JPS6237980A - Ferromagnetic reluctance apparatus - Google Patents

Ferromagnetic reluctance apparatus

Info

Publication number
JPS6237980A
JPS6237980A JP60177880A JP17788085A JPS6237980A JP S6237980 A JPS6237980 A JP S6237980A JP 60177880 A JP60177880 A JP 60177880A JP 17788085 A JP17788085 A JP 17788085A JP S6237980 A JPS6237980 A JP S6237980A
Authority
JP
Japan
Prior art keywords
ferromagnetic
thin film
magnetoresistive element
magnetic field
coil
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
JP60177880A
Other languages
Japanese (ja)
Inventor
Yoshi Yoshino
吉野 好
Hirohito Shiotani
塩谷 博仁
Kenichi Ao
建一 青
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.)
Denso Corp
Original Assignee
NipponDenso Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NipponDenso Co Ltd filed Critical NipponDenso Co Ltd
Priority to JP60177880A priority Critical patent/JPS6237980A/en
Publication of JPS6237980A publication Critical patent/JPS6237980A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N50/00Galvanomagnetic devices
    • H10N50/10Magnetoresistive devices

Abstract

PURPOSE:To manufacture a compact ferromagnetic reluctance apparatus readily by a simple constitution, by providing a thin film coil on an insulating substrate, and providing a ferromagnetic reluctance element in the coil so that the direction of magnetic lines of force agrees with the longitudinal direction. CONSTITUTION:On an insulating substrate 10 comprising glass and the like, many parallel conductors 31 are formed at a constant interval and coated with an insulating film 33. Thereafter, a ferromagnetic reluctance element 20 is formed on the film 33. Then, the element 20 is covered with an insulating film 35. The insulating films 33 and 35 at both end parts of each conductor 31 and at both end parts of the element 20 are removed. The end parts of the conductors 31 are connected with an upper conductor 39, and a thin film coil 30 is formed. At the same time of the formation of the conductor 39, terminals 41, 43 and 45 are formed. A current is conducted through the coil 30, and a bias magnetic field is imparted to the element 20.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、バイアス磁界を有する強磁性磁気抵坑装置に
関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a ferromagnetic magnetoresistive device with a bias magnetic field.

[従来の技術] 従来、強磁性薄膜を用いた磁気抵抗素子は磁気感度が良
好であるために、デジタル記録の再生ヘッドや、回転セ
ン4ノーの磁気−電気の変換素子として利用されている
。しかし、この磁気抵抗素子は、横軸に外部磁界強度を
示し縦軸に抵抗値を示す第5図の特性図に示されるよう
に、バルクハウゼン・ジャンプ(破線部90.92)や
、ヒステリシス特性に起因する検出出力の歪み(区間9
4部)等により、イの特性が不安定である。そこで、こ
の磁気抵抗素子の長手方向(F41化の容易軸方向)に
バイアス磁界を印加することで、この検出出力の不安定
な特性を改食する方法が提唱されている。
[Prior Art] Conventionally, a magnetoresistive element using a ferromagnetic thin film has good magnetic sensitivity, so it has been used as a reproducing head for digital recording and a magneto-electric conversion element for a rotation sensor. However, as shown in the characteristic diagram of FIG. 5, in which the horizontal axis represents the external magnetic field strength and the vertical axis represents the resistance value, this magnetoresistive element has a Barkhausen jump (dashed line portion 90.92) and hysteresis characteristics. Distortion of detection output due to (section 9
4) etc., the characteristics of A are unstable. Therefore, a method has been proposed to correct the unstable characteristics of the detection output by applying a bias magnetic field in the longitudinal direction of the magnetoresistive element (the direction of the easy axis of F41 conversion).

通常はこのバイアス磁界は永久磁石を用いて行なわれて
いる。即ち、磁気抵抗素子の近傍に磁界の向きを考慮し
て、永久磁石を正確に貼りつlフられている。
Usually, this bias magnetic field is created using a permanent magnet. That is, a permanent magnet is accurately pasted near the magnetoresistive element, taking into consideration the direction of the magnetic field.

[発明の解決しようとする問題点] しかし、永久磁石を正確1r二lit fl決めして貼
りつける必要から、その製造は生産f1が−にがらず、
従ってその製造コストは高いものになる。又、捷ibを
貼りつけるためにあまり小型化にもぐきないという欠点
があった。
[Problems to be Solved by the Invention] However, since it is necessary to accurately determine and affix the permanent magnets to 1r2litfl, the production f1 cannot be maintained.
Therefore, the manufacturing cost becomes high. Also, there was a drawback that it was not possible to reduce the size very much because of the attachment of the Socket IB.

そこで、本発明は、が1述した問題点をWI決した強磁
性磁気抵抗装置を提供4る事を目的とする。
SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide a ferromagnetic magnetoresistive device that overcomes the problems mentioned above.

[問題点を解決するための手段] 本発明の強磁性磁気抵抗装置は、絶縁基板と、前記絶縁
基板−Fに設けられ周囲の磁界強度に応じて電気抵抗が
変化する強磁性磁気抵抗素子と、前記絶縁基板−Fの前
記強磁性磁気抵抗素子の近傍に1110のコイル状で形
成され、通電電流に応じた強度の磁界を発生する@膜コ
イルと、前記強磁性磁気抵抗素子、前記薄膜コイルのそ
れぞれに設けられる接続端子とから構成される事を特徴
どする。
[Means for Solving the Problems] The ferromagnetic magnetoresistive device of the present invention includes an insulating substrate, a ferromagnetic magnetoresistive element that is provided on the insulating substrate-F and whose electrical resistance changes according to the strength of the surrounding magnetic field. , an @ film coil formed in a coil shape of 1110 near the ferromagnetic magnetoresistive element of the insulating substrate-F and generating a magnetic field of strength according to the applied current; the ferromagnetic magnetoresistive element; and the thin film coil. and a connection terminal provided on each of the.

本発明の強磁性磁気抵抗素子、1、従来の永久磁石を使
用するかわりに薄膜の]イルを形成し、この薄膜コイル
に電流を流すことにより必要とするバイアスの磁力を発
生させるものである。
Ferromagnetic magnetoresistive element of the present invention: 1. Instead of using a conventional permanent magnet, a thin film coil is formed, and a necessary bias magnetic force is generated by passing a current through the thin film coil.

本発明の強磁性磁気抵抗装置を構成する絶縁基−3= 板は、他の構成要素を保持し、所定の耐電)1特性と耐
電流特性を右Jる部材である。この絶縁基板と1ノで(
Jl例えば、ガラス基板、レラミックスM根、合成樹脂
基板等の(、Y来のも(根がそのまま利用できる。
The insulating base-3 plate constituting the ferromagnetic magnetoresistive device of the present invention is a member that holds other components and has predetermined electric withstand characteristics and current withstand characteristics. With this insulating board and one piece (
For example, glass substrates, Reramix M roots, synthetic resin substrates, etc. (Y) can be used as they are.

強磁↑り磁気抵抗素子tよ、磁界の存在下でこのta界
の強度に応じて電気抵抗値が変化づる磁気抵抗効果を有
Jる素子である。この磁気抵抗効果には、その材料に起
因と−4る物理効果と、ホール電界を起因とする形状効
果がある。人さな磁気抵抗すJ東を得るには、材料とし
て通常N1−C,oが用いられる。この強磁性磁気抵抗
素子は、ぞの形状が例えば矩形の薄膜状として、この絶
縁基板上に形成される。
A ferromagnetic magnetoresistive element is an element that has a magnetoresistive effect in which the electrical resistance value changes depending on the strength of the field in the presence of a magnetic field. This magnetoresistive effect includes a physical effect caused by the material and a shape effect caused by the Hall electric field. To obtain a small magnetoresistive material, N1-C,o is usually used as a material. The ferromagnetic magnetoresistive element is formed as a thin film having a rectangular shape, for example, on the insulating substrate.

薄膜コイルは、この強磁性磁気抵抗素子の近傍に設け1
うれる。ここC薄膜コイルどは巻線が形成覆るループを
真円より楕円さらに押しつぶしたものである。具体的に
は]イルバネを中心軸を通る平面で切断した時に多数の
平行した線分よりなる下方部ど上方部に分割される。こ
の下方部の各コイル線分を各々直線状とし、基板面に形
成する。
A thin film coil is provided near this ferromagnetic magnetoresistive element.
I'm happy. Here, the C thin film coil is made by compressing the loop formed by the winding wire into an elliptical shape rather than a perfect circle. Specifically, when the spring is cut along a plane passing through the central axis, it is divided into a lower part and an upper part, each consisting of a large number of parallel line segments. Each of the coil line segments in the lower part is formed into a straight line and formed on the substrate surface.

その後そのにに絶縁層を形成し、ついでイの上方に上方
部を形成するとともに上方部と下方部の各線分を電気的
に接続し、全体として薄板状のコイル状としたものであ
る。この薄膜コイルとこの強磁性磁気抵抗素子は、その
相対的なイ装置により、この薄膜コイルが発生する磁界
により、この強磁性磁気抵抗素子に所定の値以上の抵抗
値を変化させるような距離をもって配設される必要があ
る。
After that, an insulating layer is formed thereon, and then an upper part is formed above A, and the line segments of the upper part and the lower part are electrically connected, so that the whole is formed into a thin plate-like coil shape. This thin film coil and this ferromagnetic magnetoresistive element are placed at a distance such that the magnetic field generated by this thin film coil causes a resistance value of the ferromagnetic magnetoresistive element to change by a predetermined value or more due to the relative distance between the thin film coil and this ferromagnetic magnetoresistive element. need to be placed.

この薄膜コイルが発生する磁界をJ:り有効利用するに
は、この強磁性磁気抵抗素子がこのコイルの中心部に位
置するように配設されることが望ましい。又は、この薄
膜コイルの中心軸と、この強磁性磁気抵抗素子が矩形、
棒状の場合はその素子の長手方向とが平行になるように
相対的に位置決めして配設するのが望ましい。
In order to make effective use of the magnetic field generated by this thin film coil, it is desirable that this ferromagnetic magnetoresistive element be located at the center of this coil. Or, if the central axis of this thin film coil and this ferromagnetic magnetoresistive element are rectangular,
In the case of a rod-shaped element, it is preferable that the element be relatively positioned so that the longitudinal direction of the element is parallel to the element.

接続端子はこの薄膜コイル、この強磁性磁気抵抗素子の
それぞれに電気的に接続される端子である。この接続端
子は、前述した薄膜コイルの形成峙に形成される事が望
ましい。薄s−1イルに接続された端子には、この薄膜
コイルに通電覆る電圧が印加され、この強磁t4磁気抵
抗素子の端子からは外部磁界に対応した、例えば電圧信
号が取り出される。
The connection terminals are terminals that are electrically connected to each of the thin film coil and the ferromagnetic magnetoresistive element. It is desirable that this connection terminal be formed opposite to the formation of the thin film coil described above. A voltage that energizes the thin film coil is applied to the terminal connected to the thin S-1 coil, and a voltage signal, for example, corresponding to the external magnetic field is extracted from the terminal of the ferromagnetic T4 magnetoresistive element.

[作用] 絶縁基板は、強磁性磁気抵抗素子と、薄膜コイルと、接
続端子とを保持する。そして、この絶縁基板は検出Jべ
き磁場内に配設される。薄膜コイルに接続された端子に
電流が通電されると、この薄膜コイルの周囲には、この
電流に応じた磁場ができる。従って、このvAsにより
この強磁性磁気抵抗素子はその軸方向(長手方向)にバ
イアス磁界がかけられた事になる。そのため、この強磁
性磁気抵抗素子に接続された端子より取り出される信号
は、検出すべき磁場の磁界強度によらず、磁界と一義的
に対応する信号が取り出すことができる。又、この磁界
強度が零の近傍においても、このバイアス磁界が印加さ
れているために、バルクハウンゼン・ジャンプのような
現象も起らない。
[Function] The insulating substrate holds the ferromagnetic magnetoresistive element, the thin film coil, and the connection terminal. This insulating substrate is placed within the magnetic field to be detected. When a current is applied to a terminal connected to a thin film coil, a magnetic field corresponding to the current is generated around the thin film coil. Therefore, this vAs causes a bias magnetic field to be applied to this ferromagnetic magnetoresistive element in its axial direction (longitudinal direction). Therefore, the signal taken out from the terminal connected to this ferromagnetic magnetoresistive element can be taken out as a signal that uniquely corresponds to the magnetic field, regardless of the magnetic field strength of the magnetic field to be detected. Further, even when the magnetic field strength is near zero, a phenomenon such as Barkhausen jump does not occur because this bias magnetic field is applied.

[実施例] =  6 − 以下、本発明の強磁性磁気抵抗装置を具体的な実施例に
基づいて詳しく説明する。第1図は同実施例の強磁性磁
気抵抗装置の構造をd1明づる平面図、第2図は第1図
に於G′Jる強1tit’l磁気抵抗素子の中心軸を含
む而で切断した時の断面図である。
[Example] = 6 - Hereinafter, the ferromagnetic magnetoresistive device of the present invention will be described in detail based on specific examples. Fig. 1 is a plan view showing the structure of the ferromagnetic magnetoresistive device of the same embodiment, and Fig. 2 is a cutaway view including the central axis of the magnetoresistive element G'J in Fig. 1. FIG.

強磁性磁気抵抗装置は、絶縁基板10と、強磁性磁気抵
抗素子20(以下磁気抵抗素子20と略す)と、薄膜」
イル30と、接続端子41.43.45で構成される。
The ferromagnetic magnetoresistive device includes an insulating substrate 10, a ferromagnetic magnetoresistive element 20 (hereinafter abbreviated as magnetoresistive element 20), and a thin film.
30 and connection terminals 41, 43, and 45.

以下、この磁気抵抗索子20、簿膜コイル30が形成さ
れる過稈を詳細に説明する。
Hereinafter, the overculm in which the magnetoresistive rope 20 and the membrane coil 30 are formed will be explained in detail.

まず、絶縁基板10上の−1−面の第1図の破線で示す
右上りの互いに一定間隔を隔てて平行した多数の斜方状
の下部導体31を形成し、続いてこれら下部導体31を
絶縁膜33で覆うように形成する。そして、この絶縁膜
33の一■二にNi−Co合金強磁性体を用いた磁気抵
抗素子20を形成する。
First, a large number of diagonal lower conductors 31 are formed parallel to each other at regular intervals on the upper right side of the -1-plane of the insulating substrate 10 as indicated by the broken line in FIG. 1, and then these lower conductors 31 are It is formed so as to be covered with an insulating film 33. Then, a magnetoresistive element 20 using a Ni--Co alloy ferromagnetic material is formed on one and two parts of this insulating film 33.

更に、この磁気抵抗素子20を絶縁膜35で覆うように
形成する。この後、これら下部導体31の各両端部およ
びこの磁気抵抗素子20の両端部を被覆している絶縁膜
33.35の部分をエツチングしてそれらの部分の絶縁
膜を除去する。次に、絶縁膜が除去されて表出した下部
導体31の端部とイれとMり合一う下部導体31の反対
側の端部をそれぞれ結ぶJ:うににして、絶縁膜35の
上面に、豆いに一定間隔をへだてて平行し、第1図上実
線の右下り斜方状の上部導体39を形成4る。これによ
り、多数の■部導体31と多数の上部導体39が互いに
それら両端で結線された薄膜状コイル30が形成される
。なお、L部導体39の形成と同時に端子41.43.
45を形成する。 このように構成された強磁性磁気抵
抗装置は、接続端子41.43に印加された電圧により
薄膜コイル30が通電される事により磁気抵抗素子2o
は、その長手方向に磁界が印加される。そして、検出す
べき磁界がその方向、大きさが変化した時の様子は、接
続端子43.45に現れる電圧信号をグラフ化すると第
3図の曲線50のような特性図として示される。なお、
第3図は機軸に検出すべき磁界の強さを示し、縦軸に磁
気抵抗素子20の両−8一 端に発生する電圧を示す。
Furthermore, this magnetoresistive element 20 is formed so as to be covered with an insulating film 35. Thereafter, the portions of the insulating films 33 and 35 covering both ends of the lower conductor 31 and both ends of the magnetoresistive element 20 are etched to remove those portions of the insulating film. Next, connect the end of the lower conductor 31 exposed by removing the insulating film with the opposite end of the lower conductor 31 that meets the upper surface of the insulating film 35. Then, an upper conductor 39 is formed parallel to the base at a constant interval and has a diagonal shape downward to the right as shown by the solid line in FIG. As a result, a thin film coil 30 is formed in which a large number of square conductors 31 and a large number of upper conductors 39 are connected to each other at both ends thereof. Note that at the same time as forming the L portion conductor 39, the terminals 41, 43.
Form 45. In the ferromagnetic magnetoresistive device configured in this way, the thin film coil 30 is energized by the voltage applied to the connection terminals 41 and 43, so that the magnetoresistive element 2o
A magnetic field is applied in its longitudinal direction. When the direction and magnitude of the magnetic field to be detected changes, the voltage signals appearing at the connection terminals 43 and 45 are graphed as a characteristic diagram such as a curve 50 in FIG. 3. In addition,
In FIG. 3, the axis shows the strength of the magnetic field to be detected, and the vertical axis shows the voltage generated at both ends of the magnetoresistive element 20.

本実施例によれば、磁気抵抗素子2oが薄膜コイル30
の内部に位置し、磁気抵抗素子20の長手方向と薄膜コ
イル30で得られる磁力線の方向が正確に平行している
ため、前述した第5図に示したような、ヒステリシスや
バルクハウゼン・ジャンプが解消されている。従って、
従来の装置にように磁石を正確に位置決めして貼りっ【
ノる必要がない。このため、生産性の高い、つまり小型
で安価な強磁性磁気抵抗装置が実現できる。
According to this embodiment, the magnetoresistive element 2o is the thin film coil 30.
Since the longitudinal direction of the magnetoresistive element 20 and the direction of the magnetic field lines obtained by the thin film coil 30 are precisely parallel, hysteresis and Barkhausen jump as shown in FIG. It has been resolved. Therefore,
The magnets can be accurately positioned and pasted like in conventional devices.
There's no need to cry. Therefore, it is possible to realize a highly productive ferromagnetic magnetoresistive device that is small and inexpensive.

なお、第4図の特性図で示すように、磁気抵抗素子20
に印加される磁界の短手方向の成分が所定の値以上太き
(なると、第3図で示される特性曲線50が検出すべき
磁界が零に対して、この短手方向の成分、方向に応じて
移動する。この第4図の特性図の場合は、特性曲線51
は特性面Ii!50に対して移動幅D51だけ右方向に
移動している。
In addition, as shown in the characteristic diagram of FIG. 4, the magnetoresistive element 20
If the component in the transverse direction of the magnetic field applied to is thicker than a predetermined value (if the characteristic curve 50 shown in FIG. 3 is In the case of the characteristic diagram in FIG. 4, the characteristic curve 51
is the characteristic surface Ii! 50, it has moved to the right by a movement width D51.

[発明の効果] 本発明によれば、強磁性磁気抵抗装置を、絶縁−9一 基板と、強磁性磁気抵抗素子と、薄膜コイルと、接続端
子とで構成したこと(・、この強磁性磁気抵抗素子の両
端には、検出すべり礒工界と一義的に対応した信シ)が
得られる。従って、従来の装置のように、この強11竹
磁気抵抗素子の近傍に永久磁石をその方向に考慮して貼
りつける必要がないため、生産性が向上し、目つ検出精
度のよい強磁性磁気抵抗装置が実現できる。
[Effects of the Invention] According to the present invention, a ferromagnetic magnetoresistive device is composed of an insulating substrate, a ferromagnetic magnetoresistive element, a thin film coil, and a connecting terminal. At both ends of the resistive element, a signal that corresponds uniquely to the detection slip resistance is obtained. Therefore, unlike conventional devices, there is no need to stick a permanent magnet in the vicinity of the ferromagnetic magnetoresistive element in consideration of its direction, which improves productivity and improves the accuracy of ferromagnetic detection. A resistance device can be realized.

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

第1図は本発明の具体的な実施例に係る強磁性磁気抵抗
装置の構造を示す平面図、第2図は同第1図における磁
気抵抗素子の中心軸を含む面で切断した時の断面図であ
る。 第3図、第4図は同実施例装置により得られた検出すべ
き磁界と磁気抵抗素子の両端に現われる信号の関係を示
ず特性図であり、この内、第4図は磁気抵抗素子の短手
方向に印加される磁界が所定の値より大きくなった時の
同特性図である。第5図は従来技術を説明するために用
いた検出すべき磁界と、磁気抵抗素子の両端に現われる
信号の関係を示す特性図である。 10・・・絶縁基板  20・・・強磁性磁気抵抗素子
30・・・薄膜コイル 41.43.45・・・接続端子 特許出願人   日本電装株式会社 代理人    弁理士 大川 宏 同     弁理士 丸山明夫 第1図 第2図 第3迎 ΔP タト 音5 gl X 第5図 クト蔀it
FIG. 1 is a plan view showing the structure of a ferromagnetic magnetoresistive device according to a specific embodiment of the present invention, and FIG. 2 is a cross section taken along a plane including the central axis of the magnetoresistive element in FIG. 1. It is a diagram. Figures 3 and 4 are characteristic diagrams that do not show the relationship between the magnetic field to be detected obtained by the same embodiment device and the signals appearing at both ends of the magnetoresistive element. FIG. 6 is the same characteristic diagram when the magnetic field applied in the lateral direction becomes larger than a predetermined value. FIG. 5 is a characteristic diagram showing the relationship between the magnetic field to be detected and the signals appearing at both ends of a magnetoresistive element, which was used to explain the prior art. 10...Insulating substrate 20...Ferromagnetic magnetoresistive element 30...Thin film coil 41.43.45...Connection terminal Patent applicant Nippondenso Co., Ltd. Agent Patent attorney Hirotoshi Okawa Patent attorney Akio Maruyama No. Figure 1 Figure 2 Figure 3 ΔP Tato Sound 5 gl X Figure 5 Kuto It

Claims (2)

【特許請求の範囲】[Claims] (1)絶縁基板と、 前記絶縁基板上に設けられ周囲の磁界強度に応じて電気
抵抗が変化する強磁性磁気抵抗素子と、前記絶縁基板上
の前記強磁性磁気抵抗素子の近傍に薄膜のコイル状で形
成され、通電電流に応じた強度の磁界を発生する薄膜コ
イルと、  前記強磁性磁気抵抗素子、前記薄膜コイルのそれぞれ
に設けられる接続端子と、 から構成される事を特徴とする強磁性磁気抵抗装置。
(1) An insulating substrate, a ferromagnetic magnetoresistive element provided on the insulating substrate and whose electrical resistance changes depending on the strength of a surrounding magnetic field, and a thin film coil disposed near the ferromagnetic magnetoresistive element on the insulating substrate. A ferromagnetic device comprising: a thin film coil formed in a shape and generating a magnetic field with a strength according to the applied current; and a connection terminal provided on each of the ferromagnetic magnetoresistive element and the thin film coil. Magnetoresistive device.
(2)強磁性磁気抵抗素子は薄膜コイルの中心部に位置
する特許請求の範囲第1項記載の強磁性磁気抵抗装置。
(2) The ferromagnetic magnetoresistive device according to claim 1, wherein the ferromagnetic magnetoresistive element is located at the center of the thin film coil.
JP60177880A 1985-08-13 1985-08-13 Ferromagnetic reluctance apparatus Pending JPS6237980A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60177880A JPS6237980A (en) 1985-08-13 1985-08-13 Ferromagnetic reluctance apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60177880A JPS6237980A (en) 1985-08-13 1985-08-13 Ferromagnetic reluctance apparatus

Publications (1)

Publication Number Publication Date
JPS6237980A true JPS6237980A (en) 1987-02-18

Family

ID=16038669

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60177880A Pending JPS6237980A (en) 1985-08-13 1985-08-13 Ferromagnetic reluctance apparatus

Country Status (1)

Country Link
JP (1) JPS6237980A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2017216722A (en) * 2017-07-24 2017-12-07 Tdk株式会社 Rectifier and transceiver
JP2018098799A (en) * 2017-12-25 2018-06-21 Tdk株式会社 Rectifier and transceiver

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5748284A (en) * 1980-08-15 1982-03-19 Rohm Co Ltd Signal transmitting element

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5748284A (en) * 1980-08-15 1982-03-19 Rohm Co Ltd Signal transmitting element

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2017216722A (en) * 2017-07-24 2017-12-07 Tdk株式会社 Rectifier and transceiver
JP2018098799A (en) * 2017-12-25 2018-06-21 Tdk株式会社 Rectifier and transceiver

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