JPH10222816A - Thin-film magnetic head and magnetic disk drive - Google Patents
Thin-film magnetic head and magnetic disk driveInfo
- Publication number
- JPH10222816A JPH10222816A JP2345897A JP2345897A JPH10222816A JP H10222816 A JPH10222816 A JP H10222816A JP 2345897 A JP2345897 A JP 2345897A JP 2345897 A JP2345897 A JP 2345897A JP H10222816 A JPH10222816 A JP H10222816A
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- Prior art keywords
- film
- head
- insulating film
- amorphous
- silicon
- Prior art date
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Abstract
(57)【要約】
【課題】ディスクとヘッドが接触した際発生するTAを
低減し、また、MRヘッドの再生出力を向上させる。
【解決手段】含水素非晶質炭素、気層合成ダイヤモン
ド、含珪素非晶質炭素、非晶質AlN、非晶質BeO等
の熱拡散率の高い材料を、ヘッド素子の各非磁性絶縁膜
やディスク保護膜に適用する。
(57) An object of the present invention is to reduce TA generated when a disk and a head come into contact with each other and to improve the reproduction output of the MR head. SOLUTION: A material having a high thermal diffusivity, such as hydrogen-containing amorphous carbon, vapor-phase synthetic diamond, silicon-containing amorphous carbon, amorphous AlN, or amorphous BeO, is used for each non-magnetic insulating film of the head element. Applies to disc protection film.
Description
【0001】[0001]
【発明の属する技術分野】本発明は薄膜磁気ヘッド及び
その製造方法とに関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a thin film magnetic head and a manufacturing method thereof.
【0002】[0002]
【従来の技術】図3はディスクとの対向面にレールを有
する一般的な磁気ヘッドスライダの外観図である。薄膜
磁気ヘッドの薄膜磁気変換素子10の拡大図が図1及び
図2であり、図1は図3のa−a’部の断面図、また、
図2は同じ部分をディスク対向面側から見た図である。
これらの図で、ヘッド素子は読み取りにMRヘッドを、
書き込みに誘導型ヘッドを有する一般的な複合ヘッドが
示されている。図で14は薄膜磁気変換素子を支持する
スライダであり、アルミナチタンカーバイド、ジルコニ
ア等が用いられる。102は下地の絶縁膜である。11
はMRヘッドであり、下部シールド膜103、MR素子
105、上部シールド膜(誘導型ヘッドにおける下部磁
性膜)107、MR素子に電流を流す電極101、及び
各層間にある絶縁膜104、106で構成される。12
は誘導型ヘッドであり、下部磁性膜(MRヘッドにおけ
る上部シールド膜)107、コイル膜111、ギャップ
絶縁膜108、有機樹脂で構成された絶縁膜112で構
成される。更に、薄膜磁気変換素子全体は、保護絶縁膜
110によりおおわれている。下地絶縁膜102、MR
ヘッドの各層間絶縁膜104、106や誘導型ヘッドの
ギャップ絶縁膜108、保護絶縁膜110には通常酸化
珪素やアルミナが使われている。図4は磁気ディスク装
置動作時の、ヘッドスライダ1とディスク2の位置関係
を示した模式図である。通常、磁気ディスク2は、ニッ
ケル燐膜を表面に形成したアルミニウム・マグネシウム
合金円板15、コバルト合金膜等からなる磁性膜16、
非晶質炭素膜等からなるディスク表面の保護膜17、そ
してパーフルオロエーテル系潤滑膜18によって構成さ
れる。近年では、ヘッドスライダの磁気ディスク表面か
らの浮上隙間3は0.1μm以下になり、ヘッドスライ
ダとディスクが動作時に衝突する頻度が増えてきた。こ
の衝突によるヘッドクラッシュを防ぎ、また、腐食しや
すいMR素子、シールド膜等の磁性膜を保護する目的
で、最近では、ヘッドスライダのディスク対向面に含水
素非晶質炭素等からなる保護膜13が形成されている。2. Description of the Related Art FIG. 3 is an external view of a general magnetic head slider having a rail on a surface facing a disk. 1 and 2 are enlarged views of the thin-film magnetic transducer 10 of the thin-film magnetic head. FIG. 1 is a cross-sectional view taken along the line aa 'in FIG.
FIG. 2 is a view of the same portion as viewed from the disk facing surface side.
In these figures, the head element is an MR head for reading,
A typical composite head with an inductive head for writing is shown. In the figure, reference numeral 14 denotes a slider for supporting the thin-film magnetic transducer, which is made of alumina titanium carbide, zirconia or the like. Reference numeral 102 denotes a base insulating film. 11
Is an MR head, which is composed of a lower shield film 103, an MR element 105, an upper shield film (lower magnetic film in an inductive head) 107, an electrode 101 for passing a current through the MR element, and insulating films 104 and 106 between the layers. To be done. 12
Is an induction type head, which is composed of a lower magnetic film (upper shield film in an MR head) 107, a coil film 111, a gap insulating film 108, and an insulating film 112 made of an organic resin. Further, the entire thin-film magnetic transducer is covered with a protective insulating film 110. Base insulating film 102, MR
Normally, silicon oxide or alumina is used for the interlayer insulating films 104 and 106 of the head, the gap insulating film 108 and the protective insulating film 110 of the induction type head. FIG. 4 is a schematic diagram showing the positional relationship between the head slider 1 and the disk 2 during operation of the magnetic disk device. Normally, the magnetic disk 2 includes an aluminum / magnesium alloy disk 15 having a nickel-phosphorous film formed on its surface, a magnetic film 16 made of a cobalt alloy film or the like,
It is composed of a protective film 17 on the disk surface made of an amorphous carbon film or the like, and a perfluoroether lubricating film 18. In recent years, the flying gap 3 from the magnetic disk surface of the head slider has become 0.1 μm or less, and the frequency with which the head slider and the disk collide during operation has increased. For the purpose of preventing a head crash due to this collision and protecting a magnetic film such as an MR element and a shield film which are easily corroded, a protective film 13 made of hydrogen-containing amorphous carbon or the like has recently been formed on a disk facing surface of a head slider. Are formed.
【0003】[0003]
【発明が解決しようとする課題】MRヘッドとは、記録
媒体からの磁界で生じるMR素子の電気抵抗変化を検知
することで読み取りを行う磁気ヘッドであり、高記録密
度化に必須の技術である。一方、高記録密度化に伴いヘ
ッドスライダの浮上量が低くなってきたために、磁気デ
ィスクとヘッドが接触する頻度が高くなってきている。
ディスクとヘッドが接触すると、サーマルアスペリティ
(以下TAと略す)と呼ばれる現象が生じる。これは、
接触の際に発生した摩擦熱によりMR素子の温度が上昇
するために、抵抗が一瞬上昇し、読み取り信号が乱れる
という現象である。この問題を解決する方法は、信号処
理技術を用いて補償する方法(例えば、特開平6−28
785号公報)があるが、補償できるTA強度に限界が
あり、本質的な解決策とは言えない。一方、TAそのも
のを低減させる方法は、接触で生じた摩擦熱を逃がす工
夫が有効であると考えられる。具体的には、例えばMR
素子と接している非磁性絶縁膜に熱拡散率の大きな材料
を採用することである。しかし、これまでは、電気絶縁
性と熱伝導性を兼ね備え、且つプロセスの各工程に好適
な材料は報告されていなかった。また、MR素子には動
作時電流が流れているが、理論的には電流密度が大きい
ほど大きい感度が得られるはずである。しかし、MR素
子に流れる電流が大きくなると、エレクトロマイグレー
ションによりMR素子の温度が上昇するため、逆に読み
取りの感度が劣化し、また寿命も短くなるため、実際に
流せる電流値には上限(これを通電耐量という)があ
る。通電耐量を向上させ、MR素子の感度を向上させる
ためにも、TA対策同様何らかの方法でMR素子に蓄積
された熱を逃がす工夫が必要である。The MR head is a magnetic head that performs reading by detecting a change in electric resistance of an MR element caused by a magnetic field from a recording medium, and is an essential technology for increasing the recording density. . On the other hand, as the flying height of the head slider decreases with the increase in recording density, the frequency of contact between the magnetic disk and the head increases.
When the disk contacts the head, a phenomenon called thermal asperity (hereinafter abbreviated as TA) occurs. this is,
This is a phenomenon in which the temperature of the MR element rises due to the frictional heat generated at the time of contact, so that the resistance momentarily rises and the read signal is disturbed. To solve this problem, a method of compensating using a signal processing technique (for example, Japanese Unexamined Patent Publication No.
No. 785), but the TA strength that can be compensated is limited, and it cannot be said to be an essential solution. On the other hand, as a method of reducing TA itself, it is considered effective to devise to release frictional heat generated by contact. Specifically, for example, MR
A material having a large thermal diffusivity is used for the non-magnetic insulating film that is in contact with the element. However, a material that has both electrical insulation and thermal conductivity and is suitable for each step of the process has not been reported. Further, a current flows during operation in the MR element. In theory, a higher sensitivity should be obtained as the current density increases. However, when the current flowing through the MR element increases, the temperature of the MR element rises due to electromigration, and conversely, the reading sensitivity deteriorates and the life is shortened. (Referred to as current carrying capacity). In order to improve the withstand current and improve the sensitivity of the MR element, it is necessary to devise a method for releasing the heat accumulated in the MR element by some method like the TA countermeasure.
【0004】[0004]
【課題を解決するための手段】TAは、MR素子がディ
スクと接触した際に発生する瞬間的な温度上昇に起因す
るため、MR素子近傍が熱を拡散しやすい構造であれば
よいと考えられる。本発明者等は、TAを解決する手段
は、MR素子と隣接する非磁性絶縁膜の材料、形成方式
等に関し種々の検討を行った。その結果、熱拡散率が従
来のアルミナや酸化珪素の約5倍以上となるような材料
を用いると、TAに大幅な改善が見られることがわかっ
た。薄膜の熱拡散率はバルクのそれと違って絶対測定が
難しいが、光交流法(例えば、Japanese Journal of Ap
plied Physics.30(1991)1295)により相対的な測定が可
能である。種々の検討の結果、このような熱拡散率の高
い材料は、含水素非晶質炭素、気相合成ダイヤモンド、
含珪素非晶質炭素、非晶質AlN、非晶質BeO等がプ
ロセス上好適であることがわかった。このように、MR
素子と隣接する非磁性絶縁膜の材料の熱拡散率を大きく
することでTAが大幅減少する理由は、接触によって一
時的に生じた熱が、効率よく熱容量の大きいシールド膜
に拡散していくためだと考えられる。Means for Solving the Problems TA is caused by an instantaneous temperature rise that occurs when the MR element comes into contact with the disk, and therefore, it is considered that any structure that easily diffuses heat near the MR element is sufficient. . The present inventors have made various studies on the means for solving the TA with respect to the material, formation method, and the like of the nonmagnetic insulating film adjacent to the MR element. As a result, it was found that TA was significantly improved when a material having a thermal diffusivity of about 5 times or more that of conventional alumina or silicon oxide was used. It is difficult to measure the thermal diffusivity of thin films differently from that of bulk, but the optical alternating current method (for example, Japanese Journal of Ap
plied Physics. 30 (1991) 1295) allows relative measurements. As a result of various studies, such materials having a high thermal diffusivity include hydrogen-containing amorphous carbon, vapor-phase synthetic diamond,
It has been found that silicon-containing amorphous carbon, amorphous AlN, amorphous BeO, and the like are suitable for the process. Thus, MR
The reason that TA is greatly reduced by increasing the thermal diffusivity of the material of the non-magnetic insulating film adjacent to the element is that the heat temporarily generated by the contact efficiently diffuses to the shield film having a large heat capacity. It is thought that.
【0005】含水素非晶質炭素の形成方法には、スパッ
タリング法や化学蒸着法(ChemicalVapor Deposition:
以下CVDと略す)がある。スパッタリング法では、グ
ラファイトをターゲット材に用い、水素や炭化水素系ガ
スとアルゴンの混合ガス雰囲気下でマグネトロンスパッ
タリング、RFスパッタリング、DCスパッタリングの
いずれかの方法で含水素非晶質炭素を形成できる。一
方、化学蒸着法には、容量結合型プラズマや誘導結合型
プラズマ、電子サイクロトロン共鳴(Electron Cyclotr
on Resonance:以下ECRと略す)を用いたプラズマC
VD法や、イオンプレーティング等の成膜法がある。こ
の際、原料にはメタン、エタン、エチレン、ベンゼン、
トルエン等の炭化水素系原料が用いられる。どちらの手
法を用いても、成膜条件をコントロールすることで、電
気抵抗率や膜応力等を最適化できる。特に、膜中の水素
濃度は電気抵抗率、硬度、耐燃焼性に影響を及ぼす重要
なパラメータであり、10〜50atm%の範囲で選ば
れる。中でも好ましくは、20〜40atm%である。
これは、水素濃度が低すぎると絶縁性が低くなり、ま
た、逆に高すぎると膜硬度が低下するためである。ま
た、含水素非晶質炭素はシールド膜やMR膜との密着力
に欠けるため、これらの膜との界面に接着層としてS
i、炭化珪素等の膜をスパッタリング法等で形成する必
要がある。この接着層の膜厚は、なるべく薄い方がよい
が接着強度の点から1〜10nmの範囲で選ばれる。[0005] Methods of forming hydrogen-containing amorphous carbon include sputtering and chemical vapor deposition (Chemical Vapor Deposition:
Hereinafter abbreviated as CVD). In the sputtering method, hydrogen is used as a target material, and hydrogen-containing amorphous carbon can be formed by any of magnetron sputtering, RF sputtering, and DC sputtering in a mixed gas atmosphere of hydrogen or a hydrocarbon-based gas and argon. On the other hand, the chemical vapor deposition method includes capacitively coupled plasma, inductively coupled plasma, and electron cyclotron resonance (Electron Cyclotron Resonance).
on Resonance: Plasma C using ECR
There are a VD method and a film forming method such as ion plating. At this time, the raw materials are methane, ethane, ethylene, benzene,
A hydrocarbon-based material such as toluene is used. Regardless of which method is used, the electrical resistivity, film stress, etc. can be optimized by controlling the film forming conditions. In particular, the hydrogen concentration in the film is an important parameter that affects the electrical resistivity, hardness, and combustion resistance, and is selected within the range of 10 to 50 atm%. Above all, 20 to 40 atm% is preferable.
This is because if the hydrogen concentration is too low, the insulating property is lowered, and if it is too high, the film hardness is lowered. In addition, since hydrogen-containing amorphous carbon lacks adhesion to the shield film and the MR film, S is formed as an adhesive layer at the interface with these films.
It is necessary to form a film of i, silicon carbide or the like by a sputtering method or the like. The thickness of the adhesive layer is preferably as thin as possible, but is selected in the range of 1 to 10 nm from the viewpoint of adhesive strength.
【0006】気相合成ダイヤモンドの形成方法には、水
素で大量希釈した炭化水素系ガスを原料としたECR−
CVD法等がある。気相合成ダイヤモンドの場合も、シ
ールド膜やMR膜との界面に接着層はSi、炭化珪素等
の膜をスパッタリング法等で形成する必要があり、その
接着層の膜厚は、なるべく薄い方がよいが1〜10nm
の範囲で選ばれる。A method for forming a vapor-phase synthetic diamond is as follows.
There is a CVD method or the like. Also in the case of vapor-phase synthetic diamond, it is necessary to form a film of Si, silicon carbide, or the like at the interface with the shield film or the MR film by a sputtering method or the like, and the thickness of the adhesive layer is preferably as thin as possible. Good but 1-10nm
It is selected in the range of.
【0007】含珪素非晶質炭素、非晶質AlN、非晶質
BeOは、RFスパッタリング、RFマグネトロンスパ
ッタリング、電子ビーム蒸着等で形成される。含珪素非
晶質炭素は、珪素の含有量で熱拡散率、電気抵抗率をコ
ントロールできるが、これはターゲット中の珪素の比率
を変えることにより実現できる。形成された膜中の珪素
含有量は、10〜70atm%から選ばれ、中でも好ま
しくは20〜60atm%である。これは珪素が多すぎ
ると、絶縁性が低下し、また少なすぎると熱伝導性が悪
くなるからである。非晶質AlN、非晶質BeOに関し
ては、アルゴンガス雰囲気下で、あるいはそれぞれ窒
素、酸素を含むアルゴンガス雰囲気下でスパッタリン
グ、電子ビーム蒸着等を行うことで熱拡散率の高い膜を
形成できる。[0007] Silicon-containing amorphous carbon, amorphous AlN, and amorphous BeO are formed by RF sputtering, RF magnetron sputtering, electron beam evaporation, or the like. In the silicon-containing amorphous carbon, the thermal diffusivity and the electrical resistivity can be controlled by the content of silicon. This can be realized by changing the ratio of silicon in the target. The silicon content in the formed film is selected from 10 to 70 atm%, preferably 20 to 60 atm%. This is because if the amount of silicon is too large, the insulating property is reduced, and if the amount is too small, the thermal conductivity is deteriorated. Amorphous AlN and amorphous BeO can be formed into a film having a high thermal diffusivity by performing sputtering, electron beam evaporation, or the like in an argon gas atmosphere or an argon gas atmosphere containing nitrogen and oxygen, respectively.
【0008】また、本発明者等は、MR素子と隣接する
非磁性絶縁膜として上述の熱拡散率の高い材料を用いた
時、ディスク表面の保護膜はどのような材料を用いれば
好適であるか検討を行った。その結果、従来からディス
ク表面の保護膜として用いられている非晶質炭素より熱
拡散率に優れる、気相合成ダイヤモンド、含珪素非晶質
炭素、非晶質AlN、非晶質BeO等を用いることが有
効であることがわかった。従って、TAを低減するため
には、MR素子と隣接する非磁性絶縁膜は上述の熱拡散
率の高い材料を用いることが有効であるが、それに加え
て、ディスク表面の保護膜を従来の非晶質炭素より熱拡
散率に優れる気相合成ダイヤモンド、含珪素非晶質炭
素、非晶質AlN、非晶質BeO等の材料に変更するこ
とが非常に有効であることがわかった。Further, when the present inventors use the above-mentioned material having a high thermal diffusivity as the non-magnetic insulating film adjacent to the MR element, it is preferable to use any material for the protective film on the disk surface. Was examined. As a result, vapor-phase synthetic diamond, silicon-containing amorphous carbon, amorphous AlN, amorphous BeO, etc., which have a higher thermal diffusivity than the amorphous carbon conventionally used as the protective film on the disk surface, are used. Proved to be effective. Therefore, in order to reduce the TA, it is effective to use the above-mentioned material having a high thermal diffusivity as the non-magnetic insulating film adjacent to the MR element. It has been found that it is very effective to change to a material such as vapor-phase synthetic diamond, silicon-containing amorphous carbon, amorphous AlN, amorphous BeO, or the like, which has a higher thermal diffusivity than amorphous carbon.
【0009】一方、MR素子の通電耐量を向上させるた
めには、TAのような瞬間的な温度上昇と違って定常的
な温度上昇を抑える必要があると考えられる。そのため
には、極力熱伝導のいい材料を用いてヘッドを作ること
が重要である。本発明者等は、この問題に関して熱伝導
率がアルミナチタンカーバイドの約10倍である炭化珪
素をスライダ材に用い、且つスライダと下部シールド膜
の間の絶縁膜、下部シールド膜とMR素子間の絶縁膜、
MR素子と上部シールド膜間の絶縁膜、誘導型ヘッドの
ギャップ絶縁膜、ヘッド全体を保護する絶縁膜等のヘッ
ド素子を構成する全ての無機絶縁膜に含水素非晶質炭
素、気相合成ダイヤモンド、含珪素非晶質炭素、非晶質
AlN、非晶質BeO等の高熱伝導材料を用いることが
非常に有効であることを見出した。これらの無機絶縁膜
の形成手法は上述の方法と同じである。On the other hand, it is considered that it is necessary to suppress a steady temperature rise unlike an instantaneous temperature rise such as TA in order to improve the withstand current of the MR element. For that purpose, it is important to make the head using a material with good heat conduction as much as possible. With respect to this problem, the present inventors have used silicon carbide, whose thermal conductivity is about 10 times that of alumina titanium carbide, for the slider material, and the insulating film between the slider and the lower shield film and between the lower shield film and the MR element. Insulation film,
Hydrogen-containing amorphous carbon, vapor-phase synthetic diamond for all inorganic insulating films that compose the head element, such as the insulating film between the MR element and the upper shield film, the gap insulating film for the induction type head, and the insulating film for protecting the entire head It has been found that it is very effective to use a high thermal conductive material such as silicon-containing amorphous carbon, amorphous AlN, and amorphous BeO. The method for forming these inorganic insulating films is the same as the method described above.
【0010】[0010]
【発明の実施の形態】以下、図面を用いて本発明を更に
具体的に説明する。DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below more specifically with reference to the drawings.
【0011】本発明は、図1、図2に示したヘッド構造
で、MR素子105と隣接する非磁性絶縁膜104、1
06の材質を従来のアルミナ、酸化珪素から熱拡散率の
高い材料に変えることによって、ディスク2との接触に
よって生じるTAを大幅に低減するものである。実際に
このような非磁性絶縁膜を用いたところ、ヘッド1とデ
ィスク2の接触時に生じるTAの強度は従来の2分の1
から5分の1になり、複雑なプロセス変更を伴うことな
く比較的簡単な材料変更でTAを大幅に減少できること
がわかった。According to the present invention, in the head structure shown in FIG. 1 and FIG.
By changing the material No. 06 from the conventional alumina or silicon oxide to a material having a high thermal diffusivity, TA caused by contact with the disk 2 is greatly reduced. When such a non-magnetic insulating film is actually used, the strength of TA generated when the head 1 and the disk 2 come into contact with each other is half that of the conventional one.
It has been found that TA can be significantly reduced by a relatively simple material change without complicated process change.
【0012】また、スライダ材14に炭化珪素を用い、
且つスライダと下部シールド膜の間の絶縁膜102、下
部シールド膜とMR素子間の絶縁膜104、MR素子と
上部シールド膜間の絶縁膜106、誘導型ヘッドのギャ
ップ絶縁膜108、ヘッド全体を保護する絶縁膜110
を熱拡散率の高い膜に変えることにより、通電時にMR
素子のジュール加熱により発生する熱が効率よく拡散
し、再生出力が増大することが確認された。Further, when silicon carbide is used for the slider material 14,
In addition, the insulating film 102 between the slider and the lower shield film, the insulating film 104 between the lower shield film and the MR element, the insulating film 106 between the MR element and the upper shield film, the gap insulating film 108 of the inductive head, and the entire head are protected. Insulating film 110
By changing the film to a film with high thermal diffusivity,
It was confirmed that the heat generated by Joule heating of the element diffused efficiently and the reproduction output increased.
【0013】その詳細を以下の実施例で説明する。The details will be described in the following embodiments.
【0014】<実施例1>図1、図2を用いて本発明の
一実施例を説明する。<Embodiment 1> An embodiment of the present invention will be described with reference to FIGS.
【0015】スライダ14の材料はアルミナチタンカー
バイドを用いた。まず、スパッタリングによりアルミナ
からなる非磁性絶縁膜102を6μm形成し、引き続き
スパッタリング等による成膜とフォトリソグラフィ技術
を用いたパターニングにより、NiFe等からなる下部
シールド膜103を3μm所望の形状に形成した。その
上にスパッタリングにより非晶質シリコン(図示せず)
を5nm形成し、更に含水素非晶質炭素からなる非磁性
絶縁膜104を、メタンガスを原料とした容量結合型プ
ラズマCVD法を用いて180nm形成した。含水素非
晶質炭素の形成方法として基板側に高周波を印加するカ
ソードカップリング方式を用い、高周波電力120W、
メタンガス流量8sccm、ガス圧10Paという条件
で成膜を行った。この膜の水素濃度は、HFS(Hyd
rogen Forward Scattering)
分析により、約33%であった。更に非晶質シリコン
(図示せず)を5nm成膜した。引き続きNiFe等か
らなるMR素子105をスパッタリングにより形成し、
フォトリソグラフィ技術を用いて所望の形状にパターニ
ングを行った。更にハード磁性膜(図示せず)のパター
ンを形成した後、MR素子105にセンス電流を通電す
るために用いられる電極101のパターンを形成した。
その上にスパッタリングにより非晶質炭化珪素(図示せ
ず)を5nm形成し、含水素非晶質炭素からなる非磁性
絶縁膜106を200nm形成した。この非磁性絶縁膜
106は上記の非磁性絶縁膜104と同じ条件で形成し
た。更に、非晶質炭化珪素(図示せず)を5nm形成し
た後、NiFe等からなる上部シールド膜107をスパ
ッタリングにより形成しフォトリソグラフィ技術を用い
てパターニングを行った。更に、アルミナ等からなる非
磁性絶縁膜108をスパッタリングにより500nm形
成した。この絶縁膜は誘導型ヘッドのギャップ絶縁膜で
ある。続いてレジスト等からなる有機絶縁膜112、銅
等からなるコイル111、有機絶縁膜112を順次形成
する。次にNiFe等の磁性膜(図示せず)をスパッタ
リング等により200nm形成し、これをフォトリソグ
ラフィ技術を用いて所望の形状にパターニングした後、
その上にメッキにより3μmの上部磁性膜109を形成
した。最後にヘッド素子全体をおおう保護膜110とし
てアルミナ膜をスパッタリングにより形成する。この際
の膜厚は50μmであった。The material of the slider 14 is alumina titanium carbide. First, the non-magnetic insulating film 102 made of alumina was formed to a thickness of 6 μm by sputtering, and then the lower shield film 103 made of NiFe or the like was formed in a desired shape of 3 μm by film formation by sputtering and patterning using a photolithography technique. Amorphous silicon (not shown) by sputtering on it
Was formed to a thickness of 5 nm, and a nonmagnetic insulating film 104 made of hydrogen-containing amorphous carbon was formed to a thickness of 180 nm using a capacitively coupled plasma CVD method using methane gas as a raw material. As a method for forming hydrogen-containing amorphous carbon, a cathode coupling method in which a high frequency is applied to the substrate side is used, and a high frequency power of 120 W,
The film formation was performed under the conditions of a methane gas flow rate of 8 sccm and a gas pressure of 10 Pa. The hydrogen concentration of this film is HFS (Hyd
rogen Forward Scattering)
Analysis showed about 33%. Further, 5 nm of amorphous silicon (not shown) was formed. Subsequently, an MR element 105 made of NiFe or the like is formed by sputtering,
Patterning was performed into a desired shape using a photolithography technique. Further, after forming a pattern of a hard magnetic film (not shown), a pattern of the electrode 101 used for supplying a sense current to the MR element 105 was formed.
Amorphous silicon carbide (not shown) having a thickness of 5 nm was formed thereon by sputtering, and a nonmagnetic insulating film 106 made of hydrogen-containing amorphous carbon was formed to have a thickness of 200 nm. This nonmagnetic insulating film 106 was formed under the same conditions as the above nonmagnetic insulating film 104. Further, after 5 nm of amorphous silicon carbide (not shown) was formed, an upper shield film 107 made of NiFe or the like was formed by sputtering, and was patterned by photolithography. Further, a nonmagnetic insulating film 108 made of alumina or the like was formed to a thickness of 500 nm by sputtering. This insulating film is the gap insulating film of the inductive head. Subsequently, an organic insulating film 112 made of a resist or the like, a coil 111 made of copper or the like, and an organic insulating film 112 are sequentially formed. Next, a magnetic film (not shown) of NiFe or the like is formed to a thickness of 200 nm by sputtering or the like, and is patterned into a desired shape using a photolithography technique.
An upper magnetic film 109 having a thickness of 3 μm was formed thereon by plating. Finally, an alumina film is formed by sputtering as a protective film 110 covering the entire head element. The film thickness at this time was 50 μm.
【0016】このようにして形成した薄膜磁気ヘッドを
用いて、TA強度の評価を行った。図5はTA強度評価
の概略図である。故意にTAを発生させるために、磁気
ディスク2には、大きな突起を形成した。ディスクは以
下の方法で作成した。まず、ニッケル燐膜をメッキ法に
より10μm形成した後研磨を行ったアルミニウム・マ
グネシウム合金円板15上に、クロム100nm、コバ
ルト合金膜30nmからなる磁性膜16をスパッタリン
グにより形成した。続いてディスク表面に非晶質炭素膜
をスパッタリングにより30nm形成し、これをフォト
リソグラフィ技術を用いてエッチングすることで、直径
5μm、高さ20nmの突起20を有する保護膜19を
形成した。最後に、膜厚2nmのパーフルオロエーテル
系潤滑膜を付着させた。本実施例の方法で作成したヘッ
ドとディスクを用い、通常より浮上量を下げ、ヘッド素
子と突起19との接触によりTAを故意に発生させる試
験を行ったところ、TA強度は図6に示すように従来の
ヘッドの約2分の1に低下する。Using the thin-film magnetic head thus formed, the TA strength was evaluated. FIG. 5 is a schematic diagram of TA strength evaluation. Large protrusions were formed on the magnetic disk 2 in order to intentionally generate TA. The disc was created by the following method. First, a magnetic film 16 made of 100 nm of chromium and 30 nm of a cobalt alloy film was formed by sputtering on an aluminum / magnesium alloy disk 15 polished after forming a nickel-phosphorous film to a thickness of 10 μm by plating. Subsequently, an amorphous carbon film having a thickness of 30 nm was formed on the disk surface by sputtering, and this was etched using a photolithography technique, thereby forming a protective film 19 having a projection 20 with a diameter of 5 μm and a height of 20 nm. Finally, a 2 nm-thick perfluoroether-based lubricating film was attached. Using a head and a disk produced by the method of the present embodiment, a test was conducted in which the flying height was reduced below normal and TA was intentionally generated by contact between the head element and the projection 19, and the TA strength was as shown in FIG. In addition, it is about half that of the conventional head.
【0017】<実施例2>本実施例では、実施例1で下
部シールド膜とMR素子間の絶縁膜104、MR素子と
上部シールド膜間の絶縁膜106として用いた含水素非
晶質炭素の代わりに、気相合成ダイヤモンドを用いた。
この時、上記絶縁膜104、106の膜厚は、それぞれ
180nm、200nmであった。<Embodiment 2> In this embodiment, the hydrogen-containing amorphous carbon used as the insulating film 104 between the lower shield film and the MR element and the insulating film 106 between the MR element and the upper shield film in Example 1 is used. Instead, vapor phase synthetic diamond was used.
At this time, the thicknesses of the insulating films 104 and 106 were 180 nm and 200 nm, respectively.
【0018】本実施例の方法で作製したヘッドとディス
クを用い、通常より浮上量を下げTAを故意に発生させ
る試験を行ったところ、TA強度は従来のヘッドの約4
分の1に低下する。Using a head and a disk manufactured by the method of the present embodiment, a test was conducted to lower the flying height and to intentionally generate TA. The TA strength was about 4 times that of the conventional head.
It is reduced by a factor of one.
【0019】<実施例3>本実施例では、実施例1で下
部シールド膜とMR素子間の絶縁膜104、MR素子と
上部シールド膜間の絶縁膜106として用いた含水素非
晶質炭素の代わりに、含珪素非晶質炭素を用いた。ただ
し、含珪素非晶質炭素は磁性膜との密着性が非常にいい
ため、実施例1で含水素非晶質炭素の前後の工程で形成
した非晶質シリコン、非晶質炭化珪素は、本実施例では
不必要である。以下に、含珪素非晶質炭素の形成方法を
詳細に述べる。Embodiment 3 In this embodiment, the hydrogen-containing amorphous carbon used as the insulating film 104 between the lower shield film and the MR element and the insulating film 106 between the MR element and the upper shield film in Example 1 is used. Instead, silicon-containing amorphous carbon was used. However, since the silicon-containing amorphous carbon has very good adhesion to the magnetic film, the amorphous silicon and the amorphous silicon carbide formed in the steps before and after the hydrogen-containing amorphous carbon in Example 1 are This is unnecessary in this embodiment. The method for forming silicon-containing amorphous carbon will be described in detail below.
【0020】ターゲット材に珪素と炭素のモル比が30
対70である焼結体を用いて、RFマグネトロンスパッ
タリングにより絶縁膜104、106を形成した。成膜
条件は、高周波電力500W、アルゴンガス流量30s
ccm、ガス圧1Paであった。この膜の珪素濃度は、
RBS(Rutherford Backscatte
ring Spectrometry)分析により、約
38atm%であった。また、絶縁膜104、106の
膜厚は、それぞれ180nm、200nmであった。The target material has a molar ratio of silicon to carbon of 30.
The insulating films 104 and 106 were formed by RF magnetron sputtering using the sintered body of the pair 70. The film formation conditions were a high frequency power of 500 W and an argon gas flow rate of 30 s.
ccm and gas pressure was 1 Pa. The silicon concentration of this film is
RBS (Rutherford Backscatter)
It was about 38 atm% by Ring Spectrometry) analysis. The thicknesses of the insulating films 104 and 106 were 180 nm and 200 nm, respectively.
【0021】本実施例の方法で作製したヘッドとディス
クを用い、通常より浮上量を下げTAを故意に発生させ
る試験を行ったところ、TA強度は従来のヘッドの約3
分の1に低下する。Using a head and a disk produced by the method of this embodiment, a test was conducted in which the flying height was lowered and TA was intentionally generated, and the TA strength was about 3 that of the conventional head.
It is reduced to one-fold.
【0022】<実施例4>本実施例では、実施例1で下
部シールド膜とMR素子間の絶縁膜104、MR素子と
上部シールド膜間の絶縁膜106として用いた含水素非
晶質炭素の代わりに、非晶質AlNを用いた。以下に、
非晶質AlNの形成方法を詳細に述べる。<Embodiment 4> In this embodiment, the hydrogen-containing amorphous carbon used as the insulating film 104 between the lower shield film and the MR element and the insulating film 106 between the MR element and the upper shield film in Example 1 is used. Instead, amorphous AlN was used. less than,
A method for forming amorphous AlN will be described in detail.
【0023】ターゲット材に、AlNを用いて、RFマ
グネトロンスパッタリングにより絶縁膜104、106
を形成した。成膜条件は、高周波電力1000W、アル
ゴンガス流量30sccm+窒素ガス流量5sccm、
ガス圧1.3Paであった。また、絶縁膜104、10
6の膜厚は、それぞれ180nm、200nmであっ
た。Insulating films 104 and 106 are formed by RF magnetron sputtering using AlN as a target material.
Was formed. The film forming conditions are: high frequency power 1000 W, argon gas flow rate 30 sccm + nitrogen gas flow rate 5 sccm,
The gas pressure was 1.3 Pa. In addition, the insulating films 104 and 10
The film thickness of No. 6 was 180 nm and 200 nm, respectively.
【0024】本実施例の方法で作製したヘッドとディス
クを用い、通常より浮上量を下げTAを故意に発生させ
る試験を行ったところ、TA強度は従来のヘッドの約3
分の1に低下する。Using a head and a disk manufactured by the method of this embodiment, a test was conducted in which the flying height was lowered and the TA was intentionally generated, and the TA strength was about 3 that of the conventional head.
It is reduced by a factor of one.
【0025】<実施例5>本実施例では、実施例1で下
部シールド膜とMR素子間の絶縁膜104、MR素子と
上部シールド膜間の絶縁膜106として用いた含水素非
晶質炭素の代わりに、非晶質BeOを用いた。以下に、
非晶質BeOの形成方法を詳細に述べる。Example 5 In this example, the hydrogen-containing amorphous carbon used as the insulating film 104 between the lower shield film and the MR element and the insulating film 106 between the MR element and the upper shield film in Example 1 was used. Instead, amorphous BeO was used. less than,
The method for forming amorphous BeO will be described in detail.
【0026】ターゲット材に、BeOを用いて、RFマ
グネトロンスパッタリングにより絶縁膜104、106
を形成した。成膜条件は、高周波電力800W、アルゴ
ンガス流量50sccm+酸素ガス流量5sccm、ガ
ス圧1.3Paであった。また、絶縁膜104、106
の膜厚は、それぞれ180nm、200nmであった。The insulating films 104 and 106 are formed by RF magnetron sputtering using BeO as a target material.
Was formed. The film formation conditions were a high frequency power of 800 W, an argon gas flow rate of 50 sccm + an oxygen gas flow rate of 5 sccm, and a gas pressure of 1.3 Pa. Further, the insulating films 104 and 106
Had a film thickness of 180 nm and 200 nm, respectively.
【0027】本実施例の方法で作製したヘッドとディス
クを用い、通常より浮上量を下げTAを故意に発生させ
る試験を行ったところ、TA強度は従来のヘッドの約3
分の1に低下する。Using a head and a disk manufactured by the method of this embodiment, a test was conducted in which the flying height was lowered than usual and TA was intentionally generated. As a result, the TA strength was about 3 that of the conventional head.
It is reduced by a factor of one.
【0028】<実施例6>本実施例では、実施例1で下
部シールド膜とMR素子間の絶縁膜104、MR素子と
上部シールド膜間の絶縁膜106として用いた含水素非
晶質炭素の代わりに、含珪素非晶質炭素を用い、且つ、
ディスク保護膜としても、従来の非晶質炭素の代わりに
含珪素非晶質炭素を用いた。含珪素非晶質炭素は異種材
料との密着性が非常にいいため、実施例1で含水素非晶
質炭素の前後の工程で形成した非晶質シリコン、非晶質
炭化珪素は、本実施例では不必要である。以下に、ヘッ
ド、ディスクそれぞれに用いられた含珪素非晶質炭素の
形成方法を詳細に述べる。<Embodiment 6> In this embodiment, the hydrogen-containing amorphous carbon used as the insulating film 104 between the lower shield film and the MR element and the insulating film 106 between the MR element and the upper shield film in Example 1 is used. Instead, silicon-containing amorphous carbon is used, and
As the disk protective film, silicon-containing amorphous carbon was used instead of conventional amorphous carbon. Since silicon-containing amorphous carbon has very good adhesion to different materials, the amorphous silicon and amorphous silicon carbide formed in the steps before and after the hydrogen-containing amorphous carbon in Example 1 were used in this embodiment. Not necessary in the example. Hereinafter, a method of forming the silicon-containing amorphous carbon used for each of the head and the disk will be described in detail.
【0029】まず、ヘッド素子の場合、ターゲット材に
珪素と炭素のモル比が30対70である焼結体を用い
て、RFマグネトロンスパッタリングにより絶縁膜10
4、106を形成した。成膜条件は、高周波電力500
W、アルゴンガス流量30sccm、ガス圧1Paであ
った。この膜の膜中珪素濃度は、RBS(Ruther
ford Backscattering Spect
rometry)分析により、約38atm%であっ
た。また、上記絶縁膜104、106の膜厚は、それぞ
れ180nm、200nmであった。First, in the case of the head element, an insulating film 10 is formed by RF magnetron sputtering using a sintered body having a molar ratio of silicon and carbon of 30:70 as a target material.
4, 106 were formed. The film forming conditions are high-frequency power 500
W, the flow rate of argon gas was 30 sccm, and the gas pressure was 1 Pa. The silicon concentration in the film is RBS (Ruther
ford Backscattering Spec
analysis) was about 38 atm%. The insulating films 104 and 106 had film thicknesses of 180 nm and 200 nm, respectively.
【0030】また、ディスク保護膜形成の際には、ター
ゲット材に珪素と炭素のモル比が40対60である焼結
体を用いて、RFマグネトロンスパッタリングにより上
記絶縁膜104、106を形成した。成膜条件は、高周
波電力500W、アルゴンガス流量30sccm、ガス
圧1Paであった。この膜の珪素濃度は、RBS(Ru
therford Backscattering S
pectrometry)分析により、約49atm%
であった。実施例1同様、このディスク保護膜にもフォ
トリソグラフィ技術を用いて、直径5μm、高さ20n
mの突起を形成した。In forming the disk protective film, the insulating films 104 and 106 were formed by RF magnetron sputtering using a sintered body having a silicon / carbon molar ratio of 40 to 60 as a target material. The film formation conditions were a high frequency power of 500 W, an argon gas flow rate of 30 sccm, and a gas pressure of 1 Pa. The silicon concentration of this film is RBS (Ru
theford Backscuttering S
Spectrometry) analysis shows about 49 atm%
Met. As in the case of the first embodiment, the disk protective film was formed by photolithography using a diameter of 5 μm and a height of 20 n.
m projections were formed.
【0031】本実施例の方法で作製したヘッドとディス
クを用い、通常より浮上量を下げTAを故意に発生させ
る試験を行ったところ、TA強度は従来のヘッド、ディ
スクの組合せの場合の約5分の1に低下する。Using a head and a disk manufactured by the method of the present embodiment, a test was conducted to lower the flying height and to intentionally generate TA. The TA strength was about 5 times that of the conventional combination of head and disk. It is reduced to one-fold.
【0032】<実施例7>図1、図2を用いて本発明の
一実施例を説明する。<Embodiment 7> An embodiment of the present invention will be described with reference to FIGS.
【0033】スライダ14の材料として炭化珪素を用い
た。実施例1同様、スパッタリング、メッキ、フォトリ
ソグラフィ等の薄膜プロセスを用いてヘッド材料を積層
し、MRヘッド11と誘導型ヘッド12からなるヘッド
素子10を作製した。本実施例では、スライダと下部シ
ールド膜の間の絶縁膜102、下部シールド膜とMR素
子間の絶縁膜104、MR素子と上部シールド膜間の絶
縁膜106、誘導型ヘッドのギャップ絶縁膜108、ヘ
ッド全体を保護する絶縁膜110に含水素非晶質炭素を
用いた。以下に上記含水素非晶質炭素の具体的形成方法
を示す。Silicon carbide was used as the material of the slider 14. As in Example 1, head materials were laminated by using a thin film process such as sputtering, plating, photolithography, etc., and a head element 10 composed of an MR head 11 and an inductive head 12 was produced. In this embodiment, the insulating film 102 between the slider and the lower shield film, the insulating film 104 between the lower shield film and the MR element, the insulating film 106 between the MR element and the upper shield film, the gap insulating film 108 of the inductive head, Hydrogen-containing amorphous carbon was used for the insulating film 110 that protects the entire head. Hereinafter, a specific method for forming the hydrogen-containing amorphous carbon will be described.
【0034】グラファイトをターゲットとしたRFスパ
ッタリングにより含水素非晶質炭素を形成した。高周波
電力800W、アルゴンガス流量46sccm+メタン
ガス流量4sccm、ガス圧7Paという条件で成膜を
行った。この膜の水素濃度は、HFS(Hydroge
n Forward Scattering)分析によ
り、約35atm%であった。Hydrogen-containing amorphous carbon was formed by RF sputtering using graphite as a target. Film formation was performed under the following conditions: high frequency power 800 W, argon gas flow rate 46 sccm + methane gas flow rate 4 sccm, and gas pressure 7 Pa. The hydrogen concentration of this film is HFS (Hydrogen
n Forward Scattering analysis showed about 35 atm%.
【0035】含水素非晶質炭素は、それ自身接着性が低
いので、前後の工程で接着層として非晶質炭化珪素を4
nm形成した。また、各層の膜厚は、スライダと下部シ
ールド膜の間の絶縁膜102が8μm、下部シールド膜
とMR素子間の絶縁膜104が180nm、MR素子と
上部シールド膜間の絶縁膜106が200nm、誘導型
ヘッドのギャップ絶縁膜108が500nm、ヘッド全
体を保護する絶縁膜110が45μmであった。Since hydrogen-containing amorphous carbon itself has low adhesiveness, amorphous silicon carbide is used as an adhesive layer in the preceding and subsequent steps.
nm formed. The thickness of each layer is 8 μm for the insulating film 102 between the slider and the lower shield film, 180 nm for the insulating film 104 between the lower shield film and the MR element, and 200 nm for the insulating film 106 between the MR element and the upper shield film. The gap insulating film 108 of the induction type head was 500 nm, and the insulating film 110 for protecting the entire head was 45 μm.
【0036】このようにして形成した薄膜磁気ヘッドを
用いて、ヘッド再生出力の評価を行った。その結果、図
7に示すように再生出力のピークが高電流密度側にシフ
トし、且つピーク位置での再生出力が従来ヘッドの1.
5倍に改善された。すなわち、MR素子の放熱が効果的
に行われるために、高い電流密度でも温度上昇による再
生出力の低下が押さえられることが明らかになった。こ
の際、従来のヘッドも本実施例のヘッドも、それぞれバ
イアス磁界の最適化を行うことによって、それぞれの出
力波形が対称になるような条件で比較を行った。また、
実施例1と同様、本実施例の方法で作成したヘッドと大
きな突起を有するディスクを用い、通常より浮上量を下
げTAを故意に発生させる試験を行ったところ、TA強
度は従来のヘッドの約2分の1に低下する。The thin-film magnetic head thus formed was used to evaluate the head reproduction output. As a result, as shown in FIG. 7, the reproduction output peak is shifted to the high current density side, and the reproduction output at the peak position is 1.
It has improved five times. In other words, it has been clarified that since the heat radiation of the MR element is effectively performed, even at a high current density, a decrease in the reproduction output due to a rise in temperature is suppressed. At this time, both the conventional head and the head of this embodiment were compared under the condition that the respective output waveforms were symmetrical by optimizing the bias magnetic field. Also,
As in the case of the first embodiment, a test was performed using the head formed by the method of the present embodiment and a disk having large projections to lower the flying height and deliberately generate TA. It is reduced by half.
【0037】<実施例8>図1、図2を用いて本発明の
一実施例を説明する。<Embodiment 8> An embodiment of the present invention will be described with reference to FIGS.
【0038】スライダ14の材料として炭化珪素を用い
た。実施例1同様、スパッタリング、メッキ、フォトリ
ソグラフィ等の薄膜プロセスを用いてヘッド材料を積層
し、MRヘッド11と誘導型ヘッド12からなるヘッド
素子10を作製した。本実施例では、スライダと下部シ
ールド膜の間の絶縁膜102、下部シールド膜とMR素
子間の絶縁膜104、MR素子と上部シールド膜間の絶
縁膜106、誘導型ヘッドのギャップ絶縁膜108、ヘ
ッド全体を保護する絶縁膜110に気相合成ダイヤモン
ドを用いた。Silicon carbide was used as the material of the slider 14. As in Example 1, head materials were laminated by using a thin film process such as sputtering, plating, photolithography, etc., and a head element 10 composed of an MR head 11 and an inductive head 12 was produced. In this embodiment, the insulating film 102 between the slider and the lower shield film, the insulating film 104 between the lower shield film and the MR element, the insulating film 106 between the MR element and the upper shield film, the gap insulating film 108 of the induction type head, Vapor phase synthetic diamond is used for the insulating film 110 that protects the entire head.
【0039】気相合成ダイヤモンドは、それ自身接着性
が低いので、前後の工程で接着層として非晶質シリコン
を5nm形成した。また、各層の膜厚は、スライダと下
部シールド膜の間の絶縁膜102が2μm、下部シール
ド膜とMR素子間の絶縁膜104が180nm、MR素
子と上部シールド膜間の絶縁膜106が200nm、誘
導型ヘッドのギャップ絶縁膜108が500nm、ヘッ
ド全体を保護する絶縁膜110が20μmであった。Since vapor-phase synthetic diamond itself has low adhesiveness, amorphous silicon having a thickness of 5 nm was formed as an adhesive layer in the preceding and following steps. The thickness of each layer is 2 μm for the insulating film 102 between the slider and the lower shield film, 180 nm for the insulating film 104 between the lower shield film and the MR element, 200 nm for the insulating film 106 between the MR element and the upper shield film, The gap insulating film 108 of the induction type head was 500 nm, and the insulating film 110 protecting the entire head was 20 μm.
【0040】このようにして形成した薄膜磁気ヘッドを
用いて、ヘッド再生出力の評価を行った。その結果、再
生出力のピークが高電流密度側にシフトし、且つピーク
位置での再生出力が従来ヘッドの2倍に改善された。ま
た、実施例1と同様、本実施例の方法で作成したヘッド
と大きな突起を有するディスクを用い、通常より浮上量
を下げTAを故意に発生させる試験を行ったところ、T
A強度は従来のヘッドの約4分の1に低下する。Using the thin film magnetic head thus formed, the head reproduction output was evaluated. As a result, the peak of the reproduction output shifted to the high current density side, and the reproduction output at the peak position was improved to twice that of the conventional head. Also, as in Example 1, a test was performed using the head formed by the method of the present example and a disk having large projections to lower the flying height from normal and to intentionally generate TA.
The A strength is reduced to about 1/4 of that of the conventional head.
【0041】<実施例9>図1、図2を用いて本発明の
一実施例を説明する。<Embodiment 9> An embodiment of the present invention will be described with reference to FIGS.
【0042】基板として炭化珪素を用いた。実施例1同
様、スパッタリング、メッキ、フォトリソグラフィ等の
薄膜プロセスを用いてヘッド材料を積層し、MRヘッド
11と誘導型ヘッド12からなるヘッド素子10を作製
した。本実施例では、スライダと下部シールド膜の間の
絶縁膜102、下部シールド膜とMR素子間の絶縁膜1
04、MR素子と上部シールド膜間の絶縁膜106、誘
導型ヘッドのギャップ絶縁膜108、ヘッド全体を保護
する絶縁膜110に含珪素非晶質炭素を用いた。以下に
上記含珪素非晶質炭素の具体的形成方法を示す。Silicon carbide was used as a substrate. As in Example 1, head materials were laminated by using a thin film process such as sputtering, plating, photolithography, etc., and a head element 10 composed of an MR head 11 and an inductive head 12 was produced. In this embodiment, the insulating film 102 between the slider and the lower shield film and the insulating film 1 between the lower shield film and the MR element
04, silicon-containing amorphous carbon was used for the insulating film 106 between the MR element and the upper shield film, the gap insulating film 108 of the induction type head, and the insulating film 110 for protecting the entire head. The specific method for forming the silicon-containing amorphous carbon will be described below.
【0043】ターゲット材に、珪素と炭素のモル比が3
5対60である焼結体を用いて、RFマグネトロンスパ
ッタリングにより含珪素非晶質炭素を形成した。成膜条
件は、高周波電力500W、アルゴンガス流量30sc
cm、ガス圧1Paであった。この膜の珪素濃度は、R
BS(Rutherford Backscatter
ing Spectrometry)分析により、約4
4atm%であった。各層の膜厚は、スライダと下部シ
ールド膜の間の絶縁膜102が5μm、下部シールド膜
とMR素子間の絶縁膜104が180nm、MR素子と
上部シールド膜間の絶縁膜106が200nm、誘導型
ヘッドのギャップ絶縁膜108が450nm、ヘッド全
体を保護する絶縁膜110が40μmであった。The target material has a molar ratio of silicon to carbon of 3
Using a 5 to 60 sintered body, silicon-containing amorphous carbon was formed by RF magnetron sputtering. The film formation conditions were a high frequency power of 500 W and an argon gas flow rate of 30 sc.
The gas pressure was 1 cm and the gas pressure was 1 Pa. The silicon concentration of this film is R
BS (Rutherford Backscatter)
ing Spectrometry) analysis reveals about 4
It was 4 atm%. Regarding the film thickness of each layer, the insulating film 102 between the slider and the lower shield film is 5 μm, the insulating film 104 between the lower shield film and the MR element is 180 nm, the insulating film 106 between the MR element and the upper shield film is 200 nm, and the inductive type is used. The gap insulating film 108 of the head was 450 nm, and the insulating film 110 protecting the entire head was 40 μm.
【0044】このようにして形成した薄膜磁気ヘッドを
用いて、ヘッド再生出力の評価を行った。その結果、再
生出力のピークが高電流密度側にシフトし、且つピーク
位置での再生出力が従来ヘッドの1.8倍に改善され
た。また、実施例1と同様、本実施例の方法で作成した
ヘッドと大きな突起を有するディスクを用い、通常より
浮上量を下げTAを故意に発生させる試験を行ったとこ
ろ、TA強度は従来のヘッドの約3分の1に低下する。Using the thin-film magnetic head thus formed, the head reproduction output was evaluated. As a result, the peak of the reproduction output shifted to the high current density side, and the reproduction output at the peak position was improved to 1.8 times that of the conventional head. As in the case of the first embodiment, a test was conducted using the head formed by the method of the present embodiment and a disk having large projections to lower the flying height and deliberately generate TA. To about one-third.
【0045】<実施例10>図1、図2を用いて本発明
の一実施例を説明する。<Embodiment 10> An embodiment of the present invention will be described with reference to FIGS.
【0046】スライダ14の材料として炭化珪素を用い
た。実施例1同様、スパッタリング、メッキ、フォトリ
ソグラフィ等の薄膜プロセスを用いてヘッド材料を積層
し、MRヘッド11と誘導型ヘッド12からなるヘッド
素子10を作製した。本実施例では、スライダと下部シ
ールド膜の間の絶縁膜102、下部シールド膜とMR素
子間の絶縁膜104、MR素子と上部シールド膜間の絶
縁膜106、誘導型ヘッドのギャップ絶縁膜108、ヘ
ッド全体を保護する絶縁膜110に非晶質AlNを用い
た。以下に上記非晶質AlNの具体的形成方法を示す。Silicon carbide was used as the material of the slider 14. As in Example 1, head materials were laminated by using a thin film process such as sputtering, plating, photolithography, etc., and a head element 10 composed of an MR head 11 and an inductive head 12 was produced. In this embodiment, the insulating film 102 between the slider and the lower shield film, the insulating film 104 between the lower shield film and the MR element, the insulating film 106 between the MR element and the upper shield film, the gap insulating film 108 of the induction type head, Amorphous AlN was used for the insulating film 110 that protects the entire head. The specific method for forming the amorphous AlN will be described below.
【0047】ターゲット材に、 AlNを用いて、RF
マグネトロンスパッタリングにより非晶質AlNを形成
した。成膜条件は、高周波電力1000W、アルゴンガ
ス流量30sccm+窒素ガス流量5sccm、ガス圧
1.3Paであった。また、各層の膜厚は、スライダと
下部シールド膜の間の絶縁膜102が5μm、下部シー
ルド膜とMR素子間の絶縁膜104が180nm、MR
素子と上部シールド膜間の絶縁膜106が200nm、
誘導型ヘッドのギャップ絶縁膜108が500nm、ヘ
ッド全体を保護する絶縁膜110が50μmであった。RF is obtained by using AlN as a target material.
Amorphous AlN was formed by magnetron sputtering. The film forming conditions were a high frequency power of 1000 W, an argon gas flow rate of 30 sccm + a nitrogen gas flow rate of 5 sccm, and a gas pressure of 1.3 Pa. The thickness of each layer is 5 μm for the insulating film 102 between the slider and the lower shield film, 180 nm for the insulating film 104 between the lower shield film and the MR element, and for the MR film.
The insulating film 106 between the element and the upper shield film is 200 nm,
The gap insulating film 108 of the induction type head was 500 nm, and the insulating film 110 for protecting the entire head was 50 μm.
【0048】このようにして形成した薄膜磁気ヘッドを
用いて、ヘッド再生出力の評価を行った。その結果、再
生出力のピークが高電流密度側にシフトし、且つピーク
位置での再生出力が従来ヘッドの1.6倍に改善され
た。また、実施例1と同様、本実施例の方法で作成した
ヘッドと大きな突起を有するディスクを用い、通常より
浮上量を下げTAを故意に発生させる試験を行ったとこ
ろ、TA強度は従来のヘッドの約3分の1に低下する。Using the thin film magnetic head thus formed, the head reproduction output was evaluated. As a result, the reproduction output peak was shifted to the high current density side, and the reproduction output at the peak position was improved to 1.6 times that of the conventional head. Further, as in the case of Example 1, using the head prepared by the method of this example and a disk having large protrusions, a test was conducted in which the flying height was lowered than usual and TA was intentionally generated. About one-third.
【0049】<実施例11>図1、図2を用いて本発明
の一実施例を説明する。<Embodiment 11> An embodiment of the present invention will be described with reference to FIGS.
【0050】スライダ14の材料として炭化珪素を用い
た。実施例1同様、スパッタリング、メッキ、フォトリ
ソグラフィ等の薄膜プロセスを用いてヘッド材料を積層
し、MRヘッド11と誘導型ヘッド12からなるヘッド
素子10を作製した。本実施例では、スライダと下部シ
ールド膜の間の絶縁膜102、下部シールド膜とMR素
子間の絶縁膜104、MR素子と上部シールド膜間の絶
縁膜106、誘導型ヘッドのギャップ絶縁膜108、ヘ
ッド全体を保護する絶縁膜110に非晶質BeOを用い
た。以下に上記非晶質BeOの具体的形成方法を示す。Silicon carbide was used as the material of the slider 14. As in Example 1, head materials were laminated by using a thin film process such as sputtering, plating, photolithography, etc., and a head element 10 composed of an MR head 11 and an inductive head 12 was produced. In this embodiment, the insulating film 102 between the slider and the lower shield film, the insulating film 104 between the lower shield film and the MR element, the insulating film 106 between the MR element and the upper shield film, the gap insulating film 108 of the inductive head, Amorphous BeO was used for the insulating film 110 for protecting the entire head. Hereinafter, a specific method for forming the amorphous BeO will be described.
【0051】ターゲット材に、BeOを用いて、RFマ
グネトロンスパッタリングにより上記絶縁膜104、1
06を形成した。成膜条件は、高周波電力800W、ア
ルゴンガス流量50sccm+酸素ガス流量5scc
m、ガス圧1.3Paであった。また、各層の膜厚は、
スライダと下部シールド膜の間の絶縁膜102が4μ
m、下部シールド膜とMR素子間の絶縁膜104が18
0nm、MR素子と上部シールド膜間の絶縁膜106が
200nm、誘導型ヘッドのギャップ絶縁膜108が5
00nm、ヘッド全体を保護する絶縁膜110が40μ
mであった。BeO is used as the target material, and the insulating films 104 and 1 are formed by RF magnetron sputtering.
06 was formed. The film forming conditions are high-frequency power 800 W, argon gas flow rate 50 sccm + oxygen gas flow rate 5 sccc.
m, and the gas pressure was 1.3 Pa. The film thickness of each layer is
The insulating film 102 between the slider and the lower shield film has a thickness of 4 μm.
m, the insulating film 104 between the lower shield film and the MR element is 18
0 nm, the insulating film 106 between the MR element and the upper shield film is 200 nm, and the gap insulating film 108 of the inductive head is 5 nm.
00 nm, the insulating film 110 for protecting the entire head is 40 μm.
It was m.
【0052】このようにして形成した薄膜磁気ヘッドを
用いて、ヘッド再生出力の評価を行った。その結果、再
生出力のピークが高電流密側にシフトし、且つピーク位
置での再生出力が従来ヘッドの1.6倍に改善された。
また、実施例1と同様、本実施例の方法で作成したヘッ
ドと大きな突起を有するディスクを用い、通常より浮上
量を下げTAを故意に発生させる試験を行ったところ、
TA強度は従来のヘッドの約3分の1に低下する。Using the thin-film magnetic head thus formed, the head reproduction output was evaluated. As a result, the reproduction output peak was shifted to the high current density side, and the reproduction output at the peak position was improved to 1.6 times that of the conventional head.
Also, as in Example 1, a test was performed using the head formed by the method of the present example and a disk having large projections to reduce the flying height below normal and to intentionally generate TA.
The TA intensity is reduced to about one third of the conventional head.
【0053】[0053]
【発明の効果】本発明によれば、熱拡散率の高い非磁性
絶縁膜をヘッド素子の構成材料や、ディスク保護膜とし
て選択することにより、ディスクとヘッドが接触した際
発生するTAを低減し、また、効率的にMR素子の放熱
を行えるため再生出力を向上させることができる。According to the present invention, the non-magnetic insulating film having a high thermal diffusivity is selected as the constituent material of the head element and the disk protective film to reduce the TA generated when the disk and the head come into contact with each other. Also, since the MR element can efficiently dissipate heat, the reproduction output can be improved.
【図1】薄膜磁気ヘッド素子部の断面図。FIG. 1 is a sectional view of a thin-film magnetic head element section.
【図2】薄膜磁気ヘッド素子部をディスク対向面から見
た説明図。FIG. 2 is an explanatory view of the thin-film magnetic head element section viewed from a disk facing surface.
【図3】薄膜磁気ヘッドスライダの斜視図。FIG. 3 is a perspective view of a thin-film magnetic head slider.
【図4】磁気ディスク装置動作時のヘッドスライダとデ
ィスクの位置関係の説明図。FIG. 4 is an explanatory diagram of a positional relationship between a head slider and a disk when the magnetic disk device is operating.
【図5】TA評価時のヘッドスライダとディスクの説明
図。FIG. 5 is an explanatory diagram of a head slider and a disk at the time of TA evaluation.
【図6】従来のヘッドと本発明の一実施例のヘッドのT
A強度の比較を示す特性図。FIG. 6 shows T of a conventional head and a head of one embodiment of the present invention.
The characteristic view which shows the comparison of A intensity.
【図7】従来のヘッドと本発明の一実施例のヘッドの再
生出力飽和点の比較を示す特性図。FIG. 7 is a characteristic diagram showing a comparison of reproduction output saturation points of a conventional head and a head of one embodiment of the present invention.
10…薄膜磁気ヘッド素子 11…MRヘッド、 12…誘導型ヘッド、 13…ヘッドスライダ表面の保護膜、 101…電極、 102…下地絶縁膜、 103…下部シールド膜、 104…絶縁膜、 105…MR素子、 106…絶縁膜、 107…上部シールド膜、 108…誘導型素子のギャップ絶縁膜、 109…上部磁性膜、 110…保護絶縁膜、 111…コイル膜、 112…有機絶縁膜。 DESCRIPTION OF SYMBOLS 10 ... Thin film magnetic head element 11 ... MR head, 12 ... Inductive head, 13 ... Protective film on the surface of a head slider, 101 ... Electrode, 102 ... Under-insulating film, 103 ... Lower shield film, 104 ... Insulating film, 105 ... MR Element 106: Insulating film 107: Upper shield film 108: Gap insulating film of inductive element 109: Upper magnetic film 110: Protective insulating film 111: Coil film 112: Organic insulating film
───────────────────────────────────────────────────── フロントページの続き (72)発明者 時末 裕充 神奈川県小田原市国府津2880番地株式会社 日立製作所ストレージシステム事業部内 (72)発明者 斉木 教行 神奈川県小田原市国府津2880番地株式会社 日立製作所ストレージシステム事業部内 ──────────────────────────────────────────────────続 き Continuing on the front page (72) Inventor Hiromitsu Toshimatsu 2880 Kozu, Odawara-shi, Kanagawa Prefecture, Hitachi, Ltd.Storage Systems Division (72) Inventor Noriyuki Saiki 2880 Kozu, Kozu, Odawara-shi, Kanagawa Hitachi Storage Corporation System Division
Claims (8)
込みに誘導型ヘッドを用いる磁気ヘッドにおいて、下部
シールド膜とMR素子間の絶縁膜、上記MR素子と上部
シールド膜間の絶縁膜として、含水素非晶質炭素、気相
合成ダイヤモンド、含珪素非晶質炭素、非晶質AlN、
非晶質BeOのうち少なくとも一つの材料を用いること
を特徴とする薄膜磁気ヘッド。In a magnetic head using a magnetoresistive head for reading and an inductive head for writing, an insulating film between a lower shield film and an MR element and an insulating film between the MR element and an upper shield film are included. Hydrogen amorphous carbon, vapor-phase synthetic diamond, silicon-containing amorphous carbon, amorphous AlN,
A thin-film magnetic head using at least one material of amorphous BeO.
型ヘッドを用いる磁気ヘッドにおいて、下部シールド膜
とMR素子間の絶縁膜、上記MR素子と上部シールド膜
間の絶縁膜として含水素非晶質炭素を用いる際に、上記
含水素非晶質炭素中の水素濃度が10〜50atm%で
あることを特徴とする薄膜磁気ヘッド。2. A magnetic head using an MR head for reading and an inductive head for writing, wherein a hydrogen-containing amorphous film is used as an insulating film between the lower shield film and the MR element and an insulating film between the MR element and the upper shield film. When using carbon, the hydrogen concentration in the hydrogen-containing amorphous carbon is 10 to 50 atm%.
型ヘッドを用いる磁気ヘッドにおいて、下部シールド膜
とMR素子間の絶縁膜、MR素子と上部シールド膜間の
絶縁膜として含珪素非晶質炭素を用いる際に、上記含珪
素非晶質炭素中の珪素濃度が10〜70atm%である
ことを特徴とする薄膜磁気ヘッド。3. A magnetic head using an MR head for reading and an inductive head for writing, wherein silicon-containing amorphous carbon is used as an insulating film between the lower shield film and the MR element and an insulating film between the MR element and the upper shield film. Wherein the silicon concentration in the silicon-containing amorphous carbon is 10 to 70 atm%.
型ヘッドを用いる磁気ヘッドの製造方法で、下部シール
ド膜とMR素子間の絶縁膜、MR素子と上部シールド膜
間の絶縁膜として含水素非晶質炭素を用いる際に、スパ
ッタリング法、化学蒸着法により形成した非晶質珪素あ
るいは非晶質炭化珪素の接着層を介して、上記含水素非
晶質炭素を化学蒸着法、スパッタリング法等により形成
する請求項2に記載の薄膜磁気ヘッドの製造方法。4. A method of manufacturing a magnetic head using an MR head for reading and an induction type head for writing, comprising a hydrogen-containing non-insulating film as an insulating film between a lower shield film and an MR element and an insulating film between an MR element and an upper shield film. When amorphous carbon is used, the above hydrogen-containing amorphous carbon is deposited by a chemical vapor deposition method, a sputtering method, or the like through an adhesive layer of amorphous silicon or amorphous silicon carbide formed by a sputtering method, a chemical vapor deposition method. The method of manufacturing a thin film magnetic head according to claim 2, wherein the thin film magnetic head is formed.
型ヘッドを用いる磁気ヘッドの製造方法であって、下部
シールド膜とMR素子間の絶縁膜、MR素子と上部シー
ルド膜間の絶縁膜として気相合成ダイヤモンドを用いる
際に、スパッタリング法、化学蒸着法により形成した非
晶質珪素あるいは非晶質炭化珪素の接着層を介して、上
記気相合成ダイヤモンドを化学蒸着法により形成する請
求項1に記載の薄膜磁気ヘッドの製造方法。5. A method of manufacturing a magnetic head using an MR head for reading and an inductive head for writing, comprising: an insulating film between a lower shield film and an MR element; and an insulating film between an MR element and an upper shield film. When the phase-synthesized diamond is used, the vapor-phase synthesized diamond is formed by the chemical vapor deposition method via an adhesive layer of amorphous silicon or amorphous silicon carbide formed by the sputtering method or the chemical vapor deposition method. A method for manufacturing the thin film magnetic head described.
型ヘッドを用いる磁気ヘッドの製造方法であって、下部
シールド膜とMR素子間の絶縁膜、MR素子と上部シー
ルド膜間の絶縁膜として含珪素非晶質炭素、非晶質Al
N、非晶質BeOのいずれか一つの絶縁膜を用いる際
に、上記絶縁膜をスパッタリング法により形成する請求
項1に記載の薄膜磁気ヘッドの製造方法。6. A method for manufacturing a magnetic head using an MR head for reading and an inductive head for writing, comprising an insulating film between the lower shield film and the MR element and an insulating film between the MR element and the upper shield film. Silicon amorphous carbon, amorphous Al
2. The method according to claim 1, wherein the insulating film is formed by a sputtering method when using any one of N and amorphous BeO.
型ヘッドを用いる磁気ディスク装置において、下部シー
ルド膜とMR素子間の絶縁膜、及びMR素子と上部シー
ルド膜間の絶縁膜に含水素非晶質炭素、気相合成ダイヤ
モンド、含珪素非晶質炭素、非晶質AlN、非晶質Be
Oのうち少なくとも一つの材料を用い、且つディスク表
面の保護膜として気相合成ダイヤモンド、含珪素非晶質
炭素、非晶質AlN、非晶質BeOのうち少なくとも一
つの材料を用いることを特徴とする磁気ディスク装置。7. A magnetic disk drive using an MR head for reading and an inductive head for writing, wherein a hydrogen-containing amorphous film is formed on an insulating film between the lower shield film and the MR element and an insulating film between the MR element and the upper shield film. Carbon, gas-phase synthetic diamond, silicon-containing amorphous carbon, amorphous AlN, amorphous Be
O, and at least one material selected from the group consisting of vapor-phase synthetic diamond, silicon-containing amorphous carbon, amorphous AlN, and amorphous BeO as a protective film on the disk surface. Magnetic disk drive.
型ヘッドを用いる磁気ヘッドにおいて、ヘッドを支持す
るスライダの材料に炭化珪素を用い、且つスライダと下
部シールド膜の間の絶縁膜、下部シールド膜とMR素子
間の絶縁膜、MR素子と上部シールド膜間の絶縁膜、誘
導型ヘッドのギャップ絶縁膜、ヘッド全体を保護する絶
縁膜として、含水素非晶質炭素、気相合成ダイヤモン
ド、含珪素非晶質炭素、非晶質AlN、非晶質BeOの
うち少なくとも一つを用いることを特徴とする磁気ヘッ
ド。8. A magnetic head using an MR head for reading and an inductive head for writing, using silicon carbide as a material of a slider supporting the head, and an insulating film and a lower shield film between the slider and the lower shield film. Hydrogen-containing amorphous carbon, vapor-phase synthetic diamond, silicon-containing, as an insulating film between the MR element and the MR element, an insulating film between the MR element and the upper shield film, a gap insulating film of the inductive head, and an insulating film for protecting the entire head. A magnetic head using at least one of amorphous carbon, amorphous AlN, and amorphous BeO.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2345897A JPH10222816A (en) | 1997-02-06 | 1997-02-06 | Thin-film magnetic head and magnetic disk drive |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2345897A JPH10222816A (en) | 1997-02-06 | 1997-02-06 | Thin-film magnetic head and magnetic disk drive |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH10222816A true JPH10222816A (en) | 1998-08-21 |
Family
ID=12111075
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2345897A Pending JPH10222816A (en) | 1997-02-06 | 1997-02-06 | Thin-film magnetic head and magnetic disk drive |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH10222816A (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6414825B1 (en) * | 1998-10-06 | 2002-07-02 | Tdk Corporation | Thin film device, thin film magnetic head and magnetoresistive element |
| US6636395B1 (en) | 1999-06-03 | 2003-10-21 | Tdk Corporation | Magnetic transducer and thin film magnetic head using the same |
| US6947259B2 (en) | 2002-07-30 | 2005-09-20 | Tdk Corporation | Magnetic head, magnetic head device and magnetic recording/reproducing device |
| US7088560B2 (en) | 2002-04-10 | 2006-08-08 | Tdk Corporation | Thin film magnetic head including a heat dissipation layer, method of manufacturing the same and magnetic disk drive |
-
1997
- 1997-02-06 JP JP2345897A patent/JPH10222816A/en active Pending
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6414825B1 (en) * | 1998-10-06 | 2002-07-02 | Tdk Corporation | Thin film device, thin film magnetic head and magnetoresistive element |
| US6636395B1 (en) | 1999-06-03 | 2003-10-21 | Tdk Corporation | Magnetic transducer and thin film magnetic head using the same |
| US7088560B2 (en) | 2002-04-10 | 2006-08-08 | Tdk Corporation | Thin film magnetic head including a heat dissipation layer, method of manufacturing the same and magnetic disk drive |
| US7126794B2 (en) | 2002-04-10 | 2006-10-24 | Tdk Corporation | Thin film magnetic head including heat dissipation, method of manufacturing the same, and magnetic disk drive |
| US6947259B2 (en) | 2002-07-30 | 2005-09-20 | Tdk Corporation | Magnetic head, magnetic head device and magnetic recording/reproducing device |
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