles by ~γ and reducing the diagonal columnar portions.
[実施例]
以下、図面を参照しながら本発明の具体例について更に
詳細に説明する。[Example] Hereinafter, specific examples of the present invention will be described in more detail with reference to the drawings.
第1図は本発明の磁気記録媒体の製造に使用される連続
斜め蒸着装置の一例を、J<すa四囲である。FIG. 1 shows an example of a continuous oblique evaporation apparatus used for manufacturing the magnetic recording medium of the present invention, where J<a4.
真空系1で排気された真空槽2内において、送り出しロ
ール3から送り出された基体4は、ガイドロール5を介
して円筒状キャンロール6に沿って移動し、再びガイド
ロール5を介して巻き取りロール7に巻き取られる。こ
の時、円筒状キャンロール6の下に配設されたるつぼ8
内にセットされたCo−2ONiから成る蒸発源9を加
熱蒸発させ、防着板10aおよび10bを用い、Co−
2ONiの蒸気流11の入射角を90〜50″の範囲に
規制しながら600人/secの析出速度 で基体4上
にCo−2ONiより成る厚さ1500人の磁性層を形
成する。In the vacuum chamber 2 evacuated by the vacuum system 1, the substrate 4 sent out from the delivery roll 3 moves along the cylindrical can roll 6 via the guide roll 5, and is wound up again via the guide roll 5. It is wound up on roll 7. At this time, a crucible 8 placed under the cylindrical can roll 6
The evaporation source 9 made of Co-2ONi set in the interior is heated and evaporated, and the Co-
A magnetic layer of Co--2ONi with a thickness of 1500 layers is formed on the substrate 4 at a deposition rate of 600 layers/sec while regulating the incident angle of the 2ONi vapor flow 11 within the range of 90 to 50''.
基体には、表面に平均直径約500人の突起を106個
/mta2有する厚さ9μmのポリエチレンテレフタレ
ートフィルムを用いた。A polyethylene terephthalate film with a thickness of 9 μm and having 10 6 protrusions/mta2 with an average diameter of about 500 on the surface was used as the substrate.
実1j1−
第2図(a)に示されるように、円筒状キャンロール6
に沿って移動する基体4に入射するC。Actual 1j1- As shown in FIG. 2(a), a cylindrical can roll 6
C incident on the substrate 4 moving along.
−2ONiの蒸気流11の低入射角部Aに、ガス吹田[
]12から種々の流MのArガスを吹付けることにより
磁気記録媒体を作製した。The gas Suita [
] 12 to produce magnetic recording media by spraying Ar gas in various flows M.
K五阻λ
第2図(b)に示されるように、円筒状キャンロール6
に沿って移動する基体4に入射するC。As shown in FIG. 2(b), the cylindrical can roll 6
C incident on the substrate 4 moving along.
−2ONiの蒸気流11の高入射角部Bに、ガス吹出口
13から種々の流量のArガスを吹付けることにより磁
気記録媒体を作製した。Magnetic recording media were fabricated by spraying Ar gas at various flow rates from the gas outlet 13 onto the high incidence angle portion B of the -2ONi vapor flow 11.
支五匠1
第2図(C)に示されるように、円筒状キャンロール6
に沿って移動する基体4に入射するC。Support Gosho 1 As shown in Figure 2 (C), cylindrical can roll 6
C incident on the substrate 4 moving along.
−2ONiの蒸気流11の低入射角部Aと高入射角部B
に、それぞれガス吹出口12.13から種々の流量のA
rガスを吹付けることにより磁気記録媒体を作製した。Low incidence angle part A and high incidence angle part B of vapor flow 11 of -2ONi
A of various flow rates from the gas outlet 12 and 13, respectively.
A magnetic recording medium was produced by spraying r gas.
実施例1において蒸気流の低入射角部にガスを吹付ける
ことにより作製された磁気記録媒体の断面を第3図(a
)に示す。図示されているように、柱状構造の磁性体粒
子20の頂部寄りが立ちトげられることに伴い、斜め成
分が減少し、垂直な柱状構造に近くなる。FIG. 3(a) shows a cross section of the magnetic recording medium manufactured by blowing gas to the low incident angle portion of the vapor flow in Example 1.
). As shown in the figure, as the columnar structure of the magnetic particles 20 is raised toward the top, the oblique component decreases and the structure becomes closer to a vertical columnar structure.
第3図(b)は実施例2で作製された磁気記録媒体の断
面図である。磁性体蒸気流の高入射角部にガスが吹付け
られ、柱状構造の基部寄りは倒伏されたような形になる
ため、頂部寄りは垂直に起sitされたような形になる
。FIG. 3(b) is a cross-sectional view of the magnetic recording medium manufactured in Example 2. The gas is blown to the high incidence angle part of the magnetic vapor flow, and the base of the columnar structure has a flattened shape, while the top has a vertically sitted shape.
第3図(C)は実施例3で作製された磁気記録媒体の断
面図である。磁性体蒸気流の低入射角部と高入射角部に
ガスが吹付けられ、柱状構造の基部寄りが立ちtげられ
るとともに、頂部寄りも8翫γされるので、柱状構造は
あたかもS字状のような形になる。FIG. 3(C) is a cross-sectional view of the magnetic recording medium manufactured in Example 3. Gas is blown into the low incidence angle and high incidence angle parts of the magnetic vapor flow, and the base of the columnar structure is raised up, and the top is also tilted 8 degrees, making the columnar structure look like an S-shape. It will look like this.
基体4の表面に突起14がある場合、磁性体粒J’20
は第4図に示されるように、突起の位置および形状に対
応した凸状部を形成する。これは前記第3図(a)〜(
C)に示された何れの柱状構造の磁性体粒子によっても
同等に形成される。柱状構造の頂部寄りが巾11″1′
杖にqちLげられているためと思われる。When there are protrusions 14 on the surface of the base 4, magnetic particles J'20
As shown in FIG. 4, a convex portion is formed corresponding to the position and shape of the protrusion. This is shown in Figure 3 (a)-(
It is equally formed by magnetic particles having any of the columnar structures shown in C). The width near the top of the columnar structure is 11″1′
I think it's because he's being blown away by the cane.
表面形状観察の結果、いずれの実施例においても、ガス
流にの多いほど、ベースフィルムの表面形状に近い磁性
層表面が得られることを確認した。As a result of observing the surface shape, it was confirmed that in all Examples, the larger the gas flow, the more the surface shape of the magnetic layer could be obtained, which was closer to the surface shape of the base film.
このように、斜め蒸着時に磁性体粒子の蒸気流に吹付け
るガスの壜と方向を、31節することにより、種々の形
状のベースフィルムに対し、必要とする表面形状を有す
る磁性層が容易に得られる。In this way, by adjusting the bottle and direction of the gas that is blown onto the vapor flow of magnetic particles during oblique deposition, it is possible to easily form a magnetic layer with the required surface shape on base films of various shapes. can get.
ガス流量を増大させれば柱状構造の立ち上がりも大きく
なる。一般的な指標として、ガス流量は200〜100
0J/winの範囲内である。200J /win末滴
では柱状構造の立ち−Lげ効果が不)−分である。−・
方、1000 J /win超では蒸気流の乱れにより
柱状構造の形成が困難になる。If the gas flow rate is increased, the rise of the columnar structure will also be increased. As a general indicator, the gas flow rate is 200-100
It is within the range of 0J/win. In the case of 200 J/win droplets, the columnar structure's elongation effect is negligible. −・
On the other hand, if it exceeds 1000 J/win, it becomes difficult to form a columnar structure due to turbulence in the vapor flow.
吹付は用ガスは、Arのみでなく、チッ素、ヘリウム、
002などのガスや、これらのイオン化ガス、あるいは
、酸素などの酸化性ガスと混合しても良く、その効果も
変わらず、質埴の大きいガスはど立−Lげ効果が大きい
。The gas used for spraying is not only Ar, but also nitrogen, helium,
It may be mixed with a gas such as 002, an ionized gas thereof, or an oxidizing gas such as oxygen, and the effect remains the same; a gas with a large amount of carbon has a large oxidizing effect.
ガスの吹付け[−1の数および方向は、前記実施例で例
示されたものに限定されない。磁性体粒子の蒸気流の方
向を変えることができれば、吹付は口の数や方向は特に
限定されず、同様の柱状構造q]−げ効果が得られる。The number and direction of gas blowing [-1 are not limited to those exemplified in the above embodiments. As long as the direction of the vapor flow of the magnetic particles can be changed, the number and direction of the spraying holes are not particularly limited, and the same columnar structure q] - effect can be obtained.
磁性体粒子の蒸気流の密度が低い程効果が大きいが、低
すぎるき、形状のコントロールは困難になる。The lower the density of the vapor flow of magnetic particles, the greater the effect, but if the density is too low, it becomes difficult to control the shape.
磁性体粒子の蒸着速度に対する吹付はガスの流量の比率
自体は本発明の必須要件ではないが、−般的には、80
〜180対1の範囲内であることが好ましい。Although the ratio of the gas flow rate to the deposition rate of magnetic particles is not an essential requirement of the present invention, it is generally 80%
Preferably, the ratio is in the range of 1 to 180:1.
実施例1〜3で得られた各磁気記録媒体は、走査形電子
顕微鏡(日立製8520−LB型)で、表面形状を観察
し、触$1式表面粗さ計で磁性層表面の粗度をa1定し
た。The surface shape of each magnetic recording medium obtained in Examples 1 to 3 was observed using a scanning electron microscope (Hitachi Model 8520-LB), and the roughness of the magnetic layer surface was measured using a $1 type surface roughness meter. was determined as a1.
各実施例において、吹付けるガスの総流量が2001
/winのときを基準として、それぞれ得られた磁気テ
ープの表面粗度の測定結果を第5図に示す。ガス流量、
吹付は方向により、表面粗度が変化するのが理解される
。In each example, the total flow rate of the gas to be blown was 2001
FIG. 5 shows the measurement results of the surface roughness of the magnetic tapes obtained using the case of /win as a reference. gas flow rate,
It is understood that the surface roughness changes depending on the direction of spraying.
なお、この実施例では、基体にポリエチレンテレフタレ
ートフィルムを用いたが、一般に連続斜め蒸着に用いら
れる基体であれば、いずれも本発明の磁気記録媒体で使
用できる。In this example, a polyethylene terephthalate film was used as the substrate, but any substrate that is generally used for continuous oblique vapor deposition can be used in the magnetic recording medium of the present invention.
また、基体表面の突起形状は、シワのようなミミズ状、
粒伏など通常基体表面に形成可能な形状であれば、形状
、密度にかかわらず、本発明の方法が用いられる。In addition, the shape of the protrusions on the surface of the base is wrinkle-like, earthworm-like,
The method of the present invention can be used regardless of the shape or density as long as the shape can be formed on the surface of the substrate, such as grain compaction.
蒸発源に用いられる磁性材も、Co N iに限らず
、Co−Cr+ Co−Few Co−Mn5
Co−Ti+ Ni−Cr、N1−Fee Ni−Fe
−Cr、 Co−N1−Crq Cot Nie Fe
など、通常用いられる材料はいずれも使用できる。The magnetic material used for the evaporation source is not limited to CoNi, but also Co-Cr+ Co-Few Co-Mn5.
Co-Ti+ Ni-Cr, N1-Fee Ni-Fe
-Cr, Co-N1-Crq Cot Nie Fe
Any commonly used materials can be used.
また、本発明の方法は磁性層の形成以外にも使用できる
。例えば、ド地層、保護層など、連続斜め蒸着法を用い
て膜を形成する時であれば、いずれも、本発明の、方法
が使用できる。Furthermore, the method of the present invention can be used for purposes other than forming magnetic layers. For example, the method of the present invention can be used in any case where a film such as a base layer or a protective layer is formed using a continuous oblique evaporation method.
[発明の効果]
以上説明したように、本発明の製造方法により得られた
磁気記録媒体は高密度記録が可能な面内記録膜の形成に
適した斜め蒸着磁性膜をfrするが、磁性膜は斜め柱状
部分と昨直柱状部分とからなる柱状構造の磁性体粒子に
より形成されている。[Effects of the Invention] As explained above, the magnetic recording medium obtained by the manufacturing method of the present invention has an obliquely deposited magnetic film suitable for forming an in-plane recording film capable of high-density recording. is formed by magnetic particles having a columnar structure consisting of an oblique columnar part and a straight columnar part.
柱状構造の頂部寄りに重置柱状部分が存在すると、表面
に突起を有する基体に磁性体粒子を斜め蒸着させても、
丁の突起の形状と大体同じ形状の凸状部が、下の突起の
位置に対応した位置に形成される。If there is an overlapping columnar part near the top of the columnar structure, even if magnetic particles are obliquely deposited on a substrate with protrusions on the surface,
A convex portion having approximately the same shape as the protrusion of the knife is formed at a position corresponding to the position of the lower protrusion.
かくして、斜め蒸着膜でありながら、垂直蒸着膜の場合
とほぼ同じ形状の凸状部を表面に有する磁性膜を形成す
ることができる。その結果、磁気ヘッドの走行方向に依
存せず、走行性およびヘッドタッチに優れた磁気記録媒
体が得られる。In this way, although it is an obliquely deposited film, it is possible to form a magnetic film that has convex portions on its surface that are approximately the same shape as those of a vertically deposited film. As a result, a magnetic recording medium that is independent of the running direction of the magnetic head and has excellent running properties and head touch can be obtained.
また、基体の表面の突起の有無に拘わらず、柱状粒子の
頂部寄りを立ちあげ、斜め柱状部分を少なくするとカラ
ー信号S/Nが約+1.0dB程度改丹されることが確
認された。It was also confirmed that, regardless of the presence or absence of protrusions on the surface of the substrate, when the columnar particles were raised near the top and the oblique columnar portions were reduced, the color signal S/N was improved by about +1.0 dB.
第1図は本発明の磁気記録媒体の製造に使用される連続
斜め蒸着装置の一例を示すW1霞図であり、第2図(a
)〜(C)は磁性体の蒸気流に対するガスの吹付は態様
を示す構成図であり、第3図(a)〜(C)は基体の平
滑部分に形成された柱状構造の断面図であり、第4図は
基体の突起部分に形成された柱状構造の断面図であり、
第5図は磁性層の表面粗さとガス吹付は量との関係を示
す特性図であり、第6図は表面に突起を有する基体に磁
性体を従来の方法に従って斜め蒸着させて得られた磁気
記録媒体の断面図である。
1・・・真空系、2・・・真空榊、3・・・送出ロール
、4・・・基体、5・・・カイトロール、6・・・キャ
ンロール、7・・・巻取ロール、8・・・るつぼ、9・
・・蒸発源、10a。FIG. 1 is a W1 haze diagram showing an example of a continuous oblique evaporation apparatus used for manufacturing the magnetic recording medium of the present invention, and FIG.
) to (C) are configuration diagrams showing the manner in which gas is sprayed onto the vapor flow of the magnetic material, and FIGS. 3(a) to (C) are cross-sectional views of the columnar structure formed on the smooth part of the base. , FIG. 4 is a cross-sectional view of the columnar structure formed on the protruding portion of the base,
Fig. 5 is a characteristic diagram showing the relationship between the surface roughness of the magnetic layer and the amount of gas sprayed, and Fig. 6 is a characteristic diagram showing the relationship between the surface roughness of the magnetic layer and the amount of gas sprayed. FIG. 2 is a cross-sectional view of a recording medium. DESCRIPTION OF SYMBOLS 1... Vacuum system, 2... Vacuum Sakaki, 3... Delivery roll, 4... Substrate, 5... Kite roll, 6... Can roll, 7... Winding roll, 8 ... Crucible, 9.
...Evaporation source, 10a.
Claims (3)
の柱状構造磁性層を形成することからなる磁気記録媒体
の製造方法において、前記磁性体粒子の蒸気流の高入射
側および/または低入射側にガスを吹付けることにより
、前記柱状構造中に斜め柱状部分と垂直柱状部分とを形
成させることを特徴とする磁気記録媒体の製造方法。(1) In a method for manufacturing a magnetic recording medium, which comprises forming a columnar structured magnetic layer of magnetic particles on a non-magnetic substrate by continuous oblique vapor deposition, 1. A method of manufacturing a magnetic recording medium, characterized in that a diagonal columnar portion and a vertical columnar portion are formed in the columnar structure by spraying gas on an incident side.
特徴とする請求項(1)記載の磁気記録媒体の製造方法
。(2) The method for manufacturing a magnetic recording medium according to claim (1), wherein the columnar structure has an oblique columnar portion closer to the base.
、斜め柱状部分と垂直柱状部分とからなる柱状構造の磁
性体粒子が前記突起の形状に沿った凸状部を有する磁性
層表面を形成することを特徴とする請求項(1)記載の
磁気記録媒体の製造方法。(3) A magnetic layer in which protrusions are distributed on the surface of the nonmagnetic substrate, and magnetic particles having a columnar structure consisting of oblique columnar portions and vertical columnar portions have convex portions that follow the shape of the protrusions. 2. The method of manufacturing a magnetic recording medium according to claim 1, further comprising forming a surface.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8566688A JPH01258226A (en) | 1988-04-07 | 1988-04-07 | Production of magnetic recording medium |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8566688A JPH01258226A (en) | 1988-04-07 | 1988-04-07 | Production of magnetic recording medium |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01258226A true JPH01258226A (en) | 1989-10-16 |
Family
ID=13865146
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP8566688A Pending JPH01258226A (en) | 1988-04-07 | 1988-04-07 | Production of magnetic recording medium |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01258226A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH046627A (en) * | 1990-04-23 | 1992-01-10 | Matsushita Electric Ind Co Ltd | Highly function thin film and production thereof |
JP2006156854A (en) * | 2004-11-30 | 2006-06-15 | Tdk Corp | Magnetic thin film and its forming method |
-
1988
- 1988-04-07 JP JP8566688A patent/JPH01258226A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH046627A (en) * | 1990-04-23 | 1992-01-10 | Matsushita Electric Ind Co Ltd | Highly function thin film and production thereof |
JP2006156854A (en) * | 2004-11-30 | 2006-06-15 | Tdk Corp | Magnetic thin film and its forming method |
JP4529081B2 (en) * | 2004-11-30 | 2010-08-25 | Tdk株式会社 | Magnetic thin film |
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