JPH0444803B2 - - Google Patents

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Publication number
JPH0444803B2
JPH0444803B2 JP33712689A JP33712689A JPH0444803B2 JP H0444803 B2 JPH0444803 B2 JP H0444803B2 JP 33712689 A JP33712689 A JP 33712689A JP 33712689 A JP33712689 A JP 33712689A JP H0444803 B2 JPH0444803 B2 JP H0444803B2
Authority
JP
Japan
Prior art keywords
magnetic
permeability
thin film
main
magnetic permeability
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
Application number
JP33712689A
Other languages
Japanese (ja)
Other versions
JPH02198010A (en
Inventor
Nobuaki Furuya
Yoshio Watanabe
Yasuhiko Nakayama
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 JP1337126A priority Critical patent/JPH02198010A/en
Publication of JPH02198010A publication Critical patent/JPH02198010A/en
Publication of JPH0444803B2 publication Critical patent/JPH0444803B2/ja
Granted 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 本発明は記録媒体に垂直方向に記録または再生
を行う磁気ヘツドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION FIELD OF INDUSTRIAL APPLICATION The present invention relates to a magnetic head that performs recording or reproduction perpendicularly to a recording medium.

従来例の構成とその問題点 高密度に磁気記録を行う方式として垂直磁化記
録方式が提案されている(たとえば特開昭52−
134706号公報、特開昭53−3209号公報参照)。こ
の方式は記録された磁化の反磁界が少く、高密度
に磁気記録できる特徴があるが、垂直異方性を有
する記録媒体を必要とすると共に垂直方向の磁界
の強い垂直磁気記録用ヘツドを必要とする。第1
図は従来提案されている垂直磁気記録用ヘツドの
一例である。垂直磁気異方性を有する磁化層1の
下層に媒体高透磁率層2を有する磁気記録媒体3
の磁化層1に近接して、高透磁率薄膜4を非磁性
体5で挟込んだ主磁極6を設け、この主磁極6の
回りにコイル7を巻き電気的入力または出力とし
て垂直磁気記録または再生を行う。本構成の従来
ヘツドは記録体はコイル7を流れる電流により形
成された磁気回路8を通る磁束におり、磁化層1
の高透磁率薄膜4に近接した部分を磁化して記録
する。また逆に再生時は、磁化層1の高透磁率薄
膜4に近接した部分の磁化による磁束が磁気回路
8を通つて流れ、コイル7を鎖交することにより
コイル7より電気信号として出力される。ここで
従来の磁気ヘツドは磁気回路8の磁気抵抗が大き
いために、記録時および再生時とも効率の悪い欠
点があつた。磁気抵抗が大きくなる原因には3つ
あり、その第1は高透磁率薄膜4が一般に厚みが
1μm程度で薄い反面数mmの長さがあるためパーマ
ロイ等の高透磁率材料で形成しても磁気抵抗が大
きくなつてしまうためである。また第2の原因は
高透磁率薄膜4から媒体高透磁率層2には透磁率
が小さい空気中を通つて磁気回路8が形成される
ため磁気抵抗が大きくなることである。さらに媒
体高透磁率層2の厚みが1μm以下で磁気回路8の
一部となる部分の長さが数mmと大きいことにより
磁気抵抗が大きくなつてしまうことが第3の原因
である。
Conventional configurations and their problems Perpendicular magnetization recording has been proposed as a method for performing high-density magnetic recording (for example,
134706, JP-A-53-3209). This method has the feature that the demagnetizing field of the recorded magnetization is small and enables high-density magnetic recording, but it requires a recording medium with perpendicular anisotropy and a perpendicular magnetic recording head with a strong perpendicular magnetic field. shall be. 1st
The figure shows an example of a conventional perpendicular magnetic recording head. A magnetic recording medium 3 having a medium high permeability layer 2 under a magnetization layer 1 having perpendicular magnetic anisotropy
A main magnetic pole 6 in which a high magnetic permeability thin film 4 is sandwiched between non-magnetic materials 5 is provided in close proximity to the magnetized layer 1, and a coil 7 is wound around the main magnetic pole 6 to provide electrical input or output for perpendicular magnetic recording or Perform playback. In the conventional head with this configuration, the recording medium is in the magnetic flux passing through the magnetic circuit 8 formed by the current flowing through the coil 7, and the magnetic layer 1
A portion close to the high magnetic permeability thin film 4 is magnetized and recorded. Conversely, during reproduction, the magnetic flux due to the magnetization of the portion of the magnetic layer 1 that is close to the high magnetic permeability thin film 4 flows through the magnetic circuit 8, interlinks the coil 7, and is output from the coil 7 as an electrical signal. . Here, in the conventional magnetic head, since the magnetic circuit 8 has a large magnetic resistance, the conventional magnetic head has a disadvantage of poor efficiency both during recording and reproduction. There are three reasons why the magnetic resistance increases. The first is that the high magnetic permeability thin film 4 is generally thick.
This is because although it is thin at about 1 μm, it is several mm long, so even if it is made of a high magnetic permeability material such as permalloy, the magnetic resistance will be large. The second reason is that the magnetic circuit 8 is formed from the high magnetic permeability thin film 4 to the medium high magnetic permeability layer 2 through air having low magnetic permeability, so that the magnetic resistance increases. Furthermore, the third cause is that the thickness of the medium high magnetic permeability layer 2 is 1 μm or less and the length of the portion that becomes a part of the magnetic circuit 8 is several mm, which increases the magnetic resistance.

以上述べたように従来の垂直磁気記録用ヘツド
は磁気抵抗が大きい欠点のため、記録または再生
の効率が悪い欠点があつた。
As mentioned above, conventional perpendicular magnetic recording heads have a drawback of high magnetic resistance, which has the drawback of poor recording or reproducing efficiency.

さらに上記従来例は外部磁界の影響を受けやす
い欠点を有している。この様子を第2図に示す。
図で第1図と同じ部分は同一番号を付けて示し
た。外部からの不用なノイズ磁界は磁気回路9を
通つてコイル7を鎖交して外部ノイズとしてコイ
ル7より電気信号ノイズとなる。これは高透磁率
薄膜4が外部ノイズ磁界のアンテナとなるためと
考えられる。
Furthermore, the conventional example described above has the disadvantage that it is susceptible to the influence of external magnetic fields. This situation is shown in FIG.
In the figure, the same parts as in FIG. 1 are indicated with the same numbers. The unnecessary noise magnetic field from the outside interlinks the coil 7 through the magnetic circuit 9 and becomes electrical signal noise from the coil 7 as external noise. This is considered to be because the high magnetic permeability thin film 4 serves as an antenna for external noise magnetic fields.

このように従来構成の磁気ヘツドでは記録・再
生効率、外部磁界の影響の点で欠点を有してい
た。
As described above, magnetic heads of conventional configurations have drawbacks in terms of recording/reproducing efficiency and the influence of external magnetic fields.

発明の目的 本発明は上記従来の欠点を解消するもので、記
録または再生効率を大幅に改善し、外部ノイズ磁
界の影響を受けやすい欠点を除いた磁気ヘツドを
提供することを目的とするものである。
OBJECT OF THE INVENTION The present invention solves the above-mentioned conventional drawbacks, and aims to provide a magnetic head that greatly improves recording or reproducing efficiency and eliminates the drawback of being susceptible to external noise magnetic fields. be.

発明の構成 本発明は上記目的を達成するもので、垂直磁気
異方性を有する磁化層の下層に高透磁率層を有す
る磁気記録媒体に近接して高透磁率磁性薄膜を設
け、前記高透磁率磁性薄膜の、前記磁化層に近接
する部が少なくとも非磁性体により挟持されてお
り、前記高透磁率磁性薄膜と磁気的に接続された
第1の高透磁率体を少なくとも有する構造の主磁
極と、前記主磁極に近接または接続して設けられ
た第2の高透磁率体と、前記磁気記録媒体を挟ん
で、前記主磁極と反対側に設けられた第3の高透
磁率体とを具備し前記第2と第3の前記高透磁率
体の対向する部分の面積をSu、前記第2と第3
の高透磁率体間の平均距離をu、前記第1と第2
の高透磁率体の対向する部分の面積をSv、前記
第1と第2の高透磁率体間の平均距離をvとした
とき、 v/Sv>u/Su となるごとく構成されたことを特徴とする磁気ヘ
ツドを提供するものである。
Structure of the Invention The present invention achieves the above object, and includes providing a high permeability magnetic thin film in close proximity to a magnetic recording medium having a high permeability layer under a magnetization layer having perpendicular magnetic anisotropy. A main magnetic pole having a structure in which a portion of a magnetic thin film close to the magnetization layer is sandwiched by at least a nonmagnetic material, and at least a first high magnetic permeability material is magnetically connected to the high permeability magnetic thin film. a second high magnetic permeability body provided close to or connected to the main magnetic pole; and a third high magnetic permeability body provided on the opposite side of the main magnetic pole with the magnetic recording medium in between. The area of the opposing portions of the second and third high magnetic permeability bodies is Su, and the area of the second and third high magnetic permeability bodies is Su,
Let the average distance between the high magnetic permeability materials be u, the first and second
When the area of the opposing parts of the high magnetic permeability bodies is Sv, and the average distance between the first and second high magnetic permeability bodies is v, it is assumed that v/Sv>u/Su. The present invention provides a magnetic head with the following characteristics.

実施例の説明 以下に本発明の実施例を図面を周いて説明す
る。
DESCRIPTION OF EMBODIMENTS Examples of the present invention will be described below with reference to the drawings.

第3図は本発明の一実施例による磁気ヘツドの
断面図を示すもので、第1図と同一部分には同一
番号を付して示した。
FIG. 3 shows a sectional view of a magnetic head according to an embodiment of the present invention, and the same parts as in FIG. 1 are designated by the same numbers.

本実施例は、磁化層1と媒体高透磁率層2より
なる磁気記録媒体3に近接して高透磁率薄膜4を
設け、その一部に接続して第1の高透磁率ブロツ
ク10を設け、上記高透磁率薄膜4の磁気記録媒
体3に近い部分を非磁性体5で挟込んだ先端部分
17を含む主磁極6を設ける。主磁極6に近接し
て第2の高透磁率ブロツク11を磁気記録媒体3
の主磁極6側に設ける。さらに磁気記録媒体3の
主磁極6の反対側に第3の高透磁率ブロツク12
を設ける。主磁極6のまわりにコイル7が巻かれ
ている。
In this embodiment, a high magnetic permeability thin film 4 is provided adjacent to a magnetic recording medium 3 consisting of a magnetic layer 1 and a medium high permeability layer 2, and a first high magnetic permeability block 10 is provided connected to a part of the thin film 4. , a main magnetic pole 6 including a tip portion 17 sandwiched between nonmagnetic materials 5 is provided at a portion of the high magnetic permeability thin film 4 near the magnetic recording medium 3 . A second high magnetic permeability block 11 is placed adjacent to the main magnetic pole 6 on the magnetic recording medium 3.
Provided on the main magnetic pole 6 side. Furthermore, a third high magnetic permeability block 12 is provided on the opposite side of the main magnetic pole 6 of the magnetic recording medium 3.
will be established. A coil 7 is wound around the main pole 6.

第4図は第3図に示した磁気ヘツドの主磁極先
端部12の拡大図である。第4図において、第2
と第3の高透磁率体11,12の対向する部分の
面積をSu、両者の平均距離をuとし、第1と第
2の高透磁率体10,11の対向する部分の面積
をSv、両者の平均距離をvとした時に、 v/Sv>u/Su となるごとく構成されている。
FIG. 4 is an enlarged view of the main pole tip 12 of the magnetic head shown in FIG. In Figure 4, the second
The area of the opposing parts of the third high magnetic permeability bodies 11 and 12 is Su, the average distance between them is u, and the area of the opposing parts of the first and second high magnetic permeability bodies 10 and 11 is Sv, When the average distance between the two is v, it is constructed so that v/Sv>u/Su.

かかる構成による本実施例の効果を述べる。第
1の高透磁率ブロツク10を高透磁率薄膜4に磁
気的に接続して設けたことにより、高透磁率薄膜
4の磁気抵抗を大幅に低下させることができる。
また第2の高透磁率ブロツク11を主磁極6に近
接または接続して磁気記録媒体3の主磁極6側に
設けたことにより、磁気回路13が形成され、磁
気回路13が空気中を通ることがなく、磁気抵抗
を大幅に減少させることができた。またさらに第
3の高透磁率ブロツク12を磁気記録媒体3の主
磁極6の反対側に設けたことにより、磁気回路1
3が媒体高透磁率層2を通る距離を短かくでき、
媒体高透磁率層2の磁気抵抗を大幅に低下させる
効果が得られた。
The effects of this embodiment with such a configuration will be described. By providing the first high magnetic permeability block 10 magnetically connected to the high magnetic permeability thin film 4, the magnetic resistance of the high magnetic permeability thin film 4 can be significantly reduced.
Furthermore, by providing the second high magnetic permeability block 11 near or connected to the main magnetic pole 6 on the main magnetic pole 6 side of the magnetic recording medium 3, a magnetic circuit 13 is formed, and the magnetic circuit 13 can pass through the air. There was no magnetic resistance, and the magnetic resistance could be significantly reduced. Furthermore, by providing the third high magnetic permeability block 12 on the opposite side of the main magnetic pole 6 of the magnetic recording medium 3, the magnetic circuit 1
3 can shorten the distance through the medium high permeability layer 2,
The effect of significantly lowering the magnetic resistance of the medium high permeability layer 2 was obtained.

さらに本実施例において外部ノイズ磁界の影響
を少なくするためには第4図中の磁気回路16の
磁気抵抗が磁気回路14の磁気抵抗より大きく外
部磁束の多くが磁気回路14を通ることが望まし
いが、このためには、第1の高透磁率ブロツク1
0と第2の高透磁率ブロツク11の間の磁気抵抗
が、第2の高透磁率ブロツク11と第3の高透磁
率ブロツク12の間の磁気抵抗より大きいことが
望ましい。
Furthermore, in this embodiment, in order to reduce the influence of external noise magnetic fields, it is desirable that the magnetic resistance of the magnetic circuit 16 in FIG. , for this purpose a first high permeability block 1
0 and the second high permeability block 11 is preferably greater than the reluctance between the second high permeability block 11 and the third high permeability block 12.

従つて第1の高透磁率ブロツク10と第2の高
透磁率ブロツク11の間の磁気抵抗を第2の高透
磁率ブロツク11と第3の高透磁率ブロツク12
の間の磁気抵抗より大きく設定すればよい。磁気
抵抗は面積に反比例し、長さに比例するので上記
の条件は次式で与えられる。
Therefore, the magnetic resistance between the first high magnetic permeability block 10 and the second high magnetic permeability block 11 is reduced by the magnetic resistance between the second high magnetic permeability block 11 and the third high magnetic permeability block 12.
It is sufficient to set the magnetic resistance to be larger than the magnetic resistance between the two. Since magnetic resistance is inversely proportional to area and proportional to length, the above condition is given by the following equation.

v/Sv>u/Su すなわち、上記の条件を満足する構成に第1、
第2、第3の高透磁率ブロツクを配置した時に、
外部ノイズの影響が少く、またヘツドの記録・再
生効率の高いものが得られる。
v/Sv>u/Su In other words, the first,
When the second and third high permeability blocks are placed,
The influence of external noise is small, and the recording/reproducing efficiency of the head is high.

第5図は本実施例の構成が外部ノイズ磁界の影
響が少いことを説明するため磁気ヘツドの断面図
である。第5図において、外部からのノイズ磁界
は磁気抵抗の少い磁気回路14に主に通過し磁気
抵抗の大きい磁気回路15,16を通る量が少い
ため全体として外部ノイズ磁界がコイル7を鎖交
する量が少くなり、外部ノイズの影響を大きく減
少する。
FIG. 5 is a sectional view of the magnetic head for explaining that the configuration of this embodiment is less affected by external noise magnetic fields. In FIG. 5, the external noise magnetic field mainly passes through the magnetic circuit 14 with low magnetic resistance, and a small amount passes through the magnetic circuits 15 and 16 with high magnetic resistance, so that the external noise magnetic field as a whole links the coil 7. This greatly reduces the influence of external noise.

なお、具体的には高透磁率薄膜4は従来よく使
用されるパーマロイの他にさらに飽和磁化が高く
透磁率も大きいCoとZuを主成分とするアモルフ
アス材料、例えばCoZrNb又はCoFeZrNbなどの
アモルフアス材料を1μm程度スパツタリングで形
成し、主磁極先端部分17の長さを100μm程度と
する。第1の高透磁率ブロツク10はフエライト
材料などで形成し、厚み100μm長さ5mm程度であ
る。第2の高透磁率ブロツク11はフエライト材
料などからなり、第1の高透磁率ブロツク10よ
り十分大きく構成し、空間の磁気抵抗を減少させ
る。媒体裏面の第3の高透磁率ブロツク12も第
2の高透磁率ブロツク11と対向する面を大きく
とつて磁気抵抗を減少させ、フエライト材料など
を使用する。
Specifically, the high magnetic permeability thin film 4 is made of an amorphous material whose main components are Co and Zu, which have higher saturation magnetization and higher magnetic permeability, such as CoZrNb or CoFeZrNb, in addition to permalloy, which is commonly used in the past. It is formed by sputtering to about 1 μm, and the length of the main pole tip portion 17 is about 100 μm. The first high magnetic permeability block 10 is made of ferrite material and has a thickness of about 100 μm and a length of about 5 mm. The second high magnetic permeability block 11 is made of ferrite material or the like, and is configured to be sufficiently larger than the first high magnetic permeability block 10 to reduce the magnetic resistance of the space. The third high magnetic permeability block 12 on the rear surface of the medium also has a large surface facing the second high magnetic permeability block 11 to reduce magnetic resistance, and is made of ferrite material or the like.

発明の効果 以上要するに本発明は垂直磁気異方性を有する
磁化層の下層に高透磁率層を有する磁気記録媒体
に近接して高透磁率磁性薄膜を設け、前記高透磁
率磁性薄膜の、前記磁化層に近接する部が少なく
とも非磁性体により挟持されており、前記高透磁
率磁性薄膜と磁気的に接続された第1の高透磁率
体を少なくとも有する構造の主磁極と、前記主磁
極に近接または接続して設けられた第2の高透磁
率体と、前記磁気記録媒体を挟んで、前記主磁極
と反対側に設けられた第3の高透磁率体とを具備
し前記第2と第3の前記高透磁率体の対向する部
分の面積をSu、前記第2と第3の高透磁率体間
の平均距離をu、前記第1と第2の高透磁率体の
対向する部分の面積をSv、前記第1と第2の高
透磁率体間の平均距離をvとしたとき、 v/Sv>u/Su となるごとく構成されたことを特徴とする磁気ヘ
ツドの磁気回路の抵抗を低下させ、記録または再
生の効率を高くすると共に、外部ノイズ磁界の影
響を低下させる利点を有する。
Effects of the Invention In summary, the present invention provides a high permeability magnetic thin film in close proximity to a magnetic recording medium having a high permeability layer under a magnetic layer having perpendicular magnetic anisotropy, and a main magnetic pole having a structure in which a portion adjacent to the magnetization layer is sandwiched by at least a non-magnetic material and has at least a first high magnetic permeability material magnetically connected to the high magnetic permeability magnetic thin film; A second high magnetic permeability body provided adjacent to or connected to the second high magnetic permeability body, and a third high magnetic permeability body provided on the opposite side of the main magnetic pole with the magnetic recording medium in between. The area of the opposing portion of the third high magnetic permeability body is Su, the average distance between the second and third high magnetic permeability body is u, and the opposing portion of the first and second high magnetic permeability body A magnetic circuit of a magnetic head characterized in that it is configured such that v/Sv>u/Su, where Sv is the area of the magnetic head and v is the average distance between the first and second high magnetic permeability bodies It has the advantage of lowering resistance, increasing recording or reproducing efficiency, and reducing the influence of external noise magnetic fields.

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

第1図は従来の垂直磁気ヘツドの断面図、第2
図は外部ノイズ磁界の影響を示す従来の垂直磁気
ヘツドの断面図、第3図は本発明の一実施例によ
る磁気ヘツドの断面図、第4図は本発明の磁気ヘ
ツドの主磁極先端部の拡大図、第5図は本発明の
磁気ヘツドの外部磁界の影響を示す磁気ヘツド断
面図である。 1……磁化層、2……媒体高透磁率層、3……
磁気記録媒体、4……高透磁率薄膜、5……非磁
性体、6……主磁極、7……コイル、8,9,1
3,14,15,16……磁気回路、10……第
1の高透磁率ブロツク、11……第2の高透磁率
ブロツク、12……第3の高透磁率ブロツク、1
7……主磁極先端部分。
Figure 1 is a sectional view of a conventional perpendicular magnetic head;
FIG. 3 is a sectional view of a conventional perpendicular magnetic head showing the influence of an external noise magnetic field. FIG. 3 is a sectional view of a magnetic head according to an embodiment of the present invention. FIG. The enlarged view, FIG. 5, is a sectional view of the magnetic head showing the influence of an external magnetic field on the magnetic head of the present invention. 1...Magnetization layer, 2...Medium high permeability layer, 3...
Magnetic recording medium, 4... High magnetic permeability thin film, 5... Nonmagnetic material, 6... Main magnetic pole, 7... Coil, 8, 9, 1
3, 14, 15, 16...Magnetic circuit, 10...First high magnetic permeability block, 11...Second high magnetic permeability block, 12...Third high magnetic permeability block, 1
7... Main magnetic pole tip.

Claims (1)

【特許請求の範囲】 1 垂直磁気異方性を有する磁化層の下層に高透
磁率層を有する磁気記録媒体に近接して高透磁率
磁性薄膜を設け、前記高透磁率磁性薄膜の、前記
磁化層に近接する部が少なくとも非磁性体により
挟持されており、前記高透磁率磁性薄膜と磁気的
に接続された第1の高透磁率体を少なくとも有す
る構造の主磁極と、前記主磁極に近接して設けら
れた第2の高透磁率体と、前記磁気記録媒体を挟
んで、前記主磁極と反対側に設けられた第3の高
透磁率体とを具備し、前記第2と第3の前記高透
磁率体の対向する部分の面積をSu、前記第2と
第3の高透磁率体間の平均距離をu、前記第1と
第2の高透磁率体の対向する部分の面積をSv、
前記第1と第2の高透磁率体間の平均距離をvと
したとき、 v/Sv>u/Su となるごとく構成されたことを特徴とする磁気ヘ
ツド。 2 高透磁率磁性薄膜が、Co,Zrを主成分とす
るアモルフアス材料よりなることを特徴とする特
許請求の範囲第1項記載の磁気ヘツド。 3 高透磁率磁性薄膜が、Co,Fe,Zr,Nbを含
むアモルフアス材料よりなることを特徴とする特
許請求の範囲第1項記載の磁気ヘツド。
[Scope of Claims] 1. A high permeability magnetic thin film is provided adjacent to a magnetic recording medium having a high magnetic permeability layer under a magnetization layer having perpendicular magnetic anisotropy, and the magnetization of the high permeability magnetic thin film is a main magnetic pole having a structure in which a portion adjacent to the layer is sandwiched by at least a non-magnetic material and has at least a first high magnetic permeability material magnetically connected to the high magnetic permeability magnetic thin film; and a main magnetic pole adjacent to the main magnetic pole. and a third high magnetic permeability body provided on the opposite side of the main magnetic pole with the magnetic recording medium in between, The area of the opposing portions of the high magnetic permeability bodies is Su, the average distance between the second and third high magnetic permeability bodies is u, and the area of the opposing portions of the first and second high magnetic permeability bodies is Sv,
A magnetic head characterized in that, where v is the average distance between the first and second high magnetic permeability bodies, v/Sv>u/Su. 2. The magnetic head according to claim 1, wherein the high permeability magnetic thin film is made of an amorphous material containing Co and Zr as main components. 3. The magnetic head according to claim 1, wherein the high permeability magnetic thin film is made of an amorphous material containing Co, Fe, Zr, and Nb.
JP1337126A 1989-12-26 1989-12-26 Magnetic head Granted JPH02198010A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1337126A JPH02198010A (en) 1989-12-26 1989-12-26 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1337126A JPH02198010A (en) 1989-12-26 1989-12-26 Magnetic head

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP58161308A Division JPS6052907A (en) 1983-09-01 1983-09-01 Magnetic head

Publications (2)

Publication Number Publication Date
JPH02198010A JPH02198010A (en) 1990-08-06
JPH0444803B2 true JPH0444803B2 (en) 1992-07-22

Family

ID=18305688

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1337126A Granted JPH02198010A (en) 1989-12-26 1989-12-26 Magnetic head

Country Status (1)

Country Link
JP (1) JPH02198010A (en)

Also Published As

Publication number Publication date
JPH02198010A (en) 1990-08-06

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