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JPS5816265B2 - Entoujikukenshiyutsusouchi - Google Patents
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JPS5816265B2 - Entoujikukenshiyutsusouchi - Google Patents

Entoujikukenshiyutsusouchi

Info

Publication number
JPS5816265B2
JPS5816265B2 JP50009070A JP907075A JPS5816265B2 JP S5816265 B2 JPS5816265 B2 JP S5816265B2 JP 50009070 A JP50009070 A JP 50009070A JP 907075 A JP907075 A JP 907075A JP S5816265 B2 JPS5816265 B2 JP S5816265B2
Authority
JP
Japan
Prior art keywords
cylindrical magnetic
magnetic domain
cylindrical
magnetic field
elements
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.)
Expired
Application number
JP50009070A
Other languages
Japanese (ja)
Other versions
JPS5184531A (en
Inventor
高橋一清
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
Nippon Electric 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP50009070A priority Critical patent/JPS5816265B2/en
Publication of JPS5184531A publication Critical patent/JPS5184531A/ja
Publication of JPS5816265B2 publication Critical patent/JPS5816265B2/en
Expired legal-status Critical Current

Links

Description

【発明の詳細な説明】 この発明は円筒磁区拡大素子と、強磁性体の磁気抵抗効
果を利用した磁気抵抗検出素子とを有する円筒磁区検出
装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a cylindrical magnetic domain detection device having a cylindrical domain expansion element and a magnetoresistive detection element that utilizes the magnetoresistive effect of a ferromagnetic material.

従来、磁気抵抗検出素子を用いた微小円筒磁区検出装置
(10ミクロン以下の直径を有する円筒;磁区を対象に
する)では円筒磁区を移動させるための強磁性体片を適
当に配列して円筒磁区を拡大して円筒磁区の検出を行な
っている。
Conventionally, in a micro cylindrical magnetic domain detection device using a magnetoresistive detection element (a cylinder with a diameter of 10 microns or less; the target is a magnetic domain), ferromagnetic pieces for moving the cylindrical magnetic domain are appropriately arranged to detect the cylindrical magnetic domain. The cylindrical magnetic domain is detected by enlarging the image.

また回転磁界と強磁性体片からの磁界によって誘起され
る雑音を消去するためにタミー検出素子およびタミー検
出素子を用いて差動接続をすることによって前記雑音を
消去または軽減させている。
Further, in order to eliminate noise induced by the rotating magnetic field and the magnetic field from the ferromagnetic piece, the noise is eliminated or reduced by differentially connecting a tummy detection element and a tummy detection element.

従来の円筒磁区検出装置の1例としては1971年に刊
行されたエイ・アイ・ビー・コンファレンス・プロシー
ディンゲス(AIP C0NFERRENCE PRO
−CEIIDDINGS)、5巻、235頁に掲載の論
文に記載されている。
An example of a conventional cylindrical magnetic domain detection device is the AIP Conference Proceedings published in 1971.
-CEIIDDINGS), volume 5, page 235.

しかしながら、この種の円筒磁区検出装置では高価な差
動増巾器当りに実効的な磁気抵抗素子が1個しか接続さ
れていないし、回転磁界の1周期内に1ビット信号しか
検出されていないために、高い性能コスト比を得ること
が難;かしかった。
However, in this type of cylindrical magnetic domain detection device, only one effective magnetoresistive element is connected to each expensive differential amplifier, and only one bit signal is detected within one period of the rotating magnetic field. However, it was difficult to obtain a high performance-cost ratio.

特に高速大容量の記憶装置を作るような場合には並列的
に円筒磁区を検出する個所(あるいは磁気抵抗素子)が
多くなり、差動増巾器の個数も多くなるので記憶装置の
性能コスト比が非常に悪くなる。
In particular, when creating a high-speed, large-capacity storage device, the number of places (or magnetoresistive elements) that detect cylindrical magnetic domains in parallel increases, and the number of differential amplifiers also increases, which reduces the performance cost ratio of the storage device. becomes very bad.

したがって、従来の円筒磁区検出装置では高価な差動増
巾器を経済的に有効に活用できない欠陥があった。
Therefore, the conventional cylindrical magnetic domain detection device has a drawback in that the expensive differential amplifier cannot be used economically and effectively.

本発明の第1の目的は上記欠陥を除去する新しい装置構
成を提供することにある。
A first object of the present invention is to provide a new device configuration that eliminates the above-mentioned defects.

本発明の第2の目的は読取り速度の高い円筒磁区検出装
置を提供することに、ある。
A second object of the present invention is to provide a cylindrical magnetic domain detection device with high reading speed.

本発明によれば、回転磁界の1周期内の相異なる時刻に
円筒磁区を拡大する複数個の円筒磁区拡大素子と、前記
円筒磁区拡大素子の各々に接近して配置された少なくと
も1個の磁気抵抗検出素子と、複数個の前記磁気抵抗検
出素子に電流を供給する電流源と、複数個の前記磁気抵
抗検出素子からの信号を前記1周期内で順次に増巾する
差動増巾器とを含む円筒磁区検出装置を提供することが
できる。
According to the present invention, a plurality of cylindrical magnetic domain expanding elements that expand a cylindrical magnetic domain at different times within one cycle of a rotating magnetic field, and at least one magnetic domain expanding element disposed close to each of the cylindrical magnetic domain expanding elements a resistance detection element, a current source that supplies current to the plurality of magnetoresistive detection elements, and a differential amplifier that sequentially amplifies signals from the plurality of magnetoresistive detection elements within the one cycle; A cylindrical magnetic domain detection device including:

第1図は従来の円筒磁区検出装置の概略図を示している
FIG. 1 shows a schematic diagram of a conventional cylindrical magnetic domain detection device.

円筒磁区板中の円筒磁区は回転磁界口に従って、円筒磁
区板に密接して配置された強磁性体薄片(以後Tまたは
Iパターンと言う)10゜11に導かれて移動する。
The cylindrical magnetic domain in the cylindrical magnetic domain plate moves according to the rotating magnetic field opening guided by a ferromagnetic thin piece (hereinafter referred to as T or I pattern) 10° 11 arranged closely to the cylindrical magnetic domain plate.

■パターン98,99゜100まで移動すると円筒磁区
は拡大されて円筒磁区500のようになる。
(2) When the pattern moves to 98, 99° 100, the cylindrical magnetic domain is expanded and becomes a cylindrical magnetic domain 500.

更に回転磁界60が回転すると円筒磁区500は縮小さ
れてもとの太きさにもどり、TIパターン12,13の
上を移産する。
When the rotating magnetic field 60 further rotates, the cylindrical magnetic domain 500 is reduced and returns to its original thickness, and is transferred over the TI patterns 12 and 13.

円筒磁区500の浮遊磁界は磁気抵抗検出素子の感知部
分300の磁化状態を以前の状態から変化させる。
The stray magnetic field of the cylindrical magnetic domain 500 changes the magnetization state of the sensing portion 300 of the magnetoresistive sensing element from its previous state.

このとき、感知部分300の電気抵抗が変化するので電
流源40から導体50を通して電流を供給すると感知部
分300の電気抵抗の変化は電圧変化に変換されて信号
出力を得ることができる。
At this time, since the electrical resistance of the sensing part 300 changes, when a current is supplied from the current source 40 through the conductor 50, the change in the electrical resistance of the sensing part 300 is converted into a voltage change, and a signal output can be obtained.

しかしながら、感知部分300には円筒磁区500の浮
遊磁界と共に回転磁界60および拡大のための■パター
ン9B、99,100からの浮遊磁界も印加され、これ
らによる雑音が信号出力に混入してSN比が悪くなる。
However, in addition to the floating magnetic field of the cylindrical magnetic domain 500, the rotating magnetic field 60 and stray magnetic fields from the patterns 9B, 99, 100 for expansion are also applied to the sensing portion 300, and noise from these is mixed into the signal output and the S/N ratio is reduced. Deteriorate.

そこで、この従来の円筒磁区検出装置ではダミーの感知
部分301を設けて、これにダミー拡大用■パターン2
00,201.202の浮遊磁界と回転磁界60を印加
する。
Therefore, in this conventional cylindrical magnetic domain detection device, a dummy sensing portion 301 is provided, and a dummy enlargement ■ pattern 2 is provided on this.
A floating magnetic field of 00, 201, 202 and a rotating magnetic field 60 are applied.

感知部分301に電流源41から導体50を通して電流
を印加するとそこに雑音電圧が発生する。
When a current is applied to the sensing portion 301 from the current source 41 through the conductor 50, a noise voltage is generated there.

この雑音電圧と前記雑音の混入した信号電圧とを差動増
巾器42に入力すると雑音電圧は差動増巾器42の同相
入力成分になるので消去される。
When this noise voltage and the signal voltage mixed with the noise are input to the differential amplifier 42, the noise voltage becomes an in-phase input component of the differential amplifier 42 and is therefore eliminated.

そして信号電圧のみが出力端子43に現われ、出力信号
電圧は第2図のようになる。
Then, only the signal voltage appears at the output terminal 43, and the output signal voltage becomes as shown in FIG.

第1図のTパターン、20および21は誤って入って来
た円筒磁区がダミー拡大パターンに入ったときにそれを
掃き出すために用いられる。
The T patterns 20 and 21 in FIG. 1 are used to sweep out erroneously incoming cylindrical magnetic domains when they enter the dummy enlarged pattern.

以上が従来の円筒磁区検出装置の概略図を用いた説明で
ある。
The above is an explanation using a schematic diagram of a conventional cylindrical magnetic domain detection device.

以上の説明から理解できるように従来の円筒磁区検出装
置は回転磁界の1周期内に1ビツトを検出するのに感知
素子2個、円筒磁区拡大パターン2組、電流源2イ詠差
動増巾器1個を要し、高価である。
As can be understood from the above explanation, the conventional cylindrical magnetic domain detection device requires two sensing elements, two sets of cylindrical domain expansion patterns, two current sources, and a differential amplification device to detect one bit within one period of a rotating magnetic field. It requires one container and is expensive.

更に第2図から明確なように1周期(T′)に1ビツト
の出力信号(Vs)t、か検出できない。
Furthermore, as is clear from FIG. 2, it is not possible to detect one bit of the output signal (Vs) t in one period (T').

即ち、従来の円筒磁区検出装置では各種素子が有効に使
われていない。
That is, in the conventional cylindrical magnetic domain detection device, various elements are not used effectively.

故に、データ転送速度を1ビツト1周期以上に高めるこ
とができないという欠点がある。
Therefore, there is a drawback that the data transfer rate cannot be increased beyond one bit per period.

第3図は本発明の実施例の概略図を示し、この実施例で
は同−回転磁界内に4種類の円筒磁区移動路1.λ、A
、鼻を有している。
FIG. 3 shows a schematic diagram of an embodiment of the present invention, in which four types of cylindrical domain movement paths 1. λ, A
, has a nose.

第1の移動路1では、円筒磁区30は回転磁界90の回
転に伴ってTIパターンの上を移動し、回転磁界90の
方向がaのときに拡大用パターン7Q、71゜72によ
って拡大される。
In the first movement path 1, the cylindrical magnetic domain 30 moves on the TI pattern with the rotation of the rotating magnetic field 90, and is expanded by the enlargement patterns 7Q, 71°72 when the direction of the rotating magnetic field 90 is a. .

拡大された円筒磁区30の浮遊磁界は磁気抵抗検出素子
の感知部分34によって感知される。
The stray magnetic field of the expanded cylindrical domain 30 is sensed by the sensing portion 34 of the magnetoresistive sensing element.

第2の移動路2ではTIパターン上を移動してきた円筒
磁区31は回転磁界90の方向がbのときに拡大パター
ン73゜74.75によって拡大されて、その浮遊磁界
は磁;気抵抗検出素子の感知部分35によって感知され
る。
In the second movement path 2, the cylindrical magnetic domain 31 that has moved on the TI pattern is expanded by the enlarged pattern 73°74.75 when the direction of the rotating magnetic field 90 is b, and the stray magnetic field is magnetic; is sensed by the sensing portion 35 of.

同様にして、移動路3の円筒磁区、32は回転磁界90
の方向がCのときに拡大パターン76゜77.7Bによ
って拡大されて、その浮遊磁界は感知部分36によって
感知される。
Similarly, the cylindrical magnetic domain 32 of the moving path 3 is a rotating magnetic field 90
When the direction of is C, the stray magnetic field is magnified by the magnifying pattern 76°77.7B and is sensed by the sensing portion 36.

移動路4の円筒9磁区33は回転磁界90の方向がdの
ときに拡大パターン79,80,81によって拡大され
て、その浮遊磁界は感知部分37によって感知される。
The cylindrical magnetic domain 33 of the moving path 4 is expanded by the expansion patterns 79, 80, 81 when the direction of the rotating magnetic field 90 is d, and the stray magnetic field is sensed by the sensing portion 37.

このように移動路1,2,3.4の中を移動している円
筒磁区はそれぞれ回転磁界の異なった位相でi感知され
る。
In this way, the cylindrical magnetic domains moving in the movement paths 1, 2, 3.4 are sensed at different phases of the rotating magnetic field.

回転磁界と拡大用パターンによって感知部分34に生じ
る雑音と感知部分36に生じる雑音は同相であり、また
感知部分35に生じる雑音と感知部分37に生じる雑音
も同相であるので第3図のような結線をすると差動増巾
器54でンは感知部分34,35,36j37から生じ
た雑音が消去される。
Since the noise generated in the sensing portion 34 and the noise generated in the sensing portion 36 due to the rotating magnetic field and the magnifying pattern are in the same phase, and the noise generated in the sensing portion 35 and the noise generated in the sensing portion 37 are also in phase, the noise generated in the sensing portion 35 and the sensing portion 37 is also in phase, so that When the wires are connected, the differential amplifier 54 eliminates noise generated from the sensing portions 34, 35, and 36j37.

感知部分34と37には電流源50から、また感知部分
35と36には電流源51から電流が供給される。
Sensing sections 34 and 37 are supplied with current from a current source 50, and sensing sections 35 and 36 are supplied with current from a current source 51.

円筒磁区30,31゜32.33は異なった位相で感知
部分34.35゜・36,37に感知されるので、各々
の感知部分から生じた信号は消去されることなく差動増
巾器54によって増巾される。
Since the cylindrical magnetic domains 30, 31°, 32.33 are sensed by the sensing parts 34, 35°, 36, 37 with different phases, the signals generated from each sensing part are not canceled and are sent to the differential amplifier 54. The width is increased by

差動増巾器54から得られた信号電圧波形の一例を第4
図で示す。
An example of the signal voltage waveform obtained from the differential amplifier 54 is shown in the fourth example.
Illustrated in the diagram.

図中の縦軸は信号電圧Vsである。The vertical axis in the figure is the signal voltage Vs.

この図でPl、P4はそれぞれ感知部分34と感知部分
37による円筒磁区30と円筒磁区33の検出信号であ
り、P2.P3は感知部分35と感知部分3Bによる円
筒磁区31と同筒磁区32の検出信号である。
In this figure, Pl and P4 are detection signals of the cylindrical magnetic domain 30 and the cylindrical magnetic domain 33 by the sensing portion 34 and the sensing portion 37, respectively, and P2. P3 is a detection signal of the cylindrical magnetic domain 31 and the cylindrical magnetic domain 32 by the sensing portion 35 and the sensing portion 3B.

以上の説明から理解できるように、本発明による円筒磁
区検出装置ではダミー検出素子を用いることなく雑音を
消去することができ、ざらに差動増巾器を有効に利用す
ることができる。
As can be understood from the above description, the cylindrical magnetic domain detection device according to the present invention can eliminate noise without using a dummy detection element, and can effectively utilize a differential amplifier.

第3図による本発明の実施例では差動増巾器が1個、電
流源が2個であって従来の装置の数と変らないが、4つ
の独立した情報を検出することができ、しかも4倍の転
送速度を得ることができる。
The embodiment of the present invention shown in FIG. 3 has one differential amplifier and two current sources, which is the same number as the conventional device, but it can detect four independent pieces of information. You can get four times the transfer speed.

各磁気抵抗検出素子もまた有効に使用されている。Magnetoresistive sensing elements are also used effectively.

実施例では回転磁界の4方向における拡大検出について
述べたが、本発明はこれに限定するものでなく任意の異
なる方向における拡大検出をも含むものである。
Although the embodiment describes magnified detection of the rotating magnetic field in four directions, the present invention is not limited to this, but also includes magnified detection in any different directions.

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

第1図は従来の円筒磁区検出装置の概略図であり、第2
図は検出波形であり、第3図は本発明による円筒磁区検
出装置の一実施例を示す概略図であり、第4図はその検
出波形である。 第3図において、L2,3,4は移動路、30,31.
32゜33は円筒磁区、34,35,36,37は磁気
抵抗検出素子の感知部分、50.51は電流源、54G
−1差動増巾器、70〜81は拡大用パターンである。
Figure 1 is a schematic diagram of a conventional cylindrical magnetic domain detection device;
The figure shows the detected waveform, FIG. 3 is a schematic diagram showing an embodiment of the cylindrical magnetic domain detecting device according to the present invention, and FIG. 4 shows the detected waveform. In FIG. 3, L2, 3, 4 are travel paths, 30, 31 .
32゜33 is a cylindrical magnetic domain, 34, 35, 36, 37 are sensing parts of magnetoresistive sensing elements, 50.51 is a current source, 54G
-1 differential amplifier, 70 to 81 are expansion patterns.

Claims (1)

【特許請求の範囲】 1 回転磁界の1周期内の相異なる時刻に円筒磁区を拡
大する複数個の円筒磁区拡大素子と、前記円筒磁区拡大
素子の各々に接近して配置された少なくとも1個の磁気
抵抗検出素子と、複数個の前。 記磁気抵抗検出素子の各々に電流を供給する電流源と、
複数個の前記磁気抵抗検出素子からの信号を前記1周期
内で順次に増巾する差動増巾器とを含む円筒磁区検出装
置。 ・
[Scope of Claims] 1. A plurality of cylindrical magnetic domain expanding elements that expand cylindrical magnetic domains at different times within one cycle of a rotating magnetic field, and at least one cylindrical magnetic domain expanding element disposed close to each of the cylindrical magnetic domain expanding elements. Magnetoresistive sensing element and multiple pieces in front. a current source that supplies current to each of the magnetoresistive sensing elements;
A cylindrical magnetic domain detection device including a differential amplifier that sequentially amplifies signals from a plurality of the magnetoresistive detection elements within the one cycle.・
JP50009070A 1975-01-21 1975-01-21 Entoujikukenshiyutsusouchi Expired JPS5816265B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP50009070A JPS5816265B2 (en) 1975-01-21 1975-01-21 Entoujikukenshiyutsusouchi

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP50009070A JPS5816265B2 (en) 1975-01-21 1975-01-21 Entoujikukenshiyutsusouchi

Publications (2)

Publication Number Publication Date
JPS5184531A JPS5184531A (en) 1976-07-23
JPS5816265B2 true JPS5816265B2 (en) 1983-03-30

Family

ID=11710338

Family Applications (1)

Application Number Title Priority Date Filing Date
JP50009070A Expired JPS5816265B2 (en) 1975-01-21 1975-01-21 Entoujikukenshiyutsusouchi

Country Status (1)

Country Link
JP (1) JPS5816265B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS545335A (en) * 1977-06-15 1979-01-16 Hitachi Ltd Detection system of magnetic bubble
US8888688B2 (en) 2000-04-03 2014-11-18 Intuitive Surgical Operations, Inc. Connector device for a controllable instrument

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5630634B2 (en) * 1971-12-20 1981-07-16

Also Published As

Publication number Publication date
JPS5184531A (en) 1976-07-23

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