JP3313795B2 - Magnetoresistive magnetic head - Google Patents

Magnetoresistive magnetic head

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Publication number
JP3313795B2
JP3313795B2 JP36111792A JP36111792A JP3313795B2 JP 3313795 B2 JP3313795 B2 JP 3313795B2 JP 36111792 A JP36111792 A JP 36111792A JP 36111792 A JP36111792 A JP 36111792A JP 3313795 B2 JP3313795 B2 JP 3313795B2
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JP
Japan
Prior art keywords
magnetoresistive
output
magnetic
head
current
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
JP36111792A
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Japanese (ja)
Other versions
JPH06203331A (en
Inventor
祥児 渕上
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 Corp
Panasonic Holdings Corp
Original Assignee
Panasonic Corp
Matsushita Electric Industrial Co Ltd
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Filing date
Publication date
Application filed by Panasonic Corp, Matsushita Electric Industrial Co Ltd filed Critical Panasonic Corp
Priority to JP36111792A priority Critical patent/JP3313795B2/en
Publication of JPH06203331A publication Critical patent/JPH06203331A/en
Application granted granted Critical
Publication of JP3313795B2 publication Critical patent/JP3313795B2/en
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Expired - Lifetime legal-status Critical Current

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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、ハードディスクドライ
ブ装置等で磁気記録媒体上に浮上して磁気記録を行う磁
気抵抗効果型磁気ヘッドに関するものであり、特にこの
磁気抵抗効果型磁気ヘッドの磁気抵抗素子の形状を改良
したものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magneto-resistance effect type magnetic head for performing magnetic recording by floating on a magnetic recording medium in a hard disk drive or the like, and more particularly to a magneto-resistance effect type magnetic head. This is an improvement in the shape of the element.

【0002】[0002]

【従来の技術】近年、コンピュータの外部記録装置で
は、その高速記録、高速読み出し出し等の高速性や大容
量記録性の要求から、ハードディスクドライブ装置が多
く利用されるようになってきている。このハードディス
クドライブ装置は、最近のコンピュータの小型化および
軽量かに対応すべくハードディスクドライブ装置の小型
高容量化を実現が望まれており、この小型高容量化を行
う為に、現在では磁気記録媒体の速度に依存せずに高出
力が得られる磁気ヘッドとして、磁気抵抗素子を用いた
磁気抵抗効果型磁気ヘッドの開発が望まれている。
2. Description of the Related Art In recent years, hard disk drives have been widely used as external recording devices for computers because of their demands for high-speed recording and high-speed reading and high-capacity recording. For this hard disk drive device, it is desired to realize a small and high capacity hard disk drive device in order to respond to recent miniaturization and light weight of a computer. It is desired to develop a magnetoresistive magnetic head using a magnetoresistive element as a magnetic head capable of obtaining high output without depending on the speed of the magnetic head.

【0003】以下に従来の磁気抵抗効果型磁気ヘッドに
ついて説明する。図4において(a)は、従来の磁気抵
抗効果型磁気ヘッドの構成を示す図であり、この磁気抵
抗効果型磁気ヘッドは、外部磁界に対して抵抗値変化を
示す動作を行う磁気抵抗素子からなる磁束検知部1、お
よび磁気抵抗素子の抵抗値変化を電圧変化に変えるため
電流を磁気抵抗素子に供給するためのリード部2等によ
り構成されている。
A conventional magnetoresistive head will be described below. FIG. 4A is a diagram showing a configuration of a conventional magnetoresistive magnetic head. This magnetoresistive magnetic head is composed of a magnetoresistive element which performs a change in resistance value with respect to an external magnetic field. And a lead 2 for supplying a current to the magnetoresistive element for changing a change in resistance of the magnetoresistive element into a change in voltage.

【0004】なお、この磁気抵抗効果型磁気ヘッドのリ
ード部を流れる電流の方向は、図4において矢印3で示
す方向である。そして、この磁気抵抗効果型磁気ヘッド
の磁束検知部1は、電流aで囲まれており、電流流入部
8の幅と電流流出部9の幅が等しく形成されている。
The direction of the current flowing through the read portion of the magneto-resistance effect type magnetic head is the direction indicated by arrow 3 in FIG. The magnetic flux detector 1 of the magnetoresistive head is surrounded by the current a, and the width of the current inlet 8 and the width of the current outlet 9 are equal.

【0005】以上のように構成された磁気抵抗効果型磁
気ヘッドの斜視図を図5に示す。この磁気抵抗効果型磁
気ヘッドの素子部は、磁気記録媒体面から見ると図6に
示すような構成になっており、磁束検知部1およびリー
ド部2は、非磁性の絶縁層11を介して磁気シールド1
0の間に設置されている。
FIG. 5 is a perspective view of the magnetoresistive head constructed as described above. The element section of the magnetoresistive head has a configuration as shown in FIG. 6 when viewed from the surface of the magnetic recording medium. The magnetic flux detecting section 1 and the lead section 2 are connected via a nonmagnetic insulating layer 11. Magnetic shield 1
It is installed between 0.

【0006】ここで上記構成の磁気抵抗効果型磁気ヘッ
ドの実際の動作を図7に示す。まず、磁気記録媒体4の
媒体上には、媒体内部磁化方向7で示されるような一方
向性の磁化がデータとして記録されている。この記録さ
れた磁化の反転方向から媒体外部磁束6が空中に放出さ
れ、これによって形成される媒体磁界上を磁気抵抗素子
の磁束検知部1が通過するようになる。
FIG. 7 shows the actual operation of the magneto-resistance effect type magnetic head having the above configuration. First, on the medium of the magnetic recording medium 4, unidirectional magnetization as indicated by the internal magnetization direction 7 of the medium is recorded as data. The magnetic flux 6 external to the medium is emitted into the air from the direction of reversal of the recorded magnetization, and the magnetic flux detecting unit 1 of the magnetoresistive element passes over the medium magnetic field formed by this.

【0007】この時、上記媒体磁束に対応した磁束検知
部1の抵抗値変化がリード部2に電流を流すことで電圧
変化として得られる。この磁気抵抗効果型磁気ヘッドを
トラック幅方向に左右に移動させた際の出力変化を図4
(a)に示す。この図4(a)に見られるように、磁気
抵抗効果型磁気ヘッドを左右に移動させたとき+(プラ
ス)側に移動した際には、出力は急速に減少し、−(マ
イナス)側に移動した際には一定の出力値を示した後に
出力減少を示し、トラック幅方向に対する出力の特性は
左右対称となる。
At this time, a change in the resistance value of the magnetic flux detector 1 corresponding to the medium magnetic flux is obtained as a voltage change by flowing a current through the lead 2. FIG. 4 shows an output change when the magnetoresistive head is moved right and left in the track width direction.
(A). As can be seen from FIG. 4A, when the magnetoresistive head is moved to the left or right, the output decreases rapidly and moves to the minus side. When it moves, it shows a constant output value and then shows a decrease in output, and the output characteristic in the track width direction is symmetrical.

【0008】以上のように構成された従来の磁気抵抗効
果型磁気ヘッドについて、以下にその動作を説明する。
図8に示されるような磁気抵抗素子部の拡大図におい
て、磁気記録媒体4が磁気抵抗素子部に対し、オフトラ
ック他を生じた場合のa点とb点の磁束検知部能力を考
えてみる。
The operation of the conventional magnetoresistive head constructed as described above will be described below.
In the enlarged view of the magnetoresistive element section as shown in FIG. 8, consider the magnetic flux detecting section capabilities at points a and b when the magnetic recording medium 4 generates off-track and the like with respect to the magnetoresistive element section. .

【0009】初期のa点およびb点の磁化の方向は、外
部磁界に対し線型な出力を発生するためにバイアス磁界
が付加されており既に電流方向3とθの角度を持ってお
り、従ってa点とb点の磁界の方向はMaおよびMbの
方向を向いている。また、磁気記録媒体4からの磁束の
方向はBaおよびBbの方向を向いており、これらa点
およびb点においてBaおよびBbのベクトル磁束成分
として寄与する。
The initial magnetization directions at point a and point b have a bias magnetic field added to generate a linear output with respect to an external magnetic field and already have an angle of θ with the current direction 3; The directions of the magnetic field at points b and b are in the directions of Ma and Mb. The direction of the magnetic flux from the magnetic recording medium 4 is in the directions of Ba and Bb, and contributes as vector magnetic flux components of Ba and Bb at points a and b.

【0010】このとき、磁気抵抗素子の抵抗ρは、電流
と磁化ベクトルのなす角θおよび抵抗変化率△ρを用い
て、ρ=△ρ・cos2θにより与えられる。従って、
a点における電流3とBaとのなす角をθa、b点にお
ける電流3とBbとのなす角をθbとすると、a点の抵
抗変化量は、ρ=△ρ(cos2θa−cos2θ)、
b点の抵抗変化量は、ρ=△ρ(cos2θb−cos
2θ)となる。一方、b点においてはBbとMbのなす
角が殆ど並行でありθb≒θになる為、磁気抵抗効果型
磁気ヘッドにおいては出力が得られない。
At this time, the resistance ρ of the magnetoresistive element is given by ρ = △ ρ · cos 2θ using the angle θ between the current and the magnetization vector and the resistance change rate △ ρ. Therefore,
Assuming that the angle between the current 3 and Ba at the point a is θa and the angle between the current 3 and Bb at the point b is θb, the resistance change at the point a is ρ = △ ρ (cos2θa−cos2θ),
The resistance change amount at point b is ρ = △ ρ (cos2θb-cos
2θ). On the other hand, at point b, the angle between Bb and Mb is almost parallel and θb ≒ θ, so that no output is obtained in the magnetoresistive head.

【0011】これに対して、図9に示すように磁気記録
抵抗素子部の右端に位置した場合、a点とb点の磁束検
知能力を考えると、磁気記録媒体4からの磁束の方向
は、BaおよびBbの方向であり、この場合のヘッド出
力はa点およびb点においてBaとMaのなす角およ
び、BbとMbのなす角に対応したものになる。
On the other hand, as shown in FIG. 9, when positioned at the right end of the magnetic recording resistance element portion, the direction of the magnetic flux from the magnetic recording medium 4 is: The head outputs in this case correspond to the angle between Ba and Ma and the angle between Bb and Mb at points a and b.

【0012】故にa点とb点において若干の出力差が生
じる。従って、磁気抵抗素子の左右両端での検知能力が
違い、図4(b)に示されるようなトラック幅方向にお
いて左右非対称な出力特性になってしまう。
Therefore, a slight output difference occurs between the point a and the point b. Therefore, the detection capabilities at the left and right ends of the magnetoresistive element are different, resulting in output characteristics that are asymmetrical in the track width direction as shown in FIG. 4B.

【0013】[0013]

【発明が解決しようとする課題】以上の説明から明らか
なように、上記従来の磁気抵抗効果型磁気ヘッドの構成
では、左右非対称なトラック幅方向の出力特性になり、
ヘッド中心のずれの方向によっては出力が得られない事
態をまねく為、ヘッド出力における中心と磁気抵抗素子
の形状上の中心が位置違いを発生するようになる。従っ
て、この磁気抵抗素子の出力によりトラック位置の制御
信号を得る場合には、右にずれた場合に得られる制御信
号と、左にずれた場合に得られる制御信号の間に差が発
生してしまうという問題が生じていた。
As is apparent from the above description, the above-described structure of the conventional magnetoresistive magnetic head has an output characteristic in the track width direction that is asymmetrical in the left-right direction.
An output cannot be obtained depending on the direction of displacement of the center of the head, so that the center of the head output and the center of the shape of the magnetoresistive element cause a positional difference. Therefore, when a control signal for the track position is obtained from the output of the magnetoresistive element, a difference occurs between the control signal obtained when the signal is shifted to the right and the control signal obtained when the signal is shifted to the left. There was a problem that it would.

【0014】本発明は以上の問題点に鑑み、オフトラッ
ク時に左右対称な出力が得られる磁気抵抗効果型磁気ヘ
ッドを提供することを目的とする。
In view of the above problems, an object of the present invention is to provide a magnetoresistive head capable of obtaining a symmetrical output during off-track.

【0015】[0015]

【課題を解決するための手段】上記問題点を解決するた
め、本発明は、磁束検知部の幅が電流流入部分に比べ電
流流出部分近傍で狭くなっている磁気抵抗素子形状を有
する磁気抵抗効果型磁気ヘッドの構成にしたものであ
る。
SUMMARY OF THE INVENTION In order to solve the above problems, the present invention provides a magnetoresistive element having a magnetoresistive element shape in which the width of a magnetic flux detecting portion is narrower near a current outflow portion than in a current inflow portion. This is a configuration of a type magnetic head.

【0016】[0016]

【作用】従って、本発明の磁気抵抗効果型磁気ヘッド
は、上記の磁束検知部の幅が電流流入部分に比べ電流流
出部分近傍で狭くした構成により、電流流出部分近傍で
幅が狭くなっているため、検知部での左右どちらの方向
の位置ずれに対しても出力を得ることが出来るようにな
り、磁気抵抗効果型磁気ヘッドにおけるトラック幅方向
の出力特性を左右対称にするという作用を奏するもので
ある。これは、素子の形状中心を出力中心に揃えること
ができるものであり、オフトラック時における出力特性
が左右対称の磁気抵抗効果型磁気ヘッドが構成されるも
のである。
Therefore, in the magnetoresistive head according to the present invention, the width of the magnetic flux detecting portion is narrower near the current outflow portion than in the current inflow portion, so that the width is smaller near the current outflow portion. For this reason, it is possible to obtain an output even when the detection unit is displaced in either the left or right direction, and to provide an effect that the output characteristics in the track width direction of the magnetoresistive head are made symmetrical. It is. This enables the shape center of the element to be aligned with the output center, and constitutes a magnetoresistive head having symmetric output characteristics during off-track.

【0017】[0017]

【実施例】本発明の実施例を、図面を参照しながら説明
する。図1(a)は、本発明の一実施例における磁気抵
抗効果型磁気ヘッドを示すものである。図1(a)にお
いて、外部磁界に対し抵抗値変化を示す磁気抵抗素子か
らなる磁束検知部1が設けられ、これらは一般に磁気抵
抗効果を示すFe−Ni系合金あるいはCo−Ni系合
金が使用される。この磁気抵抗素子は、真空蒸着法やス
パッタ法などの真空成膜法により成膜され、成膜は反磁
界を抑制し出力を向上するために500Å程度の特に薄
い膜厚にして使用される。
DESCRIPTION OF THE PREFERRED EMBODIMENTS Embodiments of the present invention will be described with reference to the drawings. FIG. 1A shows a magnetoresistive head according to an embodiment of the present invention. In FIG. 1 (a), a magnetic flux detecting section 1 composed of a magnetoresistive element exhibiting a change in resistance with respect to an external magnetic field is provided, and these are generally made of an Fe-Ni alloy or a Co-Ni alloy exhibiting a magnetoresistive effect. Is done. This magnetoresistive element is formed by a vacuum film forming method such as a vacuum evaporation method or a sputtering method. The film is formed to have a particularly thin film thickness of about 500 ° in order to suppress the demagnetizing field and improve the output.

【0018】また、図1(a)中では、磁気抵抗素子に
供給するためのリード部2が設けられ、このリード部2
には、一般に電気抵抗の低い金あるいはアルミニウム等
が用いられが、特に電気的拡散のエレクトロマイグレー
ションをおさえる場合には、リード部2としてタングス
テンが使用される。上記リード部2の成膜に際しては、
真空蒸着法やスパッタ法、CVD法などの真空成膜法が
一般に採用される。これらのリード部2の成膜の形状
は、写真製版技術(フォトリソグラフィー技術)により
任意形状の保護成膜を形成し、化学的食刻あるいは物理
的食刻による加工により形成される。
In FIG. 1A, a lead portion 2 for supplying a magnetic resistance element is provided.
In general, gold, aluminum, or the like having a low electric resistance is used. Tungsten is used as the lead portion 2 particularly when electromigration of electric diffusion is suppressed. When forming the lead 2,
In general, a vacuum deposition method such as a vacuum deposition method, a sputtering method, and a CVD method is employed. These lead portions 2 are formed by forming a protective film of an arbitrary shape by a photoengraving technique (photolithography technique) and processing the film by chemical etching or physical etching.

【0019】ここで本発明の磁気抵抗効果型磁気ヘッド
において特徴的な点は、図1(a)に示すごとく、電流
流入部8における素子幅が電流流出部9のbにおいて上
記電流流入部8よりも狭くなっている点である。
Here, the characteristic point of the magnetoresistive head according to the present invention is that, as shown in FIG. 1A, the element width of the current inflow section 8 is smaller than that of the current inflow section 8b at the current outflow section 9b. It is narrower than that.

【0020】以上のように構成された本実施例の磁気抵
抗効果型磁気ヘッドについて以下にその動作を説明す
る。図3に示されるような磁気抵抗素子部の拡大図にお
いて、磁気記録媒体4が、磁気抵抗素子部に対してオフ
トラックを生じた場合のa点とb点の磁束検知能力を考
えてみる。
The operation of the magneto-resistance effect type magnetic head of the embodiment constructed as described above will be described below. In the enlarged view of the magnetoresistive element portion as shown in FIG. 3, consider the magnetic flux detecting ability at points a and b when the magnetic recording medium 4 has an off-track with respect to the magnetoresistive element portion.

【0021】まず、初期のa点の磁化の方向は、外部磁
界に対し線型な出力を発生するためにバイアス磁界が付
加されており、既に電流方向3とθの角度を持ってい
る。a点の磁化の方向はMaの方向を向いている。
First, a bias magnetic field is added to the initial magnetization direction at point a in order to generate a linear output with respect to an external magnetic field, and the magnetization direction already has an angle of θ with the current direction 3. The direction of magnetization at point a is oriented in the direction of Ma.

【0022】しかし、b点においては図1(a)bに示
されるように幅が狭くなっているため電流の方向がb点
のiで示される方向を向いている。故に、バイアス磁界
が付与されて得られるb点の磁化の方向はMbとなる。
従って、磁気記録媒体4からの磁束BbとMbは、お互
いに角度を持つことになり、従来の磁気抵抗効果型磁気
ヘッドでは電流流入部8の幅と電流流出部9の幅が等し
く形成されていてb点においてはBbとMbのなす角が
殆ど並行になってθb≒θになる為、このb点において
は出力が得られなかったものが、本発明の形状を用いる
ことにより出力を得ることが出来るようになる。
However, since the width at point b is narrow as shown in FIG. 1 (a) b, the direction of the current is in the direction indicated by i at point b. Therefore, the direction of the magnetization at point b obtained by applying the bias magnetic field is Mb.
Therefore, the magnetic fluxes Bb and Mb from the magnetic recording medium 4 have an angle to each other, and the width of the current inflow portion 8 and the width of the current outflow portion 9 are formed equal in the conventional magnetoresistance effect type magnetic head. At point b, since the angle between Bb and Mb is almost parallel and θb ≒ θ, an output cannot be obtained at point b. However, an output can be obtained by using the shape of the present invention. Can be done.

【0023】また、図4に示す様に、磁気記録媒体4が
磁気抵抗素子部の右端に位置した場合、a点とb点の磁
束検知能力を考えると、磁気記録媒体4からの磁束の方
向は、BaおよびBbの方向となる。ゆえに、これらは
a点およびb点においてBaとMaのなす角、およびB
bとMbのなす角に対応した出力が発生する。従って、
a点とb点において出力差はあるが、それぞれに出力が
得られるようになる。
Further, as shown in FIG. 4, when the magnetic recording medium 4 is located at the right end of the magnetoresistive element portion, the direction of the magnetic flux from the magnetic recording medium 4 is considered in consideration of the magnetic flux detection capability at points a and b. Is the direction of Ba and Bb. Therefore, these are the angle between Ba and Ma at points a and b, and B
An output corresponding to the angle between b and Mb is generated. Therefore,
Although there is an output difference between point a and point b, an output can be obtained for each.

【0024】以上のように本実施例によれば、磁気抵抗
効果型磁気ヘッドの磁束検知部幅が電気流入部分に比
べ、電気流出部分近傍で狭くなっている磁気抵抗素子形
状を備えることにより、図1(b)に示されるような、
トラック幅方向の出力特性が左右対称である磁気抵抗効
果型磁気ヘッドが得られるものである。従って、この磁
気抵抗素子の出力によりトラック位置の制御信号を得る
場合には、右にずれた場合と、左にずれた場合との両方
で出力が得られるようになり、いずれの場合でも位置ず
れを制御する制御信号を発して、素子の形状中心を出力
中心に揃えることができるようになる。
As described above, according to this embodiment, the magnetoresistive effect type magnetic head has a magnetoresistive element shape in which the width of the magnetic flux detecting portion is smaller in the vicinity of the electric outflow portion than in the electric inflow portion. As shown in FIG.
A magnetoresistive head having a symmetrical output characteristic in the track width direction can be obtained. Accordingly, when a track position control signal is obtained from the output of the magnetoresistive element, an output can be obtained both in the case of shifting to the right and in the case of shifting to the left. Is generated, and the shape center of the element can be aligned with the output center.

【0025】[0025]

【発明の効果】以上述べたごとく本発明は、磁束検知部
の幅が電流流入部分に比べ電流流出部分の近傍で狭くな
って磁気抵抗素子形状を有することを特徴とする磁気抵
抗効果型磁気ヘッドであるので、磁気抵抗効果素子の左
右に端部の再生能力を等しくすることができるものであ
り、これにより、本発明は、トラック幅方向の出力特性
が、左右対称であるという効果を有した磁気抵抗効果型
磁気ヘッドを実現することができる。
As described above, according to the present invention, the width of the magnetic flux detecting portion is smaller in the vicinity of the current outflow portion than in the current inflow portion, so that the magnetic head has a magnetoresistive element shape. Therefore, the reproduction capability of the left and right ends of the magnetoresistive effect element can be made equal, whereby the present invention has an effect that the output characteristics in the track width direction are symmetric. A magnetoresistive head can be realized.

【0026】よって、トラック幅方向の出力特性が左右
対称であるので、この磁気抵抗素子の出力によりオフト
ラック時にトラック位置が右にずれた場合と、左にずれ
た場合との両方で出力が得られるようになり、いずれの
場合でも位置ずれを制御する制御信号を発して、素子の
形状中心を出力中心に揃えることができるという効果を
有する。
Accordingly, since the output characteristics in the track width direction are symmetrical, the output of this magnetoresistive element can be obtained both when the track position shifts to the right during off-track and when the track position shifts to the left. In any case, a control signal for controlling the displacement can be issued, and the shape center of the element can be aligned with the output center.

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

【図1】(a)は本発明の一実施例における磁気抵抗効果
型磁気ヘッドの構成図、(b)は本発明によって得られる
左右対称のトラック幅方向の出力特性図、
1A is a configuration diagram of a magnetoresistive magnetic head according to an embodiment of the present invention, FIG. 1B is an output characteristic diagram of a symmetrical track width direction obtained by the present invention,

【図2】本発明の素子形状において、磁束検知部分の左
端に磁気記録媒体がある場合の各部の出力を示す図、
FIG. 2 is a diagram showing the output of each unit when a magnetic recording medium is located at the left end of a magnetic flux detection part in the element shape of the present invention;

【図3】本発明の素子形状において、磁束検知部分の右
端に磁気記録媒体があるる場合の各部の出力を示す図、
FIG. 3 is a diagram showing the output of each unit when a magnetic recording medium is present at the right end of a magnetic flux detection part in the element shape of the present invention;

【図4】(a)は従来例における磁気抵抗効果型磁気ヘッ
ドの構成図、(b)は従来例において得られる左右非対称
のトラック幅方向の出力特性図、
FIG. 4A is a configuration diagram of a magnetoresistive effect type magnetic head according to a conventional example, FIG.

【図5】従来例における磁気抵抗効果型磁気ヘッドの構
成図、
FIG. 5 is a configuration diagram of a conventional magnetoresistive head;

【図6】従来例における磁気抵抗効果型磁気ヘッドの磁
気記録媒体面からの外観図、
FIG. 6 is an external view of a magnetoresistive head according to a conventional example as viewed from a magnetic recording medium surface.

【図7】磁気抵抗効果型磁気ヘッドの動作を示す図、FIG. 7 is a diagram showing an operation of the magnetoresistive head;

【図8】磁束検知部分の左端に磁気記録媒体がある場合
の各部の出力を示す図、
FIG. 8 is a diagram showing the output of each unit when the magnetic recording medium is at the left end of the magnetic flux detection unit;

【図9】磁束検知部分の右端に磁気記録媒体がある場合
の各部の出力を示す図。
FIG. 9 is a diagram showing the output of each unit when a magnetic recording medium is at the right end of the magnetic flux detection unit.

【符号の説明】[Explanation of symbols]

1 磁束検知部 2 リード部 3 電流の方向 4 磁気記録媒体 5 磁気抵抗素子内の磁束 6 媒体外部磁界 7 媒体内部磁化方向 8 電流流入部 9 電流流出部 10 磁気シールド 11 絶縁層 DESCRIPTION OF SYMBOLS 1 Magnetic flux detection part 2 Lead part 3 Current direction 4 Magnetic recording medium 5 Magnetic flux in a magnetoresistive element 6 Medium external magnetic field 7 Medium internal magnetization direction 8 Current inflow part 9 Current outflow part 10 Magnetic shield 11 Insulation layer

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 磁束検知部の幅が、電流流入部分に比べ
電流流出部分の近傍で狭くなった磁気抵抗素子形状を有
することを特徴とする磁気抵抗効果型磁気ヘッド。
1. A magnetoresistive head according to claim 1, wherein the width of the magnetic flux detecting portion is smaller in the vicinity of the current outflow portion than in the current inflow portion.
JP36111792A 1992-12-29 1992-12-29 Magnetoresistive magnetic head Expired - Lifetime JP3313795B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP36111792A JP3313795B2 (en) 1992-12-29 1992-12-29 Magnetoresistive magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP36111792A JP3313795B2 (en) 1992-12-29 1992-12-29 Magnetoresistive magnetic head

Publications (2)

Publication Number Publication Date
JPH06203331A JPH06203331A (en) 1994-07-22
JP3313795B2 true JP3313795B2 (en) 2002-08-12

Family

ID=18472276

Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP3313795B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3388944B2 (en) * 1995-06-06 2003-03-24 富士通株式会社 Magnetic disk drive and reproducing method thereof

Also Published As

Publication number Publication date
JPH06203331A (en) 1994-07-22

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