JPS6240786A - Magnetic coupling isolator using magnetic reluctance element - Google Patents

Magnetic coupling isolator using magnetic reluctance element

Info

Publication number
JPS6240786A
JPS6240786A JP60180414A JP18041485A JPS6240786A JP S6240786 A JPS6240786 A JP S6240786A JP 60180414 A JP60180414 A JP 60180414A JP 18041485 A JP18041485 A JP 18041485A JP S6240786 A JPS6240786 A JP S6240786A
Authority
JP
Japan
Prior art keywords
pattern
magnetic
conductor pattern
magnetoresistive element
coupling isolator
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
JP60180414A
Other languages
Japanese (ja)
Inventor
Yoshio Sato
良夫 佐藤
Akira Hirano
明 平野
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fujitsu Ltd
Original Assignee
Fujitsu Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP60180414A priority Critical patent/JPS6240786A/en
Publication of JPS6240786A publication Critical patent/JPS6240786A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To manufacture an magnetic coupling isolator small in size and low in production cost, and to improve its high frequency characteristics, by composing it of an input conductor pattern and an output magnetic reluctance element. CONSTITUTION:An input conductor pattern 1 using a thin film conductor, and an output magnetic reluctance element 3 formed through an insulating film 2 on the pattern 1 are provided. A magnetic field change in response to the variation in the input current of the pattern 1 is detected by the element 3, and its signal is output as a voltage change. Thus, the function as a magnetic coupling isolator can be performed.

Description

【発明の詳細な説明】 〔概 要〕 磁気抵抗素子を用いた磁気結合アイソレーターであって
、導電パターンによる磁界を磁気抵抗素子で検出する方
式により、入力と出力を電気的に絶縁し、その間の信号
伝達を高速に行なうことができ、且つ素子の固体素子化
を可能とする。
[Detailed Description of the Invention] [Summary] A magnetic coupling isolator using a magnetoresistive element, which electrically isolates input and output by using a method in which the magnetic field generated by a conductive pattern is detected by the magnetoresistive element, and Signal transmission can be performed at high speed, and the device can be made into a solid-state device.

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

本発明は磁気抵抗素子を用いた磁気結合アイソレーター
に関するものである。
The present invention relates to a magnetically coupled isolator using a magnetoresistive element.

〔従来の技術〕[Conventional technology]

アイソレーターを形成するには、何らかの方法で電気的
に絶縁した状態で信号を伝達しなければならない。従来
はその信号伝達に磁界あるいは光を用いていた。
To form an isolator, signals must be transmitted while being electrically isolated in some way. Conventionally, magnetic fields or light have been used for signal transmission.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

磁界を利用したものはトランス結合型アイソレーターで
比較的小型のものが実用化されているが、大きさがやや
大きいことと、同波数特性に限界(〜30KHz)があ
った。また光を利用するものはホトカブラ型アイソレー
ターで小型かつ高速(〜MHz)のものが実用化されて
いるが価格がやや高いという欠点があった。
Relatively small transformer-coupled isolators that utilize magnetic fields have been put into practical use, but they are somewhat large and have a limited wavenumber characteristic (~30 KHz). In addition, photocoupler type isolators that use light are small and have a high speed (up to MHz) that have been put into practical use, but they have the drawback of being rather expensive.

本発明はこのような点に鑑みて創作されたもので、導電
パターンと磁気抵抗素子を用い、周波数特性が良く、且
つ安価で小型に製造できるアイソレーターを提供するこ
とを目的としている。
The present invention was created in view of these points, and an object of the present invention is to provide an isolator that uses a conductive pattern and a magnetoresistive element, has good frequency characteristics, and can be manufactured inexpensively and compactly.

C問題点を解決するための手段〕 このため本発明においては、薄膜導体を用いた入力用導
体パターン1と、BbF!+体パターン1上に絶縁膜2
を介して設けられた出力用磁気抵抗素子3とより成るこ
とを特徴としている。
Means for Solving Problem C] Therefore, in the present invention, the input conductor pattern 1 using a thin film conductor and the BbF! Insulating film 2 on + body pattern 1
It is characterized in that it consists of an output magnetoresistive element 3 provided via an output magnetoresistive element 3.

〔作 用〕[For production]

導体パターン1の入力電流の変化に応じた磁界変化を磁
気抵抗素子3にて検知し、その信号を電圧変化として出
力することにより磁気結合アイソレーターとしての機能
を果すことが可能となる。
By detecting changes in the magnetic field in accordance with changes in the input current of the conductor pattern 1 with the magnetoresistive element 3 and outputting the signal as a voltage change, it is possible to function as a magnetic coupling isolator.

〔実施例〕〔Example〕

第1図は本発明の実施例を示す図であり、aはは平面図
、bはa図のb−b’−b#線における断面図である。
FIG. 1 is a diagram showing an embodiment of the present invention, in which a is a plan view and b is a cross-sectional view taken along line bb'-b# of diagram a.

本実施例は第1図a、bに示すように、導体で形成され
た導体パターン1と、該導体パターンと絶縁層2を介し
た磁気抵抗素子3 (2点鎖線で囲った部分)とが基板
4の上に設けられている。そして基板4にはガラス又は
Si等が用いられ、導体パターンにはAu等の金属が、
絶縁層2にはSiO□の絶縁破壊電圧の高いものが用い
られる。
In this embodiment, as shown in FIGS. 1a and 1b, a conductor pattern 1 made of a conductor and a magnetoresistive element 3 (the part surrounded by the two-dot chain line) are connected to the conductor pattern with an insulating layer 2 interposed therebetween. It is provided on the substrate 4. The substrate 4 is made of glass or Si, and the conductor pattern is made of metal such as Au.
The insulating layer 2 is made of SiO□, which has a high dielectric breakdown voltage.

また磁気抵抗素子3にはバーバーポール型が用いられて
いる。このバーバーポール型磁気抵抗素子3は厚さ50
0〜1000人、幅訳8μmのパーマロイ等の軟磁性薄
膜を用いたつづら折り状パターンの1対5,6が左右対
称に形成され、その各一方の端部はそれぞれスルーホー
ル7.8を通して引出し用導体パターン9.10に接続
され、他方の各端部はスルーホール11を通して同一の
引出し用薄体パターン12に接続され、さらにつづら折
り状パターン5.6の上には第2図に示すようにパター
ン5には斜め45″、パターン6には斜め135 ’で
幅2.8 p m、ギ+−/プ2.11Imのピンチで
導体パターン13が形成されている。
Further, the magnetoresistive element 3 is of a barber pole type. This barber pole type magnetoresistive element 3 has a thickness of 50 mm.
0 to 1000 people, 1 pair 5 and 6 of a zigzag pattern using a soft magnetic thin film such as permalloy with a width of 8 μm are formed symmetrically, and one end of each is used for drawing out through a through hole 7.8. The conductor pattern 9.10 is connected to the conductor pattern 9.10, and each other end thereof is connected to the same drawer thin pattern 12 through the through hole 11, and on the meander-like pattern 5.6 there is a pattern as shown in FIG. The conductor pattern 13 is formed with a diagonal of 45'' on pattern 5 and a width of 2.8 pm with a width of 2.8 pm and a width of 2.11 Im on pattern 6.

このように構成された本実施例は、第3図の回路図に示
すようにつづら折り状パターン5及び6を可変抵抗14
を介し直流電圧分が等しくv。となるように並列に直流
電源■。、に接続し、導体パターン9.10を差動増幅
器15に接続しておき、第1図の導体パターンlに入力
電流lを流せばその変化により磁界が変化し、つづら折
り状パターン5,6には第4図の如く位相が180°異
なる出力電圧VL、V、が生ずる。つづら折り状パター
ン5,6の寸法を同一に作成しておけば出力電圧■、と
■6は等しくなり、これらを差動増幅器15で増幅すれ
ば■。は相殺され、変化分ΔVL、ΔvRのみ強調し合
い約2×ΔvLが得られる。
In this embodiment configured in this way, the zigzag patterns 5 and 6 are connected to the variable resistor 14 as shown in the circuit diagram of FIG.
The DC voltage component is equal across v. ■ DC power supply in parallel so that. , and the conductor patterns 9 and 10 are connected to the differential amplifier 15. If an input current l is applied to the conductor pattern l shown in FIG. As shown in FIG. 4, output voltages VL and V whose phases are different by 180° are generated. If the dimensions of the zigzag patterns 5 and 6 are made the same, the output voltages ■ and ■6 will be equal, and if they are amplified by the differential amplifier 15, the output voltages ■ and ■6 will be equal. are canceled out, and only the changes ΔVL and ΔvR are emphasized to obtain approximately 2×ΔvL.

ここで第1図の如く導体パターン1を流れる電流■の方
向と磁気抵抗素子3のつづら折り状パターン5.6の長
手方向(形状による磁化容易方間)Mとが平行となるよ
うに配置すると、出力ΔV1、Δ■えは最大となる。な
お導体パターン1の幅は素子全体の領域S(第1図に示
す)よりも120%以上にとることが均一な磁界を得る
点で望ましい。
If the direction of the current (2) flowing through the conductor pattern 1 and the longitudinal direction (direction of easy magnetization depending on the shape) of the zigzag pattern 5.6 of the magnetoresistive element 3 are arranged so as to be parallel to each other as shown in FIG. The outputs ΔV1 and Δ■ are maximum. Note that it is desirable that the width of the conductive pattern 1 be 120% or more of the area S of the entire element (shown in FIG. 1) in order to obtain a uniform magnetic field.

また本実施の大きさは5008mX500μm程度の大
きさであり、これをデバイスとして作製する場合には入
力電流生成用のトランジスタ及び出力を差動で増幅する
トランジスタ等を同一チップに形成すると更に小型化す
ることができる。また特性としては、入力電流±20m
Aの時、出力約士10mVが得られ、限界周波数は約1
0MH2まで可能である。
In addition, the size of this implementation is approximately 5008 m x 500 μm, and when fabricating this as a device, it can be further miniaturized by forming a transistor for input current generation, a transistor for differentially amplifying the output, etc. on the same chip. be able to. In addition, the characteristics are input current ±20m
When A, an output of approximately 10 mV is obtained, and the limit frequency is approximately 1
Possible up to 0MH2.

〔発明の効果〕〔Effect of the invention〕

以上述べてきたように、本発明によれば、入力用導体パ
ターンと出力用磁気抵抗素子とよりなる構成で、小型、
安価に製造でき、且つ高周波数特性が良好であり、実用
的には極めて有用である。
As described above, according to the present invention, the configuration consisting of the input conductor pattern and the output magnetoresistive element is small,
It can be manufactured at low cost and has good high frequency characteristics, making it extremely useful in practice.

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

第1図は本発明の実施例を示す図、 第2図はその磁気抵抗素子の一部を示す拡大図、第3図
は本発明の実施例を用いる回路図、第4図は本発明の実
施例の入力及び出力波形を示す図である。 第1図、第2図、第3図において、 1は入力用導体パターン、 2は絶縁層、 3は磁気抵抗素子、 4は基板、 5.6はつづら折り状パターン、 7.8.11はスルーホール、 9.10.12は引出し用導体パターン、13はつづら
折り状パターンの上の導体パターン、14は可変抵抗、 15は差動増幅器である。 本発明の実施例を示す図 第1図 3・・・磁気抵抗センサ 4・・・基板 9、IO,+2−’−引出し用導体 を示す拡大図 第2図 13・・・ 導体パターン 本発明の実施例を用いる回路を示す図 第3図 5.6・・・つづら折り状ノeターン 14・・・可変抵抗 15・・・差動増幅器 本発明の実施例の入力及び出力波形 を示す図 第4図
FIG. 1 is a diagram showing an embodiment of the present invention, FIG. 2 is an enlarged view showing a part of the magnetoresistive element, FIG. 3 is a circuit diagram using the embodiment of the present invention, and FIG. 4 is a diagram showing an embodiment of the present invention. It is a figure which shows the input and output waveform of an Example. 1, 2, and 3, 1 is an input conductor pattern, 2 is an insulating layer, 3 is a magnetoresistive element, 4 is a substrate, 5.6 is a meandering pattern, and 7.8.11 is a through hole. 9.10.12 is a lead-out conductor pattern; 13 is a conductor pattern on the serpentine pattern; 14 is a variable resistor; and 15 is a differential amplifier. Figures showing embodiments of the present invention Figure 1 Figure 3 Magnetoresistive sensor 4 Enlarged diagram showing substrate 9, IO, +2-'-drawing conductor Figure 2 13 Conductor pattern of the present invention Figure 3 showing the circuit using the embodiment 5.6...Meander-shaped E-turn 14...Variable resistor 15...Differential amplifier Figure 4 showing the input and output waveforms of the embodiment of the present invention figure

Claims (2)

【特許請求の範囲】[Claims] 1.薄膜導体を用いた入力用導体パターン(1)と、該
導体パターン(1)上に絶縁膜(2)を介して設けられ
た出力用磁気抵抗素子(3)とよりなることを特徴とす
る磁気抵抗素子を用いた磁気結合アイソレーター。
1. A magnetic device characterized by comprising an input conductor pattern (1) using a thin film conductor, and an output magnetoresistive element (3) provided on the conductor pattern (1) via an insulating film (2). Magnetic coupling isolator using resistive elements.
2.上記磁気抵抗素子(3)としてバーバーポール型磁
気抵抗素子を用い、該素子を、その磁化容易方向が導体
パターン(1)中の電流の流れる方向と平行となる様に
配置したことを特徴とする特許請求の範囲第1項記載の
磁気抵抗素子を用いた磁気結合アイソレーター。
2. A barber pole type magnetoresistive element is used as the magnetoresistive element (3), and the element is arranged so that its direction of easy magnetization is parallel to the direction of current flow in the conductor pattern (1). A magnetic coupling isolator using the magnetoresistive element according to claim 1.
JP60180414A 1985-08-19 1985-08-19 Magnetic coupling isolator using magnetic reluctance element Pending JPS6240786A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60180414A JPS6240786A (en) 1985-08-19 1985-08-19 Magnetic coupling isolator using magnetic reluctance element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60180414A JPS6240786A (en) 1985-08-19 1985-08-19 Magnetic coupling isolator using magnetic reluctance element

Publications (1)

Publication Number Publication Date
JPS6240786A true JPS6240786A (en) 1987-02-21

Family

ID=16082838

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60180414A Pending JPS6240786A (en) 1985-08-19 1985-08-19 Magnetic coupling isolator using magnetic reluctance element

Country Status (1)

Country Link
JP (1) JPS6240786A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008227081A (en) * 2007-03-12 2008-09-25 Omron Corp Magnetic coupler element and magnetic coupling type isolator
JP2009246191A (en) * 2008-03-31 2009-10-22 Tdk Corp Magnetic coupler
US7948349B2 (en) 2007-10-31 2011-05-24 Tdk Corporation Magnetic coupler

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008227081A (en) * 2007-03-12 2008-09-25 Omron Corp Magnetic coupler element and magnetic coupling type isolator
US7948349B2 (en) 2007-10-31 2011-05-24 Tdk Corporation Magnetic coupler
JP2009246191A (en) * 2008-03-31 2009-10-22 Tdk Corp Magnetic coupler

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