JPH0418778A - Magnetoresistive device - Google Patents

Magnetoresistive device

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Publication number
JPH0418778A
JPH0418778A JP2122005A JP12200590A JPH0418778A JP H0418778 A JPH0418778 A JP H0418778A JP 2122005 A JP2122005 A JP 2122005A JP 12200590 A JP12200590 A JP 12200590A JP H0418778 A JPH0418778 A JP H0418778A
Authority
JP
Japan
Prior art keywords
magnetoresistive
intermediate terminal
elements
magnetic field
voltage
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
JP2122005A
Other languages
Japanese (ja)
Inventor
Shingo Usui
碓井 真吾
Masaaki Kusumi
雅昭 久須美
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.)
Sony Magnescale Inc
Original Assignee
Sony Magnescale 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 Sony Magnescale Inc filed Critical Sony Magnescale Inc
Priority to JP2122005A priority Critical patent/JPH0418778A/en
Publication of JPH0418778A publication Critical patent/JPH0418778A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain a magnetoresistive device where a midpoint potential hardly deviates in operation by a method wherein an external resistor is so adjusted as to make an average voltage between an output terminal and an intermediate terminal nearly half as high as a prescribed voltage. CONSTITUTION:Magnetoresistance elements 3 and 4 are formed on an alumina board 2 through evaporation, and a wiring pattern 5, external resistors 6 and 7, an intermediate terminal 8, and output terminals 9 and 10 are printed. In this case, the elements 3 and 4 are so disposed as to enable current flow paths 3a and 4a to extend crossing each other at right angles and connected in series. An intermediate terminal 8 is provided to a connection point 11 of the elements 3 and 4. Furthermore, the resistors 6 and 7 are connected to the elements 3 and 4 in series, and output terminals 9 and 10 are provided to the ends of the resistors 6 and 7 opposite to their ends connected to the elements 3 and 4. Furthermore, the magnetoresistance elements 3 and 4 are covered with a phenolic resin 50.

Description

【発明の詳細な説明】 [産業上の利用分野〕 本発明は、強磁性体磁気抵抗素子(以下、必要に応じて
磁気抵抗素子という)を使用し、例えば、位置センサと
して利用するのに好適な磁気抵抗装置に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention uses a ferromagnetic magnetoresistive element (hereinafter referred to as a magnetoresistive element as necessary), and is suitable for use as a position sensor, for example. The present invention relates to a magnetic resistance device.

[発明の概要] 本発明は、例えば、位置センサとして使用される磁気抵
抗装置において、電流通路の方向が相互に略直交して配
置されるとともに直列に接続される磁気抵抗素子と、こ
の磁気抵抗素子の接続点において形成される中間端子と
、それぞれの磁気抵抗素子に直列および/または並列に
接続される外部抵抗と、このそれぞれの外部抵抗の中間
端子側の反対側に形成される出力端子とを存するもので
、前記両出力端子間に所定電圧を加えた状態で、かつそ
れぞれの磁気抵抗素子を略飽和磁化以上の磁界中に磁界
と略直交する方向および磁界と略平行する方向に向きを
変更して配置し、向きを変更した前後における出力端子
と中間端子間における平均電圧が前記所定電圧の略1/
2の電圧になるように前記外部抵抗を調整することによ
り、磁気抵抗素子番こおける中点電位を正しく設定でき
るようにしたものである。
[Summary of the Invention] The present invention provides a magnetoresistive device used, for example, as a position sensor. An intermediate terminal formed at the connection point of the element, an external resistor connected in series and/or parallel to each magnetoresistive element, and an output terminal formed on the opposite side of the intermediate terminal side of each external resistor. With a predetermined voltage applied between both output terminals, each magnetoresistive element is oriented in a direction substantially perpendicular to the magnetic field and in a direction substantially parallel to the magnetic field in a magnetic field of approximately saturation magnetization or higher. The average voltage between the output terminal and the intermediate terminal before and after changing the arrangement and changing the direction is approximately 1/1/1 of the predetermined voltage.
By adjusting the external resistance so that the voltage becomes 2, the midpoint potential of the magnetoresistive element can be set correctly.

[従来の技術1 強磁性体磁気抵抗素子を有する磁気抵抗装置として、例
えば、特開昭箱62−293683号公報に開示された
技術がある。この技術は磁気抵抗素子ブロックと印刷抵
抗ブロックとを一体に構成し、印刷抵抗ブロックの印刷
抵抗を磁気抵抗素子に合わせてトリミングすることで、
中点電位からの子方向と一方向への出力電圧のずれが均
等になるようにしたものである。
[Prior Art 1] As a magnetoresistive device having a ferromagnetic magnetoresistive element, for example, there is a technology disclosed in Japanese Patent Laid-Open No. 62-293683. This technology integrates a magnetoresistive element block and a printed resistance block, and trims the printed resistance of the printed resistance block to match the magnetoresistive element.
The deviation of the output voltage from the midpoint potential in the child direction and in one direction is made equal.

[発明が解決しようとする課題1 しかしながら、上記従来の磁気抵抗装置では、第11図
に示すように、強磁性体磁気抵抗素子に固有の磁気ヒス
テリシスに起因して中点電位がずれているのを知らない
でトリミングを行ってしまうことになり、トリミングさ
れた磁気抵抗装置に実際に磁界が与えられた場合には、
中点電位がずれている七いう問題があった。
[Problem to be Solved by the Invention 1] However, in the conventional magnetoresistive device described above, as shown in FIG. If a magnetic field is actually applied to the trimmed magnetoresistive device,
There was a problem that the midpoint potential was off.

本発明はかかる点に鑑み、実際の使用状態において中点
電位がずれない磁気抵抗装置を提供することを目的とす
る。
In view of this, an object of the present invention is to provide a magnetoresistive device in which the midpoint potential does not shift during actual use.

[課題を解決するための手段コ 本発明磁気抵抗装置は、例えば、第1図および第2に示
すように1.電流通路(3a)、(4a)の方向が相互
に略直交して配置されるとともに直列に接続される磁気
抵抗素子(3)、(4)と、磁気抵抗素子(3)、(4
)の接続点(11)において形成される中間端子(8)
と、それぞれの磁気抵抗素子(3)、(4)に直列およ
び/または並列に接続される外部抵抗(6)、(7)と
、それぞれの外部抵抗(6)、(7)の中間端子(8)
側の反対側に形成される出力端子(9)、(10)とを
有し、この出力端子(9)、(10)間に所定電圧を加
えた状態で、かつそれぞれの磁気抵抗素子(3)、(4
)を略飽和磁化以−トの磁界中に磁界と略直交する方向
および磁界と略平行する方向に向きを変更して配置し、
向きを変更した前後における出力端子(9)と中間端子
(8)間における平均電圧(または出力端子(10)と
中間端子(8)間における平均電圧)が前記所定電圧の
略】/2の電圧になるように前記外部抵抗(6)、(7
)を調整したものである。
[Means for Solving the Problems] The magnetoresistive device of the present invention has the following features, for example, as shown in FIGS. Magnetoresistive elements (3), (4) are arranged in such a way that the directions of current paths (3a), (4a) are substantially orthogonal to each other and are connected in series;
) intermediate terminal (8) formed at the connection point (11) of
, external resistors (6), (7) connected in series and/or parallel to the respective magnetoresistive elements (3), (4), and intermediate terminals of the respective external resistors (6), (7) ( 8)
It has output terminals (9) and (10) formed on the opposite side of the side, and when a predetermined voltage is applied between the output terminals (9) and (10), and each magnetoresistive element (3 ), (4
) is placed in a magnetic field at approximately saturation magnetization or higher, with its orientation changed in a direction approximately perpendicular to the magnetic field and a direction approximately parallel to the magnetic field,
The average voltage between the output terminal (9) and the intermediate terminal (8) (or the average voltage between the output terminal (10) and the intermediate terminal (8)) before and after changing the direction is the predetermined voltage /2. The external resistors (6) and (7
) is adjusted.

[作用] したがって本発明によれば、出力端子(9)、(10)
間に所定電圧を加えた状態で、かつそれぞれの磁気抵抗
素子(3)、(4)を略飽和磁化以−七の磁界中に磁界
と直交する方向および磁界と平行する方向に向きを変更
して配置し、向きを変更した前後における出力端子(9
)と中間端子(8)間における平均電圧(または出力端
子(10)と中間端子(8)間における平均電圧)が前
記所定電圧の略1/2の電圧になるように前記外部抵抗
(6)、(7)を調整することにより、向きを変更した
前後における出力端子(9)と中間端子(8)から磁気
抵抗素子(3)側を見た平均の合成抵抗値と、向きを変
更した前後における出力端子(10)と中間端子(8)
から磁気抵抗素子(4)側を見た平均の合成抵抗値とを
互いに略等しい値にできる。
[Function] Therefore, according to the present invention, the output terminals (9), (10)
With a predetermined voltage applied between the magnetoresistive elements (3) and (4), the respective magnetoresistive elements (3) and (4) are placed in a magnetic field of approximately saturation magnetization or higher, and their orientations are changed in a direction perpendicular to the magnetic field and in a direction parallel to the magnetic field. the output terminals (9) before and after changing the orientation.
) and the intermediate terminal (8) (or the average voltage between the output terminal (10) and the intermediate terminal (8)) is approximately 1/2 of the predetermined voltage. , (7), the average combined resistance value when looking at the magnetoresistive element (3) side from the output terminal (9) and intermediate terminal (8) before and after changing the direction, and the average combined resistance value before and after changing the direction. Output terminal (10) and intermediate terminal (8) at
and the average combined resistance value when looking at the magnetoresistive element (4) side can be made approximately equal to each other.

[実施例] 以下、第1図〜第7図を参照しながら、この発明による
磁気抵抗装置の一実施例について説明する。
[Embodiment] Hereinafter, an embodiment of the magnetoresistive device according to the present invention will be described with reference to FIGS. 1 to 7.

第1図および第2図において、(1)は本実施例におけ
る磁気抵抗装置を示し、この磁気抵抗装置(1)は、ア
ルミナ基板(2)を含み、アルミナ基板(2)上には、
磁気抵抗素子(3)、(4)が蒸着技術により形成され
るとともに、配線パターン(5)、外部抵抗(6)、(
7)(以下、必要に応じて、抵抗という)、中間端子(
8)および出力端子(9)、(10)が印刷技術により
形成されている。この場合、磁気抵抗素子(3)、(4
)は、周知のように、実線でその方向が示される電流通
路(3a)、(4a)の方向が相互に略直交するように
配置されるとともに電気的に直列に接続されている。ま
た、この磁気抵抗素子(3)、(4)の接続点(11)
において中間端子(8)が形成されている。さらδこ、
抵抗(6L (7)は、それぞれ磁気抵抗素子(3)、
(4)に直列に接続され、この抵抗(6)、(7)にお
ける中間端子(8)の反対側にはそれぞれ出力端子(9
)、(10)が形成されている。なお、磁気抵抗素7−
(3)、(4)はフェノール樹脂(50)によって覆わ
れている。
In FIG. 1 and FIG. 2, (1) shows the magnetoresistive device in this example, and this magnetoresistive device (1) includes an alumina substrate (2), and on the alumina substrate (2),
Magnetoresistive elements (3), (4) are formed by vapor deposition technology, and wiring patterns (5), external resistors (6), (
7) (hereinafter referred to as a resistor as necessary), intermediate terminal (
8) and output terminals (9) and (10) are formed by printing technology. In this case, the magnetoresistive elements (3), (4
) are arranged so that the directions of the current paths (3a) and (4a), whose directions are shown by solid lines, are substantially perpendicular to each other, and are electrically connected in series. In addition, the connection point (11) between the magnetoresistive elements (3) and (4)
An intermediate terminal (8) is formed at. Sara δko,
The resistance (6L (7) is a magnetoresistive element (3),
(4) in series, and the resistors (6) and (7) have an output terminal (9) on the opposite side of the intermediate terminal (8), respectively.
), (10) are formed. In addition, the magnetoresistive element 7-
(3) and (4) are covered with phenolic resin (50).

第3図は前記磁気抵抗装置(1)の中点電位調整用ジグ
(12)の構成を示し、第4図はそのIV−IV線断面
にかかる斜視図を示す。第3図および第4図において、
中点電位調整用ジグ(12)は、ジグベース(13)を
含み、このジグヘース(13)上にば、辺部に凹部(1
4)、(15)を有するキャビティ(16)が形成され
るとともに、図示するように磁化されたマグネント(1
7)、(18)が埋め込まれている。このマグネント(
17)、(1B)の作用下に、キャビティ(16)の近
くに矢印で示す方向の略平等磁界へが生成される。なお
、この平等磁界Aは前記磁気抵抗素子(3)、(4)の
略飽和磁化以七の磁界の強さとなるようにマグネント(
17)、(18)を選択しておくものとする。
FIG. 3 shows the structure of the midpoint potential adjustment jig (12) of the magnetoresistive device (1), and FIG. 4 shows a perspective view taken along the line IV--IV. In Figures 3 and 4,
The midpoint potential adjustment jig (12) includes a jig base (13), and on the jig base (13), a recess (1
4), (15) is formed, and a magnetized magnet (1) is formed as shown in the figure.
7) and (18) are embedded. This magnet (
17), (1B), a substantially uniform magnetic field is generated near the cavity (16) in the direction indicated by the arrow. Note that this uniform magnetic field A is applied to the magnet (
17) and (18) are selected.

第5図は前記した磁気抵抗装置(1)(第1図参照)の
はめ込み用ジグ(19)を示し、このはめ込み用ジグ(
19)の辺部には前記キャビティク16)の四部(14
)、(15)に対応した凹部(20)、(21)が形成
されるとともに、磁気抵抗袋W(1)のはめ込み用の孔
部(22)が形成されている。
Fig. 5 shows the fitting jig (19) of the above-mentioned magnetoresistive device (1) (see Fig. 1).
The four parts (14) of the cavity 16) are attached to the sides of the cavity 19).
), (15) are formed, and a hole (22) for fitting the magnetic resistance bag W(1) is formed.

次に、−ト記実施例の動作について説明する。Next, the operation of the above embodiment will be explained.

まず、第5図に示すはめ込み用ジグ(19)の孔部(2
2)に第1図に示す磁気抵抗装置(1)をはめ込み、磁
気抵抗装置(1)のはめ込まれたはめ込み用ジグ(19
)の凹部(20)、(21)を第3図に示すジグベース
(13)のキャビティ(16)に形成された凹部(j4
)、(15)に合わせるようにして、磁気抵抗装置(1
)のはめ込まれたはめ込み用ジグ(19)をキャビティ
(16)内に挿入する(第6図参照)。
First, the hole (2) of the fitting jig (19) shown in FIG.
2), fit the magnetic resistance device (1) shown in Figure 1 into the fitting jig (19) into which the magnetic resistance device (1) is fitted.
) are formed in the cavity (16) of the jig base (13) shown in FIG.
), (15), and magnetoresistive device (1
) is inserted into the cavity (16) (see Fig. 6).

次に、第6図に示す状態において、第7図に示すように
、磁気抵抗装置(1)の中間端子(8)および出力端子
(9)、(10)に抵抗値の等しい抵抗(23)、(2
4)をブリッジ接続するとともに、所定電圧V。
Next, in the state shown in FIG. 6, as shown in FIG. ,(2
4) is bridge-connected and a predetermined voltage V is applied.

の電池(25)を抵抗(23)、(24)の両端子間に
接続する。ここで、抵抗(23)、 (24)の中間端
子(26)と磁気抵抗装置(1)の中間端子(8)間に
レーザトリミング装置(図示せず)を構成する電圧測定
用端子(図示せず)を接続し、その間の電圧V=V、を
測定する。この場合、第6図および第7図から理解され
るように、磁気抵抗素子(3)の電流通路(3a)と平
等磁界Aとは直交状態になり、電流通路(4a)と平等
磁界Aとは平行状態になる。
A battery (25) is connected between both terminals of the resistors (23) and (24). Here, a voltage measurement terminal (not shown) constituting a laser trimming device (not shown) is connected between the intermediate terminal (26) of the resistors (23) and (24) and the intermediate terminal (8) of the magnetoresistive device (1). ) and measure the voltage between them, V=V. In this case, as understood from FIGS. 6 and 7, the current path (3a) of the magnetoresistive element (3) and the uniform magnetic field A are orthogonal to each other, and the current path (4a) and the uniform magnetic field A becomes parallel.

次に、第8回に示すように、磁気抵抗装置(1)のはめ
込まれたはめ込み用ジグ(19)を第6図に示す方向か
ら時計方向に略90度回転した状態で、電圧V−V2を
測定する。この場合、第7図および第8図から理解され
るように、磁気抵抗素子(3)の電流通路(3a)と平
等磁界Aとは平行状態になり、電流通路(4a)と平等
磁界Aとは直交状態になる。
Next, as shown in the 8th episode, with the fitting jig (19) fitted into the magnetoresistive device (1) rotated approximately 90 degrees clockwise from the direction shown in FIG. Measure. In this case, as understood from FIGS. 7 and 8, the current path (3a) of the magnetoresistive element (3) and the uniform magnetic field A are in a parallel state, and the current path (4a) and the uniform magnetic field A becomes orthogonal.

そして、この状態において電圧1 v、 l ’−I 
V2となるように抵抗(6)または抵抗(7)をトリミ
ング(いわゆる、ファンクショントリミング)すること
により、出力端子(9)と中間端子(8)間(または出
力端子(10)と中間端子(8)間)における平均電圧
、すなわち、第6図の状態における出力端子(9)と中
間端子(8)間の電圧(または出力端子(10)と中間
端子(8)間における電圧)と第8図の状態における出
力端子(9)と中間端子(8)間の電圧(または出力端
子(10)と中間端子(8)間における電圧)との平均
電圧が前記所定電圧■。の略1/2の電圧になる。
In this state, the voltage 1 v, l'-I
By trimming the resistor (6) or resistor (7) (so-called function trimming) so that V2 ), that is, the voltage between the output terminal (9) and the intermediate terminal (8) (or the voltage between the output terminal (10) and the intermediate terminal (8)) in the state of FIG. The average voltage between the output terminal (9) and the intermediate terminal (8) (or the voltage between the output terminal (10) and the intermediate terminal (8)) in the state of is the predetermined voltage (2). The voltage will be approximately 1/2 of that.

したがって、l−リミング後においては、磁気抵抗素子
(3)、(4)の向きを変更した前(第6図)と後(第
8図)における出力端子(9)と中間端子(8)から磁
気抵抗素子(3)側を見た平均の合成抵抗値と、向きを
変更した前(第6図)と後(第8図)における出力端子
(10)と中間端子(8)から磁気抵抗素子(4)側を
見た平均の合成抵抗値とが互いに略等しい値になる。
Therefore, after L-rimming, from the output terminal (9) and the intermediate terminal (8) before (Fig. 6) and after (Fig. 8) the orientation of the magnetoresistive elements (3) and (4) is changed. The average combined resistance value when looking at the magnetoresistive element (3) side, and the magnetoresistive element from the output terminal (10) and intermediate terminal (8) before (Fig. 6) and after (Fig. 8) the direction has been changed. (4) The average combined resistance values when looking at the side are approximately equal to each other.

なお、出力端子(9)と中間端子(8)間等の電圧を直
接測定せずに中間端子(26)と中間端子(8)間の電
圧を測定するのは、向きを変更した前後における測定電
圧の変化率を大きくして測定誤差の影響を小さくするた
めである。
Note that measuring the voltage between the intermediate terminal (26) and the intermediate terminal (8) without directly measuring the voltage between the output terminal (9) and the intermediate terminal (8), etc. is the measurement before and after changing the direction. This is to increase the rate of change in voltage and reduce the influence of measurement errors.

ト記したように、本実施例によれば、磁気抵抗装置(1
)を構成する磁気抵抗素子(3)、(4)に飽和磁化以
上の磁界を加えながら、かつ磁界の方向を90度向きを
かえた前後における中間端子(26)と中間端子(8)
間の電圧■が略等しい値になるように抵抗(6)、(7
)をトリミングしているので、磁気ヒステリシスに起因
する中点電位のずれを除去することができるという効果
を奏する。したがって、磁気抵抗素子(1)を製造する
際の歩留りが向−Lするという利点も得られる。特に、
磁気抵抗装置を高精度位置センサとして使用する際にお
いても、予め磁気ヒステリシス範囲の小さい磁気抵抗素
子を選別する必要がなくなり、製造コストが低下すると
いう利点も得られる。
As mentioned above, according to this embodiment, the magnetoresistive device (1
) The intermediate terminal (26) and the intermediate terminal (8) before and after applying a magnetic field higher than saturation magnetization to the magnetoresistive elements (3) and (4) constituting the magnetic resistance elements (3) and (4) and changing the direction of the magnetic field by 90 degrees.
Connect resistors (6) and (7) so that the voltage between
) is trimmed, it is possible to eliminate a shift in the midpoint potential caused by magnetic hysteresis. Therefore, there is also an advantage that the yield when manufacturing the magnetoresistive element (1) is improved. especially,
Even when the magnetoresistive device is used as a high-precision position sensor, there is no need to select in advance a magnetoresistive element with a small magnetic hysteresis range, and there is an advantage that manufacturing costs are reduced.

第9図および第10図は、この発明の他の実施例の構成
およびその電気回路図を示すものである。
FIGS. 9 and 10 show the structure and electrical circuit diagram of another embodiment of the present invention.

なお、第9図および第10図において、第1図および第
2図に示すものと同じものには同じ符号をつけている。
In FIGS. 9 and 10, the same components as those shown in FIGS. 1 and 2 are given the same reference numerals.

第9図に示す磁気抵抗装置(101)は第1図に示す磁
気抵抗素子(1)の抵抗(6)、(7)に代替して抵抗
(106)、(107)を磁気抵抗素子(3)、(4)
に並列に接続したものである。したがって、この実施例
においても第7図と同様に外部回路を接続し、第6図と
第8図を参照して説明したよう乙こ抵抗(106)、(
107)をトリミングすることにより、磁気ヒステリシ
スに起因する中点電位のずれを除去することができる。
The magnetoresistive device (101) shown in FIG. 9 replaces the resistors (6) and (7) of the magnetoresistive element (1) shown in FIG. 1 with resistors (106) and (107). ), (4)
are connected in parallel. Therefore, in this embodiment as well, the external circuit is connected in the same way as in FIG. 7, and the resistor (106) and (
107), it is possible to remove the shift in the midpoint potential caused by magnetic hysteresis.

なお、L記の実施例においては、磁気抵抗装置(1)、
(101)の向きを90度回転するように構成している
が、これに限らず、マグネッ1−(17)、(18)を
90度回転するようムこしてもよい。また、予め磁化さ
れたマグネソh (17)、(18)、すなわち、永久
磁石に代替して電磁石を用いてもよい。また、電磁石あ
るいは空心コイル4個を正方形の各辺に配置して、対向
する2辺に置かれた電磁石あるいは空心コイル毎に交互
に電流を流すように構成することにより、磁界の方向を
自動的に90度回転するようにしてもよい。
In addition, in the embodiment described in L, the magnetoresistive device (1),
(101) is configured to be rotated by 90 degrees, but the present invention is not limited to this, and magnets 1-(17) and (18) may be rotated by 90 degrees. Furthermore, an electromagnet may be used in place of a pre-magnetized magnetometer (17), (18), that is, a permanent magnet. In addition, by arranging four electromagnets or air-core coils on each side of a square, and arranging current to flow alternately between the electromagnets or air-core coils placed on two opposing sides, the direction of the magnetic field can be automatically adjusted. It may also be rotated 90 degrees.

[発明の効果] 本発明によれば、磁気抵抗装置を構成する調整用の外部
抵抗の調整時に、この磁気抵抗装置を構成する磁気抵抗
素子に飽和磁化以上の磁界を加えながら調整しているの
で、磁気ヒステリシスに起因する中点電位のずれを木質
的に除去することができ、したがって、実際の使用状態
において、中点電位がずれることのない磁気抵抗装置が
得られるという効果を奏する。
[Effects of the Invention] According to the present invention, when adjusting the external resistance for adjustment constituting the magnetoresistive device, the adjustment is performed while applying a magnetic field higher than the saturation magnetization to the magnetoresistive element constituting the magnetoresistive device. , the shift in the midpoint potential caused by magnetic hysteresis can be effectively eliminated, and therefore, a magnetoresistive device can be obtained in which the midpoint potential does not shift in actual use.

なお、本発明は上述の実施例に限定されることなく、本
発明の要旨を逸脱しない範囲で種々変更し得ることは明
らかである。
Note that the present invention is not limited to the above-described embodiments, and it is clear that various changes can be made without departing from the gist of the present invention.

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

第1図は本発明による磁気抵抗装置の一実施例の構成を
示す斜視図、 第2図は第1図に示す磁気抵抗装置の回
路図、第3図は中点電位調整用ジグの平面図、第4図は
第3図に示す中点電位調整用ジグの■−■綿断面断面か
る斜視図、第5図は磁気抵抗装置はめ込み用ジグの斜視
図、第6図は磁気抵抗装置に平等磁界を加えている状態
を示す平面図、第7図は磁気抵抗装置を構成する外部抵
抗をトリミングする際の回路図、第8図は磁気抵抗装置
に第6図に示す状態に対して90度方向の異なる平等磁
界を加えている状態を示す平面図、第9図は本発明によ
る磁気抵抗装置の他の実施例の構成を示す斜視図、第1
0図は第9図に示す磁気抵抗装置の回路図、第11図は
従来技術における磁気ヒステリシスに起因する中点電位
のずれを示す説明に供する線図である。 (1)は磁気抵抗装置、(3)、(4)は磁気抵抗素子
、(3a)、(4a)は電流通路、(6)、(7)は外
部抵抗、(8)は中間端子、(9)、(10)は出力端
子である。
FIG. 1 is a perspective view showing the configuration of an embodiment of a magnetoresistive device according to the present invention, FIG. 2 is a circuit diagram of the magnetoresistive device shown in FIG. 1, and FIG. 3 is a plan view of a jig for adjusting the midpoint potential. , Fig. 4 is a perspective view of the jig for adjusting the mid-point potential shown in Fig. 3, showing the cross-section of the cross-section of the cotton, Fig. 5 is a perspective view of the jig for fitting the magnetoresistive device, and Fig. 6 is equivalent to the magnetoresistive device. A plan view showing the state in which a magnetic field is applied, Fig. 7 is a circuit diagram when trimming the external resistor that constitutes the magnetoresistive device, and Fig. 8 shows the magnetoresistive device at 90 degrees with respect to the state shown in Fig. 6. FIG. 9 is a plan view showing a state in which uniform magnetic fields in different directions are applied; FIG. 9 is a perspective view showing the configuration of another embodiment of the magnetoresistive device according to the present invention;
0 is a circuit diagram of the magnetoresistive device shown in FIG. 9, and FIG. 11 is a diagram for explaining the shift in midpoint potential caused by magnetic hysteresis in the prior art. (1) is a magnetoresistive device, (3) and (4) are magnetoresistive elements, (3a) and (4a) are current paths, (6) and (7) are external resistors, (8) is an intermediate terminal, ( 9) and (10) are output terminals.

Claims (1)

【特許請求の範囲】  電流通路の方向が相互に略直交して配置されるととも
に直列に接続される磁気抵抗素子と、磁気抵抗素子相互
の接続点において形成される中間端子と、 それぞれの磁気抵抗素子に直列および/または並列に接
続される外部抵抗と、 それぞれの外部抵抗の中間端子側の反対側に形成される
出力端子とを有し、 前記両出力端子間に所定電圧を加えた状態で、かつそれ
ぞれの磁気抵抗素子を略飽和磁化以上の磁界中に磁界と
略直交する方向および磁界と略平行する方向に向きを変
更して配置し、向きを変更した前後における出力端子と
中間端子間における平均電圧が前記所定電圧の略1/2
の電圧になるように前記外部抵抗を調整したことを特徴
とする磁気抵抗装置。
[Scope of Claims] Magnetoresistive elements whose current paths are arranged substantially perpendicular to each other and connected in series, an intermediate terminal formed at a connection point between the magnetoresistive elements, and each magnetic resistance element. It has an external resistor connected in series and/or parallel to the element, and an output terminal formed on the opposite side of the intermediate terminal side of each external resistor, and when a predetermined voltage is applied between the two output terminals. , and each magnetoresistive element is placed in a magnetic field of approximately saturation magnetization or higher with its orientation changed in a direction approximately perpendicular to the magnetic field and in a direction approximately parallel to the magnetic field, and between the output terminal and the intermediate terminal before and after changing the orientation. The average voltage at is approximately 1/2 of the predetermined voltage.
A magnetoresistive device characterized in that the external resistor is adjusted so that the voltage becomes .
JP2122005A 1990-05-11 1990-05-11 Magnetoresistive device Pending JPH0418778A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2122005A JPH0418778A (en) 1990-05-11 1990-05-11 Magnetoresistive device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2122005A JPH0418778A (en) 1990-05-11 1990-05-11 Magnetoresistive device

Publications (1)

Publication Number Publication Date
JPH0418778A true JPH0418778A (en) 1992-01-22

Family

ID=14825209

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2122005A Pending JPH0418778A (en) 1990-05-11 1990-05-11 Magnetoresistive device

Country Status (1)

Country Link
JP (1) JPH0418778A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0823127A (en) * 1994-07-05 1996-01-23 Matsushita Electric Ind Co Ltd Magnetoresistance element and manufacture
JPH0823129A (en) * 1994-07-08 1996-01-23 Matsushita Electric Ind Co Ltd Magnetoresistance element and manufacture

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0823127A (en) * 1994-07-05 1996-01-23 Matsushita Electric Ind Co Ltd Magnetoresistance element and manufacture
JPH0823129A (en) * 1994-07-08 1996-01-23 Matsushita Electric Ind Co Ltd Magnetoresistance element and manufacture

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