JPS59207675A - Magnetoresistance element - Google Patents

Magnetoresistance element

Info

Publication number
JPS59207675A
JPS59207675A JP58080894A JP8089483A JPS59207675A JP S59207675 A JPS59207675 A JP S59207675A JP 58080894 A JP58080894 A JP 58080894A JP 8089483 A JP8089483 A JP 8089483A JP S59207675 A JPS59207675 A JP S59207675A
Authority
JP
Japan
Prior art keywords
film
magnetic field
permanent magnet
bias
permalloy
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
JP58080894A
Other languages
Japanese (ja)
Inventor
Masahiro Kitada
北田 正弘
Hideo Tanabe
英男 田辺
Noboru Shimizu
昇 清水
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP58080894A priority Critical patent/JPS59207675A/en
Publication of JPS59207675A publication Critical patent/JPS59207675A/en
Pending legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N50/00Galvanomagnetic devices
    • H10N50/10Magnetoresistive devices

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  • Magnetic Heads (AREA)
  • Hall/Mr Elements (AREA)

Abstract

PURPOSE:To make the intensity of a bias magnetic field sufficiently intense, by using a Permalloy film and a thin permanent magnet film as a multilayer shunt film in applying the bias magnetic field intensity. CONSTITUTION:On a substrate 1, a Permalloy film 2 comprising, e.g., Fe-82% Ni, is formed. Then, a Co-20%Pt alloy film 3, which is a permanent magnet film, is formed on the Permalloy film 2. Thereafter, an electrode 4 for conducting a current through said two-layer thin film is formed by Al, Au, or the like. The bias intensity is increased from a curve 6, which indicates the bias intensity caused by the magnetic field formed only by a current, by the amount of the permanent magnetic field, owing to the overlapped magnetic field of the magnetic field formed by the current and the magnetic field formed by the permanent magnet.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明はバイアス磁界を印加した磁気抵抗効果型素子に
関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a magnetoresistive element to which a bias magnetic field is applied.

〔発明の背景〕[Background of the invention]

磁気ディスク、磁気テープ装置などの再生用磁気ヘッド
として使用する磁気抵抗効果型ヘッドでは、再生出力を
大きくするなどのため、磁気抵抗効果膜に適当なバイア
ス磁界を印加することが行なわれている。バイアス磁界
印加法については各種の方法が提案されているが、一長
一短があシ、実用化するためには、なお改良が必要であ
る。   −〔発明の目的〕 本発明は充分なバイアス磁界が印加され且つノイズも少
ない磁気抵抗効果素子の提供を目的とするものである。
In magnetoresistive heads used as reproduction magnetic heads for magnetic disks, magnetic tape devices, etc., an appropriate bias magnetic field is applied to the magnetoresistive film in order to increase the reproduction output. Various methods have been proposed for applying a bias magnetic field, but each has its own merits and demerits, and further improvements are needed to put them into practical use. - [Object of the Invention] The object of the present invention is to provide a magnetoresistive element to which a sufficient bias magnetic field can be applied and which has little noise.

〔発明の概要〕[Summary of the invention]

本発明は磁気抵抗膜(パーマロイ膜)と電気的に接触す
るように多層膜として電流バイアス線を設置したことを
特徴とするシャントバイアス型磁気抵抗効果型素子に於
て、通常シャント膜として使用されるTi々どの非磁性
金属ではなく、永久磁石特性を有する薄膜としたことを
特徴とする。
The present invention relates to a shunt bias type magnetoresistive element characterized in that a current bias line is installed as a multilayer film so as to be in electrical contact with a magnetoresistive film (permalloy film), which is normally used as a shunt film. It is characterized by being made of a thin film that has permanent magnetic properties, rather than being made of non-magnetic metals such as Ti.

本構造は永久磁石膜にも電流を通じせしめて電流のつく
る磁界でパーマロイ膜にバイアス磁界を印加すると同時
に、永久磁石膜による磁界によってもバイアス磁界を印
加せしめるものである。この方法によって、従来非磁性
金属からなるシャントバイアス印加磁場では不十分であ
った磁界強度が、永久磁石膜を用いることによって十分
なバイアス磁場が得られるようになった。また、永久磁
石膜の着磁力向を適当に調整することにより、パーマロ
イ膜の単磁区化が促され、磁壁移動に基づくバルクハウ
ゼンノイズの低減に顕著な効果がある。
In this structure, a current is passed through the permanent magnet film, and the magnetic field generated by the current applies a bias magnetic field to the permalloy film, and at the same time, a bias magnetic field is also applied by the magnetic field generated by the permanent magnet film. With this method, a magnetic field strength that was insufficient in the conventional shunt bias applied magnetic field made of non-magnetic metal can now be obtained by using a permanent magnet film. Furthermore, by appropriately adjusting the direction of the magnetizing force of the permanent magnet film, the formation of a single magnetic domain in the permalloy film is promoted, which has a remarkable effect on reducing Barkhausen noise caused by domain wall movement.

本発明の効果を以下の実施例によって詳しく説明する。The effects of the present invention will be explained in detail with reference to the following examples.

〔発明の実施例および効果〕[Embodiments and effects of the invention]

実施例1 第1図は本発明による磁気抵抗効果素子の断面構造を示
したもので、ガラス等の所望の基板1上にpe−82%
Njからなるパーマロイ膜2を形成し、次にパーマロイ
上に永久磁石膜であるC0−20%Pt3を形成する。
Example 1 FIG. 1 shows the cross-sectional structure of a magnetoresistive element according to the present invention.
A permalloy film 2 made of Nj is formed, and then a C0-20% Pt3 film, which is a permanent magnet film, is formed on the permalloy.

次に、当該2層薄膜に電流を通ずるための電極4をkt
あるいはAU等で形成する。これによって、磁気抵抗効
果を示すパーマロイ膜とシャント電流用永久磁石膜であ
るCo−20%Pt膜を備えた磁気抵抗効果素子が作製
される。第2図は当該素子の出力−電圧特性で、曲線5
は永久磁石薄膜3を通電方向(パーマロイ膜の磁化容易
方向)と垂直に着磁した場合で、電流によって形成され
た磁界と永久磁石による磁界との重畳磁界により、電流
だけで形成された磁界によるバイアス強度を示す曲線6
より永久磁石膜の分だけバイアス強度で増大する。曲線
6は永久磁石膜の着磁力向を電流の方向と平行にして、
実効的に永久磁石膜からのバイアス磁界が印加されない
ようにしたものである。永久磁石の着磁の角度(パーマ
ロイ膜の磁化容易軸と着磁方向の角度に等しい)を第2
図5.6で示す曲線の中間の状態で行なうと、7の曲線
が得られる。また、第3図8で示すパーマロイ膜の容易
磁化方向9に対してバイアス磁界を印加する方向10を
9の方向との角度として60° 以下にすると、磁気抵
抗効果素子の出力電圧−磁場特性にみられるバルクハウ
ゼンノイズが著しく低減する。第4図に第3図で示した
9と10の角度αとバルクハウゼンノイズとの関係曲線
を示した。これはパーマロイ膜の単磁区化などに関係が
あるものとみられる。本素子の以上のような特性を発揮
させるためには、永久磁石膜兼シャント電流膜であるc
o−ptとの間の反応による両者の特性劣化を防止しな
ければならない。このためには、第1図で示したパーマ
ロイ膜2の上にco−pt膜を形成する際、基板温度が
250C以上にならないように基板を十分に冷却しなけ
ればならない。250C以上になると両者の反応によシ
第2図で示すような特性が得られない。
Next, the electrode 4 for passing current through the two-layer thin film is kt
Alternatively, it is formed using AU or the like. As a result, a magnetoresistive element including a permalloy film exhibiting a magnetoresistive effect and a Co-20% Pt film serving as a shunt current permanent magnet film is manufactured. Figure 2 shows the output-voltage characteristics of the device, with curve 5
is the case when the permanent magnet thin film 3 is magnetized perpendicular to the current direction (the permalloy film's easy magnetization direction). Curve 6 showing bias strength
The bias strength increases by the amount of the permanent magnet film. Curve 6 is obtained by setting the direction of the magnetizing force of the permanent magnet film parallel to the direction of the current,
This effectively prevents the bias magnetic field from being applied from the permanent magnet film. The angle of magnetization of the permanent magnet (equal to the angle between the easy axis of magnetization of the permalloy film and the direction of magnetization) is set as the second
If this is done in the middle state of the curve shown in Figure 5.6, a curve 7 will be obtained. Furthermore, if the direction 10 in which the bias magnetic field is applied to the easy magnetization direction 9 of the permalloy film shown in FIG. The visible Barkhausen noise is significantly reduced. FIG. 4 shows a relationship curve between angles α of 9 and 10 shown in FIG. 3 and Barkhausen noise. This seems to be related to the formation of a single magnetic domain in the permalloy film. In order to exhibit the above-mentioned characteristics of this device, it is necessary to use c, which is a permanent magnet film and shunt current film.
It is necessary to prevent the deterioration of the characteristics of both due to the reaction with the o-pt. For this purpose, when forming a co-pt film on the permalloy film 2 shown in FIG. 1, the substrate must be sufficiently cooled so that the substrate temperature does not exceed 250C. If the temperature exceeds 250C, the characteristics shown in FIG. 2 cannot be obtained due to the reaction between the two.

以上の実施例から明らかなように、本発明の効果は非常
に大きい。
As is clear from the above examples, the effects of the present invention are very large.

つぎに上記発明に関連した第2の発明を説明する。まず
、本第2の発明の実施態様を示すと、パーマロイ等の所
望の磁気抵抗効果膜を用いた磁気抵抗効果型感磁素子に
おいて、当該磁気抵抗効果膜と多層構造になるように金
属からなるシャント薄膜を形成して磁気抵抗効果膜にバ
イアス磁界を印加する素子構造で、シャント膜の一部と
して永久磁石膜を用い、かつ永久磁石膜とパーマロイの
間の拡散反応を防止し、シャント膜の一部となる高融点
金属膜を設けたことを特徴とする磁気抵抗効果型素子で
ある。
Next, a second invention related to the above invention will be explained. First, to describe an embodiment of the second invention, in a magnetoresistive magnetosensitive element using a desired magnetoresistive film such as permalloy, the element is made of metal so as to form a multilayer structure with the magnetoresistive film. This element structure forms a shunt thin film and applies a bias magnetic field to the magnetoresistive film.It uses a permanent magnet film as part of the shunt film, and prevents the diffusion reaction between the permanent magnet film and permalloy. This is a magnetoresistive element characterized by having a high melting point metal film as a part of the element.

磁気ディスク、磁気テープ装置などの再生用磁気ヘッド
として使用される磁気抵抗効果型ヘッドでは、再生出力
を大きくするなどのために磁気抵抗効果薄膜に適当なバ
イアス磁界を印加することが行なわれている。バイアス
磁界の印加法には永久磁石膜を設置する方法、バーバー
ポール電極形成法、反強磁性膜による方法、電流バイア
ス線による方法、磁気抵抗効果膜を互いに平行に設置し
て相互にバイアスを印加する方法、などが開発されてい
る。これらの方法には一長一短がアシ、実用化するため
には、なお改良が必要でおる。
In magnetoresistive heads used as reproduction magnetic heads for magnetic disks, magnetic tape devices, etc., an appropriate bias magnetic field is applied to the magnetoresistive thin film in order to increase the reproduction output. . Methods for applying a bias magnetic field include installing a permanent magnet film, barber pole electrode formation method, antiferromagnetic film method, current bias wire method, and magnetoresistive films are installed parallel to each other and bias is applied to each other. A method to do this has been developed. These methods have their advantages and disadvantages, and further improvements are required before they can be put into practical use.

本第2の発明は磁気抵抗膜と電気的に接触するように多
層膜として電流バイアス線を設置したことを特徴とする
シャントバイアス型磁気抵抗効果素子の改善に関わるも
ので、本第2の発明に於てはシャントバイアス膜の一部
に永久磁石特性を有する金属薄膜を用いることによシ、
通電電流のつくる磁場に永久磁石薄膜からの磁場を重畳
させて、効果的に磁気抵抗薄膜にバイアス磁界を印加し
たことを特徴とする磁気抵抗効果型薄膜素子でめる。
The second invention relates to the improvement of a shunt bias type magnetoresistive element characterized in that a current bias line is provided as a multilayer film so as to be in electrical contact with a magnetoresistive film. In this case, by using a thin metal film with permanent magnetic properties as part of the shunt bias film,
A magnetoresistive thin film element characterized in that a bias magnetic field is effectively applied to a magnetoresistive thin film by superimposing the magnetic field from a permanent magnet thin film on the magnetic field created by a current.

これによって、永久磁石薄膜も含めたシャント薄膜に印
加するために要する通電電流密度が減少し、シャント薄
膜の通電破断寿命が伸び、素子の信頼性が向上するとと
もに、永久磁石薄膜の磁化方向を調整することにより、
磁気抵抗膜に発生するバルクハウゼンノイズなどの低減
効果もある。しかし、通常Co−pt、co−Beなど
の金属性永久磁石膜とパーマロイ膜を直接2層にすると
、素子プロセス温度が200〜300C以上になると接
触界面で両者の反応が起こり、特に軟磁気拐料であるパ
ーマロイ膜の特性が劣化する。このため、パーマロイ膜
と上記永久磁石膜との間に両者と反応しないバリヤ層を
形成すると特性劣化の少ない磁気抵抗素子の作製が可能
となる。以上のごとく、本第2の発明は永久磁石薄膜を
シャントバイアス膜に使用するとき、パーマロイ膜との
間にバリヤ層を形成し、以上の3層からなることを特徴
とする磁気抵抗素子である。以下本紀2の発明を実施例
によシ詳細を述べる。
This reduces the current density required to be applied to the shunt thin film, including the permanent magnet thin film, extends the current rupture life of the shunt thin film, improves the reliability of the device, and adjusts the magnetization direction of the permanent magnet thin film. By doing so,
It also has the effect of reducing Barkhausen noise generated in the magnetoresistive film. However, when a permanent magnetic film made of a metal such as Co-pt or co-Be and a permalloy film are directly formed into two layers, a reaction occurs between the two at the contact interface when the device process temperature exceeds 200 to 300C. The properties of the permalloy film, which is the raw material, deteriorate. Therefore, by forming a barrier layer between the permalloy film and the permanent magnet film that does not react with both, it becomes possible to manufacture a magnetoresistive element with less deterioration of characteristics. As described above, the second invention is a magnetoresistive element characterized in that when a permanent magnet thin film is used as a shunt bias film, a barrier layer is formed between the permanent magnet thin film and the permalloy film, and is composed of the above three layers. . The invention of this document 2 will be described in detail below using examples.

実施例2 第5図は本第2の発明による磁気抵抗効果素子の実施例
を示す素子の断面図で、ガラス等の所望の基板11上に
Fe−82%Ni組成からなるパーマロイ膜12を形成
し、次にパーマロイの上に永久磁石膜であるCo−20
%pt膜14とパーマロイ膜の相互拡散を防ぎ、かつこ
の膜自体が電流バイアス磁場を生成するためのMO薄膜
13を形成し、これに通電に必要な電極15を形成した
ものである。第6図は当該素子の出力電圧−磁場特性で
、曲線16は永久磁石薄膜14を通電方向と垂直に着磁
した場合で、電流によって形成された磁界と永久磁石に
よる磁界とによって、電流だけの磁界によるバイアス強
度を示す曲線17よシ永久磁石膜の分だけバイアス強度
が増大している。
Example 2 FIG. 5 is a cross-sectional view of an element showing an example of the magnetoresistive element according to the second invention, in which a permalloy film 12 having a Fe-82% Ni composition is formed on a desired substrate 11 such as glass. Next, a permanent magnetic film of Co-20 is placed on the permalloy.
An MO thin film 13 is formed to prevent mutual diffusion between the %pt film 14 and the permalloy film, and this film itself generates a current bias magnetic field, and an electrode 15 necessary for current conduction is formed thereon. FIG. 6 shows the output voltage-magnetic field characteristics of the device. Curve 16 shows the case where the permanent magnet thin film 14 is magnetized perpendicular to the direction of current flow. According to curve 17 showing the bias strength due to the magnetic field, the bias strength increases by the amount of the permanent magnet film.

曲線17は永久磁石膜の着磁を電流の方向と平行にして
、実効的に永久磁石膜からのバイアス磁界が印加されな
いようにしたものである。永久磁石の着磁の角度(パー
マロイ膜の磁化容易軸と着磁方向の角度に等しい)を第
6図16.17で示す曲線の中間の状態で着磁を行なう
と、18の曲線で示すような曲1116.17の中間の
バイアス磁界強度を示す素子が得られる。したがって、
永久磁石膜の役割によシ、電流バイアス単独でバイアス
強度を印加するよりも、よシ大きなバイアス磁界強度が
得られる。また、第7図19で示すパーマロイ膜の容易
磁化方向20に対してバイアス磁界を印加する方向21
を20の方向との角度として60°以下にすると、磁気
抵抗効果素子の出力電力−磁場特性にみられるバルクハ
ウゼンノイズが著しく低減する。第8図に第7図で示し
た20と21の角度α(着磁角度)とバルクハウゼンノ
イズとの関係曲線22を示したが、着磁角度αが60°
以下になるとノイズが著しい減少を示す。
Curve 17 indicates that the permanent magnet film is magnetized parallel to the direction of the current so that no bias magnetic field is effectively applied from the permanent magnet film. When the permanent magnet is magnetized with the angle of magnetization (equal to the angle between the axis of easy magnetization and the magnetization direction of the permalloy film) in the middle of the curve shown in Figure 6, 16.17, it will be as shown in curve 18. An element exhibiting a bias magnetic field strength between the curves 1116 and 17 is obtained. therefore,
Due to the role of the permanent magnet film, a larger bias magnetic field strength can be obtained than when bias strength is applied solely by current bias. Further, the direction 21 in which a bias magnetic field is applied to the easy magnetization direction 20 of the permalloy film shown in FIG.
When the angle with respect to the direction of 20 is set to 60 degrees or less, Barkhausen noise observed in the output power-magnetic field characteristics of the magnetoresistive element is significantly reduced. Fig. 8 shows a relationship curve 22 between the angle α (magnetization angle) of 20 and 21 shown in Fig. 7 and Barkhausen noise, where the magnetization angle α is 60°.
Below, the noise shows a significant reduction.

これはパーマロイ膜の単磁区化などと関係があるものと
みられる。
This seems to be related to the single magnetic domain of the permalloy film.

したがって、本第2の発明の方法によりバイアス磁界強
度の増大と素子ノイズの低減が実現できた。
Therefore, by the method of the second invention, it was possible to increase the bias magnetic field strength and reduce device noise.

本素子を400Cで3〜5時間熱処理してもMOバリヤ
層の反応阻止効果のため、特性は熱処(9) 理前と変化なかった。
Even when this element was heat-treated at 400C for 3 to 5 hours, the characteristics did not change from those before heat treatment (9) due to the reaction inhibiting effect of the MO barrier layer.

実施例3 実施例2と同様の基板11の上にco−pt永久磁石膜
14を形成し、次にco−pt膜の永久磁石膜の反応を
防止するための高融点金属のMo2Bを被着し、次にパ
ーマロイ膜12、これに通電するための電極15を形成
した素子の第6図で示したものと同様の特性を測定した
ところ、全く同じ効果を示す素子が得られた。
Example 3 A co-pt permanent magnet film 14 is formed on the same substrate 11 as in Example 2, and then Mo2B, a high melting point metal, is deposited to prevent the reaction of the permanent magnet film of the co-pt film. Next, when characteristics similar to those shown in FIG. 6 were measured for an element in which a permalloy film 12 and an electrode 15 for conducting current were formed thereon, an element exhibiting exactly the same effect was obtained.

実施例4 実施例2,3と同様の構造の素子に於て、13で示した
反応阻止金属をTaとした場合も同じ効果が得られた。
Example 4 In an element having the same structure as Examples 2 and 3, the same effect was obtained when Ta was used as the reaction inhibiting metal shown in 13.

実施例5 実施例2.3と同様の構造の素子に於て、14で示した
永久磁石膜をCo−10%Reとした場合も同様の効果
が得られた。
Example 5 In an element having the same structure as in Example 2.3, the same effect was obtained when the permanent magnet film shown in 14 was made of Co-10%Re.

以上の実施例から本第2の発明の効果は明らかである。The effects of the second invention are clear from the above examples.

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

(10) 第1図は本発明の素子の構造を示す断面図、第2図は該
素子の出力電圧−磁場特性を示すグラフ、第3図は永久
磁石膜への着磁の方向を示す斜視図、第4図は素子のバ
ルクハウゼンノイズを示スクラフ、第5図は本第2の発
明の磁気抵抗効果素子の断面構造を示す図、第6図は本
第2の発明素子の電圧−磁場特性を示すグラフ、第7図
は本第2の発明素子の電流方向と永久磁石への着磁の方
向とのなす角度を示す図、第8図は着磁角度とノイズの
発生率を示すグラフ、第9図は第5図で示した素子の構
造の積層膜の順序を変えた素子を示す断面図である。 1・・・基板、2・・・パーマロイ膜、3・・・co−
pt合(11) 第1 図 9 呆 2 図 χ 3 図 n ¥:14 図 θ   3I!760  2j
(10) Fig. 1 is a cross-sectional view showing the structure of the element of the present invention, Fig. 2 is a graph showing the output voltage-magnetic field characteristics of the element, and Fig. 3 is a perspective view showing the direction of magnetization of the permanent magnet film. 4 is a graph showing the Barkhausen noise of the device, FIG. 5 is a diagram showing the cross-sectional structure of the magnetoresistive element of the second invention, and FIG. 6 is a voltage-magnetic field diagram of the device of the second invention. A graph showing the characteristics, FIG. 7 is a graph showing the angle between the current direction of the second invention element and the direction of magnetization of the permanent magnet, and FIG. 8 is a graph showing the magnetization angle and noise generation rate. , FIG. 9 is a sectional view showing an element in which the order of the laminated films of the element structure shown in FIG. 5 is changed. DESCRIPTION OF SYMBOLS 1...Substrate, 2...Permalloy film, 3...co-
pt combination (11) 1st figure 9 dumb 2 figure χ 3 figure n ¥:14 figure θ 3I! 760 2j

Claims (1)

【特許請求の範囲】[Claims] パーマロイ等の所望の磁気抵抗効果膜を用いた磁気抵抗
効果型素子に於て、当該磁気抵抗効果素子にバイアス磁
界強度を印加するのにパーマロイ膜と多層にしてシャン
ト電流膜を形成する構造の素子で、シャント膜として永
久磁石薄膜を使用したことを特徴とする磁気抵抗素子。
In a magnetoresistive element using a desired magnetoresistive film such as permalloy, an element having a structure in which a shunt current film is formed by forming a multilayer with a permalloy film in order to apply a bias magnetic field intensity to the magnetoresistive element. A magnetoresistive element characterized by using a permanent magnet thin film as a shunt film.
JP58080894A 1983-05-11 1983-05-11 Magnetoresistance element Pending JPS59207675A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58080894A JPS59207675A (en) 1983-05-11 1983-05-11 Magnetoresistance element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58080894A JPS59207675A (en) 1983-05-11 1983-05-11 Magnetoresistance element

Publications (1)

Publication Number Publication Date
JPS59207675A true JPS59207675A (en) 1984-11-24

Family

ID=13731065

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58080894A Pending JPS59207675A (en) 1983-05-11 1983-05-11 Magnetoresistance element

Country Status (1)

Country Link
JP (1) JPS59207675A (en)

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