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JP4038437B2 - Magnetic head slider and magnetic disk apparatus - Google Patents
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JP4038437B2 - Magnetic head slider and magnetic disk apparatus - Google Patents

Magnetic head slider and magnetic disk apparatus Download PDF

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Publication number
JP4038437B2
JP4038437B2 JP2003031841A JP2003031841A JP4038437B2 JP 4038437 B2 JP4038437 B2 JP 4038437B2 JP 2003031841 A JP2003031841 A JP 2003031841A JP 2003031841 A JP2003031841 A JP 2003031841A JP 4038437 B2 JP4038437 B2 JP 4038437B2
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flying height
recording
reproducing
magnetic disk
slider
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JP2004241092A (en
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昌幸 栗田
英一 小平
鈞国 徐
幹夫 徳山
晃司 三宅
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株式会社日立グローバルストレージテクノロジーズ
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    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/48Disposition or mounting of heads or head supports relative to record carriers ; arrangements of heads, e.g. for scanning the record carrier to increase the relative speed
    • G11B5/58Disposition or mounting of heads or head supports relative to record carriers ; arrangements of heads, e.g. for scanning the record carrier to increase the relative speed with provision for moving the head for the purpose of maintaining alignment of the head relative to the record carrier during transducing operation, e.g. to compensate for surface irregularities of the latter or for track following
    • G11B5/60Fluid-dynamic spacing of heads from record-carriers
    • G11B5/6005Specially adapted for spacing from a rotating disc using a fluid cushion
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/48Disposition or mounting of heads or head supports relative to record carriers ; arrangements of heads, e.g. for scanning the record carrier to increase the relative speed
    • G11B5/58Disposition or mounting of heads or head supports relative to record carriers ; arrangements of heads, e.g. for scanning the record carrier to increase the relative speed with provision for moving the head for the purpose of maintaining alignment of the head relative to the record carrier during transducing operation, e.g. to compensate for surface irregularities of the latter or for track following
    • G11B5/60Fluid-dynamic spacing of heads from record-carriers
    • G11B5/6005Specially adapted for spacing from a rotating disc using a fluid cushion
    • G11B5/6011Control of flying height
    • G11B5/6064Control of flying height using air pressure

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  • Adjustment Of The Magnetic Head Position Track Following On Tapes (AREA)

Description

【0001】
【発明の属する技術分野】
本発明は、磁気ディスク装置の高記録密度化を実現するための磁気ヘッドスライダ構造に係わり、特に磁気ディスクと磁気ヘッドの距離を調整する機能を持った浮上量調整スライダに関する。
【0002】
【従来の技術】
磁気ディスク装置は、回転する磁気ディスクと、記録再生素子を搭載しロードビームによって支持および径方向位置決めされた磁気ヘッドスライダ(単にスライダとも呼ぶ)を有し、スライダが相対的に磁気ディスク上を走行して磁気ディスク上に記録された磁気情報を読み書きする。前記スライダは空気潤滑軸受として空気のくさび膜効果によって浮上し、磁気ディスクとスライダが直接は固体接触しないようになっている。磁気ディスク装置の高記録密度化と、それによる装置の大容量化あるいは小型化を実現するためには、スライダと磁気ディスクの距離、すなわちスライダ浮上量を縮め、線記録密度を上げることが有効である。
【0003】
従来からスライダ浮上量の設計においては、加工ばらつきや使用環境気圧差、使用環境温度差などによる浮上量低下を見込み、最悪条件でもスライダとディスクが接触しないように、浮上量マージンを設けてきた。ヘッド個体毎に、または使用環境に応じて浮上量を調整する機能を設けたスライダを実現すれば上記マージンを廃することができ、スライダとディスクの接触は防ぎつつ記録再生素子の浮上量を大幅に縮めることができる。例えば、薄膜抵抗体から成る加熱装置を記録再生素子近傍に設け、スライダの一部を必要に応じて加熱して熱膨張、突出させ、記録再生素子の浮上量を調整するスライダ構造が提案されている(例えば、特許文献1参照)。
【特許文献1】
特開平5−20635号公報(第3頁)。
【0004】
【発明が解決しようとする課題】
第一に、再生素子寿命の課題がある。現在主流となっている磁気抵抗効果(MR効果)を利用した再生素子は熱負荷に弱く、高温に晒される時間が長いと寿命が短くなるという特徴がある。特開平5−20635号公報によって示された方法は有効な浮上量調整方法であるが、現在の記録再生素子に適用しようとすると、加熱装置である薄膜抵抗体が記録再生素子のごく近くに位置するため、加熱によって再生素子の寿命を低減してしまう恐れがある。
【0005】
第二に、浮上量調整方向の課題がある。同公報によって示された方式は記録再生素子部を熱膨張によって突出させる方式なので、通電によって浮上量は小さくなる。環境気圧(使用高度)に関しては、空気軸受がうける圧力が大きい高圧(低地)では浮上量が大きく、低圧(高地)になるに従って浮上量が小さくなる傾向がある。従って、高地でも接触しない浮上面設計をし、低地では常に通電して浮上量を下げる必要があるが、低地で使われる方が高地で使われるよりも頻度が高いので、同公報によって示された浮上量調整方向は逆の方向に比べて要する電力が大きくなる。
【0006】
以上まとめると、再生素子への熱負荷を小さくすること、および通電によって浮上量を大きくする方向の調整方法を開発すること、この二点が本発明によって解決しようとする課題である。
【0007】
【課題を解決するための手段】
上記課題は、第一に加熱装置である薄膜抵抗体を記録再生素子から十分離すこと、第二に抵抗体への通電にともなう浮上面一部の突出によって浮上面で発生する空気圧力が増加するように浮上面設計すること、この二点により解決される。
第一の点に関し、薄膜抵抗体が前記記録再生素子から0.1mm以上離れている必要がある。記録再生素子が空気流出端中央にある場合、流出端付近で記録再生素子の両側にそれぞれ少なくとも0.1mm以上離して薄膜抵抗体を設置すると良い。
第二の点に関し、現在産業界で広く使われている2段ステップ軸受スライダの浮上面は、実質的に平行な3つの面、すなわち(1)記録再生素子が設置されたレール面、(2)ステップ軸受である浅溝面、(3)負圧ポケットである深溝面、から構成されているが、近年、レール面を記録再生素子が設置された最上面(素子設置面と呼称)と、約5nm乃至50nmのごく浅いステップ軸受面(超浅溝面と呼称)の2つの面に分割し、浮上面が合計4つの平行な面から構成される3段ステップ軸受スライダが新たに提案されている。3段ステップスライダは素子設置面を小さく幅狭にして、周囲には素子設置面よりわずかに低い超浅溝面を設けたことにより、スライダのロール方向傾斜にかかわらず素子設置面が最もディスクに近くなることを保証でき、記録再生素子の低浮上化に寄与する。また、素子設置面を小さくしても超浅溝面が空気圧力を発生し荷重を支えているので、ディスク微小うねりへの追従性を損なうことはないという特徴がある。
前記の薄膜抵抗体は浮上面表面に露出して、あるいは浮上面から法線方向内部にある程度の距離を持った位置に形成される。薄膜抵抗体を浮上面に投影した位置が、前記超浅溝面領域内あるいはその近傍にあると、薄膜抵抗体に通電加熱して周囲を熱膨張変形させた時に、超浅溝面がディスク側に変位し、超浅溝面で発生する空気圧力が増加することによって、スライダ全体の浮上量および記録再生素子の浮上量が増加する。すなわち通電によって浮上量が増加する方向の浮上量調整である。
ここまで述べた手段により再生素子の寿命に影響せず、要する消費電力が小さい浮上量調整が実現できる。その結果、ヘッド個体毎に、または使用環境に応じて浮上量を調整することによって浮上量マージンを廃することができ、スライダとディスクの接触は防ぎつつ記録再生素子の浮上量を大幅に縮め、磁気ディスク面記録密度の増大、更には装置の大容量化あるいは小型化に寄与する。
【0008】
【発明の実施の形態】
本発明の実施形態に係わる磁気ヘッドスライダおよびこれを用いた磁気ディスク装置について、図面を用いて以下説明する。
【0009】
本発明の一実施例による磁気ディスク装置の概略構成を図1に示す。磁気ヘッドスライダ1には、磁気情報を記録再生する記録再生素子が搭載されている。磁気ディスク10は磁気情報が格納され、スピンドルモータによって回転される。磁気ヘッドスライダ1は、板ばね状のロードビームに取り付けられており、ロードビームによって磁気ディスク面への押し付け荷重を与えられ、ロードビームとともにボイスコイルモータによって磁気ディスク10の径方向にシーク動作し、磁気ディスク面全体で記録再生を行う。磁気ヘッドスライダ1は、装置の停止時あるいは読み書き命令が一定時間無い時に、磁気ディスク10上からランプ14上に待避する。
なお、ここではロード・アンロード機構を備えた装置を示したが、装置停止中は磁気ヘッドスライダ1が磁気ディスク10のある特定の領域で待機するコンタクト・スタート・ストップ方式の磁気ディスク装置でも本発明の効果は同様に得られる。
【0010】
図2は本発明の第一の実施形態を示すスライダ斜視図である。スライダ1は、アルミナとチタンカーバイドの焼結体に代表される材料の基板(ウエハ)部分1aと、基板上に薄膜プロセスで記録再生素子や配線パターンが形成され、アルミナなどの硬質保護膜で覆われた薄膜ヘッド部分1bから成る。
【0011】
スライダ1は長さ1.25mm、幅1.0mm、厚さ0.3mmのほぼ直方体形状をしており、浮上面9、空気流入端面12、空気流出端面13、両側の側面、背面の計6面から構成される。浮上面9にはイオンミリングやエッチングなどのプロセスによって微細な段差が設けられており、図示されていないディスク10と対向して空気圧力を発生し、背面に負荷される荷重を支える空気軸受の役目を果たしている。
【0012】
浮上面9には前記のように段差が設けられ、実質的に平行な4種類の面に分類される。最もディスクに近い素子設置面5、素子設置面より約5nm深い超浅溝面6、素子設置面より約150nm深いステップ軸受面である浅溝面7、素子設置面より約1μm深くなっている深溝面8の4種類である。なお、図示するように素子設置面5、超浅溝面6、浅溝面7はそれぞれ複数の構成要素5a、5b、5c、構成要素6a、6b、構成要素7a、7bに分割されている。浮上面の流出端側中央付近拡大図を図3に示す。また、空気流出端側から見た図を図4に示す。図4のD1、D2、D3はそれぞれ約5nm、約150nm、1μmである。
【0013】
磁気ディスク10が回転することで生じる空気流が、ステップ軸受である浅溝面7からレール面である素子設置面5、超浅溝面6へ進入する際に、先すぼまりの流路によって圧縮され、正の空気圧力を生じる。一方、レール面や浅溝面から深溝面8へ空気流が進入する際には流路の拡大によって、負の空気圧力が生じる。
【0014】
磁気ヘッドスライダ1は空気流入端12側の浮上量が空気流出端側13の浮上量より大きくなるような姿勢で浮上するように設計されている。従って流出端近傍の浮上面がディスク10に最も接近する。流出端近傍では、素子設置面5aが周囲の超浅溝面6a、6b、浅溝面7a、深溝面8に対して突出しているので、スライダピッチ姿勢およびロール姿勢が一定限度を超えて傾かない限り、素子設置面5aが最も磁気ディスク10に近づくことになる。磁気ヘッド(記録素子2および再生素子3から構成される)は、素子設置面5aの、薄膜ヘッド部分に形成されている。また少なくとも素子設置面5aは、記録再生素子の腐食を防ぐためにカーボン等の保護膜で被膜されている。
【0015】
素子設置面5と超浅溝面6の間の約5nmの段差形成方法は、約5nmの前記カーボン膜を酸素アッシング等の手段で除去することによって得るのが容易な方法である。
【0016】
超浅溝面6aおよび6bの、薄膜ヘッド部分には、薄膜抵抗体による加熱装置4a、4bが薄膜プロセスを用いて形成されている。加熱装置4a、4bは浮上面表面に露出している様子を示したが、浮上面表面から内部に一定の距離だけ離れていてもよい。薄膜抵抗体として本実施例では、材質がパーマロイ、厚さが0.5mm、幅が3μmの細線を、奥行き60μm、幅60μmの領域に蛇行させ、間隙はアルミナで埋めて発熱体を形成した。
【0017】
従来の技術に対する本実施例の特徴は、再生素子3から加熱装置4aまたは4bまでの距離Dが、0.1mm以上となっていることである。また、加熱装置4a、4bの位置(あるいは浮上面に投影した位置)が素子設置面5aではなく、超浅溝面6a、6bであることである。
【0018】
加熱装置の目的は、熱膨張変形によって記録再生素子と磁気ディスク間のスペーシングを調整し、前記浮上量マージンを無用化することである。近年、浮上量マージンは10nm以下で設計されているため、浮上量の変化量は最大10nmあれば十分である。熱膨張変形量と浮上量変化量との関係が1対1であると仮定すれば、熱膨張変形量も10nmあれば十分である。薄膜抵抗体からの発熱によるヘッド伝熱解析およびヘッド変形解析結果によれば、10nm熱膨張変形させるためには50mWの熱を薄膜抵抗体が発すればよい。その場合、10℃以上の温度上昇をするのは薄膜抵抗体の近傍だけであり、0.1mm離れた位置では温度上昇は限定されている。すなわち、加熱装置4を再生素子3から0.1mm以上離せば、再生素子の寿命に与える影響はごく限定され、信頼性の高い磁気ヘッドスライダを提供できる。なお、熱膨張変形量と浮上量変化量との関係は厳密には1対1ではないが、後で述べる浮上面設計の工夫によって、1対1に近づけることができる。
【0019】
次に図5を用い、使用環境の気圧差に起因する浮上量変動を補償する場合を例にとって、浮上量の調整原理を示す。図5のA図は低地条件におけるディスク10と記録再生素子2、3との位置関係を模式的に示したものである。低地条件での素子浮上量をH0とする。
【0020】
図5のB図は高地条件における位置関係を示す。高地で気圧が低い場合、同じ浮上量で比べると素子設置面5a等の浮上面で発生する空気圧力が小さくなり、同じ荷重で比べると浮上量は小さくなる。すなわち素子浮上量H1はH0より小さくなり、その差は現在の設計浮上量に比べて無視できない量である。低地でぎりぎり接触しない設計にすると高地ではディスクとスライダの接触が起こり、スライダ振動による記録再生エラー、サーマルアスペリティによる読み取りエラー、摩耗による素子ダメージなどを引き起こす。逆に高地でも接触しない設計をすると低地では高い浮上量で使わざるを得なくなり、記録密度を上げることができない。
【0021】
図5のC図は高地条件において本発明の磁気ヘッドスライダ構造によって加熱装置4a、4bに通電して超浅溝面6a、6bを熱膨張変形させた様子を示す。超浅溝面6a、6bで発生する空気圧力が増加することにより、高地で気圧が低くなった分を補償し、素子浮上量H2を元の素子浮上量H0と同等にすることができる。
【0022】
以上、気圧差起因の浮上量変動を補償する方法について説明したが、温度差起因の浮上量変動を補償する場合についても、記録素子の発熱による素子突出分をキャンセルする場合についても、またヘッド個体差による浮上量変動を調整する場合についても、同様である。
【0023】
従来の浮上量調整方法は、記録再生素子の近傍に加熱装置を置き、記録再生素子近傍だけ突出させて、通電によって浮上量を下げるやり方である。この方法の場合、高地で接触しないよう設計し、低地では浮上量が増える分、通電して突出させて浮上量を小さくすることになる。磁気ディスク装置の使用場所を考慮すると高地より低地の頻度が大きいため、通電する時間、あるいは大きな入力電力を要する時間が長くなり、消費電力が大きい。一方本発明の浮上量調整方法は、加熱装置付近の浮上面をディスクに近づけて浮上面面積を増やし、通電によって浮上量を上げるやり方である。この方法の場合、低地で接触しないよう設計し、高地では浮上量が減る分、通電して浮上量を大きくすることになる。高地で使用される頻度は(装置個別で見れば高地で使用される頻度の方が大きいものもあるが、機種全体で見れば)小さいため、要する消費電力は小さくて済む。
【0024】
次に浮上量の検知方法について述べる。気圧や温度を測るセンサを別途設ける方法もあるが、気圧、温度、個体差など全ての影響が入った状態で、接触が起こる(近すぎる)ことなく、かつ磁気情報の再生にエラーが起こる(遠すぎる)こともない、という2つの条件が満足されれば問題ないため、接触や再生エラーを監視してそれらが起こった時だけ加熱装置への入力電力を調整するフィードバック制御をするのが最も簡単な制御方法である。なお、ロードによる衝撃で素子が傷つくのを防ぐため、スライダをディスクにロードする時、特に装置起動時は、加熱装置に通電して浮上量を高くしておくのが有効である。
【0025】
装置起動時からの制御アルゴリズムを図9に示す。接触の検知方法については後述する。気圧差起因の浮上量変動およびヘッド個体差による浮上量変動を補償する方法については図示したように起動時のみでよいが、温度差起因の浮上量変動に関しては、規定の時間間隔毎に、あるいは使用中常に、接触および再生エラーを監視する必要がある。
【0026】
接触を検知する方法は、(1)アコースティックエミッション(AE)センサを用いる方法、(2)接触発熱によって再生信号に表れるノイズであるサーマルアスペリティを監視する方法、(3)接触摩擦力によってスライダがピボット回りに微小回転しオフトラックが起こるオフトラック信号を監視する方法、などがある。
【0027】
一方、磁気情報の再生エラーについてはいわゆるビットエラーレートを監視すればよい。再生エラーと違って記録エラーは監視するのが難しいが、記録時は記録素子のコイル発熱によって素子部が膨張して再生時より浮上量が低いのが一般的であるため、再生エラーが起こらない条件ならば記録エラーが起こる可能性も低い。
【0028】
また、浮上量調整に関わる別の方法としては、再生信号の振幅を用いて再生素子と媒体間の距離をその場観測する方法があり、これを応用することもできる。
【0029】
加熱装置4a、4bの位置(あるいは浮上面に投影した位置)が素子設置面5aではなく、超浅溝面6a、6bとなっている利点は、加熱装置4を加熱しない場合に、多少のロール姿勢があったとしても、浮上面の中で記録再生素子に極近い部分が最下点(ディスクに最も近い点)になることが保証できる点である。言い換えれば、最小浮上量位置における浮上量と記録再生素子位置における浮上量の差異が少なく、浮上量のロスが少ないということである。逆に素子設置面の流出端側エッジの幅が広い場合、最小浮上量位置と記録再生素子位置の距離が大きく、浮上量のロスが大きくなる。
【0030】
素子設置面の流出端側エッジの幅を狭く、30μmから60μm程度にすると、ディスクへの接近性能が良くなることが知られており、本実施例の構造はディスクへの接近性能向上の点からも有利である。
【0031】
図2乃至図5において超浅溝面6a、6bとした部分の高さを、素子設置面5aと同じにした場合、上記のように浮上量のロスが本実施例に比べて大きく、またディスクへの接近性能も向上しないものの、本発明の効果は同様に得られる。すなわち、再生素子3と加熱装置4の位置が0.1mm以上あるので再生素子寿命への影響は小さく、また通電によって浮上量が大きくなる方向の調整であるので、要する消費電力も小さい。
【0032】
前述した熱膨張変形量と浮上量変化量との関係は厳密には1対1ではないが、素子設置面の流出端側の幅をできるだけ小さくし、一方超浅溝面の幅をできるだけ大きくすると良い。言い換えれば、素子設置面で受け持つ荷重と超浅溝面で受け持つ荷重の比を調整し、素子設置面で受け持つ荷重の比率をできるだけ小さくすると、前記熱膨張変形量と浮上量変化量の関係を1対1に近づけることができる。図6に、素子設置面5aで受け持つ荷重の比率をできるだけ小さくした例を本発明の第二の実施例として図示する。素子設置面の面積をパラメータにして発生する圧力変化を解析した結果、素子設置面5aの面積は0.005平方mm以下にすると好適である。
【0033】
図7は本発明の第三の実施形態を示すスライダ斜視図の、流出端付近拡大図である。第一の実施例で示した番号と同じ番号は同じものを示している。本実施例と第一および第二の実施例との違いは、加熱装置4a、4bを設置した超浅溝面6a、6bが、素子設置面5aから離れ、浅溝面7aで隔てられている点である。このようにすると、加熱装置4a、4bから再生素子3までの距離Dが第一および第二の実施例と比べて大きくなり、再生素子が加熱されて寿命に影響する危険性が更に小さくなる。また、熱膨張によって変形するのが超浅溝面6a、6bだけに限定され、浅溝面で隔てられた素子設置面5aはほとんど動かないので、前述した熱膨張変形量と浮上量変化量の関係が1対1に近づく。素子設置面5aの面積はできるだけ小さく、0.005平方mm以下にすると好適である。
【0034】
図7において超浅溝面6a、6bとした部分の高さを、素子設置面5aと同じにした場合、浮上量のロスが本実施例に比べて大きく、またディスクへの接近性能も向上しないものの、本発明の効果は同様に得られる。
【0035】
図8は本発明の第四の実施形態を示すスライダ斜視図の、流出端付近拡大図である。第一の実施例で示した番号と同じ番号は同じものを示している。本実施例と第一乃至第三の実施例との違いは、加熱装置4a、4bを設置した超浅溝面6a、6bが、素子設置面5aから離れ、深溝面8で隔てられている点である。このようにすると、加熱装置4a、4bから再生素子3までの距離Dが第一乃至第三の実施例と比べて更に大きくなり、再生素子が加熱されて寿命に影響する危険性が一層小さくなる。また、熱膨張によって変形するのが超浅溝面6a、6bだけに限定され、浅溝面で隔てられた素子設置面5aはほとんど動かないので、前述した熱膨張変形量と浮上量変化量の関係が1対1に近づく。素子設置面5aの面積はできるだけ小さく、0.005平方mm以下にすると好適である。
【0036】
図8において超浅溝面6a、6bとした部分の高さを、素子設置面5aと同じにした場合、浮上量のロスが本実施例に比べて大きく、またディスクへの接近性能も向上しないものの、本発明の効果は同様に得られる。
【0037】
【発明の効果】
本発明の、第一に加熱装置である薄膜抵抗体を記録再生素子から十分離したこと、第二に抵抗体への通電にともなう浮上面一部の突出によって浮上面で発生する空気圧力が増加するように浮上面設計したこと、この二点により、再生素子の寿命に影響せず、要する消費電力が小さい浮上量調整が実現できる。その結果、ヘッド個体毎に、または使用環境に応じて浮上量を調整することによって浮上量マージンを廃することができ、スライダとディスクの接触は防ぎつつ記録再生素子の浮上量を大幅に縮め、磁気ディスク面記録密度の増大、更には装置の大容量化あるいは小型化に寄与する。
【図面の簡単な説明】
【図1】 本発明の磁気ヘッドスライダを搭載する磁気ディスク装置。
【図2】 本発明の第1実施例のスライダ。
【図3】 第1実施例のスライダ流出端付近拡大図。
【図4】 第1実施例のスライダを流出端側から見た図。
【図5】 第1実施例の浮上量調整メカニズム説明図。
【図6】 第2実施例のスライダ流出端付近拡大図。
【図7】 第3実施例のスライダ流出端付近拡大図。
【図8】 第4実施例のスライダ流出端付近拡大図。
【図9】 本発明の磁気ヘッドスライダ制御方法を示すフロー図。
【符号の説明】
1…磁気ヘッドスライダ、1a…スライダ基板部分、1b…スライダ薄膜ヘッド部分、2…記録素子、3…再生素子、4…加熱装置、5…素子設置面、5a、5b、5c…素子設置面構成要素、6…超浅溝面、6a,6b,6c、…超浅溝面構成要素、7…浅溝面、7a,7b…浅溝面構成要素、8…深溝面、9…浮上面、10…磁気ディスク、11…磁気ディスク装置、12…空気流入端面、13…空気流出端面、14…ランプ、D…再生素子と加熱装置の距離、D1…超浅溝面の素子設置面からの深さ、D2…浅溝面の素子設置面からの深さ、D3…深溝面の素子設置面からの深さ、H0…低地での素子浮上量、H1…高地で加熱しない場合の素子浮上量、H2…高地で加熱した場合の浮上量
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a magnetic head slider structure for realizing a high recording density of a magnetic disk device, and more particularly to a flying height adjustment slider having a function of adjusting a distance between a magnetic disk and a magnetic head.
[0002]
[Prior art]
The magnetic disk device has a rotating magnetic disk and a magnetic head slider (also referred to simply as a slider) mounted with a recording / reproducing element and supported by a load beam and positioned in the radial direction, and the slider relatively runs on the magnetic disk. The magnetic information recorded on the magnetic disk is read and written. The slider floats as an air-lubricated bearing by the wedge film effect of air so that the magnetic disk and the slider are not in direct solid contact. In order to increase the recording density of a magnetic disk device and increase the capacity or size of the device, it is effective to increase the linear recording density by reducing the distance between the slider and the magnetic disk, that is, the slider flying height. is there.
[0003]
Conventionally, in the design of the slider flying height, a flying height margin has been provided so that the slider and the disk do not come into contact with each other even in the worst conditions, with the expectation that the flying height will decrease due to processing variations, operating environment pressure differences, operating environment temperature differences, and the like. If a slider with a function to adjust the flying height according to the individual head or according to the usage environment is realized, the above margin can be eliminated, and the flying height of the recording / reproducing element is greatly increased while preventing contact between the slider and the disk. Can be shortened. For example, there has been proposed a slider structure in which a heating device composed of a thin film resistor is provided in the vicinity of a recording / reproducing element, and a part of the slider is heated as necessary to thermally expand and protrude to adjust the flying height of the recording / reproducing element. (For example, refer to Patent Document 1).
[Patent Document 1]
JP-A-5-20635 (page 3).
[0004]
[Problems to be solved by the invention]
First, there is a problem of the read element life. A reproducing element using the magnetoresistive effect (MR effect), which is currently in the mainstream, has a feature that it is weak against heat load and has a short life if exposed to a high temperature for a long time. The method disclosed in Japanese Patent Application Laid-Open No. 5-20635 is an effective flying height adjustment method. However, when it is applied to the current recording / reproducing element, the thin film resistor as a heating device is positioned very close to the recording / reproducing element. Therefore, there is a possibility that the life of the reproducing element is reduced by heating.
[0005]
Secondly, there is a problem of the flying height adjustment direction. Since the system disclosed in the publication is a system in which the recording / reproducing element portion is protruded by thermal expansion, the flying height is reduced by energization. Regarding the atmospheric pressure (operating altitude), the flying height tends to increase at high pressure (low altitude) where the pressure applied to the air bearing is large, and the flying height tends to decrease as the pressure decreases (high altitude). Therefore, it is necessary to design a floating surface that does not contact even at high altitudes, and to always lower the flying height by energizing in low altitudes. However, it is more frequently used in low altitudes than in high altitudes, so it was indicated in the same publication. The amount of power required for the flying height adjustment direction is larger than that for the opposite direction.
[0006]
In summary, the present invention aims to solve these two problems: reducing the thermal load on the reproducing element and developing an adjustment method in the direction of increasing the flying height by energization.
[0007]
[Means for Solving the Problems]
The above-mentioned problems are: firstly, the thin film resistor, which is a heating device, is sufficiently separated from the recording / reproducing element, and secondly, the air pressure generated on the air bearing surface increases due to a part of the air bearing surface protruding when the resistor is energized. Thus, designing the air bearing surface is solved by these two points.
Regarding the first point, the thin film resistor needs to be separated from the recording / reproducing element by 0.1 mm or more. When the recording / reproducing element is at the center of the air outflow end, a thin film resistor is preferably provided at least 0.1 mm apart on both sides of the recording / reproducing element near the outflow end.
Regarding the second point, the air bearing surface of the two-step step bearing slider currently widely used in the industry has three substantially parallel surfaces, that is, (1) a rail surface on which a recording / reproducing element is installed, (2 ) It is composed of a shallow groove surface that is a step bearing, and (3) a deep groove surface that is a negative pressure pocket, but in recent years, the rail surface is the uppermost surface (referred to as an element installation surface) on which a recording / reproducing element is installed, A three-step step bearing slider is newly proposed which is divided into two surfaces of a very shallow step bearing surface (referred to as an ultra-shallow groove surface) of about 5 nm to 50 nm, and the air bearing surface is composed of a total of four parallel surfaces. Yes. The three-step slider has a small and narrow element installation surface, and an ultra-shallow groove surface slightly lower than the element installation surface around it. It can be guaranteed that the distance is close and contributes to a low flying height of the recording / reproducing element. Further, even if the element installation surface is reduced, the super shallow groove surface generates air pressure and supports the load, so that the followability to the micro waviness of the disk is not impaired.
The thin film resistor is exposed to the surface of the air bearing surface or formed at a position having a certain distance in the normal direction from the air bearing surface. If the position where the thin film resistor is projected onto the air bearing surface is in or near the ultra-shallow groove surface area, the super-shallow groove surface will be on the disk side when the thin-film resistor is energized and heated to thermally expand the surroundings. When the air pressure generated on the ultra-shallow groove surface increases, the flying height of the entire slider and the flying height of the recording / reproducing element increase. That is, the flying height adjustment in a direction in which the flying height increases by energization.
By the means described so far, it is possible to realize the flying height adjustment with low power consumption without affecting the life of the reproducing element. As a result, the flying height margin can be eliminated by adjusting the flying height for each individual head or according to the usage environment, and the flying height of the recording / reproducing element is greatly reduced while preventing contact between the slider and the disk. This contributes to an increase in recording density on the magnetic disk surface, and further to an increase in capacity or size of the apparatus.
[0008]
DETAILED DESCRIPTION OF THE INVENTION
A magnetic head slider and a magnetic disk apparatus using the same according to an embodiment of the present invention will be described below with reference to the drawings.
[0009]
A schematic configuration of a magnetic disk apparatus according to an embodiment of the present invention is shown in FIG. The magnetic head slider 1 is equipped with a recording / reproducing element for recording / reproducing magnetic information. The magnetic disk 10 stores magnetic information and is rotated by a spindle motor. The magnetic head slider 1 is attached to a leaf spring-shaped load beam, and a pressing load is applied to the magnetic disk surface by the load beam, and seek operation is performed in the radial direction of the magnetic disk 10 by the voice coil motor together with the load beam. Recording and playback are performed on the entire magnetic disk surface. The magnetic head slider 1 is retracted from the magnetic disk 10 onto the ramp 14 when the apparatus is stopped or when there is no read / write command for a predetermined time.
Here, an apparatus having a load / unload mechanism is shown. However, even in a contact start / stop type magnetic disk apparatus in which the magnetic head slider 1 stands by in a specific area of the magnetic disk 10 while the apparatus is stopped. The effects of the invention can be obtained similarly.
[0010]
FIG. 2 is a perspective view of the slider showing the first embodiment of the present invention. The slider 1 has a substrate (wafer) portion 1a of a material typified by a sintered body of alumina and titanium carbide, a recording / reproducing element and a wiring pattern formed on the substrate by a thin film process, and covered with a hard protective film such as alumina. It consists of a thin film head portion 1b.
[0011]
The slider 1 has a substantially rectangular parallelepiped shape with a length of 1.25 mm, a width of 1.0 mm, and a thickness of 0.3 mm, and a total of 6 on the air bearing surface 9, the air inflow end surface 12, the air outflow end surface 13, both side surfaces, and the back surface. Consists of faces. The air bearing surface 9 is provided with fine steps by processes such as ion milling and etching, and functions as an air bearing that generates air pressure opposite to the disk 10 (not shown) and supports the load applied to the back surface. Plays.
[0012]
The air bearing surface 9 is provided with a step as described above, and is classified into four types of substantially parallel surfaces. The element mounting surface 5 closest to the disk, the ultra-shallow groove surface 6 that is approximately 5 nm deeper than the element mounting surface, the shallow groove surface 7 that is a step bearing surface approximately 150 nm deeper than the element mounting surface, and the deep groove that is approximately 1 μm deeper than the element mounting surface There are four types of surface 8. As shown in the figure, the element installation surface 5, the ultra shallow groove surface 6, and the shallow groove surface 7 are divided into a plurality of components 5a, 5b, 5c, components 6a, 6b, and components 7a, 7b, respectively. FIG. 3 shows an enlarged view of the vicinity of the center on the outflow end side of the air bearing surface. Moreover, the figure seen from the air outflow end side is shown in FIG. In FIG. 4, D1, D2, and D3 are about 5 nm, about 150 nm, and 1 μm, respectively.
[0013]
When the air flow generated by the rotation of the magnetic disk 10 enters from the shallow groove surface 7 which is a step bearing into the element installation surface 5 which is a rail surface and the super shallow groove surface 6, the flow path is tapered. Compressed, producing positive air pressure. On the other hand, when the air flow enters the deep groove surface 8 from the rail surface or the shallow groove surface, a negative air pressure is generated due to the expansion of the flow path.
[0014]
The magnetic head slider 1 is designed to fly in such a posture that the flying height on the air inflow end 12 side is larger than the flying height on the air outflow end side 13. Therefore, the air bearing surface near the outflow end is closest to the disk 10. In the vicinity of the outflow end, the element installation surface 5a protrudes from the surrounding super shallow groove surfaces 6a, 6b, shallow groove surface 7a, and deep groove surface 8, so that the slider pitch posture and the roll posture do not tilt beyond a certain limit. As long as the element mounting surface 5 a is closest to the magnetic disk 10. The magnetic head (consisting of the recording element 2 and the reproducing element 3) is formed on the thin film head portion of the element installation surface 5a. At least the element installation surface 5a is coated with a protective film such as carbon in order to prevent corrosion of the recording / reproducing element.
[0015]
The method of forming a step of about 5 nm between the element installation surface 5 and the ultra-shallow groove surface 6 is an easy method to obtain by removing the carbon film of about 5 nm by means such as oxygen ashing.
[0016]
On the thin film head portions of the ultra-shallow groove surfaces 6a and 6b, heating devices 4a and 4b using thin film resistors are formed using a thin film process. Although the heating devices 4a and 4b have been shown to be exposed on the air bearing surface, they may be separated from the air bearing surface by a certain distance. In this embodiment, the thin film resistor was made of a permalloy material, a thickness of 0.5 mm, and a width of 3 μm meandering in a region having a depth of 60 μm and a width of 60 μm, and the gap was filled with alumina to form a heating element.
[0017]
The feature of this embodiment over the prior art is that the distance D from the reproducing element 3 to the heating device 4a or 4b is 0.1 mm or more. Further, the positions of the heating devices 4a and 4b (or the positions projected on the air bearing surface) are not the element installation surface 5a but the ultra-shallow groove surfaces 6a and 6b.
[0018]
The purpose of the heating device is to adjust the spacing between the recording / reproducing element and the magnetic disk by thermal expansion and deformation, thereby eliminating the flying height margin. In recent years, since the flying height margin is designed to be 10 nm or less, it is sufficient that the flying height change amount is 10 nm at the maximum. Assuming that the relationship between the thermal expansion deformation amount and the flying height change amount is 1: 1, it is sufficient that the thermal expansion deformation amount is also 10 nm. According to the results of head heat transfer analysis and head deformation analysis due to heat generation from the thin film resistor, the thin film resistor only needs to generate 50 mW of heat in order to undergo thermal expansion deformation of 10 nm. In that case, the temperature rise of 10 ° C. or more is only in the vicinity of the thin film resistor, and the temperature rise is limited at a position 0.1 mm away. That is, if the heating device 4 is separated from the reproducing element 3 by 0.1 mm or more, the influence on the life of the reproducing element is very limited, and a highly reliable magnetic head slider can be provided. Strictly speaking, the relationship between the amount of thermal expansion deformation and the amount of change in flying height is not 1: 1, but it can be made closer to 1: 1 by devising the floating surface design described later.
[0019]
Next, the principle of adjusting the flying height will be described with reference to FIG. 5, taking as an example the case of compensating for the flying height fluctuation caused by the atmospheric pressure difference in the usage environment. FIG. 5A schematically shows the positional relationship between the disk 10 and the recording / reproducing elements 2 and 3 under the lowland condition. Let H0 be the flying height of the element under low-land conditions.
[0020]
FIG. 5B shows the positional relationship under high altitude conditions. When the atmospheric pressure is low at a high altitude, the air pressure generated on the floating surface such as the element installation surface 5a becomes smaller when compared with the same flying height, and the flying height becomes smaller when compared with the same load. That is, the element flying height H1 is smaller than H0, and the difference is an amount that cannot be ignored compared to the current design flying height. If the design is such that there is no marginal contact at low altitudes, contact between the disk and slider occurs at high altitudes, causing read / write errors due to slider vibration, read errors due to thermal asperity, and element damage due to wear. Conversely, if the design is such that it does not contact even at high altitudes, it must be used with a high flying height at low altitudes, and the recording density cannot be increased.
[0021]
FIG. 5C shows a state in which the heating devices 4a and 4b are energized and the super-shallow groove surfaces 6a and 6b are thermally expanded and deformed by the magnetic head slider structure of the present invention under high altitude conditions. By increasing the air pressure generated in the ultra-shallow groove surfaces 6a and 6b, it is possible to compensate for the lowering of the atmospheric pressure at high altitude, and to make the element flying height H2 equal to the original element flying height H0.
[0022]
Although the method for compensating for the flying height variation caused by the pressure difference has been described above, the case where the flying height variation caused by the temperature difference is compensated, the case where the element protrusion due to the heat generation of the recording element is canceled, and the individual head are also described. The same applies when adjusting the flying height fluctuation due to the difference.
[0023]
A conventional flying height adjustment method is a method in which a heating device is placed in the vicinity of the recording / reproducing element, and only the vicinity of the recording / reproducing element is projected to lower the flying height by energization. In the case of this method, it is designed not to contact at high altitude, and the flying height is reduced by energizing and projecting by the amount of increase in the flying height at low altitude. Considering the place where the magnetic disk device is used, since the frequency of the lowland is higher than the highland, the time for energization or the time required for large input power becomes long, and the power consumption is large. On the other hand, the flying height adjustment method of the present invention is a method of increasing the flying height by energization by increasing the flying surface area by bringing the flying surface near the heating device closer to the disk. In the case of this method, it is designed not to contact in the lowland, and the flying height is increased by energizing as the flying height decreases in the highland. Since the frequency of use at high altitudes is small (in terms of individual devices, although the frequency of use at high altitudes is higher for all devices), it requires less power consumption.
[0024]
Next, a method for detecting the flying height will be described. There is also a method of separately providing sensors for measuring atmospheric pressure and temperature, but in the state where all influences such as atmospheric pressure, temperature, individual differences are included, contact does not occur (too close) and an error occurs in reproduction of magnetic information ( If the two conditions are satisfied, it is best to monitor the contact and regeneration errors and perform feedback control to adjust the input power to the heating device only when they occur. It is a simple control method. In order to prevent the element from being damaged by the impact due to the load, it is effective to increase the flying height by energizing the heating device when the slider is loaded on the disk, especially when the apparatus is activated.
[0025]
FIG. 9 shows a control algorithm from when the apparatus is activated. A contact detection method will be described later. As shown in the figure, the method of compensating for the flying height fluctuation caused by the atmospheric pressure difference and the flying height fluctuation caused by the individual head difference is only required at the time of start-up. It is necessary to monitor contact and regeneration errors at all times during use.
[0026]
The method for detecting contact includes (1) a method using an acoustic emission (AE) sensor, (2) a method for monitoring thermal asperity, which is noise that appears in a reproduction signal due to contact heat generation, and (3) a slider pivoting by contact frictional force. For example, there is a method of monitoring an off-track signal in which a slight rotation occurs and off-track occurs.
[0027]
On the other hand, what is necessary is just to monitor what is called a bit error rate about the reproduction | regeneration error of magnetic information. Unlike playback errors, recording errors are difficult to monitor, but during recording, the element part expands due to coil heat generation of the recording element and the flying height is generally lower than during playback, so playback errors do not occur If the condition is met, the possibility of a recording error is low.
[0028]
In addition, as another method for adjusting the flying height, there is a method of in-situ observation of the distance between the reproducing element and the medium using the amplitude of the reproducing signal, which can be applied.
[0029]
The advantage that the positions of the heating devices 4a and 4b (or the positions projected onto the air bearing surface) are not the element installation surface 5a but the ultra-shallow groove surfaces 6a and 6b is that when the heating device 4 is not heated, some rolls Even if there is an attitude, it is possible to guarantee that the portion of the air bearing surface that is very close to the recording / reproducing element is the lowest point (the point that is closest to the disk). In other words, there is little difference between the flying height at the minimum flying height position and the flying height at the recording / reproducing element position, and the flying height loss is small. Conversely, when the width of the edge on the outflow end side of the element installation surface is wide, the distance between the minimum flying height position and the recording / reproducing element position is large, and the flying height loss increases.
[0030]
It is known that when the width of the edge on the outflow end side of the element installation surface is narrowed to about 30 μm to 60 μm, the access performance to the disk is improved, and the structure of this embodiment is from the point of improving the access performance to the disk. Is also advantageous.
[0031]
When the heights of the super shallow groove surfaces 6a and 6b in FIGS. 2 to 5 are the same as those of the element installation surface 5a, the flying height loss is larger as compared with the present embodiment as described above, and the disk The effect of the present invention can be obtained in the same manner, although the approaching performance to is not improved. That is, since the position of the reproducing element 3 and the heating device 4 is 0.1 mm or more, the influence on the life of the reproducing element is small, and the adjustment is made in the direction in which the flying height is increased by energization, and thus the required power consumption is small.
[0032]
Strictly speaking, the relationship between the amount of thermal expansion deformation and the amount of change in flying height is not 1: 1, but if the width of the outflow end side of the element installation surface is made as small as possible, while the width of the ultra-shallow groove surface is made as large as possible. good. In other words, if the ratio of the load on the element installation surface to the load on the ultra-shallow groove surface is adjusted and the ratio of the load on the element installation surface is made as small as possible, the relationship between the thermal expansion deformation amount and the flying height change amount is 1 Can be close to one-on-one. FIG. 6 shows an example in which the ratio of the load on the element installation surface 5a is made as small as possible as the second embodiment of the present invention. As a result of analyzing the pressure change generated by using the area of the element installation surface as a parameter, the area of the element installation surface 5a is preferably 0.005 square mm or less.
[0033]
FIG. 7 is an enlarged view of the vicinity of the outflow end of the slider perspective view showing the third embodiment of the present invention. The same numbers as those shown in the first embodiment are the same. The difference between the present embodiment and the first and second embodiments is that the ultra-shallow groove surfaces 6a and 6b provided with the heating devices 4a and 4b are separated from the element installation surface 5a and separated by the shallow groove surface 7a. Is a point. In this way, the distance D from the heating devices 4a, 4b to the reproducing element 3 becomes larger than in the first and second embodiments, and the risk that the reproducing element is heated and affects the life is further reduced. Further, the deformation due to the thermal expansion is limited to the super-shallow groove surfaces 6a and 6b, and the element installation surface 5a separated by the shallow groove surface hardly moves. Therefore, the above-described thermal expansion deformation amount and flying height change amount The relationship approaches one to one. The area of the element installation surface 5a is as small as possible and is preferably 0.005 square mm or less.
[0034]
In the case where the heights of the super shallow groove surfaces 6a and 6b in FIG. 7 are the same as those of the element installation surface 5a, the flying height loss is larger than that of the present embodiment, and the performance of accessing the disk is not improved. However, the effects of the present invention can be obtained similarly.
[0035]
FIG. 8 is an enlarged view of the vicinity of the outflow end of the slider perspective view showing the fourth embodiment of the present invention. The same numbers as those shown in the first embodiment are the same. The difference between the present embodiment and the first to third embodiments is that the ultra-shallow groove surfaces 6a and 6b provided with the heating devices 4a and 4b are separated from the element installation surface 5a and separated by the deep groove surface 8. It is. In this way, the distance D from the heating devices 4a, 4b to the reproducing element 3 is further increased as compared with the first to third embodiments, and the risk that the reproducing element is heated and affects the life is further reduced. . Further, the deformation due to thermal expansion is limited only to the super-shallow groove surfaces 6a and 6b, and the element installation surface 5a separated by the shallow groove surface hardly moves. The relationship approaches one to one. The area of the element installation surface 5a is as small as possible and is preferably 0.005 square mm or less.
[0036]
In FIG. 8, when the height of the super shallow groove surfaces 6a and 6b is the same as that of the element installation surface 5a, the flying height loss is larger than that of the present embodiment, and the access performance to the disk is not improved. However, the effects of the present invention can be obtained similarly.
[0037]
【The invention's effect】
In the present invention, firstly, the thin film resistor, which is a heating device, is sufficiently separated from the recording / reproducing element, and secondly, the air pressure generated on the air bearing surface increases due to the protrusion of the air bearing surface partly due to energization of the resistor. By designing the air bearing surface as described above, it is possible to realize a flying height adjustment that requires less power consumption without affecting the life of the reproducing element. As a result, the flying height margin can be eliminated by adjusting the flying height for each individual head or according to the usage environment, and the flying height of the recording / reproducing element is greatly reduced while preventing contact between the slider and the disk. This contributes to an increase in recording density on the magnetic disk surface, and further to an increase in capacity or size of the apparatus.
[Brief description of the drawings]
FIG. 1 shows a magnetic disk drive equipped with a magnetic head slider of the present invention.
FIG. 2 is a slider according to a first embodiment of the present invention.
FIG. 3 is an enlarged view of the vicinity of the slider outflow end of the first embodiment.
FIG. 4 is a diagram of the slider of the first embodiment viewed from the outflow end side.
FIG. 5 is an explanatory diagram of a flying height adjustment mechanism according to the first embodiment.
FIG. 6 is an enlarged view of the vicinity of the slider outflow end of the second embodiment.
FIG. 7 is an enlarged view of the vicinity of the slider outflow end of the third embodiment.
FIG. 8 is an enlarged view of the vicinity of a slider outflow end according to a fourth embodiment.
FIG. 9 is a flowchart showing a magnetic head slider control method of the present invention.
[Explanation of symbols]
DESCRIPTION OF SYMBOLS 1 ... Magnetic head slider, 1a ... Slider board | substrate part, 1b ... Slider thin film head part, 2 ... Recording element, 3 ... Reproducing element, 4 ... Heating device, 5 ... Element installation surface, 5a, 5b, 5c ... Element installation surface structure Element 6 ... Ultra-shallow groove surface, 6a, 6b, 6c, Ultra-shallow groove surface component, 7 ... Shallow groove surface, 7a, 7b ... Shallow groove surface component, 8 ... Deep groove surface, 9 ... Air bearing surface, 10 DESCRIPTION OF SYMBOLS ... Magnetic disk, 11 ... Magnetic disk apparatus, 12 ... Air inflow end surface, 13 ... Air outflow end surface, 14 ... Lamp, D ... Distance between reproduction | regeneration element and heating apparatus, D1 ... Depth from element installation surface of ultra shallow groove surface D2: Depth of shallow groove surface from element installation surface, D3: Depth of deep groove surface from element installation surface, H0: Element flying height in low altitude, H1: Element flying height when not heating in high altitude, H2 ... Floating height when heated at high altitude

Claims (5)

回転する磁気ディスクと対向する空気軸受面と、前記磁気ディスクに情報を記録する記録素子及び前記磁気ディスクから情報を再生する再生素子と、これらの素子と前記磁気ディスク面との距離を熱膨張によって調整する加熱装置とを有する磁気ヘッドスライダにおいて、
前記空気軸受面は、前記記録素子及び再生素子が設置された第一の面と、この第一の面から所定の深さを有する第二の面と、この第二の面から所定の深さを有する第三の面とを備え、
前記加熱装置を前記空気軸受面に投影した位置が、前記記録再生素子が設置された部分とは前記第二の面或いは前記第三の面で隔てられている磁気ヘッドスライダ。
An air bearing surface facing the magnetic disk rotates, the reproducing device for reproducing information from the recording element and the magnetic disk for recording information on the magnetic disk, the thermal expansion of the distance between these elements the magnetic disk surface in the magnetic head slider and a tO aDJUST pressurized thermal device,
The air bearing surface, the recording element and the first surface reproducing device is installed, a second surface and a predetermined depth from the second surface having a predetermined depth from the first surface A third surface having
The projection position of the heating device to the air bearing surface, the write element and the installation portion said second surface or magnetic head slider that has been separated by said third face.
基板部と、この基板部上に形成された記録素子及び再生素子並びに加熱装置を有するヘッド部とを備えた磁気ヘッドスライダにおいて、
前記ヘッド部は、前記記録素子及び再生素子が設置された第一の面と、この第一の面から所定の深さを有する第二の面とを備え
前記加熱装置を前記ヘッド部の空気軸受面に投影した位置が、前記第二の面内のみにある磁気ヘッドスライダ。
A substrate portion, the magnetic head slider and a head portion having a recording element and a reproducing element and heating equipment formed in the substrate portion on,
The head portion includes a first surface on which the recording element and the reproducing element are installed, and a second surface having a predetermined depth from the first surface ,
Wherein a heating device is projected to the air bearing surface of the head portion position, magnetic head slider only on the second plane.
前記第二の面の一部分の、前記第一の面からの深さが、前記加熱装置の作用によって縮まる請求項1または2に記載の磁気ヘッドスライダ。Wherein a portion of the second surface, the depth from the first surface is a magnetic head slider according to Motomeko 1 or 2 that shrink by the action of the heating device. 記記素子及び再生素子が設置されたパッドの面積が0.005平方mm以下である請求項1乃至3のいずれか1項に記載の磁気ヘッドスライダ。The magnetic head slider according to any preceding one of crisis recording element and a reproducing element the installed area of the pad is Ru der 0.005 square mm Motomeko 1 to 3. 請求項1乃至4記載の磁気ヘッドスライダを備えた磁気ディスク装置。  A magnetic disk drive comprising the magnetic head slider according to claim 1.
JP2003031841A 2003-02-10 2003-02-10 Magnetic head slider and magnetic disk apparatus Expired - Fee Related JP4038437B2 (en)

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JP2006190374A (en) 2005-01-05 2006-07-20 Hitachi Global Storage Technologies Netherlands Bv Method for setting energization amount of heater provided in magnetoresistive head and magnetic disk device
JP2007141325A (en) 2005-11-16 2007-06-07 Alps Electric Co Ltd Contact type thin-film magnetic head
US7593188B2 (en) 2006-03-31 2009-09-22 Hitachi Global Storage Technologies Netherlands, B.V. Low protrusion compensation air bearing
JP2007293948A (en) 2006-04-21 2007-11-08 Fujitsu Ltd Information recording / reproducing apparatus, head flying height control method, head flying control circuit
JP2008090888A (en) 2006-09-29 2008-04-17 Hitachi Global Storage Technologies Netherlands Bv Magnetic head slider and magnetic disk device
JP5318428B2 (en) 2008-01-11 2013-10-16 株式会社日立製作所 Magnetic head slider and magnetic disk device
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