JPH03225622A - Production of perpendicular magnetic recording medium - Google Patents
Production of perpendicular magnetic recording mediumInfo
- Publication number
- JPH03225622A JPH03225622A JP2086790A JP2086790A JPH03225622A JP H03225622 A JPH03225622 A JP H03225622A JP 2086790 A JP2086790 A JP 2086790A JP 2086790 A JP2086790 A JP 2086790A JP H03225622 A JPH03225622 A JP H03225622A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- thickness
- sputtering
- magnetic recording
- perpendicular magnetic
- 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
Landscapes
- Manufacturing Of Magnetic Record Carriers (AREA)
Abstract
Description
【発明の詳細な説明】
イ0発明の目的
〔産業上の利用分野〕
本発明はスチルビデオ用フロッピーディスク等に用いら
れる垂直磁気記録媒体の製造方法に関する。DETAILED DESCRIPTION OF THE INVENTION Object of the Invention [Field of Industrial Application] The present invention relates to a method for manufacturing a perpendicular magnetic recording medium used in floppy disks for still videos and the like.
近年、磁気記録の高密度化の要求に伴い磁性層が磁性材
料のみによって形成された、いわゆる連続磁性薄膜磁気
記録媒体(以下連続媒体と称す)の研究が盛んに行われ
ている。In recent years, with the demand for higher density magnetic recording, research has been actively conducted on so-called continuous magnetic thin film magnetic recording media (hereinafter referred to as continuous media) in which the magnetic layer is formed only of magnetic materials.
真空蒸着法、スパッタ法、あるいはメツキ法によって作
製される連続媒体は、磁性層が連続した磁性薄膜である
ため長手記録は勿論のこと、垂直磁気記録に於て特に磁
気記録密度の飛躍的向上が期待されており、画像或いは
OA用の各種磁気テープ、或いは磁気ディスク等様々な
製品形態への応用開発が進められている。Continuous media manufactured by vacuum evaporation, sputtering, or plating have a continuous magnetic thin film layer, so they can be used not only for longitudinal recording, but also for perpendicular magnetic recording, which can dramatically improve magnetic recording density. There are high expectations for this technology, and progress is being made to apply it to various product forms such as various magnetic tapes for images or OA, or magnetic disks.
一方、最近のフロッピーディスクの小型化の要求ととも
に、磁気記録技術の向上によって、テレビ信号の1画面
分を表示するのに要する時間にあたる、1760秒の周
期で回転させながら静止画の映像信号を記録する、いわ
ゆる2インチスチルビデオ用フロッピーディスク(以下
Sv用FDと称す)が登場している。この2インチSv
用FDに記録される映像信号は、原理的にはVTRに使
用されているものと同じであり、低周波数領域に色信号
を、高周波領域に輝度信号を記録している。しかしなが
ら、静止画であるSVは、動きのあるVTRに比べ高い
画質が要求されるため、記録する周波数帯域をVTRよ
りも広く設定し、水平解像度を標準のベータVTRの2
40本に対して標準Svは357本となっている。更に
ベータVTR,SVともに高画質化の要求は高く、記録
周波数の帯域を広くしたハイバンド化が進められ、エキ
ステンデッド°デイフイニションベータVTR(以下E
DベータVTR)と、ハイバンドSvが商品化されてい
る。しかしながら、EDベータVTRの水平解像度は5
60本であるのに対し、ハイバンドSvは520本とほ
ぼ同程度の解像度が要求される。On the other hand, with the recent demand for smaller floppy disks and improvements in magnetic recording technology, still image video signals can be recorded while rotating at a cycle of 1760 seconds, which is the time required to display one screen of a television signal. A so-called 2-inch still video floppy disk (hereinafter referred to as Sv FD) has appeared. This 2 inch Sv
The video signal recorded on a commercial FD is, in principle, the same as that used in a VTR, with a color signal recorded in a low frequency region and a luminance signal recorded in a high frequency region. However, since SV, which is a still image, requires higher image quality than VTR with movement, the recording frequency band is set wider than that of VTR, and the horizontal resolution is set to 2 that of standard Beta VTR.
The standard Sv has 357 lines compared to 40 lines. Furthermore, there is a high demand for higher image quality for both Beta VTR and SV, and progress has been made toward high-band recording frequencies that widen the recording frequency band.
D Beta VTR) and high band Sv have been commercialized. However, the horizontal resolution of ED Beta VTR is 5
In contrast, the high band Sv requires approximately the same resolution of 520 lines.
従って、更に飛躍的な画質の向上を図るため、高密度磁
気記録が期待され、特に2インチSV用FDのスパッタ
リング法により作製された垂直磁気記録媒体の採用が検
討されている。ここで高画質Svシステムを垂直磁気記
録媒体で行う場合に於て、従来の標準Svシステム及び
ハイバンドSvシステムに対して解像度の低いシステム
との互換性(以下下位互換性と称す)をとることを考え
た場合、デジタル記録などの大幅な記録方式の変更を行
わず、色信号及び輝度信号の記録帯域のみ更に広くした
高画質化の方法が考えられる。Therefore, in order to further dramatically improve image quality, high-density magnetic recording is expected, and in particular, the use of perpendicular magnetic recording media manufactured by the sputtering method for 2-inch SV FDs is being considered. When performing a high-quality Sv system on a perpendicular magnetic recording medium, it is necessary to maintain compatibility (hereinafter referred to as backward compatibility) with a system with lower resolution than the conventional standard Sv system and high-band Sv system. When considering this, a method of improving image quality may be considered in which only the recording bands of color signals and luminance signals are further widened without making any major changes to the recording method such as digital recording.
ところが、垂直磁気記録媒体の記録特性は非常に高い記
録密度まで記録再生ができる反面、低記録密度の時の再
生出力が低いため、従来のSv用映像信号をそのまま記
録再生した場合、色信号のC/Hの値が足りず、下位互
換性がとれないという欠点があった。この点に対し、本
発明者はかねてより垂直磁気記録媒体に於ける低周波数
領域での再生出力を向上させる手段として、CoCr層
の磁気記録層のみで形成される垂直記録層が形成される
初期の、まだ十分に垂直配向ができていない、いわゆる
初期配向層のはたらきを検討してきた。この初期配向層
は、第1図に示すように垂直磁気記録媒体の静磁気特性
を振動型磁気特性測定装置であるVSMなどで測定し、
垂直磁気記録の場合に磁化困難方向である膜面に平行な
方向(面内方向)について磁気ヒステリシス曲線を測定
した時、初期配向層は磁気ヒステリシス曲線原点付近の
初期磁化曲線領域に生ずる磁化の跳躍部分Aをいうが、
従来数多く作製されたCoCr層のみから成る垂直磁気
記録媒体のうち、再生出力の大きなものがごくまれに含
まれており、その媒体の面内方向の磁気ヒステリシス曲
線を検討したところ、再生出力の大きな垂直磁気記録媒
体に於ては、第2図に示すように初期配向層の長手磁化
方向の成分を多く含む層、即ち初期配向層4の厚い垂直
磁気記録媒体であることが分かった。これは従来の製造
方法で作られたCoCr垂直磁気記録媒体の初期配向層
の厚さが約50オングストロームであるのに対し、再生
出力の大きい垂直磁気記録媒体については初期配向層の
厚さは200〜500オングストロームであった。この
再生出力の増加のメカニズムについてはまだ十分に解明
されていないが以下のように考えられる。However, although the recording characteristics of perpendicular magnetic recording media allow recording and reproduction up to extremely high recording densities, the reproduction output at low recording densities is low. There was a drawback that the C/H value was insufficient and backward compatibility could not be achieved. In view of this, the present inventors have long sought to improve the reproduction output in the low frequency region of perpendicular magnetic recording media by using We have been studying the function of the so-called initial alignment layer, which has not yet achieved sufficient vertical alignment. This initial orientation layer is determined by measuring the magnetostatic properties of the perpendicular magnetic recording medium using a vibrating magnetic property measuring device such as VSM, as shown in FIG.
When a magnetic hysteresis curve is measured in the direction parallel to the film surface (in-plane direction), which is the direction in which magnetization is difficult in the case of perpendicular magnetic recording, the initial alignment layer is a jump in magnetization that occurs in the initial magnetization curve region near the origin of the magnetic hysteresis curve. Part A is referred to as
Among the many perpendicular magnetic recording media made of only a CoCr layer that have been manufactured in the past, there are very few that have a large reproduction output, and when we examined the magnetic hysteresis curve in the in-plane direction of the medium, we found that It has been found that the perpendicular magnetic recording medium is a perpendicular magnetic recording medium with a thick initial orientation layer 4, which is a layer containing many components in the longitudinal magnetization direction of the initial orientation layer, as shown in FIG. This means that the thickness of the initial orientation layer of a CoCr perpendicular magnetic recording medium manufactured using a conventional manufacturing method is approximately 50 angstroms, whereas the thickness of the initial orientation layer of a perpendicular magnetic recording medium with a high reproduction output is approximately 200 angstroms. ~500 angstroms. Although the mechanism of this increase in reproduction output has not yet been fully elucidated, it is thought to be as follows.
第2図に示すように記録及び再生時に磁性層と磁気ヘッ
ド6との間に流れる磁力線7は、垂直磁気記録層3の中
ではベースフィルム5に対しほぼ垂直に流れ、初期配向
層4で水平方向に流れる。As shown in FIG. 2, magnetic lines of force 7 flowing between the magnetic layer and the magnetic head 6 during recording and reproduction flow almost perpendicularly to the base film 5 in the perpendicular magnetic recording layer 3, and horizontally in the initial orientation layer 4. flow in the direction.
この時、初期配向層はベースフィルム方向の面内方向の
磁化を持つことにより、長手記録の記録再生を行うとと
もに磁力NA7のリターンパスとなり、再生出力を増大
させる。At this time, since the initial orientation layer has magnetization in the in-plane direction in the direction of the base film, it performs recording and reproduction of longitudinal recording and serves as a return path for magnetic force NA7, increasing reproduction output.
この初期配向層の厚さについてベースフィルムの磁気記
録層を形成する前のベースフィルムからのガス出し条件
、及びベースフィルムの表面状態などの変化によって変
化することはわかっているが、主に初期配向層の厚さを
薄くする方向で検討されており、そのなかでゲルマニウ
ム、チタンなどの下地層を設けて垂直磁気記録層を形成
し易くするものが主流であった。It is known that the thickness of this initial orientation layer changes depending on the gas release conditions from the base film before forming the magnetic recording layer of the base film and changes in the surface condition of the base film. Studies have been conducted to reduce the thickness of the layer, and the mainstream has been to provide an underlayer of germanium, titanium, etc. to facilitate the formation of the perpendicular magnetic recording layer.
従って、意図的に初期配向層を厚くし、その厚みを再現
性よく制御する方法は確立されていなかった。Therefore, no method has been established for intentionally increasing the thickness of the initial alignment layer and controlling the thickness with good reproducibility.
本発明はかかる現状に鑑みてなされたものであり、その
目的とするところは、垂直磁気記録の際の再生出力を高
めるため、ベースフィルム上の初期配向層を厚くして、
垂直磁気記録の際の記録密度を向上すると共に、再生出
力を増大した垂直磁気記録媒体を得るため、初期配向層
の厚みを制御する垂直磁気記録媒体の製造方法を提供す
ることにある。The present invention has been made in view of the current situation, and its purpose is to thicken the initial orientation layer on the base film in order to increase the reproduction output during perpendicular magnetic recording.
An object of the present invention is to provide a method for manufacturing a perpendicular magnetic recording medium in which the thickness of an initial alignment layer is controlled in order to improve the recording density during perpendicular magnetic recording and to obtain a perpendicular magnetic recording medium with increased reproduction output.
口0発明の構成
〔課題を解決するための手段〕
本発明は以上の課題を解決するために、ベースフィルム
上に垂直磁気記録層の容易磁化方向と直角方向に容易磁
化方向を持つ初期配向層の形成時のスパッタ時のアルゴ
ンガス圧力を制御した製造方法を提供するもので、本発
明により初期配向層の厚さを再現性良く制御した垂直磁
気記録媒体が得られる。Structure of the Invention [Means for Solving the Problems] In order to solve the above problems, the present invention provides an initial orientation layer having an easy magnetization direction perpendicular to the easy magnetization direction of the perpendicular magnetic recording layer on a base film. According to the present invention, a perpendicular magnetic recording medium in which the thickness of the initial alignment layer is controlled with good reproducibility can be obtained.
即ち本発明は、スパッタリング法により高分子のベース
フィルム上にCoCr膜を形成する際に、スパッタ時の
アルゴンガス圧力を7X10−3Torr以上の高い圧
力でCoCr第1層を形成し、更にその上に1×10−
3Torr以下の低い圧力でCoCr第2層を形成する
ことを特徴とする垂直磁気記録媒体の製造方法である。That is, in the present invention, when forming a CoCr film on a polymer base film by a sputtering method, a CoCr first layer is formed at a high argon gas pressure of 7X10-3 Torr or more during sputtering, and then 1×10−
This is a method of manufacturing a perpendicular magnetic recording medium characterized by forming a CoCr second layer at a low pressure of 3 Torr or less.
スパッタ圧力を変化させつつCrが18.5重量%を含
むCoCr膜を形成し、様々な膜厚に於けるベースフィ
ルム面内方向についての磁気ヒステリシス曲線の第1図
に示す初期磁化曲線領域の跳躍の幅Aの量を測定した結
果を第3図に示す。A CoCr film containing 18.5% by weight of Cr was formed while changing the sputtering pressure, and the jump in the initial magnetization curve region shown in Figure 1 of the magnetic hysteresis curve in the in-plane direction of the base film at various film thicknesses was observed. The results of measuring the amount of width A are shown in FIG.
即ち、横軸にスパッタリングを行ったCoCr膜の全膜
厚を示し、その中で初期配向層にあたる磁気ヒステリシ
ス曲線の跳躍量を厚さに換算して測定した値を縦軸に示
す。That is, the horizontal axis shows the total film thickness of the sputtered CoCr film, and the vertical axis shows the value measured by converting the jump amount of the magnetic hysteresis curve corresponding to the initial alignment layer into thickness.
従って第3図はCoCr層の厚さと初期配向層の厚さと
の関係を示すが、横軸のCoCr層の全層の厚さに対し
、縦軸に示すCoCr層の厚さが垂直磁気記録層でない
初期配向層となっていることを示している。Therefore, Fig. 3 shows the relationship between the thickness of the CoCr layer and the thickness of the initial orientation layer. This indicates that the initial orientation layer is not
ここでスパッタの人力電力は500Wとし、スパッタ時
のアルゴンガス圧力の条件の範囲は1〜9 Xl0−”
Torr、又全膜厚の範囲はO〜1000オングストロ
ームとした。第3図より、5X10−3Torr以上の
スパッタアルゴンガス圧力の時には厚さが200オング
ストロ一ム以上の初期配向層が得られることがわかる。Here, the manual power for sputtering is 500 W, and the range of argon gas pressure conditions during sputtering is 1 to 9 Xl0-"
Torr and the total film thickness ranged from 0 to 1000 angstroms. It can be seen from FIG. 3 that an initial orientation layer having a thickness of 200 angstroms or more can be obtained when the sputtering argon gas pressure is 5.times.10@-3 Torr or higher.
次に5〜9X10−3Torrで、第1回目のCoCr
スパッタ膜を200オングストローム形成し、さらに1
×10−3Torrで第2回目のCoCrスパッタ膜を
0.2μm形成した。Next, at 5 to 9X10-3 Torr, the first CoCr
A sputtered film is formed to a thickness of 200 angstroms, and then 1
A second CoCr sputter film was formed to a thickness of 0.2 μm at ×10 −3 Torr.
この時の初期配向層の厚さをVSMにより測定した結果
を第4図に示す。The thickness of the initial alignment layer at this time was measured by VSM and the results are shown in FIG.
第4図より、初期配向層の厚みは第1回目CoCrスパ
ッタ膜の厚さとほぼ同じ200オングストロームで一定
値を示している。従って、7X10−3Torr以上で
初期配向層を形成し、その上に通常の0.8〜lX1O
−3Torrで垂直磁気記録層を形成する時、初期配向
層の厚さはほぼ第1回目のCoCrスパッタ膜の厚さと
することができることが確認され、本発明の目的とした
初期配向層の厚さの制御ができる垂直磁気記録媒体の製
造方法を提供出来る。From FIG. 4, the thickness of the initial alignment layer shows a constant value of 200 angstroms, which is almost the same as the thickness of the first CoCr sputtering film. Therefore, an initial alignment layer is formed at 7X10-3 Torr or more, and a normal 0.8 to 1X1O
It has been confirmed that when forming a perpendicular magnetic recording layer at −3 Torr, the thickness of the initial alignment layer can be approximately the same as the thickness of the first CoCr sputtering film, which is the thickness of the initial alignment layer aimed at in the present invention. It is possible to provide a method for manufacturing a perpendicular magnetic recording medium that can control the following.
以下、本発明の実施例を図を用い説明する。 Embodiments of the present invention will be described below with reference to the drawings.
(実施例1)
厚さ30μmのポリイミドフィルム上に、スパッタパワ
ー500W、スパッタアルゴンガス圧力5X10−3T
orrで、200オングストロームの厚さにCrが重量
比で18.5%のCoCr第1層膜を作製し、その上に
スパッタパワー500W、スパッタアルゴンガス圧力1
×10− ”Torrで0.2μmの厚さに第1層と同
一組成のCoCr第2層膜を形成した。(Example 1) Sputtering power was 500W and sputtering argon gas pressure was 5X10-3T on a polyimide film with a thickness of 30μm.
A CoCr first layer film with a thickness of 200 angstroms and a Cr content of 18.5% by weight was formed using a sputtering method with a sputtering power of 500 W and a sputtering argon gas pressure of 1.
A CoCr second layer having the same composition as the first layer was formed to a thickness of 0.2 μm at ×10−” Torr.
(実施例2)
実施例1の条件に於て、第1層膜形成のスパッタ圧力を
7X10”−3Torrとし厚さを300オングストロ
ームとし、第2層膜は実施例1と同一条件とした。(Example 2) Under the conditions of Example 1, the sputtering pressure for forming the first layer film was 7×10''-3 Torr and the thickness was 300 angstroms, and the second layer film was formed under the same conditions as Example 1.
(実施例3)
実施例1の条件に於て、第1層膜形成のスパッタ圧力を
8X10−3Torrとし厚さを400オングストロー
ムとし、第2層膜は実施例1と同一条件とした。(Example 3) Under the conditions of Example 1, the sputtering pressure for forming the first layer film was 8×10 −3 Torr and the thickness was 400 angstroms, and the second layer film was formed under the same conditions as Example 1.
(実施例4)
実施例1の条件に於て、第1層膜形成のスパッタ圧力を
9X10’−”Torrとし、厚さを500オングスト
ロームとし、第2層膜は実施例1と同じ条件とした。(Example 4) Under the conditions of Example 1, the sputtering pressure for forming the first layer film was 9 x 10'-'' Torr, the thickness was 500 angstroms, and the second layer film was formed under the same conditions as Example 1. .
(実施例5)
実施例1の条件に於て、第1層膜形成のスパツタ圧力を
9 X1O−3Torrとし厚さを200オングストロ
ームとし、第2層膜は実施例1と同じ条件とした。(Example 5) Under the conditions of Example 1, the sputtering pressure for forming the first layer was 9 X1O-3 Torr and the thickness was 200 angstroms, and the second layer was formed under the same conditions as Example 1.
(実施例6)
実施例1の条件に於て、第1層膜形成のスパッタ圧力を
9 Xl0−3Torrとし厚さを300オングストロ
ームとし、第2層膜は実施例1と同じ条件とした。(Example 6) Under the conditions of Example 1, the sputtering pressure for forming the first layer film was 9 Xl0-3 Torr and the thickness was 300 angstroms, and the second layer film was formed under the same conditions as Example 1.
(実施例7)
実施例1の条件に於て、第1層膜形成のスパッタ圧力を
9 Xl0−3Torrとし厚さを400オングストロ
ームとし、第2層膜は実施例1と同じ条件とした。(Example 7) Under the conditions of Example 1, the sputtering pressure for forming the first layer film was 9 Xl0-3 Torr and the thickness was 400 angstroms, and the second layer film was formed under the same conditions as Example 1.
実施例1ないし7により生成したCoCr磁性層につい
てVSHにより初期配向層の厚さを測定し、第1層膜の
厚さと比較した結果を第5図に示す6第5図から、初期
配向層厚さと第1層膜厚さはほぼ等しいことが分かる。The thickness of the initial alignment layer was measured by VSH for the CoCr magnetic layers produced in Examples 1 to 7, and the results of comparison with the thickness of the first layer film are shown in FIG. 5.6 From FIG. 5, the initial alignment layer thickness It can be seen that the thickness of the first layer and the thickness of the first layer are almost the same.
ハ1発明の効果
〔発明の効果〕
以上述べたように、本発明によるCrが18.5重量%
含むCoCr合金をポリイミドフィルム上にスパッタし
て垂直磁気記録媒体を形成し、ポリイミドフィルム上に
初期配向層を形成する時、スパッタ時のアルゴンガス圧
力の値を従来に比べて高い圧力とし、スパッタ層の厚さ
を制御することにより垂直磁気記録層に直角方向に容易
磁化方向を持つ初期配向層の形成により再生出力が大き
い高密度記録を可能とするCoCr垂直磁気記録媒体が
形成出来る。又ベースフィルム上にスパッタする時のア
ルゴンガス圧力を制御することにより、初期配向層の厚
さを再現性良く制御したCoCr垂直磁気記録媒体が得
られる。C1 Effect of the invention [Effect of the invention] As stated above, the Cr according to the present invention is 18.5% by weight.
When forming a perpendicular magnetic recording medium by sputtering a CoCr alloy containing CoCr alloy onto a polyimide film and forming an initial alignment layer on the polyimide film, the argon gas pressure during sputtering is set to a higher pressure than before, and the sputtered layer is By controlling the thickness of the CoCr perpendicular magnetic recording medium, a CoCr perpendicular magnetic recording medium that enables high-density recording with a large reproduction output can be formed by forming an initial orientation layer having an easy magnetization direction perpendicular to the perpendicular magnetic recording layer. Furthermore, by controlling the argon gas pressure during sputtering onto the base film, a CoCr perpendicular magnetic recording medium in which the thickness of the initial alignment layer is controlled with good reproducibility can be obtained.
第1図はベースフィルム上の初期配向層を示す垂直磁気
記録媒体のベースフィルム面内方向の磁気ヒステリシス
曲線の図。
第2図は十分な初期配向層を持った垂直磁気記録媒体の
記録再生過程を示す断面図。
第3図はCoCr膜厚さ全体の厚さと、その初期配向層
の厚さとの関係をスパッタ時のアルゴンガス圧力を変え
測定した特性図。
第4図はCoCr第1層のスパッタ圧力を変化させて、
CoCr第2層を形成した時の初期配向き厚さを示す特
性図。
第5図は本発明の実施例に於けるCoCr第1層の厚さ
と、初期配向層の厚さとの関係を示す特性図。
A・・・初期配向層による磁化の跳躇の領域、B・・・
CoCr磁性層全体の磁束密度の値、3・・・垂直磁気
記録層、4・・・初期配向層、5・・・ベースフィルム
、6・・・磁気ヘッド、7・・・磁力線。FIG. 1 is a diagram of a magnetic hysteresis curve in the in-plane direction of the base film of a perpendicular magnetic recording medium showing an initial orientation layer on the base film. FIG. 2 is a cross-sectional view showing the recording and reproducing process of a perpendicular magnetic recording medium having a sufficient initial orientation layer. FIG. 3 is a characteristic diagram obtained by measuring the relationship between the overall thickness of the CoCr film and the thickness of its initial alignment layer by changing the argon gas pressure during sputtering. FIG. 4 shows that by changing the sputtering pressure of the first CoCr layer,
FIG. 3 is a characteristic diagram showing the initial orientation thickness when forming a CoCr second layer. FIG. 5 is a characteristic diagram showing the relationship between the thickness of the first CoCr layer and the thickness of the initial alignment layer in an example of the present invention. A... Region of magnetization jumping due to the initial orientation layer, B...
Value of the magnetic flux density of the entire CoCr magnetic layer, 3... Perpendicular magnetic recording layer, 4... Initial orientation layer, 5... Base film, 6... Magnetic head, 7... Lines of magnetic force.
Claims (1)
にCoCr膜を形成する際に、スパッタ時のアルゴンガ
ス圧力を7×10^−^3Torr以上の高い圧力でC
oCr第1層を形成し、更にその上に1×10^−^3
Torr以下の低い圧力でCoCr第2層を形成するこ
とを特徴とする垂直磁気記録媒体の製造方法。1. When forming a CoCr film on a polymer base film by the sputtering method, the argon gas pressure during sputtering is set to a high pressure of 7 x 10^-^3 Torr or higher.
Form the first layer of oCr, and further layer 1×10^-^3 on top of it.
A method for manufacturing a perpendicular magnetic recording medium, characterized in that a CoCr second layer is formed at a low pressure of Torr or less.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2086790A JPH03225622A (en) | 1990-01-31 | 1990-01-31 | Production of perpendicular magnetic recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2086790A JPH03225622A (en) | 1990-01-31 | 1990-01-31 | Production of perpendicular magnetic recording medium |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH03225622A true JPH03225622A (en) | 1991-10-04 |
Family
ID=12039108
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2086790A Pending JPH03225622A (en) | 1990-01-31 | 1990-01-31 | Production of perpendicular magnetic recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH03225622A (en) |
-
1990
- 1990-01-31 JP JP2086790A patent/JPH03225622A/en active Pending
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US6767651B2 (en) | Magnetic recording medium, method for manufacturing a magnetic recording medium and magnetic recording device | |
| US5492774A (en) | Perpendicular magnetic recording medium and process for production of the same | |
| US6242085B1 (en) | Magnetic recording medium and method for producing the same | |
| JPH09212855A (en) | Magnetic recording medium, magnetic head, and magnetic recording / reproducing apparatus using the same | |
| JPS60229220A (en) | Magnetic recording medium | |
| KR20070067600A (en) | Vertical Magnetic Recording Discs with Ultra-thin Nucleation Membranes for Improving Corrosion Resistance and Methods for Making the Discs | |
| US4743348A (en) | Magnetic medium for horizontal magnetization recording and method for making same | |
| US5349478A (en) | Magnetic recording and/or reproducing method having a double azimuth head arrangement | |
| US5496620A (en) | Magnetic recording medium | |
| KR100292587B1 (en) | Magnetic recording method of digital image signal | |
| US6310748B1 (en) | Magnetic thin film magnetic recording medium | |
| JP2988188B2 (en) | Magnetic recording medium and method of manufacturing the same | |
| JP4482849B2 (en) | Perpendicular magnetic recording medium and manufacturing method thereof | |
| JP3682132B2 (en) | Method for manufacturing magnetic recording medium | |
| JP4232564B2 (en) | Perpendicular magnetic recording medium | |
| EP0576954B1 (en) | Method of magnetically recording information on magnetic recording medium | |
| JPS5868234A (en) | Composite magnetic recording medium | |
| JPH03178028A (en) | Magnetic recording medium | |
| JPH03225619A (en) | Perpendicular magnetic recording medium | |
| JPH03268308A (en) | Vertical magnetic recording medium | |
| JPS5961012A (en) | perpendicular magnetic recording medium | |
| JPS6095912A (en) | Manufacture of co-zr amorphous alloy soft magnetic film | |
| JPH03242818A (en) | Magnetic recording medium | |
| JPH05182172A (en) | Perpendicular magnetic recording medium and its production as well as perpendicular magnetic recording and/or reproducing method using the same | |
| JPH03245324A (en) | Continuous magnetic thin film medium |