JPH0567314A - Manufacture of magneto-resistance effect type head - Google Patents
Manufacture of magneto-resistance effect type headInfo
- Publication number
- JPH0567314A JPH0567314A JP22781891A JP22781891A JPH0567314A JP H0567314 A JPH0567314 A JP H0567314A JP 22781891 A JP22781891 A JP 22781891A JP 22781891 A JP22781891 A JP 22781891A JP H0567314 A JPH0567314 A JP H0567314A
- Authority
- JP
- Japan
- Prior art keywords
- film
- magnetoresistive
- magnetic field
- head
- 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
Links
Landscapes
- Magnetic Heads (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は磁気ディスク装置、ある
いは磁気テープ装置に用いられる磁気ヘッドの再生素子
に関し、特に、再生感度が高く、かつ、再生波形歪のな
い磁気抵抗効果型ヘッドに関す。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a reproducing element of a magnetic head used in a magnetic disk device or a magnetic tape device, and more particularly to a magnetoresistive head having high reproducing sensitivity and no reproduced waveform distortion.
【0002】[0002]
【従来の技術】磁気抵抗効果素子上に反強磁性膜として
FeMnを形成し、バルクハウゼン雑音に起因した再生
波形歪を抑えるといった公知例は、例えば、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 TRANSACTIONS ONMAGNETICS)VOL.25,No.
5,1989 に記載されている。ここではウエハ段階
での素子特性を調べているに留まり、ヘッド化して記録
再生特性を調べた上での問題点は抽出されていない。実
際に磁気抵抗効果素子をヘッド化したり、また、記録再
生分離型ヘッドの再生素子として使うには、ウエハプロ
セス,機械加工プロセス上での問題点がある。例えば、
記録ヘッドを再生ヘッド上に形成した記録再生分離型ヘ
ッドのウエハプロセス中には、記録ヘッドのコイルを埋
め込むためのレジスト絶縁層を硬化させる高温プロセス
がある。このプロセスでは、ウエハを200℃程度の高
温にまで加熱する必要がある。交換結合膜として、例え
ば、FeMn膜を用いた場合、この膜のキュリー点は1
60℃前後にある。このため、レジスト絶縁層を硬化さ
せる高温プロセス中(200℃程度)に浮遊磁界の影響
を受けて分散してしまう磁気抵抗効果素子の磁化方向に
対応してFeMn膜の磁化方向が分散するなどの問題が
ある。このように磁気抵抗効果素子の磁化方向が分散し
た状態で素子を交換結合膜のキュリー点以上にまで昇温
すると、交換結合膜の磁化方向がばらついて磁気抵抗効
果素子の磁区構造を乱し、再生動作時にバルクハウゼン
雑音に起因した再生波形歪が発生するといった問題が生
じる。2. Description of the Related Art A known example in which FeMn is formed as an antiferromagnetic film on a magnetoresistive effect element to suppress a reproduced waveform distortion caused by Barkhausen noise is described in, for example, I.E.
EE Transactions ON MAGNETICS VOL.25, No.
5, 1989. Here, only the device characteristics are examined at the wafer stage, and no problems have been extracted after examining the recording / reproducing characteristics by forming a head. There are problems in the wafer process and the machining process when the magnetoresistive effect element is actually used as a head or used as a reproducing element of a recording / reproducing separated type head. For example,
In the wafer process of the recording / reproducing separated type head in which the recording head is formed on the reproducing head, there is a high temperature process of hardening the resist insulating layer for embedding the coil of the recording head. In this process, it is necessary to heat the wafer to a high temperature of about 200 ° C. When a FeMn film is used as the exchange coupling film, the Curie point of this film is 1
It is around 60 ° C. For this reason, the magnetization direction of the FeMn film is dispersed corresponding to the magnetization direction of the magnetoresistive effect element which is dispersed under the influence of the stray magnetic field during the high temperature process of curing the resist insulating layer (about 200 ° C.). There's a problem. When the element is heated to a temperature above the Curie point of the exchange coupling film in a state where the magnetization direction of the magnetoresistive effect element is dispersed, the magnetization direction of the exchange coupling film varies and disturbs the magnetic domain structure of the magnetoresistive effect element. There arises a problem that a reproduced waveform distortion occurs due to Barkhausen noise during a reproducing operation.
【0003】[0003]
【発明が解決しようとする課題】本発明は、ウエハプロ
セス、あるいは機械加工プロセス中にばらついてしまう
磁気抵抗効果素子および交換結合膜の磁化方向を、磁気
抵抗効果素子が形成された際の磁化容易方向により完全
に揃えることを目的とする。SUMMARY OF THE INVENTION According to the present invention, the magnetization directions of the magnetoresistive effect element and the exchange coupling film, which are varied during the wafer process or the machining process, are easily magnetized when the magnetoresistive effect element is formed. The aim is to align perfectly in the direction.
【0004】[0004]
【課題を解決するための手段】上記目的はウエハプロセ
ス、あるいは機械加工プロセス終了後にヘッド素子を磁
気抵抗効果素子の磁化容易方向と同一方向の外部磁界を
印加した雰囲気中で交換結合膜のキュリー点以上に加熱
し、その後、磁界を印加した状態で室温まで徐々に冷却
することで達成される。The above object is to achieve a Curie point of the exchange coupling film in an atmosphere in which an external magnetic field is applied to the head element in the same direction as the easy magnetization direction of the magnetoresistive effect element after the wafer process or the machining process is completed. This is achieved by heating above and then gradually cooling to room temperature with a magnetic field applied.
【0005】[0005]
【作用】図1(a)に示すように磁気抵抗効果素子は、も
ともとの磁化容易方向を向いた外部磁界を印加すること
で素子内の磁化方向を完全に揃えて単磁区化することが
できる。しかし、これとは180度反対方向に外部磁界
を印加すると、図1(b)に示したように、素子内の磁化
方向が細かい単位で分散してしまうといった問題が生じ
る。また、もともとの磁化容易方向に対して0度、ある
いは180度からずれた方向に外部磁界を印加すると、
図1(c)のように素子内がいくつもの磁区に分かれてし
まう。図1(b),(c)に示したように、素子内の磁化方
向が分散していると再生動作時の波形歪の原因となるバ
ルクハウゼン雑音を発生させるといった問題がある。雑
音を発生させずに安定な再生特性を確保するには、ま
ず、図1(a)のように、素子内の磁化方向を揃える必要
がある。さらに再生特性を安定させるには、磁気抵抗効
果素子内の磁化変化を起こしにくくする方法が有効であ
り、このため交換結合膜が用いられる。交換結合膜はキ
ュリー点以上に加熱されると、図2(a)に示すように、
磁化方向が外部磁界の印加方向を向くようになる。ここ
で図2(b)に示すように温度を徐々に室温まで下げてい
くと、交換結合膜内の磁化方向は膜厚方向に対して交互
の方向を向き、磁気抵抗効果素子との境界では磁気抵抗
効果素子と反対方向を向いて磁気抵抗効果素子内の磁化
を固着する働きがある。ただしこの場合、初期の磁気抵
抗効果素子内の磁化状態が乱れていては、バルクハウゼ
ン雑音を低減するといった効果はなくなる。よって、安
定した再生特性を得るためにはウエハプロセス、あるい
は機械加工プロセス終了後にヘッド素子を磁気抵抗効果
素子の磁化容易方向と同一方向の外部磁界を印加した雰
囲気中で交換結合膜のキュリー点以上に加熱し、その後
は磁界を印加した状態で室温まで徐々に冷却する必要が
ある。As shown in FIG. 1 (a), the magnetoresistive effect element can be made into a single magnetic domain by completely aligning the magnetization direction in the element by applying an external magnetic field originally oriented in the easy magnetization direction. .. However, when an external magnetic field is applied in a direction opposite to this by 180 degrees, there arises a problem that the magnetization directions in the element are dispersed in fine units, as shown in FIG. Also, when an external magnetic field is applied in a direction deviating from the original easy magnetization direction by 0 degree or 180 degrees,
As shown in FIG. 1C, the inside of the element is divided into many magnetic domains. As shown in FIGS. 1B and 1C, when the magnetization directions in the element are dispersed, there is a problem in that Barkhausen noise that causes waveform distortion during a reproducing operation is generated. In order to secure stable reproduction characteristics without generating noise, it is first necessary to align the magnetization directions in the element as shown in FIG. Further, in order to stabilize the reproducing characteristic, it is effective to make the magnetization change in the magnetoresistive effect element less likely to occur, and therefore, the exchange coupling film is used. When the exchange-coupling film is heated above the Curie point, as shown in FIG.
The magnetization direction comes to face the direction of applying the external magnetic field. Here, when the temperature is gradually lowered to room temperature as shown in FIG. 2B, the magnetization directions in the exchange coupling film alternate with the film thickness direction, and at the boundary with the magnetoresistive effect element. It functions to fix the magnetization in the magnetoresistive effect element in the direction opposite to that of the magnetoresistive effect element. However, in this case, if the initial magnetization state in the magnetoresistive element is disturbed, the effect of reducing Barkhausen noise is lost. Therefore, in order to obtain stable reproduction characteristics, after the wafer process or the machining process, the head element is heated to the Curie point of the exchange coupling film or higher in an atmosphere in which an external magnetic field in the same direction as the easy magnetization direction of the magnetoresistive element is applied. After that, it is necessary to gradually cool to room temperature while applying a magnetic field.
【0006】[0006]
【実施例】以下、本発明の実施例を図面を用いて説明す
る。まず、図3は本発明で作製した両側シールドタイプ
のシャントバイアス型磁気抵抗効果ヘッドの感磁部付近
を、媒体対向面から見た図である。シールド膜10には
平坦性に優れた膜厚1μmのCo系非晶質合金膜を用い
ている。極薄絶縁層11はアルミナ膜である。磁気抵抗
効果素子12はパーマロイであり、膜厚は15nm以下
である。パーマロイ上には交換結合膜としてキュリー点
が160℃前後にある膜厚40nmのFeMn13、およ
び膜厚30nmのNbシャント膜14が形成されてい
る。この実施例ではFeMn膜が磁気抵抗効果素子上全
面に形成されているが、全面に形成する必要は必ずしも
ない。なお磁気抵抗効果型ヘッドのトラック幅は一対の
Cuリード線15の間隔で規定されており、この間隔は
1μmである。また一対のシールド層の間隔は0.25
μm 以下である。このヘッドをチップ加工終了後に磁
場中で熱処理することにより、再生特性の変化を調べた
結果について次に述べる。Embodiments of the present invention will be described below with reference to the drawings. First, FIG. 3 is a view of the vicinity of the magnetic sensitive portion of the double-sided shield type shunt bias type magnetoresistive head manufactured according to the present invention, as viewed from the medium facing surface. As the shield film 10, a Co type amorphous alloy film having a thickness of 1 μm and excellent in flatness is used. The ultrathin insulating layer 11 is an alumina film. The magnetoresistive effect element 12 is permalloy and has a film thickness of 15 nm or less. On the permalloy, an FeMn 13 having a film thickness of 40 nm and a Nb shunt film 14 having a film thickness of 30 nm having Curie points around 160 ° C. are formed as exchange coupling films. In this embodiment, the FeMn film is formed on the entire surface of the magnetoresistive effect element, but it is not always necessary to form it on the entire surface. The track width of the magnetoresistive head is defined by the distance between the pair of Cu lead wires 15, and this distance is 1 μm. The distance between the pair of shield layers is 0.25.
μm or less. The results of investigating the change in the reproducing characteristic by heat-treating this head in a magnetic field after the chip processing is described below.
【0007】図4は熱処理時の温度変化をモニタした結
果である。昇温は10℃/分程度の速さで行ない、素子
温度が200℃に達したらここで30分間保持する。そ
の後は約4℃/分のペースで徐々に冷却を行なった。な
お、この熱処理は窒素雰囲気中で行なっている。ここで
熱処理時の外部磁界の印加方向と測定される再生波形と
の関係を図5に示す。この測定はスパッタ媒体を用い記
録密度を1KFCIに設定して行なった。なお、ヘッド
媒体間のスペーシング0.05μmである。外部からの
印加磁界は大きさが1KOeの直流磁界である。図5の
結果から外部磁界の印加方向を磁気抵抗効果素子の磁化
容易方向と揃えることで、再生歪のない安定した再生特
性を得られることがわかる。次に、外部から印加する直
流磁界の大きさによって再生波形歪がどのように変化す
るのかを測定した結果を図6に示す。この測定はセンス
電流を上下パルスの振幅値が対称となる最適値からゼロ
に戻すという操作を百回繰り返して行なった場合、再生
波形に歪の現れる回数をパーセンテージで表したもので
ある。測定は六個のヘッドを用いて行なったが、この結
果から外部磁界強度を1KOeにすれば再生波形歪率は
5%以下におさえることができ実用上問題とならないこ
とがわかった。FIG. 4 shows the result of monitoring the temperature change during the heat treatment. The temperature is raised at a rate of about 10 ° C./minute, and when the element temperature reaches 200 ° C., it is held here for 30 minutes. After that, the material was gradually cooled at a rate of about 4 ° C / minute. Note that this heat treatment is performed in a nitrogen atmosphere. FIG. 5 shows the relationship between the applied direction of the external magnetic field during the heat treatment and the measured reproduced waveform. This measurement was performed using a sputter medium and setting the recording density to 1 KFCI. The spacing between the head media is 0.05 μm. The magnetic field applied from the outside is a DC magnetic field having a magnitude of 1 KOe. From the results shown in FIG. 5, it can be seen that stable reproduction characteristics without reproduction distortion can be obtained by aligning the direction of application of the external magnetic field with the easy magnetization direction of the magnetoresistive effect element. Next, FIG. 6 shows the result of measurement of how the reproduced waveform distortion changes depending on the magnitude of the DC magnetic field applied from the outside. In this measurement, when the operation of returning the sense current from the optimum value in which the amplitude values of the upper and lower pulses are symmetrical to zero to 100 times is repeated, the number of times the reproduced waveform is distorted is expressed as a percentage. The measurement was performed using six heads. From these results, it was found that the reproduced waveform distortion factor could be suppressed to 5% or less by setting the external magnetic field strength to 1 KOe, which is not a practical problem.
【0008】[0008]
【発明の効果】本発明により、再生波形歪のない磁気抵
抗効果型ヘッドを実現することが可能になる。According to the present invention, it is possible to realize a magnetoresistive head having no reproduced waveform distortion.
【図1】磁気抵抗効果素子内の磁化状態の説明図。FIG. 1 is an explanatory diagram of a magnetized state in a magnetoresistive effect element.
【図2】交換結合膜内の磁化状態の説明図。FIG. 2 is an explanatory diagram of a magnetization state in an exchange coupling film.
【図3】本発明による磁気ヘッドの感磁部を摺動面側か
ら見た断面図。FIG. 3 is a cross-sectional view of the magnetic sensing part of the magnetic head according to the present invention as viewed from the sliding surface side.
【図4】本発明の実施例による熱処理を行なう際の素子
温度の時間変化の説明図。FIG. 4 is an explanatory diagram of a change in element temperature over time when performing heat treatment according to an example of the present invention.
【図5】本発明の効果の説明図。FIG. 5 is an explanatory diagram of effects of the present invention.
【図6】本発明による磁場中熱処理を行なう際の印加磁
界強度と再生波形歪との関係を示す特性図。FIG. 6 is a characteristic diagram showing a relationship between applied magnetic field strength and reproduced waveform distortion when performing heat treatment in a magnetic field according to the present invention.
10…シールド膜、11…絶縁層、12…磁気抵抗効果
素子、13…交換結合膜、14…シャント膜、15…リ
ード線。10 ... Shield film, 11 ... Insulating layer, 12 ... Magnetoresistive effect element, 13 ... Exchange coupling film, 14 ... Shunt film, 15 ... Lead wire.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 由比藤 勇 東京都国分寺市東恋ケ窪1丁目280番地 株式会社日立製作所中央研究所内 (72)発明者 小山 直樹 東京都国分寺市東恋ケ窪1丁目280番地 株式会社日立製作所中央研究所内 (72)発明者 北田 正弘 東京都国分寺市東恋ケ窪1丁目280番地 株式会社日立製作所中央研究所内 (72)発明者 中谷 亮一 東京都国分寺市東恋ケ窪1丁目280番地 株式会社日立製作所中央研究所内 ─────────────────────────────────────────────────── ─── Continuation of front page (72) Inventor Yuu Yuto 1-280 Higashi Koikeku, Kokubunji, Tokyo Inside Central Research Laboratory, Hitachi, Ltd. (72) Inventor Naoki Koyama 1-280 Higashi Koikeku, Kokubunji, Tokyo Hitachi Ltd. (72) Inventor Masahiro Kitada 1-280, Higashi Koikekubo, Kokubunji, Tokyo Hitachi, Ltd. Central Research Center (72) Inventor Ryoichi Nakatani, 1-280, Higashi Koikeku, Tokyo Kokubunji City
Claims (8)
気抵抗効果素子との間で磁気的な交換結合を引き起こす
反強磁性膜が形成されている磁気抵抗効果型ヘッドにお
いて、前記反強磁性膜が形成された後、前記磁気抵抗効
果素子の磁化容易方向と同一方向の外部磁界を印加した
状態で前記反強磁性膜のキュリー点以上の温度まで一度
昇温した後、室温まで徐々に冷却することを特徴とする
磁気抵抗効果型ヘッドの製造方法。1. A magnetoresistive head in which an antiferromagnetic film that causes magnetic exchange coupling with the magnetoresistive element is formed on at least a part of the magnetoresistive element. After the film is formed, it is once heated to a temperature equal to or higher than the Curie point of the antiferromagnetic film in the state where an external magnetic field in the same direction as the easy magnetization direction of the magnetoresistive element is applied, and then gradually cooled to room temperature. A method of manufacturing a magnetoresistive effect head, comprising:
の磁化容易方向は、前記磁気抵抗効果素子を蒸着法、あ
るいはスパッタ法により形成する際に加える外部磁界の
印加方向により決定される磁気抵抗効果型ヘッドの製造
方法。2. The magnetic resistance according to claim 1, wherein the easy magnetization direction of the magnetoresistive effect element is determined by an application direction of an external magnetic field applied when the magnetoresistive effect element is formed by a vapor deposition method or a sputtering method. Method of manufacturing effective head.
効果素子を形成する際に印加される磁界方向と同一方向
の外部磁界が、前記磁気抵抗効果素子との間で交換結合
を引き起こす反強磁性膜を形成する際にも印加される磁
気抵抗効果型ヘッドの製造方法。3. The anti-strong magnetic field according to claim 1, wherein an external magnetic field in the same direction as a magnetic field applied when forming the magnetoresistive effect element causes exchange coupling with the magnetoresistive effect element. A method of manufacturing a magnetoresistive head that is also applied when forming a magnetic film.
との間で交換結合を引き起こす反強磁性膜はFeとMn
を主成分とする合金膜である磁気抵抗効果型ヘッドの製
造方法。4. The antiferromagnetic film which causes exchange coupling with the magnetoresistive effect element according to claim 1, wherein Fe and Mn are used.
A method of manufacturing a magnetoresistive head which is an alloy film containing as a main component.
ウエハプロセス終了後に行う磁気抵抗効果型ヘッドの製
造方法。5. The method of manufacturing a magnetoresistive head according to claim 1, wherein the heat treatment in a magnetic field is performed after the completion of all wafer processes.
摺動面を研磨した後に行う磁気抵抗効果型ヘッドの製造
方法。6. The heat treatment in a magnetic field according to claim 1,
A method of manufacturing a magnetoresistive head after polishing a sliding surface.
の磁化容易方向に印加する磁界が1KOe以上である磁
気抵抗効果型ヘッドの製造方法。7. The method for manufacturing a magnetoresistive head according to claim 1, wherein the magnetic field applied in the easy magnetization direction of the magnetoresistive element is 1 KOe or more.
化容易方向はトラック幅方向である磁気抵抗効果型ヘッ
ドの製造方法。8. A method of manufacturing a magnetoresistive head according to claim 1, wherein the easy magnetization direction of the magnetoresistive effect element is the track width direction.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22781891A JPH0567314A (en) | 1991-09-09 | 1991-09-09 | Manufacture of magneto-resistance effect type head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22781891A JPH0567314A (en) | 1991-09-09 | 1991-09-09 | Manufacture of magneto-resistance effect type head |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0567314A true JPH0567314A (en) | 1993-03-19 |
Family
ID=16866859
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP22781891A Pending JPH0567314A (en) | 1991-09-09 | 1991-09-09 | Manufacture of magneto-resistance effect type head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0567314A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH076330A (en) * | 1993-06-14 | 1995-01-10 | Tdk Corp | Production of magneto-resistance effect head |
-
1991
- 1991-09-09 JP JP22781891A patent/JPH0567314A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH076330A (en) * | 1993-06-14 | 1995-01-10 | Tdk Corp | Production of magneto-resistance effect head |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP3022023B2 (en) | Magnetic recording / reproducing device | |
| US6449131B2 (en) | Canted longitudinal patterned exchange biased dual-stripe magnetoresistive (DSMR) sensor element and method for fabrication thereof | |
| US20020164828A1 (en) | Tunneling magnetoresistance transducer and method for manufacturing the same | |
| JP3172000B2 (en) | Magnetic recording / reproducing device | |
| US5978186A (en) | Magnetic head and reproducing apparatus with head having central core with winding thereabout and wire therethrough | |
| JPH07169037A (en) | In-surface type magnetic recording medium and its manufacture and magnetic recorder employing the medium | |
| JP2924825B2 (en) | Magnetoresistive element and magnetoresistive sensor using the same | |
| JP2849354B2 (en) | Magnetic transducer and thin-film magnetic head | |
| JP3378549B2 (en) | Magnetic head | |
| JPH0567314A (en) | Manufacture of magneto-resistance effect type head | |
| KR19990013803A (en) | Magnetic head | |
| US5687044A (en) | Magnetoresistive head with micro-crystallite shielding layer | |
| JPS63129512A (en) | Production of magnetoresistance effect type magnetic head | |
| Cain et al. | Dual exchange biased NiFe-TbCo unshielded MR heads for high density recording | |
| JPS5987616A (en) | Magnetic thin film head | |
| JPH0845035A (en) | Thin film magnetic head | |
| JP3082003B2 (en) | Method of manufacturing magnetoresistive head | |
| JP3083090B2 (en) | Magnetoresistive sensor | |
| JPH10334422A (en) | Magnetic recording device | |
| JP2000231706A (en) | Magnetic recording and reproducing head and magnetic storage device using the same as well as its production | |
| JPS6391811A (en) | Production of magnetic head | |
| JPH06282802A (en) | Magnetic recorder-reproducer | |
| JPH10222817A (en) | Magnetoresistive sensor | |
| JP2003006818A (en) | Magnetoresistive read head using two anti-parallel ferromagnetic films | |
| JPH05182146A (en) | Thin film magnetic head |