JPH08203032A - Magneto-resistance effect reproducing head - Google Patents

Magneto-resistance effect reproducing head

Info

Publication number
JPH08203032A
JPH08203032A JP7011245A JP1124595A JPH08203032A JP H08203032 A JPH08203032 A JP H08203032A JP 7011245 A JP7011245 A JP 7011245A JP 1124595 A JP1124595 A JP 1124595A JP H08203032 A JPH08203032 A JP H08203032A
Authority
JP
Japan
Prior art keywords
magnetic
reproducing head
bias
magnetoresistive
region
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
JP7011245A
Other languages
Japanese (ja)
Inventor
Ikuo Saito
郁夫 斎藤
Chiaki Ishikawa
千明 石川
Katsuhisa Fujimoto
勝久 藤本
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP7011245A priority Critical patent/JPH08203032A/en
Publication of JPH08203032A publication Critical patent/JPH08203032A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE: To suppress the generation of Barkhausen noise and to improve the symmetry of an offtrack characteristic by making the influence of a bias magnetic field and the diamagnetic field generated by magnetization of the magnetosensitive part itself uniform. CONSTITUTION: This reproducing head is provided with a magneto-resistance layer 10 having the central part magnetosensitive region 11 having an elliptic shape for detecting the leakage magnetic field from a medium. This resistance layer 10 has the region 11 and an end part magnetic domain control region 12 for controlling the generation of the Barkhausen noise by controlling the magnetic domain structure the central part magnetosensitive region. The longitudinal direction bias is generated by a hard magnetic material layer 30 which is formed in parallel with the resistance layer 10 and comes into direct contact with the end part magnetic domain control region 12. The transverse direction bias is generated by a shunt film 20 and SAL film 21 in parallel with the resistance layer 10. The influence of the bias magnetic field and the diamagnetic field generated by the magnetization of the magnetosensitive part itself is then made uniform. Consequently, the generation of the Barkhausen noise is controlled.

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、磁気記録媒体から情報
信号を読み取るための再生ヘッドに係り、特に、改良さ
れた磁気抵抗効果型再生ヘッドに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a reproducing head for reading an information signal from a magnetic recording medium, and more particularly to an improved magnetoresistive effect reproducing head.

【0002】[0002]

【従来の技術】従来、磁気抵抗効果(MR)センサまた
はヘッドと呼ばれる磁気読み取り変換機が知られてい
る。このようなセンサは、大きな線密度の磁気表面から
データを読み取ることができることが知られている。M
Rセンサは、磁気抵抗効果材料から作った読み取り素子
の抵抗変化を使って、磁気信号を素子が感知する磁束の
量及び方向の関数として検出する。
2. Description of the Related Art Conventionally, a magnetic reading converter called a magnetoresistive (MR) sensor or a head is known. It is known that such sensors can read data from magnetic surfaces of high linear density. M
The R sensor uses the resistance change of a read element made of a magnetoresistive material to detect a magnetic signal as a function of the amount and direction of magnetic flux sensed by the element.

【0003】従来の技術では、MR素子が最適に動作す
るためには、二つのバイアス磁界をかける必要があるこ
とが開示されている。一つは磁束に対する応答が線形に
なるようにMR素子に横方向バイアス磁界をかける。こ
のバイアス磁界は、磁気媒体の面に垂直で、平坦なMR
素子の表面に平行である。いま一つは、MR素子内の多
磁区作用から生じるバルクハウゼンノイズを抑えるため
に、磁気媒体の表面に平行、かつMR素子の長手方向に
かける縦方向バイアスである。
The prior art discloses that it is necessary to apply two bias magnetic fields for the MR element to operate optimally. One is to apply a lateral bias magnetic field to the MR element so that the response to the magnetic flux becomes linear. This bias magnetic field is perpendicular to the plane of the magnetic medium and has a flat MR.
It is parallel to the surface of the device. The other is a vertical bias applied in parallel with the surface of the magnetic medium and in the longitudinal direction of the MR element in order to suppress Barkhausen noise caused by multi-domain effect in the MR element.

【0004】MRセンサ用のバイアス法および装置が従
来技術で多数開発されている。しかし、記録密度を大き
くするにつれて、記録トラックをより狭くし、トラック
に沿った線記録密度を大きくすることが必要になってき
た。これらの用件を満たす小形MRセンサは、従来技術
を使用して実現することはできない。
Many biasing methods and devices for MR sensors have been developed in the prior art. However, as the recording density has increased, it has become necessary to narrow the recording track and increase the linear recording density along the track. Small MR sensors that meet these requirements cannot be realized using conventional techniques.

【0005】これらの従来技術の問題に対する概念上の
解決策が、パターン化した縦方向バイアスの実施によっ
て得られた。この解決策は、特開昭60−59518 号および
特開平2−220213 号に記述されている。簡単にいうと、
上記従来例はMR層の端部領域を適切な単磁区状態に
し、この結果、MR層の中央感磁部領域内に単磁区状態
が誘導されるものである。これは、MR層の端部領域に
接して、MR膜より保磁力の大きい強磁性帯層を設ける
ことで、端部領域内だけに縦方向バイアスを発生させる
ことによって実現できる。この概念の実施例では、縦方
向バイアスは、硬磁性体層と軟磁性MR層の強磁性交換
結合もしくは静磁結合によって実現される。
A conceptual solution to these prior art problems has been obtained by implementing patterned longitudinal biasing. This solution is described in JP-A-60-59518 and JP-A-2-220213. Simply put,
In the above-mentioned conventional example, the end region of the MR layer is brought into an appropriate single domain state, and as a result, the single domain state is induced in the central magnetic sensitive region of the MR layer. This can be realized by providing a ferromagnetic band layer having a coercive force larger than that of the MR film in contact with the end region of the MR layer to generate a longitudinal bias only in the end region. In an embodiment of this concept, the longitudinal bias is realized by ferromagnetic exchange coupling or magnetostatic coupling between the hard magnetic layer and the soft magnetic MR layer.

【0006】[0006]

【発明が解決しようとする課題】これらの従来技術で
は、いずれもヘッドの感度もしくはヘッドのバルクハウ
ゼンノイズ抑制等に着目しているが、トラック幅方向の
感度分布は図3のbに示すように左右非対称になる。と
ころが位置決め用のサーボ信号読み取り用ヘッドとして
用いるためには、オフトラック特性の対称性が必要とさ
れる。オフトラック特性の対称性を悪くする要因の一つ
に感磁部端部における反磁界の非一様性がある。
In all of these conventional techniques, attention is paid to the sensitivity of the head or suppression of Barkhausen noise of the head, but the sensitivity distribution in the track width direction is as shown in FIG. It becomes asymmetrical. However, in order to use it as a servo signal reading head for positioning, symmetry of off-track characteristics is required. One of the factors that deteriorate the symmetry of the off-track characteristics is the non-uniformity of the demagnetizing field at the end of the magnetic sensitive section.

【0007】本発明の目的は、位置決め用のサーボ信号
読み取り用ヘッドとして用いるのに適した、オフトラッ
ク特性の対称性が良好な磁気抵抗効果型再生ヘッドを得
ることにある。
An object of the present invention is to obtain a magnetoresistive effect reproducing head suitable for use as a servo signal reading head for positioning and having a good symmetry of off-track characteristics.

【0008】[0008]

【課題を解決するための手段】上記問題を解決するため
に、本発明は中央感磁部または横方向バイアス膜あるい
はその両方の形状を、従来のように多角形のみで形成す
るのでなく、回転楕円体または厚さ一様の楕円形もしく
は楕円形を近似する多角形に形成し、感磁部端部におけ
る反磁界の非一様性の影響を減少させることにより達せ
られる。
In order to solve the above-mentioned problems, the present invention does not form the central magnetic field sensing portion and / or the lateral bias film or both of them with polygons as in the prior art, but rotates them. This can be achieved by forming an ellipsoid or an ellipse having a uniform thickness or a polygon approximating an ellipse to reduce the influence of non-uniformity of the demagnetizing field at the end of the magnetic sensitive section.

【0009】[0009]

【作用】図4は従来の矩形のMRヘッドに横方向バイア
スを印加したときの反磁界を模式的に示したものであ
る。横方向バイアス磁界により、感磁部領域の磁化は約
45度傾き、また縦方向バイアス磁界により磁区制御領
域の磁化は膜の長手方向を向く。このような磁化状態が
矩形をした感磁部に作る反磁界は、MR膜の左下部より
右下部の方が小さい。トラック幅方向の感度分布が左右
で非対称になる原因は、媒体からの漏洩磁界の影響が強
いMR膜の下部において、反磁界の影響が左右で異なる
ことによる。
FIG. 4 schematically shows a demagnetizing field when a lateral bias is applied to a conventional rectangular MR head. The lateral bias magnetic field causes the magnetization of the magnetic sensitive region to be inclined by about 45 degrees, and the longitudinal bias magnetic field causes the magnetization of the magnetic domain control region to be oriented in the longitudinal direction of the film. The demagnetizing field created in the magnetic sensitive portion having such a rectangular magnetized state is smaller in the lower right portion than in the lower left portion of the MR film. The reason why the sensitivity distribution in the track width direction is asymmetric between left and right is that the effect of the demagnetizing field is different between the left and right in the lower part of the MR film where the effect of the leakage magnetic field from the medium is strong.

【0010】本発明によれば、中央感磁部または横方向
バイアス膜あるいはその両方の形状を、回転楕円体また
は厚さ一様の楕円形もしくは楕円形を近似する多角形に
形成することにより、感磁部または横方向バイアス膜あ
るいはその両方の反磁界の影響を均一にすることができ
るので、オフトラック特性の対称性が良好な磁気抵抗効
果型再生ヘッドを得ることが出来る。
According to the present invention, by forming the shape of the central magnetic sensing portion and / or the lateral bias film or both into a spheroid or an ellipse of uniform thickness or a polygon approximating an ellipse, Since the influence of the demagnetizing field of the magnetic sensitive section and / or the lateral bias film or both of them can be made uniform, it is possible to obtain a magnetoresistive effect reproducing head having good symmetry of off-track characteristics.

【0011】[0011]

【実施例】本発明による代表的な磁気抵抗効果再生ヘッ
ドは、図1に示すように、媒体からの漏洩磁界を検出す
るための楕円形をした中央部感磁領域11を有する磁気
抵抗層10によって特徴づけられる。磁気抵抗層10
は、中央部感磁領域11および中央部感磁領域の磁区構
造を制御し、バルクハウゼンノイズの発生を制御するた
めの端部磁区制御領域12に分けられる。
DESCRIPTION OF THE PREFERRED EMBODIMENTS A typical magnetoresistive effect reproducing head according to the present invention, as shown in FIG. 1, has a magnetoresistive layer 10 having an oval central magnetic sensitive area 11 for detecting a leakage magnetic field from a medium. Characterized by Magnetoresistive layer 10
Are divided into a central magnetic sensitive region 11 and an end magnetic domain control region 12 for controlling the magnetic domain structure of the central magnetic sensitive region and controlling the generation of Barkhausen noise.

【0012】図2は本発明による代表的な磁気抵抗効果
再生ヘッドの断面図であり、ヘッドは磁気抵抗層10,
横方向バイアス印加用シャント膜20,SAL膜21,
縦方向バイアス印加用硬磁性体層30,電極層40から
構成される。本実施例では、SAL膜形状も楕円形に形
成をした。ヘッドの形成はスパッタリング法により、楕
円型に形成するためには、マスクをもちいた。
FIG. 2 is a sectional view of a typical magnetoresistive effect reproducing head according to the present invention.
Lateral bias application shunt film 20, SAL film 21,
It comprises a hard magnetic layer 30 for longitudinal bias application and an electrode layer 40. In this example, the SAL film was also formed into an elliptical shape. The head was formed by a sputtering method, and a mask was used to form the head into an elliptical shape.

【0013】ここで、縦方向バイアスは磁気抵抗層10
に平行とし、端部磁区制御領域12に直接接する硬磁性
体層30によって発生させる。また、横方向バイアスは
磁気抵抗層10に平行するシャント膜20およびSAL
膜21によって発生させる。電極層40は、信号検出電
流およびバイアス電流を磁気抵抗層10およびシャント
膜20に伝え、出力信号を外部電気回路に伝えるための
電気経路である。
Here, the longitudinal bias is the magnetoresistive layer 10.
And is generated by the hard magnetic layer 30 that is in parallel with the edge magnetic domain control region 12 and is in direct contact with the end magnetic domain control region 12. Further, the lateral bias is applied to the shunt film 20 and SAL parallel to the magnetoresistive layer 10.
It is generated by the membrane 21. The electrode layer 40 is an electric path for transmitting a signal detection current and a bias current to the magnetoresistive layer 10 and the shunt film 20 and transmitting an output signal to an external electric circuit.

【0014】本実施例では、磁気抵抗層の厚さを5から
20nm、硬磁性体層の厚さを10から100nm、シ
ャント膜の厚さを10から40nmとした。電極内端面
間の距離Tは5μm、硬磁性体内面間距離Wは7μmと
した。磁気抵抗層は長径Wが7μmまた短径すなわち高
さHが6μmの楕円形に形成した。また磁気抵抗層はN
i−Fe合金、硬磁性体層はCoPtCr合金、シャン
ト膜はNb膜とした。硬磁性体層はCo合金系の磁気記
録媒体材料が有効であった。
In this embodiment, the magnetoresistive layer has a thickness of 5 to 20 nm, the hard magnetic layer has a thickness of 10 to 100 nm, and the shunt film has a thickness of 10 to 40 nm. The distance T between the inner end surfaces of the electrode was 5 μm, and the distance W between the inner surfaces of the hard magnetic body was 7 μm. The magnetoresistive layer was formed in an elliptical shape having a long diameter W of 7 μm and a short diameter, that is, a height H of 6 μm. The magnetoresistive layer is N
The i-Fe alloy, the hard magnetic layer was a CoPtCr alloy, and the shunt film was an Nb film. For the hard magnetic layer, a Co alloy-based magnetic recording medium material was effective.

【0015】図3は本実施例のヘッドと、従来ヘッドの
トラック幅方向の感度分布を示したものである。図にお
いてaは本実施例のMRヘッドのトラック幅方向の感度
分布を示し、bは従来型MRヘッドのトラック幅方向の
感度分布を示す。本測定は、MRヘッドのトラック幅よ
り狭い領域に記録した媒体を、トラック幅方向に移動し
ながら再生出力の計測を行ったものである。記録用ヘッ
ドとしてはトラック幅0.5μm の磁気誘導型ヘッド
(アイイーイーイー トランザクションズ オンマグネ
ティクス(IEEE Trans. Magn.)Vol.27,4678(1
991))を用いた。
FIG. 3 shows the sensitivity distribution in the track width direction of the head of this embodiment and the conventional head. In the figure, a shows the sensitivity distribution in the track width direction of the MR head of this embodiment, and b shows the sensitivity distribution in the track width direction of the conventional MR head. In this measurement, the reproduction output was measured while moving the medium recorded in an area narrower than the track width of the MR head in the track width direction. As a recording head, a magnetic induction type head having a track width of 0.5 μm (IEEE Trans. Magn.) Vol. 27, 4678 (1
991)) was used.

【0016】図から、従来型のMRヘッドのトラック幅
方向の感度分布は、本実施例のMRヘッドのトラック幅
方向の感度分布より左右の非対称性が大きいことが分か
る。実際、本実施例のMRヘッドの感度のピークはヘッ
ドの中心にあるが、従来型のMRヘッドの感度のピーク
は12.5% 中心から左側にある。
From the figure, it can be seen that the sensitivity distribution in the track width direction of the conventional MR head has a greater left-right asymmetry than the sensitivity distribution in the track width direction of the MR head of this embodiment. In fact, the sensitivity peak of the MR head of this embodiment is in the center of the head, whereas the sensitivity peak of the conventional MR head is 12.5% to the left of the center.

【0017】なお、MR素子に横方向バイアス磁界を印
加する方法として、電流バイアス法,シャントバイアス
法,ソフトバイアス法,SALバイアス法のいずれを用
いても、同様の効果が得られる。また膜の順序を入れ替
えても、対称性が良く成る効果は保持される。
The same effect can be obtained by using any of the current bias method, the shunt bias method, the soft bias method, and the SAL bias method as a method for applying the lateral bias magnetic field to the MR element. Even if the order of the films is changed, the effect of improving the symmetry is maintained.

【0018】本実施例では、中央部感磁領域およびSA
L膜の両方を楕円形に形成をしたが、どちらか一方のみ
でも、対称化の効果が認められる。
In the present embodiment, the central magnetic sensitive area and SA
Both of the L films were formed into an elliptical shape, but the symmetrization effect can be observed with only one of them.

【0019】[0019]

【発明の効果】本発明は、バイアス磁界および感磁部自
身の磁化によって生じる反磁界の影響を一様化すること
により、低減する効果があり、オフトラック特性の対称
性が良好な磁気抵抗効果型再生ヘッドを得ることが出来
る。
The present invention has the effect of reducing the effect by uniformizing the influence of the bias magnetic field and the demagnetizing field generated by the magnetization of the magnetically sensitive portion itself, and the magnetoresistive effect with good symmetry of the off-track characteristics. A mold reproducing head can be obtained.

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

【図1】本発明の一実施例の磁気抵抗効果再生ヘッドの
要部裏面図。
FIG. 1 is a rear view of a main part of a magnetoresistive effect reproducing head according to an embodiment of the present invention.

【図2】本発明による磁気抵抗効果再生ヘッドの実施例
の断面図。
FIG. 2 is a sectional view of an embodiment of a magnetoresistive effect reproducing head according to the present invention.

【図3】本発明と従来のヘッドにおける、トラック幅方
向の感度分布図。
FIG. 3 is a sensitivity distribution diagram in the track width direction of the head of the present invention and the conventional head.

【図4】従来の磁気抵抗効果再生ヘッドにおけるバイア
ス磁界中の反磁界の模式図。
FIG. 4 is a schematic diagram of a demagnetizing field in a bias magnetic field in a conventional magnetoresistive effect reproducing head.

【符号の説明】[Explanation of symbols]

10…磁気抵抗層、11…中央部感磁領域、12…端部
磁区制御領域、20…シャント膜、21…SAL膜、3
0…硬磁性体層、40…電極。
DESCRIPTION OF SYMBOLS 10 ... Magnetoresistive layer, 11 ... Central magnetic field sensitive area, 12 ... Edge magnetic domain control area, 20 ... Shunt film, 21 ... SAL film, 3
0 ... Hard magnetic layer, 40 ... Electrode.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】中央部感磁領域と端部磁区制御領域を有す
る磁気抵抗層,この両側に接続された電極,磁気抵抗層
に横方向バイアスを発生するためのパターン,磁気抵抗
層を磁気シールドするために両側に設けた軟磁性膜、お
よびこれを支持する基体からなる磁気抵抗効果再生ヘッ
ドにおいて、中央感磁部または横方向バイアス膜あるい
はその両方の形状を、回転楕円体または厚さ一様の楕円
形もしくは楕円形を近似する多角形に形成することを特
徴とする磁気抵抗効果再生ヘッド。
1. A magnetoresistive layer having a central magnetic sensitive region and an end magnetic domain control region, electrodes connected to both sides thereof, a pattern for generating a lateral bias in the magnetoresistive layer, and a magnetic shield for the magnetoresistive layer. In the magnetoresistive effect reproducing head including a soft magnetic film provided on both sides for supporting the magnetic resistance effect reproducing head, the shape of the central magnetically sensitive portion and / or the lateral bias film is equal to the spheroid or the uniform thickness. 2. A magnetoresistive effect reproducing head characterized by being formed into an elliptical shape or a polygonal shape approximating the elliptical shape.
【請求項2】前記磁気抵抗層は磁気抵抗効果または巨大
磁気抵抗効果で動作することを特徴とした請求項1に記
載の磁気抵抗効果再生ヘッド。
2. The magnetoresistive effect reproducing head according to claim 1, wherein the magnetoresistive layer operates by a magnetoresistive effect or a giant magnetoresistive effect.
JP7011245A 1995-01-27 1995-01-27 Magneto-resistance effect reproducing head Pending JPH08203032A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7011245A JPH08203032A (en) 1995-01-27 1995-01-27 Magneto-resistance effect reproducing head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7011245A JPH08203032A (en) 1995-01-27 1995-01-27 Magneto-resistance effect reproducing head

Publications (1)

Publication Number Publication Date
JPH08203032A true JPH08203032A (en) 1996-08-09

Family

ID=11772564

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7011245A Pending JPH08203032A (en) 1995-01-27 1995-01-27 Magneto-resistance effect reproducing head

Country Status (1)

Country Link
JP (1) JPH08203032A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08297814A (en) * 1995-04-28 1996-11-12 Nec Corp Magneto-resistance effect element
AT407803B (en) * 1996-11-06 2001-06-25 Diplomingenieur Hans Schiebel Magnetic field sensor
WO2002035559A2 (en) * 2000-10-24 2002-05-02 Motorola, Inc. Magnetic layer formed of multiple sub-element layers
US6529352B1 (en) 1996-05-13 2003-03-04 Nec Corporation Magnetoresistive sensing element and magnetic head using the magnetoresistive sensing element

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08297814A (en) * 1995-04-28 1996-11-12 Nec Corp Magneto-resistance effect element
US6529352B1 (en) 1996-05-13 2003-03-04 Nec Corporation Magnetoresistive sensing element and magnetic head using the magnetoresistive sensing element
AT407803B (en) * 1996-11-06 2001-06-25 Diplomingenieur Hans Schiebel Magnetic field sensor
WO2002035559A2 (en) * 2000-10-24 2002-05-02 Motorola, Inc. Magnetic layer formed of multiple sub-element layers
WO2002035559A3 (en) * 2000-10-24 2002-07-18 Motorola Inc Magnetic layer formed of multiple sub-element layers
US6579625B1 (en) 2000-10-24 2003-06-17 Motorola, Inc. Magnetoelectronics element having a magnetic layer formed of multiple sub-element layers

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