JPS6367249B2 - - Google Patents

Info

Publication number
JPS6367249B2
JPS6367249B2 JP55148343A JP14834380A JPS6367249B2 JP S6367249 B2 JPS6367249 B2 JP S6367249B2 JP 55148343 A JP55148343 A JP 55148343A JP 14834380 A JP14834380 A JP 14834380A JP S6367249 B2 JPS6367249 B2 JP S6367249B2
Authority
JP
Japan
Prior art keywords
lead wire
magnetic detection
magnetoresistive
detection section
magnetic
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
JP55148343A
Other languages
Japanese (ja)
Other versions
JPS5774819A (en
Inventor
Takeshi Sawada
Hiroichi Goto
Shuzo Abiko
Akira Niimi
Hiroshi Yoneda
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.)
Canon Inc
Canon Electronics Inc
Original Assignee
Canon Inc
Canon Electronics Inc
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 Canon Inc, Canon Electronics Inc filed Critical Canon Inc
Priority to JP14834380A priority Critical patent/JPS5774819A/en
Publication of JPS5774819A publication Critical patent/JPS5774819A/en
Publication of JPS6367249B2 publication Critical patent/JPS6367249B2/ja
Granted legal-status Critical Current

Links

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
    • G11B5/398Specially shaped layers

Description

【発明の詳細な説明】 本発明は磁気抵抗効果型再生ヘツドに係り、さ
らに詳しくは磁気テープや磁気デイスクあるいは
磁気スケール等の磁気記録媒体の磁界を電気信号
に変換するために磁気抵抗効果を利用した磁気抵
抗効果型再生ヘツドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetoresistive playback head, and more specifically, uses the magnetoresistive effect to convert the magnetic field of a magnetic recording medium such as a magnetic tape, magnetic disk, or magnetic scale into an electrical signal. This invention relates to a magnetoresistive reproducing head.

磁気抵抗効果素子は素子の電気抵抗Rが磁界に
よつて変化するもので、その変化の過程は次式で
表わされる。
In a magnetoresistive element, the electric resistance R of the element changes depending on a magnetic field, and the process of this change is expressed by the following equation.

R=R0+△R cos2θ (1) この第(1)式の内容を図を用いて説明する。第1
図において符号1で示すものは磁気抵抗効果素子
で、この素子1に電流が矢印4で示す方向に流れ
ているとする。この状態で外部から磁気信号が矢
印3で示す方向に加わると強磁性体あるいはフエ
リ磁性体でできた磁気抵抗効果素子1の磁化方向
が矢印2で示す方向になつたとする。そして電流
の方向4と磁化方向2とのなす角をθとするとこ
の時の抵抗Rが(1)式で表わされる。(1)式において
R0は電流の流れる方向と磁化方向とが90゜をなす
時の抵抗値、△Rは最大抵抗変化量を示す。
R=R 0 +△R cos 2 θ (1) The contents of this equation (1) will be explained using figures. 1st
In the figure, it is assumed that the reference numeral 1 indicates a magnetoresistive element, and a current flows through this element 1 in the direction indicated by an arrow 4. Assume that when a magnetic signal is applied from the outside in the direction shown by the arrow 3 in this state, the magnetization direction of the magnetoresistive element 1 made of a ferromagnetic material or a ferrimagnetic material becomes the direction shown by the arrow 2. If the angle between the current direction 4 and the magnetization direction 2 is θ, the resistance R at this time is expressed by equation (1). In equation (1)
R 0 is the resistance value when the current flow direction and the magnetization direction form an angle of 90°, and ΔR is the maximum resistance change amount.

このようにして素子は外部からの磁気信号によ
つて磁化方向が変化し、抵抗値の変化が表れる。
このような磁気検出素子の概略構造は第2図に示
す如きである。
In this way, the magnetization direction of the element changes in response to an external magnetic signal, resulting in a change in resistance value.
The schematic structure of such a magnetic detection element is as shown in FIG.

即ち、第2図において符号5は磁気抵抗効果素
子で、抵抗加熱蒸着、EB(真空)蒸着、スパツタ
リング、メツキ、CVDなどの薄膜堆積法によつ
て基板6の側面に形成され、厚さは0.01〜0.1μm
程度であり、その材料はNi−Fe合金又はNi−Co
合金が一般的である。この磁気抵抗素子5の両側
にはリード線7が薄い層をなして薄膜堆積法によ
り磁気抵抗効果素子5と電気的に接続されるよう
に形成されている。又、磁気抵抗効果素子5とリ
ード線7とはICの作成技術で知られたフオトリ
ゾグラフイーなどを利用して形状が整えられる。
That is, in FIG. 2, reference numeral 5 denotes a magnetoresistive element, which is formed on the side surface of the substrate 6 by a thin film deposition method such as resistance heating evaporation, EB (vacuum) evaporation, sputtering, plating, or CVD, and has a thickness of 0.01. ~0.1μm
The material is Ni-Fe alloy or Ni-Co
Alloys are common. Lead wires 7 are formed as a thin layer on both sides of the magnetoresistive element 5 and are electrically connected to the magnetoresistive element 5 by a thin film deposition method. Further, the shapes of the magnetoresistive element 5 and the lead wires 7 are adjusted using photolithography, which is known as an IC manufacturing technique.

このような構造を有する磁気検出素子は記録媒
体8上の磁化部分9からのy方向成分磁界を検知
し、その抵抗が変化する。
The magnetic detection element having such a structure detects the y-direction component magnetic field from the magnetized portion 9 on the recording medium 8, and its resistance changes.

このように極めて単純な構造により磁界の検出
が可能であるため、再生専用の薄膜磁気ヘツドと
して多く利用されている。そして、さらに簡略に
製造するために磁気抵抗効果素子部分とリード線
部分を同一材料で作り、一回の成膜、一回のフオ
トリゾグラフイーにより磁気検出素子を作ること
が本出願人により先に提案されている。この提案
の概略を第3図に示す。
Since the magnetic field can be detected with such an extremely simple structure, it is often used as a thin film magnetic head for reproduction only. In order to further simplify manufacturing, the applicant previously proposed that the magnetoresistive element part and the lead wire part be made of the same material, and that the magnetic sensing element be made by one film formation and one photolithography process. has been proposed. Figure 3 shows an outline of this proposal.

第3図において符号10で示す部分は磁気検出
部で、符号11で示す部分がリード線部分であり
両者は同一材質で一体に形成されている。
In FIG. 3, the part designated by numeral 10 is a magnetic detection section, and the part designated by numeral 11 is a lead wire part, both of which are integrally formed of the same material.

このような一体化された検出素子は構造が簡単
で製作が容易ではあるが、外部の雑音磁界に対し
てリード線部分11が抵抗値の変化を示し、この
リード線部分11は磁気検出部10と、直列に接
続された状態となつているため磁気検出部10の
検出した抵抗変化が少い時は相対的に雑音が多く
なり、SN比の低下を招く恐れがある。雑音磁界
としてはモーターの磁界、電源トランスからの磁
界、電源リード線による磁界、あるいは地磁気な
どが考えられる。
Although such an integrated detection element has a simple structure and is easy to manufacture, the lead wire portion 11 exhibits a change in resistance value in response to an external noise magnetic field. Since they are connected in series, when the resistance change detected by the magnetic detection section 10 is small, there is a relatively large amount of noise, which may lead to a decrease in the SN ratio. Possible noise magnetic fields include the magnetic field of a motor, the magnetic field from a power transformer, the magnetic field from power lead wires, and the earth's magnetism.

一般に磁気記録装置の中ではモーターや電源ト
ランスなどからわずかながら交流磁界が出てお
り、何らかの対策が必要である。
Generally, in magnetic recording devices, a small amount of alternating magnetic field is emitted from the motor, power transformer, etc., and some kind of countermeasure is required.

本発明は以上のような事情に鑑み成されたもの
で、磁気的な雑音に対して影響されることが少
く、SN比の極めて良好な磁気抵抗効果型再生ヘ
ツドを提供することを目的としている。
The present invention has been made in view of the above circumstances, and it is an object of the present invention to provide a magnetoresistive playback head that is less affected by magnetic noise and has an extremely good signal-to-noise ratio. .

本発明においては上記の目的を達成するため
に、同一基板上に同一材質で磁気抵抗効果素子と
リード線部を薄膜堆積法により形成した再生ヘツ
ドにおいて、リード線部分を流れる電流の方向が
互いに直角を成すように配置した実質的に幅の等
しい1以上の第1および第2のリード線部から構
成すると共に、これら第1および第2のリード線
部を直列に接続すると共に第1のリード線部の合
計の長さと前記第2のリード線部合計の長さを実
質的に等しくした構造を採用した。
In order to achieve the above object, the present invention provides a read head in which a magnetoresistive element and a lead wire portion are formed of the same material on the same substrate by a thin film deposition method, so that the directions of currents flowing through the lead wire portion are perpendicular to each other. The structure includes one or more first and second lead wire parts having substantially equal widths arranged so as to form the same width, and the first and second lead wire parts are connected in series, and the first lead wire A structure is adopted in which the total length of the second lead wire portion is substantially equal to the total length of the second lead wire portion.

以下、図面に示す実施例に基いて本発明の詳細
を説明する。
Hereinafter, details of the present invention will be explained based on embodiments shown in the drawings.

第4図は本発明の原理的な構成を説明するもの
で、図において全体を符号12で示す磁気検出素
子は全体が磁気抵抗効果をもつ素材から薄膜堆積
法により形成されている。この磁気検出素子12
は左右対称で、かつ直角に屈曲した形状を有し、
その一端の水平部は磁気検出部13となつてお
り、この磁気検出部13の両端部には直角に屈曲
する立ち上り部14,14に連続しておりこの立
ち上り部14の他端は磁気検出部13と平行な状
態で直角に屈曲する水平部15,15に連続し、
水平部15の他端は直角に立ち上り、かつ、互に
接近した状態にある立ち上り部16に連続し、こ
の立ち上り部16の他端は外側に向つて水平に伸
びる水平部17,17に連続し、水平部17,1
7はさらに立ち上り部18に連続している。これ
らの各部分14〜18はリード線部分を構成して
いる。
FIG. 4 explains the basic structure of the present invention, and the magnetic detection element, which is indicated by the reference numeral 12 in the figure, is formed entirely from a material having a magnetoresistive effect by a thin film deposition method. This magnetic detection element 12
has a shape that is bilaterally symmetrical and bent at right angles,
The horizontal part at one end is a magnetic detection section 13, and both ends of this magnetic detection section 13 are continuous with rising sections 14, 14 bent at right angles, and the other end of this rising section 14 is a magnetic detection section. Continuing with the horizontal parts 15, 15 bent at right angles in a state parallel to 13,
The other end of the horizontal portion 15 is continuous with a rising portion 16 that rises at a right angle and is close to each other, and the other end of this rising portion 16 is continuous with horizontal portions 17, 17 that extend horizontally toward the outside. , horizontal part 17,1
7 further continues to the rising portion 18. Each of these parts 14 to 18 constitutes a lead wire part.

従つて、立ち上り部14を流れる電流の向きを
矢印19で示し、水平部15を流れる電流の向き
を矢印20で示すと、両者は90゜の角度で方向を
変えて流れており、立ち上り部14、水平部15
の長さは等しくなるように形成されている。
Therefore, if the direction of the current flowing through the rising portion 14 is indicated by an arrow 19, and the direction of the current flowing through the horizontal portion 15 is indicated by an arrow 20, they both flow in different directions at an angle of 90 degrees, and the direction of the current flowing through the rising portion 14 is indicated by an arrow 20. , horizontal part 15
are formed to have equal lengths.

このような構造を有する磁気検出素子12に対
して、第4図に矢印21で示す外部磁界が印加さ
れると、これによつて生じる磁化方向は点線の矢
印22,23で示すように一定の方向となる。な
お、この場合、素子の膜厚が0.01〜0.05μmと極
めて薄く、幅が10〜50μmであるため、反磁界は
無視し得る。
When an external magnetic field indicated by the arrow 21 in FIG. direction. Note that in this case, since the film thickness of the element is extremely thin at 0.01 to 0.05 μm and the width is 10 to 50 μm, the demagnetizing field can be ignored.

以上の構造のもとに立ち上り部14の磁化方向
である矢印22と電流の方向である矢印19のな
す角度をθとすると、この部分の抵抗R14は R14=Rl+△Rl cos2θ (2) となる。(2)式においてRlは立ち上り部14の最小
抵抗値、△Rlは最大変化量である。
Based on the above structure, if the angle between the arrow 22, which is the magnetization direction of the rising portion 14, and the arrow 19, which is the current direction, is θ, then the resistance R 14 of this part is R 14 = R l + △R l cos 2 θ (2). In equation (2), R l is the minimum resistance value of the rising portion 14, and ΔR l is the maximum amount of change.

同様にして水平部15の抵抗R15は最小抵抗値
をRr、最大抵抗変化量△Rrとすると次式となる。
Similarly, the resistance R 15 of the horizontal portion 15 is expressed by the following equation, where R r is the minimum resistance value and ΔR r is the maximum resistance change.

R15=Rr+△Rr cos2φ (3) (3)式において角度φはθを用いて表現すると次
式で表わされる。
R 15 =R r +△R r cos 2 φ (3) In equation (3), the angle φ is expressed using θ as the following equation.

φ=90゜−θ (4) 従つて、(3)式は次式のように変形できる。 φ=90゜−θ (4) Therefore, equation (3) can be transformed as shown below.

R15=Rr+△Rr sin2θ (3)′ ここで、立ち上り部14、水平部15は直列に
接続され、さらに、Rr=Rl、△Rr=△Rlとなる
ように形状が設定されていれば、両者の抵抗の和
Rは次式のように一定値となる。
R 15 = R r + △R r sin 2 θ (3)' Here, the rising part 14 and the horizontal part 15 are connected in series, and further, R r = R l and △R r = △R l . If the shape is set to , the sum R of both resistances will be a constant value as shown in the following equation.

R=R14+R15=2Rr+△Rr(cos2θ+sin2θ) =2Rr+△Rr=一定 (5) このようにリード線部分に第1および第2のリ
ード線部分を設け、両部分を直列に接続すると共
に、両部分を流れる電流の方向が90゜の角度をな
すように設定すれば、リード線部分と磁気検出部
とを一体に薄膜堆積法によつて形成しても、磁気
雑音に影響されず、SN比の良好な磁気検出素子、
従つて、再生ヘツドを得ることができる。
R = R 14 + R 15 = 2R r + △R r (cos 2 θ + sin 2 θ) = 2R r + △R r = constant (5) In this way, the first and second lead wire parts are provided in the lead wire part. If both parts are connected in series and the direction of the current flowing through both parts is set at a 90° angle, the lead wire part and the magnetic detection part can be integrally formed by the thin film deposition method. A magnetic detection element with a good signal-to-noise ratio, which is not affected by magnetic noise.
Therefore, a reproducing head can be obtained.

第5図は本発明の一実施例を説明するもので、
図中、第4図と同一部分または相当する部分には
同一符号を符し、その説明は省略する。
FIG. 5 illustrates an embodiment of the present invention.
In the figure, the same or corresponding parts as in FIG. 4 are denoted by the same reference numerals, and the explanation thereof will be omitted.

第5図において磁気検出部13の長さを2l1
立ち上り部14の長さをl2とし、l1=l2とすれば
磁気検出部13に表われるノイズも立ち上り部1
4によりキヤンセルされ、SN比向上に効果があ
る。
In FIG. 5, the length of the magnetic detection section 13 is 2l 1 ,
If the length of the rising part 14 is l 2 and l 1 = l 2 , then the noise appearing in the magnetic detection part 13 will also be the same as that of the rising part 1.
4, which is effective in improving the signal-to-noise ratio.

第6図は本発明の他の実施例を説明するもの
で、図において符号13で示す磁気検出部の両端
からは左右対称に内側に向かつて「く」の字状に
屈曲する折曲部24,25が連続しており、両折
曲部24,25は直角に交差している。そして、
折曲部24と磁気検出部13とは45゜の角度で交
差している。
FIG. 6 explains another embodiment of the present invention, in which bent portions 24 are symmetrically bent inward from both ends of the magnetic detection portion indicated by reference numeral 13 in the figure in a dogleg shape. , 25 are continuous, and both bent portions 24 and 25 intersect at right angles. and,
The bent portion 24 and the magnetic detection portion 13 intersect at an angle of 45°.

このような構造を採用するとリード線部分の長
さを短かくし、抵抗値の低下をはかることがで
き、抵抗による熱雑音の低下をはかることができ
る。実際にはリード線部の抵抗は第6図において
磁気検出部13の長さをL、磁気検出部13から
リード線部の端部までの長さをHとすると、同一
寸法内で第4図に示した原理の構造を採用した場
合と比較して1/√2となり、かつ、耐ノイズ性
は変らないと言う優れた効果が得られる。
If such a structure is adopted, the length of the lead wire portion can be shortened, the resistance value can be reduced, and the thermal noise due to the resistance can be reduced. In reality, the resistance of the lead wire section is within the same dimensions as shown in Figure 4, assuming that the length of the magnetic detection section 13 in FIG. This is 1/√2 compared to the case where the structure based on the principle shown in is adopted, and the excellent effect that the noise resistance remains unchanged can be obtained.

第7図は本発明のもう1つの実施例を説明する
もので、リード線部の抵抗値をできるだけ下げよ
うとする例である。リード線部分の抵抗値を下げ
たい場合にはリード線部分の許されている線幅を
全て使うことが望ましい。第7図はこのような目
的に加えて、さらに耐ノイズ特性を増大させよう
とする構造である。即ち、第7図において符号2
6で示す部分はリード線部分で、左右対称に形成
されているため、一方の側のみ示してある。この
リード線部分26は許すかぎりの幅をもつて極め
て幅広に形成されている。しかし、このリード線
部分26は直角に蛇行する細溝27aを複数条平
行にエツチングで形成することにより、同様に蛇
行する電流通路27を複数条形成してある。符号
28で示すものは電流通路の屈曲部を隔てるため
の溝である。
FIG. 7 illustrates another embodiment of the present invention, which is an example in which the resistance value of the lead wire portion is attempted to be lowered as much as possible. If it is desired to lower the resistance value of the lead wire portion, it is desirable to use the entire allowable line width of the lead wire portion. In addition to this purpose, FIG. 7 shows a structure intended to further increase noise resistance. That is, in FIG.
The part indicated by 6 is a lead wire part, and since it is formed symmetrically, only one side is shown. This lead wire portion 26 is formed to be as wide as possible. However, this lead wire portion 26 has a plurality of meandering current paths 27 formed therein by etching a plurality of thin grooves 27a that meander at right angles in parallel. What is indicated by the reference numeral 28 is a groove for separating the bent portions of the current path.

今、上記のように構成された電流通路の1つを
選んでその繰り返されるパターンの1周期分AB
間を考え、磁気検出部13と直角に電流が流れる
部分の長さをr1,r2,r3、平行に流れる部分の長
さをl1,l2とすれば、 l1+l2=r1+r2+r3=const(一定) (6) となるような電流通路パターンを構成することが
できる。
Now, select one of the current paths configured as above and conduct AB for one period of the repeated pattern.
Considering the distance between the two, let r 1 , r 2 , r 3 be the lengths of the parts where the current flows at right angles to the magnetic detection unit 13, and l 1 , l 2 be the lengths of the parts where the currents flow in parallel, then l 1 + l 2 = A current path pattern can be configured such that r 1 +r 2 +r 3 = const (constant) (6).

このような構造を採用すれば、リード線部分2
6全体の断面積は増大し、抵抗の小さいリード線
部分を得ることが出来ると共に電流通路が直角に
屈曲しているため、同相のノイズを除去すること
ができ、SN比の極めて優れた再生ヘツドを得る
ことができる。
If such a structure is adopted, the lead wire portion 2
6.The overall cross-sectional area has been increased, making it possible to obtain a lead wire portion with low resistance, and the current path is bent at right angles, making it possible to eliminate in-phase noise and creating a playback head with an extremely excellent signal-to-noise ratio. can be obtained.

以上の説明から明らかなように、本発明によれ
ば、磁気的ノイズに対して影響されにくい、極め
てSN比の良好な再生ヘツドを得ることができる。
As is clear from the above description, according to the present invention, it is possible to obtain a reproducing head that is less susceptible to magnetic noise and has an extremely good signal-to-noise ratio.

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

第1図は磁気抵抗効果素子の原理を示す説明
図、第2図および第3図は従来の磁気抵抗効果型
再生ヘツドのそれぞれ異なつた構造を説明する斜
視図および素子部分の正面図、第4図は本発明の
原理の説明図、第5図〜第7図は本発明のそれぞ
れ異なつた実施例を説明する正面図である。 5……磁気抵抗効果素子、6……基板、12…
…磁気検出素子、13……磁気検出部、14……
立ち上り部、15……水平部、24,25……屈
曲部、26……リード線部、27……電流通路、
27a……細溝。
FIG. 1 is an explanatory diagram showing the principle of a magnetoresistive effect element, FIGS. 2 and 3 are perspective views and front views of the element portion, respectively, illustrating different structures of a conventional magnetoresistive read head. The figure is an explanatory diagram of the principle of the invention, and FIGS. 5 to 7 are front views illustrating different embodiments of the invention. 5... Magnetoresistive element, 6... Substrate, 12...
...Magnetic detection element, 13... Magnetic detection section, 14...
Rising part, 15...Horizontal part, 24, 25...Bending part, 26...Lead wire part, 27...Current path,
27a...Narrow groove.

Claims (1)

【特許請求の範囲】 1 同一基板上に磁気検出部とリード線部とを薄
膜堆積法により強磁性体あるいはフエリ磁性体で
ある磁気抵抗効果素材を用いて一体形成した磁気
抵抗効果型再生ヘツドにおいて、前記リード線部
はこれに流れる電流の方向が互いに直角を成すよ
うに配置した実質的に幅の等しい第1および第2
のリード線部を夫々1以上含み、前記第1および
第2のリード線部を直列に接続すると共に該第1
のリード線部の合計の長さと前記第2のリード線
部合計の長さを実質的に等しくしたことを特徴と
する磁気抵抗効果型再生ヘツド。 2 磁気検出部に直接的に接続されている第1あ
るいは第2のリード線部の長さを磁気検出部の長
さの1/2とした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再生ヘツド。 3 磁気検出部に直接的に接続されている第1あ
るいは第2のリード線部を流れる電流の方向が磁
気検出部の軸線方向と45゜をなすように配置した
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再生ヘツド。 4 前記リード線部は第1および第2のリード線
部を直列接続した線条が複数条並列に形成されて
な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再生ヘツド。
[Scope of Claims] 1. In a magnetoresistive playback head in which a magnetic detection section and a lead wire section are integrally formed on the same substrate using a magnetoresistive material, which is a ferromagnetic material or a ferrimagnetic material, by a thin film deposition method. , the lead wire portion has first and second lead wires having substantially equal widths arranged such that the directions of current flowing through the lead wire portions are perpendicular to each other.
the first and second lead wire portions are connected in series, and the first and second lead wire portions are connected in series;
A magnetoresistive effect type read head, characterized in that the total length of the second lead wire portion is substantially equal to the total length of the second lead wire portion. 2. Claim 1, characterized in that the length of the first or second lead wire section directly connected to the magnetic detection section is 1/2 of the length of the magnetic detection section. magnetoresistive playback head. 3. A patent claim characterized in that the direction of the current flowing through the first or second lead wire section directly connected to the magnetic detection section is arranged at an angle of 45 degrees with the axial direction of the magnetic detection section. A magnetoresistive read head according to item 1 or 2. 4. The magnetic resistance according to claim 1 or 2, wherein the lead wire portion is formed by a plurality of parallel wires in which first and second lead wire portions are connected in series. Effective regeneration head.
JP14834380A 1980-10-24 1980-10-24 Magnetic resistance effect type reproducing head Granted JPS5774819A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14834380A JPS5774819A (en) 1980-10-24 1980-10-24 Magnetic resistance effect type reproducing head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14834380A JPS5774819A (en) 1980-10-24 1980-10-24 Magnetic resistance effect type reproducing head

Publications (2)

Publication Number Publication Date
JPS5774819A JPS5774819A (en) 1982-05-11
JPS6367249B2 true JPS6367249B2 (en) 1988-12-23

Family

ID=15450640

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14834380A Granted JPS5774819A (en) 1980-10-24 1980-10-24 Magnetic resistance effect type reproducing head

Country Status (1)

Country Link
JP (1) JPS5774819A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5260607A (en) * 1975-11-13 1977-05-19 Matsushita Electric Ind Co Ltd Magnetic head
JPS5668918A (en) * 1979-11-06 1981-06-09 Sanyo Electric Co Ltd Magnetic card reader

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5260607A (en) * 1975-11-13 1977-05-19 Matsushita Electric Ind Co Ltd Magnetic head
JPS5668918A (en) * 1979-11-06 1981-06-09 Sanyo Electric Co Ltd Magnetic card reader

Also Published As

Publication number Publication date
JPS5774819A (en) 1982-05-11

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