JPS5870421A - Magnetic recording medium - Google Patents

Magnetic recording medium

Info

Publication number
JPS5870421A
JPS5870421A JP56167514A JP16751481A JPS5870421A JP S5870421 A JPS5870421 A JP S5870421A JP 56167514 A JP56167514 A JP 56167514A JP 16751481 A JP16751481 A JP 16751481A JP S5870421 A JPS5870421 A JP S5870421A
Authority
JP
Japan
Prior art keywords
layer
magnetic
tape
magnetic recording
electrical resistance
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.)
Granted
Application number
JP56167514A
Other languages
Japanese (ja)
Other versions
JPH0321966B2 (en
Inventor
Toshiaki Izumi
泉 俊明
Fumio Maruta
丸田 文生
Takanori Kobuke
古武家 隆敬
Kiyoshi Noguchi
潔 野口
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.)
TDK Corp
Original Assignee
TDK Corp
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 TDK Corp filed Critical TDK Corp
Priority to JP56167514A priority Critical patent/JPS5870421A/en
Publication of JPS5870421A publication Critical patent/JPS5870421A/en
Publication of JPH0321966B2 publication Critical patent/JPH0321966B2/ja
Granted 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
    • G11B5/62Record carriers characterised by the selection of the material
    • G11B5/64Record carriers characterised by the selection of the material comprising only the magnetic material without bonding agent
    • G11B5/66Record carriers characterised by the selection of the material comprising only the magnetic material without bonding agent the record carriers consisting of several layers
    • G11B5/672Record carriers characterised by the selection of the material comprising only the magnetic material without bonding agent the record carriers consisting of several layers having different compositions in a plurality of magnetic layers, e.g. layer compositions having differing elemental components or differing proportions of elements

Landscapes

  • Compositions Of Macromolecular Compounds (AREA)
  • Magnetic Record Carriers (AREA)

Abstract

PURPOSE:To increase the surface electric resistance and to control the noise by covering the uppermost layer of a magnetic thin multilayer film with an oxidized magnetic layer. CONSTITUTION:A vapor-deposited Al layer or the like as an intermediate layer is laid on a base film of polyethylene terephthalate or the like. On the intermediate layer a vapor-deposited layer such as a magnetic thin Co.Ni alloy film is laid, and by repeating the stage, a vapor-deposited multilayer film is formed. A magnetic thin film of an oxidized alloy such as Co.Ni oxide is finally laid as the uppermost layer.

Description

【発明の詳細な説明】 この発明は、高密度、高分解能の磁気記録媒体に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a high-density, high-resolution magnetic recording medium.

近年、磁気記録技術の進展に伴ない、高密度、IWi分
解能のものが望まれており、小型VTRやカメラ一体型
VTR1さらにPCM対応録音機などが提案されるにつ
れて、それらに用いるための新しい媒体が必要になって
きている。
In recent years, as magnetic recording technology has progressed, high density and IWi resolution have been desired, and as compact VTRs, camera-integrated VTRs, and PCM compatible recorders have been proposed, new media for use in these devices have been proposed. is becoming necessary.

こうした状況下にあって、真空技術を用いたrlVl型
膜磁気記録媒体が注目されている。中でも蒸青、イオン
シレーティング、スパッタリングなどによって非磁性の
基体上に直接強磁性層を形成して磁気記録媒体とする方
法についてに1広く実用化のための研究が進んでいる。
Under these circumstances, rlVl type film magnetic recording media using vacuum technology are attracting attention. Among these methods, research is being widely conducted on methods for forming magnetic recording media by directly forming a ferromagnetic layer on a non-magnetic substrate by blue vaporization, ion silating, sputtering, etc. for practical use.

しかるに上記蒸着テープ全オーディオテープ用として設
計する際に考慮すべき特性には抽々あるが、中でも表向
電気抵抗は重要な項目である。元来塗布タイプの磁気テ
ープは主に酸化鉄と高分子バインダーからイji4性層
が形成されているため、電気抵抗は109Ω以−ヒの高
い値になっていた。このために電気抵抗値が問題となる
のは、走行によって各所に生じる帯電がテープから逃げ
にくく、いわゆる放電ノイズとして音声信号に市なり、
耳ざわりであることが主であった。この点を解決するた
めに磁性塗料に導電性材料を混合したり、逆(/C>η
市、性の薄膜ケペース裏面に設けるなどしてテープ全体
としての電気抵抗を下げる技術が実用化さ扛てい乙。
However, there are many characteristics that should be taken into consideration when designing the vapor-deposited tape for use with all audio tapes, among which surface electrical resistance is an important item. Originally, coating type magnetic tape had an electrical resistance of 10@9 ohms or higher, since the negative layer was formed mainly from iron oxide and a polymeric binder. For this reason, the electrical resistance value becomes a problem because the electrical charge generated in various places during running is difficult to escape from the tape, and it is reflected in the audio signal as so-called discharge noise.
The main thing was that it was audible. To solve this problem, it is possible to mix conductive materials into magnetic paints, or to reverse (/C>η
A technology has been put into practical use that lowers the electrical resistance of the tape as a whole by installing a thin film on the back of the tape.

しかしながら、蒸着テープなどの場合、磁性層は金属あ
るいは合金から構成され、高分子バインダーなどを含ま
ないので、電気抵抗が極端に低くなり、このためヘッド
周囲のシール性の悪いデツキなどでは録音時に問題を生
じろことがある。すなわち、電気抵抗が(夕めて低いテ
ープいわゆる5ヘツドタイプと称されるデツキで何片し
た場合、消去ヘッド、録音ヘッド、再生ヘッド間の回路
が、録音ヘッドで発生するバイアス磁界セ、消去ヘッド
からの消去磁界に誘起されて、再生ヘッドにノイズ金ひ
き起すことが判っている。
However, in the case of vapor-deposited tapes, etc., the magnetic layer is made of metal or alloy and does not contain a polymer binder, so the electrical resistance is extremely low, which causes problems during recording when using decks with poor sealing around the head. may occur. In other words, when a number of pieces of a so-called 5-head type tape deck with low electrical resistance are made, the circuit between the erasing head, recording head, and playback head is affected by the bias magnetic field generated by the recording head, and the erasing head. It has been found that noise is induced in the read head by the erase magnetic field from the magnetic field.

この、【うな現象は、例えば竹開昭56−47924に
も開示されているところである。そこで、上述したよう
な問題は、デ゛ンキを製造する際に自己113すn、#
Iはとんど回読することが可能であると思われるが、l
+11気デ−プの製造上からも酸化が望まれているとこ
ろである。さらに」二d己ノイズの多くは(lf4気テ
ープ!〈而の屯気抵抗金市めることによって低減できる
もので4;〕す、その一つの亀イ決法として前出の烏−
開昭56−47924に開示された如く、連kA一体で
ある助ル:)磁性層にクラックを設けて部分的に不連続
部分である絶縁層をつくることが1ノを案されており、
ある程度有効であるとしても尚膜磁性層にクラックを連
続的に再現性よく形成する技術は棒めて困難である。
This phenomenon is also disclosed in Takekai 56-47924, for example. Therefore, the above-mentioned problems arise when manufacturing a deck.
It seems possible to read I many times, but l
Oxidation is also desired from the viewpoint of manufacturing +11 air tape. Furthermore, much of the noise can be reduced by using LF4K tape!
As disclosed in Japanese Patent Publication No. 56-47924, it has been proposed to provide cracks in the magnetic layer to create an insulating layer that is partially discontinuous.
Even if this technique is effective to some extent, it is extremely difficult to develop a technique for continuously forming cracks in the magnetic layer with good reproducibility.

この発明は、上1本1−だ事情に鑑みてなされたもので
あり、多層に形成された磁性層の磁気ヘッド側の最上層
を酸化された磁性層で欅うことにより、磁気テープ表面
の電気抵抗を制御できることを見出したもので、中間層
を含み、5層もしくはそれ以上の強4B1性層からプ、
cる薄膜(磁気記録媒体にあって、最上層がその強磁性
体の酸化物からなるものは表面電気抵抗が高くすること
ができ、ノイズが改ψ〒さ扛ると共に電磁変換7時性も
すぐれた磁気記録媒体となるものである。
This invention was made in view of the above situation, and by covering the top layer on the magnetic head side of a multi-layered magnetic layer with an oxidized magnetic layer, the surface of the magnetic tape can be improved. It was discovered that the electrical resistance can be controlled, and it is made of five or more strong 4B1 layers including an intermediate layer.
A thin film (a magnetic recording medium whose top layer is made of an oxide of the ferromagnetic material) can have a high surface electrical resistance, which reduces noise and improves electromagnetic conversion characteristics. This makes an excellent magnetic recording medium.

以F1この発明による実施例を添付した図面にもとづい
て詳細に説明する。
Hereinafter, embodiments of the present invention will be described in detail with reference to the accompanying drawings.

〈実施例〉 15μm厚さのポリエチレンテレフタレートのベースフ
ィルムを用意し、その−にに真空蒸着法によってアルミ
ニウムの中間層のあるコバルト・ニツノ1ル合金の強J
i?、4性層を形成1〜だ。
<Example> A base film of polyethylene terephthalate with a thickness of 15 μm was prepared, and a strong J of cobalt-nitrate alloy with an intermediate layer of aluminum was prepared on the base film by vacuum evaporation method.
i? , forming 4 sexual layers 1~.

蒸Ajの際の圧力は5 ×il]−5pa (約2 X
 1O−5Torr)、制6111温度は冷却ギーヤン
を用いて0℃とし、蒸a IIψ厚はアルミニウム中間
層の場合、250χ、コバルト・ニッケル合金層は1o
ooXとした。
The pressure during steaming Aj is 5 ×il]-5pa (approximately 2
1O-5 Torr), the control temperature was set to 0℃ using a cooling Guyan, the vapor aIIψ thickness was 250χ for the aluminum intermediate layer, and 1o for the cobalt-nickel alloy layer.
It was set as ooX.

いわゆるが[め7A A法によってデージ長さ方向の保
磁力金約61]00el/こなるように開側1した。
The so-called open side 1 was made by the A method so that the coercive force in the longitudinal direction of the dage was approximately 61]00 el/g.

以」−の条件で非磁性の中間層を含みながら多層の蒸沼
膜全形成した。このときの層数と感度の関係は第1図に
示すようになつ九図において層数は強イ心性層の叔、I
(&度は幅’、、8mmに切断したカセットテープのル
にし、4.75%で335Hzの相対出力を示した。こ
7しによると層数が1ないし2の場合は、このテープは
あまり良い感度を示さないが、これに対して5層以上の
磁性I−からなるテープはそれよりすぐれた感度を示す
ことが明らかになった。
A multilayer steamed film including a nonmagnetic intermediate layer was entirely formed under the following conditions. The relationship between the number of layers and the sensitivity in this case is as shown in Figure 1. In Figure 1, the number of layers is
(The width of a cassette tape cut to 8 mm was found to have a relative output of 335 Hz at 4.75%.According to this paper, when the number of layers is 1 or 2, this tape does not have much power. However, it has been found that tapes consisting of five or more layers of magnetic I- exhibit better sensitivity.

つき゛に一トロ己のサンプルを・つくる際に、最」二層
をコバルト・ニッケルの酸化物層とし、酸素分圧はいく
つかの11Eカとして酸化の度合いの異なるサンプルを
得た。たたし、この時保磁力は合金の場合と同様に概ね
6oooeになるように斜方蒸着の際の入射角を調整し
た。上述したようにして得られたサンプルの最上層形成
時の酸素分圧とテープ表面の電気抵抗は第2図に示した
ようになった。
When making my own samples, I made the second most layer a cobalt-nickel oxide layer and set the oxygen partial pressure at several levels of 11E to obtain samples with different degrees of oxidation. However, at this time, the incident angle during oblique deposition was adjusted so that the coercive force was approximately 6 oooo as in the case of the alloy. The oxygen partial pressure and electrical resistance of the tape surface at the time of forming the uppermost layer of the sample obtained as described above were as shown in FIG.

ここで電気抵抗とはテープを幅5.8市、長さ20Cr
rLにしてその両端で測定した電気抵抗をいう。
Here, the electrical resistance means that the tape has a width of 5.8 cm and a length of 20 Cr.
It refers to the electrical resistance measured at both ends of rL.

このとき感度は第1図の各点に対して1〜2dB低くな
った。これは酸素を磁性層の中にとりこんだために磁束
密度が減、少したことによる。なお、得られたサンプル
について酸化の度合いとノイズの関係を調べると、上述
のように表面電気抵抗が低く、導電、性のあるテープは
5ヘツドクイフ0のデツキで、ヘッドのシールを悪くし
たものは、録音同時再生時に、再生信号に含1れるノイ
ズが単に書生した場合に比べて太きくなるのだが、酸化
シ吻の最上層を形成することによってこの綴和かなされ
るものである。すなわち両ノイズレベルの差をテープ表
向の電気抵抗との関係で示せば第5図のようになる。
At this time, the sensitivity was 1 to 2 dB lower than each point in FIG. This is because the magnetic flux density is reduced due to the introduction of oxygen into the magnetic layer. In addition, when examining the relationship between the degree of oxidation and noise for the obtained samples, as mentioned above, the tape with low surface electrical resistance, conductivity, and properties has a 5-head quif of 0, while the tape with poor head sealing has When recording and playing back at the same time, the noise contained in the playback signal becomes louder than when it is simply written, but this is compensated for by forming the top layer of oxidized proboscis. That is, if the difference between the two noise levels is shown in relation to the electrical resistance on the surface of the tape, the result will be as shown in FIG.

ここでノイズレベルは555H1のノイズ成分である。Here, the noise level is the noise component of 555H1.

−J: gb i、lT 5図によると、200Ωを越
える衣ini 71を気也抗のテープはノイズレベル差
は1dB以Fとなり、実用上に問題はない。このとき、
感1止は数100のサンプルに比べて1d”4M度低く
なったにとど1つだので、テープのSN比はノイズレベ
ル差がなくなった分たけ改善さ7したことになり、実用
上間)1り↓のない範囲となった。
-J: gb i, lT According to Figure 5, the noise level difference of the tape with a resistance of more than 200 Ω is 1 dB or more, and there is no problem in practical use. At this time,
Since the 1st stop was only 1d"4M degrees lower than the hundreds of samples, the S/N ratio of the tape was improved by the amount that the noise level difference disappeared, and in practical terms it was ) is in a range with no 1 or ↓.

なお、ノイズレベル差のこの1す1向はオーディオ周波
数領域、のどこでも凹しであった。捷だ磁性層が4層以
上の揚台でも、200Ω以上のtjL杭になるとこの発
明の実施例と同様にノイズレベルi1.宝は2dB以下
となる。
Note that this difference in noise level was concave everywhere in the audio frequency region. Even if the platform has four or more twisted magnetic layers, if the tjL pile is 200Ω or more, the noise level i1. Treasure is less than 2dB.

以上詳ホ111 VC説明したように、この発明(でよ
る磁気記録((lj、体il−[、族A4テープを実用
化する上で不【扛、dr? ’jcノイズの1・1層題
をIW決したものであり、T業的効果Q、1顧岩であ6
゜ なJ、−1実施1夕11に示した磁1住尼・、中間層の
形成において、その力tkがこの発明による主旨を逸脱
しない範囲で変更することは可能であり、イオンブレー
ティングやスパッタリングなども用い得るものである。
As explained above in detail, this invention (magnetic recording ((lj, body il- The IW decision was made, and the T business effect Q, 1 Guiwa 6
In the formation of the intermediate layer shown in Example 1 and 11, the force tk can be changed without departing from the gist of the present invention, and it is possible to use ion brating or other methods. Sputtering or the like can also be used.

特に酸素雰囲気と電気抵抗との関係については、その他
の条件、例えば蒸発速度、基体の移動速度などが影響を
与えるので、この発明の有効な範囲を限定するものでは
ない。
In particular, the relationship between the oxygen atmosphere and the electrical resistance is influenced by other conditions, such as the evaporation rate and the movement rate of the substrate, so this does not limit the effective scope of the present invention.

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

第1図はこの発明の実施例で得られた磁気テープの磁性
層数と感度の関係図、第2図は6層目を形成する際の真
空槽内の酸化分圧とできあがったテープ表面の′電気抵
抗との関係図、第5図171:5層の磁性層で最上層が
酸化物層である場合の表面電気抵抗とノイズレベル差の
関係図である。 ’l−!fjFF出願人 東京電気化学工業株式会社代
理人 弁理士 佐 藤 英 昭 智ポ嘱壜8 ミ   粒  記 ′ くし愕児
Figure 1 shows the relationship between the number of magnetic layers and the sensitivity of the magnetic tape obtained in the example of the present invention, and Figure 2 shows the relationship between the oxidation partial pressure in the vacuum chamber when forming the sixth layer and the surface of the finished tape. 'Relationship Diagram with Electrical Resistance, Figure 5 171: A diagram showing the relationship between surface electrical resistance and noise level difference when the top layer is an oxide layer in a five-layer magnetic layer. 'l-! fjFF Applicant Tokyo Denki Kagaku Kogyo Co., Ltd. Agent Patent Attorney Hide Sato

Claims (2)

【特許請求の範囲】[Claims] (1)  真空中で非磁性基体上に中間層を含み、強磁
性層を6層以上設けてなる磁気記録媒体において、上記
複数の強磁性層のうち最上層が強磁性体の酸化物からな
ることを特徴とする磁気記録媒体。
(1) In a magnetic recording medium comprising an intermediate layer and six or more ferromagnetic layers on a non-magnetic substrate in vacuum, the uppermost layer of the plurality of ferromagnetic layers is made of a ferromagnetic oxide. A magnetic recording medium characterized by:
(2)上6白岐気記録媒体において、幅5.8mm、長
さ20cmの両端で測定した電気抵抗が200Ω以上で
あることを特徴とする特許請求の範囲第(1)項記載の
磁気記録媒体。
(2) The magnetic recording medium according to claim (1), wherein the electrical resistance measured at both ends of a width of 5.8 mm and a length of 20 cm is 200Ω or more. Medium.
JP56167514A 1981-10-20 1981-10-20 Magnetic recording medium Granted JPS5870421A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56167514A JPS5870421A (en) 1981-10-20 1981-10-20 Magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56167514A JPS5870421A (en) 1981-10-20 1981-10-20 Magnetic recording medium

Publications (2)

Publication Number Publication Date
JPS5870421A true JPS5870421A (en) 1983-04-26
JPH0321966B2 JPH0321966B2 (en) 1991-03-25

Family

ID=15851090

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56167514A Granted JPS5870421A (en) 1981-10-20 1981-10-20 Magnetic recording medium

Country Status (1)

Country Link
JP (1) JPS5870421A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6056915U (en) * 1983-09-28 1985-04-20 大日本印刷株式会社 magnetic recording medium
JPS6056916U (en) * 1983-09-28 1985-04-20 大日本印刷株式会社 magnetic recording medium
JP2002367135A (en) * 2001-06-06 2002-12-20 Matsushita Electric Ind Co Ltd Magnetic recording medium and manufacturing method therefor

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5720920A (en) * 1980-07-14 1982-02-03 Sekisui Chem Co Ltd Magnetic recording medium and its manufacture

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5720920A (en) * 1980-07-14 1982-02-03 Sekisui Chem Co Ltd Magnetic recording medium and its manufacture

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6056915U (en) * 1983-09-28 1985-04-20 大日本印刷株式会社 magnetic recording medium
JPS6056916U (en) * 1983-09-28 1985-04-20 大日本印刷株式会社 magnetic recording medium
JP2002367135A (en) * 2001-06-06 2002-12-20 Matsushita Electric Ind Co Ltd Magnetic recording medium and manufacturing method therefor

Also Published As

Publication number Publication date
JPH0321966B2 (en) 1991-03-25

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