JPS58143435A - Manufacture of magnetic recording medium - Google Patents

Manufacture of magnetic recording medium

Info

Publication number
JPS58143435A
JPS58143435A JP2621382A JP2621382A JPS58143435A JP S58143435 A JPS58143435 A JP S58143435A JP 2621382 A JP2621382 A JP 2621382A JP 2621382 A JP2621382 A JP 2621382A JP S58143435 A JPS58143435 A JP S58143435A
Authority
JP
Japan
Prior art keywords
vapor
oxygen
partial pressure
deposition
speed
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
Application number
JP2621382A
Other languages
Japanese (ja)
Inventor
Koichi Shinohara
紘一 篠原
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 JP2621382A priority Critical patent/JPS58143435A/en
Publication of JPS58143435A publication Critical patent/JPS58143435A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/84Processes or apparatus specially adapted for manufacturing record carriers
    • G11B5/85Coating a support with a magnetic layer by vapour deposition

Landscapes

  • Manufacturing Of Magnetic Record Carriers (AREA)
  • Thin Magnetic Films (AREA)

Abstract

PURPOSE:To obtain a magnetic tape with good durability, by forming a ferromagnetic layer on the surface of a tapelike base which moves along a cooling roll, etc., so that the partial pressure of oxygen is maximum and the ratio between the whole pressure of gas other than oxygen and a mean vapor-deposition speed is less than a specific value. CONSTITUTION:The inside of a vacuum tank 10 is partitioned by a partition 11 into a take-up room 12 and a vaporation room 13 to form mutually independent evacuation systems and on the tapelike base 2 which moves along a cylindrical can 1 as shown by an arrow, the magnetic layer is formed by emitting an electron beam 7 from an electron gun 6 to a vapor-deposition source 3 for Co-Ni, etc. In this case, the minimum angle of incidence of the vapor flow passed through the mask 4 is limited; when the part where the vapor is received is A, the center of the can 1 is 0, and the part that the vapor strikes at an angle close to a tangent is A, the mean vapor-desposition speed R (Angstrom /sec) depending upon the angle AOB and the moving speed V of the substrate 1 is calculated, and vapor deposition is carried out so that the relation when the partial pressure of oxygen is maximized and the partial pressure of gas other than oxygen is denoted as Pt is satisfied. In this case, Pa is pressure unit pascal. Thus, the long-life magnetic tape which is durable even when stored under various conditions.

Description

【発明の詳細な説明】 本発明は、高分子成形物等のテープ状基体に、直接又は
非磁性層を介して、強磁性層を真空蒸着にて形成する磁
気記録媒体の製造方法に係る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for producing a magnetic recording medium, in which a ferromagnetic layer is formed by vacuum deposition on a tape-shaped substrate such as a polymer molded product, either directly or via a nonmagnetic layer.

磁気記録に於て、強磁性金属薄膜層を磁性層とした媒体
の短波長記録での有用性は良く知られている。
In magnetic recording, the usefulness of a medium having a ferromagnetic metal thin film layer as a magnetic layer for short wavelength recording is well known.

ところで、この媒体を、ヘリカルスキャンのビデオ用途
に適用し、実用規模で短波長記録をおし進めていく上で
問題となるのは、腐蝕、摩耗に対しての強磁性層の耐性
である。
However, in applying this medium to helical scan video applications and promoting short wavelength recording on a practical scale, the problem is the resistance of the ferromagnetic layer to corrosion and abrasion.

従来この種の問題の解決のためにとられた方法の多くは
、塗布、メッキ、真空蒸着、スパッタ。
Conventionally, many of the methods used to solve this type of problem include coating, plating, vacuum deposition, and sputtering.

プラズマ、OVD等の公知の薄膜形成法によシ、有機物
、金属、酸化物、金属間化合物2合金等の薄膜保護層を
配する方法であった。
The method was to deposit a thin film protective layer of an organic material, metal, oxide, intermetallic compound 2 alloy, etc. by a known thin film forming method such as plasma or OVD.

これらの方法で得た薄膜により保護効果を期待するには
、最低600人の膜厚を必要とし、この膜厚は記録波長
0.5μmの時の−edB近いスペース損失をもたりす
もので、実用上好ましくない。
In order to expect a protective effect from a thin film obtained by these methods, a film thickness of at least 600 mm is required, and this film thickness causes a space loss close to -edB at a recording wavelength of 0.5 μm. Practically unfavorable.

本発明はかかる点に鑑みなされたもので、磁性層を構成
する金属の酸化膜を表面に形成する部分酸化を利用する
ことを基本とし、数多くの実験の結果、薄膜の保護効果
が成膜条件に重要な関係があることを尽きとめ、本発明
を完成させたもあである。以下に図面を用い本発明の説
明を行う。
The present invention was developed in view of the above, and is based on the use of partial oxidation to form an oxide film on the surface of the metal constituting the magnetic layer.As a result of numerous experiments, the protective effect of the thin film was determined under the film formation conditions. I have completed the present invention by determining that there is an important relationship between the two. The present invention will be explained below using the drawings.

第1図は本発明を実施するだめの装置の一例を示す。FIG. 1 shows an example of an apparatus for carrying out the invention.

本発明においては同図に示すように、回転する冷却支持
体としての例えば円筒状キャン1に沿ってテープ状基体
2を移動させることが要件のひとつである。
In the present invention, as shown in the figure, one of the requirements is to move the tape-shaped substrate 2 along, for example, a cylindrical can 1 as a rotating cooling support.

なお第1図では、冷却支持体として円筒状キャン1を示
したが、エンドレスベルト状の冷却体であっても良いし
、円筒状キャンと上記ベルトの組み合わせであってもよ
い。
Although FIG. 1 shows a cylindrical can 1 as a cooling support, it may be an endless belt-like cooling body or a combination of a cylindrical can and the above belt.

本発明においては、強磁性膜形成時の真空雰囲気におけ
る最大分圧成分が酸素であるとともに、酸素を除く他の
気体の全圧Pt(Pa)と、蒸着速度の間に一定の関係
を保持することが、強磁性膜の後述する耐性の改良に大
きな寄与をする点にある。
In the present invention, the maximum partial pressure component in the vacuum atmosphere during the formation of the ferromagnetic film is oxygen, and a certain relationship is maintained between the total pressure Pt (Pa) of other gases other than oxygen and the deposition rate. This fact greatly contributes to improving the durability of the ferromagnetic film, which will be described later.

蒸着速度は、回転する冷却支持体に沿って移動するテー
プ状基体が蒸着を受ける時間で、得られた膜厚を割った
値を平均蒸着速度R〔入/式〕として定義する。
The vapor deposition rate is defined as the average vapor deposition rate R [in/formula], which is the value obtained by dividing the obtained film thickness by the time during which the tape-shaped substrate moving along the rotating cooling support undergoes vapor deposition.

さて第1図に示すように、円筒状キャン1の周側面に沿
って移動するテープ状基体2は、蒸発源3からの蒸気流
の一部で蒸着される。抗磁力の制御に、マスク4による
蒸気流の最小入射角が制限される。このマスクは、ニー
ドル弁6の調節によシ、酸素を導入するノズルも兼ね合
わせている。
Now, as shown in FIG. 1, the tape-shaped substrate 2 moving along the circumferential side of the cylindrical can 1 is evaporated with a portion of the vapor flow from the evaporation source 3. Controlling the coercive force limits the minimum angle of incidence of the vapor flow by the mask 4. This mask also serves as a nozzle for introducing oxygen by adjusting the needle valve 6.

勿論、独立に配設することを拒むものではないが、簡略
化して示した。回転キャンの回転軸の中心を0とし、か
つ接線に近い角度で蒸気の入射する部分をムとしまた最
小入射角で蒸気を受ける部分をBとし、さらに基体の移
動速度をV(m/5ecJとし、キャンの直径を2D(
m)とすれば、〈ムOBを2πラジアンと比較し、また
膜厚上測定すれば、平均蒸着速度R〔入/see、lは
算出される。
Of course, this does not mean that they can be arranged independently, but they are shown in a simplified manner. Let the center of the rotation axis of the rotary can be 0, and let the part where the steam is incident at an angle close to the tangent line be M, and the part that receives the steam at the minimum angle of incidence be B, and furthermore, let the moving speed of the base be V (m/5ecJ). , set the diameter of the can to 2D (
m), the average deposition rate R[in/see, l can be calculated by comparing OB with 2π radians and measuring the film thickness.

蒸発源の加熱は電子銃6より放射される加速電子ビーム
7により行われる。8はテープ状基体の送り出し軸、9
は巻き取り軸である。前処理のためのグロー処理手段、
後処理のだめのグロー処理手段、フリーローラ、エキス
パンダゴムローラ等の図示は略したが、必要に応じて配
されるのは勿論である。
The evaporation source is heated by an accelerated electron beam 7 emitted from an electron gun 6. 8 is a feeding shaft for the tape-like base; 9
is the winding shaft. glow treatment means for pretreatment;
Although the glow processing means for post-processing, free rollers, expander rubber rollers, etc. are not shown in the drawings, they are of course provided as necessary.

真空槽10は、かくへき11によシ、主として巻取機構
を具備する巻取室12と蒸着の行われる蒸着室13に仕
切られ、それぞれ独立した排気系14.15が配設され
る。
The vacuum chamber 10 is partitioned into a winding chamber 12 mainly equipped with a winding mechanism and a deposition chamber 13 where vapor deposition is performed, each of which is provided with an independent exhaust system 14, 15.

第2図は例えばステ/レスの薄板を溶接して得たエンド
レスベルト16を2つの回転駆動体17゜18により、
一定の周速で冷却しながら回転させ、これに沿わせて基
体2を搬送する場合を示す。同図におけるA、Bは第1
図における場合と同様である。
FIG. 2 shows an endless belt 16 obtained by welding thin steel plates, for example, by two rotary drive bodies 17 and 18.
A case is shown in which the substrate 2 is rotated at a constant circumferential speed while being cooled, and the substrate 2 is conveyed along this rotation. A and B in the same figure are the first
This is the same as in the figure.

これらの装置を利用して、ポリエチレンテレフタレート
フィルム(厚さ10μm)の基体を用い長さ1000m
にわたって蒸着を行い、フィルムの平坦化処理後、%イ
/チ幅にスリットして磁気テープを作成し、次いでこの
磁気テープ100m分をリールに巻き込み、60’C9
5%RHの環境に一定蒔間保持した後、オープンデツキ
により、記録波長0.83μmの再生を行い、目づまり
の頻度が、1 oomのテープ長当り3回を限度とし、
3回以上になった日数を目づまり開始日数としてデータ
をまとめた。
Using these devices, a substrate of polyethylene terephthalate film (thickness 10 μm) was used to create a film with a length of 1000 m.
After the film is flattened, it is slit to a width of %1/1 to create a magnetic tape.Then, 100m of this magnetic tape is wound onto a reel to form a 60'C9
After maintaining a constant sowing period in an environment of 5% RH, playback was performed at a recording wavelength of 0.83 μm using an open deck, and the frequency of clogging was limited to 3 times per 1 oom tape length.
The data was summarized as the number of days when the number of clogs occurred three or more times as the number of days when clogging started.

蒸発源は、mgo  からなる耐火物容器、あるいはZ
rO2からなる耐火物容器を用い、電子ビームは、電子
銃のカンード形状、ウェネルト電極形状、両者の相対位
置関係を最適化し、広範な蒸着速度(3oO人/sec
〜80oO人/5ec)の検討が可能になるよう調整し
た。
The evaporation source is a refractory container made of mgo or Z
Using a refractory container made of rO2, the electron beam is produced by optimizing the cand shape of the electron gun, the shape of the Wehnelt electrode, and the relative positional relationship between the two.
Adjustments were made to enable examination of ~80oO people/5ec).

磁性材料はGo80%Ni2O%を主として用いたが、
後述する関係が材料組成に依存するか否かについては、
0086%Ni 15%、Go90%Ni1o%、0o
7E%Ni25%、 Go 70 % Ni 30%、
Co100%の材料組成のものについて確認した。
The magnetic material mainly used was Go80%Ni2O%, but
Regarding whether the relationship described below depends on the material composition,
0086%Ni 15%, Go90%Ni1o%, 0o
7E% Ni25%, Go 70% Ni 30%,
A material composition of 100% Co was confirmed.

基板に関するゲ存性の有無は、厚さについてはポリエチ
レンテレフタレートフィルムで厚さ6μmから26μm
までのものについて調べ、材質については、厚み26μ
m一定とし、ポリアミドフィルム、ポリイミドフィルム
について調べた。
Regarding the thickness of the substrate, the thickness of the polyethylene terephthalate film is 6 μm to 26 μm.
I researched the materials up to 26μ thick.
Polyamide film and polyimide film were investigated with m constant.

なお真空度の測定は、ポンプの引き口近くと、成膜され
る基体位置近くにヌードゲージを配置して、相対的な関
係を調べることによシ行なった。
The degree of vacuum was measured by placing nude gauges near the outlet of the pump and near the position of the substrate on which the film was to be formed, and examining the relative relationship.

又質祉分析器を用いての較正も行い、酸素分圧を全圧か
ら差し引いた値を算出しPt(Pa)とした。
Calibration was also performed using a quality analyzer, and the value obtained by subtracting the oxygen partial pressure from the total pressure was calculated as Pt (Pa).

真空排気系の種類による差がみられるかどうかについて
は、油拡散ポンプ系、油拡散ポンプに液体窒素のトラッ
プを用いた系、クライオポンプ系、油拡散ポンプとコー
ルドパネル系、ターボモレキュラーポンプ系をそれぞれ
用いた場合について確認した。又油拡散ポンプ系につい
ては、鉱物油。
Regarding whether there are differences depending on the type of vacuum evacuation system, we investigated oil diffusion pump systems, oil diffusion pumps with liquid nitrogen traps, cryopump systems, oil diffusion pumps and cold panel systems, and turbo molecular pump systems. We confirmed the cases in which each was used. For oil diffusion pump systems, use mineral oil.

シリコン油等、沸点の異なる数種の油を用いその影響を
調べた。
We investigated the effects of several oils with different boiling points, such as silicone oil.

円筒状キャンの直径は1mとし、電子ビーム発生用とし
て30KV最大6ムの同軸加速形の電子銃を用い、Zr
O2製容器に0080%Ni2O%を入れて、最小入射
角36で酸素分圧2 X 10  Totrのもとで蒸
着し、電子ビームの照射条件と基体の移動速度を変え、
Pt / R(Pa−5ec1人〕をパラメータとして
ヘッド目づまシ開始日を調べた。その結果を第3図に示
す。
The diameter of the cylindrical can was 1 m, and a coaxial acceleration type electron gun of 30 KV and a maximum of 6 m was used to generate the electron beam.
0080%Ni2O% was placed in an O2 container and evaporated under an oxygen partial pressure of 2 x 10 Totr at a minimum incident angle of 36, changing the electron beam irradiation conditions and the moving speed of the substrate.
The head blinding start date was investigated using Pt/R (one Pa-5ec) as a parameter.The results are shown in FIG.

第3図から目づまり開始日が急に落ち込むゾーンがPt
/R= 7 X 10 〜8 X 10  [Pa−5
ec1人]の間に存在することが明らかである。第3図
中のエラーパーは、1000m長の磁気テープを10巻
に分割した10点のデータより求めたもので、Pt/R
が7 X 10 〜8 X 10  (Pa−5ec/
入〕以上になると、目づまシ開始日が早くなるとともに
、エラーパーの幅も広くなることが示されている。
From Figure 3, the zone where the clogging start date suddenly drops is Pt.
/R= 7 X 10 ~ 8 X 10 [Pa-5
ec1 person]. The error par in Figure 3 was obtained from data at 10 points obtained by dividing a 1000 m long magnetic tape into 10 rolls, and was obtained from Pt/R
is 7 X 10 ~ 8 X 10 (Pa-5ec/
It has been shown that when the value exceeds 1, the start date of the blind date becomes earlier and the range of error par becomes wider.

この傾向は、これまで述べた諸条件を変化させても殆ん
ど変わらなかった。
This tendency remained almost unchanged even when the various conditions mentioned above were changed.

蒸着後、酸化性のグロー処理、あるいはオゾン処理を施
した場合については、目づまり開始日の絶対値は変わる
が、前述のように急に落ち込む変曲点が存在することは
殆んど変らず、膜質に欠陥のあることを示びている。
If oxidizing glow treatment or ozone treatment is applied after vapor deposition, the absolute value of the clogging start date will change, but the fact that there will be an inflection point where there is a sudden drop as mentioned above will hardly change. , indicating that the film quality is defective.

気体成分としてN2. N20. N2. Go、 0
02等を用いた場合、ポンプ系等の条件により、大小は
あるものの、Pt/Rがほぼ類似の傾向を示すことは興
味深いことであり、その原因については、詳しく調べて
いるが、一種の汚染と考えていいと考えられる。
N2 as a gas component. N20. N2. Go, 0
It is interesting that when using 02 etc., the Pt/R shows almost similar trends, although there are differences in size depending on the conditions of the pump system etc. The cause is being investigated in detail, but it may be a type of contamination. It can be considered that this is the case.

また、第2図において、01ム=20cm 、 02B
 〜60crrL、 0102 :100CWLとし、
0080%Ni2O%を磁性材料とし、酸素分圧3X1
0  Totr下で最小入射角を40とし厚さ0.1μ
m〜0.3μmの磁性層を形成した。
Also, in Figure 2, 01mm = 20cm, 02B
~60crrL, 0102:100CWL,
0080%Ni2O% as magnetic material, oxygen partial pressure 3X1
Under 0 Totr, the minimum incident angle is 40 and the thickness is 0.1μ.
A magnetic layer with a thickness of m to 0.3 μm was formed.

Pt /Rが10 (Pa−sec/人〕台での目づま
シ開始日の飽和値は、60℃96%RHで平均260日
、40’に90%RHで平均440日で変曲点はPt 
/ R=8.3 X 10  (P a−sec1人〕
に存在した。
When Pt/R is 10 (Pa-sec/person), the saturation value on the start date of blindness is 260 days on average at 60°C and 96% RH, and 440 days on average at 90% RH at 40', and the inflection point is Pt
/ R = 8.3 x 10 (Pa-sec 1 person)
existed in

以上に述べたことから明らかなように、本発明によi)
 Pt/Rを7 X 10  (Pa−5ec/人〕以
下に保持して磁性層を形成することによシ、各種環境で
の保存に耐える、耐性の優れた磁気記録媒体を容易に得
ることができ、本発明の工業的有価値性は犬である。
As is clear from the above, the present invention provides i)
By forming a magnetic layer with Pt/R maintained below 7 x 10 (Pa-5ec/person), it is possible to easily obtain a highly durable magnetic recording medium that can withstand storage in various environments. The industrial value of this invention is in dogs.

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

第1図は本発明を実施するための装置の一例を示す図、
第2図は上記装置の要部の変形例を示す図、第3図は本
発明の詳細な説明するための図で、Pt/Rに対するヘ
ッド目づまり開始日の関係を示す。 1・・・・・・円筒状キャン、2・・・・・・テープ状
基体、3・・・・・・蒸発源、6・・・・・・ニードル
弁、6・・・・・・電子銃、10・・・・・・真空槽。
FIG. 1 is a diagram showing an example of an apparatus for carrying out the present invention;
FIG. 2 is a diagram showing a modification of the essential parts of the above-mentioned apparatus, and FIG. 3 is a diagram for explaining the present invention in detail, showing the relationship between the head clogging start date and Pt/R. 1... Cylindrical can, 2... Tape-shaped substrate, 3... Evaporation source, 6... Needle valve, 6... Electronic Gun, 10... Vacuum tank.

Claims (1)

【特許請求の範囲】 回転する冷却支持体に沿って移動するテープ状基体上に
、最大分圧成分が酸素である真空中で蒸着法によシ強磁
性層を形成する際、酸素を除く他の気体の全圧をPt(
Pa)とし、平均蒸着速度をR〔人/就〕とする時、P
t/R≦7X 10−’ (Pa−55/人〕の関係を
満足するようにすることを特徴とする磁気記録媒体の製
造方法。
[Claims] When a ferromagnetic layer is formed on a tape-shaped substrate moving along a rotating cooling support by a vapor deposition method in a vacuum in which the maximum partial pressure component is oxygen, other than oxygen is removed. Let the total pressure of the gas be Pt(
Pa) and the average deposition rate is R [person/person], then P
A method for manufacturing a magnetic recording medium, characterized in that the relationship t/R≦7X10-' (Pa-55/person) is satisfied.
JP2621382A 1982-02-19 1982-02-19 Manufacture of magnetic recording medium Pending JPS58143435A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2621382A JPS58143435A (en) 1982-02-19 1982-02-19 Manufacture of magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2621382A JPS58143435A (en) 1982-02-19 1982-02-19 Manufacture of magnetic recording medium

Publications (1)

Publication Number Publication Date
JPS58143435A true JPS58143435A (en) 1983-08-26

Family

ID=12187144

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2621382A Pending JPS58143435A (en) 1982-02-19 1982-02-19 Manufacture of magnetic recording medium

Country Status (1)

Country Link
JP (1) JPS58143435A (en)

Similar Documents

Publication Publication Date Title
JPS5841439A (en) Magnetic recording medium and its manufacture
US4835070A (en) Magnetic recording medium and method of producing the same
JPS58143435A (en) Manufacture of magnetic recording medium
JPH0437484B2 (en)
JP2505024B2 (en) Method and apparatus for manufacturing magnetic recording medium
JPS6148128A (en) Manufacture of magnetic recording medium
JP3358352B2 (en) Film forming equipment
JPH0896339A (en) Magnetic recording medium
JP3831424B2 (en) Method for manufacturing magnetic recording medium
JPH07114731A (en) Production of magnetic recording medium
JPH07192259A (en) Production of magnetic recording medium
JPH0817050A (en) Magnetic recording medium
JPH05234075A (en) Film forming method and manufacture of magnetic recording medium
JPH0798868A (en) Production of magnetic recording medium
JPH10149540A (en) Production of magnetic recording medium
JP2002327272A (en) Film forming apparatus
JPS61278027A (en) Production of magnetic recording medium
JPH05334669A (en) Production and producing apparatus for magnetic recording medium
JPS62298026A (en) Production of magnetic recording medium
JPH11279765A (en) Thin film forming apparatus and method, and cylindrical can
JPH0636281A (en) Manufacture of magnetic recording medium
JPH08194933A (en) Magnetic recording medium, its manufacture and its manufacturing apparatus
JPS6262431A (en) Production of magnetic recording medium
JPH10188277A (en) Apparatus for production of tape-like magnetic recording medium and its production
JPH06338052A (en) Production of magnetic recording medium