JPH01264622A - Magneto-resistance effect type magnetic head - Google Patents

Magneto-resistance effect type magnetic head

Info

Publication number
JPH01264622A
JPH01264622A JP9154888A JP9154888A JPH01264622A JP H01264622 A JPH01264622 A JP H01264622A JP 9154888 A JP9154888 A JP 9154888A JP 9154888 A JP9154888 A JP 9154888A JP H01264622 A JPH01264622 A JP H01264622A
Authority
JP
Japan
Prior art keywords
sliding surface
theta
magnetic
magnetic head
noise
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
JP9154888A
Other languages
Japanese (ja)
Inventor
Naoki Koyama
直樹 小山
Hideo Tanabe
英男 田辺
Koji Takano
公史 高野
Noboru Shimizu
昇 清水
Kazuo Shiiki
椎木 一夫
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 JP9154888A priority Critical patent/JPH01264622A/en
Publication of JPH01264622A publication Critical patent/JPH01264622A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/33Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only
    • G11B5/39Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects
    • G11B5/3903Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects using magnetic thin film layers or their effects, the films being part of integrated structures
    • G11B5/398Specially shaped layers
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/33Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only
    • G11B5/39Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects
    • G11B5/3903Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects using magnetic thin film layers or their effects, the films being part of integrated structures

Landscapes

  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Magnetic Heads (AREA)

Abstract

PURPOSE:To decrease the noises generated by adjacent tracks by parting a magnetic head element except in a track part from a sliding surface. CONSTITUTION:A magneto-resistance effect type element 2 is curved with respect to the sliding surface 1 so that the part 21 except the track width is parted from the sliding surface 1. A magnetic shielding layer 3 consisting of a soft magnetic material is provided between the surface 1 and the element 2. The Barkhausen noise output increases with an increase in theta if the angle between the curved part of the element 2 and the sliding surface is designated as theta in this constitution. On the other hand, the crosstalk noise output decreases with an increase in the theta. Any noise outputs change with the theta in such a manner and the noises of both can be successfully decreased by setting the theta to a 5-40 deg. range. The similar effect is obtainable even if the layer 3 is not formed; however, the crosstalk noises increase in such a case. The better result is, therefore, obtd. when the layer 3 is provided.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、高密度磁気記録に係り、特に再生感度の高い
磁気抵抗効果型磁気ヘッドに関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to high-density magnetic recording, and particularly to a magnetoresistive magnetic head with high reproduction sensitivity.

〔従来の技術〕[Conventional technology]

強磁性金属薄膜の磁気抵抗効果を利用した磁気抵抗効果
型磁気ヘッド(以下、MRヘヘッと記す)は、再生出力
が記録媒体の走行速度に依存せず、狭トラツク化が容易
であることから、高密度磁気記録用再生ヘッドとして注
目されている。しかしながら、MRヘヘッにおいては、
狭トラツク化により、MR素子内での不規則な磁壁移動
に起因するバルクハウゼンノイズが増大する。このバル
クハウゼンノイズが再生感度を劣化させ、狭トラツク化
を妨げる要因の]つとなっていた。
A magnetoresistive magnetic head (hereinafter referred to as MR head), which utilizes the magnetoresistive effect of a ferromagnetic metal thin film, has a reproduction output that does not depend on the running speed of the recording medium and can easily narrow the track. It is attracting attention as a reproducing head for high-density magnetic recording. However, in MR hehe,
The narrowing of the track increases Barkhausen noise caused by irregular domain wall movement within the MR element. This Barkhausen noise deteriorates reproduction sensitivity and is one of the factors that prevents narrowing of the track.

このノイズを低減するためには、MR素子が、単磁区構
造をとるようにすることが有効であり、この方法として
、MR素子の形状をアスペクト比の大きなストライプ状
や、額縁状の閉磁路構造とすることなどが提案されてい
る。
In order to reduce this noise, it is effective to make the MR element have a single magnetic domain structure.As a method, the shape of the MR element can be changed to a stripe shape with a large aspect ratio or a closed magnetic circuit structure like a picture frame. It has been proposed that

このような技術に関しては日本応用磁気学会誌第11巻
 第2号(1987年)第95頁から98頁において論
じられている。
Such techniques are discussed in Journal of the Japan Society of Applied Magnetics, Vol. 11, No. 2 (1987), pp. 95-98.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上記技術はバルクハウゼンノイズは低減できるものの、
MR素子の長さがトラック幅よりも長くなる。このため
隣接するトラックによるクロストークが発生し、ノイズ
の原因となるという問題があった。
Although the above technology can reduce Barkhausen noise,
The length of the MR element becomes longer than the track width. Therefore, there is a problem in that crosstalk between adjacent tracks occurs, causing noise.

本発明は、バルクハウゼンノイズを低減すると同時に隣
接するトラックによるクロストークノイズをも低減した
磁気抵抗効果型ヘッドを提供することにある。
An object of the present invention is to provide a magnetoresistive head that reduces Barkhausen noise and at the same time reduces crosstalk noise caused by adjacent tracks.

〔課題を解決するための手段〕[Means to solve the problem]

上記目的はトラック幅以上の長さを有するMR素子にお
いて、トラック幅部分だけを摺動面に露出させ、トラッ
ク幅の両側のMR素子を除々に摺動面から遠ざけて、わ
ん曲した形状を持たせることによって達成される。すな
わち、トラック幅以外の部分のMR素子と媒体との間隔
を大きくすることによって、隣接1へラックから流入す
る磁束が激減するため、クロストークノイズは減少する
The above purpose is to expose only the track width portion to the sliding surface in an MR element having a length longer than the track width, and gradually move the MR elements on both sides of the track width away from the sliding surface to create a curved shape. This is achieved by That is, by increasing the distance between the MR element and the medium in areas other than the track width, the magnetic flux flowing from the rack to the adjacent 1 is drastically reduced, and thus crosstalk noise is reduced.

さらに、このMR素子と摺動面との間に、磁気的なシー
ルド層となる軟磁性体を設けることによってクロストー
クノイズをさらに低減することができる。
Further, crosstalk noise can be further reduced by providing a soft magnetic material serving as a magnetic shield layer between the MR element and the sliding surface.

〔作用〕[Effect]

第2図、第3図を用いて本発明の詳細な説明する。第2
図はMRヘヘッ構造を示す平面図である。
The present invention will be explained in detail using FIGS. 2 and 3. Second
The figure is a plan view showing the structure of the MR head.

摺動面1に対してMR素子2をわん曲させ、トラック幅
以外の部分21を摺動面1から離しである。
The MR element 2 is curved with respect to the sliding surface 1, and the portion 21 other than the track width is separated from the sliding surface 1.

また、摺動面とMR素子のあいだに軟磁性体からなる磁
気遮へい層3を設けである。MR素子の両端部21は電
極4で被覆しである。
Further, a magnetic shielding layer 3 made of a soft magnetic material is provided between the sliding surface and the MR element. Both ends 21 of the MR element are covered with electrodes 4.

同図において、MR素子のわん曲部と摺動面のなす角度
を0とする。第3図は、上記MR素子を用いて磁気ヘッ
ドを作製し、その再生時のノイズ−をθをパラメータに
調べたものである。○印はバルクハウゼンノイズ出力を
示し、θの増加とともに増加する。これは、0が大きく
なるとMR:M子の形状異方性が低下するため、磁区が
発生しやすくなるものと考えられる。一方、X印はクロ
ストークノイズ出力を示し、θが大きくなると低下する
。これは、θが大きくなると、MR素子の両端部分が、
摺動面から離れるために、隣接トラックからのノイズが
低減するものと考えられる。このように、いずれのノイ
ズ出力も0に対して変化し、両者のノイズを低減するた
めには、θを5°から40’の範囲、さらに好ましくは
20°前後の角度とすることが良いことがわかる。
In the figure, the angle between the curved portion of the MR element and the sliding surface is assumed to be 0. FIG. 3 shows a magnetic head manufactured using the above MR element, and the noise during reproduction was investigated using θ as a parameter. The circle indicates the Barkhausen noise output, which increases as θ increases. This is considered to be because as 0 increases, the shape anisotropy of the MR:M element decreases, making it easier for magnetic domains to occur. On the other hand, the mark X indicates the crosstalk noise output, which decreases as θ increases. This means that as θ increases, both ends of the MR element become
It is thought that noise from adjacent tracks is reduced because the tracks are separated from the sliding surface. In this way, both noise outputs change with respect to 0, and in order to reduce both noises, it is better to set θ to a range of 5° to 40', more preferably around 20°. I understand.

なお、第2図に示した磁気遮へい層3がない場合におい
ても、同様な結果が得られるが、クロストークノイズは
増加する。したがって、磁気遮へい層を設けたほうが好
ましい。
Note that even in the case where the magnetic shielding layer 3 shown in FIG. 2 is not provided, similar results can be obtained, but crosstalk noise increases. Therefore, it is preferable to provide a magnetic shielding layer.

〔実施例〕〔Example〕

以下、本発明の一実施例を第1図により説明する。本図
(a)はMRヘヘッの斜視図であり、(b)。
An embodiment of the present invention will be described below with reference to FIG. This figure (a) is a perspective view of the MR head, and (b) is a perspective view of the MR head.

(c)はそれぞれ、A−A’およびB−B’の断面図を
示す。同図において、MR素子2は絶縁層5を介して上
下の磁気シールド層31に挟まれている。MR素子の幅
は40μmで、中央の10μmの部分だけ摺動面に露出
させ、両側は摺動面に対して15°の角度で後退させで
ある。また素子の高さは8μmである。ここで、磁気シ
ールド層31は、膜厚2μmのパーマロイからなる。ま
た、MR素子2は膜厚500人のパーマロイと膜厚20
00人のTi膜からなる。電極パターン4は、膜厚20
00人のAuからなる。ここで、MR素子の動作に必要
なバイアス磁界は、素子においてTi膜に分流される電
流によって印加する。(シャントバイアス方式)。
(c) shows cross-sectional views along AA' and BB', respectively. In the figure, an MR element 2 is sandwiched between upper and lower magnetic shield layers 31 with an insulating layer 5 in between. The width of the MR element was 40 μm, and only the central 10 μm portion was exposed to the sliding surface, and both sides were set back at an angle of 15° with respect to the sliding surface. Further, the height of the element is 8 μm. Here, the magnetic shield layer 31 is made of permalloy with a thickness of 2 μm. In addition, the MR element 2 is made of permalloy with a film thickness of 500 mm and a film thickness of 20 mm.
It consists of a Ti film of 0.00 people. The electrode pattern 4 has a film thickness of 20
Consists of 00 Au. Here, the bias magnetic field necessary for the operation of the MR element is applied by a current shunted to the Ti film in the element. (Shunt bias method).

本実施例により作製した再生ヘッドと、従来構造の矩形
状すなわちO=0°のMR素子を持つ再生ヘッドのクロ
ス1−一りノイズを比較した。その結果本実施例のほう
が約2dBノイスが低く、ノイズ低減に効果のあること
がわかった。
Cross 1-1 noise was compared between the reproducing head manufactured according to this example and the reproducing head having a rectangular MR element having a conventional structure, that is, O=0°. As a result, it was found that this example had lower noise by about 2 dB and was more effective in reducing noise.

第4図に、本発明の他の実施例を示す。同図(a)は、
MRヘヘッの斜視図であり、(b)、(C)は、それぞ
れA−A’、B−B’の断面図である。M 1−<素子
2の幅は40μmで高さは8μmである。中央の長さ1
0μmの部分だけ摺動面に露出させ、両側は摺動面に対
して15°の角度で後退させである。また、この摺動面
とMR素子端部21の間には磁気シールド層3]の−・
部から構成されるシールド層32が存在する。
FIG. 4 shows another embodiment of the invention. In the same figure (a),
It is a perspective view of MR head, and (b) and (C) are sectional views of AA' and BB', respectively. M1-<The width of element 2 is 40 μm and the height is 8 μm. center length 1
Only a 0 μm portion was exposed on the sliding surface, and both sides were set back at an angle of 15° with respect to the sliding surface. Moreover, between this sliding surface and the MR element end 21, there is a magnetic shield layer 3].
There is a shield layer 32 consisting of parts.

ここで、MR素子2は、第j−の実施例と同様に、膜厚
500人のパーマロイと、膜厚2000人のTj膜から
なる。また電極4は、膜厚2000人のAυ膜からなる
。磁気シールド層は膜厚1μmのパーマロイからなり、
その一部を加工することによってシールド層32を形成
する。また、シールド層としてパーマロイ膜を用いたが
、他の軟磁性膜、例えば、F eA Q  b j合金
やco系非晶質合金などを用いることもできる。さらに
、基板として、M n、 −Z nなどのフェライト基
板を用いた場合には、基板を磁気シールド層と兼用する
ことができる。
Here, the MR element 2 is made of permalloy with a thickness of 500 strands and a Tj film with a thickness of 2000 strands, as in the j-th embodiment. Further, the electrode 4 is made of an Aυ film with a thickness of 2000. The magnetic shield layer is made of permalloy with a thickness of 1 μm,
A shield layer 32 is formed by processing a portion of the shield layer. Further, although a permalloy film is used as the shield layer, other soft magnetic films such as FeA Q b j alloy or co-based amorphous alloy can also be used. Furthermore, when a ferrite substrate such as M n or -Z n is used as the substrate, the substrate can also be used as a magnetic shield layer.

上記ヘッドにお刑るバイアス方式としてはシャントバイ
アス方式を用いたが、他のバイアス方式として知られる
バーバボール方式、永久磁石バイアス方式、ソフトフィ
ルムバイアス方式およびこれらを複合したバイアス方式
を用いることもできる。
Although a shunt bias method was used as the bias method for the above head, other known bias methods such as barber ball method, permanent magnet bias method, soft film bias method, and a combination of these bias methods can also be used. .

上記のM R素子2と同一寸法で直線状のMR素子を持
つヘッドと、本実施例によるヘッドの再生時のノイズを
測定した。その結果、本実施例のヘッドのほうがクロス
トークノイズは約4dB低く、ノイズ低減に効果のある
ことがわかった。また、バルクハウゼンノイズはほとん
ど観測されず、両ヘットの間で著しい差は見られなかっ
た。
Noise during reproduction was measured for a head having a linear MR element having the same dimensions as the above-mentioned MR element 2, and for the head according to this example. As a result, it was found that the crosstalk noise of the head of this example was about 4 dB lower and was effective in reducing noise. Additionally, Barkhausen noise was hardly observed, and no significant difference was observed between the two heads.

なお上記実施例において、MR索子2はいずれもわん曲
した矩形状であったが、第5図に示すようにMR素子端
部22を摺動面1に対して傾けることによって額縁状の
形状を持つM R素子にも適用することができる。また
本実施例ではMR素子の輪郭を直線であられしたか、な
だらかな円弧状の曲線を用いても同様な効果が得られる
In the above embodiments, each of the MR cords 2 had a curved rectangular shape, but by tilting the MR element end 22 with respect to the sliding surface 1, as shown in FIG. It can also be applied to an MR element with Further, in this embodiment, the same effect can be obtained even if the outline of the MR element is made into a straight line or by using a gentle arc-shaped curve.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、トラック部分以外のMR素子を摺動面
から遠ざけることができるので、隣接トラックによって
生じるノイズが低減できる。さらに感磁部以外のMR素
子端部と摺動面とのあいだに軟磁性層を設けることによ
って、より効果的に隣接トラックからのノイズを低減で
きる。
According to the present invention, since the MR elements other than the track portion can be moved away from the sliding surface, noise caused by adjacent tracks can be reduced. Furthermore, by providing a soft magnetic layer between the sliding surface and the end of the MR element other than the magnetic sensing portion, noise from adjacent tracks can be more effectively reduced.

【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磁気ヘッドの斜視図およ
び断面図、第2図は本発明の詳細な説明するMR素子の
平面図、第3図は本発明の効果をあられすノイズ出力と
テーパ角の関係を示すグラフ、第4図は本発明の他の実
施例を示す磁気ヘッドの斜視図および断面図、第5図は
本発明の他の実施例を示すMR素子の平面図である。 1・・・摺動図、2・・・MR素子、4・・・電極パタ
ーン、5・・・絶縁層、21・・・MR素子端部、31
・・・磁気シールド層、32・・・シールド層。
FIG. 1 is a perspective view and a sectional view of a magnetic head showing an embodiment of the present invention, FIG. 2 is a plan view of an MR element explaining the present invention in detail, and FIG. 3 is a noise output showing the effects of the present invention. 4 is a perspective view and a sectional view of a magnetic head showing another embodiment of the present invention, and FIG. 5 is a plan view of an MR element showing another embodiment of the present invention. be. DESCRIPTION OF SYMBOLS 1... Sliding diagram, 2... MR element, 4... Electrode pattern, 5... Insulating layer, 21... MR element end part, 31
...Magnetic shield layer, 32... Shield layer.

Claims (1)

【特許請求の範囲】 1、磁気抵抗効果型磁気ヘッドにおいて、感磁部となる
磁気抵抗効果素子の形状が、摺動面に対してわん曲し、
一部分だけが摺動面に露出していることを特徴とする磁
気抵抗効果型磁気ヘッド。 2、摺動面と磁気抵抗効果素子のわん曲部分とのなす角
度が5°〜40°の間にあることを特徴とする特許請求
の範囲第1項記載の磁気抵抗効果型磁気ヘッド。 3、摺動面に露出した部分と除いて摺動面と磁気抵抗効
果素子の間に、軟磁性層を有することを特徴とする特許
請求の範囲第1項記載の磁気抵抗効果型磁気ヘッド。 4、磁気抵抗効果素子の摺動面の間にある軟磁性層が、
磁気抵抗効果素子の両端または片側にある軟磁性層と磁
気的に結合されていることを特徴とする特許請求の範囲
第1項記載の磁気抵抗効果型磁気ヘッド。
[Claims] 1. In a magnetoresistive magnetic head, the shape of a magnetoresistive element serving as a magnetic sensing part is curved with respect to a sliding surface,
A magnetoresistive magnetic head characterized by having only a portion exposed to the sliding surface. 2. The magnetoresistive magnetic head according to claim 1, wherein the angle between the sliding surface and the curved portion of the magnetoresistive element is between 5° and 40°. 3. The magnetoresistive magnetic head according to claim 1, further comprising a soft magnetic layer between the sliding surface and the magnetoresistive element except for the portion exposed to the sliding surface. 4. The soft magnetic layer between the sliding surfaces of the magnetoresistive element is
2. The magnetoresistive magnetic head according to claim 1, wherein the magnetoresistive head is magnetically coupled to a soft magnetic layer at both ends or one side of the magnetoresistive element.
JP9154888A 1988-04-15 1988-04-15 Magneto-resistance effect type magnetic head Pending JPH01264622A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9154888A JPH01264622A (en) 1988-04-15 1988-04-15 Magneto-resistance effect type magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9154888A JPH01264622A (en) 1988-04-15 1988-04-15 Magneto-resistance effect type magnetic head

Publications (1)

Publication Number Publication Date
JPH01264622A true JPH01264622A (en) 1989-10-20

Family

ID=14029542

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9154888A Pending JPH01264622A (en) 1988-04-15 1988-04-15 Magneto-resistance effect type magnetic head

Country Status (1)

Country Link
JP (1) JPH01264622A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03273514A (en) * 1990-03-23 1991-12-04 Nec Corp Magnetoresistance effect head
JPH03276411A (en) * 1990-03-27 1991-12-06 Nec Corp Magneto-resistance effect type head device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03273514A (en) * 1990-03-23 1991-12-04 Nec Corp Magnetoresistance effect head
JPH03276411A (en) * 1990-03-27 1991-12-06 Nec Corp Magneto-resistance effect type head device

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