JP3842509B2 - Thin film magnetic head - Google Patents

Thin film magnetic head Download PDF

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Publication number
JP3842509B2
JP3842509B2 JP2000022066A JP2000022066A JP3842509B2 JP 3842509 B2 JP3842509 B2 JP 3842509B2 JP 2000022066 A JP2000022066 A JP 2000022066A JP 2000022066 A JP2000022066 A JP 2000022066A JP 3842509 B2 JP3842509 B2 JP 3842509B2
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Prior art keywords
pole
magnetic
magnetic pole
recording
yoke
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JP2001216610A (en
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正文 望月
千春 三俣
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Alps Alpine Co Ltd
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Alps Electric Co Ltd
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Description

【0001】
【発明の属する技術分野】
本発明は記録・再生分離の磁気ヘッドに係り、特に高密度高周波ディジタル記録を可能にする薄膜磁気ヘッドに関わる。
【0002】
【従来の技術】
近年、磁気記録装置の記録密度の向上は著しく、計算機用の磁気ディスク装置の分野では、記録密度の増加が年率100%以上の割合で進んでいる。1平方インチあたり数Gbから数10Gb以上の記録密度を達成するために、再生用の磁気ヘッド(以下、再生ヘッドと称す)として、従来のインダクティブ型よりも格段に再生出力の高い磁気抵抗及び巨大磁気抵抗効果素子(以下、MR素子と称す)を用いたMRヘッドが実用化されている。一方、記録用の磁気ヘッド(以下、記録ヘッドと称す)には、従来の電磁誘導現象を利用したインダクティブ型の薄膜ヘッドが用いられている。現実には、この再生ヘッドと記録ヘッドを一体に組み合わせたMR複合薄膜磁気ヘッドが用いられている。以下、このMR複合薄膜磁気ヘッドを薄膜磁気ヘッドと称する。
【0003】
図8は現在用いられている薄膜磁気ヘッドの構造を示している。基板1の上に、下部シールド2、絶縁層3、中部磁極4が形成され、下部シールド2と中部磁極4の間に、MR素子5が構成されている。ここで中部磁極4はシールドとしての機能も備える。中部磁極4の上に記録ギャップ膜6が形成され、さらに薄膜コイル7が形成されている。薄膜コイルを絶縁するために絶縁層8が形成され、さらに上部磁極(ポールチップ9a、ヨーク9b)が形成され最上層にこれらを保護するための保護層10が形成されている。記録トラック幅1ミクロン以下のヘッドにおいて上部磁極を2つの部分から製造することが有効であることが特開平11−213331に示されている。この薄膜磁気ヘッドは、薄膜コイル7に記録電流を印加して上部磁極9と中部磁極4に記録磁束を誘起して、記録ギャップ近傍で上部磁極9と中部磁極4からの漏洩磁界により、エアベアリング面11の近傍に設置した記録媒体に磁化パターンを記録する。再生は記録媒体の磁化パターンから発生する磁界をMR素子で検出する。
【0004】
【発明が解決しようとする課題】
磁気ディスク装置の分野では、高密度、高周波化が進んでいる。周波数が高くなった場合には、必要な記録信号の変化に、磁極の磁束変化が追従できず記録磁界の立ち上がり時間に遅れが生じる。この遅延は、オーバーライト特性(O/W)や非線型磁化遷移点シフト(Non Linear TransitionShift;NLTS)などの記録再生特性が劣化するという問題がある。必要な記録信号の変化に、いかに磁極の磁束変化を追従させるかということが、従来技術の解決すべき課題である。本発明の目的は、この問題点を抑制した薄膜磁気ヘッドを提供することにある。
【0005】
【課題を解決するための手段】
本発明の薄膜磁気ヘッドは、下部シールドと中部磁極の間に読み取り用の磁気抵抗効果素子を有し、非磁性材料よりなるギャップ層を挟んで前記中部磁極と対向する上部磁極を有し、前記上部磁極はポールチップとヨークで構成され、前記ポールチップのギャップ層側の幅が記録トラック幅を規定する幅であり、前記ポールチップの端面が前記中部磁極の端面とともにエアベアリング面を構成し、前記ヨークは前記ポールチップと前記中部磁極の間に設けられ、前記ヨークと中部磁極と接合する面はバックコンタクト面であり、前記ヨークの中部磁極と接合する部分はバックヨークであり、前記エアベアリング面において磁気記録媒体に対する書き込み用の磁束を発生させるように中部磁極と上部磁極の間に薄膜コイルを有し、前記バックヨークと接する部分の前記中部磁極の膜厚を前記エアベアリング面付近の中部磁極の膜厚以下にしたことを特徴とする。
【0006】
次に、本発明の作用について説明する。本発明は磁気ヘッドの磁路内に発生する渦電流損失を小さくすることにより記録信号の変化に対する磁極の磁束変化の遅れ時間が小さくできる点に着目している。
【0007】
しかし、磁気記録装置の高記録密度化に伴い、記録磁極のトラック幅を1mm以下の寸法となるように狭トラック化が進んでいる。単一の上部磁極を形成使用とするとプロセス的には従来構造では困難になってきている。上部磁極を二つの部分に分けて製造する方法が有利である。その場合、中部磁極とヨークが接する面S1(以下、バックコンタクト面と称す)に接するバックヨーク9cの体積が増加してしまう。そのため、渦電流損失が大きくなってしまう。磁気記録ヘッドはエアベアリング面付近の磁極先端の絞り部分以外の磁路の断面積φの積が等しいことが望ましい。しかし、プロセス上の問題から、バックコンタクト面S1の面積のみ大きくなっている。そこで、この点を考慮して、記録磁界強度を減少させることなしに必要な記録信号の変化に、磁極の磁束変化を追従させることを目的とした。
【0008】
まず、我々は、バックヨーク9cの体積の記録磁界強度、磁界立ち上がり時間への影響を検討した。バックヨーク9cの体積を小さくすることにより記録磁界強度を減少させることなしに、記録磁界の立ち上がり時間を小さくできることを見出した。この原因は、渦電流損失を小さくできたためである。また、バックヨークに隣接するサイドヨーク9dの体積を減少させても記録磁界強度に影響はない。そこで、記録磁界を減少させることなく、磁気ヘッドの渦電流損失を減少させ、必要な記録信号の変化に、磁極の磁束変化が追従させることをはかった。
【0009】
【発明の実施の形態】
1は、記録磁界の立ち上がりの改善を説明するグラフである。図2および図5は参考例の薄膜磁気ヘッドの断面図である。
【0010】
参考例)図1に、本形態と従来例の薄膜磁気ヘッドの記録磁界の立ち上がり特性を示す。同図中、本形態の薄膜磁気ヘッドは図2の構成とした。図1に示すように、従来の構成に比べて本発明の構成は記録磁界の立ち上がりが早い。したがって、本形態によれば記録磁界を減少させることなく、必要な記録信号の変化に対する磁極の磁束変化の遅れを減少させることができる。
【0011】
図2の薄膜磁気ヘッドはバックコンタクト面S1からポールチップ9aのギャップ膜6と接する面の反対側の上端面S2までの距離L1よりバックコンタクト面S1からバックヨーク9cのバックコンタクト面S1と接する反対側の面S3までの距離L2を小さく構成する。これにより、バックコンタクト面上で増加する磁路の面積の増加を減少させることができる。積層の順序を説明する。まず、絶縁膜を被覆したアルミナチタンカーバイド基板1の上に、NiFe合金の下部シールド2と、アルミナ膜とMR素子5とアルミナ膜と、中部磁極層4を積層して構成する。前記MR素子5を挟むアルミナ膜同士は再生ギャップとして機能する絶縁層3を構成する。次に中部磁極4の上に記録ギャップ膜6を形成したのち、ポールチップ9aを構成する。次に、絶縁層である例えばアルミナ膜を形成後、全体をCMP(Chemical Mecanical Polish)にて平坦化する。その後、薄膜コイル7同士の隙間を埋めるレジストの絶縁層8と、ヨーク9bを形成した。ヨーク9bは、その中央部で薄膜コイルを覆い、その後部で中部磁極4と接合させる。この接合面をバックコンタクト面S1という。つぎに、このヨーク9bのバックコンタクト面S1上の部分であるバックヨーク9cの面S3をイオンミリング等のイオンビームエッチングで削っていき、ポールチップ9aの上面S2より下にする。その後、このポールチップ9a及びヨーク9bの上には保護膜10を被覆する。各々の膜を適宜の形状・厚さの成膜・パターニングしながら上述の積層構造と作製する。この積層構造において、記録ギャップ膜および再生素子5のある側は、研磨して媒体対向面(エアベアリング面)11を形成する。中部磁極は、例えばNi濃度83wt%のNiFe合金で構成する。
【0012】
参考例)また、3に示すように、このバックヨーク9cの大部分をイオンミリング等のイオンビームエッチングで削除し、バックヨーク9cの中部磁極と接する面の断面の長さL3がヨーク9bの膜厚t9b以下になるように形成した。これにより、バックコンタクト面S1上で増加する磁路の面積の増加を減少することができる。
【0013】
参考例)また、のヘッドを図4に示した。図4(a)は上部磁極の平面図であり、図4(b)は図4(a)の4Aから4A’における断面図である。図4に示すように、の磁気ヘッドは、バックヨーク9cとサイドヨーク9dを含む点線で囲った領域A1を削除し、それらの体積がヨーク9b作成時点より少なく作成した。さらに、バックコンタクト面S1下の中部磁極を同時に削除しても良い。
【0014】
参考例)また、5に示すように、の磁気ヘッドは、バックヨーク9cとサイドヨーク9dをイオンミリング等のイオンビームエッチングで削除し、バックヨーク9cの中部磁極と接する面の断面の長さL3がヨーク9bの膜厚t9b以下に形成した。さらに、バックコンタクト面S1下の中部磁極4bを同時に削除するか、あらかじめバックコンタクト面S1下の中部磁極4bがないように中部磁極を形成しても良い。
【0015】
(実施形態)また、本実施形態では図6に示すようにバックコンタクト面S1下の中部磁極4bの膜厚t4bを、エアベアリング面付近の中部磁極4の膜厚t4より薄く作成した。場合によっては、t4bを0としてもよい。
【0016】
いずれの態も、発生記録磁界強度を減少させないよう、磁束の流れる磁路の断面積を減少させ、渦電流を抑制して、必要な記録信号の変化に対する磁極の磁束変化の遅れを減少させ、オーバーライト特性(O/W)や非線型磁化遷移点シフト(NLTS)などの記録再生特性の劣化を抑制して、高密度・高周波記録を実現できる薄膜磁気ヘッドを提供できる。
【0017】
(実施形態)次に、本発明の一実施形態に係る薄膜磁気ヘッドの製造工程の要部を図7で説明する。図6は、図7の製造工程で上部磁極を形成した薄膜磁気ヘッドである。アルミナチタンカーバイドからなる非磁性の基板1の上にアルミナの絶縁膜1aをスパッタで成膜する(2−a)。絶縁膜1aの上にCoTaZrの軟磁性膜をスパッタで成膜し、必要な形状にこの軟磁性膜をパターニングして、下部シールド2を得る。次に下部シールド2の上にアルミナの絶縁層3とMR素子5を形成する(2−b)。中部磁極を短くするための絶縁層3aを作製する。絶縁層3の上に、絶縁層3aと同一平面を構成するようにしてに中部磁極4を形成し、つづけて中部磁極4と絶縁層3aの上に中部磁極4を延長して形成する。次に記録ギャップ膜6を形成する(2−d)。その後、実施形態と同様の後工程を実施することにより、図6の断面図に示す薄膜磁気ヘッドを得る。
【0018】
上記の本実施形態の薄膜磁気ヘッドにおいて、MR素子には次に挙げるものを用いることができる。例えば、磁気抵抗効果膜とスペーサとSAL膜を備えるSALバイアス型MR素子、反強磁性膜を接合した軟磁性膜と非磁性金属膜と軟磁性膜を備えるスピンバルブ型MR素子、複数の軟磁性膜を積層した構成を備えるGMR素子、2つの軟磁性膜で絶縁膜を挟む構成を備えたトンネル接合型MR素子等である。これらの再生素子の再生トラック幅は、薄膜磁気ヘッドの上部磁極先端の幅(記録トラック幅)以下の大きさにすることが好ましい。
【0019】
【発明の効果】
以上述べてきたように、本発明によればバックコンタクト部分の体積を減少させる事により、必要な記録信号の変化に対する磁極の磁束変化の遅れを減少させ、オーバーライト特性(O/W)や非線型磁化遷移点シフト(NLTS)などの記録再生特性の劣化を抑制して、高密度・高周波記録を実現できる薄膜磁気ヘッドを提供できる。
【図面の簡単な説明】
【図1】図2の形態による記録磁界の立ち上がり特性を示すグラフ。
【図2】参考例の薄膜磁気ヘッドの断面図。
【図3】参考例の薄膜磁気ヘッドの断面図。
【図4】参考例の薄膜磁気ヘッドの断面図。
【図5】参考例の薄膜磁気ヘッドの断面図。
【図6】本発明の一実施形態の薄膜磁気ヘッドの断面図。
【図7】本発明の一実施形態の製法を説明する工程図。
【図8】従来の薄膜磁気ヘッドの断面図。
【符号の説明】
1 基板、
1a 絶縁膜、
2 下部シールド、
3 絶縁層、
4 中部磁極、
4b バックヨークと接する中部磁極、
5 再生素子、
6 記録ギャップ膜、
7 薄膜コイル、
8 絶縁層、
9a ポールチップ、
9b ヨーク、
9c バックヨーク、
9d サイドヨーク、
10 保護膜、
11 エアベアリング面、
S1 バックコンタクト面、
S2 ポールチップのギャップ膜と接する反対側の面、
S3 バックヨークのバックコンタクト面と反対側の面、
L1 S1とS2の距離、
L2 S1とS3の距離、
L3 バックコンタクト面の辺の長さ、
t4 中部磁極のエアベアリング面付近の膜厚
t4b バックコンタクト面に接する中部磁極の膜厚
t9b ヨークの膜厚
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a recording / reproducing separated magnetic head, and more particularly to a thin film magnetic head that enables high-density high-frequency digital recording.
[0002]
[Prior art]
In recent years, the recording density of magnetic recording devices has been remarkably improved, and in the field of computer magnetic disk devices, the recording density has been increasing at an annual rate of 100% or more. In order to achieve a recording density of several Gb to several tens of Gb per square inch, as a magnetic head for reproduction (hereinafter referred to as “reproduction head”), a magnetic resistance and a huge regenerative power much higher than those of the conventional inductive type An MR head using a magnetoresistive element (hereinafter referred to as an MR element) has been put into practical use. On the other hand, an inductive thin film head using a conventional electromagnetic induction phenomenon is used as a magnetic head for recording (hereinafter referred to as a recording head). Actually, an MR composite thin film magnetic head in which this reproducing head and recording head are combined together is used. Hereinafter, this MR composite thin film magnetic head is referred to as a thin film magnetic head.
[0003]
FIG. 8 shows the structure of a thin film magnetic head currently used. A lower shield 2, an insulating layer 3, and a middle magnetic pole 4 are formed on the substrate 1, and an MR element 5 is formed between the lower shield 2 and the middle magnetic pole 4. Here, the middle magnetic pole 4 also has a function as a shield. A recording gap film 6 is formed on the middle magnetic pole 4, and a thin film coil 7 is further formed. An insulating layer 8 is formed to insulate the thin film coil, an upper magnetic pole (pole tip 9a, yoke 9b) is formed, and a protective layer 10 is formed on the uppermost layer to protect them. Japanese Patent Laid-Open No. 11-213331 shows that it is effective to manufacture an upper magnetic pole from two parts in a head having a recording track width of 1 micron or less. This thin film magnetic head applies a recording current to the thin film coil 7 to induce a recording magnetic flux in the upper magnetic pole 9 and the middle magnetic pole 4, and in the vicinity of the recording gap, a leakage magnetic field from the upper magnetic pole 9 and the middle magnetic pole 4 causes an air bearing. A magnetization pattern is recorded on a recording medium installed in the vicinity of the surface 11. In reproduction, a magnetic field generated from the magnetization pattern of the recording medium is detected by an MR element.
[0004]
[Problems to be solved by the invention]
In the field of magnetic disk devices, high density and high frequency are progressing. When the frequency becomes high, the change in the magnetic flux of the magnetic pole cannot follow the change in the required recording signal, and the rise time of the recording magnetic field is delayed. This delay has a problem that the recording / reproduction characteristics such as the overwrite characteristic (O / W) and the non-linear magnetization transition point shift (NLTS) deteriorate. How to make the magnetic flux change of the magnetic pole follow the required change of the recording signal is a problem to be solved by the prior art. An object of the present invention is to provide a thin film magnetic head in which this problem is suppressed.
[0005]
[Means for Solving the Problems]
The thin film magnetic head of the present invention includes a magnetoresistive element for reading between a lower shield and a middle magnetic pole, and has an upper magnetic pole facing the middle magnetic pole with a gap layer made of a nonmagnetic material interposed therebetween, The upper magnetic pole is composed of a pole tip and a yoke, the width on the gap layer side of the pole tip is a width that defines the recording track width, and the end surface of the pole tip constitutes an air bearing surface together with the end surface of the middle magnetic pole, The yoke is provided between the pole tip and the middle magnetic pole, a surface joining the yoke and the middle magnetic pole is a back contact surface, and a portion joining the middle magnetic pole is the back yoke, the air bearing A thin film coil between the middle magnetic pole and the upper magnetic pole so as to generate a magnetic flux for writing to the magnetic recording medium on the surface, The thickness of the middle pole of the portion in contact with the click, characterized in that it has the following thickness of the central pole in the vicinity of the air bearing surface.
[0006]
Next, the operation of the present invention will be described. The present invention focuses on the fact that the delay time of the magnetic flux change of the magnetic pole with respect to the change of the recording signal can be reduced by reducing the eddy current loss generated in the magnetic path of the magnetic head.
[0007]
However, with the increase in recording density of magnetic recording apparatuses, the track width is being narrowed so that the track width of the recording magnetic pole becomes 1 mm or less. If a single upper magnetic pole is formed and used, it is difficult to process the conventional structure. A method of manufacturing the top pole in two parts is advantageous. In that case, the volume of the back yoke 9c in contact with the surface S1 (hereinafter referred to as the back contact surface) where the middle magnetic pole and the yoke are in contact increases. As a result, eddy current loss increases. The magnetic recording head desirably has the same product of the cross-sectional area φ of the magnetic path other than the constricted portion at the tip of the magnetic pole near the air bearing surface. However, only the area of the back contact surface S1 is increased due to a process problem. Therefore, in view of this point, an object of the present invention is to make the magnetic flux change of the magnetic pole follow the change of the necessary recording signal without reducing the recording magnetic field strength.
[0008]
First, we examined the influence of the volume of the back yoke 9c on the recording magnetic field strength and the magnetic field rise time. It has been found that the rise time of the recording magnetic field can be reduced without decreasing the recording magnetic field strength by reducing the volume of the back yoke 9c. This is because eddy current loss can be reduced. Further, even if the volume of the side yoke 9d adjacent to the back yoke is reduced, the recording magnetic field strength is not affected. Therefore, the eddy current loss of the magnetic head is reduced without reducing the recording magnetic field, and the magnetic flux change of the magnetic pole follows the change of the necessary recording signal.
[0009]
DETAILED DESCRIPTION OF THE INVENTION
FIG. 1 is a graph illustrating an improvement in the rise of the recording magnetic field. 2 and 5 are sectional views of a thin film magnetic head of a reference example .
[0010]
Reference Example FIG. 1 shows the rising characteristics of the recording magnetic field of the thin film magnetic heads of this embodiment and the conventional example. In FIG. 2, the thin film magnetic head of this embodiment has the configuration shown in FIG. As shown in FIG. 1, the configuration of the present invention has a faster rise of the recording magnetic field than the conventional configuration. Therefore, according to this embodiment , it is possible to reduce the delay of the magnetic flux change of the magnetic pole with respect to the required change of the recording signal without reducing the recording magnetic field.
[0011]
The thin film magnetic head of FIG. 2 is opposite to the back contact surface S1 from the back contact surface S1 to the back contact surface S1 of the back yoke 9c from the distance L1 from the back contact surface S1 to the upper end surface S2 on the opposite side of the surface contacting the gap film 6 of the pole tip 9a. The distance L2 to the side surface S3 is made small. Thereby, the increase in the area of the magnetic path which increases on the back contact surface can be reduced. The order of lamination will be described. First, a lower shield 2 made of NiFe alloy, an alumina film, an MR element 5, an alumina film, and a middle magnetic pole layer 4 are laminated on an alumina titanium carbide substrate 1 covered with an insulating film. The alumina films sandwiching the MR element 5 constitute an insulating layer 3 that functions as a reproduction gap. Next, after forming the recording gap film 6 on the middle magnetic pole 4, a pole tip 9a is formed. Next, for example, an alumina film as an insulating layer is formed, and then the whole is planarized by CMP (Chemical Mechanical Polish). Thereafter, a resist insulating layer 8 that fills the gap between the thin film coils 7 and a yoke 9b were formed. The yoke 9b covers the thin film coil at the center and is joined to the middle magnetic pole 4 at the rear. This joint surface is referred to as a back contact surface S1. Next, the surface S3 of the back yoke 9c, which is a portion on the back contact surface S1 of the yoke 9b, is shaved by ion beam etching such as ion milling so that it is below the upper surface S2 of the pole tip 9a. Thereafter, a protective film 10 is coated on the pole tip 9a and the yoke 9b. Each film is formed with the above-described laminated structure while forming and patterning each film with an appropriate shape and thickness. In this laminated structure, the recording gap film and the side where the reproducing element 5 is provided are polished to form a medium facing surface (air bearing surface) 11. The middle magnetic pole is made of, for example, a NiFe alloy having a Ni concentration of 83 wt%.
[0012]
( Reference Example ) As shown in FIG. 3, most of the back yoke 9c is removed by ion beam etching such as ion milling, and the length L3 of the cross section of the surface in contact with the middle magnetic pole of the back yoke 9c is the yoke 9b. The film thickness t9b or less was formed. Thereby, the increase in the area of the magnetic path which increases on the back contact surface S1 can be reduced.
[0013]
( Reference Example ) Another head is shown in FIG. 4A is a plan view of the upper magnetic pole, and FIG. 4B is a cross-sectional view taken from 4A to 4A ′ in FIG. As shown in FIG. 4, in the other magnetic head, the area A1 surrounded by the dotted line including the back yoke 9c and the side yoke 9d was deleted, and the volume thereof was made smaller than the time when the yoke 9b was created. Further, the middle magnetic pole below the back contact surface S1 may be deleted at the same time.
[0014]
( Reference Example ) Further, as shown in FIG. 5, in another magnetic head, the back yoke 9c and the side yoke 9d are eliminated by ion beam etching such as ion milling, and the cross section of the surface in contact with the middle magnetic pole of the back yoke 9c is used. The length L3 is less than the film thickness t9b of the yoke 9b. Further, the middle magnetic pole 4b below the back contact surface S1 may be deleted at the same time, or the middle magnetic pole may be formed in advance so that there is no middle magnetic pole 4b below the back contact surface S1.
[0015]
(Embodiment 1 ) In this embodiment , as shown in FIG. 6, the film thickness t4b of the middle magnetic pole 4b below the back contact surface S1 is made thinner than the film thickness t4 of the middle magnetic pole 4 near the air bearing surface. In some cases, t4b may be set to zero.
[0016]
Any form state also, so as not to reduce the occurrence recording magnetic field intensity, reduce the cross-sectional area of the magnetic path of flow of magnetic flux, to suppress eddy currents, to reduce the delay of the magnetic poles of the magnetic flux change with respect to the change of the necessary recording signal Further, it is possible to provide a thin film magnetic head capable of realizing high-density and high-frequency recording while suppressing deterioration of recording / reproduction characteristics such as overwrite characteristics (O / W) and non-linear magnetization transition point shift (NLTS).
[0017]
(Embodiment 2 ) Next, the main part of the manufacturing process of a thin film magnetic head according to an embodiment of the present invention will be described with reference to FIG. FIG. 6 shows a thin film magnetic head in which an upper magnetic pole is formed in the manufacturing process of FIG. An insulating film 1a made of alumina is formed on the nonmagnetic substrate 1 made of alumina titanium carbide by sputtering (2-a). A CoTaZr soft magnetic film is formed on the insulating film 1a by sputtering, and this soft magnetic film is patterned into a necessary shape, whereby the lower shield 2 is obtained. Next, an alumina insulating layer 3 and an MR element 5 are formed on the lower shield 2 (2-b). An insulating layer 3a for shortening the middle magnetic pole is produced. The middle magnetic pole 4 is formed on the insulating layer 3 so as to form the same plane as the insulating layer 3a, and then the middle magnetic pole 4 is formed on the middle magnetic pole 4 and the insulating layer 3a. Next, the recording gap film 6 is formed (2-d). Thereafter, by carrying out the subsequent steps as in Embodiment 1, to obtain a thin film magnetic head shown in the sectional view of FIG.
[0018]
In the thin film magnetic head of the present embodiment, the following can be used as the MR element. For example, a SAL bias MR element including a magnetoresistive film, a spacer, and a SAL film, a soft magnetic film bonded with an antiferromagnetic film, a spin valve MR element including a nonmagnetic metal film and a soft magnetic film, and a plurality of soft magnetic elements A GMR element having a structure in which films are stacked, a tunnel junction MR element having a structure in which an insulating film is sandwiched between two soft magnetic films, and the like. The reproducing track width of these reproducing elements is preferably set to be smaller than the width (recording track width) of the top pole tip of the thin film magnetic head.
[0019]
【The invention's effect】
As described above, according to the present invention, by reducing the volume of the back contact portion, the delay of the magnetic flux change of the magnetic pole with respect to the required change of the recording signal is reduced, and the overwrite characteristics (O / W) and non- It is possible to provide a thin film magnetic head capable of realizing high-density and high-frequency recording by suppressing deterioration of recording and reproducing characteristics such as linear magnetization transition point shift (NLTS).
[Brief description of the drawings]
FIG. 1 is a graph showing rise characteristics of a recording magnetic field according to the embodiment of FIG .
FIG. 2 is a cross-sectional view of a thin film magnetic head of a reference example .
FIG. 3 is a cross-sectional view of a thin film magnetic head of a reference example .
FIG. 4 is a cross-sectional view of a thin film magnetic head of a reference example .
FIG. 5 is a sectional view of a thin film magnetic head of a reference example .
FIG. 6 is a cross-sectional view of a thin film magnetic head according to an embodiment of the invention.
FIG. 7 is a process diagram for explaining a manufacturing method according to an embodiment of the present invention.
FIG. 8 is a cross-sectional view of a conventional thin film magnetic head.
[Explanation of symbols]
1 substrate,
1a insulating film,
2 Bottom shield,
3 Insulating layer,
4 Middle magnetic pole,
4b Middle magnetic pole in contact with the back yoke,
5 reproducing element,
6 recording gap film,
7 Thin film coil,
8 Insulating layer,
9a Pole tip,
9b York,
9c Back yoke,
9d side yoke,
10 Protective film,
11 Air bearing surface,
S1 Back contact surface,
S2 Opposite surface in contact with the gap film of the pole tip,
S3 The surface opposite the back contact surface of the back yoke,
L1 Distance between S1 and S2,
L2 Distance between S1 and S3,
L3 Length of side of back contact surface,
t4 Thickness of the middle magnetic pole in the vicinity of the air bearing surface t4b Thickness of the middle magnetic pole in contact with the back contact surface t9b Thickness of the yoke

Claims (1)

下部シールドと中部磁極の間に読み取り用の磁気抵抗効果素子を有し、非磁性材料よりなるギャップ層を挟んで前記中部磁極と対向する上部磁極を有し、前記上部磁極はポールチップとヨークで構成され、前記ポールチップのギャップ層側の幅が記録トラック幅を規定する幅であり、前記ポールチップの端面が前記中部磁極の端面とともにエアベアリング面を構成し、前記ヨークは前記ポールチップと前記中部磁極の間に設けられ、前記ヨークと中部磁極と接合する面はバックコンタクト面であり、前記ヨークの中部磁極と接合する部分はバックヨークであり、前記エアベアリング面において磁気記録媒体に対する書き込み用の磁束を発生させるように中部磁極と上部磁極の間に薄膜コイルを有する薄膜磁気ヘッドにおいて、前記バックヨークと接する部分の前記中部磁極の膜厚を前記エアベアリング面付近の中部磁極の膜厚以下にしたことを特徴とする薄膜磁気ヘッド。  A magnetoresistive element for reading is provided between the lower shield and the middle magnetic pole, and has an upper magnetic pole facing the middle magnetic pole across a gap layer made of a nonmagnetic material. The upper magnetic pole is a pole tip and a yoke. And the width of the pole tip on the gap layer side defines the recording track width, the end face of the pole tip constitutes an air bearing surface together with the end face of the middle magnetic pole, and the yoke and the pole tip Provided between the middle magnetic poles, the surface that joins the yoke and the middle magnetic pole is a back contact surface, and the portion that joins the middle magnetic pole of the yoke is a back yoke, and is used for writing to the magnetic recording medium on the air bearing surface In the thin film magnetic head having a thin film coil between the middle magnetic pole and the upper magnetic pole so as to generate a magnetic flux of Thin-film magnetic head, characterized in that the thickness of the central pole of the portion in contact with the following film thickness of central pole near the air bearing surface.
JP2000022066A 2000-01-31 2000-01-31 Thin film magnetic head Expired - Fee Related JP3842509B2 (en)

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