JPH048847B2 - - Google Patents

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Publication number
JPH048847B2
JPH048847B2 JP16086283A JP16086283A JPH048847B2 JP H048847 B2 JPH048847 B2 JP H048847B2 JP 16086283 A JP16086283 A JP 16086283A JP 16086283 A JP16086283 A JP 16086283A JP H048847 B2 JPH048847 B2 JP H048847B2
Authority
JP
Japan
Prior art keywords
layer
magnetic
magnetoresistive
thin film
recording medium
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
Application number
JP16086283A
Other languages
Japanese (ja)
Other versions
JPS6050712A (en
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 filed Critical
Priority to JP16086283A priority Critical patent/JPS6050712A/en
Publication of JPS6050712A publication Critical patent/JPS6050712A/en
Publication of JPH048847B2 publication Critical patent/JPH048847B2/ja
Granted legal-status Critical Current

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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
    • G11B5/33Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only
    • G11B5/39Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects
    • G11B5/3903Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects using magnetic thin film layers or their effects, the films being part of integrated structures

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

Description

【発明の詳細な説明】 (イ) 産業上の利用分野 本発明は、短波長で磁気記録された信号を再生
するのに適した磁気抵抗効果型薄膜磁気ヘツドに
関するものである。
DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application The present invention relates to a magnetoresistive thin film magnetic head suitable for reproducing signals magnetically recorded at short wavelengths.

(ロ) 従来技術 一般に、磁気抵抗効果型薄膜磁気ヘツドの短波
長再生特性を向上させるためには、磁気的シール
ド層の間隙(例えば、1μm程度)に磁気抵抗効
果素子層を配置して隣接信号の影響を小さくする
ことや、強いバイアス磁界(例えば、200Oe程
度)の下で磁気抵抗効果素子層の記録媒体摺動面
近傍のみに感度を持たせ、実効的スペーシングロ
スを減少させることが有効である。
(b) Prior art In general, in order to improve the short wavelength reproduction characteristics of a magnetoresistive thin film magnetic head, a magnetoresistive element layer is arranged in a gap (for example, about 1 μm) between magnetic shielding layers to transmit adjacent signals. It is effective to reduce the effective spacing loss by reducing the influence of the magnetic field, and by making the magnetoresistive element layer sensitive only near the recording medium sliding surface under a strong bias magnetic field (for example, about 200 Oe). It is.

然し乍ら、上記した磁気的シールドの効果及び
強いバイアス磁界の効果を併用した短波長再生特
性の良い磁気抵抗効果型薄膜磁気ヘツドを得るた
めには、以下の点を十分考慮しなければならな
い。即ち、第1に強いバイアス磁界を印加でき、
しかも該バイアス磁界の強さを容易に制御して適
正値に設定できるようなバイアス磁界発生手段を
備えること、第2に斯るバイアス磁界が磁気的シ
ールド層に引き込まれて、磁気抵抗効果素子層に
有効に作用しなくなることのないような磁気的シ
ールド手段を用いること、第3に磁気的シールド
層、磁気抵抗効果素子層、通電端子用導電体層、
バイアス磁界発生手段層等の特に各パターン端部
の段差部での電気的導通、絶縁がそれぞれの目的
に応じて十分になされるような構成にすることで
ある。
However, in order to obtain a magnetoresistive thin film magnetic head with good short wavelength reproduction characteristics that combines the effects of the magnetic shield and the strong bias magnetic field described above, the following points must be fully considered. That is, first, a strong bias magnetic field can be applied;
Moreover, it is provided with a bias magnetic field generating means that can easily control the strength of the bias magnetic field and set it to an appropriate value. Thirdly, a magnetic shielding layer, a magnetoresistive element layer, a conductive layer for a current-carrying terminal,
The object of the present invention is to create a structure in which electrical conduction and insulation, particularly at the stepped portions of the ends of each pattern, of the bias magnetic field generating means layer, etc., can be sufficiently achieved depending on the respective purpose.

ところが、従来技術では上記した点を十分に満
足した信頼性の高い磁気抵抗効果型薄膜磁気ヘツ
ドを提供することが出来なかつた。
However, the prior art has not been able to provide a highly reliable magnetoresistive thin film magnetic head that fully satisfies the above points.

(ハ) 発明の目的 本発明は斯る点に鑑み成されたもので、短波長
再生特性に優れ且つ信頼性の高い磁気抵抗効果型
薄膜磁気ヘツドを提供しようとするものである。
(c) Object of the Invention The present invention has been made in view of the above points, and an object thereof is to provide a magnetoresistive thin film magnetic head which has excellent short wavelength reproduction characteristics and is highly reliable.

(ニ) 発明の構成 即ち、本発明は上記した目的を達成するため
に、第1の非磁性基板上に少なくとも第1の磁気
的シールド層、第1の電気的磁気的絶縁層、磁気
抵抗効果素子層、通電端子用導電体層、第2の電
気的磁気的絶縁層並びに第2の磁気的シールド層
兼バイアス磁界発生用導電体層を順次形成した
後、第2の非磁性基板を補強用として接合して成
る磁気抵抗効果型薄膜磁気ヘツドであつて、前記
各層の内、通電端子用導電体層以外の層の端面を
記録媒体摺動面側に露出させると共に、前記第1
の磁気的シールド層、磁気抵抗効果素子層、第2
の磁気的シールド層兼バイアス磁界発生用導電体
層の記録媒体摺動面に垂直方向の幅をそれぞれ
Ws1、WMR、Ws2とし、前記通電端子用導電体
層の磁気抵抗効果素子層との接続部先端の記録媒
体摺動面からの距離をdとする時、WMR<Ws2
<d<Ws1になるようにしたものである。
(d) Structure of the Invention That is, in order to achieve the above-mentioned object, the present invention provides at least a first magnetic shield layer, a first electric and magnetic insulating layer, and a magnetoresistive layer on a first non-magnetic substrate. After sequentially forming the element layer, the conductive layer for current-carrying terminals, the second electric/magnetic insulating layer, and the second magnetic shielding layer/bias magnetic field generation conductive layer, a second non-magnetic substrate is used for reinforcement. The magnetoresistive thin film magnetic head is formed by bonding a magnetoresistive thin film magnetic head, in which the end surfaces of the layers other than the conductor layer for the current-carrying terminal are exposed to the recording medium sliding surface side, and
magnetic shield layer, magnetoresistive element layer, second
The width in the direction perpendicular to the recording medium sliding surface of the magnetic shielding layer/bias magnetic field generation conductor layer of
Ws1, WMR, Ws2, and when the distance from the recording medium sliding surface to the tip of the connection part of the conductor layer for the current-carrying terminal with the magnetoresistive element layer is d, WMR<Ws2
<d<Ws1.

(ホ) 実施例 以下、本発明の一実施例について図面と共に説
明する。
(E) Embodiment An embodiment of the present invention will be described below with reference to the drawings.

ここで、第1図は本発明による磁気抵抗効果型
薄膜磁気ヘツドの一例を示す1トラツク分の磁気
抵抗効果素子層近傍での模式的平面図、第2図は
第1図のA−A′断面図である。
Here, FIG. 1 is a schematic plan view showing an example of the magnetoresistive thin film magnetic head according to the present invention in the vicinity of one track of the magnetoresistive element layer, and FIG. 2 is a line A-A' in FIG. FIG.

図における1は第1の非磁性基板(例えばフオ
トセラム、ソーダガラス)、2は第1の磁気的シ
ールド層(例えば、パーマロイ、センダスト、膜
厚0.1μm)、3は第1の電気的磁気的絶縁層(例
えば、SiO2、Al2O3、膜厚0.1〜1μm)、4は磁気
抵抗効果素子層(例えば、パーマロイ、膜厚0.03
〜0.06μm)、5は通電端子用導電体層(例えば、
Cu、Au、Al、膜厚0.3〜1μm……接着層として
0.01〜0.1μmのCr、Tiが積層されることもある)、
6は第2の電気的磁気的絶縁層(例えば、SiO2
Al2O3、膜厚0.1〜1μm)、7は第2の磁気的シー
ルド層兼バイアス磁界発生用導電体層(例えば、
パーマロイ、センダスト等の導電性の高透磁率磁
性材、膜厚0.1〜1μm)、8は被覆層(例えば
SiO2、Al2O3膜厚0.1〜1μm)で、Pは記録媒体
摺動面側を示している。そして、実際には被覆層
8上にガラス系又はエポキシ系接着材を介して第
2の非磁性基板(例えばフオトセラム、ソーダガ
ラス)が接合され記録媒体摺動面から0.1〜1mm
離れた位置の被覆層8上にはバイアス磁界発生用
のバルク状永久磁石9(例えばSmCo5、アルニ
コ、Baフエライト……磁気抵抗効果素子層4の
ストライプ幅方向に着磁されている)が配置され
る。
In the figure, 1 is the first non-magnetic substrate (e.g. photoceram, soda glass), 2 is the first magnetic shield layer (e.g. permalloy, sendust, film thickness 0.1 μm), and 3 is the first electrical and magnetic insulator. layer (e.g. SiO 2 , Al 2 O 3 , film thickness 0.1 to 1 μm), 4 is a magnetoresistive element layer (e.g. permalloy, film thickness 0.03 μm).
~0.06μm), 5 is a conductor layer for current-carrying terminal (e.g.
Cu, Au, Al, film thickness 0.3-1μm...as adhesive layer
0.01~0.1μm Cr, Ti may be laminated),
6 is a second electrically and magnetically insulating layer (e.g. SiO 2 ,
Al 2 O 3 , film thickness 0.1 to 1 μm), 7 is a second magnetic shielding layer and bias magnetic field generation conductor layer (for example,
Conductive high permeability magnetic material such as permalloy or sendust, film thickness 0.1 to 1 μm), 8 is a coating layer (e.g.
SiO 2 , Al 2 O 3 film thickness: 0.1 to 1 μm), and P indicates the recording medium sliding surface side. In reality, a second non-magnetic substrate (for example, photoceram, soda glass) is bonded onto the coating layer 8 via a glass-based or epoxy-based adhesive, 0.1 to 1 mm from the recording medium sliding surface.
A bulk permanent magnet 9 (for example, SmCo 5 , alnico, Ba ferrite...magnetized in the stripe width direction of the magnetoresistive element layer 4 ) for generating a bias magnetic field is arranged on the covering layer 8 at a distant position. be done.

この様に、本発明による磁気抵抗効果型薄膜磁
気ヘツドでは、第1の非磁性基板1上に第1の磁
気的シールド層2、第1の電気的磁気的絶縁層
3、磁気抵抗効果素子層4、通電端子用導電体層
5、第2の電気的磁気的絶縁層6、第2の磁気的
シールド層兼バイアス磁界発生用導電体層7、被
覆層8が上記の順序で所定の形状に形成され、前
記各層の内少なくとも通電端子用導電体層5以外
の層の端面が記録媒体摺動面に露出した構造にな
つている。更に、第1の磁気的シールド層2、磁
気抵抗効果素子層4、第2の磁気的シールド層兼
バイアス磁界発生用導電体層7の記録媒体摺動面
に垂直方向の幅をそれぞれWs1、WMR、Ws2と
し、前記通電端子用導電体層5の磁気抵抗効果素
子層4との接続部先端の記録媒体摺動面Pからの
距離をdとした時、WMR、Ws2<d<Ws1とな
るように構成している。具体的には、WMR5μ
m、Ws210μm、d15μm、Ws120μm程度
である。
As described above, in the magnetoresistive thin film magnetic head according to the present invention, the first magnetic shield layer 2, the first electric/magnetic insulating layer 3, and the magnetoresistive element layer are disposed on the first nonmagnetic substrate 1. 4. The conductive layer 5 for current-carrying terminals, the second electrically magnetic insulating layer 6, the second magnetic shielding layer/bias magnetic field generation conductive layer 7, and the covering layer 8 are formed into a predetermined shape in the above order. Among the layers, at least the end surfaces of the layers other than the conductor layer 5 for current-carrying terminals are exposed to the recording medium sliding surface. Furthermore, the widths of the first magnetic shield layer 2, the magnetoresistive element layer 4, and the second magnetic shield layer/bias magnetic field generation conductor layer 7 in the direction perpendicular to the recording medium sliding surface are Ws1 and WMR, respectively. , Ws2, and when the distance from the recording medium sliding surface P of the tip of the connection part of the conductor layer 5 for the current-carrying terminal with the magnetoresistive element layer 4 is d, WMR is such that Ws2<d<Ws1. It is composed of Specifically, WMR5μ
m, Ws about 210 μm, d about 15 μm, and Ws about 120 μm.

ここで、磁気抵抗効果素子層4から少し離れた
位置に配置されたバルク状永久磁石9と、磁気抵
抗効果素子層4近傍に配置された第2の磁気シー
ルド層兼バイアス磁界発生用導電体層7を併用す
るようにしているのは、斯るバルク状永久磁石9
でメインの強いバイアス磁界を発生させると共
に、斯る導電体層7から発生する補助的なバイア
ス磁界を該導電体層7に流す電流を制御すること
で変化せしめて磁気抵抗効果素子層4に作用する
バイアス磁界の強さを微調整するためである。
Here, a bulk permanent magnet 9 is arranged at a position slightly apart from the magnetoresistive element layer 4, and a second magnetic shielding layer/bias magnetic field generation conductor layer is arranged near the magnetoresistive element layer 4. 7 is used together with such a bulk permanent magnet 9.
In addition to generating a main strong bias magnetic field, the auxiliary bias magnetic field generated from the conductive layer 7 is changed by controlling the current flowing through the conductive layer 7, thereby acting on the magnetoresistive element layer 4. This is to finely adjust the strength of the bias magnetic field.

また、磁気的シールド手段を磁気抵抗素子層4
を覆いきれる程度の薄膜で形成しているので、磁
気的シールド手段と前記バルク状永久磁石9との
間の距離l1を必然的に磁気抵抗効果素子層4とバ
ルク状永久磁石9との間の距離l2と同程度にする
ことが出来(具体的に、記録媒体摺動面Pからバ
ルク状永久磁石9までの距離dM500μmとする
と、WMR<Ws2〓dMであるからl1=(dM−
Ws2)l2=(dM−WMR)となる)、更に磁気
的シールド層2,7と磁気抵抗効果素子4との膜
厚の違いをあまり大きくしていないので、バイア
ス磁界を磁気抵抗効果素子層4にも十分作用させ
ることが出来る。そして、この程度の膜厚の磁気
的シールド層であつても必然的にバイアス磁界に
垂直な方向に長く伸びた構造を有しているため、
少なくとも記録媒体摺動面近傍はバイアス磁界方
向に飽和してしまうことはなく、記録媒体上の隣
接信号をシールドする効果は十分にある。
Further, the magnetic shielding means is provided in the magnetoresistive element layer 4.
The distance l1 between the magnetic shielding means and the bulk permanent magnet 9 is necessarily the same as the distance l1 between the magnetoresistive element layer 4 and the bulk permanent magnet 9. (Specifically, if the distance dM from the recording medium sliding surface P to the bulk permanent magnet 9 is 500 μm, then since WMR<Ws2〓dM, l1=(dM−
Furthermore, since the difference in film thickness between the magnetic shield layers 2 and 7 and the magnetoresistive element 4 is not too large, the bias magnetic field is applied to the magnetoresistive element layer 4. It can also work well. Even a magnetic shield layer with this thickness inevitably has a structure that extends long in the direction perpendicular to the bias magnetic field.
At least the vicinity of the recording medium sliding surface is not saturated in the direction of the bias magnetic field, and the effect of shielding adjacent signals on the recording medium is sufficient.

また、本発明では第1の磁気的シールド層2、
磁気抵抗効果素子層4、第2の磁気的シールド層
兼バイアス磁界発生用導電体層7の記録媒体摺動
面Pに垂直方向の幅をそれぞれWMR<Ws2<d
<Ws1となるように構成することで、各層間(特
に段差部)での電気的導通、絶縁がそれぞれの目
的に応じて十分になされるようにしている。即
ち、ここでd≠0とするのは一般に塑性変形し易
いCu、Au、Al等で形成される通電端子用導電体
層5の先端が記録媒体摺動面P側に露出している
と記録媒体摺動面を通して周辺の第1の磁気的シ
ールド層2或いは第2の磁気的シールド層兼バイ
アス磁界発生用導電体層7と電気的に短絡する危
険性が大きくこれを防ぐためである。また、
WMR<Ws1、WMR<Ws2とするのは第1の磁
気的シールド層2と第2の磁気的シールド層兼バ
イアス磁界発生用導電体層7が磁気抵抗効果素子
層4を覆いきつてシールド効果を十分に発揮でき
るようにするためである。そしてWs2<dとする
のは通電端子用導電体層5先端の段差部では前記
第2の磁気的電気的絶縁層6が薄くなるので、こ
の上を前記第2と磁気的シールド層兼バイアス磁
界発生用導電体層7が覆うと通電端子用導電体層
5と電気的に短絡する危険性が大きくこれを防ぐ
ためである。またd<Ws1とするのは第1の磁気
的シールド層2の端部の段差部でその上に前記第
1の磁気的電気的絶縁層3を介して形成される非
常に薄い磁気抵抗効果素子層4の通電用端子引き
出し部4′(前記通電端子用導電体層5と接続す
るためのもの)が段差を覆いきれずに断線する危
険性が大きく、磁気抵抗効果素子層4の該段差部
を磁気抵抗効果素子層より充分厚い通電端子用導
電体層5で覆うことによつて電気的導通を補うよ
うに構成するためである。
Further, in the present invention, the first magnetic shield layer 2,
The widths of the magnetoresistive element layer 4 and the second magnetic shield layer/bias magnetic field generation conductor layer 7 in the direction perpendicular to the recording medium sliding surface P are WMR<Ws2<d, respectively.
By configuring the structure such that <Ws1, electrical conduction and insulation between each layer (particularly at stepped portions) can be sufficiently achieved according to each purpose. That is, d≠0 here means that the tip of the conductor layer 5 for the current-carrying terminal, which is generally formed of Cu, Au, Al, etc. that easily undergoes plastic deformation, is exposed on the recording medium sliding surface P side. This is to prevent an electrical short circuit from occurring through the medium sliding surface with the surrounding first magnetic shield layer 2 or the second magnetic shield layer/bias magnetic field generating conductor layer 7. Also,
WMR<Ws1 and WMR<Ws2 are set because the first magnetic shield layer 2 and the second magnetic shield layer/bias magnetic field generation conductor layer 7 tightly cover the magnetoresistive element layer 4 to achieve a shielding effect. This is to enable them to perform to their full potential. The reason why Ws2<d is set is because the second magnetic and electrical insulating layer 6 becomes thinner at the step part at the tip of the conductor layer 5 for the current-carrying terminal, so that the second magnetic shield layer and the bias magnetic field are formed on this layer. This is to prevent a large risk of an electrical short circuit with the current-carrying terminal conductor layer 5 if it is covered by the generation conductor layer 7. Furthermore, d<Ws1 is a very thin magnetoresistive element formed at the stepped portion at the end of the first magnetic shield layer 2 with the first magnetic and electrical insulating layer 3 interposed therebetween. There is a great risk that the current-carrying terminal draw-out portion 4' of the layer 4 (for connecting with the conductor layer 5 for the current-carrying terminal) cannot cover the step and is disconnected. This is because the structure is such that electrical continuity is compensated for by covering the conductor layer 5 for current-carrying terminals which is sufficiently thicker than the magnetoresistive element layer.

(ヘ) 発明の効果 上述した如く本発明による磁気抵抗効果型薄膜
磁気ヘツドは、磁気的シールドの効果と強いバイ
アス磁界の効果を併用することによつて、即ち磁
気抵抗効果素子層を間隙の狭い磁気的シールド層
間に配することで隣接信号の影響を小さくし、尚
且つ斯る磁気抵抗効果素子層に強いバイアス磁界
を有効に作用させることによつて、短波長で記録
された信号の再生能力を向上させることが出来
る。
(F) Effects of the Invention As described above, the magnetoresistive thin film magnetic head according to the present invention utilizes both the effect of magnetic shielding and the effect of a strong bias magnetic field, that is, the magnetoresistive element layer is formed with a narrow gap. By placing it between magnetic shield layers, the influence of adjacent signals is reduced, and by effectively applying a strong bias magnetic field to the magnetoresistive element layer, the ability to reproduce signals recorded at short wavelengths is improved. can be improved.

更に、本発明では磁気抵抗効果型薄膜磁気ヘツ
ドを構成する各層の記録媒体摺動面に垂直方向の
幅を夫々うまく設定することによつて各層間の段
差部分での電気的導通、絶縁に対する配慮を十分
に成し、製造工程中或いは使用中の不良が発生し
難く、信頼性を大幅に向上させることが出来る。
Furthermore, in the present invention, consideration is given to electrical conduction and insulation at the stepped portion between each layer by appropriately setting the width in the direction perpendicular to the recording medium sliding surface of each layer constituting the magnetoresistive thin film magnetic head. Therefore, defects are less likely to occur during the manufacturing process or during use, and reliability can be greatly improved.

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

図は本発明による磁気抵抗効果型薄膜磁気ヘツ
ドを示し、第1図はその1トラツク分の磁気抵抗
効果素子層近傍での模式的平面図、第2図は第1
図のA−A′断面図である。 2……第1の磁気的シールド層、3……第1の
電気的磁気的絶縁層、4……磁気抵抗効果素子
層、5……通電端子用導電体層、6……第2の電
気的磁気的絶縁層、7……第2の磁気的シールド
層兼バイアス磁界発生用導電体層。
The figures show a magnetoresistive thin film magnetic head according to the present invention, in which FIG.
It is a sectional view taken along line AA' in the figure. 2...First magnetic shielding layer, 3...First electric and magnetic insulating layer, 4...Magnetoresistive element layer, 5...Conductor layer for current-carrying terminal, 6...Second electricity magnetic insulating layer, 7... second magnetic shielding layer and conductive layer for generating bias magnetic field;

Claims (1)

【特許請求の範囲】 1 第1の非磁性基板上に少なくとも第1の磁気
的シールド層、第1の電気的磁気的絶縁層、磁気
抵抗効果素子層、通電端子用導電体層、第2の電
気的磁気的絶縁層並びに第2の磁気的シールド層
を順次形成した後、第2の非磁性基板を補強用と
して接合してなる磁気抵抗効果型薄膜磁気ヘツド
であつて、前記各層の内、通電端子用導電体層以
外の層の端面を記録媒体摺動面側に露出させると
共に、前記第1の磁気的シールド層、磁気抵抗効
果素子層、第2の磁気的シールド層の記録媒体摺
動面に垂直方向の幅をそれぞれWs1、WMR、
Ws2とし、前記通電端子用導電体層の磁気抵抗効
果素子層との接続部先端の記録媒体摺動面からの
距離をdとする時、WMR<Ws2<d<Ws1であ
ることを特徴とする磁気抵抗効果型薄膜磁気ヘツ
ド。 2 前記第2の磁気的シールド層がバイアス磁界
発生用導電体層を兼ねることを特徴とする特許請
求の範囲第1項記載の磁気抵抗効果型薄膜磁気ヘ
ツド。 3 前記各層が形成された第1の非磁性基板上
で、少なくとも前記第1の磁気的シールド層を覆
わない位置にバルク状永久磁石を配置することを
特徴とする特許請求の範囲第1項または第2項記
載の磁気抵抗効果型薄膜磁気ヘツド。
[Claims] 1. On a first non-magnetic substrate, at least a first magnetic shield layer, a first electric and magnetic insulating layer, a magnetoresistive element layer, a conductive layer for a current-carrying terminal, a second A magnetoresistive thin film magnetic head is formed by sequentially forming an electrically magnetic insulating layer and a second magnetic shielding layer, and then bonding a second nonmagnetic substrate for reinforcement, which comprises: The end faces of the layers other than the conductor layer for current-carrying terminals are exposed to the recording medium sliding surface side, and the recording medium sliding of the first magnetic shield layer, the magnetoresistive effect element layer, and the second magnetic shield layer is performed. The width in the direction perpendicular to the surface is Ws1, WMR,
Ws2, and when d is the distance from the recording medium sliding surface of the tip of the connection portion of the conductive layer for the current-carrying terminal with the magnetoresistive element layer, WMR<Ws2<d<Ws1. Magnetoresistive thin film magnetic head. 2. The magnetoresistive thin film magnetic head according to claim 1, wherein the second magnetic shield layer also serves as a conductive layer for generating a bias magnetic field. 3. A bulk permanent magnet is disposed on the first non-magnetic substrate on which each of the layers is formed, at least at a position that does not cover the first magnetic shield layer. 2. The magnetoresistive thin film magnetic head according to item 2.
JP16086283A 1983-08-31 1983-08-31 Magneto-resistance effect type thin film magnetic head Granted JPS6050712A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16086283A JPS6050712A (en) 1983-08-31 1983-08-31 Magneto-resistance effect type thin film magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16086283A JPS6050712A (en) 1983-08-31 1983-08-31 Magneto-resistance effect type thin film magnetic head

Publications (2)

Publication Number Publication Date
JPS6050712A JPS6050712A (en) 1985-03-20
JPH048847B2 true JPH048847B2 (en) 1992-02-18

Family

ID=15723980

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16086283A Granted JPS6050712A (en) 1983-08-31 1983-08-31 Magneto-resistance effect type thin film magnetic head

Country Status (1)

Country Link
JP (1) JPS6050712A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2022208791A1 (en) 2021-03-31 2022-10-06 株式会社エイシング Information processing device, method, and program

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5311385A (en) * 1991-12-18 1994-05-10 Minnesota Mining And Manufacturing Company Magnetoresistive head with integrated bias and magnetic shield layer

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2022208791A1 (en) 2021-03-31 2022-10-06 株式会社エイシング Information processing device, method, and program

Also Published As

Publication number Publication date
JPS6050712A (en) 1985-03-20

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