JPS6052907A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPS6052907A
JPS6052907A JP16130883A JP16130883A JPS6052907A JP S6052907 A JPS6052907 A JP S6052907A JP 16130883 A JP16130883 A JP 16130883A JP 16130883 A JP16130883 A JP 16130883A JP S6052907 A JPS6052907 A JP S6052907A
Authority
JP
Japan
Prior art keywords
magnetic
permeability
magnetic permeability
high magnetic
pole
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
JP16130883A
Other languages
Japanese (ja)
Other versions
JPH0320803B2 (en
Inventor
Nobuaki Furuya
古谷 伸昭
Yasuhiko Nakayama
中山 靖彦
Yoshio Watanabe
由雄 渡辺
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 JP16130883A priority Critical patent/JPS6052907A/en
Priority to US06/640,595 priority patent/US4672494A/en
Publication of JPS6052907A publication Critical patent/JPS6052907A/en
Publication of JPH0320803B2 publication Critical patent/JPH0320803B2/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
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/1278Structure or manufacture of heads, e.g. inductive specially adapted for magnetisations perpendicular to the surface of the record carrier
    • 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
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/187Structure or manufacture of the surface of the head in physical contact with, or immediately adjacent to the recording medium; Pole pieces; Gap features

Landscapes

  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Magnetic Heads (AREA)

Abstract

PURPOSE:To improve the efficiency of reproduction and at the same time to prevent an external noise magnetic field by providing a thin film of high permeability formed as prescribed at a place near a magnetized layer of a recording medium, a block of high permeability, a main magnetic pole made of a nonmagnetic substance, a substance of high permeability set close to the main magnetic pole and another substance of high permeability set at the opposite side to the main magnetic pole. CONSTITUTION:A thin film 4 of high permeability is formed close to a magnetic recording medium 3 consisting of a magnetized layer 1 and a layer 2 of high permeability, and a block 10 of high permeability is formed following to a part of the film 4. A main magnetic pole 6 contains a tip part 17 where the film 4 is anclosed by a nonmagnetic substance 5 at the area close to the medium 3. A block 10 of high permeability is provided close to the pole 6, and a block 12 of high permeability is provided at the opposite side to the pole 6. A coil 7 is wound around the pole 6. Both blocks 10 and 11 are set close to the pole 6. In this way, the magnetic resistance of the film 4 is reduced, thus improving the efficiency of reproduction and reducing the effect of external noises.

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
気ヘッドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a magnetic head that performs recording or reproduction in a direction perpendicular 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62−134706号
公報、特開昭63−3209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ッド
を必要とする。第1図は従来提案されている垂直磁気記
録用ヘッドの一例である。垂直磁気異方f1ミを有する
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
6で挾込んだ主磁極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。
Conventional Structures and Problems The perpendicular magnetization recording method has been proposed as a method for performing high-density magnetic recording (see, for example, Japanese Patent Laid-Open No. 62-134706 and Japanese Patent Laid-Open No. 63-3209). This method has the feature that the demagnetizing field of recorded magnetization is small and allows high-density magnetic recording, but it requires a recording medium with perpendicular anisotropy and a perpendicular magnetic recording head with a strong magnetic field in the perpendicular direction. shall be. FIG. 1 shows an example of a conventionally proposed perpendicular magnetic recording head. A magnetic recording medium 3 has a medium high permeability layer 2 under the magnetic layer 1 having a perpendicular magnetic anisotropy f1. A magnetic pole 6 is provided, and a coil 7 is wound around the main magnetic pole 6 to perform perpendicular magnetic recording or reproduction as electrical input or output.

木構成の従来ヘッ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を通る磁束により、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。
In the conventional head having a tree structure, the recording medium is formed by magnetic flux passing through a magnetic circuit 8 formed by a current flowing through a coil 7, and the magnetic layer 1 is
A portion close to the high magnetic permeability thin film 4 is magnetized and recorded.

また逆に再生時は、磁化層1の高透磁率薄膜4Vc近接
した部分の磁化による磁束が磁気回路8を通って流れ、
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ッドは磁気回路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
率の悪い欠点があった。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1
/1m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っ
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っ
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nと大きいこ
とにより磁気抵抗が大きくなってしまうことが第3の原
因である。
Conversely, during reproduction, the magnetic flux due to the magnetization of the portion of the magnetic layer 1 adjacent to the high permeability thin film 4Vc flows through the magnetic circuit 8,
By interlinking the coil 7, the coil 7 outputs an electric signal. Here, the conventional magnetic head has a magnetic circuit 8
Because of its high magnetic resistance, it had the 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 1.
This is because although it is thin at about 1 m, 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 cause is the high magnetic permeability thin film 4.
Since the magnetic circuit 8 is formed in the medium high magnetic permeability layer 2 through air having a low magnetic permeability, the magnetic resistance becomes large. 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 as large as several n, which increases the magnetic resistance.

以上述べたように従来の垂直磁気記録用ヘッドは磁気抵
抗が大きい欠点のため、記録または再生の効率が悪い欠
点があった。
As described above, the conventional perpendicular magnetic recording head has a drawback of high magnetic resistance, resulting in 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。
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. 2, in which the same parts as in FIG. 1 are designated by the same numbers.

外部からの不用なノイズ磁界は磁気回路9を通ってコイ
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。
The unnecessary noise magnetic field from the outside passes through the magnetic circuit 9, interlinks the coil 7, 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ッドでは記録・再生効率、
外部磁界の影響の点で欠点を有していた。
In this way, magnetic heads with conventional configurations have low recording and reproducing efficiency.
It had a drawback in terms of the influence of external magnetic fields.

発明の目的 本発明は上記従来の欠点全解消するもので、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ッドを提供することを目的と
するものである。
OBJECTS OF THE INVENTION The present invention eliminates all of 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ケ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
により挾持されており、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挾んで、前
記主磁極と反対側に設けられた第3の高透磁率体と全具
備したこと全特徴とする磁気ヘッド全提供するものであ
る。
Structure of the Invention The present invention achieves the above object by 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 non-magnetic material, and has at least a first high magnetic permeability material 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. It provides a magnetic head with all the features.

実施例の説明 以下に本発明の実施例を図面を用いて説明する。Description of examples Embodiments 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ッドの断面図を
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の高透磁率ブロック1o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6
で挾込んだ先端部分17を含む主磁極6を設ける。主磁
極6に近接して第2の高透磁率ブロック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の高透磁率ブロック12を設け
る。主磁極6のまわりにはコイル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 magnetization layer 1 and a medium high magnetic permeability layer 2, and a first high magnetic permeability block 1o is provided connected to a part of the thin film 4. , a portion of the high magnetic permeability thin film 4 near the magnetic recording medium 3 is covered with a non-magnetic material 6.
A main magnetic pole 6 including a tip portion 17 sandwiched between the main poles 6 and 6 is provided. A second high magnetic permeability block 11 is provided close to the main magnetic pole 6 on the main magnetic pole 6 side of the magnetic recording medium 3 . Further, 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. A coil 7 is wound around the main pole 6.

かかる構成による本実施例の効果を述べる。第1の高透
磁率ブロック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。
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.

捷た第2の高透磁率ブロック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の高透磁率ブロック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13が媒体高透磁率層2を通る短目11ヲ短かく
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。
By providing the twisted second high magnetic permeability block 11 close to 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 passes through the air. We were able to significantly reduce magnetic resistance without any problems. 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 short distance 11 of the magnetic circuit 13 passing through the medium high magnetic permeability layer 2 can be shortened, and the medium height can be reduced. The effect of significantly reducing the magnetic resistance of the magnetic permeability layer 2 was obtained.

なお、第2の高透磁率ブロック11は主磁極6の少くも
片側(Cあれば良く、非磁性体6は磁気記録媒体3に近
接した、高透率薄膜4の先端部分を少と挾込む構造であ
れば良い。
The second high magnetic permeability block 11 is formed on at least one side of the main magnetic pole 6 (C is sufficient, and the non-magnetic material 6 is sandwiched between the tip portion of the high permeability thin film 4 near the magnetic recording medium 3). Any structure is fine.

以上述べた、3ケ所の磁気抵抗を減少式せる組合せの構
成により全体の磁気抵抗を大幅に減少させることが可能
となり、ヘッドの効率が記録再生とも大きく改善される
。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Zn(i7主成分とするアモルファス材料、例えばC
oZrNb 又はCoFeZrNbなどのアモルファス
材料f1ttm秤度スバノクリ/グで形成し、主磁極先
端部分17の長さ’(5100μm程度とする。第1の
高透磁率ブロック10はフェライト材料などで形成し、
厚み100μm長さ6闘程度である。第2の高透磁率ブ
ロック11はフェライト材料などからなり、第1の高透
磁率ブロック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の高透磁率ブロック1
2も第2の高透磁率ブロック11と対向する面を大きく
とって磁気抵抗全減少させ、フェライト材料などを使用
する。
The above-described combination of structures for reducing the magnetic resistance at three locations makes it possible to significantly reduce the overall magnetic resistance, and the efficiency of the head is greatly improved in both recording and reproduction. Specifically, the high magnetic permeability thin film 4 is made of CO, which has higher saturation magnetization and higher magnetic permeability than permalloy, which is commonly used conventionally.
and Zn (amorphous material whose main component is i7, e.g. C
The first high magnetic permeability block 10 is formed of an amorphous material such as oZrNb or CoFeZrNb, and the length of the main pole tip portion 17 is approximately 5100 μm.The first high permeability block 10 is formed of a ferrite material, etc.
The thickness is 100 μm and the length is about 6 mm. The second high magnetic permeability block 11 is made of a 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. Third high permeability block 1 on the back side of the medium
2 also has a large surface facing the second high magnetic permeability block 11 to completely reduce magnetic resistance, and uses ferrite material or the like.

第4図は本実施例の構成が外部ノイズ磁界の影響が少い
ことの説明図で、外部からのノイズ磁界は全体的に通路
の大きい磁気回路14を主に通過し比較的通路の小さい
磁気回路16.16’i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
ノイズの影響が犬きく減少する。
FIG. 4 is an explanatory diagram showing that the configuration of this embodiment is less affected by external noise magnetic fields; the noise magnetic field from the outside mainly passes through the magnetic circuit 14, which has a relatively large path, and the magnetic circuit 14, which has a relatively small path. Since the amount passing through the circuits 16 and 16'i is small, the amount by which the external noise magnetic field interlinks with the coil 7 is reduced as a whole, and the influence of external noise is significantly reduced.

第6図は上記実施例の最適化のための説明図で、第3図
の主磁極先端部17の部分拡大図である。
FIG. 6 is an explanatory diagram for optimizing the above embodiment, and is a partially enlarged view of the main pole tip 17 in FIG. 3.

媒体高透磁率層2を磁気が通る磁気回路18に比較して
第3の高透磁率ブロックを磁気が通過する磁気回路19
の磁気抵抗をさらに減少させるためには、高透磁率薄膜
4と第2の高透磁率ブロック11との距離βが第3の高
透磁率ブロック12と媒体高透磁率層2との距離tより
大きくする必要がある。
A magnetic circuit 19 in which magnetism passes through the third high magnetic permeability block compared to a magnetic circuit 18 in which magnetism passes through the medium high magnetic permeability layer 2.
In order to further reduce the magnetic reluctance of It needs to be bigger.

また第6図に示すように本実施例において、再生時に媒
体からの磁束が十分にコイル7と鎖交するためにはコイ
ル7を鎖交する磁気回路20がコイル7を鎖交しない磁
気回路21より磁気抵抗が小さいことが望ましい。この
ためには第1の高透磁率ブロック1oと媒体高透磁率層
2との間の磁気抵抗が、第2の高透磁率ブロック11と
第3の高透磁率ブロック12の間の磁気抵抗より大きい
ことが条件となる。磁気抵抗は磁路の距離に比例し、面
積に反比例するから、第1の高透磁率ブロック1oが媒
体高透磁率層2に面した部分の面積’ji7sd、平均
距離dとし、第2の高透磁率ブロック11と第3の高透
磁率ブロック12の対面する部分の面積をSu、平均距
離をUとすると、d/5d)u/Suとすることにより
上記条件が満たされる。
Furthermore, as shown in FIG. 6, in this embodiment, in order for the magnetic flux from the medium to sufficiently interlink with the coil 7 during reproduction, the magnetic circuit 20 that interlinks the coil 7 is replaced by a magnetic circuit 21 that does not interlink the coil 7. It is desirable that the magnetic resistance be lower. For this purpose, the magnetic resistance between the first high magnetic permeability block 1o and the medium high magnetic permeability layer 2 must be greater than the magnetic resistance between the second high magnetic permeability block 11 and the third high magnetic permeability block 12. The condition is that it is large. Since magnetic resistance is proportional to the distance of the magnetic path and inversely proportional to the area, the area of the first high magnetic permeability block 1o facing the medium high magnetic permeability layer 2 is assumed to be 'ji7sd, the average distance is d, and the second high magnetic resistance is If the area of the facing portion of the magnetic permeability block 11 and the third high magnetic permeability block 12 is Su, and the average distance is U, then the above condition is satisfied by setting d/5d)u/Su.

捷た同様に第1の高透磁率ブロック10と媒体高透磁率
層2との間の磁気抵抗が第1の高透磁率ブロック1Qと
第2の高透磁率ブロック11との間の磁気抵抗より大き
いことも条件となる。このためには、d/Sd>v/S
vとすることが必要である。ここで第1の高透磁率ブロ
ック10と第2の高透磁率ブロック11の対向する部分
の面積をSv、平均距離をVとしている。
Similarly, the magnetic resistance between the first high magnetic permeability block 10 and the medium high magnetic permeability layer 2 is greater than the magnetic resistance between the first high magnetic permeability block 1Q and the second high magnetic permeability block 11. Being large is also a condition. For this, d/Sd>v/S
It is necessary to set it to v. Here, the area of the opposing portions of the first high magnetic permeability block 10 and the second high magnetic permeability block 11 is Sv, and the average distance is V.

さらに本実施例において外部ノイズ磁界の影響を少くす
るためには第7図中の磁路16の磁気抵抗が磁路14の
磁気抵抗より大きく外部磁束の多くが磁路14を通るこ
とが望ましいが、このだめには、第1の高透磁率ブロッ
ク1oと第2の高透磁率ブロック110間の磁気抵抗が
、第2の高透磁率ブロック11と第3の高透磁率ブロッ
ク12の間の磁気抵抗より大きいことが望捷しい。
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 path 16 in FIG. , in this case, the magnetic resistance between the first high magnetic permeability block 1o and the second high magnetic permeability block 110 is the same as the magnetic resistance between the second high magnetic permeability block 11 and the third high magnetic permeability block 12. It is desirable that the resistance be greater than that.

従って第1の高透磁率ブロック1oが媒体高透磁率層2
に面した部分の面積Sd及びその平均距離dと、第1の
高透磁率ブロック10と第2の高透磁率ブロック11の
対向する部分の面積Sv及びその平均距離Vとの間にd
/Sd>V/Svの関係を満たすように構成することが
望捷しい。
Therefore, the first high permeability block 1o is the medium high permeability layer 2.
There is a distance d between the area Sd of the facing portion and its average distance d, and the area Sv and the average distance V of the opposing portions of the first high magnetic permeability block 10 and the second high magnetic permeability block 11.
It is desirable to configure it so that the relationship /Sd>V/Sv is satisfied.

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挾持され
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
記主磁極に近接寸たは接続して設けられた第2の筒透磁
率体と、前記磁気記録媒体を挾んで、前記主磁極と反対
側に設けられた第3の高透磁体とを只備したことを特徴
とする磁気ヘッドを提供するもので、磁気ヘッドの磁気
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 short, the present invention provides a high permeability magnetic thin film in close proximity to a magnetic recording medium having a high magnetic permeability layer below a magnetization layer having perpendicular magnetic anisotropy. 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 cylindrical magnetic permeability body provided adjacently or connected to each other, and a third high magnetic permeability body provided on the opposite side of the main magnetic pole with the magnetic recording medium sandwiched therebetween. The present invention provides a magnetic head characterized in that it has the advantage of lowering the resistance of the magnetic circuit of the magnetic head, 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 drawings]

第1図は従来の垂直磁気記録用ヘッドの断面図、第2図
は外部ノイズ磁界の影響を示す従来の垂直磁気記録用ヘ
ッドの断面図、第3図は本発明の一実施例による磁気ヘ
ッドの断面図、第4図は外部ノイズ磁界の影響を示す本
実施例による磁気ヘッドの断面図、第5図乃至第7図は
本実施例の最適構造を示す部分拡大図である。 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、6・・・・・非磁性体、6・・・・・主磁極、
7・・・・・・コイル、8,9゜14.15,16.1
B、19,20.21・・・0.。 磁気回路、10・・・・・第1の高透磁率ブロック、1
1・・・・・・第2の高透磁率ブロック、12・山・・
第3の高透磁率ブロック、17・・・・・・主磁極先端
部分。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 す− 〆 巳り時4ゴ 3図 1/2 4図 : ’、171 第5図 2 41− 第7図 1
FIG. 1 is a sectional view of a conventional perpendicular magnetic recording head, FIG. 2 is a sectional view of a conventional perpendicular magnetic recording head showing the influence of an external noise magnetic field, and FIG. 3 is a magnetic head according to an embodiment of the present invention. FIG. 4 is a cross-sectional view of the magnetic head according to this embodiment showing the influence of an external noise magnetic field, and FIGS. 5 to 7 are partially enlarged views showing the optimal structure of this embodiment. DESCRIPTION OF SYMBOLS 1...Magnetic layer, 2...Medium high permeability layer, 3...Magnetic recording medium, 4...High magnetic permeability thin film, 6... ...Non-magnetic material, 6...Main magnetic pole,
7... Coil, 8,9°14.15,16.1
B, 19, 20.21...0. . Magnetic circuit, 10...First high magnetic permeability block, 1
1...Second high permeability block, 12. Mountain...
Third high permeability block, 17...main magnetic pole tip portion. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Fig. 4 - Figure 3 Figure 1/2 Figure 4: ', 171 Figure 5 2 41- Figure 7 1

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挾持されており、前記高
級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
気記録媒体を挾んで、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たことを特徴とする磁気ヘ
ッド。 (2)主磁極が磁化層に近接する部分における高透磁率
磁性薄膜と第2の高透磁率体との間の距離eを、高透磁
率層と第3の高透磁率体との間の距離tよりも大きくし
たことを特徴とする特許請求の範囲第1項記載の磁気ヘ
ッド。 (3)第1の高透磁率体と高透磁率層の対向する部分の
面積isd、第1の高透磁率体と高透磁率層間の平均距
離をd、第2と第3の高透磁率体の対向する部分の面積
をSu、第2と第3の高透磁率体間の平均距離をU、第
1と第2の高透磁率体の対向する部分の面積をSv、第
1と第2の高透磁率体間の平均距離をVとしたとき、d
15d>u/Su、d/Sd>v/Svとなるごとく構
成されたことを特徴とする特許請求の範囲第1項記載の
磁気ヘッド。 (4)第2と第3の高透磁率体の対向する部分の面積を
Su、第2と第3の高透磁率体間の平均距離をU、第1
と第2の高透磁率体の対向する部分の面積をSv、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 / S v )u / S u となるごとく構成されたことを特徴とする特許請求の範
囲第1項記載の磁気ヘシド。 (6)高透磁率磁性薄膜が、Co 、Zrを主成分とす
るアモルファス材料よりなることを特徴とする特許請求
の範囲第1項記載の磁気ヘッド。 (6)高透磁率磁性薄膜が、Go 、Fe 、 Zr 
、Nbを含むアモルファス材料よりなることを特徴とす
る特許請求の範囲第6項記載の磁気ヘッド。
[Scope of Claims] (1) A high permeability magnetic thin film is provided in close proximity to a magnetic recording medium having a high permeability layer under a magnetization layer having perpendicular magnetic anisotropy, and the high permeability magnetic thin film is 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 flux magnetic thin film; A second high magnetic permeability body provided close to or connected to each other, and a third high magnetic permeability body provided on the opposite side of the main magnetic pole with the magnetic recording medium sandwiched therebetween. magnetic head. (2) The distance e between the high magnetic permeability magnetic thin film and the second high magnetic permeability body in the part where the main magnetic pole is close to the magnetic layer is the distance e between the high magnetic permeability layer and the third high magnetic permeability body. A magnetic head according to claim 1, characterized in that the distance is greater than the distance t. (3) The area isd of the opposing portion of the first high magnetic permeability body and the high magnetic permeability layer, d is the average distance between the first high magnetic permeability body and the high magnetic permeability layer, and the second and third high magnetic permeability The area of the opposing parts of the body is Su, the average distance between the second and third high magnetic permeability bodies is U, the area of the opposing parts of the first and second high magnetic permeability bodies is Sv, and the first and second high permeability bodies are Sv. When the average distance between two high permeability materials is V, d
2. The magnetic head according to claim 1, wherein the magnetic head is configured such that 15d>u/Su and d/Sd>v/Sv. (4) The area of the opposing parts of the second and third high magnetic permeability bodies is Su, the average distance between the second and third high magnetic permeability bodies is U, and the first
The area of the opposing portion of the second high magnetic permeability body is Sv, and the area of the first
The magnetic heside according to claim 1, characterized in that, when the average distance between the second high magnetic permeability body and the second high magnetic permeability body is V, v/Sv)u/Su. (6) 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. (6) High permeability magnetic thin film made of Go, Fe, Zr
7. The magnetic head according to claim 6, wherein the magnetic head is made of an amorphous material containing Nb.
JP16130883A 1983-09-01 1983-09-01 Magnetic head Granted JPS6052907A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP16130883A JPS6052907A (en) 1983-09-01 1983-09-01 Magnetic head
US06/640,595 US4672494A (en) 1983-09-01 1984-08-14 Magnetic head for effecting perpendicular magnetic recording

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16130883A JPS6052907A (en) 1983-09-01 1983-09-01 Magnetic head

Related Child Applications (2)

Application Number Title Priority Date Filing Date
JP33712689A Division JPH02198010A (en) 1989-12-26 1989-12-26 Magnetic head
JP33712789A Division JPH02198011A (en) 1989-12-26 1989-12-26 Magnetic head

Publications (2)

Publication Number Publication Date
JPS6052907A true JPS6052907A (en) 1985-03-26
JPH0320803B2 JPH0320803B2 (en) 1991-03-20

Family

ID=15732630

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16130883A Granted JPS6052907A (en) 1983-09-01 1983-09-01 Magnetic head

Country Status (1)

Country Link
JP (1) JPS6052907A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5611612A (en) * 1979-07-02 1981-02-05 Toshiba Corp Magnetic head of vertical magnetizing type

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5611612A (en) * 1979-07-02 1981-02-05 Toshiba Corp Magnetic head of vertical magnetizing type

Also Published As

Publication number Publication date
JPH0320803B2 (en) 1991-03-20

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