JPH011113A - Manufacturing method of thin film magnetic head - Google Patents

Manufacturing method of thin film magnetic head

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Publication number
JPH011113A
JPH011113A JP62-155816A JP15581687A JPH011113A JP H011113 A JPH011113 A JP H011113A JP 15581687 A JP15581687 A JP 15581687A JP H011113 A JPH011113 A JP H011113A
Authority
JP
Japan
Prior art keywords
thin film
insulating layer
head
ferromagnetic thin
manufacturing
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
JP62-155816A
Other languages
Japanese (ja)
Other versions
JPS641113A (en
Inventor
光司 大塚
量二 南方
一義 今江
吉良 徹
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.)
Sharp Corp
Original Assignee
Sharp Corp
Filing date
Publication date
Application filed by Sharp Corp filed Critical Sharp Corp
Priority to JP62-155816A priority Critical patent/JPH011113A/en
Publication of JPS641113A publication Critical patent/JPS641113A/en
Publication of JPH011113A publication Critical patent/JPH011113A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〈産業上の利用分野〉 本発明は、−軸磁気異方性を有する磁性薄膜に信号磁界
を印加し、それを磁化容易軸方向の電気抵抗変化として
検出する磁気抵抗効果素子(以下、MR素子という)を
具備して磁気記録媒体に記録された信号の検出を行なう
薄膜磁気ヘッド(以下、薄膜MRヘッドという)に関す
る。
[Detailed Description of the Invention] <Industrial Application Field> The present invention relates to a magnetoresistive system that applies a signal magnetic field to a magnetic thin film having -axis magnetic anisotropy and detects it as a change in electrical resistance in the direction of the easy axis of magnetization. The present invention relates to a thin film magnetic head (hereinafter referred to as a thin film MR head) that includes an effect element (hereinafter referred to as an MR element) and detects a signal recorded on a magnetic recording medium.

〈従来の技術〉 従来、薄膜MRヘッドは巻線型の磁気ヘッドと比較して
、多くの利点があることが知られている。
<Prior Art> It has been known that thin film MR heads have many advantages over wire-wound magnetic heads.

この薄膜MRヘッドは磁気テープ等の磁気記録媒体に書
キ込まれた信号磁界を受けることにより、MR素子内部
の磁化方向が変化し、この磁化方向の変化に応じたMR
素子の内部抵抗の変化を外部出力として取り出すもので
ある。従ってM14M Rヘッドは磁束応答型のヘッド
であり、磁気記録媒体の移送速度に依存せずに信号磁界
を再生できる。
This thin film MR head changes the magnetization direction inside the MR element by receiving a signal magnetic field written on a magnetic recording medium such as a magnetic tape, and the MR head responds to the change in the magnetization direction.
The change in internal resistance of the element is extracted as an external output. Therefore, the M14M R head is a magnetic flux responsive head and can reproduce a signal magnetic field without depending on the transport speed of the magnetic recording medium.

又、この薄膜MRヘッドは半導体の微細加工技術を適用
することにより高集積化及び多素子化が容易であるので
、制密度記録が行なわれる固定ヘッド弐PCM録音機の
再生用磁気ヘッドとして有望視されている。
In addition, this thin-film MR head can be easily fabricated with high integration and multi-element technology by applying semiconductor microfabrication technology, so it is seen as a promising magnetic head for playback in fixed-head PCM recorders that perform density-controlled recording. has been done.

このようなMR素子は外部磁界に対して2乗変化を示す
感応特性をもつことから、MR素子を再生ヘッドとして
構成する場合、所定のバイアス磁界が必要となる。この
バイアス磁界を印加する方法には導体に直流電流を流す
ことにより、バイアス磁界を誘起する方法及びCo−P
層等の高抗磁力薄膜を用いてバイアス磁界を印加する方
法等が知られている。
Since such an MR element has a sensitivity characteristic that exhibits a square change with respect to an external magnetic field, a predetermined bias magnetic field is required when the MR element is configured as a read head. Methods of applying this bias magnetic field include a method of inducing a bias magnetic field by flowing a direct current through a conductor, and a method of inducing a bias magnetic field by flowing a direct current through a conductor, and a method of inducing a bias magnetic field by flowing a direct current through a conductor.
A method is known in which a bias magnetic field is applied using a high coercive force thin film such as a magnetic layer.

一方、MR素子単体で構成した薄膜MRヘッドよりもM
R素子をヘッド先端から離して磁気記録媒体に発生した
磁束をMRヘッドまで導く磁束導入路(ヨーク)を配置
したヨーク型MRヘッド(以下、YMRヘッドという)
と呼ばれる薄膜磁気ヘッドの方が信号の分離能の向上や
MR素子の耐久性の向上に有利であることが知られてい
る。
On the other hand, the M
A yoke-type MR head (hereinafter referred to as a YMR head) in which the R element is separated from the head tip and a magnetic flux introducing path (yoke) is arranged to guide the magnetic flux generated in the magnetic recording medium to the MR head.
It is known that a thin-film magnetic head called .

従来のYMRヘッドになるMR素子部の製造方法を第3
図及び第4図に示す。但し、第4図は第3図のA−B断
面の構造を示す。
The third method for manufacturing the MR element part of the conventional YMR head
It is shown in FIG. However, FIG. 4 shows the structure taken along the line A-B in FIG. 3.

基板1上にMR素子となる強磁性薄膜5(N1−Fe合
金膜)が蒸着法等により形成され、同図(alに示すよ
うに目的の形状に加工される。
A ferromagnetic thin film 5 (N1-Fe alloy film), which will become an MR element, is formed on a substrate 1 by a vapor deposition method or the like, and is processed into a desired shape as shown in FIG.

MR素子のトラック幅は多トラツク構成となるため通常
50〜200μm程度に設定される。
Since the MR element has a multi-track configuration, the track width of the MR element is usually set to about 50 to 200 .mu.m.

M R素子のトラック幅が小さくなると、磁区状態が不
可逆的に変化して、△R/R特性にバルクハウゼン・ノ
イズが発生しやすくなる。そこで、上記強磁性薄膜5の
両端部に同図(blに示す如く高抗磁力薄膜7Co−P
層を備えて、容易軸方向に弱い磁界を印加して磁壁な消
失させバルクハウゼン・ノイズのないMR素子を得る必
要がある。尚、上記、高保磁力薄膜7は無電解メツキに
より作成される。
When the track width of the MR element becomes smaller, the magnetic domain state changes irreversibly, making Barkhausen noise more likely to occur in the ΔR/R characteristics. Therefore, as shown in the same figure (bl), a high coercive force thin film 7Co-P is attached to both ends of the ferromagnetic thin film 5.
It is necessary to provide an MR element without Barkhausen noise by applying a weak magnetic field in the easy axis direction to eliminate the domain walls. Note that the high coercive force thin film 7 mentioned above is created by electroless plating.

また上記強磁性薄膜5が形成された後リード部となる導
電層8がAlやA6−Cu等を蒸着或いはRFスパッタ
することにより形成され、ケミカルエツチングして同図
(C1に示すようにヘッド等の所望形状に加工される。
Further, after the ferromagnetic thin film 5 is formed, a conductive layer 8 which will become a lead part is formed by vapor deposition or RF sputtering of Al, A6-Cu, etc., and is chemically etched to form a head etc. as shown in the same figure (C1). It is processed into the desired shape.

〈発明が解決しようとする問題点〉 上記YMRヘッドの製造工程において、高保磁力薄膜7
を作成するための無電解メツキ膜は、メツキされる面積
が小さくなるほどメツキの前処理条件及びメツキ条件が
厳しくなる。従っそ、MR素子のトラック幅が小さくな
るほど被着面積部分が小さくなり、無電解メツキにより
作成される高抗磁力薄膜の再現性が悪かった。
<Problems to be Solved by the Invention> In the manufacturing process of the above YMR head, the high coercive force thin film 7
The pre-treatment conditions and plating conditions for electroless plating for creating an electroless plating film become stricter as the area to be plated becomes smaller. Therefore, as the track width of the MR element becomes smaller, the deposited area becomes smaller, and the reproducibility of the high coercive force thin film produced by electroless plating is poor.

即ち、メツキ前処理条件を厳しくすると、MR素子とな
る強磁性薄膜の膜厚が200〜500λと非常に薄いた
め前処理液で腐食される。また、メツキがされやすい条
件にすると、高抗磁力薄膜の特性が劣化する問題があっ
た。
That is, if the plating pretreatment conditions are made stricter, the ferromagnetic thin film forming the MR element is very thin, 200 to 500λ, and will be corroded by the pretreatment liquid. Furthermore, if the conditions are such that plating is likely to occur, there is a problem in that the characteristics of the high coercive force thin film deteriorate.

また強磁性薄膜5Cリード部8を接続する工程に於いて
も、MR素子となる強磁性薄膜の表面はリードのエツチ
ング液及びレジスト剥離液にさらされる。従って、上記
強磁性薄膜は200〜500Aと非常に薄いため、強磁
性薄膜の表面が酸化等されると、薄膜MR素子の特性が
劣化する問題もあった。
Further, in the step of connecting the lead portion 8 of the ferromagnetic thin film 5C, the surface of the ferromagnetic thin film that will become the MR element is exposed to the lead etching solution and the resist stripping solution. Therefore, since the ferromagnetic thin film is very thin at 200 to 500 A, there is a problem in that the characteristics of the thin film MR element deteriorate if the surface of the ferromagnetic thin film is oxidized or the like.

本発明は薄膜磁気ヘッドに使用されるMR素子に係わる
高抗磁力薄膜の無電解メツキの再現性を向上し、かつ強
磁性薄膜の表面を酸化から防止して、薄膜MR素子の特
性改善を目的とする。
The purpose of the present invention is to improve the reproducibility of electroless plating of high coercive force thin films related to MR elements used in thin film magnetic heads, and to prevent the surface of ferromagnetic thin films from oxidation, thereby improving the characteristics of thin film MR elements. shall be.

〈問題点を解決するための手段〉 MR素子の下地絶縁層SiO1MR素子となる強磁性薄
膜、MR素子の上部絶縁層SiOを順次積層し、上記強
磁性薄膜と上部絶縁層SiOの二層を同時加工後、リー
ド部の強磁性薄膜上を被う上部絶縁層SiOをエツチン
グし、高抗磁力薄膜、導電層を順次積層したことを特徴
とする。
<Means for solving the problem> A ferromagnetic thin film serving as the MR element and an upper insulating layer SiO of the MR element are sequentially laminated, and the two layers of the above ferromagnetic thin film and the upper insulating layer SiO are simultaneously formed. After processing, the upper insulating layer SiO covering the ferromagnetic thin film of the lead portion is etched, and a high coercive force thin film and a conductive layer are sequentially laminated.

〈実施例〉 第1図は、本発明に係る実施例のYMRヘッドの平面構
成を示す。第2図(alは第1図のA−B断面の構造を
示し、第2図(blは第1図のC−Dlr面の構造を示
す。
<Example> FIG. 1 shows a planar configuration of a YMR head according to an example of the present invention. FIG. 2 (al shows the structure of the cross section A-B in FIG. 1, and FIG. 2 bl shows the structure of the C-Dlr plane of FIG. 1.

下部ヨークを形成する基板11はN i −Z nフェ
ライト又はM n −Z nフェライトから成る。この
基板ll上に5i02.Si3N4等から成る第1絶縁
層2がRFスパッタ法又はP−CVD法等により形成さ
れる。次にこの第1絶縁層2上にM o +Cu、A#
或いはA 11− Cu合金膜等からなる導体層3がR
Fスパッタ法、蒸着法等により形成される。この導体層
3をバイアス層の形状に加工するために、ケミカルエツ
チング法、スパッタエツチング法等が用いられる。具体
例を上げて説明すると、ケミカルエツチング法の場合C
u膜は硝酸(H’N03)十過硫酸アンモニウム((N
H3)2S208)生水(H2O)、A6及びAe−C
u膜は水酸化カリウム(KOH)十過硫酸アンモニウム
((N)13)2S20ρ+水(HO)又はリン酸(H
3P04)十硝酸(HNO3)+酢酸(CHC00H)
生水(H2O)なるエラチンダ液を用いれば良い。スパ
ッタエツチング法の場合1M o 、 A l 、 C
u等の膜はArガスを導入すれば公知の手法により加工
することができる。
The substrate 11 forming the lower yoke is made of N i -Zn ferrite or M n -Zn ferrite. 5i02. on this board ll. A first insulating layer 2 made of Si3N4 or the like is formed by RF sputtering, P-CVD, or the like. Next, on this first insulating layer 2, M o +Cu, A#
Alternatively, the conductor layer 3 made of A11-Cu alloy film or the like is R
It is formed by F sputtering method, vapor deposition method, etc. In order to process this conductor layer 3 into the shape of a bias layer, a chemical etching method, a sputter etching method, etc. are used. To explain with a specific example, in the case of chemical etching method, C
The u film is made of nitric acid (H'N03) ammonium decaprosulfate ((N
H3)2S208) Raw water (H2O), A6 and Ae-C
The u membrane consists of potassium hydroxide (KOH) ammonium tenpersulfate ((N)13)2S20ρ + water (HO) or phosphoric acid (H
3P04) Deca-nitric acid (HNO3) + acetic acid (CHC00H)
Elachinda liquid, which is raw water (H2O), may be used. In the case of sputter etching method 1M o , A l , C
Films such as u can be processed by a known method by introducing Ar gas.

上述のよう―形成された導体層3上に蒸着法等によりS
iOからなる第2絶縁層4が形成される。
S is deposited on the conductor layer 3 formed as described above by vapor deposition or the like.
A second insulating layer 4 made of iO is formed.

該SiO膜4は表面平滑性、膜質に優れているので、次
に積層するMR素子となる強磁性薄膜1’Ji−Fe合
金膜5は良好な磁気特性をもつ。Ni−Fe合金膜5上
にSiOからなる第3絶縁層5i06が形成される。
Since the SiO film 4 has excellent surface smoothness and film quality, the ferromagnetic thin film 1'Ji-Fe alloy film 5, which will become the MR element to be laminated next, has good magnetic properties. A third insulating layer 5i06 made of SiO is formed on the Ni-Fe alloy film 5.

ここで、パーアロイ蒸着膜5の下地層及び上側保護層と
して、Si0層4,6を用いた場合のパーアロイ(Ni
−Fe合金膜)膜の特性について以下述べる。
Here, peralloy (Ni
-Fe alloy film) The characteristics of the film will be described below.

ガラス基板上に厚さ約40OAのSi0層を蒸着法で形
成した後、厚さ約320λのNi−Fe合金膜を磁場中
で蒸着法で形成し、該N i −F e合金膜上に厚さ
約40OAのSiOを形成した試料を磁場中で200℃
2時間真空中アニールし声時の磁気特性の変化を第1表
に示す。尚比較のため、N i −F e合金膜の上下
C3iO3を形成した場合も示す。磁歪定数λ5はNi
−Fe合金膜の組成に著しく敏感なので、Ni−Fe合
金膜と下地との拡散による組成変化を検出するのに適し
ている。
After forming a Si0 layer with a thickness of about 40 OA on a glass substrate by vapor deposition, a Ni-Fe alloy film with a thickness of about 320λ is formed by vapor deposition in a magnetic field, and a thick Si0 layer is formed on the Ni-Fe alloy film. A sample with approximately 40 OA of SiO formed was heated at 200°C in a magnetic field.
Table 1 shows the changes in magnetic properties during 2-hour vacuum annealing. For comparison, a case where C3iO3 is formed on the upper and lower sides of the Ni--Fe alloy film is also shown. The magnetostriction constant λ5 is Ni
Since it is extremely sensitive to the composition of the -Fe alloy film, it is suitable for detecting compositional changes due to diffusion between the Ni-Fe alloy film and the underlying layer.

第1表 第1表かられかるように、N i −F e合金膜の上
下にSi0層を形成した場合はλ5の変化が小さく、拡
散を防止している。
As can be seen from Table 1, when Si0 layers are formed above and below the Ni-Fe alloy film, the change in λ5 is small and diffusion is prevented.

上記条件により形成された、強磁性薄膜5と第3絶縁層
Si、06の二層について、第1図に示すMR素子部a
及びMR素子のリード部b 、cC該当する形状にスパ
ッタエツチング法、又はイオン・ミーリング法により加
工する。導入ガスとして、Arガスを用いれば良い。
Regarding the two layers of the ferromagnetic thin film 5 and the third insulating layer Si, 06 formed under the above conditions, the MR element part a shown in FIG.
And the lead portions b and c of the MR element are processed into appropriate shapes by sputter etching or ion milling. Ar gas may be used as the introduced gas.

次に、MR素子aを被う第3絶縁層6を残し外リードb
、cに該当する部分を被う絶縁層5i06をRIE(リ
アクティブ・イオン・エツチング)法によりエツチング
する。導入ガスとしてCF4(フレオン14)、CF4
+H2、CF4+H2を用いれば良い。上記RIE法に
よりSiOをエツチングしたリードb、c部分の強磁性
薄膜上にCo−P7層を無電解メツキ法により作成する
Next, leaving the third insulating layer 6 covering the MR element a, the outer lead b
, c is etched by an RIE (reactive ion etching) method. CF4 (Freon 14), CF4 as introduced gas
+H2 and CF4+H2 may be used. A Co--P7 layer is formed by electroless plating on the ferromagnetic thin film of the leads b and c in which SiO has been etched by the above RIE method.

無電解メツキ法によりメツキされたC o −P 7層
の面私はリードb、cのほぼ全域にわたるため従来と比
較して約300〜1000倍と大きくでき、再現性良く
作成することができる。
Since the surface of the Co-P 7 layer plated by the electroless plating method covers almost the entire area of leads b and c, it can be made about 300 to 1000 times larger than the conventional one, and can be produced with good reproducibility.

次にMR素子のリード部す、c分に導電層Al又はA 
11− Cu %if等8を蒸着法又はRFスパッタ法
により作成し、ケミカルエッチ法又はドライエツチング
法により成形する。
Next, a conductive layer of Al or A is applied to the lead portions of the MR element.
11- Cu %if etc. 8 is prepared by vapor deposition or RF sputtering, and molded by chemical etching or dry etching.

上記工程を経てMR素子を作成する場合MR素子aの本
体部分は第3絶縁層SiOに被覆されているため、エツ
チング液及びレジスト剥離液にさらされることがないの
で、強磁性薄膜5の表面が酸化されることがなく、磁気
特性の劣化がない。
When creating an MR element through the above steps, the main body of the MR element a is covered with the third insulating layer SiO, so it is not exposed to the etching solution and the resist stripping solution, so that the surface of the ferromagnetic thin film 5 is No oxidation and no deterioration of magnetic properties.

また、MR素子a部分とリードb、cの接触面積が大キ
いので、コンタクト抵抗も無視できる。
Further, since the contact area between the MR element a part and the leads b and c is large, contact resistance can also be ignored.

次にフロントギツプ部dを被う上記第1.第2゜第3絶
縁層をエツチング後、第2図+a+の如< G aP部
となる絶縁層9を新たにRFスパッタ法、P−CVD法
により形成する。従来のYMRヘッドの製造工程と同様
に上部ヨーク部10と下部ヨーク部11の接続する部分
の絶縁層をRIE法によりエツチング後、上部ヨーク↓
0となるN i −F e合金膜を作成してYMRヘッ
ドが完成する。
Next, the first part that covers the front cast part d. After etching the second and third insulating layers, a new insulating layer 9, which will become the GaP section, is formed by RF sputtering and P-CVD as shown in FIG. 2+a+. Similar to the manufacturing process of conventional YMR heads, after etching the insulating layer at the connecting portion of the upper yoke part 10 and lower yoke part 11 using the RIE method, the upper yoke ↓
A YMR head is completed by creating a N i -Fe alloy film that has a value of 0.

尚上記の実施例ではY M Rヘッドについて説明した
が、本発明はノンシールド型MRヘッド、両面シールド
型MRヘッド等の他のMRヘッドに応用しても、同様の
効果を有することは明らかである。
In the above embodiments, the YMR head was explained, but it is clear that the present invention can have similar effects even when applied to other MR heads such as non-shielded MR heads and double-sided shielded MR heads. be.

〈発明の効果〉 以上詳述したように、本発明を用いれば、MR素子部を
構成する良好な磁気特性をもつ高抗磁力薄膜が再現良く
形成でき、かつ、強磁性薄膜の表面酸化を生じることな
く加工することができるので、良好な特性をもつMRヘ
ッドが得られる。
<Effects of the Invention> As detailed above, by using the present invention, a high coercive force thin film with good magnetic properties constituting the MR element portion can be formed with good reproducibility, and the surface oxidation of the ferromagnetic thin film can be prevented. Since the process can be carried out without any problems, an MR head with good characteristics can be obtained.

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

第1図は本発明に係る一実施例の平面図、第2図(al
は第1図のA−B断面図、第2図(blは第1図のC−
D断面図、第3図は従来の薄膜MRヘッドの平面図、第
4図は同ヘッドの断面図である。 2.9・・・絶縁層、3.8・・・導体層、4,6・・
SiO絶縁膜、5・・・強磁性薄膜、7・・・高抗磁力
薄膜、10・・・上部ヨーク、11・・・下部ヨーク。 代理人 弁理士 杉 山 毅 至(他1名)ユ l [
・: //下鮮3−り ′ス 2 5コ tσ) 1/T印3−り 蕊 2 灘 (b) 第3図 第4 図
FIG. 1 is a plan view of one embodiment of the present invention, and FIG. 2 (al.
is a sectional view taken along line A-B in Figure 1, and Figure 2 is a cross-sectional view taken along line C-B in Figure 1.
3 is a plan view of a conventional thin film MR head, and FIG. 4 is a sectional view of the same head. 2.9... Insulating layer, 3.8... Conductor layer, 4,6...
SiO insulating film, 5... ferromagnetic thin film, 7... high coercive force thin film, 10... upper yoke, 11... lower yoke. Agent: Patent Attorney Takeshi Sugiyama (and 1 other person)
・: // Lower surface 3-ri's 2 5 pieces tσ) 1/T mark 3-ri's 2 Nada (b) Fig. 3 Fig. 4

Claims (1)

【特許請求の範囲】[Claims] 1、印加される信号磁界の変化を一軸磁気異方性を有す
る強磁性薄膜の電気抵抗変化として検出する磁気抵抗効
果型の薄膜磁気ヘッドの製造方法に於いて、絶縁層Si
O、強磁性薄膜、絶縁層SiOを順次積層し、上記、強
磁性薄膜、絶縁層SiOの2層を同時加工後に、該強磁
性薄膜上の絶縁層SiOをエッチングし、高抗磁力薄膜
、導電層を順次積層したことを特徴とする薄膜磁気ヘッ
ドの製造方法。
1. In a method for manufacturing a magnetoresistive thin film magnetic head that detects changes in an applied signal magnetic field as changes in electrical resistance of a ferromagnetic thin film having uniaxial magnetic anisotropy, an insulating layer of Si
O, a ferromagnetic thin film, and an insulating layer SiO are sequentially laminated, and after simultaneous processing of the above two layers, the ferromagnetic thin film and the insulating layer SiO, the insulating layer SiO on the ferromagnetic thin film is etched to form a high coercive force thin film and a conductive layer. A method for manufacturing a thin film magnetic head characterized by sequentially laminating layers.
JP62-155816A 1987-06-22 Manufacturing method of thin film magnetic head Pending JPH011113A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62-155816A JPH011113A (en) 1987-06-22 Manufacturing method of thin film magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62-155816A JPH011113A (en) 1987-06-22 Manufacturing method of thin film magnetic head

Publications (2)

Publication Number Publication Date
JPS641113A JPS641113A (en) 1989-01-05
JPH011113A true JPH011113A (en) 1989-01-05

Family

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