JP2979966B2 - Magnetic head - Google Patents

Magnetic head

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Publication number
JP2979966B2
JP2979966B2 JP6189106A JP18910694A JP2979966B2 JP 2979966 B2 JP2979966 B2 JP 2979966B2 JP 6189106 A JP6189106 A JP 6189106A JP 18910694 A JP18910694 A JP 18910694A JP 2979966 B2 JP2979966 B2 JP 2979966B2
Authority
JP
Japan
Prior art keywords
magnetic
recording medium
bias
magnetic head
recording
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
JP6189106A
Other languages
Japanese (ja)
Other versions
JPH07334820A (en
Inventor
敏男 安藤
昭彦 野村
裕文 今岡
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.)
Victor Company of Japan Ltd
Original Assignee
Victor Company of Japan Ltd
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Filing date
Publication date
Application filed by Victor Company of Japan Ltd filed Critical Victor Company of Japan Ltd
Priority to JP6189106A priority Critical patent/JP2979966B2/en
Publication of JPH07334820A publication Critical patent/JPH07334820A/en
Application granted granted Critical
Publication of JP2979966B2 publication Critical patent/JP2979966B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

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、磁気ヘッドに係り、特
に高密度な垂直磁気記録信号を高効率で再生することが
できる磁気ヘッドに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic head and, more particularly, to a magnetic head capable of reproducing a high density perpendicular magnetic recording signal with high efficiency.

【0002】[0002]

【従来の技術】一般に、磁化方向を面内水平方向に設定
した面内記録に代わる次世代の高密度記録方式として、
磁化方向を媒体の厚み方向に設定した垂直磁気記録の研
究開発が盛んに行なわれている。一方、磁気ヘッドに関
しては、高密度で且つ高出力が得られることから、再生
ヘッドとして磁気抵抗効果を利用した磁気抵抗効果素子
型の磁気ヘッドが注目されており、一部では既に実用化
されている。
2. Description of the Related Art In general, as a next-generation high-density recording method which replaces in-plane recording in which the magnetization direction is set in the in-plane horizontal direction,
Research and development on perpendicular magnetic recording in which the magnetization direction is set in the thickness direction of the medium has been actively conducted. On the other hand, as for a magnetic head, a high-density and high-output can be obtained, and therefore, a magneto-resistive element-type magnetic head utilizing a magneto-resistive effect has been attracting attention as a reproducing head, and some magnetic heads have already been put to practical use. I have.

【0003】垂直磁気記録媒体の信号を記録再生する磁
気抵抗効果素子型の磁気ヘッドとして、例えば平板状の
磁気抵抗効果素子を2層構造に積層し、この素子全体に
一方向に電流を流すことによって互いに他方の磁気抵抗
効果素子に逆方向に平行にバイアス磁界をかけておき、
磁気記録媒体から発生する磁界によって生ずる2層の磁
気抵抗効果素子の磁化変化の差を信号として検出する方
法が提案されている(特公昭63−29327号公報を
参照)。
As a magnetoresistive element type magnetic head for recording and reproducing signals from a perpendicular magnetic recording medium, for example, a plate-shaped magnetoresistive element is laminated in a two-layer structure, and a current flows in one direction in the entire element. , A bias magnetic field is applied in parallel to the other magnetoresistive element in the opposite direction,
There has been proposed a method of detecting, as a signal, a difference between changes in magnetization of two layers of magnetoresistive elements caused by a magnetic field generated from a magnetic recording medium (see Japanese Patent Publication No. Sho 63-29327).

【0004】この場合、磁気記録媒体の磁化反転部分を
磁気ヘッドが跨いだ時に磁化変化が生じて出力が出るこ
とになり、孤立再生波形が単峰波となる。従って、現在
用いられている磁気記録再生装置における面内記録媒体
をリング型磁気ヘッドで再生した時の波形と同形である
ため、上記磁気抵抗効果素子型の磁気ヘッドを磁気記録
再生装置に利用する場合、特別な波形整形操作は不要に
なるという利点を有している。
In this case, when the magnetic head straddles the magnetization reversal portion of the magnetic recording medium, a change in magnetization occurs and an output is produced, and the isolated reproduction waveform becomes a single peak wave. Therefore, since the waveform of the in-plane recording medium in the magnetic recording / reproducing apparatus currently used is the same as the waveform when reproduced by the ring type magnetic head, the magnetic head of the magnetoresistive element type is used for the magnetic recording / reproducing apparatus. In this case, there is an advantage that a special waveform shaping operation becomes unnecessary.

【0005】[0005]

【発明が解決しようとする課題】ところで、上述したよ
うな磁気抵抗効果素子を用いた従来の磁気ヘッドにあっ
ては中間層を介して積層された一対の磁気抵抗効果素子
と磁気記録媒体との間で形成される磁気回路における磁
束の漏れが比較的大きく、再生出力も比較的小さくなっ
てしまうという問題点があった。
By the way, in the conventional magnetic head using the above-described magneto-resistance effect element, a pair of the magneto-resistance effect element and the magnetic recording medium laminated with an intermediate layer interposed therebetween. There is a problem that the leakage of magnetic flux in the magnetic circuit formed between them is relatively large and the reproduction output is relatively small.

【0006】更には、十分な大きさのバイアス磁界を得
るためには大きな電流を必要とし、このように電流を大
きくすることは消費電力の増大、電源装置の大型化、発
熱によるノイズの増加や素子の破壊等の問題を生ずるこ
とになる。
Further, a large current is required to obtain a sufficiently large bias magnetic field. Increasing the current in such a manner increases power consumption, increases the size of a power supply device, increases noise due to heat generation, and the like. This causes a problem such as destruction of the element.

【0007】本発明は、以上のような問題点に着目し、
これを有効に解決すべく創案されたものであり、その目
的は漏れ磁束を減少させて再生効率を向上させることが
できる磁気ヘッドを提供することにある。
[0007] The present invention focuses on the above problems,
The present invention has been made to solve this problem effectively, and an object of the present invention is to provide a magnetic head capable of reducing the leakage magnetic flux and improving the reproduction efficiency.

【0008】[0008]

【課題を解決するための手段】本発明は、上記問題点を
解決するために、磁気記録媒体の走行方向に対して、
対の磁気抵抗効果素子と、前記一対の磁気抵抗効果素子
間に介挿した中間層と、前記磁気記録媒体の反対側の前
記一対の磁気抵抗効果素子の端部間を接続するリターン
コアとからなる磁気ヘッドにおいて、前記中間層は、導
電性を有した強磁性体又は、反強磁性体からなるように
構成したものである。
SUMMARY OF THE INVENTION In order to solve the above problems, the present invention provides a pair of magnetoresistive elements and a pair of magnetoresistive elements in a running direction of a magnetic recording medium.
An intermediate layer interposed therebetween, and a front side opposite to the magnetic recording medium.
A return connecting between the ends of the pair of magnetoresistive elements
In a magnetic head comprising a core , the intermediate layer is a conductive layer.
It is composed of a ferromagnetic or antiferromagnetic material having electrical conductivity .

【0009】[0009]

【作用】本発明は、以上のように構成したので、磁気記
録媒体の記録を再生する場合には、この記録媒体と、磁
気ヘッドの磁気抵抗効果素子、リターンコアにより磁気
回路が構成される。従って、磁気抵抗効果素子の記録媒
体とは反対側の端部がリターンコアにより接続されてい
るので漏れ磁束が非常に少なくなり、再生効率を大幅に
向上させることができる。
According to the present invention, the magnetic circuit is constituted by the recording medium, the magneto-resistive element of the magnetic head, and the return core when reproducing data from the magnetic recording medium. Therefore, since the end of the magnetoresistive element opposite to the recording medium is connected by the return core, the leakage magnetic flux is extremely reduced, and the reproduction efficiency can be greatly improved.

【0010】特に、記録媒体として記録層の下部に軟磁
性下地層を設けたものを用いた場合には、この軟磁性下
地層が磁気回路の一部を形成することになり、一層、漏
れ磁束を減少させることができるので再生効率を更に向
上させることができる。
In particular, when a recording medium having a soft magnetic underlayer provided below the recording layer is used, this soft magnetic underlayer forms a part of a magnetic circuit, and furthermore, the leakage magnetic flux is increased. Can be reduced, so that the reproduction efficiency can be further improved.

【0011】[0011]

【実施例】以下に、本発明に係る磁気ヘッドの一実施例
を添付図面に基づいて詳述する。図1は本発明に係る磁
気ヘッドを示す概略断面図、図2は図1中のII−II
線矢視断面図、図3は記録媒体の記録層と再生波形との
関係を示す図である。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the magnetic head according to the present invention will be described below in detail with reference to the accompanying drawings. FIG. 1 is a schematic cross-sectional view showing a magnetic head according to the present invention, and FIG. 2 is a II-II in FIG.
FIG. 3 is a diagram showing a relationship between a recording layer of a recording medium and a reproduced waveform.

【0012】図示するようにこの磁気ヘッド1は、一対
の板状の磁気抵抗効果素子2、2を有しており、この一
対の磁気抵抗効果素子2、2は例えば絶縁性材料或いは
磁気抵抗効果素子に対して比較的比抵抗の大きい導電性
材料よりなる中間層3を介して磁気記録媒体4の走行方
向、すなわち図中X方向へサンドイッチ状に積層されて
いる。
As shown in the figure, the magnetic head 1 has a pair of plate-shaped magnetoresistive elements 2, 2, which are made of, for example, an insulating material or a magnetoresistive effect. The elements are sandwiched in the running direction of the magnetic recording medium 4, that is, in the X direction in the drawing, via an intermediate layer 3 made of a conductive material having a relatively large specific resistance to the elements.

【0013】そして、この一対の磁気抵抗効果素子2、
2の、記録媒体4とは反対側の端部間を接続して例えば
Ni−Fe(パーマロイ)、Co−Zr−Nb、Co−
Zr−Ta等の軟磁性体よりなるリターンコア5が設け
られており、これにより一方の磁気抵抗効果素子2、記
録媒体4、他方の磁気抵抗効果素子2及びリターンコア
5を順次通る閉ループよりなる磁気回路を形成してい
る。
The pair of magnetoresistive elements 2,
2 is connected between the opposite ends of the recording medium 4 to form, for example, Ni-Fe (Permalloy), Co-Zr-Nb, Co-
A return core 5 made of a soft magnetic material such as Zr-Ta is provided, thereby forming a closed loop that sequentially passes through one magnetoresistive element 2, the recording medium 4, the other magnetoresistive element 2, and the return core 5. A magnetic circuit is formed.

【0014】そして、記録媒体4の平面方向と平行にな
る方向の磁気抵抗効果素子2、2の両端側には電極6、
6が接続されており、これらの磁気抵抗効果素子2、2
に同方向に向かうバイアス兼センス電流Iを流すように
なっている。このように2つの磁気抵抗効果素子2、2
に同方向のバイアス兼センス電流を流すことにより、そ
れぞれの素子2、2を通るバイアス兼センス電流の作用
により生ずる磁界が相互に反対方向に向かうように各素
子内に形成され、結果的に上記した磁気回路を一方向に
向かうバイアス磁界Hが生じることになる。尚、図1に
おいてバイアス兼センス電流は紙面の垂直方向上方に向
けて流れている。
Electrodes 6 are provided on both ends of the magnetoresistive elements 2, 2 in a direction parallel to the plane of the recording medium 4.
6 are connected to these magnetoresistive elements 2, 2
And a bias / sense current I flowing in the same direction. Thus, the two magnetoresistance effect elements 2, 2
By flowing a bias and sense current in the same direction through the elements, magnetic fields generated by the action of the bias and sense current passing through the respective elements 2 and 2 are formed in the respective elements so as to be directed in mutually opposite directions. A bias magnetic field H is generated in the magnetic circuit in one direction. In FIG. 1, the bias / sense current flows upward in the vertical direction of the drawing.

【0015】この場合、中間層3として導電性材料を用
いた場合には、電極6は、図2に示すように全部で一対
のみ設ければよいが、中間層3として絶縁性材料を用い
た場合には、各磁気抵抗効果素子2、2の両端にそれぞ
れ一対、全部で二対の電極6、6を設けるようにする。
中間層3として導電性材料を用いた場合には、強いバイ
アス磁界を発生させるためのシャント膜として作用させ
ることができる。また、この中間層3としては、導電性
材料の中でも磁気抵抗効果素子2、2と磁気的相互作用
を及ぼす強磁性体或いはFeMn、CoMn等の反強磁
性体を用いることができ、これらを用いることにより磁
気抵抗効果素子の磁壁の動きを抑制でき、バルクハウゼ
ンノイズを低減することができる。
In this case, when a conductive material is used for the intermediate layer 3, only one pair of electrodes 6 may be provided as shown in FIG. 2, but an insulating material is used for the intermediate layer 3. In this case, two pairs of electrodes 6, 6 are provided at both ends of each of the magnetoresistive elements 2, 2, respectively.
When a conductive material is used as the intermediate layer 3, it can function as a shunt film for generating a strong bias magnetic field. Further, as the intermediate layer 3, a ferromagnetic material or an antiferromagnetic material such as FeMn or CoMn, which magnetically interacts with the magnetoresistive elements 2 and 2 among conductive materials, can be used. Thus, the motion of the domain wall of the magnetoresistive element can be suppressed, and Barkhausen noise can be reduced.

【0016】一方、記録媒体4としては、例えば円板状
のガラスやアルミニウム等よりなる非磁性基体7上に垂
直磁気記録用の記録層8を設けた垂直記録方式のディス
ク状の記録媒体4を用いることができ、特に、図示例の
ように非磁性基体7と記録層8との間に軟磁性下地層9
を介在させた記録媒体を用いた場合には、この軟磁性下
地層9が磁気回路の一部を構成するように作用するの
で、漏れ磁束を一層抑制することが可能となる。
[0016] On the other hand, recorded as the medium 4, for example, disc-shaped glass or disc-shaped recording medium of the perpendicular recording system having a recording layer 8 of the perpendicular magnetic recording on the non-magnetic group body 7 made of aluminum or the like 4, a soft magnetic underlayer 9 between the nonmagnetic substrate 7 and the recording layer 8 as shown in FIG.
In the case of using a recording medium in which a soft magnetic underlayer is interposed, the soft magnetic underlayer 9 acts so as to constitute a part of the magnetic circuit, so that it is possible to further suppress the leakage magnetic flux.

【0017】次に、以上のように構成された実施例の作
用について説明する。まず、再生時において電極6、6
を介して一対の磁気抵抗効果素子2、2に同方向(図1
中において紙面の垂直方向上方向)に向かうバイアス兼
センス電流Iを流すことにより、各素子2、2を中心と
して図中反時計方向に向かうバイアス磁界Hがそれぞれ
生じ、結果的に、一対の磁気抵抗効果素子2、2、リタ
ーンコア5及び記録媒体8により形成される閉ループの
磁気回路には図中反時計方向に向かうバイアス磁界が生
じて各素子2、2中には相互に反対方向に向かう磁界が
発生する。
Next, the operation of the embodiment configured as described above will be described. First, during reproduction, the electrodes 6, 6
Through the pair of magnetoresistive elements 2 and 2 in the same direction (FIG. 1).
The bias and sense current I flowing in the direction perpendicular to the plane of the drawing (upward in the drawing) causes a bias magnetic field H that flows in the counterclockwise direction in FIG. In the closed-loop magnetic circuit formed by the resistance effect elements 2 and 2, the return core 5 and the recording medium 8, a bias magnetic field is generated in the counterclockwise direction in the drawing, and the elements 2 and 2 are directed in opposite directions. A magnetic field is generated.

【0018】このような状態で磁気ヘッド1と記録媒体
4を水平方向へ相対移動させることにより、この磁気ヘ
ッド1が記録層8の磁化反転部分を跨いだ時に磁化の変
化方向に応じて上方へ或いは下方へ突状の再生出力が得
られる(図3参照)。尚、記録層8中の矢印は磁化の方
向を示している。
[0018] By relatively moving the magnetic head 1 to the recording medium 4 in the horizontal direction in this state, the upper in accordance with the change direction of magnetization when the magnetic head 1 is straddling the magnetization reversal portion of the serial Rokuso 8 A downward or upward projection output is obtained (see FIG. 3). The arrow in the recording layer 8 indicates the direction of magnetization.

【0019】ここで、磁気抵抗効果素子2、2の記録媒
とは反対側の端部(図1中の上端部)には軟磁性体
よりなるリターンコア5を接合してあるので、磁気抵抗
の少ない強い閉ループを形成することができ、従って、
記録層8から発生した磁束は途中で漏れることが少なく
なり、各磁気抵抗効果素子2、2内の磁束密度Byが大
きくなって効率的に再生することができる。
Here, a return core 5 made of a soft magnetic material is joined to the end (upper end in FIG. 1) of the magnetoresistive elements 2 and 2 on the side opposite to the recording medium 4 , so that the A strong closed loop with low resistance can be formed,
The magnetic flux generated from the recording layer 8 is less likely to leak on the way, and the magnetic flux density By in each of the magnetoresistive elements 2, 2 is increased, so that efficient reproduction can be performed.

【0020】このような漏れ磁束の減少作用はリターン
コア5を設けるだけで大きく発揮でき、従って、記録媒
体4としては軟磁性下地層9を設けた媒体及び設けてい
ない媒体ともに再生効率を向上させることができる。し
かしながら、図1に示すように記録媒体4中に軟磁性下
地層9を設けた場合には、この部分が磁気回路の磁路と
して作用するので一層強い閉ループを形成でき、従っ
て、更に再生効率を向上させることができる。
Such a function of reducing the leakage magnetic flux can be exerted greatly only by providing the return core 5, and therefore, as the recording medium 4, the reproducing efficiency is improved for both the medium provided with the soft magnetic underlayer 9 and the medium not provided. be able to. However, when the soft magnetic underlayer 9 is provided in the recording medium 4 as shown in FIG. 1, this portion functions as a magnetic path of the magnetic circuit, so that a stronger closed loop can be formed, and thus the reproduction efficiency can be further improved. Can be improved.

【0021】また、上述のように漏れ磁束を大幅に少な
くすることができるので、小さなバイアス兼センス電流
Iでも十分な大きさのバイアス磁界を発生させることが
でき、従って、その分、消費電力も減少させることが可
能となる。
Further, since the leakage magnetic flux can be greatly reduced as described above, a sufficiently large bias magnetic field can be generated even with a small bias and sense current I, and accordingly, power consumption is correspondingly reduced. It is possible to reduce it.

【0022】また、中間層3として、絶縁性材料でなく
導電性材料を用いると、この層がバイアス磁界を発生さ
せるためのシャント膜としても作用し、更に強いバイア
ス磁界Hを発生させることができるのみならず、各素子
2、2にバイアス兼センス電流Iを流すための電極6も
一対で済み、この構造を簡単化することができる。
When a conductive material is used for the intermediate layer 3 instead of an insulating material, this layer also functions as a shunt film for generating a bias magnetic field, and can generate a stronger bias magnetic field H. In addition, only one pair of electrodes 6 for flowing the bias and sense current I to each of the elements 2 and 2 is required, and this structure can be simplified.

【0023】更に、この中間層3として、各素子2、2
と磁気的相互作用を及ぼす強磁性体或いは反強磁性体を
用いることにより、磁気抵抗効果素子の磁壁の動きを抑
制することができ、バルクハウゼンノイズも抑制するこ
とができる。
Further, each of the elements 2, 2
By using a ferromagnetic material or an antiferromagnetic material having a magnetic interaction with the magnetic field, the motion of the domain wall of the magnetoresistive element can be suppressed, and Barkhausen noise can also be suppressed.

【0024】次に、本発明の作用効果を確認するため
に、有限要素法による磁界解析によってコンピュータシ
ミュレーションを行なったのでその結果を示す。シミュ
レーションの条件は以下の通りである。
Next, in order to confirm the operation and effect of the present invention, computer simulation was performed by magnetic field analysis using the finite element method, and the results are shown. The simulation conditions are as follows.

【0025】・記録層8:Hc=1500 Oe,Bs
=6500 G,膜厚=0.05μm ・軟磁性下地層9:Bs=12000 G,透磁率μ=
2000,膜厚=0.5μm ・磁気抵抗効果素子2:Bs=9000 G,透磁率μ
=1000,膜厚=0.05μm,高さh=3μm,比
抵抗=1 ・中間層3:膜厚g=0.2μm,比抵抗=5 ・リターンコア5:Bs=12000 G,透磁率μ=
1000 ・スペーシングd:0.05μm ・バイアス兼センス電流I:40mA(バイアス磁界H
の算出時のみ) ・要素分割数:1000〜3000
Recording layer 8: Hc = 1500 Oe, Bs
= 6500 G, thickness = 0.05 μm Soft magnetic underlayer 9: Bs = 12000 G, permeability μ =
2000, film thickness = 0.5 μm ・ Magnetoresistance effect element 2: Bs = 9000 G, permeability μ
= 1000, film thickness = 0.05 μm, height h = 3 μm, specific resistance = 1 ・ Intermediate layer 3: film thickness g = 0.2 μm, specific resistance = 5 ・ Return core 5: Bs = 12000 G, magnetic permeability μ =
1000 Spacing d: 0.05 μm Bias / sense current I: 40 mA (bias magnetic field H
(Only when calculating) ・ Number of element divisions: 1000 to 3000

【0026】まず、再生効率のシミュレーション結果に
ついて述べる。図4はリターンコア及び軟磁性下地層の
有無に対する再生効率の記録密度特性を示すグラフであ
る。再生特性は両磁気抵抗効果素子2、2の、記録媒体
4からの磁束による素子内部のy方向の磁束密度Byを
高さ方向に積分した値:∫Bydyの差:Δ∫Bydy
で定義した。図中、曲線Aは軟磁性下地層及びリターン
コアともに設けない場合、曲線Bは軟磁性下地層は設け
てリターンコアは設けない場合、曲線Cは軟磁性下地層
及びリターンコアともに設けた場合をそれぞれ示す。
First, the simulation results of the regeneration efficiency will be described. FIG. 4 is a graph showing the recording density characteristics of the reproduction efficiency with respect to the presence or absence of the return core and the soft magnetic underlayer. The reproduction characteristic is a value obtained by integrating in the height direction the magnetic flux density By in the y direction of the inside of the magnetoresistive elements 2 and 2 due to the magnetic flux from the recording medium 4: difference of ∫Bydy: Δ∫Bydy.
Defined. In the figure, curve A represents the case where neither the soft magnetic underlayer nor the return core is provided, curve B represents the case where the soft magnetic underlayer is provided and no return core is provided, and curve C represents the case where both the soft magnetic underlayer and the return core are provided. Shown respectively.

【0027】このグラフから明らかなように、軟磁性下
地層9を設けた記録媒体を用いることにって再生効
率をある程度まで改善することができるが(曲線A、B
参照)、リターンコアを設けることにより磁気回路の強
い閉ループを形成でき、再生効率を大幅に改善できるこ
とが判明する(曲線C参照)。
[0027] This graph as is clear from, it is possible to improve the regeneration efficiency I by the the use of the recording medium 4 having a soft magnetic underlayer 9 to some extent (curve A, B
It is found that the provision of the return core can form a strong closed loop of the magnetic circuit, thereby greatly improving the reproduction efficiency (see curve C).

【0028】図5はリターンコアを設けなかった場合の
軟磁性下地層の透磁率μと再生効率との関係を示すグラ
フである。このグラフから明らかなように、軟磁性下地
の透磁率μは約10以上あれば再生効率に十分な効
果を発揮することができ、従って、本実施例の磁気ヘッ
を使用する時には下地層の透磁率μが約10以上の
記録媒体を組み合わせることにより、その再生効率を格
段に向上させることができる。また、磁気抵抗効果素子
2、2に設けるリターンコア5も上記下地層と同様な作
用を生ずるので、その透磁率μも約10以上に設定する
のが好ましい。尚、リターンコア5及び軟磁性下地層9
の膜厚は、磁気ヘッド全体の寸法、スペーシングd、垂
直記録層の膜厚等から判断して十分に厚くすればよい。
FIG. 5 is a graph showing the relationship between the magnetic permeability μ of the soft magnetic underlayer and the reproduction efficiency when no return core is provided. As is apparent from this graph, if the permeability μ is about 10 or more of the soft magnetic underlayer 9 can exhibit a sufficient effect on the regeneration efficiency, therefore, lower when using the magnetic head 1 of this embodiment By combining a recording medium having a magnetic permeability μ of the underlayer of about 10 or more, the reproduction efficiency can be remarkably improved. Also, since the return core 5 provided on the magnetoresistive elements 2 and 2 has the same effect as the underlayer, its magnetic permeability μ is preferably set to about 10 or more. The return core 5 and the soft magnetic underlayer 9
The film thickness may be made sufficiently large by judging from the dimensions of the entire magnetic head, spacing d, film thickness of the perpendicular recording layer, and the like.

【0029】次に、最適バイアス兼センス電流値Iopt
を検討するためにバイアス電界のシミュレーション結果
について述べる。表1は、軟磁性下地層及びリターンコ
アの有無を適宜組み合わせた時の、素子全体に流す最適
バイアス兼センス電流値Iopt を示したものである。I
opt は磁気抵抗効果素子中心における垂直バイアス磁界
Hyが、磁気抵抗効果素子の異方性磁界Hkの1/2で
ある800A/mになる電流として定義した。また、表
1中のRは磁気抵抗効果素子に対する中間層の比抵抗で
あり、∞は中間層が絶縁体であることを意味する。
Next, the optimum bias and sense current value I opt
The simulation results of the bias electric field will be described in order to study. Table 1 shows the optimum bias and sense current value I opt flowing through the entire device when the presence or absence of the soft magnetic underlayer and the return core are appropriately combined. I
opt is defined as a current at which the vertical bias magnetic field Hy at the center of the magnetoresistive element becomes 800 A / m, which is の of the anisotropic magnetic field Hk of the magnetoresistive element. Further, R in Table 1 is the specific resistance of the intermediate layer with respect to the magnetoresistive element, and ∞ means that the intermediate layer is an insulator.

【0030】[0030]

【表1】 [Table 1]

【0031】表1より明らかに、リターンコア5を設け
ることにより、軟磁性下地層9の有無に係わらず、電流
値Iopt を非常に小さくすることができ、少ない電流で
十分な大きさのバイアス磁界を得られることが判明し
た。特に、軟磁性下地層を有する記録媒体を組み合
わせることにより、大幅に電流値を小さくできることが
判明した。
It is apparent from Table 1 that the provision of the return core 5 makes it possible to make the current value I opt extremely small irrespective of the presence or absence of the soft magnetic underlayer 9. It was found that a magnetic field could be obtained. In particular, it has been found that the current value can be significantly reduced by combining the recording medium 4 having the soft magnetic underlayer 9 .

【0032】また、一対の磁気抵抗効果素子間に介在さ
せる中間層の材料として、比抵抗値が磁気抵抗効果素子
の5倍程度の導電性材料を用いると、バイアス電界を発
生させるためのシャント膜としても作用させることがで
きるので、より電流値Ioptを低下させて、効率を改善
することができる。尚、上記シャント膜としての作用を
十分に発揮させるためには比抵抗の値はMR特性と膜厚
等によって適宜定められる。
When a conductive material having a specific resistance of about five times that of the magnetoresistive element is used as a material of the intermediate layer interposed between the pair of magnetoresistive elements, a shunt film for generating a bias electric field is used. Therefore, the current value I opt can be further reduced, and the efficiency can be improved. In order to sufficiently exhibit the function as the shunt film, the value of the specific resistance is appropriately determined depending on the MR characteristics, the film thickness, and the like.

【0033】[0033]

【発明の効果】以上説明したように、本発明の磁気ヘッ
ドによれば次のように優れた作用効果を発揮することが
できる。一対の磁気抵抗効果素子の一端部をリターンコ
アにより接続するようにしたので強い閉ループの磁気回
路を形成でき、従って、漏れ磁束を大幅に減少させるこ
とができるので再生効率を大幅に向上させることができ
る。また、上述のように漏れ磁束を少なくできることか
ら必要なバイアス磁界を発生させるための電流も少なく
て済み、その分、消費電力を削減することができる。
に、中間層に強磁性体や反強磁性体を用いることによ
り、磁気抵抗効果素子の磁壁の動きを抑制することがで
き、バルクハウゼンノイズを抑制できるので、磁気ヘッ
ドのS/N比を向上させることができる。
As described above, according to the magnetic head of the present invention, the following excellent functions and effects can be exhibited. Since one end of the pair of magnetoresistive elements is connected by a return core, a strong closed-loop magnetic circuit can be formed. Therefore, the leakage magnetic flux can be greatly reduced, thereby greatly improving the reproduction efficiency. it can. Further, since the leakage magnetic flux can be reduced as described above, the current for generating the necessary bias magnetic field can be reduced, and the power consumption can be reduced accordingly. Change
The use of a ferromagnetic or antiferromagnetic material for the intermediate layer
The movement of the domain wall of the magnetoresistive effect element can be suppressed.
The magnetic head, since Barkhausen noise can be suppressed.
The S / N ratio of the gate can be improved.

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

【図1】本発明に係る磁気ヘッドを示す概略断面図であ
る。
FIG. 1 is a schematic sectional view showing a magnetic head according to the present invention.

【図2】図1中のII−II線矢視断面図である。FIG. 2 is a sectional view taken along line II-II in FIG.

【図3】記録媒体の記録層と再生波形との関係を示す図
である。
FIG. 3 is a diagram showing a relationship between a recording layer of a recording medium and a reproduced waveform.

【図4】リターンコア及び軟磁性下地層の有無に対する
再生効率の記録密度に対する再生効率の記録密度特性を
示すグラフである。
FIG. 4 is a graph showing a recording density characteristic of a reproduction efficiency with respect to a recording density of a reproduction efficiency with or without a return core and a soft magnetic underlayer.

【図5】リターンコアを設けなかった場合の軟磁性下地
層の透磁率と再生効率との関係を示すグラフである。
FIG. 5 is a graph showing the relationship between the magnetic permeability of the soft magnetic underlayer and the reproduction efficiency when no return core is provided.

【符号の説明】[Explanation of symbols]

1…磁気ヘッド、2…磁気抵抗効果素子、3…中間層、
4…磁気記録媒体、5…リターンコア、6…電極、7…
非磁性基体、8…記録層、9…軟磁性下地層。
DESCRIPTION OF SYMBOLS 1 ... Magnetic head, 2 ... Magnetoresistance effect element, 3 ... Intermediate layer,
4 ... magnetic recording medium, 5 ... return core, 6 ... electrode, 7 ...
Nonmagnetic substrate, 8: recording layer, 9: soft magnetic underlayer.

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭50−129007(JP,A) 特公 昭63−29327(JP,B2) (58)調査した分野(Int.Cl.6,DB名) G11B 5/39 ──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-50-129007 (JP, A) JP-B-63-29327 (JP, B2) (58) Fields investigated (Int. Cl. 6 , DB name) G11B 5/39

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 磁気記録媒体の走行方向に対して、一対
の磁気抵抗効果素子と、前記一対の磁気抵抗効果素子間
に介挿した中間層と、前記磁気記録媒体の反対側の前記
一対の磁気抵抗効果素子の端部間を接続するリターンコ
アとからなる磁気ヘッドにおいて、前記中間層は、導電
性を有した強磁性体又は、反強磁性体からなることを特
徴とする磁気ヘッド。
1. A pair of magnetoresistive elements, between a pair of magnetoresistive elements in a running direction of a magnetic recording medium.
And an intermediate layer interposed in the magnetic recording medium.
A return cable that connects between the ends of a pair of magnetoresistive elements
In the magnetic head comprising:
A magnetic head comprising a ferromagnetic or antiferromagnetic material having properties .
JP6189106A 1994-06-06 1994-06-06 Magnetic head Expired - Lifetime JP2979966B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6189106A JP2979966B2 (en) 1994-06-06 1994-06-06 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6189106A JP2979966B2 (en) 1994-06-06 1994-06-06 Magnetic head

Publications (2)

Publication Number Publication Date
JPH07334820A JPH07334820A (en) 1995-12-22
JP2979966B2 true JP2979966B2 (en) 1999-11-22

Family

ID=16235472

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6189106A Expired - Lifetime JP2979966B2 (en) 1994-06-06 1994-06-06 Magnetic head

Country Status (1)

Country Link
JP (1) JP2979966B2 (en)

Also Published As

Publication number Publication date
JPH07334820A (en) 1995-12-22

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