JPS5846765B2 - Jikihed - Google Patents

Jikihed

Info

Publication number
JPS5846765B2
JPS5846765B2 JP49095772A JP9577274A JPS5846765B2 JP S5846765 B2 JPS5846765 B2 JP S5846765B2 JP 49095772 A JP49095772 A JP 49095772A JP 9577274 A JP9577274 A JP 9577274A JP S5846765 B2 JPS5846765 B2 JP S5846765B2
Authority
JP
Japan
Prior art keywords
magnetic
thin plate
ferromagnetic thin
magnetic field
signal
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
JP49095772A
Other languages
Japanese (ja)
Other versions
JPS5123126A (en
Inventor
謙二 金井
深 小林
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP49095772A priority Critical patent/JPS5846765B2/en
Publication of JPS5123126A publication Critical patent/JPS5123126A/en
Publication of JPS5846765B2 publication Critical patent/JPS5846765B2/en
Expired legal-status Critical Current

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  • Magnetic Heads (AREA)

Description

【発明の詳細な説明】 本発明はパーマロイ等の強磁性体に磁界を印加したとき
に電気的抵抗値が変化する、いわゆる磁気抵抗効果を利
用した磁気ヘッドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic head that utilizes the so-called magnetoresistive effect, in which the electrical resistance value changes when a magnetic field is applied to a ferromagnetic material such as permalloy.

この磁気抵抗効果を利用した磁気ヘッドの原理的構成と
しては従来より第1図に示されるような構成のものが考
えられていた。
As a principle structure of a magnetic head that utilizes this magnetoresistive effect, a structure as shown in FIG. 1 has been conventionally considered.

すなわち、第1図イにおいて、記録媒体1である磁気テ
ープと垂直y方向に強磁性薄板よりなる磁気抵抗効果素
子2を当接または近接させ、磁気抵抗効果素子2の長手
方向(Z方向)の両端に電極3,4を配置し、電極3,
4間に定電流jを流し、記録媒体1かものy方向の信号
磁界によりZ方向の抵抗値変化を電極3,4間の電圧変
化より検出する方式である。
That is, in FIG. 1A, the magnetoresistive element 2 made of a ferromagnetic thin plate is brought into contact with or close to the magnetic tape, which is the recording medium 1, in the perpendicular y direction, and the magnetoresistive element 2 is moved in the longitudinal direction (Z direction). Electrodes 3 and 4 are arranged at both ends, and electrodes 3 and 4 are arranged at both ends.
In this method, a constant current j is passed between the electrodes 3 and 4, and a change in resistance value in the Z direction is detected from a change in voltage between the electrodes 3 and 4 using a signal magnetic field in the y direction of the recording medium 1.

この方式では磁気抵抗効果素子2のy方向の記録媒体1
からの距離をWとすると、記録媒体1からの信号磁界の
強さはこの距離Wについて指数函数的に減少し、特に記
録媒体上の記録波長が短い領域では、磁気抵抗効果素子
2の巾方向の信号磁界減衰は非常に大きなものとなる。
In this method, the recording medium 1 in the y direction of the magnetoresistive element 2
If the distance from The signal magnetic field attenuation becomes extremely large.

このような減衰を回避する方法として第1図口に示すよ
うに磁気抵抗効果素子2を記録媒体1と平行に配置する
とy方向の分離損失は殆んどなくなるが、磁気抵抗効果
素子2は一般に薄板であるため記録媒体1との摺動によ
る摩耗が問題となり実用上問題がある。
As a way to avoid such attenuation, if the magnetoresistive element 2 is arranged parallel to the recording medium 1 as shown in the opening of Figure 1, the separation loss in the y direction will almost disappear, but the magnetoresistive element 2 is generally Since it is a thin plate, wear due to sliding with the recording medium 1 becomes a problem, which poses a practical problem.

さらに磁気抵抗効果の抵抗変化△ρは強磁性薄板の磁化
方向と電流方向とのなす角度をθ、aとbを定数とする
と、 という関係式が成立っている。
Further, the resistance change Δρ due to the magnetoresistive effect has the following relational expression, where θ is the angle between the magnetization direction of the ferromagnetic thin plate and the current direction, and a and b are constants.

また、印加磁界Hと抵抗変化率△ρ/△ρmaX と
の関係は第2図に示すような特性となり、信号磁界と抵
抗変化率は著しく非直線な特性であり、この非直線性と
ダイナミックレンヂを可及的に広くするためにバイアス
磁界Hbを加えて動作点を第2図のP点に設定する必要
がある。
Furthermore, the relationship between the applied magnetic field H and the resistance change rate △ρ/△ρmaX has the characteristics shown in Figure 2, and the signal magnetic field and the resistance change rate have extremely nonlinear characteristics, and this nonlinearity and the dynamic range In order to make this as wide as possible, it is necessary to apply a bias magnetic field Hb and set the operating point to point P in FIG.

本発明はこれらの問題を解決したものであり、以下図面
を参照して、その実施例をあげ説明する。
The present invention solves these problems, and examples thereof will be described below with reference to the drawings.

第3図において、6は強磁性薄板であり一部に所定の幅
gの磁気空隙5を有する閉磁気回路を形成するよう構成
されている。
In FIG. 3, a ferromagnetic thin plate 6 is constructed to form a closed magnetic circuit having a magnetic gap 5 having a predetermined width g in a part thereof.

また、この閉磁気回路の一部には略々直線状部Iが形成
されている。
Further, a substantially linear portion I is formed in a part of this closed magnetic circuit.

しかして、前記直線状部の両端部、すなわち、前記閉磁
気回路の磁束の流れる方向に所定の距離だけ離れて検出
用電極8,9が設げられている。
Detection electrodes 8 and 9 are provided at both ends of the linear portion, that is, separated by a predetermined distance in the direction in which the magnetic flux of the closed magnetic circuit flows.

12は永久磁石で、図に示すように、強磁性薄板6の直
線状部7に近接して配置されている。
Reference numeral 12 denotes a permanent magnet, which is arranged close to the linear portion 7 of the ferromagnetic thin plate 6, as shown in the figure.

以上のように構成することにより、記録媒体(図示せず
)よりの信号磁束は、空隙5よりピックアップされ、前
記磁性薄板が閉磁気回路を構成しているため、記録媒体
より離れた位置にある前記直線状部にも有効に導かれる
ものである。
With the above configuration, the signal magnetic flux from the recording medium (not shown) is picked up through the air gap 5, and since the magnetic thin plate forms a closed magnetic circuit, the signal magnetic flux is located at a distance from the recording medium. It is also effectively guided to the linear portion.

従って、この直線状部7を流れる信号磁束に応じた直線
状部7の電気的抵抗値の変化を前記検出用電極間の電圧
変化として検出できるものである。
Therefore, a change in the electrical resistance value of the linear portion 7 according to the signal magnetic flux flowing through the linear portion 7 can be detected as a voltage change between the detection electrodes.

さらに、磁気抵抗効果素子として働く強磁性薄板6の直
線状部7は一軸異方向性に配向され、その磁化容易方向
は矢印10の方向、すなわち、信号磁束の流れる方向お
よび検出電流の方向と一致させている。
Further, the linear portion 7 of the ferromagnetic thin plate 6 that acts as a magnetoresistive element is uniaxially anisotropically oriented, and its easy magnetization direction coincides with the direction of the arrow 10, that is, the direction in which the signal magnetic flux flows and the direction of the detection current. I'm letting you do it.

また、前記磁化容易方向と直角方向(矢印11)にバイ
アス磁界を印加するよう例えば磁石12が設げられてい
る。
Further, a magnet 12, for example, is provided to apply a bias magnetic field in a direction (arrow 11) perpendicular to the easy magnetization direction.

一方磁気抵抗効果素子の比抵抗値ρと素子の強磁性薄板
の磁化方向と電流となす角度θとの関係より、角度変化
と抵抗変化の関係は第5図に示すようにθ−45°のと
き最大となる。
On the other hand, from the relationship between the specific resistance value ρ of the magnetoresistive element and the angle θ between the magnetization direction of the ferromagnetic thin plate of the element and the current, the relationship between the angle change and the resistance change is as shown in Figure 5. maximum when

即ち、磁気感応用素子の印加磁界に対する感度が最も良
く、且つダイナミック、レンジの広い所に動作点を設定
できる。
That is, the operating point can be set at a location where the magnetic sensing element has the best sensitivity to the applied magnetic field and a wide dynamic range.

なお、第5図の抵抗変化は抵抗変化の最大値△ρmax
で正規化して示している。
Note that the resistance change in Fig. 5 is the maximum value of resistance change △ρmax
It is normalized and shown.

このような動作特性を考慮して、所定の値の前記バイア
ス磁界Hbを印加すると直線部7の磁化の方向が配向方
向から略45°傾斜した動作点に設定することが出来る
In consideration of such operating characteristics, when the bias magnetic field Hb of a predetermined value is applied, the direction of magnetization of the straight portion 7 can be set to an operating point inclined at approximately 45 degrees from the orientation direction.

信号磁界による電気抵抗値の変化を大きく検出するため
には磁気抵抗素子の抵抗値はできるだけ高い方が望まし
いので、素子の長手方向と電流の方向は一致させた構成
にするのが得策である。
In order to detect a large change in electrical resistance due to a signal magnetic field, it is desirable that the resistance value of the magnetoresistive element be as high as possible, so it is a good idea to configure the element so that the longitudinal direction of the element matches the direction of the current.

以上のように本発明によれば、磁気抵抗効果素子に与え
るバイアス磁界が記録媒体に影響を与えることのない構
造にすることができ、また、素子の長手方向と信号磁束
の方向が一致するため素子形状による反磁界の影響を非
常に小さくした構成で動作させることができる。
As described above, according to the present invention, it is possible to create a structure in which the bias magnetic field applied to the magnetoresistive element does not affect the recording medium, and also because the longitudinal direction of the element coincides with the direction of the signal magnetic flux. It is possible to operate with a configuration in which the influence of the demagnetizing field due to the element shape is extremely reduced.

さらに、磁性薄膜の磁化容易方向と信号磁束通過方向と
を一致させていることもあって、構造が簡単な磁気抵抗
効果型磁気ヘッドを得ることができる。
Furthermore, since the easy magnetization direction of the magnetic thin film and the signal magnetic flux passing direction are made to coincide with each other, it is possible to obtain a magnetoresistive magnetic head with a simple structure.

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

第1図イ、中主それぞれ従来の磁気抵抗効果型磁気ヘッ
ドを示す斜視図、第2図は同動作説明図、第3図は本発
明の一実施例を模式的に示す斜視図、第4図は同要部斜
視図、第5図は磁気抵抗効果素子の電気抵抗変化率と磁
化回転角との関係を示す図である。 5・・・・・・磁気空隙、6・・・・・・強磁性薄板(
磁気抵抗効果素子)、8,9・・・・・・検出用電極、
12・・・・・・磁石。
Fig. 1A is a perspective view showing a conventional magnetoresistive magnetic head, Fig. 2 is an explanatory view of the same operation, Fig. 3 is a perspective view schematically showing an embodiment of the present invention, and Fig. 4 is a perspective view showing a conventional magnetoresistive magnetic head. The figure is a perspective view of the same main part, and FIG. 5 is a diagram showing the relationship between the rate of change in electrical resistance and the magnetization rotation angle of the magnetoresistive element. 5...Magnetic air gap, 6...Ferromagnetic thin plate (
magnetoresistive effect element), 8, 9... detection electrode,
12... Magnet.

Claims (1)

【特許請求の範囲】[Claims] 1 強磁性薄板により一部に磁気空隙を有する閉磁気回
路を構成し、この閉磁気回路を通る信号磁束の方向に所
定の距離だけ離して検出用電極を設けるとともに、この
両電極間であって前記磁気空隙を含まない強磁性薄板の
部分に近接して永久磁石を配置し、前記部分を流れる電
流の方向と直角な方向のバイアス磁界を印加し、さらに
信号磁束の流れる方向を磁化容易方向とすることを特徴
とする磁気ヘッド。
1 A closed magnetic circuit having a magnetic air gap in a part is constructed using a ferromagnetic thin plate, and a detection electrode is provided a predetermined distance apart in the direction of the signal magnetic flux passing through this closed magnetic circuit, and a detection electrode is provided between the two electrodes. A permanent magnet is placed close to a portion of the ferromagnetic thin plate that does not include a magnetic gap, a bias magnetic field is applied in a direction perpendicular to the direction of current flowing through the portion, and the direction in which the signal magnetic flux flows is set as the easy magnetization direction. A magnetic head characterized by:
JP49095772A 1974-08-20 1974-08-20 Jikihed Expired JPS5846765B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP49095772A JPS5846765B2 (en) 1974-08-20 1974-08-20 Jikihed

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP49095772A JPS5846765B2 (en) 1974-08-20 1974-08-20 Jikihed

Publications (2)

Publication Number Publication Date
JPS5123126A JPS5123126A (en) 1976-02-24
JPS5846765B2 true JPS5846765B2 (en) 1983-10-18

Family

ID=14146764

Family Applications (1)

Application Number Title Priority Date Filing Date
JP49095772A Expired JPS5846765B2 (en) 1974-08-20 1974-08-20 Jikihed

Country Status (1)

Country Link
JP (1) JPS5846765B2 (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3493694A (en) * 1966-01-19 1970-02-03 Ampex Magnetoresistive head
JPS5610684A (en) * 1979-07-04 1981-02-03 Nippon Kokan Kk Vertical lime baking kiln

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3493694A (en) * 1966-01-19 1970-02-03 Ampex Magnetoresistive head
JPS5610684A (en) * 1979-07-04 1981-02-03 Nippon Kokan Kk Vertical lime baking kiln

Also Published As

Publication number Publication date
JPS5123126A (en) 1976-02-24

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