JPH0444371A - Magnetoresistance device - Google Patents

Magnetoresistance device

Info

Publication number
JPH0444371A
JPH0444371A JP2151497A JP15149790A JPH0444371A JP H0444371 A JPH0444371 A JP H0444371A JP 2151497 A JP2151497 A JP 2151497A JP 15149790 A JP15149790 A JP 15149790A JP H0444371 A JPH0444371 A JP H0444371A
Authority
JP
Japan
Prior art keywords
magnetic field
patterns
film patterns
thin film
ferromagnetic film
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
JP2151497A
Other languages
Japanese (ja)
Inventor
Michiko Endou
みち子 遠藤
Shigemi Kurashima
茂美 倉島
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 JP2151497A priority Critical patent/JPH0444371A/en
Publication of JPH0444371A publication Critical patent/JPH0444371A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain a highly saturated magnetic field and a required resistance value by forming a plurality of a thin ferromagnetic film patterns which are slender in parallel and striped electrodes which are common to the plurality of thin ferromagnetic film patterns. CONSTITUTION:Thin ferromagnetic film patterns 20 are arranged to wind mean deringly. A slit 22 is provided on the pattern located in a region subject a high outside magnetic field, thereby producing a plurality of stripes of thin patterns which are parallel to the thin ferrofmagnetic film patterns 20. More over, electrodes 21, which comprise Au or the like striped on the slant, are installed on the surface of the thin ferromagnetic film patterns 20. The electrode patterns 21 are installed so that they may be common to the plurality of stripes of patterns which go in parallel. This construction eliminates a marked differ ence between the electric resistance of the thin ferromagnetic film patterns and that of a region subject to a weak outside magnetic field, thereby increasing the saturated magnetic field in a section where the thin ferromagnetic film patterns are made slender. It is, therefore, possible to extend the range of detec tion magnetic field and moreover obtain a required resistance value.

Description

【発明の詳細な説明】 〔概 要〕 磁界を検出する磁気抵抗素子に関し、 飽和磁界が高く且つ所望の抵抗値を得ることを目的とし
、 強磁性薄膜を用いたバーバーポール型磁気抵抗素子にお
いて、平行する細長い複数の強磁性薄膜パターンと、そ
の複数の強磁性薄膜パターンに共通するように形成され
た縞状の電極パターンとより成るように構成する。
[Detailed Description of the Invention] [Summary] Regarding a magnetoresistive element that detects a magnetic field, the barber-pole magnetoresistive element using a ferromagnetic thin film aims to have a high saturation magnetic field and obtain a desired resistance value. It is composed of a plurality of parallel elongated ferromagnetic thin film patterns and a striped electrode pattern formed in common to the plurality of ferromagnetic thin film patterns.

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

本発明は磁界を検出する磁気抵抗素子に関する。 The present invention relates to a magnetoresistive element that detects a magnetic field.

磁気抵抗素子は高感度であるため磁気回路と組合わせて
角度センサや加速度センサなどに応用されている。その
とき、検出する磁界範囲、外乱磁界に対する耐ノイズ性
などの諸条件により、磁気抵抗素子の飽和磁界、感度、
抵抗などの最適値が決定される。そのため上記のような
緒特性が要求通り設計できることが必要とされる。
Magnetoresistive elements have high sensitivity, so they are used in combination with magnetic circuits in angle sensors, acceleration sensors, and the like. At that time, depending on various conditions such as the magnetic field range to be detected and noise resistance against disturbance magnetic fields, the saturation magnetic field, sensitivity,
Optimal values for resistance etc. are determined. Therefore, it is necessary to be able to design the above-mentioned characteristics as required.

〔従来の技術〕[Conventional technology]

従来のバーバーポール型磁気抵抗素子を第3図に示す。 A conventional barber pole type magnetoresistive element is shown in FIG.

これは同図に示すように酸化膜を成長させたシリコン基
板1に形成した抵抗体パターン2と外部接続素子3.4
.5を一体に接続した構成であり、抵抗体パターン2は
つづら折れ状に形成されたパーマロイ等の軟磁性薄膜6
に傾斜した縞状に導電体く例えば金)7が形成されてい
る。そして予め抵抗体パターン2をその長手方向に初期
磁化したのち、所定の電流を端子3,4.5間に印加し
、抵抗体パターン2の長さ方向と直交する外部磁界He
xを印加すると該抵抗体パターン2に抵抗値の変化が生
じ、この抵抗値変化から外部磁界Hexの有無を検出す
ることができるようになっている。
As shown in the figure, this consists of a resistor pattern 2 formed on a silicon substrate 1 on which an oxide film has been grown, and external connection elements 3 and 4.
.. 5 are integrally connected, and the resistor pattern 2 is a soft magnetic thin film 6 such as permalloy formed in a zigzag shape.
A conductive material (for example, gold) 7 is formed in a striped shape that is slanted. After initially magnetizing the resistor pattern 2 in its longitudinal direction, a predetermined current is applied between the terminals 3 and 4.5, and an external magnetic field He perpendicular to the length direction of the resistor pattern 2 is applied.
When x is applied, a change in resistance value occurs in the resistor pattern 2, and the presence or absence of an external magnetic field Hex can be detected from this change in resistance value.

第4図に上記の磁気抵抗素子を用いた加速度センサの概
念図を示す。これは同図に示すように基板10の上に、
先端に永久磁石11を有するばね12の一端が支持固定
され、永久磁石11の近傍に2つの磁気抵抗素子13a
、13bが配設されている。そして加速度が加わると、
ばね12が撓み、永久磁石11が振れる。この永久磁石
11の振れにより磁気抵抗素子13a、13bには磁界
の変化が生じ、この磁界強度の変化に応じた出力が磁気
抵抗素子から出力されるようになっている。
FIG. 4 shows a conceptual diagram of an acceleration sensor using the above magnetoresistive element. As shown in the figure, on the substrate 10,
One end of a spring 12 having a permanent magnet 11 at its tip is supported and fixed, and two magnetic resistance elements 13a are placed near the permanent magnet 11.
, 13b are arranged. And when acceleration is added,
The spring 12 bends and the permanent magnet 11 swings. This deflection of the permanent magnet 11 causes a change in the magnetic field in the magnetoresistive elements 13a, 13b, and the magnetoresistive elements output an output corresponding to the change in the magnetic field strength.

このような加速度センサでは、永久磁石11と磁気抵抗
素子13a・13bとの距離が小さいという構造上、永
久磁石11からの磁界は磁気抵抗素子チップ内で均一で
はない。ところが従来の磁気抵抗素子は第3図のように
チップ上のどの場所でも強磁性薄膜パターン6の幅が等
しいた約、感度や飽和磁界特性はチップ内で均一である
。そのだt永久磁石11からの磁界強度が強い部分(磁
気抵抗素子13a・13bの永久磁石11に近い部分)
は実際には飽和磁界以上の磁界が印加されていて、永久
磁石11の変位があっても、即ち磁界の変化があっても
全く出力の出ない状態になっている場合がある。
In such an acceleration sensor, since the distance between the permanent magnet 11 and the magnetoresistive elements 13a and 13b is small, the magnetic field from the permanent magnet 11 is not uniform within the magnetoresistive element chip. However, in the conventional magnetoresistive element, the width of the ferromagnetic thin film pattern 6 is the same everywhere on the chip as shown in FIG. 3, so the sensitivity and saturation magnetic field characteristics are uniform within the chip. That's the part where the magnetic field strength from the permanent magnet 11 is strong (the part near the permanent magnet 11 of the magnetoresistive elements 13a and 13b)
Actually, a magnetic field higher than the saturation magnetic field is applied, and even if there is a displacement of the permanent magnet 11, that is, a change in the magnetic field, there are cases where no output is produced at all.

反対に永久磁石11から遠い部分は磁界強度も弱く出力
が小さくなる。
On the contrary, the magnetic field strength is weak in the part far from the permanent magnet 11, and the output is small.

このため第5図に示すように、磁界の強い部分の強磁性
薄膜パターン6aは飽和磁界が高くなるように磁界の弱
い部分よりパターン幅を狭くしたものが提案されている
。(特願平2−61629号)〔発明が解決しようとす
る課題〕 従来の磁気抵抗素子では、飽和磁界を高くしようとする
と、強磁性薄膜の膜厚を厘くするか、パターン幅を細く
することで対応していた。
For this reason, as shown in FIG. 5, it has been proposed that the ferromagnetic thin film pattern 6a in the region where the magnetic field is strong has a narrower pattern width than the region where the magnetic field is weaker so that the saturation magnetic field becomes higher. (Patent Application No. 2-61629) [Problems to be Solved by the Invention] In conventional magnetoresistive elements, in order to increase the saturation magnetic field, it is necessary to reduce the thickness of the ferromagnetic thin film or narrow the pattern width. I was dealing with this.

そのだ約第5図の加速度センサ用磁気抵抗素子のように
不均一磁界を検出するたtの強磁性薄膜パターン6は磁
界の強い範囲と弱い範囲とではパターン幅が異なるもの
であった。しかしこの場合は、パターン幅が異なる部分
で素子の感度、飽和磁界はそれぞれ異なるものの、同一
膜厚のパターンであるため、パターン幅が異なると抵抗
値が異なり、磁気抵抗素子全体で見るとパターン幅が一
番細い部分の抵抗の割合が大きくなってしまうという問
題があった。
On the other hand, the ferromagnetic thin film pattern 6 for detecting a non-uniform magnetic field, such as the magnetoresistive element for an acceleration sensor shown in FIG. 5, has a pattern width that differs between a strong magnetic field range and a weak magnetic field range. However, in this case, although the sensitivity and saturation magnetic field of the element differ in parts with different pattern widths, since the patterns have the same thickness, the resistance value differs depending on the pattern width, and when looking at the entire magnetoresistive element, the pattern width There was a problem in that the ratio of resistance at the thinnest portion of the wire was increased.

本発明は上記従来の問題点に鑑み、飽和磁界が高く且つ
所望の抵抗値が得られる磁気抵抗素子を提供することを
目的とする。
SUMMARY OF THE INVENTION In view of the above conventional problems, an object of the present invention is to provide a magnetoresistive element that has a high saturation magnetic field and can obtain a desired resistance value.

〔課題を解決するための手段〕[Means to solve the problem]

上記目的を達成するために、本発明の磁気抵抗素子では
、強磁性薄膜を用いたバーバーポール型磁気抵抗素子に
おいて、平行する細長い複数の強磁性薄膜パターン20
と、その複数の強磁性薄膜パターン20に共通するよう
に形成された縞状の電極パターン21とより成ることを
特徴とする。
In order to achieve the above object, in the magnetoresistive element of the present invention, in a barber pole magnetoresistive element using a ferromagnetic thin film, a plurality of parallel elongated ferromagnetic thin film patterns 20
and a striped electrode pattern 21 formed in common to the plurality of ferromagnetic thin film patterns 20.

〔作 用〕[For production]

本発明の磁気抵抗素子は第1図の原理説明図に示すよう
に強磁性薄膜パターン20の幅が極約て小さくなってお
り、且つ電極パターン21が複数の強磁性薄膜パターン
20を並列にするように配置されているたと、飽和磁界
が高く (検出磁界範囲が広い)、且つ希望の抵抗値の
ものが得られる。
In the magnetoresistive element of the present invention, as shown in the principle explanatory diagram of FIG. 1, the width of the ferromagnetic thin film pattern 20 is extremely small, and the electrode pattern 21 arranges a plurality of ferromagnetic thin film patterns 20 in parallel. If arranged in this way, the saturation magnetic field will be high (the detected magnetic field range will be wide) and the desired resistance value will be obtained.

〔実施例〕〔Example〕

第2図は本発明の実施例を示す図である。同図において
、20は強磁性薄膜パターン、21は電極パターンであ
る。
FIG. 2 is a diagram showing an embodiment of the present invention. In the figure, 20 is a ferromagnetic thin film pattern, and 21 is an electrode pattern.

本実施例は同図に示すように、強磁性薄膜パターン20
をつづら折れ状とし、且つ外部磁界の強い領域にある部
分にはスリット22を入れて強磁性薄膜パターン20を
平行する複数条の細いパターンとし、外部磁界の弱い領
域にある部分にはスリットを入れずパターン幅は太いま
まとし、さらに、強磁性薄膜パターン20上には斜約縞
状のAu等からなる電極パターン21を設けている。こ
の電極パタ−ン21は、強磁性薄膜パターン20のパタ
ーン幅を細くした部分では、平行する複数条のパターン
に共通して設けられている。
In this embodiment, as shown in the figure, a ferromagnetic thin film pattern 20
The ferromagnetic thin film pattern 20 is made into a zigzag shape, and slits 22 are inserted in the region where the external magnetic field is strong, so that the ferromagnetic thin film pattern 20 has a plurality of parallel thin strips, and slits are inserted in the region where the external magnetic field is weak. The pattern width is kept wide, and furthermore, an oblique striped electrode pattern 21 made of Au or the like is provided on the ferromagnetic thin film pattern 20. This electrode pattern 21 is provided in common to a plurality of parallel patterns in the portion where the pattern width of the ferromagnetic thin film pattern 20 is narrowed.

このように構成された本実施例は、強磁性薄膜パターン
200幅が、外部磁界の強い領域では細くなっているが
、電極パターン21が複数の強磁性薄膜パターンを並列
にするように配置されているた給、該部分の強磁性薄膜
パターンの電気抵抗は外部磁界の弱い領域の部分と大差
がなくなる。また強磁性薄膜パターンを細くした部分は
飽和磁界が高くなる。従って検出磁界範囲が広くなり、
且つ希望の抵抗値のものが得られる。
In this embodiment configured in this way, the width of the ferromagnetic thin film pattern 200 is narrow in areas where the external magnetic field is strong, but the electrode pattern 21 is arranged so that a plurality of ferromagnetic thin film patterns are arranged in parallel. As a result, the electrical resistance of the ferromagnetic thin film pattern in this area is not much different from that in the area where the external magnetic field is weak. Furthermore, the saturation magnetic field becomes higher in the thinner part of the ferromagnetic thin film pattern. Therefore, the detection magnetic field range becomes wider,
Moreover, a desired resistance value can be obtained.

〔発明の効果〕〔Effect of the invention〕

以上説明した様に、本発明によれば、外部磁界の強い領
域にある強磁性薄膜パターンをパターン幅の細い複数の
パターンに分け、且つ該複数のパターンに共通する電極
パターンを設けることにより、核部の飽和磁界を高くで
き、且つ希望の抵抗値が得られるため、外部磁界の不均
一があっても、磁気飽和することなく磁界の変化を検出
することができ、高性能化を図ることができる。
As explained above, according to the present invention, a ferromagnetic thin film pattern in a region with a strong external magnetic field is divided into a plurality of narrow pattern width patterns, and a common electrode pattern is provided to the plurality of patterns, whereby the core Since the saturation magnetic field of the magnetic field can be increased and the desired resistance value can be obtained, changes in the magnetic field can be detected without magnetic saturation even if the external magnetic field is non-uniform, and high performance can be achieved. can.

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

第1図は本発明の原理説明図、 第2図は本発明の実施例を示す図、 第3図は従来のバーバーポール型磁気抵抗素子を示す図
、 第4図は磁気抵抗素子を用いた加速度センサを示す概念
図、 第5図は不均一磁界検出用の磁気抵抗素子を示す図であ
る。 図において、 20は強磁性薄膜パターン、 21は電極パターン を示す。 本発明の原理説明図 第1図 20・・・強磁性薄膜パターン 21・・・電極パターン ノ1 第3図 本発明の実施例を示す図 第2図 20・・・強磁性薄膜パターン 21・・・電極パターン 22・・・スリット センサを示す概念の 第4図
Fig. 1 is a diagram illustrating the principle of the present invention, Fig. 2 is a diagram showing an embodiment of the present invention, Fig. 3 is a diagram showing a conventional barber pole type magnetoresistive element, and Fig. 4 is a diagram showing a conventional barber pole type magnetoresistive element. A conceptual diagram showing an acceleration sensor. FIG. 5 is a diagram showing a magnetoresistive element for detecting a non-uniform magnetic field. In the figure, 20 indicates a ferromagnetic thin film pattern, and 21 indicates an electrode pattern. 20...Ferromagnetic thin film pattern 21...Electrode pattern No. 1 Fig. 3 Diagram showing an embodiment of the present invention Fig. 2 20...Ferromagnetic thin film pattern 21...・Electrode pattern 22...Fourth conceptual diagram showing a slit sensor

Claims (1)

【特許請求の範囲】 1、強磁性薄膜を用いたバーバーポール型磁気抵抗素子
において、 平行する細長い複数の強磁性薄膜パターン20と、その
複数の強磁性薄膜パターン20に共通するように形成さ
れた縞状の電極パターン21とより成ることを特徴とす
る磁気抵抗素子。
[Claims] 1. In a barber pole type magnetoresistive element using a ferromagnetic thin film, a plurality of parallel elongated ferromagnetic thin film patterns 20 and a plurality of ferromagnetic thin film patterns 20 formed in common to each other. A magnetoresistive element characterized by comprising a striped electrode pattern 21.
JP2151497A 1990-06-12 1990-06-12 Magnetoresistance device Pending JPH0444371A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2151497A JPH0444371A (en) 1990-06-12 1990-06-12 Magnetoresistance device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2151497A JPH0444371A (en) 1990-06-12 1990-06-12 Magnetoresistance device

Publications (1)

Publication Number Publication Date
JPH0444371A true JPH0444371A (en) 1992-02-14

Family

ID=15519797

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2151497A Pending JPH0444371A (en) 1990-06-12 1990-06-12 Magnetoresistance device

Country Status (1)

Country Link
JP (1) JPH0444371A (en)

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