JPH04188433A - Manufacture of magnetic recording medium - Google Patents
Manufacture of magnetic recording mediumInfo
- Publication number
- JPH04188433A JPH04188433A JP31925590A JP31925590A JPH04188433A JP H04188433 A JPH04188433 A JP H04188433A JP 31925590 A JP31925590 A JP 31925590A JP 31925590 A JP31925590 A JP 31925590A JP H04188433 A JPH04188433 A JP H04188433A
- Authority
- JP
- Japan
- Prior art keywords
- crucible
- magnetic
- electron beams
- recording medium
- electron beam
- 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】
口産業上の利用分野コ
本発明は磁気記録媒体の製造方法に関する。史に詳細に
は、本発明は記録再生特性の改暦された磁気記録媒体の
製造方法に関する。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a method of manufacturing a magnetic recording medium. More specifically, the present invention relates to a method of manufacturing a magnetic recording medium with improved recording/reproducing characteristics.
[従来の技術]
高密度記録技術に対する要求の、グ6まりと共に、光記
録、半導体メモリなき様々な分野で活発な技術改良が進
められるようになった。特に磁気記録の分野では従来の
磁性粉塗布型記録媒体に代わり、高密度記録材料として
Co−Ni5 Co−Crなどの磁性薄膜の研究が盛ん
に行われるようになった。[Prior Art] With the increasing demand for high-density recording technology, active technological improvements have been made in various fields including optical recording and semiconductor memory. In particular, in the field of magnetic recording, research has been actively conducted on magnetic thin films such as Co--Ni5 Co--Cr as high-density recording materials in place of conventional magnetic powder-coated recording media.
・般に、coなとの強磁性金属あるいはそれらの合金(
例えば、Co−N1)からなる磁性薄膜を有する磁気記
録媒体は、強磁性金属あるいはその合金を真空槽内に設
けられた坩堝内で電−f線照射により溶解し、加熱され
蒸発した金属蒸気をポリエステルなどのプラスチ、クフ
ィルムからなるJ1磁磁性体」−に被着することにより
形成される。・In general, ferromagnetic metals such as cobalt or their alloys (
For example, a magnetic recording medium having a magnetic thin film made of Co-N1) is produced by melting a ferromagnetic metal or its alloy by electric f-ray irradiation in a crucible installed in a vacuum chamber, and then releasing the heated and evaporated metal vapor. It is formed by adhering it to a J1 magnetic material made of plastic or film such as polyester.
〔発明が解決しようとする課題]
前記電子線照射は、坩堝内の金属を均一に加熱させるた
めに、電子線を所定の距離で走査させる方法か用いられ
ている。[Problems to be Solved by the Invention] In the electron beam irradiation, a method is used in which the electron beam is scanned at a predetermined distance in order to uniformly heat the metal in the crucible.
しかし、この方法では、特に大型装置になると、電子線
の照射スボ7ト位置か坩堝の端部に在る場合はと、非磁
性基体へ到達する粒子の入射角度か斜め方向に分散し、
柱状粒子の成長や結晶の配向性か悪化して記録+jf生
特性に悪影響を与える。However, with this method, especially when using a large device, if the electron beam is at the irradiation spot or at the end of the crucible, the particles reaching the nonmagnetic substrate will be dispersed at an angle of incidence or in an oblique direction.
The growth of columnar grains and the orientation of crystals deteriorate, which adversely affects recording +JF characteristics.
従って、本発明の目的は、ijr記従来技術における入
射粒子角度が斜め方向に分散しているという問題を解決
し、以て記録再生特性の改占された磁気記録媒体を提供
することである。Therefore, an object of the present invention is to solve the problem of the incident particle angles being obliquely dispersed in the prior art, and to provide a magnetic recording medium with improved recording and reproducing characteristics.
[課題を解決するためのf段コ
前記目的を達成するために、本発明では、電子線加熱に
よる連続蒸着法で、非磁性基体りに強磁性金属薄膜層を
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
、
強磁性金属材料を溶解する坩堝に電子線を照射して加熱
蒸発させるにあたり、電子線の走査幅りと、坩堝内の強
磁性金属材料表面と蒸発粒子の非磁性基体への最低入射
角度部分までの距離Hか、H/ (L/2)≧0.8
の関係を満足することを特徴とする磁気記録媒体の製造
方法を提供する。[F Steps to Solve the Problems] In order to achieve the above objects, the present invention provides a magnetic recording medium in which a ferromagnetic metal thin film layer is formed on a non-magnetic substrate by a continuous deposition method using electron beam heating. In the manufacturing method, when a crucible in which a ferromagnetic metal material is melted is irradiated with an electron beam to heat and evaporate it, the scanning width of the electron beam and the contact between the surface of the ferromagnetic metal material in the crucible and the evaporated particles on the non-magnetic substrate are determined. Provided is a method for manufacturing a magnetic recording medium characterized in that the distance H to the lowest incident angle portion satisfies the following relationship: H/(L/2)≧0.8.
[作用]
本発明考が長年にわたり広範な実験を続けた紡毛、非磁
性基体トに強磁性金属層を電r−線加熱蒸着法により形
成するにあたり、坩堝内にr・め充填した強磁性金属材
料に、電r1i!を走査しながら照射して加熱蒸発させ
て蒸着する際、第1図(a)に示す電子線の走査幅り、
と、第1図(b)に示す坩堝内の強磁性金属材料表面か
ら蒸発拉rの昇磁ff1基体への最低入射角度部分まで
の距1111tHが、H/ (L/2)≧0.8
の関係を満足さぜるこ乏により記録lT生特性か改西さ
れた磁気記録媒体が得られることを発見した。[Function] In forming a ferromagnetic metal layer on a non-magnetic substrate by electric r-ray heating evaporation method, the present invention has carried out extensive experiments for many years. The material is electric r1i! When performing vapor deposition by heating and evaporating by irradiating while scanning, the scanning width of the electron beam shown in Fig. 1 (a),
And, the distance 1111tH from the surface of the ferromagnetic metal material in the crucible to the lowest incident angle part of the evaporator r to the magnetized ff1 substrate shown in FIG. 1(b) is H/(L/2)≧0.8. It has been discovered that a magnetic recording medium with improved recording characteristics can be obtained by satisfying the following relationship.
これは、坩堝内の強磁性金属材料表面から 非磁性基体
までの距離を大きくすること、および/または、電子線
の走査幅を狭くすることによって、蒸発粒子の非磁性基
体への入射角度分散を減少させ、粒子の成長や結晶の配
向性を均一にするものである。This is done by increasing the distance from the surface of the ferromagnetic metal material in the crucible to the nonmagnetic substrate and/or by narrowing the scanning width of the electron beam to reduce the incident angle dispersion of the evaporated particles onto the nonmagnetic substrate. This reduces the amount of particles and makes the grain growth and crystal orientation uniform.
しかし、電子線の走査幅りと、坩堝内の強磁性金属材料
表面から蒸発$!7 Tの非磁性J^体への最低入射角
度部分までの距#Hが、H/ (L/2)<0.8では
、電Y−線の照射スポット位置か坩堝の端部にある時に
、非磁性基体りに到達する粒子の入射角度か極めて分散
し、粒子の成長や結晶の配向性が、を化する。However, due to the scanning width of the electron beam and the evaporation from the surface of the ferromagnetic metal material in the crucible! 7 When the distance #H to the lowest incident angle part of T to the non-magnetic J^ body is H/ (L/2) < 0.8, when the electric Y-ray irradiation spot position is at the end of the crucible In this case, the angle of incidence of the particles reaching the nonmagnetic substrate is extremely dispersed, and the growth of the particles and the orientation of the crystals are changed.
本発明の製造り法は垂直蒸nおよび斜め蒸着の別なく、
電子線加熱による連続蒸着ならば全てについて実施でき
る。The manufacturing method of the present invention includes vertical deposition and oblique deposition.
Continuous deposition using electron beam heating can be carried out for all types of deposition.
本発明の磁気記録媒体に使用される非磁性基板としては
、ポリイミド、ポリエステル、ポリエチレンテレフタレ
ート等の高分子フィルムなとが好適である。As the nonmagnetic substrate used in the magnetic recording medium of the present invention, polymer films such as polyimide, polyester, polyethylene terephthalate, etc. are suitable.
[実施例コ 以ド、実施例により本発明を更に詳細に説明する。[Example code] Hereinafter, the present invention will be explained in more detail with reference to Examples.
実11外↓二」Y
厚さ10μmのポリエチレンテレフタレートフィルムお
よびCo−20at%Ni合金を連続真空蒸着装置に挿
増し、lXl0−5Torr以上まて真空脱気した。次
いで、電子銃のビームを走査して坩堝内のCo−Ni合
金を照射して加熱蒸発させ、回転ドラt、に沿って走行
するボリエ千し/テレフタレートフィルムl−に厚さ0
.2μmのCo−N1からなる強磁性金属層を?JRJ
形成した。このとき、表1に示すように、電子線の走査
幅りと、坩堝内の強磁性金属材料表面と蒸発粒子の非磁
性基体への最低入射角度部分との距離Hを変化させて蒸
着した。その後、所定の幅に裁断して磁気テープを作製
した。Example 11 Outside ↓ 2''Y A 10 μm thick polyethylene terephthalate film and a Co-20at%Ni alloy were added to a continuous vacuum evaporation apparatus and vacuum degassed to a pressure of 1X10-5 Torr or more. Next, the beam of the electron gun is scanned to irradiate the Co-Ni alloy in the crucible to heat and evaporate it to form a film with a thickness of 0 on the Bolier/terephthalate film l- running along the rotating drum.
.. A ferromagnetic metal layer made of Co-N1 with a thickness of 2 μm? J.R.J.
Formed. At this time, as shown in Table 1, the scanning width of the electron beam and the distance H between the surface of the ferromagnetic metal material in the crucible and the lowest incident angle portion of the evaporated particles onto the nonmagnetic substrate were varied. Thereafter, it was cut into a predetermined width to produce a magnetic tape.
表1
各実施例における磁気テープについて、試料振動型磁力
計を用いて磁気特性を測定した。また、電磁変換特性測
定機を用いて7MHzの正位波を記録した時の7MHz
の1耳生出力を測定した。表2に、各実施例のテープの
角形比および7MHzrJ、主出力(標キメクルテープ
比)を示す。Table 1 Magnetic properties of the magnetic tapes in each example were measured using a sample vibrating magnetometer. In addition, 7MHz when recording a 7MHz positive wave using an electromagnetic conversion characteristic measuring device
The raw output of one ear was measured. Table 2 shows the squareness ratio, 7 MHzrJ, and main output (standard square tape ratio) of the tapes of each example.
表2
表2に示された結果から明らかなように、実施例1〜4
で得られた、H/ (L/2)≧0.8の要件を満たす
磁気テープは、この要件を満たさない実施例5の磁気テ
ープに比べて、角形比および7MHz M主出力が共に
高いことから、本発明の磁気テープ製造方法によれば、
記録再生特性を向上させることができる。Table 2 As is clear from the results shown in Table 2, Examples 1 to 4
The magnetic tape obtained by satisfying the requirement of H/(L/2)≧0.8 has a higher squareness ratio and 7MHz M main output than the magnetic tape of Example 5 which does not meet this requirement. According to the magnetic tape manufacturing method of the present invention,
Recording and reproducing characteristics can be improved.
[発明の効果]
以上説明したように、本発明によれば、電子線加熱によ
る連続斜め蒸着法で非磁性基体−ヒに強磁性金属薄膜層
を形成するために、強磁性金属材料を溶解する坩堝に電
子線を照射して加熱蒸発させる際、電子線の走査幅りと
、坩堝内の強磁性金属材料表面と蒸発粒子の非磁性基体
への最低入射角度部分までの距離Hが、H/(L/2)
≧0.8となるようにして蒸着を行うと記録再生特性か
向f−シた磁気記録媒体か得られる。[Effects of the Invention] As explained above, according to the present invention, a ferromagnetic metal material is melted in order to form a ferromagnetic metal thin film layer on a non-magnetic substrate by a continuous oblique evaporation method using electron beam heating. When a crucible is irradiated with an electron beam to heat and evaporate, the scanning width of the electron beam and the distance H between the surface of the ferromagnetic metal material in the crucible and the lowest incident angle of the evaporated particles on the non-magnetic substrate are H/ (L/2)
If vapor deposition is carried out in such a way that the ratio of ≧0.8 is satisfied, a magnetic recording medium with recording and reproducing characteristics opposite to f can be obtained.
第1図(a)は連続斜め74打装置における蒸発源とド
ラムを側面から見た模式図であり、第1図(b)は連続
斜め蒸着装置における蒸発源とドラムを正面から見た模
式図である。
1・・・回転ドラム、2・・・非磁性基体、3・・・坩
堝。Fig. 1(a) is a schematic diagram of the evaporation source and drum in a continuous diagonal 74-stroke device as seen from the side, and Fig. 1(b) is a schematic diagram of the evaporation source and drum in the continuous oblique evaporation device as seen from the front. It is. 1... Rotating drum, 2... Non-magnetic substrate, 3... Crucible.
Claims (1)
強磁性金属薄膜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、 強磁性金属材料を溶解する坩堝に電子線を照射して加熱
蒸発させるにあたり、電子線の走査幅Lと、坩堝内の強
磁性金属材料表面と蒸発粒子の非磁性基体への最低入射
角度部分までの距離Hが、H/(L/2)≧0.8 の関係を満足す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 that involves forming a ferromagnetic metal thin film layer on a nonmagnetic substrate by a continuous vapor deposition method using electron beam heating, a crucible in which a ferromagnetic metal material is melted is irradiated with an electron beam. During heating and evaporation, the scanning width L of the electron beam and the distance H between the surface of the ferromagnetic metal material in the crucible and the lowest angle of incidence of the evaporated particles onto the non-magnetic substrate are H/(L/2)≧0. .8 A method for manufacturing a magnetic recording medium, characterized by satisfying the following relationship.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31925590A JPH04188433A (en) | 1990-11-22 | 1990-11-22 | Manufacture of magnetic recording medium |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31925590A JPH04188433A (en) | 1990-11-22 | 1990-11-22 | Manufacture of magnetic recording medium |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH04188433A true JPH04188433A (en) | 1992-07-07 |
Family
ID=18108154
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP31925590A Pending JPH04188433A (en) | 1990-11-22 | 1990-11-22 | Manufacture of magnetic recording medium |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH04188433A (en) |
-
1990
- 1990-11-22 JP JP31925590A patent/JPH04188433A/en active Pending
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