JPH05159224A - Thin film magnetic head - Google Patents

Thin film magnetic head

Info

Publication number
JPH05159224A
JPH05159224A JP32163291A JP32163291A JPH05159224A JP H05159224 A JPH05159224 A JP H05159224A JP 32163291 A JP32163291 A JP 32163291A JP 32163291 A JP32163291 A JP 32163291A JP H05159224 A JPH05159224 A JP H05159224A
Authority
JP
Japan
Prior art keywords
magnetic
core
magnetic pole
thin film
pole portion
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
JP32163291A
Other languages
Japanese (ja)
Inventor
Tetsuji Soeda
哲司 添田
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 JP32163291A priority Critical patent/JPH05159224A/en
Publication of JPH05159224A publication Critical patent/JPH05159224A/en
Pending legal-status Critical Current

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  • Magnetic Heads (AREA)

Abstract

PURPOSE:To unnecessitate the impression of a magnetic field for applying uniaxial anisotropy to a magnetic pole part in the case of forming a magnetic substance core concerning the thin film magnetic head for recording and reproducing to be loaded on a hard disk device. CONSTITUTION:Since a magnetic substance core 1 is provided in a certain shape having a magnetic pole part 3 spreading on the extension of a magnetic pole part 2 and on the opposite side of a back core part 16, the uniaxial anisotropy caused by shape anisotropy can be applied to the magnetic pole part 2 of the magnetic substance core 1.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明はハードディスク装置に搭
載される記録再生用の薄膜磁気ヘッドに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a recording / reproducing thin film magnetic head mounted on a hard disk drive.

【0002】[0002]

【従来の技術】以下に従来の薄膜磁気ヘッドについて説
明する。
2. Description of the Related Art A conventional thin film magnetic head will be described below.

【0003】図4および図5に示すように、Al23
TiCなどのセラミック基板14上に、Al23の下地
絶縁層11をスパッタリング法により形成し、蒸着法あ
るいはスパッタリング法により下地パーマロイ層を形成
する。次に、下地パーマロイ層の上にフォトレジストを
塗布し、磁性体コア1の形状のマスクを用いて露光し、
さらに現像して磁性体コア1の形状をしたレジストを形
成する。
As shown in FIGS. 4 and 5, Al 2 O 3
A base insulating layer 11 of Al 2 O 3 is formed on a ceramic substrate 14 such as TiC by a sputtering method, and a base permalloy layer is formed by a vapor deposition method or a sputtering method. Next, a photoresist is applied on the underlying permalloy layer, and exposed using a mask having the shape of the magnetic core 1.
Further development is performed to form a resist having the shape of the magnetic core 1.

【0004】その後、前記した方法により形成されたレ
ジストのない下地パーマロイ層の上に、めっき法により
下部磁性膜4,5を、膜付けする。
Thereafter, the lower magnetic films 4 and 5 are formed by plating on the resist-free base permalloy layer formed by the above-mentioned method.

【0005】次に、露光、現像を行いレジストを除去
し、さらにイオンミリングにより磁性体コア1の形状以
外の部分の下地パーマロイ層を除去する。
Next, exposure and development are performed to remove the resist, and the underlying permalloy layer other than the shape of the magnetic core 1 is removed by ion milling.

【0006】その上に、絶縁体となるレジスト12を形
成し、第1導体コイル6、レジスト12、第2導体コイ
ル7、レジスト12の層を形成する。
A resist 12 serving as an insulator is formed thereon, and layers of the first conductor coil 6, the resist 12, the second conductor coil 7 and the resist 12 are formed.

【0007】第1,2の導体コイル6,7の形成および
レジスト12による絶縁体の形成後はスパッタリング法
により下地パーマロイ層を形成する。次に、下部磁性膜
4,5の形成時と同様にして上部磁性膜8,9用のコア
形状のレジストを形成する。さらに、レジストのない下
地パーマロイ層の上に、めっき法により上部磁性膜8,
9を形成する。
After the formation of the first and second conductor coils 6 and 7 and the formation of the insulator by the resist 12, a base permalloy layer is formed by a sputtering method. Next, a core-shaped resist for the upper magnetic films 8 and 9 is formed in the same manner as when forming the lower magnetic films 4 and 5. Further, the upper magnetic film 8 is formed by plating on the underlying permalloy layer having no resist,
9 is formed.

【0008】最後に、Al23の保護膜15をスパッタ
法により形成したのち、表面がフラットになるようにラ
ップ加工する。図中の10はギャップ、13は磁極部、
16はバックコア部である。
Finally, after forming a protective film 15 of Al 2 O 3 by the sputtering method, lapping is performed so that the surface becomes flat. In the figure, 10 is a gap, 13 is a magnetic pole portion,
16 is a back core part.

【0009】上部磁性膜8,9および下部磁性膜4,5
の形成の際、磁歪が正(>0)の場合には、図7(a)
のような磁区構造を呈する。また、磁歪が負(<0)の
場合には図7(b)のような磁区構造を呈する。
Upper magnetic films 8 and 9 and lower magnetic films 4,5
When the magnetostriction is positive (> 0) during formation of
It exhibits a magnetic domain structure like. When the magnetostriction is negative (<0), the magnetic domain structure shown in FIG.

【0010】また、図4に示したような磁性体コア1が
延長した磁極部13を有する形状では、形状異方性によ
り図6に示したような縦方向に磁壁をもった磁区構造を
呈する。これに図6に示したようなX軸方向に磁界を印
加することにより、形状異方性の磁区構造に打ち勝っ
て、図7(b)に示したような磁区構造になる。すなわ
ち、磁性体コア1の形成時に、磁界の印加を必要とす
る。
Further, the shape having the extended magnetic pole portion 13 of the magnetic core 1 as shown in FIG. 4 has a magnetic domain structure having domain walls in the vertical direction as shown in FIG. 6 due to shape anisotropy. .. By applying a magnetic field to this in the X-axis direction as shown in FIG. 6, a magnetic domain structure having a shape anisotropy is overcome and a magnetic domain structure as shown in FIG. 7B is obtained. That is, it is necessary to apply a magnetic field when forming the magnetic core 1.

【0011】[0011]

【発明が解決しようとする課題】上記のように従来の磁
極体コア1の形状では、磁性体コア1の形成時に、形状
異方性に打ち勝つ程度の磁界の印加を必要であるという
問題点を有していた。
As described above, the conventional shape of the magnetic pole body core 1 requires the application of a magnetic field that overcomes the shape anisotropy when the magnetic body core 1 is formed. I had.

【0012】本発明は上記従来の問題点を解決するもの
で、磁性体コアの形成時に一軸異方性を磁極部に与える
ための磁界の印加を必要としない薄膜磁気ヘッドを提供
することを目的とする。
The present invention solves the above-mentioned conventional problems, and an object of the present invention is to provide a thin film magnetic head which does not require the application of a magnetic field for imparting uniaxial anisotropy to a magnetic pole portion when forming a magnetic core. And

【0013】[0013]

【課題を解決するための手段】この目的を達成するため
に本発明の薄膜磁気ヘッドは磁極部の延長上で、かつ、
バックコア部と反対側に広がる磁極部を有する形状の磁
性体コアを設けている。
In order to achieve this object, a thin film magnetic head of the present invention has a magnetic pole portion extended and
A magnetic core having a shape having a magnetic pole portion extending to the opposite side of the back core portion is provided.

【0014】[0014]

【作用】この構成により、磁性体コアの磁極部に形状異
方性による一軸異方性を付与することとなる。
With this structure, uniaxial anisotropy due to shape anisotropy is given to the magnetic pole portion of the magnetic core.

【0015】[0015]

【実施例】以下本発明の一実施例について、図面を参照
しながら説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings.

【0016】本発明の一実施例を示す図1および図2で
は、従来例と同一部品に同一番号を付して説明は省略す
る。
In FIGS. 1 and 2 showing an embodiment of the present invention, the same parts as those of the conventional example are designated by the same reference numerals and the description thereof will be omitted.

【0017】本実施例の特徴とするところは、前述従来
の磁性体コア1を図1および図2に示すようにバックコ
ア部16と反対側に広がりをもった磁極部3を形成した
磁性体コア1とした点である。
The feature of this embodiment lies in that the above-mentioned conventional magnetic core 1 is formed with a magnetic pole portion 3 having a spread on the side opposite to the back core portion 16 as shown in FIGS. This is the point where core 1 is set.

【0018】この構成より、磁極部2はX方向に磁界を
印加することなく、形状異方性により図3に示したよう
なX方向に磁壁をもった磁区構造にできる。
With this structure, the magnetic pole portion 2 can have a magnetic domain structure having domain walls in the X direction as shown in FIG. 3 due to the shape anisotropy without applying a magnetic field in the X direction.

【0019】バックコア部16と反対側に広がりをもっ
た磁極部3は、薄膜プロセス終了後に、ラップ加工によ
り除去される。すなわち、磁極部3は磁極部2に形状異
方性による一軸異方性を付与するためのみに必要であ
り、一軸異方性を付与したのちは不要となり、最終的に
は除去される。
The magnetic pole portion 3 having a side opposite to the back core portion 16 is removed by lapping after the thin film process is completed. That is, the magnetic pole portion 3 is necessary only for imparting uniaxial anisotropy due to the shape anisotropy to the magnetic pole portion 2, becomes unnecessary after imparting the uniaxial anisotropy, and is finally removed.

【0020】ここで、磁極部3がなく磁極部2のみでも
一軸異方性を付与できるが、磁極部3を形成することに
より、磁性体コア1のエッジ部の膜厚が厚くなるため、
ラップ加工により切除することにより、膜厚分布の良い
磁極部2が得られる。
Here, uniaxial anisotropy can be imparted only by the magnetic pole portion 2 without the magnetic pole portion 3, but since the magnetic pole portion 3 is formed, the film thickness at the edge portion of the magnetic core 1 becomes thicker.
By cutting off by lapping, the magnetic pole portion 2 having a good film thickness distribution can be obtained.

【0021】なお磁性体コア1の磁極部2の縦横比は
0.6以下とすることが望ましい。以上のように本実施
例によれば、磁極部2の延長上で、かつバックコア部1
6と反対側に広がる磁極部3を有する形状の磁性体コア
1を設けることにより、薄膜磁気ヘッドの磁性体コア1
の形成時に一軸異方性を磁極部2に与えるための磁界を
必要とせず、形状異方性でのみ磁性体コア1の磁極部2
に一軸異方性を与えることができる。これにより磁界を
与えるための磁石を小型化または不要にできるため、磁
性体形成装置の簡略化や低コスト化ができる。
It is desirable that the magnetic pole portion 2 of the magnetic core 1 has an aspect ratio of 0.6 or less. As described above, according to the present embodiment, the extension of the magnetic pole portion 2 and the back core portion 1 are performed.
By providing the magnetic core 1 having a shape having the magnetic pole portion 3 which spreads to the side opposite to 6, the magnetic core 1 of the thin film magnetic head
A magnetic field for giving uniaxial anisotropy to the magnetic pole portion 2 is not required at the time of forming the magnetic pole, and the magnetic pole portion 2 of the magnetic core 1 is formed only by the shape anisotropy.
Can be given uniaxial anisotropy. As a result, the magnet for applying the magnetic field can be made smaller or unnecessary, so that the magnetic material forming apparatus can be simplified and the cost can be reduced.

【0022】[0022]

【発明の効果】以上の実施例の説明からも明らかなよう
に本発明は、磁極部の延長上で、かつバックコア部と反
対側に広がる磁極部を有する形状の磁性体コアを設けた
構成により、磁性体コアの形成時に一軸異方性を磁極部
に与えるため磁界の印加を必要としない優れた薄膜磁気
ヘッドを実現できるものである。
As is apparent from the above description of the embodiments, the present invention is provided with a magnetic core having a shape having a magnetic pole portion extending on the extension of the magnetic pole portion and on the side opposite to the back core portion. As a result, an excellent thin film magnetic head that does not require application of a magnetic field can be realized because uniaxial anisotropy is given to the magnetic pole portion when the magnetic core is formed.

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

【図1】本発明の一実施例の薄膜磁気ヘッドの要部の概
念を保護膜を欠載して示した平面略図
FIG. 1 is a schematic plan view showing a concept of a main part of a thin film magnetic head according to an embodiment of the present invention with a protective film omitted.

【図2】図1のA−A′断面の薄膜磁気ヘッドの要部断
面図
FIG. 2 is a cross-sectional view of a main part of the thin film magnetic head taken along the line AA ′ in FIG.

【図3】本発明の一実施例の薄膜磁気ヘッドの磁性体コ
アの磁区構造を示す図
FIG. 3 is a diagram showing a magnetic domain structure of a magnetic core of a thin film magnetic head according to an embodiment of the present invention.

【図4】従来の薄膜磁気ヘッドの要部の概念を保護膜を
欠載して示した平面略図
FIG. 4 is a schematic plan view showing a concept of a main part of a conventional thin film magnetic head without a protective film.

【図5】図4のB−B′断面の薄膜磁気ヘッドの要部断
面図
5 is a cross-sectional view of the main part of the thin-film magnetic head taken along the line BB ′ in FIG.

【図6】従来の薄膜磁気ヘッドの磁性体コアの磁区構成
を示す図
FIG. 6 is a diagram showing a magnetic domain configuration of a magnetic core of a conventional thin film magnetic head.

【図7】(a)同薄膜磁気ヘッドの磁性体コアの磁歪が
正の場合の磁区構造を示す図 (b)同薄膜磁気ヘッドの磁性体コアの磁歪が負の場合
の磁区構造を示す図
FIG. 7A is a diagram showing a magnetic domain structure when the magnetostriction of a magnetic core of the thin film magnetic head is positive; FIG. 7B is a diagram showing a magnetic domain structure when the magnetostriction of the magnetic core of the thin film magnetic head is negative.

【符号の説明】[Explanation of symbols]

1 磁性体コア 2 磁極部 3 磁極部 16 バックコア部 1 magnetic core 2 magnetic pole part 3 magnetic pole part 16 back core part

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 平面状に巻回された一層ないし多層の導
体コイルと、前記導体コイルを絶縁する絶縁体と、前記
導体コイルを挟む二層以上の磁性膜で平面状に形成され
た磁性体コアを備えた薄膜磁気ヘッドであって、磁極部
の延長上で、かつバックコア部と反対側に広がる磁極部
を有する形状の前記磁性体コアを設けた薄膜磁気ヘッ
ド。
1. A magnetic body formed in a plane by a one-layer or multi-layer conductor coil wound in a plane, an insulator for insulating the conductor coil, and two or more magnetic films sandwiching the conductor coil. A thin film magnetic head having a core, wherein the magnetic core is provided in a shape having a magnetic pole part extending on the side opposite to the back core part on extension of the magnetic pole part.
【請求項2】 磁性体コアは、その磁極部の一軸異方性
を形状異方性により形成した請求項1記載の薄膜磁気ヘ
ッド。
2. The thin film magnetic head according to claim 1, wherein the magnetic core is formed by uniaxial anisotropy of its magnetic pole portion by shape anisotropy.
JP32163291A 1991-12-05 1991-12-05 Thin film magnetic head Pending JPH05159224A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32163291A JPH05159224A (en) 1991-12-05 1991-12-05 Thin film magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32163291A JPH05159224A (en) 1991-12-05 1991-12-05 Thin film magnetic head

Publications (1)

Publication Number Publication Date
JPH05159224A true JPH05159224A (en) 1993-06-25

Family

ID=18134674

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32163291A Pending JPH05159224A (en) 1991-12-05 1991-12-05 Thin film magnetic head

Country Status (1)

Country Link
JP (1) JPH05159224A (en)

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