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JP4812064B2 - Magnetic sensor - Google Patents
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JP4812064B2 - Magnetic sensor - Google Patents

Magnetic sensor Download PDF

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Publication number
JP4812064B2
JP4812064B2 JP2001302723A JP2001302723A JP4812064B2 JP 4812064 B2 JP4812064 B2 JP 4812064B2 JP 2001302723 A JP2001302723 A JP 2001302723A JP 2001302723 A JP2001302723 A JP 2001302723A JP 4812064 B2 JP4812064 B2 JP 4812064B2
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Japan
Prior art keywords
magnetic
impedance
magnetic sensor
core
sensor
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JP2001302723A
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Japanese (ja)
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JP2003110161A (en
Inventor
亜希子 大島
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Tokin Corp
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NEC Tokin Corp
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Description

【0001】
【発明の属する技術分野】
本発明は、磁気を高感度、高精度に検出するための磁気センサに関し、特にインピーダンス変化を活用した磁気インピーダンスセンサに関するものである。
【0002】
【従来の技術】
この種の磁気センサは、磁性体に数MHz以上の高周波電圧を印加した場合に生ずる表皮効果の表皮深さが透磁率の平方の逆数に比例することと、この磁性体の透磁率が、外部磁場により大きく変動することから、磁性体のインピーダンスが外部磁場によって変動する性質を利用したものである。
【0003】
高透磁率の磁性体の外部磁場によるインピーダンス変動は、1MHz以上の高周波ドライブ電流で検出されるため、上記の効果を利用した磁気センサは磁気インピーダンスセンサとも呼ばれている。
【0004】
ところで、磁性体のインピーダンス変動を利用した磁気センサとしての応用の試みは、特開昭59−2204号に開示されている。
【0005】
さらに、1989年に第13回日本応用磁気学会において、加茂芳邦氏、島田寛氏により、磁性体を、薄膜とワイヤに形成した場合に関して、それぞれの高周波電気抵抗の外部磁場による変化について開示されている。
【0006】
その後、1992年に電気学会マグネディックス研究会にて毛利佳年雄氏らによって、ワイヤ形状で、従来のMR素子の10倍のインピーダンス変化率を持つ素子が開示されている。
【0007】
薄膜形状での開発も行われており、特開平8−75835号においては、磁性膜により固定磁気バイアスを加え、被検出磁界の変動によるインピーダンス変動を線形的に検出することが開示されている。
【0008】
本出願人は、特開平10−270774号にて、磁気インピーダンスセンサ素子基板上に、磁気検出コアを2辺組み入れたブリッジ回路を取り込み、抵抗辺と磁気検出コアのインピーダンスをほぼ等しくした構成を提案した。このような構成にすることで、磁気検出コアのインピーダンス変動を電圧変動として検出し、磁気検出感度の向上と、オフセット削減の機能を持たせることを実現した。
【0009】
さらに、特開2000−206217号において、抵抗辺を非磁性体にして小型化し、渦巻きコイル、薄膜コイル、磁性膜による磁気バイアス手段を提案した。
【0010】
また、非磁性基板上に高透磁率磁性膜を形成して構成され、直線が途中で複数回平行に折り返されて長手方向に対し垂直な方向となるように磁気異方性がつけられた素子が、特開平9−127218号において開示されている。このように、複数回折り返すことで、磁性膜の総延長を長くしても素子全体を短くし小型化できる。また、高インピーダンスになり、使用しやすい素子となる。
【0011】
【発明が解決しようとする課題】
しかしながら、これらの従来の素子では、線形範囲が狭く低感度領域が広いために、磁場の検出のための余分な処理回路が必要となるという問題があった。
【0012】
本発明は、上記の課題を解決し、線形範囲が広く、高感度領域が広い磁気センサを提供することにある。
【0013】
【課題を解決するための手段】
上記課題を解決するために、本発明によれば、磁性体に高周波電圧を印加した際に生じる表皮効果の表皮深さが外部磁場に対して変化することにより、前記磁性体のインピーダンスが変動する効果を利用した磁気センサにおいて、つづら折り構造で、長さ、幅の異なる複数の磁性膜を直列につないだ磁性コアを具備し、前記複数の磁性膜の各々のインピーダンス値が等しいことを特徴とする磁気センサが得られる。各々の磁性膜のインピーダンス値を、ほぼ等しくすることで、磁気特性を足し合わせる効果が大きくなる。
【0014】
また、本発明によれば、上記の磁気センサにおいて、前記複数の磁性膜の各々の幅が30%以上異なることを特徴とする磁気センサが得られる。
【0016】
また、本発明によれば、上記の磁気センサにおいて、前記磁性コアの幅に対する長さの比が600以下、10以上の範囲である磁気センサが得られる。磁性コアの幅に対する長さの比が、これより小さなものであると、感度が低くなり、大きなものは、反磁界の影響が大きくなり、磁区形成が困難になるためである。
【0017】
また、本発明において、磁性コアの長さは、数ミリ以内であることが、磁気センサの小型化のために好ましい。
【0018】
【発明の実施の形態】
以下に、本発明の実施の形態を説明する。
【0019】
(実施の形態1)
MI(磁気インピーダンス)効果を利用した実施の形態1の磁気センサを次のようにして作製した。まず、誘電体基板を洗浄し、フォトレジストにてマスキングして磁性膜をスパッタする。次に、リフトオフによりパターニングを行うことで、図1の形状のアモルファス磁性薄膜による磁性コア1を形成する。次いで、真空中で熱処理を行う。この熱処理によって磁性膜の横方向に磁化容易軸が形成され、磁気センサとしての感度が向上する。その後、電極も同様にリフトオフで形成することで、実施の形態1の磁気センサを得る。
【0020】
上記の方法によって作製した磁性コアの特性について、図2〜5にて示して説明する。図2に、磁性コアの幅を30%ずつ変えたときの磁気特性を示した。磁性コアの幅を変えるとき、幅が狭い場合は、バイアスポイント(インピーダンスの変化量が最大の時の外部磁界(Oe))を低いところに持つ特性が得られる。幅が広くなるにしたがってバイアスポイントは、高磁界側になる。これは、磁性コアの幅が狭い場合は、図3に示すように、還流磁区の割合が幅の広い素子(図4)に比べて大きい。磁気検出方向である素子長手方向に外部磁界が生じたとき、磁化回転が起きる領域が少ないため、磁化回転が容易に起こり、低磁場において磁化の向きが揃うものと考えられる。また、磁性コアの幅を30%未満で変えても効果は小さい。図5に、磁性コアの長さを変えた場合の磁気特性を示した。磁性コアの長さが変化するとき、幅が等しいならぼ磁性コアの長い方がインピーダンスは高く、短い方がインピーダンスは低い。バイアスポイントは、素子の長さが短い方が少し高い磁界に出現する。
【0021】
次に、図1の本発明の磁気センサにおける、幅の違う磁性膜をつづら形状に直列につないだときの磁性コアの特性について説明する。幅の異なる磁性コアをつづら折りにして直列につなぎ合わせることで、上記で説明した単体の磁性コアの特性を足し合わせた磁気特性が得られる。図6に、それぞれの特性を足し合わせた磁気特性を示した。幅が狭いものは長さを短くし、幅の広いものはコアの長さを長くすることで、それぞれの磁性コアのインピーダンスをほぼ等しくできる。インピーダンスが大きいものほど磁気特性への関与が大きくなるので、どの磁性コアも等しいインピーダンスとなるのが好ましい。
【0022】
従来の幅の等しい磁性膜からなるつづら折り構造の磁性コアの磁気特性を図7に示した。感度のない領域が数Oeあり、線形範囲が狭い傾向がある。磁性コアの長さと幅を変えてインピーダンス特性を設計すると、図6に示すように、線形範囲が広くなり、感度のない領域をなくすことができる。このように、素子の設計において磁気特性を制御できる。
【0023】
(実施の形態2)
実施の形態2の磁気センサを次のようにして作製した。まず、誘電体基板を洗浄し、磁性膜をスパッタする。次に、フォトレジストにてマスキングしてイオンミリング装置および他方式の湿式エッチングにてパターニングを行うことで、図1の形状のアモルファス磁性薄膜による磁性コア1を形成する。次いで、真空中で熱処理を行う。この熱処理によって、磁性膜の横方向に磁化容易軸が形成され、磁気センサのとしての感度が向上する。その後、フォトレジストにてマスキングして非磁性導体膜をスパッタする。リフトオフによりパターニングを行うことで電極を形成して、磁気センサを得る。この磁気センサは、実施の形態1と同様に、線形範囲が広くなり、感度のない領域をなくすことができる。
【0024】
(実施の形態3)
実施の形態3の磁気センサを次のようにして作製した。まず、誘電体基板を洗浄し、フォトレジストにてマスキングし、磁性膜を無電解めっきにて生成する。次に、リフトオフによりパターニングを行うことで、図1の形状のアモルファス磁性薄膜による磁性コア1が形成する。次いで、真空中で熱処理を行う。この熱処理によって磁性膜の横方向に磁化容易軸が形成され、磁気センサのとしての感度が向上する。その後、フォトレジストにてマスキングして非磁性導体膜をスパッタする。リフトオフによりパターニングを行うことで電極を形成して、磁気センサを得る。この磁気センサは、実施の形態1と同様に、線形範囲が広くなり、感度のない領域をなくすことができる。
【0025】
【発明の効果】
以上説明したように、本発明によれば、線形範囲が広く、高感度領域が広い磁気センサを提供することができた。
【図面の簡単な説明】
【図1】本発明の磁気センサにおける磁性コアの形状を示す平面図。
【図2】磁性コアの幅を変化させたときの外部磁界に対するインピーダンス変化及び磁気感度を示す図。図2(a)は、インピーダンスの変化を示す図。図2(b)は、磁気感度を示す図。
【図3】幅の狭い素子の磁区構造及び外部磁界を受けた時の磁区の変化の様子を示す図。図3(a)は、磁区構造を示す図。図3(b)は、磁区の変化の様子を示す図。
【図4】幅の広い素子の磁区構造及び外部磁界を受けた時の磁区の変化の様子を示す図。図4(a)は、磁区構造を示す図。図4(b)は、磁区の変化の様子を示す図。
【図5】磁性コアの長さを変化させたときの外部磁界に対するインピータンス変化及び磁気感度を示す図。図5(a)は、インピーダンスの変化を示す図。図5(b)は、磁気感度を示す図。
【図6】形状が異なる磁性コアを直列に接続したつづら素子を有する本発明の磁気センサにおける外部磁界に対するインピーダンス変化及び磁気感度を示す図。図6(a)は、インピーダンスの変化を示す図。図6(b)は、磁気感度を示す図。
【図7】磁性コアの幅が等しいつづら素子を有する従来の磁気センサにおける外部磁界に対するインピーダンス変化及び磁気感度を示す図。図7(a)は、インピーダンスの変化を示す図。図7(b)は、磁気感度を示す図。
【符号の説明】
1 磁性コア
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a magnetic sensor for detecting magnetism with high sensitivity and high accuracy, and more particularly to a magnetic impedance sensor utilizing impedance change.
[0002]
[Prior art]
In this type of magnetic sensor, the skin depth of the skin effect that occurs when a high frequency voltage of several MHz or more is applied to a magnetic material is proportional to the inverse of the square of the magnetic permeability, and the magnetic permeability of this magnetic material is Since it fluctuates greatly depending on the magnetic field, it utilizes the property that the impedance of the magnetic material fluctuates with an external magnetic field.
[0003]
Since the impedance fluctuation due to the external magnetic field of the magnetic material having high permeability is detected by a high frequency drive current of 1 MHz or more, the magnetic sensor using the above effect is also called a magnetic impedance sensor.
[0004]
By the way, an attempt of application as a magnetic sensor using impedance variation of a magnetic material is disclosed in Japanese Patent Laid-Open No. 59-2204.
[0005]
Furthermore, in 1989, at the 13th Japan Society of Applied Magnetics, Yoshikazu Kamo and Hiroshi Shimada disclosed changes in the high-frequency electrical resistance due to an external magnetic field when a magnetic material was formed into a thin film and a wire. Yes.
[0006]
Thereafter, Toshio Mohri et al. At the Institute of Electrical Engineers of Japan in 1992 disclosed a wire-shaped element having an impedance change rate 10 times that of a conventional MR element.
[0007]
Development in the form of a thin film is also underway, and Japanese Patent Application Laid-Open No. 8-75835 discloses that a fixed magnetic bias is applied by a magnetic film to linearly detect impedance fluctuations due to fluctuations in the detected magnetic field.
[0008]
In Japanese Patent Application Laid-Open No. 10-270774, the present applicant proposes a configuration in which a bridge circuit incorporating two sides of a magnetic detection core is incorporated on a magnetic impedance sensor element substrate, and the impedances of the resistance side and the magnetic detection core are substantially equal. did. By adopting such a configuration, it was possible to detect the impedance fluctuation of the magnetic detection core as a voltage fluctuation, and to provide the functions of improving the magnetic detection sensitivity and reducing the offset.
[0009]
Furthermore, in Japanese Patent Application Laid-Open No. 2000-206217, a magnetic bias means using a spiral coil, a thin film coil, and a magnetic film was proposed by reducing the size by making the resistance side nonmagnetic.
[0010]
Also, an element formed by forming a high-permeability magnetic film on a non-magnetic substrate and giving magnetic anisotropy so that a straight line is folded back several times in the middle to be perpendicular to the longitudinal direction. Is disclosed in JP-A-9-127218. In this way, by turning back multiple times, the entire element can be shortened and downsized even if the total extension of the magnetic film is lengthened. In addition, the impedance becomes high and the device is easy to use.
[0011]
[Problems to be solved by the invention]
However, these conventional devices have a problem that an extra processing circuit for detecting a magnetic field is required because the linear range is narrow and the low sensitivity region is wide.
[0012]
An object of the present invention is to solve the above problems and provide a magnetic sensor having a wide linear range and a wide high sensitivity region.
[0013]
[Means for Solving the Problems]
In order to solve the above-described problems, according to the present invention, the skin depth of the skin effect that occurs when a high frequency voltage is applied to a magnetic material changes with respect to an external magnetic field, whereby the impedance of the magnetic material varies. In the magnetic sensor using the effect, the magnetic sensor includes a magnetic core in which a plurality of magnetic films having different lengths and widths are connected in series with a zigzag folded structure, and the impedance values of the plurality of magnetic films are equal to each other. A magnetic sensor is obtained. By making the impedance values of the respective magnetic films substantially equal, the effect of adding the magnetic characteristics is increased.
[0014]
In addition, according to the present invention, in the above magnetic sensor, a magnetic sensor is obtained in which the width of each of the plurality of magnetic films is different by 30% or more.
[0016]
Moreover, according to the present invention, in the above magnetic sensor, a magnetic sensor having a length ratio to the width of the magnetic core in the range of 600 or less and 10 or more can be obtained. When the ratio of the length to the width of the magnetic core is smaller than this, the sensitivity is lowered, and when the ratio is larger, the influence of the demagnetizing field is increased, and the magnetic domain formation becomes difficult.
[0017]
In the present invention, the length of the magnetic core is preferably within a few millimeters in order to reduce the size of the magnetic sensor.
[0018]
DETAILED DESCRIPTION OF THE INVENTION
Hereinafter, embodiments of the present invention will be described.
[0019]
(Embodiment 1)
The magnetic sensor of the first embodiment using the MI (magnetic impedance) effect was manufactured as follows. First, the dielectric substrate is washed, masked with a photoresist, and a magnetic film is sputtered. Next, patterning is performed by lift-off to form the magnetic core 1 made of an amorphous magnetic thin film having the shape shown in FIG. Next, heat treatment is performed in a vacuum. By this heat treatment, an easy axis of magnetization is formed in the lateral direction of the magnetic film, and the sensitivity as a magnetic sensor is improved. Thereafter, the magnetic sensor of the first embodiment is obtained by similarly forming the electrodes by lift-off.
[0020]
The characteristics of the magnetic core produced by the above method will be described with reference to FIGS. FIG. 2 shows the magnetic characteristics when the width of the magnetic core is changed by 30%. When changing the width of the magnetic core, if the width is narrow, a characteristic having a low bias point (external magnetic field (Oe) when the amount of change in impedance is maximum) is obtained. As the width becomes wider, the bias point becomes the higher magnetic field side. When the width of the magnetic core is narrow, as shown in FIG. 3, the ratio of the return magnetic domain is larger than that of the wide element (FIG. 4). When an external magnetic field is generated in the longitudinal direction of the element, which is the direction of magnetic detection, since there are few regions where magnetization rotation occurs, it is considered that magnetization rotation occurs easily and the magnetization directions are aligned in a low magnetic field. Further, even if the width of the magnetic core is changed by less than 30%, the effect is small. FIG. 5 shows the magnetic characteristics when the length of the magnetic core is changed. When the length of the magnetic core changes, if the width is the same, the longer the magnetic core, the higher the impedance, and the shorter, the lower the impedance. The bias point appears in a slightly higher magnetic field when the element length is shorter.
[0021]
Next, the characteristics of the magnetic core in the magnetic sensor of the present invention shown in FIG. 1 when magnetic films having different widths are connected in series in a spelling shape will be described. By magnetically folding the magnetic cores having different widths and connecting them in series, the magnetic characteristics obtained by adding the characteristics of the single magnetic cores described above can be obtained. FIG. 6 shows magnetic characteristics obtained by adding the respective characteristics. When the width is narrow, the length is shortened, and when the width is wide, the length of the core is lengthened, so that the impedance of each magnetic core can be made substantially equal. Since the greater the impedance, the greater the contribution to the magnetic properties, it is preferable that all the magnetic cores have the same impedance.
[0022]
FIG. 7 shows the magnetic characteristics of a conventional magnetic core having a zigzag structure composed of magnetic films having the same width. There are several Oe insensitive areas and the linear range tends to be narrow. When the impedance characteristics are designed by changing the length and width of the magnetic core, as shown in FIG. 6, the linear range is widened and an insensitive region can be eliminated. In this way, the magnetic characteristics can be controlled in the element design.
[0023]
(Embodiment 2)
The magnetic sensor of Embodiment 2 was produced as follows. First, the dielectric substrate is cleaned and a magnetic film is sputtered. Next, masking with a photoresist and patterning with an ion milling apparatus and other types of wet etching form the magnetic core 1 made of an amorphous magnetic thin film having the shape shown in FIG. Next, heat treatment is performed in a vacuum. By this heat treatment, an easy axis of magnetization is formed in the lateral direction of the magnetic film, and the sensitivity as a magnetic sensor is improved. Thereafter, the non-magnetic conductor film is sputtered by masking with a photoresist. Electrodes are formed by patterning by lift-off to obtain a magnetic sensor. As in the first embodiment, this magnetic sensor has a wide linear range and can eliminate an insensitive region.
[0024]
(Embodiment 3)
The magnetic sensor according to the third embodiment was manufactured as follows. First, the dielectric substrate is cleaned, masked with a photoresist, and a magnetic film is formed by electroless plating. Next, patterning is performed by lift-off to form the magnetic core 1 made of an amorphous magnetic thin film having the shape shown in FIG. Next, heat treatment is performed in a vacuum. By this heat treatment, an easy axis of magnetization is formed in the transverse direction of the magnetic film, and the sensitivity as a magnetic sensor is improved. Thereafter, the non-magnetic conductor film is sputtered by masking with a photoresist. Electrodes are formed by patterning by lift-off to obtain a magnetic sensor. As in the first embodiment, this magnetic sensor has a wide linear range and can eliminate an insensitive region.
[0025]
【The invention's effect】
As described above, according to the present invention, a magnetic sensor having a wide linear range and a wide high sensitivity region can be provided.
[Brief description of the drawings]
FIG. 1 is a plan view showing the shape of a magnetic core in a magnetic sensor of the present invention.
FIG. 2 is a diagram showing impedance change and magnetic sensitivity with respect to an external magnetic field when the width of a magnetic core is changed. FIG. 2A is a diagram showing a change in impedance. FIG. 2B shows the magnetic sensitivity.
FIG. 3 is a diagram showing a magnetic domain structure of a narrow element and how a magnetic domain changes when an external magnetic field is received. FIG. 3A shows a magnetic domain structure. FIG. 3B is a diagram showing a state of change of magnetic domains.
FIG. 4 is a diagram showing a magnetic domain structure of a wide element and how the magnetic domain changes when receiving an external magnetic field. FIG. 4A shows a magnetic domain structure. FIG. 4B is a diagram showing a change in the magnetic domain.
FIG. 5 is a diagram showing changes in impedance and magnetic sensitivity with respect to an external magnetic field when the length of a magnetic core is changed. FIG. 5A is a diagram showing a change in impedance. FIG. 5B shows magnetic sensitivity.
FIG. 6 is a diagram showing an impedance change and magnetic sensitivity with respect to an external magnetic field in the magnetic sensor of the present invention having a spelling element in which magnetic cores having different shapes are connected in series. FIG. 6A shows a change in impedance. FIG. 6B shows magnetic sensitivity.
FIG. 7 is a diagram showing impedance change and magnetic sensitivity with respect to an external magnetic field in a conventional magnetic sensor having spelled elements having equal magnetic core widths. FIG. 7A shows a change in impedance. FIG. 7B shows the magnetic sensitivity.
[Explanation of symbols]
1 Magnetic core

Claims (3)

磁性体に高周波電圧を印加した際に生じる表皮効果の表皮深さが外部磁場に対して変化することにより、前記磁性体のインピーダンスが変動する効果を利用した磁気センサにおいて、つづら折り構造で、長さ、幅の異なる複数の磁性膜を直列につないだ磁性コアを具備し、前記複数の磁性膜の各々のインピーダンス値が等しいことを特徴とする磁気センサ。In the magnetic sensor using the effect that the impedance of the magnetic material varies due to the change in the skin depth of the skin effect caused by the application of high-frequency voltage to the magnetic material with respect to the external magnetic field, A magnetic sensor comprising a magnetic core in which a plurality of magnetic films having different widths are connected in series, and the impedance values of the plurality of magnetic films are equal . 請求項1記載の磁気センサにおいて、前記複数の磁性膜の各々の幅が30%以上異なることを特徴とする磁気センサ。2. The magnetic sensor according to claim 1, wherein the width of each of the plurality of magnetic films differs by 30% or more. 請求項1または2に記載の磁気センサにおいて、前記磁性コアの幅に対する長さの比が600以下、10以上の範囲にあることを特徴とする磁気センサ。 3. The magnetic sensor according to claim 1 , wherein a ratio of a length to a width of the magnetic core is in a range of 600 or less and 10 or more.
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