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JPH07101494B2 - Metal thin film magnetic recording medium - Google Patents
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JPH07101494B2 - Metal thin film magnetic recording medium - Google Patents

Metal thin film magnetic recording medium

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Publication number
JPH07101494B2
JPH07101494B2 JP59195002A JP19500284A JPH07101494B2 JP H07101494 B2 JPH07101494 B2 JP H07101494B2 JP 59195002 A JP59195002 A JP 59195002A JP 19500284 A JP19500284 A JP 19500284A JP H07101494 B2 JPH07101494 B2 JP H07101494B2
Authority
JP
Japan
Prior art keywords
recording medium
magnetic recording
thin film
metal thin
emissivity
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 - Lifetime
Application number
JP59195002A
Other languages
Japanese (ja)
Other versions
JPS6173229A (en
Inventor
秀樹 吉田
幹夫 村居
可治 前澤
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 JP59195002A priority Critical patent/JPH07101494B2/en
Publication of JPS6173229A publication Critical patent/JPS6173229A/en
Publication of JPH07101494B2 publication Critical patent/JPH07101494B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 産業上の利用分野 本発明は高温時の耐久性を改良した金属薄膜型磁気記録
媒体に関するものである。
Description: TECHNICAL FIELD The present invention relates to a metal thin film type magnetic recording medium having improved durability at high temperatures.

従来の構成とその問題点 近年、金属薄膜型磁気記録媒体は高密度磁気記録媒体と
して注目され、次第に実用化されつつある。
Conventional Configuration and Problems Thereof In recent years, a metal thin film type magnetic recording medium has attracted attention as a high density magnetic recording medium and is gradually being put into practical use.

以下に従来の金属薄膜型磁気記録媒体について説明す
る。
The conventional metal thin film type magnetic recording medium will be described below.

第1図は従来の金属薄膜型磁気記録媒体の断面図を示す
ものであり、1は基板、2は磁性層である。金属薄膜型
磁気記録媒体の電磁変換特性は従来用いられてきた塗布
型磁気記録媒体や近年用いられつつある酸化物薄膜磁気
記録媒体の電磁変換特性と較べ、高密度記録時に非常に
優れた特性を示すことが知られている。しかし金属薄膜
型磁気記録媒体は従来の塗布型磁気記録媒体や酸化物薄
膜磁気記録媒体と較べ、実用耐久性に難点があるとさ
れ、耐久性の向上が課題とされている。耐久性は様々な
環境において異なるが、金属薄膜型磁気記録媒体にとっ
て特に問題となる条件の1つとして例えば50℃以上とい
う高温時の耐久性は重要である。高温時の耐久性が他の
環境での耐久性と較べて劣るのは、おそらく金属薄膜型
磁気記録媒体の磁性面側放射率が低い為、高温時の冷却
作用が、従来の塗布型磁気記録媒体や酸化物薄膜磁気記
録媒体と較べて劣る為、磁性面側表面の温度が上昇し耐
久性が悪化すると考えられる。
FIG. 1 is a sectional view of a conventional metal thin film magnetic recording medium, in which 1 is a substrate and 2 is a magnetic layer. The electromagnetic conversion characteristics of the metal thin film magnetic recording medium are much better than those of the coating type magnetic recording medium which has been used conventionally and the oxide thin film magnetic recording medium which has been used in recent years. It is known to show. However, it is said that the metal thin film magnetic recording medium has a difficulty in practical durability as compared with the conventional coating type magnetic recording medium and the oxide thin film magnetic recording medium, and improvement of the durability is an issue. Although the durability varies in various environments, one of the conditions that are particularly problematic for the metal thin film magnetic recording medium is the durability at a high temperature of 50 ° C. or higher, for example. The durability at high temperature is inferior to the durability in other environments, probably because the emissivity of the magnetic surface side of the metal thin film magnetic recording medium is low, so that the cooling effect at high temperature is Since it is inferior to the medium and the oxide thin film magnetic recording medium, it is considered that the temperature on the magnetic surface side rises and the durability deteriorates.

従来の金属薄膜型磁気記録媒体では、この高温時の環境
下においては磁性層が磁気ヘッドにより削られ易く、十
分な耐久性を持たなかった。
In the conventional metal thin film type magnetic recording medium, the magnetic layer is easily scraped by the magnetic head under the environment at the high temperature, and the durability is not sufficient.

発明の目的 本発明は上記従来の問題点を解消するもので、高温時に
おける耐久性を向上させた金属薄膜型磁気記録媒体を提
供するものである。
An object of the present invention is to solve the above-mentioned conventional problems and to provide a metal thin film type magnetic recording medium having improved durability at high temperature.

発明の構成 本発明は磁性面表面の100℃の波長1μmでの放射率を
0.3より大きくした金属薄膜型磁気記録媒体であり、高
温低湿下の耐久性を向上することのできるものである。
Structure of the invention The present invention is to measure the emissivity of a magnetic surface at a wavelength of 1 μm at 100 ° C
A metal thin film type magnetic recording medium having a size larger than 0.3, which can improve durability under high temperature and low humidity.

実施例の説明 以下本発明の実施例について、図面を参照しながら説明
する。
Description of Embodiments Embodiments of the present invention will be described below with reference to the drawings.

第2図は本発明の実施例における金属薄膜型磁気記録媒
体の基本構成を示す図である。第2図において、3は基
板、4は磁性層、5は放熱層である。基板3上に磁性層
4を構成し、さらにその上に放熱層5を構成し、磁性面
側表面の100℃の波長1μmでの放射率が0.3より大きく
なるようにする。
FIG. 2 is a diagram showing a basic structure of a metal thin film type magnetic recording medium in an embodiment of the present invention. In FIG. 2, 3 is a substrate, 4 is a magnetic layer, and 5 is a heat dissipation layer. The magnetic layer 4 is formed on the substrate 3, and the heat dissipation layer 5 is further formed on the magnetic layer 4, so that the emissivity of the magnetic surface side surface at 100 ° C. at a wavelength of 1 μm is larger than 0.3.

ここで基板1としてはプラスチック,金属等から適宜選
択され、磁性層2としてはCo,CoNi,Co−p,Ni−P,CoNip,
CoCr,FeCr,FeCoCr等の磁性金属材料を主成分として構成
され、磁性層2の形成方法としては真空蒸着法,スパッ
タ法,イオンプレーティング法,メッチ法等から適宜選
択される。放熱層3としては、酸化物,窒化物,炭化
物,プラスチック,樹脂等の非金属材料から適宜選択さ
れる。放熱層3の形成方法としては真空蒸着法,スパッ
タ法,イオンプレーティング法,CVD法,イオン注入法,
コーティング法,プラズマ溶射法等から適宜選択され
る。
Here, the substrate 1 is appropriately selected from plastic, metal, etc., and the magnetic layer 2 is made of Co, CoNi, Co-p, Ni-P, CoNip,
A magnetic metal material such as CoCr, FeCr, or FeCoCr is used as a main component, and the method for forming the magnetic layer 2 is appropriately selected from a vacuum deposition method, a sputtering method, an ion plating method, a metch method and the like. The heat dissipation layer 3 is appropriately selected from non-metal materials such as oxides, nitrides, carbides, plastics and resins. As the method for forming the heat dissipation layer 3, vacuum deposition method, sputtering method, ion plating method, CVD method, ion implantation method,
It is appropriately selected from coating method, plasma spraying method and the like.

電磁変換特性の観点から磁性層4の厚みは500〜3,000Å
が望ましく、放熱層の厚みは1,000Å以下更に望ましく
は500Å以下、磁性層側表面となる放熱層表面の平均粗
さは1,000Å以下、更に望ましくは500Å以下であること
が望ましい。従来、放熱層を持たない金属薄膜型磁気記
録媒体においては、磁性面側表面は金属に近く、表面形
状の影響や非金属成分の影響を受けた場合においても、
波長1μmでの放射率はせいぜい0.2以下であった。本
発明においては放射率の高い材質で放熱層を形成し、磁
性面側表面層である放熱層表面の放射率を0.3以上にす
ることにより磁性面側の放熱性を高め、従来の塗布型磁
気記録媒体や酸化物薄膜磁気記録媒体と同程度の放射率
とする。
The magnetic layer 4 has a thickness of 500 to 3,000Å from the viewpoint of electromagnetic conversion characteristics.
Desirably, the thickness of the heat dissipation layer is 1,000 Å or less, more preferably 500 Å or less, and the average roughness of the surface of the heat dissipation layer which is the magnetic layer side surface is 1,000 Å or less, more preferably 500 Å or less. Conventionally, in a metal thin film type magnetic recording medium having no heat dissipation layer, the magnetic surface side surface is close to metal, and even when affected by the surface shape or non-metal component,
The emissivity at a wavelength of 1 μm was 0.2 or less at most. In the present invention, the heat dissipation layer is formed of a material having a high emissivity, and the emissivity of the surface of the heat dissipation layer, which is the magnetic surface side, is set to 0.3 or more to enhance the heat dissipation of the magnetic surface side, and the conventional coating type magnetic The emissivity is similar to that of the recording medium or the oxide thin film magnetic recording medium.

又、放射率の測定条件および測定方法について説明す
る。
Moreover, the measurement conditions and the measurement method of the emissivity will be described.

波長を1μmと限定したのは100℃の放射における測定
信頼性の向上を意図したものである。本発明の趣旨は磁
性層表層部の放熱による冷却効果を利用するものであ
り、単一波長の放射率を問題とするものではない。しか
し、周囲環境が50℃の時磁性層表面は摩擦により50℃以
上の高温となり、100℃前後での放熱性を考慮すべき必
要があると考えられ、100℃での放射率を精度良く測定
する条件として波長を1μmと限定するものである。放
射率の波長依存性については一般的な種々のフイルター
を用いることにより容易に実現可能であり、実際には放
射率はあまり波長依存を持たず、容易に測定可能と考え
られる。また、放射率は100℃での放射エネルギーも放
射温度計で校正することにより測定できる。
The limitation of the wavelength to 1 μm is intended to improve the measurement reliability in radiation at 100 ° C. The gist of the present invention is to utilize the cooling effect of the surface layer of the magnetic layer due to heat dissipation, and does not pose a problem with the emissivity of a single wavelength. However, when the ambient environment is 50 ° C, the surface of the magnetic layer becomes a temperature of 50 ° C or higher due to friction, and it is considered necessary to consider the heat dissipation at about 100 ° C. Therefore, the emissivity at 100 ° C can be measured accurately. As a condition, the wavelength is limited to 1 μm. The wavelength dependence of the emissivity can be easily realized by using various general filters, and it is considered that the emissivity has little wavelength dependence and can be easily measured. The emissivity can be measured by calibrating the radiant energy at 100 ° C with a radiation thermometer.

以上のように金属薄膜型磁気記録媒体は、磁性面側表面
の放射率が従来の塗布型磁気記録媒体や酸化物薄膜型磁
気記録媒体と同様に放熱性が良好であり、例えば50℃と
いった高温時での使用においても放射による冷却作用に
より磁性面側表面温度の上昇を防止し、耐久性を向上さ
せるものと考えられる。
As described above, the metal thin film magnetic recording medium has good emissivity as in the case of the conventional coating type magnetic recording medium and oxide thin film type magnetic recording medium with the emissivity of the magnetic surface side surface being high at a high temperature such as 50 ° C. It is considered that even in the occasional use, the cooling effect due to radiation prevents the surface temperature on the magnetic surface side from rising and improves the durability.

以下に本発明のさらに具体的な一実施例を説明する。A more specific embodiment of the present invention will be described below.

(実施例1) 基板として厚み10μmのポリエチレンテレフタレートを
用い、Co−Ni(20wt%)を直径500mmの円筒キャンに沿
って蒸着した。蒸着は入射角が90゜となる接線方向から
開始され、次第に入射角は低くなり40゜の入射角となる
まで蒸着する。蒸着中に雰囲気ガスとしてO2ガスを導入
し抗磁力を得た。得られた蒸着膜はHc=1020Oe,δ=150
0Å,Br=4400Gaussであった。この磁性膜の上にエポキ
シ樹脂のコーティングを行ない、放熱層を形成した。エ
ポキシ樹脂の塗布量が少ない時、連続膜とはならずアイ
ランド状であり、塗布量が消えると次第に連続膜とな
る。エポキシ樹脂層厚みはアイランド状の場合には80〜
110Åで膜厚変化は少なくこの領域においてはスペーシ
ングロスによる電磁変換特性はほとんど同一であり、被
覆率の差から放射率が変化する。これらの試料の放射率
と50℃50%Rhにおけるフェライトヘッドを有する回転シ
リンダーによるスチル寿命の関係を第3図に示す。なお
放射率は100℃における波長1μmの放射率である。第
3図から明らかな様に放射率の上昇に伴ない50℃におけ
る耐久性は向上する。
Example 1 Polyethylene terephthalate having a thickness of 10 μm was used as a substrate, and Co—Ni (20 wt%) was vapor-deposited along a cylindrical can having a diameter of 500 mm. The vapor deposition starts from the tangential direction at which the incident angle becomes 90 °, and gradually decreases until the incident angle becomes 40 °. O 2 gas was introduced as an atmospheric gas during vapor deposition to obtain a coercive force. The obtained vapor deposition film has Hc = 1020 Oe, δ = 150
It was 0Å, Br = 4400 Gauss. Epoxy resin was coated on this magnetic film to form a heat dissipation layer. When the coating amount of the epoxy resin is small, it does not become a continuous film but has an island shape, and when the coating amount disappears, it becomes a continuous film gradually. Epoxy resin layer thickness is 80-
At 110Å, there is little change in film thickness, and in this region the electromagnetic conversion characteristics due to spacing loss are almost the same, and the emissivity changes due to the difference in coverage. FIG. 3 shows the relationship between the emissivity of these samples and the still life of a rotating cylinder having a ferrite head at 50 ° C. and 50% Rh. The emissivity is the emissivity at a wavelength of 1 μm at 100 ° C. As is clear from FIG. 3, the durability at 50 ° C. improves as the emissivity increases.

以上のように本実施例によれば、100℃の波長1μmで
の放射率を0.3以上とすることにより、高温時の耐久性
を向上させることができ、望ましくは0.5以上とするこ
とにより高温時の耐久性は大幅に向上する。
As described above, according to the present embodiment, by setting the emissivity at a wavelength of 1 μm at 100 ° C. to be 0.3 or more, the durability at high temperature can be improved. The durability of is greatly improved.

(実施例2) 基板として厚み50μmの芳香族ポリイミドを用い、Co−
Cr(20ωt%)をArガス雰囲気中でスパッタし、膜厚30
00ÅのCoCr垂直磁化膜を形成した。CoCr膜の形成後連続
してArとN2の混合ガス雰囲気中でスパッタし、厚み300
ÅのCoCr窒化物を形成した。ArとN2ガスの混合比率を変
化させることにより、各種の放射率の試料を作成した。
これらの試料の放射率と50℃50%Rhにおけるアモルファ
スヘッドを有する回転シリンダーによるスチル寿命の関
係を第4図に示す。第3図から明らかな様に放射率の上
昇に伴ない50℃における耐久性は向上する。
(Example 2) A 50 μm thick aromatic polyimide was used as a substrate, and Co-
Cr (20ωt%) is sputtered in Ar gas atmosphere, and the film thickness is 30
A 00Å CoCr perpendicular magnetic film was formed. After forming the CoCr film, continuously sputter it in a mixed gas atmosphere of Ar and N 2 to obtain a thickness of 300
Å CoCr nitride formed. Samples with various emissivities were prepared by changing the mixing ratio of Ar and N 2 gas.
The relationship between the emissivity of these samples and the still life of a rotating cylinder having an amorphous head at 50 ° C. and 50% Rh is shown in FIG. As is clear from FIG. 3, the durability at 50 ° C. improves as the emissivity increases.

以上のように本実施例によれば、100℃の波長1μmで
の放射率を0.3以上とすることにより、高温時の耐久性
を向上させることができ、望ましくは0.5以上とするこ
とにより、高温時の耐久性を大幅に向上することができ
る。
As described above, according to the present embodiment, the emissivity at a wavelength of 1 μm at 100 ° C. of 0.3 or more can improve the durability at high temperature, and preferably 0.5 or more, the high temperature The durability of the time can be greatly improved.

なお、本実施例では2種類の試料について具体的に効果
を示したが、本発明を構成する前述の他の材料の組み合
わせにおいても、同様の効果を有することを確認した。
又、実施例に示したとおり放熱層の形成は磁性層と別に
作ることもできるし同時に作ることもできる。さらに前
実施例では磁気記録媒体として磁気テープを例にして説
明したが、本発明の要旨を逸脱しない範囲で磁気ディス
ク,磁気シートの形態をとることもできるものである。
In this example, the specific effects were shown for two kinds of samples, but it was confirmed that the same effects were obtained even in the combination of the above-mentioned other materials constituting the present invention.
Further, as shown in the embodiment, the heat dissipation layer can be formed separately from the magnetic layer or can be formed simultaneously. Further, in the previous embodiment, a magnetic tape was described as an example of the magnetic recording medium, but it is also possible to take the form of a magnetic disk or a magnetic sheet without departing from the scope of the present invention.

発明の効果 以上のように本発明は磁性面側表面の100℃の波長1μ
mでの放射率を0.3より大きくすることにより、高温時
の耐久性を向上させた金属薄膜型磁気記録媒体を提供す
ることができ、その実用的効果は大きい。
As described above, the present invention has a wavelength of 1 μ at 100 ° C. on the magnetic surface side.
By setting the emissivity at m greater than 0.3, it is possible to provide a metal thin film type magnetic recording medium having improved durability at high temperatures, and its practical effect is great.

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

第1図は従来の金属薄膜型磁気記録媒体を示す断面図、
第2図は本発明の実施例における金属薄膜型磁気記録媒
体を示す断面図、第3図,第4図は本発明の実施例にお
ける耐久性の改善を示す図である。 3……基板、4……磁性層、5……放熱層。
FIG. 1 is a sectional view showing a conventional metal thin film magnetic recording medium,
FIG. 2 is a sectional view showing a metal thin film type magnetic recording medium in an embodiment of the present invention, and FIGS. 3 and 4 are views showing improvement of durability in the embodiment of the present invention. 3 ... Substrate, 4 ... Magnetic layer, 5 ... Heat dissipation layer.

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭52−153707(JP,A) 特開 昭56−156931(JP,A) 特開 昭54−143111(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (56) Reference JP-A 52-153707 (JP, A) JP-A 56-156931 (JP, A) JP-A 54-143111 (JP, A)

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】磁性面側表面の100℃の波長1μmでの放
射率が0.3より大きいことを特徴とする金属薄膜型磁気
記録媒体。
1. A metal thin film type magnetic recording medium having an emissivity of more than 0.3 at a wavelength of 1 μm at 100 ° C. on the magnetic side surface.
JP59195002A 1984-09-18 1984-09-18 Metal thin film magnetic recording medium Expired - Lifetime JPH07101494B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59195002A JPH07101494B2 (en) 1984-09-18 1984-09-18 Metal thin film magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59195002A JPH07101494B2 (en) 1984-09-18 1984-09-18 Metal thin film magnetic recording medium

Publications (2)

Publication Number Publication Date
JPS6173229A JPS6173229A (en) 1986-04-15
JPH07101494B2 true JPH07101494B2 (en) 1995-11-01

Family

ID=16333897

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59195002A Expired - Lifetime JPH07101494B2 (en) 1984-09-18 1984-09-18 Metal thin film magnetic recording medium

Country Status (1)

Country Link
JP (1) JPH07101494B2 (en)

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6020809B2 (en) * 1976-06-17 1985-05-23 松下電器産業株式会社 Magnetic film and its manufacturing method
JPS6049971B2 (en) * 1978-04-27 1985-11-06 松下電器産業株式会社 magnetic recording medium
JPS56156931A (en) * 1980-05-06 1981-12-03 Nec Corp Magnetic storage medium

Also Published As

Publication number Publication date
JPS6173229A (en) 1986-04-15

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