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JP2010190571A - Magnetic detector - Google Patents

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JP2010190571A
JP2010190571A JP2007144686A JP2007144686A JP2010190571A JP 2010190571 A JP2010190571 A JP 2010190571A JP 2007144686 A JP2007144686 A JP 2007144686A JP 2007144686 A JP2007144686 A JP 2007144686A JP 2010190571 A JP2010190571 A JP 2010190571A
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magnetic field
output
field strength
series circuit
output waveform
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Katsuya Kikuiri
勝也 菊入
Kiyoshi Sato
清 佐藤
Yoshito Sasaki
義人 佐々木
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Alps Alpine Co Ltd
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Alps Electric Co Ltd
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Priority to JP2007144686A priority Critical patent/JP2010190571A/en
Priority to PCT/JP2008/059678 priority patent/WO2008149711A1/en
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/02Measuring direction or magnitude of magnetic fields or magnetic flux
    • G01R33/06Measuring direction or magnitude of magnetic fields or magnetic flux using galvano-magnetic devices
    • G01R33/09Magnetoresistive devices
    • G01R33/093Magnetoresistive devices using multilayer structures, e.g. giant magnetoresistance sensors
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y25/00Nanomagnetism, e.g. magnetoimpedance, anisotropic magnetoresistance, giant magnetoresistance or tunneling magnetoresistance

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  • Crystallography & Structural Chemistry (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Magnetic Variables (AREA)
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a magnetic detector which, especially, can generate a magnetic field detection signal for a the magnetic field intensity change of an external magnetic field more easily as compared to the conventional technique, and enables standardization of an integrated circuit. <P>SOLUTION: A first output waveform A is acquired from a first output extraction portion of a first series circuit, and a second output waveform B is acquired from a second extraction portion of a second series circuit. The first and second output waveforms A and B cross each other, when an external magnetic field H in the (+) direction has a first magnetic field intensity H1, and when an external magnetic field H in the (-) direction has a second magnetic field intensity H2 respectively, and the relation in magnitude between the output values of the first output waveform A and the second output waveform B when the magnetic field intensity is larger than the first and second magnetic field intensities H1 and H2 reverses when the magnetic field intensity is smaller than the first and second magnetic field intensities H1 and H2. Thereby, the magnetic field detection signal with respect to the magnetic field intensity change of the external magnetic field can be generated more easily as compared to the conventional technique. <P>COPYRIGHT: (C)2010,JPO&INPIT

Description

本発明は、磁気抵抗効果素子を備えた磁気検出装置に係り、特に、磁界検知信号を従来に比べて簡単に生成でき、また集積回路の標準化を可能とした磁気検出装置に関する。   The present invention relates to a magnetic detection device including a magnetoresistive effect element, and more particularly, to a magnetic detection device that can easily generate a magnetic field detection signal as compared with the related art and can standardize an integrated circuit.

折畳み式携帯電話等の電子機器や冷蔵庫等の電化製品の開閉検知に磁気抵抗効果素子を用いた磁気検出装置(磁気センサ)を用いることが可能である。   It is possible to use a magnetic detection device (magnetic sensor) using a magnetoresistive effect element for opening / closing detection of an electronic device such as a folding cellular phone or an electrical appliance such as a refrigerator.

前記磁気抵抗効果素子は、外部磁界の磁界強度に対して電気抵抗値が変化するため、抵抗変化に基づく電圧変化によって磁気検出装置に侵入する外部磁界の磁界強度の強弱を検知することが可能である。   Since the magnetoresistive effect element changes its electric resistance value with respect to the magnetic field strength of the external magnetic field, it is possible to detect the strength of the magnetic field strength of the external magnetic field that enters the magnetic detection device by a voltage change based on the resistance change. is there.

前記磁気検出装置は、磁気抵抗効果素子や固定抵抗素子を備える抵抗素子部と、前記抵抗素子部に接続され、前記電圧変化に基づいて、オン信号あるいはオフ信号(磁界検知信号)を生成し出力するための集積回路(IC)とで構成される。
特開平10−82795号公報 特開2004−198186号公報 特開2004−20466号公報 特開平10−160748号公報
The magnetic detection device is connected to the resistance element portion including a magnetoresistive effect element and a fixed resistance element, and generates and outputs an on signal or an off signal (magnetic field detection signal) based on the voltage change. And an integrated circuit (IC).
Japanese Patent Laid-Open No. 10-82895 JP 2004-198186 A Japanese Patent Application Laid-Open No. 2004-20466 JP-A-10-160748

従来では、前記集積回路内に、前記磁界検知信号の生成のために必要な基準電圧を設定するために抵抗等を備えた基準電圧設定回路を設けて、基準電圧を調整することが必要であった。   Conventionally, it has been necessary to adjust a reference voltage by providing a reference voltage setting circuit including a resistor or the like in the integrated circuit to set a reference voltage necessary for generating the magnetic field detection signal. It was.

また基準電圧の調整は、例えば抵抗素子部を変更すればその都度、行う必要があり、かかる場合、集積回路自体を交換しなければならず、また抵抗素子部はそのままでも、基準電圧を変更したい場合には別の基準電圧に調整された集積回路に交換することが必要であったため、従来の構成では、集積回路を標準化できず、コスト高になった。   In addition, for example, adjustment of the reference voltage must be performed every time the resistance element portion is changed. In such a case, the integrated circuit itself must be replaced, and the reference voltage should be changed without changing the resistance element portion. In some cases, it was necessary to replace the integrated circuit with a different reference voltage, and the conventional configuration could not standardize the integrated circuit, resulting in an increase in cost.

上記に挙げた各特許文献には、上記した従来課題の認識はなく当然、それに対する解決手段も提示されていない。   In each of the above-mentioned patent documents, there is no recognition of the above-described conventional problems, and naturally no solution means is provided.

そこで本発明は上記従来の課題を解決するためのものであり、特に、外部磁界の磁界強度変化に対する磁界検知信号を従来に比べて簡単に生成でき、また集積回路の標準化を可能とした磁気検出装置を提供することを目的としている。   Accordingly, the present invention is to solve the above-described conventional problems, and in particular, magnetic detection that can easily generate a magnetic field detection signal for a change in magnetic field strength of an external magnetic field as compared with the conventional one, and enables standardization of an integrated circuit. The object is to provide a device.

本発明における磁気検出装置は、
複数の抵抗素子にて構成される第1直列回路及び第2直列回路を備える抵抗素子部と、前記第1直列回路の第1出力取り出し部及び前記第2直列回路の第2出力取り出し部から得られる出力値に基づいて磁界検知信号を生成するための制御部を備える集積回路と、を有し、
少なくとも前記第1直列回路には、外部磁界に対して電気抵抗値が変化する磁気抵抗効果を利用した磁気抵抗効果素子を備え、
前記第1出力取り出し部から得られる第1の出力波形と、前記第2出力取り出し部から得られる第2の出力波形は、(+)方向の外部磁界が第1の磁界強度のとき、及び、前記(+)方向とは逆方向の(−)方向の外部磁界が第2の磁界強度のときに夫々交わり、
前記第1の磁界強度及び前記第2の磁界強度よりも大きい磁界強度のときと、前記第1の磁界強度及び第2の磁界強度よりも小さい磁界強度のときとで、前記第1の出力波形と前記第2の出力波形との出力値の大小関係が反転しており、
前記制御部では、前記出力値の大小関係に基づいて前記磁界検知信号を生成することを特徴とするものである。
The magnetic detection device in the present invention is
Obtained from a resistance element portion including a first series circuit and a second series circuit constituted by a plurality of resistance elements, a first output extraction portion of the first series circuit, and a second output extraction portion of the second series circuit. An integrated circuit including a control unit for generating a magnetic field detection signal based on the output value obtained,
At least the first series circuit includes a magnetoresistive effect element using a magnetoresistive effect in which an electric resistance value changes with respect to an external magnetic field,
The first output waveform obtained from the first output extraction unit and the second output waveform obtained from the second output extraction unit are when the external magnetic field in the (+) direction has the first magnetic field strength, and When the external magnetic field in the (−) direction opposite to the (+) direction has the second magnetic field strength,
The first output waveform when the magnetic field strength is larger than the first magnetic field strength and the second magnetic field strength and when the magnetic field strength is smaller than the first magnetic field strength and the second magnetic field strength. And the magnitude relationship between the output values of the second output waveform is inverted,
The control unit generates the magnetic field detection signal based on the magnitude relationship of the output values.

本発明では、前記第1の出力波形と前記第2の出力波形との出力値の大小関係に基づいて磁界検知信号を生成しているので、従来のように、わざわざ、集積回路内に基準電圧設定回路を設ける必要がなく、従来に比べて簡単に検知信号を生成できる。また、本発明では、集積回路側を標準化することも可能である。   In the present invention, since the magnetic field detection signal is generated based on the magnitude relationship between the output values of the first output waveform and the second output waveform, the reference voltage is purposely included in the integrated circuit as conventionally. There is no need to provide a setting circuit, and the detection signal can be generated more easily than in the prior art. In the present invention, it is also possible to standardize the integrated circuit side.

また本発明では、前記第2直列回路にも前記磁気抵抗効果素子を備え、
前記第1の出力波形、および、前記第2の出力波形のどちらか一方は、外部磁界の磁界強度が(+)方向および(−)方向に大きくなるにつれて、出力値が徐々に大きくなる出力上昇領域を備え、
他方は、外部磁界の磁界強度が(+)方向および(−)方向に大きくなるにつれて、出力値が徐々に小さくなる出力降下領域を備え、
(+)方向の外部磁界側に現れる出力上昇領域と出力降下領域は、前記第1の磁界強度のときに交わり、(−)方向の外部磁界側に現れる出力上昇領域と出力降下領域は、前記第2の磁界強度のときに交わる構成であることが好ましい。
In the present invention, the second series circuit also includes the magnetoresistive element,
One of the first output waveform and the second output waveform has an output increase in which the output value gradually increases as the magnetic field strength of the external magnetic field increases in the (+) direction and the (−) direction. With areas,
The other has an output drop region in which the output value gradually decreases as the magnetic field strength of the external magnetic field increases in the (+) direction and the (−) direction,
The output increase region and the output decrease region appearing on the external magnetic field side in the (+) direction intersect at the first magnetic field strength, and the output increase region and the output decrease region appearing on the external magnetic field side in the (−) direction are A configuration that intersects at the second magnetic field strength is preferable.

また本発明では、前記第1直列回路には第1の磁気抵抗効果素子と第1の固定抵抗素子とを備え、前記第2直列回路には第2の磁気抵抗効果素子と第2の固定抵抗素子とを備え、入力端子側あるいはグランド端子側のどちらか一方に前記第1の磁気抵抗効果素子と前記第2の固定抵抗素子が、他方に、前記第2の磁気抵抗効果素子と前記第1の固定抵抗素子が夫々接続されており、
前記第1の磁気抵抗効果素子と前記第2の磁気抵抗効果素子は同じ膜構成であり、前記第1の固定抵抗素子と前記第2の固定抵抗素子は同じ膜構成であることが、上記した出力上昇領域あるいは出力下降領域を備えた第1の出力波形および第2の出力波形を適切に得ることができるとともに、温度係数(TCR)のばらつきを抑制でき好適である。
In the present invention, the first series circuit includes a first magnetoresistance effect element and a first fixed resistance element, and the second series circuit includes a second magnetoresistance effect element and a second fixed resistance. A first magnetoresistive effect element and the second fixed resistance element on one of the input terminal side and the ground terminal side, and the second magnetoresistive effect element and the first on the other side. Fixed resistance elements are connected respectively.
The first magnetoresistive effect element and the second magnetoresistive effect element have the same film configuration, and the first fixed resistance element and the second fixed resistance element have the same film configuration, as described above. The first output waveform and the second output waveform having an output increase region or an output decrease region can be appropriately obtained, and variations in temperature coefficient (TCR) can be suppressed, which is preferable.

また本発明では、前記第1の磁界強度、及び、前記第2の磁界強度を調整するための調整用抵抗を接続可能とした端子部が前記第1直列回路、前記第2直列回路の少なくともいずれか一方に接続して設けられていることが好ましい。   Further, in the present invention, the terminal portion that can be connected to an adjustment resistor for adjusting the first magnetic field strength and the second magnetic field strength is at least one of the first series circuit and the second series circuit. It is preferable to be connected to either of them.

これにより、集積回路を標準化しても、所定の抵抗値から成る調整用抵抗を前記端子部に取り付けるだけで簡単且つ自由に前記第1の磁界強度、及び前記第2の磁界強度を調整できる。   Thereby, even if the integrated circuit is standardized, the first magnetic field strength and the second magnetic field strength can be easily and freely adjusted simply by attaching an adjusting resistor having a predetermined resistance value to the terminal portion.

また本発明では、前記磁気抵抗効果素子は、巨大磁気抵抗効果(GMR効果)を利用したGMR素子であることが好ましい。これにより、ヒステリシスが小さい出力波形を適切に得ることができ、適切に外部磁界の磁界強度変化に対する磁界検知信号を生成することが可能である。   In the present invention, the magnetoresistive element is preferably a GMR element utilizing a giant magnetoresistive effect (GMR effect). Thereby, it is possible to appropriately obtain an output waveform having a small hysteresis and appropriately generate a magnetic field detection signal with respect to a change in the magnetic field strength of the external magnetic field.

また本発明では、前記磁気抵抗効果素子には、膜厚方向に磁化方向が固定された固定磁性層と、外部磁界に対して磁化方向が変動するフリー磁性層と前記固定磁性層と前記フリー磁性層との間に位置する非磁性中間層との積層部分を備え、無磁場状態での前記固定磁性層及びフリー磁性層の磁化方向は、外部磁界の方向に対して直交方向に揃えられていることが好ましい。これにより第1の磁界強度と第2の磁界強度をほぼ同じ強度に設定でき、外部磁界検知のタイミングを双極にてほぼ同じにすることが可能になる。   In the present invention, the magnetoresistive element includes a pinned magnetic layer whose magnetization direction is fixed in the film thickness direction, a free magnetic layer whose magnetization direction varies with respect to an external magnetic field, the pinned magnetic layer, and the free magnetic layer. It has a laminated part with a nonmagnetic intermediate layer located between the layers, and the magnetization direction of the pinned magnetic layer and the free magnetic layer in the absence of a magnetic field is aligned in a direction perpendicular to the direction of the external magnetic field It is preferable. As a result, the first magnetic field strength and the second magnetic field strength can be set to substantially the same strength, and the timing of external magnetic field detection can be made substantially the same with bipolar.

本発明の磁気検出装置によれば、外部磁界の磁界強度変化に対する磁界検知信号を従来に比べて簡単に生成でき、また集積回路の標準化が可能となる。   According to the magnetic detection device of the present invention, a magnetic field detection signal corresponding to a change in magnetic field strength of an external magnetic field can be generated more easily than in the prior art, and the integrated circuit can be standardized.

図1は本実施形態の磁気検出装置20の回路構成図である。
図1に示す本実施形態の磁気検出装置20は、抵抗素子部21と集積回路(IC)22とを有して構成される。
FIG. 1 is a circuit configuration diagram of a magnetic detection device 20 of the present embodiment.
A magnetic detection device 20 according to this embodiment shown in FIG. 1 includes a resistance element unit 21 and an integrated circuit (IC) 22.

前記抵抗素子部21には、第1の磁気抵抗効果素子23と第1の固定抵抗素子24とが第1出力取り出し部25を介して直列接続された第1直列回路26、第2の磁気抵抗効果素子27と第2の固定抵抗素子28とが第2出力取り出し部29を介して直列接続された第2直列回路30が設けられる。   The resistance element section 21 includes a first series circuit 26 in which a first magnetoresistive element 23 and a first fixed resistance element 24 are connected in series via a first output extraction section 25, a second magnetoresistance A second series circuit 30 in which the effect element 27 and the second fixed resistance element 28 are connected in series via the second output extraction unit 29 is provided.

図1に示すように前記集積回路22には、入力端子(電源)39、グランド端子42及び外部出力端子40が設けられている。   As shown in FIG. 1, the integrated circuit 22 is provided with an input terminal (power source) 39, a ground terminal 42, and an external output terminal 40.

また図1に示すように、前記抵抗素子部21の第1直列回路26と直列に調整用抵抗(固定抵抗素子)50を接続するための外付け用端子51,52が設けられている。   As shown in FIG. 1, external terminals 51 and 52 for connecting an adjustment resistor (fixed resistance element) 50 in series with the first series circuit 26 of the resistance element section 21 are provided.

前記入力端子39、グランド端子42および外部出力端子40は外部に露出しており、夫々図示しない機器側の端子部とワイヤボンディングやダイボンディング等で電気的に接続されている。また前記外付け用端子51,52は、磁気検出装置20の購入者が、前記磁気検出装置20の磁気感度を調整すべく、調整用抵抗(固定抵抗)50を簡単に接続できるように外部に露出していることが望ましい。   The input terminal 39, the ground terminal 42, and the external output terminal 40 are exposed to the outside, and are electrically connected to terminal portions on the device side (not shown) by wire bonding, die bonding, or the like. The external terminals 51 and 52 are externally provided so that a purchaser of the magnetic detection device 20 can easily connect an adjustment resistor (fixed resistor) 50 in order to adjust the magnetic sensitivity of the magnetic detection device 20. It is desirable to be exposed.

図1に示すように集積回路22内には、差動増幅器35とコンパレータ38とを有する制御部34が設けられている。   As shown in FIG. 1, a control unit 34 having a differential amplifier 35 and a comparator 38 is provided in the integrated circuit 22.

前記差動増幅器35の入力部に、前記第1直列回路26の第1出力取り出し部25及び第2直列回路30の第2出力取り出し部29が夫々、接続されている。   A first output extraction section 25 of the first series circuit 26 and a second output extraction section 29 of the second series circuit 30 are connected to the input section of the differential amplifier 35, respectively.

前記コンパレータ38の入力部は、前記差動増幅器35の出力部と接続され、前記コンパレータ38の出力部が前記外部出力端子40に接続されている。   The input part of the comparator 38 is connected to the output part of the differential amplifier 35, and the output part of the comparator 38 is connected to the external output terminal 40.

前記第1磁気抵抗効果素子23及び第2磁気抵抗効果素子27は、外部磁界の磁界強度変化に基づいて巨大磁気抵抗効果(GMR効果)を発揮するGMR素子である。   The first magnetoresistive element 23 and the second magnetoresistive element 27 are GMR elements that exhibit a giant magnetoresistive effect (GMR effect) based on a change in magnetic field strength of an external magnetic field.

図10に示すように、前記第1磁気抵抗効果素子23及び第2磁気抵抗効果素子27は共に、基板70上に、下から下地層60,シード層61、反強磁性層62、固定磁性層63、非磁性中間層64、フリー磁性層65、及び保護層66の順で積層されている。前記下地層60は、例えば、Ta,Hf,Nb,Zr,Ti,Mo,Wのうち1種または2種以上の元素の非磁性材料で形成される。前記シード層61は、NiFeCrあるいはCrで形成される。前記反強磁性層62は、元素α(ただしαは、Pt,Pd,Ir,Rh,Ru,Osのうち1種または2種以上の元素である)とMnとを含有する反強磁性材料、又は、元素αと元素α′(ただし元素α′は、Ne,Ar,Kr,Xe,Be,B,C,N,Mg,Al,Si,P,Ti,V,Cr,Fe,Co,Ni,Cu,Zn,Ga,Ge,Zr,Nb,Mo,Ag,Cd,Sn,Hf,Ta,W,Re,Au,Pb、及び希土類元素のうち1種または2種以上の元素である)とMnとを含有する反強磁性材料で形成される。例えば前記反強磁性層62は、IrMnやPtMnで形成される。前記固定磁性層63及びフリー磁性層65はCoFe合金、NiFe合金、CoFeNi合金等の磁性材料で形成される。また前記非磁性中間層64はCu等で形成される。また前記保護層66はTa等で形成される。前記固定磁性層63やフリー磁性層65は積層フェリ構造(磁性層/非磁性層/磁性層の積層構造であり、非磁性層を挟んだ2つの磁性層の磁化方向が反平行である構造)であってもよい。また前記固定磁性層63やフリー磁性層65は材質の異なる複数の磁性層の積層構造であってもよい。   As shown in FIG. 10, the first magnetoresistive effect element 23 and the second magnetoresistive effect element 27 are both on the substrate 70 from below, the underlayer 60, the seed layer 61, the antiferromagnetic layer 62, and the fixed magnetic layer. 63, a nonmagnetic intermediate layer 64, a free magnetic layer 65, and a protective layer 66 are laminated in this order. The underlayer 60 is made of, for example, a nonmagnetic material of one or more elements selected from Ta, Hf, Nb, Zr, Ti, Mo, and W. The seed layer 61 is made of NiFeCr or Cr. The antiferromagnetic layer 62 includes an anti-ferromagnetic material containing an element α (where α is one or more of Pt, Pd, Ir, Rh, Ru, and Os) and Mn. Or, element α and element α ′ (where element α ′ is Ne, Ar, Kr, Xe, Be, B, C, N, Mg, Al, Si, P, Ti, V, Cr, Fe, Co, Ni) , Cu, Zn, Ga, Ge, Zr, Nb, Mo, Ag, Cd, Sn, Hf, Ta, W, Re, Au, Pb, and rare earth elements are one or more elements) and It is formed of an antiferromagnetic material containing Mn. For example, the antiferromagnetic layer 62 is made of IrMn or PtMn. The pinned magnetic layer 63 and the free magnetic layer 65 are made of a magnetic material such as a CoFe alloy, a NiFe alloy, or a CoFeNi alloy. The nonmagnetic intermediate layer 64 is made of Cu or the like. The protective layer 66 is made of Ta or the like. The pinned magnetic layer 63 and the free magnetic layer 65 have a laminated ferrimagnetic structure (magnetic layer / nonmagnetic layer / magnetic layer laminated structure in which the magnetization directions of two magnetic layers sandwiching the nonmagnetic layer are antiparallel) It may be. The pinned magnetic layer 63 and the free magnetic layer 65 may have a laminated structure of a plurality of magnetic layers made of different materials.

前記第1磁気抵抗効果素子23及び第2磁気抵抗効果素子27では、前記反強磁性層62と前記固定磁性層63とが接して形成されているため磁場中熱処理を施すことにより前記反強磁性層62と前記固定磁性層63との界面に交換結合磁界(Hex)が生じ、前記固定磁性層63の磁化方向は一方向に固定される。図9では、前記固定磁性層63の磁化方向63aを矢印方向で示している。第1磁気抵抗効果素子23及び第2磁気抵抗効果素子27において前記固定磁性層63の磁化方向63aは共に図示X2方向である。   In the first magnetoresistive element 23 and the second magnetoresistive element 27, the antiferromagnetic layer 62 and the pinned magnetic layer 63 are formed in contact with each other. An exchange coupling magnetic field (Hex) is generated at the interface between the layer 62 and the pinned magnetic layer 63, and the magnetization direction of the pinned magnetic layer 63 is fixed in one direction. In FIG. 9, the magnetization direction 63a of the pinned magnetic layer 63 is indicated by the arrow direction. In the first magnetoresistive element 23 and the second magnetoresistive element 27, the magnetization direction 63a of the pinned magnetic layer 63 is the X2 direction shown in the drawing.

また、無磁場状態(外部磁界が作用していないとき)での前記フリー磁性層65の磁化方向65aは、第1磁気抵抗効果素子23と第2磁気抵抗効果素子27共に、図示X2方向である。よって無磁場状態では、前記固定磁性層63の磁化方向63aと前記フリー磁性層65の磁化方向65aは平行状態である。   In addition, the magnetization direction 65a of the free magnetic layer 65 in the absence of a magnetic field (when no external magnetic field is applied) is the X2 direction in the drawing for both the first magnetoresistance effect element 23 and the second magnetoresistance effect element 27. . Therefore, in the non-magnetic state, the magnetization direction 63a of the pinned magnetic layer 63 and the magnetization direction 65a of the free magnetic layer 65 are in a parallel state.

なお前記固定磁性層63とフリー磁性層65の磁化方向63a,65aは、反平行であってもよいが、以下では、前記固定磁性層63の磁化方向63aと前記フリー磁性層65の磁化方向65aは平行状態であるとして説明する。   The magnetization directions 63a and 65a of the pinned magnetic layer 63 and the free magnetic layer 65 may be antiparallel. Hereinafter, the magnetization direction 63a of the pinned magnetic layer 63 and the magnetization direction 65a of the free magnetic layer 65 will be described. Will be described as being in a parallel state.

外部磁界Hは図示X方向と直交する図示Y方向に向けて作用する。ここで、Y方向のうち図10の紙面方向に向う方向を(+)方向、紙面から離れる方向を(−)方向とする。   The external magnetic field H acts in the Y direction shown orthogonal to the X direction shown. Here, in the Y direction, the direction toward the paper surface in FIG. 10 is defined as the (+) direction, and the direction away from the paper surface is defined as the (−) direction.

図10のように、固定磁性層63の磁化方向63aとフリー磁性層65の磁化方向65aとが平行状態のとき前記磁気抵抗効果素子23,27の電気抵抗値は最も小さくなる。   As shown in FIG. 10, when the magnetization direction 63a of the pinned magnetic layer 63 and the magnetization direction 65a of the free magnetic layer 65 are in parallel, the electric resistance values of the magnetoresistive elements 23 and 27 are the smallest.

外部磁界Hが前記(+)方向へ作用すると、前記フリー磁性層65の磁化方向65aは、(+)方向に向けて変化し、(+)方向の外部磁界Hの磁界強度が大きくなるにつれて前記磁気抵抗効果素子23,27の電気抵抗値は徐々に大きくなっていく。   When the external magnetic field H acts in the (+) direction, the magnetization direction 65a of the free magnetic layer 65 changes toward the (+) direction, and the magnetic field strength of the external magnetic field H in the (+) direction increases as the magnetic field strength increases. The electric resistance values of the magnetoresistive effect elements 23 and 27 are gradually increased.

また外部磁界Hが前記(−)方向へ作用すると、前記フリー磁性層65の磁化方向65aは、(−)方向に向けて変化し、(−)方向の外部磁界Hの磁界強度が大きくなるにつれて前記磁気抵抗効果素子23,27の電気抵抗値は徐々に大きくなっていく。   When the external magnetic field H acts in the (−) direction, the magnetization direction 65a of the free magnetic layer 65 changes toward the (−) direction, and the magnetic field strength of the external magnetic field H in the (−) direction increases. The electric resistance values of the magnetoresistive effect elements 23 and 27 are gradually increased.

一方、第1固定抵抗素子24、及び、第2固定抵抗素子28は、いずれも外部磁界Hに対して電気抵抗値は変化しない。   On the other hand, the electrical resistance value of the first fixed resistance element 24 and the second fixed resistance element 28 does not change with respect to the external magnetic field H.

図10に示すように、第1固定抵抗素子24、及び、第2固定抵抗素子28は、前記第1磁気抵抗効果素子23や第2磁気抵抗効果素子27と同じ材料構成で形成されるが、前記第1磁気抵抗効果素子23や第2磁気抵抗効果素子27と異なって、フリー磁性層65と非磁性中間層64とが逆積層されている。すなわち、第1固定抵抗素子24、及び、第2固定抵抗素子28は、下から下地層60、シード層61、反強磁性層62、固定磁性層63、フリー磁性層65、非磁性中間層64、及び保護層66の順に積層される。前記フリー磁性層65は、前記固定磁性層63に接して形成されるため、第1磁気抵抗効果素子23や第2磁気抵抗効果素子27のように外部磁界に対して磁化変動せず、もはやフリー磁性層65として機能しない(固定磁性層63と同様に磁化方向が固定された磁性層である)。   As shown in FIG. 10, the first fixed resistance element 24 and the second fixed resistance element 28 are formed with the same material configuration as the first magnetoresistive effect element 23 and the second magnetoresistive effect element 27. Unlike the first magnetoresistive effect element 23 and the second magnetoresistive effect element 27, a free magnetic layer 65 and a nonmagnetic intermediate layer 64 are reversely stacked. That is, the first fixed resistance element 24 and the second fixed resistance element 28 are, from the bottom, the underlayer 60, the seed layer 61, the antiferromagnetic layer 62, the fixed magnetic layer 63, the free magnetic layer 65, and the nonmagnetic intermediate layer 64. , And the protective layer 66 in this order. Since the free magnetic layer 65 is formed in contact with the pinned magnetic layer 63, unlike the first magnetoresistive effect element 23 and the second magnetoresistive effect element 27, the magnetization does not fluctuate with respect to an external magnetic field and is no longer free. It does not function as the magnetic layer 65 (like the pinned magnetic layer 63, it is a magnetic layer whose magnetization direction is fixed).

このように、第1固定抵抗素子24、及び、第2固定抵抗素子28を、前記第1磁気抵抗効果素子23や第2磁気抵抗効果素子27と同じ材料構成で形成することで、前記第1磁気抵抗効果素子23及び第2磁気抵抗効果素子27の温度係数(TCR)および、各固定抵抗素子24、27の温度係数のばらつきを抑制できる。また、図1に示す第1磁気抵抗効果素子23、第2磁気抵抗効果素子27、第1固定抵抗素子24、及び第2固定抵抗素子28を、外部磁界Hが作用していない無磁場状態(外部磁界ゼロ)において全て同じ電気抵抗値に設定できる。   As described above, the first fixed resistance element 24 and the second fixed resistance element 28 are formed of the same material structure as that of the first magnetoresistive effect element 23 and the second magnetoresistive effect element 27, so that the first fixed resistance element 24 and the second fixed resistance element 28 are formed. Variations in the temperature coefficient (TCR) of the magnetoresistive effect element 23 and the second magnetoresistive effect element 27 and the temperature coefficient of the fixed resistance elements 24 and 27 can be suppressed. Further, the first magnetoresistance effect element 23, the second magnetoresistance effect element 27, the first fixed resistance element 24, and the second fixed resistance element 28 shown in FIG. All of them can be set to the same electric resistance value at zero external magnetic field.

入力端子39あるいはグランド端子42のどちらか一方に、第1磁気抵抗効果素子23と第2固定抵抗素子28が、他方に、第2磁気抵抗効果素子27と第1固定抵抗素子24が夫々接続されるが、以下では図1のように、第1磁気抵抗効果素子23と第2固定抵抗素子28がグランド端子42側に、第2磁気抵抗効果素子27と第1固定抵抗素子24とが入力端子39側に夫々接続されているものとして説明する。   The first magnetoresistance effect element 23 and the second fixed resistance element 28 are connected to either the input terminal 39 or the ground terminal 42, and the second magnetoresistance effect element 27 and the first fixed resistance element 24 are connected to the other, respectively. However, in the following, as shown in FIG. 1, the first magnetoresistance effect element 23 and the second fixed resistance element 28 are on the ground terminal 42 side, and the second magnetoresistance effect element 27 and the first fixed resistance element 24 are on the input terminal. The description will be made assuming that they are respectively connected to the 39 side.

図1に示す外付け用端子51,52に調整用抵抗50(調整抵抗R=0Ω)を接続せず、前記端子部51,52間を短絡させると、前記第1直列回路26の第1出力取り出し部25から得られる外部磁界Hに対する第1の出力波形Aと、前記第2直列回路30の第2出力取り出し部29から得られる外部磁界Hに対する第2の出力波形Bは、図2に示す状態にて現れる。なお、図2は従来技術を示す。   When the adjustment resistor 50 (adjustment resistor R = 0Ω) is not connected to the external terminals 51 and 52 shown in FIG. 1 and the terminal portions 51 and 52 are short-circuited, the first output of the first series circuit 26 is obtained. The first output waveform A with respect to the external magnetic field H obtained from the extraction unit 25 and the second output waveform B with respect to the external magnetic field H obtained from the second output extraction unit 29 of the second series circuit 30 are shown in FIG. Appears in state. FIG. 2 shows the prior art.

図2に示すように外部磁界Hがゼロのとき、第1の出力波形Aの出力値と第2の出力波形Bの出力値は同じ値になるが、それ以外のとき、第1の出力波形Aの出力値は、第2の出力波形Bの出力値よりも常に大きい。よって、差動増幅器35より得られる差動出力は、外部磁界Hに対して常に0(V)以上か、0(V)以下となる。このため、図2の出力波形の場合、差動増幅器35より得られる差動出力に対する基準電圧を0(V)よりも高い位置、あるいは、0(V)よりも低い位置に設定すべく、図1の集積回路に抵抗等で構成される基準電圧設定用回路を設けることが必要である。   As shown in FIG. 2, when the external magnetic field H is zero, the output value of the first output waveform A and the output value of the second output waveform B become the same value, but otherwise, the first output waveform The output value of A is always larger than the output value of the second output waveform B. Therefore, the differential output obtained from the differential amplifier 35 is always 0 (V) or more or 0 (V) or less with respect to the external magnetic field H. Therefore, in the case of the output waveform of FIG. 2, in order to set the reference voltage for the differential output obtained from the differential amplifier 35 to a position higher than 0 (V) or a position lower than 0 (V). It is necessary to provide a reference voltage setting circuit composed of a resistor or the like in one integrated circuit.

本実施形態では図1に示す外付け用端子51,52に調整用抵抗50を接続する。これにより、前記第1直列回路26の第1出力取り出し部25から得られる中点電位が変化する。図1の形態では、調整用抵抗50を接続することで、第1出力取り出し部25から得られる中点電位は小さくなる。   In this embodiment, the adjustment resistor 50 is connected to the external terminals 51 and 52 shown in FIG. As a result, the midpoint potential obtained from the first output extraction unit 25 of the first series circuit 26 changes. In the configuration of FIG. 1, the midpoint potential obtained from the first output extraction unit 25 is reduced by connecting the adjustment resistor 50.

図3は、抵抗値Rが91Ωの調整用抵抗50を接続した場合の第1の出力波形Aと第2の出力波形Bを示すグラフ、図4は、抵抗値Rが200Ωの調整用抵抗50を接続した場合の第1の出力波形Aと第2の出力波形Bを示すグラフ、図5は、抵抗値Rが330Ωの調整用抵抗50を接続した場合の第1の出力波形Aと第2の出力波形Bを示すグラフ、図6は、抵抗値Rが430Ωの調整用抵抗50を接続した場合の第1の出力波形Aと第2の出力波形Bを示すグラフ、図7は、抵抗値Rが560Ωの調整用抵抗50を接続した場合の第1の出力波形Aと第2の出力波形Bを示すグラフ、である。なお図3ないし図7はいずれもシミュレーション結果であり、ここで挙げた調整用抵抗50の具体的抵抗値は例示であって、調整用抵抗50の抵抗範囲を規制するものでなく、また後述する磁界強度H1,H2(感度磁界)の値も例示である。   FIG. 3 is a graph showing a first output waveform A and a second output waveform B when an adjustment resistor 50 having a resistance value R of 91Ω is connected, and FIG. 4 is an adjustment resistor 50 having a resistance value R of 200Ω. FIG. 5 is a graph showing the first output waveform A and the second output waveform B when connected, and FIG. 5 shows the first output waveform A and the second output waveform A when the adjustment resistor 50 having a resistance value R of 330Ω is connected. FIG. 6 is a graph showing the first output waveform A and the second output waveform B when the adjustment resistor 50 having a resistance value R of 430Ω is connected, and FIG. 7 shows the resistance value. It is a graph which shows the 1st output waveform A and the 2nd output waveform B at the time of connecting the adjustment resistance 50 whose R is 560 (ohm). 3 to 7 are simulation results, and the specific resistance value of the adjustment resistor 50 listed here is an example, and does not regulate the resistance range of the adjustment resistor 50, and will be described later. The values of the magnetic field strengths H1 and H2 (sensitivity magnetic field) are also examples.

第2の出力波形Bは、図2ないし図7において変わりないが、第1の出力波形Aは、前記調整用抵抗50を接続するとともに、調整抵抗を徐々に大きくすることで、全体的に出力値が低下して、図中の縦軸方向に降下し、前記第1の出力波形Aと第2の出力波形Bとが2点で交わるとともに、その交点が変動する。   The second output waveform B does not change in FIGS. 2 to 7, but the first output waveform A is output as a whole by connecting the adjusting resistor 50 and gradually increasing the adjusting resistor. The value decreases and falls in the direction of the vertical axis in the figure. The first output waveform A and the second output waveform B intersect at two points, and the intersection changes.

例えば図4を例に詳しく説明すると、第1の出力波形Aは、外部磁界Hの磁界強度が(+)方向に大きくなるにつれて、出力値が徐々に大きくなる第1の出力上昇領域A1と、外部磁界Hの磁界強度が(−)方向に大きくなるにつれて、出力値が徐々に大きくなる第2の出力上昇領域A2とを備える。   For example, referring to FIG. 4 as an example, the first output waveform A includes a first output increase area A1 in which the output value gradually increases as the magnetic field strength of the external magnetic field H increases in the (+) direction, A second output increase region A2 in which the output value gradually increases as the magnetic field strength of the external magnetic field H increases in the (−) direction.

また、第2の出力波形Bは、外部磁界Hの磁界強度が(+)方向に大きくなるにつれて、出力値が徐々に小さくなる第1の出力降下領域B1と、外部磁界Hの磁界強度が(−)方向に大きくなるにつれて、出力値が徐々に小さくなる第2の出力降下領域B2とを備える。   The second output waveform B includes the first output drop region B1 in which the output value gradually decreases as the magnetic field strength of the external magnetic field H increases in the (+) direction, and the magnetic field strength of the external magnetic field H is ( A second output drop region B2 in which the output value gradually decreases as the value increases in the-) direction.

図4に示すように、前記第1の出力上昇領域A1と前記第1の出力降下領域B1は、(+)方向の外部磁界Hが第1の磁界強度H1のときに交わり、前記第2の出力上昇領域A2と前記第2の出力降下領域B2は、(−)方向の外部磁界Hが第2の磁界強度H2のときに交わる。   As shown in FIG. 4, the first output increase region A1 and the first output decrease region B1 intersect when the external magnetic field H in the (+) direction is the first magnetic field strength H1, and the second output increase region A1 The output increase region A2 and the second output decrease region B2 intersect when the external magnetic field H in the (−) direction is the second magnetic field strength H2.

よって、図4に示すように、前記第1の磁界強度H1及び第2の磁界強度H2よりも大きい磁界強度のとき、前記第1の出力波形Aの出力値は、第2の出力波形Bの出力値よりも常に高く、一方、前記第1の磁界強度H1及び第2の磁界強度H2よりも小さい磁界強度のとき、前記第1の出力波形Aの出力値は、第2の出力波形Bの出力値よりも常に低い状態にある。   Therefore, as shown in FIG. 4, when the magnetic field strength is larger than the first magnetic field strength H1 and the second magnetic field strength H2, the output value of the first output waveform A is the second output waveform B. When the magnetic field strength is always higher than the output value and smaller than the first magnetic field strength H1 and the second magnetic field strength H2, the output value of the first output waveform A is the second output waveform B. It is always lower than the output value.

したがって差動増幅器35により得られた差動出力は、図8のように、外部磁界Hの磁界強度が絶対値で20Oeよりも大きいとき常に正値となり、前記磁界強度が絶対値で20Oeより小さいとき常に負値となる。   Therefore, the differential output obtained by the differential amplifier 35 is always positive when the magnetic field strength of the external magnetic field H is larger than 20 Oe in absolute value as shown in FIG. 8, and the magnetic field strength is smaller than 20 Oe in absolute value. Sometimes it is negative.

図1に示すコンパレータ38にて、例えば、差動出力が正値の場合、オン信号を生成し、差動出力が負値の場合、オフ信号を生成するように設定する。これにより、外部磁界Hの磁界強度が絶対値で20Oeよりも大きくなると差動出力は正値となってオン信号が生成され、外部磁界Hの磁界強度が絶対値で20Oeよりも小さくなると差動出力は負値となってオフ信号が生成される。   In the comparator 38 shown in FIG. 1, for example, an ON signal is generated when the differential output is a positive value, and an OFF signal is generated when the differential output is a negative value. Thereby, when the magnetic field strength of the external magnetic field H becomes larger than 20 Oe in absolute value, the differential output becomes a positive value and an ON signal is generated, and when the magnetic field strength of the external magnetic field H becomes smaller than 20 Oe in absolute value, the differential output becomes differential. The output is negative and an off signal is generated.

このように、本実施形態では、第1の出力波形Aと第2の出力波形Bとが第1の磁界強度H1のときと第2の磁界強度H2のときで交わり、しかも前記第1の磁界強度H1及び前記第2の磁界強度H2よりも大きい磁界強度のときと、前記第1の磁界強度H1及び第2の磁界強度H2よりも小さい磁界強度のときとで、前記第1の出力波形Aと前記第2の出力波形Bとの出力値の大小関係が反転するので、前記制御部34では、外部磁界Hの磁界強度変化に対する磁界検知信号(オン信号、オフ信号)を生成する際、前記第1の出力波形Aの出力値が前記第2の出力波形Bの出力値よりも大きくなるか、あるいは小さくなるか(図8の差動出力が正値となるか負値となるか)を判別することで、前記磁界検知信号の生成が可能である。   As described above, in the present embodiment, the first output waveform A and the second output waveform B intersect when the first magnetic field strength H1 and the second magnetic field strength H2, and the first magnetic field. The first output waveform A when the magnetic field intensity is larger than the intensity H1 and the second magnetic field intensity H2 and when the magnetic field intensity is smaller than the first magnetic field intensity H1 and the second magnetic field intensity H2. Since the magnitude relationship between the output values of the second output waveform B and the second output waveform B is reversed, the control unit 34 generates the magnetic field detection signal (on signal, off signal) with respect to the change in the magnetic field strength of the external magnetic field H. Whether the output value of the first output waveform A is larger or smaller than the output value of the second output waveform B (whether the differential output in FIG. 8 becomes a positive value or a negative value). By determining, the magnetic field detection signal can be generated.

よって従来のように、わざわざ、基準電圧設定用回路を集積回路22内に設けなくてもよく、また抵抗素子部21が変更されてもその都度、基準電圧の調整を行う必要がなく、従来に比べて簡単に磁界検知信号を生成できる。   Therefore, unlike the conventional case, the reference voltage setting circuit does not have to be provided in the integrated circuit 22, and it is not necessary to adjust the reference voltage each time the resistance element portion 21 is changed. Compared with this, the magnetic field detection signal can be easily generated.

図4では、オン信号とオフ信号が切り換わる外部磁界Hの磁界強度H1,H2(感度磁界)は±20Oeであったが、前記調整用抵抗50の抵抗値Rを変えれば、前記磁界強度H1,H2(感度磁界)の大きさも変化する。   In FIG. 4, the magnetic field strengths H1 and H2 (sensitivity magnetic field) of the external magnetic field H at which the ON signal and the OFF signal are switched are ± 20 Oe. However, if the resistance value R of the adjustment resistor 50 is changed, the magnetic field strength H1 is changed. , H2 (sensitivity magnetic field) also changes.

図3では、前記磁界強度H1,H2(感度磁界)は、±10Oe、図5では、前記磁界強度H1,H2(感度磁界)は、±30Oe、図6では、前記磁界強度H1,H2(感度磁界)は、±40Oe、図7では、前記磁界強度H1,H2(感度磁界)は、±50Oeである。   3, the magnetic field strengths H1, H2 (sensitivity magnetic field) are ± 10 Oe, in FIG. 5, the magnetic field strengths H1, H2 (sensitivity magnetic field) are ± 30 Oe, and in FIG. 6, the magnetic field strengths H1, H2 (sensitivity). Magnetic field) is ± 40 Oe, and in FIG. 7, the magnetic field strengths H1 and H2 (sensitivity magnetic fields) are ± 50 Oe.

よって集積回路22側を標準化しても、調整用抵抗50の抵抗値Rを変えることで、簡単且つ自由に前記磁界強度H1,H2(感度磁界)を変化させることが可能である。このように集積回路22を標準化して製造できるため製造コストを低減することが可能である。   Therefore, even if the integrated circuit 22 side is standardized, the magnetic field strengths H1 and H2 (sensitivity magnetic fields) can be easily and freely changed by changing the resistance value R of the adjustment resistor 50. In this way, since the integrated circuit 22 can be standardized and manufactured, the manufacturing cost can be reduced.

なお前記コンパレータ38では、図8に示すように、オン信号生成のための閾値(スレッショルドレベルLV1)を、差動出力0(V)よりもやや大きい値にて設定し、オフ信号生成の閾値(スレッショルドレベルLV2)を差動出力0(V)よりもやや小さい値にて設定する(シュミット・トリガー入力)。これにより、チャタリングを防止できる。   In the comparator 38, as shown in FIG. 8, the threshold for generating the on signal (threshold level LV1) is set to a value slightly larger than the differential output 0 (V), and the threshold for generating the off signal ( The threshold level LV2) is set to a value slightly smaller than the differential output 0 (V) (Schmitt trigger input). Thereby, chattering can be prevented.

図1に示す構成では、第1磁気抵抗効果素子23、第2磁気抵抗効果素子27、第1固定抵抗素子24、第2固定抵抗素子28の各抵抗値が同じになるように調整していたが、例えば、磁気抵抗効果素子23,27と固定抵抗素子24,28の抵抗値を異ならせることで、前記調整用抵抗50を設けずとも(外付け用端子51,52間を短絡)、図3ないし図7に示すように第1の出力波形Aと第2の出力波形Bを第1の磁界強度H1と第2の磁界強度H2にて、交差させることが出来る。   In the configuration shown in FIG. 1, the first magnetoresistive effect element 23, the second magnetoresistive effect element 27, the first fixed resistance element 24, and the second fixed resistance element 28 are adjusted to have the same resistance value. However, for example, by making the resistance values of the magnetoresistive effect elements 23 and 27 and the fixed resistance elements 24 and 28 different from each other, the adjustment resistor 50 is not provided (the external terminals 51 and 52 are short-circuited). As shown in FIGS. 3 to 7, the first output waveform A and the second output waveform B can be crossed by the first magnetic field strength H1 and the second magnetic field strength H2.

ただし上記の構成の場合でも、図1のように外付け用端子51,52を設けて、調整用抵抗50の接続を可能にすれば、集積回路22側を標準化しても、簡単且つ自由に前記磁界強度H1,H2(感度磁界)を変化させることが可能となる。   However, even in the case of the above configuration, if external terminals 51 and 52 are provided as shown in FIG. 1 and the adjustment resistor 50 can be connected, the integrated circuit 22 side can be standardized easily and freely. The magnetic field strengths H1 and H2 (sensitivity magnetic fields) can be changed.

また、第1磁気抵抗効果素子23、および第2磁気抵抗効果素子27は同じ膜構成であることで温度係数(TCR)のばらつきを小さくできる。また第1固定抵抗素子24および第2固定抵抗素子28も同じ膜構成であることで温度係数(TCR)のばらつきを小さくできる。このとき、前記第1固定抵抗素子24および第2固定抵抗素子28は前記第1磁気抵抗効果素子23、および第2磁気抵抗効果素子27と異なる材料構成であってもよいが、図10で説明したように材料構成を同じにすることで、簡単に全ての抵抗素子の無磁場状態での抵抗値を一定にでき、しかもより効果的に温度係数(TCR)のばらつきを小さくできる。そして、図1のように外付け用端子51,52を設けて、調整用抵抗50の接続を可能にすることで、安定した温度係数(TCR)を有するとともに、前記磁界強度H1,H2(感度磁界)を簡単且つ自由に変化させることが可能な磁気検出装置を得ることができ、より好適である。   Further, since the first magnetoresistive effect element 23 and the second magnetoresistive effect element 27 have the same film configuration, variation in temperature coefficient (TCR) can be reduced. Further, since the first fixed resistance element 24 and the second fixed resistance element 28 also have the same film configuration, variation in temperature coefficient (TCR) can be reduced. At this time, the first fixed resistance element 24 and the second fixed resistance element 28 may have a material structure different from that of the first magnetoresistive effect element 23 and the second magnetoresistive effect element 27, but will be described with reference to FIG. As described above, by using the same material configuration, it is possible to easily make the resistance values of all the resistance elements constant in the absence of a magnetic field, and to more effectively reduce the variation in temperature coefficient (TCR). Then, by providing external terminals 51 and 52 as shown in FIG. 1 and allowing the adjustment resistor 50 to be connected, the magnetic field strengths H1 and H2 (sensitivity) are obtained while having a stable temperature coefficient (TCR). A magnetic detection device capable of easily and freely changing the magnetic field) can be obtained, and is more preferable.

前記磁気抵抗効果素子23,27は、例えばAMR素子でもよいが、図10に示すように、巨大磁気抵抗効果(GMR効果)を利用したGMR素子であることが、ヒステリシスが小さい出力波形を適切に得ることができ、適切に外部磁界Hの磁界強度変化に対する検知信号を生成することができ好適である。   The magnetoresistive effect elements 23 and 27 may be, for example, AMR elements. However, as shown in FIG. 10, the GMR element using the giant magnetoresistive effect (GMR effect) can appropriately output an output waveform with small hysteresis. The detection signal for the change in the magnetic field strength of the external magnetic field H can be appropriately generated, which is preferable.

また図10に示すようにGMR素子で形成された前記磁気抵抗効果素子23,27には、膜厚方向に磁化方向が固定された固定磁性層63と、外部磁界に対して磁化方向が変動するフリー磁性層65と前記固定磁性層63と前記フリー磁性層65との間に位置する非磁性中間層64との積層部分を備え、無磁場状態(外部磁界Hがゼロ)での前記固定磁性層63及びフリー磁性層65の磁化方向は、外部磁界Hの方向(図示Y方向)に対して直交方向(図示X方向)に揃えられていることが好ましい。なおGMR素子以外にTMR素子を用いることも可能である。   As shown in FIG. 10, the magnetoresistive elements 23 and 27 formed of GMR elements have a pinned magnetic layer 63 whose magnetization direction is fixed in the film thickness direction, and a magnetization direction that fluctuates with respect to an external magnetic field. The pinned magnetic layer includes a laminated portion of a free magnetic layer 65, the pinned magnetic layer 63, and a nonmagnetic intermediate layer 64 positioned between the free magnetic layer 65 and has no magnetic field (external magnetic field H is zero). It is preferable that the magnetization directions of 63 and the free magnetic layer 65 are aligned in a direction orthogonal to the direction of the external magnetic field H (Y direction in the drawing) (X direction in the drawing). In addition to the GMR element, a TMR element can be used.

これにより図4に示すように、第1の出力波形A及び第2の出力波形Bを略V字形か、あるいは逆略V字形にできる。しかも、図3ないし図7に示すように、第1の磁界強度H1と第2の磁界強度H2をほぼ同じ強度に設定できる。したがって、(+)方向に外部磁界Hが作用した場合、(−)方向に外部磁界Hが作用した場合の双方において、同じタイミングで検知信号の生成・出力を行うことが可能である。   As a result, as shown in FIG. 4, the first output waveform A and the second output waveform B can be made substantially V-shaped or reverse substantially V-shaped. Moreover, as shown in FIGS. 3 to 7, the first magnetic field strength H1 and the second magnetic field strength H2 can be set to substantially the same strength. Therefore, it is possible to generate and output the detection signal at the same timing both when the external magnetic field H acts in the (+) direction and when the external magnetic field H acts in the (−) direction.

本実施形態の磁気検出装置20は折畳み式携帯電話等の携帯機器や冷蔵庫等の電化製品の例えば開閉検知に使用されるが、かかる場合、磁気検出装置20には(+)方向あるいは(−)方向からのどちらかの方向からのみの外部磁界Hが作用する。本実施形態の磁気検出装置20は双極検知が可能なので、磁気検出装置20に(+)方向の外部磁界Hおよび(−)方向の外部磁界のどちらが作用しても外部磁界Hを検知でき、しかもその検知を双極にて同じタイミングで行うことが可能である。よって前記磁気検出装置および磁石の予め定められた取り付け方向に対してどちらか一方を逆に取り付けてしまっても外部磁界Hの検知は可能であり、したがって、取り付けの作業性を向上できる。
また本実施形態の磁気検出装置であれば双極検知が必要な用途にも適用できる。
The magnetic detection device 20 of the present embodiment is used for, for example, opening / closing detection of portable devices such as a folding cellular phone and electrical appliances such as a refrigerator. In such a case, the magnetic detection device 20 has a (+) direction or (−). The external magnetic field H acts only from either direction from the direction. Since the magnetic detection device 20 of the present embodiment can perform bipolar detection, the external magnetic field H can be detected regardless of which of the external magnetic field H in the (+) direction and the external magnetic field in the (−) direction acts on the magnetic detection device 20. The detection can be performed at the same timing with bipolar. Therefore, the external magnetic field H can be detected even if one of the magnetic detection device and the magnet is attached in reverse with respect to the predetermined attachment direction, and therefore the workability of the attachment can be improved.
Further, the magnetic detection device of the present embodiment can be applied to uses that require bipolar detection.

図1の実施形態では、第1直列回路26に外付け用端子51,52が接続して設けられているが、第2直列回路30に接続して設けられていてもよく、また前記第1直列回路26及び第2直列回路30の双方に接続して設けられていてもよい。   In the embodiment of FIG. 1, external terminals 51 and 52 are connected to the first series circuit 26, but they may be connected to the second series circuit 30, and the first series circuit 26 may be connected to the first series circuit 26. It may be connected to both the series circuit 26 and the second series circuit 30.

また本実施形態では、磁気抵抗効果素子23,27は、第1直列回路26及び第2直列回路30の双方に設けられているが、例えば第2直列回路30を構成する2つの抵抗素子を共に固定抵抗素子としてもよい。このとき第2の出力波形Bは図9のように出力値が一定の直線状となるが、前記第1の出力波形Aは略V字形であり、前記第1の出力波形Aと第2の出力波形Bは、(+)方向及び(−)方向の外部磁界Hの対してそれぞれ前記磁界強度H1,H2(感度磁界)にて交わるので、図4及び図8にて説明したのと同様に、外部磁界Hの磁界強度変化に対する検知信号を生成する際、前記第1の出力波形Aの出力値が前記第2の出力波形Bとの出力値よりも大きくなるか、あるいは小さくなるか(差動出力が正値となるか負値となるか)を判別することで、前記検知信号の生成が可能である。   In the present embodiment, the magnetoresistive effect elements 23 and 27 are provided in both the first series circuit 26 and the second series circuit 30. For example, the two resistance elements constituting the second series circuit 30 are both combined. It may be a fixed resistance element. At this time, the second output waveform B is a straight line with a constant output value as shown in FIG. 9, but the first output waveform A is substantially V-shaped, and the first output waveform A and the second output waveform A Since the output waveform B intersects with the external magnetic field H in the (+) direction and the (−) direction at the magnetic field strengths H1 and H2 (sensitivity magnetic fields), respectively, as described with reference to FIGS. When generating a detection signal for a change in magnetic field strength of the external magnetic field H, whether the output value of the first output waveform A is larger or smaller than the output value of the second output waveform B (difference) The detection signal can be generated by determining whether the dynamic output is a positive value or a negative value.

本実施形態の磁気検出装置の回路構成図、The circuit block diagram of the magnetic detection apparatus of this embodiment, 調整抵抗Rが0Ωのときの外部磁界Hと第1の出力波形Aおよび第2の出力波形Bとの関係を示すグラフ、A graph showing the relationship between the external magnetic field H and the first output waveform A and the second output waveform B when the adjustment resistor R is 0Ω; 調整抵抗Rを図2より大きくしたときの外部磁界Hと第1の出力波形Aおよび第2の出力波形Bとの関係を示すグラフ、2 is a graph showing the relationship between the external magnetic field H and the first output waveform A and the second output waveform B when the adjustment resistor R is made larger than that in FIG. 調整抵抗Rを図3より大きくしたときの外部磁界Hと第1の出力波形Aおよび第2の出力波形Bとの関係を示すグラフ、3 is a graph showing the relationship between the external magnetic field H and the first output waveform A and the second output waveform B when the adjustment resistor R is made larger than that in FIG. 調整抵抗Rを図4より大きくしたときの外部磁界Hと第1の出力波形Aおよび第2の出力波形Bとの関係を示すグラフ、4 is a graph showing the relationship between the external magnetic field H and the first output waveform A and the second output waveform B when the adjustment resistor R is made larger than that in FIG. 調整抵抗Rを図5より大きくしたときの外部磁界Hと第1の出力波形Aおよび第2の出力波形Bとの関係を示すグラフ、A graph showing the relationship between the external magnetic field H and the first output waveform A and the second output waveform B when the adjustment resistor R is made larger than that in FIG. 調整抵抗Rを図6より大きくしたときの外部磁界Hと第1の出力波形Aおよび第2の出力波形Bとの関係を示すグラフ、6 is a graph showing the relationship between the external magnetic field H and the first output waveform A and the second output waveform B when the adjustment resistor R is larger than that in FIG. 差動出力と外部磁界Hとの関係を示すグラフ、A graph showing the relationship between the differential output and the external magnetic field H; 図3ないし図7とは異なる、第1の出力波形Aおよび第2の出力波形Bとの関係を示すグラフ、A graph showing a relationship between the first output waveform A and the second output waveform B, which is different from those shown in FIGS. 本実施形態の磁気抵抗効果素子と固定抵抗素子との断面図、Sectional drawing of the magnetoresistive effect element and fixed resistance element of this embodiment,

符号の説明Explanation of symbols

20 磁気検出素装置
21 抵抗素子部
22 集積回路(IC)
23 第1磁気抵抗効果素子
24 第1固定抵抗素子
25 第1出力取り出し部
26 第1直列回路
27 第2磁気抵抗効果素子
28 第2固定抵抗素子
29 第2出力取り出し部
30 第2直列回路
34 制御部
35 差動増幅器
38 コンパレータ
39 入力端子
40 外部出力端子
42 グランド端子
50 調整用抵抗
51、52 外付け用端子
62 反強磁性層
63 固定磁性層
64 非磁性中間層
65 フリー磁性層
66 保護層
70 基板
20 Magnetic Detection Element Device 21 Resistance Element Unit 22 Integrated Circuit (IC)
23 1st magnetoresistive effect element 24 1st fixed resistance element 25 1st output extraction part 26 1st series circuit 27 2nd magnetoresistance effect element 28 2nd fixed resistance element 29 2nd output extraction part 30 2nd series circuit 34 Control Unit 35 differential amplifier 38 comparator 39 input terminal 40 external output terminal 42 ground terminal 50 adjusting resistors 51 and 52 external terminal 62 antiferromagnetic layer 63 pinned magnetic layer 64 nonmagnetic intermediate layer 65 free magnetic layer 66 protective layer 70 substrate

Claims (6)

複数の抵抗素子にて構成される第1直列回路及び第2直列回路を備える抵抗素子部と、前記第1直列回路の第1出力取り出し部及び前記第2直列回路の第2出力取り出し部から得られる出力値に基づいて磁界検知信号を生成するための制御部を備える集積回路と、を有し、
少なくとも前記第1直列回路には、外部磁界に対して電気抵抗値が変化する磁気抵抗効果を利用した磁気抵抗効果素子を備え、
前記第1出力取り出し部から得られる第1の出力波形と、前記第2出力取り出し部から得られる第2の出力波形は、(+)方向の外部磁界が第1の磁界強度のとき、及び、前記(+)方向とは逆方向の(−)方向の外部磁界が第2の磁界強度のときに夫々交わり、
前記第1の磁界強度及び前記第2の磁界強度よりも大きい磁界強度のときと、前記第1の磁界強度及び第2の磁界強度よりも小さい磁界強度のときとで、前記第1の出力波形と前記第2の出力波形との出力値の大小関係が反転しており、
前記制御部では、前記出力値の大小関係に基づいて前記磁界検知信号を生成することを特徴とする磁気検出装置。
Obtained from a resistance element portion including a first series circuit and a second series circuit constituted by a plurality of resistance elements, a first output extraction portion of the first series circuit, and a second output extraction portion of the second series circuit. An integrated circuit including a control unit for generating a magnetic field detection signal based on the output value obtained,
At least the first series circuit includes a magnetoresistive effect element using a magnetoresistive effect in which an electric resistance value changes with respect to an external magnetic field,
The first output waveform obtained from the first output extraction unit and the second output waveform obtained from the second output extraction unit are when the external magnetic field in the (+) direction has the first magnetic field strength, and When the external magnetic field in the (−) direction opposite to the (+) direction has the second magnetic field strength,
The first output waveform when the magnetic field strength is larger than the first magnetic field strength and the second magnetic field strength, and when the magnetic field strength is smaller than the first magnetic field strength and the second magnetic field strength. And the magnitude relationship between the output values of the second output waveform is inverted,
The control unit generates the magnetic field detection signal based on a magnitude relationship between the output values.
前記第2直列回路にも前記磁気抵抗効果素子を備え、
前記第1の出力波形、および、前記第2の出力波形のどちらか一方は、外部磁界の磁界強度が(+)方向および(−)方向に大きくなるにつれて、出力値が徐々に大きくなる出力上昇領域を備え、
他方は、外部磁界の磁界強度が(+)方向および(−)方向に大きくなるにつれて、出力値が徐々に小さくなる出力降下領域を備え、
(+)方向の外部磁界側に現れる出力上昇領域と出力降下領域は、前記第1の磁界強度のときに交わり、(−)方向の外部磁界側に現れる出力上昇領域と出力降下領域は、前記第2の磁界強度のときに交わる請求項1記載の磁気検出装置。
The second series circuit also includes the magnetoresistive effect element,
One of the first output waveform and the second output waveform has an output increase in which the output value gradually increases as the magnetic field strength of the external magnetic field increases in the (+) direction and the (−) direction. With areas,
The other has an output drop region in which the output value gradually decreases as the magnetic field strength of the external magnetic field increases in the (+) direction and the (−) direction,
The output increase region and the output decrease region appearing on the external magnetic field side in the (+) direction intersect at the first magnetic field strength, and the output increase region and the output decrease region appearing on the external magnetic field side in the (−) direction are The magnetic detection device according to claim 1, which intersects at the second magnetic field strength.
前記第1直列回路には第1の磁気抵抗効果素子と第1の固定抵抗素子とを備え、前記第2直列回路には第2の磁気抵抗効果素子と第2の固定抵抗素子とを備え、入力端子側あるいはグランド端子側のどちらか一方に前記第1の磁気抵抗効果素子と前記第2の固定抵抗素子が、他方に、前記第2の磁気抵抗効果素子と前記第1の固定抵抗素子が夫々接続されており、
前記第1の磁気抵抗効果素子と前記第2の磁気抵抗効果素子は同じ膜構成であり、前記第1の固定抵抗素子と前記第2の固定抵抗素子は同じ膜構成である請求項2記載の磁気検出装置。
The first series circuit includes a first magnetoresistance effect element and a first fixed resistance element, and the second series circuit includes a second magnetoresistance effect element and a second fixed resistance element, The first magnetoresistance effect element and the second fixed resistance element are provided on either the input terminal side or the ground terminal side, and the second magnetoresistance effect element and the first fixed resistance element are provided on the other side. Each connected,
3. The first magnetoresistive effect element and the second magnetoresistive effect element have the same film configuration, and the first fixed resistance element and the second fixed resistance element have the same film configuration. Magnetic detection device.
前記第1の磁界強度、及び、前記第2の磁界強度を調整するための調整用抵抗を接続可能とした端子部が前記第1直列回路、前記第2直列回路の少なくともいずれか一方に接続して設けられている請求項1ないし3のいずれかに記載の磁気検出装置。   A terminal portion capable of connecting an adjustment resistor for adjusting the first magnetic field strength and the second magnetic field strength is connected to at least one of the first series circuit and the second series circuit. The magnetic detection device according to claim 1, wherein the magnetic detection device is provided. 前記磁気抵抗効果素子は、巨大磁気抵抗効果(GMR効果)を利用したGMR素子である請求項1ないし4のいずれかに記載の磁気検出装置。   The magnetic detection device according to claim 1, wherein the magnetoresistive element is a GMR element using a giant magnetoresistive effect (GMR effect). 前記磁気抵抗効果素子には、膜厚方向に磁化方向が固定された固定磁性層と、外部磁界に対して磁化方向が変動するフリー磁性層と前記固定磁性層と前記フリー磁性層との間に位置する非磁性中間層との積層部分を備え、無磁場状態での前記固定磁性層及びフリー磁性層の磁化方向は、外部磁界の方向に対して直交方向に揃えられている請求項5記載の磁気検出装置。   The magnetoresistive element includes a pinned magnetic layer whose magnetization direction is fixed in a film thickness direction, a free magnetic layer whose magnetization direction varies with respect to an external magnetic field, and the pinned magnetic layer and the free magnetic layer. 6. The magnetization direction of the pinned magnetic layer and the free magnetic layer in the absence of a magnetic field is provided in a direction perpendicular to the direction of the external magnetic field. Magnetic detection device.
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