JPH0782622B2 - Magnetoresistive magnetic head - Google Patents

Magnetoresistive magnetic head

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Publication number
JPH0782622B2
JPH0782622B2 JP32513892A JP32513892A JPH0782622B2 JP H0782622 B2 JPH0782622 B2 JP H0782622B2 JP 32513892 A JP32513892 A JP 32513892A JP 32513892 A JP32513892 A JP 32513892A JP H0782622 B2 JPH0782622 B2 JP H0782622B2
Authority
JP
Japan
Prior art keywords
film
shield
permalloy
magnetic
head
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 - Lifetime
Application number
JP32513892A
Other languages
Japanese (ja)
Other versions
JPH06195643A (en
Inventor
延行 石綿
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 JP32513892A priority Critical patent/JPH0782622B2/en
Publication of JPH06195643A publication Critical patent/JPH06195643A/en
Publication of JPH0782622B2 publication Critical patent/JPH0782622B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は磁気ディスク装置、磁気
テープ装置などに用いられる磁気抵抗(以下MRと称す
る)効果型磁気ヘッドに関し、特に、NR素子が絶縁体
層を介して磁気シールド層で挟み込まれた構造のシール
ド型磁気抵抗効果型磁気ヘッドに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetoresistive (hereinafter referred to as MR) effect type magnetic head used in a magnetic disk device, a magnetic tape device, etc., and particularly, an NR element is a magnetic shield layer via an insulating layer. The present invention relates to a shield type magnetoresistive effect magnetic head having a sandwiched structure.

【0002】[0002]

【従来の技術】図2にMR素子が絶縁体層を介して磁気
シールド層で挟み込まれた従来のッッシールド型磁気抵
抗効果型磁気ヘッドの概略図を示す。基板上に成膜され
たアルミナ膜上に下シールド膜を成膜したパタン化す
る。その上にSiO2 あるいはアルミナなどの絶縁膜を
形成し、その上にMR素子を成膜する。さらに金あるい
はタングステンやタンタルなどで電極を形成し、絶縁膜
を成膜した上に上シールド膜を形成しパタン化する。シ
ールド材料としては従来、パーマロイ膜が用いられてき
た。例えば、ジャーナルオブアプライドフィジックス6
7巻4847頁に記載されている。(J.Appl.P
hys.67(9),pp4847,1990)あるい
は特開昭61−248211号公報参照。
2. Description of the Related Art FIG. 2 is a schematic view of a conventional shielded magnetoresistive head having an MR element sandwiched between magnetic shield layers with an insulating layer interposed therebetween. The lower shield film is formed on the alumina film formed on the substrate to form a pattern. An insulating film such as SiO 2 or alumina is formed thereon, and an MR element is formed thereon. Further, an electrode is formed from gold, tungsten, tantalum, or the like, an insulating film is formed, and then an upper shield film is formed to form a pattern. Conventionally, a permalloy film has been used as a shield material. For example, Journal of Applied Physics 6
7: 4847. (J. Appl. P
hys. 67 (9), pp4847, 1990) or JP-A-61-248211.

【0003】しかしながら、パーマロイ膜は硬度がビッ
カース硬度で200程度と低いため、媒体対抗面の研磨
の際に、基板との偏摩耗が発生する、パーマロイ膜がい
わゆる膜だれを起こしMR素子膜を圧迫したり変形させ
たりする、などの問題を発生させていた。これにより、
再生効率の低下、製造歩留りの低下が生じていた。
However, since the hardness of the permalloy film is as low as about 200 in Vickers hardness, uneven wear between the permalloy film and the substrate occurs during polishing of the medium-opposing surface. The permalloy film causes so-called film droop and presses the MR element film. It caused problems such as doing and deforming. This allows
Regeneration efficiency was lowered and production yield was lowered.

【0004】また、パーマロイ膜は飽和磁束密度が最大
10KGであり、効果的な磁気シールドを行うためには
1μm程度の膜厚が必要であった。そのため、下シール
ドによる段差が大きくなり、下シールド上の絶縁膜を十
分に厚くしないと下シールド膜とMR素子膜との絶縁が
取れなかった。更に、下シールドによる段差によりMR
素子膜や電極膜の導通不良が生じやすかった。この問題
を解決するために、図3のように、下シールドト同じ高
さに絶縁層をあらかじめ形成し絶縁層を埋め込んだ後に
更に絶縁層を形成する、といった方法も考えられた。し
かしながら、この方法は製造プロセスを複雑にしてい
た。製造プロセスの複雑化は製造歩留りの低下を招いて
いた。
Further, the permalloy film has a maximum saturation magnetic flux density of 10 KG, and a film thickness of about 1 μm was required for effective magnetic shielding. Therefore, the step due to the lower shield becomes large, and the insulation between the lower shield film and the MR element film cannot be obtained unless the insulating film on the lower shield is sufficiently thick. Furthermore, due to the step difference due to the lower shield, MR
The conduction failure of the element film and the electrode film was likely to occur. In order to solve this problem, as shown in FIG. 3, a method of forming an insulating layer in advance at the same height as the lower shield, burying the insulating layer, and then forming the insulating layer was also considered. However, this method complicates the manufacturing process. The complicated manufacturing process has led to a reduction in manufacturing yield.

【0005】[0005]

【発明が解決しようとする課題】本発明は、シールド膜
による偏摩耗やMR素子膜への物理的ダメージ、およ
び、シールド膜、特に、図2における下シールド膜の段
差による。下シールド膜とMR素子膜との絶縁不良、M
R素子膜や電極膜の導通不良といった問題を、加工プロ
セスを複雑にすることなく解決し、シールド型磁気抵抗
効果型ヘッドの効率を安定させ製造歩留りを向上させる
ことを目的としている。
SUMMARY OF THE INVENTION The present invention is based on uneven wear due to the shield film, physical damage to the MR element film, and a step of the shield film, particularly the lower shield film in FIG. Poor insulation between lower shield film and MR element film, M
The object of the present invention is to solve the problem of poor conduction of the R element film and the electrode film without complicating the processing process, to stabilize the efficiency of the shield type magnetoresistive head and to improve the manufacturing yield.

【0006】[0006]

【課題を解決するための手段】電極が接触しているMR
素子を絶縁体層を介して磁気シールド層で挟み込んだ構
造の磁気抵抗効果型磁気ヘッドにおいて、磁気シールド
層をFeMN(MはTa,Zr,Nb,Hf,Tiの中
から選択される少なくとも一種類の元素、Nは窒素)を
主成分とした軟磁性体で構成することを特徴とする。F
eMNはFexy z の組成で表した場合、x,y,
zを原子%とすると72≦x≦82、8≦y≦13、1
0≦z≦15、x+y+z=100を満たすことが最適
である。さらにこの軟磁性体は体心方向格子の結晶粒の
集合体であり、かつ、結晶粒の平均粒径は10nm以下
であり、かつ、結晶粒のおのおのの結晶軸方向に一定の
規則の無いことが望ましい。
[MEANS FOR SOLVING THE PROBLEMS] MR in which electrodes are in contact
In a magnetoresistive effect magnetic head having a structure in which an element is sandwiched by magnetic shield layers with an insulating layer interposed between them, the magnetic shield layers are FeMN (M is at least one selected from Ta, Zr, Nb, Hf, and Ti). Element, and N is nitrogen) as a main component. F
If eMN is expressed with the composition of Fe x M y N z, x , y,
When z is atomic%, 72 ≦ x ≦ 82, 8 ≦ y ≦ 13, 1
It is optimal to satisfy 0 ≦ z ≦ 15 and x + y + z = 100. Furthermore, this soft magnetic material is an aggregate of crystal grains in a body-centered lattice, the average grain size of the crystal grains is 10 nm or less, and there is no fixed rule in the crystal axis direction of each crystal grain. Is desirable.

【0007】FeMNについては、特願平4−9467
5号(平成4年4月15日出願)及び1992年電子情
報通信学会春季大会講演論文集のC433(p5−5
3)参照。
Regarding FeMN, Japanese Patent Application No. 4-9467
No. 5 (filed on April 15, 1992) and C433 (p5-5) of the 1992 IEICE Spring Conference
See 3).

【0008】[0008]

【作用】FeMN膜は発明者の検討によれば、飽和磁束
密度が15KG以上と高く、また、透磁率が1MHzで
3000以上と高く、保磁力が0.10e以下と小さ
い。すなわち磁気シールド材料としては好適な磁気特性
を持っている。さらに、ビッカース硬度が1000程度
と高く、極めて高硬度である。
According to the inventors' study, the FeMN film has a high saturation magnetic flux density of 15 KG or more, a high magnetic permeability of 3000 or more at 1 MHz, and a coercive force of 0.10 e or less. That is, it has suitable magnetic properties as a magnetic shield material. Furthermore, the Vickers hardness is as high as about 1000, which is extremely high hardness.

【0009】これらの性質から、FeMN膜をシールド
型MRヘッドのシールド材として用いることにより、パ
ーマロイ膜で発生していた媒体対向面研磨による偏摩耗
やMR素子膜への物理的ダメージが抑制される。更に、
飽和磁束密度がパーマロイ膜に比べて1.5倍以上と高
いことから、シールド膜厚を1.5分の1に減少させる
ことができる。このことから、図2における下シールド
膜の段さによる、下シールド膜とMR素子との絶縁不
良、MR素子膜や電極膜の導通不良といった問題を、加
工プロセスを複雑にすることなく解決し、シールド型磁
気抵抗効果型ヘッドの効率を安定させ製造歩留りを向上
させることができる。
From these properties, by using the FeMN film as the shield material of the shield type MR head, the uneven wear and the physical damage to the MR element film due to the medium facing surface polishing which are generated in the permalloy film are suppressed. . Furthermore,
Since the saturation magnetic flux density is 1.5 times or more higher than that of the permalloy film, the shield film thickness can be reduced to 1 / 1.5. From this, the problems such as the insulation failure between the lower shield film and the MR element and the conduction failure between the MR element film and the electrode film due to the step of the lower shield film in FIG. 2 are solved without complicating the processing process, It is possible to stabilize the efficiency of the shield type magnetoresistive head and improve the manufacturing yield.

【0010】[0010]

【実施例】図1に本発明によるシールド型MRヘッドを
示した。比較としてシールド材料にパーマロイ膜を用い
た図2のものを作成した。基板1とてアルチック(Al
23 −Tic)を用いた。ヘッド諸元として、トラッ
ク巾8μm、シールド巾36μm、MR素子膜5と上シ
ールド8間は0.3μm、MR素子膜5と下シールド3
間は0.2μm、MR素子膜においてMR膜(パーマロ
イ)厚40nm、シャントバイアス膜厚60nm、中間
膜厚20nm、素子幅5μmとした。シールド材料とし
て、パーマロイ膜を用いたとき(図2)には膜厚1μ
m、本発明による場合のFeMN膜として8.5at%
Ta−13at%N−残余Fe膜を用いたとき(図1)
には膜厚0.65μmとした。パーマロイ膜の飽和磁束
密度は9.5KG、FeTaN膜のそれは16KGであ
った。
EXAMPLE FIG. 1 shows a shield type MR head according to the present invention. For comparison, the one shown in FIG. 2 using a permalloy film as a shield material was prepared. Substrate 1 is AlTiC (Al
2 O 3 -Tic) was used. As head specifications, the track width is 8 μm, the shield width is 36 μm, the distance between the MR element film 5 and the upper shield 8 is 0.3 μm, and the MR element film 5 and the lower shield 3 are
The gap was 0.2 μm, the MR film (permalloy) thickness was 40 nm, the shunt bias film thickness was 60 nm, the intermediate film thickness was 20 nm, and the device width was 5 μm. When a permalloy film is used as the shield material (Fig. 2), the film thickness is 1μ.
m, 8.5 at% as a FeMN film in the case of the present invention
When using a Ta-13 at% N-residual Fe film (FIG. 1)
The film thickness was set to 0.65 μm. The saturation magnetic flux density of the permalloy film was 9.5 KG and that of the FeTaN film was 16 KG.

【0011】媒体対向面を研磨したところ、パーマロイ
膜シールドの場合アルミナ膜との段差が大きくパーマロ
イ膜の偏摩耗が顕著であった。更に、パーマロイ膜はい
わゆる膜だれを生じ、これによってMR素子膜が物理的
に圧迫された。これはパーマロイ膜の硬度がビッカース
硬度で200程度と低く、アルミナ膜の1000程度に
比べて著しく低いことによると思われた。FeTaN膜
シールドの場合アルミナ膜との段差はほとんど観測され
ず、MR素子膜への物理的ダメージもなかった。これは
FeTaN膜の硬度がアルミナ膜と同程度に高いことに
よると考えられた。FeTaN膜において今回シールド
膜として用いた組成以外の組成であっても、軟磁気特性
の良好な組成範囲での組成であればビッカース硬度は1
000程度と高いことから、同様な効果が得られる。ま
たMとしてTa以外の元素、すなわち、Zr,Nb,H
f,Tiの中から選択される少なくとも一種類の元素で
あるならば、飽和磁束密度は15KG以上と高いことか
ら、同様な効果が得られる。
When the medium facing surface was polished, the permalloy film shield had a large step with the alumina film, and the uneven wear of the permalloy film was remarkable. Furthermore, the permalloy film causes so-called film sagging, which physically presses the MR element film. It is considered that this is because the hardness of the permalloy film is as low as about 200 in Vickers hardness, which is significantly lower than the hardness of about 1000 for the alumina film. In the case of the FeTaN film shield, almost no step difference with the alumina film was observed, and there was no physical damage to the MR element film. It is considered that this is because the hardness of the FeTaN film is as high as that of the alumina film. Even if the composition of the FeTaN film is different from the composition used as the shield film this time, the composition has a Vickers hardness of 1 as long as the composition is in a composition range having good soft magnetic characteristics.
Since it is as high as about 000, the same effect can be obtained. Further, as M, an element other than Ta, that is, Zr, Nb, H
If at least one kind of element selected from f and Ti is used, the saturation magnetic flux density is as high as 15 KG or more, and the same effect can be obtained.

【0012】シールド材としてFeTaN膜を用いた場
合、図1のようにシールド膜厚が薄くなることから、下
シールドによる段差がパーマロイ膜を用いた図2に比べ
て小さくなる。このことから、下シールド膜の段差によ
る、下シールド膜とMR素子膜との絶縁不良、MR素子
膜や電極膜の導通不良による故障が減少し、ヘッド効率
を安定させ製造歩留りを向上させることができた。Fe
TaN膜において今回シールド膜として用いた組成以外
の組成であっても、軟磁気特性の良好な組成範囲での組
成であれば飽和磁束密度は15KG以上と高いことか
ら、同様な効果が得られる。またMとしてTa以外の元
素、すなわち、Zr,Nb,Hf,Tiの中から選択さ
れる少なくとも一種類の元素であるならば、飽和磁束密
度は15KG以上と高いことから、同様な効果が得られ
る。
When the FeTaN film is used as the shield material, the shield film thickness becomes thin as shown in FIG. 1, so that the step due to the lower shield becomes smaller than that in FIG. 2 which uses the permalloy film. From this, it is possible to reduce failures due to the insulation failure between the lower shield film and the MR element film due to the step of the lower shield film and the failure in conduction between the MR element film and the electrode film, and to stabilize the head efficiency and improve the manufacturing yield. did it. Fe
Even if the composition of the TaN film is other than the composition used as the shield film this time, the same effect can be obtained because the saturation magnetic flux density is as high as 15 KG or more as long as the composition is in a composition range with good soft magnetic characteristics. If M is an element other than Ta, that is, at least one kind of element selected from Zr, Nb, Hf, and Ti, the saturation magnetic flux density is as high as 15 KG or more, and the same effect can be obtained. .

【0013】[0013]

【発明の効果】本発明により、MRヘッドのシールド材
としてパーマロイ膜を用いていた際に発生していた媒体
対向面研磨によるシールド膜の偏摩耗やMR素子膜への
物理的ダメージが抑制された。更に、FeMN膜は飽和
磁束密度がパーマロイ膜に比べて1.5倍以上と高いこ
とから、シールド膜厚を1.5分の1程度に減少させる
ことができ、下シールド膜の段差による、下シールド膜
とMR素子膜との絶縁不良、MR素子膜や電極膜の導通
不良といった問題を、加工プロセスを複雑にすることな
く解決することができた。以上により、シールド型磁気
抵抗効果型ヘッドの効率が安定し、製造歩留りが向上し
た。
According to the present invention, uneven wear of the shield film and physical damage to the MR element film due to polishing of the medium facing surface, which occurred when the permalloy film was used as the shield material of the MR head, were suppressed. . Furthermore, since the saturation magnetic flux density of the FeMN film is 1.5 times higher than that of the permalloy film, the shield film thickness can be reduced to about 1 / 1.5, and The problems such as poor insulation between the shield film and the MR element film and poor continuity of the MR element film and the electrode film could be solved without complicating the processing process. As described above, the efficiency of the shield type magnetoresistive head was stabilized and the manufacturing yield was improved.

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

【図1】本発明によるシールド型磁気抵抗型ヘッドの媒
体対向面を示す図である。
FIG. 1 is a diagram showing a medium facing surface of a shielded magnetoresistive head according to the present invention.

【図2】従来のシールド型磁気抵抗型ヘッドの媒体対向
面を示す図である。
FIG. 2 is a diagram showing a medium facing surface of a conventional shielded magnetoresistive head.

【図3】従来のシールド型磁気抵抗型ヘッドの媒体対向
面を示す図である。
FIG. 3 is a diagram showing a medium facing surface of a conventional shielded magnetoresistive head.

【符号の説明】[Explanation of symbols]

1 基板 2 アルミナ層 3 下シールド 4 絶縁層 5 MR素子膜 6 電極 7 絶縁層 8 上シールド 1 Substrate 2 Alumina Layer 3 Lower Shield 4 Insulating Layer 5 MR Element Film 6 Electrode 7 Insulating Layer 8 Upper Shield

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 電極が接触している磁気抵抗素子を絶縁
体層を介して磁気シールド層で挟み込んだ構造の磁気抵
抗効果型磁気ヘッドであって、前記磁気シールド層がF
eMN(MはTa,Zr,Nb,Hf,Tiの中から選
択される少なくとも一種類の元素、Nは窒素)を主成分
とした軟磁性体であることを特徴とする磁気抵抗効果型
磁気ヘッド。
1. A magnetoresistive effect magnetic head having a structure in which a magnetoresistive element in contact with an electrode is sandwiched by magnetic shield layers with an insulating layer interposed between the magnetic shield layers.
A magnetoresistive effect magnetic head comprising a soft magnetic material containing eMN (M is at least one element selected from Ta, Zr, Nb, Hf, and Ti, N is nitrogen) as a main component. .
JP32513892A 1992-12-04 1992-12-04 Magnetoresistive magnetic head Expired - Lifetime JPH0782622B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32513892A JPH0782622B2 (en) 1992-12-04 1992-12-04 Magnetoresistive magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32513892A JPH0782622B2 (en) 1992-12-04 1992-12-04 Magnetoresistive magnetic head

Publications (2)

Publication Number Publication Date
JPH06195643A JPH06195643A (en) 1994-07-15
JPH0782622B2 true JPH0782622B2 (en) 1995-09-06

Family

ID=18173487

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32513892A Expired - Lifetime JPH0782622B2 (en) 1992-12-04 1992-12-04 Magnetoresistive magnetic head

Country Status (1)

Country Link
JP (1) JPH0782622B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002133614A (en) 2000-10-30 2002-05-10 Tdk Corp Thin film magnetic head and its manufacturing method
US6989971B2 (en) 2002-04-05 2006-01-24 Hitachi Global Storage Technologies Netherlands, B.V. Giant magnetoresistance (GMR) read head with reactive-ion-etch defined read width and fabrication process

Also Published As

Publication number Publication date
JPH06195643A (en) 1994-07-15

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