JPS63142511A - Magneto-resistance type magnetic head - Google Patents

Magneto-resistance type magnetic head

Info

Publication number
JPS63142511A
JPS63142511A JP29075186A JP29075186A JPS63142511A JP S63142511 A JPS63142511 A JP S63142511A JP 29075186 A JP29075186 A JP 29075186A JP 29075186 A JP29075186 A JP 29075186A JP S63142511 A JPS63142511 A JP S63142511A
Authority
JP
Japan
Prior art keywords
width
magnetic
magneto
easy magnetization
magnetic field
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
JP29075186A
Other languages
Japanese (ja)
Inventor
Akira Hirano
明 平野
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP29075186A priority Critical patent/JPS63142511A/en
Publication of JPS63142511A publication Critical patent/JPS63142511A/en
Pending 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
    • 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
    • G11B5/3906Details related to the use of magnetic thin film layers or to their effects
    • G11B5/3945Heads comprising more than one sensitive element
    • G11B5/3948Heads comprising more than one sensitive element the sensitive elements being active read-out elements
    • G11B5/3958Heads comprising more than one sensitive element the sensitive elements being active read-out elements the active elements being arranged in a single plane, e.g. "matrix" disposition
    • G11B5/3961Heads comprising more than one sensitive element the sensitive elements being active read-out elements the active elements being arranged in a single plane, e.g. "matrix" disposition disposed at an angle to the direction of the track or relative movement
    • 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
    • G11B5/48Disposition or mounting of heads or head supports relative to record carriers ; arrangements of heads, e.g. for scanning the record carrier to increase the relative speed
    • G11B5/488Disposition of heads

Landscapes

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

Abstract

PURPOSE:To detect even a minute shift against a track of a magnetic storage medium, and to improve the detection accuracy by making the width of a magneto-resistance element which consists of a magnetic anisotropic material, and whose axis-of-easy magnetization direction is used as lengthwise direction, different in the center part and the side part. CONSTITUTION:As for a slender magneto-resistance element 12 which consists of a magnetic anisotropic material such as 'Permalloy(R)', etc., and whose axis-of-easy magnetization, the center part in the lengthwise direction is a narrow width magnetism detecting part 12a, and both outsides are wide width magnetism detecting parts 12b, 12c. In the magneto-resistance element 12, an equipotential thin wire 13 consisting of a good conductive material is formed at an angle of 30-60 deg. with its axis-of-easy magnetization. When a prescribed current is allowed to flow to a magnetism detecting element 11 constituted in such a way, and an external magnetic field is brought close, an output characteristic of the element 11 is related to width w1 of the center narrow width part, its length l and wide width w2. When the length l of the center part 12a is made almost equal to width of a track of a magnetic storage medium, a shift of the external magnetic field can be detected clearly from its output.

Description

【発明の詳細な説明】 〔概要〕 等電位良導電細条が形成された磁気異方性材料の磁気抵
抗素子を具えた磁気ヘッドにおいて、該抵抗素子の長さ
方向の中央部をその側部より狭幅または広幅にしたこと
により、 外部磁界の位置検知精度を向上させたものである。
[Detailed Description of the Invention] [Summary] In a magnetic head equipped with a magnetoresistive element made of a magnetically anisotropic material on which equipotential and highly conductive stripes are formed, the longitudinal center portion of the resistance element is connected to its side portions. By making the width narrower or wider, the accuracy of detecting the position of the external magnetic field is improved.

〔産業上の利用分野〕[Industrial application field]

本発明は良導電細条の形成された磁気抵抗素子を具えた
磁気抵抗形磁気ヘッド、特に磁気記憶媒体に所望の情報
を書き込みおよび読み取りするWZR用磁気ヘッドが、
該媒体のトラックを正確にトレースするためのサーボ用
として使用する磁気ヘッドの改良に関する。
The present invention provides a magnetoresistive magnetic head equipped with a magnetoresistive element formed with highly conductive stripes, particularly a WZR magnetic head for writing and reading desired information on a magnetic storage medium.
The present invention relates to an improvement in a magnetic head used for servo for accurately tracing tracks on the medium.

記憶媒体に所望の情報を書き込みおよび読み取るための
W/R用磁気ヘッドを、記憶媒体のトラックと正しく対
向させる必要からサーボ用磁気ヘッドが使用される。
A servo magnetic head is used because a W/R magnetic head for writing and reading desired information on a storage medium needs to be correctly opposed to the tracks of the storage medium.

記憶情報の高密度化によりトラック幅が狭くなり、例え
ば1トラックの記憶密度が16000〜25000BP
I(ピント/インチ)、トラック密度が1200〜15
00T P I  (トラック/インチ)の磁気ディス
クにおいて、書き込まれた情報トラックの幅は13〜1
8μmであり、該トラック幅の50%側方にずれたW/
R用磁気ヘッドからの出力は約50%に低減する。
As the density of stored information increases, the track width becomes narrower, and for example, the storage density of one track is 16,000 to 25,000 BP.
I (focus/inch), track density 1200-15
On a 00T P I (tracks per inch) magnetic disk, the width of the written information track is 13 to 1
8 μm, and the W/ is shifted laterally by 50% of the track width.
The output from the R magnetic head is reduced to about 50%.

そこで、W/R用磁気ヘッドは記憶媒体のトラックと正
確に対向させる必要があるが、一般にトラックの両側に
はそれぞれ約2μmの幅で情報の書き込まれないガート
バンドがあり、100%の出力が得られる余裕度は左右
に2μmである。
Therefore, it is necessary for the W/R magnetic head to accurately face the track of the storage medium, but generally there is a guard band on each side of the track with a width of about 2 μm and no information is written, so that 100% output cannot be achieved. The margin obtained is 2 μm on the left and right sides.

他方、通常のサーボ用磁気ヘッドは、トラック幅の約2
倍(例えば26μm)の範囲でトラックの位置を検出す
る構成になっている。
On the other hand, a normal servo magnetic head has a track width of about 2
The structure is such that the track position can be detected within a range twice as large (for example, 26 μm).

〔従来の技術〕[Conventional technology]

磁気抵抗を利用し外部磁界を検出するサーボ用磁気ヘッ
ドは、磁気異方性材料にてなりその容易磁化軸方向を長
さとした磁気抵抗素子に、良導電性等電位の細条パター
ンを設けたバーバーポール型磁気検出素子が広く用いら
れている。
A servo magnetic head that uses magnetic resistance to detect an external magnetic field is a magnetic resistance element made of a magnetically anisotropic material whose length is in the direction of its easy magnetization axis, and a pattern of highly conductive equipotential strips is provided on the magnetic resistance element. Barber pole type magnetic sensing elements are widely used.

第4図は従来のバーバーポール型磁気検出素子の要部を
示す斜視図であり、磁気検出素子1は、磁気異方性材料
の容易磁化軸を長さ方向にした細長い磁気抵抗素子2に
、良導電性等電位の細条3および電極4をパターン形成
してなる。一般にパーマロイを使用した磁気抵抗素子2
は、検出部2aと一対の接続部2bからなり、細条3と
電極4には金を使用している。
FIG. 4 is a perspective view showing the main parts of a conventional barber pole type magnetic sensing element. The magnetic sensing element 1 consists of an elongated magnetoresistive element 2 whose length direction is the axis of easy magnetization of a magnetically anisotropic material. It is formed by patterning well-conducting equipotential strips 3 and electrodes 4. Magnetoresistive element 2 that generally uses permalloy
consists of a detection section 2a and a pair of connection sections 2b, and the strips 3 and electrodes 4 are made of gold.

かかる磁気検出素子1において、磁気検出部2aの長さ
は例えば26μmであり、検出部2aの中心から左右で
逆方向に傾斜した良導電細条3の傾斜角度は、検出部2
aの長さ方向に対し30〜60度(例えば45度)であ
り、磁気検出部2aの長さより狭幅の外部磁界の位置に
対応し、出力電圧が変わることで磁気記憶媒体のトラッ
クとの位置ずれを検出することができる。
In such a magnetic detection element 1, the length of the magnetic detection part 2a is, for example, 26 μm, and the inclination angle of the highly conductive strips 3, which are inclined in opposite directions on the left and right sides from the center of the detection part 2a, is
The angle is 30 to 60 degrees (for example, 45 degrees) with respect to the length direction of a, and corresponds to the position of the external magnetic field narrower than the length of the magnetic detection section 2a. Positional deviation can be detected.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

第5図は従来の磁気検出素子1の出力特性図であり、縦
軸を出力電圧へV、横軸を外部磁界から入力した磁界の
強さHとしたとき、出力特性Aは外部磁界(磁気記憶媒
体のトラックからの磁界)が検出部1aの中心に位置し
たとき零であり、入力磁界が該中心から右または左にず
れるとそのずれに対応し十電圧または一電圧として出力
する。
FIG. 5 is an output characteristic diagram of the conventional magnetic detection element 1. When the vertical axis is the output voltage V, and the horizontal axis is the strength H of the magnetic field input from the external magnetic field, the output characteristic A is the external magnetic field (magnetic field). When the magnetic field (from the track of the storage medium) is located at the center of the detection unit 1a, it is zero, and when the input magnetic field shifts to the right or left from the center, it outputs 10 voltages or 1 voltage corresponding to the shift.

即ち、従来の磁気検出素子1は、検出部1aの中心と磁
気記憶媒体のトラックとのずれが微小であるとき、出力
が±Ovの近傍で振れるため検出精度が低下するという
問題点があり、磁気記憶媒体の高密度化に伴ってその改
善が強く要望されるようになった。
That is, the conventional magnetic detection element 1 has a problem in that when the deviation between the center of the detection part 1a and the track of the magnetic storage medium is minute, the output swings around ±Ov, resulting in a decrease in detection accuracy. With the increasing density of magnetic storage media, there has been a strong demand for improvements.

〔問題点を解決するための手段〕[Means for solving problems]

上記問題点の除去を目的とした本発明は、磁気検出素子
の幅によって出力が変化することに着目し実現したもの
であり、第1図によれば、磁気異方性材料からなりその
容易磁化軸方向を長さとした長さ方向の中央部12aを
その側部12b、 12cより狭幅または広幅に形成し
た細長い磁気抵抗素子12を具え、抵抗素子12にその
該容易磁化軸方向と30〜60度の角度で良導電材料か
らなる等電位細条13を形成してなることを特徴とする
磁気抵抗形磁気ヘッドである。
The present invention, which aims to eliminate the above-mentioned problems, was realized by focusing on the fact that the output changes depending on the width of the magnetic detection element.According to FIG. The magnetoresistive element 12 is provided with an elongated magnetoresistive element 12 in which the central part 12a in the longitudinal direction with the length in the axial direction is narrower or wider than the side parts 12b and 12c, and the resistance element 12 has a 30 to 60 mm width in the direction of the easy magnetization axis. This is a magnetoresistive magnetic head characterized in that equipotential strips 13 made of a highly conductive material are formed at an angle of 10°.

(作用〕 上記手段によれば、磁気抵抗素子の中央部に外部磁界が
対向するときと、該素子の側部が外部磁界が対向すると
きとで該素子からの出力が変化する。従って、外部磁界
に磁気抵抗素子の中央部が対向していた磁気ヘッドが側
方に少しずれると、そのずれは磁気抵抗素子の側部から
の+または一出力として急峻に変化させることが可能で
あり、従来の磁気抵抗素子では出力が±0近傍となるず
れを高精度に検出できるようになる。
(Function) According to the above means, the output from the magnetoresistive element changes depending on when the external magnetic field faces the central part of the element and when the external magnetic field faces the side parts of the element. When the magnetic head, whose central part of the magnetoresistive element faces the magnetic field, shifts slightly to the side, the shift can be changed sharply as a positive or negative output from the side of the magnetoresistive element. With this magnetoresistive element, it is possible to detect with high precision a deviation where the output is close to ±0.

〔実施例〕〔Example〕

以下に、図面を用いて本発明の実施例による磁気抵抗形
磁気ヘッドを説明する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS Magnetoresistive magnetic heads according to embodiments of the present invention will be described below with reference to the drawings.

第1図は本発明の一実施例に係わる磁気検出素子の要部
を示す斜視図(イ)とその出力特性図(ロ)である。
FIG. 1 is a perspective view (a) showing a main part of a magnetic detection element according to an embodiment of the present invention, and a diagram of its output characteristics (b).

第1図(イ)において、磁気検出素子IIは長さ方向を
容易磁化軸とした磁気抵抗素子12に、良導電性等電位
の細条13および電極14をパターン形成してなる。
In FIG. 1(A), the magnetic detection element II is formed by forming a pattern of highly conductive equipotential strips 13 and electrodes 14 on a magnetoresistive element 12 whose axis of easy magnetization is in the longitudinal direction.

パーマロイ等の磁気異方性材料にてなり、その容易磁化
軸を長さ方向とした細長い磁気抵抗素子12は、長さ方
向の中央に位置する狭幅磁気検出部12aと、検出部1
2aの外側の広幅磁気検出部12b。
The elongated magnetoresistive element 12, which is made of a magnetically anisotropic material such as permalloy and whose axis of easy magnetization is in the longitudinal direction, has a narrow magnetic detecting section 12a located at the center in the longitudinal direction, and a detecting section 1.
A wide magnetic detection section 12b outside of 2a.

12cと、外部回路に接続するため検出部12b、 1
2cの外側にそれぞれ設けた接続部12d、12eから
なり、接続部12d、12eの上には最端位置の細条1
3に接続する電極14が被着されている。
12c, and a detection section 12b, 1 for connection to an external circuit.
It consists of connecting parts 12d and 12e provided on the outside of the connecting parts 12d and 12e, respectively.
An electrode 14 connected to 3 is deposited.

実施例として、厚さ約500人のパーマロイからなる磁
気抵抗素子12に、その容易磁化軸方向と45度の傾斜
で厚さ約5000人の金の各細条13は、磁気抵抗素子
12より10倍厚いことおよび、金の導電率がパーマロ
イのそれより約10〜15倍高いことで等電位になる。
As an example, in a magnetoresistive element 12 made of permalloy about 500 mm thick, each strip 13 of about 5000 mm thick gold at an angle of 45 degrees with its axis of easy magnetization is placed 10 mm thicker than the magnetoresistive element 12. It is equipotential because it is twice as thick and the conductivity of gold is about 10-15 times higher than that of permalloy.

かかる磁気検出素子1)に所定の電流を流し、外部磁界
を近づけたとき、素子1)の出力特性は狭幅磁気検出部
12aの幅W1とその長さlおよび広幅磁気検出部12
b、 12cの幅W2に係わる。
When a predetermined current is passed through the magnetic detection element 1) and an external magnetic field is brought close to it, the output characteristics of the element 1) are determined by the width W1 of the narrow magnetic detection section 12a, its length l, and the wide magnetic detection section 12.
b, relates to the width W2 of 12c.

そこで、幅W1を8mm、長さlを記憶媒体のトラック
幅と同一にし、幅W2を16n+mにしたとき磁気検出
素子1)の出力は第1図(I+)に示す如くなる。
Therefore, when the width W1 is set to 8 mm, the length l is set to be the same as the track width of the storage medium, and the width W2 is set to 16n+m, the output of the magnetic sensing element 1) becomes as shown in FIG. 1 (I+).

第1図(rl)において、縦軸は出力電圧±Δ■。In FIG. 1 (rl), the vertical axis represents the output voltage ±Δ■.

横軸は図中の磁気記憶トラック5の長さに対応する軸で
あり、振幅の小さい特性Bはトラック5が狭幅磁気検出
部12aに対向するときの出力、振幅の大きい特性Cは
トラック5が広幅磁気検出部12bまたは12cに対向
するときの出力であり、出力BとCはトラック5を細分
化し付与された極性に対応し正弦波状になる。
The horizontal axis is an axis corresponding to the length of the magnetic storage track 5 in the figure. Characteristic B with a small amplitude is the output when the track 5 faces the narrow magnetic detection section 12a, and characteristic C with a large amplitude is the output when the track 5 faces the narrow magnetic detection section 12a. is the output when facing the wide magnetic detection section 12b or 12c, and the outputs B and C have a sine wave shape corresponding to the polarity given by subdividing the track 5.

そこで、図中に点線で示すように特性BとCの中間にス
ライスレベルLを設定すると、トラ・7り5に対し磁気
検出素子1)がずれるたときパルスが発生するので、該
パルスの発生しない位置にW/R用磁気ヘッドを移動さ
せる。
Therefore, if the slice level L is set between characteristics B and C as shown by the dotted line in the figure, a pulse will be generated when the magnetic detection element 1) deviates from the 7-axis 5. Move the W/R magnetic head to a position where it is not used.

なお、第2図は本発明に係わる磁気検出部の幅と出力と
の関係を示す図であり、縦軸を出力電圧±へ■、横軸を
入力磁界の強さとしたとき、正弦波状の外部磁界が入力
し得られる出力は磁気検出部の幅が大きくなると増大す
る。即ち、磁気検出部の幅を8mmとした特性りと16
mn+にした特性Eは、図中に一点鎖線と実線とで示す
ように立ち上がり角度が異なり、外部磁界の移動を同一
にした特性Eは、特性りのそれより出力が大きくなる。
Note that FIG. 2 is a diagram showing the relationship between the width and output of the magnetic detection section according to the present invention, where the vertical axis represents the output voltage ± and the horizontal axis represents the strength of the input magnetic field. The output obtained by inputting a magnetic field increases as the width of the magnetic detection section increases. In other words, the characteristics when the width of the magnetic detection part is 8 mm are 16
The characteristic E with mn+ has different rise angles as shown by the dashed line and the solid line in the figure, and the characteristic E with the same movement of the external magnetic field has a larger output than the characteristic E.

なお、磁気検出素子1)において、狭幅磁気検出部12
aの長さβが外部磁界の幅より小さいとき、外部磁界が
長さlを越えない移動に対し、従来と同じ出力しか得ら
れない。他方、長さlが外部磁界の幅より大きいときは
、狭幅磁気検出部12aの出力に、広幅磁気検出部12
bまたは12cの一部分からの出力が重畳するため、そ
の分出力変化が小さくなる。従って、最も明確に外部磁
界のずれを検出するには、長さlを外部磁界の幅と同一
にしたときである。
Note that in the magnetic detection element 1), the narrow magnetic detection section 12
When the length β of a is smaller than the width of the external magnetic field, only the same output as the conventional one can be obtained for a movement in which the external magnetic field does not exceed the length l. On the other hand, when the length l is larger than the width of the external magnetic field, the output of the narrow magnetic detecting section 12a is connected to the wide magnetic detecting section 12.
Since the outputs from part of b or 12c are superimposed, the output change becomes smaller accordingly. Therefore, the deviation of the external magnetic field can be detected most clearly when the length l is made equal to the width of the external magnetic field.

第3図は本発明の他の実施例に係わる磁気検出素子の要
部を示す斜視図である。
FIG. 3 is a perspective view showing the main parts of a magnetic detection element according to another embodiment of the present invention.

第3図において、磁気検出素子21は長さ方向を容易磁
化軸とした磁気抵抗素子22に、良導電性等電位の細条
23および電極24をパターン形成してなる。
In FIG. 3, a magnetic detection element 21 is formed by forming a pattern of highly conductive equipotential strips 23 and electrodes 24 on a magnetoresistive element 22 whose axis of easy magnetization is in the longitudinal direction.

パーマロイ等の磁気異方性材料にてなり、その容易磁化
軸を長さ方向とした細長い磁気抵抗素子22は、長さ方
向の中央に位置する広幅磁気検出部22aと、検出部2
2aの外側の狭幅磁気検出部22b。
The elongated magnetoresistive element 22, which is made of a magnetically anisotropic material such as permalloy and whose axis of easy magnetization is in the longitudinal direction, has a wide magnetic detecting section 22a located at the center in the longitudinal direction, and a detecting section 2.
A narrow magnetic detection section 22b outside of 2a.

22cと、外部回路に接続するため検出部22b、 2
2cの外側にそれぞれ設けた接続部22d 、 22e
からなり、接続部22d 、 22eの上には最端位置
の細条23に接続する電極24が被着されている。
22c, and a detection section 22b, 2 for connection to an external circuit.
Connection parts 22d and 22e provided on the outside of 2c, respectively.
An electrode 24 connected to the strip 23 at the extreme end is attached on top of the connecting portions 22d and 22e.

かかる磁気検出素子21は、前記磁気検出素子1)の狭
幅磁気検出部12aと広幅磁気検出部12bを置き換え
た構成であり、広幅磁気検出部22aの長さを外部磁界
<vA気記憶媒体のトラックからの磁界)の幅と同一に
したとき、最も高精度に該外部磁界とのずれを検知でき
る。
This magnetic detection element 21 has a configuration in which the narrow magnetic detection part 12a and the wide magnetic detection part 12b of the magnetic detection element 1) are replaced, and the length of the wide magnetic detection part 22a is set such that the external magnetic field<vA of the magnetic storage medium. When the width is the same as that of the magnetic field from the track, the deviation from the external magnetic field can be detected with the highest accuracy.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明によれば、幅が異なる磁気検
出部を組み合わせ磁気検出素子を構成したことにより、
外部磁界の微小なずれも検出可能となり、高密度磁気デ
ィスクに使用するW/R磁気ヘッドのサーボ用磁気ヘッ
ドに応用したとき、記憶情報の書き込みおよび読み取り
を高精度にした効果が顕著である。
As explained above, according to the present invention, by configuring a magnetic detection element by combining magnetic detection parts with different widths,
Even minute deviations in the external magnetic field can be detected, and when applied to a servo magnetic head of a W/R magnetic head used in a high-density magnetic disk, the effect of increasing the accuracy of writing and reading stored information is remarkable.

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

第1図は本発明の一実施例に係わる磁気検出素子の斜視
図とその出力特性図、 第2図は本発明に係わる磁気検出部の幅と出力との関係
を示す図、 第3図は本発明の他の実施例に係わる磁気検出素子の斜
視図、 第4図は従来のバーバーポール型磁気検出素子の斜視図
、 第5図は従来の磁気検出素子の出力特性図、である。 図中において、 IL21は磁気検出素子、 12.22は磁気抵抗素子、 12a、22aは磁気検出部の中央部、12b、 12
c、 22b、 22cは磁気検出部の両側部、13.
23は等電位細条、 を示す。 (イ) δ (町 箒2図
FIG. 1 is a perspective view of a magnetic detection element according to an embodiment of the present invention and its output characteristic diagram. FIG. 2 is a diagram showing the relationship between the width and output of a magnetic detection section according to the present invention. FIG. FIG. 4 is a perspective view of a conventional barber-pole type magnetic detecting element; FIG. 5 is an output characteristic diagram of the conventional magnetic detecting element. In the figure, IL21 is a magnetic detection element, 12.22 is a magnetoresistive element, 12a, 22a are the central part of the magnetic detection part, 12b, 12
c, 22b, 22c are both sides of the magnetic detection section, 13.
23 indicates an equipotential strip. (b) δ (Town broom 2 diagram

Claims (2)

【特許請求の範囲】[Claims] (1)磁気異方性材料からなりその容易磁化軸方向を長
さとした長さ方向の中央部(12a)をその側部(12
b、12c)より狭幅または広幅に形成した細長い磁気
抵抗素子(12)を具え、該抵抗素子(12)にその該
容易磁化軸方向と30〜60度の角度で良導電材料から
なる等電位細条(13)を形成してなることを特徴とす
る磁気抵抗形磁気ヘッド。
(1) The central part (12a) is made of a magnetically anisotropic material and its length is in the direction of its easy magnetization axis, and the side part (12a) is
b, 12c) comprises an elongated magnetoresistive element (12) formed narrower or wider than the above, and an equipotential made of a highly conductive material is attached to the resistance element (12) at an angle of 30 to 60 degrees with the axis of easy magnetization. A magnetoresistive magnetic head characterized by forming strips (13).
(2)前記特許請求の範囲第1項において、前記中央部
(12a)の長さ(L_1)が磁気記憶媒体のトラック
幅とほぼ等しいことを特徴とする磁気抵抗形磁気ヘッド
(2) The magnetoresistive magnetic head according to claim 1, wherein the length (L_1) of the central portion (12a) is approximately equal to the track width of the magnetic storage medium.
JP29075186A 1986-12-04 1986-12-04 Magneto-resistance type magnetic head Pending JPS63142511A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29075186A JPS63142511A (en) 1986-12-04 1986-12-04 Magneto-resistance type magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29075186A JPS63142511A (en) 1986-12-04 1986-12-04 Magneto-resistance type magnetic head

Publications (1)

Publication Number Publication Date
JPS63142511A true JPS63142511A (en) 1988-06-14

Family

ID=17760057

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29075186A Pending JPS63142511A (en) 1986-12-04 1986-12-04 Magneto-resistance type magnetic head

Country Status (1)

Country Link
JP (1) JPS63142511A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5117319A (en) * 1987-02-18 1992-05-26 Alps Electric Co., Ltd. Magnetic movement sensing device
EP0777214A3 (en) * 1995-11-30 1998-11-11 Quantum Corporation Longitudinally biased magnetoresistive sensor having a concave shaped active region to reduce Barkhausen noise by achieving a substantially single magnetic domain state

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5117319A (en) * 1987-02-18 1992-05-26 Alps Electric Co., Ltd. Magnetic movement sensing device
EP0777214A3 (en) * 1995-11-30 1998-11-11 Quantum Corporation Longitudinally biased magnetoresistive sensor having a concave shaped active region to reduce Barkhausen noise by achieving a substantially single magnetic domain state

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