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JPH04236382A - Integrated magnetoresistance effect element circuit - Google Patents

Integrated magnetoresistance effect element circuit

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Publication number
JPH04236382A
JPH04236382A JP3004188A JP418891A JPH04236382A JP H04236382 A JPH04236382 A JP H04236382A JP 3004188 A JP3004188 A JP 3004188A JP 418891 A JP418891 A JP 418891A JP H04236382 A JPH04236382 A JP H04236382A
Authority
JP
Japan
Prior art keywords
transistor
collector
magnetoresistive element
base
magnetoresistance effect
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
JP3004188A
Other languages
Japanese (ja)
Inventor
Masami Muranaka
村中 雅美
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Original Assignee
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP3004188A priority Critical patent/JPH04236382A/en
Publication of JPH04236382A publication Critical patent/JPH04236382A/en
Pending legal-status Critical Current

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  • Networks Using Active Elements (AREA)
  • Measuring Magnetic Variables (AREA)

Abstract

PURPOSE:To decrease the number of magnetoresistance effect elements to a half and miniaturize a chip or reduce power current in an integration magnetoresistance effect element. CONSTITUTION:An integration magnetoresistance effect circuit consists of magnetoresistance effect elements 2, 3 which detect several different magnetic fields and change those resistance values, a current mirror circuit which is connected with the magnetoresistance effect elements 2, 3 and consists of transistors 4, 5 in order to equalize current to flow through these, and an amplifier circuit 6 which amplifies the potential difference between junctions of magnetoresistance effect elements 2, 3 and transistors 4, 5.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明は、集積化磁気抵抗効果素
子(以下、磁気抵抗効果素子をMR素子と呼ぶ)回路に
関し、特にその回路構成に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an integrated magnetoresistive element (hereinafter referred to as an MR element) circuit, and particularly to its circuit configuration.

【0002】0002

【従来の技術】従来、この種の集積化MR素子回路は、
図7に示すように、同一の磁界を検知する第1及び第4
のMR素子2及び18と、同様に同一の磁界を検知する
第2及び第3のMR素子3及び17とが、ブリッジ接続
され、その中点電位の電位差を増幅器6により増幅して
出力を得る構成となっていた。
[Prior Art] Conventionally, this type of integrated MR element circuit has
As shown in FIG. 7, the first and fourth sensors detect the same magnetic field.
MR elements 2 and 18 and second and third MR elements 3 and 17, which similarly detect the same magnetic field, are bridge-connected, and the potential difference between their midpoint potentials is amplified by an amplifier 6 to obtain an output. It was configured.

【0003】第1〜第4のMR素子2,3,17,18
の初期抵抗値R0 として、磁界を検知したときの各M
R素子の抵抗変動値をΔRとすると、第1と第4のMR
素子2,18が磁界を検知したとき、電位差ΔV1 は
、VCCを直流電圧源の電圧値とした時、 ΔV1 =(−VCC・4R)÷2R0 ……(1)と
なる。同様に第2と第3のMR素子3,17が磁界を検
知すると ΔV2 =(VCC・4R)÷2RO ……(2)とな
り、これらの電位差を入力として増幅器6で増幅し、出
力を得ていた。
[0003] First to fourth MR elements 2, 3, 17, 18
As the initial resistance value R0 of each M when the magnetic field is detected,
If the resistance fluctuation value of the R element is ΔR, the first and fourth MR
When the elements 2 and 18 detect a magnetic field, the potential difference ΔV1 becomes ΔV1 = (-VCC·4R)÷2R0 (1), where VCC is the voltage value of the DC voltage source. Similarly, when the second and third MR elements 3 and 17 detect a magnetic field, ΔV2 = (VCC 4R) ÷ 2RO (2), and these potential differences are used as input and amplified by the amplifier 6 to obtain an output. Ta.

【0004】0004

【発明が解決しようとする課題】この従来の集積化MR
素子回路は、4つのMR素子を用いるため素子チップ面
積が大型化し、またチップ面積に限界がある場合には素
子の抵抗値を大きくすることができず、その結果電源電
流を減少させるこが困難である等の欠点がある。
[Problem to be solved by the invention] This conventional integrated MR
Since the element circuit uses four MR elements, the element chip area becomes large, and if the chip area is limited, the resistance value of the element cannot be increased, and as a result, it is difficult to reduce the power supply current. There are drawbacks such as:

【0005】[0005]

【課題を解決するための手段】本発明の集積化MR素子
回路は、2つのMR素子と、これら2つのMR素子のそ
れぞれが電流入力端子と電流出力端子に接続された電流
ミラー回路と、この電流ミラー回路の電流入力端子と電
流出力端子との電位差を増幅する差動増幅回路とを有し
て構成される。
[Means for Solving the Problems] The integrated MR element circuit of the present invention includes two MR elements, a current mirror circuit in which each of these two MR elements is connected to a current input terminal and a current output terminal, and The current mirror circuit includes a differential amplifier circuit that amplifies the potential difference between the current input terminal and the current output terminal of the current mirror circuit.

【0006】[0006]

【実施例】次に本発明について図面を参照して説明する
DESCRIPTION OF THE PREFERRED EMBODIMENTS Next, the present invention will be explained with reference to the drawings.

【0007】図1は本発明の一実施例である。FIG. 1 shows an embodiment of the present invention.

【0008】第1及び第2のMR素子2,3は、それぞ
れ異った磁界を検知し、抵抗値が変化する。第1のMR
素子2の一端は第1のNPNトランジスタ4のコレクタ
とベースに接続され、第2のMR素子3の一端は第2の
NPNトランジスタ5のコレクタに接続されている。第
1および第2のNPNトランジスタ4,5のベース同士
およびエミッタ同士は共通に接続されて電流ミラー回路
を形成している。第1及び第2のNPNトランジスタ4
,5は同一平面上に作成され、非常に近い特性を持つよ
うになされている。第1および第2のMR素子2,3の
他端と第1及び第2のNPNトランジスタ4,5のエミ
ッタ間に直流電圧源1が接続されている。MR素子2,
3と電流ミラー回路との各接続点はそれらの電位差を増
幅する差動増幅型式の増幅器6に接続されている。 NPNトランジスタ4と5は、電流ミラー回路となって
いるためそこに流れる電流I1 ,I2 はI1 =I
2 ……(3) の関係にある。また、直流電圧源1の電圧値をVCC,
NPNトランジスタ4,5のベース・エミッタ間電圧を
VBE,MR素子2,3の抵抗をR2,R3とするとN
PNトランジスタ4,5のコレクタ電圧V1 ,V2 
はそれぞれ V1 =VCC−I1 R2……(4)V2 =VCC
−I2 R3……(5)I1 =I2 =(VCC−V
BE)÷R2……(6)磁界の変化により、MR素子2
の抵抗値が4R変化するとコレクタ電圧V2とV1 の
電位差ΔVは、MR素子2,3の初期抵抗値をそれぞれ
R0 とすると、ΔV=(VCC−VBE)×(−4R
)÷R0 ……(6)となる。同様にMR素子3が変化
したときはΔV=(VCC−VBE)×(4R)÷R0
 ……(7)となる。
The first and second MR elements 2 and 3 detect different magnetic fields, and their resistance values change. 1st MR
One end of the element 2 is connected to the collector and base of the first NPN transistor 4, and one end of the second MR element 3 is connected to the collector of the second NPN transistor 5. The bases and emitters of the first and second NPN transistors 4 and 5 are commonly connected to form a current mirror circuit. First and second NPN transistors 4
, 5 are created on the same plane and have very similar characteristics. A DC voltage source 1 is connected between the other ends of the first and second MR elements 2 and 3 and the emitters of the first and second NPN transistors 4 and 5. MR element 2,
3 and the current mirror circuit are connected to a differential amplification type amplifier 6 that amplifies the potential difference between them. Since the NPN transistors 4 and 5 form a current mirror circuit, the currents I1 and I2 flowing therein are I1 = I
2 ...(3) There is a relationship. In addition, the voltage value of DC voltage source 1 is VCC,
If the base-emitter voltage of NPN transistors 4 and 5 is VBE, and the resistances of MR elements 2 and 3 are R2 and R3, then N
Collector voltages V1 and V2 of PN transistors 4 and 5
are respectively V1 = VCC - I1 R2... (4) V2 = VCC
-I2 R3... (5) I1 = I2 = (VCC-V
BE)÷R2...(6) Due to changes in the magnetic field, the MR element 2
When the resistance value changes by 4R, the potential difference ΔV between the collector voltages V2 and V1 becomes ΔV=(VCC-VBE)×(-4R
)÷R0...(6). Similarly, when MR element 3 changes, ΔV=(VCC-VBE)×(4R)÷R0
...(7).

【0009】ΔVの電位差を増幅回路6により増幅し、
出力を得ることができる。
[0009] The potential difference of ΔV is amplified by an amplifier circuit 6,
You can get the output.

【0010】図2はNPNトランジスタ4,5のベース
電流の影響を軽減させるためにNPNトランジスタ7の
ベース・エミッタ間をNPNトランジスタ4のコレクタ
・ベース間に付け加えた実施例である。
FIG. 2 shows an embodiment in which an NPN transistor 7 between the base and emitter is added between the collector and base of the NPN transistor 4 in order to reduce the influence of the base currents of the NPN transistors 4 and 5.

【0011】図3は、NPNトランジスタ4,5,7の
代りにPNPトランジスタ8〜10で回路を構成した実
施例である。
FIG. 3 shows an embodiment in which the circuit is constructed with PNP transistors 8 to 10 instead of NPN transistors 4, 5, and 7.

【0012】図4は、NMOSトランジスタ11,12
を使用して回路を構成した実施例である。
FIG. 4 shows NMOS transistors 11 and 12.
This is an example in which a circuit is constructed using the following.

【0013】図5は、NPNトランジスタ13,14を
MR素子とNPNトランジスタ4の間およびMR素子3
とNPNトランジスタ5との間にそれぞれ加えて電流ミ
ラー回路に使用しているトランジスタのベース電流によ
る入出力電流の変動を軽減させた実施例である。
FIG. 5 shows how the NPN transistors 13 and 14 are connected between the MR element and the NPN transistor 4 and between the MR element 3.
This is an embodiment in which fluctuations in input/output current due to base currents of transistors added between the NPN transistor 5 and the NPN transistor 5 and used in the current mirror circuit are reduced.

【0014】また、図6は、増幅器6への入力電圧をレ
ベルシフトするためのダイオード15,16を付加した
実施例である。
FIG. 6 shows an embodiment in which diodes 15 and 16 are added to level shift the input voltage to the amplifier 6.

【0015】[0015]

【発明の効果】以上説明したように、本発明は、それぞ
れ異った磁界を検知するMR素子に電流ミラー回路を付
加し、差動増幅によって差電圧を検出・増幅することに
より、MR素子の数を半分に減少させることができ、そ
の結果チップ面積の減少あるいは、消費電力の低減等の
効果がある。
As explained above, the present invention adds a current mirror circuit to each MR element that detects different magnetic fields, and detects and amplifies the difference voltage by differential amplification. The number can be reduced by half, resulting in reductions in chip area and power consumption.

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

【図1】本発明の第1の実施例を示す回路図である。FIG. 1 is a circuit diagram showing a first embodiment of the present invention.

【図2】本発明の第2の実施例を示す回路図である。FIG. 2 is a circuit diagram showing a second embodiment of the present invention.

【図3】本発明の第3の実施例を示す回路図である。FIG. 3 is a circuit diagram showing a third embodiment of the present invention.

【図4】本発明の第4の実施例を示す回路図である。FIG. 4 is a circuit diagram showing a fourth embodiment of the present invention.

【図5】本発明の第5の実施例を示す回路図である。FIG. 5 is a circuit diagram showing a fifth embodiment of the present invention.

【図6】本発明の第6の実施例を示す回路図である。FIG. 6 is a circuit diagram showing a sixth embodiment of the present invention.

【図7】従来のMR素子回路を示す回路図である。FIG. 7 is a circuit diagram showing a conventional MR element circuit.

【符号の説明】[Explanation of symbols]

1    直流電圧源 2,3,17,18    MR素子 4,5,7,13,14    NPNトランジスタ8
,9,10    PNPトランジスタ11,12  
  MOSトランジスタ6    増幅器 15,16    ダイオード
1 DC voltage source 2, 3, 17, 18 MR element 4, 5, 7, 13, 14 NPN transistor 8
, 9, 10 PNP transistor 11, 12
MOS transistor 6 Amplifier 15, 16 Diode

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】  一端が直流電源の一方の端子にそれぞ
れ接続された第1及び第2の磁気抵抗効果素子と、前記
第1の磁気抵抗効果素子の一端が電源入力端に接続され
、前記第2の磁気抵抗効果素子の一端が電流出力端に接
続され、共通端子が前記直流電源の他方の端子に接続さ
れた電流ミラー回路と、前記第1及び第2の磁気抵抗効
果素子の各前記一端に第1および第2の入力が接続され
てそれらの差電圧を増幅する増幅回路とを有することを
特徴とする集積化磁気抵抗効果素子回路。
1. First and second magnetoresistive elements, one end of which is connected to one terminal of a DC power source, one end of the first magnetoresistive element is connected to a power input terminal, and one end of the first magnetoresistive element is connected to a power input terminal, a current mirror circuit in which one end of the second magnetoresistive element is connected to a current output end and a common terminal is connected to the other terminal of the DC power supply; and one end of each of the first and second magnetoresistive elements. 1. An integrated magnetoresistive element circuit comprising: an amplifier circuit to which first and second inputs are connected and which amplifies a voltage difference therebetween.
【請求項2】  前記電流ミラー回路は前記電流入力端
にコレクタおよびベースが電気的に接続された第1のト
ランジスタと、前記電流出力端にコレクタが電気的に接
続され、前記第1のトランジスタのベースにベースが電
気的に接続され、前記第1のトランジスタのエミッタに
エミッタおよび前記共通端子にエミッタが電気的に接続
された第2のトランジスタとを含んで構成されているこ
とを特徴とする請求項1記載の集積化磁気抵抗効果素子
回路。
2. The current mirror circuit includes a first transistor having a collector and a base electrically connected to the current input terminal, and a collector of the first transistor having a collector electrically connected to the current output terminal. A second transistor whose base is electrically connected to the base, whose emitter is electrically connected to the emitter of the first transistor, and whose emitter is electrically connected to the common terminal. 2. The integrated magnetoresistive element circuit according to item 1.
【請求項3】  前記電流ミラー回路は、前記第1のト
ランジスタのコレクタとベースとの間に、該第1のトラ
ンジスタのコレクタにベースが接続され、該第1のトラ
ンジスタのベースにエミッタが接続された第3のトラン
ジスタを有していることを特徴とする請求項2記載の集
積化磁気抵抗効果素子回路。
3. The current mirror circuit has a base connected to the collector of the first transistor, and an emitter connected to the base of the first transistor, between the collector and the base of the first transistor. 3. The integrated magnetoresistive element circuit according to claim 2, further comprising a third transistor.
【請求項4】  前記電流ミラー回路は前記第1及び第
2のトランジスタがそれぞれ電界効果トランジスタで構
成されていることを特徴とする請求項2記載の集積化磁
気抵抗効果素子回路。
4. The integrated magnetoresistive element circuit according to claim 2, wherein the first and second transistors of the current mirror circuit are each comprised of a field effect transistor.
【請求項5】  前記電流ミラー回路は、コレクタが前
記第1の磁気抵抗効果素子の前記一端に接続され、エミ
ッタが前記第1のトランジスタのコレクタに接続された
第4のトランジスタと、コレクタとベースが前記第2の
磁気抵抗効果素子の前記一端と前記第4のNPNトラン
ジスタのベースに接続され、エミッタが前記第2のトラ
ンジスタのコレクタに接続された第5のNPNトランジ
スタとを備えていることを特徴とする請求項2記載の集
積化磁気抵抗効果素子回路。
5. The current mirror circuit includes a fourth transistor whose collector is connected to the one end of the first magnetoresistive element and whose emitter is connected to the collector of the first transistor, and a collector and a base. is connected to the one end of the second magnetoresistive element and the base of the fourth NPN transistor, and includes a fifth NPN transistor whose emitter is connected to the collector of the second transistor. An integrated magnetoresistive element circuit according to claim 2, characterized in that the integrated magnetoresistive element circuit is characterized in that:
JP3004188A 1991-01-18 1991-01-18 Integrated magnetoresistance effect element circuit Pending JPH04236382A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3004188A JPH04236382A (en) 1991-01-18 1991-01-18 Integrated magnetoresistance effect element circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3004188A JPH04236382A (en) 1991-01-18 1991-01-18 Integrated magnetoresistance effect element circuit

Publications (1)

Publication Number Publication Date
JPH04236382A true JPH04236382A (en) 1992-08-25

Family

ID=11577733

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3004188A Pending JPH04236382A (en) 1991-01-18 1991-01-18 Integrated magnetoresistance effect element circuit

Country Status (1)

Country Link
JP (1) JPH04236382A (en)

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